Let \(\gamma_1\)be the ratio of molar specific heat at constant pressure and molar specific heat at constant volume of a monoatomic gas and \(\gamma_2\) be the similar ratio of diatomic gas. Considering the diatomic gas molecule as a rigid rotator, the ratio, \(\frac{\gamma_1}{\gamma_2}\) is :
\(\frac{21}{25}\)
\(\frac{25}{21}\)
\(\frac{35}{27}\)
\(\frac{27}{35}\)
To solve this problem, we need to understand the concepts of molar specific heat capacities and the ratio \( \gamma \) (gamma). The gamma ratio for a gas is defined as:
\(\gamma = \frac{C_p}{C_v}\)
where:
For a monoatomic gas:
Thus, for a monoatomic gas:
\(\gamma_1 = \frac{C_p}{C_v} = \frac{\frac{5}{2}R}{\frac{3}{2}R} = \frac{5}{3}\)
For a diatomic gas considered as a rigid rotator:
Thus, for a diatomic gas:
\(\gamma_2 = \frac{C_p}{C_v} = \frac{\frac{7}{2}R}{\frac{5}{2}R} = \frac{7}{5}\)
Now, we need to find the ratio of \( \gamma_1 \) to \( \gamma_2 \):
\(\frac{\gamma_1}{\gamma_2} = \frac{\frac{5}{3}}{\frac{7}{5}} = \frac{5}{3} \times \frac{5}{7} = \frac{25}{21}\)
Hence, the ratio \( \frac{\gamma_1}{\gamma_2} \) is \( \frac{25}{21} \), which is the correct answer.
Match List-I with List-II.
| List-I | List-II |
| (A) Heat capacity of body | (I) \( J\,kg^{-1} \) |
| (B) Specific heat capacity of body | (II) \( J\,K^{-1} \) |
| (C) Latent heat | (III) \( J\,kg^{-1}K^{-1} \) |
| (D) Thermal conductivity | (IV) \( J\,m^{-1}K^{-1}s^{-1} \) |
In the given cycle ABCDA, the heat required for an ideal monoatomic gas will be:

The pressure of a gas changes linearly with volume from $A$ to $B$ as shown in figure If no heat is supplied to or extracted from the gas then change in the internal energy of the gas will be Is
