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Numerical Heat Transfer, Part B: Fundamentals
An International Journal of Computation and Methodology
Volume 71, 2017 - Issue 3
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Original Articles

Hybrid atomistic-continuum simulation of nucleate boiling with a domain re-decomposition method

, , &
Pages 217-235 | Received 02 Sep 2016, Accepted 28 Nov 2016, Published online: 27 Mar 2017
 

ABSTRACT

In this study, a domain re-decomposition hybrid atomistic-continuum method is developed to conduct a multiscale/multiphase investigation on the bubble nucleation. In addition to the conventional coupling scheme, this method is capable of re-partitioning the molecular and continuum domains once it is necessary during the simulation. Giving the fact that the accurate modeling of interface tracking and phase change are still problematic for continuum mechanics on microscale, our coupling method directly avoids these issues since CFD domain takes care of a single-phase flow while the molecular domain simulates the bubble growth.

Nomenclature

Aj=

cross-section area

Cp=

heat capacity

E=

Lennard–Jones potential energy

f=

conservative force on atom

I=

identity matrix

k=

Boltzmann constant

m=

mass of atom

N=

total number of atoms

P=

atoms number to be inserted

r=

distance between two atoms

rc=

cutoff distance

=

average velocity of molecules

uif=

normal velocity at the boundary of CFD

=

atoms initial average potential energy

=

atoms average potential energy at time t

v=

velocity

V=

region volume

ε=

depth of potential well

μ=

dynamic viscosity

ρ=

fluid density

σ=

zero-crossing distance for the potential

τ=

coupling interval

Subscripts=
i=

cell index i

j=

atom index j

l=

liquid

Nomenclature

Aj=

cross-section area

Cp=

heat capacity

E=

Lennard–Jones potential energy

f=

conservative force on atom

I=

identity matrix

k=

Boltzmann constant

m=

mass of atom

N=

total number of atoms

P=

atoms number to be inserted

r=

distance between two atoms

rc=

cutoff distance

=

average velocity of molecules

uif=

normal velocity at the boundary of CFD

=

atoms initial average potential energy

=

atoms average potential energy at time t

v=

velocity

V=

region volume

ε=

depth of potential well

μ=

dynamic viscosity

ρ=

fluid density

σ=

zero-crossing distance for the potential

τ=

coupling interval

Subscripts=
i=

cell index i

j=

atom index j

l=

liquid

Acknowledgment

The authors greatly appreciate the support of the Office of Naval Research under Grant No. N00014-14-1-0402.

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