4.6 Article

Distribution of 1-Butyl-3-methylimidazolium Bistrifluoromethylsulfonimide in Mesoporous Silica As a Function of Pore Filling

Journal

JOURNAL OF PHYSICAL CHEMISTRY C
Volume 117, Issue 30, Pages 15754-15762

Publisher

AMER CHEMICAL SOC
DOI: 10.1021/jp404990q

Keywords

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Funding

  1. Fluid Interface Reactions, Structures, and Transport (FIRST) Center
  2. U.S. Department of Energy, Office of Science, Office of Basic Energy Sciences
  3. Energy Frontier Research Center

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Rotational dynamics of the ionic liquid (IL) 1-butyl-3-methylimidazolium bistrifluoromethylsulfonimide, [C(4)mim][Tf2N], 1, as a neat liquid, and confined in mesoporous silica were investigated by spin-spin (T-2) and spin-lattice (TO relaxation measurements and C-13 NMR spectroscopy. Translational dynamics (self-diffusion) were monitored via the diffusion coefficient, D, obtained with pulsed field gradient NMR measurements. These data were used to determine the distribution of 1 in the pores of KIT-6, a mesoporous silica with a bicontinuous gyroid pore structure, as a function of filling fraction. Relaxation studies performed as a function of filling factor and temperature reveal a dynamic heterogeneity in both translational and rotational motions for 1 at filling factors, f = 0.2-1.0 (f = 1 corresponds to fully filled pores). Spin-lattice and spin-spin relaxation times reveal that the motion of 1 in silica mesopores conforms to that expected for a two-dimensional relaxation model. The relaxation dynamics are interpreted using a two-state, fast exchange model for all motions; a slow rotation (and translation) of molecules in contact with the surface and a faster motion approximated by the values for bulk relaxation and diffusion. Compound 1 retains liquid-like behavior at all filling factors and temperatures that extend to ca. 50 degrees below the bulk melting point. Translational motion in these systems, interpreted with MD-simulated diffusivity limits, confirms the high propensity of 1 to form a monolayer film on the silica surface at low filling factors. The attractive interaction of 1 with the surface is greater than that for self-association of 1. The trends in diffusion data at short and long diffusion time suggest that the population of surface-bound 1 is in intimate contact with 1 in the pores. This condition is most easily met at higher filling fractions with successive additions of 1 increasing the layer thickness built up on the surface layer.

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