Maryland. Aberdeen Proving Ground. 1949A discussion is first given of the general problem of the flow of gas in a gun, of the simplified problem known as the Lagrange problem, and of the Pidduck-Kent special solution of the differential equation of the Lagrange problem. This special solution is commonly supposed to be the limiting solution of the latter. An improved derivation is then given of the Pidduck-Kent solution, the improvement consisting in accounting for gas imperfection by means of a covolume correction.
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