1 / 1

Counterion dynamics and the mechanical properties of fuel cell membranes

B. A. C. Counterion dynamics and the mechanical properties of fuel cell membranes. DMR-0454672. K. Page 1 , R. Moore 2 , J.K. Park 2 , V. García Sakai 3,4. 1 NIST, 2 University of Southern Mississippi, 3 University of Maryland, 4 CHRNS.

stash
Télécharger la présentation

Counterion dynamics and the mechanical properties of fuel cell membranes

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript


  1. B A C Counterion dynamics and the mechanical properties of fuel cell membranes DMR-0454672 K. Page1, R. Moore2, J.K. Park2, V. García Sakai3,4 1NIST, 2University of Southern Mississippi, 3University of Maryland, 4CHRNS Perfluorosulfonate ionomers (PFSIs) are of great importance in polymer electrolyte membrane fuel cell (PEMFC) applications. The CHRNS backscattering spectrometer HFBS has been used to study the most widely used PFSI, Nafion, neutralized with tetramethyl (TMA+) and tetrabutyl (TBA+) ammonium ions. Elastic scans (fig. A) unequivocally show that in both cases the onset of counter-ion mobility takes place at the -relaxation temperature, lending support to the notion of a process whereby ions hop among ionic aggregates. Further information has been obtained from quasielastic scans that probe the diffusional motion of the counter-ions. The behavior of the width of the scattering, measured above the -relaxation temperature (fig. B), suggests random jump-diffusion within confined regions. The ratio of the elastic intensity to the elastic plus quasielastic intensity (the “EISF”*), fig. C, affords additional insights into the geometry of the diffusional motion. At low T the dynamics are dominated by local motions of the alkyl “arms” of the counter-ions. At high T the counter-ions move over much larger distances. *EISF  elastic incoherent structure factor K. Page, R. Moore, J.K. Park, and V. García Sakai, paper in preparation

More Related