Calculating the Capacitance — Question 3

Section 25-2 · Physics pages 4036–4037

Question 3 A coaxial capacitance depends logarithmically on its radius ratio Long coaxial conductors have radii a and b>a and overlap length L. The gap is vacuum. Neglect end effects and let the inner conductor charge per length be λ. a b Schematic; labels, not drawing lengths, specify the data. (a) Derive the capacitance per unit length. (b) Find its leading approximation for b=a+d with d much smaller than a and identify the effective plate area.
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Question 3 - Solution A coaxial capacitance depends logarithmically on its radius ratio a b (a) Method and calculation Er = λ/(2πϵ0r), V = ∫b a Erdr = λ 2πϵ0 ln(b/a). C/L = λ/V = 2πϵ0 ln(b/a). (b) Interpretation and further calculation ln(1 + d/a) ≃d/a ⇒C ≃2πϵ0aL d . Aeffective = 2πaL. Physical check The logarithm contains a dimensionless radius ratio; capacitance is proportional to length only while end effects remain negligible.

Question 3

A coaxial capacitance depends logarithmically on its radius ratio

Long coaxial conductors have radii a and b>a and overlap length L. The gap is vacuum. Neglect end effects and let the inner conductor charge per length be λ\lambda.

Diagram shown in the original SVG worksheet.

  1. Derive the capacitance per unit length.

  2. Find its leading approximation for b=a+d with d much smaller than a and identify the effective plate area.

Question 3 - Solution

A coaxial capacitance depends logarithmically on its radius ratio

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Er=λ/(2πϵ0r),V=∫abErdr=λ2πϵ0ln⁡(b/a).E_r=\lambda/(2\pi\epsilon_0r),\quad V=\int_a^bE_rdr=\frac{\lambda}{2\pi\epsilon_0}\ln(b/a).C/L=λ/V=2πϵ0ln⁡(b/a).C/L=\lambda/V=\frac{2\pi\epsilon_0}{\ln(b/a)}.

(b) Interpretation and further calculation

ln⁡(1+d/a)≃d/a⇒C≃2πϵ0aLd.\ln(1+d/a)\simeq d/a\Rightarrow C\simeq\frac{2\pi\epsilon_0aL}{d}.Aeffective=2πaL.A_{\mathrm{effective}}=2\pi aL.

Physical check

The logarithm contains a dimensionless radius ratio; capacitance is proportional to length only while end effects remain negligible.