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Question #42169

Difficulty: 8/10 | 🟢 Free

The Question

A cylindrical vessel of constant cross-sectional area AA contains a liquid of mass MM. Initially, the liquid is at a uniform temperature T0T_0 and has height HH. The density of the liquid varies with temperature as ρ(T)=ρ0[1−γ(T−T0)]\rho(T) = \rho_0[1 - \gamma(T - T_0)], where γ\gamma is the volumetric expansion coefficient (assume γΔT≪1\gamma \Delta T \ll 1). The liquid is subjected to two different heating processes:

Process I: The liquid is heated uniformly to a final temperature T0+ΔTT_0 + \Delta T. Process II: The liquid is heated such that its temperature varies linearly with height zz from the bottom, with the bottom at T0T_0 and the top surface at T0+2ΔTT_0 + 2\Delta T.

Let UIU_I and UIIU_{II} be the final gravitational potential energies of the liquid in Process I and Process II, respectively. Assuming the vessel does not expand, find the difference UI−UIIU_I - U_{II}.

Options

  • A.

    16MgHγΔT\frac{1}{6} M g H \gamma \Delta T

  • B.

    13MgHγΔT\frac{1}{3} M g H \gamma \Delta T

  • C.

    12MgHγΔT\frac{1}{2} M g H \gamma \Delta T

  • D.

    0

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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

State Function vs Path Function|Gravitational Potential Energy (System)|Variation of Density with Temperature

Why This Question Is Tricky

Common Mistakes

This question tests the misconception that gravitational potential energy is a pure state function of macroscopic variables (like total mass and average temperature) or depends only on the final geometric boundaries of the system.

Students often calculate the final height of the fluid, find it to be identical in both processes (Hf≈H(1+γΔT)H_f \approx H(1 + \gamma \Delta T)), and incorrectly conclude that the potential energies must be equal (Option D).

The trap exposes the deep coupling between thermodynamics and mechanics: the spatial distribution of density (the thermal path) shifts the Center of Mass independently of the geometric boundaries.

In the gradient process, the lower half is cooler and denser, concentrating more mass at a lower height and resulting in a lower overall potential energy.

Quick Facts About This Question

Question Information

SubjectPhysics
ChapterThermodynamics - Class 11 Part 2
ConceptState Function vs Path Function
Difficulty8
Cognitive Load7
Target Solve Time160 sec
AccessFree