1.5cm application of open-source cfd package (openfoam) …

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Application of open-source CFD package (OpenFOAM) to membrane distillation modeling Albert S. Kim 1* , Siu Fung Tang 1 (UG), Ho-Saeng Lee 2 , Deok-Soo Moon 2 , Hyeon-Ju Kim 2 1 Department of Civil and Environmental Engineering, University of Hawai‘i at Manoa, Honolulu, Hawai‘i, USA 2 Korea Research Institute of Ships & Ocean Engineering, Republic of Korea Introduction I Membrane Distillation (MD) is an anisothermal separation process where vapor molecules are thermally driven due to the partial pressure gradient. I What are the advantages of MD as compared to reverse osmosis? MD 1. requires less operating energy for pressure 2. requires lower footprint than conventional distillation processes 3. is insensitive to (high) feed concentration 4. can be (easily) operated using renewable (solar) energy I What are the current issues in MD research & development? 1. Design of membranes and modules 2. Wetting prevention through membrane pores 3. Lower permeate flux and membrane fouling 4. Cost analysis for energy supply and optimized operation Vacuum Membrane Distillation (VMD) I Hot feed stream is in contact with the membrane interface, and the permeate side is maintained near a vacuum condition, i.e., about 0.03 atm. I VMD can produce fresh water and recover precious volatile chemicals (1,2) . Figure 1: Schematic diagram of VMD system. I Hot feed stream enters the module system from the right side and leaves to the left side. The distillate stream of generated vapor molecules leaves the top part of the module to the right side. The unidirectional-stream flows maintain the transmembrane pressure gradient pseudo-constant. Recent Research Activities Figure 2: The MD and VMD publication numbers over years. Measurable flux across porous membrane I Vapor mass flux is indirectly considered as the convective heat flux, which allows us to predict the overall performance of VMD. I The effective heat transfer equation may be Q m = Q conductive + Q convective (1) = -κ m (κ s ,) T - 4 3 d p (νH w ) (2) = - ˜ κ m (κ s , , T ) T (3) where ν and H w are the incidence rate and evaporation enthalpy of vapor molecules. OpenFOAM’s Application on VMD I OpenFOAM stands for "Open source Field Operation and Manipulation (3) ." I OpenFOAM is a C++ toolbox for continuum mechanics problems, including CFD with the development of customized numerical solvers and pre-/post-processing utilities. I The necessary setups for performing calculations on VMD are following: (1) mesh generation (2) setting up boundary conditions (3) running simulations and visualization (4) heat flux calculations (1) mesh generation Figure 3: VMD sample mesh. Rectangular meshes for VMD simulations were generated using blockMesh and snappyHexMesh. Figure 4: Boundary regions of the computational domain. The mesh consists of five regions: topAir, membrane, bottomWater, leftSolid, and rightSolid. (2) setting up boundary conditions Table 1: Boundary conditions of major regions I Boundaries of leftSolid and rightSolid are CoupledTemperature in contact with the membrane; otherwise zeroGradient. (3) running simulations and visualization Figure 5: Postprocess visualization using ParaView (4) : variation of regional temperatures (T ) and their gradient normal to the membrane surface (T ). (4) heat flux calculations I Two cases are run to calculate the convective heat flux, Q convective : Q convective = Q permbl - Q imperm (4) where Q permbl = Q m and Q imperm = Q conductive . I In the impermeable case, pores are completely blocked. I In the permeable case, pores are open for heat convection. Figure 6: Heat flux vs. feed temperature for porosities of ε =0.75 & ε =0.65. I Conductive heat transfer rates (of the impermeable cases) are negligible in VMD operations, and hence most heat fluxes are due to the migration of vapor molecules, carrying their latent heat (i.e., evaporation enthalpy) (5) . Concluding Remarks 1. An OpenFOAM method to simulate VMD is successfully developed. 2. Transmembrane mass transfer of vapor molecules is transformed to a difference between heat transfer rates of permeable and impermeable membranes, having the same intrinsic thermal conductivity. 3. This method has a great potential to design VMD systems in module and pilot scales, including complex fluid flow. References 1. Desalination, 410 (2017) 77–90. 2. Desalination and Water Treatment, 58 (2017) 351–359. 3. OpenFOAM: http://openfoam.org and http://oepnfoam.com 4. ParaView: https://www.paraview.org/ 5. Journal of Membrane Science, 455 (2014) 168–186. Acknowledgements

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Page 1: 1.5cm Application of open-source CFD package (OpenFOAM) …

Application of open-source CFD package (OpenFOAM)to membrane distillation modeling

Albert S. Kim1∗, Siu Fung Tang1 (UG), Ho-Saeng Lee2, Deok-Soo Moon2, Hyeon-Ju Kim2

1Department of Civil and Environmental Engineering, University of Hawai‘i at Manoa, Honolulu, Hawai‘i, USA2Korea Research Institute of Ships & Ocean Engineering, Republic of Korea

Introduction

I Membrane Distillation (MD) is an anisothermal separation process wherevapor molecules are thermally driven due to the partial pressure gradient.

I What are the advantages of MD as compared to reverse osmosis? MD1. requires less operating energy for pressure2. requires lower footprint than conventional distillation processes3. is insensitive to (high) feed concentration4. can be (easily) operated using renewable (solar) energy

I What are the current issues in MD research & development?1. Design of membranes and modules2. Wetting prevention through membrane pores3. Lower permeate flux and membrane fouling4. Cost analysis for energy supply and optimized operation

Vacuum Membrane Distillation (VMD)

I Hot feed stream is in contact with the membrane interface, and thepermeate side is maintained near a vacuum condition, i.e., about 0.03 atm.

I VMD can produce fresh water and recover precious volatile chemicals(1,2).

Figure 1: Schematic diagram of VMD system.

I Hot feed stream enters the module system from the right side and leavesto the left side. The distillate stream of generated vapor molecules leavesthe top part of the module to the right side. The unidirectional-stream flowsmaintain the transmembrane pressure gradient pseudo-constant.

Recent Research Activities

Figure 2: The MD and VMD publication numbers over years.

Measurable flux across porous membrane

I Vapor mass flux is indirectly considered as the convective heat flux, whichallows us to predict the overall performance of VMD.

I The effective heat transfer equation may be

Qm = Qconductive +Qconvective (1)= −κm (κs, ε)∇T −

4

3dp∇ (νHw) (2)

= −κ̃m (κs, ε, T )∇T (3)where ν and Hw are the incidence rate and evaporation enthalpy of vapormolecules.

OpenFOAM’s Application on VMD

I OpenFOAM stands for "Open source Field Operation and Manipulation(3)."I OpenFOAM is a C++ toolbox for continuum mechanics problems,

including CFD with the development of customized numerical solvers andpre-/post-processing utilities.

I The necessary setups for performing calculations on VMD are following:(1) mesh generation(2) setting up boundary conditions(3) running simulations and visualization(4) heat flux calculations

(1) mesh generation

Figure 3: VMD sample mesh. Rectangular meshes for VMD simulations weregenerated using blockMesh and snappyHexMesh.

Figure 4: Boundary regions of the computational domain. The mesh consists offive regions: topAir, membrane, bottomWater,

leftSolid, and rightSolid.

(2) setting up boundary conditions

Table 1: Boundary conditions of major regions

I Boundaries of leftSolid and rightSolid are CoupledTemperature incontact with the membrane; otherwise zeroGradient.

(3) running simulations and visualization

Figure 5: Postprocess visualization using ParaView(4): variation of regionaltemperatures (T ) and their gradient normal to the membrane surface (∇T ).

(4) heat flux calculations

I Two cases are run to calculate the convective heat flux, Qconvective:

Qconvective = Qpermbl −Qimperm (4)where Qpermbl = Qm and Qimperm = Qconductive.I In the impermeable case, pores are completely blocked.I In the permeable case, pores are open for heat convection.

Figure 6: Heat flux vs. feed temperature for porosities of ε = 0.75 & ε = 0.65.

I Conductive heat transfer rates (of the impermeable cases) are negligible inVMD operations, and hence most heat fluxes are due to the migration ofvapor molecules, carrying their latent heat (i.e., evaporation enthalpy)(5).

Concluding Remarks

1. An OpenFOAM method to simulate VMD is successfully developed.2. Transmembrane mass transfer of vapor molecules is transformed to a

difference between heat transfer rates of permeable and impermeablemembranes, having the same intrinsic thermal conductivity.

3. This method has a great potential to design VMD systems in module andpilot scales, including complex fluid flow.

References

1. Desalination, 410 (2017) 77–90.2. Desalination and Water Treatment, 58 (2017) 351–359.3. OpenFOAM: http://openfoam.org and http://oepnfoam.com

4. ParaView: https://www.paraview.org/5. Journal of Membrane Science, 455 (2014) 168–186.

Acknowledgements