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Question #42560

Difficulty: 8/10 | 🟢 Free

The Question

For a certain diatomic gas, the molar heat capacity at constant volume is given by CV=f(T)2RC_V = \frac{f(T)}{2} R, where f(T)f(T) represents the effective number of degrees of freedom. Due to the gradual unfreezing of vibrational modes at high temperatures, f(T)f(T) varies non-linearly with temperature TT as f(T)=5+(T−T0)22T02f(T) = 5 + \frac{(T - T_0)^2}{2T_0^2} for T≥T0T \ge T_0. Calculate the change in internal energy of n=2 molesn = 2 \text{ moles} of this gas when it is heated from T=T0T = T_0 to T=3T0T = 3T_0 at constant volume.

Options

  • A.

    343RT0\frac{34}{3} R T_0

  • B.

    16 R T_0

  • C.

    12 R T_0

  • D.

    14 R T_0

Check Your Answer

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

Equipartition Theorem|Energy of Vibrational Modes|Calculus (Integration)

Why This Question Is Tricky

Common Mistakes

This question tests the fundamental understanding of the Equipartition Theorem during the transition phase of vibrational mode activation.

A common trap is for students to blindly apply the state formula U=f2nRTU = \frac{f}{2}nRT to calculate ΔU=f22nRT2−f12nRT1\Delta U = \frac{f_2}{2}nRT_2 - \frac{f_1}{2}nRT_1, which yields the incorrect trap answer of 16RT016 R T_0.

This algebraic shortcut is physically invalid because U=f2nRTU = \frac{f}{2}nRT is derived under the assumption that ff is constant from absolute zero.

When degrees of freedom are temperature-dependent (unfreezing), the internal energy must be rigorously integrated using dU=nCVdTdU = n C_V dT.

Quick Facts About This Question

Question Information

SubjectPhysics
ChapterThermodynamics - Class 11 Part 2
ConceptEquipartition Theorem
Difficulty8
Cognitive Load7
Target Solve Time160 sec
AccessFree