Releases: python-hydro/pyro2
pyro 4.4.0
4.4.0
-
the gresho problem (compressible) now takes Mach number as input
instead of pressure (#287, #288) -
doc updates to reflect how we run with the Pyro class (#266, #276,
#284, #285) and other general docs cleaning (#265, #268, #270,
#271) -
pylint CI update (#283); python version bump in actions (#281)
-
a new HLLC solver with corrections for low Mach number was added
(based on Minioshima & Miyoshi 2021) (#282) -
documenting and clean-ups of problem setups for each of the
solvers (adding docstrings that appear in the docs) (#272, #273,
#274, #275, #277, #279, #280)
pyro 4.3.0
4.3.0
-
it is now possible to define a problem setup in a Jupyter
notebook (#262, #264) -
fix a bug in the artificial viscosity for spherical coords (#263)
-
I/O is disabled by default when running in Jupyter (#259)
-
problem setups no longer check if the input grid is
CellCenterData2d (#258) -
the Pyro class interface was simplified to have command line
parameter use the dict interface (#257) -
problem setups no longer use a _*.defaults file, but instead
specify their runtime parameters via a dict in the problem module
(#255) -
the compressible_sr solver was removed (#226)
-
gresho problem uses more steps by default now (#254)
-
the 4th order compressible solver only needs 4 ghost cells, not 5
(#248) -
the compressible solver comparison docs were changed to an
interactive Jupyter page (#243, #246, #249, #252) -
some interfaces were cleaned-up to require keyword args (#247)
-
developers were added to the zenodo file (#242)
-
doc updates (#241)
pyro 4.2.0
4.2.0
-
docs reorganization (#214, #221, #222, #234, #239) and new
examples (#228, #236) -
remove driver.splitting unused parameter (#238)
-
clean-ups of the Pyro class (#219, #232, #233) including disabling
verbosity and vis by default when using it directly (#220, #231) -
the
advection_fv4
solver now properly averages the initial
conditions from centers to cell-averages -
each problem initial conditions file now specifies a
DEFAULT_INPUTS
(#225) -
the gresho initial conditions were fixed to be closer to the
source of the Miczek et al. paper (#218) -
the RT initial conditions were tweaked to be more symmetric (#216)
-
the colorbar tick labels in plots were fixed (#212)
-
the compressible solver now supports 2D spherical geometry
(r-theta) (#204, #210, #211) -
the mesh now supports spherical geometry (r-theta) (#201, #217)
-
the compressible Riemann solvers were reorganized (#206)
-
python 3.12 was added to the CI (#208)
-
comment fixes to the compressible FV4 solver (#207)
pyro 4.1.0
4.1
-
Switched to pyproject.toml (#195)
-
pytest improvements allowing it to be run more easily (#194)
-
plotvar.py script improvements (#178)
-
a new viscous Burgers solver was added (#171)
-
a new viscous incompressible solver was added with a lid-drive
cavity test problem (#138) -
the incompressible solver was synced up with the Burgers solver
(#168, #169) -
convergence.py can now take any variable and multiplicative
factor, as well as take 3 plotfiles to estimate convergence
directly. (#165) -
the multigrid solver output is now more compact (#161)
-
plot.py can fill ghostcells now (#156)
-
a new inviscid Burgers solver was added (#144)
-
a new convergence_error.py script for incompressible was added to
make the convergence plot for that solver (#147) -
regression tests can now be run in parallel (#145)
-
fixes for numpy > 1.20 (#137)
-
we can now Ctrl+C to abort when visualization is on (#131)
pyro 4.0.1
pyro 4.0.1
pyro 4.0.0
This begins a new development campaign, with the source updated to
conform to a standard python packaging format, allowing us to put
it up on PyPI, and install and run from anywhere.
JOSS paper version
This is the version associated with the pyro JOSS paper
3.0
This is the version submitted to JOSS.
Since the release for the first pyro paper, the code has undergone considerable development, gained a large number of solvers, adopted unit testing through pytest
and documentation through sphinx
, and a number of new contributors. pyro's functionality can now be accessed directly through a Pyro()
class, in addition to the original commandline script interface. This new interface in particular allows for easy use within Jupyter notebooks. We also now use HDF5 for output instead of python's pickle()
function. Previously, we used Fortran to speed up some performance-critical portions of the code. These routines could be called by the main python code by first compiling them using f2py
. In the new version, we have replaced these Fortran routines by python functions that are compiled at runtime by numba
. Consequently, pyro is now written entirely in python.
version used in the paper
This version will reproduce the results in the revision of the pyro paper.