Theoretical Probing of Weak Anion–Cation Interactions in Certain Pyridinium-Based Ionic Liquid Ion Pairs and the Application of Molecular Electrostatic Potential in Their Ionic Crystal Density Determination: A Comparative Study Using Density Functional Approach
Abstract:A comprehensive study on the structure, nature of interaction, and properties of six ionic pairs of 1-butylpyridinium and 1-butyl-4-methylpyridinium cations in combination with tetrafluoroborate (BF), chloride (Cl), and bromide (Br) anions have been carried out using density functional theory (DFT). The anion-cation interaction energy (ΔE), thermochemistry values, theoretical band gap, molecular orbital energy order, DFT-based chemical activity descriptors [chemical potential (μ), chemical hardness (η), and el… Show more
“…Furthermore, the intensity of dispersion interaction increased quickly as we examined increasingly large cages, due to the greater negative values for E dis . It is well-known that the dispersion interactions are among the important non-covalent interactions for many host-guest systems [44,45,46,47,48]. However, the values we calculated E dis are within 8 kcal for both Li@C n and Li + @C n in this work.…”
Section: Resultscontrasting
confidence: 56%
“…In order to directly depict the physical image of the interaction between carbon cages and the hosted Li and Li + , here non-covalent interaction analysis is discussed based on the reduced density gradient (RDG). It is well known that RDG has become an effective tool to reveal the non-covalent interaction of various host-guest systems [44,45,46,47,48]. The visualizations of RDG for Li@C n and Li + @C n with n = 20, 24, 44, 48, 50 and 70 are shown in Figure 4.…”
This work reveals first principle results of the endohedral fullerenes made from neutral or charged single atomic lithium (Li or Li+) encapsulated in fullerenes with various cage sizes. According to the calculated binding energies, it is found that the encapsulation of a single lithium atom is energetically more favorable than that of lithium cation. Lithium, in both atomic and cationic forms, exhibits a clear tendency to depart from the center in large cages. Interaction effects dominate the whole encapsulation process of lithium to carbon cages. Further, the nature of the interaction between Li (or Li+) and carbon cages is discussed based on reduced density gradient, energy decomposition analysis, and charge transfer.
“…Furthermore, the intensity of dispersion interaction increased quickly as we examined increasingly large cages, due to the greater negative values for E dis . It is well-known that the dispersion interactions are among the important non-covalent interactions for many host-guest systems [44,45,46,47,48]. However, the values we calculated E dis are within 8 kcal for both Li@C n and Li + @C n in this work.…”
Section: Resultscontrasting
confidence: 56%
“…In order to directly depict the physical image of the interaction between carbon cages and the hosted Li and Li + , here non-covalent interaction analysis is discussed based on the reduced density gradient (RDG). It is well known that RDG has become an effective tool to reveal the non-covalent interaction of various host-guest systems [44,45,46,47,48]. The visualizations of RDG for Li@C n and Li + @C n with n = 20, 24, 44, 48, 50 and 70 are shown in Figure 4.…”
This work reveals first principle results of the endohedral fullerenes made from neutral or charged single atomic lithium (Li or Li+) encapsulated in fullerenes with various cage sizes. According to the calculated binding energies, it is found that the encapsulation of a single lithium atom is energetically more favorable than that of lithium cation. Lithium, in both atomic and cationic forms, exhibits a clear tendency to depart from the center in large cages. Interaction effects dominate the whole encapsulation process of lithium to carbon cages. Further, the nature of the interaction between Li (or Li+) and carbon cages is discussed based on reduced density gradient, energy decomposition analysis, and charge transfer.
“… 18 It is also known that the tetrafluoroborate anion is weakly coordinated as a local interaction in the pyridinium-based ionic liquid, and it is pointed out that the van der Waals effect, which is weaker than the hydrogen-bonding type interaction, dominates the interaction between the cation and the anion. 58 Tsuzuki et al performed MP2/6-311G** level ab initio calculation for [BF 4 ] − complexes with 1-ethyl-3-metylimidazolium cation [emim] + , 1-ethyl-2,3-dimethylimidazolium cation [emmim] + , ethylpyridinium cation [epy] + , and N -ethyl- N , N , N -trimethylammonium [(C 2 H 5 )(CH 3 ) 3 N] + . 46 The total interaction energies of the ion pair were −85.2, −81.8, −82.4, and −85.2 kcal/mol, respectively, and were not very different.…”
We performed terahertz time-domain spectroscopy and infrared
spectroscopy
of imidazolium-based, pyridinium-based, and tetraalkylammonium-based
tetrafluoroborate ionic liquids to study their characteristic intermolecular
and intramolecular vibrational modes to clarify interactions between
various cations and the tetrafluoroborate anion. It was found that
the central frequency of the intermolecular vibrational band for these
ionic liquids has a relatively high frequency, ranging from 90 to
100 cm
–1
. In the 900–1150 cm
–1
range, the intramolecular vibrational absorption band of the 3-fold
degenerate mode of tetrafluoroborate anions in the ionic liquids was
observed. Although the tetrafluoroborate anion is attributable to
one of the weakly coordinated anions, the spectroscopic splitting
behavior of the 3-fold degenerate mode differs depending on the cation
species. It was revealed that the degenerate mode is very sensitive
to local interactions between the tetrafluoroborate anion and each
cation.
“…Density is one of the most significant factor for energetic materials as higher density means that more energy will be packed per unit volume in these materials. 33 Specifically, crystal density can directly influence the detonation performance which is shown in the Kamlet–Jacobs equation. By replacing the nitro group or inserting the different bridges, the structure of bistriazole was changed, which will cause different effect in density.…”
We designed four series of energetic anions by replacing nitro group (NO2) with trinitromethyl group (C(NO2)3) or by inserting N-bridging groups (–NH–, –NH–NH–, –NN–, –NN(O)–) into the bistriazole frameworks.
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