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A disc of radius 15 cm rotates with a speed of 33\(\frac13\)rpm. Two coins are placed on it at 4 cm and 14 cm from its centre. If the coefficient of friction between the coins and the disc is 0.15, which of the two coins will revolve with the disc ?

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Data : r = 15 cm = 0.15 m,

f = 33\(\frac13\) rpm = \(\frac{100}{3\times60}\) rev/s = \(\frac59\) Hz, µ= 0.15, r1

= 4 cm = 0.04 m, r2 = 14 cm = 0.14 m

Angular speed, \(\omega\) = 2\(\pi\)f = 2 x 3.142 x \(\frac59\) = \(\frac{31.42}{9}\)

= 3.491 rad/s

To revolve with the disc without slipping, the necessary centripetal force must be less than or equal to the limiting force of static friction.

Limiting force of static friction, fs = µs N = µs (mg) where m is the mass of the coin and N = mg is the normal force on the coin. 

∴ mω2r ≤ µs (mg) or ω2r ≤ µs

µsg = 0.15 × 9.8 = 1.47 m/s2 

For the first coin, r1 = 0.04 m. 

∴ ω2r1 = (3.491)2 × 0.04 = 12.19 × 0.04  = 0.4876 m/s2

Since, ω2r1 < µsg, this coin will revolve with the disc. For the second coin, r2 = 0.14 m. ∴ ω2r2 = (3.491)2 × 0.14 = 12.19 × 0.14 = 1.707 m/s2

Since, ω2r2 > µsg, this coin will not revolve with the disc. 

Thus, only the coin placed at 4 cm from the centre will revolve with the disc.

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