4n
n
2n
3n
To solve this problem, we need to understand how the frequency of potential energy relates to the frequency of an object in simple harmonic motion (SHM).
In SHM, the displacement \( x \) of the body can be expressed as:
\(x = A \cos(\omega t + \phi)\)
where:
The potential energy \( U \) in SHM is given by:
\(U = \frac{1}{2} k x^2\)
where \( k \) is the spring constant.
Substituting the expression for \( x \) in the potential energy formula, we get:
\(U = \frac{1}{2} k (A \cos(\omega t + \phi))^2\)
\(U = \frac{1}{2} k A^2 \cos^2(\omega t + \phi)\)
Recall the trigonometric identity:
\(\cos^2(\theta) = \frac{1 + \cos(2\theta)}{2}\)
Using this identity, the potential energy becomes:
\(U = \frac{1}{2} k A^2 \cdot \frac{1 + \cos(2\omega t + 2\phi)}{2}\)
Simplifying:
\(U = \frac{1}{4} k A^2 + \frac{1}{4} k A^2 \cos(2\omega t + 2\phi)\)
This shows that the potential energy oscillates with a frequency that is twice the frequency of the displacement.
Therefore, if the frequency of the SHM is \( n \), then the frequency of the potential energy is \( 2n \).
Hence, the correct answer is 2n.