An ideal system operating with n moles of an ideal monatomic gas performs the cycle shown in the P−V diagram to the right. All parts of the cycle are carried out slowly and reversibly. Starting at state a, where its volume and pressure are (V0,p0), the gas undergoes an isothermal expansion until it reaches state b where its volume and pressure are (8V0,p0/8). In process b→c the gas is cooled at constant volume to (8V0,p0/32). Process c→a is an adiabatic compression back to state a.