NVAMediumJEE 2026Kinetic Energy & Work-Energy Theorem

JEE Physics 2026 Question with Solution

A flywheel having mass 3kg3\,kg and radius 5m5\,m is free to rotate about a horizontal axis. A string having negligible mass is wound around the wheel and the loose end of the string is connected to a 3kg3\,kg mass. The mass is kept initially and released. Kinetic energy of the flywheel when the mass descends by 3m3\,m is _____ J. (g=10ms2)\left(g=10\,m\,s^{-2}\right)

% Given Given: M=3kg,R=5m,m=3kg,h=3m,g=10ms2M = 3\,kg, \quad R = 5\,m, \quad m = 3\,kg, \quad h = 3\,m, \quad g = 10\,m\,s^{-2}

Answer

Correct answer:30

Step-by-step solution

Standard Method

Given: M=3kgM = 3\,kg, R=5mR = 5\,m, m=3kgm = 3\,kg, h=3mh = 3\,m, g=10ms2g = 10\,m\,s^{-2}

Find: Kinetic energy of the flywheel after the mass descends by 3m3\,m.

Concept: The loss in gravitational potential energy of the falling mass is converted into translational kinetic energy of the mass and rotational kinetic energy of the flywheel.

Moment of inertia of the flywheel is

I=12MR2I=\frac{1}{2}MR^2

Apply energy conservation:

mgh=12mv2+12Iω2mgh=\frac{1}{2}mv^2+\frac{1}{2}I\omega^2

Loss in potential energy:

mgh=3×10×3=90 Jmgh = 3 \times 10 \times 3 = 90\ \text{J}

Relate linear and angular speed:

v=Rωω=vRv=R\omega \Rightarrow \omega=\frac{v}{R}

Substitute moment of inertia:

I=12(3)(5)2=752I=\frac{1}{2}(3)(5)^2=\frac{75}{2}

Now put these into the energy equation:

90=12(3)v2+12(752)(v5)290=\frac{1}{2}(3)v^2+\frac{1}{2}\left(\frac{75}{2}\right)\left(\frac{v}{5}\right)^2 90=32v2+754v22590=\frac{3}{2}v^2+\frac{75}{4}\cdot\frac{v^2}{25} 90=32v2+34v290=\frac{3}{2}v^2+\frac{3}{4}v^2 90=94v290=\frac{9}{4}v^2 v2=40v^2=40

Kinetic energy of the flywheel:

Kflywheel=12Iω2K_{\text{flywheel}}=\frac{1}{2}I\omega^2 Kflywheel=127524025K_{\text{flywheel}}=\frac{1}{2}\cdot\frac{75}{2}\cdot\frac{40}{25} Kflywheel=30 JK_{\text{flywheel}}=30\ \text{J}

Therefore, the kinetic energy of the flywheel is 30J30\,\text{J}.

Energy Split Explanation

Given: A falling mass of 3kg3\,kg is attached to a flywheel of mass 3kg3\,kg and radius 5m5\,m.

Find: The rotational kinetic energy gained by the flywheel.

The total gravitational potential energy lost is

90 J90\ \text{J}

This energy is shared between:

  1. Translational kinetic energy of the hanging mass
  2. Rotational kinetic energy of the flywheel

Because the string does not slip,

v=Rωv=R\omega

so both kinetic energy terms can be written using the same speed variable.

Using

I=12MR2=752I=\frac{1}{2}MR^2=\frac{75}{2}

we get

12Iω2=12752v225=34v2\frac{1}{2}I\omega^2=\frac{1}{2}\cdot\frac{75}{2}\cdot\frac{v^2}{25}=\frac{3}{4}v^2

Also,

12mv2=32v2\frac{1}{2}mv^2=\frac{3}{2}v^2

Hence the energy equation becomes

90=32v2+34v2=94v290=\frac{3}{2}v^2+\frac{3}{4}v^2=\frac{9}{4}v^2

which gives

v2=40v^2=40

Then the flywheel kinetic energy is

34v2=34×40=30 J\frac{3}{4}v^2=\frac{3}{4}\times 40=30\ \text{J}

Therefore, the required kinetic energy is 30J30\,\text{J}.

Common mistakes

  • Using only mgh=12mv2mgh=\frac{1}{2}mv^2 is incorrect because part of the lost potential energy goes into rotational kinetic energy of the flywheel. Always include both translational and rotational terms.

  • Taking the moment of inertia incorrectly is a common error. For a solid disc flywheel, use I=12MR2I=\frac{1}{2}MR^2, not MR2MR^2.

  • Forgetting the no-slip relation v=Rωv=R\omega gives mismatched linear and angular quantities. First connect vv and ω\omega before substituting into the energy equation.

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