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Colloid and Interface Lab Department of Chemical Engineering HONGIK UNIVERSITY
Miok Ko†, Jennifer Moon ‡, and Won Ryoo†*
†Department of Chemical Engineering, Hongik University, 72-1 Sangsu-Dong, Mapo-Ku, Seoul 121-791, Korea
& ‡Department of Chemical and Biological Engineering, 596 UCB, University of Colorado, Boulder, CO, 80309-0596, USA
Introduction
Conclusions
ExperimentsTheory
• Increased oil prices and global warming calls for the development
of renewable energy.
• Entropy of mixing may be a novel source of energy.
• Reverse Electro Dialysis (RED) is a non-polluting technology
used to recover energy from the entropy of mixing.
• Currently, renewable energy occupies only 3% of total energy
production in Korea.
• Solar, wind, and hydro- power systems have been the focus thus far.
• Ion transport direction is controlled through use of anion and
cation exchange membranes.
• Brine and fresh water are brought into contact thru an alternating
series of anion exchange membranes (AEM) and cation exchange
membranes (CEM).
• The concentration difference between the solutions forces anions
and cations to migrate through the AEMs and CEMs.
• Space charging produces a potential difference that can be
recovered as electrical energy.
• Electricity is generated from the oxidation of Fe2+ and reduction
of Fe3+ at the anode and cathode, respectively.
Entropy of mixing effect
Selective ion transfer in AEM and CEM
• Explore the possibility of recovering energy from
the controlled mixing of salt and fresh water
• Develop and characterize RED stacked cells with
commercial ion exchange membranes
• Optimize the structure of the RED stacked cell to
maximize power output by varying channel thickness
and electrode material
Theory of electrical potential and current
V1.0
5.000.1
3599.0
ln
C/mol96485
K298J/molK314.892.0
]Na[
]Na[
ln 
















 

rightL
leftH
oc
zF
RT
V


• Nernst equation for electrical potential across a membrane (open-circuit voltage)
• Nernst-Planck equation for ionic current








dx
dV
RT
zF
dx
d
DJ eff
]Na[]Na[
dA
x
FDi effsc  



]Na[
Whr286.0
kJ03.1

 STHG


4
6
3
6 Fe(CN)eFe(CN)
Lumped-parameter Modeling
• Stacking resulted in linear increase in open circuit voltage. (~0.09 V/membrane)
• The short circuit current increased linearly with effective membrane area.
• High flowrates lead to increased short circuit current due to the reduction in concentration polarization
adjacent membrane surfaces.
• The maximum in short circuit current was limited by the ion transport in the ion exchange membraned
• The channel thickness was the most crucial factor in RED performance.
17 g NaCl/L
Fresh Water
1 L
Sea water
34 g NaCl/L
1L
Low entropy
High entropy
Energy consumed
for separation
Free energy
recovery
Renewable Energy Status (%) in S. Korea, 2011
Background
Objectives
AEM CEM
Principles of RED
Ion flux Short circuit current
• Boundary condition (BC)
» Uniform Concentration at Inlet:
• Model for convective diffusion
Reverse Electro Dialysis Equivalent Circuit Model (ECM)
• An ideal RED system can be described as an ECM.
• Concentration gradient is not uniform throughout
membrane area
• Curved streamline with a velocity field makes it
difficult to model
• Corner areas are not fully utilized
• Ion exchange membrane samples
Channel design of previous study
• Uniform concentration gradient develops along flow direction
• Straight streamline enables simplified modeling
• Ions may migrate through the entire area of membrane
Improved channel design of this study
Schematic representation of RED
e-
e-
e-
  02  LH
L
z CC
D
β
dz
dC
bV

  02  LH
H
z CC
D
β
dz
dC
bV
 thicknessmembrane
tcoefficiendiffusionD
fractionareaopenmeshβ
velocitylsuperficiaV
thicknessspacerb
z






2
where
• Local concentration
00 HZH CC 
00 LZL CC 
bV
Dz
LHLH
H
z
e
CCCC
C 






 





 

22
0000
bV
Dz
LHLH
L
z
e
CCCC
C 






 





 

22
0000
• Short circuit current
dA
CC
FDi LH
sc  




 



 










bV
DL
LHzsc
z
eCCFwbVi 

100
ntcoeffictiediffusionD
constantfaradayF
areaopeningmeshβ
thicknessspacerb



2
thicknessmembrane
widthmembranew
areamembraneA




where
Re Re
Rsp Rsp
Rf=R(AEM)+R(fresh water channel)
Rs=R(CEM)+R(sea water channel)
Rfp=R(parasitic resistance of fresh water channel)
Rsp=R(parasitic resistance of sea water channel)
Rssp=R(parasitic resistance of sea water slit)
Rsfp=R(parasitic resistance of fresh water slit)
Re=R(electrode)
Rs
Load resistance
Voltmeter
V
AmmeterA
RCEMRs
Rfp
Rf Rf
R
Rfp
RfRs
fresh water
sea water
Anode Cathode
CEM CEM CEM CEMAEM AEM AEM
Repeating unit
Rs Rf
Rfp
CEM AEM
Rsp
Rssp Rssp Rssp Rssp
Rsfp Rsfp Rsfp Rsfp
• Experimental conditions
0
0.5
1
1.5
2
2.5
3
0.0 1.0 2.0 3.0
Pmax(W)
CL (g/L)
0.0
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
0.0
0.1
0.2
0.3
0.4
0.5
0.0 1.0 2.0 3.0
isc(A)
Vocperpaircell(V)
CL (g/L)
Voc/units
isc
0 10 20 30 40 50 60 70 80
China
USA
Germany
Japan
Canada
India
UK
France
Brazil
Australia
Korea
RECAI Rank
Countries
Ranking of Countries Based on RE Capacity,
2013
(New & Renewable Energy Center, KEMCO, 2013)
(Adapted from Global Cleantech Center, 2014)
Fresh Water Concentration Simulation Results
Results & Discussion
Concentration (g/L) Diffusion coefficient * 106 (cm2/s) Membrane
thickness
(mm)
Mean
velocity
(Ṽ, cm/s)
Membrane dimension Channel
thickness
(2b, mm)
Sea water
(CH)
Fresh water
(CL)
In-Water
(DW)
In-Membrane
(DM)
Width
(W, cm)
Length
(L, cm)
35 0.5 13.3 0.2~0.5 0.08 ~ 0.11 0.5 ~ 25 5 5 0.1 ~ 0.2
• RED cell design
• Press-cutter design for IEM and spacers
• RED Characterization apparatus
• Linear I-V characteristics,
thus maximum power
performance at the mid
point observed for stack
cells of 5 pair AEM/CEM.
• The maximum power
density measured as high
as 2.2 W/m2 for
synthesized membranes.
• The power performance
increased with an increase
in flowrate due to the
reduction in concentration
polarization.

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KIChE RED Poster 20151021

  • 1. Colloid and Interface Lab Department of Chemical Engineering HONGIK UNIVERSITY Miok Ko†, Jennifer Moon ‡, and Won Ryoo†* †Department of Chemical Engineering, Hongik University, 72-1 Sangsu-Dong, Mapo-Ku, Seoul 121-791, Korea & ‡Department of Chemical and Biological Engineering, 596 UCB, University of Colorado, Boulder, CO, 80309-0596, USA Introduction Conclusions ExperimentsTheory • Increased oil prices and global warming calls for the development of renewable energy. • Entropy of mixing may be a novel source of energy. • Reverse Electro Dialysis (RED) is a non-polluting technology used to recover energy from the entropy of mixing. • Currently, renewable energy occupies only 3% of total energy production in Korea. • Solar, wind, and hydro- power systems have been the focus thus far. • Ion transport direction is controlled through use of anion and cation exchange membranes. • Brine and fresh water are brought into contact thru an alternating series of anion exchange membranes (AEM) and cation exchange membranes (CEM). • The concentration difference between the solutions forces anions and cations to migrate through the AEMs and CEMs. • Space charging produces a potential difference that can be recovered as electrical energy. • Electricity is generated from the oxidation of Fe2+ and reduction of Fe3+ at the anode and cathode, respectively. Entropy of mixing effect Selective ion transfer in AEM and CEM • Explore the possibility of recovering energy from the controlled mixing of salt and fresh water • Develop and characterize RED stacked cells with commercial ion exchange membranes • Optimize the structure of the RED stacked cell to maximize power output by varying channel thickness and electrode material Theory of electrical potential and current V1.0 5.000.1 3599.0 ln C/mol96485 K298J/molK314.892.0 ]Na[ ]Na[ ln                     rightL leftH oc zF RT V   • Nernst equation for electrical potential across a membrane (open-circuit voltage) • Nernst-Planck equation for ionic current         dx dV RT zF dx d DJ eff ]Na[]Na[ dA x FDi effsc      ]Na[ Whr286.0 kJ03.1   STHG   4 6 3 6 Fe(CN)eFe(CN) Lumped-parameter Modeling • Stacking resulted in linear increase in open circuit voltage. (~0.09 V/membrane) • The short circuit current increased linearly with effective membrane area. • High flowrates lead to increased short circuit current due to the reduction in concentration polarization adjacent membrane surfaces. • The maximum in short circuit current was limited by the ion transport in the ion exchange membraned • The channel thickness was the most crucial factor in RED performance. 17 g NaCl/L Fresh Water 1 L Sea water 34 g NaCl/L 1L Low entropy High entropy Energy consumed for separation Free energy recovery Renewable Energy Status (%) in S. Korea, 2011 Background Objectives AEM CEM Principles of RED Ion flux Short circuit current • Boundary condition (BC) » Uniform Concentration at Inlet: • Model for convective diffusion Reverse Electro Dialysis Equivalent Circuit Model (ECM) • An ideal RED system can be described as an ECM. • Concentration gradient is not uniform throughout membrane area • Curved streamline with a velocity field makes it difficult to model • Corner areas are not fully utilized • Ion exchange membrane samples Channel design of previous study • Uniform concentration gradient develops along flow direction • Straight streamline enables simplified modeling • Ions may migrate through the entire area of membrane Improved channel design of this study Schematic representation of RED e- e- e-   02  LH L z CC D β dz dC bV    02  LH H z CC D β dz dC bV  thicknessmembrane tcoefficiendiffusionD fractionareaopenmeshβ velocitylsuperficiaV thicknessspacerb z       2 where • Local concentration 00 HZH CC  00 LZL CC  bV Dz LHLH H z e CCCC C                  22 0000 bV Dz LHLH L z e CCCC C                  22 0000 • Short circuit current dA CC FDi LH sc                        bV DL LHzsc z eCCFwbVi   100 ntcoeffictiediffusionD constantfaradayF areaopeningmeshβ thicknessspacerb    2 thicknessmembrane widthmembranew areamembraneA     where Re Re Rsp Rsp Rf=R(AEM)+R(fresh water channel) Rs=R(CEM)+R(sea water channel) Rfp=R(parasitic resistance of fresh water channel) Rsp=R(parasitic resistance of sea water channel) Rssp=R(parasitic resistance of sea water slit) Rsfp=R(parasitic resistance of fresh water slit) Re=R(electrode) Rs Load resistance Voltmeter V AmmeterA RCEMRs Rfp Rf Rf R Rfp RfRs fresh water sea water Anode Cathode CEM CEM CEM CEMAEM AEM AEM Repeating unit Rs Rf Rfp CEM AEM Rsp Rssp Rssp Rssp Rssp Rsfp Rsfp Rsfp Rsfp • Experimental conditions 0 0.5 1 1.5 2 2.5 3 0.0 1.0 2.0 3.0 Pmax(W) CL (g/L) 0.0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 0.0 0.1 0.2 0.3 0.4 0.5 0.0 1.0 2.0 3.0 isc(A) Vocperpaircell(V) CL (g/L) Voc/units isc 0 10 20 30 40 50 60 70 80 China USA Germany Japan Canada India UK France Brazil Australia Korea RECAI Rank Countries Ranking of Countries Based on RE Capacity, 2013 (New & Renewable Energy Center, KEMCO, 2013) (Adapted from Global Cleantech Center, 2014) Fresh Water Concentration Simulation Results Results & Discussion Concentration (g/L) Diffusion coefficient * 106 (cm2/s) Membrane thickness (mm) Mean velocity (Ṽ, cm/s) Membrane dimension Channel thickness (2b, mm) Sea water (CH) Fresh water (CL) In-Water (DW) In-Membrane (DM) Width (W, cm) Length (L, cm) 35 0.5 13.3 0.2~0.5 0.08 ~ 0.11 0.5 ~ 25 5 5 0.1 ~ 0.2 • RED cell design • Press-cutter design for IEM and spacers • RED Characterization apparatus • Linear I-V characteristics, thus maximum power performance at the mid point observed for stack cells of 5 pair AEM/CEM. • The maximum power density measured as high as 2.2 W/m2 for synthesized membranes. • The power performance increased with an increase in flowrate due to the reduction in concentration polarization.