The Electric Field Due to a Point Charge — Question 5

Section 22-3 · Physics pages 3520–3521

Question 5 A weak uniform background shifts a point-charge field null Two equal positive charges Q are fixed at x = ±a. A weak uniform background field Ebˆx is added. Seek a null near x = 0, with |x| ≪a. Use (1 + u)−2 = 1 −2u + O(u2). x Q 0 Q Schematic; labels, not drawing lengths, specify the data. (a) Expand the source field to first order and find the shifted null. (b) Express a self-consistency condition on Eb, and determine the shift if Eb = .0400 kQ/a2.
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Question 5 - Solution A weak uniform background shifts a point-charge field null x Q 0 Q (a) Method and calculation Ex = kQ[(a + x)−2 −(a −x)−2] + Eb. Ex ≃−4kQ a3 x + Eb ⇒x∗≃Eba3 4kQ . (b) Interpretation and further calculation |x∗|/a = |Eb|a2 4kQ ≪1. Eb = .0400 kQ/a2 ⇒x∗/a ≃.0100. The null shifts right so the stronger leftward contribution of the right-hand charge cancels the positive background. Physical check This is a local expansion, not an assertion that the approximate root is exact for large backgrounds.

Question 5

A weak uniform background shifts a point-charge field null

Two equal positive charges Q are fixed at x=±ax=\pm a. A weak uniform background field Eb𝒙̂E_b\hat{\mathbf x} is added. Seek a null near x=0x=0, with |x|≪a|x|\ll a. Use (1+u)−2=1−2u+O(u2)(1+u)^{-2}=1-2u+O(u^2).

Diagram shown in the original SVG worksheet.

  1. Expand the source field to first order and find the shifted null.

  2. Express a self-consistency condition on EbE_b, and determine the shift if Eb=.0400kQ/a2E_b=.0400\,kQ/a^2.

Question 5 - Solution

A weak uniform background shifts a point-charge field null

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Ex=kQ[(a+x)−2−(a−x)−2]+Eb.E_x=kQ[(a+x)^{-2}-(a-x)^{-2}]+E_b.Ex≃−4kQa3x+Eb⇒x*≃Eba34kQ.E_x\simeq-\frac{4kQ}{a^3}x+E_b\Rightarrow x_*\simeq\frac{E_ba^3}{4kQ}.

(b) Interpretation and further calculation

|x*|/a=|Eb|a24kQ≪1.|x_*|/a=\frac{|E_b|a^2}{4kQ}\ll1.Eb=.0400kQ/a2⇒x*/a≃.0100.E_b=.0400\,kQ/a^2\Rightarrow x_*/a\simeq.0100.The null shifts right so the stronger leftward contribution of the right-hand charge cancels the positive background.

Physical check

This is a local expansion, not an assertion that the approximate root is exact for large backgrounds.