Modeling of degradation mechanisms in low temperature fuel cells. Thomas Jahnke, Georg Futter

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DLR.de Chart 1 Modeling of degradation mechanisms in low temperature fuel cells Thomas Jahnke, Georg Futter German Aerospace Center (DLR), Institute of Engineering Thermodynamics, Computational Electrochemistry, Pfaffenwaldring 38-40, 70569 Stuttgart, Germany

DLR.de Chart 2 Motivation The development of predictive fuel cell models is of particular importance for the improvement of cell design and operating strategies. "Prediction is very difficult, especially about the future." Niels Bohr Why is it difficult to predict fuel cell degradation? Complex system: processes on very different time and length scales Details of the involved mechanisms often unknown Degradation depends on local conditions inside the cell Interplay of the degradation mechanisms

DLR.de Chart 3 How to derive predictive models? ANODE Educt CATHODE Educt Product Product Multi-scale cell models Model validation Degradation models PSD 3.2 2.8 2.4 2.0 100% ECSA 90% ECSA 80% ECSA 1.6 1.2 0.8 0.4 0.0-0.4 0.5 1.0 1.5 2.0 2.5 3.0 Radius / nm

DLR.de Chart 4 PART I Catalyst degradation in DMFC

DLR.de Chart 5 Reversible and irreversible degradation for DMFC: Experimental observations Experimental observation 1 : reversible and irreversible performance loss during operation Most of the loss can be recovered by short air stop (refresh procedure) Irreversible degradation is observed mainly at cathode side: loss of ECSA Questions: What are the mechanisms leading to reversible and irreversible degradation? How to describe the mechanisms by physical models? How can we avoid/reduce catalyst degradation? [1]: F. Bresciani et al., Int. J. Hydrogen Energy 39 (2014) 21647-21656

DLR.de Chart 6 Catalyst degradation in DMFC ANODE CATHODE MeOH + H 2 O O 2 CO 2 H 2 O Cell performance Reversible degradation Irreversible degradation

DLR.de Chart 7 Catalyst degradation: DMFC cell model Degradation rates depend on local conditions in the cell, e.g., local potential and local species concentrations. To obtain the local conditions coupling of the degradation with a cell model is needed The developed 1D cell model includes Species transport through the layers Multi-step reaction pathways for methanol oxidation and oxygen reduction reaction

DLR.de Chart 8 Catalyst degradation: DMFC cell model

DLR.de Chart 9 Catalyst degradation: Particle growth mechanism The loss of electrochemical active surface area (ECSA) at the cathode is mainly responsible for performance degradation Loss of ECSA is related to a growth of the platinum particles Different processes can contribute to the particle growth: Ostwald ripening Coalescence Key property for mathematical desciption: particle size distribution (PSD) N(r) Balance equation for PSD N( r, t) t + r r N( r, t) t Ostwald δ N( r, t) = δt Coal

DLR.de Chart 10 Catalyst degradation: Coalescence mechanism Movement of the platinum particles on the carbon support can lead to coalescence of the particles The coalescence can be described by an integro-differential equation for the particle distribution: r 3 3 δn( r, t) 2 N(( r r' ) = r D r N r t t ( ') ( ', ) 3 3 δ ( r r' ) Coal 0 Coalescence of two particles to one with size r Mechanisms for particle diffusion: (i) Ion attachment/detachment 1 : (ii) Adatom diffusion 2 (high temp.): 1/3 2/3, t) dr' 0 D( r) ~ r D( r) ~ r ( D( r) + D( r') ) N( r, t) N( r', t) dr Coalescence of a particle with size r [1]: S.V. Khare, N.C. Bartelt, T.L. Einstein, Physical Review Letters 75 (1995) 2148 [2]: F. Behafarid, B.R. Cuenya, Surface Science 606 (2012) 908 1 4

DLR.de Chart 11 Catalyst degradation: Ostwald ripening Change of particle sizes due to Pt dissolution and precipitation Pt Pt 2+ + 2 e The particle stability depends on the particle size (surface energy): µ GT = µ ( r) µ ( ) = 2Ωγ r Experimental observation: Degradation is accelerated by cycling. Explanation: The formation and reduction of platinum oxides play an important role for the dissolution A model for the oxide formation is needed

DLR.de Chart 12 Catalyst degradation: Effect of platinum oxides Simple platinum oxide model: Platinum oxides form a protective layer at high potentials, reducing the dissolution Pt + H 2 O PtO + 2H + + 2e - At low potential the oxides are reduced Going back to high potential leads to accelerated dissolution until the protective layer is formed again Pt Pt 2+ + 2 e Fast degradation expected after sweep from low to high potential Sweep to low potential Sweep to high potential

DLR.de Chart 13 Catalyst degradation: Effect of platinum oxides Recent experiments show that faster dissolution occurs during sweep to low potentials [1] contradiction to simple model! Advanced model: Include the place exchange between platinum and oxygen atoms Pt + H 2 O PtO surf + 2H + + 2e - PtO surf PtO bulk PtO bulk + H 2 O PtO 2 + 2H + + 2e - Dissolution occurs also during the place exchange accelerated degradation during sweep to low potentials PtO bulk + 2 H + Pt 2+ + H 2 O [1] A. A. Topalov et al., Chem. Sci. 5 (2014) 631

DLR.de Chart 14 Catalyst degradation: Modeling the particle growth The particle growth mechanisms lead to a change in the PSD and a loss of ECSA Time evolution of ECSA depends on the mechanism ECSA/ECSA 0 1.0 0.8 0.6 0.4 Experiment Simulation mechanism I Simulation mechanism II 0 100 200 300 400 500 600 700 800 9001000 Time / h

DLR.de Chart 15 Catalyst degradation: Modeling the particle growth The particle growth mechanisms lead to a change in the PSD and a loss of ECSA Time evolution of ECSA depends on the mechanism The shape of the PSD also depends on the mechanism: Tail at small particle sizes is formed during Ostwald ripening Tail at large particle sizes and second peak is formed during coalescence Analyzing the PSD (e.g. with transmission electron microscopy) can help identifying the relevant degradation mechanism PSD PSD 3.2 2.8 2.4 2.0 100% ECSA 90% ECSA 80% ECSA 1.6 1.2 0.8 0.4 0.0-0.4 0.5 1.0 1.5 2.0 2.5 3.0 Radius / nm 3.2 2.8 2.4 2.0 Ostwald ripening 100% ECSA 90% ECSA 80% ECSA 1.6 1.2 0.8 0.4 0.0 0.5 1.0 1.5 2.0 2.5 3.0 Radius / nm Coalescence

DLR.de Chart 16 Catalyst degradation: Modeling the refresh procedure Recovery of reversible degradation is observed after stopping the air flow Oxygen starvation leads to low a cathode potential (due to methanol crossover) Low potential allows for reduction of platinum oxides recovery of cell performance O 2 partial pressure / Pa 20000 15000 10000 5000 0 0 1000 2000 3000 4000 Time / s 1.0 0.8 0.6 0.4 Cathode potential / V Oxide coverage / - 1.1 1.0 0.9 0.8 0.7 0.6 0.5 0.4 0.3 0.2 0.1 0.0-0.1 0.6 0.8 1.0 Cathode potential / V Coverages / - 1.0 0.5 0.0 PtO surf PtO bulk PtO 2 0 1000 2000 Time / s 3000 4000

DLR.de Chart 17 Catalyst degradation: Modeling the refresh procedure Refresh leads to a reduction of the oxides recovery of reversible degradation But accelerated irreversible degradation due to reduction of protective layer enhanced place exchange rate Trade-off between performance optimization and irreversible degradation Oxide coverage / - 1.0 0.9 0.8 0.7 0.6 0.5 0.4 0.3 0.2 0.1 0.0 0 1000 2000 3000 4000 5000 6000 Time / s

DLR.de Chart 18 PART II Membrane degradation in PEMFC

DLR.de Chart 19 Membrane degradation Membrane degradation can occurs in terms of Membrane thinning Pin-hole formation Loss of conductivity Questions: Which mechanisms lead to membrane degradation? How can we describe these mechanisms by a physical model? How can we avoid/reduce membrane degradation?

DLR.de Chart 20 Membrane Degradation: Overview O 2 + 2H + + 2e - H 2 O 2

DLR.de Chart 21 Membrane degradation: Coupling with cell model Membrane degradation strongly depends on the local conditions Water content in the membrane Anode oxygen concentration due to crossover Anode and cathode potential Iron ion concentrations Rib Gas channel Anode Cathode Gas channel PEM Rib The degradation model has to be imbedded in a complete cell model CLs Rib Gas channel

DLR.de Chart 22 Membrane degradation: Hydrogen peroxide formation Two electron transfer: O 2 + 2H + + 2e - H 2 O 2 Equilibrium potential E 0 =0.695V Reaction rate 2 rr = kk HH2 OO 2 cc OO2 cc HH + c H 2 O 2 kk HH2 OO 2 = kk 0 exp EE aa RRRR exp ααff RRRR ηη 2ee Reaction favored by the low potential at anode Reaction rate depends on the oxygen crossover

DLR.de Chart 23 Membrane degradation: Radical formation Radical formation due to H 2 O 2 decomposition [1] [1] [1]: Ghelichi et al., J. Phys. Chem. B, 2014.

DLR.de Chart 24 Membrane degradation: Radical attack Two radical attack mechanisms can occur [1]: Unzipping of the back bones Attack on the side chains Only side chain scission affects the conductivity [1]: Ghelichi et al., J. Phys. Chem. B, 2014.

DLR.de Chart 25 Summary The development of predictive fuel cell models is challenging: Catalyst and membrane degradation are complex multi-step processes The degradation strongly depends on the local conditions inside the cell DMFC show reversible and irreversible performance degradation Irreversible degradation, related to a reduction of the electrochemical active surface area, can be described by a particle growth model Reversible degradation is caused by platinum oxide formation Both mechanisms are strongly coupled Chemical degradation of the membrane in PEMFC proceeds in several steps: Oxygen crossover from cathode to anode Hydrogen peroxide formation Radical formation Radical attack of the membrane Specific in situ and ex situ experiments are required to identify and quantify certain mechanisms

DLR.de Chart 26 "It can scarcely be denied that the supreme goal of all theory is to make the irreducible basic elements as simple and as few as possible without having to surrender the adequate representation of a single datum of experience Albert Einstein Thank you for your attention The research leading to these results has received funding from the European Union's Seventh Framework Program (FP7/2007-2013) for the Fuel Cells and Hydrogen Joint Technology Initiative under grant agreement n 256776, n.303419 and n 621216! Premium Act