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An inductor of inductance L = 400 mH and resistors of resistances R1 = 2W and R2 = 2W are connected to a battery of emf 12V as shown in the figure. The internal resistance of the battery is negligible. The switch S is closed at t = 0. The potential drop across L as a function of time is –

A

6 e–5t V

B

12te3tV\frac{12}{t}e^{- 3t}V

C

6(1et/0.2)V6\left( 1 - e^{- t/0.2} \right)V

D

12 e–5t V

Answer

12 e–5t V

Explanation

Solution

I = I0 (1 – e–t/t ) (t = L/R2)

e =LdIdt\frac{LdI}{dt} = +LI0et/ττ\frac{+ LI_{0}e^{–t/\tau}}{\tau}

e = E0×LR×L/R\frac{E_{0} \times L}{R \times L/R} e–t/t

e = E 0 e–t/t

e = 12e–5t

So option (4) is correct

Note : Smart work : At t = 0 inductor acts as open CRt and P.D across inductor will be 12V which is possible only in option (4).