| | 191 | }}} |
| | 192 | |---------------- |
| | 193 | {{{#!td style="vertical-align:top" |
| | 194 | [=#bc_p_b '''bc_p_b'''] |
| | 195 | }}} |
| | 196 | {{{#!td style="vertical-align:top" |
| | 197 | C*20 |
| | 198 | }}} |
| | 199 | {{{#!td style="vertical-align:top" |
| | 200 | 'neumann' |
| | 201 | }}} |
| | 202 | {{{#!td |
| | 203 | Bottom boundary condition of the perturbation pressure.\\\\ |
| | 204 | Allowed values are '' 'dirichlet' '', '' 'neumann' '' and '' 'neumann+inhomo' ''. '' 'dirichlet' '' sets p(k=0)=0.0, '' 'neumann' '' sets p(k=0)=p(k=1). '' 'neumann+inhomo' '' corresponds to an extended Neumann boundary condition where heat flux or temperature inhomogeneities near the surface (pt(k=1)) are additionally regarded (see Shen and LeClerc (1995, Q.J.R. Meteorol. Soc., 1209)). This condition is only permitted with the Prandtl-layer switched on ([#prandtl_layer prandtl_layer]), otherwise the run is terminated.\\\\ |
| | 205 | Since at the bottom boundary of the model the vertical velocity disappears (w(k=0) = 0.0), the consistent Neumann condition ('' 'neumann' '' or '' 'neumann+inhomo' '') dp/dz = 0 should be used, which leaves the vertical component w unchanged when the pressure solver is applied. Simultaneous use of the Neumann boundary conditions both at the bottom and at the top boundary ([#bc_p_t bc_p_t]) usually yields no consistent solution for the perturbation pressure and should be avoided. |
| | 206 | }}} |
| | 207 | |---------------- |
| | 208 | {{{#!td style="vertical-align:top" |
| | 209 | [=#<insert_parameter_name> '''<insert_parameter_name>'''] |
| | 210 | }}} |
| | 211 | {{{#!td style="vertical-align:top" |
| | 212 | <insert type> |
| | 213 | }}} |
| | 214 | {{{#!td style="vertical-align:top" |
| | 215 | <insert value> |
| | 216 | }}} |
| | 217 | {{{#!td |
| | 218 | <insert explanation> |
| | 219 | }}} |
| | 220 | |---------------- |
| | 221 | {{{#!td style="vertical-align:top" |
| | 222 | [=#<insert_parameter_name> '''<insert_parameter_name>'''] |
| | 223 | }}} |
| | 224 | {{{#!td style="vertical-align:top" |
| | 225 | <insert type> |
| | 226 | }}} |
| | 227 | {{{#!td style="vertical-align:top" |
| | 228 | <insert value> |
| | 229 | }}} |
| | 230 | {{{#!td |
| | 231 | <insert explanation> |
| | 232 | }}} |
| | 233 | |---------------- |
| | 234 | {{{#!td style="vertical-align:top" |
| | 235 | [=#<insert_parameter_name> '''<insert_parameter_name>'''] |
| | 236 | }}} |
| | 237 | {{{#!td style="vertical-align:top" |
| | 238 | <insert type> |
| | 239 | }}} |
| | 240 | {{{#!td style="vertical-align:top" |
| | 241 | <insert value> |
| | 242 | }}} |
| | 243 | {{{#!td |
| | 244 | <insert explanation> |