The correct option is B b+1b
From first law of thermodynamics,
dQ=dU+dW ...(i)
we can write small amount of work done as dW=PdV
For an adiabatic process heat supplied is zero i.e dQ=0
From Eq(i),
⇒dQ=dU+PdV
⇒0=dU+PdV
substituting value of U
⇒d(a+bPV)+PdV=0 ...(ii)
since a & b are constants, da=0, db=0
Applying chain rule for finding d(bPV) and putting in Eq (ii)
⇒bPdV+bVdP+PdV=0
or (b+1)PdV+bVdP=0
Dividing both sides by PV,
⇒(b+1)dVV+bdPP=0 ...(iii)
Integrating Eq.(iii) both sides,
⇒(b+1)logV+blogP=constant
⇒logVb+1+logPb=constant
Applying logm+logn=log(mn)
⇒log(Vb+1Pb)=constant
⇒Vb+1Pb=constant
Taking power 1b both sides,
⇒PVb+1b=constant1b
⇒PVb+1b=constant ...(iv)
Comparing Eq. (iv) with PVγ=constant
∴γ=b+1b