supplementary materials


gk2080 scheme

Acta Cryst. (2007). E63, m1791    [ doi:10.1107/S160053680702689X ]

Bis[2,4-dibromo-6-(cyclopropyliminomethyl)phenolato]nickel(II)

L.-Z. Li and L.-H. Wang

Abstract top

The title compound, [Ni(C10H8Br2NO)2], is a mononuclear nickel(II) complex. The NiII atom, located on an inversion centre, exhibits a square-planar coordination geometry. The metal atom is bonded to two phenolate O atoms and two imine N atoms from two Schiff base ligands.

Comment top

Schiff base complexes have been of great interest for a long time (Chaturvedi, 1977; Archer & Wang, 1990; Costamagna et al., 1992; Yamada, 1999). These complexes play an important role in the development of coordination chemistry related to catalysis and enzymatic reactions, magnetism and molecular architectures. Recently, we have reported a few transition metal complexes (Wang & Li, 2007a,b; Li & Wang, 2007a). As an extension of the work on the structural investigation of these complexes, the title nickel(II) complex is reported here.

The title complex is a centrosymmetric mononuclear nickel(II) complex. The NiII atom, lying on the inversion centre, is four-coordinated and shows a square planar coordination geometry. It is bonded to two phenolate O and two imine N atoms from two Schiff base ligands. The Ni–O and Ni–N bond lengths are comparable to the corresponding values observed in other Schiff base nickel(II) complexes.

Related literature top

For related literature on Schiff base complexes, see: Chaturvedi (1977); Archer & Wang (1990); Costamagna et al. (1992); Yamada (1999); Li & Wang (2007); Wang & Li (2007a,b).

Experimental top

3,5-Dibromosalicylaldehyde (0.2 mmol, 56.4 mg) and cyclopropylamine (0.2 mmol, 11.5 mg) were dissolved in a methanol solution (20 ml). The mixture was stirred at room temperature for 30 min, giving a clear yellow solution. To this solution was added a methanol solution (5 ml) of Ni(NO3)2·6H2O (0.1 mmol, 29.1 mg) with stirring. The resulting mixture was stirred for a further 30 min at room temperature, giving a clear red solution. After allowing the solution to stand in air for a week, red block-shaped crystals were formed.

Refinement top

H atoms were placed in idealized positions and constrained to ride on their parent atoms, with C–H = 0.93–0.97 Å and Uiso(H) = 1.2Ueq(C).

Computing details top

Data collection: SMART (Bruker, 1998); cell refinement: SAINT (Bruker, 1998); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 1997a); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997a); molecular graphics: SHELXTL (Sheldrick, 1997b); software used to prepare material for publication: SHELXTL.

Figures top
[Figure 1] Fig. 1. Molecular structure of (I) at 30% probability level.
Bis(2,4-dibromo-6-cyclopropyliminomethylphenolato)nickel(II) top
Crystal data top
[Ni(C10H8Br2NO)2]F000 = 668
Mr = 694.70Dx = 2.217 Mg m3
Monoclinic, P21/cMo Kα radiation
λ = 0.71073 Å
a = 8.0170 (16) ÅCell parameters from 1834 reflections
b = 9.2420 (18) Åθ = 2.5–25.3º
c = 14.088 (3) ŵ = 8.63 mm1
β = 94.62 (3)ºT = 298 (2) K
V = 1040.4 (4) Å3Block, red
Z = 20.23 × 0.20 × 0.17 mm
Data collection top
Bruker SMART CCD area-detector
diffractometer
2362 independent reflections
Radiation source: fine-focus sealed tube1801 reflections with I > 2σ(I)
Monochromator: graphiteRint = 0.041
T = 298(2) Kθmax = 27.5º
ω scanθmin = 2.6º
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
h = 10→10
Tmin = 0.152, Tmax = 0.241k = 12→11
8738 measured reflectionsl = 18→17
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.036H-atom parameters constrained
wR(F2) = 0.084  w = 1/[σ2(Fo2) + (0.0393P)2]
where P = (Fo2 + 2Fc2)/3
S = 1.02(Δ/σ)max < 0.001
2362 reflectionsΔρmax = 0.51 e Å3
133 parametersΔρmin = 0.56 e Å3
Primary atom site location: structure-invariant direct methodsExtinction correction: none
Crystal data top
[Ni(C10H8Br2NO)2]V = 1040.4 (4) Å3
Mr = 694.70Z = 2
Monoclinic, P21/cMo Kα
a = 8.0170 (16) ŵ = 8.63 mm1
b = 9.2420 (18) ÅT = 298 (2) K
c = 14.088 (3) Å0.23 × 0.20 × 0.17 mm
β = 94.62 (3)º
Data collection top
Bruker SMART CCD area-detector
diffractometer
2362 independent reflections
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
1801 reflections with I > 2σ(I)
Tmin = 0.152, Tmax = 0.241Rint = 0.041
8738 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.036133 parameters
wR(F2) = 0.084H-atom parameters constrained
S = 1.02Δρmax = 0.51 e Å3
2362 reflectionsΔρmin = 0.56 e Å3
Special details top

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 > 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*/Ueq
Ni10.50000.00000.50000.02886 (18)
Br10.91324 (5)0.02357 (5)0.26991 (3)0.04253 (15)
Br21.30178 (6)0.38800 (5)0.48338 (3)0.05101 (16)
O10.6838 (3)0.0172 (3)0.43016 (19)0.0342 (6)
N10.6038 (4)0.1142 (3)0.6033 (2)0.0283 (7)
C10.8438 (5)0.1940 (4)0.5221 (3)0.0298 (8)
C20.8144 (5)0.0988 (4)0.4431 (3)0.0292 (8)
C30.9399 (5)0.0995 (4)0.3777 (3)0.0294 (8)
C41.0802 (5)0.1830 (4)0.3890 (3)0.0327 (9)
H41.16010.17820.34480.039*
C51.1037 (5)0.2754 (4)0.4667 (3)0.0335 (9)
C60.9869 (5)0.2807 (4)0.5324 (3)0.0357 (9)
H61.00300.34260.58440.043*
C70.7349 (5)0.1926 (4)0.5975 (3)0.0323 (9)
H70.76190.25530.64810.039*
C80.5247 (5)0.1218 (4)0.6926 (3)0.0327 (9)
H80.41040.16020.68720.039*
C90.5548 (6)0.0033 (5)0.7635 (3)0.0435 (11)
H9A0.63420.07160.74980.052*
H9B0.46060.02980.79680.052*
C100.6219 (5)0.1516 (5)0.7862 (3)0.0431 (11)
H10A0.74170.16640.78600.052*
H10B0.56800.20820.83300.052*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Ni10.0286 (4)0.0337 (4)0.0244 (4)0.0010 (3)0.0028 (3)0.0023 (3)
Br10.0411 (3)0.0576 (3)0.0295 (2)0.0009 (2)0.00693 (18)0.00779 (19)
Br20.0382 (3)0.0608 (3)0.0544 (3)0.0152 (2)0.0063 (2)0.0010 (2)
O10.0311 (15)0.0441 (17)0.0282 (15)0.0076 (13)0.0066 (12)0.0065 (12)
N10.0308 (18)0.0289 (17)0.0258 (16)0.0011 (14)0.0059 (13)0.0026 (13)
C10.031 (2)0.029 (2)0.030 (2)0.0037 (17)0.0048 (16)0.0030 (16)
C20.031 (2)0.033 (2)0.0234 (19)0.0064 (17)0.0015 (15)0.0053 (16)
C30.032 (2)0.035 (2)0.0219 (19)0.0047 (17)0.0021 (15)0.0017 (15)
C40.026 (2)0.043 (2)0.030 (2)0.0045 (18)0.0067 (16)0.0054 (17)
C50.028 (2)0.035 (2)0.037 (2)0.0020 (17)0.0028 (17)0.0078 (18)
C60.039 (2)0.038 (2)0.030 (2)0.0029 (19)0.0013 (17)0.0016 (17)
C70.037 (2)0.034 (2)0.0257 (19)0.0017 (18)0.0021 (16)0.0052 (16)
C80.035 (2)0.039 (2)0.025 (2)0.0066 (18)0.0084 (17)0.0064 (16)
C90.048 (3)0.050 (3)0.033 (2)0.002 (2)0.012 (2)0.0020 (19)
C100.042 (3)0.057 (3)0.032 (2)0.011 (2)0.0080 (19)0.009 (2)
Geometric parameters (Å, °) top
Ni1—O11.844 (3)C4—C51.389 (5)
Ni1—O1i1.844 (3)C4—H40.9300
Ni1—N1i1.931 (3)C5—C61.370 (5)
Ni1—N11.931 (3)C6—H60.9300
Br1—C31.896 (4)C7—H70.9300
Br2—C51.898 (4)C8—C91.489 (6)
O1—C21.291 (4)C8—C101.502 (5)
N1—C71.284 (5)C8—H80.9800
N1—C81.456 (5)C9—C101.498 (6)
C1—C61.398 (5)C9—H9A0.9700
C1—C21.423 (5)C9—H9B0.9700
C1—C71.429 (5)C10—H10A0.9700
C2—C31.418 (5)C10—H10B0.9700
C3—C41.363 (5)
O1—Ni1—O1i180.0C5—C6—C1120.6 (4)
O1—Ni1—N1i87.67 (12)C5—C6—H6119.7
O1i—Ni1—N1i92.33 (12)C1—C6—H6119.7
O1—Ni1—N192.33 (12)N1—C7—C1127.2 (3)
O1i—Ni1—N187.67 (12)N1—C7—H7116.4
N1i—Ni1—N1180.0C1—C7—H7116.4
C2—O1—Ni1130.5 (2)N1—C8—C9119.1 (3)
C7—N1—C8116.3 (3)N1—C8—C10122.4 (3)
C7—N1—Ni1124.5 (3)C9—C8—C1060.1 (3)
C8—N1—Ni1119.1 (2)N1—C8—H8114.8
C6—C1—C2121.3 (4)C9—C8—H8114.8
C6—C1—C7118.2 (4)C10—C8—H8114.8
C2—C1—C7120.2 (3)C8—C9—C1060.4 (3)
O1—C2—C3121.4 (3)C8—C9—H9A117.7
O1—C2—C1123.6 (3)C10—C9—H9A117.7
C3—C2—C1115.1 (3)C8—C9—H9B117.7
C4—C3—C2123.3 (3)C10—C9—H9B117.7
C4—C3—Br1118.2 (3)H9A—C9—H9B114.9
C2—C3—Br1118.5 (3)C9—C10—C859.5 (3)
C3—C4—C5119.9 (3)C9—C10—H10A117.8
C3—C4—H4120.1C8—C10—H10A117.8
C5—C4—H4120.1C9—C10—H10B117.8
C6—C5—C4119.9 (4)C8—C10—H10B117.8
C6—C5—Br2120.5 (3)H10A—C10—H10B115.0
C4—C5—Br2119.6 (3)
Symmetry codes: (i) −x+1, −y, −z+1.
Selected geometric parameters (Å, °) top
Ni1—O11.844 (3)Ni1—N11.931 (3)
O1—Ni1—O1i180.0O1—Ni1—N192.33 (12)
O1—Ni1—N1i87.67 (12)
Symmetry codes: (i) −x+1, −y, −z+1.
Acknowledgements top

The project is sponsored by the Scientific Research Foundation for the Returned Overseas Chinese Scholars, State Education Ministry (BZYO 7002).

references
References top

Archer, R. D. & Wang, B. (1990). Inorg. Chem. 29, 39–43.

Bruker (1998). SMART (Version 5.628) and SAINT (Version 6.02). Bruker AXS Inc., Madison, Wisconsin, USA.

Chaturvedi, K. K. (1977). J. Inorg. Nucl. Chem. 39, 901–903.

Costamagna, J., Vargas, J., Latorre, R., Alvarado, A. & Mena, G. (1992). Coord. Chem. Rev. 119, 67–88.

Li, L.-Z. & Wang, L.-H. (2007). Acta Cryst. E63, m749–m750.

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

Sheldrick, G. M. (1997a). SHELXS97 and SHELXL97. University of Göttingen, Germany.

Sheldrick, G. M. (1997b). SHELXTL. Version 5.1. Bruker AXS Inc., Madison, Wisconsin, USA.

Wang, L.-H. & Li, L.-Z. (2007a). Acta Cryst. E63, m1214–m1216.

Wang, L.-H. & Li, L.-Z. (2007b). Acta Cryst. E63, m1217–m1219.

Yamada, S. (1999). Coord. Chem. Rev. 190–192, 537–555.