27 resultados para Molecular Structure

em Deakin Research Online - Australia


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The solid-state structures of the previously known para-substituted diphenyltellurium dichlorides, (p-XC6H4)2TeCl2 (X=H (1), Me (2), MeO (3)) were investigated by 125Te MAS NMR spectroscopy and in case of 2 by single crystal X-ray diffraction. The 125Te-NMR shielding anisotropy (SA) was studied by tensor analyses based on relative intensities of the observed spinning sidebands. Solid-state NMR parameters, namely the isotropic chemical shift (δiso), anisotropy (ζ) and asymmetry (η), were discussed in relation to the molecular structures established by X-ray crystallography. The asymmetry (η) was found to be particularly sensitive to structural differences stemming mostly from the diverse secondary Te...Cl interactions, but no correlation with geometric parameters could be established.


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The dimeric tetraorganodistannoxane [n-Bu2(F)SnOSn(F)t-Bu2]2 (1) was prepared by the reaction of (t-Bu2SnO)3 with n-Bu2SnF2 and characterized in solution by multinuclear NMR spectroscopy and ESI MS spectrometry and in the solid state by 119Sn MAS NMR spectroscopy and single crystal X-ray diffraction.

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Structural data (X-ray and solution and solid-state 119Sn NMR) show that skew-trapezoidal-bipyramidal diorganotin compounds of 2-quinaldate are invariably monomeric, owing to the steric bulk of the carboxylate ligand. In contrast, most of the analogous compounds of 2-picolinate (2-pic) can increase their coordination number by polymerization or the incorporation of solvent in their coordination sphere in the solid state. The exceptional compound is tBu2Sn(2-pic)2 (3), for which no increase in coordination number is apparent, a result that is correlated with the bulky tert-butyl groups. Thus, judicious choice of tin or ligand substituents can be exploited to dictate coordination number and/or the degree of supramolecular aggregation in the investigated systems.

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The reaction of Me3SbCl2 and (Me2SnS)3 afforded the complex (Me3SbS)2Me2SnCl2 in high yields, whose molecular structure features both hypercoordinated tin and antimony atoms. In solution, (Me3SbS)2Me2SnCl2 undergoes a reversible dissociation and ligand interchange reaction to give Me3SbS, Me3SbCl2 and (Me2SnS)3.

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Many problems in chemistry depend on the ability to identify the global minimum or maximum of a function. Examples include applications in chemometrics, optimization of reaction or operating conditions, and non-linear least-squares analysis. This paper presents the results of the application of a new method of deterministic global optimization, called the cutting angle method (CAM), as applied to the prediction of molecular geometries. CAM is shown to be competitive with other global optimization techniques for several benchmark molecular conformation problem. CAM is a general method that can also be applied to other computational problems involving global minima, global maxima or finding the roots of nonlinear equations.

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The molecular geometry, the three dimensional arrangement of atoms in space, is a major factor determining the properties and reactivity of molecules, biomolecules and macromolecules. Computation of stable molecular conformations can be done by locating minima on the potential energy surface (PES). This is a very challenging global optimization problem because of extremely large numbers of shallow local minima and complicated landscape of PES. This paper illustrates the mathematical and computational challenges on one important instance of the problem, computation of molecular geometry of oligopeptides, and proposes the use of the Extended Cutting Angle Method (ECAM) to solve this problem.

ECAM is a deterministic global optimization technique, which computes tight lower bounds on the values of the objective function and fathoms those part of the domain where the global minimum cannot reside. As with any domain partitioning scheme, its challenge is an extremely large partition of the domain required for accurate lower bounds. We address this challenge by providing an efficient combinatorial algorithm for calculating the lower bounds, and by combining ECAM with a local optimization method, while preserving the deterministic character of ECAM.


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In order to explore the various possible property trends in ionic liquid mixtures, five different ionic liquids were mixed with N-methyl-N-propylpyrrolidinium bis(trifluoromethylsulfonyl)amide ([C3mpyr][NTf2]), and the viscosities, excess molar volumes, ionic conductivities, and phase diagrams of the mixtures were determined over a range of temperatures. In a number of the mixtures the crystallization of both components was completely suppressed and no melting point was observable. Such mixtures of similar ionic liquids thus have potential for use in low-temperature applications by extending the liquid range to Tg. The molar conductivities and viscosities are described as approximating predictable or “simple” mixing behaviors, while excess molar volumes were found to show a variety of mixing and nonideal mixing effects. Mixture equations for viscosity and conductivity are discussed and analyzed. An immiscibility window was observed in the trihexyl(tetradecyl)phosphonium bis(trifluoromethylsulfonyl)amide ([P6,6,6,14][NTf2]) in the [C3mpyr][NTf2] system in the [C3mpyr][NTf2]-rich region. Unusual physical properties are exhibited by miscible compositions near the demixing line. These compositions are described as [P6,6,6,14][NTf2]-like, even up to 0.5 mol fraction of [C3mpyr][NTf2].

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CI2H8BrN, monoclinic, Pl21/cl (No. 14), a = 7.555(6) Å, b =7.727(3) Å, c =16.643(2) Å, β =98.95(2)°, V =959.8 Å3 , Z =4, Rgt(F) =0.033, wRref(F2) =0.097, T =173 K.

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The molecular structure of (Ph3SnO2C)3C6H3 reveals distorted tetrahedral C3O geometries for each tin atom. No intermolecular Sn...O associations occur between the molecules so that the trinuclear molecule may be considered monomeric. An increase in coordination number at tin is indicated by 119Sn NMR measurements conducted in d6-DMSO solution and this has been confirmed by a structure analysis of (DMSO·Ph3SnO2C)3C6H3·2 DMSO. In this structure, the tin atom geometries are distorted trigonal bipyramidal, existing within trans-C3O2 donor sets. Thus, while is it possible for the tin atoms to increase their coordination numbers in (Ph3SnO2C)3C6H3, molecular aggregation to form polymeric arrays is precluded, most likely due to steric constraints.


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The synthesis and molecular structure are reported of the first example of a diorganotin oxide, {p-[R(O)SnCH2SiMe2]2C6H4}3 (3) (R = (Me3Si)2CH), in which two six-membered Sn3O3 units are linked by three -CH2Si(Me)2C6H4Si(Me)2CH2- spacers.

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B3LYP/6-311+G(d) calculations indicate that (HBO)3 (4) and (HBO)4 (5) possess (zero-point energy corrected) strain enthalpies of 11.4 and 31.6 kJ mol−1, respectively. The absence of eight-membered (RBO)4 rings is attributed to a combination of ring strain and the lability of the B---O bond. The synthesis, characterization and molecular structure of (PhBO)3·pyridine (1) are described and chemical phenomena related to the addition of amines to triorganoboroxine rings are rationalized in terms of relief of ring strain in 4.


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The molecular structure of the centrosymmetric hexanuclear title compound, [iPrSn(O)(O2CCH3)]6·4CHCl13 or [Sn6O6(C3H7)6(C2H3O2)6]·4CHCl3, adopts the `drum' motif, in which two (iPrSnO)3 caps are linked via six μ3-oxo atoms and six acetate groups. The Sn atoms are in distorted octahedral environments, defined by a CO5 donor set for each of the three independent Sn atoms.

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The crystal and molecular structure of Gingras' salt [n-Bu4N]+ [Ph3SnF2] is reported, which reveals a variety of inter- and intramolecular C---H...F hydrogen bonding interactions. A 119Sn MAS-NMR spectrum was recorded and a tensor analysis has been performed according to the method of Herzfeld and Berger. The results are discussed in terms of the molecular structure and are compared with the parent compound Ph3SnF as well as with Mes3SnF (Mes=mesityl).