supplementary materials


sj2505 scheme

Acta Cryst. (2008). E64, m844    [ doi:10.1107/S1600536808015559 ]

Bis[(E)-4-chloro-2-(2-furylmethyliminomethyl)phenolato]iron(II)

D.-S. Xia, W. Chen, J. Huang and Q.-F. Zeng

Abstract top

The Fe atom of the title compound, [Fe(C12H9ClNO2)2], lies on a crystallographic twofold rotation axis. The FeII atom is four-coordinated in a tetrahedral geometry by the O and N atoms of the two Schiff base ligands. The O atom of the furan substituent in the ligand unit is not involved in coordination to the Fe atom.

Comment top

As part of our ongoing interest in the structure of iron complexes (Zhu et al., 2003), we report herein the crystal structure of the title compound, a new mononuclear iron(II) complex, (I), Fig. 1, derived from the Schiff base ligand 4-chloro-2-[(furan-2-ylmethylimino)methyl]phenol.

Compound (I) possesses crystallographic two-fold symmetry. The FeII atom in (I) is four-coordinate in a tetrahedral geometry, binding to the O and N atoms of two Schiff base ligands. The O atom of the furan substituent in the ligand lies well away from the coordination sphere of the Fe atom. The coordinate bond values (Table 1) are comparable to values observed in other iron(II) complexes (Chen & Wang, 2006; Chen et al., 2007; Ran et al., 2006; Ye et al., 2007).

Related literature top

For related structures, see: Chen & Wang (2006); Chen et al. (2007); Ran et al. (2006); Ye et al. (2007); Zhu et al. (2003).

Experimental top

5-Chlorosalicylaldehyde (62.4 mg, 0.2 mmol), furan-2-ylmethylamine (19.4 mg, 0.2 mmol), and FeCl2 (12.6 mg, 0.1 mmol) were dissolved in methanol (30 ml). The mixture was stirred for 30 min at room temperature. The resulting solution was kept still in air for a few days, yielding brown crystals.

Refinement top

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

Computing details top

Data collection: SMART (Bruker, 1998); cell refinement: 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).

Figures top
[Figure 1] Fig. 1. The structure of (I) showing 30% probability displacement ellipsoids and the atom-numbering scheme. Numbered atoms are related to un-numbered atoms by the symmetry code 1-x, y, 1-z.
Bis[(E)-4-chloro-2-(2-furylmethyliminomethyl)phenolato]iron(II) top
Crystal data top
[Fe(C12H9ClNO2)2]F000 = 536
Mr = 525.15Dx = 1.529 Mg m3
Monoclinic, C2Mo Kα radiation
λ = 0.71073 Å
Hall symbol: C 2yCell parameters from 823 reflections
a = 22.550 (4) Åθ = 2.4–26.2º
b = 4.6270 (6) ŵ = 0.93 mm1
c = 13.822 (3) ÅT = 298 (2) K
β = 127.73 (3)ºBlock, brown
V = 1140.6 (4) Å30.21 × 0.21 × 0.20 mm
Z = 2
Data collection top
Bruker SMART CCD area-detector
diffractometer
1262 independent reflections
Radiation source: fine-focus sealed tube973 reflections with I > 2σ(I)
Monochromator: graphiteRint = 0.035
T = 298(2) Kθmax = 26.0º
ω scansθmin = 1.9º
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
h = 21→27
Tmin = 0.829, Tmax = 0.836k = 5→0
1314 measured reflectionsl = 17→0
Refinement top
Refinement on F2Hydrogen site location: inferred from neighbouring sites
Least-squares matrix: fullH-atom parameters constrained
R[F2 > 2σ(F2)] = 0.060  w = 1/[σ2(Fo2) + (0.1149P)2 + 2.2051P]
where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.203(Δ/σ)max = 0.001
S = 1.06Δρmax = 0.60 e Å3
1262 reflectionsΔρmin = 0.40 e Å3
151 parametersExtinction correction: SHELXL97 (Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
1 restraintExtinction coefficient: 0.011 (3)
Primary atom site location: structure-invariant direct methodsAbsolute structure: Flack (1983), 0 Friedel pairs
Secondary atom site location: difference Fourier mapFlack parameter: 0.02 (9)
Crystal data top
[Fe(C12H9ClNO2)2]V = 1140.6 (4) Å3
Mr = 525.15Z = 2
Monoclinic, C2Mo Kα
a = 22.550 (4) ŵ = 0.93 mm1
b = 4.6270 (6) ÅT = 298 (2) K
c = 13.822 (3) Å0.21 × 0.21 × 0.20 mm
β = 127.73 (3)º
Data collection top
Bruker SMART CCD area-detector
diffractometer
1262 independent reflections
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
973 reflections with I > 2σ(I)
Tmin = 0.829, Tmax = 0.836Rint = 0.035
1314 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.060H-atom parameters constrained
wR(F2) = 0.203Δρmax = 0.60 e Å3
S = 1.06Δρmin = 0.40 e Å3
1262 reflectionsAbsolute structure: Flack (1983), 0 Friedel pairs
151 parametersFlack parameter: 0.02 (9)
1 restraint
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*/Ueq
Fe10.50000.5044 (3)0.50000.0419 (6)
Cl10.87863 (17)0.7649 (11)1.0179 (3)0.0929 (13)
N10.5246 (5)0.728 (2)0.6435 (8)0.055 (2)
O10.5933 (4)0.313 (2)0.5865 (7)0.067 (2)
O20.4619 (6)0.600 (3)0.7844 (9)0.102 (4)
C10.6584 (5)0.630 (3)0.7611 (9)0.053 (2)
C20.6554 (5)0.419 (2)0.6848 (9)0.053 (3)
C30.7253 (6)0.309 (3)0.7192 (11)0.069 (3)
H30.72500.16860.67090.083*
C40.7929 (6)0.406 (3)0.8218 (11)0.068 (3)
H40.83770.33170.84290.081*
C50.7933 (6)0.620 (3)0.8943 (10)0.065 (3)
C60.7284 (6)0.737 (3)0.8663 (10)0.070 (3)
H60.73000.88240.91450.084*
C70.5937 (6)0.759 (3)0.7390 (10)0.066 (3)
H70.60210.87860.80030.079*
C80.4677 (6)0.890 (3)0.6455 (11)0.067 (3)
H8A0.49261.03360.71000.080*
H8B0.43290.98820.56810.080*
C90.4259 (6)0.683 (3)0.6671 (10)0.061 (3)
C100.4146 (12)0.427 (6)0.786 (2)0.137 (10)
H100.42420.34980.85600.164*
C110.3509 (10)0.381 (4)0.6710 (18)0.105 (6)
H110.31090.26060.64660.126*
C120.3594 (7)0.555 (4)0.5982 (13)0.087 (5)
H120.32380.57810.51410.104*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Fe10.0384 (9)0.0462 (11)0.0399 (9)0.0000.0233 (7)0.000
Cl10.0661 (17)0.122 (3)0.0664 (18)0.012 (2)0.0279 (15)0.017 (2)
N10.062 (5)0.047 (5)0.065 (5)0.000 (5)0.044 (4)0.005 (4)
O10.065 (4)0.068 (6)0.066 (4)0.001 (4)0.040 (4)0.017 (4)
O20.093 (6)0.136 (12)0.089 (6)0.016 (7)0.062 (5)0.022 (7)
C10.052 (5)0.054 (6)0.053 (5)0.001 (5)0.032 (5)0.006 (5)
C20.053 (5)0.050 (8)0.053 (5)0.005 (5)0.031 (5)0.009 (5)
C30.061 (6)0.062 (8)0.088 (8)0.007 (6)0.048 (6)0.008 (7)
C40.056 (6)0.070 (9)0.081 (7)0.012 (6)0.043 (6)0.019 (7)
C50.048 (6)0.081 (9)0.055 (6)0.001 (6)0.026 (5)0.013 (6)
C60.071 (7)0.077 (9)0.059 (6)0.001 (7)0.038 (6)0.010 (7)
C70.074 (7)0.067 (8)0.054 (6)0.004 (7)0.038 (6)0.002 (6)
C80.070 (7)0.059 (7)0.079 (7)0.019 (6)0.049 (6)0.009 (6)
C90.061 (6)0.067 (8)0.070 (7)0.011 (6)0.048 (6)0.005 (6)
C100.161 (17)0.15 (3)0.199 (19)0.037 (18)0.158 (17)0.06 (2)
C110.112 (12)0.085 (11)0.167 (17)0.000 (11)0.110 (13)0.004 (13)
C120.080 (8)0.088 (14)0.102 (9)0.001 (9)0.061 (8)0.007 (9)
Geometric parameters (Å, °) top
Fe1—O11.888 (8)C3—H30.9300
Fe1—O1i1.888 (8)C4—C51.402 (17)
Fe1—N11.992 (8)C4—H40.9300
Fe1—N1i1.992 (8)C5—C61.377 (16)
Cl1—C51.746 (12)C6—H60.9300
N1—C71.294 (13)C7—H70.9300
N1—C81.499 (12)C8—C91.493 (16)
O1—C21.310 (12)C8—H8A0.9700
O2—C101.34 (2)C8—H8B0.9700
O2—C91.352 (14)C9—C121.328 (18)
C1—C21.411 (14)C10—C111.35 (2)
C1—C71.424 (15)C10—H100.9300
C1—C61.429 (15)C11—C121.39 (2)
C2—C31.431 (15)C11—H110.9300
C3—C41.374 (16)C12—H120.9300
O1—Fe1—O1i124.0 (6)C4—C5—Cl1119.4 (9)
O1—Fe1—N195.2 (3)C5—C6—C1118.1 (13)
O1i—Fe1—N1113.5 (3)C5—C6—H6121.0
O1—Fe1—N1i113.5 (3)C1—C6—H6121.0
O1i—Fe1—N1i95.2 (3)N1—C7—C1127.6 (11)
N1—Fe1—N1i117.3 (5)N1—C7—H7116.2
C7—N1—C8115.9 (9)C1—C7—H7116.2
C7—N1—Fe1120.0 (8)C9—C8—N1109.7 (10)
C8—N1—Fe1123.9 (7)C9—C8—H8A109.7
C2—O1—Fe1123.4 (7)N1—C8—H8A109.7
C10—O2—C9106.7 (14)C9—C8—H8B109.7
C2—C1—C7123.7 (10)N1—C8—H8B109.7
C2—C1—C6121.3 (10)H8A—C8—H8B108.2
C7—C1—C6115.0 (11)C12—C9—O2108.5 (12)
O1—C2—C1124.5 (9)C12—C9—C8135.8 (12)
O1—C2—C3118.3 (10)O2—C9—C8115.7 (11)
C1—C2—C3117.3 (9)O2—C10—C11111.3 (16)
C4—C3—C2121.8 (12)O2—C10—H10124.4
C4—C3—H3119.1C11—C10—H10124.4
C2—C3—H3119.1C10—C11—C12103.7 (16)
C3—C4—C5119.1 (10)C10—C11—H11128.2
C3—C4—H4120.5C12—C11—H11128.2
C5—C4—H4120.5C9—C12—C11109.7 (14)
C6—C5—C4122.4 (11)C9—C12—H12125.2
C6—C5—Cl1117.9 (11)C11—C12—H12125.2
Symmetry codes: (i) −x+1, y, −z+1.
Table 1
Selected geometric parameters (Å, °)
top
Fe1—O11.888 (8)Fe1—N11.992 (8)
O1—Fe1—O1i124.0 (6)O1—Fe1—N1i113.5 (3)
O1—Fe1—N195.2 (3)N1—Fe1—N1i117.3 (5)
Symmetry codes: (i) −x+1, y, −z+1.
Acknowledgements top

no acknowledgements

references
References top

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

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Ran, J.-W., Gong, D.-J. & Li, Y.-H. (2006). Acta Cryst. E62, m2668–m2669.

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Ye, Y.-H., Han, Y., Chen, T.-T. & Liu, C.-H. (2007). Acta Cryst. E63, m1963.

Zhu, H.-L., Xia, D.-S., Zeng, Q.-F., Wang, Z.-G. & Wang, D.-Q. (2003). Acta Cryst. E59, m1020–m1021.