Abstract
In the title compound, [Cu(C2O4)(C13H20N4)(H2O)]·2H2O, the CuII atom exhibits a distorted square-pyramidal geometry with the two N atoms of the imidazole ligand and the two O atoms of the oxalate ligand forming the basal plane, while the O atom of the coordinated water molecule is in an apical position. The CuII atom is shifted 0.232 (2) Å out of the basal plane toward the water molecule. The asymmetric unit is completed by two solvent water molecules. These water molecules participate in the formation of an intricate three-dimensionnal network of hydrogen bonds involving the coordinated water molecule and the NH groups.
Related literature
For the chemical properties of imidazole derivatives, see: Bouwman et al. (2000 ▶). For synthesis, see: Delgado et al. (2008 ▶). For related structures, see: Beznischenko et al. (2007 ▶); Pajunen (1981 ▶).
Experimental
Crystal data
[Cu(C2O4)(C13H20N4)(H2O)]·2H2O
M r = 437.94
Monoclinic,
a = 12.1711 (13) Å
b = 23.167 (2) Å
c = 7.4400 (8) Å
β = 107.304 (1)°
V = 2002.9 (4) Å3
Z = 4
Mo Kα radiation
μ = 1.13 mm−1
T = 298 K
0.35 × 0.18 × 0.12 mm
Data collection
Rigaku Mercury CCD area-detector diffractometer
Absorption correction: multi-scan (CrystalClear; Rigaku, 2005 ▶) T min = 0.693, T max = 0.876
10119 measured reflections
3528 independent reflections
1958 reflections with I > 2σ(I)
R int = 0.071
Refinement
R[F 2 > 2σ(F 2)] = 0.045
wR(F 2) = 0.092
S = 0.81
3528 reflections
248 parameters
H-atom parameters constrained
Δρmax = 0.34 e Å−3
Δρmin = −0.31 e Å−3
Data collection: CrystalClear (Rigaku, 2005 ▶); 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: 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, global. DOI: 10.1107/S1600536811001012/dn2649sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536811001012/dn2649Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report
Table 1. Hydrogen-bond geometry (Å, °).
| D—H⋯A | D—H | H⋯A | D⋯A | D—H⋯A |
|---|---|---|---|---|
| O5—H51⋯O4i | 0.85 | 2.58 | 3.177 (4) | 128 |
| O5—H52⋯O4ii | 0.85 | 1.90 | 2.748 (4) | 174 |
| N2—H2⋯O2iii | 0.86 | 2.09 | 2.943 (4) | 171 |
| N4—H4⋯O7 | 0.86 | 2.03 | 2.847 (4) | 158 |
| O6—H6F⋯O5iv | 0.85 | 2.50 | 3.259 (4) | 149 |
| O6—H6G⋯O4v | 0.85 | 2.30 | 3.057 (5) | 148 |
| O7—H7C⋯O3vi | 0.85 | 2.03 | 2.882 (4) | 178 |
| O7—H7D⋯O6 | 0.85 | 1.97 | 2.818 (4) | 177 |
Symmetry codes: (i)
; (ii)
; (iii)
; (iv)
; (v)
; (vi)
.
supplementary crystallographic information
Comment
Imidazole derivatives are versatile ligands towards transition metal ions both in man-made and natural systems. They are not only used for catalytic and biocatalysts but also for dioxygen transport and electron storage (Bouwman et al., 2000). As part of our interest in imidazole derivatives, we report here the crystal structure of a new copper complex.
The structure around CuII is best decribed as distorted square pyramid environnement with the two N atoms of the imidazole ligand and the two O atoms of the oxalate forming the basal plane whereas the oxygen atom of the coordinated water molecule is in apical position. As expected, the copper atom is shifted ca 0.232 (2)Å out of the basal plane toward the water molecule. The asymmetric unit is completed by two solvate water molecules. The distances and angles within the square pyramid framework agree with related structures (Beznischenko et al., 2007); Pajunen, 1981).
These water molecules participate to the formation of an intricated hydrogen bonds resulting in three dimensionnal network involving the coordinated water molecule and the NH groups (Table 1, Fig. 2).
Experimental
Crystals of the title compound were synthesized by the reaction between copper(II) nitrate trihydrate, potassium oxalate and 4,4'-methanediylbis(2-ethyl-5-methyl-1H-imidazole) ligand. Copper salt and oxalate chemicals used (reagent grade) were commercially available, the 4,4'-methanediylbis(2-ethyl-5-methyl-1H-imidazole) ligand was synthesized as described below . 0.2 mmol(48.4 mg) solid copper(II) nitrate trihydrate was added to a 15 ml aqueous solution of 0.1 mmol(16.6 mg) potassium oxalate under continuous stirring. The suspension was heated at 40–50 °C during 1 h. Then this suspension was mixed with a 5 ml EtOH solution of 0.1 mmol(23.2mg)4,4'-methanediylbis(2-ethyl-5-methyl-1H-imidazole). Finally, the blue solution which results from the mixture was filtered off and allowed to evaporate at room temperature(Delgado, et al.,2008). Single crystals of the title compound as blue prisms were grown from the solution by slow evaporation at room temperature within a few days.
The ligand 4,4'-methanediylbis(2-ethyl-5-methyl-1H-imidazole) was synthesized as follows: 4.35 g (30 mmol) 2-ethyl-5-methylimidazole was added to a solution of 1.5 g (15 mmol)glycine (40% in H2O). This suspension was vigorously stirred, and 3.1 g (30 mmol) formaldehyde (37% in H2O) was added dropwise. The resulting turbid mixture was made alkaline with a concentrated sodium hydroxide solution until a pH of 12 was reached(Bouwman, et al.,2000). The reaction mixture was stirred for 8 days at room temperature in a closed vessel. During which time a white solid formed. The white solid was collected by filtration, washed with acetonitrile and diethyl ether, and air-dry at room temperature.
Refinement
All H atoms attached to C atoms and N atom were fixed geometrically and treated as riding with C—H = 0.96 Å (methyl) or 0.97 Å (methylene) and N—H = 0.86 Å with Uiso(H) = 1.2Ueq(C or N) or Uiso(H) = 1.5Ueq(methyl) . H atoms of water molecules were located in difference Fourier maps and included in the subsequent refinement using restraints (O-H= 0.85 (1)Å and H···H= 1.40 (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.
The asymmetric unit of (I) with the atom-labelling scheme. Displacement ellipsoids are drawn at the 30% probability level. H atoms are represented as small spheres of arbitrary radii. Hydrogen bonds are shown as dashed lines.
Fig. 2.
A packing view down the a axis showing the three dimensionnal network. Hydrogen bonds are shown as dashed lines. For the sake of clarity, H atoms not involved in hydrogen bonding have been omitted.
Crystal data
| [Cu(C2O4)(C13H20N4)(H2O)]·2H2O | F(000) = 916 |
| Mr = 437.94 | Dx = 1.452 Mg m−3 |
| Monoclinic, P21/c | Mo Kα radiation, λ = 0.71073 Å |
| Hall symbol: -P 2ybc | Cell parameters from 1383 reflections |
| a = 12.1711 (13) Å | θ = 3.0–26.0° |
| b = 23.167 (2) Å | µ = 1.13 mm−1 |
| c = 7.4400 (8) Å | T = 298 K |
| β = 107.304 (1)° | Prism, blue |
| V = 2002.9 (4) Å3 | 0.35 × 0.18 × 0.12 mm |
| Z = 4 |
Data collection
| Rigaku MODEL? CCD area-detector diffractometer | 3528 independent reflections |
| Radiation source: fine-focus sealed tube | 1958 reflections with I > 2σ(I) |
| graphite | Rint = 0.071 |
| Detector resolution: 8.192 pixels mm-1 | θmax = 25.0°, θmin = 2.5° |
| φ and ω scans | h = −14→14 |
| Absorption correction: multi-scan (CrystalClear; Rigaku, 2005) | k = −27→21 |
| Tmin = 0.693, Tmax = 0.876 | l = −8→8 |
| 10119 measured reflections |
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)] = 0.045 | Hydrogen site location: inferred from neighbouring sites |
| wR(F2) = 0.092 | H-atom parameters constrained |
| S = 0.81 | w = 1/[σ2(Fo2) + (0.0336P)2] where P = (Fo2 + 2Fc2)/3 |
| 3528 reflections | (Δ/σ)max = 0.003 |
| 248 parameters | Δρmax = 0.34 e Å−3 |
| 0 restraints | Δρmin = −0.31 e Å−3 |
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 | 0.76270 (4) | 0.413233 (19) | 0.51168 (7) | 0.03980 (17) | |
| O1 | 0.7228 (2) | 0.49415 (10) | 0.4554 (4) | 0.0521 (8) | |
| O2 | 0.7628 (2) | 0.56946 (12) | 0.2999 (4) | 0.0607 (9) | |
| O3 | 0.8807 (2) | 0.43059 (12) | 0.3849 (4) | 0.0489 (8) | |
| O4 | 0.9308 (3) | 0.50045 (13) | 0.2201 (5) | 0.0744 (11) | |
| O5 | 0.8745 (2) | 0.44573 (12) | 0.8111 (4) | 0.0598 (8) | |
| H51 | 0.8928 | 0.4356 | 0.9259 | 0.090* | |
| H52 | 0.9316 | 0.4637 | 0.7948 | 0.090* | |
| N1 | 0.6093 (2) | 0.39498 (13) | 0.5450 (4) | 0.0350 (8) | |
| N2 | 0.4439 (3) | 0.39461 (14) | 0.6014 (5) | 0.0454 (9) | |
| H2 | 0.3882 | 0.4056 | 0.6423 | 0.055* | |
| N3 | 0.8036 (3) | 0.33050 (12) | 0.5306 (5) | 0.0392 (8) | |
| N4 | 0.8869 (3) | 0.24674 (13) | 0.5968 (5) | 0.0435 (9) | |
| H4 | 0.9396 | 0.2212 | 0.6395 | 0.052* | |
| C1 | 0.5428 (3) | 0.42338 (16) | 0.6240 (5) | 0.0355 (10) | |
| C2 | 0.4464 (3) | 0.34484 (17) | 0.5008 (6) | 0.0455 (11) | |
| C3 | 0.5486 (3) | 0.34484 (16) | 0.4666 (6) | 0.0365 (10) | |
| C4 | 0.5695 (3) | 0.47801 (16) | 0.7361 (6) | 0.0441 (11) | |
| H4A | 0.6252 | 0.5000 | 0.6946 | 0.053* | |
| H4B | 0.4998 | 0.5009 | 0.7111 | 0.053* | |
| C5 | 0.6159 (4) | 0.46803 (18) | 0.9430 (7) | 0.0665 (14) | |
| H5A | 0.6874 | 0.4474 | 0.9698 | 0.100* | |
| H5B | 0.5617 | 0.4458 | 0.9850 | 0.100* | |
| H5C | 0.6284 | 0.5045 | 1.0073 | 0.100* | |
| C6 | 0.3461 (3) | 0.30308 (19) | 0.4455 (7) | 0.0729 (16) | |
| H6A | 0.3218 | 0.2942 | 0.5538 | 0.109* | |
| H6B | 0.3696 | 0.2683 | 0.3973 | 0.109* | |
| H6C | 0.2835 | 0.3203 | 0.3503 | 0.109* | |
| C7 | 0.9028 (3) | 0.30417 (17) | 0.6091 (6) | 0.0403 (10) | |
| C8 | 0.7732 (4) | 0.23503 (16) | 0.5055 (6) | 0.0417 (11) | |
| C9 | 0.7212 (3) | 0.28746 (16) | 0.4628 (6) | 0.0385 (10) | |
| C10 | 1.0158 (3) | 0.33196 (18) | 0.7043 (7) | 0.0669 (15) | |
| H10A | 1.0293 | 0.3614 | 0.6207 | 0.080* | |
| H10B | 1.0092 | 0.3514 | 0.8161 | 0.080* | |
| C11 | 1.1157 (4) | 0.2954 (2) | 0.7594 (10) | 0.116 (3) | |
| H11A | 1.1282 | 0.2785 | 0.6494 | 0.173* | |
| H11B | 1.1038 | 0.2654 | 0.8408 | 0.173* | |
| H11C | 1.1816 | 0.3180 | 0.8248 | 0.173* | |
| C12 | 0.7272 (3) | 0.17517 (16) | 0.4687 (6) | 0.0559 (13) | |
| H12A | 0.6454 | 0.1766 | 0.4111 | 0.084* | |
| H12B | 0.7438 | 0.1544 | 0.5854 | 0.084* | |
| H12C | 0.7626 | 0.1560 | 0.3860 | 0.084* | |
| C13 | 0.5996 (3) | 0.30202 (16) | 0.3626 (6) | 0.0450 (11) | |
| H13A | 0.5540 | 0.2669 | 0.3434 | 0.054* | |
| H13B | 0.5952 | 0.3176 | 0.2398 | 0.054* | |
| C14 | 0.7802 (3) | 0.51976 (19) | 0.3595 (6) | 0.0420 (11) | |
| C15 | 0.8731 (4) | 0.48180 (19) | 0.3153 (6) | 0.0465 (11) | |
| O6 | 1.1845 (3) | 0.07904 (14) | 0.6127 (5) | 0.0904 (11) | |
| H6F | 1.1814 | 0.0493 | 0.6779 | 0.136* | |
| H6G | 1.1552 | 0.0701 | 0.4975 | 0.136* | |
| O7 | 1.0089 (3) | 0.14122 (14) | 0.7024 (6) | 0.1067 (15) | |
| H7C | 0.9722 | 0.1194 | 0.7563 | 0.160* | |
| H7D | 1.0608 | 0.1214 | 0.6762 | 0.160* |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| Cu1 | 0.0386 (3) | 0.0339 (3) | 0.0511 (3) | 0.0007 (2) | 0.0197 (3) | 0.0014 (3) |
| O1 | 0.0566 (19) | 0.0352 (17) | 0.078 (2) | 0.0074 (13) | 0.0411 (18) | 0.0105 (15) |
| O2 | 0.066 (2) | 0.041 (2) | 0.084 (3) | 0.0000 (15) | 0.0355 (19) | 0.0150 (17) |
| O3 | 0.0421 (17) | 0.046 (2) | 0.066 (2) | 0.0043 (13) | 0.0285 (16) | 0.0026 (15) |
| O4 | 0.079 (2) | 0.064 (2) | 0.105 (3) | −0.0064 (17) | 0.067 (2) | 0.012 (2) |
| O5 | 0.0454 (18) | 0.084 (2) | 0.051 (2) | −0.0148 (15) | 0.0156 (16) | −0.0019 (16) |
| N1 | 0.0313 (18) | 0.037 (2) | 0.039 (2) | 0.0026 (14) | 0.0142 (17) | 0.0010 (15) |
| N2 | 0.033 (2) | 0.047 (2) | 0.060 (3) | 0.0009 (16) | 0.0204 (18) | 0.0009 (18) |
| N3 | 0.036 (2) | 0.033 (2) | 0.050 (2) | 0.0015 (16) | 0.0155 (18) | 0.0029 (16) |
| N4 | 0.044 (2) | 0.035 (2) | 0.055 (3) | 0.0080 (16) | 0.0182 (19) | 0.0012 (17) |
| C1 | 0.035 (2) | 0.033 (3) | 0.038 (3) | 0.0006 (19) | 0.009 (2) | 0.0045 (19) |
| C2 | 0.039 (3) | 0.041 (3) | 0.055 (3) | −0.002 (2) | 0.012 (2) | −0.006 (2) |
| C3 | 0.029 (2) | 0.040 (3) | 0.037 (3) | −0.0010 (18) | 0.006 (2) | −0.0020 (19) |
| C4 | 0.045 (3) | 0.035 (3) | 0.057 (3) | 0.0029 (19) | 0.022 (2) | 0.000 (2) |
| C5 | 0.070 (3) | 0.065 (3) | 0.061 (4) | 0.013 (3) | 0.014 (3) | −0.006 (3) |
| C6 | 0.046 (3) | 0.068 (4) | 0.109 (5) | −0.016 (2) | 0.032 (3) | −0.021 (3) |
| C7 | 0.040 (3) | 0.031 (3) | 0.052 (3) | 0.003 (2) | 0.017 (2) | 0.000 (2) |
| C8 | 0.057 (3) | 0.034 (2) | 0.043 (3) | −0.002 (2) | 0.028 (2) | −0.007 (2) |
| C9 | 0.040 (3) | 0.040 (3) | 0.038 (3) | −0.002 (2) | 0.015 (2) | −0.008 (2) |
| C10 | 0.042 (3) | 0.052 (3) | 0.100 (5) | 0.003 (2) | 0.011 (3) | −0.001 (3) |
| C11 | 0.051 (4) | 0.068 (4) | 0.205 (8) | 0.010 (3) | 0.004 (4) | 0.008 (4) |
| C12 | 0.065 (3) | 0.038 (3) | 0.073 (4) | −0.005 (2) | 0.034 (3) | −0.011 (2) |
| C13 | 0.044 (3) | 0.042 (3) | 0.050 (3) | −0.003 (2) | 0.016 (2) | −0.010 (2) |
| C14 | 0.040 (3) | 0.042 (3) | 0.042 (3) | −0.007 (2) | 0.011 (2) | 0.003 (2) |
| C15 | 0.043 (3) | 0.046 (3) | 0.053 (3) | −0.009 (2) | 0.017 (2) | −0.001 (2) |
| O6 | 0.086 (3) | 0.076 (3) | 0.114 (3) | 0.0166 (19) | 0.038 (2) | −0.001 (2) |
| O7 | 0.119 (3) | 0.070 (2) | 0.167 (4) | 0.045 (2) | 0.098 (3) | 0.062 (2) |
Geometric parameters (Å, °)
| Cu1—O1 | 1.951 (2) | C4—H4B | 0.9700 |
| Cu1—N3 | 1.975 (3) | C5—H5A | 0.9600 |
| Cu1—O3 | 1.980 (3) | C5—H5B | 0.9600 |
| Cu1—N1 | 2.000 (3) | C5—H5C | 0.9600 |
| Cu1—O5 | 2.362 (3) | C6—H6A | 0.9600 |
| O1—C14 | 1.283 (4) | C6—H6B | 0.9600 |
| O2—C14 | 1.230 (4) | C6—H6C | 0.9600 |
| O3—C15 | 1.287 (4) | C7—C10 | 1.493 (5) |
| O4—C15 | 1.216 (4) | C8—C9 | 1.363 (5) |
| O5—H51 | 0.8489 | C8—C12 | 1.490 (5) |
| O5—H52 | 0.8497 | C9—C13 | 1.485 (5) |
| N1—C1 | 1.311 (4) | C10—C11 | 1.437 (5) |
| N1—C3 | 1.407 (4) | C10—H10A | 0.9700 |
| N2—C1 | 1.342 (4) | C10—H10B | 0.9700 |
| N2—C2 | 1.380 (5) | C11—H11A | 0.9600 |
| N2—H2 | 0.8599 | C11—H11B | 0.9600 |
| N3—C7 | 1.323 (4) | C11—H11C | 0.9600 |
| N3—C9 | 1.398 (4) | C12—H12A | 0.9600 |
| N4—C7 | 1.344 (4) | C12—H12B | 0.9600 |
| N4—C8 | 1.375 (5) | C12—H12C | 0.9600 |
| N4—H4 | 0.8603 | C13—H13A | 0.9700 |
| C1—C4 | 1.497 (5) | C13—H13B | 0.9700 |
| C2—C3 | 1.341 (5) | C14—C15 | 1.543 (5) |
| C2—C6 | 1.515 (5) | O6—H6F | 0.8505 |
| C3—C13 | 1.501 (5) | O6—H6G | 0.8503 |
| C4—C5 | 1.491 (6) | O7—H7C | 0.8504 |
| C4—H4A | 0.9700 | O7—H7D | 0.8495 |
| O1—Cu1—N3 | 171.72 (13) | C2—C6—H6A | 109.5 |
| O1—Cu1—O3 | 82.66 (11) | C2—C6—H6B | 109.5 |
| N3—Cu1—O3 | 91.60 (12) | H6A—C6—H6B | 109.5 |
| O1—Cu1—N1 | 92.73 (11) | C2—C6—H6C | 109.5 |
| N3—Cu1—N1 | 90.62 (12) | H6A—C6—H6C | 109.5 |
| O3—Cu1—N1 | 159.73 (12) | H6B—C6—H6C | 109.5 |
| O1—Cu1—O5 | 86.16 (11) | N3—C7—N4 | 109.4 (3) |
| N3—Cu1—O5 | 100.35 (12) | N3—C7—C10 | 127.0 (4) |
| O3—Cu1—O5 | 95.07 (11) | N4—C7—C10 | 123.6 (4) |
| N1—Cu1—O5 | 104.34 (11) | C9—C8—N4 | 105.6 (3) |
| C14—O1—Cu1 | 114.9 (3) | C9—C8—C12 | 131.6 (4) |
| C15—O3—Cu1 | 113.8 (2) | N4—C8—C12 | 122.9 (4) |
| Cu1—O5—H51 | 140.0 | C8—C9—N3 | 108.5 (3) |
| Cu1—O5—H52 | 106.7 | C8—C9—C13 | 130.1 (4) |
| H51—O5—H52 | 107.4 | N3—C9—C13 | 121.4 (3) |
| C1—N1—C3 | 106.3 (3) | C11—C10—C7 | 117.6 (4) |
| C1—N1—Cu1 | 132.3 (3) | C11—C10—H10A | 107.9 |
| C3—N1—Cu1 | 121.2 (2) | C7—C10—H10A | 107.9 |
| C1—N2—C2 | 108.6 (3) | C11—C10—H10B | 107.9 |
| C1—N2—H2 | 125.5 | C7—C10—H10B | 107.9 |
| C2—N2—H2 | 125.8 | H10A—C10—H10B | 107.2 |
| C7—N3—C9 | 107.0 (3) | C10—C11—H11A | 109.5 |
| C7—N3—Cu1 | 131.0 (3) | C10—C11—H11B | 109.5 |
| C9—N3—Cu1 | 121.9 (3) | H11A—C11—H11B | 109.5 |
| C7—N4—C8 | 109.4 (3) | C10—C11—H11C | 109.5 |
| C7—N4—H4 | 125.3 | H11A—C11—H11C | 109.5 |
| C8—N4—H4 | 125.2 | H11B—C11—H11C | 109.5 |
| N1—C1—N2 | 110.2 (3) | C8—C12—H12A | 109.5 |
| N1—C1—C4 | 127.8 (3) | C8—C12—H12B | 109.5 |
| N2—C1—C4 | 121.9 (3) | H12A—C12—H12B | 109.5 |
| C3—C2—N2 | 105.9 (3) | C8—C12—H12C | 109.5 |
| C3—C2—C6 | 131.7 (4) | H12A—C12—H12C | 109.5 |
| N2—C2—C6 | 122.3 (3) | H12B—C12—H12C | 109.5 |
| C2—C3—N1 | 108.9 (3) | C9—C13—C3 | 113.3 (3) |
| C2—C3—C13 | 130.3 (4) | C9—C13—H13A | 108.9 |
| N1—C3—C13 | 120.8 (3) | C3—C13—H13A | 108.9 |
| C5—C4—C1 | 113.4 (3) | C9—C13—H13B | 108.9 |
| C5—C4—H4A | 108.9 | C3—C13—H13B | 108.9 |
| C1—C4—H4A | 108.9 | H13A—C13—H13B | 107.7 |
| C5—C4—H4B | 108.9 | O2—C14—O1 | 124.7 (4) |
| C1—C4—H4B | 108.9 | O2—C14—C15 | 121.0 (4) |
| H4A—C4—H4B | 107.7 | O1—C14—C15 | 114.2 (4) |
| C4—C5—H5A | 109.5 | O4—C15—O3 | 125.3 (4) |
| C4—C5—H5B | 109.5 | O4—C15—C14 | 120.6 (4) |
| H5A—C5—H5B | 109.5 | O3—C15—C14 | 114.2 (4) |
| C4—C5—H5C | 109.5 | H6F—O6—H6G | 107.5 |
| H5A—C5—H5C | 109.5 | H7C—O7—H7D | 108.5 |
| H5B—C5—H5C | 109.5 |
Hydrogen-bond geometry (Å, °)
| D—H···A | D—H | H···A | D···A | D—H···A |
| O5—H51···O4i | 0.85 | 2.58 | 3.177 (4) | 128 |
| O5—H52···O4ii | 0.85 | 1.90 | 2.748 (4) | 174 |
| N2—H2···O2iii | 0.86 | 2.09 | 2.943 (4) | 171 |
| N4—H4···O7 | 0.86 | 2.03 | 2.847 (4) | 158 |
| O6—H6F···O5iv | 0.85 | 2.50 | 3.259 (4) | 149 |
| O6—H6G···O4v | 0.85 | 2.30 | 3.057 (5) | 148 |
| O7—H7C···O3vi | 0.85 | 2.03 | 2.882 (4) | 178 |
| O7—H7D···O6 | 0.85 | 1.97 | 2.818 (4) | 177 |
Symmetry codes: (i) x, y, z+1; (ii) −x+2, −y+1, −z+1; (iii) −x+1, −y+1, −z+1; (iv) −x+2, y−1/2, −z+3/2; (v) −x+2, y−1/2, −z+1/2; (vi) x, −y+1/2, z+1/2.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: DN2649).
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/S1600536811001012/dn2649sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536811001012/dn2649Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report


