Cylinder C (mass 10.0 kg and radius 0.070m) rolls without slipping on hill H as shown in fig. The string does not stretch and is wrapped around the cylinder C.

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Sol. As the string is unstrechable, when the center of C move up the inclined plane a distance Δ x , the 2kg mass will also drop Δ x. However, as an additional length Δ x of the string is also released in the process, the 2 kg mass will actually drop 2 Δ x . Thus when the 2kg mass moves down one meter , C will move up the inclined plane 0.5 m, or vertically up 0.5 sin 30º = 0.25 m. Ans.
The force involved are shown in above fig. The above effect means that for the 2kg mass we have
2m
= mg – F.
For the cylinder we have
M
= F + f – Mg sin 30º
I
= (F – f) R,
Where I =
MR 2 . Furthermore, as the cylinder
rolls without slipping we also have
= R 
The above equations give
=
g = –0.0435g
= –0.426 ms –2 Ans.
Thus the acceleration has magnitude 0.426 ms –2 and acts downward along the inclined plane
f = 4M (
+ g) = 40 × 0.57g = 23.0N. Its direction is upward along the inclined plane.
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