Augusto Rivera1, Jaime Ríos-Motta1, Michael Bolte2. 1. Universidad Nacional de Colombia, Sede Bogotá, Facultad de Ciencias, Departamento de Química, Cra 30 No.45-03, Bogotá, Código Postal 111321, Colombia. 2. Institut für Anorganische Chemie, J. W. Goethe-Universität Frankfurt, Max-von-Laue-Strasse 7, 60438 Frankfurt/Main, Germany.
Abstract
The structure of the title compound, C8H16N4, which consists of four fused seven-membered rings, has been redetermined at 173 K. This redetermination corrects the orientation of two H atoms, which were located at unrealistic positions in the original room-temperature study [Murray-Rust (1974 ▶). J. Chem. Soc. Perkin Trans. 2, pp. 1136-1141]. The complete mol-ecule is generated by -42m symmetry, with one quarter of a mol-ecule [one N atom (site symmetry m), two C atoms (one with site symmetry m and the other with site symmetry 2) and two H atoms] in the asymmetric unit. No directional inter-actions beyond van der Waals contacts are apparent in the crystal structure.
The structure of the title compound, C8H16N4, which consists of four fused seven-membered rings, has been redetermined at 173 K. This redetermination corrects the orientation of two H atoms, which were located at unrealistic positions in the original room-temperature study [Murray-Rust (1974 ▶). J. Chem. Soc. Perkin Trans. 2, pp. 1136-1141]. The complete mol-ecule is generated by -42m symmetry, with one quarter of a mol-ecule [one N atom (site symmetry m), two C atoms (one with site symmetry m and the other with site symmetry 2) and two H atoms] in the asymmetric unit. No directional inter-actions beyond van der Waals contacts are apparent in the crystal structure.
For the original synthesis procedure, see: Bischoff (1898 ▶). For the previous determination of the structure, see: Murray-Rust (1974 ▶). For crystal structures containing the title compound as a fragment, see: Rivera et al. (2007 ▶); Glister et al. (2005 ▶). For a description of the Cambridge Crystallographic Database, see: Allen et al. (2002 ▶).
Stoe IPDS II two-circle diffractometerAbsorption correction: multi-scan (X-AREA; Stoe & Cie, 2001 ▶) T
min = 0.973, T
max = 0.9774336 measured reflections264 independent reflections264 reflections with I > 2σ(I)R
int = 0.049
Refinement
R[F
2 > 2σ(F
2)] = 0.050wR(F
2) = 0.141S = 1.12264 reflections18 parametersH-atom parameters constrainedΔρmax = 0.27 e Å−3Δρmin = −0.17 e Å−3Data collection: X-AREA (Stoe & Cie, 2001 ▶); cell refinement: X-AREA; data reduction: X-AREA; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: XP in SHELXTL (Sheldrick, 2008 ▶); software used to prepare material for publication: SHELXL97.Crystal structure: contains datablock(s) I, New_Global_Publ_Block. DOI: 10.1107/S1600536814002608/hb7192sup1.cifStructure factors: contains datablock(s) I. DOI: 10.1107/S1600536814002608/hb7192Isup2.hklClick here for additional data file.Supporting information file. DOI: 10.1107/S1600536814002608/hb7192Isup3.cmlCCDC reference:Additional supporting information: crystallographic information; 3D view; checkCIF report
C8H16N4
Dx = 1.336 Mg m−3
Mr = 168.25
Mo Kα radiation, λ = 0.71073 Å
Tetragonal, I42m
Cell parameters from 11628 reflections
a = 7.4065 (7) Å
θ = 3.8–27.9°
c = 7.6235 (8) Å
µ = 0.09 mm−1
V = 418.20 (9) Å3
T = 173 K
Z = 2
Block, colourless
F(000) = 184
0.32 × 0.28 × 0.27 mm
Stoe IPDS II two-circle diffractometer
264 reflections with I > 2σ(I)
Radiation source: Genix 3D IµS microfocus X-ray source
Hydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.050
H-atom parameters constrained
wR(F2) = 0.141
w = 1/[σ2(Fo2) + (0.0809P)2 + 0.2587P] where P = (Fo2 + 2Fc2)/3
S = 1.12
(Δ/σ)max < 0.001
264 reflections
Δρmax = 0.27 e Å−3
18 parameters
Δρmin = −0.17 e Å−3
Geometry. All e.s.d.'s (except the e.s.d. in the dihedral angle between two l.s. planes)
are estimated using the full covariance matrix. The cell e.s.d.'s are taken
into account individually in the estimation of e.s.d.'s in distances, angles
and torsion angles; correlations between e.s.d.'s in cell parameters are only
used when they are defined by crystal symmetry. An approximate (isotropic)
treatment of cell e.s.d.'s is used for estimating e.s.d.'s involving l.s.
planes.
Authors: Augusto Rivera; Juan Manuel Uribe; Jicli José Rojas; Jaime Ríos-Motta; Michael Bolte Journal: Acta Crystallogr E Crystallogr Commun Date: 2015-04-09