Tutorial: Multi-Species Lattice Boltzmann Models and Applications
Tutorial: Multi-Species Lattice Boltzmann Models and Applications
Tutorial: Multi-Species Lattice Boltzmann Models and Applications
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<strong>Lattice</strong> <strong>Boltzmann</strong> solvers <strong>and</strong> applications<br />
Rule of computation for the list<br />
LBM formulation by variable transformation<br />
The components of the molecular velocity V 1 <strong>and</strong> V 2 are the lists<br />
with 9 elements. Before proceeding to the definition of the local<br />
equilibrium function f σ(∗) , we define the rule of computation for the<br />
list.<br />
Let h <strong>and</strong> g be the lists defined by h = [h 0 , h 1 , h 2 , · · · , h 8 ] T <strong>and</strong><br />
g = [g 0 , g 1 , g 2 , · · · , g 8 ] T . Then, hg is the list defined by<br />
[h 0 g 0 , h 1 g 1 , h 2 g 2 , · · · , h 8 g 8 ] T . The sum of all the elements of the list<br />
h is denoted by 〈h〉, i.e. 〈h〉 = ∑ 8<br />
i=0 h i.<br />
Then, the (dimensionless) density ρ σ <strong>and</strong> momentum q σi = ρ σ u σi<br />
are defined by<br />
ρ σ = 〈f σ 〉, q σi = 〈V i f σ 〉. (37)<br />
Pietro Asinari, PhD (Politecnico di Torino) <strong>Multi</strong>-<strong>Species</strong> LB <strong>Models</strong> Rome, Italy, on July 5-9, 2010 21 / 51