The heat capacity of one mole of an ideal gas is found to be $C_V = \frac{3R(1 + aRT)}{2}$,where $a$ is a constant. The equation obeyed by this gas during a reversible adiabatic expansion is

  • A
    $TV^{3/2} e^{aRT} = \text{constant}$
  • B
    $TV^{3/2} e^{3aRT/2} = \text{constant}$
  • C
    $TV^{3/2} = \text{constant}$
  • D
    $TV^{3/2} e^{2aRT/3} = \text{constant}$

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