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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2008 Aug 23;64(Pt 9):m1192. doi: 10.1107/S1600536808026457

cis-Bis(butyl­amine-κN)bis­[sulfa­diazine(1−)-κ2 N,N′]copper(II) penta­hydrate

Hümeyra Paşaoğlu a, Gökhan Kaştaş a,*, Zerrin Heren b, Orhan Büyükgüngör a
PMCID: PMC2960652  PMID: 21201631

Abstract

In the title compound {systematic name: cis-bis­[4-amino-N-(pyrimidin-2-yl)benzene­sulfonamidato-κ2 N,N′]bis­(butyl­amine-κN)copper(II) penta­hydrate}, [Cu(C10H9N4O2S)2(C4H11N)2]·5H2O or [Cu(sdz)2(ba)2]·5H2O [ba is butyl­amine and sdz = sulfadiazine(1−)], the copper(II) cation is six-coordinated by four N atoms of two sulfadiazine ligands and two N atoms of butyl­amine ligands. The copper(II) ion and one of the water mol­ecules lie on twofold rotation axes. One of the butyl groups is disordered over two sites, with occupancies of 0.395 (8) and 0.605 (8). The geometry around the S atom is distorted tetra­hedral. The crystal structure involves inter­molecular N—H⋯N and N—H⋯O hydrogen bonds. N—H⋯N hydrogen bonds between sdz ligands lead to a sheet structure parallel to the ab plane.

Related literature

For related structures, see: Heren et al. (2006 ▶); Chung et al. (1975 ▶).graphic file with name e-64-m1192-scheme1.jpg

Experimental

Crystal data

  • [Cu(C10H9N4O2S)2(C4H11N)2]·5H2O

  • M r = 790.04

  • Orthorhombic, Inline graphic

  • a = 22.623 (6) Å

  • b = 10.342 (5) Å

  • c = 16.250 (6) Å

  • V = 3802 (2) Å3

  • Z = 4

  • Mo Kα radiation

  • μ = 0.74 mm−1

  • T = 296 K

  • 0.34 × 0.21 × 0.19 mm

Data collection

  • Stoe IPDS2 diffractometer

  • Absorption correction: integration (X-RED32; Stoe & Cie, 2002 ▶) T min = 0.821, T max = 0.899

  • 57960 measured reflections

  • 4235 independent reflections

  • 2098 reflections with I > 2σ(I)

  • R int = 0.085

Refinement

  • R[F 2 > 2σ(F 2)] = 0.048

  • wR(F 2) = 0.141

  • S = 0.90

  • 4235 reflections

  • 234 parameters

  • H-atom parameters constrained

  • Δρmax = 0.65 e Å−3

  • Δρmin = −0.45 e Å−3

Data collection: X-AREA (Stoe & Cie, 2002 ▶); cell refinement: X-AREA; data reduction: X-RED32 (Stoe & Cie, 2002 ▶); 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 I, global. DOI: 10.1107/S1600536808026457/cf2216sup1.cif

e-64-m1192-sup1.cif (22.2KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536808026457/cf2216Isup2.hkl

e-64-m1192-Isup2.hkl (179.7KB, 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
N5—H5A⋯N2i 0.86 2.53 3.359 (5) 162
N4—H4A⋯O5ii 0.90 2.45 3.337 (6) 171
N4—H4B⋯O4iii 0.90 2.25 3.119 (6) 161
N5—H5B⋯O5iv 0.86 2.26 3.113 (5) 170

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

Acknowledgments

The authors thank the Faculty of Arts and Sciences, Ondokuz Mayıs University, Turkey, for the use of the Stoe IPDS2 diffractometer (purchased under grant No. F279 of the University Research Fund).

supplementary crystallographic information

Comment

In the title complex (I), the copper(II) ion is six-coordinated by four N atoms of sulfadiazine ligands and two N atoms of butylammonium ligands. The copper(II) ion and one of the water molecules lie on twofold rotation axes. It is found that the Cu–Nsdz and Cu–Nba bond distances are nearly equal. The bond angles around the S atom correspond to a distorted tetrahedral geometry. The C4–N5 bond distance and the torsion angle C1–S1–N1–C7 are comparable to those observed in related structures (Heren et al., 2006; Chung et al., 1975). One of the butyl groups is disordered over two sites with occupancies of 0.395 (8):0.605 (8) (see Fig. 1).

The packing of (I) is stabilized by intermolecular N—H···N and N—H···O hydrogen bonds (Table 1). The N—H···N hydrogen bond takes place between sdz ligands and it is seen that these hydrogen bonds generate a sheet structure parallel to the ab plane (Fig. 2). The H atoms of water molecules could not be located from a Fourier map. However, it is possible to see that water molecules are involved in hydrogen bonds with sdz and ba ligands on the basis of interatomic distances.

Experimental

A solution of butylamine (2 mmol) in ethanol (20 ml) was added dropwise with stirring to a solution of Cu(II) sulfadiazine (1 mmol) in methanol (40 ml). The solution was heated and stirred for 3 h at 343 K and then the mixture was cooled to room temperature. The blue crystals were filtered off, washed with cold distilled water and acetone, and dried in vacuo. Analysis calculated: C 42.62, H 5.84, N 17.76%; found: C 43.08, H 5.72, N 18.25%.

Refinement

One butyl group shows disorder and was modelled with two different orientations and site occupancies of 0.395 (8):0.605 (8). The H atoms of water molecules could not be located from a Fourier map. All other H atoms were placed in geometrically idealized positions with distances N—H = 0.86–0.90 Å, C—H = 0.93–0.97 Å, and were refined as riding atoms with Uiso(H) = 1.2Ueq(C,N) and Uiso(Hmethyl) = 1.5Ueq(C).

Figures

Fig. 1.

Fig. 1.

The molecular structure of (I), with atom labels and 30% probability displacement ellipsoids. Only the major part of the disordered ba ligand is included. [Symmetry code: (i) -x + 1, y, -z + 1/2.]

Fig. 2.

Fig. 2.

A view of the complex showing the sheet structure parallel to the ab plane. The butyl groups, water molecules and some hydrogen bonds have been omitted for clarity. Other hydrogen bonds are shown as dashed lines. [Symmetry code: (i) -x + 1/2, y - 1/2, z.]

Crystal data

[Cu(C10H9N4O2S)2(C4H11N)2]·5H2O F000 = 1594
Mr = 790.04 Dx = 1.347 Mg m−3
Orthorhombic, Pbcn Mo Kα radiation λ = 0.71069 Å
Hall symbol: -P 2n 2ab Cell parameters from 30097 reflections
a = 22.623 (6) Å θ = 1.8–27.1º
b = 10.342 (5) Å µ = 0.74 mm−1
c = 16.250 (6) Å T = 296 K
V = 3802 (2) Å3 Prism, blue
Z = 4 0.34 × 0.21 × 0.19 mm

Data collection

Stoe IPDS2 diffractometer 4235 independent reflections
Radiation source: fine-focus sealed tube 2098 reflections with I > 2σ(I)
Monochromator: graphite Rint = 0.085
T = 296 K θmax = 27.2º
rotation method scans θmin = 1.8º
Absorption correction: integration(X-RED32; Stoe & Cie, 2002) h = −28→28
Tmin = 0.821, Tmax = 0.900 k = −13→13
57960 measured reflections l = −20→20

Refinement

Refinement on F2 Secondary atom site location: difference Fourier map
Least-squares matrix: full Hydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.048 H-atom parameters constrained
wR(F2) = 0.141   w = 1/[σ2(Fo2) + (0.0787P)2] where P = (Fo2 + 2Fc2)/3
S = 0.90 (Δ/σ)max < 0.001
4235 reflections Δρmax = 0.65 e Å−3
234 parameters Δρmin = −0.45 e Å−3
Primary atom site location: structure-invariant direct methods Extinction correction: none

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 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. 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 Occ. (<1)
C1 0.33524 (14) 0.7316 (3) 0.45323 (19) 0.0565 (8)
C2 0.29637 (16) 0.8185 (4) 0.4879 (2) 0.0684 (9)
H2 0.3109 0.8929 0.5129 0.082*
C3 0.23634 (16) 0.7970 (4) 0.4860 (2) 0.0752 (10)
H3 0.2108 0.8559 0.5107 0.090*
C4 0.21358 (15) 0.6879 (4) 0.4473 (2) 0.0689 (9)
C5 0.25293 (17) 0.6011 (4) 0.4128 (2) 0.0728 (10)
H5 0.2387 0.5271 0.3870 0.087*
C6 0.31255 (15) 0.6227 (3) 0.4160 (2) 0.0664 (9)
H6 0.3382 0.5628 0.3927 0.080*
C7 0.41743 (13) 0.8242 (3) 0.3032 (2) 0.0565 (8)
C8 0.36943 (17) 0.9966 (4) 0.2474 (3) 0.0800 (11)
H8 0.3452 1.0686 0.2536 0.096*
C9 0.39032 (17) 0.9691 (4) 0.1702 (3) 0.0847 (12)
H9 0.3802 1.0190 0.1247 0.102*
C10 0.42700 (16) 0.8638 (4) 0.1637 (2) 0.0745 (10)
H10 0.4427 0.8426 0.1125 0.089*
C11 0.3906 (2) 0.4981 (5) 0.2216 (4) 0.124 (2)
H11A 0.3706 0.5801 0.2136 0.149*
H11B 0.3925 0.4841 0.2806 0.149*
C12 0.3518 (2) 0.4000 (5) 0.1892 (4) 0.1116 (17)
H12A 0.3740 0.3199 0.1854 0.134*
H12B 0.3409 0.4246 0.1337 0.134*
C13A 0.2962 (4) 0.3733 (8) 0.2362 (5) 0.088 (2) 0.605 (8)
H13A 0.2764 0.4549 0.2461 0.105* 0.605 (8)
H13B 0.3070 0.3376 0.2893 0.105* 0.605 (8)
C13B 0.2848 (5) 0.4111 (13) 0.1823 (9) 0.088 (2) 0.395 (8)
H13C 0.2709 0.4851 0.2134 0.105* 0.395 (8)
H13D 0.2733 0.4223 0.1253 0.105* 0.395 (8)
C14A 0.2505 (12) 0.277 (3) 0.1934 (18) 0.108 (4) 0.605 (8)
H14A 0.2169 0.2658 0.2286 0.162* 0.605 (8)
H14B 0.2692 0.1954 0.1841 0.162* 0.605 (8)
H14C 0.2380 0.3132 0.1418 0.162* 0.605 (8)
C14B 0.261 (2) 0.299 (4) 0.213 (3) 0.108 (4) 0.395 (8)
H14D 0.2186 0.3043 0.2115 0.162* 0.395 (8)
H14E 0.2736 0.2879 0.2693 0.162* 0.395 (8)
H14F 0.2741 0.2270 0.1810 0.162* 0.395 (8)
N1 0.43499 (11) 0.7422 (3) 0.36300 (16) 0.0586 (7)
N2 0.38163 (12) 0.9265 (3) 0.31428 (17) 0.0635 (7)
N3 0.44067 (12) 0.7910 (3) 0.22883 (16) 0.0596 (7)
N4 0.44912 (14) 0.5158 (3) 0.1947 (2) 0.0896 (10)
H4A 0.4478 0.5356 0.1408 0.108*
H4B 0.4677 0.4391 0.1990 0.108*
N5 0.15418 (15) 0.6661 (4) 0.4447 (2) 0.1001 (11)
H5A 0.1407 0.5976 0.4213 0.120*
H5B 0.1302 0.7209 0.4664 0.120*
O1 0.42208 (10) 0.8844 (2) 0.48919 (14) 0.0690 (6)
O2 0.43907 (10) 0.6530 (2) 0.49927 (15) 0.0731 (7)
O3 0.02149 (14) 0.6126 (3) 0.4017 (2) 0.1193 (11)
O4 0.0000 0.7493 (5) 0.2500 0.151 (2)
O5 0.43200 (14) 0.3833 (3) 0.5011 (3) 0.1410 (15)
S2 0.41156 (4) 0.75774 (8) 0.45398 (5) 0.0588 (2)
Cu1 0.5000 0.64823 (6) 0.2500 0.0647 (2)

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
C1 0.0482 (17) 0.062 (2) 0.0590 (17) −0.0025 (16) 0.0034 (15) 0.0033 (16)
C2 0.056 (2) 0.068 (2) 0.081 (2) −0.0050 (18) 0.0009 (18) −0.0092 (19)
C3 0.053 (2) 0.080 (2) 0.093 (3) 0.0044 (19) 0.0133 (19) −0.005 (2)
C4 0.051 (2) 0.078 (2) 0.078 (2) −0.0120 (19) −0.0005 (17) 0.007 (2)
C5 0.059 (2) 0.077 (2) 0.083 (2) −0.013 (2) −0.0008 (19) −0.005 (2)
C6 0.054 (2) 0.069 (2) 0.076 (2) −0.0018 (17) 0.0045 (17) −0.0079 (18)
C7 0.0426 (17) 0.064 (2) 0.063 (2) −0.0072 (16) 0.0046 (15) 0.0020 (16)
C8 0.067 (2) 0.084 (3) 0.088 (3) 0.012 (2) −0.003 (2) 0.020 (2)
C9 0.068 (2) 0.105 (3) 0.081 (3) 0.004 (2) −0.003 (2) 0.028 (2)
C10 0.057 (2) 0.100 (3) 0.066 (2) −0.001 (2) 0.0069 (17) 0.007 (2)
C11 0.089 (3) 0.096 (3) 0.187 (6) −0.029 (3) 0.050 (3) −0.047 (4)
C12 0.080 (3) 0.108 (4) 0.146 (4) −0.006 (3) 0.002 (3) −0.049 (3)
C13A 0.079 (4) 0.092 (5) 0.092 (5) −0.012 (4) 0.002 (4) −0.018 (4)
C13B 0.079 (4) 0.092 (5) 0.092 (5) −0.012 (4) 0.002 (4) −0.018 (4)
C14A 0.081 (11) 0.103 (9) 0.140 (15) −0.017 (6) −0.014 (8) −0.034 (8)
C14B 0.081 (11) 0.103 (9) 0.140 (15) −0.017 (6) −0.014 (8) −0.034 (8)
N1 0.0480 (15) 0.0615 (16) 0.0664 (16) 0.0056 (13) 0.0059 (12) 0.0030 (14)
N2 0.0588 (17) 0.0636 (17) 0.0679 (17) 0.0086 (14) 0.0022 (14) 0.0019 (15)
N3 0.0506 (16) 0.0697 (17) 0.0585 (16) −0.0061 (14) 0.0041 (12) −0.0026 (14)
N4 0.070 (2) 0.087 (2) 0.112 (3) 0.0022 (18) 0.0034 (19) −0.021 (2)
N5 0.0505 (18) 0.110 (3) 0.140 (3) −0.0131 (19) 0.004 (2) −0.009 (2)
O1 0.0574 (14) 0.0741 (15) 0.0755 (14) −0.0064 (12) −0.0044 (12) −0.0138 (12)
O2 0.0606 (15) 0.0799 (16) 0.0787 (15) 0.0053 (13) −0.0093 (12) 0.0243 (13)
O3 0.079 (2) 0.125 (3) 0.155 (3) 0.0017 (19) 0.018 (2) −0.008 (2)
O4 0.174 (6) 0.091 (3) 0.188 (6) 0.000 0.053 (4) 0.000
O5 0.073 (2) 0.096 (2) 0.253 (5) 0.0007 (18) −0.015 (3) −0.001 (3)
S2 0.0469 (4) 0.0667 (5) 0.0629 (5) −0.0008 (4) −0.0020 (4) 0.0035 (4)
Cu1 0.0516 (3) 0.0697 (4) 0.0726 (4) 0.000 0.0051 (3) 0.000

Geometric parameters (Å, °)

C1—C6 1.377 (5) C12—C13B 1.524 (13)
C1—C2 1.378 (5) C12—H12A 0.970
C1—S2 1.748 (3) C12—H12B 0.970
C2—C3 1.377 (5) C13A—C14A 1.592 (16)
C2—H2 0.930 C13A—H13A 0.970
C3—C4 1.391 (5) C13A—H13B 0.970
C3—H3 0.930 C13B—C14B 1.37 (5)
C4—N5 1.363 (5) C13B—H13C 0.970
C4—C5 1.382 (5) C13B—H13D 0.970
C5—C6 1.368 (5) C14A—H14A 0.960
C5—H5 0.930 C14A—H14B 0.960
C6—H6 0.930 C14A—H14C 0.960
C7—N2 1.344 (4) C14B—H14D 0.960
C7—N1 1.351 (4) C14B—H14E 0.960
C7—N3 1.361 (4) C14B—H14F 0.960
C8—N2 1.334 (5) N1—S2 1.579 (3)
C8—C9 1.371 (6) N3—Cu1 2.025 (3)
C8—H8 0.930 N4—Cu1 2.002 (3)
C9—C10 1.373 (5) N4—H4A 0.900
C9—H9 0.930 N4—H4B 0.900
C10—N3 1.336 (4) N5—H5A 0.860
C10—H10 0.930 N5—H5B 0.860
C11—N4 1.407 (5) O1—S2 1.449 (2)
C11—C12 1.441 (6) O2—S2 1.450 (2)
C11—H11A 0.970 Cu1—N4i 2.002 (3)
C11—H11B 0.970 Cu1—N3i 2.025 (3)
C12—C13A 1.496 (9)
C6—C1—C2 118.4 (3) C12—C13A—H13B 108.3
C6—C1—S2 119.9 (3) C14A—C13A—H13B 108.3
C2—C1—S2 121.8 (3) H13A—C13A—H13B 107.4
C3—C2—C1 121.0 (3) C14B—C13B—C12 107 (2)
C3—C2—H2 119.5 C14B—C13B—H13C 110.2
C1—C2—H2 119.5 C12—C13B—H13C 110.2
C2—C3—C4 120.4 (4) C14B—C13B—H13D 110.2
C2—C3—H3 119.8 C12—C13B—H13D 110.2
C4—C3—H3 119.8 H13C—C13B—H13D 108.5
N5—C4—C5 121.0 (4) C13A—C14A—H14A 109.5
N5—C4—C3 120.8 (4) C13A—C14A—H14B 109.5
C5—C4—C3 118.1 (3) H14A—C14A—H14B 109.5
C6—C5—C4 120.9 (4) C13A—C14A—H14C 109.5
C6—C5—H5 119.6 H14A—C14A—H14C 109.5
C4—C5—H5 119.6 H14B—C14A—H14C 109.5
C5—C6—C1 121.2 (3) C13B—C14B—H14D 109.5
C5—C6—H6 119.4 C13B—C14B—H14E 109.5
C1—C6—H6 119.4 H14D—C14B—H14E 109.5
N2—C7—N1 125.1 (3) C13B—C14B—H14F 109.5
N2—C7—N3 123.4 (3) H14D—C14B—H14F 109.5
N1—C7—N3 111.5 (3) H14E—C14B—H14F 109.5
N2—C8—C9 124.2 (4) C7—N1—S2 120.8 (2)
N2—C8—H8 117.9 C8—N2—C7 116.2 (3)
C9—C8—H8 117.9 C10—N3—C7 118.1 (3)
C8—C9—C10 116.3 (4) C10—N3—Cu1 134.4 (2)
C8—C9—H9 121.8 C7—N3—Cu1 106.8 (2)
C10—C9—H9 121.8 C11—N4—Cu1 119.4 (3)
N3—C10—C9 121.7 (4) C11—N4—H4A 107.5
N3—C10—H10 119.1 Cu1—N4—H4A 107.5
C9—C10—H10 119.1 C11—N4—H4B 107.5
N4—C11—C12 123.4 (4) Cu1—N4—H4B 107.5
N4—C11—H11A 106.5 H4A—N4—H4B 107.0
C12—C11—H11A 106.5 C4—N5—H5A 120.0
N4—C11—H11B 106.5 C4—N5—H5B 120.0
C12—C11—H11B 106.5 H5A—N5—H5B 120.0
H11A—C11—H11B 106.5 O1—S2—O2 113.88 (15)
C11—C12—C13A 117.0 (5) O1—S2—N1 113.99 (15)
C11—C12—C13B 125.3 (6) O2—S2—N1 104.77 (15)
C11—C12—H12A 108.0 O1—S2—C1 107.76 (15)
C13A—C12—H12A 108.0 O2—S2—C1 108.16 (15)
C13B—C12—H12A 125.1 N1—S2—C1 108.02 (15)
C11—C12—H12B 108.0 N4—Cu1—N4i 93.7 (2)
C13A—C12—H12B 108.0 N4—Cu1—N3i 162.98 (13)
C13B—C12—H12B 70.1 N4i—Cu1—N3i 92.38 (13)
H12A—C12—H12B 107.3 N4—Cu1—N3 92.38 (13)
C12—C13A—C14A 116.0 (14) N4i—Cu1—N3 162.98 (13)
C12—C13A—H13A 108.3 N3i—Cu1—N3 86.36 (16)
C14A—C13A—H13A 108.3
C6—C1—C2—C3 0.5 (5) C9—C10—N3—Cu1 −169.6 (3)
S2—C1—C2—C3 179.3 (3) N2—C7—N3—C10 −0.2 (5)
C1—C2—C3—C4 −1.4 (6) N1—C7—N3—C10 179.9 (3)
C2—C3—C4—N5 −179.6 (4) N2—C7—N3—Cu1 171.8 (2)
C2—C3—C4—C5 1.4 (6) N1—C7—N3—Cu1 −8.1 (3)
N5—C4—C5—C6 −179.5 (4) C12—C11—N4—Cu1 −176.0 (5)
C3—C4—C5—C6 −0.5 (6) C7—N1—S2—O1 −55.6 (3)
C4—C5—C6—C1 −0.4 (6) C7—N1—S2—O2 179.3 (2)
C2—C1—C6—C5 0.4 (5) C7—N1—S2—C1 64.1 (3)
S2—C1—C6—C5 −178.4 (3) C6—C1—S2—O1 174.2 (3)
N2—C8—C9—C10 −1.4 (6) C2—C1—S2—O1 −4.6 (3)
C8—C9—C10—N3 1.1 (6) C6—C1—S2—O2 −62.3 (3)
N4—C11—C12—C13A 166.6 (7) C2—C1—S2—O2 118.9 (3)
N4—C11—C12—C13B −149.2 (9) C6—C1—S2—N1 50.6 (3)
C11—C12—C13A—C14A 172.7 (14) C2—C1—S2—N1 −128.2 (3)
C13B—C12—C13A—C14A 59.0 (16) C11—N4—Cu1—N4i 108.9 (5)
C11—C12—C13B—C14B −132 (2) C11—N4—Cu1—N3i −140.5 (5)
C13A—C12—C13B—C14B −42 (2) C11—N4—Cu1—N3 −55.2 (4)
N2—C7—N1—S2 2.7 (4) C10—N3—Cu1—N4 −79.3 (4)
N3—C7—N1—S2 −177.4 (2) C7—N3—Cu1—N4 110.6 (2)
C9—C8—N2—C7 0.9 (6) C10—N3—Cu1—N4i 169.9 (4)
N1—C7—N2—C8 179.8 (3) C7—N3—Cu1—N4i −0.1 (5)
N3—C7—N2—C8 −0.1 (5) C10—N3—Cu1—N3i 83.7 (3)
C9—C10—N3—C7 −0.4 (5) C7—N3—Cu1—N3i −86.4 (2)

Symmetry codes: (i) −x+1, y, −z+1/2.

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
N5—H5A···N2ii 0.86 2.53 3.359 (5) 162
N4—H4A···O5iii 0.90 2.45 3.337 (6) 171
N4—H4B···O4iv 0.90 2.25 3.119 (6) 161
N5—H5B···O5v 0.86 2.26 3.113 (5) 170

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

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: CF2216).

References

  1. Chung, H. K., Hoon, S. K., Young, K. Y. & Il-Hwan, S. (1975). J. Korean Phys. Soc.8, 37–48.
  2. Farrugia, L. J. (1997). J. Appl. Cryst.30, 565.
  3. Farrugia, L. J. (1999). J. Appl. Cryst.32, 837–838.
  4. Heren, Z., Paşaoğlu, H. & Kaştaş, G. (2006). Acta Cryst. E62, o3437–o3439.
  5. Macrae, C. F., Edgington, P. R., McCabe, P., Pidcock, E., Shields, G. P., Taylor, R., Towler, M. & van de Streek, J. (2006). J. Appl. Cryst.39, 453–457.
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  7. Stoe & Cie (2002). X-AREA and X-RED32 Stoe & Cie, Darmstadt, Germany.

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/S1600536808026457/cf2216sup1.cif

e-64-m1192-sup1.cif (22.2KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536808026457/cf2216Isup2.hkl

e-64-m1192-Isup2.hkl (179.7KB, hkl)

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


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