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On slow evaporation of an ethyl acetate solution, the title compound, C22H24N2O3, crystallizes simultaneously in two crystalline forms, differing in colour, size and shape. The mol­ecule in the violet plate-like monoclinic crystal reported here is almost planar with the exception of the di­methyl­cyclo­hexene moiety, which has a twisted conformation. The red triclinic crystals [see Kolev et al. (2001a), Acta Cryst. E57, o966-o967] are built of the same mol­ecules with similar geometry; however, the cyclo­hexene fragment in the triclinic crystal has a more symmetric sofa conformation. Another difference between the structures is the existence of a non-classical hydrogen bond involving one of the nitrile groups in the triclinic form. The mol­ecules in the monoclinic form are held together by van der Waals interactions.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536801015203/ya6055sup1.cif
Contains datablocks I, global

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536801015203/ya6055Isup2.hkl
Contains datablock I

CCDC reference: 175368

Key indicators

  • Single-crystal X-ray study
  • T = 291 K
  • Mean [sigma](C-C) = 0.003 Å
  • R factor = 0.054
  • wR factor = 0.136
  • Data-to-parameter ratio = 14.7

checkCIF results

No syntax errors found

ADDSYM reports no extra symmetry


Yellow Alert Alert Level C:
ABSMU_01 Alert C The ratio of given/expected absorption coefficient lies outside the range 0.99 <> 1.01 Calculated value of mu = 0.081 Value of mu given = 0.080 PLAT_371 Alert C Long C(sp2)-C(sp1) Bond C(7) - C(8) = 1.42 Ang. PLAT_371 Alert C Long C(sp2)-C(sp1) Bond C(7) - C(9) = 1.43 Ang.
0 Alert Level A = Potentially serious problem
0 Alert Level B = Potential problem
3 Alert Level C = Please check

Comment top

Due to their solvatochromic behaviour (Lemke, 1970), the derivatives of 2-(5,5-dimethyl-3-styrylcyclohex-2-enylidene)malononitrile are supposed to be good candidates for nonlinear optical (NLO) and electrooptical applications. In the course of our investigations on this class of substances, we studied the crystal structures of the title compound, (I).

The mean molecular plane orientations in the monoclinic crystal of the title compound alternate between (113) and (113). The least-squares plane through atoms C1/C2/C3/C4/C6 in the cyclohexene ring indicates a better planarity for the plane in the triclinic crystal (Kolev et al., 2001a) [χ2 = 44, maximum deviation from planarity = 0.0090 (19) Å] than in the monoclinic crystal [χ2 = 676, maximum deviation from planarity = 0.035 (3) Å]. The dihedral angle between this plane and the least-squares plane of the C14—C19 phenyl ring is 4.69 (5)° in the triclinic and 8.87 (8)° in the monoclinic crystal, which means that the deviations from the overall planarity of the molecule are also smaller in the triclinic crystal. The six torsion angles in the cyclohexene ring [triclinic: -0.8 (3), 1.7 (3), -28.6 (3), 51.7 (2), 27.2 (3) and -51.4 (2)°; monoclinic: -3.0 (4), -2.7 (4), 32.0 (3), -52.8 (3), -21.2 (3) and 47.8 (3)°; both sequences correspond to endocyclic torsion angles associated with the bonds C1—C2 through C6—C1 in the cycle] indicate a higher symmetry of the conformation of the cyclohexene ring in the triclinic crystal.

In the triclinic crystal, the intermolecular contact of 2.60 Å between the H10C and N2(x + 1, y, z) atoms indicates a non-classical hydrogen bond [with the C10—H10C ··· N2(x + 1, y, z) angle equal to 160°], whereas the molecules in the monoclinic crystal are held together by pure van der Waals interactions.

Experimental top

The title compound was synthesized using a general procedure described by Lemke (1970). The preparation of the starting compound, 3,5,5-trimethyl(cyclohex-2-enylidene)malonodinitrile, C12H14N2, is described in one of our previous papers (Kolev et al., 2001b). The starting compound (5 mmol) was dissolved in 60 ml of dry toluene by continuous stirring. 2,4,6-Trimethoxy-benzaldehyde (5 mmol) was added to the solution, and nearly 1 ml of triethylamine was used as a catalyst. The solution became red after a few minutes and the resulting compound precipitated. After 6 h reaction time, the solution was cooled and 2-{5,5-dimethyl-3-[2-(2,4,6-trimethoxyphenyl)vinyl]cyclohex-2-enylidene}- malononitrile was isolated and recrystallized twice from ethyl acetate with an excellent yield of 92% (m.p. 477–478 K). The purity of the compound was confirmed by elemental analysis, IR, UV-vis and mass spectrometry. Two types of crystals, different in colour, size and shape, were grown simultaneously from an ethyl acetate solution by slow evaporation over a period of several days. They were separated manually.

Refinement top

H atoms were placed in calculated positions with Uiso constrained to be 1.5Ueq of the carrier atom for the methyl-H and 1.2Ueq for the remaining H atoms.

Computing details top

Data collection: COLLECT (Nonius, 1998); cell refinement: DENZO and SCALEPACK (Otwinowski & Minor, 1997); data reduction: DENZO and SCALEPACK; program(s) used to solve structure: SHELXS97 (Sheldrick, 1990); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: SHELXTL-Plus (Sheldrick, 1991); software used to prepare material for publication: SHELXL97 (Sheldrick, 1997), PARST95 (Nardelli, 1995) and PLATON (Spek, 2001).

Figures top
[Figure 1] Fig. 1. View of the title compound showing the labelling of non-H atoms. Displacement ellipsoids are shown at 50% probability level. H atoms are drawn as circles of arbitrary radii.
(I) top
Crystal data top
C22H24N2O3F(000) = 776
Mr = 364.43Dx = 1.209 Mg m3
Monoclinic, P21/nMo Kα radiation, λ = 0.71073 Å
a = 10.7130 (3) ÅCell parameters from 30702 reflections
b = 9.0471 (3) Åθ = 3.1–25.4°
c = 20.6565 (7) ŵ = 0.08 mm1
β = 90.1565 (13)°T = 291 K
V = 2002.05 (11) Å3Plate, violet
Z = 40.5 × 0.3 × 0.15 mm
Data collection top
Nonius KappaCCD
diffractometer
1654 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tubeRint = 0.063
Graphite monochromatorθmax = 25.4°, θmin = 3.1°
Detector resolution: 19 vertical, 18 horizontal pixels mm-1h = 1212
277 frames via ω–rotation (Δω = 1°) and two times 5 s per frame with 3 sets at different κ–angles scansk = 1010
30702 measured reflectionsl = 2424
3595 independent 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)] = 0.054Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.136H-atom parameters constrained
S = 0.95 w = 1/[σ2(Fo2) + (0.0589P)2]
where P = (Fo2 + 2Fc2)/3
3595 reflections(Δ/σ)max < 0.001
244 parametersΔρmax = 0.15 e Å3
0 restraintsΔρmin = 0.16 e Å3
Crystal data top
C22H24N2O3V = 2002.05 (11) Å3
Mr = 364.43Z = 4
Monoclinic, P21/nMo Kα radiation
a = 10.7130 (3) ŵ = 0.08 mm1
b = 9.0471 (3) ÅT = 291 K
c = 20.6565 (7) Å0.5 × 0.3 × 0.15 mm
β = 90.1565 (13)°
Data collection top
Nonius KappaCCD
diffractometer
1654 reflections with I > 2σ(I)
30702 measured reflectionsRint = 0.063
3595 independent reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0540 restraints
wR(F2) = 0.136H-atom parameters constrained
S = 0.95Δρmax = 0.15 e Å3
3595 reflectionsΔρmin = 0.16 e Å3
244 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 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
O10.10139 (17)0.90442 (19)0.11949 (8)0.0608 (5)
O20.42499 (17)1.2395 (2)0.16927 (8)0.0702 (6)
O30.34379 (18)1.0912 (2)0.05091 (8)0.0667 (6)
N10.3470 (2)0.3285 (3)0.19234 (12)0.0763 (8)
N20.3435 (2)0.4407 (3)0.01276 (12)0.0730 (8)
C10.0244 (2)0.7186 (3)0.06374 (11)0.0439 (7)
C20.0796 (2)0.6328 (3)0.05675 (12)0.0484 (7)
H2A0.11730.62870.01630.058*
C30.1332 (2)0.5494 (3)0.10815 (11)0.0443 (7)
C40.0761 (2)0.5612 (3)0.17384 (11)0.0516 (7)
H4A0.11540.64200.19710.062*
H4B0.09260.47090.19770.062*
C50.0648 (3)0.5875 (3)0.17162 (11)0.0488 (7)
C60.0906 (2)0.7210 (3)0.12797 (11)0.0531 (7)
H6A0.17980.72670.12000.064*
H6B0.06640.81000.15100.064*
C70.2374 (2)0.4644 (3)0.09854 (12)0.0462 (7)
C80.2971 (3)0.3882 (3)0.15042 (14)0.0541 (8)
C90.2964 (2)0.4523 (3)0.03675 (14)0.0513 (7)
C100.1314 (3)0.4501 (3)0.14482 (13)0.0674 (9)
H10A0.21970.46790.14320.101*
H10B0.11480.36710.17250.101*
H10C0.10140.42940.10200.101*
C110.1124 (3)0.6189 (3)0.23995 (11)0.0688 (9)
H11A0.07050.70420.25710.103*
H11B0.09610.53510.26720.103*
H11C0.20070.63730.23840.103*
C120.0679 (2)0.8073 (3)0.01057 (11)0.0474 (7)
H12A0.02650.79950.02880.057*
C130.1659 (2)0.9015 (3)0.01442 (12)0.0487 (7)
H13A0.20120.90820.05540.058*
C140.2251 (2)0.9934 (3)0.03385 (11)0.0441 (7)
C150.1980 (2)0.9932 (3)0.10053 (12)0.0470 (7)
C160.2659 (2)1.0761 (3)0.14411 (12)0.0503 (7)
H16A0.24681.07320.18800.060*
C170.3627 (3)1.1635 (3)0.12208 (13)0.0500 (7)
C180.3915 (2)1.1729 (3)0.05700 (12)0.0507 (7)
H18A0.45561.23380.04260.061*
C190.3225 (2)1.0889 (3)0.01405 (12)0.0469 (7)
C200.0710 (3)0.8997 (3)0.18625 (12)0.0708 (9)
H20A0.00200.83360.19270.106*
H20B0.04840.99700.20070.106*
H20C0.14190.86550.21050.106*
C210.5353 (3)1.3159 (4)0.15154 (13)0.0894 (11)
H21A0.56951.36470.18890.134*
H21B0.51591.38800.11890.134*
H21C0.59521.24690.13490.134*
C220.4402 (3)1.1844 (3)0.07536 (12)0.0698 (9)
H22A0.44411.17510.12160.105*
H22B0.51881.15560.05680.105*
H22C0.42271.28520.06410.105*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O10.0710 (14)0.0688 (12)0.0427 (11)0.0252 (11)0.0075 (10)0.0015 (9)
O20.0683 (14)0.0987 (15)0.0435 (12)0.0360 (12)0.0040 (10)0.0147 (11)
O30.0832 (15)0.0771 (13)0.0399 (11)0.0340 (11)0.0080 (10)0.0066 (9)
N10.077 (2)0.088 (2)0.0637 (18)0.0232 (15)0.0099 (15)0.0043 (14)
N20.0706 (19)0.0879 (19)0.0605 (17)0.0119 (14)0.0111 (15)0.0050 (14)
C10.0482 (18)0.0435 (16)0.0400 (16)0.0007 (13)0.0036 (13)0.0022 (12)
C20.0524 (19)0.0552 (17)0.0377 (16)0.0046 (14)0.0003 (14)0.0030 (13)
C30.0456 (18)0.0490 (16)0.0382 (16)0.0012 (14)0.0062 (13)0.0010 (13)
C40.054 (2)0.0604 (18)0.0401 (16)0.0031 (14)0.0057 (14)0.0011 (13)
C50.0523 (19)0.0546 (17)0.0395 (16)0.0051 (14)0.0015 (13)0.0036 (13)
C60.0565 (19)0.0579 (18)0.0448 (16)0.0066 (14)0.0000 (14)0.0009 (13)
C70.0456 (18)0.0536 (17)0.0393 (16)0.0021 (14)0.0078 (14)0.0010 (13)
C80.0460 (19)0.0621 (19)0.0541 (19)0.0053 (15)0.0027 (15)0.0029 (16)
C90.0453 (19)0.0513 (18)0.057 (2)0.0085 (13)0.0070 (16)0.0004 (14)
C100.067 (2)0.0667 (19)0.069 (2)0.0056 (16)0.0030 (16)0.0097 (16)
C110.069 (2)0.093 (2)0.0443 (17)0.0125 (17)0.0060 (15)0.0048 (15)
C120.0533 (19)0.0511 (17)0.0379 (16)0.0033 (14)0.0012 (13)0.0031 (13)
C130.0549 (19)0.0488 (16)0.0425 (16)0.0004 (15)0.0002 (14)0.0006 (13)
C140.0492 (18)0.0452 (16)0.0379 (16)0.0039 (14)0.0012 (13)0.0046 (12)
C150.0528 (19)0.0450 (16)0.0431 (17)0.0029 (14)0.0002 (14)0.0018 (13)
C160.0544 (19)0.0621 (19)0.0344 (15)0.0087 (15)0.0034 (14)0.0002 (14)
C170.0524 (19)0.0565 (17)0.0411 (17)0.0053 (15)0.0038 (15)0.0103 (13)
C180.0546 (19)0.0549 (17)0.0426 (17)0.0097 (14)0.0066 (14)0.0053 (13)
C190.0572 (19)0.0502 (17)0.0334 (16)0.0030 (15)0.0021 (14)0.0033 (13)
C200.087 (2)0.075 (2)0.0500 (18)0.0258 (17)0.0180 (17)0.0008 (15)
C210.075 (2)0.130 (3)0.063 (2)0.048 (2)0.0064 (18)0.0252 (19)
C220.090 (2)0.072 (2)0.0479 (18)0.0294 (18)0.0142 (16)0.0019 (15)
Geometric parameters (Å, º) top
O1—C151.368 (3)C10—H10B0.960
O1—C201.419 (3)C10—H10C0.960
O2—C171.366 (3)C11—H11A0.960
O2—C211.418 (3)C11—H11B0.960
O3—C191.362 (3)C11—H11C0.960
O3—C221.427 (3)C12—C131.355 (3)
N1—C81.150 (3)C12—H12A0.930
N2—C91.147 (3)C13—C141.443 (3)
C1—C21.365 (3)C13—H13A0.930
C1—C121.437 (3)C14—C151.409 (3)
C1—C61.506 (3)C14—C191.416 (3)
C2—C31.423 (3)C15—C161.378 (3)
C2—H2A0.9300C16—C171.382 (3)
C3—C71.371 (3)C16—H16A0.930
C3—C41.494 (3)C17—C181.383 (3)
C4—C51.528 (3)C18—C191.381 (3)
C4—H4A0.9700C18—H18A0.930
C4—H4B0.9700C20—H20A0.960
C5—C111.529 (3)C20—H20B0.960
C5—C61.532 (3)C20—H20C0.960
C5—C101.536 (3)C21—H21A0.960
C6—H6A0.9700C21—H21B0.960
C6—H6B0.9700C21—H21C0.960
C7—C81.424 (4)C22—H22A0.960
C7—C91.430 (4)C22—H22B0.960
C10—H10A0.960C22—H22C0.960
C15—O1—C20118.2 (2)H11A—C11—H11C109.5
C17—O2—C21117.9 (2)H11B—C11—H11C109.5
C19—O3—C22118.8 (2)C13—C12—C1123.8 (2)
C2—C1—C12120.0 (2)C13—C12—H12A118.1
C2—C1—C6119.2 (2)C1—C12—H12A118.1
C12—C1—C6120.8 (2)C12—C13—C14131.4 (2)
C1—C2—C3123.4 (2)C12—C13—H13A114.3
C1—C2—H2A118.3C14—C13—H13A114.3
C3—C2—H2A118.3C15—C14—C19115.9 (2)
C7—C3—C2121.1 (2)C15—C14—C13125.7 (2)
C7—C3—C4120.5 (2)C19—C14—C13118.3 (2)
C2—C3—C4118.3 (2)O1—C15—C16122.1 (2)
C3—C4—C5113.0 (2)O1—C15—C14116.0 (2)
C3—C4—H4A109.0C16—C15—C14121.9 (2)
C5—C4—H4A109.0C15—C16—C17119.5 (2)
C3—C4—H4B109.0C15—C16—H16A120.3
C5—C4—H4B109.0C17—C16—H16A120.3
H4A—C4—H4B107.8O2—C17—C16114.8 (2)
C4—C5—C11109.5 (2)O2—C17—C18123.6 (2)
C4—C5—C6108.5 (2)C16—C17—C18121.7 (2)
C11—C5—C6109.7 (2)C19—C18—C17118.0 (2)
C4—C5—C10110.1 (2)C19—C18—H18A121.0
C11—C5—C10109.1 (2)C17—C18—H18A121.0
C6—C5—C10110.0 (2)O3—C19—C18122.2 (2)
C1—C6—C5115.0 (2)O3—C19—C14114.8 (2)
C1—C6—H6A108.5C18—C19—C14123.0 (2)
C5—C6—H6A108.5O1—C20—H20A109.5
C1—C6—H6B108.5O1—C20—H20B109.5
C5—C6—H6B108.5H20A—C20—H20B109.5
H6A—C6—H6B107.5O1—C20—H20C109.5
C3—C7—C8121.8 (2)H20A—C20—H20C109.5
C3—C7—C9122.3 (2)H20B—C20—H20C109.5
C8—C7—C9115.9 (2)O2—C21—H21A109.5
N1—C8—C7178.8 (3)O2—C21—H21B109.5
N2—C9—C7179.1 (3)H21A—C21—H21B109.5
C5—C10—H10A109.5O2—C21—H21C109.5
C5—C10—H10B109.5H21A—C21—H21C109.5
H10A—C10—H10B109.5H21B—C21—H21C109.5
C5—C10—H10C109.5O3—C22—H22A109.5
H10A—C10—H10C109.5O3—C22—H22B109.5
H10B—C10—H10C109.5H22A—C22—H22B109.5
C5—C11—H11A109.5O3—C22—H22C109.5
C5—C11—H11B109.5H22A—C22—H22C109.5
H11A—C11—H11B109.5H22B—C22—H22C109.5
C5—C11—H11C109.5
C12—C1—C2—C3175.9 (2)C20—O1—C15—C160.4 (4)
C6—C1—C2—C33.0 (4)C20—O1—C15—C14179.6 (2)
C1—C2—C3—C7179.7 (2)C19—C14—C15—O1178.0 (2)
C1—C2—C3—C42.7 (4)C13—C14—C15—O14.5 (4)
C7—C3—C4—C5150.4 (2)C19—C14—C15—C162.8 (4)
C2—C3—C4—C532.0 (3)C13—C14—C15—C16174.7 (2)
C3—C4—C5—C11172.4 (2)O1—C15—C16—C17179.9 (2)
C3—C4—C5—C652.8 (3)C14—C15—C16—C170.7 (4)
C3—C4—C5—C1067.7 (3)C21—O2—C17—C16171.9 (3)
C2—C1—C6—C521.2 (3)C21—O2—C17—C188.8 (4)
C12—C1—C6—C5160.0 (2)C15—C16—C17—O2179.1 (2)
C4—C5—C6—C147.8 (3)C15—C16—C17—C181.5 (4)
C11—C5—C6—C1167.4 (2)O2—C17—C18—C19179.2 (2)
C10—C5—C6—C172.6 (3)C16—C17—C18—C191.5 (4)
C2—C3—C7—C8175.7 (2)C22—O3—C19—C180.5 (4)
C4—C3—C7—C81.8 (4)C22—O3—C19—C14180.0 (2)
C2—C3—C7—C91.3 (4)C17—C18—C19—O3179.8 (2)
C4—C3—C7—C9178.8 (2)C17—C18—C19—C140.7 (4)
C2—C1—C12—C13176.2 (2)C15—C14—C19—O3177.7 (2)
C6—C1—C12—C132.6 (4)C13—C14—C19—O34.6 (3)
C1—C12—C13—C14177.1 (2)C15—C14—C19—C182.8 (4)
C12—C13—C14—C156.6 (4)C13—C14—C19—C18174.9 (2)
C12—C13—C14—C19176.0 (3)

Experimental details

Crystal data
Chemical formulaC22H24N2O3
Mr364.43
Crystal system, space groupMonoclinic, P21/n
Temperature (K)291
a, b, c (Å)10.7130 (3), 9.0471 (3), 20.6565 (7)
β (°) 90.1565 (13)
V3)2002.05 (11)
Z4
Radiation typeMo Kα
µ (mm1)0.08
Crystal size (mm)0.5 × 0.3 × 0.15
Data collection
DiffractometerNonius KappaCCD
diffractometer
Absorption correction
No. of measured, independent and
observed [I > 2σ(I)] reflections
30702, 3595, 1654
Rint0.063
(sin θ/λ)max1)0.604
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.054, 0.136, 0.95
No. of reflections3595
No. of parameters244
H-atom treatmentH-atom parameters constrained
Δρmax, Δρmin (e Å3)0.15, 0.16

Computer programs: COLLECT (Nonius, 1998), DENZO and SCALEPACK (Otwinowski & Minor, 1997), DENZO and SCALEPACK, SHELXS97 (Sheldrick, 1990), SHELXTL-Plus (Sheldrick, 1991), SHELXL97 (Sheldrick, 1997), PARST95 (Nardelli, 1995) and PLATON (Spek, 2001).

 

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