| 13 | |---------------- |
| 14 | {{{#!td style="vertical-align:top;width: 50px" |
| 15 | 30/04/14 |
| 16 | }}} |
| 17 | {{{#!td style="vertical-align:top;width: 50px" |
| 18 | LB |
| 19 | }}} |
| 20 | {{{#!td style="vertical-align:top;width: 75px" |
| 21 | r1383 |
| 22 | }}} |
| 23 | {{{#!td style="vertical-align:top" |
| 24 | 3.10 |
| 25 | }}} |
| 26 | {{{#!td style="vertical-align:top" |
| 27 | C |
| 28 | }}} |
| 29 | {{{#!td style="vertical-align:top" |
| 30 | Renamed variables which store large scale forcing tendencies:\\ |
| 31 | pt_lsa -> td_lsa_lpt, pt_subs -> td_sub_lpt, q_lsa -> td_lsa_q, q_subs -> td_sub_q, high|lowpt_lsa -> high|low_td_lsa_lpt, ... (flow_statistics.f90, ls_forcing.f90, modules.f90) |
| 32 | |
| 33 | Neumann boundary conditions were added to the profile data output of large scale advection and large scale subsidence and nudging terms at nzt+1. (flow_statistics.f90, nudging.f90, subsidence.f90) |
| 34 | |
| 35 | The weighting factor that is used in the summation of nudging and subsidence tendencies for profile data output was changed from weight_pres to weight_substep. (nudging.f90, subsidence.f90) |
| 36 | }}} |