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Question #42518

Difficulty: 8/10 | 🟢 Free

The Question

A solid cylindrical rod of length LL, cross-sectional area AA, Young's modulus YY, and coefficient of linear thermal expansion α\alpha is rigidly clamped between two immovable walls at an ambient temperature T0T_0. It is heated via a calorimetry setup involving a hot liquid, reaching an initial uniform temperature T0+ΔT0T_0 + \Delta T_0. The combined heat capacity of the rod (excluding elastic energy) and the liquid is C0C_0. The system is then allowed to cool. The calorimeter loses heat to the surroundings at a rate dQdt=−k(T−T0)\frac{dQ}{dt} = -k(T - T_0), where kk is a positive constant and TT is the instantaneous temperature. Assuming the rod and liquid are always in thermal equilibrium, what is the time tt taken for the system to cool to T0+ΔT02T_0 + \frac{\Delta T_0}{2}?

Options

  • A.

    C0kln⁡2+YALα2ΔT02k\frac{C_0}{k} \ln 2 + \frac{Y A L \alpha^2 \Delta T_0}{2k}

  • B.

    C0kln⁡2+YALα2ΔT0k\frac{C_0}{k} \ln 2 + \frac{Y A L \alpha^2 \Delta T_0}{k}

  • C.

    C0kln⁡2−YALα2ΔT02k\frac{C_0}{k} \ln 2 - \frac{Y A L \alpha^2 \Delta T_0}{2k}

  • D.

    C0kln⁡2\frac{C_0}{k} \ln 2

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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

Calorimetry with Heat Loss|Thermal Stress Calculation|Internal Energy Dependency

Why This Question Is Tricky

Common Mistakes

This question tests the coupling of macroscopic thermodynamics with solid mechanics.

The primary trap is neglecting the elastic potential energy stored in the rod due to thermal stress when clamped between rigid walls.

Students commonly assume the heat capacity of the system is constant (C0C_0) and use dQ=C0dTdQ = C_0 dT, leading to the standard exponential cooling time (Option D).

However, the constrained expansion results in internal elastic potential energy being stored in the rod, Uelastic=12YALα2(ΔT)2U_{elastic} = \frac{1}{2} Y A L \alpha^2 (\Delta T)^2.

This makes the effective heat capacity temperature-dependent (Ceff=C0+YALα2ΔTC_{eff} = C_0 + Y A L \alpha^2 \Delta T), requiring integration of a modified differential equation to find the correct cooling time.

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Question Information

SubjectPhysics
ChapterThermal Properties of Matter - Class 11 Part 2
ConceptCalorimetry with Heat Loss
Difficulty8
Cognitive Load7
Target Solve Time160 sec
AccessFree