Abstract

Modeling liquid-vapor phase change using the lattice Boltzmann (LB) method has attracted significant attention in recent years. In this paper, we propose an improved three-dimensional thermal multiphase LB model for simulating liquid-vapor phase change. The proposed model has the following features. First, it is still within the framework of the thermal LB method using a temperature distribution function and therefore retains the fundamental advantages of the thermal LB method. Second, in the existing thermal LB models for liquid-vapor phase change, the finite-difference computations of the gradient terms ∇·u and ∇T usually require special treatment at boundary nodes, while in the proposed thermal LB model these two terms are calculated locally. Moreover, in some of the existing thermal LB models, the error term ∂_{t_{0}}(Tu) is eliminated by adding local correction terms to the collision process in the moment space, which causes these thermal LB models to be limited to the D2Q9 lattice in two dimensions and the D3Q15 or D3Q19 lattice in three dimensions. Conversely, the proposed model does not suffer from such an error term and therefore the thermal LB equation can be constructed on the D3Q7 lattice, which simplifies the model and improves the computational efficiency. Numerical simulations are carried out to validate the accuracy and efficiency of the proposed thermal multiphase LB model for simulating liquid-vapor phase change.

Highlights

  • In the past three decades, the lattice Boltzmann (LB) method has been developed into a very efficient numerical methodology for simulating fluid flow and heat transfer [1,2,3,4,5,6]

  • The present model does not suffer from the error term caused by ∂t0 (T u) and the thermal LB equation can be constructed on the D3Q7 lattice

  • An improved 3D thermal multiphase LB model has been proposed for liquid-vapor phase change, which consists of a 3D pseudopotential LB model for simulating the density and velocity fields, and an improved thermal LB equation for modeling the temperature field

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Summary

INTRODUCTION

In the past three decades, the lattice Boltzmann (LB) method has been developed into a very efficient numerical methodology for simulating fluid flow and heat transfer [1,2,3,4,5,6]. Huang et al [32] recently devised a thermal multiphase LB model for liquid-vapor phase change by introducing a total-kinetic-energy-based thermal LB equation to recover the energy equation of nonideal fluids. Compared with the temperature-based thermal LB models mentioned in the second category, the total-energy-based and total-kinetic-energy-based thermal LB models usually have a simpler source term for simulating liquid-vapor phase change. There is no such a problem in the thermal multiphase LB models that utilize a temperature distribution function, in which the thermal boundary treatment does not involve the density This is the main reason why many researchers prefer to use a temperature-based thermal multiphase LB model to simulate liquid-vapor phase change.

THREE-DIMENSIONAL PSEUDOPOTENTIAL MULTIPHASE LB MODEL
IMPROVED 3D THERMAL LB MODEL
Target macroscopic temperature equation
Thermal LB-BGK equation
Thermal LB-MRT equation
NUMERICAL SIMULATIONS
Validation of the D2 law
Droplet evaporation on a heated surface
Bubble nucleation and departure
Findings
SUMMARY
Full Text
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