For an adiabatic expansion of an ideal gas, the fractional change in its pressure is equal to: (Where \( \gamma \) is the ratio of specific heats).
\( -\dfrac{1}{\gamma}\dfrac{dV}{V} \)
\( -\gamma \dfrac{V}{dV} \)
\( \dfrac{dV}{V} \)
\( -\gamma \dfrac{dV}{V} \)