Literature DB >> 21579262

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

Grzegorz Dutkiewicz, K Veena, B Narayana, H S Yathirajan, Maciej Kubicki.   

Abstract

The title compound, C(15)H(10)BrFO, is isostructural with (2E)-1-(4-chloro-phen-yl)-3-(4-fluoro-phen-yl)prop-2-en-1-one [Qiu et al. (2006 ▶). Acta Cryst. E62, o3525-o3526], but the structures of other dihalogen analogues, without fluorine, are different, although they are also isostructural within the series. The mol-ecule is approximately flat, the dihedral angle between the ring planes being 8.49 (13)°. In the crystal structure, inter-molecular C-H⋯O, C-H⋯F and C-H⋯Br hydrogen bonds link mol-ecules into V-shaped ribbons running parallel to [101] and stacked with an inter-planar distance of approximately 3.53 Å (centroid-vcentroid distance = 3.857 Å)..

Entities:  

Year:  2010        PMID: 21579262      PMCID: PMC2979273          DOI: 10.1107/S1600536810015485

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


Related literature

For general background to chalcones, see: Dhar (1981 ▶); Goto et al. (1991 ▶); Uchida et al. (1998 ▶); Indira et al. (2002 ▶); Sarojini et al. (2006 ▶). For a description of the Cambridge Structural Database, see: Allen (2002 ▶). For the isostructurality index, see: Kálmán et al. (1991 ▶). For related halogen derivatives, see: Ng, Razak, et al. (2006 ▶); Ng, Shettigar et al. (2006 ▶); Qiu et al. (2006 ▶); Wang et al. (2005 ▶); Yang et al. (2006 ▶).

Experimental

Crystal data

C15H10BrFO M = 305.14 Monoclinic, a = 4.0060 (5) Å b = 23.1253 (12) Å c = 13.4933 (9) Å β = 96.344 (6)° V = 1242.36 (19) Å3 Z = 4 Cu Kα radiation μ = 4.49 mm−1 T = 295 K 0.4 × 0.2 × 0.1 mm

Data collection

Oxford Diffraction SuperNova (single source at offset) Atlas diffractometer Absorption correction: multi-scan (CrysAlis PRO; Oxford Diffraction, 2009 ▶) T min = 0.386, T max = 1.000 4548 measured reflections 2435 independent reflections 2299 reflections with I > 2σ(I) R int = 0.018

Refinement

R[F 2 > 2σ(F 2)] = 0.043 wR(F 2) = 0.116 S = 1.12 2435 reflections 203 parameters All H-atom parameters refined Δρmax = 0.73 e Å−3 Δρmin = −0.50 e Å−3 Data collection: CrysAlis PRO (Oxford Diffraction, 2009 ▶); cell refinement: CrysAlis PRO; data reduction: CrysAlis PRO; program(s) used to solve structure: SIR92 (Altomare et al., 1993 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: XP (Siemens, 1989 ▶); software used to prepare material for publication: SHELXL97. Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536810015485/rz2439sup1.cif Structure factors: contains datablocks I. DOI: 10.1107/S1600536810015485/rz2439Isup2.hkl Additional supplementary materials: crystallographic information; 3D view; checkCIF report
C15H10BrFOF(000) = 608
Mr = 305.14Dx = 1.631 Mg m3
Monoclinic, P21/nCu Kα radiation, λ = 1.54178 Å
Hall symbol: -P 2ynCell parameters from 4020 reflections
a = 4.0060 (5) Åθ = 3.3–75.1°
b = 23.1253 (12) ŵ = 4.49 mm1
c = 13.4933 (9) ÅT = 295 K
β = 96.344 (6)°Prism, colourless
V = 1242.36 (19) Å30.4 × 0.2 × 0.1 mm
Z = 4
Oxford Diffraction SuperNova (single source at offset) Atlas diffractometer2435 independent reflections
Radiation source: Nova (Cu) X-ray Source2299 reflections with I > 2σ(I)
mirrorRint = 0.018
Detector resolution: 5.2679 pixels mm-1θmax = 75.2°, θmin = 3.8°
ω–scanh = −3→5
Absorption correction: multi-scan (CrysAlis PRO; Oxford Diffraction, 2009)k = −28→27
Tmin = 0.386, Tmax = 1.000l = −16→14
4548 measured reflections
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.043Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.116All H-atom parameters refined
S = 1.12w = 1/[σ2(Fo2) + (0.0695P)2 + 0.5227P] where P = (Fo2 + 2Fc2)/3
2435 reflections(Δ/σ)max < 0.001
203 parametersΔρmax = 0.73 e Å3
0 restraintsΔρmin = −0.50 e Å3
Geometry. All s.u.'s (except the s.u. in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell s.u.'s are taken into account individually in the estimation of s.u.'s in distances, angles and torsion angles; correlations between s.u.'s in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell s.u.'s is used for estimating s.u.'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 > 2σ(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
Br10.64900 (8)0.251119 (13)0.06664 (2)0.06378 (18)
F10.8178 (6)0.08073 (9)0.99300 (12)0.0843 (6)
C10.7067 (7)0.07919 (13)0.89344 (19)0.0548 (6)
C20.5320 (8)0.03177 (13)0.85733 (18)0.0544 (6)
H20.507 (9)−0.0022 (15)0.902 (3)0.073 (10)*
C30.4195 (7)0.03031 (11)0.75622 (18)0.0482 (6)
H30.297 (9)−0.0027 (13)0.722 (3)0.073 (10)*
C40.4894 (6)0.07548 (10)0.69363 (16)0.0400 (5)
C50.6687 (7)0.12313 (12)0.73467 (19)0.0489 (6)
H50.725 (10)0.1543 (15)0.699 (3)0.078 (10)*
C60.7766 (8)0.12519 (14)0.8363 (2)0.0572 (7)
H60.914 (9)0.1585 (15)0.870 (3)0.078 (11)*
C70.3685 (6)0.07087 (10)0.58732 (16)0.0417 (5)
H70.190 (7)0.0422 (13)0.571 (2)0.051 (8)*
C80.4515 (6)0.10426 (10)0.51437 (17)0.0423 (5)
H80.627 (7)0.1331 (13)0.525 (2)0.053 (8)*
O90.1120 (5)0.05436 (8)0.38882 (13)0.0589 (5)
C90.3051 (6)0.09403 (10)0.41020 (17)0.0401 (5)
C100.3943 (5)0.13412 (10)0.32965 (16)0.0368 (5)
C110.2928 (6)0.11865 (11)0.23070 (17)0.0426 (5)
H110.184 (8)0.0847 (13)0.217 (2)0.060 (8)*
C120.3662 (6)0.15324 (11)0.15256 (17)0.0462 (5)
H120.294 (7)0.1403 (12)0.083 (2)0.054 (8)*
C130.5401 (6)0.20384 (11)0.17354 (17)0.0427 (5)
C140.6406 (6)0.22126 (11)0.27017 (19)0.0461 (5)
H140.716 (12)0.2556 (13)0.277 (3)0.075 (13)*
C150.5676 (6)0.18557 (10)0.34762 (17)0.0436 (5)
H150.646 (8)0.1983 (13)0.419 (2)0.059 (8)*
U11U22U33U12U13U23
Br10.0534 (3)0.0764 (3)0.0619 (3)0.00176 (12)0.00788 (16)0.03331 (14)
F10.1142 (16)0.1010 (15)0.0343 (8)−0.0239 (12)−0.0074 (9)−0.0034 (8)
C10.0614 (16)0.0684 (16)0.0341 (12)−0.0027 (13)0.0027 (10)−0.0040 (11)
C20.0702 (17)0.0569 (15)0.0362 (12)−0.0062 (13)0.0067 (11)0.0058 (11)
C30.0589 (14)0.0470 (13)0.0386 (11)−0.0078 (11)0.0049 (10)0.0009 (10)
C40.0422 (12)0.0436 (11)0.0344 (10)0.0012 (9)0.0052 (8)0.0013 (9)
C50.0573 (15)0.0465 (13)0.0429 (12)−0.0077 (11)0.0059 (10)0.0020 (10)
C60.0648 (17)0.0624 (16)0.0437 (13)−0.0148 (13)0.0031 (12)−0.0074 (12)
C70.0449 (12)0.0435 (11)0.0365 (11)−0.0004 (9)0.0036 (9)−0.0011 (9)
C80.0441 (12)0.0455 (12)0.0368 (11)−0.0024 (10)0.0021 (9)−0.0005 (9)
O90.0744 (13)0.0577 (11)0.0428 (9)−0.0259 (10)−0.0017 (8)0.0021 (8)
C90.0440 (12)0.0411 (11)0.0351 (10)−0.0001 (9)0.0038 (8)−0.0003 (9)
C100.0357 (11)0.0393 (11)0.0349 (10)0.0039 (8)0.0019 (8)−0.0005 (8)
C110.0483 (13)0.0418 (12)0.0366 (11)−0.0031 (9)0.0000 (9)−0.0012 (9)
C120.0499 (13)0.0536 (13)0.0337 (11)0.0025 (10)−0.0014 (9)0.0032 (9)
C130.0360 (11)0.0487 (12)0.0432 (11)0.0063 (9)0.0037 (8)0.0111 (9)
C140.0435 (12)0.0430 (13)0.0513 (13)−0.0063 (10)0.0027 (10)0.0005 (10)
C150.0474 (12)0.0454 (12)0.0372 (11)−0.0032 (10)0.0008 (9)−0.0032 (9)
Br1—C131.899 (2)C8—C91.481 (3)
F1—C11.368 (3)C8—H80.97 (3)
C1—C61.361 (4)O9—C91.214 (3)
C1—C21.362 (4)C9—C101.501 (3)
C2—C31.389 (3)C10—C151.385 (3)
C2—H21.00 (3)C10—C111.399 (3)
C3—C41.391 (3)C11—C121.381 (3)
C3—H30.99 (3)C11—H110.91 (3)
C4—C51.396 (3)C12—C131.375 (4)
C4—C71.466 (3)C12—H121.00 (3)
C5—C61.392 (4)C13—C141.381 (3)
C5—H50.91 (4)C14—C151.388 (3)
C6—H61.02 (4)C14—H140.85 (3)
C7—C81.322 (3)C15—H151.02 (3)
C7—H70.98 (3)
C6—C1—C2123.8 (2)C9—C8—H8117.1 (18)
C6—C1—F1118.1 (3)O9—C9—C8121.4 (2)
C2—C1—F1118.1 (3)O9—C9—C10119.4 (2)
C1—C2—C3118.0 (2)C8—C9—C10119.2 (2)
C1—C2—H2119.8 (19)C15—C10—C11118.3 (2)
C3—C2—H2122.0 (19)C15—C10—C9123.94 (19)
C2—C3—C4120.9 (2)C11—C10—C9117.8 (2)
C2—C3—H3124 (2)C12—C11—C10121.1 (2)
C4—C3—H3115 (2)C12—C11—H11119 (2)
C3—C4—C5118.8 (2)C10—C11—H11120 (2)
C3—C4—C7118.2 (2)C13—C12—C11118.8 (2)
C5—C4—C7123.0 (2)C13—C12—H12122.5 (17)
C6—C5—C4120.5 (2)C11—C12—H12118.7 (17)
C6—C5—H5115 (2)C12—C13—C14122.0 (2)
C4—C5—H5124 (2)C12—C13—Br1119.16 (18)
C1—C6—C5118.1 (3)C14—C13—Br1118.80 (19)
C1—C6—H6118 (2)C13—C14—C15118.3 (2)
C5—C6—H6124 (2)C13—C14—H14116 (3)
C8—C7—C4127.1 (2)C15—C14—H14125 (3)
C8—C7—H7118.0 (16)C10—C15—C14121.5 (2)
C4—C7—H7114.6 (16)C10—C15—H15120.5 (17)
C7—C8—C9120.5 (2)C14—C15—H15118.0 (17)
C7—C8—H8122.0 (18)
C6—C1—C2—C30.1 (5)O9—C9—C10—C15169.3 (2)
F1—C1—C2—C3−180.0 (3)C8—C9—C10—C15−9.8 (3)
C1—C2—C3—C41.2 (4)O9—C9—C10—C11−10.0 (3)
C2—C3—C4—C5−1.5 (4)C8—C9—C10—C11170.8 (2)
C2—C3—C4—C7179.0 (2)C15—C10—C11—C120.7 (4)
C3—C4—C5—C60.3 (4)C9—C10—C11—C12−179.8 (2)
C7—C4—C5—C6179.9 (3)C10—C11—C12—C13−0.4 (4)
C2—C1—C6—C5−1.3 (5)C11—C12—C13—C14−0.6 (4)
F1—C1—C6—C5178.9 (3)C11—C12—C13—Br1178.96 (18)
C4—C5—C6—C11.0 (5)C12—C13—C14—C151.3 (4)
C3—C4—C7—C8−168.8 (3)Br1—C13—C14—C15−178.27 (18)
C5—C4—C7—C811.6 (4)C11—C10—C15—C140.0 (4)
C4—C7—C8—C9−179.7 (2)C9—C10—C15—C14−179.4 (2)
C7—C8—C9—O9−1.5 (4)C13—C14—C15—C10−1.0 (4)
C7—C8—C9—C10177.7 (2)
D—H···AD—HH···AD···AD—H···A
C7—H7···O9i0.98 (3)2.62 (3)3.512 (3)151 (2)
C3—H3···O9i0.99 (3)2.41 (3)3.358 (3)160 (2)
C15—H15···Br1ii1.02 (3)2.92 (3)3.845 (2)151 (2)
C12—H12···F1iii1.00 (3)2.55 (3)3.351 (3)137 (2)
Table 1

Hydrogen-bond geometry (Å, °)

D—H⋯AD—HH⋯ADAD—H⋯A
C7—H7⋯O9i0.98 (3)2.62 (3)3.512 (3)151 (2)
C3—H3⋯O9i0.99 (3)2.41 (3)3.358 (3)160 (2)
C15—H15⋯Br1ii1.02 (3)2.92 (3)3.845 (2)151 (2)
C12—H12⋯F1iii1.00 (3)2.55 (3)3.351 (3)137 (2)

Symmetry codes: (i) ; (ii) ; (iii) .

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3.  Crystal structure, Hirshfeld surface analysis and DFT studies of (E)-1-(4-bromo-phen-yl)-3-(3-fluoro-phen-yl)prop-2-en-1-one.

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4.  Crystal structure and Hirshfeld surface analysis of (E)-3-(3-iodo-phen-yl)-1-(4-iodo-phen-yl)prop-2-en-1-one.

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