xref: /libCEED/examples/fluids/README.md (revision fc14f3f6da76d04d40791c75bce6e7b0db0dbb7b)
1ccaff030SJeremy L Thompson## libCEED: Navier-Stokes Example
2ccaff030SJeremy L Thompson
3ccaff030SJeremy L ThompsonThis page provides a description of the Navier-Stokes example for the libCEED library, based on PETSc.
4b8962995SJeremy L ThompsonPETSc v3.17 or a development version of PETSc at commit 0e95d842 or later is required.
5ccaff030SJeremy L Thompson
677841947SLeila GhaffariThe Navier-Stokes problem solves the compressible Navier-Stokes equations in three dimensions using an explicit time integration.
777841947SLeila GhaffariThe state variables are mass density, momentum density, and energy density.
8ccaff030SJeremy L Thompson
977841947SLeila GhaffariThe main Navier-Stokes solver for libCEED is defined in [`navierstokes.c`](navierstokes.c) with different problem definitions according to the application of interest.
10ccaff030SJeremy L Thompson
11bc7bbd5dSLeila GhaffariBuild by using:
12ccaff030SJeremy L Thompson
13ccaff030SJeremy L Thompson`make`
14ccaff030SJeremy L Thompson
15bc7bbd5dSLeila Ghaffariand run with:
16ccaff030SJeremy L Thompson
17bc7bbd5dSLeila Ghaffari```
18bc7bbd5dSLeila Ghaffari./navierstokes -ceed [ceed] -problem [problem type] -degree [degree]
19bc7bbd5dSLeila Ghaffari```
20ccaff030SJeremy L Thompson
21bc7bbd5dSLeila Ghaffari## Runtime options
22ccaff030SJeremy L Thompson
23bc7bbd5dSLeila Ghaffari% inclusion-fluids-marker
24ccaff030SJeremy L Thompson
25bc7bbd5dSLeila GhaffariThe Navier-Stokes mini-app is controlled via command-line options.
26bc7bbd5dSLeila GhaffariThe following options are common among all problem types:
27ccaff030SJeremy L Thompson
28bc7bbd5dSLeila Ghaffari:::{list-table} Common Runtime Options
29bc7bbd5dSLeila Ghaffari:header-rows: 1
30ccaff030SJeremy L Thompson
31bc7bbd5dSLeila Ghaffari* - Option
32bc7bbd5dSLeila Ghaffari  - Description
33bc7bbd5dSLeila Ghaffari  - Default value
34ccaff030SJeremy L Thompson
35bc7bbd5dSLeila Ghaffari* - `-ceed`
36bc7bbd5dSLeila Ghaffari  - CEED resource specifier
37bc7bbd5dSLeila Ghaffari  - `/cpu/self/opt/blocked`
38ccaff030SJeremy L Thompson
39bc7bbd5dSLeila Ghaffari* - `-test`
40bc7bbd5dSLeila Ghaffari  - Run in test mode
41bc7bbd5dSLeila Ghaffari  - `false`
42ccaff030SJeremy L Thompson
43bc7bbd5dSLeila Ghaffari* - `-compare_final_state_atol`
44bc7bbd5dSLeila Ghaffari  - Test absolute tolerance
45bc7bbd5dSLeila Ghaffari  - `1E-11`
46ccaff030SJeremy L Thompson
47bc7bbd5dSLeila Ghaffari* - `-compare_final_state_filename`
48bc7bbd5dSLeila Ghaffari  - Test filename
49bc7bbd5dSLeila Ghaffari  -
50ccaff030SJeremy L Thompson
51bc7bbd5dSLeila Ghaffari* - `-problem`
52bc7bbd5dSLeila Ghaffari  - Problem to solve (`advection`, `advection2d`, `density_current`, or `euler_vortex`)
53bc7bbd5dSLeila Ghaffari  - `density_current`
54ccaff030SJeremy L Thompson
55bc7bbd5dSLeila Ghaffari* - `-implicit`
56bc7bbd5dSLeila Ghaffari  - Use implicit time integartor formulation
57bc7bbd5dSLeila Ghaffari  -
58ccaff030SJeremy L Thompson
59bc7bbd5dSLeila Ghaffari* - `-degree`
60bc7bbd5dSLeila Ghaffari  - Polynomial degree of tensor product basis (must be >= 1)
61bc7bbd5dSLeila Ghaffari  - `1`
62ccaff030SJeremy L Thompson
632288fb52SJeremy L Thompson* - `-q_extra`
64bc7bbd5dSLeila Ghaffari  - Number of extra quadrature points
65*fc14f3f6SLeila Ghaffari  - `0`
66ccaff030SJeremy L Thompson
67bc7bbd5dSLeila Ghaffari* - `-viz_refine`
68bc7bbd5dSLeila Ghaffari  - Use regular refinement for visualization
69bc7bbd5dSLeila Ghaffari  - `0`
70ccaff030SJeremy L Thompson
71bc7bbd5dSLeila Ghaffari* - `-output_freq`
720b22eb44SJames Wright  - Frequency of output, in number of steps. `0` has no output, `-1` outputs final state only
73bc7bbd5dSLeila Ghaffari  - `10`
74ccaff030SJeremy L Thompson
75bc7bbd5dSLeila Ghaffari* - `-output_dir`
76bc7bbd5dSLeila Ghaffari  - Output directory
77bc7bbd5dSLeila Ghaffari  - `.`
78ccaff030SJeremy L Thompson
7969293791SJames Wright* - `-output_add_stepnum2bin`
8069293791SJames Wright  - Whether to add step numbers to output binary files
8169293791SJames Wright  - `false`
8269293791SJames Wright
8369293791SJames Wright* - `-continue`
8469293791SJames Wright  - Continue from previous solution (input is step number of previous solution)
8569293791SJames Wright  - `0`
8669293791SJames Wright
8769293791SJames Wright* - `-continue_filename`
8869293791SJames Wright  - Path to solution binary file from which to continue from
8969293791SJames Wright  - `[output_dir]/ns-solution.bin`
9069293791SJames Wright
9169293791SJames Wright* - `-continue_time_filename`
9269293791SJames Wright  - Path to time stamp binary file from which to continue from
9369293791SJames Wright  - `[output_dir]/ns-time.bin`
9469293791SJames Wright
954534a52eSLeila Ghaffari* - `-bc_wall`
964534a52eSLeila Ghaffari  - Use wall boundary conditions on this list of faces
974534a52eSLeila Ghaffari  -
984534a52eSLeila Ghaffari
994534a52eSLeila Ghaffari* - `-wall_comps`
1004534a52eSLeila Ghaffari  - An array of constrained component numbers for wall BCs
1014534a52eSLeila Ghaffari  -
1024534a52eSLeila Ghaffari
1034534a52eSLeila Ghaffari* - `-bc_slip_x`
1044534a52eSLeila Ghaffari  - Use slip boundary conditions, for the x component, on this list of faces
1054534a52eSLeila Ghaffari  -
1064534a52eSLeila Ghaffari
1074534a52eSLeila Ghaffari* - `-bc_slip_y`
1084534a52eSLeila Ghaffari  - Use slip boundary conditions, for the y component, on this list of faces
1094534a52eSLeila Ghaffari  -
1104534a52eSLeila Ghaffari
1114534a52eSLeila Ghaffari* - `-bc_slip_z`
1124534a52eSLeila Ghaffari  - Use slip boundary conditions, for the z component, on this list of faces
1134534a52eSLeila Ghaffari  -
1144534a52eSLeila Ghaffari
1154534a52eSLeila Ghaffari* - `-bc_inflow`
1164534a52eSLeila Ghaffari  - Use inflow boundary conditions on this list of faces
1174534a52eSLeila Ghaffari  -
1184534a52eSLeila Ghaffari
1194534a52eSLeila Ghaffari* - `-bc_outflow`
1204534a52eSLeila Ghaffari  - Use outflow boundary conditions on this list of faces
1214534a52eSLeila Ghaffari  -
12289d0f5c0SLeila Ghaffari
1237ec884f8SJames Wright* - `-bc_freestream`
1247ec884f8SJames Wright  - Use freestream boundary conditions on this list of faces
1257ec884f8SJames Wright  -
1267ec884f8SJames Wright
127bc7bbd5dSLeila Ghaffari* - `-snes_view`
128bc7bbd5dSLeila Ghaffari  - View PETSc `SNES` nonlinear solver configuration
129bc7bbd5dSLeila Ghaffari  -
13089d0f5c0SLeila Ghaffari
131bc7bbd5dSLeila Ghaffari* - `-log_view`
132bc7bbd5dSLeila Ghaffari  - View PETSc performance log
133bc7bbd5dSLeila Ghaffari  -
134ccaff030SJeremy L Thompson
135bc7bbd5dSLeila Ghaffari* - `-help`
136bc7bbd5dSLeila Ghaffari  - View comprehensive information about run-time options
137bc7bbd5dSLeila Ghaffari  -
138bc7bbd5dSLeila Ghaffari:::
139ccaff030SJeremy L Thompson
1407ec884f8SJames WrightFor the case of a square/cubic mesh, the list of face indices to be used with `-bc_wall`, `bc_inflow`, `bc_outflow`, `bc_freestream`  and/or `-bc_slip_x`, `-bc_slip_y`, and `-bc_slip_z` are:
1414534a52eSLeila Ghaffari
14288626eedSJames Wright:::{list-table} 2D Face ID Labels
14388626eedSJames Wright:header-rows: 1
14488626eedSJames Wright* - PETSc Face Name
14588626eedSJames Wright  - Cartesian direction
14688626eedSJames Wright  - Face ID
14788626eedSJames Wright
14888626eedSJames Wright* - faceMarkerBottom
14988626eedSJames Wright  - -z
15088626eedSJames Wright  - 1
15188626eedSJames Wright
15288626eedSJames Wright* - faceMarkerRight
15388626eedSJames Wright  - +x
15488626eedSJames Wright  - 2
15588626eedSJames Wright
15688626eedSJames Wright* - faceMarkerTop
15788626eedSJames Wright  - +z
15888626eedSJames Wright  - 3
15988626eedSJames Wright
16088626eedSJames Wright* - faceMarkerLeft
16188626eedSJames Wright  - -x
16288626eedSJames Wright  - 4
16388626eedSJames Wright:::
16488626eedSJames Wright
16588626eedSJames Wright:::{list-table} 2D Face ID Labels
16688626eedSJames Wright:header-rows: 1
16788626eedSJames Wright* - PETSc Face Name
16888626eedSJames Wright  - Cartesian direction
16988626eedSJames Wright  - Face ID
17088626eedSJames Wright
17188626eedSJames Wright* - faceMarkerBottom
17288626eedSJames Wright  - -z
17388626eedSJames Wright  - 1
17488626eedSJames Wright
17588626eedSJames Wright* - faceMarkerTop
17688626eedSJames Wright  - +z
17788626eedSJames Wright  - 2
17888626eedSJames Wright
17988626eedSJames Wright* - faceMarkerFront
18088626eedSJames Wright  - -y
18188626eedSJames Wright  - 3
18288626eedSJames Wright
18388626eedSJames Wright* - faceMarkerBack
18488626eedSJames Wright  - +y
18588626eedSJames Wright  - 4
18688626eedSJames Wright
18788626eedSJames Wright* - faceMarkerRight
18888626eedSJames Wright  - +x
18988626eedSJames Wright  - 5
19088626eedSJames Wright
19188626eedSJames Wright* - faceMarkerLeft
19288626eedSJames Wright  - -x
19388626eedSJames Wright  - 6
19488626eedSJames Wright:::
1954534a52eSLeila Ghaffari
196019b7682STimothy Aiken### Advection
197019b7682STimothy Aiken
19817be3a41SJeremy L ThompsonFor testing purposes, there is a reduced mode for pure advection, which holds density $\rho$ and momentum density $\rho \bm u$ constant while advecting "total energy density" $E$.
19917be3a41SJeremy L ThompsonThese are available in 2D and 3D.
200019b7682STimothy Aiken
201019b7682STimothy Aiken#### 2D advection
202019b7682STimothy Aiken
203bc7bbd5dSLeila GhaffariFor the 2D advection problem, the following additional command-line options are available:
204ccaff030SJeremy L Thompson
205bc7bbd5dSLeila Ghaffari:::{list-table} Advection2D Runtime Options
206bc7bbd5dSLeila Ghaffari:header-rows: 1
20789d0f5c0SLeila Ghaffari
208bc7bbd5dSLeila Ghaffari* - Option
209bc7bbd5dSLeila Ghaffari  - Description
210bc7bbd5dSLeila Ghaffari  - Default value
211bc7bbd5dSLeila Ghaffari  - Unit
21289d0f5c0SLeila Ghaffari
213bc7bbd5dSLeila Ghaffari* - `-rc`
214bc7bbd5dSLeila Ghaffari  - Characteristic radius of thermal bubble
215bc7bbd5dSLeila Ghaffari  - `1000`
216bc7bbd5dSLeila Ghaffari  - `m`
21789d0f5c0SLeila Ghaffari
218bc7bbd5dSLeila Ghaffari* - `-units_meter`
219bc7bbd5dSLeila Ghaffari  - 1 meter in scaled length units
220bc7bbd5dSLeila Ghaffari  - `1E-2`
221bc7bbd5dSLeila Ghaffari  -
22289d0f5c0SLeila Ghaffari
223bc7bbd5dSLeila Ghaffari* - `-units_second`
224bc7bbd5dSLeila Ghaffari  - 1 second in scaled time units
225bc7bbd5dSLeila Ghaffari  - `1E-2`
226bc7bbd5dSLeila Ghaffari  -
22789d0f5c0SLeila Ghaffari
228bc7bbd5dSLeila Ghaffari* - `-units_kilogram`
229bc7bbd5dSLeila Ghaffari  - 1 kilogram in scaled mass units
230bc7bbd5dSLeila Ghaffari  - `1E-6`
231bc7bbd5dSLeila Ghaffari  -
23277841947SLeila Ghaffari
233bc7bbd5dSLeila Ghaffari* - `-strong_form`
234bc7bbd5dSLeila Ghaffari  - Strong (1) or weak/integrated by parts (0) residual
235bc7bbd5dSLeila Ghaffari  - `0`
236bc7bbd5dSLeila Ghaffari  -
23777841947SLeila Ghaffari
238bc7bbd5dSLeila Ghaffari* - `-stab`
239bc7bbd5dSLeila Ghaffari  - Stabilization method (`none`, `su`, or `supg`)
240bc7bbd5dSLeila Ghaffari  - `none`
241bc7bbd5dSLeila Ghaffari  -
24277841947SLeila Ghaffari
243bc7bbd5dSLeila Ghaffari* - `-CtauS`
244bc7bbd5dSLeila Ghaffari  - Scale coefficient for stabilization tau (nondimensional)
245bc7bbd5dSLeila Ghaffari  - `0`
246bc7bbd5dSLeila Ghaffari  -
24777841947SLeila Ghaffari
248bc7bbd5dSLeila Ghaffari* - `-wind_type`
249bc7bbd5dSLeila Ghaffari  - Wind type in Advection (`rotation` or `translation`)
250bc7bbd5dSLeila Ghaffari  - `rotation`
251bc7bbd5dSLeila Ghaffari  -
25277841947SLeila Ghaffari
253bc7bbd5dSLeila Ghaffari* - `-wind_translation`
254bc7bbd5dSLeila Ghaffari  - Constant wind vector when `-wind_type translation`
255bc7bbd5dSLeila Ghaffari  - `1,0,0`
256bc7bbd5dSLeila Ghaffari  -
25789d0f5c0SLeila Ghaffari
258bc7bbd5dSLeila Ghaffari* - `-E_wind`
259bc7bbd5dSLeila Ghaffari  - Total energy of inflow wind when `-wind_type translation`
260bc7bbd5dSLeila Ghaffari  - `1E6`
261bc7bbd5dSLeila Ghaffari  - `J`
262bc7bbd5dSLeila Ghaffari:::
263e43605a5SLeila Ghaffari
264bc7bbd5dSLeila GhaffariAn example of the `rotation` mode can be run with:
265e43605a5SLeila Ghaffari
266bc7bbd5dSLeila Ghaffari```
2674534a52eSLeila Ghaffari./navierstokes -problem advection2d -dm_plex_box_faces 20,20 -dm_plex_box_lower 0,0 -dm_plex_box_upper 1000,1000 -bc_wall 1,2,3,4 -wall_comps 4 -wind_type rotation -implicit -stab supg
268bc7bbd5dSLeila Ghaffari```
269e43605a5SLeila Ghaffari
270bc7bbd5dSLeila Ghaffariand the `translation` mode with:
271e43605a5SLeila Ghaffari
272bc7bbd5dSLeila Ghaffari```
2734534a52eSLeila Ghaffari./navierstokes -problem advection2d -dm_plex_box_faces 20,20 -dm_plex_box_lower 0,0 -dm_plex_box_upper 1000,1000 -units_meter 1e-4 -wind_type translation -wind_translation 1,-.5 -bc_inflow 1,2,3,4
274bc7bbd5dSLeila Ghaffari```
2754534a52eSLeila GhaffariNote the lengths in `-dm_plex_box_upper` are given in meters, and will be nondimensionalized according to `-units_meter`.
276e43605a5SLeila Ghaffari
277019b7682STimothy Aiken#### 3D advection
278019b7682STimothy Aiken
279bc7bbd5dSLeila GhaffariFor the 3D advection problem, the following additional command-line options are available:
280e43605a5SLeila Ghaffari
281bc7bbd5dSLeila Ghaffari:::{list-table} Advection3D Runtime Options
282bc7bbd5dSLeila Ghaffari:header-rows: 1
283e43605a5SLeila Ghaffari
284bc7bbd5dSLeila Ghaffari* - Option
285bc7bbd5dSLeila Ghaffari  - Description
286bc7bbd5dSLeila Ghaffari  - Default value
287bc7bbd5dSLeila Ghaffari  - Unit
288e43605a5SLeila Ghaffari
289bc7bbd5dSLeila Ghaffari* - `-rc`
290bc7bbd5dSLeila Ghaffari  - Characteristic radius of thermal bubble
291bc7bbd5dSLeila Ghaffari  - `1000`
292bc7bbd5dSLeila Ghaffari  - `m`
293e43605a5SLeila Ghaffari
294bc7bbd5dSLeila Ghaffari* - `-units_meter`
295bc7bbd5dSLeila Ghaffari  - 1 meter in scaled length units
296bc7bbd5dSLeila Ghaffari  - `1E-2`
297bc7bbd5dSLeila Ghaffari  -
298e43605a5SLeila Ghaffari
299bc7bbd5dSLeila Ghaffari* - `-units_second`
300bc7bbd5dSLeila Ghaffari  - 1 second in scaled time units
301bc7bbd5dSLeila Ghaffari  - `1E-2`
302bc7bbd5dSLeila Ghaffari  -
303e43605a5SLeila Ghaffari
304bc7bbd5dSLeila Ghaffari* - `-units_kilogram`
305bc7bbd5dSLeila Ghaffari  - 1 kilogram in scaled mass units
306bc7bbd5dSLeila Ghaffari  - `1E-6`
307bc7bbd5dSLeila Ghaffari  -
308e43605a5SLeila Ghaffari
309bc7bbd5dSLeila Ghaffari* - `-strong_form`
310bc7bbd5dSLeila Ghaffari  - Strong (1) or weak/integrated by parts (0) residual
311bc7bbd5dSLeila Ghaffari  - `0`
312bc7bbd5dSLeila Ghaffari  -
313e43605a5SLeila Ghaffari
314bc7bbd5dSLeila Ghaffari* - `-stab`
315bc7bbd5dSLeila Ghaffari  - Stabilization method (`none`, `su`, or `supg`)
316bc7bbd5dSLeila Ghaffari  - `none`
317bc7bbd5dSLeila Ghaffari  -
318e43605a5SLeila Ghaffari
319bc7bbd5dSLeila Ghaffari* - `-CtauS`
320bc7bbd5dSLeila Ghaffari  - Scale coefficient for stabilization tau (nondimensional)
321bc7bbd5dSLeila Ghaffari  - `0`
322bc7bbd5dSLeila Ghaffari  -
323e43605a5SLeila Ghaffari
324bc7bbd5dSLeila Ghaffari* - `-wind_type`
325bc7bbd5dSLeila Ghaffari  - Wind type in Advection (`rotation` or `translation`)
326bc7bbd5dSLeila Ghaffari  - `rotation`
327bc7bbd5dSLeila Ghaffari  -
328e43605a5SLeila Ghaffari
329bc7bbd5dSLeila Ghaffari* - `-wind_translation`
330bc7bbd5dSLeila Ghaffari  - Constant wind vector when `-wind_type translation`
331bc7bbd5dSLeila Ghaffari  - `1,0,0`
332bc7bbd5dSLeila Ghaffari  -
333e43605a5SLeila Ghaffari
334bc7bbd5dSLeila Ghaffari* - `-E_wind`
335bc7bbd5dSLeila Ghaffari  - Total energy of inflow wind when `-wind_type translation`
336bc7bbd5dSLeila Ghaffari  - `1E6`
337bc7bbd5dSLeila Ghaffari  - `J`
338e43605a5SLeila Ghaffari
339bc7bbd5dSLeila Ghaffari* - `-bubble_type`
340bc7bbd5dSLeila Ghaffari  - `sphere` (3D) or `cylinder` (2D)
341bc7bbd5dSLeila Ghaffari  - `shpere`
342bc7bbd5dSLeila Ghaffari  -
343e43605a5SLeila Ghaffari
344bc7bbd5dSLeila Ghaffari* - `-bubble_continuity`
345bc7bbd5dSLeila Ghaffari  - `smooth`, `back_sharp`, or `thick`
346bc7bbd5dSLeila Ghaffari  - `smooth`
347bc7bbd5dSLeila Ghaffari  -
348bc7bbd5dSLeila Ghaffari:::
349ccaff030SJeremy L Thompson
350bc7bbd5dSLeila GhaffariAn example of the `rotation` mode can be run with:
351ccaff030SJeremy L Thompson
352bc7bbd5dSLeila Ghaffari```
3534534a52eSLeila Ghaffari./navierstokes -problem advection -dm_plex_box_faces 10,10,10 -dm_plex_dim 3 -dm_plex_box_lower 0,0,0 -dm_plex_box_upper 8000,8000,8000 -bc_wall 1,2,3,4,5,6 -wall_comps 4 -wind_type rotation -implicit -stab su
354bc7bbd5dSLeila Ghaffari```
355ccaff030SJeremy L Thompson
356bc7bbd5dSLeila Ghaffariand the `translation` mode with:
357ccaff030SJeremy L Thompson
358bc7bbd5dSLeila Ghaffari```
3594534a52eSLeila Ghaffari./navierstokes -problem advection -dm_plex_box_faces 10,10,10 -dm_plex_dim 3 -dm_plex_box_lower 0,0,0 -dm_plex_box_upper 8000,8000,8000 -wind_type translation -wind_translation .5,-1,0 -bc_inflow 1,2,3,4,5,6
360bc7bbd5dSLeila Ghaffari```
361ccaff030SJeremy L Thompson
362019b7682STimothy Aiken### Inviscid Ideal Gas
363019b7682STimothy Aiken
364019b7682STimothy Aiken#### Isentropic Euler vortex
365019b7682STimothy Aiken
366bc7bbd5dSLeila GhaffariFor the Isentropic Vortex problem, the following additional command-line options are available:
367ccaff030SJeremy L Thompson
368bc7bbd5dSLeila Ghaffari:::{list-table} Isentropic Vortex Runtime Options
369bc7bbd5dSLeila Ghaffari:header-rows: 1
370ccaff030SJeremy L Thompson
371bc7bbd5dSLeila Ghaffari* - Option
372bc7bbd5dSLeila Ghaffari  - Description
373bc7bbd5dSLeila Ghaffari  - Default value
374bc7bbd5dSLeila Ghaffari  - Unit
375ccaff030SJeremy L Thompson
376bc7bbd5dSLeila Ghaffari* - `-center`
377bc7bbd5dSLeila Ghaffari  - Location of vortex center
378bc7bbd5dSLeila Ghaffari  - `(lx,ly,lz)/2`
379bc7bbd5dSLeila Ghaffari  - `(m,m,m)`
380ccaff030SJeremy L Thompson
381bc7bbd5dSLeila Ghaffari* - `-units_meter`
382bc7bbd5dSLeila Ghaffari  - 1 meter in scaled length units
383bc7bbd5dSLeila Ghaffari  - `1E-2`
384bc7bbd5dSLeila Ghaffari  -
385ccaff030SJeremy L Thompson
386bc7bbd5dSLeila Ghaffari* - `-units_second`
387bc7bbd5dSLeila Ghaffari  - 1 second in scaled time units
388bc7bbd5dSLeila Ghaffari  - `1E-2`
389bc7bbd5dSLeila Ghaffari  -
390ccaff030SJeremy L Thompson
391bc7bbd5dSLeila Ghaffari* - `-mean_velocity`
392bc7bbd5dSLeila Ghaffari  - Background velocity vector
393bc7bbd5dSLeila Ghaffari  - `(1,1,0)`
394bc7bbd5dSLeila Ghaffari  -
395ccaff030SJeremy L Thompson
396bc7bbd5dSLeila Ghaffari* - `-vortex_strength`
397bc7bbd5dSLeila Ghaffari  - Strength of vortex < 10
398bc7bbd5dSLeila Ghaffari  - `5`
399bc7bbd5dSLeila Ghaffari  -
400932417b3SJed Brown
401932417b3SJed Brown* - `-c_tau`
402932417b3SJed Brown  - Stabilization constant
403504dc8e0SLeila Ghaffari  - `0.5`
404932417b3SJed Brown  -
405bc7bbd5dSLeila Ghaffari:::
406ccaff030SJeremy L Thompson
407bc7bbd5dSLeila GhaffariThis problem can be run with:
408ccaff030SJeremy L Thompson
409bc7bbd5dSLeila Ghaffari```
4104534a52eSLeila Ghaffari./navierstokes -problem euler_vortex -dm_plex_box_faces 20,20,1 -dm_plex_box_lower 0,0,0 -dm_plex_box_upper 1000,1000,50 -dm_plex_dim 3 -bc_inflow 4,6 -bc_outflow 3,5 -bc_slip_z 1,2 -mean_velocity .5,-.8,0.
411bc7bbd5dSLeila Ghaffari```
412ccaff030SJeremy L Thompson
413019b7682STimothy Aiken#### Sod shock tube
414019b7682STimothy Aiken
415019b7682STimothy AikenFor the Shock Tube problem, the following additional command-line options are available:
416019b7682STimothy Aiken
417019b7682STimothy Aiken:::{list-table} Shock Tube Runtime Options
418019b7682STimothy Aiken:header-rows: 1
419019b7682STimothy Aiken
420019b7682STimothy Aiken* - Option
421019b7682STimothy Aiken  - Description
422019b7682STimothy Aiken  - Default value
423019b7682STimothy Aiken  - Unit
424019b7682STimothy Aiken
425019b7682STimothy Aiken* - `-units_meter`
426019b7682STimothy Aiken  - 1 meter in scaled length units
427019b7682STimothy Aiken  - `1E-2`
428019b7682STimothy Aiken  -
429019b7682STimothy Aiken
430019b7682STimothy Aiken* - `-units_second`
431019b7682STimothy Aiken  - 1 second in scaled time units
432019b7682STimothy Aiken  - `1E-2`
433019b7682STimothy Aiken  -
434019b7682STimothy Aiken
435019b7682STimothy Aiken* - `-yzb`
436019b7682STimothy Aiken  - Use YZB discontinuity capturing
437019b7682STimothy Aiken  - `none`
438019b7682STimothy Aiken  -
439019b7682STimothy Aiken
440019b7682STimothy Aiken* - `-stab`
441019b7682STimothy Aiken  - Stabilization method (`none`, `su`, or `supg`)
442019b7682STimothy Aiken  - `none`
443019b7682STimothy Aiken  -
444019b7682STimothy Aiken:::
445019b7682STimothy Aiken
446019b7682STimothy AikenThis problem can be run with:
447019b7682STimothy Aiken
448019b7682STimothy Aiken```
449019b7682STimothy Aiken./navierstokes -problem shocktube -yzb -stab su -bc_slip_z 3,4 -bc_slip_y 1,2 -bc_wall 5,6 -dm_plex_dim 3 -dm_plex_box_lower 0,0,0 -dm_plex_box_upper 1000,100,100 -dm_plex_box_faces 200,1,1 -units_second 0.1
450019b7682STimothy Aiken```
451019b7682STimothy Aiken
452019b7682STimothy Aiken### Newtonian viscosity, Ideal Gas
453019b7682STimothy Aiken
45488626eedSJames WrightFor the Density Current, Channel, and Blasius problems, the following common command-line options are available:
455ccaff030SJeremy L Thompson
45688626eedSJames Wright:::{list-table} Newtonian Ideal Gas problems Runtime Options
457bc7bbd5dSLeila Ghaffari:header-rows: 1
458ccaff030SJeremy L Thompson
459bc7bbd5dSLeila Ghaffari* - Option
460bc7bbd5dSLeila Ghaffari  - Description
461bc7bbd5dSLeila Ghaffari  - Default value
462bc7bbd5dSLeila Ghaffari  - Unit
463ccaff030SJeremy L Thompson
464bc7bbd5dSLeila Ghaffari* - `-units_meter`
465bc7bbd5dSLeila Ghaffari  - 1 meter in scaled length units
46688626eedSJames Wright  - `1`
467bc7bbd5dSLeila Ghaffari  -
468ccaff030SJeremy L Thompson
469bc7bbd5dSLeila Ghaffari* - `-units_second`
470bc7bbd5dSLeila Ghaffari  - 1 second in scaled time units
47188626eedSJames Wright  - `1`
472bc7bbd5dSLeila Ghaffari  -
473ccaff030SJeremy L Thompson
474bc7bbd5dSLeila Ghaffari* - `-units_kilogram`
475bc7bbd5dSLeila Ghaffari  - 1 kilogram in scaled mass units
47688626eedSJames Wright  - `1`
477bc7bbd5dSLeila Ghaffari  -
478ccaff030SJeremy L Thompson
479bc7bbd5dSLeila Ghaffari* - `-units_Kelvin`
480bc7bbd5dSLeila Ghaffari  - 1 Kelvin in scaled temperature units
481bc7bbd5dSLeila Ghaffari  - `1`
482bc7bbd5dSLeila Ghaffari  -
483ccaff030SJeremy L Thompson
484bc7bbd5dSLeila Ghaffari* - `-stab`
485bc7bbd5dSLeila Ghaffari  - Stabilization method (`none`, `su`, or `supg`)
486bc7bbd5dSLeila Ghaffari  - `none`
487bc7bbd5dSLeila Ghaffari  -
488ccaff030SJeremy L Thompson
489932417b3SJed Brown* - `-c_tau`
49088626eedSJames Wright  - Stabilization constant, $c_\tau$
491504dc8e0SLeila Ghaffari  - `0.5`
492932417b3SJed Brown  -
493932417b3SJed Brown
49488626eedSJames Wright* - `-Ctau_t`
49588626eedSJames Wright  - Stabilization time constant, $C_t$
49688626eedSJames Wright  - `1.0`
49788626eedSJames Wright  -
498ccaff030SJeremy L Thompson
49988626eedSJames Wright* - `-Ctau_v`
50088626eedSJames Wright  - Stabilization viscous constant, $C_v$
50194c01735SLeila Ghaffari  - `36, 60, 128 for degree = 1, 2, 3`
50288626eedSJames Wright  -
503ccaff030SJeremy L Thompson
50488626eedSJames Wright* - `-Ctau_C`
50588626eedSJames Wright  - Stabilization continuity constant, $C_c$
50688626eedSJames Wright  - `1.0`
50788626eedSJames Wright  -
508ccaff030SJeremy L Thompson
50988626eedSJames Wright* - `-Ctau_M`
51088626eedSJames Wright  - Stabilization momentum constant, $C_m$
51188626eedSJames Wright  - `1.0`
51288626eedSJames Wright  -
51388626eedSJames Wright
51488626eedSJames Wright* - `-Ctau_E`
51588626eedSJames Wright  - Stabilization energy constant, $C_E$
51688626eedSJames Wright  - `1.0`
51788626eedSJames Wright  -
518ccaff030SJeremy L Thompson
519bc7bbd5dSLeila Ghaffari* - `-cv`
520bc7bbd5dSLeila Ghaffari  - Heat capacity at constant volume
521bc7bbd5dSLeila Ghaffari  - `717`
522bc7bbd5dSLeila Ghaffari  - `J/(kg K)`
523ccaff030SJeremy L Thompson
524bc7bbd5dSLeila Ghaffari* - `-cp`
525bc7bbd5dSLeila Ghaffari  - Heat capacity at constant pressure
526bc7bbd5dSLeila Ghaffari  - `1004`
527bc7bbd5dSLeila Ghaffari  - `J/(kg K)`
528ccaff030SJeremy L Thompson
529bc7bbd5dSLeila Ghaffari* - `-g`
530bc7bbd5dSLeila Ghaffari  - Gravitational acceleration
531bc7bbd5dSLeila Ghaffari  - `9.81`
532bc7bbd5dSLeila Ghaffari  - `m/s^2`
533ccaff030SJeremy L Thompson
534bc7bbd5dSLeila Ghaffari* - `-lambda`
535bc7bbd5dSLeila Ghaffari  - Stokes hypothesis second viscosity coefficient
536bc7bbd5dSLeila Ghaffari  - `-2/3`
537bc7bbd5dSLeila Ghaffari  -
538ccaff030SJeremy L Thompson
539bc7bbd5dSLeila Ghaffari* - `-mu`
540bc7bbd5dSLeila Ghaffari  - Shear dynamic viscosity coefficient
541bc7bbd5dSLeila Ghaffari  - `75`
542bc7bbd5dSLeila Ghaffari  -  `Pa s`
54377841947SLeila Ghaffari
544bc7bbd5dSLeila Ghaffari* - `-k`
545bc7bbd5dSLeila Ghaffari  - Thermal conductivity
546bc7bbd5dSLeila Ghaffari  - `0.02638`
547bc7bbd5dSLeila Ghaffari  - `W/(m K)`
548a1df05f8SJed Brown
549a1df05f8SJed Brown* - `-newtonian_unit_tests`
550a1df05f8SJed Brown  - Developer option to test properties
551a1df05f8SJed Brown  - `false`
552a1df05f8SJed Brown  - boolean
553de2fdd78SJames Wright
5545c0afad3SJames Wright* - `-state_var`
5555c0afad3SJames Wright  - State variables to solve solution with. `conservative` ($\rho, \rho \bm{u}, \rho e$) or `primitive` ($P, \bm{u}, T$)
5565c0afad3SJames Wright  - `conservative`
5575c0afad3SJames Wright  - string
558bc7bbd5dSLeila Ghaffari:::
55977841947SLeila Ghaffari
5607ec884f8SJames Wright#### Newtonian Wave
5617ec884f8SJames Wright
562061ff11eSJames WrightThe newtonian wave problem has the following command-line options in addition to the Newtonian Ideal Gas options:
5637ec884f8SJames Wright
56489e3cb53SJames Wright:::{list-table} Newtonian Wave Runtime Options
5657ec884f8SJames Wright:header-rows: 1
5667ec884f8SJames Wright
5677ec884f8SJames Wright* - Option
5687ec884f8SJames Wright  - Description
5697ec884f8SJames Wright  - Default value
5707ec884f8SJames Wright  - Unit
5717ec884f8SJames Wright
572f1e435c9SJed Brown* - `-freestream_riemann`
573f1e435c9SJed Brown  - Riemann solver for boundaries (HLL or HLLC)
574f1e435c9SJed Brown  - `hllc`
575f1e435c9SJed Brown  -
576f1e435c9SJed Brown
577f1e435c9SJed Brown* - `-freestream_velocity`
5787ec884f8SJames Wright  - Freestream velocity vector
5797ec884f8SJames Wright  - `0,0,0`
5807ec884f8SJames Wright  - `m/s`
5817ec884f8SJames Wright
582f1e435c9SJed Brown* - `-freestream_temperature`
5837ec884f8SJames Wright  - Freestream temperature
5847ec884f8SJames Wright  - `288`
5857ec884f8SJames Wright  - `K`
5867ec884f8SJames Wright
587f1e435c9SJed Brown* - `-freestream_pressure`
58889e3cb53SJames Wright  - Freestream pressure
5897ec884f8SJames Wright  - `1.01e5`
5907ec884f8SJames Wright  - `Pa`
5917ec884f8SJames Wright
5927ec884f8SJames Wright* - `-epicenter`
5937ec884f8SJames Wright  - Coordinates of center of perturbation
5947ec884f8SJames Wright  - `0,0,0`
5957ec884f8SJames Wright  - `m`
5967ec884f8SJames Wright
5977ec884f8SJames Wright* - `-amplitude`
5987ec884f8SJames Wright  - Amplitude of the perturbation
5997ec884f8SJames Wright  - `0.1`
6007ec884f8SJames Wright  -
6017ec884f8SJames Wright
6027ec884f8SJames Wright* - `-width`
6037ec884f8SJames Wright  - Width parameter of the perturbation
6047ec884f8SJames Wright  - `0.002`
6057ec884f8SJames Wright  - `m`
6067ec884f8SJames Wright
6077ec884f8SJames Wright:::
6087ec884f8SJames Wright
6097ec884f8SJames WrightThis problem can be run with the `newtonianwave.yaml` file via:
6107ec884f8SJames Wright
6117ec884f8SJames Wright```
6127ec884f8SJames Wright./navierstokes -options_file newtonianwave.yaml
6137ec884f8SJames Wright```
6147ec884f8SJames Wright
6157ec884f8SJames Wright```{literalinclude} ../../../../../examples/fluids/newtonianwave.yaml
6167ec884f8SJames Wright:language: yaml
6177ec884f8SJames Wright```
618a1df05f8SJed Brown
619019b7682STimothy Aiken#### Density current
620019b7682STimothy Aiken
621061ff11eSJames WrightThe Density Current problem has the following command-line options in addition to the Newtonian Ideal Gas options:
62288626eedSJames Wright
62388626eedSJames Wright:::{list-table} Density Current Runtime Options
62488626eedSJames Wright:header-rows: 1
62588626eedSJames Wright
62688626eedSJames Wright* - Option
62788626eedSJames Wright  - Description
62888626eedSJames Wright  - Default value
62988626eedSJames Wright  - Unit
63088626eedSJames Wright
63188626eedSJames Wright* - `-center`
63288626eedSJames Wright  - Location of bubble center
63388626eedSJames Wright  - `(lx,ly,lz)/2`
63488626eedSJames Wright  - `(m,m,m)`
63588626eedSJames Wright
63688626eedSJames Wright* - `-dc_axis`
63788626eedSJames Wright  - Axis of density current cylindrical anomaly, or `(0,0,0)` for spherically symmetric
63888626eedSJames Wright  - `(0,0,0)`
63988626eedSJames Wright  -
64088626eedSJames Wright
64188626eedSJames Wright* - `-rc`
64288626eedSJames Wright  - Characteristic radius of thermal bubble
64388626eedSJames Wright  - `1000`
64488626eedSJames Wright  - `m`
64588626eedSJames Wright
64688626eedSJames Wright* - `-theta0`
64788626eedSJames Wright  - Reference potential temperature
64888626eedSJames Wright  - `300`
64988626eedSJames Wright  - `K`
65088626eedSJames Wright
65188626eedSJames Wright* - `-thetaC`
65288626eedSJames Wright  - Perturbation of potential temperature
65388626eedSJames Wright  - `-15`
65488626eedSJames Wright  - `K`
65588626eedSJames Wright
65688626eedSJames Wright* - `-P0`
65788626eedSJames Wright  - Atmospheric pressure
65888626eedSJames Wright  - `1E5`
65988626eedSJames Wright  - `Pa`
66088626eedSJames Wright
66188626eedSJames Wright* - `-N`
66288626eedSJames Wright  - Brunt-Vaisala frequency
66388626eedSJames Wright  - `0.01`
66488626eedSJames Wright  - `1/s`
66588626eedSJames Wright:::
66688626eedSJames Wright
667bc7bbd5dSLeila GhaffariThis problem can be run with:
668ccaff030SJeremy L Thompson
669bc7bbd5dSLeila Ghaffari```
67088626eedSJames Wright./navierstokes -problem density_current -dm_plex_box_faces 16,1,8 -degree 1 -dm_plex_box_lower 0,0,0 -dm_plex_box_upper 2000,125,1000 -dm_plex_dim 3 -rc 400. -bc_wall 1,2,5,6 -wall_comps 1,2,3 -bc_slip_y 3,4 -mu 75
67188626eedSJames Wright```
67288626eedSJames Wright
673019b7682STimothy Aiken#### Channel flow
674019b7682STimothy Aiken
675061ff11eSJames WrightThe Channel problem has the following command-line options in addition to the Newtonian Ideal Gas options:
67688626eedSJames Wright
67788626eedSJames Wright:::{list-table} Channel Runtime Options
67888626eedSJames Wright:header-rows: 1
67988626eedSJames Wright
68088626eedSJames Wright* - Option
68188626eedSJames Wright  - Description
68288626eedSJames Wright  - Default value
68388626eedSJames Wright  - Unit
68488626eedSJames Wright
68588626eedSJames Wright* - `-umax`
68688626eedSJames Wright  - Maximum/centerline velocity of the flow
68788626eedSJames Wright  - `10`
68888626eedSJames Wright  - `m/s`
68988626eedSJames Wright
69088626eedSJames Wright* - `-theta0`
69188626eedSJames Wright  - Reference potential temperature
69288626eedSJames Wright  - `300`
69388626eedSJames Wright  - `K`
69488626eedSJames Wright
69588626eedSJames Wright* - `-P0`
69688626eedSJames Wright  - Atmospheric pressure
69788626eedSJames Wright  - `1E5`
69888626eedSJames Wright  - `Pa`
699a1df05f8SJed Brown
700a1df05f8SJed Brown* - `-body_force_scale`
701a1df05f8SJed Brown  - Multiplier for body force (`-1` for flow reversal)
702a1df05f8SJed Brown  - 1
703a1df05f8SJed Brown  -
70488626eedSJames Wright:::
70588626eedSJames Wright
70688626eedSJames WrightThis problem can be run with the `channel.yaml` file via:
70788626eedSJames Wright
70888626eedSJames Wright```
70988626eedSJames Wright./navierstokes -options_file channel.yaml
71088626eedSJames Wright```
71188626eedSJames Wright```{literalinclude} ../../../../../examples/fluids/channel.yaml
71288626eedSJames Wright:language: yaml
71388626eedSJames Wright```
71488626eedSJames Wright
715019b7682STimothy Aiken#### Blasius boundary layer
716019b7682STimothy Aiken
717061ff11eSJames WrightThe Blasius problem has the following command-line options in addition to the Newtonian Ideal Gas options:
71888626eedSJames Wright
71988626eedSJames Wright:::{list-table} Blasius Runtime Options
72088626eedSJames Wright:header-rows: 1
72188626eedSJames Wright
72288626eedSJames Wright* - Option
72388626eedSJames Wright  - Description
72488626eedSJames Wright  - Default value
72588626eedSJames Wright  - Unit
72688626eedSJames Wright
727fb455ff0SLeila Ghaffari* - `-velocity_infinity`
72888626eedSJames Wright  - Freestream velocity
72988626eedSJames Wright  - `40`
73088626eedSJames Wright  - `m/s`
73188626eedSJames Wright
732fb455ff0SLeila Ghaffari* - `-temperature_infinity`
733fb455ff0SLeila Ghaffari  - Freestream temperature
73488626eedSJames Wright  - `288`
73588626eedSJames Wright  - `K`
73688626eedSJames Wright
737fb455ff0SLeila Ghaffari* - `-temperature_wall`
738fb455ff0SLeila Ghaffari  - Wall temperature
73907d14e58SLeila Ghaffari  - `288`
740fb455ff0SLeila Ghaffari  - `K`
741fb455ff0SLeila Ghaffari
742fb455ff0SLeila Ghaffari* - `-delta0`
743fb455ff0SLeila Ghaffari  - Boundary layer height at the inflow
744fb455ff0SLeila Ghaffari  - `4.2e-3`
745fb455ff0SLeila Ghaffari  - `m`
746fb455ff0SLeila Ghaffari
74788626eedSJames Wright* - `-P0`
74888626eedSJames Wright  - Atmospheric pressure
74988626eedSJames Wright  - `1.01E5`
75088626eedSJames Wright  - `Pa`
75188626eedSJames Wright
75291eaef80SJames Wright* - `-platemesh_refine_height`
75391eaef80SJames Wright  - Height at which `-platemesh_Ndelta` number of elements should refined into
75488626eedSJames Wright  - `5.9E-4`
75588626eedSJames Wright  - `m`
75688626eedSJames Wright
75791eaef80SJames Wright* - `-platemesh_Ndelta`
75891eaef80SJames Wright  - Number of elements to keep below `-platemesh_refine_height`
75988626eedSJames Wright  - `45`
76088626eedSJames Wright  -
76188626eedSJames Wright
76291eaef80SJames Wright* - `-platemesh_growth`
76388626eedSJames Wright  - Growth rate of the elements in the refinement region
76488626eedSJames Wright  - `1.08`
76588626eedSJames Wright  -
76688626eedSJames Wright
76791eaef80SJames Wright* - `-platemesh_top_angle`
76888626eedSJames Wright  - Downward angle of the top face of the domain. This face serves as an outlet.
76988626eedSJames Wright  - `5`
77088626eedSJames Wright  - `degrees`
771ba6664aeSJames Wright
772ba6664aeSJames Wright* - `-stg_use`
773ba6664aeSJames Wright  - Whether to use stg for the inflow conditions
774ba6664aeSJames Wright  - `false`
775ba6664aeSJames Wright  -
77691eaef80SJames Wright
77791eaef80SJames Wright* - `-platemesh_y_node_locs_path`
77891eaef80SJames Wright  - Path to file with y node locations. If empty, will use mesh warping instead.
77991eaef80SJames Wright  - `""`
78091eaef80SJames Wright  -
781fb455ff0SLeila Ghaffari
78207d14e58SLeila Ghaffari* - `-n_chebyshev`
783fb455ff0SLeila Ghaffari  - Number of Chebyshev terms
784fb455ff0SLeila Ghaffari  - `20`
785fb455ff0SLeila Ghaffari  -
786fb455ff0SLeila Ghaffari
78707d14e58SLeila Ghaffari* - `-chebyshev_`
78807d14e58SLeila Ghaffari  - Prefix for Chebyshev snes solve
78907d14e58SLeila Ghaffari  -
79007d14e58SLeila Ghaffari  -
79107d14e58SLeila Ghaffari
79288626eedSJames Wright:::
79388626eedSJames Wright
79488626eedSJames WrightThis problem can be run with the `blasius.yaml` file via:
79588626eedSJames Wright
79688626eedSJames Wright```
79788626eedSJames Wright./navierstokes -options_file blasius.yaml
79888626eedSJames Wright```
79988626eedSJames Wright
80088626eedSJames Wright```{literalinclude} ../../../../../examples/fluids/blasius.yaml
80188626eedSJames Wright:language: yaml
802bc7bbd5dSLeila Ghaffari```
803ba6664aeSJames Wright
804ba6664aeSJames Wright#### STG Inflow for Flat Plate
805ba6664aeSJames Wright
80617be3a41SJeremy L ThompsonUsing the STG Inflow for the blasius problem adds the following command-line options:
807ba6664aeSJames Wright
808ba6664aeSJames Wright:::{list-table} Blasius Runtime Options
809ba6664aeSJames Wright:header-rows: 1
810ba6664aeSJames Wright
811ba6664aeSJames Wright* - Option
812ba6664aeSJames Wright  - Description
813ba6664aeSJames Wright  - Default value
814ba6664aeSJames Wright  - Unit
815ba6664aeSJames Wright
816ba6664aeSJames Wright* - `-stg_inflow_path`
817ba6664aeSJames Wright  - Path to the STGInflow file
818ba6664aeSJames Wright  - `./STGInflow.dat`
819ba6664aeSJames Wright  -
820ba6664aeSJames Wright
821ba6664aeSJames Wright* - `-stg_rand_path`
822ba6664aeSJames Wright  - Path to the STGRand file
823ba6664aeSJames Wright  - `./STGRand.dat`
824ba6664aeSJames Wright  -
825ba6664aeSJames Wright
826ba6664aeSJames Wright* - `-stg_alpha`
827ba6664aeSJames Wright  - Growth rate of the wavemodes
828ba6664aeSJames Wright  - `1.01`
829ba6664aeSJames Wright  -
830ba6664aeSJames Wright
831ba6664aeSJames Wright* - `-stg_u0`
832ba6664aeSJames Wright  - Convective velocity, $U_0$
833ba6664aeSJames Wright  - `0.0`
834ba6664aeSJames Wright  - `m/s`
835ba6664aeSJames Wright
836ba6664aeSJames Wright* - `-stg_mean_only`
837ba6664aeSJames Wright  - Only impose the mean velocity (no fluctutations)
838ba6664aeSJames Wright  - `false`
839ba6664aeSJames Wright  -
840ba6664aeSJames Wright
84130af3636SJames Wright* - `-stg_strong`
84230af3636SJames Wright  - Strongly enforce the STG inflow boundary condition
84330af3636SJames Wright  - `false`
84430af3636SJames Wright  -
84530af3636SJames Wright
84689060322SJames Wright* - `-stg_fluctuating_IC`
84789060322SJames Wright  - "Extrude" the fluctuations through the domain as an initial condition
84889060322SJames Wright  - `false`
84989060322SJames Wright  -
85089060322SJames Wright
851ba6664aeSJames Wright:::
852ba6664aeSJames Wright
853ba6664aeSJames WrightThis problem can be run with the `blasius.yaml` file via:
854ba6664aeSJames Wright
855ba6664aeSJames Wright```
856ba6664aeSJames Wright./navierstokes -options_file blasius.yaml -stg_use true
857ba6664aeSJames Wright```
858ba6664aeSJames Wright
85917be3a41SJeremy L ThompsonNote the added `-stg_use true` flag
86017be3a41SJeremy L ThompsonThis overrides the `stg: use: false` setting in the `blasius.yaml` file, enabling the use of the STG inflow.
861