Sum rule in quantum mechanics: Difference between revisions

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The '''Minnaert resonance'''<ref>{{Citation |last=Minnaert |first=M. |authorlink=Marcel Minnaert |year=1933 |title=On musical air-bubbles and the sound of running water |journal=Philosophical Magazine |volume=16 |issue=104 |pages=235–248 |doi=10.1080/14786443309462277}}</ref> is the [[acoustic resonance|acoustic]] [[resonance]] frequency of a single bubble in an infinite domain of water (neglecting the effects of [[surface tension]] and [[viscous]] [[attenuation]]). The resonant frequency is given by
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:<math>
  f = \cfrac{1}{2\pi a}\left(\cfrac{3\gamma~p_A}{\rho}\right)^{1/2}
</math>
where <math>a</math> is the radius of the bubble, <math>\gamma</math> is the [[polytropic]] coefficient, <math>p_A</math> is the [[Ambient space|ambient]] pressure, and <math>\rho</math> is the density of water.  This formula can also be used to find the resonant frequency of a bubble cloud with <math>a</math> as the radius of the cloud and <math>\rho</math> the difference between the density of water and the bulk density of the cloud. For a bubble in water at standard pressure <math>(p_A=100~ {\rm kPa}, ~ \rho=1000~ {\rm kg/m^3})</math>, this equation reduces to
<math>
  f a \approx 3.26~ \rm m/s
</math>,
where <math> f~ </math> is the resonant frequency of the bubble.
 
== References ==
<references/>
 
== External links ==
*[http://ams.allenpress.com/perlserv/?request=get-document&doi=10.1175%2F1520-0426(2000)017%3C0847%3ALFRSOB%3E2.0.CO%3B2&ct=1  Low-Frequency Resonant Scattering of Bubble Clouds] by Paul A. Hwang and William J. Teague, 2000, Journal of Atmospheric and Oceanic Technology, vol. 17, no. 6, pp.&nbsp;847-853.
 
[[Category:Sound]]
[[Category:Bubbles]]

Latest revision as of 20:37, 3 December 2014

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