a solid cylinder of mass m and radius r rolls without slipping down an inclined plane of length l and height h the speed of its centre of mass when reach the bottom of inclined plane
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The speed of its center of mass when reach the bottom of inclined plane is r(4gh/3r²)^1/2
Given-
- Mass of solid cylinder = M
- Radius of cylinder = r
- Length of the inclined plane = l
- Height of the plane = h
Let v be the velocity of center of mass. Now according to the conservation of energy.
Potential energy at the top = Kinetic energy of the rotation + Kinetic energy of the translational motion at the bottom.
By substituting the value we get
mgh = 1/2 mv² + 1/2 Iω² where
v = rω and I = 1/2 mr²
So,
ω² = 4gh/3r²
Kinetic energy = 1/2 mv² = 1/2 mr²ω²
v = rω = r (4gh/3r²)^1/2
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