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Question #42993

Difficulty: 8/10 | 🟢 Free

The Question

Two rigid coils, 1 and 2, have self-inductances L1L_1 and L2L_2. Their mutual inductance depends on the separation xx between them as M(x)=M0(1−xd)M(x) = M_0 \left(1 - \frac{x}{d}\right) for 0≤x≤d0 \le x \le d, where M0M_0 and dd are positive constants. Coil 1 is held fixed at x=0x = 0. Coil 2 is moved slowly from x=0x = 0 to x=dx = d by an external mechanical agent. During this displacement, the currents in the coils are maintained at constant positive values I1I_1 and I2I_2 respectively by ideal batteries. Let WextW_{ext} be the mechanical work done by the external agent and WelecW_{elec} be the net extra electrical work done by the batteries (excluding the work done to compensate for Joule heating). Which of the following represents the pair (Wext,Welec)(W_{ext}, W_{elec})?

Options

  • A.

    (M0I1I2,−2M0I1I2)(M_0 I_1 I_2, -2 M_0 I_1 I_2)

  • B.

    (−M0I1I2,0)(-M_0 I_1 I_2, 0)

  • C.

    (−M0I1I2,2M0I1I2)(-M_0 I_1 I_2, 2 M_0 I_1 I_2)

  • D.

    (M0I1I2,−M0I1I2)(M_0 I_1 I_2, -M_0 I_1 I_2)

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Correct Answer

Step-by-Step Solution

Explanation

How the Examiner Thinks

Multi-Concept_Bridge

Master problems that require linking physics and math concepts to solve complex competitive questions.

Concepts Behind This Question

Energy Stored in Inductor|Mutual Inductance Reciprocity|Work-Energy Theorem Validity

Why This Question Is Tricky

Common Mistakes

This question tests the fundamental thermodynamic distinction between constant-flux and constant-current electro-mechanical systems.

Students often incorrectly apply the work-energy theorem by equating the mechanical work done by the external agent directly to the change in magnetic potential energy (Wext=ΔUmW_{ext} = \Delta U_m), which yields −M0I1I2-M_0 I_1 I_2.

This assumes an isolated 'fixed-flux' system where no external electrical work is done.

However, because the currents are maintained constant by external batteries, the system is 'fixed-current'.

The batteries act as an energy pump, doing electrical work against the motional back-EMF generated by the changing mutual inductance.

The correct energy balance requires accounting for both mechanical and electrical work: Wext+Welec=ΔUmW_{ext} + W_{elec} = \Delta U_m, where the electrical work done by the sources is exactly twice the change in magnetic energy (Welec=2ΔUmW_{elec} = 2\Delta U_m).

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Question Information

SubjectPhysics
ChapterElectromagnetic Induction - Class 12
ConceptEnergy Stored in Inductor
Difficulty8
Cognitive Load7
Target Solve Time160 sec
AccessFree