Potential of a Charged Isolated Conductor — Question 1

Section 24-11 · Physics pages 3992–3993

Question 1 A conductor interior retains the surface voltage despite having no field Use k = 8.99 × 109 N m2/C2. An isolated conducting sphere of radius .150 m carries charge +6.00 nC. It is in vacuum with no other sources, and V(infinity)=0. R Cross-section of concentric spherical surfaces; labels specify radii. (a) Find V(r) inside and outside, then evaluate at the center and at r=.450 m. (b) Find the exterior surface field and the field at the center; explain their relation to the potential profile.
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Question 1 - Solution A conductor interior retains the surface voltage despite having no field R (a) Method and calculation V (r) = { kQ/R r ≤R, kQ/r r ≥R. V (0) = 359.6 V, V (.450 m) = 119.867 V. (b) Interpretation and further calculation E(R+) = kQ/R2 = 2397.33 V/m, E(0) = 0. r < R : dV/dr = 0 ⇒Er = 0, although the constant interior voltage is nonzero. Physical check The sphere potential is continuous at the surface, while its normal derivative jumps because surface charge is present.

Question 1

A conductor interior retains the surface voltage despite having no field

Use k=8.99×109Nm2/C2k=8.99\times10^9\,\mathrm{N\,m^2/C^2}. An isolated conducting sphere of radius .150 m carries charge +6.00 nC. It is in vacuum with no other sources, and V(infinity)=0.

Diagram shown in the original SVG worksheet.

  1. Find V(r) inside and outside, then evaluate at the center and at r=.450 m.

  2. Find the exterior surface field and the field at the center; explain their relation to the potential profile.

Question 1 - Solution

A conductor interior retains the surface voltage despite having no field

Diagram shown in the original SVG worksheet.

(a) Method and calculation

V(r)={kQ/Rr≤R,kQ/rr≥R.V(r)=\begin{cases}kQ/R&r\le R,\\kQ/r&r\ge R.\end{cases}V(0)=359.6V,V(.450m)=119.867V.V(0)=359.6\,\mathrm V,\quad V(.450\,\mathrm m)=119.867\,\mathrm V.

(b) Interpretation and further calculation

E(R+)=kQ/R2=2397.33V/m,E(0)=0.E(R^+)=kQ/R^2=2397.33\,\mathrm{V/m},\quad E(0)=0.r<R:dV/dr=0⇒Er=0,r<R:\quad dV/dr=0\Rightarrow E_r=0,although the constant interior voltage is nonzero.

Physical check

The sphere potential is continuous at the surface, while its normal derivative jumps because surface charge is present.