| 18 | |---------------- |
| 19 | {{{#!td style="vertical-align:top;width: 50px" |
| 20 | 14/07/17 |
| 21 | }}} |
| 22 | {{{#!td style="vertical-align:top;width: 50px" |
| 23 | FH |
| 24 | }}} |
| 25 | {{{#!td style="vertical-align:top;width: 75px" |
| 26 | r2312 |
| 27 | }}} |
| 28 | {{{#!td style="vertical-align:top" |
| 29 | 4.0 |
| 30 | }}} |
| 31 | {{{#!td style="vertical-align:top" |
| 32 | B, C |
| 33 | }}} |
| 34 | {{{#!td style="vertical-align:top" |
| 35 | Various improvements of the LCM (check_parameters.f90, data_output_ptseries.f90, lpm_droplet_collision.f90, lpm_droplet_condensation.f90, lpm_init.f90, lpm_read_restart_file.f90, microphysics_mod.f90, mod_particle_attributes.f90, package_parin.f90): |
| 36 | |
| 37 | (i) SGS particle motions are now possible if 'curvature_solution_effects = .TRUE.'. |
| 38 | |
| 39 | (ii) Initialization of aerosol spectra has been improved ([../../app/parpar#aero_type aero_type], [../../app/parpar#aero_weight aero_weight]). |
| 40 | |
| 41 | (iii) New, more stable Rosenbrock method for the numerical integration of the diffusional growth equation. |
| 42 | |
| 43 | (iv) Gas-kinetic effects are now considered in the diffusional growth equation. |
| 44 | |
| 45 | (v) Collision and coalescence now considers redistribution of aerosol mass. |
| 46 | |
| 47 | (vi) Collision and coalescence does not underestimate collisions if the timestep is too long. |
| 48 | }}} |