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In a temperature-pressure (\( T\)-\(\mathit{\Pi} \) diagram, an adiabatic curve \(\sim V^{1-\frac{1}{\gamma}}\) was plotted. The product \(T_1 \, {\mathit{\Pi}_1}^{\frac{1}{\gamma}-1}\) BEFORE the adiabatic process is equal to the product \(T_2 \, {\mathit{\Pi}_2}^{\frac{1}{\gamma}-1}\) AFTER the adiabatic process.