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Question #82124

Difficulty: 5/10 | 🟢 Free

The Question

A metallic rod of initial length L0L_0 (in m\text{m}) and cross-sectional area AA (in m2\text{m}^2) is at an initial temperature T0T_0 (in K\text{K}). Its coefficient of linear thermal expansion is α\alpha (in K−1\text{K}^{-1}). The Young's modulus of the material varies with temperature TT as Y(T)=Y01+β(T−T0)Y(T) = \frac{Y_0}{1 + \beta (T - T_0)}, where Y0Y_0 (in N m−2\text{N m}^{-2}) and β\beta (in K−1\text{K}^{-1}) are positive constants. A tensile force FF (in N\text{N}) is gradually applied to the rod, increasing from 00 to F0F_0. Simultaneously, the temperature of the rod is increased from T0T_0 to T0+ΔTT_0 + \Delta T. The force is increased such that it is always proportional to the temperature change, i.e., F(T)=F0ΔT(T−T0)F(T) = \frac{F_0}{\Delta T} (T - T_0). Assuming the rod is free to expand and strains are small, what is the total work done (in J\text{J}) by the applied force FF during this process?

Options

  • A.

    12F0L0αΔT+F02L02AY0(1+43βΔT)\frac{1}{2} F_0 L_0 \alpha \Delta T + \frac{F_0^2 L_0}{2 A Y_0} \left( 1 + \frac{4}{3} \beta \Delta T \right)

  • B.

    12F0L0αΔT+F02L02AY0(1+βΔT)\frac{1}{2} F_0 L_0 \alpha \Delta T + \frac{F_0^2 L_0}{2 A Y_0} \left( 1 + \beta \Delta T \right)

  • C.

    F02L02AY0(1+43βΔT)\frac{F_0^2 L_0}{2 A Y_0} \left( 1 + \frac{4}{3} \beta \Delta T \right)

  • D.

    12F0L0αΔT+F02L02AY0\frac{1}{2} F_0 L_0 \alpha \Delta T + \frac{F_0^2 L_0}{2 A Y_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

Work Done in Stretching|Thermal Expansion of Area and Volume|Integration

Why This Question Is Tricky

Examiner Levers

Dimensional Analysis

Tests if the student verifies units/dimensions before selecting.

Difficulty Boost : +2

Common Mistakes

This question tests the fundamental definition of work W=∫FdlW = \int F dl against the common oversimplification of using W=12FmaxΔLtotalW = \frac{1}{2} F_{max} \Delta L_{total}.

Students often incorrectly apply the formula for elastic potential energy by superimposing the final thermal and stress strains, failing to recognize that when Young's modulus is temperature-dependent and force is applied simultaneously with heating, the work integral is path-dependent.

The non-commutativity of the strain superposition requires a rigorous line integral over the (T,F)(T, F) state space, exposing the flaw in treating total strain as a simple linear addition for energy calculations.

Quick Facts About This Question

Question Information

SubjectPhysics
ChapterMechanical Properties of Solids - Class 11 Part 2
ConceptWork Done in Stretching
Difficulty5
Cognitive Load6
Target Solve Time140 sec
AccessFree