Electric Current — Question 10

Section 26-1 · Physics pages 4170–4171

Question 10 Two current probes expose charge accumulating between their planes Two probes bracket a wire segment. Toward +x, they measure IL = I0 and IR = I0(1 −e−t/τ) for t ≥0. The segment starts neutral. Qmseg +x IL IR Wire cross-section and reference direction; dimensions are schematic. (a) Find its excess charge as a function of time and its limiting charge. (b) Find the time when 90 percent of the limiting charge has accumulated, and explain why the steady currents eventually agree.
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Question 10 - Solution Two current probes expose charge accumulating between their planes Qmseg +x IL IR (a) Method and calculation dQseg/dt = IL −IR = I0e−t/τ. Qseg = I0τ(1 −e−t/τ), Q∞= I0τ. (b) Interpretation and further calculation 1 −e−t90/τ = .9 ⇒t90 = τ ln 10. lim t→∞(IL −IR) = 0 ⇒lim dQseg/dt = 0. Physical check The segment retains a finite excess charge after accumulation stops; steady transport does not require exact neutrality.

Question 10

Two current probes expose charge accumulating between their planes

Two probes bracket a wire segment. Toward +x+x, they measure IL=I0I_L=I_0 and IR=I0(1−e−t/τ)I_R=I_0(1-e^{-t/\tau}) for t≥0t\ge0. The segment starts neutral.

Diagram shown in the original SVG worksheet.

  1. Find its excess charge as a function of time and its limiting charge.

  2. Find the time when 90 percent of the limiting charge has accumulated, and explain why the steady currents eventually agree.

Question 10 - Solution

Two current probes expose charge accumulating between their planes

Diagram shown in the original SVG worksheet.

(a) Method and calculation

dQseg/dt=IL−IR=I0e−t/τ.dQ_{\mathrm{seg}}/dt=I_L-I_R=I_0e^{-t/\tau}.Qseg=I0τ(1−e−t/τ),Q∞=I0τ.Q_{\mathrm{seg}}=I_0\tau(1-e^{-t/\tau}),\quad Q_\infty=I_0\tau.

(b) Interpretation and further calculation

1−e−t90/τ=.9⇒t90=τln⁡10.1-e^{-t_{90}/\tau}=.9\Rightarrow t_{90}=\tau\ln10.limt→∞(IL−IR)=0⇒lim⁡dQseg/dt=0.\lim_{t\to\infty}(I_L-I_R)=0\Rightarrow\lim dQ_{\mathrm{seg}}/dt=0.

Physical check

The segment retains a finite excess charge after accumulation stops; steady transport does not require exact neutrality.