Crystal and molecular structure of carbonylcyanide-4-chlorophenylhydrazone(4-chlorophenylhydrazonopropanedinitrile)

1984 ◽  
Vol 49 (10) ◽  
pp. 2363-2370
Author(s):  
Viktor Vrábel ◽  
Ernest Šturdík ◽  
Michal Dunaj-Jurčo ◽  
Jan Lokaj ◽  
Ján Garaj

The crystal structure of carbonylcyanide-4-chlorophenylhydrazone was solved by the single crystal X-ray diffraction method and interpreted by the heavy atom method. The compound crystallizes in the P21/c monoclinic group with 4 molecules per unit cell and with lattice parameters: a = 1.1843(3), b = 0.5944(1), c = 1.4922(3) nm and β = 117.92(2)°. The structure was refined by the least squares method for 1 078 observed reflections to a final value of R = 4.9%. The crystal structure consists of monomeric units, where hydrogen bonds were observed between atoms N3...H5 0.2193 nm and N3...H3 0.2404 nm between two molecules transformable through centre of symmetry -x, -y, -z. The name 4-chlorophenylhydrazonopropanedinitrile is recommended for the studied compound on the basis of this X-ray structural analysis.

1975 ◽  
Vol 53 (22) ◽  
pp. 3383-3387 ◽  
Author(s):  
Joseph Hubert ◽  
André L. Beauchamp ◽  
Roland Rivest

The crystal and molecular structure of dithiocyanato(triphenylarsine)mercury(II) has been determined from X-ray diffraction data. The crystals are monoclinic, space group P21/c, with a = 10.290(7), b = 21.199(23), c = 10.719(7) Å, β = 112.00(2)°, and Z = 4. The structure has been solved by the heavy-atom method and refined by block-diagonal least-squares calculations. The agreement factor R obtained for 2607 'observed' reflections is 0.030. The crystal consists of single molecules. The 'characteristic' coordination number of mercury is three, with two sulfur and one arsenic atoms at the apexes of a triangle. The nitrogen atoms of the thiocyanate groups are at 2.67 and 2.74 Å from the adjoining mercury atoms and therefore link the different molecules together.


1980 ◽  
Vol 45 (8) ◽  
pp. 2147-2151 ◽  
Author(s):  
Jan Lokaj ◽  
Ján Garaj ◽  
Viktor Kettmann ◽  
Viktor Vrábel

Crystal and molecular structure of nickel(II) dimethyldithiocarbamate, Ni[S2CN(CH3)2]2 was solved by X-ray structural analysis and refined by the least squares method to R = 0.06 for 1065 reflections. The compound crystallizes in a space group P I and the triclinic unit cell has the dimensions: a = 6.521 (7), b = 6.798 (9), c = 7.633 (4), α = 67.21 (8)°, β = 67.34 (6)° γ =85.59 (9)°. The experimentally observed density is 1.75 g cm-3 and the calculated value for Z = 1 is 1.73 g cm-3. In the structure , the Ni atom occupies a special position in the centre of symmetry and is coordinated by four sulphur atoms in a plane: Ni-S 0.2218 (4) and 0.2198 nm S1-Ni-S2 angle 79.62 (8)°. The ligand S2CNC2 is nearly planar.


1982 ◽  
Vol 47 (10) ◽  
pp. 2623-2632 ◽  
Author(s):  
Viktor Vrábel ◽  
Jan Lokaj ◽  
Ján Garaj ◽  
František Pavelčík

The crystal structure of [Cu(H2O)(en)2][Cu2(CN)3(SeCN)] was solved by single crystal X-ray structural analysis in the triclinic system with a space group of P1 and in the monoclinic system with a space group of C2. In the triclinic system the unit cell has dimensions of a = 0.8445(3), b = 0.7903(3), c = 0.8444(3) nm, α = 119.58(2), β = 118.59(2) and γ = 93.63(3)° and, in the monoclinic system, a = 1.3331(4), b = 0.8670(2), c = 0.8267(3), β = 122.60(2)°. The structure was refined by the least squares method to final value of R = 5.5% in the triclinic system and R = 7.8% in the monoclinic system. The coordination sphere around the Cu(II) atom is square pyramidal, formed of two ethylenediamine molecules and one water molecule. The Cu(I) atoms are tetrahedrally coordinated by bridging SeCN and CN ligands to form infinite three-dimensional chains. The SeCN group is bonded to the Cu(I) atoms through the Se atom at distances of 0.2731(3) and 0.2745(3) nm.


1984 ◽  
Vol 218 (3) ◽  
pp. 677-689 ◽  
Author(s):  
T Ishida ◽  
M Kenmotsu ◽  
Y Mino ◽  
M Inoue ◽  
T Fujiwara ◽  
...  

In order to investigate the structure-activity relationship of [Leu5]- and [Met5]enkephalins, [(4′-bromo)Phe4, Leu5]-, [(4′-bromo)Phe4, Met5]- and [Met5] enkephalins were synthesized and crystallized. The crystal structure of [(4′-bromo) Phe4, Leu5]- enkephalin was determined by X-ray diffraction method using the heavy atom method and refined to R = 0.092 by the least-squares method. The molecule in this crystal took essentially the same type I' beta-turn conformation found in [Leu5]enkephalin [Smith & Griffin (1978) Science 199, 1214-1216). On the other hand, the preliminary three-dimensional Patterson analyses showed that the most probable conformations of [(4′-bromo)Phe4,Met5]- and [Met5]enkephalins are both the dimeric extended forms. Based on these insights, the biologically active conformation of enkephalin was discussed in relation to the mu- and delta-receptors.


1983 ◽  
Vol 61 (12) ◽  
pp. 2809-2812 ◽  
Author(s):  
P. Michael Boorman ◽  
Joanne M. Ball ◽  
Kelly J. Moynihan ◽  
Vikram D. Patel ◽  
John F. Richardson

The complex (Me2S)Cl3W(μ-SPh)2WCl3(SMe2), 1, has been isolated as one product of the 1:1 reaction between WCl4(Me2S)2 and SiMe3(SPh) in CH2Cl2 solution. A single crystal X-ray diffraction study shows that the molecule has the relatively unusual edge-shared bioctahedral structure, with a W—W bond length of 2.759(1) Å. The dimethyl sulfide ligands occupy positions trans to one another in the equatorial mean plane of the molecule, which has two-fold symmetry imposed on it. The structure was solved by the heavy atom method and refined to R = 0.044 and Rw = 0.058 for 2001 reflections. Crystals of 1 are monoclinic, space group C2/c, with a = 17.445(4), b = 12.594(2), c = 11.509(3) Å, β = 91.22(1)°, and Z = 4.


1982 ◽  
Vol 47 (10) ◽  
pp. 2633-2638 ◽  
Author(s):  
Jan Lokaj ◽  
Viktor Kettmann ◽  
František Pavelčík ◽  
Viktor Vrábel ◽  
Ján Garaj

The crystal and molecular structure of [Fe(S2CN(C3H5)2)3] was solved by X-ray structural analysis and refined by the least squares method to give R = 0.09 for 1 834 observed reflections. The compound crystallizes in the C2/c space group and the monoclinic unit cell has dimensions of a = 18.709(6), b = 10.217(3), c = 15.546(6) . 10-10 m, β = 106.03(3)°. The experimentally observed density is 1.35 Mg m-3 and the calculated value for Z = 4 is 1.33 Mg m-3. In the structure the iron atom occupies a special position on the two-fold axis and is coordinated by six sulfur atoms in a trigonally deformed octahedron: Fe-S1 2.340(6), Fe-S2 2.367(7), Fe-S3 2.323(6) . 10-10 m. The S2CNC2 ligands are approximately planar.


1983 ◽  
Vol 48 (5) ◽  
pp. 1272-1280 ◽  
Author(s):  
Eleonóra Kellö ◽  
Viktor Vrábel ◽  
Viktor Kettmann ◽  
Ján Garaj

The structure of {Zn[S2CN(C3H5)2]2}2 was solved by X-ray structural analysis. The heavy atom method was used in interpretation of the structure. The dimeric compound crystallizes in the triclinic system with a space group of P1 and lattice parameters of a = 0.8218(2), b = 0.9462(6), c = 1.2942(9) nm, α = 77.70(5), β = 77.46(4), γ = 78.25(4)°. The experimentally determined density value for Z = 2 is 1.42 Mg m-3 and the calculated value is 1.44 Mg m-3. In the dimeric molecule each Zn atom is coordinated by five sulfur atoms at distances of Zn-S1 0.2346, Zn-S2 0.2339, Zn-S3 0.2468, Zn-S4 0.2846, Zn-S'4 0.2387 nm in a deformed trigonal bipyramid. The coordination number of Zn can be expressed as 3 + 1 + 1. The distance between two zinc atoms is 0.3580 nm.


1990 ◽  
Vol 55 (9) ◽  
pp. 2216-2225 ◽  
Author(s):  
Jan Ondráček ◽  
Jitka Soldánová ◽  
František Jursík

The crystal and molecular structure of the title compound was determined by X-ray diffraction. The structure was solved by the heavy-atom method and refined to an R value of 0.118 for 997 observed reflections. The unit cell is monoclinic with a = 11.980(1), b = 12.130(1), c = 12.641(1) Å, β = 108.18(1)°, Z = 4. The space group is P21/c. The crystals are composed of sym-fac-[Co(dtp)(R,S)-Asp]+, ClO4-, and H2O held together probably in a network of hydrogen bonds. The structural data obtained allow an explanation for the sym-fac-[Co(dtp)(S)-Asp]+ isomer optical activity contributions which can arise from the distorted chair conformation of one of the two dpt fused chelate rings, the donor atom distortions from the defined plane, and the (S)-aspartic acid vicinal chirality.


1984 ◽  
Vol 62 (3) ◽  
pp. 601-605 ◽  
Author(s):  
Masood A. Khan ◽  
Clovis Peppe ◽  
Dennis G. Tuck

The crystal structure of the title compound has been determined by the heavy atom method. The crystals are orthorhombic, space group Pbca, with unit cell dimensions a = 22.795(3) Å, b = 17.518(2) Å, c = 12.396(3) Å, Z = 8; R = 0.0409 for 1527 unique "observed" reflections. The structure is disordered, with each halogen site (X) occupied by 75% Br, 25% I. The molecule consists of two X2(tmen)In units (tmen = N,N,N′,N′-tetramethylethanediamine) with distorted trigonal bipyramidal geometry, joined by an In—In bond 2.775(2) Å in length.


1986 ◽  
Vol 51 (11) ◽  
pp. 2521-2527 ◽  
Author(s):  
Jan Lokaj ◽  
Eleonóra Kellö ◽  
Viktor Kettmann ◽  
Viktor Vrábel ◽  
Vladimír Rattay

The crystal and molecular structure of SnBu2(pmdtc)2 has been solved by X-ray diffraction methods and refined by a block-diagonal least-squares procedure to R = 0.083 for 895 observed reflections. Monoclinic, space group C2, a = 19.893(6), b = 7.773(8), c = 12.947(8) . 10-10 m, β = 129.07(5)°, Z = 2, C20H38N2S4Sn. Measured and calculated densities are Dm = 1.38(2), Dc = 1.36 Mg m-3. Sn atom, placed on the twofold axes, is coordinated with four S atoms in the distances Sn-S 2.966(6) and 2.476(3) . 10-10 m. Coordination polyhedron is a strongly distorted octahedron. Ligand S2CN is planar.


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