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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2011 Mar 9;67(Pt 4):m411. doi: 10.1107/S1600536811007938

Di-μ-glutarato-κ4 O 1:O 5-bis­[aqua­(1,10-phenanthroline-κ2 N,N′)copper(II)]

Yong-Hong Zhou a,*
PMCID: PMC3099891  PMID: 21753943

Abstract

In the centrosymmetric dinuclear title complex, [Cu2(C5H6O4)2(C12H18N2)2(H2O)2], the CuII atom displays a dis­torted square-pyramidal coordination environment with the basal plane occupied by two phenanthroline N atoms and two O atoms from different glutarate dianions while a water mol­ecule is located at the apical position. Of the two water H atoms, one is engaged in an intra­molecular hydrogen bond with a free oxygen of the dianion whereas the second is engaged in an inter­molecular hydrogen bond, building a corrugated layer parallel to (100). These layers are further connected through π–π stacking inter­actions involving symmetry-related phenanthroline rings [centroid–centroid distance = 3.5599 (17) and 3.5617 (18) Å], building a three dimensionnal network. C—H⋯π inter­actions involving the phenanthroline ring system are also observed.

Related literature

For coordination modes of the glutarate anion, see: Ghosh et al. (2007); Kim et al. (2005); Rather & Zaworotko (2003); Zheng et al. (2004); Vaidhyanathan et al. (2004); Girginova et al. (2007). graphic file with name e-67-0m411-scheme1.jpg

Experimental

Crystal data

  • [Cu2(C5H6O4)2(C12H18N2)2(H2O)2]

  • M r = 783.72

  • Monoclinic, Inline graphic

  • a = 10.2767 (11) Å

  • b = 10.5935 (14) Å

  • c = 15.5998 (16) Å

  • β = 107.114 (1)°

  • V = 1623.1 (3) Å3

  • Z = 2

  • Mo Kα radiation

  • μ = 1.38 mm−1

  • T = 298 K

  • 0.26 × 0.25 × 0.23 mm

Data collection

  • Bruker SMART CCD area-detector diffractometer

  • Absorption correction: multi-scan (SADABS; Bruker, 1997) T min = 0.716, T max = 0.742

  • 7937 measured reflections

  • 2867 independent reflections

  • 2275 reflections with I > 2σ(I)

  • R int = 0.028

Refinement

  • R[F 2 > 2σ(F 2)] = 0.031

  • wR(F 2) = 0.083

  • S = 1.07

  • 2867 reflections

  • 226 parameters

  • H-atom parameters constrained

  • Δρmax = 0.31 e Å−3

  • Δρmin = −0.28 e Å−3

Data collection: SMART (Bruker, 1997); cell refinement: SAINT (Bruker, 1997); data reduction: SAINT; program(s) used to solve structure: SHELXTL (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: ORTEPIII (Burnett & Johnson, 1996), ORTEP-3 for Windows (Farrugia, 1997) and PLATON (Spek, 2009); software used to prepare material for publication: SHELXL97.

Supplementary Material

Crystal structure: contains datablocks I, New_Global_Publ_Block. DOI: 10.1107/S1600536811007938/dn2661sup1.cif

e-67-0m411-sup1.cif (24.2KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536811007938/dn2661Isup2.hkl

e-67-0m411-Isup2.hkl (137.9KB, hkl)

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

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

Cg1 is the centroid of the N1,C6–C10 ring

D—H⋯A D—H H⋯A DA D—H⋯A
O5—H51⋯O4 0.89 1.81 2.659 (3) 158
O5—H52⋯O2i 0.88 1.89 2.762 (3) 169
C2—H2ACg1i 0.97 2.88 3.754 (3) 151

Symmetry code: (i) Inline graphic.

Acknowledgments

The project was supported by the Natural Science Foundation of Anhui Provincial Education Commission (No. KJw2008B65ZC) and the Open Foundation of Anhui Key Laboratory of Energetic Materials (No. KLEM2009004).

supplementary crystallographic information

Comment

For many yeras, there is a growing interest in developing organic-inorganic hybrid materials owing to their intriguing structures, new topologies, and potential applications(Ghosh et al., 2007; Kim et al.,2005). Carboxylic acids have been proved to be versatile functional moieties in generating interesting hybrid materials by interacting with metal ions. The abilities of its anion to metal ions in diverse and unique linking modes can be regarded as a major factor in making the carboxylate function a versatile structure directing moiety.

Metal glutarates are one class of dicarboxylate system which exhibit interesting structural features. Previous investigations have demonstrated that glutaric acid presents interesting behaviors due to its conformational flexibility and coordination diversity (Rather et al., 2003; Zheng et al., 2004; Vaidhyanathan et al., 2004; Girginova et al., 2007). We report here the crystal structure of the title compound.

The title complex, [Cu(C12H18N2)(C5H6O4)(H2O)]2, is a dinuclear compound organized around inversion center. The CuII displays a distorted square pyramidal coordination environment (Fig. 1). The basal plane is occupied by two nitrogen atoms of the phenanthroline [Cu—N(1) = 2.014 (2)Å and Cu—N(2) = 2.022 (2) Å] and two O atoms from different glutarate dianions[Cu—O(1) = 1.954 (2)Å and Cu—O(3) = 1.947 (2) Å], whereas one water molecule is located at the apical position at a significantly longer distance[Cu—O(5) = 2.380 (2) Å]. The glutarate dianions act as a bidentate ligand bridging the two CuII ions which are separated by 8.476 Å.

There is an intramolecular hydrogen bond involving one H of the water and the O4 oxygen of one dianion within the dinuclear complex. The second H atom of the water is engaged in hydrogen bond interaction with the O2 oxygen atom of symmetry related dinuclear complex building then a corrugated layer parallel to the (1 0 0) plane (Fig. 2, Table 1). The layers are interconnected through π-π stacking involving the symmetry related N1,C6,C7,C8,C9,C10 (A) and N2,C11,C12,C13,C14,C15 (B) phenanthroline rings (Fig. 2, Table 2) building a three dimensional network. The packing is further stabilized by weak C—H···π interaction involving the symmetry related ring A (Table 1).

Experimental

The title complex was prepared by the addition of the stoichiometric amount of CuCl2 (0.134 g, 1 mmol) to an ethanol solution of glutaric acid (0.264 g, 2 mmol) and 1,10-phenanthroline monohydrate(0.396 g, 2 mmol), the pH was adjusted to ~6 with 0.2 mol.L-1 KOH solution. The resulting solution was stirred for 30 min at room temperature and then filtered. Blue single crystals were isolated from the solution at room temperature over two weeks.

Refinement

All H atoms attached to C atoms were fixed geometrically and treated as riding with C—H = 0.93 Å (aromatic) or 0.97 Å (methylene) with Uiso(H) = 1.2Ueq(C). H atoms of water molecule were located in difference Fourier maps and included in the subsequent refinement using restraints (O—H= 0.88 (1)Å and H···H= 1.50 (2) Å) with Uiso(H) = 1.5Ueq(O). In the last cycles of refinement, they were treated as riding on their parent O atoms.

Figures

Fig. 1.

Fig. 1.

The molecular structure of the title compound with the atom labeling scheme. Displacement thermal paremeters are represented at the 30% probability level. Hydrogen bonds are shown as dashed lines. H atoms not involved in hydrogen bondings have been omitted for the sake of clarity. [Symmetry code: (i) -x + 1, -y + 1, -z + 1]

Fig. 2.

Fig. 2.

Partial packing view showing the formation of layer through O—H···O hydrogen bonds which are shown as dashed lines. H atoms not involved in hydrogen bondings have been omitted for the sake of clarity.

Crystal data

[Cu2(C5H6O4)2(C12H18N2)2(H2O)2] F(000) = 804
Mr = 783.72 Dx = 1.604 Mg m3
Monoclinic, P21/c Mo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ybc Cell parameters from 3334 reflections
a = 10.2767 (11) Å θ = 2.4–27.3°
b = 10.5935 (14) Å µ = 1.38 mm1
c = 15.5998 (16) Å T = 298 K
β = 107.114 (1)° Block, blue
V = 1623.1 (3) Å3 0.26 × 0.25 × 0.23 mm
Z = 2

Data collection

Bruker SMART CCD area-detector diffractometer 2867 independent reflections
Radiation source: fine-focus sealed tube 2275 reflections with I > 2σ(I)
graphite Rint = 0.028
φ and ω scans θmax = 25.0°, θmin = 2.4°
Absorption correction: multi-scan (SADABS; Bruker, 1997) h = −11→12
Tmin = 0.716, Tmax = 0.742 k = −12→10
7937 measured reflections l = −18→16

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)] = 0.031 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.083 H-atom parameters constrained
S = 1.07 w = 1/[σ2(Fo2) + (0.0346P)2 + 1.103P] where P = (Fo2 + 2Fc2)/3
2867 reflections (Δ/σ)max < 0.001
226 parameters Δρmax = 0.31 e Å3
0 restraints Δρmin = −0.28 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 0.34382 (3) 0.54797 (3) 0.21857 (2) 0.03292 (13)
N1 0.2087 (2) 0.4429 (2) 0.12652 (14) 0.0299 (5)
N2 0.3977 (2) 0.6012 (2) 0.10928 (14) 0.0318 (5)
O1 0.5068 (2) 0.61750 (19) 0.30440 (12) 0.0416 (5)
O2 0.5850 (2) 0.43066 (19) 0.28151 (13) 0.0432 (5)
O3 0.2798 (2) 0.4813 (2) 0.31524 (13) 0.0467 (5)
O4 0.1462 (3) 0.6404 (2) 0.32731 (17) 0.0689 (7)
O5 0.2215 (2) 0.74242 (19) 0.19357 (13) 0.0441 (5)
H51 0.1900 0.7287 0.2401 0.066*
H52 0.2746 0.8093 0.2014 0.066*
C1 0.5979 (3) 0.5330 (3) 0.32214 (17) 0.0318 (6)
C2 0.7228 (3) 0.5601 (3) 0.39982 (18) 0.0397 (7)
H2A 0.7284 0.6499 0.4125 0.048*
H2B 0.8038 0.5354 0.3841 0.048*
C3 0.7158 (3) 0.4873 (3) 0.48313 (18) 0.0380 (7)
H3A 0.6265 0.4993 0.4910 0.046*
H3B 0.7266 0.3980 0.4735 0.046*
C4 0.1767 (3) 0.4723 (3) 0.43155 (18) 0.0401 (7)
H4A 0.1805 0.3816 0.4242 0.048*
H4B 0.0869 0.4938 0.4356 0.048*
C5 0.2012 (3) 0.5385 (3) 0.35137 (18) 0.0387 (7)
C6 0.1142 (3) 0.3640 (3) 0.13755 (19) 0.0370 (7)
H6 0.1091 0.3496 0.1953 0.044*
C7 0.0230 (3) 0.3025 (3) 0.0664 (2) 0.0417 (7)
H7 −0.0423 0.2487 0.0768 0.050*
C8 0.0291 (3) 0.3208 (3) −0.0187 (2) 0.0401 (7)
H8 −0.0321 0.2800 −0.0667 0.048*
C9 0.1287 (3) 0.4017 (3) −0.03337 (18) 0.0339 (6)
C10 0.2164 (3) 0.4611 (2) 0.04186 (17) 0.0292 (6)
C11 0.3172 (3) 0.5485 (2) 0.03226 (17) 0.0294 (6)
C12 0.3286 (3) 0.5760 (3) −0.05311 (18) 0.0368 (7)
C13 0.4278 (3) 0.6647 (3) −0.0576 (2) 0.0445 (8)
H13 0.4398 0.6864 −0.1126 0.053*
C14 0.5061 (3) 0.7183 (3) 0.0194 (2) 0.0472 (8)
H14 0.5717 0.7776 0.0171 0.057*
C15 0.4890 (3) 0.6853 (3) 0.1024 (2) 0.0397 (7)
H15 0.5435 0.7237 0.1542 0.048*
C16 0.1444 (3) 0.4307 (3) −0.11997 (19) 0.0429 (8)
H16 0.0881 0.3915 −0.1707 0.051*
C17 0.2384 (3) 0.5131 (3) −0.12896 (19) 0.0453 (8)
H17 0.2455 0.5299 −0.1859 0.054*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
Cu1 0.0360 (2) 0.0377 (2) 0.02556 (18) 0.00182 (16) 0.00982 (14) −0.00183 (15)
N1 0.0338 (12) 0.0290 (12) 0.0281 (11) 0.0019 (10) 0.0112 (10) 0.0016 (9)
N2 0.0340 (13) 0.0280 (12) 0.0336 (12) 0.0029 (10) 0.0105 (10) 0.0010 (10)
O1 0.0444 (12) 0.0396 (12) 0.0349 (11) 0.0059 (10) 0.0024 (9) −0.0066 (9)
O2 0.0467 (13) 0.0412 (12) 0.0381 (11) 0.0073 (10) 0.0072 (9) −0.0055 (9)
O3 0.0591 (14) 0.0546 (14) 0.0325 (11) 0.0083 (11) 0.0230 (10) 0.0053 (10)
O4 0.095 (2) 0.0595 (16) 0.0710 (16) 0.0257 (15) 0.0535 (15) 0.0232 (14)
O5 0.0495 (12) 0.0443 (12) 0.0379 (11) −0.0074 (10) 0.0120 (9) −0.0047 (9)
C1 0.0351 (15) 0.0379 (17) 0.0232 (13) −0.0013 (13) 0.0097 (11) 0.0041 (12)
C2 0.0365 (16) 0.0490 (18) 0.0310 (14) −0.0073 (14) 0.0057 (12) 0.0045 (13)
C3 0.0428 (17) 0.0383 (17) 0.0316 (15) −0.0051 (13) 0.0090 (13) 0.0043 (13)
C4 0.0410 (17) 0.0481 (19) 0.0319 (15) −0.0069 (14) 0.0117 (13) −0.0004 (13)
C5 0.0417 (17) 0.0492 (19) 0.0253 (14) −0.0065 (15) 0.0100 (12) −0.0020 (14)
C6 0.0390 (16) 0.0338 (16) 0.0417 (16) 0.0031 (13) 0.0174 (13) 0.0044 (13)
C7 0.0359 (16) 0.0317 (16) 0.0580 (19) −0.0016 (13) 0.0147 (14) −0.0013 (14)
C8 0.0325 (16) 0.0339 (16) 0.0475 (18) 0.0027 (13) 0.0019 (13) −0.0101 (14)
C9 0.0342 (15) 0.0326 (15) 0.0313 (14) 0.0095 (12) 0.0041 (12) −0.0017 (12)
C10 0.0319 (14) 0.0280 (14) 0.0274 (13) 0.0071 (12) 0.0084 (11) 0.0002 (11)
C11 0.0320 (14) 0.0287 (14) 0.0287 (14) 0.0089 (12) 0.0105 (11) 0.0026 (11)
C12 0.0443 (17) 0.0357 (16) 0.0342 (15) 0.0159 (13) 0.0177 (13) 0.0100 (12)
C13 0.0488 (19) 0.0447 (19) 0.0476 (18) 0.0138 (15) 0.0260 (15) 0.0163 (15)
C14 0.0453 (18) 0.0354 (17) 0.070 (2) 0.0027 (14) 0.0307 (17) 0.0137 (16)
C15 0.0370 (16) 0.0318 (16) 0.0503 (18) 0.0004 (13) 0.0131 (14) −0.0021 (14)
C16 0.0475 (18) 0.0480 (19) 0.0289 (15) 0.0103 (15) 0.0046 (13) −0.0058 (13)
C17 0.058 (2) 0.055 (2) 0.0246 (15) 0.0181 (17) 0.0136 (14) 0.0054 (14)

Geometric parameters (Å, °)

Cu1—O3 1.947 (2) C4—C3i 1.520 (4)
Cu1—O1 1.9545 (19) C4—H4A 0.9700
Cu1—N1 2.014 (2) C4—H4B 0.9700
Cu1—N2 2.022 (2) C6—C7 1.387 (4)
Cu1—O5 2.385 (2) C6—H6 0.9300
N1—C6 1.329 (3) C7—C8 1.362 (4)
N1—C10 1.360 (3) C7—H7 0.9300
N2—C15 1.320 (4) C8—C9 1.404 (4)
N2—C11 1.362 (3) C8—H8 0.9300
O1—C1 1.266 (3) C9—C10 1.401 (4)
O2—C1 1.243 (3) C9—C16 1.440 (4)
O3—C5 1.267 (3) C10—C11 1.429 (4)
O4—C5 1.225 (4) C11—C12 1.402 (4)
O5—H51 0.8897 C12—C13 1.403 (4)
O5—H52 0.8804 C12—C17 1.435 (4)
C1—C2 1.511 (4) C13—C14 1.359 (4)
C2—C3 1.531 (4) C13—H13 0.9300
C2—H2A 0.9700 C14—C15 1.401 (4)
C2—H2B 0.9700 C14—H14 0.9300
C3—C4i 1.520 (4) C15—H15 0.9300
C3—H3A 0.9700 C16—C17 1.340 (5)
C3—H3B 0.9700 C16—H16 0.9300
C4—C5 1.518 (4) C17—H17 0.9300
O3—Cu1—O1 91.32 (9) H4A—C4—H4B 108.2
O3—Cu1—N1 91.85 (9) O4—C5—O3 125.6 (3)
O1—Cu1—N1 165.65 (9) O4—C5—C4 119.0 (3)
O3—Cu1—N2 173.39 (9) O3—C5—C4 115.3 (3)
O1—Cu1—N2 94.62 (9) N1—C6—C7 122.6 (3)
N1—Cu1—N2 81.69 (9) N1—C6—H6 118.7
O3—Cu1—O5 99.10 (8) C7—C6—H6 118.7
O1—Cu1—O5 95.20 (7) C8—C7—C6 120.0 (3)
N1—Cu1—O5 98.12 (8) C8—C7—H7 120.0
N2—Cu1—O5 83.28 (8) C6—C7—H7 120.0
C6—N1—C10 117.9 (2) C7—C8—C9 119.4 (3)
C6—N1—Cu1 129.16 (18) C7—C8—H8 120.3
C10—N1—Cu1 112.87 (17) C9—C8—H8 120.3
C15—N2—C11 117.8 (2) C10—C9—C8 117.3 (3)
C15—N2—Cu1 129.3 (2) C10—C9—C16 117.9 (3)
C11—N2—Cu1 112.56 (17) C8—C9—C16 124.8 (3)
C1—O1—Cu1 108.23 (17) N1—C10—C9 122.8 (2)
C5—O3—Cu1 125.2 (2) N1—C10—C11 116.4 (2)
Cu1—O5—H51 91.5 C9—C10—C11 120.7 (2)
Cu1—O5—H52 113.4 N2—C11—C12 123.6 (3)
H51—O5—H52 112.2 N2—C11—C10 116.3 (2)
O2—C1—O1 123.0 (2) C12—C11—C10 120.0 (2)
O2—C1—C2 120.8 (3) C11—C12—C13 116.9 (3)
O1—C1—C2 116.1 (3) C11—C12—C17 118.2 (3)
C1—C2—C3 110.1 (2) C13—C12—C17 124.9 (3)
C1—C2—H2A 109.6 C14—C13—C12 119.0 (3)
C3—C2—H2A 109.6 C14—C13—H13 120.5
C1—C2—H2B 109.6 C12—C13—H13 120.5
C3—C2—H2B 109.6 C13—C14—C15 120.7 (3)
H2A—C2—H2B 108.1 C13—C14—H14 119.6
C4i—C3—C2 113.5 (2) C15—C14—H14 119.6
C4i—C3—H3A 108.9 N2—C15—C14 121.9 (3)
C2—C3—H3A 108.9 N2—C15—H15 119.1
C4i—C3—H3B 108.9 C14—C15—H15 119.1
C2—C3—H3B 108.9 C17—C16—C9 121.4 (3)
H3A—C3—H3B 107.7 C17—C16—H16 119.3
C5—C4—C3i 109.7 (2) C9—C16—H16 119.3
C5—C4—H4A 109.7 C16—C17—C12 121.8 (3)
C3i—C4—H4A 109.7 C16—C17—H17 119.1
C5—C4—H4B 109.7 C12—C17—H17 119.1
C3i—C4—H4B 109.7

Symmetry codes: (i) −x+1, −y+1, −z+1.

Hydrogen-bond geometry (Å, °)

Cg1 is the centroid of the N1,C6–C10 ring
D—H···A D—H H···A D···A D—H···A
O5—H51···O4 0.89 1.81 2.659 (3) 158
O5—H52···O2ii 0.88 1.89 2.762 (3) 169
C2—H2A···Cg1ii 0.97 2.88 3.754 (3) 151

Symmetry codes: (ii) −x+1, y+1/2, −z+1/2.

Table 2 Table 2 π-π stacking interactions (Å)

Cg1 is the centroid of the N1,C6–C10 ring. Cg2 is the centroid of the N2,C11–C15 ring

CgI CgJ centroid-to-centroid interplanar vector Slippage
Cg1 Cg1ii 3.5599 (17) 3.342 1.226
Cg2 Cg2iii 3.5617 (18) 3.374 1.142

Symmetry codes: (ii)-x,1-y,1-z; (iii) 1-x, 1-y, -zSlippage = vertical displacement between ring centroids.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: DN2661).

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, New_Global_Publ_Block. DOI: 10.1107/S1600536811007938/dn2661sup1.cif

e-67-0m411-sup1.cif (24.2KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536811007938/dn2661Isup2.hkl

e-67-0m411-Isup2.hkl (137.9KB, hkl)

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


Articles from Acta Crystallographica Section E: Structure Reports Online are provided here courtesy of International Union of Crystallography

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