In an isobaric process of an ideal gas, the ratio of work done by the system $(W)$ during the expansion and the heat exchanged $(Q)$ is $(\gamma = \frac{C_p}{C_v})$

  • A
    $\gamma$
  • B
    $\gamma-1$
  • C
    $\frac{\gamma}{\gamma-1}$
  • D
    $\frac{\gamma-1}{\gamma}$

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