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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2011 Apr 22;67(Pt 5):m621. doi: 10.1107/S160053681101422X

cis-Bis[1,1-dibenzyl-3-(furan-2-yl­carbonyl)thio­ureato-κ2 O,S]copper(II)

Hiram Pérez a,*, Cecilia C P da Silva b, Ana M Plutín c, Carlos A de Simone b, Javier Ellena b
PMCID: PMC3089162  PMID: 21754333

Abstract

In the title compound, [Cu(C20H17N2O2S)2], the CuII atom is coordinated by the S and O atoms of two 1,1-dibenzyl-3-(furan-2-ylcarbon­yl)thio­ureate ligands in a distorted square-planar geometry. The two O and two S atoms are mutually cis to each other. The Cu—S and Cu—O bond lengths lie within the ranges of those found in related structures. The dihedral angle between the planes of the two chelating rings is 26.15 (6)°.

Related literature

For general background, see: Arslan et al. (2003 ▶). For synthesis details, see: Nagasawa & Mitsunobu (1981 ▶). For related structures, see: Binzet et al. (2006 ▶); Gomes et al. (2007 ▶); Pérez et al. (2011 ▶).graphic file with name e-67-0m621-scheme1.jpg

Experimental

Crystal data

  • [Cu(C20H17N2O2S)2]

  • M r = 762.37

  • Monoclinic, Inline graphic

  • a = 18.8390 (3) Å

  • b = 10.8730 (2) Å

  • c = 19.6200 (3) Å

  • β = 114.748 (1)°

  • V = 3649.79 (10) Å3

  • Z = 4

  • Mo Kα radiation

  • μ = 0.76 mm−1

  • T = 293 K

  • 0.49 × 0.44 × 0.39 mm

Data collection

  • Nonius KappaCCD area-detector diffractometer

  • Absorption correction: gaussian (Coppens et al., 1965 ▶) T min = 0.779, T max = 0.886

  • 21982 measured reflections

  • 7413 independent reflections

  • 6761 reflections with I > 2σ(I)

  • R int = 0.027

Refinement

  • R[F 2 > 2σ(F 2)] = 0.049

  • wR(F 2) = 0.122

  • S = 1.07

  • 7413 reflections

  • 460 parameters

  • H-atom parameters constrained

  • Δρmax = 0.23 e Å−3

  • Δρmin = −0.39 e Å−3

Data collection: COLLECT (Enraf–Nonius, 2000 ▶); cell refinement: SCALEPACK (Otwinowski & Minor, 1997 ▶); data reduction: DENZO (Otwinowski & Minor, 1997 ▶), SCALEPACK and SORTAV (Blessing, 1987 ▶, 1989 ▶); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: ORTEP-3 for Windows (Farrugia, 1997 ▶) and Mercury (Macrae et al., 2006 ▶); software used to prepare material for publication: WinGX (Farrugia, 1999 ▶).

Supplementary Material

Crystal structure: contains datablocks global, I. DOI: 10.1107/S160053681101422X/bt5517sup1.cif

e-67-0m621-sup1.cif (29.2KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S160053681101422X/bt5517Isup2.hkl

e-67-0m621-Isup2.hkl (355.4KB, hkl)

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

Acknowledgments

The authors thank the Grupo de Cristalografia, IFSC, USP, Brazil, for allowing the X-ray data collection. The authors acknowledge financial support from the PhD Cooperative Program ICTP/CLAF.

supplementary crystallographic information

Comment

N-acyl-N',N'-disubstituted thioureas have attracted the attention of researches over the last three decades with regard to coordination behaviour towards transition metals (Arslan et al., 2003). During complex formation, the ligand is deprotonated, which results in a neutral complex with a six-membered ring chelating the metal ion.

In the crystal structure of the title complex, the two furoylthiourea molecules adopt a cis conformation, bonded to the central CuII ion as shown in Fig. 1. The complex coordination geometry is a distorted square-plane as reflected by angles O1—Cu—S2 [166.02 (6)°] and O2—Cu—S1 [163.52 (7)°]. The distance of Cu atom from the best plane through the coordination sphere is 0.2486 (1) Å. The chelate ring systems, Cu–O1–C1–N1–C2–S1 and Cu–O2–C21–N3–C22–S2, are nearly planar with the largest deviations from the best plane being -0.118 (1) Å for C2 and 0.114 (2) Å for C22, respectively. The dihedral angle of 26.15 (6)° between these chelate planes indicates a strong distortion from square planar towards tetrahedral geometry. By comparison, the corresponding O—Ni—S angles and dihedral angle for the NiII analog (Pérez et al., 2011) are 169.66 (5)°, 170.09 (6)° and 20.33 (6)°, respectively. As a result, the square-planar coordination geometry of the title molecule is more distorted. The Cu—S and Cu—O bond lengths lie within the range of those found in the related structures (Gomes et al., 2007, Binzet et al., 2006). The bond lengths of the thiocarbonyl and carbonyl bonds are longer than the average for C═S (1.68 Å) and C═O (1.20 Å) in thioureas, while the C—N bonds in the chelate rings are all shorter than the average for C—N single bond of about 1.48 Å. This indicates extensive electronic delocalization within the complex rings. Fig. 2 shows the arrangement of the complex molecules in the unit cell.

Experimental

The 1,1-dibenzyl-3-[(furan-2-yl)-carbonyl]thiourea ligand was prepared using the standard procedure previously reported in the literature (Nagasawa & Mitsunobu, 1981) by the reaction of furoyl chloride with KSCN in anhydrous acetone, and then condensation with dibenzylamine. To an ethanol solution (30 ml) containing the ligand (0.70 g, 2 mmol) was added an ethanol solution of Cu(CH3COO)2.H2O (0.20 g, 1 mmol). The solution was stirred at room temperature for 2 h, and at once a solution of NaOH (1 N) was added to adjust pH to the neutral value. The mixture was filtered and the filtrate was evaporated under reduced pressure to give a green solid, which was washed with acetone. Single crystals were obtained by slow evaporation of a chloroform/dichloromethane solution (1:1, v/v) of the complex.

Refinement

H atoms were positioned geometrically and refined as riding atoms, with C—H = 0.93 Å and Uiso(H) = 1.2Ueq(C) for aromatic, and C—H = 0.97 Å and 1.5Ueq(C) for methylene.

Figures

Fig. 1.

Fig. 1.

The molecular structure of title compound. Displacement ellipsoids are drawn at the 50% probability level.

Fig. 2.

Fig. 2.

Crystal packing of title complex, viewed along [010]. H atoms have been omitted for clarity.

Crystal data

[Cu(C20H17N2O2S)2] F(000) = 1580
Mr = 762.37 Dx = 1.387 Mg m−3
Monoclinic, P21/n Mo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2yn Cell parameters from 22283 reflections
a = 18.8390 (3) Å θ = 2.9–26.7°
b = 10.8730 (2) Å µ = 0.76 mm−1
c = 19.6200 (3) Å T = 293 K
β = 114.748 (1)° Prism, blue
V = 3649.79 (10) Å3 0.49 × 0.44 × 0.39 mm
Z = 4

Data collection

Nonius KappaCCD area-detector diffractometer 7413 independent reflections
Radiation source: Enraf–Nonius FR590 6761 reflections with I > 2σ(I)
graphite Rint = 0.027
Detector resolution: 9 pixels mm-1 θmax = 26.7°, θmin = 3.0°
CCD rotation images, thick slices scans h = −23→23
Absorption correction: gaussian (Coppens et al., 1965) k = −13→13
Tmin = 0.779, Tmax = 0.886 l = −24→24
21982 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)] = 0.049 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.122 H-atom parameters constrained
S = 1.07 w = 1/[σ2(Fo2) + (0.0633P)2 + 1.1325P] where P = (Fo2 + 2Fc2)/3
7413 reflections (Δ/σ)max = 0.001
460 parameters Δρmax = 0.23 e Å−3
0 restraints Δρmin = −0.39 e Å−3

Special details

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
Cu 0.508045 (16) 0.07839 (3) 0.297423 (16) 0.04477 (11)
S2 0.59888 (4) 0.07792 (6) 0.25262 (4) 0.05644 (19)
S1 0.53343 (5) 0.27665 (7) 0.32023 (5) 0.0707 (2)
O1 0.45058 (10) 0.06749 (15) 0.35857 (10) 0.0493 (4)
O2 0.46288 (11) −0.07565 (18) 0.25155 (12) 0.0641 (5)
O3 0.39877 (11) −0.02783 (16) 0.45314 (11) 0.0570 (4)
O4 0.35836 (12) −0.2514 (2) 0.18813 (13) 0.0763 (6)
N1 0.44597 (11) 0.26752 (17) 0.40284 (11) 0.0424 (4)
N2 0.47257 (11) 0.45499 (18) 0.36697 (11) 0.0429 (4)
N3 0.53966 (11) −0.14815 (18) 0.19153 (11) 0.0447 (4)
N4 0.65912 (11) −0.09441 (17) 0.19891 (11) 0.0425 (4)
C1 0.43832 (12) 0.1451 (2) 0.39995 (12) 0.0395 (5)
C2 0.47889 (13) 0.3315 (2) 0.36579 (13) 0.0420 (5)
C3 0.40694 (13) 0.0971 (2) 0.45135 (13) 0.0415 (5)
C4 0.38350 (16) 0.1503 (3) 0.50008 (15) 0.0574 (7)
H4 0.3837 0.234 0.51 0.069*
C5 0.35819 (19) 0.0537 (3) 0.53378 (17) 0.0668 (8)
H5 0.338 0.0618 0.5695 0.08*
C6 0.36918 (17) −0.0499 (3) 0.50399 (17) 0.0626 (7)
H6 0.358 −0.1279 0.5165 0.075*
C7 0.43616 (13) 0.5172 (2) 0.41091 (12) 0.0422 (5)
H7A 0.4716 0.58 0.4417 0.051*
H7B 0.4291 0.4577 0.4444 0.051*
C8 0.35843 (13) 0.5760 (2) 0.36437 (12) 0.0414 (5)
C9 0.29283 (14) 0.5045 (3) 0.32657 (14) 0.0545 (6)
H9 0.2976 0.4193 0.3272 0.065*
C10 0.22047 (16) 0.5575 (3) 0.28797 (17) 0.0673 (8)
H10 0.1768 0.5086 0.2627 0.081*
C11 0.21354 (17) 0.6836 (3) 0.28721 (16) 0.0685 (8)
H11 0.1648 0.72 0.2616 0.082*
C12 0.27814 (18) 0.7558 (3) 0.32403 (17) 0.0681 (8)
H12 0.2732 0.8409 0.3231 0.082*
C13 0.35041 (16) 0.7019 (2) 0.36246 (15) 0.0540 (6)
H13 0.3941 0.7512 0.3873 0.065*
C14 0.50761 (15) 0.5373 (2) 0.33057 (14) 0.0495 (6)
H14A 0.4777 0.6131 0.3175 0.059*
H14B 0.5031 0.4993 0.2842 0.059*
C15 0.59256 (15) 0.5687 (2) 0.37715 (14) 0.0465 (5)
C16 0.63705 (15) 0.5165 (2) 0.44601 (14) 0.0533 (6)
H16 0.615 0.4577 0.4658 0.064*
C17 0.71447 (18) 0.5511 (3) 0.48607 (18) 0.0709 (8)
H17 0.7439 0.516 0.5327 0.085*
C18 0.7477 (2) 0.6370 (4) 0.4571 (2) 0.0827 (10)
H18 0.7994 0.6608 0.4842 0.099*
C19 0.7043 (2) 0.6874 (3) 0.3881 (2) 0.0791 (10)
H19 0.727 0.7445 0.368 0.095*
C20 0.62787 (18) 0.6542 (3) 0.34867 (18) 0.0621 (7)
H20 0.599 0.6895 0.302 0.075*
C21 0.47872 (13) −0.1453 (2) 0.20874 (13) 0.0441 (5)
C22 0.59750 (13) −0.0648 (2) 0.21315 (12) 0.0405 (5)
C23 0.42344 (14) −0.2456 (2) 0.17448 (13) 0.0491 (6)
C24 0.42619 (19) −0.3425 (3) 0.13331 (16) 0.0645 (7)
H24 0.4649 −0.3597 0.1169 0.077*
C25 0.3587 (2) −0.4131 (3) 0.1198 (2) 0.0890 (11)
H25 0.3443 −0.4861 0.0927 0.107*
C26 0.3200 (2) −0.3554 (4) 0.1530 (2) 0.0917 (12)
H26 0.2728 −0.3822 0.1524 0.11*
C27 0.66466 (15) −0.2122 (2) 0.16429 (13) 0.0476 (6)
H27A 0.628 −0.2702 0.1693 0.057*
H27B 0.7168 −0.2456 0.191 0.057*
C28 0.64762 (15) −0.1988 (2) 0.08239 (14) 0.0484 (6)
C29 0.57841 (18) −0.1499 (3) 0.03292 (17) 0.0744 (9)
H29 0.5418 −0.1239 0.0501 0.089*
C30 0.5620 (2) −0.1384 (4) −0.04314 (18) 0.0916 (11)
H30 0.5149 −0.104 −0.0762 0.11*
C31 0.6151 (2) −0.1776 (4) −0.06883 (19) 0.0873 (11)
H31 0.6042 −0.1704 −0.1195 0.105*
C32 0.6840 (2) −0.2271 (3) −0.02047 (19) 0.0816 (10)
H32 0.7201 −0.2543 −0.0381 0.098*
C33 0.70071 (19) −0.2372 (3) 0.05522 (17) 0.0648 (7)
H33 0.7483 −0.2703 0.0881 0.078*
C34 0.72555 (14) −0.0120 (2) 0.21270 (13) 0.0453 (5)
H34A 0.7097 0.0719 0.2159 0.054*
H34B 0.7394 −0.0166 0.1704 0.054*
C35 0.79670 (14) −0.0422 (2) 0.28359 (14) 0.0452 (5)
C36 0.79724 (17) −0.0283 (3) 0.35352 (16) 0.0621 (7)
H36 0.7525 −0.0007 0.3577 0.074*
C37 0.8635 (2) −0.0550 (3) 0.41754 (18) 0.0785 (9)
H37 0.8628 −0.0459 0.4644 0.094*
C38 0.9302 (2) −0.0947 (3) 0.4126 (2) 0.0787 (9)
H38 0.9748 −0.1119 0.4558 0.094*
C39 0.93044 (19) −0.1087 (4) 0.3436 (2) 0.0822 (10)
H39 0.9754 −0.136 0.3397 0.099*
C40 0.86415 (17) −0.0825 (3) 0.27935 (18) 0.0648 (8)
H40 0.865 −0.0922 0.2326 0.078*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
Cu 0.04319 (18) 0.04824 (19) 0.04929 (19) 0.00021 (12) 0.02570 (14) −0.01030 (13)
S2 0.0615 (4) 0.0452 (4) 0.0818 (5) −0.0050 (3) 0.0489 (4) −0.0158 (3)
S1 0.0980 (6) 0.0474 (4) 0.1073 (6) −0.0094 (4) 0.0828 (5) −0.0144 (4)
O1 0.0552 (10) 0.0469 (9) 0.0563 (10) −0.0054 (7) 0.0336 (8) −0.0133 (8)
O2 0.0590 (11) 0.0696 (13) 0.0804 (13) −0.0178 (9) 0.0454 (10) −0.0342 (10)
O3 0.0683 (11) 0.0439 (9) 0.0703 (12) −0.0069 (8) 0.0403 (10) −0.0053 (9)
O4 0.0626 (12) 0.0881 (16) 0.0874 (15) −0.0211 (11) 0.0405 (11) −0.0213 (12)
N1 0.0440 (10) 0.0412 (10) 0.0481 (10) 0.0014 (8) 0.0252 (9) −0.0018 (9)
N2 0.0474 (11) 0.0409 (10) 0.0433 (10) 0.0041 (8) 0.0218 (9) 0.0028 (8)
N3 0.0473 (11) 0.0462 (11) 0.0446 (10) −0.0001 (9) 0.0233 (9) −0.0041 (9)
N4 0.0487 (11) 0.0396 (10) 0.0472 (11) 0.0025 (8) 0.0279 (9) −0.0029 (8)
C1 0.0328 (11) 0.0457 (13) 0.0402 (11) 0.0035 (9) 0.0154 (9) −0.0033 (10)
C2 0.0432 (12) 0.0420 (12) 0.0429 (12) 0.0009 (9) 0.0202 (10) −0.0027 (10)
C3 0.0412 (12) 0.0375 (12) 0.0477 (12) −0.0010 (9) 0.0204 (10) −0.0025 (10)
C4 0.0742 (18) 0.0493 (14) 0.0653 (16) 0.0050 (13) 0.0456 (15) −0.0022 (13)
C5 0.080 (2) 0.073 (2) 0.0662 (18) 0.0004 (15) 0.0490 (16) 0.0085 (15)
C6 0.0674 (18) 0.0558 (16) 0.0739 (19) −0.0076 (13) 0.0389 (15) 0.0094 (14)
C7 0.0445 (12) 0.0419 (12) 0.0371 (11) 0.0055 (10) 0.0140 (10) −0.0031 (10)
C8 0.0432 (12) 0.0443 (13) 0.0358 (11) 0.0047 (10) 0.0157 (10) −0.0013 (9)
C9 0.0476 (14) 0.0512 (15) 0.0579 (15) 0.0003 (11) 0.0153 (12) −0.0010 (12)
C10 0.0427 (14) 0.083 (2) 0.0657 (18) −0.0004 (14) 0.0126 (13) 0.0011 (16)
C11 0.0495 (16) 0.090 (2) 0.0579 (16) 0.0248 (15) 0.0144 (13) 0.0093 (16)
C12 0.075 (2) 0.0539 (16) 0.0663 (18) 0.0252 (15) 0.0209 (15) 0.0085 (14)
C13 0.0550 (15) 0.0451 (14) 0.0536 (14) 0.0078 (11) 0.0145 (12) −0.0023 (12)
C14 0.0591 (15) 0.0446 (13) 0.0481 (13) 0.0048 (11) 0.0258 (12) 0.0084 (11)
C15 0.0572 (14) 0.0372 (12) 0.0530 (14) 0.0043 (10) 0.0309 (12) −0.0026 (10)
C16 0.0573 (15) 0.0509 (15) 0.0557 (14) 0.0048 (12) 0.0277 (13) −0.0016 (12)
C17 0.0568 (17) 0.080 (2) 0.0663 (18) 0.0095 (15) 0.0166 (15) −0.0163 (16)
C18 0.0609 (19) 0.083 (2) 0.113 (3) −0.0150 (17) 0.045 (2) −0.037 (2)
C19 0.085 (2) 0.0617 (19) 0.115 (3) −0.0185 (17) 0.066 (2) −0.0185 (19)
C20 0.079 (2) 0.0470 (15) 0.0763 (18) −0.0002 (13) 0.0483 (16) 0.0032 (13)
C21 0.0447 (12) 0.0476 (13) 0.0416 (12) −0.0001 (10) 0.0198 (10) −0.0043 (10)
C22 0.0472 (12) 0.0414 (12) 0.0390 (11) 0.0047 (10) 0.0240 (10) 0.0021 (9)
C23 0.0489 (14) 0.0550 (15) 0.0448 (13) −0.0050 (11) 0.0210 (11) −0.0044 (11)
C24 0.082 (2) 0.0624 (17) 0.0602 (16) −0.0189 (15) 0.0406 (15) −0.0195 (14)
C25 0.111 (3) 0.082 (2) 0.072 (2) −0.044 (2) 0.037 (2) −0.0325 (18)
C26 0.076 (2) 0.110 (3) 0.088 (2) −0.046 (2) 0.032 (2) −0.019 (2)
C27 0.0567 (14) 0.0395 (12) 0.0550 (14) 0.0068 (10) 0.0316 (12) −0.0018 (11)
C28 0.0561 (14) 0.0446 (13) 0.0512 (13) −0.0004 (11) 0.0290 (12) −0.0095 (11)
C29 0.0671 (19) 0.098 (2) 0.0580 (17) 0.0151 (17) 0.0262 (15) −0.0092 (17)
C30 0.084 (2) 0.122 (3) 0.0528 (18) 0.013 (2) 0.0128 (17) −0.0080 (19)
C31 0.112 (3) 0.101 (3) 0.0537 (17) −0.017 (2) 0.040 (2) −0.0148 (18)
C32 0.104 (3) 0.093 (2) 0.074 (2) −0.003 (2) 0.062 (2) −0.0129 (19)
C33 0.0751 (19) 0.0673 (18) 0.0683 (17) 0.0095 (15) 0.0461 (15) 0.0000 (14)
C34 0.0550 (14) 0.0404 (12) 0.0544 (13) −0.0022 (10) 0.0366 (12) −0.0017 (11)
C35 0.0531 (14) 0.0383 (12) 0.0527 (13) −0.0045 (10) 0.0305 (12) −0.0040 (10)
C36 0.0674 (17) 0.0714 (18) 0.0568 (15) 0.0016 (14) 0.0353 (14) −0.0061 (14)
C37 0.086 (2) 0.095 (3) 0.0522 (17) 0.0030 (19) 0.0257 (17) −0.0060 (16)
C38 0.069 (2) 0.076 (2) 0.071 (2) 0.0052 (16) 0.0100 (17) −0.0041 (16)
C39 0.0589 (19) 0.097 (3) 0.087 (2) 0.0159 (17) 0.0274 (18) −0.005 (2)
C40 0.0599 (17) 0.079 (2) 0.0643 (17) 0.0119 (14) 0.0345 (15) −0.0024 (14)

Geometric parameters (Å, °)

Cu—O1 1.9269 (16) C15—C16 1.379 (4)
Cu—S1 2.2128 (8) C15—C20 1.389 (4)
O1—C1 1.257 (3) C16—C17 1.388 (4)
N1—C1 1.338 (3) C16—H16 0.93
Cu—O2 1.9230 (18) C17—C18 1.373 (5)
Cu—S2 2.2272 (7) C17—H17 0.93
S1—C2 1.726 (2) C18—C19 1.369 (5)
S2—C22 1.730 (2) C18—H18 0.93
O2—C21 1.256 (3) C19—C20 1.367 (5)
O3—C6 1.353 (3) C19—H19 0.93
O3—C3 1.369 (3) C20—H20 0.93
O4—C23 1.362 (3) C21—C23 1.462 (3)
O4—C26 1.364 (4) C23—C24 1.342 (4)
N1—C2 1.332 (3) C24—C25 1.412 (4)
N2—C2 1.349 (3) C24—H24 0.93
N2—C14 1.463 (3) C25—C26 1.322 (5)
N2—C7 1.472 (3) C25—H25 0.93
N3—C21 1.326 (3) C26—H26 0.93
N3—C22 1.342 (3) C27—C28 1.508 (3)
N4—C22 1.342 (3) C27—H27A 0.97
N4—C34 1.470 (3) C27—H27B 0.97
N4—C27 1.474 (3) C28—C29 1.366 (4)
C1—C3 1.462 (3) C28—C33 1.380 (4)
C3—C4 1.341 (3) C29—C30 1.397 (4)
C4—C5 1.425 (4) C29—H29 0.93
C4—H4 0.93 C30—C31 1.364 (5)
C5—C6 1.325 (4) C30—H30 0.93
C5—H5 0.93 C31—C32 1.358 (5)
C6—H6 0.93 C31—H31 0.93
C7—C8 1.506 (3) C32—C33 1.388 (4)
C7—H7A 0.97 C32—H32 0.93
C7—H7B 0.97 C33—H33 0.93
C8—C13 1.376 (3) C34—C35 1.509 (3)
C8—C9 1.384 (3) C34—H34A 0.97
C9—C10 1.379 (4) C34—H34B 0.97
C9—H9 0.93 C35—C40 1.379 (4)
C10—C11 1.376 (4) C35—C36 1.376 (3)
C10—H10 0.93 C36—C37 1.381 (4)
C11—C12 1.372 (4) C36—H36 0.93
C11—H11 0.93 C37—C38 1.370 (5)
C12—C13 1.380 (4) C37—H37 0.93
C12—H12 0.93 C38—C39 1.365 (5)
C13—H13 0.93 C38—H38 0.93
C14—C15 1.513 (4) C39—C40 1.382 (5)
C14—H14A 0.97 C39—H39 0.93
C14—H14B 0.97 C40—H40 0.93
O2—Cu—O1 89.08 (7) C16—C17—H17 119.9
O2—Cu—S1 163.52 (7) C19—C18—C17 119.6 (3)
O1—Cu—S1 93.68 (5) C19—C18—H18 120.2
O2—Cu—S2 94.35 (5) C17—C18—H18 120.2
O1—Cu—S2 166.02 (6) C18—C19—C20 120.4 (3)
S1—Cu—S2 86.86 (2) C18—C19—H19 119.8
C22—S2—Cu 107.99 (8) C20—C19—H19 119.8
C2—S1—Cu 108.45 (8) C19—C20—C15 121.1 (3)
C1—O1—Cu 131.58 (15) C19—C20—H20 119.4
C21—O2—Cu 130.97 (16) C15—C20—H20 119.4
C6—O3—C3 106.3 (2) O2—C21—N3 131.1 (2)
C23—O4—C26 105.7 (2) O2—C21—C23 115.7 (2)
C2—N1—C1 124.29 (19) N3—C21—C23 113.0 (2)
C2—N2—C14 122.62 (19) N3—C22—N4 115.52 (19)
C2—N2—C7 122.24 (19) N3—C22—S2 127.25 (17)
C14—N2—C7 114.91 (19) N4—C22—S2 117.15 (17)
C21—N3—C22 125.4 (2) C24—C23—O4 110.3 (2)
C22—N4—C34 124.03 (19) C24—C23—C21 131.5 (2)
C22—N4—C27 122.60 (19) O4—C23—C21 118.1 (2)
C34—N4—C27 113.32 (18) C23—C24—C25 106.4 (3)
O1—C1—N1 130.5 (2) C23—C24—H24 126.8
O1—C1—C3 116.3 (2) C25—C24—H24 126.8
N1—C1—C3 113.16 (19) C26—C25—C24 106.8 (3)
N1—C2—N2 116.5 (2) C26—C25—H25 126.6
N1—C2—S1 128.01 (18) C24—C25—H25 126.6
N2—C2—S1 115.40 (17) C25—C26—O4 110.9 (3)
C4—C3—O3 109.6 (2) C25—C26—H26 124.5
C4—C3—C1 133.4 (2) O4—C26—H26 124.5
O3—C3—C1 116.99 (19) N4—C27—C28 112.5 (2)
C3—C4—C5 106.7 (2) N4—C27—H27A 109.1
C3—C4—H4 126.7 C28—C27—H27A 109.1
C5—C4—H4 126.7 N4—C27—H27B 109.1
C6—C5—C4 106.1 (2) C28—C27—H27B 109.1
C6—C5—H5 126.9 H27A—C27—H27B 107.8
C4—C5—H5 126.9 C29—C28—C33 118.3 (3)
C5—C6—O3 111.3 (2) C29—C28—C27 120.6 (2)
C5—C6—H6 124.4 C33—C28—C27 121.1 (2)
O3—C6—H6 124.4 C28—C29—C30 120.8 (3)
N2—C7—C8 114.41 (18) C28—C29—H29 119.6
N2—C7—H7A 108.7 C30—C29—H29 119.6
C8—C7—H7A 108.7 C31—C30—C29 119.9 (3)
N2—C7—H7B 108.7 C31—C30—H30 120.1
C8—C7—H7B 108.7 C29—C30—H30 120.1
H7A—C7—H7B 107.6 C32—C31—C30 120.0 (3)
C13—C8—C9 118.8 (2) C32—C31—H31 120
C13—C8—C7 120.5 (2) C30—C31—H31 120
C9—C8—C7 120.6 (2) C31—C32—C33 120.1 (3)
C10—C9—C8 121.0 (3) C31—C32—H32 120
C10—C9—H9 119.5 C33—C32—H32 120
C8—C9—H9 119.5 C28—C33—C32 120.9 (3)
C11—C10—C9 119.4 (3) C28—C33—H33 119.6
C11—C10—H10 120.3 C32—C33—H33 119.6
C9—C10—H10 120.3 N4—C34—C35 113.34 (19)
C12—C11—C10 120.3 (3) N4—C34—H34A 108.9
C12—C11—H11 119.8 C35—C34—H34A 108.9
C10—C11—H11 119.8 N4—C34—H34B 108.9
C11—C12—C13 119.9 (3) C35—C34—H34B 108.9
C11—C12—H12 120 H34A—C34—H34B 107.7
C13—C12—H12 120 C40—C35—C36 118.2 (3)
C12—C13—C8 120.6 (3) C40—C35—C34 119.9 (2)
C12—C13—H13 119.7 C36—C35—C34 121.9 (2)
C8—C13—H13 119.7 C35—C36—C37 120.7 (3)
N2—C14—C15 115.0 (2) C35—C36—H36 119.6
N2—C14—H14A 108.5 C37—C36—H36 119.6
C15—C14—H14A 108.5 C38—C37—C36 120.5 (3)
N2—C14—H14B 108.5 C38—C37—H37 119.7
C15—C14—H14B 108.5 C36—C37—H37 119.7
H14A—C14—H14B 107.5 C39—C38—C37 119.3 (3)
C16—C15—C20 118.2 (3) C39—C38—H38 120.3
C16—C15—C14 123.7 (2) C37—C38—H38 120.3
C20—C15—C14 118.1 (2) C38—C39—C40 120.3 (3)
C15—C16—C17 120.5 (3) C38—C39—H39 119.9
C15—C16—H16 119.8 C40—C39—H39 119.9
C17—C16—H16 119.8 C35—C40—C39 120.9 (3)
C18—C17—C16 120.2 (3) C35—C40—H40 119.5
C18—C17—H17 119.9 C39—C40—H40 119.5
O2—Cu—S2—C22 −9.59 (11) C15—C16—C17—C18 −0.6 (4)
O1—Cu—S2—C22 94.2 (2) C16—C17—C18—C19 −0.7 (5)
S1—Cu—S2—C22 −173.12 (9) C17—C18—C19—C20 1.1 (5)
O2—Cu—S1—C2 89.5 (2) C18—C19—C20—C15 −0.3 (5)
O1—Cu—S1—C2 −9.81 (11) C16—C15—C20—C19 −0.9 (4)
S2—Cu—S1—C2 −175.82 (9) C14—C15—C20—C19 179.6 (3)
O2—Cu—O1—C1 −168.3 (2) Cu—O2—C21—N3 13.8 (4)
S1—Cu—O1—C1 −4.5 (2) Cu—O2—C21—C23 −170.15 (19)
S2—Cu—O1—C1 87.3 (3) C22—N3—C21—O2 −6.4 (4)
O1—Cu—O2—C21 −169.5 (3) C22—N3—C21—C23 177.5 (2)
S1—Cu—O2—C21 90.5 (3) C21—N3—C22—N4 170.6 (2)
S2—Cu—O2—C21 −3.1 (3) C21—N3—C22—S2 −12.8 (4)
Cu—O1—C1—N1 16.9 (4) C34—N4—C22—N3 175.0 (2)
Cu—O1—C1—C3 −166.58 (16) C27—N4—C22—N3 −2.1 (3)
C2—N1—C1—O1 −8.8 (4) C34—N4—C22—S2 −1.9 (3)
C2—N1—C1—C3 174.5 (2) C27—N4—C22—S2 −179.00 (17)
C1—N1—C2—N2 171.5 (2) Cu—S2—C22—N3 18.8 (2)
C1—N1—C2—S1 −12.3 (3) Cu—S2—C22—N4 −164.70 (15)
C14—N2—C2—N1 178.3 (2) C26—O4—C23—C24 −0.7 (3)
C7—N2—C2—N1 4.1 (3) C26—O4—C23—C21 −177.1 (3)
C14—N2—C2—S1 1.6 (3) O2—C21—C23—C24 −172.0 (3)
C7—N2—C2—S1 −172.62 (16) N3—C21—C23—C24 4.8 (4)
Cu—S1—C2—N1 19.6 (2) O2—C21—C23—O4 3.4 (4)
Cu—S1—C2—N2 −164.11 (15) N3—C21—C23—O4 −179.8 (2)
C6—O3—C3—C4 0.4 (3) O4—C23—C24—C25 0.4 (4)
C6—O3—C3—C1 180.0 (2) C21—C23—C24—C25 176.1 (3)
O1—C1—C3—C4 −176.3 (3) C23—C24—C25—C26 0.1 (4)
N1—C1—C3—C4 0.8 (4) C24—C25—C26—O4 −0.5 (5)
O1—C1—C3—O3 4.2 (3) C23—O4—C26—C25 0.8 (4)
N1—C1—C3—O3 −178.7 (2) C22—N4—C27—C28 103.0 (3)
O3—C3—C4—C5 −0.8 (3) C34—N4—C27—C28 −74.3 (3)
C1—C3—C4—C5 179.7 (3) N4—C27—C28—C29 −56.7 (3)
C3—C4—C5—C6 0.9 (3) N4—C27—C28—C33 124.3 (3)
C4—C5—C6—O3 −0.7 (4) C33—C28—C29—C30 −0.3 (5)
C3—O3—C6—C5 0.2 (3) C27—C28—C29—C30 −179.4 (3)
C2—N2—C7—C8 −109.9 (2) C28—C29—C30—C31 0.7 (6)
C14—N2—C7—C8 75.5 (3) C29—C30—C31—C32 −0.4 (6)
N2—C7—C8—C13 −112.8 (3) C30—C31—C32—C33 −0.4 (6)
N2—C7—C8—C9 71.2 (3) C29—C28—C33—C32 −0.4 (5)
C13—C8—C9—C10 −0.4 (4) C27—C28—C33—C32 178.6 (3)
C7—C8—C9—C10 175.6 (2) C31—C32—C33—C28 0.8 (5)
C8—C9—C10—C11 −0.1 (4) C22—N4—C34—C35 101.4 (3)
C9—C10—C11—C12 0.5 (5) C27—N4—C34—C35 −81.2 (2)
C10—C11—C12—C13 −0.4 (5) N4—C34—C35—C40 114.7 (3)
C11—C12—C13—C8 −0.1 (4) N4—C34—C35—C36 −66.7 (3)
C9—C8—C13—C12 0.5 (4) C40—C35—C36—C37 −0.5 (4)
C7—C8—C13—C12 −175.5 (2) C34—C35—C36—C37 −179.1 (3)
C2—N2—C14—C15 −84.6 (3) C35—C36—C37—C38 0.6 (5)
C7—N2—C14—C15 89.9 (2) C36—C37—C38—C39 −0.5 (6)
N2—C14—C15—C16 5.7 (3) C37—C38—C39—C40 0.3 (6)
N2—C14—C15—C20 −174.8 (2) C36—C35—C40—C39 0.2 (5)
C20—C15—C16—C17 1.4 (4) C34—C35—C40—C39 178.9 (3)
C14—C15—C16—C17 −179.1 (2) C38—C39—C40—C35 −0.2 (5)

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: BT5517).

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 global, I. DOI: 10.1107/S160053681101422X/bt5517sup1.cif

e-67-0m621-sup1.cif (29.2KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S160053681101422X/bt5517Isup2.hkl

e-67-0m621-Isup2.hkl (355.4KB, hkl)

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


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