Effective aperture \( A_e \) is related to directivity \( D \) and wavelength \( \lambda \) by:
\[
A_e = \frac{D \cdot \lambda^2}{4\pi}
\]
Given:
\[
D = 100, f = 150\, \text{MHz} \Rightarrow \lambda = \frac{c}{f} = \frac{3 \times 10^8}{150 \times 10^6} = 2\, \text{m}
\]
Now,
\[
A_e = \frac{100 \cdot (2)^2}{4\pi} = \frac{400}{4\pi} = \frac{100}{\pi} \approx 31.8 \, \text{m}^2
\]