| Literature DB >> 21580297 |
P S Pereira Silva1, M Ramos Silva, J A Paixão, A Matos Beja.
Abstract
In the title compound, CH(6)N(3) (+)·C(7)H(6)Entities:
Year: 2010 PMID: 21580297 PMCID: PMC2983752 DOI: 10.1107/S160053681000396X
Source DB: PubMed Journal: Acta Crystallogr Sect E Struct Rep Online ISSN: 1600-5368
| CH6N3+·C7H6NO2− | |
| Orthorhombic, | Mo |
| Hall symbol: -P 2ac 2n | Cell parameters from 8009 reflections |
| θ = 2.8–27.5° | |
| µ = 0.10 mm−1 | |
| Irregular edge, light brown | |
| 0.33 × 0.19 × 0.15 mm |
| Bruker APEX2 CCD area-detector diffractometer | 1323 independent reflections |
| Radiation source: fine-focus sealed tube | 960 reflections with |
| graphite | |
| φ and ω scans | θmax = 28.1°, θmin = 2.7° |
| Absorption correction: multi-scan ( | |
| 19879 measured reflections |
| Refinement on | Primary atom site location: structure-invariant direct methods |
| Least-squares matrix: full | Secondary atom site location: difference Fourier map |
| Hydrogen site location: inferred from neighbouring sites | |
| H atoms treated by a mixture of independent and constrained refinement | |
| 1323 reflections | (Δ/σ)max < 0.001 |
| 85 parameters | Δρmax = 0.13 e Å−3 |
| 0 restraints | Δρmin = −0.20 e Å−3 |
| Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes. |
| Refinement. Refinement of |
| O1 | 0.34385 (6) | 0.11290 (10) | −0.04842 (10) | 0.0519 (3) | |
| C1 | 0.43652 (10) | 0.2500 | 0.13590 (17) | 0.0390 (4) | |
| C2 | 0.46854 (8) | 0.10235 (14) | 0.19926 (13) | 0.0462 (3) | |
| H2 | 0.4490 | 0.0019 | 0.1577 | 0.055* | |
| C3 | 0.52869 (8) | 0.10183 (16) | 0.32253 (14) | 0.0542 (3) | |
| H3 | 0.5491 | 0.0015 | 0.3630 | 0.065* | |
| C4 | 0.55904 (11) | 0.2500 | 0.3867 (2) | 0.0556 (5) | |
| C5 | 0.37086 (10) | 0.2500 | 0.00390 (17) | 0.0391 (4) | |
| N4 | 0.61881 (15) | 0.2500 | 0.5120 (3) | 0.0886 (7) | |
| H4 | 0.6353 (13) | 0.149 (3) | 0.543 (2) | 0.106* | |
| N1 | 0.25025 (7) | 0.10833 (13) | 0.66469 (14) | 0.0551 (3) | |
| H1A | 0.2845 (9) | 0.1093 (16) | 0.7576 (18) | 0.066* | |
| H1B | 0.2285 (9) | 0.016 (2) | 0.6258 (17) | 0.066* | |
| N2 | 0.17018 (11) | 0.2500 | 0.47745 (19) | 0.0563 (4) | |
| H2A | 0.1493 (9) | 0.147 (2) | 0.4470 (16) | 0.068* | |
| C6 | 0.22330 (11) | 0.2500 | 0.6031 (2) | 0.0426 (4) |
| O1 | 0.0705 (6) | 0.0334 (4) | 0.0519 (5) | −0.0031 (4) | −0.0139 (4) | −0.0006 (3) |
| C1 | 0.0415 (8) | 0.0398 (8) | 0.0358 (7) | 0.000 | 0.0050 (6) | 0.000 |
| C2 | 0.0489 (6) | 0.0455 (6) | 0.0442 (6) | 0.0021 (5) | 0.0014 (5) | 0.0013 (5) |
| C3 | 0.0530 (7) | 0.0627 (8) | 0.0467 (7) | 0.0100 (6) | −0.0004 (5) | 0.0089 (6) |
| C4 | 0.0443 (9) | 0.0813 (14) | 0.0411 (9) | 0.000 | −0.0018 (8) | 0.000 |
| C5 | 0.0460 (8) | 0.0335 (8) | 0.0380 (8) | 0.000 | 0.0035 (7) | 0.000 |
| N4 | 0.0818 (13) | 0.1110 (19) | 0.0732 (13) | 0.000 | −0.0344 (11) | 0.000 |
| N1 | 0.0655 (7) | 0.0379 (6) | 0.0618 (7) | 0.0026 (5) | −0.0206 (5) | −0.0012 (5) |
| N2 | 0.0656 (10) | 0.0446 (9) | 0.0587 (9) | 0.000 | −0.0226 (8) | 0.000 |
| C6 | 0.0419 (8) | 0.0398 (8) | 0.0460 (8) | 0.000 | −0.0036 (7) | 0.000 |
| O1—C5 | 1.2575 (11) | C4—N4 | 1.390 (3) |
| C1—C2i | 1.3910 (13) | C5—O1i | 1.2575 (11) |
| C1—C2 | 1.3910 (13) | N4—H4 | 0.89 (2) |
| C1—C5 | 1.490 (2) | N1—C6 | 1.3188 (13) |
| C2—C3 | 1.3796 (17) | N1—H1A | 0.940 (15) |
| C2—H2 | 0.9300 | N1—H1B | 0.875 (16) |
| C3—C4 | 1.3886 (15) | N2—C6 | 1.329 (2) |
| C3—H3 | 0.9300 | N2—H2A | 0.923 (16) |
| C4—C3i | 1.3886 (15) | C6—N1i | 1.3188 (13) |
| C2i—C1—C2 | 117.65 (14) | O1—C5—O1i | 122.98 (14) |
| C2i—C1—C5 | 121.18 (7) | O1—C5—C1 | 118.50 (7) |
| C2—C1—C5 | 121.18 (7) | O1i—C5—C1 | 118.50 (7) |
| C3—C2—C1 | 121.34 (11) | C4—N4—H4 | 113.7 (13) |
| C3—C2—H2 | 119.3 | C6—N1—H1A | 119.5 (8) |
| C1—C2—H2 | 119.3 | C6—N1—H1B | 118.1 (10) |
| C2—C3—C4 | 120.50 (12) | H1A—N1—H1B | 121.7 (13) |
| C2—C3—H3 | 119.7 | C6—N2—H2A | 115.3 (9) |
| C4—C3—H3 | 119.7 | N1i—C6—N1 | 119.95 (15) |
| C3—C4—C3i | 118.64 (15) | N1i—C6—N2 | 120.02 (8) |
| C3—C4—N4 | 120.68 (8) | N1—C6—N2 | 120.02 (8) |
| C3i—C4—N4 | 120.68 (8) | ||
| C2i—C1—C2—C3 | 1.2 (2) | C2i—C1—C5—O1 | −179.70 (13) |
| C5—C1—C2—C3 | −179.36 (12) | C2—C1—C5—O1 | 0.8 (2) |
| C1—C2—C3—C4 | −0.1 (2) | C2i—C1—C5—O1i | −0.8 (2) |
| C2—C3—C4—C3i | −1.0 (3) | C2—C1—C5—O1i | 179.70 (13) |
| C2—C3—C4—N4 | 179.23 (16) |
| H··· | ||||
| N1—H1A···O1ii | 0.940 (15) | 1.869 (16) | 2.8068 (14) | 175.4 (13) |
| N1—H1B···O1iii | 0.875 (16) | 2.107 (16) | 2.9032 (15) | 151.0 (13) |
| N2—H2A···O1iii | 0.923 (16) | 2.099 (16) | 2.9408 (8) | 151.1 (12) |
Hydrogen-bond geometry (Å, °)
| H⋯ | ||||
|---|---|---|---|---|
| N1—H1 | 0.940 (15) | 1.869 (16) | 2.8068 (14) | 175.4 (13) |
| N1—H1 | 0.875 (16) | 2.107 (16) | 2.9032 (15) | 151.0 (13) |
| N2—H2 | 0.923 (16) | 2.099 (16) | 2.9408 (8) | 151.1 (12) |
Symmetry codes: (i) ; (ii) .