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Electromagnetic Induction question

2023 · 10 Apr · Shift 2 · Q60
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  5. /2023 · 10 Apr · Shift 2 · Q60

Electromagnetic Induction question

2023 · 10 Apr · Shift 2 · Q60

JEE MainPhysicsElectromagnetic InductionNumerical+4 / −1
A square loop of side 2.0 cm2.0 \mathrm{~cm}2.0 cm is placed inside a long solenoid that has 50 turns per centimetre and carries a sinusoidally varying current of amplitude 2.5 A2.5 \mathrm{~A}2.5 A and angular frequency 700 rad s−1700 ~\mathrm{rad} ~\mathrm{s}^{-1}700 rad s−1. The central axes of the loop and solenoid coincide. The amplitude of the emf induced in the loop is x×10−4 Vx \times 10^{-4} \mathrm{~V}x×10−4 V. The value of xxx is ‾\underline{\hspace{2cm}}​.  (Take, π=227 ) \text { (Take, } \pi=\frac{22}{7} \text { ) } (Take, π=722​ ) 
Numerical answer
View written solutionFree

Correct answer: 44

  1. Magnetic field inside a long solenoid

For a long solenoid, B=μ0nIB = \mu_0 n IB=μ0​nI where:

  • μ0=4π×10−7 H m−1\mu_0 = 4\pi \times 10^{-7}\ \text{H m}^{-1}μ0​=4π×10−7 H m−1
  • n=n =n= number of turns per unit length
  • III is the current

Given:

  • Turns per centimetre =50= 50=50

So turns per metre, n=50×100=5000 m−1n = 50 \times 100 = 5000\ \text{m}^{-1}n=50×100=5000 m−1

The current varies sinusoidally with amplitude I0=2.5 AI_0 = 2.5\ \text{A}I0​=2.5 A and angular frequency ω=700 rad s−1\omega = 700\ \text{rad s}^{-1}ω=700 rad s−1

Hence magnetic field amplitude is B0=μ0nI0B_0 = \mu_0 n I_0B0​=μ0​nI0​

  1. Flux through the square loop

Side of square loop: a=2.0 cm=2.0×10−2 ma = 2.0\ \text{cm} = 2.0 \times 10^{-2}\ \text{m}a=2.0 cm=2.0×10−2 m

Area of loop: A=a2=(2.0×10−2)2=4.0×10−4 m2A = a^2 = (2.0 \times 10^{-2})^2 = 4.0 \times 10^{-4}\ \text{m}^2A=a2=(2.0×10−2)2=4.0×10−4 m2

Since the loop axis coincides with the solenoid axis, magnetic field is perpendicular to the plane of the loop, so flux is Φ=BA\Phi = BAΦ=BA

If I=I0sin⁡ωtI = I_0 \sin \omega tI=I0​sinωt then B=μ0nI0sin⁡ωtB = \mu_0 n I_0 \sin \omega tB=μ0​nI0​sinωt

Thus, Φ=μ0nAI0sin⁡ωt\Phi = \mu_0 n A I_0 \sin \omega tΦ=μ0​nAI0​sinωt

  1. Induced emf

Induced emf is e=∣dΦdt∣e = \left|\frac{d\Phi}{dt}\right|e=​dtdΦ​​

So amplitude of induced emf is e0=μ0nAI0ωe_0 = \mu_0 n A I_0 \omegae0​=μ0​nAI0​ω

Substitute values: e0=(4π×10−7)(5000)(4.0×10−4)(2.5)(700)e_0 = (4\pi \times 10^{-7})(5000)(4.0 \times 10^{-4})(2.5)(700)e0​=(4π×10−7)(5000)(4.0×10−4)(2.5)(700)

Now simplify step-by-step:

5000×4.0×10−4=25000 \times 4.0 \times 10^{-4} = 25000×4.0×10−4=2

So, e0=4π×10−7×2×2.5×700e_0 = 4\pi \times 10^{-7} \times 2 \times 2.5 \times 700e0​=4π×10−7×2×2.5×700

2×2.5=52 \times 2.5 = 52×2.5=5

Therefore, e0=4π×10−7×5×700e_0 = 4\pi \times 10^{-7} \times 5 \times 700e0​=4π×10−7×5×700

5×700=35005 \times 700 = 35005×700=3500

Hence, e0=4π×3500×10−7e_0 = 4\pi \times 3500 \times 10^{-7}e0​=4π×3500×10−7

4×3500=140004 \times 3500 = 140004×3500=14000

So, e0=14000π×10−7=14π×10−4 Ve_0 = 14000\pi \times 10^{-7} = 14\pi \times 10^{-4}\ \text{V}e0​=14000π×10−7=14π×10−4 V

Using π=227\pi = \frac{22}{7}π=722​, e0=14×227×10−4=44×10−4 Ve_0 = 14 \times \frac{22}{7} \times 10^{-4} = 44 \times 10^{-4}\ \text{V}e0​=14×722​×10−4=44×10−4 V

Thus, x=44x = 44x=44

  1. Comparison with stored answer

Derived answer: 444444

Stored correct answer: 444444

They agree.

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