Abstract
The title compound, [Cu(H2O)6]Cl2·2C6H12N4·4H2O, was prepared under mild hydrothermal conditions. The asymmetric unit consists of one half of the [Cu(H2O)6]2+ cation, a hexamethylenetetramine molecule, two solvent water molecules and a chloride ion. The formula unit is generated by crystallographic inversion symmetry. The Cu atom lies on a crystallographic inversion centre. It is in a slightly distorted octahedral coordination environment. In the crystal structure, intermolecular O—H⋯O, O—H⋯N and O—H⋯Cl hydrogen bonds link the components into a three-dimensional network.
Related literature
For a related structure, see: Kinzhibalo et al. (2002 ▶).
Experimental
Crystal data
[Cu(H2O)6]Cl2·2C6H12N4·4H2O
M r = 594.99
Triclinic,
a = 9.321 (3) Å
b = 9.3923 (16) Å
c = 9.4261 (16) Å
α = 119.523 (2)°
β = 94.153 (3)°
γ = 101.065 (3)°
V = 691.1 (3) Å3
Z = 1
Mo Kα radiation
μ = 1.04 mm−1
T = 291 (2) K
0.36 × 0.29 × 0.15 mm
Data collection
Bruker SMART CCD diffractometer
Absorption correction: multi-scan (SADABS; Sheldrick, 1996 ▶) T min = 0.709, T max = 0.860
5328 measured reflections
2551 independent reflections
2083 reflections with I > 2σ(I)
R int = 0.027
Refinement
R[F 2 > 2σ(F 2)] = 0.041
wR(F 2) = 0.108
S = 1.05
2551 reflections
151 parameters
H-atom parameters constrained
Δρmax = 0.30 e Å−3
Δρmin = −0.51 e Å−3
Data collection: SMART (Bruker, 2002 ▶); cell refinement: SAINT (Bruker, 2002 ▶); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: SHELXTL (Sheldrick, 2008 ▶); software used to prepare material for publication: SHELXTL.
Supplementary Material
Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536808020916/lh2645sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536808020916/lh2645Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report
Table 1. Selected geometric parameters (Å, °).
| Cu1—O2 | 2.017 (2) |
| Cu1—O1 | 2.045 (2) |
| Cu1—O3 | 2.053 (2) |
| O2—Cu1—O2i | 180 |
| O2—Cu1—O1 | 87.24 (9) |
| O2—Cu1—O1i | 92.76 (9) |
| O1—Cu1—O1i | 180 |
| O2—Cu1—O3i | 90.30 (10) |
| O1—Cu1—O3i | 86.64 (9) |
| O2—Cu1—O3 | 89.70 (10) |
| O1—Cu1—O3 | 93.36 (9) |
| O3i—Cu1—O3 | 180 |
Symmetry code: (i)
.
Table 2. Hydrogen-bond geometry (Å, °).
| D—H⋯A | D—H | H⋯A | D⋯A | D—H⋯A |
|---|---|---|---|---|
| O1—H1W⋯N3 | 0.82 | 2.04 | 2.814 (3) | 158 |
| O1—H2W⋯O5ii | 0.83 | 1.94 | 2.734 (3) | 162 |
| O2—H3W⋯N2iii | 0.83 | 1.99 | 2.800 (3) | 167 |
| O2—H4W⋯O4iii | 0.83 | 1.89 | 2.700 (3) | 165 |
| O3—H5W⋯Cl1 | 0.82 | 2.54 | 3.190 (2) | 137 |
| O3—H6W⋯N1iv | 0.82 | 2.00 | 2.805 (3) | 165 |
| O4—H7W⋯Cl1 | 0.83 | 2.35 | 3.170 (3) | 168 |
| O4—H8W⋯N4v | 0.84 | 2.00 | 2.829 (4) | 174 |
| O5—H9W⋯Cl1 | 0.83 | 2.43 | 3.245 (3) | 169 |
| O5—H10W⋯Cl1vi | 0.83 | 2.37 | 3.200 (3) | 175 |
Symmetry codes: (ii)
; (iii)
; (iv)
; (v)
; (vi)
.
Acknowledgments
We thank the Natural Science Foundation of Henan Province and the Key Discipline Foundation of Zhoukou Normal University for financial support of this research.
supplementary crystallographic information
Comment
The asymmetric unit and some symmetry related atoms are shown in Fig.1. The asymmetric unit consists of one half of hexaaqua CuII cation, one chloride anion, one uncoordinated neutral hexamethylenetetramine molecule and two molecules of water of crystallization. In the crystal structure, hydrogen bonding between [Cu(H2O)6]2+ cations and hexamethylenetetramine molecules, and those between [Cu(H2O)6]2+ cations and chloride ions are shown in Fig. 2 and Fig.3, respectively. A 16-membered ring formed by cations and hexamethylenetetramine moieties via the H-bonding interactions propagates along the c-axis. The chloride ion H-bonded with the uncoordinated water molecules gives rise to a number of anionic ring systems (Fig. 3). One of the hydrogen atoms of the uncoordinated water molecule connects the chloride ion and forms a 16-membered ring. The combonation of these anionic and cationic frameworks results in the formation of a three-dimensional network.
Experimental
All reagents were of AR grade and used without further purification. C6H12N4 (1.401 g, 10 mmol) was dissolved in 50 ml EtOH/H2O (V:V = 1:1) solution, then the resultant solution was added in 10 ml double-distilled water containing CuCl2.2H2O (0.171 g, 1 mmol), The resulting solution was heated at 373 K for 96 h. After cooling to room temperature, blue crystals were obtained in a yield up to 48.6%.
Refinement
H atoms bonded to O atoms were located in a difference map and included in their 'as found' positions with Uiso(H) = 1.5Ueq(O). Other H atoms were positioned geometrically with C-H = 0.97 Å and with Uiso(H)=1.2Ueq(C). All H atoms were treated as riding.
Figures
Fig. 1.
The asymmetric unit and symmetry related atoms of the title compound with 30% probability ellipsoids [symmetry code: (A) -x+1, -y, -z].
Fig. 2.
Hydrogen bonding [dashed lines] in part of the crystal structure between [Cu(H2O)6]2+ cations, hexamethylenetetramine molecules and water molecules.
Fig. 3.
Hydrogen bonding [dashed lines] in part of the crystal structure between the [Cu(H2O)6]2+ cations, chloride anions and water molecules.
Crystal data
| [Cu(H2O)6]Cl2·2C6H12N4·4H2O | Z = 1 |
| Mr = 594.99 | F000 = 315 |
| Triclinic, P1 | Dx = 1.430 Mg m−3 |
| Hall symbol: -P 1 | Mo Kα radiation λ = 0.71073 Å |
| a = 9.321 (3) Å | Cell parameters from 1415 reflections |
| b = 9.3923 (16) Å | θ = 2.5–22.9º |
| c = 9.4261 (16) Å | µ = 1.04 mm−1 |
| α = 119.523 (2)º | T = 291 (2) K |
| β = 94.153 (3)º | Block, blue |
| γ = 101.065 (3)º | 0.36 × 0.29 × 0.15 mm |
| V = 691.1 (3) Å3 |
Data collection
| Bruker SMART CCD diffractometer | 2551 independent reflections |
| Radiation source: fine-focus sealed tube | 2083 reflections with I > 2σ(I) |
| Monochromator: graphite | Rint = 0.027 |
| Detector resolution: 0 pixels mm-1 | θmax = 25.5º |
| T = 291(2) K | θmin = 2.5º |
| φ and ω scans | h = −11→11 |
| Absorption correction: multi-scan(SADABS; Sheldrick, 1996) | k = −11→11 |
| Tmin = 0.709, Tmax = 0.860 | l = −11→11 |
| 5328 measured reflections |
Refinement
| Refinement on F2 | Secondary atom site location: difference Fourier map |
| Least-squares matrix: full | Hydrogen site location: inferred from neighbouring sites |
| R[F2 > 2σ(F2)] = 0.041 | H-atom parameters constrained |
| wR(F2) = 0.108 | w = 1/[σ2(Fo2) + (0.0473P)2 + 0.4567P] P = (Fo2 + 2Fc2)/3 |
| S = 1.06 | (Δ/σ)max < 0.001 |
| 2551 reflections | Δρmax = 0.30 e Å−3 |
| 151 parameters | Δρmin = −0.51 e Å−3 |
| Primary atom site location: structure-invariant direct methods | Extinction correction: none |
Special details
| 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 F^2^ against ALL reflections. The weighted R-factor wR and goodness of fit S are based on F^2^, conventional R-factors R are based on F, with F set to zero for negative F^2^. The threshold expression of F^2^ > σ(F^2^) is used only for calculating R-factors(gt) etc. and is not relevant to the choice of reflections for refinement. R-factors based on F^2^ 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 | ||
| Cu1 | 0.5000 | 0.0000 | 0.0000 | 0.03048 (18) | |
| Cl1 | 0.18946 (11) | 0.17433 (12) | 0.43516 (12) | 0.0544 (3) | |
| O1 | 0.3831 (2) | 0.1341 (3) | −0.0575 (3) | 0.0410 (6) | |
| H1W | 0.3885 | 0.2251 | 0.0267 | 0.061* | |
| H2W | 0.3032 | 0.0955 | −0.1237 | 0.061* | |
| O2 | 0.6183 (3) | 0.2239 (3) | 0.1983 (3) | 0.0458 (6) | |
| H3W | 0.6168 | 0.2522 | 0.2960 | 0.069* | |
| H4W | 0.6825 | 0.2950 | 0.1926 | 0.069* | |
| O3 | 0.3576 (3) | −0.0289 (3) | 0.1457 (3) | 0.0468 (6) | |
| H5W | 0.3400 | 0.0621 | 0.2072 | 0.070* | |
| H6W | 0.3653 | −0.0847 | 0.1901 | 0.070* | |
| O4 | 0.1965 (3) | 0.5031 (3) | 0.7782 (3) | 0.0481 (6) | |
| H7W | 0.2086 | 0.4204 | 0.6934 | 0.072* | |
| H8W | 0.1057 | 0.4942 | 0.7787 | 0.072* | |
| O5 | 0.1485 (3) | 0.0517 (4) | 0.7004 (4) | 0.0741 (9) | |
| H9W | 0.1697 | 0.0946 | 0.6432 | 0.111* | |
| H10W | 0.0599 | −0.0029 | 0.6717 | 0.111* | |
| N1 | 0.3348 (3) | 0.7402 (3) | 0.2551 (3) | 0.0349 (6) | |
| N2 | 0.3362 (3) | 0.6544 (3) | 0.4602 (3) | 0.0347 (6) | |
| N3 | 0.3419 (3) | 0.4512 (3) | 0.1727 (3) | 0.0339 (6) | |
| N4 | 0.1150 (3) | 0.5418 (3) | 0.2441 (3) | 0.0352 (6) | |
| C1 | 0.3865 (4) | 0.7928 (4) | 0.4281 (4) | 0.0372 (7) | |
| H1A | 0.3493 | 0.8884 | 0.5004 | 0.045* | |
| H1B | 0.4945 | 0.8297 | 0.4544 | 0.045* | |
| C2 | 0.3940 (4) | 0.5117 (4) | 0.3491 (4) | 0.0367 (7) | |
| H2A | 0.3622 | 0.4193 | 0.3685 | 0.044* | |
| H2B | 0.5021 | 0.5469 | 0.3747 | 0.044* | |
| C3 | 0.1779 (4) | 0.4020 (4) | 0.1381 (4) | 0.0399 (8) | |
| H3A | 0.1418 | 0.3631 | 0.0225 | 0.048* | |
| H3B | 0.1433 | 0.3083 | 0.1550 | 0.048* | |
| C4 | 0.1704 (4) | 0.6831 (4) | 0.2180 (4) | 0.0390 (8) | |
| H4A | 0.1311 | 0.7774 | 0.2886 | 0.047* | |
| H4B | 0.1342 | 0.6476 | 0.1034 | 0.047* | |
| C5 | 0.3921 (4) | 0.5949 (4) | 0.1478 (4) | 0.0384 (8) | |
| H5A | 0.5002 | 0.6301 | 0.1718 | 0.046* | |
| H5B | 0.3584 | 0.5583 | 0.0324 | 0.046* | |
| C6 | 0.1729 (4) | 0.5996 (4) | 0.4188 (4) | 0.0388 (8) | |
| H6A | 0.1335 | 0.6931 | 0.4911 | 0.047* | |
| H6B | 0.1386 | 0.5079 | 0.4386 | 0.047* |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| Cu1 | 0.0393 (3) | 0.0273 (3) | 0.0255 (3) | 0.0104 (2) | 0.0087 (2) | 0.0133 (2) |
| Cl1 | 0.0599 (6) | 0.0441 (5) | 0.0534 (6) | 0.0137 (5) | 0.0259 (5) | 0.0190 (5) |
| O1 | 0.0505 (14) | 0.0335 (12) | 0.0335 (12) | 0.0193 (11) | 0.0002 (10) | 0.0117 (10) |
| O2 | 0.0663 (16) | 0.0310 (12) | 0.0231 (11) | −0.0071 (11) | 0.0028 (11) | 0.0093 (10) |
| O3 | 0.0699 (17) | 0.0442 (14) | 0.0551 (15) | 0.0328 (13) | 0.0383 (13) | 0.0372 (13) |
| O4 | 0.0416 (14) | 0.0439 (14) | 0.0435 (14) | 0.0008 (11) | 0.0087 (11) | 0.0151 (12) |
| O5 | 0.0623 (18) | 0.088 (2) | 0.070 (2) | 0.0023 (16) | −0.0133 (15) | 0.0494 (19) |
| N1 | 0.0419 (16) | 0.0337 (15) | 0.0399 (15) | 0.0157 (13) | 0.0169 (12) | 0.0237 (13) |
| N2 | 0.0422 (15) | 0.0331 (14) | 0.0248 (13) | 0.0026 (12) | 0.0077 (11) | 0.0143 (12) |
| N3 | 0.0421 (15) | 0.0299 (14) | 0.0300 (14) | 0.0139 (12) | 0.0067 (12) | 0.0141 (12) |
| N4 | 0.0353 (15) | 0.0330 (15) | 0.0333 (14) | 0.0089 (12) | 0.0074 (12) | 0.0141 (12) |
| C1 | 0.0456 (19) | 0.0255 (16) | 0.0339 (17) | 0.0049 (14) | 0.0106 (15) | 0.0117 (14) |
| C2 | 0.0448 (19) | 0.0355 (18) | 0.0335 (17) | 0.0093 (15) | 0.0032 (14) | 0.0214 (15) |
| C3 | 0.0403 (19) | 0.0323 (18) | 0.0335 (18) | 0.0067 (15) | 0.0012 (15) | 0.0090 (15) |
| C4 | 0.047 (2) | 0.0410 (19) | 0.0398 (18) | 0.0225 (16) | 0.0150 (15) | 0.0240 (16) |
| C5 | 0.047 (2) | 0.046 (2) | 0.0327 (17) | 0.0224 (17) | 0.0174 (15) | 0.0240 (16) |
| C6 | 0.048 (2) | 0.0343 (18) | 0.0359 (18) | 0.0082 (15) | 0.0176 (15) | 0.0190 (15) |
Geometric parameters (Å, °)
| Cu1—O2 | 2.017 (2) | N2—C2 | 1.469 (4) |
| Cu1—O2i | 2.017 (2) | N2—C1 | 1.475 (4) |
| Cu1—O1 | 2.045 (2) | N3—C3 | 1.472 (4) |
| Cu1—O1i | 2.045 (2) | N3—C2 | 1.473 (4) |
| Cu1—O3i | 2.053 (2) | N3—C5 | 1.476 (4) |
| Cu1—O3 | 2.053 (2) | N4—C3 | 1.467 (4) |
| O1—H1W | 0.8200 | N4—C4 | 1.472 (4) |
| O1—H2W | 0.8260 | N4—C6 | 1.474 (4) |
| O2—H3W | 0.8254 | C1—H1A | 0.9700 |
| O2—H4W | 0.8330 | C1—H1B | 0.9700 |
| O3—H5W | 0.8200 | C2—H2A | 0.9700 |
| O3—H6W | 0.8246 | C2—H2B | 0.9700 |
| O4—H7W | 0.8304 | C3—H3A | 0.9700 |
| O4—H8W | 0.8351 | C3—H3B | 0.9700 |
| O5—H9W | 0.8312 | C4—H4A | 0.9700 |
| O5—H10W | 0.8289 | C4—H4B | 0.9700 |
| N1—C1 | 1.462 (4) | C5—H5A | 0.9700 |
| N1—C5 | 1.473 (4) | C5—H5B | 0.9700 |
| N1—C4 | 1.477 (4) | C6—H6A | 0.9700 |
| N2—C6 | 1.466 (4) | C6—H6B | 0.9700 |
| O2—Cu1—O2i | 180 | C4—N4—C6 | 107.7 (2) |
| O2—Cu1—O1 | 87.24 (9) | N1—C1—N2 | 111.9 (2) |
| O2i—Cu1—O1 | 92.76 (9) | N1—C1—H1A | 109.2 |
| O2—Cu1—O1i | 92.76 (9) | N2—C1—H1A | 109.2 |
| O2i—Cu1—O1i | 87.24 (9) | N1—C1—H1B | 109.2 |
| O1—Cu1—O1i | 180 | N2—C1—H1B | 109.2 |
| O2—Cu1—O3i | 90.30 (10) | H1A—C1—H1B | 107.9 |
| O2i—Cu1—O3i | 89.70 (10) | N2—C2—N3 | 112.0 (2) |
| O1—Cu1—O3i | 86.64 (9) | N2—C2—H2A | 109.2 |
| O1i—Cu1—O3i | 93.36 (9) | N3—C2—H2A | 109.2 |
| O2—Cu1—O3 | 89.70 (10) | N2—C2—H2B | 109.2 |
| O2i—Cu1—O3 | 90.30 (10) | N3—C2—H2B | 109.2 |
| O1—Cu1—O3 | 93.36 (9) | H2A—C2—H2B | 107.9 |
| O1i—Cu1—O3 | 86.64 (9) | N4—C3—N3 | 112.7 (3) |
| O3i—Cu1—O3 | 180 | N4—C3—H3A | 109.1 |
| Cu1—O1—H1W | 109.5 | N3—C3—H3A | 109.1 |
| Cu1—O1—H2W | 126.7 | N4—C3—H3B | 109.1 |
| H1W—O1—H2W | 113.2 | N3—C3—H3B | 109.1 |
| Cu1—O2—H3W | 124.5 | H3A—C3—H3B | 107.8 |
| Cu1—O2—H4W | 124.2 | N4—C4—N1 | 112.3 (2) |
| H3W—O2—H4W | 110.9 | N4—C4—H4A | 109.2 |
| Cu1—O3—H5W | 109.5 | N1—C4—H4A | 109.2 |
| Cu1—O3—H6W | 123.5 | N4—C4—H4B | 109.2 |
| H5W—O3—H6W | 113.5 | N1—C4—H4B | 109.2 |
| H7W—O4—H8W | 110.2 | H4A—C4—H4B | 107.9 |
| H9W—O5—H10W | 111.4 | N1—C5—N3 | 112.0 (2) |
| C1—N1—C5 | 108.3 (2) | N1—C5—H5A | 109.2 |
| C1—N1—C4 | 108.1 (2) | N3—C5—H5A | 109.2 |
| C5—N1—C4 | 108.3 (3) | N1—C5—H5B | 109.2 |
| C6—N2—C2 | 108.5 (2) | N3—C5—H5B | 109.2 |
| C6—N2—C1 | 108.5 (2) | H5A—C5—H5B | 107.9 |
| C2—N2—C1 | 108.0 (2) | N2—C6—N4 | 112.1 (2) |
| C3—N3—C2 | 108.0 (3) | N2—C6—H6A | 109.2 |
| C3—N3—C5 | 108.1 (2) | N4—C6—H6A | 109.2 |
| C2—N3—C5 | 107.7 (2) | N2—C6—H6B | 109.2 |
| C3—N4—C4 | 108.1 (3) | N4—C6—H6B | 109.2 |
| C3—N4—C6 | 107.9 (2) | H6A—C6—H6B | 107.9 |
| C5—N1—C1—N2 | −58.7 (3) | C3—N4—C4—N1 | −57.9 (3) |
| C4—N1—C1—N2 | 58.3 (3) | C6—N4—C4—N1 | 58.4 (3) |
| C6—N2—C1—N1 | −58.5 (3) | C1—N1—C4—N4 | −58.8 (3) |
| C2—N2—C1—N1 | 58.9 (3) | C5—N1—C4—N4 | 58.3 (3) |
| C6—N2—C2—N3 | 58.4 (3) | C1—N1—C5—N3 | 58.7 (3) |
| C1—N2—C2—N3 | −59.0 (3) | C4—N1—C5—N3 | −58.2 (3) |
| C3—N3—C2—N2 | −57.7 (3) | C3—N3—C5—N1 | 58.0 (3) |
| C5—N3—C2—N2 | 58.8 (3) | C2—N3—C5—N1 | −58.5 (3) |
| C4—N4—C3—N3 | 58.1 (3) | C2—N2—C6—N4 | −58.6 (3) |
| C6—N4—C3—N3 | −58.2 (3) | C1—N2—C6—N4 | 58.5 (3) |
| C2—N3—C3—N4 | 58.1 (3) | C3—N4—C6—N2 | 58.2 (3) |
| C5—N3—C3—N4 | −58.2 (3) | C4—N4—C6—N2 | −58.3 (3) |
Symmetry codes: (i) −x+1, −y, −z.
Hydrogen-bond geometry (Å, °)
| D—H···A | D—H | H···A | D···A | D—H···A |
| O1—H1W···N3 | 0.82 | 2.04 | 2.814 (3) | 158 |
| O1—H2W···O5ii | 0.83 | 1.94 | 2.734 (3) | 162 |
| O2—H3W···N2iii | 0.83 | 1.99 | 2.800 (3) | 167 |
| O2—H4W···O4iii | 0.83 | 1.89 | 2.700 (3) | 165 |
| O3—H5W···Cl1 | 0.82 | 2.54 | 3.190 (2) | 137 |
| O3—H6W···N1iv | 0.82 | 2.00 | 2.805 (3) | 165 |
| O4—H7W···Cl1 | 0.83 | 2.35 | 3.170 (3) | 168 |
| O4—H8W···N4v | 0.84 | 2.00 | 2.829 (4) | 174 |
| O5—H9W···Cl1 | 0.83 | 2.43 | 3.245 (3) | 169 |
| O5—H10W···Cl1vi | 0.83 | 2.37 | 3.200 (3) | 175 |
Symmetry codes: (ii) x, y, z−1; (iii) −x+1, −y+1, −z+1; (iv) x, y−1, z; (v) −x, −y+1, −z+1; (vi) −x, −y, −z+1.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: LH2645).
References
Associated Data
This section collects any data citations, data availability statements, or supplementary materials included in this article.
Supplementary Materials
Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536808020916/lh2645sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536808020916/lh2645Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report



