A Microscopic View of Ohm's Law — Question 1

Section 26-5 · Physics pages 4232–4233

Question 1 A step field builds drift toward a finite steady velocity Use the relaxation model m d⃗vd/dt = −e⃗E −m⃗vd/τ, with electron charge −e, mass m and constant positive relaxation time tau. At t=0 a uniform field E0ˆx is switched on in an initially zero-drift electron gas of density n. t Jx Axes and labels specify the model; the sketch is schematic. (a) Solve for drift velocity and current density. (b) Find when the current reaches 95 percent of its steady value and state the steady conductivity.
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Question 1 - Solution A step field builds drift toward a finite steady velocity t Jx (a) Method and calculation vx(t) = −eE0τ m (1 −e−t/τ). Jx = −nevx = ne2τ m E0(1 −e−t/τ). (b) Interpretation and further calculation Jx/J∞= .95 ⇒t95 = τ ln 20 = 2.99573τ. σ0 = J∞/E0 = ne2τ/m. Physical check Scattering balances the electric force in steady drift; it does not stop all microscopic motion.

Question 1

A step field builds drift toward a finite steady velocity

Use the relaxation model mdv→d/dt=−eE→−mv→d/τm\,d\vec v_d/dt=-e\vec E-m\vec v_d/\tau, with electron charge −e-e, mass m and constant positive relaxation time tau. At t=0 a uniform field E0x̂E_0\hat x is switched on in an initially zero-drift electron gas of density n.

Diagram shown in the original SVG worksheet.

  1. Solve for drift velocity and current density.

  2. Find when the current reaches 95 percent of its steady value and state the steady conductivity.

Question 1 - Solution

A step field builds drift toward a finite steady velocity

Diagram shown in the original SVG worksheet.

(a) Method and calculation

vx(t)=−eE0τm(1−e−t/τ).v_x(t)=-\frac{eE_0\tau}{m}(1-e^{-t/\tau}).Jx=−nevx=ne2τmE0(1−e−t/τ).J_x=-nev_x=\frac{ne^2\tau}{m}E_0(1-e^{-t/\tau}).

(b) Interpretation and further calculation

Jx/J∞=.95⇒t95=τln⁡20=2.99573τ.J_x/J_\infty=.95\Rightarrow t_{95}=\tau\ln20=2.99573\tau.σ0=J∞/E0=ne2τ/m.\sigma_0=J_\infty/E_0=ne^2\tau/m.

Physical check

Scattering balances the electric force in steady drift; it does not stop all microscopic motion.