| Literature DB >> 21582305 |
L Yu Izotova, J M Ashurov, B T Ibragimov, E Weber.
Abstract
During an attempt to prepare a cocrystal of N-phenyl-phthalimide, C(14)H(9)NO(2), with N-(2,3,4,5,6-penta-fluoro-phen-yl)phthalimide, a new ortho-rhom-bic polymorph of the first component was obtained. This new form has Z' = 0.5 and the mol-ecule is located around a twofold axis, whereas in the previously reported polymorph (space group Pbca), the mol-ecule has no crystallographically imposed symmetry. Pairs of C-H⋯O inter-actions between inversion-related phthalimide units arrange mol-ecules into tapes that are further assembled into (010) layers via stacking inter-actions between phthalimide fragments [inter-planar distance = 3.37 (5) Å].Entities:
Year: 2009 PMID: 21582305 PMCID: PMC2968531 DOI: 10.1107/S1600536809006746
Source DB: PubMed Journal: Acta Crystallogr Sect E Struct Rep Online ISSN: 1600-5368
| C14H9NO2 | |
| Orthorhombic, | Mo |
| Hall symbol: -P 2n 2ab | Cell parameters from 25 reflections |
| θ = 10–25° | |
| µ = 0.10 mm−1 | |
| Needle, colourless | |
| 0.2 × 0.05 × 0.05 mm |
| Stoe Stadi-4 diffractometer | |
| Radiation source: fine-focus sealed tube | θmax = 26.0°, θmin = 1.7° |
| graphite | |
| ω–2τ scans | |
| 1039 measured reflections | |
| 1039 independent reflections | 3 standard reflections every 60 reflections |
| 662 reflections with | intensity decay: 3.9% |
| Refinement on | Secondary atom site location: difference Fourier map |
| Least-squares matrix: full | Hydrogen site location: inferred from neighbouring sites |
| H-atom parameters constrained | |
| (Δ/σ)max < 0.001 | |
| 1039 reflections | Δρmax = 0.17 e Å−3 |
| 80 parameters | Δρmin = −0.15 e Å−3 |
| 0 restraints | Extinction correction: |
| Primary atom site location: structure-invariant direct methods | Extinction coefficient: 0.0123 (18) |
| 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. |
| Refinement. Refinement of |
| N1 | 0.0000 | 0.39051 (14) | 0.2500 | 0.0475 (9) | |
| O1 | 0.3444 (4) | 0.40588 (9) | 0.0909 (3) | 0.0624 (7) | |
| C1 | 0.1048 (7) | 0.58237 (14) | 0.2026 (4) | 0.0740 (12) | |
| H1 | 0.1731 | 0.6164 | 0.1709 | 0.089* | |
| C2 | 0.2140 (6) | 0.53244 (14) | 0.1544 (4) | 0.0626 (10) | |
| H2 | 0.3548 | 0.5324 | 0.0916 | 0.075* | |
| C3 | 0.1056 (5) | 0.48304 (12) | 0.2034 (3) | 0.0491 (8) | |
| C4 | 0.1752 (6) | 0.42378 (12) | 0.1702 (4) | 0.0479 (8) | |
| C5 | 0.0000 | 0.33042 (18) | 0.2500 | 0.0498 (11) | |
| C6 | 0.1868 (6) | 0.30175 (13) | 0.3253 (4) | 0.0601 (9) | |
| H6 | 0.3125 | 0.3213 | 0.3754 | 0.072* | |
| C7 | 0.1855 (6) | 0.24375 (14) | 0.3257 (5) | 0.0765 (12) | |
| H7 | 0.3099 | 0.2241 | 0.3771 | 0.092* | |
| C8 | 0.0000 | 0.2150 (2) | 0.2500 | 0.0820 (19) | |
| H8 | 0.0000 | 0.1759 | 0.2500 | 0.098* |
| N1 | 0.044 (2) | 0.049 (2) | 0.049 (2) | 0.000 | 0.0052 (18) | 0.000 |
| O1 | 0.0502 (13) | 0.0738 (15) | 0.0631 (15) | 0.0017 (12) | 0.0078 (12) | 0.0049 (12) |
| C1 | 0.088 (3) | 0.0545 (19) | 0.079 (3) | −0.0123 (18) | −0.033 (2) | 0.0080 (18) |
| C2 | 0.063 (2) | 0.066 (2) | 0.059 (2) | −0.0128 (18) | −0.0198 (18) | 0.0059 (18) |
| C3 | 0.0502 (17) | 0.0543 (18) | 0.0427 (18) | −0.0033 (14) | −0.0134 (15) | 0.0018 (14) |
| C4 | 0.0409 (16) | 0.0589 (19) | 0.0438 (17) | −0.0017 (16) | −0.0061 (15) | 0.0036 (15) |
| C5 | 0.048 (2) | 0.050 (3) | 0.052 (3) | 0.000 | 0.003 (2) | 0.000 |
| C6 | 0.0476 (18) | 0.062 (2) | 0.070 (2) | 0.0027 (17) | −0.0001 (18) | 0.0049 (18) |
| C7 | 0.057 (2) | 0.067 (2) | 0.106 (3) | 0.013 (2) | 0.011 (2) | 0.018 (2) |
| C8 | 0.058 (3) | 0.057 (3) | 0.130 (5) | 0.000 | 0.033 (4) | 0.000 |
| N1—C4i | 1.408 (3) | C3—C4 | 1.487 (4) |
| N1—C4 | 1.408 (3) | C5—C6 | 1.380 (4) |
| N1—C5 | 1.430 (5) | C5—C6i | 1.380 (4) |
| O1—C4 | 1.211 (3) | C6—C7 | 1.380 (4) |
| C1—C2 | 1.389 (4) | C6—H6 | 0.9300 |
| C1—C1i | 1.389 (8) | C7—C8 | 1.378 (4) |
| C1—H1 | 0.9300 | C7—H7 | 0.9300 |
| C2—C3 | 1.378 (4) | C8—C7i | 1.378 (4) |
| C2—H2 | 0.9300 | C8—H8 | 0.9300 |
| C3—C3i | 1.389 (6) | ||
| C4i—N1—C4 | 111.6 (4) | N1—C4—C3 | 105.8 (3) |
| C4i—N1—C5 | 124.22 (18) | C6—C5—C6i | 120.7 (4) |
| C4—N1—C5 | 124.22 (18) | C6—C5—N1 | 119.6 (2) |
| C2—C1—C1i | 121.2 (2) | C6i—C5—N1 | 119.6 (2) |
| C2—C1—H1 | 119.4 | C7—C6—C5 | 119.5 (4) |
| C1i—C1—H1 | 119.4 | C7—C6—H6 | 120.3 |
| C3—C2—C1 | 117.4 (3) | C5—C6—H6 | 120.3 |
| C3—C2—H2 | 121.3 | C8—C7—C6 | 120.0 (4) |
| C1—C2—H2 | 121.3 | C8—C7—H7 | 120.0 |
| C2—C3—C3i | 121.4 (2) | C6—C7—H7 | 120.0 |
| C2—C3—C4 | 130.2 (3) | C7—C8—C7i | 120.3 (5) |
| C3i—C3—C4 | 108.40 (16) | C7—C8—H8 | 119.8 |
| O1—C4—N1 | 125.2 (3) | C7i—C8—H8 | 119.8 |
| O1—C4—C3 | 129.0 (3) |