An ideal gas at pressure \( P \) is adiabatically compressed so \( ...
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An ideal gas at pressure \( P \) is adiabatically compressed so
\( \mathrm{P} \) that its density becomes \( n \) times the initial value. The final
W pressure of the gas will be \( \left(\gamma=C_{p} / C_{v}\right) \) :
(A) \( n^{\gamma} P \)
(B) \( n^{-\gamma} P \)
(C) \( n^{(\gamma-1)} P \)
(D) \( n^{(1-\gamma)} P \)
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