An adiabatic process involves an ideal gas undergoing changes without heat exchange with its surroundings. The work performed during such a process is understood through the adiabatic process equation: PVγ = constant, where P denotes pressure, V represents volume, and γ (gamma) is the adiabatic index or specific heat ratio (Cp/Cv).
The work done (W) in an adiabatic process is given by the relation: W = (P1V1 - P2V2) / (γ - 1).
Leveraging the adiabatic condition, work done can also be expressed in terms of the volume change: W = (Cv(T1 - T2))/(1-γ).
Relating work done directly to volume change yields: W = ((P1V1 - P2V2))/(γ - 1)) = K(V21-γ - V11-γ)/(1-γ).
Consequently, the work done in an adiabatic change is directly dependent on the gas's volume. Therefore, the work done in an adiabatic change is determined by the change in its volume.
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 \( R = 8 \, \text{J/molK} \)):
