In an adiabatic process,the work involved during expansion or compression of an ideal gas is given by

  • A
    $n C_v \Delta T$
  • B
    $\frac{nR}{\gamma - 1} (T_2 - T_1)$
  • C
    $- 2.303 nRT \log \frac{V_2}{V_1}$
  • D
    $(A) \text{ and } (B) \text{ both}$

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