A generic length-scale equation for geophysical turbulence models
By L. Umlauf, H. Burchard. 2003
1,092 citations recorded by the source corpus.
Subfields: Atmospheric Science, Oceanography
View Paper: https://www.semanticscholar.org/paper/24fd6403615fc7a6c5d9b6156e4f1e8d4d280af2
How researchers see this paper
The researchers whose trusted networks rank it highest, strongest advocate first. Every researcher gets a different order.
In Atmospheric Science
- James C. McWilliams
- António M. Baptista
- Yinglong J. Zhang
- Alexander F. Shchepetkin
- A. Sogachev
- Hernan G. Arango
- L. Umlauf
- H. Burchard
In Oceanography
- James C. McWilliams
- António M. Baptista
- Yinglong J. Zhang
- Alexander F. Shchepetkin
- Hernan G. Arango
- A. Sogachev
- B. Fox‐Kemper
- H. Burchard
Citations in the corpus
- The physical oceanography of the transport of floating marine debris (2020, methodology): “On the other hand, Langmuir circulation and turbulence are not commonly included explicitly in regional or global ocean models, although recent software developments in GOTM (Umlauf and Burchard 2003) and CVMix (Griffies et al 2015) may make using parameterisations of Langmuir turbulence easier (Li ”
- Second-order turbulence closure models for geophysical boundary layers. A review of recent work (2005, methodology): “The methodology to derive these constraints has been discussed by detail by Umlauf and Burchard (2003).”
- A Note on Two-Equation Closure Modelling of Canopy Flow (2009, background): “During the last two decades, models using two-equation closure have attracted great attention in the geophysical modelling community and a number of authors have found it is sufficient for most practical tasks (Wang and Takle 1995; Umlauf and Burchard 2003; Castro et al. 2003; Hipsey et al. 2004; ”
- Development of a three-dimensional, regional, coupled wave, current, and sediment-transport model (2008, neutral): “2003) as implemented by Warner et al. (2005) that also includes the option for surface fluxes of turbulence kinetic energy due to wave breaking.”
- Seamless cross-scale modeling with SCHISM (2016, neutral): “…in [m 2 s −1 ] κ vertical eddy diffusivity, for tracers, in [m 2 s −1 ] F h horizontal diffusion and mass sources/sinks The differential system ( 1 –4 ) is closed with turbulence closure of the generic length-scale model of Umlauf and Burchard (2003) , and proper initial and boundary conditions…”
- The MyOcean IBI Ocean Forecast and Reanalysis Systems: operational products and roadmap to the future Copernicus Service (2015, methodology): “Vertical mixing is parameterized according to a k–ε model implemented in the generic form proposed by Umlauf and Burchard (2003) including surface wave breaking induced mixing, while tracers and momentum subgrid lateral mixing is parameterized according to bilaplacian operators.”
- Ocean forecasting in terrain-following coordinates: Formulation and skill assessment of the Regional Ocean Modeling System (2008, methodology): “Finally, the Generic Length Scale (GLS) approach [11] is a generalized two-equation model that takes advantage of the similarities among several two-equation turbulence closure models that have been used for turbulence modeling.”
- SELFE: A semi-implicit Eulerian–Lagrangian finite-element model for cross-scale ocean circulation (2008, methodology): “SELFE uses the Generic Length Scale (GLS) turbulence closure of Umlauf and Burchard (2003), which has the advantage of encompassing most of the 2.5-equation closure models (k–e(Rodi, 1984); k–x (Wilcox, 1998); Mellor and Yamada, 1982).”
- Modification of Two-Equation Models to Account for Plant Drag (2006, methodology): “to make ϕ completely identifiable with any of the traditional variables like El, e and ω ,b y simply adopting the parameters from Table 1 ( Umlauf and Burchard 2003 ).”