Group velocity and phase velocity of a matter wave

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SUMMARY

The discussion centers on the derivation of the group velocity and phase velocity of a matter wave, specifically using the relation ω² = k²c² + m²c⁴/ħ². Participants clarify that the phase velocity is defined as vₚ = ω/k, while the group velocity is given by v₍g₎ = dω/dk. The correct differentiation leads to the conclusion that v₍g₎ = c²/v, contrasting with the initial confusion regarding the relationship between phase velocity and particle velocity. Ultimately, the correct expression for phase velocity is confirmed as vₚ = c²/v.

PREREQUISITES
  • Understanding of wave mechanics and wave equations
  • Familiarity with the concepts of group velocity and phase velocity
  • Knowledge of differentiation in calculus
  • Basic principles of quantum mechanics, particularly matter waves
NEXT STEPS
  • Study the derivation of the wave equation for matter waves in quantum mechanics
  • Learn about the implications of group and phase velocities in different wave types
  • Explore advanced differentiation techniques in calculus relevant to physics
  • Review the Wikipedia page on wave motion for additional context and examples
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Students of physics, particularly those studying quantum mechanics, as well as educators and anyone interested in the mathematical foundations of wave behavior in matter waves.

andrepd
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Hi. Today I sat my final first year Modern Physics exam. It went very well, however I got stuck in one question. It asked (i) to prove the following relation for the matter wave \omega^{2}=k^{2}c^{2}+m^{2}c^{4}/\hbar^{2} and (ii) to obtain the group velocity and phase velocity of a matter wave from that relation. (i) was easy, so was obtaining the group velocity, but I got stuck on obtaining c^2/v for the phase velocity. If someone could walk me thorough that deduction, I would appreciate it. Thanks.
 
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The phase velocity is v = ω/k. The group velocity is g = dω/dk. Differentiate the relationship you have, and you get 2 ω dω/dk = 2k c2, which immediately gives you vg = c2.
 
If I'm not mistaken, differentiating our expression for ω(k) yields vg=(k/ω)c^2, which, if we know beforehand that the phase velocity equals c^2/v, can express as vg=v. However, I'm unsure how we get from vf = ω/k = \sqrt{\frac{k^{2}c^{2}+m^{2}c^{4}/\hbar^{2}}{k^{2}}} to vf=c^2/v.
 
andrepd said:
If I'm not mistaken
You're mistaken.
 
Bill_K said:
You're mistaken.

Care to explain then? dω/dk=d/dk(\sqrt{k^{2}c^{2}+m^{2}c^{4}/\hbar^{2}})=1/2*(k^{2}c^{2}+m^{2}c^{4}/\hbar^{2})^{-1/2}*2kc^{2}=\frac{k}{\omega}c^{2}=\frac{v}{c^{2}}*c^2=v

This was my thought process. Care to point my mistake?

EDIT: This, however, presumes previous knowledge that vf=c^2/v. Hence my question.
 
andrepd said:
Care to explain then? =\frac{k}{\omega}c^{2}=\frac{v}{c^{2}}*c^2=v
This was my thought process. Care to point my mistake?.
In the last step you've used v = k/ω, whereas actually v = ω/k.

It's easier anyway to do it the way I showed. Do NOT take the square root. Simply differentiate the given relationship as it stands. The LHS is ω2, and its derivative is 2 ω dω/dk. The RHS is k2c2 + m2c42, and its derivative is 2 k c2. That gives what you want immediately.
 
This yields the the same result for the *group* velocity. However, I am having trouble with the derivation of the *phase* velocity, \omega/k, which, in the context of matter waves, is not equal to v, but rather to c^2/v.
 
The phase velocity is always ω/k, andrepd, I don't care what the context. It's the group velocity that may differ. This is a general fact for wave motion of any kind: sound waves, water waves, gravity waves, matter waves or what have you. The phase velocity is the velocity at which a wave crest travels, and the expression for it just comes from taking exp(i(kx - ωt)) and rewriting it as exp(ik(x - vt)), from which v = ω/k. If you're still not clear, I suggest you read the Wikipedia page.
 
I know that, however, that is now what I was looking for. I know that the phase velocity equals ω/k. Again, I wanted to know how I can prove this relation \omega/k=\sqrt{\frac{k^{2}c^{2}+m^{2}c^{4}/\hbar^{2}}{k^{2}}}=c^{2}/v

I've figured it now. For the record:

\sqrt{\frac{k^{2}c^{2}+m^{2}c^{4}/\hbar^{2}}{k^{2}}}=\sqrt{c^{2}+\frac{m^{2}c^{4}}{k^{2}\hbar^{2}}}=\sqrt{c^{2}+\frac{m^{2}c^{4}}{\gamma^{2}m^{2}v^{2}}}=\sqrt{c^{2}+(1-v^{2}/c^{2})\frac{c^{4}}{v^{2}}}=\sqrt{c^{2}+\frac{c^{4}}{v^{2}}-c^{2}}=c^{2}/v

That was it.
 
  • #10
I know that the phase velocity equals ω/k
You've said repeatedly that it wasn't.
I've figured it now.
Good. Now try figuring out the easier approach in #2.
 
  • #11
You. are. wrong. I don't know if you still haven't understood what I needed, but you nevertheless made several mistakes.

"vg = c2"
It's not, according to the very wikipedia article you linked me to, vg = c2/v, where vg is the group velocity, vp is the phase velocity, and v is the particle velocity.

"You're mistaken."
I most certainly wasn't, seeing as your next post contained the exact same differentiation I made, calculated in a slightly different way.

"In the last step you've used v = k/ω, whereas actually v = ω/k."
I did not. I assumed vg = ω/k = c2/v.

"The phase velocity is always ω/k"
Correct

"v = ω/k"
Incorrect. the phase velocity is ω/k, not the particle velocity. Once again. vp = ω/k = c2/v

"You've said repeatedly that [phase velocity] wasn't [equal to] ω/k."
I searched the thread, and can find no statement of the sort. I find this:
derivation of the *phase* velocity, ω/k,
 

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