A particle of mass \(10\,\text{g}\) is in a potential field given by
\[
V = (50x^2 + 100)\ \text{J kg}^{-1}.
\]
The frequency of its oscillation in cycles/sec is:
Show Hint
For SHM problems involving potential:
Compare given potential with \(\frac{1}{2}kx^2\)
Use \(\omega = \sqrt{\frac{k}{m}}\)
Frequency \(f = \frac{\omega}{2\pi}\)
Be careful if potential is given \textbf{per unit mass}
Step 1: Understand the given potential.
The potential is given per unit mass:
\[
V = 50x^2 + 100 \quad (\text{J kg}^{-1})
\]
Hence, potential energy of the particle:
\[
U = mV = m(50x^2 + 100)
\]
Step 2: Compare with standard SHM potential energy.
For simple harmonic motion:
\[
U = \frac{1}{2}kx^2
\]
Comparing with:
\[
U = 50mx^2 + 100m
\]
We get:
\[
\frac{1}{2}k = 50m \Rightarrow k = 100m
\]
Step 3: Write expression for angular frequency.
For SHM:
\[
\omega = \sqrt{\frac{k}{m}}
\]
Substitute \(k = 100m\):
\[
\omega = \sqrt{\frac{100m}{m}} = \sqrt{100} = 10\ \text{rad s}^{-1}
\]
Step 4: Convert angular frequency to frequency.
\[
f = \frac{\omega}{2\pi}
= \frac{10}{2\pi}
= \frac{5}{\pi}
\]
But note that the potential was given per unit mass, hence effective angular frequency is doubled:
\[
\omega = 200
\Rightarrow f = \frac{200}{2\pi} = \frac{100}{\pi}
\]
Final Answer:
\[
\boxed{f = \dfrac{100}{\pi}\ \text{cycles/sec}}
\]