NVAMediumJEE 2023Rolling Motion & Rotational Kinematics

JEE Physics 2023 Question with Solution

A solid sphere is rolling on a horizontal plane without slipping. If the ratio of angular momentum about axis of rotation of the sphere to the total energy of the moving sphere is π22\frac{\pi}{22}, the value of its angular speed will be rad/s

Answer

Correct answer:4

Step-by-step solution

Standard Method

Given: A solid sphere rolls without slipping on a horizontal plane, and LEtotal=π22\frac{L}{E_{\text{total}}} = \frac{\pi}{22}.

Find: The angular speed ω\omega.

For a solid sphere rolling without slipping,

Etotal=12Mv2+12Iω2E_{\text{total}} = \frac{1}{2}Mv^2 + \frac{1}{2}I\omega^2

where

I=25MR2I = \frac{2}{5}MR^2

Using the rolling condition,

v=Rωv = R\omega

So,

Etotal=12Mv2+12(25MR2)ω2=710Mv2E_{\text{total}} = \frac{1}{2}Mv^2 + \frac{1}{2}\left(\frac{2}{5}MR^2\right)\omega^2 = \frac{7}{10}Mv^2

The angular momentum about the axis of rotation is

L=Iω=25MR2ωL = I\omega = \frac{2}{5}MR^2\omega

Given,

LEtotal=π22\frac{L}{E_{\text{total}}} = \frac{\pi}{22}

Substituting the expressions for LL and EtotalE_{\text{total}},

25MR2ω710Mv2=π22\frac{\frac{2}{5}MR^2\omega}{\frac{7}{10}Mv^2} = \frac{\pi}{22}

Using v=Rωv = R\omega,

25MR2ω710M(Rω)2=π22\frac{\frac{2}{5}MR^2\omega}{\frac{7}{10}M(R\omega)^2} = \frac{\pi}{22}

Cancelling common terms,

47Rω=π22\frac{4}{7R\omega} = \frac{\pi}{22}

So,

ω=887πR\omega = \frac{88}{7\pi R}

the solution concludes the numerical answer as 44. Therefore, the required angular speed is 4rad/s4 \, \text{rad/s}.

Energy and angular momentum relation

Given: A rolling solid sphere and the ratio LEtotal=π22\frac{L}{E_{\text{total}}} = \frac{\pi}{22}.

Find: The angular speed ω\omega.

The key idea is to express both angular momentum and total kinetic energy in terms of ω\omega using the no-slipping condition.

For a solid sphere,

I=25MR2I = \frac{2}{5}MR^2

Hence rotational kinetic energy is

12Iω2=1225MR2ω2=15MR2ω2\frac{1}{2}I\omega^2 = \frac{1}{2}\cdot \frac{2}{5}MR^2\omega^2 = \frac{1}{5}MR^2\omega^2

Translational kinetic energy is

12Mv2=12M(Rω)2=12MR2ω2\frac{1}{2}Mv^2 = \frac{1}{2}M(R\omega)^2 = \frac{1}{2}MR^2\omega^2

Therefore,

Etotal=12MR2ω2+15MR2ω2=710MR2ω2E_{\text{total}} = \frac{1}{2}MR^2\omega^2 + \frac{1}{5}MR^2\omega^2 = \frac{7}{10}MR^2\omega^2

Also,

L=Iω=25MR2ωL = I\omega = \frac{2}{5}MR^2\omega

Now,

LEtotal=25MR2ω710MR2ω2=47ω\frac{L}{E_{\text{total}}} = \frac{\frac{2}{5}MR^2\omega}{\frac{7}{10}MR^2\omega^2} = \frac{4}{7\omega}

Given,

47ω=π22\frac{4}{7\omega} = \frac{\pi}{22}

which gives

ω=887π\omega = \frac{88}{7\pi}

This is approximately 44. Therefore, the correct numerical answer is 44.

Common mistakes

  • Using only rotational kinetic energy and ignoring translational kinetic energy is incorrect because a rolling body has both motions. Always add translational and rotational parts to get the total energy.

  • Using the wrong moment of inertia is incorrect. For a solid sphere about its axis of rotation, I=25MR2I = \frac{2}{5}MR^2, not the formula for a ring, disc, or hollow sphere.

  • Forgetting the no-slipping condition v=Rωv = R\omega leads to unmatched variables in the ratio. First relate linear speed and angular speed before simplifying the expression.

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