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Application of quadrature to collision terms

The moment-transport equations discussed above become more and more complicated as the order increases. Moreover, these equations are not closed. In quadrature-based moment methods, the velocity-distribution function is reconstructed from a finite set of moments, thereby providing a closure. In this section, we illustrate how the closure hypothesis is applied to solve the moment-transport equations with hard-sphere collisions. For clarity, we will consider the monodisperse case governed by Eq. (6.131). Formally, we can re-express this equation in conservative form  [Pg.261]

The quadrature-based closure of Eqs. (6.176) and (6.177) then proceeds as follows. Let / (f, X, v) denote the velocity-distribution function reconstructed from the transported moments (Eq. 6.173), and define the negative- and positive-integer moments for [Pg.262]

Analogous moments can be defined for directions X2 and X3. Since / is a known function, these moments can be computed (usually analytically) for any choice of (h,h,h)- Thus, using each set of moments, we can construct an arbitrarily high-order quadrature representation that can be used to evaluate the integrals in Eqs. (6.176) and (6.177). Formally, we can express the reconstruction procedure as [Pg.262]

An important point that is evident from the expressions in Eqs. (6.179) and (6.180) is that it suffices to know the functional form of / in order to account for the effect of [Pg.263]


See other pages where Application of quadrature to collision terms is mentioned: [Pg.261]    [Pg.261]    [Pg.263]    [Pg.265]   


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