2019
DOI: 10.1016/j.ijmultiphaseflow.2019.04.006
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An interfacial lattice Boltzmann flux solver for simulation of multiphase flows at large density ratio

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Cited by 22 publications
(25 citation statements)
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“…e multiple-relaxation-time collision operator is applied to study the influence of different parameters, including the gas/liquid viscosity ratio and liquid film thickness. Wang et al [24] and Li et al [25] have built an interfacial lattice Boltzmann flux solver for high-density ratio multiphase phenomena, and the droplet splashing on the stationary thin film is also simulated successfully. Due to the existence of the shear stress in the liquid film, the dynamic behaviors of the droplet impact on a moving liquid film are more complex.…”
Section: Introductionmentioning
confidence: 99%
“…e multiple-relaxation-time collision operator is applied to study the influence of different parameters, including the gas/liquid viscosity ratio and liquid film thickness. Wang et al [24] and Li et al [25] have built an interfacial lattice Boltzmann flux solver for high-density ratio multiphase phenomena, and the droplet splashing on the stationary thin film is also simulated successfully. Due to the existence of the shear stress in the liquid film, the dynamic behaviors of the droplet impact on a moving liquid film are more complex.…”
Section: Introductionmentioning
confidence: 99%
“…The LB evolution equation with the BGK collision operator for C‐H equation can be written as 26,31,34 : gαfalse(x+bold-italiceαΔt,t+Δtfalse)gαfalse(x,tfalse)=gαitaliceqfalse(x,tfalse)gαfalse(x,tfalse)τg+ΔitalictGαfalse(x,tfalse),α=0,1,,N, where g α is the distribution function for order parameter with discrete velocity e α at physical location x = ( x , y ) and time step t ; τ g is the non‐dimensional relaxation parameter related to the mobility; N is the number of the streaming directions, and the superscript eq of g α denotes a local equilibrium state which is given by 20,30,35 : gαitaliceq=leftϕ3μϕθMfalse(1ωαfalse)α=0,3ωαfalse(μϕθM+ϕbold-italiceαufalse)α=1,,N, here ω α is the weighting coefficient which is given by ω 0 = 4/9, ω 1 − 4 = 1/9, ω 5 − 8 = 1/36 in D2Q9 model, and the discrete velocities can be defined as 36 : bold-italiceα=leftfalse(0,0false)c,α=0...…”
Section: Methodsologymentioning
confidence: 99%
“…Thus, there are two different phase‐field based multiphase models: one is to couple C‐H equation with N‐S equations and another is to couple A‐C equation with N‐S equations. In the recent decade, interests are growing in adopting the phase‐field theory to simulate multiphase flows, among which the LBM has attracted wide publicity 13‐32 …”
Section: Introductionmentioning
confidence: 99%
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