If, at t=0^{+} , the voltage across the coil is 120 V, the value of resistance R is
(a) 0 Ω (b) 20 Ω
(c) 40 Ω (d) 60 Ω
i_{ L }\left(0^{-}\right)=\frac{\text { Total voltage }}{\text { Sum of resistance }}
=\frac{120}{20+40}=2 A [Position 1]
In the inductor, the current does not change simultaneously.
Therefore,
i_{ L }\left(0^{+}\right)=i_{ L }\left(0^{-}\right)=2 A [Position 2].
Voltage across the inductor at t=0^{+}
V_{ L }\left(0^{+}\right)=120 V
By applying KVL,
120 = 2(40 + R + 20) ⇒ R = 0 Ω