4n
n
2n
3n
In simple harmonic motion (SHM), the potential energy (PE) of a body oscillating at a frequency depends on the displacement from its equilibrium position. The potential energy function is given by:
\(PE = \frac{1}{2} k x^2\)
where \(k\) is the spring constant and \(x\) is the displacement.
The displacement \( x \) varies as:
\(x(t) = A \cos(\omega t + \phi)\)
where:
The potential energy can be expressed as:
\(PE = \frac{1}{2} k A^2 \cos^2(\omega t + \phi)\)
This can be rewritten in terms of trigonometric identities:
\(\cos^2(\theta) = \frac{1 + \cos(2\theta)}{2}\)
Thus, the expression becomes:
\(PE = \frac{1}{4} k A^2 (1 + \cos(2\omega t + 2\phi))\)
The term \(\cos(2\omega t + 2\phi)\) suggests that the potential energy oscillates with a frequency of \(2\omega\).
Therefore, since \(\omega = 2\pi n\), the frequency of the potential energy is \(2n\).
Hence, the correct answer is 2n.
Using a variable frequency ac voltage source the maximum current measured in the given LCR circuit is 50 mA for V = 5 sin (100t) The values of L and R are shown in the figure. The capacitance of the capacitor (C) used is_______ µF.

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The output (Y) of the given logic implementation is similar to the output of an/a …………. gate.
We can note there involves a continuous interchange of potential and kinetic energy in a simple harmonic motion. The system that performs simple harmonic motion is called the harmonic oscillator.
Case 1: When the potential energy is zero, and the kinetic energy is a maximum at the equilibrium point where maximum displacement takes place.
Case 2: When the potential energy is maximum, and the kinetic energy is zero, at a maximum displacement point from the equilibrium point.
Case 3: The motion of the oscillating body has different values of potential and kinetic energy at other points.