I /y4-<^6 t 2/, t ^/. "" xr A TREATISE ON PLANE AND SPHERICAL TRIG0NOMETRY. BY WILLIAM CHAUVENET. PROFESSOR OF MATHEMATICS AND ASTRONOMY IN WASHINGTON UNIVERSITY SAINT LOUIS. PHIL AD ELPHIA: J. B. LIPPINCOTT COMPANY. 1887. Entered according to Act of Congress, in tna year 1850, by WILLIAM CHAUVENET, in the Clerk's Offioe of the District Court of the Eastern District of Pennsylvania. -- -- PREFACE. I HAVE in this treatise endeavored to arrange a course of trigonometrical study sufficiently extensive to enable the student to comprehend readily any applications of trigonometry he may meet with in the works of the best modern mathematicians. With this object, some topics have been introduced which are not usually found in works devoted specially to this subject. Among those topics, the most important is the solution of the general spherical triangle, or the triangle whose sides and angles are not limited, according to the usual practice, to values less than 180~. The advantage of introducing such triangles into astronomical investigations is sufficiently shown in the applications made of them in the works of BESSEL and other German mathematicians; and especially in the Theoria Motus Corporum COelestium of GAUSS, who was the first to suggest their employment. The subject of Finite Differences of triangles, plane and spherical, occupies a large space in Cagnoli's treatise, but has not been admitted into more recent works. It here occupies only a few pages, but no important result of 3 4 PREFACE. Cagnoli's Table has been omitted, while a number of the formulaa are much simpler than the corresponding ones given by him. Although my plan embraces a much more extensive course than is contained in the text-books commonly used, I have studiously kept in view the wants of academic and collegiate classes; and have so arranged the work that a selection of subjects of immediate importance may be readily made. The more elementary portions are printed in a larger type, and are intended to form, independently of the matter in the smaller type, a connected treatise which may be studied as though it were in a separate volume. Those who may afterwards wish to extend their knowledge will appreciate the advantage of having the higher departments of the subject treated in connection with those fundamental ones to which they are most intimately re lated. W.C. U. S. NAVAL ACADEMY, Annapolis, Md., May 1, 1850 NOTE TO THE FOURTH EDITION. IN this edition, besides a number of minor changes, and the correction of somt typographical errors, a very important modification has been made in the solution of the equation tan x = p tan y by series (p. 145), which was given in former editions in the usual form as stated by all writers on trigonometry. This form was discovered to lack generality, and consequently to fail in certain applications, in consequence of the omission of the arbitrary term nr now introduced. Several subsequent investigations, depending on this, have in like manner been rectified. W. C..T. S. NAVAL ACADEMY, April 1, 1854. CONTENTS. PART I. PLANE TRIGONOMETRY. CHAPTER I. PAGI MEASURES OF ANGLES AND ARCS........................................................ 9 CHAPTER II. SINES, TANGENTS, AND SECANTS. FUNDAMENTAL FORMULE........................ 14 CHAPTER III. TRIGONOMETRIC FUNCTIONS OF ANGULAR MAGNITUDE IN GENERAL.................. 22 Sine and Tngent of a Small Angle or Arc......................................... 30 CHAPTER IV. GENERAL FORMULE......................................................................... 31 Formulae for Multiple Angles............................................................ 36 Relations of Three Angles............................................................... 38 Inverse Trigonometric Functions....................................................... 41 CHAPTER V. TRIGONOMETRIC TABLES..................................................... 43 Elementary Method of Constructing the Trigonometric Table................ 47 CHAPTER VI. SOLUTION OF PLANE RIGHT TRIANGLES...................................................... 61 Additional Formulae for Right Triangles.................4................... 54 CHAPTER VII. FORMULA FOR THE SOLUTION OF PLANE OBLIQUE TRIANGLES...................... 67 A2 6 6 CONTENTS. CHAPTER VIII. PAG SOLUTION OF PLANE OBLIQUE TRIANGLES........................................... 64 Area of a Plane Triangle...................................................... 74 CHAPTER IX. MISCELLANEOUS PROBLEMS RELATING TO PLANE TRIANGLES........................... 7 CHAPTER X. SOLUTION OF CERTAIN TRIGONOMETRIC EQUATIONS AND OF NUMERICAL EQUATIONS OF THE SECOND AND THIRD DEGREES..................................... 85 CHAPTER XI. DIFFERENCES AND DIFFERENTIALS OF THE TRIGONOMETRIC FUNCTIONS............ 101 CHAPTER XII. DIFFERENCES AND DIFFERENTIALS OF PLANE TRIANGLES................................. 105 CHAPTER XIII. TRIGONOMETRIC SERIES. DEVELOPMENTS OF THE FUNCTIONS OF AN ANGLE IN TERMS OF THE ARC, AND RECIPROCALLY.......................................... 115 Computation of Natural Sines and Cosines by Series.............................. 116 Computation of the Ratio of the Circumference of a Circle to its Diameter 120 Computation of Logarithmic Sines and Cosines.................................... 122 CHAPTER XIV. EXPONENTIAL FORMULAE. TRINOMIAL OR QUADRATIC FACTORS..................... 127 CHAPTER XV. TRIGONOMETRIC SERIES CONTINUED. MULTIPLE ANGLES.............................. 135 Development of the Sine and Cosine of the Multiple Angle in a Series of Ascending Powers of the Cosine of the Simple Angle........................... 137 Development of the Sine and Cosine of the Multiple Angle in a Series of Ascending Powers of the Sine of the Simple Angle.............................. 134 Development of the Sine and Cosine of the Multiple Angle in a Series of Ascending Powers of the Tangent of the Simple Angle....................... 140 Development of any power of the Cosine of the Simple Angle in a Series of Sines or Cosines of the Multiple Angles, the Cosine of. the Simple Angle being positive..................................................................... 141 Development of any power of the Cosine of the Simple Angle in a Series of Sines or Cosines of the Multiple Angles, the Cosine of the Simple Angle being negative......................................................................... 142 Development of any power of the Sine of the Simple Angle in a Series of Sines or Cosines of the Multiple Angles.......................................... 144 Certain Equations developed in Series of Multiple Angles........................ 145 CONTENTS. 7 PART II. SPHERICAL TRIGONOMETRY. CHAPTER I. PAE GENERAL FORMUL..E.................................................................... 149 Gauss's Theorem............................................................................. 161 Additional Formule........................................................................ 162 Deduction of the Formulae of Plane Triangles from those of Spherical Triangles............................................................................. 166 CHAPTER II. SOLUTION OF SPHERICAL RIGHT TRIANGLES................................................ 167 Additional Formulas for the Solution of Spherical Right Triangles........... 176 Quadrantal and Isosceles Triangles...................................................... 177 CHAPTER III. SOLUTION OF SPHERICAL OBLIQUE TRIANGLES......................................... 178 Solution of Spherical Oblique Triangles by means of a Perpendicular...... 206 Computation of Spherical Formulae by the Gaussian Table...................... 211 CHAPTER IV. SOLUTION OF THE GENERAL SPHERICAL TRIANGLE...................................... 214 Note upon Gauss's Equations............................................................ 227 CHAPTER V. AREA OF A SPHERICAL TRIANGLE............................................................ 229 CHAPTER VI. DIFFERENCES AND DIFFERENTIALS OF SPHERICAL TRIANGLES......................... 232 CHAPTER VII. APPROXIMATE SOLUTION OF SPHERICAL TRIANGLES IN CERTAIN CASES............ 241 Legendre's Theorem....................................................................... 244 CHAPTER VIII. MISCELLANEOUS PROBLEMS OF SPHERICAL TRIGONOMETRY......................... 246 PART I. PLANE TRIGONOMETRY. CHAPTER I. MEASURES OF ANGLES AND ARCS. 1. TRIGONOMETRY is that branch of Mathematics which treats of methods of subjecting angles and triangles to numerical computation. 2. PLANE TRIGONOMETRY treats of methods of computing plane angles and triangles. It embraces the investigation of the relations of angles in general, a branch of the science not necessarily connected with the elementary solution of triangles, and which has been distinguished as the Angular Analysis. 3. By the solution of a triangle, in trigonometry, is meant the computation of unknown parts of the triangle from given ones. The triangle has six parts; three angles and three sides. It is shown in geometry, that when any three of these parts are given, provided one of them is a side, the triangle may be constructed, and the unknown parts found by mechanical measurement. In the same cases, by trigonometry, we compute the unknown parts from the three given ones, without resorting to construction and measurement: a method of inferior accuracy, on account of the unavoidable imperfections of the instruments employed, and the difficulty of distinguishing with the eye the smallest subdivisions of lines and angles. But here also the case is excluded in which the three angles are given without a side, because there may be an indefinite number oe plane triangles, whose angles are equal to the same three given ones, as 2 9 10 PLANE TRIGONOMETRY. Pig. 1. in Fig. 1. the triangles A B C, A B C; B, &c. In this case, all these triangles B/> are similar, and their sides are proB/ /zi. ~portional; or the ratio of A B to A 0 / At_- -— C \> is equal to the ratio of A'B'to A' C', A"- -- - ------- ' &c.; so that the ratios of the sides to each other are fixed or determinate, although the absolute lengths of these sides are indeterminate. 4. Now, in order to subject a triangle to computation, we must first express the sides and angles by numbers. For this purpose proper units of measure must be adopted. The unit of measure for the sides of plane triangles is a straight line, as an inch, a foot, a mile, &c.; and the number expressing a side is the number of units of the adopted kind that the side contains. 5. The units by which angles are expressed are, the degree, minute, and second; distinguished by the characters 0~ '. A degree is an angle equal to v of a right angle; or a degree is 3s- of the whole angular space about a point, or 3-0 of four right Fig. 2. angles. Thus, Fig. 2, if the angular space about A' 0 is divided into 360 equal parts, of which A OB is one, then A OB is one degree. The right angle will be expressed by 90~; two right angles by 0 - 180~, and the whole angular space about a point by 360~. A"',A minute is an angle equal to g of a degree. Therefore, 1~ = 60'; and a right angle =-90 x 60'= 5400'. A second is an angle equal to Ul of a minute. Therefore, 1'= 60": 1 =60 60"= 3600"; and a right angle =90 x 60 x 60" 324000". Angles less than seconds are sometimes expressed by thirds, fourths, fifths, &c., marked '" Iv v, &c.; a third being g of a second; a fourth, do of a third; &c. But the more convenient method is to express them as decimal parts of a second; thus { of a right angle will be either 12~ 51' 25" 42"' 5117, &c. or more conveniently 12~ 51' 25".714, &c. 6. The above division of angles is called sexagesimal, from the divisor 60 employed in the subdivision of the degree. The centesimal division, however, would be preferable in all cases, but cannot now be generally introduced without, at the same time, changing the arrangement of all our tables, the graduation of astronomical and MEASURES OF ARCS. 11 other instruments, charts, &c. Nevertheless, the attempt has been made in France, and several standard works exist in the French language, in which it is employed throughout. In the centesimal or French division, the right angle is divided into 100 degrees, the degree into 100 minutes; the minute into 100 seconds, &c. The reduction of these denominations from one to the other requires only a change in the position of the decimal point; thus, in this system 60~ 75' 84"'8 is the same as 607584"'or 60~075848 or 0Oq6075848, the symbol q denoting a quadrant or right angle. To convert centesimal into sexagesimal degrees, since 100~ dec. = 90~ sex. deduct one tenth from the number of centesimal degrees. EXAMPLE. Required the number of sex. degrees in 85~ 47' 43" dec 85~04743 cent. Deduct z = 8 -54743 76~092687 sex. degrees and dec. parts. 55'.6122 36".732 or 76~ 55' 36".732 sexagesimal. To convert sexagesimal into centesimal degrees, since we must take o of the "ex., divide by 9 and move the decimal point oneplace to the right. EXANMPLE. Required the number of centesimal degrees in 76~ 55' 36" 732 sex. Reducing the minutes and seconds to the decimal of a degree, we have 760~92687 sex. io~ of which is 85~-4743 cent. or 85~ 47' 43" centesimal. To distinguish the degrees of the centesimal from those of the sexagesimal divi sion, the former are frequently called grades, and are denoted by the character s instead of o; thus the preceding angle would be 85g 47' 43". MEASURES OF ARCS. 7. Since the angles at the center of a circle are proportional to the arcs of the circumference intercepted between their sides, these arcs may be taken as the measures of the angles, and we may express both the arc and the angle by the number of units of arc intercepted on the circumference. The units of arc are also the degree, minute, and second. They are the arcs which subtend angles of a degree, a minute, and a second, respectively, at the center. A degree of arc is thus always 3-0 of the circumference, whatever the radius of the circle may be: and we obtain the same numerical expression of Fig. 3. an angle, whether we refer it directly to the angular unit, or to the corresponding unit of arc. The right angle A OA', Fig. 3, and its measure, the B quadrant AA', are therefore both expressed by ~ } 90~; the semicircumference by 1800, and the whole circumference by 360~. A"' 8 The radius of the circle employed in measuring angles is then 12 PLANE TRIGONOMETRY. arbitrary, and we may assume for it such a value as will most simplify our calculations. This value is unity; that is, the linear unit employed in expressing the sides of our triangles, or other lines considered. This value will be generally used throughout this treatise. 9. To find the length of an are of a given number of degrees, minutes, &c. The semi-circumference of a circle whose radius is unity is known to be 3.14159265; or, the radius being R, the semi-circumference is 3.14159265 R. hence When R — 1 Arc 180~ = 3.14159265R 3.14159265 c 1~ -0.017453293R = 0.017453293 1' = 0.0002908882R =0.0002908882 1" = 0.0000048481371 = 0.0O0004848137 An arc x therefore, in the circle whose radius is unity, being expressed in degrees, or minutes, or seconds, we find its length by the formula Arc x = 0.017453293 x~ = 0.0002908882:' = 0.000004848137 x". As these factors for finding the length of an arc are often used, it is convenient to have their logarithms prepared.* Thus Arc x = [8.2418774] x~ = [6.4637261] x' = [4.6855749] x" In which the rectangular brackets are used to express that the logarithm of the factor is given instead of the factor itself. EXAMPLE. What is the length of the arc x =38~ 17'48", the radius being - 1. 38~ 17' 48" = 137868" log. 5.1394635 Log. factor for seconds 4.6855749 x= 0.6684031 log. x 9.8250384 10. To find the number of degrees, ~c. in an are equal to the radius. We have, from the preceding article, * The logarithms in the examples of this work will be taken from Stanley's Tables, (published in New Haven, by Durrie and Peck,) the best tables of seven-figure logarithms yet published in this country. MEASURES OF ARCS. 13 1800 _=- --- 570-2957795 3.14159265 2957 =3437'.74677 =206264.806 11. The angle at the center measured by an arc equal to the radius, is often taken as the unit of angular measure, as this angle will be of an invariable magnitude, whatever is the length of the radius. If x is the number of such units in a given angle, the number of degrees, &c., in it will be found by multiplying by the value of the radius in degrees, &c., found in the preceding article. Thus, ~ x R~ 57~02957795 x = [1 7581226] x x' _ xR' = 3437'"74677 x = [3-5362739] x x" - x R" = 206264".806 x = [5-3144251] x Reciprocally, the angle being given in degrees, &c., we reduce it to the unit radius, by dividing by R~, R', or R", thus, R~ x' R" X- =o_ _ which is evidently the same as multiplying by the factors of Art. 9. It appears, then, that an angle is expressed in the unit of this article by the length of the arc which measures the angle in the circle whose radius is unity Hence, an angle thus expressed is said to be given in arc. If we put (as is usual) 7r = 3-14159265 ~ ~ w is the circular measure of two right angles, or it is the expression of two right angles in arc. In trigonometry it is therefore common to employ 7r to denote an angular magnitude of 180~; - a right angle; 2 zr four right angles, &c. 12. The complement of an angle or arc is the remainder obtained by subtracting the angle or arc from 90~. The supplement of an angle or arc is the remainder obtained by subtracting the angle or arc from 180~. Thus the complement of 30~ is 60~; the supplement of 30~ is 150~. Two angles or arcs are complements of each other when their sum is 90~. They are supplements of each other when their sum is 180. 13. According to these definitions, the complement of an aro that exceeds 90~ is negative. Thus the complement of 120~ is 90~- -120~ = —30~. In like manner the supplement of 2000 ti 180' - 200~ =- 20~. 11 PLANE TRIGONOMETRY. CHAPTER II. SINES, TANGENTS, AND SECANTS. FUNDAMENTAL FORMULE. 11. HAVING expressed the sides and angles of triangles by numbers, we are next to find such relations between them as shall enable us to combine these two different species of quantity in computation. As every oblique triangle may be resolved into two right triangles by dropping a perpendicular from one of the angles upon the opposite side, the solution of all triangles is readily made to depend upon Fig. 4. that of right triangles. Let us therefore B" consider a series of right triangles, AB C; B AB'C', AB"C, c., Fig. 4, i which have a common angle A. The angles at B, B', B", being also equal, the triangles are A c a' c" similar; and by geometry BC: AB = B'C': AB' = B"C": AB" or by the definitions of ratio and proportion, BC _ B'C' B" C" AB AB' AB" In like manner it follows that BC B' C' B"C" AC A C' AC" AB _AB' AB" and a AC =A C' A C" Hence it appears that the ratios of the sides to each other are the same in all right triangles having the same acute angle; and, therefore, if these ratios are known in any one of these triangles, they will be known in all of them. These ratios, then, depending on the value of the angle alone, without regard to the absolute lengths of the sides, may be considered as indices of the angle, and have received special names, as follows: 15. The SINE of the angle is the quotient of the opposite side divided by the hypotenuse. SINES, TANGENTS, AND SECANTS. 15 Thus, in the right triangle AB 0, Fig. 5, 1 we designate the sides by the small letters a, b, c, we shall have, (whatever the absolute length of the sides) Fig. 5. B bc a A b — 0 b sin A a-, sin B== c C 16. The TANGENT of the angle is the quotient of the opposite side divided by the adjacent side. Thus tan A - tan B=6' a 17. The SECANT of the angle is the quotient of the hypotenuse divided by the adjacent side. Thus sec A sec B b a 18. The COSINE, COTANGENT, and COSECANT of an angle, are respectively the SINE, TANGENT, and SECANT of the complement of the angle. Since the sum of the two acute angles of a right triangle is one right angle, or 90~, they are, by Art. 12, complements of each other; therefore, according to the preceding definitions, we shall have sin A cos B - c tan A -— = cot B == a b see A = cosec B = _ b cos A = sin B =c cot A tan B= a cosec A = sec B = - a (1) 19. Since -is the reciprocal of -, it follows from the first and a C last of these equations, that the sine and cosecant of the same angle are reciprocals; and from the other equations, also, that the cosine and secant, the tangent and cotangent are reciprocals. That is, sinA ~1 1 sin A -= 1- cosec A= - - cosec A sin A cos A = secA - (2) sec A cos A tan A = cot A= - conf, A tan A t wvu IL -I..1 i dr more briefly, sin A cosec A - cos A sec A = tan A cot A = 1 J (3w PLANE TRIGONOMETRY. t6 SINES, &C. OF ARCS. -Fig. 6. 20. The sine, tangent, and secant of B"'~ —' ~r/~- an are are respectively the sine, tangent, D TAr and secant of the angle at the center AF- /c. A measured by that arc. Thus, Fig. 6, 0 BC / I yB' sin A B - sin A OB= - A"' The sine of an are, therefore, does not depend upon the absolute length of the are, but upon the ratio of the arc to the whole circumference, (Art. 7.) It follows that the relations (2) and (3) are also applicable when A expresses an arc. 21. If the radius = 1, all the trigonometric functions above defined may be represented in or about the circle by straight lines. Representing the arc AB, or angle AOB, by x, we have, when OA.- OB = 1,.B C.B CG sin BC BC BC AT AT OT OT secx-=-O =- 1 O and from the arc A'B = 900 - x we find in the same way cos x = BD =OC cot x = A'T' cosec x - OT' Therefore, in the circle whose radius is unity, the sine of an are, or of the angle at the center measured by that arc, is the perpendicular let fall from one extremity of the arc upon the diameter passing through the other extremity. The trigonometric tangent is that part of the tangent drawn at one extremity of the arc, which is intercepted between that extremity and the diameter (produced) passing through the other extremity. The secant is that part of the produced diameter which is intercepted between the center and the tangent. The cosine is the distance from the center to the foot of the sine. In a circle of any other radius than unity, the trigonometric FUNDAMENTAL FORMULAE. 17 functions of an arc will be equal to the lines drawn as above, divided by that radius. The properties here stated have heretofore been used by mostwriters upon trigonometry as definitions, but without limiting the radius to unity; and it is evidently from this mode of viewing these functions that they have derived their names. 22. Besides the functions already defined, others have been occasionally employed to facilitate particular calculations, as the versed sine, which in the circle is the portion of the diameter intercepted between the extremity of the are and the foot of the sine; thus. Fig. 6, the versed sine of A B is A C, or the radius being = 1, versin x = 1 - cos x (4) by means of which formula we may always substitute versed sines for cosines, and reciprocally. The coversed sine (covers.) is the versed sine of the complement, and suversed sine (suvers.) is the versed sine of the supplement. The chords of arcs have also been used, and may be substituted for sines by the formula ch x = 2 sin - x (5) which is evident from Fig. 6, where if the are -BB'= x, we have chord B B' =3 2 B - =2 sin A B. 23. From what has now been stated, the student will perceive that angles are to be subjected to computation by means of the quantities sine, cosine, &c., commonly designated by the comprehensive term trigonometric functions.* It becomes necessary, therefore, for the computer to know the values of these functions for any given value of the angle. The trigonometric tables contain these values for every minute, and sometimes for every second, from 0~ to 90~; and with these tables all the numerical computations of trigonometry are carried on. In practice, then, we are not required to compute the functions themselves, and we shall therefore defer the methods for that purpose to a subsequent part of this work, and proceed at once with the investigation of the formule and methods by which these tables are rendered available. FUNDAMENTAL FORMULE. 24. Given the sine of an angle, to find the cosine. From the right triangle ABC, Fig. 7, we Fig. 7. have by geometry a2 + b2 = c2 B Dividing by c2, this equation becomes a a2 b2 C2~~~~~~~ C2b. C C~~/~ * Also trigonometric lines, from the properties explained in Art. 21 3 B 2 L8 PLANE TRIGONOMETRY. or, by the definitions of sine and cosine (1), sin2 A + cos A = 1 (6j in which the notation sin2 A signifies ", the square of the sine of A." From this formula, if the sine is given, we find cos2 A = 1 - sin2 A = (1 + sin A) (1 - sin A) cos A = (1 -sin2 A) = /[(1 + sin A) (1 - sin A)] (7) and if the cosine is given, we find sin A = (1 - cos2 A) = [(1 + cos A) (1 - cos A)] () 25. Given the sine and cosine of an angle, to find the tangent. By (1) we have a tan A - also sin A a b a cos A c c b sin A therefore tan A =sin cos A And since the cotangent is the reciprocal of the tangent, cos A cot A = -.sin A 26. Given the tangent of an angle, to find the secant. The right triangle A B, Fig. 7, gives 2= b2 + a2 Dividing by 62, this becomes C2 a2 b21 + 2 (9) (10) or, by the definitions of secant and tangent (1), sec2A = 1 + tan2A (11) This formula applied to the complement of A gives cosec2 A = 1 + cot2 A (12) AFig. 8. 27. The preceding formulae are also T directly obtained from Fig. 8. If the / D I^B angle A OB, or the arc AB, be denoted All _ / HcA by x, the right triangle OBC, gives 0\ ~ /,~BC2 + C02 OB2 or rem g tt te r s ^__\~ ^^^or remembering that the radius is unity, A." by Art. 21, 3in2 x + cos2 x = 1 (13) FUNDAMENTAL FORMULA. 19 The triangle OBC gives by the definition, Art. 16, BC tan A OB B OC0 sin x or tan x (14) Since the angle BCD is the complement of BO, tan BOD cot x, and the triangle BOD gives BD O6 tan BOD D - cos x 01 cot x = -- (15) sin x In a similar manner the triangles AO T, A' OT' give sec2 x-1 + tan2x (16) cosec2 x = 1 + cot2 x (17) 28. The following equations are easily demonstrated by combining (13), (14), (15), (16), (17), and employing the property of the reciprocals (2). They are of frequent use. 1 tan x cos x sin x -= tan x cos x - (18) cosec x sec x cot x 1 cot x sin x cos x = cot x sin x = _ 19 sec x cosec x tan x sin x = (1 -cos' x), cos x = (1 - sin'x) (20) sec x = (1 + tana x), cosec x =/ (1 + cot x) (21) tan z= (sec'x- 1), cot =s /(cosec'x-1) (22) tan x 1 cot x 1 cos x - v/(1 + cot x) 4 (1 - tan x) (24) sin x _ (1 cos" x) tan x - (26) v/(1- sina x) cos x cos x cot x = <(1 -Cos sin x(26 cotx( __ —___o___ V(1-sin ) ( 29. To find the sine, &c. of 300 and 60~. In Fig. 8, let the arc AB = 30~, and BB' = 2 AB = 60~. By Art. 21, sin AB = BC, and by geometry the chord of 60~, or of one. sixth of the circumference, is equal to the radius =- 1; therefore 2 sin 30~ =- 2 BC = BB' 1 whence sin 30~ = == cos 60~ (27) PLANE TRIGONOMETRY. and by (7) cos 30~ = /[(1 + t) (1- i)] =,/( x g) whence cos 30~ =- / 3 = sin 60~ (28) then, by (9) and (2), sin 300 1 tan 300 s- = cot 60~ (29) cos 30~ - V = C cot 300= tan = = tan 600 (30) 1 2 see 300 cos 300 - cosec 600 (31) cosec 300 = sin 30= 2 = sec 60~ (32) 30. To find the sine, &c. of 45~ Since 45~ is the complement of 45~, we have sin 45~ = cos 45~ whence by (13), putting x = 45~, sin2 45~ + cos2 45~ = 2 sin2 45~ = 2 cos2 45~ = 1 sin2 45~ = cos2 450 = 1 sin 45~ = cos 45~ = v 0 = ~ 2 (33) sin 450 tan 450 =cot45~0 os4 =1 (34) cos 450 sec 45~ = cosec 45~ = sin 4 = -/ 2 (35) Fig. 9. A' T These values are readily verified in the circle, / 4D B-^ - Fig. 9, where OA TA' is a square described upon /~ /] \ the radius. The diagonal OT bisects the right - / C- A angle, whence AOT = 45~, and tan 45~ = AT -= OA = 1; cot 450 -A' T= 1; sin 45~ = BC - OC = cos 45~, &c. 31. The sines and cosines of two angles being given, to find the sine and cosine of the sum, and the sine and cosine of the difference of those angles. Fig. 10. Fig. 11. Let the two angles be A 0 B ca and B O C, Figs. 10 and 11. B_,/ B^ At any point B in the line O B draw B C perp. to 0 B. '//^ |^ // | Draw BA and C D perp. to o0 -- - Q_ __0 A-OD OA, and BE perp. to CD. FUNDAMENTAL FORMULiE. 21 Then the triangles B CE and B OA are mutually equiangular, the three sides of the one being perp. to the three sides of the other respectively; therefore the angle B CE = A OB. Let x=AOB=BCE y=BOC Then, Fig. 10, x + y = COD Fig. 11, x — y= COD and in CD BA CE BA CE Fig. 10, sin(x + y) = C - CY 0 = 0+ CO CD BA -E BA CE Fig. 11, sin(x - y)= CO CO- CO CO and in both figures BA BA BO CO = BO X =sin xcos y CE CE CB CO CB X CO =cosx sin y which being substituted in the above expressions of sin (x + y) and sin (x - y) give sin (x + y) = sin x cos y + cos x sin y (36) sin (x - y) = sin x cos y - cos x sin y (37) Again in OD OA-EB OA EB Fig. 10, cos (x + y) = C O-= — C -- OACOD OA + EB OA EB Fig. 11, cos ( —y) =O - C — OC 0 and in both figures, OA OA OB O-=: - X -x = cos x cos y EB EB BC OC OC- = sin xsin y therefore cos (x ) cosx cos y - sin sin y (38) cos (x - y) = cos x cos y + sin x siny (39) and (36), (37), (38), and (39) are the required formule. These may be considered as the fundamental formulae of the trigonometric analysis, and will form the basis of our subsequent investigations. They are equally applicable to arcs represented by x and y (Art. 20). do PLANE TRIGONOMETRY. CHAPTER III. TRIGONOMETRIC FUNCTIONS OF ANGULAR MAGNITUDE IN GENERAi, 82. THE definitions of sine, &c. given in the preceding chapter apply only to acute angles, since the angle is there assumed to be one of the oblique angles of a right triangle. But we shall now take a more general view of angular magnitude and of the functions by means of which it is subjected to computation. Fig. 12. If, Fig. 12, we suppose the line OA to revolve ~ A from the position OA to OA' in the direction of the arc AA' (or from right to left), it will describe B an angular magnitude of 90~; when it arrives at 0 A OA" it will have described an angular magnitude of 180~; at OA"', 270; and at OA again, 360~. A"', If it now continue its revolution, when it arrives at OA' again, it will have described an angular magnitude of 360~ + 90~, or 450~; and thus we may readily conceive of an angular magnitude of any number of degrees. In like manner we may have arcs equal to or greater than one, two, or more circumferences. To obtain trigonometric functions for angles and arcs thus generally considered, we shall avail ourselves of the fundamental formulae established in the preceding chapter; first deducing their values analytically, and then explaining their geometrical signification. 33. To find the sine, &c. of 0~ and 900. In (37) and (39) let x = y; the first members become sin (x - x) = sin 0~, and cos (x - x) = cos 00; and by (13) they are reduced to sin 0~ = sin x cos x - cos x sin x = 0 cos 0~ = cos2 x + sin2 x = 1 and since 0~ and 90~ are complements of each other, Art. 12, sin 0~ = cos 90~ = 0 (40) cos 0~ = sin 90~ = 1 (41) from which by (9) and (2) sin 00 0 tan 00 = cot 90 -- = = (42, cos 0 - FUNCTIONS OF ANGULAR MAGNITUDE. 1 1 cot 0~= tan 90~ t n = =0~ (43) 1 1 sec 0~ = cosec 90~ - --- = 1 (44) cos 0~ I cosec 0~ = sec 90~ -1 1 (45) sin 0~ - 0 -0 34. To find the sine, fc. of 1800. In (36) and (38) let = y = 90~; these equations become by means of the preceding values sin 180~ 1 x 0 + 0x 1=- 0 (46) cos 180~ x O x -lxl= —1 (47) whence by (9) and (2) o 1 tan 180~ = 0 cot 1800 = oo (48) 1 1 sec 180~= =- 1 cosec 1800 = oo (49) 35. To find the sine, &c. of 270~. In (36) and (38) let x =180~, y = 90~, then sin270~ = Ox +(- x 1 = - 1 (50) cos 270~ =(- 1) x 0- x 1 = 0 (51) -1 1 tan 270~ = - 0 oo cot 270~ - = 0 (52) 1 1 sec 270~0= 0- o cosec 270~ = - 1 (53) 36. To find the sine, fc. of 360~. In (36) and (38) let z y= 180~; then sin 360 = Ox (- 1) + (-1) x = 0 (54) cos360~=( —1) x(-1) -0 x0=1 (55) the same values as for 0~, whence it follows that all the trig. fune tions of 360~ are the same as those of 0~. The same process continued will give for 450~ (= 360 + 900), the same trig. functions as those of 90~; for 540~ the same functions as for 180~, &c. 24 PLANE TRIGONOMETRY 37. The preceding values now furnish us at once with the values of the functions for all possible values of the angle. In (36) and (38) let x = 0~, they are reduced to sin y = sin 0~ cos y + cos 0~ sin y = sin y cos = cos 0~ cosy - sin 0~ sin y = cos y which are simply identical equations, and reveal no new property. But if in (37) and (39) we put x = 0~, we have, after substituting the functions of 0~, sin (- y) = -sin y cos (- y) = cos y (56) whence by (9) and (2) sin ( — y) - sil y tan( -) -cosin(- y) =-Siy -tany (57) cos (- y) cos sin ( ) - s y (5) ) cos(-y) cos se y y59) cosec (-y) sin - - -sin =. - cosec y (60) sin (- y) sn y or, the sin., tan., cot., and cosec. of the negative of an angle are the negative of the sin., tan., cot., and cosec. of the angle itself; and the cos. and sec. are the same as those of the angle itself. 38. In (37) and (39) let x = 90~; we find after reduction sin (90~ - y) = cos y cos (90~ - y) = sin y which agree with the definition of cosine, but give no new relations. But in (36) and (38) let x = 90~, we find sin (90~ + y) = cos y, cos (90~ + y) - sin y (61) whence by (9) and (2), tan (90~ + y) = - coty cot (90~ + y) = - tan y (62) sec (900 + y) = - cosec y cosec (900 + y) = secy (63) or, the sin. and cosec. of an angle are equal to the cos. and sec. of the excess of the angle above 90~; and the cos., tan., cot., and sen. are equal to the negatives of the sin., cot., tan., and cosec. of the excess of the angle alove 90~. FUNCTI NS OF ANGULAR MAGNITUDE. 25 39. In (37) and (39) let x 180~; we find sin (180~ - y) = sin y cos (180~ - y) = - cos y (64; tan (180~ - y) = - tan y cot (180-) = - cot y (65) sec (1800 -y) - se y cosec (180 - y) = cosec y (66' or, the sin. and cosec. of the supplement of an angle are the same as those of the angle itself; and the cos., tan., cot., and sec. are the negative of those of the angle itself. 40. If y is acute (that is, less than 90~), all its trig. functions are positive; and since its supplement 180~ - y is obtuse (that is, greater than 90~), it follows from the preceding article, that the sin. and ccsec. of an obtuse angle are positive, while its cos., tan.. cot., and sec. are negative. 41. In (36) and (38) let x = 180~; we find sin (180~ + y) - siny cos (180 + y) = -cos y (67) tan (1800 + y) tan y cot (180 + y) = cot y (68) sec (180~ + y) =- sec y cosec (180~ + y) = - cosecy (69) by means of which, if y is acute, we obtain the values of the sines, &c. of angles between 180~ and 270~. 42. In (37) and (39) let x = 270~; we find sin (270 - y) = - cos y cos (270 - y) = - sin y (70) tan (270 - y) = cot y cot (270 - y) = tan y (71) sec (270 - y) = - cosec y cosec (270~ - ) = - sec y (72) 43. In (36) and (38) let x = 2700; we find sin (270~ + y) = - cosy cos (270 + y) = sin y (73) tan (270~ + y) = - cot y cot (270~ + y) = - tany (74) sec (270~ + y) = cosec y cosec (2700 + y) = - sec y (75) 44. In (37) and (39) let x = 360~; we find sin (360~ - y) = - sin y cos (360 - y) = cos y (76) tan (360~ -y) = - tan y cot (360~ - y) = -cot y (77) sec (360~ - y) = sec y cosec (360 - y) =- cosecy (78; or the functions of 360~ - y are the same as those of - y (Art. 37) 45. In (36) and (38) let x = 360~; we find sin (360~ + y) = sin y cos (360~ + y) = cos y (79, or, the functions of an angle which exceeds 360~ are the same as those of the excess above 360~. 4 C PLANE TRIGONOMETRY. It follows that the functions of 720~ + y are the same as those of 360~ + y, and therefore the same as those of y; and in like manner for an angle which exceeds any multiple of 360~. 46. Since y - 90~ is the negative of 90~ - y, we obtain from Art. 37, sin (y - 90~) = - sin (90~ - y) _ - cos y cos (y - 900) =cos (900 - y) =sin y whence also tan., &c.; and in the same manner we may find the functions of y - 180~, y - 270~, y - 360~, &c. 47. We shall now give the geometrical interpretation of the preceding results. rig.13. In Fig. 13, let the radius revolve from the B position OA to OA', OA", &c., as in Art. 32, si/ s \ sithus describing a continuously increasing an1 C> ~gular magnitude; or, which is equivalent, let Al" O A the arc commencing at A increase continuoussin _ i / ly to AB, AA', AB', &c. Then the changes \ cos- _ os B / in the values of the several trigonometric lines ~,A"' may be traced as follows. 1st. The sine being, by Art. 21, the perpendicular from one extremity of the arc upon the diameter drawn through the other extremity, we shall have sin AB = B C, sin AB' = B' C', sin A A" B" = B" C', sin AA"B"' = B"'C, and if we make AB = A" B' = A" B" = AB"' = y we have siny = BC sin (180~ - y) = B' C' sin (180~ + y) = B" ' sin (360~ - y) = B"' C The lines BC, B' C', B" C', B"' C, however, represent only the numerical values of the sines, and are here equal. But the results above obtained from our formulae enable us to distinguish between them by means of their algebraic signs. Thus, by (64), (67), (76), sin (180~ - y) =sin y sin (1800 + y)=-sin y sin (360 -y)= - sin y so that the sines from 0~ to 180~ are positive, while those from 180~ to 360~ are negative; or the sines which are above the diameter A A" are positive, while those which are below this diameter are FUNCTIONS OF ANGULAR MAGNITUDE. 27 negative; or still more generally, the sines that have opposite atrections, with reference to the fixed diameter from which they are measured, have opposite signs. 2d. The cosine being, by Art. 21, the distance from the center to the foot of the sine, we have cos y =o 0 cos (180~ - y)= 0 C' cos (180~ + y)= 0 C' cos (360~ - y)= 00 but by (64), (67), (76), cos (180 - y) = - cos y cos (180~ + y) = - cosy cos (360~ - y) = cos y so that the cosines on the right of the diameter A'A"' are positive, while those on the left of this diameter are negative; or rather the cosines that have opposite directions, with reference to the diameter from which they are measured, have opposite signs. We have here only exhibited a well-known principle in the application of analysis to geometry, viz.: that all lines measured in opposite directions from a fixed line have opposite signs. To interpret the results (56), it is only necessary to observe that a negative arc will be one reckoned from A towards B"', or in the opposite direction to that of the positive arc, so that sin A B"' = sin (- y) B"'" = - B -= - siny cos ASB' = cos (- y) = 0 C= cosy as in (56). The same principle applies to the tangents, but it will be simpler in practice to obtain their signs (as also those of the secants), ana. lytically, from those of the sine and cosine, as has been already shown. It will be sufficient to bear in mind the following table, which is alsc expressed by Fig. 13. 1st QUAD. 2d QUAD. 3d QUAD. 4th QUAD. SINE + + - CCSINE + + PLANE TRIGONOMETRY. Fig. 13. 48. The particular values of the sine and k,>,~~.B cosine at A, A', A", &c., or sin. and cos. of / ~+ sn 0~, 90~, 1800, &c. may also be found by Fig. 13, upon the same principles; but this Al C.o - A we leave to the student. B"\ - sin- / 49. GENERAL REMARK.-In the demon\os -- ostB stratimn of the fundamental formulae for A',, sin (x y), and cos (x y), Art. 31, the angles x, y and xiy were all taken less than 90~ and positive. In this chapter these formulae have been applied to angles of any magnitude, and the resulting functions have been shown to take opposite signs when the lines representing them take opposite directions. It follows that, in deducing trigonometric formulae from geometrical figures, we need not embarrass our demonstrations with the consideration of the various cases of the problem, or of the various values of the angles of the figure. The formula deduced from any supposed position of the lines of the figure will be of general application, provided in the practical application of this formula to the particular cases, we observe those values and signs of the trigonometric functions which have now been determined. 50. The results of this chapter may be expressed by a few general formulae. From (79) it appears that all the trigonometric functions return to the same values after one or more complete revolutions of 360~. If we represent the semi-circumference, or two right angles, by Tr (Art. 11), and let n = any whole number or zero, we shall have sin 4 n 0 cos 4 n -1 (81) 2 (81) sin (4 n + 1) - 1 cos (4 n + 1) 2 0 (82) sin (4 n + 2) =0 cos (4 n + 2) =-1 (83) sin(4 + 3) -=- 1 cos (4n + 3) -=0 (84) whence tan 4 n = 0 tan (4 n + 1) 2 tan (4 n +2) - =0 tan (4n+ 3) - =c or the tan. of the even multiples (f = 0, and of the odd multiples - cto. so that we may write more simply 'an2n -=0 tan (2 n + 1) - =- 0 2t (w) FUNCTIONS OF ANGULAR MAGNITUDE. 29 In these formulae we have only to give n one of the values 0, 1, 2, 3, 4, &c., to obtain the functions of any given multiple of the right angle. Thus, we find Bin 450l~ sin 5 - sin (4 -+ 1) - 1 by making n = 1, in (82). Since the subtraction of 8 n from the arc will not change the functions, tal above formulae are also true when n is a negative whole number. 51. In a similar manner we obtain sin [4 n - y] + sin cos [4 n + ] =cos y (86 sin[(4n+l) -+y]=cosy cos [(4n+1) +y] =- siny(87) sin [(4n +2) j-+y =-siny cos (4 n + 2) + y -cosy (88) sin [(4 n+3) 2+y = —cosy cos [(4 3) + ] =siny (89) tan [2 n + ] tan tan [(2 n + 1) + =-cot y (90) in which n may be any whole number, positive or negative, and y any angle, positive or negative. 52. A still more concise form may be given to the formule of the two preceding articles, as follows: n being, as before, any whole number, positive or negative. sin 2 n 0 cos 2 n - (-1) (91) sin(2 n + 1) =(-1)" cos (2 n + 1) = (92) sin 2 n -^ Y]=-(-l)nsiny cos 2 n - + y]- (-l)ncosy (93) n [(2n-4 1)- +y ]=-(-l)"cos y cos[(2n+ i) 2 +y = ---- )siny (94) and from these (85) and (90) may be directly deduced. 53. We have seen that an angle being given, there is but one corresponding sine. On the other hand, a sine being given, there is an indefinite number of angles corresponding; for if a denote the given sine, and y any corresponding angle, then a is also the sine of all the angles - y, 2 T + y, 3 - y, &c. - y, - 2 - + y, - 3 z - y, &c. or in general a = sin y =: sin [ n +- (- l) y] (96) o2 80 PLANE TRIGONOMETRY. In like manner if a is a given cosine, and y any corresponding angle, a = cos y = cos (2 n or i y) (96) and if a is a given tangent corresponding to the angle y, a = tan y = tan (n -+- y) (97) SINE AND TANGENT OF A SMALL ANGLE OR ARC. Fig. 14. 54. When the angle A OB = x, Fig. 14, Zs Al very small, the sine and tangent are very nearly equal to the arc AB, which measures the angle, ~ the radius being unity; and the cosine and secant 0Al A are nearly equal to OA= 1 (Art. 21). Therefore, to find the sine or tangent of a very small Al,,, angle approximately, we have only to find the ength of the arc by Art. 9; thus sin 1" = arc 1" = 0.000004848137 log. sin 1" = 4.6855749 and x being a small angle, or arc, expressed in seconds, sin x = tan x = x sin 1" (98) If x is expressed in minutes, sin x = tan x = x sin ' (99) If x expresses the length of the arc, the radius being unity, sin x = tan x = x (100) The employment of these approximate values must be governed by the degree of accuracy required in a particular application. It is found, for example, that they are sufficiently accurate when the nearest second only is required in our results, provided the angle does not much exceed 1~. 55. If x and y are any two small angles, it follows from the preceding article that sin x: sin y = x sin 1": y sin 1" = x: y that is, the sines (or tangent) of small angles are proportional to the angles themselves. The av ication of this theorem, however, lilk that of the preceding, mus depend upon the accuracy required in the problem in which it is emplofed.* * For a full discussion of the limits under which this theorem may be employed, see a paper, by the author of this work, in the Astronomical Journal, (Cambridge, Miss.) Vol. i. p. 84. GENERAL FORMULA. 81 CHAPTER IV. GENERAL FORMULAE. 56. WE, have already obtained four fundamental equations, (36), (37), (38), and (39), involving two angles, x and y. From these we shall now deduce a number of formule, either required in the subsequent parts of this work, or of general utility in the applications of trigonometry. 57. The sum and difference of the equations (36) and (37) are sin (x + y) + sin (x - y) = 2 sin x cos y (101) sin (x + y) - sin (x - y) =2 cos x sin y (102) and the sum and difference of (38) and (39) are cos (x + y) + cos (x -y) = 2 cos x cos y (103) cos (x + y) - cos (x - y) = - 2 sin sinin y (104) 58. If we put x + y -x x-y.y whence 2 x =x' +', y', x (x' + y') 2y = x'-y', y = (X' - y) equation (101) will become sin x' + sin y' = 2 sin - (x' + y') cos - (x' -y) and (102), (103), and (104) admit of a similar transformation. But since x' and y' admit of all varieties of value, we may omit the accents and apply the formulae to any two angles x and y; we have thus sin x + sin y = 2 snm (x + y) cos 1 (x - y) (105) sin x - sin y = 2 cos I (x + y) sin - (x - y) (106) cos x + cos y = 2 cos - (x + y) cos I ( - y) (107) cos x - cos y — 2 sin X (x + y) sin (x - y) (108) Each of these equations may be enunciated as a theorem; thus 382 PLANE TRIGONOMETRY (105) expresses that ",the sum of the sines of any two angles is equal to twice the sine of half the sum of the angles multiplied by the cosine of half their difference." These formula are of frequent use (especially in computations performed by logarithms), in transforming a sum or difference into a product. 59. Dividing (105) by (106), we have by (14) and (15) sin x - siny tan ' (x + y) cot l- (x - y) sin x - sin y or by (2) sin x +siny tan(x y) (109) sin x - siny tan ~- (x - y) and from (107) and (108) we find in the same manner -Cos --- =c- - tan (x + y) tan I ( - y) (110) cos x + cosy 2\ y \ \ We find also sin x + siny Cos -cosy tan (x + y) (111) sin-sin- y =tan (x- y) (112) cos x + cosy sin x + sin y cos x cosy 2 - sin x - sin cot + cos -- cosy 60. Divide the equations (36), (37), (38) and (39) by cos x cos y; then by (14) we have sin( + ) tan x + tan y (15 cos x cos y sin (x - = tan x - tan y (116) cos x cos y cos (x + y)'= 1 - tan x tan y (117) cos x cos y cos (x — y) + tan x tan y (8 cos x cos y GENERAL FORMULAE. 61. Divide (36), (37), (38) and (39) by sin x sin y; and by sin x cos y; then sin (x s y) g^ =s -coty t cot x (119) cos (x: cot coty F 1 (120) sin x sin y sin (x- 1 = = cot x tan y (121) sin x cos y osin (x o) - cot x F tan y(122) sin x cos y 62. Divide (115) by (117), and (116) by (118); then by (14) tan x- +tan y tan (x + ) tan n y) (123) 1 - tan x tan y tan (x - y) tan x -tany (124) tan tan (124)tany by which, when the tangents of two angles are given, we may compute the tangent of their sum or difference. To find the cotangent of the sum or difference when the cotangents of the angles are given, divide (120) by (119), cot / (x- cot y cot x =F 115 cot y4 cot x 63. Dividing (115) by (116), and (117) by (118), (or from the equations of Art. 61), we have sin (x + y) tan x + tan y coty + cot (6x sin (x - y) tan x- tan y -cot y - cot x cos (x +y) 1 — tan x tan y cot x cot y -1 (7 cos (x -y) -1 + tan x tany 3ot x cot y + 1 64. Formulke for secants are obtained from those for cosines by means of (2), thus we find sec (z tby) --- cos x cos y =F sin x sin y and multiplying numerator and denominator by sec x sec y, ( i \ 1sec a sec y, sec (x -4- y) tan z setan y (128) v5 -v/1 =ptan x tan 34 PLANE TRIGONOMETRY. Alsc since 1 1 cos y if: cos x sec x _t: sec y --- = - cos x cosy cos x cos y we find by (107) and (108) 2 cos - (x + y) cos I (x - y) sec x - sec y = 2 CO ( + Y) c y) (129) cos x cos y sec x - sec Y = 2 sin s (x + y) sin (x -y) (13G sec x — sec y - ( - — 3 cos x cos y In the same manner from (105) and (106) 2 sin x (x + y) cos a (x - y) cosec x + cosec y = — 2 (131) sin x sin y 2 cos ~ (x + y) sin k (x- y) cosec x-cosec y = — sin x sin y (132) sin a sin y \^OM! These formulae, although generally omitted in treatises on trigonometry, will be found useful in a subsequent part of this work. 65. The product of (36) and (37), and of (38) and (39), are sin (x + sin (x - y)= sin2 x cos2 - cos2 x sin2y cos (x + y) cos (x - y) = cos2 x cos2 y- sin2 x sin2y By (13) we have cos2 x = 1 - sin2 x and cos2 y 1 - sin/ y, which substituted in the preceding equations, give sin (x + y) sin (x - y) = sin2 - si2 = cos2y - cos2 x (133) cos (x + y) cos ( - y) = cos2 - sin2 = cos2 y sin2 x (134) 66. In (36), (38) and (123), let y = x, we find sin 2 x 2 sin x cos x (135) cos 2 x =cos2 x - sin2 x (136) 2 tan x tan 2 1- tan2x (137) by which the functions of the double angle may be found from those of the simple angle. 67. To find the functions of the half angle from those of the whole angle, we have, from (13) and (136), cos2 x + sin2 x = 1 cos2 x - sin2 x - cos 2 x the sum and difference of which are 2 cos2 x = 1 +'cos 2 x 2 sin2x = 1 - cos 2 x GENERAL FORMUL.E. 35 As these express the relations of an angle 2 x and its half x, their meaning will not be changed by writing x and ~ x instead of 2 x and x; whence 2 cos2 = 1 + x cos x (138) 2 sin2 ~ x 1 - cos x (139) the quotient of which is 1 +- cos x tan2 x =1 + cos (140) 68. The fcllowing may be proposed as exercises. 2 tan I x 2 sin x- = -tan xcotx+tanix (141) 2 tan ~ x 2 tan z =t(142) tan x -1 — tans- - x= cot x x-tanx (142) tan ~ x - 2 cot x tan x -1 = 0 (143) tan f x - 2 cosec x tan x - 1 = 0 (144) 1 - tang I z cos x = tan (145) 1 - cos z tan t x = cosec x- cot x = x (146) sin x cot x = cosec x + cot x c= Cs x (147) sin x 14- sin x - cos x t 1 +- sin x - cos (148) 69. Several useful formule result from the preceding, by introducing 45~ or 30~. If x = 45~ in (36), (37), (38), and (39), we have, by (33), cos y vq sin y sin (45~ y) = cos (45~ =F y) - (149) whence cos y q- sin y tan (45~ i y) = cot (45 = y) = (150) cos y=F sin y in which either the upper signs must be taken throughout, or the lower signs throughout. If we divide the numerator and denominator of (150) by cos y or sin y, 1 - tan y cot y 1 tan (45~ y) = -1 tan y - cot y F 1 (151 6 PLANE TRIGONOMETRY. From this, by (57), tan -- 1 tan (y - 45) tan + (152) 70. Again, let x = 90~ d= y in (138), (139) (140), and (146), sin (4.50 ~ y) = cos (45~0 = y) = (1 s y) (153) tanr(450o ) = ( 1 ^ );l:tF sin y ) (154) tan (450 ^1) (154 F 1 sin y tan (45~ i y) = sy 1 + - s in ycos y (155 From the last we find 2 tan (45~ + ~ y) + tan (45~ - y y) -- =2 sec y (156) Cos y tan (450- y)- tan (45~ - ~ y) - = 2 tan y (157) cos y the quotient of which is tan (450 + I y) - tan (450 - s y) in tan (45~ + I y) + tan (45~0 - y)5) 71. In (101), (102), (103) and (104), let x = 30; then by (27) and (28) sin (30~ + y) + sin (30~ -y) = cos y (159) sin (30 + y)- sin (30 - y) = sin y V 3 (160) cos (30~ + y) + cos(30~ - y)= cos y 3 (161) cos (30~ + y) - cos (30 - y) = - sin y (162) and in a similar manner we may introduce 60~; but it is unnecessary to extend these substitutions, as they involve no difficulty, and can be made as occasion demands. FORMUL2E FOR MULTIPLE ANGLES. 72. From (101) and (102) we have sin (y + x) 2 sin y cos x - sin (y- x) sin (y + x) 2 cos y sin x + sin (y - x) in which let y = (m - 1) x; then sin ma = 2 sin (m - 1) z cos x - sin (m - 2) x (163) sin mx 2 cos (m - 1) x sin x + sin (m - 2) x '164) which are the general formula for computing the sine of any multiple mx, from the lower multiples (m — 1) x and (m - 2) x, and the simple angle x. FORMULAE FOR MULTIPLE ANGLES. 87 If we make m successively 1, 2, 3, 4, &c., these formule give sin x = sin x = sin x sin 2 x =2 sin x cos x = 2 cosx sin sin 3 x =2 sin 2 x cosz - sin x = 2 cos 2 x sin x - sin x sin 4 x = 2 sin 3 x cos z - sin 2 x = 2 cos 3 x sin x + sin 2 x &c. &c. 73. From (103) and (104) cos (y +- x) = 2 cos y cos x - cos (y -x) cos (y + x) = - 2 sin y sin x +- cos (y - x) which if we put y = (m - 1) x, become cos mx = 2 cos ( - 1) x cos x - cos (m -2) x (165) cos mx = - 2 sin (m - 1) x sin x + cos (m - 2) z (166) If m is taken successively equal to 1, 2, 3, 4, &c. cos x - cos X - cos x cos 2 x = 2 cos x cos - 1 - 2 sin x sin x - 1 cos 3 x = 2 cos 2 x cos x - cos x - 2 sin 2 x sin x - cos x cos 4 x = 2 cos 3 x cos x - cos 2 z = - 2 sin 3 x sin x - cos 2 x &c. &c. 74. In (123) let y = (m - 1) x; then tan mx tan (m-1) x - tan z (167) 1 - tan (m - 1) x tan x whence tan 2 x - tan x tan x = tan x tan 3 x tn — - 1 - tan 2 x tan x 2 tan x tan 3 x - tan x tan 2 x tans tan 4 xt3t 1 - tan z 1 -tan 8 X tan z &c. 75. If in the expression for sin 3 x, Art. 72, we substitute the value of sin 2 x, we find sin 3 x = 4 sin x cos3 x - sin x by which we find the sine of the multiple directly from the functions of the simple angle. If this be substituted in the expression for sin 4 x, the latter will also be expressed in terms of the simple angle. By these successive substitutions we easily obtain the following tables: sin x = sin x sin 2 x = 2 sin x cos x sin 3 x = 4 sin x cos' x - sin x sin 4 x = 8 sin x cos3 x - 4 sin x cos x &c. 76. cos x = cos x cos 2 x = 2 cos x- 1 cos 3 x = 4 cos x - 3cos x cos 4 x 8 cos' x - 8 cos x + 1 D 38 PLANE TRIGONOMETRY. 77. If in these equations we substitute for cos2 x = I - sin' x they become sin x = — sin z sin 2 x = 2 sin x / (1 - sin2 x) sin 3 x = 3 sin - 4 sin' x sin 4 z = (4 sin x - 8 sin' x) / (1 - sin' x) &c. 78. cos x - (1-sin x) cos 2 x = 1 - 2 sin2 x cos 3 x = (1 - 4 sin2 x) / (1 - sin' x) cos 4 x = 1 - 8 sin' x + 8 sin4 x &c. From the preceding tables it appears that the cosine of the multiple angle may always be expressed rationally in terms of the cosine of the simple angle; but that the sine of only the odd multiples and the cosine of only the even multiples can be expressed rationally in terms of the sine of the simple angle. 79. By successive substitutions we find from the formulae of Art. 74. tan x tan x 2 tan x tan 2 x =-ta 1 -tan' x 3 tan x - tan' x tan 3 x -- - 1 - 3 tans x 4 tan x- 4 tan3 x 1 —6 tan' x + tan4 x &c. 80. The preceding results are but particular applications of general formulae to be given hereafter, (Chapter XV.) They are introduced here for the convenience of reference in elementary applications. The powers of the sine or cosine of the simple angle may also be expressed in the multiples of the angle: but they are most readily obtained from the general formulae of Chapter XV. RELATIONS OF THREE ANGLES. 81. Let x, y, and z be any three angles; we have, by (36) and (38), sin (x + y + z) = sin (x + y) cos z + cos (x + y) sin z =sin x cos y cos z - cos x sin y cos z + cos x cos y sin z - sin x sin y sin z (18) cos (x + y + z) = cos (x + y) cos z - sin (x + y) sin z = cos x cos y cos z - sin x sin y cos z - sin x cos y sin z - cos x sin y sin z (169) and in the same way we may develop the sines and cosines of x +- y - z, x -y - z, &c.; but we may find these directly from (168) and (169) by changing the sign of z. y, &c., and observing (56). RELATIONS OF THREE ANGLES. 39 The quotient of (168) divided by (169) gives, after dividing the numerator and denominator by cos x cos y cos z, tan (x + y 4 z) atan x - tan y - tan z tan z tan y tan z 17) 1 - tan x tan y - tan x tan z - tan y tan z 1 82. Let z, y and z be any three angles, and from the equations sin (x - z) = sin x cos z - cos x sin z sin (y- z) = sin y cos z - cos y sin z let cos z be eliminated; we find sin y sin (x - z) - sin x sin (y - z) = sin z (sin x cos y - cos x sin y) = sin z sin (x - y) If sin z is eliminated, we find cos y sin (x - z) - cos x sin (y - z) = cos z sin (x - y) These equations may be more elegantly expressed, as follows: sin x sin (y - z) + sin y sin (z - x) - sin z sin (x - y) == 0 (171) cos x sin (y - z) - cos y sin (z - x) + cos z sin (x - y) = 0 (172) A number of similar relations may be deduced from these by substituting 90~:z z, &c., for x, &c. 83. Let v = I (x + y + 2) we have by (104) 2 sin v sin (v - x) = cos x - cos (2 v - x) = cos x - cos (y + z) 2 sin (v - y) sin (v - z) = cos (y - z) - cos (2 v - y - z) = cos (y - z) - cos x the product of which is 4 sin v sin (v - x) sin (v - y) sin (v - z) cos x [cos (y - z) - cos (y + z)] - cos' - cos (y - z) cos (y - z) Reducing the second member by (103) and (134); 4 sin v sin (v - x) sin (v -y) sin (v - z) = 2 cos z cos y cos z- cos8 x - cos y -cos z + 1 (173) In the same manner we find 4 cos v cos (v - x) cos (v - y) cos (v - z) = 2 cos x cos y cos z + cos x + cos" y + cos' z - 1 (174) 84. The following may be proposed as exercises. sin x - sin y+ sin z- sin (x+ y + z) = 4 sin ~ (x + y) sin - (x+4 z) sin (y-+z) (175) cos x* cosy - cosz-+ cos (z+y-t) = 4cost (xty) cos -(x+z) cos (Y z- ) (176) sin (x 4' y 4- z) tan x '4 tan y 4 tan z - tan z tan y tan z -- os cos y cos z (177) Cos x cos y cos z cos ( y + Z) 78 cot x + cot y +- cot z- cot x cot y cot z = - sin x sin y sinz (178) 40 PLANE TRIGONOMETRY. 4 [sin (x+y+z} —2 sin x sin y sin z]2 = 4 [sin (xay) cos z- cos (x-y) sin zJ' [= - cos (2 x + 2 y)] (1+ cos 2 z) + [1 + cos (2 x-2 y)] (1 cos2z) (17) (179) - 2 (sin 2 x + sin 2 y) sin 2 z 2 (14-sin 2 xsin2y-sin2 xsin 2 z- sin2ysin2z- cos 2xcos 2 ycos2z) 85. Let the sum of three angles x, y and z be ar, or a multiple of 7r, that is, an even multiple of - a condition which is expressed by the equation x+ y + z-2 n. (180) then, tan (x + y +- z),= 0, and the first member of (170) being thus reduced to zero, the numerator of the second number must be zero, or tan x - tan y - tan z= tan x tan y tan z (181) an equation, it must be remembered, that is true only under the condition (180). Since x, y and z may be selected in an infinite variety of ways so as to satisfy (180), it follows from (181) that there is an infinite number of solutions of the problem, "to find three numbers whose sum is equal to their product." Let the sum of three angles x, y and z be - or an odd multiple of; that is, let 2 2 x + y + + - (2 n + 1)- (182) then, tan (x +- y + z) = oc, and the denominator of (170) must be zero, or tan x tan y + tan x tan z + tan y tan z = 1 which, divided by tan x tan y tan z, gives cot x + cot y + cot z = cot x cot y cot z (183) a relation that holds only under the condition (182). 86. Let fx+y+z-t- =n;r=- 2n 1 ((184) We have by (93) and (91) cos (x - y - z) = cos (n n - 2 z) = (- )" cos 2 z cos (x - y - z) = cos (n r - 2 y) = (- 1)" cos 2 y cos (y + z - x) = cos (n - 2 x) = (- 1) cos 2 x cos (y + z + x) = cos n 7I (- 1) the svms of the first two and of the second two are by (103) 2 cos x cos (y - z) = (- 1)" (cos 2 z + cos 2 y) 2 cos x cos (y + z) = (- 1)" (cos 2 x + 1) and the sum and difference of these equations are 4 cos x cos y cos z = (- 1)" (cos 2 z + cos 2 y - cos 2 x -- 1) 4 cos x sin y sin z = (- 1)" (cos 2 z + cos 2 y - cos 2 x - 1) 0l -+- 4 cos x cos y cos z = cos 2 x - cos 2 y - cos 2 z - 1 (185):t 4 cos x sin y sin z = - cos 2 x + cos 2 y + cos 2 z - 1 (186) the upper sign being taken when n in (184) is even, the lower when n is odd. INVERSE TRIGONOMETRIC FUNCTIONS. 41 In the same manner we obtain =p 4 sin x sin y sin z= sin 2 x - sin 2 y - sin 2 z (187) =F 4 sin x cos y cos z =- sin 2 x -- sin 2 y - sin 2 z (188) the signs being taken as above. Again, let zx+y+z = (2n+1)2 (189; we shall find by the same process fi 4 sin x sin y sin z - cos 2 x -+ cos 2 y + cos 2 z- 1 (190) i 4 sin x cos y cos z - cos 2 x - cos 2 y + cos 2 z + 1 (191):4 4 cos x cosy cos z sin 2 x + sin 2 y + sin 2 z (192) =t 4 cos x sin y sin z - sin 2 x + sin 2 y - sin 2 z (193) -r or - according as n in (189) is even or odd. INVERSE TRIGONOMETRIC FUNCTIONS. 87. If y = in x y is an explicit function of x, and, since x and y are mutually dependent, x is an implicit function of y; but to express x in the form of an explicit function of y, we write* x = sin-' y which is read, 4x equal to the angle (or arc) whose sine is y," and x is called the inverse function of y, or of sine x. In like manner tan- y is ", the angle or arc whose tangent is y," &c. 88. Many of the formula already given may be conveniently expressed with the aid of this notation. Thus, by (16), x = sec-' v (1 + tan' x) or if we put y = tan x tan-' y = sec-' V/ (1 + y) * This notation was suggested by the use of the negative exponents in algebra. If we have y = nx, we also have x - n - y, where y is a function of x, and x is the corresponding inverse function of y. The latter equation might be read " x is a quantity which multiplied by n gives y." It may be necessary to caution the beginner against the error of supposing that sin-' y is equivalent to I For a general view of the nature of inverse functions, see Peirce's Diff Calo Arts. 13, et seq. 6 D 2 42 PLANE TRIGONOMETRY. And in the same way the formulae of Art. 28 give 1 y sin- y = cosec -- = cos- (1 - y') = tan -- (1 cos- y = sec- - sin- / (1-y) tan- / ( Y) tan-y c= ot- =' sin 1 + os V (1+ Y2) Formula (123) and (124) may be written x =1= y = tan. tan x:i tan y z -=tay = tan —' 1 Fq tan x tan y or putting t = tan x, t' = tan y, tan ' t - tan-1 t' = tan-' 1 = (194) Also the formulae of Arts. 67 and 68 give cos- y= 2 sin - ( -Y) 2 cos-J(~ ) = 2 tan J( Y) 2y 2y _ _Y 2 tan-' y = sin1 + =y tan-1 COS, 1 + y 1 -2 y1- 1 + y 89. We may also employ the notation sin-1 (cos x) or "tho arc whose sine is equal to the cosine of x," i. e. "the complement of x"; and sin (cos-' y) or "the sine of the arc whose cosine is y," &c. We shall have accordingly sin (sin-' y) = y tan (tan-' y) = y &c. sin -1 (sin x) = x tan-' (tan x) = x &c. But it must be observed that since the same sine or tangent corresponds to an infinite number of angles, (Art. 53,) these last equations should be wmitten sin-' (sin x) = n 7r + (- 1)" x, tan -1 (tan x) = n -f x which are equivalent to (95) and (97). TRIGONOMETRIC T~LBLES. 48 CHAPTER V. TRIGONOMETRIC TABLES. 90. BEFORE proceeding to the numerical computation ef triangles and to other applications of the preceding formula, the student should make himself acquainted with the arrangement of, and the mode of consulting, the trigonometric tables. We shall here speak of those points only that are common to all tables, but it will be necessary to consult also the explanations that are always prefixed to a table in order to understand any peculiarity that may attach to it. We suppose also that he is acquainted with the nature and use of the common tables of logarithms of numbers. There are two principal trigonometric tables;* the first, called the Table of Natural Sines, sc., contains simply the numerical values of the sines, tangents, &c. for each given value of the angle; the * The most convenient seven-figure tables yet published in this country are Stan. ley's, already mentioned, p. 12. Attached to these are also five-figure tables, and a table of anti-logarithms. Computers, engaged in extensive and varied calculations, generally provide themselves not only with tables of seven figures, but also with those of six, of five, and even of four figures-the selection and use of a particular table in any case being determined by the degree of precision sought for in the results. We might, indeed, employ seven-figure, or even ten-figure tables in all cases, and reject the final figures of our results, when a lower degree of approximation is thought sufficient; but it is clearly a loss of time and labor to employ other figures besides those which are necessary in arriving at the proposed degree of precision. The best six-figure tables are to be found in Bremiker's Nova Tabula Berolinensis, (Berlin, 1852,) which are distinguished for simplicity of arrangement, as well as aocuracy. Bowditch's five-figure tables, in his Epitome of Navigation, are valuable on account of their undoubted accuracy. Four-figure tables are to be found in various collections, as for instance, in Schumacher's Hiilfstafeln, (edited by Warnstorf.) Of the German seven-figure tables we may cite those of Vega, of which Bremiker's edition is the best: of the English, Taylor's, Hutton's, Babbage's, Shortrede's; and *f the French, Callet's, Bagay's, Borda's. Taylor's, Shortrede's, and Bagay's give the log. functions to every second of the quadrant; Borda's give the functions corresponding to the centesimal division of angles, (Art. 6.) For computations requiring more than seven figures recourse must be had to the ten-figure tables of Vlacq, Thesaurus Logarithmorum Completus, edited by Vega, 'Leipzig, 1794.) 44 PLANE TRIGONOMETRY. second, called the Table of Logarithmic Sines, &c., contains the lo. garithms of the numbers in the first table. As the greater part of the computations of trigonometry are carried on by logarithms, the latter table is by far the most useful. TABLE OF NATURAL SINES, &C. 91. The arrangement of this table will be understood from a simple inspection. It contains the sines, &c. of angles between zero and 90~, generally for every minute, and the functions of angles consisting of a number of degrees, minutes, and seconds, have to be found by interpolations similar in their nature to those that are required in using tables of logarithms of numbers. This interpolation is based upon the supposition that the differences of the sines, &c., are proportional to the differences of the angles; and this proportion, though theoretically inexact, gives, in general, a sufficient approximation, provided the differences of the angles of the table are sufficiently small. When the greatest accuracy is desired, the tables should give the angles to every second, or at least to every 10", and the sines, &c., should be given to at least seven decimal places. 92. As every angle between 45~ and 90~ is the complement of another between 45~ and 0~, every sine of an angle less than 45~ is the cosine of another greater than 45~; every tangent is a cotangent, &c.; hence the angles at the top of the tables generally extend only to 45~, and the same functions answer for the remaining 45~, by giving them at the bottom of the table the names of the complemental functions. 93. As the sines, &c., pass through all their possible numerical values, while the angle varies from 0~ to 90~, the tables are not extended beyond 90~; but we easily deduce the functions of all other angles by the principles of Chap. III. For the functions of an angle between 90~ and 180~, we may take thie same functions of its supplement, observing to prefix the proper algebraic sign, Art. 39. Thus, from Hutton's Tables we find sin '140~ 16' = sin 39~ 44' = 0.6392153 cos 140~ 16' = - cos 39~ 44' = - 0.7690278 tan 140~ 16' = - tan 39~ 44' - 0.8311992 cot 140~ 16' - - cot 39~ 44' - 1.2030810 sec 140~ 16' = - sec 39~ 44 - 1.3003431 cosec 140~ 16' - cosec 39~ 44 - 1.5644181 TABLE OF TRIGONOMETRIC SINES. 45 remembering that in the 2d quadrant all the functions are negative except the sine, and its reciprocal, the cosecant. Or, we may (Art. 38) deduct 90~ from the given angle and take from the table the complemental functions of the remainder, prefixing the signs as before; thus sin 140~ 16' - c's 50~ 16'= &c. cos 140~ 16' = - sin 50~ 16' = &c. which is the better practical method, as the subtraction of 90~ may be performed mentally. 94. For angles between 180~ and 270~, we deduct 180~ and take the same functions of the remainder, prefixing the signs that belong to the 3d quadrant, Art. 41; thus sin 220~ 26' - sin 40~ 26' cos 220~ 26' = - cos 40~ 26' tan 220~ 26' = + tan 40~ 26' &c. 95. For angles between 270~ and 360~, we may deduct 270~ and take the complemental functions of the remainder, prefixing the signs that belong to the 4th quadrant, Art. 43; thus sin 331~ 27' = - cos 61~ 27' cos 331~ 27' = + sin 61~ 27' tan 331~ 27' = - cot 61~ 27' &c. Or we may take the same functions of the difference between the angle and 360~, Art. 44, observing the signs. 96. Above 360~ we deduct 360~, and take the same functions with their signs, Art. 45; and if the angle exceeds 720~, 1080~, &c., we deduct 720~, 1080~, &c.; thus cos 840~ 45' cos 120~ 45~ =- sin 30~ 45' tan 1372~ 13' = tan 292~ 13' - cot 22~ 13' TABLE OF LOGARITHMIC SINES, &C. 97. In this table we find the logarithms of the numbers in the Table of Natural Sines arranged in precisely the same manner; it will therefore require but little additional explanation. As the sines and cosines are all less than unity (being by their definitions proper fractions), their logarithms properly have negative indices; but these are avoided in the usual manner by increasing the 46 PLANE TRIGONOMETRY. index by 10, so that we find the index 9 instead of - 1, 8 instead of - 2, &c. The tangents under 45~ being also less than unity, the indices ofitheir logs. are also increased by 10. In some tables, to preserve uniformity, the indices of the logs. of all the functions are increased by 10, so that the log. secants and cosecants are always greater than 10. In using these tables, we have the general rule that for each log. function added in forming a sum we must deduct 10 from that sum. 98. Since sec A - cos A we have log sec A = - log cos A or since the tabular log. cos. is increased by 10, log sec A = 10 - log cos A that is, the log. secant is the arithmetical complement of the tabular log. cosine. For a like reason log. cosec. is the ar. co. of the log. sin.; and log. cot. is the ar. co. of the log. tan. Also since sin A tan A -- cos A log ban A = log sin A - log cos A by which property, together with the preceding, we may obtain by subtraction only, the log. tan. cot. sec. and cosec. from a table containing only the log. sin. and cos. 99. When the natural sines, &c. are negative, we shall in this work indicate it by prefixing the negative sign also to their logarithms;* thus we shall write cos 140~ 16' = - 0.7690278 and log cos 140~ 16' = - 9.8859420 * Strictly speaking, negative numbers have no logarithms, but in practice, the multiplication, division, &c. of numbers is performed without reference to their signs, 1. e. as if they were all positive, and the sign of the result is then deduced from the signs of the factors according to the rules of algebra. We employ logarithms simply to effect the first of these operations, i. e. the multiplication, division, &c. of the numbers considered as positive; and to facilitate the second operation, or the determination of the sign, we prefix to the logs. the signs which are prefixed to the numbers to which they belong. CONSTRUCTION OF TRIGONOMETRIC TABLES. 47 As the logs. of all the trig. functions are positive (being rendered so by the addition of 10 where necessary), it will easily be remembered that the sign in the latter case is not that of the logarithm, but of the number to which it belongs. ELEMENTARY METHOD OF CONSTRUCTING THE TRIGONOMETRIC TABLE. 100. By dividing 7r = 3.1415926 by the number of seconds in 180~, we found (Art. 9) the length of the arc 1", and (Art. 54), the sine of 1", which is sensibly equal to the arc. In the same manner we find, by dividing by 10800, sin 1' = 0.0002908882 and by (7) cos 1' = / (1 - sin2 1') = [( + sin 1') ( - sin ')] = V (1.0002908882 x.9997091118) or performing the arithmetical operations cos 1' = 0.9999999577 Then by (101) and (103) sin (x + y) = 2 sin x cos y - sin (x - y) cos (x + y) 2 cos x cos y - cos (x -y) in which we can suppose y to be constantly equal to 1' and x to become successively 1', 2', 3', &c. Thus, first substituting y = 1', sin (x + 1') = 2 sin x cos 1' - sin (x - 1) cos (x + 1) =2 cos x cos ' - cos (x - 1) then if x = 1', 2', 3', &c., we find for the sines sin 2' = 2 cos 1' sin 1' - sin 0' = 0.0005817764 sin 3' - 2 cos 1' sin 2' - sin 1' = 0.0008726646 sin 4' - 2 cos 1' sin 3' - sin 2' = 0.0011635526 sin 5' - 2 cos 1' sin 4' - sin 3' - 0.0014544407 &c. &c. ard for the cosines cos 2' = 2 cos 1' cos ' - cos 0' = 0.9999998308 cos 3' = 2 cos 1' cos 2' cos 1' = 0.9999996193 cos 4' = 2 cos 1' cos 3' - cos 2' = 0.9999993232 cos 5' = 2 cos 1' cos 4' - cos 3' = 0.9999989425 &c. &c. PLANE TRIGONOMETRY. The whole difficulty in this operation consists in the multiplication of each successive sine or cosine by 2 cos 1' = 1.9999999154; but this multiplication is much shortened by observing that 2 cos 1'= 1.9999999154 = 2 -.0000000846 so that if we put m =.0000000846 we have 2 cos 1' 2 - m and therefore sin 2' = 2 sin 1' - sin 0' - m sin 1' sin 3' = 2 sin 2' - sin 1' - m sin 2' sin 4' - 2 sin 3' - sin 2' - m sin 3' &c. cos 2' = 2 cos 1' - cos 0' - m cos 1' cos 3' = 2 cos 2' - cos 1' - m cos 2' cos 4' = 2 cos 3' - cos 2' - m cos 3' &c. which are computed with great facility. 101. It is not necessary, however, to continue this process beyond 300; for by (159) and (162) we have sin (30~ + y) = cos y - sin (30~ -y) cos(30~ + y) = cos (30~ - y) - sin y so that the table is continued above 30~ by the simple subtraction of the sines and cosines under 30~ previously found. Thus, making y successively 1', 2', 3', &c. sin 30~ 1' = cos 1' - sin 29~ 59' sin 30~ 2' = cos 2' - sin 29~ 58' sin 30~ 3' - cos 3' - sin 29~ 57' &c. cos 30~ 1' = cos 29~ 59' - sin 1' cos 30~ 2' = cos 29~ 58' - sin 2 cos 30~ 3' = cos 29~ 57' - sin 3' &c. This last process requires to be continued only to 45~ since the sines and cosines of the angles above 45~ will be respectively the cosines and sines of their complements below 45~. CONSTRUCTION OF TRIGONOMETRIC TABLES. 49 102. The tangents and cotangents may be found from the sines and cosines by the formulae sin x cos x tan x cot x --- cos x sin x and the secants and cosecants by the formulae 1 1 sec x = -- cosec x = - cos x sin x 103. In so extended a computation as the construction of the entire table, it is necessary to verify the accuracy of the work from time to time, by separate and independent calculations. By means of (138) and (139) we can find from the cosine of an angle the sine and cosine of its half; hence from the cos. 45~ = / we can find sin. and cos. of 22~ 30', and from these the sin. and cos. of 11~ 15 by the same formulae; and from cos. 30~ == - 3 we can find sin. and cos. of 15~, 7~ 30', and 3~ 45'. If these agree with those found by the first process, the whole work may be considered as correct. 104. There are various other angles whose functions can be expressed under finite forms more or less simple, and may therefore be employed for the purpose of verification. Let x == 18~; then 3 x - 2 x = 90~ and cos 3 x = sin 2 x, whence, by Art. 76, 4 cos' x - 3 cos x cos 3 x 2 sin x cos x 4 cos x - 3 = 2 sin x 4 (1 - sin x) - = 2 sin x sin2 x -+ sin x = which equation of the 2d degree being resolved, gives sin z = sin 180 cos 72~ V 5- 1 4 whence cos 18~ - sin 72~ = / (10 + 2 V 5) 4 From these by (138) and (139), we find the sine and cosine of 9~ and 360; than by (37) and (39) those of 360- 300 = 60, whence those of 3~; after which it will be easy to form a table of the exact values of the sines and cosines for every 3~ of the quadrant.* These expressions, however, are not of much use, directly, in the construction of tables, as we have much better methods; but they lead to a formula of verification which is of some importance. We find cos 36~ - 5 - 1 4 * A table of this kind is given by Cagnoli in his Trigonometric. E 7 50 PLANE TRIGONOMETRY. And by (102) sin (72~ + y) - sin (720 - y) -2 cos 72~ sin y = sin sin (36~ + y) - sin (36~ - y) = 2 cos 36~ sin y -= v/5 1 sin y the difference of these equations gives sin (36~ + y) - sin (360 - y) = sin (72~ + y) - sin (720 - y) + sin y which is Euler'sformula of verification. By giving y any value at pleasure, the correctness of five sines of the tables is examined. By substituting 90~ - y for y in this formula it is easily reduced to the following sin (90~ - y) + sin (180 + y) + sin (18~- y) = sin (540 + y) + sin (54 -y) which is known as Legendre's formula, though not essentially different from Euler's. 105. The method that has here been given for computing the trigonometric table, though simple in principle is nevertheless sufficiently operose. The method by infinite series, to be given hereafter, will be found to be much more rapid and simple in practice. SOLUTION OF PLANE RIGHT TRIANGLES. 51 CHAPTER VI. SOLUTION OF PLANE RIGHT TRIANGLES. 106. IN order to solve a plane right triangle, two parts in addition to the right angle must be given, one of which must be a side. The solution is effected directly by means of our Fig. 15. definitions of sine, &c., which are expressed by B the equations (1). As three of the six functions are only the reciprocals of the other three, we shall base the solutions upon the following three; A b c (Fig. 15): a b a sin A - cosA - tanA - c c b Since each of these equations expresses a relation between three parts-an angle and two sides-it follows that in order to apply them, or in order to solve the triangle trigonometrically, there must be given two of these parts; and that of the three parts considered, one must be an angle while the other two are sides. Thus, if an angle and side are given, the third part sought must be a side; but if two sides are given, the third part sought must be an angle. In every instance the choice of the proper equation will be determined by the precept,-employ that trigonometric function of the angle which is equal to the ratio of the two sides considered. 107. CASE. I. Given the hypotenuse and one angle, or c and A. To find a. We consider a, e and A; and since the ratio of a and c is given by the sine, we have sin A = - whence a = c sin A (195) To find b. Considering b, c and A, we have the ratio of b and c expressed by the cosine, or b cos A = - whence b = c cos A (196) To find B. We have B = 90 - A. 52 PLANE TRIGONOMETRY. The required quantities a and b being equal to the product of twn factors, the computation is conveniently performed by the addition of the logarithms of these factors. EXAMPLES. 1. Given c = 672.3412, A = 35~ 16' 25"; to find the other parts. By (195) By (196) c = 672.3412 log 2.8275897 log 2.8275897 A = 35~ 16' 25" log sin 9.7615382 log cos 9.9119049 a = 388.2647 log* 2.5891279 b = 548.9018 log* 2.7394946 Ans. a = 388.2647 b = 548.9018 B = 54~ 43' 35" 2. Given c = 42567-2, B = 87~ 49' 10"; find the other parts. Ans. a = 1619.626 b = 42536.37 A = 2~10'50" 108. CASE II. Given the hypotenuse and one side, or c and b. To solve this case trigonometrically, we must first find an angle. To find A. We have cos A = - a. We have, by the precding case, To find a. We have, by the preceding case, (197) a sin A -- c a = c sin A (198) But a may be found by geometry from the equation a2 + 2 = c2 whence a2 = c2 - b2 a =./ (c2 - 62) = v [(c + b) (c - b)] EXAMPLES. 1. Given c = 672.3412, b = 548.9018; find A and a. By (197) By (198) b = 548.9018 log 2.7394946 c = 672.3412 log 2.8275897 log 2.8 A = 35~ 16'25" log cos 9.9119049 log sin 9.7 (199);275897 '615382 a 388.2647 log 2.5891279 * Ten is rejected from each of these indices because the logarithms of the sine and cosine in the table are ten too great. Art. 97 SOLUTION OF PLANE RIGHT TRIANGLES. By (199) = 672.3412 b = 548.9018 + b = 1221.2430 log 3.0868021 c - = 123.4394 log 2.0914538 2)5.1782559 a = 388.2647 log 2.5891279 Ans. A - 35~16'25" B = 54~ 43'35" a - 388.2647 2 Given c =.092357, b =.058018; find a. Ans. a =.071859 109. CASE III. Given an angle and its adjacent side, or A and b. To find a. We have tan A = - whence a = b tan A. (200, To find c. We have 6 b cos A = - whence, by (2), c = -- 5 sec A (201) or directly from the secant sec A - -- whence c = b sec A EXAMPLES. 1. Given A = 88~ 59', b = 2.234875 find the other parts. Ans. a = 125.9365 c = 125.9563 B = 1~ 1' 2. Given B = 60~, a =10; find c. (See Art. 29). Ans. c = 20. 110. CASE IV. Given an angle and its opposite side, or A and a. To find c. We have a a sin A =- ac = = a cosec A (202) c sin A To find b. We have a a tan A = - b = = a cot A (203) b tan 54 PLANE TRIGONOMETRY. EXAMPLES. 1. Given A = 25~ 18'48", a =.085623; find b. Ans. b =.1810278 2. Given B = 39 17'5", b =.01; find c. Ans. c =.0157934 111. CASE V. Given the two sides, or a and b. To find A and B. We have tanA = cotB = -- (204) To find c. We have sinA =- = a a cosec A (205) <c sin A We may also find c directly by geometry, from C2 = a2 + b2 whence < = V/ (a2 + b2) but this is not readily computed by logarithms. EXAMPLES. 1. Given a = 30, 6 = 40; find c. Ans. c = 50 2. Given a = 8.678912, b = 2.463878; find A and c. Ans. A = 740 9' 4".1 c = 9.021875 ADDITIONAL FORMULA FOR RIGHT TRIANGLES. 112. By inspecting the tables it will be seen that when the angles are very small, the cosines differ very little from each other; consequently a small angle cannot be found with very great accuracy from its cosine. For a similar reason an angle that is nearly 90~ cannot be accurately computed from its sine. It is therefore desirable, when a required angle is small, to find it by its sine, and when near 90~ by its cosine, or in either case by its tangent or cotangent; and for this purpose special formulae are sometimes necessary. We shall deduce several such formulae, from which one adapted to a particular case may be selected. 113. From (197) we find, by (139) b c- b 1- cos A = 2 sinO 4 A = 1 -- c c sin A = c ) (206) which may be used instead of (197), when A is small, that is when b is nearly equal to c. It gives also c -b 2 c sin i A (207' vy which c - b may be accurately found when A is small ADDITIONAL FORMULAE FOR RIGHT TRIANGLES. Also from (197), by (140) 1 - cos A\ \ - ( b\ - Q tan A = (j +coA) = J c- ) =. (208) 114. From the equation a sin A - c we deduce by (153) and (154) sin (450 f ~ A) = J ( a) (209) cos (45~ A) = J ( ) (210) tan (450~ A) _ ( (211) a and from tan A = - we find by (151), b ~ a tan (450 ~t A) = (212) 115. By (136) we have bV as cos 2 A -- cos A - sin' A = which, since 2 A = A + 90~ - B = 90~ - (B - A), gives sin (B- A) ( + a) ((213) By (135) 2ab cos (B - A) = sin 2 A = 2 sin A cosA = 2- (214) and from (213) and (214) tan (B- A) - (b + ) ( a) (215) by which B - A is found with great accuracy when b and a are nearly equal EXAMPLE. Given c = 4602-836, b = 4602-21059 to find A. By (206). c- b = 0-62541 log 9-7961648 2 c = 9205-672 log 3-9640555 2)5-8321093 i A = 28' 20".18 log sin ~ A = 7-9160547 A = 56' 40"'36 The ordinary process gives log cos A = 9 9999410, whence A - 56' 40". These results are obtained by Stanley's Tables, in which the log. sines, &c., are given for every 10" for the first 15~. A greater discrepancy between the two results would be found by tables in which the functions were given only for each minute. A slight error remains in the value of i A - 28' 20"-18, on account of the large differences of the log. sines in this part of the table, or rather on account of the 5 I PLANE TRIGONOMETRY. rapid change of these dciferences. We avoid the use of these large differences, and gain somewhat in accuracy, by employing the approximate value of sin. i A given by (98), whence si - A = i A sin 1", Thus we have found above y A = 1700"-12 = 28' 20"-12 sin J A sin 1" log sin 4 A = 7-9160547 Art. 54, log sin 1" = 4-6855749 log i A = 8-204798 But to obtain ~ A with the utmost precision, recourse must be had to the following process, which is constantly employed in observatories, and wherever small angles are to be computed with extreme accuracy. Special tables are prepared containing for every minute from 0~ to 2~ the logarithms of sin x tan x h and - k x x which do not vary rapidly, and may therefore be taken with accuracy from the tables. Then we have sin x sin x x — x. x. h x tan x tan x = x. - = x.. x sin x ht tan x x = k A table of this kind will be found on page 156 of Stanley's Tables, where the notation used is q - log sin x, n = log x sin x and therefore in the column marked q —n we find the log —. Thus in the above x example we have found and from the table 4 A = 1700"-14 - 28' 20".14 log sin i A = q = 7-9160547 — n = 4-6855700 log i A = n - 382304847 which is the true value of i A within 0"01. Stanley's Table contains also the values of tall x log- = q - n (q = log tan x, n =log x) x log i — = q n sin X log - = q +- n tan x (q = log cosec x, n = log x) ( =log cot log cot, log x) the use of which may easily be inferred from the example just given. FORMULAE FOR OBLIQUE TRIANGLES 57 CHAPTER VII. FORMULAE FOR THE SOLUTION OF PLANE OBLIQUE TRIANGLES 116. As every oblique triangle may be resolved into two right triangles by a perpendicular from one of the angles upon the opposite side, we are enabled to deduce all the formulae for their solution from those of the preceding chapter. 117. The sides of a plane triangle are proportional to the sines of their opposite angles. Denote the angles of the triangle AB C, Fig.16. Fig. 16, by A, B and C, and the sides oppo- b site these angles respectively by a, b and c. From C draw CP perp. to AB and put A p B COP = p. Then in the right triangles A CP, B aP, we have, by (195) p = b sin A, p =a sin B whence b sin A = a sin B which, converted into a proportion, gives a: b = sin A: sin B (216) and in the same way we may prove that a: c = sin A: sin 0: c = sin B: sin 0 and these three proportions may be written as one, thus: a: b: =sin A: sin B: sin C (217) a b ~ or thus, (218) sin A sin B sin ( When the perpendicular falls without the Fig.17. triangle, Fig. 17, the angle CB P is the supplement of B, but by Art. 39, it has the same / i sina, so that the triangle CB P gives A - p = a sin OBP = a sin B 8 r58 PLANE TRIGONOMETRY. the same as was found from Fig. 16. The proposition is therefore general in its application.* 118. The sum of any two sides of a plane triangle is to their difference as the tangent of half the sum of the opposite angles is to the tangent of half their difference. For, by the preceding article, a: b = sin A: sin B whence, by composition and division, a + b: a - b = sin A + sin B: sin A - sin B But from (109) if x = A, y = B we obtain the proportion sin A + sin B: sin A - sin B = tan 1 (A + B): tan - (A - B) which, compared with the above, gives a + b: a- b = tan (A + B): tan I (A - B) (219) This may also be written a + b _ tan I (A + B) a- b tan 1 (A - B) (220) and we may infer the same relation between 6, c, B, C and a, c, A, C. 119. The square of any side of a triangle is equal to the sum of the squares of the other two sides diminished by twice the rectangle of these sides multiplied by the cosine of their included angle. Fig. 16. In the triangle AB C, Figs. 16 and 17,* we have either A B BP=c-AP orBP=AP-c P B Fig. 17. but in both cases C. BP2= AP2 +c2-2c xAP d B/Z p Adding CP2 to both members, we find B a2 = b2 + c2- 2c X AP But the triangle A CP gives by (196) AP = b cos A * The consideration of Fig. 17 was not strictly necessary according to the principle stated in Art. 49. It may, however, be useful for the student to verify that principle when convenient. FORMULAE FOR OBLIQUE TRIANGLES. 59 which substituted in the preceding equation gives a2 - b2 + c2 -2 be cos A (221) as was to be proved. We have in the same way b2 a2 + c2 2ac cos B (222) 2= a2 + b2 2 ab cos CG (223) 120. The same result is obtained from the following equations (which are evident from Fig. 16, where c = A P + PB) a = b cos C + c cos B b - c cos A + a cos C (224) c = a cos B + b cos A From the first of these c cos B = a - 6 cos C whence ce cos' B = a — 2 ab cos C + 6' cos7 C' and from (218), c' sin' B = b6 sin' C the sum of which two equations is, by (13), c' = a' - 2 ab cos C + 6 -121. From (221) we find b2 + C2 _ a2 cos A - 2 be (225) by which an angle is found when the three sides are given; but to adapt it for convenient computation by logarithms, the following transformations are necessary: Subtract both members from unity; then 2 be - b2- C a2 a a2- (b -) I - cos A.. -- --- 1-cosA =2 be 2 be But, by (139), making x = A, we have 1 - cos A 2 sin2 ~ A Also, the numerator of the second member being the difference of two squares may be resolved into two factors, viz.: the sum and the difference of a and b - c; thus,,, -(b )2= a - ( - c)] x [a+ (-c)] = (a- b+ c)(a+ b- c) Substituting these values in the above equation and dividing by 2 sin2 W A. = (a - + ) (a+ -) (22 si 4n A =(226) 4 be 60 PLANE TRIGONOMETRY. This may be simplified by representing the half sum of the three sides by s, or by putting a + b + c-2 s a+6+c —2s whence a - + c = a +b + c - 2b = 2s-2b= 2 ( - b) a + b- c = a + b + c - 2 c = 2s-2 c = 2(- c) which substituted in (226) give sin2A ( - ) (8- ) (227) -- be In the same manner we should find from (222) and (223) sin2 J B (s a) (s c) in2 = a) (8-6) (228) 122. Add both members of (225) to unity; then 2 be + b2 + c2 - a2 (b + c)2-a 1 + cos A = 2 bc 2 bc 2 be 2 be But by (138) 1 + cosA = 2 cos2 A Also, (b+ C)2- a2 = (b+ c a)+ + - a) therefore cos2 - A - (b + c + a) (b + c - a) 2cos tA- 4 be Substituting 8 in the numerator as in the preceding article Cos 2 = (s - a) (229) cos2 A 8- (229) and therefore also cos2 B, co2 - a C (230) ac 2 ab 123. Dividing (227) by (229), we have, by (14) tan2 1A A = (231) 2 8(s - a) and in the same manner tan B = ( - a) (s - c) tan2 -a) (- 232) s (8 - 6 2 8- (s - c) FORMULAE FOR OBLIQUE TRIANGLES. 61 124. The preceding formulT. are sufficient for the resolution of all the usual cases of plane triangles; but there are others that are occasionally useful. From (218) we find, by (105), (106) and (135), a + b sin A si B sin (A B) cos (A - B) c sin C sin -2 C cos - C a-b sin A - sin B cos (A + B) sin (A - ) c sin C sin I C cos I C But since A + B + C = 180~, A + B == 1800 - C, (A + Bz) = 900 - C sin I (A + B) = cos j C, cos I (A + B) = sin C by means of which we find a + b cos g (A - B) _ cos (A - B) (233) c sin - C cos A (A + B) a-b sin, (A- B) sin ( (A - )( (234) c - - cos ~ C = sin ~ (A + B) The quotient of (233) divided by (234) gives (220). 125. Adding unity to both. members of (233), or subtracting it, we have, oy (103) and (104) a + b+ c cos ~ (A + B) + cos ~ (A - B) 2 cos I A cos ~ B c cos ~ (A - B) sin 7 C a + b-c _ cos (A - B) - cos A (A + B) _ 2 sin A sin ~ B c cos Yf (A - B) sin ( C Similarly from (234) we find c + a-b sin (A +B) + sin (A - B) 2sin A cos B c sin A (A + B) cos C c- a -b sin (A + B) - sin (A - B) 2 cos 2 A sin B c sin (A + B) cos C Substituting s =- (a + b + c), these equations become s cos A cos ( B25 7 Y == — smi - (285) C sin ~ C s - = sin A sin B (23) a sin j C 6 s- b sin A cos ^ B (2 ---— ss_ --- ---._ (237) c cos j C -a cos A sin B (28 Y cos 2 - (2as c cos ~- C F 62 PLANE TRIGONOMETRY. From these equations we can deduce immediately (227) &c.; for example exchanging c for b in (236), we have s- b sin A sin C b sin i B which, multiplied by (236) gives (227). 126. Four times the product of (227) and (229) is by (135) 4 sin A = 8 (8 - a) (8 - b) (8 - c) whence 2 sin A = --- /[s ( - a) ( —b) (-c)] (239) Exchanging A for B and C successively, this gives also 2 sin B -- / [s (s - a) (s -b) (s - c)] (240) ac sin C (7 - a) ( - b) (s - c)] (241) In these equations put* K-= - / [8 ( - a~) (s - b) (a - c)] (242) then sin A = - sin B - sin C= 2 (243) be ac ab The quotient of the first of these divided by the second is sin A ac a sin B be b which brings us back to the theorem of Art. 117. 127. The sum of A, B and C being 180~, and the sum of; A, i B and ~ C being 90~, we have, by Arts. 85 and 86, the following relations among the angles of a A.. triangle. tan A + tan B + tan C= tan A tan B tan C cot ~ A + cot i B 4 cot i C = cot ~ A cot i B cot j C sinA + sinB - sinC= 4cos A cos Bcos C sinA - sin B- sin C= 4 sin A sinjBcos (C cos A - cos B + cos C- 1 - 4 sin i A sin i B sin 6 C cos A + cos B - cos C-+ 1 = 4 cos i A cos i B sin i C m the last of which we may interchange A, B and C. These relations may be substituted in the equations of Art. 125. * K is the area of the triangle. See Art. 148. FORMULAE FOR OBLIQUE TRIANGLES. 128 The following equations are added as exercises. tan ~ A s - b — B - tan A tan tan = B -- tan -j- s -— a s sin (A - B) (a + b) (a - b) sin (A + B) c tan j A tan j B cot ~ C0 ( ) cot ~ A + -ot B + cot C7= f K' sin ~ A n i B sin C Kb a6cs abccos 2 1 cos - B cos -= a-b — a 1 (2 a' + 2 at4+ 2 b cd 1- a- -d) 68 "4 PLANE TRIGONOMETRY. CHAPTER VIII. SOLUTION OF PLANE OBLIQUE TRIANGLES. Fig. 18. C A/ ~ B 129. CASE I. Given two angles and one side, or A, B and a. Fig. 18. To find the third angle. We have C= 1800 -(A + B) Tofind b and c. We apply the theorem of Art. 117, and state the proportions thus: the sine of the angle opposite the given side is to the sine of the angle opposite the required side, as the given side is to the required side. Thus we have sin A: sin B = a: b whence and a sin B b — = -.. = a sin B cosec A sin A sin A: sin C= a: c a sin 61 e = - a =n = a sin C cosec A sin A (244) whence (245) EXAMPLES. 1. Given A = 50~ 38' 52", B = 60~ 7' 25" to find C, b and c. A = 50~ 38' 52" B = 60~ 7'25" C = 69~ 13' 43" a = 412.6708 A + B = 110~ 46' 17" C = 69~ 13' 43" By (244). log cosec 0.1116730 log sin 9.9380702 log 2.6156037 log b 2.6653469 b = 462.7505 and a = 412.6708, By (245). log cosec 0.1116730 log sin 9.9708129 log 2.6156037 log c 2.6980896 a= 498.9875 SOLUTION OF OBLIQUE TRIANGLES. 65 2. Given A = 100~ 16' 35", B = 25~ 16' 13", and b = 29.167 find a and c. Ans. a = 67.22857 c - 55.59178 130. CASE I. Given A, B and a. Second solution. We find C = 180~ - (A + B); then, by (233) and (234) +os (B - C) cos (B - C)(2 cos (Bq- C) - sin A24) sin (B- C) sin ~ (B - ) b-c = a. in(B+- C) a. cos ~ (247) sin (B + C) cos j A which give the sum and difference of the required sides; adding half the difference to half the sum, we find the greater side, and subtracting half the difference from half the sum, we find the less side. 131. CASE I. Given A, B and a. Third Soluti6n. When A and B are nearly equal, and great accuracy is desired, we may compute the difference between a and b; for we have, from (244), a sin B sin A - sin B a -b = a- a, sin A sin A or a - b 2 a cos I (A + B; sin ) i (A - B) sin A EXAMPLE. Given A - 35~ 40' 12"-3, B = 35~ 37' 48"-6, and a = 26246-948. A = 35~ 40' 12"-3 log cosec 0-2342442 0-23424 B = 35~ 37' 48".6 log 2 0-3010300 0'30103 i (A + B) = 35~ 39' 0"-5 log cos 9-9098720 9-90987 i (A - B) 0~ 1' 11"-9 log sin 6-5423038 6-54230 a = 26246-948 log 4-4190788 4-41908 a- b 25-499 log 1-4065288 1 40652 b = 26221-449 One of the advantages of this process is, that a - b may be found with sufficient accuracy with five-figure tables, as in the second column of logarithms above. If a had been given to ten figures instead of eight, we should still have been able with the seven-figure logs. to find a - b to seven figures, and therefore b to ten figures, which could not be done by the ordinary methods without ten-figure tables. 132. CASE II. Given two sides and an angle opposite one of them, or a, b and A. To find B. To find the angle opposite the other given side, we apply Art. 117, and state the proportion thus: the side opposite the given angle is to the side opposite the required angle as the sine of the given angle is to the sine of the required angle. Thus, with the present data, we have a: b = sin A: sin B whence sin =- s (249 9 r2 66 PLANE TRIGONOMETRY. To find C. We have C= 180~ - (A + B) To find c. Having found C, we now have the data of Case I. therefore, by (245) c = a sin C cosec A (250) 133. It is shown in geometry that when two Fig. 19. sides and an angle opposite one of them are given, there may be constructed two triangles, as in Fig. 19, whenever the given angle is... B/'. acute and the given side opposite to it is less than the other given side. In one of them, the required angle B is acute, and in the other it is obtuse, and the two values are supplements of each other; for B = BB'C= 180~ - AB' These two values of B are given in the trigonometric solution by.he consideration that sin B found by (249) is at once the sine of an acute angle, and the sine of its supplement, Art. 39. In general, when an angle is determined Fig. 20. only by its sine, it admits of two values, supple- /9 ments of each other, unless the conditions of the problem are such as to exclude one of these values. In the present case, the obtuse value of B is excluded when a is greater than b, and c. there is but one triangle whether A is acute or obtuse, as in Fig. 20. A /B 134. If the given parts were such that a = b sin A a would be equal to the perpendicular from C upon the side c, and we should have but one solution, namely, a right triangle, B and its supplement both being 90~. 135. If the given parts were such that a < b sin A a would be less than the perpendicular from C and the problem would be impossible. It would also be impossible if a < b while A > 90~. 136. When there are two solutions, represent the two values of B by B' and B", then the two values of C will be C' = 180 - (A + B') = 180 - B' - A = B" - A (251) G"= -1800 - (A + ~'B = 1800 - B"- A = B' - A (252) SOLUTION OF OBLIQUE TRIANGLES. 67 and the two values of c will be e'= a sin C' cosec A =" = a sin C" cosec A (253) EXAMPLES. 1. Given a = 31.23879, 6 = 49.00117 and A = 32~ 18'; find B, 0 and c. a = 31.23879 b = 49.00117 A= 32 18' B' - 560 56' 56".3 B" - 123~ 3' 3".7 ' '= 90~45' 3".7 Cf -= 240 38'56".3 ar. co. log 8.5053058 log 1.6902064 log sin 9.7278277 log sin 9.9233399 log sin 9.9999627 log cosec A 0.2721723 log a 1.4946942 log c' 1.7668292 c' = 58.45601 Ans. B =56~ 56'56"-3 C= 90~ 45' 3"/7 or c = 58-45601 J log sin 9.6201962 0.2721723 1.4946942 log c" 1.3870627 c"= 24.38163 B = 1230 3' 3"7 C = 240 38' 56"'3 e = 24'38163 2. Given a =.051234, b =.042356, A = 55; find B, C and c. Ans. B = 42~ 37' 32".7 C= 820 22'27".3 =.06199202 3. Given a =.042356, b =.051234, A = 55~; find B, C and c. Ans. B = 82~ 14' 35"'7 B = 97~ 45' 24"'3 ( = 42~ 45' 24" 3 or C = 27~ 14' 35"-7 C = '03510331 J c = 02366993 4. Given a = 40, b = 50, A =53~ 7' 48".4; find B. Ans. B = 900. 5. Given a = 40, b = 50, A = 60; solve the triangle. Ans. Impossible. 6. Given b = 40, c = 50, B = 100~; solve the triangle. Ans. Impossible, PLANE TRI GONOMETRY. Vig 21. 137. CASE II. Given a, b and A. Second Solution. We may solve, separately, the two right triangles A P C, BPC, Fig. 21, which is a convenient method when there are A B two solutions. We first find B by (249); then we have p AP =-b cosA, BP= a cos B and c=AP~+BP The cosine of the obtuse value of B is negative, (Art. 39), so that BP is then negative, and we have the two values of c from the formula c = A P BP There will be but one solution, if B P> A P, for c cannot be negative. 138. CASE III. Given two sides and the included angle, or a, b and (C, To find A and B. We have first A + B = 180~- C (A + B)=90~ - C from which we next find the half difference of A and B by tne theorem of Art. 118, which gives a + b: a - b = tan I (A + B): tan |- (A - B) a -- a-b _ tani(A-B) b tan 2 (A+B) a+bcot 21 (254) The half difference added to the half sum gives the greater angle, (opposite to the greater given side), and the half difference subtracted from the half sum gives the less angle. To find c. We have the data of Case I., and therefore c a sin C cosec A = b sin C cosec B (255) EXAMPLES. 1. Given a =.062387, b =.023475, and C = 110032'; find A, B and c. A + B = 180~ - C= 69~ 28' a + b=.085862 ar. co. log 1.0661990 a- b =.038912 log 8.5900836 i (A + B) = 34~ 44' log tan 9.8409174 i(A- B) = 17 26' 33" log tan 9.4972000 A= 520 10'33" B = 17~ 17'27" log cosec 0.5269189 C = 110~ 32' log sin 9.9714931 b =.023475 log 8.3706056 c.0739635 log 8.8690176 Ans. A = 52~ 10' 33" B = 17~ 17' 27" c =.0739635 SOLUTION OF OBLIQUE TRIANGLES. 69 2. Given a = 31.0005, b = 15.1101, C = 10~ 15'; find A and B. Ans. A = 160 17'13".7 B = 9~27/46"'3 8. Given a = 2.463878, b = 9.021875 and C = 74~ 9'4".2; find A and B. Ans. A-= 15~ 50'55".8 B = 90~ 0' 0" 4. Given b = 15.1101, c = 31.0005, A = 10~ 15'; find B and C. Ans. B = 9~ 27' 46".3 C = 160~ 17' 13".7 139. Having found A and B as above, the most convenient mode of finding c is by (233) or (234), which give =( + ) cos (A + B) (256) cos j (A - B) sinj (A + B) = (a- b) sin (A+ B) (257) for we have, from the process of finding A and B, the log. of a + b, or of a - b, and the values of i (A + B) and j (A - B), so that we have only two new logs. to find, which are taken out at the same opening of the tables with the tangents of (A + B) and j (A - B). 140. CASE III. Given a, b and C. Second Solution. When a and b are given by their logarithms, which occurs when they are deduced by a logarithmic process from other data (as, for example, in the computation of a series of triangles in a survey), we proceed as follows. Let x be an auxiliary angle, such that a tan x = (258) an assumption always admissible, since a tangent may have any value from 0 tooo. We deduce tan x-1 a-b tan x+ 1 a+b or by (152) tan ( 456) - b Which substituted in (254) gives tan 1 (A - B).= tan (x - 450) tan X{ (A + B) (259) 70 PLANE TRIGONOMETRY. We find x from (258) and employ its value in (259). As this mnethod does not require the preparation of a + b and a - 6, it is luite as short in practice as (254). EXAMPLE. Given log a = 8-7950941, log b = 8-3706056, and C = 110~ 32'. (Same as Ex. 1. Art. 138.) log a = 87950941 log b = 8 3706056 x = 69~ 22' 46"-8 log tan 0-4244885 - 450 = 24~ 22' 46"/8 log tan 9-6562825 A (A + B) = 34~ 44' log tan 9-8409174 X (A - B) = 17~ 26' 32" 9 log tan 9-4971999 141. CASE III. Given a, b, and C. Third Solution. in terms of the data, we have, from (218) and (224) c sin A = a sin C c cosA = b - a cos ' the quotient of which is a sin C tan A -- b- a cos C and in the same manner b sin C tan B = a b- cos C 142. CASE III. Given a, b and C. Fourth Solution. data, we have, by (223) c = a2 + b - 2 ab cos C To express A or B directly (260) (261) To find c directly from the which, however, is not adapted for logarithmic computation. follows. Substitute by (139) cos C = 1 - 2 sin2 j C It may be adaptea as then c= a- + b - 2 ab + 4 ab sin2 C7 = (a - b)' + 4 ab sin2 I C c_ (a —b) (l 4 ab sinS' C' c=(a- 4(l+ _(a- ) Let x be an auxiliary angle, such that 4 ab sin2 j C tan x = (a - b) 2 sin a 7 /a"C or tan a = _i — C /ab a - b (262) (263) SOLUTION OF OBLIQUE TRIANGLES. 71 then the radical in the above equation becomes V/(1 + tan2 x) = sec x; therefore, c = (a- b) sec x (264) 143. We may also adapt (223) for logarithmic computation by means of (138) which gives cos C= - 1 + 2 cos2 I C whence c' = a' + b + 2 ab - 4 ab cos i4 C c _ (a -r b) + ( 1 —abcas C Let 2 cos C - sin z = ---- / ab a + b then the radical becomes / (1- sin" x) = cos x; therefore, c - (a + b) cos x (265) (266) (267) 144. It is to be observed, that the supposition (263) is always possible, since a tangent may have any value between 0 and o, and therefore an angle x may always be found having any given number as its tangent. As the greatest value of a sine is unity, it is not so obvious that the supposition (266) is always possible; but whatever the values of a and b (a - b) > therefore whence (a + b)9> 4 ab 2 ab < 1 a+b <1 a+ b= therefore the second member of (266) is never greater than unity. EXAMPLE. Given a =- 062387, b = -023475, =- 110~ 32'; (same as Ex. 1, Art. 138) a = -062387 b = -023475 a + b =.085862 g C = 55~ 16' By (266) and (267). log 8-7950941 log 8-3706056 2)7-1656997 log ab = 8-5828499 ar. co. log 1-0661990 1. cos 9-7556902 log 2 0-3010300 1. sin x 9-7057691 c = -07396344 log 8-933&010 1. cos x 9-9352161 log 8-8690171 72 PLANE TRIGONOMIETRY. 145. CASE IV. -xiven the three sides, or a, b and c. To find A, B and C. We have from (227) and (228), sinrA J ((- b)(Cs-)) sinMB=(-) -c) (268) sin C J((s-a) (s -b)) ab cr by (229) and (230) cosA-J (s(s a) b ) Cos B = J (s (- b). (269) cos C = J (s C)t ur by (231) and (232) tan A _J (sb ) * l tan B === 2 ( (s —) (270) s (s - b) tan2 S (s a) (s 2 s (s - C) In these formulae s = ~ (a + b + c). Either of these three methods may, in general, be employed, but (268) is to be preferred when the half angle is less than 45~, and (269) when the half angle is more than 450.* When all the angles are required, (270) will be the simplest, as it requires but four different logs. to be taken from the tables. It is accurate for all values of the angle. * See Art. 112. SOLUTION OF OBLIQUE TRIANGLES. 73 EXAMPLES. 1. Given a = 10, b = 12, c = 14; find the angles. By (268). arcol 9.0000000 a -10 b-=12 =-14 2 s= 36 s =18 # —a- 8 ar col 9,0000000 ar co 1 8.9208188 arcol 8.9208188 ar co 1 8.8538720 ar co 1 8.8538720 log 0.9030900 log 0.9030900 8 - = 6 log 0.7781513 log 0.778151T s -- = 4 log 0.6020600 log 0.6020600 2)9.1549021 2)9.3590220 2)9.6020601 log sines 1A 9.5774510 ~ B 9.6795110 I C 9.801030G ~ A = 22~ 12' 27".6 1 B - 280 33'39".0 ~ C=39013'53".5 A = 440 24' 55"2 B = 57~ 7'18".0 C= 78~ 27'47".0 Verification. A + B + C== 180~ 2. Given a =.8706, b = -0916, c =.7902; find the angles. Ans. A = 149~ 49' 0".4 B = 3~ 1'56".2 C= 27~ 9' 3".4 3. Given a =.5123864, b =.3538971, c =.3090507; find C. Ans. C = 36018'10".2 146. The computation by (270), when all the angles are required, will be much facilitated by the introduction of an auxiliary quantity* J((s a)(-)(s-c)) (271) from which we ind by (270) tan A s= a' s - a tan I B = --- tan j C (272 8 - C * This quantity r is the radius of the inscribed circle. See (289) G 74 PLANE TRIGONOMETRY. EXAMPLr. Given a = 6053, b = 4082, c - 7068. We find s = 8601-5 ar. co. log 6-0654258 - a = 2548-5 log 3-4062846 s - b = 4519-5 log 3-6550904 s- c = 1533 5 log 3-1856838 2)6-3124846 logr = 3.1562423 i A - 29~ 20' 54"*47 7 log tan j A = logs - a = 9-7499577 i B - 17~ 35' 31"*70 log tan log tan } B = log - - = 9'5011519 -* 6 i C - 43~ 3'33"'*8 verification. 90~ 0' 0" OC Fig. 22. 3 ) 7 log tan I C = log s - c = 9-9705585 147. The case where the three sides are given is some a times solved as follows. From C, Fig. 22, draw perp. to c. Then A ji B A a =- A P A+ CP2, BC2 = BP~+ -CPA the difference of which is A C2 - BC2 = AP - BP2 or (A+ B C) (A C-BC) = (A~P+ BP) (AP - BP) and if A P- B P = d, this equation gives Cr d _ (b + a) (b - a) Then since AP+ B c and A we have Then, since A P q- 27 P - c, and A P - B P = d, we have (2'1) AP= I (c+ d), and in the right triangles A CP, B C P AP cos A = - 6 BP= c ( - d) BP cos B -- a (274) (275) so that (273), (274) and (275) solve the problem. When d> c, B.P is negative, cos B is negative, and B is an obtuse angle, (Art. 39). AREA OF A PLANE TRIANGLE. 148. Representing the area by K, and the perpendicular CP, Fig. 22, byp, we have, by geometry, K = p In the triangle A CP, we have p = b sin A, whence K= 6bc sin A - be sin I A cos 1 A by which the area is computed from two sides and the included angle. Substituting in (277) the values of sin IA and cos ~ A by (268) and (269), = [ (. ( ac) (s- ) (s c)] by which the area is computed from the three sides. (276) (277) (278) PROBLEMS RELATING TO PLANE TRIANGIES CHAPTER IX. MISCELLANEOUS PROBLEMS RELATING TO PLANE TRIANGLES. 149. In a given plane triangle, to find the perpendicular from one of the angles upo0 the opposite side. Letp be the perpendicular from C upon c. We have p bsinA (279 or by (239) and (278), 2 2K p 2= s[ (s - a) (s- - b) (s - c)] (280) C C the expression for p in terms of the three sides, where s i ~ (+ b+ - c) and K is the area of the triangle. If we substitute in (279) sin A = - sin C, it becomes ab p =- sin C (281) C sin B sin A sin B sin A sin B (2 sin C sin (A t- B) When the triangle is right-angled at C, (282) becomes C p =c sin A cos A - sin 2 A the expression for the perpendicular upon the hypotenuse. 150. If p', p", p"', denote the perpendiculars upon the sides a, b, e respectively, we have from (280) 1 1 1 a+ b+ c s +7+P 2K K= (288) 76 PLANE TRIGONOMETRY. 151 To find the radius of the circle circumscribed about a plane triangle. Pig. 23. The center 0 of the circle, Fig. 23, lies in the perpen uc~ - dicular erected from the middle point of one of the sides/ as A B. Let the radius == R. We have, by geometry, AOD -= AOB = C 0/ \ 1 sTdand in the triangle A 0 D, B B AD c sin AOD sinC-AO whence R 2 sin (284) Substituting the value of sin C from (241), abc abce 4\/[s (s-a) (s -b) (s - c)] 47 (285) From (229) and (230), we easily find cos I A cos I B cos f C=abc which combined with (285) gives 4 cos ~ A cos ~ B cos G (286) 152. To find the radius of the circle inscribed in a plane triangle. Fig. 24. The required center 0, Fig. 24, is in the ina /^~ D ^tersection of the three lines bisecting the angles, BE s_'^\/\^ ~and each of the perpendiculars OD, 0 E, OF, is equal to the required radius = r. The value of o/a I -t O F in terms of AB = c, OAB = ~ A, -od A V F< B|2^ O A = A - B is by (282) sin I Asin I B sin A sin (28) 7 C. Bsin.(A+- B) =- cos ' C( This is reduced by means of (236) to r = (s - c) tan I C (288) Substituting the valae of tan I C, r ((s-a)(s —b) (s-c)) (289) This is reduced by means of (231) and (232) to r = s tan I A tan I B tan I C (290J PROBLEMS RELATING TO PLANE TRIANGLES. 77 153. Besides the inscribed circle, strictly so called, there are three other circles that touch the three sides, (or sides produced), and are exterior to the triangle, as in Fig. 25, These have been named escribed circles. Their centers are found Fig. 25. geometrically, by bisecting the exterior angles B C C', CBB', &c. Designate the centers of the circles lying within the angles A, B, and C respectively, by 0', 0", and 0"', and their radii by r', r", r'". We find the perpendiculars from 0', &o., upon B C, &c by (282) to be cosBs s B c o s B- c os cos r sin - (B + C) cos A r" b. cos I A cs s C b c os A cos sin (A + C) cos j B cos - A cos ~ B cos ~ A cos 1B r C.-. --- sin - (A + B) cos c C7 By means of (235) we reduce those.values to r' - s tan - A, r" -= s tan ~ B, r'" = s tan ~ C Substituting the values of tan ~ A, &c. / f s.-b) (s -- c)) R \ s --- a s -a s —,) s-b~-,, s (s - ) (s-c) K s - 4 (-C c - 2 91 (291) (2921 I 1 78 PLANE TRIGONOMETRY. Also, by means of (236) applied successively to a, b and c, we may reduce (291) to the following: r' = (s - a) tan 4 A cot 4 B cot i C r = (8 - b) cot A tan 4 B cot C (\294) r'" = (s - c) cot A cot~ B tan C J 154. Relations between the radii of the circumscribed, inscribed, and three escribed circles of the preceding article, and the three perpendiculars from the angles upon the opposite sides. The four equations of (289) and (293) give K' K' r r' -' r"' (295~ r ',I I - s (s-a) (s-b) (s -c) =K (295, Dividing this successively by re, r', &c. r' "' r"' r r" 'r" s r' = (s -a)' r =(,-b),,, l (s c)( rr, j Again, we have, (Art. 127), tan I A tan I B + tan A tan C+ tan B tan C = 1 and substituting in this the value of the tangents from (292) r' r" r'i r ' ' + rl'"' + r" r"' = s= - 1 1 1 1 I' + (297) From (292) we find tan IA Tr' tan4B r r" tan A r' tan B tan ~ j -- r" from which it follows that in Fig. 25, the distances A D and B D', are equal (D, D' being the points of contact of the circles 0', O" with A B produced), and therefore B D = A D'. Other curious geometrical properties may be traced with the aid of our equations. From (284), a 65 c 4 sin Acos A 4 sin B cosB - 4sin C cos j which combined with (287) and (291) give, by Art. 127, R- =4 sin ~ Asin ~ B sin = cos A + cos - + cos C- 1 R - 4 sin ~ A cos J B cos C = - cos A + cos B + cos C+ 1 TI^ -#~~~~~~~~~~~' ~(298) - ==4 cos A A sin j B cos C = cos A - cos B + cos C+ 1 - = 4 cos ~ A cos ~ B sin; C = cosA + cos B - cos C+ 1 PROBLEMS RELATING TO PLANE TRIANGLES. 79 Changing the signs of the first of these equations, the sum of the four is r' + r" + r"' — r * += 4 R -- 4 R = i (r' + r" + r" - r) (299) Finally, if p', p", p"' denote the three perpendiculars from the angles upon the 6ides a, b, c respectively we have by (283), (289) and (297) the following relation: 1 1 1 1 1 i 1 1(299) -1~4 i+ -+ -- (299+) 155. To find the distance between the centers of the circumscribed and inscribed circles.* Let P, Fig. 26, be the center of the circumscribed, Fig. 26. and 0, that of the inscribed circle. Put P 0 - D. By Arts 151 and 152, PAB =90~- C, OAB-?A / whence PA O = 90~- C- A = i (B- C) and by (221) B P 0 = PA2 + OA- 2 PA. OA cos PAO ro 2 Rrcos (B - C) or D ~ -=.R ' sin -- sin] i A sin ~ A B 298_ 4 Rr sin - B sin C By (298)A si sin' ~ A - sin I A 2 Rrcos (B+ C) therefore Da R - 2Rcos C sin I A or D2 R= 2 - 2 Rr (300) 156. Let P ' = D', Fig. 26, 0' being the center of the escribed circle lying within the angle A. If r' = radius of this circle, we have, as in the preceding rticle r" 2 RT' cos (B- C) Dfg =- R + sin2 - A sin j A r_ 44 Rr' cos i B cos i C sin2 ~ A sin I A D'2 Rg + 2 Rr' D"n = iR + 2 Rr" (1 D'"' = RB + 2 Rr"' * Hymers' Trig. Appendix, Art. 58. 80 PLANE TRIGONOMETRY. the expressions for the distances of the centers of the three escribed circles from that of the circumscribed circle. The sum of (300) and (301) gives by (299) D - + D/' +4 D", —. +..2 = 12 R3 (302) 157. Given two sides of a plane triangle and the difference of their opposite angles, (or a, b, and A - B), to solve the triangle. We have ~ (A + B) directly from (220), which also solves the case where two angles and the sum or difference of two sides are given. 158. Given the angles and the sum of the sides, (or A, B, C, ard a +- b + c = 2 s). By (235) sin I C c == s. cos A. cos - B ind a and b are found by similar formule. 159. Given one angle, the opposite side, and thv sum of the squares of the other two aides, (or C, c, and a2 +- b = e). In the identical equations (a + b)2 -- e + 2 ab, (a - b)' e' - 2 ab substitute the value of 2 ab given by (223), namely, 2 ab -c cos C we find (a + b) = e + Cos C' (a- 6) = e2- ' / ' cosG 0' ' } cos C which determine a - b, and a - b, and therefore a and b. To compute these equations by logarithms, let e - s ( (e - c) 92 cos C cos C (303) then (a b)2 - e- +- g', (a -b)' = es - g= that is a + b is the hypotenuse of a right triangle whose sides are e and g; and a - b is one side of a right triangle whose other side is g, and whose hypotenuse is e. Let the angle opposite g be denoted by x in the first triangle and by x' in the second, then by the formulae of right triangles tan x = a+ b e see x (304) sin x' - a - e cosx' e so that the problem is solved by logarithms by finding log g from (303) and employing its value in (304). The above may serve as an example of a geometrical method of introducing the auxiliary quantities, which is occasionally useful. The analytical process in the present instance is similar to that of Art. 143; thus a + b = (l +)- c-b e f(1- — ) PROBLEMS RELATING TO PLANE TRIANGLES. 81 therefore if tan x g we have J (1 - = sec x and if sin x' = we ave J(-cos ' whence the same formulae as before. 160. Given an angle, its opposite side, and the difference of the squares of the other two sides, (or C, c, and at - b = fAs). We have by multiplying (233) by (234) sin (A - B) _ as- b f sin C - cs sin (A - B) - sin C whence A - B, and since A + B - 180~ - C, the angles are determined. There will be two solutions given by sin (A - B) except where the obtuse value of A - / is greater than A + B. 161. Given the three perpendiculars from the three angles upon the opposite sides. Denote the perps. upon a, b and c respectively by a', b' and c, and let 1 1, 1 a" b" --- — C a' b6' c' Tf k = 2 area of the triangle aa' - bb' = cc' = k and therefore a a" k, b = b" I, c C c"k Substituting these values of a, b and c in (225), (227,) &c. c "6 i- c"" — a" i (s" - b") (s" —c") cos A = --- sin = -&c. 2 bc" ' s i A -- -- ", &c. in which 2 s" - a" + b6" c". 162. Given the radii of the circumscribed and inscribed circles, and the perpendicedar from one of the angles upon the opposite side, to solve the triangle. Let c be the side to which the perpendicular (p) is drawn. We have found for R, r and p the expressions c c c: 2 sin GC 2 sin (A + B) -4 sin ~ (A + B) cos i (A + B) sin A sin ~ B sin (A-+ B) sin A sin B p- C sin (A- B) 11 82 Eliminating c we have PLANE TRIGONOMETRY. 2 — =-. sin A sin /' 2R ( R- = 4 cos I (A - B) sin' A-4 sin JB (m) (n) from which two equations A and B are to be found. Developing cos j (A + B), (n) becomes r - = — 4 sin A cos - A sin B cos B- 4 sins I Asin' B = sin A sin B - 4 sin2 i A sin2 4 B which subtracted fron (m) gives p-2r = 4 sins - A sing ~ B 2R Dividing the square of (m) by (o), we find p?I 4 =4cos' A cos B 2R (p- 2r) 2 whence sin A sin = B J (- - [2 cos A cos 4B = 2 V/ [2 R (p - 2 r)] The difference and sum of these two equations give (o) cos 4 (A + B)-= v [2 R(p-2r)] cos ~ (A + - ) p V, [2 R (p- 2 r)] p-r os (A - B) = [2 R (p - 2 r)] which determine 4 (A + B) and 4 (A - B) and therefore A and B. are then found by the formula c = 2 R sin C I (305) The sides Fig. 27. a A -- B 163. In a given plane triangle A B C, Fig. 27, to find as point 12 wuch that the three lines drdwn from this point to the angles A, B and C shall make gfven angles with each other. Let the given angles be P P C =- and A P 0 = and the required angles PA C = x PB C = y The sum of the angles of the quadrilateral A CB Pis x + y 4- ac- + + = 860~ whence I (x + y) = 180~ -, ( - + t+ C) (306) PROBLEMS RELATING TO PLANE TRIANGLES. 83 In the triangles A P C, B P C, we have b sin x a sin y sin x a sin. ~P a=. in - sin f si in sin y 6' sin from which sin x + sin y tan (x - y) m 1 sin x - sin y tan (x - y) m- 1 tan (x - y) - tan i (x + y) r+1 To compute this equation by logarithms, let a sin tan m = asin b sin ar (307' then by (152), tan ~ (x - y) = tan ( - 45~) tan I (x + y) Bo that the angles x and y are found by (306) and (307). 164. The following problems are proposed as exercises. In a plane triangle A B C - 1. Given c, the perp. upon c = p and a +- = m. 4?) sin2 x = 4,- - a -b =- c cos z (m + c) (m - c) tan I= 2 pc (r + c) ( - c) 2. Given c, the perp. upon c = p, and a - b = n. 4 p2 tan2 a =x + n) a+ b =csec (c + -) (c - n) tan - i = (c + n) (c -n) 2 pc 8 Given C, c, and ab _ q. 2q tanx - cos C a + b- c sec c sin x' = sin C a- = ccosx' 4. Given C, the perp. from C = p, and a + b = m. tan x - - tan C c = m tan I x p f. Given C, the perp. from C- =p, and a - b = n. tan x - -cot I C c = ncot p 6, Given c, C, and a + 6 = m. COs si-B) (A-i- BCo ) cos ~ (A - B) 1sin C a - b = C ~~~~c cos j C 84 PLANE TRIGONOMETRY. 7. Given c, A, and a + b = m. tan B - - cot A m+ c 8. Given a + 6 b= m, the perp. upon c - p, and the difference of the segments of c d. c = m! (i- m P ) tan (A + B) J [(r d_ ( m P d-4 )] tan (A - B) m2-d or with an auxiliary angle 4? sin x = - c= m cos x (m + d) (m - d) M. d tan 4 (A + B) = ~sin x tan x tan i (A - B) = sin z 9. Given the perimeter = 2 s, C, and the perp. from C = p. tan" x - cot g C c = cosa x 2 10. Given c, a + b = m and the radius of the inscribed circle = r. sin x (m +c a - b - c cos z c m - c 2r tan C = m - c 11. Given c, a - b = n, and the radius of the inscribed circle = r. tan x = (c ) (-n) a + b = c cot (x - 45~) 4 r2 12. Given the radii r', r", r"', of the three escribed circles. (Arts. 153,.54) tan" ~ A = r' r" + r' r"' + r1" r."' 1S5. Given the sides of a quadrilateral inscribed in a circle, to find its angles and area. Fig. 28. In Fig. 28, let A B = a, B C - b, C D = c, A = d. Let 2 s = a + b + c + d and K = area of A B C D; then from the triangles ABC', ADC, observing that B = 180~ —D \ we find sin I B (s- a) (s-b) s B (s-c) (s- d) ab + ed ab+ -- d \ /~ (, -tan'i B (s-a) (s -b) [ — )( —( -- () (s - d) S = / [(s - a) (s - ) (s - c) (s - d)] (808) SOLUTION OF TRIGONOMETRIC EQUATIONS. 85 CHAPTER X. SOLUTION OF CERTAIN TRIGONOMETRIC EQUATIONS AND OF NUMERICAL EQUATIONS OF THE SECOND AND THIRD DEGREES. 166. THE solution of a problem in which the unknown quantity is an angle, often depends upon that of one or more equations, involving different functions of the angle, which cannot be reduced by merely algebraic transformations. We shall select a few simple examples of such equations from among those that most frequently occur in astronomy. 167. To find zfrom the equation sin (z + z) = m sin z (309) in which a and m are given. We have, by (119), sin ( ca + z) = sin ca sin z (cot z + cot os) which becomes identical with (309) by taking sin a (cot z + cot o,) = m whence the required solution cot z --- cot c (310) sin a If the proposed equation were sin (o, - z) = m sin z (311) we should find cot z - + ot 0 (312) sin o& Unless z is limited by the nature of the problem in which these equations are employed, there will be an indefinite number of solutions; for all the angles z, z + 180~, z + 360~, z + 540~, &c., in general all the angles z + n ir have the same cotangent. [See (68), (79).] In most cases, however, we consider only the first two of these solutions, taking the values of z always less than 360~. H 86 PLANE TRIGONOMETRY Stmilar remarks apply in all cases where an angle is determined by a single trigonometric function; but if the problem is such as to give the values of two functions of the required angle, as the sine and cosine, the solution is entirely determinate under 360~, since there cannot be two different angles less than 360~ that have the same sine and cosine. 168. The solution of the preceding article requires the use of a table of natural cotangents; to obtain a formula adapted for logarithmic computation entirely, we deduce from (309) the following sin (oa + z) + sin z m + 1 sin ( + z) - sin z m- 1 But by (109), if x = a + z, y = z, we have sin (o + z) + sin z tan (z + ~- ) sin (, + z) - sin z tan c which substituted above, gives tan (z + 1- = -- tan which determines z + 2- a, whence z is found by deducting o. The computation of this equation is facilitated in most cases by introducing an auxiliary angle, such that tan qp = m an assumption always admissible, since while the angle vanes from 0 to 90~ the tangent varies from 0 to co, so that an angle p may always be found having any given number as its tangent. We have then by (152), m - 1 tan (+1 - 14 r-i- =tan-1 = cot (<p - 45~) m - 1 tan p - 1 and the preceding solution becomes tan >p = m, tan (z + I a) = cot ( -- 45~) tan - (313) The logarithmic solution of (311) is found in the same manner to be tan (p = m, tan (z - 1 ) = cot (p + 45~) tan - cc (314! SOLUTION OF TRIGONOMETRIC EQUATIONS. 169. To find z from the equation tan (oa + z) = m tan z (315) We deduce tan (a + z) + tan _ m + 1 tan (c + z) - tan z -- 1 so that by (126) and (152) the solution is tan = m, sin (a + 2 z) = cot () - 45~) sin a (316) 170. To find z from the equation tan (o + z) tan z = m (317) We deduce 1 + tan (o + z) tan _ 1 + m 1- tan (a + z) tan z 1 -— m so that by (127) and (151) the solution is tan p = m, cos (o + 2 ) = tan(450 - p) cos (318) 171. To find z from the equation sin ( c tz) sinz =m (319) By (108) we find cos ~ - cos (:t 2 z) = ~ 2 sin (ac z) sin z -= t 2 m whence cos (c =-+ 2 z) = cos a =F 2 m (319*) which determines a M5 2 z, and hence 2 z. From (319*) we have four values of aL =: 2 z between 0~ and 720~; therefore, four values of 2 z between the same limits, and four values of z between 0~ and 360~. In general, we shall have four solutions under 360~ in all cases where the double angle is determined by a single function. The logarithmic solution of (319) varies with the signs of m and z. Thus, if the equation is sin (a + z) sin z = m m being essentially positive, we have by (133) cos c - cos2 (z + at) = sin (ca + z) sin z = m cos? (z + i a) = coSr ac - and by (133) again this is solved by cos 0 = m, cosa (z +4 i ) = sin ( + ~ C) sin (0 - } ) and the other cases are solved by similar methods. 88 PLANE TRIGONOMETRY. 172. The preceding examples will suffice to indicate the method to be followed with all the equations of the following table. The solutions of the equations involving cosines may be obtained from those involving sines, by exchanging z for 90~ -- z, or et for 900 =. a. Logarithmic solutions of the first four will be obtained by imitating the process of Art. 171. EQUATIONS. ISOLUTIONS. _ _. _..~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ 1. sin (cc z) sin z = m 2. cos (x c z) cos z = m 3. sin (a tz) cos z m 4. cos (a -i z) sin z = rm 5. sin ( -t z) == nm sin Z 6. cos (a ~ z) = m cos z 7. sin (a -i z) = m cos z 8. cos (a = ) = m sin z 9. tan (a e z) tan z m 10. tan (a -z) = m tanz cos ( - 2 z) = cos 2 m cos (rt - 2 z) = 2 m - cos a sin (a:t 2 z) = 2 7i - sin sin (ac b 2 z) = sin cc:= 2 rm tan =m, tan (z t -- a) = cot (< q 450) tan tan, = m, tan ( — Z ~ 2) = tan (45~ - c) cot A. tan - = mr, tan (450 -- I a z) = tan (150 -_) tan (450 + 2- j tan - im, tan (450~ - I a F Z) = tan (45~ -0 a) tan (a - 45~) tan 0 = m, cos (a 2 z) = tan (45~ F >) ',os C tan 0 = m, sin (2 z: a) = cot ((:zF 45~) sin a In the numerical solutions the signs of the angles and their functions must be carefully obstrved. The signs of the functions should be prefixed to their logarithms, according to Art. 99. The auxiliary angle 0 may be taken numerically less than 90~ in all cases, but positive or negative according to the sign of its tangent. It can easily be shown that we shall thus obtain the same values of z as by taking 0 in the 2d quadrant when its tangent is negative, or in the 3d quadrant when its tangent is positive EXAMPLE. Find z from (317) when a = 65~ and m = 1-5196154. By (318) log tan 0 -- log mn* + 0-181733' 0 56~39' 9" 45-0 — 11~ 39' 9, log tan (45~ - 9) - 93143426 log cos ac + 9-6259483 log tan (45~ - 0) cos a = log cos (a + 2 z) - 8-9402909 + 2 z 950 or 265~ or 455~ or 625~ a 65~ 2 z 30~ or 200~ or 390~ or 560u z 15~ or 100~ or 195C or 280~ * It must be remembered that in this employment of the signs + and -, these signs belong to the natural numbers; and when the logs. are addea or subtracted, the sign of the result is to be determined according to the rules of multiplication and division in algebra. SOLUTION OF TRIGONOMETRIC EQUATIONS. 89 i78. To find zfrom the equation sin (a + z) = m sin (R + a). Put z' =,6 + z, d' - a - /, then this equation becomes sin (a - z') = m sin z' which is of the form (309) and may be solved by (309*) or (311); then z = z' —. In the same manner equations of this form, involving cosines or tangents, may be reduced to those of the preceding table. 174. To find k and z from the equations k sill z- m= (320) k cos z n We have, by division, tan z - n which gives two values of z, one less, the other greater than 180~; whence, also, two values of k from either of the equations m n sin z cos z The solution becomes entirely determinate (z not exceeding 360~) as follows: 1st. When the sign of k is given. For if k is positive, sin z has the sign of m, and cos z the sign of n, and z must be taken in the quadrant denoted by these signs. If k is negative, the signs of sin z and cos z are the opposite to those of m and n, and z must be taken accordingly. 2d. When z is restricted by either the condition z 180~, or z > 180~. For under either of these conditions the tangent gives but one solution. If z < 180~, k has the sign of m; and if z > 1800 c has the opposite sign to that of m. 3d. When z is restricted to acute values, positive or negative. For under this condition a positive tangent will give z between 0~ and + 90~; and a negative tangent, between 0~ and - 90~; and k will always have the sign of n. It follows that m and n being any given numbers whatever, we may always satisfy the conditions expressed by (320), 1st, by a positive number k and an angle z between 0~ and 360~; 2d, by a number k (unrestricted as to sign) and an angle z < 180~; 3d, by a number k (unrestricted as to sign) and an angle z > 180"; and 4th, by a number k, and an angle z in the 1st or 4th quadrant. 12 a2 PLANE TRIGONOMETRY. EXAMPLE. To find k ai;d z from (320), (k being a positive number), whmw m - 0.3076258, n = + 0.4278735. k sin z - 0.3076258 k cos z + 0.4278735 (a) log k sin z - 9.4880228 (b) log c cos z + 9.6313147 (a)-(b) log tan z - 9.8567081 z 324~ 17' 6".6 (c) log sin z - 9.7662280 (a) (c) log k + 9.7217948 k + 0.5269808 Upon this problem and the deductions we have made from it, rests the method of introducing the auxiliary angles required in solving many of the formulae of spherical trigonometry. It is applicable to any equation that can be reduced to the form of that solved in the following article. 175. To solve the equation m cos z + n sin z = q (321' m, n and q being given. The first member will be reduced to the form k sin (cp + z) by as suming k and (p such that k sin p = m, k cos p = n (322) whence c sin ( cos z + k cos p sinz = q sin (p + z)- _ (323) Therefore, if k and cp be found from (322) by the preceding article, (k being limited to positive values), we can then find by (323) the value p + z and therefore of z. There will be two solutions from the two values of <p + z given by (323). SOLUTION OF TRIGONOMETRIC EQUATIONS. f91 If we restrict p to values less than 180~, (as we may do according to the last article), we may find it by the equation m tan p = sin (,< + z) ==- sin = - cos p m n I (324) and then and in this form it will be unnecessary to find k.* EXAMPLE. To find z from (321) when m = - 1.0498332, n = + 0.7466898, and q = - 0.4316893. By (322) and (323). log m = log k sin p- - 0.0211203 log n = log k cos qp + 9.8731402 log tan 9p - 0.1479801 p 305~ 25' 20" log sin p - 9.9111059 log k + 0.1100144 log q -9.6351713 log sin (ap + z) - 9.5251569 f 199~ 34'40" ) XI or 3400 25'20" - 105~ 50'40" I or 35~ 0' 0' To avoid the negativ- value of z, we may take for the first value of By (324). log m - 0-0211203 logn + 9.8731402 log tan p - 0.1479801 P 125~ 25' 20" log sin p + 9.9111059 log q -9.6351713 ar co log m - 99788797 log sin (p + z) + 9.5251569,+ f 19~ 34' 40' or 160~ 25' 20" - 105~ 50'40" or 35~ 0' 0 in the first of these solutions, p + z, 360~ + 199~ 34' 40" = 559~ 34' 40" whence z 559~ 34'40"- 305~ 25' 20" =254~ 9' 20". The se cond solution gives a like result. If we suppose <p in (324) to be limited to acute values positive or negative, we take p = - 54~ 34'40", which gives q + z= 199~ 34' 40," or 340~ 25' 20", whence the same values of z as before. We may repeat the latter part of the work with cos p for verifi. cation. * The solution is, by (323), impossible when - is greater than unity; and by adding the squares of (322), k =- m + no; therefore the solution is impossible when > r- + n*. PLANE TRIGONOMETRY. 176. To solve the egu.tion a sin ( + z) + b sin (6 + z) + c sin (k + z) + &c. = q (326) Developing by (36) and putting a sin a + 6b sin 3 + c sin + &c. = n a cos a + b cos +1 c cos + &c. = n this becomes m cos z + n sin z -= which is solved in the preceding article. The same process applies if any or all of the terms contain cosines. 177. To find k and z from the equations k sin (a + z) 26) k sin (3 + z) n J The sum and difference of these equations are, by (105) and (106), 2 k sin [- (a + 13) + z] cos t (a - f) = n + Z 2 k cos [a (a + 1) + z] sin (a - ) = m - n whence 2 k sin [- (a + ) + z] = - n cos 4 (a - 3) (827) 2 k cos [ (a +3) + z] = in ( — ) from which 2 k and i (a +- /) 4- z are determined by Art. 174. The logs. of the second members of these equations should be computed separately, for the purpose of readily discovering the signs of the sine and cosine in the first members. The solution is determinate (according to Art. 174) when the sign of k is given. From (327) we find, by division, tan [a (a -+ l) + z] = +n tan (a - ) (328) which requires a less number of logs. than the separate computation of (327), but we are obliged to refer to (327) to determine (by an inspection of the second members) the signs of the sine and cosine. If we assume n tan = - m (329t we may compute (328) by the formula tan [- (a +- 1) + z] = tan (45~ + 0) tan i (a - l) SOLUTION OF TRIGONOMETRIC EQUATIONS. 98. EXAMPLE. In (826) given a = 200~, / - 140~, m - - 042345 and n - 0-20123, to find z and k, k being positive. By (327). m + n - 0062468 - n - 0-22222 (a + - ) 1700 (a- /) 300 log (m + n) - 9-7956575 log cos - (a - A) + 9-9375306 (a) log 2 k sin [4 (a + /3) - z] - 98581270 log (n -n) - 9-3467831 log sin 4 (a - ) - 9-6989700 (b) log 2 k cos [ (a + /3) + z] - 9-6478131 (a) - (b) log tan [- (a + /3) + z] + 02103140 4 (a + /+ z) 2380 21' 38"6 z 68~ 21' 38"-6 (c) log sin [4 (a - /) + z] - 9-9301171 (a) - (c) log 2 k + 9-9280099 2 k 0-8472467 k 0-4236234 178. A more general solution of (326) is the following.* Let 2 be any angle assumed at pleasure, and in (171) let x = a - z, y = / - z, z' = — z (distinguishing the z of (171) by an accent); then we shall find sin (a - 3) sin ( - + z) = sin (a - 2) sin (/ + z) - sin (/ -2 ') sin (a + z) In this let, (whose value is arbitrary) be exchanged for? +- 90~; then sin (a- 3) cos (' +- z) = - cos (a - 2) sin (/ +- z) + cos (/3 - 2) sin (a + z) Multiplying these equations by k and substituting m and n from (326) k sin (a - /) sin ( -+ z) m sin (y - /3) -n sin (- a) (33 k sin (a - ) cos ( +- z) = m cos (n - 1) - cos ( - a) which (> being assumed at pleasure), determine k and -4- z. If we take - =- 0, we find - m sin q-3- n sin a tan z -- in cos / - n cos a If =- a, i sin (a + z) = m k co (a + z) = Cos (a-)- n (831) k COS (a 4 — 2) -- -7-(sad sin (a -A ) If? =-, we have a similar result. If -- = 4 (a + A) we obtain the solution of the preceding article. If k is required, without first finding z, we have, by adding the squares of (330) k sin (a -A ) = / [ma+ - n 2 m n cos (a - )] (332) * GAUSS. Theoria Motus Corporum Coelestium, Art. 78. 94 PLANE TRIGONOMETRY. 179. To find k and zfrom the equations k cos (a + z) = m (333) k cos (3+ z) = n These are reduced to the form (326) by substituting 90~ 4+ and 90~ + - for a and /. We find, however, by a process similar to that of Art. 177, 2 k siu [~ (a + /) + z] = -- ( sin (a - [(334) 2 k cos [ (a + ) + ] - co i ( - cos k (a+-13) j or tan = -- n ^ (385) cot [+ (a + #) + z] = tan (450 + 0) tan i (a- 0) EXAMPLE. In (333) given a = 280~ 16', / - 200~ 10', m = - 062342, and n 0-69725, find z and k, k being positive. Ans. z = 207~ 5' 34"-4 ck = 1-0273643 180. The more general solution of (333) may be found directly from (172), but it will be simpler to obtain it from (330) by substituting 90~ + a for a, and 90~ + /1 for A, whence k sin (a - /) sin (y + z) - m cos (y - ) + n cos (y- a) (336) k sin (a - () cos (r + z) = m sin (y - ) - n sin (y- a), being arbitrary as before. If y 0, we find -m cos /3 - n cos a tan z t - m sin /-+ n sin a If y = a, - m cos (a -/) + n1 in(a+)= sin (a - ) (37) k cos (a + z) = J If y i= (a +- A), we obtain the solution (334). If k is required directly, the sum of the squares of (336) gives k sin (a - /) = ^ [m' - n - 2 m n cos (a- f)] bb in Art. 178. i81. The solutions of the preceding articles may be applied to a single equation of the form n sin (a + z) = m sin (f/ + z) which is a more general form of (309). For if we assume k sin (a + z) - m we have k sin (/ +- z) n whence k and z are found by Arts, 177, 178. EQUATIONS OF THE SECOND AND THIRD DEGREES. 182 In like manner, if the proposed equation is n cos (a + z) = m cos (s? + z) we assume k cos (a + z) ='m whence k cos ( + 2z) = -n and k and z are found by Arts. 179, 180. As the sign of k (in this and the preceding article) may be arbitrarily assumed, there will be two solutions. NUMERICAL EQUATIONS OF THE SECOND AND THIRD DEGREES. 183. To solve the equation x5+ px + q = 0 (338) when q is essentially positive, and p either positive or negative. We have from (144), exchanging x for 0, tan2 0 - 2 cosec 0 tan 0 - 1 = 0 (339) and (338) may be reduced to this form by substituting x = z/q In which we may take the radical only with the positive sign, since we may assume X and z to have the same sign. We thus reduce (338) to p z'~- z -+ 1 O V q which compared with (339) gives - 2 cosec 0 =, z = tan o 2,/q or sin 0 - =, x == /qtan i 0 (340) which gives two values of 0 less than 360~ and consequently two values of x. If 0 be the least of these two values of 0 less than 360~ (= 2 r), all the values of 0 which have the same sine are 0 w 0 2w 0, 3r - - o, &c. and all the values of tan i 0 are tan i 0, cot I 0, tan i 0, cot i 0, &c. Hence the two roots of (338) are found by the formulae sn 0=-,, = /~I ta, I 0, x _A = -cot 84),n which 0 may be always taken < 90~ with the signi of its sine, and / q is to be regarded as a positive quantity. As long as 2 / q is not greater than p, this solution is possible, but when 2 / q >p, sin 0 is not possible, and both roots are imaginary; which agrees with what is shown in algebra. 96 PLANE TRIGONOMETRY. 184. To solve the equation xi +px - q 0 (342) when - q is essentially negative, p being either positive or negative. We have, by (143) tan* f + - 2 cot ( tan ( - 1 = 0 and (342) is reduced to this form by substituting x = z/q whence z + z — = 0 The required solution is therefore 2 cot f -- z =tan 2 or tan = —, z = / q tan ~ 0 (343) If 0 is the least value of 6, all the values of 0 which have the same tangent are 0, v+ 0, 2 - + 0, 3 r + o, &c. and all the values of tan (p are tan I 0, -cot - 0, tan ~ 0, - cot ~ 0, &c. Therefore the two roots of (342) are found by the formulae tan 0 _= - xl= v/ t tan 0, x = - a/ q cot o (344) p in which, as before, the radical is to be taken as positive, and 0 < 90~ with the sign of its tangent. In this case both roots are real, since tan 0 is always possible. 185. To solve a numerical equation of the third degree. It is shown in algebra that any equation of the third degree may be reduced to one. in which the 2d term is wanting; we need consider therefore only the form x3 +- ax + b = O (345) To resolve this, put x = y + z x=y4-z we find (3 y z + a) (y + z) + y3 + + b = 0 Now x may be decomposed into two parts, y and z, in an infinite variety of ways, and we may therefore suppose that y and z are such as to satisfy the condition 3yz - a = 0 which reduces the first term of the preceding equation to 0, and gives the two con ditions a yz —, y' + ~z = — b Put y = ta, z' = to; then we have as t2 t -- 7, t, + tq — b EQUATIONS OF THE SECOND AND THIRD DEGREES. 97 so that, by the theory of equations, t, and t, are the two roots of an equation of the a3 second degree in which the absolute term is - - and the coefficient of the second 27 term is b; that is, they are the roots of the equation a3 t + bt- 7 = (m) If then we find the two roots t, and t, of (m) by the preceding methods we shall have x =_ y + z - ~t + ts (n) It will be necessary to consider the sign of a in the equation (m). 1st. When a is positive, (m) comes under the form (342) and the solution by (344) gives 2 a3" r^l aa tan 0 = T8 q ~' t, = t, -- -- tan 0= N = 27 tan,,= ~2- cot 0 and by (n) x J- 3 -( tan 0 - cot i 0) and if we assume tan i = -9/ tan i 0 this becomes, by (142) la x=- 2 -- cot Collecting these results we have, for the solution of (345), when a is positive, 2 as tan 0 = J - 2-, tan i p =_ tan 10 3 ~~~~~1 a~(36) x -2 - 2 cot J in which the radicals J - and - 3 are to be considered positive, and 0 is to be taken < 90~ with the sign of the tangent. But two of the three values of V tan I G being imaginary, the given equation has but one real root.* * If r represent the real value of 3 tan ~ 0, and a,, a, the two imaginary roots of unity, the real value of z is a ( 1\ 1 - 3 t r J and the imaginary values are or since, a, s= 1ra or since a, a, - 1 x J 3 (ra, X3 J ra,- -) - I 18 I 98 PLANE TRIGONOMETRY. 214. Whlen a is negative and — 4 a3 < 27 be. Equation (m) becomes + bt+ ( —27 and is of the form (338); its roots are therefore found by (341) which gives 2 1 a3 --- a3 sin 6 =- J- 27 - 27 a-3 at, = tan0 t = - - cot 0 and by (n) x -- 3 (a tan 0 -+ cot 0) or if we put, as before, tan 2 0 -= s tan 4 0, the solution of (345), when a is negative, is sin 0 = -- t t- tan ~ = tan o 0 __f (347) / a xz 22 --- cosec 0 which gives one real root, (the other two being imaginary, as above), when sin 0 is possible, i. e. when - 4 a3 < 27 b3.* Substituting the values of a, and a. -1+ /-3 - _ - a-3 a, 2 a. 2 and also r = tan 0 -= cot we find xa =J -3 (cot 0 + cosec 0 V - 3) x, =J - (cot 0 - cosec - 3) or finally, x, being the real root, the imaginary roots are X, x, V8 X = - - - sec / - 1 ri x /3 2 -: 2 + s/ sec - 1 2 2 * The two imaginary roots will be found, by a process similar to that employed i the preceding note, to be 2 2 xin wi, is the rel root found by 347 = - -a ---~2 --- cos P V - 1 in whiah x, is the reol root found by (347). EQUATIONS OF THE SECOND AND THIRD DEGREES. 99 3d. When a is negative and - 4 a'> 27 b'. In this case sin 0, in (347), is impossible and the preceding solution fails. This is the irreducible case of Cardan's rule, the roots appearing under imaginary forms, although it is known that they are all three real. It is, however, readily solved trigonometrically. In Art. 77, putting s for x, we have sin3 0 - -a sin - + sin 3 0 = m') and (345) may be reduced to this form by substituting x =- kz a b whence z - z + - 0 (N) ao that we must have a 3 or k —2 -- C., 3 in which the radical is to be taken positive, so that x and z shall have the same sign. Comparing (m') and (n') we have also 6 b I 27 i 27 b sin 3 0 — or sin 3 0 = - - | 4 a which is a possible sine in the present case. We may therefore take z = sin and the solution is b~ 1 27 sin30 =3 2 -- 2sin J — (348) which gives three real roots by the different values of 3 p, which have the same sine. If 0 is the least of these values, all the values of 3 p are expressed by 2 n zr + 0 and (2 n + 1) 7 -0 n being any integer or 0; and all the values of S are expressed by 2n 2 n -- 1 = W-~+ +, 0= 3 — ~= *0 Now all integers are included in the forms 3 m, 3 m + 1 and 3 m - 1. If n = 3 m, the above values of Sb are _= 2m7r+~*, 0 =_ 2m r+ - r -2 -whence sin 0 = sin ~ 0, sin 6 = sin * (r- 0) If n = 3 m + 1, we find in the same way sin _ sin r ( -0), sin =- 0 the same as before. If n =- 3 m - 1, we find both values to be sin 0 = - sin i ((r + 9) 100 PLANE TRIGONOMETRY so that tnere are but three different values of sin 0. Substituting these in 3(48), the three roots of (345), when a is negative and - 4 a' > 27 b, are found by b 6 27 sin 0 - - x, =2J —3sin 0 — _ ___. (849) a a, = --- 2 sin i (r+ 0) = -2 - sin (60~+ - 0) x,_-2J 3-sini(rr+e)==-2 I-4 sin(60~+ 0) in which 0 < 90~ with the sign of its sine, and the radicals are taken with the positive sign. EXAMPLES. 1. Solve (345) when a = - 6-101315, b - - 5766578. We find log- - = -- 0-002651* which being greater than any log. sine, we take its arithmetical complement and proceed by (349). Then log sin 0 = - 9,9974349 0= - 83 46' 44" 0 - 27055'34". 7 60~- - 0 87055'34".7 _ (600 + 0) -3204'25" 3 log sin - 9-6705571 9-9997155 - 97251024 log 2J — 0-4551811 0-4551811 04551811 log x, -0-1257382 log x, 0-4548966 log x, - 0-1802835 x, = - 1-335790 x = 2-850339 x, = - 1-514549 2. Solve (345) when a = - 7, and b = 7. Ans. x, = 1-356896, x -= 1-692021, x, = - 3048917. 8. Solve (345) when a = 1-5, and b = - 45. Ans. The real root = 384163975. It may be observed that the algebraic sum of the three roots is always zero, in consequence of the absence of the term in x' from the given equation. This is easily shown from (349) where there are three real roots, and from the forms in the notes p. 98, where there are imaginary roots. This principle furnishes a simple verification of the values found by (349). * The sign - here belongs to the number of which this is the logarithm DIFFERENCES AND DIFFERENTIALS. 101 CHAPTER XI. DIFFERENCES AND DIFFERENTIALS OF THE TRIGONOMETRIC FUNCTIONS. 186. IN the applications of trigonometry, it is often required to compute a function of one angle from that of an angle which differs from the first by a small quantity. In such cases it is generally most convenient to compute the difference of the two functions, which may be applied to either to obtain the other. 187. To find the increment of the sine or cosine of an angle, corresponding to a given increment of the angle. Let the angle x be increased by A x, (this notation signifying difference, or increment of x), and let the corresponding difference or increment of the sine be expressed by A sin x and of the cosine by A cos x; we have, by this notation, A sin x = sin (x + A x) - sin x A cos x = cos (x + ax) - cos x and by (106) and (108) A sin x = 2 cos (x + 3 A x) sin 1 A x (350) cos x= -2 sin (x + 2 a x) sin I A x (351) which are the required formule. We here consider the difference always as an increment, i. e. an increase, and give it the positive (algebraic) sign; its essential sign may, however, be negative, and it will then be in fact a decrement. Thus, in (351) the second member will be negative so long as x <180~, and therefore the increment of the cosine is negative; that is, from 0~ to 180~ the cosine decreases as the angle increases. In like manner A sin x is negative when x > 90~, and < 270~. 188. To find the increment of the tangent and cotangent. We have A tan x = tan (x + A x) - tan x A cot x = cot (x + x) - cot x and by (116) and (119) sin A x A tan x= c sin A x -c = sec(x+ Axsesx sin Ax (352) cos (x + A x) cos x -- sin A x a cot x — sin - x -- -- _ cosec (x + A x) cosec x sin A x (353) sin ( + AX) sin X i2 102 PLANE TRIGONOMIETRY. 189 T6 find the increment of the secant and cosecant. We have A sec x= sec (x + A ) - sec x A cosec x = cosec (x - A x) - cosec x or by (130) and (132) 2 sin (x + -2 A x) sin ( 3 x see x = 8 2 (354) cos (x + A x) cos; - 2 cos (x -+ a x) sin i A xa A cosec x = — 2- (55 sin (x +- x) sin x 190. To find the increments of the squares of the trigonometric functions corresponding to a given increment of the angle. We have A sin2 x = sin2 (x +- A x) - sin' x = cos x - cos2 (x + A x) whence by (133) sin x =- a cos2 x = sin (2 x+- a x) sin a x (356) From (115), (116), and (119) we deduce tan x - tan y _sin (x - y) sin (x- y) cot x cot - sy in (x + y) sin (x-y) sin x; sin' y whence sin (2 x +- a x) sin A x- a tan'a: --- (357) cos2 (x + a a) cos1 x( - sin (2 x + A x) sin A x sin2 (x + A x) sin2 x (858) From (16) we have sec2 (x + A x) = tan' (x + A x) - 1 sec2 x = tan' x -- the difference of which gives A sec2 x = a tan2 x (359) and in the same manner, from (17), A cosec2 x = A cot' x (360) and the values of A tan2 x, A cot2 x, may be substituted in (359) and (360). 191. When the increment of an angle, or arc, is infinitely small, it is called the differential of the angle, or arc; and the correspond ing increments of the trigonometric functions are the differentials of these functions. The differential of x is denoted by dx; of sin x by d sin x, &c. DIFFERENCES AND DIFFERENTIALS. 103 192. To find the differentials of the trigonometric functions from the differential of the angle. Let the angle x and its increment Ax be expressed in the unit of Art. 11; or, which is equivalent, let x and Ax be the arcs which measure the angle and its increment in the circle whose radius = 1. It is evident that the less the arc, the more nearly does it coincide with its sine or tangent; therefore, when Ax is infinitely small, or becomes dx, sin dx =dx sin 1 dx = dx This may be demonstrated more rigorously thus. When dx is infinitely small, we have cos dx = 1, whence sin dx n dx - = cos dx = 1 tan dx sin dx = tan dx but the arc cannot be less than the sine, nor greater than the tan gent, and therefore dx = sin dx = tan dx Again, when ax is infinitely small, or becomes dx, we must, according to the principles of the differential calculus, reject it when connected with finite quantities by the signs + or -; thus we must substitute x for x + dx, or for x + 2 dx. Upon these principles we find the differentials directly from the finite differences (350), (351), (352), (353), (354) and (355) as follows: d sin x = cos x dx (361) d cos x =- sin x dx (362) dtan x = sec2 x d= (1 + tan2x) dx (363) d cot x - cosec2 x x =- (1 + cot2 x) dx (364) d sec x - tan x sec x dx (365) d cosec x =- cot x cosec x dx (366) 193. In the same manner the equations (356), (357), (358), (359) and (360) give d sins x = - d cosx x sin 2 x dx (367) d tan' x = d sec x s= 2 - dx (368) COS4 x 2 sin x 2 tan x COSa X Co08 X sin 2 x dcotsx = d cosecs x _ sin'x Z(~u -2 cos x -2 cot x sin dx s xin (371\ 104 PLANE TRIGONOMETRY. 194. Although the equations (361), (362), (363), (364), (365) and (366), are rigorously true only when dx is infinitely small, they may be used when dx is a finite difference, instead of the equations, (350), (351), (352), (353), (354) and (355), provided dx is sufficiently small to be considered equal to its sine without sensible error, and is also very small in comparison with x. This is very frequently the case in practice, and the differential equations are then preferred on account of their simplicity. It is only necessary to observe that dx must be expressed in are, i. e. in terms of the unit radius; if it is given in seconds, it may be reduced to arc by Art. 9. 195. To find the differential of an angle from the differentials of its functions. Fiom (361) we have d sin x dx = n (372) cos X but it is convenient in this case to employ the notation of inverse functions, Art. 87. Thus, if y = sin x, x = sin- y, and the preceding equation becomes dsin-ly 4 d y (378) [n the same manner from (362), &c., we find d cos-y- ( - y) (374) d tan-l y _= y2 (375) - dy d cot-ly = + (376) dy d sec-l y ( 1) (377) -y dy (y2 d cosec-' y =Y v (y - 1) (378) DIFFERENCES AND DIFFERENTIALS OF PLANE TRIANGLES. 105 CHAPTER XII. DIFFERENCES AND DIFFERENTIALS OF PLANE TRIANGLES. 196. IN trigonometrical investigations it is Fig.29. C' often necessary to determine the effect of a small change in one of the data, upon the computed parts. Thus, Fig. 29, if A, AB and / A C, of the plane triangle AB C, are the data, A B and A C is subject to an error of C C', the required parts will be subject to errors which are respectively, the differences between A CB and AC'B, A B Cand A B C', B C and B C'. In the same figure, the data may be supposed to be A, A B and AB C, and the angle AB C may be regarded as subject to the error CB C' which produces the corresponding errors in the remaining parts. In the same manner, the data may be A, A B, and A CB, A CB being variable; or, A, A B, and B C, B C being variable. In all these instances, A and A B are constant, while the remaining four parts are variable, and may be considered as receiving, simultaneously, certain increments which are related to each other. We propose, then, to solve the general problem: In a plane triangle, any two parts being constant, and the rest variable, to determine the relations between the increments of the variable parts. It is evident that the solution of this problem resolves itself into an investigation of the differences of two triangles which have two parts in common. We shall consider the several cases successively; distinguishing the triangle formed from the given one by the application of the increments, as the derived triangle. 197. CASE I. A and e constant. The six parts of the given triangle, A B C, Fig. 29, being A, B, C, a, b, c, those of the derived triangle formed by varying all but A and c, are A, B.+ AB, C + A C, a + Aa, b + Ab, and c. In these two triangles we have A B+ B + = 1800 A + B + AB + C + = 180~ whence AB + A G = 0, AB= - A C (379) 14 106 PLANE TRIGONOMETRY. Also in the two triangles we have a = c sin A cosec C (m) a + Aa = c sin A cosec (C + AC) (n) the half difference of which by (355) is - _ - c sin A cos(C + ~ AC) sin A 7 (C 2z asin C sin (C + AC) JA a I Aa _ acos(C7+A) (380) (380) sin i AB sin AC sin(C + AC) The half sum of (m) and (n) by (131) is c sin A sin (C + 1 a c) cos ~ AC a + Aa=2 2 a 2 sin Csin (C + AC) which combined with (p) gives ~Aa + ~Aa Aa /g 2 2 - =_8 tan 1 B tan 1 AC tan (G + AC) ( From (260) we have c sin A tan ---- b - c cosA whence b - ccosA = c sinA cot C 6 + Ab - c cos A = c sin. cot (C + AC) the difference of which by (353) is c sin A sin AC sin Csin (C+ AC) therefore Ab Ab a sin AB ' - sin AC - sin (Ca+ a) (82) DIFFERENCES OF PLANE TRIANGLES 107 This equation gives by (135) ~2 ab a sin aC cos 6 a C sin (C + AC) and dividing (380) by this Aa = cos (C + C) Ab cos A(7 ~ C It is to be observed that the increments (or half increments) of the angles must be deduced from their sines or tangents, since it is only by these functions that a small angle can be accurately determined. Moreover, a small arc being nearly equal to its sine or tangent, the equations (380), (381) and (382) express very nearly the ratios of the increments of the sides to the increments of the angles, or rather to those increments reduced to arc by Art. 9, or Art. 54. 198. CASE II. A and a constant. We have as in the preceding case AB =- A C; and in the two triangles 6 sin A a sin B (b + Ab) sin A = a sin (B + AB) the difference and sum of which give Ab sin A =a cos (B + 2 aB) sin I AB (p) (b + I Ab) sin A = a sin (B + I AB) cos -1 AB whence by division Ab I Ab _ b + Ab (384) tan aB tan 1 AC tan (B + AB) In the same way 1A~hc 1 c c ".... =2 2 (385) tan Ca = tan I AB tan (C + l AC) From the equations c sin A = a sin C (c + Ac) sinA = a sin (C + AC) we find we AcsinA = a cos (C + 1 AC) sin I AC 2 L Ll r v 2 2VjIlu2Y (A) 108 PLANE TRIGONOMETRY. which combined with the equation (p) gives, since sin!AC 7=- sinIA-B, ab =_ cos(B + B) (38) ac cos (C + A kAC) From (p) we also have.A6 A Ab 6 cos (B + AB) (387 sin ~ aB sin j AC sin B which, when A b is to be found from AB, is more convenient than (384). In the same way from (q) a 6Ac aC c cos (C + j aC) sin AC sin sin A sin C 199. CASE III. b and a constant. We have c sin B = b sin C c sin (B + AB) = b sin (C7 + AC) the sum and difference of which give csin (B + i AB) cos - AB = b sin (C+ i AC)cosAC7 (p) ccos (B + } AB) sin,AB = b cos (C + I AC) sin AC (q) the quotient of these gives tan B aB tan (B +- B) tan Aa tan (C +- ) a C) By (224) we have a = b cos C + c cos B a + Aa = b cos ( + AC) + c cos (B + B) the sum and difference of which give a+ Aa b cos(C + aC) cosA -AC +ccos (B + AB) cos AB - Aa b= sin(C+ - AC) sin A+ csin (B + aB) sin aB These expressions are reduced by (p) and (q) to a + Aa cos (B + 1 AB) cos - AB cot 1 (tan 1AB + tan AC) (r) -- ~ Aa=e sin (B + AB) os B (tan AB + tan I AC) (s) and by division Aa a + aa (390) tan I A C cot (B 4- i B) ( ) DIFFERENNCES OF PLANE TRIANGLES 109 In the same way we have - ~Aa a ~+ 1 Aa = - (2gl) tan -aB cot (C + AC) (8 Since the sum of the three angles is constant, AA + AB + AC= 0 (AB + AC) = - AA therefore by (115) sin I (AB + aC) tan AB + tan ~ AC= 2YABcos 2 2 cos I B cos A sin I AA cos AB cos AC ( which substituted in (s) gives a _ c sin (B + AB) -- (892) sin - aA cos 1 AC and in the same manner aa b sin ( + aC3) - 2 2 (393) sin 1A - cos j aB Substituting (t) in (r) we find sin AC _ ccos (B + 1 B)394) sin 1 AA a + aa sin A aB b cos (7 + Ae) whence also sinAB bcos( (395) sin - AA a + A aa By differencing the equation a2 = b2 + c2 2 bc cos A we find instead of (392) and (393) 1 Aa bc sin (A + - AA)96 sin 1 A = a a6) K 110 PLANE TRIGONOMETRY. 200. CASE IV. A and B constant. We have sin B b- - a sin A sin B snb + A A (a + Aa) sin B sin A whence Ab = -- Aa In this case the third angle is also constant and there are but three variables related by the equation siAa AsinB sn (397) sinA = sinB -- sin C This case is not strictly included in the general problem as stated in Art. 196, since the two triangles have not two parts in common. 201. The second members of the equations (380), (381), (382), (383), (384), (385), (386), (387), (388), (389), (390), (391), (392), (393), (394), (395), (396), involve the increments themselves, which are the quantities sought. It is therefore necessary, in many cases, to solve these equations by successive approximations. For a first approximation we consider the increments in the second member to be = 0, employing B for B + AB, &c., and taking cos I AB = 1, &c. This will evidently produce but a slight error so long as the increments are small as compared with the entire parts of the triangle. We then obtain a second approximation, by recomputing the equation in its complete form, employing in the second members the approximate values of the increments. With these second values we may, in the same way, obtain a third approximation, &c. Theoretically, it requires an infinite number of such approximations to arrive at a perfect result; but in practice, the tenths or hundredths of seconds being the limits of accuracy, it is rare that more than a second approximation is necessary. It is also to be observed that in computing the values of small quantities such as the increments in question, we may employ logarithms of only four or five decimal places and take the angles to the nearest minute. This is in fact one of the chief advantages of computing by differential formulae, rather than by the direct formulae applied to each of the two triangles successively. DIFFERENTIAL VARIATIONS OF PLANE TRIANGLES. 111 EXAMPLE. In a plane triangle whose parts are A = 58 41' 48".9 = 35~ 11' 3"4 C = 86~ 7' 7 '-7 a = 6053 b = 4082 c = 7068 let A and a be constant while b is diminished by 50.5; to find the change in the angle B. We have in this case Ab = - 50.5; and by (387) s Ab sin B sin ~ AB -- b cos (B + ~ AB) 1ST APPROX. 2D APPROX. 2 ab - 25.25 b 4082 B 350 11' 35~ 11' A AB 0 -15' B + - AB 35~ 11' 34o 56' log ab -1.4023 ar. co. log. b 6.3891 - 7.5520 log sin B 9.7606 ar. co. 1. cos (B + i aB) 0.0876 0.0863 log. sin - AB -7.6396 - 7.6383 ~AB - 15' 0" - 14'56".8 It is evident that changing the angle B + - AB by only three seconds would not affect the fourth place of its cosine; a third approximation is therefore unnecessary, and we have finally AB =- 29'53".6. As the log. sines of small angles do not vary proportionally with the angles, it will conduce to accuracy to employ the methods explained in Art. 115. DIFFERENTIAL VARIATIONS OF PLANE TRIANGLES. 202. The equations (380), (381), (382), (383), (384), (385), (386), (387), (388), (389), (390), (391), (392), (393), (394), (395), (396) and (397) become differential by making the increments infinitely small, that is, by omitting the increments when connected with finite quanti 112 PLANE TRIGONOMETRY. ties by the signs + or -, and substituting the increment itself for its sine or tangent, and unity for its cosine, (Art. 192.) The character d must also be substituted for A. These changes being made, we easily deduce the following differential relations. CASE I. A and c constant. dB - dC da da d-B -d- -= -a cot U db _ db a (398) dB d C sin C da a cos C db CASE II. A and a constant. dB =- d d db db ~dB ^^d6 b c6t B dB dc de det (399) c cot (399) d0 dB db cos B de cos J CASE III. b and c constant. dA +dB+d C 0 dB tan B dC tan C dea da ( - =- a tan B, - =-a tan a (400) da d- csB = sin B b sin dA d c dB b --- CcosB, --- CO dA a dA a DIFFERENTIAL VARIATIONS OF PLANE TRIANGLES. 113 CASE IV. The angles, A, B, C, constant. da db de - = _ = _^- (401) sin A sin B sin ( 203. These differential relations are often employed when the increments are very small, instead of the equations of finite differences. We have already seen that the equation of differences often requires to be solved by successive approximations, the first approximation being in fact obtained by employing the corresponding differential equation. In all cases therefore where a second approximation in the use of finite differences could not alter the result of the first, it is plain that the differential equation is sufficiently accurate. The increments of the angles must generally be expressed in arc. Thus if dB is given in seconds we must divide it by R" = 206264".8, or substitute dB sin 1" for dB. dA But in such fractions as dA-, this substitution is evidently unnedff> cessary provided the two increments are always expressed in the same unit, as minutes, seconds, &c. EXAMPLE. In a plane triangle whose parts are A - 58 41' 48".9 B = 350 11' 3".4 C= 86~ 7' 7"-7 a = 6053 b = 4082 c = 7068 suppose b and c to be constant and the angle A to receive the inmre. ment dA = 20".6; find da and dC. From (400) we have da = dA sin 1" c sin B dC -- dA ccosB dC --- a log dA 1.3139 log (- dA) - 1.3139 log sin 1" 4.6856 log c 3.8493 log c 3.8493 log cos B 9.9124 log sin B 9.7606 ar. co. log a 6.2180 log da 9.6094 og dC - 1.2936 da 0.407 dC - 19".7 15 K2 114 PLANE TRIGONOMETRY. 204. The error of employing the differentials in any case may be determined approximately by developing the equation of finite differences and comparing it with the corresponding differential equation. We shall select a simple example. We have from (387) and its corresponding differential equation in (399) ~ ab= b cos (B + AB) sin a sin B ab - b cot B AB sin 1" the first of which when developed gives ib = b cot B sin AB — 2 b sin (B + i AB) sin ~ AB sin I AB 4Abhicot~sin siA B-B siniB sin B 4 or substituting sin 4 AB -_ ~ aB sin 1", sin 1B -= A 1 AB sin 1", and also B for B +- I AB in the second term, which will affect so small a term but slightly, ab = b cot B AB sin 1" - (- B sin 1") Comparing this with the differential equation above, the error of employing the latter is approximately b - (aB sin 1")2 which for aB = 1~ is - 000015 b. It appears from this example that the error is expressed by a term involving the square of the increment; and if we develop all the equations of finite differences we shall find that they differ from the corresponding differential equations by terms involving the squares and higher powers of the increment. Hence, employing the differentials instead of the finite differences amounts to neglecting the terms involving the squares and higher powers of the increments. 205. The differential relations above obtained could have been deduced more directly from the formulae of plane triangles by differentiation, employing the values of the differentials given in Art. 192. Thus in CASE I, A and e being constant, if we differentiate the equation a - c sin A cosec C we have da = c sinA d cosec a -c sin A cot C cosec C d O - a cot C d is in (398) The student may exercise himself by deducing the other relations of (398), (899) and (400) in a similar manner. TRIGONOMETRIC SERIES. 15 CHAPTER XIII. TRIGONOMETRIC SERIES. DEVELOPMENTS OF THE FUNCTIONS OF AN ARC IN TERMS OF THE ARC, AND RECIPROCALLY.* 206. THE investigation of trigonometric series is most readily carried on with the aid of a few elementary principles of the Differential Calculus. All that will be required here will be no more than is generally given in the first chapter of a treatise on that subject, namely, the differentiation of simple algebraic functions, and Taylor's Theorem. We shall employ the following expression of this theorem: d.fy A ___ fy h2 d3 fy h3 f (y + h) =fy + d. * + + dy l 2- + &C. (402) dy 1 y2 1.2 dy3 1.2.3 (o) in which fy denotes what f (y + h) becomes when h = 0 and d.f d2.fy &c., are the successive differential coefficients, or de. dy dy2 rivatives of fy. 207. To develop sinx and cos x in terms of x. We shall first develop sin (y + x) and cos (y + x) by (402). By (361) and (362), if fy = sin y we have d.fy d sin y we have — = - - cos y dy dy d2.fy d cos y dy2r dy — r - sin y dy2 dy c.f y d sin y -L - - -j —= -- cosy dy3 dy - CO Y d4.fy d cos y -d/ 4dy — sin y dey4 -- dy ---- * The leading results of this Chapter being of very general utility and constant application are printed in the larger type, but as they are not referred to in the subsequent large print of this work, and moreover require a limited acquaintance with the Differential Calculus, the student can omit them at the first perusal, and pass directly to Part II 116 PLANE TRIGONOMETRY. so that the values of the coefficients of the series (402) recur in the order + sin y, + cosy, - sin y, - cosy, and therefore f (y + x) X X2 X3 sin (y + x) =sit y + cosy — - sin y 2- cos y 23 + &c. (403) If we commence with fy = cosy the coefficients will recur in the order + cosy, - sin y, - cosy, + siny, and (402) will give X X2 X3 cos(y + ) = cosy - siny 1 -cosy.2 + sin y 12 +&c. (404) If now we put y = 0 in (403) and (404), sin y = 0, cos y = 1, tht alternate terms of the series vanish, and we have X X3 X5 X7 sin x = T - 123 + 1'234-5 - 12-3-4567 + &c (405 X2 X4 X6 cos x = 1 - 2 + 1 4 123456 + &c. (406) It may be observed that (406) can be deduced from (405) by dif. ferentiation. 208. The series (405) and (406) are directly available for the construction of the trigonometric table. For this purpose x in the series must be expressed in are, since (361) and (362), upon which the pre ceding demonstration rests, require x to be in are, Art. 9. EXAMPLE. Find cos. 10~. Reducing 10~ to arc, by Art. 9, we have x = 10 x.01745329 =.1745329 and computing separately the positive and negative terms of (406), X2 1-=1 - 12 = -.01523086 4 s6.23 —4 -.00003866 -. -.00000004 1.2.3.4 1...6 1.00003866 -.01523090 -.01523090 cos 10~ =.98480776 agreeing with the tables, which give.9848078. The student may, for practice, verify any other sine or cosine of his table TRIGONOMETRIC SERIES. 117 209. To develop tan x in terms of x. Representing the coefficients in the series (405) and (406) by letters, we have x - ax' - a, x' - a, x' + &c. tan X _ (407 -1 - a, xa 4- a, x' - a, x + &c. 1 1 In which a, -- a, = -2 &c. 1' 2 1&2 c. If we perform the division of the numerator by the denominator, we perceive that the result will be a series containing only odd powers of x, and commencing with the term x. But as the law for the successive formation of the coefficients is not easily shown in this way, we shall resort to the following process. Assume the series to be tan x = c, x +- c, x' + c x + &c. () and differentiate it; we find, by (363), after dividing by dx, 1 + tan' x = c, + 3 c, xz + 5 c, x' + &c. or, since from the division of (407) we know that c, = 1, tan2 x = 3ca2 + 5 c, x' + 7 c, x + 9 c,z 8+ &. (n) The square of (m) is tan'z x= x2+, x' -, c', c x at c,+ C C + C, &c. + c, e, c + C, c, +. c + &c. +c,, + c, c, + &c. + C, c, + &c. which compared with (n) gives 1 c, = C, c, es (Cs Ce + C.C,) c = -5 (c, c, + c, c,) c,= - (C, c, + C, c, + c, c,) 1 Ca= - (c, c, + C, C, + C, c, + -, C) &c. &c. where the law of derivation is obvious. We have preserved the factor c,, although it is equal to unity, in order to render this law more apparent. Since the first and last terms of these expressions are equal, as also the terma equally distant from them, we may write them as follows: c,-= 1 *1 cs = 3 (c, ct) c,= 6 (2, ac,) = - (2 c, c, +, c,) el = 9 (2 C, c, + 2 c,, + c, c,) &c. &c. 118 PLANE TRIGONOMETRY. n in which form any coefficient c,, +, when n is even, is expressed by - terms all ol 2 whose coefficients are = 2; and when n is odd, by 2 terms all of whose coefficients are 2 except the last, which is 1.* If we now substitute the value of c, - 1, and deduce the numerical values of the coefficients successively, we shall find x' 2 x' 17 x7 62 x' 1382 x" tan z -= =.+ + + 3.57 + 3 3.5.79 &c. (408) 210. To develop cot x zn terms of x. If we invert (407) we have 1 - a, x ~- a, x4 - &c. cot x = - (409) x - a, x + -a, X - & 1 and the first term of the actual division is -, the second term - (a, - a,) x, and x the succeeding terms evidently involve only the odd powers of x. Therefore let 1 cot x = - - d x -d- d, x - &c. (o) x The coefficients cannot be determined by the method of the preceding article in consequence of the negative exponent in the first term; but they are directly deducible from those of the series for tan x. We have by (142) tan x = cot x - 2 cot 2x (p) Now the series (o) being true for any value of x will give cot 2 x by substituting 2 z for x, whence 1 2 cot 2 x -- - 23 d x - 24 d3 x -2 2' d,z' - &c. x Subtracting this from (o) we have by (p) tan x == (23- 1) d,x + (24 - 1) d, z + (2' - 1) d, xz + &c. Designating the coefficients of (408) by c,, c,, c,, &c. we have also tan x = c, x - Cx a - + C, ' +- & and the comparison of these two values of tan x gives C, C, __ C, = 2- 1 =(2 - 1) (2+ 1) 1 3, C, C, __ C 2' - 1 (2 —1) (2-+ 1) 3-5 c, - c, Cs 28- 1 (23-1) (23+ l) 7-9 &c. &c. 2n+, __ * Euler, and after him Cagnoli and others, make these coefficients depend upon those of the series sin x and cos x, but the number of given quantities by which each coefficient is expressed is double the number required in the method of the text TRIGONOMETRIC SERIES. 119 Substituting the values from (408) 1 2 C, = 1 C, =, -- 8 &c. and reducing the coefficients to their simplest forms, we find the series (o) to be 1 x x3 2 xz zx 2 x' cot x 3 3. - 3. - 3 -5j9.11 -&c. (410) cot X = - - - - - 3357. x 3 3aA5 33-5-7 33.7 '7 33'5'7'9'11 211. By a process similar to that of Art. 209, but which we leave to the student, we find X 5 x' 61 x6 277 z' sec x =- 1 2 + 2a3 + - 235 23.7 + &c. (411) And from (408) and (410) by means of the formula cosec x = Y (cot ~ x +4 tan j x) we find 1 x 7 x3 31 x' 127 x' cosec xz = -+ 2 + ' 4 5+ 3 23. 7 235 7 + + &c. (4122\ 212. To develop sin-1 y in terms of y. (See Art. 87). Let x = sin-'y (or sin x= y); then by (373) dy - (1 - y2) Developing the second member by the Binomial Theorem, dx 1P3 1-3-5 1+ 21y2 + 13 y4 1 35 y6 & (m) 2.4+2, 4.6 +&c. (?n) As this contains only even powers of y, the series from which it would be obtained by differentiation must contain only odd powers of y; therefore, let x == ay + ya3y3 a5 +5 a7y7 + &c. (n) There will be no term independent of y if we limit x to values between 0 and -4 900, for then when y = 0 we must also have x = 0.* Differentiating, we have dx dy - al + 3 ay2 + 5 ay4 + 7 a7y6 + &c. which compared with (m) gives 1 1.3 1-3-5 al= 1 a3 = 5a5 2-4 7a7= 246 &c. * The series (413) obtained under this limitation expresses but one of the values of sin-'y, but if we denote the series by s, we shall have by (95) the following expression, including all the values, sin-' y n 7r 4 (- l)s n being an integer, positive or negative, or zero. 120 PLANE TRIGONOMETRY. therefore (n) becomes 1 y3 1'3 ys 1'3'5 y' x —sin -y=y + g 3+ 2.4 5 +2 -7 +&c (413) It is unnecessary to develop cos-ly since we have 7T cos-y = -2 sin-'y 213. To develop tan- y. Let = tan- y, then by (375) dx( d - (1 + y2)-1 = 1 -y2 + y4- y6 + &c. (m) from which we infer, as in the preceding problem, that the required series contains only odd powers of y; therefore let x = aly + ay3 + a5y5 + ay7 + &c. (n) then d =al + 3 y2 + 5 a5y4 + 7 a7y6 + &c. which, compared with (m), gives a = 1 3 =- 1 5a =1 7a7=- 1 &c. so that the series is x == tan- y= y -- ^y3 + y5 _ ~ Y7 + &c. (414) 214. To compute the ratio (= r) of the circumference of a circle to its diameter. We have heretofore assumed this ratio to be known from geometry, where it is found by means of circumscribed and inscribed polygons which are made to differ from the circle by as small a quantity as we please; but (414) enables us to express its value in a series. We have tan 1, therefore if we make y = 1 in (414) we have n 1 1 1 1 w__1 - + -&c. (415) 4-=1 — I + 5 - 7 + - -&c. (115) But this series converges too slowly to be of any use. To obtain a rapidly converging series ymust be a small fraction. We might employ tan -= _ (Art. 29), but in consequence of the radical, it is 6 ~/ 3 TRIGONOMETRIC SERIES. 121 simpler to resolve 4 into two or more arcs whose tangents are known, and to compute the value of each of these arcs by the series. To effect this let 71 -tan- tan a tn- t' (416 then by (123) t+ t tan — 1 tt 1 —t whence t' t (417) 1 + t from which, assuming any value of t at pleasure, the corresponding value of t' is found. If we take t =, we find t' = -; therefore by (416) and (414) - tan-l 1 + tan-'1 4 = 3.14159 more accurately 3.14159 26535 897931 If we take t we find t but the abe serupposition is 4=.636476 +.3217506 =.7853982 4 7r = 3.14159 more accurately 7r = 3.14159 26535 89793 If we take t 4 we find t' 3 but the above supposition is evidently the best adapted for rendering both series sufficiently converg ent.* 215. To resolve sin x and cos x into factors. The series (405) shows that x is a factor of sin x, and gives sin x =x (1- 123 + 1 2345-&c) * See NOTE at the end of thus chapter, p. 124. L 16 122 PLANE TRIGONOMETRY. and the factors of the series within the parenthesis must evidently be of the form X2 x1-A- (q) A being a constant, but having a different value in each factor. The required factors must be such as to reduce the second member of (p) to zero whenever the first member is zero. Now sin z is zero for the value x = 0, whence x is a factor as already seen, and also for x = =t n r, n being any integer; therefore the general value of (q) is 1 Awhence A =- n2 v which, substituted in (q), gives as the general factor 1 X Making n successively = 1, 2, 3' &c., the equation (p) becomes therefore sin x=x( 1 1-) _. )(1 3 i )* (419) The factors of cos x in (406) must also be of the form (q); but cos x is zero for z =_ f (2 n + 1) —, n being any integer or zero, and the general value of (q) is 1 (2n+-1)7 0 4A.2a whence A (2n+ 1) —r 22 which, substituted in (q), gives the general factor 2a2 x (2n + 1)2 Making n successively - 0, 1, 2, 3, &c., we have COS X (1 _s x) (1 32 xa ( 5a..* (420) 216. Logarithmic sines and cosines. By means of (419) and (420) the logarithmic sines and cosines of the tables are readily computed. Put x = m 2, then i2 -) A1 4a A1 6) *n sin m cos m - ) 5 * * and taking the logarithms log sin =log + log log 1- -) + log (1 + l n o+l log ( + log (1- ) +log (1 ) TRIGONOMETRIC SERIES. 123 Developing these logs. by the known formula log (1 -) - n - A + - n + 1 n3 4- &c.) (in which M = modulus of common logs.) and arranging according to the powers ef m, we have mx 7 log sin -- log - + log m.l / 1 1 T ' i + l +0 +&e' 4Ii1 1 11 - &c. By summing the constant numerical series, and substituting the value of the modulus Al = -43429 44819 and also of 2 these formula become log sin = 10 19611 98770 + log m -- &C. By summing the constant numerical series, and substituting the value of the modulus M -- -43429 44819 and also of 2' these formulse become log sin -~- 10.19611 98770 q- log m - m' X 0-17859 64471 - m4 X 0-0146889690 - m6 X 0-0023011796 - nw X 0'0004258450 - m'~ X 0 00008 49075 - mr' X 0-00001 76758 -- m" X 000000 37870 - ml" X 0-00000 08284 - m8 X 0-00000 01841 - &c. (421) log cos - = 10 - mn X 0-53578 93412 - m' X 0-22033 45350 - mn X 0-14497 43131 - in X 0-10859 04688 - mn' X 008686 03766 -- m'2 X 0-07238 25502 - mn" X 0-06204 20818 -- nm' X 0-05428 68115 - m'8 X 0-04825 49426 - &c. (422; In these expressions 10 is added to render the logarithms positive, as is usual in the tables.* * See the preface to Callet's Tables, for the coefficients of these series carried to 20 decimal places, and for other forms given them by which they are rendered still more convenient. 124 PPLANE TRIGONOMETRY. EXAIMPLE. Compute log sin 9~. We have 1 m X 90~ = 9~ m log m- =- and therefore by (421) log sin 9~ = 10-19611 98770 - 1 -- 000178 59645 - 00000 14689 - 000000 00023 - 10-19611 98770 - 100178 74357 log sin 90 ~ 919433 24413 217. If in (419) we put x - we have zsin I-12 /4(-1 I 16% 2 V 22 ( 42 6* - (2- 1)(2+(1) ( (1)(4 1) (6-1)(6+1)... 2 2. 2. 4. 4. 6. 6.. n r 2 2 4 4 6 6 hence 2 1 3 3 5 7 (423 which is Wallis's expression of sr. NOTE to page 121. Computation of vr. Many other series besides those of Art. 214, may be given for computing nr. One method of obtaining them is to resolve tan-x t and tan-' t' into two others, and thus make i 7r to depend upon three or more arcs. From (194) we easily deduce 1 ~1 n tan-' - tan-' -- tan-' (a) m m + n m'-+ m n —1 1 1 n tan-' - = tan-' - - tan-' (b) m m -n m -m n+1 - in which m being given, n may be assumed at pleasure. The numerators of the fractions in the last terms will reduce to unity when m2 + 1 is divisible by n; if therefore we assume n and p so as to satisfy the condition np = m + 1 (c) we shall have 1 _ 1 1 tan-' - tan-' - - tan-' - a m m Jr- n m+n - 1 1 tan-1 - = tan' -- - tan-' (t) m m - n p- m TRIGONOMETRIC SERIES. 125 For example, let m = 3; then ma + 1 = 10 = 1 X 10 = 2 X 5, so that we may take n = 1, p - 10; or n = 2, p = 5, whence by (d) and (e) 1 1 1 tan-' tan-'+ tan-' 1 1 = tan- - tan -' I 1 = tan-' - + tan-l' Substituting in (418) 1 1 1 - = tan-' - + tan-' + tan-' 1 1 1 = 2 tan- -- tan-' - I 7 2 tan-' 1 + tan-1 () 1 1 1 = tan-' -- + n- tan- tn-' (g) The equation (/) was employed by CLATJSEN of Germany, in computing T to 200 decimal places, and (g) was employed by DASE, also of Germany, in computing 7r to the same number of figures. These computations were carried on independently of each other, and the results when communicated to SCHUMIACHER, (who gives them in the Astronomische Nachrichten, No. 589), were found to agree to the last figure They prove the value previously found by Mr. Rutherford to be erroneous beyond the 150th figure. By means of the formulae (a), (b), (c), (d) and (e) we may again subdivide the arcs as often as we please. Thus, it is easy to deduce 1 1 1 = 2 tan-' + tan-'1 + 2 tan-' 2 tan-' + tan-' - + tan-' + tan-' 5 4 7 268 1 1 1 1 =4 tan-' - - tan- ' + tan-' - + tan-' 268 - 4 tan-' ' tan"-' + tan-' 26 1 1 4 tan-' -tan-'' a o 239 which last is known as liachin's formula. In deducing it we have reduced the differnmce of two arcs to a single arc by means of formula (a). Another method is, to find by trial, or otherwise, an arc a multiple of which is nearly equal to 4, and whose cotangent is a whole number; and then deduce the L2 t26 PLANE TRIGONOMETRY. difference between this multiple and -. Thus it is known (from the trigonometri tables) that cot 11~ 16' - 6 nearly; therefore by the last formula of Art. 79, putting tan x, 1 120 4 ttan -'tan 11 and by (194) 120 ~ 120 1 tan-' - = t an-' - tan-' 1 tan-' 119 4 119 239 therefore 1 1 4 tan-' - tan-' 4 6i 239 as was found above. If we resolve tan-'- by means of (c), (d) and (e), we have m = 239, m + 1 = 57122 = 213' = np, which offers several suppositions for n and p; if we take n = 13 =- 169 andp = 2-13 =- 338, we find by (e) 1 1 1 - 4 tan-' — tan-' -+ tan-' 4 T_' 50 -- which was employed by Rutherford. If we take n = 1, p = 67122, we find by (d) 1 - 1 1 V — 4 tan-' I - tanm- __ - tau_, 4 w 6 240 - -5 EXPONENTIAL FORMUL.E. 127 CHAPTER XIV. EXPONENTIAL FORMUL2E. TRINOMIAL OR QUADRATIC FACTORS. 218. To demonstrate Euler's formulce cos x =- (e "/- + e- -1) (424) sin x — 1 (e/-1 e-z 1) (425) in which e is the Naperian base of logarithms, or, 1 1 1 e =l + + 123 + &c. It is shown in the theory of logarithms that x 12 x3 x4 ex 1 -+ ()+ (+ ( )+ &c. (426) (1) (2 (3) (4) wheve for brevity we write (1) =1 (2)== 1.2 (3)= 1.2.3, &c. We have by (405) and (406), employing the above notation, X2 X4 X6 cos X - 1 + $-+&c. x X3 x5 x7 sin x= (1) (3) + (5) (7) + &C. the terms of which are the same as those of (426), but with alternate signs. If the signs in these two series were all positive, the sum of the two would be equal to (426); and it is evident that we shall make them positive by substituting 2 =- z2 or x == z -1 which gives z2 Z4 Z6 cosx=1 + + + + &cO s-1 (2) + (+) + () & + i2 44 +6 sin x =z s/ -- 11 ' - -- '-. &C. (3-) + + (7-) 128 PLANE TRIGONOMETRY. o1. _: Z Z. Z5,Z 2o sin x- = (1) + (3 (5) ( + (7) + &C. whence ~1 X ~Z Z2 Z3 cosx + V — 1sin x = 1 + ) + 2) +- + &c. e' (1) (2) (3) But 1 -- 1 x -x 1 V"~ - — =-i-/, V-=-V -/ therefore cos x - v -1 sin x = e-xf-l (427) If in this equation we substitute - x for x, we have, by (56), cosx + / - 1 sin x = e v- (428) The sum and difference of these equations are 2 cos x = e '-1 + e-"z -1 (429) 2 V - 1 sin x = ex -- - e- v-l (430) whence (424) and (425). 219. The quotient of (430) divided by (429) is eX-1 - e-x/-i e2a/-i - 1 V/ - 1 tan x-= (431) exr'-: + e — /'-1 e2 ' '-1 + 1 220. If we put y= el-1 = cosx + - 1 sin x (432) we have y-= e- -~1 = cos x - V - 1 sin x (433) and (429) and (430) become 2 cos x = y + y-' (434) 2 -/ - 1 sin x = y - y-1 (435) If mx be substituted for x in these formulae, we have ymn = em v-1 = cos mx +/ V- 1 sin mx (436) y-m = e-mxv -1 = cos mx — V - 1 sin mx (437) 2 cos mx = ym + y-m (438) 2 / - ism mx = yM - y-" (439) EXPONENTIAL FORMULAE. 129 221. Moivre's Formula. The value of ym from (432), compared with (436) gives (cos x + V - 1 sin x)m= cos mx + - 1 sin mx (440) which is Moivre's Formula. It shows that the involution of the expression cos x + / - 1 sin x is effected by the multiplication of the angle. Again, if we multiply (432) by cos x' + /V- 1 sin x' — e' -- we have (cos x + - 1 sin x) (cos x' + V - 1 sin x') - e (=+x'). I cos (x + x') + V/ - 1 sin (x + x') which shows that factors of this form are multiplied by the additioi. of the angles. We have also (cosx+ / — sinx) (cosx —/-l sin x)=cos2x+sin2x=eo= 1 (441) 222. Generalform of JMoivre's Formula. As long as m is an integer, both members of (440) can have but one value; but if m -= P the first member becomes _p (cos - / - 1 sin x) ' = -/ (cos x -/ -1 sin x)P which has q different values* in consequence of the radical of the degree q, while the second member cos P x + - -1 sin — x (a q q has but one value. In order that both members may have the same generality, as should be the case with every analytical expression, it is necessary to suppose that we take for the arc x not merely the arc less than the circumference which has the given sine and cosine, but also all the arcs which have the same sine and cosine; that is, c denoting the circumference, all the arcs - C, x - 2, x + 3 c, &c. Now there is an infinite number of these arcs, but only q of them can give different values to (a); for all the values of the arc in (a) will be P 2 Pc p 2pc P (q- 1)pC ix, X+-, x+.....e.x+., q q q q q q q P x + P + - l)PC, &c...... &C. g g q q * That is q values real and imaginary; thus it is shown in algebra th:t +/,.= + a and-a; /aa-=+a, a(-1+ 3) and a ( —~j'/ ), /a' —+a, - a, - a /-1, - a /- -1; &c. 1" 130 PLANE TRIGONOMETRY. But -P x + -- -P x + pc has the same sign and cosine as - x; q q q q P __ _ 4- 1) P P.P, P pC x J? — ) -_ ( -- x +- ) + pc the same sine and cosine as - x 4- -, &c.; q q (r 4' <? <? so that after the first q terms of the above series, the same values of the sine and cosine return ad infinitum. Representing, therefore, the circumference by 2 sr, the equation is entirely general under the form (cos x +- - sinx) = cos P (2 n ax)+V-lsin (2 n +x) (442) q q in which n is any number of the series 0, 1, 2, 3.....q - 1. 223. Trigonometric expressions of the real and imaginary roots of unity. If x = 0 in (442) it gives (1) ~_ = cos P 2 n r+ /- 1 sin - 2 nr (443) q q or (1)" = cos 2 mn7r-/-l sin 2 mnnr (444) m being fractional or integral. If p = 1, (443) gives 2n r 2nsr / 1 = cos — + / -1 sin — t445) which expresses the q roots of unity by making n successively 0, 1, 2, 3... q - 3 For example, let q = 4, (445) gives for n = 0, /1 = cos 0 + - 1 sin 0 = 1 n- =, 4/1 = cos — + /- 1 sin - -1 n = 2, 1 = cos - 1 sin r - 1 n = 3, 1 = cos - + - sin - - Cs 2 as found in algebra. Tf x = - in (442), it gives m/ ^ m(4 n + 1) Jr sinm (4ln + 1) 7r (v'- 1)~ = cos - + v- 1 si 2 (446) (V~l~m~cos 2 2 which shows that an imaginary term of any degree can be reduced to a binomial of the form A + B / - 1. If x = 7r in (442) we find (- 1)' = cos m (2 n + 1) rr - / — 1 sin m (2 n + 1) (447) 224. To reduce an imaginary quantity of the form (a + b / - 1)" to the frms A + B./ /- 1. Let k and x be determined from the equations k cosx = a, ksinx-= b oy Art. 174; then, by Moivre's Formula, (a + b /- 1)m = km (cos x + / -1 sin x)" k" (cos mx +- - 1 sin mx) and putting A = k" cos mx, B = k" sin mx, (a+ b /- 1)m = A B - TRINOMIAiL OR QUADRATIC FACTORS. 131 TRINOMIAL OR QUADRATIC FACTORS. 225. To find the quadratic (trinomial) factors of the expression z"m - 2 z cos - + 1; m being integral. By (438) and (434) we have ya; - 2 ym cos mx - 1 = 0 y2 -2y cosx + 1 =-0 Therefore if we put y = z, mx = 2 n 7r + 0, or x = -, we have m z2" - 2z" cos + 1 = 0 (448) z' -2z cos 2n 1 = 0 (449) m As these two equations exist at the same time, they have common roots, and the second is therefore a divisor or factor of the first; but this factor has m values in consequence of the m values of cos + - (Art. 222), found by making m n = 0, 1, 2, 3... m - 1. Therefore the m quadratic factors of (448) are all ex pressed by (449), and we have e" - 2zm c + 1 ( 2 z Cos + ) X (z — 2 cos....- t 1) X (z- 2 z cos r.-+- +1) x... X (z'-2zcos2(m -1) ++ l 1) (450) 226. To obtain the simple factors of (448), we have only to find the two simple factors of each of the quadratic factors in (450), or to find the two factors of the general quadratic (449). Now, by the theory of equations, if z, and za are the two roots of (449), the first member is equal to (z - z,) (z - Z,) but we have by (432) 2 n n-. 2nr+- p z = y = cos x +- /- 1 sin x = cos +- + /- 1 sin - ' ' m ' ' m which gives the two values of z by the double sign belonging to / - 1. Therefore the simple factors of (448) are all included in the form ( 2nmr+-. n2+\ z- cos - v/- 1 sin - 1 I~~~~~L nt~~~~~/ (451) 132 PLANE TRIGONOMETRY EXAMPLES. 1. Find the quadratic and simple factors of z' -2 z + 1 Here m =2, 2 cos == 2, cos = 1, = 0; and by (450), z' 2 z -+ = (z - 2 z cos 0 + 1) (z -2 z cos + 1) = (z —2z+1) (z+ 2z+ 1) by (451) [z- (cos 0 +- V - 1 sin 0)] X [z- (cos 0 - -/ - 1 sin 0)] X [z - (cos 7r +- / - 1 sin v)] X [z - (cos - /- 1 sin r)] ( —1) (z- 1) (z + 1) (z+ 1) 2. Find the factors of z' + 2 z' + 1. Here m = 2, 2 cos 0 = -2, -_, and 4 + 22 -+ 1 - (zq + 1) (z + 1) = ( -/-1) (z+ /-1) (z / —1)(z +/-1) 3. Find the factors of Z4 - z' + 1. 4 - z' + 1 = (z - 2 z os 30~ + 1) (z2 + 2 z os 300 + 1) = (z - z V 3+ 1) (z+ z / 3 8+ 1) = (z - / 3- Z - ) (z - 3 V + V —1) X (Z+ - /3+ - 1) (z - 2 /3 I / -1) 4. Find the factors of z6 - 2 z' + 1. - 2z4 1 (' -2z - 1) (z' z — 1) (z+ z- 1) =- (z - 1)" (z + + - / - 3)2 (z - + V/ - 8)' 227. To find the quadratic factors of zm - 1 when m is odd. In (450) let q = 0, it becomes (z —1) _ (z-1l) X ( z-2zcos + 1 ) X ( z-2z cos + 1 X.. X ( -- 2zcos -2(m 1+ 1) (452) N'ow m being odd, m - 1 is even, and the number of trinomial factors in (452) 5.xclusive of (z - 1)2, is even; but cos 2 --- 1) cos 2 - CO 2 m \ m / rn so that the first and last of these factors are equal. In the same manner it is shovwn that any two of these factors equally distant from the first and last are equal, TRINOMIAL OR QUADRATIC FACTORS. 133 therefore, uniting these equal factors and extracting the square root of both members, we have, when m is odd, m- 1 (z - 1) X ( z -2 z cos 2- + ) X (z — 2zcos -- +1 ) X (- 2 z cos (m- )7+ (453 228. To find the quadraticfactors of zn - 1, when m is even. When m is even, m - 1 is odd, the number of factors in (452), exclusive of (z - 1)', is odd, and the middle factor will not combine with any other. This factor is the ( ) and contains 2 ( ) cos - cos - 1 m and is therefore equal to 2 + 2 z + 1 = (Z + 1)2 so that uniting the remaining factors, and extracting the square root, we have, when n is even, 2 —1 -= (- 1) (Z+ 1) X ( -2 zos - + 1) X (z —2zcos 4 -+ 1) X..*. X (z-2z cos (m 2)+ )r (454) 229. To find the factors of zm + 1, when m is odd. In (450) let 0 = ar, it gives (m+ 1)' = ( - 2 z cos - + 1) X (z- 2z cos-+ 1). m X,.. X (zo -2z co(2s -1) + 1) m and it is easily shown, as in the preceding articles, that the factors equally distant from the first and last are equal, and that the middle term is z + -2 z + 1 = (z + 1)". M 134 PLANE TRIGONOMETRY. Hence we find, when m is odd, sm + 1 == (z + 1) X ( -2 z cos71- 1) X - 2z2 cos -- + ) m X... X - 2 z cos (m ) (455 230. To find the factors of zm + 1, when m is even. The same process gives zm" 1 (z'- 2z cos +- 1) m X (2 — 2 cos — + 1 X. *.. x. X ( -2z cos 'm +- 1) (456) 231. The simple factors of (453) and (454) are obtained from (451) by putting ~ = 0, and those of (455) and (456) by putting s =- r. There will be found pairs of equal factors as in the preceding articles, but all the different simple factors will be found by taking only the positive sign of the radical 4 - 1. 232. Any function of the form zm -2p zm + q may also be resolved into quadratic factors. It is only necessary to reduce it to one of the preceding forms. By resolving the equation 2m - 2p zm q = (457) we shall find from its two values of zm z-m2p zm+q (-m (p + Vp q)) X (zt-P (p-V - )) and if we put the absolute term in one of these factors == am (according to its sign) it becomes zm =am am m - ) am (z'm z 1) in which z = az', and the factors of this last expression may be found by one of the preceding articles. If, however, the values of zm in (457) are imaginary, i. e. if p2 < q, this method fails to discover the real quadratic factors, and we must proceed as follows. Put q - an, then the proposed function becomes m 2 — P _ 1 _am (iZms p. m + 1 am a —a am.+) a -- —.z in which z = az'; and since in the present case p < a"m, is a proper fraction, and we may put P = cos 0, which reduces the given function to the foim (450) am MULTIPLE ANGLES. 135 CHAPTER XV. TRIGONOMETRIC SERIES CONTINUED. MULTIPLE ANGLES. 233, THE true developments of sin mx and cos mx in series, when m is not restricted to integral values, were first obtained by Poinsot, and form the subject of a memoir read by him before the French Academy of Sciences, in 1823.* The following problem is the basis of these investigations. 234. To develop (k -- v/k- 1) 1, in a series of ascending powers of k. Let z = (k +- /k-l)m (a) and assume z = A- + At k + A, k - AkS... + An kn.,.. { Differentiating (a) and putting dz dk we find ~-' = (m ( -k-l) X (1 + / ) -= Xm z the square of which gives m z - ( - 1) z = 0 Differentiating this and putting dz' dk we find, after dividing by z', m z - kz' — (k- - )z" = O (d) Again, differentiating (b) twice, we find, z' = A, + 2A, Ak- + 3 A. k.... + nA 1 —. z" = 1.2A, + 2.3 A, k+ 3.4A,k... + (n - 1) nAnk k —. ') Substituting in (d) the values of z, z', z", given by (b) and (e), we have D = mAo + 2A, t+ Pm A,.. -.. + -m1 An k. --- A -- 2 A,... -- n An -1.2 A... - (n - 1nA... 4-1.2A, +2.3A,' +-3.4A.. - (n+- 1) (n + 2) A,,.... mn which each of the coefficients of the powers of k must be zero. To discover the aw which governs these coefficients, it will suffice to examine that of the general;erm, or the coefficient of kn, which is (m' - n) An + (n + 1) (n + 2) A,+ =0 whence m'm - n' A (n 1) (n+2) n * See the published memoir, " Recherches sur l'Analyse des Sections Angulaires.' 'aris, 1825 [3,j6 ~ PLANE TRIGONOMETRY. so that frem the first coefficient, A,, we find by making n = 0, 2, 4, 6, &o., ms 1 "2 m - 22 mA (m2 - 22) ~A4 - Aa - 34 -- m - 4 m (in2 - 22) (m) - 42). A,. - A, -- 5-6 1'2'123456 4 &c. and from the second coefficient, A,, we find by making n = 1, 3, 5, &c. A?- a 1A A, _ - 3A (M A. 4-5 2 3.4.5 i2 - 5, (m2 - 12) (m2 - 38) (m - 52) A~ 6-7 A= 2-3-4-5-6-7 52- A &c. Therefore, if we put m2 k m (m 2- 22) m2 (mln- 22) (m2 —4 k4) =1 T- -2 + 172' 3) k4 12.346 — 6 - + c. m23 1 (am - 12) (m - 83) k c. K' —k - 2- k +; —4. 2'3 2'3'4'5 the equation (b) becomes z AoK+ A, K' and it only remains to find Ao and A,. In (a), (b), (c) and (e), put k = 0; we find z = (v/- 1)" = Ao ' = m (/- 1) -' = Al Therefore we have, finally, z = (k + / k2- )m = (V1 - 1)" + (/ - )1)"-1 m K' (458) 235. To develop (/ 1 - h' + h - 1)" in a series of ascending powers of h. We nave (V1 - h2 + h / - 1)" =( - 1)m (h + / Ah - 1) therefore by (458), exchanging k for h, (V1 - h' + /-1)" (V m [(V -_ 1)m. i+ (V/_ l)m-' mH'] in which H and T' are what K and K' become when h is put for k. Combining the imaginary factors in the second member, observing that (v- 1)" x (/ - ')Im = (,/ 1)m = (1); MULTIPLE ANGLES. 137 (which must not be put equal to unity, since m may be a fraction, and unity has imaginary roots,) and also that nm-( (/- 1) X (v-1)"'- V - 1 (v/- 1)-' X (/ —1)"- ' =_ 1 (1) we have ( -h2 + h -/- 1)"' =(1) H' - Jd - 1 (1) m H' (459) in which H_-l m1 h2 m (-2) h4 &e. 12- 1.2.3-4 h m 1 (7n - 12 (1n) (m - 3) h- &c. H' ~ h-&C. 2.- 3 2.34.5 236. To develop the sine and cosine of the multiple angle in a series of ascending powers of the cosine of the simple angle. When mn is an integer, this problem requires us simply to develop sin mx and cos mx in a series of powers of cos x; but when m is a fraction - -, the angle mx has q values which have the same sine and cosine, (Art. 222), if we consider x tc represent all the angles which have the same sine and cosine as the simple angle. We shall therefore employ Moivre's Formula in its general form (442), or (cos x 4- ' - 1 sin x)m = cos m (2 n 7r - x) +- / - 1 sin m (2 n t -+- x) Putting k = cos x we have by (458) and (446), (cos x ~+ /- lsin )m- = (k + - // k 1) )m = ( -1) K4- (- 1),- m K' = cos(? (4n + I ) J. K + — l sin (I m - + ) n ) X +cos (( -- 1)( n'.m / m — Sin(( — ) (4 n+ 1) ).K' Comparing the real and imaginary terms of these two values of (cos x +/- 1 sin x)v. we have cos m (2n v + x) = cos( -(4 n — )~ ). KX+ cos ((m-i) (4n' +1) 7) m K' 2 m 2 sinm (2n + x) = sin (m(4n - +1). K sin ((nm-1) (4 n'- + 1) r) If m is a fraction= -, each member of these equations receives q values by taking successively for n, or n', the numbers of the series 0, 1, 2, 3,... - 1; but we are now to show what values of n and n' correspond to each other in the two members. Let x- 2- then ~ 0, K = 1, K'- O, and we have 2' m (4n+ 1) 1 m (4 n' + 1) ) 2 2 Sn (4 nq- 1) - sn m (4 n'- 1) r sin sin 18 M2 138 PLANE TRIGONOMETRY. therefore these two angles can only differ by some multiple of 2 ar, or we must have m (4 n + 1) r m (4n' + 1)+ 2 n -- -- 2- k 2 n" ' 2 2 whence m (n - n') = n" but m being a fraction P, and n, n' numbers of the series 0, 1, 2,... q - 1, we q cannot have m (n - n') equal to an integer n", unless it is zero;* therefore n - n' = 0, n = n' and the above developments are cos m (2 n=r + x)=cos m (4n- ) T). K+cos((m-1)(4nl) ). mK (4 sil m (2 n 7r + x)=sin (m (4 n + 1) )K ((m-1) (4n 1 mK (461) in which m1 m2 (m - 2) cos4x-&c K -- I -- cos x - +'' - &C 1-2 1-2-3-4 i — 1* (m ' - 1) (m' - 3!) K' = cosx- 23 cos3 x- (X 23 COS' - & It hence appears that, in general, it requires the combination of two series to express the cosine and sine of a multiple angle in powers of the cosine of the simple angle, when m is fractional. 237. When m is an integer, one of the terms of (460) and (461) will always become zero, and we shall have but a single series to express the function of the multiple angle. The first members become in all cases cos (2 mn r + mx) = cos mx sin (2 mn Tr - mx) = sin mx and the second members vary according to the form of m. In (460), if m = 4 m', cos mx -= K m = 4 m' 4- 1, cos mx = (mK' m = 4 m' + 2, cos mx - K m = 4 m' ~- 3, cos mx =- mK' J and since when m is even, the series K terminates, and when m is odd, the series K' terminates, these four equations are all finite expressions, and will give the equations nf Art. 76, by making m = 1, 2, 3, &c. In (461), if m = 4 m', sin mx = - mK m = 4 m' - 1, sin mx = m = 4 m' - 2, sin mx = miK' m = 4 m' 4- 3, sin mx = - K * Since - is supposed to be reduced to its lowest terms, p and q are prime to each q. p (n -n') other, tnerefore, if - ( ) is not zero, q must divide n - n'; which is impossible, since the greatest value of either n or n' is q - 1. MULTIPLE ANGLES. 139 In these fcrmulse, however, the series do not termir. te, but by differentiating (162) we find for 2 __ 2a m = 4m', sin nx=- m sin x (co - os3 z + &c.) m = 4 m' -+1, sin nx = sinx (1 - cosa x + &c.) * (46s m 22a ms = 4 m'+- 2, sin mx = m sin x (cos x- 23 cos3 x - &c.) -- 12 m 4 m' +3, sin mx = - sin x (1 - 1' cos2 x + &c.) all of which terminate and give the equations of Art. 75. 238. To develop the sine and cosine of the multiple angle in a series of ascending powers.f the sine of the simple angle. We take as before (cos x + V - 1 sin x)m = cos m (2 nzr - x)+ / —lsin m (2 nz + z) Putting h = sin x, we have, by (459) and (444), (cos x + / - 1 sin x)^ = (/1 -Ah + Ah / - )m = (1) Ha+ V/ -- (1) - m' = cos mn'tr. H+ V /- 1 sin mn'r. H +- /-1 cos (m - 1) n' 7. mi' - sin (m - 1) n' r. m J Comparing the real and imaginary terms of these equations, cos m (2nr -+ x) = cos mn'. H- sin (m — 1) n' T. mH' sin m (2 nr +- x) = sin mn'r 7 H - cos (m -1) n' 7. m7H' and to find what values of n and n' correspond, let x = 0, then h= sin x = 0, H = 1 IE' = 0, and we have cos 2mn 7r =0 cos mn' i sin 2 mn r = sin mn'mr from which we infer that 2 m nr = m n'r, or 2 n = n', and hence cos m (2nr +- x) = cos 2 mnz. Ir- sin 2 (m - 1) nz. mH' (464) sin m (2 nr -+ x) = sin 2 mn r. H4- cos 2 (m - 1) nT. mH' (465) in which m being a fraction =_ -, nis any number of the series 0, 1, 2, 3,... - -1; and m2 mi (m- 22) sin x — &. H =1 -- sin x + 1234 sin &c. ' =in -- I,2 (i n ~ - 12) (n2 - 3')., i' = sin x - 2-' sin'x+ - s &c 239. When m is an integer, the first members of (464) and (465) become cos ms tnd sin mx; and the coefficients of the second members zontain only multiples of 2 r-; therefore we have cos mx -= 1T sin mx = mH' But the series H terminates only when m is even, and the series H' only when m t 140 PLANE TRIGONOMETRY. odd, and we must also employ the derivatives of these equations to obtain finite expressions in all cases; thus we have also cdlI dH' sin mx = cos mx = - zclx dx Therefore differentiating the series H and H', we shall have, when m = 2 m', cos mx =1 - - sins x -+ &c. 1 (466) m = 2m' 4, cos mx = cosx(l- 12- sin2 x + &c.)a n = 2 m', sin mx = m cos x (sin x -- 2'- sin' x - &c.) p.~~~ ~ ' (467) m = 2 m'+ 1, sin mx = m (sin z 2- 3 sin2 x + &c.) all of which terminate, and give the equations of Arts. 77 and 78. 240. To develop the sine and cosine of the multiple angle in a series of ascending powers of the tangent of the simple angle. We have cos m (2 nr + x) - /- 1 sin m (2 n r q- x) = (cos x + V/ 1 sin x)m cosm x (1 -+ / - 1 tan x)" Expanding by the Binomial Theorem, and putting T=1 m (m-1) 2 m (m- 1) (m- 2) (m-3) tan T = 1 ta'xm2 tan( m2 -- ae. T' = m tan x - m tana3 x - &c. 1'2'3 We have cosm (2 nr - ) + /- 1 sin m (2 n - +x) - cosm x (T - -1 T') But the imaginary and real quantities are not yet distinctly separated in the second member, for m being fractional cosm x has a number of imaginary values. If we designate its real value by cos" x, all its values are included in the expression cos' x (1)m = cos" x (cos 2 mn'wr - + - 1 sin 2 mn'w) which, substituted above for cosm x gives cos m (2 nr —x) + / —1 sin m (2 nr +- x) -cosm x (cos 2 mn'w. T- sin 2 mn' r T') - V — 1 cosm x (sin 2 mna'. T + cos 2 mnn'. T') Comparing the real and imaginary terms, we now have cos m (2 nr - x) = cosm x (cos 2 mn'r. T — sin 2 mr;r. T') sin m (2 n r - x) = cos" x (sin 2 mn'r. T - cos 2 mn' 7r. T') and it is shown as in the preceding problems that n = n', whence cos m (2 nwr + x) = cos" x (cos 2 mnr. -- sin 2 mnwr. T') (468) sin m (2 n -r - x) = cosm x (sin 2 mnw. T- cos 2 mnr. T') (4691 MULTIPLE ANGLES. 141 in which m being a fraction = —, n is any number of the series, ), 1, 2,,.. - I; And cos'1 x denotes only the real value of./(cos x)p. 241. By the division of (469) by (468) tan 2 mnr c. T~+ 1' tan m (2 nr + x) = _tan 2 mn r. iT' (470) T- tan 2 mn r. T' 242. When m is an integer, both the series T and T' terminate, and in all cases cos 2 nn r =- 1, sin 2 mn -r = 0; and (468), (469) and (470) give' cos mx = cosm x. T (471) sin mx = cosm x. T' (472) tan mx = — (473) which last expression embraces all the equations of Art. 79.* 243. Before the memoir of Poinsot, developments were given for the multiple arcs in series of descending powers of the sine or cosine of the simple arc; but he has shown that these developments are impossible, except when m is integral, and in this case the series are the same as the preceding, with the terms written in inverse order. 244. To develop anypower of the cosine of the simple angle in a series of sines or cosines of the multiple angles, the cosine of the simple angle being positive. If y = cos x +- a/ 1 sin x, we have, by (434) and the Binomial Theorem. (2 cos x) = (y +- y —l)rn = ynm + ym-.+ n y(m-4 + &C. and by Moivre's Formula, ym = cos m (2 n r + x) + — 1 sin m (2 nr + x) mym- -2 mcos (m- 2) (2 n r -x) - m/ - 1 sin(m -2) (2 n + x) m(m -1) y_ m (r-i) (r-i) (2-Y 4- 2' - cos (m-4) (2 n +x)+m( 2 - 1-lsin(m-4)(2n +x) &c. &c. Therefore, if we put P+,,n- = cos m (2 n7r + x) + m cos (m -2) (2 nr +- x) - &c P'i,, +X = sin m (2 n r- + x) + n sin (m - 2) (2 n r + x) + &c. we have (2 cos x)m = Pn+x + V - 1 P' 2?21, (a) Now m being a fraction (2 cos x)m has imaginary values, but when cos x is positive, it will have at least one real positive value, and then (2 cos x)" being understood to lenote only this real value, all the values are included in the formula (2 cos x)m X (1)n" = (2 cos x)m (cos 2 mn'7r + / - 1 sin 2 mn'vr) Although the formulae for multiple angles require, in general, the combination ot two series when m is not an integer, yet there are certain cases, even when mn is a fraction, in which one or the other of the series will disappear. See the memoir ef?Poineot, cited at the beginning of this chapter. 142 PLANE TRIGONOMETRY. Therefore we have (2 cos x)- (cos 2 mn' - / - 1 sin 2 mn' ) = Pn2,,r + %/ - 1 aP ns+a Comparing the real and imaginary terms, (2 cos x)m cos 2mn'7r = P-n, +. (2 cos x)m sin 2 mn's = P',n, +X and to find the corresponding values of n and n', let x = 0, then (2 cos x)"' = 2m" and tie series become Pn,,,s cos 2 mn r (1 + m+ m ---( --- + &c.) cos 2 mnsr (1 + 1)" = 2m cos 2 mn r and in the same way P'ar = 2 m sin 2 mn r Therefore our formulas become 2m cos 2 mn' r = 2m cos 2 mn?r 2" sin 2 mn' rr = 2" sin 2 mn rr and as in former cases, it is shown that n = n', so that we have finally (2 cos x)m= P 2 + X (474) cos 2mn r (2 cos x)m = — in 2 - (475) sin 2 mu?r From this it appears that the real and positive value of (2 cos x)mmay be expressed either by a series of cosines or by one of sines of the multiple angles, and by comparing (474) and (475), we have the following constant relation between these series. P'an +x - sin 2 mn r Pnffi, cos 2mn 245. If n = 0, (474) gives (2 cos x)A=P; = cos mx + m cos (m-2) x + m ( ) cos (m- 4) x + &c. (476) which may be employed as the general development of the real value of (2 cos x)m, when x < 246. The same supposition of n = 0, gives sin 2 mn 7r = 0, and (475) give? therefore, 0 =P'-sin x + m sin (m - 2) x + 2 )2 sin (m- 4) x + &c. (477) e remarkable property of this series of sines of multiple arcs, which holds for al1 values of m, provided x < -. 247. To develop any power of the cosine of the simple angle in a series of sines or cosines vf ie?multiple a!itfles, i/e cusinle of the simple angle being negative. MULTIPLE ANGLES 143 If the denominator of v is even, there is no real value of (2 cos x)m when cos x is negative; but we may put (2 cos x)m = ( -2 cos x)'" (- 1)m (-2 cos x)m [cos m (2 n' + 1) / - 1 sin m (2 n'+ 1) ] Which, substituted in equation (a) of Art. 244, gives (- 2 cos x) Cos m (2 n' 4- 1) >r = P,,, r+ (- 2 cos x)m sin m (2 n' + 1) v = Pn,,+, Making =- r, cos x = - 1, (- 2 cos x)n = 2m, and the series become, by the process shown in Art. 244, P(2 n +1) =- 2m cos m (2n + 1) r P'(,+t), = 2," sin m (2 n + 1) r dnd we hae 2m cos m (2 n' +- 1)r = 2m cos m (2 n + 1) r 2m sin m (2 n' + 1) r = 2m sin m (2 n + 1) r whence, as before, n = n', and our formulae are (- 2 cos x)m = os p (2 n + 1)r- (478) (- 2 cos x) = si 2 +x) (479) sin m (2 n 4 1) 5 by which it appears that the real value of (- 2 cos x)m is also expressed either by a series of cosines or of sines of multiple arcs, which series have the constant relation P'I7,n +x sin m (2 n +- 1) v Pn+rr COs m (2 n + 1) n 248. If n 0, (478) and (479) give ( 2 cos x)-m = - (cos mx + m cos (m — 2) x + &c.) (480) (COS M - cos m 7r (-2 cos x) - P r _ 1 (sin mx -m m sin (m-:) x + &c.) (481) ( 2 cos sin m r sin m 7r In this case sin m z7 is not zero, unless m is an integer, so that the series P', does not become zero when x > 2 and both (480) and (481) may be employed as the true developments of (- 2 cos x)m. 249. When m is an integer, the series (476) and (480) always terminate at the (m +- 1)th term; and, since in (480) cos m 7r = it 1, according as m is even or odd, and (- 2 cos x)m =:f: (2 cos x)m in the same cases, both (476) and (480) beconme (2 cos x)m = cos mx+ m cos (m - 2) x + (- ) cos (m - 4) x + &. (482) But the series (481) becomes zero, so that (482) is the only series by which (2 cos x)m can be developed in functions of the multiple arcs, when m is integral. 144 PLANE TRIGONOMETRY. 250. To develop any power of the sine of the simple angle, in a series of sines or cosines of the multiple angles. If y = cos x +- / - 1 sin x, we have, by (435) and the Binomial Theorem, (/ -1)m (2 sin x)m - (y - y-l)m -_ ym_ - ym- _ m (m - 1 m)..4 &c = M - mym --- - -- ym-4 _ &C. 2 in which ym, ym-A, &c. have the same values as in Art. 244, but the signs of the coefficients are alternately + and -, so that if we put Qann+x = cosm (2n 7r + x) -m cos (m - 2) (2n + x) + &c. Q'anr+ -= sin (2 n + x) - m sin (m - 2) (2 n r + x) + &c. we have (/- 1)m (2 sin x)m = Qanf+ z + /- 1 Q'anf+x Substituting the value of ( 1 - l)m by (446), and comparing the real and imaginary terms, we find m (4 n'4-+ 1) r _ (2 sin x)m cos m (4 n+ Qnnr+x (2 sin x)m sin m (4 '+ 1) 2 and if we make x = X-, we shall find by the process frequently employed above, that n = n'; whence (2 sin x)m = t( n r (483; cos m (4 +1) (48;7 (2 sin x) — Q"2r+X (44 (2 sin xm (4 n 1) (484) so that the real value of (2 sin x)m may be developed in either the cosines or sines of the multiples. The two series have the constant relation Q'n T -r sin i m (4n + 1) nr Q2nn + COS - 1 (4 n + 1) r 251. If n = 0 in (483) and (484), V. 1 (2 sin X)?71 = - - _ __ (cos mx - m cos Cm- 2) x4-F &c.) (48b) cos 2 mrr cos 21 mv (2 sin )m (sin mx m sin (m - 2) x - &c.) (486) sin -1 m- sin m vr both of which series are applicable when m is fractional. 252. When m is an integer, one or the other of the series (485), (486), will always be zero, according to the form of m, and there will be but one series to express. (2 sin x)7n. If m = 47', (2 sin x)m cos mx-m cos (m-2) x — &c. (487) m 4 m' + 1, (2 sin )- = sin nx - m sin (m - 2) x - &c. (488! m = 4 m'4- 2, (2 sin )' = - (cos mx — m cos (m -2) + &c.) (489) In = 4 m' + 3, (2 sin x)7 = - (sin mx -- m sin (m - 2) x + &c.) (490) MULTIPLE ANGLES. 145 253. The series (485) and (486) become zero when m is an integer, as follows: If m = 2m', 0 =sin mx - m sin (m - 2) x + &c. (491) m = 2 m' + 1, 0 = cos n - m cos (m - 2) x + &c. (492) The reason why these series are zero is obvious, since they terminate ab the (m + l)th term, the terms equally distant from the first and last are equal with opposite signs, and the middle term of (491) is zero. 254. Given the equation tanx (493 tan x-=p tan y (5JLA y t 4 (493) to express x -= y in a series of multiples of y. Substituting the values of tan x and tan y given by (431) ex,-I- 1 ey-Yv - - 1 eXY- 1 - p' P eV' -i + 1 whence = ( + 1) evY1/- (p-1) p+ 1-( - 1) ea/or rutting q= 2 (494) eSYT;/_1 _ -q e —y2YV —( 1 q e yyV — 1- qe3Y8-' Taking the Naperian logarithms of both members, 2 (x -y) v/- 1 = log (1 - e-q2yv-) -log (1 - qep -'1) and developing the second member by the formula log (1 - n) - n - na - A n - &c. we have 2 (x - y) / - 1 -- q e-y - e-4 ' -- q e-Yl3e-y - &c + q eYyl/-' - q ey-, ' ~ V q3eGy-'t + &c. Substituting in the second member by (430), - y = q sin 2y + qa sin 4y + q3 sin 6y + &. (b) The equation (a) might have been put under the form 1 — eyl/-' es (+Y) I/- - -- 1 - e-ay —i from which, by taking the logarithms and substituting as before, sin 2y sin 4y sin 6 y x - y- - q -- &C. (c) q 2 - 3 ' In this investigation, we have, in effect, used Moivre's formula, in its limited or less general form; but the requisite generality may be given to our results, by observing, that (493) would hold if we were to substitute tan x = tan (n'r +- ), tany -tan (n"'- +y), and therefore we may substitute for the first member of (h). 19 N 146 PLANE TRIGONOMETRY. n'%r - x - (n"7r + y) - z - y — (n" - n') r- = x -y - nr, n being (like n and n") ari arbitrary integer or zero. Hence, the required general development of x - y in series is - y = nr + q sin 2 y +- &q sin 4 y +- q sin 6 y - &c. (495) In like manner, since tan x = tan (x - n'), tan, = tan (y - n"r), we may substitute in the first member of (c), x-n'r — y —n"7-r= x+-y- nr, and the general development of r + y in series is sin 2y sin 4y sin 6y. z - y n - _ - 22 g- &c. (496) g 2 3 In these formulse x and y are supposed to be expressed in arc, and to obtain x:; y in seconds, the terms of the series must be divided by sin 1". 255. The preceding problem is particularly useful in finding x when p and y are given, and x is nearly equal to y; in which case p is nearly equal to unity, either? or - is a small fraction, and one of the series (495), (496) converges rapidly. q EXAMPLES. 1. Given y = 50~ and p =- 100065, to find x from (493). Taking only the first term of the series (495), and assuming n - 0, 2 y 100~ log sin 2 y 9-99335 q -200065 log q 6-51174 2-00065 ar co log sin 1" 5-31443 x - y = 65".995 log (x - y) 1-81952 x - 50~ 1' 5".995 2. Given y = 50~ and - - 1-00065, to find x from (493). In this case 2-00065 q 00065 and the computation by (496), if we assume n =- 0, is 2 y = 100~ log sin 2 y 9'99335 1 -00065 1\,, ~ - - 2U0005 log ( — — 6.51174 -q- - 2.00065 ar co log sin 1" 5-31443 x + y = - 65"-995 log (x 4- y) - 181952 x = - y - 65"*995 = - 50~ 1' 5"-995 or, ifn = 1, = 180~ - 50 1' 5".995 = 129~ 58' 54".005. In general, (493) is to be solved by (495) when p is positive, and by (496) whenp Is negative. 256. Given the equation sin (x + z) =- m sin z (497) (c express z in a series of multiples of a. We deduce as in Art 168, tan (z - i a) m tan ' — m —1 t- n~* MULTIPLE ANGLES. 147 which is reduced to (493) by putting x-=z+ Y =_ P-_-1 p —1 1 whence -p 1 = and (495) becomes sin a sin 2 a sin 3 a( z = n+ + - + — 3 + &c. (4981 m Z r m 3m which is to be employed when m > 1; and (496) becomes z s- = -- - mn sin a - i v1' sin 2 a - -?3 sin 3 e - &. (499) which is to be employed when m < 1, n being any integer or zero. 257. Given the equation m silln tan z = - (500) 1 -+ Tn cos to express z in a series of multiples of z. This equation in the form sin z rn sin a cos os 1 m cos gives sin z + in sin z cos ac = m cos z sin c sin z = -m sin (a - z) tan (z - ) = - tan a which is reduced to (493) by substituting m 1 xZ - ~a y = P =m 1 p —1 1 whence = -- p + 1 z and tho series (495) and (496) become sin a sin 2 s sin 3 a. ( ) - =.- - + 2 m 3 n (50 z = n 7r -- m sin c - i m' sin 2 a +- i m sin 3 - &c. (502) 258. Given the equation m sin A tan z --- om s (503) 1 mcos c to express z in a series of multiples of e. The equation (500) becomes (503) by changing the signs of both m and:t: the rame changes in (501) and (502) give sin t sin 2 A sin 3 a z + = n z - --- - - &c. (504) m 2 mi 3 in' z = n 7r - m sin a 4- ~ ms sin 2 a 4- 5 m' sin 3 ct 4 &c. (505) 148 PLANE TRIGONOMETRY. 259 In aplane triangle A B C, given a, b and C, to find A or B by a series of multiples of C. By (260) a - sin C tan A = a 1 --- cos C which, compared with (503), gives, by (505), a a sin 2 C a3 sin 3 C. A= sin 2 ++-3 3 - &. (50,) n being necessarily = 0 in this case. B is found by the same series, interchanging a and b. 260. In a plane triangle, A B C, given a, b and C, to find c by a series of multiples of C. We have c =- a — b2 - 2 ab cos C (507) c' bA 2b cos C - 1 aa aa a by (451) = [b _(cos C+/- sin C)] X [ — (cos C — /-l sin C)] b = b1 (cos oC+-/-lsin C)]x[1- -- (cosc-^/-lsin) j Taking the common logarithms, employing in the second member the formula log (1 - n) = - M (n + ( n' + j n' + &c.) and applying Moivre's Formula (440) in expressing the powers of cos Ci - 1 sin 0, we have 2 log c - 2 log b = - [a (cosC+/-l sinC)+ -- (cos2. C+ - 1 sin2 C)+&c.] -M [- (cosC- - - 1 sin ) + — (cos 2 C- - 1 sin2 ) +&c.] logcl M(ca Ca cos2 C a' cos3C + ) (08) log C log b — M- cos C -... ' {-+ &C. (508) This series was first given by Legendre. The series (495) and (496), upon which are based those of the subsequent articles, (Arts. 256, 257, 258 and 259), are due to Lagrange. PART II. SPHERICAL TRIGONOMETRY. CHAPTER I. GENERAL FORMULAE. 1. SPHERICAL TRIGONOMETRY treats of the methods of computing the unknown from the known parts of a spherical triangle. It is shown in geometry,* that a spherical triangle may, in general, be constructed when any three of its six parts are given, (not excepting the case where the three angles are given). We are now to investigate the methods by which, in the same cases, the unknown parts may be computed. We shall at first confine our attention to such triangles only as are treated of in geometry, namely, those whose sides are each less than a semicircumference, and whose angles are each less than two right angles; that is, those in which every part is less than 180~. 2. It is shown in geometry, that if a solid angle is formed at the center of a sphere by three planes, the three arcs in which these planes intersect the surface of the sphere form a spherical triangle. Now the real objects of investigation in spherical trigonometry are the mutual relations of the angles of inclination of the faces and edges of a solid angle; but, for convenience, the spherical triangle which forms the base of the solid angle is substituted for it. The sides of the triangle being proportional to the angles of inclination of the edges of the solid angle, are taken to represent those angles; and the angles which those sides form with each other are regarded * The student is here supposed to be acquainted with Spherical Geometry, at least so much of it as is to be found in Legendre's treatise, or in that of Prof. Peirce, of Harvard University. N2 149 150 SPHERICAL TRIGONOMETRY. as identical with the angles of inclination of the faces of the solid angle. But, since varying the radius of the sphere would not, in any respect, change the solid angle, or the values of the angles which enter into it, the mutual relations in question ought to be deduced without any reference to the magnitude of the radius of the sphere. In fact, we shall deduce our fundamental formulae from a direct consideration of the solid angle itself. 3. In a spherical triangle, the sines of the sides are proportional to the sines of the opposite angles. Fig.. Let AB C, Fig. 1, be a spherical B triangle, 0 the center of the sphere. The angles of the triangle are the 0 / \ inclinations of the planes A OB, c, A 0 C and B O C, to each other, and c\ _P a will be designated by A, B and C; b / their opposite sides respectively will be designated by a, b and c, as in A plane triangles. The trigonometric functions of these sides will be the same as those of the angles BO C, AO C, AO B, which they subtend at the center of the sphere. (PI. Trig. Art. 20.) From any point B' in 0 B, let fall B'P perpendicular to the plane AO C; and through B'P let the planes B'PA', B'PC' be drawn perpendicular to OA and 0 C, intersecting the plane OAC in the lines PA', PC', and the planes AOB, BOC in the lines A'B', B'C'. The plane triangles A'P B', B'P C' are right angled at P; and OA'B', O C'B' are right angled at A' and C'. The angle B'AP, being formed by two lines perpendicular to OA, is the measure of the inclination of the planes A B, A 0 C, or of the angle A; and B' C'P is the measure of the angle C. We have therefore, by P1. Trig. Art. 15, B'P sin A = sin B'A'P =B'P sin C = sin B'C'P = B whence sin A B'P B' C' B' ' sin C B'A X B'P B'A' ( GENERAL FORMULA. 101 B'C' Again, sin a = sin B'OC = -B' sin c = sin B' OA' - BA sin a B'C' B'O B'C' whence O x sin c B'O B'A' B'A' (n) Comparing (m) and (n), sin a sin A sin c sin C which in the form of a proportion is sin a: sin c= sin A: sin C7 which is the theorem that was to be proved. 4. In Fig. 1, A, a, C and c, are each less than 90~, but the construction would not vary if any of these parts were greater than 90~, except that the points A' and C' might be found in the lines AO, CO, produced throughO; and one or more of the right triangles A'B'P, &c., would contain the supplements of A, a, C, or c instead of these quantities themselves. But the sine of an angle and of its supplement being the same, the preceding demonstration would still be valid, so that the theorem is applicable to any spherical triangle. Indeed, according to P1. Trig. Art. 49, this result follows from the nature of the trigonometric functions themselves, and the demonstration of the preceding theorem might therefore be considered as general, without requiring a special examination of the various positions of the lines of the diagram. 5. In a spherical triangle, the cosine of any side is equal to the product of the cosines of the other two sides, plus the continued pro. duct of the sines of those sides and the cosine of the included angle. Let the plane B'A'C' Fig. 2, be Fig. 2. B drawn perp. to OA, intersecting the Bi planes A OB, BO Cand AOC, in the linesA'B', B'C'and A'C'. Then the 0 -\ angle B'A'C' = A, and B'OC' = a, if and by P1. Trig. Art. 119, in the triangles A'B'C', OB'C', we have J B'C' = A'B'2 + AC'2 - 2 A'B'. A'C' cos A B'C' =0 B OB'2 ' - 2 0 B'. O C' cos a SPHERICAL T.RIGONOMETRY. Subtracting the first of these equations from the second, and ob. serving that in the right triangles OA'B', OA'C', 0 B'2 - A' B'2 = 0 A'2, 0 '2 - A' /'2 = 0OA'2 we have = 2 OA'2 + 2A'B'. A'C'cosA - 2 O B'. 0 C cos a OA'. OAi' A'B'.A'C' whence cos a -- - - -- -- +. OC cosA whence cs OB'. OC' OB'. OC0 Substituting the trigonometric functions derived from the right tri angles OA'B', OA'C', cos a = cos b cos c + sin b sin c cos A (2) which is the theorem to be proved. It may be regarded as the fundamental theorem, for the preceding (1) can be deduced from it, but as the process is somewhat circuitous, we have preferred deducing the two theorems from independent constructions. 6. In the construction of Fig. 2, both b and c are supposed less than 90~, while no restriction is placed upon A and a; but the equation (2) is no less applicable to all the other cases if the principle of P1. Trig. Art. 49 be granted. As that principle may not be suffiFig. 3. ciently evident to the student unacquainted with analyti- ccal geometry, we shall verify it in this case, as follows.* a 1st. In the triangle A BO, (Fig. 3), let b < 90~ and / Ae c> 90~. Produce BA, BC to meet in B', forming the l lune B B"; then A B' 180~ - c, and b are both < 90~, b\ / | and the preceding demonstration would apply to the A\ / triangle A B'C. Therefore, applying (2) to A B'v, we have B' cos (180-a) = cos b cos (1800- c)+sin sin (180- c) cos (180 -A) or by P1. Trig. (64), -cos a = - cos b cos c - sin b sin c os A and changing all the signs cos a = cos b cos c - sin b sin c cos A the same result that would have been found by applying (2) directly to ABC. * Hymer's Spherical Trigonometry. Cambridge, 1841. GENERAL FORMULAJ. 153 2d. In the triangle ABC, Fig. 4, let b > 90~, c > 90~; Fig.4 produce AB and AC to meet in A'; then A'B andA'C A being both less than 90~, the formula (2) is applicable to A'B C. Therefore cos a = cos (180~ - b) cos (1800 - c) + sin (180~ - b) sin (180~ - c) cos A \ = (- cos b) (- cos c) + sin b sin c cosA - cos bos s e + sin b sin c cos A A' the same result as before. 7. The theorems expressed.by (1) and (2) being applied successively to the several parts of the triangle, give the two following groups: sin a sin B = sin b sin A sin b sin C = sin c sin B (3) sin c sin A - sin a sin C cos a = cos b cos c + sin b sin c cos A cos b - cos c cos a + sin c sin a cos B (4) cos c = cos a cos b + sin a sin b cos C J 8. Let A'B'C', Fig. 5, be the polar triangle Fig5. of ABC, and designate its angles and sides by A, B, C', a', b' and c. Then, by geometry, A' = 180~ - a, a' = 180C -A B' = 180 - b, b' = 180~ -B / C' = 180 -, c =180 - C B' a' and applying the first equation of (4) to A'B'C', cos a = cos b' cos c' + sin b' sin c' cos A or by P1. Trig. (64), - cos A = (- cos B) (- cos C) + sin B sin C (- cos a) - cos A = cos B cos C - sin B sin C cos a Changing the signs of this, we have the first of the following group: cos A = - cos B cos C + sin B sin C cos a cos B= - cos C cos A + sin C sin A cos b ( cos C = - cos A cos B + sin A sin B cos c 20 15 1 SPIiERICAL TRIGONOMETRY. It is thus that, by means of the polar triangle, any formula of a spherical triangle may be immediately transformed into another, in which angles take the place of sides, and sides of angles. 9. Several other important fundamental groups of formule are obtained from the preceding with the greatest ease. The first of (4) multiplied by cos c is cos a cos c = cos b cos2 c + sin sinin cos c cos A and the second of (4) is the same as cos a cos c + sin a sin c cos B = cos b the difference of which is sin a sin c cos B = (1 - cos2 c) cos b - sin b sin c cos c cos A Since 1 - cos2 c = sin2c, this may be divided by sin c, and gives sin a cos B = sin c cos b - cos c sin b cos A whence sin b cos C = sin a cos c - cos a sin c cos B (6) sin c cos A = sin b cos a - cos b sin a cos C If we interchange B and C, and therefore also b and c, the group becomes sin a cos C = sin b cos c - cos b sin c cos A sin b cos A = sin c cos a - cos c sin a cos B (7) sin c cos B =-sin a cos b - cos a sin b cos J 10. If (6) and (7) are applied to the polar triangle, they give, after changing the signs of all the terms, sin A cos b= sin C cos B + cos C sin B cos a sin B cos c= sin A cos C + cos A sin C cos b ] (8) sin C cos a sin B cos A + cos B sin A cos J and sin A cos - sin B cos C + cos B sin C cos a sin B cos a sin Ci cos A + cos C sin A cos b (9) sin C cos b = sin A cos B + cos A sin B cos c 11. Dividing the first of (6) by the following derived from (3), sin a sin B = sin b sin A GENERAL FORMULME. 155 we find the first of the following group sin A cot B sin c cot b - cos e cos A sin B cot C = sin a cot e - cos a cos B. (10) sin Cv cot A = sin b cota - cos b cos C and in the same way from (7), or by interchanging the letters B and (, b and c in (10), we find sin A cot C= sin b cote - cos b cos A sin B cot A sin c cota - cos c cosB (11) sin C cotB = sin a cot b - cosa cos C If (10) are applied to the polar triangle, we find (11), so that no new relations are elicited. 12. The preceding formule are sufficient to furnish a theoretical solution for every case of spherical triangles, but some transformsa tions are required to facilitate their application in practice. In the first of (4) substitute, by P1. Trig. (139), cos A = 1 - 2 sin2 1 A we find, by P1. Trig. (39), cos a = cos (b - c)- 2 sin b sin c sin2 A (12 and we have similar expressions for cos b and cos c. If we substitute in (4), by P1. Trig. (138), cos A = - 1 + 2 cos2 -A we find, by P1. Trig. (38), cos a = cos (b + c) + 2 sin b sin c cos2 - A (13) and, of course, similar expressions for cos b and cos c. 13. Substituting in (5) cos a = 1 - 2sin2 a = - 1 + 2 cos2 ~ a we find by the same process cosA = -cos (B + C) - 2 sin B sin C sin2 a (14) cos A= -cos (B- C) + 2 sin B sin C cos2 ~ a (15) which might have been obtained by applying (12) and (13) to the polar triangle. 156 SPHERICAL TRIGONOMETRY. 14. If in (12) we substitute cos a = 1 -- 2 sinl a, cos (3 — c) = -- 2 sin (b - c), we obtain the first of the following equations; and the others are obtained by a similar process from (12), (13), (14) and (15). sina y a sin' -1 (b-c ) + sin b sin c sin" 2 A (16) sin' a = sin (6 + c)- sin b sin c cos 2 (17) cos'2 a cos s1 (6 - c)- sin b sin c sin2 4 A (18) cos2 a = cos' (b + c ) + sin b sin c cos A (19) sin' iA = cos' ~ (B + C) + sin B sin C sin ~- a (20) sin I A = cos' - (B — C) - sin B sin C cosa a (21) cos2' A =sin i (B + C) - sin B sin C sin" ~ a (22) cos' A sin' (B - C) sin B sin C cos - a (23) 15. By P1. Trig. we have 1 - cos' A - sin' } A cos A -= cos' A- sin2 - A whence cos b cos c = cos b cos c cos i4 A + cos b cos c sin' i A sin b sin c cos A = sin b sin c cos ~ A - sin b sin c sin2 A the sum of which is, by (4), cos a = cos (b - c) cos2 ~ A + cos (b + c) sin' Ja (24) and substituting 1 - 2 sin2a a, &c., for cos a, &c. sin, = a = sin' ~ (b - c) cos2 A + sin2 - (b + c) sin2 A (2;) cos ~ a =cos' (b - c) cos A 4- cos' ~ (b +- c) sin2 I A (26) In the same manner we deduce from (5) cosA = - cos (B - C) sin a - cos (B - C) cosa a (27) sin' A = cos2 (B- C) sin a -+ cos' ((B + C) cos' a (28) cos 1 A sin' 1 (B - C) sin2 a + sina2 (B + C) cos a (29) It is hardly necessary to add that each of the equations (12 to 29) gives a group of three, by applying it successively to the three sides or three angles of the triangle. 16. From (12) we find in A cos (b-c) - cos a 2 sin b sin c If, in P1. Trig. (108), we put x =a, y b- c whence - (x + y)= (a+ b -c), (x - y) (a -b+c) we find cos (6 - c) - cos a 2 si (a - b + c) sin - (a + - c) which, substituted in the above equation, gives si 21A sin (a - + c) sin '(a+ b-c) (3- 2 sin b sin c GENERAL FORMUL.E. Let s denote the half sum of the sides, that is, let a+ b+ c=2s, 1 (a + + )-= then a -6 c = a + b + c -2 b -2s -2 = 2(s - b) a + b - c = a + b + c-2 c =2s-2 c=2 (s- ) which substituted in (30) give sin2A sin (s - b) sin (s- c) 2 sin b sin c whence also sin2 B sn (s - c) sin (s - a) 2- ~ sin c sin a sin21 C = sin(s -a)sin (s - b) 2 sin a sin b 17. From (13) we find 2 cos a - cos (b + c) cos2 2 A =sin c - j2 sin b sin c 15; (31) and from P1. Trig. (108), by making =b +c, y =a (x + y) = -1 (a + b +< ), i (x - ) = i (b + c - a) we find cos a - cos (b + c) = 2 sin i (a + b + c) sin } (b + c - a) which, substituted above, gives 2 1 A _ sin I (a + + c) sin - ( + c - a) COS2 ~J A 2 = 2 cos2Asn +~~II ~sin b sin c Introducing, as in the preceding article, s= - (a + b + c), cos A -- sin s sin (s - a) sin b sin c cos2B sin s sin (s - b) sin c sin a os 21 = sin s sin (s -- C) sin a sin b OJ (32) (33) 158 SPHERICAL TRIGONOMETRY. 18. The quotient of (31) divided by (33) gives sin (s - b) sin (s - c) tan2 ~A = tan2 A= sin s sin (s - a) tn B =sin (s - c) sin (s - a) ( sin 8- sin ( ) - b) tan2 1 sin (s - a) sin ( 8- b) sin s sin (s - e) 19. From (14) we find cos A + cos (B + C) sin2 ~ a- -- sm2 =_ 2 sin B sin 0 from which, by P1. Trig. (107), we deduce -CS (A + B + C) cos 1 (B+ - A) (5) sin2 I a 2 (35) 2 sin.B sin C and if we put (A + B + C)= s 8121 - _ cos Scos (S- A) sin2 ~ a = — -2 a sin B sin C sn - cs S cos Sc S- B) (36) sin2 - (36) sin C sinA n2 -- cosscos (s- C) sin A sin B The first member of each of these equations being a square, the second member must be essentially positive, although its algebraic sign is negative; in fact, since by geometry 2 > 180~, S> 90~, cos S is negative, and - cos S is positive. 20. From (15) we find cos A + cos (B - C) COS2 a —= 2 sin B sin C from which we deduce, by a process similar to the preceding, O cs (A-B B + C) cos (A + B-) (3) COS2 s a -- ( 2 sin B sin G) GENERAL FORMULE. 159 cos (- B) cos (S - C) cos2 2 a..= os 2 s sin B sin C cos2 = cos( C) cos(- A) (38) ~2 ~ sin 0 sin A " os2 1 c cos (- A) cos (S- B) 2 sin A sin B 21. Frcm (36) and (38) 21 - -cos Scos (S - A) tan2 a =cos ( - B) cos (S- C) tj 2~ zb - cos S cos (s - B) ( tan2 t b - I - b-S<;c rys ( (39) 2 cos ( - C) cos (S - A) tan2 ~ec - - cos S cos (S - C) tn2 cos (S- A) cos (- B) We might have deduced (36), (38), (39), by applying (31), (33), (34) to the polar triangle. 22. Napier's Analogies. Dividing the 1st of (34) by the 2d, we find tan I A sin (s - b) tan 2- B sin (s-a) Regarding this as a proportion, we have, by composition and division, tan A A + tan 1 B _sin (s - b) + sin (s - a) tan ~ A - tan 1 B sin (s - b)- sin (s - a) In P1. Trig. (109), if we put x = s - b, y = - a, whence x + y 2 s - a- - = x- y=a-b we nave sin (s - b) + sin(s - a) tan 1 e sin (s - b) - sin (s - a) - tan ~ (a- 6) and by P1. Trig. (126), tan A. + tan B sin - (A + B) tan - tan B sin L1 (A - B) 160 SPHERICAL TRIGONOMETRY. Therefore (mn) becomes sin 1 (A + B) tan 2 c 2 21P t~ sin (A - B) tan I (a - ) (40) or sin 1 (A -+ B): sin 2 (A -B)= tan -: tan j (a — b) which is the first of Napier's Analogies. 23. Again, the product of the 1st and 2d of (34) gives tan 1 A tan B sn ( - c) Sill S or 1: tan I A tan B = sin s: sin (s- c) whence, by composition and division, 1 -tan A tan ~ B sins - sin (s - c) 1 + tan Atan X B sin s + sin (s - c) By P1. Trig. (109), if x = s, y = s - c, we have sin s - sin (s - c) tan t c sins + sin (s - c) - tan (a + b) and by P1. Trig. (127), 1-tan A tan B _cos 1 (A + B) 1 + tan A tan ~ B cos (A - B) Therefore (n) becomes cos - (A + B) a tan - c cos (A - B) tan l (a + b) (41) or co(A+ cos(A )cos(A -B) tan c: tan a+b (a ) which is the second of Napier's Analogies. 24. If (40) and (41) are applied to the polar triangle, we shal find sin 1 (a + b) cot1 ] sin ~ (a - ) tan (A -B) (42) or sin - (a + b): sin 1 (a - ) cot - C: tan (A- B) cos (a + b) cot 1 C cos ~ (a - b) tan (A + B) (43) or cos - (a + b): cos (a - ) = cot ~ C: tan ~ (A + B) which are the third and fourth of Napier's Analogies. GENERAL FORMULA. 161 25. Gauss's Theorem. If p = cos ~ c sin ~ (A - B) P coos s (a - b) q = cos c cos ~ (A + B) Q = sin Ccos - (a + ) r = sin c sin (A - B) R cos C sin (a- 5) a = sin 4 c cos ~ (A -B) S = sin C sin (a - b) then the products p X q, p X r, p X s, q X r, q X s, r X s, are respectively equal to the vroducts P X Q, PX R, P X S, Q X R, Q X S, R X S. First. From (3) we have sin c (sin A:= sin B) = sin C (sin a ~: sin b) which, by PI. Trig. (105), (106) and (135), are reduced to sin ] c cos ] c sin ~ (A + B) cos ~ (A - B) = sin C C cos ~ C sin ~ (a + b) cos (a - b) sin ] c cos ~ co s s ~ (A + B) sin ] (A -B) = sin ] C cos ~ C cos (a + b) sin (a -- ) or ps =PS and qr QR Second. From (6) and (7) sin c (cos B ~- cos A) = (1 qF cos C) sin (a ~h b) which, by P1. Trig. are reduced to sin j c CS cos (A B) cco I (A -+ B) c - sin Ca sin C sin (a+ b) cosW (a ) sin c cos ~ c sin - (A + B) sin ] (A - B) = cos ] C cos I C sin j (a -b) cos ( (a - b) or qs = QS and pr = PR Third. From (8) and (9) (1+- cos c) sin (A it B) - sin C (cos b:fh cos a) which, by PI. Trig. are reduced to cos i cos in ( B) cos (A B)sin -A ) cos sin cos C (a 6) c os (a - ) sin ] c sin I c sin ] (A - B) cos ~ (A -B) =sin 1 C cos C sin j (a + b) sin (a — ) or pq = PQ and rs = RS 26. The notation of the preceding article being still employed, the quantities p", gq, r, a, are respectively equal to P", Q1, RI, S2. We have pq X pr= PQ X PR and qr = QR the quotient of which is p2 = P2 whence p = ~ P and in the same way q2 = Qa q = =t: Q r - R2 r - R s S2 s — ' S 21 o2 162 SPHERICAL TRIGONOMETRY. 27. In these last equations, the positive sign must be used in all the second members, or the negative sign in all of them. For if we take p=+ P the equations pq = PQ, pr =PR, ps PS being divided by this, give q-=+ Q, r= +R s=+S and if we take p =-P the same equations, divided by this, give q = - Q, r - R, s = - S We have therefore the following, which are generally cited as Gauss's Equations. cos I c sin -A (A - B) = cos C cos (a - b) cos c cos (A + B) sin C cos (a + (b) 2 2 2 2(44) sin z c sin -- (A - B) = cos - C sin 1 (a- b) sin c cos 2- ( - 1B) sin C sin I (a + b) or cos 4 c sin 1 (A + B) c= - o- C cos ~ (a - 6) cos -c cos - A (A - B) = -sin C cos ~ (a + b) sin - c sin (A - B) = - cos C sin ( — (a b) sin 2- c cos 1 (A - B) - sin 1 C sin 2- (a + b) If, however, we consider only those triangles whose parts are all less than 180~, the first of these groups, (44), is alone applicable, for we must then have p = + P: since cos -c, sin (A c+ ), cos - C, cos - (a - b) are then all positive quantities. The use of (45) will be seen in the chapter on the solution of the general spherical triangle. Napier's Analogies, (40), (41), (42) and (43) can be deduced directly from (44). ADDITIONAL FORIULaE. 28. We shall here add some formula which, though not so frequently used as the preceding, are either remarkable for their elegance and symmetry, or of importance in certain inquiries of astronomy and geodesy. 29. The product of (30) and (32) gives sin2 A = 4 sin s sin (s - a) sin (s - b) sin (s -c) (46) Bin" A == --------------- - ------- 7 --—,(46) sin' b sin2 c Put na= sin s sin (s -a) sin (s - b) sin (s -c) (47) 2n then sin A sinb sin c and in the same manner (48) 2n sin B 2 n sin a sin c the quotient of which is din A sin a sin B sin b which is our first theorem, Art. 3. As (48) was obtained from (30) and (32), anc these from (4) without the aid of (3), we may consider the whole fabric of spherical trigonometry as resting upon the fundamental formulae (4). ADDITIONAL FORMULE. 1 63 130 We have also from (35) and (37) sin a c- 4 cos S ( - co (s (S - B) cos (S -- ) ( sin' B sin' C and if VN = - cos S cos (S -A) cos (S - B) cos (S- C) (50) 22 sin a = —. (51) sin B sin C From (48) and (51), n sin a sin b sin e N sin A sin B sin C 81. If we develop (47) and (50) by P1. Trig. (173) and (174) 4 n2 = 1 - cos a -cos b - cos c 2 cosa cos b cos (5) 4 N2 = 1- cos A - cos B- cos C- 2 cosA cos B cos C (54! 32. The following simple results are easily deduced from the equations (31 to 38) cos - A cos ~ B sin s sin ~ C sin c cos - A sin B _ sin (s - a) cos - c sin c * (55) sin ~ A cos B _ sin (s - b) cos I C sin c sin I A sin B - sin (s - c) sin ~ C sin c sin I a sin ~- b - cos S cos c sin C sin a cos b cos (S - A) sin ~ c sin C cos ~ a sin 5 b cos (S- B)56) sin I c sin C cos c a cos _ cos (S- C) cos ~ c sinC j 33. By means of (55) and (56) we can deduce expressions for the functions of 9, s - a, &c., in terms of the angles, or of S, - A, &c., in terms of the sides We have, from (51), 2N N sin c o 2 sin AosnB sin A 2 s in cos sin B cos I B which, substituted in (55), gives Ni sin s 7 57) 2 sin ~4 sin - B sin I C N sin (s - c) - -cos-Acos B sin (58) whence, by interchanging the letters, we have also sin (s - a) and sin (s - b). 164 SPHERICAL TRIGONOMETRY. Again, we have sin (8 - c) = sin 8 cos c - cos a sin c whence sin s cos c - sin (s - c) sin c which, by (55), is reduced to s cos A s B cos c - sin ~ A sin ( B sin * C and from the equation oos (s - c) = cos 8 cos c + sin a sin e we find, by substituting (55) and (59), cos ( -- c) -= - sin ~ A sin ~ B cos c + cos ~ A cos (60 cos (3 - c) = si (60) sin ~ C To eliminate c from the second members of (59) and (60), we have, by (5), cos C + cos A cos B COS C - - -- sin A sin B whence Acos~, Acos a + cos A cos B cos ~ A cos ~ B cos c = s Asi 4 sin ~ A sin ~ B cos C + cos A cos B sin Asin k B cos c 4- sc_ 4 cos ~ A cos ~ B which, substituted in (59) and (60), give cos A - cos B +- cos C- 1 - sin2 j A - sin2 B - sin2 G (C c0 4 sin 4 Asin3 B sin IC 2sin Asin} B sin C s cos A +- cos B -- cos C + 1 cos: AA +- cos2 B - cos2 C(6 cos (s c) 4 cos - A cos sin C - 2 cos A cos iB sin C ) From the preceding we easily deduce tan ~= 2 N sin c cos A + cos B+ cos - 1 cos c - tan A tan B (6 2 2N sin c tan _ - _____ 2 N sin c= (64) tan (s - c) = cos A + cos B - cos C+ 1 - cot ~ A cos B - co (64) 84. The equations (57 to 64) applied to the polar triangle, giv3, -- cos S = c — c(65) 2 cos ~ a cos ~ 6 cos c cos (S- C) = (6C, 2 sin } a sin } b cos ~ ~ sin _ sin j a sin ~ b cos C' - cos ~ a cos l b cos s c ADDITIONAL FORMiULAE. 165 Si 1 + cos a + cos b + cos c c2 a cos2 b +- cos2 3 c- 1 4 cos j a cos j 6 cos c 2 cos 4 a cos b cos (6 c sin (S - C) = )cos a cos b cos C- sin 4 a sin b c) cos c ( 6 1 - cos a - cos b + cos c sin2 I- a + sin2 b - sin2 3 c sin (s - ) -(70) 4 sin 3 a sin 3 b cos I c 2 sin a sin 6 cos j c 2n sin C7 1 - cos a +- cos b - cos c cos C + cot ~ a cot ( b 71) 2n sin C aot (S - C) 2n sin a (72) t (- ) 1 - cos a - cos b +t cos c cos + tan 3 a tan (2) 35. From (68) we find 1 - sin S 2 cos cos bC a c-os b c 2 a cos2 b - cos2 c + 1(7 2 cos 4 a cos 4 b cos 4 c 1 + sinS 2 cos a cos 6 cos c - cos2 a + cos2 b - cos2 -1 (74) 1 +- sin S - (74) 2 cos I a cos 1 b cos ~ c the numerators of which may be reduced by PI. Trig. (173) and (174), by making s = 4 a,y = b, z = c, whence v = (a + b + c) =, v - z = (s - a), &c.: therefore, 1 - sin S 2 sin s sin I (s -a) sin I (s -b) sin i ( - c) ( cos 4 a cos 4 b cos 4 c 1 + sin S = 2 cos js cos (s -a) cos (s -b) cos ~( —c) (76) cos I a cos 4 6 cos 4 c The product of these equations reproduces (65); their quotient is, by P1. Trig. (154), tan2 (45~ -- S) = tan ~ s tan 4 (s - a) tan 4 (s - b) tan ( (a - c) (77) 86. Cagnoli's Equation.-Multiplying the first equation of (4) by cos A, we find cos a cos A = cos b cos c cos A + sin b sin c - sin b sin c sin2 A and from (5) in a similar manner, cos a cos A = - cos B cos C cos a + sin B sin - sin B sin a sinW a Observing that by (3) we have sin b sin c sin2 A - sin B sin C sin2 a, these two equations give, sin b sin c + cos b cos c cos A = sin B sin - cos B cos Ccos a (78) a relation between the six parts of the triangle, first given by CAGNOLI. It is a property of this equation that either member is afunction which has the same value in a given spherical triangle and its polar triangle. Thus, if we distinguish the sides and angles of the polar triangle by accents, we have* sin b sin c + cos b cos c cos A = sin bI sin c - + cos b cos c/ cos A/ (79) * Sec Mathematical Monthly, (Cambridge, Mass.,) vol. i. p. 282. 166 SPHERICAL TRIGONOMETRY. T7 To dedeus the formulce of plane triangles from those of spherical triangles. The analogy of many of the preceding formule with those of plane triangles is sufficiently obvious. We can, in fact, deduce the plane formulae from those of this chapter, by regarding the plane triangle as described upon a sphere whose radius is infinite, the triangle being an infinitely small portion of the sphere. The quantities a, b and c, must, in this case, express the absolute lengths of the sides; and the angles which a b they subtend at the center of the sphere, expressed in arc, will be -, -, -, r beab c ing the radius of the sphere. When r is very large, -, -, -- are very small, and we a a may express the values of sin -, cos -, &c. approximately, by one or two terms of their expansions in series, P1. Trig. (405) and (406), and if their values be substituted in our spherical formulae, we shall obtain approximate relations between the sides and angles of the triangle. If we then make r infinite we shall obtain exact relations between the sides and angles of a plane triangle. Thus we have a a as aa sin sin- -+ &C- a - 4- &c. sinA sin r r 2.3r3 2.3r2 -&c. sinB sin b= 6 b b3 & sinp- 2.r ~&c. b -2 -3+&c r r C). ~3 22.3 r& and making r infinite, we find the formula of P1. Trig. sin A a sin B b In the same manner a b c a / b~ c2 b cu cos- — cos-cos - 1 - a +&c.- 1 - - +bc &c. r r r 2r 2 r' 2 r/ 4 -- cos A 3 sin b ic b b3 C s s r 2.3 r' 2.3 r3 bs cS co A c - a --- +&c b3 c 2 bc —. - &c. ba 2 be cosA _ 2b Formulm that involve only the sines or tangents of the sides may be reduced imn mediately to the plane formula by substituting a, b, &c., for sin a, tan a, &c. Thus. (31 to 34) give the corresponding formule of P1. Trig. by omitting the symbol sin. and (40), (41), by omitting the symbol tan. when these symbols are prefixed to sides SOLUTION OF SPHERICAL RIGHT TRIANGLES.;67 CHAPTER II. SOLUTION OF SPHERICAL RIGHT TRIANGLES. 38. WHEN one of the angles of a spherical triangle is a right angle, the general formulae of the preceding chapter assume forms that are remarkably analogous to the relations established for the solution of plane right triangles, and equally simple in their appli. cation. 39. Let C= 90~, Fig. 6. From (3) we Fig.6. B.ave s sin A -= sin Ca sin e b but since C = 90~, sin C== 1; therefore, sin a 1 sin A -- sin sin c and, in the same manner, } (80; sin b sinB= -- sin e that is, the sine of either oblique angle of a spherical right triangle is equal to the quotient of the sine of the opposite side divided by the sine of the hypotenuse. Compare PI. Trig. (1). 40. From (11), we find sin b cot c-sin A cot C COS =Acos b but if C = 90~, cot C= 0; therefore, sin b cot c cos A = - - tan b cot c cos b tjr tan b tan a osA tn - cosB - - (81 ~t~~mxr c ~tan 168 SPHERICAL TRIGONOMETRY. that is, the cosine of either angle is equal to the tangent of the adjacent side, divided by the tangent of the hypotenuse. Compare P1. Trig. (1). 41. From (10), we have, sin b cot a - cos b cos U cot A sin C which, when C-= 90~, becomes sin b cot A = sin b cot a -- tan a or, taking the reciprocals, tan a tan b tan A = tan B (82) sin b sin a that is, the tangent of either angle is equal to the tangent of the opposite side, divided by the sine of the adjacent side. Compare P1. Trig. (1). 42. From (5), we find, A cos B+cos C cos A sin A = cos b sin C and if C= 90~, cos B cos A sin A = sin B (83) cos b cos a that is, the cosine of either angle, divided by the cosine of its opposite side, is equal to the sine of the other angle. In P1. Trig. we have sin A = cos B. 43. From (4), we have, cos c = cos a cos b + sin a sin b cos C or, when C =90~, cos c == cos a cos b (84) that is, the cosine of the hypotenuse is equal to the product of the cosines of the two sides. In P1. Trig. c2 = a2 + b2. 44. From (5), cos C + cos A cos B cos c = sin A sin B or, when C= 90~, cos A cos B cos c = siA sinB cotA cotB (85) Csin~ A si B SOLUTION OF SPHERICAL RIGHT TRIANGLES. 169 bat is, the cosine of the hypotenuse is equal to the product of the co. tangents of the two angles. In P1. Trig., 1 = cot A cot B. 45. No difficulty will be found in remembering the preceding formule for spherical right triangles, if they are associated with the corresponding ones for plane triangles: thus, In plane right triangles. In spherical right triangles. s a 4 b sin a - in b sinA=- sinB=- ssinA sinB=c c sin c sin c b a tan b tan a cosA =- cos B = cos A — cos B — c c tan c tan c a b tan a tan b tanA - tan B -- tan A - tan B= b a sin b sin a cos B cosA inA =cos B, sinB =cosA sin A= — sin B = cos b cos a c2 = a2 + b2 Cos C = Cos a cos b 1 =cotA cot B cos c = cot A cot B 46. Napier's Rules. By putting these ten equations under a different form, Napier contrived to express them all in two rules, which, though artificial, are very generally employed as aids to the memory. In these rules, the complements of the hypotenuse and of the two oblique angles are employed instead of the hypotenuse and the angles themselves. The right angle not entering into the formula, they express the relations of five parts, but in the rules the five parts considered are a, b, co. c, co. A and co. B. Any one of these parts being called a middle part, the two immediately adjacent may be called adjacent parts and the remaining two, opposite parts. The right angle not being considered, the two sides including it are regarded as adjacent parts. The rules are: I. The sine of the middle part is equal to the product of the tangents of the adjacent parts. II. The sine of the middle part is equal to the product of the cosines of the opposite parts. The correctness of these rules will be shown by taking each of the five parts as middle part, and comparing the equations thus found with those already demonstrated. 1st. Let co. c be the middle part; then co. A and co. B are the adjacent parts, a and b the opposite parts, and the rules give sin (co. c) = tan (co. A) tan (co. B) or cos c cot A cot B sin (co. c) = cos a cos b cos c =cos a cos b which are (85) and (84). 2d. Let co. A be the middle part; then co. c and b are the adjacent parts, co. B mnd a the opposite parts, and the rules give sin (co. A) = tan (co. c) tan b or cos A = cot c tan b sin (co. A) = cos (co. B) cos a cos A = sin B cos a 22 P ,170 USPHERICAL TRIGONOMETRY. In the same mainer, if co. B is taken as the middle part, sin (co. B) = tan (co. c) tan a or cos B = cot c tan a sin (co. B) = cos (co. A) cos b cos B = sin.4 co b and these four equations are the same as (81) and (83). 3d. Le; a be the middle part; then co. B and b are the adjacent parts, co. A and co. c the opposite parts, and the rules give, sin a = tan (co. B) tan b or sin a= cot B tan b sin a = cos (co. A) cos (co. c) sin a = sin A sin c In the same manner, if b is taken as the middle part, sin b = tan (co. A) tan a or sin b = cot A tan a sin b = cos (co. B) cos (co. c) sin b = sin B sin c and these four equations are the same as (80) and (82). It appears, therefore, that these rules include all the ten equations previously proved; and they include no others, since we have taken each part successively as the middle part. In the application of these rules, it is unnecessary to use the notation co. A, co. B, co. c, since we may write down at once sin A for cos (co. A), &c.* 47. In order to solve a spherical right triangle, two parts must be given, and from the equations of Art. 45, that equation must be selected which expresses the relation between these two parts and the required part. When Napier's Rules are employed, it is only necessary to determine which of the three parts-the two given and the one required-is to be taken as the middle part. " These three parts are either all adjacent to each other, in which case the middle one is taken as the middle part, and the other two are adjacent parts; or one is separated from the other two, and then the part which stands by itself is the middle part, and the other two are opposite parts."t 48. In order to distinguish the functions of parts less than 90~ from those greater than 90~, it will be necessary carefully to observe their algebraic signs, according to P1. Trig. Art. 40. But when a required part is determined by its sine, since the sine of an angle and of its supplement are the same, there will be two angles, both of which may be regarded as solutions, except when this ambiguity is removed by either of the following principles. * If we employ as the five parts, the hypotenuse, the two angles, and the complements of the two sides including the right angle, these parts will be the complements of those used in Napier's Rules, and we shall have MvAUDUIT'S RULES.-I. The cosine of the middle part is equal to the product of the cotangents of the adjacent parts. II. The cosine of the middle part is equal to the product of the sines of the oppositeparts. With a little attention at the commencement, however, and by observing the analogy exhibited in Art. 45, the student will find that he will have little use for either of these artificial rules. t Peirce's Spherical Trigonometry. SOLUTION OF SPHERICAL RIGHT TRIANGLES. 171 49. In a right spherical triangle, an angle and its opposite side are always in the same quadrant, that is, either both less or both greater than 90~. For, by (83), cos B sin A = — cos b in which, since sin A is always positive, (A < 180~), cos B and cos b must have the same sign; that is, B and b must be either both less or both greater than 90~. 50. Wilen the two sides including the right angle are in the same quadrant, the hypotenuse is less than 900, and when the two sides are in different quadrants, the hypotenuse is greater than 90~. For, by (84), cos = cos a os b in which, if a and b are in the same quadrant, cos a and cos b have like signs, and cos c is positive, that is, e < 90~; but if a and b are in different quadrants, cos a and cos b have different signs, and cos c is negative, that is, c > 90~. We proceed now to the solution of the several cases. 51. CASE I. Given the h/ypotenuse and one angle, or c and A, Fig. 6. To find a. The relation among the three Fig. 6. B parts, c, A, and a, (as in P1. Trig. with the same data), is given by the sine of A; and by Art. 45, Cb sin a sin A = s sin c from which we find* sin a = sin csin A (86) There will be two values of a corresponding to the same sine, but, by Art. 49, the true value is that which is in the same quadrant as A. To find b. The relation among the three parts, c, A, and b, (as in P1. Trig. with the same data), is given by the cosine of A, or, tan b cos A = -- tan c from whicht tan b -= tan c cos A (87) * This equation would be found by Napier's Rules, taking a as the middle part. t We find the same result by Napier's Rules, taking co. A as the middle part. 172 SPHERICAL TRIGONOMETRY. To find B. We have, by (85),* cos c = cot A cot B from which cotB - co = cos c tanA (88) cot A The quadrants in which b and B are to be taken, will be determined by means of the signs of tan b and cot B, according to P1. Trig. Art. 40. Oheck. To guard against numerical errors, it is often expedient to compute the same quantity by two different and independent methods. In many cases, however, we may test the accuracy of several operations by a single formula, which may be called the check. In the present instance, when the three parts, a, b, and B, have been found, we should have, by (82), the relation sin a = tan b cot B so that if the work is correct, we shall find log sin a = log tan b + log cot B EXAMPLES. 1. Given c = 110~ 46' 20", A = 80~ 10' 30", to solve the triangle. By (86). By (87). By (88). c,log sin 9,9708106 log tan - 0.4210061 log cos - 9.5498045 A, log sin 9.9935833 log cos + 9.2320794 log tan + 0.7615038 log sin a 9.9643939 log tan b - 9.6530855 log cot B - 0.3113083 log tan b - 9.6530855 Ch eck. log sin a + 9.9643938 Ans. a =67~ 6'52".7, b = 15546'42".7, B = 153~ 58'24".5 2. Given c = 120~, A = 1200; solve the triangle. Ans. a = 131~ 24' 34".7 b = 40~ 53' 36"2 B = 49 6' 23 '.8 52. If A - 90~, we must also have, by (85), c - 90~, and then 0 0 tanb - tan B -- sB that b and B are both indeterminate; that is, there is an indefinite number or triangles which satisfy the given values of c and A; but since cos B = cos b sin A = cos b we always have B = b; and since sin a = sin c sin A = 1 we have a = 90~, and all the parts of the triangle are equal to 900, except b and B If only c is given = 900, all the parts of the triangle are equal to 90~, except A and a; and we have A = a. * Or by Napier's Rules, taking co. c as the middle part. SOLUTION OF SPHERICAL RIGHT TRIANGLES. 53. CASE II. Given thze hypotenuse and a side, or c and a. To find A. We have by (80), sin a sin A = ~- =- cosec e sin a (89) sin ce To find B. By (81), tan a cos B = — = cot c tan a (90) tan c Tofind b. By (84), cos c = cos a cos b COS C from which cos b = -- = cos C sec a (91) Check. We have between A, B, and b, the relation cos B = sin A cos b EXAMPLES. 1. Given c = 140~, a = 20~; solve the triangle. By (89). By (90). By (91). c,logcosec 0.1919325 log cqt - 0.0761865 log cos - 9.8842540 a, log sin 9.5340517 log tan + 9.5610659 log sec + 0.0270142 log sin A 9.7259842 log cos B - 9.6372524 log cos b - 9.9112682 log sin A + 9.7259842 Cheek. log cos B - 9.6372524 Ans. A== 32~ 8'48".1 B = 115~ 42' 23".8 b = 1440 36' 28".4 2. Given c = 101~ 16' 16".7, b = 115~ 42' 38".5; find A. Ans. A = 65 32' 56".4 54. When a = c and consequently both = 90~, sin A = 1, A 90~, and 0 0 cosB =- cos b- =C0 cosco b BO that B = b, but both are indeterminate as in Art. 52. r2 174 SPHERICAL TRIGONOMETRY. 55. CASE III. Given one angle and its opposite side, or A and a. We shall have sin a sin A = s. whence sin c = cosec A sin a (92) tan A tan a sin b = cot A tan a (93) sin B =cos A sin B = cos A see a (94) cos a Check. sin b = sin c sin B In this case, there are always two solutions, all the required parts being determined by their sines, and the ambiguity not being removed by either Art. 49 or Art. 50. This also appears from Fig. 7. Fig. 7. If AB and AC be produced to meet in A', ABA' and A ACA' are semicircumferences and A -A'; the triangles ABC and A'BC both contain the given parts A and a, c but c', 1' and B' are respectively the supplements of c, b and B. It must not be inferred that in every case all the required parts are less than 90~ in one triangle, and greater than 90~ in the other; but the proper values for each triangle must be selected by Arts. 49 and 50. A' EXAMPLES. 1. Given A = 100~, a = 112~; solve the triangle. Ans. c = 70~ 18'10.2 )c = 1090 41'49".8 b=154~ 7'26".5 or b = 250 52'33".5 B = 152~ 23' 1".3 B= 27~ 36'58".7 2. Given A = 80~, a = 68~; solve the triangle. Ans. c= 70 18'10"2 ) c= 1090 41'49'.8 b = 25 52' 33".5 > or 6 = 154~ 7' 26".5 B- 27 36' 58".7 J tB 152 23' 1".3 8. Given B = 150~, b = 160~; solve the triangle. Ans. = 136~ 50' 23"3 ) c 43~ 9' 36".7 a= 39~ 4'50".7 or a = 140~ 55' 9".3 A = 67~ 9'42".7 )A = 112~ 50'17".3 SOLUTION OF SPHERICAL RIGHT TRIANGLES. 175 56. CASE IV. Given one angle and its adjacent side, or A and b. We shall find the required parts by the equations cos B sin A cos b (95) tan a =tan A sin b (96) cot c = cos A cot b (97) Check. cos -B tan a cot c EXAMPLES. 1 Given A = 80~ 10' 30", b = 155~ 46' 42".7; solve the triangle. Ans. B = 153~ 58' 24/.5 a= 67~ 6'52".6 C = 110~ 46' 20".0 2. Given B = 152~ 23' 1".3, a = 112~ 0' 0"; solve the triangle. Ans. A = 100~ b=154~ 7'26"<5 c= 70 18'10".2 57. CASE V. Given the two sides, a and b. We find the required parts by the equations cos = cos a cos b (98) cot A = cot a sin b (99) cot B = sin a cot b (100) Check. cos c = cotA cot B EXAMPLE. Given a = 116, b = 16~ solve the triangle. Ans. c = 114~ 55' 20'.4 A = 970 39'24".4 B - 17~ 41' 39"9 58. CASE VI. Given the two angles, A and B. The required parts are found by the formule cos c = cot A cot B (101) cos a = cos A cosec B (102) cos b = cosec A cos B (103) Check. cos c = cos a cos b 176 SPHERICAL TRIGONOMETRY. EXAMPLE. Given A = 60~ 47' 24".3, B = 57~ 16' 20".2; solve the triangle. Ans. c 68~ 56' 28".9 a = 54~ 32' 32".1 b 51~ 43' 36".1 ADDITIONAL FORMULE FOR THE SOLUTION OF SPAERICAL RIGHT TRIANGLES. 59. As in plane trigonometry, cases occur in which particular solutions of greater accuracy than the ordinary ones are required. (P1. Trig. Art. 112.) 50. From (89) we find 1 -sin A sin c - sin a 1+ sin A sin c - sin a which by P1. Trig. (154) and (109) is reduced to tan2 (450 - ~ A) = an (c - ) (104) tan 4 (c + a) (104) which will give a more accurate result than (89), when A is nearly 90~. 61. From (91) we find 1 cosb cos a-cos c 1 +cosb cos a + cos c or tans ~ b = tan ~ (c + a) tan ~ (c - a) (105) which may be employed instead of (91) when b is small, or nearly 1800. 62. From (90) we find 1 cos B tan c - tan a -- cos B tan c + tan a tan B sin (c a) (106) 2 sin (c + a) which may be employed instead of (90) when B is small, or nearly 180~. 63. By similar transformations the formula (101), (102) and (103) become tan' c = s (A - B) (107) tan2 ~ a - tan [I (A - B) - 45~] tan [45~ +- (A - B)] (108) tan2 - b = tan [- (A + B)- 45~] tan [45~0- 4 (A- B)] (109) We have also, by (14), - cos (A 4- B) - cos C sn" - c 2 2 sin A sin B which, when C =90~, becomes - - cos (A +- B) sin2 2 c - -- (A — + (110) 2 2 sin A sin and from (15), in the same manner, cos (A - B) 2 sin A i si/) (111) QUADRANTAL AND ISOSCELES TRIANGLES. 177 of which (110) may be used when c is small, and (111) when c is nearly 180~, instead of (101). 64. The equations (92), (93), and (94), of CASE III. give tan I (A — a) tans (45~ — ~ C) -t 2 ((A+ ) (112) sin (A - a) tan (450 b) - si (A ) (113) b) sin (A + a) tan2 (45~- 2 B) = tan a (A - a) tan -- (A + a) (114) The roots of these equations having the double sign, we may take the angles 45~ - I c, etc. either with the positive or negative sign, whence the two solutions of the problem, as in Art. 55. 65. Some of the solutions may be adapted for computation by the table of natu. ral sines. Thus from (86), (95), and (98), sin a = - [cos (c -A)- coS (c + A)] (115) cosB=- 2 [sin (b + A) - sin (b - A)] (116) cos c [cos (a + b) + cos ( - b)] (117) 66. The following relations are occasionally useful: From (83) we have cos a sin A cos A sin 2A (118) cos b sinB cos B sin 2B ( From (80) and (83), sin B sin A cos A sin 2 A sin c sin a cos a sin 2 a From (80) and (84), sin A sin a cos a sin 2 a ( = _ _ =-.-_ (120) cos b sin c cos c sin 2c 67. Various relations may be deduced from the general formulae of the preceding chapter by making C = 90~. The following are easily obtained: sin (c - a) cos c tan b tan - - cos a sin b tan 2 B sin (c - a) = cos c tan b cot 4 B = cos a sin b cot 4 B cos (c - a) = cos b + sin a sin b tan -2 B cos (c - a) = cos b - sin a sin b cot - B sin (a - b) = 2 sin c sin 4 (A +- B) sin -- (A - B) sin (a + b) =2 sin c cos 4- (A + B) cos 4 (A -B) cos I a cos I b sin - a sin b sin S= cos S =- - cos I c cos c tan S = -cot 1 a cot ~ b (121) QUADRANTAL AND ISOSCELES TRIANGLES. 68.. The polar triangle of the right triangle is a quadrantal triangle, one side (the side opposite the angle C) being equal to 90~. The solution of such triangles is as simple as that of right triangles, the formula for the purpose being obtained from the preceding, by the process of Art. 8. It is unnecessary to produce them here, as quadrantal triangles are generally avoided in practice, and when unavoidable are readily solved by means of the polar triangle. An isosceles triangle is easily solved by dividing it into two right triangles by a trerpendicular from the angle included by the equal sides. 23 179 SPHERICAL TRIGONOMETIY. CHAPTER IIL SOLUTION OF SPHERICAL OBLIQUE TRIANGLES. 69). In the solution of spherical oblique triangles, a required part may sometimes be found by its sine, in which case there will be two values of that part, answering to the conditions, unless the proper value can be determined by other considerations. In certain cases, the true value can be selected by applying one or more of the following principles, some of which are demonstrated in geometry. We still consider only those triangles each of whose parts is less than 180~0 I. The greater side is opposite the greater angle, and conversely. II. Eaclh side is less than the sum of the other two. 'III. The sum of the sides is less than 360~. IV. The suzm of the angles is greater than 180~. V..Each angle is greater than the difference between 180~ and the sum of the other two angles. For, by IV., whence, A + B + C> 1800 A > 180~ - (B + C) Fig. 8. But if B + C> 180~, we have, in the polar A' triangle, A'B'C', Fig. 8, by II., c'/ A \b' a' < b' + -' C/\ b or 180~- A< 180~ -B + 180~- C — 800 so - (B + C) B'- A > (B )- C)-1800 VI. A side which differs more from 90~ than another side, is zn the same quadrant as its opposite angle. For, by (4), we have cos a - cos b cos c cos A = - i sin b sin c in which the denominator is always positive. If, then, a differs SOLUTION OF SPHERICAL OBLIQUE TRIANGLES. 179 more frcm 90~ than b or than c, we have, (neglecting the signs for a moment), cos a > cos b or > cos c and still more cos a > cos b cos c Hence cos a being numerically greater than cos b cos c, the sign of the whole numerator, and therefore the sign of cos A, is the same as that of cos a; that is, A and a are in the same quadrant. VII. An angle which differs more from 90~ than another anylc. is in the same quadrant as its opposite side. For, by (5), cos A + cos B cos C cos a =.-.-a cos a- sin B sin U in which, if A differs more from 90~ than B, or than C, cos A determines the sign of the whole fraction, and therefore the sign of cos a. VIII. In every spherical triangle there are at least two sides which are in the same cuadrants as their opposite angles respectively. This follows from VI. and VII. IX. The sum of two sides is greater than, equal to, or less than, 180~, according as the sum of the two olpposite angles is greater than, equal to, or less than, 180~. In other words, the half sum of two sides is in the same quadrant as the half sum of the opposite angles. For, by (41), tan 1 (a + b) cos -1 (A + B)-= tan Ic coS 1 (A - B) the second member of which is always positive, so that tan - (a -L b) and cos I (A + B) must have the same sign. 70. CASE I. Given two sides and the in- Pig. 9. a eluded angle, or b, c and A. (Fig. 9.) First Solution; when the third side and a one of the remaining angles are required. \ To find a. The relation between the given A parts b, c, A and the required part a is expressed by the first equation of (4), cos a = cos c cos b + sin c sin b cos A () by which a may be found by computing separately the two terms of the second member and adding their values to form the natural cosine of a; but we should thus be required to use, besides the table of log. sines, also the table of logarithms of numbers, and the table of natural sines and cosines. To adapt it for logarithmic computation by the table of log. sines exclusively, we employ the process of 180 SPHERICAL TRIGONOMETRY. P1. Trig., Arts. 174, 175. Thus, let k be a number and cp an auxiliary angle such that k sin p = sin b cos A k cos P = cos b ( then (M) becomes cos a = k (cos c cos cp + sin c sin p) = cos(c - ) (mn so that k and cp being found from (m) we may find a by (m'). But we may eliminate k by dividing the first equation of (m) by the second, cos b and substituting in m' the value of —, whence we have, for cos (p finding a, tanp = tan b cos A c cos (c - q) cos b (122) cos (p which are the formulae commonly employed.* To find B. The relation between b, c, A and B, is, by the first equation of (10), sin c cot b -cos c cos A cotB=- - sin A (N) This may be adapted for logarithms by the process above employed, but to assimilate it to (M) we multiply the numerator and denominator of the second member by sin b, whence cot B sin c cos b - cos c sin b cos A sin b sin A which by (m) becomes t k sin (c - (p) t sin b sin A (n) sin b cos A or substituting the value of k = sin -, the formula for finding B aren tan <p = tan b cos A ) tB sin (c-(p) cot A S(123) sin p J * We might have assumed k sin cos 6, k cos ~, = sin 6 cos A, which would have reduced (n) to cos a =- k sin (c + I). In this way all the solutions that follew may be varied. SOLUTION OF SPHERICAL OBLIQUE TRIANGLES. 181 In the use of these formulae, as indeed of all that follow, the signs of all the functions must be carefully observed, according to P1. Trig. Arts. 37 and 40. We may take q between 0 and 180~, less or greater than 90~, according as the sign of its tangent is positive or negative; or we may take it numerically less than 90~ in all cases, but positive or negative according to the sign of its tangent, (P1. Trig. Arts. 37 and 174). Check. The quotient of (n) divided by (m) is cot B tan (C- (p) cos a sin b sin A which multiplied by the following, from (3), sin a sin B = sin b sin A gives tan a cos B = tan (c - p) (124) by which the values of a and B, found by (122) and (123), may be verified. 71. If a and C were required, the solution would evidently be similar, only interchanging b and c, B and C. By the fundamental formulae we should have cos a = cos b cos c + sin b sin c cos A sin b cos e - cos b sin c cos A (0) cot C= - sin c sin A and denoting the auxiliary angle in this case by X, the logarithmic solution would be tan Z = tan c cos A cos (b - X) cos c COS a os a cos cos (125) cot C<_ sin (b -) cot A cot C:1=tn( sin % Check. tan a cos C0= tan (b -- Q SPHERICAL TRIGONOMETRY. EXAMPLES. 1 Given 6 = 120~ 0' 30", c = 70~ 20'20" A= 50~ 10' 10"; find a and B. By (122). b - 120~ 80' 30" log tan b - 0.2297071 A = 50 10' 10" log cos A + 9.8065322 p = 132~ 36' 44".2* log tan 4p - 0.0362393 c = 70~ 20'20".0 e - cp = — 62016'24".2 By (122). By (123). By (124). log cos (c —) + 9-6676893 log sin (c- ) - 9-9470304 log tan (c - )- 02793410 ar co log cos ~ - 0-1693898 ar co log sin - + 0-1331505 log tan a + 0-4291648 log cos b - 9'7055761 log cot A + 9 9212038 log cos B - 9.8501762 log eos a- 9 5426552 log cot B- 0 0013847 Check. -0-2793410 a 690 34' 55"'9 2. Given b = 120~ 30' 30", find a and 7. B = 135~ 5'28"/8 = 70~ 20' 20", A = 50~ 10' 10"; Ans. a = 69~ 34' 55",9 C = 50~ 30' 8".4 3. Given b = 99~ 40' 48", find a and B. 4. Given b = 990 40'48", find a and C. 5. Given b = 98~ 2' 20", find a and (. = 100~ 49' 30", A = 65~ 33'10"; Ans. a = 64 23' 15".0 B = 95~ 38' 4".0 c = 100~ 49' 30", A = 65~ 33' 10"; Ans. a = 64~ 23' 15".0 C= 97~ 26' 29".1 c =80~ 35' 40", A = 10~ 16' 30"; An8. a = 20~ 13' 30".1 C= 30~ 35' 56".7 72. If B, C and a were all required, we might find a and C by (125), and then B by Art. 3, which gives sin a: sin b - sin A: sin B or sin b sin A sin B = sin a sin a ' We may also take p = -470 23' 15"'8, whence c- = 117~ 43' 35" 8S which will give the same values of a and B as found in the text SOLUTION OF SPHERICAL OBLIQUE TRIANGLES. Of the two values of B less than 180~ given by this formula, the proper one may generally be selected by the principles of Art. 69. There are cases, however, in which all the conditions there given are satisfied by both values of B,* and on this account it is preferable, in general, to combine (123) and (125), or to employ the following solution, when the three unknown parts are all to be found. 73. CASE I. Given b, e and A. Second Solution; when the two remaining angles are required, or when the three unknown parts are all required. We have, by Napier's Analogies, (42) and (43), sin 2 (b + c) sin - (b - c) cot - A: tan I (B - C) cos i (b + c): cos i (b - c) cot A: tan 1 (B + C) whence tan ~ (B- C)= ncot 1 A (126) sin ~ (b + c)cot tan (B + (7) 2 ) cot -1 A (127) 2 v / cos (6b + () 217 which determine ~ (B - C) and ~ (B + C); then the half difference added to the half sum gives the greater angle, and the half difference subtracted from the half sum gives the less angle. If c > b, we may write c - b, C - B, in the place of b - c, B - C. We may now find a by either of Napier's Analogies, (40), (41), which givet tan a sin2 (B tan 1 (b - c) (128) tan a = cos(B- tan 1 (b + c) (129) tan oas(B-C) 2 *B By Art. 69, VI., if b differs more from 90~ than c, B is in the same quadrant as b, and all ambiguity is removed. If c differs more from 90~ than b, we may finn a and B by (122) and (123), and then C by the formula sin c sin A sin C = — sin a C being taken in the same quadrant as c. t We may also find a from any one of Gauss's Equations (44), which become, ir the present case, cos 4 a sin 4 (B + C) = cos j A cos ~ (b - c) cos a cos (B + C) = sin } A cos 4 (b + c) sin - a sin (B - C) cos 4 A sin (b - c) sin i a cos 1 (B - C) = sin 4 A sin 4 (6 + c) t84 SPHERICAL TRIGONOMETRY. EXAMPLES. 1. Given b = 120~ 30' 30", c = 700 20' 20", A = 50~ 10' 10"; ind B, C and a. We have 1 (b + c)= 95~ 25' 25" 2 (b - c) = 25~ 5' 5" 2A = 25~ 5' 5" By (126). Or co log sin 1 (b + c) + 0.0019487 logsin I (b - c) + 9.6273228 log cot 1 A + 0.3296529 log tan I (B - C) + 9.9589244 ~ (B - C)= 42~ 17' 40".2 B = 135 5' 28".8 By (128). arco log sin (B — C)+0.1720227 log sin 2(B+ C) +9.9994824 logtan ( 6 - e )+9.6703471 log tan 1 a + 9.8418522 a = 340 47' 28".0 By (127). ar co log cos ~ (b + c) - 1.0244829 log cos 2 (6 - e) + 9.9569757 log cot A + 0.3296529 log tan I (B + C) - 1.3111115 (B + C) = 92~ 47' 48".6 C= 50~ 30' 8".4 By (129). ar co log cos I(B- C))+ 0.1309469 log cos-(B+ C)- 8.6883709 log tan 1(b + c)- 1.0225342 log tan 2 a + 9.8418520 Ans. B = 135~ 5' 28".8 C= 50~ 30' 8".4 a = 69~ 34' 56".0 2. Given b = 99~ 40' 48", c = 100~ 49' 30", A = 65~ 33' 10"; find B C and a. Ans. B = 95~ 38' 4".0 a = 97~ 26' 29".1 a = 64~ 23' 15".1 74. It may be remarked with regard to (128) and (129) that, when b and c (and consequently B and C) are nearly equal, a small error in the previous determination of the small angle 1 (B - C) may produce a large one in log sin i (B - C), and consequently in log tan 2 a found by (128). In that case, therefore, (129) must be preferred. In like manner, if I (b - c), and consequently I (B +- C), are nearly equal to 90~, (129) will become inaccurate, and then (128) is to be preferred. Formula (128) would fail entirely if B = C, and formula (129) would fail if i (B + C') = 90~, since the second members inthese cases would assume the inde0 terminate form -. 75. CASE I. Given b, c and A. Third Solution. When the third side is alone required, the computation by (122) is in most cases as convenient as any other; but the e are various other methods SOLUTION OF SPHERICAL OBLIQUE TRIANGLES. 185 derived from the formulae of the preceding chapter, which havw been employed with advantage in particular applications. Among the most convenient are the following, from (12) and (13): cos a = cos (b - c) - 2 sin b sin c sin2 - A (130) cos a = cos (b + c) + 2 sin b sin c cos2 I A (131) The computation of these requires the use of natural cosines and numbers, the signs of which must be carefully observed. EXAMPLE. Given b = 99~ 40' 48", c = 100~ 49' 30", A = 65~ 33' 10"; find a. By (130).* = A 32~ 46' 35" b- c= - 1~ 8'42" log sin2 1 A = 2 log sin I A 9.4669752 log sin c 9.9922023 log sin b 9.9937722 log 2 0.3010300 - 0.5675181 log 9.7539797 - 2 sin b sin nat cc c sin2 A = ff )s (b - c) = + 0.9998003 nat cos a =- + 0.4322822 By (131). a = 64~ 23' 15" 2 A = 32~ 46' 35" b + c = 200~ 30' 18" log cos2 2 A = 2 log cos ~ A log sin c log sin b log 2 = + 1-3689240 log 9.8493748 9.9922023 9.9937722 0.3010300 0.1363793 + 2sin b sin c cos2 A = nat cos (b + c) = - 0.9366416 nat cos a = + 0.4322824 a = 64~ 23' 15" 76. In Art. 14, we have deduced several formulae by which ~ a may be computed We may adapt (17) and (18) for logarithmic computation, as follows: sinS0 = sin b sin c cost I A sin' I a = sin 1 (D + c) - sin" sin [I (b + c) -+ 0] sin [I (b + c) - 0] } (132) sin2 0 = sin 6 sin c sin2s A coss I a = cos I (b - c) - sins 0 J (133) cos [I (b - c) + P] cos [~ (b -c) — ] ) of which (132) is to be preferred when 1 a < 45~, and (133) when I a > 45~. 2I * The computation of (130) is facilitated by the use of a special table (given in many treatises on navigation), from which, with the argument A is taken the logarithm of 2 sin2 ~ A = versin A. [P1. Trig. (4) and (139)] M4 2 186 SPHERICAL TBIG(ONOMETRY. Fig. 9. C a, 5~2B ' C _~~~ 77. CasE II. Given two anyles ani the included side, or A, C and b. (Fig. 9). First Solution; when the third angle and one of the remaining sides are required. To find B. The relation between A, 6, b and B, is, by (5), cos B = - cos a cos A + sin C sin A cos b (M) which is adapted for logarithms by the method employed in the preceding case. Thus, let h sin 9 = cosA h cosS = sin A cos b then (M) becomes cos B = (sin C cos -- cos C sin -) =h sin (C —) cos A or, eliminating h c= i 9' the formula for finding B are 9 ~ sin th cot S = tan A cos b cos sin (C - ) cos A sin n (inm) (ml (134) To find a. From the third equation of (10), we find, sin 0 cot A + cos C cosb cot a = sin b sin C cosA + cos Csin A cosb siA sinA in b which, by (m), becomes h cos (C — ) cot a -= - sin A sin b sin A cos b or, eliminating h = cs - we have, for finding a, cot - = tan A cos b cos (C- )cot b cot a = -- cos ' (N) (n) (135) As in the preceding case, we may either take 9 always between 0 and 180~, less or greater than 90~ according as its tangent is posi SOLUTION OF SPHERICAL OBLIUE TRIANGLES. 187 tive or negative; or we may take & numerically less than 90' in all cases, positive or negative, according to the sign of its tangent. (PI. Trig. Art. 174.) Check. The quotient of (n) by (m') is cot a cot (C - ) cos B sinsin A sin b which, multiplied by sin B sin a = sin A sin b gives tan cos a =cot (C- b) (136) by which the values of B and a, found by (134) and (135), may be verified. 78. If B and c were required, the solution would be similar, only interchanging a and c, A and C. By the fundamental formulae, we should have, cos B = - cos A cos C + sin A sin Ccosb sin A cos C + cos A sin C cos b (o6 cot c = sin C sin b and denoting the auxiliary angle by ', the logarithmic solution would be cot = tan C cos b sin (A - <) cos C cos - sin < (1871 cos (A - ) cot b cot c - cos C Check. tan B cos = cot (A - ) EXAMPLES. 1. Given A = 135~ 5' 28".8, C= 50~ 30' 8".4, b = 69~ 34' 55".9; find B and a. By (134). A = 135~ 5'28"'8 log tanA - 9'9986154 b = 69~ 34' 55"-9 log cos b + 9-5426553 = 109~ 10' 31".0* log cot 9- 9.5412707 C = 50~ 30' 8".4 C-9&=- 58040'22'.6 - We may also take = - 70~ 49' 29"'0, whence C -- = 121~ 19' 37"'4, which will evidently give the same results as those obtained in the text. L88 SPHERICAL TRIGONOMETRY. By (134). By (135). log sin (C-A)- 99315664 logcos (C —) + 9-7159386 ar co log sin &-+0 0247897 ar co log cos&-0-4835187 log cos A- 9-8501762 log cot b - 9-5708352 log cos B-+ 9-8065323 log cot a - 9-7702925 B= 500 10'10"-0 a —1200 30' 29"9 By (136). log cot (C- a) - 9.7843722 log tan B +0-0787962 log cos a -9-7055757 Check. -9-7843719 Ans. B= 50~ 10'10"oU a = 1200 30' 29"-9 2. GivenA= 135~ 5'28"'8, C= 50030'8"'4, = 69034'55"/9; find B and c. Ans. B = 50~ 10' 10"/0 C = 700 20'20"0 3. Given A = 650 33 10", find B and a. C = 95~ 38' 4", b = 100~ 49' 30,; 4. Given A=97~ 26' 29", find B and a. Ans. B= 97~ 26'29" a = 64~ 23'15" C = 95~ 38' 4", b =64~ 23'15"; Ans. B= 650 33'10" a = 100~ 49' 30' 79. If a, c and B were all required, we might find B and c by (137), and then a by Art. 3, which gives, sin B: sin A = sin b: sin a sin A sin b si snB (138) Of the two values of a given by this equation, the proper one is to be selected, if possible, by the principles of Art. 69.* But as cases occur in which all the conditions there given are satisfied by both values of a, it is preferable, in general, to combine (135) and (137), or to employ the following solution when the three unknown parts are all to be found. * By Art. 69, VII., when A differs more from 90~ than C, a must be taken in the same quadrant with A, and all ambiguity is removed. If, then, by A we always denote that angle which differs more from 90~ than the other given angle, we may always solve this case by means of (187) and (138), without meeting with any ditCfi culty in determining the quadrant in which a is to be taken. SOLUTION OF SPHERICAL OBLIQUE TRIANGLES. 189 80. CASE II. Given A, C and b. Second Solution; when the two remaining sides, or when the three unknown parts are all required. We have, by Napier's Analogies, (40) and (41), sin 4 (A + C): sin - (A - C) = tan 1 b: tan - (a - c) cos 1 (A + C): cos 4 (A - C) = tan 4: tan 4 (a + c) whence sin -L (A - C) tan - (a -?) =., tan - 5 2tan / s(in c) (A + C) 2 tan CCos (a c) tan - tan 1 i(a + =tan i T(139) which determine 1 (a - c) and 1 (a + c); then the half difference added to the half sum gives the greater side, and the half difference subtracted from the half sum gives the less side. If C> A, we may write C - A, c - a in the place of A - C, a - c. We may now find B by either of Napier's Analogies, (42) and (43), which give* sin 4 (a + c) cot B = 2 tan (A- C) 2 sin 4 (a - c) cot}B/-: cos (a + ctanA+ cos - (a -- ) tc (140) (141) EXAMPLES. 1. Given A = 135~ 5' 28".6, C = 50~ 30' 8"6, b = 69~ 34' 56"2; find a, c and B. We have 1 (A + C)= 92~ i7' 48".6 (A - C) = 420 17'40".0 1 b = 34~ 47' 28"1 Then, by (139), ar colog sin' (A+ C)+0.0005176 log sin} (A- C)+9.8279768 log tan b + 9.8418527 tog tan} (a - c) +9.6703471 2(a-c)= 25~ 5' 5".0 a = 120~ 30' 30".0 ar co log cos (A + C)-1.3116286 log cos~(A- C)+9.8690535 log tan 46 b -9.8418527 logtanl(a + c) -1.0225348 4 (a + c)= 95~ 25' 25".0 = 70~ 20'20".0 * We may also find B by any one of Gauss's Equations, (44), interchanging B %nd C, b and c. 190 SPHERICAL TRIGONOMETRY. By (140). ar co log sin ( a - c) + 0.3726772 log sin( a + c) + 9.9980523 logtan2(A- C)+ 9.9589234 log cot 2 B + 0.32'6529 B = 250 b' 5"0 By (141). ar co log cos( a - c) + 0.0430243 log cos}( a + c) - 89755171 log tan~(A+ C) - 1.3111110 *log cot 2 B + 0.3296524 Ans. a = 120~ 30' 30" = 700 20'20" B= 50 10'10" 2. Given A 95~ 38' 4", C = 97~ 26' 29", b = 64~ 23' 15"; find a, c and B. Ans. a= 99~ 40'48" c = 100~ 49' 30" B = 650 33'10" 81. CASE II. Given A, C and b. Third Sotltion. Wzen the thiqrd angle B is alone,'equ,^ed, the computation by (134) is in most cases as convenient as xny Ather, but there are other methods (corresponding to those given iA Art. 75 for finding a) which may occasionally be serviceable. By 114) and (15) we have cos B= - cos (A + C) - 2 sin A sin C sin2 - b (142) cos B= - cos (A - ) + 2 sin A sin C cos2 b (143) the computation of which is similar to that of (130) and (131). Given A = 95~ 38' 4", find B. b = 32~ 11'37".5 A + C =193~ 4'33" EXAMPLE. C= 97~ 26'29", b = 64~ 23'15"; By (142). log sin2 6b = 2 log sin 6 b 9.4531022 log sin A 9.9978967 log sin C 9.9963268 log 2 0.3010300 - - 0.5602162 log 9.7483557 - 2 sin A sin Csin2 1 b - nat cos (A + C) = + 0.9740715 nat cos B = - 0.4138553 B = 65 33' 9"' * For the reasons given in Art. 74, (141) is, in this example, not so accurato as (140). SOLUTION OF SPHERICAL OBLIQUE TRIANGLES. 191 82 In Art. 14, several formulae are given, by which - B may be computed By (21) and (22) we have sin I B cost2 (A - C) - sin A sin C cos~ b cos2 4 B sin2 4 (A - C) - sin A sin C sin' 4 b which may be adapted for logarithms, thus: sin' 2 = sin A sin C cos' 4 b sin j4 B = cos' 4 (A - C) - sin (144) = cos [ (A- ) + 0] cos [4 (A- - ) 0] sin 0 = sin A sin C sin2 I b cosS2 B sin2 4 (A + C) - sin 0 (145) sin [4 (A + C) + 0] sin [i (A + C)- p] of which (144) is to be preferred when 4 B < 45~, and (145) when I B > 45~. 83. Case II. might have been reduced to Case I. by means of the polar triangle, Art. 8; for there will be known in the polar triangle, two sides and an angle oppobite one of them, being the supplements of the given angles and side of the proposed triangle. The polar triangle being solved, therefore, by Case I., and its two remaining angles and third side found, the supplements of these parts would be the two sides and third angle required in the proposed triangle. It is easily seen, also, that all the formulas above given for this case might have been obtained by these considerations. 84. CASE. III. Given two sides and an ig. 9. angle oppos;Te one of them; or a, b, and A. Fig. 9. a First Slution, in which each required part is deduced directly from fundamental AB A -i formrta independently of the other two parts. c To find c. We have, by (4),* cos c cos b + sin c sin b cos A = cos a (M) t9 molve which, let k sin p = sin b cos A k cos p cos b then (M) becomes c cos (e - p) = cos a or putting c - (p = ', k cos '== cos a = +, +(i * This formula has been already employed and adapted for logarithms in Case 1; but, for the sake of clearness, it is repeated. The student will remark that a simple transformation of (122) gives (146). It will also be observed that the given angle and the given side adjacent to it, in each of the first four cases, are denoted by A and b. in order that the auxiliaries p and e may have the same values throughout 192 SPHERICAL TRIGONOMETRY. The auxiliary cp will be fully determined by (m), being taken between 0 and 180~, and always positive (P1. Trig. Art. 174); but, as the cosine of an angle is also the cosine of the negative of that angle [PI. Trig. (56)], we may take (' in (m') either with the positive or the negative sign, so that c = p =~ p'. There will thus be two values of c answering to the same data, both of which will be admissible, except when (p + (' exceeds 180~, in which case the only solution is c = - p —'; and except when ep' exceeds cp (which would make c negative), in which case the only solution is c = p + (p'. Therefore, eliminating k, we have for finding c, tan p = tan b cos A cos ' cos s cos a (146) cos b c= <p fc ' J To find C. We have by (10), cos C cos b + sin C cot A = sin b cot a or, multiplying by sin A, cos C sin A cos b + sin C cos A = sin A sin b cot a (S) to solve which, let h sin = cos A h cos = sin A cos b then (N) becomes h cos (7 - -) = sin A sin b cot a or putting - 9 = ', h cos ' = sin A sin b cot a C a + 9' Here - will be fully determined, while 9' found by its cosine may be either positive or negative, so that we shall have in general two values of C( = - 9', corresponding respectively to the two values of c; but, as before, values greater than 180~, and negative values, being excluded, there will in certain cases be but one solution. sin A cos b Eliminating h = —, we have, then, for finding C, cos 1^7 SOLUTION OF SPHERICAL OBLIQUE TRIANGLES. 193 cot = tan A cos b cos 9'= cos - tan b cot a (147) (o g& 4 J To find B. We have several methods: 1st, directly by (3), sin A sin b(148) ~~~sinn a which gives two values of B, supplements of each other, corresponding respectively to the two values of c and C. We shall presently see how to determine which are the corresponding values of c, C and B. 2d. In (123), ( has the same value as in (146), and therefore putting in (123), - cp = p', we have sin q' cot A cot B = -- (149) sin (P which gives two values of B by the positive and negative values of p'. 3d. By (124), cos B = tan I' cot a (150) which also gives two values of B by the positive and negative values of p'. 4th. In (134), 9 has the same value as in (147), and therefore put ting in (134), C - & = ', sin 9' cos A cos B = sin (151) sill S v which gives two values of B, as before. 5th. By (136), cot B = tan y' cos a (152) which gives two values of B, as before. The formula (149) shows that when p' is positive, cot B and cot A have the same sign, that is, B and A are in the same quadrant; and that, when cp' is negative, cot B and cot A have different signs, that is, B and A are in different quadrants. A like result follows from (151), with reference to y'. Hence, that value of B which is in the same quadrant as A, belongs to the triangle in which c = -p +;', C = - + -'; and that value of B which is in a different quadrant from A, belongs to the triangle in which e = e - I', C = - a'. This precept enables us to employ (148) without ambiguity. In the 25 R m9s SPHERICAL TRIGONOMETRY. use of (149), (150), (151) and (152), it is only necessary carefully to observe the signs of the several terms. CIecJcs. Of the various formulae above given for finding B, one or more may be employed for the purpose of verification. When c and 0 have been found, the most simple check is the following, from (3), sin C sin A sin c sin a (153) which, indeed, might have been employed to find C, after c was found, and reciprocally, but for the ambiguity attaching to the sines. 85. According to Art. 69, VI., if b differs more from 90~ than a, B must be in the same quadrant as b, and, since but one of the two values of B can satisfy this condition, there will be but one solution. In that case c and C' will each be found to have but one admissible value. 86. The problem will be altogether impossible, when a differs more from 90~ than b, and is yet not in the same quadrant with A. In such case, we should find that ( + p'> 180~, and p - ' < 0; +S > 180o, 3- ' < 0. The problem will also be impossible, when sin A sin b > sin a, since, by (148), we shall then have sin B > 1. EXAMPLES. 1. Given a = 40~ 16', b = 47~ 44', = 52~ 30'; find B. a = 40~ 16' b = 47~ 44' A= 52~ 30/ B = 65~ 16' 35" or B = 114~ 43' 25" By (148). ar co log sin a 0-1895350 log sin b 9-8692449 log sin A 9-8994667 log sin B 9-9582466 2. With the same data, find c and B. a= A== By (146.) 40~ 16' log cos a+9.8825499 47~ 44' log tan b +0.0414996 ar co log cos b+0.1722547 52~ 30' log cos A+ 9.7844471 330 48' 51".4 log tan (+9.8259467 log cos p + 9.9195204 ~'==-19~ 30' 29".0 P,= 530 19'20".4 e-= 14~ 18'22"'4 log cos p'+9 9743250 SOLUTION OF SPIERICAL OBLIQUE TRIANGLES. 195 By (149). Check. (150). cp = 330 48'51".4 arcologsin(p+0.2545328 log cot a+ 00720848 c' =I- 19 30'29".0 log sin'~-9.5236676 logtanp':~9.5493427 A= 52030' 0" logcotA+9 8849805 i-9621427.5 B, 65 114~ 34o"1} logcotB-I9-6631809 logcosBi=9-6214275 B,=- 114043'25"l1 Ans. e = 53~ 19' 20"'4 14~ 18' 22/'4 B = 65~ 16' 34/"9 or B = 114~ 43' 25"'1 8. Given a = 120~, b = 70~, A = 130~; find C and B. By (147). a = 120~ log cot a -9.7614394 b = 70~ log cos b +9.5340517 log tan b +0.4389341 A = 130~ log tan A- 0.0761865 9-= 112~ 10' 33".6 log cot - -9.6102382 log cos 9 —9.5768627 ' = 53~ 13' 13".8 log cos 9'+9.7772362 C= 165~ 23'47".4 C= 58 57' 19".8 By (151). Chek. (152). - = 112 10'33".6 ar co logsin -+ 0.033755 log cos a —96989700 9'=-= 530 13'13".8 logsin9'~:9.9036030 logtanY'~=0.1263669 A= 130~ 0' 0" logcosA-9.8080675: =9.8253369 f> 123"~ 46'37". 5 } B= 560 13'22".5 log cosBq:9.7450460 log cot BTF9.8253369 Ans. C= 165~ 23'47'".4 C = 58~ 57'19".8 B =123 46' 37".5 or B = 56 13' 22".5 4. Given a = 70~, b = 120~, A = 130~; find C. By (147). a - 70 log cot a + 9.5610659 b = 120~ log cos b - 9.6989700 log tan b - 0.2385606 A = 130~ logtanA- 00761865 9 = 59~ 12' 37".0 log cot 9 + 9.7751565 log cos 9 + 9.7091756 9' -= -108~ 49'35".1 logcos9' - 9.5088021 = 168~ 2 12".1, taking 9' with the positive sign only, since its negative value would render C negative. l'. g SPHERICAL TRIGONOMETRY. 5. Given a = 99~ 40' 48", b = 64~ 23' 15", A = 35- 38'4"; find C, Cand B. Ans. c =100~ 49 30" C= 97~ 26' 29" B = 65~ 33'10" 6. Given a = 40~ 5'25".6, b = 118~ 22'7".3, A = 29~ 42' 33" 8 find c, C and B. Ans. c = 153~ 38' 42".4) ( c 90~ 5'41".0 ==160~ 1'24".4 or C= 50~18'55".2 B= 42~ 37'17".5 B 137~ 22' 42".5 7. Given a = 69 34' 56", b = 1200 30'30", A = 50 10' 10"; find c and (7. Ans. = 70~ 220'2 C= 50~ 30' 8".4 8. Given a = 120~ 30' 30", = 69~ 34' 56", A = 50~ 10' 10"; find c and C. Ans. Impossible. 9. Given a = 40~, b = 60~, A = 50~; solve the triangle. Ans. Impossible. 87. CASE III. Given a, b and A. Second Solution. We find B by the formula sin A sin b sin B sin a and then by Napier's Analogies, (41) and (43), cos (A +B) tanc - ) tan (a + b) cot C= cos I (a - b) or by (40) and (42), sin I (A s o and o n two solutions, except when for one of these values the second meotr ers become negative, for c and b t l tan 90, theircotangents must be po si tiv 2 sin ~( a -- b ) in which we employ successively the two ~alues of B, and obtain two solutions, except when for one of these values the second merez hers become negative, for ~1 e and ~ C being less than 901, their tangents must be positive. SOLUTION OF SPHERICAL OBLIQUE TRIANGLES. 197 We leave it to the student to apply these formula to the preceding examples. 88. To determine by inspection of the data a, b and A, whether there are two solutions, or but one. 1st. It has already been seen, Art. 85, that when b differs more from 90~ than a, B must be in the same quadrant as b, and there can be but one solution. It remains to show, 2d. That when a differs more from 90~ than b, there will necessarily be two sol, *ions. We have, by the first of (4), cos a- cos b cos c sin csin b cos A Two solutions exist so long as both values of c are positive, and less than 1800, that is, so long as sin c is positive. Now when a differs more from 90~ than b, we have. (neglecting the signs for a moment), cos a > cos b > cos b cos c therefore the numerator of the above value of sin c has the sign of cos a. But by Art. 69, VI., a and A are in the same quadrant, and cos a and cos A have the same sign; consequently also, the numerator and denominator have the same sign, and the value of the fraction, or of sin c, is positive, as was to be proved.* Hence, there is but one solution when the side opposite the given angle differs less from0 90~ than the other given side, and two solutions when the side opposite the given angle difers more from 90~ than the other given side. 89. CASE IV. Given two angles and a side opposite one of them, or A, B and b. (Fig. 9). First Solution, in which each required Fig. 9. C part is deduced directly from the fundamental formulae. a To find c. We have, by (10), B sin c cot - cos cos A= sinA cot B A- =/ - or multiplying by sin b, sin c cos b - cos c sin b cos A = sin A cot B sin b (M) to solve which we take k sin q = sin 5 cos A k cos =p cos 6 * The same proposition may be otherwise proved thus. By the equations (m) %nd (m') Art. 84, we have cos b cos a sin b cos k sin c Cos 0 = k ~ cos IC- k = _. cos A from the third of which we see that k has the sign of cos A; if then a differs more from 90~ than b, that is, if cos a and cos A have the same sign, cos O' is positive, and 0' < 90~. Also since, (neglecting signs), cos a > cos b, we have cos a' > cos e, or O' differs more from 90~ than 0 Hence 0' < p and 0' < 180~ - 0, or 0 -' > 0 and 0 + I' < 180~, or both values of c are between 0 and 180~. R2 198 SPHERICAL TRIGONOMETRY. then, putting c -;p = p', (M) becomes k sin P' = sin A cot B sinb ) + e = p + z ' or eliminating k, we have, for finding c, tan p = tan b cos A sin c' = sin p tan A cot B (156) C = C + p' Here q' being determined by its sine, will have two values, supplements of each other, which being successively added to q, give two values of c. When the second member of the formula sin Ip' = sin gp tan A cot B is negative, sin p', and therefore p' is negative, and the two supplemental values of cp' must be successively subtracted from $. There will be two solutions, then, except when one of the values of c exceeds 180~, or when one of them is negative. To find C. We have, by (5), sin C sin A cos b - cos cos A = cos B (N) whence, if we put h sin 9- cos A h cos 9 = sin A cosb b and also a - 9- 'y, we have h sin Y = cos B (n') C =. ~, Eliminating h, we have cot — =tan A cos b. sin 9 cosB B sin 9 ---- cos A 1 157 e = + a' As 9' is also determined by its sine, it will have two supplemental values, which will both be added to or loth subtracted from $5, (according to the sign of sin 9',) thus giving two values of C, except when one of them exceeds 1800, or when one of them is negative. SOLUTION OF SPHERICAL OBLIQUE TRIANGLES. 1993 To find a. We have several methods: 1st, directly by (3). which gives sinb sin A sin a = -sin b (158) 2d. By (146), where p and q' have the same values as in this case, cos ' cos b cos a cos (1591 3d. By (150), cot a = cot I' cos B (160) 4th. By (147), where 9 and 9' have the same values as in this case, cos y' cot b cot a cos c (161\ cos9 5th. By (152), cos a = cot L' cot B (162) Each of the last four formula gives two supplemental values of a by the two values of p' or 9', employed in the second members. From (156) we have cos A = tan <p cot b which with (159) gives cos a sin b cosA = cos s' x insp The sign of the second member of this equation depends upon that of cos (p', since sin b and sin qp are always positive. Hence when cos qp' is positive, cos a and cos A must have like signs; and when cos P' is negative, cos a and cos A must have different signs. A like result follows from the first of (157) and (161) with reference to 'I. Hence, that value of a which is in the same quadrant with A belongs to the triangle in which (p' < 90~,:'< 90~; and that value of a zwhich is in a different quadrant from A belongs to the triangle in which p' > 90~, -' > 90~. This precept enables us to employ (158) without ambiguity. In the use of (159), (160), (161), and (162), it is only necessary to observe the algebraic signs of the several terms. Checks. Of the various formula above given for finding a, one or more may be employed for the purpose of verification. When c and 0 have been found, however, the most simple check is 200 SPHERICAL TRIGONOMETRY. sin C sinB (163) sin c sill which might have been employed for finding C after c was found, or reciprocally, but for the ambiguity attaching to the sines. 90. According to Art. 69, VII., if A differs more from 90~ than B, a must be in the same quadrant with A. But since the two values of a are supplements of each other, only one of them can satisfy this condition, and there will then be but one solution. In such case c and C will each be found to have but one admissible value. 91. The problem will be impossible when B differs more from 90~ than A, and yet is not in the same quadrant with b. In such case we should find both values of c (and both values of C) to be greater than 180~, or both negative. The problem will also be impossible when sin b sin A > sin B, since by (158) we shall then have sin a > 1. EXAMPLES. 1. Given A = 132~ 16', B = 139~ 44', b = 127~ 30'; find a. By (158). B = 139~ 44' 0" ar co log sin B 0.1895350 A = 132~ 16' 0" log sin A 9.8692449 b = 127~ 30' 0" log sin b 9.8994667 a = 65~ 16' 35".1 log sin a 9.9582466 or a = 114~ 43' 24".9 2. With the same data, find C and a. By (157). B= 139~44' 0" log cos B-9.8825499 A- 132~ 16' 0" log tan A-0.0414996 ar co log cos A-0.1722547 b= 127~30 " log cos b-9.7844471 - = 56~ 11' 8".6 logcotS +-9.8259467 log sin &+9.919 ronL 9=+ 70~29'31"'0 ] +:tl 2 } 109~0 30' 9".0 l}-...log sin &'+ 99743250 C0= 126o 40'39".6 CA= 1650 41'37"'F SOLUTION OF SPHERICAL OBLIQUE TRIANGLES. 201 By (161). Check. (162). a = 56~11' 8".6 arcologcos3-+0.2545328 logcot B-0.0720848 j~~~~ 0 } l co &tk95267 lo o> —.482 a'= 70~ 29'31". '2 =109~ 30'29". b =127~ 30' 0" a1 =114 43'25". a,= 65~ 16'34". 10 logcosS'~9.5236676 log cotY'~9.5493427 log cot 6-9.8849805 =F9.6214275 } log cot aF9.6631809 logcosaT=9.621427 Ans. C= 126~40'39".6 C= 165 41'37".6 a = 1140 43'25".1 or a = 65016'34".9 3. Given A = 110~, B = 600, b = 50~; find c and a. By (156). == A = b = 60~ 1100 500 logcosA-9.5340517 logtanb +0.0761865 logtanp —9.6102382 log cotB+ 9.9614394 logtanA-0.4389341 log sin p+ 9.5768627 log sin p'-9.7772362 p = 157049'26".4 (p'= — 36046'46".2 a= —143013'13".8 ce = 121~ 2'40"-2 == 14036'12"6 J By (159). G7ieck. (160). cp = 157~49'26".4 arcologcosp —0.0333755 log cosB+9.6989700 13-14'46131".2 } logcosp'~9 9036030 log cotp'q-0.1263669 b = 50~ 0' 0" logcosb +9.8080675 F9-8253369 =a 12346'37"5 1 logeos a =97450460 log cot a=F98253369 a = 56013'22//5 ) Ans. c = 121~ 2'40"'2 f c = 14~ 36' 12"'6 a = 1230 46' 37"5 or a -= 56~ 13' 22"'5 4. Given A = 60~, B= 110~, b = 50C; find c. Ans. e = 11~ 57/ 47".9 5. Given A == 115 36' 45", B = 80 19' 12", b = 84~ 21' 56": find a, c and (. Ans. a = 114~ 26' 50" c = 82~ 33' 1" C= 79~ 10' 30" 6. Given A = 61 37' 52"-7, B = 139~ 54'84".4, 6=150~ 17'26".2; Gnd a, c and C. Ans. a = 42~ 37'17'/5 a = 137~ 22'42".5 c = 129~ 41' 4".8 or c = 19~ 58' 35".6 C= 89~ 54'19".0 C= 26~ 21'17".6 26 202 SPHERICAL TRIGONOMET RY. 7. Given A 70~, B= 120~, b = 80~; solve the triangle. Ans. Impossible. a. Given A= 60~, B 40~, b = 50~; solve the triangle. Ans. Impossible. 92. CASE IV. Given A, B and b. Second Solution. We find a by the formula sin b sin A sin a = --- sin B and then by Napier's Analogies we find c and C, precisely as in Case III., Art. 87, employing successively, in (154) or (155), the two values of a given by the preceding equation. There will be but one solution, if one of these values renders the second members of (154) or (155) negative. The student should apply this method to the preceding examples. 93. To determine by inspection of the data A, B and b, whether there are two solutions or but one. 1st. It has already been seen, Art. 90, that when A differs more from 90~ than B, a must be in the same quadrant with A, and there can be but one solution. It remains to show that, 2d. When B differs more from 90~ than A, there will necessarily be two solutions We have, by (5), cos B-b cos A cos 0 sin C --- sin A cos b Two solutions exist so long as both values of C are less than 1800, and both positive, that is, so long as sin C is positive. Now when B differs more from 90~ than A, we have, (neglecting signs for a moment), cos B > cos A > cos A cos C therefore the numerator of the value of sin Chas the sign of cos B. But by Art. 69, VII., B and b are in the same quadrant, consequently the numerator and denominator have the same sign, and the value of the fraction, or of sin Cis always positive, as was to be proved.* Hence, there is butt one solution when the angle opposite the given side differs less from 90~ than the other given angle; and two solutions when the angle opposite the given side differs mnore from 90~ than the other given angle. 94. CASE IV. might have been reduced to Ca-e III. by means of the polar triangle of Art. 8. For there will be known in the polar triangle two sides and an angle opposite one of them, being the supplements of the given angles and side of the proposed triangle. The polar triangle being solved, therefore, by Case III., and its two remaining angles and third side found, the supplements of these parts will be the required sides and third angle of the proposed triangle. * It may be shown that both values of C will be admissible, by a process of reasonmng similar to that employed in the note on page 197, applied to the equations of Art 89. SOLUTION OF SPHE IICAL OBLIQUE TRI NGLES. 203 95. CASE V. Given thie three sides, or a, b Fig. 9. and c. (Fig. 9.) We have three methods / for computing the half angles: ist. By the sines, from (31), remembering B that A 8= 2 (a + b + e) sin A - sin (s - b) sin (s - c) -2 (8 sin 6 sin si _ 2 (sin (s -?) sin (s -a)) 2d. By the cosines, from (33), ssin sinl (s - a) \ cos 2 A 2 ( sin b sin c wa^A=^ ~^b~m- - ) cost 1 f (sin. s sin (s - c) cos I = ( -. N \ sin a sin b 3d. By the tangents, from (34), tan - A j (sin (s - ) sin (s -) ) 2 sin s sin (s - a) tank C= / (sin (s - c) sin (s - ) tan. ^ B = ( — ^- -) s (166 2 ^ ^ sin s sin (s - 6) s/ v sin s sin (S - C) When only one of the angles is required, the simplest method will be by (165), but if the required angle is less than 90~, it will be found more accurately by (164), for then - A < 45~, and the sine varies more rapidly than the cosine. And, for a similar reason, if the angle is greater than 90~, we should prefer (165). By (166) we always have an accurate result, although the formula is not quite so simple. When the three angles are required, (166) will require the least labor, since sin a, sin b, and sin c, are not then required. 204 SPHERICAL TRIGONOMETRY. No ailDiguity can arise in these solutions, since the half angles must be less than 90~; they require therefore no attention to the algebraic signs. EXAMPLES. 1. Givena = 100~, b = 50, = 60; find A. a =1000 b = 500 log cosec 0.1157460 c = 60 log cosec 0.0624694 2 s =2100 =105~ log sin 9.9849438 Q —a= 50 log sin 8.9402960 2)9.1034552 LA= 690 7'52".7 logcos 9.5517276 A = 138~ 15'45"4 2. With the same data, find all the angles. By (166). s=1050 1. cosec 0.0150562 1. cosec 0.0150562 1. cosec 0.0150562 s-a= 50 1. cosec 1.0597040 1. sin 8.9402960 1. sin 8.9402960 s-b= 550 1. sin 9.9133645 1. cosec 0.0866355 1. sin 9.9133645 -c — 450 1. sin 9.8494850 1. sin 9.8494850 1. cosec 0.1505150 2)0.8376097 2)8.8914727 2)9.0192317 1. tan 0.4188049 1. tan 9.4457364 1. tan 9.5096159 A -= 69~ 7'52".7 ~IB=150 35'37".0 -1C= 17054'59".1 Ans. A = 1380 15'45".4 B= 31~ 11'14".0 C= 350 49'58".2 3. Given a = 100, = 7~, c = 4; find the angles. Ans. A 128~ 44' 45""1 B = 330 1112"/0 C = 18 15' 31"'1 96. The method by (166), may be put under the following convenient form. Let p -(sin (s- a) sin ( - b) sin (s - c) sin s then (167) P P C- P tan A= -. tan' B tan _ - Asin (s - a)' sin (s - b)' sin (s - c) which are similar to the formulae of P1. Trig. Art. 146, and are computed in the same manner. SOLUTION OF SPHERICAL OBLIQUE rRIANGLES. 205 97. CASE V. Given a, b and c. Second Solution. If the whole angle is required directly,* we have cos a - cos b cos c cos A sin a sin c which may be adapted for logarithms by an auxiliary thus: cos -- Cos b cos c cosA = 2 sin ( + a) sin - ~) (168) sin b sin J Or thus, cos b cos c cot 6 -. sin a (169) sin (i - a) cos A sin ( -- (a) sin b sin c sin I 98. CASE VI. Given the three angles, or Fig9. a A, B and (. (Fig. 9). We have three methods of finding the half sids: 1st. By the sines, [36). 2d. By the cosines, (38). A 3d. By the tangents, (39). The computations are conducted precisely in the same form as those of the preceding case. EXAMPLE. Given A = 120~, B = 130~, C = 80~; find c. Ans. c - 41~ 44' 14".6 99. The formulae (39) may be arranged for convenient use in the same manner as the corresponding formulae of the preceding case, Art. 96. 100. CASE VI. Given A, 3 and C. Second Solution. We have, by (5), cos A + cos B cos C,os a -- sin B sin C which may be adapted for logarithms by an auxiliary, thus: cos 0- =cos B cos C 2 cos '- (_4 q- ~) cos ~ (A - ) (170) cos a (0) sin B sin C or. cos B cos C tan = sin A (171) cos (A - (b) cos a = sin B sin C cos sin B sin C cos p * See NOTE at the end of this chapter, p. 211, for the method of computing many of the general formula of spherical trigonometry directly, without the aid of auxiliary angles. S 208 SPHERICAL TRIGONOMETRY. SOLUTION OF OBLIQUE SPHERICAL TRIANGLES BY MEANS OF A PERPENDICULAR. 101. All the cases of oblique spherical triangles may be solved by dividing the triangle into two right triangles by a perpendicular from one of the vertices to the 'pposite side, and solving these partial triangles by the methods of the preceding chapter. Bowditch has given two rules, based upon Napier's Rules, (Art. 46), by which the application of this method is facilitated. 102. Bowditch's Rules for Oblique Triangles. "If in a Fig. 10. C spherical triangle, (Fig. 10), two right triangles are formed by a perpendicular let fall from one of its vertices upon the opposite side; and if, in the two right triangles, the middle parts are so taken that the perpen- \ \-~B dicular is an adjacent part in both of them; then.-~ '. — F/ The sines of the middle parts in the two triangles are proportional to the tangents of the adjacentparts. But if the perpendicular is an opposite part in both the triangles, then The sines of the middle parts are proportional to the cosines of the opposite parts. To prove which rules, let M denote the middle part in one of the right triangles, A an adjacent part, and 0 an opposite part. Also, let m denote the middle part in the other triangle, a an adjacent part, and o an opposite part; and let p denote the perpendicular. First. If the perpendicular is an adjacent part in both triangles, we have, by N:pier's Rules, (Art. 46,) sin AM = tan A tan p sin m = tan a tanp whence sin M tan A tan p tan A sin m tan a tan p tan a or sin M: sin m - tan A: tan a Secondly. If the perpendicular is an opposite part in both triangles, we have6 br Napier's Rules sin AM = cos 0 cos p sin m = cos o cosp whence sin Al cos 0 cos p cos 0 sin m cos o cos p cos o or sin JM: sin m = cos 0: cos o" * We proceed to solve the six cases of spherical triangles with the aid of a perpenrs dicular. It will be seen, however, that Bowditch's Rules are applicable but in the first four cases. * Peirce's Spherical Trigonometry, Art. 44. SOLUTION OF SPHERICAL OBLIQUE TRIANGLES. 103. CASE I. Given b, c and A. Let the perpendicular C P, Fig. 10, be drawn rom C, (that is, in such a manner as to put two given parts in one of the right triangles). Then the right triangle A C P gives, by Napier's Rules, if we put AP= =, tan 0 = tan b cos A (172) then taking co. b and co. a as middle parts in the two triangles, A P = ~ and B P- c - q, * are the opposite parts, whence, by Bowditch's Rules, cos: cos (c -$) = cos b: cos a whence cos (c - -) cos b ( cos a -- (173) COS (b Again, taking A P and 'PB as middle parts, co. A and co. B are adjacent parts, whence, by Bowditch's Rules, sin p: sin (c - ) = cot A: cot B whence sin (c - 0) cot 74) cot B (174) sin ~ and the formulae (172), (173), (174). agree entirely with (122) and (123). The triangle B CP gives as a check tan a cos B = tan (c- ) (175) which agrees with (124). By drawing the perpendicular from B, we may in the same manner obtain the formulae (125). The angle C may be found by the proportion sin a: sin c = sinA: sin C or if C has been found by means of a perpendicular from B, B may be found by a similar proportion, as in Art. 72; and the quadrant in which the angle is to be taken must be determined by the principles of Art. 69. 104. CASE II. Given A, C and b. Let the perpendicular be drawn as before, Fig. 10, and let A CP =, B P =C- -t then, by Napier's Rules, cot 5 = tan A cos b (176) and by Bowditch's Rules, taking co. A and co. B as middle parts, and therefore co. A C P and co. B C P as opposite parts, sin:: sin (C- s) = cos A: cos B whence cos B = sin (C -- ) cos A (177) sin * If A P should exceed A B, (that is, if the perpendicular should fall without the triangle), B P would be equal to A P - A B -= p - c, and the solution could be modified accordingly. But the true results will always be obtained by regarding B P as negative; that is, by still taking B P = c - p and attending to the signs of all the terms as already exemplified, p. 182. f If A C P > A C B, B C P = C - A P will become negative, but the true results are still found by attending to the signs, as already shown, p. 187. 208 SPHERICAL TRIGONOMETRY. Again taking co. A C P and co. B C P as middle parts, and therefore co. b and co. 1 as adjacent parts, Bowditch's Rules give cos: cos (C- ) = cot b: cot a whence t os (C — ) cot (178) cot a == -- - - -(178) cos and (176), (177), (178), agree entirely with (134) and (135). The triangle B C P gives tan B cos a = cot (C- -) (179) which agrees with (136). By drawing the perpendicular from A, we may in the same manner obtain the formulae (137). The side c may be found from the proportion sin A: sin C = sin a: sin c and Art. 69; or c being found by means of a perpendicular from A, we may find a by a similar proportion. 105. CASE III. Given a, b and A. Let the per. >^l pendicular be drawn from C, Fig 10, as in the preceding cases, and let A P = -, B P=-'; then, by Napier's Rules, tan. = tan b cos A (180) 1A- } B and, by Bowditch's Rules, cos b: cos a = cos q0: cos 0' whence cos 0 cos a (181) cos be and then c = + 0 -In Art. 84, we have found, from analytical considerations, that this case admits of two solutions, and that the general expression for c is c = 0 +-t 0' (182) In fact, let us attempt to construct the triangle with the data a, b and A. Having constructed A equal to the given angle, and b equal to the adjacent side, Fig. 11, let Fig. 11. a small circle be described about C as a,/,'. pole, with a (circular) radius = a; this cir// \ a\ cle intersects the great circle AB in two / / \ \ \\ points, B and B', and both triangles, ACB and ACB' contain the same data a, b and A. / ' \ } / '/,-/ IIf the perpendicular CP is drawn, we have X _ -.:: BP - B'P, so that in one of the triangles. B' the side c AB =- AP +- PB = 0 + ',V and in the other, c = AB' = AP- B'P =- ( - '. If both points of intersection, B and B', fall on the same side of A, and within 180~ of A, both solutions will be ndmissible. To find C, let ACP = 5, and BCP -= ', then by Napier's Rules, cot a — = tan A cos b (183) SOLUTION OF SPHERICAL OBLIQUE TRIANGLES. 2G9 and by Bowditch's Rules, cot b: cot a = cos: cos ' whence cos Y' = cos tan b cot a (184) and since in Fig. 11, C - ACB = ACP + BCP = + Y, or (7 = 4 CB'= ACP - B'CP = - ', we have C =a ~ a' (185) and the formulae (180), (181), (182), (183), (184), (185), agree entirely with (146) and (147). After c was found, we might have found C from the proportion sin a: sin c sin A: sin C (186) and B is found from the proportion sin a: sin b = sin A: sin B (187) The two values of B determined by (187), are both admissible when c has two values as above. It is also evident, from Fig. 11, that the two values of B are supplemental. To determine the corresponding values of c and B, we observe that, by Art. 49, the perpendicular CP is in the same quadrant with A and with CBP and CB'P, and therefore CB'A is in a different quadrant from A. Hence, that value of B which is in the same quadrant as A corresponds to the value of c - ( -+ ~ ', and that value of B which is in a different quadrant from A corresponds to the value of c = 0 - 0'; which agrees with what is shown in Art. 84. In computing (186), the two values of c must be employed successively, and the formula computed twice. At each computation we shall have two values of C found from the sine, one of which must be selected by Art. 69. But as the application of the principles of Art. 69 is tedious and embarrassing, it is better to find C by (184) and (185). The formulae (149), (150), (151), (152), for finding B, may easily be delaced by Napier's and Bowditch's Rules. 106. CASE IV. Given A, B and b. Let the perpendicular be drawn as before, Fig. 10, and let AP -=, BP =- ', then as before, tan 0 =tan b cos A (188; and by Bowditch's Rules, cot A: cot B -- sin 1: sin I' whence sin ' - = sin ( tan A cot B c 0 + of 3 (189) which agree with (156). But 9' having two supplemental values determined by the sine, c has two values, as already explained in Art. 89. To show the same geometrically, let B', Fig. 12. Fig. 12, be the acute value of (b', and about C as a pole, let a small circle be described passing through B, and intersecting the B" / great circle AB again in B". Let B"C be drawn, and produced to meet AB again in B', forming the lune B"B'. Then we have B' = B" = CBA 27 s 2 21.0 SPHERICAL TRIGONOMETRY. FiG. 12. so that in both triangles, ACB and ACB, _c _ ---— the value of the angle opposite the side b - 'J / B,^\ - IB' is the same, that is, both triangles contain the same data, A, B and b. Now \ P, 1800 = B"B' = B"P + B'P = BP+- B'P, "x~^~ ^ / ~ so that BP and B'P are supplements of each other. In the triangle A CB we have c = 0 + 0' = AP + BP and in the triangle A CB' we have c - 0 + '/ = AP + B'P and hence the two values of c are found by giving 0' its acute and obtuse values successively, as already shown analytically. By Art. 49, UP must be in the same quadrant with A; hence, if B is in the same quadrant with A, P falls between A and B, as in the figure, and for the same reason, between A and "B. But if A and B were in different quadrants, both points, B and B, might fall between A and P. The two values of c would then be found by the formula c = 4 — ' t' taking, successively, its acute and obtuse values. In that case, tan A and cot B would have opposite signs in (189), sin (' would be negative, which would make p' negative, so that the true results will be obtained, without reference to a diagram, by attending to the signs of the several terms, as already fully exemplified, p. 201. To find C, let ACP -=, BOP = 2', then we have, as before, cot, = tan A cos b (190) and by Bowditch's Rules cos A: cos B -- sin: sin Y' whence sin' -- sin a cos B sin scos A (191) C - 2 -~- ' J which agree with (157). It is evident from Fig. 12, that BCP and B'CP, are supplemental, and that the remarks above made with reference to 4' apply also to 3'. After c was found, we might have found C by the proportion sin b: sin c = sin B: sin C (192) and a is found by the proportion sin B: sin A - sin b: sin a (193j The tw) values of a found by (193) are both admissible when c has two values. From Art. 50, it follows that when BP is acute, a must be in the same quadrant with CP, that is, (Art. 49), in the same quadrant with A; and when BP is obtuse, a must be in a different quadrant from A. That is, that value of a which is in the same quadrant wzith A, belongs to the triangle in zwhich 4' < 90~, and that value of a which is in a different quadrant from A, belongs to the triangle in which p' > 90~; which agrees with Art. 89. The formulas (159), (160), (161), and (162), for finding a may easily be deduced by Napier's and Bowditch's Rules. SOLUTION OF SPHERICAL OBLIQUE TRIANGLES. 211 107. CASE V. Given a, band c. The perpendicular Fig. 13. cannot be drawn, in this case, so that two of the given parts siall be in one triangle; nevertheless the case can be solved by means of a perpendicular. Let the perp. be drawn from any angle, as C, Fig. 13, and as before, put AP = 0, BP = 0'; then by Bowditch's Rules, cos: cos ' cos b: cos a cos <' - cos (p cos a - cos b whence cos +' + cos s cos a + cos b or, by P1. Trig. (110), tan 1 (0 + 0') tan (- 0') =tan (b + a) tan 1 (- a) whence, since - + {-' = c, tan 2 ( - ') = tan (b + a) tan (b - a) cot c(194) (P + 0') = c which determine - (0 - ') and ~ ( -+- p') whence 9 and ~'. The angles A and B are then determined by Napier's Rules. 108. CASE VI. Given A, B and C. In Fig. 13, let ACP -=, BCP = a'; then, by Bowditch's Rules, sin: sin Y' cos A: cos B whence sin- sin ' cos A -cos B sill + sin ' cos A +- cos B or, by P1. Trig. (109) and (110), tan (s ) = tan + (B + A) tan I (B-A) tan ~ (a - a') nhence, since a - + ' = C, tan ( - ) tan - (B + A) tan (B A) tan C r ( - ~ ') = B C which determine n (a - a') and (a + a') and therefore a and '. The sides a and b tre then found by Napier's Rules. NOTE REFERRED TO ON PAGE 205. Computation of Spherical Formulx by the Gaussian Table. The Gaussian Table is a table, first suggested by Gauss, for readily computing the logarithm of the sum or difference of two quantities, when the logarithms of these quantities are given. If p and q are the two numbers whose logarithms are given, p being the greater number, (or logp the greater logarithm), we have, in the first place p + q q (1+ ) p (1 ) If, then, we put x = -, we have log x - logp - log q log (p + q) = log q + log (1 + x) cr log ( 4- q) =log p +log (1+ 212 SPHERICAL TRIGONOMETRY. Downes's Table XXII., with the argument log x, the difference of thn. given logarithms, gives log (1 + x), which being added to log q, the less logarithm, gives the required log. sum, or log (p -- q). Table XXIII., with the argument log x, gives log 1 + - which, being added to logp, the greater logarithm, gives the required log. sum. Either table may, in general, be employed, but one or the other may be found more convenient in a particular application, and therefore both are given Again, we have -- q =p( -- P so that, putting, as before, x = —, we have log x = logp - log q log (p - q) = logp + log (1 ---) Downes's TableXXIV., with the argument, log x, gives log (1 — ) which, being added to the greater logarithm, gives the required log. difference, or log (p - q). With these tables, then, we may readily compute any of the preceding formulas which contain two terms in the second member, without the aid of auxiliary angles EXAMPLES. 1. Given b = 120~ 30' 30", c = 70~ 20' 20", A = 50~ 10' 10"; find a. (Sam, as Ex. 1. p. 182). The formula is cos a = cos b cos c + sin b sin c cos A which will be thus computed: log cos b - 9-70557 log cos c + 9-52693 log q - 923250 log sin b + 9-93529 log sin c + 9-97391 log cosA + 9-80654 logp + 9-71574 logp - log q - log x - 0-48324 The terms p and q have opposite signs, and although, by the formula, they are to De added (algebraically), an arithmetical difference is required. By marking the signs of all the quantities, as above, we shall always know whether a sum or difference is required by the sign before log x. In this case this sign being negative, we are to find a difference, and therefore, by Table XXIV., we take log (1 - ) 9-82694 log p - 9-71574 log cos a + 9-54268 a - 69~ 34' 52" SOLUTION OF SPHERICAL OBLIQUE TRIANGLES. 2. With the same data, find B. The formula is sin c cot b - cos c cos A cot B =.i sin A which m st here be put under the form sin c cot b cot B = cos c cot A sin A and is thus computed: log sin c + 9-97391 log cot b - 9-77029 ar co log sinA -+ 0-11467 log p - 9-85887 log (- cos c) - 9-52693 log cot A + 9-92121 log q - 9-44814 logp - log q - log x + 0.41073 where the sign before log x being positive, the tables for log. sum must be used. By Table XXII., we have log (1 + x) 0-55325 (which is to be added to the less log.) log q - 9-44814 log cot B - 000139 or, by Table XXIII., we have log (1 + 1-) 0-14252 (which is to be added to the greater log.) log p - 985887 log cot B - 000139 B = 135~ 5' 31" In these isolated examples, the labor of computation is very little less than with the use of an auxiliary angle, as on p. 182; but the Gaussian Table has greatly the advantage when the same formula is to be repeatedly computed with successive values of one of the data while the others remain constant. Thus, in the first of the preceding examples, if successive values of a are to be found corresponding to successive values of A, while b and c are constant, log q will be constant, and log x will take successive values, corresponding to those of log cos A, so that after the first value of a is found the succeeding ones are rapidly obtained. On the other hand, as the auxiliary p in the formula (122), depends upon A, the whole process would have to be repeated in finding each value of a. For other forms of the Gaussian Table, see the original table, (to five places of decimals), by Gauss, published in Zach's fl~onatliche Correspondenz, Nov. 1812; Matthiessen's, (to seven places), Altona, 1817; in Vega's Sammlung mathematischer Taeln, (five places), Leipzig, 1840; Zech, (seven places), Leipzig, 1849; Shortrede's C:llection of Tables, (seven places), Edinburgh, 1849; Gray's Tablesfor the Computaton of Life Contingencies, (six places), London, 1849; Schumacher's Hdlfstafeln, new ed. (four places). 214 SPHERICAL TRIGONOMETRY. CHAPTER IV. SOLUTION OF THE GENERAL SPHERICAL TRIANGLE. 109. WE have thus far, following the usual course, considered those spherical triangles only whose sides and angles are less than 180~. In the applications of this subject in astronomy, however, it is often necessary to consider triangles whose sides or angles exceed 180~. (For example, the right ascension of a heavenly body, admitting of all values from 0~ to 360~, may be one part of such a triangle). We may, it is true, in such cases, always substitute another triangle whose parts are the supplements to 180~ or 360~ of those of the proposed triangle; but this mode, although very generally regarded as the simplest, is not really so in the cases alluded to. The construction of figures for discovering the supplemental triangles is often embarrassing and liable to mistake, while the solutions, when obtained, are mostly deficient in generality, and can only be regarded as solutions of the particular cases of a general problem. But if we proceed by a method that is as applicable when the parts of the triangle exceed as when they are less than 1800, we may investigate a problem under the simplest supposition of the values of these parts, and rely upon the generality of the method to cover all the particular cases. 110. We shall first endeavor, in an elementary manner, to give the student a conception of the nature of the general spherical triangle. Fig. 14. Let AB/C, Fig. 14, be any spherical triangle whose parts C/ are all less than 180~; then the remainder or complement 7 / / \a \ of the sphere is also a spherical triangle whose sides are b/ \ \ and c, and whose angles are 360~ - A, 3600~- B I 6b \ } and 60~ -C. We shall distinguish these triangles from each other by means of accents, writing the letters wvithin \ A / the triangle to which they respectively belong, as ir Fig. 14. The sides are common, but when referred to ae sides of A'B'C', they will be denoted by a', b' and c'. Again, one of the sides may exceed 180~, as the side a of the triangle ABC, Fig. 15. In this triangle, it is evident that we must have A > 180~, so long as B, C, b and c are each < 10~. In the triangle A'B'C' we have A' < 180~, while B'> 1800, ' > 180~. Fig. 15. Fig. 16 B' CB' S CS c _ b R 4'A If we next suppose two of the sides to exceed 180~, as a and b, Fig 16, these sides intersecting in two points whose distance is 180~, the figure ceases to present the SOLUTION OF THE GENERAL SPHERICAL TRIPkNLGLE. triangle as an enclosed surface, but it will presently appear that such triangles are solved by the same general methods that apply in other cases. To form a just conception of the triangle in this case, we may conceive Fig. 16 to be obtained frioni Fig. 15 by carrying the point A along the arc CA produced until it crosses the side a the points A and B may then be joined either by an arc less than 180~, as in Fig. 16. or by its supplement to 860~, as in Fig. 17, in Fig. 17 which last case every side exceeds 180~. In B'. —,. these figures, to avoid confusion, the point A, /B, is not placed in its true position according to perspective. In each figure we have two triangles, whose sides are common, and whose angles are sup- \ plements to 360~. It will be easy to trace the two triangles signified by ABC and A'B'C', by. remarking that the letters in each case are all --- on the same side of the perimeter of the triangle. We may go farther, ana suppose the arc joining A and B to be a circumference - the arc AB, or any number of circumferences +- AB; and similarly the angles may be supposed to be altogether unlimited; but since the relative positions of any three points of the sphere must be fully determined by arcs and angles less than 360~, nothing is gained by passing beyond this limit. 111. All the formelce of Chactier I. are aipplicable to the yeneral spherical triangle. This proposition might be considered as established by the principle of P1. Trig. Art. 49, but it is also very easily established by a continuation of the process of Spher. Trig. Art. 6, where the fundamental equation was shown to apply to all triangles whose parts are less than 180~. It was proved inArt. 29, that all the equations of Chap. I. may be deduced from the fundamental one, cos a = cos b cos c - sin b sin c eos A (I) We have then only to prove the generality of this single equation. 1st. Let all the sides be < 180, but A' >180~, Fig. 14. The formula being true for the triangle ABC, we have cos a = cos b cos c - sin b sin c cos (360~ - A') or in the triangle A'B'C', by Pl. Trig. (76), cos a' - os b'o s s c' - sin b' sin c' cos A' 2d. Let a>180~, Fig. 15, and produce a to complete the great circle. The triangles ABC and A'B'C' are respectively the difference and sum of a hemisphere and the triangle A'ik, all of whose parts are < 180~. In the triangle A'i7c we have, in terms of the parts of ABC, cos (360~ - a) = cos b cos c + sin b sin c cos (360~ - A) and in terms of the parts of A'B'C', cos (360~ - a') = cos b' cos c' 4- sin b' sin c' cos A' both of which reduce to the form (ai). But it is here necessary to show that the formula may also be applied to each of the other angles: thus the triangle A'ik gives cos b = cos (360~ - a) cos c + sin (360" - a) sin c cos (180~ - B) cos b' = cos (3600 - a') cos c'+ sin (360~ - a') sin c'cos (B' -180~) both of which reduce to the form (nI). 216 SPHERICAL TRIGCONOMETRY. 3d Let a > 180~, b >180~, Fig. 18; these arcs intersect at i. and the triangle A'B'2 g ives Fig. 18. c,1 \\\ / cos (a - 180~) = cos (b - 180~) cos c - sin (b - 1800) sin c cos (3600 - I) cos (a'- 1800) = cos (b'- 180) cos c' sill (b' - 180~) sin c' cos A' which reduce to the form (i); and in the same way the formula applies to the angle B. We have also cos c = cos (a - 180~) cos (b - 180~) + sin (a - 1800) sin (b - 1800) cos i and since cos i = cos C = cos (3600 - C') - cos C', this also reduces to the form (M) for both A B C and A' B' C'. 4th. Let a > 1800, b > 1800, c > 1800, Fig. 19; the side c being produced to complete the circle, the triangle i k I gives Fig. 19..B A C( cos (a -1800) = cos (b- 1800 cos (360~-c) + sin (b- 180~) sin (3600~-c) cos, and since cos I = cos (180~ - A) - cos A = cos (A' - 180~) - - cos A', this reduces to the form (n) for both A B C and A' B' C'; and in the same way the formula applies to the angle B. We have also cos (360 - c) = cos (a - 1800) cos (b - 1800) + sin (a - 1800) sin (b - 180) cos i, and since cos i = cos C = cos C', this reduces to the form (N) for both A B and A' B' C'. The cases in which the angles or sides exceed 360~ are included in the preceding, in consequence of PI. Trig. Art. 45. 112. The preceding demonstration, though tedious, has the advantage of giving a definite conception of the figures which our formula represent. But perhaps the 'most satisfactory (as it is the most elegant) method, is to rest the dernonstration of our fundamental equations themselves upon the principles of analytical geometry, and, for the sake of those who are acquainted with that subject, we add the following investigation: Any point of the sphere may be referred by rectangular co-ordinates to three planes passing through the centre of the sphere at right angles to each other. Let O be the centre of the sphere, Fig. 20, and A B C a spherical triangle upon its surface. Let one of the co-ordinate planes, as X Y. coincide with the great cir~le A B, and let the axis of Xpass through B. If C.P be drawn perpendicular SOLUTION OF THE GENERAL SPHERICAL TRIANGLE. 21.7 tt the plane XY, and CP' and PP' to the axis OX, the co-ordinates of the pent C are x = OP', y PP', z CP Fig. 20. Fig. 2L z z 0S 0 P Y AY the values of which (0 C being taken - 1) are X -- cos a y = sin a cos B z - in a sin B If now the axis of X be made to pass through A, Fig. 21, without changing the position of the plane X Y we shall have for x', y', z', the co-ordinates of Creferred to the new axes, x' - cos b y' -= - sin b cos A z' = sin b sin A The axis of z being unchanged, the relations between x', y', and x, y, are expressed simply by the formulre for the transformation of co-ordinates in a plane; the inclination of the new axes to the first is here expressed by c, and the formulae of transformation are therefore x = x' cos C - y' sin c y = x' sin c + y' cos c z = z' substituting the values of the co-ordinates, we have at once the three following indamental equations: cos a = cos c cos b - sin c sin b cos A sin a cos B sin c cos b - cos c sin b cos A (N) sin sinin B = sin b sin A ihlch are identical with (4), (6), and (3). 113. Having established the complete generality of our fundamental equations, we may now employ for the solution of the general triangle any of those deduced from them in Chap. I. As a single trigonometric function is not sufficient to determine an unlimited tngle or arc, (P1. Trig. Art. 53), it becomes necessary in most cases to deduce expressions for both the sine and cosine of the required part. It will be found that all the six cases of the general triangle admit of two solutions, but that they all become determinate, when, in addition to the other data, the sign of the sine cr cosine of one of the required parts is given. In the practical applications in astronomy, 't mostly hasppens t:hat the conditions of the problem supply this sign. 28 T 216 SPHERICAL TRIGONOMETRY. 114. CASE I. Given b, c and A. Firsl Solution; when one of the remaining un. gles, as B, and the third side a are required. The relations between the given and required parts are cos a -- cos c cos b + sin c sin b cos A sin a cos B = sin c cos b -cos c sin b cos A ((19t) sin a sin B -= sin b sin A The signs of the second members will be known from their computed numerical values; the sign of cos a is therefore known. If the sign of sin a is also given, the quadrant in which a must be taken will be known; the second and third equations will determine the sign of the sine and cosine of B, and therefore the quadrant in which B is to be taken. In like manner, if the sign of either cos B or sin B is given, that of sin a becomes known, and the problem is determinate. If no conditions are atttached to the required parts, there must be two solutions. The numerical solution will be conducted as follows: The values of the second members (or simply their logarithms) are to be separately computed, and their signs carefully noted; then the quotient of the 3d by the 2d (or the difference of their logs.) will give tan B, and hence B, which will be taken in the quadrant indicated by the signs of the sine and cosine. Then the Od divided by sin B, or the 2d by cos B, will give sin a, which, agreeing with the value from the 1st equation, will serve to verify the correctness of the whole process. This solution may be adapted for logarithms by the methods employed in the preceding chapter. 1st. Let k and (, be determined by the equations k sin Q = sin b cos A k cos - cos b k being a positive number (P1. Trig. Art. 174); then (7 (197) cos a = k cos (c - p) sin a cos B = - sin (c -) sin a sin B = sin b sin A 2d. Eliminating k, and taking 4 < 180~, (P1. Trig. Art. 174), tan -= tan b cos A ( < 180~) cos b cos a= - cos (c - 4) oC~~os4? -~ (198) cos b sin a cosB = cos sin (c- ) cos 0 sin a sin B -sin b sin A 3d If it e quadrant in which a is to be taken is given, we may give the preceding equations tae following form: tan -= tan b cos A (< < 180~) tan a cos B = tan (c - ) sin (P tan A l tan a sin B = o- cos (c -- ) J SOLUTION OF THE GENERAL SPHERICAL TRIANGLE. 219 4th. If both a and b are less than 180~, as not unfrequentlj happens in the applications of this problem, let Ic~k ~ sin a sin b k theli n a nd n are both positive numbers (k being positive) and (197) gives m sin - cos A mr cos - cot b n sin B =sin in tan A (2001 n cos B = sin (c - ) cot a = cot (c- ~) cosB J Check. We find sin (c- ) sin a cos B tan A sin i sin b cos A tan B L (2X5 cos (c - () cos a cos) cos b besides which we may employ, in connection with (200), the equation sin a sin B sin b sin A; or in connection with (197) or (198) the equation tan a cos B tan (c- (). Or when (]97) and (198) are employed, we may find a both by its sine and its cosine. 115. The angle C may be found in the same manner as B, interchanging B and C, b and c, in the preceding formulae. But when B and C7are both required, the Second Solution to be given presently is preferable. EXAMPLE. Given A = 261~ 16' b = 45~ 54' c - 138~ 32', and a < 180~; to find a and B. We shall first employ (197). The first column of the following computation, con taining the symbols expressing the operations to be performed, should be prepared before opening the tables: A 2610 16' b 45~ 54' c 138~ 32' log sin A 9-9949352 log cos A - 9-1813744 log sin b + 9-8562008 log cos b = logk cos 0 + 9-8425548 log sin b cos A = logk sin - 9-0375752 log tan - 9-1950204 log cos 0 + 9-9947336 logk + 9-8478212 p 351~ 5'42"-6 *c -- 147~ 26' 17"-4 a As 0 > c, we take c = 138~ 32' + 360~, so that c - p may be a positive angle; but it would be equally convenient to take c -0 - 212~ 33' 42"fi 220 SPHERICAL TRIGONOMETRY. log sin (c - 0) + 9-7309514 log cos (c - 0) - 9-9257303 logk cos (c- ) = log cos a - 9.7735515 a 126~ 25' 6"6 (1) log sin b sin A = log sin a sin B - 9-8511360 logk sin (c - 0) = log sin a cos B - 9'5787726 log tan B - 0-2723634 B 298~ 6' 26"'8 log sin a + 9-9056351 log sn B - 9-9455009 (1) Check. log sin asin B -9-8511360 If a were not limited, we should have two solutions, the second being a = 2330 34' 53"'4, B - 118~ 6' 26"'8. We shall next give the computation by (200), which is applicable to this example, since botl a and b are less than 180~. A 261~ 16' b 45~ 54' c 138~ 32' log cos A = log m sin 0 - 9-1813744 log cot b = log m cos 0 + 9-9863540 log tan p - 9-1950204 8 351~ 5'42"-6 c - 147~ 26' 17"'4 log tan A log sin 0 log tan A sin 0 = log n sin B log sin (c - 0) = log n cos B log tan B + 0-8135608 - 9-1897534 - 00033142 + 9-7309514 - 02723628 B 298~ 6' 26"-9 log cos B + 9-6731379 log cot (c - 9) - 0-1947789 log cos B cot (c- 0) = log cot a - 9-8679168 a 126~ 25' 6"'7 116. CASE I. Given b, c and A. Second Solution; when the two angles B and U, tr when all the remaining parts are required. We have, by Gauss's Equations (44), cos ~ a sin i (B + C) = cos (b- c) cos A A cos - a cos 2- (B + C) cos - c (b + c) sin ~ A sin ~ a sin1 (B - C) = sin 1 (b - c) cos A (2 ) sin i- a cos i- (B - C) - sin - (6 + c) sin 4 A From the first two we deduce ~ (B + C) and cos J- a, and from the second two (B - C) and sin - a, whence B, C and a. The problem becomes determinate, as before; that is, when a is limited by one of the conditions a < 180~, or a> 180~ for then the signs of both cos ~ a and sin 1 a will be known.* * By Art. 27, Gauss's Equations may also be taken with the negative sign when the triangle is unlimited, as in the group (45), but the same final results are oltained from either (44) or (45). See note at the end of this chapter, p. 227. SOLUTION OF THE GENERAL SPHERICAL TRIANGLE. 22? EXAMPLE. Same as in Art. 115. a < 180~. A 261~ 16' b 45~ 54' c 138~ 32' (b - c) 460 19' (b + c) 920 13' Y A 130~ 38' log d = log cos (b - c) + 9-8392719 log e = log sin (b - ) - 9-8592393 log f = log cos g (b + c) - 8-5874694 log g = log sin A (b + c) + 9-9996749 log cos 1 A - 9-8137250 log sin i A + 9-8801803 log d cos i A = log cos ~ a sin i (B 4- C) - 9-6529969 log f sin i A = log cos a a cos 1(B + C) - 8-4676497 log tan i (B +- C) -+ 1-1853472 i (B + C) 266~ 15' 58".0 log sin ~ (B + C) - 9-9990771 log cos i a + 9-6539198 - a 630 12' 33"3 log e cos A - log sin ~ a sin (B - C) + 9-6729643 log g sin i A = log sin - a cos (B - C) + 9-8798552 log tan (B - C) + 9-7931091 -- (B - C) 310 50' 28".7 log sin i (B - C) + 9-7222788 Verification. log sin - a + 9-9506855 a 630 12' 33"'3 B = 298~ 6' 26"-7 Ans. 7C = 234~ 25' 29"-3 a = 126~ 25' 6"-6 117. If a only is required, we may find it by one of the methods of Arts. 75 and 76; ani if the sign of sin a is given, the solution is determinate. If the sign of sin B or of sin C is given, we find that of sin a by inspecting the equation sin A sin b sin A sin c sin a - -- sin B sin C 118. CASE II. Given A, C and b. First Solution; when the third angle B, and tne of the remaining sides (as a) are required. The general relations between the given and required parts are cos B - cos C cos A + sin C sin A cos b sin B cos a = sin C cos A + cos C sin A cos b (203) sin B sin a = sin A sin b which are solved in the same manner as (196). The problem is determinate when the sign of either sin B, cos a, or sin a is given. T2 222 SPHERICAL TRIGONOMETRY. Adapting (203 for logarithms, we find 1st. *k sin a = cos A (kp k cos 5 sin A cos b cos B = k sin ( — ) sin B cos a = k cos (C — ) sin B sin a= sin A sin b 2d. cot = tan A cos ( cos A. cos s sin (C - ) sin a Sin (C- ) sin B cos a = cos (- ) sin c (C-) sin B sin a = sin A sin b 8d. When th i quadrant in which B is to be taken is given cot 3 = tan A cos b ( tan B cos a - cot (C - 3) tan b cos 3 tan B sin a. —.. sin (C - Z) 4th. When A and B are both less than 180~, let k sin B P = sin A= -A then p and q are positive numbers, and we have from (204), iositive) 1 (204) 3 < 180~) (205) < 180~) - J (206) J p sin = cot A pos a c os b q sin a = tan b cos 3 (207) q cos a = cos (C - a) cot B = tan (C - ) cos a Checks. We have cos (C- ) sin Bosa tan b cos, sin A cos b tan a sin (C- k) cos B sin ' cos A:- The same factor k is used here and in (197), although the auxiliaries f and s are different. To show that k has the same value in (197) and (204), let the squares of the equations k sin =- sin b cos A k cos = cos b be added; we find k (sin' 0 + cos2 ) = k- = cos 6b + sin' b cosA A 1 - sin" b smn A and in the same manner, from the equations k sin = cos A k cos -sin A cos b we find k =- 1 - sin2 b sin2 A and ther fore, in both cases, k _= / (1 - sin2 b sin' A) SOLUTION OF THE GENERAL SPIHERICAL TRIANGLE. 223 besides which we may employ, with (207), the equation sin B sin a = sin A sin b; or with (204) and (205), the equation tan B cos a = cot (C -- ). Also, when (204) or (205) is employed, we may find B both by its sine and its cosine. These formulae are computed in the same manner as those of preceding case. 119. CASE II. Given A, C and b. Second Soletion; when the two sides, a and c, or all the remaining parts, are required. We employ Gauss's Equations in the following form: sin -2 B sin - (a - c) = cos 4 (A - C) sin 4 b sin - B cos I- ( + c) = cos - (A- + C) cos b cos sin (a-) = sin (a-(A C) b cos 1 B cos e (a - c) == sin -4 (A + C) cos 4 b (209) whica are solved in the same manner as (202). EXAMIPLE. (1;a A _ 1210 30(] 0"'8, = 42~ 15' 13"-7, b =- 40~ 0' 10", and B > 180~. By (209). b 40~ 0'10"0 -A 121~ 36' 19"8 C 420 15' 13"7 4 (A - C) 390 40' 33/" - (A + C) 81 55' 46"-7 b 20~ 0' 5".0 log d — log cos (A - C) 4- 9-8863038 log e = log sin - (A - C) - 9-8051224 logf -- log cos (- (A- C) - 9-1473326 logg - log sin 1 (A + C) + 9-9956775 log sin 1 b + 9-5340806 log cos l b + 9-9729820 log d sin b =log sin B? sin I (a + c) + 9-4203844 logf cos - b =- log sin 2 B cos - (a 4- c) + 9-1203146 log tan - (a 4- c) + 0-3000698 4 ( +- c) 630 23' 3".3 log sin -- (a - c) 4- 9-9513526 log sin A- B + 9-4690318 4 B 1620 52'28"'6 log (.- e sin 2 b) = log (- cos 4 B) sin 4 (a - c) - 9-3392030 *log (-g cos - b) - log (- cos - B) cos (a - c) - 99686595 log tan 4 (a - c) + 9-3705435 (a - c) 193012'32"/9 a -=. 256~ 35'36"'2 tAns. c _ 230010'30/'1 l B- 325044'57"'2 f The sign of eaca olf these factors is changed because B > 180~, and cos i B is Segative. tj It was necessary to increase 2- (a 4- c) by 360~, to obtain c. The corresponding value of b would be 616~ 35' 36' -2. See note at the end of this chapter, p. 227. 224 SPHERICAL TRIGONOMETRY. 120. When B only is required, we may employ the methods of Arts. 81 and 82, which are determinate when the sign of sin B is given; or when that of either sin a or sin c is given, since we may then find that of sin B by inspecting the equations sin A sin b sin C sin b sin B = --- = sin a sin c 121. CASE III. Given a, b and A. First Solution; when the three remaining parts B, C, and c are all required. We find B by the equation sin A sin b sin B -sin (210) sin a which is determinate when the sign of cos B is given. Then, to find C, we have - cos C cos A - sin C sinA cos b cos B sin C cos A + cos C sin A cos b = sin B cos a which have already been employed and adapted for logarithms in Art. 118. If we denote the auxiliary by 3, and put C - == ', we find, from (204), k sin - = cos A (k positive) k cos -= sin A cos b k sin ' cosB (211) k cos 5' = sin B cos a C = - +' J To find c, we have cos c cos b - sin c sin b cos A = cos a sin c cos b - cos c sin b cos A = sin a cos B which have already been employed and adapted for logarithms in Art. 113. If we denote the auxiliary by 0, and put c - = 0b', we find, from (197), k sin 0 = sin b cos A (k positive) k cos - cos b k sin 0' = sin a cos B (212) k cos ' = cos a c = 0 + 0' Checks. We have sin 3 cos A cos tan a sin 3' cos B cos 6' tan b (213) sin _ tanB cos _ cos b (21 sin ' tan A cos 0' cos a One of which maybe used as a check when either C or c has been alone computed.M When both C and c have been found, the obvious check is sin C sin A sin c sin a The following relations deserve a passing notice: sin 0 cos 5' sin ' cos 3 - sin b sin B - sin a sin A cos 0' sin 5 cos 0 sin 6' tan v tan o' sin 2 0 sin 2 5' sin2 b sin 2 sin 2 = sin a SOLUTION OF THE GENERAL SPHERICAL TRIANGLE. 225 EXAMPLE. Given a - 126~ 25' 6"-6, b = 188~ 32' 0', A = 261~ 16' 0", and cos B negative a 126~25' 6"-6 b 138~ 32' 0"0 -A 261~ 16' 0"'0 By (210), log sin a + 9-9056351 log sin b +- 98209788 log sinA - 9-9949352 log sinB - 9-9102789 B 2340 25'29".3 By (211), log cos b - 9-8746795 log sin A cos b = log k cos S + 9-8696147 log cos A = log k sin s - 91813744 log tan a - 9-3117597 3480 24' 53"-0 log cos a - 9-7735515 log sin B cos a = log k cos 9' + 9-6838304 log cos B = log k sin a' - 9-7647520 log tan ' - 0-0809216 a' 309 41' 33"-7 &a ' = C 298~ 6'26"-7 By (212), log sin b cos A == log k sin 0 - 9-0023532 log cos b = log k cos 0 - 9 8746795 log tan 0 + 9-1276737 0 1870 38'31"13 log sin a cos B = log k sin 0' - 9-6703871 log cos a = log k cos I' - 9-7735515 log tan 4' + 9-8968356 q0 218~ 15'28"-6 0 + ' = c 450 53' 59".9 log sin C - 9-9455010 log sin c + 9-8562006 (sinG) -/. log (sin C - 00893004 aGheck. log (.sina - 00893001 \sin a / In this example, both s + s' and ( 4- ~' exceed 360~, and consequently we have to deduct 360~ from each of them. We might have avoided this, however, by taking a' = - 50~ 18' 26"-3, ' = - 141~ 44' 31"-4. 122. CASE III. Given a, b and A. Second Solution; when C and c are required without finding B. We have only to eliminate B from the fourth equation of (211) by means of (210), and then (omitting the third equation) determine a' by its cosine, observing, however to take it so that sin a' shall have the sign of cos B, which sign is supposed to be given. The formula for finding C thus become 29 226 SPHERICAL TRIGONOMETRY. k sin = cos A (k positive) k cos -- sin A cos b cos '-= cos ~ cot a tan b > (216) (V' < 180~ with the sign of cos B) C = a + 3' To find c, we observe that sin O' has the sign of sin a cos B, so that we have the following formulae: k sin 0 = sin b cos A (k positive) k cos 0 = cos 6 cos 0 cos a cos f co s a (216) (I' < 180~ with the sign of sin a cos B) C = -+ - Check. The equation (214). 123. CASE IV. Given A, B and 6. First Solution; when the three remaining parts a, c and C are all required. We find a by the equation sin a= sinAsinb (217) sin 8 which is determinate when the sign of cos a is given. The remainder of the solution is by (211) and (212). 124. CASE IV. Given A, B and b. Second Solution; when c and C are required, without finding a. We easily find, from (211), k sin a = cos A (k positive) k cos -= sin A cos b sin <, sin s cos B cos A (218) (cos S' and sin B cos a to have the same sign) And from (212), k sin 0 = sin b cos A (k positive) ) k cos 0 = cos b sin O' = sin 0 tan A cot B 2 (219) (cos I' and cos a to have the same sign) c 0+ 01 J Check. The equation (214) 125. CASE V. Given a, b and c. The formula cos a-cos b cos c(2 cos A ---- (220) sin b sin c determines A when the sign of sin A is known. If the sign of sin B or of sin 0 if gi ten, that of sin A becomes known by the equation sin A sin B sin C sin a sin b sin c SOLUTION OF THE GENERAL SPHERICAL TRIANIGLE. 227 The formulas (31), (33), (34), may be used, each of which will become determinate when the sign of either sin A, sin B, or sin C is known. 126. CASE VI. Given A, B and C. The formula cos A + cos B cos (221) cos a --- (221) sin B sin C determines a when the sign of sin a is given. If the sign of sin b or of sin c is given, that of sin a becomes known by the equation sin a sin b sin c sin A sin B sin C The formulas (36), (38), (39), may be used, each of which will be determinatp when the sign of either sin a, sin b, or sin c is known. NOTE UPON GAUSS'S EQUATIONS. In the unlimited spherical triangle, we may consider any part, as a, to have an infinite number of values, viz. a, a - 360~, a - 720~, &c., expressed generally by the formula a + 2 n vr, n being any whole number or zero; and since sin a = sin (a + 2 n,r) cos a = cos (a +- 2 n r) all those equations of Chap. I. that involve only sin a and cos a will not be changed by the substitution of a - 2 n Ir for a. A similar substitution may be made for each of the parts, or for all of them, at the same time, so that there is an infinite series of triangles to which these equations are applicable. But the substitution of a - 360~ for a, in Gauss's Equations, (202), will change the sign of all of them, since sin i (a - 360~) =- sin ~ a cos ~ (a + 360~) - -cos a a while the substitution of a - 720~ for a will not change their sign, since sin ~ (a + 720~) = sin I a cos i (a - 720~) = cos a a In general, their sign is changed by the substitution of a + (4 n + 2) v for a, and it is not changed by the substitution of a - 4 n nr. The same results follow like substitutions for each of the parts. It follows that these equations taken only with the positive sign, do not include all the triangles of the infinite series above spoken of, and that they are complete only when taken with the double sign, and expressed in two distinct groups, as (44) and (45) of Art. 27. In practice, however, we may take them with the positive sign only; for they will then give at least one of the triangles of the series, from which all the others, (and particularly that whose parts are less than 360~), may be directly deduced by the application of 360~.* This will be illustrated by the example of Art. 119, p. 223; we there find i (a + c) = 63~ 23' 3".3 (a - c) = 193~ 12' 32"-9 or rather, since i (a + c) should be greater than - (a - c), (a + c) = 4230 23' 3"-3 (a - c) = 1930 12' 32".9 * Gauss (Theoria Motus Corp. Cce. Art. 54) recommends the use of the positive sign only, observing that any side or angle may be diminished or increased by 360~, as the case may require, but confines himself to the statement of this practical precept, without explaining the grounds upon which it rests. 228 SPHERICAL TRIGONOMETRY. whence a - 616~ 35' 36"-2 c - 230~ 10' 30"-4 which is the proper solution of the equations taken with the positive sign. If now we deduct 360~ from a, and take, as on p. 223, a =- 256~ 35' 36".6 c = 230~ 10' 30"-4 we have the solution that would have been obtained by taking the negative sign in all the equations; for we now have (a + c) = 2430 23' 3"-3 i (a - c) = 13~ 12' 32"-9 which, differing from the former values by 180~, must change the sign of all the equations. I have given some further particulars respecting unlimited spherical triangles, and a fuller discussion of Gauss's Equations, in an essay which the reader will find in the Astronomical Journal, Vol. I., published at Cambridge, Mass. AREA OF A SPHERICAL TRIANGLE. 229 CHAPTER V. AREA OF A SPHERICAL TRIANGLE. 127. Given the three angles of a spherical triangle, to compute the area. This problem is solved in geometry, where it is proved that the surface of a spherical triangle is measured by the excess of the sum of its three angles over two right angles, by which is meant, that the area is as many times the area of the tri-rectangular triangle as there are right angles in the excess of the sum of the angles over two rqiht angles, To express this analytically, let r = radius of the sphere T — =surface of the tri-rectangular triangle = ~ surface of a sphere = 1 7r r2 2S= A+B+ C K = area of the triangle ABC. Also, let the angles A, B and ( be expressed in the unit of Art. 11, that is, let A, B, C denote the arcs which measure the angles in a circle whose radius is unity. The right angle expressed in the same unit is -, therefore the number of right angles in 2 S is 7r 4S 22~ 2 7r and we have, according to the above theorem of geometry, 45S 2 T K=TX x( — 2) =- (2 —.r) or K= r2(2S- r) (222) and if the radius of the sphere is taken = 1 K= =2S —r 223) 128. In a plane triangle the sum of the angles is equal to 7r, and in a spherical triangle the sum exceeds 7r by Kr; hence this quantity, K, is commonly called the spherical excess. u SPHERICAL TRIGONOMETRY 129 Given the three sides, to find the area. By (223), we have sin K = sin (S — ) - -cos S V/ I h (224) cos jK= cos (S —) = sin S tan K K = - cot S in which we have only to substitute the values of cos S, sin S, and cot S, given in Art. 34, to obtain the required solution. We find, [s.= (a +- b +4 c)], sin- K-= V [sin s sin (s - a) sin (s - b) sin (s - c)] 25) 2 cos ~ a cos ~ b cos ~ c cos a ~- cos b ~- cos c 4- 1 cos j K= - — ______ 4 cos 4 a cos 6b cos 4 c cos' 4 a+ cos' b - cos' C - I 6) 2 cos 4 a cos b cos 4 c The numerator of (225) being denoted by n, we find, cot -K- 1 + cos a + cos b6 cos c (227) 2n which is known as De Gua's formula. Again, from the formula of Art. 35, since 1 - sin S = 2 sin 2~K, 1 + sin S 2 cos 2K, we find [ sin s sin (s - a) sin } (s - b) sin j (s - c)] cos K ~= [cos s cos 4 s - a) cos (s - b) cos j (s - c)1 (228) Lo4T=v [_cos 4 a cos b cos I c tan — /[tan stan (s - a) tan (s —b) tan 4 (s-c)] JI the last of which is known as Lhuillier's formula. 130. Git en two sides and the included angle, (or a, b and C) tofind the area. We have, from (224), by (71), cot 4 a cot ~ b - cos C sin C tan 4 a tan 4 b sin C2 t 1+tan 4 a tan ~ b cos (29) AREA OF A SPHERICAL TRIANGLE. 231 131. If we admit more than three parts of the triangle into the expression of A, we have by (56) and (67), sin i a sin i b sin K C - - sin C cos j c j (230) cos j a cos b+sina sin i b cos C coscoa c J the quotient of which gives (229). 132. Since there are always two triangles upon the surface of the sphere which have the same three sides, (Art. 110), the angles not being limited to values less than 180~, the formulae (225), (226), (227) should give the areas of both of them, and their sum should be equal to the surface of the sphere = 4 9r. In fact, by (225), sin J- K may be either positive or negative, while by (226) the cosine is fully determined, so that these formula give two values of i K whose sum is 2 ar, and therefore two values of K, whose sum is 4 v. It lollows that (225) alone is not sufficiently determinate when the triangle is unlimited, since it gives four solutions. The most convenient formula is therefore (228), for we must always have j K < ar, and the double sign of the radical gives the two values of j K, one less and the other greater than j. ''32 SPHERICAL TRIGONOMETRY. CHAPTER VI. DIFFERENCES AND DIFFERENTIALS OF SPHERICAL TRIANGLES. 133. Two parts of a spherical triangle being constant, and a third receiving an increment, it is required to deduce the corresponding increments of the remaining three parts. As in plane triangles, (P1. Trig. Chap. XII.), this will be effected by a comparison of two triangles having two parts in common. The triangle formed from the given one by applying the increments to the variable parts will be distinguished as the derived triangle. We shall first consider the increments as finite differences, an give them the positive sign, (P1. Trig. Art. 187). 134. CASE I. A and c constant. The parts of Fig.22 ABf, Fig. 22, being A, c, B, C, a, b, those of the derived triangle ABC' are A, B, B + Aa, C+ AC, a + Aa, b + Ab; and the parts of the differential A B triangle BOO' are a, a + Aa, Ab, 180 ~- C, C + AC and AB. We have, then, in BCC', by (3), sin Ab sin (a + Aa) sin a sin aB - sin sin (C+ AC) (23 Also, in BCC', by (40), we have sin1 (180~- C+ C + ) tan -- ab sin j (180~ - C- a- aCT) tan (a + Aa- a) whence tan I- Aa cos (C + AC) 232 tan - ALb cos I AC By (41) we fnd in a similar manner, tan 2 Ab tan (a + 2 Aa) 23 sin G, C i (C + 2AC) By `42), sin ~ Aa sin (a + a)234 tan -- -AB tan ( C + ~A ( /) DIFFERENCES OF SPHERICAL TRTIANLES 233 By (43), tnan _ cos (a + ) (235 2 2 Y/(285 tanAB C cos A,a By combining (232) and (233), tan - A _ tan (a + l Aa)(236 tanA tan( + = C) (236) As these formulae involve the increments in the second members, they are to be computed by successive approximations. (See P1. Trig. Art. 201). 135. CASE II. A and a constant. The given Fig.23. triangle being A B C, Fig. 23, the parts of the derived triangle A' B C are A, a, B + A B, b -+ Ab, C + AC, c + Ac. Although the figure appears tow show that the angle B is diminished, it is still proper A to represent the angle A'B C by B + AB, to preserve uniformity in the algebraic signs of the increments; the essential signs being given by the equations of differences themselves. Hence we put the angle A B A'=A B - AB C - B - (B + AB) = - ABJoining A A' we have in B A A' and CA A', by (43), cos (c + I AC): Cos 1 A = - cot i aB: tan (A'AB + AA'B) cos (b + 1 Ab): cos ~ Ab - cot AC tan 2 (A'A 0 + A A'C) but since A is constant, or B A C = B A' C we find that the fourth terms of these proportions are equal; whence tan AB _ cos (b + - Ab) cos I Ac 2an 2 2U (237) tan I AdC cos (c + 1 Ac) cos I Ab In the polar triangle of A B C, the constants are still an angle andl its opposite side, and the preceding equation applied to this polar triangle (by Art. 8) gives tan I Ab cos (B + ~ AB) cos } AC tan AC Ac cos (C + aC) cos A AB In AB C and A B O we have sin i sin B = sin A sin b sin a sin (B - AB) = sin A sin (b -t- Ala 30 u2 234 SPHERICAL TRIGONOMETRY. the difference and sum of which give sin a cos (B + 2 AB) sin 1 AB sin A cos (b + i Ab) sin 1 Ab sin a sin (B + i AB) cos 1 AB = sin A sin (b + } A6) cos ~ Ab from which, by division, we find tan 1 Ab tan (b+ i Ab) (2~ tan j AB tan (B + ~ AB) and in the same manner tan - Ac tan (c + Ac) (240) tan AC tan (C+ j AC) The product of (237) and (239) gives sin Ab _ sin (b + I Ab) cos 1 Ac tan AC - cos (c + ~ Ac) tan (B + A B) ) whence also* sin 4 Ac sin (c + - Ac) cos A2b 2 2 (242) tan AB cos (b + I Ab) tan (C + AC) ( ) Fig. 24. Fig.24. 136. CASE III. b and c constant. The given / triangle being ABC, Fig. 24, the parts of the derived triangle A B C' are b, c, a + Aa, B + AB, / + AC, A + AA. Joining C C' we have in B C C', '^ -^J by (42), B sin (a + Aa): sin I Aa = cot AB: tan 1 (B C '- B C'C) But observing that A C' = A 0, A CC' = A C'C, we have B C' A CC'- 0 B C'C = A C'O + C + aa (B C' - B C'C) = - (C + AC) and the above proportion gives, therefore, sin Aa _a sin (a + I Aa) tan i AB cot(C + ) A(243) * The equations (239), (240), (241), and (242), contain each two factors less thln the corresponding equations given by Cagnoli. DIFFERENCES OF SPHERICAL TRIANGLES, 235 In the same manner we should find sin X Aa sin (a + g Aa) tan AC C cot (B + -AB) The quotient of (243) and (244) gives tan ' aB tan (B + AB) (245) tan i AC tan (C + A7)( In A B C and A B C', by (4), we have cos a = cos b cos c + sin b sin cos A cos (a + Aa) = cos b cos c + sin b sin c cos (A + hA) the difference of which gives sin I-2 a sin b sin c sin (A + AA) (246) sin -I AA sin (a + 1 Aa) The quotient of (243) divided by (246) gives sin A _A sin2 (a + l Aa) tan (C + ~ AC) ( - - = - - 2(247) tan AB sin b sin c sin (A + I AA) and from (244) and (246), in the same manner, sin 1 AA sin2 (a + I Aa) tan (B + AB) (248) tan I AC sin b sin c sin (A + I AA) 137. CASE IV. B and C constant. The equations of the preceding case (243 to 248), applied to the polar triangle, give sin AA a sin (A + 1 AA) 249 tan 1 ab cot (c + 1 AC) sin i AA sin (A + 1 AA) (250) tan i ac cot (b + } Ab) tan 4 Ab tan (b + 1 A) (251) tan I Ac tan (c + I ac) sin 1 AA sin B sin ' sin (a + x Aa) 252 sin i Aa sin (A + - A) 236 SPHERICAL TRIGONOMETRY. sin L Aa sin2 (A + 1 AA) tan (c + - Ac) 2 tan 1 Ab sin B sin ( sin (a + 1 Aa) sin 1 Aa sin2 (A + 1 AA) tan (b + 1 Ab)4) tan ~ Ac sin B sin C sin (a + i Aa) FINITE DIFFERENCES OF SPHERICAL RIGHT TRIANGLES. 138. All the preceding equations are, of course, applicable to right triangles, or to quadrantal triangles, and in some cases they assume simpler forms. Thus in Case I., if the variable C = 90~ (231) and (232) become sin Ab = sin (a + Aa) sin AB tan - Aa =- tan - Ab tan1 A AC and similar modifications take place in other cases. 139. When one of the constants is 90~, the preceding equations do not generally assume any simpler forms, but they may be transformed so as to involve the same variables in both members, which is generally desirable in their practical applications.* The method that we shall follow is so simple that it will be un, necessary to repeat it in every case. A single example will suffice to explain it. Let C (= 90~) and b be the constants; to find the relation of Ao and A B, we have between the two variables and the constant 6, the equations sin B = sin b cosec c sin (B + AB) = sin b cosec (c + Ac) the difference and sum of which, by P1. Trig. (105), (106), (131), and (132), are 2 sin b cos (c + ~ Ac) sin ~ Ae 2 cos (B +- AB) sin AB - B 2sinbcos( sin c sin (c + A c) 2 sin b sin (c + 1 ac) cos Ac 2 sin (B + ~AB) cos ~ AB = 2 + 2 Y"/ VVU 2 L-sin c sin (c + Ac) * Cagnoli gives these equations reduced so as to involve the same variables in noth members; but in almost every instance his formulae involve two factors more than are necessary, and are far less simple and convenient than those here given. DIFFERENCES OF SPHERICAL TRIANGLES. 2837 and the quotient of these is tan - AB tan 1 Ac tan (.B+ AB) tan (c + -2 Ac) which gives the first equation of the following article. This process always eliminates the constant, and is applicable in every case. When the equation to be differenced involves cosines, we employ P1. Trig. (107) and (108); if tangents, (115) and (116); if cotangents, (122); if secants, (129) and (130). The results are as follows: 140. CASE I. a = 90~ and b constant. tanA c tan( +-A c) tan'aB - tan(B+IAB) sin A a sin(2a+ a) sin AA - sin(2A+ AA) sin Ac sin(2 c + c) tan1AA - cot(A+ AA) 2 2",IP tan-A c cot(e +-A ) tan-A a cot( a + 2- a) tan'A a tan(a +-A a) sin B = sin (2SB +B) tan|-AA tan(A +I2AA) tan1 AB - cot (B+ 2 AB) (255) (256) (257) 141. CASE II. C = 90~ and c constant. sinAA sin (2A +AA) siB sin sin (2B+AB) taniA a tan(a + 1- a) 2 2 tan1AA - tan(A+ -AA) sin A a sin (2 a+A a).an'AB cot(B+ 2AB) tan1-Aa cot(a +Aa) tanlA b cot(b +LA b) tanA b tan(b +A b) tan~AB tan(B + -AB) sin A b sin (2 b +A b) tanAJA cot (A+ AA) 2 2L"2 ~a (258) (259) (260) 142. CASE III. C = 90~ and A constant. tan1- c tan(c +-A c) tanI a tan( a+ A a) tan~Ac cot (c +-A c) sin AB sin (2 B + AB) sin Ac sin(2 e +A c ) sin b sin(2 b + b) sin A a sin (2 a +A a) tan~A b - tan( b + A b) 2 2 L tan A b tan aB cot( b + b) cot (B+ ~AB) (261) (262) (263) tannAa cot(a+ Aa) tanAB - tan(B+ 'AB) 2 2~ L 143. If a constant side is 90~, the equations of finite differences for the triangle may be obtained hy applying the preceding equlations to the polar triangle 238 SPHERICAL TRIGONOMETRY. DIFFERENTIAL VARIATIONS OF SPHERICAL OBLIQUE TRIANGLES. 144. To obtain the differential variations, we have only to make the increments infinitely small in the equations of finite differences, observing the principles of P1. Trig. Art. 192. Or we may differentiate the equations of spherical triangles directly, employing the differentials of the trigonometric functions given in PI. Trig. Art. 192 For example, A and c being constant, to find the relation of d a and dB, we have sin A sin c = sin a sin C the differential of which is 0 = sin a d sin C + sin Cd sin a = sin a cos Cd C + cos a sin C da da tan a dC tan C and to find the relation of d a and d b, we have cos a = cos b cos c + sin b sin c cos A - sin a d a = - sin b cos c d b + cos b sin c cos A d b d a sin b cos c - cos b sin c cos A d b sin a or by (7), da - c= os C d b results which agree with those found from (236) and (232), by making Aa, Ab and AC infinitely small. By either method then, the following equations may be readily verified. 145. CASE I. A and c constant. d a tan a d b sin a d C tan dB sin C 264) d a d b tan a db- cos d = - sin O (265) da sin a d C dB- tanC d - cos a (266) d ~ - tan (7 d/~v DIFFERENTIAL VARIATIONS OF SPHERICAL, TRIANGLES. 235 146. CASE II. A and a constant. dB cos b d C0- cos c d b tan b dB tanB d b sin b d a- cos ctan B 147. CASE III. b and c constant. da d B- - sin a tan C dB tanB d C-= tan 0 dA sin A dB - sin Bcos d b cos B d c - cos 0 d c tan c d C tan C d c sin c d B cos b tan C da d a =- sin a tan B dC —= da dA a sin b sin C d A sin A d - sin C cos B (267) (268) (269i (270) (271) (272) 148. CASE IV. dA da —b d b d c da d b B and a constant. sin A tan c tan b tan c sin a sin b cos c dA d c dA d a sin A tan b (273) sin B sin c (274) (275) d a sin a d c sin c cos b DIFFERENTIAL VARIATIONS OF SPHERICAL RIGHT TRIANGLES. The preceding may also be used for right triangles; but it may be desirable to have the same variables in both members, as in the following formulse derived from those of Arts. 140, 141, and 142: 149. CASE I. a - 90~ and b constant. d c tan c d c cot c dB = tan B d a cot a d a sin 2 a d a 2 tan a dA = sin 2 A d B: sin 2B d c sin 2 c d A tan A d A = 2cotA d =- cot B (276) (277) (278) 240 SPHERICAL TRIGONOMETRY. 150. CASE II. C = 90~ and c constant. d A sin 2A d a cot a (279) d B -sin 2B d b cot b d a tan a d b tan b d A tan A d B= tan B 28 d a sin 2 a d b sin 2 b 8 d B 2 cot B d A 2 cotA ) 151. CASE III. C = 90~ and A constant. d c tan c d a sin 2 a (2 d a tana d b 2tan b ( d e 2 cot c d b cot b d~B sin 2 B dB cot (283) d e sin 2 c d a cot a d b sin 2 b d B tan (284) 152. The differential variations are often employed for approximate results, instead of the equations of finite differences, when the increments are very small. The remarks of P1. Trig. Art. 203, apply here also, but it is not necessary to introduce the radius in seconds, since all the parts of a spherical triangle are expressed in the same unit. DIFFERENTIAL VARIATIONS OF SPHERICAL TRIANGLES WHEN ALL THE PARTS ARE VARIABLE. 153. Let the equation cos a = cos b cos c - sin b sin c cos A be diffeientiated, all the parts being variable; we find sin ada (sin b cos c - cos b sin c cos A)db +- (sin c cos b - cos c sin b cos A) d c + sin b sin'c sin A dA Dividing by sin a, this becomes, by (7) and (3), da = cos Cdb + cos Bdc + sin b sin CdA (285) and in the same manner from the 2d and 3d equations of (4) we find db = cos A dc - cos Cda - sin c sin A dB (286) dc = cos B da+ cos A d b + sin a sin BdC (287) From these three equations, any three of the six differentials d a, d b, dc, dA, d B, d C, being given, the other three maybe determined by the usual processes of elimination. If any one of the parts be supposed constant, its differential will become zero, and these equations will assume simpler forms. If two of the parts be suppcsed constant, we can easily deduce all the equations of Arts. 145, 146, 147 and 148. APPROXIMATE SOLUTION OF SPHERICAL TRIANGLES. 241 CHAPTER VII. APPROXIMATE SOLUTION OF SPHERICAL TRIANGLES IN CERTAIN CASES. 154. WHEN some of the parts of the triangle are small, or nearly 90~, or nearly 180~, approximate solutions may be employed with advantage. These are generally found by means of series. 155. In a spherical right triangle (the right angle being C), given A and c, to find b We have tan b = cos A tan c (288) which is of the form in P1. Trig. (493), and may therefore be developed by (495) and (496) by putting x = b, y = c, p = cos A, whence p - 1 1 - cos A an2 A P - P 1 1 + cosA - and (495) and (496) become, [taking n = 0 in (495), and n = 1 in (496)], b c - tan2 A sin 2 c + tan' A sin 4 c -&c. (289) b r-c + cot' 2 A sin 2 c -- cot' - A sin 4 c + &c. (290) If A is small, cos A is nearly equal to unity, and b exceeds c by a small quantity which is approximately found by one or more terms of the series (289). If A is nearly 1800, or cos A nearly - 1, b exceeds — c by a small quantity, which is found by (290). For examples of the mode of computation, see P1. Trig. Art. 255. 156. Although these solutions are termed approximate, it must not be inferred that they are less accurate in practice than the direct solution of (288) by the tables; for the logarithmic tables are themselves only approximate, and the neglect of the higher powers in such series as (289) and (290) may involve a less theoretical error than the similar neglect of the higher powers in the series by which the tables are computed. In the examples of P1. Trig. Art. 255, the thousandths of a second were found with accuracy, which could not have been effected by a direct solution with less than eight decimal places in the logarithms. These considerations lead to the frequent employment of approximate solutions in astronomy. 157. If A and b are given, to find c, we have tan c - sec A tan b which is reduced to P1. Trig. (493), by putting x = c, y = b, p = sec A, sec A - 1 1 cosA see A 1 1 - cos A and the series will be c = b + tan2' A sin 2 b + - tan4 - A sin 4b +- &c. (291) = —b - cot2 A sin 2 b- cot4 A sin 4 b - &c. (292) 31 V 242 SPHERICAL TRIGONOMETRY. 158. Similar solutions apply to the equations of right triangles, tan a = sin b tan A cotB = cos c tan A the last being solved under the form tan (90~ - B) = cos c tan A We may also compute, in the same manner, the auxiliaries p and 9 in (122) and (134), so frequently employed in the solutions of oblique triangles. 159. In a right spherical triangle, given c and A, to find a, when A is nearly 90~. We have sin a = sin A sin c (293) from which we deduce tan (c- a) = tan' (450 - 4 A) tan i (c + a) (294) From this we may find c - a, which is supposed very small, by successive approximations. For a first approximation, let a = c in the second member, and find thence the value of c - a and of a; for a second approximation substitute in the second member the value of a just found; and so on until two successive values agree as nearly as may be desired. EXAMPLE. Given A = 89~, c -= 87~; find a. Here 45~ - 4 A = 0~ 30', and for the first approximation 4 (c + a) = 87~. log tan 4 (c -+ a) 1-28060 log tan2 (45~ - I A) 5-88172 ar co log sin 1" 5631443 i (c a) = 299"-74 log 1 (c - a) 2-4767.5 a 7 87 - 9' 59"'48 86~ 50' 0"-52 2D APPROx. 3D APROex. 4TH APPROX. 4 (c + a) 86~ 55' 0" 86~ 55' 8" 86~ 55' 8"-17 log tan 4 (c + a) 1-26868 1-26899 1-26900 tan2 (450 - 4 A) log ta 119615 1-19615 119615 sin i" log 4 (c - a) 2-46483 2-46514 2-46515 - (c - a) 291"-63 291".83 291"'84 c - a 9' 43"-26 9' 43"-66 9' 43"-68 a 86~ 50' 16"-74 86~ 50' 16"-34 86~ 50' 16"-32 The direct solution of (293) gives a - 86~ 50' 16", but cannot give the fractions of a second without tables of more than seven figure logs. We have given this problem, however, not so much on account of its particular utility, as for the purpose of introducing the method of approximation to which it leads, and which is often employed. The process here explained may obviously be applied to any equation if the form sin x = mn sin y when m is nearly equal to unity. APPROXIMATE SOLUTION OF SPHERICAL TRIANGLES. 243 160. In a spherical oblique triangle, given two sides and the included anqle, to find the other angles and side by series. If a, b and C are the data, to find c, we have cos c = cos a cos b - sin a sin b cos C Substituting half arcs, sin'2 c = sin2 ~ a cos b 6 + cos, a sin2 ~ b - 2 sin a a cos I b cos I a sin I b cos C which is of the form P1. Trig. (507), and may be developed by (508) by substituting sin i c for c, sin ~ a cos I b for a, and cos ~ a sin i b for b; so that (508) becomes log sin c = logcos asin b-M J[ tan a c os (C+ &c.] (295) To find A and B, we have, tan i (A + B) = is-+ ) cot C - cos ( (a + b) cot tan (A -- B) = sin ( cot b) sin j (a ) cotb) whence n,,, _ (cot Ia - tann,b tan [ ~ t- -~ ( cA Jr )]-( (t a + tan a tan [i.-ni l~ UA B} tan a+ (^ tan b tan [R - (A - B)] = (ta ta ) tan C a6 (tan 1 a -tan - Comparing these equations with P1. Trig. (493), and developing by (495), n = 0, t-n-^ ~b ({ tan _ bh\~ sin2C rr 4(A +B)= aC- i sin C ct a &c. (296) cot a~(cot j a) 'r i- (A - B)_ C= + t sin n sn a 2 + &. (297) If we develop by (496), we find c( s i -oon t ) sin 2 " (9) r — (A+B)=- C+ tota ) sin - ota sin2 &c. (298) (tan (ta - a ) a ib 2 -&c. (299) i~ — ~ (A — ~) = -- ~a —a (tai yi aa — sin 2 C I -,(AB_. tn) =a - C- s tn) n Csi- 2 -c. (299' tanb sin \tan 46/ 2 from which a selection will be made in any particular case, according to the convergency of the series. The terms of the series are in arc, and must be reduced to seconds, by dividing by sin 1". This solution may be applied to the case where two angles and the included side are the data, by means of the polar triangle. 161. To express the area of a spherical triangle in series. Compaing (229) with P1. Trig. (500), and developing by (502), we find 4 K- = tan i a tan 4 b sin C - tan 4i a tan2 4 b sin 2 C + &o. (800) 244 SPHERICAL TRIGONOMETRY. 162 LEGENDRE'S THEOREM. If the sides of a spherical triangle are very smnall cornvarpd with the radius of the sphere, and a plane triangle be formed whose sides are equal to those of the spherical triangle, then each angle of the plane triangle is equal to the corresponding angle of the spherical triangle minus one-third of the spherical excess. Let a, b and c be the sides of the spherical triangle expressed in arc, the radius of the sphere being unity; and let A', B' and C' be the angles of the plane triangle whose sides are a, b and c. Then we have, in the spherical triangle, cos a cos - cos b cos c cos A = sin b sin c Substitute in the second member of this, the values of cos a, &c., in series, by P1. Trig. (405) and (406), neglecting only powers above the fourth, viz. cos a = 1 - - ac+ '- a' cos b 1 — b- Ib; b 4 sin b b= - b cos c = 1 - c 4- c' sin c = c - c we find cos A = ~ (b' + c2 - a2) + -L (a - 64 - c4- 6 b2 c2) b c [1 -- (b + c)] Multiplying the numerator and denominator by 1 +- i (b +- c2), and neglecting terms of a higher order than the fourth, as before, we have sA c - a 4 a' b' + c' - 2 a'2 - 2 ac' - 2 bc 2 b c 24b c which, by P1. Trig. (225) and (239), becomes cos A - cos A' - i be sin2 A' Let A = A' - x, then since x is small, we may put cos x - 1, so that, by P1. Trig. (38), cos A = cos A'- x sin A' whence x =- b c sin A' But I b c sin A' - area of the plane triangle = very nearly area of the spherical triangle = K, whence x =}dK A' =A- -X The same reasoning applies to each of the other angles, so that B' _ B-K C' C -C jK which proves the theorem. 163. This theorem is applied in geodetical surveying, and is found to be sufficiently accurate for triangles whose sides are considerably greater than 1~. It is to be remembered that the sides are to be expressed in arc; and if they are given in feet (for example), they must be reduced to arc by dividing by the radius in feet, or, which is equivalent, the area must be divided by the square of this radius. If then r = radius of the earth in units of any kind, a, b and c the sides of the triangle in units of the same kind, and k the area of the plane triangle, we shall have K in seconds, by the equation K 7c s_ k r~ sin 1" EXAMPLE. In a triangle upon the earth's surface, given 6 = 183496-2 feet, c = 156122-1 feet, and A = 48~ 4' 32".35; to find the remaining parts. APPROXIMATE SOLUTION OF SPHERICAL TRIANGLES. 245 We have k -= - b c sin A, and the mean value of r = 20888780 feet. Hence log b 5-26363 log c 5-19346 log sin A 9-87159 ar co log 2 r2 sin 1" 0-37356 K 5"'04 log K 0-70224 It is evident that great accuracy in the value of r and of the other data is not required in computing K. We now have i K = 1"-68, A' = 48~ 4' 30"'67, and by solving the plane triangle with the data A', b and c, we find a = 140580-0 feet B' = 76~ 12' 22".19 C' - 55~ 43' 7"13 Adding i KI to each of these angles, the angles of the spherical triangle are B = 76~ 12' 23"'87 C = 55~ 43' 8"-81. For further details respecting geodetical triangles, and for the methods of solving spheroidal triangles, special works upon geodesy must be consulted, such as Legendre's Analyse des Triangles traces sur la surface d'une sple'oide; Puissant's Traits de Geodesie; Puissant's Nouvel essai de trigonometrie spheroidique; Fischer's Lehrbuch der hbheren Geoddsie; various papers by Gauss, Bessel, &c. 164. To solve a spherical triangle when two of its sides are nearly 90~. If a and b are nearly 90~, c and C are nearly equal, and it will be expedient to compute the small quantity C- c by an approximate method. We have, by (25), sin' 4 c -= sin2 I (a + b) sin2 4 C + sin' 4 (a - b) cos' 4 C and by P1. Trig. sin sin C sin (a + b) + cos' i (a + b)] sin2 I C the difference of which equations is sin i (C + c) sin i (C- c) = cost 4 (a + b) sin C - sin2 I (a - b) cos' C Let a' 90~ -a b' = 90~ b a' and b' being very small: also, since C and c are nearly equal, put (C+ c)= C then the above equation becomes sin C sin ~ (C- c) = sin (a' + b') sin C sin - (a'- b') cos' C Dividing by sin C = 2 sin 4 C cos 4 C, and substituting the arcs 4 (C- c), (a' + b'), 4 (a' - b'), for their sines, we find C-c = sin -1" [( ' b) tan C - (- ' ) cot 4 C] (301) which is the required approximate formula for the case when a', b' and C are given to find c. If a', b' and c are given, to find C, we may exchange C for c in the second member, whence - = sin 1" [( 2 + 2) tan i c - b'2 ) cot i c] (302) v2 246 SPHERICAL TRIGONOMETRY. CHAPTER VIII. MISCELLANEOUS PROBLEMS OF SPHERICAL TRIGONOMETRY. 165. In a given spherical triangle, to find the perpendicular from one of the angles upon the opposite side. Fig. 25. Denoting the perpendicular upon the side c (Fig. 25) C by p, we have sinp = sin b sin A (303, If the three sides or the three angles are given, we find by (48), or (51), and (303), ~A ~.. 2n 2NV jA<=^ B sin p = —. (304) sin c sin C in which n and N are given by (47) and (50). If we admit more than three parts of the triangle into the expression of p, we have, by (55), (56), and (303), 2 sinAsin s B 2 cos i a cos i b si - i sin s - s in -- cos S (305) cos j C sin ~ c 166. To find the radius of the circle described about a given spherical triangle. Fig. 26. The radius here understood is the arc 0 A = 0 B = 0 C, Fig. 26, drawn from the pole of the small circle CAs~ \ ~A B C to either of the angles. Let OAB = OBA =- x then - O CA + O CB = OA C + OB C = A - x + B- x = x (A + B -C)= S- putting S= (A + B + C). The triangle A O B being isosceles, the perpendicular O P bisects the side c, therefore if 0 A - R, we have tali c tan R = tal ta (306) cos x cos (S - C) or, by (66), 2 in si n asi b sin ic tan R -- (307= n By applying the principles of Art. 37, this will give the corresponding formulse of P1. Trig. (285). 167. From (65) and (66) we find cos (S - C) - cos S cot ~ a cot i b by which (306) is reduced to tan R _taan a tan ~ b tan ~ c, - cos S MISCELLANEOUS PROBLEMS. 247 Also, by the last equation of (56), (306) becomes sin c c tan - (309) cos t a cos b sin G 168. Substituting in (306) for tan 4 c by (39), _ / _ —_ - cos S_ tan s = / ( (S - ) cos (S- B) cos (S- = or, by (50), -cos ( tan R N (310 169. Let the sides of the triangle A B C, Fig. 27, be pro- Fig. 27 duced to meet in A', B', and C'; and denote the radii of the circles circumscribed about A'B C, B'A C, C'AB by R', R", R"' respectively. Then if 2 S' denote the sum of the angles of A' B C, (A, B and C being the angles of ABC), B, 2S'= 2- B- C~+ A S'-A' = =-(A +B+ C) =7r-S so that (306) applied to A' B C gives c tatan ' a tan 1 a cos (S'- A') - cos S and in like manner ___n _ b (311) tan R" (3 — - cos S tan R"' tan 4 c - cos S Substituting for tan 4 a, &c., by (39), or for cos S by (69), cos (S -A) 2 sin o a cos ~ b cos C e tan R' - n N n tan R" cos (S -B) 2 cos a sin ~b cos (812) tan R" --- o -- = ) (312) cos (S-C) cos nacos-bsin- c 170. Combining (310) with (312), we find the relation cot R cot R' cot R" cot R"' = N2 (313) If this be multiplied successively by the squares of (310) and (312), we obtain tan R cot R' cot R" cot R"' = cos* S cot R tan R' cot R" cot R"' = cos* (S - A) (814) cot R cot R' tan R" cot R"' = cos2 (S - B) cot R cot R' cot R" tan R"' = cos' (S - C) 248 SPHERICAL TRIGONOMETRY. 171. Again, from (310) and (312) we find - tan R + tan R' + tan R" + tan R"' cos S + cos (S - A) + cos (S - B) + cos (S - C) N 2 cos ~ A cos i (B + C) + 2 cos ~ A cos J (B - C) N whence - tan R -tn - tan " + tan R tan 4cos 4cos Bcos C (815 We shall find in a similar manner 4 cos.4 Asin 4 B sin ~ C tan R - tan R' + tan R" + tan R"' 4 cos si s N 4 sin A cos Bsin C tan R + tan R' - tan R" + tan R'" 4 sin. A. sin i a. (316) 4 sin A sin B cosf C tan R + tan R' + tan R" - tan R'" 4 in It is also easily shown that 2 t 2 cos~A cos B cos C tan2 R + tan2 R' + tan2 R" + tan' 2 +- 2~' cos cos (317) 172. To find the radius of the circle inscribed in a given spherical triangle. Fig. 28. In Fig. 28, 0 being the pole of the required circle, / draw OP', OP" and OP'" to the points of contact, and join OA, OB. We have 0P" — 0P"' and the triangles A OP" and A OP"' right-angled at P" and P"; hence o Jl^'^or^. A sin OP" sin OPP"' sin OA P" - sin OA P'" B -'sin A O sin sinAP A. therefore 0 A P" = 0 A P'", (for we cannot have OA P" =- - OA P"'), and the pole of the inscribed circle is consequently found by the same construction as inplano, namely, by bisecting the angles of the triangle. If then we put s = 4 (a + b + c), and r = radius of the inscribed circle, we have A P'" + B P' + CP' = AP"' a = s, A P"' = s- a and the right triangle A 0 P"' gives tan r = sin (s - a) tan 4 A (818) corresponding with the formula of P1. Trig. (288). Substituting, in (318), the value of tan 4 A, tan r J(sin (s - a) sin (s - b) sin (s - )) <~J \ sin s n or tan r==- (319) sn sin Substituting, in (318), the value of sin (s - a) given by (58), tan r = co --- co(320) 2 cos ~ A cos ~ B cos ~ C Also, by (51), we have N =- sin B sin C sin a, which reduces (320) to sin B sin A. tan r = sin -sin" sin a (821l fos ~ A MISCELLANEOUS PROBLEMS. 249 173. Let the radii of the circles inscribed in the three triangles A'BC, B'AC, C'AB of Fig. 27, be r', r" and r"'. Then if s' denote the half sum of the sides of A'BC, we have 2 s' = 2 - - c + a s' - a = - - (a+ b 6 c) = r - so that (318) applied to the three triangles, gives tan r' - sin s tan I A tan r" = sin s tan ~ B (822) tan r"' = sin s tan ~ C Substituting in these the values of tan i A, &c., or of sins, n N an sin (s - a) 2 cos A sin j B sin C tan r" ---- (323 sin (s - b) 2 sin } A cos j B sin C ( n N tan r"' - N sin (s - c) 2 sin A sin I B cos } C Also, by (321), tan' = cos Bcos C sin a cos 2 A s cos C C cos A tan r" = cs c sin6 b (324) cos ~ B cos A cosB sin c tan r"' = sin c cos -1 C 174. The product of (319) and (323) gives n4 tan r tan r' tan r" tan r"' = _- n' (325) whence, as in Art. 170, cot r tan r' tan r" tan r"' - sin' s tan r cot r' tan r" tan r"' = sin2 (s - a) tan r tan r' cot r" tan r"' = sin' (s - b) (326) tan r tan r' tan r" cot r"' = sin' (s - c) 175. We find from (319) and (323), as in Art. 171, 4 sin a- a sin b sin ~ c cot r + cot r' - cot r" + cot r"' = 4 sin 4 a cos ( b cos A c cot r - cot r' + cot r" + cot r"' -- 4 cos c a sin b cos ~ c cot r + cot r' - cot r" - cot r"' 4 cos 8 a cos 2 b sin 2 c cot r +4 cot r' + cot r" - cot r'" = 2 - 2 cos a cos b cos c cot r +- cotS r''- cot' r" t' -— ot/ = - - 82 250 SPHERICAL TRIGONOMETRY. 176. From (309) and (321), we find tan r 4 sin A sin B sin i cos I a cosb cos (828) tan R From (307) and the first of (327), - cot r + cot r' + cot r" + cot r"' = 2 tan R (329) From (315) and (320), - tan R + tan R' + tan R" + tan R"' = 2 cot r (330) and other similar relations are found by comparing (312) with (327), and (316) with (323). 177. The following relations are also worth remarking. If p is the perpendicular from C upon c, 2 sin i a sin } b tan R sinp = -{ 1 (331) 2 cos A cosB - cot r sinp - in - sin ~ C 178. The pole of the circle inscribed in a spherical triangle is also the pole of the circle circumscribed about the polar triangle; and the radii of these circles are complements of each other. The arcs bisecting the angles of a given triangle will evidently bisect the sides of the polar triangle, and will be perpendicular to those sides respectively; the common intersection of these arcs is therefore at once the pole of the circle inscribed in the first and circumscribed about the second. Again, if we join the angular points of the polar triangle with this common pole, the arcs thus drawn, being produced to meet the sides of the first triangle, are perpendicular to those sides, and therefore pass through the points of contact of the inscribed circle. Each of these arcs - 90~, and is at the same time the sum of the two radii of the circles in question. This latter property is also obvious from the analytical expressions of the two radii. By means of it, we might have deduced all the formulas for the inscribed from those for the circumscribed circle, or vice versa. 179. 27 find the arc joining the poles of the circles inscribed in, and circumscribed about a given spherical triangle.* Fig. 29. C Let 0 be the pole of the circumscribed circle, Fig. 29, and 0' that of the inscribed circle. Put o_~ \ 000' D); then 20 1~ ' | cosD = cos A 0 cos A 0' sin A 0 sin A ' cos OA 0O By Art. 166, we have OAB = S- C, whence ---- B OAO' = S- C- ( A = i (B- C) We have also cos AO' = cos O'P cos AP = cos r cos (s - a) sin O'P sin r sin A O' AP A sin O'AP- sin ~ A * Hymer's Spherical Trigonometry MISCELLANEOUS PROBLEMS. 251 'Vher:fore, cos D cos t (B - C) ccs -D = cot r cos (8 - a) - tan R cos (B — cos R sin r sin i A Substituting by (319), (307), and (44), cos D sin s cos (s - a)+ 2 sin } b sin c sin i (b + c) f os R sinr n sin a - sin b - sin c 2n whence,:y (53), / cosD \' 1 -+ sinasinb -sinasinc sibsinbsin-cosacosbcosc Tacos R sin r 2 n7 by PL. Trig. (179), =(sin 8 + 2 sin a sin I b sin c) = (cotr + tan R)2 cos' D = cost (R- r) - cos' R sin' r sin D = sin2 (R - r) - cos2 R sini r (332) If the inscribed circle is inscribed in A'BC, Fig. 27, and its radius = r'. we have, by a similar process, sin2 D' = sin2 (R + r') - cos2 R sin' r' (338) 180. To find the equilateral spherical triangle inscribed in a given circle. If R = radius of the given circle, and A = one of the angles of the equilateral triangle, we have, by (310), and P1. Trig. Art. 76, tan- - cos - A 3 cos yA-4 cos A cos3 ~ A cos3 ~ A whence cos i A = (4 tan ) (334) 181. To find the equilateral spherical triangle circumscribed about a given circle. If r - radius of the given circle, and a = one of the sides of the triangle, we find sin i a=,|(4 + cot= r )3 4f(4+cot ) (335) 182. Given the base and area of a spherical triangle, to find the locus of the vertex. Fig. 30. Let a = the given base, and K = area of ABC, Fig. 30. Produce AB and AC to meet in A'. Let 0 be the pole of the circle described about A'BC. The radius of this B~ | circle is given by the first equation of (311), which, by // \ L~ (224) becomes tan ') sn a K (335) sin ~ ---^A -l / The second member of this equation, being constant for all the triangles of the same base a, and the same area K, shows that R'is also constant, and consequently, that the nro.;Di SPHERICAL TRIGONOMETRY. point A is always found upon the circumference of the same small circle A'BC. But A and A' being the extremities of the same diameter of the sphere, A is als6 found upon a small circle, equal and parallel to the circle A'BC. The perpendicular distance (p') of 0 from the base BC, is found by the equation cos R' cos P' -— os a cos i a and the pole of the locus of A is in the same perpendicular, at a distance from BC = -pi' = p, whence cos R' cosp -cos - (337) The equations (336) and (337) determine the radius and position of the pole of the required locus, which may therefore be constructed. This elegant proposition is due to Lexell. 183. To find the angle between the chords of two sides of a spherical triangle. Fig. 31. In Fig. 31, O being the center of the circumscribed circle, the angle between tne ohords of the sides AC and BC is half the spherical angle AOB. If, then, C, = angle between the chords of a and b we have cos C( = cos AOP = sin OAP cos AP or, by Art. 166, cos C, = sin'(S - C) cos -2 c (338) By (72) this becomes cos C, = sin 1 a sin ~ b + cos a a cos ~ b cos C (339) 184. The preceding problem is employed for geodetical triangles, in which C, differs very little from C, in which case it is expedient to compute the small difference C - C, = x. We easily reduce (339) to the following: zos C, = cos (a - b) cos' ~ C- cos i (a + b) sin' C a =cos2 C -2 sin I (a-b) cos' C-sin I C+ 2 sinI 4(a + b) sinm C Subtracting cos C = cos i C - sin2 i C, we have, sin (C+ C,) sin (C- a,) = sin j (a+ b) sin~ I C- sin' I (a — b) C acs or approximately, taking sin ~ (C + C,) = sin C = 2 sin ( cos ~ C and sin (C- C,) =- x sin 1" z being expressed in seconds, 1 1 x = -- sin' (a 4- b) tan IC- si 1" sin' 2 (a -- b) cot ' ' 840) MISCELLANEOUS PROBLEMS. 253 1R f a great circle (DE, Fig. 32) bisect the base of a spherical triangle zt right angles, any great circle (FG), perpendicular to it, divides the sides (AC, BC) into segments whose sines are proportional; that is, sin FA: sin FC = sin GB: sin GC (341).,et P be the pole of ED, (DP = 90~), and Fig. 32. PGF any great circle drawn through P, and therefore perpendicular to DE. Then, since C PB + PA = 2 PD =180~ 0 we have, by (3), sin F sin FA sin P sin PA sin P sin PB A sin G sin GB sin F sin FC sin G sin G D B whence, by division, the theorem (341). The arc FG is analogous to the parallel to the base in plane triangles. 186. If two arcs of great circles, (AB, CD, Fig. 33), terminated by any circle, intersect, the products of the tangents of the semi-segments are equal to one another; that is, tan ~ AE tan ~ EB = tan I CE tan I- ED (342) Let P be the pole of the circle DACB. Join PE and draw the perpendiculars PF, PG, bisecting the arcs AB and CD. Then we have cos FE cos PE cos PE cos GE cos -FB cos PB - cos PD cos GD cos FE- cos FB cos GE- cos G ) cos FE + cos FB cos GE + cos GD which, by P1. Trig. (110), gives (342). Fig. 33. B 187. If three arcs be drawn from the angles of a spherical triangle through the same point, to meet the opposite sides, the products of the sines of the alternate segments of the sides will be equal. Thus, in Fig. 34, we shall have sin AB' sin CA' sin BC' = sin CB' sin BA' sin AC' (343) For we easily find sin AB' sin AP sin APB' sin CB' sin CP sin CPB' sin AA' sin C(P. sin CPA' sin BA' sin BP sin BPA' sinB C' sin BP sin BPC' sinAC' sin AP sin APC' Fig. 34. C Multiplying these equations together, the product of the second members is unity, whence (343). Thn same property is easily extended to the segments of the angles. 188. It follows, that when three arcs are drawn from the three angles, so as to satisfy the condition (343), they must intersect in the same point. This occurs in the same cases as in plane triangles, that is, when the angles are bisected; when the sides are bisected; when the three arcs are drawn from the angles to the points of W 254 SPHERICAL TRIGONOMETRY. contact of the inscribed circle; and when the three arcs are the three perpendiculars upon the sides. The first three of these cases are obvious. To prove the last, if A', B' and C', Fig. 84, are right angles, we have cosAB' cos CA' cos BC' cosAB cos CA cos BC cos CB' cos BA' ce AC' cos CB cos BA cos AC whence cosAB' cos CA' cos BC' - cos CB' cos BA' cos AC' and in the same manner we find tan AB' tan CA' tan B C'- tan CB' tan BA' tanAC' The product of these two equations gives the condition (343), and therefore the per. pendiculars intersect in the same point. 189. To find the arc drawn from any angle of a spherical triangle to a given point in the opposite side. In the triangle PA A", Fig. 35, let PA' be drawn; we have Fig. 35. P _"_ — _- \ A_ _!_ —i A" A' cos PA' sin A A" = cos PA' sin (A A' + A' A") = cos P A' cos A'A" sin A A' - cos P A' cos A A' sin But in the triangles PA A', P A'A" we have, by (4), cos PA' cos A A' cos PA - sin PA' sin AA' cos PA'A cos PA' cos A'A" = cos PA" + sin PA' sin A'A" cos PA'A A'A" which substituted above give cos PA' sin A A" - cos PA sin A'A" - cos PA" sin AA' (344) which determines PA', the sides PA and PA" and the segments of the side A A" being given. 190. Let three arcs PA, PA', PA", Fig. 35, passing through the same point P, be intersected by two others A A" and B B" whose intersection is Q; we have several symmetrical relations among the parts of the figure which find their application in astronomy. Let the points A, A', A" be given in position by their distances from Q, and prt A Q -= AB tj PB =-, A'Q A= a' A'B' -t' PB' =, A" Q = " AB" B = tPB" PB" =- By P1. Trig. (171), we have sin a sin (a' - ac") + sin a' sin (a" - a) + sin a" sin (ae- a') = 0 and in Fig. 35, sin / sin B sin," sin B" sin a sin B = — i sin Q sin, MISCELLANEOUS PROBLEMS. 25 5 whence sin 2 sin " sin B" sin c -- s sin Qsi and similarly sin f' sin?n" Sin B" sin '/ sin Q sin &" sin 2" sin B" sin a" = -- sin. y" sin Q which, substituted above, give sin2 2 ( ',") q sin f/' sin f/" si sin ' - ') +- - ' sin (c"- ) -+ -, sin (- a') = 0 (345 sin -y ) / sin V vn a) sin ^/I 'S Again, if we express (344) in the notation of this article, it becomes cos (f+ 2) sin ('-")+cos (3'+ iin (n (" —) + cos ("+ ") sin (a-a')=0 (346) which, added to (345), gives sin(in42-) sin(Q'-4-?') sin(2"~- 2,") sin +)sin(s(-a")+ sin( " —) + sin( " sin(a —a')= 0 (347) tan?, tanil, tan2V 191. If P is the pole of A Q, we have A +:, = ' + ' — = "+," = 900 and (345) and (347) both give tan 2 sin (L' - a") + tan /' sin (a" - a) + tan '" sin (a - ') = 0 (348) 192. To find the inclination of two adjacent faces of a regular polyhedron, and the radii of the inscribed and circumscribed spheres. Let C and E, Fig. 36, be the centres of two adjacent faces whose common edge is A B; 0 the centre of the inscribed and circumscribed spheres. Draw 0 D bisecting AB at right angles; draw CD, ED, which will also evidently be perpendicular to A B; and put I =- inclination of the faces = CD E Big. 36. R = radius of the circumscribed sphere = 0A = 0 B A r = radius of the inscribed sphere = 0 C = 0 E a = one of the edges = A B / m = number of faces that form a solid angle n = number of sides of a face Suppose a sphere to be described about the centre 0 \ with any radius, and c a d the triangle formed upon its sur- \ face by the planes COD, O A, A 0 D; this triangle is \ Pight-angled at d and gives c' d cos c a d \ cos cd = os — \a\ sin a c d But cos c d _ cos C 0 D, and C 0 D = 90~ - CDo= -I I c a d = j angle of the planes 0 A C and A E 1 2 r 7r 2 7 m 1 2cr c acd^=~ACB= 1. ^ 7 -- 2 n n 256 SPHERICAL TRIGONOMETRY. 9r therefore cos sin i 1' — c (49) sin - n Then from the triangles 0 CD, A CD, &c., we find r 2 tan II cot (350) n r = R os ac R cot a c d cot c ad = R cot - cot - n m R -- tan j tan- (361) 2 m 193. To find the surface and volume of a regular polyhedron. Let f= number of faces of the polyhedron; =- the surface, and V= the volume; then the area of each face (the notation of the preceding article being continued) is equal to n nr A B X CD X n = a - cotwhence nf r S = a9 - cot- (352) n and since V= SX -r, nf V= a' 2 tanI cot2 - (353) 24 ff n 194. To find the surface and volume of a parallelopiped, given the edges anl their inclinations to each other. Fig. 37. Let 0 P, Fig. 37, be a parallelopiped, whose edges OA = a, OB r b, O C =c, and their inclinations B 0 C =-., A 0 C =- /, /A OB = y, are given. p The area of any face, as B C, is found by c / / / the formula b c sin a, and therefore fox the whole surface, we have / S =-^ 2 (b csin a + a csin + asin) (354).^~ \ / \^~ / ~To find the volume, let CD be the altitude, then A2t V-= base AB X CD = a b sin X CD Suppose a sphere to be described about 0, whose intersections with the planes BOG, AOG, AOB and DO0 are B'C' = a, A'C' =,2, A'B' = -, and C'D'. The triangle A'C'D' is right-angled at D', whence CD = c sin C'D' = c sin / sin C'A'B' or by (46), if o= + (x + 3 + '), C D = / [sin sin (s- a) sin (r- l) sin ( -- )].whence V= 2 a b c [sin s sin (o- a) sin (o - B) sin (o- -?)] (855) THE END.