July 2006
Communications of the American Ceramic Society
2307
1
1
0
0
0
0
0
.2
.0
.8
.6
.4
.2
.0
1.4
Table I. Characteristics of Cells and their Y O -Stabilized
3
2
7
7
8
8
00 °C
50 °C
00 °C
50 °C
ZrO (YSZ) Electrolyte Films
2
NSCELL
1.2
NYCELLA NYCELLB NYCELLC
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0
0
0
0
.0
.8
.6
.4
.2
Thickness of YSZ
28
66.1
1.02
8
10
67.1
film (mm)
Activation energy of YSZ
film (kJ/mol)
68.6
Open circuit voltage of
cells at 8001C (V)
Maximum power density at 1.12
1.02
1.35
1.01
1.13
2
8
001C (W/cm )
0.0
0
1
2
3
4
Current density (A/cm2)
2
densities are 1.14, 0.82, 0.49, and 0.28 W/cm at 8501, 8001, 7501,
and 7001C, respectively.
Fig. 5. The I-V-P characteristic of NSCELL with a 12 mm thick Y
2 3
O -
Figure 6 shows two typical impedance spectra under the
open-circuit condition at 8001C for both NYCELL and
NSCELL. The NYCELL was tested using humidified hydro-
gen as fuel, and the NSCELL was operated using methane as
fuel. The total area specific resistance of the NYCELL at 8001C
stabilized ZrO
oxidant.
2
(YSZ) film. Methane was used as fuel and ambient air as
Fig. 2(d), was composed of spherical-shaped particles with an
average particle size of 0.2 mm.
2
2
was 0.35 O ꢀ cm , of which 0.04 O ꢀ cm came from the YSZ
(
2) Microstructure of YSZ Film and Electrode
2
electrolyte film and 0.31 O ꢀ cm from the interfacial polarization
Figures 3(a) and (b) show the surface micrographs of the NiO–
YSZ anode-supported YSZ film and the NiO–SDC anode-sup-
ported YSZ film, respectively. It can be seen that the YSZ films
were composed of irregular grains without cracks or pinholes.
The green YSZ film possessed a relative density of 46% before
sintering. After sintering at 14001C for 4 h, the relative density
increased to 97%. The shrinkage of the NiO–YSZ anode and
the NiO–SDC anode was 21.64% and 21.70%, respectively. The
resistance. So, for the NYCELL, the resistance of YSZ film was
only about 11.4% of the total cell resistance. For the NSCELL,
the resistance of YSZ film was 12.5% of the total cell resistance
when methane was used as fuel. So, the cell performance was
basically limited by the electrode polarization rather than the
YSZ film resistance.
Several NYCELLs were fabricated and tested with humidi-
fied H as fuel and ambient air as oxidant. Table I summarizes
2
the characteristics of these cells including the thickness of YSZ
films, values of the activation energy of YSZ films, OCV of cells,
and maximum power densities.
‘
‘z-direction’’ shrinkage of the YSZ electrolyte film was calcu-
lated by comparing the thickness of the green film with the
sintered film. The results showed that the ‘‘z-direction’’ shrink-
age for the NiO–YSZ anode-supported film was 21.8%, while
this ratio for the NiO–SDC anode-supported film was 22.4%.
Figure 3(c) shows the cross-sectional SEM micrograph of the
NYCELL with a 10 mm thick YSZ film. Figure 3(d) exhibits the
cross-sectional view of the NSCELL with a 12 mm thick YSZ
film. As can be seen from Figs. 3(c) and (d), the YSZ films were
almost fully dense, and both the anode and the cathode exhib-
ited a porous structure. The anode porosity was about 63% as
tested using the standard Archimedes method. The porosity for
cathode was estimated from the SEM photos to be about 45%.
Figure 4 shows the I-V-P characteristic of NYCELL with a
IV. Conclusions
In conclusion, high-quality YSZ electrolyte films were success-
fully fabricated on porous NiO–YSZ and NiO–SDC anode
substrates by a handy film fabrication technique. The cells ex-
hibited excellent performance in the intermediate temperature
range of 6001–8001C. The impedance results showed that the
performance of the cell was controlled by the electrode polari-
zation rather than the resistance of YSZ electrolyte films.
1
1
6
0 mm thick YSZ film. The maximum power densities are 1.64,
.40, 1.06, 0.60, and 0.30 W/cm at 8501, 8001, 7501, 7001, and
501C, respectively. It was seen that the open circuit voltage
2
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(
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3
4
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6
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Fig. 6. Impedance spectra of cells measured under the open-circuit
condition.
&