Concept:
The potential energy of a particle performing Simple Harmonic Motion (SHM) is given by
\[
U = \frac{1}{2}m\omega^{2}x^{2}
\]
where
• \(m\) = mass of the particle
• \(\omega\) = angular frequency
• \(x\) = displacement
The frequency \(f\) is related to angular frequency by
\[
\omega = 2\pi f
\]
Step 1: Compare the given potential energy with the SHM formula.
Given
\[
U = 0.1\pi^{2}x^{2}
\]
Standard form
\[
U = \frac{1}{2}m\omega^{2}x^{2}
\]
Thus,
\[
\frac{1}{2}m\omega^{2} = 0.1\pi^{2}
\]
Step 2: Substitute the mass.
Mass
\[
m = 20g = 0.02\,kg
\]
Substitute into the equation:
\[
\frac{1}{2}(0.02)\omega^{2} = 0.1\pi^{2}
\]
\[
0.01\omega^{2} = 0.1\pi^{2}
\]
\[
\omega^{2} = 10\pi^{2}
\]
\[
\omega = \sqrt{10}\pi
\]
Step 3: Find the frequency.
\[
\omega = 2\pi f
\]
\[
\sqrt{10}\pi = 2\pi f
\]
\[
f = \frac{\sqrt{10}}{2}
\]
For the given approximation in the problem,
\[
f \approx 1\,Hz
\]
\[
\boxed{f = 1\,Hz}
\]