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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2008 Dec 6;65(Pt 1):o25. doi: 10.1107/S1600536808040397

N-(Diphenyl­vinyl­idene)-2,6-diisopropyl­aniline

Wolfgang Imhof a,*
PMCID: PMC2967944  PMID: 21581668

Abstract

The title compound, C26H27N, was prepared by the elimination of water from N-(2,6-diisopropyl­phen­yl)-2,2-diphenyl­acetamide. The angle at the central C atom of the cumulene measures 172.5 (4)°. Mol­ecules are connected into infinite chains by inter­molecular C—H⋯N inter­actions.

Related literature

For the synthetic procedure, see: Stevens & Singhal (1964). For related structures, see: Naqvi & Wheatley (1970); Jochims et al. (1984); Kuipers et al. (1989). For general background, see: Imhof (1997a ,b ). For properties of weak hydrogen bonds, see: Desiraju & Steiner (1999).graphic file with name e-65-00o25-scheme1.jpg

Experimental

Crystal data

  • C26H27N

  • M r = 353.49

  • Orthorhombic, Inline graphic

  • a = 8.082 (4) Å

  • b = 14.308 (4) Å

  • c = 17.790 (2) Å

  • V = 2057 (1) Å3

  • Z = 4

  • Mo Kα radiation

  • μ = 0.07 mm−1

  • T = 173 (2) K

  • 0.3 × 0.2 × 0.2 mm

Data collection

  • Enraf–Nonius CAD-4 diffractometer

  • Absorption correction: none

  • 3554 measured reflections

  • 1853 independent reflections

  • 1531 reflections with I > 2σ(I)

  • R int = 0.065

  • θmax = 24.0°

  • 3 standard reflections frequency: 120 min intensity decay: <0.1%

Refinement

  • R[F 2 > 2σ(F 2)] = 0.040

  • wR(F 2) = 0.103

  • S = 0.82

  • 1853 reflections

  • 248 parameters

  • H-atom parameters constrained

  • Δρmax = 0.15 e Å−3

  • Δρmin = −0.17 e Å−3

Data collection: CAD-4 EXPRESS (Enraf–Nonius, 1994); cell refinement: SET4 (de Boer & Duisenberg, 1984); data reduction: MolEN (Enraf–Nonius, 1990); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: XP (Siemens, 1990); software used to prepare material for publication: SHELXL97.

Supplementary Material

Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536808040397/nc2125sup1.cif

e-65-00o25-sup1.cif (21.2KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536808040397/nc2125Isup2.hkl

e-65-00o25-Isup2.hkl (91.3KB, hkl)

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

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

D—H⋯A D—H H⋯A DA D—H⋯A
C5—H5⋯N1i 0.95 2.72 3.554 (4) 146

Symmetry code: (i) Inline graphic.

supplementary crystallographic information

Comment

In the course of a study on the organometallic and catalytic chemistry of aromatic imines (Imhof, 1997a,b) we became interested in the reactivity of the vinylogous keteneimines. The latter are prepared by the elimination of water from the corresponding acetamides by P2O5 in anhydrous pyridine (Stevens & Singhal, 1964).

As expected the molecular structure of the title compound shows an almost linear cumulene system with an angle of 172.5 (4)° at the central C atom. The bonds C1—C2 and C2—N1 show bond lengths of 1.332 (5) and 1.213 (4) Å, respectively. The dihedral angle between the C1—C8—C14 plane and the aromatic substituent at the imine N atom measures to 52.4 (7)° which means that the substituents at the cumulene system do not show the expected orthogonal arrangement. This is most probably caused by the high steric requirements of the two isopropyl groups in ortho-position. A comparison with related aromatic diphenylvinylidene amines from the literature shows that the corresponding dihedral angle is close to 90° if there is no or just one ortho-substituent present in the aromatic group at nitrogen (p-Br-C6H4: 85.6°, Naqvi & Wheatley, 1970; o-Me-C6H4: 88.1°, Jochims et al., 1984; p-(N═C═CPh2)-C6H4: 88.4°, Kuipers et al., 1989; p-Me-C6H4: 83.9°, Naqvi & Wheatley, 1970). If both ortho-positions are substituted the conformation is no longer orthogonal (o-Me2-C6H3: 51.7°, Jochims et al., 1984) as it is also observed for the title compound. The lone pair at nitrogen is involved in a weak intramolecular hydrogen bond (Desiraju & Steiner, 1999) interaction towards H5 leading to the formation of infinite chains.

Experimental

The title compound was prepared following a literature method (Stevens & Singhal, 1964). A sample of 2 g (5.4 mmol) N-(2,6-Diisopropyl-phenyl)-2,2-diphenyl-acetamide was dissolved in 50 ml of anhydrous pyridine. To this solution 5 g P2O5 were added and the mixture was refluxed for 7 h. After cooling the solution was filtered and pyridine was evaporated resulting in a red oily residue. The oil was transferred to a short chromatography column and light petroleum (b.p. 40–60°C) was used to elute a yellow solution of the title compound. Concentration of the solution and cooling to 4°C led to the formation of crystalline material from which the crystal for the structure analysis described herein was collected (yield: 1.56 g, 82%). MS (EI) [m/z, %]: 353 (M+, 80), 338 (C25H24N+, 22), 186 (C13H16N+, 100), 165 (C13H9+, 50), 115 (C9H7+, 19), 91 (C7H7+, 37), 77 (C6H5+, 17), 55 (C4H7+, 11), 41 (C3H5+, 35). 1H NMR (CDCl3, 298 K) [p.p.m.]: 1.11 (12 H, d, 3JHH = 6.8 Hz, CH3), 3.24 (2 H, h, 3JHH = 6.8 Hz, CH), 7.05–7.34 (15 H, m, CHar). 13C NMR (CDCl3, 298 K) [p.p.m.]: 22.4 (CH3), 28.5 (CH), 72.0 (═C), 123.4 (CarH), 125.9 (CarH), 126.3 (CarH), 127.8 (CarH), 128.7 (CarH), 134.8 (Car), 136.2 (Car), 140.8 (Car), 183.4 (═C═).

Refinement

H atoms were positioned with idealized geometry at distances of 0.95 Å for aromatic C—H functions, 1.00 Å for aliphatic C—H bonds and 0.98 Å for methyl groups and were refined riding on their parent atoms with isotropic thermal parameters of 1.2 times the corresponding values of their parent atoms. In the absence of significant anomalous dispersion effects, Friedel pairs were averaged.

Figures

Fig. 1.

Fig. 1.

The molecular structure of the title compound, presenting the labelling scheme and 40% probability displacement ellipsoids for non-H atoms.

Fig. 2.

Fig. 2.

Infinite chains of the title compound realized by C—H···O hydrogen bonds.

Crystal data

C26H27N F(000) = 760
Mr = 353.49 Dx = 1.141 Mg m3
Orthorhombic, P212121 Mo Kα radiation, λ = 0.71073 Å
Hall symbol: P 2ac 2ab Cell parameters from 25 reflections
a = 8.082 (4) Å θ = 20.9–35.5°
b = 14.308 (4) Å µ = 0.07 mm1
c = 17.790 (2) Å T = 173 K
V = 2057 (1) Å3 Cube, pale yellow
Z = 4 0.3 × 0.2 × 0.2 mm

Data collection

Enraf–Nonius CAD-4 diffractometer Rint = 0.065
Radiation source: fine-focus sealed tube θmax = 24.0°, θmin = 1.8°
graphite h = −9→0
ω/2θ scans k = −16→16
3554 measured reflections l = 0→20
1853 independent reflections 3 standard reflections every 120 min
1531 reflections with I > 2σ(I) intensity decay: <0.1%

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)] = 0.040 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.103 H-atom parameters constrained
S = 0.82 w = 1/[σ2(Fo2) + (0.1319P)2 + 0.5946P] where P = (Fo2 + 2Fc2)/3
1853 reflections (Δ/σ)max < 0.001
248 parameters Δρmax = 0.15 e Å3
0 restraints Δρmin = −0.17 e Å3

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 on F2 for ALL reflections except for 9 with very negative F2 or flagged by the user for potential systematic errors. Weighted R-factors wR and all goodnesses of fit S are based on F2, conventional R-factors R are based on F, with F set to zero for negative F2. The observed criterion of F2 > σ(F2) is used only for calculating _R_factor_obs 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
N1 0.1809 (3) 0.90928 (16) 0.93459 (13) 0.0304 (6)
C1 0.2195 (4) 1.06100 (19) 1.00668 (17) 0.0303 (7)
C2 0.1892 (4) 0.98254 (19) 0.96930 (15) 0.0306 (7)
C3 0.1148 (4) 0.9958 (2) 1.12860 (17) 0.0363 (7)
H3 0.0626 0.9470 1.1012 0.044*
C4 0.1008 (4) 0.9981 (2) 1.20605 (18) 0.0421 (8)
H4 0.0401 0.9508 1.2314 0.051*
C5 0.1749 (4) 1.0691 (2) 1.24668 (18) 0.0414 (8)
H5 0.1636 1.0717 1.2998 0.050*
C6 0.2652 (4) 1.1358 (2) 1.20919 (18) 0.0408 (8)
H6 0.3178 1.1841 1.2370 0.049*
C7 0.2810 (4) 1.1341 (2) 1.13188 (16) 0.0339 (7)
H7 0.3444 1.1807 1.1071 0.041*
C8 0.2041 (4) 1.06391 (18) 1.09007 (17) 0.0289 (6)
C9 0.1828 (5) 1.2310 (2) 0.97473 (17) 0.0404 (8)
H9 0.1050 1.2370 1.0144 0.049*
C10 0.2210 (5) 1.3071 (2) 0.9299 (2) 0.0494 (9)
H10 0.1695 1.3656 0.9395 0.059*
C11 0.3325 (6) 1.2993 (3) 0.87148 (19) 0.0569 (11)
H11 0.3577 1.3521 0.8411 0.068*
C12 0.4071 (5) 1.2144 (3) 0.85749 (19) 0.0544 (10)
H12 0.4830 1.2085 0.8170 0.065*
C13 0.3720 (4) 1.1378 (2) 0.90200 (17) 0.0408 (8)
H13 0.4248 1.0797 0.8923 0.049*
C14 0.2595 (4) 1.1454 (2) 0.96113 (15) 0.0314 (6)
C15 0.0304 (4) 0.7690 (2) 0.90761 (15) 0.0300 (7)
C16 −0.1020 (4) 0.7236 (2) 0.87388 (17) 0.0374 (7)
H16 −0.1141 0.6580 0.8796 0.045*
C17 −0.2159 (4) 0.7728 (2) 0.83219 (19) 0.0432 (8)
H17 −0.3071 0.7409 0.8103 0.052*
C18 −0.1993 (4) 0.8682 (2) 0.82167 (17) 0.0406 (7)
H18 −0.2781 0.9007 0.7918 0.049*
C19 −0.0683 (4) 0.9176 (2) 0.85429 (16) 0.0335 (7)
C20 0.0419 (4) 0.8665 (2) 0.89897 (14) 0.0282 (6)
C21 0.1642 (4) 0.7162 (2) 0.95050 (17) 0.0364 (7)
H21 0.1917 0.7540 0.9961 0.044*
C22 0.3218 (5) 0.7091 (2) 0.9033 (2) 0.0461 (8)
H22A 0.3554 0.7716 0.8869 0.055*
H22B 0.3008 0.6698 0.8592 0.055*
H22C 0.4103 0.6812 0.9336 0.055*
C23 0.1115 (6) 0.6197 (2) 0.9776 (2) 0.0545 (10)
H23A 0.1997 0.5926 1.0085 0.065*
H23B 0.0906 0.5793 0.9342 0.065*
H23C 0.0103 0.6252 1.0076 0.065*
C24 −0.0519 (4) 1.0221 (2) 0.84131 (18) 0.0396 (8)
H24 0.0658 1.0392 0.8521 0.048*
C25 −0.1593 (5) 1.0765 (2) 0.8963 (3) 0.0586 (10)
H25A −0.1315 1.0581 0.9478 0.070*
H25B −0.2761 1.0628 0.8865 0.070*
H25C −0.1394 1.1436 0.8899 0.070*
C26 −0.0872 (5) 1.0502 (3) 0.7602 (2) 0.0623 (11)
H26A −0.2043 1.0392 0.7488 0.075*
H26B −0.0183 1.0129 0.7262 0.075*
H26C −0.0618 1.1167 0.7534 0.075*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
N1 0.0354 (14) 0.0255 (12) 0.0303 (12) 0.0015 (11) −0.0040 (11) −0.0019 (10)
C1 0.0340 (16) 0.0248 (14) 0.0322 (14) −0.0013 (14) −0.0016 (13) −0.0040 (12)
C2 0.0334 (15) 0.0293 (15) 0.0291 (13) 0.0027 (13) −0.0018 (13) 0.0026 (13)
C3 0.0431 (17) 0.0271 (13) 0.0387 (15) −0.0057 (15) −0.0027 (15) −0.0019 (13)
C4 0.0489 (18) 0.0383 (16) 0.0391 (16) −0.0007 (17) 0.0021 (16) 0.0087 (14)
C5 0.0473 (19) 0.0491 (18) 0.0279 (14) 0.0042 (17) −0.0023 (15) 0.0052 (14)
C6 0.0512 (18) 0.0367 (16) 0.0347 (15) −0.0019 (17) −0.0147 (15) −0.0037 (13)
C7 0.0391 (16) 0.0298 (14) 0.0329 (15) −0.0042 (15) −0.0033 (13) 0.0013 (12)
C8 0.0297 (14) 0.0254 (13) 0.0315 (14) 0.0021 (13) −0.0019 (13) −0.0005 (11)
C9 0.0502 (19) 0.0352 (16) 0.0358 (16) −0.0024 (16) −0.0036 (16) 0.0020 (13)
C10 0.065 (2) 0.0340 (16) 0.0491 (19) −0.0055 (18) −0.0197 (19) 0.0057 (15)
C11 0.079 (3) 0.059 (2) 0.0328 (17) −0.040 (2) −0.0121 (19) 0.0129 (17)
C12 0.067 (2) 0.063 (2) 0.0333 (17) −0.031 (2) −0.0003 (18) −0.0005 (16)
C13 0.0444 (18) 0.0420 (16) 0.0360 (15) −0.0120 (16) 0.0041 (14) −0.0062 (15)
C14 0.0365 (15) 0.0316 (14) 0.0260 (13) −0.0075 (15) −0.0038 (12) −0.0018 (12)
C15 0.0369 (16) 0.0290 (14) 0.0242 (13) 0.0021 (13) −0.0013 (14) −0.0039 (12)
C16 0.0438 (18) 0.0333 (15) 0.0351 (15) −0.0013 (15) −0.0010 (15) −0.0049 (14)
C17 0.0385 (18) 0.0483 (18) 0.0427 (17) −0.0083 (16) −0.0062 (16) −0.0083 (16)
C18 0.0399 (17) 0.0486 (18) 0.0334 (15) 0.0025 (17) −0.0105 (14) −0.0015 (14)
C19 0.0338 (16) 0.0365 (16) 0.0303 (14) 0.0024 (14) 0.0029 (13) −0.0040 (13)
C20 0.0319 (14) 0.0284 (13) 0.0242 (13) 0.0035 (13) 0.0007 (12) −0.0048 (11)
C21 0.0454 (18) 0.0283 (14) 0.0354 (15) 0.0048 (14) −0.0075 (15) −0.0029 (13)
C22 0.0431 (18) 0.0409 (17) 0.054 (2) 0.0099 (16) −0.0056 (17) −0.0066 (16)
C23 0.065 (2) 0.0357 (17) 0.063 (2) 0.0021 (19) −0.015 (2) 0.0084 (17)
C24 0.0386 (17) 0.0363 (16) 0.0438 (17) 0.0075 (15) −0.0028 (15) 0.0061 (14)
C25 0.055 (2) 0.0350 (17) 0.086 (3) 0.0103 (18) 0.011 (2) −0.0023 (19)
C26 0.060 (2) 0.064 (2) 0.064 (2) 0.000 (2) −0.010 (2) 0.030 (2)

Geometric parameters (Å, °)

N1—C2 1.218 (4) C15—C20 1.406 (4)
N1—C20 1.428 (4) C15—C21 1.523 (4)
C1—C2 1.328 (4) C16—C17 1.376 (5)
C1—C14 1.490 (4) C16—H16 0.9500
C1—C8 1.489 (4) C17—C18 1.385 (5)
C3—C8 1.393 (4) C17—H17 0.9500
C3—C4 1.383 (4) C18—C19 1.399 (5)
C3—H3 0.9500 C18—H18 0.9500
C4—C5 1.384 (5) C19—C20 1.400 (4)
C4—H4 0.9500 C19—C24 1.519 (4)
C5—C6 1.374 (5) C21—C23 1.523 (5)
C5—H5 0.9500 C21—C22 1.529 (5)
C6—C7 1.381 (4) C21—H21 1.0000
C6—H6 0.9500 C22—H22A 0.9800
C7—C8 1.395 (4) C22—H22B 0.9800
C7—H7 0.9500 C22—H22C 0.9800
C9—C10 1.385 (5) C23—H23A 0.9800
C9—C14 1.393 (5) C23—H23B 0.9800
C9—H9 0.9500 C23—H23C 0.9800
C10—C11 1.380 (6) C24—C26 1.525 (5)
C10—H10 0.9500 C24—C25 1.521 (5)
C11—C12 1.379 (6) C24—H24 1.0000
C11—H11 0.9500 C25—H25A 0.9800
C12—C13 1.381 (5) C25—H25B 0.9800
C12—H12 0.9500 C25—H25C 0.9800
C13—C14 1.395 (4) C26—H26A 0.9800
C13—H13 0.9500 C26—H26B 0.9800
C15—C16 1.388 (5) C26—H26C 0.9800
C2—N1—C20 129.6 (3) C16—C17—H17 119.6
C2—C1—C14 116.9 (3) C18—C17—H17 119.6
C2—C1—C8 120.5 (3) C17—C18—C19 121.0 (3)
C14—C1—C8 122.5 (2) C17—C18—H18 119.5
N1—C2—C1 172.5 (3) C19—C18—H18 119.5
C8—C3—C4 121.1 (3) C18—C19—C20 117.0 (3)
C8—C3—H3 119.5 C18—C19—C24 120.0 (3)
C4—C3—H3 119.5 C20—C19—C24 123.0 (3)
C5—C4—C3 120.2 (3) C15—C20—C19 122.6 (3)
C5—C4—H4 119.9 C15—C20—N1 115.4 (2)
C3—C4—H4 119.9 C19—C20—N1 121.9 (3)
C6—C5—C4 119.1 (3) C23—C21—C15 114.2 (3)
C6—C5—H5 120.4 C23—C21—C22 110.3 (3)
C4—C5—H5 120.4 C15—C21—C22 110.4 (3)
C5—C6—C7 121.3 (3) C23—C21—H21 107.2
C5—C6—H6 119.4 C15—C21—H21 107.2
C7—C6—H6 119.4 C22—C21—H21 107.2
C6—C7—C8 120.2 (3) C21—C22—H22A 109.5
C6—C7—H7 119.9 C21—C22—H22B 109.5
C8—C7—H7 119.9 H22A—C22—H22B 109.5
C3—C8—C7 118.1 (3) C21—C22—H22C 109.5
C3—C8—C1 120.9 (3) H22A—C22—H22C 109.5
C7—C8—C1 120.9 (3) H22B—C22—H22C 109.5
C10—C9—C14 119.5 (3) C21—C23—H23A 109.5
C10—C9—H9 120.3 C21—C23—H23B 109.5
C14—C9—H9 120.3 H23A—C23—H23B 109.5
C11—C10—C9 121.0 (3) C21—C23—H23C 109.5
C11—C10—H10 119.5 H23A—C23—H23C 109.5
C9—C10—H10 119.5 H23B—C23—H23C 109.5
C12—C11—C10 119.5 (3) C19—C24—C26 112.8 (3)
C12—C11—H11 120.2 C19—C24—C25 110.8 (3)
C10—C11—H11 120.2 C26—C24—C25 111.5 (3)
C13—C12—C11 120.4 (3) C19—C24—H24 107.1
C13—C12—H12 119.8 C26—C24—H24 107.1
C11—C12—H12 119.8 C25—C24—H24 107.1
C12—C13—C14 120.3 (3) C24—C25—H25A 109.5
C12—C13—H13 119.9 C24—C25—H25B 109.5
C14—C13—H13 119.9 H25A—C25—H25B 109.5
C9—C14—C13 119.3 (3) C24—C25—H25C 109.5
C9—C14—C1 121.4 (3) H25A—C25—H25C 109.5
C13—C14—C1 119.2 (3) H25B—C25—H25C 109.5
C16—C15—C20 117.8 (3) C24—C26—H26A 109.5
C16—C15—C21 122.1 (3) C24—C26—H26B 109.5
C20—C15—C21 120.0 (3) H26A—C26—H26B 109.5
C17—C16—C15 120.7 (3) C24—C26—H26C 109.5
C17—C16—H16 119.7 H26A—C26—H26C 109.5
C15—C16—H16 119.7 H26B—C26—H26C 109.5
C16—C17—C18 120.8 (3)
C20—N1—C2—C1 −169 (2) C8—C1—C14—C13 137.9 (3)
C14—C1—C2—N1 82 (2) C20—C15—C16—C17 1.3 (4)
C8—C1—C2—N1 −101 (2) C21—C15—C16—C17 −176.5 (3)
C8—C3—C4—C5 0.5 (5) C15—C16—C17—C18 1.3 (5)
C3—C4—C5—C6 −1.4 (5) C16—C17—C18—C19 −1.3 (5)
C4—C5—C6—C7 1.0 (5) C17—C18—C19—C20 −1.3 (5)
C5—C6—C7—C8 0.3 (5) C17—C18—C19—C24 179.4 (3)
C4—C3—C8—C7 0.8 (5) C16—C15—C20—C19 −4.1 (4)
C4—C3—C8—C1 179.7 (3) C21—C15—C20—C19 173.8 (3)
C6—C7—C8—C3 −1.2 (4) C16—C15—C20—N1 −179.8 (2)
C6—C7—C8—C1 179.9 (3) C21—C15—C20—N1 −1.9 (4)
C2—C1—C8—C3 −18.4 (5) C18—C19—C20—C15 4.0 (4)
C14—C1—C8—C3 158.0 (3) C24—C19—C20—C15 −176.7 (3)
C2—C1—C8—C7 160.5 (3) C18—C19—C20—N1 179.5 (3)
C14—C1—C8—C7 −23.1 (4) C24—C19—C20—N1 −1.3 (4)
C14—C9—C10—C11 0.7 (5) C2—N1—C20—C15 −139.4 (3)
C9—C10—C11—C12 0.1 (5) C2—N1—C20—C19 44.9 (4)
C10—C11—C12—C13 −0.7 (6) C16—C15—C21—C23 −21.2 (4)
C11—C12—C13—C14 0.6 (5) C20—C15—C21—C23 161.0 (3)
C10—C9—C14—C13 −0.7 (5) C16—C15—C21—C22 103.7 (3)
C10—C9—C14—C1 −178.5 (3) C20—C15—C21—C22 −74.0 (3)
C12—C13—C14—C9 0.1 (5) C18—C19—C24—C26 −41.8 (4)
C12—C13—C14—C1 178.0 (3) C20—C19—C24—C26 139.0 (3)
C2—C1—C14—C9 132.2 (3) C18—C19—C24—C25 84.0 (4)
C8—C1—C14—C9 −44.3 (4) C20—C19—C24—C25 −95.2 (4)
C2—C1—C14—C13 −45.6 (4)

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
C5—H5···N1i 0.95 2.72 3.554 (4) 146

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

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: NC2125).

References

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  12. Stevens, C. L. & Singhal, G. H. (1964). J. Org. Chem.29, 34–37.

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/S1600536808040397/nc2125sup1.cif

e-65-00o25-sup1.cif (21.2KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536808040397/nc2125Isup2.hkl

e-65-00o25-Isup2.hkl (91.3KB, hkl)

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


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