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Electromagnetic Induction question

2019 · 8 Apr · Shift 1 · Q63
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Electromagnetic Induction question

2019 · 8 Apr · Shift 1 · Q63

JEE MainPhysicsElectromagnetic InductionMCQ+4 / −1
A 20 Henry inductor coil is connected to a 10 ohm resistance in series as shown in figure. The time at which rate of dissipation of energy (joule's heat) across resistance is equal to the rate at which magnetic energy is stored in the inductor is : JEE Main 2019 (Online) 8th April Morning Slot Physics - Electromagnetic Induction Question 99 English
  1. A
    2ln⁡2{2 \over {\ln 2}}ln22​
  2. B
    ln⁡2{\ln 2}ln2
  3. C
    2ln⁡22{\ln 2}2ln2
  4. D
    12ln⁡2{1 \over 2}{\ln 2}21​ln2
View written solutionFree

Correct answer: C

  1. Current growth in an RLRLRL circuit

For a series RLRLRL circuit connected to a DC source, the current grows as

i(t)=I0(1−e−t/τ)i(t)=I_0\left(1-e^{-t/\tau}\right)i(t)=I0​(1−e−t/τ)

where

τ=LR\tau=\frac{L}{R}τ=RL​

Given:

L=20 H,R=10 ΩL=20\,\text{H}, \qquad R=10\,\OmegaL=20H,R=10Ω

So,

τ=2010=2 s\tau=\frac{20}{10}=2\,\text{s}τ=1020​=2s

Hence,

i(t)=I0(1−e−t/2)i(t)=I_0\left(1-e^{-t/2}\right)i(t)=I0​(1−e−t/2)
  1. Rate of dissipation of energy in the resistor

Power dissipated in the resistor is

PR=i2RP_R=i^2RPR​=i2R

So,

PR=RI02(1−e−t/2)2P_R=R I_0^2\left(1-e^{-t/2}\right)^2PR​=RI02​(1−e−t/2)2
  1. Rate at which magnetic energy is stored in the inductor

Magnetic energy stored in the inductor is

U=12Li2U=\frac12 Li^2U=21​Li2

Therefore,

dUdt=Lididt\frac{dU}{dt}=Li\frac{di}{dt}dtdU​=Lidtdi​

Now,

i=I0(1−e−t/2)i=I_0\left(1-e^{-t/2}\right)i=I0​(1−e−t/2)

Differentiate:

didt=I0⋅12e−t/2\frac{di}{dt}=I_0\cdot \frac{1}{2}e^{-t/2}dtdi​=I0​⋅21​e−t/2

Thus,

dUdt=L⋅I0(1−e−t/2)⋅I012e−t/2\frac{dU}{dt}=L\cdot I_0\left(1-e^{-t/2}\right)\cdot I_0\frac12 e^{-t/2}dtdU​=L⋅I0​(1−e−t/2)⋅I0​21​e−t/2

Using L=20L=20L=20,

dUdt=20⋅I02⋅12(1−e−t/2)e−t/2\frac{dU}{dt}=20\cdot I_0^2\cdot \frac12 \left(1-e^{-t/2}\right)e^{-t/2}dtdU​=20⋅I02​⋅21​(1−e−t/2)e−t/2 dUdt=10I02(1−e−t/2)e−t/2\frac{dU}{dt}=10I_0^2\left(1-e^{-t/2}\right)e^{-t/2}dtdU​=10I02​(1−e−t/2)e−t/2
  1. Set the two rates equal

We need

PR=dUdtP_R=\frac{dU}{dt}PR​=dtdU​

So,

10I02(1−e−t/2)2=10I02(1−e−t/2)e−t/210I_0^2\left(1-e^{-t/2}\right)^2=10I_0^2\left(1-e^{-t/2}\right)e^{-t/2}10I02​(1−e−t/2)2=10I02​(1−e−t/2)e−t/2

Cancel common factors 10I0210I_0^210I02​ and (1−e−t/2)\left(1-e^{-t/2}\right)(1−e−t/2):

1−e−t/2=e−t/21-e^{-t/2}=e^{-t/2}1−e−t/2=e−t/2

Therefore,

1=2e−t/21=2e^{-t/2}1=2e−t/2 e−t/2=12e^{-t/2}=\frac12e−t/2=21​

Taking natural logarithm,

−t2=ln⁡(12)=−ln⁡2-\frac{t}{2}=\ln\left(\frac12\right)=-\ln 2−2t​=ln(21​)=−ln2 t2=ln⁡2\frac{t}{2}=\ln 22t​=ln2 t=2ln⁡2t=2\ln 2t=2ln2
  1. Match with the options
t=2ln⁡2t=2\ln 2t=2ln2

So the correct option is:

C: 2ln⁡22\ln 22ln2

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