study of detailed degradation behavior of solid oxide ... g. schiller dlr.pdf · dlr.de • chart...
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Study of Detailed Degradation Behavior of Solid Oxide Electrolyzer Cells (SOEC)
Günter Schiller1, Michael Hörlein1, Frank Tietz2, K.A. Friedrich1
1German Aerospace Center (DLR),Institute of Engineering Thermodynamics, Stuttgart, Germany
2Forschungszentrum Jülich (JÜLICH)Institute for Energy and Climate ResearchMaterials Synthesis and Processing (IEK-1)
ICACC'16, Daytona Beach, January 24-29, 2016
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Outline
• Introduction: Need for energy storagePrinciple of solid oxide electrolysis
• Motivation and concept
• Cell manufacturing and characterization
• Degradation study and results from post-mortem analyses
• Conclusion
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Storage of Electricity from Renewable Energy Sources
Need for energy storage Increasing fluctuating power generation Mobile applications
Electrical energy difficult to store Conversion to chemical energy
Water electrolysis: H2O + Wel H2 + ½ O2
Solid oxide electrolysis is one possible conversion technology
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Principle of Solid Oxide Electrolysis
Advantages:
• High temperature (600 - 900°C)• Fast reaction kinetics• Low overvoltage• High efficiency & high current densities
• No noble metals as catalysts
• Fuel versatility: CO2 electrolysis Co-electrolysis of H2O/CO2 possible Syn-gas production External (or internal) hydrocarbon
formationProblem:Low longevity - Degradation
Pel
+ -
O2
Air H2O
O2-
Anode -Oxygen electrode
Cathode -Fuel electrode
Electrolyte
H2
e- e-
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Present Work – Motivation and Concept
Systematic study: operating parameter degradation
Temperature (T)
Fuel gas humidity (AH)
Current density (i)
Experimental concept:
Degradation experiments for 1000 h
Test rig – quadruple cell measurement
Identical temperature, gas supply (and also incidents)
Four different current densities simultaneously
Fuel electrode supported cells from FZ Jülich and CeramTec
Ni-8YSZ support | Ni-8YSZ | 8YSZ | CGO | LSCF
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Objectives
To gain fundamental understanding of degradation processes Distinguish between degradation processes Identify degradation mechanisms Correlate them with operating parameters
To optimize cells for electrolysis operation
To adapt operating parameters for low degradation
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Substrate Anode Electrolyte
Warm pressing withCoat Mix powder
or tape casting
Screen printing Cofiring of anodeand electrolyte
transparentelectrolyte
Laser-cutting todimensions up to
200 x 200 mm2
CathodeCurrentcollector
Solid oxidefuel cell
Screen printing
1200°C
1400°C
1100°C
Manufacturing Steps of SOFC Anode-Supported Cells
PVD-CGO
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Solid Oxide Electrolyser Cells: Planar Design
MaterialsAnode: (La,Sr)(Fe,Co)O3
Diffusion barrier: CGO – 1-5 µmElectrolyte: 8YSZ – 5-10 µmCathode: Ni/YSZCathode Substrate: Ni/YSZ
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I-V Curves at 750 °C as a Function of Steam Content(Flow rates: 2 l/min H2/H2O, 3 l/min air)
0,4
0,5
0,6
0,7
0,8
0,9
1
1,1
1,2
1,3
1,4
‐1,5 ‐1 ‐0,5 0 0,5 1 1,5
Cell Vo
ltage / V
Current density / A*cm‐2
750°C ‐ 7%AH
750°C ‐ 40%AH
750°C ‐ 60%AH
750°C ‐ 80%AH
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I-V Curves at 800 °C as a Function of Steam Content(Flow rates: 2 l/min H2/H2O, 3 l/min air)
0,4
0,5
0,6
0,7
0,8
0,9
1
1,1
1,2
1,3
1,4
‐1,5 ‐1 ‐0,5 0 0,5 1 1,5
Cell Vo
ltage / V
Current density / A*cm‐2
800°C ‐ 7%AH
800 C ‐ 40%AH
800°C ‐ 60%AH
800°C ‐ 80%AH
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Degradation Experiment and Impedance Data Interpretation
4 cells measured simultaneously at different current densities
Linear degradation after initial phase
Be careful with interpretation of voltage degradation rate
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Degradation Experiment and Impedance Data Interpretation
• Degradation rate at 1.5 A/cm2 only 13 % higher than at 1.0 A/cm2
• Degradation rate at 0.5 A/cm2
significantly lower
• ASR degradation rate about 30% compared to 3% voltage degradation (per 1000 h @ 0.5 A/cm2)
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13 kHz 170 Hz10 Hz
Levenberg-Marquardtalgorithm
DRT-Spectra
Impedance - Spectra
Information for improved CNLS fitting
Degradation Experiment and Impedance Data InterpretationMethod 1: DRT‐Analysis with parameter variation
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Degradation Experiment and Impedance Data InterpretationMethod 2: Physico‐chemical modelling
5 rate limiting processes: Ohmic contributions First Fuel Electrode (FE) Process: 1-2·104 Hz
Charge transfer reaction at TPB coupled with ionic transport in porouselectrode geometry
Second Fuel Electrode (FE) Process: approx. 1·103 HzCharge transfer coupled at TPB
Oxygen Electrode Process: 1-2·102 Hz Mass transport limitation: 1-2·101 Hz
Diffusion through FE-support along with gas conversion
Both methods are in good agreement!
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Equivalent circuit model
L1: High frequency induction P0: Ohmic resistance (> 105 Hz) P1: Fuel electrode process A (~ 104 Hz) P2: Fuel electrode process B (~ 103 Hz) P3: Oxygen electrode process (~ 102 Hz) P4: Fuel electrode mass transport (~ 101 Hz)
P0
P1P3 P2
P4
L1 P0 P1 P2 P3 P4
G W
Degradation Experiment and In-situ Data Interpretation
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Influence of Current Density on Degradation
Ohmic resistance contributes more than 50% of total ASR
∆R
Degradation of ohmic resistance is most severe
Oxygen electrode has small ASR but high contribution to degradation
Fuel electrode process 1 degrades while process 2 improves performance
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Influence of Current Density on Degradation
P_0: Ohmic resistance Obvious correlation with current density Linear degradation with time
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Influence of Current Density on Degradation
P_1: Fuel electrode process 1 Also obvious correlation with current density Degradation initially fast but slowing down with time
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Influence of Current Density on Degradation
P_2: Fuel electrode process 2 Offset of 1.0 A/cm2 curve is likely artifact (compare process 3) Degradation independent of current density Initial improvement of performance Very stable after initial change
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Influence of Current Density on Degradation
P_3: Oxygen electrode process Shift shown by 1.0 A/cm2 curve is likely artifact (compare process 2) Initially stable afterwards linear degradation Degradation independent of current density
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Influence of Current Density on Degradation
P_4: Fuel electrode mass transport Very little degradation Independent of current density
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Influence of Current Density on Degradation
Degradation after 1000 h Ohmic resistance: strong dependence on current density
Dependence possibly exponential
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Influence of Current Density on Degradation
Degradation after 1000 h Fuel electrode process 1: clear linear dependence on current density Other three processes: no current dependency
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Humidification
Ohmic resistance (R_0): Dependent on current density
Fuel electrode polarization (R_1+2): Lower degradation rate at higher
humidities… … but higher degradation
dependence on current density
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Humidification
Oxygen electrode polarization (R_3): Humidity has very little influence
Fuel electrode polarization (R_4): Generally small degradation Lower at higher humidity No obvious trend
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Post-mortem Analysis – Electrolyte
Reference 1000 h @ OCV 1000 h @ 1.5 A/cm2
Ohmic resistance:Weakening of YSZ|CGO|LSCF interface probably formation of cracks Visible cracks probably formed during sample preparation along weakened
microstructure
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Post-mortem Analysis – Oxygen Electrode
Reference 1000 h @ OCV 1000 h @ 1.5 A/cm2
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Post-mortem Analysis – Oxygen Electrode
1000 h @ 0.5 A/cm2
Formation of a new crystalline compound Higher polarization change more pronounced More detailed analyses necessary for reliable information on new phase
1000 h @ 1.0 A/cm2
Reference1000 h @ OCV
1000 h @ 1.5 A/cm2
Sr(Co0.8Fe0.2)O2.53
LSCF
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Post-mortem Analysis – Oxygen Electrode
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Post-mortem Analysis – Fuel Electrode
Percolation Ni almost completely percolated Ni can be separated from percolation network in cross sectionEDX measurement: no Ni depletion
Ni
YSZ
PoreConductive Phase
(Percolated Ni)
Non-percolated Ni
1000 h @ 1.5 A/cm2, 850°C and 80% MH
Non-percolated Ni
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Conclusion
Correlation between degradation and current density has been investigated Ohmic resistance dominates degradation and increases with current
density Oxygen electrode contributes significantly to degradation and is indepen-
dent of current density Higher frequency fuel electrode process is significant for degradation and
dependent of current density Lower frequency fuel electrode process is stable after initial activation and
independent of current density No degradation in mass transport limitation Results of post-mortem analyses give further information and must be
further evaluated
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Acknowledgment
I‘d like to thank my PhD student Michael Hörlein for his scientific workand strong effort and Frank Tietz and his co-workers from Forschungs-zentrum Jülich for manufacturing and providing cathode-supported cellsfor electrolysis operation.
Financial support from Helmholtz Association in the frame of theHelmholtz Energy Alliance „Stationary electrochemical solid statestorage and conversion“ is gratefully acknowledged.
Thank you for your attention
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