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Simple Harmonic Motion question

2025 · 24 Jan · Shift 2 · Q70
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  5. /2025 · 24 Jan · Shift 2 · Q70

Simple Harmonic Motion question

2025 · 24 Jan · Shift 2 · Q70

JEE MainPhysicsSimple Harmonic MotionMCQ+4 / −1
A particle oscillates along the xxx-axis according to the law, x(t)=x0sin⁡2(t2)x(\mathrm{t})=x_0 \sin ^2\left(\frac{\mathrm{t}}{2}\right)x(t)=x0​sin2(2t​) where x0=1 mx_0=1 \mathrm{~m}x0​=1 m. The kinetic energy (K)(\mathrm{K})(K) of the particle as a function of xxx is correctly represented by the graph
  1. A
    JEE Main 2025 (Online) 24th January Evening Shift Physics - Simple Harmonic Motion Question 5 English Option 1
  2. B
    JEE Main 2025 (Online) 24th January Evening Shift Physics - Simple Harmonic Motion Question 5 English Option 2
  3. C
    JEE Main 2025 (Online) 24th January Evening Shift Physics - Simple Harmonic Motion Question 5 English Option 3
  4. D
    JEE Main 2025 (Online) 24th January Evening Shift Physics - Simple Harmonic Motion Question 5 English Option 4
View written solutionFree

Correct answer: D

  1. Given motion

The particle moves as x(t)=x0sin⁡2(t2),x0=1 m.x(t)=x_0\sin^2\left(\frac{t}{2}\right), \qquad x_0=1\text{ m}.x(t)=x0​sin2(2t​),x0​=1 m.

Use the identity sin⁡2(t2)=1−cos⁡t2.\sin^2\left(\frac{t}{2}\right)=\frac{1-\cos t}{2}.sin2(2t​)=21−cost​. So, x=x02(1−cos⁡t).x=\frac{x_0}{2}(1-\cos t).x=2x0​​(1−cost).

Hence, cos⁡t=1−2xx0.\cos t=1-\frac{2x}{x_0}.cost=1−x0​2x​.


  1. Find velocity

Differentiate x(t)x(t)x(t): v=dxdt=x0⋅2sin⁡(t2)cos⁡(t2)⋅12.v=\frac{dx}{dt}=x_0\cdot 2\sin\left(\frac{t}{2}\right)\cos\left(\frac{t}{2}\right)\cdot \frac12.v=dtdx​=x0​⋅2sin(2t​)cos(2t​)⋅21​. Thus, v=x0sin⁡(t2)cos⁡(t2)=x02sin⁡t.v=x_0\sin\left(\frac{t}{2}\right)\cos\left(\frac{t}{2}\right)=\frac{x_0}{2}\sin t.v=x0​sin(2t​)cos(2t​)=2x0​​sint.

Therefore, v2=x024sin⁡2t.v^2=\frac{x_0^2}{4}\sin^2 t.v2=4x02​​sin2t.

Now, sin⁡2t=1−cos⁡2t=1−(1−2xx0)2.\sin^2 t=1-\cos^2 t=1-\left(1-\frac{2x}{x_0}\right)^2.sin2t=1−cos2t=1−(1−x0​2x​)2.

So, v2=x024[1−(1−2xx0)2].v^2=\frac{x_0^2}{4}\left[1-\left(1-\frac{2x}{x_0}\right)^2\right].v2=4x02​​[1−(1−x0​2x​)2].

Expand: (1−2xx0)2=1−4xx0+4x2x02.\left(1-\frac{2x}{x_0}\right)^2=1-\frac{4x}{x_0}+\frac{4x^2}{x_0^2}.(1−x0​2x​)2=1−x0​4x​+x02​4x2​. Hence, 1−(1−2xx0)2=4xx0−4x2x02.1-\left(1-\frac{2x}{x_0}\right)^2=\frac{4x}{x_0}-\frac{4x^2}{x_0^2}.1−(1−x0​2x​)2=x0​4x​−x02​4x2​.

Therefore, v2=x024(4xx0−4x2x02)=x0x−x2.v^2=\frac{x_0^2}{4}\left(\frac{4x}{x_0}-\frac{4x^2}{x_0^2}\right)=x_0x-x^2.v2=4x02​​(x0​4x​−x02​4x2​)=x0​x−x2.


  1. Kinetic energy as a function of xxx

K=12mv2=12m(x0x−x2).K=\frac12 mv^2=\frac12 m(x_0x-x^2).K=21​mv2=21​m(x0​x−x2).

Since x0=1x_0=1x0​=1, K=12m(x−x2).K=\frac12 m(x-x^2).K=21​m(x−x2).

This is a quadratic in xxx:

  • opens downward,
  • zero at x=0x=0x=0 and x=1x=1x=1,
  • maximum at x=x02=12.x=\frac{x_0}{2}=\frac12.x=2x0​​=21​.

So the correct graph is an inverted parabola between x=0x=0x=0 and x=1x=1x=1, touching the axis at both ends.


  1. Match with options

That corresponds to Option D.


  1. Comparison with stored answer

Stored correct answer: D

My derived answer: D

They agree.

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