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Tutorial: Multi-Species Lattice Boltzmann Models and Applications

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<strong>Lattice</strong> <strong>Boltzmann</strong> solvers <strong>and</strong> applications<br />

LBM formulation by variable transformation<br />

Solution: solving locally a linear system of equations<br />

In the general case, Eq. (45) can be recasted as<br />

〈V i g σ + 〉 = q<br />

σi + − θ ∑<br />

λ+ σ χ σς (x + σ q<br />

ςi + − x+ ς q<br />

σi + ), (46)<br />

ς<br />

where q<br />

σi + = ρ+ σ u + σi <strong>and</strong> χ σς =<br />

m2 B σς<br />

. (47)<br />

m σ m ς B mm<br />

Finally, grouping together common terms yields<br />

[<br />

]<br />

∑<br />

〈V i g σ + 〉 = 1 + θ λ + σ (χ σς x + ς ) q<br />

σi + − θ λ+ σ x + σ<br />

ς<br />

∑<br />

(χ σς q<br />

ςi + ). (48)<br />

ς<br />

Clearly the previous expression defines a linear system of<br />

algebraic equations for the unknowns q + σi .<br />

Pietro Asinari, PhD (Politecnico di Torino) <strong>Multi</strong>-<strong>Species</strong> LB <strong>Models</strong> Rome, Italy, on July 5-9, 2010 28 / 51

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