a disc at rest rolls down a hill of height (3×9.8) without slipping .what is its velocity when it reaches the bottom
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The easiest way to solve these problems is to apply conservation of energy. The disc at rest only has potential energy. If we define the datum (h=0) to be the bottom of the hill, then the disc will have no potential energy at the bottom of the hill. All the potential energy will be converted to linear kinetic energy as well as rotational kinetic energy.
PE=(KE)linear+(KE)rotational
mgh=12mv2+12Iω2 ——- equation 1
but the mass moment of inertia of a disc about its rotating axis is I=12mR2
and the angular velocity ω=vR
equation 1 becomes:
mgh=12mv2+12(12mR2)(vR)2
or
mgh=12mv2+14mv2
or
mgh=34mv2
or
gh=34v2
(9.8)(3)9.8=34v2
or
(9.8)9.8=14v2
take square root of both sides gives:
9.8=12v
v=2(9.8)=19.6m/s
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