The molar specific heat of an ideal gas at constant pressure and constant volume is $C_{p}$ and $C_{v}$ respectively. If $R$ is the universal gas constant and $\gamma = \frac{C_p}{C_v}$,then $C_v =$

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

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The molar specific heats of an ideal gas at constant pressure and constant volume are denoted by $C_P$ and $C_V$ respectively. If $\gamma = C_P/C_V$ and $R$ is the universal gas constant,then $C_V = $ ........

If the molar specific heat at constant volume is $\frac{3R}{2}$,then the adiabatic index $\gamma$ is:

The ratio of specific heats $(\gamma)$ of an ideal gas is given by

Match the $\frac{C_{P}}{C_{v}}$ ratio for ideal gases with different types of molecules:
Molecule type $\frac{C_{P}}{C_{v}}$
$A$. Monoatomic $I$. $\frac{7}{5}$
$B$. Diatomic rigid molecules $II$. $\frac{9}{7}$
$C$. Diatomic non-rigid molecules $III$. $\frac{4}{3}$
$D$. Triatomic rigid molecules $IV$. $\frac{5}{3}$

If $C_P$ and $C_V$ are the specific heats of unit mass of nitrogen at constant pressure and constant volume respectively,then:

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