Potential Due to a Group of Point Charges — Question 9

Section 24-6 · Physics pages 3908–3909

Question 9 An antisymmetric pair makes the perpendicular bisector a zero-work track Charges +Q at x=a and -Q at x=-a have Q,a>0. A probe q follows the y axis from y=b to y=c, constrained by an ideal guide. −Q +Q y q Schematic; labels, not drawing lengths, specify the data. (a) Find V(y) and the electric work along the guide. (b) Find the electric field along the y axis and the transverse guide force needed to keep the probe on it.
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Question 9 - Solution An antisymmetric pair makes the perpendicular bisector a zero-work track −Q +Q y q (a) Method and calculation V (0, y) = kQ √ a2 + y2 − kQ √ a2 + y2 = 0. We = q[V (0, b) −V (0, c)] = 0. (b) Interpretation and further calculation E(0, y) = − 2kQa (a2 + y2)3/2 ˆx. Fguide = + 2kQqa (a2 + y2)3/2 ˆx. Physical check The guide force is transverse to the allowed velocity and does no work, while cancelling a generally nonzero electric force.

Question 9

An antisymmetric pair makes the perpendicular bisector a zero-work track

Charges +Q at x=a and -Q at x=-a have Q,a>0. A probe q follows the y axis from y=b to y=c, constrained by an ideal guide.

Diagram shown in the original SVG worksheet.

  1. Find V(y) and the electric work along the guide.

  2. Find the electric field along the y axis and the transverse guide force needed to keep the probe on it.

Question 9 - Solution

An antisymmetric pair makes the perpendicular bisector a zero-work track

Diagram shown in the original SVG worksheet.

(a) Method and calculation

V(0,y)=kQa2+y2−kQa2+y2=0.V(0,y)=\frac{kQ}{\sqrt{a^2+y^2}}-\frac{kQ}{\sqrt{a^2+y^2}}=0.We=q[V(0,b)−V(0,c)]=0.W_e=q[V(0,b)-V(0,c)]=0.

(b) Interpretation and further calculation

𝑬(0,y)=−2kQa(a2+y2)3/2𝒙̂.\mathbf E(0,y)=-\frac{2kQa}{(a^2+y^2)^{3/2}}\hat{\mathbf x}.𝑭guide=+2kQqa(a2+y2)3/2𝒙̂.\mathbf F_{\mathrm{guide}}=+\frac{2kQqa}{(a^2+y^2)^{3/2}}\hat{\mathbf x}.

Physical check

The guide force is transverse to the allowed velocity and does no work, while cancelling a generally nonzero electric force.