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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2011 Dec 10;68(Pt 1):m38–m39. doi: 10.1107/S1600536811052512

Poly[[{μ3-dihydrogen [(pyridin-4-yl­methyl­imino)­bis­(methyl­ene)]diphos­phon­ato-κ5 O:O′,N,O′′:N′}copper(II)] dihydrate]

Shi-Yong Zhang a, Zhong-Gao Zhou a,*, Ke-Jun Wang a
PMCID: PMC3254309  PMID: 22259339

Abstract

In the title polymer, {[Cu(C8H12N2O6P2)]·2H2O}n, the geometry of the five-coordinate CuII ion can best be described as slightly distorted square-pyramidal formed by one N and two O atoms of an N(CH2PO3H)2 group and one N atom from a pyridine ring. The elongated apex of the pyramid is occupied by one O atom from a third diphospho­nate ligand. The inter­connection of Cu2+ ions by the diphospho­nate ligands results in the formation of a double-chain array along the b axis, in which the two sub-chains are inter­locked by pairs of PO3 groups. The outside of each sub-chain is decorated by other PO3 groups. These double chains are further assembled into a three-dimensional supra­molecular architecture via a large number of O—H⋯O hydrogen bonds between the phospho­nate groups and lattice water mol­ecules.

Related literature

For background to metal phospho­nate chemistry, see: Maeda (2004); Mao (2007); Shimizu et al. (2009). For the synthetic strategy of attaching functional groups to a phospho­nic acid ligand, see: Drumel et al. (1995); Mao et al. (2002); Liang & Shimizu (2007); Du et al. (2006, 2010b ). For a structurally related complex, see: Song & Mao (2005). For the zwitterionic behavior of amino­phospho­nic acid, see: Yang et al. (2008); Du et al. (2009, 2010a ).graphic file with name e-68-00m38-scheme1.jpg

Experimental

Crystal data

  • [Cu(C8H12N2O6P2)]·2H2O

  • M r = 393.71

  • Triclinic, Inline graphic

  • a = 8.9250 (3) Å

  • b = 9.0000 (3) Å

  • c = 10.5066 (3) Å

  • α = 75.648 (2)°

  • β = 67.124 (2)°

  • γ = 67.126 (2)°

  • V = 711.75 (4) Å3

  • Z = 2

  • Mo Kα radiation

  • μ = 1.80 mm−1

  • T = 296 K

  • 0.40 × 0.03 × 0.02 mm

Data collection

  • Bruker APEXII CCD diffractometer

  • Absorption correction: multi-scan (SADABS; Bruker, 2008) T min = 0.605, T max = 0.746

  • 7659 measured reflections

  • 3267 independent reflections

  • 2309 reflections with I > 2σ(I)

  • R int = 0.043

Refinement

  • R[F 2 > 2σ(F 2)] = 0.046

  • wR(F 2) = 0.118

  • S = 1.03

  • 3267 reflections

  • 202 parameters

  • 6 restraints

  • H atoms treated by a mixture of independent and constrained refinement

  • Δρmax = 0.50 e Å−3

  • Δρmin = −0.60 e Å−3

Data collection: APEX2 (Bruker, 2008); cell refinement: SAINT (Bruker, 2008); 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) and DIAMOND (Brandenburg, 2010); software used to prepare material for publication: SHELXTL.

Supplementary Material

Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536811052512/fj2483sup1.cif

e-68-00m38-sup1.cif (17.3KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811052512/fj2483Isup2.hkl

e-68-00m38-Isup2.hkl (160.2KB, hkl)

Additional supplementary materials: crystallographic information; 3D view; checkCIF report

Table 1. Hydrogen-bond geometry (Å, °).

D—H⋯A D—H H⋯A DA D—H⋯A
O1—H1B⋯O1W 0.82 1.68 2.494 (4) 169
O6—H6C⋯O2W 0.82 1.75 2.567 (5) 172
O1W—H1WA⋯O5i 0.83 (2) 1.92 (2) 2.746 (4) 177 (5)
O1W—H1WB⋯O5ii 0.84 (2) 1.93 (2) 2.747 (4) 167 (5)
O2W—H2WA⋯O1iii 0.85 (2) 2.09 (3) 2.882 (4) 155 (5)
O2W—H2WB⋯O3iv 0.85 (2) 1.96 (3) 2.776 (4) 161 (6)

Symmetry codes: (i) Inline graphic; (ii) Inline graphic; (iii) Inline graphic; (iv) Inline graphic.

Acknowledgments

This work was supported by the NSF of Jiangxi Provincial Education Department (grant No. GJJ10714).

supplementary crystallographic information

Comment

During the past few decades, the syntheses of metal phosphonates with various structures has attracted much attention, owing to their potential applications in areas such as catalysis, ion exchange, intercalation chemistry, and material chemistry (Maeda, 2004; Mao, 2007; Shimizu et al., 2009). The strategy of attaching functional groups such as amine, hydroxyl, carboxylate, sulfonate, and sulfone groups to the phosphonic acid has proven to be an effective method for the isolation of a variety of metal phosphonates with new structures (Drumel et al., 1995; Mao et al., 2002; Liang & Shimizu, 2007; Du et al. 2006, 2010b). Recently, we are interested in the combination of multiple functional groups to phosphonic acid as a more complex ligand. Herein, we report a copper(II) phosphonate based on an amino-bis(methyl-phosphonic acid) ligand, which contains pyridyl group as an additional functional group. As far as we are aware, only one layered cobalt(II) phosphonate has been reported based on the same ligand (Song & Mao, 2005).

The title compound (I) features a one-dimensional double-chain structure. The formula of it contains one Cu2+ ion, one H2L2- anion and two lattice water molecules. Cu(1) ion is five-coordinate and its coordination geometry can be described as a slightly distorted square-pyramid (Fig. 1): the square plane is formed by one N and two O atoms of a N(CH2PO3H)2 group as well as one N atom of a pyridyl group from two H2L2- ligand, and the prolonged apex of the pyramid is occupied by one O atom from a third H2L2- ligand. The H2L2- ligand in compound (I) acts as a pentadentate chelating and bridging ligand. It chelates one Cu2+ ion by its N(CH2PO3H)2 group in a tridentate fashion (2O and 1 N), and also bridges with other two Cu2+ ions via its pyridyl group and a third O atom (Scheme 1). The two phosphonate groups of the H2L2- ligand both are 1H-protonated as the requirement for charge balance and also as indicated by two much longer P—O bonds. It is worthy of note that the strongly basic N atom in the H2L2- ligand is not protonated but bonded to a Cu2+ ion, which is rarely observed for phosphonic acid ligands containing a tertiary amine group (Yang et al., 2008; Du et al., 2009, 2010a).

The interconnection of the Cu2+ ions by the HL2- anions results in the formation of a one-dimensional double-chain array along the b-axis, in which the two sub-chains are inter-locked by pairs of P(1)O3 groups and the outside of each sub-chain is decorated by P(2)O3 groups. It is worthy of note that such two sub-chains are related by inversion centers, and the shortest Cd···Cd distance between them is 5.170 (4) Å while that in each sub-chain is 9.000 (1) Å. These double-chains are further assembled into a three-dimensional supramolecular architecture via a large number of hydrogen bonds between the phosphonate groups and lattice water molecules (Fig. 3 and Table 1).

Experimental

4-Pyridyl-CH2N(CH2PO3H2)2 (0.2 mmol) was dissolved in 4 ml H2O and poured into a test tube, then CuCl2.2H2O (0.15 mmol) dissolved in 8 ml EtOH was carefully layered onto it and left to stand at room temperature. Blue column-shaped crystals of (I) were obtained after about two weeks later. IR data for (I) (KBr, cm-1): 3477(s), 3228(s), 3141(m), 3079(m), 2975(m), 2913(m), 2376(m), 1846(m), 1624(s), 1502(m), 1448(m), 1433(m), 1350(m), 1266(s), 1221(m), 1173(s), 1140(versus), 1065(s), 1051(s), 1032(s), 945(s), 929(m), 906(m), 866(m), 844(m), 795(m), 742(m), 648(m), 588(s), 524(m), 482(m), 453(m).

Refinement

C-bound H atoms were placed in idealized positions and constrained to ride on their parent atoms, with C—H distances of 0.93 or 0.97 Å, and with Uiso(H) = 1.2Ueq(C). H atoms of –PO3H- groups were also placed in idealized positions and constrained to ride on their parent atoms, with O—H distances of 0.82 Å, and with Uiso(H) = 1.2Ueq(O). Water H atoms were located in a difference map and refined with Uiso(H) values set at 1.5Ueq(O). The O—H distances of water were restrained to be 0.85 (1) Å.

Figures

Fig. 1.

Fig. 1.

View of the selected unit of (I), showing the atom-numbering scheme. Displacement ellipsoids are drawn at the 30% probability level. [Symmetry codes: (i) x, y + 1, z; (ii) -x + 1, -y + 1, -z + 1; (iii) x, y - 1, z.]

Fig. 2.

Fig. 2.

View of the double-chain structure of (I) along the b-axis. The CPO3 tetrahedra are shaded in purple. Cu, N and C atoms are drawn as cyan, blue and black circles, respectively.

Fig. 3.

Fig. 3.

View of the structure of (I) down the b-axis. For display details, see the caption for Fig. 2. Hydrogen bonds are represented by dashed lines.

Crystal data

[Cu(C8H12N2O6P2)]·2H2O Z = 2
Mr = 393.71 F(000) = 402
Triclinic, P1 Dx = 1.837 Mg m3
Hall symbol: -P 1 Mo Kα radiation, λ = 0.71073 Å
a = 8.9250 (3) Å Cell parameters from 1430 reflections
b = 9.0000 (3) Å θ = 2.1–27.6°
c = 10.5066 (3) Å µ = 1.80 mm1
α = 75.648 (2)° T = 296 K
β = 67.124 (2)° Needle, blue
γ = 67.126 (2)° 0.40 × 0.03 × 0.02 mm
V = 711.75 (4) Å3

Data collection

Bruker APEXII CCD diffractometer 3267 independent reflections
Radiation source: fine-focus sealed tube 2309 reflections with I > 2σ(I)
graphite Rint = 0.043
phi and ω scans θmax = 27.6°, θmin = 2.1°
Absorption correction: multi-scan (SADABS; Bruker, 2008) h = −10→11
Tmin = 0.605, Tmax = 0.746 k = −11→11
7659 measured reflections l = −13→13

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)] = 0.046 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.118 H atoms treated by a mixture of independent and constrained refinement
S = 1.03 w = 1/[σ2(Fo2) + (0.055P)2 + 0.1702P] where P = (Fo2 + 2Fc2)/3
3267 reflections (Δ/σ)max < 0.001
202 parameters Δρmax = 0.50 e Å3
6 restraints Δρmin = −0.60 e Å3

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 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 0.47006 (6) 0.60143 (5) 0.25556 (5) 0.02485 (17)
P1 0.69833 (14) 0.32696 (12) 0.39341 (11) 0.0237 (2)
P2 0.17163 (14) 0.57368 (13) 0.21239 (12) 0.0265 (3)
N1 0.5076 (4) −0.1825 (4) 0.2025 (3) 0.0240 (7)
N2 0.4396 (4) 0.3746 (4) 0.2980 (3) 0.0207 (7)
C1 0.3823 (5) −0.0485 (5) 0.1777 (4) 0.0282 (9)
H1A 0.2869 −0.0590 0.1696 0.034*
C2 0.3912 (5) 0.1042 (5) 0.1641 (4) 0.0293 (10)
H2A 0.3025 0.1945 0.1457 0.035*
C3 0.5301 (5) 0.1261 (4) 0.1773 (4) 0.0233 (9)
C4 0.6596 (6) −0.0148 (5) 0.1992 (4) 0.0294 (9)
H4A 0.7570 −0.0076 0.2065 0.035*
C5 0.6465 (5) −0.1652 (5) 0.2102 (4) 0.0273 (9)
H5A 0.7364 −0.2575 0.2233 0.033*
C6 0.5389 (5) 0.2920 (4) 0.1674 (4) 0.0243 (9)
H6A 0.4964 0.3607 0.0933 0.029*
H6B 0.6587 0.2831 0.1412 0.029*
C7 0.5053 (5) 0.2840 (5) 0.4152 (4) 0.0235 (9)
H7A 0.5324 0.1684 0.4164 0.028*
H7B 0.4179 0.3168 0.5029 0.028*
C8 0.2500 (5) 0.4113 (5) 0.3387 (4) 0.0224 (8)
H8A 0.1931 0.4454 0.4312 0.027*
H8B 0.2255 0.3151 0.3391 0.027*
O1 0.8567 (4) 0.1971 (3) 0.3047 (3) 0.0309 (7)
H1B 0.9034 0.2423 0.2302 0.046*
O2 0.6750 (3) 0.4935 (3) 0.3111 (3) 0.0278 (6)
O3 0.7175 (4) 0.3101 (3) 0.5319 (3) 0.0307 (7)
O4 0.2907 (3) 0.6731 (3) 0.1706 (3) 0.0273 (6)
O5 0.1664 (4) 0.5097 (3) 0.0961 (3) 0.0356 (7)
O6 −0.0163 (4) 0.6712 (4) 0.2955 (3) 0.0393 (8)
H6C −0.0137 0.7334 0.3394 0.059*
O1W 1.0256 (4) 0.3000 (4) 0.0716 (3) 0.0381 (8)
H1WA 1.065 (6) 0.366 (5) 0.078 (5) 0.057*
H1WB 0.964 (6) 0.344 (5) 0.021 (5) 0.057*
O2W −0.0383 (5) 0.8732 (4) 0.4421 (4) 0.0462 (9)
H2WA −0.037 (7) 0.965 (4) 0.397 (5) 0.069*
H2WB 0.053 (5) 0.832 (6) 0.464 (6) 0.069*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
Cu1 0.0279 (3) 0.0187 (3) 0.0339 (3) −0.0064 (2) −0.0186 (2) −0.0011 (2)
P1 0.0258 (6) 0.0185 (5) 0.0290 (6) −0.0027 (4) −0.0154 (5) −0.0030 (4)
P2 0.0283 (6) 0.0233 (5) 0.0369 (6) −0.0077 (5) −0.0215 (5) −0.0020 (5)
N1 0.0277 (18) 0.0195 (17) 0.0268 (19) −0.0072 (14) −0.0117 (15) −0.0025 (14)
N2 0.0248 (17) 0.0177 (16) 0.0235 (17) −0.0068 (14) −0.0127 (15) −0.0014 (13)
C1 0.026 (2) 0.023 (2) 0.042 (3) −0.0039 (17) −0.018 (2) −0.0081 (19)
C2 0.030 (2) 0.022 (2) 0.040 (3) −0.0025 (18) −0.020 (2) −0.0054 (18)
C3 0.028 (2) 0.0192 (19) 0.023 (2) −0.0061 (17) −0.0087 (18) −0.0038 (16)
C4 0.031 (2) 0.028 (2) 0.034 (2) −0.0097 (19) −0.015 (2) −0.0042 (19)
C5 0.028 (2) 0.0169 (19) 0.039 (3) −0.0065 (17) −0.017 (2) −0.0003 (18)
C6 0.028 (2) 0.022 (2) 0.027 (2) −0.0063 (17) −0.0142 (18) −0.0024 (17)
C7 0.031 (2) 0.0188 (19) 0.023 (2) −0.0078 (17) −0.0125 (18) 0.0005 (16)
C8 0.023 (2) 0.022 (2) 0.026 (2) −0.0100 (17) −0.0100 (18) −0.0025 (17)
O1 0.0302 (16) 0.0228 (15) 0.0335 (17) −0.0006 (13) −0.0123 (14) −0.0028 (13)
O2 0.0279 (16) 0.0194 (14) 0.0395 (17) −0.0054 (12) −0.0194 (14) 0.0008 (13)
O3 0.0312 (17) 0.0335 (16) 0.0321 (17) −0.0054 (13) −0.0200 (14) −0.0043 (13)
O4 0.0315 (16) 0.0234 (14) 0.0367 (17) −0.0100 (12) −0.0243 (14) 0.0038 (13)
O5 0.049 (2) 0.0308 (16) 0.0431 (19) −0.0148 (15) −0.0302 (16) −0.0026 (14)
O6 0.0290 (17) 0.0360 (18) 0.061 (2) −0.0048 (14) −0.0248 (16) −0.0111 (16)
O1W 0.041 (2) 0.0387 (19) 0.042 (2) −0.0163 (16) −0.0204 (16) 0.0014 (15)
O2W 0.048 (2) 0.0337 (19) 0.061 (2) −0.0053 (17) −0.030 (2) −0.0057 (17)

Geometric parameters (Å, °)

Cu1—O2 1.949 (3) C2—C3 1.390 (5)
Cu1—O4 1.949 (2) C2—H2A 0.9300
Cu1—N1i 2.008 (3) C3—C4 1.385 (5)
Cu1—N2 2.080 (3) C3—C6 1.501 (5)
Cu1—O3ii 2.315 (3) C4—C5 1.376 (5)
P1—O3 1.495 (3) C4—H4A 0.9300
P1—O2 1.514 (3) C5—H5A 0.9300
P1—O1 1.570 (3) C6—H6A 0.9700
P1—C7 1.827 (4) C6—H6B 0.9700
P2—O5 1.497 (3) C7—H7A 0.9700
P2—O4 1.518 (3) C7—H7B 0.9700
P2—O6 1.563 (3) C8—H8A 0.9700
P2—C8 1.831 (4) C8—H8B 0.9700
N1—C1 1.340 (5) O1—H1B 0.8200
N1—C5 1.341 (5) O3—Cu1ii 2.315 (3)
N1—Cu1iii 2.008 (3) O6—H6C 0.8200
N2—C7 1.489 (5) O1W—H1WA 0.832 (19)
N2—C8 1.492 (5) O1W—H1WB 0.836 (19)
N2—C6 1.507 (5) O2W—H2WA 0.846 (19)
C1—C2 1.376 (6) O2W—H2WB 0.848 (19)
C1—H1A 0.9300
O2—Cu1—O4 167.12 (11) C3—C2—H2A 119.4
O2—Cu1—N1i 93.65 (12) C4—C3—C2 115.6 (3)
O4—Cu1—N1i 92.92 (12) C4—C3—C6 122.4 (4)
O2—Cu1—N2 86.48 (11) C2—C3—C6 121.9 (3)
O4—Cu1—N2 86.29 (11) C5—C4—C3 121.1 (4)
N1i—Cu1—N2 176.50 (13) C5—C4—H4A 119.4
O2—Cu1—O3ii 96.97 (11) C3—C4—H4A 119.4
O4—Cu1—O3ii 94.37 (11) N1—C5—C4 121.9 (4)
N1i—Cu1—O3ii 87.53 (12) N1—C5—H5A 119.0
N2—Cu1—O3ii 95.93 (11) C4—C5—H5A 119.0
O3—P1—O2 116.53 (16) C3—C6—N2 115.5 (3)
O3—P1—O1 108.57 (16) C3—C6—H6A 108.4
O2—P1—O1 110.13 (17) N2—C6—H6A 108.4
O3—P1—C7 110.01 (18) C3—C6—H6B 108.4
O2—P1—C7 103.88 (16) N2—C6—H6B 108.4
O1—P1—C7 107.31 (17) H6A—C6—H6B 107.5
O5—P2—O4 115.75 (17) N2—C7—P1 109.1 (3)
O5—P2—O6 108.56 (17) N2—C7—H7A 109.9
O4—P2—O6 111.15 (16) P1—C7—H7A 109.9
O5—P2—C8 112.42 (17) N2—C7—H7B 109.9
O4—P2—C8 103.00 (16) P1—C7—H7B 109.9
O6—P2—C8 105.44 (18) H7A—C7—H7B 108.3
C1—N1—C5 118.3 (3) N2—C8—P2 108.1 (3)
C1—N1—Cu1iii 120.0 (3) N2—C8—H8A 110.1
C5—N1—Cu1iii 121.1 (3) P2—C8—H8A 110.1
C7—N2—C8 111.7 (3) N2—C8—H8B 110.1
C7—N2—C6 112.3 (3) P2—C8—H8B 110.1
C8—N2—C6 112.8 (3) H8A—C8—H8B 108.4
C7—N2—Cu1 107.6 (2) P1—O1—H1B 109.5
C8—N2—Cu1 104.3 (2) P1—O2—Cu1 119.08 (16)
C6—N2—Cu1 107.7 (2) P1—O3—Cu1ii 133.88 (16)
N1—C1—C2 121.7 (4) P2—O4—Cu1 117.93 (16)
N1—C1—H1A 119.1 P2—O6—H6C 109.5
C2—C1—H1A 119.1 H1WA—O1W—H1WB 109 (4)
C1—C2—C3 121.3 (4) H2WA—O2W—H2WB 107 (4)
C1—C2—H2A 119.4

Symmetry codes: (i) x, y+1, z; (ii) −x+1, −y+1, −z+1; (iii) x, y−1, z.

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
O1—H1B···O1W 0.82 1.68 2.494 (4) 169
O6—H6C···O2W 0.82 1.75 2.567 (5) 172
O1W—H1WA···O5iv 0.83 (2) 1.92 (2) 2.746 (4) 177 (5)
O1W—H1WB···O5v 0.84 (2) 1.93 (2) 2.747 (4) 167 (5)
O2W—H2WA···O1vi 0.85 (2) 2.09 (3) 2.882 (4) 155 (5)
O2W—H2WB···O3ii 0.85 (2) 1.96 (3) 2.776 (4) 161 (6)

Symmetry codes: (iv) x+1, y, z; (v) −x+1, −y+1, −z; (vi) x−1, y+1, z; (ii) −x+1, −y+1, −z+1.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: FJ2483).

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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, global. DOI: 10.1107/S1600536811052512/fj2483sup1.cif

e-68-00m38-sup1.cif (17.3KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811052512/fj2483Isup2.hkl

e-68-00m38-Isup2.hkl (160.2KB, hkl)

Additional supplementary materials: crystallographic information; 3D view; checkCIF report


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