2006
DOI: 10.1063/1.2187070
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Equations of state in a lattice Boltzmann model

Abstract: In this paper we consider the incorporation of various equations of state into the single-component multiphase lattice Boltzmann model. Several cubic equations of state, including the van der Waals, Redlich-Kwong, and Peng-Robinson, as well as a noncubic equation of state (Carnahan-Starling), are incorporated into the lattice Boltzmann model. The details of phase separation in these nonideal single-component systems are presented by comparing the numerical simulation results in terms of density ratios, spuriou… Show more

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Cited by 783 publications
(536 citation statements)
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“…38 The pseudo-potential model introduces the nearest-neighboring interaction between fluid particles to describe the intermolecular potential, and the phase separation occurs with a properly chosen potential function. Although significant advances have recently been made, [43][44][45] further improvements are necessary for the pseudo-potential model to minimize spurious velocities at interface and control numerical instability for the flows with low capillary number and viscosity ratio. The free-energy model suffers from the lack of Galilean invariance, 32 although the local conservation of mass and momentum is satisfied.…”
Section: Methodsmentioning
confidence: 99%
“…38 The pseudo-potential model introduces the nearest-neighboring interaction between fluid particles to describe the intermolecular potential, and the phase separation occurs with a properly chosen potential function. Although significant advances have recently been made, [43][44][45] further improvements are necessary for the pseudo-potential model to minimize spurious velocities at interface and control numerical instability for the flows with low capillary number and viscosity ratio. The free-energy model suffers from the lack of Galilean invariance, 32 although the local conservation of mass and momentum is satisfied.…”
Section: Methodsmentioning
confidence: 99%
“…However, use of this equation of state limits the density ratio between the heavy and light phases to about 100 and results in large spurious currents at the liquid-gas interface that hamper the tracking of passive tracer particles in this region. Here, following previous work [39,40], the Carnahan-Starling equation of state,…”
Section: Simulation Methodsmentioning
confidence: 99%
“…In addition, Sbragaglia et al [20] have devised a free-energy formulation of the pseudopotential LB model. Furthermore, several attempts have been made by Yuan and Schaefer [21], Falcucci et al [22], and Kupershtokh et al [23] to break through the low-density-ratio restriction.…”
Section: Introductionmentioning
confidence: 99%