The Traveling Electromagnetic Wave, Quantitatively — Question 10

Section 33-3 · Physics pages 5430–5431

Question 10 A harmonic waveform can translate rigidly without being sinusoidal A vacuum field is Ey = E0[sin ϕ + 1 2 sin 2ϕ], where ϕ = kx −ωt and omega=ck. Seek a single +x traveling waveform with no static field offset. x Ey Schematic; labels, not drawing lengths, specify the data. (a) Find Bz and show how the second harmonic frequency and wave number are related. (b) At phase zero find the time and spatial derivatives of Ey and use them to verify the transport equation.
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Question 10 - Solution A harmonic waveform can translate rigidly without being sinusoidal x Ey (a) Method and calculation Bz = E0 c [sin ϕ + 1 2 sin 2ϕ] . k2 = 2k, ω2 = 2ω ⇒ω2/k2 = c . (b) Interpretation and further calculation ∂xEy|ϕ=0 = kE0(1 + 1) = 2kE0, ∂tEy|ϕ=0 = −2ωE0. ∂tEy + c∂xEy = 0 at all phases. Physical check In nondispersive vacuum all harmonics share the same phase speed, so their sum preserves its shape.

Question 10

A harmonic waveform can translate rigidly without being sinusoidal

A vacuum field is Ey=E0[sin⁡ϕ+12sin⁡2ϕ]E_y=E_0[\sin\phi+\tfrac12\sin2\phi], where ϕ=kx−ωt\phi=kx-\omega t and omega=ck. Seek a single +x traveling waveform with no static field offset.

Diagram shown in the original SVG worksheet.

  1. Find Bz and show how the second harmonic frequency and wave number are related.

  2. At phase zero find the time and spatial derivatives of Ey and use them to verify the transport equation.

Question 10 - Solution

A harmonic waveform can translate rigidly without being sinusoidal

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Bz=E0c[sin⁡ϕ+12sin⁡2ϕ].\boxed{B_z=\frac{E_0}{c}[\sin\phi+\tfrac12\sin2\phi]}.k2=2k,ω2=2ω⇒ω2/k2=c.k_2=2k,\quad\omega_2=2\omega\Rightarrow\boxed{\omega_2/k_2=c}.

(b) Interpretation and further calculation

∂xEy|ϕ=0=kE0(1+1)=2kE0,∂tEy|ϕ=0=−2ωE0.\left.\partial_xE_y\right|_{\phi=0}=kE_0(1+1)=2kE_0,\quad\left.\partial_tE_y\right|_{\phi=0}=-2\omega E_0.∂tEy+c∂xEy=0at all phases.\boxed{\partial_tE_y+c\partial_xE_y=0}\quad\text{at all phases}.

Physical check

In nondispersive vacuum all harmonics share the same phase speed, so their sum preserves its shape.