The coordination of the dimethylthallium ion in the crystal and molecular structure of 1,10-phenanthroline-dimethylthallium (III) perchlorate

1972 ◽  
Vol 331 (1585) ◽  
pp. 161-169 ◽  
Keyword(s):  
Molecular Structure ◽  
Crystal Structure ◽  
Single Crystal ◽  
Crystal And Molecular Structure ◽  
Pentagonal Bipyramid ◽  
Equatorial Position ◽  
Polymeric Structure ◽  
X Ray

A single crystal X-ray analysis of the crystal structure of [TlMe 2 1,10-phen]ClO 4 confirms the presence of a bent dimethylthallium group with a C-Tl-C angle of 168.3 (1.5)°. The thallium coordination is best described as a distorted pentagonal bipyramid with one equatorial position vacant. The equatorial bonds are predominantly electrostatic, and the perchlorate ions are bidentate giving rise to a polymeric structure in the crystal.

Crystal Structure of (NH4)2[Mo3S(S2)6] Containing the Novel Isolated Cluster [MO3S13]2-

1979 ◽  
Vol 34 (3) ◽  
pp. 434-436 ◽  
Author(s):  
A. Müller ◽  
S. Pohl ◽  
M. Dartmann ◽  
J. P. Cohen ◽  
J. M. Bennett ◽  
...  
Keyword(s):  
Molecular Structure ◽  
Crystal Structure ◽  
Aqueous Solutions ◽  
Single Crystal ◽  
Ammonium Salt ◽  
Crystal And Molecular Structure ◽  
Monoclinic Space Group ◽  
The Novel ◽  
Mean Values ◽  
X Ray

Abstract The novel tri-nuclear metal-sulfur cluster [Mo3S(S2)6]2- can be obtained as its ammonium salt by the reaction of a Moiv containing aqueous solutions with polysulfide. Its crystal and molecular structure has been determined by a single crystal X-ray study. The crystals are monoclinic (space group Cm, with a = 11.577(6) Å, b = 16.448(7) Å, c = 5.716(2) Å, β = 117.30(3)°, V = 967.2 Å3 , Z = 2, dexptl. = 2.54(2) g/cm3 , dcal = 2.54 g/cm3). The structure consists of isolated [Mo3S(S2)6]2- units, with three Mo atoms at the vertices of a triangle. There are bridging as well as terminal S22--ligands lying above and below the Mo3-plane (bond distances: Mo-Mo = 2.722 Å, Mo-S(terminal) = 2.435, Mo-S(bridging) = 2.452, Mo3-S = 2.353(4) Å and S-S = 2.04 Å (mean values)).

5-Allyl-9-oxobenzomorphans. Part 2. The Crystal and Molecular Structure of an Unusual Product of Dequaternization of 5-Allyl-9-oxobenzomorphan Methobromide

1975 ◽  
Vol 53 (21) ◽  
pp. 3276-3284 ◽  
Author(s):  
Farid R. Ahmed ◽  
Michel Saucier ◽  
Ivo Monković
Keyword(s):  
Molecular Structure ◽  
Crystal Structure ◽  
Single Crystal ◽  
Least Squares ◽  
Crystal And Molecular Structure ◽  
Heavy Atom ◽  
Methoxy Derivative ◽  
X Ray ◽  
Unusual Product ◽  
Single Crystal Analysis

The synthesis of 5-allyl-2'-methoxy-9-oxo-6,7-benzomorphan (5b) is described. The 10-hydroxy-2-methyl-1,11-propano-9H-indeno-1,2,10,11-tetrahydro[2,1-c]pyridine (7a) and the corresponding 6-methoxy derivative (7b) are unexpected products of pyrolysis of 5-allyl-2-methyl-9-oxobenzomorphan methobromide (4a) and 5-allyl-2′-methoxy-2-methyl-9-oxobenzomorphan methobromide (4b) respectively. The molecular structure of 7a (C16H19NO) has been determined from spectral and microanalytical data, and confirmed by X-ray single crystal analysis on its hydrobromide salt using the heavy atom technique. The crystals of [C16H20NO]+Br− are monoclinic, P21/a, with a = 13.724(2), b = 14.022(3), c = 7.495(2) Å, β = 97.33(5)°, and Z = 4. The crystal structure has been refined by block-diagonal least-squares calculations to R and Rw = 0.036 for the 2197 observed reflections. The N atom has planar trigonal coordination, and forms one double and two single C—N bonds of lengths 1.273(4), 1.465(4), and 1.474(4) Å, respectively. The Br is hydrogen-bonded to O. The N and O atoms are trans.

Adiponitrile at 100 K

2017 ◽  
Vol 73 (11) ◽  
pp. 937-940 ◽  
Author(s):  
Rüdiger W. Seidel ◽  
Richard Goddard ◽  
Nils Nöthling ◽  
Christian W. Lehmann
Keyword(s):  
Molecular Structure ◽  
Crystal Structure ◽  
Low Temperature ◽  
Single Crystal ◽  
Large Scale ◽  
Crystal And Molecular Structure ◽  
Monoclinic Space Group ◽  
Space Group ◽  
X Ray ◽  
Intermolecular Contacts

Adiponitrile, C6H8N2, is a key intermediate in the synthesis of the polyamide Nylon 66 and is produced industrially on a large scale. We have determined the crystal and molecular structure of adiponitrile by single-crystal X-ray analysis at 100 K, a suitable crystal (m.p. 275 K) having been grown from the melt at low temperature. The compound crystallizes in the monoclinic space group P21/c with Z = 2. In the crystal structure, the molecule adopts an exact C i-symmetric gauche–anti–gauche conformation of the C—C—C—C skeleton about an inversion centre. The molecules are densely packed, with short intermolecular contacts between the α-H and nitrile N atoms.

Studies of the rhenium–oxygen bond. II. The crystal and molecular structure of µ-oxobis(cis-dichloro-cis-di(pyridine)-trans-oxorhenium(V)), ORe(C5H5N)2Cl2ORe(C5H5N)2Cl2O

1978 ◽  
Vol 56 (2) ◽  
pp. 179-188 ◽  
Author(s):  
Colin James Lyne Lock ◽  
Graham Turner
Keyword(s):  
Molecular Structure ◽  
Crystal Structure ◽  
Single Crystal ◽  
Least Squares ◽  
Crystal And Molecular Structure ◽  
The Other ◽  
Full Matrix ◽  
X Ray ◽  
Ray Methods ◽  
Oxygen Bond

The crystal structure of µ-oxobis(cis-dichloro-cis-di(pyridine)-trans-oxorhenium(V)), ORe(C5H5N)2Cl2•O•Re(C5H5N)2Cl2O bas been studied by single crystal X-ray methods. The crystals were orthorhombic with lattice parameters a = 15.367(2), b = 10.283(2), c = 16.685(2) Å. The space group was Pna21 and there were four formula weights per unit cell. A total of 3339 reflections, of which 2990 were observed, were examined, and the structure refined by full matrix least squares (treating the pyridine rings as groups) to an R2 value of 0.0449. The dimer had a roughly rectilinear O—Re—O—Re—O backbone with pairs of chlorine atoms and pyridine molecules arranged cis in each half of the dimer. The two halves of the dimer were arranged such that the pairs of cis atoms in one half were rotated about the Re(1)–Re(2) axis almost 113 ° when compared to the corresponding pair in the other half. Important bond lengths (Re—O(terminal), 1.715(16), 1.764(16); Re—O(bridging), 1.943(16), 1.903(16); Re—Cl, 2.356(5)–2.390(5); Re—N, 2.116(16)–2.180(16)) were close to previously observed values. The molecule was markedly disturbed from the idealized structure and this was caused by intramolecular non-bonded interactions.

The crystal and molecular structure of (±)-('E')-N-Acetylpiperidine-2-carboxylic acid

1980 ◽  
Vol 33 (1) ◽  
pp. 215 ◽  
Author(s):  
ID Rae ◽  
CL Raston ◽  
AH White
Keyword(s):  
Molecular Structure ◽  
Crystal Structure ◽  
Carboxylic Acid ◽  
Single Crystal ◽  
Least Squares ◽  
Crystal And Molecular Structure ◽  
X Ray Diffraction ◽  
Space Group ◽  
X Ray

The crystal structure of N-acetylpiperidine-2-carboxylic acid has been determined by single-crystal X-ray diffraction methods at 295(1) K and refined by least squares to a residual of 0.039 for 846 'observed' reflections. Crystals are orthorhombic, with space group Pbca, a 13.684(6), b 11.602(4), c 11.171(4)Ǻ, Z 8. The ring is a chair structure in which, contrary to an earlier proposal based on 1H n.m.r. studies, there is almost perfect staggering about the C(2)-C(3) bond.

Notizen: Kristall- und Molekülstruktur von Bis (trimethylsilyl)amino-trimethylsilyliminophosphin bei —130 °C / Crystal and Molecular Structure of Bis (trimethylsilyl)amino-trimethylsilyliminophosphine at —130 °C

1977 ◽  
Vol 32 (11) ◽  
pp. 1344-1345 ◽  
Author(s):  
Siegfried Pohl
Keyword(s):  
Molecular Structure ◽  
Crystal Structure ◽  
Single Crystal ◽  
Phosphorus Atom ◽  
Crystal And Molecular Structure ◽  
Multiple Bond ◽  
X Ray ◽  
R Value

The crystal structure of R2N–P=NR (R = Si(CH3)3) was determined by single crystal X-ray data collected at —130 °C and refined to a conventional R-value of 0.029. The structure exhibits a two-connected phosphorus atom. The short P = N multiple bond (154.5 pm) indicates a 3pπ(P)—2pπ(Ν) interaction. The N–P–N angle was found to be 108.4°.

Studies of β-Diketone Complexes of Rhenium. VII. The Crystal and Molecular Structure of Oxodichloropentane-2,4-dionatotriphenylphosphinerhenium(V)

1975 ◽  
Vol 53 (11) ◽  
pp. 1548-1553 ◽  
Author(s):  
C. J. L. Lock ◽  
Che'ng Wan
Keyword(s):  
Molecular Structure ◽  
Crystal Structure ◽  
Single Crystal ◽  
Least Squares ◽  
Crystal And Molecular Structure ◽  
Rhenium Atom ◽  
Full Matrix ◽  
X Ray ◽  
Bonding Interaction ◽  
Ray Methods

The crystal structure of oxodichloropentane-2,4-dionatotriphenylphosphinerhenium(V) has been studied by single crystal X-ray methods. The crystals are triclinic with lattice parameters a = 11.023(8) Å, b = 13.523(8) Å, c = 9.360(7) Å, α = 90.2(1)°, β = 114.1(1)°, γ = 67.7(2)°. The space group is [Formula: see text] and there are two formula weights per unit cell. A total of 2891 reflections, of which 2447 were observed, were examined, and the structure was refined by full matrix least squares to an R2 value of 0.0782. The ligands are arranged around the rhenium atom such that the nearest six atoms are at the corners of a very distorted octahedron. Most of this distortion appears to be caused by nonbonding repulsive interactions. The short oxo–phosphine distance, 2.85(1) Å, suggests the possibility of a weak bonding interaction. Observed bond distances (Re—Cl, 2.35 Å av; Re—O(oxo), 1.69(1) Å; Re—O(diketone), 1.99(1), 2.10(1) Å; Re—P, 2.431(4) Å) are close to those observed previously in similar compounds.

The crystal and molecular structure of dipyrrolidylthiuram disulfide

1983 ◽  
Vol 36 (7) ◽  
pp. 1371 ◽  
Author(s):  
GA Williams ◽  
JR Statham ◽  
AH White
Keyword(s):  
Molecular Structure ◽  
Crystal Structure ◽  
Single Crystal ◽  
Least Squares ◽  
Dihedral Angle ◽  
Crystal And Molecular Structure ◽  
Structural Parameters ◽  
Monoclinic Space Group ◽  
X Ray Diffraction ◽  
X Ray

The crystal structure of dipyrrolidylthiuram disulfide has been determined by single-crystal X-ray diffraction techniques at 295 K. Crystals are monoclinic, space group C2/c, unit cell a 13.835(3), b 10.422(2), c 9.427(3) �, β 97.08(2)� and Z 4. Automatic diffractometry has provided significant Bragg intensities for 1402 independent reflections, and the structure has been refined by least-squares methods to R 0.037. The structure consists of discrete C4H8NC(S)S2C(S)NC4H8 molecules. Half of each molecule is crystallographically unique with distances S-S 2.002(1), and C-S 1.804(2) and 1.645(2) �. The dihedral angle between planar C2NC(S)S portions is 87.9�. The relevance of the derived structural parameters to the question of why the tris(pyrrolidine-1-carbodithioato)iron(III) complex is, uniquely, high spin is discussed.

The Meisenheimer rearrangement in heterocyclic synthesis. II. Synthesis and X-ray crystal structure of a tetrahydro-1H-2,3-benzoxazocine and preparation of a hexahydro-2,3-benzoxazonine

1980 ◽  
Vol 33 (6) ◽  
pp. 1323 ◽  
Author(s):  
JB Bremner ◽  
EJ Browne ◽  
PE Davies ◽  
CLWAH Raston
Keyword(s):  
Molecular Structure ◽  
Crystal Structure ◽  
Acetic Acid ◽  
Crystal And Molecular Structure ◽  
Phosphorus Oxychloride ◽  
Crystallographic Analysis ◽  
Heterocyclic Synthesis ◽  
Reaction Conditions ◽  
X Ray ◽  
Heterocyclic Derivatives

The heterocyclic derivatives, 8,9-dimethoxy-3-methyl-1-phenyl-3,4,5,6- tetrahydro-1H-2,3-benzoxazocine(3a) and 9,10-dimethoxy-3-methyl-1- phenyl-1,3,4,5,6,7-hexahydro-2,3-benzoxazonine (3b),examples of two new ring systems, have been prepared by Meisenheimer rearrangement of the corresponding 2-benzazepine and 2-benzazocine N-oxide derivatives (2a) and (2b). The Bischler-Napieralski-type cyclization reaction was used in the preparation of the tertiary amine precursors of these N-oxides reaction conditions for the cyclization were critical and phosphorus oxychloride in refluxing butanenitrile was found to give the best yields of the seven- or eight-membered cyclic imine intermediates. Reductive cleavage of the benzoxazocine derivative (3a) with zinc in acetic acid followed by N-methylation gave the expected product, [2-{3- (dimethylamino)propyl}-4,5-di-methoxyphenyl]phenylmethanol (12). The crystal and molecular structure of (3a) has been determined by X-ray crystallographic analysis.

scholarly journals X-Ray Single Crystal Structural Analysis of Magnetically Oriented Microcrystals

2014 ◽  
Vol 70 (a1) ◽  
pp. C1138-C1138
Author(s):  
Chiaki Tsuboi ◽  
Kazuki Aburaya ◽  
Shingo Higuchi ◽  
Fumiko Kimura ◽  
Masataka Maeyama ◽  
...  
Keyword(s):  
Molecular Structure ◽  
Crystal Structure ◽  
Single Crystal ◽  
Three Dimensional ◽  
Diffraction Measurement ◽  
X Ray Diffraction ◽  
Data Set ◽  
Uv Curable ◽  
X Ray

We have developed magnetically oriented microcrystal array (MOMA) technique that enables single crystal X-ray diffraction analyses from microcrystalline powder. In this method, microcrystals suspended in a UV-curable monomer matrix are there-dimensionally aligned by special rotating magnetic field, followed by consolidation of the matrix by photopolymerization. From thus achieved MOMAs, we have been succeeded in crystal structure analysis for some substances [1, 2]. Though MOMA method is an effective technique, it has some problems as follows: in a MOMA, the alignment is deteriorated during the consolidation process. In addition, the sample microcrystals cannot be recovered from a MOMA. To overcome these problems, we performed an in-situ X-ray diffraction measurement using a three-dimensional magnetically oriented microcrystal suspension (3D MOMS) of L-alanine. An experimental setting of the in-situ X-ray measurement of MOMS is schematically shown in the figure. L-alanine microcrystal suspension was poured into a glass capillary and placed on the rotating unit equipped with a pair of neodymium magnets. Rotating X-ray chopper with 10°-slits was placed between the collimator and the suspension. By using this chopper, it was possible to expose the X-ray only when the rotating MOMS makes a specific direction with respect to the impinging X-ray. This has the same effect as the omega oscillation in conventional single crystal measurement. A total of 22 XRD images of 10° increments from 0° to 220° were obtained. The data set was processed by using conventional software to obtain three-dimensional molecular structure of L-alanine. The structure is in good agreement with that reported for the single crystal. R1 and wR2 were 6.53 and 17.4 %, respectively. RMSD value between the determined molecular structure and the reported one was 0.0045 Å. From this result, we conclude that this method can be effective and practical to be used widely for crystal structure analyses.

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