Verified Solution • 2025–26 Session moderate

QJEEM25Phd41f: JEE Main 2025 Physics - Class 11 JEEM25Phd41f Solution: A solid sphere of mass ' ' and radius ' ' is allowed to roll…

A solid sphere of mass ' mm ' and radius ' rr ' is allowed to roll without slipping from the highest point of an inclined plane of length ' LL ' and makes an angle 30∘30^{\circ} with the horizontal. The speed of the particle at the bottom of the plane is v1v_1 . If the angle of inclination is increased to 45∘45^{\circ} while keeping LL constant. Then the new speed of the sphere at the bottom of the plane is v2v_2 . The ratio v12:v22v_1^2: v_2^2 is

Multiple Choice Options

  • A 1:31: 3
  • B 1:21: 2
  • C 1:21: \sqrt{2}
  • D 1:31: \sqrt{3}

Step-by-Step Verified Solution

Let's analyze the problem step-by-step.

Energy conservation:

When the sphere rolls without slipping, its gravitational potential energy converts into both translational and rotational kinetic energy. The energy conservation equation is given by:

mgLsin⁡θ=12mv2+12Iω2mgL\sin\theta = \frac{1}{2}mv^2 + \frac{1}{2}I\omega^2

where:

Lsin⁡θL\sin\theta is the vertical height,

II is the moment of inertia, and

ω\omega is the angular speed.

Moment of Inertia and Rolling Condition:

For a solid sphere, the moment of inertia about its center is:

I=25mr2I = \frac{2}{5}mr^2

Since the sphere rolls without slipping, the linear speed vv and the angular speed ω\omega are related by:

v=rω⇒ω=vrv = r\omega \quad \Rightarrow \quad \omega = \frac{v}{r}

Total Kinetic Energy:

Substituting the rolling condition into the rotational kinetic energy gives:

Kamp;=12mv2+12(25mr2)(vr)2amp;=12mv2+12(25mr2)v2r2amp;=12mv2+15mv2amp;=710mv2\begin{aligned} K &= \frac{1}{2}mv^2 + \frac{1}{2}\left(\frac{2}{5}mr^2\right) \left(\frac{v}{r}\right)^2 \\ &= \frac{1}{2}mv^2 + \frac{1}{2}\left(\frac{2}{5}mr^2\right) \frac{v^2}{r^2} \\ &= \frac{1}{2}mv^2 + \frac{1}{5}mv^2 \\ &= \frac{7}{10}mv^2 \end{aligned}

Finding v2v^2 in Terms of LL and sin⁡θ\sin\theta :

Equate the initial potential energy to the final kinetic energy:

mgLsin⁡θ=710mv2mgL\sin\theta = \frac{7}{10}mv^2

Solving for v2v^2 :

v2=107gLsin⁡θv^2 = \frac{10}{7}gL\sin\theta

Apply to the Two Cases:

For θ=30∘\theta = 30^\circ , since sin⁡(30∘)=12\sin(30^\circ) = \frac{1}{2} :

v12=107gL(12)=57gLv_1^2 = \frac{10}{7}gL\left(\frac{1}{2}\right) = \frac{5}{7}gL

For θ=45∘\theta = 45^\circ , since sin⁡(45∘)=12\sin(45^\circ) = \frac{1}{\sqrt{2}} :

v22=107gL(12)v_2^2 = \frac{10}{7}gL\left(\frac{1}{\sqrt{2}}\right)

Calculate the Ratio v12v22\frac{v_1^2}{v_2^2} :

v12v22amp;=(57gL)(107gL12)amp;=5102amp;=22\begin{aligned} \frac{v_1^2}{v_2^2} &= \frac{\left(\frac{5}{7}gL\right)}{\left(\frac{10}{7}gL\frac{1}{\sqrt{2}}\right)} \\ &= \frac{5}{10}\sqrt{2} \\ &= \frac{\sqrt{2}}{2} \end{aligned}

Expressing this ratio as v12:v22v_1^2 : v_2^2 , we have:

v12:v22=1:2v_1^2 : v_2^2 = 1 : \sqrt{2}

Conclusion:

According to the options given, the correct answer is:

Option C: 1:21:\sqrt{2} .

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