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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2008 Nov 22;64(Pt 12):m1590. doi: 10.1107/S1600536808037999

Poly[[(μ3-5,6-dicarboxy­bicyclo­[2.2.2]oct-7-ene-2,3-dicarboxyl­ato)(1,10-phenanthroline)copper(II)] monohydrate]

Yun-Yu Liu a,*, Yu-Jiang Zhuo a, Xing-Qi Li a, Ji-Cheng Ma a
PMCID: PMC2960067  PMID: 21581190

Abstract

In the title compound, {[Cu(C12H10O8)(C12H8N2)]·H2O}n, the CuII ion is five-coordinated by two N atoms from one phenanthroline ligand and three O atoms from three different H2 L 2− anions (H4 L is bicyclo­[2.2.2]oct-7-ene-2,3,5,6-tetra­carboxylic acid) in a distorted square-pyramidal geometry. Each H2 L 2− ion bridges three CuII atoms to form a zigzag sheet parallel to the ab plane. The crystal structure is consolidated by O—H⋯O hydrogen bonds.

Related literature

For general background, see: Yang et al. (2008).graphic file with name e-64-m1590-scheme1.jpg

Experimental

Crystal data

  • [Cu(C12H10O8)(C12H8N2)]·H2O

  • M r = 543.96

  • Monoclinic, Inline graphic

  • a = 6.5900 (4) Å

  • b = 15.1650 (8) Å

  • c = 10.7490 (6) Å

  • β = 95.244 (9)°

  • V = 1069.73 (10) Å3

  • Z = 2

  • Mo Kα radiation

  • μ = 1.08 mm−1

  • T = 293 (2) K

  • 0.33 × 0.21 × 0.20 mm

Data collection

  • Bruker APEX CCD area-detector diffractometer

  • Absorption correction: multi-scan (SADABS; Sheldrick, 1996) T min = 0.696, T max = 0.803

  • 6580 measured reflections

  • 4555 independent reflections

  • 4343 reflections with I > 2σ(I)

  • R int = 0.022

Refinement

  • R[F 2 > 2σ(F 2)] = 0.026

  • wR(F 2) = 0.065

  • S = 1.04

  • 4555 reflections

  • 333 parameters

  • 2 restraints

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

  • Δρmax = 0.31 e Å−3

  • Δρmin = −0.37 e Å−3

  • Absolute structure: Flack (1983), 1914 Friedel pairs

  • Flack parameter: 0.008 (8)

Data collection: SMART (Bruker, 1998); cell refinement: SAINT (Bruker, 1998); data reduction: SAINT (Bruker, 1998); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: SHELXTL-Plus (Sheldrick, 2008); software used to prepare material for publication: SHELXTL-Plus (Sheldrick, 2008).

Supplementary Material

Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536808037999/ci2718sup1.cif

e-64-m1590-sup1.cif (25.7KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536808037999/ci2718Isup2.hkl

e-64-m1590-Isup2.hkl (218.6KB, hkl)

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

Table 1. Selected bond lengths (Å).

N1—Cu1 2.0072 (17)
N2—Cu1 2.0119 (19)
O2—Cu1 1.9640 (15)
Cu1—O3i 1.9355 (15)
Cu1—O7ii 2.3398 (18)

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

Table 2. Hydrogen-bond geometry (Å, °).

D—H⋯A D—H H⋯A DA D—H⋯A
O5—H5⋯O1W 0.82 1.84 2.567 (2) 148
O8—H8⋯O2iii 0.82 1.79 2.594 (2) 166
O1W—HW11⋯O4iv 0.82 (3) 1.97 (3) 2.777 (3) 167 (3)
O1W—HW12⋯O1v 0.82 (2) 2.05 (3) 2.763 (3) 145 (4)

Symmetry codes: (iii) Inline graphic; (iv) Inline graphic; (v) Inline graphic.

Acknowledgments

The authors thank the Science Foundation for Young Teachers of Northeast Normal University (grant Nos. 20080305 and 20080304) for financial support.

supplementary crystallographic information

Comment

Coordination polymers based on poly(carboxylic acids) have been investigated in the area of solid state and material science (Yang et al., 2008). We selected bicyclo[2.2.2]oct-7-ene-2,3,5,6-tetracarboxylic acid (H4L) as a poly(carboxylic acid) ligand and phenanthroline (phen) as a secondary ligand, generating a new coordination polymer, [Cu(phen)(H2L)].H2O, which is reported here.

In the title compound, each CuII atom is five-coordinated by two N atoms from one phen ligand, and three O atoms from three different H2L2- anions in a distorted square-pyramidal geometry (Fig. 1 and Table 1). Each H2L2- bridges three CuII atoms to form a two-dimensional layer structure (Fig. 2). The O–H···O hydrogen bonds (Table 2) further consolidate the crystal structure.

Experimental

A mixture of H4L (0.5 mmol), phen (0.5 mmol), NaOH (1 mmol) and CuCl2.2H2O (0.5 mmol) was suspended in deionized water (12 ml) and sealed in a 20-ml Teflon-lined autoclave. The mixture was heated at 373 K for 7 d and then the autoclave was slowly cooled to room temperature. The grown single crystals were collected, washed with deionized water and dried.

Refinement

H atoms on C atoms were generated geometrically and refined as riding atoms with C—H = 0.93–0.98 Å and Uiso(H) = 1.2Ueq(C). The H atoms of the water molecules were located in a difference Fourier map and refined with an O—H distance restraint of 0.85 (1) Å and with Uiso(H) = 1.2Ueq(O).

Figures

Fig. 1.

Fig. 1.

Part of the polymeric structure of the title compound, showing the atomic numbering scheme. Displacement ellipsoids are drawn at the 30% probability level. Symmetry codes: (i) x - 1, y, z; (ii) 2 - x, y - 1/2, 2 - z.

Fig. 2.

Fig. 2.

View of a zigzag sheet structure in the title compound.

Crystal data

[Cu(C12H10O8)(C12H8N2)]·H2O F000 = 558
Mr = 543.96 Dx = 1.689 Mg m3
Monoclinic, P21 Mo Kα radiation λ = 0.71069 Å
Hall symbol: P 2yb Cell parameters from 4555 reflections
a = 6.5900 (4) Å θ = 1.1–28.4º
b = 15.1650 (8) Å µ = 1.08 mm1
c = 10.7490 (6) Å T = 293 K
β = 95.244 (9)º Block, blue
V = 1069.73 (10) Å3 0.33 × 0.21 × 0.20 mm
Z = 2

Data collection

Bruker APEX CCD area-detector diffractometer 4555 independent reflections
Radiation source: fine-focus sealed tube 4343 reflections with I > 2σ(I)
Monochromator: graphite Rint = 0.022
T = 293 K θmax = 28.4º
φ and ω scans θmin = 2.3º
Absorption correction: multi-scan(SADABS; Sheldrick, 1996) h = −8→8
Tmin = 0.696, Tmax = 0.803 k = −19→17
6580 measured reflections l = −6→14

Refinement

Refinement on F2 Hydrogen site location: inferred from neighbouring sites
Least-squares matrix: full H atoms treated by a mixture of independent and constrained refinement
R[F2 > 2σ(F2)] = 0.026   w = 1/[σ2(Fo2) + (0.0256P)2] where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.065 (Δ/σ)max = 0.001
S = 1.04 Δρmax = 0.31 e Å3
4555 reflections Δρmin = −0.37 e Å3
333 parameters Extinction correction: none
2 restraints Absolute structure: Flack (1983), 1914 Friedel pairs
Primary atom site location: structure-invariant direct methods Flack parameter: 0.008 (8)
Secondary atom site location: difference Fourier map

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
C1 0.8692 (4) 0.81993 (17) 0.5050 (2) 0.0327 (5)
H1 0.9536 0.8445 0.5700 0.039*
C2 0.9222 (4) 0.82867 (19) 0.3826 (2) 0.0382 (6)
H2 1.0408 0.8583 0.3669 0.046*
C3 0.7992 (4) 0.79351 (17) 0.2862 (2) 0.0362 (6)
H3 0.8341 0.7990 0.2047 0.043*
C4 0.6199 (3) 0.74901 (17) 0.31010 (18) 0.0285 (5)
C5 0.4749 (4) 0.71054 (18) 0.2161 (2) 0.0352 (6)
H5A 0.4972 0.7156 0.1322 0.042*
C6 0.3084 (4) 0.66765 (18) 0.2479 (2) 0.0361 (6)
H6 0.2186 0.6434 0.1853 0.043*
C7 0.2660 (4) 0.65841 (16) 0.3763 (2) 0.0291 (5)
C8 0.1009 (4) 0.61105 (18) 0.4178 (2) 0.0364 (6)
H8B 0.0083 0.5828 0.3606 0.044*
C9 0.0779 (4) 0.60707 (19) 0.5428 (2) 0.0377 (6)
H9 −0.0301 0.5758 0.5711 0.045*
C10 0.2174 (4) 0.65023 (17) 0.6279 (2) 0.0329 (5)
H10 0.1995 0.6473 0.7127 0.039*
C11 0.4003 (3) 0.69806 (15) 0.46831 (19) 0.0240 (4)
C12 0.5789 (3) 0.74318 (14) 0.43543 (18) 0.0237 (5)
C13 1.0048 (3) 0.90548 (13) 0.94151 (18) 0.0192 (4)
H13 0.9289 0.8814 1.0080 0.023*
C14 1.0387 (3) 1.00356 (15) 0.97408 (18) 0.0223 (4)
H14 0.9159 1.0382 0.9497 0.027*
C15 1.0971 (3) 1.00950 (14) 1.11723 (18) 0.0220 (4)
H15 0.9782 0.9919 1.1598 0.026*
C16 1.2682 (3) 0.94109 (14) 1.14952 (18) 0.0211 (4)
H16 1.1993 0.8873 1.1736 0.025*
C17 1.3679 (3) 0.91758 (15) 1.02845 (19) 0.0229 (4)
H17 1.4990 0.8879 1.0479 0.027*
C18 1.2122 (3) 0.85576 (14) 0.95247 (18) 0.0203 (4)
H18 1.1978 0.8014 1.0002 0.024*
C19 1.3913 (3) 0.99816 (16) 0.94838 (19) 0.0288 (5)
H19 1.5166 1.0168 0.9246 0.035*
C20 1.2195 (4) 1.03987 (15) 0.91496 (19) 0.0268 (5)
H20 1.2108 1.0873 0.8600 0.032*
C21 0.8703 (3) 0.88961 (15) 0.82048 (19) 0.0208 (4)
C22 1.2984 (3) 0.83259 (15) 0.82983 (19) 0.0237 (4)
C23 1.4200 (4) 0.96369 (15) 1.2593 (2) 0.0265 (5)
C24 1.1515 (3) 1.10347 (15) 1.1550 (2) 0.0240 (5)
N1 0.7020 (3) 0.77771 (12) 0.53121 (15) 0.0253 (4)
N2 0.3738 (3) 0.69509 (13) 0.59172 (16) 0.0251 (4)
O1 0.7941 (3) 0.95074 (11) 0.75885 (15) 0.0331 (4)
O2 0.8349 (2) 0.80701 (10) 0.79532 (13) 0.0256 (3)
O1W 1.4570 (4) 0.98510 (18) 1.59374 (17) 0.0537 (6)
O3 1.4401 (2) 0.77476 (12) 0.84210 (14) 0.0323 (4)
O4 1.2381 (2) 0.86940 (12) 0.73066 (14) 0.0323 (4)
O5 1.3290 (3) 0.95633 (14) 1.36461 (15) 0.0406 (4)
H5 1.4105 0.9685 1.4244 0.061*
O6 1.5975 (3) 0.97879 (13) 1.25429 (17) 0.0402 (4)
O7 1.2819 (3) 1.12253 (12) 1.23587 (16) 0.0358 (4)
O8 1.0345 (3) 1.16299 (13) 1.09436 (17) 0.0443 (5)
H8 1.0703 1.2125 1.1181 0.066*
Cu1 0.59195 (3) 0.760541 (17) 0.697564 (19) 0.02264 (7)
HW11 1.378 (5) 0.952 (2) 1.625 (3) 0.050 (10)*
HW12 1.575 (4) 0.969 (3) 1.613 (4) 0.078 (14)*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
C1 0.0300 (12) 0.0339 (14) 0.0336 (12) −0.0050 (11) 0.0001 (10) 0.0004 (10)
C2 0.0364 (14) 0.0379 (15) 0.0413 (13) −0.0056 (12) 0.0101 (11) 0.0070 (11)
C3 0.0433 (15) 0.0387 (14) 0.0276 (11) 0.0050 (11) 0.0095 (10) 0.0068 (9)
C4 0.0351 (11) 0.0263 (13) 0.0238 (9) 0.0057 (11) 0.0014 (8) 0.0009 (9)
C5 0.0486 (16) 0.0344 (15) 0.0218 (10) 0.0106 (11) −0.0018 (10) −0.0044 (9)
C6 0.0425 (15) 0.0343 (14) 0.0292 (11) 0.0029 (12) −0.0098 (10) −0.0086 (10)
C7 0.0311 (12) 0.0253 (12) 0.0300 (11) 0.0023 (10) −0.0023 (9) −0.0075 (9)
C8 0.0286 (12) 0.0344 (14) 0.0446 (14) −0.0020 (11) −0.0059 (10) −0.0113 (10)
C9 0.0314 (13) 0.0350 (15) 0.0465 (14) −0.0084 (11) 0.0030 (11) −0.0058 (11)
C10 0.0318 (13) 0.0335 (14) 0.0339 (12) −0.0055 (11) 0.0066 (10) −0.0044 (10)
C11 0.0260 (11) 0.0210 (11) 0.0244 (10) 0.0044 (9) −0.0014 (8) −0.0037 (8)
C12 0.0270 (10) 0.0196 (13) 0.0240 (9) 0.0042 (8) −0.0003 (8) −0.0017 (7)
C13 0.0199 (10) 0.0184 (11) 0.0194 (9) −0.0018 (8) 0.0014 (8) −0.0009 (7)
C14 0.0236 (11) 0.0192 (10) 0.0229 (10) 0.0006 (9) −0.0049 (8) −0.0024 (8)
C15 0.0198 (10) 0.0224 (11) 0.0236 (10) −0.0003 (8) −0.0002 (8) −0.0015 (8)
C16 0.0233 (10) 0.0187 (10) 0.0208 (9) −0.0020 (8) −0.0007 (8) −0.0015 (7)
C17 0.0175 (10) 0.0259 (12) 0.0247 (10) 0.0002 (9) −0.0007 (8) −0.0037 (8)
C18 0.0199 (10) 0.0215 (11) 0.0190 (9) 0.0006 (8) −0.0004 (7) −0.0012 (7)
C19 0.0284 (12) 0.0312 (13) 0.0276 (11) −0.0119 (10) 0.0062 (9) −0.0042 (9)
C20 0.0357 (12) 0.0215 (11) 0.0223 (10) −0.0076 (10) −0.0026 (9) 0.0017 (8)
C21 0.0182 (10) 0.0220 (12) 0.0216 (10) −0.0008 (9) −0.0006 (8) −0.0013 (8)
C22 0.0212 (10) 0.0254 (12) 0.0248 (10) −0.0034 (8) 0.0036 (8) −0.0029 (8)
C23 0.0330 (13) 0.0197 (11) 0.0256 (10) 0.0030 (9) −0.0043 (9) 0.0010 (8)
C24 0.0238 (11) 0.0221 (12) 0.0262 (11) 0.0028 (9) 0.0031 (9) −0.0032 (8)
N1 0.0252 (9) 0.0254 (12) 0.0251 (8) −0.0010 (8) 0.0008 (7) −0.0022 (7)
N2 0.0242 (9) 0.0245 (10) 0.0264 (9) 0.0010 (8) 0.0006 (7) −0.0030 (7)
O1 0.0381 (10) 0.0263 (9) 0.0323 (9) 0.0023 (8) −0.0117 (7) 0.0020 (7)
O2 0.0265 (8) 0.0205 (8) 0.0283 (7) −0.0040 (7) −0.0051 (6) −0.0019 (6)
O1W 0.0514 (14) 0.0778 (17) 0.0291 (9) −0.0253 (13) −0.0121 (9) 0.0156 (10)
O3 0.0290 (8) 0.0397 (12) 0.0282 (7) 0.0106 (8) 0.0033 (6) −0.0084 (7)
O4 0.0349 (9) 0.0392 (10) 0.0225 (7) 0.0009 (8) 0.0016 (6) 0.0024 (7)
O5 0.0447 (10) 0.0543 (13) 0.0211 (7) −0.0153 (9) −0.0054 (7) −0.0004 (7)
O6 0.0254 (9) 0.0509 (13) 0.0424 (10) 0.0001 (8) −0.0069 (7) −0.0105 (8)
O7 0.0387 (10) 0.0224 (9) 0.0427 (10) 0.0004 (7) −0.0164 (8) −0.0049 (7)
O8 0.0502 (11) 0.0249 (10) 0.0528 (11) 0.0103 (9) −0.0222 (9) −0.0094 (8)
Cu1 0.02218 (12) 0.02490 (13) 0.02043 (10) −0.00053 (12) −0.00032 (8) −0.00387 (11)

Geometric parameters (Å, °)

C1—N1 1.326 (3) C15—C16 1.548 (3)
C1—C2 1.398 (3) C15—H15 0.98
C1—H1 0.93 C16—C23 1.515 (3)
C2—C3 1.364 (4) C16—C17 1.552 (3)
C2—H2 0.93 C16—H16 0.98
C3—C4 1.405 (4) C17—C19 1.511 (3)
C3—H3 0.93 C17—C18 1.564 (3)
C4—C12 1.401 (3) C17—H17 0.98
C4—C5 1.448 (3) C18—C22 1.523 (3)
C5—C6 1.346 (4) C18—H18 0.98
C5—H5A 0.93 C19—C20 1.318 (3)
C6—C7 1.440 (3) C19—H19 0.93
C6—H6 0.93 C20—H20 0.93
C7—C11 1.401 (3) C21—O1 1.220 (3)
C7—C8 1.410 (3) C21—O2 1.298 (3)
C8—C9 1.367 (3) C22—O4 1.236 (3)
C8—H8B 0.93 C22—O3 1.279 (3)
C9—C10 1.399 (3) C23—O6 1.198 (3)
C9—H9 0.93 C23—O5 1.334 (3)
C10—N2 1.323 (3) C24—O7 1.200 (3)
C10—H10 0.93 C24—O8 1.320 (3)
C11—N2 1.354 (3) N1—Cu1 2.0072 (17)
C11—C12 1.434 (3) N2—Cu1 2.0119 (19)
C12—N1 1.356 (3) O2—Cu1 1.9640 (15)
C13—C21 1.525 (3) O1W—HW11 0.82 (3)
C13—C14 1.540 (3) O1W—HW12 0.822 (19)
C13—C18 1.556 (3) O3—Cu1i 1.9355 (15)
C13—H13 0.98 O5—H5 0.82
C14—C20 1.505 (3) O7—Cu1ii 2.3398 (18)
C14—C15 1.554 (3) O8—H8 0.82
C14—H14 0.98 Cu1—O3iii 1.9355 (15)
C15—C24 1.516 (3) Cu1—O7iv 2.3398 (18)
N1—C1—C2 122.0 (2) C15—C16—C17 108.75 (16)
N1—C1—H1 119.0 C23—C16—H16 105.8
C2—C1—H1 119.0 C15—C16—H16 105.8
C3—C2—C1 119.7 (2) C17—C16—H16 105.8
C3—C2—H2 120.2 C19—C17—C16 111.41 (18)
C1—C2—H2 120.2 C19—C17—C18 106.48 (17)
C2—C3—C4 120.0 (2) C16—C17—C18 105.53 (16)
C2—C3—H3 120.0 C19—C17—H17 111.1
C4—C3—H3 120.0 C16—C17—H17 111.1
C12—C4—C3 116.4 (2) C18—C17—H17 111.1
C12—C4—C5 118.2 (2) C22—C18—C13 116.14 (16)
C3—C4—C5 125.3 (2) C22—C18—C17 108.15 (17)
C6—C5—C4 121.3 (2) C13—C18—C17 106.20 (16)
C6—C5—H5A 119.4 C22—C18—H18 108.7
C4—C5—H5A 119.4 C13—C18—H18 108.7
C5—C6—C7 121.6 (2) C17—C18—H18 108.7
C5—C6—H6 119.2 C20—C19—C17 114.4 (2)
C7—C6—H6 119.2 C20—C19—H19 122.8
C11—C7—C8 116.8 (2) C17—C19—H19 122.8
C11—C7—C6 118.0 (2) C19—C20—C14 113.8 (2)
C8—C7—C6 125.2 (2) C19—C20—H20 123.1
C9—C8—C7 119.4 (2) C14—C20—H20 123.1
C9—C8—H8B 120.3 O1—C21—O2 124.26 (19)
C7—C8—H8B 120.3 O1—C21—C13 121.4 (2)
C8—C9—C10 119.8 (2) O2—C21—C13 114.15 (18)
C8—C9—H9 120.1 O4—C22—O3 124.92 (19)
C10—C9—H9 120.1 O4—C22—C18 121.8 (2)
N2—C10—C9 122.1 (2) O3—C22—C18 113.28 (18)
N2—C10—H10 119.0 O6—C23—O5 124.8 (2)
C9—C10—H10 119.0 O6—C23—C16 125.9 (2)
N2—C11—C7 123.2 (2) O5—C23—C16 109.01 (19)
N2—C11—C12 116.08 (19) O7—C24—O8 122.7 (2)
C7—C11—C12 120.70 (19) O7—C24—C15 123.8 (2)
N1—C12—C4 123.4 (2) O8—C24—C15 113.40 (19)
N1—C12—C11 116.42 (17) C1—N1—C12 118.41 (18)
C4—C12—C11 120.14 (19) C1—N1—Cu1 128.81 (15)
C21—C13—C14 114.04 (17) C12—N1—Cu1 112.72 (14)
C21—C13—C18 115.24 (16) C10—N2—C11 118.6 (2)
C14—C13—C18 110.05 (17) C10—N2—Cu1 128.54 (16)
C21—C13—H13 105.5 C11—N2—Cu1 112.83 (15)
C14—C13—H13 105.5 C21—O2—Cu1 125.43 (14)
C18—C13—H13 105.5 HW11—O1W—HW12 109 (4)
C20—C14—C13 111.19 (17) C22—O3—Cu1i 114.82 (14)
C20—C14—C15 105.24 (17) C23—O5—H5 109.5
C13—C14—C15 107.38 (17) C24—O7—Cu1ii 130.37 (16)
C20—C14—H14 110.9 C24—O8—H8 109.5
C13—C14—H14 110.9 O3iii—Cu1—O2 89.24 (7)
C15—C14—H14 110.9 O3iii—Cu1—N1 162.98 (7)
C24—C15—C16 114.85 (17) O2—Cu1—N1 94.97 (7)
C24—C15—C14 110.54 (18) O3iii—Cu1—N2 96.53 (7)
C16—C15—C14 107.01 (16) O2—Cu1—N2 170.11 (7)
C24—C15—H15 108.1 N1—Cu1—N2 81.84 (7)
C16—C15—H15 108.1 O3iii—Cu1—O7iv 92.84 (7)
C14—C15—H15 108.1 O2—Cu1—O7iv 84.71 (6)
C23—C16—C15 116.02 (18) N1—Cu1—O7iv 103.96 (7)
C23—C16—C17 113.89 (18) N2—Cu1—O7iv 86.97 (7)
N1—C1—C2—C3 0.4 (4) C15—C14—C20—C19 57.3 (2)
C1—C2—C3—C4 0.2 (4) C14—C13—C21—O1 −1.8 (3)
C2—C3—C4—C12 −0.3 (4) C18—C13—C21—O1 −130.5 (2)
C2—C3—C4—C5 178.6 (2) C14—C13—C21—O2 −177.45 (17)
C12—C4—C5—C6 −2.2 (4) C18—C13—C21—O2 53.9 (2)
C3—C4—C5—C6 178.8 (3) C13—C18—C22—O4 17.8 (3)
C4—C5—C6—C7 0.4 (4) C17—C18—C22—O4 −101.4 (2)
C5—C6—C7—C11 2.0 (4) C13—C18—C22—O3 −164.32 (18)
C5—C6—C7—C8 −176.8 (3) C17—C18—C22—O3 76.5 (2)
C11—C7—C8—C9 0.9 (4) C15—C16—C23—O6 −114.2 (3)
C6—C7—C8—C9 179.8 (2) C17—C16—C23—O6 13.2 (3)
C7—C8—C9—C10 0.3 (4) C15—C16—C23—O5 71.4 (2)
C8—C9—C10—N2 −0.4 (4) C17—C16—C23—O5 −161.24 (19)
C8—C7—C11—N2 −2.3 (3) C16—C15—C24—O7 −23.1 (3)
C6—C7—C11—N2 178.8 (2) C14—C15—C24—O7 −144.3 (2)
C8—C7—C11—C12 176.3 (2) C16—C15—C24—O8 160.03 (19)
C6—C7—C11—C12 −2.6 (3) C14—C15—C24—O8 38.8 (2)
C3—C4—C12—N1 −0.1 (3) C2—C1—N1—C12 −0.8 (4)
C5—C4—C12—N1 −179.1 (2) C2—C1—N1—Cu1 −177.84 (18)
C3—C4—C12—C11 −179.3 (2) C4—C12—N1—C1 0.6 (3)
C5—C4—C12—C11 1.6 (3) C11—C12—N1—C1 179.9 (2)
N2—C11—C12—N1 0.2 (3) C4—C12—N1—Cu1 178.13 (18)
C7—C11—C12—N1 −178.5 (2) C11—C12—N1—Cu1 −2.6 (2)
N2—C11—C12—C4 179.5 (2) C9—C10—N2—C11 −0.9 (4)
C7—C11—C12—C4 0.8 (3) C9—C10—N2—Cu1 −179.39 (19)
C21—C13—C14—C20 −88.1 (2) C7—C11—N2—C10 2.3 (3)
C18—C13—C14—C20 43.2 (2) C12—C11—N2—C10 −176.4 (2)
C21—C13—C14—C15 157.29 (17) C7—C11—N2—Cu1 −179.00 (18)
C18—C13—C14—C15 −71.42 (19) C12—C11—N2—Cu1 2.3 (2)
C20—C14—C15—C24 56.4 (2) O1—C21—O2—Cu1 −23.2 (3)
C13—C14—C15—C24 174.93 (17) C13—C21—O2—Cu1 152.23 (14)
C20—C14—C15—C16 −69.3 (2) O4—C22—O3—Cu1i 9.8 (3)
C13—C14—C15—C16 49.2 (2) C18—C22—O3—Cu1i −167.97 (14)
C24—C15—C16—C23 26.6 (3) O8—C24—O7—Cu1ii −7.8 (4)
C14—C15—C16—C23 149.70 (18) C15—C24—O7—Cu1ii 175.59 (14)
C24—C15—C16—C17 −103.3 (2) C21—O2—Cu1—O3iii −77.88 (17)
C14—C15—C16—C17 19.8 (2) C21—O2—Cu1—N1 85.60 (17)
C23—C16—C17—C19 −91.2 (2) C21—O2—Cu1—O7iv −170.81 (17)
C15—C16—C17—C19 39.8 (2) C1—N1—Cu1—O3iii 94.5 (3)
C23—C16—C17—C18 153.60 (18) C12—N1—Cu1—O3iii −82.7 (3)
C15—C16—C17—C18 −75.3 (2) C1—N1—Cu1—O2 −9.3 (2)
C21—C13—C18—C22 26.2 (3) C12—N1—Cu1—O2 173.52 (15)
C14—C13—C18—C22 −104.5 (2) C1—N1—Cu1—N2 −179.9 (2)
C21—C13—C18—C17 146.43 (17) C12—N1—Cu1—N2 2.94 (15)
C14—C13—C18—C17 15.8 (2) C1—N1—Cu1—O7iv −95.1 (2)
C19—C17—C18—C22 59.7 (2) C12—N1—Cu1—O7iv 87.74 (15)
C16—C17—C18—C22 178.16 (17) C10—N2—Cu1—O3iii −21.4 (2)
C19—C17—C18—C13 −65.7 (2) C11—N2—Cu1—O3iii 160.06 (15)
C16—C17—C18—C13 52.9 (2) C10—N2—Cu1—N1 175.7 (2)
C16—C17—C19—C20 −57.8 (2) C11—N2—Cu1—N1 −2.86 (15)
C18—C17—C19—C20 56.8 (2) C10—N2—Cu1—O7iv 71.1 (2)
C17—C19—C20—C14 5.7 (3) C11—N2—Cu1—O7iv −107.43 (15)
C13—C14—C20—C19 −58.6 (2)

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

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
O5—H5···O1W 0.82 1.84 2.567 (2) 148
O8—H8···O2ii 0.82 1.79 2.594 (2) 166
O1W—HW11···O4v 0.82 (3) 1.97 (3) 2.777 (3) 167 (3)
O1W—HW12···O1vi 0.82 (2) 2.05 (3) 2.763 (3) 145 (4)

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

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: CI2718).

References

  1. Bruker (1998). SMART and SAINT Bruker AXS Inc., Madison, Wisconsin, USA.
  2. Flack, H. D. (1983). Acta Cryst. A39, 876–881.
  3. Sheldrick, G. M. (1996). SADABS University of Göttingen, Germany.
  4. Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
  5. Yang, J., Ma, J.-F., Batten, S. R. & Su, Z.-M. (2008). Chem. Commun. pp. 2233–2235. [DOI] [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 global, I. DOI: 10.1107/S1600536808037999/ci2718sup1.cif

e-64-m1590-sup1.cif (25.7KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536808037999/ci2718Isup2.hkl

e-64-m1590-Isup2.hkl (218.6KB, hkl)

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


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