Literature DB >> 23723797

N-[(E)-4-Bromo-benzyl-idene]-2,3-di-methyl-aniline.

Li-Xia Sun1, Ling-Zhi Zhu, Jun-Kai Wang.   

Abstract

The title compound, C15H14BrN, has an E conformation about the C=N bond and the dihedral angle between the benzene rings is 50.7 (2)°. In the crystal, mol-ecules are linked via C-H⋯π inter-actions, forming columns propagating along [010].

Entities:  

Year:  2013        PMID: 23723797      PMCID: PMC3647831          DOI: 10.1107/S1600536813008088

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


Related literature

Schiff base derivativies have many pharmaceutical activities. For their anti­fungal effects, see: Aziz et al. (2010 ▶), for their radical scavenging activity, see: Lu et al. (2012 ▶), for their inhibition of enzyme activity, see: Schmidt et al. (2009 ▶) and for their anti­bacterial activity, see: Shi et al. (2010 ▶). For related structures, see: Sun et al. (2011a ▶,b ▶); Guo et al. (2011 ▶). For standard bond lengths, see: Allen et al. (1987 ▶).

Experimental

Crystal data

C15H14BrN M = 288.18 Monoclinic, a = 12.945 (9) Å b = 7.857 (5) Å c = 14.497 (10) Å β = 113.384 (8)° V = 1353.3 (16) Å3 Z = 4 Mo Kα radiation μ = 3.02 mm−1 T = 296 K 0.25 × 0.20 × 0.19 mm

Data collection

Bruker APEXII CCD diffractometer Absorption correction: multi-scan (SADABS; Sheldrick, 1996 ▶) T min = 0.519, T max = 0.598 5865 measured reflections 2525 independent reflections 1154 reflections with I > 2σ(I) R int = 0.058

Refinement

R[F 2 > 2σ(F 2)] = 0.042 wR(F 2) = 0.112 S = 0.94 2525 reflections 157 parameters H-atom parameters constrained Δρmax = 0.35 e Å−3 Δρmin = −0.25 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. Click here for additional data file. Crystal structure: contains datablock(s) global, I. DOI: 10.1107/S1600536813008088/su2578sup1.cif Click here for additional data file. Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536813008088/su2578Isup2.hkl Click here for additional data file. Supplementary material file. DOI: 10.1107/S1600536813008088/su2578Isup3.cml Additional supplementary materials: crystallographic information; 3D view; checkCIF report
C15H14BrNF(000) = 584
Mr = 288.18Dx = 1.414 Mg m3
Monoclinic, P21/nMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ynCell parameters from 2505 reflections
a = 12.945 (9) Åθ = 2.7–25.5°
b = 7.857 (5) ŵ = 3.02 mm1
c = 14.497 (10) ÅT = 296 K
β = 113.384 (8)°Block, yellow
V = 1353.3 (16) Å30.25 × 0.20 × 0.19 mm
Z = 4
Bruker APEXII CCD diffractometer2525 independent reflections
Radiation source: fine-focus sealed tube1154 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.058
φ and ω scansθmax = 25.5°, θmin = 2.7°
Absorption correction: multi-scan (SADABS; Sheldrick, 1996)h = −15→10
Tmin = 0.519, Tmax = 0.598k = −9→7
5865 measured reflectionsl = −15→17
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.042H-atom parameters constrained
wR(F2) = 0.112w = 1/[σ2(Fo2) + (0.0477P)2] where P = (Fo2 + 2Fc2)/3
S = 0.94(Δ/σ)max < 0.001
2525 reflectionsΔρmax = 0.35 e Å3
157 parametersΔρmin = −0.25 e Å3
0 restraintsExtinction correction: SHELXL97 (Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methodsExtinction coefficient: 0.0298 (19)
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
Br10.07853 (5)0.88838 (7)0.11686 (4)0.0919 (4)
C10.0611 (4)0.8732 (5)0.3942 (3)0.0581 (13)
H10.00910.90560.42050.070*
C20.0362 (4)0.8999 (5)0.2939 (3)0.0643 (13)
H2−0.03150.95040.25290.077*
C30.1122 (5)0.8513 (5)0.2554 (3)0.0547 (12)
C40.2111 (4)0.7767 (7)0.3137 (4)0.0736 (15)
H40.26160.74310.28600.088*
C50.2363 (4)0.7508 (6)0.4154 (3)0.0682 (15)
H50.30420.70020.45570.082*
C60.1617 (4)0.7992 (5)0.4572 (3)0.0477 (11)
C70.1882 (4)0.7675 (5)0.5637 (3)0.0513 (12)
H70.25920.72580.60360.062*
C80.1554 (4)0.7691 (5)0.7095 (3)0.0434 (11)
C90.2578 (4)0.8290 (6)0.7761 (3)0.0582 (13)
H90.30600.88420.75250.070*
C100.2887 (4)0.8071 (7)0.8781 (3)0.0713 (14)
H100.35860.84520.92310.086*
C110.2169 (4)0.7295 (6)0.9130 (3)0.0602 (13)
H110.23820.71630.98180.072*
C120.1130 (4)0.6702 (5)0.8474 (3)0.0500 (12)
C130.0802 (3)0.6918 (5)0.7437 (3)0.0449 (11)
C140.0371 (4)0.5812 (6)0.8890 (4)0.0776 (16)
H14A0.07500.57180.96070.116*
H14B0.01910.46950.86020.116*
H14C−0.03090.64570.87260.116*
C15−0.0326 (4)0.6292 (6)0.6700 (3)0.0758 (15)
H15A−0.08690.63840.69950.114*
H15B−0.02620.51240.65350.114*
H15C−0.05640.69700.61000.114*
N10.1199 (3)0.7938 (4)0.6039 (2)0.0501 (9)
U11U22U33U12U13U23
Br10.1350 (6)0.0914 (5)0.0529 (3)−0.0264 (4)0.0410 (3)0.0038 (3)
C10.064 (3)0.061 (3)0.052 (3)0.015 (3)0.025 (3)0.005 (2)
C20.075 (4)0.054 (3)0.061 (3)0.021 (3)0.024 (3)0.008 (3)
C30.069 (3)0.050 (3)0.044 (2)−0.006 (3)0.023 (3)0.005 (2)
C40.069 (4)0.104 (4)0.061 (3)−0.012 (3)0.039 (3)−0.015 (3)
C50.051 (3)0.095 (4)0.060 (3)0.013 (3)0.024 (3)0.000 (3)
C60.051 (3)0.047 (3)0.048 (3)−0.001 (2)0.023 (2)−0.001 (2)
C70.058 (3)0.047 (3)0.050 (3)0.002 (2)0.022 (3)0.000 (2)
C80.047 (3)0.034 (3)0.049 (3)0.004 (2)0.018 (2)0.001 (2)
C90.062 (3)0.055 (3)0.063 (3)−0.015 (3)0.030 (3)−0.005 (2)
C100.065 (3)0.089 (4)0.057 (3)−0.024 (3)0.021 (3)−0.020 (3)
C110.072 (4)0.066 (4)0.044 (3)−0.004 (3)0.024 (3)−0.002 (2)
C120.062 (3)0.043 (3)0.053 (3)0.002 (2)0.032 (3)0.003 (2)
C130.051 (3)0.037 (3)0.046 (2)0.002 (2)0.018 (2)−0.005 (2)
C140.093 (4)0.080 (4)0.070 (3)−0.008 (3)0.042 (3)0.009 (3)
C150.059 (3)0.100 (4)0.062 (3)−0.015 (3)0.018 (3)−0.005 (3)
N10.061 (2)0.048 (2)0.048 (2)0.004 (2)0.028 (2)0.0032 (17)
Br1—C31.901 (4)C8—N11.426 (5)
C1—C21.375 (6)C9—C101.380 (6)
C1—C61.387 (5)C9—H90.9300
C1—H10.9300C10—C111.366 (6)
C2—C31.365 (6)C10—H100.9300
C2—H20.9300C11—C121.383 (6)
C3—C41.355 (6)C11—H110.9300
C4—C51.393 (6)C12—C131.401 (5)
C4—H40.9300C12—C141.513 (6)
C5—C61.382 (5)C13—C151.509 (6)
C5—H50.9300C14—H14A0.9600
C6—C71.464 (5)C14—H14B0.9600
C7—N11.253 (5)C14—H14C0.9600
C7—H70.9300C15—H15A0.9600
C8—C91.377 (5)C15—H15B0.9600
C8—C131.395 (5)C15—H15C0.9600
C2—C1—C6121.6 (4)C10—C9—H9120.1
C2—C1—H1119.2C11—C10—C9120.1 (4)
C6—C1—H1119.2C11—C10—H10120.0
C3—C2—C1119.1 (4)C9—C10—H10120.0
C3—C2—H2120.5C10—C11—C12121.0 (4)
C1—C2—H2120.5C10—C11—H11119.5
C4—C3—C2121.5 (4)C12—C11—H11119.5
C4—C3—Br1119.2 (4)C11—C12—C13119.6 (4)
C2—C3—Br1119.3 (4)C11—C12—C14119.3 (4)
C3—C4—C5119.3 (4)C13—C12—C14121.0 (4)
C3—C4—H4120.4C8—C13—C12118.5 (4)
C5—C4—H4120.4C8—C13—C15120.3 (4)
C6—C5—C4120.9 (4)C12—C13—C15121.1 (4)
C6—C5—H5119.6C12—C14—H14A109.5
C4—C5—H5119.6C12—C14—H14B109.5
C5—C6—C1117.7 (4)H14A—C14—H14B109.5
C5—C6—C7120.2 (4)C12—C14—H14C109.5
C1—C6—C7122.1 (4)H14A—C14—H14C109.5
N1—C7—C6123.3 (4)H14B—C14—H14C109.5
N1—C7—H7118.4C13—C15—H15A109.5
C6—C7—H7118.4C13—C15—H15B109.5
C9—C8—C13120.8 (4)H15A—C15—H15B109.5
C9—C8—N1121.1 (4)C13—C15—H15C109.5
C13—C8—N1117.9 (4)H15A—C15—H15C109.5
C8—C9—C10119.9 (4)H15B—C15—H15C109.5
C8—C9—H9120.1C7—N1—C8119.4 (4)
C6—C1—C2—C30.4 (7)C9—C10—C11—C120.6 (8)
C1—C2—C3—C40.4 (7)C10—C11—C12—C13−0.8 (7)
C1—C2—C3—Br1−179.8 (3)C10—C11—C12—C14178.5 (4)
C2—C3—C4—C5−0.7 (7)C9—C8—C13—C12−2.6 (6)
Br1—C3—C4—C5179.5 (4)N1—C8—C13—C12−178.6 (4)
C3—C4—C5—C60.3 (7)C9—C8—C13—C15179.0 (4)
C4—C5—C6—C10.4 (7)N1—C8—C13—C153.0 (6)
C4—C5—C6—C7178.6 (4)C11—C12—C13—C81.7 (6)
C2—C1—C6—C5−0.8 (7)C14—C12—C13—C8−177.6 (4)
C2—C1—C6—C7−178.9 (4)C11—C12—C13—C15−179.9 (4)
C5—C6—C7—N1−173.1 (4)C14—C12—C13—C150.9 (6)
C1—C6—C7—N14.9 (7)C6—C7—N1—C8−176.2 (4)
C13—C8—C9—C102.5 (6)C9—C8—N1—C744.6 (6)
N1—C8—C9—C10178.4 (4)C13—C8—N1—C7−139.3 (4)
C8—C9—C10—C11−1.5 (7)
D—H···AD—HH···AD···AD—H···A
C2—H2···Cg2i0.932.993.830 (6)151
C15—H15B···Cg1ii0.962.993.781 (6)140
Table 1

Hydrogen-bond geometry (Å, °)

Cg1 and Cg2 are the centroids of the C8–C13 and C1–C6 rings, respectively.

D—H⋯A D—HH⋯A DA D—H⋯A
C2—H2⋯Cg2i 0.932.993.830 (6)151
C15—H15BCg1ii 0.962.993.781 (6)140

Symmetry codes: (i) ; (ii) .

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