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QJEEM24Phcf47: JEE Main 2024 Physics - Class 11 JEEM24Phcf47 Solution: A cylinder is rolling down on an inclined plane of inclination…

A cylinder is rolling down on an inclined plane of inclination 60∘60^{\circ} . It's acceleration during rolling down will be x3m/s2\frac{x}{\sqrt{3}} m / s^2 , where x=x= ________ (use g=10 m/s2\mathrm{g}=10 \mathrm{~m} / \mathrm{s}^2 ).

Step-by-Step Verified Solution

To determine the acceleration of a cylinder rolling down an inclined plane without slipping, we can use Newton's second law and the concept of rolling motion. For an inclined plane at an angle θ\theta , the component of gravitational acceleration along the plane is gsin⁡θg \sin \theta . However, because the cylinder is rolling and not sliding, not all of this component accelerates the center of mass; some of it goes into causing rotational acceleration about the center of mass.

For a rolling cylinder, the moment of inertia II is I=12mr2I = \frac{1}{2} m r^2 , where mm is the mass of the cylinder and rr is the radius. The condition for rolling without slipping is that the linear acceleration aa of the center of mass is equal to the radius rr times the angular acceleration α\alpha , i.e., a=rαa = r \alpha .

To find the linear acceleration aa , we use the torque τ\tau about the center of mass caused by the gravitational force down the incline. The torque due to gravity is τ=mgsin⁡θ⋅r\tau = mg \sin \theta \cdot r , and from Newton's second law for rotation, the angular acceleration is given by

α=τI=mgsin⁡θ⋅r12mr2=2gsin⁡θr\alpha = \frac{\tau}{I} = \frac{mg \sin \theta \cdot r}{\frac{1}{2} m r^2} = \frac{2g \sin \theta}{r}

Now using a=rαa = r \alpha :

a=r(2gsin⁡θr)=2gsin⁡θa = r \left( \frac{2g \sin \theta}{r} \right) = 2g \sin \theta

But we must account for the fact that only a portion of the gravitational acceleration goes into translating the cylinder down the plane due to the rolling condition. This is where we apply the concept of the ``rolling factor'' for a cylinder, which is 23\frac{2}{3} for a solid cylinder, meaning 23\frac{2}{3} of the gravitational component is used for translation.

The acceleration of the center of mass for the cylinder is therefore:

a=23gsin⁡θa = \frac{2}{3} g \sin \theta

Now we plug in the values of θ=60∘\theta = 60^{\circ} (which has sin⁡60∘=32\sin 60^{\circ} = \frac{\sqrt{3}}{2} ) and g=10  m/s2g = 10 \; m/s^2 :

a=23⋅10⋅32=1033a = \frac{2}{3} \cdot 10 \cdot \frac{\sqrt{3}}{2} = \frac{10 \sqrt{3}}{3}

To match the given expression x3m/s2\frac{x}{\sqrt{3}} m / s^2 , let's manipulate our expression for aa :

a=1033=1033⋅33=10⋅33⋅3=103m/s2a = \frac{10 \sqrt{3}}{3} = \frac{10 \sqrt{3}}{3} \cdot \frac{\sqrt{3}}{\sqrt{3}} = \frac{10 \cdot 3}{3 \cdot \sqrt{3}} = \frac{10}{\sqrt{3}} m/s^2

Hence, the value of xx is 1010 .

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