The mean free path \( \lambda \) of a gas molecule is the average distance a molecule travels between successive collisions.
It is given by the formula:
$$ \lambda = \frac{1}{\sqrt{2} \pi d^2 n} $$
where \( d \) is the diameter of the gas molecule and \( n \) is the number density of the gas molecules (number of molecules per unit volume), which is proportional to the concentration.
For two gases at the same concentration, \( n_1 = n_2 = n \).
Let the diameters of the molecules of the two gases be \( d_1 \) and \( d_2 \), and their mean free paths be \( \lambda_1 \) and \( \lambda_2 \), respectively.
The ratio of their diameters is given as \( d_1 : d_2 = 1 : 2 \), so \( \frac{d_1}{d_2} = \frac{1}{2} \).
The mean free paths are:
$$ \lambda_1 = \frac{1}{\sqrt{2} \pi d_1^2 n} $$
$$ \lambda_2 = \frac{1}{\sqrt{2} \pi d_2^2 n} $$
The ratio of their mean free paths is:
$$ \frac{\lambda_1}{\lambda_2} = \frac{\frac{1}{\sqrt{2} \pi d_1^2 n}}{\frac{1}{\sqrt{2} \pi d_2^2 n}} = \frac{\sqrt{2} \pi d_2^2 n}{\sqrt{2} \pi d_1^2 n} = \frac{d_2^2}{d_1^2} = \left( \frac{d_2}{d_1} \right)^2 $$
Since \( \frac{d_1}{d_2} = \frac{1}{2} \), we have \( \frac{d_2}{d_1} = 2 \).
$$ \frac{\lambda_1}{\lambda_2} = (2)^2 = 4 $$
Therefore, the ratio of their mean free paths is \( \lambda_1 : \lambda_2 = 4 : 1 \).