The Traveling Electromagnetic Wave, Quantitatively — Question 7

Section 33-3 · Physics pages 5424–5425

Question 7 A supplied dispersion law separates phase speed from packet speed In an ideal transparent dispersive medium, a transverse mode obeys ω2 = ω2 p + c2k2 for positive k. Define phase speed as omega/k and the narrow-packet group speed as dω/dk. k ω ωp Schematic; labels, not drawing lengths, specify the data. (a) Derive both speeds and their product. (b) At ω = 2ωp find both speeds in units of c. Explain why a phase speed above c does not by itself establish faster-than-c information transport.
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Question 7 - Solution A supplied dispersion law separates phase speed from packet speed k ω ωp (a) Method and calculation k = √ ω2 −ω2p c ⇒vϕ = c √ 1 −ω2p/ω2 . vg = c2k ω = c √ 1 −ω2p/ω2, vϕvg = c2 . (b) Interpretation and further calculation ω = 2ωp ⇒vϕ = 2c/ √ 3, vg = √ 3c/2 . vϕ > c describes phase crests; vg < c for this packet model . Physical check A narrow-packet group speed is defined here; determining a signal front requires the full causal response of the medium.

Question 7

A supplied dispersion law separates phase speed from packet speed

In an ideal transparent dispersive medium, a transverse mode obeys ω2=ωp2+c2k2\omega^2=\omega_p^2+c^2k^2 for positive k. Define phase speed as omega/k and the narrow-packet group speed as dω/dkd\omega/dk.

Diagram shown in the original SVG worksheet.

  1. Derive both speeds and their product.

  2. At ω=2ωp\omega=2\omega_p find both speeds in units of c. Explain why a phase speed above c does not by itself establish faster-than-c information transport.

Question 7 - Solution

A supplied dispersion law separates phase speed from packet speed

Diagram shown in the original SVG worksheet.

(a) Method and calculation

k=ω2−ωp2c⇒vϕ=c1−ωp2/ω2.k=\frac{\sqrt{\omega^2-\omega_p^2}}{c}\Rightarrow\boxed{v_\phi=\frac{c}{\sqrt{1-\omega_p^2/\omega^2}}}.vg=c2kω=c1−ωp2/ω2,vϕvg=c2.\boxed{v_g=\frac{c^2k}{\omega}=c\sqrt{1-\omega_p^2/\omega^2},\quad v_\phi v_g=c^2}.

(b) Interpretation and further calculation

ω=2ωp⇒vϕ=2c/3,vg=3c/2.\omega=2\omega_p\Rightarrow\boxed{v_\phi=2c/\sqrt3,\quad v_g=\sqrt3c/2}.vϕ>c describes phase crests;vg<c for this packet model.v_\phi>c\text{ describes phase crests};\quad\boxed{v_g<c\text{ for this packet model}}.

Physical check

A narrow-packet group speed is defined here; determining a signal front requires the full causal response of the medium.