(a) Using conservation of energy.
$\ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \frac{1}{2}{mv}^{2} - \frac{GMm}{R} = 0 - \frac{GMm}{2R}$
$or\ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \frac{1}{2}{mv}^{2} = \frac{GMm}{R} - \frac{GMm}{2R}$
$or\ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ v^{2} = 2\frac{GM}{R}\left\lbrack 1 - \frac{1}{2} \right\rbrack$
$or\ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ v^{2} = \frac{GM}{R}\ \ \ $
$But\ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ {gR}^{2} = GM$
$\therefore\ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ v = \sqrt{\frac{{gR}^{2}}{R}}$
$or\ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ v = \sqrt{gR}$