To solve this problem, we need to understand the mixture of gases and the concept of specific heat capacities. Specifically, we're looking at a mixture of helium (He) and hydrogen (H2) gases, and we're given the ratio of specific heat capacities, \(\frac{C_P}{C_V}\), for the mixture.
The ratio \(\frac{C_P}{C_V}\) is known as the adiabatic index \( \gamma \) (gamma). For the mixture, this is given as \(\frac{3}{2}\).
Helium (\( \text{He} \)) is a monoatomic gas with \(\gamma = \frac{5}{3}\).
Hydrogen (\( \text{H}_2 \)) is a diatomic gas with \(\gamma = \frac{7}{5}\).
Let \( n_{He} \) be the number of moles of helium, which is 2 moles.
Let \( n_{H_2} \) be the number of moles of hydrogen, which is \( n \) moles.
The formula for the effective \( \gamma \) (gamma) of a mixture of two gases is given by:
\[\gamma_{\text{mix}} = \frac{n_{He}\cdot C_{V,He} \cdot \gamma_{He} + n_{H_2}\cdot C_{V,H_2} \cdot \gamma_{H_2}}{n_{He}\cdot C_{V,He} + n_{H_2}\cdot C_{V,H_2}}\]To solve this for \( n \):
Substitute these values into the formula for \( \gamma_{\text{mix}} \):
\[\frac{3}{2} = \frac{2 \cdot \frac{3R}{2} \cdot \frac{5}{3} + n \cdot \frac{5R}{2} \cdot \frac{7}{5}}{2 \cdot \frac{3R}{2} + n \cdot \frac{5R}{2}}\]Solving the equation:
\[\frac{3}{2} = \frac{5R + 7nR}{3R + 5nR}\]Multiply both sides by the denominator to clear the fraction:
\[3R + 5nR = \frac{3}{2} \cdot (5R + 7nR)\]Continue to simplify:
\[6R + 10nR = 15R + 21nR\]Rearrange terms:
\[6R - 15R = 21nR - 10nR \] \[ -9R = 11nR \]\]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
