Equipotential Surfaces — Question 10

Section 24-3 · Physics pages 3850–3851

Question 10 Normal spacing changes along one parabolic equipotential family A two-dimensional potential is V = A(y −bx2), with A > 0 in V/m and b > 0 in inverse meters. Consider nearby levels separated by small |δV |. x Schematic; labels, not drawing lengths, specify the data. (a) Find their shapes and the local electric field. (b) Derive their normal spacing at x and its ratio to the spacing at x=0; evaluate the ratio at x = 1/(2b).
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Question 10 - Solution Normal spacing changes along one parabolic equipotential family x (a) Method and calculation V = Vc ⇒y = bx2 + Vc/A. E = 2Abxˆx −Aˆy, |E| = A √ 1 + 4b2x2. (b) Interpretation and further calculation δn ≃ |δV | A √ 1 + 4b2x2 , δn(x) δn(0) = 1 √ 1 + 4b2x2 . x = 1/(2b) : δn(x)/δn(0) = 1/ √ 2. Physical check The vertical separation is constant, but the relevant distance for field strength is along the local normal.

Question 10

Normal spacing changes along one parabolic equipotential family

A two-dimensional potential is V=A(y−bx2)V=A(y-bx^2), with A>0A>0 in V/m and b>0b>0 in inverse meters. Consider nearby levels separated by small |δV||\delta V|.

Diagram shown in the original SVG worksheet.

  1. Find their shapes and the local electric field.

  2. Derive their normal spacing at x and its ratio to the spacing at x=0; evaluate the ratio at x=1/(2b)x=1/(2b).

Question 10 - Solution

Normal spacing changes along one parabolic equipotential family

Diagram shown in the original SVG worksheet.

(a) Method and calculation

V=Vc⇒y=bx2+Vc/A.V=V_c\Rightarrow y=bx^2+V_c/A.𝑬=2Abx𝒙̂−A𝒚̂,|𝑬|=A1+4b2x2.\mathbf E=2Abx\hat{\mathbf x}-A\hat{\mathbf y},\quad|\mathbf E|=A\sqrt{1+4b^2x^2}.

(b) Interpretation and further calculation

δn≃|δV|A1+4b2x2,δn(x)δn(0)=11+4b2x2.\delta n\simeq\frac{|\delta V|}{A\sqrt{1+4b^2x^2}},\quad\frac{\delta n(x)}{\delta n(0)}=\frac1{\sqrt{1+4b^2x^2}}.x=1/(2b):δn(x)/δn(0)=1/2.x=1/(2b):\quad\delta n(x)/\delta n(0)=1/\sqrt2.

Physical check

The vertical separation is constant, but the relevant distance for field strength is along the local normal.