The Traveling Electromagnetic Wave, Qualitatively β€” Question 1

Section 33-2 Β· Physics pages 5392–5393

Question 1 A simultaneous field reversal preserves the direction of a traveling wave A vacuum plane wave travels along +x. At one event its electric field is E = βˆ’Eβˆ—Λ†y with positive E*. Use B = Λ†n Γ— E/c, where n is the propagation unit vector. +x Ey = βˆ’Eβˆ— Bz = βˆ’Eβˆ—/c into Schematic; labels, not drawing lengths, specify the data. (a) Find B and the direction of the cross product E cross B. (b) Compare reversing both fields with reversing only B. Which change preserves propagation along +x?
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Question 1 - Solution A simultaneous field reversal preserves the direction of a traveling wave +x Ey = βˆ’Eβˆ— Bz = βˆ’Eβˆ—/c into (a) Method and calculation B = Λ†x Γ— (βˆ’Eβˆ—Λ†y)/c = βˆ’(Eβˆ—/c)Λ†z . E Γ— B = (E2 βˆ—/c)Λ†x. (b) Interpretation and further calculation (βˆ’E) Γ— (βˆ’B) = E Γ— B β‡’same direction . E Γ— (βˆ’B) = βˆ’E Γ— B β‡’opposite direction . Physical check In a sinusoidal traveling wave both fields reverse every half-cycle; the energy-transport direction remains fixed.

Question 1

A simultaneous field reversal preserves the direction of a traveling wave

A vacuum plane wave travels along +x. At one event its electric field is 𝑬=βˆ’E*yΜ‚\mathbf E=-E_*\hat y with positive E*. Use 𝑩=n̂×𝑬/c\mathbf B=\hat n\times\mathbf E/c, where n is the propagation unit vector.

Diagram shown in the original SVG worksheet.

  1. Find B and the direction of the cross product E cross B.

  2. Compare reversing both fields with reversing only B. Which change preserves propagation along +x?

Question 1 - Solution

A simultaneous field reversal preserves the direction of a traveling wave

Diagram shown in the original SVG worksheet.

(a) Method and calculation

𝑩=xΜ‚Γ—(βˆ’E*yΜ‚)/c=βˆ’(E*/c)zΜ‚.\mathbf B=\hat x\times(-E_*\hat y)/c=\boxed{-(E_*/c)\hat z}.𝑬×𝑩=(E*2/c)xΜ‚.\mathbf E\times\mathbf B=(E_*^2/c)\hat x.

(b) Interpretation and further calculation

(βˆ’π‘¬)Γ—(βˆ’π‘©)=𝑬×𝑩⇒same direction.(-\mathbf E)\times(-\mathbf B)=\mathbf E\times\mathbf B\Rightarrow\boxed{\text{same direction}}.𝑬×(βˆ’π‘©)=βˆ’π‘¬Γ—π‘©β‡’opposite direction.\mathbf E\times(-\mathbf B)=-\mathbf E\times\mathbf B\Rightarrow\boxed{\text{opposite direction}}.

Physical check

In a sinusoidal traveling wave both fields reverse every half-cycle; the energy-transport direction remains fixed.