Potential of a Charged Isolated Conductor — Question 2

Section 24-11 · Physics pages 3994–3995

Question 2 Connected distant spheres share voltage in proportion to their radii Two conducting spheres of radii R and 2R are very far apart. Initially the smaller carries Q>0 and the larger is neutral. A thin wire connects them until electrostatic equilibrium. Neglect wire charge and mutual influence. R 2R Schematic; labels, not drawing lengths, specify the data. (a) Find the final charges and common potential relative to infinity. (b) Find the two surface field magnitudes and their ratio.
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Question 2 - Solution Connected distant spheres share voltage in proportion to their radii R 2R (a) Method and calculation Q1 + Q2 = Q, kQ1 R = kQ2 2R ⇒Q2 = 2Q1. Q1 = Q/3, Q2 = 2Q/3, Vf = kQ/(3R). (b) Interpretation and further calculation E1 = kQ 3R2 , E2 = k(2Q/3) (2R)2 = kQ 6R2 . E1/E2 = 2. Physical check Equal voltage does not mean equal charge or equal field; the distant-sphere approximation neglects the other sphere contribution at each surface.

Question 2

Connected distant spheres share voltage in proportion to their radii

Two conducting spheres of radii R and 2R are very far apart. Initially the smaller carries Q>0 and the larger is neutral. A thin wire connects them until electrostatic equilibrium. Neglect wire charge and mutual influence.

Diagram shown in the original SVG worksheet.

  1. Find the final charges and common potential relative to infinity.

  2. Find the two surface field magnitudes and their ratio.

Question 2 - Solution

Connected distant spheres share voltage in proportion to their radii

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Q1+Q2=Q,kQ1R=kQ22R⇒Q2=2Q1.Q_1+Q_2=Q,\quad\frac{kQ_1}{R}=\frac{kQ_2}{2R}\Rightarrow Q_2=2Q_1.Q1=Q/3,Q2=2Q/3,Vf=kQ/(3R).Q_1=Q/3,\quad Q_2=2Q/3,\quad V_f=kQ/(3R).

(b) Interpretation and further calculation

E1=kQ3R2,E2=k(2Q/3)(2R)2=kQ6R2.E_1=\frac{kQ}{3R^2},\quad E_2=\frac{k(2Q/3)}{(2R)^2}=\frac{kQ}{6R^2}.E1/E2=2.E_1/E_2=2.

Physical check

Equal voltage does not mean equal charge or equal field; the distant-sphere approximation neglects the other sphere contribution at each surface.