The potential energy (U) of a simple harmonic oscillator as a function of its displacement (x) from the equilibrium position is given by:
\(U =\frac 12kx^2\)
In the case of a simple harmonic oscillator, the maximum displacement (amplitude) is given by A, and when the particle is halfway to its endpoint, the displacement is \(\frac A2\).
So, the potential energy at this point is:
\(U = \frac 12k(\frac A2)^2\)
\(U = \frac 12k(\frac{ A^2}{4})\)
\(U = \frac 18kA^2\)
The total energy (E) of the simple harmonic oscillator is given by:
\(E = \frac 12kA^2\)
Now, to find the potential energy when the particle is halfway to its endpoint, we can substitute the expression for E:
\(\frac UE\)= \(\frac {\frac 18kA^2 }{ \frac 12kA^2}\)
\(\frac UE\)= \(\frac {\frac18}{\frac 12}\)
\(\frac UE\) = \(\frac 14\)
\(U\) = \(\frac 14E\)
So, the correct option is (C): \(\frac 14E\)
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.