Outputs
Outputs from Parthenon are controled via <parthenon/output*>
blocks,
where *
should be replaced by a unique integer for each block.
To disable an output block without removing it from the intput file set
the block’s dt < 0.0
.
In addition to time base outputs, two additional options to trigger outputs (applies to HDF5 and restart outputs) exist.
Signaling: If
Parthenon
catches a signal, e.g.,SIGALRM
which is often sent by schedulers such as Slurm to signal a job of exceeding the job’s allocated walltime,Parthenon
will gracefully terminate and write output files with afinal
id rather than a number. This also applies to theParthenon
internal walltime limit, e.g., when executing an application with the-t HH:MM:SS
parameter on the command line.File trigger: If a user places a file with the name
output_now
in the working directory of a running application,Parthenon
will write output files with anow
id rather than a number. After the output is being written theoutput_now
file is removed and the simulation continues normally. The user can repeat the process any time by creating a newoutput_now
file.
Note, in both cases the original numbering of the output will be
unaffected and the final
and now
files will be overwritten each
time without warning. ## HDF5
Parthenon allows users to select which fields are captured in the HDF5
(.phdf
) dumps at runtime. In the input file, include a
<parthenon/output*>
block, list of variables, and specify
file_type = hdf5
. A dt
parameter controls the frequency of
outputs for simulations involving evolution. If the optional parameter
single_precision_output
is set to true
, all variable data will
be written in single precision. A <parthenon/output*>
block might
look like
<parthenon/output1>
file_type = hdf5
# nonexistent variables/swarms are ignored
variables = density, velocity, & # comments are still ok
energy # notice the & continuation character
# for multiline lists
swarms = tracers, photons # Particle swarms
swarm_variables = x, y, z # swarm variables output for every swarm
# Each swarm can sepcify in a separate list which additional
# variables it would like to output.
tracers_variables = x, y, z, rho, id
photons_variables = x, y, z, frequency
dt = 1.0
file_number_width = 6 # default: 5
use_final_label = true # default: true
This will produce an hdf5 (.phdf
) output file every 1 units of
simulation time containing the density, velocity, and energy of each
cell. The files will be identified by a 6-digit ID, and the output file
generated upon completion of the simulation will be labeled
*.final.*
rather than with the integer ID.
HDF5 and restart files write variable field data with inline compression
by default. This is especially helpful when there are sparse variables
allocated only in a few blocks, because all other blocks would write
zeros of these variables, which can drastically increase output file
size (and decrease I/O performance) without compression. The optional
parameter hdf5_compression_level
can be used to set the compression
level (between 1 and 9, default is 5). Compression can be disabled
altogether with the CMake build option
PARTHENON_DISABLE_HDF5_COMPRESSION
.
See the Building Parthenon for more details.
Tuning HDF5 Performance
Tuning IO parameters can be passed to Parthenon through the use of environment variables. Available environment variables are:
Environment Variable |
Initial State |
Value Type |
Description |
---|---|---|---|
H5_sieve_buf_size
H5_meta_block_size
H5_alignment_threshold
H5_alignment_alignment
H5_defer_metadata_flush
MPI_access_style
MPI_collective_buffering
MPI_cb_block_size
MPI_cb_buffer_size
|
disabled
disabled
disabled
disabled
disabled
enabled
disabled
N/A
N/A
|
int
int
int
int
int
string
int
int
int
|
Sets the maximum size of the data sieve buffer, in bytes. The value should be equal to a multiple of the disk block size. If no value is set then the default is 256 KiB.
Sets the minimum metadata block size, in bytes. If no value is set then the default is 8 MiB. May help performance if enabled.
The threshold value, in bytes, of H5Pset_alignment. Setting to 0 forces everything to be aligned. If a value is not set then the default is 0. Setting the environment variable automatically enables alignment.
The alignment value, in bytes, of H5Pset_alignment. If a value is not set then the default is 8 MiB. Setting the environment variable automatically enables alignment. H5Pset_alignment sets the alignment properties of a file access property list. Choose an alignment that is a multiple of the disk block size, enabling this usually shows better performance on parallel file systems. However, enabling may increase the file size significantly.
Value of 1 enables deferring metadata flush. Value of 0 disables. Experiment with before using.
Specifies the manner in which the file will be accessed until the file is closed. Default is “write_once”
Value of 1 enables MPI collective buffering. Value of 0 disables. Experiment with before using.
Sets the block size, in bytes, to be used for collective buffering file access. Default is 1 MiB.
Sets the total buffer space, in bytes, that can be used for collective buffering on each target node, usually a multiple of cb_block_size. Default is 4 MiB.
|
Restart Files
Parthenon allows users to output restart files for restarting a simulation. The restart file captures the input file, so no input file is required to be specified. Parameters for the input can be overriden in the usual way from the command line. At a future date we will allow for users the ability to extensively edit the parameters stored within the restart file.
In the input file, include a <parthenon/output*>
block and specify
file_type = rst
. A dt
parameter controls the frequency of
outputs for simulations involving evolution. A <parthenon/output*>
block might look like
<parthenon/output7>
file_type = rst
dt = 1.0
This will produce an hdf5 (.rhdf
) output file every 1 units of
simulation time that can be used for restarting the simulation.
To use this restart file, simply specify the restart file with a
-r <restart.rhdf>
at the command line. It is an error to specify an
input file with the -i
flag when using the restart option.
For physics developers: The fields to be output are automatically
selected as all the variables that have either the Independent
or
Restart
Metadata
flags specified. No other intervention is
required by the developer.
History Files
In the input file, include a <parthenon/output*>
block and specify
file_type = hst
. A dt
parameter controls the frequency of
outputs for simulations involving evolution. A <parthenon/output*>
block might look like
<parthenon/output8>
file_type = hst
dt = 1.0
This will produce a text file (.hst
) output file every 1 units of
simulation time. The content of the file is determined by the functions
enrolled by a specific package, see History output.
Ascent (optional)
Parthenon supports in situ visualization and analysis via the external
Ascent library.
Support for Ascent is disabled by default and must be enabled via PARTHENON_ENABLE_ASCENT=ON
during configure.
In the input file, include a <parthenon/output*>
block and specify file_type = ascent
.
A dt
parameter controls the frequency of outputs for simulations involving evolution.
Note that in principle Ascent can control its own output cadence (including
automated tiggers).
If you want to call Ascent on every cycle, set dt
to a value smaller than the actual simulation dt
.
The mandatory actions_file
parameter points to a separate file that defines
Ascent actions in .yaml
or .json
format, see
Ascent documentation for a complete list of options.
A <parthenon/output*>
block might look like:
<parthenon/output9>
file_type = ascent
dt = 1.0
actions_file = my_actions.yaml
see also the advection example input file and actions file.
Note by default “field filtering” is enabled for Ascent in Parthenon, i.e.,
only fields that are used in Ascent actions are published.
There may be cases, where Ascent cannot determine which fields it needs for
an action and will fail.
In this case, add an ascent_options.yaml
file to the run directory containing:
field_filtering: false
to override at runtime. See Ascent documenation for more information.
Python scripts
The scripts/python
folder includes scripts that may be useful for
visualizing or analyzing data in the .phdf
files. The phdf.py
file defines a class to read in and query data. The movie2d.py
script shows an example of using this class, and also provides a
convenient means of making movies of 2D simulations. The script can be
invoked as
python3 /path/to/movie2d.py name_of_variable *.phdf
which will produce a png
image per dump suitable for encoding into a
movie.
Visualization software
Both ParaView and
VisIt are
capable of opening and visualizing Parthenon graphics dumps. In both
cases, the .xdmf
files should be opened. In ParaView, select the
“XDMF Reader” when prompted.
Preparing outputs for yt
Parthenon HDF5 outputs can be read with the python visualization library
yt as certain variables are named when
adding fields via StateDescriptor::AddField
and
StateDescriptor::AddSparsePool
. Variable names are added as a
std::vector<std::string>
in the variable metadata. These labels are
optional and are only used for output to HDF5. 4D variables are named
with a list of names for each row while 3D variables are named with a
single name. For example, the following configurations are acceptable:
auto pkg = std::make_shared<StateDescriptor>("Hydro");
/* ... */
const int nhydro = 5;
std::vector<std::string> cons_labels(nhydro);
cons_labels[0]="Density";
cons_labels[1]="MomentumDensity1";
cons_labels[2]="MomentumDensity2";
cons_labels[3]="MomentumDensity3";
cons_labels[4]="TotalEnergyDensity";
Metadata m({Metadata::Cell, Metadata::Independent, Metadata::FillGhost},
std::vector<int>({nhydro}), cons_labels);
pkg->AddField("cons", m);
const int ndensity = 1;
std::vector<std::string> density_labels(ndensity);
density_labels[0]="Density";
m = Metadata({Metadata::Cell, Metadata::Derived}, std::vector<int>({ndensity}), density_labels);
pkg->AddField("dens", m);
const int nvelocity = 3;
std::vector<std::string> velocity_labels(nvelocity);
velocity_labels[0]="Velocity1";
velocity_labels[1]="Velocity2";
velocity_labels[2]="Velocity3";
m = Metadata({Metadata::Cell, Metadata::Derived}, std::vector<int>({nvelocity}), velocity_labels);
pkg->AddField("vel", m);
const int npressure = 1;
std::vector<std::string> pressure_labels(npressure);
pressure_labels[0]="Pressure";
m = Metadata({Metadata::Cell, Metadata::Derived}, std::vector<int>({npressure}), pressure_labels);
pkg->AddField("pres", m);
The yt
frontend needs either the hydrodynamic conserved variables or
primitive compute derived quantities. The conserved variables must have
the names "Density"
, "MomentumDensity1"
, "MomentumDensity2"
,
"MomentumDensity3"
, "TotalEnergyDensity"
while the primitive
variables must have the names "Density"
, "Velocity1"
,
"Velocity2"
, "Velocity3"
, "Pressure"
. Either of these sets
of variables must be named and present in the output, with the primitive
variables taking precedence over the conserved variables when computing
derived quantities such as specific thermal energy. In the above
example, including either "cons"
or "dens"
, "vel"
, and
"pres"
in the HDF5 output would allow yt
to read the data.
Additional parameters can also be packaged into the HDF5 file to help
yt
interpret the data, namely adiabatic index and code unit
information. These are identified by passing true
as an optional
boolean argument when adding parameters via
StateDescriptor::AddParam
. For example,
pkg->AddParam<double>("CodeLength", 100,true);
pkg->AddParam<double>("CodeMass", 1000,true);
pkg->AddParam<double>("CodeTime", 1,true);
pkg->AddParam<double>("AdibaticIndex", 5./3.,true);
pkg->AddParam<int>("IntParam", 0,true);
pkg->AddParam<std::string>("EquationOfState", "Adiabatic",true);
adds the parameters CodeLength
, CodeMass
, CodeTime
,
AdiabaticIndex
, IntParam
, and EquationOfState
to the HDF5
output. Currently, only int
, float
, and std::string
parameters can be included with the HDF5.
Code units can be defined for yt
by including the parameters
CodeLength
, CodeMass
, and CodeTime
, which specify the code
units used by Parthenon in terms of centimeters, grams, and seconds by
writing the parameters. In the above example, these parameters dictate
yt
to interpret code lengths in the data in units of 100 centimeters
(or 1 meter per code unit), code masses in units of 1000 grams (or 1
kilogram per code units) and code times in units of seconds (or 1 second
per code time). Alternatively, this unit information can also be
supplied to the yt
frontend when loading the data. If code units are
not defined in the HDF5 file or at load time, yt
will assume that
the data is in CGS
.
The adiabatic index can also be specified via the parameter
AdiabaticIndex
, defined at load time for yt
, or left as its
default 5./3.
.
For example, the following methods are valid to load data with yt
filename = "parthenon.out0.00000.phdf"
#Read units and adiabatic index from the HDF5 file or use defaults
ds = yt.load(filename)
#Specify units and adiabatic index explicitly
units_override = {"length_unit" : (100, "cm"),
"time_unit" : (1, "s"),
"mass_unit" : (1000,"g")}
ds = yt.load(filename,units_override=units_override,gamma=5./3.)
Currently, the yt
frontend for Parthenon is hosted on the
parthenon-frontend
branch of this yt fork. In
the future, the Parthenon frontend will be included in the main yt
repo.