Literature DB >> 21587921

(2E)-1-(2-Bromo-phen-yl)-3-(4-bromo-phen-yl)prop-2-en-1-one.

Jerry P Jasinski, Ray J Butcher, K Veena, B Narayana, H S Yathirajan.   

Abstract

The title compound, C(15)H(10)Br(2)O, is a chalcone with 2-bromo-phenyl and 4-bromo-phenyl rings bonded to opposite sides of a propenone group. The dihedral angle between mean planes of the benzene rings is 71.3 (1)°. The angle between the mean plane of the prop-2-ene-1-one group and the mean planes of the 2-bromo-phenyl and 4-bromo-phenyl rings are 64.2 (9) and 71.3 (1)°, respectively. A weak inter-molecular C-H⋯O inter-action and two weak C-Br⋯π inter-actions are observed, which contribute to the stability of the crystal packing.

Entities:  

Year:  2010        PMID: 21587921      PMCID: PMC3006939          DOI: 10.1107/S1600536810022956

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


Related literature

For the radical quenching properties of included phenol groups, see: Dhar (1981 ▶). For the biological activity of chalcones, see: Dimmock et al. (1999 ▶). For related structures, see: Ng et al. (2006 ▶); Teh et al. (2006 ▶). For bond-length data, see: Allen et al. (1987 ▶)

Experimental

Crystal data

C15H10Br2O M = 366.05 Monoclinic, a = 5.6988 (5) Å b = 9.5462 (9) Å c = 23.8532 (15) Å β = 91.021 (8)° V = 1297.46 (18) Å3 Z = 4 Cu Kα radiation μ = 7.79 mm−1 T = 110 K 0.62 × 0.47 × 0.26 mm

Data collection

Oxford Diffraction Xcalibur Ruby Gemini diffractometer Absorption correction: analytical (CrysAlis RED; Oxford Diffraction, 2007 ▶) T min = 0.078, T max = 0.315 4592 measured reflections 2532 independent reflections 2454 reflections with I > 2σ(I) R int = 0.027

Refinement

R[F 2 > 2σ(F 2)] = 0.045 wR(F 2) = 0.152 S = 1.32 2532 reflections 164 parameters H-atom parameters constrained Δρmax = 1.27 e Å−3 Δρmin = −1.00 e Å−3 Data collection: CrysAlis PRO (Oxford Diffraction, 2007 ▶); cell refinement: CrysAlis PRO; data reduction: CrysAlis PRO; 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/S1600536810022956/dn2577sup1.cif Structure factors: contains datablocks I. DOI: 10.1107/S1600536810022956/dn2577Isup2.hkl Additional supplementary materials: crystallographic information; 3D view; checkCIF report
C15H10Br2OF(000) = 712
Mr = 366.05Dx = 1.874 Mg m3
Monoclinic, P21/cCu Kα radiation, λ = 1.54178 Å
Hall symbol: -P 2ybcCell parameters from 3417 reflections
a = 5.6988 (5) Åθ = 4.6–74.1°
b = 9.5462 (9) ŵ = 7.79 mm1
c = 23.8532 (15) ÅT = 110 K
β = 91.021 (8)°Prism, colorless
V = 1297.46 (18) Å30.62 × 0.47 × 0.26 mm
Z = 4
Oxford Diffraction Xcalibur Ruby Gemini diffractometer2532 independent reflections
Radiation source: Enhance (Cu) X-ray Source2454 reflections with I > 2σ(I)
graphiteRint = 0.027
Detector resolution: 10.5081 pixels mm-1θmax = 74.1°, θmin = 5.0°
ω scansh = −6→6
Absorption correction: analytical (CrysAlis RED; Oxford Diffraction, 2007)k = −6→11
Tmin = 0.078, Tmax = 0.315l = −29→25
4592 measured reflections
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-atom parameters constrained
wR(F2) = 0.152w = 1/[σ2(Fo2) + (0.0631P)2 + 9.323P] where P = (Fo2 + 2Fc2)/3
S = 1.32(Δ/σ)max < 0.001
2532 reflectionsΔρmax = 1.27 e Å3
164 parametersΔρmin = −1.00 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: 0.0029 (4)
Experimental. IR data (KBr) ν cm-1: 3048 cm-1 (C—H str) 1671 cm-1 (C=O), 1685 cm-1 (C=C).
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
Br11.27853 (11)0.55820 (6)0.36129 (3)0.0217 (3)
Br20.14170 (10)0.10866 (6)0.65074 (2)0.0182 (2)
O11.2468 (7)0.2116 (5)0.37198 (18)0.0211 (9)
C10.9316 (10)0.3480 (6)0.3361 (2)0.0144 (11)
C21.0220 (10)0.4768 (6)0.3200 (2)0.0157 (11)
C30.9269 (12)0.5525 (7)0.2759 (3)0.0223 (13)
H3A0.99120.64060.26580.027*
C40.7337 (12)0.4969 (7)0.2462 (2)0.0239 (14)
H4A0.66700.54680.21540.029*
C50.6406 (11)0.3698 (7)0.2619 (3)0.0219 (13)
H5A0.51030.33200.24160.026*
C60.7359 (10)0.2973 (6)0.3069 (2)0.0180 (12)
H6A0.66690.21140.31800.022*
C71.0493 (10)0.2574 (6)0.3798 (2)0.0149 (11)
C80.9223 (11)0.2193 (6)0.4304 (2)0.0181 (12)
H8A0.98880.14850.45370.022*
C90.7192 (10)0.2767 (6)0.4462 (2)0.0162 (11)
H9A0.65270.34660.42250.019*
C100.5903 (10)0.2408 (6)0.4972 (2)0.0162 (11)
C110.6596 (11)0.1294 (7)0.5320 (3)0.0201 (12)
H11A0.79860.07900.52380.024*
C120.5304 (11)0.0913 (6)0.5780 (3)0.0190 (12)
H12A0.57880.01550.60130.023*
C130.3279 (10)0.1664 (6)0.5895 (2)0.0151 (11)
C140.2554 (10)0.2787 (6)0.5566 (2)0.0180 (12)
H14A0.11780.32990.56540.022*
C150.3891 (10)0.3146 (6)0.5105 (2)0.0173 (12)
H15A0.34150.39140.48770.021*
U11U22U33U12U13U23
Br10.0195 (4)0.0157 (4)0.0300 (4)−0.0029 (2)0.0034 (3)−0.0038 (2)
Br20.0190 (4)0.0196 (4)0.0161 (3)−0.0020 (2)0.0042 (2)0.0011 (2)
O10.015 (2)0.021 (2)0.027 (2)0.0034 (17)0.0043 (16)0.0015 (18)
C10.015 (3)0.016 (3)0.012 (2)0.004 (2)0.007 (2)−0.001 (2)
C20.013 (3)0.017 (3)0.017 (3)−0.001 (2)0.005 (2)−0.003 (2)
C30.028 (3)0.020 (3)0.019 (3)0.006 (2)0.012 (2)0.002 (2)
C40.027 (3)0.030 (4)0.015 (3)0.014 (3)0.004 (2)0.003 (2)
C50.018 (3)0.029 (3)0.019 (3)0.007 (2)0.001 (2)−0.005 (2)
C60.013 (3)0.019 (3)0.022 (3)−0.001 (2)0.004 (2)−0.001 (2)
C70.015 (3)0.009 (2)0.020 (3)−0.001 (2)−0.001 (2)−0.004 (2)
C80.023 (3)0.014 (3)0.017 (3)−0.002 (2)0.000 (2)0.000 (2)
C90.017 (3)0.013 (3)0.018 (3)−0.001 (2)−0.002 (2)0.000 (2)
C100.018 (3)0.014 (3)0.017 (3)−0.002 (2)−0.001 (2)−0.001 (2)
C110.020 (3)0.018 (3)0.022 (3)0.005 (2)0.001 (2)0.002 (2)
C120.022 (3)0.016 (3)0.019 (3)0.003 (2)0.000 (2)0.003 (2)
C130.018 (3)0.016 (3)0.011 (2)−0.003 (2)0.002 (2)−0.001 (2)
C140.014 (3)0.020 (3)0.020 (3)0.003 (2)0.002 (2)−0.001 (2)
C150.017 (3)0.016 (3)0.020 (3)0.000 (2)−0.001 (2)0.003 (2)
Br1—C21.913 (6)C8—C91.341 (9)
Br2—C131.903 (6)C8—H8A0.9500
O1—C71.225 (7)C9—C101.471 (8)
C1—C21.389 (8)C9—H9A0.9500
C1—C61.391 (8)C10—C151.388 (8)
C1—C71.504 (8)C10—C111.402 (8)
C2—C31.380 (9)C11—C121.381 (9)
C3—C41.403 (10)C11—H11A0.9500
C3—H3A0.9500C12—C131.390 (9)
C4—C51.378 (10)C12—H12A0.9500
C4—H4A0.9500C13—C141.386 (8)
C5—C61.380 (9)C14—C151.392 (8)
C5—H5A0.9500C14—H14A0.9500
C6—H6A0.9500C15—H15A0.9500
C7—C81.463 (8)
C2—C1—C6117.9 (5)C7—C8—H8A117.5
C2—C1—C7122.5 (5)C8—C9—C10125.7 (5)
C6—C1—C7119.4 (5)C8—C9—H9A117.1
C3—C2—C1122.1 (6)C10—C9—H9A117.1
C3—C2—Br1117.8 (5)C15—C10—C11118.3 (5)
C1—C2—Br1120.1 (4)C15—C10—C9119.9 (5)
C2—C3—C4118.7 (6)C11—C10—C9121.8 (5)
C2—C3—H3A120.6C12—C11—C10121.5 (6)
C4—C3—H3A120.6C12—C11—H11A119.3
C5—C4—C3119.9 (6)C10—C11—H11A119.3
C5—C4—H4A120.0C11—C12—C13118.4 (5)
C3—C4—H4A120.0C11—C12—H12A120.8
C4—C5—C6120.3 (6)C13—C12—H12A120.8
C4—C5—H5A119.9C14—C13—C12121.9 (5)
C6—C5—H5A119.9C14—C13—Br2119.6 (4)
C5—C6—C1121.1 (6)C12—C13—Br2118.5 (4)
C5—C6—H6A119.5C13—C14—C15118.4 (5)
C1—C6—H6A119.5C13—C14—H14A120.8
O1—C7—C8120.4 (5)C15—C14—H14A120.8
O1—C7—C1120.0 (5)C10—C15—C14121.5 (5)
C8—C7—C1119.6 (5)C10—C15—H15A119.3
C9—C8—C7124.9 (5)C14—C15—H15A119.3
C9—C8—H8A117.5
C6—C1—C2—C3−1.4 (8)O1—C7—C8—C9171.3 (6)
C7—C1—C2—C3173.0 (5)C1—C7—C8—C9−11.4 (9)
C6—C1—C2—Br1176.2 (4)C7—C8—C9—C10−179.3 (5)
C7—C1—C2—Br1−9.4 (7)C8—C9—C10—C15175.9 (6)
C1—C2—C3—C4−0.3 (9)C8—C9—C10—C11−6.7 (9)
Br1—C2—C3—C4−177.9 (4)C15—C10—C11—C121.2 (9)
C2—C3—C4—C50.8 (9)C9—C10—C11—C12−176.3 (6)
C3—C4—C5—C60.4 (9)C10—C11—C12—C13−0.2 (9)
C4—C5—C6—C1−2.1 (9)C11—C12—C13—C14−0.9 (9)
C2—C1—C6—C52.6 (8)C11—C12—C13—Br2177.1 (5)
C7—C1—C6—C5−172.0 (5)C12—C13—C14—C151.0 (9)
C2—C1—C7—O1−62.2 (7)Br2—C13—C14—C15−177.1 (4)
C6—C1—C7—O1112.2 (6)C11—C10—C15—C14−1.1 (9)
C2—C1—C7—C8120.6 (6)C9—C10—C15—C14176.4 (5)
C6—C1—C7—C8−65.1 (7)C13—C14—C15—C100.1 (9)
D—H···AD—HH···AD···AD—H···A
C12—H12A···O1i0.952.463.368 (7)159
Br1···Cg2Br1–PerpC2—Br1···Cg2
C2—Br1···Cg2i3.522 (2)3.488154.82 (17)
C13—-Br2···Cg1ii3.827 (2)3.377165.44 (17)
Table 1

Hydrogen-bond geometry (Å, °)

D—H⋯AD—HH⋯ADAD—H⋯A
C12—H12A⋯O1i0.952.463.368 (7)159

Symmetry code: (i) .

Table 2

C—Br⋯π inter­actions (Å, °)

Cg1 and Cg2 are the centroids of the C1–C6 and C10–C15 rings, respectively.

 Br1⋯Cg2Br1–PerpC2—Br1⋯Cg2
C2—Br1⋯Cg2i3.522 (2)3.488154.82 (17)
C13—-Br2⋯Cg1ii3.827 (2)3.377165.44 (17)

Symmetry codes: (i) ; (ii) .

  2 in total

Review 1.  Bioactivities of chalcones.

Authors:  J R Dimmock; D W Elias; M A Beazely; N M Kandepu
Journal:  Curr Med Chem       Date:  1999-12       Impact factor: 4.530

2.  A short history of SHELX.

Authors:  George M Sheldrick
Journal:  Acta Crystallogr A       Date:  2007-12-21       Impact factor: 2.290

  2 in total
  1 in total

1.  (2E)-1-(3-Bromo-phen-yl)-3-(4,5-dimeth-oxy-2-nitro-phen-yl)prop-2-en-1-one.

Authors:  Jerry P Jasinski; Ray J Butcher; C S Chidan Kumar; H S Yathirajan; A N Mayekar
Journal:  Acta Crystallogr Sect E Struct Rep Online       Date:  2010-10-23
  1 in total

北京卡尤迪生物科技股份有限公司 © 2022-2023.