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Question #42569

Difficulty: 8/10 | 🟢 Free

The Question

Consider an intrinsic semiconductor at temperature TT with a temperature-dependent energy band gap Eg(T)=E0−αTE_g(T) = E_0 - \alpha T, where E0E_0 and α\alpha are positive constants. The intrinsic carrier density is given by ni(T)=AT3/2exp⁡(−Eg(T)2kBT)n_i(T) = A T^{3/2} \exp\left(-\frac{E_g(T)}{2k_B T}\right), where AA is a temperature-independent constant and kBk_B is the Boltzmann constant. Treating the thermally excited electrons and holes as a non-degenerate ideal gas, the Helmholtz free energy per unit volume of this electron-hole gas is f=−2nikBTf = -2 n_i k_B T. Which of the following represents the electronic entropy per unit volume (SeS_e) and the internal energy per unit volume (ueu_e) of the electron-hole gas?

Options

  • A.

    Se=ni(5kB+E0T),ue=ni(E0+3kBT)S_e = n_i \left( 5 k_B + \frac{E_0}{T} \right), \quad u_e = n_i (E_0 + 3 k_B T)

  • B.

    Se=ni(5kB+Eg(T)T),ue=ni(Eg(T)+3kBT)S_e = n_i \left( 5 k_B + \frac{E_g(T)}{T} \right), \quad u_e = n_i (E_g(T) + 3 k_B T)

  • C.

    Se=ni(3kB+E0T),ue=ni(E0+32kBT)S_e = n_i \left( 3 k_B + \frac{E_0}{T} \right), \quad u_e = n_i \left(E_0 + \frac{3}{2} k_B T\right)

  • D.

    Se=ni(3kB+Eg(T)T),ue=ni(Eg(T)+32kBT)S_e = n_i \left( 3 k_B + \frac{E_g(T)}{T} \right), \quad u_e = n_i \left(E_g(T) + \frac{3}{2} k_B T\right)

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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

Entropy and Reversibility|Equipartition Theorem|Energy Band Gap Temperature Dependency

Why This Question Is Tricky

Common Mistakes

This question targets a profound misconception in semiconductor thermodynamics: conflating the temperature-dependent band gap Eg(T)E_g(T) with the internal energy of electron-hole pair formation.

Students often naively assume the internal energy is ue=ni(Eg(T)+3kBT)u_e = n_i(E_g(T) + 3k_B T) by applying the equipartition theorem and adding the instantaneous gap energy.

However, Eg(T)E_g(T) actually represents the change in Helmholtz free energy (ΔF\Delta F) required to create a pair.

By forcing students to derive entropy from the free energy f=−2nikBTf = -2n_i k_B T, the math reveals that the αT\alpha T term in Eg(T)E_g(T) cancels out during differentiation.

The true internal energy of formation is E0E_0, demonstrating that the temperature dependence of the band gap is purely an entropic effect driven by electron-phonon interactions and lattice expansion.

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Question Information

SubjectPhysics
ChapterThermodynamics - Class 11 Part 2
ConceptEntropy and Reversibility
Difficulty8
Cognitive Load7
Target Solve Time160 sec
AccessFree