The variation of pressure $P$ with volume $V$ for an ideal monatomic gas during an adiabatic process is shown in figure. At point $A$ the magnitude of rate of change of pressure with volume is
Diffcult
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(d)
$P V^y=$ constant
$P \propto V^{-\gamma}$
$\frac{d P}{P}=-\gamma \frac{d V}{V}$
$\frac{d P}{d V}=\gamma \frac{P}{V}$
$=\frac{5}{3} \times \frac{3 P_0}{2 V_0}$
$=\frac{5 P_0}{2 V_0}$
Then $\left(\frac{d P}{d V}\right)=\frac{5 P_0}{2 V_0}$
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