Gauss' Law and Coulomb's Law — Question 2

Section 23-4 · Physics pages 3694–3695

Question 2 A cone captures a solid-angle fraction of a point-source flux A point charge q is at the center of a sphere. Consider the outward spherical cap 0 ≤θ ≤α, where 0 ≤α ≤π. Use k = 1/(4πϵ0). α q Meridional section of a cone and sphere; the cone angle is measured from its axis. (a) Derive its solid angle and electric flux from Coulomb field. (b) Find the cone half-angle that captures one quarter of the total signed flux. State whether increasing the sphere radius changes this fraction.
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Question 2 - Solution A cone captures a solid-angle fraction of a point-source flux α q (a) Method and calculation dΩ= sin θ dθ dϕ, Ω= 2π ∫α 0 sin θ dθ = 2π(1 −cos α). Φcap = kqΩ= q 2ϵ0 (1 −cos α). (b) Interpretation and further calculation Φcap q/ϵ0 = 1 −cos α 2 = 1 4 ⇒α = 60◦. Er ∝R−2, Acap ∝R2 ⇒Φcap is independent of R. Physical check The radius cancellation is the geometric signature of the inverse-square field.

Question 2

A cone captures a solid-angle fraction of a point-source flux

A point charge q is at the center of a sphere. Consider the outward spherical cap 0≤θ≤α0\le\theta\le\alpha, where 0≤α≤π0\le\alpha\le\pi. Use k=1/(4πϵ0)k=1/(4\pi\epsilon_0).

Diagram shown in the original SVG worksheet.

  1. Derive its solid angle and electric flux from Coulomb field.

  2. Find the cone half-angle that captures one quarter of the total signed flux. State whether increasing the sphere radius changes this fraction.

Question 2 - Solution

A cone captures a solid-angle fraction of a point-source flux

Diagram shown in the original SVG worksheet.

(a) Method and calculation

dΩ=sin⁡θdθdϕ,Ω=2π∫0αsin⁡θdθ=2π(1−cos⁡α).d\Omega=\sin\theta\,d\theta\,d\phi,\quad\Omega=2\pi\int_0^\alpha\sin\theta\,d\theta=2\pi(1-\cos\alpha).Φcap=kqΩ=q2ϵ0(1−cos⁡α).\Phi_{\mathrm{cap}}=kq\Omega=\frac{q}{2\epsilon_0}(1-\cos\alpha).

(b) Interpretation and further calculation

Φcapq/ϵ0=1−cos⁡α2=14⇒α=60∘.\frac{\Phi_{\mathrm{cap}}}{q/\epsilon_0}=\frac{1-\cos\alpha}{2}=\tfrac14\Rightarrow\alpha=60^\circ.Er∝R−2,Acap∝R2⇒Φcap is independent of R.E_r\propto R^{-2},\quad A_{\mathrm{cap}}\propto R^2\Rightarrow\Phi_{\mathrm{cap}}\text{ is independent of }R.

Physical check

The radius cancellation is the geometric signature of the inverse-square field.