Crystal and molecular structure of 1-diazo-2,3,4,5-tetraphenylcyclopentadiene

M_r = 396.30, monoclinic space group P 2₁/c, a = 10.145(2), b = 18.523(4), c = 12.443(2) Å, β = 110.31(2)°, V = 2193(1) ų, Z = 4, D_x = 1.201 Mg m⁻³, F(000) = 832, λ(MoKα) = 0.71069 Å, μ = 0.7 mm⁻¹. The crystal structure was determined by direct methods and refined by least-squares procedure to the discrepancy factor R = 0.039.     

Crystal and molecular structure of 1-(p-nitrophenyl)-2-acetylamino-3-brom-propen-2-on-1, C11H9BrN2O4

M_r = 313.11, orthorhombic space group Pbca, a = 8.165(1), b = 9.491(2), c = 32.207(5) Å V = 2496(1) ų, D_X = 1.667 Mgm⁻³, Z = 8, F(000) = 1248, λ(MoKα) = 0.71069 Å, μ = 32.7 mm⁻¹. The crystal structure was determined by direct methods and refined by least-squares procedure to the discrepancy factor R = 0.065. Positions of hydrogen atoms were calculated. The structure determined by x-ray analysis confirms the chemical results.     

Crystal and molecular structure of 5-diazo-2,2-dimethyl-4,6-dioxo-1,3-dioxane and 5-diazo-1,3-dimethylpyrimidin-2,4,6-trione

C₆N₂O₄H₆: M_r = 170.12, orthorhombic space group Pbca, a = 6.751(2), b = 13.669(4), c = = 16.845(4) Å, V = 1555(1) ų, D_x = 1.248 Mgm⁻³, Z = 8, F(000) = 704, λ(moKα) = 0.71069 Å, μ = 1.1 mm⁻¹. The crystal structure was determined by direct methods and refined by least-squares procedure to the discrepancy factor R = 0.039. C₆N₄O₃H₆: M_r = 182.14, monoclinic space group C2/c, a = 17.726(8), b = 6.191(12), c = 16.062(6) Å, β = 117.59 (3)°, V = 1562 (1) ų, D_x = 1.549 Mgm⁻³, Z = 8, F(000) = 752, λ(MoKα) = 0.71069 Å, μ = 1.2 mm⁻¹. The crystal structure was determined by direct methods and refined by least-squares procedure to the discrepancy factor R = 0.056.     

Crystal and molecular structures of N-alkyl-N,N-dimethyl-3-(heptamethyltrisiloxan-3-yl) propylammonium bromides

C₁₆H₄₂NO₂Si₃Br: M_r = 444.76, monoclinic space group P 2₁/c, a = 23.300(8), b = 8.918(4), c = 13.403(2) Å, β = 101.69(4)°, V = 2727(1) ų, D_x = 1.08 Mgm⁻³, D_exp = 1.06 Mgm⁻³, Z = 4, F(000) = 932, λ(MoKα) = 0.71069 Å, μ = 16.3 cm⁻¹. The crystal structure was determined by direct methods and refined by least-squares procedure to the discrepancy factor R = 0.117. C₁₅H₄₀NO₂ Si₃Br: M_r = 430.34, monoclinic space group P2₁/c, a = 23.460(4), b = 8.518(2), c = 13.403(2) Å, β = 102.03(2)°, V = 2619(1) ų, D_x = 1.09 Mgm⁻³, D_exp = 1.07 Mg⁻³, Z = 4, F (000) = 920, λ(MoKα) = 0.71069 Å, μ = 33.9 cm⁻¹. The crystal structure was determined by least-squares refinement of the structure model derived from structure determination of C₁₆H₄₂NO₂·Si₃Br to the discrepancy factor R = 0.099. C₁₆H₄₂NO₂Si₃Br: Daten siehe oben. C₁₅H₄₀NO₂Si₃Br: Daten siehe oben.     

Crystal and Molecular Structure of mer-Co(4-CH3C5H4N)3(N3)3

The crystal structure of mer-Co(4-CH₃C₅H₄N)₃(N₃)₃has been determined by single crystal X-ray methods at 300 K. The compound crystallizes in the monoclinic space group C 2/c, a = 19.087(6), b = 16.769(4), c = 15.845(4) Å, β = 119.04(2)°, V = 4434(2) ų, M_r = 464.42. Z = 8, D_x = 1.391 Mgm⁻³, F(000) = 1920, λ (MoKα) = 0.71069 Å, μ = 0.802 mm⁻¹. The cobalt(III) ions are octahedrally coordinated to three azide groups and to three 4-methyl-pyridine molecules to form isolated coordination polyhedra.     

Crystal structure of 4,5-dihydro-6-(2-thienyl)-3(2H) pyridazinone azine, (C16H16N16S2)

M_r = 484, monoclinic, P 2₁/c, a = 5.567(1), b = 7.857(2), c = 19.194(10) Å, β = 99.97(3)°, V = 826.9 ų, Z′ = 2, D_x = 1.43 g · cm⁻³, F(000) = 372, MoKα, λ = 0.71069 Å, μ = 0.328 mm⁻¹, final R = 0.055 for 889 observed reflections, T = 293 K. The compound was prepared from a direct unusual reaction of 6-(2-thienyl)-2,3,4,5-tetrahydropyridazine-3-one with hydrazine hydrate. The structure was solved by direct methods and refined by full-matrix least squares. The molecule in the solid state consists of a dimer with its two equivalent halves related by a center of symmetry at the middle of the N N bond. Each molecular fragment is nearly planar and the N N bond between the two halves is 1.296(5) Å indicating that it is a partial double bond.     

Structure of monoclinic acridine orange hydrochloride monohydrate,C17H19N3 · HCl · H2O

M_r = 319.82, monoclinic P2₁/a, Z = 4, a = 14.545(5), b = 15.562(6), c = 8.538(4) Å, β = 120.66(3)°, V = 1662(1) ų, D_m = 1.27 Mgm⁻³, D_x = 1.278 Mgm⁻³, λ(MoKα) = 0.71069 Å, μ(MoKα) = 0.24 mm⁻¹, T = 297 K. Final R = 0.049 for 1485 observed reflections. All hydrogen atoms were located and refined isotropically. Bond lengths (σ = 0.004 Å) and angles (σ = 0.3°) are normal. The substance is a derivative of acridine. The structure consists of chloride anions, bisdimethylaminoacridinium cations and water molecules. In the solid state the molecules are approximately planar. Pairs of cations form dimers with parallel planes connected by an I inversion centre and plane distances of 3.474 Å. They overlap with partial areas of all three six membered rings.     

The crystal structure of dodecyltrimethylammoniumbromide

C₁₅H₃₄BrN, monoclinic, P 2₁/m, a = 21.603(9), b = 7.261(3), c = 5.636(2) Å, β = 86.85(2)°, Z = 2, V = 882.72 ų, D_x = 1.160 g/cm³, μ(MoKα) = 2.45 cm⁻¹, λ(MoKα) = 0.71069 Å. The structure of this cationic surfactant was solved with Patterson methods and refined to R = 0.091 for 2057 measured reflections. The dodecyl chains are slightly screwed around their chain axes. The hydrocarbon chains are statistically disordered. The polar regions satisfy the mirror plane which is by remaining parts only statistically fulfilled. In the process of structure refinement statistical disorder has been included by separation of some atom positions. The sublattice of the hydrocarbon chains is nearly O⟂ with a_s = 5.14, b_s = 7.26, c_s = 2.52 Å.     

Structure of N-5-Anilino-pentadien-(2,4)-ylidenaniliniumperchlorate,C17H17N2O4Cl

M_r=348.65, monoclinic, P2₁/n, a=11.088(2), b=17.521(3), c=8.845(2) Å, β=98.87(3)⁰, Z=4, V=1697.8(8) ų, D_x=1.368(1) Mgm⁻³, μ(MoKα)=0.256 mm⁻¹, λ(MoKα)=0.71069 Å, T=296 K. Final R=0.040 for 2454 independent reflections excluding those with |F₀|<4σ(|F₀|). Intensities were measured with an automatic diffractometer. The structure belongs to the openchained cyanines. Characteristic for this class of compounds is their nearly ideal polymethinic electron structure with its main geometrical features: equalisation of bond lengths, alternation of bond angles, planarity of the polymethinic chain. All three features are significantly to be observed in the structure. The bond angle alternation determines essentially the shape of the molecules and the molecular packing.     

The molecular and crystal structure of 2-oxo-1-pyrrolidine-acetamide

C₆H₁₀N₂O₂, P1 , a = 6,607(2) Å, b = 8,538(2) Å, c = 6,392(2) Å, α = 102,43(2)°, β = 91,11(2)°, y = 79,82(2)°, V = 349,1 ų, Z = 2, D_m = 1,36 g × cm⁻³, D_x = 1,35 g × × cm⁻³, MoKα radiation, λ = 1.71069 Å, μ(MoKα) = 1.11 cm⁻¹. The structure was solved by direct methods. The parameters were refined by full matrix least squares technique to a final R = 0.088 for 834 reflections with ∥F₀∥ > 4σ(F₀). The dihedral angle between the least-squares plane through the pyrrolidine ring and that through the acetamide group is 90.4°. The N H … O hydrogen bonds connect molecules to form bands parallel to the z axis.     

Crystal structure of a newly oxidized aristolane sesquiterpenes,C15H22O3, from aristolochia debilis

M_r = 250, orthorhombic, P 2₁2₁2₁, a = 9.583(6), b = 11.786(8), c = 12.298(9) Å, V = 1389.0 ų, Z = 4, D_x = 1.20 g cm⁻³, F(000) = 544, MoK_α, λ = 0.71069 Å, μ = 0.88 cm⁻¹. Final R = 0.023 for 1006 observed reflections, T = 293 K. The structure was solved by direct methods and refined by full-matrix least squares. It is an α, β unsaturated carbonyl compound with a trisubstituted double bonds. No significant variation in aromatic bond lengths. The strain affecting the molecule is largely due to angular deformation which is partly due to the fusion of the rings and partly due to substitution of H-atoms by methyl groups and oxygen atoms.     

Crystal structure determination of bis-dimethyl heptamethine cyanine chloride,C11N2H19Cl · 4 H2O

Mr = 286.59, monoclinic superposition structure C 121, Z = 4, a = 15.248(3), b = = 6.942 (3), c = 9.074(1) Å, β = 120.1(1)°, V = 827(1) ų, D_m = 1.13(1) Mg m⁻³, D_x = = 1.15 Mg m⁻³, λ(MoK_α) = 0.71069 Å, μ = 0.243 mm⁻¹, F (000) = 312, T = 296 K, final R = 0.061 for 802 reflections. All hydrogen atoms were located. The structure consists of chloride anions, bis-dimethyl heptamethine cyanine cations and water molecules. The structure of bis-dimethyl heptamethine cyanine chloride is disordered, e.g. there exist partial coincidence operations, leading to more than one stacking mode of the bis-dimethyl heptamethin cyanine chains. The crystal structure consists of rows of molecule along the a-axis. The C C bonds show the bond length compensation, typical of polymethines, towards a partial double bond (mean value 1.38 Å) between formally sp²-hybridized C atoms. The C N bond lengths to the methyl carbon atoms (mean value 1.49 Å) correspond to normal C N single bonds. The valence angles at the C atoms of the heptamethine chain clearly alternate and deviate systematically from 120°. This is also observed in other structures of a similar type. The structure determined by X-ray analysis confirms the chemical results.     

Static Disorder in Hexagonal Crystal Structures of C60 at 100 K and 20 K

C₆₀ · 2C₈H₁₀ (100 K): hexagonal space group P6₃, a = 23.694(4), c = 10.046(2) Å, V = 4884(2) ų, D_x = 1.903 g cm⁻³, Z = 6, F(000) = 2856, γ(CuKa) = 1.54178 Å, μ = 0.84 mm⁻¹. C₆₀ · 2C₈H₁₀ (20 K): hexagonal space group P6₃, a = 23.67(1), c = 10.02(1) Å, V = 4862(6) ų, D_x = 1.912 g cm⁻³, Z = 6, F(000) = 2856, γ(CuKa) = 1.54178 Å, μ = 0.84 mm⁻¹. The structures were determined by Patterson syntheses and rigid-body refinements. The C₆₀ molecules show two orientations with one molecular centre in common. The solvent molecules are disordered too. Static disorder could not be overcome or influenced by cooling down. A coordination number of 10 was found for the fullerene molecules.     

Crystal structure determination of 2-acetylamino-4-benzoyl-5,5-dimethyl-4,5-dihydro-1,3,4-thiadiazolin,C13H15N3O2S

Thiosemicarbazone is receiving increasing interest because of the biological activity of some of its derivatives. Mr = 277.35, space group P2₁2₁2₁, Z = 4, a = 9.290(3), b = = 11.512(2), c = 13.286(2) Å, V = 1421 (1) ų, D_m = 1.29(1) Mg m⁻³, D_x = 1.296 Mg m⁻³, λ(MoK_α) = 0.71062 Å, μ = 0.230 mm⁻¹, F(000) = 584, T = 296 K, final R = 0.028 for 1255 reflections. All hydrogen atoms were located. The structure determed by X-ray analysis confirms the chemical results. The structure analysis of the title compound is described and its molecular and crystal structure discussed.     

Crystal Structure of a Complex of Sarcosine with Barium Chloride

Single crystals of sarcosine barium chloride tetrahydrate were crystallised from a saturated aqueous solution containing stoichiometric amounts of sarcosine and barium chloride, in 2: 1 proportion. The intensity data were collected using a CAD-4 diffractometer with graphite monochromated MoKα radiation. The crystal data are as follows: a = 7.235(1) Å, b = 10.668(4) Å, c = 15.686(3) Å, V = 1210.7 ų, F.W. = 369.33, d_expt, = 2.02 g · cm⁻³, d_calc = 2.026 g · cm⁻³, Z = 4 and the space group is P2₁2₁2₁. The structure has been solved to an R value of 0.02 for all the 1239 reflections with I > 2σ(I). The sarcosine molecule exists as zwitterion in the structure. The barium ion is found to have 10-fold coordination with nine oxygens and a chlorine taking part in coordination. All the water oxygens and chlorines take part in hydrogen bonds except carboxyl oxygens.     

Crystal Structure Investigation of 2-Pheny limidazo [f]1,10-phenanthroline

The crystal structure of the title compound (PIP) has been determined by single crystal X-ray diffraction methods. C₁₉H₁₂N₄. C₂H₅OH crystallizes in the monoclinic space group P2₁/n with a = 11.4414(8), b = 12.6052(9), c = 12.4627(8) Å, β = 100.345(2)°, Z = 4, V = 1768.17 ų, D_cal = 1.286 Mg. m⁻³, μ (MoKα) = 0.80 cm^-1, F(000) = 720. The structure was solved by the direct methods and refined by full-matrix least-squares method to a final R = 0.0337 and R_w = 0.0332 for 2306 reflections with F₀ > 4σ(F₀). The phenl ring and the imidazo[f]1,10-phenanthroline moiety are coplanar in the crystal. The packing of the molecules involves hydrogen bonded association of the hydroxyl group of ethanol both with the N H of the imidazole moiety of one PIP and one nitrogen atom of the phenanthroline moiety of another PIP.     

Structures of Azomethine Imines of the Pyrazolidone-(3)-type, (III) The Structure of 1-[Anthryl-(9)-methylene]-pyrazolidone-(3)-betaine

C₁₈H₁₄N₂O, Pbca, a = 19.541(4) Å, b = 14.800(2) Å, c = 9.572(3) Å, Z = 8, U = 2768.3 ų, D_x = 1.32 g cm⁻³, μ(MoKα) = 0.93 cm⁻⁻¹, crystal size 0.5 × 0.2 × 0.1 mm, colourless. Final R = 0.077 for 1177 independent reflections excluded those with |F₀| < 8 σ(F₀). The intensities were measured with an automatic diffractometer. The azomethine imine unit of the molecule has a geometry in approximate agreement with a polymethinic electron structure. The conjugation of the azomethine imine unit with the anthryl unit is only small. The anthryl ring and the five membered pyrazolidone ring include a dihedral angle of 65.4°. The main intermolecular forces are C–H … N hydrogen bridges.     

Crystal Structure Determination of Nickel (2,2-Dipyridyl) Sulphate Hexahydrate [Ni(C10H8N2) · 4 H2O]SO4 · 2H2O

[Ni(C₁₀H₈N₂) · 4 H₂O]SO₄ · 2 H₂O, Mr = 418.7, monoclinic, P1 , a = 7.781(3), b = 9.421(3), c = 11.457(4) Å, α = 87.54(2)º, β = 96.40(2)º, γ = 102.58(2)º, ν = 814.5 Å, D_x = 1.26 g/cm³, Z = 2, (MoKx) = 0.71073 Å, μ = 7.0 cm⁻¹: T = 23 °C, R = 0.047 for 2139 reflections having intensities greater than 36. The structure was solved using the Patterson heavy-atom method and the remaining atoms were located in succeeding difference Fourier syntheses. The structure was then refined by full matrix least-squares using anisotropic temperature factors. Hydrogen atoms were located and their positions and isotropic parameters were refined.     

Structure refinement with X-ray powder diffraction data for synthetic calcium hydroxyapatite by Rietveld method

Ca₅(PO₄)₃OH, M_r = 502.3, hexagonal, P 6₃/m, a = 9.4207(3), c = 6.8780(2) Å, V = 528.67 ų, Z = 2, D_x = 3.156 Mg · m⁻³, CuKα, λKα₁ = 1.54051, λKα₂ = 1.54433 Å, μ = 26.25 mm⁻¹, F(000) = 500, T = 294 K. The powder diffraction pattern was analysed by the Rietveld method. The parameters were refined by the program PFSR (DBW2.9) to final R-factors R_p = 0.079, R_wp = 0.081 and R_B = 0.015.     

Structure of the OD-disordered 2-Hydroxy-4-methoxy-2H-1,4-benzoxazin-3-one,C9H9NO4

The X-ray diagrams of the title compound show pronounced maxima on diffuse streaks parallel c* and unusual extinctions. The intensity distribution is compatible with the assumption of a disordered (OD) structure consisting of one kind of layers. The structure contains ordered domains with the crystal data: monoelinic, space group P 2₁/a, lattice parameters a = 15.910(5), b = 8.365(4), c = 15.747(5) Å, β = 120.34(6)°, V = 1809 ų, Z = 8, M_r = 195.1, D_x = 1.432 Mg m⁻³, μ(MoKα) = 0.36 mm⁻¹, final R = 0.129 for 859 observed reflections. The asymmetric unit is constituted of two crystallographically independent molecules related by a pseudo glide plane. The crystal used for X-ray analysis proved to be twinned.