Deuterated Water Effect in a Room Temperature Ionic Liquid: N,N-Diethyl-N-methyl-N-2-methoxyethyl Ammonium Tetrafluoroborate
Hiroshi Abe,*,υ Yusuke Imai,υ Takahiro Takekiyo,φ and Yukihiro Yoshimuraφ
υDepartment of Materials and Science and Engineering, National Defense Academy,
1-10-20, Hashirimizu, Yokosuka, Kanagawa 239-8686, Japan
φDepartment of Applied Chemistry, National Defense Academy, 1-10-20, Hashirimizu,
Yokosuka, Kanagawa 239-8686, Japan
J. Phys. Chem. B 114, pp. 2834-2839 (2010).
Abstract
A deuterated water effect in the room temperature ionic liquid (RTIL) N,N-diethyl-N-methyl-N-2-methoxyethyl ammonium tetrafluoroborate, [DEME][BF4], is observed in its crystal domain structures; crystallization temperature, Tc; crystal superstructures; and volume contractions. The above effect, seen
in [DEME][BF4]-0.9 mol % H2O mixtures, is reduced in 1.0 mol % 0.75H2OE 0.25D2O and 0.9 mol % 0.5H2OE 0.5D2O mixtures and is completely suppressed in 1.3 mol % D2O mixtures. Interestingly, Tc decreased systemically with D substitutions of water. In contrast to the crystal state, it was found that there is no difference between H2O and D2O mixtures in the liquid state, on the basis of X-ray diffraction patterns.
At around 80-90 mol % H2O, the intermolecular correlation of [DEME][BF4] as a local structure changes to that of bulk water.
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Figure 1. |
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Figure 2. H2O and D2O concentration dependences of Q position at the maximum intensity, Qmax, of X-ray diffraction patterns (Figure 1). Qmax values increase drastically above 90 mol % H2O and D2O. |
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Figure 3. (a) X-ray diffraction intensity of pure [DEME][BF4] in electron units per molecule. Solid curve reveals calculated °i{fi(Q)}2 + R°iIi comp(Q). (b) Weighted structure function of pure [DEME][BF4]. |
Figure 4. Radial distribution function of [DEME][BF4]-x mol % H2O mixtures. At 90 mol % H2O as a crossover point from the [DEME][BF4] network to a bulk water one, molecular correlation visibly decreases. |
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Figure 5. X-ray diffraction patterns at -80 C of (a) [DEME]-[BF4]-0.9 mol % H2O, (b) -1.0 mol % 0.75H2OE 0.25D2O, (c) -0.9 mol % 0.5H2OE 0.5D2O, and (d) -1.3 mol % D2O. Closed squares show the aO ~ bO ~ 2cO modulated lattice, and open triangles show the 2aO ~ bO ~ 2cO modulated one. Open circles and closed circles are calculated positions of the orthorhombic lattices, aO ~ bO ~ cO and aO ~ bO ~ cO, respectively. |
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Figure 6. Crystallization temperature in 1 mol % (1-y)H2OE yD2O mixtures. With increasing y, Tc visibly decreases. |
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Figure 7. Rocking curves at -80 C of (a) [DEME][BF4]-0.9 mol% H2O, (b) -1.0 mol % 0.75H2OE 0.25D2O, (c) -0.9 mol % 0.5H2OE 0.5D2O, and (d) -1.3 mol % D2O. |
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Figure 8. A bonding scheme of (a) H2O and (b) D2O in crystal. In protonated water, gon-centeringh is preferred, whereas goff-centeringh occurs in deuterated water. The atomic distance between oxygens, dOO, varies depending on the interaction. |
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Figure 9. Optimized structures of the BF4--n(H2O) (n= 1-4) complex using the B3LYP/6-311++G(d,p) basis set. Green, brown, gray, and red represent the boron, fluorine, hydrogen, and oxygen atoms. In the case of the BF4--2H2O complex, the BF4- anion takes two arrangement patterns with two water molecules; one is a linear arrangement (b-1) and another is a perpendicular arrangement (b-2). The former is energetically more stable than the latter (’E=1.6 kJ/mol). |
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Figure 10. Nearly free hydrogen bond band of water mapping in the liquid and solid states. NFHB is selectively observed in the Raman spectra, where NFHB reveals the OH oscillator which does not form a hydrogen bonding network among water molecules, as in pure bulk water. |
References
Last Modified: April 1, 2009