| Literature DB >> 23794992 |
Tarek Ben Rhaiem1, Habib Boughzala, Ahmed Driss.
Abstract
The title salt, (C6H14N2)2[Sb2Cl10]·2H2O, was obtained by slow evaporation of an acidic solution of 1,4-di-aza-bicyclo-[2.2.2]octane and SbCl3. The crystal structure consists of (C6H14N2)(2+) cations, [Sb2Cl10](4-) double octa-hedra and lattice water mol-ecules. All mol-ecular components are situated on special positions. The cation and the lattice water mol-ecule exhibit mirror symmetry, whereas the anion has site symmetry 2/m. The cations, anions and water mol-ecules are alternately arranged into columns along [010]. Individual columns are joined into layers extending along (001). Intra-layer N-H⋯O and inter-layer N-H⋯Cl hydrogen-bonding inter-actions lead to the formation of a three-dimensional network.Entities:
Year: 2013 PMID: 23794992 PMCID: PMC3684890 DOI: 10.1107/S160053681301307X
Source DB: PubMed Journal: Acta Crystallogr Sect E Struct Rep Online ISSN: 1600-5368
| (C6H14N2)2[Sb2Cl10]·2H2O | |
| Melting point: 571 K | |
| Orthorhombic, | Mo |
| Hall symbol: -P 2 2n | Cell parameters from 1700 reflections |
| θ = 2.4–27.0° | |
| µ = 2.81 mm−1 | |
| Prism, colourless | |
| 0.50 × 0.43 × 0.36 mm | |
| Enraf–Nonius CAD-4 diffractometer | 1488 reflections with |
| Radiation source: fine-focus sealed tube | |
| Graphite monochromator | θmax = 27.0°, θmin = 2.4° |
| non–profiled ω/2θ scans | |
| Absorption correction: ψ scan (North | |
| 2797 measured reflections | 2 standard reflections every 120 min |
| 1700 independent reflections | intensity decay: 1% |
| 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 | |
| 1700 reflections | Δρmax = 0.59 e Å−3 |
| 82 parameters | Δρmin = −0.37 e Å−3 |
| 0 restraints | Extinction correction: |
| Primary atom site location: structure-invariant direct methods | Extinction coefficient: 0.0099 (5) |
| Experimental. Number of psi-scan sets used was 5 Theta correction was applied. Averaged transmission function was used. No Fourier smoothing was applied. |
| 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 |
| Occ. (<1) | |||||
| Sb | 0.40193 (3) | 0.407356 (11) | 0.5000 | 0.03327 (11) | |
| Cl1 | 0.16885 (14) | 0.46510 (7) | 0.5000 | 0.0678 (4) | |
| Cl2 | 0.62462 (11) | 0.31027 (6) | 0.5000 | 0.0471 (3) | |
| Cl3 | 0.30372 (8) | 0.33776 (3) | 0.26053 (10) | 0.04669 (19) | |
| Cl4 | 0.5000 | 0.5000 | 0.23812 (14) | 0.0534 (3) | |
| N1 | 0.3554 (4) | 0.20234 (16) | 0.5000 | 0.0406 (8) | |
| H1 | 0.3861 | 0.2438 | 0.5000 | 0.049* | |
| N2 | 0.2710 (4) | 0.09024 (15) | 0.5000 | 0.0443 (8) | |
| H2 | 0.2394 | 0.0489 | 0.5000 | 0.053* | |
| C1 | 0.1931 (4) | 0.20125 (18) | 0.5000 | 0.0433 (9) | |
| H1A | 0.1563 | 0.2231 | 0.3961 | 0.052* | 0.50 |
| H1B | 0.1563 | 0.2231 | 0.6039 | 0.052* | 0.50 |
| C2 | 0.1428 (5) | 0.1332 (2) | 0.5000 | 0.0537 (12) | |
| H2A | 0.0836 | 0.1251 | 0.6039 | 0.064* | 0.50 |
| H2B | 0.0836 | 0.1251 | 0.3961 | 0.064* | 0.50 |
| C3 | 0.4100 (3) | 0.17034 (16) | 0.6617 (5) | 0.0535 (8) | |
| H3A | 0.3730 | 0.1921 | 0.7657 | 0.064* | |
| H3B | 0.5158 | 0.1720 | 0.6646 | 0.064* | |
| C4 | 0.3595 (4) | 0.10141 (15) | 0.6615 (5) | 0.0541 (8) | |
| H4A | 0.4432 | 0.0729 | 0.6626 | 0.065* | |
| H4B | 0.3013 | 0.0929 | 0.7660 | 0.065* | |
| O | 0.3071 (4) | −0.04203 (13) | 0.5000 | 0.0522 (8) |
| Sb | 0.03290 (16) | 0.02973 (15) | 0.03718 (16) | −0.00263 (10) | 0.000 | 0.000 |
| Cl1 | 0.0468 (6) | 0.0716 (8) | 0.0850 (9) | 0.0239 (6) | 0.000 | 0.000 |
| Cl2 | 0.0379 (5) | 0.0543 (6) | 0.0492 (6) | 0.0080 (4) | 0.000 | 0.000 |
| Cl3 | 0.0517 (4) | 0.0401 (4) | 0.0483 (4) | −0.0104 (3) | −0.0131 (3) | 0.0003 (3) |
| Cl4 | 0.0639 (7) | 0.0548 (6) | 0.0414 (5) | 0.0027 (5) | 0.000 | 0.000 |
| N1 | 0.0392 (17) | 0.0292 (15) | 0.053 (2) | −0.0064 (13) | 0.000 | 0.000 |
| N2 | 0.050 (2) | 0.0268 (15) | 0.056 (2) | 0.0011 (14) | 0.000 | 0.000 |
| C1 | 0.036 (2) | 0.0315 (18) | 0.062 (3) | 0.0061 (16) | 0.000 | 0.000 |
| C2 | 0.0314 (19) | 0.039 (2) | 0.091 (4) | −0.0053 (18) | 0.000 | 0.000 |
| C3 | 0.0447 (16) | 0.0601 (19) | 0.0557 (19) | −0.0037 (14) | −0.0143 (15) | −0.0024 (16) |
| C4 | 0.0640 (19) | 0.0475 (16) | 0.0508 (18) | 0.0084 (14) | −0.0059 (17) | 0.0100 (15) |
| O | 0.0487 (17) | 0.0359 (15) | 0.072 (2) | −0.0019 (13) | 0.000 | 0.000 |
| Sb—Cl1 | 2.4520 (12) | N2—H2 | 0.9100 |
| Sb—Cl3i | 2.4904 (7) | C1—C2 | 1.492 (6) |
| Sb—Cl3 | 2.4904 (7) | C1—H1A | 0.9700 |
| Sb—Cl2 | 2.8755 (11) | C1—H1B | 0.9700 |
| Sb—Cl4 | 2.9107 (8) | C2—H2A | 0.9700 |
| N1—C3 | 1.481 (4) | C2—H2B | 0.9700 |
| N1—C3i | 1.481 (4) | C3—C4 | 1.511 (4) |
| N1—C1 | 1.487 (5) | C3—H3A | 0.9700 |
| N1—H1 | 0.9100 | C3—H3B | 0.9700 |
| N2—C2 | 1.478 (5) | C4—H4A | 0.9700 |
| N2—C4i | 1.485 (4) | C4—H4B | 0.9700 |
| N2—C4 | 1.485 (4) | ||
| Cl1—Sb—Cl3i | 88.39 (3) | N1—C1—H1A | 109.9 |
| Cl1—Sb—Cl3 | 88.39 (3) | C2—C1—H1A | 109.9 |
| Cl3i—Sb—Cl3 | 93.37 (3) | N1—C1—H1B | 109.9 |
| Cl1—Sb—Cl2 | 164.64 (4) | C2—C1—H1B | 109.9 |
| Cl3i—Sb—Cl2 | 81.11 (2) | H1A—C1—H1B | 108.3 |
| Cl3—Sb—Cl2 | 81.11 (2) | N2—C2—C1 | 109.4 (3) |
| Cl4—Sb—Cl3 | 90.19 (1) | N2—C2—H2A | 109.8 |
| Cl4—Sb—Cl3i | 173.84 (1) | C1—C2—H2A | 109.8 |
| Cl4—Sb—Cl1 | 86.69 (4) | N2—C2—H2B | 109.8 |
| Cl4—Sb—Cl2 | 104.42 (1) | C1—C2—H2B | 109.8 |
| C3—N1—C3i | 111.4 (3) | H2A—C2—H2B | 108.2 |
| C3—N1—C1 | 109.3 (2) | N1—C3—C4 | 109.0 (3) |
| C3i—N1—C1 | 109.3 (2) | N1—C3—H3A | 109.9 |
| C3—N1—H1 | 108.9 | C4—C3—H3A | 109.9 |
| C3i—N1—H1 | 108.9 | N1—C3—H3B | 109.9 |
| C1—N1—H1 | 108.9 | C4—C3—H3B | 109.9 |
| C2—N2—C4i | 109.8 (2) | H3A—C3—H3B | 108.3 |
| C2—N2—C4 | 109.8 (2) | N2—C4—C3 | 108.5 (3) |
| C4i—N2—C4 | 110.8 (4) | N2—C4—H4A | 110.0 |
| C2—N2—H2 | 108.8 | C3—C4—H4A | 110.0 |
| C4i—N2—H2 | 108.8 | N2—C4—H4B | 110.0 |
| C4—N2—H2 | 108.8 | C3—C4—H4B | 110.0 |
| N1—C1—C2 | 108.9 (3) | H4A—C4—H4B | 108.4 |
| H··· | ||||
| N1—H1···Cl2 | 0.91 | 2.59 | 3.340 (4) | 140 |
| N1—H1···Cl3 | 0.91 | 2.77 | 3.390 (3) | 126 |
| N1—H1···Cl3i | 0.91 | 2.77 | 3.390 (3) | 126 |
| N2—H2···O | 0.91 | 2.00 | 2.780 (4) | 143 |
Hydrogen-bond geometry (Å, °)
|
|
| H⋯ |
|
|
|---|---|---|---|---|
| N1—H1⋯Cl2 | 0.91 | 2.59 | 3.340 (4) | 140 |
| N1—H1⋯Cl3 | 0.91 | 2.77 | 3.390 (3) | 126 |
| N1—H1⋯Cl3i | 0.91 | 2.77 | 3.390 (3) | 126 |
| N2—H2⋯O | 0.91 | 2.00 | 2.780 (4) | 143 |
Symmetry code: (i) .