At point \(A\), the recorder is equidistant from both loudspeakers, so the path difference is zero.
As the recorder moves from \(A\) to \(B\), the path difference between the two sound waves changes, producing alternating maxima and minima due to interference.
Step 1: Determine the change in path difference.
Horizontal distance of point \(A\) from the midpoint of the speakers is \(40 \, \text{m}\).
Vertical displacement from \(A\) to \(B\) is \(25 \, \text{m}\).
Distance of \(B\) from the upper speaker \(L_1\):
\[
BL_1 = \sqrt{40^2 + (25 - 5)^2} = \sqrt{1600 + 400} = \sqrt{2000} = 20\sqrt{5}
\]
Distance of \(B\) from the lower speaker \(L_2\):
\[
BL_2 = \sqrt{40^2 + (25 + 5)^2} = \sqrt{1600 + 900} = \sqrt{2500} = 50
\]
Hence, path difference at point \(B\) is:
\[
\Delta = BL_2 - BL_1 = 50 - 20\sqrt{5}
\]
Using \( \sqrt{5} = 2.23 \):
\[
\Delta = 50 - (20 \times 2.23) = 50 - 44.6 = 5.4 \, \text{m}
\]
Step 2: Relate path difference to number of cycles.
One complete cycle of maxima and minima corresponds to a path difference change of one wavelength \( \lambda \).
Given number of cycles \( = 10 \):
\[
10\lambda = 5.4
\]
\[
\lambda = 0.54 \, \text{m}
\]
Step 3: Calculate frequency.
Using \( v = f\lambda \):
\[
f = \frac{v}{\lambda} = \frac{324}{0.5}
\]
\[
f = 648 \, \text{Hz}
\]
Final Answer:
\[
\boxed{648}
\]