Calculating the Field from the Potential — Question 3

Section 24-9 · Physics pages 3956–3957

Question 3 Cylindrical angular variation requires the inverse-radius gradient factor In cylindrical coordinates for s>0, V (s, ϕ, z) = A ln(s/a) + B cos ϕ. Use ∇V = ˆs∂sV + ˆϕs−1∂ϕV + ˆz∂zV . s ϕ Schematic; labels, not drawing lengths, specify the data. (a) Find the field components. (b) Find the circulation along a full circle of radius s and the voltage difference along a semicircle from angle 0 to π.
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Question 3 - Solution Cylindrical angular variation requires the inverse-radius gradient factor s ϕ (a) Method and calculation Es = −A/s, Eϕ = B sin ϕ/s, Ez = 0. E = −A s ˆs + B sin ϕ s ˆϕ. (b) Interpretation and further calculation I E · dl = Z 2π 0 B sin ϕ dϕ = 0. V (π) −V (0) = − Z π 0 B sin ϕ dϕ = −2B. Physical check The physical arc element is s dphi, which cancels the inverse-radius factor in the tangential field.

Question 3

Cylindrical angular variation requires the inverse-radius gradient factor

In cylindrical coordinates for s>0, V(s,ϕ,z)=Aln⁡(s/a)+Bcos⁡ϕV(s,\phi,z)=A\ln(s/a)+B\cos\phi. Use ∇V=𝒔̂∂sV+𝝓̂s−1∂ϕV+𝒛̂∂zV\nabla V=\hat{\mathbf s}\partial_sV+\hat{\boldsymbol\phi}s^{-1}\partial_\phi V+\hat{\mathbf z}\partial_zV.

Diagram shown in the original SVG worksheet.

  1. Find the field components.

  2. Find the circulation along a full circle of radius s and the voltage difference along a semicircle from angle 0 to π\pi.

Question 3 - Solution

Cylindrical angular variation requires the inverse-radius gradient factor

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Es=−A/s,Eϕ=Bsin⁡ϕ/s,Ez=0.E_s=-A/s,\quad E_\phi=B\sin\phi/s,\quad E_z=0.𝑬=−As𝒔̂+Bsin⁡ϕs𝝓̂.\mathbf E=-\frac A s\hat{\mathbf s}+\frac{B\sin\phi}s\hat{\boldsymbol\phi}.

(b) Interpretation and further calculation

∮𝑬⋅d𝒍=∫02πBsin⁡ϕdϕ=0.\oint\mathbf E\cdot d\mathbf l=\int_0^{2\pi}B\sin\phi\,d\phi=0.V(π)−V(0)=−∫0πBsin⁡ϕdϕ=−2B.V(\pi)-V(0)=-\int_0^\pi B\sin\phi\,d\phi=-2B.

Physical check

The physical arc element is s dphi, which cancels the inverse-radius factor in the tangential field.