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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2011 Nov 23;67(Pt 12):m1796–m1797. doi: 10.1107/S1600536811047398

Aqua­(1,10-phenanthroline-κ2 N,N′)(valinato-κ2 N,O)copper(II) nitrate dihydrate

Araceli Tovar-Tovar a, Juan-Carlos García-Ramos a, Marcos Flores-Alamo a,*, Lena Ruiz-Azuara a
PMCID: PMC3238705  PMID: 22199582

Abstract

In the title compound, [Cu(C5H10NO2)(C12H8N2)(H2O)]NO3·2H2O, the CuII atom displays a distorted square-pyramidal coordination (τ = 0.03) where the water mol­ecule occupies the apical position and the base is defined by the N atom, one of the O atoms from the valinate ligand, and both phenanthroline N atoms. The phenanthroline chelate ring plane is slightly distorted from planarity (r.m.s. deviation = 0.0057 Å), whereas the five-membered ring formed by the valinate ligand presents an envelope conformation with the N atom being the flap atom. The crystal packing is stabilized by O—H⋯O and N—H⋯O hydrogen-bonding inter­actions, creating a three-dimensional network superstructure.

Related literature

For investigations related to anti­cancer compounds, see: Ruiz-Azuara (1996, 1997). For a description of the geometry of complexes with five-coordinate CuII atoms, see: Rao et al. (1981); Addison et al. (1984); Le et al. (2006); Dalhus & Görbitz (1999).graphic file with name e-67-m1796-scheme1.jpg

Experimental

Crystal data

  • [Cu(C5H10NO2)(C12H8N2)(H2O)]NO3·2H2O

  • M r = 475.94

  • Triclinic, Inline graphic

  • a = 7.9020 (19) Å

  • b = 9.610 (3) Å

  • c = 14.327 (4) Å

  • α = 81.89 (3)°

  • β = 75.04 (2)°

  • γ = 87.92 (2)°

  • V = 1040.6 (5) Å3

  • Z = 2

  • Mo Kα radiation

  • μ = 1.10 mm−1

  • T = 298 K

  • 0.45 × 0.27 × 0.21 mm

Data collection

  • Siemens P4 diffractometer

  • Absorption correction: ψ scan (XSCANS; Siemens, 1993) T min = 0.729, T max = 0.794

  • 5563 measured reflections

  • 4551 independent reflections

  • 3807 reflections with I > 2σ(I)

  • R int = 0.024

  • 3 standard reflections every 97 reflections intensity decay: 4.9%

Refinement

  • R[F 2 > 2σ(F 2)] = 0.037

  • wR(F 2) = 0.094

  • S = 1.06

  • 4551 reflections

  • 297 parameters

  • 18 restraints

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

  • Δρmax = 0.45 e Å−3

  • Δρmin = −0.33 e Å−3

Data collection: XSCANS (Siemens, 1993); cell refinement: XSCANS; data reduction: XSCANS; program(s) used to solve structure: SIR2004 (Burla et al., 2005); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: ORTEP-3 for Windows (Farrugia, 1997); software used to prepare material for publication: WinGX (Farrugia, 1999).

Supplementary Material

Crystal structure: contains datablock(s) global, I. DOI: 10.1107/S1600536811047398/jj2109sup1.cif

e-67-m1796-sup1.cif (22.8KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811047398/jj2109Isup2.hkl

e-67-m1796-Isup2.hkl (218.4KB, hkl)

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

Table 1. Selected bond lengths (Å).

Cu1—N1 2.0320 (19)
Cu1—N2 1.9975 (19)
Cu1—N3 1.992 (2)
Cu1—O2 1.9349 (16)
Cu1—O3W 2.263 (2)

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

D—H⋯A D—H H⋯A DA D—H⋯A
O3W—H3A⋯O1W 0.83 (2) 2.02 (2) 2.778 (3) 153 (3)
N3—H01⋯O1W 0.87 (3) 2.15 (3) 2.967 (4) 156 (2)
O3W—H3B⋯O2W 0.84 (2) 1.92 (2) 2.753 (3) 171 (3)
O1W—H1A⋯O4i 0.80 (2) 2.02 (2) 2.810 (4) 170 (3)
O1W—H1B⋯O4ii 0.82 (2) 2.19 (2) 2.881 (4) 143 (2)
O1W—H1B⋯O5ii 0.82 (2) 2.48 (2) 3.245 (5) 156 (3)
O2W—H2A⋯O1iii 0.80 (2) 2.05 (2) 2.836 (3) 167 (3)
O2W—H2B⋯O1iv 0.84 (2) 2.02 (2) 2.851 (3) 174 (3)
N3—H02⋯O3v 0.82 (3) 2.46 (3) 3.229 (4) 158 (2)
N3—H02⋯O5v 0.82 (3) 2.58 (3) 3.168 (4) 130 (2)

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

Acknowledgments

We thank CONACYT 87806, PAPIIT IN 227110 and PICSA10–61 for their financial support of this work. MFA is indebted to Dr A. L. Maldonado-Hermenegildo for useful comments.

supplementary crystallographic information

Comment

Investigations related to anticancer compounds (Ruiz-Azuara, 1996; 1997) that involve essential metals has been of considerable interest during the last three decades. In this context, we have prepared and crystallized the complex [Cu(H2O)(val)(phen)]NO3. 2H2O (val is valinate and phen is 1,10-phenantroline), (I).

The asymmetric unit consists of one [Cu(H2O)(val)(phen)] cationic complex, one nitrate anion and two water molecules. The metallic centre display a distorted square-pyramidal coordination (τ =0.03) where the water molecule occupies the apical position. The base is defined by the N and one of the O atoms from the valinate ligand, and both phenanthroline N atoms. The phenanthroline chelate-ring plane is slightly distorted from planarity (r.m.s. = 0.0057), whereas the five-membered ring formed by the valine ligand (defined by atoms N3, C14, C13, O2 and Cu), presents an envelope conformation on N3 (q2 = 0.2121 and φ = 141.74 °) (Rao et al., 1981). The CuII ion coordinates two nitrogen atoms of phen and the amino nitrogen and one carboxylate oxygen atoms of L-Val [Cu1–N1 = 2.0320 (19), Cu1–N2 = 1.9975 (19), Cu1–N3 = 1.992 (2), and Cu1–O2 = 1.9349 (16) Å], while one water oxygen atom is axial [Cu1–O3w = 2.263 (2) Å]. The resulting coordination geometries are in a distorted square-pyramidal orientation (figure 1), where N1,N2, N3, O2 and Cu1 for the complex deviate by -0.0079, 0.0085, -0.0085, 0.0079 and 0.2064 Å, respectively, from the least-squares plane (0.84710x+0.53076y+0.02687z = 12.60140) defined by the four ligating atoms N1,N2, N3, and O2. This indicates that the five atoms in the equatorial positions are approximately coplanar with τ of 0.03 (Addison, et al., 1984). The bond angles observed around the central Cu atom range from 82.13 (8) – 99.01 (8)° in equatorial positions and from 93.90 (8) – 98.54 (8)° for apical positions, showing the angle variability in the geometry adopted by the five coordinate CuII complexe (Le et al., 2006). The carboxyl group of the amino acid coordinates to CuIIvia one oxygen atom as an unidentate group. Electron delocalization has been observed in the carboxyl group. However, the bond distances (1.270 (3) Å) between the coordinated oxygen atoms and the carbon atoms are slightly longer (1.254 Å) than those between the uncoordinated oxygen atoms and the carbon atoms as expected (Dalhus & Görbitz, 1999).

The nitrate ion and two water molecules are not involved in the coordination sphere of the Cu ion, but are in the crystal lattice. In the supramolecular network there are O—H···O and N—H···O hydrogen bond interactions and weak O—H···O and N—H···O intermolecular interactions (table 1) that help stabilize crystal packing. The O1w donor-acceptor atom of water molecule solvate interacts with O4 acceptor atom of the nitrate group and the N3 donor atom of the amino group, forming R42(6) and 2R21(6) motifs, respectively. In addition the hydrogen bond formed from the O3w donor atom of the water coordinated to the metal and O2w donor-acceptor atom of the water solvate and O1 acceptor atom of carboxylate group form a C22(5) motif. All these interactions lead to infinite three-dimensional network superstructure with base vectors: #1 = [0 1 0], #2 = [1 0 0], #3 = [0 0 1].

Experimental

1 mmol (0.232 g) of hemi-pentahydrated Cu(NO3)2 was dissolved in 5 ml of water and mixed with the corresponding amount of 1,10-phenanthroline (1 mmol, 0.180 g) previously dissolved in alcohol (5 ml). To the resulting a deprotonated solution (10 ml) of L-valine (1 mmol, 0.117 g) was added under constant stirring to get a deep-blue product. Further purification was done washing the solid several times with water. The solid was isolated with 95% yield. Single crystals suitable for X-ray diffraction were obtained by slow evaporation of MeOH. Anal. calcd. for C17H24N4O8Cu (475.94 g/mol): C, 42.90; H, 5.08; N, 11.77. Found: C, 42.53; H, 5.11; N, 11.81.

Refinement

H atoms bonded to N and O atoms were located in difference maps and were refined with free coordinates and Uiso(H) = 1.2Ueq(N) and 1.2Ueq(N). H atoms attached to C atoms were placed in geometrically idealized positions, and refined as riding on their parent atoms, with C—H distances fixed to 0.930 (aromatic CH), 0.960 (methyl CH3) and 0.980 Å (methine CH2) with Uiso(H) = 1.5 Ueq(methyl C) or 1.2 Ueq(C).

Figures

Fig. 1.

Fig. 1.

The structure of the title compound, showing the atomic numbering scheme. Non-H atoms are shown with 30% probability displacement ellipsoids.

Crystal data

[Cu(C5H10NO2)(C12H8N2)(H2O)]NO3·2H2O Z = 2
Mr = 475.94 F(000) = 494
Triclinic, P1 Dx = 1.519 Mg m3
a = 7.9020 (19) Å Mo Kα radiation, λ = 0.71073 Å
b = 9.610 (3) Å Cell parameters from 43 reflections
c = 14.327 (4) Å θ = 3.4–12.5°
α = 81.89 (3)° µ = 1.10 mm1
β = 75.04 (2)° T = 298 K
γ = 87.92 (2)° Prism, blue
V = 1040.6 (5) Å3 0.45 × 0.27 × 0.21 mm

Data collection

Siemens P4 diffractometer Rint = 0.024
graphite θmax = 27.0°, θmin = 2.1°
2θ/ω scans h = −1→10
Absorption correction: ψ scan (XSCANS; Siemens, 1993) k = −12→12
Tmin = 0.729, Tmax = 0.794 l = −18→18
5563 measured reflections 3 standard reflections every 97 reflections
4551 independent reflections intensity decay: 4.9%
3807 reflections with I > 2σ(I)

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)] = 0.037 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.094 H atoms treated by a mixture of independent and constrained refinement
S = 1.06 w = 1/[σ2(Fo2) + (0.0399P)2 + 0.2653P] where P = (Fo2 + 2Fc2)/3
4551 reflections (Δ/σ)max = 0.002
297 parameters Δρmax = 0.45 e Å3
18 restraints Δρmin = −0.33 e Å3

Special details

Experimental. IR (KBr disc, cm-1): 3426 w, 3285 m, 1623s, 1609 s, 1526 m, 1427 m, 1384 s, 1052 br, 871 m, 725 m.
Geometry. All s.u.'s (except the s.u. in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell s.u.'s are taken into account individually in the estimation of s.u.'s in distances, angles and torsion angles; correlations between s.u.'s in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell s.u.'s is used for estimating s.u.'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 > 2σ(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 0.7560 (3) 0.9436 (3) 0.53537 (17) 0.0414 (5)
H1 0.6717 1.0131 0.5489 0.05*
C2 0.7973 (4) 0.8559 (3) 0.6127 (2) 0.0516 (6)
H2 0.7417 0.8675 0.6768 0.062*
C3 0.9208 (4) 0.7526 (3) 0.5934 (2) 0.0532 (7)
H3 0.9488 0.6936 0.6446 0.064*
C4 1.0053 (3) 0.7357 (2) 0.4965 (2) 0.0466 (6)
C5 1.1376 (4) 0.6333 (3) 0.4671 (3) 0.0613 (8)
H5 1.1738 0.5721 0.5146 0.074*
C6 1.2105 (4) 0.6237 (3) 0.3725 (3) 0.0622 (8)
H6 1.2944 0.5547 0.3561 0.075*
C7 1.1626 (3) 0.7164 (3) 0.2966 (2) 0.0507 (7)
C8 1.2337 (4) 0.7153 (3) 0.1953 (3) 0.0636 (8)
H8 1.3207 0.651 0.1736 0.076*
C9 1.1755 (4) 0.8078 (3) 0.1297 (2) 0.0651 (8)
H9 1.222 0.8068 0.0631 0.078*
C10 1.0460 (4) 0.9041 (3) 0.1627 (2) 0.0534 (7)
H10 1.0061 0.9662 0.1172 0.064*
C11 1.0336 (3) 0.8191 (2) 0.32296 (19) 0.0386 (5)
C12 0.9551 (3) 0.8280 (2) 0.42369 (18) 0.0365 (5)
C13 0.6115 (3) 1.2912 (2) 0.34579 (17) 0.0358 (5)
C14 0.6524 (3) 1.2917 (2) 0.23517 (17) 0.0405 (5)
H14 0.5457 1.2598 0.2218 0.049*
C15 0.6933 (4) 1.4373 (2) 0.17649 (19) 0.0482 (6)
H15 0.5934 1.4978 0.2001 0.058*
C16 0.8549 (5) 1.5035 (3) 0.1919 (3) 0.0712 (9)
H16A 0.8409 1.505 0.2604 0.107*
H16B 0.8687 1.5979 0.1585 0.107*
H16C 0.9567 1.4494 0.1666 0.107*
C17 0.7096 (6) 1.4343 (3) 0.0687 (2) 0.0808 (11)
H17A 0.8131 1.3833 0.0415 0.121*
H17B 0.7173 1.5288 0.0354 0.121*
H17C 0.6085 1.3891 0.0611 0.121*
N1 0.9771 (3) 0.91087 (19) 0.25678 (14) 0.0400 (4)
N2 0.8335 (2) 0.93059 (18) 0.44303 (14) 0.0350 (4)
N3 0.7883 (3) 1.1840 (2) 0.20673 (15) 0.0401 (4)
N4 0.2440 (4) 0.2073 (3) 0.0776 (2) 0.0687 (7)
O1 0.5238 (2) 1.38833 (16) 0.38275 (13) 0.0476 (4)
O2 0.6628 (2) 1.18555 (16) 0.39525 (11) 0.0420 (4)
O1W 0.6192 (4) 0.9891 (3) 0.11506 (19) 0.0879 (8)
O3 0.2044 (4) 0.2401 (4) 0.1587 (2) 0.1056 (10)
O2W 0.6251 (3) 0.6568 (2) 0.41289 (15) 0.0551 (5)
O4 0.3953 (4) 0.1763 (3) 0.0356 (2) 0.1061 (10)
O3W 0.5655 (3) 0.91409 (19) 0.31501 (14) 0.0492 (4)
O5 0.1312 (4) 0.2054 (3) 0.0322 (2) 0.0906 (8)
Cu1 0.79360 (4) 1.04401 (3) 0.322595 (19) 0.03449 (10)
H1A 0.547 (3) 1.035 (3) 0.094 (2) 0.052*
H1B 0.653 (4) 0.925 (2) 0.082 (2) 0.052*
H2A 0.587 (4) 0.658 (3) 0.4705 (12) 0.052*
H2B 0.591 (4) 0.581 (2) 0.4010 (18) 0.052*
H02 0.885 (4) 1.221 (3) 0.188 (2) 0.041*
H3A 0.572 (4) 0.908 (3) 0.2571 (12) 0.052*
H01 0.752 (4) 1.144 (3) 0.165 (2) 0.041*
H3B 0.578 (4) 0.832 (2) 0.3410 (16) 0.052*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
C1 0.0417 (13) 0.0409 (12) 0.0405 (12) −0.0020 (10) −0.0096 (10) −0.0033 (9)
C2 0.0562 (16) 0.0562 (15) 0.0420 (13) −0.0161 (13) −0.0152 (12) 0.0040 (11)
C3 0.0598 (17) 0.0465 (14) 0.0583 (16) −0.0121 (12) −0.0331 (14) 0.0134 (12)
C4 0.0440 (14) 0.0351 (12) 0.0664 (17) −0.0038 (10) −0.0296 (13) 0.0036 (11)
C5 0.0549 (17) 0.0399 (13) 0.099 (3) 0.0068 (12) −0.0439 (18) 0.0021 (14)
C6 0.0470 (16) 0.0438 (14) 0.103 (3) 0.0183 (12) −0.0325 (17) −0.0148 (15)
C7 0.0365 (13) 0.0360 (12) 0.082 (2) 0.0076 (10) −0.0166 (13) −0.0149 (12)
C8 0.0462 (16) 0.0553 (16) 0.087 (2) 0.0151 (13) −0.0041 (15) −0.0294 (16)
C9 0.0649 (19) 0.0583 (17) 0.0625 (18) 0.0075 (15) 0.0063 (15) −0.0206 (14)
C10 0.0624 (17) 0.0427 (13) 0.0468 (14) 0.0065 (12) 0.0013 (13) −0.0088 (11)
C11 0.0315 (11) 0.0279 (10) 0.0568 (14) 0.0023 (9) −0.0111 (10) −0.0076 (9)
C12 0.0338 (11) 0.0263 (10) 0.0508 (13) −0.0007 (8) −0.0154 (10) −0.0012 (9)
C13 0.0386 (12) 0.0268 (10) 0.0420 (12) 0.0026 (9) −0.0095 (10) −0.0067 (8)
C14 0.0457 (13) 0.0302 (10) 0.0450 (13) 0.0044 (9) −0.0121 (11) −0.0031 (9)
C15 0.0595 (16) 0.0289 (11) 0.0527 (14) 0.0057 (11) −0.0134 (12) 0.0031 (10)
C16 0.081 (2) 0.0494 (16) 0.077 (2) −0.0162 (16) −0.0099 (18) −0.0042 (15)
C17 0.125 (3) 0.0559 (18) 0.0584 (19) −0.001 (2) −0.031 (2) 0.0153 (14)
N1 0.0427 (11) 0.0303 (9) 0.0430 (11) 0.0062 (8) −0.0047 (9) −0.0045 (8)
N2 0.0361 (10) 0.0297 (8) 0.0388 (10) 0.0011 (7) −0.0098 (8) −0.0025 (7)
N3 0.0490 (12) 0.0303 (9) 0.0372 (10) 0.0061 (9) −0.0058 (9) −0.0037 (8)
N4 0.0638 (17) 0.0525 (14) 0.0730 (19) 0.0042 (12) 0.0036 (15) 0.0074 (13)
O1 0.0562 (11) 0.0321 (8) 0.0531 (10) 0.0152 (8) −0.0100 (8) −0.0125 (7)
O2 0.0544 (10) 0.0344 (8) 0.0368 (8) 0.0153 (7) −0.0114 (7) −0.0076 (6)
O1W 0.116 (2) 0.101 (2) 0.0612 (15) −0.0010 (17) −0.0442 (15) −0.0188 (13)
O3 0.115 (2) 0.133 (3) 0.0578 (15) 0.011 (2) −0.0038 (15) −0.0138 (16)
O2W 0.0665 (13) 0.0449 (10) 0.0520 (11) −0.0081 (9) −0.0089 (10) −0.0100 (9)
O4 0.0671 (17) 0.103 (2) 0.131 (3) 0.0137 (15) 0.0094 (17) −0.0271 (19)
O3W 0.0577 (11) 0.0433 (9) 0.0466 (10) −0.0016 (8) −0.0122 (9) −0.0078 (8)
O5 0.091 (2) 0.0889 (19) 0.0850 (18) −0.0104 (15) −0.0212 (16) 0.0139 (14)
Cu1 0.04126 (17) 0.02603 (13) 0.03374 (15) 0.00937 (10) −0.00668 (11) −0.00374 (9)

Geometric parameters (Å, °)

C1—N2 1.328 (3) C14—C15 1.526 (3)
C1—C2 1.395 (4) C14—H14 0.98
C1—H1 0.93 C15—C17 1.520 (4)
C2—C3 1.372 (4) C15—C16 1.526 (4)
C2—H2 0.93 C15—H15 0.98
C3—C4 1.407 (4) C16—H16A 0.96
C3—H3 0.93 C16—H16B 0.96
C4—C12 1.399 (3) C16—H16C 0.96
C4—C5 1.433 (4) C17—H17A 0.96
C5—C6 1.344 (5) C17—H17B 0.96
C5—H5 0.93 C17—H17C 0.96
C6—C7 1.426 (4) Cu1—N1 2.0320 (19)
C6—H6 0.93 Cu1—N2 1.9975 (19)
C7—C11 1.410 (3) Cu1—N3 1.992 (2)
C7—C8 1.416 (5) N3—H02 0.82 (3)
C8—C9 1.358 (5) N3—H01 0.87 (3)
C8—H8 0.93 N4—O3 1.207 (4)
C9—C10 1.390 (4) N4—O5 1.233 (4)
C9—H9 0.93 N4—O4 1.238 (4)
C10—N1 1.326 (3) Cu1—O2 1.9349 (16)
C10—H10 0.93 O1W—H1A 0.802 (15)
C11—N1 1.353 (3) O1W—H1B 0.822 (15)
C11—C12 1.430 (4) O2W—O2W 0
C12—N2 1.357 (3) O2W—H2A 0.804 (15)
C13—O1 1.239 (3) O2W—H2B 0.840 (15)
C13—O2 1.270 (3) Cu1—O3W 2.263 (2)
C13—C14 1.533 (3) O3W—H3A 0.828 (15)
C14—N3 1.484 (3) O3W—H3B 0.841 (15)
N2—C1—C2 121.9 (2) C16—C15—C14 112.7 (2)
N2—C1—H1 119 C17—C15—H15 107.1
C2—C1—H1 119 C16—C15—H15 107.1
C3—C2—C1 119.4 (3) C14—C15—H15 107.1
C3—C2—H2 120.3 C15—C16—H16A 109.5
C1—C2—H2 120.3 C15—C16—H16B 109.5
C2—C3—C4 120.2 (2) H16A—C16—H16B 109.5
C2—C3—H3 119.9 C15—C16—H16C 109.5
C4—C3—H3 119.9 H16A—C16—H16C 109.5
C12—C4—C3 116.4 (2) H16B—C16—H16C 109.5
C12—C4—C5 118.2 (3) C15—C17—H17A 109.5
C3—C4—C5 125.4 (2) C15—C17—H17B 109.5
C6—C5—C4 121.4 (3) H17A—C17—H17B 109.5
C6—C5—H5 119.3 C15—C17—H17C 109.5
C4—C5—H5 119.3 H17A—C17—H17C 109.5
C5—C6—C7 121.7 (2) H17B—C17—H17C 109.5
C5—C6—H6 119.1 C10—N1—C11 118.6 (2)
C7—C6—H6 119.1 C10—N1—Cu1 129.92 (18)
C11—C7—C8 116.0 (3) C11—N1—Cu1 111.50 (15)
C11—C7—C6 118.3 (3) C1—N2—C12 118.8 (2)
C8—C7—C6 125.7 (3) C1—N2—Cu1 128.22 (16)
C9—C8—C7 120.3 (2) C12—N2—Cu1 112.97 (15)
C9—C8—H8 119.8 C14—N3—Cu1 109.71 (14)
C7—C8—H8 119.8 C14—N3—H02 109.7 (19)
C8—C9—C10 119.4 (3) Cu1—N3—H02 106.4 (19)
C8—C9—H9 120.3 C14—N3—H01 103.7 (18)
C10—C9—H9 120.3 Cu1—N3—H01 109.8 (18)
N1—C10—C9 122.6 (3) H02—N3—H01 117 (3)
N1—C10—H10 118.7 O3—N4—O5 119.8 (3)
C9—C10—H10 118.7 O3—N4—O4 123.2 (4)
N1—C11—C7 123.0 (2) O5—N4—O4 117.0 (3)
N1—C11—C12 117.17 (19) C13—O2—Cu1 116.53 (15)
C7—C11—C12 119.8 (2) H1A—O1W—H1B 109 (2)
N2—C12—C4 123.2 (2) H2A—O2W—H2B 106 (2)
N2—C12—C11 116.22 (19) Cu1—O3W—H3A 109 (2)
C4—C12—C11 120.5 (2) Cu1—O3W—H3B 108 (2)
O1—C13—O2 123.5 (2) H3A—O3W—H3B 105.7 (19)
O1—C13—C14 119.28 (19) O2—Cu1—N3 84.00 (8)
O2—C13—C14 117.12 (18) O2—Cu1—N2 92.38 (7)
N3—C14—C15 114.5 (2) N3—Cu1—N2 168.37 (9)
N3—C14—C13 108.83 (18) O2—Cu1—N1 166.85 (8)
C15—C14—C13 113.78 (19) N3—Cu1—N1 99.01 (8)
N3—C14—H14 106.4 N2—Cu1—N1 82.13 (8)
C15—C14—H14 106.4 O2—Cu1—O3W 98.54 (8)
C13—C14—H14 106.4 N3—Cu1—O3W 95.92 (9)
C17—C15—C16 111.1 (3) N2—Cu1—O3W 95.55 (8)
C17—C15—C14 111.4 (2) N1—Cu1—O3W 93.90 (8)
N2—C1—C2—C3 −0.3 (4) C7—C11—N1—Cu1 −179.17 (19)
C1—C2—C3—C4 0.2 (4) C12—C11—N1—Cu1 1.5 (3)
C2—C3—C4—C12 −0.4 (4) C2—C1—N2—C12 0.7 (3)
C2—C3—C4—C5 179.2 (3) C2—C1—N2—Cu1 179.91 (18)
C12—C4—C5—C6 −1.0 (4) C4—C12—N2—C1 −0.9 (3)
C3—C4—C5—C6 179.4 (3) C11—C12—N2—C1 179.9 (2)
C4—C5—C6—C7 1.2 (5) C4—C12—N2—Cu1 179.74 (18)
C5—C6—C7—C11 −0.8 (4) C11—C12—N2—Cu1 0.5 (2)
C5—C6—C7—C8 179.2 (3) C15—C14—N3—Cu1 149.15 (18)
C11—C7—C8—C9 −1.1 (4) C13—C14—N3—Cu1 20.5 (2)
C6—C7—C8—C9 179.0 (3) O1—C13—O2—Cu1 178.54 (18)
C7—C8—C9—C10 0.3 (5) C14—C13—O2—Cu1 2.4 (3)
C8—C9—C10—N1 0.8 (5) C13—O2—Cu1—N3 8.10 (18)
C8—C7—C11—N1 0.9 (4) C13—O2—Cu1—N2 177.01 (18)
C6—C7—C11—N1 −179.1 (2) C13—O2—Cu1—N1 112.1 (3)
C8—C7—C11—C12 −179.8 (2) C13—O2—Cu1—O3W −87.02 (18)
C6—C7—C11—C12 0.2 (4) C14—N3—Cu1—O2 −16.23 (17)
C3—C4—C12—N2 0.8 (3) C14—N3—Cu1—N2 −88.6 (4)
C5—C4—C12—N2 −178.8 (2) C14—N3—Cu1—N1 176.68 (17)
C3—C4—C12—C11 180.0 (2) C14—N3—Cu1—O3W 81.77 (17)
C5—C4—C12—C11 0.4 (3) C1—N2—Cu1—O2 13.0 (2)
N1—C11—C12—N2 −1.4 (3) C12—N2—Cu1—O2 −167.75 (16)
C7—C11—C12—N2 179.3 (2) C1—N2—Cu1—N3 84.5 (4)
N1—C11—C12—C4 179.3 (2) C12—N2—Cu1—N3 −96.2 (4)
C7—C11—C12—C4 0.0 (3) C1—N2—Cu1—N1 −179.0 (2)
O1—C13—C14—N3 168.0 (2) C12—N2—Cu1—N1 0.24 (15)
O2—C13—C14—N3 −15.7 (3) C1—N2—Cu1—O3W −85.8 (2)
O1—C13—C14—C15 38.9 (3) C12—N2—Cu1—O3W 93.43 (16)
O2—C13—C14—C15 −144.7 (2) C10—N1—Cu1—O2 −114.1 (4)
N3—C14—C15—C17 61.3 (3) C11—N1—Cu1—O2 65.0 (4)
C13—C14—C15—C17 −172.6 (3) C10—N1—Cu1—N3 −11.8 (3)
N3—C14—C15—C16 −64.4 (3) C11—N1—Cu1—N3 167.33 (17)
C13—C14—C15—C16 61.7 (3) C10—N1—Cu1—N2 179.9 (2)
C9—C10—N1—C11 −1.0 (4) C11—N1—Cu1—N2 −0.96 (16)
C9—C10—N1—Cu1 178.1 (2) C10—N1—Cu1—O3W 84.8 (2)
C7—C11—N1—C10 0.1 (4) C11—N1—Cu1—O3W −96.04 (17)
C12—C11—N1—C10 −179.2 (2)

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
O3W—H3A···O1W 0.83 (2) 2.02 (2) 2.778 (3) 153 (3)
N3—H01···O1W 0.87 (3) 2.15 (3) 2.967 (4) 156 (2)
O3W—H3B···O2W 0.84 (2) 1.92 (2) 2.753 (3) 171 (3)
O1W—H1A···O4i 0.80 (2) 2.02 (2) 2.810 (4) 170 (3)
O1W—H1B···O4ii 0.82 (2) 2.19 (2) 2.881 (4) 143 (2)
O1W—H1B···O5ii 0.82 (2) 2.48 (2) 3.245 (5) 156 (3)
O2W—H2A···O1iii 0.80 (2) 2.05 (2) 2.836 (3) 167 (3)
O2W—H2B···O1iv 0.84 (2) 2.02 (2) 2.851 (3) 174 (3)
N3—H02···O3v 0.82 (3) 2.46 (3) 3.229 (4) 158 (2)
N3—H02···O5v 0.82 (3) 2.58 (3) 3.168 (4) 130 (2)

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

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: JJ2109).

References

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  3. Dalhus, B. & Görbitz, C. H. (1999). Acta Cryst. C55, 1547–1555. [DOI] [PubMed]
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  11. Siemens (1993). XSCANS Siemens Analytical X-ray Instruments Inc., Madison, Wisconsin, USA.

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) global, I. DOI: 10.1107/S1600536811047398/jj2109sup1.cif

e-67-m1796-sup1.cif (22.8KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811047398/jj2109Isup2.hkl

e-67-m1796-Isup2.hkl (218.4KB, hkl)

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


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