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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2012 Feb 17;68(Pt 3):o778. doi: 10.1107/S1600536812006629

(2E,6E)-2,6-Bis(2,6-dichloro­benzyl­idene)­cyclo­hexa­none

Gholam Hossein Mahdavinia a,*, Maryam Mirzazadeh a, Vahid Amani b, Behrouz Notash c
PMCID: PMC3297849  PMID: 22412652

Abstract

The title compound, C20H14Cl4O, was prepared by the reaction of 2,6-dichloro­benzaldehyde and cyclo­hexa­none. In the mol­ecule, the central cyclo­hexa­none ring adopts an envelope conformation, while the terminal benzene rings make a dihedral angle of 57.87 (9)°.

Related literature  

For background and applications of aryl­idene cyclo­alkanones, see: Deli et al. (1984); Nakano et al. (1987); Kawamata et al. (1996); Dimmock et al. (2003); Raj et al. (2003); Gangadhara (1995). For related structures, see: Yu et al. (2000); Zhou (2007).graphic file with name e-68-0o778-scheme1.jpg

Experimental  

Crystal data  

  • C20H14Cl4O

  • M r = 412.11

  • Orthorhombic, Inline graphic

  • a = 17.917 (4) Å

  • b = 7.3094 (15) Å

  • c = 14.093 (3) Å

  • V = 1845.7 (7) Å3

  • Z = 4

  • Mo Kα radiation

  • μ = 0.65 mm−1

  • T = 120 K

  • 0.6 × 0.35 × 0.33 mm

Data collection  

  • Stoe IPDS 2T diffractometer

  • 13510 measured reflections

  • 4946 independent reflections

  • 4682 reflections with I > 2σ(I)

  • R int = 0.043

Refinement  

  • R[F 2 > 2σ(F 2)] = 0.031

  • wR(F 2) = 0.071

  • S = 1.04

  • 4946 reflections

  • 226 parameters

  • 1 restraint

  • H-atom parameters constrained

  • Δρmax = 0.25 e Å−3

  • Δρmin = −0.20 e Å−3

  • Absolute structure: Flack (1983), 2369 Friedel pairs

  • Flack parameter: 0.01 (4)

Data collection: X-AREA (Stoe & Cie, 2005); cell refinement: X-AREA; data reduction: X-RED32 (Stoe & Cie, 2005); program(s) used to solve structure: SHELXTL (Sheldrick, 2008); program(s) used to refine structure: SHELXTL; molecular graphics: SHELXTL; software used to prepare material for publication: SHELXTL.

Supplementary Material

Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536812006629/xu5466sup1.cif

e-68-0o778-sup1.cif (19.2KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812006629/xu5466Isup2.hkl

e-68-0o778-Isup2.hkl (242.3KB, hkl)

Supplementary material file. DOI: 10.1107/S1600536812006629/xu5466Isup3.cml

Additional supplementary materials: crystallographic information; 3D view; checkCIF report

Acknowledgments

We are grateful to the Islamic Azad University, Marvdasht Branch, for financial support.

supplementary crystallographic information

Comment

Cross-aldol condensation of aromatic aldehydes with cyclic ketones is an important protocol for the synthesis of arylidene cycloalkanones, which are very important precursors to potentially bioactive pyrimidine derivates (Deli et al., 1984), intermediates for agrochemical, pharmaceuticals and perfumes (Nakano et al., 1987), new organic material for nonlinear optical applications (Kawamata et al., 1996), cytotoxic analogous (Dimmock et al., 2003), bis-spiropyrrolidines (Raj et al., 2003) and the units of liquid crystalline polymers (Gangadhara, 1995). Usually, this condensation process is catalyzed by strong acid or base.

In the molecule of the title compound, (Fig. 1), the bond lengths and angles are within normal ranges (Yu et al., 2000; Zhou, 2007). A dihedral angle of 57.87 (9) A is found between the mean planes of the two benzene rings.

Experimental

To a 10 ml solution of KOH (0.11 g) in ethanol at 313 K in a round bottom flask, cyclohexanone (5.0 mmol, 0.50 g) and 2,6-dichlorobenzaldehyde (10 mmol, 1.75 g) was added and the mixture was stirred for 2 min. The resulting product was then isolated by simple filtration from the reaction mixture and given washings with water to remove any trace of KOH remaining on the product. Yellow crystals, yield 97%, 1.98 g, m. p. 455–458 K.

Refinement

All H atoms were positioned geometrically with C–H = 0.93–0.97 Å and constrained to ride on their parent atoms, with Uiso(H) = 1.2Ueq(C).

Figures

Fig. 1.

Fig. 1.

The molecular structure of the title molecule, with the atom-numbering scheme. Displacement ellipsoids are drawn at the 50% probability level.

Crystal data

C20H14Cl4O F(000) = 840
Mr = 412.11 Dx = 1.483 Mg m3
Orthorhombic, Pna21 Mo Kα radiation, λ = 0.71073 Å
Hall symbol: P 2c -2n Cell parameters from 4949 reflections
a = 17.917 (4) Å θ = 2.3–29.2°
b = 7.3094 (15) Å µ = 0.65 mm1
c = 14.093 (3) Å T = 120 K
V = 1845.7 (7) Å3 Needle, yellow
Z = 4 0.6 × 0.35 × 0.33 mm

Data collection

Stoe IPDS 2T diffractometer 4682 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tube Rint = 0.043
Graphite monochromator θmax = 29.2°, θmin = 2.3°
rotation method scans h = −24→24
13510 measured reflections k = −8→10
4946 independent reflections l = −19→19

Refinement

Refinement on F2 Secondary atom site location: difference Fourier map
Least-squares matrix: full Hydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.031 H-atom parameters constrained
wR(F2) = 0.071 w = 1/[σ2(Fo2) + (0.0318P)2 + 0.5994P] where P = (Fo2 + 2Fc2)/3
S = 1.04 (Δ/σ)max = 0.001
4946 reflections Δρmax = 0.25 e Å3
226 parameters Δρmin = −0.20 e Å3
1 restraint Absolute structure: Flack (1983), 2369 Friedel pairs
Primary atom site location: structure-invariant direct methods Flack parameter: 0.01 (4)

Special details

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)

x y z Uiso*/Ueq
Cl1 0.23181 (3) 1.40628 (7) 0.99333 (3) 0.03179 (11)
Cl3 −0.14648 (3) 0.88978 (7) 0.82912 (3) 0.03028 (10)
Cl4 0.05216 (3) 0.35099 (7) 0.89917 (4) 0.03460 (11)
Cl2 0.30403 (3) 0.77001 (7) 1.16748 (4) 0.03902 (13)
C12 0.04419 (9) 0.8310 (2) 0.91901 (11) 0.0196 (3)
O1 0.04467 (7) 0.94480 (19) 1.07669 (9) 0.0237 (3)
C6 0.27374 (10) 1.0891 (2) 1.07795 (12) 0.0211 (3)
C13 0.07918 (9) 0.9234 (2) 1.00226 (12) 0.0185 (3)
C7 0.19499 (9) 1.0268 (2) 1.07289 (12) 0.0199 (3)
H7 0.1686 1.0178 1.1295 0.024*
C9 0.19554 (9) 0.9844 (3) 0.89597 (12) 0.0253 (3)
H9A 0.2490 0.9679 0.9032 0.030*
H9B 0.1872 1.1026 0.8666 0.030*
C15 −0.05043 (9) 0.6110 (2) 0.85940 (12) 0.0209 (3)
C5 0.32884 (10) 0.9818 (3) 1.12039 (12) 0.0252 (4)
C18 −0.11451 (11) 0.3989 (3) 0.71361 (15) 0.0317 (4)
H18 −0.1354 0.3295 0.6651 0.038*
C8 0.15938 (9) 0.9827 (2) 0.99274 (12) 0.0186 (3)
C1 0.29745 (11) 1.2584 (3) 1.04280 (12) 0.0253 (4)
C16 −0.02454 (10) 0.4355 (3) 0.83722 (14) 0.0246 (3)
C10 0.16500 (10) 0.8350 (3) 0.83127 (13) 0.0278 (4)
H10A 0.1873 0.8457 0.7688 0.033*
H10B 0.1777 0.7157 0.8568 0.033*
C19 −0.14239 (10) 0.5721 (3) 0.73292 (14) 0.0281 (4)
H19 −0.1820 0.6191 0.6979 0.034*
C11 0.08055 (10) 0.8530 (3) 0.82365 (12) 0.0260 (4)
H11A 0.0681 0.9721 0.7978 0.031*
H11B 0.0615 0.7605 0.7806 0.031*
C3 0.42366 (10) 1.2027 (3) 1.08876 (13) 0.0318 (4)
H3 0.4733 1.2393 1.0916 0.038*
C14 −0.01489 (9) 0.7245 (2) 0.93404 (12) 0.0211 (3)
H14 −0.0350 0.7210 0.9948 0.025*
C20 −0.11038 (10) 0.6741 (3) 0.80531 (12) 0.0222 (3)
C17 −0.05563 (11) 0.3289 (3) 0.76625 (15) 0.0295 (4)
H17 −0.0373 0.2122 0.7541 0.035*
C4 0.40302 (11) 1.0347 (3) 1.12538 (14) 0.0296 (4)
H4 0.4384 0.9584 1.1530 0.036*
C2 0.37123 (11) 1.3166 (3) 1.04810 (13) 0.0298 (4)
H2 0.3850 1.4306 1.0246 0.036*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
Cl1 0.0347 (2) 0.0280 (2) 0.0326 (2) −0.00606 (18) −0.00506 (19) 0.0103 (2)
Cl3 0.0346 (2) 0.0290 (2) 0.0272 (2) 0.00852 (18) −0.00735 (18) −0.00764 (19)
Cl4 0.0329 (2) 0.0303 (2) 0.0406 (3) 0.00904 (18) −0.0048 (2) −0.0030 (2)
Cl2 0.0393 (2) 0.0295 (2) 0.0483 (3) −0.0027 (2) −0.0170 (2) 0.0103 (2)
C12 0.0205 (7) 0.0212 (8) 0.0172 (7) 0.0006 (6) −0.0003 (6) −0.0023 (6)
O1 0.0229 (6) 0.0316 (7) 0.0167 (5) −0.0022 (5) 0.0025 (4) −0.0034 (5)
C6 0.0233 (7) 0.0252 (8) 0.0147 (6) −0.0025 (6) −0.0014 (6) −0.0006 (6)
C13 0.0185 (7) 0.0214 (7) 0.0157 (7) 0.0020 (6) 0.0008 (6) 0.0017 (6)
C7 0.0214 (7) 0.0217 (7) 0.0166 (7) −0.0015 (6) −0.0011 (6) 0.0020 (6)
C9 0.0218 (8) 0.0344 (10) 0.0197 (7) −0.0056 (7) 0.0038 (7) −0.0032 (8)
C15 0.0188 (7) 0.0219 (8) 0.0219 (7) −0.0041 (6) 0.0023 (6) −0.0011 (6)
C5 0.0273 (9) 0.0279 (9) 0.0204 (8) −0.0009 (7) −0.0027 (7) −0.0023 (7)
C18 0.0259 (9) 0.0345 (10) 0.0348 (10) −0.0081 (8) 0.0025 (7) −0.0151 (9)
C8 0.0196 (7) 0.0193 (7) 0.0169 (6) −0.0001 (6) 0.0001 (6) 0.0010 (6)
C1 0.0267 (8) 0.0313 (9) 0.0179 (7) −0.0039 (7) −0.0008 (6) 0.0017 (7)
C16 0.0228 (7) 0.0228 (8) 0.0283 (9) −0.0013 (6) 0.0026 (7) −0.0026 (7)
C10 0.0276 (8) 0.0360 (10) 0.0197 (7) −0.0038 (7) 0.0050 (7) −0.0068 (8)
C19 0.0233 (8) 0.0340 (10) 0.0270 (9) −0.0018 (7) −0.0015 (7) −0.0090 (8)
C11 0.0289 (8) 0.0331 (10) 0.0160 (7) −0.0077 (7) 0.0011 (7) −0.0018 (7)
C3 0.0220 (8) 0.0518 (12) 0.0216 (8) −0.0093 (8) 0.0008 (7) −0.0069 (8)
C14 0.0212 (7) 0.0233 (8) 0.0187 (7) −0.0006 (7) −0.0001 (6) −0.0014 (6)
C20 0.0217 (8) 0.0232 (8) 0.0216 (8) −0.0014 (7) 0.0017 (6) −0.0040 (6)
C17 0.0281 (9) 0.0241 (9) 0.0362 (10) −0.0048 (7) 0.0066 (8) −0.0085 (8)
C4 0.0232 (8) 0.0412 (11) 0.0243 (8) 0.0021 (8) −0.0063 (7) −0.0062 (8)
C2 0.0299 (9) 0.0386 (10) 0.0210 (8) −0.0137 (8) 0.0032 (7) 0.0017 (8)

Geometric parameters (Å, º)

Cl1—C1 1.743 (2) C5—C4 1.386 (3)
Cl3—C20 1.7370 (19) C18—C17 1.388 (3)
Cl4—C16 1.7414 (19) C18—C19 1.388 (3)
Cl2—C5 1.742 (2) C18—H18 0.9300
C12—C14 1.331 (2) C1—C2 1.391 (3)
C12—C13 1.492 (2) C16—C17 1.385 (3)
C12—C11 1.502 (2) C10—C11 1.523 (3)
O1—C13 1.228 (2) C10—H10A 0.9700
C6—C5 1.396 (3) C10—H10B 0.9700
C6—C1 1.399 (3) C19—C20 1.388 (2)
C6—C7 1.484 (2) C19—H19 0.9300
C13—C8 1.507 (2) C11—H11A 0.9700
C7—C8 1.337 (2) C11—H11B 0.9700
C7—H7 0.9300 C3—C2 1.380 (3)
C9—C8 1.510 (2) C3—C4 1.382 (3)
C9—C10 1.524 (3) C3—H3 0.9300
C9—H9A 0.9700 C14—H14 0.9300
C9—H9B 0.9700 C17—H17 0.9300
C15—C20 1.396 (2) C4—H4 0.9300
C15—C16 1.399 (3) C2—H2 0.9300
C15—C14 1.483 (2)
C14—C12—C13 118.29 (15) C15—C16—Cl4 118.34 (14)
C14—C12—C11 123.35 (15) C11—C10—C9 109.69 (15)
C13—C12—C11 118.23 (14) C11—C10—H10A 109.7
C5—C6—C1 115.73 (17) C9—C10—H10A 109.7
C5—C6—C7 121.37 (17) C11—C10—H10B 109.7
C1—C6—C7 122.89 (16) C9—C10—H10B 109.7
O1—C13—C12 121.19 (15) H10A—C10—H10B 108.2
O1—C13—C8 121.32 (16) C18—C19—C20 119.04 (18)
C12—C13—C8 117.45 (14) C18—C19—H19 120.5
C8—C7—C6 124.63 (15) C20—C19—H19 120.5
C8—C7—H7 117.7 C12—C11—C10 111.02 (15)
C6—C7—H7 117.7 C12—C11—H11A 109.4
C8—C9—C10 112.35 (15) C10—C11—H11A 109.4
C8—C9—H9A 109.1 C12—C11—H11B 109.4
C10—C9—H9A 109.1 C10—C11—H11B 109.4
C8—C9—H9B 109.1 H11A—C11—H11B 108.0
C10—C9—H9B 109.1 C2—C3—C4 120.58 (18)
H9A—C9—H9B 107.9 C2—C3—H3 119.7
C20—C15—C16 115.85 (16) C4—C3—H3 119.7
C20—C15—C14 122.20 (16) C12—C14—C15 123.77 (15)
C16—C15—C14 121.93 (16) C12—C14—H14 118.1
C4—C5—C6 122.88 (19) C15—C14—H14 118.1
C4—C5—Cl2 118.28 (15) C19—C20—C15 122.83 (18)
C6—C5—Cl2 118.83 (14) C19—C20—Cl3 118.41 (14)
C17—C18—C19 120.36 (18) C15—C20—Cl3 118.76 (13)
C17—C18—H18 119.8 C16—C17—C18 118.97 (18)
C19—C18—H18 119.8 C16—C17—H17 120.5
C7—C8—C13 116.69 (15) C18—C17—H17 120.5
C7—C8—C9 123.82 (15) C3—C4—C5 119.07 (19)
C13—C8—C9 119.47 (14) C3—C4—H4 120.5
C2—C1—C6 122.69 (18) C5—C4—H4 120.5
C2—C1—Cl1 118.25 (16) C3—C2—C1 119.02 (19)
C6—C1—Cl1 119.03 (14) C3—C2—H2 120.5
C17—C16—C15 122.94 (18) C1—C2—H2 120.5
C17—C16—Cl4 118.69 (15)
C14—C12—C13—O1 −20.1 (3) C14—C15—C16—Cl4 −0.5 (2)
C11—C12—C13—O1 163.96 (17) C8—C9—C10—C11 55.7 (2)
C14—C12—C13—C8 157.57 (16) C17—C18—C19—C20 0.2 (3)
C11—C12—C13—C8 −18.4 (2) C14—C12—C11—C10 −132.96 (18)
C5—C6—C7—C8 −112.5 (2) C13—C12—C11—C10 42.8 (2)
C1—C6—C7—C8 68.8 (3) C9—C10—C11—C12 −61.2 (2)
C1—C6—C5—C4 −2.0 (3) C13—C12—C14—C15 −173.89 (16)
C7—C6—C5—C4 179.24 (17) C11—C12—C14—C15 1.8 (3)
C1—C6—C5—Cl2 179.18 (13) C20—C15—C14—C12 −92.9 (2)
C7—C6—C5—Cl2 0.4 (2) C16—C15—C14—C12 85.4 (2)
C6—C7—C8—C13 −179.65 (16) C18—C19—C20—C15 0.7 (3)
C6—C7—C8—C9 2.1 (3) C18—C19—C20—Cl3 −179.49 (15)
O1—C13—C8—C7 12.3 (2) C16—C15—C20—C19 −0.8 (3)
C12—C13—C8—C7 −165.39 (16) C14—C15—C20—C19 177.55 (17)
O1—C13—C8—C9 −169.41 (17) C16—C15—C20—Cl3 179.37 (13)
C12—C13—C8—C9 12.9 (2) C14—C15—C20—Cl3 −2.3 (2)
C10—C9—C8—C7 146.11 (18) C15—C16—C17—C18 0.8 (3)
C10—C9—C8—C13 −32.1 (2) Cl4—C16—C17—C18 −176.99 (15)
C5—C6—C1—C2 0.9 (3) C19—C18—C17—C16 −0.9 (3)
C7—C6—C1—C2 179.69 (17) C2—C3—C4—C5 0.2 (3)
C5—C6—C1—Cl1 −177.17 (13) C6—C5—C4—C3 1.4 (3)
C7—C6—C1—Cl1 1.6 (2) Cl2—C5—C4—C3 −179.70 (14)
C20—C15—C16—C17 0.1 (3) C4—C3—C2—C1 −1.2 (3)
C14—C15—C16—C17 −178.32 (17) C6—C1—C2—C3 0.6 (3)
C20—C15—C16—Cl4 177.86 (13) Cl1—C1—C2—C3 178.73 (14)

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: XU5466).

References

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Associated Data

This section collects any data citations, data availability statements, or supplementary materials included in this article.

Supplementary Materials

Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536812006629/xu5466sup1.cif

e-68-0o778-sup1.cif (19.2KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812006629/xu5466Isup2.hkl

e-68-0o778-Isup2.hkl (242.3KB, hkl)

Supplementary material file. DOI: 10.1107/S1600536812006629/xu5466Isup3.cml

Additional supplementary materials: crystallographic information; 3D view; checkCIF report


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