Changes between Version 18 and Version 19 of doc/tec/discret


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Timestamp:
Nov 25, 2019 9:05:25 AM (5 years ago)
Author:
Giersch
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  • doc/tec/discret

    v18 v19  
    1212The bottom boundary of the model domain is indicated by the first ''w''-component (''w(k=0)'') whereas the top boundary is indicated by ''w(k=nz)''. In case of no-slip (Dirichlet) condition at the ground, the first grid point for scalars and ''u'',''v'' is defined at the same height as ''w(k=0)'' (0m) to simulate a constant flux layer using Monin–Obukhov similarity theory. In case of free-slip (Neumann) condition, however, the first grid point for scalars and ''u'',''v'' lies at ''-dz/2'' within the ground and using a constant flux layer is not allowed anymore. At the top boundary, the last scalar grid point (''nz+1'') is ''dz/2'' above ''w(k=nz)'', similar to the bottom in case of free-slip (Neumann) condition. However, if the user wants to have exact symmetric vertical boundaries, he or she must shift the uppermost grid point for scalars and ''u'',''v'' to the height of ''w(k=nzt)''.
    1313
    14 '''Note''': Due to same array sizes of ''u'', ''v'', and ''w'' the uppermost grid point of the model domain is ''w(k=nz+1)''. This point doesn't play a role for solving the mode equations.     
     14'''Note''': Due to same array sizes of ''u'', ''v'', and ''w'' the uppermost grid point of the model domain is ''w(k=nz+1)''. This point doesn't play a role for solving the model equations.     
    1515
    1616[[Image(02.png,600px,border=1)]]