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Question #43370

Difficulty: 8/10 | 🟢 Free

The Question

A circuit consists of an ideal battery of electromotive force VV, a fixed resistor of resistance R0R_0, and a variable resistor connected in series. At time t=0t=0, the variable resistor is at an initial temperature T0T_0 and has a resistance R0R_0. The variable resistor has a temperature coefficient of resistance α\alpha such that its resistance at temperature TT is given by R(T)=R0[1+α(T−T0)]R(T) = R_0[1 + \alpha(T - T_0)]. The heat capacity of the variable resistor also varies with temperature as C(T)=C0[1+α(T−T0)]C(T) = C_0[1 + \alpha(T - T_0)], where C0C_0 is a positive constant. Assuming that all the Joule heat generated in the variable resistor is retained by it (adiabatic process) and the fixed resistor maintains a constant resistance R0R_0, find the time tt at which the current in the circuit drops to V3R0\frac{V}{3R_0}.

Options

  • A.

    19C0R03αV2\frac{19 C_0 R_0}{3 \alpha V^2}

  • B.

    7C0R03αV2\frac{7 C_0 R_0}{3 \alpha V^2}

  • C.

    6C0R0αV2\frac{6 C_0 R_0}{\alpha V^2}

  • D.

    19C0R06αV2\frac{19 C_0 R_0}{6 \alpha V^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

Temperature Coefficient (Alpha)|Kirchhoff’s Loop Rule|Power Dissipation Ratio

Why This Question Is Tricky

Common Mistakes

This problem tests the student's ability to couple non-linear circuit dynamics with thermodynamics.

The primary trap lies in the misapplication of Joule heating and heat capacity.

Students often incorrectly assume a steady state, use a constant initial power dissipation P0=V2/(4R0)P_0 = V^2/(4R_0), or forget that the current I(t)I(t) is dynamically dependent on the changing resistance R(t)R(t) via Kirchhoff's Loop Rule (ignoring the fixed series resistor).

Furthermore, the problem introduces a temperature-dependent heat capacity C(T)C(T) which scales linearly with resistance.

Failing to express dQdQ strictly in terms of RR and dRdR leads to unsolvable or incorrect differential equations.

The correct approach requires setting up a first-order differential equation linking dtdt and dRdR by continuously updating the power P=I2RP = I^2R as the series loop resistance increases.

Quick Facts About This Question

Question Information

SubjectPhysics
ChapterCurrent Electricity - Class 12
ConceptTemperature Coefficient (Alpha)
Difficulty8
Cognitive Load7
Target Solve Time160 sec
AccessFree