Changeset 2541 for trunk/DOC/TexFiles/Chapters/Chap_ZDF.tex

Timestamp:

2011-01-09T05:55:20+01:00 (13 years ago)

Author:

gm

Message:

v3.3beta: #658 hopefully the final update, including MPP sum, SIGN, IOM, fldread documentation

File:

• trunk/DOC/TexFiles/Chapters/Chap_ZDF.tex (modified) (3 diffs)

trunk/DOC/TexFiles/Chapters/Chap_ZDF.tex

@@ -246 +246 @@
 \subsubsection{Surface wave breaking parameterization}
 %-----------------------------------------------------------------------%
-
 Following \citet{Mellor_Blumberg_JPO04}, the TKE turbulence closure model has been modified 
 to include the effect of surface wave breaking energetics. This results in a reduction of summertime 
@@ -329 +328 @@
 %--------------------------------------------------------------%
 
-% add here a description of "penetration of TKE" and the associated namelist parameters
-% \np{nn\_etau}, \np{rn\_efr}, \np{nn\_htau}
+To be add here a description of "penetration of TKE" and the associated namelist parameters
+ \np{nn\_etau}, \np{rn\_efr} and \np{nn\_htau}.
 
 % from Burchard et al OM 2008 : 
-% 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).
+% 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; Large et al., 1994; Meier, 2001; Axell, 2002; St. Laurent and Garrett, 2002).
 
 
@@ -355 +354 @@
 of \eqref{Eq_zdftke_e}) should balance the loss of kinetic energy associated with
 the vertical momentum diffusion (first line in \eqref{Eq_PE_zdf}). To do so a special care 
-have to be taken for both the time and space discretization of the TKE equation \citep{Burchard_OM02}.
+have to be taken for both the time and space discretization of the TKE equation 
+\citep{Burchard_OM02,Marsaleix_al_OM08}.
 
 Let us first address the time stepping issue. Fig.~\ref{Fig_TKE_time_scheme} shows