Mixed-layer similarity: Difference between revisions
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An empirical method of finding universal relationships between [[boundary layer|boundary layer]] variables that are made dimensionless using the [[Deardorff velocity]] ''w''<sub>*</sub>, the [[mixed-layer depth|mixed-layer depth]] ''z''<sub>''i''</sub>, and the mixed-layer [[temperature scale]] [[File:ams2001glos-Mex01.gif|link=|ams2001glos-Mex01]], where [[File:ams2001glos-Mex02.gif|link=|ams2001glos-Mex02]] is the surface kinematic [[heat flux]].<br/> The resulting universal relationships are valid only for convective [[mixed layers]]. An example is <blockquote>[[File:ams2001glos-Me11.gif|link=|center|ams2001glos-Me11]]</blockquote><br/>''Compare'' [[local free-convection similarity]], [[local similarity]], [[similarity theory]], [[dimensional analysis]], [[Buckingham Pi theory]].<br/> Stull, R. B. 1988. An Introduction to Boundary Layer Meteorology. 666 pp. | |||
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Latest revision as of 11:50, 29 March 2024
An empirical method of finding universal relationships between boundary layer variables that are made dimensionless using the Deardorff velocity w*, the mixed-layer depth zi, and the mixed-layer temperature scale , where is the surface kinematic heat flux.
The resulting universal relationships are valid only for convective mixed layers. An example is
Compare local free-convection similarity, local similarity, similarity theory, dimensional analysis, Buckingham Pi theory.
Stull, R. B. 1988. An Introduction to Boundary Layer Meteorology. 666 pp.
The resulting universal relationships are valid only for convective mixed layers. An example is
Compare local free-convection similarity, local similarity, similarity theory, dimensional analysis, Buckingham Pi theory.
Stull, R. B. 1988. An Introduction to Boundary Layer Meteorology. 666 pp.