Binding energy of gas molecule with two pyrazine molecules as organic linker in metal�Corganic framework: its theoretical evaluation and understanding of determining factors

We explored the interactions of gas molecules such as H₂, CH₄, C₂H₄, C₂H₆, CO₂, and CS₂ sandwiched by two pyrazine (Pz) molecules, which were employed as a model of organic linker in the Hofmann-type metal?Corganic framework (MOF). The MP2.5/aug-cc-pVTZ method was employed here, because this method presents almost the same binding energy as that calculated by the CCSD(T)/aug-cc-pVDZ with MP2.5-evaluated basis set extension effects to aug-cc-pVTZ basis set. The binding energy of the gas molecule increases in the order H₂?<?CH₄?<?CO₂?<?C₂H₄????C₂H₆?<?CS₂. The energy decomposition analysis of the interaction energy indicates that the electrostatic term presents the largest contribution to the interaction energy at the Hartree?CFock level. However, the dispersion interaction provides dominant contribution to the total binding energy at correlated level. We newly found a linear correlation between the z-component of polarizability of gas molecules and dispersion energy, where the z-axis was taken to be perpendicular to two Pz rings. These results are useful for understanding and predicting the binding energy of the gas molecule with the organic linkers of MOF.     

Studies by the electron cyclotron resonance (ECR) technique: VIII. Interaction of low-energy electrons with the chlorine-containing molecules CCl4, CHCl3, CH2Cl2, CnH2n+1 Cl(n = 1 to 4). C2H3Cl,COCl2, NOCl,CNCl and Cl2

Rate constants, in some cases also activation energies and energy dependences, were measured for the capture of low-energy electrons by the molecules CCl₄, CHCl₃, CH₂Cl₂, C_nH_2n+1 Cl(n = 1 to 4), C₂H₃Cl, COCl₂, NOCl, CNCl and Cl₂ Potential energy curves were calculated for a number of negative ions.For ineffective scavengers the possibility of contributing scattering effects on the observed changes in signal intensity upon electron energy variation is indicated. In CCl₄ the observed energy dependence suggests the existence of intermediate negative ions. For Cl₂ good agreement was obtained between the calculated curves based on experimental data for electron capture and a recent self-consistent field analysis.     

Synthesis and fluorescence properties of covalently linked homo- and hetero-porphyrin dyads containing meso-tolyl porphyrin and meso-furyl porphyrin sub-units

Three porphyrin building blocks with N₄, N₃S and N₂S₂ cores having three meso-furyl groups and one meso-iodophenyl group were synthesized and characterized. The porphyrin building blocks were used to synthesize six porphyrin dyads such as N₄-N₄, N₃S-N₃S, N₂S₂-N₂S₂, N₄-N₃S, N₄-N₂S₂ and N₃S-N₂S₂ containing meso-tolyl and meso-furyl porphyrin sub-units under mild Pd(0) mediated coupling conditions. Steady state fluorescence studies indicated an efficient energy transfer from the meso-tolyl porphyrin sub-unit to the meso-furyl porphyrin sub-unit in all six dyads. This study supported the argument that the meso-furyl porphyrins can be used as good energy acceptors when meso-aryl porphyrins act as energy donors in their metal free form.     

Thermodynamic properties of normal and deuterated cyclopropenes

The specific heat, entropy, enthalpy, and Gibbs free energy of cyclopropene-d₀, cyclopropene-1-d₁, cyclopropene-3-d₁, cyclopropene-1,2-d₂, cyclopropene-3,3-d₂, cyclopropene-1,3,3-d₃, and cyclopropene-d₄ have been calculated for the temperature range 100–1500 K using the rigid-rotor and harmonic oscillator model. The standard enthalpy and Gibbs free energy of formation of cyclopropene-d₀ have also been evaluated for the same temperature range using the experimental standard enthalpy of formation at 298.15 K.     

Ligands of low electronegativity in the vsepr model: electron-rich hydrides MH3E2, MH4E,MH5E,and MH6E

Hydrides FH₃, ClH₃, and OH^?₃ of type MH₃E₂ are calculated to adopt D_3h structures: NH₃^2?, PH₃^2?, and SH₃^? each have two energy minima, one at D_3h and the other at a T-shaped geometry, of which the D_3his the more stable for SH₃^? but the less stable for NH₃^2? and PH₃^2?. Hydrides NH₄^2?, OH₄, and ClH₄⁺ of type MH₄E have a single energy minimum at T_d: CH₄^2?, SiH₄^2?, PH₄^?, and SH₄ each have two minima, one at T_d (more stable for SH₄ only) and one at an SF₄-like C_2v geometry, which is the more stable for CH₄^2?, SiH₄^2? and PH₄^?. D_3h and C_4V structures are very close in energy for all hydrides of type MH₅E, with no activation barrier between the two configurations: D_3h is the more stable configuration for OH₅^?, FH₅, SH₅, and ClH₅, but C_4V is the more stable for NH₅^2?, SiH₅^3?, and PH₅^?. The T_1u bending force constant in hydrides MH₆E becomes negative, for C_3V distortion, in PH₆^3? and SiH₆^4?. Both the equilibrium geometries and the force constants strongly support an interpretation, in terms of the second-order Jahn-Teller effect, of the observed stereochemical inactivity of non-bonding electrons in the presence of ligands of low electronegativity. Molecular energies, equilibrium geometries, orbital energies and electron populations are reported for all species considered in this study. Three molecular states of ClH₄^?, of type MH₄E₂, were also briefly investigated.     

The ground-state potential energy function of PO+

The ground-state potential energy function of PO⁺ has been calculated from the set of molecular constants B _e, ω_e, a _i (i = 1, … , 5), R _e, D _e and C₄ in the form of generalized potential energy function previously suggested by us for solving the inverse spectroscopic problem.     

Structure and stability of SiH+4

Ab initio calculations at the 4-31G level are carried out on the species SiH_n (n = 0 to 4) and the corresponding ions. SiH⁺₄ is found to distort from T_d to D_2d. C_2v, and C_3v, with the latter structure being the lowest in energy by 11 kcal/mole. Consistent with experimental mass spectroscopy, SiH⁺₄ is found to be much less stable to dissociation than CH⁺₄.     

Spin-Hamiltonian parameters and angular distortion for the trigonal Nd3+ center in congruent LiNbO3

The 52 × 52 energy matrix related to the ground multiplet ⁴I_9/2 and the first to third excited multiplets ⁴I_11/2, ⁴I_13/2 and ⁴I_15/2 for 4f³ ions in trigonal crystal field under an external magnetic field is established. By diagonalizing the energy matrix, the spin-Hamiltonian parameters (g factor g_//, g_⊥ and hyperfine structure constants ¹⁴³A_//, ¹⁴³A_⊥, ¹⁴⁵A_//, ¹⁴⁵A_⊥) of the trigonal Nd³⁺ center in congruent LiNbO₃ crystal are calculated. The calculated results are in reasonable agreement with the experimental values. From the calculations, the negative signs of hyperfine structure constants are suggested and the angular distortion of the trigonal Nd³⁺ center in LiNbO₃, which is unable to be determined by EXAFS measurement, is obtained. The results are discussed.     

Thermal degradation of polyisobutylene studied using factor-jump thermogravimetry

The overall activation energy of the thermal degradation of polyisobutylene has been measured using factor-jump thermogravimetry to be 206±1 kJ/mole over the range 365 to 405° in N₂ at 800 mm Hg pressure and flowing at 4 mm/s over the sample. This is consistent with some values reported for thermal degradation in vacuum and in solution. In 5 mm Hg of N₂, an apparent activation energy of 218±2 kJ/mole was found, and in vacuum the apparent activation energy is 238±13 kJ/mole. Troublesome bubbling made the vacuum values difficult to measure. Substitution of reasonable values for the activation energies of initiation,E _i , termination,E _t , and the activation energy,E _a , for vacuum degradation in the equationE _a =E _i /2E _d -E _t /2 yields an activation energy E_d=84 kJ/mole for the unzipping reaction. This equation presupposes a degradation mechanism of random initiation, unzipping, and bimolecular termination. Substitution of reasonable values for the heat of polymerization, ΔH, in the definition ΔH=E _p ?e _d suggests that the activation energy of the polymerization reaction at 375° is approximately 30 kJ/mole.     

Correlation between thermal electron transfer in solution and photoelectron emission

The activation free energy for electron transfer in solution or at electrodes is correlated to the corresponding Franck—Condon determined reorganization free energy R_m for photoelectron emission. Excellent to fair agreement is obtained between the activation free energies predicted from R_m and experimental values. Data are given for V²⁺, Cr²⁺, Mn²⁺, Fe²⁺, Co²⁺, and Fe(CN)^4?₆ in aqueous solution.     

Effect of O2/CH4 ratio on the optimal specific-energy-input (SEI) for oxidative reforming of biogas in a plasma-shade reactor

In a novel plasma-shade reactor for oxidative reforming of biogas (CH₄/CO₂ = 3/2), the effects of specific-energy-input (SEI) on CH₄ and CO₂ conversions and energy cost of syngas were investigated at O₂/CH₄ ratios ranged from 0.42 to 0.67. At each of O₂/CH₄ ratios, V-shape profiles of energy cost of syngas increasing with SEI were observed, reaching the lowest value at the optimal SEI (Opt-SEI). With the increase of O₂/CH₄ ratio, the Opt-SEI decreased significantly. Moreover, at the Opt-SEI, O₂ and CH₄ conversions and dry-basis concentration of syngas increased and energy cost of syngas decreased greatly with the increase of O₂/CH₄ ratio.     

Solubility of gases in butanols: IV. Solubilities of nonpolar gases in 2-methyl-2-propanol at 303.15 K and 101.33 kPa partial pressure of gas

Solubilities of 15 nonpolar gases (He, Ne, Ar, Kr, Xe, H₂, D₂, N₂, O₂, CH₄, C₂H₄, C₂H₆, CF₄, SF₆, and CO₂) in 2-methyl-2-propanol (tert-butanol) have been measured at the temperature 303.15 K and 101.33 kPa partial pressure of gas. Standard changes of the Gibbs energy of solution have been also determined from experimental data. The Lennard–Jones 6,12 pair potential parameters have been estimated for that solvent using the Scaled Particle Theory (SPT) and these parameters have been compared with those corresponding to the other isomers of butanol. It can be concluded that the derived energy parameters provide a measurement of the association of the alkanol. A version of the UNIFAC model has been applied and the corresponding interaction parameters for alkanes and alkanols have been determined.     

Enhanced visible-light photocatalytic activities of porous olive-shaped sulfur-doped BiVO4-supported cobalt oxides

Porous S-doped bismuth vanadate with an olive-like morphology and its supported cobalt oxide (y wt% CoO_x/BiVO_4−δS_0.08, y = 0.1, 0.8, and 1.6) photocatalysts were fabricated using the dodecylamine-assisted alcohol-hydrothermal and incipient wetness impregnation methods, respectively. It is shown that the y wt% CoO_x/BiVO_4−δS_0.08 photocatalysts were single-phase with a monoclinic scheetlite structure, a porous olive-like morphology, a surface area of 8.8–9.2 m²/g, and a bandgap energy of 2.38–2.41 eV. There was the co-presence of surface Bi⁵⁺, Bi³⁺, V⁵⁺, V³⁺, Co³⁺, and Co²⁺ species in y wt% CoO_x/BiVO_4−δS_0.08. The 0.8 wt% CoO_x/BiVO_4−δS_0.08 sample performed the best for methylene blue degradation under visible-light illumination. The photocatalytic mechanism was also discussed. We believe that the sulfur and CoO_x co-doping, higher oxygen adspecies concentration, and lower bandgap energy were responsible for the excellent visible-light-driven catalytic activity of 0.8 wt% CoO_x/BiVO_4−δS_0.08.     

The electronic structures of tetrahedral oxo-complexes. The nature of the “charge transfer” transitions

The electronic structures of MnO^?₄, MnO^2?₄, MnO^3?₄, CrO^2?₄, CrO^3?₄, VO^3?₄, RuO₄, RuO^?₄, RuO^2?₄, TcO^?₄ and MoO^2?₄ have been investigated using the Hartree-Fock-Slater Discrete Variational Method. The calculated ordering of the valence orbitals of all the comlexes is: t₁, 4t₂, 3a₁, 1c, 3t₂, with t₁ the orbital of highest energy. The calculated single transition energies are in good agreement with experimental values and indicate the uniform assignment: t₁ → 2e(v₁), 4t₂ → 2e(v₂). t₁ → 5t₂(v₃), and 4t₂ → 5t₂(v₄). A/D values, calculated from the theory of magnetic circular dichroism (MDC) also support this assignment.Population analyses reveal that all complexes, whether d⁰, d¹ or d², have d-orbital populations close to those of the corresponding M²⁺ ions in which two electrons have been removed from the (n + 1)s orbital of M. This is also true of the excited states, such as t₁ → 2e and 4t₂ → 2e, where a transfer of charge from the ligands to the metal has previously been assumed. It is shown that, instead of a transfer of charge from ligands to metal, electronic excitation consists of a rearrangement of electron density both at the ligands and at the metal.     

Isotropic C6, C8 and C10 interaction coefficients for CH4, C2H6, C3H8, n-C4H10 and cyclo-C3H6

The non-empirical generalized Kirkwood, Unsöld, and the single-Δ Unsöld methods (with double-zeta quality SCF wave-functions) are used to calculate isotropic dispersion (and induction) energy coefficients C_2n, with n ? 5, for interactions involving ground state CH₄, C₂H₆, C₃H₈, n-C₄H₁₀ and cyclo-C₃H₆. Results are also given for the related multipole polarizabilities α_l, multipole sums S₁/(0) and S₁(?1) which are evaluated using sum rules, and the permanent multipole moments. for l = 1 (dipole) to l = 3 (octupole). Estimates of the reliability of the non-empirical methods, for the type of molecules considered, are obtained by a comparison with accurate literature values of α₁S₁(?1) and C₆. This, and the asymptotic properties of the multipolar expansion of the dispersion energy, the use to discuss recommended representation for the isotropic long range interaction energies through R^?10 where R is the intermolecular separation.     

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.     

Irreversible thermodynamics of transport across charged membranes : Part III - efficiency of energy conversion in separation processes with nafion 120 membrane from phenomenological transport coefficients

In separation processes with charged membranes, as in electrodialysis units or electrochemical cells, the efficiency of conversion of electrical energy into the concentration gradient of an electrolyte is depressed by the immediate flow of water in the direction opposite to the solute flow. The equations for energy conversion in transport of ions and water across a cation-exchange membrane are derived in the present paper treating the system as a three-flow process and employing phenomenological transport equations. With these equations, the two-flow (q_1E, q_wE, q_1w and overall (q̃_E) degrees of coupling and the total (η) and component (η_1E,η_wE) efficiencies of energy conversion have been computed for the system sodium chloride/Nafion 120 membrane at temperatures of 298 and 333 K and for solute concentrations between 0.05 and 4 M. Considering the continuous separation processes, the so-called “driving region” and the energy requirement to keep the concentration difference in the adjacent compartments constant (static head) have been calculated and discussed.     

Oxidation of Styrene to Benzaldehyde Catalyzed by Schiff Base Functionalized Triazolylidene Ni(II) Complexes

Four new Schiff base functionalized 1,2,3-triazolylidene nickel complexes, [Ni-(L₁NHC)₂](PF₆)₂; 3, [Ni-(L₂NHC)₂](PF₆)₂; 4, [Ni-(L₃NHC)](PF₆)₂; 7 and [Ni-(L₄NHC)](PF₆)₂; 8, (where L₁NHC = (E)-3-methyl-1-propyl-4-(2-(((2-(pyridin-2-yl)ethyl)imino)methyl)phenyl)-1H-1,2,3-triazol-3-ium hexafluorophosphate(V), 1, L₂NHC = (E)-3-methyl-4-(2-((phenethylimino)methyl)phenyl)-1-propyl-1H-1,2,3-triazol-3-ium hexafluorophosphate(V), 2, L₃NHC = 4,4′-(((1E)-(ethane-1,2-diylbis(azanylylidene))bis(methanylylidene))bis(2,1-phenylene))bis(3-methyl-1-propyl-1H-1,2,3-triazol-3-ium) hexafluorophosphate(V), 5, and L₄NHC = 4,4′-(((1E)-(butane-1,4-diylbis(azanylylidene))bis(methanylylidene))bis(2,1-phenylene))bis(3-methyl-1-propyl-1H-1,2,3-triazol-3-ium) hexafluorophosphate(V), 6), were synthesised and characterised by a variety of spectroscopic methods. Square planar geometry was proposed for all the nickel complexes. The catalytic potential of the complexes was explored in the oxidation of styrene to benzaldehyde, using hydrogen peroxide as a green oxidant in the presence of acetonitrile at 80 °C. All complexes showed good catalytic activity with high selectivity to benzaldehyde. Complex 3 gave a conversion of 88% and a selectivity of 70% to benzaldehyde in 6 h. However, complexes 4 and 7–8 gave lower conversions of 48–74% but with higher (up to 90%) selectivity to benzaldehyde. Results from kinetics studies determined the activation energy for the catalytic oxidation reaction as 65 ± 3 kJ/mol, first order in catalyst and fractional order in the oxidant. Results from UV-visible and CV studies of the catalytic activity of the Ni-triazolylidene complexes on styrene oxidation did not indicate any clear possibility of generation of a Ni(II) to Ni(III) catalytic cycle.     

Molecular structures and infrared spectra of SiZrH4: A theoretical study

Molecular structures of the SiZrH₄ complex were investigated at BPW91, BPW91/IEF-PCM, B3LYP, and MP2 levels of theory with substantial basis sets. Relative stability of the stable conformers is fairly dependent on the methods, solvent effects, and zero-point energy corrections. All the four levels of calculations indicated that the singlet HSi(μ-H)ZrH₂, trans-Si(μ-H)₂ZrH₂, cis-Si(μ-H)₂ZrH₂, and the triplet Si(μ-H)₃ZrH are stable and comparable in energy. The energy of these four isomers is well below that of the Zr(³F₂) + SiH₄ system. The trans-dibridged, rather than the tribridged, isomer was always predicted to be the most stable one by all the four levels of calculations. For the two dibridged isomers, the two SiH₂ stretching modes are highly coupled with the two ZrH₂ stretching modes. And such coupling cannot be removed by the full deuteration.