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Question #42657

Difficulty: 8/10 | 🟢 Free

The Question

A semi-infinite solid rod of constant cross-sectional area AA extends along the x-axis from x=0x = 0 to x→∞x \to \infty. The thermal conductivity of the material varies spatially as k(x)=k0(1+xL)2k(x) = k_0 \left(1 + \frac{x}{L}\right)^2, where k0k_0 and LL are positive constants. Heat is generated internally throughout the rod at a steady volumetric rate (power per unit volume) given by q(x)=q0(1+xL)2q(x) = \frac{q_0}{\left(1 + \frac{x}{L}\right)^2}, where q0q_0 is a positive constant. The end of the rod at x=0x = 0 is perfectly insulated. If the temperature as x→∞x \to \infty approaches a constant reference temperature T∞T_\infty, what is the steady-state temperature T0T_0 at the insulated end x=0x = 0?

Options

  • A.

    T∞+q0L22k0T_\infty + \frac{q_0 L^2}{2 k_0}

  • B.

    T∞+q0L2k0T_\infty + \frac{q_0 L^2}{k_0}

  • C.

    T∞+q0L23k0T_\infty + \frac{q_0 L^2}{3 k_0}

  • D.

    T∞+2q0L2k0T_\infty + \frac{2 q_0 L^2}{k_0}

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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

Reference Potential Convention|First Law Application|Steady State Temperature Gradient|Integration

Why This Question Is Tricky

Common Mistakes

This question tests the student's ability to apply the First Law of Thermodynamics (energy conservation) and Fourier's Law in a distributed parameter system, serving as an exact electro-thermal analogy to Gauss's Law for non-uniform charge distributions.

The primary trap (Option B) exploits the misconception of lumping distributed generation into a single point source.

Students often calculate the total heat generated (Qtotal=q0ALQ_{total} = q_0 A L) and the total thermal resistance (Rtotal=L/(k0A)R_{total} = L / (k_0 A)), and incorrectly multiply them (ΔT=QtotalRtotal\Delta T = Q_{total} R_{total}) as if all heat must traverse the entire resistance.

This ignores the spatial distribution of the heat flux H(x)H(x), which is zero at the insulated boundary and grows asymptotically, requiring a rigorous integration of the local temperature gradient.

Quick Facts About This Question

Question Information

SubjectPhysics
ChapterElectrostatic Potential and Capacitance - Class 12
ConceptReference Potential Convention
Difficulty8
Cognitive Load7
Target Solve Time160 sec
AccessFree