Proving the group velocity equation.

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SUMMARY

The group velocity equation, expressed as V_{g}=V_{p}-\lambda \frac{d V_{p}}{d\lambda}, is derived from the dispersion relation ω = ω(k) by expanding it in a Taylor series around the average wavelength λ. The relationship between group velocity (Vg) and phase velocity (Vp) is established by differentiating the Taylor series term by term. This derivation emphasizes that the group velocity is meaningful only under conditions of smooth dispersion, avoiding scenarios with anomalous or high dispersion.

PREREQUISITES
  • Understanding of wave mechanics and harmonic waves
  • Familiarity with Taylor series expansion
  • Knowledge of dispersion relations in physics
  • Concept of phase velocity and group velocity
NEXT STEPS
  • Study the derivation of the dispersion relation ω = ω(k) in various materials
  • Learn about the implications of anomalous dispersion on wave propagation
  • Explore applications of group velocity in optics and telecommunications
  • Investigate numerical methods for analyzing wave groups in complex media
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Students and professionals in physics, particularly those focusing on wave mechanics, optics, and telecommunications, will benefit from this discussion.

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Homework Statement



A wave group is generated as a superposition of harmonic waves of average wavelength lambda. Show that
V_{g}=V_{p}-\lambda \frac{d V_{p}}{d\lambda }

The Attempt at a Solution



All I know is that Vg = dw/dk and Vf = w/k. I am not sure what I need to do.
 
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Assume the dispersion relation ω = ω(k) has some well-behaved functional form, expand it in a Taylor series about the average wavelength, differentiate the Taylor series term by term, recognize ω/k as the phase velocity and keep only the first two terms. Note that because we are dropping higher-order terms, the group velocity only really has meaning when the dispersion relation of the material is fairly smooth, i.e. no anomalous dispersion or high dispersion.
 

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