supplementary materials


Acta Cryst. (2009). E65, o739    [ doi:10.1107/S1600536809007430 ]

(E)-1-(4-Chlorophenyl)-3-[4-(dimethylamino)phenyl]prop-2-en-1-one

X. Lei and X. Bai

Abstract top

The title compound, C17H16ClNO, was synthesized using a solvent-free method by reaction of 4-(dimethylamino)benzaldehyde with 4-chloroacetophenone and NaOH. The chlorophenyl ring makes a dihedral angle of 18.1 (3)° with the central propenone unit, while the (dimethylamino)phenyl group is disordered over two orientations of equal occupancies, which make dihedral angles with the central propenone unit of 32.9 (3) and 57.4 (3)°, respectively.

Comment top

This paper discloses a user-friendly, solvent-free protocol for the synthesis of chalcones, starting from the fragrant aldehydes and fragrant ketones in the presence of NaOH. The method can be considered to be a general route for chalcone synthesis, and the title compound was prepared in this way.

The bond lengths and angles of the molecule (Fig. 1) are normal and comparable to those observed in the related compound (Li et al., 1992). The (dimethylamino)phenyl group exhibits rotational disorder, with one orientation including atoms C10, C11, C12, C13, C14 and C15, and another orientation including C10, C11', C12', C13, C14' and C15'. The refined site occupancy factors for the two orientations is 0.500 (5).

Related literature top

For a related structure, see: Li et al. (1992).

Experimental top

4-(Dimethylamino)benzaldehyde (0.5 mmol) and 4-chloroacetophenone (0.5 mmol), NaOH (0.5 mmol) were mixed in 50 ml flask under solvent-free conditions After stirring for 6 min at 373 K, the mixture was slowly solidified to give the title compound. Recrystallization from ethanol gave a yellow crystalline solid. Elemental analysis calculated: C 71.45, H 5.64, N 4.90%; found: C 71.53, H 5.56, N 4.95%.

Refinement top

All H atoms were positioned geometrically and refined using a riding model with C—H = 0.93–0.96 Å and Uiso(H) = 1.2 or 1.5Ueq(C). The five-membered ring was treated as disordered between two orientations with site occupancy factors refined to 0.500 (5). The bonds N1—C16, N1—C16', N1—C17 and N1—C17' were restrained to be 1.47 (1)Å.

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 showing 30% probability displacement ellipsoids for non-H atoms.
(E)-1-(4-Chlorophenyl)-3-[4-(dimethylamino)phenyl]prop-2-en-1-one top
Crystal data top
C17H16ClNOF(000) = 600
Mr = 285.76Dx = 1.283 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ybcCell parameters from 987 reflections
a = 16.792 (2) Åθ = 2.5–19.9°
b = 14.5602 (16) ŵ = 0.25 mm1
c = 6.1160 (8) ÅT = 298 K
β = 98.333 (2)°Needle, yellow
V = 1479.5 (3) Å30.42 × 0.20 × 0.13 mm
Z = 4
Data collection top
Bruker SMART CCD
diffractometer
2605 independent reflections
Radiation source: fine-focus sealed tube1066 reflections with I > 2˘I)
graphiteRint = 0.068
φ and ω scansθmax = 25.0°, θmin = 1.9°
Absorption correction: multi-scan
(SADABS; Sheldrick, 2003)
h = 1919
Tmin = 0.901, Tmax = 0.968k = 1712
7357 measured reflectionsl = 77
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.059Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.170H-atom parameters constrained
S = 0.90 w = 1/[σ2(Fo2) + (0.0749P)2]
where P = (Fo2 + 2Fc2)/3
2605 reflections(Δ/σ)max < 0.001
237 parametersΔρmax = 0.16 e Å3
4 restraintsΔρmin = 0.12 e Å3
Crystal data top
C17H16ClNOV = 1479.5 (3) Å3
Mr = 285.76Z = 4
Monoclinic, P21/cMo Kα radiation
a = 16.792 (2) ŵ = 0.25 mm1
b = 14.5602 (16) ÅT = 298 K
c = 6.1160 (8) Å0.42 × 0.20 × 0.13 mm
β = 98.333 (2)°
Data collection top
Bruker SMART CCD
diffractometer
2605 independent reflections
Absorption correction: multi-scan
(SADABS; Sheldrick, 2003)
1066 reflections with I > 2˘I)
Tmin = 0.901, Tmax = 0.968Rint = 0.068
7357 measured reflectionsθmax = 25.0°
Refinement top
R[F2 > 2σ(F2)] = 0.059H-atom parameters constrained
wR(F2) = 0.170Δρmax = 0.16 e Å3
S = 0.90Δρmin = 0.12 e Å3
2605 reflectionsAbsolute structure: ?
237 parametersFlack parameter: ?
4 restraintsRogers parameter: ?
Special details top

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.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/UeqOcc. (<1)
Cl11.12683 (6)0.14642 (9)1.2060 (3)0.1285 (7)
N10.34724 (18)0.1225 (2)0.8419 (7)0.0891 (11)
O10.80650 (17)0.1009 (2)0.4377 (6)0.1225 (12)
C10.8071 (2)0.1135 (2)0.6344 (8)0.0739 (11)
C20.8853 (2)0.1192 (2)0.7831 (7)0.0683 (10)
C30.8921 (2)0.1538 (2)0.9959 (7)0.0742 (11)
H30.84600.17121.05300.089*
C40.9663 (2)0.1627 (2)1.1247 (7)0.0801 (11)
H40.97010.18681.26660.096*
C51.0345 (2)0.1356 (3)1.0416 (9)0.0831 (12)
C61.0292 (3)0.0990 (3)0.8348 (9)0.0889 (13)
H61.07550.07920.78160.107*
C70.9552 (2)0.0914 (2)0.7048 (7)0.0792 (11)
H70.95200.06730.56290.095*
C80.7314 (2)0.1221 (2)0.7236 (7)0.0754 (11)
H80.73430.12720.87620.090*
C90.6615 (2)0.1233 (3)0.6088 (7)0.0872 (12)
H90.66170.12250.45680.105*
C100.5811 (2)0.1255 (3)0.6741 (6)0.0639 (9)
C110.5655 (5)0.0979 (6)0.8724 (14)0.055 (2)0.500 (5)
H110.60760.08210.98210.065*0.500 (5)
C120.4860 (5)0.0928 (6)0.9147 (13)0.059 (2)0.500 (5)
H120.47730.06511.04630.070*0.500 (5)
C130.4234 (2)0.1232 (2)0.7863 (7)0.0639 (10)
C140.4419 (4)0.1658 (5)0.5679 (11)0.057 (2)0.500 (5)
H140.40070.18850.46410.068*0.500 (5)
C150.5208 (4)0.1695 (5)0.5295 (12)0.059 (2)0.500 (5)
H150.53390.20120.40750.070*0.500 (5)
C160.2783 (5)0.0794 (8)0.7432 (18)0.103 (4)0.500 (5)
H16A0.25830.11020.60740.154*0.510 (7)
H16B0.23830.08150.84040.154*0.510 (7)
H16C0.29020.01660.71280.154*0.510 (7)
C170.3364 (5)0.1683 (7)1.0661 (13)0.106 (4)0.500 (5)
H17A0.38110.15261.17580.158*0.510 (7)
H17B0.28740.14661.11230.158*0.510 (7)
H17C0.33380.23371.04830.158*0.510 (7)
C11'0.5658 (5)0.1596 (6)0.8637 (16)0.060 (2)0.500 (5)
H11'0.60890.18420.95810.073*0.500 (5)
C12'0.4923 (4)0.1618 (6)0.9327 (12)0.060 (2)0.500 (5)
H12'0.48590.18701.06880.072*0.500 (5)
C14'0.4368 (4)0.0774 (5)0.6145 (12)0.059 (2)0.500 (5)
H14'0.39490.04450.53440.070*0.500 (5)
C15'0.5112 (4)0.0760 (5)0.5472 (12)0.064 (2)0.500 (5)
H15'0.51840.04360.42030.076*0.500 (5)
C16'0.2804 (4)0.1498 (7)0.6472 (14)0.090 (3)0.500 (5)
H16D0.29190.20950.59310.135*0.490 (7)
H16E0.22900.15090.69880.135*0.490 (7)
H16F0.27910.10560.53020.135*0.490 (7)
C17'0.3231 (5)0.0619 (6)0.9866 (13)0.079 (3)0.500 (5)
H17D0.34310.00190.95900.119*0.490 (7)
H17E0.26540.06040.96880.119*0.490 (7)
H17F0.34370.08041.13470.119*0.490 (7)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Cl10.0640 (8)0.1472 (12)0.1697 (14)0.0010 (6)0.0012 (8)0.0022 (9)
N10.053 (2)0.084 (2)0.132 (3)0.0039 (18)0.021 (2)0.008 (3)
O10.085 (2)0.211 (4)0.078 (2)0.001 (2)0.0324 (18)0.006 (2)
C10.069 (3)0.072 (3)0.087 (3)0.0025 (19)0.033 (2)0.000 (2)
C20.061 (2)0.061 (2)0.089 (3)0.0045 (18)0.032 (2)0.003 (2)
C30.059 (3)0.080 (3)0.087 (3)0.0014 (18)0.024 (2)0.003 (2)
C40.074 (3)0.075 (3)0.094 (3)0.001 (2)0.022 (2)0.003 (2)
C50.060 (3)0.074 (3)0.118 (4)0.003 (2)0.023 (3)0.007 (3)
C60.071 (3)0.084 (3)0.120 (4)0.003 (2)0.043 (3)0.005 (3)
C70.074 (3)0.074 (3)0.097 (3)0.001 (2)0.037 (3)0.007 (2)
C80.062 (2)0.090 (3)0.077 (3)0.010 (2)0.021 (2)0.015 (2)
C90.071 (3)0.130 (3)0.063 (3)0.021 (2)0.018 (2)0.019 (2)
C100.058 (2)0.075 (2)0.059 (3)0.007 (2)0.0076 (19)0.001 (2)
C110.050 (5)0.057 (5)0.056 (6)0.007 (4)0.003 (4)0.004 (5)
C120.069 (6)0.057 (5)0.052 (5)0.006 (5)0.013 (4)0.000 (4)
C130.050 (2)0.054 (2)0.087 (3)0.0039 (19)0.005 (2)0.008 (2)
C140.057 (5)0.051 (5)0.058 (5)0.002 (3)0.000 (3)0.008 (3)
C150.066 (5)0.053 (5)0.058 (5)0.007 (4)0.012 (4)0.003 (3)
C160.076 (6)0.114 (8)0.118 (10)0.024 (6)0.015 (6)0.030 (7)
C170.071 (6)0.151 (9)0.098 (8)0.002 (5)0.025 (5)0.002 (6)
C11'0.053 (5)0.058 (6)0.067 (6)0.005 (5)0.001 (4)0.012 (5)
C12'0.058 (5)0.072 (6)0.051 (5)0.008 (5)0.011 (4)0.008 (4)
C14'0.047 (4)0.060 (6)0.067 (5)0.005 (3)0.000 (4)0.011 (4)
C15'0.067 (5)0.064 (6)0.060 (5)0.005 (4)0.008 (4)0.006 (4)
C16'0.049 (5)0.111 (8)0.105 (8)0.001 (5)0.001 (5)0.014 (6)
C17'0.076 (5)0.094 (7)0.071 (7)0.011 (5)0.023 (5)0.011 (5)
Geometric parameters (Å, °) top
Cl1—C51.729 (4)C11—H110.930
N1—C17'1.353 (7)C12—C131.296 (8)
N1—C131.370 (4)C12—H120.930
N1—C161.377 (7)C13—C14'1.292 (7)
N1—C171.559 (7)C13—C12'1.468 (8)
N1—C16'1.565 (7)C13—C141.545 (8)
O1—C11.215 (4)C14—C151.379 (8)
C1—C81.460 (5)C14—H140.930
C1—C21.486 (5)C15—H150.930
C2—C31.385 (5)C16—H16A0.960
C2—C71.391 (4)C16—H16B0.960
C3—C41.379 (5)C16—H16C0.960
C3—H30.930C17—H17A0.960
C4—C51.376 (5)C17—H17B0.960
C4—H40.930C17—H17C0.960
C5—C61.364 (5)C11'—C12'1.362 (10)
C6—C71.380 (5)C11'—H11'0.930
C6—H60.930C12'—H12'0.930
C7—H70.930C14'—C15'1.372 (9)
C8—C91.278 (5)C14'—H14'0.930
C8—H80.930C15'—H15'0.930
C9—C101.463 (5)C16'—H16D0.960
C9—H90.930C16'—H16E0.960
C10—C11'1.320 (9)C16'—H16F0.960
C10—C111.339 (9)C17'—H17D0.960
C10—C151.399 (8)C17'—H17E0.960
C10—C15'1.495 (8)C17'—H17F0.960
C11—C121.398 (10)
C17'—N1—C13123.1 (5)N1—C13—C12'122.2 (5)
C13—N1—C16130.6 (5)C12—C13—C14114.4 (5)
C13—N1—C17116.6 (4)N1—C13—C14122.0 (4)
C16—N1—C17112.5 (5)C15—C14—C13118.8 (6)
C17'—N1—C16'114.4 (6)C15—C14—H14120.6
C13—N1—C16'113.7 (5)C13—C14—H14120.6
O1—C1—C8120.0 (4)C14—C15—C10119.9 (6)
O1—C1—C2119.6 (3)C14—C15—H15120.0
C8—C1—C2120.4 (4)C10—C15—H15120.0
C3—C2—C7118.0 (4)N1—C16—H16A109.5
C3—C2—C1122.8 (3)N1—C16—H16B109.5
C7—C2—C1119.2 (4)H16A—C16—H16B109.5
C4—C3—C2121.1 (4)N1—C16—H16C109.5
C4—C3—H3119.5H16A—C16—H16C109.5
C2—C3—H3119.5H16B—C16—H16C109.5
C5—C4—C3119.5 (4)N1—C17—H17A109.5
C5—C4—H4120.2N1—C17—H17B109.5
C3—C4—H4120.2H17A—C17—H17B109.5
C6—C5—C4120.6 (4)N1—C17—H17C109.5
C6—C5—Cl1120.5 (3)H17A—C17—H17C109.5
C4—C5—Cl1118.9 (4)H17B—C17—H17C109.5
C5—C6—C7119.8 (4)C10—C11'—C12'125.5 (7)
C5—C6—H6120.1C10—C11'—H11'117.2
C7—C6—H6120.1C12'—C11'—H11'117.2
C6—C7—C2120.9 (4)C11'—C12'—C13118.2 (7)
C6—C7—H7119.6C11'—C12'—H12'120.9
C2—C7—H7119.6C13—C12'—H12'120.9
C9—C8—C1125.2 (4)C13—C14'—C15'121.8 (6)
C9—C8—H8117.4C13—C14'—H14'119.1
C1—C8—H8117.4C15'—C14'—H14'119.1
C8—C9—C10131.4 (4)C14'—C15'—C10121.1 (6)
C8—C9—H9114.3C14'—C15'—H15'119.4
C10—C9—H9114.3C10—C15'—H15'119.4
C11—C10—C15119.4 (5)N1—C16'—H16D109.5
C11—C10—C9123.4 (4)N1—C16'—H16E109.5
C15—C10—C9116.7 (4)H16D—C16'—H16E109.5
C9—C10—C15'122.2 (4)N1—C16'—H16F109.5
C10—C11—C12120.1 (6)H16D—C16'—H16F109.5
C10—C11—H11120.0H16E—C16'—H16F109.5
C12—C11—H11120.0N1—C17'—H17D109.5
C13—C12—C11125.6 (7)N1—C17'—H17E109.5
C13—C12—H12117.2H17D—C17'—H17E109.5
C11—C12—H12117.2N1—C17'—H17F109.5
C14'—C13—N1118.5 (4)H17D—C17'—H17F109.5
C12—C13—N1123.5 (5)H17E—C17'—H17F109.5
C14'—C13—C12'118.6 (5)
Acknowledgements top

This project was supported by the Foundation of Tianshui Normal University.

references
References top

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

Li, Z.-D., Huang, L.-Z., Su, G.-B. & Wang, H.-Y. (1992). Chin. J. Struct. Chem. 11, 1–4.

Sheldrick, G. M. (2003). SADABS. University of Göttingen, Germany.

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