metal-organic compounds
{4-Bromo-2-[2-(methylamino)ethyliminomethyl]phenolato}thiocyanatocopper(II)
aChemical Engineering and Pharmaceutics College, Henan University of Science and Technology, Luoyang, Henan 471003, People's Republic of China, and Department of Chemistry, Pingdingshan University, Henan 467000, People's Republic of China
*Correspondence e-mail: junying-ma@163.com
In the title mononuclear copper(II) complex, [Cu(C10H12BrN2O)(NCS)], the CuII ion is coordinated by two N atoms and one O atom from a Schiff base ligand, and by one N atom from a thiocyanate anion, giving a square-planar geometry. In the symmetry-related molecules are linked by an N—H⋯S hydrogen bond.
Related literature
For related literature, see: Diao & Li (2007); Diao et al. (2007); Ma et al. (2005); Ma, Gu et al. (2006); Ma, Lv et al. (2006); Ma, Wu et al. (2006); Wei et al. (2007).
Experimental
Crystal data
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Refinement
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Data collection: SMART (Bruker, 1998); cell SAINT (Bruker, 1998); 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.
Supporting information
10.1107/S1600536808016589/su2051sup1.cif
contains datablocks global, I. DOI:Structure factors: contains datablock I. DOI: 10.1107/S1600536808016589/su2051Isup2.hkl
N-Methylethane-1,2-diamine (0.5 mmol, 37.0 mg) and 5-bromosalicylaldehyde (0.5 mmol, 100.5 mg) were dissolved in methanol (30 ml). The mixture was stirred for 1 h to obtain a clear yellow solution. To this solution was added with stirring a methanol solution (20 ml) of copper(II) acetate (0.5 mmol, 99.6 mg) and a methanol solution (10 ml) of ammonium thiocyanate (0.5 mmol, 38.0 mg). After keeping the resulting solution in air for a few days, blue block-shaped crystals were formed.
All the H atoms were placed in geometrically idealized positions and constrained to ride on their parent atoms with C—H = 0.93 - 0.97 Å, with Uiso(H) = 1.2 or 1.5Ueq(C). An unassigned maximum residual density (1.68 Å3) was observed 1.03 Å from Br1, which is due to the tail-effects of the heavy atom Br1. The structure contains solvent accessible voids of 119 Å3, which may perhaps accommodate a partially occupied solvent molecule.
Data collection: SMART (Bruker, 1998); cell
SAINT (Bruker, 1998); data reduction: SAINT (Bruker, 1998); 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).Fig. 1. The molecular structure of compound (I), showing the atomic numbering scheme and the displacement ellipsoids drawn at the 30% probability level. |
[Cu(C10H12BrN2O)(NCS)] | F(000) = 748 |
Mr = 377.75 | Dx = 1.691 Mg m−3 |
Monoclinic, P21/n | Mo Kα radiation, λ = 0.71073 Å |
Hall symbol: -P 2yn | Cell parameters from 1708 reflections |
a = 5.952 (3) Å | θ = 2.5–25.3° |
b = 19.660 (3) Å | µ = 4.30 mm−1 |
c = 12.718 (2) Å | T = 298 K |
β = 94.331 (3)° | Block, blue |
V = 1484.0 (8) Å3 | 0.32 × 0.32 × 0.31 mm |
Z = 4 |
Bruker SMART CCD area-detector diffractometer | 2997 independent reflections |
Radiation source: fine-focus sealed tube | 1875 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.071 |
ω scan | θmax = 26.5°, θmin = 2.6° |
Absorption correction: multi-scan (SADABS; Sheldrick, 1996) | h = −7→7 |
Tmin = 0.259, Tmax = 0.267 | k = −24→24 |
11246 measured reflections | l = −15→15 |
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)] = 0.076 | Hydrogen site location: inferred from neighbouring sites |
wR(F2) = 0.181 | H-atom parameters constrained |
S = 1.11 | w = 1/[σ2(Fo2) + (0.0672P)2 + 4.7203P] where P = (Fo2 + 2Fc2)/3 |
2997 reflections | (Δ/σ)max < 0.001 |
164 parameters | Δρmax = 1.68 e Å−3 |
0 restraints | Δρmin = −0.84 e Å−3 |
[Cu(C10H12BrN2O)(NCS)] | V = 1484.0 (8) Å3 |
Mr = 377.75 | Z = 4 |
Monoclinic, P21/n | Mo Kα radiation |
a = 5.952 (3) Å | µ = 4.30 mm−1 |
b = 19.660 (3) Å | T = 298 K |
c = 12.718 (2) Å | 0.32 × 0.32 × 0.31 mm |
β = 94.331 (3)° |
Bruker SMART CCD area-detector diffractometer | 2997 independent reflections |
Absorption correction: multi-scan (SADABS; Sheldrick, 1996) | 1875 reflections with I > 2σ(I) |
Tmin = 0.259, Tmax = 0.267 | Rint = 0.071 |
11246 measured reflections |
R[F2 > 2σ(F2)] = 0.076 | 0 restraints |
wR(F2) = 0.181 | H-atom parameters constrained |
S = 1.11 | Δρmax = 1.68 e Å−3 |
2997 reflections | Δρmin = −0.84 e Å−3 |
164 parameters |
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. |
x | y | z | Uiso*/Ueq | ||
Cu1 | 0.77313 (15) | 0.20764 (5) | 0.04645 (8) | 0.0407 (3) | |
N1 | 1.0514 (10) | 0.1635 (3) | 0.0963 (5) | 0.0392 (15) | |
N2 | 0.8291 (12) | 0.2634 (4) | 0.1796 (7) | 0.058 (2) | |
H2A | 0.7645 | 0.2393 | 0.2304 | 0.070* | |
N3 | 0.4927 (12) | 0.2539 (4) | 0.0002 (6) | 0.053 (2) | |
O1 | 0.7104 (8) | 0.1410 (3) | −0.0588 (4) | 0.0460 (14) | |
S1 | 0.0695 (4) | 0.29376 (15) | −0.0863 (2) | 0.0664 (8) | |
Br1 | 1.31654 (16) | −0.06412 (5) | −0.23999 (9) | 0.0633 (4) | |
C1 | 1.1328 (13) | 0.0028 (4) | −0.1792 (7) | 0.044 (2) | |
C2 | 0.9203 (14) | 0.0131 (4) | −0.2253 (8) | 0.049 (2) | |
H2 | 0.8712 | −0.0121 | −0.2845 | 0.059* | |
C3 | 0.7799 (13) | 0.0596 (4) | −0.1860 (7) | 0.047 (2) | |
H3 | 0.6360 | 0.0657 | −0.2184 | 0.057* | |
C4 | 0.8518 (13) | 0.0994 (4) | −0.0946 (6) | 0.0367 (18) | |
C5 | 1.0688 (12) | 0.0860 (4) | −0.0492 (6) | 0.0369 (18) | |
C6 | 1.2068 (14) | 0.0376 (4) | −0.0913 (7) | 0.045 (2) | |
H6 | 1.3497 | 0.0291 | −0.0592 | 0.054* | |
C7 | 1.1533 (13) | 0.1183 (4) | 0.0480 (7) | 0.042 (2) | |
H7 | 1.2941 | 0.1047 | 0.0773 | 0.051* | |
C8 | 1.1509 (15) | 0.1902 (5) | 0.1982 (7) | 0.052 (2) | |
H8A | 1.3140 | 0.1889 | 0.1997 | 0.062* | |
H8B | 1.1038 | 0.1625 | 0.2557 | 0.062* | |
C9 | 1.0734 (14) | 0.2612 (5) | 0.2099 (7) | 0.051 (2) | |
H9A | 1.1028 | 0.2760 | 0.2824 | 0.061* | |
H9B | 1.1531 | 0.2912 | 0.1650 | 0.061* | |
C10 | 0.7370 (17) | 0.3305 (6) | 0.1855 (10) | 0.083 (4) | |
H10A | 0.8001 | 0.3526 | 0.2482 | 0.125* | |
H10B | 0.5763 | 0.3276 | 0.1874 | 0.125* | |
H10C | 0.7728 | 0.3562 | 0.1248 | 0.125* | |
C11 | 0.3146 (15) | 0.2696 (4) | −0.0378 (7) | 0.048 (2) |
U11 | U22 | U33 | U12 | U13 | U23 | |
Cu1 | 0.0271 (5) | 0.0511 (6) | 0.0429 (6) | 0.0011 (4) | −0.0028 (4) | −0.0086 (5) |
N1 | 0.028 (3) | 0.047 (4) | 0.041 (4) | −0.004 (3) | −0.006 (3) | −0.001 (3) |
N2 | 0.040 (4) | 0.062 (5) | 0.070 (5) | −0.001 (4) | −0.005 (4) | −0.022 (4) |
N3 | 0.030 (4) | 0.069 (5) | 0.058 (5) | 0.008 (3) | −0.006 (3) | −0.015 (4) |
O1 | 0.025 (3) | 0.055 (4) | 0.056 (4) | 0.006 (3) | −0.009 (2) | −0.012 (3) |
S1 | 0.0412 (13) | 0.0813 (18) | 0.0744 (18) | 0.0000 (13) | −0.0115 (12) | 0.0316 (15) |
Br1 | 0.0480 (6) | 0.0520 (6) | 0.0910 (8) | 0.0037 (4) | 0.0131 (5) | −0.0149 (5) |
C1 | 0.036 (4) | 0.030 (4) | 0.068 (6) | 0.003 (3) | 0.014 (4) | −0.002 (4) |
C2 | 0.035 (5) | 0.045 (5) | 0.066 (6) | −0.005 (4) | 0.001 (4) | −0.009 (4) |
C3 | 0.029 (4) | 0.047 (5) | 0.064 (6) | 0.000 (4) | −0.014 (4) | −0.007 (4) |
C4 | 0.031 (4) | 0.033 (4) | 0.044 (5) | 0.001 (3) | −0.006 (3) | −0.002 (4) |
C5 | 0.029 (4) | 0.040 (4) | 0.041 (5) | 0.004 (3) | 0.004 (3) | 0.013 (4) |
C6 | 0.042 (5) | 0.037 (4) | 0.057 (5) | 0.000 (4) | −0.002 (4) | 0.007 (4) |
C7 | 0.028 (4) | 0.043 (5) | 0.055 (5) | 0.003 (4) | −0.007 (4) | 0.015 (4) |
C8 | 0.048 (5) | 0.065 (6) | 0.039 (5) | −0.011 (4) | −0.017 (4) | −0.003 (4) |
C9 | 0.039 (5) | 0.075 (6) | 0.038 (5) | −0.006 (4) | −0.002 (4) | −0.022 (5) |
C10 | 0.051 (6) | 0.092 (8) | 0.106 (9) | 0.038 (6) | −0.005 (6) | −0.039 (7) |
C11 | 0.042 (5) | 0.051 (5) | 0.050 (5) | −0.015 (4) | −0.001 (4) | −0.004 (4) |
Cu1—O1 | 1.890 (5) | C2—H2 | 0.9300 |
Cu1—N1 | 1.934 (6) | C3—C4 | 1.439 (11) |
Cu1—N3 | 1.952 (7) | C3—H3 | 0.9300 |
Cu1—N2 | 2.024 (7) | C4—C5 | 1.399 (10) |
N1—C7 | 1.262 (10) | C5—C6 | 1.390 (11) |
N1—C8 | 1.479 (10) | C5—C7 | 1.446 (12) |
N2—C10 | 1.432 (12) | C6—H6 | 0.9300 |
N2—C9 | 1.476 (11) | C7—H7 | 0.9300 |
N2—H2A | 0.9100 | C8—C9 | 1.481 (12) |
N3—C11 | 1.172 (11) | C8—H8A | 0.9700 |
O1—C4 | 1.282 (9) | C8—H8B | 0.9700 |
S1—C11 | 1.612 (10) | C9—H9A | 0.9700 |
Br1—C1 | 1.911 (8) | C9—H9B | 0.9700 |
C1—C6 | 1.356 (12) | C10—H10A | 0.9600 |
C1—C2 | 1.368 (12) | C10—H10B | 0.9600 |
C2—C3 | 1.358 (12) | C10—H10C | 0.9600 |
O1—Cu1—N1 | 92.3 (3) | C6—C5—C4 | 121.6 (8) |
O1—Cu1—N3 | 89.5 (3) | C6—C5—C7 | 116.9 (7) |
N1—Cu1—N3 | 178.1 (3) | C4—C5—C7 | 121.4 (7) |
O1—Cu1—N2 | 168.3 (3) | C1—C6—C5 | 119.9 (8) |
N1—Cu1—N2 | 83.4 (3) | C1—C6—H6 | 120.1 |
N3—Cu1—N2 | 94.7 (3) | C5—C6—H6 | 120.1 |
C7—N1—C8 | 120.0 (7) | N1—C7—C5 | 125.2 (7) |
C7—N1—Cu1 | 126.0 (5) | N1—C7—H7 | 117.4 |
C8—N1—Cu1 | 113.9 (5) | C5—C7—H7 | 117.4 |
C10—N2—C9 | 112.8 (8) | N1—C8—C9 | 108.4 (7) |
C10—N2—Cu1 | 120.2 (7) | N1—C8—H8A | 110.0 |
C9—N2—Cu1 | 107.4 (5) | C9—C8—H8A | 110.0 |
C10—N2—H2A | 105.0 | N1—C8—H8B | 110.0 |
C9—N2—H2A | 105.0 | C9—C8—H8B | 110.0 |
Cu1—N2—H2A | 105.0 | H8A—C8—H8B | 108.4 |
C11—N3—Cu1 | 166.5 (7) | N2—C9—C8 | 108.1 (7) |
C4—O1—Cu1 | 126.5 (5) | N2—C9—H9A | 110.1 |
C6—C1—C2 | 120.7 (8) | C8—C9—H9A | 110.1 |
C6—C1—Br1 | 121.4 (6) | N2—C9—H9B | 110.1 |
C2—C1—Br1 | 117.9 (7) | C8—C9—H9B | 110.1 |
C3—C2—C1 | 121.1 (8) | H9A—C9—H9B | 108.4 |
C3—C2—H2 | 119.4 | N2—C10—H10A | 109.5 |
C1—C2—H2 | 119.4 | N2—C10—H10B | 109.5 |
C2—C3—C4 | 120.6 (7) | H10A—C10—H10B | 109.5 |
C2—C3—H3 | 119.7 | N2—C10—H10C | 109.5 |
C4—C3—H3 | 119.7 | H10A—C10—H10C | 109.5 |
O1—C4—C5 | 125.7 (7) | H10B—C10—H10C | 109.5 |
O1—C4—C3 | 118.1 (7) | N3—C11—S1 | 177.5 (9) |
C5—C4—C3 | 116.1 (7) |
D—H···A | D—H | H···A | D···A | D—H···A |
N2—H2A···S1i | 0.91 | 2.76 | 3.635 (9) | 162 |
Symmetry code: (i) x+1/2, −y+1/2, z+1/2. |
Experimental details
Crystal data | |
Chemical formula | [Cu(C10H12BrN2O)(NCS)] |
Mr | 377.75 |
Crystal system, space group | Monoclinic, P21/n |
Temperature (K) | 298 |
a, b, c (Å) | 5.952 (3), 19.660 (3), 12.718 (2) |
β (°) | 94.331 (3) |
V (Å3) | 1484.0 (8) |
Z | 4 |
Radiation type | Mo Kα |
µ (mm−1) | 4.30 |
Crystal size (mm) | 0.32 × 0.32 × 0.31 |
Data collection | |
Diffractometer | Bruker SMART CCD area-detector diffractometer |
Absorption correction | Multi-scan (SADABS; Sheldrick, 1996) |
Tmin, Tmax | 0.259, 0.267 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 11246, 2997, 1875 |
Rint | 0.071 |
(sin θ/λ)max (Å−1) | 0.628 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.076, 0.181, 1.11 |
No. of reflections | 2997 |
No. of parameters | 164 |
H-atom treatment | H-atom parameters constrained |
Δρmax, Δρmin (e Å−3) | 1.68, −0.84 |
Computer programs: SMART (Bruker, 1998), SAINT (Bruker, 1998), SHELXS97 (Sheldrick, 2008), SHELXL97 (Sheldrick, 2008), SHELXTL (Sheldrick, 2008).
D—H···A | D—H | H···A | D···A | D—H···A |
N2—H2A···S1i | 0.91 | 2.76 | 3.635 (9) | 162 |
Symmetry code: (i) x+1/2, −y+1/2, z+1/2. |
Acknowledgements
The author acknowledges support from the Scientific Research Foundation of Henan University of Science and Technology (project No. 05-072).
References
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This is an open-access article distributed under the terms of the Creative Commons Attribution (CC-BY) Licence, which permits unrestricted use, distribution, and reproduction in any medium, provided the original authors and source are cited.
Recently, we have reported on teh crystal structure alanyses of some metal complexes derived from Schiff base ligands (Ma, Lv et al., 2006; Ma, Gu et al., 2006; Ma, Wu et al., 2006; Ma et al., 2005). As part of a further investigation of the structures of such complexes, the title mononuclear copper(II) complex, (I), is reported on here.
In complex (I), the Cu atom is coordinated by two nitrogen atoms and one oxygen atom from a Schiff base ligand, and by one nitrogen atom from a thiocyanate anion, giving a square planar geometry (Fig. 1). All the bond lengths and angles related to the Cu atom in the complex are within normal ranges, and comparable to the values observed in other similar copper(II) complexes (Wei et al., 2007; Diao et al., 2007; Diao & Li, 2007). The four coordinating atoms around the Cu centre are approximately coplanar, giving a square-planar geometry with an average deviation of 0.090 (5) Å; the Cu atom lies 0.095 (2) Å above this plane. The C8—C9—N2—C10 torsion angle is 1.5 (3)°.
In the crystal structure of compound (I) symmetry related molecules are linked by an N—H···S hydrogen bond (Table 1).