dc.contributor.author |
Prakash, Prabhat |
|
dc.contributor.author |
Shylendran, Ardhra |
|
dc.contributor.author |
Fall, Birane |
|
dc.contributor.author |
Zdilla, Michael J. |
|
dc.contributor.author |
Wunder, Stephanie L. |
|
dc.contributor.author |
Venkatnathan, Arun |
|
dc.coverage.spatial |
United States of America |
|
dc.date.accessioned |
2012-09-20T03:32:51Z |
|
dc.date.available |
2012-09-20T03:32:51Z |
|
dc.date.issued |
2022-03 |
|
dc.identifier.citation |
Prakash, Prabhat; Shylendran, Ardhra; Fall, Birane; Zdilla, Michael J.; Wunder, Stephanie L. and Venkatnathan, Arun, “Mechanism of ion conduction and dynamics in tris(N,N-dimethylformamide) perchloratosodium solid electrolytes”, The Journal of Physical Chemistry C, DOI: 10.1021/acs.jpcc.1c09005, vol. 126, no. 10, pp. 4744-4750, Mar. 2022. |
en_US |
dc.identifier.issn |
1932-7447 |
|
dc.identifier.issn |
1932-7455 |
|
dc.identifier.uri |
http://dx.doi.org/10.1021/acs.jpcc.1c09005 |
|
dc.identifier.uri |
https://repository.iitgn.ac.in/handle/123456789/7585 |
|
dc.description.abstract |
(DMF)3NaClO4 is a soft-solid cocrystalline electrolyte with channels of Na+ ions, which can be reversibly converted to a less conductive form (DMF)2NaClO4 by the application of pressure or heat, leading to a melt- or press-castable electrolyte. Molecular dynamics simulations performed on the 3:1 stoichiometry suggest that Na+ ions conduct via a one-dimensional channel, which is supported by van-Hove autocorrelation function analysis. The simulations show that the transference number for Na+ ions is 0.43 at room temperature and exceeds 0.5 at higher temperatures in the molten mixture. The calculated activation energy for the diffusion of Na+ ions from MD simulations is 45 kJ mol-1. The minimum-energy path of Na+ ion migration in a 3:1 crystal is assessed using periodic density functional theory calculations, which provides a barrier of 33 kJ mol-1 for Na+ ion conduction, in reasonable agreement with the experimental value of 25 kJ mol-1. The motion of Na+ ions during conduction is vacancy-driven because the presence of a vacancy site enables jump events for Na+ ions. The activation energy is the penalty for a sodium ion to leave the octahedrally coordinated DMF ligand field via a transition state where only three molecules of DMF form a 3-O-Na trigonal planar geometry, with no involvement of ClO4- in the coordination sphere of the transition state. In contrast, the calculated activation energy barrier for the 2:1 stoichiometry is higher (Ea,DFT = 43 kJ mol-1, Ea,exp = 49 kJ mol-1) due at least in part to the partial coordination of strongly binding perchlorate anions with Na+ ions in the transition state. |
|
dc.description.statementofresponsibility |
by Prabhat Prakash, Ardhra Shylendran, Birane Fall, Michael J. Zdilla, Stephanie L. Wunder and Arun Venkatnathan |
|
dc.format.extent |
vol. 126, no. 10, pp. 4744-4750 |
|
dc.language.iso |
en_US |
en_US |
dc.publisher |
American Chemical Society |
en_US |
dc.subject |
Cocrystalline electrolyte |
en_US |
dc.subject |
Ion conduction |
en_US |
dc.subject |
Perchloratosodium solid electrolytes |
en_US |
dc.subject |
DMF ligand |
en_US |
dc.subject |
Van-Hove autocorrelation |
en_US |
dc.title |
Mechanism of ion conduction and dynamics in tris(N,N-dimethylformamide) perchloratosodium solid electrolytes |
en_US |
dc.type |
Article |
en_US |
dc.relation.journal |
Journal of Physical Chemistry C |
|