2015
DOI: 10.3390/e17117406
|View full text |Cite
|
Sign up to set email alerts
|

Extension of the Improved Bounce-Back Scheme for Electrokinetic Flow in the Lattice Boltzmann Method

Abstract: Abstract:In this paper, an improved bounce-back boundary treatment for fluid systems in the lattice Boltzmann method [Yin, X.; Zhang J. J. Comput. Phys. 2012, 231, 4295-4303] is extended to handle the electrokinetic flows with complex boundary shapes and conditions. Several numerical simulations are performed to validate the electric boundary treatment.Simulations are presented to demonstrate the accuracy and capability of this method in dealing with complex surface potential situations, and simulated results… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
2
1

Citation Types

0
6
0

Year Published

2017
2017
2022
2022

Publication Types

Select...
6

Relationship

0
6

Authors

Journals

citations
Cited by 7 publications
(6 citation statements)
references
References 41 publications
0
6
0
Order By: Relevance
“…For the considered incompressible flow, with ρ = constant, they read: bold∇u=0 and ρ(normal∂bold-italicunormal∂t+bold-italicubold∇u)=bold∇p+μ2bold-italicu+bold-italicF, where μ is the dynamic viscosity. The discretized LBM model for the electric field is [3537,40]: hifalse(bold-italicxbold+bold-italicci,s+1false)hifalse(bold-italicx,sfalse)=1τΨfalse[hifalse(bold-italicx,sfalse)hieqfalse(bold-italicx,sfalse)false]+ωiρeϵ with hieq=ωiΨ,1emΨ=ihi, τΨ=3χ+12, where hi…”
Section: Mathematical Models and Lattice Boltzmann Methods Implementationmentioning
confidence: 99%
See 1 more Smart Citation
“…For the considered incompressible flow, with ρ = constant, they read: bold∇u=0 and ρ(normal∂bold-italicunormal∂t+bold-italicubold∇u)=bold∇p+μ2bold-italicu+bold-italicF, where μ is the dynamic viscosity. The discretized LBM model for the electric field is [3537,40]: hifalse(bold-italicxbold+bold-italicci,s+1false)hifalse(bold-italicx,sfalse)=1τΨfalse[hifalse(bold-italicx,sfalse)hieqfalse(bold-italicx,sfalse)false]+ωiρeϵ with hieq=ωiΨ,1emΨ=ihi, τΨ=3χ+12, where hi…”
Section: Mathematical Models and Lattice Boltzmann Methods Implementationmentioning
confidence: 99%
“…where μ is the dynamic viscosity. The discretized LBM model for the electric field is [35][36][37]40]:…”
Section: Mathematical Models and Lattice Boltzmann Methods Implementationmentioning
confidence: 99%
“…The Poisson equation is the partial differential equation. From which, the electrical field can be derived [18,19,22,23,27] 2Ψ=ρeϵ, where Ψ is the electric potential, ρ e is the volumetric charge density and ϵ is the dielectric constant of the material. To solve the Poison equation with the LBM, a fictive time-dependent term is added and the equation becomes normal∂Ψnormal∂t=χ2Ψ+ρeϵ. Introducing a parameter χ , which depends on the dielectric constant of the material, different dielectric material can be simulated.…”
Section: Mathematical and Numerical Modelsmentioning
confidence: 99%
“…To obtain the appropriate values such as electric field intensity on the curving electrode surface, the physical boundary node x b (as shown in Figure 2) on the electrode surface is inserted between the solid node x s and the fluid node x f (Chen et al , 2015). The node values of x b is calculated using the linear interpolation scheme, and the fraction of the intersected line in the solid domain region is Δ = | x s − x b |/ | x s − x f |.…”
Section: Mathematical Modelmentioning
confidence: 99%
“…Zhang and Kwok (2005) investigated the EHD drop deformation affected by an electric field. In addition, Oulaid et al (2013) and Chen et al (2015, 2016) developed the novel and accurate boundary treatments of LBM to electrokinetic flow with complex boundaries. In this research works, the electrostatic potential in a liquid electrolyte solution is solved by the electric double layer theory and the Poisson–Boltzmann equation.…”
Section: Introductionmentioning
confidence: 99%