The beat frequency \( f_b \) is given by the absolute difference in the frequencies of the two pipes:
\[
f_b = |f_A - f_B|
\]
where \( f_A \) is the frequency of the longer pipe, and \( f_B \) is the frequency of the shorter pipe.
We are given:
- The beat frequency \( f_b = 2 \, \text{beats/sec} \),
- The length of the first pipe, \( L_A = 22 \, \text{cm} \),
- The length of the second pipe, \( L_B = 22.5 \, \text{cm} \).
For open pipes, the frequency \( f \) is inversely proportional to the length \( L \), i.e.,
\[
f \propto \frac{1}{L}
\]
Thus, we can write:
\[
\frac{f_A}{f_B} = \frac{L_B}{L_A}
\]
Now, substituting the lengths of the pipes:
\[
\frac{f_A}{f_B} = \frac{22.5}{22}
\]
\[
f_A = f_B \times \frac{22.5}{22} = f_B \times 1.0227
\]
Now, we know the difference in their frequencies is equal to the beat frequency:
\[
f_A - f_B = 2 \, \text{beats/sec}
\]
Substitute \( f_A = 1.0227 f_B \) into the equation:
\[
1.0227 f_B - f_B = 2
\]
\[
0.0227 f_B = 2
\]
Solving for \( f_B \):
\[
f_B = \frac{2}{0.0227} = 88 \, \text{Hz}
\]
Thus, the frequency of the shorter pipe is \( 88 \, \text{Hz} \).