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Question #43720

Difficulty: 8/10 | 🟢 Free

The Question

A dilute colloidal suspension of spherical semiconductor particles, each of radius rr and positive charge qq, is confined in a fluid medium between x=0x = 0 and x=Lx = L. A uniform electric field EE is applied in the +x+x direction. The fluid is subjected to a steady temperature gradient such that the local absolute temperature is T(x)=T0(1+αx)T(x) = T_0(1 + \alpha x), where T0T_0 and α\alpha are positive constants. The dynamic viscosity of the fluid varies with temperature as η(T)=η0T0T\eta(T) = \eta_0 \frac{T_0}{T}.

The particle flux is governed by the Nernst-Planck equation J=n(x)vd(x)−D(x)dndxJ = n(x)v_d(x) - D(x)\frac{dn}{dx}, where n(x)n(x) is the local particle concentration, vd(x)v_d(x) is the local drift velocity determined by Stokes' drag, and D(x)D(x) is the local diffusion coefficient given by the Stokes-Einstein relation D(x)=kBT(x)6πη(x)rD(x) = \frac{k_B T(x)}{6\pi\eta(x) r}.

Assuming steady-state conditions with zero net flux (J=0J = 0), which of the following expressions correctly represents the concentration profile n(x)n(x)?

Options

  • A.

    n(x)=n(0)(1+αx)qEαkBT0n(x) = n(0) (1 + \alpha x)^{\frac{qE}{\alpha k_B T_0}}

  • B.

    n(x)=n(0)exp⁡[qEkBT0(x+αx22)]n(x) = n(0) \exp\left[ \frac{qE}{k_B T_0} \left( x + \frac{\alpha x^2}{2} \right) \right]

  • C.

    n(x)=n(0)exp⁡[qEαkBT0(1−11+αx)]n(x) = n(0) \exp\left[ \frac{qE}{\alpha k_B T_0} \left( 1 - \frac{1}{1+\alpha x} \right) \right]

  • D.

    n(x)=n(0)exp⁡[qEkBT0x]n(x) = n(0) \exp\left[ \frac{qE}{k_B T_0} x \right]

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

Drift vs Diffusion Current|Trajectory of Charged Particle|Viscosity and Stokes' Law

Why This Question Is Tricky

Common Mistakes

This question tests the fundamental origins of the drift-diffusion model under non-equilibrium thermodynamic conditions.

The primary trap lies in the temperature-dependent viscosity η(T)\eta(T).

Students often mistakenly calculate an effective constant diffusion coefficient D0D_0 or assume a constant drift velocity vd0v_{d0}, leading to incorrect exponential profiles (Options B and C).

By forcing the use of the local force balance (Stokes' drag) and the local Stokes-Einstein relation, the problem reveals a beautiful physical cancellation: the local viscosity η(x)\eta(x) drops out entirely when net flux is zero.

The concentration profile is dictated purely by the ratio of the conservative electric work to the local thermal energy, yielding a power-law distribution rather than the standard isothermal exponential decay.

Quick Facts About This Question

Question Information

SubjectPhysics
ChapterSemiconductor Electronics: Materials, Devices, and Simple Circuits - Class 12
ConceptDrift vs Diffusion Current
Difficulty8
Cognitive Load7
Target Solve Time160 sec
AccessFree