The Electric Field Due to an Electric Dipole β€” Question 9

Section 22-4 Β· Physics pages 3548–3549

Question 9 A neutral system has an origin-independent dipole moment For discrete charges define p = βˆ‘ i qiri. Shift the coordinate origin by vector b, so riβ€² = ri βˆ’b. x βˆ’q new origin positive charge Schematic; labels, not drawing lengths, specify the data. (a) Derive the transformation of the dipole moment and state the condition for invariance. (b) Apply it to βˆ’q at x = 0 and +q at x = d, then to βˆ’q at x = 0 and +2q at x = d, when the origin is shifted to x = d/2.
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Question 9 - Solution A neutral system has an origin-independent dipole moment x βˆ’q new origin positive charge (a) Method and calculation pβ€² = βˆ‘ i qi(ri βˆ’b) = p βˆ’b βˆ‘ i qi. pβ€² = p βˆ’Qtotalb, Qtotal = 0 β‡’pβ€² = p. (b) Interpretation and further calculation (βˆ’q, +q) : px = qd, pxβ€² = qd. (βˆ’q, +2q) : px = 2qd, pxβ€² = 2qd βˆ’q(d/2) = 3 2qd. A charged system still has a definable moment about a chosen origin, but it lacks the origin independence of a neutral dipole. Physical check The physical field does not depend on the coordinate origin; a complete expansion changes its other terms consistently.

Question 9

A neutral system has an origin-independent dipole moment

For discrete charges define 𝒑=βˆ‘iqi𝒓i\mathbf p=\sum_iq_i\mathbf r_i. Shift the coordinate origin by vector 𝒃\mathbf b, so 𝒓iβ€²=𝒓iβˆ’π’ƒ\mathbf r_i\prime=\mathbf r_i-\mathbf b.

Diagram shown in the original SVG worksheet.

  1. Derive the transformation of the dipole moment and state the condition for invariance.

  2. Apply it to βˆ’q-q at x=0x=0 and +q+q at x=dx=d, then to βˆ’q-q at x=0x=0 and +2q+2q at x=dx=d, when the origin is shifted to x=d/2x=d/2.

Question 9 - Solution

A neutral system has an origin-independent dipole moment

Diagram shown in the original SVG worksheet.

(a) Method and calculation

𝒑′=βˆ‘iqi(𝒓iβˆ’π’ƒ)=π’‘βˆ’π’ƒβˆ‘iqi.\mathbf p\prime=\sum_iq_i(\mathbf r_i-\mathbf b)=\mathbf p-\mathbf b\sum_iq_i.𝒑′=π’‘βˆ’Qtotal𝒃,Qtotal=0⇒𝒑′=𝒑.\mathbf p\prime=\mathbf p-Q_{\mathrm{total}}\mathbf b,\quad Q_{\mathrm{total}}=0\Rightarrow\mathbf p\prime=\mathbf p.

(b) Interpretation and further calculation

(βˆ’q,+q):px=qd,pxβ€²=qd.(-q,+q):\quad p_x=qd,\quad p_x\prime=qd.(βˆ’q,+2q):px=2qd,pxβ€²=2qdβˆ’q(d/2)=32qd.(-q,+2q):\quad p_x=2qd,\quad p_x\prime=2qd-q(d/2)=\tfrac32qd.A charged system still has a definable moment about a chosen origin, but it lacks the origin independence of a neutral dipole.

Physical check

The physical field does not depend on the coordinate origin; a complete expansion changes its other terms consistently.