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Rotational Motion question

2022 · 26 Jul · Shift 1 · Q65
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  5. /2022 · 26 Jul · Shift 1 · Q65

Rotational Motion question

2022 · 26 Jul · Shift 1 · Q65

JEE MainPhysicsRotational MotionNumerical+4 / −1
A disc of mass 1 kg1 \mathrm{~kg}1 kg and radius R\mathrm{R}R is free to rotate about a horizontal axis passing through its centre and perpendicular to the plane of disc. A body of same mass as that of disc is fixed at the highest point of the disc. Now the system is released, when the body comes to the lowest position, its angular speed will be 4x3R rad⁡s−14 \sqrt{\frac{x}{3 R}} \,\operatorname{rad}{s}^{-1}43Rx​​rads−1 where x=‾x=\underline{\hspace{2cm}}x=​. (g=10 ms−2)\left(g=10 \mathrm{~ms}^{-2}\right)(g=10 ms−2)
Numerical answer
View written solutionFree

Correct answer: 5

  1. Given system
  • Mass of disc =1 kg= 1\,\text{kg}=1kg
  • Radius of disc =R= R=R
  • A body of mass 1 kg1\,\text{kg}1kg is fixed at the highest point on the rim.
  • Axis passes through the centre of the disc and is perpendicular to the plane of the disc.

We need the angular speed when the attached body reaches the lowest point.


  1. Use conservation of mechanical energy

Initially, the attached mass is at the top of the disc. Finally, it comes to the bottom.

So the attached mass falls through a vertical distance: 2R2R2R

Hence loss in gravitational potential energy is ΔU=mg(2R)=(1)(10)(2R)=20R\Delta U = mg(2R) = (1)(10)(2R)=20RΔU=mg(2R)=(1)(10)(2R)=20R

This becomes rotational kinetic energy of the whole system.


  1. Find total moment of inertia about the axis

(a) Disc

Moment of inertia of a disc about its central axis: Idisc=12MR2=12(1)R2=R22I_{\text{disc}} = \frac{1}{2}MR^2 = \frac{1}{2}(1)R^2=\frac{R^2}{2}Idisc​=21​MR2=21​(1)R2=2R2​

(b) Attached body

It is a point mass of 1 kg1\,\text{kg}1kg at distance RRR from the axis, so Imass=mR2=(1)R2=R2I_{\text{mass}} = mR^2 = (1)R^2 = R^2Imass​=mR2=(1)R2=R2

(c) Total

Itotal=R22+R2=3R22I_{\text{total}} = \frac{R^2}{2}+R^2 = \frac{3R^2}{2}Itotal​=2R2​+R2=23R2​


  1. Apply energy conservation

At the lowest position, 12Itotalω2=20R\frac{1}{2}I_{\text{total}}\omega^2 = 20R21​Itotal​ω2=20R

Substitute Itotal=3R22I_{\text{total}}=\frac{3R^2}{2}Itotal​=23R2​: 12(3R22)ω2=20R\frac{1}{2}\left(\frac{3R^2}{2}\right)\omega^2=20R21​(23R2​)ω2=20R

3R24ω2=20R\frac{3R^2}{4}\omega^2=20R43R2​ω2=20R

ω2=803R\omega^2=\frac{80}{3R}ω2=3R80​

ω=803R=453R\omega=\sqrt{\frac{80}{3R}}=4\sqrt{\frac{5}{3R}}ω=3R80​​=43R5​​


  1. Compare with given form

Given: ω=4x3R\omega = 4\sqrt{\frac{x}{3R}}ω=43Rx​​

From our result: ω=453R\omega = 4\sqrt{\frac{5}{3R}}ω=43R5​​

So, x=5x=5x=5


  1. Comparison with stored answer

Stored correct answer: 555

Our derived answer: 555

They match.

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