That this argument applies principally to solid forged guns I am ready

to admit; and that guns forged of hoops, rings, and bars, in smaller

sections, are free from this objection, I am also ready to admit. These

guns are, however, liable to objections equally fatal, both as regards

their enduring and projective powers, as I shall presently show.

Experience proves that brass guns are inferior, both in sharpness of

shooting and in range, to cast-iron guns: this is undoubtedly

attributable to the greater softness of brass than of cast iron; and for

the same reason a wrought-iron gun, though made as sound as one of cast

iron, would be inferior in these two important points. But when a

wrought-iron gun is composed of many particles imperfectly secured (and

no mechanical force is sufficient to secure perfect cohesion in large

masses), the wrought becomes doubly inferior to the cast gun: a shot

projected from such a gun starts from an unsound base; a large portion

of the explosive force is absorbed by the variety of sections composing

the gun, to the injury both of the accuracy and length of range of the

projectile. The softer metals cannot be beneficially used in the

construction of large guns, because they destroy the force of the

expellant without making any equivalent return; and the softer the metal

and the greater its substance, the more clearly is this important fact

demonstrated. Thus, in experiments made with large cannon for increasing

the weight of the gun beyond a certain proportion to that of the

projectile, a gun of ten tons weight and ten inch bore would not exceed

in range a gun of five tons, if the charge of powder were the same; on

account of the indisputable fact that much more force of the expellant

is destroyed, whilst more than double the force is absorbed for the

recoil of the ten ton than of the five ton gun; and the loss from these

two causes must materially affect the flight of the projectile, though

fired at exactly the same elevation.

The great defect which experiment shows to exist in the hoop-and-stave

wrought iron gun, and which renders the gun self-destroying, is

separation at points between the trunnions and cascable of the gun. The

force acting first upon the breech, it yields, and the force is then

brought to bear upon the longitudinal portion of the gun behind the

trunnions; the staves have thus to bear the first strain, and, after a

few shots, become elongated. An opening of the hoops at their junction

with each other (most frequently between the breech and trunnions)

begins, after a very few shots, to be distinctly visible, and increases

at every discharge, until further proceeding amounts to madness, or

recklessness of human life.

That enormous engine, Mallet’s monster mortar, of which I give an

engraving on page 100, clearly proves this to be the case. It will be

observed to be constructed with a solid cast iron breech end, the

dimensions of which will be seen by referring to the engraving. Abutting

upon this are a succession of wrought iron hoops, ingeniously inserted

into each other, and more firmly secured by six outside staves of great

dimensions, which, at the muzzle ring, pass through openings in the

muzzle ring, with heads like enormous rivets. The binding power is given

by “quoin-like” wedges, driven through the opposite end of the stave,

beneath the projection of the cast breech, giving power to tighten the

longitudinal binders by a blow when required.

[Illustration: Mallet’s Mortar.]

DIMENSIONS.

Tons. cwt. qrs. lbs.

Cast iron base with wrought iron breech shrunk

into bore 21 19 0 2

Wood carriage complete, with wrought iron screw

and spanner for elevating mortar 8 8 0 14

Bottom part of mortar to fit on top of the breech 7 5 3 23

Part of mortar (a ring) to fit on the top of the

above 5 8 3 23

Do. do. do. 3 0 2 13

Muzzle ring 1 2 3 12

Wood ring 0 0 1 0

Wrought iron ring 0 4 3 4

Wrought iron conical ring to fix on top of muzzle

ring 0 3 3 25

T-headed bolts, with gibs and keys for fixing

mortar to base: may be called outer staves 1 16 2 0

Wood-wedges, &c., for elevating 0 13 3 22

Outer pin, with cross for turning mortar round 0 8 3 14

------------------

Total weight 50 13 2 21

Weight of shell unfilled, 26 cwt. 2 qrs.; diameter, 36 inches.

This is notorious as a monster failure, even with a charge of powder

amounting to only one half what the projector fondly hoped would be

perfectly harmless in its effects. This Brobdignagian toy has proved to

be fearfully expensive, the cost having been estimated at eight thousand

pounds. It has, I believe, been the largest and most expensive

experiment indulged in by the noble “projector,”[6] and I sincerely hope

it will be the last.

[6] Lord Palmerston.

The preceding pages will have done much to remove from an unbiassed mind

any favourable impression of the advantages expected to result from the

use of wrought-iron cannon. The knowledge of this subject, even among

talented and scientific men, appears to be at a very low ebb, as is

evinced by the multitude of failures that have taken place; not one

success of any moment has as yet been attained, and not a discovery has

been made worthy of being chronicled.

* * * * *

Having enlarged thus much on the qualities of a metal which it is

certain can never supersede the use of cast-iron, even though it be

freed from the defects found practically to exist in our present

constructed iron artillery; and having also alluded to the fact that the

_form_ has much influence on the durability of cast-iron guns, I now

proceed to the more important point of the qualities of cast-iron

itself.

Little doubt exists that guns cast a hundred years ago were more durable

than those of more recent formation; it is evident, therefore, that

apart from mere form, some material depreciation must have taken place

in the quality of the metal. The use of hot blast-furnaces, better

fluxes, and improved chemical knowledge in the reduction of metallic

ores, though highly profitable in a commercial point of view, doubling

the products of our mines, and enriching their proprietors, has,

unfortunately rendered English cast-iron perfectly unfit for the

formation of cannon, if increased range and greater strain by high

elevation are to be the order of the day.

The durability of Russian cast-iron is unquestionably greater than that

manufactured in England. Some cause must exist for this; and the

question arises, is the ore superior to ours, or does the superiority of

Russian iron depend on their method of smelting? The latter is, we

believe, the cause of the superiority of Russian iron; for experiments

show that Russian ore, smelted in an English furnace, yields the same

kind of cast-iron as is produced from the ore found in England. The

inference, therefore, is plain, that the difference in the process of

smelting makes all the difference in the quality of the iron.

Two thousand years ago the Romans, or their dependents, smelted iron in

the county of Durham: vast accumulations of slag exist there at the

present time; and thousands of tons have been beneficially re-smelted by

two adjoining iron-works, and a percentage of iron obtained sufficient

to prove that the Romans were little indebted to fluxes or hot blasts

for the quality of iron they obtained. The Russians cannot boast of

these adjuncts any more than the Romans: the old agents, wood and

energy, are alone employed in the smelting of their ores; and in the

absence of scientific aids, though they obtain a much smaller aggregate

quantity of metal, yet it is undoubtedly of a much superior quality.

With the Romans, also, the yield was meagre, but the quality was good;

now, however, circumstances are reversed, quantity, not quality, being

the order of the day.

The use of coals instead of wood in the process of smelting has

introduced a mixture which is very prejudicial. Most of the coal, even

from our very best mines, contains a large quantity of pyrites, or

bisulphuret of iron, which, combining with the cast-iron, injures it to

an incalculable extent.

These facts fully explain why our cast-iron guns are not so good now as

formerly. Select the most suitable mine in the kingdom, erect a furnace

on the most improved principles, employ wood fuel only, avoid fluxes and

hot and cold blasts, and be content with the small amount of metal

produced, and beyond all doubt the quality will be all that the most

sanguine founder or artillerist could wish.

Thus the inferiority of our cast-iron guns has been accounted for, and a

method suggested, which, if efficiently carried out, would effect the

desired improvement.

* * * * *

We are indebted to Krupp for the first suggestion of, as well as the

first attempt to introduce, a cast steel gun of greater durability and

power than the best cast-iron gun which has yet been manufactured.

Steel, possessing, as it does, hardness to any desired extent, ductility

in an equal degree, tenacity unrivalled, and all the other requisites,

is destined to take the place of all other metals in the construction of

artillery. This metal waits only to be tested; and the greater the

extent to which the trial is carried, the more confident we are that it

will answer every purpose.

Krupp, like many other men with valuable ideas, has been peculiarly

unfortunate in his attempts to carry them out. With a vast amount of

knowledge of the science of metallurgy, he wants more knowledge in the

not inferior science of projectiles; the most important point being to

ascertain the form of gun calculated to be suitable for new metal, of

the use of which, for cannon, the world possesses no antecedent

knowledge.

The only failures Mr. Krupp has made (if they can, strictly speaking,

be so called), have arisen from mal-construction, imperfect form, and

unscientific combinations; defects which might be expected from a mere

novice, though not from experienced artillerists or founders of

artillery. The trial of the only steel gun sent by Mr. Krupp to this

country, was conducted in the most absurd manner, and on wholly

unscientific principles. I will endeavour to convey some idea of this

most extraordinary of experiments. Whether Mr. Krupp was unacquainted

with the durability of his metal, or was persuaded, against his will, to

conduct the experiment as he did, I know not, but the following is what

took place:--

In 1851 Mr. Krupp brought to Woolwich a specimen steel gun of ten-inch

bore, weighing about four tons. He was induced (but why, I am at a loss

to conceive,) to construct a cast-iron jacket, or outer gun, into which

his steel gun was inserted up to the trunnions. The steel gun was

separated from its cast-iron jacket by a space of half an inch in its

whole length, except at each end, where the jacket was fitted to the gun

with a moderate degree of tightness; thus the gun and jacket consisted

of two tubes, one within the other, fastened only at their extremities,

and that by a very slight force. The result, as might have been

expected, was the bursting both of the gun and its case; but that the

steel gun or its jacket would have stood the test, if subjected to it

singly, cannot be doubted. The difference of expansion between the steel

gun and its jacket would be quite enough to account for its bursting.

Had the contact of the two been perfect throughout the whole length,

but allowing half an inch all around for the expansion of the steel gun

in that part which was subjected to the greatest pressure, the very act

of restraining it in other parts so as to prevent equal expansion, would

be perfectly certain to produce a fracture. Mr. Krupp’s friends have

complained loudly of unfair treatment, whether justly or not, no opinion

need now be given; but it is much to be regretted that his experiment

was not carried out on scientific principles. The introduction of cast

steel guns will be the most essential improvement in artillery: and an

extensive series of experiments, extending over many years, during which

time I have manufactured gun-barrels of steel alone, ought to give my

opinion some weight on this subject.

Laminated steel gun-barrels were well known in 1851; but the English

bugbear, prejudice, raised a clamour against them, which was echoed by

interest and ignorance, and thus their general adoption was for a long

time prevented. However, in the short space of seven years, they have

become universally adopted, with the most beneficial results; better

shooting, less annoyance from recoil, less weight to carry, and greater

safety to the sportsman, being the principal. And so it will be with

steel cannon; as a short time will suffice to enable scientific

investigation to remove all prejudices against them.

The external form of cannon is a question of vital importance, but one

which is little understood by artillerists of the present day. Whilst it

is a demonstrable fact that all excessive bulk of cast-iron causes

weakness in proportion to the excess, no effectual steps have as yet

been taken by the Government to ascertain what is the due proportion of

metal which ought to exist in different parts of the gun. The American

authority on naval gunnery, Captain Dhalgren, has paid considerable

attention to this subject; and if the reports on the durability of

American heavy ordnance can be relied on (and there is no reason why

they should not) his investigations have been attended with much

success.

Captain Dhalgren has extended the principle acted upon many years ago by

Mr. Monck; his great improvement consisting in lessening the weight of

iron in front of the trunnions, and adding to that of the breech. In

cannon, as in fowling-pieces, weight in the fore part is useless;

conducing neither to the safety of the gun, nor to the smartness of its

shooting. For endurance, it is necessary that the expansion should be

equal in every part of the gun; rigidity in one part increasing the

strain on the immediately adjacent parts, which, if much reduced, are

thus rendered liable to fracture. The breech has to endure the

lengthened explosion produced by the burning of the gunpowder; and, as

this continues until it has overcome the inertia of the projectile, it

is necessary in all cases that the maximum of strength should be in the

breech of the gun. When the projectile is once in motion the strength of

the tube may be rapidly decreased; the only strain it has to bear is

exerted whilst the projectile is passing over it; and this strain, in

properly constructed guns, becomes of shorter and shorter duration as

the projectile attains its highest velocity at the muzzle of the gun.

The greatest strain a gun has to bear near the muzzle is that produced

by the condensation of the column of air in front of the charge; and in

almost every form of English ordnance the weight of metal here is

greater than is necessary.

The Russian guns which have been brought to this country present the

same superabundance of metal at the muzzle, whilst at the breech there

appears to be a deficiency; and when we take into consideration the

extraordinary reports of their endurance, we must ascribe it to some

other cause than the proper distribution of metal. Their endurance is no

doubt owing in part to the goodness of the metal, in part also to the

form of the breech, to the uniformity of thickness in the sides of the

arch, and, lastly, to the absence of those protuberances called

“reinforce rings.” These rings might with propriety be termed “rings of

destruction;” for wherever irregularities exist in the substance of the

metal, there the waves of vibration are interrupted, and the weak point

then becomes fractured. The science of spring-making in all its

varieties demonstrates the truth of this statement. Leave on a

coach-spring an abutment of metal like a “reinforce ring,” and a few

motions will be sufficient to break it, however well the spring may be

constructed in every other part. The rigidity of this protuberance, by

interrupting the waves of vibration, causes additional vibration in the

adjacent and more yielding part, and thus produces fracture. The same

thing occurs in all ill-constructed artillery: where the vibrations are

checked, there is always a danger of some weaker part giving way. But

the laws which regulate the distribution of vibrations in metal

substances are not yet understood by artillerists, or cannon would be

differently constructed. Those unscientific protuberances called

“trunnions,” which are to be seen in almost every description of gun,

prove the accuracy of my assertions. These protuberances, if

scientifically considered, would soon be discarded, since they tend not

only to the rapid destruction of the cannon, but also exert a most

injurious influence on the direction of the projectile. The most

wonderful shooting ever heard of (and which has been before alluded to)

is partly to be attributed to the absence of trunnions. Trunnions act as

the fulcrum of a scale-beam; they allow the breech and muzzle of the gun

to oscillate, but in an opposite direction to a scale beam. Rifled

cannon can never be correctly constructed whilst any weight impinges on

the gun in front of the first starting point of the projectile; they

must have the fulcrum behind the point of discharge, and the more nearly

in a direct line the better.

Rifled cannon will in some few years be perfectly constructed of cast

steel; the projectile being made of gun metal, _i. e._, ninety-five

parts of copper to five parts of tin, or of lead and its alloys, and at

a probable cost of ten times that of a cast-iron projectile of equal

weight.

Rifled cannon must be elevated by raising the muzzle; no depression of

the breech must occur as by the usual elevating screw; and the recoil

must be received and borne by fastenings and axle in rear of the breech

only. Trunnions and all impinging influences are incompatible with

correctness of fire. The muzzle must be raised in a similar manner to

the raising of a hand rifle, the recoil being thrown backwards, in as

direct a line as possible with that of the shot.

It is only on account of the difficulty of experimenting with rifled

cannon that they are at all behind rifled muskets in point of

perfection. The ardent lover of science is appalled when an experiment

costs hundreds of pounds. We have not a General Jacob everywhere who can

afford to spend a thousand or two in experiments; but, nevertheless, the

lover of science, could he experiment, might attain such extraordinary

accuracy of range, as to blow up a smaller magazine than that of

Kurrachee at four times the distance; and that, too, with a more certain

effect, though with a projectile heavier than several of Jacob’s rifles

tied together. Correct direction is certain in proportion to the

increase of weight; deflection being in the minimum with the heavier

weight, from the well known law of momentum. That astute and energetic

sovereign, the Emperor Napoleon, is pursuing experiments with rifled

cannon; with what result there can be little doubt.

It must be by the use of rifled cannon that our artillery will regain

the place it has lost. A short time will suffice to make the disparity

between our artillery and small arms as great as when we were content

with the six-pounder field gun and old “Brown Bess.” Ranges will only be

ruled by sight, and objects will be hit eventually with as much ease at

5,000 yards as they now are at 1,000. Steel, rifled cannon, and

projectiles of gun-metal will assuredly bring about as complete a

revolution in artillery as the Greenerian rifle and bullet have effected

in small arms.

The form of gun best suited for all purposes has yet to be determined;

and we have pointed out these defects in our artillery with the hope

that some of the great practical philosophers of the present age may

devote themselves to the study of this question. It is nearly allied to

the science of bell-making, and a few more fractures of Big Ben will

extend our knowledge of the subject, and produce a remedy which lies not

very deep below the surface. The laws which should guide us in the

construction of cast steel guns, so as to insure their durability, are

very analogous to those which determine the durability of bells; for the

laws which regulate disintegration of crystalline structures are very

similar. Hitherto the rule of thumb has, unfortunately, been the only

rule observed in measuring out the quantity of metal which shall

surround that portion of a cannon which has to sustain the most violent

concussion.

Professor Barlow many years ago proved, to the satisfaction of the

Institution of Civil Engineers, that the metal in any cylinder decreases

in utility in proportion to the square of its distance from the centre:

that the outside of a gun of the form now used, in fact, is only

one-ninth as useful as the inside; being three times as far from the

centre. If we double the thickness, the outside, being five times as far

from the centre as the inside, will be but one-twenty-fifth as useful;

or in plain English, nearly useless. The reason of this is simple, and I

will endeavour to explain it.

“A bar of cast iron one inch thick each way and 40 inches long will

stretch about one-twentieth of an inch, if a weight of about four tons

be suspended by it. When the weight is removed, the cast iron nearly

recovers its previous form, and is uninjured; but if it be stretched

more, by a greater weight, it is permanently injured.

“A bar of the same thickness, but three times as long--120 inches--will

stretch three times as much, or three-twentieths of an inch, with the

same weight; or if only one-third the weight--one ton and a third--be

suspended, it will stretch one-twentieth of an inch, the same as the

shorter bar.

“If we suspend 16 tons by four bars, one inch thick and 40 inches long,

they will each stretch one-twentieth of an inch only, and remain

uninjured; but if we attempt to do so with two bars 40 inches long and

two 120 inches long, then, when the whole have lengthened one-twentieth

of an inch, the short ones are exerting a force of eight tons, but the

long ones that of only two and two-thirds tons. The weight, therefore,

will still further lengthen the bars, and permanently injure the short

ones; perhaps break them first, and then the long ones.

“This is the way a gun is burst. The inside is a series of bars of iron,

say 40 inches long, in the form of a ring; the outside a series of

rings, representing the bars three times as long.”

Warfare, since the first introduction of gunnery into Europe, has been

like one continued series of experiments for testing the efficacy of our

guns. No description of gun we now possess can lay any claim to

existence fifty years ago: the great majority of our guns now in use are

of a much more recent date.

With one or two exceptions, no artillery has been constructed on any

scientific theory; some alteration has been made, and if a gun of a

certain form and dimensions gave a certain result, then an extension or

emulation of that gun was tried; and if it succeeded a loud cry of

exultation was raised, and the discovery was announced to the world as a

great improvement.

[Illustration: Russian 56-pounder gun.]

[Illustration: 8-inch British gun.]

Colonel Prejudice has invented a vastly improved description of gun;

another guess is made, and so different forms of guns are multiplied.

Can there be a more striking illustration of this than the one which

took place during the late Crimean war? It was boasted that the whole

human race might be exterminated by the new invention; but the

“Lancaster gun” turned out to be most unscientific in its construction,

and most eccentric in its action. Had such a thing as scientific

knowledge in gunnery existed among the artillerists of the day, such a

monstrosity would have been buried soon after its birth; instead of

being allowed to squander large sums of money at every discharge, and

then at last to become a “Whistling Jemmy” for our bluejackets to laugh

at.

The form of cannon no doubt exercises a vital influence over their

durability; bad form and imperfection of material combined, tended to

produce the rapid destruction of our guns during the late important

struggle.

The gun which has been experimented with to the greatest extent, and

which has withstood all trials successfully, is a Russian

fifty-six-pounder; taken, I believe, at Bomarsund. In this gun there are

two great peculiarities; the shape, as will be seen in the diagram,

differs from all our own guns: it is a “chambered gun,” and the metal is

taken away from the outside precisely as the contraction increases on

the inside thus giving an equal thickness of metal in every part, of the

arc (see page 114).

In contrast with this, we give a cut of our 8-inch gun, which most

nearly resembles it as a chambered gun (see page 114).

The reader’s attention is especially directed to the dissimilarity in

the distribution of the metal in the two guns. The want of uniform

thickness of metal in our 8-inch gun must be sufficient to convince any

one that, if the Russian gun be properly constructed, the principle of

ours must be radically wrong. That such is the case, indeed, I cannot

doubt, the Russian gun having undergone such a test as would have

destroyed six of ours. The gun has since been made two inches larger in

the bore, and even oval-bored, for firing shells, which should alone be

enough to destroy it; and yet with all this the gun remains perfect.

The gun which most nearly resembles this is our English carronade; and

that these guns have some important principle in their shape is proved

by their great durability under all trials; and I believe that the tests

to which the carronade has been subjected have been more severe than

that of any other piece in the British service.

There have been many shrewd conjectures as to the cause of this

durability; one of these was very pungent, viz., “the invention was not

by one of the cloth.” An examination of the drawing of the 68-pounder

carronade will enable the reader to perceive the great similarity

between this and the Russian gun before spoken of (see page 114).

[Illustration: 68-pound carronade.]

The manufacture of these guns was originally in the hands of the

inventors, and it is quite evident that they must have taken great pains

with the form of the gun, and also have taken special care that the

material of which it was constructed was of the very best quality.

There is too much reason to doubt the proficiency of military men in

the science of metallurgy; and the British system of depending solely on

their knowledge for the last half century, has no doubt proved an

obstacle to advancement in the science of gunnery.

[Illustration: Monck’s 56-pounder gun.]

The gun which ranks next is Monck’s 56-pounder. Although not a chambered

gun, it will be seen, from the diagram (see p. 117), to be an attempt

(if not a perfectly successful one) to obtain uniformity of thickness in

every part of the arc. The durability of these guns ranks as we have

placed them.

The next in rotation is the 8-inch or 68-pounder (see p. 114); which,

although not the original sized gun that was rifled for the Lancaster

shell, yet it was the one eventually used for that projectile up to the

end of its very brief career.

[Illustration: 10-inch or 86-pounder gun.]

The 10-inch gun of 95 cwt., delineated at page 117, will be seen to be

defective in its outlines when tested by the principles before laid

down, and the fact of more 10-inch guns bursting at Sebastopol than any

others (mortars only excepted), may be taken as exclusive evidence of

its imperfection.

The bursting of mortars is quite notorious, especially the 13-inch

mortars used for sea-service in the attack on Sweaborg. A slight

examination of the engraving of one will be sufficient to convince any

person that, if what has already been advanced on the form of guns can

lay claim to being scientific, then this is of all guns the most

unscientific that was ever manufactured. Its durability, too, like its

shape, is of a very low order.

[Illustration: 13-inch sea-service mortar.]

The 13-inch land mortar depicted below is a much more serviceable

production, because it contains much less metal.

[Illustration: 13-inch land-service mortar.]

Mortars will retain their place in spite of all improvements. Rifling is

inapplicable to them. Their principal utility consists in obtaining a

vertical fire; the shell being pitched to a great height, so as to fall

into places that cannot be assailed by a horizontal fire.

The late Joseph Manton has the merit of being the first modern inventor

of rifled cannon. His idea was, that if a motion on an axis parallel to

the horizon could be given to cannon balls, they would range farther and

with greater accuracy. As there exists great difficulty in causing the

rifling in a gun to act upon an iron ball, he constructed a cup of wood,

into which the ball was fitted, projections being made upon the wood to

fit into the groves of the rifle; the spinning motion thus being

communicated to the ball by its wooden adjunct. The result was twofold;

for the expansions of the wood during the explosion, filled the tube of

the gun tight, and effectually destroyed the windage. The government of

the day did offer him a premium of one farthing each; but “Joe”

over-reached himself, asking the sum of £30,000 down; this was refused,

and the patent was allowed to expire without the Government taking any

advantage of it, and experiments ceased to be made in this direction.

Rifled cannon have now, however, become a certainty. Mechanically

speaking, they are as easily to be produced as hand rifles. The general

application has, however, vast difficulties, which must be overcome

before their use can become general. Small arm projectiles suitable for

rifles must of necessity be made of ductile metal, and all the attempts

previously made, whether with brass or iron guns, are alike useless. The

mass in motion, even when of equal hardness with the gun (as in the case

of cast iron guns and cast iron shot), invariably destroys that in a

comparative state of rest; and the rifling is obliterated after a very

few discharges. In a brass gun the destruction is certainly not so

rapid, on account of the different nature of the metal; yet the

destruction of the gun for all useful purposes is equally effectual. It

is evident, then, that success cannot be obtained by using the present

materials in rifled cannon; and the question inevitably arises, what

better material can we use? Wrought iron shells have already been

thoroughly tried in the Lancaster oval gun, with a well-known result.

Great hopes were at one time entertained, that something suitable would

result from Mr. Bessemer’s discovery of the combustion of carbon, and

that an iron of sufficient ductility, yet without the usual hardness,

would be produced; but this, it appears, is still a myth.

Extent of range and accuracy of fire in gunnery will in future be of so

much importance in war, that it is not extravagant to assert, that in

contests between well-matched belligerents, the precious metals (if they

gave any advantage to the user) would be unhesitatingly used in

projectiles. But on the score of economy, science need not be impeded.

Gun-metal projectiles and cast steel cannon would work as effectually

together as lead and iron in small arms.

Some other mixtures less expensive might be produced (lead and copper in

certain proportions are very ductile), and at the same time sufficiently

strong to resist all tendency to squash; as the softer metals would

inevitably do. The more ductile metals are limited in their utility, by

the same law which limits the use of pure lead: that is, to given

weight, height of column, or velocity. Great doubt exists whether a

bullet made of gun metal, and of the same proportionate dimensions and

form as an Enfield bullet, but fitted for a ten-inch gun, would not, if

fired with the proportionate charge of powder (namely, seventeen

pounds), be as completely squashed, or driven in upon itself, as the

Enfield bullet if fired with the old Brown Bess charge of four drachms

and a half.

Considerable time and experience will be required to ascertain the

proportions of metallic mixture necessary to meet all contingencies;

this, however, is a matter of detail, and must extend over so large an

area, that it can be handled only by the government officials, with the

necessary “sinews” of experiment. Nevertheless it must be undertaken;

and the sooner it is done the better, for the prestige of that nation

which would lead the van of improvement in gunnery, and increase its

power of attack and defence beyond those of its rivals.

Rifled cannon is a generic term of endless application, presenting to

the mind modifications of projectiles in endless variety, ranging from

the “_light firebrand_” to the twice deadly rocket: not rockets of that

eccentric and erratic character by which Congreve made an undying name;

but real _bonâ fide_ rifle rockets, which shall hit the dead-lights in

the quarter-gallery of a frigate, carry away the halyards of your

enemies’ ensign (making him drop his colours at the first shot) or dash

the glass from the hand of the pilot. All such imaginary feats will yet

be accomplished; though the reader may smile at the idea. My experience

with rockets goes to justify me in asserting that rockets discharged

from a gun, under certain circumstances, can be as effectually

controlled, and kept to a direct course, as a bullet fired from a rifle.

The rocket, however, may be fired a much greater distance than we have

ever been able to project a bullet; because, in addition to the force

which projects it from the gun, its flight is maintained by the self

sustaining agency in the body of the rocket. Rockets require a much

smaller charge of powder to project them than that which is used for a

bullet; a rocket started by its own force, expends, in acquiring even an

approximation to its highest velocity, at least one-third of the force

with which it is charged; but when projected by a small charge of

gunpowder this force is saved, and the flight of the rocket is

afterwards sustained by the force with which it is charged.

Firing rockets from cannon can only be practised under certain

circumstances. The observations already made on the granulation of

gunpowder will have prepared the reader for this announcement. When

fired from a cannon under the old régime, the rocket was projected at

high velocity, and the case of the rocket was destroyed by the very

force which set it in motion. A rocket suitable for artillery should be

cast of gun metal, with a frame of considerable strength. In form it

should nearly approximate to an expansive bullet; but, instead of the

limited length of one and three quarters diameter; it should approach to

four diameters; two of which, at least, should be appropriated to the

cylinder behind the head.

The head is charged with composition more densely driven than is

customary in the ordinary rocket; the tubes in the cylinder are also

charged with a composition equally dense. The outer frame of the rocket

is cast with suitable projections to fit the grooves of the gun: the

spiral of these grooves is considerable, being one turn in every three

feet, in order to impart to the rocket an effectual spinning motion when

in a low state of velocity. The rocket properly constructed is then

placed in the rocket-gun, and fired in the usual way; but it is

essential that the gunpowder used should be of a suitable quality: its

combustion must be as slow as possible, a starting velocity of from 500

to 800 feet per second being sufficient to ensure the flight of the

self-sustaining projectile to the end of its range. This principle may

be extended from a light firebrand, as already stated, to that of a

rocket charged in the head with the most deadly and destructive

fulminate.

It may appear absurd to speak of fulminates being projected; since all

experiments show that fulminates, even when adulterated, will not stand

the concussion of a discharge, but invariably ignite in the gun, however

carefully placed or packed in the shell which contains them: for this

reason fulminates have never been successfully used. But if the

fulminate is placed in the head of a rocket, this objection may be

obviated. The gradual manner in which velocity is given to a rocket does

not subject it to violent displacement during its flight; neither need

the concussion in the gun be severe, owing to the nature of the

gunpowder used, which in its gradual expansion is analogous to steam:

thus the field for the application of fulminates is opened to an

unlimited extent.

My own experience on this subject has been limited to its application

for the saving of life from shipwreck, where the application of a line

to the rocket limits its range and velocity; but sufficient is left in a

rocket of an inch and a half diameter effectually to carry out a line of

a quarter of an inch diameter to a distance of 600 or 800 yards: that

is, more than double the distance obtained by either Manby’s apparatus

or the rockets now in use; which, lamentable to state, are quite

inadequate to the purposes for which they are intended.

Though the improvements in rifled cannon are at present only in their

infancy, they have nevertheless attained to an extraordinary degree of

perfection, verifying all our predictions to the letter.

A writer in the _Times_ makes the following statements in favour of Mr.

Whitworth’s improvements:--

“While some men of really inventive talent, and a great many charlatans,

have been permitted to waste the public money in trying vainly to

improve our artillery, it seems passing strange that it should not long

ago have been discovered how impossible it was to hope for successful

results in the direction in which they were working. It was clear that

while increased range and precision of firing were wanted, it was nearly

as important to bring the charges of ammunition and the weight of metal

in guns into more manageable proportions to each other, and to the

facilities for transit on active service. No sensible man can have

witnessed the frightful damage done to the efficiency of our army in the

Crimea by the exigencies of the siege-train during the winter of 1854-5

without being impressed with this conviction. The principle of the rifle

offered an obvious suggestion for the proper means of working out the

foregoing problem; but then for artillery, rifling by grooves would not

do without the use of a pliant metal in the projectile, and the cost of

lead rendered its application to that purpose impracticable. It was

necessary, therefore, to alter the existing mode of rifling, and to

modify the bore of the cannon, so that an iron projectile could be

discharged from it, rotating on its own axis in the line of flight. This

result once secured, it is obvious that a field-piece or gun of position

would become a rifle on a large scale, and that the same immense

increase of range and of penetration which had been realised by the

smaller weapon as compared with Brown Bess, would be placed at the

command of the artillery service. It is consolatory, after a series of

failures worthy even of Brunel in launching the _Leviathan_, that the

country has at last the well-grounded hope of an improvement by which

our ordnance may be placed on a proper footing. In pursuing those

careful experiments which he undertook for the Government, principally

to improve the rifle, Mr. Whitworth, the eminent machinist, adopted a

polygonal spiral bore of a uniform pitch, but more rapid than could be

attained by grooves. This bore has enabled him to surpass immensely the

range and penetration of the Enfield rifle; but even these advantages,

important as they are, scarcely surpass those which it places within the

reach of our artillery service. The strain of the projectile being

distributed evenly over every side of the polygon, iron can be

substituted for lead in the projectile, and this simple but beautiful

mechanical appliance at once becomes available for cannon.”

The powerful aid of the _Times_ is “almost success;” though in this

instance it has signally failed, the boasted accuracy there spoken of

not having been yet obtained. This has no doubt arisen in part from the

fact that Mr. Whitworth’s great mechanical knowledge would not suffice

to make him _au fait_ at the compound science of gunnery. His “polygonal

spiral bore of uniform pitch, more rapid than could be obtained by

grooves,” is after all only an experimental gun, not sufficiently

developed as yet for practical utility. Still, the writer already

alluded to has favoured us with the following remarks in the _Times_:

“Moreover, Mr. Whitworth has discovered in the course of his

experiments, that according to the quickness of the turn in the polygon

is the length of the projectile that may be fired; so that 24 lb. and

48 lb. shot have been sent to extraordinary ranges with half the usual

charge of powder, from an ordinary 12-pounder howitzer. Here, then, is

at once the solution of the whole question which has troubled the brains

of so many inventors, real or pretended, for years. The artilleryman at

one stride resumes the relative position to the soldier of the line

which the Enfield rifle had so perilously deprived him of, and this

mechanical country, after finding herself on the level of France,

Russia, and other European States, is once more, as during the

Peninsular campaigns, enabled to assert her natural superiority in the

manufacture of cannon. We trust that no petty jealousies on the part of

narrow-minded officials will be allowed to interfere with the course of

Mr. Whitworth’s experiments, and that the encouragement which he is now

receiving from the Minister at War and the Commander-in-Chief will

enable him, at no remote date, to realise for the benefit of the army

and the nation that revolution in gunnery which the results already

obtained by him promise.”

Report says that 25,000_l._ is the amount of encouragement Mr. Whitworth

has received from the Minister of War and the Commander-in-Chief; an

adequate sum with which to conduct such an experiment, but not

sufficient to insure success.

Of the success of Mr. Whitworth’s polygonal projectile, on a large

scale, none need speculate, for the principle is self-destructive.

Lancaster’s oval shell, oscillated in its flight, took a flight so

extraordinary, on account of the resistance of the atmosphere on the

protuberances of the oval, that the principle may be regarded as fully

established that enlarged projectiles must be smooth and free from

projections that “saw the air,” otherwise range and accuracy of fire

will be sacrificed. The principle of Mr. Whitworth’s polygonal bore is

fully discussed in its proper place, and will here receive only a

passing notice.

To Mr. W. G. Armstrong, of Newcastle-upon-Tyne, much more credit is due

than can be claimed for Mr. Whitworth. Long before the paid efforts of

Mr. Whitworth, Mr. Armstrong had made the subject of rifled cannon a

special study, and the success of his investigations has been such as to

couple his name with those of the earliest inventors of effectual rifled

cannon. Mr. Armstrong may also lay claim to being an originator of

wrought steel cannon; though here his name stands second as an inventor,

for to Mr. Krupp is due the honour of first introducing cast steel

cannon to the notice of our Government.

Mr. Armstrong tells his own tale so well in the columns of the _Times_

that we cannot do better than quote it:--

“In the latter part of 1854, I submitted to the Duke of Newcastle, then

Minister at War, a proposal for a gun which I anticipated would possess

great superiority over the common forms of light artillery, and I

undertook, with his Grace’s authority, to construct a field-piece in

conformity with the plan I had suggested. The gun was accordingly soon

afterwards made, and has since, during a period of nearly two years,

been the subject of numerous experiments, partly upon the ordnance

firing-ground at Shoeburyness; but principally under my own direction in

this neighbourhood.

“I have hitherto avoided publicity in reference to these experiments,

but, as matured results of much interest and importance have now been

arrived at, and as other names are already before the public in

connection with gun experiments made during the same period, I feel that

I may now, without impropriety, give some information on the subject.

“With a view to strength and durability, the gun is composed internally

of steel and externally of wrought iron, applied in a twisted or spiral

form, as in a musket or fowling-piece. The bore is nearly two inches in

diameter, and is rifled. The projectile is a pointed cylinder 6-1/2

inches long, and its weight is 5 lb. It is made of cast iron, coated

with lead, and is fired from the gun with a charge of 10 ounces of

powder; it contains a small cavity in the centre, and may be used either

as a shot or a shell. When applied as a shell, the cavity is filled with

powder, and a detonating fuse is inserted in front, so as to fire the

powder in the centre on striking an object. When used as a shot, the

powder is omitted, and an iron point, which favours penetration, is

substituted for the fuse. The gun is constructed to load at the breech,

the object being not only to obviate the disadvantages of sponging and

loading from the front, but also to allow the projectile to be larger in

diameter than would enter at the muzzle, and thus to insure its taking

the impress of the grooves and completely filling the bore. The piece

weighs 5 cwt., and is mounted upon a carriage which bears a general

resemblance to that of an ordinary 6-pounder field gun, but which

embraces a pivot frame and recoil slide. A screw is also applied, not

only for elevating and depressing the gun, but also for moving it

horizontally, by which means great delicacy of aim is effected. The

recoil slide has an upward inclination, which enables the gun, after

running back, to recover its position by gravity; and its use is to

relieve the pivot-frame and adjusting screws from injurious concussion.

“I shall now give some particulars of the experiments recently made with

this gun on the coast of Northumberland, near the village of Whitley,

under the official inspection of Colonel Wilmot.

“Fourteen shots were in the first instance fired from a distance of

1,500 yards at a timber butt, 5 ft. wide 7-1/2 ft. high. Six of these

were expended in finding the elevation proper for the distance, but

after that was determined every succeeding shot hit the object without

previous graze. The final elevation of the gun was 4 deg. 26 min., and

the mean lateral distance of the shot-marks from a vertical line through

the centre of the butt was only 11-1/2 in.

“Persons who are conversant with artillery practice will be able to

appreciate the accuracy of this firing; but, for the information of

those who are unacquainted with the subject, I may state that the

ordinary 6-pounder field-piece, which in point of weight forms the

nearest approach to the present gun, is perfectly useless at a distance

of 1,500 yards, and is very uncertain even at 1,000 yards. It is only,

therefore, with heavy artillery that a comparison can be drawn; and it

will be sufficient to state that in tabulating the practice made with

such ordnance the deflections are invariably recorded in yards, whereas

with this rifled gun they can only be properly given in inches.

“With respect to penetration, the following particulars will be regarded

as equally remarkable, considering the small weight of the shot and the

length of the range. The butt was 3 ft. thick, and was composed of six

layers of rock elm bolted together, so as to form a solid block. One

shot passed entirely through; another struck near the edge and glanced;

and the remaining six penetrated within a few inches of the opposite

side.

“Shell firing was next tried at a distance of 1,500 yards; the gun being

fired at the same elevation and with the same charge as in the previous

practice at the butt.

“In this case two targets were erected, one behind the other, so as to

appear as one object when viewed from the gun, and a space of 30 feet

was left between them. The front target was intended to exhibit the

perforations of the shell before bursting, and the back one to show the

effect of the fragments resulting from explosion.

“After some preliminary experiments twenty-two shells were fired at the

front target, and of these only one missed the object of aim. The

following are the particulars:--Seventeen hit the first target direct,

and burst behind it, the fragments penetrating the second one; three

grazed and burst immediately in front of the first target, and

perforated both with the pieces; one hit the bottom of the first target

and exploded in the ground, and the remaining one missed entirely and

burst on some rocks nearly on line beyond. A strong side wind was

blowing at the time, and accounted for the deviation of this single

shell.

“Four shells and three shots were then fired at an elevation of 6

degrees, from a distance of 2,000, or, more accurately, 1,964 yards. All

these struck within the breadth of the target; but the elevation being

scarcely sufficient, they all fell a little short, except one shell,

which, ranging somewhat further than the others, hit the target and

burst as usual.

“The results of this shell-firing were as follows:--The front target

contained 51 holes, and the back one 164, while the ground between and

adjacent to the targets exhibited about 70 perforations by fragments of

shells, the greater portion of which were afterwards recovered by

digging.

“With respect to ranges exceeding 2,000 yards, I may state that on

previous occasions the gun had been tried up to 3,000 yards--a distance

which was reached with an elevation of 11 deg., and the usual charge of

10 ounces of powder, or 1-8th the weight of the projectile. By

augmenting the charge the range is increased, but the accuracy is

impaired; and I therefore adhere to the 10-ounce charge, which gives

ample penetration, as the experiments at the butt will testify. I may

also observe that the ranges obtained with this charge bear a favourable

comparison with those of the heaviest round-shot guns fired with a much

larger proportion of powder.

“It is a curious fact, and one which greatly increases the efficiency of

the shells, that owing to the bursting charge requiring a minute space

of time to mature its ignition after the firing of the fuse by impact,

the shell is enabled to travel four or five feet after striking an

object before disruption takes place. Hence, therefore, it acts as a

shot before it bursts as a shell. When it perforates a target the

explosion may be seen to take place at a few feet beyond, and when it

grazes it has time to rise, and may be observed to burst after clearing

the ground. If, therefore, it were fired against a ship, it would first

penetrate the side in its entirety, and then, bursting, traverse the

deck in fragments; or if directed against troops, it would pierce the

front line as a bullet, and operate like grape-shot beyond. The shells

explode with equal certainty whether the first substance struck be hard

or soft; and, in fact, they even burst on the surface of water, provided

the elevation of the gun be not too great. The bursting charge is very

small, but it suffices to break the shell into about 30 pieces, which

pursue their forward course without too much dispersion.

“It is impossible to contemplate the results obtained with this gun

without being impressed with the important part it is calculated to

perform in warfare. Opposed to any ordinary field-piece, it would be

like the Greener rifle against the old musket; and no gun could be

worked at an embrasure if a fire of shells were directed against it by

one of these rifled pieces placed within the distance of a mile. In

naval operations, also, guns of this description, but of larger size,

might apparently be applied with great effect--more especially as a

system of breech loading, combined with a self-recovering recoil action,

would be peculiarly advantageous in firing from portholes. Even light

5-pounders, sending their shells from great distances through the sides

of a ship and sweeping the decks with fragments of lead and iron, would

produce very destructive effects; and a small swift steamer carrying a

few such guns might prove a very troublesome opponent to a large ship of

war. But if the dimensions of the gun were increased so as to adapt it

for shells of 20 lb. or 30 lb., still more terrible injury could be

inflicted at greater distances; and the ponderous artillery now used at

sea would be of little service when opposed to the accurate and

long-range firing of such rifled shell-guns.”

Since the publication of these remarks, rifled artillery of Mr.

Armstrong’s production has, we believe, been extensively tried. The

results of these trials have been most extraordinary; and the principle

is, we believe, identical with the expansive principle bearing my

cognomen: an extension of the principle of the Greener and Enfield

rifle, hereafter to be described. I have had the honour of being

consulted both by English and foreign authorities, and I have assisted

in constructing rifled artillery for several years; and the experience

thus obtained justifies me in making known to the world some of my

observations on this subject.

Rifled cannon with elongated projectiles, similar in shape and principle

to the Greenerian bullet, give, with charges inferior to those of the

old régime and calibre, more than double the range, with ten times

greater accuracy.

Now, either of these points, if gained, would be most important

improvements, and when combined would produce the most extraordinary

results. But this is not all: a great diminution in the weight of the

gun might also be effected; and these advantages may be still further

extended when we have had time to increase our knowledge of the valuable

materials with which we are only just now becoming acquainted.

The following table will show the advantages to be gained both in length

and accuracy of range.

Before reverting to the table, it may be necessary to remind the reader

that the great reduction in the weight of guns arises from the adoption

of the elongated projectile. For example: the diameter of the

_elongated_ projectile for an “18-pounder” is much less than the

diameter of the gun for the _spherical_ 18-pounder; thus allowing the

thickness of metal to be equal in both guns. The gun for the elongated

projectile may be greatly reduced in weight without at all diminishing

its strength, simply on account of the great diminution in the diameter

of the arc.

There is another important fact, which Mr. Whitworth, with all his

boasting, has carefully concealed: viz., that a much greater pressure is

exerted upon the square inch in the lesser than in the larger diameter

of bore; and to conceal this fact, whilst claiming merit for a bullet of

50-gauge exceeding in range one of 25-gauge, the charge of gunpowder

being alike in both cases, appears very like deception. Any engineer

will tell us that the pressure in the lesser is twice as great as in the

larger bore; and this explains why greater velocity is given to the

projectile.

With these explanations the reader will be better prepared to weigh

carefully my observations. My task would, doubtless, have been rendered

more easy, if a clear elucidation of the principles of the expansive

bullet could have been given thus early in the work; but it is thought

better to do this in its proper place. I will only add here, that

although two bullets, one elongated, the other spherical, and of equal

diameter, meet with the same amount of atmospheric resistance, yet the

one containing twice as much matter as the other retains its medium

velocity nearly double the distance. With these explanatory remarks I

give the following table:--

------------------+-------------+-------+--------------+----------

|Present Range|Present|Reduced Weight|Range when

|of Guns. |Weight.|when Rifled. |Rifled.

------------------+-------------+-------+--------------+----------

6-pndr. | 1,500 yds. | 17 | 12 cwts. |3,000 yds.

9-pndr. | 1,600 „ | 26 | 18 „ |4,000 „

12-pndr. | 1,700 „ | 34 | 22 „ |4,500 „

18-pndr. | 1,780 „ | 42 | 29 „ |5,000 „

24-pndr. | 1,850 „ | 50 | 34 „ |5,500 „

32-pndr. | 2,000 „ | 63 | 42 „ |6,000 „

48-pndr. | 2,500 „ | 70 | 45 „ |6,500 „

56-pndr. | 5,000 „ | 85 | 60 „ |8,000 „

68-pndr. or 8-in. | 4,500 „ | 85 | 60 „ |8,000 „

86-pndr. or 10-in.| 4,700 „ | 95 | 65 „ |9,000 „

------------------+-------------+-------+--------------+----------

The reader must understand that all the guns given in this table were

not rifled, and that they have not all been subjected to trial. The 6,

12, 18, 24, and 48-pounders have been tried, with the results given

above; but the heavier guns have not as yet been tested: the ranges and

weights given in the table have, however, been derived from the results

yielded in the trial of the lesser guns, and may be safely relied on as

scientific data; being, in truth, rather under than over the mark.

All experiments clearly establish one very important principle, long

known to those acquainted with the science of projectiles, viz., “That

the heavier the projectile, the less the deflection.” Thus it is quite

possible that the longest ranges may ultimately be obtained without any

perceptible deflection. And when we observe that the deflection of an

ordinary 32-shot in a range of 2,000 yards, is 50 feet, and in 2,500

yards, 80 feet, whilst the elongated shot, at a much greater distance,

is not deflected half as many inches, I think we may fairly say that our

knowledge of gunnery is yet in its infancy. Fulminating powder may be

used as an auxiliary in shells for various important purposes; such, for

instance, as destroying an entire fleet; and it is clearly within the

range of possibility that by its agency the largest ship may be

destroyed by a single shot. The accuracy of rifled cannon renders it an

easy task to strike a plank only one inch above the water line, and the

penetration of an elongated gun-metal or lead-alloyed shell would enable

us to reach the innermost parts of the magazine: for it is scarcely

possible to produce even an iron casing which shall resist the power of

such projectiles. It is possible, therefore, that we may see the noblest

fleet destroyed in a few minutes by the agency of such projectiles.

I will endeavour to give an outline of the method by which this may be

effected. A long rifled cannon, constructed for an elongated gun-metal

shell; of from fifty-six to eighty-six pounds, and with an extreme range

of from 6,000 to 7,000 yards, may be considered to be a suitable

instrument. This shell should be charged in the head with a given

quantity of the fulminate, such as would be most calculated to prevent

the tendency to explode from the concussion produced by the discharge of

the gun. It will be necessary to place the fulminate in thin layers

between sheets of prepared caoutchouc, or some other preparation of

India-rubber; having thus arranged the fulminate in the head of the

shell and secured it there, the usual method of filling the remainder is

resorted to, and the aperture is securely screwed up: fuses not being

necessary in this arrangement.

The difficulty in using this shell is to prevent its explosion when the

gun is discharged; and to obviate this all our engineering skill is

required. Time and experience will show that, by a modification of the

propelling agent, the shell may be started from a rifled cannon at a

very low velocity; the velocity being increased like that of the rocket.

This is to be done by modifying the arrangement of the gunpowder so as

to ensure the shell acquiring its greatest velocity as it leaves the

muzzle of the cannon. The result of this has been already shown. On the

shell striking any object, such as the ship’s side, the metal of the

shell is driven in upon itself, and an explosion of the fulminate

follows as a natural consequence. Experiment has proved that shells

exploding as they strike the ship’s sides, produce very little damage

beyond making a hole in the ship the size of the shell. This, no doubt,

arises from the short space of time occupied by the shell in passing

through the side of the ship; all its force being exerted in the

interior instead of on the sides of the vessel. All shells of the nature

alluded to would, at certain distances, take such a line of flight as to

ensure them dipping towards the centre of gravity, and thus exploding

the magazines, however deep below the water-line; and when we consider

the destructive effects of fulminates, we think it quite within the

range of probability that they might produce all the effects we have

spoken of.

There are many agents equally powerful to be introduced into destructive

warfare; and with the advantages to be derived from improvements in

rifled shells, which the ingenuity of the present race will certainly

effect, he would be a rash man who would set any limits to the

advancement of projectile science. The great difficulty in the use of

fulminates will be surmounted if these suggestions can be carried out;

and experiment is all that will then be necessary to establish the line

of proceeding. To effect this is the province of the Government of the

country; to wait for it to be perfected by individual skill and

enterprise would be unjust to science, and injurious to the best

interests of the nation. The needful expenditure can only be borne by

the nation, and should be entered upon, in order to effect improvement

in projectiles, with the view of maintaining our land and marine

artillery at the highest point of efficiency.

There is one question of great importance to inventors, and to which I

have paid much attention, namely, the obtaining a spiral motion in a

projectile which has been fired from a smooth bored gun. All we have

witnessed goes far to prove that the attainment of this is impossible,

in consequence of a principle not hitherto investigated by inventors. If

the course of a projectile is changed from the straight to the spiral,

it can only be done at the expense of range; and that for the following

reasons: first, the force which is necessary to induce this spiral

movement must be exerted at the expense of the force which propels it

forward; secondly, when this spiral movement is acquired, it is so much

in excess of the direct movement, that after advancing a certain

distance it falls to the ground. A very simple experiment will prove

this. Take an ordinary tin tube, cut a bullet of an elongated

form--cylindro-conical if wished--having grooves from the point

backwards, with the degree of spiral necessary to effect the object in

view. Let the bullet be made of cork or light wood, such as can be

projected by a blast from the mouth, and the result will be that the

projectile will go one-half the distance before the friction of the

atmosphere produces a motion on its axis parallel to its line of

flight; from this point it gradually loses its velocity in a forward

direction, it spins until its force is expended, and then falls

vertically to the ground. To find the sequel, try the same experiment

without grooving, and the range, with the same force, will be found to

be double. Some years ago I witnessed such a trial with a 32-pounder;

and, to the astonishment of all present, the bullet rose above the

horizontal line, and then fell to the ground, like the cork bullet of

which we have already spoken.

The endeavour to produce breech-loading cannon is an effort to obtain

uncalled-for and superfluous facility in gunnery; and if a perfect

breech-loading cannon could possibly be produced, what would it avail?

What superior property could it possess over the solid gun? It could not

be safety; for when we consider the very limited number of explosions by

which the very best guns are destroyed, it can scarcely be possible for

a gun composed of many parts to endure the intense vibrations to which

large cannon are subjected. The regular distribution of vibrations in

the metal of the gun is the great point to be attended to in the

construction of artillery; so that vibrations may not be incorrectly

induced by malformation, or by an excess or deficiency of metal at any

particular point; for where the waves of vibration are checked by an

unequal distribution of metal, or other causes, there the weak point in

a gun is always found, as all fractured guns clearly demonstrate. An

intimate acquaintance with the metallurgy of cannon, enables me to give

an almost unerring opinion as to the causes leading to the fracture.

Most undoubtedly, vibration, if judiciously distributed, is the soul of

endurance; but if injudiciously distributed is certain to result in the

destruction of the cannon. In structures composed necessarily of many

joints, obstruction to the waves of vibration must occur; the different

parts do not expand and vibrate equally; a kind of revulsion is induced;

part repels part, and destruction ensues as a natural consequence. Under

no circumstances, therefore, can a breech-loader be as safe as a solid

gun.

The facility with which breech-loaders can be charged is generally

trumpeted forth to the world as an advantage of vital importance; but

let us carefully examine this point and see if it has not been

exaggerated--whether, in fact, a solid gun cannot be charged and

discharged as rapidly as a breech-loader.

In the first place, all guns recoil; this necessitates the relaying of

the gun after every discharge, in order to obtain accuracy of aim; and

if facility of loading is to be obtained at the expense of aim, it can

scarcely be called an advantage. Aim consumes more time than loading. A

six-pounder may be loaded and fired six times in the first minute; but

it would be impossible to do this and re-lay the gun after each shot.

Where then is the advantage of firing six shots per minute if you cannot

hit six objects? And if breech-loaders could be fired _sixty_ times per

minute, what would they avail if aim was wanting? The raising or

depressing of the breech of a gun by means of the elevating screw;

slewing to the right or left, spunging the gun, and ramming home the

powder and shot, all consume time; hence we think that quickness of

loading is worthless.

Breech-loading cannon cannot be constructed for bullets of larger

diameter than that of the rifle bore, without a ductile bullet be used;

for, as is usual in breech-loading small-arms, the bullet rifles itself

as it is forced up the grooves. The projectiles for rifled cannon have

hitherto been cast with corresponding grooves and lands to fit the

internal form of the cannon. A compound shot, composed of iron, and

covered externally with ductile metal, has been tried in a few

instances; but, unfortunately, the difficulty of combining two metals so

dissimilar as iron and lead has been found so great as invariably to end

in a failure; therefore no prospect exists of bringing into play this,

the best point existing in breech-loading arms.

Lastly, the tendency of all guns to absorb the heat, developed during

explosion, puts a limit to all extreme rapidity of fire; even if this

was not already limited by the more essential point of taking aim. At

Sweaborg it was found necessary to allow an interval of five minutes

between each discharge of a mortar, and yet the whole of them burst

after an average of 120 shots. Time and ingenuity spent in planning and

constructing breech-loading cannon will always end in disappointment and

failure. Many are the plans extant, evincing great skill, perseverance,

and everything needful in point of mechanical experience, but betraying

a total ignorance of the metallurgic science and of practical results

from the use of the engine. The study of these points will save money,

time, and what is of more value, brain-work, which might be better

employed. Striving to produce perfect breech-loading cannon is like

striving to square the circle.

Gunnery in 1858: Being a Treatise on Rifles, Cannon, and Sporting Arms Explaining the Principles of the Science of Gunnery, and Describing the Newest Improvements in Fire-Arms · 第 4 / 14 章