Changes between Version 144 and Version 145 of doc/app/initialization_parameters
- Timestamp:
- Jan 6, 2011 1:12:18 PM (14 years ago)
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doc/app/initialization_parameters
v144 v145 761 761 762 762 '''Note''': Due to the larger stencil of this scheme vertical grid stretching should be handled with care. 763 The computation of turbulent fluxes takes place inside the advection routines to get a statistical evaluation consistent to the numerical solution.\\\\ 763 The computation of turbulent fluxes takes place inside the advection routines to get a statistical evaluation consistent to the numerical solution. 764 765 '''Important''': The number of ghost layers for 2d and 3d arrays changed. This affects also the user interface. Please adapt the allocation of 2d and 3d arrays in your user interface like [../userint/output#Allocate here]. Furthermore the exchange of ghost layers for 3d variables changed, so calls of exchange_horiz in the user interface have to be modified. Here an example for the u-component of velocity: CALL exchange_horiz( u , nbgp ). \\\\ 764 766 '' 'pw-scheme' ''\\\\ 765 767 The scheme of Piascek and Williams (1970, J. Comp. Phys., 6, 392-405) with central differences in the form C3 is used. … … 955 957 956 958 '''Note''': Due to the larger stencil of this scheme vertical grid stretching should be handled with care. 957 The computation of turbulent fluxes takes place inside the advection routines to get a statistical evaluation consistent to the numerical solution.\\\\ 959 The computation of turbulent fluxes takes place inside the advection routines to get a statistical evaluation consistent to the numerical solution. 960 961 '''Important''': The number of ghost layers for 2d and 3d arrays changed. This affects also the user interface. Please adapt the allocation of 2d and 3d arrays in your user interface like [../userint/output#Allocate here]. Furthermore the exchange of ghost layers for 3d variables changed, so calls of exchange_horiz in the user interface have to be modified. Here an example for the u-component of velocity: CALL exchange_horiz( pt , nbgp ). \\\\ 958 962 '' 'pw-scheme' ''\\\\ 959 963 The scheme of Piascek and Williams (1970, J. Comp. Phys., 6, 392-405) with central differences in the form C3 is used.
