(A) ω=−P ext ΔV
Work done on gas when compressed ω= is positive ∴ equation becomes ω=P ext ΔV
(B) under adiabatic conditions ω=(γ−1)(P2V2−P1V1)
since equation V2>V1 ∴ω=+ ve (work done on system)
for reversibly condition (Isothermal) ω=−nRTlnV1V2 =V2>V1 ω=−ve (work done on system) ω=−ve (for adiabatic reversibly work done by gas) ω=+ve (for isothermal reversibly work done by gas)
(C) As free expansion in there (irreserible) ∴P ext =0 ω=(−Pext×ΔV)=0
(Isothermal irreversible process)
In adiabatic ΔU=−ve ΔU=q+ω −=0+ω ω=− negative
similarly, ΔG=ΔH−TΔs
gas expand ∴Δs=+ve ΔG=ΔH−Ve =ΔV+pΔV−ve =q+w+pΔc−ve =o+w+w−ve =−ve+(−ve)−ve ΔG=−ve ∴ It is spontaneous process ∴ both take place simultaneously