| Literature DB >> 25309239 |
Laurette Schmitt1, Helen Stoeckli-Evans1.
Abstract
The heterocyclic molecule in the title solvate, C16H14N4·2CHCl3, possesses inversion symmetry, with the inversion centre situated at the centre of the pyrazine ring. The outer pyridine rings are inclined to the central pyrazine ring by 4.89 (9)°. The compound crystallized as a chloro-form disolvate with the solvent mol-ecules linked to the title mol-ecule by C-H⋯N hydrogen bonds. In the crystal, mol-ecules are further linked by π-π inter-actions involving the pyrazine and pyridine rings of neighbouring mol-ecules [inter-centroid distance = 3.5629 (12) Å; symmetry code: x, y + 1, z + 1].Entities:
Keywords: bis(2-pyridyl)pyrazine; crystal structure; pyrazine; pyridine; solvate
Year: 2014 PMID: 25309239 PMCID: PMC4186168 DOI: 10.1107/S1600536814009544
Source DB: PubMed Journal: Acta Crystallogr Sect E Struct Rep Online ISSN: 1600-5368
| C16H14N4·2CHCl3 | |
| Monoclinic, | Mo |
| Cell parameters from 12496 reflections | |
| θ = 1.5–25.6° | |
| µ = 0.81 mm−1 | |
| β = 93.885 (9)° | |
| Rod, colourless | |
| 0.45 × 0.29 × 0.23 mm |
| Stoe IPDS 2 diffractometer | 1902 independent reflections |
| Radiation source: fine-focus sealed tube | 1676 reflections with |
| Plane graphite monochromator | |
| φ + ω scans | θmax = 25.2°, θmin = 1.9° |
| Absorption correction: multi-scan ( | |
| 9566 measured reflections |
| Refinement on | Hydrogen site location: inferred from neighbouring sites |
| Least-squares matrix: full | H-atom parameters constrained |
| (Δ/σ)max = 0.002 | |
| Δρmax = 0.31 e Å−3 | |
| 1902 reflections | Δρmin = −0.30 e Å−3 |
| 129 parameters | Extinction correction: |
| 0 restraints | Extinction coefficient: 0.0064 (11) |
| 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. |
| N1 | 0.72397 (10) | 0.6344 (3) | 0.19653 (8) | 0.0368 (4) | |
| N2 | 0.89303 (10) | 0.2947 (3) | 0.25318 (8) | 0.0394 (4) | |
| C1 | 0.68638 (12) | 0.8157 (3) | 0.21400 (9) | 0.0374 (4) | |
| H1 | 0.6406 | 0.8677 | 0.1890 | 0.045* | |
| C2 | 0.78878 (11) | 0.5676 (3) | 0.23260 (8) | 0.0328 (4) | |
| C3 | 0.83238 (11) | 0.3674 (3) | 0.21341 (9) | 0.0328 (4) | |
| C4 | 0.93307 (13) | 0.1154 (3) | 0.23585 (10) | 0.0418 (5) | |
| H4 | 0.9771 | 0.0635 | 0.2627 | 0.050* | |
| C5 | 0.91455 (13) | 0.0006 (3) | 0.18141 (10) | 0.0401 (5) | |
| H5 | 0.9446 | −0.1274 | 0.1720 | 0.048* | |
| C6 | 0.85181 (12) | 0.0739 (3) | 0.14075 (9) | 0.0376 (5) | |
| C7 | 0.81112 (11) | 0.2637 (3) | 0.15755 (9) | 0.0378 (5) | |
| H7 | 0.7685 | 0.3224 | 0.1305 | 0.045* | |
| C8 | 0.82828 (15) | −0.0466 (4) | 0.08138 (11) | 0.0510 (6) | |
| H8A | 0.7910 | −0.1672 | 0.0898 | 0.077* | |
| H8B | 0.8772 | −0.1066 | 0.0642 | 0.077* | |
| H8C | 0.8012 | 0.0556 | 0.0515 | 0.077* | |
| Cl1 | 0.50499 (4) | 0.55130 (10) | 0.09961 (3) | 0.0569 (2) | |
| Cl2 | 0.65296 (4) | 0.52518 (12) | 0.03495 (3) | 0.0617 (3) | |
| Cl3 | 0.57200 (4) | 0.12697 (10) | 0.06982 (3) | 0.0582 (2) | |
| C10 | 0.59461 (13) | 0.4006 (3) | 0.09061 (10) | 0.0416 (5) | |
| H10 | 0.6275 | 0.3999 | 0.1312 | 0.050* |
| N1 | 0.0398 (9) | 0.0332 (9) | 0.0377 (9) | −0.0008 (7) | 0.0045 (7) | −0.0041 (7) |
| N2 | 0.0429 (9) | 0.0351 (9) | 0.0405 (9) | 0.0005 (7) | 0.0053 (7) | −0.0032 (7) |
| C1 | 0.0404 (10) | 0.0333 (10) | 0.0385 (10) | −0.0002 (8) | 0.0035 (8) | −0.0027 (8) |
| C2 | 0.0356 (10) | 0.0294 (10) | 0.0340 (10) | −0.0039 (8) | 0.0075 (7) | 0.0008 (8) |
| C3 | 0.0343 (9) | 0.0290 (9) | 0.0358 (10) | −0.0042 (7) | 0.0090 (7) | −0.0001 (7) |
| C4 | 0.0467 (11) | 0.0374 (11) | 0.0417 (11) | 0.0052 (9) | 0.0054 (8) | −0.0004 (8) |
| C5 | 0.0460 (11) | 0.0326 (10) | 0.0433 (11) | 0.0022 (8) | 0.0140 (9) | −0.0003 (8) |
| C6 | 0.0424 (10) | 0.0343 (10) | 0.0377 (10) | −0.0038 (8) | 0.0136 (8) | −0.0047 (8) |
| C7 | 0.0388 (10) | 0.0381 (11) | 0.0372 (10) | −0.0011 (8) | 0.0077 (8) | −0.0025 (8) |
| C8 | 0.0578 (13) | 0.0499 (13) | 0.0460 (12) | 0.0046 (10) | 0.0076 (10) | −0.0152 (10) |
| Cl1 | 0.0557 (4) | 0.0538 (4) | 0.0613 (4) | 0.0130 (3) | 0.0040 (3) | −0.0024 (3) |
| Cl2 | 0.0589 (4) | 0.0759 (5) | 0.0507 (4) | −0.0204 (3) | 0.0069 (3) | 0.0140 (3) |
| Cl3 | 0.0758 (5) | 0.0417 (4) | 0.0594 (4) | −0.0037 (3) | 0.0207 (3) | −0.0062 (2) |
| C10 | 0.0449 (11) | 0.0426 (11) | 0.0376 (11) | −0.0012 (9) | 0.0041 (8) | 0.0024 (9) |
| N1—C1 | 1.329 (3) | C5—H5 | 0.9500 |
| N1—C2 | 1.340 (3) | C6—C7 | 1.393 (3) |
| N2—C4 | 1.339 (3) | C6—C8 | 1.504 (3) |
| N2—C3 | 1.346 (3) | C7—H7 | 0.9500 |
| C1—C2i | 1.391 (3) | C8—H8A | 0.9800 |
| C1—H1 | 0.9500 | C8—H8B | 0.9800 |
| C2—C1i | 1.391 (3) | C8—H8C | 0.9800 |
| C2—C3 | 1.484 (3) | Cl1—C10 | 1.757 (2) |
| C3—C7 | 1.385 (3) | Cl2—C10 | 1.760 (2) |
| C4—C5 | 1.383 (3) | Cl3—C10 | 1.753 (2) |
| C4—H4 | 0.9500 | C10—H10 | 1.0000 |
| C5—C6 | 1.383 (3) | ||
| C1—N1—C2 | 116.90 (17) | C5—C6—C8 | 121.56 (19) |
| C4—N2—C3 | 116.44 (17) | C7—C6—C8 | 121.58 (19) |
| N1—C1—C2i | 122.74 (18) | C3—C7—C6 | 120.36 (18) |
| N1—C1—H1 | 118.6 | C3—C7—H7 | 119.8 |
| C2i—C1—H1 | 118.6 | C6—C7—H7 | 119.8 |
| N1—C2—C1i | 120.36 (17) | C6—C8—H8A | 109.5 |
| N1—C2—C3 | 117.77 (16) | C6—C8—H8B | 109.5 |
| C1i—C2—C3 | 121.87 (17) | H8A—C8—H8B | 109.5 |
| N2—C3—C7 | 122.68 (17) | C6—C8—H8C | 109.5 |
| N2—C3—C2 | 116.19 (16) | H8A—C8—H8C | 109.5 |
| C7—C3—C2 | 121.13 (17) | H8B—C8—H8C | 109.5 |
| N2—C4—C5 | 124.3 (2) | Cl3—C10—Cl1 | 110.88 (12) |
| N2—C4—H4 | 117.9 | Cl3—C10—Cl2 | 110.37 (12) |
| C5—C4—H4 | 117.9 | Cl1—C10—Cl2 | 110.64 (12) |
| C6—C5—C4 | 119.35 (19) | Cl3—C10—H10 | 108.3 |
| C6—C5—H5 | 120.3 | Cl1—C10—H10 | 108.3 |
| C4—C5—H5 | 120.3 | Cl2—C10—H10 | 108.3 |
| C5—C6—C7 | 116.86 (18) | ||
| C2—N1—C1—C2i | −0.8 (3) | C3—N2—C4—C5 | −1.7 (3) |
| C1—N1—C2—C1i | 0.7 (3) | N2—C4—C5—C6 | 1.2 (3) |
| C1—N1—C2—C3 | −179.12 (16) | C4—C5—C6—C7 | 0.6 (3) |
| C4—N2—C3—C7 | 0.5 (3) | C4—C5—C6—C8 | −179.05 (19) |
| C4—N2—C3—C2 | −179.40 (16) | N2—C3—C7—C6 | 1.2 (3) |
| N1—C2—C3—N2 | −174.82 (17) | C2—C3—C7—C6 | −178.94 (16) |
| C1i—C2—C3—N2 | 5.3 (3) | C5—C6—C7—C3 | −1.7 (3) |
| N1—C2—C3—C7 | 5.3 (3) | C8—C6—C7—C3 | 177.96 (19) |
| C1i—C2—C3—C7 | −174.56 (18) |
| H··· | ||||
| C10—H10···N1 | 1.00 | 2.50 | 3.335 (3) | 141 |
Hydrogen-bond geometry (Å, °)
|
|
| H⋯ |
|
|
|---|---|---|---|---|
| C10—H10⋯N1 | 1.00 | 2.50 | 3.335 (3) | 141 |