Interior Ballistics

Cover Interior Ballistics
Interior Ballistics
James M James Monroe Ingalls
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42689 and these in the above velocity equation give v m = 2487 f. S. We find, from Table I, taking log X as the argument, x = 10. 613; 138 INTERIOR BALLISTICS and by (m) u = 615. 19 in. Also by (k) 2/ =o". 47 and by (/) k m = 0-9394- That is 94 per cent, of the charge was burned at the assumed muzzle.
If the maximum pressure is increased to 38, 000 Ibs. , the density of loading and volume of chamber remaining as before, the velocity for a travel of 280 inches will be increased to 2503 f. S. , a
...nd the thickness of web, or diameter of the grain, will be reduced to 0^. 45. This slight diminution in the diameter of the grain increases the initial surface of combustion of the charge about 3^ per cent. , which fully accounts for the increased maximum pressure.
If we take A =0. 5, V c = 3, 000 c. I. And p m = 37, 000 Ibs. Per in. 2, there results co = 54. 19 Ibs. , v 2S o = 2570 f. S. , and 2 / =o". 66.
Trinomial Formulas for Velocity and Pressure. Trinomial formulas occur when the grains of which the charge is composed are of such form and dimensions that the form characteristic /* cannot be regarded as zero.


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