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The title compound, C17H12Cl2O, has a cyclo­hexenone ring in the half-chair conformation. The aryl ring in the side chain attached to the tetralone ring is twisted out of the plane of the α,β-unsaturated ketone plane as a result of non-bonded interactions.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S160053680200747X/ob6126sup1.cif
Contains datablocks I, 1853

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S160053680200747X/ob6126Isup2.hkl
Contains datablock I

CCDC reference: 185807

Key indicators

  • Single-crystal X-ray study
  • T = 193 K
  • Mean [sigma](C-C) = 0.003 Å
  • R factor = 0.033
  • wR factor = 0.082
  • Data-to-parameter ratio = 14.7

checkCIF results

No syntax errors found

ADDSYM reports no extra symmetry


Yellow Alert Alert Level C:
ABSTM_02 Alert C The ratio of expected to reported Tmax/Tmin(RR') is < 0.90 Tmin and Tmax reported: 0.682 0.962 Tmin' and Tmax expected: 0.852 0.956 RR' = 0.795 Please check that your absorption correction is appropriate.
0 Alert Level A = Potentially serious problem
0 Alert Level B = Potential problem
1 Alert Level C = Please check

Comment top

Recently, the synthesis and cytotoxic properties of a series of 2-arylidenebenzocycloalkanones were reported (Dimmock et al., 1999), which revealed, inter alia, that the relative positions of the two aryl rings influenced bioactivity. In order to develop structure–activity relationships in this group of compounds, analogues with ortho substituents were required, including 2-(2,4-dichlorophenylmethylene)-1-tetralone, (I). During the synthesis of (I), a second product was isolated which was shown by X-ray crystallography to be 2-(2,4-dichlorophenyl-hydroxymethyl)-1-tetralone, (II) (Oloo et al., 2002).

The cyclohexenone (C1—C2—C3—C4—C5—C10) ring of (I) has one multiple bond shared with the phenyl moiety and two external double bonds (the carbonyl O and C11 attached to C2). The atoms in the cyclohexenone ring adopted a conformation, with C2 and C3 on the same side of the plane determined by the other four atoms. Conjugation of the dichlorophenyl group with the α,β-unsaturated ketone should favor coplanarity, but steric effects interfere. The torsion angle C2—C11—C12—C17 is -39.6 (3)°, indicating that the aryl ring (C12–C17) is twisted out of the plane of the α,β-unsaturated ketone. This effect may be due to the Cl1···H11 and O···H11 non-bonded repulsions, since these interatomic distances are 2.72 and 2.40 Å, respectively. In addition, the distance between H17 and the pseudo-equatorial H atom on atom C3 is 2.29 Å, which may also contribute to the torsion angle observed.

Compound (I) has no possibility of classical hydrogen bonding. In Table 1, a non-classical intramolecular hydrogen bond is shown between H11 and O. In addition, intermolecular hydrogen bonds are listed between H4 and O, between H11 and Cl2, and between H17 and O, which link the molecules into a three-dimensional network.

Experimental top

An ice-cold solution of sodium hydroxide (0.005 mol) in water (0.25 ml) and methanol (50 ml) was added to an ice-cold solution of 2,4-dichlorobenzaldehyde (0.01 mol) and 1-tetralone (0.01 mol) in methanol (75 ml). After stirring at room temperature for 2 d, the mixture was refrigerated (268 K) for 1 d and the precipitate collected and dried. Column chromatography using keiselgel 60 and an eluting solvent of toluene afforded (I) (m.p. 381–383 K) in 56% yield, while an eluting solvent of 1% methanol in toluene led to 2-(2,4-dichlorophenyl-hydroxymethyl)-1-tetralone, (II) (m.p. 444–446 K) in 13% yield. Elemental analysis, calculated for C17H12Cl2O: C 67.35, H 3.99%; found: C 67.21, H 3.73%. The cytotoxicity of (I) was determined using murine P388 and L1210 cells, as well as human Molt 4/C8 and CEM T-lymphocytes. The IC50 values of (I) were 17.2±0.5, 34.4±5.4, 28.4±7.6 and 8.73±1.24 µM, respectively.

Refinement top

All H atoms were placed in calculated positions on their parent C atoms (C—H = 0.99 Å on aliphatic C atoms and 0.95 Å on aromatic C atoms). The Uiso value of each H atom was assigned as equal to 1.2 times the Ueq of the attached C atom.

Computing details top

Data collection: SMART (Bruker, 1998); cell refinement: SAINT (Bruker, 1998); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: Xtal3.7 (Hall et al., 2000); software used to prepare material for publication: SHELXL97.

Figures top
[Figure 1] Fig. 1. The molecular structure of (I), with displacement ellipsoids drawn at the 50% probability level.
2-(2,4-dichlorophenylmethylene)-1-tetralone top
Crystal data top
C17H12Cl2OF(000) = 624
Mr = 303.17Dx = 1.435 Mg m3
Monoclinic, P21/cMelting point = 381–383 K
Hall symbol: -P 2ybcMo Kα radiation, λ = 0.71073 Å
a = 12.3695 (9) ÅCell parameters from 5425 reflections
b = 13.7644 (10) Åθ = 2.5–25°
c = 8.2403 (6) ŵ = 0.45 mm1
β = 90.01 (1)°T = 193 K
V = 1402.98 (18) Å3Prism, colourless
Z = 40.35 × 0.10 × 0.10 mm
Data collection top
Bruker SMART1000 CCD
diffractometer
2668 independent reflections
Radiation source: fine-focus sealed tube2022 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.047
Detector resolution: 17 pixels mm-1θmax = 25.8°, θmin = 1.7°
CCD scansh = 1515
Absorption correction: multi-scan
(SADABS; Blessing, 1995)
k = 1615
Tmin = 0.682, Tmax = 0.962l = 109
8415 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)] = 0.033Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.082H-atom parameters constrained
S = 0.98 w = 1/[σ2(Fo2) + (0.0418P)2]
where P = (Fo2 + 2Fc2)/3
2668 reflections(Δ/σ)max = 0.005
181 parametersΔρmax = 0.21 e Å3
0 restraintsΔρmin = 0.19 e Å3
Crystal data top
C17H12Cl2OV = 1402.98 (18) Å3
Mr = 303.17Z = 4
Monoclinic, P21/cMo Kα radiation
a = 12.3695 (9) ŵ = 0.45 mm1
b = 13.7644 (10) ÅT = 193 K
c = 8.2403 (6) Å0.35 × 0.10 × 0.10 mm
β = 90.01 (1)°
Data collection top
Bruker SMART1000 CCD
diffractometer
2668 independent reflections
Absorption correction: multi-scan
(SADABS; Blessing, 1995)
2022 reflections with I > 2σ(I)
Tmin = 0.682, Tmax = 0.962Rint = 0.047
8415 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0330 restraints
wR(F2) = 0.082H-atom parameters constrained
S = 0.98Δρmax = 0.21 e Å3
2668 reflectionsΔρmin = 0.19 e Å3
181 parameters
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 was by full-matrix least-squares methods. 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
Cl10.53090 (4)0.24397 (4)0.41220 (7)0.04201 (16)
Cl20.64505 (4)0.04634 (4)0.80642 (6)0.03862 (15)
O0.16014 (9)0.36507 (9)0.45961 (17)0.0375 (3)
C10.12921 (13)0.28081 (14)0.4465 (2)0.0282 (4)
C20.19817 (13)0.19697 (13)0.4989 (2)0.0266 (4)
C30.14545 (13)0.09859 (14)0.5011 (2)0.0306 (4)
H3A0.10080.09220.60010.037*
H3B0.20190.04770.50420.037*
C40.07426 (14)0.08367 (14)0.3512 (2)0.0336 (5)
H4A0.12050.08120.25320.040*
H4B0.03600.02070.36050.040*
C50.00700 (14)0.16379 (15)0.3329 (2)0.0337 (5)
C60.10931 (15)0.14709 (17)0.2676 (3)0.0446 (6)
H60.12930.08320.23580.053*
C70.18195 (17)0.2225 (2)0.2486 (3)0.0553 (7)
H70.25120.21010.20320.066*
C80.15467 (16)0.3155 (2)0.2951 (3)0.0544 (7)
H80.20530.36680.28270.065*
C90.05385 (15)0.33414 (16)0.3597 (2)0.0412 (5)
H90.03500.39830.39130.049*
C100.02048 (14)0.25846 (14)0.3787 (2)0.0316 (5)
C110.30183 (14)0.21563 (13)0.5357 (2)0.0271 (4)
H110.32520.28070.51990.033*
C120.38339 (13)0.14768 (12)0.5974 (2)0.0255 (4)
C130.49238 (13)0.15561 (13)0.5509 (2)0.0257 (4)
C140.57174 (13)0.09564 (13)0.6111 (2)0.0271 (4)
H140.64440.10180.57510.032*
C150.54406 (14)0.02651 (13)0.7244 (2)0.0276 (4)
C160.43831 (14)0.01589 (14)0.7764 (2)0.0301 (4)
H160.42000.03210.85460.036*
C170.35992 (14)0.07620 (13)0.7127 (2)0.0285 (4)
H170.28740.06890.74840.034*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Cl10.0294 (2)0.0449 (3)0.0518 (4)0.0006 (2)0.0041 (2)0.0214 (3)
Cl20.0382 (3)0.0394 (3)0.0383 (3)0.0128 (2)0.0011 (2)0.0065 (2)
O0.0330 (7)0.0261 (8)0.0534 (10)0.0024 (6)0.0024 (6)0.0010 (6)
C10.0251 (8)0.0312 (11)0.0282 (11)0.0016 (8)0.0081 (8)0.0006 (8)
C20.0261 (9)0.0270 (10)0.0268 (10)0.0001 (8)0.0044 (8)0.0009 (8)
C30.0267 (9)0.0286 (10)0.0365 (11)0.0023 (8)0.0018 (8)0.0017 (9)
C40.0293 (9)0.0325 (11)0.0388 (12)0.0070 (8)0.0011 (8)0.0014 (9)
C50.0266 (9)0.0444 (12)0.0300 (11)0.0033 (8)0.0035 (8)0.0040 (9)
C60.0315 (10)0.0576 (15)0.0445 (14)0.0066 (10)0.0024 (9)0.0030 (11)
C70.0284 (11)0.084 (2)0.0530 (16)0.0002 (12)0.0090 (10)0.0073 (14)
C80.0330 (11)0.0735 (18)0.0566 (16)0.0166 (11)0.0033 (10)0.0107 (14)
C90.0331 (10)0.0475 (13)0.0429 (13)0.0084 (9)0.0030 (9)0.0056 (11)
C100.0241 (9)0.0402 (12)0.0306 (11)0.0008 (8)0.0055 (8)0.0075 (9)
C110.0286 (9)0.0220 (9)0.0309 (11)0.0002 (8)0.0024 (8)0.0028 (8)
C120.0250 (8)0.0246 (10)0.0271 (10)0.0010 (7)0.0014 (7)0.0049 (8)
C130.0281 (9)0.0253 (10)0.0237 (10)0.0034 (7)0.0003 (7)0.0012 (8)
C140.0237 (8)0.0313 (10)0.0262 (10)0.0011 (8)0.0012 (7)0.0030 (8)
C150.0316 (9)0.0265 (10)0.0247 (10)0.0063 (8)0.0027 (8)0.0043 (8)
C160.0354 (10)0.0277 (10)0.0272 (11)0.0001 (8)0.0019 (8)0.0008 (8)
C170.0256 (8)0.0295 (10)0.0304 (11)0.0019 (8)0.0031 (8)0.0038 (8)
Geometric parameters (Å, º) top
Cl1—C131.7357 (18)C7—C81.378 (3)
Cl2—C151.7386 (17)C7—H70.9500
O—C11.226 (2)C8—C91.380 (3)
C1—C101.488 (2)C8—H80.9500
C1—C21.499 (3)C9—C101.398 (3)
C2—C111.342 (2)C9—H90.9500
C2—C31.503 (2)C11—C121.467 (2)
C3—C41.530 (2)C11—H110.9500
C3—H3A0.9900C12—C171.398 (2)
C3—H3B0.9900C12—C131.406 (2)
C4—C51.500 (3)C13—C141.375 (2)
C4—H4A0.9900C14—C151.376 (3)
C4—H4B0.9900C14—H140.9500
C5—C61.394 (3)C15—C161.384 (2)
C5—C101.398 (3)C16—C171.380 (2)
C6—C71.382 (3)C16—H160.9500
C6—H60.9500C17—H170.9500
O—C1—C10120.71 (16)C9—C8—H8120.0
O—C1—C2121.69 (16)C8—C9—C10119.9 (2)
C10—C1—C2117.60 (16)C8—C9—H9120.0
C11—C2—C1117.48 (16)C10—C9—H9120.0
C11—C2—C3125.74 (16)C9—C10—C5120.29 (17)
C1—C2—C3116.76 (15)C9—C10—C1118.82 (18)
C2—C3—C4111.16 (16)C5—C10—C1120.89 (16)
C2—C3—H3A109.4C2—C11—C12127.83 (17)
C4—C3—H3A109.4C2—C11—H11116.1
C2—C3—H3B109.4C12—C11—H11116.1
C4—C3—H3B109.4C17—C12—C13116.05 (15)
H3A—C3—H3B108.0C17—C12—C11122.77 (15)
C5—C4—C3111.60 (16)C13—C12—C11121.04 (16)
C5—C4—H4A109.3C14—C13—C12122.65 (16)
C3—C4—H4A109.3C14—C13—Cl1117.53 (13)
C5—C4—H4B109.3C12—C13—Cl1119.82 (13)
C3—C4—H4B109.3C13—C14—C15118.82 (16)
H4A—C4—H4B108.0C13—C14—H14120.6
C6—C5—C10118.57 (18)C15—C14—H14120.6
C6—C5—C4121.73 (19)C14—C15—C16121.22 (16)
C10—C5—C4119.68 (16)C14—C15—Cl2118.92 (13)
C7—C6—C5120.7 (2)C16—C15—Cl2119.84 (15)
C7—C6—H6119.7C17—C16—C15118.84 (17)
C5—C6—H6119.7C17—C16—H16120.6
C8—C7—C6120.5 (2)C15—C16—H16120.6
C8—C7—H7119.8C16—C17—C12122.40 (16)
C6—C7—H7119.8C16—C17—H17118.8
C7—C8—C9120.1 (2)C12—C17—H17118.8
C7—C8—H8120.0
O—C1—C2—C1110.8 (3)C2—C1—C10—C9167.10 (17)
C10—C1—C2—C11169.74 (17)O—C1—C10—C5167.00 (18)
O—C1—C2—C3170.81 (18)C2—C1—C10—C513.6 (3)
C10—C1—C2—C38.6 (2)C1—C2—C11—C12176.61 (17)
C11—C2—C3—C4136.25 (19)C3—C2—C11—C125.2 (3)
C1—C2—C3—C442.0 (2)C2—C11—C12—C1739.6 (3)
C2—C3—C4—C554.3 (2)C2—C11—C12—C13144.8 (2)
C3—C4—C5—C6146.85 (18)C17—C12—C13—C141.5 (3)
C3—C4—C5—C1034.6 (2)C11—C12—C13—C14177.41 (16)
C10—C5—C6—C70.0 (3)C17—C12—C13—Cl1178.44 (13)
C4—C5—C6—C7178.6 (2)C11—C12—C13—Cl12.6 (2)
C5—C6—C7—C80.5 (4)C12—C13—C14—C151.6 (3)
C6—C7—C8—C90.6 (4)Cl1—C13—C14—C15178.36 (14)
C7—C8—C9—C100.3 (3)C13—C14—C15—C160.8 (3)
C8—C9—C10—C50.2 (3)C13—C14—C15—Cl2177.58 (13)
C8—C9—C10—C1179.13 (19)C14—C15—C16—C170.0 (3)
C6—C5—C10—C90.4 (3)Cl2—C15—C16—C17178.35 (13)
C4—C5—C10—C9178.93 (18)C15—C16—C17—C120.0 (3)
C6—C5—C10—C1178.96 (18)C13—C12—C17—C160.7 (3)
C4—C5—C10—C10.4 (3)C11—C12—C17—C16176.51 (16)
O—C1—C10—C912.3 (3)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C11—H11···O0.952.402.774 (2)103
C4—H4A···Oi0.992.583.470 (2)150
C11—H11···Cl2ii0.952.803.5858 (18)140
C17—H17···Oiii0.952.523.302 (2)140
Symmetry codes: (i) x, y+1/2, z1/2; (ii) x+1, y+1/2, z+3/2; (iii) x, y+1/2, z+1/2.

Experimental details

Crystal data
Chemical formulaC17H12Cl2O
Mr303.17
Crystal system, space groupMonoclinic, P21/c
Temperature (K)193
a, b, c (Å)12.3695 (9), 13.7644 (10), 8.2403 (6)
β (°) 90.01 (1)
V3)1402.98 (18)
Z4
Radiation typeMo Kα
µ (mm1)0.45
Crystal size (mm)0.35 × 0.10 × 0.10
Data collection
DiffractometerBruker SMART1000 CCD
diffractometer
Absorption correctionMulti-scan
(SADABS; Blessing, 1995)
Tmin, Tmax0.682, 0.962
No. of measured, independent and
observed [I > 2σ(I)] reflections
8415, 2668, 2022
Rint0.047
(sin θ/λ)max1)0.612
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.033, 0.082, 0.98
No. of reflections2668
No. of parameters181
H-atom treatmentH-atom parameters constrained
Δρmax, Δρmin (e Å3)0.21, 0.19

Computer programs: SMART (Bruker, 1998), SAINT (Bruker, 1998), SAINT, SHELXS97 (Sheldrick, 1997), SHELXL97 (Sheldrick, 1997), Xtal3.7 (Hall et al., 2000), SHELXL97.

Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C11—H11···O0.952.402.774 (2)103.1
C4—H4A···Oi0.992.583.470 (2)150.0
C11—H11···Cl2ii0.952.803.5858 (18)140.4
C17—H17···Oiii0.952.523.302 (2)140.1
Symmetry codes: (i) x, y+1/2, z1/2; (ii) x+1, y+1/2, z+3/2; (iii) x, y+1/2, z+1/2.
 

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