JEE Challenger
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Calculate Coefficient of Friction Between Stick and Rolling Ring

A boy is pushing a ring of mass 2 kg2\text{ kg} and radius 0.5 m0.5\text{ m} with a stick as shown in the figure. The stick applies a force of 2 N2\text{ N} on the ring and rolls it without slipping with an acceleration of 0.3 m/s20.3\text{ m/s}^2. The coefficient of friction between the ground and the ring is large enough that rolling always occurs and the coefficient of friction between the stick and the ring is (P/10)(P/10). The value of PP is

Diagram 0

Official Numerical Answer4

Step-by-Step Solution

To find the value of PP, we analyze the translational and rotational motion of the ring.

Given Data:

  • Mass of the ring, m=2 kgm = 2\text{ kg}
  • Radius of the ring, R=0.5 mR = 0.5\text{ m}
  • Force applied by the stick (normal force on the ring), N=2 NN = 2\text{ N}
  • Linear acceleration of the ring, a=0.3 m/s2a = 0.3\text{ m/s}^2
  • Coefficient of friction between the stick and the ring, μ=P10\mu = \frac{P}{10}

1. Condition for Pure Rolling

Since the ring rolls without slipping on the ground, the relation between the linear acceleration aa and the angular acceleration α\alpha is:
a=Rα  ⟹  α=aRa = R\alpha \implies \alpha = \frac{a}{R}


2. Equations of Motion

A. Translational Motion (Horizontal Direction)

Assuming the stick pushes the ring to the left with normal force N=2 NN = 2\text{ N}, the ring accelerates to the left. The static friction force from the ground, fgf_g, opposes this motion and acts towards the right.

Using Newton's second law for horizontal motion:
N−fg=maN - f_g = m a

Substitute the known values:
2−fg=2×0.32 - f_g = 2 \times 0.3
2−fg=0.6  ⟹  fg=1.4 N2 - f_g = 0.6 \implies f_g = 1.4\text{ N}

B. Rotational Motion (Torque about Center of Mass)

Taking the counterclockwise rotation as positive:

  • The moment of inertia of a ring about its central axis is I=mR2I = m R^2.
  • The friction force from the ground, fgf_g, acts to the right at the bottom point, creating a counterclockwise torque:
    τg=fgR\tau_g = f_g R
  • The friction force from the stick, fsf_s, acts at the rightmost contact point of the ring. To oppose the upward relative velocity of the contact point on the rotating ring, fsf_s acts downwards, creating a clockwise torque:
    τs=−fsR\tau_s = -f_s R

Using Newton's second law for rotation:
τnet=Iα\tau_{\text{net}} = I \alpha
fgR−fsR=(mR2)(aR)f_g R - f_s R = (m R^2) \left(\frac{a}{R}\right)

Dividing both sides by RR:
fg−fs=maf_g - f_s = m a


3. Calculation of Friction Force fsf_s and PP

Substitute fg=1.4 Nf_g = 1.4\text{ N}, m=2 kgm = 2\text{ kg}, and a=0.3 m/s2a = 0.3\text{ m/s}^2:
1.4−fs=2×0.31.4 - f_s = 2 \times 0.3
1.4−fs=0.6  ⟹  fs=0.8 N1.4 - f_s = 0.6 \implies f_s = 0.8\text{ N}

The friction force exerted by the stick on the ring is given by:
fs=μNf_s = \mu N

Substitute fs=0.8 Nf_s = 0.8\text{ N} and N=2 NN = 2\text{ N}:
0.8=μ×2  ⟹  μ=0.40.8 = \mu \times 2 \implies \mu = 0.4

Given that μ=P10\mu = \frac{P}{10}:
P10=0.4  ⟹  P=4\frac{P}{10} = 0.4 \implies P = 4