source: trunk/DOC/documentation/top_bound.tex @ 3567

Last change on this file since 3567 was 1012, checked in by aslmd, 11 years ago

LMDZ.COMMON. No need for ok_strato to activate sponge layer at model top. Default iflag_top_bound is 0 and no longer 1. Modified doc accordingly.

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1\documentclass[a4paper,10pt]{article}
2%\usepackage{graphicx}
3\usepackage{natbib}  % si appel à bibtex
4%\usepackage[francais]{babel}
5%\usepackage[latin1]{inputenc}  % accents directs (é...), avec babel
6%\usepackage{rotating}
7
8\setlength{\hoffset}{-1.in}
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10\setlength{\textwidth}{15.cm}
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21\setlength{\parindent}{0.mm}
22\setlength{\parskip}{1 em}
23\newcommand{\ten}[1]{$\times 10^{#1}$~} 
24\renewcommand{\baselinestretch}{1.}
25
26\begin{document}
27\pagestyle{plain}
28
29\begin{center}
30{\bf \LARGE 
31Documentation for LMDZ, Planets version
32
33\vspace{1cm}
34\Large
35The upper boundary sponge layer
36}
37
38\vspace{1cm}
39S\'ebastien Lebonnois , Ehouarn Millour
40
41\vspace{1cm}
42Latest version: \today
43\end{center}
44
45\section{Theoretical aspects}
46Because of the inevitable numerical boundary at the top of the model,
47upward travelling waves are found to non-physically reflect down into the
48atmosphere.
49A common remedy to this unwanted behaviour is to apply a sponge layer near
50the top of the model in order to quench these waves and avoid significant
51reflection thereof.
52In practice such quenching is done by adding a dissipative term which forces
53a relaxation of potential temperature and/or winds of the form:
54\[
55 A(t)=A_m+A_0 \exp(-\lambda t )
56\]
57Where $A_m$ is the value towards which $A$ is to asymptotically relax, and
58$\lambda$ is the inverse of the characteristic relaxation time scale.
59As there is no obvious value of $A_m$ towards which to relax, in practice
60it is often chosen to be either the zonal average of $A$ (evaluated at time $t$,
61i.e. conveniently ignoring that $A_m$ then is in fact not time-independent),
62or zero (at least for winds, since this would have little physical meaning for
63potential temperature).
64
65\section{Pratical aspects in the code}
66
67%The sponge layer is applied at the upper boundary when the \textsf{ok\_strato}
68%flag is set to {\em True} in \textsf{gcm.def}
69%(this parameter also controls the application of a second step in the
70%determination of vertical variation of coefficients for
71%the horizontal dissipation, see \textsf{inidissip.F} and
72%\textsf{disspi\_horiz.pdf} document).
73
74The tendencies for the upper boundary sponge layer are computed separately in
75the \textsf{top\_bound.F} routine (called from \textsf{leapfrog.F}) and
76added in place.
77The resulting sponge tendency \textsf{dutop}, in m/s, is also given as an output for
78diagnostics.
79
80Three parameters may be adjusted in the \textsf{gcm.def} file:
81\begin{itemize}
82\item \textsf{iflag\_top\_bound}: selects the affected layers.
83  \begin{itemize}
84  \item 1: only the top 4 layers are affected. In this case, the damping rate
85  is divided by 2 in the second layer, 4 in the third and 8 in the fourth.
86  \item 2: layers with pressure lower than 100 times the top pressure.
87  In this case, the damping rate depends linearly on the pressure.
88  \end{itemize}
89\item \textsf{mode\_top\_bound}: selects how the fields are affected.
90  \begin{itemize}
91  \item 0: No sponge layer is applied.
92  \item 1: Zonal and meridional winds are damped to zero.
93  \item 2: Zonal and meridional winds are damped to their zonally averaged value.
94  \item 3: Temperature, zonal and meridional winds are damped to their zonally
95  averaged value.
96  \end{itemize}
97\item \textsf{tau\_top\_bound}: damping rate ($\lambda$ in equation above,
98expressed in Hz) in the topmost layer.
99\end{itemize}
100
101%\begin{thebibliography}{2}
102%\providecommand{\natexlab}[1]{#1}
103%\expandafter\ifx\csname urlstyle\endcsname\relax
104%  \providecommand{\doi}[1]{doi:\discretionary{}{}{}#1}\else
105%  \providecommand{\doi}{doi:\discretionary{}{}{}\begingroup
106%  \urlstyle{rm}\Url}\fi
107
108%\end{thebibliography}
109
110\end{document}
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