In an adiabatic expansion of a gas initial and final temperatures are T1 and T2 respectively, then the change in internal energy of the gas is
Rγ−1(T2−T1)
Rγ−1(T1−T2)
R(T1−T2)
Zero
ΔU=−ΔW=−RT1−T2(γ−1)=RT2−T1γ−1