This is a problem from one of the boston olympiads A uniform ball rolls without slipping on a turntable . As viewed from the inertial lab frame, the ball moves in a circle not necessarily centered at the center of the turntable with a certain frequency xf. The frequency of rotation of the turntable is f find [100x] here [.] Is greatest integer function
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Let the angular velocity of ball be ω , and that of the turntable be Ω z ^ . Since the ball is moving in a circular motion, There must be a force action on the ball, which in this case is frictional force f f . This force cause change in linear momentum
f f = d t d p = m d t d v . . . . . . . . . . . . ( 1 )
As well as change in angular momentum.
− f f × ( l z ^ ) = I d t d ω . . . . . . . . ( 2 )
Where l is the radius of the ball. Before we go any further let us express the balls velocity in the lab frame. If we let r be the position of the ball from the center of the turntable. Its velocity can simply be expressed as the sum of the turntables velocity and the velocity of the ball.
v = ( Ω z ) ^ × r + ω × ( l z ^ ) . . . . . . . . 3
Substitute equation ( 1 ) into equation ( 2 )
m d t d v × ( − l z ^ ) = I d t d ω ⇒ d t d ω = − ( I l m ) z ^ × d t d v . . . . . 4
Take the derivative of equation ( 3 )
d t d v = Ω z ^ × d t d r + d t d ω × ( l z ^ )
Plugging the value of equation (4) to this equation and taking the cross product we get
d t d v = Ω z ^ × v + ( I m l 2 ) d t d v ⇒ a = d t d v = ⎝ ⎛ 1 + ( I m l 2 ) Ω ⎠ ⎞ z ^ × v
Momentum of inertia of a sphere I = 5 2 m l 2 , thus
a = ( 7 2 Ω ) z ^ × v
We know an object moving in a circular motion as an acceleration of a = Ω z ^ × v , So basically the ball is moving at an angular frequency of 7 2 times the frequency of the turntable.
⌊ 1 0 0 ( 7 2 ) ⌋ = 2 8