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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2010 Jan 16;66(Pt 2):m173. doi: 10.1107/S1600536810001364

Bis{2-hydr­oxy-N-[2-(2-pyrid­yl)eth­yl]benzamide}copper(I) tetra­fluoridoborate

Zhaodong Wang a, Douglas R Powell a, Robert P Houser a,*
PMCID: PMC2979673  PMID: 21579646

Abstract

The title complex, [Cu(C14H14N2O2)2]BF4, is a monomeric copper(I) species with linear two-coordinate geometry around the CuI atom. The asymmetric unit contains two half-cations that sit on crystallographic twofold rotation axes. The selected crystal was non-merohedrally twinned by a twofold rotation about an axis normal to the (100) family of planes. The ratio of the twin components refined to 0.4123 (6). Two 2-hydr­oxy-N-[2-(2-pyrid­yl)eth­yl]benzamide ligands coordinate to each CuI atom via the pyridyl N atom. Intra­molecular hydrogen bonding between the phenol OH groups and the amide O atoms imparts rigidity and planarity to the non-coordinating end of the ligand. The cationic complex is linked to the BF4 anions via hydrogen bonding between the amide NH groups in the cations and BF4 anions.

Related literature

For the synthesis and coordination chemistry of 2-hydr­oxy-N-(2-(2-pyrid­yl)eth­yl)benzamide, see: Wang et al. (2009). For the copper(I) coordination chemistry of pyridylamides, see Yang et al. (2007) and references therein.graphic file with name e-66-0m173-scheme1.jpg

Experimental

Crystal data

  • [Cu(C14H14N2O2)2]BF4

  • M r = 634.89

  • Monoclinic, Inline graphic

  • a = 21.943 (5) Å

  • b = 17.586 (4) Å

  • c = 14.607 (2) Å

  • β = 107.988 (8)°

  • V = 5361.2 (19) Å3

  • Z = 8

  • Mo Kα radiation

  • μ = 0.89 mm−1

  • T = 100 K

  • 0.40 × 0.30 × 0.12 mm

Data collection

  • Bruker APEX CCD diffractometer

  • Absorption correction: multi-scan (TWINABS; Bruker, 2001) T min = 0.714, T max = 0.905

  • 10344 measured reflections

  • 10344 independent reflections

  • 8548 reflections with I > 2σ(I)

Refinement

  • R[F 2 > 2σ(F 2)] = 0.034

  • wR(F 2) = 0.096

  • S = 1.00

  • 10344 reflections

  • 393 parameters

  • 4 restraints

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

  • Δρmax = 0.54 e Å−3

  • Δρmin = −0.39 e Å−3

Data collection: SMART (Bruker, 2007); cell refinement: SAINT (Bruker, 2007); data reduction: SAINT; program(s) used to solve structure: SHELXTL (Sheldrick, 2008); program(s) used to refine structure: SHELXTL; molecular graphics: SHELXTL; software used to prepare material for publication: SHELXTL.

Supplementary Material

Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536810001364/bt5166sup1.cif

e-66-0m173-sup1.cif (26.3KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536810001364/bt5166Isup2.hkl

e-66-0m173-Isup2.hkl (505.9KB, hkl)

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

Table 1. Selected geometric parameters (Å, °).

Cu1A—N1A 1.8872 (16)
Cu1B—N1B 1.8874 (17)
N1A—Cu1A—N1Ai 178.45 (9)
N1B—Cu1B—N1Bii 177.71 (9)

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
N9A—H9A⋯F1iii 0.72 (2) 2.23 (2) 2.923 (2) 161 (2)
O18A—H18A⋯O11A 0.83 (1) 1.79 (2) 2.554 (2) 152 (3)
N9B—H9B⋯F2iv 0.82 (1) 2.16 (1) 2.937 (2) 159 (2)
O18B—H18B⋯O11B 0.81 (1) 1.81 (2) 2.549 (2) 153 (2)

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

Acknowledgments

The National Science Foundation (CHE-0094079) supported this work. We also thank the NSF (CHE-0130835) and the University of Oklahoma for the purchase of a CCD equipped X-ray diffractometer.

supplementary crystallographic information

Comment

Our laboratory has synthesized copper(I) and copper(II) complexes of pyridylmethylamide ligands that display different coordination modes depending on whether or not the amide group is protonated (Wang, et al. 2009, and references therein). The synthesis of copper(I) complexes with these ligands is limited to the neutral form of the ligand, where the amide group is not deprotonated (Yang, et al. 2007, and references therein). Attempts to synthesize copper(I) species in the presence of base results in disproportionation of the copper(I) to copper(0) and copper(II). The title complex was synthesized with the phenol-substituted ligand 2-hydroxy-N-(2-(2-pyridyl)ethyl)benzamide. Copper(II) complexes with 2-hydroxy-N-(2-(2-pyridyl)ethyl)benzamide are either mononuclear, when synthesized in the absence of base ([Cu(C14H14N2O2)2Cl2]), or a tetracopper cluster, in the presence of base ([Cu4(C14H12N2O2)4]) (Wang, et al. 2009). The ligand in the tetracopper cluster is a dianion with the amide NH and the phenol OH both deprotonated. The title complex differs from both copper(II) complexes in that the ligand only coordinates via the pyridyl N atom.

Experimental

2-hydroxy-N-(2-(2-pyridyl)ethyl)benzamide was synthesized using a previously reported procedure (Wang, et al. 2009). The title complex, [Cu(C14H14N2O2)2]BF4, was synthesized using the following procedure: A solution of [Cu(CH3CN)4]BF4 (0.0778 g, 0.250 mmol) in CH3CN was added to a solution of 2-hydroxy-N-(2-(2-pyridyl)ethyl)benzamide (0.121 g, 0.500 mmol) in CH3CN. The resulting light yellow solution was filtered, and vapor diffusion of diethyl ether produced light yellow crystals of the title complex (0.114 g, 72% yield).

Refinement

Hydrogen atoms bonded to C were geometrically positioned and refined by a riding model. Hydrogen atom displacement parameters were set to 1.2 (1.5 for methyl) times the displacement parameters of the bonded atoms. The coordinates of the H atoms bonded to N and O were refined with U(H)=1.2Ueq(N,O). The twin law was (1 0 0.928/ 0 -1 0/ 0 0 -1). The contribution of the minor twin domain refined to 0.437 (4).

Figures

Fig. 1.

Fig. 1.

The molecular structure of the cation (molecule A) in [Cu(C14H14N2O2)2]BF4, showing the atom-numbering scheme.

Fig. 2.

Fig. 2.

The packing of [Cu(C14H14N2O2)2]BF4, viewed down the c axis, highlighting the hydrogen bonding between complex cations and BF4- anions (dashed lines). H atoms have been omitted for clarity.

Crystal data

[Cu(C14H14N2O2)2]BF4 F(000) = 2608
Mr = 634.89 Dx = 1.573 Mg m3
Monoclinic, C2/c Mo Kα radiation, λ = 0.71073 Å
a = 21.943 (5) Å Cell parameters from 6701 reflections
b = 17.586 (4) Å θ = 2.3–28.3°
c = 14.607 (2) Å µ = 0.89 mm1
β = 107.988 (8)° T = 100 K
V = 5361.2 (19) Å3 Block, colorless
Z = 8 0.40 × 0.30 × 0.12 mm

Data collection

Bruker APEX CCD diffractometer 10344 independent reflections
Radiation source: fine-focus sealed tube 8548 reflections with I > 2σ(I)
graphite Rint = 0.0000
ω scans θmax = 26.0°, θmin = 1.5°
Absorption correction: multi-scan (TWINABS; Bruker, 2001) h = −27→25
Tmin = 0.714, Tmax = 0.905 k = 0→21
10344 measured reflections l = 0→18

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)] = 0.034 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.096 H atoms treated by a mixture of independent and constrained refinement
S = 1.00 w = 1/[σ2(Fo2) + (0.058P)2] where P = (Fo2 + 2Fc2)/3
10344 reflections (Δ/σ)max < 0.001
393 parameters Δρmax = 0.54 e Å3
4 restraints Δρmin = −0.38 e Å3

Special details

Experimental. The selected crystal was twinned by a 2-fold rotation about an axis perpendicular to c. The ratio of the twin components was refined to 0.4123 (6).
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. Restraints on the N—H and O—H distances were required.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2)

x y z Uiso*/Ueq
Cu1A 0.0000 0.030574 (19) 0.7500 0.01887 (10)
N1A 0.09032 (7) 0.02912 (8) 0.79796 (11) 0.0148 (3)
C2A 0.12104 (9) 0.08497 (11) 0.85712 (14) 0.0184 (4)
H2A 0.0974 0.1287 0.8637 0.022*
C3A 0.18505 (9) 0.08182 (12) 0.90856 (14) 0.0214 (5)
H3A 0.2051 0.1224 0.9498 0.026*
C4A 0.21963 (10) 0.01848 (12) 0.89906 (14) 0.0220 (5)
H4A 0.2638 0.0143 0.9344 0.026*
C5A 0.18878 (9) −0.03911 (11) 0.83694 (14) 0.0188 (4)
H5A 0.2120 −0.0828 0.8287 0.023*
C6A 0.12434 (9) −0.03273 (11) 0.78714 (13) 0.0155 (4)
C7A 0.08947 (9) −0.09154 (11) 0.71586 (13) 0.0181 (4)
H7A1 0.0476 −0.1025 0.7253 0.022*
H7A2 0.1147 −0.1392 0.7265 0.022*
C8A 0.07893 (10) −0.06360 (12) 0.61306 (14) 0.0223 (5)
H8A1 0.0594 −0.0123 0.6060 0.027*
H8A2 0.1210 −0.0591 0.6017 0.027*
N9A 0.03805 (8) −0.11339 (10) 0.54052 (13) 0.0205 (4)
H9A 0.0537 (11) −0.1414 (13) 0.5197 (16) 0.025*
C10A −0.02547 (10) −0.11003 (11) 0.51659 (14) 0.0185 (4)
O11A −0.05148 (7) −0.06621 (8) 0.56110 (10) 0.0255 (3)
C12A −0.06483 (9) −0.15652 (11) 0.43500 (14) 0.0176 (4)
C13A −0.03803 (10) −0.20269 (11) 0.37943 (14) 0.0201 (4)
H13A 0.0072 −0.2050 0.3944 0.024*
C14A −0.07586 (10) −0.24480 (12) 0.30352 (14) 0.0217 (5)
H14A −0.0567 −0.2753 0.2662 0.026*
C15A −0.14213 (10) −0.24242 (12) 0.28176 (15) 0.0255 (5)
H15A −0.1683 −0.2718 0.2299 0.031*
C16A −0.16987 (10) −0.19767 (12) 0.33520 (15) 0.0257 (5)
H16A −0.2152 −0.1961 0.3198 0.031*
C17A −0.13206 (10) −0.15475 (11) 0.41143 (14) 0.0217 (5)
O18A −0.16259 (7) −0.11138 (9) 0.46038 (11) 0.0311 (4)
H18A −0.1339 (9) −0.0881 (13) 0.5010 (15) 0.047*
Cu1B 0.5000 0.010247 (19) 0.7500 0.02082 (11)
N1B 0.40965 (8) 0.00810 (9) 0.71312 (11) 0.0159 (3)
C2B 0.37826 (10) 0.06141 (12) 0.74773 (14) 0.0216 (5)
H2B 0.4020 0.1032 0.7823 0.026*
C3B 0.31395 (10) 0.05821 (12) 0.73547 (15) 0.0259 (5)
H3B 0.2937 0.0967 0.7614 0.031*
C4B 0.27912 (10) −0.00173 (13) 0.68487 (15) 0.0270 (5)
H4B 0.2343 −0.0050 0.6744 0.032*
C5B 0.31055 (9) −0.05727 (12) 0.64944 (14) 0.0223 (5)
H5B 0.2873 −0.0994 0.6151 0.027*
C6B 0.37568 (9) −0.05145 (11) 0.66406 (13) 0.0167 (4)
C7B 0.41130 (9) −0.10775 (11) 0.62256 (14) 0.0184 (4)
H7B1 0.3877 −0.1566 0.6103 0.022*
H7B2 0.4542 −0.1172 0.6691 0.022*
C8B 0.41838 (10) −0.07684 (11) 0.52831 (14) 0.0206 (5)
H8B1 0.3757 −0.0758 0.4790 0.025*
H8B2 0.4343 −0.0239 0.5387 0.025*
N9B 0.46169 (8) −0.12145 (9) 0.49240 (12) 0.0193 (4)
H9B 0.4468 (10) −0.1543 (10) 0.4524 (12) 0.023*
C10B 0.52477 (9) −0.11100 (10) 0.52525 (14) 0.0175 (4)
O11B 0.54836 (7) −0.06623 (8) 0.59362 (10) 0.0230 (3)
C12B 0.56650 (9) −0.15131 (10) 0.47788 (14) 0.0174 (4)
C13B 0.54194 (10) −0.19890 (11) 0.39787 (14) 0.0198 (4)
H13B 0.4970 −0.2065 0.3730 0.024*
C14B 0.58145 (11) −0.23465 (11) 0.35483 (15) 0.0233 (5)
H14B 0.5639 −0.2666 0.3007 0.028*
C15B 0.64757 (11) −0.22376 (12) 0.39108 (16) 0.0259 (5)
H15B 0.6751 −0.2488 0.3617 0.031*
C16B 0.67318 (10) −0.17715 (12) 0.46890 (15) 0.0253 (5)
H16B 0.7182 −0.1695 0.4926 0.030*
C17B 0.63318 (10) −0.14095 (11) 0.51318 (14) 0.0206 (4)
O18B 0.66125 (7) −0.09581 (9) 0.58966 (11) 0.0270 (3)
H18B 0.6323 (8) −0.0777 (13) 0.6054 (16) 0.032*
B1 0.16533 (11) 0.24811 (14) 0.09405 (19) 0.0238 (5)
F1 0.12698 (6) 0.22361 (6) 0.00247 (9) 0.0272 (3)
F2 0.12345 (6) 0.27278 (6) 0.14410 (8) 0.0265 (3)
F3 0.20174 (6) 0.18853 (8) 0.14239 (10) 0.0391 (3)
F4 0.20245 (6) 0.30833 (8) 0.08330 (10) 0.0416 (4)

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
Cu1A 0.01145 (18) 0.01777 (19) 0.0243 (2) 0.000 0.00099 (14) 0.000
N1A 0.0137 (8) 0.0140 (8) 0.0160 (9) −0.0013 (6) 0.0036 (7) 0.0018 (7)
C2A 0.0203 (10) 0.0181 (10) 0.0186 (11) −0.0015 (8) 0.0087 (8) −0.0006 (8)
C3A 0.0189 (11) 0.0256 (11) 0.0194 (11) −0.0056 (9) 0.0056 (9) −0.0044 (9)
C4A 0.0132 (11) 0.0309 (12) 0.0207 (11) −0.0022 (9) 0.0036 (8) −0.0005 (9)
C5A 0.0171 (10) 0.0219 (10) 0.0188 (11) 0.0023 (8) 0.0077 (9) 0.0012 (8)
C6A 0.0184 (10) 0.0159 (10) 0.0133 (10) −0.0004 (8) 0.0067 (8) 0.0031 (8)
C7A 0.0189 (10) 0.0163 (10) 0.0191 (11) −0.0016 (8) 0.0058 (8) −0.0007 (8)
C8A 0.0278 (12) 0.0209 (11) 0.0172 (11) −0.0062 (9) 0.0054 (9) −0.0016 (8)
N9A 0.0240 (10) 0.0188 (9) 0.0187 (9) −0.0008 (7) 0.0066 (8) −0.0055 (7)
C10A 0.0257 (11) 0.0134 (10) 0.0157 (10) 0.0025 (8) 0.0054 (8) 0.0041 (8)
O11A 0.0313 (9) 0.0235 (8) 0.0213 (8) 0.0071 (7) 0.0073 (7) −0.0050 (6)
C12A 0.0225 (11) 0.0154 (10) 0.0149 (10) 0.0015 (8) 0.0059 (8) 0.0015 (8)
C13A 0.0203 (11) 0.0201 (10) 0.0201 (11) −0.0011 (8) 0.0065 (9) 0.0000 (9)
C14A 0.0260 (12) 0.0208 (11) 0.0182 (11) −0.0001 (9) 0.0068 (9) −0.0043 (9)
C15A 0.0274 (13) 0.0240 (11) 0.0215 (12) −0.0047 (9) 0.0022 (9) −0.0015 (9)
C16A 0.0181 (11) 0.0301 (12) 0.0265 (12) 0.0009 (9) 0.0034 (9) 0.0032 (10)
C17A 0.0248 (11) 0.0219 (11) 0.0192 (11) 0.0052 (9) 0.0079 (9) 0.0039 (9)
O18A 0.0249 (9) 0.0375 (10) 0.0304 (9) 0.0099 (7) 0.0080 (7) −0.0067 (7)
Cu1B 0.01183 (19) 0.02000 (19) 0.0276 (2) 0.000 0.00163 (15) 0.000
N1B 0.0136 (9) 0.0171 (8) 0.0158 (8) 0.0025 (6) 0.0027 (7) 0.0025 (7)
C2B 0.0251 (12) 0.0208 (11) 0.0165 (11) 0.0045 (9) 0.0030 (9) 0.0015 (9)
C3B 0.0268 (12) 0.0306 (12) 0.0226 (12) 0.0121 (10) 0.0109 (10) 0.0049 (10)
C4B 0.0156 (12) 0.0419 (14) 0.0249 (12) 0.0038 (9) 0.0086 (9) 0.0100 (11)
C5B 0.0182 (11) 0.0272 (11) 0.0194 (11) −0.0043 (9) 0.0027 (9) 0.0051 (9)
C6B 0.0188 (10) 0.0182 (10) 0.0125 (10) 0.0000 (8) 0.0038 (8) 0.0050 (8)
C7B 0.0201 (11) 0.0167 (10) 0.0185 (11) −0.0011 (8) 0.0058 (8) 0.0015 (8)
C8B 0.0244 (11) 0.0194 (10) 0.0199 (11) 0.0057 (9) 0.0097 (9) 0.0024 (8)
N9B 0.0221 (9) 0.0173 (9) 0.0190 (9) 0.0003 (7) 0.0073 (7) −0.0035 (7)
C10B 0.0238 (11) 0.0129 (9) 0.0163 (10) −0.0031 (8) 0.0069 (8) 0.0035 (8)
O11B 0.0286 (8) 0.0196 (7) 0.0223 (8) −0.0059 (6) 0.0101 (6) −0.0058 (6)
C12B 0.0207 (11) 0.0150 (10) 0.0176 (10) −0.0002 (8) 0.0078 (8) 0.0027 (8)
C13B 0.0185 (10) 0.0199 (11) 0.0203 (11) −0.0004 (8) 0.0049 (9) 0.0009 (9)
C14B 0.0279 (12) 0.0228 (11) 0.0192 (11) 0.0012 (9) 0.0072 (9) −0.0025 (9)
C15B 0.0276 (12) 0.0292 (12) 0.0249 (12) 0.0076 (9) 0.0141 (10) 0.0046 (9)
C16B 0.0188 (11) 0.0303 (12) 0.0266 (12) 0.0000 (9) 0.0066 (9) 0.0061 (10)
C17B 0.0246 (11) 0.0199 (10) 0.0167 (10) −0.0035 (9) 0.0055 (9) 0.0026 (8)
O18B 0.0227 (8) 0.0306 (9) 0.0264 (8) −0.0066 (7) 0.0059 (7) −0.0073 (7)
B1 0.0174 (12) 0.0237 (12) 0.0298 (14) −0.0005 (10) 0.0064 (10) −0.0023 (11)
F1 0.0297 (7) 0.0263 (7) 0.0266 (7) −0.0038 (5) 0.0101 (6) −0.0054 (5)
F2 0.0290 (7) 0.0260 (7) 0.0259 (7) 0.0064 (5) 0.0106 (6) −0.0002 (5)
F3 0.0264 (7) 0.0396 (8) 0.0484 (9) 0.0149 (6) 0.0074 (6) 0.0076 (7)
F4 0.0320 (8) 0.0387 (8) 0.0550 (9) −0.0173 (6) 0.0147 (7) −0.0033 (7)

Geometric parameters (Å, °)

Cu1A—N1A 1.8872 (16) N1B—C2B 1.350 (2)
Cu1A—N1Ai 1.8872 (16) N1B—C6B 1.355 (2)
N1A—C2A 1.344 (2) C2B—C3B 1.368 (3)
N1A—C6A 1.356 (2) C2B—H2B 0.9500
C2A—C3A 1.374 (3) C3B—C4B 1.376 (3)
C2A—H2A 0.9500 C3B—H3B 0.9500
C3A—C4A 1.379 (3) C4B—C5B 1.385 (3)
C3A—H3A 0.9500 C4B—H4B 0.9500
C4A—C5A 1.389 (3) C5B—C6B 1.382 (3)
C4A—H4A 0.9500 C5B—H5B 0.9500
C5A—C6A 1.381 (3) C6B—C7B 1.500 (3)
C5A—H5A 0.9500 C7B—C8B 1.532 (3)
C6A—C7A 1.499 (3) C7B—H7B1 0.9900
C7A—C8A 1.528 (3) C7B—H7B2 0.9900
C7A—H7A1 0.9900 C8B—N9B 1.450 (2)
C7A—H7A2 0.9900 C8B—H8B1 0.9900
C8A—N9A 1.452 (2) C8B—H8B2 0.9900
C8A—H8A1 0.9900 N9B—C10B 1.330 (3)
C8A—H8A2 0.9900 N9B—H9B 0.815 (11)
N9A—C10A 1.330 (3) C10B—O11B 1.251 (2)
N9A—H9A 0.72 (2) C10B—C12B 1.487 (3)
C10A—O11A 1.254 (2) C12B—C13B 1.403 (3)
C10A—C12A 1.483 (3) C12B—C17B 1.405 (3)
C12A—C13A 1.399 (3) C13B—C14B 1.371 (3)
C12A—C17A 1.408 (3) C13B—H13B 0.9500
C13A—C14A 1.378 (3) C14B—C15B 1.396 (3)
C13A—H13A 0.9500 C14B—H14B 0.9500
C14A—C15A 1.390 (3) C15B—C16B 1.373 (3)
C14A—H14A 0.9500 C15B—H15B 0.9500
C15A—C16A 1.376 (3) C16B—C17B 1.395 (3)
C15A—H15A 0.9500 C16B—H16B 0.9500
C16A—C17A 1.388 (3) C17B—O18B 1.354 (2)
C16A—H16A 0.9500 O18B—H18B 0.805 (11)
C17A—O18A 1.356 (2) B1—F3 1.373 (3)
O18A—H18A 0.829 (12) B1—F4 1.374 (3)
Cu1B—N1B 1.8874 (17) B1—F2 1.408 (3)
Cu1B—N1Bii 1.8874 (17) B1—F1 1.410 (3)
N1A—Cu1A—N1Ai 178.45 (9) C6B—N1B—Cu1B 121.61 (13)
C2A—N1A—C6A 118.45 (17) N1B—C2B—C3B 123.2 (2)
C2A—N1A—Cu1A 119.31 (13) N1B—C2B—H2B 118.4
C6A—N1A—Cu1A 121.37 (13) C3B—C2B—H2B 118.4
N1A—C2A—C3A 123.17 (18) C2B—C3B—C4B 118.8 (2)
N1A—C2A—H2A 118.4 C2B—C3B—H3B 120.6
C3A—C2A—H2A 118.4 C4B—C3B—H3B 120.6
C2A—C3A—C4A 118.61 (19) C3B—C4B—C5B 118.9 (2)
C2A—C3A—H3A 120.7 C3B—C4B—H4B 120.6
C4A—C3A—H3A 120.7 C5B—C4B—H4B 120.6
C3A—C4A—C5A 118.86 (19) C6B—C5B—C4B 120.0 (2)
C3A—C4A—H4A 120.6 C6B—C5B—H5B 120.0
C5A—C4A—H4A 120.6 C4B—C5B—H5B 120.0
C6A—C5A—C4A 119.89 (19) N1B—C6B—C5B 120.84 (18)
C6A—C5A—H5A 120.1 N1B—C6B—C7B 116.97 (17)
C4A—C5A—H5A 120.1 C5B—C6B—C7B 122.11 (18)
N1A—C6A—C5A 121.00 (18) C6B—C7B—C8B 109.81 (16)
N1A—C6A—C7A 116.95 (17) C6B—C7B—H7B1 109.7
C5A—C6A—C7A 122.00 (17) C8B—C7B—H7B1 109.7
C6A—C7A—C8A 110.51 (16) C6B—C7B—H7B2 109.7
C6A—C7A—H7A1 109.5 C8B—C7B—H7B2 109.7
C8A—C7A—H7A1 109.5 H7B1—C7B—H7B2 108.2
C6A—C7A—H7A2 109.5 N9B—C8B—C7B 113.13 (16)
C8A—C7A—H7A2 109.5 N9B—C8B—H8B1 109.0
H7A1—C7A—H7A2 108.1 C7B—C8B—H8B1 109.0
N9A—C8A—C7A 113.27 (17) N9B—C8B—H8B2 109.0
N9A—C8A—H8A1 108.9 C7B—C8B—H8B2 109.0
C7A—C8A—H8A1 108.9 H8B1—C8B—H8B2 107.8
N9A—C8A—H8A2 108.9 C10B—N9B—C8B 121.34 (17)
C7A—C8A—H8A2 108.9 C10B—N9B—H9B 119.9 (15)
H8A1—C8A—H8A2 107.7 C8B—N9B—H9B 118.7 (15)
C10A—N9A—C8A 121.77 (18) O11B—C10B—N9B 120.18 (19)
C10A—N9A—H9A 121.2 (19) O11B—C10B—C12B 120.59 (18)
C8A—N9A—H9A 117.0 (19) N9B—C10B—C12B 119.21 (17)
O11A—C10A—N9A 119.95 (18) C13B—C12B—C17B 118.15 (18)
O11A—C10A—C12A 120.69 (18) C13B—C12B—C10B 122.59 (18)
N9A—C10A—C12A 119.33 (18) C17B—C12B—C10B 119.25 (18)
C13A—C12A—C17A 117.85 (18) C14B—C13B—C12B 121.41 (19)
C13A—C12A—C10A 122.77 (18) C14B—C13B—H13B 119.3
C17A—C12A—C10A 119.37 (17) C12B—C13B—H13B 119.3
C14A—C13A—C12A 121.46 (19) C13B—C14B—C15B 119.59 (19)
C14A—C13A—H13A 119.3 C13B—C14B—H14B 120.2
C12A—C13A—H13A 119.3 C15B—C14B—H14B 120.2
C13A—C14A—C15A 119.71 (19) C16B—C15B—C14B 120.5 (2)
C13A—C14A—H14A 120.1 C16B—C15B—H15B 119.7
C15A—C14A—H14A 120.1 C14B—C15B—H15B 119.7
C16A—C15A—C14A 120.2 (2) C15B—C16B—C17B 120.1 (2)
C16A—C15A—H15A 119.9 C15B—C16B—H16B 120.0
C14A—C15A—H15A 119.9 C17B—C16B—H16B 120.0
C15A—C16A—C17A 120.4 (2) O18B—C17B—C16B 117.34 (18)
C15A—C16A—H16A 119.8 O18B—C17B—C12B 122.40 (18)
C17A—C16A—H16A 119.8 C16B—C17B—C12B 120.26 (19)
O18A—C17A—C16A 117.29 (19) C17B—O18B—H18B 105.6 (17)
O18A—C17A—C12A 122.33 (18) F3—B1—F4 112.05 (19)
C16A—C17A—C12A 120.38 (19) F3—B1—F2 109.72 (19)
C17A—O18A—H18A 105.4 (18) F4—B1—F2 109.07 (18)
N1B—Cu1B—N1Bii 177.71 (9) F3—B1—F1 109.67 (19)
C2B—N1B—C6B 118.27 (17) F4—B1—F1 109.17 (19)
C2B—N1B—Cu1B 119.44 (14) F2—B1—F1 107.02 (17)
C6A—N1A—C2A—C3A −1.2 (3) C6B—N1B—C2B—C3B −0.1 (3)
Cu1A—N1A—C2A—C3A 168.21 (15) Cu1B—N1B—C2B—C3B −170.83 (15)
N1A—C2A—C3A—C4A 0.1 (3) N1B—C2B—C3B—C4B −0.5 (3)
C2A—C3A—C4A—C5A 0.9 (3) C2B—C3B—C4B—C5B 1.0 (3)
C3A—C4A—C5A—C6A −1.0 (3) C3B—C4B—C5B—C6B −0.8 (3)
C2A—N1A—C6A—C5A 1.2 (3) C2B—N1B—C6B—C5B 0.3 (3)
Cu1A—N1A—C6A—C5A −168.01 (14) Cu1B—N1B—C6B—C5B 170.80 (14)
C2A—N1A—C6A—C7A −176.21 (17) C2B—N1B—C6B—C7B 177.21 (16)
Cu1A—N1A—C6A—C7A 14.6 (2) Cu1B—N1B—C6B—C7B −12.3 (2)
C4A—C5A—C6A—N1A −0.1 (3) C4B—C5B—C6B—N1B 0.2 (3)
C4A—C5A—C6A—C7A 177.15 (18) C4B—C5B—C6B—C7B −176.57 (18)
N1A—C6A—C7A—C8A 74.4 (2) N1B—C6B—C7B—C8B −80.1 (2)
C5A—C6A—C7A—C8A −102.9 (2) C5B—C6B—C7B—C8B 96.8 (2)
C6A—C7A—C8A—N9A −172.26 (17) C6B—C7B—C8B—N9B 169.84 (16)
C7A—C8A—N9A—C10A 82.1 (2) C7B—C8B—N9B—C10B −82.9 (2)
C8A—N9A—C10A—O11A −4.3 (3) C8B—N9B—C10B—O11B 5.6 (3)
C8A—N9A—C10A—C12A 173.60 (17) C8B—N9B—C10B—C12B −172.57 (16)
O11A—C10A—C12A—C13A 175.99 (18) O11B—C10B—C12B—C13B −176.59 (18)
N9A—C10A—C12A—C13A −1.9 (3) N9B—C10B—C12B—C13B 1.6 (3)
O11A—C10A—C12A—C17A −4.0 (3) O11B—C10B—C12B—C17B 2.5 (3)
N9A—C10A—C12A—C17A 178.11 (18) N9B—C10B—C12B—C17B −179.32 (18)
C17A—C12A—C13A—C14A 0.5 (3) C17B—C12B—C13B—C14B 0.1 (3)
C10A—C12A—C13A—C14A −179.47 (19) C10B—C12B—C13B—C14B 179.18 (18)
C12A—C13A—C14A—C15A −0.7 (3) C12B—C13B—C14B—C15B 0.0 (3)
C13A—C14A—C15A—C16A 0.6 (3) C13B—C14B—C15B—C16B −0.5 (3)
C14A—C15A—C16A—C17A −0.2 (3) C14B—C15B—C16B—C17B 0.8 (3)
C15A—C16A—C17A—O18A 179.36 (19) C15B—C16B—C17B—O18B 179.90 (18)
C15A—C16A—C17A—C12A 0.0 (3) C15B—C16B—C17B—C12B −0.7 (3)
C13A—C12A—C17A—O18A −179.44 (18) C13B—C12B—C17B—O18B 179.63 (18)
C10A—C12A—C17A—O18A 0.5 (3) C10B—C12B—C17B—O18B 0.5 (3)
C13A—C12A—C17A—C16A −0.1 (3) C13B—C12B—C17B—C16B 0.2 (3)
C10A—C12A—C17A—C16A 179.85 (18) C10B—C12B—C17B—C16B −178.91 (18)

Symmetry codes: (i) −x, y, −z+3/2; (ii) −x+1, y, −z+3/2.

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
N9A—H9A···F1iii 0.72 (2) 2.23 (2) 2.923 (2) 161 (2)
O18A—H18A···O11A 0.83 (1) 1.79 (2) 2.554 (2) 152 (3)
N9B—H9B···F2iv 0.82 (1) 2.16 (1) 2.937 (2) 159 (2)
O18B—H18B···O11B 0.81 (1) 1.81 (2) 2.549 (2) 153 (2)

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

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: BT5166).

References

  1. Bruker (2001). TWINABS. Bruker AXS Inc., Madison, Wisconsin, USA.
  2. Bruker (2007). SMART and SAINT Bruker AXS Inc., Madison, Wisconsin, USA.
  3. Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
  4. Wang, Z. D., Powell, D. R. & Houser, R. P. (2009). Inorg. Chem. Commun.12, 511–514.
  5. Yang, L., Powell, D. R. & Houser, R. P. (2007). Dalton Trans. pp. 955–964. [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 I, global. DOI: 10.1107/S1600536810001364/bt5166sup1.cif

e-66-0m173-sup1.cif (26.3KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536810001364/bt5166Isup2.hkl

e-66-0m173-Isup2.hkl (505.9KB, 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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