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Acta Cryst. (2008). E64, m646-m647    [ doi:10.1107/S1600536808009562 ]

Bis{2-methoxy-6-[3-(methylamino)propyliminomethyl]phenolato}nickel(II) bis(perchlorate)

Y.-T. He

Abstract top

The asymmetric unit of the title compound, [Ni(C12H18N2O2)2](ClO4)2, consists of one-half of a centrosymmetric mononuclear Schiff base nickel(II) complex cation and one perchlorate anion. The NiII ion, lying on the inversion center, is coordinated by two N atoms and two O atoms from two Schiff base ligands, forming a square-planar geometry. The crystal packing is stabilized by N-H...O hydrogen bonds.

Comment top

Nickel(II) complexes with Schiff base ligands have been of great interest in coordination chemistry related to molecular structures and catalytical applications (Chen et al., 2008; Holm, 1960; Arıcı et al., 2005). Metal complexes derived from Schiff bases have been widely studied (Ma, Lv et al., 2006; Ma, Gu et al., 2006; Ma, Wu et al., 2006; Ma et al., 2005). However, the complexes derived from the Schiff base ligand 2-methoxy-6-[(3-methylaminopropylimino)methyl]phenol have never been reported. The author reports herein the title mononuclear nickel(II) complex.

The title compound consists of a centrosymmetric nickel(II) complex cation and two perchlorate anions (Fig. 1). The NiII ion, lying on the inversion center, is coordinated by two nitrogen atoms and two oxygen atoms from two Schiff base ligands, giving a square planar geometry. All the bond lengths and angles (Table 1) involving the NiII atom are within normal ranges, and comparable to values observed in other Schiff base nickel(II) complexes (Zhu et al., 2004; Zhao, 2007; Bian et al., 2004; Skovsgaard et al., 2005). The N1—C8—C9—C10 and C9—C10—N2—C11 torsion angles are 55.0 (3) and 2.7 (3)°, respectively. The crystal packing is stabilized by N—H···O hydrogen bonds (Table 2).

Related literature top

For related structures, see: Arıcı et al. (2005); Bian et al. (2004); Chen et al. (2008); Holm (1960); Ma, Gu et al. (2006); Ma, Lv et al. (2006); Ma, Wu et al. (2006); Ma, Wu et al. (2005); Skovsgaard et al. (2005); Zhao (2007); Zhu et al. (2004).

Experimental top

N-Methylpropane-1,3-diamine (0.5 mmol, 44.0 mg) and 3-methoxysalicylaldehyde (0.5 mmol, 76.0 mg) were dissolved in methanol (30 ml). The mixture was stirred for 1 h to obtain a clear yellow solution. To the solution was added with stirring a methanol solution (20 ml) of nickel(II) perchlorate (0.5 mmol, 192.0 mg). After keeping the resulting solution in air for a few days, red block-shaped crystals were formed.

Refinement top

All H atoms were placed in geometrically idealized positions and constrained to ride on their parent atoms with C-H = 0.93–0.97 Å, N-H = 0.90 Å, and with Uiso(H) = 1.2Ueq(C,N) and 1.5Ueq(methyl 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: SHELXL97 (Sheldrick, 2008).

Figures top
[Figure 1] Fig. 1. The molecular structure of the title compound, showing 30% probability displacement ellipsoids. Unlabelled atoms are related to labelled atoms by the symmetry operation (1 - x, 1 - y, 1 - z).
Bis{2-methoxy-6-[3-(methylamino)propyliminomethyl]phenolato}nickel(II) bis(perchlorate) top
Crystal data top
[Ni(C12H18N2O2)2](ClO4)2F000 = 1464
Mr = 702.18Dx = 1.489 Mg m3
Orthorhombic, PbcaMo Kα radiation
λ = 0.71073 Å
Hall symbol: -P 2ac 2abCell parameters from 3048 reflections
a = 13.557 (5) Åθ = 2.3–25.3º
b = 13.302 (5) ŵ = 0.86 mm1
c = 17.371 (7) ÅT = 298 (2) K
V = 3133 (2) Å3Block, red
Z = 40.33 × 0.28 × 0.27 mm
Data collection top
Bruker SMART CCD area-detector
diffractometer
3276 independent reflections
Radiation source: fine-focus sealed tube2125 reflections with I > 2σ(I)
Monochromator: graphiteRint = 0.042
T = 298(2) Kθmax = 26.6º
ω scansθmin = 2.4º
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
h = 8→17
Tmin = 0.766, Tmax = 0.802k = 16→15
16728 measured reflectionsl = 19→21
Refinement top
Refinement on F2Hydrogen site location: inferred from neighbouring sites
Least-squares matrix: fullH-atom parameters constrained
R[F2 > 2σ(F2)] = 0.055  w = 1/[σ2(Fo2) + (0.0892P)2 + 4.466P]
where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.188(Δ/σ)max = 0.001
S = 1.04Δρmax = 0.97 e Å3
3276 reflectionsΔρmin = 0.55 e Å3
199 parametersExtinction correction: SHELXL97 (Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methodsExtinction coefficient: 0.0023 (6)
Secondary atom site location: difference Fourier map
Crystal data top
[Ni(C12H18N2O2)2](ClO4)2V = 3133 (2) Å3
Mr = 702.18Z = 4
Orthorhombic, PbcaMo Kα
a = 13.557 (5) ŵ = 0.86 mm1
b = 13.302 (5) ÅT = 298 (2) K
c = 17.371 (7) Å0.33 × 0.28 × 0.27 mm
Data collection top
Bruker SMART CCD area-detector
diffractometer
3276 independent reflections
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
2125 reflections with I > 2σ(I)
Tmin = 0.766, Tmax = 0.802Rint = 0.042
16728 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.055199 parameters
wR(F2) = 0.188H-atom parameters constrained
S = 1.04Δρmax = 0.97 e Å3
3276 reflectionsΔρmin = 0.55 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 > 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.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
Ni10.50000.50000.50000.0412 (3)
Cl10.39978 (9)0.29292 (9)0.63654 (7)0.0623 (4)
O10.5954 (2)0.5558 (2)0.56985 (16)0.0550 (8)
O20.6861 (3)0.7085 (3)0.6382 (2)0.0792 (11)
O30.4646 (5)0.3472 (5)0.5938 (4)0.178 (3)
O40.4518 (5)0.2905 (5)0.7084 (4)0.169 (3)
O50.3852 (5)0.1987 (5)0.6207 (7)0.260 (6)
O60.3118 (3)0.3474 (4)0.6470 (3)0.1112 (15)
N10.6046 (3)0.4103 (3)0.45407 (18)0.0497 (8)
N20.4565 (3)0.4199 (3)0.2818 (2)0.0604 (10)
H2A0.43510.42110.33080.072*
H2B0.43630.36150.26080.072*
C10.7430 (4)0.5058 (3)0.5061 (2)0.0549 (11)
C20.6908 (3)0.5687 (3)0.5551 (2)0.0495 (10)
C30.7427 (4)0.6482 (4)0.5911 (2)0.0586 (11)
C40.8418 (4)0.6607 (4)0.5796 (3)0.0715 (14)
H40.87470.71320.60400.086*
C50.8935 (4)0.5960 (5)0.5320 (4)0.0797 (16)
H50.96110.60440.52510.096*
C60.8456 (4)0.5204 (4)0.4957 (3)0.0715 (15)
H60.88060.47740.46340.086*
C70.6969 (3)0.4249 (3)0.4641 (2)0.0563 (11)
H70.73910.37800.44180.068*
C80.5803 (4)0.3206 (3)0.4076 (3)0.0633 (12)
H8A0.51020.30740.41180.076*
H8B0.61500.26300.42860.076*
C90.6073 (4)0.3317 (4)0.3228 (3)0.0731 (15)
H9A0.67860.33480.31870.088*
H9B0.58580.27160.29590.088*
C100.5648 (4)0.4214 (4)0.2820 (3)0.0713 (14)
H10A0.58740.48230.30720.086*
H10B0.58860.42260.22940.086*
C110.4092 (6)0.5042 (4)0.2391 (4)0.099 (2)
H11A0.43230.56710.25940.149*
H11B0.33890.50020.24500.149*
H11C0.42600.49970.18560.149*
C120.7201 (6)0.8047 (4)0.6537 (4)0.113 (2)
H12A0.77550.80100.68800.169*
H12B0.66840.84330.67710.169*
H12C0.74000.83630.60650.169*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Ni10.0409 (4)0.0501 (4)0.0326 (4)0.0002 (3)0.0013 (3)0.0056 (3)
Cl10.0584 (7)0.0553 (6)0.0733 (8)0.0012 (5)0.0005 (6)0.0103 (5)
O10.0486 (17)0.073 (2)0.0437 (15)0.0064 (14)0.0031 (13)0.0133 (14)
O20.082 (3)0.078 (2)0.078 (2)0.0215 (19)0.0081 (19)0.0288 (19)
O30.144 (5)0.192 (6)0.197 (6)0.044 (4)0.085 (5)0.123 (5)
O40.184 (6)0.177 (6)0.146 (5)0.022 (5)0.090 (5)0.013 (4)
O50.145 (6)0.115 (5)0.519 (17)0.000 (4)0.079 (7)0.150 (8)
O60.081 (3)0.119 (4)0.133 (4)0.035 (3)0.008 (3)0.024 (3)
N10.057 (2)0.0515 (19)0.0406 (18)0.0053 (16)0.0010 (15)0.0024 (14)
N20.078 (3)0.061 (2)0.0424 (19)0.008 (2)0.0029 (18)0.0111 (17)
C10.047 (2)0.069 (3)0.049 (2)0.009 (2)0.0043 (19)0.009 (2)
C20.046 (2)0.063 (3)0.039 (2)0.0010 (19)0.0043 (17)0.0042 (18)
C30.062 (3)0.067 (3)0.046 (2)0.009 (2)0.004 (2)0.000 (2)
C40.059 (3)0.083 (4)0.072 (3)0.016 (3)0.012 (3)0.008 (3)
C50.044 (3)0.100 (4)0.095 (4)0.006 (3)0.007 (3)0.010 (4)
C60.047 (3)0.094 (4)0.073 (3)0.012 (3)0.002 (2)0.005 (3)
C70.054 (3)0.066 (3)0.049 (2)0.015 (2)0.000 (2)0.001 (2)
C80.073 (3)0.049 (2)0.069 (3)0.008 (2)0.004 (2)0.006 (2)
C90.071 (3)0.083 (4)0.065 (3)0.005 (3)0.004 (2)0.034 (3)
C100.082 (4)0.082 (4)0.049 (3)0.019 (3)0.016 (2)0.019 (2)
C110.140 (6)0.083 (4)0.075 (4)0.011 (4)0.027 (4)0.002 (3)
C120.159 (7)0.066 (4)0.114 (5)0.024 (4)0.037 (5)0.007 (4)
Geometric parameters (Å, °) top
Ni1—O1i1.922 (3)C3—C41.369 (7)
Ni1—O11.922 (3)C4—C51.385 (8)
Ni1—N12.018 (3)C4—H40.93
Ni1—N1i2.018 (3)C5—C61.353 (8)
Cl1—O51.298 (6)C5—H50.93
Cl1—O31.358 (5)C6—H60.93
Cl1—O61.408 (4)C7—H70.93
Cl1—O41.434 (5)C8—C91.525 (7)
O1—C21.329 (5)C8—H8A0.97
O2—C31.378 (6)C8—H8B0.97
O2—C121.386 (6)C9—C101.502 (8)
N1—C71.278 (5)C9—H9A0.97
N1—C81.477 (5)C9—H9B0.97
N2—C101.469 (7)C10—H10A0.97
N2—C111.489 (6)C10—H10B0.97
N2—H2A0.90C11—H11A0.96
N2—H2B0.90C11—H11B0.96
C1—C21.389 (6)C11—H11C0.96
C1—C61.416 (7)C12—H12A0.96
C1—C71.443 (6)C12—H12B0.96
C2—C31.416 (6)C12—H12C0.96
O1i—Ni1—O1180C4—C5—H5120.1
O1i—Ni1—N189.70 (13)C5—C6—C1120.9 (5)
O1—Ni1—N190.30 (14)C5—C6—H6119.5
O1i—Ni1—N1i90.30 (14)C1—C6—H6119.5
O1—Ni1—N1i89.70 (13)N1—C7—C1127.3 (4)
N1—Ni1—N1i180N1—C7—H7116.3
O5—Cl1—O3119.7 (6)C1—C7—H7116.3
O5—Cl1—O6113.3 (4)N1—C8—C9113.3 (4)
O3—Cl1—O6110.2 (3)N1—C8—H8A108.9
O5—Cl1—O4103.7 (6)C9—C8—H8A108.9
O3—Cl1—O499.8 (5)N1—C8—H8B108.9
O6—Cl1—O4108.4 (4)C9—C8—H8B108.9
C2—O1—Ni1125.7 (2)H8A—C8—H8B107.7
C3—O2—C12117.8 (4)C10—C9—C8116.1 (4)
C7—N1—C8114.5 (4)C10—C9—H9A108.3
C7—N1—Ni1123.0 (3)C8—C9—H9A108.3
C8—N1—Ni1122.5 (3)C10—C9—H9B108.3
C10—N2—C11114.9 (5)C8—C9—H9B108.3
C10—N2—H2A108.5H9A—C9—H9B107.4
C11—N2—H2A108.5N2—C10—C9111.9 (4)
C10—N2—H2B108.5N2—C10—H10A109.2
C11—N2—H2B108.5C9—C10—H10A109.2
H2A—N2—H2B107.5N2—C10—H10B109.2
C2—C1—C6119.8 (4)C9—C10—H10B109.2
C2—C1—C7122.6 (4)H10A—C10—H10B107.9
C6—C1—C7117.6 (4)N2—C11—H11A109.5
O1—C2—C1122.4 (4)N2—C11—H11B109.5
O1—C2—C3119.7 (4)H11A—C11—H11B109.5
C1—C2—C3117.9 (4)N2—C11—H11C109.5
C4—C3—O2124.2 (4)H11A—C11—H11C109.5
C4—C3—C2120.9 (5)H11B—C11—H11C109.5
O2—C3—C2114.8 (4)O2—C12—H12A109.5
C3—C4—C5120.6 (5)O2—C12—H12B109.5
C3—C4—H4119.7H12A—C12—H12B109.5
C5—C4—H4119.7O2—C12—H12C109.5
C6—C5—C4119.8 (5)H12A—C12—H12C109.5
C6—C5—H5120.1H12B—C12—H12C109.5
Symmetry codes: (i) −x+1, −y+1, −z+1.
Hydrogen-bond geometry (Å, °) top
D—H···AD—HH···AD···AD—H···A
N2—H2A···O1i0.901.802.691 (4)170
N2—H2A···O2i0.902.442.929 (5)114
N2—H2B···O4ii0.902.233.075 (8)157
Symmetry codes: (i) −x+1, −y+1, −z+1; (ii) x, −y+1/2, z−1/2.
Table 1
Selected geometric parameters (Å, °)
top
Ni1—O11.922 (3)Ni1—N12.018 (3)
O1i—Ni1—O1180O1—Ni1—N1i89.70 (13)
O1—Ni1—N190.30 (14)N1—Ni1—N1i180
Symmetry codes: (i) −x+1, −y+1, −z+1.
Table 2
Hydrogen-bond geometry (Å, °)
top
D—H···AD—HH···AD···AD—H···A
N2—H2A···O1i0.901.802.691 (4)170
N2—H2A···O2i0.902.442.929 (5)114
N2—H2B···O4ii0.902.233.075 (8)157
Symmetry codes: (i) −x+1, −y+1, −z+1; (ii) x, −y+1/2, z−1/2.
Acknowledgements top

The author acknowledges the Zhoukou Vocational and Technical College for a research grant.

references
References top

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