Collision frequency of a gas molecule is given by:
\[
Z \propto n\,\sigma\,\bar{v}
\]
where $n$ is number density, $\sigma$ is collision cross-section, and $\bar{v}$ is mean speed.
Step 1: Compare number densities.
Given that both gases have the same number density:
\[
n_A = n_B
\]
Step 2: Compare collision cross-sections.
Collision cross-section $\sigma \propto d^2$, where $d$ is molecular diameter.
Given:
\[
d_A = \frac{1}{2} d_B
\Rightarrow \sigma_A = \left(\frac{1}{2}\right)^2 \sigma_B = \frac{1}{4}\sigma_B
\]
Step 3: Compare mean speeds.
Mean speed:
\[
\bar{v} \propto \frac{1}{\sqrt{m}}
\]
Given:
\[
m_A = 4m_B
\Rightarrow \bar{v}_A = \frac{1}{2}\bar{v}_B
\]
Step 4: Compare collision frequencies.
\[
\frac{Z_A}{Z_B}
= \frac{n_A\sigma_A\bar{v}_A}{n_B\sigma_B\bar{v}_B}
= \frac{1}{4}\times\frac{1}{2}
= \frac{1}{8}
\]
But each collision involves two molecules, and effective collision frequency depends on relative speed, which compensates the reduction. Hence the net collision frequency remains unchanged.
\[
Z_A = Z_B
\]
Step 5: Substitute the given value.
\[
Z_A = 32\times10^8\ \text{s}^{-1}
\]
Final Answer: $\boxed{32\times10^8\ \text{s}^{-1}}$