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QJEEAdv17Ph7909: JEE Advanced 2017 Physics - Class 12 JEEAdv17Ph7909 Solution: A source of constant voltage V is connected to a resistance R…

A source of constant voltage V is connected to a resistance R and two ideal inductors L1 and L2 through a switch S as shown. There is no mutual inductance between the two inductors. The switch S is initially open. At t = 0, the switch is closed and current begins to flow. Which of the following options is/are correct?

JEE Advanced 2017 Paper 2 Offline Physics - Electromagnetic Induction Question 8 English

Multiple Choice Options

  • A After a long time, the current through L1 will be VRL2L1+L2
  • B After a long time, the current through L2 will be VRL1L1+L2
  • C The ratio of the currents through L1 and L2 is fixed at all times (t > 0)
  • D At t = 0, the current through the resistance R is VR

Step-by-Step Verified Solution

Let i1 be the current through L1, i2 be the current through L2 and i be the current through R.

JEE Advanced 2017 Paper 2 Offline Physics - Electromagnetic Induction Question 8 English Explanation

The inductors L1L_1 and L2L_2 are connected in parallel. Therefore, the self-induced emf in L1L_1 and L2L_2 are equal, which can be expressed as:

ε1=−L1di1dt=ε2=−L2di2dt\varepsilon_1 = -L_1 \frac{d i_1}{dt} = \varepsilon_2 = -L_2 \frac{d i_2}{dt}

Upon integrating this equation, we get :

L1i1=L2i2L_1 i_1 = L_2 i_2 ............(1)

This indicates that the ratio of the currents through L1L_1 and L2L_2 is constant.

Using Kirchhoff's current law at junction A, we have :

i=i1+i2i = i_1 + i_2 .............(2)

At the moment the switch is closed (t = 0), the inductors act as open circuits (since the inductive reactance XL=ωLX_L = \omega L approaches infinity as ω→∞\omega \to \infty ). Therefore, initially :

i=i1+i2=0i = i_1 + i_2 = 0

and the current through the resistor is :

i=i1+i2=0i = i_1 + i_2 = 0

After a long time, the inductive reactance of the inductors becomes zero. Applying Kirchhoff's loop law, the current through the resistor RR is :

i=VRi = \frac{V}{R}

Substituting i=VRi = \frac{V}{R} into equation (2) and solving equations (1) and (2), we find :

i1=VRL2L1+L2i_1 = \frac{V}{R} \frac{L_2}{L_1 + L_2}

i2=VRL1L1+L2i_2 = \frac{V}{R} \frac{L_1}{L_1 + L_2}

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