A spectroscopic study of hydrogen bond formation by silatranes and their analogues

The IR absorption shifts of OH and OD stretching vibrations upon interaction of silatranes XSi(OCH(CH₃)CH₂)₃N and their monocyclic analogues of the type R₂(OCHR′CH₂)₂NR$?with phenol and deuteromethanol, respectively, were measured. In the systems involving silatranes these values are higher than in systems with the corresponding ethoxysilanes. The equilibrium constants and thermodynamic parameters of the interaction of the compounds studied with phenol in n-heptane were measured by electronic spectroscopy. The interaction of phenol with the compounds studied shows two lines correlating with the thermodynamic parameters ΔH - f(ΔS). One of the lines is plotted by alkoxysilanes, cyclic and acyclic ethers. The second line corresponds to the compounds having a O-C-C-N group. This enables a conclusion to be drawn that in a non-polar medium the basic centre of silatranes and their monocyclic analogues is different from the oxygen in ethers and alkoxysilanes.     

An ab initio study of the electronic structure of diimide

Ab initio calculations on the structure and geometry of the three isomers of N₂H₂ (trans-diimide, cis-diimide, and 1,1-dihydrodiazine) were performed both on HF and CI level using gaussian basis sets with polarization functions. The trans and cis isomers have singlet ground states; the trans isomer is found to be lower in energy than the cis isomer by 6.9 kcal/mol (HF) and 5.8 kcal/mol (CI), respectively. The barrier for the trans-cis isomerization is predicted to be 56 (HF) and 55 (CI) kcal/mol. H₂ N=N has a triplet ground state with a non-planar equilibrium geometry and a rather long NN bond of 1.34 Å. Its lowest singlet state, however, is planar with an NN double bond of 1.22 Å; it is found to lie about 3 kcal/mol above the triplet and 26 kcal/mol above the singlet ground state of trans-diimide.     

Synthese de derives mono- ou disilicies au niveau d'un carbone fonctionnel

Aliphatic saturated amides treated with Me₃SiCl/Li/THF were found to react in two ways. Either alkoxysilanes, mono- or di-silylated at the functional carbon, or C-silylated amines were obtained dependent of the original amide structure and the experimental conditions. (Me₃Si)₂CHN(SiMe₃)₂ exhibited Physicochemical properties that are particular for hindered rotation about the CN bond. A general mechanism is proposed to explain these results.     

Energy analysis of metal-metal bonding in [RM-MR] (M = Zn, Cd, Hg; R = CH3, SiH3, GeH3, C5H5, C5Me5)

The metal-metal bonds of the title compounds have been investigated with the help of energy decomposition analysis at the DFT/TZ2P level. In good agreement with experiment, computations yield Hg-Hg bond distance in [H₃SiHg-HgSiH₃] of 2.706 Å and Zn-Zn bond distance in [(η⁵-C₅Me₅)Zn-Zn(η⁵-C₅Me₅)] of 2.281 Å. The Cd-Cd bond distances are longer than the Hg-Hg bond distances. Bond dissociation energies (-BDE) for Zn-Zn bonds in zincocene −70.6 kcal/mol in [(η⁵-C₅H₅)₂Zn₂] and −70.3 kcal/mol in [(η⁵-C₅Me₅)₂Zn₂] are greater amongst the compounds under study. In addition, [(η⁵-C₅H₅)₂M₂] is found to have a binding energy slightly larger than those in [(η⁵-C₅Me₅)₂M₂]. The trend of the M-M bond dissociation energy for the substituents R shows for metals the order GeH₃ < SiH₃ < CH₃ < C₅Me₅ < C₅H₅. Electrostatic forces between the metals are always attractive and they are strong (−75.8 to −110.5 kcal/mol). The results demonstrate clearly that the atomic partial charges cannot be taken as a measure of the electrostatic interactions between the atoms. The orbital interaction (covalent bonding) ΔE_orb is always smaller than the electrostatic attraction ΔE_elstat. The M-M bonding in [RM-M-R] (R = CH₃, SiH₃, GeH₃, C₅H₅, C₅Me₅; M = Zn, Cd, Hg) has more than half ionic character (56-64%). The values of Pauli repulsions, ΔE_Pauli, electrostatic interactions, ΔE_elstat, and orbital interactions, ΔE_elstat are larger for mercury compounds as compared to zinc and cadmium.     

Hydrogen bonds formed by methyl groups of acetonitrile: Infrared and calorimetric study

Solutions of acetonitrile (I) in tetrachloromethane and deuteratred solvents (S) (benzene, acctonitrile, acetone and dimethylsulphoxide) have been studied by IR absorption spectra. The observed solvent effect on the IR spectrum of I was explained in terms of the existence of complexes with hydrogen bonding of the type NCCH₃…solvent (S). The strength of the hydrogen bonding was characterized by enthalpies of specific interactions of I with solvents ΔH^I/S_int(sp). The values ΔH^I/S_int(sp) were determined both by IR spectroscopy and calorimetry and were found to be within the range 0.3–1.5 kcal mol⁻¹.     

Electronic absorption spectra of phenol(H2O)n and (phenol)n as studied by the MS MPI method

The initial stages of solvation and crystallization were studied in phenol(H₂O)_n and (phenol)_n by the use of the mass-selected MPI method in a supersonic free jet. The spectral position exhibits an irregular shift by the change of the cluster size, which is interpreted in terms of the role of phenol as a proton donor, a proton acceptor or both in the hydrogen bonding. The O⁰₀ band of the phenol—water cluster was found to converge to 276.0 nm. The phenol trimer was concluded to have a cyclic structure.     

The structure of the H3O+ (hydronium) ion

Near Hartree-Fock level ab initio molecular orbital calculations on H₃O⁺ and a minimum energy structure with θ(HOH) = 112.5° and r(OH) = 0.963 Å and an inversion barrier of 1.9 kcal/mole. By comparing these results to calculations on NH₃ and H₂O, where precise experimental geometries are known, we estimate the “true” geometry of isolated H₃O⁺ to have a structure with θ(HOH) = 110-112°, r(OH) = 0.97–0.98 Å and an inversion barrier of 2–3 kcal/mole. Our prediction for the proton affinity of water is ≈ 170 kcal/mole, which is somewhat smaller than the currently accepted value.     

μ-Oxo-bis(triorganoantimon- und -bismutsulfonate). Kristallstruktur von {(CH3)3SbOH2]2}O3SC6H5)2

μ-Oxo-bis(triorganoantimony- and -bismuthsulfonates) (R₃MO₃Sr′)₂O[M  Sb, R  Ph, benzyl, M  Bi, R  Ph; R′  Me, CH₂CH₂OH, CF₃, Ph, 4-CH₃C₆H₄, 2,4-(NO₂)₂C₆H₃] and (Me₃SbO₃SR′)₂O · nH₂O (n  2, R′  CF₃, Ph, 4-CH₃C₆H₄; n  0, R′  CH₃, CH₂CH₂OH) have been prepared by reaction of (Ph₃SbO)₂ and Me₃Sb(OH)₂, respectively, with appropriate sulfonic acids or with (R₃MX)₂O (R  Ph, benzyl; X  Br) and R′SO₃H in the presence of Ag₂O. The anhydrous compounds (Me₃SbO₃SR′)₂O are obtained by heating the hydrates. Me₃Sb(OH)₂ and 2,4-(NO₂)₂C₆H₃SO₃H react to give the hydroxosulfonate Me₃Sb(OH)O₃SR′. CH₃OH solvolyzes the products. A covalent structure, with pentacoordinated Sb or Bi atoms, unidentate O₃SR′ ligands and μ-oxygen in apical, and R in equatorial positions, is inferred from the vibrational data for all nonhydrated sulfonate compounds. A correlation between ν_as(SbOSb) vibration and SbOSb bond angles in hexaphenyl distiboxans was established, which indicates that the SbOSb bridges are linear in (Ph₃SbO₃SR′)₂O (R′  2,4-(NO₂)₂C₆H₃, 2,4,6-(NO₂)₃C₆H₂) and bent in the other compounds. Data also indicate that there is a linear BiOBi bridge in (Ph₃BiO₃SCH₂CH₂OH)₂O. The hydrated compounds have a distinctly different ionic structure one H₂O being coordinated apically to each of the pentacoordinated Sb atoms in the cation [(Me₂SbOH₂)₂O]²⁺. This proposal is verified by the crystal structure determination of (Me₃SbO₃SPh)₂O · 2H₂O which revealed an ionic structure: [(Me₃SbOH₂)₂O](O₃SPh)₂. The angles μ-OSbO(H₂O) of 171.7(2) and 171.0(2)° and μ-OSbC(CH₃) of 98.3° (mean) reflect the distortion of the trigonal bipyramidal surrounding of the Sb atoms, and the long SbO(H₂O) distance of 244.4(5) pm (mean) the rather weak bonding of the water molecules to Sb. The distances S [144.6(6) pm (mean)] and the angles OSO [112.6(4)° (mean)] in the sulfonate anion are essentially identical. Hydrogen bonds exist between the water ligands and O atoms of the anions.     

73GE, 17O, 13C NMR Spectra of alkoxygermanes

¹³C, ¹⁷O and ⁷³Ge NMR spectra of seven tetraalkoxygermanes have been investigated. ⁷³Ge resonance signals in these compounds are more sensitive to structure variations than those of ²⁹Si in isostructural alkoxysilanes. ¹⁷O and ¹³C NMR spectra of alkoxygermanes Me_4-n Ge(OR)_n (R = Et, Pr, Bu, i-Bu, s-Bu, CH₂CHCH₂, CH₂CH₂OMe, CH₂CF₃; n = 1–3) have been studied.It has been shown that the magnitude of (p—d)_τ-bonding in the GeO bond is smaller than in the SiO bond, but variation in the extent of (p—d)_τ-overlapping in alkozygermanes with different substituents is similar to that in the isostructural alkoxysilanes.     

The [Cp(CO)2Fe] (Fp) group as a donor in donor/acceptor substituted disilanes: synthesis,structure and electronic properties of FpSi2Me4C6H4CHC(CN)2

UV–vis absorption spectroscopy and cyclic voltammetry are used to study electronic interactions in the donor/acceptor substituted disilane FpSi₂Me₄C₆H₄CHC(CN)₂ (Fp=η⁵-C₅H₅Fe(CO)₂) (1). The synthesis of 1 was achieved by a conventional chemical route, the model substances FpSiMe₃ (2), FpSi₂Me₅ (3) and FpSi₂Me₄C₆H₅ (4) were obtained by the electrolysis of Fp₂ in the presence of the appropriate chlorosilane. The structure of 1, determined by X-ray diffraction, exhibits an all-trans-array of the FeSiSiC_aryl fragment, a basic requirement for optimal through-bond interaction. UV–vis and CV data indicate strong intramolecular donor/acceptor interaction in 1.     

(Aroyloxymethyl)trifluorosilanes: a new class of pentacoordinate silicon compounds

A new class of organosilicon compounds containing a pentacoordinate silicon atom, (aroyloxymethyl)trifluorosilanes (AFS), has been prepared. The presence of an intramolecular coordinate F₃Si ← OC bond is supported by X-ray diffraction, IR spectroscopy and dipole moment data. Si ← O coordination in AFS has been shown to remain intact in the gaseous and liquid states below 420 K as well as in solution in most organic solvents. The dielectric constant of the medium significantly affects the nature of the coordinate Si ← O bond and that of the SiF, CO, COC bonds. In pyridine the intramolecular coordinate Si ← O interaction is disturbed or greatly weakened.At 420–500 K a reversible reaction takes place: ArC$\text{OOCH}{}_2\text{Si}$F₃ α ArCOOCH₂SiF₃ The changes in enthalpy and entropy are equal in this case: ?△H  8.1 ± 0.7 kcal/mol; ?°_S  15.3 ± 0.8 e.u. _T  450 K An assignment of bands in the IR spectra of AFS resulting from vibrations of atoms in the SiF₃, >CO and COC groups is given. The electron impact-induced primary disintegration of the molecular ion 4-XC₆H₄COOCH₂Si

mainly involves abstraction of a fluorine atom.     

A force field study of the chemical reaction between ethylene and cis-N2H2

The fully optimized geometry of the activated complex which occurs as an intermediate in the concerted H-transfer reaction between C₂H₄ and cis-N₂H₂ has been determined using the ab initio FORCE method of Pulay. The activation energy for the synchronous transfer of two hydrogen atoms from cis-N₂H₂ to ethylene is found to be 18.8kcal/mol, i.e. substantially lower than the previously estimated energy barrier of around 60 kcal/mol. The same method applied to trans-N₂H₂ and semilinear N₂H₂ gave an isomerization energy of 49.7 kcal/mol indicating that the isomerization of trans-N₂H₂ to the cis form might be the overall rate-controlling step.     

Iron(III) p-toluenesulfonate catalyzed synthesis of homoallyl ethers from acetals and aldehydes

Iron(III) p-toluenesulfonate, Fe(OTs)₃·6H₂O, is an inexpensive, versatile and commercially available catalyst for the allylation of acetals using allyltrimethylsilane to yield homoallyl ethers in moderate to good yields. The one-pot conversion of aldehydes to homoallyl ethers using alkoxysilanes has also been accomplished using Fe(OTs)₃·6H₂O as a catalyst. The use of mild reaction conditions and a relatively non-corrosive catalyst make this method an attractive option for the synthesis of a range of homoallyl ethers.     

The nature of the bonding of Li+ to H2O and NH3; A3 initio studies

Ab initio wavefunctions have been calculated for the complex of Li⁺ with NH₃ and H₂O in order to better characterize the nature of the bonding. Hartree—Fock and generalized valence bond calculations were performed using a double zeta basis plus polarization functions. The binding energies obtained at the GVB level are D_e (Li⁺ — NH₃) = 40.4 kcal/mol and D_e (Li⁺ ? H₂O) = 37.6 kcal/mol, in reasonable agreement with experimental values. Model calculations indicate that the Li⁺ ? base bond is basically electrostatic. Small basis sets were found to lead to D_e as large as 75 kcal/mol for Li⁺ — NH₃, a significant overestimation. Repulsions due to the Li⁺ core are responsible for keeping the Li⁺ too far away for significant relaxation effects.     

1,1-Dimethyl-1-silaethylene : Heat of formation,ionization potential and the energy of the siliconcarbon π-bond

The thermodynamic cycle consisting of thermal decomposition and dissociative ionization processes for 1,1-dimethyl-1-silacyclobutane is calculated. The heat of formation and the ionization potential (IP) for 1,1-dimethyl-1-sila-ethylene (DMSE) have been obtained: ΔH^o_f(DMSE) = 15.5 ± 5 kcal/mol; IP(DMSE) = 7.5 ± 0.3 eV. The siliconcarbon π-bond energy in DMSE is estimated: D_π(SiC)  28 ± 8 kcal/mol.     

Symmetrically bifurcate hydrogen bonding—III (sym-o,o′ diacyl)-diphenylamines

Symmetrically bifurcate three-centre hydrogen bonding,

, was found in several (sym-o,o′-diacyl)-diphenylamines, [o(RCOC₆H₄)]₂NH.     

Comparative mass spectrometric investigation of transition metal polymethylcyclopentadienylcarbonyl complexes: II mass spectra of RnC5H5–nMN(CO)3 (R = CH3, n = 0–5; R = t-C(CH3)3, n = 1)

Investigation of π-(CH_3nC₅H_5–nMn(CO)₃ (Me_n-CpMnT) n = 0−5 and t-butyl CpMnT mass spectra showed that Me_nCpMnT molecular ion (M⁺) fragmentation occurs by a simpler scheme than that for Me_nCpReT M⁺ molecular ions. The reason is that MnCp and MnCO bonds are not as strong as the ReCp and ReCO bonds, and the relative “inertness” (compared to Re) of the Mn atom (ion), coordinated to the methylcyclopentadienyl ligand. Variations of M⁺ molecular ion intensity with different values of n are probably due to a complexity of electronic and spatial methyl-carbonyl group interactions in M⁺.     

Übergangsmetall-substituierte phosphane,arsane und stibane : XXIX. Metallierte arsane und stibane mit chiralem eisen-substituenten

The reaction of Cp(CO)₂FeEMe₂ (E  As, Sb, Bi) with Me₃P, Et₃P, Me₂PhP and (MeO)₃P leads to a CO/R₃P exchange and formation of the chiral derivatives Cp(CO)(R₃P)FeEMe₂. Cp(CO)[(MeO)₃P]FeEMe₂ rearranges already at room temperature to Cp(CO)[(Me₃E]FeP(O)(OMe)₂ which is transformed by (MeO)₃P to Cp(CO)[(MeO)₃P]FeP(O)(OMe)₂. The high nucleophilicity of the new organometallic Lewis bases is established by the easy conversion of Cp(CO)(Me₃P)FeSbMe₂ to [Cp(CO)(Me₃P)Fe(SbMe₃)]I with MeI, or to [Cp(CO)(Me₃P)FeSbMe₂Fe(CO)LCp]Hal (L  CO, Hal  Cl; L  Me₃P, Hal  Br) with Cp(CO)LFe-Hal, respectively. The new compounds are characterized by spectroscopy and elementary analyses.     

Measurement of barriers to aryl rotation in Cp(CO)2FeCHC6H5+ and Cp(CO)2FeCH(p-CH3C6H4)+

The first observation of barriers to rotation about the C_arylC_carbene bonds in aryl-substituted metal carbene complexes is reported. Using variable temperature ¹H NMR, barriers of 9.1 and 10.4 kcal/mol have been determined for Cp(CO)₂FeCHC₆H₅⁺ and Cp(CO)₂FeCH(p-CH₃C₆H₄)⁺, respectively. The data clearly indicate a geometry of the complex in which the aryl ring lies coplanar with FeC_carbeneC_ipso plane.     

Enthalpies of the formation and decomposition of hydrogen trioxide HOOOH in an aqueous solution

The enthalpies of the formation and decomposition of hydrogen trioxide are estimated from the heating curves of peroxide-radical condensates synthesized from gaseous O₂ + H₂ mixtures. Enthalpy of decomposition Н₂О₃(aq.) → Н₂О(liq.) + О₂(gas) is ?31.2 ± 1.5 kcal/mol, and enthalpy of formation Δ_fH(H₂O₃, aq.) =–37.5 ± 1.6 kcal/mol. Both values correspond to the temperature range of 240–265 K.