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gforget |
1.25 |
C $Header: /u/gcmpack/MITgcm/verification/lab_sea/code_ad/SEAICE_OPTIONS.h,v 1.24 2012/12/22 18:09:01 gforget Exp $ |
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jmc |
1.4 |
C $Name: $ |
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heimbach |
1.1 |
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jmc |
1.9 |
C *==========================================================* |
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jmc |
1.14 |
C | SEAICE_OPTIONS.h |
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C | o CPP options file for sea ice package. |
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jmc |
1.9 |
C *==========================================================* |
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jmc |
1.14 |
C | Use this file for selecting options within the sea ice |
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C | package. |
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jmc |
1.9 |
C *==========================================================* |
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heimbach |
1.1 |
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#ifndef SEAICE_OPTIONS_H |
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#define SEAICE_OPTIONS_H |
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#include "PACKAGES_CONFIG.h" |
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#include "CPP_OPTIONS.h" |
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jmc |
1.14 |
#ifdef ALLOW_SEAICE |
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C Package-specific Options & Macros go here |
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heimbach |
1.1 |
C-- Write "text-plots" of certain fields in STDOUT for debugging. |
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#undef SEAICE_DEBUG |
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C-- Allow sea-ice dynamic code. |
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C This option is provided to allow use of TAMC |
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C on the thermodynamics component of the code only. |
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C Sea-ice dynamics can also be turned off at runtime |
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C using variable SEAICEuseDYNAMICS. |
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#define SEAICE_ALLOW_DYNAMICS |
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C-- By default, the sea-ice package uses its own integrated bulk |
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C formulae to compute fluxes (fu, fv, EmPmR, Qnet, and Qsw) over |
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C open-ocean. When this flag is set, these variables are computed |
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C in a separate external package, for example, pkg/exf, and then |
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C modified for sea-ice effects by pkg/seaice. |
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#define SEAICE_EXTERNAL_FLUXES |
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dimitri |
1.23 |
C-- This CPP flag has been retired. The number of ice categories |
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C used to solve for seaice flux is now specified by run-time |
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C parameter SEAICE_multDim. |
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C Note: be aware of pickup_seaice.* compatibility issues when |
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C restarting a simulation with a different number of categories. |
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mlosch |
1.22 |
c#define SEAICE_MULTICATEGORY |
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heimbach |
1.1 |
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dimitri |
1.23 |
C-- run with sea Ice Thickness Distribution (ITD); |
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C set number of categories (nITD) in SEAICE_SIZE.h |
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#undef SEAICE_ITD |
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gforget |
1.18 |
C-- Since the missing sublimation term is now included |
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C this flag is needed for backward compatibility |
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#define SEAICE_DISABLE_SUBLIM |
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dimitri |
1.23 |
C-- Suspected missing term in coupled ocn-ice heat budget (to be confirmed) |
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gforget |
1.19 |
#define SEAICE_DISABLE_HEATCONSFIX |
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dimitri |
1.23 |
C-- Default is constant seaice salinity (SEAICE_salt0); Define the following |
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C flag to consider (space & time) variable salinity: advected and forming |
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C seaice with a fraction (=SEAICE_saltFrac) of freezing seawater salinity. |
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C- Note: SItracer also offers an alternative way to handle variable salinity. |
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ifenty |
1.11 |
#define SEAICE_VARIABLE_SALINITY |
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jmc |
1.9 |
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jmc |
1.14 |
C-- Tracers of ice and/or ice cover. |
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#undef ALLOW_SITRACER |
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#ifdef ALLOW_SITRACER |
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C-- To try avoid 'spontaneous generation' of tracer maxima by advdiff. |
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# define ALLOW_SITRACER_ADVCAP |
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#endif |
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jmc |
1.4 |
C-- By default the seaice model is discretized on a B-Grid (for |
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heimbach |
1.1 |
C historical reasons). Define the following flag to use a new |
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C (not thoroughly) test version on a C-grid |
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#define SEAICE_CGRID |
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jmc |
1.9 |
C-- Only for the C-grid version it is possible to |
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heimbach |
1.1 |
#ifdef SEAICE_CGRID |
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dimitri |
1.23 |
C enable JFNK code by defining the following flag |
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# undef SEAICE_ALLOW_JFNK |
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C enable LSR to use global (multi-tile) tri-diagonal solver |
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# undef SEAICE_GLOBAL_3DIAG_SOLVER |
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jmc |
1.9 |
C enable EVP code by defining the following flag |
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# define SEAICE_ALLOW_EVP |
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# ifdef SEAICE_ALLOW_EVP |
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dimitri |
1.23 |
C-- When set use SEAICE_zetaMin and SEAICE_evpDampC to limit viscosities |
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C from below and above in seaice_evp: not necessary, and not recommended |
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jmc |
1.9 |
# undef SEAICE_ALLOW_CLIPZETA |
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# endif /* SEAICE_ALLOW_EVP */ |
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dimitri |
1.23 |
C regularize zeta to zmax with a smooth tanh-function instead |
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C of a min(zeta,zmax). This improves convergence of iterative |
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C solvers (Lemieux and Tremblay 2009, JGR). No effect on EVP |
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# undef SEAICE_ZETA_SMOOTHREG |
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jmc |
1.9 |
C allow the truncated ellipse rheology (runtime flag SEAICEuseTEM) |
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# undef SEAICE_ALLOW_TEM |
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#else /* not SEAICE_CGRID, but old B-grid */ |
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C-- By default for B-grid dynamics solver wind stress under sea-ice is |
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C set to the same value as it would be if there was no sea-ice. |
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C Define following CPP flag for B-grid ice-ocean stress coupling. |
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# define SEAICE_BICE_STRESS |
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C-- By default for B-grid dynamics solver surface tilt is obtained |
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C indirectly via geostrophic velocities. Define following CPP |
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C in order to use ETAN instead. |
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# define EXPLICIT_SSH_SLOPE |
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dimitri |
1.23 |
C-- Defining this flag turns on FV-discretization of the B-grid LSOR solver. |
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C It is smoother and includes all metric terms, similar to C-grid solvers. |
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C It is here for completeness, but its usefulness is unclear. |
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jmc |
1.14 |
# undef SEAICE_LSRBNEW |
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heimbach |
1.1 |
#endif /* SEAICE_CGRID */ |
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jmc |
1.9 |
C-- When set limit the Ice-Loading to mass of 1/5 of Surface ocean grid-box |
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#undef SEAICE_CAP_ICELOAD |
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C-- When set use SEAICE_clipVelocties = .true., to clip U/VICE at 40cm/s, |
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dimitri |
1.23 |
C not recommended |
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jmc |
1.9 |
#undef SEAICE_ALLOW_CLIPVELS |
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dimitri |
1.23 |
C-- When set cap the sublimation latent heat flux in solve4temp according |
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C to the available amount of ice+snow. Otherwise this term is treated |
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C like all of the others -- residuals heat and fw stocks are passed to |
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C the ocean at the end of seaice_growth in a conservative manner. |
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C SEAICE_CAP_SUBLIM is not needed as of now, but kept just in case. |
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#undef SEAICE_CAP_SUBLIM |
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heimbach |
1.3 |
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dimitri |
1.23 |
C-- Enable free drift code |
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heimbach |
1.13 |
#define SEAICE_ALLOW_FREEDRIFT |
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gforget |
1.8 |
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jmc |
1.14 |
#endif /* ALLOW_SEAICE */ |
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heimbach |
1.1 |
#endif /* SEAICE_OPTIONS_H */ |
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CEH3 ;;; Local Variables: *** |
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CEH3 ;;; mode:fortran *** |
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CEH3 ;;; End: *** |
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