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
It is on the nature of the metal that the goodness of the shooting
principally depends. That barrel which is possessed of the greatest
degree of elasticity and tenacity, will throw its shot strongest and
closest with the least artificial friction. It is on the knowledge of
the qualities and temperatures of the various irons, and on practice in
the art of shooting, that a man’s ability in making guns shoot with
precision must rest. All plans are merely methods by which an
unscientific maker has most frequently succeeded. It would be no
difficult task to produce a hundred barrels which will shoot nearly
alike; yet every barrel shall be different in its bore.
The length of friction depends entirely on the length of the barrel.
Long barrels require more than short, though the latter require it in a
greater degree. A mode of creating friction, much practised by those who
are ignorant of the true method, is to bore the barrels as rough and as
full of rings as possible. These rings are often taken for flaws; though
that may be ascertained by noticing whether or not they have the same
inclination as the twist, and whether or not they are at the jointing of
a spiral. If they be not, the chance is that the barrel is ring-bored,
as it is termed. This roughness, however, answers the same as friction
by relief; but barrels thus roughened are very liable to lead, and
become foul. While the well-bored barrel will fire forty shots as well
as twenty, these cannot be fired more than twenty times with safety and
effect.
Each of the barrels in the table below, if 3-16ths thick at the breech,
is equal to the pressure stated. The resistance of a charge of shot of
one ounce we find to be more than before stated; and the additional
increase of explosive force obtained at the moment of ignition, requires
the amount to be much greater in computation, therefore, we may safely
take a pressure of 1,700 pounds to the inch of tube. The reader will
perceive, on reference to the following table, that with the tube filled
with powder for an inch in length, which is a small charge, the
explosive force will be equal to 40,000 pounds, or nearly 1,700 pounds
to the inch.
Public-domain text, read in full here on John Shaqi.
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