A force f acts tangentially at the highest point of a disc of mass m kept on a rough horizontal plane. If the disc rolls without slipping, the acceleration of centre of the disc is
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The acceleration of centre of the disc is a = 4F / 3m
Explanation:
- The force F acting on the sphere moves it towards right.
- The contact point between force and sphere will slip towards right
- Thus the static friction( force f shown ) on the sphere will act towards left.
Let
Radius of the sphere = r
Linear acceleration = a
Since there is slipping alpha "α"= r a
For linear motion F - f = ma ----- (1)
Where "f" is the frictional force
For rotational motion, torque about center "τ" = Fr+fr = Iα=( 1/2 mr^2 ) a/r
F+f= 1/2 ma ---- (2)
From (1) and (2) adding, we get 2 F = 3 / 2 ma
a= 4F / 3m
Thus the acceleration of centre of the disc is a = 4F / 3m
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