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i n t e r n a t i o n a l j o u rn a l o f h y d r o g e n en e r g y 3 8 ( 2 0 1 3 ) 7 3e8 1
Available online at w
journal homepage: www.elsevier .com/locate/he
Efficient hydrogen production from aqueous methanol ina PEM electrolyzer with porous metal flow field: Influenceof PTFE treatment of the anode gas diffusion layer
Anh Tuan Pham, Tomohiro Baba, Tatsuki Sugiyama, Toshio Shudo*
Graduate School of Science and Engineering, Tokyo Metropolitan University, 1-1 Minamiosawa, Hachioji, Tokyo 192-0397, Japan
a r t i c l e i n f o
Article history:
Received 24 April 2012
Received in revised form
8 October 2012
Accepted 10 October 2012
Available online 8 November 2012
Keywords:
Hydrogen production
Methanol electrolysis
Porous metal flow field
Proton exchange membrane (PEM)
Gas diffusion layer
Polytetrafluoroethylene (PTFE)
* Corresponding author. Tel./fax: þ81 426772E-mail address: [email protected] (T. Shu
0360-3199/$ e see front matter Copyright ªhttp://dx.doi.org/10.1016/j.ijhydene.2012.10.0
a b s t r a c t
In a proton exchange membrane (PEM) methanol electrolyzer, the even supply of reactant
to and the smooth removal of carbon dioxide from the anode are very important in order to
achieve a high hydrogen production performance. An appropriate design of flow field and
gas diffusion layer (GDL) is a key factor in satisfying the above requirements. Previous
research has shown that hydrogen production performance of the PEM methanol elec-
trolyzer cell was largely improved with a porous flow field made of sintered spherical metal
powder compared with a conventional groove type flow field. Based on this improvement,
the current study investigated the influence of polytetrafluoroethylene (PTFE) treatment of
the anode GDL on hydrogen production performance of the PEM methanol electrolyzer
with porous metal flow fields. Influences of operating conditions such as methanol
concentration and cell temperature with the flow field were also investigated.
Copyright ª 2012, Hydrogen Energy Publications, LLC. Published by Elsevier Ltd. All rights
reserved.
1. Introduction describes an aqueous methanol electrolysis process with the
Hydrogen is one of the most promising energy carriers for the
future owing to its clean and sustainable energy. Among
many methods to produce hydrogen, water electrolysis with
a proton exchange membrane (PEM) [1e9] is one of the most
convenient ways since it offers a number of advantages for
the hydrogen production such as high gas purity and
compatibility with renewable energy sources (e.g. wind, solar).
Besides the water, aqueous methanol can also be electrolyzed
to generate hydrogen [10e14]. With lower Gibbs free energy
for methanol, hydrogen production performance in the
aqueous methanol electrolysis proceeds at much lower
voltage than that in the water electrolysis [10e14]. Fig. 1
715.do).2012, Hydrogen Energy P36
following reactions:
Anode :CH3OHþH2O/CO2þ6Hþ þ6e E0a ¼0:016V vs: SHE
(1)
Cathode : 6Hþ þ 6e/3H2 E0c ¼ 0 V vs: SHE (2)
Overall : CH3OHþH2O/3H2 þ CO2 E0 ¼ 0:016 V vs: SHE
(3)
The standard potential for the methanol oxidation reaction
(MOR) shown in Reaction (1) is only 0.016 V vs. the standard
hydrogen electrode (vs. SHE) at 298 K, while that for hydrogen
reduction reaction (HRR) shown in Reaction (2) is 0 V (vs. SHE).
ublications, LLC. Published by Elsevier Ltd. All rights reserved.
Table 1 e Specification of the MEAs.
MEA1 MEA2 MEA3
Polymer membrane Nafion 117 (175 mm)
Reaction area 25 cm2 (5 5 cm)
Anode catalyst PteRu 1.0 mg/cm2
Cathode catalyst Pt 1.0 mg/cm2
PTFE content in
the anode GDL
0 wt% 5 wt% 10 wt%
PTFE content in
the cathode GDL
10 wt%
6e- 6e-
3H26H+6H+CO2
CH3OH + H2O
Anode GDL
Cathode GDL
Cathode CL
Anode CL Membrane
Power supply
Fig. 1 e Aqueous methanol electrolysis.
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 8 ( 2 0 1 3 ) 7 3e8 174
As a result of the substantially reduced operating voltage,
the energy requirement from methanol electrolysis can be
reduced significantly. In addition to this, the corrosion in the
PEM methanol electrolysis is less severe than that in the PEM
water electrolysis which needs more than 1.23 V to start
producing hydrogen. Carbon-based and stainless steel mate-
rials, therefore, can be used in the PEM methanol electrolysis,
while these materials which are vulnerable to corrosion at
high operating voltage cannot be used in the anode section of
the PEM water electrolysis [7].
At the anode of a PEM methanol electrolyzer cell, aqueous
methanol is transferred to the catalyst layer and decomposed
to carbon dioxide molecules. Because of having the same
function of the anode, the setup for the PEM methanol elec-
trolyzer cell can be quite similar to that for a direct methanol
fuel cell (DMFC) as shown in Fig. 3. It is well known that the
sluggish kinetics of the MOR [15e18], the permeation of
methanol from the anode to the cathode (i.e. methanol
crossover) [15e18], and cathode flooding [15] are key barriers
that has hampered the development of DMFC technology.
Especially, the crossover of methanol causes a severe prob-
lems including a mixed potential on the cathode (i.e.
decreasing the cathode potential), low fuel utilization effi-
ciency, etc. Because of this, most DMFCs uses relatively thick
membrane (e.g. Nafion 117) [19,20] and low methanol
concentration (i.e. <10 wt%) [21] to lower the methanol
crossover. Unlike the DMFC, water is not produced in the
cathode of PEM methanol electrolyzer cell and the flooding is
not a problem. Therefore, the major challenges for better
performance in the PEM methanol electrolyzer cell exist only
on the anode side. Besides improving the sluggish kinetics of
the MOR, the mass transport related to supply of aqueous
methanol and removal of CO2 is also highly concerned as in
the DMFC. Previous research has shown that hydrogen
production performance of the PEMmethanol electrolyzer cell
was largely improved with a porous flow field (PFF) made of
sintered spherical metal powder (SMP) compared with
a conventional groove type flow field [14]. This is attributed to
an increase in effective electrode area by using the porous
material which enables the flow field to supply reactant
evenly to the electrode and remove carbon dioxide smoothly.
A lower interfacial contact resistance with the SMP is also
a reason for the improvement.
Besides the flow field, an appropriate design of the anode
gas diffusion layer (GDL) shown in Fig. 1 is also an interesting
topic for better performance in the PEMmethanol electrolyzer
cell. Since having the same setup as above mentioned,
amembraneelectrodeassembly (MEA) forDMFChasbeenused
in the previous research by the authors [14].While the GDLs on
both sides of MEA for DMFC are usually coated with a poly-
tetrafluoroethylene (PTFE), there have been attempts to opti-
mize the amount of PTFE in the anode GDL in order to improve
the cell performance of DMFC [22e26]. Scott et al. [22] and
Oedegaard et al. [23] found that adding PTFE to the anode GDL
might lead to better gas transfer in the liquid phase and have
a positive effect on the cell performance of a DMFC. Krishna-
murthy and Deepalochani [24] concluded that anode micro-
porous layer and anode GDL should be coated with an appro-
priate amount of PTFE to achieve an ideal cell performance.
Meanwhile, Gogel et al. [25] and Xu et al. [26] found that the
anode GDL of a DMFC need not be wet-proofedwith PTFE from
the view point of enhancing the mass transport of aqueous
methanol solution. So far, there has been no clear consensus
showingwhether thePTFEcontent in theanodeGDLofDMFCis
needed or not. To our knowledge, the influence of PTFE treat-
ment of the anode GDL on the hydrogen production perfor-
mance of the PEM methanol electrolyzer cell has not been
addressedyet. In this study, theMEAswithdifferent amountof
PTFE in the anode GDL were used in experiments to analyze
their influence on hydrogen production performance of the
PEM methanol electrolyzer cell with porous metal flow field.
Moreover, the influences of operating conditions such as the
methanol concentration and the cell temperature on the
performance with the flow field were also investigated.
2. Experimental
2.1. Membrane electrode assembly
Specifications of theMEAs tested in this research are shown in
Table 1. The MEAs were made with 5 layers including anode
GDL, anode catalyst layer (CL), electrolytemembrane, cathode
CL, and cathode GDL as depicted in Fig. 1. Carbon paper
(Toray TGP-H-90) with the thickness of 0.28 mm was used as
GDL on both sides of the three MEAs. The PTFE contents in the
Table 2 e Specification of the tested sintered sphericalmetal powder for flow field.
Composition Fee19Cre12Nie2Mo (JIS SUS316L)
Grain diameter 350e500 mm
Pore ratio 48%
i n t e r n a t i o n a l j o u rn a l o f h y d r o g e n en e r g y 3 8 ( 2 0 1 3 ) 7 3e8 1 75
anode GDL of the three MEAs were varied from 0 to 5 and to
10 wt%, while that in the cathode GDL of three MEAs were the
same amount of 10 wt% as listed in Table 1. A Nafion 117
polymer membrane was used as the electrolyte for all the
MEAs. The catalyst layers were coated on both sides of the
membrane with the reaction area of 25 cm2. All the three
MEAs had the same catalyst loadings. The catalyst loading on
the anode was 1.0 mg/cm2 (PteRu), and that on cathode was
1.0 mg/cm2 (Pt). The catalysts were with carbon support and
the percentage of PteRu or Pt to carbon powderwas 50wt%. At
present, the use of binary PteRu catalyst on the anode
[17,18,27e32] is found to be the most active manner to
improve the sluggish kinetics of the MOR. During the meth-
anol oxidation reaction, methanol adsorbs on Pt surfaces and
undergoes through a sequence of dehydrogenation steps to
form adsorbed CO (i.e. COads) as shown in Reaction (4). COads
strongly adsorbs onto the Pt catalyst and can poison the anode
catalyst if only a pure Pt catalyst is used. Consequently, the
surface area of catalyst is reduced and the cell performance is
degraded. Hence, it is important to remove COads for recov-
ering the catalytic activity of Pt/C. The addition of a second
metal (i.e. Ru) to the Pt catalyst tends to improve the problem
of poisoning by carbon monoxide since Ru act as promoting
sites to oxidize water as in Reaction (7). The hydroxyl radical
(i.e. OHads) from the oxidized watermolecule oxidizes COads to
produce carbon dioxide in Reaction (8).
The bi-functional mechanism of the PteRu catalyst
mentioned above is regulated by the operating potential and
temperature. Iwasita [29] has reported that, at the potential
below 0.4 V, Pt is a good catalyst for methanol adsorption, but
not for water dissociation; while Ru is able to dissociate water
but it cannot adsorb methanol. However, the bi-functional
mechanism of the PteRu catalyst is of limited use with
further increase in potential and temperature. It is well known
that Pt can dissociate water well at high potential [29], and as
reported by Gasteiger et al. [27] and Kauranen et al. [28], Ru can
adsorb methanol at high temperature of above 60 C. For
different operating conditions (i.e. potential and temperature),
theMOR can undergoes through different reactions as follows:
Ptþ CH3OH/PtðCOÞads þ 4Hþ þ 4e (4)
Ruþ CH3OH/RuðCOÞads þ 4Hþ þ 4e (5)
PtþH2O/PtðOHÞads þHþ þ e (6)
RuþH2O/RuðOHÞads þHþ þ e (7)
ðCOÞads þ ðOHÞads/CO2 þHþ þ e (8)
Besides the COads, formaldehyde and formic acid can also be
formed as intermediate species during the MOR [18,29e32]. As
seen in the Reaction (1), the MOR requires the molecular ratio
of water to methanol to be 1:1. A complete 6 electrons anodic
oxidation to CO2 can be completed as the molecular ratio of
water to methanol has to be much higher than the stoichio-
metric 1:1 ratio [18,32]. In contrast, if the water in the anode
catalyst layer is insufficient, the MOR will be incomplete to
form either formic acid or formaldehyde as shown in Reac-
tions (9) and (10):
CH3OHþH2O/HCOOHþ 4Hþ þ 4e (9)
CH3OH/HCOHþ 2Hþ þ 2e (10)
If the low methanol concentration is applied to the PEM
methanolelectrolysis, themolecularratioofwatertomethanol is
muchhigher than thestoichiometric1:1 ratio.Consequently, the
formationofeitherformicacidorformaldehydecanbeneglected.
2.2. Porous flow field
Table2showsspecificationsofthesinteredmetalpowderporous
materialusedforflowfieldof thePEMmethanolelectrolyzercell
in this study. The metal powder was made of a corrosion-
resisting type stainless steel (JIS SUS316L; Fee19Cre12Nie2Mo)
by an inert gas atomization method. Spherical metal powders
with 350e500 mm grain diameter were placed in the separator
block and sintered each other and also sintered to the separator
block. The sintered metal powder is in a porous structure with
a porosity of around 48%. The surface image of the porous
structurewhichwas obtainedwith a laser scanningmicroscope
(Keyence VK-9700) is shown in Fig. 2. The separator block was
madeofthesamematerialasthemetalpowderandhadtheflow
field depth of 2mm. The flowfield volumewas 2.9 cc.
2.3. Experimental setup
This study used a single cell for the experiments. Setup of the
tested hydrogen production cell including end plates, gaskets,
collectors, separators, and MEA is schematically shown in
Fig. 3. The silicon rubber gaskets were used for sealing the cell.
The tightening torque of cell assembling bolts was set evenly
at 120 cNm for all the experiments. The electrolysis was
conducted by applying electric current from a DC power
supply to the electrolyzer at a constant voltage mode to
generate hydrogen at the cathode. Temperatures of the cell
and aqueous methanol were controlled during experiments
by putting them into a constant temperature vessel (As one
DOV-450P). Methanolewatermixtureswere fed into the anode
by using a peristaltic pump, the cell temperature was
measuredwith a thermocouple. AC impedancemeter (Kikusui
KFM2030) was used to measure the cell impedance with
a frequency range from 3000 to 0.1 Hz.
3. Results and discussion
3.1. Influence of PTFE treatment of the anode GDL
3.1.1. Hydrogen production performanceFig. 4 shows the influence of PTFE treatment of the anode GDL
on hydrogen production performance of the PEM methanol
0
0.05
0.10
0.15
0.20
0.3 0.4 0.5 0.6 0.7
10wt% PTFE in the anode GDL
0wt%
5wt%
Aqueous methanol concentration: 2.6MAnode feed rate: 10cc/minCell temperature: 303K
Cell voltage [V]
Cu
rren
t d
en
sity [A
/cm
2
]
Fig. 4 e Influence of PTFE treatment of the anode GDL on
the hydrogen production performance with 2.6 M aqueous
methanol concentration.Fig. 2 e Surface of the tested sintered spherical metal
powder for flow field.
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 8 ( 2 0 1 3 ) 7 3e8 176
electrolyzer cell with the three MEAs shown in Table 1. The
porous metal flow field which exhibited higher hydrogen
production performance than the conventional groove type
flow field [14] was employed in this study. Aqueous methanol
solution with 2.6 M concentration was fed to the anode at the
flow rate of 10 cc/min. Temperatures of the cell and aqueous
methanol solution were set at 303 K. The obtained results
indicate that current density of the PEMmethanol electrolyzer
cell is increased by reducing the amount of PTFE in the anode
GDL. The MEA without PTFE in the anode GDL shows the
highest current density. Because the current density is theo-
retically proportional to the rate of hydrogen production, this
signifies that hydrogen production performance of the PEM
methanol electrolyzer cell is improved by reducing the
amount of PTFE in the anode GDL, and the MEA without PTFE
in the anode GDL exhibits the best hydrogen production
performance.
3.1.2. Impedance analysisElectrochemical impedance spectroscopy is an effective tool
for investigating the phenomena in fuel cell [33e35] or PEM
electrolysis cell [2,5,6,8]. Since the influence of PTFE amount
Gasket
Anode inlet
End plate
Collector
Separator
Carbon paper
Anode outlet
Cathode outlet
End plate
Collector
Separator
Carbon paper
Cathode outletMEA
Fig. 3 e Setup of the tested electrolyzer cell with proton
exchange membrane.
on cell can be recognized by the changes in cell resistance and
reaction resistance obtained from impedance analysis, the
electrochemical impedance spectroscopy was applied to the
electrolyzer cell in this study. Fig. 5 shows the AC impedance
of the cell measured at the current density of 0.2 A/cm2 for the
three cases with different PTFE contents of 0, 5, and 10 wt% in
the anode GDL. The impedance data were obtained at the
frequencies from 3000 to 0.1 Hz. The figure is a ColeeCole plot
showing the imaginary part Im Z and real part Re Z of the
measured complex impedance Z:
Z ¼ ReZþ jImZ (11)
The first intersection of the arc and horizontal axis corre-
sponds to the cell resistance including membrane, electrodes,
gas diffusion layers, separators, and collectors. While the
difference between the low and high frequency intercept
corresponds to the reaction resistance which includes acti-
vation resistance and diffusion resistance. As seen in Fig. 5,
the cell resistances decrease with reducing the amount of
PTFE in the anode GDL. The reduced cell resistances can be
mainly caused by a lower interfacial contact resistance
between the MEA and anode flow field because the difference
among three setups is just the amount of PTFE in the anode
Aqueous methanol concentration: 2.6MAnode feed rate: 10cc/minCurrent density: 0.2A/cm2
Cell temperature: 303K5wt% PTFE in the anode GDL
10wt%
0wt%
5
10
15
010 15 20 25 30 35
ReZ
-Im
Z
f=0.8Hz
f=2000Hz
Fig. 5 e AC impedance data with different amount of PTFE
in the anode GDL.
Methanol concentration [M]
0.55
0.60
0.65
0.70
0.75
0 1 2 3 4 5 6
with PTFE (MEA3)
w/o PTFE (MEA1)
Anode feed rate: 10cc/minCurrent density: 0.15A/cm2
Cell temperature: 303K
Cell vo
ltag
e [V
]
Fig. 6 e Influence of PTFE treatment of the anode GDL on
the hydrogen production performance with different
aqueous methanol concentrations.
333K40
45
50
55
60
65
70
75
0 1 2 3 4 5 6
303K
Surface tension (mN/m)303K 333K
Water 71.18 66.36Methanol 22.02 19.27
Methanol concentration [M]
Su
rface ten
sio
n [m
N/m
]
Fig. 7 e Surface tension of aqueous methanol solutions.
i n t e r n a t i o n a l j o u rn a l o f h y d r o g e n en e r g y 3 8 ( 2 0 1 3 ) 7 3e8 1 77
GDL. Due to the non-conductive property of PTFE, the increase
in amount of PTFE on the anode GDL surface results in higher
interfacial contact resistance between the MEA and anode
flow field. In addition, water content inside the membrane
may also contribute to the difference in cell resistances. By
reducing the amount of PTFE in the anode GDL, the water
content inside the membrane can be increased. This may
result in higher ionic conductivity of the membrane [37] and
lead to the reduction in cell resistances.
With reducing the amount of PTFE in the anode GDL, the
reaction resistances are also lowered as shown in Fig. 5. The
low frequency range of the ColeeCole plot represents the
diffusion resistance, and the high frequency range represents
the activation resistance. The lower reaction resistance with
reduced PTFE conditions is mostly caused by the reduction in
diffusion resistancewhich appears on the right side of the arc.
An increased wettability of the anode GDL with reducing PTFE
amount can be a main reason for the decreased diffusion
resistance. With the increased wettability of GDL, more
aqueous methanol solution can be diffused through the GDL
to the anode catalyst layer. Here, the removal of CO2 may
adversely affect the diffusion resistance. Some reports indi-
cate that the appearance of PTFE in the anode GDLmay lead to
a better gas transfer in DMFC [22,23]. However, the effect on
diffusion of aqueous methanol solution by the increased
wettability was more dominant as shown in Fig. 5.
The results of impedance analyses suggest that the lower
cell resistance and reaction resistance are the reasons for the
improved hydrogen production by reducing the amount of
PTFE in the anode GDL. Therefore, from a view point of
improving the hydrogen production performance by reducing
the cell resistance and enhancing the supply of reactants to
the anode catalyst layer, the carbon paper without PTFE
treatment can be preferred to be the anode GDL of PEM
methanol electrolyzer cell employing the PFF made of SMP.
3.2. Influence of aqueous methanol concentration
Fig. 6 shows the influence of PTFE treatment of the anode GDL
on hydrogen production of the PEMmethanol electrolyzer cell
with different aqueous methanol concentrations including 1,
2, 2.6, 3, 4, and 6 M at the current density of 0.15 A/cm2. Two
typical MEAs with different PTFE content of 0 and 10 wt% in
the anode GDL were used in the experiments of this section.
The anode feed rate and cell temperature were set at the same
conditions as the experiments shown in Fig. 4. From the
results, it could be firstly seen that the MEA without PTFE in
the anode GDL (i.e. MEA1) exhibited lower applied voltage
compared to the MEA with 10 wt% PTFE in the anode GDL
(i.e. MEA3) at any tested aqueous methanol concentrations.
Because the current density is theoretically proportional to
the rate of hydrogen production, the lower applied voltage
results in higher hydrogen production efficiency.
For both MEAs, the applied voltage decreases with
increasing methanol concentration in the low concentration
range. This may be related to the change in surface tension of
aqueous methanol solution with concentration shown in
Fig. 7. The surface tension in the figure was estimated based
on the experimental data and correlation reported by Vazquez
et al. [36]. Due to the lower surface tension of methanol
compared to water, higher concentration solution has lower
surface tension and higher wettability. The higher wettability
may allowmore aqueousmethanol diffuse through the GDL to
the anode catalyst layer and result in lower applied voltage at
the same current density.
In the high concentration range, the applied voltage tends
to increase with increasingmethanol concentration in spite of
the decrease in surface tension. The change in membrane
conductivity with methanol concentration can be a reason for
this trend. Mukundan et al. [38] reported that proton
conductivity of Nafion 117 immersed in 50 wt% aqueous
methanol was about 35 mS/cm at the temperature of 303 K
which is about 50 mS/cm lower than that in liquid water. As
known, Nafion membrane is described as a series of clusters
interconnected by narrow pores. The hydrophilic regions
around the clusters of sulphonated side chains can lead to the
absorption of large quantities of water. Within these hydrated
regions, the Hþ ions are weakly attracted to the SO3 group and
are able to move. Although the hydrated regions are some-
what separate, it is still possible for the Hþ ions to move
through the supporting long molecule structure of Nafion
membrane if the effective hydrated regions are large enough
to facilitate their movement [15]. Due to the lower polarity of
methanol compared to water, the increase in methanol
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 8 ( 2 0 1 3 ) 7 3e8 178
concentration may increase the cluster size of Nafion
membrane [12], and thus may reduce the effective hydrated
regions. This may decrease ionic conductivity of the electro-
lyte membrane and contribute to the increased resistance of
electrolyzer cell as plotted in Fig. 8. The increased cell resis-
tance by increasing methanol concentration leads to higher
applied voltages in the high concentration range as shown in
Fig. 6.
The applied voltage with the MEA1 in Fig. 6 is lowest at
2.6 M aqueous methanol concentration, while that with the
MEA3 is lowest at 3M. The difference in this “minimum-point”
between theMEA1 andMEA3 can be explained by the different
amount of PTFE in the anode GDL. Due to its higher wetta-
bility, the MEA1 which has no PTFE treatment of the anode
GDL may allow more aqueous methanol solution diffuse
through the GDL to the anode catalyst layer compared to the
MEA3 at the same aqueousmethanol concentration. However,
more aqueous methanol solution diffused to the anode cata-
lyst layer may also result in reducing the ionic conductivity of
the electrolyte membrane as above mentioned, thus lowering
hydrogen production performance of the PEM methanol
electrolyzer cell at higher aqueous methanol concentration.
For this reason, the optimum methanol concentration with
the MEA3 is higher than that with the MEA1.
3.3. Influence of cell temperature
Fig. 9 shows the influence of PTFE treatment of the anode GDL
on hydrogen production performance of the PEM methanol
electrolyzer cell with different cell temperatures. Aqueous
methanol solution with 2.6 M concentration was fed to the
anode with the feed rate of 10 cc/min. As seen in Fig. 9, even
with or without PTFE treatment of the anode GDL, the current
densities at the cell temperature of 333 K are found to be
significantly higher than those at the cell temperature of 303 K
when the same voltages are applied. Regardless the cell
temperature, the casewith theMEA1 exhibits higher hydrogen
production performance than the case with the MEA3.
The measured AC impedance shown in Fig. 10 can explain
the improved hydrogen production performance by
increasing cell temperature in Fig. 9. Firstly, with increasing
temperature, the kinetic energy of reaction and the catalytic
11
12
13
14
1 2 2.6 3 4 6
Anode feed rate: 10cc/minCurrent density: 0.15A/cm2
Cell temperature: 303Kw/o PTFE (MEA1)
Methanol con
Ce
ll re
sis
ta
nc
e [m
Ω]
centration [M]
Fig. 8 e Cell resistance as a function of aqueous methanol
concentrations.
activity are enhanced, while the energy difference resulting
from the Gibbs free energy of products and reactants in the
Reaction (3) is decreased towards the negative side (i.e. reac-
tion tends to occur spontaneously). Because of this, the acti-
vation resistance is reduced at higher temperature. In
addition, as can be seen in Fig. 7, the surface tension of
aqueous methanol solution decreases at higher temperature.
The lower surface tension would allow more aqueous meth-
anol solution diffuse through the anode GDL to the anode
catalyst layer, thus reducing the diffusion resistance of reac-
tant. Due to these facts, the reaction resistance which
includes activation resistance and diffusion resistance is
reduced significantly at higher temperature. Secondly, it is
known that the water uptake (i.e. the number of water mole-
cules per sulfonic acid site) increases with temperature,
resulting in higher water content inside themembrane [37]. In
addition, even with the same value of water uptake, the ion
conductivity of Nafionmembrane increases with temperature
[37,38]. The increase in water content and ion conductivity
results in lower ionic resistance of membrane, thus the cell
resistance is reduced at higher temperature. The above anal-
ysis suggests that the reduction in ionic resistance of
membrane and reaction resistance can be the reasons for the
improved hydrogen production performance of each MEAs at
higher cell temperature.
Fig. 11 explains the improved hydrogen production
performance with reducing the amount of PTFE in the anode
GDL at the cell temperature of 333 K. From the results, it can be
seen that the cell resistance decreases with reducing the
amount of PTFE in the anode GDL. The decrease in interfacial
contact resistance and the increase in water content by
reducing the PTFE mentioned in Section 3.1.2 can be the
reasons for the reduced cell resistance. Meanwhile, unlike the
trend for the cell temperature of 303 K shown in Fig. 5, the
reaction resistance is almost similar for the two caseswith the
MEA1 and the MEA3 at higher cell temperature. The lower
surface tension of aqueousmethanol solutionwith increase in
temperature shown in Fig. 7 may be a reason for the insig-
nificant difference in reaction resistance between the two
cases. With the lower surface tension, aqueous methanol is
easily to diffuse through the anode GDL to the anode catalyst
layer, even with PTFE. This may mitigate the advantage of the
0
0.05
0.10
0.15
0.20
0.3 0.4 0.5 0.6 0.7
with PTFE(MEA3)
w/o PTFE(MEA1)
Cell voltage [V]
303K
333K
Cu
rren
t d
en
sity [A
/cm
2
]
Anode feed rate: 10cc/minAqueous methanol concentration: 2.6M
Fig. 9 e Influence of PTFE treatment of the anode GDL on
the hydrogen production performance with different cell
temperatures.
co
nversio
n efficien
cy [%
]
Anode feed rate: 10cc/minAqueous methanol concentration: 2.6M
Co
nsu
med
electric en
erg
y [kW
h/N
m
0.50
0.75
1.00
1.25
1.50with PTFE
(MEA3)
w/o PTFE(MEA1)
80
85
90333K
303K
0
5
10
15
20
0 5 10 15 20 25 30 35ReZ [mΩ]
-Im
Z [m
Ω]
Aqueous methanol concentration: 2.6MAnode feed rate: 10cc/minCurrent density: 0.2A/cm2
w/o PTFE (MEA1)
333K 303K
f=1.58Hzf=2000Hz
Fig. 10 e AC impedance data with different cell
temperatures.
i n t e r n a t i o n a l j o u rn a l o f h y d r o g e n en e r g y 3 8 ( 2 0 1 3 ) 7 3e8 1 79
non-PTFE anode GDL on aqueous methanol diffusion through
the GDL at higher cell temperature, and the reaction resis-
tance is almost similar for the two cases.
Energ
y
Current density [A/cm ]
0.05 0.10
75
0.15 0.2070
Fig. 12 e Consumed electric energy and energy conversion
efficiency of the PEM methanol electrolyzer cell with and
without PTFE in the anode GDL at different cell
temperatures.
3.4. Energy conversion efficiency
Fig. 12 shows the consumed electric energy and energy
conversion efficiency for the results in Fig. 9. The energy
conversion efficiency in the figure was calculated with the
higher heating value (HHV) of produced hydrogen and
consumed energy as follows:
h ¼ HHV of produced H2
HHV of consumed MeOHþ Consumed electric energy
(12)
The rates of hydrogen production and methanol
consumption for the Eq. (12) were estimated by the Reaction
(3) with the measured current densities in Fig. 9, while the
HHV values of methanol and hydrogen were at standard
condition (i.e. 298 K, 1 atm).
The results in Fig. 12 indicate that energy conversion effi-
ciency of the PEM methanol electrolyzer cell with the MEA1 is
higher than that with the MEA3 at the both cell temperatures
0
5
10
15
20
0 5 10 15 20 25 30 35
-Im
Z [m
Ω]
ReZ [mΩ]
Aqueous methanol concentration: 2.6MAnode feed rate: 10cc/minCurrent density: 0.2A/cm2
Cell temperature: 333K
w/o PTFE(MEA1) with PTFE
(MEA3)
f=1.58Hzf=2000Hz
Fig. 11 e AC impedance data with the MEA1 and MEA3 at
cell temperature of 333 K.
of 303 and 333 K. Regardless the PTFE treatment of the anode
GDL, the energy conversion efficiency is improved by
increasing cell temperature. The combination of the non-PTFE
anode GDL and the increased cell temperature exhibits the
highest energy conversion efficiency among the four cases
tested here. The smaller applied voltage shown in Fig. 9 which
lowers the consumed electric energy in Fig. 12 is the reason for
the improved energy conversion efficiency. The PEM meth-
anol electrolyzer cell achieves quite high energy conversion
75
80
85
90
w/o PTFE with PTFE w/o PTFEwith PTFE
Aqueous methanol concentration: 2.6MAnode feed rate: 10cc/minCurrent density: 0.2A/cm2
En
erg
y co
nversio
n efficien
cy [%
]
Fig. 13 e Comparison of energy conversion efficiency at the
cell temperatures of ( ) 303 K and ( ) 333 K.
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 8 ( 2 0 1 3 ) 7 3e8 180
efficiency at low current densities. When increasing the
current density, the energy conversion efficiency tends to
decrease. However, the use of the non-PTFE anode GDL or the
increased cell temperature can ease this deterioration.
Fig. 13 shows the comparison of the energy conversion effi-
ciency at the current density of 0.2 A/cm2 for the four cases in
Fig. 12. By employing the porous flow field made of sintered
spherical stainless steel powder, the cell without the PTFE treat-
mentoftheanodeGDLcanachieveaveryhighenergyconversion
efficiency of approximately 84.2% at a cell temperature of 333 K.
The utilization of awaste heat at this relatively low temperature
can be amethod to save the energy for producinghydrogen.
4. Conclusion
This study newly investigated the influence of PTFE treatment
of the anode GDL on the hydrogen production performance of
PEM methanol electrolyzer cell with porous metal flow field.
Results derived from the experiments can be summarized as
follows:
(1) Hydrogen production performance of the PEM methanol
electrolyzer cell was improved by reducing the amount of
PTFE in the anode GDL. From a view point of improving the
hydrogen production performance, the carbon paper
without PTFE treatment can be preferred to be the anode
GDL of PEM methanol electrolyzer cell employing the PFF
made of SMP.
(2) Themeasured AC impedance data indicated that the lower
cell resistance and reaction resistancewere the reasons for
the higher hydrogen production performance by reducing
the amount of PTFE in the anode GDL. The lower cell
resistance can be mainly explained by the decrease in
interfacial contact resistance by reducing the PTFE which
is non-conductive material and increases the interfacial
contact resistance between the GDL surface and flow field,
while the lower reaction resistance can be attributed to the
increase in wettability of the anode GDL by reducing the
PTFE.
(3) Hydrogen production performance of the cell was
improved by increasingmethanol concentration in the low
concentration range. The lower surface tension of the
solution with increasing methanol concentration can be
a reason for this improvement. In the high concentration
range, the hydrogen production performance tended to
decrease with increasing methanol concentration. This
may be explained by the decrease in the ionic conductivity
of the electrolyte membrane by containing methanol.
(4) Increase in cell temperature improved the hydrogen
production performance in the PEM methanol electrolyzer
cell due to the decreases in ionic resistance of membrane
and reaction resistance. By reducing the PTFE, the cell
performance was also improved at the elevated tempera-
ture. However, the decrease in reaction resistancewas less
significant and the reduced contact resistance was the
main reason for this improvement.
(5) Energy conversion efficiency of the PEM methanol elec-
trolyzer cell was improved by reducing the amount of PTFE
in the anode GDL and increasing cell temperature. By
employing the porous flow fieldmade of sintered spherical
stainless steel powder, the PEM methanol electrolyzer cell
achieved very high energy conversion efficiency of
approximately 84.2% at a cell temperature of 333 K and
a current density of 0.2 A/cm2.
Acknowledgement
The authors express their gratitude to The Sanyo Special Steel
Co., Ltd for help with the sintered spherical metal powder
stainless steel material used for the porous flow field in this
research.
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