Journal Pre-proof Perovskite ceramic membrane separator with improved biofouling resistance for yeast-based microbial fuel cells Domenico Frattini, Grazia Accardo, Yongchai Kwon PII:
S0376-7388(19)33379-4
DOI:
https://doi.org/10.1016/j.memsci.2020.117843
Reference:
MEMSCI 117843
To appear in:
Journal of Membrane Science
Received Date: 1 November 2019 Revised Date:
8 January 2020
Accepted Date: 12 January 2020
Please cite this article as: D. Frattini, G. Accardo, Y. Kwon, Perovskite ceramic membrane separator with improved biofouling resistance for yeast-based microbial fuel cells, Journal of Membrane Science (2020), doi: https://doi.org/10.1016/j.memsci.2020.117843. This is a PDF file of an article that has undergone enhancements after acceptance, such as the addition of a cover page and metadata, and formatting for readability, but it is not yet the definitive version of record. This version will undergo additional copyediting, typesetting and review before it is published in its final form, but we are providing this version to give early visibility of the article. Please note that, during the production process, errors may be discovered which could affect the content, and all legal disclaimers that apply to the journal pertain. © 2020 Published by Elsevier B.V.
Author Statement
Dr. Domenico Frattini : Dr. Frattini mainly contributed to the conceptualization and data curation as well as formal analysis of this paper. He also played a main role in writing original draft. Dr. Grazia Accardo : Dr. Accardo mainly contributed to the conceptualization and she helped to write original draft. Prof. Yongchai Kwon : Prof. Kwon mainly contributed to supervision of this paper and conceptualization of this research, while he played a role in doing the final revision of original/revised draft. He also designed funding for this research.
Perovskite ceramic membrane separator with improved biofouling resistance for yeast-based microbial fuel cells
Domenico Frattinia, Grazia Accardob, and Yongchai Kwona*
1
Perovskite ceramic membrane separator with improved
2
biofouling resistance for yeast-based microbial fuel cells
3 4
Domenico Frattinia, Grazia Accardob, and Yongchai Kwona*
5 6 7 8 9
a
Graduate School of Energy and Environment, Seoul National University of Science and Technology 232
Gongneung-ro, Nowon-gu, Seoul 01811, Republic of Korea. b
Center for Hydrogen Fuel Cell Research, KIST - Korea Institute of Science and Technology, Hwarang-ro
14-gil 5, Seongbuk-gu, Seoul 02792, Republic of Korea.
10 11 12 13 14 15
*Corresponding authors. E-mails:
[email protected] (Yongchai Kwon),
16 17 18
1
19
Abstract:
20
Ceramic-derived components in microbial fuel cells (MFCs) aim to substitute Nafion 117.
21
Ceramic membranes are a cheaper alternative and powders’ tailoring has beneficial flexibility for
22
proper surface morphology, porosity, controlled permeability, and water uptake. In this work,
23
differently from the fine fired ceramics or clay materials, barium-cerium-gadolinium oxides (BCGO)
24
powders, co-doped with lithium (Li) or cobalt (Co), are synthesized at a low temperature and then
25
sintered at 1400 and 1500°C to form the ceramic surface. Results show that the pore size is always
26
within a few microns, porosity can be varied greatly with firing temperature at fixed dwell time, and
27
the use of Li or Co can give smooth or corrugated porous particles, respectively. The permeability
28
tests show that the BCGO doped with Li cannot control the water flux from yeast extract-peptone-
29
D-glucose medium (YPD) with the yeast, and the absolute amount of biofouling is higher than that
30
of Nafion 117. BCGO doped with 5 mol% Co exhibits good permeability and lowers absolute
31
biofouling due to the unique surface morphology of parent powders. Thus, the ceramic separators
32
based on BCGO doped with Co can be an attractive alternative to expensive Nafion.
33 34
Keywords: ceramic membrane; barium-cerium-gadolinium oxide powder; permeability; perovskite;
35
yeast.
36
2
37
1. Introduction
38
Recently, microbial fuel cells (MFCs) have been recognized as profitable biodevices that
39
can generate energy from biomass [1]. The MFCs can be fed by pure organic compounds or waste
40
biomass, such as glucose or acetate, wastewater or food waste, while electricity can be directly
41
generated by them [2]. The key factor determining the performance of MFCs is the electron transfer
42
realization between bio-matter and conductive electrode [3]. For promoting the electron transfer,
43
there are two ways. First, the mediated electron transfer (MET), where mediators are required to
44
shuttle electrons effectively from the donor microorganism to the electrode acceptor, and second,
45
the direct electron transfer (DET) that electrons can be directly transferred to the anode. The
46
microorganism type and electrode materials determine the more effective electron transfer
47
mechanism [4,5]. Based on that, with the proper approach for anode modification [6–9] and an
48
efficient cathodic catalytic structure [10,11], MFCs can produce electricity from organic waste in a
49
direct way and at ambient temperature [12].
50
In terms of the economic feasibility breakdown [13] and the allometric scale-up approach
51
[14] indicated in the recent literature, developing anodes and membranes in a cost-effective way is
52
the first priority for the commercialization of large-scale MFCs in the near future. To accomplish
53
this goal, the exploration of new membrane material replacing the conventional Nafion must be
54
considered [15,16]. Nafion is a proton exchange polymeric material and is widely used in batteries
55
[17,18], and various fuel cells, including MFCs, for its superior properties [19]. However, this is
56
very expensive with the peak price of 2300 $·m-2 [9,16], and MFCs’ operating conditions are very
57
different from that of other fuel cells where Nafion performs well because this is best at relatively
58
high-temperature (>100ºC) and low humidity (20-30%) conditions in presence of concentrated
59
H2/H+ anodic gas streams. Thus, selecting or developing other proton exchange membranes for
60
MFCs is required [19]. As an alternative, ceramic-derived separators have been recently used
3
61
[21,22]. Fine Fired Clay (FFC) [23], earthenware [24], montmorillonite [25], and kaolinite [26]
62
belong to this category.
63
These ceramic-derived separators do not usually possess the desirable specific properties
64
that are related to proton transfer and ion selectivity, and so far, they are just used as
65
buffers/separators/filters [22,27] for catholyte production/anolyte cleaning in two-chamber MFCs.
66
In ceramic separators, the working principle is not based on the proton transport through sulfonated
67
side chain groups of Nafion and electro-osmotic drag across the membrane, but on water
68
permeation, diffusion, and evaporation through the microporous structure of the ceramic diaphragm.
69
In this prospect, the major concerns are associated with the resistance to biofouling, the selective
70
cation transport, and the high firing temperature of ceramics. To extend their availability to single-
71
chamber MFCs for power production, new ceramic-derived materials with advanced properties are
72
needed.
73
Therefore, differently from the simple FFC, kaolinite or earthenware used in literature, here
74
engineered and functional ceramics are designed. In this work, protons-conducting-only perovskite
75
systems derived from Barium Cerate (BaCeO3, BCO) co-doped with gadolinium (BCGO) and
76
lithium (Li) or cobalt (Co) are synthesized and characterized. To provide a common ceramic-like
77
microporosity, these electrolytes are sintered at two reduced temperatures, 1400 and 1500ºC, while
78
crystalline structure, surface morphology, and permeation phenomenology are deeply investigated.
79
The biofouling resistance, directly connected to the surface properties, in the worst possible
80
condition of direct and continuous contact between the separator/membrane and the microorganism,
81
the model yeast Saccharomyces Cerevisiae, is also examined both qualitatively and quantitatively.
82 83
2.1 Sol-gel synthesis and sintering of the co-doped BCGO ceramics
84
Perovskite powders with nominal composition of BaCe0.8Co0.05Gd0.15O3-δ (5CoBCGO) and
85
BaCe0.82Li0.03Gd0.15O3-δ (3LiBCGO) co-doped with Co (5 mol%) and Li (3 mol%) were prepared
86
from high-purity metal nitrate precursors of barium nitrate (Ba(NO3)2 >99.9%), cerium nitrate 4
87
hexahydrate (Ce(NO3)3·6H2O >99.9%), gadolinium nitrate hexahydrate (Gd(NO3)3·6H2O >99.9%),
88
cobalt nitrate (Co(NO3)2·6H2O >99.9%) and lithium nitrate (LiNO3, >98%). Nitrate precursors were
89
added to a small amount of distilled water (DIW) and mixed until they are fully dissolved at room
90
temperature [28]. The aqueous mixture was then heated up to 80°C and citric acid monohydrate
91
(C6H8O7·H2O >99.0%) was added to this mixture in a 1:1 molar ratio with the nitrates. A viscous
92
gel was formed after vigorous stirring for 30 min and the gel was decomposed by increasing the
93
temperature to 250°C for a few minutes to promote the combustion, in which citrate was the
94
complexing agent [29]. The sol-gel route is a convenient way to obtain a homogeneous and atomic
95
dispersion of the co-dopants to avoid the deleterious segregation and nucleation of metals without
96
using cryogenic temperatures during the synthesis [30,31]. All the reagents were purchased from
97
Sigma Aldrich (St. Louis, MO, United States), and used as received without further purification. A
98
reference perovskite powder without the second dopant (BCGO) was also prepared only for XRD
99
comparison.
100
After synthesis, powders were ground in an agate mortar and calcined at 1200°C for 2 h in
101
order to remove any impurity and to form the cubic perovskite structure. Then, pellets were
102
obtained by uniaxially pressing the powders at 150 MPa for 2 min and subsequently by sintering at
103
two different temperatures, 1400°C and 1500°C for 5 h, with heating and cooling rate of 3°C·min-1.
104 105
2.2 Structural and surface characterization of the co-doped BCGO ceramics
106
The lattice structures of the calcined ceramic powders and the Nafion 117 control sample
107
were investigated using XRD (Miniflex II, Rigaku Co., Tokyo, Japan) in the 2θ range of 5º – 90º
108
with a scan rate of 3º·min-1 and a scan width of 0.03º. Crystalline phase matching for the peaks’
109
identification was performed with PDXL software (Rigaku Co., Tokyo, Japan) and based on the
110
ICDD database. Rietveld refinement was used to estimate also the lattice parameters by using the
111
MAUD software [32,33].
5
112
The specific surface area according to the Brunauer–Emmett–Teller (BET) theory (SBET) of
113
the 5CoBCGO and 3LiBCGO calcined powders was determined from the complete nitrogen
114
adsorption isotherms at 77 K (ASAP 2010b absorptiometer, Micromeritics Instruments Co.,
115
Norcross, GA, United States).
116
Microstructure analysis and surface morphology of ceramic powders, pellets and of Nafion
117
were investigated by SEM in a high vacuum environment (Inspect F, FEI Co., Hillsboro, OR,
118
United States).
119
The outer surface of pellets was analyzed by X-ray photoelectron spectroscopy (XPS) to
120
determine single elements (Ce 3d and O 1s, 15 scans each, energy step size 0.10 eV, pass energy
121
50.0 eV) binding energy spectra in a high vacuum environment (K-Alpha+, Thermo Scientific Co.,
122
Waltham, MA, United States) on spots of 400 µm in diameter. The spectra were collected and
123
deconvoluted to interpret the chemical orbital bands of elements on the surface according to [34,35].
124 125
2.3 Permeation, water flux, and biofouling calculation.
126
The tested solutions for the liquid-vapor permeability experiments were distilled water
127
(DIW) or the yeast extract/Peptone/D-glucose (YPD) medium with active yeast. The YPD medium
128
composition was the same as previous work [36] and consisted of yeast extract (5 mg·mL−1),
129
peptone (2.5 mg·mL−1), D-glucose, and yeast (both at 13.18 mg·mL−1). Yeast extract, D-glucose,
130
and dried yeast from Saccharomyces Cerevisiae were purchased from Sigma Aldrich (St. Louis,
131
MO, United States), while Peptone was purchased from Duksan Pure Chemicals Co. (Seoul,
132
Gyeonggi-do, Republic of Korea). The liquid-vapor permeability testing procedure and calculations
133
for water flux, permeance, and dry/wet water uptake were referred from those described in the
134
literature [37,38]. A volume of 10 mL of the selected liquid, DIW or YPD+yeast, was poured in a
135
plastic vial and the ceramic separator or the Nafion 117 membrane sample was placed between the
136
vial and the cap; on the cap, there was a hole (diameter 7 mm) representing the pervaporation area
137
(38.47 mm2). The edge of the hole was sealed by an adhesive PTFE impermeable tape, while the 6
138
cap was sealed with parafilm and the bottom of the vial has an orifice to equilibrate the
139
internal/external pressures. For each sample and liquid, these tests were duplicated for
140
reproducibility's sake. The vials were placed upside down in a controlled environment, and water
141
losses were recorded every 30 min for 8 consecutive hours with a precision scale (ARG224
142
Adventurer 4 decimal digits, Ohaus Co., Parsippany, NJ, United States). The wet and dry water
143
uptakes were calculated as follow: −
=
−
= =
∙ 100
(1)
∙ 100
(2)
−
(3)
144
Where Utot and Udry are the total uptake and the dry water uptake of the ceramic separators
145
and Nafion 117 after 24 h, mi is the initial dry weight of the samples, mw is the final weight of the
146
samples after 24 h of wetting, and md is the dried weight of the samples after the 24 hours of testing
147
and a vacuum drying step to remove every trace of water, leaving only the solid residue
148
representing the biofilm. The net water uptake, Uwet is calculated simply As a difference of the total
149
and the dry uptake, as shown in equation 3. In fact, the Udry is referred to as the measure of the
150
biofouling when the YPD+yeast is used.
151
The permeability tests were carried out at the temperature of 26±2ºC (299±2 K) and 50±5%
152
of relative humidity (RH), and a small correction to the chemical potentials was necessary
153
according to the following equations for water flux, chemical potentials, and permeance [39]: =
( (
−
∙
) ∙ 60 1000 ∙ ∙ ∆!) 3.6
(4)
$%) &_( = $%) &_
*+,
+ .% & ∙ (/ − 298)
(5)
) ) $345_( = $345_
*+,
+ .345 ∙ (/ − 298)
(6)
) $345_6 = $345_( + 7/ ∙ ln :
A(_6 =
7; ∙
BBBBB
∆$
_6
<4 =345 4>?
@
(7) (8)
7
154
Where JLVP is the molar liquid-vapor permeation flux (mol·m-2·s-1), mtn and mtn+1 are the
155
relative weight losses (g) at the time point tn and tn+1, PMH2O is the molecular weight of water
156
(18.015 g·mol-1), ALVP is the exposed pervaporation area (mm2), ∆t is the time interval (30 min)
157
between tn and tn+1. For the chemical potentials, µ0liq_T and µ0vap_T, are the chemical potentials of
158
liquid water and water vapor at the temperature T (299 K); µ0liq_298K and µ0vap_298K are the standard
159
chemical potentials of liquid water and water vapor at 298 K and 1 atm (–237.18 and –228.59
160
kJ·mol-1, respectively); the coefficients γliq and γvap are the linear temperature coefficients for water
161
(liquid water –0.06985 kJ·mol-1·K-1, water vapor –0.18874 kJ·mol-1·K-1); µvap_RH is the chemical
162
potential of water vapor corrected for the actual value of RH (0.5) and the Psat-vap and Pamb are the
163
saturated vapor pressure at the experimental temperature (25.2 mmHg) and the ambient pressure
164
(760 mmHg), respectively.
165
The differential chemical potential across the separators and the membrane, ∆µLVP_RH, used
166
to calculate the permeance ϑT_RH in equation 8 (mol2·m-2·s-1·kJ-2) is the difference between the
167
corrected chemical potentials of liquid (eq. 5) and vapor (eq. 7), while BBBBB is the average molar
168
flux after 8 h. At the completion of the permeability test, the attached biofilms on the wet sample
169
were simply photographed, while the residual biofilm on vacuum-dried samples was optically
170
inspected by SEM to evaluate the yeast cells’ extend and attachment on the surface.
171
172
173
3. Results and Discussion 3.1 Preliminary characterization of the co-doped BCGO ceramic powders
174
It is important to characterize the calcined parent powders to inspect the results of the sol-gel
175
synthesis. The XRD patterns of the two co-doped BCGO powders are reported and compared with
176
those of a reference BCGO fabricated without the second dopant, and Nafion 117 (Fig. 1).
177
As expected, the XRD pattern of Nafion 117 shows a scattered background and broad peaks,
178
ascribed to its polymeric backbone (polytetrafluoroethylene, ICDD card N. 00-054-1595) that is 8
179
typical of this kind of material (Fig. 1a). In Fig. 1b, the XRD patterns of the BCGO systems,
180
together with the structural representation of the lattice cell, are reported. These systems have all
181
complex orthorhombic cell structures derived from the reference Barium Cerate BCO crystal
182
because all the peaks of the BCGO powders match with those of the orthorhombic perovskite
183
BaCeO3 (ICDD card N. 01-089-8268).
184 185
Fig. 1. XRD patterns of a) Nafion 117 membrane; b) BCGO and co-doped BCGO calcined powders.
186 187
The two co-dopants, i.e. gadolinium and lithium or cobalt, have different positions and
188
distribution in the lattice cell. In fact, it is well-known that Gd+3 cations substitute Ce+4 cations in
189
vertex positions, creating oxygen vacancies due to the different charges, but also stabilize protonic
190
defects thanks to the Ba2+ cation acceptors located at the center of the cell. By this phenomenon,
191
BCGO oxides can show the highest protonic conductivity at high temperatures (above 400-500°C),
192
but low chemical stability, and a low conductivity at low temperatures in presence of humidity and 9
193
water [40]. This is the reason why a second dopant cation is necessary and why Li and Co, which
194
have a tendency to become hydrated even at low temperature and to reduce the sintering
195
temperature, are selected.
196
In Nafion 117, the proton conduction mechanism is based on the H+ in water that transfers
197
through the membrane by the cation exchange sites on the sulfonated side chain. This is the proton
198
hopping mechanism or the Grotthus mechanism, while another mechanism is also possible, such as
199
the vehicular mechanism, in which protons are dragged through water nanochannels established
200
inside the polymeric matrix of Nafion [41] due to the chemical structure of Nafion examined by
201
XRD. The porous ceramic proton-conducting materials with (i) a perovskite crystal structure, (ii)
202
insertion of doping and (iii) co-doping acceptor cations, and (iv) high concentration of oxygen
203
vacancies can have similar behaviors to Nafion even at low-temperature ranges. The modifications
204
induced to lattice by the co-doping with Li and Co can be evaluated by the calculation of lattice
205
constant parameters with respect to the reference BaCeO3 system as reported in Table 1.
206
Table 1. Lattice constants of BCGO, 3LiBCGO, 5CoBCGO, and the ICDD reference Barium Cerate (IV).
a (Å)
b (Å)
c (Å)
BaCeO3 (database)
6.2517
8.7906
6.2771
BCGO
6.2363±1.1·10-3
8.7719±1.2·10-3
6.2638±1.1·10-3
3LiBCGO
6.2245±0.8·10-3
8.7697±1.0·10-3
6.2606±0.8·10-3
5CoBCGO
6.2383±0.5·10-3
8.7811±0.5·10-3
6.2216±0.5·10-3
207 208
Considering the effective ionic radii from Shannon [42] of Li+ (0.92 Å, eight-fold
209
coordination), Co2+ (0.90 Å, eight-fold coordination) and Co3+ (0.55 Å, six-fold coordination), the
210
most distorted cell is 5CoBCGO and it is because the radii of Co cations in 5CoBCGO are distant
211
from those of Ce4+ (0.97 Å, eight-fold coordination) and Gd3+ (1.05 Å, eight-fold coordination)
212
cations. In 3LiBCGO, the most distorted cell parameters are a, along the x-direction, and b, along
10
213
the y-direction, indicating that the small Li+ cations probably occupy a vacancy on the basal face of
214
the cell. Similarly, in 5CoBCGO, considering the higher amount of co-dopant, two parameters are
215
largely distorted (bc on the yz plane), and this indicates that the small Co2+/Co3+ cations can
216
substitute Ba2+ cations (1.42 Å, eight-fold coordination) at the center of the cell and/or occupy a
217
vacancy on the lateral face of the cell. The exact determination of the position of Li and Co in the
218
lattice cell is beyond the scope of this work and the main aim is to demonstrate successful co-
219
doping by considering the crystal structure and the unit cell parameters.
220
The morphology of 3LiBCGO and 5CoBCGO powders is observed by SEM (Fig. 2). In both
221
powders, hard aggregates (5-8 µm) of smaller particles (0.5-1 µm) are observed, and this means that
222
channels and pores between the particles are created and this is a beneficial feature for the vehicular
223
proton transport mechanism. Each aggregate is formed approx. by 10-12 particles or more.
11
224 225
Fig. 2. SEM of calcined co-doped BCGO powders a,c) 3LiBCGO 20000x, b) 5CoBCGO 20000x, and d)
226
5CoBCGO 30000x.
227 228
Regarding morphology, that of each sample is different. 3LiBCGO aggregates have a
229
smooth and rounded surface while sometimes the internal surfaces can show some roughness. The
230
5CoBCGO aggregates are a little bit smaller and show a less curved shape with more edges,
231
microchannels and the presence of small protuberances on the surface. This is a unique feature of
232
BCGO doped with Co, not observed in 3LiBCGO or BCGO. The specific surface area and average
233
pore size of these powders observed by BET measurements are given inTable 2.
234
Table 2. BET specific surface area and average pore size of calcined powders.
12
SBET (m2·g-1)
Average pore size (nm)
3LiBCGO
0.631
5.15
5CoBCGO
0.539
5.96
235 236
The pore size of both powders is close to 5 nm, and this is a suitable size for the vehicular
237
transport mechanism that is related to the transport of protons in presence of gas/liquids, resembling
238
Nafion [41]. However, due to the formation of hard aggregates, the specific surface area is greatly
239
reduced to 0.6 m2·g-1. Usually, the specific surface area of these materials is 6-8 m2·g-1 [43],
240
approximately ten times higher than those of Table 1. Namely, the actual surface area of co-doped
241
BCGO powders is reduced by one-tenth of the normal value because each aggregate is constituted
242
by at least 10-12 particles as observed in Fig. 2.
243
In terms of the sintering behavior of the powders at different sintering temperatures, Fig. 3
244
represents the micrographs of the sintered surfaces of 3LiBCGO and 5CoBCGO at 1400 and
245
1500°C for 5h.
13
246 247 248
Fig. 3. SEM of sintered pellets at 1500°C for 5 h a) 5CoBCGO; b) 3LiBCGO; and at 1400°C for 5 h c) 5CoBCGO; d) 3LiBCGO.
249 250
The selection of the correct sintering temperature and of the sintering aid are critical for the
251
fabrication of co-doped BCGO ceramic separators. In fact, in Fig. 3a, the 5CoBCGO sintered at
252
1500°C shows a fully densified structure with very large grains and no visible porosity. This
253
structure is proper for high-temperature proton-conducting electrolytes based on pure hopping
254
Grotthus conduction mechanism, but not for prospective ceramic separators for MFCs applications
255
where some vehicular transport is needed [26]. On the contrary, in the structure of 3LiBCGO
256
sintered at 1500°C, the surface is not fully densified (Fig. 3b), the grains are still forming, and many
257
micrometric pores are clearly visible, meaning that this structure is more suitable as a separator for
258
MFCs. By using the same sintering aids and amounts for various Gd/Sm doped ceria electrolytes,
259
Spiridigliozzi et al. [44] have found that both Li and Co can increase the relative density of 14
260
electrolytes with cubic fluorite structure, but this seems not true for the actual non-cubic and
261
orthorhombic BCGO, and the choice of the sintering aid, along with the sintering temperature, is
262
not a trivial matter. When the sintering temperature is reduced to 1400°C, the structure of
263
5CoBCGO is still constituted by large grains but there are visibly some spaces between the grains
264
not fully attached each other (Fig. 3c), not forming a diffused porous structure, but a network of
265
interspaces with size < 1 µm, indicating that the 5CoBCGO sintered at 1400°C is proper for using
266
in MFCs and is fabricated with large well-sintered zones and few voids. For the 3LiBCGO sintered
267
at 1400°C (Fig. 3d), the structure reveals that the surface is still partially sintered with much more
268
pores than those at 1500°C, although the pore size is similar. Therefore, the co-doped ceramic
269
separators sintered at 1400°C for 5h are selected for the XPS analysis and the permeability tests.
270 271
The deconvolution and area quantification of the Ce 3d spectra of the two co-doped perovskites are shown in Fig. 4.
15
272 273
Fig. 4. Deconvoluted XPS Ce 3d spectra of BCGO, 3LiBCGO and 5CoBCGO pellets sintered at 1400°C for 5 h.
274 275
The Ce 3d spectrum is rather complex and according to Aliotta et al. [34], due to the
276
presence of both Ce3+ and Ce4+, ten components of 5 doublets pairs (V, V0, V’, V’’ and V’’’ for the
277
Ce 3d5/2 orbital, and U, U0, U’, U’’ and U’’’ for the Ce 3d3/2 orbital) can be found but usually the
278
pair V0-U0 for the Ce3+ is zeroed in doped electrolytes, leaving only the pair V’-U’ for the Ce3+,
279
suggesting a limited reduction of cerium. In fact, one benefit of doping and co-doping of ceria is
280
that, depending on the oxidation state of the dopants, the reduction of Ce4+ to Ce3+ can be limited
281
thus keeping more oxygen vacancies [45,46]. The deconvolution of spectra shows that this is the
282
case of 3LiBCGO and 5CoBCGO because, by comparing the areas ascribed to the components of
283
Ce4+ and Ce3+, there is more Ce3+ in BCGO rather than 3LiBCGO and 5CoBCGO.
16
284 285
Important information about the role of surface oxygen vacancies for the protons’ hopping Grotthus mechanism is visualized in the deconvoluted O 1s spectra in Fig. 5.
286 287
Fig. 5. Deconvoluted XPS O 1s spectra of BCGO, 3LiBCGO and 5CoBCGO pellets sintered at 1400°C for 5 h.
288 289
These spectra are simpler and characterized just by two well-separated Gaussian peaks,
290
representing two specific bonds of oxygen, i.e. the metal oxide bond M-O (approx. at 529 eV) and
291
the (metal) hydroxide bond (M)-OH (approx at 532 eV). The first bond is the structural one
292
involved in the lattice of the ceramic oxide (Olattice), representing the backbone of the material; the
293
second bond is the one ascribed to the surface defects due to the co-doping (Osurface) [35] and the
294
hydration of the oxygen vacancies as the preliminary step for proton conduction [40]. Differently
295
from non-perovskite ceria systems [34,35], and the reference BCGO prepared here, there many 17
296
more defects on the surface of the 5CoBCGO, and the peak at 532 eV is higher. Moreover, the
297
5CoBCGO perovskite has a different distribution of the defects because the relative area of the
298
Osurface peaks is larger in 3LiBCGO and BCGO, and the peak is visibly shifted by 0.5-1 eV toward
299
higher energy values. This means that the (M)-OH surface bonds of 5CoBCGO are more and
300
stronger than those of 3LiBCGO, probably improving the selective uptake of protons and water
301
thanks to the specific type and dosage of the co-dopant, providing a good morphology to the
302
sintered pellet even at the reduced sintering temperature of 1400ºC.
303 304
3.2 Permeability and biofouling behavior of Nafion 117 membrane and co-doped BCGO
305
separators
306
A Nafion 117 membrane and the 3LiBCGO and 5CoBCGO ceramic separators sintered at
307
1400°C for 5h are prepared for the permeability and biofouling tests in DIW and YPD+yeast. For
308
each replicated test, values of weight losses and molar flux are recorded.
309
Firstly, the permeability of the three samples is tested with DIW (Fig. 6). In DIW, only
310
water is transported through the sample due to the liquid-vapor permeation phenomenon. In this
311
case, the internal side of the sample is in direct contact with the liquid, whereas the external side is
312
exposed to air, hence liquid water slowly diffuses from side to side of the sample and then
313
evaporates in air due to the concentration gradient between the sides of sample and the humidity of
314
the environment. Fig. 6a shows an interesting weight loss behavior of the two ceramic separators
315
compared to Nafion 117. The weight loss of 3LiBCGO is higher than that of 5CoBCGO and Nafion
316
117 due to the higher porosity and the wettability of the surface and acts like a ceramic filter under
317
constant pressure. In Nafion 117, a remarkable weight loss is observed, while the weight loss of
318
5CoBCGO, after an initial stage, is low. Meanwhile, the water molar fluxes of the three samples
319
(Fig. 6b) confirm that the samples have different behavior. Here, 3LiBCGO becomes instantly
320
hydrated and reaches an almost stable water flux after 30 min regardless of the thickness (approx. 1
321
mm). Nafion 117 (thickness approx. 200 µm) shows also fast hydration behavior, but this is not 18
322
finalized completely, and the molar flux slowly increases over time and reaches an almost stable
323
flux after 5-6 h. The behavior of 5CoBCGO is dissimilar from previous samples. After fast
324
hydration like Nafion, its flux is reduced to the minimum and the water transport takes more time
325
due to probably small porosity, wettability, and the thickness of the ceramic separator that is far
326
thicker (approx. 1 mm) than Nafion 117 (200 µm).
327 328 329
Fig. 6. Permeability results with DIW for: a) relative weight losses; b) water flux of Nafion 117 and ceramic separators.
330 331
Taken together, this is attributed to (i) different porosity of 3LiBCGO and 5CoBCGO and (ii)
332
different wettability of the internal surface of the samples exposed to the liquid. In proton-
333
conducting ceramics, the hydration of vacancies is an important step of the transport process, and
334
dopants are added to stimulate hydration, especially at low temperatures. Combined with the
335
excessive porosity and pore size of the BCGO doped with Li, it is explained that the water transport
336
in 3LiBCGO is almost free and uncontrolled, whereas the water transport in 5CoBCGO is restricted
337
and can be controlled after an initial stage. 19
338 339
340 341 342
This hypothesis is confirmed when DIW is changed into the YPD+yeast medium. The permeability tests performed with YPD+yeast are represented in Fig. 7.
Fig. 7. Permeability results with YPD+yeast for: a) relative weight losses; b) water flux of Nafion 117 and ceramic separators.
343 344
The first important findings by observing Fig. 7 and Fig. 6 is that the water flux of
345
3LiBCGO has a tenfold increase, while both Nafion and 5CoBCGO increase just twice. In the
346
presence of the YPD+yeast liquid, the water flux data and weight loss are widely ranged. Here, the
347
YPD+yeast is a reacting medium, in which the active yeast converts the glucose substrate,
348
producing H+, electrons, extra H2O and gaseous CO2 [47]. To simulate the worst situation for
349
biofouling, the vials are placed upside down and the liquid is in direct contact with the sample. The
350
extra water and gaseous CO2 byproducts are locally produced at the internal surface of the sample
351
and an overpressure may raise, pushing water and/or gases through the membrane/separator. If the
352
porosity, pore size, and wettability are suitable, these products can easily diffuse through the
353
thickness of the sample. Based on that, it is confirmed that 3LiBCGO is not eligible as a separator 20
354
for the MFCs, especially for the single-chamber design, due to its surface structure. Its porosity,
355
wettability, and filter-like behavior induce free percolation in the presence of the YPD+yeast, and
356
this does not promote a controlled pervaporation of water when the real anodic broth of yeast-MFCs
357
is used. On the contrary, Nafion and 5CoBCGO can well resist to the overpressure attributed to the
358
YPD+yeast placed on the internal side of the membrane/separator and, even if the flux increases,
359
the percolation of liquid to the external side is not observed. However, extra sealing for gas was
360
always adopted during the tests for the vials when the YPD+yeast medium was used in order to
361
minimize the eventual gas leakage from the screw cap. According to the equations 4-8, from weight loss and water flux data, it is possible to
362 363
calculate the apparent permeance at the experimental conditions (26°C/299 K, RH 50%), A
364
The calculations for the two liquids are listed in Table 3.
365
**_C) .
Table 3. Calculated permeances at 26°C and RH 50% for Nafion, 3LiBCGO, and 5CoBCGO.
Permeance (mol2·m-2·s-1·kJ-1) DIW
YPD+yeast
Nafion 117
1.16·10-3
2.33·10-3
3LiBCGO
1.65·10-3
9.05·10-3
5CoBCGO
3.35·10-4
1.86·10-3
366 367
The values for YPD+yeast also consider the eventual gas evolved from yeast reactions and
368
diffused through the samples, and are used only for this comparison. The 3LiBCGO has always the
369
highest apparent permeance, but the transport of liquid is percolative and not diffusive, especially
370
when the liquid is changed from DIW to YPD+yeast. The 5CoBCGO and Nafion 117 have almost
371
the same permeance when tested with YPD+yeast, and they have similar transport behavior, being
372
the 5CoBCGO more apt to transport water and gas under YPD+yeast condition (1.86·10-3 mol2·m-
373
2
374
the 5CoBCGO is an appropriate ceramic separator material for the MFCs.
·s-1·kJ-1) rather than under DIW (3.35·10-4 mol2·m-2·s-1·kJ-1). With that, it can be determined that
21
375
In terms of the resistance to biofouling, after the permeability test, the vials were left upside
376
down for 24 h and then opened to observe the surface conditions of the internal and external sides
377
and to quantify the uptake of the membrane/separator. The qualitative observations of the surfaces
378
after 24 h of contact with the YPD+yeast medium are shown in Fig. 8.
379 380
Fig. 8. Photographs and SEM of biofilm on samples after 24 h of pervaporation with YPD+yeast.
381 382
Briefly, the biofouling is observed in the internal side of the samples, whereas only Nafion
383
has the biofilm eventually on the external side. This is due to (i) the micrometric thickness of the
384
membrane and (ii) the strong adhesion and penetration of yeast cells that can be transported with
385
ions and water through the nanochannels of the polymeric matrix. This is not observed for the
386
ceramic separators due to the denser thickness and this is a benefit of the ceramic-derived materials.
387
However, the two ceramic materials do not have the same biofouling resistance because, in
388
3LiBCGO, a thick fouling biofilm on the internal side is located exactly like that of Nafion, while in
389
5CoBCGO, the fouling biofilm is thin, not compact and not restricted to a precise area. The SEM
390
images of the biofilm formed on the internal sides of samples after drying show that Nafion 117 and
391
3LiBCGO have a dense and compact biofilm, while the biofilm of 5CoBCGO has many breaches, 22
392
breaks, and a not-continuos structure. The original and clean ceramic surface of the separator is
393
visible in some points. Such a strong resistance to biofouling is another benefit of the ceramic-
394
derived materials.
395
396 397
These optical observations are supported by the wet and dry uptake calculations (Fig. 9).
Fig. 9. Relative wet and dry water uptakes of Nafion 117 and co-doped BCGO with a) DIW; b) YPD+yeast.
398 399
In Fig. 9, the relative uptakes of the three samples are compared and the wet/dry
400
contributions are quantified and split. As expected, in DIW the uptake is simply given by the wet
401
contribution because only water is adsorbed and then almost completely removed upon drying. The
402
situation is a bit different when YPD+yeast is the liquid (Fig. 9b). This medium contains dissolved
403
solids and the floating yeast cells that deposit on the membrane/separators and are adsorbed inside
404
pores and not removed upon drying, thus representing the dry uptake, a permanent contribution
405
leading to biofouling, in case of the yeast cells. From the relative point of view, the percentages
406
show that Nafion 117 has always the highest uptake and the incidence of biofouling is approx. 6%,
407
one-tenth of the total uptake, in presence of YPD+yeast medium. For the two ceramic separators, 23
408
the biofouling contribution is still almost one-tenth of the total uptakes, and this represents less than
409
1%. This would mean that the two ceramic separators have a far higher resistance to biofouling, but
410
this is partially true because the relative uptakes do not consider the absolute weight and thickness
411
of the materials that are completely different from Nafion 117, as demonstrated in Table 4 and
412
Table 5.
413
Table 4. Absolute wet and dry uptakes of Nafion, 3LiBCGO, and 5CoBCGO with DIW.
Nafion 117
3LiBCGO
Weight ∆wt Weight (mg) (mg) (mg)
∆wt (mg)
5CoBCGO Weight ∆wt (mg) (mg)
Initial
80.6
-
1047.0
-
1041.3
-
Wet
133.5
52.9
1172.1
125.1
1063.1
21.8
Dry
80.7
0.1
1047.1
0.1
1041.8
0.5
414 415
The data of Table 4 for the DIW case shows that the final uptake is almost zero for all the
416
samples, but the uptake of Nafion is not higher than the ceramics. Considering the total weights, the
417
3LiBCGO can adsorb more water than Nafion in the wet condition, while 5CoBCGO adsorb less
418
water than Nafion, suggesting the possibility of its partial wetting behavior. The total wet and dry
419
uptake weights measured after the YPD+yeast permeability tests are listed in Table 5.
420
Table 5. Absolute wet and dry uptakes of Nafion, 3LiBCGO, and 5CoBCGO with YPD+yeast.
Nafion 117
3LiBCGO
Weight ∆wt Weight (mg) (mg) (mg)
∆wt (mg)
5CoBCGO Weight ∆wt (mg) (mg)
Initial
81.3
-
1025.1
-
1042.4
-
Wet
125.2
43.9
1173.5
148.4
1072.6
30.2
Dry
86.4
4.1
1033.1
8.0
1045.6
3.2
421 422
Important findings are brought by the biofouling behavior of the two ceramic materials.
423
According to Fig. 9, 3LiBCGO has a lower uptake than Nafion, but from data in Table 4, the
424
opposite result is true. In fact, 3LiBCGO adsorbs more water than Nafion (148.4 mg vs 43.9 mg)
24
425
and the final dry uptake, the biofouling, is double (8 mg vs 4.1 mg). In other words, after 24 h, on
426
3LiBCGO more fouling biofilm can be deposited than on Nafion 117, meaning that Nafion may
427
have a better biofouling resistance than 3LiBCGO. On the contrary, the amount of dry biofilm in
428
5CoBCGO (3.2 mg) is slightly smaller than that in Nafion (4.1 mg), indicating that 5CoBCGO has
429
better resistance to biofouling than Nafion 117. This result is very important because a ceramic
430
material, which has similar permeability and better biofouling resistance than Nafion, can be
431
prepared, and the 5CoBCGO material can be used as a separator in yeast-MFCs and other types of
432
MFCs with single-chamber architecture. The BCGO doped with Co exhibited the best behavior and
433
resistance to biofouling, representing a very interesting and absolutely novel advanced ceramic
434
material for MFCs.
435 436
4. Conclusions
437
In this work, two advanced ceramic materials derived from proton-conducting perovskite
438
electrolytes co-doped with Li or Co were suggested to enhance proton and water transport when
439
used as membrane/separator for single-chamber yeast-MFCs. The parent perovskite system was the
440
Barium Cerate, BaCeO3, basically doped with gadolinium (BCGO), and this was directly
441
synthesized in a one-pot sol-gel synthesis in this work. Similarly, the insertions of Li (3LiBCGO)
442
and Co (5CoBCGO) atoms were done in the same one-pot synthesis to obtain the co-doped powders.
443
These co-dopants deeply modified the lattice and the unit cell, inducing measurable distortions and
444
enhancing the proton conductivity.
445
For the application as ceramic separators in MFCs and the optimization of fabrication and
446
sintering cycle, preliminary characterizations were conducted. Sintering temperature, porosity and
447
pore size were controlled and reduced. As a result, the sintering temperature of 1400°C and the
448
dwell time of 5 h were selected as optimal conditions for both 3LiBCGO and 5CoBCGO.
25
449
The 5CoBCGO has shown excellent permeability behavior and surface morphology,
450
compared to 3LiBCGO. Very high water flux and losses in the presence of the YPD+yeast medium
451
were observed from 3LiBCGO separator. On the other hand, 5CoBCGO has shown better resistance
452
to biofouling due to the minimal uptake even in the worst condition. Based on the experimental
453
evidence so far, it can be determined that the 5CoBCGO is an eligible alternative material to Nafion
454
117 for using as a separator in yeast-MFCs and other types of MFCs with single-chamber
455
architecture.
456 457
Declaration of interest
458
The authors declare no conflicts of interest.
459 460
Acknowledgment
461
Dr. Domenico Frattini was supported by the Korea Research Fellowship through the National
462
Research Foundation of Korea (NRF) funded by the Ministry of Science and ICT of Republic of
463
Korea (No. 2017H1D3A1A01013887) and this work was also supported by the NRF and the
464
Ministry of Science, ICT and Future Planning (MSIP) (No. 2016M1A2A2937143).
465
26
466
References
467
[1]
applications. A review, J. Power Sources. 356 (2017) 225–244. doi:10.1016/j.jpowsour.2017.03.109.
468 469
C. Santoro, C. Arbizzani, B. Erable, I. Ieropoulos, Microbial fuel cells: From fundamentals to
[2]
P. Pandey, V.N. Shinde, R.L. Deopurkar, S.P. Kale, S.A. Patil, D. Pant, Recent advances in the use of
470
different substrates in microbial fuel cells toward wastewater treatment and simultaneous energy
471
recovery, Appl. Energy. 168 (2016) 706–723. doi:10.1016/j.apenergy.2016.01.056.
472
[3]
K.D.Z. Duarte, D. Frattini, Y. Kwon, High performance yeast-based microbial fuel cells by
473
surfactant-mediated gold nanoparticles grown atop a carbon felt anode, Appl. Energy. 256 (2019)
474
113912. doi:10.1016/j.apenergy.2019.113912.
475
[4]
Microbiol. 14 (2006) 512–518. doi:10.1016/j.tim.2006.10.003.
476 477
[5]
B.E. Logan, Exoelectrogenic bacteria that power microbial fuel cells, Nat. Rev. Microbiol. 7 (2009) 375–381. doi:10.1038/nrmicro2113.
478 479
B.E. Logan, J.M. Regan, Electricity-producing bacterial communities in microbial fuel cells, Trends
[6]
M. Christwardana, D. Frattini, G. Accardo, S.P. Yoon, Y. Kwon, Early-stage performance evaluation
480
of flowing microbial fuel cells using chemically treated carbon felt and yeast biocatalyst, Appl.
481
Energy. 222 (2018) 369–382. doi:10.1016/j.apenergy.2018.03.193.
482
[7]
M. Christwardana, D. Frattini, K.D.Z. Duarte, G. Accardo, Y. Kwon, Carbon felt molecular
483
modification and biofilm augmentation via quorum sensing approach in yeast-based microbial fuel
484
cells, Appl. Energy. 238 (2019) 239–248. doi:10.1016/j.apenergy.2019.01.078.
485
[8]
Y. Ahn, K.S. Yoo, L.-H. Kim, Y. Kwon, Development of biofuel cell adopting multiple
486
poly(diallyldimethylammonium chloride) layers immobilized on carbon nanotube as powerful
487
catalyst, Int. J. Hydrogen Energy. 41 (2016) 17548–17556. doi:10.1016/j.ijhydene.2016.07.124.
488
[9]
M. Christwardana, Y. Kwon, Yeast and carbon nanotube based biocatalyst developed by synergetic
489
effects of covalent bonding and hydrophobic interaction for performance enhancement of
490
membraneless microbial fuel cell, Bioresour. Technol. 225 (2017) 175–182.
491
doi:10.1016/j.biortech.2016.11.051.
27
492
[10]
S. Kang, K.S. Yoo, Y. Chung, Y. Kwon, Cathodic biocatalyst consisting of laccase and gold
493
nanoparticle for improving oxygen reduction reaction rate and enzymatic biofuel cell performance, J.
494
Ind. Eng. Chem. 62 (2018) 329–332. doi:10.1016/j.jiec.2018.01.011.
495
[11]
Y. Chung, J. Ji, Y. Kwon, Performance evaluation of enzymatic biofuel cells using a new cathodic
496
catalyst containing hemin and poly acrylic acid promoting the oxygen reduction reaction, J. Mater.
497
Chem. C. 7 (2019) 11597–11605. doi:10.1039/C9TC03071A.
498
[12]
Clean. Prod. 194 (2018) 359–371. doi:10.1016/J.JCLEPRO.2018.05.155.
499 500
[13]
[14]
J. Greenman, I.A. Ieropoulos, Allometric scaling of microbial fuel cells and stacks: The lifeform case for scale-up, J. Power Sources. 356 (2017) 365–370. doi:10.1016/j.jpowsour.2017.04.033.
503 504
V.G. Gude, Wastewater treatment in microbial fuel cells - An overview, J. Clean. Prod. 122 (2016) 287–307. doi:10.1016/j.jclepro.2016.02.022.
501 502
M.N.I. Siddique, Z.A. Wahid, Achievements and perspectives of anaerobic co-digestion: A review, J.
[15]
M. Jung, W. Lee, C. Noh, A. Konovalova, G.S. Yi, S. Kim, Y. Kwon, D. Henkensmeier, Blending
505
polybenzimidazole with an anion exchange polymer increases the efficiency of vanadium redox flow
506
batteries, J. Memb. Sci. 580 (2019) 110–116. doi:10.1016/j.memsci.2019.03.014.
507
[16]
C. Noh, M. Jung, D. Henkensmeier, S.W. Nam, Y. Kwon, Vanadium Redox Flow Batteries Using
508
meta -Polybenzimidazole-Based Membranes of Different Thicknesses, ACS Appl. Mater. Interfaces.
509
9 (2017) 36799–36809. doi:10.1021/acsami.7b10598.
510
[17]
M. Jung, W. Lee, N. Nambi Krishnan, S. Kim, G. Gupta, L. Komsiyska, C. Harms, Y. Kwon, D.
511
Henkensmeier, Porous-Nafion/PBI composite membranes and Nafion/PBI blend membranes for
512
vanadium redox flow batteries, Appl. Surf. Sci. 450 (2018) 301–311.
513
doi:10.1016/j.apsusc.2018.04.198.
514
[18]
S. Jeong, L.-H. Kim, Y. Kwon, S. Kim, Effect of nafion membrane thickness on performance of
515
vanadium redox flow battery, Korean J. Chem. Eng. 31 (2014) 2081–2087. doi:10.1007/s11814-014-
516
0157-5.
517 518
[19]
D. Huang, B.Y. Song, Y.L. He, Q. Ren, S. Yao, Cations Diffusion in Nafion117 Membrane of Microbial fuel cells, Electrochim. Acta. 245 (2017) 654–663. doi:10.1016/j.electacta.2017.06.004.
28
519
[20]
H.B. Khalili, D. Mohebbi-Kalhori, M.S. Afarani, Microbial fuel cell (MFC) using commercially
520
available unglazed ceramic wares: Low-cost ceramic separators suitable for scale-up, Int. J. Hydrogen
521
Energy. 42 (2017) 8233–8241. doi:10.1016/j.ijhydene.2017.02.095.
522
[21]
cells, Bioresour. Technol. 215 (2016) 296–303. doi:10.1016/j.biortech.2016.03.135.
523 524
[22]
V. Yousefi, D. Mohebbi-Kalhori, A. Samimi, Ceramic-based microbial fuel cells (MFCs): A review, Int. J. Hydrogen Energy. 42 (2017) 1672–1690. doi:10.1016/j.ijhydene.2016.06.054.
525 526
J. Winfield, I. Gajda, J. Greenman, I. Ieropoulos, A review into the use of ceramics in microbial fuel
[23]
I. Gajda, A. Stinchcombe, I. Merino-Jimenez, G. Pasternak, D. Sanchez-Herranz, J. Greenman, I.A.
527
Ieropoulos, Miniaturized ceramic-based microbial fuel cell for efficient power generation from urine
528
and stack development, Front. Energy Res. 6 (2018) 1–9. doi:10.3389/fenrg.2018.00084.
529
[24]
P. Theodosiou, J. Greenman, I. Ieropoulos, Towards monolithically printed Mfcs: Development of a
530
3d-printable membrane electrode assembly (mea), Int. J. Hydrogen Energy. 44 (2019) 4450–4462.
531
doi:10.1016/j.ijhydene.2018.12.163.
532
[25]
Cost Microbial Fuel Cells, ChemSusChem. 9 (2016) 88–96. doi:10.1002/cssc.201501320.
533 534
G. Pasternak, J. Greenman, I. Ieropoulos, Comprehensive Study on Ceramic Membranes for Low-
[26]
A.N. Ghadge, M.M. Ghangrekar, Development of low cost ceramic separator using mineral cation
535
exchanger to enhance performance of microbial fuel cells, Electrochim. Acta. 166 (2015) 320–328.
536
doi:10.1016/j.electacta.2015.03.105.
537
[27]
E. Yang, K.J. Chae, I.S. Kim, Assessment of different ceramic filtration membranes as a separator in
538
microbial fuel cells, Desalin. Water Treat. 57 (2016) 28077–28085.
539
doi:10.1080/19443994.2016.1183523.
540
[28]
G. Accardo, C. Ferone, R. Cioffi, Influence of Lithium on the Sintering Behavior and Electrical
541
Properties of Ce 0.8 Gd 0.2 O 1.9 for Intermediate-Temperature Solid Oxide Fuel Cells, Energy
542
Technol. 4 (2016) 409–416. doi:10.1002/ente.201500275.
543
[29]
G. Accardo, D. Frattini, H.C. Ham, S.P. Yoon, Direct addition of lithium and cobalt precursors to
544
Ce0.8Gd0.2O1.95 electrolytes to improve microstructural and electrochemical properties in IT-SOFC
545
at lower sintering temperature, Ceram. Int. 45 (2019) 9348–9358. doi:10.1016/j.ceramint.2018.07.209.
29
546
[30]
K. Huang, L. Zhang, T. Xu, H. Wei, R. Zhang, X. Zhang, B. Ge, M. Lei, J.-Y. Ma, L.-M. Liu, H. Wu,
547
−60 °C solution synthesis of atomically dispersed cobalt electrocatalyst with superior performance,
548
Nat. Commun. 10 (2019) 606. doi:10.1038/s41467-019-08484-8.
549
[31]
K. Huang, R. Wang, H. Wu, H. Wang, X. He, H. Wei, S. Wang, R. Zhang, M. Lei, W. Guo, B. Ge, H.
550
Wu, Direct immobilization of an atomically dispersed Pt catalyst by suppressing heterogeneous
551
nucleation at −40 °C, J. Mater. Chem. A. 7 (2019) 25779–25784. doi:10.1039/C9TA07469D.
552
[32]
G. Accardo, G.S. Kim, H.C. Ham, S.P. Yoon, Optimized lithium-doped ceramic electrolytes and their
553
use in fabrication of an electrolyte-supported solid oxide fuel cell, Int. J. Hydrogen Energy. 44 (2019)
554
12138–12150. doi:10.1016/j.ijhydene.2019.03.052.
555
[33]
L. Lutterotti, M. Bortolotti, G. Ischia, I. Lonardelli, H.-R. Wenk, Rietveld texture analysis from
556
diffraction images, Zeitschrift Für Krist. Suppl. 2007 (2007) 125–130.
557
doi:10.1524/zksu.2007.2007.suppl_26.125.
558
[34]
C. Aliotta, L.F. Liotta, V. La Parola, A. Martorana, E.N.. Muccillo, R. Muccillo, F. Deganello, Ceria-
559
based electrolytes prepared by solution combustion synthesis: The role of fuel on the materials
560
properties, Appl. Catal. B Environ. 197 (2016) 14–22. doi:10.1016/j.apcatb.2016.02.044.
561
[35]
Formaldehyde Oxidation, Environ. Sci. Technol. 49 (2015) 8675–8682. doi:10.1021/acs.est.5b01264.
562 563
H. Tan, J. Wang, S. Yu, K. Zhou, Support Morphology-Dependent Catalytic Activity of Pd/CeO2 for
[36]
M. Christwardana, D. Frattini, G. Accardo, S.P. Yoon, Y. Kwon, Optimization of glucose
564
concentration and glucose/yeast ratio in yeast microbial fuel cell using response surface methodology
565
approach, J. Power Sources. 402 (2018) 402–412. doi:10.1016/j.jpowsour.2018.09.068.
566
[37]
membranes, J. Memb. Sci. 520 (2016) 155–165. doi:10.1016/j.memsci.2016.07.021.
567 568
X. Luo, S. Holdcroft, Water transport through short side chain perfluorosulfonic acid ionomer
[38]
M.A. Izquierdo-Gil, V.M. Barragán, J.P.G. Villaluenga, M.P. Godino, Water uptake and salt transport
569
through Nafion cation-exchange membranes with different thicknesses, Chem. Eng. Sci. 72 (2012) 1–
570
9. doi:10.1016/j.ces.2011.12.040.
571
[39]
M. Adachi, T. Navessin, Z. Xie, F.H. Li, S. Tanaka, S. Holdcroft, Thickness dependence of water
572
permeation through proton exchange membranes, J. Memb. Sci. 364 (2010) 183–193.
573
doi:10.1016/j.memsci.2010.08.011. 30
574
[40]
J. Melnik, J. Luo, K.T. Chuang, A.R. Sanger, Stability and Electric Conductivity of Barium Cerate
575
Perovskites Co- Doped with Praseodymium, Open Fuels Energy Sci. J. 1 (2008) 7–10.
576
doi:10.2174/1876973x00801010007.
577
[41]
review, J. Polym. Sci. Part B Polym. Phys. 44 (2006) 2201–2225. doi:10.1002/polb.20861.
578 579
[42]
R.D. Shannon, Revised effective ionic radii and systematic studies of interatomic distances in halides and chalcogenides, Acta Crystallogr. Sect. A. 32 (1976) 751–767. doi:10.1107/S0567739476001551.
580 581
N.W. DeLuca, Y.A. Elabd, Polymer electrolyte membranes for the direct methanol fuel cell: A
[43]
A. Bassano, V. Buscaglia, M. Viviani, M. Bassoli, M.T. Buscaglia, M. Sennour, A. Thorel, P. Nanni,
582
Synthesis of Y-doped BaCeO3 nanopowders by a modified solid-state process and conductivity of
583
dense fine-grained ceramics, Solid State Ionics. 180 (2009) 168–174. doi:10.1016/j.ssi.2008.12.026.
584
[44]
L. Spiridigliozzi, M. Biesuz, G. Dell’Agli, E. Di Bartolomeo, F. Zurlo, V.M. Sglavo, Microstructural
585
and electrical investigation of flash-sintered Gd/Sm-doped ceria, J. Mater. Sci. 52 (2017) 7479–7488.
586
doi:10.1007/s10853-017-0980-2.
587
[45]
G. Accardo, D. Frattini, H.C. Ham, J.H. Han, S.P. Yoon, Improved microstructure and sintering
588
temperature of bismuth nano-doped GDC powders synthesized by direct sol-gel combustion, Ceram.
589
Int. 44 (2018) 3800–3809. doi:10.1016/j.ceramint.2017.11.165.
590
[46]
L. Spiridigliozzi, G. Dell’Agli, G. Accardo, S.P. Yoon, D. Frattini, Electro-morphological, structural,
591
thermal and ionic conduction properties of Gd/Pr co-doped ceria electrolytes exhibiting mixed
592
Pr3+/Pr4+ cations, Ceram. Int. 45 (2019) 4570–4580. doi:10.1016/j.ceramint.2018.11.144.
593
[47]
M. Christwardana, D. Frattini, G. Accardo, S.P. Yoon, Y. Kwon, Effects of methylene blue and
594
methyl red mediators on performance of yeast based microbial fuel cells adopting polyethylenimine
595
coated carbon felt as anode, J. Power Sources. 396 (2018) 1–11. doi:10.1016/j.jpowsour.2018.06.005.
596
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Highlights
• • • •
BCGO perovskites doped with Li and Co are compared with Nafion for MFCs Synthesis, powders surface and sintering are optimized to control porosity/pore size Permeability tests simulate single-chamber worst conditions for biofouling 5CoBCGO shows better biofouling resistance due to minimal uptake
Declaration of interests ☒ The authors declare that they have no known competing financial interests or personal relationships that could have appeared to influence the work reported in this paper. ☐The authors declare the following financial interests/personal relationships which may be considered as potential competing interests: