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# A particle of mass M is placed at the center of a uniform sperical shell of mass 2M and radius R. The gravitational potential on the surface of the shell is

$(a)\;\frac{-GM}{R} \quad (b)\;\frac{-3GM}{R} \quad (c)\;\frac{-2GM}{R} \quad (d)\;zero$

$\qquad = \bigg( \large\frac{-GM}{R}\bigg)+\bigg (\large\frac{-2 GM}{R}\bigg)$
$\qquad= \large\frac{-3GM}{R}$