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Question #42961

Difficulty: 8/10 | 🟢 Free

The Question

A thin toroidal coil of mean circumference l=1.0 ml = 1.0 \text{ m} and cross-sectional area A=1.0×10−3 m2A = 1.0 \times 10^{-3} \text{ m}^2 has N=1000N = 1000 turns of wire uniformly wound on a ferromagnetic core. The core material exhibits a non-linear magnetic behavior (ignoring hysteresis) where the magnetic field BB is related to the magnetic intensity HH by the equation B=BsHHc+HB = \frac{B_s H}{H_c + H} for H>0H > 0. Here, the saturation magnetic field is Bs=2.0 TB_s = 2.0 \text{ T} and the characteristic magnetic intensity is Hc=4000 A/mH_c = 4000 \text{ A/m}. A time-varying current I(t)=αtI(t) = \alpha t is passed through the coil, where α=2.0 A/s\alpha = 2.0 \text{ A/s} and tt is the time in seconds. Calculate the magnitude of the induced EMF in the coil at t=2.0 st = 2.0 \text{ s}.

Options

  • A.

    0.25 V0.25 \text{ V}

  • B.

    0.50 V0.50 \text{ V}

  • C.

    1.00 V1.00 \text{ V}

  • D.

    0.75 V0.75 \text{ V}

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Correct Answer

Step-by-Step Solution

Explanation

How the Examiner Thinks

Variable_Constraint

Develop pure symbolic logic skills by mastering algebraic constraints without relying on numerical data.

Concepts Behind This Question

Soft vs Hard Magnetic Materials|Maxwell's Correction to Ampere's Law|Variable Force Integration

Why This Question Is Tricky

Common Mistakes

This question tests the fundamental understanding of Faraday's Law in non-linear magnetic media.

A common trap is for students to calculate the 'secant permeability' μ=BH\mu = \frac{B}{H} at t=2.0 st=2.0\text{ s} (which yields 14000 T m/A\frac{1}{4000}\text{ T m/A}) and use it to find an effective inductance L=μN2AlL = \frac{\mu N^2 A}{l}, leading to an incorrect EMF of ε=LdIdt=0.50 V\varepsilon = L \frac{dI}{dt} = 0.50\text{ V}.

Alternatively, they might use the initial permeability μi=BsHc\mu_i = \frac{B_s}{H_c} leading to 1.00 V1.00\text{ V}.

The core physical principle is that induced EMF depends strictly on the time derivative of the flux, which in a non-linear medium requires the use of the 'differential permeability' μd=dBdH\mu_d = \frac{dB}{dH}.

This punishes the blind application of lumped-circuit formulas like L=NΦIL = \frac{N\Phi}{I} and rewards a rigorous application of Maxwell-Faraday principles.

Quick Facts About This Question

Question Information

SubjectPhysics
ChapterMagnetism and Matter - Class 12
ConceptSoft vs Hard Magnetic Materials
Difficulty8
Cognitive Load7
Target Solve Time160 sec
AccessFree