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Question #84223

Difficulty: 8/10 | 🟢 Free

The Question

A uniform wire of initial length L0L_0, cross-sectional area AA, and perimeter pp is suspended in a vacuum chamber maintained at a constant ambient temperature T0T_0. A constant mechanical tension FF is applied to the wire. Simultaneously, a constant direct current II is passed through it. The resistivity of the wire varies with temperature as ρ(T)=ρ0[1+β(T−T0)]\rho(T) = \rho_0 [1 + \beta(T - T_0)], where ρ0\rho_0 is the resistivity at T0T_0. Due to lattice anharmonicity, the Young's modulus of the wire decreases with temperature as Y(T)=Y0[1−α(T−T0)]Y(T) = Y_0 [1 - \alpha(T - T_0)]. The wire loses heat to the surroundings purely by radiation. The emissivity of the wire surface is ϵ\epsilon, and the Stefan-Boltzmann constant is σ\sigma. Assuming the steady-state temperature rise ΔT=T−T0\Delta T = T - T_0 is small (ΔT≪T0\Delta T \ll T_0), what is the steady-state elastic elongation ΔL\Delta L of the wire? (Ignore the thermal expansion of the wire and assume the cross-sectional area remains approximately constant).

Options

  • A.

    FL0AY0[4σϵpAT03−I2ρ0β4σϵpAT03−I2ρ0(α+β)]\frac{F L_0}{A Y_0} \left[ \frac{4 \sigma \epsilon p A T_0^3 - I^2 \rho_0 \beta}{4 \sigma \epsilon p A T_0^3 - I^2 \rho_0 (\alpha + \beta)} \right]

  • B.

    FL0AY0[4σϵpAT034σϵpAT03−I2ρ0α]\frac{F L_0}{A Y_0} \left[ \frac{4 \sigma \epsilon p A T_0^3}{4 \sigma \epsilon p A T_0^3 - I^2 \rho_0 \alpha} \right]

  • C.

    FL0AY0[σϵpAT03−I2ρ0βσϵpAT03−I2ρ0(α+β)]\frac{F L_0}{A Y_0} \left[ \frac{\sigma \epsilon p A T_0^3 - I^2 \rho_0 \beta}{\sigma \epsilon p A T_0^3 - I^2 \rho_0 (\alpha + \beta)} \right]

  • D.

    FL0AY0[4σϵpAT03+I2ρ0β4σϵpAT03+I2ρ0(α+β)]\frac{F L_0}{A Y_0} \left[ \frac{4 \sigma \epsilon p A T_0^3 + I^2 \rho_0 \beta}{4 \sigma \epsilon p A T_0^3 + I^2 \rho_0 (\alpha + \beta)} \right]

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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

Young's Modulus Sensitivity|Relaxation Time Dependency|Binomial Approximation

Why This Question Is Tricky

Examiner Levers

Variable Manipulation

Algebraic solutions only (No numbers); tests pure symbolic logic.

Difficulty Boost : +4

Common Mistakes

This question tests the coupled nature of electro-thermal-mechanical systems, specifically targeting the misconception that steady-state electrical heating is independent of the final equilibrium temperature.

Students often incorrectly assume Pin=I2R0P_{in} = I^2 R_0 (ignoring the temperature coefficient of resistivity β\beta during the heating phase), which leads to Trap B.

Furthermore, the problem requires the correct linearization of the Stefan-Boltzmann law using the binomial approximation (Trap C tests the omission of the factor of 4).

Finally, it evaluates the ability to correctly substitute the modified, temperature-dependent Young's modulus into Hooke's law, linking the microscopic relaxation time (which dictates ρ\rho) to the macroscopic lattice anharmonicity (which dictates YY).

Quick Facts About This Question

Question Information

SubjectPhysics
ChapterMechanical Properties of Solids - Class 11 Part 2
ConceptYoung's Modulus Sensitivity
Difficulty8
Cognitive Load7
Target Solve Time160 sec
AccessFree