The Electric Field Due to an Electric Dipole — Question 7

Section 22-4 · Physics pages 3544–3545

Question 7 Equal field magnitudes around a dipole do not form a sphere In the far field of a dipole, |E| = (kp/r3) √ 1 + 3 cos2 θ. Consider the surface where the magnitude equals a specified E∗> 0. raxis req Schematic comparison of axial and equatorial radii; the contour is not an exact ellipse. (a) Derive its radius as a function of polar angle. (b) Find the axial-to-equatorial radius ratio and compare field direction at these two locations.
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Question 7 - Solution Equal field magnitudes around a dipole do not form a sphere raxis req (a) Method and calculation E∗r3 = kp √ 1 + 3 cos2 θ. r(θ) = ( kp E∗ )1/3 (1 + 3 cos2 θ)1/6. (b) Interpretation and further calculation raxis/req = 41/6 = 21/3 ≈1.25992. Eaxis ∥p, Eeq ∥−p. Equal magnitude does not require equal distance or equal direction. Physical check The entire contour must remain far from the finite source size for the point-dipole formula to apply.

Question 7

Equal field magnitudes around a dipole do not form a sphere

In the far field of a dipole, |𝑬|=(kp/r3)1+3cos⁡2θ|\mathbf E|=(kp/r^3)\sqrt{1+3\cos^2\theta}. Consider the surface where the magnitude equals a specified E*>0E_*>0.

Diagram shown in the original SVG worksheet.

  1. Derive its radius as a function of polar angle.

  2. Find the axial-to-equatorial radius ratio and compare field direction at these two locations.

Question 7 - Solution

Equal field magnitudes around a dipole do not form a sphere

Diagram shown in the original SVG worksheet.

(a) Method and calculation

E*r3=kp1+3cos⁡2θ.E_*r^3=kp\sqrt{1+3\cos^2\theta}.r(θ)=(kpE*)1/3(1+3cos⁡2θ)1/6.r(\theta)=\left(\frac{kp}{E_*}\right)^{1/3}(1+3\cos^2\theta)^{1/6}.

(b) Interpretation and further calculation

raxis/req=41/6=21/3≈1.25992.r_{\mathrm{axis}}/r_{\mathrm{eq}}=4^{1/6}=2^{1/3}\approx1.25992.𝑬axis∥𝒑,𝑬eq∥−𝒑.\mathbf E_{\mathrm{axis}}\parallel\mathbf p,\quad\mathbf E_{\mathrm{eq}}\parallel-\mathbf p.Equal magnitude does not require equal distance or equal direction.

Physical check

The entire contour must remain far from the finite source size for the point-dipole formula to apply.