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Question #42727

Difficulty: 8/10 | 🟢 Free

The Question

A perfectly insulated cylindrical conductor of length LL (m), cross-sectional area AA (m2^2), and density DD (kg/m3^3) is initially solid at a temperature T0T_0 (K). A constant total direct current II (A) is passed through it. The material has a melting point TmT_m (K) (where Tm>T0T_m > T_0), specific heat capacity cc (J/kg⋅\cdotK) in the solid phase, and latent heat of fusion LfL_f (J/kg). The electrical resistivities of the solid and liquid phases are ρs\rho_s (Ω⋅\Omega\cdotm) and ρl\rho_l (Ω⋅\Omega\cdotm) respectively, assumed independent of temperature. Assume infinite radial thermal conductivity (uniform temperature across any cross-section) and zero longitudinal heat conduction. As the conductor melts, the solid and liquid phases form parallel cylindrical channels extending the full length LL. What is the total time τ\tau (s) required for the conductor to completely melt?

Options

  • A.

    DA2I2[c(Tm−T0)ρs+Lf(ρs+ρl)2ρsρl]\frac{D A^2}{I^2} \left[ \frac{c(T_m - T_0)}{\rho_s} + \frac{L_f (\rho_s + \rho_l)}{2 \rho_s \rho_l} \right]

  • B.

    DA2I2ρs[c(Tm−T0)+Lf]\frac{D A^2}{I^2 \rho_s} \left[ c(T_m - T_0) + L_f \right]

  • C.

    DA2I2[c(Tm−T0)ρs+Lfρl−ρsln⁡(ρlρs)]\frac{D A^2}{I^2} \left[ \frac{c(T_m - T_0)}{\rho_s} + \frac{L_f}{\rho_l - \rho_s} \ln\left(\frac{\rho_l}{\rho_s}\right) \right]

  • D.

    DA2I2[c(Tm−T0)ρs+Lf(ρs+ρl)ρsρl]\frac{D A^2}{I^2} \left[ \frac{c(T_m - T_0)}{\rho_s} + \frac{L_f (\rho_s + \rho_l)}{\rho_s \rho_l} \right]

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Correct Answer

Step-by-Step Solution

Explanation

How the Examiner Thinks

Intuition_Breaker

Train your brain to resist "obvious" answers that are designed to deceive your intuition.

Concepts Behind This Question

Current Density Vector|Kirchhoff’s Junction Rule|Specific Heat Capacity of Phase Mixtures|Integration

Why This Question Is Tricky

Common Mistakes

Students often incorrectly assume that the macroscopic resistance of the wire remains constant at its initial solid-state value R=ρsL/AR = \rho_s L / A throughout the entire melting process (Option B).

This ignores the electro-thermal coupling where the newly formed liquid phase provides a parallel path for the current, altering the equivalent resistance and the total Joule heating rate I2ReqI^2 R_{eq}.

Furthermore, students might misapply the geometry of the phase boundary, assuming a longitudinal series melting front (Option C) instead of a parallel configuration, which fundamentally changes the integration of the current density distribution.

Quick Facts About This Question

Question Information

SubjectPhysics
ChapterCurrent Electricity - Class 12
ConceptCurrent Density Vector
Difficulty8
Cognitive Load7
Target Solve Time160 sec
AccessFree