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Simple Harmonic Motion question

2014 · Shift 0 · Q62
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Simple Harmonic Motion question

2014 · Shift 0 · Q62

JEE MainPhysicsSimple Harmonic MotionMCQ+4 / −1
A particle moves with simple harmonic motion in a straight line. In first τs,\tau s,τs, after starting from rest it travels a distance a,a,a, and in next τs\tau sτs it travels 2a,2a,2a, in same direction, then:
  1. A
    amplitude of motion is 3a3a3a
  2. B
    time period of oscillations is 8τ8\tau8τ
  3. C
    amplitude of motion is 4a4a4a
  4. D
    time period of oscillations is 6τ6\tau6τ
View written solutionFree

Correct answer: D

  1. Interpret the initial condition

Since the particle starts from rest in SHM, it must start from an extreme position.

So let the particle start from x=+Ax = +Ax=+A at t=0t=0t=0.

A convenient SHM equation is: x=Acos⁡(ωt)x = A\cos(\omega t)x=Acos(ωt) with velocity v=−Aωsin⁡(ωt)v = -A\omega \sin(\omega t)v=−Aωsin(ωt) which is zero at t=0t=0t=0.


  1. Use the statement about direction

In the first τ\tauτ seconds, it travels distance aaa, and in the next τ\tauτ seconds, it travels distance 2a2a2a, in the same direction.

That means during the total time interval 000 to 2τ2\tau2τ, the particle does not reverse direction.

Starting from x=Ax=Ax=A, initially it moves toward the mean position, so as long as it has not crossed the mean position, motion remains in the same direction.

Hence both intervals lie before reaching the mean position.

So distances are just decreases in position magnitude:

  • from t=0t=0t=0 to t=τt=\taut=τ: A−x(τ)=aA - x(\tau) = aA−x(τ)=a
  • from t=τt=\taut=τ to t=2τt=2\taut=2τ: x(τ)−x(2τ)=2ax(\tau) - x(2\tau) = 2ax(τ)−x(2τ)=2a

Using x(t)=Acos⁡(ωt)x(t)=A\cos(\omega t)x(t)=Acos(ωt): A−Acos⁡(ωτ)=aA - A\cos(\omega\tau)=aA−Acos(ωτ)=a Acos⁡(ωτ)−Acos⁡(2ωτ)=2aA\cos(\omega\tau)-A\cos(2\omega\tau)=2aAcos(ωτ)−Acos(2ωτ)=2a

Let θ=ωτ\theta = \omega\tauθ=ωτ Then: A(1−cos⁡θ)=a(1)A(1-\cos\theta)=a \qquad (1)A(1−cosθ)=a(1) A(cos⁡θ−cos⁡2θ)=2a(2)A(\cos\theta-\cos2\theta)=2a \qquad (2)A(cosθ−cos2θ)=2a(2)


  1. Eliminate aaa using (1)

From (1): a=A(1−cos⁡θ)a=A(1-\cos\theta)a=A(1−cosθ) Substitute into (2): A(cos⁡θ−cos⁡2θ)=2A(1−cos⁡θ)A(\cos\theta-\cos2\theta)=2A(1-\cos\theta)A(cosθ−cos2θ)=2A(1−cosθ) Cancel AAA: cos⁡θ−cos⁡2θ=2(1−cos⁡θ)\cos\theta-\cos2\theta=2(1-\cos\theta)cosθ−cos2θ=2(1−cosθ)

Now use cos⁡2θ=2cos⁡2θ−1\cos2\theta=2\cos^2\theta-1cos2θ=2cos2θ−1 So: cos⁡θ−(2cos⁡2θ−1)=2−2cos⁡θ\cos\theta-(2\cos^2\theta-1)=2-2\cos\thetacosθ−(2cos2θ−1)=2−2cosθ cos⁡θ−2cos⁡2θ+1=2−2cos⁡θ\cos\theta-2\cos^2\theta+1=2-2\cos\thetacosθ−2cos2θ+1=2−2cosθ −2cos⁡2θ+3cos⁡θ−1=0-2\cos^2\theta+3\cos\theta-1=0−2cos2θ+3cosθ−1=0 Multiply by −1-1−1: 2cos⁡2θ−3cos⁡θ+1=02\cos^2\theta-3\cos\theta+1=02cos2θ−3cosθ+1=0 Factorize: (2cos⁡θ−1)(cos⁡θ−1)=0(2\cos\theta-1)(\cos\theta-1)=0(2cosθ−1)(cosθ−1)=0

Thus, cos⁡θ=1orcos⁡θ=12\cos\theta=1 \quad \text{or} \quad \cos\theta=\frac12cosθ=1orcosθ=21​

cos⁡θ=1\cos\theta=1cosθ=1 gives a=0a=0a=0, impossible.

Hence, cos⁡θ=12\cos\theta=\frac12cosθ=21​ So, θ=π3\theta=\frac{\pi}{3}θ=3π​ (since motion is before the mean position, 0<θ<π/20<\theta<\pi/20<θ<π/2).

Thus, ωτ=π3\omega\tau=\frac{\pi}{3}ωτ=3π​


  1. Find the time period

Since ω=2πT\omega=\frac{2\pi}{T}ω=T2π​ we get 2πTτ=π3\frac{2\pi}{T}\tau=\frac{\pi}{3}T2π​τ=3π​ 2τT=13\frac{2\tau}{T}=\frac13T2τ​=31​ T=6τT=6\tauT=6τ

So option D is correct.


  1. Find the amplitude

From (1): a=A(1−12)=A2a=A\left(1-\frac12\right)=\frac{A}{2}a=A(1−21​)=2A​ Hence, A=2aA=2aA=2a

So amplitude is neither 3a3a3a nor 4a4a4a.

Thus:

  • A is false
  • B is false
  • C is false
  • D is true

  1. Final answer

The correct option is: D: time period =6τ\boxed{D:\ \text{time period }=6\tau}D: time period =6τ​

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