Universal functions: Difference between revisions

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<div class="definition"><div class="short_definition">According to the [[Monin&ndash;Obukhov similarity theory]], the dimensionless [[shear]]    <div class="display-formula"><blockquote>[[File:ams2001glos-Ue3.gif|link=|center|ams2001glos-Ue3]]</blockquote></div>  [[temperature]] gradient    <div class="display-formula"><blockquote>[[File:ams2001glos-Ue4.gif|link=|center|ams2001glos-Ue4]]</blockquote></div>    and other gradients in the [[surface layer]] are proportional to dimensionless universal [[stability]]  functions, where ''M'' is [[wind speed]], &#x003b8; is [[potential temperature]], ''u''<sub>&#x0002a;</sub> is [[friction velocity]], and &#x003b8;<sub>&#x0002a;</sub> is  the surface kinematic [[heat flux]] divided by [[friction velocity]].</div><br/> <div class="paragraph">These functions have a value of nearly 1 for neutral [[stratification]], [[range]] over 0 &lt; (''z''/''L'') &lt;  1 for unstable stratification, and ''z''/''L'' &gt; 1 for stable stratification, where ''z'' is height above the  surface and ''L'' is the [[Obukhov length]]. For strong stability (''z''/''L'' &gt;&gt; 1) the universal functions  are nearly constant. Presently the most-used universal functions are based on an experiment conducted  in Kansas in 1968, with some corrections made in the succeeding 30 years. The [[accuracy]]  is about 10% for unstable and 20% for stable stratification. The following empirical forms of the  universal functions, based on a von [[K&aacute;rm&aacute;n constant]] of k = 0.4, are currently used. For unstable  stratification:    <div class="display-formula"><blockquote>[[File:ams2001glos-Ue5.gif|link=|center|ams2001glos-Ue5]]</blockquote></div>For neutral stratification: <div class="display-formula"><blockquote>[[File:ams2001glos-Ue7.gif|link=|center|ams2001glos-Ue7]]</blockquote></div>For stable stratification: <div class="display-formula"><blockquote>[[File:ams2001glos-Ue9.gif|link=|center|ams2001glos-Ue9]]</blockquote></div>These universal functions are <br/>''also called'' [[flux-profile relationships]].</div><br/> </div>
<div class="definition"><div class="short_definition">According to the [[Monin&ndash;Obukhov similarity theory]], the dimensionless [[shear]]    <div class="display-formula"><blockquote>[[File:ams2001glos-Ue3.gif|link=|center|ams2001glos-Ue3]]</blockquote></div>  [[temperature]] gradient    <div class="display-formula"><blockquote>[[File:ams2001glos-Ue4.gif|link=|center|ams2001glos-Ue4]]</blockquote></div>    and other gradients in the [[surface layer]] are proportional to dimensionless universal [[stability]]  functions, where ''M'' is [[wind speed]], &#x003b8; is [[potential temperature]], ''u''<sub>&#x0002a;</sub> is [[friction velocity]], and &#x003b8;<sub>&#x0002a;</sub> is  the surface kinematic [[heat flux]] divided by [[friction velocity]].</div><br/> <div class="paragraph">These functions have a value of nearly 1 for neutral [[stratification]], [[range]] over 0 &lt; (''z''/''L'') &lt;  1 for unstable stratification, and ''z''/''L'' &gt; 1 for stable stratification, where ''z'' is height above the  surface and ''L'' is the [[Obukhov length]]. For strong stability (''z''/''L'' &gt;&gt; 1) the universal functions  are nearly constant. Presently the most-used universal functions are based on an experiment conducted  in Kansas in 1968, with some corrections made in the succeeding 30 years. The [[accuracy]]  is about 10% for unstable and 20% for stable stratification. The following empirical forms of the  universal functions, based on a von [[K&#x000e1;rm&#x000e1;n constant]] of k = 0.4, are currently used. For unstable  stratification:    <div class="display-formula"><blockquote>[[File:ams2001glos-Ue5.gif|link=|center|ams2001glos-Ue5]]</blockquote></div>For neutral stratification: <div class="display-formula"><blockquote>[[File:ams2001glos-Ue7.gif|link=|center|ams2001glos-Ue7]]</blockquote></div>For stable stratification: <div class="display-formula"><blockquote>[[File:ams2001glos-Ue9.gif|link=|center|ams2001glos-Ue9]]</blockquote></div>These universal functions are <br/>''also called'' [[flux-profile relationships]].</div><br/> </div>
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Latest revision as of 16:23, 20 February 2012



universal functions

According to the Monin–Obukhov similarity theory, the dimensionless shear
ams2001glos-Ue3
temperature gradient
ams2001glos-Ue4
and other gradients in the surface layer are proportional to dimensionless universal stability functions, where M is wind speed, θ is potential temperature, u* is friction velocity, and θ* is the surface kinematic heat flux divided by friction velocity.

These functions have a value of nearly 1 for neutral stratification, range over 0 < (z/L) < 1 for unstable stratification, and z/L > 1 for stable stratification, where z is height above the surface and L is the Obukhov length. For strong stability (z/L >> 1) the universal functions are nearly constant. Presently the most-used universal functions are based on an experiment conducted in Kansas in 1968, with some corrections made in the succeeding 30 years. The accuracy is about 10% for unstable and 20% for stable stratification. The following empirical forms of the universal functions, based on a von Kármán constant of k = 0.4, are currently used. For unstable stratification:
ams2001glos-Ue5
For neutral stratification:
ams2001glos-Ue7
For stable stratification:
ams2001glos-Ue9
These universal functions are
also called flux-profile relationships.


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