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QJEEM23Phaeda: JEE Main 2023 Physics - Class 11 JEEM23Phaeda Solution: A light rope is wound around a hollow cylinder of mass 5 kg and …

A light rope is wound around a hollow cylinder of mass 5 kg and radius 70 cm. The rope is pulled with a force of 52.5 N. The angular acceleration of the cylinder will be _________ rad s −2^{-2} .

Step-by-Step Verified Solution

In this problem, the net force on the cylinder is the tension TT in the rope, which is equal to the force applied to the rope:

F=T=52.5 NF=T=52.5~\mathrm{N}

The force causes the cylinder to accelerate with an angular acceleration α\alpha , which is related to its linear acceleration aa and the radius of the cylinder RR by the equation:

α=aR\alpha=\frac{a}{R}

The linear acceleration aa of the cylinder can be found using the formula F=maF=ma :

ma=F=52.5 Nma=F=52.5~\mathrm{N}

where m=5 kgm=5~\mathrm{kg} is the mass of the cylinder. Solving for aa , we get:

a=Fm=52.5 N5 kg=10.5 m/s2a=\frac{F}{m}=\frac{52.5~\mathrm{N}}{5~\mathrm{kg}}=10.5~\mathrm{m/s^2}

Substituting this value of aa into the equation for α\alpha , we get:

α=aR=10.5 m/s20.7 m=15 rad/s2\alpha=\frac{a}{R}=\frac{10.5~\mathrm{m/s^2}}{0.7~\mathrm{m}}=\boxed{15~\mathrm{rad/s^2}}

Therefore, the angular acceleration of the cylinder is 15 rad/s215~\mathrm{rad/s^2} .

Alternate Method:

Let's first draw a free body diagram of the cylinder. The force FF applied to the rope creates a tension in the rope, which in turn exerts a force on the cylinder in the opposite direction. This force is given by:

T=FT=F

where TT is the tension in the rope. The cylinder also experiences a torque due to the tension in the rope, which causes it to rotate. The torque is given by:

τ=TR\tau=TR

where RR is the radius of the cylinder.

The net torque on the cylinder is equal to the product of the moment of inertia II of the cylinder and its angular acceleration α\alpha :

τ=Iα\tau=I\alpha

The moment of inertia of a hollow cylinder about its geometrical axis which is parallel to its length is given by:

I=MR2I=MR^2

where MM is the mass of the cylinder.

Substituting the given values, we get:

τ=TR=Iα=MR2α\tau=TR=I\alpha=MR^2\alpha

Solving for α\alpha , we get:

α=TMR=FMR=52.5 N5 kg⋅0.7 m=15 rad/s2\alpha=\frac{T}{MR}=\frac{F}{MR}=\frac{52.5~\mathrm{N}}{5~\mathrm{kg}\cdot0.7~\mathrm{m}}=\boxed{15~\mathrm{rad/s^2}}

Therefore, the angular acceleration of the cylinder is 15 rad/s215~\mathrm{rad/s^2} .

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