Abstract
In the coordination polymer, [CuI(C13H11N2O2)]n, the CuI atom exists in a trigonal–planar geometry that is defined by the C=C unit, the imidazole N atom and carboxylate O atoms from three different ozagrel ligands, resulting in the formation of a three-dimensional framework.
Related literature
For background to the design and construction of coordination polymers, see: Kitagawa et al. (2004 ▶); Zhao et al. (2008 ▶). For other olefin complexes, see: Kato et al. (1997 ▶); Wang et al. (2005 ▶, 2007 ▶); Young et al. (1998 ▶); Zhang et al. (2001 ▶).
Experimental
Crystal data
[Cu(C13H11N2O2)]
M r = 290.78
Trigonal,
a = 9.7894 (19) Å
c = 10.483 (2) Å
V = 870.0 (3) Å3
Z = 3
Mo Kα radiation
μ = 1.88 mm−1
T = 293 K
0.20 × 0.20 × 0.20 mm
Data collection
Rigaku Mercury CCD diffractometer
Absorption correction: multi-scan (CrystalClear; Rigaku, 2000 ▶) T min = 0.765, T max = 1.000
6852 measured reflections
2105 independent reflections
1904 reflections with I > 2σ(I)
R int = 0.053
Refinement
R[F 2 > 2σ(F 2)] = 0.042
wR(F 2) = 0.105
S = 1.03
2105 reflections
163 parameters
1 restraint
H-atom parameters constrained
Δρmax = 0.36 e Å−3
Δρmin = −0.32 e Å−3
Absolute structure: Flack (1983 ▶), 773 Friedel pairs
Flack parameter: 0.05 (3)
Data collection: CrystalClear (Rigaku, 2000 ▶); cell refinement: CrystalClear; data reduction: CrystalClear; 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.
Supplementary Material
Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536811015005/ng5155sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536811015005/ng5155Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report
Table 1. Selected geometric parameters (Å, °).
| Cu1—N1i | 1.962 (5) |
| Cu1—C2 | 2.000 (6) |
| Cu1—O2ii | 2.007 (4) |
| Cu1—C3 | 2.030 (5) |
| C2—C3 | 1.381 (7) |
| N1i—Cu1—C2 | 151.2 (2) |
| N1i—Cu1—O2ii | 104.12 (19) |
| C2—Cu1—O2ii | 104.49 (19) |
| N1i—Cu1—C3 | 111.1 (2) |
| C2—Cu1—C3 | 40.1 (2) |
Symmetry codes: (i)
; (ii)
.
Acknowledgments
The author is grateful for grants from the National Natural Science Foundation of China (grant No. 20901037), Fujian Provincial Department of Education (grant No. JB09181) and the Program for New Century Excellent Talents in Fujian Province University (grant No. JK2010043).
supplementary crystallographic information
Comment
The design and construction of coordination polymers have been an area of explosive growth in recent years (Kitagawa et al., 2004). Some active pharmaceutical ingredients (APIs), which contain carboxylic group, N-containing ring in the structures, have also utilized for constructing specific functional coordination polymers (Zhao et al., 2008). The hydrophilic or hydrophobic groups in drug molecules may play an important role in the structures and properties of final metal- organic frameworks.
Ozagrel, (E)-3-[4-(1H-imidiazol-1-ylmethyl)phenyl]-2-propenic acid, is a selective thromboxane A2-synthetase inhibitor which is used for treating cerebrovascular disease (Kato et al., 1997). It has a carboxylic group and an imidazole ring in the structure. The molecule is an ideal building block for constructing coordination polymers with specific structures. In this contribution, we report a Cu(I)-olefin coordination polymer of ozagrel, [(C13H11N2O2)Cu(I)] (I), which was obtained under solvothermal reaction conditions. In the structure, conjugated olefinic and carboxylic groups of ozagrel link metal centers into a 3-fold helical chain which is linked into a three-dimensional framework structure by metal- imidazole coordination interactions.
Compound I crystallizes in the space group P31 with a deprotonated ozagrel anion and a Cu(I) cation in the asymmetric unit (Fig.1). There exist obvious interactions between Cu(I) center and C═C moiety of the olefin of ozagrel (Cu1—C2, Cu1—C3, Table 1). The C═C bond distance (1.381 Å) of the coordinated olefin is longer than that in free ozagrel (1.324 Å) (Wang et al., 2007). The lengthening of the C═C distance is typical for ethylene that is η2-bonded to low-valent, electron-rich, transition metals such as copper(I) (Young et al., 1998). Cu(I) ion is nearly centered in a trigonal planar geometry, which is defined by C═C moiety, imidazole N atom and carboxylic O atom from three different ozagrel molecules. Interestingly, carboxylic group of ozagrel doesn't serve as bidentate moiety as does it in [Cu(3-PYA)]n reported previously (Zhang et al., 2001). But, conjugated olefinic and carboxylic groups as bidentate spacer link Cu(I) centers into a 3-fold helical chain along c axis (Fig.2). Cu(I)-imidazole interactions further link the one-dimensional helical chain into a three-dimensional framework structure (Fig.3). Thus, ozagrel anion acting as a tridentate linker is coordinated to Cu(I) ion generating a three-dimensional coordination polymer based on one-dimensional helical chain of Cu(I) centers.
Since Schultz synthesized the first air-stable Cu(I)-olefin coordination polymer based on fumarate ligand under hydrothermal conditions (Young et al., 1998), some Cu(I)-olefin complexes with extended framework structures have been prepared by crystal engineering strategies (Wang et al., 2005). Impressively, two luminescent two-dimensional layered copper(I)-olefin coordination polymers were constructed by the use of 3(2)-pyridylacrylic acid as tetradentate linkers (Zhang et al., 2001). Therein, acrylic acid anions linked Cu(I) centers into a one-dimensional chain which was further linked into two-dimensional coordination layers by coordinated pyridyl rings. Otherwise from that in pyridylacrylic acid, the acrylic acid anion in ozagrel acts as a bidentate spacer and links Cu(I) centers into a 3-fold helical chain which is further linked into a three-dimensional framework structure by coordinated imidazole ring. In other words, rigid 3(2)-pyridylacrylic acid resulted in two-dimensional coordination layers by metal coordination to Cu(I) ion while more flexible ozagrel gave rise to a three-dimensional coordination framework. The flexible molecular structure of ozagrel could play the subtle role in the final extended structure.
In conclusion, a Cu(I)-olefin coordination polymer based on ozagrel ligand was synthesized under solvothermal conditions. Conjugated olefinic and carboxylic groups of ozagrel as bidentate spacer link Cu(I) centers into a 3-fold helical chain which is linked into a three-dimensional framework structure by metal-imidazole coordination interactions.
Experimental
Ozagrel (228 mg, 1 mmol) and Cu(NO3)2.3H2O (240 mg, 1 mmol) were suspended in 10 ml me thanol and a few drops of triethylamine were added. The mixture was placed in a 23 ml Teflon-lined autoclave, sealed, and placed in a furnace at 130 °C for 2 days. Yellow block crystals were isolated. Element analysis for C13H11N2O2 Cu1 (%), Calcd: C, 53.65; H, 3.22; N, 9.63; Found: C, 53.57; H, 3.89; N, 9.66.
Refinement
H atoms were located geometrically (C—H = 0.95–1.00 Å) with Uiso(H) = 1.2 Ueq(C).
Figures
Fig. 1.
ORTEP of compound I with 30% thermal ellipsoids. A = 1-Y,X—Y,Z+1/3; B = –X+Y,-X,Z+2/3
Fig. 2.

One-dimensional helical chain of Cu(I) along c axis in compound I. Imidazole group of ozagrel is omitted for clarity.
Fig. 3.
The three-dimensional structure of compound I viewed along c axis.
Crystal data
| [Cu(C13H11N2O2)] | Dx = 1.665 Mg m−3 |
| Mr = 290.78 | Mo Kα radiation, λ = 0.71073 Å |
| Trigonal, P31 | Cell parameters from 987 reflections |
| Hall symbol: P 31 | θ = 2.4–27.4° |
| a = 9.7894 (19) Å | µ = 1.88 mm−1 |
| c = 10.483 (2) Å | T = 293 K |
| V = 870.0 (3) Å3 | Block, yellow |
| Z = 3 | 0.20 × 0.20 × 0.20 mm |
| F(000) = 444 |
Data collection
| Rigaku Mercury CCD diffractometer | 2105 independent reflections |
| Radiation source: fine-focus sealed tube | 1904 reflections with I > 2σ(I) |
| graphite | Rint = 0.053 |
| Detector resolution: 13.6612 pixels mm-1 | θmax = 27.5°, θmin = 2.4° |
| φ and ω scans | h = −12→12 |
| Absorption correction: multi-scan (CrystalClear; Rigaku, 2000) | k = −12→12 |
| Tmin = 0.765, Tmax = 1.000 | l = −9→13 |
| 6852 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)] = 0.042 | H-atom parameters constrained |
| wR(F2) = 0.105 | w = 1/[σ2(Fo2) + (0.052P)2 + 0.5211P] where P = (Fo2 + 2Fc2)/3 |
| S = 1.03 | (Δ/σ)max < 0.001 |
| 2105 reflections | Δρmax = 0.36 e Å−3 |
| 163 parameters | Δρmin = −0.32 e Å−3 |
| 1 restraint | Absolute structure: Flack (1983), 773 Friedel pairs |
| Primary atom site location: structure-invariant direct methods | Flack parameter: 0.05 (3) |
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 | 0.44797 (7) | 0.33783 (7) | 0.62232 (6) | 0.03118 (17) | |
| O1 | 0.6474 (5) | 0.5593 (5) | 0.3892 (5) | 0.0532 (12) | |
| N1 | −0.3953 (6) | −0.0278 (5) | 0.1055 (5) | 0.0353 (11) | |
| C1 | 0.6055 (6) | 0.4173 (6) | 0.3901 (5) | 0.0335 (11) | |
| O2 | 0.6941 (4) | 0.3626 (5) | 0.3546 (4) | 0.0413 (9) | |
| N2 | −0.3899 (5) | −0.0886 (6) | 0.3067 (5) | 0.0375 (10) | |
| C2 | 0.4448 (6) | 0.2963 (6) | 0.4352 (5) | 0.0312 (11) | |
| H2 | 0.4069 | 0.1847 | 0.4093 | 0.037* | |
| C3 | 0.3305 (6) | 0.3354 (6) | 0.4620 (5) | 0.0330 (12) | |
| H3 | 0.3597 | 0.4436 | 0.4320 | 0.040* | |
| C4 | 0.1578 (6) | 0.2269 (6) | 0.4662 (5) | 0.0311 (11) | |
| C5 | 0.0875 (7) | 0.0622 (7) | 0.4627 (6) | 0.0403 (13) | |
| H5 | 0.1519 | 0.0150 | 0.4631 | 0.048* | |
| C6 | −0.0749 (7) | −0.0321 (7) | 0.4588 (6) | 0.0406 (13) | |
| H6 | −0.1213 | −0.1436 | 0.4558 | 0.049* | |
| C7 | 0.0604 (6) | 0.2919 (7) | 0.4678 (6) | 0.0387 (13) | |
| H7 | 0.1061 | 0.4034 | 0.4692 | 0.046* | |
| C8 | −0.1017 (7) | 0.1980 (7) | 0.4675 (6) | 0.0417 (14) | |
| H8 | −0.1662 | 0.2449 | 0.4731 | 0.050* | |
| C9 | −0.1707 (6) | 0.0355 (7) | 0.4591 (6) | 0.0357 (12) | |
| C10 | −0.3482 (7) | −0.0695 (9) | 0.4438 (6) | 0.0441 (15) | |
| H10A | −0.3824 | −0.1740 | 0.4824 | 0.053* | |
| H10B | −0.4031 | −0.0216 | 0.4884 | 0.053* | |
| C11 | −0.3627 (7) | 0.0271 (7) | 0.2233 (6) | 0.0403 (13) | |
| H11 | −0.3250 | 0.1340 | 0.2462 | 0.048* | |
| C12 | −0.4460 (7) | −0.2242 (7) | 0.2378 (6) | 0.0449 (14) | |
| H12 | −0.4761 | −0.3261 | 0.2701 | 0.054* | |
| C13 | −0.4504 (7) | −0.1860 (7) | 0.1143 (6) | 0.0392 (13) | |
| H13 | −0.4863 | −0.2579 | 0.0448 | 0.047* |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| Cu1 | 0.0309 (3) | 0.0364 (4) | 0.0284 (3) | 0.0185 (3) | 0.0010 (3) | 0.0030 (3) |
| O1 | 0.038 (2) | 0.035 (2) | 0.082 (4) | 0.0155 (18) | 0.004 (2) | 0.012 (2) |
| N1 | 0.041 (3) | 0.030 (2) | 0.036 (3) | 0.019 (2) | −0.003 (2) | 0.002 (2) |
| C1 | 0.029 (2) | 0.043 (3) | 0.029 (3) | 0.018 (2) | 0.002 (2) | 0.005 (2) |
| O2 | 0.037 (2) | 0.044 (2) | 0.043 (2) | 0.0197 (17) | 0.0039 (17) | 0.0035 (18) |
| N2 | 0.030 (2) | 0.044 (3) | 0.035 (3) | 0.016 (2) | −0.0026 (19) | 0.006 (2) |
| C2 | 0.030 (3) | 0.029 (2) | 0.030 (3) | 0.011 (2) | 0.002 (2) | 0.003 (2) |
| C3 | 0.031 (3) | 0.041 (3) | 0.030 (3) | 0.021 (2) | −0.005 (2) | 0.005 (2) |
| C4 | 0.032 (3) | 0.033 (3) | 0.028 (3) | 0.016 (2) | −0.002 (2) | 0.005 (2) |
| C5 | 0.041 (3) | 0.047 (3) | 0.043 (3) | 0.030 (3) | −0.002 (3) | 0.005 (3) |
| C6 | 0.036 (3) | 0.036 (3) | 0.042 (3) | 0.012 (2) | −0.001 (2) | 0.002 (2) |
| C7 | 0.029 (3) | 0.031 (3) | 0.052 (4) | 0.011 (2) | −0.006 (2) | −0.003 (3) |
| C8 | 0.036 (3) | 0.051 (3) | 0.048 (4) | 0.029 (3) | −0.007 (3) | 0.001 (3) |
| C9 | 0.031 (3) | 0.041 (3) | 0.027 (3) | 0.013 (2) | 0.000 (2) | 0.005 (2) |
| C10 | 0.030 (3) | 0.054 (4) | 0.036 (3) | 0.012 (3) | 0.001 (2) | 0.008 (3) |
| C11 | 0.041 (3) | 0.037 (3) | 0.037 (3) | 0.015 (2) | −0.002 (2) | 0.004 (2) |
| C12 | 0.050 (3) | 0.038 (3) | 0.048 (4) | 0.023 (3) | −0.002 (3) | 0.000 (3) |
| C13 | 0.047 (3) | 0.031 (3) | 0.041 (3) | 0.021 (3) | −0.003 (3) | −0.003 (2) |
Geometric parameters (Å, °)
| Cu1—N1i | 1.962 (5) | C4—C7 | 1.386 (8) |
| Cu1—C2 | 2.000 (6) | C4—C5 | 1.402 (8) |
| Cu1—O2ii | 2.007 (4) | C5—C6 | 1.383 (8) |
| Cu1—C3 | 2.030 (5) | C5—H5 | 0.9500 |
| O1—C1 | 1.237 (7) | C6—C9 | 1.392 (8) |
| N1—C11 | 1.320 (8) | C6—H6 | 0.9500 |
| N1—C13 | 1.364 (7) | C7—C8 | 1.380 (7) |
| N1—Cu1iii | 1.962 (5) | C7—H7 | 0.9500 |
| C1—O2 | 1.281 (6) | C8—C9 | 1.386 (8) |
| C1—C2 | 1.496 (7) | C8—H8 | 0.9500 |
| O2—Cu1iv | 2.007 (4) | C9—C10 | 1.521 (8) |
| N2—C11 | 1.347 (7) | C10—H10A | 0.9900 |
| N2—C12 | 1.363 (8) | C10—H10B | 0.9900 |
| N2—C10 | 1.480 (8) | C11—H11 | 0.9500 |
| C2—C3 | 1.381 (7) | C12—C13 | 1.354 (9) |
| C2—H2 | 1.0000 | C12—H12 | 0.9500 |
| C3—C4 | 1.481 (7) | C13—H13 | 0.9500 |
| C3—H3 | 1.0000 | ||
| N1i—Cu1—C2 | 151.2 (2) | C6—C5—C4 | 120.5 (5) |
| N1i—Cu1—O2ii | 104.12 (19) | C6—C5—H5 | 119.7 |
| C2—Cu1—O2ii | 104.49 (19) | C4—C5—H5 | 119.7 |
| N1i—Cu1—C3 | 111.1 (2) | C5—C6—C9 | 120.3 (5) |
| C2—Cu1—C3 | 40.1 (2) | C5—C6—H6 | 119.8 |
| O2ii—Cu1—C3 | 144.1 (2) | C9—C6—H6 | 119.8 |
| C11—N1—C13 | 106.1 (5) | C8—C7—C4 | 121.3 (5) |
| C11—N1—Cu1iii | 122.7 (4) | C8—C7—H7 | 119.3 |
| C13—N1—Cu1iii | 130.5 (4) | C4—C7—H7 | 119.3 |
| O1—C1—O2 | 123.6 (5) | C7—C8—C9 | 120.2 (5) |
| O1—C1—C2 | 121.2 (5) | C7—C8—H8 | 119.9 |
| O2—C1—C2 | 115.2 (5) | C9—C8—H8 | 119.9 |
| C1—O2—Cu1iv | 104.3 (3) | C8—C9—C6 | 119.2 (5) |
| C11—N2—C12 | 106.8 (5) | C8—C9—C10 | 121.3 (5) |
| C11—N2—C10 | 126.7 (5) | C6—C9—C10 | 119.5 (5) |
| C12—N2—C10 | 126.1 (5) | N2—C10—C9 | 109.7 (5) |
| C3—C2—C1 | 121.5 (5) | N2—C10—H10A | 109.7 |
| C3—C2—Cu1 | 71.1 (3) | C9—C10—H10A | 109.7 |
| C1—C2—Cu1 | 104.2 (3) | N2—C10—H10B | 109.7 |
| C3—C2—H2 | 116.6 | C9—C10—H10B | 109.7 |
| C1—C2—H2 | 116.6 | H10A—C10—H10B | 108.2 |
| Cu1—C2—H2 | 116.6 | N1—C11—N2 | 111.0 (5) |
| C2—C3—C4 | 126.9 (5) | N1—C11—H11 | 124.5 |
| C2—C3—Cu1 | 68.8 (3) | N2—C11—H11 | 124.5 |
| C4—C3—Cu1 | 114.9 (4) | C13—C12—N2 | 106.9 (5) |
| C2—C3—H3 | 112.8 | C13—C12—H12 | 126.6 |
| C4—C3—H3 | 112.8 | N2—C12—H12 | 126.6 |
| Cu1—C3—H3 | 112.8 | C12—C13—N1 | 109.2 (5) |
| C7—C4—C5 | 118.2 (5) | C12—C13—H13 | 125.4 |
| C7—C4—C3 | 118.2 (5) | N1—C13—H13 | 125.4 |
| C5—C4—C3 | 123.5 (5) |
Symmetry codes: (i) −x+y, −x, z+2/3; (ii) −y+1, x−y, z+1/3; (iii) −y, x−y, z−2/3; (iv) −x+y+1, −x+1, z−1/3.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: NG5155).
References
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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 datablocks I, global. DOI: 10.1107/S1600536811015005/ng5155sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536811015005/ng5155Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report


