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rework the unit test docs #1570
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************************ | ||
Comprehensive Unit Tests | ||
************************ | ||
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Generally, for each test, you simply type ``make`` in the test | ||
directory. There are a number of runtime parameters that can | ||
control the behavior. These are specified (along with defaults) | ||
in ``_parameters`` files in each test directory and can be | ||
overridden in an inputs file or on the commandline. | ||
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Some additional details on a few of the comprehensive unit tests | ||
are given below. | ||
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EOS test (``test_eos``) | ||
======================= | ||
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``Microphysics/unit_test/test_eos/`` is a unit test for the equations | ||
of state in Microphysics. It sets up a cube of data, with | ||
:math:`\rho`, :math:`T`, and :math:`X_k` varying along the three | ||
dimensions, and then calls the EOS in each zone. Calls are done to | ||
exercise all modes of calling the EOS, in order: | ||
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- ``eos_input_rt``: We call the EOS using :math:`\rho, T`. this is the | ||
reference call, and we save the :math:`h`, :math:`e`, :math:`p`, and | ||
:math:`s` from here to use in subsequent calls. | ||
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- ``eos_input_rh``: We call the EOS using :math:`\rho, h`, to recover | ||
the original :math:`T`. To give the root finder some work to do, we | ||
perturb the initial temperature. | ||
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We store the relative error in :math:`T` in the output file. | ||
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- ``eos_input_tp``: We call the EOS using :math:`T, p`, to recover the | ||
original :math:`\rho`. To give the root finder some work to do, we | ||
perturb the initial density. | ||
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We store the relative error in :math:`\rho` in the output file. | ||
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- ``eos_input_rp``: We call the EOS using :math:`\rho, p`, to recover | ||
the original :math:`T`. To give the root finder some work to do, we | ||
perturb the initial temperature. | ||
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We store the relative error in :math:`T` in the output file. | ||
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- ``eos_input_re``: We call the EOS using :math:`\rho, e`, to recover | ||
the original :math:`T`. To give the root finder some work to do, we | ||
perturb the initial temperature. | ||
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We store the relative error in :math:`T` in the output file. | ||
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- ``eos_input_ps``: We call the EOS using :math:`p, s`, to recover the | ||
original :math:`\rho, T`. To give the root finder some work to do, | ||
we perturb the initial density and temperature. | ||
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Note: entropy is not well-defined for some EOSs, so we only attempt | ||
the root find if :math:`s > 0`. | ||
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We store the relative error in :math:`\rho, T` in the output file. | ||
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- ``eos_input_ph``: We call the EOS using :math:`p, h`, to recover the | ||
original :math:`\rho, T`. To give the root finder some work to do, | ||
we perturb the initial density and temperature. | ||
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We store the relative error in :math:`\rho, T` in the output file. | ||
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- ``eos_input_th``: We call the EOS using :math:`T, h`, to recover the | ||
original :math:`\rho`. To give the root finder some work to do, we | ||
perturb the initial density. | ||
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Note: for some EOSs, :math:`h = h(\rho)` (e.g., an ideal gas), so there | ||
is no temperature dependence, and we do not do this test. | ||
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We store the relative error in :math:`\rho` in the output file. | ||
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This unit test is marked up with OpenMP directives and therefore also | ||
tests whether the EOS is threadsafe. | ||
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To compile for a specific EOS, e.g., helmholtz, do:: | ||
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make EOS_DIR=helmholtz -j 4 | ||
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Examining the output (an AMReX plotfile) will show you how big the | ||
errors are. You can use the ``amrex/Tools/Plotfile/`` tool | ||
``fextrema`` to display the maximum error for each variable. | ||
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Network test (``test_react``) | ||
============================= | ||
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``Microphysics/unit_test/test_react/`` is a unit test for the nuclear | ||
reaction networks in Microphysics. It sets up a cube of data, with | ||
:math:`\rho`, :math:`T`, and :math:`X_k` varying along the three | ||
dimensions (as a :math:`16^3` domain), and then calls the EOS in each | ||
zone. This test does the entire ODE integration of the network for | ||
each zone. | ||
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The state in each zone of our data cube is determined by the runtime | ||
parameters ``dens_min``, ``dens_max``, ``temp_min``, and ``temp_max`` | ||
for :math:`(\rho, T)`. Because each network carries different | ||
compositions, we specify the composition through runtime parameters in | ||
the ``&extern`` namelist: ``primary_species_1``, | ||
``primary_species_2``, ``primary_species_3``. These primary species | ||
will vary from X = 0.2 to X = 0.7 to 0.9 (depending on the number). | ||
Only one primary species varies at a time. The non-primary species | ||
will be set equally to share whatever fraction of 1 is not accounted | ||
for by the primary species mass fractions. | ||
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This test calls the network on each zone, running for a time | ||
``tmax``. The full state, including new mass fractions and energy | ||
release is output to a AMReX plotfile. | ||
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You can compile for a specific integrator (e.g., ``VODE``) or | ||
network (e.g., ``aprox13``) as:: | ||
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make NETWORK_DIR=aprox13 INTEGRATOR_DIR=VODE -j 4 | ||
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The loop over the burner is marked up for OpenMP and CUDA and | ||
therefore this test can be used to assess threadsafety of the burners | ||
as well as to optimize the GPU performance of the burners. |
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************** | ||
One Zone Tests | ||
************** | ||
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There are several tests that let you call the EOS or reaction network | ||
on a single zone to inspect the output directly. | ||
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``burn_cell`` | ||
============= | ||
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``burn_cell`` is a simple one-zone burn that will evolve a state with | ||
a network for a specified amount of time. This can be used to | ||
understand the timescales involved in a reaction sequence or to | ||
determine the needed ODE tolerances. | ||
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Getting Started | ||
--------------- | ||
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The ``burn_cell`` code are located in | ||
``Microphysics/unit_test/burn_cell``. To run a simulation, ensure that | ||
both an input file and an initial conditions file have been created | ||
and are in the same directory as the executable. | ||
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Input File | ||
---------- | ||
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These files are typically named as ``inputs_burn_network`` where network | ||
is the network you wish to use for your testing. | ||
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The structure of this file is is fairly self-explanatory. The run | ||
prefix defined should be unique to the tests that will be run as they | ||
will be used to identify all of the output files. Typically, the run | ||
prefix involves the name of the network being tested. The ``atol`` | ||
variables define absolute tolerances of the ordinary differential | ||
equations and the ``rtol`` variables define the relative tolerances. The | ||
second section of the input file collects the inputs that ``main.f90`` | ||
asks for so that the user does not have to input all 5+ | ||
parameters that are required every time the test is run. Each input | ||
required is defined and initialized on the lines following | ||
``&cellparams``. The use of the parameters is show below: | ||
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.. table:: The definition of parameters used in the burn_cell unit tests and specified in the second half of each inputs file. | ||
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+-----------------------+----------------------------------------+ | ||
| ``tmax`` | Maximum Time (s) | | ||
+-----------------------+----------------------------------------+ | ||
| ``nsteps`` | Number of time subdivisions | | ||
+-----------------------+----------------------------------------+ | ||
| ``density`` | State Density (:math:`\frac{g}{cm^3}`) | | ||
+-----------------------+----------------------------------------+ | ||
| ``temperature`` | State Temperature (K) | | ||
+-----------------------+----------------------------------------+ | ||
| ``massfractions(i)`` | Mass Fraction for element i | | ||
There was a problem hiding this comment. Choose a reason for hiding this commentThe reason will be displayed to describe this comment to others. Learn more. This should be something like |
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+-----------------------+----------------------------------------+ | ||
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Running the Code | ||
---------------- | ||
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To run the code, enter the burn_cell directory and run:: | ||
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./main3d.gnu.ex inputs | ||
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where ``inputs`` is the name of your inputs file. | ||
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For each of the ``numsteps`` steps defined in the inputs | ||
file, the code will output a files into a new directory titled | ||
``run_prefix_output`` where ``run_prefix`` is the run prefix defined in the | ||
inputs file. Each output file will be named using the run prefix | ||
defined in the inputs file and the corresponding timestep. | ||
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Next, run ``burn_cell.py`` using python 3.x, giving the defined run prefix as an argument. | ||
For example:: | ||
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python3 burn_cell.py react_aprox13 | ||
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The ``burn_cell.py`` code will gather information from all of the | ||
output files and compile them into three graphs explained below. | ||
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Graphs Output by ``burn_cell.py`` | ||
--------------------------------- | ||
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The file ``run-prefix_logX.png`` and ``run-prefix_logX.eps`` will display a | ||
graph of the chemical abundances as a function of the time, both on | ||
logarithmic scales, for all species involved in the simulation. An | ||
example of this graph is shown below. | ||
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.. figure:: react_aprox13_logX.png | ||
:alt: An example of a plot output by the burn_cell unit test. This is the logX output corresponding to the network aprox13. | ||
:width: 4.5in | ||
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An example of a plot output by the burn_cell unit test. This is the | ||
logX output corresponding to the network aprox13. | ||
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The file ``run-prefix_ydot.png`` and ``run-prefix_ydot.eps`` will display the | ||
molar fraction (mass fraction / atomic weight) as a function of time, | ||
both on logarithmic scales, for all species involved in the code. | ||
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The file ``run-prefix_T-edot.png`` and ``run-prefix_T-edot.eps`` will display | ||
the temperature and the energy generation rate as a function of time. | ||
Comment on lines
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There was a problem hiding this comment. Choose a reason for hiding this commentThe reason will be displayed to describe this comment to others. Learn more. This is all for the old Fortran There was a problem hiding this comment. Choose a reason for hiding this commentThe reason will be displayed to describe this comment to others. Learn more. yeah, I just moved the burn_cell docs and didn't update them, since we also need to update the README. I was thinking of that as a separate PR / maybe for the hackathon There was a problem hiding this comment. Choose a reason for hiding this commentThe reason will be displayed to describe this comment to others. Learn more. Okay, that's fine then |
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We should remove the Fortran references here