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Simple Harmonic Motion question

2016 · 9 Apr · Shift 1 · Q61
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  5. /2016 · 9 Apr · Shift 1 · Q61

Simple Harmonic Motion question

2016 · 9 Apr · Shift 1 · Q61

JEE MainPhysicsSimple Harmonic MotionMCQ+4 / −1
Two particles are performing simple harmonic motion in a straight line about the same equilibrium point. The amplitude and time period for both particles are same and equal to A and I, respectively. At time t = 0 one particle has displacement A while the other one has displacement −A2{{ - A} \over 2}2−A​ and they are moving towards each other. If they cross each other at time t, then t is :
  1. A
    T6{T \over 6}6T​
  2. B
    5T6{5T \over 6}65T​
  3. C
    T3{T \over 3}3T​
  4. D
    T4{T \over 4}4T​
View written solutionFree

Correct answer: A

  1. Write the SHM equations

Since both particles have the same amplitude AAA and time period TTT, they also have the same angular frequency ω=2πT.\omega = \frac{2\pi}{T}.ω=T2π​.

Let the displacements be x1=Acos⁡(ωt+ϕ1),x2=Acos⁡(ωt+ϕ2).x_1 = A\cos(\omega t + \phi_1), \qquad x_2 = A\cos(\omega t + \phi_2).x1​=Acos(ωt+ϕ1​),x2​=Acos(ωt+ϕ2​).


  1. Use initial conditions at t=0t=0t=0

For the first particle, at t=0t=0t=0 its displacement is AAA: x1(0)=Acos⁡ϕ1=A  ⟹  cos⁡ϕ1=1.x_1(0)=A\cos\phi_1=A \implies \cos\phi_1=1.x1​(0)=Acosϕ1​=A⟹cosϕ1​=1. So we can take ϕ1=0,\phi_1=0,ϕ1​=0, and hence x1=Acos⁡ωt.x_1=A\cos\omega t.x1​=Acosωt.

For the second particle, at t=0t=0t=0 its displacement is −A2-\dfrac{A}{2}−2A​: x2(0)=Acos⁡ϕ2=−A2  ⟹  cos⁡ϕ2=−12.x_2(0)=A\cos\phi_2=-\frac{A}{2} \implies \cos\phi_2=-\frac12.x2​(0)=Acosϕ2​=−2A​⟹cosϕ2​=−21​. Thus, ϕ2=2π3or4π3.\phi_2=\frac{2\pi}{3} \quad \text{or} \quad \frac{4\pi}{3}.ϕ2​=32π​or34π​.


  1. Use the condition “moving towards each other”

Velocity is v=dxdt=−Aωsin⁡(ωt+ϕ).v = \frac{dx}{dt} = -A\omega \sin(\omega t+\phi).v=dtdx​=−Aωsin(ωt+ϕ).

At t=0t=0t=0:

  • For particle 1, v1(0)=−Aωsin⁡0=0.v_1(0)=-A\omega\sin 0=0.v1​(0)=−Aωsin0=0. It is at extreme position x=Ax=Ax=A, so immediately after t=0t=0t=0 it moves leftward.

  • For particle 2: v2(0)=−Aωsin⁡ϕ2.v_2(0)=-A\omega\sin\phi_2.v2​(0)=−Aωsinϕ2​. To move towards particle 1 initially, since particle 2 starts at x=−A/2x=-A/2x=−A/2 (to the left of particle 1), it must move rightward, so we need v2(0)>0  ⟹  −sin⁡ϕ2>0  ⟹  sin⁡ϕ2<0.v_2(0)>0 \implies -\sin\phi_2>0 \implies \sin\phi_2<0.v2​(0)>0⟹−sinϕ2​>0⟹sinϕ2​<0. Among the two possible phases, this happens for ϕ2=4π3.\phi_2=\frac{4\pi}{3}.ϕ2​=34π​.

Therefore, x2=Acos⁡(ωt+4π3).x_2=A\cos\left(\omega t+\frac{4\pi}{3}\right).x2​=Acos(ωt+34π​).


  1. Condition for crossing each other

They cross when their displacements are equal: x1=x2.x_1=x_2.x1​=x2​. So, Acos⁡ωt=Acos⁡(ωt+4π3).A\cos\omega t = A\cos\left(\omega t+\frac{4\pi}{3}\right).Acosωt=Acos(ωt+34π​). Cancelling AAA, cos⁡ωt=cos⁡(ωt+4π3).\cos\omega t = \cos\left(\omega t+\frac{4\pi}{3}\right).cosωt=cos(ωt+34π​).

Using cos⁡α=cos⁡β  ⟹  α=2nπ±β,\cos \alpha = \cos \beta \implies \alpha = 2n\pi \pm \beta,cosα=cosβ⟹α=2nπ±β, we take the nontrivial case: ωt=−(ωt+4π3)+2nπ.\omega t = -\left(\omega t+\frac{4\pi}{3}\right)+2n\pi.ωt=−(ωt+34π​)+2nπ. Thus, 2ωt=2nπ−4π3.2\omega t = 2n\pi - \frac{4\pi}{3}.2ωt=2nπ−34π​. ωt=nπ−2π3.\omega t = n\pi - \frac{2\pi}{3}.ωt=nπ−32π​.

For the first positive time, take n=1n=1n=1: ωt=π−2π3=π3.\omega t = \pi - \frac{2\pi}{3} = \frac{\pi}{3}.ωt=π−32π​=3π​. Hence, t=π/3ω=π/32π/T=T6.t=\frac{\pi/3}{\omega} = \frac{\pi/3}{2\pi/T} = \frac{T}{6}.t=ωπ/3​=2π/Tπ/3​=6T​.


  1. Check with options

t=T6t=\frac{T}{6}t=6T​ which corresponds to Option A.


  1. Comparison with stored answer

Stored correct answer: A

Our derived answer: A

So the answer agrees with the stored correct answer.

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