If there are any who still believe in the powers ascribed to the far-famed ‘pocket-pistol,’ they will find their confidence in modern artillery10 largely shaken by the announcement that it is considered a great matter that one of Whitworth’s cannon should have thrown a shot to a distance of very nearly six miles and a half. Not only is this so, however, but it is well known that no piece of ordnance has ever flung a projectile11 to so great a distance since first fire-arms were invented; and it may be safely predicted that men will never be able to construct a cannon which—as far as range is concerned—will do much better than this one of Mr. Whitworth’s. The greatest range which had ever before been attained fell somewhat short of six miles. The 7-inch steel gun contrived12 by Mr. Lynall Thomas had flung a projectile weighing 175 lbs. to a distance of 10,075 yards; and, according to General Lefroy’s ‘Handbook of Artillery,’ that was the greatest range ever recorded. But Mr. Whitworth’s cannon has thrown a shot more than 1,000 yards farther.
Very few have any idea of the difficulties which oppose themselves to the attainment14 of a great range in artillery practice. It may seem, at first sight, the simplest possible matter to obtain an increase of range. Let the gun be made but strong enough to235 bear a sufficient charge, and range seems to be merely a question of the quantity of powder made use of. But in reality the matter is much more complicated. The artillerist1 has to contrive13 that the whole of the powder made use of shall be burned before the shot leaves the cannon, and yet that the charge shall not explode so rapidly as to burst the cannon. If he used some forms of powder, very useful for special purposes, half the charge would be blown out without doing its share of work. On the other hand, there are some combustibles (as gun-cotton and the nitrates) which burn so fast that the gun would be likely to burst before the shot could be expelled. Then, again, the shot must fit so closely that there shall be no windage, and yet not so closely as to resist too much the action of the exploding powder. Again, there is the form of the shot to be considered. A sphere is not the solid which passes most readily through a resisting medium like the air; and yet, other projectiles15, which are best so long as they maintain a certain position, meet with a greater resistance when once they begin to move unsteadily. The conoid used in ordinary rifle practice, for example, passes much more freely through the air, point first, than an ordinary spherical16 bullet; but if the point did not travel first, as would happen but for the rifling, or even if the conoidal bullet ‘swayed about’ on its course, it would meet with more resistance than a spherical bullet. Hence the question of ‘fast or slow rifling’ has to be considered. ‘Fast rifling’ gives the greater spin, but causes more resistance to the exit of236 the shot from the barrel; with ‘slow-rifling,’ these conditions are reversed.
And then the common notion is that a cannon-ball travels in the curve called a parabola, and that artillerists have nothing to do but to calculate all about this parabola, and to deduce the range from the initial velocity17 according to some simple principles depending on the properties of the curve. All this is founded on a complete misapprehension of the true difficulties in the way of the problem. Only projectiles thrown with small velocity from the earth travel in parabolic paths. A cannon-ball follows a wholly different kind of curve. The resistance of the air, which seems to most persons a wholly insignificant18 item in the inquiry19, is so enormous in the case of a cannon-ball as to become by far the most important difficulty in the way of the practical artillerist. When a 250-lb. shot is hurled20 with such force from a gun as to cover a range of six miles, the resistance of the air is about forty times the weight of the ball—that is, is equivalent to a weight of upwards21 of four tons. The range in such a case as this is but a small fraction of that which would be given by the ordinary parabolic theory.
As regards artillery practice in war, there are other difficulties in the attainment of a very extended range. Cannon meant for battering22 down forts cannot possibly be used in the same way that Whitworth’s was used at Shoeburyness. If the shot flung from this gun at an elevation23 of thirty-three degrees could have been watched, it would have been found that it fell to the237 earth at a much greater angle—that is, much more nearly in a perpendicular24 direction. On the ordinary parabolic theory, of course, the angle of fall would be the same as the angle of elevation, but under actual circumstances there is an important difference. If forts are to be battered25 down, however, it will not serve that they should be struck from above; our artillerists must perforce keep to the old method of pounding away at the face of the forts they attack. Therefore, an elevation which is all very well for mortars—that is, when the question merely is of flinging a bomb into a town or fortress—is utterly26 unsuited for ordinary artillery. With an elevation of ten degrees, Whitworth’s cannon scarcely projected the 250-lb. shot to a distance of three miles.
The progress of the modern science of gunnery certainly tends to increase the distance at which armies will engage each other. With field artillery flinging shot to a distance of two or three miles, and riflemen able to make tolerably sure practice at a distance of three-quarters of a mile, we are not likely often to hear of hand-to-hand conflicts in future warfare27. The use of breech-loaders will also tend to the same effect. Hitherto we have scarcely had experience of the results which these changes are to produce on modern warfare. At Sadowa breech-loaders did not encounter breech-loaders, and it was easy for the victors in that battle to come to close quarters with their enemies. But in a battle where both sides are armed with breech-loaders, we shall probably see another sort of238 affair altogether. The bayonet will be an almost useless addition to the soldier’s arms; a charge of cavalry28 upon well-armed infantry29 will be almost as hopeless as the famous Balaclava charge; and the artillery on either side will have to play a game at long bowls. I venture to anticipate that the first great European war will introduce a total change into the whole system of warlike man?uvres.14
(From the Daily News, November 1868.)
点击收听单词发音
1 artillerist | |
炮手,炮兵,炮术家 | |
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2 cannon | |
n.大炮,火炮;飞机上的机关炮 | |
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3 attentively | |
adv.聚精会神地;周到地;谛;凝神 | |
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4 attained | |
(通常经过努力)实现( attain的过去式和过去分词 ); 达到; 获得; 达到(某年龄、水平、状况) | |
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5 narrative | |
n.叙述,故事;adj.叙事的,故事体的 | |
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6 obstinately | |
ad.固执地,顽固地 | |
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7 incapable | |
adj.无能力的,不能做某事的 | |
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8 mythical | |
adj.神话的;虚构的;想像的 | |
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9 ordnance | |
n.大炮,军械 | |
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10 artillery | |
n.(军)火炮,大炮;炮兵(部队) | |
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11 projectile | |
n.投射物,发射体;adj.向前开进的;推进的;抛掷的 | |
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12 contrived | |
adj.不自然的,做作的;虚构的 | |
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13 contrive | |
vt.谋划,策划;设法做到;设计,想出 | |
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14 attainment | |
n.达到,到达;[常pl.]成就,造诣 | |
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15 projectiles | |
n.抛射体( projectile的名词复数 );(炮弹、子弹等)射弹,(火箭等)自动推进的武器 | |
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16 spherical | |
adj.球形的;球面的 | |
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17 velocity | |
n.速度,速率 | |
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18 insignificant | |
adj.无关紧要的,可忽略的,无意义的 | |
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19 inquiry | |
n.打听,询问,调查,查问 | |
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20 hurled | |
v.猛投,用力掷( hurl的过去式和过去分词 );大声叫骂 | |
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21 upwards | |
adv.向上,在更高处...以上 | |
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22 battering | |
n.用坏,损坏v.连续猛击( batter的现在分词 ) | |
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23 elevation | |
n.高度;海拔;高地;上升;提高 | |
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24 perpendicular | |
adj.垂直的,直立的;n.垂直线,垂直的位置 | |
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25 battered | |
adj.磨损的;v.连续猛击;磨损 | |
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26 utterly | |
adv.完全地,绝对地 | |
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27 warfare | |
n.战争(状态);斗争;冲突 | |
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28 cavalry | |
n.骑兵;轻装甲部队 | |
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29 infantry | |
n.[总称]步兵(部队) | |
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