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Question #43914

Difficulty: 8/10 | 🟢 Free

The Question

An RL circuit contains a constant voltage source V=20 VV = 20 \text{ V}, a resistor of constant resistance R=5 \OmegaR = 5 \text{ \Omega}, and a variable inductor. The inductor's core is mechanically coupled to a bimetallic strip, such that the inductance varies with the strip's temperature TT (measured above the ambient temperature) as L(T)=L0+αTL(T) = L_0 + \alpha T, where L0=1 HL_0 = 1 \text{ H} and α=0.2 H/K\alpha = 0.2 \text{ H/K}. The resistor RR is embedded in the bimetallic strip such that all its Joule heating is transferred to the strip. The strip has a heat capacity C=2 J/KC = 2 \text{ J/K} and loses heat to the surroundings according to Newton's law of cooling with a cooling constant λ=2 W/K\lambda = 2 \text{ W/K}. At a particular instant t1t_1, the current in the circuit is I=2 AI = 2 \text{ A} and the temperature of the strip is T=15 KT = 15 \text{ K} above ambient. What is the rate of change of current dIdt\frac{dI}{dt} at this instant?

Options

  • A.

    3.0 A/s3.0 \text{ A/s}

  • B.

    2.5 A/s2.5 \text{ A/s}

  • C.

    2.0 A/s2.0 \text{ A/s}

  • D.

    10.0 A/s10.0 \text{ A/s}

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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

Bimetallic Strip Curvature|Transient Current in RL Circuit|Differential Calculus

Why This Question Is Tricky

Common Mistakes

This question tests the student's ability to handle a coupled electro-thermal system where circuit parameters are time-dependent state variables.

The primary trap lies in the misapplication of Faraday's law for an inductor.

Students commonly memorize the voltage drop across an inductor as VL=LdIdtV_L = L \frac{dI}{dt}, which is only valid for a constant inductance.

When the inductance varies with time (due to the thermally induced mechanical deformation of the bimetallic strip), the correct expression derived from the rate of change of flux linkage is VL=d(LI)dt=LdIdt+IdLdtV_L = \frac{d(LI)}{dt} = L \frac{dI}{dt} + I \frac{dL}{dt}.

Failing to account for the 'motional back-EMF' term IdLdtI \frac{dL}{dt} leads directly to the incorrect option of 2.5 A/s2.5 \text{ A/s}.

Furthermore, the problem requires correctly setting up the transient thermal balance equation to find the instantaneous rate of cooling, linking Joule heating feedback to the mechanical and electrical domains.

Quick Facts About This Question

Question Information

SubjectPhysics
ChapterThermal Properties of Matter - Class 11 Part 2
ConceptBimetallic Strip Curvature
Difficulty8
Cognitive Load7
Target Solve Time160 sec
AccessFree