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First and foremost, do not subscribe to all social media marketing websites in the same time. Choose a social media software that fits your organization and marketing approach the most effective, develop your followers, and then contemplate extra social media websites.<br><br>
[[Image:Wave group.gif|frame|[[Dispersion (water waves)|Frequency dispersion]] in groups of [[gravity waves]] on the surface of deep water. The red dot moves with the phase velocity, and the green dots propagate with the [[group velocity]]. In this deep-water case, the phase velocity is twice the group velocity. The red dot overtakes two green dots when moving from the left to the right of the figure.<br>New waves seem to emerge at the back of a wave group, grow in amplitude until they are at the center of the group, and vanish at the wave group front.<br>For surface gravity waves, the water particle velocities are much smaller than the phase velocity, in most cases.]]


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[[Image:Wave opposite-group-phase-velocity.gif|thumb|frame|right|This shows a wave with the group velocity and phase velocity going in different directions. The group velocity is positive, while the phase velocity is negative.<ref name=nemirovsky2012negative>{{cite journal|last=Nemirovsky|first=Jonathan|coauthors=Rechtsman, Mikael C and Segev, Mordechai|title=Negative radiation pressure and negative effective refractive index via dielectric birefringence|journal=Optics Express|date=9 April 2012|volume=20|issue=8|pages=8907–8914|doi=10.1364/OE.20.008907|url=http://physics.technion.ac.il/~msegev/publications/NRP_Opt_Exp.pdf}}</ref>]]
 
The '''phase velocity''' of a [[wave]] is the rate at which the [[phase (waves)|phase]] of the wave [[Wave propagation|propagates in space]]. 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 (physics)|crest]]) will appear to travel at the phase velocity. The phase velocity is given in terms of the [[wavelength]] ''λ'' (lambda) and [[Wave period|period]] ''T'' as
 
:<math>v_\mathrm{p} = \frac{\lambda}{T}.</math>
 
Or, equivalently, in terms of the wave's [[angular frequency]] ''ω'', which specifies angular change per unit of time, and [[wavenumber]] (or angular wave number) ''k'', which represents the proportionality between the angular frequency ω and the linear speed (speed of propagation) ν<sub>p</sub>:
 
:<math>v_\mathrm{p} = \frac{\omega}{k}.</math>
 
To understand where this equation comes from, imagine a basic [[sine wave]], ''A''&nbsp;cos&nbsp;(''kx''−''ωt''). Given time ''t'', the source produces ''ωt/2&pi; = ft'' oscillations. At the same time, the initial wave front propagates away from the source through the space to the distance ''x'' to fit the same amount of oscillations, ''kx''&nbsp;=&nbsp;''ωt''. So that the propagation velocity ''v'' is ''v''&nbsp;=&nbsp;''x''/''t''&nbsp;=&nbsp;''ω''/''k''. The wave propagates faster when higher frequency oscillations are distributed less densely in space.<ref name="mathpages1">{{cite web|url=http://www.mathpages.com/home/kmath210/kmath210.htm |title=Phase, Group, and Signal Velocity |publisher=Mathpages.com |date= |accessdate=2011-07-24}}</ref> Formally, ''Φ''&nbsp;=&nbsp;''kx''−''ωt'' is the phase. Since ''ω''&nbsp;=&nbsp;−d''Φ''/d''t'' and ''k''&nbsp;=&nbsp;+d''Φ''/d''x'', the wave velocity is ''v''&nbsp;=&nbsp;d''x''/d''t''&nbsp;=&nbsp;''ω''/''k''.
 
== Relation to group velocity, refractive index and transmission speed ==
Since a pure sine wave cannot convey any information, some change in amplitude or frequency, known as [[modulation]], is required. By combining two sines with slightly different frequencies and wavelengths,
 
:<math>\cos[(k-\Delta k)x-(\omega-\Delta\omega)t]\; +\; \cos[(k+\Delta k)x-(\omega+\Delta\omega)t] = 2\; \cos(\Delta kx-\Delta\omega t)\; \cos(kx-\omega t),</math>
 
the amplitude becomes a sinusoid with phase speed of ''v''<sub>g</sub>&nbsp;=&nbsp;Δ''ω''/Δ''k''. It is this modulation that represents the signal content. Since each amplitude ''envelope'' contains a group of internal waves, this speed is usually called the [[group velocity]].<ref name="mathpages1"/>
In reality, the ''v''<sub>p</sub>&nbsp;=&nbsp;''ω''/''k'' and ''v''<sub>g</sub>&nbsp;=&nbsp;d''ω''/d''k'' ratios are determined by the media. The relation between phase speed, ''v''<sub>p</sub>, and speed of light, ''c'', is known as [[refractive index]], ''n''&nbsp;=&nbsp;''c''/''v''<sub>p</sub>&nbsp;=&nbsp;''ck''/''ω''. Taking the derivative of ''ω''&nbsp;=&nbsp;''ck''/''n'', we get the group speed,
 
:<math>\frac{\text{d}\omega}{\text{d}k} = \frac{c}{n} - \frac{ck}{n^2}\cdot\frac{\text{d}n}{\text{d}k}.</math>
 
Noting that ''c''/''n''&nbsp;=&nbsp;''v''<sub>p</sub>, this shows that group speed is equal to phase speed only when the refractive index is a constant: d''n''/d''k''&nbsp;=&nbsp;0.<ref name="mathpages1"/> Otherwise, when the phase velocity varies with frequency, velocities differ and the medium is called [[dispersion (optics)|dispersive]] and the function, <math>\omega(k)</math>, from which the group velocity is derived is known as a [[dispersion relation]].
The group 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]]. See [[dispersion (optics)|dispersion]] for a full discussion of wave velocities.
 
== See also ==
*[[Cherenkov radiation]]
*[[Dispersion (optics)]]
*[[Group velocity]]
*[[Propagation delay]]
*[[Shear wave splitting]]
*[[Wave propagation]]
*[[Wave propagation speed]]
*[[Planck constant]]
*[[Matter wave#Phase velocity]]
 
==References==
 
===Footnotes===
{{reflist}}
 
===Other===
{{refbegin}}
*{{citation | author-link=Léon Brillouin | last=Brillouin |first=Léon |title=Wave Propagation And Group Velocity |publisher=Academic Press Inc. |location=New York and London |year=1960 |isbn=0-12-134968-3 }}
*{{citation |last=Main |first=Iain G. |year=1988 |title=Vibrations and Waves in Physics |edition=2nd |location=New York |publisher=Cambridge University Press |isbn=0-521-27846-5 |pages=214–216 }}
*{{citation |last1=Tipler |first1=Paul A. |first2=Ralph A. |last2=Llewellyn |year=2003 |title=Modern Physics |edition=4th |location=New York |publisher=W. H. Freeman and Company |isbn=0-7167-4345-0 |pages=222–223 }}
{{refend}}
 
== External links ==
* [http://gregegan.customer.netspace.net.au/APPLETS/20/20.html Subluminal] – A Java applet
* [http://www.falstad.com/dispersion/ Simulation] – A Java applet by Paul Falstad
* [http://publicliterature.org/tools/group_and_phase_velocity/ Group and Phase Velocity] – Java applet showing the difference between group and phase velocity.
{{Velocities of Waves}}
<!-- interwiki kept as they link to sections -->
 
[[Category:Wave mechanics]]
 
[[fr:Vitesse d'une onde#Vitesse de phase]]
[[nl:Voortplantingssnelheid#Fase- en groepssnelheid]]

Latest revision as of 04:06, 4 August 2013

Frequency dispersion in groups of gravity waves on the surface of deep water. The red dot moves with the phase velocity, and the green dots propagate with the group velocity. In this deep-water case, the phase velocity is twice the group velocity. The red dot overtakes two green dots when moving from the left to the right of the figure.
New waves seem to emerge at the back of a wave group, grow in amplitude until they are at the center of the group, and vanish at the wave group front.
For surface gravity waves, the water particle velocities are much smaller than the phase velocity, in most cases.
This shows a wave with the group velocity and phase velocity going in different directions. The group velocity is positive, while the phase velocity is negative.[1]

The phase velocity of a wave is the rate at which the phase of the wave propagates in space. 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 λ (lambda) and period T as

Or, equivalently, in terms of the wave's angular frequency ω, which specifies angular change per unit of time, and wavenumber (or angular wave number) k, which represents the proportionality between the angular frequency ω and the linear speed (speed of propagation) νp:

To understand where this equation comes from, imagine a basic sine wave, A cos (kxωt). Given time t, the source produces ωt/2π = ft oscillations. At the same time, the initial wave front propagates away from the source through the space to the distance x to fit the same amount of oscillations, kx = ωt. So that the propagation velocity v is v = x/t = ω/k. The wave propagates faster when higher frequency oscillations are distributed less densely in space.[2] Formally, Φ = kxωt is the phase. Since ω = −dΦ/dt and k = +dΦ/dx, the wave velocity is v = dx/dt = ω/k.

Relation to group velocity, refractive index and transmission speed

Since a pure sine wave cannot convey any information, some change in amplitude or frequency, known as modulation, is required. By combining two sines with slightly different frequencies and wavelengths,

the amplitude becomes a sinusoid with phase speed of vg = Δωk. It is this modulation that represents the signal content. Since each amplitude envelope contains a group of internal waves, this speed is usually called the group velocity.[2] In reality, the vp = ω/k and vg = dω/dk ratios are determined by the media. The relation between phase speed, vp, and speed of light, c, is known as refractive index, n = c/vp = ck/ω. Taking the derivative of ω = ck/n, we get the group speed,

Noting that c/n = vp, this shows that group speed is equal to phase speed only when the refractive index is a constant: dn/dk = 0.[2] Otherwise, when the phase velocity varies with frequency, velocities differ and the medium is called dispersive and the function, , from which the group velocity is derived is known as a dispersion relation. The group 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. See dispersion for a full discussion of wave velocities.

See also

References

Footnotes

43 year old Petroleum Engineer Harry from Deep River, usually spends time with hobbies and interests like renting movies, property developers in singapore new condominium and vehicle racing. Constantly enjoys going to destinations like Camino Real de Tierra Adentro.

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    Naturally, you will have to pay a safety deposit and that is usually one month rent for annually of the settlement. That is the place your good religion deposit will likely be taken into account and will kind part or all of your security deposit. Anticipate to have a proportionate amount deducted out of your deposit if something is discovered to be damaged if you move out. It's best to you'll want to test the inventory drawn up by the owner, which can detail all objects in the property and their condition. If you happen to fail to notice any harm not already mentioned within the inventory before transferring in, you danger having to pay for it yourself.

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    Once you place down the one per cent choice price to carry down a non-public property, it's important to accept its situation as it is whenever you move in – faulty air-con, choked rest room and all. Get round this by asking your agent to incorporate a ultimate inspection clause within the possibility-to-buy letter. HDB flat patrons routinely take pleasure in this security net. "There's a ultimate inspection of the property two days before the completion of all HDB transactions. If the air-con is defective, you can request the seller to repair it," says Kelvin.

    15.6.1 As the agent is an intermediary, generally, as soon as the principal and third party are introduced right into a contractual relationship, the agent drops out of the image, subject to any problems with remuneration or indemnification that he could have against the principal, and extra exceptionally, against the third occasion. Generally, agents are entitled to be indemnified for all liabilities reasonably incurred within the execution of the brokers´ authority.

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fr:Vitesse d'une onde#Vitesse de phase nl:Voortplantingssnelheid#Fase- en groepssnelheid

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