Literature DB >> 21578262

2-Bromo-1,3-bis-(4-chloro-phen-yl)prop-2-en-1-one.

William T A Harrison, Q N M Hakim Al-Arique, B Narayana, H S Yathirajan, B K Sarojini.   

Abstract

In the title compound, C(15)H(9)BrCl(2)O, the two benzene rings are twisted from each other with a dihedral angle of 47.33 (8)°. The crystal structure is stabilized by aromatic π-π inter-actions between the benzene rings of neighbouring mol-ecules [centroid-centroid distance = 3.680 (2) Å], and by weak inter-molecular C-H⋯O and C-H⋯Cl inter-actions. Additionally, the crystal structure exhibits a short intra-molecular C-H⋯Br contact (H⋯Br = 2.69 Å).

Entities:  

Year:  2009        PMID: 21578262      PMCID: PMC2971337          DOI: 10.1107/S160053680903815X

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


Related literature

For background on chalcones as possible nonlinear optical materials, see: Harrison et al. (2006 ▶). For related structures with the same backbone and different substituents on the aromatic rings, see: Butcher et al. (2006 ▶, 2007 ▶); Dhanasekaran et al. (2007a ▶,b ▶); Fun et al. (2008 ▶).

Experimental

Crystal data

C15H9BrCl2O M = 356.03 Monoclinic, a = 7.7416 (3) Å b = 9.7981 (4) Å c = 9.6717 (3) Å β = 109.075 (2)° V = 693.34 (5) Å3 Z = 2 Mo Kα radiation μ = 3.34 mm−1 T = 120 K 0.18 × 0.16 × 0.06 mm

Data collection

Nonius KappaCCD diffractometer Absorption correction: multi-scan (SADABS; Bruker, 2003 ▶) T min = 0.585, T max = 0.824 12526 measured reflections 3129 independent reflections 2873 reflections with I > 2σ(I) R int = 0.040

Refinement

R[F 2 > 2σ(F 2)] = 0.036 wR(F 2) = 0.079 S = 1.04 3129 reflections 172 parameters 1 restraint H-atom parameters constrained Δρmax = 1.20 e Å−3 Δρmin = −0.46 e Å−3 Absolute structure: Flack (1983 ▶), 1434 Friedel pairs Flack parameter: 0.044 (9) Data collection: COLLECT (Nonius, 1998 ▶); cell refinement: SCALEPACK (Otwinowski & Minor, 1997 ▶); data reduction: DENZO (Otwinowski & Minor, 1997 ▶), SCALEPACK and SORTAV (Blessing, 1995 ▶); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: ORTEP-3 (Farrugia, 1997 ▶); software used to prepare material for publication: SHELXL97. Crystal structure: contains datablocks I, global. DOI: 10.1107/S160053680903815X/lx2111sup1.cif Structure factors: contains datablocks I. DOI: 10.1107/S160053680903815X/lx2111Isup2.hkl Additional supplementary materials: crystallographic information; 3D view; checkCIF report
C15H9BrCl2OF(000) = 352
Mr = 356.03Dx = 1.705 Mg m3
Monoclinic, P21Mo Kα radiation, λ = 0.71073 Å
Hall symbol: P 2ybCell parameters from 13953 reflections
a = 7.7416 (3) Åθ = 2.9–27.5°
b = 9.7981 (4) ŵ = 3.34 mm1
c = 9.6717 (3) ÅT = 120 K
β = 109.075 (2)°Block, colourless
V = 693.34 (5) Å30.18 × 0.16 × 0.06 mm
Z = 2
Nonius KappaCCD diffractometer3129 independent reflections
Radiation source: fine-focus sealed tube2873 reflections with I > 2σ(I)
graphiteRint = 0.040
Detector resolution: 10.0 pixels mm-1θmax = 27.5°, θmin = 3.1°
ω and φ scansh = −10→10
Absorption correction: multi-scan (SADABS; Bruker, 2003)k = −12→12
Tmin = 0.585, Tmax = 0.824l = −12→12
12526 measured reflections
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.036H-atom parameters constrained
wR(F2) = 0.079w = 1/[σ2(Fo2) + (0.0258P)2 + 0.5496P] where P = (Fo2 + 2Fc2)/3
S = 1.04(Δ/σ)max < 0.001
3129 reflectionsΔρmax = 1.20 e Å3
172 parametersΔρmin = −0.46 e Å3
1 restraintAbsolute structure: Flack (1983), 1434 Friedel pairs
Primary atom site location: structure-invariant direct methodsFlack parameter: 0.044 (9)
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
C10.5669 (5)0.6271 (3)0.7407 (4)0.0255 (8)
H10.57610.56210.67060.031*
C20.6586 (5)0.6046 (4)0.8887 (4)0.0266 (8)
H20.72960.52450.92060.032*
C30.6438 (4)0.7025 (4)0.9891 (3)0.0241 (6)
C40.5385 (5)0.8181 (4)0.9458 (4)0.0288 (8)
H40.52830.88251.01600.035*
C50.4479 (5)0.8387 (4)0.7982 (4)0.0292 (8)
H50.37530.91820.76700.035*
C60.4622 (5)0.7436 (3)0.6945 (4)0.0250 (8)
C70.3742 (5)0.7800 (4)0.5351 (4)0.0277 (8)
C80.3109 (5)0.6665 (4)0.4271 (4)0.0271 (8)
C90.2468 (5)0.5475 (4)0.4610 (4)0.0252 (8)
H90.25750.54160.56150.030*
C100.1645 (5)0.4256 (4)0.3785 (4)0.0237 (7)
C110.1567 (5)0.3124 (4)0.4629 (4)0.0304 (8)
H110.20570.31880.56650.037*
C120.0786 (5)0.1897 (4)0.3994 (4)0.0341 (9)
H120.07740.11190.45780.041*
C130.0028 (5)0.1849 (4)0.2478 (4)0.0303 (8)
C140.0093 (5)0.2951 (4)0.1604 (4)0.0316 (9)
H14−0.04270.28900.05700.038*
C150.0928 (5)0.4146 (4)0.2258 (4)0.0276 (8)
H150.10160.48990.16650.033*
O10.3501 (5)0.8986 (3)0.4961 (3)0.0440 (8)
Cl10.76953 (13)0.67976 (9)1.17307 (9)0.0352 (2)
Cl2−0.10057 (15)0.03386 (11)0.16691 (12)0.0460 (3)
Br10.31668 (5)0.71253 (4)0.23765 (4)0.03793 (12)
U11U22U33U12U13U23
C10.0331 (19)0.0179 (17)0.0270 (17)−0.0089 (15)0.0120 (15)−0.0038 (14)
C20.0268 (18)0.0234 (18)0.0321 (19)0.0006 (15)0.0130 (15)−0.0016 (15)
C30.0265 (15)0.0222 (16)0.0272 (14)−0.0041 (17)0.0138 (12)−0.0040 (17)
C40.0303 (19)0.0246 (18)0.037 (2)−0.0052 (16)0.0185 (16)−0.0088 (16)
C50.0298 (19)0.0202 (18)0.040 (2)−0.0016 (15)0.0142 (17)−0.0070 (16)
C60.0219 (16)0.023 (2)0.0308 (17)−0.0049 (13)0.0095 (13)0.0000 (14)
C70.0249 (18)0.0258 (19)0.0325 (19)−0.0014 (15)0.0094 (15)0.0036 (16)
C80.0251 (17)0.031 (2)0.0248 (17)−0.0008 (14)0.0068 (14)0.0095 (14)
C90.0223 (17)0.0268 (19)0.0232 (16)0.0026 (15)0.0028 (14)−0.0031 (15)
C100.0208 (16)0.0231 (18)0.0252 (17)−0.0012 (14)0.0049 (14)−0.0020 (14)
C110.038 (2)0.031 (2)0.0240 (17)−0.0122 (17)0.0122 (16)−0.0030 (16)
C120.041 (2)0.033 (2)0.0329 (17)−0.0120 (19)0.0179 (16)−0.0028 (18)
C130.0268 (17)0.034 (2)0.0318 (16)−0.0077 (16)0.0124 (14)−0.0120 (17)
C140.0270 (19)0.038 (2)0.0254 (18)0.0029 (16)0.0022 (15)−0.0114 (17)
C150.0248 (18)0.0290 (19)0.0282 (18)0.0011 (15)0.0077 (15)−0.0005 (16)
O10.075 (2)0.0152 (13)0.0357 (15)−0.0042 (14)0.0097 (15)0.0106 (12)
Cl10.0448 (5)0.0336 (6)0.0279 (4)−0.0016 (4)0.0131 (4)−0.0049 (4)
Cl20.0468 (6)0.0417 (6)0.0522 (6)−0.0183 (5)0.0199 (5)−0.0197 (5)
Br10.0425 (2)0.0432 (2)0.02831 (17)−0.0063 (2)0.01189 (14)0.01032 (19)
C1—C61.387 (5)C8—Br11.902 (3)
C1—C21.392 (5)C9—C101.462 (5)
C1—H10.9500C9—H90.9500
C2—C31.397 (5)C10—C111.391 (5)
C2—H20.9500C10—C151.402 (5)
C3—C41.378 (5)C11—C121.395 (5)
C3—Cl11.741 (3)C11—H110.9500
C4—C51.384 (5)C12—C131.391 (5)
C4—H40.9500C12—H120.9500
C5—C61.399 (5)C13—C141.382 (6)
C5—H50.9500C13—Cl21.742 (4)
C6—C71.510 (5)C14—C151.387 (6)
C7—O11.217 (5)C14—H140.9500
C7—C81.495 (5)C15—H150.9500
C8—C91.349 (5)
C6—C1—C2120.6 (3)C7—C8—Br1113.0 (2)
C6—C1—H1119.7C8—C9—C10134.7 (3)
C2—C1—H1119.7C8—C9—H9112.7
C1—C2—C3118.4 (3)C10—C9—H9112.7
C1—C2—H2120.8C11—C10—C15118.7 (3)
C3—C2—H2120.8C11—C10—C9115.2 (3)
C4—C3—C2121.8 (3)C15—C10—C9126.1 (3)
C4—C3—Cl1119.6 (3)C10—C11—C12121.6 (3)
C2—C3—Cl1118.5 (3)C10—C11—H11119.2
C3—C4—C5119.0 (3)C12—C11—H11119.2
C3—C4—H4120.5C13—C12—C11117.8 (4)
C5—C4—H4120.5C13—C12—H12121.1
C4—C5—C6120.6 (3)C11—C12—H12121.1
C4—C5—H5119.7C14—C13—C12122.1 (4)
C6—C5—H5119.7C14—C13—Cl2119.5 (3)
C1—C6—C5119.5 (3)C12—C13—Cl2118.4 (3)
C1—C6—C7123.0 (3)C13—C14—C15119.1 (3)
C5—C6—C7117.3 (3)C13—C14—H14120.5
O1—C7—C8120.8 (3)C15—C14—H14120.5
O1—C7—C6121.0 (3)C14—C15—C10120.7 (4)
C8—C7—C6118.2 (3)C14—C15—H15119.7
C9—C8—C7122.4 (3)C10—C15—H15119.7
C9—C8—Br1124.4 (3)
C6—C1—C2—C3−0.6 (5)O1—C7—C8—Br131.2 (5)
C1—C2—C3—C41.4 (5)C6—C7—C8—Br1−151.1 (3)
C1—C2—C3—Cl1−176.1 (3)C7—C8—C9—C10174.4 (4)
C2—C3—C4—C5−1.3 (5)Br1—C8—C9—C10−1.5 (6)
Cl1—C3—C4—C5176.2 (3)C8—C9—C10—C11165.5 (4)
C3—C4—C5—C60.2 (5)C8—C9—C10—C15−15.5 (7)
C2—C1—C6—C5−0.4 (5)C15—C10—C11—C12−0.4 (6)
C2—C1—C6—C7174.1 (3)C9—C10—C11—C12178.7 (3)
C4—C5—C6—C10.6 (5)C10—C11—C12—C13−2.0 (6)
C4—C5—C6—C7−174.3 (3)C11—C12—C13—C142.5 (5)
C1—C6—C7—O1−149.5 (4)C11—C12—C13—Cl2−178.3 (3)
C5—C6—C7—O125.2 (5)C12—C13—C14—C15−0.5 (5)
C1—C6—C7—C832.8 (5)Cl2—C13—C14—C15−179.6 (3)
C5—C6—C7—C8−152.5 (3)C13—C14—C15—C10−2.1 (5)
O1—C7—C8—C9−145.1 (4)C11—C10—C15—C142.5 (5)
C6—C7—C8—C932.6 (5)C9—C10—C15—C14−176.5 (4)
D—H···AD—HH···AD···AD—H···A
C1—H1···O1i0.952.473.411 (5)171
C11—H11···Cl1ii0.952.813.619 (4)143
C15—H15···Br10.952.693.377 (4)129
Table 1

Selected torsion angles (°)

C6—C7—C8—C932.6 (5)
O1—C7—C8—Br131.2 (5)
C7—C8—C9—C10174.4 (4)
Table 2

Hydrogen-bond geometry (Å, °)

D—H⋯AD—HH⋯ADAD—H⋯A
C1—H1⋯O1i0.952.473.411 (5)171
C11—H11⋯Cl1ii0.952.813.619 (4)143
C15—H15⋯Br10.952.693.377 (4)129

Symmetry codes: (i) ; (ii) .

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