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add figure with tracer statistics

1 % $Header: /u/gcmpack/manual/part3/case_studies/advection_in_gyre_circulation/adv_gyre.tex,v 1.12 2008/01/16 19:08:41 jahn Exp $
2 % $Name: $
3
4 \bodytext{bgcolor="#FFFFFFFF"}
5
6
7 \section[Gyre Advection Example]{Ocean Gyre Advection Schemes}
8 \label{www:tutorials}
9 \label{sect:eg-adv-gyre}
10 \begin{rawhtml}
11 <!-- CMIREDIR:eg-adv-gyre: -->
12 \end{rawhtml}
13
14 Author: Oliver Jahn and Chris Hill
15
16
17
18 This set of examples is based on the barotropic and baroclinic gyre MITgcm configurations,
19 that are described in the tutorial sections \ref{sect:eg-baro} and \ref{sect:eg-fourlayer}.
20 The examples in this section explain how to introduce a passive tracer into the flow
21 field of the barotropic and baroclinic gyre setups and looks at how the time evolution
22 of the passive tracer depends on the advection or transport scheme that is selected
23 for the tracer.
24
25 Passive tracers are useful in many numerical experiments. In some cases tracers are
26 used to track flow pathways, for example in \cite{Dutay02} a passive tracer is used
27 to track pathways of CFC-11 in 13 global ocean models, using a numerical
28 configuration similar to the example described in section \ref{sect:eg-offline-cfc}).
29 In other cases tracers are used as a way
30 to infer bulk mixing coefficients for a turbulent flow field, for example in
31 \cite{marsh06} a tracer is used to infer eddy mixing coefficients in the
32 Antarctic Circumpolar Current region. In biogeochemical and ecological simulations large numbers
33 of tracers are used that carry the concentrations of biological nutrients and concentrations of
34 biological species, for example in ....
35 When using tracers for these and other purposes it is useful to have a feel for the role
36 that the advection scheme employed plays in determining properties of the tracer distribution.
37 In particular, in a discrete numerical model tracer advection only approximates the
38 continuum behavior in space and time and different advection schemes introduce diferent
39 approximations so that the resulting tracer distributions vary. In the following
40 text we illustrate how
41 to use the different advection schemes available in MITgcm here, and discuss which properties
42 are well represented by each one. The advection schemes selections also apply to active
43 tracers (e.g. $T$ and $S$) and the character of the schemes also affect their distributions
44 and behavior.
45
46 \subsection{Advection and tracer transport}
47
48 In general, the tracer problem we want to solve can be written
49
50 \begin{equation}
51 \label{EQ:eg-adv-gyre-generic-tracer}
52 \frac{\partial C}{partial t} = -U \cdot \nabla C + S
53 \end{equation}
54
55 where $C$ is the tracer concentration in a model cell, $U$ is the model three-dimensional
56 flow field ( $U=(u,v,w)$ ). In (\ref{EQ:eg-adv-gyre-generic-tracer}) $S$ represents source, sink
57 and tendency terms not associated with advective transport. Example of terms in $S$ include
58 (i) air-sea fluxes for a dissolved gas, (ii) biological grazing and growth terms (for a
59 biogeochemical problem) or (iii) convective mixing and other sub-grid parameterizations of
60 mixing. In this section we are primarily concerned with
61 \begin{enumerate}
62 \item how to introduce the tracer term, $C$, into an integration
63 \item the different discretized forms of
64 the $-U \cdot \nabla C$ term that are available
65 \end{enumerate}
66
67
68 \subsection{Introducing a tracer into the flow}
69
70 The MITgcm ptracers package (see section \ref{sec:pkg:ptracers} for a more complete discussion
71 of the ptracers package and section \ref{sec:pkg:using} for a general introduction to MITgcm
72 packages) provides pre-coded support for a simple passive tracer with an initial
73 distribution at simulation time $t=0$ of $C_0(x,y,z)$. The steps required to use this capability
74 are
75 \begin{enumerate}
76 \item{\bf Activating the ptracers package.} This simply requires adding the line {\tt ptracers} to
77 the {\tt packages.conf} file in the {\it code/} directory for the experiment.
78 \item{\bf Setting an initial tracer distribution.}
79 \end{enumerate}
80
81 Once the two steps above are complete we can proceed to examine how the tracer we have created is
82 carried by the flow field and what properties of the tracer distribution are preserved under
83 different advection schemes.
84
85 \subsection{Selecting an advection scheme}
86
87 - flags in data and data.ptracers
88
89 - overlap width
90
91 - CPP GAD\_ALLOW\_SOM\_ADVECT required for SOM case
92
93 \subsection{Comparison of different advection schemes}
94
95 \begin{enumerate}
96 \item{Conservation}
97 \item{Dispersion}
98 \item{Diffusion}
99 \item{Positive definite}
100 \end{enumerate}
101
102 \input part3/case_studies/advection_in_gyre_circulation/adv_gyre_figure.tex
103
104 \begin{figure}
105 \begin{center}
106 \includegraphics*[width=\textwidth]{part3/case_studies/advection_in_gyre_circulation/stats.eps}
107 \end{center}
108 \caption{Maxima, minima and standard deviation (from left) as a function of time (in months)
109 for the gyre circulation experiment from figure~\ref{fig:adv-gyre-all}.}
110 \label{fig:adv-gyre-stats}
111 \end{figure}
112
113 \subsection{Code and Parameters files for this tutorial}
114
115 The code and parameters for the experiments can be found in the MITgcm example experiments
116 directory {\it verification/tutorial\_advection\_in\_gyre/}.
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