Question:

The displacement of a particle is given at time $t$, by $x=A \sin (-2 \omega t)+B \sin ^{2} \omega t$ Then

Updated On: Jun 13, 2023
  • the motion of the particle is SHM with an amplitude of $\sqrt{A^{2}+\frac{B^{2}}{4}}$
  • the motion of the particle is not SHM, but oscillatory with a time period of $T = \pi \omega$
  • the motion of the particle is oscillatory with a time period of $T = \pi \, 2\omega$
  • the motion of the particle is a periodic.
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The Correct Option is A

Solution and Explanation

The displacement of the particle is given by
$x=A \sin (-2 \omega t)+B \sin ^{2} \omega t$
$=-A \sin 2 \omega t+\frac{B}{2}(1-\cos 2 \omega t)$
$=-\left(A \sin 2 \omega t+\frac{B}{2} \cos 2 \omega t\right)+\frac{B}{2}$
This motion represents $S H M$ with an amplitude
$\sqrt{A^{2}+\frac{B}{4}}$ and mean position
$\sqrt{\frac{B}{2}}$.
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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