In Chapter 6 we reviewed the theory underlying transported PDF methods. In order to apply this theory to practical flow problems, numerical algorithms are required to 'solve' the PDF transport equation. In general, solving the PDF transport equation using standard finite-difference (FD) or finite-volume (FV) methods is computationally intractable for a number of reasons. For example, the velocity, composition PDF transport equation ((6. 19), p. 248) has three space variables ( x), three velocity variables ( V), N _s composition variables ( ?), and time ( t). Even for a statistically two-dimensional, steady-state flow with only one scalar, a finite-difference grid in at least five dimensions would be required! Add to this the problem of developing numerical techniques that ensure f _U, _? remains non-negative and normalized to unity at every space/time point ( x, t), and the technical difficulties quickly become insurmountable.

A tractable alternative to 'solving' the PDF transport equation is to use statistical or Monte-Carlo (MC) simulations. Unlike FV methods, MC simulations can handle a large number of independent variables, and always ensure that the resulting estimate of f _U, _? is well behaved. As noted in Section 6.8, MC simulations employ representative samples or so-called 'notional' particles. The principal challenge in constructing an MC algorithm is thus to define appropriate rules for the rates of change of the notional-particle variables so that they have statistical properties identical to f _U, _?( V