Potential Due to a Group of Point Charges — Question 8

Section 24-6 · Physics pages 3906–3907

Question 8 A compensating center charge sets one point to zero potential without zeroing its field Two charges +Q are at (±a, 0). An adjustable charge Q0 is at the origin. At P=(0,a), require V=0 with the infinity reference. Q Q0 Q P Schematic; labels, not drawing lengths, specify the data. (a) Find Q0. (b) Find the electric field at P after compensation and determine its direction.
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Question 8 - Solution A compensating center charge sets one point to zero potential without zeroing its field Q Q0 Q P (a) Method and calculation VP = 2kQ √ 2a + kQ0 a = 0. Q0 = − √ 2Q. (b) Interpretation and further calculation Ey = 2 kQa (2a2)3/2 + kQ0 a2 = kQ a2 ( 1 √ 2 − √ 2 ) . EP = −kQ √ 2a2 ˆy, Ex = 0. Physical check Potential cancellation weights each charge by inverse distance, while the vector field has a different distance and directional weighting.

Question 8

A compensating center charge sets one point to zero potential without zeroing its field

Two charges +Q are at (±a,0)(\pm a,0). An adjustable charge Q0 is at the origin. At P=(0,a), require V=0 with the infinity reference.

Diagram shown in the original SVG worksheet.

  1. Find Q0.

  2. Find the electric field at P after compensation and determine its direction.

Question 8 - Solution

A compensating center charge sets one point to zero potential without zeroing its field

Diagram shown in the original SVG worksheet.

(a) Method and calculation

VP=2kQ2a+kQ0a=0.V_P=\frac{2kQ}{\sqrt2a}+\frac{kQ_0}{a}=0.Q0=−2Q.Q_0=-\sqrt2Q.

(b) Interpretation and further calculation

Ey=2kQa(2a2)3/2+kQ0a2=kQa2(12−2).E_y=2\frac{kQ a}{(2a^2)^{3/2}}+\frac{kQ_0}{a^2}=\frac{kQ}{a^2}\left(\frac1{\sqrt2}-\sqrt2\right).𝑬P=−kQ2a2𝒚̂,Ex=0.\mathbf E_P=-\frac{kQ}{\sqrt2a^2}\hat{\mathbf y},\quad E_x=0.

Physical check

Potential cancellation weights each charge by inverse distance, while the vector field has a different distance and directional weighting.