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Question #42816

Difficulty: 8/10 | 🟢 Free

The Question

Consider a classical electron gas of mass mm and charge −e-e at temperature TT in a uniform electric field EE. In the microscopic Drude-Lorentz model, the drift velocity of an electron with thermal speed vv is given by vd(v)=eEmτ(v)v_d(v) = \frac{eE}{m}\tau(v), where τ(v)\tau(v) is the relaxation time. Assume the electrons scatter off neutral impurities such that their mean free path λ\lambda is constant and independent of vv. The macroscopic drift velocity ⟨vd⟩\langle v_d \rangle is defined as the average of vd(v)v_d(v) over the 3D Maxwell-Boltzmann speed distribution f(v)f(v). Which of the following expressions gives the correct macroscopic drift velocity? (Here kBk_B is the Boltzmann constant).

Options

  • A.

    eEλ2πmkBTeE\lambda \sqrt{\frac{2}{\pi m k_B T}}

  • B.

    eEλπ8mkBTeE\lambda \sqrt{\frac{\pi}{8 m k_B T}}

  • C.

    eEλ13mkBTeE\lambda \sqrt{\frac{1}{3 m k_B T}}

  • D.

    eEλ2mkBTeE\lambda \sqrt{\frac{2}{m k_B T}}

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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

Relaxation Time Dependency|Maxwell-Boltzmann Distribution|Temperature and Kinetic Energy

Why This Question Is Tricky

Common Mistakes

This question tests the student's ability to correctly apply statistical averaging over a velocity distribution rather than relying on lumped macroscopic parameters.

A common trap (related to Jensen's Inequality) is assuming that the average of an inverse quantity equals the inverse of the average, i.e., ⟨τ(v)⟩=λ/⟨v⟩\langle \tau(v) \rangle = \lambda / \langle v \rangle.

Students falling for this will incorrectly substitute the mean speed ⟨v⟩=8kBT/πm\langle v \rangle = \sqrt{8k_B T / \pi m} into the drift velocity formula, leading to Option B.

The correct physical approach requires integrating the speed-dependent drift velocity vd(v)∝v−1v_d(v) \propto v^{-1} over the 3D Maxwell-Boltzmann probability density function, which yields a different numerical prefactor and correctly captures the microscopic transport physics.

Quick Facts About This Question

Question Information

SubjectPhysics
ChapterCurrent Electricity - Class 12
ConceptRelaxation Time Dependency
Difficulty8
Cognitive Load7
Target Solve Time160 sec
AccessFree