(d) The gravitational force of sun on comet is radial, hence angular momentum is constant over the entire orbit. Using law of conservation of angular momentum, at locations $A$ and $B$
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$L = mv_{1}r_{1} = mv_{2}r_{2}$ or $v_{2} = \frac{v_{1}r_{1}}{r_{2}}$ …(i)
Using the principle of conservation of total energy at $A$ and $B$
$\frac{1}{2}mv_{1}^{2} - \frac{GMm}{r_{1}} = \frac{1}{2}m\ v_{2}^{2} - \frac{GMm}{r_{2}}$
or $v_{2}^{2} - v_{1}^{2} = 2GM\left( \frac{1}{r_{2}} - \frac{1}{r_{1}} \right)$ …(ii)
Putting the values from Eq. (i) in Eq. (ii) and solving, we get
$v_{1} = \left\lbrack \frac{2GMr_{2}}{r_{1}\left( r_{1} + r_{2} \right)} \right\rbrack^{1/2}$
$\therefore L = mv_{1}r_{1} = m\left\lbrack \frac{2GMr_{1}r_{2}}{\left( r_{1} + r_{2} \right)} \right\rbrack^{1/2}$