supplementary materials


lh2938 scheme

Acta Cryst. (2009). E65, m1577    [ doi:10.1107/S1600536809046212 ]

Aqua{4,4'-dibromo-6,6'-dimethoxy-2,2'-[ethane-1,2-diylbis(nitrilomethylidyne)]diphenolato}copper(II)

H. Xie

Abstract top

The title complex, [Cu(C18H16Br2N2O4)(H2O)], lies on a crystallographic mirror plane with the CuII ion coordinated by two N atoms and two O atoms of a tetradentate Schiff base ligand and one O atom from a water ligand in a slightly distorted square-pyramidal environment. The mirror plane, which coincides with the Cu-Owater bond, imposes disorder of the atoms of the ethylene group. In the crystal structure, intermolecular O-H...O hydrogen bonds link complex molecules into extended chains along [100].

Comment top

Schiff-bases can readily form stable complexes with most transition metals, in which some may exhibit interesting properties (Yu et al., 2007; Ghosh et al., 2006; Singh et al., 2007; Nayka et al., 2006). Here, we report a Cu(II) complex based on the tetradentate Schiff-base ligand N,N'-ethylenebis(5-bromo-3-methoxysalicylaldimine.

The molecular structure of the title compound is shown in Fig. 1. The complex lies on a crystallographic mirror plane with the CuII ion coordinated in a slightly distorted square-pyramidal environment. The basal plane is occupied by two N atoms and two O atoms of the Schiff-base ligand, and the apical site is occupied by the O atom of the coordinated water molecule. The CuII ion is displaced towards the Cu—Owater bond from the plane formed by the two N atoms and two O atoms by 0.224 (4) Å. The Cu—N and Cu—O bond lengths are consistent with the corresponding distances found in other Cu Schiff base complexes (Nathan, et al., 2003; Saha, et al., 2007; Xing, 2009).

Related literature top

For related structures, see: Nathan et al. (2003); Saha et al. (2007); Xing (2009). For general background to Schiff base compounds, see: Yu et al. (2007); Ghosh et al. (2006); Singh et al. (2007); Nayka et al. (2006).

Experimental top

Condensation of ethyl diamine and 5-bromo-3-methoxyl-2-hydroxy-benzaldehyde with the ratio 1:2 in ethanol gave the Schiff base ligand. The title compound was synthesized by treatment Cu(ClO4)2.6H2O and the schiff-base ligand (1:1, molar ratio) in methanol. After the mixture was stirred for for about 30 min at room temperature, it was filtered and the filtrate was allowed to partial evaporate in air for one week to produce crystals suitable for X-ray diffraction with a yield about 52%.

Refinement top

H atoms were included using the HFIX command in SHELXL-97 (Sheldrick, 2008), with C—H = 0.96 and 0.93 Å; O—H = 0.82Å and were allowed for as riding atoms with Uiso(H) = 1.5Ueq(Cmethyl) and (Uiso(H) = 1.2Ueq(C,O).

Computing details top

Data collection: APEX2 (Bruker, 2004); cell refinement: SAINT-Plus (Bruker, 2001); data reduction: SAINT-Plus (Bruker, 2001); 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 (Sheldrick, 2008).

Figures top
[Figure 1] Fig. 1. The molecular structure of the title compound with the atom-labelling scheme. Displacement ellipsoids are drawn at the 30% probability level. All H-atoms are omitted for clarity. Only one disorder component is shown with open bonds [symmetry code (A): (x, -y+1/2, z).
Aqua{4,4'-dibromo-6,6'-dimethoxy-2,2'-[ethane-1,2- diylbis(nitrilomethylidyne)]diphenolato}copper(II) top
Crystal data top
[Cu(C18H16Br2N2O4)(H2O)]F(000) = 1116
Mr = 565.70Dx = 1.926 Mg m3
Orthorhombic, PnmaMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ac 2nCell parameters from 2580 reflections
a = 8.7299 (13) Åθ = 2.9–26.7°
b = 27.968 (4) ŵ = 5.25 mm1
c = 7.9900 (12) ÅT = 293 K
V = 1950.8 (5) Å3Block, blue
Z = 40.23 × 0.20 × 0.18 mm
Data collection top
Bruker APEXII CCD
diffractometer
1759 independent reflections
Radiation source: fine-focus sealed tube1498 reflections with I > 2σ(I)
graphiteRint = 0.034
φ and ω scansθmax = 25.0°, θmin = 2.7°
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
h = 710
Tmin = 0.378, Tmax = 0.452k = 3327
8970 measured reflectionsl = 89
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.053Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.138H-atom parameters constrained
S = 1.13 w = 1/[σ2(Fo2) + (0.0394P)2 + 13.8845P]
where P = (Fo2 + 2Fc2)/3
1759 reflections(Δ/σ)max = 0.001
140 parametersΔρmax = 1.48 e Å3
1 restraintΔρmin = 1.01 e Å3
Crystal data top
[Cu(C18H16Br2N2O4)(H2O)]V = 1950.8 (5) Å3
Mr = 565.70Z = 4
Orthorhombic, PnmaMo Kα radiation
a = 8.7299 (13) ŵ = 5.25 mm1
b = 27.968 (4) ÅT = 293 K
c = 7.9900 (12) Å0.23 × 0.20 × 0.18 mm
Data collection top
Bruker APEXII CCD
diffractometer
1759 independent reflections
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
1498 reflections with I > 2σ(I)
Tmin = 0.378, Tmax = 0.452Rint = 0.034
8970 measured reflectionsθmax = 25.0°
Refinement top
R[F2 > 2σ(F2)] = 0.053 w = 1/[σ2(Fo2) + (0.0394P)2 + 13.8845P]
where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.138Δρmax = 1.48 e Å3
S = 1.13Δρmin = 1.01 e Å3
1759 reflectionsAbsolute structure: ?
140 parametersFlack parameter: ?
1 restraintRogers parameter: ?
H-atom parameters constrained
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds 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 > 2sigma(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) top
xyzUiso*/UeqOcc. (<1)
Br10.28985 (13)0.50680 (3)0.14560 (14)0.0802 (4)
Cu10.43677 (12)0.25000.01791 (14)0.0336 (3)
O10.2831 (5)0.29928 (14)0.0459 (6)0.0394 (11)
O20.0393 (5)0.35017 (16)0.0910 (7)0.0492 (12)
O30.5275 (7)0.25000.2889 (8)0.0446 (16)
H3A0.56560.27460.32570.067*
N10.5856 (6)0.2962 (2)0.0675 (8)0.0515 (16)
C10.4226 (7)0.3656 (2)0.0697 (8)0.0385 (15)
C20.2929 (7)0.3439 (2)0.0005 (8)0.0334 (13)
C30.1626 (7)0.3736 (2)0.0235 (8)0.0387 (15)
C40.1622 (8)0.4211 (2)0.0169 (9)0.0436 (16)
H40.07540.43970.00060.052*
C50.2941 (9)0.4410 (2)0.0848 (9)0.0472 (17)
C60.4200 (9)0.4150 (2)0.1124 (9)0.0484 (18)
H60.50620.42910.15960.058*
C70.5621 (8)0.3402 (2)0.1013 (9)0.0460 (17)
H70.64210.35710.15050.055*
C80.0958 (9)0.3769 (3)0.1200 (10)0.058 (2)
H8A0.07530.40150.20110.087*
H8B0.17460.35610.16150.087*
H8C0.12900.39130.01720.087*
C90.7175 (16)0.2701 (7)0.147 (2)0.054 (5)0.50
H9A0.69480.26430.26450.065*0.50
H9B0.80890.28970.14130.065*0.50
C9A0.7457 (13)0.2236 (7)0.061 (3)0.052 (5)0.50
H9A10.78120.22800.05270.063*0.50
H9A20.81770.20370.12220.063*0.50
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Br10.1002 (8)0.0319 (4)0.1084 (8)0.0054 (4)0.0121 (6)0.0259 (4)
Cu10.0301 (5)0.0275 (5)0.0433 (6)0.0000.0040 (5)0.000
O10.038 (2)0.024 (2)0.056 (3)0.0025 (18)0.006 (2)0.010 (2)
O20.038 (3)0.034 (2)0.076 (3)0.006 (2)0.014 (2)0.007 (2)
O30.053 (4)0.032 (3)0.049 (4)0.0000.011 (3)0.000
N10.035 (3)0.044 (3)0.076 (4)0.000 (3)0.013 (3)0.020 (3)
C10.041 (4)0.037 (4)0.038 (3)0.002 (3)0.001 (3)0.008 (3)
C20.039 (3)0.026 (3)0.035 (3)0.000 (3)0.000 (3)0.002 (3)
C30.041 (3)0.035 (3)0.040 (3)0.002 (3)0.001 (3)0.002 (3)
C40.049 (4)0.030 (3)0.051 (4)0.005 (3)0.004 (3)0.007 (3)
C50.065 (5)0.029 (3)0.048 (4)0.001 (3)0.005 (4)0.005 (3)
C60.054 (4)0.039 (4)0.052 (4)0.004 (3)0.000 (4)0.009 (3)
C70.038 (4)0.043 (4)0.057 (4)0.005 (3)0.008 (3)0.013 (3)
C80.052 (5)0.053 (5)0.069 (5)0.015 (4)0.011 (4)0.009 (4)
C90.031 (8)0.053 (9)0.078 (14)0.001 (7)0.009 (9)0.021 (10)
C9A0.023 (8)0.067 (11)0.066 (13)0.004 (7)0.006 (8)0.011 (11)
Geometric parameters (Å, °) top
Br1—C51.903 (7)C2—C31.420 (9)
Cu1—O1i1.937 (4)C3—C41.367 (9)
Cu1—O11.937 (4)C4—C51.389 (10)
Cu1—N11.954 (5)C4—H40.9300
Cu1—N1i1.954 (5)C5—C61.338 (10)
Cu1—O32.305 (6)C6—H60.9300
O1—C21.303 (7)C7—H70.9300
O2—C31.371 (8)C8—H8A0.9600
O2—C81.416 (8)C8—H8B0.9600
O3—H3A0.8188C8—H8C0.9600
N1—C71.277 (9)C9—C9A1.491 (19)
N1—C9Ai1.504 (10)C9—H9A0.9700
N1—C91.505 (10)C9—H9B0.9700
C1—C21.402 (9)C9A—N1i1.504 (10)
C1—C61.421 (9)C9A—H9A10.9700
C1—C71.433 (10)C9A—H9A20.9700
O1i—Cu1—O190.8 (2)C5—C4—H4120.6
O1i—Cu1—N1166.2 (3)C6—C5—C4121.8 (6)
O1—Cu1—N191.8 (2)C6—C5—Br1120.1 (6)
O1i—Cu1—N1i91.8 (2)C4—C5—Br1118.1 (5)
O1—Cu1—N1i166.2 (3)C5—C6—C1120.2 (7)
N1—Cu1—N1i82.7 (4)C5—C6—H6119.9
O1i—Cu1—O397.45 (18)C1—C6—H6119.9
O1—Cu1—O397.45 (18)N1—C7—C1125.3 (6)
N1—Cu1—O395.7 (2)N1—C7—H7117.4
N1i—Cu1—O395.7 (2)C1—C7—H7117.4
C2—O1—Cu1127.2 (4)O2—C8—H8A109.5
C3—O2—C8117.8 (5)O2—C8—H8B109.5
Cu1—O3—H3A118.5H8A—C8—H8B109.5
C7—N1—C9Ai120.7 (10)O2—C8—H8C109.5
C7—N1—C9120.0 (9)H8A—C8—H8C109.5
C7—N1—Cu1127.2 (5)H8B—C8—H8C109.5
C9Ai—N1—Cu1111.3 (9)C9A—C9—N1110.7 (14)
C9—N1—Cu1109.7 (8)C9A—C9—H9A109.5
C2—C1—C6120.2 (6)N1—C9—H9A109.5
C2—C1—C7122.8 (6)C9A—C9—H9B109.5
C6—C1—C7117.0 (6)N1—C9—H9B109.5
O1—C2—C1125.4 (6)H9A—C9—H9B108.1
O1—C2—C3118.1 (6)C9—C9A—N1i98.7 (12)
C1—C2—C3116.5 (6)C9—C9A—H9A1112.0
C4—C3—O2123.7 (6)N1i—C9A—H9A1112.0
C4—C3—C2122.6 (6)C9—C9A—H9A2112.0
O2—C3—C2113.7 (5)N1i—C9A—H9A2112.0
C3—C4—C5118.7 (7)H9A1—C9A—H9A2109.7
C3—C4—H4120.6
Symmetry codes: (i) x, −y+1/2, z.
Hydrogen-bond geometry (Å, °) top
D—H···AD—HH···AD···AD—H···A
O3—H3A···O2ii0.822.232.963 (5)150
O3—H3A···O1ii0.822.272.936 (7)139
Symmetry codes: (ii) x+1/2, y, −z+1/2.
Table 1
Hydrogen-bond geometry (Å, °)
top
D—H···AD—HH···AD···AD—H···A
O3—H3A···O2i0.822.232.963 (5)150
O3—H3A···O1i0.822.272.936 (7)139
Symmetry codes: (i) x+1/2, y, −z+1/2.
Acknowledgements top

This work was funded by a research grant from the Shanxi Datong University Foundation of Shanxi Province of the People's Republic of China (grant No. 2008 K1). We also thank Huazhong Normal University for supporting this study.

references
References top

Bruker (2001). SAINT-Plus. Bruker AXS Inc., Madison, Wisconsin, USA.

Bruker (2004). APEX2. Bruker AXS Inc., Madison, Wisconsin, USA.

Ghosh, R., Rahaman, S. H., Lin, C. N., Lu, T. H. & Ghosh, B. K. (2006). Polyhedron, 25, 3104–3112.

Nathan, L. C., Koehne, J. E., Gilmore, J. M., Hannibal, K. A., Dewhirst, W. E. & Mai, T. D. (2003). Polyhedron, 22, 887–894.

Nayka, M., Koner, R., Lin, H. H., Florke, U., Wei, H. H. & Mohanta, S. (2006). Inorg. Chem.. 45, 10764–10773.

Saha, P. K., Dutta, B., Jana, S., Bera, R., Saha, S., Okamoto, K. & Koner, S. (2007). Polyhedron, 26, 563–571.

Sheldrick, G. M. (1996). SADABS. University of Göttingen, Germany.

Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122.

Singh, K., Barwa, M. S. & Tyagi, P. (2007). Eur. J. Med. Chem. 42, 394–402.

Xing, J. (2009). Acta Cryst. E65, m469.

Yu, T. Z., Zhang, K., Zhao, Y. L., Yang, C. H., Zhang, H., Fan, D. W. & Dong, W. K. (2007). Inorg. Chem. Commun. 10, 401-403.