Metals — Question 2

Section 41-4 · Physics pages 6854–6855

Question 2 A field step reveals the time required to establish current A metal initially carries no current. At t = 0 a constant field E0 is applied. Use ˙J + J/τ = σ0E0/τ, where σ0 is the dc conductivity. t/τ J Schematic; labels, not drawing lengths, specify the data. (a) Solve for J(t) and its initial slope. (b) Find the time to reach 95 percent of the final current and the charge per area transported up to that time.
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Question 2 - Solution A field step reveals the time required to establish current t/τ J (a) Method and calculation d dt(Jet/τ) = σ0E0 τ et/τ ⇒J = σ0E0(1 −e−t/τ) . ˙J(0) = σ0E0/τ . (b) Interpretation and further calculation e−t95/τ = .05 ⇒t95 = τ ln 20 = 2.996τ . Q/A = ∫t95 0 Jdt = σ0E0τ(ln 20 −.95) . Physical check The initial response is inertial. At long times the relaxation term balances the field, leaving a finite steady current.

Question 2

A field step reveals the time required to establish current

A metal initially carries no current. At t=0t=0 a constant field E0E_0 is applied. Use J̇+J/τ=σ0E0/τ\dot J+J/\tau=\sigma_0E_0/\tau, where σ0\sigma_0 is the dc conductivity.

Diagram shown in the original SVG worksheet.

  1. Solve for J(t) and its initial slope.

  2. Find the time to reach 95 percent of the final current and the charge per area transported up to that time.

Question 2 - Solution

A field step reveals the time required to establish current

Diagram shown in the original SVG worksheet.

(a) Method and calculation

ddt(Jet/τ)=σ0E0τet/τ⇒J=σ0E0(1−e−t/τ).\frac{d}{dt}(Je^{t/\tau})=\frac{\sigma_0E_0}{\tau}e^{t/\tau}\Rightarrow\boxed{J=\sigma_0E_0(1-e^{-t/\tau})}.J̇(0)=σ0E0/τ.\boxed{\dot J(0)=\sigma_0E_0/\tau}.

(b) Interpretation and further calculation

e−t95/τ=.05⇒t95=τln⁡20=2.996τ.e^{-t_{95}/\tau}=.05\Rightarrow\boxed{t_{95}=\tau\ln20=2.996\tau}.Q/A=∫0t95Jdt=σ0E0τ(ln⁡20−.95).\boxed{Q/A=\int_0^{t_{95}}Jdt=\sigma_0E_0\tau(\ln20-.95)}.

Physical check

The initial response is inertial. At long times the relaxation term balances the field, leaving a finite steady current.