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Question: In the circuit shown in the figure, switch \({k_2}\) is open and switch \({k_1}\) is opened at \(t =...

In the circuit shown in the figure, switch k2{k_2} is open and switch k1{k_1} is opened at t=0t = 0. At time t=tot = {t_o}, switch k1{k_1} is opened and switch k2{k_2} is simultaneously closed. The variation of inductor current with time is


Explanation

Solution

when switch k1{k_1} is closed an emf is induced in the circuit. Applying the formula of emf for the inductor inducing it, we will establish a relation between inductor current and time.
In the above relation, when the boundary conditions of the second circuit alignment is inputted, we will obtain another relation between current and time.

Formulae used: emf is induced in the circuit: E=LdidtE = L\dfrac{{di}}{{dt}}.
Where EE is the induced emf and is expressed in Volts (V)(V), LL is the inductance and is expressed in Henry (H)(H), didi is the change in current and is expressed in Ampere (A)(A) and dtdt is the time taken for the current to change and is expressed in seconds (s)(s).

Step by step solution: When k1{k_1} is closed, current flows in the circuit due to the battery connected to it. The presence of the inductance coil creates a magnetic flux, which on changing, results in the induction of an electromagnetic force. This is represented by EE and is equal to LdidtL\dfrac{{di}}{{dt}}.
Applying the boundary condition at t=0t = 0 we get,
E=Ldidt di=EL×dt  E = L\dfrac{{di}}{{dt}} \\\ \Rightarrow di = \dfrac{E}{L} \times dt \\\
Upon integration within the limits of 0to0 \to {t_o} we get,
0Itodi=0toEL×dt Ito=ELto  \Rightarrow {\smallint _0}^{{I_{{t_o}}}}di = {\smallint _0}^{{t_o}}\dfrac{E}{L} \times dt \\\ \Rightarrow {I_{{t_o}}} = \dfrac{E}{L}{t_o} \\\
This linear variation is from tt to to{t_o}.
Now, applying the boundary conditions at t>tot > {t_o} having limits of to{t_o} \to \infty we get,
E=Ldidt di=EL×dt Itodi=toEL×dt IIto=EL(tto)  E = L\dfrac{{di}}{{dt}} \\\ \Rightarrow di = \dfrac{E}{L} \times dt \\\ \Rightarrow {\smallint _{{I_{{t_o}}}}}^\infty di = {\smallint ^\infty }_{{t_o}}\dfrac{E}{L} \times dt \\\ \Rightarrow {I_\infty } - {I_{{t_o}}} = \dfrac{E}{L}({t_\infty } - {t_o}) \\\
Which is impossible.
Therefore Ldidt=0L\dfrac{{di}}{{dt}} = 0 is considered.
This is a constant and therefore there is no variation in inductor current with time.
In conclusion, the correct graph is option A.

Note: The first boundary condition is not t=0t = 0. It ranges from t=0t = 0 to t=tot = {t_o}. Similarly, the second one is also a range, that is, t=tot = {t_o} to t=tt = {t_\infty }. Calculations are made to be considered in a given time period and not just at a particular instant of time.

Additional information: A LR circuit is a circuit having a combination of inductor(s) and resistor(s). In AC circuits, they reduce voltage and in DC circuits, the inductor acts as a static resistance. Therefore, the circuit given in the above problem has DC connection because no resistor is present.