@@ -315,7 +315,7 @@ SEMI_SPAN= 0.0
315315% ---- NONEQUILIBRIUM GAS, IDEAL GAS, POLYTROPIC, VAN DER WAALS AND PENG ROBINSON CONSTANTS -------%
316316%
317317% Fluid model (STANDARD_AIR, IDEAL_GAS, VW_GAS, PR_GAS,
318- % CONSTANT_DENSITY, INC_IDEAL_GAS, INC_IDEAL_GAS_POLY, MUTATIONPP, SU2_NONEQ)
318+ % CONSTANT_DENSITY, INC_IDEAL_GAS, INC_IDEAL_GAS_POLY, MUTATIONPP, SU2_NONEQ, FLUID_MIXTURE )
319319FLUID_MODEL = STANDARD_AIR
320320%
321321% Ratio of specific heats (1.4 default and the value is hardcoded
@@ -343,8 +343,9 @@ SPECIFIC_HEAT_CP= 1004.703
343343% Used with Boussinesq approx. (incompressible, BOUSSINESQ density model only)
344344THERMAL_EXPANSION_COEFF = 0.00347
345345%
346- % Molecular weight for an incompressible ideal gas (28.96 g/mol (air) default)
347- MOLECULAR_WEIGHT = 28.96
346+ % Molecular Weights of species for an incompressible ideal gas (28.96 g/mol (air) default),
347+ % For multispecies, we have N Molecular weights: W_1, W_2,...., W_N
348+ MOLECULAR_WEIGHT = 28.96, 16.043
348349%
349350% Temperature polynomial coefficients (up to quartic) for specific heat Cp.
350351% Format -> Cp(T) : b0 + b1*T + b2*T^2 + b3*T^3 + b4*T^4
@@ -708,6 +709,7 @@ SCHMIDT_NUMBER_TURBULENT= 0.7
708709%
709710% Inlet Species boundary marker(s) with the following format:
710711% (inlet_marker, Species1, Species2, ..., SpeciesN-1, inlet_marker2, Species1, Species2, ...)
712+ % For N species, N-1 transport equations are solved, the last one Y_N is solved algebraically as 1-(sum of the species 1 to (N-1))
711713MARKER_INLET_SPECIES = (inlet, 0.5, ..., inlet2, 0.6, ...)
712714%
713715% Use strong inlet and outlet BC in the species solver
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