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The title centrosymmetric Schiff base nickel(II) complex, [Ni(NCS)2(C16H22Br2N2O)2]·2CH3OH, consists of a mononuclear complex mol­ecule and two solvent methanol mol­ecules. The NiII atom lies on an inversion centre and is six-coordinated by the imine N and phenolate O atoms of the two Schiff base ligands and by the N atoms of two thio­cyanate ligands, in an octa­hedral coordination geometry. The cyclo­hexyl rings adopt chair conformations.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536807040238/sj2329sup1.cif
Contains datablocks global, I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536807040238/sj2329Isup2.hkl
Contains datablock I

CCDC reference: 660134

Key indicators

  • Single-crystal X-ray study
  • T = 298 K
  • Mean [sigma](C-C) = 0.007 Å
  • R factor = 0.045
  • wR factor = 0.107
  • Data-to-parameter ratio = 18.5

checkCIF/PLATON results

No syntax errors found



Alert level B PLAT241_ALERT_2_B Check High Ueq as Compared to Neighbors for C12 PLAT242_ALERT_2_B Check Low Ueq as Compared to Neighbors for C11 PLAT242_ALERT_2_B Check Low Ueq as Compared to Neighbors for C14
Alert level C PLAT042_ALERT_1_C Calc. and Rep. MoietyFormula Strings Differ .... ? PLAT062_ALERT_4_C Rescale T(min) & T(max) by ..................... 0.87 PLAT152_ALERT_1_C Supplied and Calc Volume s.u. Inconsistent ..... ? PLAT154_ALERT_1_C The su's on the Cell Angles are Equal (x 10000) 3000 Deg. PLAT180_ALERT_3_C Check Cell Rounding: # of Values Ending with 0 = 3 PLAT220_ALERT_2_C Large Non-Solvent C Ueq(max)/Ueq(min) ... 3.17 Ratio PLAT241_ALERT_2_C Check High Ueq as Compared to Neighbors for C13 PLAT241_ALERT_2_C Check High Ueq as Compared to Neighbors for C15 PLAT242_ALERT_2_C Check Low Ueq as Compared to Neighbors for C17 PLAT341_ALERT_3_C Low Bond Precision on C-C Bonds (x 1000) Ang ... 7
Alert level G ABSTM02_ALERT_3_G When printed, the submitted absorption T values will be replaced by the scaled T values. Since the ratio of scaled T's is identical to the ratio of reported T values, the scaling does not imply a change to the absorption corrections used in the study. Ratio of Tmax expected/reported 0.866 Tmax scaled 0.396 Tmin scaled 0.343 PLAT794_ALERT_5_G Check Predicted Bond Valency for Ni1 (2) 2.06
0 ALERT level A = In general: serious problem 3 ALERT level B = Potentially serious problem 10 ALERT level C = Check and explain 2 ALERT level G = General alerts; check 3 ALERT type 1 CIF construction/syntax error, inconsistent or missing data 7 ALERT type 2 Indicator that the structure model may be wrong or deficient 3 ALERT type 3 Indicator that the structure quality may be low 1 ALERT type 4 Improvement, methodology, query or suggestion 1 ALERT type 5 Informative message, check

Comment top

Recently, we have reported the structures of a few Schiff base copper(II) and zinc(II) complexes (Yuan & Zhang, 2005; Yuan et al., 2007). As an extension of our investigations in this area we report herein the title new mononuclear Schiff base nickel(II) complex.

The complex consists of a mononuclear complex molecule and two lattice methanol molecules (Fig. 1). The NiII atom, lying on the inversion centre, is six-coordinated by two imine N and two phenolic O atoms from two Schiff base ligands and by two N atoms from two thiocyanate ligands, in octahedral coordination. The bond lengths and angles to the Ni(II) atom are comparable to the values in other similar complexes (Diao, 2007; Li et al., 2007; Li & Wang, 2007). The cyclohexyl rings adopt chair conformations.

Related literature top

For related structures, see: Diao (2007); Yuan & Zhang (2005); Yuan et al. (2007); Li et al. (2007); Li & Wang (2007).

Experimental top

3,5-Dibromo-2-hydroxybenzaldehyde (1.0 mmol, 280.0 mg), N-cyclohexylpropane-1,3-diamine (1.0 mmol, 156.2 mg), and nickel nitrate hexahydrate (0.5 mmol, 145.4 mg) were dissolved in a methanol solution (50 ml). The mixture was stirred at room temperature for 30 min and filtered. After keeping the filtrate in air for 12 days, green block-shaped crystals were formed.

Refinement top

All H-atoms were positioned geometrically and refined using a riding model with C—H = 0.93 Å, Uiso = 1.2Ueq (C) for aromatic 0.97 Å, Uiso = 1.2Ueq (C) for CH2, 0.96 Å, Uiso = 1.5Ueq (C) for CH3, 0.90 Å, Uiso = 1.2Ueq (N) for NH and 0.82 Å, Uiso = 1.5Ueq (O) for OH atoms.

Structure description top

Recently, we have reported the structures of a few Schiff base copper(II) and zinc(II) complexes (Yuan & Zhang, 2005; Yuan et al., 2007). As an extension of our investigations in this area we report herein the title new mononuclear Schiff base nickel(II) complex.

The complex consists of a mononuclear complex molecule and two lattice methanol molecules (Fig. 1). The NiII atom, lying on the inversion centre, is six-coordinated by two imine N and two phenolic O atoms from two Schiff base ligands and by two N atoms from two thiocyanate ligands, in octahedral coordination. The bond lengths and angles to the Ni(II) atom are comparable to the values in other similar complexes (Diao, 2007; Li et al., 2007; Li & Wang, 2007). The cyclohexyl rings adopt chair conformations.

For related structures, see: Diao (2007); Yuan & Zhang (2005); Yuan et al. (2007); Li et al. (2007); Li & Wang (2007).

Computing details top

Data collection: SMART (Bruker, 1998); cell refinement: SMART; data reduction: SAINT (Bruker, 1998); 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. The structure of (I). Displacement ellipsoids are drawn at the 30% probability level. Labelled atoms are related to unlabelled atoms by the symmetry operation -x + 2, -y + 1, -z.
Bis{2,4-dibromo-6-[3-(cyclohexylammonio)propyliminomethyl]phenolato- κ2N,O}bis(thiocyanato-κN)nickel(II) methanol disolvate top
Crystal data top
[Ni(NCS)2(C16H22Br2N2O)2]·2CH4OZ = 1
Mr = 1075.31F(000) = 542
Triclinic, P1Dx = 1.621 Mg m3
Hall symbol: -P 1Mo Kα radiation, λ = 0.71073 Å
a = 9.3410 (19) ÅCell parameters from 1932 reflections
b = 10.957 (2) Åθ = 2.3–24.9°
c = 12.210 (2) ŵ = 4.21 mm1
α = 108.28 (3)°T = 298 K
β = 104.21 (3)°Block, green
γ = 100.80 (3)°0.27 × 0.23 × 0.22 mm
V = 1101.8 (4) Å3
Data collection top
Bruker SMART 1000 CCD area-detector
diffractometer
4504 independent reflections
Radiation source: fine-focus sealed tube2992 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.033
ω scansθmax = 26.5°, θmin = 1.9°
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
h = 1111
Tmin = 0.397, Tmax = 0.458k = 1313
8978 measured reflectionsl = 1515
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.045Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.107H-atom parameters constrained
S = 1.01 w = 1/[σ2(Fo2) + (0.048P)2]
where P = (Fo2 + 2Fc2)/3
4504 reflections(Δ/σ)max < 0.001
243 parametersΔρmax = 0.60 e Å3
0 restraintsΔρmin = 0.32 e Å3
Crystal data top
[Ni(NCS)2(C16H22Br2N2O)2]·2CH4Oγ = 100.80 (3)°
Mr = 1075.31V = 1101.8 (4) Å3
Triclinic, P1Z = 1
a = 9.3410 (19) ÅMo Kα radiation
b = 10.957 (2) ŵ = 4.21 mm1
c = 12.210 (2) ÅT = 298 K
α = 108.28 (3)°0.27 × 0.23 × 0.22 mm
β = 104.21 (3)°
Data collection top
Bruker SMART 1000 CCD area-detector
diffractometer
4504 independent reflections
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
2992 reflections with I > 2σ(I)
Tmin = 0.397, Tmax = 0.458Rint = 0.033
8978 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0450 restraints
wR(F2) = 0.107H-atom parameters constrained
S = 1.01Δρmax = 0.60 e Å3
4504 reflectionsΔρmin = 0.32 e Å3
243 parameters
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
Ni11.00000.50000.00000.02932 (18)
Br11.51132 (5)0.62678 (5)0.30412 (4)0.05920 (18)
Br21.33026 (6)0.98998 (5)0.64540 (4)0.06664 (19)
S10.67133 (19)0.12546 (13)0.02759 (16)0.0838 (5)
O11.1701 (3)0.5367 (2)0.1599 (2)0.0343 (6)
O20.4154 (4)0.6690 (5)0.7706 (4)0.0961 (14)
H20.39100.71630.82560.144*
N10.8749 (3)0.5875 (3)0.1069 (3)0.0308 (7)
N20.7392 (4)0.6953 (3)0.1414 (3)0.0370 (8)
H2A0.63830.67740.18150.044*
H2B0.75990.61640.15070.044*
N30.8862 (4)0.3162 (3)0.0011 (3)0.0406 (8)
C11.0902 (5)0.6977 (4)0.2983 (3)0.0346 (9)
C21.2019 (4)0.6386 (4)0.2618 (3)0.0336 (9)
C31.3531 (5)0.6978 (4)0.3463 (4)0.0369 (10)
C41.3914 (5)0.8006 (4)0.4567 (3)0.0428 (11)
H41.49300.83590.50860.051*
C51.2775 (5)0.8511 (4)0.4899 (3)0.0402 (10)
C61.1291 (5)0.8001 (4)0.4125 (3)0.0391 (10)
H61.05270.83400.43620.047*
C70.9310 (5)0.6557 (4)0.2211 (4)0.0357 (9)
H70.86120.68170.25970.043*
C80.7085 (4)0.5674 (4)0.0512 (4)0.0361 (9)
H8A0.65240.53460.09830.043*
H8B0.67240.49970.03080.043*
C90.6743 (5)0.6966 (4)0.0459 (4)0.0430 (10)
H9A0.56640.67500.00070.052*
H9B0.68970.75630.12830.052*
C100.7701 (5)0.7713 (4)0.0092 (4)0.0411 (10)
H10A0.74850.85670.00120.049*
H10B0.87840.78960.03440.049*
C110.8317 (5)0.7682 (4)0.1982 (4)0.0402 (10)
H110.94030.79830.14720.048*
C120.7835 (9)0.8882 (6)0.2053 (5)0.106 (3)
H12A0.79540.94840.12400.127*
H12B0.67550.86050.25400.127*
C130.8795 (9)0.9614 (5)0.2620 (5)0.105 (3)
H13A0.84411.03770.26750.125*
H13B0.98640.99490.20990.125*
C140.8688 (6)0.8722 (5)0.3856 (4)0.0546 (12)
H14A0.93680.92000.41680.066*
H14B0.76420.84670.44060.066*
C150.9127 (8)0.7495 (5)0.3811 (5)0.0849 (19)
H15A1.02130.77460.33470.102*
H15B0.89730.68940.46330.102*
C160.8180 (7)0.6767 (5)0.3229 (5)0.0758 (17)
H16A0.71060.64320.37400.091*
H16B0.85350.60050.31740.091*
C170.7955 (5)0.2382 (4)0.0099 (4)0.0410 (10)
C180.2958 (8)0.6214 (7)0.6636 (6)0.101 (2)
H18A0.26360.69500.64970.151*
H18B0.21120.56050.66830.151*
H18C0.32860.57530.59760.151*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Ni10.0307 (4)0.0273 (4)0.0304 (4)0.0080 (3)0.0130 (3)0.0094 (3)
Br10.0371 (3)0.0546 (3)0.0626 (3)0.0149 (2)0.0096 (2)0.0039 (2)
Br20.0754 (4)0.0546 (3)0.0433 (3)0.0061 (3)0.0193 (3)0.0090 (2)
S10.0967 (11)0.0381 (8)0.1335 (14)0.0095 (7)0.0855 (11)0.0235 (8)
O10.0354 (15)0.0317 (15)0.0306 (15)0.0110 (12)0.0085 (12)0.0059 (12)
O20.073 (3)0.122 (4)0.073 (3)0.060 (3)0.012 (2)0.002 (3)
N10.0344 (18)0.0296 (18)0.0328 (18)0.0106 (14)0.0163 (15)0.0124 (15)
N20.042 (2)0.0313 (18)0.0363 (19)0.0127 (16)0.0131 (16)0.0095 (16)
N30.040 (2)0.033 (2)0.049 (2)0.0071 (17)0.0175 (17)0.0158 (17)
C10.043 (2)0.032 (2)0.031 (2)0.0103 (19)0.0155 (19)0.0130 (18)
C20.038 (2)0.030 (2)0.034 (2)0.0088 (18)0.0141 (18)0.0133 (19)
C30.034 (2)0.033 (2)0.044 (2)0.0106 (18)0.0155 (19)0.012 (2)
C40.041 (3)0.035 (2)0.035 (2)0.006 (2)0.003 (2)0.002 (2)
C50.053 (3)0.033 (2)0.028 (2)0.006 (2)0.014 (2)0.0052 (19)
C60.049 (3)0.040 (2)0.033 (2)0.016 (2)0.023 (2)0.0115 (19)
C70.039 (2)0.034 (2)0.040 (2)0.0135 (19)0.0224 (19)0.013 (2)
C80.034 (2)0.042 (2)0.036 (2)0.0140 (19)0.0178 (18)0.0133 (19)
C90.042 (2)0.050 (3)0.042 (2)0.023 (2)0.016 (2)0.016 (2)
C100.054 (3)0.032 (2)0.041 (2)0.016 (2)0.019 (2)0.014 (2)
C110.043 (2)0.037 (2)0.037 (2)0.009 (2)0.010 (2)0.013 (2)
C120.228 (8)0.070 (4)0.096 (5)0.090 (5)0.119 (5)0.054 (4)
C130.216 (8)0.050 (3)0.082 (4)0.043 (4)0.086 (5)0.039 (3)
C140.061 (3)0.062 (3)0.052 (3)0.019 (3)0.025 (2)0.030 (3)
C150.131 (6)0.064 (4)0.101 (5)0.040 (4)0.081 (4)0.045 (4)
C160.126 (5)0.047 (3)0.085 (4)0.033 (3)0.076 (4)0.028 (3)
C170.042 (3)0.035 (2)0.048 (3)0.016 (2)0.021 (2)0.011 (2)
C180.105 (5)0.101 (5)0.097 (5)0.054 (4)0.020 (4)0.034 (4)
Geometric parameters (Å, º) top
Ni1—O12.060 (3)C8—C91.525 (6)
Ni1—O1i2.060 (3)C8—H8A0.9700
Ni1—N3i2.088 (4)C8—H8B0.9700
Ni1—N32.088 (4)C9—C101.513 (6)
Ni1—N12.090 (3)C9—H9A0.9700
Ni1—N1i2.090 (3)C9—H9B0.9700
Br1—C31.900 (4)C10—H10A0.9700
Br2—C51.900 (4)C10—H10B0.9700
S1—C171.635 (5)C11—C121.488 (6)
O1—C21.306 (4)C11—C161.496 (6)
O2—C181.365 (6)C11—H110.9800
O2—H20.8200C12—C131.520 (8)
N1—C71.272 (5)C12—H12A0.9700
N1—C81.479 (5)C12—H12B0.9700
N2—C101.490 (5)C13—C141.486 (6)
N2—C111.500 (5)C13—H13A0.9700
N2—H2A0.9000C13—H13B0.9700
N2—H2B0.9000C14—C151.490 (7)
N3—C171.150 (5)C14—H14A0.9700
C1—C61.398 (5)C14—H14B0.9700
C1—C21.416 (5)C15—C161.525 (7)
C1—C71.447 (5)C15—H15A0.9700
C2—C31.415 (5)C15—H15B0.9700
C3—C41.369 (5)C16—H16A0.9700
C4—C51.376 (5)C16—H16B0.9700
C4—H40.9300C18—H18A0.9600
C5—C61.364 (6)C18—H18B0.9600
C6—H60.9300C18—H18C0.9600
C7—H70.9300
O1—Ni1—O1i180.00 (14)C10—C9—H9A108.3
O1—Ni1—N3i88.72 (12)C8—C9—H9A108.3
O1i—Ni1—N3i91.28 (12)C10—C9—H9B108.3
O1—Ni1—N391.28 (12)C8—C9—H9B108.3
O1i—Ni1—N388.72 (12)H9A—C9—H9B107.4
N3i—Ni1—N3180.00 (18)N2—C10—C9112.9 (3)
O1—Ni1—N187.62 (11)N2—C10—H10A109.0
O1i—Ni1—N192.38 (11)C9—C10—H10A109.0
N3i—Ni1—N192.76 (13)N2—C10—H10B109.0
N3—Ni1—N187.24 (13)C9—C10—H10B109.0
O1—Ni1—N1i92.38 (11)H10A—C10—H10B107.8
O1i—Ni1—N1i87.62 (11)C12—C11—C16109.7 (4)
N3i—Ni1—N1i87.24 (13)C12—C11—N2111.7 (4)
N3—Ni1—N1i92.76 (13)C16—C11—N2110.6 (3)
N1—Ni1—N1i180.00 (15)C12—C11—H11108.2
C2—O1—Ni1124.6 (2)C16—C11—H11108.2
C18—O2—H2109.5N2—C11—H11108.2
C7—N1—C8115.6 (3)C11—C12—C13110.9 (5)
C7—N1—Ni1124.4 (3)C11—C12—H12A109.5
C8—N1—Ni1120.0 (2)C13—C12—H12A109.5
C10—N2—C11113.7 (3)C11—C12—H12B109.5
C10—N2—H2A108.8C13—C12—H12B109.5
C11—N2—H2A108.8H12A—C12—H12B108.0
C10—N2—H2B108.8C14—C13—C12111.7 (5)
C11—N2—H2B108.8C14—C13—H13A109.3
H2A—N2—H2B107.7C12—C13—H13A109.3
C17—N3—Ni1159.1 (3)C14—C13—H13B109.3
C6—C1—C2121.1 (4)C12—C13—H13B109.3
C6—C1—C7116.5 (4)H13A—C13—H13B107.9
C2—C1—C7122.5 (4)C13—C14—C15110.4 (4)
O1—C2—C3121.8 (4)C13—C14—H14A109.6
O1—C2—C1123.8 (4)C15—C14—H14A109.6
C3—C2—C1114.4 (3)C13—C14—H14B109.6
C4—C3—C2124.2 (4)C15—C14—H14B109.6
C4—C3—Br1118.4 (3)H14A—C14—H14B108.1
C2—C3—Br1117.4 (3)C14—C15—C16111.7 (4)
C3—C4—C5119.1 (4)C14—C15—H15A109.3
C3—C4—H4120.5C16—C15—H15A109.3
C5—C4—H4120.5C14—C15—H15B109.3
C6—C5—C4120.1 (4)C16—C15—H15B109.3
C6—C5—Br2121.1 (3)H15A—C15—H15B107.9
C4—C5—Br2118.9 (3)C11—C16—C15111.1 (4)
C5—C6—C1121.1 (4)C11—C16—H16A109.4
C5—C6—H6119.5C15—C16—H16A109.4
C1—C6—H6119.5C11—C16—H16B109.4
N1—C7—C1127.9 (4)C15—C16—H16B109.4
N1—C7—H7116.1H16A—C16—H16B108.0
C1—C7—H7116.1N3—C17—S1178.0 (4)
N1—C8—C9112.1 (3)O2—C18—H18A109.5
N1—C8—H8A109.2O2—C18—H18B109.5
C9—C8—H8A109.2H18A—C18—H18B109.5
N1—C8—H8B109.2O2—C18—H18C109.5
C9—C8—H8B109.2H18A—C18—H18C109.5
H8A—C8—H8B107.9H18B—C18—H18C109.5
C10—C9—C8115.8 (3)
Symmetry code: (i) x+2, y+1, z.

Experimental details

Crystal data
Chemical formula[Ni(NCS)2(C16H22Br2N2O)2]·2CH4O
Mr1075.31
Crystal system, space groupTriclinic, P1
Temperature (K)298
a, b, c (Å)9.3410 (19), 10.957 (2), 12.210 (2)
α, β, γ (°)108.28 (3), 104.21 (3), 100.80 (3)
V3)1101.8 (4)
Z1
Radiation typeMo Kα
µ (mm1)4.21
Crystal size (mm)0.27 × 0.23 × 0.22
Data collection
DiffractometerBruker SMART 1000 CCD area-detector
Absorption correctionMulti-scan
(SADABS; Sheldrick, 1996)
Tmin, Tmax0.397, 0.458
No. of measured, independent and
observed [I > 2σ(I)] reflections
8978, 4504, 2992
Rint0.033
(sin θ/λ)max1)0.628
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.045, 0.107, 1.01
No. of reflections4504
No. of parameters243
H-atom treatmentH-atom parameters constrained
Δρmax, Δρmin (e Å3)0.60, 0.32

Computer programs: SMART (Bruker, 1998), SMART, SAINT (Bruker, 1998), SHELXS97 (Sheldrick, 1997a), SHELXL97 (Sheldrick, 1997a), SHELXTL (Sheldrick, 1997b), SHELXTL.

 

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