Change the variable named *species* to be named *component*. This
better matches the utility of this variable, since it can be used to
retrieve any of the state variables. Also, update the corresponding
documentation.
The name 'H' can mean either the species by that name or the entahlpy
of the reactor, in the case of ConstPressureReactor, and the previous
behavior always returned the index of the enthalpy.
This changes the behavior to preferentially return the species, and
adds alternative names for reactor state variables that are less
likely to generate namespace collisions: 'mass', 'volume',
'int_energy', 'enthalpy', 'temperature', 'distance', 'velocity'. The
single character names are still supported.
Resolves Issue 193.
This fixes the problem of some output (notably from the 1D solver)
going to std::cout when that is not the primary output location,
e.g. when using IDLE or the IPython QtConsole.
This fixes an issue when the Python interpreter prints startup messages that
appear before the expected output lines. Known to be a problem with the Anaconda
Python distribution.
In particular, this fixes paths for Linux distros that put Python modules in
'lib64/pythonX.Y/site-packages'.
Also fixes the reported installation path for the Python module on Windows.
This corrects the behavior in cases where the correct temperature is below the
nominal minimum temperature for the phase.
Add test cases for this and analogous cases for the maximum temperature and
setState_HPorUV.
Fixes Issue 151.
The failures were caused when attempting to restore the tolerance vectors, which
have a value for each species. Since these tolerances are usually the same for
all species, the last value in the array can be used to extend the array to the
required length.
Also add some tests for this feature.
Like IdealGasReactor, this formulation uses the temperature as a state variable
to improve performance for the common use case of reactors containing ideal gas
mixtures.
This formulation of the reactor governing equations, with temperature as a state
variable, works better for ideal gas mixtures. This way, most of the Jacobian
components are derivatives at constant temperature, eliminating the need to
recompute the temperature-dependent part of the rate expressions when computing
these entries.
