/9// CORNELL UNIVERSITY LIBRARY 3 1924 073 537 254 The original of this book is in the Cornell University Library. There are no known copyright restrictions in the United States on the use of the text. http://www.archive.org/cletails/cu31924073537254 A TEEATISB ON PLANE TEIGONOMETBY CAMBRIDGE UNIVERSITY PRESS ILonftan: FETTEE LANE, E.G. C. F. CLAY, Manager ffiliinlmtBl): 100, PRINCES STREET asniin: A. ASHER AND CO. Eeipjis: ^ A. BROCKHAUS 0tto Bork: G. P. PUTNAM'S SONS JSomtia!) anti CalctittB: MACMILLAN AND CO., Ltd. All rights reserved A TREATISE ON PLANE TEIGONOMETEY BY E. W. HOBSON, Sc.D., LL.D., F.E.S., SADLEIRIAN PROFESSOR OF PURE MATHEMATICS, AND FELLOW OF CHRIST'S COLLESB, CAMBRIDGE THIRD EDITION Cambridge : at the University Press 1911 First Edition 1891 Second Edition 1897 Third Edition {revised and enlarged) 1911 PEEFACE TO THE THIED EDITION T HAVE taken the opportunity afforded by the need for a new edition to subject the whole work to a careful revision, and to introduce a considerable amount of new matter. In Chapter i I have inserted a theory of the lengths of circular arcs, and of the areas of circular sectors, based upon arithmetic definitions of their measures. Much of that part of the work which deals with Analytical Trigonometry has been re-written. Proofs of the transcendency of the numbers e and tt have been introduced into Chapter XV. It is hoped that the proof there given of the impossibility of "squaring the circle" will prove of interest to many readers to whom a detailed discussion of this very interesting result of modem Analysis has hitherto not been readily accessible. E. W. HOBSON. Christ's College, Cambridge, October, 1911. PEEFACE TO THE FIEST EDITION TN the present treatise, I have given an account, from the modern point of view, of the theory of the circular functions, and also of such applications of these functions as have been usually included in works on Plane Trigonometry. It is hoped that the work will assist in informing and training students of Mathematics who are intending to proceed considerably further in the study of Analysis, and that, in view of the fulness with which the more elementary parts of the subject have been treated, the book will also be found useful by those whose range of reading is to be more limited. The definitions given in Chapter iii, of the circular functions, were employed by De Morgan in his suggestive work on Double Algebra and Trigonometry, and appear to me to be those fi-om which the fundamental properties of the functions may be most easily deduced in such a way that the proofs may be quite general, in that they apply to angles of all magnitudes. It will be seen that this method of treatment exhibits the formulae for the sine and cosine of the sum of two angles, in the simplest light, merely as the expression of the fact that the projection of the hypothenuse of a right-angled triangle on any straight line in its plane is equal to the sum of the projections of the sides on the same line. The theorems given in Chapter vii have usually been deferred until a later stage, but as they are merely algebraical consequences of the addition theorems, there seemed to be no reason why they should be postponed. PREFACE Vll A strict proof of the expansions of the sine and cosine of an angle in powers of the circular measure has been given in Chapter viii ; this is a case in which, in many of the text books in use, the passage from a finite series to an infinite one is made without any adequate investigation of the value of the remainder after a finite number of terms, simplicity being thus attained at the expense of rigour. It may perhaps be thought that, at this stage, I might have proceeded to obtain the infinite product formulae for the sine and cosine, and thus have rounded off the theory of the functions of a real angle ; for convenience of arrangement, however, and in order that the geometrical appli- cations might not be too long deferred, the investigation of these formulae has been postponed until Chapter xvii. As an account of the theory of logarithms of numbers is given in all works on Algebra, it seemed unnecessary to repeat it here ; I have consequently assumed that the student possesses a know- ledge of the nature and properties of logarithms, sufficient for practical application to the solution of triangles by means of logarithmic tables. In Chapter xii, I have deliberately omitted to give any account of the so-called Modern Geometry of the triangle, as it would have been impossible to find space for anything like a complete account of the numerous properties which have been recently discovered; moreover many of the theorems would be more appropriate to a treatise on Geometry than to one on Trigonometry. The second part of the book, which may be supposed to commence at Chapter xiii, contains an exposition of the first principles of the theory of complex quantities ; hitherto, the very elements of this theory have not been easily accessible to the English student, except recently in Prof Chrystal's excellent treatise on Algebra. The subject of Analytical Trigonometry has been too frequently presented to the student in the state in which it was left by Euler, before the researches of Cauchy, Abel, Vlll PREFACE Gauss, and others, had placed the use of imaginary quantities and especially the theory of infinite series and products, where real or complex quantities are involved, on a firm scientific basis- In the Chapter on the exponential theorem and logarithms, I have ventured to introduce the term "generalized logarithm" for the doubly infinite series of values of the logarithm of a quantity. I owe a deep debt of gratitude to Mr W. B. Allcock, Fellow of Emmanuel College, and to Mr J. Greaves, Fellow of Christ's College, for their great kindness in reading all the proofs; their many suggestions and corrections have been an invaluable aid to me. I have also to express my thanks to Mr H. G. Dawson, Fellow of Christ's College, who has undertaken the laborious task of verifying the examples. My acknowledgments are due to Messrs A. and C. Black, who have most kindly placed at my disposal the article "Trigonometry" which I wrote for the Encyclopcedia Britannica. During the preparation of the work, I have consulted a large number of memoirs and treatises, especially German and French ones. In cases where an investigation which appeared to be private property has been given, I have indicated the source. I need hardly say that I shall be very grateful for any corrections or suggestions which I may receive from teachers or students who use j;he work. E. W. HOBSON. Christ's College, Cambridge, March, 1891. CONTENTS CHAPTER I. THE MEASUREMENT OF ANGULAR MAGNITUDE. ARTS. 1. Introduction 2 — 3. The generation of an angle of any magnitude 4. The numerical measurement of angles 5 — 10. The circular measurement of angles 11. The length of a circular arc . 12. The area of a sector of a circle Examples on Chapter I PAGES 1 1—3 3—4 4—6 7—10 10 10—11 CHAPTER II. THE MEASUREMENT OF LINES. PROJECTIONS. 13 — 16. The measurement of lines 17. Projections 12—13 13—14 CHAPTER III. THE CIRCULAR FUNCTIONS. 18 — 21. Definitions of the circular functions 22 — 24. Relations between the circular functions 25. Bange of values of the circular functions 26 — 29. Properties of the circular functions 30. Periodicity of the circular functions 31. Changes in the sign and magnitude of the circular functions 32. Graphical representation of the circular functions 33. Angles with one circular function the same 34. Determination of the circular functions of certain angles 35 — 38. The inverse circular functions Examples on Chapter III 15—18 19—20 20 21—24 24 24—26 26—28 28—29 29—32 32—33 33—35 CONTENTS CHAPTER IV. THE CIRCULAR FUNCTIONS OF TWO OR MORE ANGLES. AETS. 39—43. 44—45. 46. 47. 48. 49. 50. 51. 52. 53. 54. The addition and subtraction formulae for the sine and cosine 36 — 41 Formulae for the addition or subtraction of two sines or two cosines ........ 41 — 44 Addition and subtraction formulae for the tangent and cotangent 44 — 45 Various formulae 45 — 47 Addition formulae for three angles .... 47- — 48 Addition formulae for any number of angles . . 48 — 49 Expression for a product of sines or of cosines as the sum of sines or cosines 50 — 52 Formulae for the circular functions of multiple angles 52 — 53 Expressions for the powers of a sine or cosine as sines or cosines of multiple angles 53 — 54 Relations between inverse functions .... 54 — 55 Geometrical proofs of formulae 55 — 57 Examples on Chapter IV 58—62 CHAPTER V. THE CIRCULAR FUNCTIONS OF SUBMULTIPLE ANGLES. 55—63. Dimidiary formulae 63—69 64. The circular functions of one-third of a given angle . 70 — 72 65 — 66. Determination of the circular functions of certain angles 72 — 75 Examples on Chapter V 75 — 77 CHAPTER VI. VARIOUS THEOREMS. 67. Introduction 68. Identities and transformations 69. The solution of equations 70. EUminations 71. Relations between roots of equations 72. Maxima and minima. Inequalities 73. Porismatic systems of equations . 74 — 77. The summation of series Examples on Chapter VI 78 78—82 82—83 84—85 85—87 87—89 89—90 90—94 94—103 CONTENTS XI CHAPTER VII. EXPANSION OF FUNCTIONS OF MULTIPLE ANGLES. ARTS. 78—79. 80—83. 84. 85. 86—91. Series in descending powers of the sine or cosine Series in ascending powers of the sine or cosine The circular functions of submultiple angles Symmetrical functions of the roots of equations Factorization Examples on Chapter VII . PAGES i 104- -106 106- -109 109- -110 110- -114 114- -120 120- -123 CHAPTER VIII. RELATIONS BETWEEN THE CIRCULAR FUNCTIONS AND THE CIRCULAR MEASURE OF AN ANGLE. 92— 9.5. 96. 97—98. 100. Theorems Euler's product The limits of certain expressions .... Series for the sine and cosine of an angle in powers of its circular measure The relation between trigonometrical and alge- braical identities .... Examples on Chapter VIII .... 124—127 127—129 130—131 131—134 135 135—138 CHAPTER IX. TRIGONOMETRICAL TABLES. 101. Introduction 102—105. Calculation of tables of natural circular functions 106. The verification of numerical values 107. Tables of tangents and secants 108. Calculation by series 109. Logarithmic tables 110—111. Description and use of trigonometrical tables 112—114. The principle of proportional parts 116_117. Adaptation of formulae to logarithmic calculation 139 139—143 143 143 144—145 145 145—147 147—152 152—154 xu CONTENTS CHAPTER X. RELATIONS BETWEEN THE SIDES AND ANGLES OF A TRIANGLE. ARTS. 118—124. 125. 126. 127—128. 129. Theorems The area of a triangle Variations in the sides and angles of a triangle . Relations between the sides and angles of polygons The area of a polygon Examples on Chapter X PAGES 155—159 159 160—161 161—162 162—163 164—166 CHAPTER XI. THE SOLUTION OF TRIANGLES. 130. Introduction 131 — 133. The solution of right-angled triangles . 134 — 140. The solution of oblique-angled triangles 141 — 144. The solution of polygons 145 — 149. Heights and distances . . . . Examples on Chapter XI . . . 167 167—169 169—175 176—178 178—182 182—189 CHAPTER XII. PROPERTIES OF TIUANGLES AND QUADRILATERALS. 150. Introduction 151. The circumscribed circle of a triangle 152 — 154. The inscribed and escribed circles of a 155. The medians 156. The bisectors of the angles 157. The pedal triangle .... 158. The distances between special points 159. Expressions for the area of a triangle 160 — 163. Various properties of triangles 164 — 167. Properties of quadrilaterals 168. Properties of regular polygons 169. Examples Examples on Chapter XII 190 190—191 191—195 195—196 196—197 197—198 198—201 201 201—203 203—208 208—209 209—213 213—223 CONTENTS XUl CHAPTER XIII. COMPLEX NUMBERS. ABTS. 170. Introduction 171 — 174. The geometrical representation of a complex number 175 — 177. The addition of complex numbers . 178. The multiplication of complex numbers 179. Division of one complex number by another 180 — 185. The powers of complex numbers 186—187. De Moivre's theorem 188. Factorization . 189. Properties of the circle . 190. Examples .... Examples on Chapter XIII PAGES 224 224—227 227—229 229—231 231—232 232—236 237—239 239—240 241 241—242 243—245 CHAPTER XIV. THE THEORY OF INFINITE SERIES. 191. Introduction 192 — 196. The convergence of real series 197. The convergence of complex series 198. Continuous functions .... 199 — 201. Uniform convergence .... 202. The geometrical series .... 203 — 208. Series of ascending integral powers 209. Convergence of the product of two series 210. The convergence of double series . 211—212. The Binomial theorem .... 213 — 217. The circular functions of multiple angles 218 — 219. Expansion of the circular measure of an angle in powers of its sine .... 220 — 222. Expression of powers of sines and cosines in sines and cosines of multiple angles . 246 246—251 251—252 253 253—257 257—258 258—265 265 266—268 268—272 272—279 279—280 280—283 XIV CONTENTS CHAPTER XV. THE EXPONENTIAL FUNCTION. LOGARITHMS. AliTS. 223 — 227. The exponential series 228. Expansions of the circular functions 229 — 230('). The exponential values of the circular functions 231 — 232. Periodicity of the exponential and circular func- tions ....... 233 — 237. Analytical definition of the circular functions 238—239. Natural logarithms . 240 — 244. The general exponential function 245. Logarithms to any base . 246 — 248. Generalized logarithms 249 — 250. The logarithmic series 251. Gregory's series .... 251(')_251P). The quadrature of the circle . 252 — 254. The approximate quadrature of the 255. Trigonometrical identities . 256 — 257. The summation of series . Examples on Chapter XV circle PAGES 284—287 288 288—290 291 291—296 296—297 297—300 300 300—301 302—304 304^305 305—310 310—311 311—312 312—315 315—321 CHAPTER XVI. THE HYPERBOLIC FUNCTIONS. 258. Introduction 259. Relations between the hyperbolic functions 260—261. The addition formulae .... 262. Formulae for multiples and submultiples 263 — 265. Series for hyperbolic functions . 266. Periodicity of the hyperbolic functions 267 — 270. Area of a sector of a rectangular hyperbola 271. Expressions for the circular functions of com- plex arguments 272 — 274. The inverse circular functions of complex argu ments 275 — 276. The inverse hyperbolic functions 277. The solution of cubic equations 278. Table of the Gudermannian function Examples on Chapter XVI 322 322—323 323—324 324 324—325 326 326—331 331 331—333 333—334 335—336 336 337 CONTENTS XV CHAPTER XVII. INFINITE PRODUCTS. AKTS. PAGES 279 — 281. The convergence of infinite products . . . 338 — 342 282 — 292. Expressions for the sine and cosine as infinite pro- ducts 343 — 354 292 W. Representation of the exponential function by an infinite product 354 — 355 293 — 295. Series for the tangent, cotangent, secant, and co- secant 355 — 359 296 — 299. Expansion of the tangent, cotangent, secant, and cosecant in powers of the argument . . 360 — 364 300. Series for the logarithmic sine and cosine . . 365 — 367 301. Examples 367—369 Examples on Chapter XVII 369—373 CHAPTER XVIII. CONTINUED FRACTIONS. 302—303. Proof of the irrationality of tt . . . . 374—375 304. Transformation of the quotient of two hypergeo- metric series 375 305. Euler's transformation 376 Examples on Chapter XVIII .... 376—377 Miscellaneous Examples 378 — 383 CHAPTER I. THE MEASUREMENT OF ANGULAR MAGNITUDE. 1. The primary object of the science of Plane Trigonometry is to develope a method of solving plane triangles. A plane triangle has three sides and three angles, and supposing the magnitudes of any three of these six parts to be given, one at least of the three given parts being a side, it is possible, under certain limitations, to determine the magnitudes of the remaining three parts; this is called solving the triangle. We shall find that in order to attain this primary object of the science, it will be necessary to introduce certain functions of an angular magnitude ; and Plane Trigonometry, in the extended sense, will be under- stood to include the investigation of all the properties of these so-called circular functions and their application in analytical and geometrical investigations not connected with the solution of triangles. The generation of an angle of any magnitude. 2. The angles considered in Euclidean Geometry are all less than two right angles, but for the purposes of Trigonometry it is necessary to extend the conception of angular magnitude so as to include angles of all magnitudes, positive and negative. Let OA be a fixed straight line, and let a straight line OP, initially coinci- dent with OA, turn round the point in the counter-clockwise direction, then as it turns, it generates the angle AOP; when OP reaches the position OA', it has generated an angle equal to two right angles, and we may suppose it to go on turning in the same H. T. 1 2 THE MEASUREMENT OF ANGULAR MAGNITUDE direction until it is again coincident with OA ; it has then turned through four right angles; we may then suppose OP to go on turning in the same direction, and in fact, to make any number of complete turns round 0; each time it makes a complete revolution it describes four right angles, and if it stop in any position OP, it will, have generated an angle which may be of any absolute magnitude, according to the position of P. We shall make the convention that an angle so described is positive, and that the angle described when OP turns in the opposite or clockwise direction is negative. This convention is of course perfectly arbitrary, we might, if we pleased, have taken the clockwise direction for the positive one. In accordance with our convention then, whenever OP makes a complete counter- clockwise revolution, it has turned through four right angles reckoned positive, and whenever it makes a complete clockwise revolution, it has turned through four right angles taken negatively. As an illustration of the generation of angles of any magnitude, we may consider the angle generated by the large hand of a clock. Each hour, this hand turns through foui- right angles, and preserves no record of the number of turns it has made ; this, however, is done by the small hand, which only turns through one-twelfth of four right angles in the hour, and thus enables us to measure the angle turned through by the large hand in any time less than twelve hours. In order that the a,pgles generated by the large hand may be positive, and that the initial position may agree with that in our figure, we must suppose the hands to revolve in the opposite direction to that in which they actually revolve in a clock, and to coincide at three o'clock instead of at twelve o'clock. THE MEASUREMENT OF ANGULAR MAGNITUDE 3 3. Supposing OP in the figure to be the final position of the turning line, the angle it has described in turning from the position OA to the position OP may be any one of an infinite number of positive and negative angles, according to the number and direction of the complete revolutions the turning line has made, and any two of these angles differ by a positive or negative multiple of four right angles. We shall call all these angles bounded by the two lines OA, OP coterminal angles, and denote them by (OA, OP); the arithmetically smallest of the angles (OA, OP) is the Euclidean angle AOP, and all the others are got by adding positive or negative multiples of four right angles to the algebraical value of this. The numerical measurement of angles. 4. Having now explained what is meant by an angle of any positive or negative magnitude, the next step to be made, as regards the measurement of angles, is to fix upon a system for their numerical measurement. In order to do this, we must decide upon a unit angle, which may be any arbitrarily chosen angle of fixed magnitude ; then all other angles will be measured numerically by the ratios they bear to this unit angle. The natural unit to take would.be the right angle, but as the angles of ordinary size would then be denoted by fractions less than unity, it is more convenient to take a smaller angle as the unit. The one in ordinary use is the degree, which is one ninetieth part of a right angle. In order to avoid having to use fractions of a degree, the degree is subdivided into sixty parts called minutes, and the minute into sixty parts called seconds. Angles smaller than a second are denoted as decimals of a second, the third, which would be the sixtieth part of a second, not being used. An angle of d degrees is denoted by d°, an angle of m minutes by m', and an angle of n seconds by n", thus an angle d° m n" means an angle containing d degrees + m minutes + n seconds, and is equal to qK + qq qq + q q qq gQ of a right angle. This system of numerical measurement of angles is called the sexagesimal system. For example, the angle 23° 14' 56"-4 23 14 56-4. f ■ 1,. 1 denotes 1 1- ^ — ^^~-„^ oi a right anele. aenoieb go ^ 90 . 60 90 . 60 . 60 ^ ^ 1—2 4 THE MEASUREMENT OF ANGULAR MAGNITUDE It has been proposed to use the decimal system of measurement of angles. In this system the right angle is divided into a hundred grades, the grade into a hundred minutes, and the minute into a hundred seconds ; an angle of g grades, m minutes and n seconds is then written g^ ni «". For example, the angle 13^ 97' 4"-2 is equal to 13-97042 of a right angle. This system has however never come into use, principally becavise it would be inconvenient in turning time into grades of longitude, unless the day were divided differently than it is at present. The day might, if the system of grades were adopted, be divided into forty hours instead of twenty-four, and the hour into one hundred minutes, thus involving an alteration in the chronometers; one of our present hours of time corresponds to a difference of 50/3 grades of longitude, which being fractional is inconvenient. It is an interesting fact that the division of four right angles into 360 parts was used by the Babylonians ; there has been a good deal of speculation as to the reason for their choice of this number of subdivisions. The circular measurement of angles. 5. Although, for all purely practical purposes, the sexagesimal system of numerical measurement of angles is universally used, for theoretical purposes it is more convenient to take a different unit angle. In any circle of centre 0, suppose .45 to be an arc whose length is equal to the radius of the circle ; we shall shew that the angle AOB is of constant magnitude independent of the particular circle used; this angle is called the Radian or unit of circular measure, and the magnitude of any other angle is expressed by the ratio which it bears to this unit angle, this ratio being called the circular msasure of the angle. THE MEASUREMENT OF ANGULAR MAGNITUDE 5 6. In order to shew that the Radian is a fixed angle, we shall assume the following two theorems : (a) In the same circle, the lengths of different arcs are to one another in the same ratio as the angles which those arcs subtend at the centre of the circle. (6) The length of the whole circumference of a circle bears to the diameter a ratio which is the same for all circles. The theorem (a) is contained in Euclid, Book vi. Prop. 33, and we shall give a proof of the theorem (b) at the end of the present Chapter. From (a) it follows that arc^.B ZAOB circumference of the circle 4 right angles ' Since the arc AB is equal to the radius of the circle, the first of these ratios is, according to (b), the same in all circles, conse- quently the angle AOB is of constant magnitude independent of the particular circle used. 7. It will be shewn hereafter that the ratio of the circum- ference of a circle to its diameter is an irrational number ; that is, we are unable to give any integers m and n such that m/n is exactly equal to the ratio. We shall, in a later Chapter, give an account of the various methods which have been employed to calculate approximately the value of this ratio, which is usually denoted by tt. At present it is sufficient to say that ir can only be obtained in the form of an infinite non-recurring decimal, and that its value to the first twenty places of decimals is 3-14159265358979323846. For many purposes it will be sufficient to use the approximate value 22 • 355 3-14159. The ratios — = 3-i4285'7, -^5 = 3-1415929... may be used as approxi- mate values of w, since they agree with the correct value of w to two and six places of decimals respectively. 8. We have shewn that the radian is to four right angles in the ratio of the radius to the circumference of a circle ; the 2 radian is therefore - x a right angle ; remembering then that TT a right angle is 90°, and using the approximate value of tt, 3-1415927, we obtain for the approximate value of the radian 6 THE MEASUREMENT OF ANGULAR MAGNITUDE in degrees, 57°-2957796, or reducing the decimal of a degree to minutes and seconds, 57° 17'44"'81. The value of the radian has been calculated by Glaisher to 41 places of decimals of a second i. The value of l/n has been obtained to 140 places of decimals 2. 9. The circular measure of a right angle is ^tt, and that of two right angles is nr ; and we can now find the circular measure of an angle given in degrees, or vice versa ; if d be the number of degrees in an angle of which the circular measure is 6, we have d - = -— ■ , for each of these ratios expresses the ratio of the given IT 180 angle to two right angles ; thus j^ d is the circular measure of 180 an angle of d degrees, and 9 is the number of degrees in an angle whose circular measure is 6; if an angle is given in degrees, minutes, and seconds, as d° m n", its circular measure is (d + m/60 + n/3600) tt/ISO. The circular measure of 1° is -01745329..., of 1' is -0002908882..., and that of 1" is -000004848137 10. The circular measure of the angle AOP, subtended at the arc JLP centre of a circle by the arc AP, is equal to — ^. ;; — ; — ,- . for ■^ radius oi circle ' ^,. . . , ^ arc^P ^.AOP this ratio is equal to ^-^ or TT^n- ^ axe AB zAOB The arc AP may be greater than the whole circumference and may be measured either positively, or negatively, according to the direction in which it is measured from the starting point A, so that the circular measure of an angle of any magnitude is the measure of the arc which subtends the angle, divided by the radius of the circle. The length of an arc of a circle of radius r is rd, where 6 is the circular measure of the angle the arc subtends at the centre of the circle. The whole circumference of the circle is therefore 27rr. ' On the calculation of the value of the theoretical unit angle to a great number of places. Quarterly Journal, Vol. iv. ^ See Grunert's Archiv, Vol. i., 1841. THE MEASUREMENT OF ANGULAR MAGNITUDE 7 The length of a circular arc. 11. It has been assumed above that the length of ar circular arc is a definite conception, and that it is capable of numerical measurement; this matter will be now investigated. The primary notion of length is that of a linear interval, or finite portion of a straight line ; and the notion of the length of an arc of a curve, for example of a circular arc, must be regarded as derivative. That a given finite portion of a straight line has a length which can be represented by a definite rational or irrational number, dependent upon an assumed unit of length, will be here taken for granted. In order to define the length of a circular arc AB, we proceed as follows : Let a number of points of division A^, A^, ... ^,i_i of the arc J. 5 be assigned, and consider the unclosed polygon AA-,Ai...A^-^B\ the sum of the lengths of the sides AA-^ + A-^A^-V ... +^„_i£ of this polygon has a definite numerical value pi. Next let a new polygon AA^Ai ... An'-^B, where n' >n, be inscribed in the arc AB, the greatest side of this polygon being less than the greatest side of AA^A^ ...B; let the sum of the sides of this new unclosed polygon be p^. Proceeding further by successive subdivision of the arc AB, we obtain a sequence of inscribed unclosed polygons of which the lengths are denoted by the numbers p^, p^, ...pn, ■•• of a sequence which may be continued indefinitely. In case the number pn has a definite limit I, independent of the mode of the 8 THE MEASUREMENT OF ANGULAR MAGNITUDE successive sub-divisions of the arc AB, that mode being subject only to the condition that the greatest side of the unclosed polygon corresponding to p„ becomes indefinitely small as n i& indefinitely increased, then the arc AB is said to have the length I. In order to shew that a circular arc has a length, it is necessary to shew that this limit I exists, and this we proceed to do. It is clear from the definition that, if ABG be an arc, then if AB, EG have definite lengths, so also has AG; and that the length of ABG is the sum of the lengths of the arcs AB, BG. It will therefore be sufiicient to shew that an arc which is less than a semicircle has a definite length. In the first place we consider a particular sequence of polygons such that the corners of each polygon are also corners of all the subsequent polygons of the sequence. Denoting by Pj, Pa, ...P„, ... the lengths of these unclosed polygons, it can be shewn that P,
AA^.
Using this and the similar inequalities AiB + Se + ...+tcA > A^A^,
we have by addition, and remembering that yA^, A^S, ... are all
less than e/2r, pn+ e> A A 1 + .^1^2 + . . . + Ar-iB >l — e, there-
fore pn> I— 2e, provided n = n. Next consider a polygon
AAi'AiAg ... B, of the sequence whose lengths are Pj, Pj, ...,
so far advanced that the greatest side is less than the least side
of AoL^y ... kB, and also less than e/2s, where s is the number of
sides in this latter polygon ; as before we see that
Pn ,
thus one of the four given relations is always satisfied.
The solution of equations.
69. Examples.
(1) Solve the equation
sin 26 sec id + cos 26= cos Qd.
This equation may be written
sin 26 sec 4fl+cos 25- cos 65 = 0,
or sin 26 sec 45 + 2 sin 45 sin 25 = ;
hence sin 25=0, or sec 45 + 2 sin 45=0,
that is sin 85 = — 1.
Hence the solutions are*"
6=imn, 5 = j|m7r-(-l)"||.
(2) Solve the equation'-
cos^ asecx + sin^ a cosec x = 1, for x.
We may write the equation
cos' asin ;r+sin5 a cos .r=sin x cos x,
' This example is taken from Wolstenholme's problems.
VARIOUS THEOREMS 83
or sin^ a cos x — cos a sin* a sin ^ = sin x (cos :;; — cos a),
hence sin^ a sin (a - x) = sin x (cos x - cos a),
both sides are divisible by sin ^ (a— a*), rejecting this factor, we have
2sin2acos^(a — «) = 2sina;sin|^(a + ^)=cos^(a' — a)-cos J {3x + a),
therefore cos ^{'Sx + a) = cos ^(x — a) cos 2a,
or 2 cos ^{Zx+a) = cos ^ {x + 3a) + cos ^{x- 5a),
which may be written
cos^ (3.K + a)- cos J (^4-3a)=cos^ («- 5a) -cos -1(3^ + 0),
therefore sin ^{x-a) sin (a; + a) = - sin {x - a) sin ^{x+3a);
again rejecting the factor sin|^(A' — a), we have
sin (^+a) = - 2 cos ^(x-a) sin ^ (ii;+3a) = - {sin (x+a) +sin 2a},
whence sin (^ + a) = —sin a cos a.
The solutions are therefore
x=2n7r + a, and ^ = re7r-a+(-l)''~isin-i (sinacosa).
(3) Solve the equations
a sin (x
a sin (x+y) + b sin (x - y) =2n cos y
We have
a, sin (x+y) - b«m(x-y)=2m cos xl
-2 {asin {x + ^) + bsm {x-y)Y ^ {a sin {x+y) — b sin (x -y)Y
= 4(cos^y - cos* x) = i sin {x+y) sin {x-y).
Let -: — ; ^i = t, then i is eiven by the quadratic equation
sin(:i;-j') •
„ , „,,. ,. , sin(x+v) tan^+tan«'
Usins t for either root of this equation, we have t=—. — -. ^^ =t r — ^,
^ 1 ) sin (^ - y) tan x - tan y
whence t = — r ; also dividing one of the given equations by the other,
tan y t-1
we have = r ; and thence eliminating y by means of these two
ncosy at + b' °^
equations and the relation sec*y — tan*y=l, we have
n^ fat-by „ ft-\y. „ ,
mAatTb) ^^""'-KJ+V **° ^ = ^'
from which we find
^L n-^ fat-by^^ln^ (at-by /i-lVr*
tan .;= ±{l --, (^^ | |-, (^^ - (^j | ,
which gives four values of tan x, two corresponding to each root of the
quadratic which determines t. Thus x is found, and then y is given by
tany=— -TT tan x.
t+ l:
6—2
84 VARIOUS THEOREMS
Eliminations.
70. Examples.
_, . . , , . cos^ 6 dn? 6
IV) Elimmate 6 from the equations ; sm = ~^~7 S2\ -
^ ' ■' ^ cos(a-36) sin(a — 3fl)
,„ , sin 6 cos' 6 + cos 5 sin' 5 sin S cos 6
We nave m = : — -, -;rr^ = -■ — -, aa\ >
sin(a-2fl) sin (a -25)
whence -— =sinacot 2tf — cosa.
2m
cos*fl-sin*fl cos2fl
Also
cos 6 cos (a - Z6) - sin fl sin (a — 35) cos (n - 25)
1
cosa+sina tan25'
hence |;r — |-cosa)( cosal = sin2a,
V2m l\m, j
or 2m2— l=mcosa,
the result of the elimination.
(2) Shew that the result of eliminating 6 from, the equations
cos 3 (6 — a) _COsS(d + a-y) _C0s3a
cos{e-^) ~ cos{e+fi-y) ~ eos^
is independent of ^.
6,y-0, and zero are independent values of a; which satisfy the equation
cos 3 (a; - a) _ cos 3a .
cos (^ - /3) ~ cos /3 ■
We have
cos 3:r cos 3a + sin 3^ sin 3a = /; (cos x cos + sin .r sin ^) ,
where i=cos3a/cos/3 ; substituting for cos3.j;, sin3« their values in terms of
C08.r, sin^ respectively, then dividing throughout by cos'x, we have the
following cubic in tan^ ( = 0i
cos 3a {4 - 3 (1 +t^)} +sin 3a {St (1 + 1^) - 4t^}=i: (cos j3 + « sin j3) (1 + 1^)
or <3(Asin/3 + sin3a)H-<2(^cos/3+3cos3a) + <(/i;sin^-3sin3a)
+ icos^ — cos3a=0
hence tan 6, and tan (y- 5), are the roots of the quadratic
<2(^sin^ + sin3a) + <(icos/3+3cos3a)+/i;sin0-3sin3o=O;
^cos/3+3 cos 3a
therefore tan 5+tan(y-5) =
and tan 5tan(-y — 5) =
A8in/3 + sin3a '
i sin /3 - 3 sin 3a
/;Bin;3+sin 3a '
, , — (/;cosS + 3cos3a) , .
hence tan y = — ^^ . . „ = - cot 3a
' 4 sm 3a
or y-3a=(2r + l)^n-,
VAEIOUS THEOREMS 85
where r is any integer, thus the result of the elimination is independent
of ^.
(3) Eliminate 6 from the equations
S.COS
i + yj^^l^ xsine-ycose={a?nn?6 + b^cos^e)^.
a b
Square each of the equations, and put tan 6=t, the equations become
'■('-S)-'lH-3)-».
J2 (a2 _ a;2) + 2tsn/ + (b^-y^) = 0,
respectively, and we have to eliminate t from them.
Solving for t^ and t, we have
<2 t 1
9.,,^ ^' 6!rl!\ (^^-y^)" {a'-~)^ ^{a:^-ai-^) %xy{W-y') -
^"^^K a^^~ar) ~~¥ '^~~ ah ¥■
Hence
hence — |-%=a+6
OS
is the result of the elimination.
(4) Eliminate 6 from the equations
X sin 6 ■\- J cos ^=2astm 26, -x. cos 6 -y sin 6= & cos 29.
Solving for x and y, we find
x—acoa6{^- cos 26), y = asm6{2 + cos 26)
or a;=a!cos5(cos2 5 + 3sin2 5), y = asin fl (Scos^fl + sin^fl),
therefore a;+y=a(cos d+sin^)^, a'-y=a(cos ^-sinfl)^,
hence {x+yf=a^{\ + sm26), (a--y)^=cs*(l-sin25)
and the result is
{x +y)^ +{x-y)^=^ 2a^.
Relations between roots of equations.
71. Examples.
(1) Consider the equation
a,cos d + hsin6 = c.
Let a, P be distinct values of 6 which satisfy it, then
acosa+6sin a = o,
a cos (i+b sia p=c ;
86 VARIOUS THEOREMS
a h
therefore
sin;3-sina cosa — cos/3 sinO-a)'
hence tan |^ (/3 + a) = 6/a,
and also -cosi(i3-a) = r sin^(i8 + a) = -cos^O + a).
cod
These relations may also be found as follows : put tan ^6=t, then the
• given equation may be written
a{\-fi') + '2,ht = o{\+t^)
or «2(c+a)-26i + c-a=0.
The roots of this quadratic are tan ^a, tan ^j3,
hence tan i a tan hB= — ; — ,
1 . . ,1 , i- cosi(j8-a) c
whence we obtain the relation f .' , — ; = - .
cos-J(/3 + a) a
26
Also tania+tanij3=— — ,
from which the other relation may be obtained.
(2) Gonsider the equation
a, cos'id -Vh sin'iB + c cos 6 + di dn 6 + e=0.
Let t=iax\.^6, then the equation may be written as a biquadratic in t,
«*(a-c + e) + i!3(_46 + 2c?) + <2(_6a!+2e) + <(46 + 2rf) + (a+c+e) = 0;
if tan^^i, tan^fl2) tanj^s, tan 1^4
be the roots of this biquadratic, we have
. ,. 46-2rf ^^ ,., ,. 2e-6a
Stani5T = , 2 tan i 5, tan A ^2= r— i
2 ' a-c+«' ^ ^ ^ ' a-c+e'
Stan Jflitan^fl2tan^53= — , tan|flitanJ52tan J53tan^fl4 = —- ,
and from these relations symmetrical functions of the four tangents may be
calculated.
If 28=61+62+63+8^^6 hsLve
_ 2 tan ^ Sj - 2 tan ^ 61 tan ^ 62 tan ^ 63
~ 1 - 2 tan ^ 61 tan ^6^ + tan ^ 61 tan J ^2 tan J ^3 tan ^ 64
45-2rf+(46+2rf) _6
~a — c + e-{2e — 6a,)+a+c+e a'
We leave it as an.exercise for the student to prove the relations
a b -c —d e
cos* sin« 2cos(« — ^i) 2sin(«-6i) 2 cos J (01 + ^2-^3-^4)'
(3) //
sinacoe{a+6) tan 2a = sin fieos{^ + 6) tan 2^ = sin 7 co« (y + 5) tan 2y
= sin 8 cos (8+ 6) tan 28
VARIOUS THEOREMS 87
and no two of the angles a, /3, y, S differ by a multiple of w, skew that
a + fi+y + S + 6 is a multiple of jr.
Write each of the equal quantities equal to k, then a, ft y, 8 are roots of
the equation
sin sc cos {x + d) tan 2x = k
which may be written
2 tan^ a; (cos 6 -sin 6 tan a;)=k{l- tan* x),
, „ , 2 sin 5 , , „ 2 cos 5 , , „ ,
,nence 2tana= — y- — , 2tanatan/3 = — y — , 2 tanatan;3 tany=0,
and tan a tan 3 tan y tan 8= — 1 ;
therefore tan {a + ^ + y + 8)— -r — „ ^ — r = - tan 6,
IC — Ji cos v — K
hence a+/3 + 7+S + 5 is a multiple of tt.
(4) If a, ^,y be unequal angles each less than 2ir, prove that the equations
cos (a + 6) sec 2a= cos (6+ /3) sec 2^=cos{6 + y) sec 2y
cannot coexist unless
cos (fi+y) + cos {y+a) + cos {a+^)=0.
Writing k for each of the equal quantities, we have
cos a cos 5 — sin a sin 6 — kcoa2a=0,
cos j3 cos 5 — sin |3 sin 5 - ^ cos 2/3 = 0,
cos y cos 6 — sin y sin 6 — k cos 2-y =0,
hence eliminating cos 6, sin 0, we have
2 cos 2o sin (3 - y) =
or 2 cos O +7) 2 sin (y - (3) = 0, by Example (2), Art. 68,
hence 2cos((3 + y) = unless 2sin(y-^)=0,
that is unless sin ;^ - y) sin -^y - a) sin ^ (a - ;8) = 0.
This example may also be solved in a similar manner to Example (3).
Maxima and minima. Inequalities.
72. Examples.
(1) The greatest value of
a, cos 6 +\) sin 6 is Va^'+b^.
Put b/a = tan a, then b=\/a^+b^ ain a, a= \/a? + h^ cos a,
thus a COS 6 + b sin 6 = \/a^-'rb^ cos {6 -a),
now cos {6 - a) always lies between + 1, hence a cos 6 + b sin 6 lies between
(2) If\i.= Va^ cos^ fl + b^ siii^ 6 + fJ&'tin^B+h^cos^e, then u lies between
a + b and \/2 (a^ + b^).
88 VARIOUS THEOREMS
Let x^a^ cos2 e + ¥a\n^ e=-\{a^-^h^) + k{a^-h^)ooa'ie,
then u=n/x + 'i/a^ + l>'-x.
m2 = a2 + 6H 2 Vi {a' + 6'')2 - {^ (a^ + 6^) - 4^
hence u is greatest when a; = ^ (a^ + 6^), or the greatest value of u is V2(a^+6^) ;
also u is least whei^ ^{a^+b^)-xia greatest, that is when x is least, which will
be when cos 2d = -1, in which case x=b% and then w=a + b; this therefore is
the least value of u.
(3) Shew that if 6 lies between and n, cot ^0 — cot 6>2.
We have
.1/, x/, sinfd 3-4sin2je l +2cos^g
COt^d — C0tg= . ,*. . = : 3-*— = -j— a ,
* sinjflsinfl sin 5 sin 5
hence cot Jd — cot5 = cosec fl+coseo^fl;
now cosec 6, cosec^d are each never less than unity, if 6 lies between and tt,
hence cot ^6- cot 6>2.
(4) If the sum of n angles, each positive and less than Jtt, is given, sheio
that the sum or the product of the sines of the angles is greatest when the angles
are all equal.
A similar theorem holds for the cosines.
Let a^, 02 ... an be the angles and s be their sum. Then we have
sin a,.+sin aj=2 sin \ (a^ + ag) cos ^ {0^.-0,),
now cos \ (a,. - oj) is less than unity unless 0^=08, hence
sin a,.+sin a,<2 sin ^(ay + as)
unless ar=ag. If any two of the angles ai, 03... a, are unequal, we can
therefore increase S sin a by replacing each of those two angles by their
arithmetical mean, hence Ssina is greatest when all the angles are equal;
we have therefore 2 sin a:f«7i sin «/w.
Again sin a,, sin og = ^ {cos (a,. — a,) - cos (0^ + a,)},
and this is less than ^ (1 —cos ((v+a,)} or sin^^- (oy + Og)
unless ar=ag. Hence as before, if any two angles in the product sinai,
sina2...sina„ are unequal, we can make the product greater by replacing each
of those two angles by the arithmetic mean of the two ; it follows that
sinoi, sin 03... sin a„ is greatest when ai = a2 = ...=a„, or the greatest value of
the product is (sin s/»i)".
(5) Under the same condition as in the last example, shew that the sum of
the cosecants of the angles is least when tlie angles are all equal.
We have
cosec Or + cosec Og
-sin$(,ar °«^|c(,s|(^_o^)_cos^(a,.+a,) COS J (a^ - Og) + cos ^ (a,. + a,)]'
hence for a given value of 0^+0,, cosec a, + cosec a, has its least value when
VARIOUS THEOREMS 89
cos ^ (a, - a,)= 1, or when ar=a,. The reasoning is now similar to that in the
last example.
(6) Under the same conditions as in, the last two examples, shew that the
sum of the tangents or of the cotangents of the angles is least when the angles
are all equal.
(7) Shew that if a + /3 + 7 = jt, co« a co« /3 cos y :^ 1/8.
Porismatic systems of equations.
73. A system of equations is said to be porismatic '■ when the
equations are inconsistent unless the coefficients satisfy a certain
relation; when this relation is satisfied the equations have an
infinite number of solutions.
The system
acos0cosy + 6sin/3sin'y + c + a'(sin3+siny)+6'(cos/3 + cosy)+c'sin(|3 + -y) = O,
acosy cosa+6sinysina + c + a' (sin ■y+sina) + 6' (cosy +cosa) + c' sin (y + a) = 0,
acosacos/3 + 6sinasin|3 + c + a'(sina+sin^) + 6'(cosa + cos/3) + c'sin(a+|3) = 0,
is a system of three porismatic equations.
Consider the equation
«cosacos5 + 6sinasin5 + c+fl!'(sin5 + sina)4-6'(cos0 + cosa) + c'sin(5 + a) = O,
this is satisfied by 6=^, and by 6=y. Write this as an equation in
t&n^6 = t, thus :
i^ ( — a cos a + c+ a'sin a + 6' cos a - b' -c' sin a)+2t (b sin a + a'+c' cos a)
+ (a cos a + e + a' sin a + 6' + 6' cos a+c' sin a) = 0.
From this equation we find
tan 1^/3+ tan ^y, and tan ^0 tan J y,
u X wo . \ 2 (6 sin a + a' + c' cos a)
hence tan*(/3+y)=7r7 r, r-- ^■
2\MT n 2(acosa + 6' + c'sma)
We should find similarly
, , , 6sinS+a' + c' cos/3
tani(a + y)= ^— r; J-^>
-^ " acosj3+o +c sm0
we can now deduce the value of tan^(a— j3) ; we find for the numerator the
value
(6sin/3 + a' + c'cos/3) (a cos a + 6' + c' sin a) - (6 sin a + as' +c' cos a)
(as cos ;3 + 6' + c' sin ^)
or
2 sin |(a - ^) {(c'2 - ab) cos J (a - ^) + (os'c' - bb') cos ^ (a + ^)
-(aa'-6'c')sin^(a+^)},
' See Proc. London Math. Soc. Vol. iv. " On systems of Porismatic equations "
by Wolstenholme.
90 VARIOUS THEOREMS
and for the denominator,
(6 sin a + a' + c' cos a) (6 sin /3 + a' + c' cos ;8) + (a cos a + 6' + c' sin a)
or
(a cos /3 + 6' + c' sin j3)
(a2+c'2) cos acosj3 + (62 + c'2) sin asin/3+(a'2+6'^) + (a'& + 6'c')(sina+siu/3)
+ (aV + ah') (cos a + cos j3) + (a + 6) c' sin (a + 13) ;
dividing this fraction by sin \ (a - j3), we have this denominator equal to
(c'2 - o6) {1 + cos (a - /3)} + (aV - 66') (cos a + cos /3) — (aa' — h'cf) (sin a + sin j3),
hence
(a + 6){acosacos/3 + 6sinasin^+c+a'(sina+sin j3) + 6'(cosa + cos/3)
+ c'sin(a+^)}
is equal to c'2 - a'2 - 5'^ + oa + c6 - a6.
Hence unless the condition
c'2_a'2-6'2 + ca + c6-a6 =
is satisfied, the system of equations cannot be satisfied except by equal values
of a, j3, y. When this condition is satisfied, any one equation can be deduced
from the other two.
The swmmation of series.
74. A large number of series involving circular functions can
be summed by the method of differences. The most important
example of the use of this method is the case of a series of sines
or cosines of numbers in Arithmetical Progression.
Let the series be
//■ + 6 cos i/f) »in (0 - ^)
+(a sin i/^ + 6 cos i/r) (a sin d+ 6 cos 6) sin {-^—6)
+ (a sin ^ + 6 cos 6) {a sin <^+ 6 cos <^) sin {6 - (f>)
+ (a2 + 62) sin (0 - V') sin (i/. - 5) sin (e - 0) = ;
and interpret the equation geometrically.
4. Reduce to its simplest form, and solve the equation
cos2 e ^ cos^ a = 2 cos3 fl (cos 5 - cos a) - 2 sin' 6 (sin 6 - hin a).
5. Prove that the sum of three acute angles A, B,C, which satisfy the
relation aos^ A + coa^ B + cos^ C=\, is less than 180°.
6. If ^ +5+0=90°, shew that the least value of tanM +tan2 5 + tan2 C
is unity.
7. Find 6, from the equations
sin 5 + sin (^+sina = cos 5 + cos0 + cosa1
e + = 2a j'
8. If ^+5+C=180°, shewthat8sin^4sin^JBsinJC:t*l•
^. xain ^+y8in0+«sin\/c_4sin flsin ^ A.'^D'T'
We have p'T'_qt) ="qp' = ^' ^lence PL={R-a)coaA + -sPL,
with similar expressions for PM, PN; now
'ihLMN=PM. PNainA+PN. PLainB+PL. PMamC
={R-d)^SamAcoaBcosC+^^sP'M' . P'N'ainA
+^(R-d)2P'L'aiaA;
also ^SP'M' . P'N' sin A is the area of the triangle L'M'N', which is zero, and
^P'L'smA=^^a.P'L'=\^hP'BC=\hABC,
and 2 sin 4 cos 5 cos (7= sin 4 sin 5 sin 0;
hence 2 A LMN= {R - d)^ sin A sin £ sin C+ 2rf {R - d) sin A sin 5 sin C
= {R^ - dF) sin A sin 5 sin C.
(3) //^ A, B, C 6e any three fixed points, and P osmy point on a circle whom
centre is 0, shew that AP^. ABOO+BP^. ACOA+CP^. A AOB is constant
for all positions of P on the circle.
Denote the angles BOC, GOA, AOB by a, ft y, then a+0+y=27r, and let
the angle POA be 5. We have AP'^=OP^+OA^-WA.OPooa6,a,TA similar
expressions for BP^, CP^, hence the expression above is equal to
OP^ . i^ABC+sOA^ . hBOC-'iOPs.OA . hBOG .coae ;
PROPERTIES OF TRIANGLES AND QUADRILATERALS 211
the first two terms in this expression are independent of the position of P on
the circle, and the coef&cient of %0P in the last term is
\0A. OB. OC{oosflsina+cos(5-|-y)sin/3 + co8(/3-5)sin'y}
or ^OA. OB. (9Ccos5(sina+sin(3coS')/ + cos/3siny)
which is zero ; thus the theorem is proved.
Particular cases of this theorem are the following :
(a) P^2sin24+P£2sin2£+PC2sin2C is constant if P lies on the
circum-circle ;
(6) PA^ wa. A +PB^ sin B-k-PC^ SCO. C is constant if P lies on the
in-circle.
(c) PA^ sin A cos {B-G)-\- PB^ sin Bcos(C-A) + PC^ sin C cos (A - B)
is constant if P lies on the nine-point circle.
(4) Shew that the length of the side of the least equilateral triangle that
can he drawn with its angvlar 'points on the sides of a given triangle ABC is
2aV2
VaHb2+c2-|-4'\/3A
where A is the area of ABC.
Let DEF be such an equilateral triangle, and let the circle round DEF
cut BC and AG in H and O respectively ; the angles FOA, FEB are each 60°
thus FO, FH are in fixed directions ; also the angle HFG is 120° - C.
We have, if AF be denoted by x,
FG =xsm Ajsin 60°, FH={c- x) sin Bjsin 60°,
hence
^6*2= cosec2 60° {x^ sin^ A + {c- xf sin^ B-'2,x{c-x) sin .4 sin 5 cos (120° - C^}.
Now the radius of the circle is HOj^ sin (120° — C), hence the circle is least
when HO is least. The least value of a quadratic expression 'Kai^+'ifM + v,
14—2
212 PROPEETIES OF TKIANGLES AND QUADRILATERALS
in which X is positive, is i/-^, for Xx^ + Sux+v may be written in the form
A
X (^ + ^ j + ./ - ^ . We find therefore for the least value of HG am 60°,
fj • a„ (csin'^ + c3in^sin^cosl20°-C)' ) i
(" ^'° ain^A + sin^ £ + 2 sin 4 sin B cos (120° - C)J '
which is equal to
c sin J. sin 5 sin (1 20° — G)
{sin2 A + sin2 B+2amA sin 5 cos (1 20° - C)}4 '
\/2 b" sin A sin B sin (120° - G)
sinC'Va2+62 + c2+4\/3A
Now the side of the equilateral triangle is ^(Tsin607sin(120°- C), thus
the least value of the side is
2A^2
Va2+6Hc2+4V3A'
(5) Describe three circles mutually in contact, each of which touches two
sides of a given triangle.
Let pi, p2, p3 be the radii of the circles, then MN=2'\/p2P3,
hence a=BM+G^+MN=piCot^B+psCot^G+2 ^/pips,
with similar equations for b and c.
Let ^=piCot^4, y^=p2Cot^B, z^=p3Cot^G,
Vtan^5tauiJ(7= -cosa, Vtan^CtanJ^ = -cosjS, \/tan^yltan^5=— cosy;
we find sin2a = l-tan^5tan JC=a/«, and similarly ain^ p=b/s, ain^y =cjs,
hence we have the equations
y^+z^- %yz cos a _^-\-a?' — %zx cos |3 _ a:^ +y* — 2a^ cos y _
sin^a sin^^ "" sin^y ~ '
PROPERTIES OF TRIANGLES AND QUADRILATERALS 213
these have been considered in Art. 68, Ex. (12) ; adopting the first solution
there found, we have
x=\/s ooa((r-a), y = \/s cos(o--/3), «=V« cos ((r-y),
where 2o-=a + 0+7,
hence
pi=stan J4cos^((r — a), p2 = «tan^5oos^(o--/3), ps=sta,ii^Ocoa^(a--y)
are the required radii of the circles. The other solutions give the radii of
three sets of circles which are such that two in each set touch two sides
of the triangle produced ; of one such set, the radii are
stan^^cos^*, stan^5cos^(s-y), stan^Ccos^(«— /3).
There are altogether eight sets of circles which satisfy the conditions of
the problem.
This solution is founded on that of Lechmiitz given in the Nouvelles
Annales, Vol. v. A geometrical solution of this problem, which is known as
" Malfatti's Problem," will be found in Casey's Sequel to Euclid. A history of
the problem will be found in the Bulletin de I'Academie Royale de Belgique
for 1874, by M. Simons.
EXAMPLES ON CHAPTER XII.
1. If 6 be the angle between the diagonals of a parallelogram whose sides
a, h are inclined at an angle a to each other, shew that tan 5 = — = — 5^—.
' a^ — h^
2. If a, /3, y be the distances, from the angular points of a triangle, to
the points of contact of the inscribed circle with the sides, shew that
3. The area of a regular inscribed polygon is to that of the circumscribed
polygon, of the same number of sides, as 3 : 4 ; find the number of sides.
4. From each angle of a parallelogram a line is drawn making the same
angle, towards the same parts, with an adjacent side, taken always in the
same order ; shew that these lines will form another parallelogram similar to
the original one, \i a^~V'=%ahcoaB, where a, h are the sides, and B is an
angle of the parallelogram.
5. The straight lines which bisect the angles 4, (7 of a triangle meet the
circumference of the circum-circle in the points a, y ; shew that the straight
line ay is divided by CB, BA into three parts which are in the ratio
Biv?\A : 2 sin ^-4 sin 1^5 sin ^C: sin^^C.
214 EXAMPLES. CHAPTER XII
6. If / be the centre of tte in-circle of a triangle, la, lb, Ic perpendiculars
on the sides, pi, p2, ps the radii of circles inscribed in the quadrilaterals
Able, Be la, Calb, prove that
Pi . Pi . P3 ^ a+h + c
r-pi r-p2 r-p3 2r
7. Prove that the line joining the centres of the circum-eircle and the
. , . . , , ■., T.^ , . ,/ sinjB~sinC \
m-cu:cle of a triangle makes with BC an angle cot~i =- 7= — 7 .
° ^ \cos B + coaC-lJ
8. If, in a triangle, the feet of the perpendiculars from two angles, on the
opposite sides, be equally distant from the middle points of those sides, shew
that the other angle is 60°, or 120°, or else the triangle is isosceles.
9. If ABC be a triangle having a right-angle at C, and AS, BB drawn
perpendicularly to AB meet BG, AC produced in B, D respectively, prove
that tanC^Z>=tan3£.4(7, and hEGD=hACB.
10. If a point be taken within an equilateral triangle, such that its
distances from the angular points are proportional to the sides a, b, c of
another triangle, shew that the angles between these distances wiU be
in + A, in + B, in + O.
11. The points of contact of each of the fovu: circles touching the three
sides of a triangle are joined; prove that, if the area of the triangle thus
formed from the inscribed circle be subtracted from the sum of the areas of
those formed from the escribed circles, the remainder will be double of the
area of the original triangle.
12. If ABCD is a parallelogram and P is any point within it, prove that
A APG . cot APG- A BPD . cot BPD is independent of the position of P.
13. Three circles touching each other externally are all touched by a
fourth circle including them all.' If a, b, c be the radii of the three internal
circles, and a, ft y the distances of their centres from that of the external
circle respectively, prove that
\bc ea ah) a^ b^ c^
14. P, Q, R are points in the sides BC, CA, AB of a triangle, such that
:?.^ = ^ = 41 ; shew that AP^+BQ^+CR^ is least, when P, Q, R bisect the
PC (^A BK
sides.
15. On the sides a, 6, c of a triangle are described segments of circles
external to the triangle, containing angles a, ft y respectively, where
a+j3+y = 5r, and a triangle is formed by joining the centres of these circles;
shew that the angles of this triangle are a, ft y.
EXAMPLES. CHAPTER XII 215
16. Through the middle points of the sides of a triangle, straight lines
are drawn perpendicular to the bisectors of the opposite angles, and form
another triangle ; prove that its area is a quarter of the rectangle contained
by the perimeter of the former triangle and the radius of the circle described
about it.
17. P is a point in the plane of a triangle ABG, and L, M, N are the feet
of the perpendiculars from P on the sides ; prove that if MN+NL+LM be
constant and equal to I, the least value of
PA'^ + PB^ + PC^ is- ?V(sinM + sin2 5+sin2C').
18. Lines B'C, C'A', A'B' are drawn parallel to the sides BO, CA, AB
of a triangle, at distances ri, r^, r^ respectively; find the area of the triangle
A'B'C.
If eight triangles be so formed, the mean of their perimeters is equal to the
perimeter of the triangle ABC, but the mean of their areas exceeds its area by
(aVi2 + 6V22 + cV32)/4A.
19. On the sides of a scalene triangle ABG, as bases, similar isosceles
triangles are described, either all externally or all internally, and their vertices
are joined so as to form a new triangle A'B'C ; prove that if A'B'C be equi-
lateral, the angles at the base of the isosceles triangles are each 30° ; and that
if the triangle A'B'C be similar to ABC, the angles are each
, _, 4A
*™ a^ + V + o''
where A is the area of ABC.
20. A straight line cuts three concentric circles va A, B, C, and passes at
a distance p from their centre ; shew that the area of the triangle formed by
. . „ ^. BC.CA.AB
the tangents ax, A, B, U is .
21. If N is the centre of the nine-point circle of a triangle ABC, and
D, E, F are the middle points of the sides, prove that
BG oos. NDC+CA cos NEA+AB cos NFB=Q.
22. On the side BA of a triangle is measured BD equal io AC ; JSCand
AD are bisected in E and F ; E and F are joined ; shew that the radius of
the circle round BEF is ^BCcoseo\A.
23. If A', B', C be any points on the sides of the triangle ABC, prove
that AB'.BC .CA'-\-B'C. C'A . A'B=^4.R.AA'B'C'.
24. If X, y, 2 denote the distances of the centre of the in-circle of a
triangle from the angular points, shew that
a4^+64y4+c*z*-f.(a-l-6-fe)2ii;2y222=2(62cy22-(-c2a232ii;2-l-a262a;y).
25. D, E, F are the points where the bisectors of the angles of the
triangle ABC meet the opposite sides ; if oo, y, z are the perpendiculars
216 EXAMPLES. CHAPTER XII
drawn from A, B, C, respectively, to the opposite sides of DEF, pi, P2, Ps
those drawn from A, B, C, respectively, to the opposite sides of ABC, prove
that „ 2 », 2 « 2
^+^+%=ll + 8sini4sini5sinift
26. Shew that the distances of the orthocentre of a triangle from the
angular points are the roots of the equation
x3-2{R+r)a;^ + {r^-4:W+s^)x;-2R{s^-{r+2Rf}=0.
27. If each side of a triangle bears to the perimeter a ratio less than
2 : 5, a triangle can be formed, having its sides equal to the radii of the
escribed circles.
28. ABC is a triangle inscribed in a circle, and from 2), the middle point
of BC, a line is drawn at right angles to BG, meeting the circumference in £!
and F; AE, AF are joined. If triangles be described in the same way by
bisecting AB, AC, shew that the areas of the three triangles thus formed are
as sm{B-C):sm{C-A):sin{A-B).
29. Three circles, whose radii are a, b, 0, touch each other externally ;
prove that the radii of the two circles which can be drawn to touch the three
are abc
(bc+ca+ab) + 2'i/abc(a + b + c)
30. ABC is a triangle; on its sides equilateral triangles A'BC, EC A,
CAB are described without the triangle; prove that (1) AA', BB', CC meet
in a point 0, (2) OA'=--OB+OC,
(3) hA'B'C'=ihABC+'^{BC^+CA^-¥AB^).
a
31. A', B' are the middle points of the sides a, 6 of a triangle ; D, E are
the feet of the perpendiculars from A, B oia the opposite sides ; A'D, B'E are
bisected \nP,Q; prove that PQ=^\/a^+l^-2aboosZC.
32. The perpendiculars from the angular points of an acute-angled
triangle meet in P, and PA, PB, PC are taken for sides of a new triangle.
Find the condition that this is possible, and if it is, and a, /3, y are the angles
of the new triangle, prove that
cos a cos^ cosy 1 > D ^
1 -I 7 H a H 7V=? sec A sec^sec G.
cos A cos B cos C
33. Two points A, B are taken within a circle of radius r, whose centre
is C. Prove that the diameters of the circles which can be drawn through
A and B to touch the given circle are the roots of the equation
a;2 (rV - ffl2 52 aiii2 c) _ 2^c2 (?-2 - a6 cos C) + c2 (r* - 2r2 a6 cos C+ a2 62) = 0,
where the symbols refer to the parts of the triangle ABC.
EXAMPLES. CHAPTER XII 217
34. If a triangle be cut out in paper, and doubled over so that the crease
passes through the centre of the circumscribed circle and one of the angles J,
shew that the area of the doubled portion is
ib^am^OcoaOcosec(2C-B)aeo{C-B), where C>B.
35. From the feet of the perpendiculars from the angular points A, B, G
of a triangle, on the opposite sides, perpendiculars are drawn to the adjacent
sides; shew that the feet of these six perpendiculars lie on a circle whose
R (cos2 A cos2 B cos2 C+sin^ A sin^ B sin^ C)*.
36. Prove that if P be a point from which tangents to the three escribed
circles of the triangle ABC are equal, the distance of P from the side BC
will be
^{b+c) Bec^Asin^B sin^C.
37. If X, y, z be the sides of the squares inscribed in the triangle ABC,
on the sides BC, CA, AB, shew that -H \-- = - -\---\ (--.
X y z a r
38. AA', BB', CC are the perpendiculars from A, B, G on the opposite
sides of the triangle ABC ; Oj, 0^, O3 are the orthocentres of the triangles
AB'C, BG'A', CA'B'. Prove (1) that the triangles O1O2O3, A'B'G' are
equal, and (2) that '2,riB^=BaRhRc, where R^, Rt, Re are the radii of the
circles OiA'Oz, OsB'Oi, OiC'O^, and rj is the radius of the circle inscribed in
A'B'C, and ^1 of the circle about A'B'C.
39. If X, y, z are the distances of the centres of the escribed circles of a
triangle, from the centre of the in-circle, and d is the diameter of the ciroum-
circle, shew that
xyz + c? (a;2 +3/^ + ^) = 4(^'.
40. The lines joining the centre of the in-circle of a triangle, to the
angular points, meet that circle in A^, B^, C^; prove that the area of the
triangle A^B^G^ is ^r'^{cos^A+coa^B+coa^C).
41. If each side of a triangle be increased by the same small quantity x,
shew that the area is increased by Rx (cos J + cos 5+ cos C), nearly.
42. AA', BB', CC are diameters of a circle, D, E, F are the feet of the
perpendiculars from A', B', G' on BC, GA, AB respectively; prove that AD,
BE, €F meet in a point, and that the areas ABC, DEF are in the ratio
1 : 2 cos A cos B cos G.
43. If ID, IE, IF are drawn from the in-centre / of a triangle, perpen-
dicular to the sides, find the radii of the circles inscribed in lEAF, IFBD,
IDGE; if they are denoted by pi, p^, pg respectively, shew that
(»--2pi) (r-2/j2) (r-2p3)=r3-4pip2P3-
218 EXAMPLES. CHAPTER XII
44. Shew that the radii of the circle which touches externally each of
three given circles, of radii a, b, c which touch each other externally, is
given by
^/Rbc{b + c+R) + \/Eoa{c+a+£) + ^Iiab{a+b+E) = \/abc(a + b + c).
45. Perpendiculars AA^, BB^, CG^ to the plane of a triangle ABC are
erected at its angular points, and their respective lengths are a,b, c ; shew
that if A and Aj be the areas of ABC and A-^B^G^, then
i^^^-A^ = i{a^{x-y){x-z) + b^{y-z)(il-3(;) + c^{z-x){z-y)}
=l{ai^{x-y){x-z) + bi^i7/-z){y-x) + Ci^{z-x){z-y)}.
46. Three circles are described, each touching two sides of a triangle, and
also the inscribed circle. Shew that the area of the triangle having their
centres for angular points bears to the area of the given triangle the ratio
4 sin \A sin \B sin \ C (sin \A-^ sin ^^+sin ^C)
: cos^4cos^5cos^C(co8^4+cos^5+cos^C).
47. If the lines bisecting the angles of a triangle meet the opposite sides
in D, E, F, prove that the area of the triangle DEP is
2r2 cos ^A cos ^5 cos ^C/cos i (5 - C) cos \{C-A) cos ^{A- B),
and that
{a+bf{a + cfEF^ + {b + cf(b + afFD^ + {c-\-af{c-irbfDE^ = \QA^R{\\R+^r),
where A is the area of ABG.
48. is the centre of the circum-circle of a triangle, K is the ortho-
centre, and OK meets the circle in P and P', and the pedal lines of P and P'
in § and §' ; prove that OQ . OQ; ='i.R^ coa A cos B cos G.
49. N is the centre of the nine-point circle of a triangle ; B, E are the
middle points of CB and CA ; prove that the area of the quadrilateral NDGE
is J/)^(sin24 -|- sin 25 -1-2 sin 2 C), where p is the radius of the nine-poinb circle.
50. A triangle is formed by joining the centres of the escribed circles, a
third from this, and so on ; shew that the sides of the nth triangle are
A TT-A 3rr+A (2^-^-l)w + (-l)''-^A
a cosec -^ cosec ^ cosec — ^ — cosec ^^ _^ ,
and similar expressions.
51. If iV is the centre of the nine-point circle of ABG, and AN meets BC
in D, shew that
BN-.BA ::cos(5-C):4sin5sinC,
and that the area of BNC is \R^sia.A cos {B—G).
52. Shew that the radius of the circle which touches the three circles
BGE, EAF, FBB, where B, E, F are the feet of the perpendiculars from
A, B, G on the opposite sides, is
2iJ sin .4 sin 5 sin Ccos^^ cos 5 cos (7 (sin ^-)- sin 5 -t- sin C)
s\v? A sin^ B sin^ C- 2 sin''' A cos^ A + i cos A cos B cos CS sin BsmG'
EXAMPLES. CHAPTER XII 219
53. If from any point 0, perpendiculars OD, OE, OF are drawn to the
sides BO, GA, AB of a triangle, prove that coiADO+cotBEA + coiOPB=0.
54. If h, c, B are given, and there. are two triangles with these given
parts, shew that their inscribed circles touch, if
c2 (cos2 5 + 2 cos fi- 3) + 25c (1 -cos B) + h^=Q.
55. If , E, F are drawn straight lines B'G', C'A', A' El, equally inclined to
BC, GA, AB respectively, so as to form a triangle A'B'G' similar to ABC.
Prove that the radius of the circumscribed circle of A'B'G' is
{EF cos a + FD cos /3 + DE cos ■y)/4 si n .4 sin ^ sin C,
where a, ft y are the inclinations of AA', BB', CG' to BC, GA, AB re-
spectively.
66. If P be a point on the circum-circle whose pedal line passes through
the centroid, and if the line joining P to the orthocentre cuts the pedal line
at right angles, prove that
PA^+PB^+PG^ = 4:R^ {1-2 COS A COS B cos C).
67. D is a, point in the side BG of a triangle ; if the circles inscribed in
the triangles ABD, ACD touch AD in the same point, prove that D is the
point of contact of the in-circle of ABC with BG ; but if the radii of the
circles be equal, then
CD : BD : : coseo D + cosec C : coseo D + cosec B.
68. From a point within a circle of radius r, three radii vectores of
lengths Ti, r^, r^ are drawn to the circle, and the angle contained by any
pair is Stt/S ; shew that
3»-2(r2r3+r3ri + ?-ir2)2=()-22+»-2'-3-t-»-3^)W+»-3n+»-i'')(»-i''+»-i»-2+»-2*),
and that the distance of the point from which the radii are drawn, from the
centre of the circle, is d, where
(r2-cP)(j-2r3-|-r3ri+r,r2)=rir2r3(ri-(-j-2+r3).
69. Circles are inscribed in the triangles DiEyF-i, D^E^Fi, DsE^Fg,
where D^, Ei, Fi are the points of contact of the circle escribed to the side
BG; shew that if pi, p2, ps be the radii of these circles
-:-:- = l-tanJ^:l-tan^5:l-tanJC.
Pi Pi Pi
EXAMPLES. CHAPTER XII 221
70. In a triangle ABC, A', B', C are the centres of the circles described
each touching two sides and the inscribed circle ; shew that the area of the
triangle A'B'C is
tan ^(jr-A) tan ^{m — B) tan \{n-C)
{cosec J(7r — 4)cosec J {n- B) cosec J (ir-C)+4}f2.
71. The three tangents to the in-circle of a triangle which are parallel to
the sides are drawn ; shew that the radii of the circles inscribed in the three
triangles so cut off from the corners are given by the equation
42^_„2^2_j^2(„2 + 52^.c2_26e_2ca-2a6)^-r6=0.
72. The perpendiculars from the angular points of a triangle on the
straight line joining the orthocentre and the centre of the in-circle are p, g,r;
prove that psin^ _ gsin.B ^ rsinC
sec 5 — sec C sec C— sec 4 seo A — aeoB'
a convention being made as to the signs of ^, q, r.
73. A point is taken within an equilateral triangle, and its distances
from the angular points are u, j3, y. The internal bisectors of the angles
between (ft y), (y, a), (a, fi) meet the corresponding sides of the triangle in
P, Q, B respectively ; shew that the area of PQR is to that of the equilateral
triangle in the ratio
2a^y:(/3+y)(y + a)(a+0).
74. If I, m, n are the distances of any point in the plane of a triangle
ABC, from its angular points, and d the distance from the circum-centre,
prove that
l^ sin 24 +»i2 sin 'i.B + 'n? sin %C=i{R^-ir =Q.
76. Each of three circles, within the area of a triangle, touches the other
two, touching also two sides of the triangle ; if a be the distance between the
points of contact of one of the sides, and ft y be like distances on the other
two sides, prove that the area of the triangle of which the centres of the
circles are angular points is ^{^^y^+y^a^ + a^^^Y .
77. If a, b, c, d be the perpendiculars from the angles of a quadrilateral
upon the diagonals c^i, d^, shew that the sine of the angle between the
, , { {a+c){h+d)\ h
diagonals is equal to V" J^ j ■
222 EXAMPLES. CHAPTER XII
78. If A BOD be a quadrilateral, prove, in any manner, that the line
joining the intersection of the bisectors of the angles A and C with the
intersection of the angles B and D makes with AD an angle equal to
_j ( • sin.4-sini) + sin(^+.B) 1
(,l+cos^+cos/)+cos(J+5)J ■
79. ABODE is a plane pentagon; having given that the areas of the
triangles EAB, ABC, BOD, ODE, DEA are equal to a, h, c, d, e respectively,
shew that the area A of the polygon may be found from the equation
A^-{a + b + c + d+e)A+{ab + bc+cd+de + ea)=0.
80. Shew that if a quadrilateral whose sides, taken in order, are a, b, c, d
be such that a circle can be inscribed in it, the circle is the greatest when the
quadrilateral can be inscribed- in a circle, and that then the square on the
radius of the inscribed circle is -. , ,. , ,, .
(a+c)(6+d)
81. A polygon of 'in sides, n of which are equal to a, and n to b, is
inscribed in a circle ; shew that the radius of the circle is
w
^ + 2a6 COS — + 6^ I cosec — .
n J n
82. A quadrilateral whose sides are a, b, c, d can be inscribed in a circle ;
its external angles are bisected ; prove that the diagonals of the quadrilateral
formed by these bisecting lines are at right angles, and that the area of this
, ., , , . 1 s^{ab + cd){ad+bc)
quadrilateral is ^ — ,
^ 2 (a + c) (fi+d) Kj{s-a) (s-b) («-c) (s-d)
where 2s=a+b+c+d.
83. A quadrilateral ABOD is inscribed in a circle, and EF is its third
diagonal, which is opposite to the vertex A ; prove that if the perpendiculars
from A on BO, OD meet the circles described on AD, AB respectively as
diameters, in F, then FQ sin D = EFiaiii' A- siv?D).
84. The power of two circles with regard to one another, is defined to be
the excess of the square of the distance between their centres, over the sum
of the squares of the radii. Prove that for a triangle ABO, the power of the
inscribed circle, and that escribed circle which is opposite A, is ^{«^ + (6 — c)^},
and hence verify that if the escribed circle touches an escribed circle, the
triangle must be isosceles.
85. The sides, taken in order, of a pentagon circumscribed to a circle
are a, b, c, d, e; prove that its area is a root of the equation
x*-x^s{i2a'(b+e-c-d)-iSa'+i2acd}
+ {s-a — e)(s-b-d){s-c — e){s-d-a) (s — c-b)s^=0,
where 2« is the sum of the sides.
EXAMPLES. CHAPTER XII 223
86. If a, b, c, d be the distances of any point on the circumference of a
circle of radius r, from four consecutive angular points of an inscribed regular
polygon, find the relation between a, b, c, and d, and prove that
2_ {ab — cd){bc — a(r){ca — bd)
~{a+b-c-d){b + c-a — d){c+a-b-d){a-\-b + c+d)'
87. The perimeter and area of a convex pentagon ABODE, inscribed in a
circle, are 2s and S, and the sum of the angles at ^and B, at A and G,
are denoted by a, ^, ; shew that
«2(sin2a+ + 8in2e) + 2/S'(sina+ +sine)2=0.
88. ABCD is a convex quadrilateral of which the sides touch one circle,
while the vertices lie on another; tangents are drawn to the circumscribed
circle at A, B, C, D so as to form another convex quadrilateral ; prove that
the area of the latter is
{s(r — 2abcd) (abed)^ a-
{a- - bed) (o- — add) (o- - dab) (or - abc) '
where r is the radius of the circle ABCD, 2s=a+6 + c+ci, and
'^ )= — z — ^ ^- — - — .
p^ ^ , ^' 1 — 2r cos p -t- r^
If the modulus of z is greater than unity, the series is divergent ;
1 See Stokes' Collected Works, Vol. i.
2 On the history of this discovery see Eeiff's Gesehichte der unendlichen
Seihen.
H. T. 17
258 THE THEORY OF INFINITE SERIES
and if mod. z is unity it is also not convergent, since the sums of
the two series 2 cos nQ, S sin nQ, which have been found in Art. 74,
do not approach a definite value when n is indefinitely great.
We have, by equating the real and imaginary parts of the
series and the sum,
\—r cos 6
1 -2r cos ^H-r^
= 1 + r* cos ^ + r^ cos 2^ + . . . + r" cos n^ + ,
= r sin + r^ sin 2^ + . . . + r" sin m^ + . . . ;
1 — 2r cos 6 -Vt^
these series hold for all values of r \jia.^ between + 1, excluding
r = 1 and r = — 1, for which the series are not convergent. To see
that this is the case, we need only write — ^ for ^r in the original
series.
The geometrical series is uniformly convergent for all values of
z of which the modulus is Si—?;, where 17 is any fixed positive
number, arbitrarily small. For the remainder after the first n
^" (1 — 7j)"
terms is :; , and the modulus of this less than ^^ — ; the
\—Z 7}
series will then be such that for all values of z of which the
modulus is S 1 — 77, \Rn{z)\< e, if
(li:^<,,orifn> ^°g^+^°g^
V log (1- 17)
Hence, since it is possible to choose n so that for all values of z of
which the moduli are S 1 — 17, the remainders after n terms are
less than e, and since this clearly holds for all greater values of n,
the series converges uniformly for all such values.
It has thus been shewn that the geometrical series is uniformly
convergent in the area bounded by any circle concentric with and
interior to the circle of radius unity with the centre at the origin.
Series of ascending integral powers.
203. We shall now consider the general power-series
tto + aiZ_+ cii^" +-.. +ariz^ + ...,
where ag, a-i, a^, ... are complex numbers independent of the com-
plex variable z. Let r denote the modulus of z, and a„, a,, Oj, ...
the moduli of ao, Oi, aj, . . . . The series of moduli is
Ko + «!'" + «2'"' + . . . + a„r-" + . . . ;
THE THEORY OF INFINITE SERIES 259
when this series is. convergent the series in powers ofz is absolutely
convergent. If the series of moduli converges for any value of r
it is convergent for all smaller values of r ; and if it is divergent
for any value of r it is also divergent for all greater values of r.
As regards this series a„ + Oir + 0,7-^ + ..., three cases may arise.
(1) The series may converge for some values of r dififerent
from zero, and diverge for other values ; there then exists a positive
number p such that the series converges when r< p, and diverges
when r > p. Wh«n r* = p the series may either converge or diverge,
as the case may be.
(2) The series may converge for all values of r ; it is con-
venient to express this by p=oo .
(3) The series may diverge for all values of r except r = 0;
this may be expressed by p = 0.
In order to determine the number p in any given case, we consider
the values of 0^"- It may happen that, as n is indefinitely in-
creased, Km" converges to a definite limit A ; in that case, if e be an
1
arbitrarily chosen positive number, as small as we please, a„" lies
between -4-1-6 and A — e for all values of n with the exception of
a finite number of such values. More generally, it may happen
that a positive number A exists, such that, for all values of n
1
except a finite set, a„» 1/A. For all values of n except a finite set a„?-"< (J. -(-6)"r",
where e may be arbitrarily chosen ; if r has a value < 1/A, we can
choose 6 so that (A + e)r = m sm 9 ^~^\ ®™ r
+ — '^ gj ^sin=0- (6),
hold for all values of ^ lying between + ^tt, whatever real number
m may be.
The series (5), (6) converge absolutely when <}> = ± \-n: For,
denoting by a, the absolute value of the general term of the first
series, we have
g, _ (2>- + l)(2r + 2) ^/ , 1 , _1_\ /, _ ^\-\
a,.+i (2r)»-m« V 2r- 2W V 4W '
therefore L r [ — - — 1 ) = ^ ,
\ar+i / 2
and thus in accordance with a known test, the series is con-
vergent. The series (6) may in a similar manner be shewn to
converge. In accordance with Abel's theorem iu Art. 207, the
series (5) and (6) converge to the values cos J mvr, + sin ^m-ir, when
A similar proof will shew that the two series
m^ — 1"
cos m^/cos = 1 g-j — - sin"* <\>
+ ^ ^^j ^-sm'4>- (7),
,, , . , m(m=-2'i) . , ,
sm m^/cos 9 = m sm 9 „ sm' 9
+ —^ 5! ^sm»0- (8),
hold for all real values of m, provided lies between + ^tt.
The series (7), (8) are not valid when = + ^tt.
THE THEORY OF INFINITE SERIES 277
The series (7) terminates only when m is an odd integer, and
(8) only when m is an even integer.
215. If we take the series for cosm<^+isinm(|),from(5)and(6),
and put e = i sin ^, we have, since (cos ip + isin ^)™ = (Jl + ^^ + «)'",
the expansion
+
m (m^ -
-P)...
. (m^ -
-2s-
■3^).
(2s
-2^)..
-1)!
m^ (mJ' ■
-2s
-2h)
(2s)!
In a similar manner we have from (7) and (8)
{Jl + z'' + zy<'lJ\+z^=l+mz+ z^+ ^ ' z^ +
2! ' 3!
m(m2-2'i)...(m»-2s-2P) „
^ (2s- 1)!
, (OT'-r)(m'-3')...(m'-2s-l|') „^ ,
+ j2sy\ ' +
It can be shewn that these expansions hold for all real values
of m, provided the modulus of z is less than unity. By some
writers, these expansions are investigated directly, and then the
series (5), (6), (7), (8) are deduced. It is however not easy to
investigate these series by elementary methods, except when the
modulus of zjj\ + z^ is less than unity ; we should, with that
restriction, obtain the series for cos m^, sin m^, only when > lies
between + ^tt, which is the same restriction that applies to the
series (1) and (2). However, by employing the principle of con-
tinuity, it is seen that the above expansions are valid in the
region | ^ | < 1 of convergence of the series.
216. If in the series (5) and (6), we change ^ into ^tt - ^, we
obtain the following series which hold for values of ^ between
and IT,
cosm (^2 - "^j = 1 - 2l "^ + ~4! ^cos^"^ -... (9),
sinm f^-0l=mcos0 ^^-^-j -cos^4> + (10).
We can now find series which express cos m(f>, sin m^, when (^
278 THE THEORY OF INFINITE SERIES
has any value^. If = r-7r + <^o.' where <^i, lies between +|-7r, and
r is an integer, we have
cos m^ = cos rririr cos mc^o — sin mnr sin m^o j
also sin ^ = (— l)*" sin ^^, thus we have, if ^ lies between (r + ^) ir,
f-, m^ ■ . , \
cos wz^ = cos mr-ir 1 1 — „-: sm^ ip + ... 1
— sin (m — 1) »-7r -jm sin <^ — ■ — ^^-^-^ ' sin' ^ + . . . S . . .(11).
Similarly
sm m
+ sin(m-l)(2r' + l) ^jwicos^ ^-^^ --^003'^+ ...\ (14),
where <^ lies between rir and (r + 1) tt.
217. Series of some interest may be derived from (5) and (6),
(7) and (8), by giving m particular values^ Let <^ = ^tt, we have
then, writing x for m, in (5) and (6),
, a? xHx^-2^) „,,
cosi7ra;=l-2^ + ^^ (15),
. , x(a?-V) a;(a!^-P)(a;'-3n
sm\irx=x- ^ g, ^ +-^ g^ji ^-...(16).
Again letting m = 2x, ij)= ^ir, in (5) and (8), we have
, x" a^ix'-m xUx-'-m(a?-2') ,,^,
cosK«'=l-2!+ 4! ^ 6! " + - (^^^'
, ,„f a;(a!'-P) a;(a;2- in (a!''-2'') 1 ,,„,
smi7ra; = iV3U- ^ 3, ' + — ff '--...[ (18).
1 The formulae (11), (12), (13), (14) were given by D. F. Gregory in the
Cambridge Mathematical Journal, Vol. iv.
2 The series in this Article were obtained by Shellbaoh, see Crelle's Journal,
Vol. XLvni. ; they have also been discussed by Glaisher in the Messenger of Mathe-
matics, Vols. n. and vn. Series equivalent to (15) and (16) are given by M. David
in the Bulletin de la Soc. Math, de France, Vol. xi.
THE THEORY OF INFINITE SERIES 279
Various series may be found for powers of w, by expanding cos^Tra?,
sin ^ IT X, ... in powers of x, and equating the coefficients of the powers of x
to those picked out from the above series ; for example from (16) we have,
by equating the coefficients of ifi,
^-'^ U^ ll_3^+i^+l 1-3-5 / , 1 , 1\,
48 3 ■ 2 "^ 5 ■ 2 . 4 V S^y^ 7 ■ 2 . 4 . 6 V 32 "^ sV
Eocpansion of the circular measure of an angle in powers
of its sine.
218. If in the expansions (5) and (6), for cos m^, sin m^, in
powers of sin^, we arrange the series as series of ascending-
powers of m, as we are, by Art. 210, entitled to do, since the
series
, m" . . , m^ (m^ +2") . ^ ,
1 + 2-,sin^ + —^^ ^ sin>+ ...,
, m (m^ + P) . , ,
m sin + — ^^-;g-j sin' 9 + • • •
are convergent, we may equate the coeflficients of the various
powers of m, to the corresponding coefficients in the expansions
of cosm^, sin»i0, in powers of ^; we thus obtaiu from (6) '•'">■' p. 13^
. , 1 sin' rf) 1.3 sin" 6
1..3.5-(2r-l)sin"+^.^
+ 2.4.6...2r 2r + l ^ ^ ^'
and from (5)
. „ , 2 sin^ d) 2 . 4< sin'' 6
<^^=«^°''^ + 3 2 +375 3 +■••
2.4...(2r-2) sin^-<^
+ 3.5...(2r-l)^^+ • ^^^^'
these hold for values of (j) between + ^tt, or when <^ = ± ^tt. We
may also write them
sin-* = ^+2 3+2;4 5 + (19).
(sin-^)^ = a.H|.f+|^f + (20),
where sin"^ x, in either equation, is the positive or negative acute
angle whose sine is equal to x.
The series (19) was discovered by Newton; the method of
proof is that of Cauchy.
280 THE THEORY OF INFINITE SERIES
219. By changing x into x + h ia the series (20), and equating
the coefficients of h on both sides of the equation, which process
is equivalent to a differentiation with respect to x, and may be
justified by employing the theorems of Arts. 210 and 208, we
obtain the series
sin~i X 2 „ 2 . 4 . ,„, .
VT3^ = ^ + 3^ + 3T5^ + (21),
or putting sin > for x,
2 2 4
(^/sin^cos^ = l +5sitf^ + K-^sin*^+ (22),
or writing 2(j> = 6,
^/sin0=l+|(l-cos<^) + ^(l-cos6»)»+...
which may be written
1 12
d cosec 6=1 + ^ vers + ^-^ vers" 6+ (23).
Again, in (22), put tan <^ = y, and we obtain the series
Expression of powers of sines and cosines in sines and cosines
of multiple angles.
220. We shall now shew how expressions of the form
cos"* sin" ^ may be conveniently expressed in cosines or sines
of multiples of 6. We shall in the first instance confine our-
selves to the case of positive integral values of m and n. Let
z = cos 6 + i sin 0, then z~'^ = cos — i sin 0, hence 2 cos = 2 + z~^,
2ism0 = z — z~^, and
(2 cos 0y (2i sin 0)" = (z + z-^f (z - z'^-y ;___
if we expand the expression in z, in powers of z and z~^, we can
arrange the result in a series of terms of one of the two forms
k{£^ + z~^), k {f — z'^'), where i is a multiplier depending on m, n,
and r ; now jH' = cos r0 + i sin r0, and z'^ = cos r0 — i sin r0, by
De Moivre's Theorem, hence
k{:^-\- z-^) = 2k cos r0, 2k (a' - z-^) = 2ik sin r0,
thus we have the required expression for cos"* 5 sin" ^ in a series of
cosines or sines of multiples of 0.
THE THEORY OF INFINITE SERIES 281
Example.
Express sin^Q cos^d in series of mvltiples of 6.
We have (2isine)^ {'2cosdf={z- z-'^f {z + z-^)« = {z^ - e-^f(z+z-^)
which is equal to {z^0-5^ + lOz^-l0z-^ + 5z-«-z-'^0){z+z-^),
or a" + 29-5zf-5z8 + 10«3 + 102-10z-i-10s-3 + 5z-6 + 52-'-«-8-2-ii,
which is equal to 2t (sin 115 + sin 9fl- 5 sin 75 -5 sin 55 + 10 sin 35 + 10 sin 5),
therefore sin55 cos«5 is equal to ^ (sin 115+sin 95-5 sin 75-5 sin 55
+ 10 sin 35+ 10 sin 5).
This process may also be arranged thus, writing c for cos 5, s for sin 5,
(2c)6 = l+6 + 15 + 20 + 15+ 6+ 1,
{2is) (20)6=1+5+ 9+ 5- 5- 9- 5- 1,
(2M)2(2e)6=l+4+ 4- 4-10- 4+ 4+ 4 + 1,
(2is)3(2c)6=l+3+ 0- 8- 6+ 6+ 8- 0-3-1,
(2w)4(2e)«=l + 2- 3- 8+ 2 + 12+ 2- 8-3 + 2 + 1,
(2is)6(2c)6 = l + l- 5- 5 + 10+10-10-10+5 + 5-1-1;
here the powers of z are omitted on the right-hand side, and a figure in any
line is obtained by subtracting from the figure just above it the one that
precedes the latter.
This very convenient mode of carrying out the numerical calculation is
given by De Morgan in his Double Algebra and Trigonometry.
221. We can obtain formulae for (2 cos 0)'^ and (2 sin 6)^,
when m is a positive integer, in cosines or sines of multiples of 0,
by the method we have employed in the last Article. We have
^ !
hence
fvi (7)1 -^ 1 )
2"^' cos*"^ = cos m9 + m cos {m-2)d+ ^ — - cos (m - 4) ^ + . . . ,
where the last term is
1 m m ! .
s 71 — TTTT — r; or — ^=^ ^ — cos a,
2(im)!(im)! (^m- 1)! (fni+ 1)!
according as m is even or odd.
From
we obtain similarly
(2isin^r=(0-^-O"'=^"-m^-'+ ~^ — ' z'"-' -...+(- l)'^z-^,
^ 1
2»-i (_ 1)2 sin""^ = cos md - m cos (m-2)6
m(m — 1) . .. „ / inT in I
when m is even,
282 THE THEORY OF INFINITE SERIES
or 2"^i(-l) '^ sin'" = sin m^-m sin (m — 2)^
m(m — 1)., .. n ,, , -—x- ml . -
+ -i^sin(m-4)^-... + (-l) ^-==^^^=^s.n^
when m is odd.
These formulae have already been obtained in Chapter Vll.
222. We shall next consider the expansions of cos™^, sin*"^
in cosines and sines of multiples of d, when m is any real number
greater than — 1. We have from Art. 212,
2™ ( + cos ^^)™ cos m (^^ - k-rr)
, m(m-l) „. , m(m— ])(m-2) _, ,
= 1 + m cos ^ + —~ — cos 2^ + --^^ gY^ cos 3^ +... ,
2" (+ cos ^ = — r: 1^ TZ r^--
The second convergent gives Snellius' formula for 0,
sin cos3"a;
therefore the sum of the series is
^ = |(ltan3»a;-3l^tan3n-ia;);
- (—tan 3" a;- tana;).
75. The sum of a series of either of the forms
Ml cos a + Ma cos (« + /8) + Us cos (a + 2y8) + . .. + M„ cos {a + (n - 1) ^],
Ml sin o + 1*2 sin (a + /3) + Ms sin (a + 2^8) + . . . + m„ sin {a + (m - 1) ^},
can be found, if m, is a rational integral function of r, of any
positive integral degree s.
Let /S = Ml cos a + Ma cos (a + yS) + . . . + m„ cos (a 4- (n — 1) /8},
then
2 cos yS . S = Ml (cos (a - /S) + cos (a + /8)} + Ma {cos a + cos (a + 2.0)]
+ . . . + Mr {cos (a + r-2^) + cos (a + r/3)}
+ ... + M„ {cos {a + TO- 2/3) + cos (a + nyS)},
whence
2(1— cos y8) /S = (2mi — Ma) cos a + (2m2 — Mi - Mg) cos (a + /S) + . . .
+ (%lr — Ur-1 — Ur+i) COS (« + r — 1/S)
+ . . . + (2t<^i — M,j_2 - M„) COS (a + n — 20)
+ (2m„ — M^i) COS (a + n — 1/3) — u^ cos (a — y3) — m„ cos (a + n/8).
Now 2ur — Mr_i — Wj+i is a rational integral function of r, of degree
s — 1, whence excluding the first and the three last terms, we have
a series of the same kind, but of which the coefficients are of lower
degree than in the given series. We again multiply by 1 — cos /S,
and proceed in this way s times ; the series will then be reduced
to the form (1).
VARIOUS THEOREMS 93
Examples.
(1) Sum the series
co«a+2 cos (a + ^) + 3 cos (a + 2/3) + ...+n cos {a+(n- 1)0}.
We have in this case 2m,.-m,._i-«,.^.i = 0, 2mi-«2=0, whence
2(l-coS|3)/S'=(n + l)cos{a+(K-l)0}-cos(a-|3)-?icos(a+ra/3),
or .S'=-^(»i+l)oos{a+(»i-l)0}/(l-cos/3)
- ^ cos (a - 13)/(1 - cos ^)-^n cos (a + »3)/(l - cos j3).
(2) Sum the series
cos a + 22 cos (a+0)+32 cos (a + 2/3) + ... + n2 cos {a + (n-l)/3}.
This series will be reduced to the last one by multiplication by 2 (1 - cos 0).
76. The series
cos a + a; cos (a + ;S) + «?■ cos (a + 2/3) + ... + «""' cos {a + (n - 1) /S},
sin a + a; sin (a + yS) + a^ sin (a + 2/8) + . . . + a;""' sin {a + (w - 1 ) /3},
are recurring series of which the scale of relation is 1— 2a; cos /3 + x^,
for we have
cos (a + r/S) + cos (a + r — 2/3) = 2 cos /3 cos (a + r — 1/3),
and sin (a + r^) + sin (a + »• — 2/S) = 2 cos /S sin {a-\- r — 1/8).
The series can therefore be summed by the ordinary rule for
summing recurring series. If S denote the sum of the first series
we find
S (1 - 2a! cos /8 + x^)
= cos a — a; cos (a — /8) — a;" cos (a + n/3) + a;"+' cos {« + (w — 1) /8}.
If a; < 1, we find, by making n indefinitely great, the limiting
sum of the infinite series
cos a + a; cos {a-\- ^) + a? cos (a + 2/8) + . . .
^ , cos a - a; cos (« - /8) -^ ... „ „ ,
to be — ; Ti 7^ ^ . rutting a = 0, we find
1 — ^xcosp + a? ^
X ~~ sc cos Q
= 1 + a; cos /S + a;'' cos 2/8 +..... . ad inf ,
1 — 2a; cos /3 + x"
whence also
l-a;2
1 — 2a; cos + a^
= l + 2a!cos/8 + 2a!''cos2/3 + ...adinf. (3).
77. In some cases the sum of a series may be found by means
of a figure. We will take as an example the series (1) and (2) of
Art. 74. Let OA^, AiA^, A^A,, ... An-iAn be equal chords of a
94 EXAMPLES. CHAPTER VI
circle, and let yS be the angle between OJi produced and A^A^;
draw a straight line OX so that Aj 0X= a, then the inclinations
of OA^, A^A^, ...An-iAn, to OX, are a, a + yS, a+ 2/3, ... a+(w-l)/8,
and that of 04„ is a + J(w— l)y3; also if D be the diameter of
the circle, we have
0^1 = i) sin |j8, 0-4„ = i) sin ^n/3.
Now the sum of the projections of OA^, A^A^, ... An^^A^, on
OX, is
Oili cos a + ^.1^2 cos (a + /8) + . . . + A„^iAn cos {a + (w — 1) /S},
or Z) sin ^/3 [cos a + cos (a + /3) + . . . + cos {a + (n - 1) ;8}],
and this must equal the projection of OAn which is
0A„ cos {a + 1 (« - 1) /3),
or D sin ^mj8 cos (a + ^ (n — 1) /8}, therefore
cos a + cos (a + /3) + ... + cos {a + (n- 1) yS}
= cos (a + |(n — 1) /8} sin ^n/8 cosec ^/3.
If we project on a straight line perpendicular to OX we
obtain the sum of the series of sines.
Examples.
(1) OA is a diameter of a circle, O, P, Q... are points on the circumference
such that each angle PAO, QAP, EAQ... is a; AP, AQ, AE... meet the tangent
a< O m p, q, r Find by means ofthisfigwe the sum of the series
«ecma«e(!(m+l)a+sec(m+l)a«ec(m+2)a+... to n terms.
(2) Prove geometrically, that if a, ^,y ... k be any number of angles,
sec a sec (a+^) sin ^+ sec (a+/3) sec (a+;8+y) sin y
+ sefl(a+^+y)«ec(a+0+y+8)sin8+...
=secasec{a+^+y\-... + K)sin{^-\-y+... + K.).
EXAMPLES ON CHAPTER VI.
1. Eliminate 6 from the equations
cos'5+acos6=6, a\-D^6-\-asm.6=c.
2. Eliminate 6 irom the equations
(a + 6)tan(fl-<^) = (a-6)tan(fl+<^), acos2(^ + 6cos2fl = c.
EXAMPLES. CHAPTER VI 95
3. Prove that
{a sin ^ + 6 cos a ; then take q negative terms, q being so
chosen that Sp — S'q-i > a, and Sp — S'q< a; next take p' positive
terms such that (Sf^+y-i — 8'q a, then q' negative
terms such that Sp+p' — S'q+g' < a, and Sp+^y — S'q+q'-i > a, and so
on. Proceeding in this way, we obtain a series such that its sum
differs fi:om a by less than its last term, hence when we make the
number of terms indefinitely great its sum will converge to a.
It can also be shewn that the terms may be so re-arranged
that the new series diverges, or that it oscillates.
The convergence of complex series.
197. Suppose ^1, ^^2, ^^3, ... Zn, ... to be a sequence of complex
numbers ; thus z„ denotes Xn + iyn, where Xn and yn are real
numbers. Let
8n = z-, + Z2+ ■••+Zn, s« = «i + a!2 + . ..-!-«„, «'n = 2/i +2/2 + ■•■ + y« ;
thus Sn = Sn + is'n-
If Sn has a definite limit S, itself a complex or real number,
when n is indefinitely increased, the infinite series
Z1 + Z2+ ■•■ +Zn + ••■
is said to be convergent, and >Si is called its limiting sum, or
simply its sum.
The condition that 8 = LSn is that | /S — ;Si„ | converges to zero
as n is indefinitely increased ; thus if
S — 8n = pn (cos 6n + i sin 0n),
252 THE THKOBY OF INFINITE SERIES
we must have Lpn = 0. If S = s + is', when s and s are real, we
have s — Sn = pn cos On, s' — s'n = Pn Sin 0n ', it then follows that, if
Lpn = 0, we also have L{s — s„) = 0, L (s — s'„) = 0, or s„, s'„
converge to s and s' respectively. It thus appears that in order
that the series 2i + Z2 + Zs + ... may be convergent, it is necessary
that the two series Xi + Xs + Xs + ..., yi + y2 + ys + ••■ should both
be convergent. Conversely if these latter series are convergent,
the series of complex numbers is also convergent, for
I (S + is') - (Sn + is'n) | ^ | S - S„ ( + | s' - s'„ | J
if now Lsn = s, Ls'n = s', we can choose a value n^ of n so large
that |s — s„|<^6, \s' — s'n\<\e, provided n^n^. It follows that
I (s + is') — {sn + is'n) | = 6, if w S w^ ; and since e is arbitrary we
therefore have L (s„ + is'n) = s + is', and thus the series of complex
numbers is convergent. In case the limiting value of either
of the sums %x, ^y is not finite, or in case either of these series
oscillates, the series Xz is not convergent.
Suppose Zn = fn (cos dn + i sin 0„), then we shall shew that the
series liZ is convergent provided the series %r, in which each term
r„ is the modulus of the corresponding term Zn, is convergent.
The given series 2r„ (cos dn + i sin 5„) is convergent provided each
of the series 'LvnCosdn, XrnSmOn is convergent; now each of the
numbers VnCosdn, rn&vaOn lies between the numbers ±r„; also
the number Sn+m — Sn is for either of the series Sr cos 6, Xr sin 6
numerically less than the corresponding partial remainder for
the series 2r. If then the latter series is convergent, so is each of
the former ones ; hence the series Xzn is convergent.
The converse is not necessarily true ; thus the series
2r„ (cos On + i sin 9n)
may be convergent, whilst Sr^ is divergent.
If the series Xvn formed by the sum of the moduli is convergent,
then the series 2r„ (cos 6n + i sin dn) is said to be absolutely con-
vergent.
For example, the series of which the general term is n~^(coand+ismnB)
is absolutely convergent, since the series Sm"^ converges, whereas the con-
vergent series of which the general term is n~^(coan6+iaianff), (2i7>6>0),
is not absolutely convergent, since the series Sn''- is divergent.
THE THEORY OF INFINITE SERIES 253
Continuous functions.
198. Suppose /(«) to be a function of the complex variable
z = x-\-iy, which has a single finite value for every value of z which
lies within any given limits ; this function will then have a single
value for every point in the diagram, which lies within a certain
area ; this area may be any finite portion of the plane of repre-
sentation of z, or the whole of that plane.
Such a function is said to be continuous at the point z = Zi,
if a positive number rj can always be found such that the modulus of
f (z) — f (Zi) is less than an assigned positive number e, taken as small
as we please, for all values of z which are such that the modulus of
z — Zi is less than rj. For each value of e a value of ij must exist.
A function which satisfies this condition at every point within
any given area, is said to be continuous in that area. The boundary
of the area niay, or may not, be included.
Uniform convergence.
199. Let fn{z) be a function of or a; + iy, which is continuous
in any area ; then if the series
f{z)+f{z) + ...+f^{z) + ...
is convergent, we may denote its limiting sum by F{z). Suppose
Mz)^f{z) + ...+f^{z),
where n is any fixed number, is equal to Sn{z), then the limiting
sum oi fnj,i{z) + fn+i{z) + ■•• is called the remainder after n terms,
and may be denoted by Rn{z) ; we have therefore
F{z) = Sn{z) + Rn(z).
Now suppose that, corresponding to any given positive number e,
however small, a value of n, independent of z, can be found, such
that for all values of z represented by points lying in any given
area, the modulus of Rm(z) is less than e. where m is equal to or
greater than n, the series is said to converge uniformly for all values
of z represented by points in that area. The integer n will depend
in value upon e.
If as z approaches indefinitely near any fixed value z^ in the
area, in order that the moduli of all the remainders R'm{z) may be
less than e, it is necessary to suppose n to increase indefinitely,
254 THE THEORY OF INFINITE SERIES
then in the neighbourhood of the point Zy, the series does not con-
verge uniformly and is said to converge infinitely slowly. A
point z^ for which e can be so chosen that this happens is said
to be a point in the neighbourhood of which the convergence
is non-uniform, or sometimes simply a point of non-uniform con-
vergence in case the series converges at that point itself For any
space including such a point it is impossible to assign any fixed
value of n, such that for all values of z within that space, the
moduli of Rm are less than the sufficiently small positive number
e; and thus the series does not converge uniformly throughout
that space. When z is equal to z^, the series may be either
convergent or divergent.
We may state the matter as follows :
Suppose that as z approaches some fixed value z-i a positive
number e can be assigned such that the number of terms n of the
series /i(^:) +/i.(^^) -I- ... which must be taken, in or^er that mod.
Rm{z) < e, where m is equal to or greater than n, depends on the
modulus of z — Zi in such a way that n continually increases as
mod. {z — Zi) diminishes, and becomes indefinitely great when mod.
{z — z^ becomes indefinitely small, the series is said to converge
non-uniformly in the neighbourhood of z^.
In the neighbourhood of such a point, the rate of convergence
of the series varies infinitely rapidly, and when mod. {z — z^ is
diminished indefinitely, the series converges indefinitely slowly.
It should be observed that a convergent numerical series
cannot converge infinitely slowly ; thus when z is equal to z^, the
convergence of the series /i(^i) 4-/2(^1) + ..., if it is convergent, is
not indefinitely slow; it is only when ^r is a variable such that
mod. {z — Zi) is indefinitely diminished, that the series
converges infinitely slowly. It is consequently more exact to speak
of the non-uniform convergence of a series in the neighbourhood of
a point, than at the point itself. The number of terms n that must
be taken in order that the modulus of the remainder i2„(^^) may be
less than the sufficiently small number e, increases as z approaches
the value z^, becomes indefinitely great when mod. (z — z,) becomes
continually smaller, and then, if the series is convergent at the
point Zi, suddenly changes to a finite value; this number n is
therefore itself discontinuous in the neighbourhood of such a point.
THE THEORY OF INFINITE SERIES 255
If in any area A we have, at every point of the area,
|/i(«) I S (h, |/2(«) I S tta, ... \fn{z) I S Cf„, ...,
■where Oi, a^, ... an, ... are fixed positive numbers such that the
series aj + as +•••+«»+•• ■ is convergent, then the series
is uniformly convergent in the area A. This theorem affords a
test of uniform convergence which is of great value in application
to particular cases ; it is known as Weierstrass's test. To prove it,
we observe that, if e be an arbitrarily chosen positive number, We
may be so chosen that a„+i + a„+2 + • • • + a»+m is, for every value of
iJi, less than e, where n = ne. The modulus of
|/»+l(«) +/«+2(^) + ••• +/«+m(^) I
is, for every value of z, not greater than a^+i + an+i + ... + a«+m,
and is therefore less than e. Since this holds for every value of m,
we see that the complex series is convergent, and that for every
value of z, | i2„(^:) | < e, provided nSrie. Therefore the series
converges uniformly in A.
By some writers, a series is defined to be uniformly convergent in a
given area, when a number n can be found suoli that for all values of z, the
modulus of the remainder R^ is less than e. The definition given in the text
is more stringent than the one here mentioned ; it is possible to construct
series which converge xmiformly according to the latter but not according to
the former definition.
200. If the functions /i(0), /^(z),... are continuous for all
values of z represented by points lying in a given area A, then
the function F{z) which represents the sum of a convergent series
'S,f(z), is a continuous function for all values of z represented by
points lying in the area A, provided the series 2f(z) converges
uniformly/ in the whole area A.
For we have F{z) = Sn + Rn,n being such that for all values
of z to be considered, the modulus of -K„ is less than e; let ^
receive an increment hz, and let BF(z), BSn, S-B„ be the corre-
sponding increments of F(z), Sn , and jB„ . Then, since by supposition
the moduli of i2„ and J?„ + SJ?„ are both less than e, the modulus
of SRn is less than 26. Also since Sn is a continuous function
of z, if the modulus of Bz be small enough, the modulus of SSn is
less than e ; hence, provided mod. Sz is less than a certain value,
the modulus of S8n + SRn or of SF(z) is less than Se, since the
256 THE THEORY OF INFINITE SERIES
modulus of SSn + Si?„ is not greater than the sum of the moduli of
BS„ and Si?„. Now Se can be made as small as we please, there-
fore mod. BF(z) can be made as small as we please by making
mod. Sz small enough; that is to say the function F(z) is continuous.
It will be observed that for this proof, the less stringent definition of
uniform convergence, given in the note to Art. 199, is sufi&cient.
201. For a value z^ of z, for which the series converges non-
uniformly in the neighbourhood, the sum of the series is not
necessarily continuous; in this case the reasoning of the last
Article fails. The limiting value of the function /„(^^), when z = z^,
00
is fni^i), but it does not follow that 2 {/»(^) —fn{zi)} converges to
n
zero as z converges to z^. We may denote the sum 2 {/(^) —/(■»!)}
1
by F(n,z — Zi), a function of n, and of z — z^; now the limiting
value of F{n,z— Zi) when z is first made equal to Zi, and then n is
afterwards made infinite, is zero; but if n is first made infinite,
and afterwards z — Zj is made zero, the limiting value of F(n, z — z^
is not necessarily zero.
As an example of this phenomenon, Stokes considers the real series
1 + 5^ x{x-V%')'rfi-\-x{^-x)n-^\-x
+ ••• + „/- . IN f/_ — Tx_ , II /__ , 1N + ---;
2(1+^) n(»i+l){(K-l)x+l}(?u; + l)
when A'=0, this series becomes
1 1
;+... + -
1.2 " ra(re+l)
Now the general term is
1 2«
Ji(9i + 1) {{n-\)x+\\{nx-V\y
\n (?i-l)^+lj [« + l Tix-VX) '
therefore the sum of the series is 3, whatever value different from zero x may
have; the sum of the series = — 5 + 5—5 + ... is however unity, and thus the
sum of the series is discontinuous in the neighbourhood of the value of a:=0.
r
find
1 2
The remainder after n terms is =■ H =- ; putting this equal to e, we
71 + 1 nx->r\ ' ^ D T^
M = {^+2-f(^+l) + \/{e(«+l)-(^+2)}2-4f^(6-3)}/2€a;,
which increases indefinitely as x becomes indefinitely small ; thus the series
converges infinitely slowly when x is infinitely small ; this is the reason of the
discontinuity in the sum of the series.
THE THEORY OF INFINITE SERIES 257
The discovery of the distinction between uniform and non-uniform con-
vergence of series has usually been attributed to Seidel, who published his
" Note iiber eine Eigensohaft der Reihen welche discontinuirliche Functionen
darstellen " in the Transactions of the Bavarian Academy for 1848 ; the
theory had, however, been previously published by Stokes, in a paper "On
the Critical Values of the sums of Periodic Series*," read on Dec. 6, 1847,
before the Cambridge Philosophical Society. Although the theory is in some
respects stated more fully by Seidel than by Stokes, the latter must be
considered to have the priority in the discovery of the true cause of dis-
continuity in the functions represented by infinite series 2. The distinction
between uniform and non-uniform convergence has played a very important
part in the modern developments of the subject.
The matter is summed up by Seidel in the following theorem : — Having
given a convergent series, of which the single terms are continuous functions
of a variable z, and which represents a discontinuous function of z : one must
be able, in the immediate neighbourhood of a point where the function is
discontinuous, to assign values of z for which the series converges with any
arbitrary degree of slowness.
The geometrical series.
202. Consider the geometrical series 1+ 2 + z^-'r ... + ^"~\
where z = x + iy = r (cos 9 + i sin 6). We have for the sum of this
series the value
l-«" l — r'^(cosn6 + iainnd)
1—z 1—r (cos 6 + i sin 6) '
put l — rcosd = pcos(j}, r sin = p sin