A coin placed at 4 cm from the center
Mass of each coin =m
Radius of the disc,r=15cm=0.15m
Frequency of revolution, =100/3rev/min=100/(3x60)=5/9rev/s
Coefficient of friction, =0.15
In the given situation, the coin having a force of friction greater than or equal to the centripetal force provided by the rotation of the disc will revolve with the disc. If this is not the case, then the coin will slip from the disc.Coin placed at 4 cm:Radius of revolution, r′=4cm=0.04m
Angular frequency, =2πN=2×(22/7)×(5/9)=3.49rad/s
Frictional force, f=μmg=0.15m×10=1.5mN
Centripetal force on the coin:Fcent.=mr′ω2
=m×0.04×(3.49)2
=0.49mN
Since f>Fcent, the coin will revolve along with the record.
Coin placed at 14 cm:
Radius, r"=14cm=0.14m
Angular frequency, =3.49s−1
Frictional force, f′=1.5mN
Centripetal force is given as:
Fcent=mr"ω2
=m×0.14×(3.49)2
=1.7mN
Since f<Fcent., the coin will slip from the surface of the record.