Dec 3, 2024
8:00pm - 10:00pm
Hynes, Level 1, Hall A
Dan Donnelly III1,Moon Young Yang2,Seung Soon Jang3,Nicholas Dimakis4,William A. Goddard III2,Eugene Smotkin1
Northeastern University1,California Institute of Technology2,Georgia Institute of Technology3,The University of Texas at Rio Grande Valley4
Dan Donnelly III1,Moon Young Yang2,Seung Soon Jang3,Nicholas Dimakis4,William A. Goddard III2,Eugene Smotkin1
Northeastern University1,California Institute of Technology2,Georgia Institute of Technology3,The University of Texas at Rio Grande Valley4
Nafion has been a dominant ionomer membrane for low-temperature (~80 °C) fuel cells and electrolyzers for nearly 50 years, because of its superior chemical-mechanical stability and high protonic conductivity. Nafion morphology comprises hydrophobic (semicrystalline), interphasial (interphasial), and water-rich domains. The hydration-level-dependent size, shape, and interconnectivity of domains remains elusive, and has limited ionomer development for high-temperature operations.<br/><br/>For any hydrated Nafion membrane, characterized by a bulk H<sub>2</sub>O/SO<sub>3</sub>(H) ratio (λ), our classical molecular dynamics (CMD) simulations show a wide distribution of local λ values (λ<sub>loc</sub>). We used density functional theory (DFT) based vibrational normal mode analysis to generate unique λ<sub>loc</sub> = 0-15 spectra, each of which contributes to overall membrane FTIR transmission spectra. For λ<sub>loc</sub> < 3, the SO<sub>3</sub>H proton remains covalently bound (i.e., C<sub>1</sub> local symmetry), and yields normal modes that correspond to IR bands ~1414 and ~910 cm<sup>-1</sup> (C<sub>1 </sub>bands). For λ<sub>loc</sub> ≥ 3, the proton dissociates to form SO<sub>3</sub><sup>−</sup> (C<sub>3V </sub>local symmetry), which yields normal modes corresponding to C<sub>3V</sub> bands ~1060 and ~970 cm<sup>-1</sup>. We now correlate the coexistence of C<sub>1</sub> and C<sub>3V</sub> bands during membrane hydration/dehydration to SO<sub>3</sub><sup>−</sup>/SO<sub>3</sub>H ratios (i.e., protonation levels) generated by reactive force field (ReaxFF) MD simulations.<br/><br/>CMD simulations, governed by classical equations of motion, fail to model the dynamic exchange of protons between SO<sub>3</sub>(H) groups (i.e., exchange sites) and water/hydronium. We used ReaxFF in Nafion MD simulations to model this exchange, and to derive λ-dependent protonation levels. This is the first such use of ReaxFF, to the best of our knowledge. Our MD systems comprised 320 exchange sites, and were hydrated as follows: λ = 0, 1, 2, 3, 5, 7, 10, 15, 20. We relate the ReaxFF generated protonation levels to C<sub>1</sub> and C<sub>3V</sub> transmission-IR band intensity changes, resulting from sub-λ aliquots of water vapor injected into an initially dehydrated Nafion membrane. Illustrations of ReaxFF MD structures reveal nano-phase segregation and heterogeneity in water environments. Inner-sphere waters contribute to λ<sub>loc</sub> values and outer-sphere waters do not. Inner sphere waters either bridge multiple exchange sites (bridged) or hydrate single SO<sub>3</sub>(H) groups (non-bridged). Outer-sphere waters are either isolated or bulk-like. The applicability of our coordinated experimental/theoretical approach to hydrocarbon-based ionomers will be described.