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KAYTLIN BRINKER ADVISOR: PROFESSOR PHILIP TAYLOR CASE WESTERN RESERVE UNIVERSITY Computer Modeling of Proton Exchange Membrane Fuel Cells August 4, 2009 Physics REU 2009 Final Presentation
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fuel cells ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],Figure 2:  A fuel cell is made up of layers including the electrode made of platinum, the Stern layer consisting of the electrolyte, followed by the diffuse layer where diffuse charge can be found. Figure 1:  A fuel cell is a combination of two electrodes and an electrolyte.  The electrolyte conducts  hydrogens from the anode but blocks electrons, which are forced to enter an external circuit. The electrons and protons recombine  at the cathode creating a current, and in turn,  electrical power.
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[object Object],[object Object],[object Object],Figure 3:  A model of the electrostatic potential profile in the fuel cell membrane is given by Bazant et al.  In Fig. 1a, excess protons exist in the anodic polarization layer and a deficit on the cathodic side.  Fig. 1b I is the same case; II has an excess of protons on both sides; while III displays a deficit of protons on both sides. The dashed lines show the electrical voltage increase through the external circuit [1].  existing theory Biesheuvel, P.M., Franco, A.A., Bazant, M.Z. (2009). Diffuse Charge Effects in Fuel Cell Membranes. Journal of The Electrochemical Society.  156, B225-B233.
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problem ,[object Object],[object Object],[object Object],Figure 4:  Simulation box for Nafion membrane
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model In determining the charge distribution, we first modeled the kinetics of the Stern layer with the Butler-Volmer equation for electrochemical reactions, Next, the diffuse layer is represented by equations for the relation between field and charge density, Poisson’s equation,  and the movement of ions across the membrane including the concentration gradient and electric potential, Nernst-Planck equation,  Figure 5:  First fuel cell developed in 1839 by Sir William Grove.  NASA was the first to use fuel cells, installing them for the generation of electricity on Gemini and Apollo spacecraft in the 1960s.  http://www.energysolutionscenter.org/distgen/Tutorial/Cogeneration.htm
model The field in the electrolyte  for the Stern layer is derived from the BV equation , Since an electric field must be continuous, the field from the Stern layer must match the field in the diffuse layer. The Poisson and NP equation can be solved simultaneously for a function of the potential,  Here the fractional surface charge density change is, Figure 6:  Platinum nanoparticles (gold) with long chains of Nafion (green, blue red, and yellow) where some become adsorbed over the metallic clusters. The background contains water molecules (red and white).  http://www.nersc.gov/news/annual_reports/annrep03/advances/4.1.fuelcells.html
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results Figures 7, 8, & 9:  The potential gradient in the Stern layer depends on the charge density in the membrane.  The charge density in the diffuse layer depends on the potential gradient in the diffuse layer. Because the electric field must be continuous we can self-consistently determine these quantities.  By graphing the potential gradient from both the diffuse and Stern layers, we can obtain a value for the position, r s , where they cross.  From this we know the entire charge distribution in the membrane. Stern Layer Diffuse Layer Stern and Diffuse Layers
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conclusion ,[object Object],[object Object],Figure 10:  The charge density in the diffuse layer depends on the potential gradient in the diffuse layer coming from the charge density of the membrane in the Stern layer. Diffuse Layer + Distance Platinum - - - - + + + - - - - - + + + + + + + +
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future work ,[object Object],[object Object],Figure 11:  Model of Nafion in Materials Studio
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references ,[object Object],[object Object],[object Object],[object Object],[object Object]
special thanks ,[object Object],This research was supported by the Physics REU program at Case Western Reserve University, a Research Experience for Undergraduates (REU) funded by the  NSF grant DMR-0850037.
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Kaytlin Brinker Presentation

  • 1. KAYTLIN BRINKER ADVISOR: PROFESSOR PHILIP TAYLOR CASE WESTERN RESERVE UNIVERSITY Computer Modeling of Proton Exchange Membrane Fuel Cells August 4, 2009 Physics REU 2009 Final Presentation
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  • 13. model In determining the charge distribution, we first modeled the kinetics of the Stern layer with the Butler-Volmer equation for electrochemical reactions, Next, the diffuse layer is represented by equations for the relation between field and charge density, Poisson’s equation, and the movement of ions across the membrane including the concentration gradient and electric potential, Nernst-Planck equation, Figure 5: First fuel cell developed in 1839 by Sir William Grove. NASA was the first to use fuel cells, installing them for the generation of electricity on Gemini and Apollo spacecraft in the 1960s. http://www.energysolutionscenter.org/distgen/Tutorial/Cogeneration.htm
  • 14. model The field in the electrolyte for the Stern layer is derived from the BV equation , Since an electric field must be continuous, the field from the Stern layer must match the field in the diffuse layer. The Poisson and NP equation can be solved simultaneously for a function of the potential, Here the fractional surface charge density change is, Figure 6: Platinum nanoparticles (gold) with long chains of Nafion (green, blue red, and yellow) where some become adsorbed over the metallic clusters. The background contains water molecules (red and white). http://www.nersc.gov/news/annual_reports/annrep03/advances/4.1.fuelcells.html
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  • 17. results Figures 7, 8, & 9: The potential gradient in the Stern layer depends on the charge density in the membrane. The charge density in the diffuse layer depends on the potential gradient in the diffuse layer. Because the electric field must be continuous we can self-consistently determine these quantities. By graphing the potential gradient from both the diffuse and Stern layers, we can obtain a value for the position, r s , where they cross. From this we know the entire charge distribution in the membrane. Stern Layer Diffuse Layer Stern and Diffuse Layers
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