Literature DB >> 21200550

Bis[2-(benzyl-imino-meth-yl)-4-chloro-phenolato-κN,O]nickel(II).

Zong-Xiao Li1, Xin-Li Zhang, Xiao-Hua Pu.   

Abstract

In the mononuclear centrosymmetric title compound, [Ni(C(14)H(11)ClNO)(2)], the Ni(II) atom, lying on a center of symmetry, is four-coordinated by two O atoms and two N atoms from two Schiff base ligands, forming a slightly distorted square-planar environment. The dihedral angle between the two aromatic rings of the ligand is 72.0 (2)°. No significant hydrogen bonding or π-π stacking inter-actions are observed.

Entities:  

Year:  2007        PMID: 21200550      PMCID: PMC2915132          DOI: 10.1107/S1600536807054943

Source DB:  PubMed          Journal:  Acta Crystallogr Sect E Struct Rep Online        ISSN: 1600-5368


Related literature

For bond-length data, see: Allen et al. (1987 ▶). For related literature, see: Christensen et al. (1997 ▶); Costes et al. (2005 ▶); Hu et al. (2005 ▶); Liu et al. (2006 ▶); Wallis & Cummings (1974 ▶); Yu (2006 ▶).

Experimental

Crystal data

[Ni(C14H11ClNO)2] M = 548.09 Monoclinic, a = 13.6785 (17) Å b = 10.5986 (14) Å c = 8.6560 (13) Å β = 107.529 (2)° V = 1196.6 (3) Å3 Z = 2 Mo Kα radiation μ = 1.06 mm−1 T = 298 (2) K 0.56 × 0.44 × 0.32 mm

Data collection

Bruker SMART CCD diffractometer Absorption correction: multi-scan (SADABS; Sheldrick, 1996 ▶) T min = 0.587, T max = 0.727 5718 measured reflections 2110 independent reflections 1506 reflections with I > 2σ(I) R int = 0.039

Refinement

R[F 2 > 2σ(F 2)] = 0.043 wR(F 2) = 0.124 S = 1.08 2110 reflections 160 parameters H-atom parameters constrained Δρmax = 0.53 e Å−3 Δρmin = −0.28 e Å−3 Data collection: SMART (Bruker, 1998 ▶); cell refinement: SAINT (Bruker, 2001 ▶); data reduction: SAIn class="Chemical">NT; program(s) used to solve structure: SHELXS97 (Sheldrick, 1997 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997 ▶); molecular graphics: SHELXTL (Bruker, 2001 ▶); software used to prepare material for publication: SHELXTL. Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536807054943/ci2496sup1.cif Structure factors: contains datablocks I. DOI: 10.1107/S1600536807054943/ci2496Isup2.hkl Additional supplementary materials: crystallographic information; 3D view; checkCIF report
[Ni(C14H11ClNO)2]F000 = 564
Mr = 548.09Dx = 1.521 Mg m3
Monoclinic, P21/cMo Kα radiation λ = 0.71073 Å
Hall symbol: -P 2ybcCell parameters from 1825 reflections
a = 13.6785 (17) Åθ = 2.5–25.2º
b = 10.5986 (14) ŵ = 1.06 mm1
c = 8.6560 (13) ÅT = 298 (2) K
β = 107.529 (2)ºRhombus, green
V = 1196.6 (3) Å30.56 × 0.44 × 0.32 mm
Z = 2
Bruker SMART CCD diffractometer2110 independent reflections
Radiation source: fine-focus sealed tube1506 reflections with I > 2σ(I)
Monochromator: graphiteRint = 0.039
T = 298(2) Kθmax = 25.0º
φ and ω scansθmin = 2.5º
Absorption correction: multi-scan(SADABS; Sheldrick, 1996)h = −16→12
Tmin = 0.587, Tmax = 0.727k = −12→8
5718 measured reflectionsl = −10→10
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.043H-atom parameters constrained
wR(F2) = 0.124  w = 1/[σ2(Fo2) + (0.057P)2 + 0.6708P] where P = (Fo2 + 2Fc2)/3
S = 1.08(Δ/σ)max = 0.001
2110 reflectionsΔρmax = 0.53 e Å3
160 parametersΔρmin = −0.28 e Å3
Primary atom site location: structure-invariant direct methodsExtinction correction: none
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.
xyzUiso*/Ueq
Ni10.00000.50000.00000.0329 (2)
Cl10.48272 (9)0.77502 (16)0.44350 (18)0.0919 (6)
N10.0104 (2)0.6504 (3)0.1288 (3)0.0316 (7)
O10.13607 (19)0.4664 (3)0.0829 (3)0.0472 (7)
C10.0949 (3)0.7006 (4)0.2141 (4)0.0354 (8)
H10.08990.77370.27050.043*
C20.1963 (3)0.6549 (4)0.2309 (4)0.0359 (9)
C30.2107 (3)0.5393 (4)0.1629 (4)0.0365 (9)
C40.3123 (3)0.4982 (4)0.1878 (5)0.0467 (10)
H40.32400.42080.14610.056*
C50.3939 (3)0.5699 (5)0.2720 (5)0.0528 (11)
H50.46030.54180.28550.063*
C60.3779 (3)0.6840 (5)0.3372 (5)0.0520 (11)
C70.2809 (3)0.7283 (4)0.3197 (5)0.0451 (10)
H70.27100.80480.36530.054*
C8−0.0831 (3)0.7179 (4)0.1351 (4)0.0369 (9)
H8A−0.12540.73530.02530.044*
H8B−0.06330.79820.18930.044*
C9−0.1461 (2)0.6457 (3)0.2219 (4)0.0316 (8)
C10−0.1084 (3)0.5490 (4)0.3262 (4)0.0393 (9)
H10−0.04110.52250.34380.047*
C11−0.1688 (3)0.4897 (4)0.4064 (5)0.0469 (10)
H11−0.14220.42330.47670.056*
C12−0.2678 (3)0.5281 (4)0.3827 (5)0.0533 (12)
H12−0.30870.48780.43610.064*
C13−0.3059 (3)0.6264 (5)0.2799 (5)0.0553 (12)
H13−0.37250.65440.26510.066*
C14−0.2457 (3)0.6839 (4)0.1983 (5)0.0458 (10)
H14−0.27270.74930.12650.055*
U11U22U33U12U13U23
Ni10.0295 (4)0.0348 (4)0.0367 (4)−0.0008 (3)0.0133 (3)−0.0002 (3)
Cl10.0415 (7)0.1240 (14)0.1083 (11)−0.0314 (7)0.0197 (7)−0.0503 (10)
N10.0291 (15)0.0328 (17)0.0363 (16)0.0014 (13)0.0152 (13)0.0075 (13)
O10.0307 (14)0.0475 (19)0.0590 (17)0.0032 (11)0.0070 (13)−0.0124 (13)
C10.040 (2)0.031 (2)0.040 (2)−0.0020 (16)0.0191 (17)0.0023 (16)
C20.0311 (19)0.043 (2)0.035 (2)−0.0034 (17)0.0123 (15)0.0036 (18)
C30.033 (2)0.045 (2)0.035 (2)−0.0018 (16)0.0137 (17)0.0024 (17)
C40.035 (2)0.053 (3)0.054 (2)0.0008 (19)0.0156 (18)−0.010 (2)
C50.031 (2)0.069 (3)0.059 (3)−0.001 (2)0.0156 (19)−0.005 (2)
C60.034 (2)0.073 (3)0.050 (2)−0.014 (2)0.0137 (18)−0.008 (2)
C70.037 (2)0.049 (3)0.051 (2)−0.0103 (18)0.0162 (18)−0.008 (2)
C80.038 (2)0.032 (2)0.043 (2)0.0018 (16)0.0163 (17)0.0026 (17)
C90.0308 (18)0.033 (2)0.0309 (19)−0.0009 (15)0.0095 (15)−0.0046 (16)
C100.039 (2)0.037 (2)0.043 (2)0.0046 (17)0.0142 (17)0.0024 (18)
C110.055 (3)0.043 (2)0.047 (2)0.003 (2)0.0222 (19)0.009 (2)
C120.049 (2)0.067 (3)0.053 (2)−0.012 (2)0.029 (2)−0.001 (2)
C130.035 (2)0.079 (4)0.055 (3)0.005 (2)0.019 (2)0.002 (2)
C140.040 (2)0.055 (3)0.043 (2)0.0121 (19)0.0139 (18)0.010 (2)
Ni1—O11.817 (2)C6—C71.372 (5)
Ni1—O1i1.817 (2)C7—H70.93
Ni1—N1i1.926 (3)C8—C91.510 (5)
Ni1—N11.926 (3)C8—H8A0.97
Cl1—C61.743 (4)C8—H8B0.97
N1—C11.284 (4)C9—C101.361 (5)
N1—C81.480 (4)C9—C141.377 (5)
O1—C31.301 (4)C10—C111.380 (5)
C1—C21.434 (5)C10—H100.93
C1—H10.93C11—C121.369 (6)
C2—C31.399 (5)C11—H110.93
C2—C71.414 (5)C12—C131.367 (6)
C3—C41.409 (5)C12—H120.93
C4—C51.365 (6)C13—C141.378 (6)
C4—H40.93C13—H130.93
C5—C61.379 (6)C14—H140.93
C5—H50.93
O1—Ni1—O1i180C6—C7—C2118.6 (4)
O1—Ni1—N1i87.39 (11)C6—C7—H7120.7
O1i—Ni1—N1i92.61 (11)C2—C7—H7120.7
O1—Ni1—N192.61 (11)N1—C8—C9113.7 (3)
O1i—Ni1—N187.39 (11)N1—C8—H8A108.8
N1i—Ni1—N1180.00 (14)C9—C8—H8A108.8
C1—N1—C8114.6 (3)N1—C8—H8B108.8
C1—N1—Ni1124.9 (2)C9—C8—H8B108.8
C8—N1—Ni1120.5 (2)H8A—C8—H8B107.7
C3—O1—Ni1129.8 (3)C10—C9—C14118.7 (3)
N1—C1—C2126.4 (4)C10—C9—C8123.5 (3)
N1—C1—H1116.8C14—C9—C8117.7 (3)
C2—C1—H1116.8C9—C10—C11120.8 (3)
C3—C2—C7120.9 (3)C9—C10—H10119.6
C3—C2—C1120.5 (3)C11—C10—H10119.6
C7—C2—C1118.5 (4)C12—C11—C10120.3 (4)
O1—C3—C2123.8 (3)C12—C11—H11119.9
O1—C3—C4118.5 (4)C10—C11—H11119.9
C2—C3—C4117.6 (3)C13—C12—C11119.4 (4)
C5—C4—C3121.3 (4)C13—C12—H12120.3
C5—C4—H4119.3C11—C12—H12120.3
C3—C4—H4119.3C12—C13—C14120.1 (4)
C4—C5—C6120.1 (4)C12—C13—H13120.0
C4—C5—H5120.0C14—C13—H13120.0
C6—C5—H5120.0C9—C14—C13120.7 (4)
C7—C6—C5121.4 (4)C9—C14—H14119.6
C7—C6—Cl1118.9 (4)C13—C14—H14119.6
C5—C6—Cl1119.6 (3)
O1—Ni1—N1—C19.0 (3)C4—C5—C6—C70.0 (7)
O1i—Ni1—N1—C1−171.0 (3)C4—C5—C6—Cl1−179.7 (3)
O1—Ni1—N1—C8−171.1 (2)C5—C6—C7—C2−0.8 (6)
O1i—Ni1—N1—C88.9 (2)Cl1—C6—C7—C2178.9 (3)
N1i—Ni1—O1—C3164.0 (3)C3—C2—C7—C60.4 (5)
N1—Ni1—O1—C3−16.0 (3)C1—C2—C7—C6179.3 (3)
C8—N1—C1—C2179.6 (3)C1—N1—C8—C9−111.5 (3)
Ni1—N1—C1—C2−0.4 (5)Ni1—N1—C8—C968.5 (3)
N1—C1—C2—C3−6.1 (6)N1—C8—C9—C1019.2 (5)
N1—C1—C2—C7174.9 (3)N1—C8—C9—C14−163.5 (3)
Ni1—O1—C3—C214.1 (5)C14—C9—C10—C110.4 (6)
Ni1—O1—C3—C4−168.2 (3)C8—C9—C10—C11177.6 (4)
C7—C2—C3—O1178.5 (3)C9—C10—C11—C12−0.5 (6)
C1—C2—C3—O1−0.5 (5)C10—C11—C12—C13−0.5 (6)
C7—C2—C3—C40.7 (5)C11—C12—C13—C141.5 (7)
C1—C2—C3—C4−178.2 (3)C10—C9—C14—C130.7 (6)
O1—C3—C4—C5−179.4 (4)C8—C9—C14—C13−176.8 (4)
C2—C3—C4—C5−1.5 (6)C12—C13—C14—C9−1.6 (7)
C3—C4—C5—C61.1 (6)
Ni1—O11.817 (2)
Ni1—N11.926 (3)
O1—Ni1—O1i180
O1—Ni1—N1i87.39 (11)
O1—Ni1—N192.61 (11)

Symmetry code: (i) .

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1.  Synthesis, crystal structures, and nonlinear optical (NLO) properties of new Schiff-base nickel(II) complexes. Toward a new type of molecular switch?

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