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Rotational Motion question

2024 · 1 Feb · Shift 2 · Q89
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  5. /2024 · 1 Feb · Shift 2 · Q89

Rotational Motion question

2024 · 1 Feb · Shift 2 · Q89

JEE MainPhysicsRotational MotionNumerical+4 / −1
A uniform rod ABA BAB of mass 2 kg2 \mathrm{~kg}2 kg and length 30 cm30 \mathrm{~cm}30 cm at rest on a smooth horizontal surface. An impulse of force 0.2 Ns0.2 \mathrm{~Ns}0.2 Ns is applied to end B. The time taken by the rod to turn through at right angles will be πx s\frac{\pi}{x} \mathrm{~s}xπ​ s, where x=‾x=\underline{\hspace{2cm}}x=​ .
Numerical answer
View written solutionFree

Correct answer: 4

  1. Given data
  • Mass of rod: m=2 kgm = 2\,\text{kg}m=2kg
  • Length of rod: L=30 cm=0.30 mL = 30\,\text{cm} = 0.30\,\text{m}L=30cm=0.30m
  • Impulse applied at end BBB: J=0.2 N sJ = 0.2\,\text{N s}J=0.2N s
  • Rod is on a smooth horizontal surface, so after the impulse it undergoes:
    • translation of center of mass
    • rotation about center of mass

We need the time taken for the rod to rotate through 90∘=π290^\circ = \dfrac{\pi}{2}90∘=2π​.


  1. Angular impulse about the center of mass

The impulse is applied at the end of the rod, so its perpendicular distance from the center is

r=L2=0.302=0.15 mr = \frac{L}{2} = \frac{0.30}{2} = 0.15\,\text{m}r=2L​=20.30​=0.15m

Angular impulse about center of mass:

Jang=rJ=0.15×0.2=0.03 kg m2/sJ_{\text{ang}} = rJ = 0.15 \times 0.2 = 0.03\,\text{kg m}^2/\text{s}Jang​=rJ=0.15×0.2=0.03kg m2/s

This equals the angular momentum gained:

Iω=0.03I\omega = 0.03Iω=0.03


  1. Moment of inertia of rod about its center

For a uniform rod about an axis through its center and perpendicular to its length:

I=112mL2I = \frac{1}{12}mL^2I=121​mL2

So,

I=112(2)(0.30)2=212×0.09=0.015 kg m2I = \frac{1}{12}(2)(0.30)^2 = \frac{2}{12}\times 0.09 = 0.015\,\text{kg m}^2I=121​(2)(0.30)2=122​×0.09=0.015kg m2

Thus,

0.015 ω=0.030.015\,\omega = 0.030.015ω=0.03

ω=0.030.015=2 rad/s\omega = \frac{0.03}{0.015} = 2\,\text{rad/s}ω=0.0150.03​=2rad/s


  1. Time to rotate through 90∘90^\circ90∘

After the impulse, no external torque acts, so angular velocity remains constant at ω=2 rad/s\omega = 2\,\text{rad/s}ω=2rad/s.

Required angular displacement:

θ=π2\theta = \frac{\pi}{2}θ=2π​

Using

θ=ωt\theta = \omega tθ=ωt

t=θω=π/22=π4 st = \frac{\theta}{\omega} = \frac{\pi/2}{2} = \frac{\pi}{4}\,\text{s}t=ωθ​=2π/2​=4π​s

Given that

t=πx st = \frac{\pi}{x} \text{ s}t=xπ​ s

So,

πx=π4⇒x=4\frac{\pi}{x} = \frac{\pi}{4} \Rightarrow x = 4xπ​=4π​⇒x=4


  1. Comparison with stored answer

Derived answer: 444

Stored correct answer: 444

They match.

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