Electric Potential Energy of a System of Point Charges — Question 9

Section 24-10 · Physics pages 3988–3989

Question 9 Splitting a fixed charge maximizes the pair interaction at equal shares Two point-charge sites a distance d apart carry nonnegative charges x and Q-x, with Q>0 fixed. Consider only their mutual interaction energy; exclude intrinsic self-energies and any charge-transfer apparatus. x Q −x d Schematic; labels, not drawing lengths, specify the data. (a) Find the value of x that maximizes the mutual energy and the values that minimize it. (b) Let x = Q/2 + δq. Find the exact energy change from equal sharing and explain why this calculation alone cannot predict charge sharing between conducting objects.
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Question 9 - Solution Splitting a fixed charge maximizes the pair interaction at equal shares x Q −x d (a) Method and calculation U(x) = k dx(Q −x) = kQ2 4d −k d(x −Q/2)2. Umax = kQ2/(4d) at x = Q/2; Umin = 0 at x = 0, Q. (b) Interpretation and further calculation ∆U = −k(δq)2 d ≤0. Uphysical = Umutual + Uself + Uapparatus. Terms excluded by this idealized problem can determine the actual equilibrium. Physical check Point-charge mutual energy is useful for separated particles but is not the complete charging energy of finite conductors.

Question 9

Splitting a fixed charge maximizes the pair interaction at equal shares

Two point-charge sites a distance d apart carry nonnegative charges x and Q-x, with Q>0 fixed. Consider only their mutual interaction energy; exclude intrinsic self-energies and any charge-transfer apparatus.

Diagram shown in the original SVG worksheet.

  1. Find the value of x that maximizes the mutual energy and the values that minimize it.

  2. Let x=Q/2+δqx=Q/2+\delta q. Find the exact energy change from equal sharing and explain why this calculation alone cannot predict charge sharing between conducting objects.

Question 9 - Solution

Splitting a fixed charge maximizes the pair interaction at equal shares

Diagram shown in the original SVG worksheet.

(a) Method and calculation

U(x)=kdx(Q−x)=kQ24d−kd(x−Q/2)2.U(x)=\frac{k}{d}x(Q-x)=\frac{kQ^2}{4d}-\frac{k}{d}(x-Q/2)^2.Umax=kQ2/(4d) at x=Q/2;Umin=0 at x=0,Q.U_{\max}=kQ^2/(4d)\text{ at }x=Q/2;\quad U_{\min}=0\text{ at }x=0,Q.

(b) Interpretation and further calculation

ΔU=−k(δq)2d≤0.\Delta U=-\frac{k(\delta q)^2}{d}\le0.Uphysical=Umutual+Uself+Uapparatus.U_{\mathrm{physical}}=U_{\mathrm{mutual}}+U_{\mathrm{self}}+U_{\mathrm{apparatus}}.Terms excluded by this idealized problem can determine the actual equilibrium.

Physical check

Point-charge mutual energy is useful for separated particles but is not the complete charging energy of finite conductors.