Abstract
The asymmetric unit of the title compound (C6H14N2)[CdCl4]·H2O contained one 1,4-diazabicyclo[2.2.2]octane dication, a tetrahedral CdCl4 2− anion and a lattice water molecule. In the crystal, the solvate water molecule interacts with the cationic and anionic species via N—H⋯O and O—H⋯Cl [O⋯Cl = 3.289 (7) Å] hydrogen-bond interactions, respectively, leading to a layered supramolecular structure extending parallel to (011).
Related literature
For background to this class of compounds, see: Wei & Willett (2002 ▶); Billing & Lemmerer (2009 ▶); Samet et al. (2010 ▶) Lemmerer & Billing (2012 ▶); Ben Rhaiem et al. (2013 ▶). For related structures, see: Sun & Qu (2005 ▶); Zhang & Zhu (2012 ▶).
Experimental
Crystal data
(C6H14N2)[CdCl4]·H2O
M r = 386.40
Orthorhombic,
a = 8.528 (5) Å
b = 11.653 (2) Å
c = 13.114 (6) Å
V = 1303.2 (10) Å3
Z = 4
Mo Kα radiation
μ = 2.47 mm−1
T = 298 K
0.54 × 0.43 × 0.29 mm
Data collection
Enraf–Nonius CAD-4 diffractometer
Absorption correction: ψ scan (North et al., 1968 ▶) T min = 0.283, T max = 0.536
5639 measured reflections
2837 independent reflections
2632 reflections with I > 2σ(I)
R int = 0.075
2 standard reflections every 120 min intensity decay: 1%
Refinement
R[F 2 > 2σ(F 2)] = 0.048
wR(F 2) = 0.134
S = 1.19
2837 reflections
135 parameters
10 restraints
H-atom parameters not refined
Δρmax = 1.58 e Å−3
Δρmin = −1.44 e Å−3
Data collection: CAD-4 EXPRESS (Duisenberg, 1992 ▶); cell refinement: CAD-4 EXPRESS; data reduction: XCAD4 (Harms & Wocadlo, 1995 ▶); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97; molecular graphics: DIAMOND (Brandenburg, 2006 ▶); software used to prepare material for publication: publCIF (Westrip, 2010 ▶).
Supplementary Material
Crystal structure: contains datablock(s) I, New_Global_Publ_Block. DOI: 10.1107/S1600536814007533/ds2238sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536814007533/ds2238Isup2.hkl
CCDC reference: 967916
Additional supporting information: crystallographic information; 3D view; checkCIF report
Table 1. Hydrogen-bond geometry (Å, °).
| D—H⋯A | D—H | H⋯A | D⋯A | D—H⋯A |
|---|---|---|---|---|
| N2—H2⋯Oi | 0.84 | 2.01 | 2.783 (1) | 151 |
Symmetry code: (i)
.
supplementary crystallographic information
1. Comment
In recent years, a significant number of organic–inorganic hybrid materials based on metal halide units have been prepared and studied (Lemmerer & Billing, 2012). It has been shown that their structures can vary considerably, ranging from systems based on isolated polyhydra to ones containing extended chains and up to two- or three-dimensional networks (Ben Rhaiem et al., 2013; Samet et al., 2010; Billing & Lemmerer, 2009). Generally, the organic cations contain ammonium groups linked to the anionic framework by hydrogen bonds via halogenous tetrahedral vertices (Sun & Qu, 2005) and (Zhang & Zhu, 2012). In pseudopolymorphic cases, the water molecules can be able to coordinate the charged components strengthening the crystal cohesion as it was observed in (dabcoH2)CuCl4 and (dabcoH2)CuCl4·H2O (Wei & Willett, 2002).
The new chloridocadmate(II) compound, (C6H14N2) [CdCl4]·H2O (I), is self-assembled into alternating organic and inorganic layered structure. the organic part is made up of 1,4-diazabicyclo[2.2.2]octane cations and water molecules. The inorganic component contains isolated [CdCl4]2- units. The layers are stacked along the c axis, as illustrated in Fig. 1.
The asymmetric unit of (I) comprises one 1,4-diazabicyclo[2.2.2]octane cation, one [CdCl4]2- anion and a lattice occluded water molecule (Fig. 2).
The [CdCl4]2- unit possesses a configuration of distorted tetrahedron, so that the central cadmium (II) ion is surrounded by four chlorine atoms. The Cd–Cl bond lengths vary from 2.430 (2) Å to 2.4864 (17) Å and the Cl–Cd–Cl angles fall in the range 101.80 (6)°–116.95 (6)°.
The protonated N2 atom of the organic cation interacts via a simple hydrogen bond with oxygen atom of the water molecule (Fig. 3 and Tab. 1).
2. Experimental
The title compound (C6H14N2) [CdCl4]·H2O, (I), was obtained by the reaction of cadmium iodide CdI2 (0.19 g, 0.5 mmol) with DABCO (1,4-diazabicyclo[2.2.2]octane) (0.112 g, 1 mmol) in aqueous hydrochloric acid solution with pH ranging between 3 and 4. The mixture was stirred for several minutes. Colorless crystals suitable for X-ray diffraction analysis were obtained by slow evaporation at room temperature over 2 weeks.
3. Refinement
Hydrogen water molecules are omited. The C—H and N—H hydrogen atoms positions are generated geometrically by HFIX SHELXL command.
Figures
Fig. 1.
Packing diagram of (I), projected along the a axis.
Fig. 2.
The asymmetric unit of (I), showing the atom numbering scheme. Displacement ellipsoids are drawn at 50% probability level and H atoms are shown as small spheres of arbitrary radii.
Fig. 3.
The arrangement of ions of (I), projected along the b axis. [Symmetry code: (i) -x, y+1/2, -z + 1/2.]
Crystal data
| (C6H14N2)[CdCl4]·H2O | F(000) = 752 |
| Mr = 386.40 | Dx = 1.959 Mg m−3 |
| Orthorhombic, P212121 | Mo Kα radiation, λ = 0.71073 Å |
| Hall symbol: P 2ac 2ab | Cell parameters from 2837 reflections |
| a = 8.528 (5) Å | θ = 2.4–27° |
| b = 11.653 (2) Å | µ = 2.47 mm−1 |
| c = 13.114 (6) Å | T = 298 K |
| V = 1303.2 (10) Å3 | Prism, colorless |
| Z = 4 | 0.54 × 0.43 × 0.29 mm |
Data collection
| Enraf–Nonius CAD-4 diffractometer | 2632 reflections with I > 2σ(I) |
| Radiation source: fine-focus sealed tube | Rint = 0.075 |
| Graphite monochromator | θmax = 27.0°, θmin = 2.3° |
| non–profiled ω/2θ scans | h = −10→6 |
| Absorption correction: ψ scan (North et al. (1968) | k = −14→1 |
| Tmin = 0.283, Tmax = 0.536 | l = −16→16 |
| 5639 measured reflections | 2 standard reflections every 120 min |
| 2837 independent reflections | intensity decay: 1% |
Refinement
| Refinement on F2 | Primary atom site location: structure-invariant direct methods |
| Least-squares matrix: full | Secondary atom site location: difference Fourier map |
| R[F2 > 2σ(F2)] = 0.048 | Hydrogen site location: inferred from neighbouring sites |
| wR(F2) = 0.134 | H-atom parameters not refined |
| S = 1.19 | w = 1/[σ2(Fo2) + (0.0587P)2 + 1.6133P] where P = (Fo2 + 2Fc2)/3 |
| 2837 reflections | (Δ/σ)max = 0.001 |
| 135 parameters | Δρmax = 1.58 e Å−3 |
| 10 restraints | Δρmin = −1.44 e Å−3 |
Special details
| 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 F2 against ALL reflections. The weighted R-factor wR and goodness of fit S are based on F2, conventional R-factors R are based on F, with F set to zero for negative F2. The threshold expression of F2 > σ(F2) is used only for calculating R-factors(gt) etc. and is not relevant to the choice of reflections for refinement. R-factors based on F2 are statistically about twice as large as those based on F, and R- factors based on ALL data will be even larger. |
Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2)
| x | y | z | Uiso*/Ueq | ||
| Cd | 0.74636 (5) | 0.52500 (4) | 0.50315 (3) | 0.04606 (17) | |
| Cl1 | 0.52000 (18) | 0.40196 (13) | 0.46103 (13) | 0.0465 (3) | |
| Cl2 | 0.7583 (2) | 0.53068 (14) | 0.69230 (11) | 0.0544 (4) | |
| Cl3 | 0.9940 (2) | 0.43346 (15) | 0.46078 (15) | 0.0557 (4) | |
| Cl4 | 0.6884 (2) | 0.71103 (15) | 0.41831 (12) | 0.0542 (4) | |
| C1 | 0.4091 (7) | 0.6836 (5) | 0.2060 (5) | 0.0457 (13) | |
| H1A | 0.498 (5) | 0.6620 (12) | 0.153 (3) | 0.055* | |
| H1B | 0.4419 (18) | 0.761 (4) | 0.2435 (19) | 0.055* | |
| C2 | 0.2540 (8) | 0.6998 (6) | 0.1512 (5) | 0.0514 (13) | |
| H2A | 0.2282 (17) | 0.776 (5) | 0.1496 (5) | 0.062* | |
| H2B | 0.2617 (9) | 0.6741 (16) | 0.086 (4) | 0.062* | |
| C3 | 0.2824 (8) | 0.6248 (7) | 0.3636 (6) | 0.0583 (18) | |
| H3A | 0.3266 (11) | 0.6796 (11) | 0.4005 (8) | 0.070* | |
| H3B | 0.2613 (9) | 0.5660 (12) | 0.4042 (9) | 0.070* | |
| C4 | 0.1319 (9) | 0.6690 (6) | 0.3149 (6) | 0.065 (2) | |
| H4A | 0.0481 (16) | 0.6394 (8) | 0.3470 (8) | 0.078* | |
| H4B | 0.1274 (9) | 0.7458 (14) | 0.3198 (7) | 0.078* | |
| C5 | 0.3284 (9) | 0.4857 (5) | 0.2294 (6) | 0.0519 (16) | |
| H5A | 0.3330 (9) | 0.4244 (11) | 0.2713 (9) | 0.062* | |
| H5B | 0.3874 (13) | 0.4708 (6) | 0.1738 (11) | 0.062* | |
| C6 | 0.1623 (9) | 0.5077 (6) | 0.1985 (7) | 0.0586 (18) | |
| H6A | 0.0970 (14) | 0.4692 (9) | 0.2392 (9) | 0.070* | |
| H6B | 0.1468 (9) | 0.4843 (7) | 0.1344 (12) | 0.070* | |
| N1 | 0.3888 (6) | 0.5887 (5) | 0.2823 (4) | 0.0431 (11) | |
| H1 | 0.477 (2) | 0.5730 (6) | 0.3082 (7) | 0.052* | |
| N2 | 0.1318 (6) | 0.6341 (5) | 0.2067 (5) | 0.0554 (15) | |
| H2 | 0.043 (2) | 0.6488 (6) | 0.1811 (8) | 0.067* | |
| O | 0.1563 (8) | 0.2409 (6) | 0.3238 (6) | 0.0861 (19) |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| Cd | 0.0463 (3) | 0.0409 (2) | 0.0510 (3) | 0.00213 (18) | −0.0028 (2) | 0.00245 (17) |
| Cl1 | 0.0486 (8) | 0.0402 (7) | 0.0508 (8) | −0.0018 (6) | 0.0024 (6) | −0.0039 (6) |
| Cl2 | 0.0613 (8) | 0.0530 (8) | 0.0490 (7) | 0.0058 (9) | −0.0041 (8) | −0.0042 (6) |
| Cl3 | 0.0519 (8) | 0.0515 (8) | 0.0635 (9) | 0.0105 (7) | 0.0063 (7) | 0.0105 (8) |
| Cl4 | 0.0684 (9) | 0.0423 (7) | 0.0520 (8) | 0.0014 (7) | −0.0163 (7) | 0.0047 (7) |
| C1 | 0.042 (3) | 0.034 (3) | 0.061 (3) | −0.005 (2) | 0.004 (3) | 0.007 (3) |
| C2 | 0.049 (3) | 0.048 (3) | 0.057 (3) | −0.006 (3) | −0.001 (3) | 0.020 (3) |
| C3 | 0.063 (5) | 0.057 (4) | 0.056 (3) | −0.006 (3) | 0.006 (3) | −0.005 (3) |
| C4 | 0.062 (4) | 0.046 (4) | 0.087 (5) | 0.012 (3) | 0.032 (4) | 0.012 (4) |
| C5 | 0.055 (4) | 0.026 (2) | 0.075 (4) | 0.001 (3) | −0.008 (3) | 0.002 (3) |
| C6 | 0.061 (4) | 0.041 (3) | 0.075 (5) | −0.008 (3) | −0.016 (4) | 0.006 (3) |
| N1 | 0.042 (2) | 0.040 (2) | 0.047 (3) | 0.002 (2) | −0.005 (2) | 0.004 (2) |
| N2 | 0.038 (3) | 0.044 (3) | 0.084 (4) | 0.004 (2) | −0.004 (3) | 0.027 (3) |
| O | 0.085 (4) | 0.070 (4) | 0.103 (5) | −0.014 (3) | 0.008 (4) | −0.009 (4) |
Geometric parameters (Å, º)
| Cd—Cl3 | 2.430 (2) | C3—H3B | 0.8860 |
| Cd—Cl1 | 2.4673 (18) | C4—N2 | 1.476 (11) |
| Cd—Cl2 | 2.4835 (19) | C4—H4A | 0.8977 |
| Cd—Cl4 | 2.4864 (17) | C4—H4B | 0.8977 |
| C1—N1 | 1.502 (8) | C5—N1 | 1.479 (9) |
| C1—C2 | 1.517 (9) | C5—C6 | 1.496 (10) |
| C1—H1A | 1.0614 | C5—H5A | 0.9026 |
| C1—H1B | 1.0614 | C5—H5B | 0.9026 |
| C2—N2 | 1.485 (8) | C6—N2 | 1.499 (9) |
| C2—H2A | 0.9127 | C6—H6A | 0.8931 |
| C2—H2B | 0.9127 | C6—H6B | 0.8931 |
| C3—N1 | 1.461 (9) | N1—H1 | 0.8477 |
| C3—C4 | 1.524 (10) | N2—H2 | 0.8420 |
| C3—H3A | 0.8860 | ||
| Cl3—Cd—Cl1 | 111.93 (7) | N2—C4—H4B | 110.1 |
| Cl3—Cd—Cl2 | 101.80 (6) | C3—C4—H4B | 110.1 |
| Cl1—Cd—Cl2 | 105.73 (6) | H4A—C4—H4B | 108.4 |
| Cl3—Cd—Cl4 | 116.95 (6) | N1—C5—C6 | 108.5 (5) |
| Cl1—Cd—Cl4 | 104.53 (6) | N1—C5—H5A | 110.0 |
| Cl2—Cd—Cl4 | 115.58 (6) | C6—C5—H5A | 110.0 |
| N1—C1—C2 | 107.9 (5) | N1—C5—H5B | 110.0 |
| N1—C1—H1A | 110.1 | C6—C5—H5B | 110.0 |
| C2—C1—H1A | 110.1 | H5A—C5—H5B | 108.4 |
| N1—C1—H1B | 110.1 | C5—C6—N2 | 108.3 (5) |
| C2—C1—H1B | 110.1 | C5—C6—H6A | 110.0 |
| H1A—C1—H1B | 108.4 | N2—C6—H6A | 110.0 |
| N2—C2—C1 | 108.4 (5) | C5—C6—H6B | 110.0 |
| N2—C2—H2A | 110.0 | N2—C6—H6B | 110.0 |
| C1—C2—H2A | 110.0 | H6A—C6—H6B | 108.4 |
| N2—C2—H2B | 110.0 | C3—N1—C5 | 111.1 (6) |
| C1—C2—H2B | 110.0 | C3—N1—C1 | 110.2 (5) |
| H2A—C2—H2B | 108.4 | C5—N1—C1 | 109.0 (5) |
| N1—C3—C4 | 108.4 (6) | C3—N1—H1 | 108.8 |
| N1—C3—H3A | 110.0 | C5—N1—H1 | 108.8 |
| C4—C3—H3A | 110.0 | C1—N1—H1 | 108.8 |
| N1—C3—H3B | 110.0 | C4—N2—C2 | 109.2 (6) |
| C4—C3—H3B | 110.0 | C4—N2—C6 | 109.9 (6) |
| H3A—C3—H3B | 108.4 | C2—N2—C6 | 110.5 (6) |
| N2—C4—C3 | 108.0 (5) | C4—N2—H2 | 109.1 |
| N2—C4—H4A | 110.1 | C2—N2—H2 | 109.1 |
| C3—C4—H4A | 110.1 | C6—N2—H2 | 109.1 |
Hydrogen-bond geometry (Å, º)
| D—H···A | D—H | H···A | D···A | D—H···A |
| N2—H2···Oi | 0.84 | 2.01 | 2.783 (1) | 151 |
Symmetry code: (i) −x, y+1/2, −z+1/2.
Footnotes
Supporting information for this paper is available from the IUCr electronic archives (Reference: DS2238).
References
- Ben Rhaiem, T., Boughzala, H. & Driss, A. (2013). Acta Cryst. E69, m330. [DOI] [PMC free article] [PubMed]
- Billing, D. G. & Lemmerer, A. (2009). CrystEngComm, 11, 1549–1562.
- Brandenburg, K. (2006). DIAMOND Crystal Impact GbR, Bonn, Germany.
- Duisenberg, A. J. M. (1992). J. Appl. Cryst. 25, 92–96.
- Harms, K. & Wocadlo, S. (1995). XCAD4 University of Marburg, Germany.
- Lemmerer, A. & Billing, D. G. (2012). CrystEngComm, 14, 1954–1966.
- North, A. C. T., Phillips, D. C. & Mathews, F. S. (1968). Acta Cryst. A24, 351–359.
- Samet, A., Boughzala, H., Khemekhem, H. & Abid, Y. (2010). J. Mol. Struct. 984, 23–29.
- Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
- Sun, X.-M. & Qu, Y. (2005). Acta Cryst. E61, m1360–m1362.
- Wei, M. & Willett, R. D. (2002). J. Chem. Crystallogr. 32, 439–445.
- Westrip, S. P. (2010). J. Appl. Cryst. 43, 920–925.
- Zhang, Y. & Zhu, B. H. (2012). Acta Cryst. E68, m687. [DOI] [PMC free article] [PubMed]
Associated Data
This section collects any data citations, data availability statements, or supplementary materials included in this article.
Supplementary Materials
Crystal structure: contains datablock(s) I, New_Global_Publ_Block. DOI: 10.1107/S1600536814007533/ds2238sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536814007533/ds2238Isup2.hkl
CCDC reference: 967916
Additional supporting information: crystallographic information; 3D view; checkCIF report



