Diffusivity: Difference between revisions

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<div class="definition"><div class="short_definition">(''Also called'' coefficient of diffusion.) The ratio of the [[flux]] of a [[conservative property]]  through a specified surface by [[turbulence]] to the [[gradient]] of the mean property normal to the  surface.</div><br/> <div class="paragraph">In the special case of [[isotropic turbulence]] and no mean motion the Fickian diffusion equation  (or Fick's equation) takes the form  <div class="display-formula"><blockquote>[[File:ams2001glos-De23.gif|link=|center|ams2001glos-De23]]</blockquote></div>where ''K''<sub>''s''</sub> represents the diffusivity, &nabla;<sup>2</sup> is the [[Laplacian operator]], and <div class="inline-formula">[[File:ams2001glos-Dex05.gif|link=|ams2001glos-Dex05]]</div> is the [[mean value]] of the  property <div class="inline-formula">[[File:ams2001glos-Dex06.gif|link=|ams2001glos-Dex06]]</div>. This equation describes decreasing <div class="inline-formula">[[File:ams2001glos-Dex07.gif|link=|ams2001glos-Dex07]]</div> where the Laplacian is negative and increasing  <div class="inline-formula">[[File:ams2001glos-Dex08.gif|link=|ams2001glos-Dex08]]</div> where the Laplacian is positive. The general case is more complex. In the statically stable  [[atmosphere]] or ocean, the horizontal [[scale of turbulence]] is much greater than the vertical scale  and [[turbulent diffusion]] in the horizontal may greatly exceed [[diffusion]] in the vertical. On the  other hand, in the case of [[buoyancy]], vertical diffusion may be greater than horizontal diffusion.  <br/>''See also'' [[mixing]], [[eddy flux]], [[turbulence length scales]].</div><br/> </div><div class="reference">Fleagle, R. G., and J. A. Businger 1980. An Introduction to Atmospheric Physics. 2d ed., Academic Press, . 64&ndash;  66. </div><br/> <div class="reference">Hinze, J. O. 1975. Turbulence.  2d ed., McGraw&ndash;Hill, . 48&ndash;55. </div><br/>  
<div class="definition"><div class="short_definition">(''Also called'' coefficient of diffusion.) The ratio of the [[flux]] of a [[conservative property]]  through a specified surface by [[turbulence]] to the [[gradient]] of the mean property normal to the  surface.</div><br/> <div class="paragraph">In the special case of [[isotropic turbulence]] and no mean motion the Fickian diffusion equation  (or Fick's equation) takes the form  <div class="display-formula"><blockquote>[[File:ams2001glos-De23.gif|link=|center|ams2001glos-De23]]</blockquote></div>where ''K''<sub>''s''</sub> represents the diffusivity, &nabla;<sup>2</sup> is the [[Laplacian operator]], and <div class="inline-formula">[[File:ams2001glos-Dex05.gif|link=|ams2001glos-Dex05]]</div> is the [[mean  value|mean value]] of the  property <div class="inline-formula">[[File:ams2001glos-Dex06.gif|link=|ams2001glos-Dex06]]</div>. This equation describes decreasing <div class="inline-formula">[[File:ams2001glos-Dex07.gif|link=|ams2001glos-Dex07]]</div> where the Laplacian is negative and increasing  <div class="inline-formula">[[File:ams2001glos-Dex08.gif|link=|ams2001glos-Dex08]]</div> where the Laplacian is positive. The general case is more complex. In the statically stable  [[atmosphere]] or ocean, the horizontal [[scale of turbulence]] is much greater than the vertical scale  and [[turbulent diffusion]] in the horizontal may greatly exceed [[diffusion]] in the vertical. On the  other hand, in the case of [[buoyancy]], vertical diffusion may be greater than horizontal diffusion.  <br/>''See also'' [[mixing]], [[eddy flux]], [[turbulence length scales]].</div><br/> </div><div class="reference">Fleagle, R. G., and J. A. Businger 1980. An Introduction to Atmospheric Physics. 2d ed., Academic Press, . 64&ndash;  66. </div><br/> <div class="reference">Hinze, J. O. 1975. Turbulence.  2d ed., McGraw&ndash;Hill, . 48&ndash;55. </div><br/>  
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Latest revision as of 15:48, 25 April 2012



diffusivity

(Also called coefficient of diffusion.) The ratio of the flux of a conservative property through a specified surface by turbulence to the gradient of the mean property normal to the surface.

In the special case of isotropic turbulence and no mean motion the Fickian diffusion equation (or Fick's equation) takes the form
ams2001glos-De23
where Ks represents the diffusivity, ∇2 is the Laplacian operator, and
ams2001glos-Dex05
is the mean value of the property
ams2001glos-Dex06
. This equation describes decreasing
ams2001glos-Dex07
where the Laplacian is negative and increasing
ams2001glos-Dex08
where the Laplacian is positive. The general case is more complex. In the statically stable atmosphere or ocean, the horizontal scale of turbulence is much greater than the vertical scale and turbulent diffusion in the horizontal may greatly exceed diffusion in the vertical. On the other hand, in the case of buoyancy, vertical diffusion may be greater than horizontal diffusion.
See also mixing, eddy flux, turbulence length scales.

Fleagle, R. G., and J. A. Businger 1980. An Introduction to Atmospheric Physics. 2d ed., Academic Press, . 64– 66.

Hinze, J. O. 1975. Turbulence. 2d ed., McGraw–Hill, . 48–55.


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