#989 closed Task (fixed)
Create a branch for Smagorinsky model
Reported by: | hliu | Owned by: | Maria Luneva |
---|---|---|---|
Priority: | low | Milestone: | |
Component: | OCE | Version: | v3.4 |
Severity: | Keywords: | Smagorinsky mixing | |
Cc: |
Description
Create a branch for the implementation of Smagorinsky turbulence model based on r3452
Commit History (0)
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Change History (7)
comment:1 Changed 12 years ago by hliu
- Keywords Smagorinsky lateral mixing added
comment:2 Changed 11 years ago by acc
- Resolution set to fixed
- Status changed from new to closed
Branch included into 2012 merge ready for v3.5 release. Documentation still in preparation but closing ticket to discourage further changes on this branch.
comment:3 Changed 8 years ago by nicolasmartin
- Milestone 2012 Stream 3: New features deleted
Milestone 2012 Stream 3: New features deleted
comment:4 Changed 8 years ago by nicolasmartin
- Keywords lateral_mixing added; lateral removed
comment:5 Changed 8 years ago by nicolasmartin
- Keywords mixing removed
comment:6 Changed 7 years ago by nemo
- Keywords mixing added; lateral_mixing removed
comment:7 Changed 7 years ago by nemo
- Type changed from Development to Task
Remove 'Development' type
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Smagorinsky type diffusivity/viscosity for lateral mixing has been introduced.
When key_traldf_smag or key_dynldf_smag are defined, Smagorinsky 3D diffusivity or viscosity are calculated. These keys should be used together with key_traldf_c3d or key_dynldf_c3d respectively. Griffies and Hallberg, 2000 diffusivity-viscosity formulation has been used with the following modifications:
a) Coded stability criteria are twice strict in comparison with derived from linear stability theory to provide positiveness of solutions;
b) Numerical test demonstrated that even these stability criteria were too weak, as in this case equations can be strongly nonlinear and linear theory does not work. Additional constrains has been added (maximum value of diffusivity/viscosity), defined by rn_aht_m, rn_ahm_m_blp ,rn_ahm_m_lap
c) It has been found, that when tides are present, the input of tangential derivatives of velocity is too strong , as tidal velocity is roughly inversely proportional to the depth. Option, when only shear strain is used for calculations available : set rn_cmsh=0 , rn_smsh=0 in namelist.
Note:
Code needs a small modification to introduce new variable in namelist - background diffusivity/viscosity. Now rn_aht_0, rn_ahm_0_lap/bilap are background values, which can be confusing in other cases