| 1138 | [=#rans_const_c '''rans_const_c'''] |
| 1139 | }}} |
| 1140 | {{{#!td style="vertical-align:top" |
| 1141 | R(5) |
| 1142 | }}} |
| 1143 | {{{#!td style="vertical-align:top" |
| 1144 | 0.55, 1.44, 1.92, 0.0, 0.0 |
| 1145 | }}} |
| 1146 | {{{#!td |
| 1147 | Model parameter used in the turbulence closure for RANS mode ([#rans_mode rans_mode] = ''.T.''). Constants are |
| 1148 | {{{ |
| 1149 | #!Latex |
| 1150 | \begin{align*} |
| 1151 | \mathrm{rans\_const\_c(0)} &= c_0\\ |
| 1152 | \mathrm{rans\_const\_c(1)} &= c_1\\ |
| 1153 | \mathrm{rans\_const\_c(2)} &= c_2\\ |
| 1154 | \mathrm{rans\_const\_c(3)} &= c_3\\ |
| 1155 | \mathrm{rans\_const\_c(4)} &= c_4\\ |
| 1156 | \end{align*} |
| 1157 | }}} |
| 1158 | Default values are according to the standard TKE-e turbulence closure (see [#turbulence_closure turbulence_closure]). |
| 1159 | }}} |
| 1160 | |---------------- |
| 1161 | {{{#!td style="vertical-align:top" |
| 1162 | [=#rans_const_sigma '''rans_const_sigma'''] |
| 1163 | }}} |
| 1164 | {{{#!td style="vertical-align:top" |
| 1165 | R(2) |
| 1166 | }}} |
| 1167 | {{{#!td style="vertical-align:top" |
| 1168 | 1.0, 1.3 |
| 1169 | }}} |
| 1170 | {{{#!td |
| 1171 | Model parameter used in the turbulence closure for RANS mode ([#rans_mode rans_mode] = ''.T.''). Constants are |
| 1172 | {{{ |
| 1173 | #!Latex |
| 1174 | \begin{align*} |
| 1175 | \mathrm{rans\_const\_sigma(1)} &= \sigma_e\\ |
| 1176 | \mathrm{rans\_const\_sigma(2)} &= \sigma_\epsilon. |
| 1177 | \end{align*} |
| 1178 | }}} |
| 1179 | Default values are according to the standard TKE-e turbulence closure (see [#turbulence_closure turbulence_closure]). |
| 1180 | }}} |
| 1181 | |---------------- |
| 1182 | {{{#!td style="vertical-align:top" |
| 1183 | [=#rans_mode '''rans_mode'''] |
| 1184 | }}} |
| 1185 | {{{#!td style="vertical-align:top" |
| 1186 | L |
| 1187 | }}} |
| 1188 | {{{#!td style="vertical-align:top" |
| 1189 | .F. |
| 1190 | }}} |
| 1191 | {{{#!td |
| 1192 | If **rans_mode** = ''.T.'', the Reynolds-averaged Navier-Stokes (RANS) equations are solved and turbulence is completely parameterized. The type of turbulence parameterization can be chosen via [#turbulence_closure turbulence_closure]. |
| 1193 | }}} |
| 1194 | |---------------- |
| 1195 | {{{#!td style="vertical-align:top" |
| 1319 | }}} |
| 1320 | |---------------- |
| 1321 | {{{#!td style="vertical-align:top" |
| 1322 | [=#turbulence_closure '''turbulence_closure'''] |
| 1323 | }}} |
| 1324 | {{{#!td style="vertical-align:top" |
| 1325 | C*20 |
| 1326 | }}} |
| 1327 | {{{#!td style="vertical-align:top" |
| 1328 | '' 'Moeng_Wyngaard' '' |
| 1329 | }}} |
| 1330 | {{{#!td |
| 1331 | Parameter to choose between different turbulence closures.\\\\ |
| 1332 | The following values are allowed:\\\\ |
| 1333 | '' 'Moeng_Wyngaard' ''\\\\ |
| 1334 | Turbulence closure according to a modified version of Deardorff's subgrid-scale model by Moeng and Wyngaard (1988). See details in the [wiki:doc/tec/sgs#Deardorffsubgrid-scalemodel documentation].\\ |
| 1335 | This option is only availably if [#rans_mode rans_mode]=**.F.**.\\\\ |
| 1336 | '' 'dynamic' ''\\\\ |
| 1337 | Use a dynamic subgrid-scale model according to Germano et al. (1991) and Heinz (2008). See details in the [wiki:doc/tec/sgs#Dynamicsubgrid-scalemodel documentation].\\ |
| 1338 | This option is only availably if [#rans_mode rans_mode]=**.F.**.\\\\ |
| 1339 | '' 'TKE-l' '' \\\\ |
| 1340 | Turbulence closure utilising the Prandtl-Kolmogorov relation. See details in the [wiki:/doc/tec/rans documentation].\\ |
| 1341 | This option is only availably if [#rans_mode rans_mode]=**.T.**.\\\\ |
| 1342 | '' 'TKE-e' '' \\\\ |
| 1343 | Standard TKE-e closure for Reynolds-averaged Navier-Stokes equations. The used constants can be changed using parameters [#rans_const_c rans_const_c] and [#rans_const_sigma rans_const_sigma]. See details in the [wiki:/doc/tec/rans documentation].\\ |
| 1344 | This option is only availably if [#rans_mode rans_mode]=**.T.**.\\\\ |