The Electrical Properties of Solids — Question 10

Section 41-1 · Physics pages 6810–6811

Question 10 Charge imbalance relaxes on a conductivity-dependent time scale In a uniform ohmic material, J = σE, ∇· E = ρq/ε, and charge continuity is ∂tρq + ∇· J = 0. Treat σ, ε as constants. t ρq Schematic; labels, not drawing lengths, specify the data. (a) Derive the decay law for a small bulk free-charge imbalance. (b) Find the relaxation time for ε = 4ε0, σ = 2.00 × 10−8 S/m and ε0 = 8.854 × 10−12 F/m.
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Question 10 - Solution Charge imbalance relaxes on a conductivity-dependent time scale t ρq (a) Method and calculation ∂tρq = −σ∇· E = −(σ/ε)ρq. ρq(t) = ρq(0)e−t/τ, τ = ε/σ . (b) Interpretation and further calculation τ = 4(8.854 × 10−12)/(2.00 × 10−8). τ = 1.7708 ms . Physical check The derivation concerns bulk free-charge relaxation under a local linear constitutive law. It does not imply that all surface charge on an isolated object disappears.

Question 10

Charge imbalance relaxes on a conductivity-dependent time scale

In a uniform ohmic material, 𝑱=σ𝑬\boldsymbol J=\sigma\boldsymbol E, ∇⋅𝑬=ρq/ε\nabla\cdot\boldsymbol E=\rho_q/\varepsilon, and charge continuity is ∂tρq+∇⋅𝑱=0\partial_t\rho_q+\nabla\cdot\boldsymbol J=0. Treat σ,ε\sigma,\varepsilon as constants.

Diagram shown in the original SVG worksheet.

  1. Derive the decay law for a small bulk free-charge imbalance.

  2. Find the relaxation time for ε=4ε0\varepsilon=4\varepsilon_0, σ=2.00×10−8S/m\sigma=2.00\times10^{-8}\,\mathrm{S/m} and ε0=8.854×10−12F/m\varepsilon_0=8.854\times10^{-12}\,\mathrm{F/m}.

Question 10 - Solution

Charge imbalance relaxes on a conductivity-dependent time scale

Diagram shown in the original SVG worksheet.

(a) Method and calculation

∂tρq=−σ∇⋅𝑬=−(σ/ε)ρq.\partial_t\rho_q=-\sigma\nabla\cdot\boldsymbol E=-(\sigma/\varepsilon)\rho_q.ρq(t)=ρq(0)e−t/τ,τ=ε/σ.\boxed{\rho_q(t)=\rho_q(0)e^{-t/\tau},\quad\tau=\varepsilon/\sigma}.

(b) Interpretation and further calculation

τ=4(8.854×10−12)/(2.00×10−8).\tau=4(8.854\times10^{-12})/(2.00\times10^{-8}).τ=1.7708ms.\boxed{\tau=1.7708\,\mathrm{ms}}.

Physical check

The derivation concerns bulk free-charge relaxation under a local linear constitutive law. It does not imply that all surface charge on an isolated object disappears.