Issue 32, 2013

Influence of ionic liquid film thickness on ion pair distributions and orientations at graphene and vacuum interfaces

Abstract

Microscopic structures, orientational preferences together with mass, number and electron density distributions of 1-butyl-3-methylimidazolium hexafluorophosphate ([BMIM][PF6]) ionic liquid (IL) have been studied on a neutral hydrophobic graphene surface, and at the IL–vacuum interface using atomistic Molecular Dynamics simulations. At the IL–graphene interface, distinct mass, number and electron density distributions are observed oscillating into the bulk region with several compact structural layers. The imidazolium ring of [BMIM] cations lies preferentially flat on the graphene surface, with its methyl and butyl side chains elongated along the graphene surface. At the IL–vacuum interface, however, the distributions of [BMIM][PF6] ion pairs are strongly influenced by the thickness of IL film. With the increase of IL film thickness, the orientations of [BMIM] cations at the IL–vacuum interface change gradually from dominant flat distributions along the graphene surface to orientations where the imidazolium rings are either parallel or perpendicular to the IL–vacuum interface with tilted angles. The outmost layers are populated with alkyl groups and imparted with distinct hydrophobic character. The calculated radial distribution functions suggest that ionic structures of [BMIM][PF6] ion pairs in IL–graphene and IL–vacuum interfacial regions are significantly different from each other and also from that in bulk regions.

Graphical abstract: Influence of ionic liquid film thickness on ion pair distributions and orientations at graphene and vacuum interfaces

Article information

Article type
Paper
Submitted
21 Mar 2013
Accepted
05 Jun 2013
First published
06 Jun 2013

Phys. Chem. Chem. Phys., 2013,15, 13559-13569

Influence of ionic liquid film thickness on ion pair distributions and orientations at graphene and vacuum interfaces

Y. Wang, A. Laaksonen and Z. Lu, Phys. Chem. Chem. Phys., 2013, 15, 13559 DOI: 10.1039/C3CP51226F

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