- Timestamp:
- 2011-11-10T13:43:36+01:00 (12 years ago)
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branches/2011/dev_NOC_2011_MERGE/DOC/TexFiles/Chapters/Chap_DYN.tex
r2986 r3074 633 633 $\bullet$ Rotated axes scheme (rot) \citep{Thiem_Berntsen_OM06} (\np{ln\_dynhpg\_rot}=true) 634 634 635 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) 636 637 Note that expression \eqref{Eq_dynhpg_sco} is commonly used when the variable volume 636 638 formulation is activated (\key{vvl}) because in that case, even with a flat bottom, 637 639 the 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 641 alternative to the default \np{ln\_dynhpg\_sco}=true when \key{vvl} is active. The pressure Jacobian scheme uses 642 a constrained cubic spline to reconstruct the density profile across the water column. This method 643 maintains the monotonicity between the density nodes and is of a higher order than the linear 644 interpolation method. The pressure can be calculated by analytical integration of the density profile and 645 a pressure Jacobian method is used to solve the horizontal pressure gradient. This method should 646 provide a more accurate calculation of the horizontal pressure gradient than the standard scheme. 639 647 640 648 %--------------------------------------------------------------------------------------------------------------
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