Literature DB >> 21584018

2,2'-[5-Bromo-o-phenyl-enebis(nitrilo-methyl-idyne)]diphenol.

Jing Gao1, Yan Cheng.   

Abstract

A new tetra-dentate unsymmetrical Schiff base, C(20)H(15)BrN(2)O(2), has been synthesized from 4-bromo-o-phenyl-enediamine and salicylaldehyde in refluxing ethanol. The dihedral angles between the two hydroxy-phenyl rings and the bromo-o-phenyl-enediiminatoin group are 68.6 (1) and 8.7 (1)°; the dihedral angle between the two hydroxy-phenyl rings is 70.3 (1)°. There are two relatively strong intra-molecular of O-H⋯N hydrogen bonds.

Entities:  

Year:  2009        PMID: 21584018      PMCID: PMC2977675          DOI: 10.1107/S1600536809011581

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


Related literature

For the biological activity of Schiff bases, see: Boskovic et al. (2003 ▶); Koizumi et al. (2005 ▶); Oshiob et al. (2005 ▶). For related structures, see: Kannappan et al. (2005 ▶); Zhang et al. (2003 ▶).

Experimental

Crystal data

C20H15BrN2O2 M = 395.25 Monoclinic, a = 12.8744 (10) Å b = 5.9968 (10) Å c = 22.106 (2) Å β = 91.221 (1)° V = 1706.3 (3) Å3 Z = 4 Mo Kα radiation μ = 2.43 mm−1 T = 297 K 0.12 × 0.10 × 0.08 mm

Data collection

Bruker APEXII CCD area-detector diffractometer Absorption correction: multi-scan (SADABS; Bruker, 2001 ▶) T min = 0.760, T max = 0.830 8088 measured reflections 3009 independent reflections 2140 reflections with I > 2σ(I) R int = 0.027

Refinement

R[F 2 > 2σ(F 2)] = 0.045 wR(F 2) = 0.141 S = 1.00 3009 reflections 228 parameters 2 restraints H-atom parameters constrained Δρmax = 0.78 e Å−3 Δρmin = −0.62 e Å−3 Data collection: APEX2 (Bruker, 2004 ▶); cell refinement: SAINT-Plus (Bruker, 2001 ▶); data reduction: SAINT-Plus; 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 I, global. DOI: 10.1107/S1600536809011581/fl2239sup1.cif Structure factors: contains datablocks I. DOI: 10.1107/S1600536809011581/fl2239Isup2.hkl Additional supplementary materials: crystallographic information; 3D view; checkCIF report
C20H15BrN2O2F(000) = 800
Mr = 395.25Dx = 1.539 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ybcCell parameters from 3171 reflections
a = 12.8744 (10) Åθ = 1.6–25.5°
b = 5.9968 (10) ŵ = 2.42 mm1
c = 22.106 (2) ÅT = 297 K
β = 91.221 (1)°Block, yellow
V = 1706.3 (3) Å30.12 × 0.10 × 0.08 mm
Z = 4
Bruker APEXII CCD area-detector diffractometer3009 independent reflections
Radiation source: fine-focus sealed tube2140 reflections with I > 2σ(I)
graphiteRint = 0.027
φ and ω scansθmax = 25.1°, θmin = 1.6°
Absorption correction: multi-scan (SADABS; Bruker, 2001)h = −14→15
Tmin = 0.760, Tmax = 0.830k = −6→7
8088 measured reflectionsl = −24→26
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) = 0.141H-atom parameters constrained
S = 1.00w = 1/[σ2(Fo2) + (0.085P)2 + 0.9153P] where P = (Fo2 + 2Fc2)/3
3009 reflections(Δ/σ)max = 0.002
228 parametersΔρmax = 0.78 e Å3
2 restraintsΔρmin = −0.62 e Å3
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
Br10.27473 (4)0.20430 (9)1.05914 (2)0.0635 (2)
C10.1838 (3)0.8216 (6)0.94539 (16)0.0417 (9)
C20.1078 (2)0.7023 (5)0.97413 (14)0.0317 (8)
H20.03860.74610.97180.038*
C30.1377 (3)0.5168 (5)1.00639 (16)0.0481 (10)
H30.08780.43161.02550.058*
C40.2398 (3)0.4554 (7)1.01079 (17)0.0447 (9)
C50.3167 (3)0.5727 (7)0.98216 (18)0.0486 (10)
H50.38600.52980.98530.058*
C60.2863 (3)0.7566 (7)0.94862 (18)0.0446 (10)
C70.4151 (3)0.7950 (7)0.87700 (19)0.0464 (10)
H70.40020.64860.86600.056*
C80.4988 (3)0.9113 (7)0.84710 (18)0.0449 (9)
C90.5316 (3)1.1220 (8)0.8668 (2)0.0517 (10)
C100.6197 (4)1.2177 (9)0.8394 (2)0.0662 (13)
H100.64381.35580.85280.079*
C110.6688 (4)1.1140 (10)0.7950 (2)0.0676 (13)
H110.72601.18140.77760.081*
C120.6359 (4)0.9088 (10)0.7746 (2)0.0663 (13)
H120.67060.83870.74340.080*
C130.5525 (3)0.8076 (8)0.79998 (19)0.0547 (11)
H130.53090.66850.78600.066*
C140.0595 (3)1.0603 (7)0.90197 (16)0.0425 (9)
H140.00750.97050.91740.051*
C150.0308 (3)1.2554 (7)0.86720 (17)0.0436 (9)
C160.1076 (3)1.3984 (7)0.84457 (16)0.0485 (10)
C170.0765 (4)1.5884 (8)0.81293 (19)0.0637 (13)
H170.12631.68400.79750.076*
C18−0.0274 (5)1.6360 (8)0.8042 (2)0.0671 (14)
H18−0.04681.76560.78390.081*
C19−0.1025 (4)1.4960 (8)0.8251 (2)0.0629 (12)
H19−0.17241.52780.81800.076*
C20−0.0733 (3)1.3075 (7)0.85666 (19)0.0525 (10)
H20−0.12431.21310.87130.063*
N20.1546 (2)1.0078 (6)0.91204 (14)0.0425 (8)
N30.3615 (2)0.8877 (6)0.91782 (16)0.0501 (8)
O10.4841 (3)1.2338 (6)0.91170 (19)0.0761 (11)
H10.44031.15330.92690.114*
O20.2093 (2)1.3554 (6)0.85188 (15)0.0654 (9)
H2A0.21751.25380.87640.098*
U11U22U33U12U13U23
Br10.0748 (4)0.0534 (3)0.0618 (3)0.0087 (2)−0.0108 (2)0.0073 (2)
C10.040 (2)0.041 (2)0.044 (2)−0.0021 (17)−0.0003 (16)−0.0050 (18)
C20.0219 (16)0.037 (2)0.0360 (18)−0.0026 (15)0.0033 (14)0.0062 (16)
C30.045 (2)0.051 (3)0.049 (2)−0.0092 (19)−0.0011 (18)0.002 (2)
C40.049 (2)0.040 (2)0.045 (2)−0.0010 (18)−0.0053 (18)−0.0017 (18)
C50.045 (2)0.045 (3)0.056 (2)0.0010 (19)0.0008 (19)−0.007 (2)
C60.043 (2)0.043 (2)0.048 (2)−0.0090 (18)0.0065 (18)−0.0074 (18)
C70.039 (2)0.040 (2)0.060 (3)−0.0005 (18)−0.0018 (19)0.003 (2)
C80.038 (2)0.044 (2)0.052 (2)0.0042 (18)−0.0049 (17)0.0056 (19)
C90.037 (2)0.049 (3)0.069 (3)−0.0003 (19)0.002 (2)0.005 (2)
C100.049 (3)0.060 (3)0.089 (4)−0.011 (2)0.000 (3)0.012 (3)
C110.047 (3)0.085 (4)0.071 (3)−0.005 (3)0.008 (2)0.015 (3)
C120.055 (3)0.092 (4)0.053 (3)0.005 (3)0.011 (2)0.007 (3)
C130.050 (2)0.066 (3)0.049 (2)0.002 (2)0.001 (2)0.001 (2)
C140.046 (2)0.040 (2)0.042 (2)−0.0061 (18)0.0042 (17)0.0001 (17)
C150.056 (2)0.039 (2)0.036 (2)−0.0036 (18)0.0029 (18)−0.0023 (16)
C160.065 (3)0.046 (2)0.035 (2)−0.011 (2)0.0036 (19)−0.0024 (19)
C170.103 (4)0.048 (3)0.041 (2)−0.018 (3)0.010 (2)0.004 (2)
C180.109 (4)0.045 (3)0.046 (3)0.010 (3)−0.013 (3)0.005 (2)
C190.074 (3)0.056 (3)0.058 (3)0.012 (3)−0.006 (2)0.003 (2)
C200.057 (3)0.050 (3)0.051 (2)0.000 (2)0.000 (2)0.001 (2)
N20.0408 (18)0.0416 (19)0.0453 (18)−0.0045 (14)0.0014 (14)0.0006 (15)
N30.0393 (18)0.046 (2)0.065 (2)−0.0065 (16)0.0084 (16)−0.0063 (18)
O10.063 (2)0.052 (2)0.114 (3)−0.0116 (16)0.028 (2)−0.021 (2)
O20.060 (2)0.072 (2)0.065 (2)−0.0218 (17)0.0083 (16)0.0092 (17)
Br1—C41.895 (4)C11—C121.375 (8)
C1—C61.377 (6)C11—H110.9300
C1—C21.378 (5)C12—C131.364 (6)
C1—N21.385 (5)C12—H120.9300
C2—C31.372 (4)C13—H130.9300
C2—H20.9300C14—N21.279 (5)
C3—C41.367 (5)C14—C151.443 (5)
C3—H30.9300C14—H140.9300
C4—C51.379 (6)C15—C201.391 (6)
C5—C61.381 (6)C15—C161.409 (6)
C5—H50.9300C16—O21.341 (5)
C6—N31.430 (5)C16—C171.391 (6)
C7—N31.275 (5)C17—C181.377 (7)
C7—C81.454 (6)C17—H170.9300
C7—H70.9300C18—C191.367 (7)
C8—C91.399 (6)C18—H180.9300
C8—C131.408 (6)C19—C201.377 (6)
C9—O11.354 (5)C19—H190.9300
C9—C101.419 (6)C20—H200.9300
C10—C111.333 (7)O1—H10.8200
C10—H100.9300O2—H2A0.8200
C6—C1—C2121.2 (3)C12—C11—H11119.6
C6—C1—N2120.3 (3)C13—C12—C11120.2 (5)
C2—C1—N2118.5 (3)C13—C12—H12119.9
C3—C2—C1117.8 (3)C11—C12—H12119.9
C3—C2—H2121.1C12—C13—C8120.7 (5)
C1—C2—H2121.1C12—C13—H13119.6
C4—C3—C2121.0 (3)C8—C13—H13119.6
C4—C3—H3119.5N2—C14—C15121.7 (4)
C2—C3—H3119.5N2—C14—H14119.2
C3—C4—C5121.9 (4)C15—C14—H14119.2
C3—C4—Br1118.1 (3)C20—C15—C16119.0 (4)
C5—C4—Br1120.0 (3)C20—C15—C14120.4 (4)
C4—C5—C6117.1 (4)C16—C15—C14120.6 (4)
C4—C5—H5121.4O2—C16—C17119.2 (4)
C6—C5—H5121.4O2—C16—C15122.1 (4)
C1—C6—C5121.0 (3)C17—C16—C15118.7 (4)
C1—C6—N3118.5 (4)C18—C17—C16120.6 (4)
C5—C6—N3120.5 (4)C18—C17—H17119.7
N3—C7—C8122.0 (4)C16—C17—H17119.7
N3—C7—H7119.0C19—C18—C17121.1 (5)
C8—C7—H7119.0C19—C18—H18119.4
C9—C8—C13118.7 (4)C17—C18—H18119.4
C9—C8—C7120.9 (4)C18—C19—C20119.2 (5)
C13—C8—C7120.3 (4)C18—C19—H19120.4
O1—C9—C8122.5 (4)C20—C19—H19120.4
O1—C9—C10119.3 (4)C19—C20—C15121.4 (4)
C8—C9—C10118.1 (4)C19—C20—H20119.3
C11—C10—C9121.5 (5)C15—C20—H20119.3
C11—C10—H10119.3C14—N2—C1122.6 (3)
C9—C10—H10119.3C7—N3—C6118.6 (4)
C10—C11—C12120.8 (5)C9—O1—H1109.5
C10—C11—H11119.6C16—O2—H2A109.5
D—H···AD—HH···AD···AD—H···A
O2—H2A···N20.821.872.578 (4)145
O1—H1···N30.821.902.614 (5)145
Table 1

Hydrogen-bond geometry (Å, °)

D—H⋯AD—HH⋯ADAD—H⋯A
O2—H2A⋯N20.821.872.578 (4)145
O1—H1⋯N30.821.902.614 (5)145
  4 in total

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4.  Ferromagnetic and antiferromagnetic intermolecular interactions in a new family of Mn4 complexes with an energy barrier to magnetization reversal.

Authors:  Colette Boskovic; Roland Bircher; Philip L W Tregenna-Piggott; Hans U Güdel; Carley Paulsen; Wolfgang Wernsdorfer; Anne-Laure Barra; Eugene Khatsko; Antonia Neels; Helen Stoeckli-Evans
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  4 in total

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