Changes between Version 89 and Version 90 of doc/app/initialization_parameters


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Timestamp:
Sep 15, 2010 11:24:03 AM (14 years ago)
Author:
kanani
Comment:

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  • doc/app/initialization_parameters

    v89 v90  
    323323Parameter to switch on longwave radiation cooling at cloud-tops.\\\\
    324324Long-wave radiation processes are parameterized by the effective emissivity, which considers only the absorption and emission of long-wave radiation at cloud droplets. The radiation scheme can be used only with [#cloud_physics cloud_physics] = ''.TRUE.''.
     325}}}
     326|----------------
     327{{{#!td style="vertical-align:top"
     328[=#random_heatflux '''random_heatflux''']
     329}}}
     330{{{#!td style="vertical-align:top"
     331L
     332}}}
     333{{{#!td style="vertical-align:top"
     334.F.
     335}}}
     336{{{#!td
     337Parameter to impose random perturbations on the internal two-dimensional near surface heat flux field '''shf'''.\\\\
     338If a near surface heat flux is used as bottom boundary condition (see [#surface_heatflux surface_heatflux]), it is by default assumed to be horizontally homogeneous. Random perturbations can be imposed on the internal two-dimensional heat flux field '''shf''' by assigning '''random_heatflux''' = ''.T.''. The disturbed heat flux field is calculated by multiplying the values at each mesh point with a normally distributed random number with a mean value and standard deviation of 1. This is repeated after every timestep.\\\\
     339In case of a non-flat topography, assigning '''random_heatflux''' = ''.T.'' imposes random perturbations on the combined heat flux field '''shf''' composed of surface_heatflux at the bottom surface and [#wall_heatflux wall_heatflux](0) at the topography top face.
     340}}}
     341|----------------
     342{{{#!td style="vertical-align:top"
     343[=#<insert_parameter_name> '''<insert_parameter_name>''']
     344}}}
     345{{{#!td style="vertical-align:top"
     346<insert type>
     347}}}
     348{{{#!td style="vertical-align:top"
     349<insert value>
     350}}}
     351{{{#!td
     352<insert explanation>
     353}}}
     354|----------------
     355{{{#!td style="vertical-align:top"
     356[=#<insert_parameter_name> '''<insert_parameter_name>''']
     357}}}
     358{{{#!td style="vertical-align:top"
     359<insert type>
     360}}}
     361{{{#!td style="vertical-align:top"
     362<insert value>
     363}}}
     364{{{#!td
     365<insert explanation>
     366}}}
     367|----------------
     368{{{#!td style="vertical-align:top"
     369[=#<insert_parameter_name> '''<insert_parameter_name>''']
     370}}}
     371{{{#!td style="vertical-align:top"
     372<insert type>
     373}}}
     374{{{#!td style="vertical-align:top"
     375<insert value>
     376}}}
     377{{{#!td
     378<insert explanation>
     379}}}
     380|----------------
     381{{{#!td style="vertical-align:top"
     382[=#<insert_parameter_name> '''<insert_parameter_name>''']
     383}}}
     384{{{#!td style="vertical-align:top"
     385<insert type>
     386}}}
     387{{{#!td style="vertical-align:top"
     388<insert value>
     389}}}
     390{{{#!td
     391<insert explanation>
    325392}}}
    326393|----------------