Electric Potential Energy of a System of Point Charges — Question 10

Section 24-10 · Physics pages 3990–3991

Question 10 Changing one source charge alters only its incident pair energies Four fixed charges +q occupy square vertices A,B,C,D of side a. An external process changes the charge at A continuously from +q to -q, leaving all positions and other charges fixed. Track only mutual interaction energy. A B C D a Schematic; labels, not drawing lengths, specify the data. (a) Find the change in mutual energy using the potential at A from the other three sources. (b) Find the final total mutual energy and verify it by direct pair counting.
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Question 10 - Solution Changing one source charge alters only its incident pair energies A B C D a (a) Method and calculation Vothers(A) = kq a ( 2 + 1 √ 2 ) . ∆U = ∫−q q Vothers dqA = −2kq2 a ( 2 + 1 √ 2 ) . (b) Interpretation and further calculation Uf = kq2 a (4 + √ 2) −kq2 a (4 + √ 2) = 0. Usides = (−1 −1 + 1 + 1)kq2 a = 0, Udiagonals = (−1 + 1) kq2 √ 2a = 0. Physical check The result is a change of mutual electrostatic energy, not a claim about the total work or chemical energy of the charge-transfer mechanism.

Question 10

Changing one source charge alters only its incident pair energies

Four fixed charges +q occupy square vertices A,B,C,D of side a. An external process changes the charge at A continuously from +q to -q, leaving all positions and other charges fixed. Track only mutual interaction energy.

Diagram shown in the original SVG worksheet.

  1. Find the change in mutual energy using the potential at A from the other three sources.

  2. Find the final total mutual energy and verify it by direct pair counting.

Question 10 - Solution

Changing one source charge alters only its incident pair energies

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Vothers(A)=kqa(2+12).V_{\mathrm{others}}(A)=\frac{kq}{a}\left(2+\frac1{\sqrt2}\right).ΔU=∫q−qVothersdqA=−2kq2a(2+12).\Delta U=\int_q^{-q}V_{\mathrm{others}}\,dq_A=-\frac{2kq^2}{a}\left(2+\frac1{\sqrt2}\right).

(b) Interpretation and further calculation

Uf=kq2a(4+2)−kq2a(4+2)=0.U_f=\frac{kq^2}{a}(4+\sqrt2)-\frac{kq^2}{a}(4+\sqrt2)=0.Usides=(−1−1+1+1)kq2a=0,Udiagonals=(−1+1)kq22a=0.U_{\mathrm{sides}}=(-1-1+1+1)\frac{kq^2}{a}=0,\quad U_{\mathrm{diagonals}}=(-1+1)\frac{kq^2}{\sqrt2a}=0.

Physical check

The result is a change of mutual electrostatic energy, not a claim about the total work or chemical energy of the charge-transfer mechanism.