NVAEasyJEE 2024Faraday's Laws of EMI

JEE Physics 2024 Question with Solution

A square loop of side 10cm10 \, \text{cm} and resistance 0.7Ω0.7 \, \Omega is placed vertically in the east-west plane. A uniform magnetic field of 0.20T0.20 \, \text{T} is set up across the plane in the northeast direction. The magnetic field is decreased to zero in 1s1 \, \text{s} at a steady rate. Then, the magnitude of induced emf is x×103V\sqrt{x} \times 10^{-3} \, \text{V}. The value of xx is .

Answer

Correct answer:2

Step-by-step solution

Standard Method

Given: Side of square loop = 10cm=0.1m10 \, \text{cm} = 0.1 \, \text{m}, magnetic field = 0.20T0.20 \, \text{T}, time interval = 1s1 \, \text{s}. The loop is in the east-west vertical plane, so its area vector is along the north-south direction.

Find: The value of xx if induced emf is x×103V\sqrt{x} \times 10^{-3} \, \text{V}.

Area of the square loop:

A=(0.1)2=0.01m2A = (0.1)^2 = 0.01 \, \text{m}^2

The magnetic field is in the northeast direction, so the component perpendicular to the loop is:

B=Bcos45=0.20×12=0.1414TB_\perp = B \cos 45^\circ = 0.20 \times \frac{1}{\sqrt{2}} = 0.1414 \, \text{T}

Magnetic flux through the loop initially is:

ϕ=BA=0.1414×0.01=1.414×103Wb\phi = B_\perp A = 0.1414 \times 0.01 = 1.414 \times 10^{-3} \, \text{Wb}

Since the field decreases to zero uniformly in 1s1 \, \text{s}, the magnitude of induced emf is:

ε=ΔϕΔt=1.414×1031=1.414×103V\varepsilon = \frac{\Delta \phi}{\Delta t} = \frac{1.414 \times 10^{-3}}{1} = 1.414 \times 10^{-3} \, \text{V}

Now,

ε=x×103V\varepsilon = \sqrt{x} \times 10^{-3} \, \text{V}

so,

x=1.414=2\sqrt{x} = 1.414 = \sqrt{2}

Hence,

x=2x = 2

Therefore, the value of xx is 22.

Vector Component Method

Given: Side of square = 0.1m0.1 \, \text{m}, field magnitude = 0.20T0.20 \, \text{T}, time = 1s1 \, \text{s}.

Find: The numerical value of xx.

Take east as i^\hat{i} and north as j^\hat{j}. Since the loop is in the east-west plane, its area vector is along north-south. Using the solution approach,

A=0.01j^m2\vec{A} = 0.01 \, \hat{j} \, \text{m}^2

The magnetic field in northeast direction has equal east and north components:

B=0.202i^+0.202j^\vec{B} = \frac{0.20}{\sqrt{2}} \, \hat{i} + \frac{0.20}{\sqrt{2}} \, \hat{j}

Flux is the dot product:

Φ=BA\Phi = \vec{B} \cdot \vec{A} Φ=(0.202i^+0.202j^)(0.01j^)\Phi = \left(\frac{0.20}{\sqrt{2}} \, \hat{i} + \frac{0.20}{\sqrt{2}} \, \hat{j}\right) \cdot \left(0.01 \, \hat{j}\right) Φ=0.202×0.01=1.414×103Wb\Phi = \frac{0.20}{\sqrt{2}} \times 0.01 = 1.414 \times 10^{-3} \, \text{Wb}

Therefore, induced emf magnitude is:

ε=Φ1=1.414×103V=2×103V|\varepsilon| = \frac{\Phi}{1} = 1.414 \times 10^{-3} \, \text{V} = \sqrt{2} \times 10^{-3} \, \text{V}

Comparing with x×103V\sqrt{x} \times 10^{-3} \, \text{V}, we get x=2x = 2.

Therefore, the final answer is 22.

Common mistakes

  • Using the full magnetic field BB instead of its perpendicular component. Flux depends on B=BcosθB_\perp = B \cos \theta, so first resolve the field along the normal to the loop.

  • Taking the area vector in the plane of the loop. The area vector is always perpendicular to the plane, so for an east-west vertical plane it is along the north-south direction.

  • Writing ε=x×103V\varepsilon = x \times 10^{-3} \, \text{V} instead of the given ε=x×103V\varepsilon = \sqrt{x} \times 10^{-3} \, \text{V}. After finding emf, compare carefully with the required format before reading off xx.

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