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NEET PHYSICSMedium

A gramophone record is revolving with an angular velocity ω\omega. A coin is placed at a distance rr from the centre of the record. The static coefficient of friction is μ\mu. The coin will revolve with the record if:

A

r=μgω2r = \frac{\mu g}{\omega^2}

B

r<ω2μgr < \frac{\omega^2}{\mu g}

C

rμgω2r \le \frac{\mu g}{\omega^2}

D

rμgω2r \ge \frac{\mu g}{\omega^2}

Step-by-Step Solution

  1. Identify Forces: For the coin to revolve with the record without slipping, it requires a centripetal force directed towards the centre. The only force capable of providing this in the horizontal plane is the static friction (fsf_s) between the coin and the record.
  2. Centripetal Force: The required centripetal force is Fc=mrω2F_c = mr\omega^2, where mm is the mass of the coin.
  3. Friction Limit: The maximum value of static friction is limiting friction, fs,max=μNf_{s,max} = \mu N. Since the coin is on a horizontal surface, the normal reaction N=mgN = mg. Thus, fs,max=μmgf_{s,max} = \mu mg.
  4. Condition for No Slipping: The coin will revolve with the record only if the required centripetal force is less than or equal to the maximum available static friction. Fcfs,maxF_c \le f_{s,max} mrω2μmgmr\omega^2 \le \mu mg Canceling mass mm (since m>0m > 0): rω2μgr\omega^2 \le \mu g rμgω2r \le \frac{\mu g}{\omega^2} (Reference: NCERT Class 11, Physics Part I, Chapter 5, Section 5.10, Motion of a car on a level road).
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