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-ArmsGreener, William
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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
Greener, William
Firearms; Gunnery
2nd. Consequent on the velocity of the explosive fluids is the
resistance of that aëriform fluid filling all space. It has been
calculated that in a vacuum, matter in motion would be a long time in
coming to rest; and very providentially it is that nature in her grand
arrangements has made one element to control another. In no other
portion of nature’s work has anything more wonderful than atmospheric
air been produced; its action on the velocity of projectiles is of so
extensive a nature, that without clearly understanding that action, the
science of gunnery never can be thoroughly acquired. The resistance of
the atmosphere is in proportion to the velocity of the attempt to
displace it; the higher that velocity becomes, the greater is the
resistance. This is shown by the actions of all the fulminates. A
quantity of the fulminate of silver exploded on a copper plate will
perforate that plate, or, if fired upon a piece of wood, will bury
itself in that substance, splintering it in proportion to the quantity.
Now, ordinary gunpowder has no such effect as this, because, though it
may produce the same amount of expansive gas, it produces it at
one-fourth the velocity of the fulminates: the air is driven back upon
itself so gradually as to offer no very important resistance; but the
action of the fulminates is so rapid and so violent that the high
elasticity of the air has not time to yield, and the force is driven
into the apparently more solid material, the copper or the wood.
The mode in which atmospheric resistance mostly interferes with
projectile force is owing to the columnar form it assumes in the tubes
of all descriptions of gunnery. If the velocity of gunpowder be as great
as we suppose it to be, the displacement of a column of air must be
effected by driving the whole column in a gun-barrel of many inches,
into a column probably less than half an inch in height; or, if the
length of the tube from the starting of the charge to the muzzle be 38
inches, then will the displacement require a force capable of condensing
thirty-eight atmospheres into one, or something like 570 lbs.; without
estimating the lateral pressure of that column on the sides of the
gun-barrel, which may be safely estimated at one-half more. It may be
supposed that the column would be partially in motion for a greater
distance than half an inch in front of the projectile; but this is
disproved by the fact that time is essential to put aëriform matter in
motion, and naturally it never does so at a greater velocity than it is
familiarly known to do in the shape of winds: but the fact is better
illustrated by the frequent bursting of barrels near the muzzle, caused
by a piece of snow or clay, a piece of paper or wadding. Were a current
established around this projection it would pass on, but the air strikes
these light obstructions when in a high state of condensation, amounting
to many atmospheres in one: so many as to be nearly equal to a solid
Public-domain text, read in full here on John Shaqi.
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