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Question
A coil having an inductance L and a resistance R is connected to a battery of emf ε. Find the time taken for the magnetic energy stored in the circuit to change from one fourth of the steady-state value to half of the steady-state value.
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Solution
Given:-
Emf of the battery = ε
Inductance of the inductor = L
Resistance = R
Maximum current in the coil `= epsilon/R`
At the steady state, current in the coil, `i =epsilon/R.`
The magnetic field energy stored at the steady state is given by
\[U = \frac{1}{2}L i^2\text{ or } U\]
\[= \frac{\epsilon^2}{2 R^2}L\]
One-fourth of the steady-state value of the magnetic energy is given by
\[U' = \frac{1}{8}L\frac{E^2}{R^2}\]
Half of the value of the steady-state energy \[=\frac{1}{4}L\frac{E^2}{R^2}\]
Let the magnetic energy reach one-fourth of its steady-state value in time t1 and let it reach half of its value in time t2.
Now,
\[\frac{1}{8}L\frac{E^2}{R^2} = \frac{1}{2}L\frac{E^2}{R^2}(1 - e^{- t_1 R/L} )^2 \]
\[ \Rightarrow 1 - e^{- t_1 R/L} = \frac{1}{2}\]
\[ \Rightarrow t_1 \frac{R}{L} = \ln 2\]
And,
\[\frac{1}{4}L\frac{E^2}{R^2} = \frac{1}{2}L\frac{E^2}{R^2}(1 - e^{- t_2 R/L} )^2 \]
\[ \Rightarrow e^{- t_2 R/L} = \frac{\sqrt{2} - 1}{\sqrt{2}} = \frac{2 - \sqrt{2}}{2}\]
\[ \Rightarrow t_1 = \tau \ln\left( \frac{1}{2 - \sqrt{2}} \right) + \ln 2\]
Thus, the time taken by the magnetic energy stored in the circuit to change from one-fourth of its steady-state value to half of its steady-state value is given by
\[t_2 - t_1 = \tau \ln\frac{1}{2 - \sqrt{2}}\]
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