Abstract
The title compound, poly[[diaquacopper(II)]-μ3-hydrogenphosphito], [Cu(HPO3)(H2O)2]n, (I), has been prepared by hydrothermal synthesis at 393 K. Its non-centrosymmetric polymorph structure, (II), was known previously and has been redetermined at 193 (2) K [El Bali & Massa (2002 ▶). Acta Cryst. E58, i29–i31]. The Cu atoms in (I) and (II) are square-pyramidal coordinated. A distorted octahedral geometry around the Cu atoms is considered by including the strongly elongated apical distances of 2.8716 (15) Å in (I) and 3.000 (1) Å in (II). The Cu⋯Cu separation of the dimeric unit is 3.1074 (3) Å. The secondary building units (SBU) (the Cu2O2 dimer and two HPO3 units) in (I) are inversion related and form a two-dimensional layered structure, with sheets parallel to the bc plane, whereas in the structure of (II), the chain elements are connected via screw-axis symmetry to form a three-dimensional microporous framework. In both polymorph structures, strong O—H⋯O hydrogen bonds are observed.
Related literature
For the structure of the noncentrosymmetric polymorph, see: Handlovič (1969 ▶) and El Bali & Massa (2002 ▶). For a discussion on secondary building units (SBU), see: Biradha (2007 ▶). For the structure of an open-framework zincophosphite built up from polyhedral 12-rings, see: Harrison et al. (2001 ▶).
Experimental
Crystal data
[Cu(HPO3)(H2O)2]
M r = 179.55
Monoclinic,
a = 7.12940 (10) Å
b = 7.33460 (10) Å
c = 8.8313 (2) Å
β = 110.4280 (10)°
V = 432.76 (1) Å3
Z = 4
Mo Kα radiation
μ = 5.32 mm−1
T = 296 K
0.25 × 0.25 × 0.20 mm
Data collection
Bruker APEXII CCD diffractometer
Absorption correction: multi-scan (SHELXTL; Sheldrick, 2008 ▶) T min = 0.288, T max = 0.345
3641 measured reflections
994 independent reflections
980 reflections with I > 2σ(I)
R int = 0.023
Refinement
R[F 2 > 2σ(F 2)] = 0.018
wR(F 2) = 0.049
S = 1.18
994 reflections
85 parameters
6 restraints
H atoms treated by a mixture of independent and constrained refinement
Δρmax = 0.44 e Å−3
Δρmin = −0.42 e Å−3
Data collection: APEX2 (Bruker, 2001 ▶); cell refinement: SAINT (Bruker, 2001 ▶); 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: SHELXL97 and PLATON (Spek, 2009 ▶).
Supplementary Material
Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536809009088/si2150sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536809009088/si2150Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report
Table 1. Selected geometric parameters (Å, °).
| Cu1—O3 | 1.9293 (14) |
| Cu1—O1 | 1.9607 (14) |
| Cu1—O2 | 1.9774 (14) |
| Cu1—O4 | 1.9960 (14) |
| Cu1—O5 | 2.2396 (17) |
| Cu1—O3i | 2.8716 (15) |
| O1—Cu1—O2 | 160.25 (6) |
| O3—Cu1—O4 | 177.82 (6) |
| O3—Cu1—O5 | 97.18 (6) |
| O2—Cu1—O5 | 104.95 (6) |
Symmetry code: (i)
.
Table 2. Hydrogen-bond geometry (Å, °).
| D—H⋯A | D—H | H⋯A | D⋯A | D—H⋯A |
|---|---|---|---|---|
| O4—H4A⋯O1ii | 0.878 (17) | 1.81 (2) | 2.658 (2) | 162 (4) |
| O4—H4B⋯O2iii | 0.890 (16) | 1.864 (16) | 2.728 (2) | 163 (2) |
| O5—H5A⋯O2iii | 0.867 (18) | 2.18 (3) | 2.925 (2) | 143 (3) |
| O5—H5A⋯O3iv | 0.867 (18) | 2.60 (3) | 3.380 (2) | 151 (3) |
| O5—H5B⋯O4v | 0.851 (18) | 1.985 (18) | 2.818 (2) | 166 (3) |
Symmetry codes: (ii)
; (iii)
; (iv)
; (v)
.
Acknowledgments
The authors thank the Co-editor for help with the paper.
supplementary crystallographic information
Comment
Cu atoms in the asymmetric unit are pentahedrally coordinated and link three P atoms via phosphite O atoms (O1, O2, O3) with shorter distances and two water molecules (O4, O5) with longer distances (Fig. 1 and Table 1). A distorted octahedral geometry around the Cu atoms are considered when the strongly elongated apical Cu—O distances of 3.036 (14) Å (Handlovič, 1969), 3.000 (1) Å in II (El Bali & Massa, 2002), and 2.8716 (15) in I are included. The P atoms form the centers of a pseudo pyramid with the hydrogen phosphite groups, and each P links to three Cu via P—O—Cu bonds. The P—O bonds are in the range of 1.5178 (14) - 1.5337 (14) Å. The two-dimensional structure (Fig. 2) is built up from SBU (Biradha, 2007) (secondary building units, Fig.1), the corner sharing of tetra-meric units. One Cu atom links two P atom via O1 and O2. Two pentahedra Cu(H2O)2O3, and two pseudopyramids HPO3 form a dinucleus unit, noted as SBU. The Cu···Cu distance in the dimeric unit of I is 3.1074 (3) Å. The SBU and hydrogenphosphite polyhedra are connected into a one-dimensional chain by sharing the corner O3, and each chain links two other chains by sharing other atoms O3, forming a sheet along the bc-plane, containing 8-membered rings when the long Cu—O3c distance is neglected. In the structure of (CN3H6)2.Zn(HPO3)2, ZnO4 and HPO3building units form a 12-ring framework (Harrison et al., 2001). In both polymorph structures strong O—H···O hydrogen bonds are observed (Table 2).
Experimental
All reagents were of analytical grade. The title sample was prepared by Cu(NO3)2, H2O, H3(PO3) and (C2H5)3N triethylamine in the molar ratio 1:144:5:11 and heated at 393 K for 8 d. The blue single crystals were filtered, washed with distilled water and dried in air.
Refinement
The H atoms of the water molecules were located from a difference density map and were refined with distance restraints of d(H–H) = 1.40 (2) Å, d(O–H) = 0.90 (2) Å, and with isotropic displacement parameters. The H atom of the hydrogenphosphite group was freely refined.
Figures
Fig. 1.
A section of the structure of (I) showing the centrosymmetric SBU with the edge-sharing distorted CuO6 octahedra. Displacement ellipsoids are drawn at the 50% probability level. Atoms labelled a, b, c are symmetry-related. Symmetry codes: (a = - x, -1/2 + y, 3/2 - z; (b = - x, 1/2 + y, 3/2 - z; (c = - x, - y, 1 - z).
Fig. 2.
The layer structure of (I), viewed down the a axis.
Crystal data
| [Cu(HPO3)(H2O)2] | F(000) = 356 |
| Mr = 179.55 | Dx = 2.756 Mg m−3 |
| Monoclinic, P21/c | Mo Kα radiation, λ = 0.71073 Å |
| a = 7.1294 (1) Å | Cell parameters from 3157 reflections |
| b = 7.3346 (1) Å | θ = 3.1–27.5° |
| c = 8.8313 (2) Å | µ = 5.32 mm−1 |
| β = 110.428 (1)° | T = 296 K |
| V = 432.76 (1) Å3 | Block, blue |
| Z = 4 | 0.25 × 0.25 × 0.20 mm |
Data collection
| Bruker APEXII CCD diffractometer | 994 independent reflections |
| Radiation source: fine-focus sealed tube | 980 reflections with I > 2σ(I) |
| graphite | Rint = 0.023 |
| φ and ω scans | θmax = 27.5°, θmin = 3.1° |
| Absorption correction: multi-scan (SHELXTL; Sheldrick, 2008) | h = −9→9 |
| Tmin = 0.288, Tmax = 0.345 | k = −9→9 |
| 3641 measured reflections | l = −10→11 |
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)] = 0.018 | H atoms treated by a mixture of independent and constrained refinement |
| wR(F2) = 0.049 | w = 1/[σ2(Fo2) + (0.0209P)2 + 0.4287P] where P = (Fo2 + 2Fc2)/3 |
| S = 1.18 | (Δ/σ)max < 0.001 |
| 994 reflections | Δρmax = 0.44 e Å−3 |
| 85 parameters | Δρmin = −0.42 e Å−3 |
| 6 restraints | Extinction correction: SHELXL97 (Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4 |
| Primary atom site location: structure-invariant direct methods | Extinction coefficient: 0.134 (4) |
Special details
| 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. |
| 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 | ||
| Cu1 | 0.22809 (3) | 0.02792 (3) | 0.58956 (3) | 0.01035 (13) | |
| P1 | −0.08713 (7) | 0.28227 (6) | 0.66809 (6) | 0.00990 (15) | |
| O1 | 0.1259 (2) | 0.21752 (19) | 0.69683 (17) | 0.0145 (3) | |
| O2 | 0.2458 (2) | −0.1406 (2) | 0.42031 (17) | 0.0144 (3) | |
| O3 | 0.1081 (2) | −0.1660 (2) | 0.67218 (17) | 0.0173 (3) | |
| O4 | 0.3581 (2) | 0.22142 (19) | 0.50133 (17) | 0.0129 (3) | |
| O5 | 0.5311 (3) | 0.0183 (2) | 0.7831 (2) | 0.0234 (4) | |
| H1 | −0.116 (4) | 0.420 (4) | 0.582 (3) | 0.019 (6)* | |
| H4A | 0.298 (4) | 0.262 (5) | 0.403 (3) | 0.056 (12)* | |
| H4B | 0.482 (3) | 0.197 (4) | 0.506 (3) | 0.022 (7)* | |
| H5A | 0.630 (4) | 0.073 (4) | 0.766 (4) | 0.051 (10)* | |
| H5B | 0.580 (5) | −0.075 (3) | 0.841 (4) | 0.043 (9)* |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| Cu1 | 0.01143 (18) | 0.01023 (17) | 0.01156 (17) | −0.00141 (8) | 0.00675 (12) | −0.00082 (7) |
| P1 | 0.0107 (3) | 0.0093 (2) | 0.0109 (2) | 0.00038 (17) | 0.00539 (19) | −0.00079 (16) |
| O1 | 0.0100 (7) | 0.0186 (7) | 0.0154 (7) | −0.0006 (5) | 0.0049 (6) | −0.0061 (5) |
| O2 | 0.0115 (7) | 0.0159 (7) | 0.0179 (7) | −0.0029 (5) | 0.0076 (6) | −0.0055 (5) |
| O3 | 0.0229 (8) | 0.0169 (7) | 0.0156 (7) | −0.0058 (6) | 0.0109 (6) | 0.0018 (6) |
| O4 | 0.0118 (7) | 0.0148 (6) | 0.0124 (6) | −0.0009 (5) | 0.0046 (5) | 0.0008 (5) |
| O5 | 0.0128 (8) | 0.0286 (9) | 0.0256 (9) | 0.0001 (6) | 0.0027 (7) | 0.0126 (7) |
Geometric parameters (Å, °)
| Cu1—O3 | 1.9293 (14) | P1—O2i | 1.5337 (14) |
| Cu1—O1 | 1.9607 (14) | P1—H1 | 1.24 (3) |
| Cu1—O2 | 1.9774 (14) | O2—P1i | 1.5337 (14) |
| Cu1—O4 | 1.9960 (14) | O3—P1iii | 1.5178 (14) |
| Cu1—O5 | 2.2396 (17) | O4—H4A | 0.878 (17) |
| Cu1—O3i | 2.8716 (15) | O4—H4B | 0.890 (16) |
| P1—O3ii | 1.5178 (14) | O5—H5A | 0.867 (18) |
| P1—O1 | 1.5254 (15) | O5—H5B | 0.851 (18) |
| O3—Cu1—O1 | 92.95 (6) | O3ii—P1—H1 | 108.6 (12) |
| O3—Cu1—O2 | 88.78 (6) | O1—P1—H1 | 107.4 (13) |
| O1—Cu1—O2 | 160.25 (6) | O2i—P1—H1 | 107.6 (13) |
| O3—Cu1—O4 | 177.82 (6) | P1—O1—Cu1 | 131.06 (9) |
| O1—Cu1—O4 | 89.19 (6) | P1i—O2—Cu1 | 125.31 (8) |
| O2—Cu1—O4 | 89.35 (6) | P1iii—O3—Cu1 | 137.43 (9) |
| O3—Cu1—O5 | 97.18 (6) | Cu1—O4—H4A | 120 (2) |
| O1—Cu1—O5 | 94.36 (6) | Cu1—O4—H4B | 115.5 (18) |
| O2—Cu1—O5 | 104.95 (6) | H4A—O4—H4B | 104 (2) |
| O4—Cu1—O5 | 82.23 (6) | Cu1—O5—H5A | 119 (2) |
| O3ii—P1—O1 | 109.79 (8) | Cu1—O5—H5B | 124 (2) |
| O3ii—P1—O2i | 110.37 (8) | H5A—O5—H5B | 107 (2) |
| O1—P1—O2i | 112.85 (8) |
Symmetry codes: (i) −x, −y, −z+1; (ii) −x, y+1/2, −z+3/2; (iii) −x, y−1/2, −z+3/2.
Hydrogen-bond geometry (Å, °)
| D—H···A | D—H | H···A | D···A | D—H···A |
| O4—H4A···O1iv | 0.88 (2) | 1.81 (2) | 2.658 (2) | 162 (4) |
| O4—H4B···O2v | 0.89 (2) | 1.86 (2) | 2.728 (2) | 163 (2) |
| O5—H5A···O2v | 0.87 (2) | 2.18 (3) | 2.925 (2) | 143 (3) |
| O5—H5A···O3vi | 0.87 (2) | 2.60 (3) | 3.380 (2) | 151 (3) |
| O5—H5B···O4vii | 0.85 (2) | 1.99 (2) | 2.818 (2) | 166 (3) |
Symmetry codes: (iv) x, −y+1/2, z−1/2; (v) −x+1, −y, −z+1; (vi) −x+1, y+1/2, −z+3/2; (vii) −x+1, y−1/2, −z+3/2.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: SI2150).
References
- Biradha, K. (2007). Curr. Sci.92, 584–585.
- Bruker (2001). APEX2 and SAINT Bruker AXS Inc., Madison, Wisconsin, USA.
- El Bali, B. & Massa, W. (2002). Acta Cryst. E58, i29–i31.
- Handlovič, M. (1969). Acta Cryst. B25, 227–231.
- Harrison, W. T. A., Phillips, M. L. F. & Nenoff, T. M. (2001). J. Chem. Soc. Dalton Trans. pp. 2459–2461.
- Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
- Spek, A. L. (2009). Acta Cryst. D65, 148–155. [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 datablocks I, global. DOI: 10.1107/S1600536809009088/si2150sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536809009088/si2150Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report


