Iodination of B12H11OC(O)CH2–3, B12H11OH2–, and B12H11SCN2–

Reactions of iodination of monosubstituted derivatives of B₁₂H₁₁X^2–anion (X = OC(O)CH₃, OH, SCN) were studied. The reactions were shown to proceed smoothly to give B₁₂H₁₀(OC(O)CH₃)I^2–((carboxy)(iodo)[decahydro[I _h1551-²⁰-closo]dodecaborate(2–)] anion), B₁₂H₁₀(OH)I^2–((hydroxo)(iodo)[decahydro[I _h1551-²⁰-closo]dodecaborate(2–)] anion), and B₁₂H₁₀(SCN)I^2–((thiocyanato)(iodo)[decahydro[I _h1551-²⁰-closo]dodecaborate(2–)] anion) in high yields, irrespective of the solvent used (benzene, H₂O–ROH, where R = C₂H₅, CH₂CH₂CH₃).¹     

Structure, stability and dissociation of silanitriles RSiN (R = H2B, H2N, H2P)

Structure, stability, and dissociation of H₂BSiN, H₂NSiN, H₂PSiN and their isomers H₂BNSi, H₂NNSi, H₂PNSi have been studied in detail using ab initio MP2 and CCSD(T) methods. After dissociation of H₂BNSi, H₂NNSi, H₂PNSi and their isomers, the fragmented atoms have been considered to be either in their ground state or in their valence excited state in various dissociation channels. Only allowed dissociations of these molecules are considered. Various dissociation channels of H₂BNSi, H₂NNSi, H₂PNSi and their isomers have been explored and interesting trends are observed for the dissociation of stable isomers H₂BNSi, H₂NNSi, H₂PNSi and less stable isomers H₂BSiN, H₂NSiN, H₂PSiN. The effect of substituents on their structural properties has been discussed. The potential energy surfaces for the RSiN ? RNSi isomerization reactions have been analyzed. The structural properties of these molecules agree well with the theoretical values wherever available.     

Synthesis, IR spectra, and solid-state luminescence of triphenylguanidinium salts with the anions B10H 10 2− , B12H 12 2− , B9C2H 12 2− , [Co(C2B9H11)2]−, and [Ni(C2B9H11)2]−

Triphenylguanidinium Ph₃GH⁺ salts with the anions B₁₀H ₁₀ ^2? , B₁₂H ₁₂ ^2? , B₉C₂H ₁₂ ^2? , [Co(C₂B₉H₁₁)₂]^?, and [Ni(C₂B₉H₁₁)₂]^? were synthesized and described by DTA, IR spectroscopy, and solid-state luminescence. By IR spectroscopy, it was shown that intermolecular interactions involving the NH groups of the cation are enhanced in the sequence [Co(C₂B₉H₁₁)₂]^? ～ [Ni(C₂B₉H₁₁)₂]^? < B₉C₂H ₁₂ ^2? < B₁₂H ₁₂ ^2? < B₁₀H ₁₀ ^2? .     

Theoretical study of dodecahydro-closo-decaborane B10H12, the diprotonated boron cluster B10H 10 2−

The electronic and geometric structures of different isomers of the closo-B₁₀H₁₂ boron cluster have been calculated by the density functional theory method (in the B3LYP/6-311++G**//B3LYP/6-31G* approximation). The compound is considered to be the diprotonated (H*) analogue of the well-studied B₁₀H ₁₀ ^2? anion and serves as a model system. The increase in the relative energies of isomers and the preferred location of the extra H* protons near the opposite B(1) and B(10) “poles” are consistent with the charge separation (in the framework of the Mulliken population analysis) between B(1) and B(10). The reactions of migration of one or simultaneously two H* protons in B₁₀H₁₂ over the boron polyhedron have been considered, and the corresponding energies of elementary events E and activation barriers h have been estimated. The elementary events have been predicted in which both H* protons simultaneously move along the trajectories near the opposite B(1) and B(10) poles of the B₁₀H ₁₀ ^2? polyhedron with the same or opposite changes in the angles determining the H* position with respect to the B(1)–B(10) axis. The activation barrier to the “opposite” migration of the H* protons has been assessed to be h ～ 1.2 kcal/mol, whereas for the migration of the H* protons in the same direction, h ～ 1.4 kcal/mol. The H* proton transfer from the position near the B(1) pole to the position near the opposite B(10) pole is hindered, and higher activation barriers on the order of h ～ 13–15 kcal/mol should be overcome for this transfer to occur.     

Separation of 18α(H)-, 18β(H)-oleanane and lupane by comprehensive two-dimensional gas chromatography

18α(H)-, 18β(H)-oleanane and lupane are angiosperm-derived biomarkers that are used as age indicators for the Late Cretaceous onwards when the first proliferation of angiosperms occurred. In addition, the 18α(H)-/18β(H)-oleanane ratio is employed as a thermal maturity parameter of crude oil. However, evidence has shown that accurate quantification of these compounds has been impeded by inadequate chromatographic separation by traditional one-dimensional gas chromatography. In this study, we present the separation of 18α(H)-, 18β(H)-oleanane and lupane with comprehensive two-dimensional gas chromatography (GC×GC). Furthermore, it was observed that 18β(H)-oleanane elutes earlier than 18α(H)-oleanane in second dimension (polarity) which we attribute to steric hindrance effects. Two GC conditions have been developed in order to achieve baseline separation of the triterpenoids of interest in complex mixtures such as sediment extracts and crude oils.     

NH2SO3H and H6P2W18O62 · 18H2O-Catalyzed,Three-Component,One-Pot Synthesis of Benzo[c]acridine Derivatives

We report here two simple methods for the synthesis of benzo[c]acridine derivatives from three-component, one-pot condensation of 1-naphthylamine, dimedone, and a variety of substituted aldehydes in the presence of a catalytic amount of NH₂SO₃H or H₆P₂W₁₈O₆₂ · 18H₂O under solvent-free conditions at 120 °C or in refluxing ethanol.     

B…HY/BrY(B=C4H4,C6H6,Y=F,Cl,Br)分子间作用的电子密度拓扑研究

运用MP2/aug-cc-pVDZ对B…HY氢键复合物和B…BrY卤键复合物(B=C4H14,CdH6,Y=F,Cl,Br)的几何构型及相互作用能进行了研究.研究发现对于相同的路易斯碱来说,B…HY和B…BrY的几何构型非常类似,B…BrY卤键键能大于B…HY氢键键能.电子密度拓扑分析表明C4H4(S)…BrY,C4H4(T).…BrF之间的卤键作用介于离子键和共价键之间,其余的氢键和卤键作用均为闭壳层相互作用.形成氢键和卤键后,卤化氢和双卤分子的原子积分性质都发生了变化,B…HY中H原子能量增加,而B…BrY中Br原子能量减少.     

H6P2W18O62·18H2O–Catalyzed,Three-Component,One-Pot Synthesis of Indeno[1,2-b]quinoline-7-one Derivatives

In this work, a rapid and efficient one-pot method for the synthesis of indeno[1,2-b]quinoline-7-one derivatives by condensation of 1-naphthylamine, 1,3-indanedione, and different aldehydes in the presence of H₆P₂W₁₈O₆₂·18H₂O as a green and reusable catalyst in refluxing acetic acid is described.     

Fusopoltides B–E,new polyketides isolated from Fusarium solani B-18

Four new polyketides, fusopoltides B–E, were isolated, along with four known compounds, from Fusarium solani B-18 cultured on brown-rice. Fusopoltide B is a diastereomer of its co-isolated known compound, fusopoltide A, featuring a pentaleno[1,2-c]pyran ring system. Fusopoltide C and fusopoltides D–E are incorporated the first natural polyketides featured decahydro-pentaleno[1,2-c]pyran and pentaleno[1,2-c]furan ring systems, respectively. The structural assignments were established using comprehensive spectroscopic techniques, the modified Mosher's ester method, and electronic circular dichroism (ECD) calculations.     

Ih对称性硼,碳原子簇化合物的从头计算（I）：B32,C2B30B32H…

本文用从头计算方法研究了含３２个顶点的硼烷Ｂ３２Ｈ３２＾０＾．＾２＾－及裸原子簇Ｂ３２与Ｃ２Ｂ３０的构型，稳定性及反应活性，Ｂ３２的优化计算结果表明，１２个５配位与２０个６配位两类硼原子不在同一球面时最稳定，而且所含两种Ｂ－Ｂ核间距离（Ｒ５６，Ｒ６６）的优化值验证了Ｌｉｐｓｃｏｍｂ的经验数值，Ｂ３２，Ｂ３２３２＾２＾－电子结构及原子布居的计算表明骨架成键轨道满足Ｗａｄｅ规则。相应的计算还表明，中性     

B,B′-Bis(borazyl)- und B,B′-Polyborazylenderivate

Zusammenfassung B-Chlorborazole reagieren mit Alkalimetallen unter Kondensation. Aus Monochlorborazolderivaten entstehen so B,B-Biborazyle, aus Dichlorborazolen B,B-Polyborazylene und aus Trichlorborazolen vernetzte Polymere von guter thermischer Beständigkeit.Mit 3 AbbildungenHerrn Prof. Dr.F. Halla zum 80. Geburtstag gewidmet.     

B2H6分子中的化学键

在结构化学的教学中,常常要讨论二硼烷(B2H6)等“缺电子分子”的几何结构和化学键的性质.二硼烷的几何结构已早有定论,因为无论是它的化学性质,还是包括电子衍射、核磁共振、X-射线在内的广泛物理化学研究,都表明两个硼原子与四个端氢原子共平面,另外两个氢原子在平面的上下(如图所示).而且,该分子结构中存在三中心双电子化学键也为大家普遍接受.然而,关于B2H6分子中三中心化学键的解释在教科书中却各持己见,甚至同一本书中有两种不同的观点[1].     

Reactivity of the Ge–H,Sn–H,P–H,and Se–H Bonds in Radical Abstraction Reactions

The experimental data for the liquid- and gas-phase reactions of atoms and radicals with organoelement compounds R _{n – 1}E–H

Self-association-driven transition of the β-peptidic H12 helix to the H18 helix

Various patterns of foldameric oligomers formed by trans-ABHC ((1S,2S,3S,5S)-2-amino-6,6-dimethylbicyclo[3.3.1]heptane-3-carboxylic acid) and β(3)-hSer residues were studied. NMR, ECD and molecular modelling demonstrated that octameric and nonameric sequences with multiple i-i+3 ABHC pair repulsions attain the β-H18 helix in CD(3)OH. As a close relative of the α-helix, this helix type is stabilized by i-i+4 backbone H-bond interactions. The formation of the β-H18 helix was found to be solvent- and concentration-dependent. Upon dilution, the β-H18 → β-H12 helix transition was revealed by concentration-dependent ECD, DOSY-NMR and TEM measurements.     

11B-11B cosy NMR studies of derivatives of the octahydrotriborate anion, [B3H7(X)]− and [B3H6(X)2]−

2-D ¹¹B-¹¹B correlation (COSY) spectra have been obtained on the series of monosubstituted and disubstituted octahydrotriborate anions, [B₃H₇(X)]⁻ (X = Cl, NCS, NCSe, NCBH₃, NCBH₂Cl, NCBPh₃, NCBH₂CN, NCB₃H₇ or CNB₃H₆Cl) and [B₃H₆(Cl)(X)]⁻ (X = Cl, NCS, NCBH₂Cl or NCB₃H₇). All monosubstituted derivatives and [B₃H₆(Cl)₂]⁻ showed a coupling correlation between the substituted and unsubstituted borons. The unsymmetrically disubstituted derivatives showed only one coupling correlation, between the borons carrying the substituents. The absence of other correlations is attributed to relaxation phenomena. The correlations are independent of the solid-state structural type.     

Gas-phase solvation of Cl− with H2O,CH3OH,C2H5OH,i-C3H7OH,n-C3H7OH,and t-C4H9OH

The gas-phase clustering reactions Cl⁻ (ROH)n−1 + ROH ⇄ Cl⁻ (ROH)_n with n ⩽ 11 for ROH = H₂O, CH₃OH, C₂H₅OH, i-C₃H₇OH, n-C₃H₇OH, and t-C₄H₉OH were measured using a high-pressure mass spectrometer. It seems likely that for CH₃OH and C₂H₅OH, six ligands complete the shell structure and that ligands with n ⩾ 7 belong to the outer shell. The bond energies D(ROH---Cl⁻) increase in the order H₂O < CH₃OH < C₂H₅OH < i-C₃H₇OH < t-C₄H₉OH < n-C₃H₇OH. The observed strong bond of n-C₃H₇OH---Cl⁻ may be due to the fact that both the acidic hydrogen atoms in the −OH and terminal −CH₃ of n-C₃H₇OH interact with Cl⁻ with the most favorable configuration. For Cl⁻ switching reactions, Cl⁻ (H₂O)_n + (ROH)_n ⇄ Cl⁻ (ROH)_n + (H₂O)_n, the ΔG⁰_n values converge to the values of free energies of transfer of Cl⁻ from water to ROH solvent ( = ΔG⁰_n with n → ∞) with n ≈ 7. The observed convergence of ΔG⁰_n is due to compensation of changes in enthalpy and entropy, i.e. both ΔH⁰_n and TΔS⁰_n show increasing divergence from the values of enthalpies and entropies of transfer of Cl⁻ from water to ROH solvent, respectively, with n = 1 → 7. This is due to the stronger interactions of ROH with Cl⁻ than that of H₂O in the inner shell of Cl⁻ (ROH)_n at the expense of the less favorable entropy changes (less freedom of motion for ligands in the inner shell).     

Theoretical study on tetranuclear boron clusters: B4X4 (X = H, F, Cl, Br, I)

The molecular orbitals for B4H4, B4F4, B4Cl4, B4Br4 and B4I4 have been calculated by using all-electron or effective core potential ab initio method at the self-consistent field level using basis sets with diffuse and polarization functions. The boron-boron and boron-halide (-hydrogen) distances of these cage compounds are optimized with three kinds of basis sets constrained to a tetrahedral symmetry. According to the localization scheme of Boys, four three-centered two-electron (3c2e) B-B-B bonds localized on each of the faces of the B4 tetrahedron are derived for B4X4 clusters. The HOMO-LUMO energy gaps, atomization energies and Mulliken overlap populations of these compounds indicate that the stabilities of the clusters decrease in the sequence of B4F4 > B4Cl4, B4H4 > B4Br4 > B4I4.     

Structural, spectroscopic, electrochemical and computational studies of C,C′-diaryl-ortho-carboranes, 1-(4-XC6H4)-2-Ph-1,2-C2B10H10 (X = H, F, OMe, NMe2, NH2, OH and O−)

The influence of aryl ring substituents X (F, OMe, NMe₂, NH₂, OH and O⁻) on the physical and electronic structure of the ortho-carborane cage in a series of C,C′-diaryl-ortho-carboranes, 1-(4-XC₆H₄)-2-Ph-1,2-C₂B₁₀H₁₀ has been investigated by crystallographic, spectroscopic [nuclear magnetic resonance (NMR), UV–vis], electrochemical and computational methods. The cage C1–C2 bond lengths in this carborane series show small variations with the electron-donating strength of the substituent X, but there is no evidence of a fully evolved quinoid form within the aryl substituents in the ground state. In the ¹¹B and ¹³C NMR spectra, the ‘antipodal’ shift at B12, and the C1 shift correlates with the Hammett σ _p value of the substituent X. The UV–visible absorption spectra of the cluster compounds show marked differences when compared with the spectra of the analogous substituted benzenes. These spectroscopic differences are attributed to variation in contributions from the cage orbitals to the unoccupied/virtual orbitals involved in the transitions responsible for the observed absorption bands. Electrochemical studies (cyclic and square-wave voltammetry) carried out on the diarylcarborane series reveal that one-electron reduction takes place at the cage in every case with the voltage required for reduction of the cage influenced by the electron-donating strength of the substituent X, affording a series of carborane radicals with formal [2n + 3] electron counts. Electronic supplementary material  The online version of this article (doi:) contains supplementary material, which is available to authorized users.     

On the validity of the Buckingham-liu rule for water-dimer isotopomers AOB.OXY (A ≠ B; A,B, X,Y=1H,2D,3T)

Using 8 modifications of recently developed flexible water potentials, zeropoint energy differences between the isomeric water-dimer isotopomers differing in the hydrogen isotope involved in the hydrogen bond have been evaluated. In all the 18 possible pairs, the species bound through the heavier isotope is always lower in the energy term.Dedicated to the memory of the late Dr. Mojmír Tomáek (1931–1990).Part LVII in the series Multi-Molecular Clusters and Their Isomerism, Part LVI — see Ref. 42; for a wider perspective of the water-dimer isotopomeric isomerism — see⁴³Part XXXVI.     

Critical temperatures,pressures, and densities for the mixtures CO2–C3H8, CO2–nC4H10, C2H6–C3H8, and C3H8–nC4H10

A simple method is developed to estimate mixture critical temperatures (T_c), pressures (P_c), and densities (ρ_c) as a function of overall composition (X) from near critical region experimental coexistence data. This three-step method is applied to four mixtures, CO₂–C₃H₈, CO₂–nC₄H₁₀, C₂H₆–C₃H₈, and C₃H₈–nC₄H₁₀. Isothermal liquid–vapor coexistence data, which includes temperature, vapor pressure, coexisting densities (ρ^ℓ and ρ^v), and coexisting compositions for the more volatile component (x₁^v and x₁^ℓ) are used. In the first step, the difference of the saturated liquid and vapor densities (ρ^ℓ−ρ^v) is fitted to an empirical function in ((P_c−P)/P_c) to obtain P_c. Then P/P_c and ((ρ^ℓ+ρ^v)/2ρ_c) are simultaneously fitted to functions of a polynomial in (X₁−(x₁^v+x₁^ℓ)/2) yielding estimates of ρ_c and X₁. Finally, the discrete estimated critical data points are fitted with an equation to provide a continuous representation of the critical lines. The method is successfully tested for the mixtures, CO₂–C₃H₈ and CO₂–nC₄H₁₀, for which there is a reasonable amount of isothermal data. The procedure is then applied to the mixtures, C₂H₆–C₃H₈ and C₃H₈–nC₄H₁₀, for which there are sparse data. For all four mixtures, the critical temperature line, T_c vs. X₁, matches literature values within ±0.5%. The critical pressure line, P_c vs. X₁, and critical density line, ρ_c vs. X₁, match literature values, in general, within ±2%.