C.V. Air. Assume a reversible, adiabatic process.
Energy Eq. u2 - u1 = 0 − 1w2 ;
Entropy Eq s2 - s1 = ∫ dq/T + 1s2 gen = 0
State 1: (T1,P1) State 2: (P2, ?
So we realize that one piece of information is needed to get state 2.
Process: Adiabatic 1q2 = 0 Reversible 1s2 gen = 0
With these two terms zero we have a zero for the entropy change. So this is a constant s (isentropic) expansion process giving s2 = s1.