The Electric Field Due to an Electric Dipole — Question 8

Section 22-4 · Physics pages 3546–3547

Question 8 Zero total dipole moment can leave a nonzero higher-order field Charges +q, −2q, +q lie at x = −a, 0, +a. Use Coulomb constant k and observe at x > a. x +q −2q +q Schematic; labels, not drawing lengths, specify the data. (a) Find net charge and dipole moment about the origin, then derive the exact axial field. (b) Using (1 ± u)−2 = 1 ∓2u + 3u2 + O(u3), find the leading far-field term and explain why zero dipole moment does not mean zero field.
Show solutionHide solution
Question 8 - Solution Zero total dipole moment can leave a nonzero higher-order field x +q −2q +q (a) Method and calculation Qtotal = q −2q + q = 0, px = q(−a) + q(a) = 0. Ex = kq[(x + a)−2 −2x−2 + (x −a)−2]. (b) Interpretation and further calculation x ≫a : Ex = kq x2 [6(a/x)2 + O((a/x)4)]. Ex ≃6kqa2/x4. The charge and dipole terms cancel, exposing a faster-decaying spatial moment of the distribution. Physical check Vanishing leading moments constrain distant behavior; they do not eliminate all local fields.

Question 8

Zero total dipole moment can leave a nonzero higher-order field

Charges +q,−2q,+q+q,-2q,+q lie at x=−a,0,+ax=-a,0,+a. Use Coulomb constant k and observe at x>ax>a.

Diagram shown in the original SVG worksheet.

  1. Find net charge and dipole moment about the origin, then derive the exact axial field.

  2. Using (1±u)−2=1∓2u+3u2+O(u3)(1\pm u)^{-2}=1\mp2u+3u^2+O(u^3), find the leading far-field term and explain why zero dipole moment does not mean zero field.

Question 8 - Solution

Zero total dipole moment can leave a nonzero higher-order field

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Qtotal=q−2q+q=0,px=q(−a)+q(a)=0.Q_{\mathrm{total}}=q-2q+q=0,\quad p_x=q(-a)+q(a)=0.Ex=kq[(x+a)−2−2x−2+(x−a)−2].E_x=kq[(x+a)^{-2}-2x^{-2}+(x-a)^{-2}].

(b) Interpretation and further calculation

x≫a:Ex=kqx2[6(a/x)2+O((a/x)4)].x\gg a:\quad E_x=\frac{kq}{x^2}[6(a/x)^2+O((a/x)^4)].Ex≃6kqa2/x4.E_x\simeq6kqa^2/x^4.The charge and dipole terms cancel, exposing a faster-decaying spatial moment of the distribution.

Physical check

Vanishing leading moments constrain distant behavior; they do not eliminate all local fields.