Potential of a Charged Isolated Conductor — Question 6

Section 24-11 · Physics pages 4002–4003

Question 6 A central cavity charge shifts an isolated shell potential through its outer charge A conducting spherical shell has inner radius a, outer radius b>a and net charge Q. A point charge q is held at its center. There are no external sources; take V(infinity)=0. q a b Schematic; labels, not drawing lengths, specify the data. (a) Find the charges on both conductor surfaces and the conductor potential. (b) Find the potential in the cavity for 0 < r < a, checking its boundary value.
Show solutionHide solution
Question 6 - Solution A central cavity charge shifts an isolated shell potential through its outer charge q a b (a) Method and calculation Qinner = −q, Qouter = Q + q. Vmetal = k(Q + q) b . (b) Interpretation and further calculation V (r) = kq r −kq a + k(Q + q) b (0 < r < a). V (a−) = k(Q + q) b = Vmetal, −dV dr = kq r2 . Physical check The cavity field depends on q, while the constant offset also depends on the outer surface charge and its radius.

Question 6

A central cavity charge shifts an isolated shell potential through its outer charge

A conducting spherical shell has inner radius a, outer radius b>a and net charge Q. A point charge q is held at its center. There are no external sources; take V(infinity)=0.

Diagram shown in the original SVG worksheet.

  1. Find the charges on both conductor surfaces and the conductor potential.

  2. Find the potential in the cavity for 0<r<a0<r<a, checking its boundary value.

Question 6 - Solution

A central cavity charge shifts an isolated shell potential through its outer charge

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Qinner=−q,Qouter=Q+q.Q_{\mathrm{inner}}=-q,\quad Q_{\mathrm{outer}}=Q+q.Vmetal=k(Q+q)b.V_{\mathrm{metal}}=\frac{k(Q+q)}b.

(b) Interpretation and further calculation

V(r)=kqr−kqa+k(Q+q)b(0<r<a).V(r)=\frac{kq}{r}-\frac{kq}{a}+\frac{k(Q+q)}b\quad(0<r<a).V(a−)=k(Q+q)b=Vmetal,−dVdr=kqr2.V(a^-)=\frac{k(Q+q)}b=V_{\mathrm{metal}},\quad-\frac{dV}{dr}=\frac{kq}{r^2}.

Physical check

The cavity field depends on q, while the constant offset also depends on the outer surface charge and its radius.