Literature DB >> 21203070

Dibromido[N-propyl-N'-(2-pyridylmethyl-idene)ethane-1,2-diamine]zinc(II).

Xue-Wen Zhu1, Xu-Zhao Yang.   

Abstract

The title complex, [ZnBr(2)(C(11)H(17)N(3))], is a mononuclear zinc(II) compound derived from the Schiff base N-propyl-N'-(1-pyridin-2-ylmethyl-idene)ethane-1,2-diamine. The Zn(II) atom is five-coordinate, binding to the imine N, pyridine N, and amine N atoms of the Schiff base ligand and to two bromide anions in a distorted trigonal-bipyramidal coordination geometry. Adjacent mol-ecules are linked through inter-molecular N-H⋯Br hydrogen bonds, forming dimers.

Entities:  

Year:  2008        PMID: 21203070      PMCID: PMC2962000          DOI: 10.1107/S1600536808023660

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


Related literature

For background to the chemistry of Schiff base complexes, see: Ali et al. (2008 ▶); Biswas et al. (2008 ▶); Chen et al. (2008 ▶); Darensbourg & Frantz (2007 ▶); Habibi et al. (2007 ▶); Kawamoto et al. (2008 ▶); Lipscomb & Sträter (1996 ▶); Tomat et al. (2007 ▶); Wu et al. (2008 ▶); Yuan et al. (2007 ▶). For related structures, see: Dapporto et al. (2001 ▶); You & Zhu (2006 ▶).

Experimental

Crystal data

[ZnBr2(C11H17N3)] M = 416.47 Monoclinic, a = 8.252 (4) Å b = 12.249 (5) Å c = 14.726 (6) Å β = 94.562 (7)° V = 1483.8 (11) Å3 Z = 4 Mo Kα radiation μ = 7.02 mm−1 T = 298 (2) K 0.32 × 0.30 × 0.30 mm

Data collection

Bruker APEXII CCD area-detector diffractometer Absorption correction: multi-scan (SADABS; Sheldrick, 2004 ▶) T min = 0.212, T max = 0.227 (expected range = 0.114–0.122) 12333 measured reflections 3378 independent reflections 2167 reflections with I > 2σ(I) R int = 0.083

Refinement

R[F 2 > 2σ(F 2)] = 0.045 wR(F 2) = 0.105 S = 1.01 3378 reflections 159 parameters 1 restraint H atoms treated by a mixture of independent and constrained refinement Δρmax = 0.91 e Å−3 Δρmin = −0.80 e Å−3 Data collection: APEX2 (Bruker, 2004 ▶); cell refinement: SAINT (Bruker, 2004 ▶); data reduction: SAINT; 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. Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536808023660/sj2523sup1.cif Structure factors: contains datablocks I. DOI: 10.1107/S1600536808023660/sj2523Isup2.hkl Additional supplementary materials: crystallographic information; 3D view; checkCIF report
[ZnBr2(C11H17N3)]F000 = 816
Mr = 416.47Dx = 1.864 Mg m3
Monoclinic, P21/nMo Kα radiation λ = 0.71073 Å
Hall symbol: -P 2ynCell parameters from 1994 reflections
a = 8.252 (4) Åθ = 2.2–25.3º
b = 12.249 (5) ŵ = 7.02 mm1
c = 14.726 (6) ÅT = 298 (2) K
β = 94.562 (7)ºBlock, colorless
V = 1483.8 (11) Å30.32 × 0.30 × 0.30 mm
Z = 4
Bruker APEXII CCD area-detector diffractometer3378 independent reflections
Radiation source: fine-focus sealed tube2167 reflections with I > 2σ(I)
Monochromator: graphiteRint = 0.083
T = 298(2) Kθmax = 27.5º
ω scansθmin = 2.2º
Absorption correction: multi-scan(SADABS; Sheldrick, 2004)h = −10→10
Tmin = 0.212, Tmax = 0.227k = −15→15
12333 measured reflectionsl = −18→19
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.045H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.105  w = 1/[σ2(Fo2) + (0.0211P)2] where P = (Fo2 + 2Fc2)/3
S = 1.01(Δ/σ)max = 0.001
3378 reflectionsΔρmax = 0.91 e Å3
159 parametersΔρmin = −0.80 e Å3
1 restraintExtinction correction: SHELXL, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methodsExtinction coefficient: 0.0140 (7)
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
Zn10.04170 (7)0.30316 (4)0.86078 (4)0.02971 (19)
Br1−0.19476 (6)0.34399 (5)0.94074 (4)0.0454 (2)
Br20.00560 (8)0.29983 (5)0.69779 (4)0.0524 (2)
N10.0385 (5)0.1154 (3)0.8679 (3)0.0359 (10)
N20.2385 (5)0.2563 (3)0.9510 (3)0.0338 (10)
N30.1741 (5)0.4581 (3)0.8836 (3)0.0296 (9)
C10.1561 (6)0.0745 (4)0.9254 (3)0.0351 (12)
C20.1774 (8)−0.0353 (4)0.9398 (4)0.0495 (15)
H20.2599−0.06110.98100.059*
C30.0742 (9)−0.1061 (5)0.8922 (5)0.0606 (18)
H30.0849−0.18110.90090.073*
C4−0.0449 (8)−0.0652 (5)0.8318 (5)0.0575 (17)
H4−0.1150−0.11170.79780.069*
C5−0.0591 (7)0.0466 (5)0.8222 (4)0.0489 (15)
H5−0.14120.07430.78180.059*
C60.2635 (6)0.1575 (4)0.9712 (4)0.0367 (12)
H60.34740.13731.01380.044*
C70.3456 (6)0.3442 (4)0.9865 (4)0.0396 (13)
H7A0.45530.31721.00030.048*
H7B0.30680.37451.04170.048*
C80.3422 (6)0.4295 (4)0.9126 (4)0.0375 (13)
H8A0.40040.49410.93520.045*
H8B0.39580.40160.86110.045*
C90.1638 (6)0.5399 (4)0.8098 (4)0.0400 (13)
H9A0.19390.50610.75400.048*
H9B0.24040.59840.82520.048*
C10−0.0046 (6)0.5869 (4)0.7943 (4)0.0426 (14)
H10A−0.08250.52780.78570.051*
H10B−0.02980.62770.84780.051*
C11−0.0207 (7)0.6607 (5)0.7126 (4)0.0641 (19)
H11A0.06630.71290.71670.096*
H11B−0.12300.69830.71080.096*
H11C−0.01580.61800.65820.096*
H3A0.130 (7)0.491 (4)0.930 (3)0.080*
U11U22U33U12U13U23
Zn10.0321 (3)0.0296 (3)0.0266 (3)0.0004 (2)−0.0029 (2)−0.0032 (3)
Br10.0399 (3)0.0451 (4)0.0526 (4)−0.0043 (2)0.0125 (3)−0.0179 (3)
Br20.0811 (5)0.0481 (4)0.0263 (3)0.0018 (3)−0.0070 (3)−0.0066 (3)
N10.043 (3)0.033 (2)0.031 (3)−0.003 (2)0.002 (2)−0.001 (2)
N20.039 (3)0.032 (2)0.029 (2)0.000 (2)−0.003 (2)0.001 (2)
N30.036 (2)0.027 (2)0.026 (2)−0.0041 (17)0.0009 (19)−0.0019 (18)
C10.046 (3)0.031 (3)0.029 (3)0.002 (2)0.010 (2)0.005 (2)
C20.065 (4)0.035 (3)0.050 (4)0.007 (3)0.013 (3)0.009 (3)
C30.087 (5)0.028 (3)0.071 (5)0.002 (3)0.032 (4)0.004 (3)
C40.070 (4)0.037 (4)0.067 (5)−0.010 (3)0.019 (4)−0.010 (3)
C50.044 (3)0.047 (4)0.056 (4)−0.006 (3)0.000 (3)−0.011 (3)
C60.041 (3)0.038 (3)0.030 (3)0.008 (2)−0.002 (2)0.000 (2)
C70.042 (3)0.040 (3)0.035 (3)−0.001 (2)−0.011 (3)−0.002 (3)
C80.037 (3)0.033 (3)0.041 (3)−0.008 (2)−0.002 (2)−0.003 (3)
C90.046 (3)0.033 (3)0.041 (3)−0.009 (2)0.005 (3)0.004 (3)
C100.044 (3)0.032 (3)0.052 (4)0.002 (2)0.003 (3)0.007 (3)
C110.065 (4)0.054 (4)0.071 (5)0.004 (3)−0.004 (4)0.030 (3)
Zn1—N22.095 (4)C4—C51.380 (8)
Zn1—N32.202 (4)C4—H40.9300
Zn1—N12.303 (4)C5—H50.9300
Zn1—Br22.3954 (13)C6—H60.9300
Zn1—Br12.4102 (11)C7—C81.508 (7)
N1—C51.313 (6)C7—H7A0.9700
N1—C11.334 (6)C7—H7B0.9700
N2—C61.259 (6)C8—H8A0.9700
N2—C71.463 (6)C8—H8B0.9700
N3—C81.461 (6)C9—C101.505 (7)
N3—C91.477 (6)C9—H9A0.9700
N3—H3A0.90 (5)C9—H9B0.9700
C1—C21.371 (7)C10—C111.501 (7)
C1—C61.475 (7)C10—H10A0.9700
C2—C31.369 (8)C10—H10B0.9700
C2—H20.9300C11—H11A0.9600
C3—C41.367 (8)C11—H11B0.9600
C3—H30.9300C11—H11C0.9600
N2—Zn1—N377.83 (16)N1—C5—H5118.7
N2—Zn1—N173.04 (15)C4—C5—H5118.7
N3—Zn1—N1149.43 (15)N2—C6—C1118.2 (5)
N2—Zn1—Br2131.24 (11)N2—C6—H6120.9
N3—Zn1—Br2100.86 (11)C1—C6—H6120.9
N1—Zn1—Br291.57 (11)N2—C7—C8106.0 (4)
N2—Zn1—Br1111.33 (12)N2—C7—H7A110.5
N3—Zn1—Br199.08 (11)C8—C7—H7A110.5
N1—Zn1—Br199.94 (11)N2—C7—H7B110.5
Br2—Zn1—Br1116.88 (4)C8—C7—H7B110.5
C5—N1—C1118.1 (5)H7A—C7—H7B108.7
C5—N1—Zn1128.8 (4)N3—C8—C7109.8 (4)
C1—N1—Zn1113.1 (3)N3—C8—H8A109.7
C6—N2—C7122.7 (4)C7—C8—H8A109.7
C6—N2—Zn1121.2 (3)N3—C8—H8B109.7
C7—N2—Zn1116.1 (3)C7—C8—H8B109.7
C8—N3—C9112.0 (4)H8A—C8—H8B108.2
C8—N3—Zn1106.6 (3)N3—C9—C10111.7 (4)
C9—N3—Zn1118.3 (3)N3—C9—H9A109.3
C8—N3—H3A109 (4)C10—C9—H9A109.3
C9—N3—H3A105 (4)N3—C9—H9B109.3
Zn1—N3—H3A106 (4)C10—C9—H9B109.3
N1—C1—C2122.9 (5)H9A—C9—H9B107.9
N1—C1—C6114.3 (4)C11—C10—C9111.9 (5)
C2—C1—C6122.7 (5)C11—C10—H10A109.2
C3—C2—C1118.4 (6)C9—C10—H10A109.2
C3—C2—H2120.8C11—C10—H10B109.2
C1—C2—H2120.8C9—C10—H10B109.2
C4—C3—C2119.1 (6)H10A—C10—H10B107.9
C4—C3—H3120.5C10—C11—H11A109.5
C2—C3—H3120.5C10—C11—H11B109.5
C3—C4—C5118.8 (6)H11A—C11—H11B109.5
C3—C4—H4120.6C10—C11—H11C109.5
C5—C4—H4120.6H11A—C11—H11C109.5
N1—C5—C4122.7 (6)H11B—C11—H11C109.5
D—H···AD—HH···AD···AD—H···A
N3—H3A···Br1i0.90 (5)2.80 (4)3.539 (4)141 (5)
Zn1—N22.095 (4)
Zn1—N32.202 (4)
Zn1—N12.303 (4)
Zn1—Br22.3954 (13)
Zn1—Br12.4102 (11)
N2—Zn1—N377.83 (16)
N2—Zn1—N173.04 (15)
N3—Zn1—N1149.43 (15)
N2—Zn1—Br2131.24 (11)
N3—Zn1—Br2100.86 (11)
N1—Zn1—Br291.57 (11)
N2—Zn1—Br1111.33 (12)
N3—Zn1—Br199.08 (11)
N1—Zn1—Br199.94 (11)
Br2—Zn1—Br1116.88 (4)
Table 2

Hydrogen-bond geometry (Å, °)

D—H⋯AD—HH⋯ADAD—H⋯A
N3—H3A⋯Br1i0.90 (5)2.80 (4)3.539 (4)141 (5)

Symmetry code: (i) .

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