Potential Due to a Group of Point Charges — Question 4

Section 24-6 · Physics pages 3898–3899

Question 4 A square with alternating charges cancels both center potential and field Four fixed charges occupy square vertices (±a, ±a). Charges +Q are at (a,a) and (-a,-a); charges -Q occupy the other two vertices. Use infinity reference. +Q +Q −Q −Q Schematic; labels, not drawing lengths, specify the data. (a) Find V and the electric field at the center. (b) Find V on the entire z axis and explain whether these cancellations imply that the field is zero everywhere.
Show solutionHide solution
Question 4 - Solution A square with alternating charges cancels both center potential and field +Q +Q −Q −Q (a) Method and calculation ri = √ 2a, V (0) = k √ 2a(Q + Q −Q −Q) = 0. E(0) = − k ( √ 2a)3 ∑ i qiri = 0. (b) Interpretation and further calculation V (0, 0, z) = k ∑ i qi √ 2a2 + z2 = 0. V (x, y, 0)̸ = 0 in general; V →±∞near the respective sources. Physical check Symmetry creates special cancellation sets, not an identically vanishing potential throughout space.

Question 4

A square with alternating charges cancels both center potential and field

Four fixed charges occupy square vertices (±a,±a)(\pm a,\pm a). Charges +Q are at (a,a) and (-a,-a); charges -Q occupy the other two vertices. Use infinity reference.

Diagram shown in the original SVG worksheet.

  1. Find V and the electric field at the center.

  2. Find V on the entire z axis and explain whether these cancellations imply that the field is zero everywhere.

Question 4 - Solution

A square with alternating charges cancels both center potential and field

Diagram shown in the original SVG worksheet.

(a) Method and calculation

ri=2a,V(0)=k2a(Q+Q−Q−Q)=0.r_i=\sqrt2a,\quad V(0)=\frac{k}{\sqrt2a}(Q+Q-Q-Q)=0.𝑬(0)=−k(2a)3∑iqi𝒓i=𝟎.\mathbf E(0)=-\frac{k}{(\sqrt2a)^3}\sum_i q_i\mathbf r_i=\mathbf0.

(b) Interpretation and further calculation

V(0,0,z)=k∑iqi2a2+z2=0.V(0,0,z)=\frac{k\sum_iq_i}{\sqrt{2a^2+z^2}}=0.V(x,y,0)≠0in general;V→±∞near the respective sources.V(x,y,0)\ne0\ \text{in general};\qquad V\to\pm\infty\ \text{near the respective sources}.

Physical check

Symmetry creates special cancellation sets, not an identically vanishing potential throughout space.