Concept:
The mean free path of gas molecules is defined as the average distance travelled by a molecule between two successive collisions.
The expression for mean free path is
\[
\lambda=\frac{1}{\sqrt{2}\pi d^2 n}
\]
where
\[
d=\text{diameter of a molecule}
\]
and
\[
n=\text{number of molecules per unit volume}
\]
Thus, mean free path is inversely proportional to the square of the molecular diameter.
\[
\lambda \propto \frac{1}{d^2}
\]
Step 1: Relate diameter and radius.
Diameter of a molecule is
\[
d=2r
\]
If the radius is doubled,
\[
r' = 2r
\]
then the new diameter becomes
\[
d' = 2(2r)
\]
\[
d' = 2d
\]
Hence, the diameter also doubles.
Step 2: Apply the proportionality relation.
Since
\[
\lambda \propto \frac{1}{d^2}
\]
we have
\[
\frac{\lambda'}{\lambda}
=
\frac{d^2}{(2d)^2}
\]
\[
=
\frac{d^2}{4d^2}
\]
\[
=
\frac14
\]
Step 3: Interpret the result.
Therefore,
\[
\lambda'=\frac{\lambda}{4}
\]
Hence, the mean free path becomes one-fourth of its original value.
\[
\boxed{\lambda'=\frac{\lambda}{4}}
\]