Phase speed

The phase velocity of a wave is the rate at which the wave propagates in any medium. This is the velocity at which the phase of any one frequency component of the wave travels. For such a component, any given phase of the wave (for example, the crest) will appear to travel at the phase velocity. The phase velocity is given in terms of the wavelength (lambda) and time period as
:$v_\mathrm = \frac.$

Equivalently, in terms of the wave's angular frequency , which specifies angular change per unit of time, and wavenumber (or angular wave number) , which represent the angular change per unit of space,

:$v_\mathrm = \frac.$

To gain some basic intuition for this equation, we consider a propagating (cosine) wave . We want to see how fast a particular phase of the wave travels. For example, we can choose , the phase of the first crest. This implies , and so .

Formally, we let the phase and see immediately that and . So, it immediately follows that

:$\frac = -\frac \frac = \frac.$

As a result we observe a inverse relation between the angular frequency and wavevector. If the wave has higher frequency oscillations, the wave length must be shortened for the phase velocity to remain constant. Additionally, the phase velocity of electromagnetic radiation may – under certain circumstances (for example anomalous dispersion) – exceed the speed of light in a vacuum, but this does not indicate any superluminal information or energy transfer. It was theoretically described by physicists such as Arnold Sommerfeld and Léon Brillouin.

Group velocity

The group velocity of a collection of waves is defined as

:$v_g = \frac .$

When multiple sinusoidal waves are propagating together, the resultant superposition of the waves can result in an "envelope" wave as well as a "carrier" wave that lies inside the envelope. This commonly appears in wireless communications, modulation, a change in amplitude and/or phase is employed to send data. To gain some intuition for this definition, we consider a superposition of (cosine) waves with their respective angular frequencies and wavevectors.

:$\begin f(x, t) &= \cos(k_1 x - \omega_1 t) + \cos(k_2 x - \omega_2 t)\\ &= 2\cos\left(\frac\right)\cos\left(\frac\right)\\ &= 2f_1(x,t)f_2(x,t). \end$

So, we have a product of two waves: an envelope wave formed by and a carrier wave formed by . We call the velocity of the envelope wave the group velocity. We see that the phase velocity of is
:$\frac.$
In the continuous differential case, this becomes the definition of the group velocity.

Refractive index

In the context of electromagnetics and optics, the frequency is some function of the wave number, so in general, the phase velocity and the group velocity depend on specific medium and frequency. The ratio between the speed of light ''c'' and the phase velocity ''v''_''p'' is known as the refractive index, .

In this way, we can obtain another form for group velocity for electromagnetics. Writing , a quick way to derive this form is to observe
:$k = \frac\omega n(\omega) \implies dk = \frac\left(n(\omega) + \omega \fracn(\omega)\right)d\omega.$
We can then rearrange the above to obtain
:$v_g = \frac = \frac.$

From this formula, we see that the group velocity is equal to the phase velocity only when the refractive index is a constant . When this occurs, the medium is called non-dispersive, as opposed to dispersive, where various properties of the medium depend on the frequency . The relation is known as the dispersion relation of the medium.

See also

* Cherenkov radiation
* Dispersion (optics)
* Group velocity
*Propagation delay
*Shear wave splitting
*Wave propagation
*Wave propagation speed
*Planck constant
*Speed of light
* Matter wave#Phase velocity

References

Footnotes

Bibliography

*Crawford jr., Frank S. (1968). ''Waves (Berkeley Physics Course, Vol. 3)'', McGraw-Hill,
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Wave mechanics