Gauss' Law — Question 10

Section 23-3 · Physics pages 3690–3691

Question 10 A changing electric flux determines the net charge current through a boundary Through a fixed closed surface the outward electric flux is Φ(t) = Φ0e−t/τ for t ≥0, with Φ0, τ > 0. Define outward conventional charge current Iout = −dQenc/dt. Assume Gauss law holds at each time. t Φ Axes and labels specify the model; the sketch is schematic. (a) Derive the enclosed charge and outward current as functions of time. (b) Find the total charge leaving between 0 and τ, and the time when half the initial enclosed charge remains.
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Question 10 - Solution A changing electric flux determines the net charge current through a boundary t Φ (a) Method and calculation Qenc(t) = ϵ0Φ0e−t/τ. Iout(t) = −ϵ0 dΦ dt = ϵ0Φ0 τ e−t/τ > 0. (b) Interpretation and further calculation Qleft(0, τ) = ∫τ 0 Iout dt = ϵ0Φ0(1 −e−1). Q(t1/2) = 1 2Q(0) ⇒t1/2 = τ ln 2. Electric flux is not itself a flow of charge; charge conservation relates its time derivative to the net current here. Physical check The decreasing positive enclosed charge corresponds to a positive net outward conventional current.

Question 10

A changing electric flux determines the net charge current through a boundary

Through a fixed closed surface the outward electric flux is Φ(t)=Φ0e−t/τ\Phi(t)=\Phi_0e^{-t/\tau} for t≥0t\ge0, with Φ0,τ>0\Phi_0,\tau>0. Define outward conventional charge current Iout=−dQenc/dtI_{\mathrm{out}}=-dQ_{\mathrm{enc}}/dt. Assume Gauss law holds at each time.

Diagram shown in the original SVG worksheet.

  1. Derive the enclosed charge and outward current as functions of time.

  2. Find the total charge leaving between 0 and τ\tau, and the time when half the initial enclosed charge remains.

Question 10 - Solution

A changing electric flux determines the net charge current through a boundary

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Qenc(t)=ϵ0Φ0e−t/τ.Q_{\mathrm{enc}}(t)=\epsilon_0\Phi_0e^{-t/\tau}.Iout(t)=−ϵ0dΦdt=ϵ0Φ0τe−t/τ>0.I_{\mathrm{out}}(t)=-\epsilon_0\frac{d\Phi}{dt}=\frac{\epsilon_0\Phi_0}{\tau}e^{-t/\tau}>0.

(b) Interpretation and further calculation

Qleft(0,τ)=∫0τIoutdt=ϵ0Φ0(1−e−1).Q_{\mathrm{left}}(0,\tau)=\int_0^\tau I_{\mathrm{out}}\,dt=\epsilon_0\Phi_0(1-e^{-1}).Q(t1/2)=12Q(0)⇒t1/2=τln⁡2.Q(t_{1/2})=\tfrac12Q(0)\Rightarrow t_{1/2}=\tau\ln2.Electric flux is not itself a flow of charge; charge conservation relates its time derivative to the net current here.

Physical check

The decreasing positive enclosed charge corresponds to a positive net outward conventional current.