On the conformational problem in trisulphides: Preparation,properties and conformational analyses of bis(fluorocarbonyl)trisulphide,FC(O)SSSC(O)F

Bis(fluorocarbonyl)trisulphide, FC(O)SSSC(O)F, was prepared both by reaction of FC(O)SCl with H₂S and by ultraviolet irradiation of FC(O)SSC(O)F. Infrared data for the vapour, liquid and matrices (in Ar, Ne and N₂), as well as Raman, u.v. mass and ¹⁹F and ¹³C NMR spectra have been obtained and interpreted. Complementary measurements were also carried out to determine the dipole moment of the liquid substance.From these data, the most stable conformer was deduced to have a trans conformation of the FC(O) groups with respect to the SSS plane, with both CO bonds syn to the SS bonds.     

Vibro-conformational behaviour and normal coordinate analysis of fluorocarbonyl isocyanate,FC(O)NCO

Vibrational data of vapour, liquid and matrix-isolated fluorocarbonyl isocyanate, FC(O)NCO, were investigated. A subsequent normal coordinate analysis was performed for the A′ species of the predominant planar cis conformer (CO double bond cis with respect to the vicinal NC double bond). The following internal force constants were derived: f_CO= 12.88 mdyn Å⁻¹, f_CF=6.20 mdyn Å⁻¹ and F_CN= 4.42 mdyn Å⁻¹.     

Determination of the conformation in thioester compounds containing the NSO group through pre-resonance Raman study: Spectroscopic properties of S(N-sulphinylimine)-fluorocarbonylsulphane,FC(O)SNSO

Starting from fluorocarbonylsulphenyl chloride, FC(O)SCl, and N-trimethylsilysulphinylimine, (CH₃)₃SiNSO, the compound S(N-sulphinylimine)-fluorocarbonylsulphane, FC(O)SNSO, has been prepared. The IR, pre-resonant Raman, ¹³C NMR, mass, and UV spectra have been obtained and interpreted.The two bands appearing in the CO stretching fundamental mode region of the vibrational spectra were specially investigated to probe the existence of conformational isomerism in the molecule. From the analysis of the bands and their contours in the vapour-IR spectra, and the depolarization ratios together with the pre-resonant behaviour in the Raman spectrum of the liquid (whose extension is also evaluated), two planar forms can be determined for the molecule.The study of the CO envelope in the IR spectrum of the vapour phase reveals syn conformation (with respect to the CO and SN bonds) as the most stable structure for the molecule, and the anti conformation as the second structure.     

FC(O)SNCO的电子结构和光电离解离过程

由于拥有―C(O)S―和―NCO基团, FC(O)SNCO的分子和电子结构是非常有趣的. 利用FC(O)SCl和AgNCO制备了FC(O)SNCO,并利用HeI光电子能谱(PES)、光电离质谱(PIMS)以及理论计算研究了其分子和电子结构. 通过将实验、理论计算以及自然键轨道(NBO)分析结合起来, 获得了FC(O)SNCO的最稳定分子构型. 利用外壳层格林函数(OVGF)方法以及与相似化合物的比较, 对其光电子能谱进行了指认. 理论计算表明,对于中性分子最稳定的构型为syn-syn非平面构型, 而电离后的离子最稳定构型为syn-syn平面构型. 实验结果表明, 第一电离能来自于S的孤对电子轨道, 为10.33 eV. 第二至第六电离能分别为12.03、13.23、13.77、14.78、15.99 eV, 并对这些电离能进行了指认. 在光电离质谱中产生了六个质谱峰, 分别为SN⁺、FC(O)⁺、SNCO⁺、FC(O)SN⁺、C(O)SNCO⁺、FC(O)SNCO^+·, 其中FC(O)SNCO^+·的峰是最强峰. 结合HeI光电子能谱和理论计算, 对PIMS进行了分析,并研究了可能的电离和解离过程并对其进行了讨论.     

Molecular mechanics calculations for conformational energies and torional force constants in fluoro propenes and butenes

Experimental data on conformational energies of the molecules FH₂CHCCH₂, FH₂CFCCH₂, FH₂C(CH₃)C&.dbnd;CH₂ trans-FH₂CHCC(CH₃)H have been used to establish parameter values for the nonbonding atom ⋯ atom interaction F ⋯ C(sp²) within the Morse potential formulation. Torsional potentials have been calculated for the four molecules mentioned above and in addition for cis- and trans-FH₂CHCCHF, (FH₂C)₂CCH₂, cis-FH₂CHCCHCH₂F, CH₃FCHHCCH₂ and FH₂CCH₂HCCH₂. Calculated results have been compared with experimental values. Torsional force constants for the molecules have been obtained. A comparison between fluoro, chloro and bromo compounds is presented.     

Pre-resonance Raman,IR, 19F, 13C, 15N NMR,mass, and UV spectra in NSO containing compounds: study of S(N-sulfinylimine)-perfluoromethyldisulphane CF3SSNSO

Starting from CF₃SSCl and (CH₃)₃SiNSO, the compound S(N-sulfinylimine)-perfluoromethyl-disulphane, CF₃SSNSO, has been prepared. The IR, pre-resonant Raman, ¹⁹F, ¹³C and ¹⁵N NMR, mass, and UV spectra have been obtained and interpreted.Both Raman studies at different temperatures and those using different excitation radiations reveal the existence of the molecule in one preferred conformation. From these studies a pre-resonant effect can be determined. Its extension is associated with the particular C₁ conformation adopted for the molecule. The available spectroscopical data confirm not only the proposed structure for the molecule but are also consistent with a skew [SC(F₃) and SN], skew (SS, NS) and cis (SN, SO) conformation regarding the SS and XNSO parts of the molecule.     

Estimates for systematic empirical corrections of consistent 4–21G ab initio geometries and their correlations to total energy group increments

The structural parameters of the completely relaxed 4–21G ab initio geometries of more than 30 basic organic compounds are compared to experimental results. Some ranges for systematic empirical corrections, which relate 4–21G bond distances to experimental parameters, are associated with total energy increments. In general, for the currently feasible comparisons, the following corrections can be given which relate calculated distances to experimental r_g parameters and calculated angles to r_s-structures For CC single bond distances, deviations between calculated and observed parameters (r_g) are in the ranges of ?0.006(2) to ?0.010(2) Å for normal or unstrained hydrocarbons; ?0.011(3) to ?0.016(3) Å for cyclobutane type compounds; and +0.001(5) to +0.004(4) Å for CH₃ conjugated with CO. For CO single bonds the ranges are ?0.006(9) to +0.002(3) Å for CO conjugated with CO; and ?0.019(3) to ?0.027(9) Å for aliphatic and ether compounds. A very large and exceptional discrepancy exists for the highly strained ethylene oxide, r_s — r_e = ?0.049(5) Å and in CH₃OCH₃ and C₂H₅OCH₃ the r_s — r_e differences are ?0.029(5), ?0.040(10) and ?0.025(10) Å. Some of these discrepancies may also be due to deficiencies of the microwave substitution method caused by atomic coordinates close to inertial planes. For CN bonds, two types of NCH₃ corrections are from +0.005(6) to ?0.006(6) and from ?0.009(2) to ?0.014(6) Å; and the range for NCO is +0.012(3) to +0.028(4) Å. For isolated CC double bonds the range is + 0.025(2) to +0.028(2) Å. For conjugated CC double bonds the correction is less positive (+0.014(1) Å for benzene). For CO double bonds the corrections are ?0.004(3) to +0.003(3) Å. For bond angles of type HCH, CCH, CCC, CCO, CCO, OCO, NCO and CCC the corrections are of the order of magnitude about 1–2° (or better). Angles centered at heteroatoms are less accurate than that, when hydrogen atoms are involved. Differences in HOC and NHC angles were found in a range of ?2.3(5)° to ?6.2(4)°.     

Reaction of oxygen with a binuclear cobalt(II) hexaphosphine complex. Single-crystal X-ray structure of an extended chain cobalt(II) hexaphosphine oxide system

Molecular oxygen reacts rapidly with Co₂Cl_4-x,(eHTP)^x+ [x = 0 or 2; eHTP = (Et₂PCH₂CH₂)₂PCH₂P(CH₂CH₂PEt₂)₂] in dry acetonitrile to produce in approximately 66% yield the fully-oxygenated phosphine oxide eHTP (eHTPO) Co(II) complex [Co(eHTPO)²⁺][CoCl₄²⁻. The X-ray structure on this novel system shows an extended chain system in which the monomeric repeating unit has an octahedral Co(II) centre. The eHTPO ligand is adopting an unusual conformation with the phosphine oxide groups P(2)P(1)P(3) (P(1) is one of the internal phosphorus atoms) forming a P(1)P(2) chelate to the metal atom while P(3) bridges to another Co(eHTPO)²⁺ monomer unit making up the extended chain, instead of acting as an independent bis chelating group. The third unique coordination site on the cobalt centre is occupied by a phosphine oxide group from the other half of the eHTPO ligand which bridges over to the cobalt centre forming a facial set of three PO donor ligands. This mixed bridging/chelating conformation gives rise to fused seven- and nine-membered ring systems with a CoCo separation of 7.613(0) Å between symmetry related cobalt sites on the extended chain. This structure is the first reported for a Co(R₃PO)₆ⁿ⁺ (R = alkyl, phenyl) system.     

A dipole moment study of n-trimethyl-ammoniobenzamidates and n-benzoyliminodimethylsulphur(iv)

Analysis of the dipole moments of N-trimethylammoniobenzamidates Me₃N⁺-N^?COC₆H₄X, with X = H, p-F, p-Cl or p-NO₂, and of N-aroyliminodimethylsulphur(IV) Me₂SNCOC₆H₄X (X = H and p-NO₂) shows that, as solutes, these compounds exist in the syn conformation. Models are proposed for N-trimethylammonio-orthochloroben-zamidate and N-orthocyanobenzoyliminodimethylsulphur(IV). The (Me₃N⁺-N^t-) and (SN) dipole moments, and the (N-CO) and (SN-CO) mesomeric moments, are derived and discussed.     

Insertion of N-sulfinylsulfonamides and bis(methylsulfonyl)sulfur diimide into ironcarbon σ bonds

The N-sulfinylsulfonamides R′S(O)₂NSO (R′ = CH₃, p-CH₃C₆H₄) insert into the FeR bonds of η⁵-C₅H₅Fe(CO)₂R (R = CH₃, CH₂C₆H₅) to afford η⁵-C₅H₅Fe(CO)₂N[S(O)₂R′][S(O)R]. These products undergo oxidation by m-ClC₆H₄C(O)-OOH to η⁵-C₅H₅Fe(CO)₂N[S(O)₂R′][S(O)₂R] and rearrange on storage to η⁵-C₅H₅Fe(CO)₂S(O)[NS(O)₂R′]R. Reaction between the η⁵-C₅H₅Fe(CO)₂R and CH₃S(O)₂NSNS(O)₂CH₃ leads to the insertion products η⁵-C₅H₅Fe(CO)₂N-[S(O)₂CH₃][S(R)NS(O)₂CH₃].     

Methyl Fluorocarbonyl Disulfide (FC(O)SSMe): A Theoretical Study on the Structural and Conformational Properties of Its Neutral Ground State and Lowest‐Lying Cationic State

In this work, we present a theoretical study on the structural and conformational properties of FC(O)SSMe in its neutral and cationic ground states. The structure of the neutral molecule, as deduced from Hartree? Fock (HF), Density Functional Theory (DFT), and Møller? Plesset (MP2) methods, agrees with the experimentally determined value for the CSSC dihedral angle (C? S bonds gauche with respect to each other) and with the syn preference of the SSCO dihedral angle (C?O bond syn with respect to the S? S bond). The calculated values for these two dihedral angles are 81.9 and 4.2 degrees, respectively. From the energy difference of the anti vs. syn conformer computed at the CCSD(T)/6‐311++G** level of theory, a 3% contribution of a less‐stable conformer at room temperature is proposed. The potential barrier of rotation about the S? S bond is 5.7 kcal/mol (B3PW91/6‐311++G** approximation). The FC(O)SSMe molecule adopts a planar structure after ionization, the anti conformer (CSSC dihedral angle 180°) being the most‐stable form. For the first ionization of the title compound, the adiabatic ionization potential (IP^ad) derived from the three mentioned theoretical methods (using the 6‐311++G** basis sets) is 8.48, 9.06, and 8.99 eV, whereas the vertical ionization potential (IP^ver) is 8.96, 9.79, and 9.62 eV, respectively (experimental value: 9.0 eV). The results are compared with previous experimental studies carried out for the neutral and charged species interpreted on the basis of the Natural Bond Orbital (NBO) analysis. From these calculations, the importance of the anomeric and mesomeric effects becomes evident. The preferred conformation can be quantitatively explained by evaluation of donor/acceptor interaction energies.     

Diorganotin(IV) bis(O,O-alkylenedithiophosphates)

O,O-Alkylenedithiophosphates of diorganotin(IV) of the type R₂Sn[SP(S)O₂G]₂ (R = Me, Et, n-Bu, Ph; G = CH₂CMe₂CH₂, CMe₂CMe₂, CMe₂CH₂CHMe) have been synthesized by the reactions of diorganotin(IV) dichlorides with ammonium O,O-alkylenedithiophosphates or that of diorganotin(IV) oxides with O,O-alkylenedithiophosphoric acids in 1:2 molar ratio in benzene. These new complexes are white solids which are soluble in common organic solvents and are monomeric in refluxing benzene; and they have been characterized by elemental analysis and by different spectroscopic (IR, ¹H, ¹³C, ³¹P and ¹¹⁹Sn NMR) studies, on the basis of which a six coordinated octahedral structure has been suggested in solution.     

A dichromium(II) compound with an elongated metal-metal bond: Cr2(oxindolate)4(oxindole)2

The title compound has been prepared by reaction of (C₅H₅)₂Cr with oxindole (indole with CO in place of CH₂ at the 2-position). Red single crystals belong to space group P2₁/c with a = 10.107(4) Å, b = 22.496(7) Å, c = 9.210(3) Å, β = 93.26(3)°, V = 2091(2), and Z = 2. The centrosymmetric molecule has a CrCr distance of 2.495(4) Å. The mean CrO and CrN distances for the bonds to bridging oxindolate anions are 2.024(7) and 2.065(8) Å, respectively. There is an oxindole molecule bound at each end with a CrO axial bond of length 2.341(8) Å and a hydrogen bond from the oxindole NH group to an equatorial oxygen atom of length 2.83(1) Å. The significance of this compound with respect to CrCr bonding is discussed.     

The structure of propadienone (CH2CCO)

A complete r_o structure has been obtained for propadienone (CH₂CCCO) with the aid of ab initio molecular-orbital calculations. The effect of electron correlation has been investigated using third order Møller-Plesset perturbation theory. The molecule is found to be planar bent (CCC145°) and the calculated structure yields rotational constants which are in good agreemant with experimental values.     

Cumulated double bond systems as ligands : IV. 1H and 13C NMR studies of the intra- and inter-molecular exchange processes of cationic dialkylsulfurdiimine compounds of RhI,IrI and PtII

The preparation and properties are described of trans-[(Ph₃P)₂(CO)M(RNSNR)] [ClO₄] (M  Rh^I, Ir^I; R  Me, Et, i-Pr, t-Bu) and of cis- or trans-[L₂Pt(RNSNR)X] [ClO₄] (X  Cl^?, L  Et₂S, PhMe₂As, PhMe₂P, R  Me, t-Bu; X  CH₃, L  PhMe₂P, R  Me).¹H and ¹³C NMR data show the existence of various isomers in solution which may interconvert via intra- and inter-molecular exchange processes. A general reaction scheme for the intramolecular exchange processes is discussed.     

Coordination chemistry of sulfines : I. Synthesis and characterization of the complexes Pt(PPh3)2(XYCSO) (X,Y = aryl,S-aryl,S-alkyl,Cl). Coordination via the CS-π-bond

Reactions of Pt(PPh₃)₄ with the sulfines, XYCSO, (X, Y = aryl, S-aryl, S-alkyl, Cl) yield coordination compounds of the type Pt(PPh₃)₂(XYCSO). Infrared, ³¹P and ¹H NMR spectra reveal that in all cases the sulfine ligand is coordinated side-on via the CS π-bond (Pt—η²-CS). Reactions of Pt(PPh₃)₄ with either the E- or Z-isomer of (p-CH₃C₆H₄)(CH₃S)CSO yields the corresponding E- or Z-coordination compound, Pt(PPh₃)₂[E-(p-CH₃C₆H₄)(CH₃S)CSO] or Pt(PPh₃)₂[Z-(p-CH₃C₆H₄)(CH₃S)CSO], indicating that the configuration of the sulfine ligand is retained upon coordination to the Pt(PPh₃)₂ unit. The compounds Pt(PPh₃)₂(XYCSO), containing reactive CX and/or CY bonds (X, Y = S-aryl, S-alkyl, Cl), undergo a rearrangement in solution to give complexes of the type PtX(PPh₃)₂(YCSO).     

Molecular structure and conformation of gaseous vinyldimethylchlorosilane as determined by electron diffraction

The molecular structure of vinyldimethylchlorosilane has been determined by gas phase electron diffraction at room temperature. The least squares values of the bond lengths (r_g) and bond angles (∠_α) are : r(CH) = 1.086(6) Å, r(CC) = 1.347(5) Å, r(SiC=) = 1.838(6) Å, r(SiC) = 1.876(3) Å, r(SiCl) = 2.078(2) Å, ∠CCSi = 127.8° (1.2) and ∠=CSiCl = 107° (1). Models with pure syn form and a mixture of syn and gauche gave equally good agreement with the diffraction data.     

Rotational isomerism of O,O′-dialkyl esters of phosphorodithioic acid

Compounds (RO)₂ P(:S)SH, RPrⁱ, Buⁿ, and Octⁿ, exhibit rotational isomerism about PO and PS bonds. Temperature-dependence studies of band intensities indicate values of ΔH for the equilibria between isomers to be 2.5 kJ mol⁻¹, RPrⁱ; 3.0 kJ mol⁻¹, RBuⁿ; and ∼4.5 kJ mol⁻¹, ROctⁿ.     

Zur reaktion von metall-koordiniertem kohlenmonoxid mit yliden: XI. Einige neuartige η1-vinyl-komplexe des eisens durch deprotonierung kationischer carbenkomplexe mit trimethyl(methylen)phosphoran

Novel η¹-vinyl complexes of the type Cp(CO)(L)FeC(OMe)C(R)R′ (R = R′ = H, Me; R = H, R′ = Me; L = Me₃P, Ph₃P) are obtainied via methylation of the acyl complexes Cp(CO)(L)FeC(O)R (R = Me, Et, i-Pr) with MeOSO₂F and subsequent deprotonation of the resulting carbene complexes [Cp(CO)(L)FeC(OMe)R]SO₃F with the phosphorus ylide Me₃PCH₂. The same procedure can be applied for the synthesis of the pentamethylcyclopentadienyl derivative C₅Me₅(CO)(Me₃P)FeC(OMe)CH₂, while treatment of the hydroxy or siloxy carbene complexes [Cp(CO)(L)FeC(OR)Me]X (R = H, Me₃Si; X = SO₃CF₃) with Me₃CH₂ results in the transfer of the oxygen bound electrophile to the ylidic carbon. Some remarkable spectroscopic properties of the new complexes are reported.     

Theoretical investigations on structure, electrostatics potentials and vibrational frequencies of Li+ - CH3- O- (CH2- CH2- O)n- CH3 (n=3-7) conformers

Electronic structure, charge distributions and vibrational characteristics of CH₃ O(CH₂ CH₂ O) _n CH₃ (n=3-7) have been derived using the ab initio Hartree Fock and density functional calculations. For tri- to hexaglymes the lowest energy conformers have trans- conformation around the C-C and C-O bonds of the backbone. For heptaglyme (n=7 in the series), however, gauche-conformation around the C-C bonds renders more stability to the conformer and turns out to be 10.1 kJ mol ⁻¹ lower in energy relative to the conformer having trans-orientation around the C-C and C-O bonds. The molecular electrostatic potential topographical investigations reveal deeper minima for the ether oxygen in conformers having the gauche conformation around the C-C bonds over those for the trans- conformers. A change from trans- to gauche-conformation around the C-C bonds of the lowest energy conformer of heptaglyme engenders a triplet of intense bands ∼1,150 cm ⁻¹ in the vibrational spectra. Theoretical calculations predict that Li ⁺ binds strongly to the heptaglyme conformer in the above series. The frequency shifts in the vibrational spectra of CH₃O(CH₂CH₂O) _n CH₃- Li⁺ (n=3-7) conformers have been discussed