The first law of thermodynamics states: \[ dQ = du + dW \]
Under conditions of constant pressure, this equation simplifies to: \[ C dT = C_v dT + P dV \tag{1} \]
For the relation \( PV^2 = RT \), differentiating both sides with respect to \( T \) while maintaining constant \( P \): \[ P(2V dV) = R dT \] \[ P dV = \frac{R}{2V} dT \]
Substituting the expression for \( P dV \) into equation (1): \[ C dT = C_v dT + \frac{R}{2V} dT \] \[ C = C_v + \frac{R}{2V} \]
Therefore, the specific heat at constant pressure is expressed as: \[ C = C_v + \frac{R}{2V}. \]
A real gas within a closed chamber at \( 27^\circ \text{C} \) undergoes the cyclic process as shown in the figure. The gas obeys the equation \( PV^3 = RT \) for the path A to B. The net work done in the complete cycle is (assuming \( R = 8 \, \text{J/molK} \)):
