The boundary conditions are relatively easily implemented. At the cold boundary we specify the mass flux fractions and the temperature, that is, we solve
(13–22) |
and
(13–23) |
where is the inlet reactant fraction of the k th species and is the specified burner temperature. At the hot boundary we specify that all gradients vanish, that is,
(13–24) |
and
(13–25) |
The boundary conditions for depend on whether the given problem is a burner-stabilized or a freely propagating flame. The boundary conditions for each case are discussed in Boundary Conditions .