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Question
An inductor-coil of inductance 20 mH having resistance 10 Ω is joined to an ideal battery of emf 5.0 V. Find the rate of change of the induced emf at (a) t = 0, (b) t = 10 ms and (c) t = 1.0 s.
Solution
Given:-
Self-inductance, L = 20 mH
Emf of the battery, e = 5.0 V
Resistance, R = 10 Ω
Now,
Time constant of the coil:-
\[\tau = \frac{L}{R} = \frac{20 \times {10}^{- 3}}{10}=2\times10^{-3} s\]
Steady-state current:-
\[i_0 = \frac{e}{R} = \frac{5}{10} = 0 . 5\]
The current in the LR circuit at time t is given by
i = i0(1 − e−t/τ)
⇒ i = i0 − i0e−t/τ
On differentiating both sides, we get
\[\frac{di}{dt} = \frac{i_0}{\tau} e^{- t/\tau}\]
The rate of change of the induced emf is given by
\[R\frac{di}{dt} = R\frac{i_0}{\tau} \times e^{- t/\tau}\]
(a) At time t = 0 s, the rate of change of the induced emf is given by
\[R\frac{di}{dt} = R\frac{i_0}{\tau}\]
\[ = 10 \times \frac{0 . 5}{2 \times {10}^{- 3}}\]
\[ = 2 . 5 \times {10}^3 V/s\]
(b) At time t = 10 ms, the rate of change of the induced emf is given by
\[R\frac{di}{dt} = R\frac{i_0}{\tau} \times e^{- t/\tau}\]
Now,
For t = 10 ms = 10 × 10−3 s = 10−2 s,
\[\frac{dE}{dt} = 10 \times \frac{5}{10} \times \frac{1}{2 \times {10}^{- 3}} \times e^{- 0 . 01/(2\times 10^{- 3})} \]
= 16.844 = 17 V/s
(c) At time t = 1 s, the rate of change of the induced emf is given by
\[\frac{dE}{dt} = \frac{Rdi}{dt} = R\frac{i_0}{\tau} \times e^{- t/\tau}\]
\[= 10 \times \frac{5 \times {10}^{- 1}}{2 \times {10}^{- 3}} \times e^{- 1/(2\times 10^{- 3})}\]
= 0.00 V/s
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