(a) $(KE)_{escape} = \frac{1}{2}m\left( \sqrt{\frac{2GM}{R_{e}}} \right)^{2} = \frac{GMm}{R_{e}}$
$(KE)_{\begin{array}{r}
body\ \ \ \ \ \ \ \\
initially
\end{array}} = \frac{1}{2}\frac{GMm}{R_{e}}$
By law of conservation of energy
$\left( \begin{array}{r}
Total \\
mechanical \\
energy
\end{array} \right) = \left( \begin{array}{r}
Total\ final \\
mechanical \\
energy
\end{array} \right)$
$(KE\ + \ PE)_{surface} = (KE\ + \ PE)_{at\ height\ h}$
$\Rightarrow \ \ \ \frac{1}{2}\frac{GMM}{R_{e}} - \frac{GMm}{R_{e}} = 0 - \frac{GMm}{R_{e} + h}$
($\therefore$ velocity at maximum height is zero)
$\Rightarrow \ v = R_{e}$