Literature DB >> 22058757

1,7-Diethyl-4,10-diisopropyl-tetra-cene.

Chitoshi Kitamura, Hiroyuki Kano, Takeshi Kawase, Takashi Kobayashi, Hiroyoshi Naito.   

Abstract

The mol-ecule of the title compound, C(28)H(32), is located on a crystallographic inversion center. The ethyl groups are essentially coplanar with the tetra-cene ring, making a torsion angle of -0.4 (4)°. The isopropyl groups adopt an asymmetric conformation with their terminal methyl groups positioned on opposite sides of the tetra-cene plane [the Me-C-C-C torsion angles are -22.5 (4) and 100.9 (3)°]. In the crystal, the mol-ecules adopt an arrangement without significant π-π inter-actions along the stacking direction (y axis).

Entities:  

Year:  2011        PMID: 22058757      PMCID: PMC3201380          DOI: 10.1107/S1600536811036415

Source DB:  PubMed          Journal:  Acta Crystallogr Sect E Struct Rep Online        ISSN: 1600-5368


Related literature

For applications of tetra­cene derivatives, see: Anthony (2008 ▶). For crystallochromy, see: Klebe et al. (1989 ▶). For the synthesis, see: Kitamura et al. (2011 ▶). For structures of related alkyl-substituted tetra­cene derivatives, see: Kitamura, Abe et al. (2010 ▶); Kitamura, Tsukuda et al. (2010 ▶).

Experimental

Crystal data

C28H32 M = 368.54 Monoclinic, a = 12.901 (4) Å b = 5.057 (2) Å c = 16.962 (6) Å β = 106.513 (9)° V = 1061.0 (7) Å3 Z = 2 Mo Kα radiation μ = 0.06 mm−1 T = 203 K 0.25 × 0.13 × 0.1 mm

Data collection

Rigaku R-AXIS RAPID IP diffractometer 9469 measured reflections 2423 independent reflections 1318 reflections with I > 2σ(I) R int = 0.083

Refinement

R[F 2 > 2σ(F 2)] = 0.081 wR(F 2) = 0.282 S = 1.10 2423 reflections 130 parameters H-atom parameters constrained Δρmax = 0.26 e Å−3 Δρmin = −0.42 e Å−3 Data collection: RAPID-AUTO (Rigaku, 1999 ▶); cell refinement: PROCESS-AUTO (Rigaku, 1998 ▶); data reduction: PROCESS-AUTO; program(s) used to solve structure: SIR2004 (Burla et al., 2005 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: ORTEP-3 for Windows (Farrugia, 1997 ▶); software used to prepare material for publication: WinGX (Farrugia, 1999 ▶). Crystal structure: contains datablock(s) global, I. DOI: 10.1107/S1600536811036415/ld2024sup1.cif Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811036415/ld2024Isup2.hkl Supplementary material file. DOI: 10.1107/S1600536811036415/ld2024Isup3.cml Additional supplementary materials: crystallographic information; 3D view; checkCIF report
C28H32F(000) = 400
Mr = 368.54Dx = 1.154 Mg m3
Monoclinic, P21/nMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ynCell parameters from 3820 reflections
a = 12.901 (4) Åθ = 3.3–27.5°
b = 5.057 (2) ŵ = 0.06 mm1
c = 16.962 (6) ÅT = 203 K
β = 106.513 (9)°Prism, yellow
V = 1061.0 (7) Å30.25 × 0.13 × 0.1 mm
Z = 2
Rigaku R-AXIS RAPID IP diffractometer1318 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tubeRint = 0.083
graphiteθmax = 27.5°, θmin = 3.3°
Detector resolution: 10 pixels mm-1h = −16→16
ω scansk = −6→6
9469 measured reflectionsl = −22→22
2423 independent reflections
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.081H-atom parameters constrained
wR(F2) = 0.282w = 1/[σ2(Fo2) + (0.1483P)2] where P = (Fo2 + 2Fc2)/3
S = 1.10(Δ/σ)max < 0.001
2423 reflectionsΔρmax = 0.26 e Å3
130 parametersΔρmin = −0.42 e Å3
0 restraints
Geometry. All s.u.'s (except the s.u. in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell s.u.'s are taken into account individually in the estimation of s.u.'s in distances, angles and torsion angles; correlations between s.u.'s in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell s.u.'s is used for estimating s.u.'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 > 2σ(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.
xyzUiso*/Ueq
C10.2359 (2)0.9140 (5)−0.04992 (16)0.0445 (7)
C20.3434 (2)0.8926 (5)−0.01162 (17)0.0475 (7)
H20.39181.0027−0.02860.057*
C30.3853 (2)0.7094 (5)0.05323 (17)0.0492 (7)
H30.46060.70050.07660.059*
C40.32137 (19)0.5464 (5)0.08311 (16)0.0436 (7)
C50.20585 (18)0.5603 (5)0.04493 (15)0.0418 (7)
C60.16283 (19)0.7463 (4)−0.02117 (16)0.0428 (7)
C70.05225 (19)0.7561 (5)−0.05762 (16)0.0457 (7)
H70.0250.8765−0.10080.055*
C8−0.02107 (19)0.5923 (5)−0.03256 (16)0.0429 (7)
C9−0.13335 (19)0.6016 (5)−0.06961 (16)0.0446 (7)
H9−0.16060.722−0.11280.054*
C100.1906 (2)1.0987 (5)−0.12112 (17)0.0501 (7)
H10A0.13951.2188−0.10630.06*
H10B0.14970.9937−0.16830.06*
C110.2731 (2)1.2644 (6)−0.14795 (19)0.0597 (8)
H11A0.3221.1486−0.16580.09*
H11B0.3141.3712−0.10210.09*
H11C0.2361.3789−0.1930.09*
C120.36829 (19)0.3617 (5)0.15477 (17)0.0470 (7)
H120.32690.19430.14370.056*
C130.4870 (2)0.2951 (6)0.16758 (19)0.0586 (8)
H13A0.53060.4520.18550.088*
H13B0.49740.23240.11630.088*
H13C0.50880.15830.20910.088*
C140.3535 (2)0.4794 (6)0.23422 (18)0.0586 (8)
H14A0.27720.5090.22760.088*
H14B0.3920.64620.2460.088*
H14C0.38190.35760.27940.088*
U11U22U33U12U13U23
C10.0426 (14)0.0452 (14)0.0469 (16)−0.0039 (11)0.0144 (11)−0.0033 (11)
C20.0424 (14)0.0539 (15)0.0479 (16)−0.0092 (12)0.0153 (12)−0.0026 (12)
C30.0405 (14)0.0496 (15)0.0564 (18)−0.0035 (11)0.0120 (12)−0.0034 (12)
C40.0399 (13)0.0459 (14)0.0436 (15)−0.0020 (11)0.0099 (11)−0.0050 (11)
C50.0383 (13)0.0444 (14)0.0422 (15)−0.0013 (10)0.0108 (10)−0.0027 (11)
C60.0423 (14)0.0432 (14)0.0435 (16)−0.0015 (10)0.0134 (11)−0.0016 (11)
C70.0408 (14)0.0498 (15)0.0461 (16)0.0001 (11)0.0117 (11)0.0043 (11)
C80.0389 (14)0.0438 (14)0.0465 (16)−0.0009 (10)0.0129 (11)−0.0001 (10)
C90.0398 (13)0.0459 (14)0.0454 (16)0.0013 (11)0.0074 (11)0.0048 (11)
C100.0486 (16)0.0493 (15)0.0515 (18)−0.0053 (11)0.0125 (13)0.0029 (12)
C110.0577 (18)0.0622 (18)0.061 (2)−0.0058 (14)0.0193 (15)0.0121 (14)
C120.0398 (14)0.0497 (15)0.0491 (17)−0.0002 (11)0.0087 (11)0.0013 (12)
C130.0436 (16)0.0650 (18)0.063 (2)0.0063 (13)0.0088 (13)0.0059 (14)
C140.0576 (18)0.0711 (19)0.0466 (17)0.0016 (14)0.0140 (13)0.0007 (14)
C1—C21.359 (3)C9—H90.94
C1—C61.451 (3)C10—C111.522 (3)
C1—C101.507 (4)C10—H10A0.98
C2—C31.422 (4)C10—H10B0.98
C2—H20.94C11—H11A0.97
C3—C41.362 (3)C11—H11B0.97
C3—H30.94C11—H11C0.97
C4—C51.448 (3)C12—C131.522 (3)
C4—C121.516 (3)C12—C141.534 (4)
C5—C9i1.394 (3)C12—H120.99
C5—C61.448 (3)C13—H13A0.97
C6—C71.385 (3)C13—H13B0.97
C7—C81.411 (3)C13—H13C0.97
C7—H70.94C14—H14A0.97
C8—C91.406 (3)C14—H14B0.97
C8—C8i1.430 (5)C14—H14C0.97
C9—C5i1.394 (3)
C2—C1—C6117.7 (2)C11—C10—H10A108.3
C2—C1—C10122.9 (2)C1—C10—H10B108.3
C6—C1—C10119.4 (2)C11—C10—H10B108.3
C1—C2—C3122.2 (2)H10A—C10—H10B107.4
C1—C2—H2118.9C10—C11—H11A109.5
C3—C2—H2118.9C10—C11—H11B109.5
C4—C3—C2123.0 (2)H11A—C11—H11B109.5
C4—C3—H3118.5C10—C11—H11C109.5
C2—C3—H3118.5H11A—C11—H11C109.5
C3—C4—C5117.4 (2)H11B—C11—H11C109.5
C3—C4—C12121.7 (2)C4—C12—C13114.0 (2)
C5—C4—C12120.9 (2)C4—C12—C14110.1 (2)
C9i—C5—C6118.2 (2)C13—C12—C14109.4 (2)
C9i—C5—C4122.0 (2)C4—C12—H12107.7
C6—C5—C4119.8 (2)C13—C12—H12107.7
C7—C6—C5119.2 (2)C14—C12—H12107.7
C7—C6—C1120.9 (2)C12—C13—H13A109.5
C5—C6—C1119.8 (2)C12—C13—H13B109.5
C6—C7—C8122.6 (2)H13A—C13—H13B109.5
C6—C7—H7118.7C12—C13—H13C109.5
C8—C7—H7118.7H13A—C13—H13C109.5
C9—C8—C7122.6 (2)H13B—C13—H13C109.5
C9—C8—C8i119.0 (3)C12—C14—H14A109.5
C7—C8—C8i118.4 (3)C12—C14—H14B109.5
C5i—C9—C8122.7 (2)H14A—C14—H14B109.5
C5i—C9—H9118.7C12—C14—H14C109.5
C8—C9—H9118.7H14A—C14—H14C109.5
C1—C10—C11115.9 (2)H14B—C14—H14C109.5
C1—C10—H10A108.3
C6—C1—C2—C31.5 (4)C2—C1—C6—C5−1.4 (4)
C10—C1—C2—C3−177.3 (2)C10—C1—C6—C5177.4 (2)
C1—C2—C3—C4−1.5 (4)C5—C6—C7—C80.4 (4)
C2—C3—C4—C51.3 (4)C1—C6—C7—C8178.6 (2)
C2—C3—C4—C12−177.3 (2)C6—C7—C8—C9−179.9 (2)
C3—C4—C5—C9i178.6 (2)C6—C7—C8—C8i−0.6 (5)
C12—C4—C5—C9i−2.7 (4)C7—C8—C9—C5i179.9 (2)
C3—C4—C5—C6−1.2 (4)C8i—C8—C9—C5i0.7 (5)
C12—C4—C5—C6177.4 (2)C2—C1—C10—C11−0.4 (4)
C9i—C5—C6—C7−0.4 (4)C6—C1—C10—C11−179.2 (2)
C4—C5—C6—C7179.5 (2)C3—C4—C12—C13−22.5 (4)
C9i—C5—C6—C1−178.6 (2)C5—C4—C12—C13158.9 (2)
C4—C5—C6—C11.3 (4)C3—C4—C12—C14100.9 (3)
C2—C1—C6—C7−179.6 (2)C5—C4—C12—C14−77.7 (3)
C10—C1—C6—C7−0.7 (4)
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Authors:  Chitoshi Kitamura; Yasushi Abe; Takuya Ohara; Akio Yoneda; Takeshi Kawase; Takashi Kobayashi; Hiroyoshi Naito; Toshiki Komatsu
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