/ Ot mj Du < a given density should be given to Gunpowder far Artillery purposes^ To determine the above, Gunpowder made at Raleigh, and at Columbia for the Navy were employed, as well as different kinds received from Europe-, ami those manufactured at the Government 3 ~$ Powdev Works near Augusta. The average gravimetric densities of the Cannon Powders were as follows : Navy 1025 Raleigh : 1026 Foreign 875 Power Works 914 *Dupont's, U. S 919 *Hazard's, U. S 924 *Waltham Abbey, (English Government Powder) 872 * French War Department Powder 804 ♦These Powders were not experimented with — none to be had. Taken from Mordecai's Report on Gunpowder. The specific gravity of each description of Gunpowder would have been a more accurate representation of their comparative densities, but such was not attainable ; and the gravimetric densities given in the table, are sufficiently near approximations for the purpose proposed. Tt will be seen from it that the Navy and Raleigh Powders are very dense, and hence afforded good opportunity to compare such kinds of Powder with those of a less density. The results of such trials will be ft mnd in the tables annexed to this Report, as also those relating to the comparison of "Mill Cake" and "pressed" Powders, and the comparative strengths of grained and mealed powders, and of their mixtures. From the above series of experiments the following facts were deduced, viz: First — The density of Gunpowder, resulting from more or less com- plete pulverization of its ingredients, the time consumed in their incorporation, and the subsequent pressure of the damp mass, should not exceed 950 ounces to the cubic foot for Cannon Powders. An increase of this density cannot be fully compensated by fineness of grain, even when carried to an extreme. Second. — The most perfect intermixture of the ingredients appears to be in the " Mill Cake," which if broken up cannot afterwards be restored by pressure, since the former operation has a tendency to disturb the intimate association of the lighter and heavier particles, and thus cause a partial separation which simple pressure cannot restore. Hence that the requisite density should be obtained by working the mass of ingredients together, and not by means of pres- sure. In other words, all Cannon Powder should be made directly from " Mill Cake " of the required density, and not from cake formed by pressing Meal Powder or Powder Dust. Steaming the mixed ingredients of Gunpowder before incorporation appears to make a superior Powder in much less time. Third. — The dust formed in the manufacture of powder has about £ of the strength of the powder from which it is derived, when used for artillery charges, hence it may be used for such purpose when grain powder cannot be had. The dry dust formed by the mixture of the ingredients of Gunpowder in the rolling barrels which has never been subjected to moisture, is not a true Gunpowder composition, since the pores of the charcoal have not been tilled with the saltpetre, which can only be done by a more or less partial solution of that salt. Fourth. — A raixtun irge :i proportion as one-hajf of dust ■t materially to affect the strength of Gunpowder, hence a dusty powder is no Sign of its inferior strength. Fifth. — The size of grain of Gunp »wder has an important bearing in the service of heavy artillery; it' the grains b i too small the -train on the gun is greatly increased, with no oding increase irf initial velocity ov range to the projectile. Sixth. — A mixture of large and small grain ]> »wder appears to burn up in the laige charges tor heavy artillery as ir' composed entirely of tne smaller size of grain, hence such mixtures are hazardous for service charges. Thus a mixture <>f one-half large cannon ami one-half small cannon in a cartridge weighing 8 pounds, packed and fitting the bore of the 7 inch earn, with a 0.5 pounds holt, without windage, gave the enormous pressure of 120,000 pounds to the square inch at the moment discharge. The same charge, under precisely the same circum- stances, of large cannon powder alone, (grains A inch) gave a mean pressure of 80,000 pounds. Seventh. — A Gunpowder made of proper proportions of nitre and charcoal, without sulphur, is hut little inferior to good powder of the usual composition. Thus 65 grains of Gunpowder incorporated three hours gave 1057 feet initial velocity, whilst the same weight of the nitre and charcoal powder, under the same circumstances, gave 990 feet. Eighth. — A charge of eight pounds large cannon powder, grains .0 inch in diameter, made from "mill cake,'? and having a gravimetric density of about Ol'O, with a holt weighing 05 pounds, without windage, was entirely consumed in the seven inch gun, none of the grains being thrown out unburned. Ninth. — A similar charge in all respects, except that the powdcf had been subjected to hydraulic pressure, with a gravimetric density of about 1000, on being fired, several of the grains were thrown against the screen of boards in front of the gun, apparently without having taken fire at all by the discharge. Tenth. — The air space, in connection with a charge of powder, ena- bles us to use a much larger grain. Thus an air space of one-half calibre, in the 7 inch gun, with the 65 pounds boit, enables a charge of 10 pounds of powder to be entirely consumed within the gun, whose grains were from .75 to .90 in diameter, and 36 of which weighed one pound. Gravimetric density about 930. Second Question. — M'Tiat advantage, if any, results from the em- ployment of Air Sjmces for the partial expansion of the inflamed gases of the charge, and if advantageous, what should be their dimensions, and xohere located ^ To determine the above over one hundred trials were made, with the guns named, but mainly with the 7 inch Columbiad, with air spaces of different dimensions, from 1-10 part of a calibre to 1:5 calibres in extent. In each case the initial velocities and pressures were carefully taken, the mean results of which — in the more important cases — will be found in the appended tabular statements. In making these experiments the charges were packed into paper cartridges, tilting the Lore, or with a certain less diameter, so that the influence of the actual amount of air space might be certainly made in each case. It being plain to see that the intervals between the grains of powder — the latter being in a . more or less compact condition — would in themselves constitute an element to be taken into considera- tion ; thus a service charge for a heavy gun may be settled in the cartridge so as to occupy from ^ inch to 1 inch less space in length than when loosely poured in, hence in the trials the powder was closely packed in each cartridge. The following facts were deduced from the trials, viz : First. — Air spaces, properly proportioned to the charge of powder, greatly diminish the strain on guns, without loss of i initial velocity or range, and hence are of great importance in the service of heavy artil- lery especially. Thus 8 pounds of large cannon powder (grains .4 inch diameter) packed into a cartridge lifting the bore of the 7 inch gun, with a bolt of 05 pounds, without windage, gaVe a mean pressure of 80,000 pounds to the square inch, whilst a similar charge in all respects of 10 pounds of the same powder, with an air space of I- calibre, gave a mean pres- of 49,431 pounds; the addition of one pound weight of charge, (11 pounds of powder) whose grains were from .75 to .00 inch, with same air space, gave a mean pressure of 24,717 pounds, the same initial velocity being had in each case. Second. — Retaining the service pressure on the bore of the gun, increased velocity can be given to the projectile by the addition of a proper quantity of powder to the charge, by the use of the principle of the air space. Third. — Air spaces of about one-half the calibre of the gun appear the most advantageous., with an addition to the service charge of about one-fourth of the weight of powder. Larger air spaces give the same results of pressure, but require larger charges of powder to maintain the velocity, hence no advantage appear&tobe gained beyond the limil specified. The service charge is understood to mean a given amount of the proper size of grain powder placed in a cartridge fitting the bore of the gun, and closely parked, with a square end to the cartridge next to the projectile, and the latter, if of the rifle kind, rammed well home, to cause the cup to pass over the end of the charge, so as to avoid a par- tial air space; or, if a round shot be used, that it shall have a proper sabot attached to it. The above charge, when fired as above arranged, to give a mean pressure not exceeding that which in service is regarded as safe for the description of gun under trial. To ascertain this pressure in any required calibre or gun, let it be loaded as usual, and by means of the pressure piston ascertain the mean pressure of several fires. Having thus ascertained the service charge as above defined — which it will readily be seen will be in general less than that usually employed — add one-fourth of its weight for an air space of X- calibre. By this means the strain on the gun will be reduced to less than one-half of that due to the service charge, without loss of velocity or range. The Board have thus indicated the proper method to be pursued in arriving at the proper charges Por all descriptions of heavy artillery. The want of a gun of each cable.' to experiment with, is the reason why the charges themselves have not been determined, and such data would then have formed a part of this Report, which would have, in such case, been final. A> the foregoing determination requires the use only of the pressure piston, which can be attached without injury to the gan orguns at any ponvenient battery, it is respectfully recommended that authority be given to the Board to make use of such guns as may be selected for the above purpose, and thus enable the Board to complete its labors in a satisfactory manner. Fourth. — The air space would be most convenient as an air cham- ber in rear of the charge, or, in other words, like the chambers of Howitzers; but in the guns now in service the same end may be arrived at by diminishing the diameters of the cartridges, by passing sticks through their centres with projecting ends, or by means of tin- devise of the hollow cartridge, or by using a cross of light boards, joined at right angles and edgewise at their centres, to insert between the charge and projectile. Fifth. — As all cartridges of less diameters than the corresponding bores of guns have equivalent air spaces, such must be allowed for in practice. Also the spherical form of balls without sabots, when not rammed so as to embed themselves in the charge, have a certain amount of air space in each case, which must be taken into considers tion. Sixth. — The usual custom of making cartridges of less diameters than the bores of their respective guns, is an acknowledgement of the principle of the air space; but it has not been carried sufficiently tar, neither has any relation been heretofore established between the weight of the charge and air space employed. Seventh. — The pressures at each extremity of an air space, however long in the bore of the gun, are equal ; in other words, all parts of the bore, between the breech and projectile, experience like pressures on equal areas at the moment of inflammation of the charge. Third Question. — What arc the causes of variation in Artillery Practice, and by what means can a (greater uniformity in the results be obtained ? In the investigation of this subject the Board has no hesitation in saving, that the main cause of varied results in artillery practice arises from overlooking these important facts, that variations in the diam- eters of the cartridges, although apparently slight, and of the more or less loose state of the powder charges, have great influence on the initial velocities and ranges of projectiles, as well as on the strains sustained on the guns employed. First. — Hence uniformity in the compactness of cartridges, and in their diameters, are of the first importance in the service of artillen . Thus one pound of small cannon powder, packed into a cartridge fitting the bore of the 3 inch rifle gun, gave an initial velocity of 1260 feet to a shell of 7^ pounds weight, whilst the same amount of the same powder placed loosely in the cartridge bag gave but 1042 feci ; the shells in each case not being rammed, but dimply pressed lo its position on the charge. Again, 8 pounds large cannon powder, in the 7 inch gun, packed in a cartridge fitting the We, with ;i bolt of V>o pounds, without windage, gave an initial velocity of 1265 feet, whilst the same charge in all respects, loosely put into the cartridge bag, so as to diminish it§ diam- eter about one inch, gave only 1104 feet. Other experiments with the other calibres gave analagous results, clearly showing the fact that very considerable variations of ranges in artillery practice will be experienced, unless great care be taken in the diameters of cartridges, and the packing of the powder. A cartridge fitting the bore, with its powder packed, cannot be essentially disturbed by variations in the force or manner of ramming, whilst a cartridge of less diameter would either be burst by hard ramming, and thus fill the bore, or would be crowded up so as to occupy less space in 'a more or less degree, thus materially influencing the range of the projectile and pressure on the gun. Again, a loosely packed cartridge will admit of the ball being cushioned in it by ramming, thus decreasing more or less the airspace due to its form, and consequently affecting the range. Second. — A second cause of variation of range in smooth bore artillery arises from the windage, and consequent ballotting of the ball, which thus does not leave the muzzle of the gun in the true line of direction. Variations of range also takes place from the different degrees of quickness of burning in the charge, hence a larger amount of its force escapes around the ball before it fairly gets into motion within the gun, at one time than at others, as no two charges bum exactly in the same time. These two causes of variations may to a great extent be removed by wrapping the ball with cloth and driving it to its position. Thus with the 12 pounder Napoleon, with equal charges, packed into cartridges fitting the bore, the following results were obtained: 1st discharge, initial velocity 1288 teet. L >,1 u •• - " 1288 " With « different charge. 1st discharge, initial velocity t208 feet. •_M « - '• ' 120- •• With a still different charge, 1st discharge, initial velocitv 1220 feet. 2d " " " 1220 " G Pounder Bronze. 1st discharge, initial velocity 1290 feet. 2d " ' " " 1296 " The loss of velocity by windage is sometimes very great, amounting in some cases to the £ part, thus in the 12 pounder Napoleon : 1st discharge, ball of large windage, without sabot, velocity 1126 feet. 2nal sources of variation of range anil accuracy. It. From an insufficient rotary velocity. 2d. Prom a defective cup or saucer. 3d. From the imperfect casting, causing the shell to crack by the discharge, and thus communicate lire to its bursting charge — which failure is m general erroneously attributed to a faulty fuse. 4th. From a defective form or model, whence arises the defects of the projectile, being too weak, too heavy, or too long for the charge of powder and twist of the gun. An insufficient rotary velocity, resulting in the turning over of the projectile, sometimes within a few feet from the muzzle of the gun, may arise either from too small a charge of powder, or from the pro- jectile being too long and heavy. There are two ways of obtaining ;i higher angular velocity; either by increasing the twist of the gun, or by increasing the initial velocity. The former cannot be done except in new guns, and in these there are practical limits which cannot safely be exceeded; the increase of velocity also has its safe limits, beyond which it would create a hazardous strain on the gnu, by the necessary propelling force employed. Hence those projectiles whose defective models cannot be safely compensated by the above, and hence must remain variable in their 9 results) should be rejected. This applies particularly to those heavy bolts, and sometimes shells, which in many cases considerably exceed the limits within which a safe charge could communicate the necessary initial velocity to produce the required angular rotation. The above is mainly the reason why the Board, in their first Report, recom- mended projectiles of less weight and length than many which had been and are still employed in service. The cups or saucers at the base of rifle projectiles are frequently defective in having their edges too thick, whence they do not expand suiiicicntly quick, and thus allow a considerable portion of the force of the charge to escay around them. A certain amount of force is required in each case to expand tin' cup and cause it to take the grooves, and if any of the charge be lost from the above cause, what remains may l>e insufficient for the purpose. Hence the edges of the cups should be quite thin, or they should be sawed into several segments, to the distance of about £ of an inch from the fih^c downwards, so as to permit the latter to readily yield to the first pressure, and thus prevent the escape of a portion of the inflamed gases. The lubricating ring between the base of the projectile and cup acts mainly in assisting to close the windage at the first moment of inflam- mation, and thus more certainly insures the expansion of the base. As far as the lubrication of the gun is concerned, it can more certainly and effectually be accomplished by pouring a sufficient amount of the material melted into the bottom of the cup, which at the time of the discharge will be disperse.] throughout the boreof the gun. The lubri- cating material in this case should not be hard, but rather of a -'.siency. tii Question. — The use of the Air Space in Artillery involves the necessity of placing the projectile farther towards the muzzle, or of allowing an interval between it and the charge. What is the maximum interval that can be safely allowed, or is there any danger to the gun by thus displacing the projectile from its usual position, resting against the charge? In the series of experiments, undertaken to elucidate this subject, with the different guns at the disposal of the Board, the fact was clearly established that the common opinion, as to the danger incurred in the displacement of the projectile from the charge, is without sufficient foundation. That the maximum strain on the gun is experienced when the projectile is closely rammed home on the charge, the latter being packed and fitting the bore. That in proportion as the projec- tile is removed from the charge towards the muzzle the strain de- creases, and is at its lowest point when it is at or near the muzzle itself. Thus 2 lbs. of small cannon powder has been repeatedly fired with three balls placed within 2 calibres of the muzzle of the 6 pounder; also several charges of the same weight of powder, and the ball wrapped with cloth, and driven tightly to the same distance from the muzzle. In all these eases no injury whatever was experienced by the 10 Again In the 7 inch gun, with 8 lbs. large cannon powder, with the bolt of 65 lbs. tightly fitting the bore, the average pressure', as has i seen, was 80,000 lbs. to the square inch. When the boh was placed at 30 inches distance from the charge, all other conditions remaining the same, the pressure was only 6258 lbs., and at 2 calibres from the muzzle the pressure fell to an average of 2617 lbs. Thus no danger whatever arises from leaving a single projectile in any part of the bore, but on the contrary the strain on the gun i^ greatly decreased by removing the projectile to some distance from '.In' charge of powder. Fifth Question-. — Ts there any danger tn the Rifle Gun .should the projectile fit so tightly as to require to be driven to its position on the charge, and should it pet jammed in the act of loading, would there be hazard m firing off the gun in such condition.' Experiments conclusively demonstrate that in all cylindrical pro- jectiles which have been turned in a lathe, no amount of force that can be generally employed to drive them home on the charge, affects in the slightest degree the pressure or strain on the gun at the time oi' the discharge. This might be reasonably inferred without experiment ; tor as such projectiles cannot by any movement increase their diam- eters, the additional .strain on the gun would be simply that due to the additional force required to overcome the friction. This has for its measure the force which was expended in driving the projectile home ; but such an amount of force is inappreciable when compared to the immense force exerted by the charge in overcoming the inertia of its mass. The preceding discussions plainly show tHat no danger can be in- curred in firing off a gun, with a turned cylindrical projectile, which shall become jammed in the bore. The case would be very didereni with spherical projectiles, for as these are never turned off to a true form, it might happen that a larger diameter would be brought into action by the rolling movement, and thus operate upon the principal of the eccentric press, wedging the gun asunder : thus a tight fitting naked shot would be too hazardous for service. Sixth Question. — Is there any fixed relation between different amounts of Gunpowder and the corresponding initial velocities ; that is will successive additions of equal weights of powder produce an equal increase in the corresponding initial velocities! Experiments show that in those charge* which arc entirely consumed within the gun, and not too small in quantity, equal increments of powder correspond to nearly equal increments of velocity. Thus in the 3 inch gun 1 lb. of small cannon powder gave 1250 feet initial velocity; £ lb. gave 1040 feet; ^ lb. gave 800 feet; each quarter of a pound, starting from the half pound charge, giving about 240 feet increase of velocity. This also holds good of small arms, between certain limits: thus 45 grains of rifle musket powder, with an expanding projectile of 535 grains, in the Enfield rifle, gave 829 feet initial velocity ; 55 grains 11 gave 952 feet; 65 grama gave 1078 feet; or about 125 feet velocity for each 10 grains of powder. Below 40 grains of powder, there is not sufficient force to properly expand the base of the ball, and above 65 grains a portion of the powder is not consumed. A similar obser- vation applies to artillery practice, for below a certain initial velocity t lie cup of the rifle projectile does not expand and take the grooves, and above a certain weight of charge the powder is not wholly burned. Seventh Question.— Does a high angle of firing in the practice of Art tiler it increase the strain on the gun? Experiments were conclusive on this point, showing that firing at angles of elevation does not affect the pressure on the bore of the'gun due to the same charge fired horizontally. Thus the mean of three charges of 8 lbs. large cannon powder, .packed into a cartridge § of an inch less in diameter than the bore of the 7 inch gun, with 'a bolt of 65 lbs. without windage, gave a mean pressure of 64,000 lbs. to the square inch, when tired with the bore in the horizontal plane. The same charge in all respects, when the gun was fired at an angle of 40° elevation, gave a mean pressure of three discharges somewhat less than the above. MISCKLLAXEOTJS DATA. 1st. The projectile being placed inside of the bore and near the muzzle, with the charge of powder next to it, if the latter be fired in its extremity next to the breech, the pressure will be fonnd exceedingly small, scarcely sufficient to throw the projectile ten feet from The muzzle of the gun, as the cartridge and ball' are thrown out together before time has been given for but a smallnortion of the powder to be consumed within the gun. if the charge be fired at, its end next to the projectile the pressure and explosion will be greater, though still much inferior to what it would have been with "the cartridge at the bottom <>f tie' bore. 2d. Tin- force of the charge, in small rifle guns, must be able to im- part an initial velocity of not less than 1000 feet to the projectile, to insure the expansion of the cup into the grooves of the gun. Similar data in relation to large rifle guns remains to be determined. 3d. 'I here appears no necessity for turned bolts having a greater windage than .05 inch for smooth bore guns; and if they be made with a recess of 1| inches broad and about 3-16 inch deep, in that extremity next to the charge, and this be filled up with lubricated -trips ol cloth, all windage will be prevented, and additional force and accuracy given to this species of projectile. 4th. A few heavy charges is not proof that a gun will be able to continuously sustain them. Thus a 12 pounder gun was finally burst at a considerable less prcs*sure than what it had previously at "several limes, sustained without apparent injury. 5th; The pressures in the use of' service charges in field artillery are about half those of smooth bore heavy gunsi (5th. Half the charge of powder with a double weight of projectile, , 3 the same pressure in heavy artillerv a IV . GUNPOWDER FOR ARTILLERY. First. — It is not advantageous for cannon powder to exceed a gravi- metric density of 950. Second. — All cannon powder should be made from Mill Cake oi' the proper density, and not from pressed cake, or cake formed by pressing dust. Third. — Powder for large cannon, if made from Mill Cake of a gravimetric density of not exceeding 030, should not have a less size of grain than from ^ to ^ inch in diameter. If air spaces be employed, the grains should not be less than from .75 to .00 inch diameter for all calibers above 7 inches. For very large guns with air spaces, as the Great Blakely guns, the grains should be over one cubic in capacity i or each grain should weigh about one ounce. Fourth. — Unless the powder be of excessive density, any mixture of small cannon or fine grain powderwith large camion powder should be most carefully avoided as very hazardous in the service of heavy guns, without any corresponding increase of force or range to projectile. \ AIU SPACES. First. — Air spaces properly proportioned to the charge of powder greatly diminishes the strain on guns without loss of initial velocity or range, and hence are of great importance in the service of heavy Artillery *, they may be in front, rear, inside or outside <>f the Cartridge.. Second. — Air spaces of about one half caliber of the gun appear the most advantageous as far as tried, with an increase to the service charge of one fourth the weight of large grain powder. Third. — The most convenient form for the airspace would be a cham- ber to the gun, but the usual service Artillery may be used with air spaces by making the Cartridge hollow, and thus containing the necessary space in itself; or the cartridge being compact, with a square or flat end, two pieces of board fixed together at right angles edgewise, forming a cross, might be inserted in the bore of the gun, so as to keep the projectile a proper distance from the charge. These wood crosses could readily be made, and easily used like wads. Foiirth. — Cartridges of less diameter than the bore of the guns to which they belong have equivalent airspaces; spherical projectiles also leave spaces due to their form, next to the charge. Such air spaces however are variable in dimensions, and hence objectionable. 18 CAUSES OF VARIATION IN ARTILLERY PRACTICE. First. — Uniformity in compactness of cartridges and in their diam- eters are of the first importance in the service of Artillery, and the want of which is the main cause of variation of range in Artillery practice. Second. — Cartridges for Artillery should he made to fit the bore of the gun, the powder well packed, with the end next to the projectile flat. Such cartridges can be made by first making a cylindrical bag to fit the bore, and placing within this a thin paste board cylinder without ends of nearly the diameter of the bore. Into this pack the charge well, and insert at the open end a circle of wood about f of an inch thick, with a deep groove cut into its edge; the paper cylinder being cut just the height of the charge, the open end of the bag is drawn up tightly around this circle of wood, which is pressed down on the powder, and then firmy tied in the groove. Hollow cartridges <-;ni be made in the same manner, first inserting a hollow cylinder or paste board, or tin, with closed ends, having the required capacity of air space. Third. — Spherical projectiles for smooth bore heavy artillery should have sabots attached to them separate from the cartridge. Such sabots should be hollowed out in the end of the fibres of the wood, so as to Rover as much as practicable the part of the ball next to the charge. Such s.ihots will answer a double purpose of filling up t he empty space — the airspace being otherwise obtained — and also preventing the rolling forward of the ball in the bore in firing on a level, or at an angle of depression ; the wood cross before alluded to could be used for this last purpose. At the instant of firing the sabot is forced forward on the I >all thus filling up the windage, and preventing to a considerable degree the balloting of the projectile. Fourth. — Powders at the different batteries should be tested and sified not less than every six months, if put up in cartridges; if in the original boxes or barrels, once each year would be sufficient. In the practice of Artillery the powder of the same classification should alone be used until expended; a slight change of elevation would then maintain the same range with another class of powder. 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