Potential Due to a Continuous Charge Distribution — Question 9

Section 24-8 · Physics pages 3948–3949

Question 9 A finite cylinder center potential combines ring and axial integration A solid cylinder of radius R and half-length L has uniform volume density ρ > 0. Its axis is z and its center is the origin. Use infinity reference. O 2L Schematic; labels, not drawing lengths, specify the data. (a) Write and evaluate the double integral for V at the center. (b) Find the thin-cylinder limit L much smaller than R and show agreement with a disk of surface density σ = 2Lρ.
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Question 9 - Solution A finite cylinder center potential combines ring and axial integration O 2L (a) Method and calculation V (0) = 2πkρ ∫L −L ∫R 0 s ds dz √ s2 + z2 = 4πkρ ∫L 0 ( √ R2 + z2 −z)dz. V (0) = 2πkρ [ L √ R2 + L2 + R2 arsinh(L/R) −L2] . (b) Interpretation and further calculation L ≪R : V (0) = 4πkρLR −2πkρL2 + O(kρL3/R). Vleading = 2πk(2Lρ)R = 2πkσR. Physical check The limit refers to a finite cylinder becoming thin; no infinity reference is claimed for an infinite cylinder.

Question 9

A finite cylinder center potential combines ring and axial integration

A solid cylinder of radius R and half-length L has uniform volume density ρ>0\rho>0. Its axis is z and its center is the origin. Use infinity reference.

Diagram shown in the original SVG worksheet.

  1. Write and evaluate the double integral for V at the center.

  2. Find the thin-cylinder limit L much smaller than R and show agreement with a disk of surface density σ=2Lρ\sigma=2L\rho.

Question 9 - Solution

A finite cylinder center potential combines ring and axial integration

Diagram shown in the original SVG worksheet.

(a) Method and calculation

V(0)=2πkρ∫−LL∫0Rsdsdzs2+z2=4πkρ∫0L(R2+z2−z)dz.V(0)=2\pi k\rho\int_{-L}^{L}\int_0^R\frac{s\,ds\,dz}{\sqrt{s^2+z^2}}=4\pi k\rho\int_0^L(\sqrt{R^2+z^2}-z)dz.V(0)=2πkρ[LR2+L2+R2arsinh(L/R)−L2].V(0)=2\pi k\rho\left[L\sqrt{R^2+L^2}+R^2\operatorname{arsinh}(L/R)-L^2\right].

(b) Interpretation and further calculation

L≪R:V(0)=4πkρLR−2πkρL2+O(kρL3/R).L\ll R:\quad V(0)=4\pi k\rho LR-2\pi k\rho L^2+O(k\rho L^3/R).Vleading=2πk(2Lρ)R=2πkσR.V_{\mathrm{leading}}=2\pi k(2L\rho)R=2\pi k\sigma R.

Physical check

The limit refers to a finite cylinder becoming thin; no infinity reference is claimed for an infinite cylinder.