Maxwell's Equations — Question 7

Section 32-4 · Physics pages 5244–5245

Question 7 A vacuum standing wave separates electric and magnetic antinodes A source-free standing electric field is E = E0 cos kx cos ωt ˆy with ω = ck. Seek Bz with no static offset. x spatial factors solid E profile; dashed B profile Schematic; labels, not drawing lengths, specify the data. (a) Find Bz from Faraday law and verify its amplitude. (b) Locate electric and magnetic spatial nodes and compare the peak energy densities.
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Question 7 - Solution A vacuum standing wave separates electric and magnetic antinodes x spatial factors solid E profile; dashed B profile (a) Method and calculation ∂tBz = −∂xEy = kE0 sin kx cos ωt. Bz = (E0/c) sin kx sin ωt . (b) Interpretation and further calculation E nodes : kx = (n + 1/2)π; B nodes : kx = nπ. uE,max = ϵ0E2 0/2 = uB,max . Physical check Equal peak energy scales do not mean equal electric and magnetic energy at every place and time.

Question 7

A vacuum standing wave separates electric and magnetic antinodes

A source-free standing electric field is 𝑬=E0cos⁡kxcos⁡ωtŷ\mathbf E=E_0\cos kx\cos\omega t\,\hat y with ω=ck\omega=ck. Seek Bz with no static offset.

Diagram shown in the original SVG worksheet.

  1. Find Bz from Faraday law and verify its amplitude.

  2. Locate electric and magnetic spatial nodes and compare the peak energy densities.

Question 7 - Solution

A vacuum standing wave separates electric and magnetic antinodes

Diagram shown in the original SVG worksheet.

(a) Method and calculation

∂tBz=−∂xEy=kE0sin⁡kxcos⁡ωt.\partial_tB_z=-\partial_xE_y=kE_0\sin kx\cos\omega t.Bz=(E0/c)sin⁡kxsin⁡ωt.\boxed{B_z=(E_0/c)\sin kx\sin\omega t}.

(b) Interpretation and further calculation

E nodes:kx=(n+1/2)π;B nodes:kx=nπ.E\text{ nodes}:kx=(n+1/2)\pi;\quad B\text{ nodes}:kx=n\pi.uE,max=ϵ0E02/2=uB,max.\boxed{u_{E,\max}=\epsilon_0E_0^2/2=u_{B,\max}}.

Physical check

Equal peak energy scales do not mean equal electric and magnetic energy at every place and time.