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HISTORY AND CONSTRUCTION]
ORDNANCE
209


guns are much stronger. This is an obvious advantage, but an equally solid one is the fact that owing to the greater weight of the home-made weapon the recoil energy is less and consequently the mounting can be made of a lighter pattern. Besides, the weight of the gun is so disposed as to bring its centre of gravity as near the breech end as possible; by this means the radius of the gun house is reduced to the smallest dimension and, in consequence, there is a great saving of weight of armour. The extra weight of the gun is therefore more than compensated for.


Fig. 54.—Metallic Cartridge Case.

Table II.—Names and Weights of English Cannon, 1574
Names. Weight. Diameter
of Bore.
Diameter
of Shot.
Weight of
Shot.
Weight of
Charge.
Serpentine.
Scores of
Paces at
point-blank.
in. in.
Robinet  200 11/4 1 1 1/2 . .
Falconet  500 2  13/4 2  11/4 14
Falcon  800 23/4 21/2  21/2  21/2 16
Minion 1100 31/4 3  41/2  41/2 17
Sacre 1500 31/2 31/2 5 5 18
Demi-Culverin   2500 41/4 4 9 9 20
Culverin 4000 51/4 5 18 18 25
Demi-Cannon 6000 61/2 61/4 30 28 28
Cannon 7000 73/4 71/2 60 40 20
Eliza-Cannon 8000 8  73/4 63 42 20
Basiliske 9000 83/4 81/2 60 60 21


Table III.
Gun. Weight of 
Charge.
Weight of 
Shot.
Muzzle
Velocity.
℔. ℔. f.s.
27-pr.  66 cwt. 13·125 27  1517
131/2 pr. 37·5 cwt.    6·562 13·5 1618
63/4 pr.  20 cwt.  4·922  6·75 1696
33/8 pr.  11 cwt.  2·469 3·375 1720


Table IV.—British Smooth Bore Guns, 1860.
Official Designation of Gun. Calibre.  Weight of 
Gun.
Weight of
Charge.
Weight of 
Projectile.
Muzzle
Velocity.
Muzzle
Energy.
In. Tons. ℔. ℔. Ft. Secs. Ft. Tons.
Cast
Iron.
10 in. 87 cwt. 10  4·35 12 88·31 1292 1022
68 pr. 95 „ 8·12   4·75 16 66·25 1579 1145
 8 in. 65 „ 8·05   3·22 10  49·875 1464 742
32 pr. 58 „ 6·375 2·9 10  31·375 1690 621
24  „ 50 „ 5·823 2·5  8 23·5  1720 482
18  „ 38 „ 5·292 1·9  6 17·69 1690 350
Bro-
nze.
12  „ 18 „ 4·623 0·9  4 12·66 1769 275
 9  „ 13 „ 4·20   0·65 2·5  9·36 1614 169
 6  „  6 „ 3·668 0·3 1·5  6·23 1484  95


Table V.—British B.L. Ordnance, 1860. Armstrong System.
Official Designation of Gun. Calibre. Weight of
Gun.
Weight of
Charge.
Weight of
Projectile.
Muzzle
Velocity.
Muzzle
Energy.
In. Tons. ℔. ℔. Ft. Secs. Ft. Tons.
100 pr. 7  4·1
3·6
 *
12  103·75 1166 978
 40 „  4·75 1·75
1·6 
5 41·5 1164
1134
390
370
 20 „  3·75 0·8 
0·65
2·5  21·22 1114
 997
162
146
 12 „ 3·0 0·425  11·56 1184 112
 9 „ 3·0 0·3  1·125 9·0  1141  81
 6 „ 2·5 0·175 0·75 6·0   946  37

At a later date the velocities of these guns were altered.   * Two patterns were in existence.

Until late into the 16th century the calibres of the guns were not regulated with a view to the interchangeability of shot. In the following century ordnance was divided into classes, but even then, owing no doubt to manufacturing difficulties, there was no fixed size for the bore. The Tables II.-VII. give some idea of the size and weight of these pieces.

Table II. is taken from Cleveland’s Notes, but corrected from “An Old Table of Ordnance” (Proc. R.A.I., vol. xxviii. p. 365); the last column gives the range in scores of paces at point-blank, a term used in those days to denote the first part of the trajectory which was supposed to be a straight line. Later the point-blank range was that distance from the gun on its carriage to the first graze of the shot on the horizontal plane when the axis of the gun was placed horizontal; this depended on the height of the gun above the ground plane, but it was the only method of determining the relative power of these early guns.

In power, smooth-bore guns in Europe did not differ very much from each other, and it may be taken for granted that the progress made since has been much the same in all.

D’Antoni, in his Treatise of Fire Arms (translated by Captain Thomson, R.A.), gives particulars of Italian guns of about 1746, which are shown in Table III.

It will be seen that the velocities given in Table III. are not inferior to those obtained from guns actually in use in 1860 (see Table IV.). They were considerably higher than those for elongated rifled projectiles (Table V.) for many years after their introduction; the last-named, however, during flight only lost their velocity slowly, while the spherical shot lost their velocity so rapidly that at 2000 yds. range only about one-third of the initial velocity was retained.