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JEE Advanced 2018 · System of Particles and Rotational Motion

A ring and a disc are initially at rest, side by side, at the top of an inclined plane which makes an angle 60∘60^\circ with the horizontal. They start to roll without slipping at the same instant of time along the shortest path. If the time difference between their reaching the ground is 2−310 s\frac{2-\sqrt{3}}{\sqrt{10}}\,\text{s}, then the height of the top of the inclined plane, in metres, is ________. Take g=10 ms−2g = 10\,\text{ms}^{-2}

Answer: 0.750.75

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Written solution

Step 1: Identify the given parameters.

The given values for the inclined plane and the rolling bodies are:

θ=60∘\theta = 60^\circ Δt=2−310 s\Delta t = \frac{2-\sqrt{3}}{\sqrt{10}}\,\text{s} g=10 ms−2g = 10\,\text{ms}^{-2}

Step 2: Determine the acceleration of a body rolling without slipping.

For a body of mass MM, radius RR, and moment of inertia II rolling down an incline, the equations of motion are:

mgsin⁡θ−f=mamg\sin\theta - f = ma fR=Iα=IaRfR = I\alpha = I\frac{a}{R}

Solving for acceleration aa yields:

a=gsin⁡θ1+IMR2a = \frac{g\sin\theta}{1 + \frac{I}{MR^2}}

Step 3: Calculate the acceleration for the ring and the disc.

For the ring, I=MR2I = MR^2:

ar=gsin⁡θ2a_r = \frac{g\sin\theta}{2}

For the disc, I=12MR2I = \frac{1}{2}MR^2:

ad=23gsin⁡θa_d = \frac{2}{3}g\sin\theta

Step 4: Express the time taken to reach the bottom of the incline.

The length of the path along the incline LL is related to the height hh by:

L=hsin⁡θL = \frac{h}{\sin\theta}

Using the equation of motion from rest, L=12at2L = \frac{1}{2}at^2:

t=2Lat = \sqrt{\frac{2L}{a}}

Step 5: Find the time expressions for both bodies.

Substitute the accelerations into the time formula:

tr=4hgsin⁡2θt_r = \sqrt{\frac{4h}{g\sin^2\theta}} td=3hgsin⁡2θt_d = \sqrt{\frac{3h}{g\sin^2\theta}}

Step 6: Substitute the angle of inclination.

For θ=60∘\theta = 60^\circ, we have sin⁡2θ=34\sin^2\theta = \frac{3}{4}:

tr=16h3g=43hgt_r = \sqrt{\frac{16h}{3g}} = \frac{4}{\sqrt{3}}\sqrt{\frac{h}{g}} td=4hg=2hgt_d = \sqrt{\frac{4h}{g}} = 2\sqrt{\frac{h}{g}}

Step 7: Express the time difference.

Subtract the two times to find the difference:

Δt=tr−td=hg(43−2)\Delta t = t_r - t_d = \sqrt{\frac{h}{g}}\left(\frac{4}{\sqrt{3}} - 2\right) Δt=hg2(2−3)3\Delta t = \sqrt{\frac{h}{g}}\frac{2(2-\sqrt{3})}{\sqrt{3}}

Step 8: Solve for the height hh.

Equate the expression to the given time difference:

hg2(2−3)3=2−310\sqrt{\frac{h}{g}}\frac{2(2-\sqrt{3})}{\sqrt{3}} = \frac{2-\sqrt{3}}{\sqrt{10}} hg=3210\sqrt{\frac{h}{g}} = \frac{\sqrt{3}}{2\sqrt{10}}

Square both sides and substitute g=10 ms−2g = 10\,\text{ms}^{-2}:

hg=340\frac{h}{g} = \frac{3}{40} h=3×1040=0.75 mh = \frac{3 \times 10}{40} = 0.75\,\text{m}

Answer: 0.75

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