Skip to main content
Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2010 Sep 15;66(Pt 10):m1255. doi: 10.1107/S1600536810036135

Aqua­{N-[(4-methyl­phen­yl)sulfon­yl]glycinato(2−)-κ2 N,O}(1,10-phenan­throline)copper(II)

Miao-Ling Huang a,*
PMCID: PMC2983433  PMID: 21587403

Abstract

In the title complex, [Cu(C9H9NO4S)(C12H8N2)(H2O)], the CuII ion is coordinated in a distorted square-pyramidal geometry by the two N atoms from a 1,10-phenanthroline ligand, one N atom from the deprotonated amino group of an N-tosyl­glycinate ligand, one O atom from the carboxyl­ate part of the N-tosyl­glycinate ligand and a water O atom. Inter­molecular O—H⋯O hydrogen bonds involving the water H atoms link neighboring mol­ecules into supra­molecular chains along [010]. Weak π–π stacking inter­actions [centroid–centroid distances of 3.456 (1) and 3.691 (1) Å] between the benzene rings of 1,10-phenanthroline ligands of adjacent mol­ecules extend the chains into a layer structure parallel to (001).

Related literature

For the coordination chemistry of N-sulfonyl amino acids, see: Liang et al. (2004); Ma et al. (2008). For related structures, see: Battaglia et al. (1983); Antolini et al. (1985); Menabue & Saladini (1991).graphic file with name e-66-m1255-scheme1.jpg

Experimental

Crystal data

  • [Cu(C9H9NO4S)(C12H8N2)(H2O)]

  • M r = 488.99

  • Monoclinic, Inline graphic

  • a = 14.0788 (11) Å

  • b = 7.0588 (6) Å

  • c = 20.6993 (17) Å

  • β = 103.826 (1)°

  • V = 1997.5 (3) Å3

  • Z = 4

  • Mo Kα radiation

  • μ = 1.24 mm−1

  • T = 296 K

  • 0.32 × 0.29 × 0.25 mm

Data collection

  • Bruker SMART CCD area-detector diffractometer

  • Absorption correction: multi-scan (SADABS; Sheldrick, 2003) T min = 0.693, T max = 0.747

  • 14609 measured reflections

  • 3713 independent reflections

  • 3341 reflections with I > 2σ(I)

  • R int = 0.019

Refinement

  • R[F 2 > 2σ(F 2)] = 0.024

  • wR(F 2) = 0.065

  • S = 1.06

  • 3713 reflections

  • 281 parameters

  • H-atom parameters constrained

  • Δρmax = 0.27 e Å−3

  • Δρmin = −0.30 e Å−3

Data collection: SMART (Bruker, 2001); cell refinement: SAINT (Bruker, 2003); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: SHELXTL (Sheldrick, 2008); software used to prepare material for publication: SHELXTL.

Supplementary Material

Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536810036135/zq2057sup1.cif

e-66-m1255-sup1.cif (23.4KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536810036135/zq2057Isup2.hkl

e-66-m1255-Isup2.hkl (182.1KB, hkl)

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

Table 1. Hydrogen-bond geometry (Å, °).

D—H⋯A D—H H⋯A DA D—H⋯A
O5—H1W⋯O2i 0.85 1.87 2.717 (2) 175
O5—H2W⋯O4ii 0.85 2.00 2.847 (2) 174

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

Acknowledgments

This work was supported by the Education Department Foundation of Fujian Province of China (grant No. 2008 F5053) and the Master Construction Project of Quanzhou Normal University.

supplementary crystallographic information

Comment

As a kind of amino acid derivatives, the N-protected amino acid plays an important role in participating in the process of the life activity. The substitution of an Ar—SO2-group on the amine nitrogen of amino acids, such as glycine and B-alanine, increases the coordination donors behavior of amino acids to three types of O, N donors from carboxyl, sulfoxyl and amine respectively, which may lead to different coordination modes, thus is of great interest in studying the coordination chemistry of N-sulfonyl- amino acids for many chemical workers (Ma et al., 2008; Liang et al., 2004; Battaglia et al., 1983; Menabue et al., 1991; Antolini et al., 1985). In order to continue the research, we synthesized the title complex [Cu(C9H9NO4S)(C12H8N2)(H2O)] and characterized it by an elemental analysis and a single-crystal X-ray diffraction analysis.

The molecular structure and crystal packing diagram of the title compound are presented in Figs. 1 and 2, respectively. The asymmetric unit contains one copper cation, one Ts-gly anion, one phen molecule and one coordinated water molecule. The central copper ion adopts a distorted square-pyramidal geometry by two N(N2, N3) atoms of the 1,10-phenanthroline ligand, one N(N1) and one O(O1) atoms of the Ts-gly ion occupying basal site, while the apical position is occupied by another O atom of a water molecule. The Cu—O1 bond distance of 1.9269 (13) Å is shorter than those of other N-protected glycine complexes (1.933–1.967 Å) [Battaglia, et al., 1983; Antolini, et al., 1985; Menabue & Saladini, 1991]. Furthermore, the C—O bond distance for the coordinated O atom (1.282 (2) Å) is significantly longer than that for the uncoordinated O atom (1.233 (2) Å), which is similar to previously reported complexes (Battaglia, et al., 1983; Antolini, et al., 1985).

Intermolecular hydrogen bonds involving the water H atoms, O(5)—H(1W)···O(2)i, O(5)—H(2W)···O(4)ii (Table 1), link the neighboring molecules into one-dimensional supramolecular chains. Weak π-π stacking interactions between benzene rings of 1,10-phenanthroline ligands from adjacent molecules (centroid distances of 3.456Å and 3.691 Å) extend the one-dimensional chains into a two-dimensional layer structure.

Experimental

To a solution of Ts-gly (1 mmol) in water-DMF 1:1 (10 ml), an aqueous solution (5 ml) of CuCl2.2H2O (1 mmol) and a solution of 1,10-phenanthroline (1 mmol) in ethanol (95%, 5 ml) was added. After refluxing for 12 h at 343 K, the mixture was filtered off while hot. The green single crystals suitable for a X-ray analysis were obtained by slow evaporation of the filtrate at room temperature after 41 days. IR(KBr): 3442(vs), 1638(vs), 1586(s), 1518(s), 1493(m), 1434(s), 1382(vs), 1348(m), 1319(m), 1243(vs), 1132(vs), 1112(vs), 1078(s), 1007(s), 967(s), 940(m), 847(s), 820(m), 723(s),663(s), 589(s), 545(m) cm-1.

Refinement

H atoms bonded to C were placed geometrically and treated as riding with C—H = 0.93–0.97 Å and Uiso(H) = 1.2Ueq(C). The water H atoms were found in difference Fourier maps and refined with O—H = 0.85 Å and Uiso(H) = 1.5Ueq(O).

Figures

Fig. 1.

Fig. 1.

The molecular structure of the title compound. Displacement ellipsoids are drawn at the 30% probability level. All hydrogen atoms have been omitted for clarity reasons.

Fig. 2.

Fig. 2.

Projection showing the two-dimensional structure of the title compound formed by the intermolecular hydrogen bonds and the π-π stacking interactions.

Crystal data

[Cu(C9H9NO4S)(C12H8N2)(H2O)] F(000) = 1004
Mr = 488.99 Dx = 1.626 Mg m3
Monoclinic, P21/c Mo Kα radiation, λ = 0.71073 Å
a = 14.0788 (11) Å Cell parameters from 7260 reflections
b = 7.0588 (6) Å θ = 2.8–28.2°
c = 20.6993 (17) Å µ = 1.24 mm1
β = 103.826 (1)° T = 296 K
V = 1997.5 (3) Å3 Block, green
Z = 4 0.32 × 0.29 × 0.25 mm

Data collection

Bruker SMART CCD area-detector diffractometer 3713 independent reflections
Radiation source: fine-focus sealed tube 3341 reflections with I > 2σ(I)
graphite Rint = 0.019
φ and ω scans θmax = 25.5°, θmin = 2.8°
Absorption correction: multi-scan (SADABS; Sheldrick, 2003) h = −17→16
Tmin = 0.693, Tmax = 0.747 k = −8→8
14609 measured reflections l = −25→25

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)] = 0.024 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.065 H-atom parameters constrained
S = 1.06 w = 1/[σ2(Fo2) + (0.0287P)2 + 1.2801P] where P = (Fo2 + 2Fc2)/3
3713 reflections (Δ/σ)max = 0.001
281 parameters Δρmax = 0.27 e Å3
0 restraints Δρmin = −0.30 e Å3

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 takeninto account individually in the estimation of e.s.d.'s in distances, anglesand torsion angles; correlations between e.s.d.'s in cell parameters are onlyused 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
Cu1 0.245571 (16) 0.54423 (3) 0.471642 (10) 0.02714 (8)
S1 0.24891 (3) 0.25311 (7) 0.34767 (2) 0.02718 (12)
O1 0.35227 (10) 0.4521 (2) 0.54106 (6) 0.0376 (3)
O2 0.49352 (10) 0.2987 (2) 0.55995 (7) 0.0408 (4)
O3 0.14652 (10) 0.3036 (2) 0.32547 (7) 0.0402 (4)
O4 0.26947 (12) 0.0512 (2) 0.34674 (7) 0.0403 (4)
O5 0.32853 (10) 0.8041 (2) 0.45785 (8) 0.0430 (4)
H1W 0.3856 0.7738 0.4546 0.064*
H2W 0.3065 0.8774 0.4251 0.064*
N1 0.29113 (11) 0.3460 (2) 0.41754 (7) 0.0278 (4)
N2 0.17697 (11) 0.6304 (2) 0.54314 (7) 0.0277 (3)
N3 0.12245 (11) 0.6608 (2) 0.41228 (7) 0.0295 (4)
C1 0.41586 (13) 0.3491 (3) 0.52244 (9) 0.0282 (4)
C2 0.39262 (13) 0.2906 (3) 0.45023 (9) 0.0296 (4)
H2A 0.4378 0.3513 0.4280 0.036*
H2B 0.4000 0.1545 0.4470 0.036*
C3 0.30947 (13) 0.3556 (3) 0.28982 (9) 0.0270 (4)
C4 0.32266 (16) 0.2503 (3) 0.23598 (10) 0.0377 (5)
H4 0.3025 0.1246 0.2312 0.045*
C5 0.36591 (16) 0.3329 (4) 0.18939 (10) 0.0428 (5)
H5A 0.3745 0.2615 0.1534 0.051*
C6 0.39666 (15) 0.5203 (3) 0.19541 (10) 0.0398 (5)
C7 0.38440 (16) 0.6220 (3) 0.25016 (11) 0.0417 (5)
H7 0.4056 0.7471 0.2554 0.050*
C8 0.34130 (15) 0.5416 (3) 0.29733 (10) 0.0354 (5)
H8 0.3339 0.6122 0.3337 0.042*
C9 0.4445 (2) 0.6079 (5) 0.14447 (13) 0.0597 (7)
H9A 0.4000 0.6037 0.1014 0.090*
H9B 0.5027 0.5383 0.1433 0.090*
H9C 0.4613 0.7372 0.1564 0.090*
C10 0.20889 (15) 0.6202 (3) 0.60898 (9) 0.0345 (5)
H10 0.2727 0.5803 0.6270 0.041*
C11 0.14933 (17) 0.6676 (3) 0.65179 (10) 0.0407 (5)
H11 0.1738 0.6595 0.6976 0.049*
C12 0.05523 (16) 0.7258 (3) 0.62636 (11) 0.0376 (5)
H12 0.0151 0.7554 0.6547 0.045*
C13 0.01946 (14) 0.7407 (3) 0.55693 (10) 0.0304 (4)
C14 −0.07680 (15) 0.8059 (3) 0.52450 (11) 0.0371 (5)
H14 −0.1209 0.8361 0.5500 0.044*
C15 −0.10434 (14) 0.8240 (3) 0.45780 (11) 0.0373 (5)
H15 −0.1672 0.8662 0.4381 0.045*
C16 −0.03842 (14) 0.7795 (3) 0.41629 (10) 0.0318 (4)
C17 −0.05995 (16) 0.8052 (3) 0.34695 (11) 0.0405 (5)
H17 −0.1213 0.8484 0.3243 0.049*
C18 0.00994 (17) 0.7661 (4) 0.31331 (11) 0.0449 (6)
H18 −0.0027 0.7878 0.2677 0.054*
C19 0.10062 (16) 0.6933 (3) 0.34718 (10) 0.0394 (5)
H19 0.1472 0.6667 0.3233 0.047*
C20 0.05477 (13) 0.7091 (3) 0.44656 (9) 0.0265 (4)
C21 0.08421 (13) 0.6912 (3) 0.51756 (9) 0.0255 (4)

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
Cu1 0.02506 (13) 0.03777 (15) 0.01906 (12) 0.00538 (10) 0.00617 (9) 0.00056 (9)
S1 0.0249 (2) 0.0364 (3) 0.0212 (2) −0.00450 (19) 0.00735 (18) −0.00286 (19)
O1 0.0349 (8) 0.0548 (10) 0.0217 (7) 0.0140 (7) 0.0039 (6) −0.0026 (6)
O2 0.0281 (7) 0.0573 (10) 0.0331 (8) 0.0079 (7) 0.0001 (6) 0.0035 (7)
O3 0.0231 (7) 0.0672 (11) 0.0296 (7) −0.0047 (7) 0.0052 (6) −0.0070 (7)
O4 0.0549 (9) 0.0337 (8) 0.0325 (8) −0.0083 (7) 0.0112 (7) −0.0030 (6)
O5 0.0338 (8) 0.0421 (9) 0.0539 (10) −0.0004 (7) 0.0121 (7) 0.0114 (7)
N1 0.0222 (8) 0.0404 (10) 0.0206 (8) 0.0022 (7) 0.0048 (6) −0.0032 (7)
N2 0.0301 (8) 0.0303 (9) 0.0240 (8) 0.0005 (7) 0.0087 (6) −0.0003 (7)
N3 0.0291 (8) 0.0365 (9) 0.0230 (8) 0.0037 (7) 0.0068 (6) 0.0020 (7)
C1 0.0259 (10) 0.0330 (11) 0.0259 (9) −0.0018 (8) 0.0065 (8) 0.0036 (8)
C2 0.0245 (9) 0.0353 (11) 0.0291 (10) 0.0014 (8) 0.0066 (8) −0.0037 (8)
C3 0.0229 (9) 0.0372 (11) 0.0210 (9) −0.0001 (8) 0.0056 (7) −0.0006 (8)
C4 0.0428 (12) 0.0423 (12) 0.0310 (11) −0.0082 (10) 0.0146 (9) −0.0100 (9)
C5 0.0451 (13) 0.0600 (15) 0.0283 (11) −0.0037 (11) 0.0185 (9) −0.0091 (10)
C6 0.0317 (11) 0.0587 (15) 0.0313 (11) −0.0005 (10) 0.0120 (9) 0.0079 (10)
C7 0.0460 (13) 0.0399 (12) 0.0413 (12) −0.0065 (10) 0.0145 (10) 0.0042 (10)
C8 0.0403 (11) 0.0390 (12) 0.0296 (10) −0.0014 (9) 0.0134 (9) −0.0039 (9)
C9 0.0604 (16) 0.0773 (19) 0.0500 (15) −0.0056 (14) 0.0299 (13) 0.0149 (14)
C10 0.0370 (11) 0.0415 (12) 0.0248 (10) 0.0012 (9) 0.0071 (8) −0.0007 (9)
C11 0.0521 (13) 0.0482 (13) 0.0248 (10) 0.0024 (11) 0.0150 (9) −0.0014 (9)
C12 0.0460 (13) 0.0381 (12) 0.0365 (11) −0.0029 (10) 0.0252 (10) −0.0042 (9)
C13 0.0338 (10) 0.0249 (10) 0.0369 (11) −0.0049 (8) 0.0172 (9) −0.0036 (8)
C14 0.0315 (11) 0.0321 (11) 0.0542 (14) −0.0019 (9) 0.0233 (10) −0.0034 (10)
C15 0.0228 (10) 0.0334 (11) 0.0560 (14) 0.0005 (8) 0.0098 (9) −0.0008 (10)
C16 0.0266 (10) 0.0263 (10) 0.0406 (11) −0.0018 (8) 0.0044 (8) −0.0014 (8)
C17 0.0322 (11) 0.0408 (12) 0.0415 (12) 0.0042 (9) −0.0051 (9) 0.0015 (10)
C18 0.0475 (13) 0.0553 (15) 0.0266 (11) 0.0079 (11) −0.0017 (9) 0.0049 (10)
C19 0.0413 (12) 0.0509 (13) 0.0262 (10) 0.0083 (10) 0.0087 (9) 0.0037 (9)
C20 0.0263 (9) 0.0237 (9) 0.0299 (10) −0.0018 (7) 0.0075 (8) −0.0010 (8)
C21 0.0272 (9) 0.0225 (9) 0.0287 (9) −0.0029 (7) 0.0101 (8) −0.0017 (7)

Geometric parameters (Å, °)

Cu1—O1 1.9269 (13) C6—C9 1.512 (3)
Cu1—N1 1.9916 (16) C7—C8 1.388 (3)
Cu1—N3 2.0429 (16) C7—H7 0.9300
Cu1—N2 2.0435 (15) C8—H8 0.9300
Cu1—O5 2.2296 (15) C9—H9A 0.9600
S1—O3 1.4490 (14) C9—H9B 0.9600
S1—O4 1.4557 (16) C9—H9C 0.9600
S1—N1 1.5697 (15) C10—C11 1.398 (3)
S1—C3 1.7812 (19) C10—H10 0.9300
O1—C1 1.282 (2) C11—C12 1.367 (3)
O2—C1 1.233 (2) C11—H11 0.9300
O5—H1W 0.8499 C12—C13 1.409 (3)
O5—H2W 0.8500 C12—H12 0.9300
N1—C2 1.480 (2) C13—C21 1.404 (3)
N2—C10 1.331 (2) C13—C14 1.437 (3)
N2—C21 1.356 (2) C14—C15 1.348 (3)
N3—C19 1.329 (2) C14—H14 0.9300
N3—C20 1.360 (2) C15—C16 1.442 (3)
C1—C2 1.509 (3) C15—H15 0.9300
C2—H2A 0.9700 C16—C20 1.403 (3)
C2—H2B 0.9700 C16—C17 1.406 (3)
C3—C8 1.384 (3) C17—C18 1.363 (3)
C3—C4 1.389 (3) C17—H17 0.9300
C4—C5 1.386 (3) C18—C19 1.399 (3)
C4—H4 0.9300 C18—H18 0.9300
C5—C6 1.388 (3) C19—H19 0.9300
C5—H5A 0.9300 C20—C21 1.434 (3)
C6—C7 1.387 (3)
O1—Cu1—N1 83.32 (6) C5—C6—C9 120.5 (2)
O1—Cu1—N3 169.34 (6) C6—C7—C8 121.6 (2)
N1—Cu1—N3 106.60 (6) C6—C7—H7 119.2
O1—Cu1—N2 88.83 (6) C8—C7—H7 119.2
N1—Cu1—N2 152.58 (7) C3—C8—C7 119.55 (19)
N3—Cu1—N2 80.56 (6) C3—C8—H8 120.2
O1—Cu1—O5 91.97 (6) C7—C8—H8 120.2
N1—Cu1—O5 104.91 (6) C6—C9—H9A 109.5
N3—Cu1—O5 89.24 (6) C6—C9—H9B 109.5
N2—Cu1—O5 101.57 (6) H9A—C9—H9B 109.5
O3—S1—O4 114.99 (9) C6—C9—H9C 109.5
O3—S1—N1 108.57 (8) H9A—C9—H9C 109.5
O4—S1—N1 112.86 (9) H9B—C9—H9C 109.5
O3—S1—C3 106.66 (9) N2—C10—C11 121.93 (19)
O4—S1—C3 105.09 (9) N2—C10—H10 119.0
N1—S1—C3 108.24 (9) C11—C10—H10 119.0
C1—O1—Cu1 116.31 (12) C12—C11—C10 120.06 (19)
Cu1—O5—H1W 109.7 C12—C11—H11 120.0
Cu1—O5—H2W 120.0 C10—C11—H11 120.0
H1W—O5—H2W 105.2 C11—C12—C13 119.51 (18)
C2—N1—S1 114.99 (12) C11—C12—H12 120.2
C2—N1—Cu1 109.52 (11) C13—C12—H12 120.2
S1—N1—Cu1 135.20 (9) C21—C13—C12 116.76 (18)
C10—N2—C21 118.35 (16) C21—C13—C14 118.63 (18)
C10—N2—Cu1 128.54 (14) C12—C13—C14 124.61 (18)
C21—N2—Cu1 112.89 (12) C15—C14—C13 121.15 (19)
C19—N3—C20 117.69 (17) C15—C14—H14 119.4
C19—N3—Cu1 129.57 (14) C13—C14—H14 119.4
C20—N3—Cu1 112.74 (12) C14—C15—C16 121.40 (19)
O2—C1—O1 123.55 (18) C14—C15—H15 119.3
O2—C1—C2 119.62 (17) C16—C15—H15 119.3
O1—C1—C2 116.82 (16) C20—C16—C17 116.87 (18)
N1—C2—C1 109.72 (15) C20—C16—C15 118.53 (19)
N1—C2—H2A 109.7 C17—C16—C15 124.58 (19)
C1—C2—H2A 109.7 C18—C17—C16 119.32 (19)
N1—C2—H2B 109.7 C18—C17—H17 120.3
C1—C2—H2B 109.7 C16—C17—H17 120.3
H2A—C2—H2B 108.2 C17—C18—C19 120.1 (2)
C8—C3—C4 119.75 (18) C17—C18—H18 119.9
C8—C3—S1 120.27 (14) C19—C18—H18 119.9
C4—C3—S1 119.96 (16) N3—C19—C18 122.3 (2)
C5—C4—C3 119.9 (2) N3—C19—H19 118.9
C5—C4—H4 120.1 C18—C19—H19 118.9
C3—C4—H4 120.1 N3—C20—C16 123.56 (17)
C4—C5—C6 121.2 (2) N3—C20—C21 116.46 (16)
C4—C5—H5A 119.4 C16—C20—C21 119.94 (17)
C6—C5—H5A 119.4 N2—C21—C13 123.37 (17)
C7—C6—C5 118.00 (19) N2—C21—C20 116.33 (16)
C7—C6—C9 121.4 (2) C13—C21—C20 120.28 (17)
N1—Cu1—O1—C1 15.55 (14) S1—C3—C4—C5 177.14 (16)
N3—Cu1—O1—C1 174.4 (3) C3—C4—C5—C6 0.0 (3)
N2—Cu1—O1—C1 169.23 (15) C4—C5—C6—C7 1.1 (3)
O5—Cu1—O1—C1 −89.23 (15) C4—C5—C6—C9 179.5 (2)
O3—S1—N1—C2 173.74 (14) C5—C6—C7—C8 −1.1 (3)
O4—S1—N1—C2 45.04 (16) C9—C6—C7—C8 −179.4 (2)
C3—S1—N1—C2 −70.84 (16) C4—C3—C8—C7 1.3 (3)
O3—S1—N1—Cu1 −13.30 (17) S1—C3—C8—C7 −177.10 (16)
O4—S1—N1—Cu1 −142.00 (13) C6—C7—C8—C3 −0.1 (3)
C3—S1—N1—Cu1 102.13 (14) C21—N2—C10—C11 0.9 (3)
O1—Cu1—N1—C2 −18.70 (12) Cu1—N2—C10—C11 −173.35 (16)
N3—Cu1—N1—C2 165.30 (12) N2—C10—C11—C12 0.3 (3)
N2—Cu1—N1—C2 −93.00 (17) C10—C11—C12—C13 −1.1 (3)
O5—Cu1—N1—C2 71.57 (13) C11—C12—C13—C21 0.8 (3)
O1—Cu1—N1—S1 168.06 (15) C11—C12—C13—C14 −177.9 (2)
N3—Cu1—N1—S1 −7.94 (16) C21—C13—C14—C15 −1.6 (3)
N2—Cu1—N1—S1 93.76 (18) C12—C13—C14—C15 177.1 (2)
O5—Cu1—N1—S1 −101.67 (14) C13—C14—C15—C16 −0.2 (3)
O1—Cu1—N2—C10 2.40 (18) C14—C15—C16—C20 2.4 (3)
N1—Cu1—N2—C10 75.4 (2) C14—C15—C16—C17 −176.2 (2)
N3—Cu1—N2—C10 −176.63 (19) C20—C16—C17—C18 −1.6 (3)
O5—Cu1—N2—C10 −89.37 (18) C15—C16—C17—C18 177.0 (2)
O1—Cu1—N2—C21 −172.10 (14) C16—C17—C18—C19 2.8 (4)
N1—Cu1—N2—C21 −99.09 (17) C20—N3—C19—C18 −3.0 (3)
N3—Cu1—N2—C21 8.87 (13) Cu1—N3—C19—C18 176.61 (17)
O5—Cu1—N2—C21 96.13 (13) C17—C18—C19—N3 −0.4 (4)
O1—Cu1—N3—C19 166.8 (3) C19—N3—C20—C16 4.2 (3)
N1—Cu1—N3—C19 −35.2 (2) Cu1—N3—C20—C16 −175.48 (15)
N2—Cu1—N3—C19 172.0 (2) C19—N3—C20—C21 −173.60 (18)
O5—Cu1—N3—C19 70.10 (19) Cu1—N3—C20—C21 6.7 (2)
O1—Cu1—N3—C20 −13.6 (4) C17—C16—C20—N3 −1.9 (3)
N1—Cu1—N3—C20 144.41 (13) C15—C16—C20—N3 179.39 (18)
N2—Cu1—N3—C20 −8.39 (13) C17—C16—C20—C21 175.84 (18)
O5—Cu1—N3—C20 −110.25 (13) C15—C16—C20—C21 −2.9 (3)
Cu1—O1—C1—O2 171.25 (16) C10—N2—C21—C13 −1.2 (3)
Cu1—O1—C1—C2 −8.1 (2) Cu1—N2—C21—C13 173.90 (14)
S1—N1—C2—C1 −166.30 (13) C10—N2—C21—C20 176.91 (17)
Cu1—N1—C2—C1 18.95 (19) Cu1—N2—C21—C20 −8.0 (2)
O2—C1—C2—N1 172.71 (18) C12—C13—C21—N2 0.4 (3)
O1—C1—C2—N1 −7.9 (2) C14—C13—C21—N2 179.15 (18)
O3—S1—C3—C8 85.06 (17) C12—C13—C21—C20 −177.67 (18)
O4—S1—C3—C8 −152.43 (16) C14—C13—C21—C20 1.1 (3)
N1—S1—C3—C8 −31.60 (19) N3—C20—C21—N2 0.9 (3)
O3—S1—C3—C4 −93.29 (18) C16—C20—C21—N2 −177.04 (17)
O4—S1—C3—C4 29.22 (19) N3—C20—C21—C13 179.05 (17)
N1—S1—C3—C4 150.05 (16) C16—C20—C21—C13 1.2 (3)
C8—C3—C4—C5 −1.2 (3)

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
O5—H1W···O2i 0.85 1.87 2.717 (2) 175
O5—H2W···O4ii 0.85 2.00 2.847 (2) 174

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

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: ZQ2057).

References

  1. Antolini, L., Menabue, L. & Saladini, M. (1985). Inorg. Chem.24, 1219–1222.
  2. Battaglia, L. P., Bonamartini Corradi, A., Marcotrigiano, G., Menabue, L. & Pellacani, G. C. (1983). Inorg. Chem.22, 1902–1906.
  3. Bruker (2001). SMART Bruker AXS Inc., Madison, Wisconsin, USA.
  4. Bruker (2003). SAINT Bruker AXS Inc., Madison, Wisconsin, USA.
  5. Liang, F.-P., Chen, M.-S., Hu, R.-X. & Chen, Z.-L. (2004). Acta Cryst. C60, m269–m271. [DOI] [PubMed]
  6. Ma, L. F., Wang, L. Y., Huo, X. K., Wang, Y. Y., Fan, Y. T., Wang, J. G. & Chen, S. H. (2008). Cryst. Growth Des.8, 620–628.
  7. Menabue, L. & Saladini, M. (1991). Inorg. Chem.30, 1651–1655.
  8. Sheldrick, G. M. (2003). SADABS University of Göttingen, Germany.
  9. Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [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/S1600536810036135/zq2057sup1.cif

e-66-m1255-sup1.cif (23.4KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536810036135/zq2057Isup2.hkl

e-66-m1255-Isup2.hkl (182.1KB, 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

RESOURCES