Conductors and Insulators — Question 8

Section 21-2 · Physics pages 3406–3407

Question 8 A finite redistribution time separates transient charge from equilibrium charge A supplied model for two connected identical metal regions gives QA + QB = 12 nC and a charge difference D = QA −QB satisfying dD/dt = −D/τ, with τ = 2.0 ms. Initially (QA, QB) = (12, 0) nC. This model represents a measured equilibration law, not a universal constant for all conductors. t D Axes and labels specify the model; the sketch is schematic. (a) Solve for both charges as functions of time and evaluate them at t = 2.0 ms. (b) Find the minimum time for the magnitude of the charge difference to be at most 1 percent of its initial value.
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Question 8 - Solution A finite redistribution time separates transient charge from equilibrium charge t D (a) Method and calculation dD D = −dt τ ⇒D(t) = 12e−t/τ nC. QA = 6(1 + e−t/τ), QB = 6(1 −e−t/τ) nC. t = τ : QA ≈8.20728 nC, QB ≈3.79272 nC. (b) Interpretation and further calculation |D(t)|/|D(0)| = e−t/τ ≤.01. t ≥τ ln 100 ≈9.21034 ms. A very good equilibrium approximation occurs in finite time, although the ideal exponential becomes exactly zero only in the infinite-time limit. Physical check The sum remains constant throughout the transient; only the imbalance relaxes.

Question 8

A finite redistribution time separates transient charge from equilibrium charge

A supplied model for two connected identical metal regions gives QA+QB=12Q_A+Q_B=12 nC and a charge difference D=QA−QBD=Q_A-Q_B satisfying dD/dt=−D/τdD/dt=-D/\tau, with τ=2.0\tau=2.0 ms. Initially (QA,QB)=(12,0)(Q_A,Q_B)=(12,0) nC. This model represents a measured equilibration law, not a universal constant for all conductors.

Diagram shown in the original SVG worksheet.

  1. Solve for both charges as functions of time and evaluate them at t=2.0t=2.0 ms.

  2. Find the minimum time for the magnitude of the charge difference to be at most 1 percent of its initial value.

Question 8 - Solution

A finite redistribution time separates transient charge from equilibrium charge

Diagram shown in the original SVG worksheet.

(a) Method and calculation

dDD=−dtτ⇒D(t)=12e−t/τnC.\frac{dD}{D}=-\frac{dt}{\tau}\Rightarrow D(t)=12e^{-t/\tau}\,\mathrm{nC}.QA=6(1+e−t/τ),QB=6(1−e−t/τ)nC.Q_A=6(1+e^{-t/\tau}),\quad Q_B=6(1-e^{-t/\tau})\quad\mathrm{nC}.t=τ:QA≈8.20728nC,QB≈3.79272nC.t=\tau:\quad Q_A\approx8.20728\,\mathrm{nC},\quad Q_B\approx3.79272\,\mathrm{nC}.

(b) Interpretation and further calculation

|D(t)|/|D(0)|=e−t/τ≤.01.|D(t)|/|D(0)|=e^{-t/\tau}\le.01.t≥τln⁡100≈9.21034ms.t\ge\tau\ln100\approx9.21034\,\mathrm{ms}.A very good equilibrium approximation occurs in finite time, although the ideal exponential becomes exactly zero only in the infinite-time limit.

Physical check

The sum remains constant throughout the transient; only the imbalance relaxes.