In an adiabatic expansion of a gas initial and final temperatures are ${T_1}$ and ${T_2}$ respectively, then the change in internal energy of the gas is

  • A

    $\frac{R}{{\gamma - 1}}({T_2} - {T_1})$

  • B

    $\frac{R}{{\gamma - 1}}({T_1} - {T_2})$

  • C

    $R({T_1} - {T_2})$

  • D

    Zero

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