Iron oxide particles in a perfluorosulfonate membrane

Particles of (α-Fe₂O₃ and α-FeOOH have been observed directly in ultrathin (～ 500 Å) sections of Nafion® perfluorosulfonate membranes by transmission electron microscopy, α-Fe₂O₃ is obtained by heating a membrane, previously exchanged with 0.2 M FeCl₃, in an autoclave with water at 150°C. The individual particles are roughly spherical, ～ 100 Å in diameter, but they are grouped together in clusters ranging from a few hundred angströms up to about 1000 Å in size, which are uniformly distributed across the membrane thickness. α-FeOOH is obtained by boiling the membrane in water and exchanging first in 0.2 M FeCl₃ and then in 0.2 M KOH. Well-separated acicular or blade-shaped crystallites up to 1000 Å long and about 100 Å across are observed; they become more numerous towards the membrane surfaces. Amorphous ferric hydroxide, obtained by treating an unboiled membrane in the same way, could not be observed directly.     

An electron diffraction investigation of the molecular structure of gaseous 2,3-dimethyl-2-butene

The gas phase molecular structure of 2,3-dimethyl-2-butene has been investigated by the electron, diffraction technique. The following structural parameters (r_a structure) have been obtained: CC = 1.336±0.004 Å; C-C = 1.505±0.002 Å; C-H = 1.092±0.003 Å; ∠CC-C = 123.4±0.4°; ∠C-C-H = 110.5±0.7°; methyl torsional angle CC-C-H = 31±3°. If local C_3v symmetry is assumed then a twist of 13 ±4° of the carbon skeleton is observed. This twist reduces to virtually 0° if no local symmetry is imposed on the methyl group. The twisted structure is in good agreement with that obtained by valence force-field calculations.     

Contributions on thermal behaviour and crystal chemistry of anhydrous phosphates. XIX. Tri-chromium(II)-bis-phosphate Cr3(PO4)2 (≙ Cr6(PO4)4) – A transition metal(II)-orthophosphate with new structure type

Deep blue-violet single crystals of hitherto unknown chromous orthophosphate have been obtained reducing CrPO₄ by elemental Cr at temperatures above 1050°C in evacuated silica ampoules (NH₄I or I₂ as mineraliser). The complex structure of Cr₃(PO₄)₂ (P2₁2₁2₁, Z = 8, a = 8.4849(10) Å, b = 10.3317(10) Å, c = 14.206(2) Å) contains six crystallographically independent Cr²⁺ per unit cell. Five of them are coordinated by four oxygen atoms which form a distorted (roof shaped) square plane as first coordination sphere at interatomic distances 1.96 Å ? d(Cr? O) ? 2.15 Å. Their coordination is completed by additional oxygen atoms (2 or 3) at distances 2.32 Å ? d(Cr? O) ? 3.21 Å. The sixth Cr²⁺ shows six-fold octahedral coordination with strong radial distortion (d(Cr? O): 1.97, 2.04, 2.15, 2.28, 2.29, 2.53 Å). The four different [PO₄] groups exhibit only minor deviations from ideal tetrahedral geometry (1.51 Å ? d(P? O) ? 1.57 Å, 104.3° ? ∠(O? P? O) ? 114.4°). An unusually low magnetic moment μ_exp = 4.28(2) μ_B (θ_P = ?54.8(5) K) has been observed for Cr²⁺.     

Darstellung und Strukturanalyse von Natriumozonid

Synthesis and Crystal Structure Analysis of Sodium Ozonide Solutions of sodium ozonide in ammonia have been obtained starting from cesium ozonide via cation exchange in liquid ammonia. After addition of dimethyl amine and removing the solvent mixture pure sodium ozonide precipitates as a bright red microcrystalline powder. According to X‐ray powder data, NaO₃ is isotypical with NaNO₂ (I m2m; a = 3.5070(2) Å, b = 5.7703(3) Å, c = 5.2708(3) Å; Z = 2; Rietveld profile fitting, R_Int = 3.71%). The O–O‐distances (1.353(3) Å) are the longest observed so far in ionic ozonides, the angle of 113.0(2)° is the smallest. The frequencies of the fundamental vibrations of the ozonide anion as obtained by Infrared and Raman spectroscopy are shifted to higher wave numbers as the cation diameter is decreasing. Unlike the ozonides of the heavy alkalimetals NaO₃ represents a magnetically strongly coupled system (μ_eff = 1.45 μ_B at 250 K).     

Refinement of the Crystal Structure of Sr3Hg2

Mixtures of strontium and mercury in molar ratios of 7:3 have been annealed for 20 days at 520°C. From the pure product Sr₃Hg₂ single crystals have been obtained. Sr₃Hg₂ crystallizes in the U₃Si₂ type of structure (space group P4/mbm); the cell constants are a = 8.883 (2) Å and c = 4.553(1) Å. All of the Hg atoms are involved in Hg₂ dumbbells with Hg? Hg distances of 3.41 Å.     

Crystal and molecular structure of cis- and trans-2,4-dihydroxy-2,4-dimethylcyclohexanetrans-1-acetic acid γ-lactone

During the transformation process of limonene to tetrahydrofuran derivatives, the title compounds (±)-( 4 ) have been obtained as crystalline products and subjected to X-ray analysis. The crystals of trans-( 4 ) are orthorhombic, space group P2₁2₁2₁, with the lattice constants a = 7.0445(5) Å, b = 10.0908(4) Å, c = 14.0309(6) Å; the absolute configuration at atoms C1, C2, and C4 is R_c1, S_c2, and R_c4, respectively. The isomeric form cis-( 4 ) crystallizes in the monoclinic system, space group P2₁, with the following unit-cell parameters: a = 10.8275(4) Å, b = 8.6994(5) Å, c = 16.4722(6) Å, β = 106.515(3)°. The asymmetric part of the unit cell of cis-( 4 ) contains three independent molecules. Each of these three molecules has the identical absolute configuration at all centers of chirality: S_c1, S_c2, and R_c4. © John Wiley & Sons, Inc.     

Gas-phase electron diffraction studies of the molecular structures of pentafluoroethane,C2F5H,and monofluoroethane,C2H5F

The molecular structures of C₂F₅H and C₂H₅F have been studied using gas-phase electron diffraction data collected on the Balzers KDG2 instrument. The following values for the main independent geometrical parameters were obtained (r_a values with e.s.d. in parentheses): in C₂F₅H, C-C = 1.525(4) Å, C-F(CHF₂) = 1.347 Å, C-F(CF₃) = 1.327 Å [C-F(av.) = 1.335(2) Å], ∠CCF(av.) = 110.0(2)°; in C₂H₅F, C-C = 1.502(5) Å, C-F = 1.397(4) Å, C-H = 1.097(2) Å. ∠CCF = 110.4(2)°, ∠CCH(av.) = 113.6(4)°. Evidence is presented to show that the electron diffraction data for C₂H₅F are not compatible with values for the bond angles deduced spectroscopically.     

A new diaza‐18‐crown‐6 ligand containing two quinolin‐8‐ylmethyl side arms: Crystal structures and characterization of the ligand,the protonated ligand and its mononuclear barium(II) and dinuclear copper(II) complexes

A new 7,16‐bis(quinolin‐8‐ylmethyl)‐1,4,10,13‐tetraoxa‐7,16‐diazacyclooctadecane ligand, L, has been prepared and its crystal structure reported. In addition, the structure of the protonated ligand H₂L has been determined. H₂L is of interest because of interatomic interactions between the ligand and perchlorate ions. The mononuclear Ba(II) (Ba L ), and dinuclear Cu(II) (Cu₂L) complexes of L have been prepared and their crystal structures determined. Stability constants and other thermodynamic data valid in methanol at 23 or 25° for these and several other complexes of L have been obtained. Among the metal ions studied, L forms the most stable complex with Ba²⁺. In addition, L selectively binds Cu²⁺ over Ni²⁺ by about 3 orders of magnitude. Some of the complexes have been studied using nmr and uv‐vis spectroscopic techniques. Crystal data are given for L, space group, P2₁c, a = 8.8325(14) Å, b = 13.808(3) Å, c = 13.310(3) Å; β = 94.72(2)° Z=2, R = 0.0727; for H₂ L , space group, P2₁/c, a = 14.685(3) Å, b = 15.035(6) Å, c = 17.369(4) Å, β = 90.366(12)°, Z = 4, R = 0.0781; for Ba L , space group, Pbcn, a = 17.314(3) Å, b = 9.539(2) Å, c = 22.081(3) Å, Z = 4, R = 0.0354; and for Cu₂ L , space group, Cc, a = 19.762(2) Å, b = 14.413(2) Å, c = 14.935(2) Å, β = 98.753(12)°, Z = 4, R = 0.0564. Cu²⁺ forms a hydroxo‐bridged dinuclear complex with L while Ba²⁺ forms a mononuclear complex with L in which its two side arms are not involved in complexation.     

Die Kristallstrukturen und Phasentransformationen des tetramorphen RbGel3

Crystal Structures and Phase Transitions of the Tetramorphic RbGeI₃ The thermal behaviour of RbGeI₃ has been studied by X-ray diffraction, Raman spectroscopy, and DTA/DSC. The compound is tetramorphic. Yellow crystals of the LT-form have been obtained by crystallization from aqueous HI solutions. The orthorhombic crystal structure of LT? RbGeI₃ (space group P2₁2₁2₁; a = 10.1441(8) Å; b = 4.5460(5) Å; c = 16.8438(9) Å) shows a distorted NH₄CdCl₃ type structure with pyramidal GeI₃ anions. Three reversible phase transformations were found by heating. In a first step at 181°C LT? RbGeI₃ is transferred into the orthorhombic perovskite MT1—RbGeI₃ (red, space group Pn2₁a; a = 8.566(3) Å; b = 11.868(6) Å; c = 8.018(4) Å; RbGeBr₃ type structure) by a reconstructive phase transition. Subsequently at 221°C the phase MT2—RbGeBr₃ with a rhombohedrically deformed perovskite type structure (black, space group R3m; a = 5.990(2) Å; α = 88,89(3)°; CsGeCl₃ type structure) is formed. The high temperature modification HT? RbGeI₃ shows the cubic perovskite type structure (space group Pm3m; a = 5.994(3) (Å) and is stable above 244°C until decomposition occurs at 334°C.     

Methyl rotation in polydimethylsiloxane studied by neutron transmission

Neutron transmission of polydimethylsiloxane has been measured as a function of neutron wavelength in the range 4–10 Å, at room temperature. Scattering cross sections per hydrogen atom have been obtained and the slope (12.2 ± 0.2) barns/Å has been derived. Comparison with calibration curves relating the slope to the barrier hindering internal rotation as well as comparison with calculated neutron cross sections using the Krieger–Nelkin formalism for different dynamical situations indicates practically free rotation of CH₃ groups about their C₃ symmetry axes.     

Molecular structure of carbonyl fluoride as studied by gas electron diffraction and microwave data

The molecular structure of carbonyl fluoride has been determined by electron diffraction. The results have been used in conjunction with the rotational constants reported by Carpenter in a combined structure analysis. The values so obtained are r_z (C=O) = 1.1717 ± 0.0013 Å, r_z (C-F) = 1.3157 ± 0.0005 Å, and ∠_zF-C-F = 107.71 ± 0.08°. These agree with the corresponding parameters estimated by Carpenter from the rotational constants alone. The effective constants, α₃, representing the cubic anharmonicity of bond stretching vibrations have been estimated.     

The structure of cyclopentene oxide determined by gas phase electron diffraction

The r_g structure of cyclopentene oxide has been determined by the simultaneous least squares analysis of electron diffraction and microwave spectroscopic data. The investigation has reaffirmed previous studies indicating that the molecule prefers a boat conformation. The methylene and epoxide flap angles obtained are 152.3±2.1° and 104.7±1.0° respectively. Other structural parameters determined are: r_g (C-H avg.) = 1.120±0.004 Å; r_g (C-C avg.) = 1.538±0.002 Å; r_g (C-O) = 1.443±0.003 Å, and r_g (C-C) = 1.482±0.004 Å for the carbon-carbon bond in the three membered epoxide ring. These results compare favorably with the reported structures of ethylene oxide and cyclohexene oxide. A tentative rationalization of the unusual boat conformation is also offered.     

The molecular structure of 1,1,1-trimethoxyethane in the gas phase as determined by electron diffraction,molecular mechanics calculations and vibratio

The structure of 1,1,1-trimethoxyethane has been studied by electron diffraction in the gas phase. Although this technique cannot discriminate between a GGG (point symmetry C₃) and a TGG (C₁) conformation, vibrational spectra indicate that in the gas phase the C₁ conformer is predominant. Constraints necessary for a satisfactory leastsquares refinement were obtained from molecular mechanics calculations. The molecular geometry as obtained from r_α-refinements is as follows (r_g distances, r_α angles; standard deviations in parentheses): r(C-O central = 1.398 (6) Å, r(C-O)_terminal = 1.431(6)Å, r(C-C) = 1.527 (6) Å, r(C-H) = 1.114 (1) Å, ∠(C-O-C) = 114.0 (4)°, ∠(O-C-H) = 110.7 (4)°; the C-C-O and O-C-0 angles around the central carbon range between 106.6° and 113.1°.     

Photochemische reaktionen—XXXIII: Molekular- und kristallstruktur eines photoprodukts aus gibberelun C

In connection with studies concerning the photochemistry of carbonyl gibberellins, the structure of a ring D seco photoproduct 1 obtained upon UV irradiation of gibberellin C has been established by X-ray analysis and the molecular packing determined. The lattice parameters are a=b=11.935 Å and c=31.717 Å; the space group is P4₃2₁2. The final discrepancy factor R was 0.063.     

Electron diffraction study on the molecular structure of methane sulphonyl fluoride

The molecular structure of methane sulphonyl fluoride in the vapour state was studied by electron diffraction. Assuming a value of 2.480A?for the distance between the oxygen atoms from a microwave determination, the following geometrical parameters (r_a structure) have been obtained: r(C-H) = 1.093±0.010Å, r(S-O) = 1.410±0.003Å, r(S-F) = 1.561 ±0.004Å, r(S-C) = 1.759±0.006Å, ∠F-S-C = 98.2±1.5°, ∠-S-F = 106.2±0.4°, ∠-O-S-O = 123.1 ±1.5° and ∠H-C-H = 112.9±1.9°. All the observed variations in the molecular geometries of (CH₃)₂SO₂, CH₃SO₂Cl, CH₃SO₂F and SO₂F₂ may be accounted for by the valence shell electron pair repulsion theory. It is particularly advantageous to combine electron diffraction and microwave data in studying sulphone molecular geometries.     

Neue Alkalimetallchromchalkogenide und ihre Struktursystematik

New Alkali Metal Chromium Chalcogenides and their Structural Classification The compounds RbCr₃S₅, K₃Cr₁₁S₁₈, RbCr₅Se₈ and CsCr₅Se₈ could be obtained in the form of wellshaped crystals via fusion reactions of the alkali metal carbonates with chromium and the corresponding chalcogen. The compounds crystallize in the monoclinic space groups C2/m (RbCr₃S₅: a = 19.372(3) Å, b = 3.498(1) Å, c = 12.119(2) Å, β = 122.78(1)°, Z = 4; K₃Cr₁₁S₁₈: a = 41.876(3) Å, b = 3.463(1) Å, c = 16.315(3) Å, β = 150.07(1)°, Z = 2; RbCr₅Se₈: a = 18.737(2) Å, b = 3.623(1) Å; c = 9.016(1) Å, β = 104.65(1)°, Z = 2; CsCr₅Se₈: a = 18.795(2) Å, b = 3.637(1) Å, c = 9.104(1) Å, β = 104.52(1)°, Z = 2). We propose a structure classification from group-subgroup-relations. MAPLE calculations reveal that the reactions of the binary chalcogenides to yield the ternary compounds are exothermic in each case and are dependent on the chromium/alkali metal ratio in the ternary chalcogenides.     

A gas-phase electron-diffraction study of trvinylborane

Trivinylborane has been studied by standard electron-diffraction techniques. The best agreement with experiment is obtained with a planar dynamic model in which steric strain within the molecule is reduced by distortion of the vinyl groups, and shrinkages simulate considerable torsional motion about the B-C bonds. The following parameters (r_a basis) and e.s.d. were obtained: C-H = 1.092± 0.003 Å; C-C = 1.370 ± 0.006 Å; B-C = 1.558± 0.003 Å; ∠BCH = 116.5 ± 0.9 °; ∠BCC = 122.4 ± 0.9°; ∠CCH (trans to B) = 124.0 ± 1.6°; ∠CCH (cis to B) = 132.2 ± 2.3°. A static non-planar model has also been considered.The probable planarity of the molecule and the length of the C C bond are interpreted as evidence for π-electron delocalisation from carbon to boron.     

An electron diffraction study of 3-methyldiaziridine and 1,2-dimethyldiaziridine

The structures of the title compounds, diaziridines, (the first to be studied in the gas phase) have been determined by electron diffraction. The following principal structural parameters were obtained with the estimated standard deviations parenthesized: 3-methyldiaziridine, N-C = 1.489(9) Å, N-N = 1.444(13) Å, C-C = 1.505(16) Å, C-H = 1.107(5) Å, α =∠ (C-C, NCN) = 61.3° (0.9); 1,2-dimethyldiaziridine, (parameters of the cycle CN₂ were assumed from the previous molecule), N-C (methyl) = 1.445(3) Å, C-H = 1.108(9) Å, ∠ C-N-Me = 112.0° (0.5), the two methyl groups are in the trans position. Vibrational amplitudes were also determined for all important distances.     

Crystal structure refinement for trans-[Pd(NO3)2(H2O)2]

Single crystals of trans-[Pd(NO₃)₂(H₂O)₂] were obtained, and the crystal structure of this complex, previously obtained for polycrystals, was refined. Crystal data (BRUKER X8APEX diffractometer): a = 4.9973(7) Å, b = 10.5982(14) Å, c = 11.7008(17) Å, V = 619.70(15) ų, space group Pbca, Z = 4, d _calc = 2.856 g/cm³. The structure is composed of neutral complexes with a trans configuration. The square plane environment of the Pd atom is formed by four oxygen atoms (Pd-O(NO₃) 1.999(5) Å, Pd-O(H₂O) 2.030(5) Å) and completed to a distorted bipyramid by two intramolecular contacts (Pd…O(NO₃) 2.926 Å). The shortest hydrogen bonds are O…H 2.72 Å.     

Molecular structures of isobutene and 2,3-dimethyl-2-butene as studied by gas electron diffraction

The structures of isobutene and 2,3-dimethyl-2-butene have been studied by gas electron diffraction. For isobutene the rotational constants obtained by Laurie by microwave spectroscopy have also been taken into account. Leastsquares analyses have given the following r_g bond distances and valence angles (r_av for isobutene and r_α for dimethylbutene): for isobutene, r(CC) = 1.342±0.003 Å, r(C-C)= 1.508±0.002Å, r(C-H, methyl) = 1.119±0.007 Å, r(C-H, methylene) = 1.095±0.020 Å, ∠(C-CC) = 122.2±0.2°, ∠(H-C-H) = 107.9±0.8°, and ∠(C-C-H) 121.3±1.5°; for dimethylbutene, r(CC)= 1.353 ±0.004 Å, r(C-C) = 1.511±0.002 Å, r(C-H) = 1.118± 0.004 Å, ∠(C-CC)= 123.9±0.5°, and ∠(H-C-H)= 107.0±1.0°, where the uncertainties represent estimated limits of experimental error. The bond distances and valence angles in these molecules and in related molecules are compared with one another. The CC and C-C bond distances increase almost regularly with the number of methyl groups, and the C-C bonds in isobutene and dimethylbutene are shorter than those in acetaldehyde and acetone by about 0.01 Å. Systematic variations in the C-CC angles suggest the steric influence of methyl groups.