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Definition of mixture fraction

The interest in reformulating the conserved-variable scalars in terms of the mixture-fraction vector lies in the fact that relatively simple forms for the mixture-fraction PDF can be employed to describe the reacting scalars. However, if iVmf, then the incentive is greatly diminished since more mixture-fraction-component transport equations (Nmf) would have to be solved than conserved-variable-scalar transport equations (/V, ). We will thus assume that N m = Nmf and seek to define the mixture-fraction vector only for this case. Nonetheless, in order for the mixture-fraction PDF method to be applicable to the reacting scalars, they must form a linear mixture defined in terms of the components of the mixture-fraction vector. In some cases, the existence of linear mixtures is evident from the initial/inlet conditions however, this need not always be the case. Thus, in this section, a general method for defining the mixture-fraction vector in terms of a linear-mixture basis for arbitrary initial/inlet conditions is developed. [Pg.161]

49 iVmf = 1 is the case that is usually associated with non-premixed turbulent reacting flows. Most commercial CFD codes are designed to treat only this case. [Pg.161]

50 The names binary and ternary come from the number of feed streams that are required for a stationary flow, i.e., two and three, respectively. Some authors also use ternary for the rank-deficient case where Nm = 3 but [Pg.161]

From the definition of ol in (5.65), it is clear that when = N-m we can define the mixture-fraction vector by (x, t) = a(x, f ).51 For this case, (5.73) defines an invertible, constant-coefficient linear transformation S(0)  [Pg.162]

Furthermore, the transport equation for (x, t) is then exactly the same as (5.65). [Pg.162]


See other pages where Definition of mixture fraction is mentioned: [Pg.248]    [Pg.10]    [Pg.180]    [Pg.161]   


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