Mass spectrometry of organic compounds of the group V Elements: VI—A new type of amine fragmentation under electron impact

A new type of amine fragmentation under electron impact is elucidated for proline, sarcosine and aspartic acid derivatives and aminomethylphosphines of the general formula R₂NCH₂X. Ordinary α-cleavage affording the \documentclass{article}\pagestyle{empty}\begin{document}$ {\rm R}_2 \mathop {\rm N}\limits^{\rm + } {\rm = CH}_{\rm 2} $\end{document} ion is suppressed by elimination of a neutral HX particle and [M - HX]⁺ ion formation, or M-HX neutral particle ejection and generation of an [HX]⁺ ion from [M]⁺˙. Such fragmentation is ensured by the presence of an α-heteroatom (N, O, P, S) in one substituent (X) and a CO₂R type delocalizing group in the α-position of the other substituent (R₂N).     

On the kinetic stability of the SH3X species with X=F,Cl

Portions of the [S, H₃, X] (X=F, Cl) potential energy surfaces (PESs) were explored using the RHF, MP2, and QCISD(T) methods with emphasis on H₂ and HX eliminations, SH₃X→SHX+H₂ and SH₃X→SH₂+HX, respectively. Upon the halogen X substitution, the most favorable decomposition pathway of SH₄ went over to HX elimination, proceeding with a very low activation barrier of 6.9 (X=F) and 1.3 (X=Cl) kcal/mol. Moreover, the transition states (TSs) for H₂ elimination from SH₃X resembled the less favorable homopolar TS of SH₄. Upon the X=F substitution, the barrier to H₂ loss of SH₄ was calculated to increase from 19.5 to 21.5 kcal/mol. For X=Cl, only the indirect H₂ elimination path via the SH₂+HCl→SHCl+H₂ exchange was found. The hydrogen‐exchange reaction SH₂+HX→SH₂+HX was predicted to occur through formation of the hydrogen‐bonded complex XHSH₂ and with a relatively high barrier of 43.5 (X=F) and 38.5 (X=Cl) kcal/mol. FHSH₂ and ClHSH₂ were found to be the lowest energy species on the [S, H₃, F] and [S, H₃, Cl] PESs, lying 53.4 and 44.7 kcal/mol below SH₃F and SH₃Cl, respectively. ©1999 John Wiley & Sons, Inc. Int J Quant Chem 73: 37–43, 1999     

Evaluation of HX (X = Cl,Br, O) product distributions from chemiluminescence. I. H atom reactions

The HX product state distributions from the H+Cl₂, Br₂, NO₂Cl, PCl₃, and NO₂ reactions have been studied by the infrared chemiluminescence technique in two different laboratories with two types of reactors; a fast-flow system with = 1 Torr of Ar buffer gas and a low-pressure, cold-wall system (usually called the cold-wall arrested-relaxation method). The same Einstein coefficients were used in both laboratories to convert intensities to populations and emphasis is placed upon evaluation of the reliability of the resulting vibrational-rotational HX distributions. Good agreement was found between the HX distributions from the cold-wall reactors from the two laboratories and for both types of reactors for all of the reactions, except PCl₃. For the H+Cl₂, Br₂ and NO₂ reactions, our general results are in good accord with presently accepted data; but, our experiments provide somewhat more detail than in the literature. The NO₂Cl results are new and <f_v(HCl) > = 0.40 and <f_R(HCl) > = 0.01. The H+PCl₃ reaction appears to proceed by two channels and the HCl chemiluminescence cannot be assigned only to HCl formation via direct Cl atom abstraction.     

Why Are B ions stable species in peptide spectra?

Protonated amino acids and derivatives RCH(NH₂)C(+O)X · H⁺ (X = OH, NH₂, OCH₃) do not form stable acylium ions on loss of HX, but rather the acylium ion eliminates CO to form the immonium ion RCH = NH ₂ ⁺ . By contrast, protonated dipeptide derivatives H₂NCH(R)C(+O)NHCH(R′)C(+O)X · H⁺ [X = OH, OCH₃, NH₂, NHCH(R″)COOH] form stable B₂ ions by elimination of HX. These B₂ ions fragment on the metastable ion time scale by elimination of CO with substantial kinetic energy release (T _1/2 = 0.3–0.5 eV). Similarly, protonated N-acetyl amino acid derivatives CH₃C(+O)NHCH(R′)C(+O)X · H⁺ [X = OH, OCH₃, NH₂, NHCH(R″)COOH] form stable B ions by loss of HX. These B ions also fragment unimolecularly by loss of CO with T _1/2 values of ～ 0.5 eV. These large kinetic energy releases indicate that a stable configuration of the B ions fragments by way of activation to a reacting configuration that is higher in energy than the products, and some of the fragmentation exothermicity of the final step is partitioned into kinetic energy of the separating fragments. We conclude that the stable configuration is a protonated oxazolone, which is formed by interaction of the developing charge (as HX is lost) with the N-terminus carbonyl group and that the reacting configuration is the acyclic acylium ion. This conclusion is supported by the similar fragmentation behavior of protonated 2-phenyl-5-oxazolone and the B ion derived by loss of H-Gly-OH from protonated C₆H₅C(+O)-Gly-Gly-OH. In addition, ab initio calculations on the simplest B ion, nominally HC(+O)NHCH₂CO⁺, show that the lowest energy structure is the protonated oxazolone. The acyclic acylium isomer is 1.49 eV higher in energy than the protonated oxazolone and 0.88 eV higher in energy than the fragmentation products, HC(+O)N⁺H = CH₂ + CO, which is consistent with the kinetic energy releases measured.     

Studies on addition of arynyl Grignard reagents to (μ-dithio)bis(tricarbonyliron): —Synthesis,structures and formation mechanism of “open” and “closed” iron-sulfur cluster complexes

Arynylmagnesium bromides cleave the S? S bond of μ-S₂Fe₂(CO)₆ to give equilibrium mixtures of “open” intermediates (μ-ArC≡CS) (μ-BrMgS)Fe₂(CO)₆ and “closed” intermediates μ-[S(Ar)C=C(MgBr)S]Fe₂(CO)₆. The mixtures were treated with CpFe(CO)₂I or some of organic halides to yield corresponding “open” Fe-S complexes, whereas with CF₃CO₂H, gaseous HBr or CH₃HgCl to afford the “closed” ones. The “closed” products were also observed with those alkyl halides which eliminate HX easily. So, this kind of alkyl halides possibly functions as substrates through elimination of HX in reaction courses     

Solid‐State [2+2] Photodimerization of 1‐Aryl‐4‐pyridylbutadienes in Cation‐π‐Controlled Crystals

Irradiation of HX (X=CF₃SO₃ or CF₃CO₂) salts of 1‐aryl‐4‐pyridylbutadienes 1 a – 1 c in the solid‐state afforded syn head‐to‐tail dimers in good yields among a number of possible dimers, whereas irradiation of the neutral substrates gave a complex mixture or no products. A comparison of the X‐ray crystal structures of the neutral compounds and the HX salts clarified that their orientation modes are head‐to‐head and head‐to‐tail, respectively. Moreover, while the distances between the two neighboring double bonds of the neutral compounds are relatively far apart from each other, those of HX salts are close together, satisfying Schmidt's requirement. These findings suggested that cation‐π interactions between the pyridinium and aromatic rings are effective for the preorientation of the HX salts of substrates, leading to photodimers in high regio‐ and stereoselectivities.     

Collision induced fragmentation of mass-selected (CO2) n + clusters

The collisional velocity dependence of the cross sections for fragmentation of mass-selected (CO₂) _n ⁺ (n+2...7) clusters in collisions with Ar atoms is presented. Interesting structure can be observed in the cross sections which indicate that the collision occurs between the Ar atom and one CO₂ molecule within the cluster. The results may be explained by assuming that the collision leads to either vibrational excitation of a loosely bound CO₂ monomer which then leaves the cluster or excitation of the entire cluster to a dissociative state.     

Hydrogen abstraction by fluorine atoms: F + HX and F + DX (X = I,Br, Cl)

Absolute reaction rates for F + HX and F + DX (X = I, Br, Cl) have been obtained by monitoring the rise time of HF (DF) vibrational fluorescence following multiphoton dissociation of SF₆ in mixtures of HX (DX) and argon. The cross sections for reaction are, in units of 10^?16 cm², 4.37, 5.26, and 1.16 for HI, HBr, and HCl, respectively. The isotope effects k_HX/k_DX, are 1.29 ± 0.14, 1.29 ± 0.18, and 1.38 ± 0.29, respectively.     

A theoretical study of the condensation reactions of methyl cation with ammonia,water, hydrogen fluoride and hydrogen sulphide

Ab initio molecular orbital calculations have been used to study the condensation reactions of CH₃^? with NH₃, H₂O, HF and H₂S. Geometry optimization has been carried out at the Hartree—Fock (HF) level with the split-valence plus d-polarization 6-31G* basis set and improved relative energies obtained from calculations which employ the split-valence plus dp-polarization 6-31G** basis set with electron correlation incorporated via Moller—Plesset perturbation theory terminated at third order (MP3). Zero-point vibrational energies have also been determined and taken into account in deriving relative energies. The structures of the intermediates CH₃XH^? (X = NH₂, OH, F and SH) have been obtained and dissociation of these intermediates into CH₂X⁺ + H₂ on the one hand, and CH₃^? + HX on the other, has been examined. It is found that for those species for which the methyl condensation reaction is observed to have an appreciable rate (X = NH₂ and SH), the transition structure for hydrogen elimination from CH₃XH^? lies significantly lower in energy than the reactants CH₃^? + HX (by 75 and 70 kJ mol^?1 respectively). On the other hand, for those species for which the methyl condensation reaction is not observed (X = OH and F), the transition structure for H₂ elimination lies higher in energy than CH₃^? + HX (by 6 and 87 kJ mol^?1 respectively).     

On the mechanism of conductivity of ammonium salts

The conductivities of HSO₄^?-doped (NH₄)₂SO₄ (AS) and NH₄H₂PO₄ (ADP) crystals are investigated in the temperature range 25°?180°C. The mobility of the charge carriers (protons) is thermally activated and is expressed in accordance with the relation μ = 0.16 exp(?0.49) eV/kT and μ = 0.80 exp(?0.54 eV/kT)cm² V^?1 sec^?1 for AS and ADP crystals, respectively. Three-stage mechanism of proton transport in the lattice of ammonium salt is suggested: (1) formation of the charge carrier NH₄⁺ + X^? → NH₃ + HX, (2) reorientation of the protonated anion HX → XH, and (3) proton jump to the neighbor anion XH + X^? → X^? + HX. The activation energy for mobility is close to that for dielectric relaxation process, i.e., the only thermally activated stage in the mobility process is reorientation of the protonated anion. This very stage is also the rate-determining in the mobility as it is seen from the comparison of the correlation time for proton diffusion and the dielectric relaxation time. These experimental results are in good agreement with the known proton dynamic data in KDP-type ferroelectric crystals.     

Reactivity of verdoheme, [(OEOP)FeII(py)2]Cl,toward HX (X=F,CF3CO2, CF3SO3)

Reaction of verdoheme, [(OEOP)Fe^II(py)₂]Cl, where OEOP is the monoanion of octaethyloxoporphyrin, with HX (X = F, CF₃CO₂, CF₃SO₃) has been studied in the presence of air, producing six-coordinate iron(III) product, [OEOPFe^IIIX₂] (X = F (2), CF₃CO₂ (3)) or five-coordinate iron(II) oxoporphyrin compound, [OEOPFe^II(CF₃SO₃)] (4). Compounds 2, 3 and 4 have been isolated and characterized by spectroscopic methods. ¹H NMR spectroscopy and magnetic measurements reveal that [OEOPFe^IIIX₂] (X = F and CF₃CO₂) are paramagnetic (S = 5/2) and [OEOPFe^II(CF₃SO₃)] (4) is also paramagnetic (S = 2).     

Zum chemischen Transport von Bismutoxidhalogeniden BiOX (X = Cl,Br, I) mit Halogen,Halogenwasserstoff sowie Wasser und Bestimmung der Molwärmen von BiOX

Chemical Transport of Bismuth Oxide Halides BiOX (X = Cl, Br, I) with X₂, HX and H₂O, and Determination of the Molar Enthalpies of BiOX By comparison of calculated and experimental chemical transport behaviour of BiOX (X = Cl, Br, I) with X₂, HX, and H₂O it was shown, that we understand the transport of BiOCl, BiOBr and BiOI with X₂ and HX in terms of the well known gaseous spezies in the systems. The existence of gaseous complexes Bi(OH)₂X is be concluded from high transport rates of BiOX with water, and their enthalpies and entropies were derived. The molar enthalpies and standard entropies of BiOX were determined by low temperature C_p measurements. (Data see Inhaltsübersicht)     

CsPr(CO3)2: Erste Einkristalle eines wasserfreien ternären Selten-Erd-Carbonats

CsPr(CO₃)₂: First Single Crystals of an Anhydrous Ternary Rare-Earth Carbonate For the first time, single crystals of CsPr(CO₃)₂ were obtained by thermolysis of Cs₂(H₃O)Pr(CH₃COO)₆ at 400°C under high CO₂ pressure (300 bar) in a steel autoclave. The crystal structure (triclinic, P1 , Z = 4, a = 860.2(3), b = 887.4(3), c = 892.6(3) pm, α = 98.56(2), β = 96.19(1), γ = 115.29(2)°, V_m = 90.03(6) cm³/mol, R = 0.033, R_w = 0.029) was determined from four-circle-diffractometer data. CsPr(CO₃)₂ forms an aragonite like layer structure. Layers containing Cs⁺ and Pr³⁺ in a 1 : 1 ratio are stacked in the fashion of the hexagonal closest packing in the [001] direction. They are separated through CO₃^2? ion layers. The Pr³⁺ ions are surrounded by 8 or 9 oxygen atoms, the coordination numbers of Cs⁺ are 11 and 12. The site symmetry of the CO₃^2? ions is C₁. All bands of the internal vibrations are observed in the IR spectrum. CsPr(CO₃)₂ decomposes above in 435°C to Cs₂CO₃ and Pr₂O₂CO₃.     

Pyridinium-functionalized metalloporphyrins as bifunctional catalysts for cycloaddition of epoxides and carbon dioxide

New pyridinium-functionalized metalloporphyrins MEtPpBr₄ (M = Zn²⁺, Co²⁺, Ni²⁺, Cu²⁺; EtPp = 5, 10, 15, 20-tetra(4-(3-(N-ethyl-4-pyridyl)pyrazolyl)phenyl)porphyrin) were synthesized as bifunctional catalysts for the cycloaddition reactions of epoxides and CO₂. The effects of catalyst loading, CO₂ pressure, reaction temperature and time on catalytic activity were investigated. ZnEtPpBr₄ ( 1 ) and CoEtPpBr₄ ( 2 ) exhibited efficient activities in the cycloaddition reactions of various epoxides with CO₂ as at 120 °C under 2 MPa of CO₂ pressure without solvent. Most of corresponding cyclic carbonates could be obtained in almost quantitative yields and > 99.9% selectivity with molar ratio of epoxide/catalyst 2222 after 8 hr of reaction.     

Matrix IR studies on hydrogen-bonded complexes of hydrogen chloride and hydrogen bromide with ketene

Infrared spectra of matrices codeposited Ar/HX (X=Cl, Br) with Ar/H₂CCO mixtures have been examined. Isotopic substitutions (HX, DX, H₂CCO, D₂CCO) showed that ketene formed the 1:1 hydrogen-bonded complex with HX. The HX stretching modes were observed at 2684 cm⁻¹ in the H₂CCO–HCl complex and at 2384 cm⁻¹ in the H₂CCO–HBr complex. The ν₁ modes of the ketene submolecules were shifted to low frequency and the ν₉ modes to high frequency. It was proposed for the structure of the complex that the acid proton is bonded to the C=C pi electron system.     

Formation of unsymmetrical cis-dialkyls of platinum(II) from platinum(II) hydroxo-complexes

The (hydroxo) methyl complex Pt(OH)(CH₃)(Diphos) [Diphos = Ph₂PCH₂CH₂PPh₂] reacts with compounds containing acidic CH bonds (HX) to give unsymmetrical cis-dialkyls of general formula Pt(CH₃)X(Diphos) [X = CH₂COCH₃, CH(COCH₃)₂, CH₂CN or CH₂NO₂]; both the methyl and the cyclohexenyl complexes Pt(OH)R(Diphos) (R = CH₃ or C₆H₉) insert carbon monoxide to give hydroxycarbonyl complexes PtR(CO₂H)(Diphos) which are remarkably stable to decomposition by β-elimination.     

Extraction of certain actinide and lanthanide elements from different acid media by polyurethane foams loaded with di-(2-ethylhexyl)phosphoric acid (HDEHP)

The effect of added TBP on the extraction of uranium(VI) with a solution of di-(2-ethylhexyl)-phosphoric acid (HDEHP) in o-dichlorobenzene from nitric acid solutions has been investigated at varying concentrations of nitric acid, HDEHP, TBP and uranium(VI). The mechanism of the synergistic effect of TBP is discussed on the basis of the results and can be summarized in the following equation: UO _2(aq) ²⁺ +0.67(HX)_3(o)+2TBP_(o)UO₂X₂·2TBP_(o)+2H _(aq) ⁺ where HX denotes HDEHP and the HDEHP loaded on the foam is trimerized.     

Low-pressure collisional narrowing in CO2

We report the observation of collisional narrowing of the Q branch of the Raman spectrum for the (000) → (100) transition in CO₂ at very low pressures. The minimum linewidth is reached at ≈250 Torr. An estimate for the difference in rotational constants of the (100) state and the ground state is obtained. The narrowing of the linewidth and the changes in line-shape are interpreted in terms of velocity changing collisions and rotationally inelastic collisions between the CO₂ molecules.     

基于TiO2的绿色多相催化剂催化CO2与环氧化合物偶联反应

金属离子掺杂纳米TiO2(M-TiO2,M=Zn2+,Cu2+,Co2+,Mn2+,Ni2+)在CO2与环氧化合物的偶联反应中表现出较高的催化活性.反应以四正丁基碘化铵(TBAI)为共催化剂,在无溶剂条件下进行.考察了反应温度、反应时间和CO2压力在Zn-TiO2/TBAI体系中对反应性能的影响.作为无毒的多相催化剂,Zn-TiO2可循环使用5次,其催化活性没有明显降低.