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QJEEM22Ph894e: JEE Main 2022 Physics - Class 12 JEEM22Ph894e Solution: A coil is placed in a time varying magnetic field. If the…

A coil is placed in a time varying magnetic field. If the number of turns in the coil were to be halved and the radius of wire doubled, the electrical power dissipated due to the current induced in the coil would be :

(Assume the coil to be short circuited.)

Multiple Choice Options

  • A Halved
  • B Quadrupled
  • C The same
  • D Doubled

Step-by-Step Verified Solution

The electrical power dissipated due to the current induced in a coil placed in a time-varying magnetic field can be determined by considering Faraday's Law of Induction and the resistance of the coil.

Faraday's Law of Induction

The induced EMF ( E\mathcal{E} ) in a coil with NN turns experiencing a time-varying magnetic flux ( ΦB\Phi_B ) is given by:

E=−NdΦBdt\mathcal{E} = -N \frac{d\Phi_B}{dt}

Resistance of the Coil

The resistance ( RR ) of a wire depends on its length ( LL ) and cross-sectional area ( AA ) as well as the resistivity ( ρ\rho ) of the material:

R=ρLAR = \frac{\rho L}{A}

For a coil of radius rr and with wire of radius aa , assuming the wire is wound tightly with a length approximated by the circumference of the coil multiplied by the number of turns, we have:

L≈2πrNL \approx 2\pi r N

And the cross-sectional area of the wire is given by:

A=πa2A = \pi a^2

Thus, the resistance becomes:

R≈ρ⋅2πrNπa2=2ρrNa2R \approx \frac{\rho \cdot 2\pi r N}{\pi a^2} = \frac{2\rho r N}{a^2}

Power Dissipated

The electrical power ( PP ) dissipated in the coil is related to the induced current ( II ) and the resistance ( RR ):

P=I2RP = I^2 R

Using Ohm's Law, the induced current II can be expressed as:

I=ERI = \frac{\mathcal{E}}{R}

Substituting the expressions for E\mathcal{E} and RR :

I=NdΦBdt2ρrNa2=a22ρr⋅dΦBdtI = \frac{N \frac{d\Phi_B}{dt}}{\frac{2\rho r N}{a^2}} = \frac{a^2}{2\rho r} \cdot \frac{d\Phi_B}{dt}

Hence, the power dissipated:

P=(a22ρr⋅dΦBdt)2⋅2ρrNa2P = \left(\frac{a^2}{2\rho r} \cdot \frac{d\Phi_B}{dt}\right)^2 \cdot \frac{2\rho r N}{a^2}

P=a44ρ2r2(dΦBdt)2⋅2ρrNa2P = \frac{a^4}{4\rho^2 r^2} \left( \frac{d\Phi_B}{dt} \right)^2 \cdot \frac{2\rho r N}{a^2}

P=a22ρr⋅N(dΦBdt)2P = \frac{a^2}{2\rho r} \cdot N \left( \frac{d\Phi_B}{dt} \right)^2

Case when the number of turns is halved and the radius of the wire is doubled

Halving the number of turns:

N′=N2N' = \frac{N}{2}

Doubling the radius of the wire:

a′=2aa' = 2a

Substituting these into the power formula:

P′=(2a)22ρr⋅N2(dΦBdt)2P' = \frac{(2a)^2}{2\rho r} \cdot \frac{N}{2} \left( \frac{d\Phi_B}{dt} \right)^2

P′=4a22ρr⋅N2(dΦBdt)2P' = \frac{4a^2}{2\rho r} \cdot \frac{N}{2} \left( \frac{d\Phi_B}{dt} \right)^2

P′=4a22ρr⋅N2(dΦBdt)2P' = \frac{4a^2}{2\rho r} \cdot \frac{N}{2} \left( \frac{d\Phi_B}{dt} \right)^2

P′=2(a22ρr⋅N(dΦBdt)2)P' = 2 \left( \frac{a^2}{2\rho r} \cdot N \left( \frac{d\Phi_B}{dt} \right)^2 \right)

P′=2PP' = 2P

Thus, the electrical power dissipated in the coil would be:

Option D

Doubled

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