supplementary materials


hb5445 scheme

Acta Cryst. (2010). E66, o1412    [ doi:10.1107/S1600536810018106 ]

1-(4-Bromophenyl)-3-(3,4-dimethylphenyl)prop-2-en-1-one

Y. Zhou

Abstract top

In the title chalcone derivative, C17H15BrO, the dihedral angle between the two benzene rings is 48.13 (4)°. In the crystal, a short Br...Br contact of 3.5052 (10) Å occurs.

Comment top

As part of our search for new biologically active compounds we synthesized the title compound(I) and report its crystal structure herein.

In the crystal structure of compound(I)(fig.1),the dihedral angle between the two benzene rings(C1—C6) and (C7—C12) is 48.13 (4)°. All of the bond lengths and bond angles are in normal ranges and comparable to those in related structure (Fun et al., 2008).

Related literature top

For a related structure and background to chalcones, see: Fun et al. (2008).

Experimental top

A mixture of 4-bromohypnone (0.02 mol) and 3,4-dimethylbenzaldehyde (0.02 mol) and 10%NaOH (5 ml) was stirred in ethanol (30 ml) for 1.5 h to afford the title compound (yield 73%). Yellow blocks of (I) were obtailed by recrystallization from ethyl acetate at room temperature.

Refinement top

H atoms were positioned geometrically and allowed to ride on their parent atoms, with C—H distances of 0.93-0.96 Å, and with Uiso(H) = 1.2Ueq of the parent atoms.

Computing details top

Data collection: SMART (Bruker, 1997); cell refinement: SAINT (Bruker, 1997); data reduction: SAINT (Bruker, 1997); 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 (Sheldrick, 2008).

Figures top
[Figure 1] Fig. 1. The molecular structure of (I) with displacement ellipsoids are drawn at the 30% probability level.
1-(4-Bromophenyl)-3-(3,4-dimethylphenyl)prop-2-en-1-one top
Crystal data top
C17H15BrOZ = 2
Mr = 315.20F(000) = 320
Triclinic, P1Dx = 1.468 Mg m3
Hall symbol: -P 1Mo Kα radiation, λ = 0.71073 Å
a = 5.9786 (14) ÅCell parameters from 2198 reflections
b = 7.8437 (19) Åθ = 1.3–25.5°
c = 15.744 (4) ŵ = 2.87 mm1
α = 99.054 (4)°T = 298 K
β = 99.602 (4)°Bar, yellow
γ = 95.659 (4)°0.25 × 0.22 × 0.20 mm
V = 713.0 (3) Å3
Data collection top
Bruker SMART CCD
diffractometer
2198 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tubeRint = 0.019
graphiteθmax = 25.5°, θmin = 1.3°
phi and ω scansh = 77
3911 measured reflectionsk = 96
2620 independent reflectionsl = 1819
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.033H-atom parameters constrained
wR(F2) = 0.095 w = 1/[σ2(Fo2) + (0.048P)2 + 0.2458P]
where P = (Fo2 + 2Fc2)/3
S = 1.09(Δ/σ)max < 0.001
2620 reflectionsΔρmax = 0.45 e Å3
173 parametersΔρmin = 0.60 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: 0.048 (4)
Crystal data top
C17H15BrOγ = 95.659 (4)°
Mr = 315.20V = 713.0 (3) Å3
Triclinic, P1Z = 2
a = 5.9786 (14) ÅMo Kα radiation
b = 7.8437 (19) ŵ = 2.87 mm1
c = 15.744 (4) ÅT = 298 K
α = 99.054 (4)°0.25 × 0.22 × 0.20 mm
β = 99.602 (4)°
Data collection top
Bruker SMART CCD
diffractometer
2198 reflections with I > 2σ(I)
3911 measured reflectionsRint = 0.019
2620 independent reflectionsθmax = 25.5°
Refinement top
R[F2 > 2σ(F2)] = 0.033H-atom parameters constrained
wR(F2) = 0.095Δρmax = 0.45 e Å3
S = 1.09Δρmin = 0.60 e Å3
2620 reflectionsAbsolute structure: ?
173 parametersFlack parameter: ?
0 restraintsRogers parameter: ?
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds 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.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
Br0.57731 (6)0.43242 (4)0.100602 (19)0.06655 (18)
C110.5449 (5)0.3857 (3)0.21288 (17)0.0440 (6)
O0.2750 (3)0.2761 (3)0.48223 (13)0.0628 (6)
C100.7328 (5)0.4220 (4)0.27985 (18)0.0482 (6)
H10A0.87240.47170.27060.058*
C170.4645 (5)0.2760 (4)0.46327 (17)0.0455 (6)
C120.3349 (5)0.3142 (4)0.22550 (18)0.0506 (7)
H12A0.21000.28980.17960.061*
C90.7107 (4)0.3834 (3)0.36099 (17)0.0448 (6)
H9A0.83740.40480.40610.054*
C80.5010 (4)0.3129 (3)0.37593 (16)0.0395 (5)
C61.1464 (4)0.0981 (3)0.80706 (18)0.0453 (6)
C50.9589 (4)0.1781 (4)0.82839 (17)0.0448 (6)
C30.8289 (4)0.1904 (3)0.67426 (17)0.0408 (6)
C40.8024 (4)0.2208 (3)0.76150 (17)0.0437 (6)
H4A0.67590.27140.77550.052*
C160.6528 (5)0.2356 (3)0.60745 (17)0.0437 (6)
H16A0.51940.26560.62560.052*
C21.0206 (5)0.1157 (3)0.65442 (18)0.0459 (6)
H2A1.04480.09670.59700.055*
C70.3131 (5)0.2796 (4)0.30725 (17)0.0464 (6)
H7A0.17170.23350.31670.056*
C150.6631 (5)0.2384 (4)0.52402 (18)0.0477 (6)
H15A0.79660.21640.50360.057*
C11.1749 (5)0.0697 (3)0.72054 (19)0.0474 (6)
H1A1.30080.01840.70640.057*
C140.9249 (6)0.2180 (5)0.9221 (2)0.0674 (9)
H14A0.78850.27260.92420.101*
H14B1.05410.29500.95670.101*
H14C0.91030.11190.94500.101*
C131.3147 (6)0.0413 (4)0.8765 (2)0.0635 (8)
H13A1.43120.01060.85010.095*
H13B1.23620.04210.90340.095*
H13C1.38380.14060.92010.095*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Br0.0949 (3)0.0686 (3)0.0421 (2)0.01006 (17)0.01910 (16)0.02128 (15)
C110.0583 (16)0.0408 (13)0.0358 (13)0.0098 (12)0.0132 (12)0.0091 (11)
O0.0507 (12)0.0955 (16)0.0468 (11)0.0114 (11)0.0174 (9)0.0161 (11)
C100.0477 (15)0.0507 (15)0.0470 (15)0.0019 (12)0.0133 (12)0.0092 (12)
C170.0508 (16)0.0485 (15)0.0367 (13)0.0058 (12)0.0101 (11)0.0043 (11)
C120.0514 (16)0.0571 (17)0.0394 (14)0.0025 (13)0.0017 (12)0.0104 (12)
C90.0420 (14)0.0502 (15)0.0387 (14)0.0038 (11)0.0027 (11)0.0042 (11)
C80.0449 (14)0.0387 (13)0.0361 (13)0.0085 (10)0.0108 (10)0.0052 (10)
C60.0446 (14)0.0401 (13)0.0501 (15)0.0030 (11)0.0045 (12)0.0112 (12)
C50.0434 (14)0.0507 (15)0.0403 (14)0.0011 (11)0.0081 (11)0.0106 (12)
C30.0434 (14)0.0406 (13)0.0395 (13)0.0027 (10)0.0096 (11)0.0104 (11)
C40.0417 (14)0.0500 (15)0.0421 (14)0.0088 (11)0.0120 (11)0.0098 (12)
C160.0459 (14)0.0452 (14)0.0413 (14)0.0061 (11)0.0113 (11)0.0086 (11)
C20.0528 (15)0.0460 (14)0.0401 (14)0.0052 (12)0.0147 (12)0.0052 (11)
C70.0423 (14)0.0534 (16)0.0428 (15)0.0010 (12)0.0067 (11)0.0107 (12)
C150.0525 (16)0.0562 (16)0.0389 (14)0.0138 (13)0.0139 (12)0.0120 (12)
C10.0432 (14)0.0430 (14)0.0580 (17)0.0092 (11)0.0149 (12)0.0071 (12)
C140.0606 (19)0.103 (3)0.0422 (17)0.0175 (17)0.0120 (14)0.0157 (17)
C130.0604 (19)0.067 (2)0.064 (2)0.0181 (15)0.0032 (15)0.0181 (16)
Geometric parameters (Å, °) top
Br—C111.898 (3)C3—C21.396 (4)
C11—C101.379 (4)C3—C41.395 (4)
C11—C121.382 (4)C3—C161.470 (4)
O—C171.219 (3)C4—H4A0.9300
C10—C91.382 (4)C16—C151.329 (4)
C10—H10A0.9300C16—H16A0.9300
C17—C151.480 (4)C2—C11.389 (4)
C17—C81.495 (4)C2—H2A0.9300
C12—C71.381 (4)C7—H7A0.9300
C12—H12A0.9300C15—H15A0.9300
C9—C81.391 (4)C1—H1A0.9300
C9—H9A0.9300C14—H14A0.9600
C8—C71.396 (4)C14—H14B0.9600
C6—C11.387 (4)C14—H14C0.9600
C6—C51.400 (4)C13—H13A0.9600
C6—C131.510 (4)C13—H13B0.9600
C5—C41.393 (4)C13—H13C0.9600
C5—C141.512 (4)
C10—C11—C12121.5 (2)C3—C4—H4A118.9
C10—C11—Br119.1 (2)C15—C16—C3127.2 (3)
C12—C11—Br119.4 (2)C15—C16—H16A116.4
C11—C10—C9119.1 (2)C3—C16—H16A116.4
C11—C10—H10A120.5C1—C2—C3119.9 (2)
C9—C10—H10A120.5C1—C2—H2A120.1
O—C17—C15122.0 (3)C3—C2—H2A120.1
O—C17—C8119.9 (2)C12—C7—C8120.7 (2)
C15—C17—C8118.0 (2)C12—C7—H7A119.7
C11—C12—C7119.1 (2)C8—C7—H7A119.7
C11—C12—H12A120.5C16—C15—C17120.7 (3)
C7—C12—H12A120.5C16—C15—H15A119.6
C10—C9—C8120.8 (2)C17—C15—H15A119.6
C10—C9—H9A119.6C6—C1—C2121.8 (2)
C8—C9—H9A119.6C6—C1—H1A119.1
C9—C8—C7118.9 (2)C2—C1—H1A119.1
C9—C8—C17123.1 (2)C5—C14—H14A109.5
C7—C8—C17117.9 (2)C5—C14—H14B109.5
C1—C6—C5119.0 (2)H14A—C14—H14B109.5
C1—C6—C13120.0 (3)C5—C14—H14C109.5
C5—C6—C13121.0 (3)H14A—C14—H14C109.5
C4—C5—C6118.9 (2)H14B—C14—H14C109.5
C4—C5—C14120.0 (2)C6—C13—H13A109.5
C6—C5—C14121.1 (3)C6—C13—H13B109.5
C2—C3—C4118.2 (2)H13A—C13—H13B109.5
C2—C3—C16123.1 (2)C6—C13—H13C109.5
C4—C3—C16118.8 (2)H13A—C13—H13C109.5
C5—C4—C3122.3 (2)H13B—C13—H13C109.5
C5—C4—H4A118.9
references
References top

Bruker (1997). SMART and SAINT. Bruker AXS, Inc., Madison, Wisconsin, USA.

Fun, H.-K., Chantrapromma, S., Patil, P. S., D'Silva, E. D. & Dharmaprakash, S. M. (2008). Acta Cryst. E64, o954–o955.

Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122.