The Electric Field Due to a Charged Disk — Question 8

Section 22-6 · Physics pages 3586–3587

Question 8 Two equally charged disks have an axial field that changes sign through the midpoint Two disks of radius R at z = ±h both carry fixed uniform positive density σ. Observe only on their common axis between them. Let f(s) = 1 −s/ √ s2 + R2 for s > 0. +σ +σ z Schematic; labels, not drawing lengths, specify the data. (a) Write Ez(z) for |z| < h and find its derivative at the midpoint. (b) Give the leading field for |z| ≪h and the force direction on a positive test charge displaced slightly above the midpoint.
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Question 8 - Solution Two equally charged disks have an axial field that changes sign through the midpoint +σ +σ z (a) Method and calculation Ez(z) = 2πkσ[f(h + z) −f(h −z)], Ez(0) = 0. f′(s) = − R2 (s2 + R2)3/2 , Ez′(0) = − 4πkσR2 (h2 + R2)3/2 . (b) Interpretation and further calculation Ez(z) ≃− 4πkσR2 (h2 + R2)3/2 z. z > 0, q > 0 : Fz = qEz < 0. The nearer upper disk pushes more strongly downward, creating an axial restoring tendency. This alone says nothing about transverse stability. Physical check One-dimensional restoring behavior is insufficient to establish a freely stable electrostatic trap.

Question 8

Two equally charged disks have an axial field that changes sign through the midpoint

Two disks of radius R at z=±hz=\pm h both carry fixed uniform positive density σ\sigma. Observe only on their common axis between them. Let f(s)=1−s/s2+R2f(s)=1-s/\sqrt{s^2+R^2} for s>0s>0.

Diagram shown in the original SVG worksheet.

  1. Write Ez(z)E_z(z) for |z|<h|z|<h and find its derivative at the midpoint.

  2. Give the leading field for |z|≪h|z|\ll h and the force direction on a positive test charge displaced slightly above the midpoint.

Question 8 - Solution

Two equally charged disks have an axial field that changes sign through the midpoint

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Ez(z)=2πkσ[f(h+z)−f(h−z)],Ez(0)=0.E_z(z)=2\pi k\sigma[f(h+z)-f(h-z)],\quad E_z(0)=0.f′(s)=−R2(s2+R2)3/2,Ez′(0)=−4πkσR2(h2+R2)3/2.f\prime(s)=-\frac{R^2}{(s^2+R^2)^{3/2}},\quad E_z\prime(0)=-\frac{4\pi k\sigma R^2}{(h^2+R^2)^{3/2}}.

(b) Interpretation and further calculation

Ez(z)≃−4πkσR2(h2+R2)3/2z.E_z(z)\simeq-\frac{4\pi k\sigma R^2}{(h^2+R^2)^{3/2}}z.z>0,q>0:Fz=qEz<0.z>0,q>0:\quad F_z=qE_z<0.The nearer upper disk pushes more strongly downward, creating an axial restoring tendency. This alone says nothing about transverse stability.

Physical check

One-dimensional restoring behavior is insufficient to establish a freely stable electrostatic trap.