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Graf Isolan
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Untersuchte Arbeit:
Seite: 132, Zeilen: 2-8
Quelle: Fan et al 2004
Seite(n): 1, 7, 10, Zeilen: 1:15-18; 7:33-34; 10:22-23
DQMOM is implemented in the CFD code Fluent 6.2 by representing each node of the quadrature approximation as a distinct droplet phase. In the Eulerian multi-fluid model each droplet phase has its own momentum balance, giving the DQMOM-multi-fluid model the ability to treat polydispersed droplets, which have their own inertia and size-conditioned dynamics. Equation (6.25) is solved in the multi-fluid model as a set of user-defined scalars. [page 1]

DQMOM is implemented in the code by representing each node of the quadrature approximation as a distinct solid phase. Since in the multi-fluid model each solid phase has its own momentum balance, the nodes of the DQMOM approximation are convected with their own velocities.

[page 7]

It is thus clear that each node of the quadrature approximation is calculated in order to guarantee that the moments of the PSD are tracked with high accuracy but, at the same time, each node is treated as a distinct solid phase giving the DQMOM-multi-fluid model the ability to treat polydisperse solids.

[page 10]

The second equation in Eq. 22 is solved in the multi-fluid model as a set of user-defined scalars.

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