Velocity inertial subrange model: Difference between revisions
From Atomix
Jmmcmillan (talk | contribs) No edit summary |
m Added the inertial subrange eqn using the variables nomenclature.. |
||
| Line 5: | Line 5: | ||
}} | }} | ||
== Inertial subrange for steady-flows == | == Inertial subrange for steady-flows == | ||
<math>\Psi(\hat{k})=a_jC_k\varepsilon^{2/3}\hat{k}^{-5/3}</math> | |||
[[File:InertialSubrange.png]] | |||
== Inertial subrange for flows influenced by surface waves == | == Inertial subrange for flows influenced by surface waves == | ||
Need to add equations and figures from Lumley & Terray | Need to add equations and figures from Lumley & Terray | ||
Revision as of 18:44, 11 November 2021
| Short definition of Velocity inertial subrange model |
|---|
| The inertial subrange separates the energy-containing production range from the viscous dissipation range. |
This is the common definition for Velocity inertial subrange model, but other definitions maybe discussed within the wiki.
{{#default_form:DefineConcept}} {{#arraymap:Velocity point-measurements, Velocity profilers|,|x||}}
Inertial subrange for steady-flows
<math>\Psi(\hat{k})=a_jC_k\varepsilon^{2/3}\hat{k}^{-5/3}</math>
Inertial subrange for flows influenced by surface waves
Need to add equations and figures from Lumley & Terray
