Gauss' Law and Coulomb's Law — Question 5

Section 23-4 · Physics pages 3700–3701

Question 5 An exterior point source gives equal entering and leaving solid angles A positive point charge lies outside a smooth convex closed surface. A narrow bundle of rays from the source pierces the surface once entering and once leaving. Let the bundle subtend positive solid angle dΩat the source. Here k = 1/(4πϵ0). q Schematic; labels, not drawing lengths, specify the data. (a) Use dΦ = kq(ˆr · ˆn)dA/r2 to compare the two crossings. (b) Integrate over all intersecting rays to find total flux, and explain why the result does not imply zero field anywhere on the surface.
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Question 5 - Solution An exterior point source gives equal entering and leaving solid angles q (a) Method and calculation dΩ= |ˆr · ˆn|dA r2 . dΦin = −kq dΩ, dΦout = +kq dΩ. (b) Interpretation and further calculation dΦpair = 0 ⇒Φclosed = 0. |E| = kq/r2 > 0 at every finite nonsource point. The paired projected areas compensate for different distances, so inward and outward integrals cancel. Physical check Convexity makes the two-crossing picture simple; more complicated shapes require summing all signed crossings.

Question 5

An exterior point source gives equal entering and leaving solid angles

A positive point charge lies outside a smooth convex closed surface. A narrow bundle of rays from the source pierces the surface once entering and once leaving. Let the bundle subtend positive solid angle dΩd\Omega at the source. Here k=1/(4πϵ0)k=1/(4\pi\epsilon_0).

Diagram shown in the original SVG worksheet.

  1. Use dΦ=kq(𝒓̂⋅𝒏̂)dA/r2d\Phi=kq(\hat{\mathbf r}\cdot\hat{\mathbf n})dA/r^2 to compare the two crossings.

  2. Integrate over all intersecting rays to find total flux, and explain why the result does not imply zero field anywhere on the surface.

Question 5 - Solution

An exterior point source gives equal entering and leaving solid angles

Diagram shown in the original SVG worksheet.

(a) Method and calculation

dΩ=|𝒓̂⋅𝒏̂|dAr2.d\Omega=\frac{|\hat{\mathbf r}\cdot\hat{\mathbf n}|dA}{r^2}.dΦin=−kqdΩ,dΦout=+kqdΩ.d\Phi_{\mathrm{in}}=-kq\,d\Omega,\quad d\Phi_{\mathrm{out}}=+kq\,d\Omega.

(b) Interpretation and further calculation

dΦpair=0⇒Φclosed=0.d\Phi_{\mathrm{pair}}=0\Rightarrow\Phi_{\mathrm{closed}}=0.|𝑬|=kq/r2>0at every finite nonsource point.|\mathbf E|=kq/r^2>0\quad\text{at every finite nonsource point}.The paired projected areas compensate for different distances, so inward and outward integrals cancel.

Physical check

Convexity makes the two-crossing picture simple; more complicated shapes require summing all signed crossings.