The Electric Field Due to an Electric Dipole — Question 2

Section 22-4 · Physics pages 3534–3535

Question 2 On the perpendicular bisector the dipole field points opposite its moment The same finite dipole has −q at (−a, 0) and +q at (a, 0). Find its field at (0, y) with y > 0, defining p = 2qa. −q +q P Schematic; labels, not drawing lengths, specify the data. (a) Resolve and sum both source fields to obtain the exact vector. (b) Compare its far-field magnitude at y = r ≫a with the axial magnitude at the same center distance.
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Question 2 - Solution On the perpendicular bisector the dipole field points opposite its moment −q +q P (a) Method and calculation E+ = kq(−a, y) (a2 + y2)3/2 , E−= −kq(a, y) (a2 + y2)3/2 . Eeq = − kp (a2 + y2)3/2 ˆx. (b) Interpretation and further calculation r ≫a : |Eeq| ≃kp/r3, |Eaxial| ≃2kp/r3. |Eaxial|/|Eeq| ≃2. The vertical components cancel while both horizontal contributions point from the positive side toward the negative side. Physical check The field on the perpendicular bisector is not zero despite equal distances to the two charges.

Question 2

On the perpendicular bisector the dipole field points opposite its moment

The same finite dipole has −q-q at (−a,0)(-a,0) and +q+q at (a,0)(a,0). Find its field at (0,y)(0,y) with y>0y>0, defining p=2qap=2qa.

Diagram shown in the original SVG worksheet.

  1. Resolve and sum both source fields to obtain the exact vector.

  2. Compare its far-field magnitude at y=r≫ay=r\gg a with the axial magnitude at the same center distance.

Question 2 - Solution

On the perpendicular bisector the dipole field points opposite its moment

Diagram shown in the original SVG worksheet.

(a) Method and calculation

𝑬+=kq(−a,y)(a2+y2)3/2,𝑬−=−kq(a,y)(a2+y2)3/2.\mathbf E_+=\frac{kq(-a,y)}{(a^2+y^2)^{3/2}},\quad\mathbf E_-=\frac{-kq(a,y)}{(a^2+y^2)^{3/2}}.𝑬eq=−kp(a2+y2)3/2𝒙̂.\mathbf E_{\mathrm{eq}}=-\frac{kp}{(a^2+y^2)^{3/2}}\hat{\mathbf x}.

(b) Interpretation and further calculation

r≫a:|𝑬eq|≃kp/r3,|𝑬axial|≃2kp/r3.r\gg a:\quad|\mathbf E_{\mathrm{eq}}|\simeq kp/r^3,\quad|\mathbf E_{\mathrm{axial}}|\simeq2kp/r^3.|𝑬axial|/|𝑬eq|≃2.|\mathbf E_{\mathrm{axial}}|/|\mathbf E_{\mathrm{eq}}|\simeq2.The vertical components cancel while both horizontal contributions point from the positive side toward the negative side.

Physical check

The field on the perpendicular bisector is not zero despite equal distances to the two charges.