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i n t e r n a t i o n a l j o u r n a l o f h y d r o g e n en e r g y 3 7 ( 2 0 1 2 ) 1 6 5 5 7e1 6 5 6 9
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Towards integration of hydrolysis, decomposition andelectrolysis processes of the CueCl thermochemicalwater splitting cycle
Z. Wang*, V.N. Daggupati, G. Marin, K. Pope, Y. Xiong, E. Secnik, G.F. Naterer, K.S. Gabriel
Clean Energy Research Laboratory, Faculty of Engineering and Applied Science, University of Ontario Institute of Technology,
2000 Simcoe Street North, Oshawa, Ontario, Canada L1H 7K4
a r t i c l e i n f o
Article history:
Received 11 October 2011
Received in revised form
22 February 2012
Accepted 28 February 2012
Available online 28 April 2012
Keywords:
Thermochemical hydrogen
production
CueCl cycle
Process integration
* Corresponding author. Tel.: þ1 9057218668.E-mail addresses: [email protected],
uoit.ca (G. Marin), [email protected] (K. Pop(G.F. Naterer), [email protected] (K.S. G0360-3199/$ e see front matter Copyright ªdoi:10.1016/j.ijhydene.2012.02.172
a b s t r a c t
The thermochemical copperechlorine (CueCl) cycle is a promising technology that can
utilize various energy sources such as nuclear and solar energy to produce hydrogen with
minimal or no emissions of greenhouse gases. Past investigations have primarily focused
on the design and testing of individual unit operations of the CueCl cycle. This paper
investigates the chemical streams flowing through each individual process from the aspect
of system integration. The interactions between each of the two immediate upstream and
downstream processes are examined. Considering the integration of electrolytic hydrogen
production and cupric chloride hydrolysis steps, it is evident that an intermediate step to
concentrate CuCl2 and reduce HCl composition is required. Spray drying and crystalliza-
tion, serving as the intermediate steps, are examined from the aspects of energy require-
ments and viability of engineering. Regarding the integration of the hydrolysis and oxygen
production steps, thermodynamic and XRD analysis results are presented to study the
mutual impacts of these two steps on each other. Within the hydrolysis reactor, high
conversion of CuCl2 to Cu2OCl2 is preferable for the integration because it reduces the
release of chlorine gas during the oxygen production. Considering the integration of the
oxygen production step and electrolysis of CuCl, pulverization is needed for the solidified
CuCl. The recovery of CuCl vapour entrained in oxygen gas requires further research.
Residual CuCl2 introduced from the hydrolysis step into the oxygen production step may be
further entrained by CuCl into the electrolytic hydrogen production cell. Additionally,
thermal energy integration patterns are briefly discussed while integrating the various
chemical streams of the CueCl cycle. Steam generated from the heat recovery of cuprous
chloride can be introduced into the hydrolysis reactor to serve as a reactant.
Copyright ª 2012, Hydrogen Energy Publications, LLC. Published by Elsevier Ltd. All rights
reserved.
[email protected] (Z. Wang), [email protected] (V.N. Daggupati), gabriel.marin@e), [email protected] (Y. Xiong), [email protected] (E. Secnik), [email protected]).2012, Hydrogen Energy Publications, LLC. Published by Elsevier Ltd. All rights reserved.
i n t e rn a t i o n a l j o u r n a l o f h y d r o g e n en e r g y 3 7 ( 2 0 1 2 ) 1 6 5 5 7e1 6 5 6 916558
1. Introduction
It is becoming increasingly urgent to reduce greenhouse gas
(GHG) emissions and at the same time meet the growing
demand for a sustainable future of energy supply. Engineers
and scientists have developed innovative solutions, such as
solar, nuclear, hydroelectric, wind, and geothermal energy, to
meet the targets. Currently, electrical power grids are the
primary methods to distribute these energy forms to various
end users. However, some energy generation methods, such
as solar and wind energy, are intermittent with unstable and
highly variable power output. Sunlight is unavailable at night
and the irradiance magnitude varies monthly and seasonally.
For other energy forms, such as nuclear and geothermal, the
electricity output needs to follow the power demand on the
future power grid in order to reduce the portion of fossil fuel
based electricity on the grid. The power demand on the grid
varies on an hourly basis during the day. Therefore, it is
important to find a medium that can store and distribute the
intermittent and off-peak energy, hence reducing the “peaks
and valleys” to help achieve the demand following profile.
Hydrogen production at the intermittent and off-peak hours is
a promising option [1] because hydrogen has a higher energy
density than fossil fuels and its oxidization does not emit
GHGs [2].
Engineers and scientists have developed many technol-
ogies to produce hydrogen from clean energy. For example,
electrolysis utilizes electricity as the major input energy
form to split water, and thermochemical cycles utilize
thermal energy as the primary input form. Due to the
energy losses with electrolysis in the conversion of thermal
energy to electricity, thermochemical cycles have attracted
growing interest. Approximately 200 thermochemical
cycles of thermal water splitting that utilize various heat
sources have been reported previously [3]. Among these
cycles, the sulfureiodine (SeI) cycle is a leading example of
exclusively thermal cycles that has been scaled up from
proof-of-principle tests to a larger engineering scale facility
by the Japan Atomic Energy Agency (JAEA [4]). General
Atomics (GA [5]) developed an SeI hydrogen production
cycle capable of producing 2 kg of hydrogen per day.
Commissariat a l’energie atomique (CEA [6]) and the Sandia
National Laboratory (SNL [7]) have also extensively exam-
ined sulfur-based cycles. However, the minimum temper-
ature requirement of the SeI cycle is 850 �C, which can be
achieved by a very limited number of heat sources. Even the
temperatures of some Generation IV nuclear reactors, e.g.,
Table 1 e Chemical reactions of the copperechlorine cycle.
Reaction Process and heat flow
A Electrolysis for hydrogen production
B Hydrolysis of cupric chloride, endothermic
C Oxygen production, endothermic
Summation of all reactions
Symbols: aq, aqueous; g, gas; l, liquid; Q, heat; s, solid; VE, electricity.
supercritical water-cooled nuclear reactors [8], cannot
provide high enough temperatures.
In recent years, the copperechlorine (CueCl) cycle has
gained more attention due to its lower temperature require-
ment of 530 �C, which is about 300 �C lower than the SeI cycle.
The chemical reactions of the CueCl cycle are listed in Table 1.
Proof-of-principle experiments for each internal process have
been performed [9e11]. The experimental results have been
reported for most of the processes of the CueCl cycle, and
large laboratory scale reactors for the processes have been
tested successfully at UOIT (University of Ontario Institute of
Technology, Canada) [27]. Although the summation of the
reactions shown in Table 1 can form a closed cycle, most of
the past studies focused on individual reactors rather than an
integrated CueCl cycle with a holistic approach. Few past
studies have examined the mutual impacts between
upstream and downstream reactions.
This paper will present thermodynamic and experimental
studies of the interactions within the integrated system. This
paper will mainly discuss the engineering challenges and
solutions from the perspectives of chemical stream flows,
heat requirements and required processes. Other aspects
such as capital cost, economics, system hierarchy, process
control systems, and equipment materials will not be
considered in this paper. In particular, the chemical streams
across the boundaries between two contiguous steps of the
CueCl cycle will be quantified. The limitations and obstacles
to integration of current technologies for the various reactions
are analyzed for the system integration. The primary equip-
ment needed to process the chemical streams and facilitate
effective system integration is examined as well. The thermal
energy management aspects will also be discussed in the
paper.
2. Process integration of various reactions
2.1. Matching the chemical streams of electrolytichydrogen production and hydrolysis steps
As presented in Table 1, it can be observed that the output
stream from the electrolytic cell (reaction A) is an aqueous
solution of CuCl2, i.e., dissolved CuCl2 in water, which in
principle can directly provide water as the reactant for the
downstream hydrolysis step (reaction B). Since the tempera-
ture of the hydrolysis reaction is above 350 �C, the CuCl2 and
water reactants in the hydrolysis reaction can only exist in the
Major reaction
2CuCl (aq)þ 2HCl (aq)þVE¼H2 (g)þ 2CuCl2 (aq) in aqueous
solution, at 30e80 �C2CuCl2 (s)þH2O (g)þQ¼Cu2OCl2 (s)þ 2HCl (g), at 350e400 �CCu2OCl2 (s)þQ¼ 2CuCl (molten)þ 0.5O2 (g), at 500e530 �CH2O (l)¼H2 (g)þ 1/2O2 (g) (net reaction)
i n t e r n a t i o n a l j o u r n a l o f h y d r o g e n en e r g y 3 7 ( 2 0 1 2 ) 1 6 5 5 7e1 6 5 6 9 16559
form of solid and steam, respectively. To match the chemical
streams, the water in the aqueous solution must be evapo-
rated and then regulated to a favorable operating range
required by the hydrolysis reactor. Therefore, the following
three key questions must be answered for the process inte-
gration: (1) can the flow rate and chemical composition
leaving the electrolytic cell match the input requirements of
a hydrolysis reactor? (2) What magnitude of thermal energy
is required to evaporate the excess water? (3) should the
water be evaporated in the hydrolysis reactor? Since it is
water and cupric chloride streams that cross the boundary of
the two reactors, it is also convenient to reference their ratio,
i.e., the molar ratio of water-to-cupric chloride [9,13,14]. The
minimum water-to-cupric chloride ratio of the aqueous
solution leaving the electrolytic cell occurs at the saturation
state of solubility. The actual ratio is determined by the
operating concentrations of the electrolysis reaction. Consid-
ering the minimum ratio required by the hydrolysis reaction,
it is the stoichiometric ratio, i.e., 0.5. The actual ratio that can
be accommodated by the hydrolysis reactor is determined
from the expected conversion of CuCl2 to Cu2OCl2.
Fig. 1 illustrates amajor difference between the electrolytic
cell output stream and the required hydrolysis input. Table 2
presents the quantitative details of the differences. In Table 2,
the thermodynamic minimum ratio of water to CuCl2 in the
electrolytic cell occurs when all dissolved CuCl is fully
oxidized to CuCl2 at the anode side and all available protons
(Hþ) eventually move to the cathode side. The minimum
water-to-cupric chloride ratio for the downstream hydrolysis
process is 0.5, which is the same as the stoichiometric value.
Fig. 2 illustrates the equilibrium concentration of HCl for
the hydrolysis reaction in the temperature range below 700 �Cat the water-to-cupric chloride ratio of 0.5 and the total
system pressure of 1 bar (absolute). The equilibrium concen-
tration of HCl is calculated from the standard Gibbs energy of
the hydrolysis reaction, which is based on the standard Gibbs
formation energy of the products and reactants. Since the
specific heat used for the calculation of the standard Gibbs
formation energy of Cu2OCl2 has not been reported for above
400 �C [12], there are some discrepancies in the reported
values. Fig. 2 adopts extrapolation and sensitivity analysis for
the influence of the specific heat (�30%) on the Gibbs free
Fig. 1 e Gap between the output streams of the electrolytic cell
hydrolysis reactor.
energy of the hydrolysis reaction. Fig. 2 suggests that the
increase of the conversion of both CuCl2 and steam comes at
the cost of a temperature increase, which means that the
steam fraction in the products depends strongly on the
operating temperature of the hydrolysis reaction. To reach
a full conversion of CuCl2 to Cu2OCl2 at temperatures lower
than 400 �C, excess steam is needed, or the producedHClmust
be removed immediately to create a non-equilibrium condi-
tion. Another option for lowering the excess steam quantity is
to reduce the systemoperating pressure to below atmospheric
pressure, but thismay increase the challenge of reactor seal to
avoid the air entering the hydrolysis reactor.
In regards to the matching of the water-to-cupric chloride
ratio between hydrolysis and electrolysis, Table 2 shows that
the minimum output water-to-cupric chloride ratio of an
electrolytic cell is 7.5, which is 15 times the stoichiometric
requirement of hydrolysis. Also, in actual operation, it may be
very challenging for all of the protons to move to the cathode
side in the electrolytic cell, and HCl is also needed in order to
dissolve the reactant CuCl. Thus, there is still a concentration
of HCl at the anode side and the output stream is a ternary
system, assuming all CuCl is fully converted to CuCl2 on the
anode side. As a consequence, the water-to-cupric chloride
ratio in the hydrolysis reaction may exceed the thermody-
namic minimum value in practical operation, and HCl may
enter the hydrolysis reactor. Table 2 presents the water-to-
cupric chloride ratio considering the existence of HCl in the
output stream of the electrolytic cell versus the input
requirement of hydrolysis in proof-of-principle tests. It can be
found that the output water-to-copper chloride ratio of elec-
trolysis lies in the range of 17e34, which is 2e5 times the 7
required by hydrolysis. Practically, the output stream of the
electrolytic cell is more likely to be a quaternary system con-
sisting of water, CuCl2, HCl and CuCl due to the incomplete
conversion of CuCl. Table 2 also considers this situationwhere
the output water-to-copper ratio of the electrolysis increases
to the range of 55e270, which is 8e39 times the 7 required by
hydrolysis. Therefore, at least 2e5 times the stoichiometric
surpluswatermust be separated from the output stream of an
electrolytic cell to effectively integrate the electrolysis and
hydrolysis reactors if the electrolysis output stream directly
supplies the hydrolysis reactor. Otherwise, additional thermal
and the input streams that can be accommodated by the
0
10
20
30
40
50
60
70
80
90
100
0 100 200 300 400 500 600 700
Temperature of hydrolysis reaction, o
C
HC
l fra
ctio
n in
th
e H
Cl-
ste
am
mix
tu
re
, %
reported andextrapolated Cp+ 30% Cp
- 30% Cp
Fig. 2 e Equilibrium concentration of HCl in the hydrolysis
reaction with sensitivity analysis of specific heat of
Cu2OCl2 (steam/copper ratio[ 0.5, stoichiometric; total
system pressure[ 1 bar abs).
Table 2 e Output streams from an electrolytic cell and required input streams to hydrolysis reactor.
Operating parameters Output chemical streamsof electrolytic cell
Magnitude Input chemical streams that canbe accommodated by hydrolysis
Binary system Limit in thermodynamics (all Hþ
goes to cathode and CuCl is fully
converted to CuCl2)
Limit in thermodynamicsa
Water/CuCl2 molar ratio 7.5 (minimum) � 0.5
CuCl2, M 7.3 (maximum) N/A
T, �C 80 350e400
Ternary system Limit in ideal operation for CuCl
conversionc
(CuCl is fully converted to CuCl2)
Limit in proof-of-principle testsb
Water/CuCl2 molar ratio 17.7 (minimum) � 7.0
CuCl2, M 3.1 (maximum) N/A
HCl, M 5.3 (maximum) <30% 7.4 (maximum)
T, �C 25 350e400
Water/CuCl2 molar ratio 24.2 (minimum) � 7.0
CuCl2, M 2.3 (maximum) N/A
HCl, M 7.3 (maximum) z 7.4 (maximum)
T, �C 25 350e400
Water/CuCl2, molar ratio 33.5 (minimum) � 7.0
CuCl2, M 1.65 (maximum) N/A
HCl, M 11.8 (maximum) � 7.4 (maximum)
T, �C 25 350e400
Quaternary system Values in small lab-scale operations
(CuCl is fully converted to CuCl2)
Limit in proof-of-principle testsd
Water/CuCl2 molar ratio 55e270 � 7.0
CuCl2, M 0.2e1.0 N/A
HCl, M 6.0e11.0 Close or > 7.4 (maximum)
CuCl, M 0.2e2.0 Not known
T, �C 25 350e400
a The input minimum water-to-copper ratio is the stoichiometric value.
b The input minimum water-to-copper ratio was based on the proof-of-principle results of a fixed/fluidized bed and spray reactor [9,13,14].
c The output water-to-copper ratio was based on the 72-hour runtime data of a proof-of-principle electrolytic cell [10,11].
d The concentration of HCl in the hydrolysis product in this table is converted to an aqueous solution assuming the gaseous products are
condensed to an aqueous solution in order to be comparable with the input stream from the electrolytic cell.
i n t e rn a t i o n a l j o u r n a l o f h y d r o g e n en e r g y 3 7 ( 2 0 1 2 ) 1 6 5 5 7e1 6 5 6 916560
energy must be utilized to evaporate the water to steam. This
may reduce the thermal efficiency of the proposed CueCl
cycle.
Fig. 3 illustrates the heat transfer requirements of
a hydrolysis reactor if all required water is evaporated in the
reactor. When the water-to-cupric chloride ratio exceeds 1.5,
i.e., 3 times the stoichiometric requirement, the evaporation
heat requirement of water will exceed the reaction enthalpy.
As a consequence, the hydrolysis reactor will function more
like a steam generator. It is unclear whether the excess steam
requirement of hydrolysis is caused by thermodynamic or
kinetic limits. However, the water-to-cupric chloride ratio is
recommended to be below the transition point 1.5, so that the
heat transfer rate to the hydrolysis reactor is primarily
directed to the reaction enthalpy. Another option is to utilize
a separate steam generator. This can more readily control the
water-to-cupric chloride ratio to be close to the stoichiometric
value and provide more flexibility for the selection of reactor
types, because other intake forms of CuCl2, such as solid
powder and slurry, can be introduced into the hydrolysis
0
10
20
30
40
50
60
70
0.0 0.5 1.0 1.5 2.0water/CuCl2, molar ratio
Evaporation of water
Reaction Enthalpy
Assumptions: (1) All water is evaporated in the hydrolysis reactor.(2) Heat transfer efficiency is 100%.(3) Hydrogen production scale is 100 tonnes/day.
Fig. 3 e Comparative roles of reaction enthalpy and water
evaporation in the hydrolysis reactor.
i n t e r n a t i o n a l j o u r n a l o f h y d r o g e n en e r g y 3 7 ( 2 0 1 2 ) 1 6 5 5 7e1 6 5 6 9 16561
reactor. In addition, external water such as make-up water of
the CueCl cycle, rather than the water from the electrolytic
cell, can also be utilized. This will be studied in a later section
of this paper about the thermal energy integration. In
summary, it is crucial to reduce the water requirement of the
hydrolysis input stream.
Further consideration of the existence of large amounts
of HCl in the output stream of the electrolytic cell renders
the process integration more complicated. Table 2 presents
the minimum concentration of HCl in the output stream of
the electrolytic cell. In actual operations it lies in the range
of 5.3e11.0 M, which is very close or beyond the maximum
HCl concentration (7.4 M shown in Table 2) that can be effec-
tively produced in current experimental hydrolysis reactors
[9,13,14].
The maximum value of 7.4 M for the HCl concentration
was calculated from the minimum steam-to-cupric chloride
ratio of 7 that has been approached in proof-of-principle
tests in hydrolysis reactors [9,13,14]. Assuming there are no
side reactions competing with hydrolysis, then the molar
concentration of HCl in the gaseous product mixture of HCl
and H2O satisfies the following equation due to the stoichio-
metric mass balance of the hydrolysis reaction:
CM ¼ 2=ð2RSCu þ 1Þ (1)
where CM is the molar concentration of HCl in the gaseous
product mixture and RSCu is the molar ratio of steam to cupric
chloride. After the gas mixture is condensed to an aqueous
solution of HCl, CM still represents the molar concentration.
From the reported densities of HCl aqueous solutions at
different molar concentrations of HCl [15e17], the molarity of
HCl then corresponds to the steam-to-cupric chloride ratio.
Table 3 shows the correspondence.When the steam-to-cupric
chloride ratio is 7, the maximum HCl concentration is
approximately 7.4 M. Table 3 also shows that when the
hydrolysis reaction approaches thermodynamic equilibrium
at 375 �C, and if the specific heat is 30% lower than the
measured value, as shown in Fig. 2, then themolar percentage
of HCl in the gas mixture is approximately 23% or about 12 M
in the aqueous solution. With these assumptions,
a thermodynamic lower bound of the steam-to-cupric chlo-
ride ratio of 3.8 can be calculated. Furthermore, it is unlikely
that the specific heat is in excess of 30% below measured
values, thus the hydrolysis reactor is limited to provide
a concentration below 12 M into the electrolytic cell.
A higher HCl concentration leaving the electrolytic cell than
the hydrolysis reactor suggests that the hydrolysis reaction
may not occur and integrating the chemical streams is infea-
sible if HCl in the input streamof the hydrolysis is not removed
or the HCl concentration is not significantly reduced before
entering the hydrolysis reactor. This means an intermediate
HCl separator may be required for the integration of an elec-
trolytic cell and hydrolysis reactor. In regards to the HCl
produced from the hydrolysis reactor, it serves as the reactant
for electrolysis. However, as shown in Table 2 and Fig. 1, the
output concentration of HCl from hydrolysis is close or even
smaller than the input requirement of electrolysis, which
suggests an intermediateHCl concentratormaybeneeded.The
maximumvalue of HCl concentration in the hydrolysis reactor
is determined by the equilibrium constant which indicates the
minimum water-to-cupric chloride ratio. As discussed previ-
ously, it is unclearwhether themaximumvalueof 7.4 M for the
inputstreamofhydrolysis in theproof-of-principle is causedby
challenges of reaction kinetics or thermodynamic limits.
Therefore, accurate data for the equilibrium constant of the
hydrolysis reaction has a vital role in determiningwhether the
quaternaryoutput streamof electrolysis canbedirectlyusedas
the input stream of a hydrolysis reactor, and whether the
gaseous product from the hydrolysis reactor can be directly
utilized as an input to the electrolytic cell.
The existence of CuCl in the output stream from an elec-
trolysis reactor is another challenge of integrating with
a hydrolysis reactor. The potential chemical poisoning effect
of CuCl on hydrolysis has not been reported. However, the
presence of CuCl mixed with CuCl2 particles may reduce the
contact between steam and CuCl2 and increase the heat
transfer resistance. Therefore, it is preferable that all CuCl is
converted to CuCl2 on the anode side of the electrolytic cell or
separated fromCuCl2 before it enters a hydrolysis reactor. The
most efficientway to reduce the concentration of CuCl and the
ratio of water to CuCl2 may be to produce oversaturated CuCl2on the anode side allowing CuCl2 to precipitate on the anode
side, forming a slurry to be fed into the hydrolysis reactor.
2.2. Concentrating CuCl2 for the linkage of electrolytichydrogen production and hydrolysis steps
As discussed previously, the water-to-cupric chloride ratio in
the output stream of electrolysis is larger than required by
hydrolysis. The CuCl2 must be concentrated before it enters
the hydrolysis reactor. Currently, spray drying and crystalli-
zation are under investigation at UOIT for concentrating the
CuCl2. In spray drying, all or a portion of water is evaporated
with a drying medium. The minimum energy quantity
required by the spray drying can also be estimated by Fig. 3.
The required heat input can be below 120 �C so that waste
heat from many sources can be utilized. However, in order to
utilize low grade waste heat, the thermal efficiency is sacri-
ficed. Table 4 summarizes the large lab-scale experimental
results from UOIT and the estimates for industrial hydrogen
Table 3 e Steam-to-cupric chloride ratio and concentrations of HCl in the mixture of HCl and H2O before and aftercondensation.
Steam-to-cupricchloride molarratio (RSCu), mol/mol
Molar percentageof HCl in the gasmixture (CM), %
Molar ratio of HClto steam, mol/mol
Concentration of HCl in its aqueoussolution after condensation (molarity), M
0 �C 20 �C 100 �C
201.3 0.5 0.0050 0.28 0.27 0.26
99.9 1.0 0.010 0.55 0.55 0.53
49.2 2.0 0.021 1.12 1.12 1.07
32.3 3.1 0.032 1.70 1.69 1.63
23.8 4.1 0.043 2.28 2.27 2.19
18.8 5.2 0.055 2.88 2.87 2.76
15.4 6.3 0.067 3.50 3.48 3.35
13.0 7.4 0.080 4.12 4.09 3.95
11.1 8.6 0.094 4.76 4.72 4.55
9.7 9.8 0.108 5.40 5.36 5.17
8.6 11.0 0.123 6.06 6.02 5.79
7.7 12.2 0.139 6.74 6.68 6.43
6.9a 13.5 0.156 7.42 7.36 7.08
6.3 14.8 0.173 8.12 8.04 7.73
5.7 16.1 0.192 8.83 8.74 8.39
5.2 17.4 0.211 9.54 9.45 9.07
4.8 18.8 0.232 10.31 10.16 9.75
4.4 20.3 0.254 11.06 10.89 10.45
4.1 21.7 0.277 11.82 11.63 11.15
3.8 23.2b 0.302 12.60 12.37 11.86
a The minimum molar ratio of steam to cupric chloride is 7 in reported reactors [9,13,14].
b If the actual specific heat is 30% lower than the measured value, as shown in Fig. 2, then the molar percentage of HCl in the gas mixture is
approximately 23% when the hydrolysis reaction approaches thermodynamic equilibrium at 375 �C.
i n t e rn a t i o n a l j o u r n a l o f h y d r o g e n en e r g y 3 7 ( 2 0 1 2 ) 1 6 5 5 7e1 6 5 6 916562
production scales in terms of the processing scales of water
evaporation, heat load, and drying air. Due to the lower cost of
air, Table 4 only presents the results for air, although in
principle theworking gases such as nitrogen and heliumother
than air can also be utilized for drying to avoid the chemical
effects with oxygen.
It was found in the experiments that the heat requirement
of spray drying with air is 3e5 times the water evaporation
energy requirement shown in Fig. 3 for complete drying of the
aqueous solution of CuCl2. Although the heat input can be low
grade waste heat as experimentally examined in UOIT, the
heat transfer may require large dimensions or numbers of
heat exchangers. In addition, the drying air requirement is
also large. The experimental results at UOIT show that the
mass ratio of air to water is usually higher than 8 in order to
completely evaporate the water with air below 120 �C.Another challenge of utilizing spray drying is the recovery
of HCl from the drying air. As previously discussed, the
output stream of the electrolytic cell is a quaternary system
with HCl that must be recycled back into the CueCl cycle to
Table 4 e Requirements of heat, water and drying air for conce
H2 productionscale, tonnes/dayb
Molar ratio of waterto copper, mole/mole
Mass ratio of dryair to water,a kg
Large lab scale 0.001 17.7 8e20
Industrial scale 100 17.7 8e20
a The inlet drying air temperature is 80e120 �C and the outlet temperatu
b The runtime of the large lab-scale experiments lies in the range of 1e5
replenish the chemicals used in the cycle. Also, the water in
the drying air should also be recycled to limit water
consumption. This means the usage of spray drying will
require a number of additional processing units of equipment
for the recovery of water and HCl, in addition to heat
exchangers for the drying air to capture thermal energy from
various heat sources.
Another technology for concentrating the CuCl2 is crys-
tallization, which utilizes the solubility difference of CuCl2 at
different temperatures. The CuCl2 crystals precipitated out of
the saturated binary system of CuCl2 and water, as demon-
strated at UOIT. A significant advantage of using crystalliza-
tion is its extensivematurity for commercialmanufacturing of
hydrated CuCl2 [18], either from the chlorination of Cu by Cl2or the reaction between CuO and HCl. The recovery of CuCl2from spent etchant was also reported [19]. Therefore, tech-
nical solutions can be found from commercially available
technology. In an industrial process, a cooling bath environ-
ment created by ice and inorganic salts such as NaCl and CaCl2can expedite the crystallization kinetics and increase the
ntrating CuCl2 with spray drying.
ing/kg
Water evaporated,tonnes/day
Heat needed,MWth
Drying air flowrate, tonnes/day
0.319 0.018e0.030 3.19e6.38
31,900 1800e3000 319,000e638,000
re is 50e80 �C.h. The data were normalized to units per day for a comparable basis.
Fig. 4 e CuCl2 particles generated from spray drying (air-to-
water mass ratio is 8 and air temperature is 120 �C).
i n t e r n a t i o n a l j o u r n a l o f h y d r o g e n en e r g y 3 7 ( 2 0 1 2 ) 1 6 5 5 7e1 6 5 6 9 16563
crystal quantity by cooling the solution below 0 �C. Also, theCuCl2 aqueous solution is at a saturation state before starting
the crystallization process.
However, the energy penalty may become significant if
adopting a cooling process below the ambient temperature. To
study the cooling with a coolant at both ambient and lower
temperatures, experiments were performed for two temper-
ature drops at 80 to 22 �C and 20 to 0 �C. Fig. 5a and b shows the
dendritic crystals of hydrated CuCl2 precipitated out of an
experimental aqueous solution in the clear solution and out of
the solution, respectively. The coolants in the experiments for
the crystallization were room temperature water and
a mixture of water and ice. Experimental results showed that
60e90% of the available quantities corresponding to the
solubility difference precipitated out in four hours when the
coolant was applied to the binary system. It was also found
that before the CuCl2 solution was cooled to 33 �C, no crystals
were observed. Subsequently, CuCl2 crystals appeared rapidly
in several minutes to 60e90%. Then another two days were
required to precipitate the residual 5e10% of the quantities
accounted for by the solubility difference.
It is encouraging that CuCl2 can be precipitated out of the
aqueous solution with a coolant of ambient temperature for
the temperature drop of 80e22 �C. However, in two hours of
runtime, the crystallized quantity is only about 60% of the
total mass with the temperature drop of 80e0 �C. In addition,
a complete crystallization to reach equilibriumneeds a total of
about two days. To overcome this lengthy time challenge, the
dimensions of the crystallizer must be large enough to match
the CuCl2 feed rate required by the downstream hydrolysis
reactor, or alternatively an intermediate storage unit may be
needed.
The usage of crystallization discussed above is only suit-
able for CuCl2 solutions at the saturation state of either the
exiting stream of the electrolytic cell or after it is cooled down.
In practical operation, the exiting stream of the electrolytic
cell of the CueCl cycle may not be at the saturation state. To
utilize crystallization, the aqueous CuCl2 solution must be
saturated by some means, for example, the saturation can be
created by introducing another reagent such as HCl to satu-
rate the CuCl2. For the quaternary system of CuCl2, CuCl, HCl
and water, the saturation curve of CuCl2 is complex. A future
study on the crystallization could investigate a quaternary
system that can utilize room temperature coolant or inert
additives.
The crystallization is promising for the separation of CuCl2from a saturated binary system because of the advantages
over spray drying, wherein heat extraction from a heat source,
drying air processing, and equipment for the recovery of
additional HCl and water in the drying air are not needed with
crystallization. A filtration process can be adopted for the
separation of crystallized CuCl2 and a clear solution, which
has been tested at UOIT. The clear solution exiting the crys-
tallizer can be directly pumped back to the upstream elec-
trolyzer for reuse or for dissolution of incoming CuCl
produced in an oxygen production reactor. The energy cost of
a filtration process is primarily based on water pumping and
mechanical discharge of the slurry of hydrated CuCl2. If one
assumes the same energy cost for the discharge and pro-
cessing of solid CuCl2 in spray drying, similar power to move
and pressurize drying gas, and pump and atomize the CuCl2aqueous solution, it is expected that the crystallization can
save a significant portion of the amount of thermal energy
otherwise used for the evaporation of water in spray drying.
Compared to crystallization, the advantages of spray
drying include its ability to generate anhydrous CuCl2, but the
CuCl2 crystallized may comprise several hydrated water
molecules, i.e., CuCl2$nH2O. Consequently, the value for the
water-to-cupric chloride ratio could be larger than 2 in crys-
tallization. As to the particle size of CuCl2, it is unclear
whether smaller or larger particle sizes are more advanta-
geous. Spray drying can generate fine particles in the range of
4e50 microns and the Sauter mean value is about 31 microns
when the drying air temperature is about 120 �C and the air-
to-water mass ratio is 8e20. Fig. 4 shows the dimensions of
the particles generated from spray drying. Fig. 5a and b shows
the dimensions and structure of the crystals of hydrated
CuCl2. The length of the crystal that stems and branches can
be several millimeters to centimeters. Considering integration
with the downstream hydrolysis reaction, smaller particle
sizes may improve the hydrolysis reaction rate. However,
smaller particles are more readily entrained in a gas stream,
imposing limits on the hydrolysis reactor selection. For
example, the smaller particle size may reduce the operating
range of the steam flow rate in a fluidized bed because the
steam may carry large amounts of CuCl2 particles outside of
the reactor.
2.3. Matching the chemical streams of hydrolysis andoxygen production reactions
Fig. 6 summarizes the chemical streams of hydrolysis and
oxygen production reactions from a system integration
approach. In the hydrolysis reaction, the CuCl2 reacts with
steam producing solid Cu2OCl2 and gaseous HCl. If CuCl2 is in
Fig. 5 e (a) Dendritic crystals (CuCl2$2H2O) generated from
crystallization in clear solution (temperature decreases
from 80 to 20 �C and the minimum scale of the ruler is
mm). (b) Dendritic crystals (CuCl2$2H2O) generated from
crystallization after clear solution is removed.
i n t e rn a t i o n a l j o u r n a l o f h y d r o g e n en e r g y 3 7 ( 2 0 1 2 ) 1 6 5 5 7e1 6 5 6 916564
the form of solid particles, then the reaction is a reactant
shrinking core process wherein the size of CuCl2 reactant core
is decreasing while the thickness of the product crust
(Cu2OCl2) outside of the core is increasing. This suggests the
Fig. 6 e Chemical stream connection of the h
possibility of a simultaneous partial decomposition of the
product Cu2OCl2 when it is produced. As shown in reaction C
of Table 1, the decomposition of the Cu2OCl2 crust produces
oxygen. In addition, the core composed of CuCl2 may
decompose to CuCl and Cl2 because of the continuous heating
but insufficient contact with steam for the hydrolysis reaction.
Consequently, the undesirable gaseous products, i.e., O2 and
Cl2, will mix with the desirable product HCl to form the output
gas steam of the hydrolysis reactor. As discussed in the
previous section, HCl is utilized in the electrolytic cell for the
production of H2. Therefore, introducing O2 and Cl2 into the
electrolyzer must be avoided and any O2 and Cl2 produced in
the hydrolysis reaction should be removed before entering the
electrolytic cell, or they are not produced in the hydrolysis
reactor.
The Deacon reaction may also be another important
undesirable side reaction producing Cl2 in the hydrolysis
reaction [20]. The reaction takes place at above 400 �C if
catalyzed by CuCl2, which has been used to produce Cl2 in
industry: 4HCl (g)þO2 (g)/ 2Cl2 (g)þ 2H2O (g). To avoid the
production of O2 and Cl2, the operating conditions must lie in
a spontaneous range for the hydrolysis of CuCl2 and mean-
while in the non-spontaneous range for the Deacon reaction,
and the decomposition of Cu2OCl2 and CuCl2. The spontaneity
of the reactions can be estimated with the Gibbs energy
change. Fig. 7 shows the standard Gibbs energy change of the
reactions at various temperatures. The Gibbs energy of
Cu2OCl2 was calculated from the specific heat, standard
enthalpy and conventional entropy of Cu2OCl2 [12]. The data
for HCl, CuCl, CuCl2, H2O, Cl2 and O2 are taken from the
databank of NIST [21]. It can be found that the spontaneity
transitional temperatures of the CuCl2 hydrolysis and Cu2OCl2decomposition have a gap of 60 �C, which provides a large gap
for the adjustment of the operating temperature, so as to
avoid the decomposition of the product Cu2OCl2 in the
hydrolysis reactor.
However, the adjustment gap for the avoidance of CuCl2decomposition ismuch smaller, whichmeans othermeasures
must be adopted in order to minimize the Cl2 release. The
thermodynamic spontaneity of the decomposition of CuCl2
ydrolysis and oxygen production steps.
-40
-20
0
20
40
60
80
0 100 200 300 400 500 600 700
Temperature, o
C
Stan
dard
G
ib
bs en
erg
y o
f reactio
ns, kJ/m
ol
Fig. 7 e Thermodynamic spontaneity of hydrolysis and
side reactions.
Table 5 e Chlorine gas generated in an oxygen productionreactor from the unreacted CuCl2 in a hydrolysis reactor.
T (reactor),�C
P (reactor),kPa
Test time,minutes
Weight ofsample,a
grams
Cl2/O2,mole/mole
560 99.99 70 79.58 0.056
547 99.99 70 79.58 0.0595
516 99.99 75 79.68 0.0410
506 99.99 80 79.55 0.0389
491 99.99 70 79.42 0.0500
489 99.99 90 106.99 0.1545
a The sample is an equimolar mixture of CuO and CuCl2.
i n t e r n a t i o n a l j o u r n a l o f h y d r o g e n en e r g y 3 7 ( 2 0 1 2 ) 1 6 5 5 7e1 6 5 6 9 16565
and Cu2OCl2 is also shown in Fig. 7. It was found that the
production of Cl2 is difficult to avoid. The experiments of UOIT
also verified the thermodynamic analysis. An option is to
significantly differentiate the reaction kinetics so that the
hydrolysis proceeds much faster than the side reaction. For
example, the mixing of steam and CuCl2 can be improved by
adjusting some operating parameters such as particle size and
void fraction (the ratio of voids to particles) in the reactor to
improve the contact between steam and CuCl2. The steam
must diffuse into the core of the solid phase to reactwithCuCl2in the particle. If the steam diffusion rate was lower than the
CuCl2 decomposition rate, the side reaction would occur.
If further considering the solid products in a hydrolysis
reactor, the Cu2OCl2 crust will exist and encapsulate the
unreacted CuCl2 in the hydrolysis reaction. The crust also
creates obstacles to achieving full conversion of CuCl2 to
Cu2OCl2 because contact between the reactants CuCl2 and
steam is reduced, regardless of the steam-to-cupric chloride
ratio and the yield of HCl. The steam must penetrate the
product crust to reach CuCl2 to continue the reaction. If the
residence time of the solid particles does not cover the diffu-
sion time, then the full conversion of CuCl2 will not be ach-
ieved. As a consequence, the unreacted CuCl2 will be carried
with Cu2OCl2 to the downstreamO2 production reactor. When
the decomposition of Cu2OCl2 proceeds to produce O2, the
entrained CuCl2 may also decompose to produce Cl2, which is
carried with O2 leaving the CueCl cycle. The production of Cl2will offset the mass balance of the CueCl cycle that should
only have two output gases: H2 and O2.
Another option is to introduce some amount of Cl2 into the
hydrolysis reaction to sequestrate Cl2 production in the
decomposition of CuCl2. Thismethod can also sequestrate the
Deacon reaction. Since the solubility of Cl2 in water is much
smaller than HCl, the introduced Cl2 can be collected from
gaseous products of the hydrolysis reactor when the products
are condensed to form aqueous solution of HCl for use in the
downstream electrolytic hydrogen production reactor.
As presented in Table 5, the molar ratio of produced Cl2 to
O2 is about 0.04e0.16 in the oxygen production reactor if 50%
of the CuCl2 is not consumed in the upstream hydrolysis
reactor. In Table 5, an equimolar mixture of CuCl2 and CuO
was utilized rather than Cu2OCl2, anticipating that the CuO
would react with the released Cl2 in order to quantify the
minimum chlorine release for the CueCl cycle. If the mixture
is CuCl2 and Cu2OCl2, more Cl2 will be released. Therefore,
improving the conversion of CuCl2 in the hydrolysis reactor is
the preferable method to reduce the Cl2 release in the down-
stream oxygen production reactor.
It is preferable that the Cl2 formation is controlled below
a minimal level. The target of the current research at UOIT is
to utilize Cl2 to oxidize the counterpart of CuCl produced by
the decomposition of CuCl2. This can restore themass balance
of desirable compounds consisting of Cu and Cl elements
within the CueCl cycle. Then the solubility of Cl2 in the
aqueous solution of CuCl and HCl determines the total level of
Cl2 produced from the Deacon reaction and decomposition of
CuCl2. It was reported that the Cl2 solubility in the aqueous
chloride solution at 90 �C is approximately equivalent
to 0.5 gCl2/kgH2O or 1.3� 10�4 mol Cl2/mol H2O [22e24].
Assuming the steam-to-cupric chloride ratio is operated at the
minimum thermodynamic limit at 375 �C, then according to
Table 3, the HCl-to-steam ratio in the gaseous productmixture
is approximately 0.3. Thus, each mole of HCl produced per
mole CuCl2 will have 3.3 moles residual water mixed with the
HCl. If utilizing the condensed water to dissolve Cl2, then the
Cl2 amount is 3.9� 10�4 moles. This implies the Cl2 produced
from the Deacon reaction and CuCl2 decomposition should be
controlled to be 3e4 orders smaller than the concentration of
HCl in the hydrolysis reaction.
2.4. Matching the chemical streams of oxygenproduction and electrolytic steps
One of the chemical input streams to the electrolytic cell is
CuCl, which is produced in the upstream oxygen production
reactor. However, the CuCl produced in the oxygen production
reactor is in the form of molten salt at about 500 �C. So
auxiliary equipment is needed to solidify the CuCl and then
dissolve it in an aqueous solution of HCl. The HCl needed by
the dissolution of CuCl is produced from the hydrolysis
reactor, so the integration between the oxygen production
reactor and electrolysis must also consider the connection
with hydrolysis as well. Fig. 8 shows the chemical streams
that connect the three steps. As discussed previously, the
undesirable Cl2 gas produced from the hydrolysis reactor
must be removed from HCl before entering the CuCl
Fig. 8 e Chemical streams connecting the oxygen production and electrolytic steps.
i n t e rn a t i o n a l j o u r n a l o f h y d r o g e n en e r g y 3 7 ( 2 0 1 2 ) 1 6 5 5 7e1 6 5 6 916566
dissolution vessel. To improve the dissolution rate, it is pref-
erable that the solidified CuCl is in the form of particles or
pellets. Also, the unreacted CuCl2 in the hydrolysis reactor
may enter the oxygen production reactor and influence its
output stream that serves as the input stream of the electro-
lytic cell. It was experimentally determined that the unreacted
CuCl2 does not completely decompose in the oxygen reactor.
Fig. 9 shows the XRD results of the decomposition. It can be
found that some amounts of CuCl2 are still present in the CuCl
Fig. 9 e XRD results of the residual of CuCl2 in the s
produced from the decomposition of Cu2OCl2. Since CuCl is
utilized in the electrolytic cell, the entrained CuCl2 will enter
the electrolytic cell.
There exists an alternative reaction to produce oxygen
with the mixture of CuO and CuCl2 rather than the single
compound Cu2OCl2 [25,26]:
CuO (s)þCuCl2 (s)¼ 2CuCl (molten)þ 1/2O2 (g), at
500e530 �C (2)
olidified CuCl (reaction time of 1 h, T[ 500 �C).
i n t e r n a t i o n a l j o u r n a l o f h y d r o g e n en e r g y 3 7 ( 2 0 1 2 ) 1 6 5 5 7e1 6 5 6 9 16567
Since the mixing of CuO and CuCl2 is not ideal for the full
reaction, the following decomposition reaction will consume
a portion of CuCl2 before it reacts with CuO:
CuCl2¼CuClþ 1/2Cl2, at 300 �C and higher temperatures (3)
Consequently, there will be some unreacted CuO in the
oxygen production reaction, which was observed in past
experiments [25]. Since the unreacted CuO is distributed
within the molten CuCl product, it will be carried by CuCl into
the electrolytic cell, wherein CuO will react with HCl:
CuO (s)þ 2HCl (aq)¼ 2CuCl2 (aq)þ 2H2O (l) (4)
The consumption of HCl in reaction (4) will reduce the HCl
amount for the hydrogen production, in addition to the
introduction of undesirable excess CuCl2. Therefore, consid-
ering the substance balance for the process integration,
reaction (2) is not recommended for the oxygen production
process in the CueCl cycle.
The influence of the entrained CuCl2 on the electrolysis is
unclear, but entrained CuCl2 will have insignificant influence
on the solidification, granulation and dissolution of CuCl
because these auxiliary steps are physical and not chemical
processes. Conversely, it may even assist the percolation of
the CuCl pellets due to the high solubility of the entrained
CuCl2.
When oxygen leaves the reactor, the vapour of molten
CuCl will be entrained. Table 6 presents the CuCl vapour
pressure [28] and the quantity of CuCl entrained with oxygen
gas at various hydrogen production scales and operating
temperatures. The loss of CuCl will accumulate significantly
to several tonnes per day if the entrained CuCl is not recov-
ered. Therefore, the CuCl vapour must be recycled within the
cycle. One option is to condense the CuCl vapour when
cooling the oxygen for storage and then collect the
condensed CuCl into a dissolution vessel for the integration
of the oxygen production reactor and electrolytic cell. The
disadvantage of this option is the potential clogging of
condensed CuCl in the oxygen cooling equipment. Currently,
UOIT is examining the absorption of CuCl vapour with solid
Cu2OCl2 or CuCl2 particles. In the absorption process, oxygen
and CuCl vapour passes through an absorption bed packed
with Cu2OCl2 particles produced from the hydrolysis reactor.
Since the particle temperature is around 375 �C and the
condensation point of CuCl is 425 �C, it is expected the CuCl
Table 6 e Loss of CuCl in vapour entrained with oxygengas if the vapour is not recovered.
T,�C
Vapourpressure,
kPa
Operating pressure ofoxygen reactor, kPa
Mass loss of CuCl,tonnes/day
100tonnesH2/day
200tonnesH2/day
500 0.066 101.325 1.6 3.2
530 0.122 101.325 3.0 6.0
546 0.166 101.325 4.1 8.2
vapour can be condensed onto the surface of Cu2OCl2 parti-
cles that will decompose to CuCl and O2 in the downstream
O2 production reactor. This process can also recover the
condensation heat of CuCl and a portion of sensible heat
carried by the high temperature O2. Though CuCl2 can also be
used as the absorption reagent, it may experience decom-
position due to high local temperatures in the absorption
bed.
3. Thermal energy requirements for thesystem integration
Since two of the three chemical reactions of the CueCl cycle
shown in Table 1 are purely thermal reactions, the patterns
to integrate the processes will be strongly influenced by the
heat flows. The integration patterns will influence the overall
thermal efficiency of the hydrogen production cycle. There-
fore, the thermal energy integration patterns must aim to
recover as much thermal energy as possible which is inter-
nally released from the exothermic processes of the CueCl
cycle, while simultaneously utilizing minimum external heat
input. Regarding the integration of external heat flows within
the CueCl cycle, the studies at UOIT suggest a single heating
route for the heating fluid, where it initially passes through
the maximum temperature step, i.e., oxygen production
reaction at 530 �C, and then flows to the hydrolysis step
which requires a heat input at 375 �C. After leaving the CueCl
cycle, the heating fluid flows back to the thermal energy
source to complete the circulation. Multiple routes, such as
separate heating lines for the oxygen production and
hydrolysis steps, are not suggested so as to avoid the layout
complexity of the heat transport lines and increase the heat
usage efficiency.
Regarding the recovery of the internally released heat,
Table 7 shows the quality and quantity of input and output
heat flows for each process on the basis of stoichiometric
coefficients, i.e., the steam-to-cupric chloride ratio is 0.5 for
hydrolysis. Table 7 also shows the heat requirement consid-
ering the possible excess steam requirement of the hydrolysis
reaction. It can be found that there are three sources of heat
released from the exothermic processes: cooling the HCl
produced from hydrolysis (process B4), cooling the O2 (process
C3) and solidifying the CuCl (process C4) produced from the
oxygen production reactor. In processes C3 and C4, the heat
released has a temperature of 530 �C, which is 155 �C higher
than the hydrolysis temperature requirement of 375 �C. Thereleased heat quantity (82.71 kJ/mol) can cover the generation
of the stoichiometric steam requirement (60.5 kJ). If utilizing
the heat released in process B4 (22.38 kJ/mol) for the water
preheating and the heat released from processes C3 and C4 for
the generation of steam, the heat recovery efficiency is about
60%. A study at UOIT suggested that released heat from the
exothermic processeswould not be used to heat solid particles
due to lower efficiency than a heating fluid. Table 7 shows that
if excess steam is required, then the heat recovery load will be
increased significantly to the same magnitude as shown in
Fig. 3, indicating the vital importance of reducing the excess
steam requirement of the hydrolysis reactor.
Table 7 e Input and output heat flows in each process on the basis of stoichiometric coefficients (water-to-cupric chlorideratio in hydrolysis is 0.5) and excess steam requirement.
Label Processes in the step T, �C Heat input,kJ/mol H2
Heat output,kJ/mol H2
B 2CuCl2 (s)þH2O (g)¼CuOCuCl2 (s)þ 2HCl (g), hydrolysis step
B1 Heating CuCl2 (s) 25/375 62.70
B2 Heat of reaction 375 80.80
B3 Steam production H2O (l)¼H2O (g) 25/375 60.50
B3Xa Steam production 34.4 (l)¼ 34.4 H2O (g) 25/375 2081
B4 2HCl (g, 450 �C)/ 2HCl (g, 25 �C) 375/25 22.38
B4Xa Steam production 33.4 (l)¼ 33.4 H2O (g) 375/25 2021
C Cu2OCl2 (s)/ 2CuCl (l)þ 1/2O2 (g), oxygen production step
C1 Heating Cu2OCl2 (s) 375/530 20.20
C2 Heat of reaction 530 138.39
C3 Cooling, solidification of molten CuCl 530/25 74.74 Sum: 82.71
C4 Cooling of O2 (g) product 530/25 7.97
Total For production of 1 mole H2 362.59 105.09
For production of 100 tonnes H2/day 210 MWth 61 MWth
For production of 200 tonnes H2/day 420 MWth 122 MWth
a The steam-to-copper ratio is 17.7, i.e., steam is in excess of the stoichiometric ratio of 0.5.
i n t e rn a t i o n a l j o u r n a l o f h y d r o g e n en e r g y 3 7 ( 2 0 1 2 ) 1 6 5 5 7e1 6 5 6 916568
4. Conclusions
This paper studied the CueCl cycle from the perspective of
system integration. Thermodynamic analysis and experi-
mental results were reported in terms of effective process
integration. It is concluded that the production of a high
concentration of CuCl2 or even slurry will significantly reduce
the integration challenges with the downstream hydrolysis
reactor. The concentrating process for CuCl2 cannot be
avoided if the electrolytic cell operates under the conditions
reported in past literature. Spray drying has challenges of
high heat transfer loads, which are the same challenges that
necessitate the water requirement of a hydrolysis reactor to
be reduced. Regarding the linkage between the hydrolysis
and oxygen production reactors, it was found that the
unreacted CuCl2 in a hydrolysis reactor will result in the
release of Cl2 in the oxygen production reactor. Furthermore,
residual CuCl2 transferred from the hydrolysis reactor to the
oxygen production reactor may be further entrained to the
electrolytic hydrogen production cell. It is suggested that
a future focus of the hydrolysis reaction is to reduce the
water requirement and achieve a high conversion of CuCl2 to
Cu2OCl2. To minimize the side reactions such as the Deacon
reaction, the decomposition of CuCl2 accompanying the
hydrolysis step is crucial to an effective system integration of
the CueCl cycle. The study of thermal energy integration
shows that the heat released by the exothermic processes
can be used to generate steam as input to the hydrolysis
reactor.
Acknowledgements
Financial support from Atomic Energy of Canada Limited and
the Ontario Research Fund is greatly acknowledged.
r e f e r e n c e s
[1] Naterer G, Gabriel K, Wang ZL, Daggupati V, Gravelsins R.Thermochemical hydrogen production witha copperechlorine cycle. I: oxygen release from copperoxychloride decomposition. International Journal ofHydrogen Energy 2008;33:5439e50.
[2] EVWorld. Energy content of fuels; 2010. Available from:http://www.evworld.com/library/energy_numbers.pdf[accessed December 8, 2010].
[3] Sadhankar RR, Li J, Li H, Ryland D, Suppiah S. Hydrogengeneration using high-temperature nuclear reactors. 55thCanadian chemical engineering conference, Toronto;October 2005.
[4] Kubo S, Kasahara S, Okuda H, Terada A, Tanaka N, Inaba Y,et al. A pilot test plan of the thermochemical water-splittingiodineesulfur process. Nuclear Engineering and Design 2004;233:355e62.
[5] Schultz K. Thermochemical production of hydrogen fromsolar and nuclear energy, Technical Report for The StanfordGlobal Climate and Energy Project. San Diego, CA: GeneralAtomics; 2003.
[6] Anzieu P, Carles P, Le Duigou A, Vitart X, Lemort F. Thesulfureiodine and other thermochemical process studies atCEA. International Journal of Nuclear Hydrogen Productionand Applications 2006;1:144e53.
[7] Moore R, Parma E. A laboratory-scale sulfuric aciddecomposition apparatus for use in hydrogen productioncycles. American nuclear society annual meeting, Boston,Massachusetts; June 24e28, 2007.
[8] Buongiorno J, MacDonald PE. Supercritical water reactor(SCWR) progress report for the FY-03 generation-IV R&Dactivities for the development of the SCWR in the U.S. INEEL/EXT-03-01210; Sept 30, 2003.
[9] Lewis MA. Update on the CueCl cycle R&D effort, Workshopof the ORF Hydrogen Project at AECL Chalk RiverLaboratories. Ontario: Chalk River; October 17, 2008. p. 25e33.
[10] Sharna R, Fedkin M, Lvov S. CuCl electrolyzer for hydrogenproduction via CueCl thermochemical cycle, 219th ECS(Electrochemical Society) Meeting. Montreal, QC: Canada;May 1e6, 2011.
i n t e r n a t i o n a l j o u r n a l o f h y d r o g e n en e r g y 3 7 ( 2 0 1 2 ) 1 6 5 5 7e1 6 5 6 9 16569
[11] Suppiah S, Stolberg L, Boniface H, Tan G, McMahon S, York S,et al. Canadian nuclear hydrogen R&D programme:development of the medium-temperature CueCl cycle andcontributions to the high-temperature sulphureiodine cycle.Nuclear Production of Hydrogen, Fourth InformationExchange Meeting, Oakbrook, Illinois, USA; April 14e16,2010. p. 77e86.
[12] Parry T. Thermodynamics and magnetism of Cu2OCl2.Masters thesis. Department of Chemistry and Biochemistry,Brigham Young University; 2008.
[13] Lewis MA. CueCl cycle R&D e recent research results for thehydrolysis reaction sensitivity studies. CueCl cycle researchand development at the Argonne National Laboratory,Canadian HydrogenWorkshop on Hydrogen Production fromNon-fossil Sources. Oshawa, Ontario, Canada: University ofOntario Institute of Technology; December 20, 2007.
[14] Lewis MA, Ferrandon MS, Tatterson DF, Mathias P.Evaluation of alternative thermochemical cycles e part IIIfurther development of the CueCl cycle. InternationalJournal of Hydrogen Energy 2009;34:4136e45.
[15] United States Environmental Protection Agency Office ofInformation Analysis & Access Washington, DC 20460. EPA-745-B-99-014; December 1999. p. 29e31.
[16] Bayer Material Science Ltd. In: Industrial OperationsBasic Chemicals, editor. Product data sheet:hydrochloric acid. Germany: Bayer Material Science AG;April 2008. p. 1e4.
[17] Solvay Chemicals International (Brussels). Hydrochloricacid e density. Data sheet number: PCH-1300-0001-W-EN(WW). Issue 1; April 2005.
[18] Bertz SH, Fairchild EH. Reagents, auxiliaries and catalysts forCeC bond formation. In: Coates RM, Denmark SE, editors.Handbook of Reagents for Organic Synthesis, vol. 1. JohnWiley & Sons; 1999. p. 220e3.
[19] Basir SMA. Recovery of cupric chloride from spent copperetchant solutions: a mechanistic study. Hydrometallurgy2003;69:135e43.
[20] Pan HY, Minet RG, Benson SW, Tsotsis TT. Process forconverting hydrogen chloride to chlorine. Industrial &Engineering Chemistry Research 1994;33:2996e3003.
[21] NIST (National Institute of Standards and Technology).Chemistry WebBook; 2010. Available from: http://webbook.nist.gov/chemistry/ [accessed on February 1, 2011].
[22] Alkan M, Oktay M, Kocakerim MM, Copur M. Solubility ofchlorine in aqueous hydrochloric acid solutions. Journal ofHazardous Materials 2005;119:13e8.
[23] Sherrill MS, Izard EF. The solubility of chlorine inaqueous solutions of chlorides and the free energy oftrichloride ion. Journal of American Chemical Society1931;53:1667e74.
[24] Awakura Y, Yoshitake S, Majima H. Solubility of Cl2 gas inaqueous chloride solution. Journal of the Japan Institute ofMetals 1989;53:1134e9.
[25] Marin GD, Wang Z, Naterer GF, Gabriel K. Byproducts andreaction pathways for integration of the CueCl cycle ofhydrogen production. International Journal of HydrogenEnergy 2011;36:13414e24.
[26] Serban M, Lewis MA, Basco JK. Kinetic study of the hydrogenand oxygen production reactions in the copper-chloridethermochemical cycle. AIChE 2004 Spring National MeetingNew Orleans. LA, US; April 25e29, 2004.
[27] Naterer GF, Fowler M, Cotton J, Gabriel K. Synergistic roles ofoff-peak electrolysis and thermochemical production ofhydrogen from nuclear energy in Canada. InternationalJournal of Hydrogen Energy 2008;33:6849e57.
[28] Brewer L, Lofgren NL. The thermodynamics of gaseouscuprous chloride, monomer and trimer. Journal of theAmerican Chemical Society 1950;72:3038.