2022
DOI: 10.1016/j.jil.2021.100012
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Ether tails make a large difference for the structural dynamics of imidazolium-based ionic liquids

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Cited by 10 publications
(24 citation statements)
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“…The ionic liquids with the imide-type anions were the only samples that showed clearly separated peaks, whereas the other scattering patterns show broad, merging peaks. Broader peaks than the alkylated counterparts are frequently reported for ionic liquids with ether groups [79][80][81] and are the result of the more diffuse cation-anion arrangements stemming from the charge shielding of the cation core by the more polar functional groups. 49 We fitted the peaks with Lorentzian functions for a quantitative comparison of their positions.…”
Section: Small Angle X-ray Scatteringmentioning
confidence: 92%
“…The ionic liquids with the imide-type anions were the only samples that showed clearly separated peaks, whereas the other scattering patterns show broad, merging peaks. Broader peaks than the alkylated counterparts are frequently reported for ionic liquids with ether groups [79][80][81] and are the result of the more diffuse cation-anion arrangements stemming from the charge shielding of the cation core by the more polar functional groups. 49 We fitted the peaks with Lorentzian functions for a quantitative comparison of their positions.…”
Section: Small Angle X-ray Scatteringmentioning
confidence: 92%
“…Equation defines S ( q , t ) Here, ρ 0 is the total number density of the IL, x i and x j are atomic mole fractions, and the f i ( q ) and f j ( q ) functions are the corresponding X-ray atomic form factors. In all our calculations, we use a Lorch-type function, , W ( r ), to account for the fact that box sizes are not infinite, resulting in reciprocal space oscillations due to cutoff errors in the normalized distinct van Hove function, g d ij ( r , t ), at the edge of the box.…”
Section: Methodsmentioning
confidence: 99%
“…g d ij ( r , t ) is equal to 1 at long times, and at any time it goes to 1 at long distances. Just as we have done in several prior publications, S­( q ) and S ( q , t ) can be partitioned into useful subcomponents. ,, ,,,, These allow us to follow the structural dynamics of liquid structural motifs at specific q values. In the Results and Discussion section, we will plot the time integral of the head–anion subcomponent of S ( q , t ) squared ( S H–A ( q , t ) 2 ).…”
Section: Methodsmentioning
confidence: 99%
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