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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2011 Apr 29;67(Pt 5):o1210. doi: 10.1107/S1600536811014590

4-tert-Butyl-2-[2-(1,3,3-trimethyl­indolin-2-yl­idene)ethyl­idene]cyclo­hexa­none

Graeme J Gainsford a,*, Mohamed Ashraf a, Andrew J Kay a
PMCID: PMC3089154  PMID: 21754509

Abstract

The title mol­ecule, C23H31NO, has two alternative cyclo­hexa­none configurations at the 4-position in a ratio of 0.663 (3):0.337 (3). The plane of the five-membered planar ring in the indolin-2-yl­idene subtends an angle of 2.19 (7)° with its fused aromatic ring, an angle of 16.24 (8)° with the plane of the major cyclo­hexa­none configuration and an angle of 8.54 (15)° with the bridging planar ethyl­idene C atoms. These last atoms subtend an angle of 8.37 (16)° with the mean plane through the major cyclo­hexa­none configuration. The mol­ecules pack approximately parallel to the (Inline graphic01) plane via C—H⋯π and C—H⋯O inter­actions.

Related literature

For background information on potential applications of NLO (organic nonlinear optical material) compounds, see: Denk et al. (1990 ▶); Ma et al. (2002 ▶); Parthenopoulos & Rentzepis (1989 ▶). For synthesis details, see: Ainsworth (1963 ▶). For related compounds, see: Kawamata et al. (1998 ▶); Higham et al. (2010 ▶); Bhuiyan et al. (2011 ▶); Teshome et al. (2011 ▶). For the Cambridge Structural Database, see: Allen (2002 ▶). For graph-set notation of hydrogen bonds, see: Bernstein et al. (1995 ▶).graphic file with name e-67-o1210-scheme1.jpg

Experimental

Crystal data

  • C23H31NO

  • M r = 337.49

  • Monoclinic, Inline graphic

  • a = 9.7327 (4) Å

  • b = 17.2187 (6) Å

  • c = 12.1303 (4) Å

  • β = 100.045 (2)°

  • V = 2001.69 (13) Å3

  • Z = 4

  • Mo Kα radiation

  • μ = 0.07 mm−1

  • T = 116 K

  • 0.62 × 0.49 × 0.25 mm

Data collection

  • Bruker APEXII CCD diffractometer

  • Absorption correction: multi-scan (Blessing, 1995 ▶) T min = 0.668, T max = 0.746

  • 44399 measured reflections

  • 4500 independent reflections

  • 3690 reflections with I > 2σ(I)

  • R int = 0.043

Refinement

  • R[F 2 > 2σ(F 2)] = 0.050

  • wR(F 2) = 0.134

  • S = 1.05

  • 4500 reflections

  • 308 parameters

  • 5 restraints

  • H atoms treated by a mixture of independent and constrained refinement

  • Δρmax = 0.26 e Å−3

  • Δρmin = −0.21 e Å−3

Data collection: APEX2 (Bruker, 2005 ▶); cell refinement: SAINT (Bruker, 2005 ▶); data reduction: SAINT and SADABS (Sheldrick, 1995 ▶); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); 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: SHELXL97 and PLATON (Spek, 2009 ▶).

Supplementary Material

Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536811014590/jj2085sup1.cif

e-67-o1210-sup1.cif (35.7KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536811014590/jj2085Isup2.hkl

e-67-o1210-Isup2.hkl (220.5KB, hkl)

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

Table 1. Hydrogen-bond geometry (Å, °).

Cg1 is the centroid of the C1–C6 ring.

D—H⋯A D—H H⋯A D⋯A D—H⋯A
C5—H5⋯O1i 0.95 2.45 3.3293 (19) 154
C9—H9A⋯Cg1ii 0.98 2.65 3.5705 (17) 156

Symmetry codes: (i) Inline graphic; (ii) Inline graphic.

Acknowledgments

The authors thank Dr J. Wikaira of the University of Canterbury for her assistance in the data collection.

supplementary crystallographic information

Comment

Organic nonlinear optical (NLO) materials show much promise due to their potential application in areas such as optical power limiting, optical data storage and two-photon fluorescence imaging (Ma et al., 2002; Parthenopoulos & Rentzepis, 1989; Denk et al., 1990). Such compounds are typically push–pull conjugated systems that can be modified by altering either the donor, acceptor or conjugated interconnect moieties. However these modifications can involve trade-offs insofar as improvements to the nonlinear optical properties typically result in compounds that are more complex to prepare, have lower stabilities and higher optical losses. Conjugated ketones are useful intermediates for increasing the chain length and/or substituting different donors and acceptors onto a basic chromophore backbone. This is because conjugated ketones are quite reactive species and are able to undergo a range of carbon–carbon double bond forming reactions including the Wittig reaction, Knoevenagel condensation and Peterson olefination. With this in mind, and in line with our ongoing work on the development of novel organic NLO compounds, we sought to prepare the title compound 3 using the method outlined in Fig. 1. This compound is a useful synthon for the preparation of a range of chromophore systems as it contains an electron-rich indoline donor unit and a conjugated ketone onto which a range of acceptors can be coupled. The title molecule 3 is conveniently prepared in excellent yield by the condensation of 4-tert-butyl-2-hydroxymethylenecyclohexanone 1 with Fisher's base 2. Compound 1 was prepared from 4-tert-butylcyclohexanone using the general procedure reported by Ainsworth (1963).

Compound REFCODES below are from the CSD (Version 5.32, with Feb. 2011 updates; Allen, 2002). In the title compound 3 (Fig. 2), the cyclohexanone ring exists in two configurations, S (C18a) and R (C18b), in the ratio a:b of 0.663 (3):0.337 (3). This model made chemical sense, was stable in refinement, with insignificant difference Fourier residual density. The data supported refinement in the centrosymmetric space group P21/n even though there were 57 weak reflections (with intensities between values between 0.08 (2) and 0.87 (7)) that violated the n glide absence condition. Refinement in P21 did not improve the fit significantly as would be expected with such weak contributing data, and gave some very large correlations between thermal and positional parameters of the n glide related molecules.

The closest comparable structures for the cyclochexanone section of the molecule is QADZUQ, 4-tert-butyl-2,6-bis(4-methylbenzylidene)cyclohexanone (Kawamata et al., 1998) which has a mirror plane passing through the carbonyl, tert-butyl and their bound ring C atoms. A comparision of the cyclohexanone dimensions indicates that some electronic delocalization along the ethylidene chain is observed with the C14—C15 bond length shortened (1.472 (2), 1.490 Å), the C13—C14 bond length lengthened (1.3619 (18), 1.332 Å) and the C12—C13 bond shortened (1.4204 (19), 1.466 Å) for 3 and QADZUQ respectively. The dienone-ether macrocyclic compound WUYMIN (Higham et al., 2010) also contains copies of the 4-tert-butyl-cyclohexanone at a lower resolution (R 9.0%), with similar configurational disorder in the ratio of 0.70:0.30 as observed here.

As noted before in related indoline-based compounds there is minor buckling between the planar 5- and 6-membered rings in the indolin-2-ylidene ring of 2.19 (7)° compared with 1.81 (13)° in compound 17 (Teshome et al., 2011) and 1.38 (9)° in compound TMIPI (Bhuiyan et al., 2011). The interplanar angles confirm the consistent twist along the electronic delocalization plane: 8.54 (15)° between the 5-membered indoline ring (N1,C1,C6–C8) and the ethylidene atoms plane (C8,C12–C14) with a further 8.37 (16)° angle subtended between the latter and the average plane through the major configuration cyclohexanone atoms (C14–C16, C17a, C18a and C19). The indoline dimensions are identical to those found in the above-listed compounds.

The molecules are held in the lattice by weak C—H···π interactions (Table 1) over cell inversion centres and C—H···O hydrogen bonds, the latter forming C(10) motifs (Bernstein et al., 1995), Fig. 3.

Experimental

To a stirred solution of Fisher's base 2 (0.865 g, 5 mmole) in methanol was added compound 1 (0.91 g, 5 mmole). The mixture was refluxed for 2 h by which time its colour had changed from deep red to brown. The solvent was removed at reduced pressure and the residue purified by crystallization in ethanol, giving the title compound 3 as a yellow solid (1.5 g, 88% yield). X-ray quality crystals were grown by slow evaporation from methanol. m.p.: 450 K.

Refinement

A total of 15 outlier reflections (ΔF2/σ(F2)>4.5) were removed from the refinment using OMIT. There were 57 systematic absence violations involving weak reflections as discussed in the Comment section. The cyclohexanone ring was disordered across two configuraions (see Fig. 1); each was refined with common occupancy factors giving a final ratio a:b of 0.663 (3):0.337 (3). The bond lengths between C16 and C19 to their respective disorder atoms (C17 and C18, a and b) were restrained to be the same using SADI. The bond distances between C20b and each of the bound methyl C atoms were similarly restrained.

The methyl H atoms were constrained to an ideal geometry (C—H = 0.98 Å) with Uiso(H) = 1.5Ueq(C), but were allowed to rotate freely about the adjacent C—C bond. All other H atoms were placed in geometrically idealized positions and constrained to ride on their parent atoms with C—H distances of 1.00 (primary), 0.99 (methylene) or 0.95 (phenyl) Å with Uiso(H) = 1.2Ueq(C).

Figures

Fig. 1.

Fig. 1.

Reaction scheme showing the synthetic procedure for obtaining the title compound.

Fig. 2.

Fig. 2.

Molecular structure of the asymmetric unit (Farrugia, 1997); displacement ellipsoids are shown at the 30% probability level. H atoms not shown for clarity. Dashed bonds indicate positions of the minor (b) configuration atoms (see text).

Fig. 3.

Fig. 3.

Partial packing diagram of the unit cell showing key interactions (see text and Table 1) [Macrae et al., 2008]. Only significant H atoms are shown as balls for clarity. Symmetry (i) x - 1/2, 3/2 - y, z - 1/2 (ii) 2 - x, 1 - y, 2 - z Two ring centres are shown as purple balls: Cg1 is the centre of the C1–C6 ring at symmetry (ii).

Crystal data

C23H31NO F(000) = 736
Mr = 337.49 Dx = 1.120 Mg m−3
Monoclinic, P21/n Mo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2yn Cell parameters from 9800 reflections
a = 9.7327 (4) Å θ = 2.4–27.3°
b = 17.2187 (6) Å µ = 0.07 mm−1
c = 12.1303 (4) Å T = 116 K
β = 100.045 (2)° Block, orange
V = 2001.69 (13) Å3 0.62 × 0.49 × 0.25 mm
Z = 4

Data collection

Bruker APEXII CCD diffractometer 4500 independent reflections
Radiation source: fine-focus sealed tube 3690 reflections with I > 2σ(I)
graphite Rint = 0.043
Detector resolution: 8.333 pixels mm-1 θmax = 27.3°, θmin = 2.4°
φ and ω scans h = −12→12
Absorption correction: multi-scan (Blessing, 1995) k = −22→22
Tmin = 0.668, Tmax = 0.746 l = −15→15
44399 measured reflections

Refinement

Refinement on F2 Primary atom site location: structure-invariant direct methods
Least-squares matrix: full Secondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.050 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.134 H atoms treated by a mixture of independent and constrained refinement
S = 1.05 w = 1/[σ2(Fo2) + (0.0594P)2 + 0.720P] where P = (Fo2 + 2Fc2)/3
4500 reflections (Δ/σ)max < 0.001
308 parameters Δρmax = 0.26 e Å−3
5 restraints Δρmin = −0.21 e Å−3

Special details

Experimental. 1H NMR (500 MHz, CDCl3): δ 8.00 (d, 1H, J 10 Hz), 7.20-7.17 (m, 2H), 6.93 (t, 1H) 7.71 (d, 1H, J 5 Hz), 5.29 (d, 1H, J 10Hz), 3.22 (s, 3H), 2.56 (dd, 2H, J 5 Hz), 2.32(m, 1H), 2.15 (m, 2H), 1.95 (m, 2H), 1.63 (s, 6H), 0.98 (s, 9H). 13C NMR (75 MHz, CDCl3): δ 198.5, 165.1, 144.4, 139.5, 134.5, 127.8, 124.1, 121.8, 121.1, 106.9, 91.5, 46.8, 44.9, 39.3, 32.7, 29.7, 28.7, 27.4, 26.8, 24.0. LCMS found: MH+ 338.2475; C23H31NO requires MH+ 338.2484; Δ = -2.7 ppm
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 Occ. (<1)
O1 0.28457 (12) 0.66246 (6) 0.71213 (10) 0.0437 (3)
N1 0.79474 (12) 0.49759 (7) 1.02889 (9) 0.0283 (3)
C1 0.89106 (14) 0.53885 (8) 1.10624 (11) 0.0270 (3)
C2 1.00469 (15) 0.51059 (9) 1.18053 (12) 0.0331 (3)
H2 1.0261 0.4567 1.1848 0.040*
C3 1.08596 (16) 0.56435 (10) 1.24853 (12) 0.0379 (4)
H3 1.1654 0.5469 1.2995 0.045*
C4 1.05364 (16) 0.64254 (10) 1.24352 (12) 0.0384 (4)
H4 1.1103 0.6779 1.2915 0.046*
C5 0.93804 (15) 0.67029 (9) 1.16829 (12) 0.0320 (3)
H5 0.9150 0.7239 1.1654 0.038*
C6 0.85852 (14) 0.61754 (8) 1.09849 (11) 0.0265 (3)
C7 0.73269 (13) 0.63014 (8) 1.00634 (11) 0.0259 (3)
C8 0.70101 (13) 0.54643 (8) 0.96512 (11) 0.0262 (3)
C9 0.79355 (16) 0.41346 (8) 1.02159 (13) 0.0335 (3)
H9A 0.8428 0.3971 0.9616 0.050*
H9B 0.6969 0.3950 1.0053 0.050*
H9C 0.8401 0.3915 1.0929 0.050*
C10 0.77348 (15) 0.68104 (9) 0.91287 (12) 0.0329 (3)
H10A 0.8527 0.6574 0.8854 0.049*
H10B 0.7997 0.7329 0.9425 0.049*
H10C 0.6940 0.6852 0.8512 0.049*
C11 0.61232 (15) 0.66848 (9) 1.05326 (12) 0.0340 (3)
H11A 0.6454 0.7166 1.0921 0.051*
H11B 0.5790 0.6329 1.1059 0.051*
H11C 0.5358 0.6803 0.9916 0.051*
C12 0.60291 (14) 0.52054 (8) 0.87812 (11) 0.0299 (3)
H12 0.6070 0.4673 0.8587 0.036*
C13 0.49551 (14) 0.56575 (8) 0.81416 (11) 0.0291 (3)
H13 0.4886 0.6184 0.8360 0.035*
C14 0.40147 (14) 0.54095 (8) 0.72454 (11) 0.0286 (3)
C15 0.29387 (14) 0.59685 (9) 0.67486 (12) 0.0308 (3)
C16 0.19053 (16) 0.57155 (10) 0.57339 (14) 0.0418 (4)
H16A 0.0979 0.5924 0.5811 0.063*
H16B 0.2175 0.5965 0.5068 0.063*
C19 0.4067 (2) 0.46039 (9) 0.67678 (13) 0.0394 (4)
H19A 0.496 (2) 0.4472 (12) 0.6680 (17) 0.059*
H19B 0.375 (2) 0.4235 (12) 0.7229 (18) 0.059*
C17A 0.1748 (3) 0.48893 (14) 0.5508 (2) 0.0303 (5) 0.663 (3)
H17A 0.118 (3) 0.4799 (16) 0.480 (2) 0.045* 0.663 (3)
H17B 0.129 (3) 0.4671 (16) 0.610 (2) 0.045* 0.663 (3)
C18A 0.3166 (2) 0.45000 (15) 0.5576 (2) 0.0255 (5) 0.663 (3)
H18A 0.366 (3) 0.4800 (15) 0.507 (2) 0.038* 0.663 (3)
C20A 0.3096 (6) 0.3654 (4) 0.5180 (5) 0.0281 (10) 0.663 (3)
C21A 0.4546 (3) 0.32873 (16) 0.5326 (3) 0.0469 (7) 0.663 (3)
H21A 0.4482 0.2777 0.4964 0.070* 0.663 (3)
H21B 0.4919 0.3228 0.6126 0.070* 0.663 (3)
H21C 0.5168 0.3622 0.4982 0.070* 0.663 (3)
C22A 0.2492 (3) 0.36163 (15) 0.39073 (19) 0.0434 (6) 0.663 (3)
H22A 0.1527 0.3805 0.3776 0.065* 0.663 (3)
H22B 0.2511 0.3078 0.3648 0.065* 0.663 (3)
H22C 0.3056 0.3942 0.3496 0.065* 0.663 (3)
C23A 0.2173 (3) 0.31416 (14) 0.5787 (2) 0.0400 (6) 0.663 (3)
H23A 0.2166 0.2610 0.5497 0.060* 0.663 (3)
H23B 0.1219 0.3347 0.5659 0.060* 0.663 (3)
H23C 0.2544 0.3141 0.6591 0.060* 0.663 (3)
C17B 0.2366 (6) 0.4922 (3) 0.5221 (4) 0.0331 (11) 0.337 (3)
H17C 0.1547 0.4715 0.4705 0.050* 0.337 (3)
H17D 0.3085 0.5048 0.4764 0.050* 0.337 (3)
C18B 0.2938 (5) 0.4273 (3) 0.6024 (5) 0.0268 (10) 0.337 (3)
H18B 0.225 (6) 0.421 (3) 0.653 (4) 0.040* 0.337 (3)
C20B 0.3155 (11) 0.3475 (7) 0.5420 (9) 0.030 (2) 0.337 (3)
C21B 0.3865 (6) 0.2909 (3) 0.6310 (5) 0.0512 (15) 0.337 (3)
H21D 0.4037 0.2415 0.5954 0.077* 0.337 (3)
H21E 0.3259 0.2818 0.6863 0.077* 0.337 (3)
H21F 0.4754 0.3128 0.6683 0.077* 0.337 (3)
C22B 0.4077 (6) 0.3596 (3) 0.4542 (5) 0.0498 (15) 0.337 (3)
H22D 0.4241 0.3096 0.4203 0.075* 0.337 (3)
H22E 0.4970 0.3820 0.4897 0.075* 0.337 (3)
H22F 0.3612 0.3950 0.3962 0.075* 0.337 (3)
C23B 0.1757 (5) 0.3156 (3) 0.4890 (5) 0.0526 (16) 0.337 (3)
H23D 0.1150 0.3123 0.5454 0.079* 0.337 (3)
H23E 0.1878 0.2638 0.4589 0.079* 0.337 (3)
H23F 0.1331 0.3501 0.4282 0.079* 0.337 (3)

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
O1 0.0452 (6) 0.0324 (6) 0.0489 (7) 0.0034 (5) −0.0046 (5) −0.0071 (5)
N1 0.0312 (6) 0.0245 (6) 0.0280 (6) −0.0020 (4) 0.0014 (5) 0.0022 (4)
C1 0.0286 (7) 0.0298 (7) 0.0231 (6) −0.0024 (5) 0.0057 (5) 0.0015 (5)
C2 0.0356 (8) 0.0353 (8) 0.0280 (7) 0.0050 (6) 0.0044 (6) 0.0057 (6)
C3 0.0327 (8) 0.0506 (10) 0.0279 (7) 0.0025 (7) −0.0018 (6) 0.0026 (6)
C4 0.0362 (8) 0.0451 (9) 0.0311 (7) −0.0066 (7) −0.0018 (6) −0.0062 (6)
C5 0.0327 (7) 0.0315 (7) 0.0313 (7) −0.0029 (6) 0.0040 (6) −0.0027 (6)
C6 0.0239 (6) 0.0303 (7) 0.0252 (6) −0.0007 (5) 0.0040 (5) 0.0022 (5)
C7 0.0250 (6) 0.0247 (7) 0.0271 (6) −0.0030 (5) 0.0017 (5) 0.0007 (5)
C8 0.0261 (6) 0.0270 (7) 0.0264 (6) −0.0026 (5) 0.0066 (5) 0.0025 (5)
C9 0.0392 (8) 0.0237 (7) 0.0367 (7) −0.0017 (6) 0.0046 (6) 0.0022 (6)
C10 0.0331 (7) 0.0302 (7) 0.0342 (7) −0.0038 (6) 0.0026 (6) 0.0063 (6)
C11 0.0285 (7) 0.0367 (8) 0.0363 (7) 0.0006 (6) 0.0046 (6) −0.0049 (6)
C12 0.0331 (7) 0.0267 (7) 0.0291 (7) −0.0051 (5) 0.0033 (6) −0.0007 (5)
C13 0.0276 (7) 0.0299 (7) 0.0299 (7) −0.0049 (5) 0.0050 (5) −0.0018 (5)
C14 0.0297 (7) 0.0292 (7) 0.0263 (6) −0.0046 (5) 0.0031 (5) −0.0010 (5)
C15 0.0277 (7) 0.0321 (8) 0.0322 (7) −0.0048 (5) 0.0040 (6) −0.0023 (6)
C16 0.0269 (7) 0.0476 (10) 0.0470 (9) 0.0031 (6) −0.0046 (6) −0.0127 (7)
C19 0.0522 (10) 0.0295 (8) 0.0313 (8) 0.0017 (7) −0.0068 (7) −0.0026 (6)
C17A 0.0213 (12) 0.0320 (12) 0.0342 (13) 0.0011 (10) −0.0042 (10) −0.0044 (10)
C18A 0.0219 (11) 0.0286 (13) 0.0249 (12) −0.0020 (9) 0.0009 (9) −0.0001 (10)
C20A 0.0269 (14) 0.023 (3) 0.034 (2) −0.0007 (14) 0.0050 (12) 0.0008 (14)
C21A 0.0356 (13) 0.0441 (15) 0.0596 (18) 0.0067 (11) 0.0046 (12) −0.0154 (13)
C22A 0.0568 (16) 0.0425 (14) 0.0300 (12) −0.0024 (11) 0.0047 (11) −0.0081 (10)
C23A 0.0465 (14) 0.0316 (12) 0.0440 (14) −0.0074 (10) 0.0137 (11) −0.0016 (10)
C17B 0.027 (3) 0.036 (3) 0.032 (2) 0.001 (2) −0.005 (2) −0.0046 (19)
C18B 0.028 (2) 0.024 (2) 0.029 (2) −0.0033 (17) 0.0057 (19) 0.0004 (19)
C20B 0.040 (3) 0.013 (5) 0.039 (5) −0.005 (3) 0.009 (3) −0.009 (3)
C21B 0.069 (4) 0.028 (3) 0.053 (3) −0.003 (2) 0.002 (3) −0.004 (2)
C22B 0.054 (3) 0.049 (3) 0.052 (3) −0.005 (2) 0.024 (3) −0.013 (3)
C23B 0.039 (3) 0.049 (3) 0.068 (4) −0.009 (2) 0.005 (3) −0.029 (3)

Geometric parameters (Å, °)

O1—C15 1.2260 (18) C19—C18B 1.415 (4)
N1—C8 1.3754 (17) C19—C18A 1.565 (3)
N1—C1 1.3989 (17) C19—H19A 0.92 (2)
N1—C9 1.4513 (17) C19—H19B 0.93 (2)
C1—C2 1.3872 (19) C17A—C18A 1.524 (4)
C1—C6 1.3910 (19) C17A—H17A 0.95 (3)
C2—C3 1.391 (2) C17A—H17B 0.98 (3)
C2—H2 0.9500 C18A—C20A 1.531 (7)
C3—C4 1.381 (2) C18A—H18A 0.99 (3)
C3—H3 0.9500 C20A—C21A 1.528 (6)
C4—C5 1.403 (2) C20A—C23A 1.537 (5)
C4—H4 0.9500 C20A—C22A 1.554 (7)
C5—C6 1.3828 (19) C21A—H21A 0.9800
C5—H5 0.9500 C21A—H21B 0.9800
C6—C7 1.5228 (18) C21A—H21C 0.9800
C7—C11 1.5378 (19) C22A—H22A 0.9800
C7—C10 1.5389 (19) C22A—H22B 0.9800
C7—C8 1.5392 (18) C22A—H22C 0.9800
C8—C12 1.3684 (18) C23A—H23A 0.9800
C9—H9A 0.9800 C23A—H23B 0.9800
C9—H9B 0.9800 C23A—H23C 0.9800
C9—H9C 0.9800 C17B—C18B 1.523 (7)
C10—H10A 0.9800 C17B—H17C 0.9900
C10—H10B 0.9800 C17B—H17D 0.9900
C10—H10C 0.9800 C18B—C20B 1.587 (14)
C11—H11A 0.9800 C18B—H18B 0.99 (5)
C11—H11B 0.9800 C20B—C23B 1.504 (11)
C11—H11C 0.9800 C20B—C22B 1.521 (11)
C12—C13 1.4204 (19) C20B—C21B 1.527 (9)
C12—H12 0.9500 C21B—H21D 0.9800
C13—C14 1.3619 (18) C21B—H21E 0.9800
C13—H13 0.9500 C21B—H21F 0.9800
C14—C15 1.472 (2) C22B—H22D 0.9800
C14—C19 1.508 (2) C22B—H22E 0.9800
C15—C16 1.5114 (19) C22B—H22F 0.9800
C16—C17A 1.452 (3) C23B—H23D 0.9800
C16—C17B 1.597 (5) C23B—H23E 0.9800
C16—H16A 0.9900 C23B—H23F 0.9800
C16—H16B 0.9900
C8—N1—C1 111.58 (11) H16A—C16—H16B 107.1
C8—N1—C9 125.35 (12) C18B—C19—C14 122.8 (2)
C1—N1—C9 123.04 (11) C14—C19—C18A 114.15 (14)
C2—C1—C6 122.14 (13) C18B—C19—H19A 118.0 (13)
C2—C1—N1 128.51 (13) C14—C19—H19A 111.5 (13)
C6—C1—N1 109.35 (11) C18A—C19—H19A 104.6 (13)
C1—C2—C3 117.27 (14) C18B—C19—H19B 78.9 (13)
C1—C2—H2 121.4 C14—C19—H19B 111.0 (13)
C3—C2—H2 121.4 C18A—C19—H19B 106.6 (13)
C4—C3—C2 121.39 (14) H19A—C19—H19B 108.5 (18)
C4—C3—H3 119.3 C16—C17A—C18A 110.9 (2)
C2—C3—H3 119.3 C16—C17A—H17A 110.8 (17)
C3—C4—C5 120.74 (14) C18A—C17A—H17A 111.0 (17)
C3—C4—H4 119.6 C16—C17A—H17B 106.3 (16)
C5—C4—H4 119.6 C18A—C17A—H17B 108.2 (17)
C6—C5—C4 118.31 (14) H17A—C17A—H17B 109 (2)
C6—C5—H5 120.8 C17A—C18A—C20A 114.3 (3)
C4—C5—H5 120.8 C17A—C18A—C19 110.9 (2)
C5—C6—C1 120.13 (12) C20A—C18A—C19 112.7 (3)
C5—C6—C7 130.43 (13) C17A—C18A—H18A 105.7 (15)
C1—C6—C7 109.44 (11) C20A—C18A—H18A 107.5 (15)
C6—C7—C11 110.89 (11) C19—C18A—H18A 105.0 (15)
C6—C7—C10 110.13 (11) C21A—C20A—C18A 111.6 (4)
C11—C7—C10 109.83 (12) C21A—C20A—C23A 108.2 (3)
C6—C7—C8 101.24 (10) C18A—C20A—C23A 113.2 (5)
C11—C7—C8 113.57 (11) C21A—C20A—C22A 106.3 (5)
C10—C7—C8 110.91 (11) C18A—C20A—C22A 109.9 (3)
C12—C8—N1 122.67 (13) C23A—C20A—C22A 107.5 (4)
C12—C8—C7 128.96 (12) C18B—C17B—C16 118.4 (4)
N1—C8—C7 108.32 (11) C18B—C17B—H17A 111.2 (14)
N1—C9—H9A 109.5 C16—C17B—H18A 122.0 (12)
N1—C9—H9B 109.5 C16—C17B—H17C 107.7
H9A—C9—H9B 109.5 H18A—C17B—H17C 122.5
N1—C9—H9C 109.5 C18B—C17B—H17D 107.7
H9A—C9—H9C 109.5 C16—C17B—H17D 107.7
H9B—C9—H9C 109.5 H17A—C17B—H17D 121.5
C7—C10—H10A 109.5 H17C—C17B—H17D 107.1
C7—C10—H10B 109.5 C19—C18B—C17B 105.6 (4)
H10A—C10—H10B 109.5 C19—C18B—C20B 119.4 (5)
C7—C10—H10C 109.5 C17B—C18B—C20B 113.8 (5)
H10A—C10—H10C 109.5 C19—C18B—H18B 100 (3)
H10B—C10—H10C 109.5 C17B—C18B—H18B 106 (3)
C7—C11—H11A 109.5 C20B—C18B—H18B 110 (3)
C7—C11—H11B 109.5 C23B—C20B—C22B 110.5 (8)
H11A—C11—H11B 109.5 C23B—C20B—C21B 109.4 (7)
C7—C11—H11C 109.5 C22B—C20B—C21B 109.4 (8)
H11A—C11—H11C 109.5 C23B—C20B—C18B 109.2 (8)
H11B—C11—H11C 109.5 C22B—C20B—C18B 110.3 (7)
C8—C12—C13 126.21 (13) C21B—C20B—C18B 107.9 (8)
C8—C12—H12 116.9 C20B—C21B—H21D 109.5
C13—C12—H12 116.9 C20B—C21B—H21E 109.5
C14—C13—C12 126.32 (14) H21D—C21B—H21E 109.5
C14—C13—H13 116.8 C20B—C21B—H21F 109.5
C12—C13—H13 116.8 H21D—C21B—H21F 109.5
C13—C14—C15 116.93 (13) H21E—C21B—H21F 109.5
C13—C14—C19 122.16 (13) C20B—C22B—H22D 109.5
C15—C14—C19 120.91 (12) C20B—C22B—H22E 109.5
O1—C15—C14 123.00 (13) H22D—C22B—H22E 109.5
O1—C15—C16 118.98 (13) C20B—C22B—H22F 109.5
C14—C15—C16 118.03 (13) H22D—C22B—H22F 109.5
C17A—C16—C15 118.01 (16) H22E—C22B—H22F 109.5
C15—C16—C17B 111.8 (2) C20B—C23B—H23D 109.5
C17A—C16—H16A 107.8 C20B—C23B—H23E 109.5
C15—C16—H16A 107.8 H23D—C23B—H23E 109.5
C17B—C16—H16A 132.0 C20B—C23B—H23F 109.5
C17A—C16—H16B 107.8 H23D—C23B—H23F 109.5
C15—C16—H16B 107.8 H23E—C23B—H23F 109.5
C17B—C16—H16B 85.5
C8—N1—C1—C2 −176.44 (14) C12—C13—C14—C19 −4.0 (2)
C9—N1—C1—C2 5.6 (2) C13—C14—C15—O1 −1.7 (2)
C8—N1—C1—C6 2.69 (16) C19—C14—C15—O1 178.83 (15)
C9—N1—C1—C6 −175.30 (13) C13—C14—C15—C16 178.40 (13)
C6—C1—C2—C3 0.3 (2) C19—C14—C15—C16 −1.1 (2)
N1—C1—C2—C3 179.35 (13) O1—C15—C16—C17A −161.6 (2)
C1—C2—C3—C4 1.0 (2) C14—C15—C16—C17A 18.3 (3)
C2—C3—C4—C5 −0.7 (2) O1—C15—C16—C17B 168.3 (3)
C3—C4—C5—C6 −0.8 (2) C14—C15—C16—C17B −11.7 (3)
C4—C5—C6—C1 2.0 (2) C13—C14—C19—C18B 164.7 (3)
C4—C5—C6—C7 −177.19 (14) C15—C14—C19—C18B −15.8 (4)
C2—C1—C6—C5 −1.9 (2) C13—C14—C19—C18A −164.90 (17)
N1—C1—C6—C5 178.95 (12) C15—C14—C19—C18A 14.5 (2)
C2—C1—C6—C7 177.53 (12) C15—C16—C17A—C18A −48.0 (3)
N1—C1—C6—C7 −1.67 (15) C16—C17A—C18A—C20A −171.4 (3)
C5—C6—C7—C11 −59.72 (19) C16—C17A—C18A—C19 60.0 (3)
C1—C6—C7—C11 120.99 (13) C14—C19—C18A—C17A −43.3 (3)
C5—C6—C7—C10 62.06 (19) C14—C19—C18A—C20A −172.8 (3)
C1—C6—C7—C10 −117.23 (13) C17A—C18A—C20A—C21A −177.1 (3)
C5—C6—C7—C8 179.47 (14) C19—C18A—C20A—C21A −49.3 (4)
C1—C6—C7—C8 0.18 (14) C17A—C18A—C20A—C23A −54.8 (4)
C1—N1—C8—C12 175.08 (12) C19—C18A—C20A—C23A 73.0 (4)
C9—N1—C8—C12 −7.0 (2) C17A—C18A—C20A—C22A 65.3 (4)
C1—N1—C8—C7 −2.53 (15) C19—C18A—C20A—C22A −166.9 (3)
C9—N1—C8—C7 175.40 (12) C15—C16—C17B—C18B 42.5 (6)
C6—C7—C8—C12 −176.03 (14) C14—C19—C18B—C17B 41.3 (5)
C11—C7—C8—C12 65.07 (18) C14—C19—C18B—C20B 171.0 (4)
C10—C7—C8—C12 −59.19 (18) C16—C17B—C18B—C19 −55.4 (6)
C6—C7—C8—N1 1.39 (13) C16—C17B—C18B—C20B 171.7 (5)
C11—C7—C8—N1 −117.52 (12) C19—C18B—C20B—C23B 167.3 (5)
C10—C7—C8—N1 118.23 (12) C17B—C18B—C20B—C23B −66.8 (7)
N1—C8—C12—C13 174.55 (13) C19—C18B—C20B—C22B −71.0 (7)
C7—C8—C12—C13 −8.4 (2) C17B—C18B—C20B—C22B 54.9 (8)
C8—C12—C13—C14 177.00 (14) C19—C18B—C20B—C21B 48.5 (8)
C12—C13—C14—C15 176.56 (13) C17B—C18B—C20B—C21B 174.4 (6)

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
C5—H5···O1i 0.95 2.45 3.3293 (19) 154
C9—H9A···Cg1ii 0.98 2.65 3.5705 (17) 156

Symmetry codes: (i) x+1/2, −y+3/2, z+1/2; (ii) −x+2, −y+1, −z+2.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: JJ2085).

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 datablocks global, I. DOI: 10.1107/S1600536811014590/jj2085sup1.cif

e-67-o1210-sup1.cif (35.7KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536811014590/jj2085Isup2.hkl

e-67-o1210-Isup2.hkl (220.5KB, hkl)

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


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