The mean free path \( \lambda \) is inversely proportional to the number of molecules per unit volume \( n \).
Hence, we have the relation: \[ \lambda \propto \frac{1}{n} \] Let the initial number of molecules per unit volume be \( n_1 = 0.8 \times 10^{24} \) and the initial mean free path be \( \lambda_1 = 2.2 \times 10^{-5} \, {m} \).
When the number of molecules per unit volume is increased to \( n_2 = 1.0 \times 10^{24} \), the mean free path \( \lambda_2 \) becomes: \[ \frac{\lambda_2}{\lambda_1} = \frac{n_1}{n_2} \] Substituting the values: \[ \frac{\lambda_2}{2.2 \times 10^{-5}} = \frac{0.8 \times 10^{24}}{1.0 \times 10^{24}} = 0.8 \] Thus: \[ \lambda_2 = 0.8 \times 2.2 \times 10^{-5} = 1.76 \times 10^{-5} \, {m} \] Hence, the correct answer is (B).
For a particular ideal gas, which of the following graphs represents the variation of mean squared velocity of the gas molecules with temperature?
Draw a neat labelled diagram of Ferry's perfectly black body. Compare the rms speed of hydrogen molecules at 227°C with rms speed of oxygen molecules at 127°C. Given that molecular masses of hydrogen and oxygen are 2 and 32, respectively.