Question:

Figures 13.20 correspond to two circular motions. The radius of the circle, the period of revolution, the initial position, and the sense of revolution (i.e. clockwise or anti clockwise) are indicated on each figure.
two circular motions
Obtain the corresponding simple harmonic motions of the x-projection of the radius vector of the revolving particle P, in each case.

Updated On: Nov 7, 2023
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Solution and Explanation

Time period, \(T\) = \(2 \,s\)
Amplitude, \(A\) = \(3 \,cm\)
At time, \(t\) = \(0\), the radius vector OP makes an angle \(\frac{\pi}{2}\) with the positive x-axis, i.e., phase angle \(\phi\) =\(+\frac{\pi}{2}\)
Therefore, the equation of simple harmonic motion for the the x-projection of OP, at time t, is given by the displacement equation: 
\(x\) = \(A\cos\bigg[\frac{2\pi t}{T}+\phi\bigg]\)

=\(3\cos\bigg(\frac{2\pi t}{2}+\frac{\pi }{2}\bigg)\)=\(-3\sin\bigg(\frac{2\pi t}{2}\bigg)\)
\(\therefore\) \(x\) =\(-3\sin\pi \; t\; cm\)
Time period, \(T\) =\(4 \,s\)
Amplitude, \(a\) = \(2\,m\)
At time \(t\) = 0, OP makes an angle \(\pi\) with the x-axis, in the anticlockwise direction.
Hence, phase angle, \(\phi\) =\(+\pi\)
Therefore, the equation of simple harmonic motion for the x-projection of OP, at time t, given as:

\(x\) =\(a\cos\bigg(\frac{2\pi t}{T}+\phi\bigg)\)\(2\cos\bigg(\frac{2\pi t}{4+\pi}\bigg)\)

\(\therefore\) \(x\) =\(-2\cos\bigg(\frac{\pi}{2} t\bigg)m\)

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Concepts Used:

Simple Harmonic Motion

Simple Harmonic Motion is one of the most simple forms of oscillatory motion that occurs frequently in nature. The quantity of force acting on a particle in SHM is exactly proportional to the displacement of the particle from the equilibrium location. It is given by F = -kx, where k is the force constant and the negative sign indicates that force resists growth in x.

This force is known as the restoring force, and it pulls the particle back to its equilibrium position as opposing displacement increases. N/m is the SI unit of Force.

Types of Simple Harmonic Motion

Linear Simple Harmonic Motion:

When a particle moves to and fro about a fixed point (called equilibrium position) along with a straight line then its motion is called linear Simple Harmonic Motion. For Example spring-mass system

Conditions:

The restoring force or acceleration acting on the particle should always be proportional to the displacement of the particle and directed towards the equilibrium position.

  • – displacement of particle from equilibrium position.
  • – Restoring force
  • - acceleration

Angular Simple Harmonic Motion:

When a system oscillates angular long with respect to a fixed axis then its motion is called angular simple harmonic motion.

Conditions:

The restoring torque (or) Angular acceleration acting on the particle should always be proportional to the angular displacement of the particle and directed towards the equilibrium position.

Τ ∝ θ or α ∝ θ

Where,

  • Τ – Torque
  • α angular acceleration
  • θ – angular displacement