28 | | .F. |
29 | | }}} |
30 | | {{{#!td |
31 | | Parameter to switch on the usage of cloud droplets.\\\\ |
32 | | Cloud droplets require using particles (i.e. the NAMELIST group [../parpar particles_par] has to be included in the parameter file). Then each particle representative for a certain number of droplets. The droplet features (number of droplets, initial radius, etc.) can be steered with the respective particle parameters (see e.g. [../parpar#radius radius]). The real number of initial droplets in a grid cell is equal to the initial number of droplets (defined by the particle source parameters [../parpar#pst pst], [../parpar#psl psl], [../parpar#psr psr], [../parpar#pss pss], [../parpar#psn psn], [../parpar#psb psb], [../parpar#pdx pdx], [../parpar#pdy pdy] and [../parpar#pdz pdz]) times the [../parpar#initial_weighting_factor initial_weighting_factor].\\\\ |
33 | | In case of using cloud droplets, the default condensation scheme in PALM cannot be used, i.e. [#cloud_physics cloud_physics] must be set ''.F.''. |
| 28 | 'boussinesq' |
| 29 | }}} |
| 30 | {{{#!td |
| 31 | Parameter to choose the approximation of the model equations. Currently two approximations are available:\\\\ |
| 32 | '' 'boussinesq' ''\\ |
| 33 | The Boussinesq approximation assumes an incompressible fluid. The density is assumed to be spatially and temporally constant. Internally the density is set to 1 kg/m3. \\\\ |
| 34 | '' 'anelastic' '' \\ |
| 35 | The anelastic approximation allows for a density decrease with height. The density is however still horizontally and temporally constant. The vertical profile of the density is computed based on the [#surfaces_pressure surfaces_pressure] and the vertical profile of the potential temperature. The anelastic approximation requires [#momentum_advec momentum_advec] = "ws-scheme" and [#psolver psolver] = "poisfft", "sor" or "multigrid_noopt". [#psolver psolver] = "multigrid" is currently not supported. Furthermore, [#conserve_volume_flow conserve_volume_flow] = .TRUE. is not supported.\\\\ |
| 36 | |
| 37 | Note, that the default flux representation for input and output depends on the approximation. For details, please see [#flux_input_mode flux_input_mode] and [#flux_output_mode flux_output_mode].\\\\ |
| 227 | }}} |
| 228 | |---------------- |
| 229 | {{{#!td style="vertical-align:top;width: 150px" |
| 230 | [=#flux_input_mode '''flux_input_mode'''] |
| 231 | }}} |
| 232 | {{{#!td style="vertical-align:top;width: 50px" |
| 233 | C*40 |
| 234 | }}} |
| 235 | {{{#!td style="vertical-align:top;width: 75px" |
| 236 | 'approximation-specific' |
| 237 | }}} |
| 238 | {{{#!td |
| 239 | Parameter to choose the flux unit for input data. Currently three choices are available:\\\\ |
| 240 | '' 'kinematic' ''\\ |
| 241 | The flux input data is assumed to be given as kinematic fluxes with the unit K m/s for sensible heat fluxes, kg/kg m/s for latent heat fluxes and m2/s2 for momentum fluxes. \\\\ |
| 242 | '' 'dynamic' '' \\ |
| 243 | The flux input data is assumed to be given as dynamic fluxes with the unit W/m2 for sensible and latent heat fluxes and N/m2 for momentum fluxes.\\\\ |
| 244 | '' 'approximation-specific' '' \\ |
| 245 | The flux input representation is chosen depending on the approximation. For [#approximation approximation] = "boussinesq" the fluxes are represented as "kinematic". For [#approximation approximation] = "anelastic" the fluxes are represented as "dynamic".\\\\ |
| 246 | }}} |
| 247 | |---------------- |
| 248 | {{{#!td style="vertical-align:top;width: 150px" |
| 249 | [=#flux_output_mode '''flux_output_mode'''] |
| 250 | }}} |
| 251 | {{{#!td style="vertical-align:top;width: 50px" |
| 252 | C*40 |
| 253 | }}} |
| 254 | {{{#!td style="vertical-align:top;width: 75px" |
| 255 | 'approximation-specific' |
| 256 | }}} |
| 257 | {{{#!td |
| 258 | Parameter to choose the flux unit for output data. Currently three choices are available:\\\\ |
| 259 | '' 'kinematic' ''\\ |
| 260 | The flux output data is given as kinematic fluxes with the unit K m/s for sensible heat fluxes, kg/kg m/s for latent heat fluxes and m2/s2 for momentum fluxes. \\\\ |
| 261 | '' 'dynamic' '' \\ |
| 262 | The flux output data is given as dynamic fluxes with the unit W/m2 for sensible and latent heat fluxes and N/m2 for momentum fluxes.\\\\ |
| 263 | '' 'approximation-specific' '' \\ |
| 264 | The flux output representation is chosen depending on the approximation. For [#approximation approximation] = "boussinesq" the fluxes are represented as "kinematic". For [#approximation approximation] = "anelastic" the fluxes are represented as "dynamic".\\\\ |