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Rotational Motion question

2019 · 11 Jan · Shift 2 · Q43
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Rotational Motion question

2019 · 11 Jan · Shift 2 · Q43

JEE MainPhysicsRotational MotionMCQ+4 / −1
A string is wound around a hollow cylinder of mass 5 kg and radius 0.5m. If the string is now pulled with a horizontal force of 40 N, and the cylinder is rolling without slipping on a horizontal surface (see figure), then the angular acceleration of the cylinder will be (Neglect the mass and thickness of the string) : JEE Main 2019 (Online) 11th January Evening Slot Physics - Rotational Motion Question 180 English
  1. A
    16 rad/s2
  2. B
    20 rad/s2
  3. C
    10 rad/s2
  4. D
    12 rad/s2
View written solutionFree

Correct answer: A

  1. Given data
  • Mass of hollow cylinder: m=5 kgm = 5\,\text{kg}m=5kg
  • Radius: R=0.5 mR = 0.5\,\text{m}R=0.5m
  • Pulling force on string: F=40 NF = 40\,\text{N}F=40N
  • The cylinder is hollow, so its moment of inertia about its center is I=mR2I = mR^2I=mR2

Thus, I=5(0.5)2=5×0.25=1.25 kg m2I = 5(0.5)^2 = 5 \times 0.25 = 1.25\,\text{kg m}^2I=5(0.5)2=5×0.25=1.25kg m2


  1. Choose sign convention

Take rightward translation as positive and clockwise rotation as positive.

Since the string is pulled horizontally at the top, the force FFF produces a clockwise torque.

Let friction at the ground be fff. Its direction is to be determined by the equations.


  1. Equation of translation

Horizontal forces on the cylinder:

  • Pulling force FFF to the right
  • Friction fff at contact point

So, F+f=ma(1)F + f = ma \qquad (1)F+f=ma(1)


  1. Equation of rotation about center

Taking clockwise as positive:

  • Torque due to pulling force at the top: +FR+FR+FR
  • Torque due to friction at bottom: friction to the right gives anticlockwise torque, so contribution is −fR-fR−fR

Hence, FR−fR=IαFR - fR = I\alphaFR−fR=Iα R(F−f)=Iα(2)R(F-f)=I\alpha \qquad (2)R(F−f)=Iα(2)


  1. Rolling without slipping condition

For pure rolling, a=αR(3)a = \alpha R \qquad (3)a=αR(3)


  1. Substitute using I=mR2I=mR^2I=mR2

From (2): R(F−f)=mR2αR(F-f)=mR^2\alphaR(F−f)=mR2α F−f=mRαF-f=mR\alphaF−f=mRα

Using a=αRa=\alpha Ra=αR, we get F−f=ma(4)F-f=ma \qquad (4)F−f=ma(4)

From (1): F+f=ma(1)F+f=ma \qquad (1)F+f=ma(1)

Comparing (1) and (4): F+f=F−fF+f = F-fF+f=F−f 2f=0⇒f=02f=0 \Rightarrow f=02f=0⇒f=0

So friction is actually zero.

Then from (1): F=maF=maF=ma 40=5a40 = 5a40=5a a=8 m/s2a = 8\,\text{m/s}^2a=8m/s2

Now, α=aR=80.5=16 rad/s2\alpha = \frac{a}{R} = \frac{8}{0.5} = 16\,\text{rad/s}^2α=Ra​=0.58​=16rad/s2


  1. Match with options

α=16 rad/s2\boxed{\alpha = 16\,\text{rad/s}^2}α=16rad/s2​

So the correct option is A.


  1. Comparison with stored answer

Stored correct answer: A

Our derived answer: A

They match.

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