On the molecular structure of (CH3)2NSO2N(CH3)2 as studied by gas electron diffraction

The following bond lengths and bond angles have been deduced from a vapour phase electron diffraction study of (CH₃)₂NSO₂N(CH₃)₂: r(C-H) 1.114 ± 0.005 Å, r(S-O) 1.432 ± 0.010 Å, r(N-C) 1.475 ± 0.013 Å, r(S-N) 1.651 ± 0.003 Å, ∠N-C-H 109.3 ± 2.0°, ∠C-N-C 118.0 ± 302°, ∠S-N-C 115.2 ± 1.1°, ∠N-S-N 110.5±1.3° and ∠O-S-O 114.7±2.5°. The sulphur bond configuration and the prevailing conformation, which was identical to that in the crystal, are discussed in relation to analogous sulphide and sulphoxide derivatives.     

Electron diffraction study and CNDO/2 calculations on the complex of aluminium trichloride with ammonia,Cl3Al.NH3

The molecular geometry of the complex of aluminium trichloride with ammonia, Cl₃Al.NH₃, has been studied by electron diffraction. The most important internuclear distances in terms of r_a parameters are as follows: r(Al-Cl) = 2.100±0.005 Å, r(Al-N) = 1.996±0.019 Å, r(Cl·Cl) = 3.569±0.011 Å and r(Cl·N) = 3.165±0.012 Å. The Cl-Al-Cl bond angle in terms of an approximate r_a structure is 116.9°. The assumptions of a staggered model in the structure analysis was justified by CNDO/2 calculations. The experimental data indicate strong linkage between the donor and acceptor parts. The flat pyramidal average configuration of the AlCl₃ part of the complex suggests planar equilibrium structure for free AlCl₃. Variations in the bond configurations of the donor and acceptor parts, as compared with those of the respective free molecules, are discussed.     

The molecular structure of selenium oxychloride as studied by electron diffraction

The molecular geometry of selenium oxychloride has been studied by electron diffraction. The internuclear distances (in terms of r_a) are: r(Se-O) 1.612 ± 0.005 Å, r(Se-Cl) 2.204 ± 0.005 Å, r(Cl β O) 3.064 ± 0.012 Å, r(Cl β Cl) 3.295 ± 0.016 Å. The bond angles are ∠Cl-Se-O 105.8 ± 0.7° and ∠ Cl-Se-Cl 96.8 ± 0.7°. The structural parameters of three simple selenium-oxygen compounds are compared with those of their sulphur analogs in terms of the valence shell electron pair repulsion model.     

The thermal dissociation of the [Co(NH3)6]Cl3 and [Co(NH3)6]Br3 complexes in vacuo

The thermal dissociation of the complexes, [Co(NH₃)₆]X₃(X^?=Cl, Br), was studied in vacuo using the techniques of thermogravimetry, evolved gas analysis and mass spectrometric analysis. It was found that the reaction stoichiometry was identical to that previously determined in air but that the type of intermediate compounds formed were different. The dissociation occurred by the reactions:

     

Molecular structures of (SiCl3)2CH2 and (SiCl3)2CCl2 as studied by electron diffraction

An electron diffraction analysis of the molecular structures of 1,1,1,3,3,3-hexachloro-1,3-disilapropane and octachloro-1,3-disilapropane has been carried out. Deviations from the staggered conformation are indicated. The data may be approximated by models with C₂ symmetry and a small tilt of the SiCl₃ groups. The main bond lengths (r_g) and bond angles obtained for (SiCl₃)₂ CH₂ are: SiCl, 202.7(4); SiC, 186.6(6); CH, 109.8(24) pm, ClSiCl, 107.9(1); SiCSi, 118.3(7)°; and for (SiCl₃)₂CCl₂: SiCl, 202.0(4); SiC, 190.2(9); CCl, 179.6(9) pm; ClSiCl, 109.5(1); SiCSi, 120.6(9); ClCCl, 110.9(16); SiCCl, 106.3(3)°.     

Conformation and geometry of 2-thiophenesulphonyl chloride as studied by electron diffraction

The molecular conformation of 2-thiophenesulphonyl chloride is characterized by the perpendicular arrangement of the plane of the five-member ring and the CSCl plane, according to electron diffraction data. The sulphur bond configuration in the sulphonyl chloride moiety is consistent with the structural variations observed in a series of sulphonyl chlorides.     

The gas-phase molecular structure of CF3HgCH3 - an electron diffraction and microwave study

The molecular structure of CF₃HgCH₃ in the gas phase is determined by a joint analysis of electron diffraction and microwave data. The following geometric parameters (r_av values) are derived: r(Hg—CH₃) = 2.052(5) Å, r(Hg—CF₃) = 2.116(4) Å. r(C-F) = 1.354(2) Å. r(C—H) = 1.079(14) Å, ∠.FCF = 105.7(0.2)° and ∠HCH = 107.0(1.5)°. Error limits are twice the standard deviations.     

X-ray diffraction study of [Ru(NH3)5Cl][ReCl6] and [Ru(NH3)5Cl]2[ReCl6]Cl2 and their thermolysis products. Crystal-chemical analysis of the Ru-Re system

Binary complex salts [Ru(NH₃)₅Cl][ReCl₆] and [Ru(NH₃)₅Cl]₂[ReCl₆]Cl₂ were synthesized and characterized. An X-ray diffraction analysis showed that they were isostructural with the previously obtained isoformula salts [Rh(NH₃)₅Cl][OsCl₆] and [Ir(NH₃)₅Cl]₂[PtCl₆]Cl₂, respectively. Thermolysis of these compounds under hydrogen and helium was studied. According to X-ray phase analysis data, bimetallic solid solutions Ru_0.67Re_0.33 and Ru_0.50Re_0.50 were the final products of thermolysis. Their unit cell parameters correspond to the characteristics of alloys with similar compositions. Original Russian Text Copyright ? 2009 by S. A. Martynova, K. V. Yusenko, I. V. Korolkov, I. A. Baidina, and S. V. Korenev __________ Translated from Zhurnal Strukturnoi Khimii, Vol. 50, No. 1, pp. 126–132, January–February, 2009.     

Collisional relaxation among rotational levels of NH3 studied by infrared-microwave double resonance

Double-resonance signals induced by molecular collisions are observed in 25 inversion transitions of NH₃. It is found that the collision-induced transitions do not necessarily occur in accordance with the dipole-type selection rule reported previously.     

The molecular structure of the complex trimethylaluminium dimethyl ether, (CH3)3AlO(CH3)2, determined by gas phase electron diffraction

The molecular structure of (CH₃)₃AlO(CH₃)₂ has been determined by gas phase electron diffraction. The main molecular parameters are AlC = 1.973(11), AlO = 2.014(14), OC = 1.436(3) Å, OAlC = 98.7(1.5), AlOC = 122.6 (0.5) and COC = 114.5(1.7)°. The OC bond distance and the COC valence angle are significantly larger than those in free dimethyl ether. The three valencies of the oxygen atom appear to lie in one plane. It is suggested that the planarity of the oxygen atom is due to across-angle repulsion Al?C(O).     

Phase transitions, structural changes and molecular motions in [Zn(NH3)4](BF4)2 studied by neutron scattering, X-ray powder diffraction and nuclear magnetic resonance

Nuclear magnetic resonance (¹H NMR and ¹⁹F NMR) measurements performed at 90-295 K, inelastic incoherent neutron scattering (IINS) spectra and neutron powder diffraction (NPD) patterns registered at 22-190 K, and X-ray powder diffraction (XRPD) measurements performed at 86-293 K, provided evidence that the crystal of [Zn(NH₃)₄](BF₄)₂ has four solid phases. The phase transitions occurring at: T_C3=101 K, T_C2=117 K and T_C1=178 K, as were detected earlier by differential scanning calorimetry (DSC), were connected on one hand only with an insignificant change in the crystal structure and on the other hand with a drastic change in the speed of the anisotropic, uniaxial reorientational motions of the NH₃ ligands and BF₄⁻ anions (at T_C3 and at T_C2) and with the dynamical orientational order-disorder process (“tumbling”) of tetrahedral [Zn(NH₃)₄]²⁺ and BF₄⁻ ions (at T_C1). The crystal structure of [Zn(NH₃)₄](BF₄)₂ at room temperature was determined by XRPD as orthorhombic, space group Pnma (No. 62), a=10.523 Å, b=7.892 Å, c=13.354 Å and Z=4. Unfortunately, it was not possible to determine the structure of the intermediate and the low-temperature phase. However, we registered the change of the lattice parameters and unit cell volume as a function of temperature and we can observe only a small deviation from near linear dependence of these parameters upon temperature in the vicinity of the T_C1 phase transition.     

The transition from spinel-type structure to rocksalt-type structure in the compound CdHo2S4, as observed by electron microscopy/diffraction

At a temperature above 1173 K the spinel-type structure of CdHo₂S₄ becomes unstable and gradually transforms into a rocksalt-type structure. During transition both Cd²⁺ and Ho³⁺ cations shift. Electron diffraction patterns obtained during transition show that the Cd, which shifted from a tetrahedral to an octahedral site, distorts the sulfur lattice. This distortion becomes visible as a modulation of the sulfur matrix. The modulation originally occurs in many crystallographic directions, however, upon annealing the 〈111〉 direction becomes preferred. Small domains of the high-temperature structure of CdHo₂S₄ appear to occur also in samples that were annealed well below 1173 K for a long period.     

Evidence for two light-induced metastable states in Cl3[Ru(NH3)5NO]H2O

Differential Scanning Calorimetry measurements on irradiated Cl₃[Ru(NH₃)₅NO]H₂O reveal the existence of two light-induced long-lived metastable states SI, SII. Irradiation with light in the spectral range 400–500 nm leads to the excitation of SI. For the first time we report experimental evidence for the state SII in this compound, which can be excited by transferring SI into SII with irradiation of light in the spectral range 1000–1200 nm. The excitation and transfer of the metastable states is described and the exponential decays are evaluated according to Arrhenius' law yielding activation energies of E_A(SI)=0.73(3) eV, E_A(SII)=0.66(3) eV and frequency factors of Z(SI)=1 × 10¹² s⁻¹, Z(SII) = 5 × 10¹² s⁻¹.     

Mössbauer spectroscopy of 57Fe in NH4MnCl3, NH4FeCl3 and NH4CoCl3

The Mössbauer spectra of ⁵⁷Fe doped NH₄MnCl₃ reveal that this compound undergoes a crystallographic phase transition at 258°K and becomes magnetic at 105°K. No crystallographic transition appeared either in NH₄FeCl₃ or in ⁵⁷Fe:NH₄CoCl₃; the latter orders magnetically around 27°K.     

Molecular structure of Pt(PF3)4 by gas-phase electron diffraction

The structure of Pt(PF₃)₄ was reinvestigated making use of a new theory of intramolecular dynamic scattering. Derived molecular parameters were insensitive to the dynamic corrections. Refinements for this tetrahedral molecule yielded r_g(Pt-P) = 2.229(5) Å, r_g(P-F) = 1.550(4) Å, and ∠PtPF = 118.9°(0.4), with the indicated uncertainties representing 2.5σ. Amplitudes of vibration were also determined. Diffraction patterns were consistent with freely rotating PF₃ groups.     

The molecular structure of di-t-butylamine, NH[C(CH3)3]2, as determined by gas-phase electron diffraction: an exceptionally sterically hindered amine

Gaseous di-t-butylamine, NHBu^t₂, has been studied by electron diffraction at a nozzle temperature of ca. 293 K. The diffraction data reveal that this amine is exceedingly hindered. Repulsive steric interactions between the Bu^t groups are mainly relieved by an opening of the CNC valence angle to 135(3)°. Evidence of steric strain may also be found in the non-zero tilts (2–3°) of the Bu^t groups, defining the angle of rotation of these groups about axes through the N-bonded carbon atoms orthogonal to the NC₂ plane. The N---C and C---C bonds, 1.467(13) and 1.561(6) Å, respectively, are on the other hand relatively unstrained. Other principal geometrical parameters are unexceptional: C---H = 1.103(10) Å, NCC = 111.3(1.5)° (mean value) and CCH = 106(2)°. The position of the N-bonded hydrogen atom relative to the NC₂ plane could not be determined. The torsional positions of the Bu^t groups, with respect to the N---C bonds, could not be derived from least-squares refinements. A large number of models with Bu^t groups in various fixed positions were considered; the best fit between the observed and theoretical intensity data was obtained with one Bu^t group being twisted 19° away from the position typified by one C---C bond of this group being anti to the remote N---C bond, and the other Bu^t group similarly twisted by 30°. When viewed along the N---C bonds, the Bu^t groups are twisted in the same direction. Viewed along the C(N)C axis, these groups come close to being staggered with respect to each other. The values of the above bond distances are those of r_a parameters. Parenthesized values denote error limits, being least-squares standard deviations multiplied by a factor of three.     

NH4F对NH3低温选择性催化还原NO的影响研究

制备了一种新的氟掺杂氧化钒/氧化钛催化剂,探讨了掺杂模式、制备方法对低温SCR活性的影响.结果显示,在120~240℃反应温度下,由溶胶法制得的氟掺杂于钒(F-V)模式下的催化活性最佳,通过与未掺杂催化剂(COM)对比可知,在210℃时,氟掺杂催化剂的活性提高了35%,并于240℃时NO的脱除率达到了98.6%.通过X射线衍射试验(XRD)、透射电子显微镜(TEM)、比表面积测试(BET)、光电子能谱分析(XPS)以及H_2程序升温还原(H_2-TPR)等表征技术显示氟掺杂引起催化剂SCR活性提升主要与催化剂活性成分的良好分散性、粒子尺寸减小、比表面积及孔容增大、更强的氧化还原能力有关.另外,通过试验研究表明,氟掺杂催化剂不仅提升了SCR活性,拓宽了活性温度范围,而且还增强了抗硫与抗水性能.     

Photo-assisted electron injection at a semiconductor—NH3 interface

Illumination of a p-type semiconductor—NH₃ interface (or heterojunction) with photons of energy greater than the semiconductor band gap causes electrons to be injected into the NH₃. There is no hole injection at a n-type electrode. Suggestions are made for the required energy levels in the liquid.     

Spectroscopic studies of the AlCl3 · NH3 complex

A normal coordinate analysis for the AlCl₃ · NH₃ complex is performed. Calculations for a hypothetical complex with a planar AlCl₃ ligand are included. A deviation from planarity is found in the realistic complex. Force fields for free NH₃ and AlCl₃ molecules are employed in the construction of an initial approximate force field. The theory of kinematic coupling is used to study the frequency shifts from free to complexed ligands. A final force field is developed so as to reproduce exactly a set of observed frequencies from the literature. Calculations on mean amplitudes and perpendicular amplitude correction coefficients are reported.     

The calculation of the molecular orbital parameters for the square coplanar Cu(NH3)2+4 cation in Cu(NH3)4PtCl4

The calculation of the molecular orbital parameters of the σ-bonding square-planar Cu(NH₃)²⁺₄ cation in Cu(NH₃)₄PtCl₄ is reported, involving metal—ligand and ligand—ligand overlap integrals. In order to obtain a reasonable correlation of the magnetic g- and A-values and the electronic transition energies it is necessary to use a Cu⁺ wavefunction to represent the radially expanded Cu²⁺ wavefunction in this complex.