The Traveling Electromagnetic Wave, Qualitatively — Question 7

Section 33-2 · Physics pages 5404–5405

Question 7 Counterpropagating waves can cancel E while reinforcing B at an event Two vacuum plane waves meet. At the chosen event wave 1 travels +x with electric field E∗ˆy, while wave 2 travels -x with electric field −E∗ˆy. wave 1 wave 2 overlap event Schematic; labels, not drawing lengths, specify the data. (a) Find each magnetic field and the total E and B. (b) Evaluate the total E cross B and explain why the total fields need not obey the single-wave relation E=cB.
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Question 7 - Solution Counterpropagating waves can cancel E while reinforcing B at an event wave 1 wave 2 overlap event (a) Method and calculation B1 = ˆx × E∗ˆy/c = (E∗/c)ˆz, B2 = (−ˆx) × (−E∗ˆy)/c = (E∗/c)ˆz. Etot = 0, Btot = (2E∗/c)ˆz . (b) Interpretation and further calculation Etot × Btot = 0 . |Etot| = 0̸ = c|Btot| = 2|E∗|. Physical check The total is a superposition traveling in two directions, so a pointwise identity valid for one traveling wave cannot be imposed on it.

Question 7

Counterpropagating waves can cancel E while reinforcing B at an event

Two vacuum plane waves meet. At the chosen event wave 1 travels +x with electric field E*ŷE_*\hat y, while wave 2 travels -x with electric field −E*ŷ-E_*\hat y.

Diagram shown in the original SVG worksheet.

  1. Find each magnetic field and the total E and B.

  2. Evaluate the total E cross B and explain why the total fields need not obey the single-wave relation E=cB.

Question 7 - Solution

Counterpropagating waves can cancel E while reinforcing B at an event

Diagram shown in the original SVG worksheet.

(a) Method and calculation

𝑩1=x̂×E*ŷ/c=(E*/c)ẑ,𝑩2=(−x̂)×(−E*ŷ)/c=(E*/c)ẑ.\mathbf B_1=\hat x\times E_*\hat y/c=(E_*/c)\hat z,\quad\mathbf B_2=(-\hat x)\times(-E_*\hat y)/c=(E_*/c)\hat z.𝑬tot=0,𝑩tot=(2E*/c)ẑ.\boxed{\mathbf E_{\mathrm{tot}}=0,\quad\mathbf B_{\mathrm{tot}}=(2E_*/c)\hat z}.

(b) Interpretation and further calculation

𝑬tot×𝑩tot=0.\boxed{\mathbf E_{\mathrm{tot}}\times\mathbf B_{\mathrm{tot}}=0}.|Etot|=0≠c|Btot|=2|E*|.|E_{\mathrm{tot}}|=0\ne c|B_{\mathrm{tot}}|=2|E_*|.

Physical check

The total is a superposition traveling in two directions, so a pointwise identity valid for one traveling wave cannot be imposed on it.