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Question
A constant current exists in an inductor-coil connected to a battery. The coil is short-circuited and the battery is removed. Show that the charge flown through the coil after the short-circuiting is the same as that which flows in one time constant before the short-circuiting.
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Solution
Consider an inductance L, a resitance R and a source of emf `xi` are connected in series.
Time constant of this LR circuit is,
`tau=L/R`
let a constant current `(i_0=xi/R)` is maitened in the circuit before removal of the battery.
Charge flown in one time constant before the short-circuiting is,
\[Q_\tau = i_0 \tau..........(1)\]
Discahrge equation for LR circuit after short circuiting is given as,
\[i = i_0 e^{- \frac{t}{\tau}}\]
Change flown from the inductor in small time dt after the short circuiting is given as,
dQ = idt
Chrage flown from the inductor after short circuting can be found by interating the above eqation within the proper limits of time,
\[Q = \int_0^\infty idt\]
\[ \Rightarrow Q = \int_0^\infty i_0 e^{- \frac{t}{\tau}} dt\]
\[ \Rightarrow Q = \left[ - \tau i_0 e^{- \frac{t}{\tau}} \right]_0^\infty \]
\[ \Rightarrow Q = - \tau i_0 \left[ 0 - 1 \right]\]
\[ \Rightarrow Q = \tau i_0 ............. (2)\]
Hence, proved.
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