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Question: A chain of length *l* is placed on a smooth spherical surface of radius r with one of its ends fixed...

A chain of length l is placed on a smooth spherical surface of radius r with one of its ends fixed at the top of the surface. Length of chain is assumed to be l<πr/2. Acceleration of each element of chain when upper end is released is

A

lgr(1cosrl)\frac{\lg}{r\left( 1 - \cos\frac{r}{l} \right)}

B

rgl(1coslr)\frac{rg}{l}\left( 1 - \cos\frac{l}{r} \right)

C

rgl(1coslr)\frac{rg}{l}\left( 1 - \cos\frac{l}{r} \right)

D

rgl(1sinlr)\frac{rg}{l}\left( 1 - \sin\frac{l}{r} \right)

Answer

rgl(1coslr)\frac{rg}{l}\left( 1 - \cos\frac{l}{r} \right)

Explanation

Solution

Consider a small element dl making an angle dθ

dm = mldl=mlrdθ\frac{m}{l}dl = \frac{m}{l}rd\theta

force acting on the element

dF = (dm)g sin θ = mrg/l sin θ dθ

F = mrgl0asinθdθ\frac{mrg}{l}\int_{0}^{a}{\sin\theta d\theta}

Where, total angle α = 1/r

F = mlrg(1cosα)\frac{m}{l}rg\left( 1 - \cos\alpha \right) = mlrg(1coslr)\frac{m}{l}rg\left( 1 - \cos\frac{l}{r} \right)

or a = rgl(1coslr)\frac{rg}{l}\left( 1 - \cos\frac{l}{r} \right)