Potential Due to a Continuous Charge Distribution — Question 5

Section 24-8 · Physics pages 3940–3941

Question 5 A disk potential follows by summing concentric rings A thin disk of radius R has uniform positive surface density σ. Observe on its axis at z>0. Use infinity reference. z R P Schematic; labels, not drawing lengths, specify the data. (a) Derive V(z) from rings of radius s. (b) Find V at the disk center and show that the large-z limit agrees with a point charge of total charge Q.
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Question 5 - Solution A disk potential follows by summing concentric rings z R P (a) Method and calculation dq = 2πσs ds, V (z) = 2πkσ ∫R 0 s ds √ s2 + z2 . V (z) = 2πkσ( √ R2 + z2 −z). (b) Interpretation and further calculation V (0) = 2πkσR. z ≫R : V ≃2πkσR2 2z = kQ z , Q = πR2σ. Physical check The integrable central ring contribution gives a finite disk-center potential despite the infinitesimal kernel singularity.

Question 5

A disk potential follows by summing concentric rings

A thin disk of radius R has uniform positive surface density σ\sigma. Observe on its axis at z>0. Use infinity reference.

Diagram shown in the original SVG worksheet.

  1. Derive V(z) from rings of radius s.

  2. Find V at the disk center and show that the large-z limit agrees with a point charge of total charge Q.

Question 5 - Solution

A disk potential follows by summing concentric rings

Diagram shown in the original SVG worksheet.

(a) Method and calculation

dq=2πσsds,V(z)=2πkσ∫0Rsdss2+z2.dq=2\pi\sigma s\,ds,\quad V(z)=2\pi k\sigma\int_0^R\frac{s\,ds}{\sqrt{s^2+z^2}}.V(z)=2πkσ(R2+z2−z).V(z)=2\pi k\sigma(\sqrt{R^2+z^2}-z).

(b) Interpretation and further calculation

V(0)=2πkσR.V(0)=2\pi k\sigma R.z≫R:V≃2πkσR22z=kQz,Q=πR2σ.z\gg R:\quad V\simeq2\pi k\sigma\frac{R^2}{2z}=\frac{kQ}{z},\quad Q=\pi R^2\sigma.

Physical check

The integrable central ring contribution gives a finite disk-center potential despite the infinitesimal kernel singularity.