Group Velocity of Non-Dispersive Wave Packet

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Homework Help Overview

The discussion revolves around calculating the group velocity of a non-dispersive wave packet, with references to both light and sound waves. Participants are exploring the definitions and relationships between group and phase velocities in different contexts.

Discussion Character

  • Conceptual clarification, Assumption checking, Exploratory

Approaches and Questions Raised

  • Participants discuss the definition of group velocity and its relationship to phase velocity, particularly in non-dispersive media. There is an attempt to clarify the conditions under which these velocities are equal and how to apply the definitions to specific examples, including light pulses and sound waves.

Discussion Status

The discussion is active, with participants questioning definitions and exploring the implications of non-dispersive wave packets. Some guidance has been offered regarding the differentiation of equations related to group velocity, but there is no explicit consensus on the approach to take.

Contextual Notes

Participants are navigating potential confusion regarding definitions and the application of equations in different contexts, such as light and sound waves. There is mention of a need for a functional form to illustrate the concepts discussed.

waley

Homework Statement


I know that for a dispersive wave packet, the group velocity equals the phase velocity, which is given by v=w/k. But how do I calculate the group velocity of a non-dispersive wave packet? I'm supposed to be giving an example with any functional form.

Homework Equations


group velocity is defined by (partial derivative of w(k))/(partial derivative of k)

The Attempt at a Solution


Since w is not dependent on k, the partial derivative should equal to zero? But I'm not sure how to go from there.
 
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Could you possibly mean a photon wavepacket, i.e. a light pulse? I think you got your definition reversed - nondispersive wavepacket has its group and phase velocities equal but the dispersive one has them different. A non-dispersive lightpulse is that propagating in a non-dispersive medium, a medium whose refractive index does not vary with frequency (or wavelength). In this case if you differentiate both sides of the equation ##k = \omega n(\omega)/c ## you will get the group velocity in terms of the refractive index (as a function of ## \omega##).
 
blue_leaf77 said:
Could you possibly mean a photon wavepacket, i.e. a light pulse? I think you got your definition reversed - nondispersive wavepacket has its group and phase velocities equal but the dispersive one has them different. A non-dispersive lightpulse is that propagating in a non-dispersive medium, a medium whose refractive index does not vary with frequency (or wavelength). In this case if you differentiate both sides of the equation ##k = \omega n(\omega)/c ## you will get the group velocity in terms of the refractive index (as a function of ## \omega##).
Ah, sorry I realized after that I indeed got my definitions reversed. And I also forgot to add that I'm asking in terms of sound waves - would your equation still hold?
How exactly would I differentiate both sides - Is the derivative of k supposed to be the group velocity, and my "functional form" would be something of n in terms of w that I differentiate with respect to w?
 
Actually, would it be sufficient enough if I say that for the non-dispersive relation, since the group velocity equals the phase velocity, I just solve the phase velocity with the equation v=w/k? So if I have a functional form of, let's say, cos(x), the phase and group velocity would just be cos(x)/k?
 

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