1ea10196cSJeremy L Thompson## libCEED: Navier-Stokes Example 2ea10196cSJeremy L Thompson 3ea10196cSJeremy L ThompsonThis page provides a description of the Navier-Stokes example for the libCEED library, based on PETSc. 4b9842f74SJeremy L ThompsonPETSc v3.17 or a development version of PETSc at commit 0e95d842 or later is required. 5ea10196cSJeremy L Thompson 6a515125bSLeila GhaffariThe Navier-Stokes problem solves the compressible Navier-Stokes equations in three dimensions using an explicit time integration. 7a515125bSLeila GhaffariThe state variables are mass density, momentum density, and energy density. 8ea10196cSJeremy L Thompson 9a515125bSLeila GhaffariThe main Navier-Stokes solver for libCEED is defined in [`navierstokes.c`](navierstokes.c) with different problem definitions according to the application of interest. 10ea10196cSJeremy L Thompson 11575f8106SLeila GhaffariBuild by using: 12ea10196cSJeremy L Thompson 13ea10196cSJeremy L Thompson`make` 14ea10196cSJeremy L Thompson 15575f8106SLeila Ghaffariand run with: 16ea10196cSJeremy L Thompson 17575f8106SLeila Ghaffari``` 18575f8106SLeila Ghaffari./navierstokes -ceed [ceed] -problem [problem type] -degree [degree] 19575f8106SLeila Ghaffari``` 20ea10196cSJeremy L Thompson 21575f8106SLeila Ghaffari## Runtime options 22ea10196cSJeremy L Thompson 23575f8106SLeila Ghaffari% inclusion-fluids-marker 24ea10196cSJeremy L Thompson 25575f8106SLeila GhaffariThe Navier-Stokes mini-app is controlled via command-line options. 26575f8106SLeila GhaffariThe following options are common among all problem types: 27ea10196cSJeremy L Thompson 28575f8106SLeila Ghaffari:::{list-table} Common Runtime Options 29575f8106SLeila Ghaffari:header-rows: 1 30ea10196cSJeremy L Thompson 31575f8106SLeila Ghaffari* - Option 32575f8106SLeila Ghaffari - Description 33575f8106SLeila Ghaffari - Default value 34ea10196cSJeremy L Thompson 35575f8106SLeila Ghaffari* - `-ceed` 36575f8106SLeila Ghaffari - CEED resource specifier 37575f8106SLeila Ghaffari - `/cpu/self/opt/blocked` 38ea10196cSJeremy L Thompson 39575f8106SLeila Ghaffari* - `-test` 40575f8106SLeila Ghaffari - Run in test mode 41575f8106SLeila Ghaffari - `false` 42ea10196cSJeremy L Thompson 43575f8106SLeila Ghaffari* - `-compare_final_state_atol` 44575f8106SLeila Ghaffari - Test absolute tolerance 45575f8106SLeila Ghaffari - `1E-11` 46ea10196cSJeremy L Thompson 47575f8106SLeila Ghaffari* - `-compare_final_state_filename` 48575f8106SLeila Ghaffari - Test filename 49575f8106SLeila Ghaffari - 50ea10196cSJeremy L Thompson 51575f8106SLeila Ghaffari* - `-problem` 52575f8106SLeila Ghaffari - Problem to solve (`advection`, `advection2d`, `density_current`, or `euler_vortex`) 53575f8106SLeila Ghaffari - `density_current` 54ea10196cSJeremy L Thompson 55575f8106SLeila Ghaffari* - `-implicit` 56575f8106SLeila Ghaffari - Use implicit time integartor formulation 57575f8106SLeila Ghaffari - 58ea10196cSJeremy L Thompson 59575f8106SLeila Ghaffari* - `-degree` 60575f8106SLeila Ghaffari - Polynomial degree of tensor product basis (must be >= 1) 61575f8106SLeila Ghaffari - `1` 62ea10196cSJeremy L Thompson 63c1680e98SJeremy L Thompson* - `-q_extra` 64575f8106SLeila Ghaffari - Number of extra quadrature points 65575f8106SLeila Ghaffari - `2` 66ea10196cSJeremy L Thompson 67575f8106SLeila Ghaffari* - `-viz_refine` 68575f8106SLeila Ghaffari - Use regular refinement for visualization 69575f8106SLeila Ghaffari - `0` 70ea10196cSJeremy L Thompson 71575f8106SLeila Ghaffari* - `-output_freq` 72575f8106SLeila Ghaffari - Frequency of output, in number of steps 73575f8106SLeila Ghaffari - `10` 74ea10196cSJeremy L Thompson 75575f8106SLeila Ghaffari* - `-continue` 76575f8106SLeila Ghaffari - Continue from previous solution 77575f8106SLeila Ghaffari - `0` 78ea10196cSJeremy L Thompson 79575f8106SLeila Ghaffari* - `-output_dir` 80575f8106SLeila Ghaffari - Output directory 81575f8106SLeila Ghaffari - `.` 82ea10196cSJeremy L Thompson 83f4277be3SLeila Ghaffari* - `-bc_wall` 84f4277be3SLeila Ghaffari - Use wall boundary conditions on this list of faces 85f4277be3SLeila Ghaffari - 86f4277be3SLeila Ghaffari 87f4277be3SLeila Ghaffari* - `-wall_comps` 88f4277be3SLeila Ghaffari - An array of constrained component numbers for wall BCs 89f4277be3SLeila Ghaffari - 90f4277be3SLeila Ghaffari 91f4277be3SLeila Ghaffari* - `-bc_slip_x` 92f4277be3SLeila Ghaffari - Use slip boundary conditions, for the x component, on this list of faces 93f4277be3SLeila Ghaffari - 94f4277be3SLeila Ghaffari 95f4277be3SLeila Ghaffari* - `-bc_slip_y` 96f4277be3SLeila Ghaffari - Use slip boundary conditions, for the y component, on this list of faces 97f4277be3SLeila Ghaffari - 98f4277be3SLeila Ghaffari 99f4277be3SLeila Ghaffari* - `-bc_slip_z` 100f4277be3SLeila Ghaffari - Use slip boundary conditions, for the z component, on this list of faces 101f4277be3SLeila Ghaffari - 102f4277be3SLeila Ghaffari 103f4277be3SLeila Ghaffari* - `-bc_inflow` 104f4277be3SLeila Ghaffari - Use inflow boundary conditions on this list of faces 105f4277be3SLeila Ghaffari - 106f4277be3SLeila Ghaffari 107f4277be3SLeila Ghaffari* - `-bc_outflow` 108f4277be3SLeila Ghaffari - Use outflow boundary conditions on this list of faces 109f4277be3SLeila Ghaffari - 1108ef11c93SLeila Ghaffari 111575f8106SLeila Ghaffari* - `-snes_view` 112575f8106SLeila Ghaffari - View PETSc `SNES` nonlinear solver configuration 113575f8106SLeila Ghaffari - 1148ef11c93SLeila Ghaffari 115575f8106SLeila Ghaffari* - `-log_view` 116575f8106SLeila Ghaffari - View PETSc performance log 117575f8106SLeila Ghaffari - 118ea10196cSJeremy L Thompson 119575f8106SLeila Ghaffari* - `-help` 120575f8106SLeila Ghaffari - View comprehensive information about run-time options 121575f8106SLeila Ghaffari - 122575f8106SLeila Ghaffari::: 123ea10196cSJeremy L Thompson 124f4277be3SLeila GhaffariFor the case of a square/cubic mesh, the list of face indices to be used with `-bc_wall`, `bc_inflow`, `bc_outflow` and/or `-bc_slip_x`, `-bc_slip_y`, and `-bc_slip_z` are: 125f4277be3SLeila Ghaffari 126*bb8a0c61SJames Wright:::{list-table} 2D Face ID Labels 127*bb8a0c61SJames Wright:header-rows: 1 128*bb8a0c61SJames Wright* - PETSc Face Name 129*bb8a0c61SJames Wright - Cartesian direction 130*bb8a0c61SJames Wright - Face ID 131*bb8a0c61SJames Wright 132*bb8a0c61SJames Wright* - faceMarkerBottom 133*bb8a0c61SJames Wright - -z 134*bb8a0c61SJames Wright - 1 135*bb8a0c61SJames Wright 136*bb8a0c61SJames Wright* - faceMarkerRight 137*bb8a0c61SJames Wright - +x 138*bb8a0c61SJames Wright - 2 139*bb8a0c61SJames Wright 140*bb8a0c61SJames Wright* - faceMarkerTop 141*bb8a0c61SJames Wright - +z 142*bb8a0c61SJames Wright - 3 143*bb8a0c61SJames Wright 144*bb8a0c61SJames Wright* - faceMarkerLeft 145*bb8a0c61SJames Wright - -x 146*bb8a0c61SJames Wright - 4 147*bb8a0c61SJames Wright::: 148*bb8a0c61SJames Wright 149*bb8a0c61SJames Wright:::{list-table} 2D Face ID Labels 150*bb8a0c61SJames Wright:header-rows: 1 151*bb8a0c61SJames Wright* - PETSc Face Name 152*bb8a0c61SJames Wright - Cartesian direction 153*bb8a0c61SJames Wright - Face ID 154*bb8a0c61SJames Wright 155*bb8a0c61SJames Wright* - faceMarkerBottom 156*bb8a0c61SJames Wright - -z 157*bb8a0c61SJames Wright - 1 158*bb8a0c61SJames Wright 159*bb8a0c61SJames Wright* - faceMarkerTop 160*bb8a0c61SJames Wright - +z 161*bb8a0c61SJames Wright - 2 162*bb8a0c61SJames Wright 163*bb8a0c61SJames Wright* - faceMarkerFront 164*bb8a0c61SJames Wright - -y 165*bb8a0c61SJames Wright - 3 166*bb8a0c61SJames Wright 167*bb8a0c61SJames Wright* - faceMarkerBack 168*bb8a0c61SJames Wright - +y 169*bb8a0c61SJames Wright - 4 170*bb8a0c61SJames Wright 171*bb8a0c61SJames Wright* - faceMarkerRight 172*bb8a0c61SJames Wright - +x 173*bb8a0c61SJames Wright - 5 174*bb8a0c61SJames Wright 175*bb8a0c61SJames Wright* - faceMarkerLeft 176*bb8a0c61SJames Wright - -x 177*bb8a0c61SJames Wright - 6 178*bb8a0c61SJames Wright::: 179f4277be3SLeila Ghaffari 180575f8106SLeila GhaffariFor the 2D advection problem, the following additional command-line options are available: 181ea10196cSJeremy L Thompson 182575f8106SLeila Ghaffari:::{list-table} Advection2D Runtime Options 183575f8106SLeila Ghaffari:header-rows: 1 1848ef11c93SLeila Ghaffari 185575f8106SLeila Ghaffari* - Option 186575f8106SLeila Ghaffari - Description 187575f8106SLeila Ghaffari - Default value 188575f8106SLeila Ghaffari - Unit 1898ef11c93SLeila Ghaffari 190575f8106SLeila Ghaffari* - `-rc` 191575f8106SLeila Ghaffari - Characteristic radius of thermal bubble 192575f8106SLeila Ghaffari - `1000` 193575f8106SLeila Ghaffari - `m` 1948ef11c93SLeila Ghaffari 195575f8106SLeila Ghaffari* - `-units_meter` 196575f8106SLeila Ghaffari - 1 meter in scaled length units 197575f8106SLeila Ghaffari - `1E-2` 198575f8106SLeila Ghaffari - 1998ef11c93SLeila Ghaffari 200575f8106SLeila Ghaffari* - `-units_second` 201575f8106SLeila Ghaffari - 1 second in scaled time units 202575f8106SLeila Ghaffari - `1E-2` 203575f8106SLeila Ghaffari - 2048ef11c93SLeila Ghaffari 205575f8106SLeila Ghaffari* - `-units_kilogram` 206575f8106SLeila Ghaffari - 1 kilogram in scaled mass units 207575f8106SLeila Ghaffari - `1E-6` 208575f8106SLeila Ghaffari - 209a515125bSLeila Ghaffari 210575f8106SLeila Ghaffari* - `-strong_form` 211575f8106SLeila Ghaffari - Strong (1) or weak/integrated by parts (0) residual 212575f8106SLeila Ghaffari - `0` 213575f8106SLeila Ghaffari - 214a515125bSLeila Ghaffari 215575f8106SLeila Ghaffari* - `-stab` 216575f8106SLeila Ghaffari - Stabilization method (`none`, `su`, or `supg`) 217575f8106SLeila Ghaffari - `none` 218575f8106SLeila Ghaffari - 219a515125bSLeila Ghaffari 220575f8106SLeila Ghaffari* - `-CtauS` 221575f8106SLeila Ghaffari - Scale coefficient for stabilization tau (nondimensional) 222575f8106SLeila Ghaffari - `0` 223575f8106SLeila Ghaffari - 224a515125bSLeila Ghaffari 225575f8106SLeila Ghaffari* - `-wind_type` 226575f8106SLeila Ghaffari - Wind type in Advection (`rotation` or `translation`) 227575f8106SLeila Ghaffari - `rotation` 228575f8106SLeila Ghaffari - 229a515125bSLeila Ghaffari 230575f8106SLeila Ghaffari* - `-wind_translation` 231575f8106SLeila Ghaffari - Constant wind vector when `-wind_type translation` 232575f8106SLeila Ghaffari - `1,0,0` 233575f8106SLeila Ghaffari - 2348ef11c93SLeila Ghaffari 235575f8106SLeila Ghaffari* - `-E_wind` 236575f8106SLeila Ghaffari - Total energy of inflow wind when `-wind_type translation` 237575f8106SLeila Ghaffari - `1E6` 238575f8106SLeila Ghaffari - `J` 239575f8106SLeila Ghaffari::: 240268c6924SLeila Ghaffari 241575f8106SLeila GhaffariAn example of the `rotation` mode can be run with: 242268c6924SLeila Ghaffari 243575f8106SLeila Ghaffari``` 244f4277be3SLeila 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 245575f8106SLeila Ghaffari``` 246268c6924SLeila Ghaffari 247575f8106SLeila Ghaffariand the `translation` mode with: 248268c6924SLeila Ghaffari 249575f8106SLeila Ghaffari``` 250f4277be3SLeila 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 251575f8106SLeila Ghaffari``` 252f4277be3SLeila GhaffariNote the lengths in `-dm_plex_box_upper` are given in meters, and will be nondimensionalized according to `-units_meter`. 253268c6924SLeila Ghaffari 254575f8106SLeila GhaffariFor the 3D advection problem, the following additional command-line options are available: 255268c6924SLeila Ghaffari 256575f8106SLeila Ghaffari:::{list-table} Advection3D Runtime Options 257575f8106SLeila Ghaffari:header-rows: 1 258268c6924SLeila Ghaffari 259575f8106SLeila Ghaffari* - Option 260575f8106SLeila Ghaffari - Description 261575f8106SLeila Ghaffari - Default value 262575f8106SLeila Ghaffari - Unit 263268c6924SLeila Ghaffari 264575f8106SLeila Ghaffari* - `-rc` 265575f8106SLeila Ghaffari - Characteristic radius of thermal bubble 266575f8106SLeila Ghaffari - `1000` 267575f8106SLeila Ghaffari - `m` 268268c6924SLeila Ghaffari 269575f8106SLeila Ghaffari* - `-units_meter` 270575f8106SLeila Ghaffari - 1 meter in scaled length units 271575f8106SLeila Ghaffari - `1E-2` 272575f8106SLeila Ghaffari - 273268c6924SLeila Ghaffari 274575f8106SLeila Ghaffari* - `-units_second` 275575f8106SLeila Ghaffari - 1 second in scaled time units 276575f8106SLeila Ghaffari - `1E-2` 277575f8106SLeila Ghaffari - 278268c6924SLeila Ghaffari 279575f8106SLeila Ghaffari* - `-units_kilogram` 280575f8106SLeila Ghaffari - 1 kilogram in scaled mass units 281575f8106SLeila Ghaffari - `1E-6` 282575f8106SLeila Ghaffari - 283268c6924SLeila Ghaffari 284575f8106SLeila Ghaffari* - `-strong_form` 285575f8106SLeila Ghaffari - Strong (1) or weak/integrated by parts (0) residual 286575f8106SLeila Ghaffari - `0` 287575f8106SLeila Ghaffari - 288268c6924SLeila Ghaffari 289575f8106SLeila Ghaffari* - `-stab` 290575f8106SLeila Ghaffari - Stabilization method (`none`, `su`, or `supg`) 291575f8106SLeila Ghaffari - `none` 292575f8106SLeila Ghaffari - 293268c6924SLeila Ghaffari 294575f8106SLeila Ghaffari* - `-CtauS` 295575f8106SLeila Ghaffari - Scale coefficient for stabilization tau (nondimensional) 296575f8106SLeila Ghaffari - `0` 297575f8106SLeila Ghaffari - 298268c6924SLeila Ghaffari 299575f8106SLeila Ghaffari* - `-wind_type` 300575f8106SLeila Ghaffari - Wind type in Advection (`rotation` or `translation`) 301575f8106SLeila Ghaffari - `rotation` 302575f8106SLeila Ghaffari - 303268c6924SLeila Ghaffari 304575f8106SLeila Ghaffari* - `-wind_translation` 305575f8106SLeila Ghaffari - Constant wind vector when `-wind_type translation` 306575f8106SLeila Ghaffari - `1,0,0` 307575f8106SLeila Ghaffari - 308268c6924SLeila Ghaffari 309575f8106SLeila Ghaffari* - `-E_wind` 310575f8106SLeila Ghaffari - Total energy of inflow wind when `-wind_type translation` 311575f8106SLeila Ghaffari - `1E6` 312575f8106SLeila Ghaffari - `J` 313268c6924SLeila Ghaffari 314575f8106SLeila Ghaffari* - `-bubble_type` 315575f8106SLeila Ghaffari - `sphere` (3D) or `cylinder` (2D) 316575f8106SLeila Ghaffari - `shpere` 317575f8106SLeila Ghaffari - 318268c6924SLeila Ghaffari 319575f8106SLeila Ghaffari* - `-bubble_continuity` 320575f8106SLeila Ghaffari - `smooth`, `back_sharp`, or `thick` 321575f8106SLeila Ghaffari - `smooth` 322575f8106SLeila Ghaffari - 323575f8106SLeila Ghaffari::: 324ea10196cSJeremy L Thompson 325575f8106SLeila GhaffariAn example of the `rotation` mode can be run with: 326ea10196cSJeremy L Thompson 327575f8106SLeila Ghaffari``` 328f4277be3SLeila 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 329575f8106SLeila Ghaffari``` 330ea10196cSJeremy L Thompson 331575f8106SLeila Ghaffariand the `translation` mode with: 332ea10196cSJeremy L Thompson 333575f8106SLeila Ghaffari``` 334f4277be3SLeila 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 335575f8106SLeila Ghaffari``` 336ea10196cSJeremy L Thompson 337575f8106SLeila GhaffariFor the Isentropic Vortex problem, the following additional command-line options are available: 338ea10196cSJeremy L Thompson 339575f8106SLeila Ghaffari:::{list-table} Isentropic Vortex Runtime Options 340575f8106SLeila Ghaffari:header-rows: 1 341ea10196cSJeremy L Thompson 342575f8106SLeila Ghaffari* - Option 343575f8106SLeila Ghaffari - Description 344575f8106SLeila Ghaffari - Default value 345575f8106SLeila Ghaffari - Unit 346ea10196cSJeremy L Thompson 347575f8106SLeila Ghaffari* - `-center` 348575f8106SLeila Ghaffari - Location of vortex center 349575f8106SLeila Ghaffari - `(lx,ly,lz)/2` 350575f8106SLeila Ghaffari - `(m,m,m)` 351ea10196cSJeremy L Thompson 352575f8106SLeila Ghaffari* - `-units_meter` 353575f8106SLeila Ghaffari - 1 meter in scaled length units 354575f8106SLeila Ghaffari - `1E-2` 355575f8106SLeila Ghaffari - 356ea10196cSJeremy L Thompson 357575f8106SLeila Ghaffari* - `-units_second` 358575f8106SLeila Ghaffari - 1 second in scaled time units 359575f8106SLeila Ghaffari - `1E-2` 360575f8106SLeila Ghaffari - 361ea10196cSJeremy L Thompson 362575f8106SLeila Ghaffari* - `-mean_velocity` 363575f8106SLeila Ghaffari - Background velocity vector 364575f8106SLeila Ghaffari - `(1,1,0)` 365575f8106SLeila Ghaffari - 366ea10196cSJeremy L Thompson 367575f8106SLeila Ghaffari* - `-vortex_strength` 368575f8106SLeila Ghaffari - Strength of vortex < 10 369575f8106SLeila Ghaffari - `5` 370575f8106SLeila Ghaffari - 371d8a22b9eSJed Brown 372d8a22b9eSJed Brown* - `-c_tau` 373d8a22b9eSJed Brown - Stabilization constant 374f821ee77SLeila Ghaffari - `0.5` 375d8a22b9eSJed Brown - 376575f8106SLeila Ghaffari::: 377ea10196cSJeremy L Thompson 378575f8106SLeila GhaffariThis problem can be run with: 379ea10196cSJeremy L Thompson 380575f8106SLeila Ghaffari``` 381f4277be3SLeila 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. 382575f8106SLeila Ghaffari``` 383ea10196cSJeremy L Thompson 384*bb8a0c61SJames WrightFor the Density Current, Channel, and Blasius problems, the following common command-line options are available: 385ea10196cSJeremy L Thompson 386*bb8a0c61SJames Wright:::{list-table} Newtonian Ideal Gas problems Runtime Options 387575f8106SLeila Ghaffari:header-rows: 1 388ea10196cSJeremy L Thompson 389575f8106SLeila Ghaffari* - Option 390575f8106SLeila Ghaffari - Description 391575f8106SLeila Ghaffari - Default value 392575f8106SLeila Ghaffari - Unit 393ea10196cSJeremy L Thompson 394575f8106SLeila Ghaffari* - `-units_meter` 395575f8106SLeila Ghaffari - 1 meter in scaled length units 396*bb8a0c61SJames Wright - `1` 397575f8106SLeila Ghaffari - 398ea10196cSJeremy L Thompson 399575f8106SLeila Ghaffari* - `-units_second` 400575f8106SLeila Ghaffari - 1 second in scaled time units 401*bb8a0c61SJames Wright - `1` 402575f8106SLeila Ghaffari - 403ea10196cSJeremy L Thompson 404575f8106SLeila Ghaffari* - `-units_kilogram` 405575f8106SLeila Ghaffari - 1 kilogram in scaled mass units 406*bb8a0c61SJames Wright - `1` 407575f8106SLeila Ghaffari - 408ea10196cSJeremy L Thompson 409575f8106SLeila Ghaffari* - `-units_Kelvin` 410575f8106SLeila Ghaffari - 1 Kelvin in scaled temperature units 411575f8106SLeila Ghaffari - `1` 412575f8106SLeila Ghaffari - 413ea10196cSJeremy L Thompson 414575f8106SLeila Ghaffari* - `-stab` 415575f8106SLeila Ghaffari - Stabilization method (`none`, `su`, or `supg`) 416575f8106SLeila Ghaffari - `none` 417575f8106SLeila Ghaffari - 418ea10196cSJeremy L Thompson 419d8a22b9eSJed Brown* - `-c_tau` 420*bb8a0c61SJames Wright - Stabilization constant, $c_\tau$ 421f821ee77SLeila Ghaffari - `0.5` 422d8a22b9eSJed Brown - 423d8a22b9eSJed Brown 424*bb8a0c61SJames Wright* - `-Ctau_t` 425*bb8a0c61SJames Wright - Stabilization time constant, $C_t$ 426*bb8a0c61SJames Wright - `1.0` 427*bb8a0c61SJames Wright - 428ea10196cSJeremy L Thompson 429*bb8a0c61SJames Wright* - `-Ctau_v` 430*bb8a0c61SJames Wright - Stabilization viscous constant, $C_v$ 431*bb8a0c61SJames Wright - `36.0` 432*bb8a0c61SJames Wright - 433ea10196cSJeremy L Thompson 434*bb8a0c61SJames Wright* - `-Ctau_C` 435*bb8a0c61SJames Wright - Stabilization continuity constant, $C_c$ 436*bb8a0c61SJames Wright - `1.0` 437*bb8a0c61SJames Wright - 438ea10196cSJeremy L Thompson 439*bb8a0c61SJames Wright* - `-Ctau_M` 440*bb8a0c61SJames Wright - Stabilization momentum constant, $C_m$ 441*bb8a0c61SJames Wright - `1.0` 442*bb8a0c61SJames Wright - 443*bb8a0c61SJames Wright 444*bb8a0c61SJames Wright* - `-Ctau_E` 445*bb8a0c61SJames Wright - Stabilization energy constant, $C_E$ 446*bb8a0c61SJames Wright - `1.0` 447*bb8a0c61SJames Wright - 448ea10196cSJeremy L Thompson 449575f8106SLeila Ghaffari* - `-cv` 450575f8106SLeila Ghaffari - Heat capacity at constant volume 451575f8106SLeila Ghaffari - `717` 452575f8106SLeila Ghaffari - `J/(kg K)` 453ea10196cSJeremy L Thompson 454575f8106SLeila Ghaffari* - `-cp` 455575f8106SLeila Ghaffari - Heat capacity at constant pressure 456575f8106SLeila Ghaffari - `1004` 457575f8106SLeila Ghaffari - `J/(kg K)` 458ea10196cSJeremy L Thompson 459575f8106SLeila Ghaffari* - `-g` 460575f8106SLeila Ghaffari - Gravitational acceleration 461575f8106SLeila Ghaffari - `9.81` 462575f8106SLeila Ghaffari - `m/s^2` 463ea10196cSJeremy L Thompson 464575f8106SLeila Ghaffari* - `-lambda` 465575f8106SLeila Ghaffari - Stokes hypothesis second viscosity coefficient 466575f8106SLeila Ghaffari - `-2/3` 467575f8106SLeila Ghaffari - 468ea10196cSJeremy L Thompson 469575f8106SLeila Ghaffari* - `-mu` 470575f8106SLeila Ghaffari - Shear dynamic viscosity coefficient 471575f8106SLeila Ghaffari - `75` 472575f8106SLeila Ghaffari - `Pa s` 473a515125bSLeila Ghaffari 474575f8106SLeila Ghaffari* - `-k` 475575f8106SLeila Ghaffari - Thermal conductivity 476575f8106SLeila Ghaffari - `0.02638` 477575f8106SLeila Ghaffari - `W/(m K)` 478575f8106SLeila Ghaffari::: 479a515125bSLeila Ghaffari 480*bb8a0c61SJames WrightThe Density Current problem the following command-line options are available in 481*bb8a0c61SJames Wrightaddition to the Newtonian Ideal Gas options: 482*bb8a0c61SJames Wright 483*bb8a0c61SJames Wright:::{list-table} Density Current Runtime Options 484*bb8a0c61SJames Wright:header-rows: 1 485*bb8a0c61SJames Wright 486*bb8a0c61SJames Wright* - Option 487*bb8a0c61SJames Wright - Description 488*bb8a0c61SJames Wright - Default value 489*bb8a0c61SJames Wright - Unit 490*bb8a0c61SJames Wright 491*bb8a0c61SJames Wright* - `-center` 492*bb8a0c61SJames Wright - Location of bubble center 493*bb8a0c61SJames Wright - `(lx,ly,lz)/2` 494*bb8a0c61SJames Wright - `(m,m,m)` 495*bb8a0c61SJames Wright 496*bb8a0c61SJames Wright* - `-dc_axis` 497*bb8a0c61SJames Wright - Axis of density current cylindrical anomaly, or `(0,0,0)` for spherically symmetric 498*bb8a0c61SJames Wright - `(0,0,0)` 499*bb8a0c61SJames Wright - 500*bb8a0c61SJames Wright 501*bb8a0c61SJames Wright* - `-rc` 502*bb8a0c61SJames Wright - Characteristic radius of thermal bubble 503*bb8a0c61SJames Wright - `1000` 504*bb8a0c61SJames Wright - `m` 505*bb8a0c61SJames Wright 506*bb8a0c61SJames Wright* - `-theta0` 507*bb8a0c61SJames Wright - Reference potential temperature 508*bb8a0c61SJames Wright - `300` 509*bb8a0c61SJames Wright - `K` 510*bb8a0c61SJames Wright 511*bb8a0c61SJames Wright* - `-thetaC` 512*bb8a0c61SJames Wright - Perturbation of potential temperature 513*bb8a0c61SJames Wright - `-15` 514*bb8a0c61SJames Wright - `K` 515*bb8a0c61SJames Wright 516*bb8a0c61SJames Wright* - `-P0` 517*bb8a0c61SJames Wright - Atmospheric pressure 518*bb8a0c61SJames Wright - `1E5` 519*bb8a0c61SJames Wright - `Pa` 520*bb8a0c61SJames Wright 521*bb8a0c61SJames Wright* - `-N` 522*bb8a0c61SJames Wright - Brunt-Vaisala frequency 523*bb8a0c61SJames Wright - `0.01` 524*bb8a0c61SJames Wright - `1/s` 525*bb8a0c61SJames Wright::: 526*bb8a0c61SJames Wright 527575f8106SLeila GhaffariThis problem can be run with: 528ea10196cSJeremy L Thompson 529575f8106SLeila Ghaffari``` 530*bb8a0c61SJames 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 75 531*bb8a0c61SJames Wright``` 532*bb8a0c61SJames Wright 533*bb8a0c61SJames WrightThe Channel problem the following command-line options are available in 534*bb8a0c61SJames Wrightaddition to the Newtonian Ideal Gas options: 535*bb8a0c61SJames Wright 536*bb8a0c61SJames Wright:::{list-table} Channel Runtime Options 537*bb8a0c61SJames Wright:header-rows: 1 538*bb8a0c61SJames Wright 539*bb8a0c61SJames Wright* - Option 540*bb8a0c61SJames Wright - Description 541*bb8a0c61SJames Wright - Default value 542*bb8a0c61SJames Wright - Unit 543*bb8a0c61SJames Wright 544*bb8a0c61SJames Wright* - `-umax` 545*bb8a0c61SJames Wright - Maximum/centerline velocity of the flow 546*bb8a0c61SJames Wright - `10` 547*bb8a0c61SJames Wright - `m/s` 548*bb8a0c61SJames Wright 549*bb8a0c61SJames Wright* - `-theta0` 550*bb8a0c61SJames Wright - Reference potential temperature 551*bb8a0c61SJames Wright - `300` 552*bb8a0c61SJames Wright - `K` 553*bb8a0c61SJames Wright 554*bb8a0c61SJames Wright* - `-P0` 555*bb8a0c61SJames Wright - Atmospheric pressure 556*bb8a0c61SJames Wright - `1E5` 557*bb8a0c61SJames Wright - `Pa` 558*bb8a0c61SJames Wright::: 559*bb8a0c61SJames Wright 560*bb8a0c61SJames WrightThis problem can be run with the `channel.yaml` file via: 561*bb8a0c61SJames Wright 562*bb8a0c61SJames Wright``` 563*bb8a0c61SJames Wright./navierstokes -options_file channel.yaml 564*bb8a0c61SJames Wright``` 565*bb8a0c61SJames Wright```{literalinclude} ../../../../../examples/fluids/channel.yaml 566*bb8a0c61SJames Wright:language: yaml 567*bb8a0c61SJames Wright``` 568*bb8a0c61SJames Wright 569*bb8a0c61SJames WrightThe Blasius problem the following command-line options are available in 570*bb8a0c61SJames Wrightaddition to the Newtonian Ideal Gas options: 571*bb8a0c61SJames Wright 572*bb8a0c61SJames Wright:::{list-table} Blasius Runtime Options 573*bb8a0c61SJames Wright:header-rows: 1 574*bb8a0c61SJames Wright 575*bb8a0c61SJames Wright* - Option 576*bb8a0c61SJames Wright - Description 577*bb8a0c61SJames Wright - Default value 578*bb8a0c61SJames Wright - Unit 579*bb8a0c61SJames Wright 580*bb8a0c61SJames Wright* - `-Uinf` 581*bb8a0c61SJames Wright - Freestream velocity 582*bb8a0c61SJames Wright - `40` 583*bb8a0c61SJames Wright - `m/s` 584*bb8a0c61SJames Wright 585*bb8a0c61SJames Wright* - `-delta0` 586*bb8a0c61SJames Wright - Boundary layer height at the inflow 587*bb8a0c61SJames Wright - `4.2e-4` 588*bb8a0c61SJames Wright - `m` 589*bb8a0c61SJames Wright 590*bb8a0c61SJames Wright* - `-theta0` 591*bb8a0c61SJames Wright - Reference potential temperature 592*bb8a0c61SJames Wright - `288` 593*bb8a0c61SJames Wright - `K` 594*bb8a0c61SJames Wright 595*bb8a0c61SJames Wright* - `-P0` 596*bb8a0c61SJames Wright - Atmospheric pressure 597*bb8a0c61SJames Wright - `1.01E5` 598*bb8a0c61SJames Wright - `Pa` 599*bb8a0c61SJames Wright 600*bb8a0c61SJames Wright* - `-refine_height` 601*bb8a0c61SJames Wright - Height at which `-Ndelta` number of elements should refined into 602*bb8a0c61SJames Wright - `5.9E-4` 603*bb8a0c61SJames Wright - `m` 604*bb8a0c61SJames Wright 605*bb8a0c61SJames Wright* - `-Ndelta` 606*bb8a0c61SJames Wright - Number of elements to keep below `-refine_height` 607*bb8a0c61SJames Wright - `45` 608*bb8a0c61SJames Wright - 609*bb8a0c61SJames Wright 610*bb8a0c61SJames Wright* - `-growth` 611*bb8a0c61SJames Wright - Growth rate of the elements in the refinement region 612*bb8a0c61SJames Wright - `1.08` 613*bb8a0c61SJames Wright - 614*bb8a0c61SJames Wright 615*bb8a0c61SJames Wright* - `-top_angle` 616*bb8a0c61SJames Wright - Downward angle of the top face of the domain. This face serves as an outlet. 617*bb8a0c61SJames Wright - `5` 618*bb8a0c61SJames Wright - `degrees` 619*bb8a0c61SJames Wright::: 620*bb8a0c61SJames Wright 621*bb8a0c61SJames WrightThis problem can be run with the `blasius.yaml` file via: 622*bb8a0c61SJames Wright 623*bb8a0c61SJames Wright``` 624*bb8a0c61SJames Wright./navierstokes -options_file blasius.yaml 625*bb8a0c61SJames Wright``` 626*bb8a0c61SJames Wright 627*bb8a0c61SJames Wright```{literalinclude} ../../../../../examples/fluids/blasius.yaml 628*bb8a0c61SJames Wright:language: yaml 629575f8106SLeila Ghaffari``` 630