Equipotential Surfaces — Question 4

Section 24-3 · Physics pages 3838–3839

Question 4 Two branches of the same equipotential may meet at a critical point A local potential is V (x, y) = A(x2 −y2) with A > 0, independent of z. A sketch shows two V=0 lines crossing at the origin. x y Schematic; labels, not drawing lengths, specify the data. (a) Find both zero-potential branches and the field at their intersection. (b) Find the field at (a,a) and explain why this crossing does not allow two different voltage values at one point.
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Question 4 - Solution Two branches of the same equipotential may meet at a critical point x y (a) Method and calculation V = 0 ⇒y = x or y = −x. E = −2Axˆx + 2Ayˆy, E(0, 0) = 0. (b) Interpretation and further calculation E(a, a) = 2Aa(−ˆx + ˆy), E · (ˆx + ˆy) = 0. V (0, 0) = 0 on both branches. Different-valued level surfaces cannot intersect; equal-valued branches can meet where the gradient vanishes. Physical check At a critical point the zero field has no unique direction, so the usual nonzero normal-vector construction does not apply.

Question 4

Two branches of the same equipotential may meet at a critical point

A local potential is V(x,y)=A(x2−y2)V(x,y)=A(x^2-y^2) with A>0A>0, independent of z. A sketch shows two V=0 lines crossing at the origin.

Diagram shown in the original SVG worksheet.

  1. Find both zero-potential branches and the field at their intersection.

  2. Find the field at (a,a) and explain why this crossing does not allow two different voltage values at one point.

Question 4 - Solution

Two branches of the same equipotential may meet at a critical point

Diagram shown in the original SVG worksheet.

(a) Method and calculation

V=0⇒y=xory=−x.V=0\Rightarrow y=x\ \text{or}\ y=-x.𝑬=−2Ax𝒙̂+2Ay𝒚̂,𝑬(0,0)=𝟎.\mathbf E=-2Ax\hat{\mathbf x}+2Ay\hat{\mathbf y},\quad\mathbf E(0,0)=\mathbf0.

(b) Interpretation and further calculation

𝑬(a,a)=2Aa(−𝒙̂+𝒚̂),𝑬⋅(𝒙̂+𝒚̂)=0.\mathbf E(a,a)=2Aa(-\hat{\mathbf x}+\hat{\mathbf y}),\quad\mathbf E\cdot(\hat{\mathbf x}+\hat{\mathbf y})=0.V(0,0)=0on both branches.V(0,0)=0\quad\text{on both branches}.Different-valued level surfaces cannot intersect; equal-valued branches can meet where the gradient vanishes.

Physical check

At a critical point the zero field has no unique direction, so the usual nonzero normal-vector construction does not apply.