| Literature DB >> 26279881 |
José A Fernandes1, Bing Liu2, João P C Tomé3, Luís Cunha-Silva2, Filipe A Almeida Paz1.
Abstract
Both the 3-amino-2H,4H-1,2,4-triazolium cation and the pyrazine-2-carboxyl-ate anion in the title salt, C2H5N4 (+)·C5H3N2O2 (-), were formed by an unexpected deca-rboxylation reaction, from 5-amino-1H-1,2,4-triazole-3-carb-oxy-lic acid and pyrazine-2,3-di-carb-oxy-lic acid, respectively. The dihedral angle between the pyrazine ring (r.m.s. deviation = 0.008 Å) and the carboxyl-ate group in the anion is 3.7 (3)°. The extended structure of the salt contains a supra-molecular zigzag tape in which cations and anions are engaged in strong and highly directional N-H⋯N,O hydrogen bonds, forming R 2 (2)(8) and R 2 (2)(9) graph-set motifs. The packing between the tapes is mediated by π-π stacking inter-actions between the triazole and pyrazine rings.Entities:
Keywords: crystal structure; decarboxylation; hydrogen bonding; ionothermal synthesis; triazolium salt; π–π stacking interactions
Year: 2015 PMID: 26279881 PMCID: PMC4518908 DOI: 10.1107/S205698901501172X
Source DB: PubMed Journal: Acta Crystallogr E Crystallogr Commun
Figure 1The asymmetric unit of the title salt. Non-H atoms are represented as displacement ellipsoids drawn at the 50% probability level, while H atoms are depicted as small spheres with arbitrary radii. The atomic labelling scheme for all non-H atoms is provided. Hydrogen bonds are represented as dashed lines.
Hydrogen-bond geometry (, )
|
|
| H |
|
|
|---|---|---|---|---|
| N4H4 | 0.90(1) | 1.77(1) | 2.655(3) | 166(3) |
| N5H5O1i | 0.90(1) | 1.73(1) | 2.632(3) | 176(3) |
| N6H6 | 0.90(1) | 1.97(1) | 2.853(3) | 169(3) |
| N6H6 | 0.90(1) | 2.21(1) | 3.099(3) | 169(3) |
Symmetry code: (i) .
Figure 2Supramolecular tape running parallel to the [010] direction of the unit cell. N—H⋯N and N—H⋯N hydrogen bonds are depicted as dashed aqua and pink lines, respectively. Graph-set motifs present in the structure are highlighted. For geometric details of the represented supramolecular contacts, see Table 1 ▸. π–π stacking interactions between two adjacent supramolecular tapes are shown as orange dashed lines.
Experimental details
| Crystal data | |
| Chemical formula | C2H5N4 +C5H3N2O2 |
|
| 208.19 |
| Crystal system, space group | Monoclinic, |
| Temperature (K) | 296 |
|
| 7.0599(5), 12.1868(8), 10.8385(6) |
| () | 103.593(4) |
|
| 906.40(10) |
|
| 4 |
| Radiation type | Mo |
| (mm1) | 0.12 |
| Crystal size (mm) | 0.09 0.04 0.03 |
| Data collection | |
| Diffractometer | Bruker X8 Kappa CCD APEXII |
| Absorption correction | Multi-scan ( |
|
| 0.989, 0.997 |
| No. of measured, independent and observed [ | 12089, 1858, 1037 |
|
| 0.077 |
| (sin /)max (1) | 0.625 |
| Refinement | |
|
| 0.059, 0.133, 1.02 |
| No. of reflections | 1858 |
| No. of parameters | 148 |
| No. of restraints | 5 |
| H-atom treatment | H atoms treated by a mixture of independent and constrained refinement |
| max, min (e 3) | 0.19, 0.20 |
Computer programs: APEX2 (Bruker, 2006 ▸), SAINT-Plus (Bruker, 2005 ▸), SHELXS97 and SHELXTL (Sheldrick, 2008 ▸), SHELXL2014 (Sheldrick, 2015 ▸) and DIAMOND (Brandenburg, 2009 ▸).
| C2H5N4+·C5H3N2O2− | |
| Monoclinic, | Mo |
| Cell parameters from 1298 reflections | |
| θ = 2.6–19.7° | |
| µ = 0.12 mm−1 | |
| β = 103.593 (4)° | |
| Block, colourless | |
| 0.09 × 0.04 × 0.03 mm |
| Bruker X8 Kappa CCD APEXII diffractometer | 1037 reflections with |
| Radiation source: fine-focus sealed tube | |
| ω / φ scans | θmax = 26.4°, θmin = 2.6° |
| Absorption correction: multi-scan ( | |
| 12089 measured reflections | |
| 1858 independent reflections |
| Refinement on | 5 restraints |
| Least-squares matrix: full | Hydrogen site location: mixed |
| H atoms treated by a mixture of independent and constrained refinement | |
| (Δ/σ)max < 0.001 | |
| 1858 reflections | Δρmax = 0.19 e Å−3 |
| 148 parameters | Δρmin = −0.20 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. |
| N1 | 0.2890 (3) | 0.79063 (17) | 0.49872 (19) | 0.0389 (6) | |
| N2 | 0.0664 (3) | 0.79145 (18) | 0.2472 (2) | 0.0468 (6) | |
| C1 | 0.2177 (4) | 0.8840 (2) | 0.4404 (2) | 0.0334 (6) | |
| C2 | 0.1066 (4) | 0.8815 (2) | 0.3165 (2) | 0.0412 (7) | |
| H2 | 0.0571 | 0.9476 | 0.2797 | 0.049* | |
| C3 | 0.1381 (4) | 0.6995 (2) | 0.3059 (2) | 0.0448 (7) | |
| H3 | 0.1147 | 0.6334 | 0.2623 | 0.054* | |
| C4 | 0.2461 (4) | 0.6993 (2) | 0.4297 (3) | 0.0442 (7) | |
| H4 | 0.2912 | 0.6326 | 0.4668 | 0.053* | |
| C5 | 0.2560 (4) | 0.9921 (2) | 0.5101 (2) | 0.0378 (7) | |
| O1 | 0.1745 (3) | 1.07442 (14) | 0.45075 (15) | 0.0481 (6) | |
| O2 | 0.3628 (3) | 0.99415 (14) | 0.61986 (16) | 0.0543 (6) | |
| N3 | 0.7128 (4) | 0.94320 (19) | 0.8957 (2) | 0.0622 (8) | |
| N4 | 0.6167 (4) | 0.88117 (19) | 0.7929 (2) | 0.0476 (6) | |
| H4A | 0.535 (3) | 0.912 (2) | 0.7253 (18) | 0.071* | |
| N5 | 0.7480 (3) | 0.76575 (18) | 0.93596 (19) | 0.0417 (6) | |
| H5 | 0.778 (4) | 0.6996 (13) | 0.972 (2) | 0.063* | |
| N6 | 0.5628 (4) | 0.6942 (2) | 0.7405 (2) | 0.0540 (7) | |
| H6A | 0.473 (3) | 0.714 (2) | 0.6709 (19) | 0.081* | |
| H6B | 0.585 (5) | 0.6271 (13) | 0.775 (3) | 0.081* | |
| C6 | 0.6369 (4) | 0.7751 (2) | 0.8181 (2) | 0.0365 (7) | |
| C7 | 0.7892 (5) | 0.8695 (2) | 0.9782 (3) | 0.0553 (8) | |
| H7 | 0.8649 | 0.8861 | 1.0584 | 0.066* |
| N1 | 0.0450 (14) | 0.0290 (13) | 0.0400 (12) | −0.0006 (11) | 0.0049 (10) | 0.0005 (10) |
| N2 | 0.0557 (16) | 0.0387 (14) | 0.0406 (12) | 0.0008 (12) | 0.0005 (11) | −0.0086 (12) |
| C1 | 0.0331 (15) | 0.0309 (15) | 0.0355 (13) | −0.0004 (13) | 0.0067 (11) | 0.0022 (12) |
| C2 | 0.0495 (18) | 0.0320 (16) | 0.0367 (14) | 0.0061 (14) | −0.0007 (13) | 0.0020 (12) |
| C3 | 0.0487 (19) | 0.0352 (17) | 0.0478 (16) | −0.0016 (15) | 0.0059 (14) | −0.0099 (13) |
| C4 | 0.0499 (18) | 0.0299 (16) | 0.0497 (16) | 0.0036 (14) | 0.0056 (14) | 0.0028 (13) |
| C5 | 0.0420 (17) | 0.0344 (16) | 0.0330 (13) | 0.0001 (14) | 0.0006 (12) | 0.0036 (12) |
| O1 | 0.0625 (14) | 0.0319 (11) | 0.0402 (10) | 0.0058 (9) | −0.0074 (9) | 0.0021 (8) |
| O2 | 0.0708 (14) | 0.0375 (12) | 0.0399 (10) | 0.0067 (10) | −0.0165 (10) | −0.0025 (9) |
| N3 | 0.089 (2) | 0.0419 (15) | 0.0461 (14) | 0.0029 (15) | −0.0032 (13) | 0.0024 (12) |
| N4 | 0.0625 (18) | 0.0367 (15) | 0.0386 (13) | 0.0037 (13) | 0.0019 (12) | 0.0061 (11) |
| N5 | 0.0480 (14) | 0.0362 (15) | 0.0359 (12) | 0.0025 (12) | −0.0004 (11) | 0.0083 (11) |
| N6 | 0.0607 (18) | 0.0440 (16) | 0.0491 (15) | −0.0005 (15) | −0.0038 (13) | 0.0030 (13) |
| C6 | 0.0391 (17) | 0.0349 (18) | 0.0348 (13) | 0.0044 (13) | 0.0068 (12) | 0.0057 (12) |
| C7 | 0.074 (2) | 0.046 (2) | 0.0383 (15) | 0.0020 (17) | −0.0026 (15) | 0.0012 (14) |
| N1—C4 | 1.335 (3) | N3—C7 | 1.293 (3) |
| N1—C1 | 1.341 (3) | N3—N4 | 1.384 (3) |
| N2—C2 | 1.323 (3) | N4—C6 | 1.322 (3) |
| N2—C3 | 1.328 (3) | N4—H4A | 0.902 (10) |
| C1—C2 | 1.387 (3) | N5—C6 | 1.338 (3) |
| C1—C5 | 1.512 (3) | N5—C7 | 1.353 (3) |
| C2—H2 | 0.9300 | N5—H5 | 0.901 (10) |
| C3—C4 | 1.379 (4) | N6—C6 | 1.321 (3) |
| C3—H3 | 0.9300 | N6—H6A | 0.899 (10) |
| C4—H4 | 0.9300 | N6—H6B | 0.896 (10) |
| C5—O2 | 1.250 (2) | C7—H7 | 0.9300 |
| C5—O1 | 1.256 (3) | ||
| C4—N1—C1 | 115.6 (2) | C7—N3—N4 | 102.9 (2) |
| C2—N2—C3 | 114.9 (2) | C6—N4—N3 | 111.1 (2) |
| N1—C1—C2 | 120.2 (2) | C6—N4—H4A | 126 (2) |
| N1—C1—C5 | 120.1 (2) | N3—N4—H4A | 121.7 (19) |
| C2—C1—C5 | 119.8 (2) | C6—N5—C7 | 105.9 (2) |
| N2—C2—C1 | 124.4 (2) | C6—N5—H5 | 121.3 (18) |
| N2—C2—H2 | 117.8 | C7—N5—H5 | 132.7 (18) |
| C1—C2—H2 | 117.8 | C6—N6—H6A | 115 (2) |
| N2—C3—C4 | 122.0 (2) | C6—N6—H6B | 115 (2) |
| N2—C3—H3 | 119.0 | H6A—N6—H6B | 128 (3) |
| C4—C3—H3 | 119.0 | N6—C6—N4 | 126.2 (2) |
| N1—C4—C3 | 123.0 (2) | N6—C6—N5 | 126.9 (2) |
| N1—C4—H4 | 118.5 | N4—C6—N5 | 106.9 (2) |
| C3—C4—H4 | 118.5 | N3—C7—N5 | 113.2 (2) |
| O2—C5—O1 | 125.0 (2) | N3—C7—H7 | 123.4 |
| O2—C5—C1 | 119.3 (2) | N5—C7—H7 | 123.4 |
| O1—C5—C1 | 115.7 (2) | ||
| C4—N1—C1—C2 | 0.3 (4) | N1—C1—C5—O1 | −176.1 (2) |
| C4—N1—C1—C5 | 179.5 (2) | C2—C1—C5—O1 | 3.1 (4) |
| C3—N2—C2—C1 | 1.2 (4) | C7—N3—N4—C6 | 0.8 (3) |
| N1—C1—C2—N2 | −1.4 (4) | N3—N4—C6—N6 | 179.8 (3) |
| C5—C1—C2—N2 | 179.4 (2) | N3—N4—C6—N5 | −0.9 (3) |
| C2—N2—C3—C4 | −0.1 (4) | C7—N5—C6—N6 | 179.9 (3) |
| C1—N1—C4—C3 | 0.8 (4) | C7—N5—C6—N4 | 0.6 (3) |
| N2—C3—C4—N1 | −1.0 (4) | N4—N3—C7—N5 | −0.4 (4) |
| N1—C1—C5—O2 | 3.7 (4) | C6—N5—C7—N3 | −0.1 (4) |
| C2—C1—C5—O2 | −177.1 (2) |
| H··· | ||||
| N4—H4 | 0.90 (1) | 1.77 (1) | 2.655 (3) | 166 (3) |
| N5—H5···O1i | 0.90 (1) | 1.73 (1) | 2.632 (3) | 176 (3) |
| N6—H6 | 0.90 (1) | 1.97 (1) | 2.853 (3) | 169 (3) |
| N6—H6 | 0.90 (1) | 2.21 (1) | 3.099 (3) | 169 (3) |