Calculating the Capacitance — Question 2

Section 25-2 · Physics pages 4034–4035

Question 2 A spherical capacitor approaches the self-capacitance of one sphere Concentric conducting spheres have radii a and b>a and charges +Q and -Q. The gap is vacuum; k = 1/(4πϵ0). a b Schematic; labels, not drawing lengths, specify the data. (a) Derive their capacitance from the radial field. (b) Take b to infinity and then compare the exact capacitance with that of a narrow gap b=a+d.
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Question 2 - Solution A spherical capacitor approaches the self-capacitance of one sphere a b (a) Method and calculation Va −Vb = ∫b a Q 4πϵ0r2 dr = Q 4πϵ0 (1/a −1/b). C = 4πϵ0 ab b −a. (b) Interpretation and further calculation b →∞: C →4πϵ0a. b = a + d : C = 4πϵ0a2 d (1 + d/a), with planar leading term ϵ0(4πa2)/d for d much smaller than a. Physical check The isolated-sphere limit uses infinity as the second terminal; the small-gap limit uses the inner sphere area.

Question 2

A spherical capacitor approaches the self-capacitance of one sphere

Concentric conducting spheres have radii a and b>a and charges +Q and -Q. The gap is vacuum; k=1/(4πϵ0)k=1/(4\pi\epsilon_0).

Diagram shown in the original SVG worksheet.

  1. Derive their capacitance from the radial field.

  2. Take b to infinity and then compare the exact capacitance with that of a narrow gap b=a+d.

Question 2 - Solution

A spherical capacitor approaches the self-capacitance of one sphere

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Va−Vb=∫abQ4πϵ0r2dr=Q4πϵ0(1/a−1/b).V_a-V_b=\int_a^b\frac{Q}{4\pi\epsilon_0r^2}dr=\frac{Q}{4\pi\epsilon_0}(1/a-1/b).C=4πϵ0abb−a.C=4\pi\epsilon_0\frac{ab}{b-a}.

(b) Interpretation and further calculation

b→∞:C→4πϵ0a.b\to\infty:\ C\to4\pi\epsilon_0a.b=a+d:C=4πϵ0a2d(1+d/a),b=a+d:\ C=\frac{4\pi\epsilon_0a^2}{d}(1+d/a),with planar leading term ϵ0(4πa2)/d\epsilon_0(4\pi a^2)/d for d much smaller than a.

Physical check

The isolated-sphere limit uses infinity as the second terminal; the small-gap limit uses the inner sphere area.