Difference between dispersive medium and non-dispersive medium.

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Dispersive media exhibit a phase velocity that varies with frequency, while non-dispersive media have a constant phase velocity regardless of frequency. The equation ω = √(4β/m)sin(Ka/2) describes wave behavior in a dispersive medium, which can be simplified to ω = νsK in the limit of low frequency (K→0), where νs represents phase velocity. This simplification indicates that ω = νsK is valid for both dispersive and non-dispersive media, but in non-dispersive media, νs remains constant. Understanding these distinctions is crucial for analyzing wave propagation in different media types.
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Hello experts!

I have 2 questions.

1)Difference between dispersive and non-dispersive medium.

2)ω=\sqrt{\frac{4β}{m}}sin\frac{Ka}{2} is a relation for dispersive medium. How to reduce it to non-dispersive relation? Here is some math work I have performed to reduce it to non-dispersive relation i.e.

At low frequency K→0
so,
sin(\frac{Ka}{2})→\frac{Ka}{2}
so the equation becomes,
ω=\frac{2}{a}νs\frac{Ka}{2}
or,
ω=νsK
where, νs is phase velocity.

So ω=νsK is the relation for non-dispersive medium? Is it?

Thanks in advance.
 
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shayaan_musta said:
Hello experts!

I have 2 questions.

1)Difference between dispersive and non-dispersive medium.

2)ω=\sqrt{\frac{4β}{m}}sin\frac{Ka}{2} is a relation for dispersive medium. How to reduce it to non-dispersive relation? Here is some math work I have performed to reduce it to non-dispersive relation i.e.

At low frequency K→0
so,
sin(\frac{Ka}{2})→\frac{Ka}{2}
so the equation becomes,
ω=\frac{2}{a}νs\frac{Ka}{2}
or,
ω=νsK
where, νs is phase velocity.

So ω=νsK is the relation for non-dispersive medium? Is it?

Thanks in advance.
Don't know what are β and m in your equations, however, for every frequency ω you can write that ω is equal to phase velocity multiplied wave vector modulus k, only that in a dispersive medium the phase velocity is not constant but depends on k (or ω, depending on which is your independent variable):

νs(k) = \frac{ω(k)}{k}

Group velocity (if of interest) is instead the derivative: νg(k) = \frac{dω(k)}{dk}.
 
Late reply.

But you are the only one up till now who replied me. So thanks for reply.

β is spring constant. It is come from the derivation of 1D mono-atomic.

m is the mass of the atoms.

You mean ω=vsk is not for the non-dispersive medium?
 
shayaan_musta said:
Late reply.

But you are the only one up till now who replied me. So thanks for reply.

β is spring constant. It is come from the derivation of 1D mono-atomic.

m is the mass of the atoms.

You mean ω=vsk is not for the non-dispersive medium?
ω=vsk is valid in both cases. If the medium is non-dispersive, vs is a constant, independent of k; if it's dispersive, vs depends on k.
 
Oh great
Thanks a lot.

Best answer.
Thanks.

And one thing I want to say you that kindly, visit this solid state portion at least once a week but try it every week. Because only you are here to answer the post. No one else.

Thanks once again.
 
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