176 | | [=#<insert_parameter_name> '''<insert_parameter_name>'''] |
177 | | }}} |
178 | | {{{#!td style="vertical-align:top" |
179 | | <insert type> |
180 | | }}} |
181 | | {{{#!td style="vertical-align:top" |
182 | | <insert value> |
183 | | }}} |
184 | | {{{#!td |
185 | | <insert explanation> |
| 176 | [=#bc_ns '''bc_ns'''] |
| 177 | }}} |
| 178 | {{{#!td style="vertical-align:top" |
| 179 | C*20 |
| 180 | }}} |
| 181 | {{{#!td style="vertical-align:top" |
| 182 | 'cyclic' |
| 183 | }}} |
| 184 | {{{#!td |
| 185 | Boundary condition along y (for all quantities).\\\\ |
| 186 | By default, a cyclic boundary condition is used along y.\\\\ |
| 187 | '''bc_ns''' may also be assigned the values '' 'dirichlet/radiation' '' (inflow from rear ("north"), outflow to the front ("south")) or '' 'radiation/dirichlet' '' (inflow from front ("south"), outflow to the rear ("north")). This requires the multi-grid method to be used for solving the Poisson equation for perturbation pressure (see [../d3par#psolver psolver]) and it also requires cyclic boundary conditions along x (see |
| 188 | [#bc_lr bc_lr]).\\\\ |
| 189 | In case of these non-cyclic lateral boundaries, a Dirichlet condition is used at the inflow for all quantities (initial vertical profiles - see [#initializing_actions initializing_actions] - are fixed during the run) except u, to which a Neumann (zero gradient) condition is applied. At the outflow, a radiation condition is used for all velocity components, while a Neumann (zero gradient) condition is used for the scalars. For perturbation pressure Neumann (zero gradient) conditions are assumed both at the inflow and at the outflow.\\\\ |
| 190 | For further details regarding non-cyclic lateral boundary conditions see [#bc_lr bc_lr]. |