|
| | 523_higher-order-fd.create_scheme (name, solver) |
| | The numerical scheme, grid construction and plotter of one run.
|
| |
| | 523_higher-order-fd.build_and_run (name, directory, peano_installation, end_time) |
| | Generate, compile and run one setup within directory.
|
| |
| | 523_higher-order-fd.probe (directory, point, output_file) |
| | Probe all snapshots at one point.
|
| |
| | 523_higher-order-fd.profile (directory) |
| | Probe lapse and phi in the centre of each volume or grid cell along the line y=z=h/2, i.e.
|
| |
| | 523_higher-order-fd.radius (x) |
| |
| | 523_higher-order-fd.time_steps (directory) |
| | Number of time steps and average wall clock time per time step.
|
| |
| | 523_higher-order-fd.plot_over_time_and_profile (runs, names, file_name) |
| | Lapse next to the puncture over time (left) and along the x-axis at the last snapshot all runs share (right)
|
| |
| | 523_higher-order-fd.plot_fourier_analysis () |
| | Fourier analysis of the fourth-order central differences and of the Kreiss-Oliger dissipation.
|
| |
|
| | 523_higher-order-fd.Here = os.path.dirname(os.path.abspath(__file__)) |
| |
| | 523_higher-order-fd.PeanoRoot = os.path.abspath(os.path.join(Here, "..", "..", "..", "..")) |
| |
| str | 523_higher-order-fd.PatchFile = "solution-CCZ4.peano-patch-file" |
| |
| float | 523_higher-order-fd.Mass = 1.0 |
| |
| float | 523_higher-order-fd.DomainOffset = -9.0 |
| |
| float | 523_higher-order-fd.DomainSize = 18.0 |
| |
| int | 523_higher-order-fd.CellsPerAxis = 9 |
| |
| int | 523_higher-order-fd.PatchSize = 10 |
| |
| int | 523_higher-order-fd.VolumesPerAxis = CellsPerAxis * PatchSize |
| |
| float | 523_higher-order-fd.H = DomainSize / VolumesPerAxis |
| |
| int | 523_higher-order-fd.Threads = 4 |
| |
| float | 523_higher-order-fd.TimeInBetweenPlots = 0.5 |
| |
| | 523_higher-order-fd.DissipationSubset = list(range(0, 23)) + [53, 54] |
| | Unknowns which the restricted Kreiss-Oliger dissipation damps: Q0-Q22 (G, K, theta, Z, lapse, shift, b) and Q53-Q54 (traceK, phi)
|
| |
| dict | 523_higher-order-fd.Runs |
| | The runs: name -> (Kreiss-Oliger sigma or None, lopsided advection, quantities of the dissipation or None for all).
|
| |
| dict | 523_higher-order-fd.Style |
| | Colours, markers and labels per run, so all pictures use the same ones.
|
| |
| | 523_higher-order-fd.parser |
| |
| | 523_higher-order-fd.default |
| |
| | 523_higher-order-fd.help |
| |
| | 523_higher-order-fd.type |
| |
| | 523_higher-order-fd.float |
| |
| | 523_higher-order-fd.nargs |
| |
| | 523_higher-order-fd.args = parser.parse_args() |
| |
| | 523_higher-order-fd.work_directory |
| |
| dict | 523_higher-order-fd.runs = {} |
| |
| | 523_higher-order-fd.directory = os.path.join(os.path.abspath(work_directory), name) |
| |
| | 523_higher-order-fd.runtime |
| |
| | 523_higher-order-fd.success |
| |
| | 523_higher-order-fd.x |
| |
| | 523_higher-order-fd.t |
| |
| | 523_higher-order-fd.lapse |
| |
| | 523_higher-order-fd.phi |
| |
| int | 523_higher-order-fd.centre = VolumesPerAxis // 2 |
| |
| | 523_higher-order-fd.statistics = time_steps(directory) |
| |
| list | 523_higher-order-fd.ko_runs = [name for name in Style if name.startswith("fd4-ko") and name in runs] |
| |
| list | 523_higher-order-fd.lopsided_runs |
| |
1.9.8