Abstract
In this article, a new mathematical model, based on the modified enthalpy formulation of Two-Phase Mixture Model (TPMM), is developed by considering non-Darcy flow and Local Thermal Non-Equilibrium (LTNE) conditions to describe numerically the two-dimensional problems of the complete evaporation process inside an asymmetrically heated porous evaporator. The governing equations have been discretised using Finite Volume Method (FVM) on a fixed non-staggered grid layout. The in-house code has been validated against experimental data and the results show good agreement between them. Three different models have been employed for the partitioning of the wall heat flux. Only the effect of the heat flux has been analysed, while all other parameters and properties have been kept fixed during the present investigation. The numerical simulations indicated that the locally high heat flux significantly influences the working fluid flow performances, and lead to extend the superheated vapour region towards the exit of the evaporator. The results also show that the two-phase zone significantly expanded in the axial direction and does not occupy a large portion inside the channel due to the energy transport through the two-phase region is significantly higher in the flow direction as compared to the transverse direction, caused by the decrease in the effective diffusion coefficient in this region and higher axial velocity. Numerical analysis reveal that the different models for the partitioning of the wall heat flux have almost no influence on the overall predictions, except in the vicinity of the wall. The results clearly demonstrate that the numerical simulations with the modified h-formulation by considering non-Darcy law and LTNE model are indispensable for the problem of complete evaporation process, particularly under the high both heat flux and inlet velocity conditions.
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Notes
Difference of about 3.5 °C has been reported by Alomar et al. [6] for the maximum wall heat flux case.
This assumption is valid only for negligible pressure drop through the evaporator, which is true for low mass flow rate applications, as in the present case.
This model assumes that the solid and the fluid phases are in thermal non-equilibrium with each other and they coexist at different temperature in all three regions.
This term an important factor that has the largest impact on growth of the two-phase region, especially in the case that the temperature of the solid phase exceeds the saturation temperature.
α = l and α = v for liquid and vapour phases, respectively.
Based on the pore diameter, the phase velocities and the properties of the local phase.
The numerical values of the recommended parameters may be found in Alomar et al. [2] and hence they are not repeated here for the sake of brevity.
The exit length has been carefully chosen in order to avoid the influence of exit boundary condition on the internal solution.
The lower and the upper values correspond to the properties of vapour (\( {k}_f^{\ast }={k}_v^{\ast } \)) and liquid (\( {k}_f^{\ast }={k}_l^{\ast } \)) phases, respectively [6].
Abbreviations
- a s :
-
Specific surface of the porous medium, 1/m
- b :
-
Body force vector per unit mass, m/s2
- \( \tilde{\mathbf{b}} \) :
-
Normalized body force vector per unit mass =b/g
- C p :
-
Specific heat, J/kgK
- d p :
-
Characteristic pore size of porous matrix, m
- D :
-
Capillary diffusion coefficient, m2/s
- ev :
-
Total evaporated volume fraction
- f :
-
Hindrance function
- Fr :
-
Froude number \( ={u}_{in}/{u}_g={u}_{in}/\sqrt{g\;W}=R{e}_{in}/R{e}_g \)
- g :
-
Acceleration due to gravitational vector, m/s2
- h :
-
Specific enthalpy, J/kg
- h fg :
-
Latent heat of vaporization =hv, sat − hl, sat, J/kg
- h sα :
-
Convective heat transfer coefficient in the pores, W/m2K
- j :
-
Diffusive mass flux vector, kg/m2s
- J :
-
Capillary pressure function
- krl, krv :
-
Relative permeabilities for liquid and vapour, respectively
- k :
-
Thermal conductivity, W/mK
- K :
-
Permeability of porous matrix, m2
- l :
-
Length of individual segments, m
- L :
-
Length of the porous channel, m
- n :
-
Exponent of saturation in the expression for relative permeabilities
- p :
-
Effective pressure, Pa
- p c :
-
Capillary pressure, Pa
- Pe :
-
Peclet number =uinW/α = RePr
- Pr :
-
Prandtl number =μ Cp/k
- \( {\dot{q}}^{\hbox{'}\hbox{'}} \) :
-
Heat flux, W/m2
- Q ∗ :
-
Normalized heat flux \( ={\dot{q}}^{\hbox{'}\hbox{'}}W/\mu {h}_{fg} \)
- \( {\dot{q}}_{sf}^{\hbox{'}\hbox{'}\hbox{'}} \) :
-
Heat exchange term between fluid and solid phases, W/m3
- Re :
-
Reynolds number =uinW/ν
- Re g :
-
Gravitational Reynolds number=ugW/νl
- Re p :
-
Reynolds number based on pore diameter and local phase properties
- Re K :
-
Fluid Reynolds number based on the length scale of the permeability
- s :
-
Liquid saturation
- T :
-
Temperature, K
- u :
-
Velocity component vector, m/s
- u g :
-
Gravitational velocity vector \( \sqrt{\mathbf{g}\;W},\mathrm{m}/\mathrm{s} \)
- W :
-
Height of the duct, m
- x, y :
-
horizontal and vertical Coordinates, respectively, m
- α :
-
Thermal diffusivity =k/ρ Cp, m2/s
- β :
-
Isobaric expansion coefficient, K−1
- ΔT :
-
Temperature difference for relaxation of Γh is in the single-phase regions, K
- Δρ :
-
Difference in densities=(ρl − ρv), kg/m3
- γ h :
-
Advection correction coefficient
- Γ h :
-
Diffusion coefficient in enthalpy equation, kg/m s
- ε :
-
Porosity
- λ :
-
Relative mobility
- μ :
-
Dynamic viscosity, kg/ms
- ν :
-
Kinematics viscosity, m2/s
- ρ :
-
Density, kg/m3
- σ :
-
Surface tension, N/m
- \( \tilde{\sigma} \) :
-
Normalized surface tension coefficient \( ={\rho}_l\sigma W/{\mu}_l^2 \)
- eff :
-
Effective
- f :
-
Fluid
- i, e, h :
-
Inlet, exit and heated, respectively
- in :
-
Inlet
- k :
-
Kinetic
- l :
-
Liquid
- max:
-
Maximum value
- min:
-
Minimum value
- s :
-
Solid
- sat :
-
Saturation
- v :
-
Vapour
- w :
-
Wall
- *:
-
Dimensionless
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Highlights
• Complete phase change process inside porous media has been considered.
• Modified enthalpy formulation has been used including the non-Darcian effects along with local thermal non-equilibrium model.
• Conservation equations have been solved by finite volume method on non-staggered grid layout.
• Two dimensional phase change problem is considered as demonstrative example.
• Smoothing of effective diffusion coefficient is required as remedy.
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Alomar, O.R. Numerical investigation of two-phase flow in a horizontal porous evaporator with localised heating using non-Darcian flow and two equations model. Heat Mass Transfer 56, 1203–1221 (2020). https://doi.org/10.1007/s00231-019-02784-x
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DOI: https://doi.org/10.1007/s00231-019-02784-x