Question:

A particle executes simple harmonic motion between $x=- A$ and $x=+ A$. If time taken by particle to go from $x=0$ to $\frac{A}{2}$ is 2 s; then time taken by particle in going from $x=\frac{A}{2}$ to $A$ is

Updated On: Apr 28, 2025
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The Correct Option is C

Approach Solution - 1

The correct answer is (C) : 4s

Let time from 0 to is
from to is
then


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Approach Solution -2

Let's consider a particle undergoing simple harmonic motion (SHM). Understanding the Problem: We are given that the time taken for the particle to travel from its equilibrium position (0) to half of its amplitude (A/2) is denoted as $t_1$. The time taken for the particle to travel from A/2 to the full amplitude (A) is denoted as $t_2$. Key Concepts: SHM Equation: The displacement of a particle in SHM is often described by the equation $x(t) = A \sin(\omega t)$, where:
$x(t)$ is the displacement at time $t$
$A$ is the amplitude
$\omega$ is the angular frequency Derivation: 1. Time to reach A/2:
When the particle is at A/2, we have:
$$\frac{A}{2} = A \sin(\omega t_1)$$
$$\frac{1}{2} = \sin(\omega t_1)$$
$$\omega t_1 = \sin^{-1}(\frac{1}{2}) = \frac{\pi}{6}$$
2. Time to reach A:
When the particle is at A, we have:
$$A = A \sin(\omega (t_1 + t_2))$$
$$1 = \sin(\omega (t_1 + t_2))$$
$$\omega (t_1 + t_2) = \sin^{-1}(1) = \frac{\pi}{2}$$
We also know that the time to reach A/2 from 0 is $\omega t_1 = \frac{\pi}{6}$.
The time to reach A from A/2 can be written as:
$$\omega t_2 = \omega (t_1 + t_2) - \omega t_1 = \frac{\pi}{2} - \frac{\pi}{6} = \frac{\pi}{3}$$
3. Ratio of Times:
We can find the ratio of $t_1$ to $t_2$:
$$\frac{\omega t_1}{\omega t_2} = \frac{\pi/6}{\pi/3} = \frac{1}{2}$$
$$\frac{t_1}{t_2} = \frac{1}{2}$$
4. Finding t2:
We are given that $t_1 = 2$ seconds.
Using the ratio, we can find $t_2$:
$$t_2 = 2 t_1 = 2 \times 2 = 4 \text{ seconds}$$ Conclusion: The time taken for the particle to travel from A/2 to A is 4 seconds.
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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