Literature DB >> 22590406

1,4-Bis[4-(tert-butyl-sulfan-yl)phen-yl]buta-1,3-diyne.

Nadine Seidel1, Sebastian Förster, Wilhelm Seichter, Edwin Weber.   

Abstract

The asymmetric unit of the title compound, C(24)H(26)S(2), consits of one half-mol-ecule, which is located on a center of inversion. The two benzene rings are exactly coplanar while the tert-butyl group is oriented nearly perpendicular to the ring plane [C-S-C-C = -81.14 (11)°].

Entities:  

Year:  2012        PMID: 22590406      PMCID: PMC3344644          DOI: 10.1107/S1600536812017710

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


Related literature

For background to this work, see: Pearson & Tour (1997 ▶); Kergueris et al. (1999 ▶). For related structures, see: Kergueris et al. (1999 ▶); Mayor et al. (2003 ▶). For the synthetic procedure, see: van Dijk et al. (2006 ▶). For the unsubstituted 1,4-diphenyl­buta-1,3-diyne, see: Hori et al. (1987 ▶).

Experimental

Crystal data

C24H26S2 M = 378.57 Monoclinic, a = 13.6286 (5) Å b = 6.4269 (2) Å c = 14.1290 (5) Å β = 116.937 (2)° V = 1103.29 (7) Å3 Z = 2 Mo Kα radiation μ = 0.25 mm−1 T = 153 K 0.53 × 0.20 × 0.05 mm

Data collection

Bruker APEXII CCD area-detector diffractometer Absorption correction: multi-scan (SADABS; Sheldrick, 2004 ▶) T min = 0.881, T max = 0.989 11825 measured reflections 3028 independent reflections 2450 reflections with I > 2σ(I) R int = 0.025

Refinement

R[F 2 > 2σ(F 2)] = 0.034 wR(F 2) = 0.091 S = 1.04 3028 reflections 121 parameters H-atom parameters constrained Δρmax = 0.35 e Å−3 Δρmin = −0.20 e Å−3 Data collection: APEX2 (Bruker, 2007 ▶); cell refinement: SAINT (Bruker, 2007 ▶); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: ORTEP-3 (Farrugia, 1997 ▶); software used to prepare material for publication: SHELXTL (Sheldrick, 2008 ▶). Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536812017710/nc2274sup1.cif Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812017710/nc2274Isup2.hkl Supplementary material file. DOI: 10.1107/S1600536812017710/nc2274Isup3.cml Additional supplementary materials: crystallographic information; 3D view; checkCIF report
C24H26S2F(000) = 404
Mr = 378.57Dx = 1.140 Mg m3
Monoclinic, P21/nMo Kα radiation, λ = 0.71073 Å
a = 13.6286 (5) ÅCell parameters from 4805 reflections
b = 6.4269 (2) Åθ = 2.8–30.5°
c = 14.1290 (5) ŵ = 0.25 mm1
β = 116.937 (2)°T = 153 K
V = 1103.29 (7) Å3Plate, colourless
Z = 20.53 × 0.20 × 0.05 mm
Bruker APEXII CCD area-detector diffractometer3028 independent reflections
Radiation source: fine-focus sealed tube2450 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.025
phi and ω scansθmax = 29.4°, θmin = 2.8°
Absorption correction: multi-scan (SADABS; Sheldrick, 2004)h = −17→18
Tmin = 0.881, Tmax = 0.989k = −8→8
11825 measured reflectionsl = −19→17
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.034Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.091H-atom parameters constrained
S = 1.04w = 1/[σ2(Fo2) + (0.0415P)2 + 0.3498P] where P = (Fo2 + 2Fc2)/3
3028 reflections(Δ/σ)max < 0.001
121 parametersΔρmax = 0.35 e Å3
0 restraintsΔρmin = −0.20 e Å3
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.
xyzUiso*/Ueq
S10.93054 (2)0.80456 (5)0.55276 (2)0.02231 (10)
C10.93335 (10)0.62309 (18)0.64857 (9)0.0206 (2)
C20.90994 (11)0.68270 (19)0.73135 (10)0.0250 (3)
H20.88740.82140.73430.030*
C30.91924 (11)0.5417 (2)0.80912 (10)0.0261 (3)
H30.90190.58320.86430.031*
C40.95429 (10)0.33764 (19)0.80637 (10)0.0234 (3)
C50.97762 (11)0.2782 (2)0.72369 (10)0.0257 (3)
H51.00130.14020.72120.031*
C60.96658 (11)0.41878 (19)0.64538 (10)0.0247 (3)
H60.98170.37600.58900.030*
C70.78266 (11)0.8255 (2)0.45814 (11)0.0308 (3)
C80.73566 (15)0.6125 (3)0.41517 (14)0.0523 (5)
H8A0.77860.54820.38310.078*
H8B0.65890.62710.36140.078*
H8C0.73910.52470.47330.078*
C90.78203 (13)0.9643 (3)0.37009 (13)0.0467 (4)
H9A0.70600.98600.31590.070*
H9B0.82410.89720.33780.070*
H9C0.81551.09890.40010.070*
C100.72009 (13)0.9298 (3)0.51159 (14)0.0480 (4)
H10A0.72370.84160.56970.072*
H10B0.64300.94920.45950.072*
H10C0.75341.06530.53990.072*
C110.97122 (11)0.1931 (2)0.88969 (10)0.0259 (3)
C120.98954 (11)0.0698 (2)0.95990 (10)0.0265 (3)
U11U22U33U12U13U23
S10.02344 (15)0.02417 (15)0.02180 (16)0.00002 (11)0.01242 (12)0.00352 (11)
C10.0213 (5)0.0224 (5)0.0181 (6)−0.0005 (4)0.0090 (5)0.0011 (4)
C20.0327 (7)0.0210 (6)0.0255 (6)0.0017 (5)0.0169 (5)0.0000 (5)
C30.0347 (7)0.0264 (6)0.0222 (6)0.0008 (5)0.0173 (5)−0.0011 (5)
C40.0267 (6)0.0230 (6)0.0205 (6)−0.0010 (5)0.0107 (5)0.0013 (4)
C50.0330 (7)0.0218 (6)0.0237 (6)0.0030 (5)0.0141 (5)−0.0002 (5)
C60.0307 (6)0.0257 (6)0.0212 (6)0.0022 (5)0.0148 (5)−0.0005 (5)
C70.0244 (6)0.0385 (7)0.0259 (7)0.0009 (5)0.0083 (5)0.0080 (6)
C80.0453 (9)0.0535 (10)0.0391 (9)−0.0178 (8)0.0026 (8)−0.0021 (8)
C90.0375 (8)0.0616 (11)0.0362 (8)0.0078 (7)0.0125 (7)0.0244 (8)
C100.0305 (8)0.0661 (11)0.0508 (10)0.0153 (8)0.0215 (7)0.0150 (9)
C110.0321 (6)0.0246 (6)0.0235 (6)0.0000 (5)0.0147 (5)−0.0011 (5)
C120.0340 (7)0.0246 (6)0.0246 (6)0.0015 (5)0.0167 (6)−0.0007 (5)
S1—C11.7740 (12)C7—C91.528 (2)
S1—C71.8509 (13)C7—C101.526 (2)
C1—C21.3980 (17)C8—H8A0.9800
C1—C61.3964 (17)C8—H8B0.9800
C2—C31.3852 (17)C8—H8C0.9800
C2—H20.9500C9—H9A0.9800
C3—C41.4022 (17)C9—H9B0.9800
C3—H30.9500C9—H9C0.9800
C4—C51.3957 (17)C10—H10A0.9800
C4—C111.4339 (17)C10—H10B0.9800
C5—C61.3828 (17)C10—H10C0.9800
C5—H50.9500C11—C121.2042 (18)
C6—H60.9500C12—C12i1.370 (3)
C7—C81.517 (2)
C1—S1—C7103.83 (6)C9—C7—S1103.49 (10)
C2—C1—C6119.01 (11)C10—C7—S1110.13 (10)
C2—C1—S1121.60 (9)C7—C8—H8A109.5
C6—C1—S1119.27 (9)C7—C8—H8B109.5
C3—C2—C1120.72 (11)H8A—C8—H8B109.5
C3—C2—H2119.6C7—C8—H8C109.5
C1—C2—H2119.6H8A—C8—H8C109.5
C2—C3—C4119.99 (12)H8B—C8—H8C109.5
C2—C3—H3120.0C7—C9—H9A109.5
C4—C3—H3120.0C7—C9—H9B109.5
C5—C4—C3119.25 (11)H9A—C9—H9B109.5
C5—C4—C11119.79 (11)C7—C9—H9C109.5
C3—C4—C11120.89 (11)H9A—C9—H9C109.5
C6—C5—C4120.49 (11)H9B—C9—H9C109.5
C6—C5—H5119.8C7—C10—H10A109.5
C4—C5—H5119.8C7—C10—H10B109.5
C5—C6—C1120.52 (11)H10A—C10—H10B109.5
C5—C6—H6119.7C7—C10—H10C109.5
C1—C6—H6119.7H10A—C10—H10C109.5
C8—C7—C9110.82 (14)H10B—C10—H10C109.5
C8—C7—C10111.40 (14)C12—C11—C4177.35 (14)
C9—C7—C10110.38 (13)C11—C12—C12i179.74 (18)
C8—C7—S1110.35 (11)
C7—S1—C1—C2−81.14 (11)C11—C4—C5—C6−177.00 (12)
C7—S1—C1—C6103.04 (11)C4—C5—C6—C10.9 (2)
C6—C1—C2—C3−0.12 (19)C2—C1—C6—C5−0.87 (19)
S1—C1—C2—C3−175.95 (10)S1—C1—C6—C5175.06 (10)
C1—C2—C3—C41.1 (2)C1—S1—C7—C8−55.80 (12)
C2—C3—C4—C5−1.11 (19)C1—S1—C7—C9−174.41 (11)
C2—C3—C4—C11175.99 (12)C1—S1—C7—C1067.60 (12)
C3—C4—C5—C60.13 (19)
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