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Changeset 3074 for branches/2011/dev_NOC_2011_MERGE/DOC/TexFiles/Chapters/Chap_DYN.tex – NEMO

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Timestamp:
2011-11-10T13:43:36+01:00 (12 years ago)
Author:
acc
Message:

Branch dev_NOC_2011_MERGE. #874. Step 11. Merge in changes from the dev_r2802_NOCL_prjhpg. Partially imposed coding standards (more could be done); added missing namelist changes and added first attempt at documentation

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  • branches/2011/dev_NOC_2011_MERGE/DOC/TexFiles/Chapters/Chap_DYN.tex

    r2986 r3074  
    633633$\bullet$ Rotated axes scheme (rot) \citep{Thiem_Berntsen_OM06} (\np{ln\_dynhpg\_rot}=true) 
    634634 
    635 Note that expression \eqref{Eq_dynhpg_sco} is used when the variable volume  
     635$\bullet$ Pressure Jacobian scheme (prj) \citep{Thiem_Berntsen_OM06} (\np{ln\_dynhpg\_prj}=true) 
     636 
     637Note that expression \eqref{Eq_dynhpg_sco} is commonly used when the variable volume  
    636638formulation is activated (\key{vvl}) because in that case, even with a flat bottom,  
    637639the coordinate surfaces are not horizontal but follow the free surface  
    638 \citep{Levier2007}. The other pressure gradient options are not yet available. 
     640\citep{Levier2007}. Only the pressure jacobian scheme (\np{ln\_dynhpg\_prj}=true) is available as an  
     641alternative to the default \np{ln\_dynhpg\_sco}=true when \key{vvl} is active.  The pressure Jacobian scheme uses  
     642a constrained cubic spline to reconstruct the density profile across the water column. This method 
     643maintains the monotonicity between the density nodes and is of a higher order than the linear 
     644interpolation method. The pressure can be calculated by analytical integration of the density profile and 
     645a pressure Jacobian method is used to solve the horizontal pressure gradient. This method should 
     646provide a more accurate calculation of the horizontal pressure gradient than the standard scheme. 
    639647 
    640648%-------------------------------------------------------------------------------------------------------------- 
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