The Traveling Electromagnetic Wave, Qualitatively — Question 3

Section 33-2 · Physics pages 5396–5397

Question 3 The sign inside the phase identifies the direction of motion Two scalar profiles are EA = E0 cos(kx −ωt) and EB = E0 cos(kx + ωt), with positive k and omega and omega/k=c. Both electric fields point along y. kx −ωt kx + ωt x Schematic; labels, not drawing lengths, specify the data. (a) Follow a constant phase to find each propagation velocity. (b) Find the corresponding signed magnetic fields and explain why using the same Bz sign for both profiles fails.
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Question 3 - Solution The sign inside the phase identifies the direction of motion kx −ωt kx + ωt x (a) Method and calculation kx −ωt = ϕ ⇒dx/dt = +ω/k = +c . kx + ωt = ϕ ⇒dx/dt = −ω/k = −c . (b) Interpretation and further calculation BAz = EA/c, BBz = −EB/c . ˆy × ˆz = ˆx, ˆy × (−ˆz) = −ˆx. Physical check The sign relation between B and E changes when the propagation direction changes, even if their electric polarization is identical.

Question 3

The sign inside the phase identifies the direction of motion

Two scalar profiles are EA=E0cos⁡(kx−ωt)E_A=E_0\cos(kx-\omega t) and EB=E0cos⁡(kx+ωt)E_B=E_0\cos(kx+\omega t), with positive k and omega and omega/k=c. Both electric fields point along y.

Diagram shown in the original SVG worksheet.

  1. Follow a constant phase to find each propagation velocity.

  2. Find the corresponding signed magnetic fields and explain why using the same Bz sign for both profiles fails.

Question 3 - Solution

The sign inside the phase identifies the direction of motion

Diagram shown in the original SVG worksheet.

(a) Method and calculation

kx−ωt=ϕ⇒dx/dt=+ω/k=+c.kx-\omega t=\phi\Rightarrow\boxed{dx/dt=+\omega/k=+c}.kx+ωt=ϕ⇒dx/dt=−ω/k=−c.kx+\omega t=\phi\Rightarrow\boxed{dx/dt=-\omega/k=-c}.

(b) Interpretation and further calculation

BAz=EA/c,BBz=−EB/c.\boxed{B_{Az}=E_A/c,\qquad B_{Bz}=-E_B/c}.ŷ×ẑ=x̂,ŷ×(−ẑ)=−x̂.\hat y\times\hat z=\hat x,\quad\hat y\times(-\hat z)=-\hat x.

Physical check

The sign relation between B and E changes when the propagation direction changes, even if their electric polarization is identical.