For an adiabatic expansion of an ideal gas, the fractional change in its pressure is equal to (where γ is the ratio of specific heats) :

1
−γ\(\frac{dV}{V}\)
2
−γ\(\frac{V}{dV}\)
3
\(−\frac{1}{\gamma} \frac{dV}{V}\)
4
More than one of the above
5
None of the above

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