(b) At t = 0, inductor behaves like an infinite resistance. So at
$\ \ \ \ t = 0,\ i = \frac{V}{R_{2}}$
And at $t = \infty,$ inductor behaves like a conducting wire,
$i = \frac{V}{R_{eq}} = \frac{V(R_{1} + R_{2})}{R_{1}R_{2}}$
Reviewed by Dr. Abubacker
Physics Educator & NEET/JEE Specialist
Ph.D. in Physics with 19+ years of teaching experience.