The Traveling Electromagnetic Wave, Qualitatively — Question 2

Section 33-2 · Physics pages 5394–5395

Question 2 Electric and magnetic zeros coincide in one vacuum traveling wave At a fixed point in a +x vacuum plane wave, Ey(t) = E0 sin ωt, with positive E0 and omega. There are no other waves or static fields. t normalized fields Ey/E0 = cBz/E0 Schematic; labels, not drawing lengths, specify the data. (a) Find Bz(t) and the first positive time when both fields reach their positive maxima. (b) Find both fields at t=pi/omega and determine the sign of E cross B immediately before and immediately after that time.
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Question 2 - Solution Electric and magnetic zeros coincide in one vacuum traveling wave t normalized fields Ey/E0 = cBz/E0 (a) Method and calculation Bz(t) = Ey(t)/c = (E0/c) sin ωt . tmax = π/(2ω) . (b) Interpretation and further calculation t = π/ω ⇒Ey = Bz = 0 . E × B = E2 0 c sin2 ωt ˆx ⇒+ˆx on both sides . Physical check The fields are in phase at a point; a time delay between their maxima would contradict this single traveling-wave model.

Question 2

Electric and magnetic zeros coincide in one vacuum traveling wave

At a fixed point in a +x vacuum plane wave, Ey(t)=E0sin⁡ωtE_y(t)=E_0\sin\omega t, with positive E0 and omega. There are no other waves or static fields.

Diagram shown in the original SVG worksheet.

  1. Find Bz(t) and the first positive time when both fields reach their positive maxima.

  2. Find both fields at t=pi/omega and determine the sign of E cross B immediately before and immediately after that time.

Question 2 - Solution

Electric and magnetic zeros coincide in one vacuum traveling wave

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Bz(t)=Ey(t)/c=(E0/c)sin⁡ωt.\boxed{B_z(t)=E_y(t)/c=(E_0/c)\sin\omega t}.tmax=π/(2ω).\boxed{t_{\max}=\pi/(2\omega)}.

(b) Interpretation and further calculation

t=π/ω⇒Ey=Bz=0.t=\pi/\omega\Rightarrow\boxed{E_y=B_z=0}.𝑬×𝑩=E02csin⁡2ωtx̂⇒+x̂ on both sides.\mathbf E\times\mathbf B=\frac{E_0^2}{c}\sin^2\omega t\,\hat x\Rightarrow\boxed{+\hat x\text{ on both sides}}.

Physical check

The fields are in phase at a point; a time delay between their maxima would contradict this single traveling-wave model.