- Timestamp:
- 2010-11-19T21:36:45+01:00 (13 years ago)
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branches/nemo_v3_3_beta/DOC/TexFiles/Chapters/Chap_ZDF.tex
r2376 r2414 326 326 327 327 328 %\subsubsection{Mixing just below the mixed layer}329 %-------------------------------------------------------------- -%328 \subsubsection{Mixing just below the mixed layer} 329 %--------------------------------------------------------------% 330 330 331 331 % add here a description of "penetration of TKE" and the associated namelist parameters 332 % \np{nn\_etau}, \np{rn\_efr}, \np{nn\_htau} 333 334 % from Burchard et al OM 2008 : 335 % the most critical process not reproduced by statistical turbulence models is the activity of internal waves and their interaction with turbulence. After the Reynolds decomposition, internal waves are in principle included in the RANS equations, but later partially excluded by the hydrostatic assumption and the model resolution. Thus far, the representation of internal wave mixing in ocean models has been relatively crude (e.g. Mellor, 1989; Largeetal., 1994; Meier, 2001; Axell, 2002; St. Laurent and Garrett, 2002). 336 337 332 338 333 339 % -------------------------------------------------------------------------------------------------------------
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