| 538 | |---------------- |
| 539 | {{{#!td style="vertical-align:top" |
| 540 | [=#use_sgs_for_particles '''use_sgs_for\\_particles'''] |
| 541 | }}} |
| 542 | {{{#!td style="vertical-align:top" |
| 543 | L |
| 544 | }}} |
| 545 | {{{#!td style="vertical-align:top" |
| 546 | .F. |
| 547 | }}} |
| 548 | {{{#!td |
| 549 | Use subgrid-scale velocities for particle advection.\\ |
| 550 | These velocities are calculated from the resolved and subgrid-scale TKE using the Monte-Carlo random-walk method described by Weil et al. (2004, JAS, 61, 2877-2887). When using this method, the timestep for the advancement of the particles is limited by the so-called Lagrangian time scale. This may be smaller than the current LES timestep so that several particle (sub-) timesteps have to be carried out within one LES timestep. In order to limit the number of sub-timesteps (and to limit the CPU-time), the minimum value for the particle timestep is defined by the package parameter [#dt_min_part dt_min_part].\\\\ |
| 551 | Setting '''use_sgs_for_particles''' = ''.T.'' automatically forces [../inipar#use_upstream_for_tke use_upstream_for_tke] = ''.T.''. This inhibits the occurrence of large (artificial) spatial gradients of the subgrid-scale TKE which otherwise would lead to wrong results for the particle advection. |
| 552 | }}} |