Potential of a Charged Isolated Conductor — Question 10

Section 24-11 · Physics pages 4010–4011

Question 10 A charged sphere in a uniform external field remains equipotential while its density varies A conducting sphere of radius R carries net charge Q in a uniform external field E0ˆz. Its exterior potential is supplied as V = −E0(r −R3/r2) cos θ + kQ/r. Here θ is measured from positive z and E0 > 0. z E0 E0 Schematic; labels, not drawing lengths, specify the data. (a) Find the surface potential and both exterior field components at r=R. (b) Find the surface charge density and the minimum Q for it to be nonnegative everywhere. Use σ = ϵ0Er(R+).
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Question 10 - Solution A charged sphere in a uniform external field remains equipotential while its density varies z E0 E0 (a) Method and calculation V (R, θ) = kQ/R, Eθ = −E0(1 −R3/r3) sin θ ⇒Eθ(R) = 0. Er = E0(1 + 2R3/r3) cos θ + kQ/r2 ⇒Er(R) = 3E0 cos θ + kQ/R2. (b) Interpretation and further calculation σ(θ) = ϵ0[3E0 cos θ + kQ/R2]. σmin = ϵ0[−3E0 + kQ/R2] ≥0 ⇒Q ≥3E0R2/k. Physical check The supplied external uniform field has no infinity-zero potential; the stated formula fixes its reference. Integrating the cosine surface term gives zero net induced charge.

Question 10

A charged sphere in a uniform external field remains equipotential while its density varies

A conducting sphere of radius R carries net charge Q in a uniform external field E0𝒛̂E_0\hat{\mathbf z}. Its exterior potential is supplied as V=−E0(r−R3/r2)cos⁡θ+kQ/rV=-E_0(r-R^3/r^2)\cos\theta+kQ/r. Here θ\theta is measured from positive z and E0>0E_0>0.

Diagram shown in the original SVG worksheet.

  1. Find the surface potential and both exterior field components at r=R.

  2. Find the surface charge density and the minimum Q for it to be nonnegative everywhere. Use σ=ϵ0Er(R+)\sigma=\epsilon_0 E_r(R^+).

Question 10 - Solution

A charged sphere in a uniform external field remains equipotential while its density varies

Diagram shown in the original SVG worksheet.

(a) Method and calculation

V(R,θ)=kQ/R,Eθ=−E0(1−R3/r3)sin⁡θ⇒Eθ(R)=0.V(R,\theta)=kQ/R,\quad E_\theta=-E_0(1-R^3/r^3)\sin\theta\Rightarrow E_\theta(R)=0.Er=E0(1+2R3/r3)cos⁡θ+kQ/r2⇒Er(R)=3E0cos⁡θ+kQ/R2.E_r=E_0(1+2R^3/r^3)\cos\theta+kQ/r^2\Rightarrow E_r(R)=3E_0\cos\theta+kQ/R^2.

(b) Interpretation and further calculation

σ(θ)=ϵ0[3E0cos⁡θ+kQ/R2].\sigma(\theta)=\epsilon_0[3E_0\cos\theta+kQ/R^2].σmin=ϵ0[−3E0+kQ/R2]≥0⇒Q≥3E0R2/k.\sigma_{\min}=\epsilon_0[-3E_0+kQ/R^2]\ge0\Rightarrow Q\ge3E_0R^2/k.

Physical check

The supplied external uniform field has no infinity-zero potential; the stated formula fixes its reference. Integrating the cosine surface term gives zero net induced charge.