A new insight to the role of bubble properties on inertial effect in particle–bubble interaction

In this study the impact of bubble surface characterization (mobility or immobility), its diameter and velocity is investigated on inertial forces in particle–bubble collision efficiency (E_C). Three models including Sutherland (E_C-SU), Schulze (E_C-SC), and generalized Sutherland Equation (E_C-GSE) were taken into account with regard to their differences from the inertial point of view in the particle size range of 1–100?µm. Bubble diameters of 0.08, 0.12, and 0.15?cm and bubble velocities of 10, 20 and 30?cm/s were selected to study the flotation of chalcopyrite. Weber and Paddock collision model (E_C-W&P) was taken for evaluation of the effect of bubble surface mobility on E_C. It was found that when the bubble diameter is 0.12?cm, reducing bubble velocity from 30 to 20?cm/s, the inertia force can be ignored for wider range of particle size. Corresponding particle size in cross-sectional point between GSE and Schulze collision models was introduced for better evaluation of the positive and negative particle inertial effects. The best agreement between them was taken for bubble diameter of 0.12?cm and velocity of 20?cm/s. It was concluded that the influence of bubble velocity is more effective than bubble diameter regarding its role on particle inertial forces in particle–bubble interaction.     

Proton donor–acceptor property of matrix during the sol–gel reaction

The UV–VIS absorption spectrum of thymol blue (TB), which was used for an in situ probe for the proton donor–acceptor property of the surrounding matrix, has been observed as a function of time during the sol–gel–xerogel reactions of tetraethyl orthosilicate under HCl catalyzed and uncatalyzed conditions. The value of relative abundance, RA _Z , of zwitter ion species was calculated. In the ethanol-containing system, RA _Z increased for 7 h, then decreased until 114 h had passed, and finally increased gradually. These dynamic changes of the RA _Z were commonly observed for all the systems. The final RA _Z values were expected larger than 0.7 irrespective of the initial chemical composition. The characteristic increase and decrease in RA _Z are ascribed to the increase and decrease in proton-donating ability from the surrounding matrix to encapsulated TB molecules. A general acidity function, H ₋, of the matrix was estimated.     

Solvent interactions in the excited state of non-planar donor—acceptor molecules

In order to probe solute—solvent interactions in the intramolecular charge transfer (TICT) state of 2,6,N,N-tetramethylcyanoaniline (TMCA) fluorescence spectra, quantum yields and lifetimes of this compound were measured in binary mixtures of n-hexane with chlorinated hydrocarbons. An isoemissive point in the fluorescence spectra was observed as the composition of the solvent was varied. Evidence for both clustering of polar solvent molecules around the excited solute and for non-specific long-range interactions with the polar bulk of the solution was found. The properties of the solvent affect primarily the efficiency of non-radiative deactivation. Fluorescence quenching by saturated amines gives good evidence that TMCA emission arises from a highly polar state in both polar and non-polar solutions.     

Modelling the molecular weight distribution in terpolymerization systems with donor–acceptor complexes

In this work we present, for the first time, a mathematical development of the moments of the molecular weight distribution in terpolymerization systems where donor–acceptor complexes are formed and the propagating reactions are carried out according to the complex participation model. The resulting set of equations is applied to the system formed by vinyl chloride (VC), vinyl acetate (VAc) and maleic anhydride (MA), in order to show the use of the equations and the type of information that might be obtained from them.     

A perturbation theoretical method for determination of the dependence of the intramolecular X–H(D) potential on the hydrogen bond strength

A perturbation theoretical method is proposed that allows determination of the function describing the dependence of the intramolecular XH(D) potential on the hydrogen bond strength. Treating the XH(D) oscillators as mixed cubic–quartic oscillators in which the stretch–stretch couplings of the ν(X–H(D)) mode with the internal modes of the radical X may be neglected, and introducing the hydrogen bonding influence through the changes in the harmonic diagonal force constants (as proposed by Sceats and Rice [41]), it is possible to extract the analytical form of the function ) from the experimental versus correlations. The other parameters obtained by the empirical correlations, within this model, also have an exact physical meaning. The method is applicable to weak hydrogen bonds as well as to hydrogen bonds of intermediate strength, and, strictly speaking, to linear X– systems. However, extension to arbitrary geometry may be easily done. This revised version was published online in July 2006 with corrections to the Cover Date.     

O–H···C hydrogen bond in the methane–water complex

Quantum chemical calculations were performed at different levels of theory (SCF, DFT, MP2, and CCSD(T)) to determine the geometry and electronic structure of the HOH···CH₄ complex formed by water and methane molecules, in which water is a proton donor and methane carbon (sp³) is an acceptor. The charge distribution on the atoms of the complex was analyzed by the CHelpG method and Hirshfeld population analysis; both methods revealed the transfer of electron charge from methane to water. According to the natural bond orbital (NBO) analysis data, the charge transfer upon complexation is caused by the interaction between the σ orbital of the axial С–H bond of methane directed along the line of the O–H···C hydrogen bridge and the antibonding σ* orbital of the О–H bond of the water molecule. Topological analysis of electron density in the HOH···CH₄ complex by the AIM method showed that the parameters of the critical point of the bond between hydrogen and acceptor (carbon atom) for the O–H···C interaction are typical for Н-bonded systems (the magnitude of electron density at the critical point of the bond, the sign and value of the Laplacian). It was concluded that the intermolecular interaction in the complex can be defined as an Н bond of O–H···σ(С–H) type, whose energy was found to be 0.9 kcal/mol in MP2/aug-cc-pVQZ calculations including the basis set superposition error (BSSE).     

Nanoscale cooperativity on a series of statistical methacrylates copolymers with electron donor–acceptor pendant groups

Standard and StepScan DSC studies have been performed on a series of statistical methacrylate copolymers with electron-donor and electron-acceptor pendant groups that form intramolecular electron transfers. From standard DSC analysis we concluded that glass transition temperature slowly increased with increasing electron-acceptor monomeric moiety ratio up to 0.5 in the main chain. Using StepScan DSC method we calculated the size and volume of cooperative rearranging region as well mean temperature fluctuation at glass transition temperature. It was estimated also the average number of monomer units in the cooperative rearranging region. All parameters were calculated according to the method proposed by Donth based on Heat Capacity Spectroscopy. The results show that the presence of intermonomeric electron transfers decreased the chain mobility, as well as the cooperativity of relaxation processes of these structures in the glass transition range. This is reflected by minimal values of these parameters around 0.4 ratio of copolymer composition. Such behavior is similar to that of crosslinked or confined systems (e.g., nanocomposites, thin films) that have reduced chain mobility.     

Homolytic dissociation in hydrogen-bonding liquids: energetics of the phenol O–H bond in methanol and the water O–H bond in water

The energetics of the phenol O–H bond in methanol and the water O–H bond in liquid water were investigated by microsolvation modelling and statistical mechanics Monte Carlo simulations. The microsolvation approach was based on density functional theory calculations. Optimised structures for clusters of phenol and the phenoxy radical with one and two methanol molecules are reported. By analysing the differential solvation of phenol and the phenoxy radical in methanol, we predict that the phenol O–H homolytic bond dissociation enthalpy in solution is 24.3±11 kJ/mol above the gas-phase value. The analysis of the water O–H bond dissociation by microsolvation was based on optimised structures of OH–(H₂O)_1–6 and –(H₂O)_1–7 clusters. Microsolvation modelling and statistical mechanics simulations predict that the HO–H bond dissociation enthalpies in the gas phase and in liquid water are very similar. Our results stress the importance of estimating the differences between the solvation enthalpies of the radical species and the parent molecule and the limitations of local models based on microsolvation.Proceedings of the 11th International Congress of Quantum Chemistry satellite meeting in honor of Jean-Louis Rivail     

IR spectroscopic study of the hydrogen bond network in the water–3-amino-1-propanol system and its comparison with the spatial network of hydrogen bonds in the water–monoethanolamine system

IR spectroscopy was used to explore the water–3-amino-1-propanol (3AP) system in the range of 400–4000 cm^-1. Based on the stretching vibrations of OH, NH₂ and CH groups and skeletal bending vibrations of 3AP it was concluded that mixed spatial networks are formed in the water–3AP system that predominate at medium 3AP concentrations. The obtained results are similar to the IR spectroscopic data for the water–monoethanolamine system, viz., the networks of both amino alcohols are incorporated into the spatial     

C–H bond activation in the total syntheses of natural products

The transition metal-mediated C–H bond activation has emerged as a powerful and ideal method for the total syntheses of natural products and pharmaceuticals, and has had a significant impact on synthetic planning and strategy in complex natural products.In this review, we describe selected recent examples of the transition metal-mediated C–H bond activation strategies for the rapid syntheses of natural products.     

A DFT study on the structure–property relationship of amino-, nitro- and nitrosotetrazoles, and their N-oxides: new high energy density molecules

We explore herein the structure, stability, heat of explosion, density, and the performance properties of amino, nitro, and nitroso substituted tetrazoles and their N-oxides using the density functional theory calculations at the B3LYP/aug-cc-pVDZ level. N-Nitro compounds have lower densities compared with those of C-nitrotetrazoles. Kamlet-Jacob semi-empirical equations were used to calculate the performance properties of designed compounds. The higher performance of tetrazole-N-oxides is due to their higher densities (2.110–2.287 g/cm³). Heat of explosion, stability, density and performance properties are related to the number and relative positions of NO₂, NH₂, and NO groups of the tetrazole ring. The designed molecules satisfy the criteria of high energy materials.     

Features of strong O–H⋯O and N–H⋯O hydrogen bond manifestation in vibrational spectra

The work deals with the establishment of the dependence of the vibrational frequencies of strong O–H?O and N–H?O hydrogen bonds for the diagnosing the bonds themselves. To this end, the Raman spectra of a large number of different normal and deutero-substituted crystals characterized by the presence of strong O–H?O and N–H?O bonds are measured and the quantum chemical calculation is performed for one of these compounds. The dependence of the O–H stretching frequency on the O?O distance is constructed differing from that previously known for short O?O contacts. The mechanisms of significant broadening of the O–H vibration band in strong O–H?O hydrogen bonds are considered. Different dependences of the N–H vibrational frequencies in N–H?O bonds are reported and the causes of this diversity are discussed.     

Production of 24Na and 28Mg by the interaction of uranium with 15–600 Mev protons

Excitation functions for formation of ²⁴Na and ²⁸Mg in the interaction of uranium with protons have been determined radiochemically between 15 and 600 MeV. After a sharp initial rise the excitation functions show a smooth increase up to 400 MeV, whereafter they become slightly steeper.By comparing available excitation functions for reactions leading to ²⁴Na and ²⁸Mg, it seems most likely that these light fragments are formed in a binary process.     

Studies on the molecular interaction of Erythrosine ‘B’ with surfactants

The spectroscopic investigation on anionic dye, Erythrosine ‘B’(EB) with three different types of surfactants such as CTAB (cationic), sodium lauryl sulphate (SLS; anionic) and Triton X-100 (TX-100),Tween-20, 40, 60 and 80 (nonionic) in aqueous media shows that EB forms a 1:1 molecular complex with TX-100, Tweens and CTAB. No interaction is observed between EB and SLS. The thermodynamic and spectrophotometric properties of these complexes suggest that EB forms a strong charge transfer (CT) complex with TX-100 and Tweens whereas the interaction of EB with CTAB is coulombic in nature. Photogalvanic and photoconductometric studies also support the above interactions. In addition to this, the electron-donating ability among the nonionic surfactants, i.e. TX-100 and Tweens towards dye, role of surface in CT interaction, the site of CT interaction and the intensity and stability of CT interaction between EB and nonionic surfactants have been pointed out.     

A new proposed mechanism for the cathodic reduction of a carbon–chlorine bond in 2-acetylphenyltrichloroacetate

The cathodic reduction of 2-acetylphenyltrichloroacetate at a controlled potential of −0.5 V (vs SCE) yields 3,3-dichloro-4-hydroxy-4-methyl-3,4-dihydrocoumarin. The charge consumption is 1e⁻/substrate molecule, which is in agreement with a non-conventional R–X→R⁻+X mechanism.     

A study of interaction of two ethylene molecules by the semiempirical complete configuration interaction method in π-electron approximation

The semiempirical complete configuration interaction method in -electron approximation has been used to calculate the energies of states of a system composed of two interacting ethylene molecules and having the D _2h symmetry. Oscillator strengths for the allowed transitions have been also calculated. If conjugation effects between the ethylene molecules are disregarded the hypochromism found by Nesbet is not obtained in this higher approximation. Consideration of conjugation effects results in hypochromism of the longest-wavelength allowed transition. The bathochromic shift of this band occurs at smaller distances between the two ethylene molecules than the hypochromic effect. Some general features of transannular interaction and the rôle of conjugation effects in the hypochromism of helical polynucleotides are discussed. The qualitative similarity of the cyclobutadiene energy spectra calculated by the semiempirical and by the theoretical methods of complete configuration interaction is pointed out.

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Zusammenfassung Mittels der halbempirischen Methode der vollständigen Konfigurationswechselwirkung wurden die Eigenwerte der Energie eines Systems von gp-Elektronen, bestehend aus zwei äthylenmolekülen mit der Symmetrie D _2h , sowie die Oszillatorstärke erlaubter Übergänge berechnet. Bei Vernachlässigung der Konjugationseffekte tritt der hypochrome Effekt Nesbets in dieser höheren Näherung nicht auf. Berücksichtigung von Konjugationseffekten ergibt eine Intensitätsschwächung der Bande des langwelligsten erlaubten Überganges. Bei dieser Bande überwiegt bei kleinem Abstand der Äthylenmoleküle der bathochrome Effekt. Einige allgemeine Aspekte transannularer Wechselwirkung und die Rolle von Konjugationseffekten im Hypochromismus spiraliger Polynukleotide werden erörtert. Die qualitative Ähnlichkeit von Cyclobutadienspektren, die einerseits nach der halbempirischen, andererseits nach der theoretischen Methode der vollständigen Konfigurationswechselwirkung berechnet wurden, wird aufgezeigt.

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Résumé A l'aide de la méthode semiempirique de l'interaction de configuration complète, les valeurs propres de l'énergie d'un système d'électrons gp, consistant en deux molécules d'éthylène et ayant la symétrie D _2h , et les forces oscillatrices des transitions permises ont été calculées. Si l'on néglige les effets de conjugaison, l'effet hypochrome de Nesbet n'apparaît pas dans cette approximation élevée. Si l'on tient compte des effets de conjugaison, il en résulte une diminution de l'intensité de la transition permise de plus grande longueur d'onde. Dans le cas de cette bande, l'effet bathochrome l'emporte, quand la distance entre les molécules d'éthylène est petite. Quelques aspects communs des interactions transannulaires et le rôle des effets de conjugaison dans l'hypochromisme des polynucléotides en hélice sont discutés. On montre la ressemblance qualitative entre les spectres du cyclobutadiène, calculés et par la méthode semiempirique et par la méthode théorique de l'interaction de configuration complète.

     

Homodesmotic method of determining the O–H bond dissociation energies in phenols

The dissociation energy of the O–H bond has been calculated by the homodesmotic reaction method for phenolic compounds, which are well-known antioxidants, including for natural phenols. Use of moderately complex computational levels, such as B3LYP/6-31G(d), is sufficient for reliably estimating the D(O–H) value for phenols within the homodesmotic approach. The O–H bond dissociation energy for monosubstituted phenols has been calculated, and the additive character of the effect of methyl groups on D(O–H) in methylphenols has been demonstrated: the introduction of a CH₃ group into the aromatic ring decreases the D value by 7.8 kJ/mol (ortho position), 1.8 kJ/mol (meta position), and 7.6 kJ/mol (para position). The O–H bond strength has been calculated for a number of ubiquinols, selenophens, flavonoids, and chromanols. The D(O–H) value recommended for α-tocopherol is 328.0 ± 1.3 kJ/mol.     

Disruptive influence of the host cage C60 on the guest He–H+ bond and bonding in H3+

Although a helium atom prefers to stay at the centre of a fullerene (C₆₀) cage and a proton binds with one of the carbon atoms from inside, DFT(MN15)/cc-pVTZ and DLPNO-MP2/def2-TZVP calculations show that the helium atom and the proton in HeH⁺ prefer to stay away from the centre of the cage, weakening the He–H⁺ covalent bond considerably. Both the helium atom and the proton exhibit noncovalent interactions with the carbon atoms of two pentagons at the opposite ends of the fullerene cage. Our calculations also show that a linear arrangement of H₃⁺ (inside C₆₀), pointing towards the centres of two pentagons opposite to each other, with the proton breaking away from H_2, is energetically more favored over the equilateral triangle geometry of free H₃⁺.