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In the title compound, C15H13Cl2NOS, the benzene and thio­phene rings make a dihedral angle of 10.8 (1)°. The dimethyl­amino substituent and the α,β-unsaturated carbonyl group are almost coplanar with respect to the aromatic ring, forming dihedral angles of 4.73 (3)° and 5.0 (2)°, respectively. In the crystal structure, mol­ecules are connected into two-dimensional layers by weak C—H...Cl hydrogen bonds and C—Cl...O [Cl...O = 3.073 (2) Å] inter­actions. These layers are stacked with short C(meth­yl)–H...π contacts betweeen the layers.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536810014364/im2193sup1.cif
Contains datablocks I, global

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536810014364/im2193Isup2.hkl
Contains datablock I

CCDC reference: 778031

Key indicators

  • Single-crystal X-ray study
  • T = 295 K
  • Mean [sigma](C-C) = 0.003 Å
  • R factor = 0.038
  • wR factor = 0.109
  • Data-to-parameter ratio = 17.1

checkCIF/PLATON results

No syntax errors found



Alert level C PLAT431_ALERT_2_C Short Inter HL..A Contact Cl2 .. O6 .. 3.07 Ang. PLAT910_ALERT_3_C Missing # of FCF Reflections Below Th(Min) ..... 1 PLAT152_ALERT_1_C The Supplied and Calc. Volume s.u. Differ by ... -3 Units PLAT480_ALERT_4_C Long H...A H-Bond Reported H16A .. C~G~ .. 3.01 Ang. PLAT716_ALERT_1_C H...A Unknown or Inconsistent Label .......... C~G~ H16A C~G~ PLAT717_ALERT_1_C D...A Unknown or Inconsistent Label .......... C~G~ C16 C~G~ PLAT718_ALERT_1_C D-H..A Unknown or Inconsistent Label .......... C~G~ C16 H16A C~G~ PLAT912_ALERT_4_C Missing # of FCF Reflections Above STh/L= 0.600 553
0 ALERT level A = In general: serious problem 0 ALERT level B = Potentially serious problem 8 ALERT level C = Check and explain 0 ALERT level G = General alerts; check 4 ALERT type 1 CIF construction/syntax error, inconsistent or missing data 1 ALERT type 2 Indicator that the structure model may be wrong or deficient 1 ALERT type 3 Indicator that the structure quality may be low 2 ALERT type 4 Improvement, methodology, query or suggestion 0 ALERT type 5 Informative message, check

Comment top

Chalcones derivatives are known for their interesting pharmacological activities. Radical quenching properties of the phenolic groups present in many chalcones have raised interest in using the compounds themselves or chalcone rich plant extracts as drugs or food preservatives. Apart from being biologically important compounds, chalcone derivatives show non-linear optical properties with excellent blue light transmittance and good crystallizability (Indira et al., 2002; Sarojini et al., 2006). They provide a necessary configuration to show NLO property with two planar rings connected by a conjugated double bond. Synthesis and antimicrobial evaluation of new chalcones containing a 2,5-dichlorothiophene moiety is reported (Tomar et al., 2007). Here, we report the synthesis and crystal structure of the new chalcone derivative, (2E)-1-(2,5-dichlorothiophen-3-yl)-3-(4-dimethylamino-phenyl)prop-2-en-1-one (I, Scheme 1) .

The molecule as a whole does not deviate significantly from planarity (Fig. 1). Dihedral angles between the constituent planar fragments are relatively small. The two ring planes of the phenyl and thiophene groups make a dihedral angle of 10.8 (1)°. The dimethylamino substituent and the α,β-unsaturated carbonyl moeity are inclined with respect to the phenyl ring plane by 4.73 (3)° and 5.0 (2)°, respectively. The bond lengths pattern within the C(=O)—C=C- fragment shows significant conjugation with shorter formal single bonds compared to formal double bonds that are longer than typical values.

In the crystal structure an intermolecular C–H···Cl hydrogen bond (H···Cl distance 2.72 Å, C–H···Cl angle 168°) and C—Cl···O interactions connect the molecules into approximately planar layers parallel to (101) (Fig. 2). The chlorine oxygen interaction also is almost linear (C2–Cl2···O6 angle of 167.6 (8)°) and relatively short (Cl2···O6 3.073 (2) Å). These layers are stacked on each other showing additional intermolecular C–H···π interactions with H16A···Cg distance of 3.01Å (Cg is the centroid of the phenyl ring).

Related literature top

For applications of chalcone derivatives, see: Indira et al. (2002); Sarojini et al. (2006); Tomar et al. (2007).

Experimental top

1-(2,5-Dichlorothiophen-3-yl)ethanone (1.95 g, 0.01 mol) was mixed with 4-dimethylamino)-benzaldehyde (1.49 g, 0.01 mol) and dissolved in ethanol (30 ml). 3 ml of KOH (50%) was added to this solution. The reaction mixture was stirred for 6 hours. The resulting crude solid was filtered, washed successively with distilled water and finally recrystallized from ethanol (95%) to give the pure chalcone. Crystals suitable for x-ray diffraction studies were grown by slow evaporation of solution in toluene (M.P.: 358 K).

Refinement top

H atoms were placed in idealized positions and constrained to ride on their parent atoms, with C–H = 0.93 Å and Uiso(H) = 1.2 Ueq(C) for phenyl hydrogen and olefinic CH groups and with 0.96 Å and Uiso(H) = 1.5 Ueq(C) for CH3 groups.

Structure description top

Chalcones derivatives are known for their interesting pharmacological activities. Radical quenching properties of the phenolic groups present in many chalcones have raised interest in using the compounds themselves or chalcone rich plant extracts as drugs or food preservatives. Apart from being biologically important compounds, chalcone derivatives show non-linear optical properties with excellent blue light transmittance and good crystallizability (Indira et al., 2002; Sarojini et al., 2006). They provide a necessary configuration to show NLO property with two planar rings connected by a conjugated double bond. Synthesis and antimicrobial evaluation of new chalcones containing a 2,5-dichlorothiophene moiety is reported (Tomar et al., 2007). Here, we report the synthesis and crystal structure of the new chalcone derivative, (2E)-1-(2,5-dichlorothiophen-3-yl)-3-(4-dimethylamino-phenyl)prop-2-en-1-one (I, Scheme 1) .

The molecule as a whole does not deviate significantly from planarity (Fig. 1). Dihedral angles between the constituent planar fragments are relatively small. The two ring planes of the phenyl and thiophene groups make a dihedral angle of 10.8 (1)°. The dimethylamino substituent and the α,β-unsaturated carbonyl moeity are inclined with respect to the phenyl ring plane by 4.73 (3)° and 5.0 (2)°, respectively. The bond lengths pattern within the C(=O)—C=C- fragment shows significant conjugation with shorter formal single bonds compared to formal double bonds that are longer than typical values.

In the crystal structure an intermolecular C–H···Cl hydrogen bond (H···Cl distance 2.72 Å, C–H···Cl angle 168°) and C—Cl···O interactions connect the molecules into approximately planar layers parallel to (101) (Fig. 2). The chlorine oxygen interaction also is almost linear (C2–Cl2···O6 angle of 167.6 (8)°) and relatively short (Cl2···O6 3.073 (2) Å). These layers are stacked on each other showing additional intermolecular C–H···π interactions with H16A···Cg distance of 3.01Å (Cg is the centroid of the phenyl ring).

For applications of chalcone derivatives, see: Indira et al. (2002); Sarojini et al. (2006); Tomar et al. (2007).

Computing details top

Data collection: CrysAlis PRO (Oxford Diffraction, 2009); cell refinement: CrysAlis PRO (Oxford Diffraction, 2009); data reduction: CrysAlis PRO (Oxford Diffraction, 2009); program(s) used to solve structure: SIR92 (Altomare et al., 1993); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: ORTEP-3 (Farrugia, 1997) and Mercury (Macrae et al., 2008); software used to prepare material for publication: Stereochemical Workstation Operation Manual (Siemens, 1989) and SHELXL97 (Sheldrick, 2008).

Figures top
[Figure 1] Fig. 1. Molecular structure of (I), showing 50% probability displacement ellipsoids and the atom-numbering scheme.
[Figure 2] Fig. 2. Crystal packing of (I) viewed along the b axis. C–H···Cl hydrogen bonds and C—Cl···O interactions are shown as dashed lines.
[Figure 3] Fig. 3. C–H···π interactions in the stack of molecules (I).
(E)-1-(2,5-Dichloro-3-thienyl)-3-[4-(dimethylamino)phenyl]prop-2-en-1-one top
Crystal data top
C15H13Cl2NOSZ = 2
Mr = 326.22F(000) = 336
Triclinic, P1Dx = 1.450 Mg m3
Hall symbol: -P 1Mo Kα radiation, λ = 0.71073 Å
a = 7.2637 (9) ÅCell parameters from 5611 reflections
b = 8.1136 (9) Åθ = 2.6–28.2°
c = 13.478 (2) ŵ = 0.57 mm1
α = 89.011 (9)°T = 295 K
β = 79.71 (1)°Block, yellow
γ = 73.07 (1)°0.6 × 0.3 × 0.3 mm
V = 747.2 (2) Å3
Data collection top
Oxford Diffraction Xcalibur
diffractometer with an Eos detector
3152 independent reflections
Radiation source: Enhance (Mo) X-ray Source2403 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.018
Detector resolution: 16.1544 pixels mm-1θmax = 28.3°, θmin = 2.6°
ω scanh = 99
Absorption correction: multi-scan
(CrysAlis PRO; Oxford Diffraction, 2009)
k = 1010
Tmin = 0.785, Tmax = 1.000l = 1717
8710 measured reflections
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)] = 0.038Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.109H-atom parameters constrained
S = 1.10 w = 1/[σ2(Fo2) + (0.0546P)2 + 0.1725P]
where P = (Fo2 + 2Fc2)/3
3152 reflections(Δ/σ)max = 0.001
184 parametersΔρmax = 0.37 e Å3
0 restraintsΔρmin = 0.40 e Å3
Crystal data top
C15H13Cl2NOSγ = 73.07 (1)°
Mr = 326.22V = 747.2 (2) Å3
Triclinic, P1Z = 2
a = 7.2637 (9) ÅMo Kα radiation
b = 8.1136 (9) ŵ = 0.57 mm1
c = 13.478 (2) ÅT = 295 K
α = 89.011 (9)°0.6 × 0.3 × 0.3 mm
β = 79.71 (1)°
Data collection top
Oxford Diffraction Xcalibur
diffractometer with an Eos detector
3152 independent reflections
Absorption correction: multi-scan
(CrysAlis PRO; Oxford Diffraction, 2009)
2403 reflections with I > 2σ(I)
Tmin = 0.785, Tmax = 1.000Rint = 0.018
8710 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0380 restraints
wR(F2) = 0.109H-atom parameters constrained
S = 1.10Δρmax = 0.37 e Å3
3152 reflectionsΔρmin = 0.40 e Å3
184 parameters
Special details top

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.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
S10.67788 (8)0.11979 (8)1.11606 (4)0.05238 (18)
Cl20.49256 (8)0.25700 (9)0.94627 (4)0.0620 (2)
C20.6887 (3)0.2294 (3)1.00611 (14)0.0407 (4)
C30.8555 (3)0.2780 (2)0.98033 (14)0.0383 (4)
C40.9777 (3)0.2234 (3)1.05438 (15)0.0431 (5)
H4A1.09800.24431.05070.052*
Cl51.00237 (10)0.05512 (9)1.23148 (4)0.0699 (2)
C50.9014 (3)0.1398 (3)1.12908 (15)0.0454 (5)
C60.9255 (3)0.3667 (3)0.89011 (15)0.0432 (5)
O61.0970 (2)0.3669 (2)0.87491 (13)0.0636 (5)
C70.7927 (3)0.4499 (3)0.82226 (16)0.0473 (5)
H7A0.66210.45190.83780.057*
C80.8548 (3)0.5232 (3)0.73845 (16)0.0456 (5)
H8A0.98450.52420.72830.055*
C90.7452 (3)0.6010 (2)0.66156 (15)0.0412 (4)
C100.5490 (3)0.6086 (3)0.66361 (15)0.0435 (5)
H10A0.48200.56650.71880.052*
C110.4534 (3)0.6765 (3)0.58656 (15)0.0435 (5)
H11A0.32330.67950.59080.052*
C120.5478 (3)0.7420 (2)0.50101 (14)0.0399 (4)
C130.7440 (3)0.7332 (3)0.49862 (16)0.0489 (5)
H13A0.81250.77350.44320.059*
C140.8364 (3)0.6662 (3)0.57683 (16)0.0500 (5)
H14A0.96620.66410.57310.060*
N150.4527 (3)0.8088 (2)0.42422 (14)0.0527 (5)
C160.2469 (4)0.8283 (3)0.4313 (2)0.0669 (7)
H16A0.22670.71650.43080.100*
H16B0.20150.89060.37490.100*
H16C0.17560.89060.49290.100*
C170.5519 (4)0.8642 (4)0.33356 (17)0.0657 (7)
H17A0.59620.95940.34970.098*
H17B0.46360.89960.28680.098*
H17C0.66230.77070.30370.098*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
S10.0501 (3)0.0691 (4)0.0431 (3)0.0253 (3)0.0097 (2)0.0124 (3)
Cl20.0468 (3)0.0961 (5)0.0581 (4)0.0360 (3)0.0242 (3)0.0189 (3)
C20.0371 (10)0.0488 (11)0.0378 (10)0.0123 (9)0.0117 (8)0.0027 (8)
C30.0376 (10)0.0399 (10)0.0387 (10)0.0103 (8)0.0124 (8)0.0024 (8)
C40.0383 (10)0.0475 (12)0.0464 (11)0.0125 (9)0.0160 (9)0.0042 (9)
Cl50.0750 (4)0.0881 (5)0.0490 (3)0.0178 (3)0.0300 (3)0.0209 (3)
C50.0479 (11)0.0516 (12)0.0372 (10)0.0104 (9)0.0162 (9)0.0060 (9)
C60.0400 (10)0.0458 (11)0.0467 (11)0.0139 (9)0.0138 (9)0.0059 (9)
O60.0461 (9)0.0881 (12)0.0681 (11)0.0317 (8)0.0226 (8)0.0325 (9)
C70.0437 (11)0.0525 (12)0.0500 (12)0.0165 (10)0.0170 (9)0.0138 (10)
C80.0436 (11)0.0482 (12)0.0490 (12)0.0165 (9)0.0139 (9)0.0072 (9)
C90.0448 (11)0.0398 (11)0.0408 (10)0.0144 (9)0.0091 (8)0.0057 (8)
C100.0447 (11)0.0474 (12)0.0389 (10)0.0165 (9)0.0046 (8)0.0086 (9)
C110.0382 (10)0.0496 (12)0.0436 (11)0.0148 (9)0.0078 (8)0.0083 (9)
C120.0451 (11)0.0370 (10)0.0379 (10)0.0119 (8)0.0085 (8)0.0044 (8)
C130.0474 (12)0.0568 (13)0.0456 (12)0.0226 (10)0.0054 (9)0.0145 (10)
C140.0404 (11)0.0612 (14)0.0528 (13)0.0217 (10)0.0098 (9)0.0138 (10)
N150.0540 (11)0.0618 (12)0.0466 (10)0.0205 (9)0.0163 (8)0.0205 (8)
C160.0601 (15)0.0778 (17)0.0707 (16)0.0228 (13)0.0302 (13)0.0236 (13)
C170.0734 (17)0.0800 (17)0.0454 (13)0.0247 (14)0.0132 (12)0.0191 (12)
Geometric parameters (Å, º) top
S1—C21.717 (2)C10—C111.371 (3)
S1—C51.717 (2)C10—H10A0.9300
Cl2—C21.7175 (19)C11—C121.411 (3)
C2—C31.366 (3)C11—H11A0.9300
C3—C41.433 (3)C12—N151.364 (3)
C3—C61.489 (3)C12—C131.401 (3)
C4—C51.333 (3)C13—C141.371 (3)
C4—H4A0.9300C13—H13A0.9300
Cl5—C51.718 (2)C14—H14A0.9300
C6—O61.226 (2)N15—C171.439 (3)
C6—C71.462 (3)N15—C161.443 (3)
C7—C81.335 (3)C16—H16A0.9600
C7—H7A0.9300C16—H16B0.9600
C8—C91.444 (3)C16—H16C0.9600
C8—H8A0.9300C17—H17A0.9600
C9—C141.391 (3)C17—H17B0.9600
C9—C101.403 (3)C17—H17C0.9600
C2—S1—C589.86 (10)C10—C11—C12121.54 (19)
C3—C2—S1113.70 (14)C10—C11—H11A119.2
C3—C2—Cl2130.86 (16)C12—C11—H11A119.2
S1—C2—Cl2115.43 (11)N15—C12—C13121.88 (18)
C2—C3—C4110.04 (18)N15—C12—C11121.47 (19)
C2—C3—C6130.73 (17)C13—C12—C11116.65 (18)
C4—C3—C6119.18 (17)C14—C13—C12120.89 (19)
C5—C4—C3113.12 (18)C14—C13—H13A119.6
C5—C4—H4A123.4C12—C13—H13A119.6
C3—C4—H4A123.4C13—C14—C9123.04 (19)
C4—C5—S1113.29 (15)C13—C14—H14A118.5
C4—C5—Cl5127.12 (17)C9—C14—H14A118.5
S1—C5—Cl5119.59 (13)C12—N15—C17121.73 (19)
O6—C6—C7121.58 (19)C12—N15—C16121.05 (19)
O6—C6—C3117.89 (17)C17—N15—C16117.22 (19)
C7—C6—C3120.54 (17)N15—C16—H16A109.5
C8—C7—C6121.49 (19)N15—C16—H16B109.5
C8—C7—H7A119.3H16A—C16—H16B109.5
C6—C7—H7A119.3N15—C16—H16C109.5
C7—C8—C9127.96 (19)H16A—C16—H16C109.5
C7—C8—H8A116.0H16B—C16—H16C109.5
C9—C8—H8A116.0N15—C17—H17A109.5
C14—C9—C10116.05 (18)N15—C17—H17B109.5
C14—C9—C8120.06 (18)H17A—C17—H17B109.5
C10—C9—C8123.80 (18)N15—C17—H17C109.5
C11—C10—C9121.81 (18)H17A—C17—H17C109.5
C11—C10—H10A119.1H17B—C17—H17C109.5
C9—C10—H10A119.1
C5—S1—C2—C30.36 (17)C6—C7—C8—C9176.1 (2)
C5—S1—C2—Cl2179.45 (13)C7—C8—C9—C14177.7 (2)
S1—C2—C3—C40.3 (2)C7—C8—C9—C101.0 (4)
Cl2—C2—C3—C4179.25 (16)C14—C9—C10—C110.0 (3)
S1—C2—C3—C6176.89 (17)C8—C9—C10—C11176.8 (2)
Cl2—C2—C3—C62.0 (4)C9—C10—C11—C120.1 (3)
C2—C3—C4—C50.1 (3)C10—C11—C12—N15179.72 (19)
C6—C3—C4—C5177.47 (18)C10—C11—C12—C130.3 (3)
C3—C4—C5—S10.1 (2)N15—C12—C13—C14179.7 (2)
C3—C4—C5—Cl5179.88 (15)C11—C12—C13—C140.9 (3)
C2—S1—C5—C40.28 (18)C12—C13—C14—C91.0 (4)
C2—S1—C5—Cl5179.74 (14)C10—C9—C14—C130.5 (3)
C2—C3—C6—O6166.3 (2)C8—C9—C14—C13176.4 (2)
C4—C3—C6—O610.7 (3)C13—C12—N15—C174.0 (3)
C2—C3—C6—C713.5 (3)C11—C12—N15—C17175.4 (2)
C4—C3—C6—C7169.47 (18)C13—C12—N15—C16175.5 (2)
O6—C6—C7—C83.0 (3)C11—C12—N15—C165.2 (3)
C3—C6—C7—C8176.8 (2)
Hydrogen-bond geometry (Å, º) top
Cg is the centroid of the phenyl ring.
D—H···AD—HH···AD···AD—H···A
C16—H16B···Cl5i0.962.723.664 (2)168
C16—H16A···Cgii0.963.013.899 (3)155
Symmetry codes: (i) x1, y+1, z1; (ii) x+1, y+1, z+1.

Experimental details

Crystal data
Chemical formulaC15H13Cl2NOS
Mr326.22
Crystal system, space groupTriclinic, P1
Temperature (K)295
a, b, c (Å)7.2637 (9), 8.1136 (9), 13.478 (2)
α, β, γ (°)89.011 (9), 79.71 (1), 73.07 (1)
V3)747.2 (2)
Z2
Radiation typeMo Kα
µ (mm1)0.57
Crystal size (mm)0.6 × 0.3 × 0.3
Data collection
DiffractometerOxford Diffraction Xcalibur
diffractometer with an Eos detector
Absorption correctionMulti-scan
(CrysAlis PRO; Oxford Diffraction, 2009)
Tmin, Tmax0.785, 1.000
No. of measured, independent and
observed [I > 2σ(I)] reflections
8710, 3152, 2403
Rint0.018
(sin θ/λ)max1)0.666
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.038, 0.109, 1.10
No. of reflections3152
No. of parameters184
H-atom treatmentH-atom parameters constrained
Δρmax, Δρmin (e Å3)0.37, 0.40

Computer programs: CrysAlis PRO (Oxford Diffraction, 2009), SIR92 (Altomare et al., 1993), ORTEP-3 (Farrugia, 1997) and Mercury (Macrae et al., 2008), Stereochemical Workstation Operation Manual (Siemens, 1989) and SHELXL97 (Sheldrick, 2008).

Hydrogen-bond geometry (Å, º) top
Cg is the centroid of the phenyl ring.
D—H···AD—HH···AD···AD—H···A
C16—H16B···Cl5i0.962.723.664 (2)168.3
C16—H16A···Cgii0.963.013.899 (3)154.8
Symmetry codes: (i) x1, y+1, z1; (ii) x+1, y+1, z+1.
 

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