Reactions of TiCl4, VCl4 and VOCl3 with tetraalkyldiphosphine disulphides

Summary The reactions of MCl₄ (M = Ti or V) with R₂P(S)P(S)R₂ (R = Me or Et) yield hexacoordinate complexes MCl₄ · R₂P(S)P(S)R₂ (M = Ti or V; R = Me or Et), whereas similar reactions with VOCl₃ lead to reduction of vanadium and give rise to the vanadium(IV) pentacoordinated complexes: VOCl₂-R₂P(S)P(S)R₂ (R = Me or Et). All the compounds have been characterized by elemental analyses, i.r., visible and e.p.r. spectra, which show thecis-chelate character of these ligands, although in the complexes containing Et₄P₂S₂ the i.r. spectra indicates that thegauche conformation of the ligand is implicated in bonding to the metal. The occupation of the sixth coordination site in pentacoordinate complexes, VOCl₂ · R₂P(S)P(S)R₂, by different donor solvents, has been studied by means of visible and e.p.r. spectra.     

Thermochemistry of gaseous ethylsilanes and their radical cations

The dissociation behavior of energy-selected tetraethylsilane, triethylsilane, and diethylsilane photocations is studied using the threshold photoelectron-photoion coincidence (TPEPICO) technique. In the 8–12. 5 eV photon energy range, 0 K dissociation onsets have been measured from the TPEPICO data. The dissociation channels observed include loss of ethane, hydrogen molecule, ethyl radical and hydrogen atom, depending upon the molecular ion under investigation. The thermochemistry of the molecular ions and dissociation fragments is obtained by an analysis that takes into account the kinetics and internal energy distributions of the ions. The various dissociation onsets permit the reevaluation of both neutral and ionic silane thermochemistry. We observed 298-K ethyl group values of 60±10 and 94±10 kJ mol^?1 for neutral and ionic silanes, respectively. These values are considerably smaller than the previously reported values of 86 and 130 kJ mol^?1, respectively. Finally, a Δ _f H ^° (298 K) of ?141.5 ± 21 kJ/mol for neutral diethyl silane is derived from the dissociative ionization onset of diethylsilane.     

Thermochemistry of the hydrates of k2CoCl4

A study of the dissociation pressure of crystalline K₂CoCl₄·2H₂O. The reactions can be summed up as K₂CoCl₄·nH₂O(c) = K₂CoCl₄·mH₂O(c)+(nm)H₂O (v). Below 50°C, n = 2 and 1, m = 1 and 0, above 50°C, n = 2 and m = 0. Below 50°C, the dihydrate is octahedral, the monohydrate and anhydrous compounds are tetrahedral. ΔH° and ΔS° are respectively 7.0 kcal and 14.2 e.u. for the loss of the first mole of water and 12.7 kcal and 32.0 e.u. for the loss of the last mole of water. Above 50°C, ΔH° and ΔS° are respectively 29.8 kcal and 77.6 e.u. for the loss of both waters. The changes in structure are discussed using the spectral and magnetic properties as indications for structural changes.     

Extraction and spectrophotometric determination of vanadium with 4-(2-thiazolylazo)resorcinol and tetraphenylarsonium and phosphonium chlorides

Extraction of vanadium-4-(2-thiazolylazo)resorcinol complexes by quaternary salts such as triphenylmethylarsonium iodide, tetraphenylarsonium chloride, and tetraphenylphosphonium chloride has been studied. Quantitative extraction is achieved with tetraphenylarsonium and tetraphenylphosphonium chlorides in the pH region between 3.5 and 5. The optimum conditions for the extraction and spectrophotometric determination of vanadium in the extract are: pH 3.8–4.0, the concentration of vanadium 0.1–0.4 μg/ml. Effective molar absorptivity at λ_max = 555 is (2.55 ± 0.05) × 10⁴ liters mol⁻¹ cm⁻¹. Beer's law is obeyed. Relative standard deviation is 2–10% depending on the concentration level. The composition of the extracted complexes was studied in the solution and in the solid state. For their characterization chemical and spectral evidence and comparison with the vanadium-PAR complexes have been combined.     

An unrestricted CNDO-MO calculation of VCl4

The electronic structure of the tetrahedral molecule VCl₄ is investigated within the unrestricted CNDO-MO approximation. The Hartree-Fock equations have been solved using an unrestricted SCF method for open-shell configurations. An iterative procedure is used that employs a single spinprojection to insure a relatively pure doublet state. The metal and ligand valence orbitals have been varied in an attempt to minimize the total energy. Expanded 3s and 3p chlorine orbitals are indicated while the optimum vanadium orbitals 4s(₄=1.50), 4p(d ³p²) and 3d(d ⁸) are obtained. Calculations assuming the unpaired electron occupies the 3a ₁, 2e and 4t ₂ molecular orbitals indicate that the 3a ₁ orbital is always the lone electron orbital. This result with the minimum total energy indicate that the ² A ₁ state is the ground state configuration. Extended basis functions for the chlorine valence electrons are used to obtain this result.

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Zusammenfassung Die Elektronenstruktur von tetraedrischem VCl₄ wird mittels einer CNDO-MO-Methode untersucht, bei der die HF-Gleichungen durch ein uneingeschränktes SCF-Verfahren für offene Schalen gelöst werden. Dies involviert ein iteratives Vorgehen mit einer einfachen Spinprojektion, so daß ein relativ reiner Dublettzustand resultiert. Sowohl die Metall-als auch die Liganden-Valenzorbitale sind variiert worden, um E _ges minimal zu machen. Die optimalen Vd-Zustände und Entwicklungen für die 3s- und 3p-Zustände werden angegeben. Die Rechnungen zeigen, daß das einsame Elektron immer im 3a ₁-Zustand sitzt, so daß die Grundkonfiguration von der Rasse ² A ₁ ist.

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Résumé Étude de la structure électronique de la molécule tétraédrique VCl₄ dans l'approximation CNDO-MO sans restriction de spin. Les équations de Hartree-Fock ont été résolues en utilisant une méthode SCF à couches ouvertes sans restriction. Le procédé itératif emploie une projection de spin afin d'assurer un état doublet relativement pur. Les orbitales de valence du métal et du ligand ont été modifiées afin d'essayer de minimiser l'énergie totale. On indique des orbitales étendues 3s et 3p pour le chlore, et l'on obtient des orbitales optimales pour le vanadium: 4s( ₄=150), 4p(d ³p³) et 3d(d ⁸). Des calculs montrent que des trois orbitales moléculaires 3a ₁, 2e et 4t ₂, l'électron célibataire occupe toujours la première. Ce résultat ainsi que celui sur l'énergie totale minimale indique que l'état ² A ₁ est la configuration de l'état fondamental. Une base étendue pour les électrons de valence du chlore est utilisée pour obtenir ce résultat.

     

A CNDO-MO calculation of VCl4

The electronic structure of the tetrahedral molecule VCL₄ is investigated within the CNDO-MO approximations. The metal and ligand valence orbitals, 3d, 4s, 4p; and 3s, 3p; respectively, have been systematically varied in an attempt to minimize the total energy; “optimum” V 4s(χ₄ = 1.10) and 4p(d ³ p ²) orbitals have been established, but V 3d(d ⁿ ) and Cl(-δ) valence orbitals are only seen to favor lower energy for expanded orbitals. Since determining the one-electron molecular orbital level which is occupied by the vanadium lone electron is a major aspect of this investigation, all calculations have been performed in triplicate: calculations assuming the unpaired electron occupies the 3a ₁, 2 _e and 4t ₂ molecular orbital (ground state electronic configurations² A ₁,² E, and² T ₂, respectively). The Hartree-Fock equations have been solved by Roothaan's SCF method for open shells, but off-diagonal multipliers between filled and partly filled molecular orbitals of the same symmetry have been neglected. As a qualitative estimate of the error introduced by this simplification, the pertinent overlap integrals between the eigenfunctions from calculations for the three possible configurations,² A ₁,² E, and² T ₂, are investigated as functions of the component 3d(d ⁿ ) and Cl(-δ) valence orbitals. The overlap integrals from the relevant² A ₁ and² T ₂ calculations are reasonably small, but the neglect of off-diagonal multipliers in calculations on the² E state is found to be a poor approximation. An ordering of the non-filled molecular orbitals in VCl₄ of 4t ₂ < 3a ₁ < 2e < 5t ₂ seems most consistent with the numerous calculations. This suggested ground state electronic configuration of² T ₂ introduces new aspects to the consideration of a (dynamic) Jahn-Teller effect in VCl₄. Experimental data pertinent to the electronic structure of VCl₄ has been briefly summarized, but unfortunately it is inadequate to confirm or deny the present calculations.     

Multireference calculations of the electronic structure of VF2 and VCl2

We investigated the electronic structure of two members of the transition-metal dihalide family, VF(2) and VCl(2). Using the configuration-interaction method in large basis sets we calculated the lowest 17 states of these molecules in the vicinity of their ground-state geometry. We compute the ground-state bond lengths, vibrational frequencies, and dissociation energies. In contrast to predictions of ligand-field theory, we find (4)Sigma(g) (-) ground states for both molecules.     

Action of water and alcohols on acid chlorides in the gaseous state

Conclusions The esterification and hydrolysis of a number of acid chlorides (dimethyldichlorosilane, SiCl₄, acetyl chloride) fail to go when they are treated with water or with alcohols in the gas phase.Deceased.Translated from Izvestiya Akademii Nauk SSSR, Seriya Khimicheskaya, No. 6, pp. 1332–1334, June, 1973.     

Massenspektrometrische Beobachtungen und chemische Transportexperimente mit den Systemen VCl3/Al2Cl6 und VCl2/Al2Cl6

Mass Spectroscopic Observations and Chemical Transport Experiments with the Systems VCl₃/Al₂Cl₆ and VCl₂/Al₂Cl₆ By mass spectrometry the equilibrium VCl_3,s + 0.5 Al₂Cl_6,g ? VAlCl_6,g has been determined: ΔH°(298) = 25.6(±0.5) kcal; ΔS°(298) = 23.0(±3) cal/K, ΔCp (assumed) = ?4 cal/K. This is approximately in agreement with results determined by ligand field spectroscopy by ANUNDSKÅS and ØYE (A. and Ø.). For the dimerization of VCl_3,g values for ΔH and ΔS have been derived. The molecule VAl₂Cl₉ assumed by A. and Ø. could not been observed by mass spectrometry. For the VCl₂/Al₂Cl₆ complex, observed by chemical transport, A. and Ø. give the formula VAl₃Cl₁₁. This molecule could not been observed by mass spectrometry. This suggests a smaller concentration, compared with the results of A. and Ø. Stabilization of VCl_2,s (by metal-nietal-bonds) shifts the reaction to the left, whith explains the lower complex concentration as well as the larger molecular weight of the complex. With chlorides stabilized by stronger metal-metal bonds (MoCl₃, MoCl₂, Nb₃Cl₈) AlCl₃ complexes are not formed in observable concentrations. The chemical transport of VCl₂ with Al₂Cl₆ needs relatively high temperatures (973 → 873 K). In this case the addition of SiCl₄ hinders the attack of the quartz ampoule by Al₂Cl₆. Using a VCl₃ + VCl₂ mixture, VCl₃ is transported by Al₂Cl₆ (673 → 623 K) into the colder region. If afterwords the ampoule is reversed, VCl₃ again moves into the colder region, but the thermal decomposition of VCl₃ at the same time causes that a VCl₂-residue remains in the hot region.     

Hydrogen/deuterium abstraction by chlorine atoms from gaseous ethyl chlorides. Secondary kinetic isotope effects in the system CH3CH2Cl,CH3CHDCl,CH3CD2Cl

The abstraction of hydrogen/deuterium from CH₃CH₂Cl, CH₃CHDCl, and CH₃CD₂Cl by photochemically generated ground-state chlorine atoms has been investigated over the temperature range of 8–94°C using methane as a competitor. Rate constant data for the following reactions have been obtained: The temperature dependence of the relative rate constants k_i/k_j was found to conform to the Arrhenius rate law, where the stated error limits are one standard deviation: and k_r is the rate constant for the reference reaction (CH₄ + Cl → CH₃ + HCl). The β secondary kinetic isotope effects (k₂/k₃/k₄) are close to unity and show a slight inverse temperature dependence. Both preexponential factors and activation energies decrease as a result of deuterium substitution in the adjacent chloromethyl group. The trends are well outside the limits of experimental error.     

Kristallstrukturen von MgCr2O4-Typ Li2VCl4 und Spinell-Typ Li2MgCl4 und Li2CdCl4

Crystal Structures of MgCrO₄-type Li₂VCl₄ and Spinel-type Li₂MgCl₄ and Li₂CdCl₄ The crystal structures of the ternary lithium chlorides Li₂MCl₄ (M = Mg, V, Cd) have been determined firstly by X-ray single-crystal experiments. Li₂MgCl₄ and Li₂CdCl₄ crystallize in an inverse spinel structure (space group Fd3 m, Z = 8, a = 1 040.1(2) and 1 062.06(9) pm, structural parameters u = 0.25699(2) and 0.2550(1), R = 1.7 and 3.7% for 218 and 211 unique reflections). The Li? Cl distances of the tetrahedrally coordinated Li⁺ ions are significantly greater than calculated with Shannon's crystal radii ( > 238 ± 1 instead of 233 pm). Contrary to the results of X-ray powder data reported in the literature, Li₂VCl₄ crystallizes in the distorted spinel structure of MgCr₂O₄ type (space group F4 3m, Z = 8, a = 1 037.49(2) pm, R = 5.9% for 217 unique reflections). The decrease of the site symmetry of the octahedrally coordinated ions (V²⁺, Li⁺) from 3 m to 3m resulting in contracted and widened tetrahedral M₄ entities of the spinel structure is obviously caused by V? V metal—metal bonds (shortest V? V distance 366.2(7) pm).     

Thermochemistry of Gd2BaCuO5 and LuBa2Cu3Ox

Solution calorimetry, using 6.0 M HCl as a solvent, is used to study the thermochemistry of Gd2BaCuO5 and the high-temperature superconductor LuBa2Cu3O6.92. For the first time, the standard formation enthalpies of these phases have been determined as follows: DeltafH(o)(Gd2BaCuO 5, s, 298.15 K) = -2618.6 +/- 7.4 kJ/mol; DeltafH(o)(LuBa2Cu3O6.92, s, 298.15 K) = -2693.1 +/- 11.9 kJ/mol. The thermodynamic stability at room temperature has been assessed. The results show that Gd211 and Lu123 are thermodynamically stable with respect to binary oxides and unstable with respect to interaction with CO 2 at ambient temperatures. Lu123 is thermodynamically stable with respect to assemblages containing combinations of Lu2O3, CuO, and BaCuO2 and thermodynamically unstable with respect to interactions with water.     

Far IR and Raman spectra of some gaseous titanium,zirconium and hafnium cyclopentadienyl chlorides

The far IR and Raman spectra of gaseous (C₅H₅)TiCl₃ and (C₅H₅)₂MCl₂ species (M = Ti, Zr and Hf) are reported. The results are compared to the previous vibrational analysis of the corresponding species in the solid and matrix isolated phases. The assignment of the metal skeletal vibrations is reexamined in further detail on the basis of the new spectroscopic measurements. The torsional frequencies and the related potential barriers are investigated.     

Thermochemistry,Reaction Paths,and Kinetics on the Secondary Isooctane Radical Reaction with 3O2

2,2,4‐Trimethylpentane, also known as isooctane, is used as one of the model fuel species on spark and homogeneous charge compression ignition engines. This study presents thermochemical and kinetic properties in the oxidation of the secondary isooctane radical, which includes the peroxy radical formed from the ³O₂ association, the hydroperoxy alkyl radicals formed from the intramolecular hydrogen transfers, and the products formed from reactions of the hydroperoxy alkyl radicals. Geometries, vibration frequencies, internal rotor potentials, and thermochemical properties, Δ_fH, S°(T), and C°_p(T) (5 K ≤ T ≤ 5000 K) were calculated at the individual B3LYP/6–31G(d,p) and the composite CBS‐QB3 calculation method. The standard enthalpies of formation at 298 K were evaluated using isodesmic reaction schemes with several work reactions for each species. Entropy and heat capacities were determined using geometric parameters and frequencies from the B3LYP/6–31G(d,p) calculations for the lowest energy conformer. Internal rotor barriers were determined. Application of group additivity with comparison to calculated values is also illustrated. Transition states and kinetic parameters for intramolecular hydrogen atom transfer and molecular elimination channels were characterized to evaluate reaction paths and kinetics. Kinetic parameters were determined versus pressure and temperature for the chemical activated formation and unimolecular dissociation of the peroxide adduct. Multifrequency quantum Rice–Ramsperger–Kassel analysis was used for k(E) with master equation analysis for falloff. The kinetic analysis shows that the main reaction channels are the formation of isooctene ((CH3)₃CCH=C(CH₃)₂) + HO₂^?, and the formation of the cyclic: (CH₃)₂‐y(CCH₂CHO)‐(CH₃)₂, (CH₃)₃C‐y(CHCO)‐(CH₃)₂, and (CH₃)₃C‐y(CHCHCH₂O)‐(CH₃).     

白硼钙石的合成新方法及其热化学研究(英)

0IntroductionTherearemanykindsofhydratedcalciumbo-rates,bothnaturalandsynthetic.Someofthemarematerialsusedinglass,potteryandporcelainenamelindustry,especiallyinunalkaliglassindustry.4CaO·5B2O3·7H2O,calledpriceite,isacalciumboratemin-eral,notfoundinCaO-B…     

Cyclopolymerization of isoprene with VCl4–AlEt2Br catalyst system

Isoprene was polymerized at 30°C with VCl₄–AlEt₂Br catalyst system in n-hexane. A linear dependence of rate of polymerization on the monomer and catalyst concentrations was found. The overall activation energy was 8.96 kcal/mole. Infrared spectra of polyisoprene showed the presence of cyclic structure, indicating a cationic mechanism of polymerization.     

Thermochemistry of disputed soot formation intermediates C4H3 and C4H5

Accurate isomeric energy differences and standard enthalpies of formation for disputed intermediates in soot formation, C(4)H(3) and C(4)H(5), have been determined through systematic extrapolations of ab initio energies. Electron correlation has been included through second-order Z-averaged perturbation theory (ZAPT2), and spin-restricted, open-shell coupled-cluster methods through triple excitations [ROCCSD, ROCCSD(T), and ROCCSDT] utilizing the correlation-consistent hierarchy of basis sets, cc-pVXZ (X = D, T, Q, 5, and 6), followed by extrapolations to the complete basis set limit via the focal point method of Allen and co-workers. Reference geometries were fully optimized at the ROCCSD(T) level with a TZ(2d1f,2p1d) basis set. Our analysis finds that the resonance-stabilized i-C(4)H(3) and i-C(4)H(5) isomers lie 11.8 and 10.7 kcal mol(-1) below E-n-C(4)H(3) and E-n-C(4)H(5), respectively, several kcal mol(-1) (more, less) than reported in recent (diffusion Monte Carlo, B3LYP density-functional) studies. Moreover, in these systems Gaussian-3 (G3) theory suffers from large spin contamination in electronic wave functions, poor reference geometries, and anomalous vibrational frequencies, but fortuitous cancellation of these sizable errors leads to isomerization energies apparently accurate to 1 kcal mol(-1). Using focal-point extrapolations for isodesmic reactions, we determine the enthalpies of formation (delta(f)H(0) (composite function)) for i-C(4)H(3), Z-n-C(4)H(3), E-n-C(4)H(3), i-C(4)H(5), Z-n-C(4)H(5), and E-n-C(4)H(5) to be 119.0, 130.8, 130.8, 78.4, 89.7, and 89.1 kcal mol(-1), respectively. These definitive values remove any remaining uncertainty surrounding the thermochemistry of these isomers in combustion models, allowing for better assessment of whether even-carbon pathways contribute to soot formation.