| | 952 | [=#residual_limit '''residual_limit'''] |
| | 953 | }}} |
| | 954 | {{{#!td style="vertical-align:top" |
| | 955 | R |
| | 956 | }}} |
| | 957 | {{{#!td style="vertical-align:top" |
| | 958 | 1.0E-6 |
| | 959 | }}} |
| | 960 | {{{#!td |
| | 961 | Largest residual permitted for the multi-grid scheme (in s^-2^m^-3^).\\\\ |
| | 962 | This is a parameter to steer the accuracy of the multi-grid scheme (see [#psolver psolver]). The assigned cycle (v- or w-cycle, see [#mg_cycles mg_cycles]) is passed through until the residual falls below the limit given by '''residual_limit'''. If this is not the case after 1000 cycles, the PALM aborts with a corresponding error message.\\\\ |
| | 963 | The reciprocal value of this parameter can be interpreted as a factor by the divergence of the provisional velocity field is approximately reduced after the multi-grid scheme has been applied (thus the default value causes a reduction of the divergence by approx. 6 orders of magnitude). |
| | 964 | }}} |
| | 965 | |---------------- |
| | 966 | {{{#!td style="vertical-align:top" |
| | 967 | [=#<insert_parameter_name> '''<insert_parameter_name>'''] |
| | 968 | }}} |
| | 969 | {{{#!td style="vertical-align:top" |
| | 970 | <insert type> |
| | 971 | }}} |
| | 972 | {{{#!td style="vertical-align:top" |
| | 973 | <insert value> |
| | 974 | }}} |
| | 975 | {{{#!td |
| | 976 | <insert explanation> |
| | 977 | }}} |
| | 978 | |---------------- |
| | 979 | {{{#!td style="vertical-align:top" |
| | 980 | [=#<insert_parameter_name> '''<insert_parameter_name>'''] |
| | 981 | }}} |
| | 982 | {{{#!td style="vertical-align:top" |
| | 983 | <insert type> |
| | 984 | }}} |
| | 985 | {{{#!td style="vertical-align:top" |
| | 986 | <insert value> |
| | 987 | }}} |
| | 988 | {{{#!td |
| | 989 | <insert explanation> |
| | 990 | }}} |
| | 991 | |---------------- |
| | 992 | {{{#!td style="vertical-align:top" |
| | 993 | [=#<insert_parameter_name> '''<insert_parameter_name>'''] |
| | 994 | }}} |
| | 995 | {{{#!td style="vertical-align:top" |
| | 996 | <insert type> |
| | 997 | }}} |
| | 998 | {{{#!td style="vertical-align:top" |
| | 999 | <insert value> |
| | 1000 | }}} |
| | 1001 | {{{#!td |
| | 1002 | <insert explanation> |
| | 1003 | }}} |
| | 1004 | |---------------- |
| | 1005 | {{{#!td style="vertical-align:top" |
| | 1006 | [=#<insert_parameter_name> '''<insert_parameter_name>'''] |
| | 1007 | }}} |
| | 1008 | {{{#!td style="vertical-align:top" |
| | 1009 | <insert type> |
| | 1010 | }}} |
| | 1011 | {{{#!td style="vertical-align:top" |
| | 1012 | <insert value> |
| | 1013 | }}} |
| | 1014 | {{{#!td |
| | 1015 | <insert explanation> |
| | 1016 | }}} |
| | 1017 | |---------------- |
| | 1018 | {{{#!td style="vertical-align:top" |
| | 1440 | }}} |
| | 1441 | |---------------- |
| | 1442 | {{{#!td style="vertical-align:top" |
| | 1443 | [=#recycling_width '''recycling_width'''] |
| | 1444 | }}} |
| | 1445 | {{{#!td style="vertical-align:top" |
| | 1446 | R |
| | 1447 | }}} |
| | 1448 | {{{#!td style="vertical-align:top" |
| | 1449 | 0.1 * [#nx nx] * [#dx dx] |
| | 1450 | }}} |
| | 1451 | {{{#!td |
| | 1452 | Distance of the recycling plane from the inflow boundary (in m).\\\\ |
| | 1453 | This parameter sets the horizontal extension (along the direction of the main flow) of the so-called recycling domain which is used to generate a turbulent inflow (see [#turbulent_inflow turbulent_inflow]). '''recycling_width''' must be larger than the grid spacing ([#dx dx]) and smaller than the length of the total domain ([#nx nx] * dx). |
| | 1454 | }}} |
| | 1455 | |---------------- |
| | 1456 | {{{#!td style="vertical-align:top" |
| | 1457 | [=#rif_max '''rif_max'''] |
| | 1458 | }}} |
| | 1459 | {{{#!td style="vertical-align:top" |
| | 1460 | R |
| | 1461 | }}} |
| | 1462 | {{{#!td style="vertical-align:top" |
| | 1463 | 1.0 |
| | 1464 | }}} |
| | 1465 | {{{#!td |
| | 1466 | Upper limit of the flux-Richardson number.\\\\ |
| | 1467 | With the Prandtl layer switched on (see [#prandtl_layer prandtl_layer]]), flux-Richardson numbers ('''rif''') are calculated for z=zp (k=1) in the 3d-model (in the [[1d-model]] for all heights). Their values in particular determine the values of the friction velocity (1d- and 3d-model) and the values of the eddy diffusivity (1d-model). With small wind velocities at the Prandtl layer top or small vertical wind shears in the 1d-model, '''rif''' can take up unrealistic large values. They are limited by an upper ('''rif_max''') and lower limit (see [#rif_min rif_min]) for the flux-Richardson number. The condition '''rif_max''' > rif_min must be met. |
| | 1468 | }}} |
| | 1469 | |---------------- |
| | 1470 | {{{#!td style="vertical-align:top" |
| | 1471 | [=#rif_min '''rif_min'''] |
| | 1472 | }}} |
| | 1473 | {{{#!td style="vertical-align:top" |
| | 1474 | R |
| | 1475 | }}} |
| | 1476 | {{{#!td style="vertical-align:top" |
| | 1477 | -5.0 |
| | 1478 | }}} |
| | 1479 | {{{#!td |
| | 1480 | Lower limit of the flux-Richardson number.\\\\ |
| | 1481 | For further explanations see [#rif_max rif_max]. The condition rif_max > '''rif_min''' must be met. |
| | 1482 | }}} |
| | 1483 | |---------------- |
| | 1484 | {{{#!td style="vertical-align:top" |
| | 1485 | [=#roughness_length '''roughness_length'''] |
| | 1486 | }}} |
| | 1487 | {{{#!td style="vertical-align:top" |
| | 1488 | R |
| | 1489 | }}} |
| | 1490 | {{{#!td style="vertical-align:top" |
| | 1491 | 0.1 |
| | 1492 | }}} |
| | 1493 | {{{#!td |
| | 1494 | Roughness length (in m).\\\\ |
| | 1495 | This parameter is effective only in case that a Prandtl layer is switched on (see [#prandtl_layer prandtl_layer]). |
| | 1496 | }}} |
| | 1497 | |---------------- |
| | 1498 | {{{#!td style="vertical-align:top" |
| | 1499 | [=#<insert_parameter_name> '''<insert_parameter_name>'''] |
| | 1500 | }}} |
| | 1501 | {{{#!td style="vertical-align:top" |
| | 1502 | <insert type> |
| | 1503 | }}} |
| | 1504 | {{{#!td style="vertical-align:top" |
| | 1505 | <insert value> |
| | 1506 | }}} |
| | 1507 | {{{#!td |
| | 1508 | <insert explanation> |