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): \(\frac 14E\)
The center of a disk of radius $ r $ and mass $ m $ is attached to a spring of spring constant $ k $, inside a ring of radius $ R>r $ as shown in the figure. The other end of the spring is attached on the periphery of the ring. Both the ring and the disk are in the same vertical plane. The disk can only roll along the inside periphery of the ring, without slipping. The spring can only be stretched or compressed along the periphery of the ring, following Hooke’s law. In equilibrium, the disk is at the bottom of the ring. Assuming small displacement of the disc, the time period of oscillation of center of mass of the disk is written as $ T = \frac{2\pi}{\omega} $. The correct expression for $ \omega $ is ( $ g $ is the acceleration due to gravity):
AB is a part of an electrical circuit (see figure). The potential difference \(V_A - V_B\), at the instant when current \(i = 2\) A and is increasing at a rate of 1 amp/second is:
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.