It is not by sitting still at a grand distance and calling the human race larvae that men are to be helped.
– Albert Einstein
The following question on transients in LR circuit was asked in the All India Engineering/Architecture Entrance Examination (AIEEE) 2009:
An inductor of inductance L = 400 mH and resistors of resistances R1 = 2 Ω and R2 = 2 Ω are connected to a battery of emf 12 V 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
(1) 12 e–5t V
(2) 6 e–5t V
(3) (12/t) e–3t
(4) 6(1– e–t/0.2) V
The exponential growth of current I in an LR circuit is given by
I = I0 (1– e–Rt/L) where I is the current at the instant t, I0 is the final maximum current equal to V/R where V is the
Therefore potential drop across L at the instant t = L (I0R/L) e–Rt/L = I0R e–Rt/L
In the present problem I0 = 6 A (since V = 12 volt and R = R2 = 2 Ω) and L = 400 mH = 0.4 H.
Therefore, the potential drop across L at the instant t = 6×2×e–2t/0.4 = 12 e–5t volt [Option (1)].
Let us try the following question involving transients in a CR circuits:
Suppose the inductor in the above question is replaced by a capacitor of capacitance 1000 μF. The switch S is closed at time t = 0. The charging current flowing through the capacitor as a function of time is
(1) 12 e–500t A
(2) 6 e–500t A
(3) 12e–t/1000 A
(4) 6(1– e–t/500) A
The exponential growth of charge Q on a capacitor in a CR circuit is given by
Q = Q0 (1– e–t/RC) where Q is the charge at the instant t, Q0 is the final maximum charge which is equal to CV. The charging current I flowing through the capacitor is given by
I = dQ/dt = (Q0/RC) e–t/RC = (CV/RC) e–t/RC = (V/R) e–t/RC
Here V = 12 volt, C = 1000 μF = 0.001 F and R = R2 = 2 Ω
Therefore, the charging current I flowing through the capacitor = 6× e–t/(2×0.001) = 6 e–500t A.
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