The Electric Field Due to a Point Charge — Question 8

Section 22-3 · Physics pages 3526–3527

Question 8 Two symmetry-point readings separate the sum and difference of source charges Unknown charges qL, qR are fixed at (−a, 0) and (a, 0). At the origin, Ex = kQ0/a2. At (0, a), the measured y component is kQ0/( √ 2a2), where Q0 > 0 is known. Other sources are absent. qL qR P Schematic; labels, not drawing lengths, specify the data. (a) Derive equations for the charge sum and difference. (b) Find both charges and predict the x component of the field at (0, a).
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Question 8 - Solution Two symmetry-point readings separate the sum and difference of source charges qL qR P (a) Method and calculation Ex(0) = k(qL −qR) a2 ⇒qL −qR = Q0. Ey(0, a) = k(qL + qR) 2 √ 2a2 ⇒qL + qR = 2Q0. (b) Interpretation and further calculation qL = 3 2Q0, qR = 1 2Q0. Ex(0, a) = k(qL −qR) 2 √ 2a2 = kQ0 2 √ 2a2 . Measurements on different symmetry locations isolate different linear combinations of the unknown charges. Physical check The x component at the elevated point need not vanish when the source charges differ.

Question 8

Two symmetry-point readings separate the sum and difference of source charges

Unknown charges qL,qRq_L,q_R are fixed at (−a,0)(-a,0) and (a,0)(a,0). At the origin, Ex=kQ0/a2E_x=kQ_0/a^2. At (0,a)(0,a), the measured y component is kQ0/(2a2)kQ_0/(\sqrt2a^2), where Q0>0Q_0>0 is known. Other sources are absent.

Diagram shown in the original SVG worksheet.

  1. Derive equations for the charge sum and difference.

  2. Find both charges and predict the x component of the field at (0,a)(0,a).

Question 8 - Solution

Two symmetry-point readings separate the sum and difference of source charges

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Ex(0)=k(qL−qR)a2⇒qL−qR=Q0.E_x(0)=\frac{k(q_L-q_R)}{a^2}\Rightarrow q_L-q_R=Q_0.Ey(0,a)=k(qL+qR)22a2⇒qL+qR=2Q0.E_y(0,a)=\frac{k(q_L+q_R)}{2\sqrt2a^2}\Rightarrow q_L+q_R=2Q_0.

(b) Interpretation and further calculation

qL=32Q0,qR=12Q0.q_L=\tfrac32Q_0,\quad q_R=\tfrac12Q_0.Ex(0,a)=k(qL−qR)22a2=kQ022a2.E_x(0,a)=\frac{k(q_L-q_R)}{2\sqrt2a^2}=\frac{kQ_0}{2\sqrt2a^2}.Measurements on different symmetry locations isolate different linear combinations of the unknown charges.

Physical check

The x component at the elevated point need not vanish when the source charges differ.