Flux of an Electric Field — Question 10

Section 23-2 · Physics pages 3670–3671

Question 10 A growing aperture reconstructs a nonuniform normal field A family of rectangular apertures lies in z = 0, spanning 0 ≤x ≤a and 0 ≤y ≤W. The normal field depends only on x. Measurements give Φ(a) = Ca2 + Da3 for every 0 ≤a ≤L, with positive-z orientation. a L W Schematic; labels, not drawing lengths, specify the data. (a) Infer Ez(x) by differentiating the measured flux with respect to a. (b) Compare the field at the far edge of an aperture with its area-averaged field, and determine when they agree for a > 0.
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Question 10 - Solution A growing aperture reconstructs a nonuniform normal field a L W (a) Method and calculation Φ(a) = W ∫a 0 Ez(x) dx, dΦ da = WEz(a). Ez(x) = 2Cx + 3Dx2 W . (b) Interpretation and further calculation ⟨Ez⟩= Φ(a) Wa = Ca + Da2 W . Ez(a) −⟨Ez⟩= Ca + 2Da2 W = 0 ⇒C + 2Da = 0. For nonzero C and D, a positive solution exists only when their signs are opposite and a = −C/(2D) lies within L. Physical check The field reconstruction uses a continuous family of aperture measurements; a single integrated reading cannot determine an arbitrary profile.

Question 10

A growing aperture reconstructs a nonuniform normal field

A family of rectangular apertures lies in z=0z=0, spanning 0≤x≤a0\le x\le a and 0≤y≤W0\le y\le W. The normal field depends only on x. Measurements give Φ(a)=Ca2+Da3\Phi(a)=C a^2+D a^3 for every 0≤a≤L0\le a\le L, with positive-z orientation.

Diagram shown in the original SVG worksheet.

  1. Infer Ez(x)E_z(x) by differentiating the measured flux with respect to a.

  2. Compare the field at the far edge of an aperture with its area-averaged field, and determine when they agree for a>0a>0.

Question 10 - Solution

A growing aperture reconstructs a nonuniform normal field

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Φ(a)=W∫0aEz(x)dx,dΦda=WEz(a).\Phi(a)=W\int_0^aE_z(x)\,dx,\quad\frac{d\Phi}{da}=WE_z(a).Ez(x)=2Cx+3Dx2W.E_z(x)=\frac{2Cx+3Dx^2}{W}.

(b) Interpretation and further calculation

⟨Ez⟩=Φ(a)Wa=Ca+Da2W.\langle E_z\rangle=\frac{\Phi(a)}{Wa}=\frac{Ca+Da^2}{W}.Ez(a)−⟨Ez⟩=Ca+2Da2W=0⇒C+2Da=0.E_z(a)-\langle E_z\rangle=\frac{Ca+2Da^2}{W}=0\Rightarrow C+2Da=0.For nonzero C and D, a positive solution exists only when their signs are opposite and a=−C/(2D)a=-C/(2D) lies within L.

Physical check

The field reconstruction uses a continuous family of aperture measurements; a single integrated reading cannot determine an arbitrary profile.