| Literature DB >> 31417799 |
Batirbay Torambetov1, Shaxnoza Kadirova1, Turdibek Toshmurodov2, Jamshid Mengnorovich Ashurov3, Nusrat Agzamovich Parpiev1, Abdukhakim Ziyaev2.
Abstract
The reaction of 2-methyl-thio-5-amino-1,3,4-thia-diazole (Me-SNTD; C3H5N3S2) with copper(II) acetate monohydrate [Cu(OAc)2·H2O; C4H8CuO5] resulted in the formation of the title binuclear compound, [Cu2(C2H3O2)4(C3H5N3S2)2] or [Cu2(OAc)4(Me-SNTD)2]. The structure has triclinic (P ) symmetry with a crystallographic inversion centre located at the midpoint of the line connecting the Cu atoms in the dimer. These two Cu atoms of the dimer [Cu⋯Cu = 2.6727 (6) Å] are held together by four carboxyl-ate groups. Each Cu atom is further coordinated to the N atom of an Me-SNTD mol-ecule and exhibits a Jahn-Teller-distorted octa-hedral geometry. The dimers are connected into infinite chains by hydrogen bonds between the NH (Me-SNTD) and the carboxyl-ate groups of neighbouring mol-ecules, generating an R 2 2(12) ring motif. The mol-ecules are further linked by C-H⋯π inter-actions between the thia-diazole rings and the methyl groups of the acetate units.Entities:
Keywords: copper(II); crystal structure; hydrogen bonding.; thiadiazole
Year: 2019 PMID: 31417799 PMCID: PMC6690473 DOI: 10.1107/S2056989019010272
Source DB: PubMed Journal: Acta Crystallogr E Crystallogr Commun
Figure 1The molecular structure of [Cu2(OAc)4(Me-SNTD)2] with the atom-numbering scheme. Displacement ellipsoids are drawn at the 25% probability level. Intramolecular hydrogen bonds are shown as dashed lines. Atoms labelled with the suffix A are generated by the symmetry operation 2 − x, 1 − y, 1 − z.
Hydrogen-bond geometry (Å, °)
Cg is the centroid of the S1/N1/N2/C1/C2 ring.
|
|
| H⋯ |
|
|
|---|---|---|---|---|
| N3—H3 | 0.86 (1) | 2.16 (2) | 2.963 (4) | 156 (4) |
| N3—H3 | 0.86 (1) | 2.11 (3) | 2.884 (4) | 150 (4) |
Symmetry codes: (i) ; (ii) .
Figure 2Part of the crystal structure with hydrogen bonds shown as dashed lines. For clarity, H atoms not involved in hydrogen bonding are omitted.
Figure 3Packing of the structural units in (I). Hydrogen bonds are indicated by blue dashed lines and C—H⋯π interactions by black dashed lines.
Experimental details
| Crystal data | |
| Chemical formula | [Cu2(C2H3O2)4(C3H5N3S2)2] |
|
| 657.69 |
| Crystal system, space group | Triclinic, |
| Temperature (K) | 571 |
|
| 8.1069 (4), 8.8955 (4), 9.0421 (5) |
| α, β, γ (°) | 100.656 (4), 98.966 (4), 97.643 (4) |
|
| 624.14 (5) |
|
| 1 |
| Radiation type | Cu |
| μ (mm−1) | 5.70 |
| Crystal size (mm) | 0.44 × 0.38 × 0.28 |
| Data collection | |
| Diffractometer | Rigaku Oxford Diffraction Xcalibur, Ruby |
| Absorption correction | Multi-scan ( |
|
| 0.083, 1.000 |
| No. of measured, independent and observed [ | 11239, 2582, 2244 |
|
| 0.052 |
| (sin θ/λ)max (Å−1) | 0.630 |
| Refinement | |
|
| 0.040, 0.118, 1.07 |
| No. of reflections | 2582 |
| No. of parameters | 165 |
| No. of restraints | 2 |
| H-atom treatment | H atoms treated by a mixture of independent and constrained refinement |
| Δρmax, Δρmin (e Å−3) | 0.47, −0.44 |
Computer programs: CrysAlis PRO (Rigaku OD, 2018 ▸), SHELXL (Sheldrick, 2015 ▸) and OLEX2 (Dolomanov et al., 2009 ▸).
| [Cu2(C2H3O2)4(C3H5N3S2)2] | |
| Triclinic, | |
| Cu | |
| Cell parameters from 5762 reflections | |
| θ = 5.0–75.8° | |
| α = 100.656 (4)° | µ = 5.70 mm−1 |
| β = 98.966 (4)° | |
| γ = 97.643 (4)° | Block, blue |
| 0.44 × 0.38 × 0.28 mm |
| Rigaku Oxford Diffraction Xcalibur, Ruby diffractometer | 2582 independent reflections |
| Radiation source: fine-focus sealed X-ray tube, Enhance (Cu) X-ray Source | 2244 reflections with |
| Graphite monochromator | |
| Detector resolution: 10.2576 pixels mm-1 | θmax = 76.2°, θmin = 5.1° |
| ω scans | |
| Absorption correction: multi-scan (CrysAlisPro; Rigaku OD, 2018) | |
| 11239 measured reflections |
| Refinement on | 2 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 | |
| 2582 reflections | Δρmax = 0.47 e Å−3 |
| 165 parameters | Δρmin = −0.44 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. |
| Cu1 | 0.94133 (5) | 0.41682 (4) | 0.59528 (5) | 0.03080 (16) | |
| S1 | 0.77895 (10) | 0.21114 (9) | 1.00281 (9) | 0.0416 (2) | |
| S2 | 0.42143 (12) | 0.08505 (14) | 0.83586 (12) | 0.0659 (3) | |
| O4 | 1.0956 (3) | 0.3780 (2) | 0.2926 (2) | 0.0403 (5) | |
| O2 | 0.8200 (3) | 0.5370 (3) | 0.2953 (3) | 0.0409 (5) | |
| O1 | 0.7249 (3) | 0.3994 (3) | 0.4563 (3) | 0.0458 (5) | |
| O3 | 1.0032 (3) | 0.2430 (2) | 0.4575 (3) | 0.0438 (5) | |
| N3 | 1.0840 (4) | 0.3406 (3) | 0.9585 (3) | 0.0442 (6) | |
| N2 | 0.8489 (3) | 0.2883 (3) | 0.7575 (3) | 0.0354 (5) | |
| N1 | 0.6790 (3) | 0.2193 (3) | 0.7215 (3) | 0.0385 (6) | |
| C1 | 0.9196 (4) | 0.2903 (3) | 0.8988 (3) | 0.0327 (6) | |
| C6 | 1.0679 (4) | 0.2556 (3) | 0.3428 (3) | 0.0363 (6) | |
| C4 | 0.7032 (4) | 0.4586 (3) | 0.3410 (4) | 0.0367 (6) | |
| C2 | 0.6271 (4) | 0.1756 (3) | 0.8362 (4) | 0.0383 (6) | |
| C7 | 1.1194 (5) | 0.1119 (4) | 0.2574 (5) | 0.0567 (9) | |
| H7A | 1.106850 | 0.114281 | 0.150585 | 0.085* | |
| H7B | 1.048657 | 0.021473 | 0.270116 | 0.085* | |
| H7C | 1.235495 | 0.108716 | 0.297339 | 0.085* | |
| C5 | 0.5263 (4) | 0.4374 (5) | 0.2518 (5) | 0.0565 (9) | |
| H5A | 0.459075 | 0.495634 | 0.311649 | 0.085* | |
| H5B | 0.477358 | 0.329410 | 0.228270 | 0.085* | |
| H5C | 0.529261 | 0.473477 | 0.158389 | 0.085* | |
| C3 | 0.3241 (6) | 0.0719 (6) | 0.6412 (5) | 0.0740 (13) | |
| H3C | 0.373741 | 0.001172 | 0.574724 | 0.111* | |
| H3D | 0.341504 | 0.172515 | 0.616365 | 0.111* | |
| H3E | 0.204871 | 0.034989 | 0.627943 | 0.111* | |
| H3A | 1.119 (5) | 0.357 (4) | 1.0554 (14) | 0.048 (10)* | |
| H3B | 1.149 (5) | 0.377 (5) | 0.903 (5) | 0.070 (13)* |
| Cu1 | 0.0315 (2) | 0.0301 (2) | 0.0309 (3) | 0.00161 (15) | 0.00874 (17) | 0.00645 (16) |
| S1 | 0.0421 (4) | 0.0494 (4) | 0.0336 (4) | −0.0010 (3) | 0.0112 (3) | 0.0114 (3) |
| S2 | 0.0408 (5) | 0.0941 (7) | 0.0623 (6) | −0.0141 (5) | 0.0082 (4) | 0.0347 (6) |
| O4 | 0.0516 (13) | 0.0353 (10) | 0.0367 (12) | 0.0105 (9) | 0.0164 (10) | 0.0054 (9) |
| O2 | 0.0312 (10) | 0.0497 (11) | 0.0409 (12) | 0.0015 (9) | 0.0043 (9) | 0.0130 (10) |
| O1 | 0.0333 (11) | 0.0572 (13) | 0.0450 (13) | −0.0018 (9) | 0.0039 (9) | 0.0154 (11) |
| O3 | 0.0599 (14) | 0.0309 (9) | 0.0423 (13) | 0.0072 (9) | 0.0171 (11) | 0.0056 (9) |
| N3 | 0.0374 (14) | 0.0580 (16) | 0.0353 (16) | −0.0021 (11) | 0.0051 (12) | 0.0132 (13) |
| N2 | 0.0371 (13) | 0.0357 (11) | 0.0334 (13) | −0.0002 (9) | 0.0077 (10) | 0.0106 (10) |
| N1 | 0.0375 (13) | 0.0409 (12) | 0.0373 (14) | −0.0007 (10) | 0.0072 (11) | 0.0138 (10) |
| C1 | 0.0377 (14) | 0.0286 (11) | 0.0339 (15) | 0.0037 (10) | 0.0127 (12) | 0.0081 (11) |
| C6 | 0.0389 (15) | 0.0318 (13) | 0.0352 (16) | 0.0085 (11) | 0.0027 (12) | 0.0006 (11) |
| C4 | 0.0294 (13) | 0.0399 (14) | 0.0369 (17) | 0.0024 (11) | 0.0060 (12) | 0.0004 (12) |
| C2 | 0.0365 (15) | 0.0382 (14) | 0.0408 (17) | 0.0001 (11) | 0.0084 (13) | 0.0130 (12) |
| C7 | 0.077 (3) | 0.0424 (17) | 0.056 (2) | 0.0278 (17) | 0.0212 (19) | 0.0030 (15) |
| C5 | 0.0329 (16) | 0.075 (2) | 0.059 (2) | 0.0039 (15) | 0.0028 (16) | 0.0144 (19) |
| C3 | 0.053 (2) | 0.093 (3) | 0.067 (3) | −0.015 (2) | −0.004 (2) | 0.024 (2) |
| Cu1—Cu1i | 2.6728 (8) | N3—H3B | 0.856 (10) |
| Cu1—O4i | 2.0007 (19) | N2—N1 | 1.394 (3) |
| Cu1—O2i | 1.983 (2) | N2—C1 | 1.313 (4) |
| Cu1—O1 | 1.962 (2) | N1—C2 | 1.282 (4) |
| Cu1—O3 | 1.970 (2) | C6—C7 | 1.510 (4) |
| Cu1—N2 | 2.180 (2) | C4—C5 | 1.502 (4) |
| S1—C1 | 1.745 (3) | C7—H7A | 0.9600 |
| S1—C2 | 1.740 (3) | C7—H7B | 0.9600 |
| S2—C2 | 1.752 (3) | C7—H7C | 0.9600 |
| S2—C3 | 1.789 (5) | C5—H5A | 0.9600 |
| O4—C6 | 1.262 (4) | C5—H5B | 0.9600 |
| O2—C4 | 1.267 (4) | C5—H5C | 0.9600 |
| O1—C4 | 1.251 (4) | C3—H3C | 0.9600 |
| O3—C6 | 1.249 (4) | C3—H3D | 0.9600 |
| N3—C1 | 1.339 (4) | C3—H3E | 0.9600 |
| N3—H3A | 0.857 (10) | ||
| O4i—Cu1—Cu1i | 83.88 (6) | N2—C1—S1 | 113.1 (2) |
| O4i—Cu1—N2 | 94.39 (9) | N2—C1—N3 | 124.8 (3) |
| O2i—Cu1—Cu1i | 84.10 (7) | O4—C6—C7 | 117.0 (3) |
| O2i—Cu1—O4i | 89.30 (9) | O3—C6—O4 | 125.8 (3) |
| O2i—Cu1—N2 | 94.80 (9) | O3—C6—C7 | 117.2 (3) |
| O1—Cu1—Cu1i | 82.97 (7) | O2—C4—C5 | 117.6 (3) |
| O1—Cu1—O4i | 89.12 (10) | O1—C4—O2 | 124.5 (3) |
| O1—Cu1—O2i | 167.07 (9) | O1—C4—C5 | 117.8 (3) |
| O1—Cu1—O3 | 90.92 (10) | S1—C2—S2 | 119.34 (18) |
| O1—Cu1—N2 | 98.11 (10) | N1—C2—S1 | 115.2 (2) |
| O3—Cu1—Cu1i | 83.44 (7) | N1—C2—S2 | 125.5 (3) |
| O3—Cu1—O4i | 167.22 (9) | C6—C7—H7A | 109.5 |
| O3—Cu1—O2i | 87.81 (10) | C6—C7—H7B | 109.5 |
| O3—Cu1—N2 | 98.26 (9) | C6—C7—H7C | 109.5 |
| N2—Cu1—Cu1i | 177.95 (7) | H7A—C7—H7B | 109.5 |
| C2—S1—C1 | 86.58 (14) | H7A—C7—H7C | 109.5 |
| C2—S2—C3 | 100.75 (18) | H7B—C7—H7C | 109.5 |
| C6—O4—Cu1i | 122.12 (19) | C4—C5—H5A | 109.5 |
| C4—O2—Cu1i | 122.8 (2) | C4—C5—H5B | 109.5 |
| C4—O1—Cu1 | 125.6 (2) | C4—C5—H5C | 109.5 |
| C6—O3—Cu1 | 124.56 (19) | H5A—C5—H5B | 109.5 |
| C1—N3—H3A | 121 (3) | H5A—C5—H5C | 109.5 |
| C1—N3—H3B | 119 (3) | H5B—C5—H5C | 109.5 |
| H3A—N3—H3B | 119 (4) | S2—C3—H3C | 109.5 |
| N1—N2—Cu1 | 116.61 (18) | S2—C3—H3D | 109.5 |
| C1—N2—Cu1 | 128.89 (19) | S2—C3—H3E | 109.5 |
| C1—N2—N1 | 113.1 (2) | H3C—C3—H3D | 109.5 |
| C2—N1—N2 | 112.1 (3) | H3C—C3—H3E | 109.5 |
| N3—C1—S1 | 122.1 (2) | H3D—C3—H3E | 109.5 |
| H··· | ||||
| N3—H3 | 0.86 (1) | 2.16 (2) | 2.963 (4) | 156 (4) |
| N3—H3 | 0.86 (1) | 2.11 (3) | 2.884 (4) | 150 (4) |
| C7—H7 | 0.96 | 3.00 | 3.346 (4) | 103 |