The Electric Field Due to a Point Charge — Question 6

Section 22-3 · Physics pages 3522–3523

Question 6 Removing one member of a symmetric charge ring exposes its missing contribution Eight equal positive point charges q occupy the vertices of a regular octagon of circumradius R. One vertex lies on the positive x axis. Coulomb constant is k. x Schematic; labels, not drawing lengths, specify the data. (a) Find the center field before and after removing the charge at that vertex. (b) Instead of removing it, replace that charge by −2q. Find the new center field using a change in source charge rather than resumming all eight contributions.
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Question 6 - Solution Removing one member of a symmetric charge ring exposes its missing contribution x (a) Method and calculation Einitial = 0, Eremoved source = −kq R2 ˆx. Eafter removal = + kq R2 ˆx. (b) Interpretation and further calculation ∆q = −2q −q = −3q. ∆E = −k∆q R2 ˆx = +3kq R2 ˆx. The original symmetric sum cancels, leaving only the field of the change. Physical check The missing contribution points opposite the field left by its removal.

Question 6

Removing one member of a symmetric charge ring exposes its missing contribution

Eight equal positive point charges q occupy the vertices of a regular octagon of circumradius R. One vertex lies on the positive x axis. Coulomb constant is k.

Diagram shown in the original SVG worksheet.

  1. Find the center field before and after removing the charge at that vertex.

  2. Instead of removing it, replace that charge by −2q-2q. Find the new center field using a change in source charge rather than resumming all eight contributions.

Question 6 - Solution

Removing one member of a symmetric charge ring exposes its missing contribution

Diagram shown in the original SVG worksheet.

(a) Method and calculation

𝑬initial=𝟎,𝑬removedsource=−kqR2𝒙̂.\mathbf E_{\mathrm{initial}}=\mathbf0,\quad\mathbf E_{\mathrm{removed\ source}}=-\frac{kq}{R^2}\hat{\mathbf x}.𝑬afterremoval=+kqR2𝒙̂.\mathbf E_{\mathrm{after\ removal}}=+\frac{kq}{R^2}\hat{\mathbf x}.

(b) Interpretation and further calculation

Δq=−2q−q=−3q.\Delta q=-2q-q=-3q.Δ𝑬=−kΔqR2𝒙̂=+3kqR2𝒙̂.\Delta\mathbf E=-\frac{k\Delta q}{R^2}\hat{\mathbf x}=+\frac{3kq}{R^2}\hat{\mathbf x}.The original symmetric sum cancels, leaving only the field of the change.

Physical check

The missing contribution points opposite the field left by its removal.