Electric Current — Question 4

Section 26-1 · Physics pages 4158–4159

Question 4 A changing branch current requires temporary charge storage For 0 ≤t ≤T, currents I1 = I0 and I2 = I0t/T enter a small node, while I3 = 3I0t/T leaves it. Initially its excess charge is zero. I1 I2 I3 Q Schematic; labels, not drawing lengths, specify the data. (a) Derive the stored charge and determine its maximum. (b) Find the final charge and explain whether zero final charge permits unequal instantaneous currents.
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Question 4 - Solution A changing branch current requires temporary charge storage I1 I2 I3 Q (a) Method and calculation dQ/dt = I1 + I2 −I3 = I0(1 −2t/T). Q(t) = I0(t −t2/T), Qmax = I0T/4 at t = T/2. (b) Interpretation and further calculation Q(T) = I0(T −T) = 0. ∫T 0 (Iin −Iout) dt = 0, Iin̸ = Iout in general. Physical check The usual equal-current junction rule is the special case of negligible charge accumulation.

Question 4

A changing branch current requires temporary charge storage

For 0≤t≤T0\le t\le T, currents I1=I0I_1=I_0 and I2=I0t/TI_2=I_0t/T enter a small node, while I3=3I0t/TI_3=3I_0t/T leaves it. Initially its excess charge is zero.

Diagram shown in the original SVG worksheet.

  1. Derive the stored charge and determine its maximum.

  2. Find the final charge and explain whether zero final charge permits unequal instantaneous currents.

Question 4 - Solution

A changing branch current requires temporary charge storage

Diagram shown in the original SVG worksheet.

(a) Method and calculation

dQ/dt=I1+I2−I3=I0(1−2t/T).dQ/dt=I_1+I_2-I_3=I_0(1-2t/T).Q(t)=I0(t−t2/T),Qmax=I0T/4at t=T/2.Q(t)=I_0(t-t^2/T),\quad Q_{\max}=I_0T/4\ \text{at }t=T/2.

(b) Interpretation and further calculation

Q(T)=I0(T−T)=0.Q(T)=I_0(T-T)=0.∫0T(Iin−Iout)dt=0,Iin≠Ioutin general.\int_0^T(I_{\mathrm{in}}-I_{\mathrm{out}})\,dt=0,\quad I_{\mathrm{in}}\ne I_{\mathrm{out}}\ \text{in general}.

Physical check

The usual equal-current junction rule is the special case of negligible charge accumulation.