Appendix B: FlameMaster Diffusion Flamelet Control File
A FlameMaster control file for generating diffusion flamelets is replicated here for the reader to use as a template for their set of conditions.
### Newton Solver ####
TStart = 0.1e-4
TEnd = 10.0
DampFlag = TRUE
LambdaMin = 1.0e-2
UseNumericalJac is TRUE
UseModifiedNewton = TRUE
MaxIter = 350
TolRes = 1.0e-3
TolDy = 1.0e-4
#### Grid ####
DeltaNewGrid = 20
OneSoluOneGrid is TRUE
initialgridpoints = 81
maxgridpoints =359
Q = -0.25
R = 60
#OutputPath is ./upperBranch_rightMoving
OutputPath is./upperBranch_leftMoving
#OutputPath is ./lowerBranch_rightPoint
#OutputPath is ./lowerBranch_leftMoving
WriteRes is TRUE
WriteEverySolution is TRUE
StartProfilesFile is ./N-C12H26_p468_8chi800000tf0288to0111
#StartProfilesFile is ./N-C12H26_p468_8chi497.037tf0288to0111Tst0941
#StartProfilesFile is ./N-C12H26_p468_8chi00500tf0288to0111
#StartProfilesFile is ./lowerBranch_rightPoint/N-C12H26_p468_8chi5e+09tf0288to0111
MechanismFile is ndodecane_31spec.pre
globalReaction is N-C12H26 + 18.5O2 == 12CO2 + 13H2O;
fuel is N-C12H26
oxidizer is O2
#### Flame ####
ConstLewisNumber is TRUE
LewisNumberFile is LewisNumberOne
ArclengthCont = TRUE
Flame is Counterflow Diffusion in Mixture Fraction Space
EquationOfState is PengRobinson
Scalar DissipationRate =1e6 #Starting rate
#Scalar DissipationRate =1.1e6 #Upper branch - right moving value
Scalar DissipationRate =1e1 #Upper branch - left moving value
#Scalar DissipationRate =50e8 #Lower Branchure right point
#Scalar DissipationRate =1e3 #Extinction branch, left
# Additional Values to constrain the curve to have resolution near the turning point of the S-curve
#Scalar DissipationRate = 1.000000e06
# Note: If the pressure continuation to shift the conditions is not quite
# exactly the pressure you want, then on the next property shift, just adjust
# this initial pressure to be the pressure that you want, and it should update
# the pressure and whatever the other property you selected.
pressure = 46.884e6
#### Boundary Conditions ####
Fuel Side {
dirichlet {
t=288.889
Y->N-C12H26 = 1.0
}
}
Oxidizer Side {
dirichlet {
t=111.111
Y->O2 = 1.00
}
}
Appendix C: FlameMaster Premixed Flamelet Control File
A FlameMaster control file for generating premixed flamelets is replicated here for the reader to use as a template for their set of conditions.
#### Newton solver ####
UseNumericalJac is TRUE
UseSecondOrdJac is TRUE
UseModifiedNewton = TRUE
DampFlag = TRUE
LambdaMin = 1.0e-3
MaxIter = 2000
TolRes = 1.0e-16
TolDy = 1e-12
#### grid ####
DeltaNewGrid = 50
OneSolutionOneGrid = TRUE
initialgridpoints = 80
maxgridpoints = 360
q = -0.25
R = 60
#### Sensitivity Analysis ####
#ReactionFluxAnal is TRUE
#### I/O ####
WriteEverySolution = TRUE
#PrintMolarFractions is TRUE
OutputPath is ./output
#StartProfilesFile is ./CH4_p01_0phi1_0006tu0300
StartProfilesFile is ./output/CH4_p01_0phi1_0000tu0300
#### Chemistry ####
MechanismFile is drm19.pre
globalReaction is CH4 + 2O2 == CO2 + 2H2O;
EquationOfState is IdealGasLaw
fuel is CH4
oxidizer is O2
#### Flame ####
ConstLewisNumber is TRUE
LewisNumberFile is LewisNumberOne
Flame is UnstretchedPremixed
ExactBackward is TRUE
phi = 0.95
phi = 0.9
phi = 0.85
phi = 0.8
phi = 0.75
pressure = 101325
#### Boundary conditions ####
#ConstMassFlux is TRUE
#MassFlux = 0.3
Unburnt Side {
dirichlet {
t = 300
Y->CH4 = 0.0552
Y->O2 = 0.2201
Y->N2 = 0.7247
}
}
Appendix D: Species Renaming
Occasionally there will be a case where the species names that FlameMaster uses (and the names that are written to the flamelet table) conflict with Stream’s table processor (bad characters, etc.). A Python utility has been written that will take an input file containing a mapping of old names to new names and rename the species in a provided ascii flamelet table.
Command:
bin/flamelet/utilities/flamemaster-tools/loci_table_species_rename.py Table.dat rename.dat
Appendix E: Pruning FlameMaster Counterflow-Diffusion Flamelets
In the course of generating a suite of counterflow-diffusion flamelets using FlameMaster, it is possible to generate a large number of flamelets
due to FlameMaster’s use of an automatic arclength-continuation method. A resolution of 5 to 10 flamelets per decade of the scalar dissipation rate
is usually sufficient. A collection of many flamelet solutions also runs a possible risk of having an overlapping flamelet solution. When this happens,
the uniqueness of the Z-C manifold that is used to interpolate becomes polluted and the tabulated values can become erroneous. To remedy this issue, a Python
utility script is provided in the utilities/flamemaster_tools
directory of the Flamelet Table Tool. The script is named flamemaster_flamelet_pruning.py
.
A summary of the options that the script takes is provided below:
Argument |
Type |
Description |
---|---|---|
–flamelets_path |
str (required) |
Absolute or relative path to directory with flamelets |
–minimum_arclength |
float (required) |
Threshold that removed flamelets that are closer than this distance together |
–output_dir_name |
str (required) |
Name of directory to output pruned flamelets to |