343 | | [=#<insert_parameter_name> '''<insert_parameter_name>'''] |
344 | | }}} |
345 | | {{{#!td style="vertical-align:top" |
346 | | <insert type> |
347 | | }}} |
348 | | {{{#!td style="vertical-align:top" |
349 | | <insert value> |
350 | | }}} |
351 | | {{{#!td |
352 | | <insert explanation> |
353 | | }}} |
354 | | |---------------- |
355 | | {{{#!td style="vertical-align:top" |
356 | | [=#<insert_parameter_name> '''<insert_parameter_name>'''] |
357 | | }}} |
358 | | {{{#!td style="vertical-align:top" |
359 | | <insert type> |
360 | | }}} |
361 | | {{{#!td style="vertical-align:top" |
362 | | <insert value> |
363 | | }}} |
364 | | {{{#!td |
365 | | <insert explanation> |
366 | | }}} |
367 | | |---------------- |
368 | | {{{#!td style="vertical-align:top" |
369 | | [=#<insert_parameter_name> '''<insert_parameter_name>'''] |
370 | | }}} |
371 | | {{{#!td style="vertical-align:top" |
372 | | <insert type> |
373 | | }}} |
374 | | {{{#!td style="vertical-align:top" |
375 | | <insert value> |
376 | | }}} |
377 | | {{{#!td |
378 | | <insert explanation> |
379 | | }}} |
380 | | |---------------- |
381 | | {{{#!td style="vertical-align:top" |
382 | | [=#<insert_parameter_name> '''<insert_parameter_name>'''] |
383 | | }}} |
384 | | {{{#!td style="vertical-align:top" |
385 | | <insert type> |
386 | | }}} |
387 | | {{{#!td style="vertical-align:top" |
388 | | <insert value> |
389 | | }}} |
390 | | {{{#!td |
391 | | <insert explanation> |
392 | | }}} |
393 | | |---------------- |
394 | | {{{#!td style="vertical-align:top" |
395 | | [=#<insert_parameter_name> '''<insert_parameter_name>'''] |
396 | | }}} |
397 | | {{{#!td style="vertical-align:top" |
398 | | <insert type> |
399 | | }}} |
400 | | {{{#!td style="vertical-align:top" |
401 | | <insert value> |
402 | | }}} |
403 | | {{{#!td |
404 | | <insert explanation> |
| 343 | [=#u_bulk '''u_bulk'''] |
| 344 | }}} |
| 345 | {{{#!td style="vertical-align:top" |
| 346 | R |
| 347 | }}} |
| 348 | {{{#!td style="vertical-align:top" |
| 349 | 0.0 |
| 350 | }}} |
| 351 | {{{#!td |
| 352 | u-component of the predefined bulk velocity (in m/s).\\\\ |
| 353 | This parameter comes into effect if [#conserve_volume_flow conserve_volume_flow] = ''.T.'' and [#conserve_volume_flow_mode conserve_volume_flow_mode] = '' 'bulk_velocity'.'' |
| 354 | }}} |
| 355 | |---------------- |
| 356 | {{{#!td style="vertical-align:top" |
| 357 | [=#use_ug_for_galilei_tr '''use_ug_for_galilei_tr'''] |
| 358 | }}} |
| 359 | {{{#!td style="vertical-align:top" |
| 360 | L |
| 361 | }}} |
| 362 | {{{#!td style="vertical-align:top" |
| 363 | .T. |
| 364 | }}} |
| 365 | {{{#!td |
| 366 | Switch to determine the translation velocity in case that a Galilean transformation is used.\\\\ |
| 367 | In case of a Galilean transformation (see [#galilei_transformation galilei_transformation]), '''use_ug_for_galilei_tr''' = ''.T.'' ensures that the coordinate system is translated with the geostrophic windspeed.\\\\ |
| 368 | Alternatively, with '''use_ug_for_galilei_tr''' = ''.F.,'' the geostrophic wind can be replaced as translation speed by the (volume) averaged velocity. However, in this case the user must be aware of fast growing gravity waves, so this choice is usually not recommended! |
| 369 | }}} |
| 370 | |---------------- |
| 371 | {{{#!td style="vertical-align:top" |
| 372 | [=#v_bulk '''v_bulk'''] |
| 373 | }}} |
| 374 | {{{#!td style="vertical-align:top" |
| 375 | R |
| 376 | }}} |
| 377 | {{{#!td style="vertical-align:top" |
| 378 | 0.0 |
| 379 | }}} |
| 380 | {{{#!td |
| 381 | v-component of the predefined bulk velocity (in m/s). |
| 382 | |
| 383 | This parameter comes into effect if conserve_volume_flow = .T. and conserve_volume_flow_mode = 'bulk_velocity'. |
| 384 | }}} |
| 385 | |---------------- |
| 386 | {{{#!td style="vertical-align:top" |
| 387 | [=#ws_vertical_gradient '''ws_vertical_gradient'''] |
| 388 | }}} |
| 389 | {{{#!td style="vertical-align:top" |
| 390 | R(10) |
| 391 | }}} |
| 392 | {{{#!td style="vertical-align:top" |
| 393 | 10 * 0.0 |
| 394 | }}} |
| 395 | {{{#!td |
| 396 | Gradient(s) of the profile for the large scale subsidence/ascent velocity (in (m/s) / 100 m). |
| 397 | |
| 398 | This gradient holds starting from the height level defined by ws_vertical_gradient_level (precisely: for all uv levels k where zu(k) > ws_vertical_gradient_level, w_subs(k) is set: w_subs(k) = w_subs(k-1) + dzu(k) * ws_vertical_gradient) up to the top boundary or up to the next height level defined by ws_vertical_gradient_level. A total of 10 different gradients for 11 height intervals (10 intervals if ws_vertical_gradient_level(1) = 0.0) can be assigned. |
| 399 | |
| 400 | Example: |
| 401 | |
| 402 | ws_vertical_gradient = -0.002, 0.0, |
| 403 | ws_vertical_gradient_level = 0.0, 1000.0, |
| 404 | |
| 405 | That defines the subsidence/ascent profile to be linear up to z = 1000.0 m with a surface value of 0 m/s. For z > 1000.0 m up to the top boundary the gradient is 0.0 (m/s) / 100 m (it is assumed that the assigned height levels correspond with uv levels). |
| 406 | |
| 407 | With an appropriate construction of w_subs the height of the boundary layer z_i can be kept approximately constant. |
| 408 | |
| 409 | Attention: |
| 410 | The large scale vertical motion is only applied to the prognostic equation for the scalar quantities (potential temperature, humidity if humidity = .T. or passive scalar if passive_scalar = .T.) because it cannot be applied to the momentum equations due to incompressibility. Thus, the model is not mass consistent. |
| 411 | }}} |
| 412 | |---------------- |
| 413 | {{{#!td style="vertical-align:top" |
| 414 | [=#ws_vertical_gradient |
| 415 | _level '''ws_vertical_gradient |
| 416 | _level'''] |
| 417 | }}} |
| 418 | {{{#!td style="vertical-align:top" |
| 419 | R(10) |
| 420 | }}} |
| 421 | {{{#!td style="vertical-align:top" |
| 422 | 10 * 0.0 |
| 423 | }}} |
| 424 | {{{#!td |
| 425 | |
| 426 | |
| 427 | |
| 428 | Height level from which on the gradient for the subsidence/ascent velocity defined by ws_vertical_gradient is effective (in m). |
| 429 | |
| 430 | The height levels have to be assigned in ascending order. The default values result in a profile which is zero everywhere regardless of the values of ws_vertical_gradient. For the piecewise construction of the subsidence/ascent velocity profile see ws_vertical_gradient. |