$A$ uniform chain of length $l$ and mass $m$ lies on the surface of a smooth hemisphere of radius $R$ $(R > l)$ with one end tied to the top of the hemisphere as shown in the figure. Gravitational potential energy of the chain with respect to the base of the hemisphere is

  • A
    $\frac{m g l}{2}$
  • B
    $\frac{m g R^2}{l} \sin \left(\frac{l}{R}\right)$
  • C
    $\frac{m g R^2}{l} \sin \left(\frac{R}{l}\right)$
  • D
    $\frac{m g l^2}{R} \sin \left(\frac{l}{R}\right)$

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