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Dual-quadrature representation

In the dual-quadrature representation corresponding to Eq. (3.87), the weights and nodes are neither time-nor space-independent since ka depends on the transported moments. [Pg.93]

Lage, P. L. C. 2011 On the representation of QMOM as a weighted-residual method -the dual-quadrature method of generalized moments. Computers Chemical Engineering 35(11), 2186-2203. [Pg.472]

The convenience of this second case has been noticed by several authors (6-8). The adjoint equation provides an alternative exact representation (dual) for the characteristic. Then, if several values of S are being studied, the effect on N may be computed by quadrature involving only one solution of the adjoint equation. This alternative exact procedure therefore avoids recomputing the equation in N for every S. Thus, Pendlebury (9) Studies the multiplication in a subcritical system as an external source of neutrons impinges at different places on the surface and in doing so has only to solve the (adjoint) transport equation once. [Pg.314]


See other pages where Dual-quadrature representation is mentioned: [Pg.84]    [Pg.93]    [Pg.93]    [Pg.96]    [Pg.99]    [Pg.398]    [Pg.84]    [Pg.93]    [Pg.93]    [Pg.96]    [Pg.99]    [Pg.398]   
See also in sourсe #XX -- [ Pg.84 , Pg.92 , Pg.93 , Pg.96 , Pg.99 , Pg.424 ]




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Quadrature

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