- Timestamp:
- Jun 30, 2020 3:05:20 PM (4 years ago)
- File:
-
- 1 edited
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palm/trunk/SOURCE/lagrangian_particle_model_mod.f90
r4546 r4585 25 25 ! ----------------- 26 26 ! $Id$ 27 ! Limit logarithmically interpolated particle speed to the velocity component 28 ! at the first prognostic grid point (since no stability corrected interpolation 29 ! is employed the particle speed could be overestimated in unstable conditions). 30 ! 31 ! 4546 2020-05-24 12:16:41Z raasch 27 32 ! Variables iran and iran_part completely removed, added I/O of parallel random numbers to restart 28 33 ! file … … 3717 3722 !-- as sensitivity studies revealed no significant effect of 3718 3723 !-- using the neutral solution also for un/stable situations. 3724 !-- However, as the stability correction is missing the particle 3725 !-- speed may be overestimated compared to the velocity component 3726 !-- at the first prognostic grid point. Hence, the particle speed 3727 !-- is limited. 3719 3728 u_int(n) = -usws_int / ( us_int * kappa + 1E-10_wp ) & 3720 3729 * log_z_z0_int - u_gtrans 3730 3731 u_int(n) = SIGN( MIN( ABS( u_int(n) ), ABS( u(k_wall+1,jp,ip) ) ), u_int(n) ) 3732 3721 3733 ENDIF 3722 3734 ! … … 3812 3824 !-- as sensitivity studies revealed no significant effect of 3813 3825 !-- using the neutral solution also for un/stable situations. 3826 !-- However, as the stability correction is missing the particle 3827 !-- speed may be overestimated compared to the velocity component 3828 !-- at the first prognostic grid point. Hence, the particle speed 3829 !-- is limited. 3814 3830 v_int(n) = -vsws_int / ( us_int * kappa + 1E-10_wp ) & 3815 3831 * log_z_z0_int - v_gtrans 3832 3833 v_int(n) = SIGN( MIN( ABS( v_int(n) ), ABS( v(k_wall+1,jp,ip) ) ), v_int(n) ) 3816 3834 3817 3835 ENDIF
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