29 research outputs found
Composition of Ni2+ cation solvation shell in NiCl2āmethanol solution by multinuclear NMR
1H-, 2H- and 13C-NMR spectra have been used to test the Ni2+ solvation shell composition in the 1.1 molal methanol solution of NiCl2. It has been confirmed that Clā anion takes part in the nearest environment of Ni2+ cation at all the temperatures investigated. Using 2H-NMR allowed us to detect for the first time OD-signal of methanol in the primary solvation shell of Ni2+ cation. Both 2H- and 13C-NMR spectra show that the composition of the cation solvation shell becomes more complicated at temperatures lower than 220āK
Local Structure in Terms of Nearest-Neighbor Approach in 1-Butyl-3-methylimidazolium-Based Ionic Liquids: MD Simulations
Description of the local microscopic
structure in ionic liquids
(ILs) is a prerequisite to obtain a comprehensive understanding of
the influence of the nature of ions on the properties of ILs. The
local structure is mainly determined by the spatial arrangement of
the nearest neighboring ions. Therefore, the main interaction patterns
in ILs, such as cationāanion H-bond-like motifs, cationācation
alkyl tail aggregation, and ring stacking, were considered within
the framework of the nearest-neighbor approach with respect to each
particular interaction site. We employed classical molecular dynamics
(MD) simulations to study in detail the spatial, radial, and orientational
relative distribution of ions in a set of imidazolium-based ILs, in
which the 1-butyl-3-methylimidazolium (C<sub>4</sub>mim<sup>+</sup>) cation is coupled with the acetate (OAc<sup>ā</sup>), chloride
(Cl<sup>ā</sup>), tetrafluoroborate (BF<sub>4</sub><sup>ā</sup>), hexafluorophosphate (PF<sub>6</sub><sup>ā</sup>), trifluoromethanesulfonate
(TfO<sup>ā</sup>), or bisĀ(trifluoromethanesulfonyl)Āamide (TFSA<sup>ā</sup>) anion. It was established that several structural
properties are strongly anion-specific, while some can be treated
as universally applicable to ILs, regardless of the nature of the
anion. Namely, strongly basic anions, such as OAc<sup>ā</sup> and Cl<sup>ā</sup>, prefer to be located in the imidazolium
ring plane next to the CāH<sup>2/4ā5</sup> sites. By
contrast, the other four bulky and weakly coordinating anions tend
to occupy positions above/below the plane. Similarly, the H-bond-like
interactions involving the H<sup>2</sup> site are found to be particularly
enhanced in comparison with the ones at H<sup>4ā5</sup> in
the case of asymmetric and/or more basic anions (C<sub>4</sub>mimOAc,
C<sub>4</sub>mimCl, C<sub>4</sub>mimTfO, and C<sub>4</sub>mimTFSA),
in accordance with recent spectroscopic and theoretical findings.
Other IL-specific details related to the multiple H-bond-like binding
and cation stacking issues are also discussed in this paper. The secondary
H-bonding of anions with the alkyl hydrogen atoms of cations as well
as the cationācation alkyl chain aggregation turned out to
be poorly sensitive to the nature of the anion
Complexation of Ni(ClO<sub>4</sub>)<sub>2</sub> and Mg(ClO<sub>4</sub>)<sub>2</sub> with 3āHydroxyflavone in Acetonitrile Medium: Conductometric, Spectroscopic, and Quantum Chemical Investigation
The
complex formation of NiĀ(ClO<sub>4</sub>)<sub>2</sub> and MgĀ(ClO<sub>4</sub>)<sub>2</sub> with 3-hydroxyflavone (HL, flavonol) in acetonitrile
was studied using conductometric and spectroscopic methods. It was
found that interaction of nickel cation with HL leads to formation
of the doubly charged [NiĀ(HL)]<sup>2+</sup> complex, whereas in solutions
of magnesium perchlorate the complex with anion [MgClO<sub>4</sub>(HL)]<sup>+</sup> is formed. Using the extended LeeāWheaton
equation, the limiting equivalent conductivities of [NiĀ(HL)]<sup>2+</sup> and [MgClO<sub>4</sub>(HL)]<sup>+</sup> and thermodynamic constants
of their formation were obtained at 288, 298, 308, 318, and 328 K.
Calculated Stokeās radii indicate weak solvation of the formed
complexes and low temperature stability of their solvation shells.
On the basis of the quantum chemical calculations and noncovalent
interactions analysis, it is found that in the solvated [NiĀ(HL)]<sup>2+</sup> and [MgClO<sub>4</sub>(HL)]<sup>+</sup> complexes interaction
of the Ni<sup>2+</sup> and Mg<sup>2+</sup> cations with flavonol occurs
via the carbonyl group of HL. Complexation with Ni<sup>2+</sup> does
not change the internal structure of HL greatly: in the [NiĀ(HL)]<sup>2+</sup> complex, flavonol shows an intramolecular H-bond between
3-hydroxyl and carbonyl groups. When a complex with [MgClO<sub>4</sub>]<sup>+</sup> is formed, the OH group turns out of the plane of the
chromone moiety that leads to rupture of an intramolecular H-bond
in the ligand molecule. Moreover, in the [MgClO<sub>4</sub>(HL)]<sup>+</sup> complex, perchlorate anion possesses a strong ability to
interact with HL, forming an intracomplex H-bond between hydrogen
of the 3-hydroxyl group and oxygen of ClO<sub>4</sub><sup>ā</sup>. Its strength is more pronounced than in the intramolecular one
in both [NiĀ(HL)]<sup>2+</sup> and uncomplexed 3-hydroxyflavone
Electronic Properties of Carbon Nanotubes Intercalated with Li<sup>+</sup> and Mg<sup>2+</sup>: Effects of Ion Charge and Ion Solvation
The influence of bare and solvated
cations imbedded inside single-walled
carbon nanotubes (SWCNTs) on the SWCNT electronic properties is studied
by <i>ab initio</i> electronic structure calculations. The
roles of ion charge and ion solvation are investigated by comparing
Li<sup>+</sup> vs Mg<sup>2+</sup> and Li<sup>+</sup> vs its solvatocomplex
with two ethylene carbonate (EC) molecules, [Li(EC)<sub>2</sub>]<sup>+</sup>. Two
achiral nanotubes with
similar radii but different electronic structure are considered, namely,
the metallic, (15,15) armchair, and semiconducting, (26,0) zigzag,
SWCNTs. The intercalation process is energetically favorable for both
CNT topologies, with all bare cations and the solvatocomplex under
investigation, with the doubly charged Mg<sup>2+</sup> ion exhibiting
the highest energy gain. Insertion of the bare ions into the SWCNTs
increases the electronic entropy. The electronic entropy changes because
the ions introduce new energy levels near the Fermi level. Those initially
empty levels of the cations accept electron density and generate electronic
holes in the valence band of both SWCNT topologies. As a consequence,
the semiconducting (26,0) zigzag SWCNT becomes metallic, exhibiting
hole conductivity. Solvation of the bare Li<sup>+</sup> ion by EC
molecules completely screens the influence of the ion charge on the
SWCNT electronic properties, independent of the topology. The last
fact validates the common practice of employing standard, nonpolarizable
force field models in classical molecular dynamics simulations of
electrolyte solutions interacting with CNTs. The strong dependence
of the nanotube electronic properties on the presence of bare ions
can be used for development of novel cation sensors for mass spectroscopy
applications