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Numerical Heat Transfer, Part B: Fundamentals
An International Journal of Computation and Methodology
Volume 70, 2016 - Issue 4
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Original Articles

Numerical modeling of interfacial heat and mass transport phenomena during a phase change using ANSYS-Fluent

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Pages 322-339 | Received 23 May 2016, Accepted 23 Jun 2016, Published online: 06 Oct 2016
 

ABSTRACT

Numerical modeling of phase change requires accurate estimations of heat and mass transport at the interface. The present work develops a model in ANSYS-Fluent with user-defined functions to address phase change with a planar interface. An interface boundary method determines the heat fluxes with the exact location of the interface without interpolation functions. Five cases are analyzed based on the classic Stefan problem for validating the model. The numerical model is validated against closed form theoretical solutions with agreement within 0.55%. This work can be extended to include curvature effects and the interaction between the interface and heterogeneous surfaces.

Nomenclature

Aint=

interface area in the cell (m2)

cp=

specific heat (J/kg K)

dT=

superheat/subcooled level (K)

dy=

cell length (m)

F1=

phase 1 volume of fraction

=

source term in the enthalpy equation (W/m3)

k=

thermal conductivity (W/m-K)

L=

latent heat of evaporation (J/kg)

l=

domain length (m)

p=

pressure (N/m2)

T=

temperature (K)

t=

time (s)

u=

velocity (m/s)

Vcell=

cell volume (m3)

Y=

analytic interface displacement (m)

y=

y-coordinate (m)

α=

thermal diffusivity (m2/s)

λ=

growth rate constant

μ=

dynamic viscosity (Pa s)

ν=

ratio of thermal diffusivities between phases

ρ=

density (kg/m3)

=

mass source term (kg/s m3)

ϕ=

ratio of densities between phases

Nomenclature

Aint=

interface area in the cell (m2)

cp=

specific heat (J/kg K)

dT=

superheat/subcooled level (K)

dy=

cell length (m)

F1=

phase 1 volume of fraction

=

source term in the enthalpy equation (W/m3)

k=

thermal conductivity (W/m-K)

L=

latent heat of evaporation (J/kg)

l=

domain length (m)

p=

pressure (N/m2)

T=

temperature (K)

t=

time (s)

u=

velocity (m/s)

Vcell=

cell volume (m3)

Y=

analytic interface displacement (m)

y=

y-coordinate (m)

α=

thermal diffusivity (m2/s)

λ=

growth rate constant

μ=

dynamic viscosity (Pa s)

ν=

ratio of thermal diffusivities between phases

ρ=

density (kg/m3)

=

mass source term (kg/s m3)

ϕ=

ratio of densities between phases

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