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Notes on tags used in MITgcmUV |
Notes on tags used in MITgcmUV |
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============================== |
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o pkg/seaice/seaice_calc_l/rhs.F: replace maskW/S by maskInW/S; this fixes |
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a serious convergence problem when open boundaries are involved |
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o pkg/ggl90: fix computation of control volumes for the case of |
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ALLOW_GGL90_HORIZDIFF (probably not used very often): move control volumes |
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up half a grid cell from C-centered to W-centered (pointed out by C. Eden) |
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o pkg/seaice: simplify seaice_evp by avoiding use of extra fields u/vIceC |
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o pkg/autodiff |
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- Add inAdMode switch for SEAICEuseDYNAMICS: |
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SEAICEuseDYNAMICSinAdMode |
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(extend logic in ADAUTODIFF_INADMODE_SET) |
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o pkg/seaice |
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- Step 1 of merging ice-thickness distribution (ITD) code from |
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MITgcm_contrib/torge/itd/ (author: Torge Martin) |
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The code implements concept laid out in Thorndike et al. (1975); |
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code is enabled via CPP flag SEAICE_ITD |
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nITD (in SEAICE_SIZE.h) defines number of ice thickness categories; |
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code is not complete yet!! |
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- SEAICE_SIZE.h now included in almost all seaice routines |
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o verification (using seaice): |
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- switch back seaice-dynamics (+ lower SOLV_MAX_ITERS) in ADM exp. |
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global_ocean.cs32x15.seaice ; update results. |
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- compile B-grid dynamics in FW test exp 1D_ocean_ice_column ; |
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- compile C-grid dynamics with #define SEAICE_ALLOW_JFNK in FW test exp |
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offline_exf_seaice (previously compiling B-grid). |
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o pkg/exf: |
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- fix some STOP conditions in exf_check.F (from Aug 28, modifs did not allow |
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to specify neither just 1 comp of wind or wind-stress, nor no surface momentum |
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forcing): just replace CPP option ALLOW_ATM_WIND with run-time param useAtmWind. |
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o pkg/layers (adjust changes from Sept 19): |
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- do snap-shot output and fill diagnostics from inside iLa loop (layers_calc.F) |
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this allows to remove "layers_maxNum" dimension from all layers arrays. |
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o pkg/layers (adjust changes from Sept 19): |
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- remove ALLOW_LAYERS_OUTPUT ; fix snap-shot and time-ave output ; |
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- snap-shot extended to all type of layers (not just the 1rst type); |
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- remove layers variables when corresponding CPP option is undef. |
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o pkg/layers: |
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- rename pkg/layers variable and add new output (layer exist & un-weighted |
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velocity in layer) |
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o pkg/seaice: |
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- simplify (?) ocean-drag coefficent computations by using |
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the same routine in all three solvers (saves some code lines) |
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- remove global fields DRAGA and DRAGS from C-grid code and |
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declare them locally in lsr.F (the only place where they are |
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still used) |
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- update AD output of lab_sea.evp (very sensitive anyway). |
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o pkg/seaice: add Jacobian-free Newton Krylov solver for ice dynamics |
o pkg/seaice: add Jacobian-free Newton Krylov solver for ice dynamics |
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(Lemieux et al. 2010, 2012). Turn on with the usual SEAICE_ALLOW_JFNK |
(Lemieux et al. 2010, 2012). Turn on with the usual SEAICE_ALLOW_JFNK |
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and SEAICEuseJFNK=.true. A few things to note: |
and SEAICEuseJFNK=.true. A few things to note: |
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orthogonalization method. Needs to be replaced. Original code |
orthogonalization method. Needs to be replaced. Original code |
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from J.-F. Lemieux |
from J.-F. Lemieux |
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- preconditioner for FGMRES is a stripped down version of LSOR |
- preconditioner for FGMRES is a stripped down version of LSOR |
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- SOLV_MAX_ITERS is now used for LSOR as a solver and as a |
- SOLV_MAX_ITERS is now used for LSOR as a solver and as a |
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preconditioner. For the preconditioner, the default is set to 10. |
preconditioner. For the preconditioner, the default is set to 10. |
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- Jacobian times vector is computed with finite differences |
- Jacobian times vector is computed with finite differences |
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- marginally related to JFNK-solver: add a smooth regularization for |
- marginally related to JFNK-solver: add a smooth regularization for |
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