| 13 | |---------------- |
| 14 | {{{#!td style="vertical-align:top;width: 50px" |
| 15 | 07/04/16 |
| 16 | }}} |
| 17 | {{{#!td style="vertical-align:top;width: 50px" |
| 18 | FH |
| 19 | }}} |
| 20 | {{{#!td style="vertical-align:top;width: 75px" |
| 21 | r1822 |
| 22 | }}} |
| 23 | {{{#!td style="vertical-align:top" |
| 24 | 4.0 |
| 25 | }}} |
| 26 | {{{#!td style="vertical-align:top" |
| 27 | C, B |
| 28 | }}} |
| 29 | {{{#!td style="vertical-align:top" |
| 30 | '''Changed:''' |
| 31 | |
| 32 | * lpm_advec: turbulent velocity fluctuations can be used (use_sgs_for_particles), terminal velocity is computed from a parameterization by Rogers et al. (1993) |
| 33 | * lpm_droplet_collision: a new collision algorithm is available (collision_algorithm='all_or_nothing', 'average_impact' turns on the original algorithm) |
| 34 | * lpm_collision_kernel: the PALM kernel has been removed. Terminal velocities are also computed by the parameterization of Rogers et al. (1993) (analogously to lpm_advec) |
| 35 | * microphysics: Kessler bulk microphysics are not integrated in microphyics (i.e., calc_precipitation and impact_of_latent_heat are deleted). Microphysics can be steered via cloud_scheme with the following options: 'saturation_adjust' is a simple saturation adjustment scheme without precipitation, 'kessler' turns on the (one-moment) precipitation parametrization by Kessler (1996), 'seifert_beheng' the (two-moment) precipitation parameterization by Seifert and Beheng (2006). |
| 36 | * several routines of the LPM (Lagrangian particle model): Tails are now removed. |
| 37 | |
| 38 | '''Bugfixes:''' |
| 39 | |
| 40 | * Calculation of the turbulent enhancement factor of collection efficiency is corrected |
| 41 | }}} |