Buy article online - an online subscription or single-article purchase is required to access this article.
Download citation
Download citation
link to html
The crystal structure of the title compound, C20H20N2, contains two independent mol­ecules in the asymmetric unit. These mol­ecules differ significantly only in the torsion angles of the di­methyl­cyclo­hexene moieties, which have twisted conformations. The mol­ecules are nearly planar except for the C(CH3)2 groups.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536802015891/cv6143sup1.cif
Contains datablocks I, ccd1755

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536802015891/cv6143Isup2.hkl
Contains datablock I

CCDC reference: 198954

Key indicators

  • Single-crystal X-ray study
  • T = 291 K
  • Mean [sigma](C-C) = 0.002 Å
  • R factor = 0.043
  • wR factor = 0.082
  • Data-to-parameter ratio = 19.8

checkCIF results

No syntax errors found

ADDSYM reports no extra symmetry


Yellow Alert Alert Level C:
PLAT_371 Alert C Long C(sp2)-C(sp1) Bond C(7) - C(7') = 1.42 Ang. PLAT_371 Alert C Long C(sp2)-C(sp1) Bond C(7') - C(8) = 1.43 Ang. PLAT_371 Alert C Long C(sp2)-C(sp1) Bond C(27) - C(27') = 1.43 Ang. PLAT_371 Alert C Long C(sp2)-C(sp1) Bond C(27') - C(28) = 1.44 Ang.
0 Alert Level A = Potentially serious problem
0 Alert Level B = Potential problem
4 Alert Level C = Please check

Comment top

In the course of our investigations on organic electro-optical, non-linear optical and photorefractive materials we determined the crystal structure of the title compound, (I). As a result of its solvatochromism, it is expected to be a good candidate for photorefractive and electro-optical applications.

The conversion of basic 2-(3,5,5-trimethyl-cyclohex-2-enylidene)-malononitrile into the corresponding 2-[5,5-dimethyl-3-(2-p-tolyl-vinyl)-cyclohex-2-enylidene]-malononitrile is a way to enhance the charge-transfer transition on the molecular level – a requisite for the design of efficient second- and third-order non-linear optical materials.

The crystal contains no classical H-bonds, but C11—H11···N21 [H···A = 2.62, D···A = 3.391 (2) Å, D—H···A = 141°] is a possible non-classical H-bond.

The dihedral angle between the least-squares planes through atoms C1, C2, C3, C11, C12 and through C13, C14, C15, C16, C17, C18 is 8.24 (9)°, whereas the corresponding angle in the other molecule in the asymmetric unit is only 3.74 (9)°

Experimental top

The title compound was synthesized for the first time, according to a general procedure described by Lemke (1970): 3.72 g (20 mmol) 2-(3,5,5-trimethyl-cyclohex-2-enylidene)-malononitrile and 3.71 ml (20 mmol) 4-methyl-benzaldehyde were dissolved in 80 ml dry toluene by continuous stirring and heating under reflux for 60 min. Piperidine (1 ml) was used as a catalyst. After a few minutes, the solution became dark red. The bright-yellow precipitate was obtained after evaporation of the solvent. The product was filtered and washed with ethanol and recrystallized from ethyl acetate. Yield of the recrystallized product: 33%; melting point: 428–429 K. UV-vis(EtOH): λmax (log ε) = 270.5 nm (3.702), 398.5 nm (4.329).

The purity of the compound was confirmed by elemental analysis, IR, UV–vis and mass spectrometry. Crystals were grown from ethyl acetate by slow evaporation at room temperature over a period of a week.

Refinement top

Hydrogen atoms were placed in calculated positions with Uiso constrained to be 1.5 times Ueq of the carrier atom for the methyl-H and 1.2 times Ueq for the remaining H atoms. The methyl groups were allowed to rotate but not to tip.

Computing details top

Data collection: COLLECT (Nonius, 1998); cell refinement: DENZO and SCALEPACK (Otwinowski & Minor, 1997); data reduction: DENZO and SCALEPACK (Otwinowski & Minor, 1997); 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, PARST95 (Nardelli, 1995), PLATON (Spek, 2001).

Figures top
[Figure 1] Fig. 1. : View of the title compound, showing the labelling of all non-H atoms. Displacement ellipsoids are shown at 50% probability levels. H atoms are omitted for clarity.
(I) top
Crystal data top
C20H20N2F(000) = 1232
Mr = 288.38Dx = 1.095 Mg m3
Monoclinic, P21/nMo Kα radiation, λ = 0.71073 Å
a = 13.5270 (3) ÅCell parameters from 62924 reflections
b = 16.1781 (3) Åθ = 3.0–27.5°
c = 16.3616 (4) ŵ = 0.06 mm1
β = 102.3807 (9)°T = 291 K
V = 3497.32 (13) Å3Block, orange
Z = 80.50 × 0.40 × 0.32 mm
Data collection top
Nonius KappaCCD
diffractometer
2602 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tubeRint = 0.021
Graphite monochromatorθmax = 27.5°, θmin = 3.0°
Detector resolution: 19 vertical, 18 horizontal pixels mm-1h = 1717
332 frames via ω–rotation (Δω=1%) and two times 50 s per frame (7 sets at different κ–angles) scansk = 2020
62924 measured reflectionsl = 2120
7998 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)] = 0.043Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.082H atoms treated by a mixture of independent and constrained refinement
S = 0.96 w = 1/[σ2(Fo2) + (0.020P)2]
where P = (Fo2 + 2Fc2)/3
7998 reflections(Δ/σ)max = 0.004
403 parametersΔρmax = 0.11 e Å3
0 restraintsΔρmin = 0.16 e Å3
Crystal data top
C20H20N2V = 3497.32 (13) Å3
Mr = 288.38Z = 8
Monoclinic, P21/nMo Kα radiation
a = 13.5270 (3) ŵ = 0.06 mm1
b = 16.1781 (3) ÅT = 291 K
c = 16.3616 (4) Å0.50 × 0.40 × 0.32 mm
β = 102.3807 (9)°
Data collection top
Nonius KappaCCD
diffractometer
2602 reflections with I > 2σ(I)
62924 measured reflectionsRint = 0.021
7998 independent reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0430 restraints
wR(F2) = 0.082H atoms treated by a mixture of independent and constrained refinement
S = 0.96Δρmax = 0.11 e Å3
7998 reflectionsΔρmin = 0.16 e Å3
403 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
N111.37461 (12)1.07691 (10)0.20345 (10)0.1155 (6)
N121.04516 (14)1.04989 (11)0.12227 (13)0.1379 (7)
C11.19046 (11)1.22876 (11)0.17206 (9)0.0604 (4)
C21.09392 (11)1.26751 (10)0.15643 (9)0.0680 (5)
H21.03671.23420.14370.082*
C31.08103 (11)1.34968 (11)0.15904 (9)0.0623 (4)
C41.17014 (11)1.40573 (9)0.17793 (9)0.0728 (5)
H4A1.18291.42050.23670.087*
H4B1.15391.45610.14570.087*
C51.26668 (11)1.36884 (10)0.15884 (10)0.0642 (4)
C61.28160 (10)1.28266 (9)0.19747 (9)0.0667 (4)
H6A1.33871.25640.18080.080*
H6B1.29781.28780.25790.080*
C7'1.19918 (13)1.14513 (12)0.16686 (10)0.0703 (5)
C71.29627 (16)1.10696 (10)0.18646 (11)0.0831 (6)
C81.11342 (17)1.09183 (13)0.14237 (13)0.0931 (6)
C91.25917 (11)1.36340 (10)0.06422 (10)0.0894 (5)
H9A1.20231.32960.03940.134*
H9B1.32001.33930.05360.134*
H9C1.25051.41780.04040.134*
C101.35787 (11)1.42245 (10)0.19752 (10)0.1041 (6)
H10A1.41791.39950.18420.156*
H10B1.36521.42400.25720.156*
H10C1.34781.47750.17550.156*
C110.97749 (12)1.38139 (10)0.14388 (9)0.0728 (5)
H110.92581.34310.12720.087*
C120.94999 (12)1.45826 (11)0.15134 (9)0.0735 (5)
H121.00181.49680.16640.088*
C130.84572 (11)1.49007 (11)0.13833 (9)0.0618 (4)
C140.76117 (13)1.44029 (10)0.10865 (9)0.0742 (5)
H140.76981.38520.09550.089*
C150.66467 (12)1.47273 (12)0.09870 (9)0.0777 (5)
H150.60911.43870.07940.093*
C160.64903 (12)1.55413 (13)0.11672 (10)0.0707 (5)
C170.73269 (14)1.60248 (10)0.14484 (9)0.0733 (5)
H170.72401.65790.15680.088*
C180.82856 (12)1.57138 (11)0.15581 (9)0.0693 (5)
H180.88341.60590.17550.083*
C190.54425 (11)1.59006 (11)0.10691 (11)0.1130 (7)
H19A0.53631.61250.15950.170*
H19B0.49481.54750.08940.170*
H19C0.53491.63310.06560.170*
N210.85430 (12)1.20647 (10)0.17807 (12)0.1281 (7)
N220.53030 (14)1.23723 (10)0.09187 (12)0.1345 (7)
C210.66978 (11)1.05270 (11)0.13122 (9)0.0607 (4)
C220.57310 (11)1.01495 (10)0.11321 (9)0.0648 (4)
H220.51671.04860.09580.078*
C230.55808 (11)0.93317 (10)0.11985 (9)0.0593 (4)
C240.64602 (10)0.87616 (9)0.14470 (9)0.0664 (4)
H24A0.63010.82420.11510.080*
H24B0.65580.86480.20410.080*
C250.74496 (11)0.90951 (9)0.12691 (10)0.0612 (4)
C260.76026 (10)0.99808 (9)0.15887 (9)0.0660 (4)
H26A0.77760.99710.21950.079*
H26B0.81711.02190.13970.079*
C27'0.68112 (13)1.13673 (12)0.12954 (10)0.0708 (5)
C270.77752 (16)1.17541 (11)0.15513 (12)0.0871 (6)
C280.59609 (16)1.19229 (12)0.10832 (12)0.0893 (6)
C290.83399 (10)0.85649 (9)0.17207 (10)0.0927 (6)
H29A0.82550.80080.15140.139*
H29B0.83610.85670.23110.139*
H29C0.89610.87870.16200.139*
C300.74160 (11)0.90711 (9)0.03272 (10)0.0907 (5)
H30A0.73300.85110.01320.136*
H30B0.80370.92880.02220.136*
H30C0.68590.94000.00380.136*
C310.45442 (11)0.90331 (10)0.10517 (9)0.0688 (5)
H310.40380.94280.09040.083*
C320.42446 (12)0.82642 (10)0.11044 (9)0.0736 (5)
H320.47520.78700.12500.088*
C330.32006 (12)0.79614 (12)0.09597 (9)0.0666 (5)
C340.23642 (13)0.84819 (11)0.07418 (9)0.0804 (5)
H340.24590.90440.06670.097*
C350.13982 (13)0.81694 (14)0.06364 (10)0.0876 (6)
H350.08510.85270.04870.105*
C360.12179 (14)0.73462 (15)0.07453 (10)0.0792 (6)
C370.20395 (16)0.68380 (11)0.09348 (11)0.0892 (6)
H370.19400.62740.09920.107*
C380.30084 (13)0.71359 (12)0.10440 (10)0.0825 (5)
H380.35490.67700.11780.099*
C390.01594 (11)0.70198 (12)0.06891 (10)0.1205 (7)
H39A0.00170.69990.12390.181*
H39B0.01070.64740.04530.181*
H39C0.03180.73780.03400.181*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
N110.1170 (13)0.1041 (13)0.1325 (15)0.0537 (11)0.0425 (12)0.0315 (11)
N120.1369 (17)0.0865 (15)0.182 (2)0.0126 (12)0.0168 (14)0.0068 (13)
C10.0638 (11)0.0640 (13)0.0563 (11)0.0118 (10)0.0191 (9)0.0075 (9)
C20.0613 (11)0.0594 (13)0.0867 (13)0.0066 (9)0.0234 (9)0.0078 (10)
C30.0559 (11)0.0627 (12)0.0723 (12)0.0089 (10)0.0230 (9)0.0075 (10)
C40.0705 (11)0.0646 (12)0.0852 (12)0.0082 (10)0.0208 (10)0.0023 (9)
C50.0559 (11)0.0664 (12)0.0712 (13)0.0013 (9)0.0156 (9)0.0070 (10)
C60.0624 (11)0.0746 (13)0.0634 (11)0.0120 (10)0.0144 (9)0.0047 (10)
C7'0.0800 (13)0.0602 (13)0.0744 (12)0.0200 (12)0.0248 (10)0.0065 (10)
C70.1055 (15)0.0654 (14)0.0840 (14)0.0240 (12)0.0328 (13)0.0132 (10)
C80.1029 (17)0.0639 (16)0.1135 (17)0.0066 (12)0.0253 (14)0.0101 (13)
C90.0793 (12)0.1126 (15)0.0819 (14)0.0044 (10)0.0302 (10)0.0250 (11)
C100.0774 (12)0.0970 (15)0.1324 (17)0.0158 (11)0.0106 (11)0.0005 (12)
C110.0743 (13)0.0586 (13)0.0887 (13)0.0076 (10)0.0245 (10)0.0088 (10)
C120.0726 (12)0.0708 (14)0.0802 (13)0.0003 (11)0.0230 (9)0.0051 (11)
C130.0462 (11)0.0758 (14)0.0639 (12)0.0095 (10)0.0128 (9)0.0092 (10)
C140.0737 (12)0.0701 (12)0.0752 (12)0.0131 (11)0.0082 (10)0.0059 (10)
C150.0598 (12)0.0867 (15)0.0822 (13)0.0033 (11)0.0054 (10)0.0014 (11)
C160.0606 (12)0.0791 (14)0.0723 (12)0.0123 (11)0.0142 (10)0.0107 (11)
C170.0770 (12)0.0649 (13)0.0836 (13)0.0176 (11)0.0298 (10)0.0131 (10)
C180.0730 (13)0.0615 (13)0.0785 (12)0.0023 (10)0.0274 (10)0.0060 (10)
C190.0696 (12)0.1343 (18)0.1311 (17)0.0363 (12)0.0124 (11)0.0072 (13)
N210.1130 (14)0.0941 (14)0.1878 (19)0.0431 (11)0.0557 (13)0.0135 (12)
N220.1422 (17)0.0913 (14)0.1758 (18)0.0354 (11)0.0467 (14)0.0109 (12)
C210.0639 (11)0.0596 (13)0.0624 (11)0.0020 (10)0.0224 (9)0.0031 (9)
C220.0559 (11)0.0632 (12)0.0764 (12)0.0004 (10)0.0167 (9)0.0017 (10)
C230.0531 (10)0.0604 (12)0.0667 (11)0.0024 (10)0.0180 (8)0.0030 (9)
C240.0619 (11)0.0590 (11)0.0796 (12)0.0029 (9)0.0178 (9)0.0000 (9)
C250.0572 (11)0.0578 (12)0.0702 (12)0.0030 (9)0.0174 (9)0.0058 (9)
C260.0590 (11)0.0672 (12)0.0741 (11)0.0073 (9)0.0194 (9)0.0073 (10)
C27'0.0764 (13)0.0584 (13)0.0839 (13)0.0067 (11)0.0314 (10)0.0011 (11)
C270.0995 (15)0.0586 (13)0.1149 (17)0.0135 (12)0.0490 (14)0.0021 (11)
C280.1078 (17)0.0629 (15)0.1046 (16)0.0004 (12)0.0395 (14)0.0024 (12)
C290.0715 (11)0.0831 (13)0.1232 (16)0.0144 (10)0.0205 (10)0.0006 (11)
C300.0983 (13)0.0908 (14)0.0921 (15)0.0007 (10)0.0408 (11)0.0169 (11)
C310.0647 (12)0.0634 (12)0.0801 (12)0.0008 (9)0.0197 (9)0.0003 (10)
C320.0709 (12)0.0699 (13)0.0832 (13)0.0007 (10)0.0235 (10)0.0023 (10)
C330.0506 (11)0.0791 (14)0.0732 (12)0.0094 (11)0.0202 (9)0.0061 (10)
C340.0669 (12)0.0886 (14)0.0857 (13)0.0114 (12)0.0163 (10)0.0147 (10)
C350.0628 (13)0.1206 (19)0.0773 (13)0.0042 (12)0.0107 (10)0.0159 (12)
C360.0642 (13)0.1130 (18)0.0617 (12)0.0252 (14)0.0165 (10)0.0129 (12)
C370.0890 (14)0.0825 (15)0.1050 (16)0.0297 (14)0.0408 (12)0.0234 (12)
C380.0717 (13)0.0720 (15)0.1112 (15)0.0085 (10)0.0363 (11)0.0139 (11)
C390.0783 (13)0.181 (2)0.1025 (15)0.0537 (13)0.0208 (11)0.0208 (13)
Geometric parameters (Å, º) top
N11—C71.1446 (18)N21—C271.1424 (19)
N12—C81.136 (2)N22—C281.136 (2)
C1—C7'1.3623 (18)C21—C27'1.3690 (18)
C1—C21.4215 (18)C21—C221.4160 (18)
C1—C61.4945 (17)C21—C261.4987 (17)
C2—C31.3426 (17)C22—C231.3465 (17)
C2—H20.9300C22—H220.9300
C3—C111.4619 (18)C23—C311.4535 (18)
C3—C41.4870 (17)C23—C241.4911 (17)
C4—C51.5277 (17)C24—C251.5279 (17)
C4—H4A0.9700C24—H24A0.9700
C4—H4B0.9700C24—H24B0.9700
C5—C61.5262 (17)C25—C261.5242 (17)
C5—C101.5297 (17)C25—C301.5324 (18)
C5—C91.5320 (18)C25—C291.5332 (17)
C6—H6A0.9700C26—H26A0.9700
C6—H6B0.9700C26—H26B0.9700
C7'—C71.424 (2)C27'—C271.426 (2)
C7'—C81.432 (2)C27'—C281.442 (2)
C9—H9A0.9600C29—H29A0.9600
C9—H9B0.9600C29—H29B0.9600
C9—H9C0.9600C29—H29C0.9600
C10—H10A0.9600C30—H30A0.9600
C10—H10B0.9600C30—H30B0.9600
C10—H10C0.9600C30—H30C0.9600
C11—C121.3114 (17)C31—C321.3168 (17)
C11—H110.9300C31—H310.9300
C12—C131.4734 (19)C32—C331.4653 (19)
C12—H120.9300C32—H320.9300
C13—C181.3764 (18)C33—C381.3731 (19)
C13—C141.3979 (18)C33—C341.3940 (19)
C14—C151.3838 (18)C34—C351.3770 (19)
C14—H140.9300C34—H340.9300
C15—C161.3757 (19)C35—C361.372 (2)
C15—H150.9300C35—H350.9300
C16—C171.3716 (18)C36—C371.364 (2)
C16—C191.5083 (19)C36—C391.5104 (19)
C17—C181.3665 (18)C37—C381.3717 (19)
C17—H170.9300C37—H370.9300
C18—H180.9300C38—H380.9300
C19—H19A0.9600C39—H39A0.9600
C19—H19B0.9600C39—H39B0.9600
C19—H19C0.9600C39—H39C0.9600
C7'—C1—C2121.01 (16)C27'—C21—C22121.78 (15)
C7'—C1—C6121.31 (15)C27'—C21—C26120.25 (15)
C2—C1—C6117.64 (15)C22—C21—C26117.81 (15)
C3—C2—C1123.47 (15)C23—C22—C21123.76 (15)
C3—C2—H2118.3C23—C22—H22118.1
C1—C2—H2118.3C21—C22—H22118.1
C2—C3—C11117.92 (15)C22—C23—C31118.04 (15)
C2—C3—C4120.36 (14)C22—C23—C24120.29 (14)
C11—C3—C4121.71 (15)C31—C23—C24121.63 (14)
C3—C4—C5114.18 (13)C23—C24—C25114.19 (13)
C3—C4—H4A108.7C23—C24—H24A108.7
C5—C4—H4A108.7C25—C24—H24A108.7
C3—C4—H4B108.7C23—C24—H24B108.7
C5—C4—H4B108.7C25—C24—H24B108.7
H4A—C4—H4B107.6H24A—C24—H24B107.6
C6—C5—C4108.37 (12)C26—C25—C24109.07 (12)
C6—C5—C10108.86 (13)C26—C25—C30109.97 (12)
C4—C5—C10110.05 (14)C24—C25—C30110.14 (12)
C6—C5—C9109.90 (13)C26—C25—C29109.01 (12)
C4—C5—C9110.77 (12)C24—C25—C29109.89 (13)
C10—C5—C9108.88 (13)C30—C25—C29108.75 (13)
C1—C6—C5112.94 (12)C21—C26—C25114.13 (12)
C1—C6—H6A109.0C21—C26—H26A108.7
C5—C6—H6A109.0C25—C26—H26A108.7
C1—C6—H6B109.0C21—C26—H26B108.7
C5—C6—H6B109.0C25—C26—H26B108.7
H6A—C6—H6B107.8H26A—C26—H26B107.6
C1—C7'—C7120.30 (17)C21—C27'—C27121.95 (17)
C1—C7'—C8122.67 (17)C21—C27'—C28122.46 (16)
C7—C7'—C8117.03 (17)C27—C27'—C28115.41 (16)
N11—C7—C7'178.9 (2)N21—C27—C27'177.9 (2)
N12—C8—C7'179.4 (3)N22—C28—C27'178.8 (2)
C5—C9—H9A109.5C25—C29—H29A109.5
C5—C9—H9B109.5C25—C29—H29B109.5
H9A—C9—H9B109.5H29A—C29—H29B109.5
C5—C9—H9C109.5C25—C29—H29C109.5
H9A—C9—H9C109.5H29A—C29—H29C109.5
H9B—C9—H9C109.5H29B—C29—H29C109.5
C5—C10—H10A109.5C25—C30—H30A109.5
C5—C10—H10B109.5C25—C30—H30B109.5
H10A—C10—H10B109.5H30A—C30—H30B109.5
C5—C10—H10C109.5C25—C30—H30C109.5
H10A—C10—H10C109.5H30A—C30—H30C109.5
H10B—C10—H10C109.5H30B—C30—H30C109.5
C12—C11—C3126.70 (16)C32—C31—C23127.06 (16)
C12—C11—H11116.7C32—C31—H31116.5
C3—C11—H11116.7C23—C31—H31116.5
C11—C12—C13126.84 (16)C31—C32—C33127.21 (16)
C11—C12—H12116.6C31—C32—H32116.4
C13—C12—H12116.6C33—C32—H32116.4
C18—C13—C14117.45 (14)C38—C33—C34116.90 (15)
C18—C13—C12120.17 (16)C38—C33—C32120.37 (17)
C14—C13—C12122.39 (17)C34—C33—C32122.73 (17)
C15—C14—C13120.22 (16)C35—C34—C33120.44 (17)
C15—C14—H14119.9C35—C34—H34119.8
C13—C14—H14119.9C33—C34—H34119.8
C16—C15—C14121.49 (16)C36—C35—C34122.02 (18)
C16—C15—H15119.3C36—C35—H35119.0
C14—C15—H15119.3C34—C35—H35119.0
C17—C16—C15117.65 (16)C37—C36—C35117.12 (17)
C17—C16—C19120.32 (18)C37—C36—C39121.3 (2)
C15—C16—C19122.03 (17)C35—C36—C39121.6 (2)
C18—C17—C16121.71 (16)C36—C37—C38121.81 (18)
C18—C17—H17119.1C36—C37—H37119.1
C16—C17—H17119.1C38—C37—H37119.1
C17—C18—C13121.48 (15)C37—C38—C33121.66 (16)
C17—C18—H18119.3C37—C38—H38119.2
C13—C18—H18119.3C33—C38—H38119.2
C16—C19—H19A109.5C36—C39—H39A109.5
C16—C19—H19B109.5C36—C39—H39B109.5
H19A—C19—H19B109.5H39A—C39—H39B109.5
C16—C19—H19C109.5C36—C39—H39C109.5
H19A—C19—H19C109.5H39A—C39—H39C109.5
H19B—C19—H19C109.5H39B—C39—H39C109.5
C7'—C1—C2—C3178.61 (15)C27'—C21—C22—C23175.12 (15)
C6—C1—C2—C33.6 (2)C26—C21—C22—C230.3 (2)
C1—C2—C3—C11178.41 (14)C21—C22—C23—C31175.69 (13)
C1—C2—C3—C40.8 (2)C21—C22—C23—C242.1 (2)
C2—C3—C4—C523.3 (2)C22—C23—C24—C2523.4 (2)
C11—C3—C4—C5157.48 (13)C31—C23—C24—C25158.86 (13)
C3—C4—C5—C648.76 (17)C23—C24—C25—C2647.71 (17)
C3—C4—C5—C10167.69 (13)C23—C24—C25—C3073.06 (16)
C3—C4—C5—C971.87 (17)C23—C24—C25—C29167.16 (12)
C7'—C1—C6—C5150.42 (14)C27'—C21—C26—C25157.49 (14)
C2—C1—C6—C531.84 (18)C22—C21—C26—C2527.04 (19)
C4—C5—C6—C152.81 (17)C24—C25—C26—C2149.54 (17)
C10—C5—C6—C1172.48 (13)C30—C25—C26—C2171.34 (15)
C9—C5—C6—C168.36 (15)C29—C25—C26—C21169.52 (12)
C2—C1—C7'—C7177.09 (14)C22—C21—C27'—C27174.05 (15)
C6—C1—C7'—C70.6 (2)C26—C21—C27'—C271.2 (2)
C2—C1—C7'—C82.6 (2)C22—C21—C27'—C280.9 (2)
C6—C1—C7'—C8179.72 (15)C26—C21—C27'—C28176.17 (15)
C2—C3—C11—C12173.25 (16)C22—C23—C31—C32178.41 (15)
C4—C3—C11—C126.0 (2)C24—C23—C31—C320.7 (2)
C3—C11—C12—C13178.22 (14)C23—C31—C32—C33179.77 (14)
C11—C12—C13—C18174.14 (16)C31—C32—C33—C38179.65 (16)
C11—C12—C13—C145.6 (2)C31—C32—C33—C340.3 (3)
C18—C13—C14—C150.7 (2)C38—C33—C34—C351.3 (2)
C12—C13—C14—C15178.98 (14)C32—C33—C34—C35178.10 (15)
C13—C14—C15—C160.6 (2)C33—C34—C35—C360.5 (3)
C14—C15—C16—C170.2 (2)C34—C35—C36—C372.3 (3)
C14—C15—C16—C19179.42 (14)C34—C35—C36—C39175.55 (15)
C15—C16—C17—C180.8 (2)C35—C36—C37—C382.4 (3)
C19—C16—C17—C18178.80 (14)C39—C36—C37—C38175.46 (15)
C16—C17—C18—C130.7 (2)C36—C37—C38—C330.7 (3)
C14—C13—C18—C170.1 (2)C34—C33—C38—C371.2 (2)
C12—C13—C18—C17179.60 (14)C32—C33—C38—C37178.20 (15)

Experimental details

Crystal data
Chemical formulaC20H20N2
Mr288.38
Crystal system, space groupMonoclinic, P21/n
Temperature (K)291
a, b, c (Å)13.5270 (3), 16.1781 (3), 16.3616 (4)
β (°) 102.3807 (9)
V3)3497.32 (13)
Z8
Radiation typeMo Kα
µ (mm1)0.06
Crystal size (mm)0.50 × 0.40 × 0.32
Data collection
DiffractometerNonius KappaCCD
diffractometer
Absorption correction
No. of measured, independent and
observed [I > 2σ(I)] reflections
62924, 7998, 2602
Rint0.021
(sin θ/λ)max1)0.649
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.043, 0.082, 0.96
No. of reflections7998
No. of parameters403
H-atom treatmentH atoms treated by a mixture of independent and constrained refinement
Δρmax, Δρmin (e Å3)0.11, 0.16

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

 

Subscribe to Acta Crystallographica Section E: Crystallographic Communications

The full text of this article is available to subscribers to the journal.

If you have already registered and are using a computer listed in your registration details, please email support@iucr.org for assistance.

Buy online

You may purchase this article in PDF and/or HTML formats. For purchasers in the European Community who do not have a VAT number, VAT will be added at the local rate. Payments to the IUCr are handled by WorldPay, who will accept payment by credit card in several currencies. To purchase the article, please complete the form below (fields marked * are required), and then click on `Continue'.
E-mail address* 
Repeat e-mail address* 
(for error checking) 

Format*   PDF (US $40)
   HTML (US $40)
   PDF+HTML (US $50)
In order for VAT to be shown for your country javascript needs to be enabled.

VAT number 
(non-UK EC countries only) 
Country* 
 

Terms and conditions of use
Contact us

Follow Acta Cryst. E
Sign up for e-alerts
Follow Acta Cryst. on Twitter
Follow us on facebook
Sign up for RSS feeds