
(a) As the inductors are in parallel, therefore, induced emf across the two inductors is the same $ie,$
$e_{1} = e_{2}$
$L_{1}\left( \frac{di_{1}}{dt} \right)\ \ = L_{2}\left( \frac{di_{2}}{dt} \right)$
Integrating both sides w.r.t. $t,$ we get
$L_{1}i_{1} = L_{2}i_{2}$
$\therefore\ \ \ \ \frac{i_{1}}{i_{2}} = \frac{L_{2}}{L_{1}}\ $