2007
DOI: 10.1007/s00158-007-0105-7
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Topology optimization of flow domains using the lattice Boltzmann method

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Cited by 102 publications
(71 citation statements)
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“…The method is attractive because it is algorithmically simple, lends itself well to parallel implementation, and is relatively easy to extend to more complicated physics, such as porous media [11][12][13], or multiphase flows [14,15]. The use of the LBM for topology optimization was pioneered by Pingen et al [16], who used the density approach to topology optimization. The work is extended to multiphase flow problems by Makhija et al [8].…”
Section: Introductionmentioning
confidence: 99%
“…The method is attractive because it is algorithmically simple, lends itself well to parallel implementation, and is relatively easy to extend to more complicated physics, such as porous media [11][12][13], or multiphase flows [14,15]. The use of the LBM for topology optimization was pioneered by Pingen et al [16], who used the density approach to topology optimization. The work is extended to multiphase flow problems by Makhija et al [8].…”
Section: Introductionmentioning
confidence: 99%
“…The optimization method has recently been extended to transient and dynamic flow problems (Kreissl et al, 2011;Deng et al, 2011) though still limited to laminar flows. Traditionally the finite element method has been used for the modeling of topology optimization problems; however, fluid flow problems have also been optimized using the finite volume method (Othmer, 2008), the Lattice-Boltzmann method (Pingen et al, 2007) and kinetic gas theory (Evgrafov et al, 2008). A few works on flow components that are able to pump a fluid and have been designed by topology optimization have been promoted.…”
Section: Primary Inflow Outflowmentioning
confidence: 99%
“…Since we do not model the vertical dimension of Ω, we omit the Boussinesqapproximation buoyancy term proportional to T e , which is typically included on the right-hand side of (2). We modify κ and α to model obstacles to heat and air flow in Ω, such as walls, doors, and windows, as described in [30], [31]. In particular, when the point x corresponds to a material that blocks air, we choose α(x) u(x), which results in u(x) ≈ 0, and when the point x corresponds to air then we choose α(x) = 0.…”
Section: A Cfd Modelmentioning
confidence: 99%