The volume of $1 \; mole$ of an ideal gas with the adiabatic exponent $\gamma$ is changed according to the relation $V = \frac{b}{T}$,where $b$ is a constant. The amount of heat absorbed by the gas in the process if the temperature is increased by $\Delta T$ will be:

  • A
    $\frac{R}{\gamma - 1} \Delta T$
  • B
    $\left( \frac{2 - \gamma}{\gamma - 1} \right) R \Delta T$
  • C
    $\frac{R \Delta T}{\gamma - 1}$
  • D
    $\left( \frac{1 - \gamma}{\gamma + 1} \right) R \Delta T$

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