Literature DB >> 21580015

Bis[2-(1,3-benzothia-zol-2-ylsulfan-yl)eth-yl] ether.

Hui-Guo Chen, Xiao-Feng Li, Yan An, Li-Hui Yao, Wei-Sheng Liu.   

Abstract

The complete molecule of title compound, C(18)H(16)N(2)OS(4), is generated by crystallographic twofold symmetry, with the O atom lying on the rotation axis. The dihedral angle between the ring systems is 80.91 (2)°. In the crystal, adjacent mol-ecules are connected through π-π stacking inter-actions [centroid-centroid distance = 3.882 (2) Å], forming a three-dimensional network.

Entities:  

Year:  2009        PMID: 21580015      PMCID: PMC2980199          DOI: 10.1107/S1600536809052301

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


Related literature

For coordination polymers in supra­molecular chemistry and crystal engineering, see: Robinson & Zaworotko (1995 ▶); Yaghi & Li (1996 ▶); Fujita et al. (1995 ▶); Tong et al. (2000 ▶); Bu et al. (2003 ▶); Long et al. (2004 ▶); Massue et al. (2007 ▶); Zou et al. (2004 ▶).

Experimental

Crystal data

C18H16N2OS4 M = 404.57 Monoclinic, a = 24.617 (3) Å b = 4.7085 (3) Å c = 17.7866 (15) Å β = 116.571 (13)° V = 1843.9 (3) Å3 Z = 4 Cu Kα radiation μ = 4.81 mm−1 T = 293 K 0.18 × 0.15 × 0.07 mm

Data collection

Oxford Diffraction Xcalibur Sapphire3 diffractometer Absorption correction: multi-scan (CrysAlis RED; Oxford Diffraction, 2005 ▶) T min = 0.765, T max = 1.000 2930 measured reflections 1682 independent reflections 1353 reflections with I > 2σ(I) R int = 0.020

Refinement

R[F 2 > 2σ(F 2)] = 0.043 wR(F 2) = 0.129 S = 1.05 1682 reflections 114 parameters H-atom parameters constrained Δρmax = 0.27 e Å−3 Δρmin = −0.25 e Å−3 Data collection: CrysAlis CCD (Oxford Diffraction, 2005 ▶); cell refinement: CrysAlis CCD; data reduction: CrysAlis RED (Oxford Diffraction, 2005 ▶); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: SHELXTL (Sheldrick, 2008 ▶); software used to prepare material for publication: OLEX2 (Dolomanov et al., 2009 ▶). Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536809052301/ng2684sup1.cif Structure factors: contains datablocks I. DOI: 10.1107/S1600536809052301/ng2684Isup2.hkl Additional supplementary materials: crystallographic information; 3D view; checkCIF report
C18H16N2OS4F(000) = 840
Mr = 404.57Dx = 1.457 Mg m3
Monoclinic, C2/cCu Kα radiation, λ = 1.54178 Å
Hall symbol: -C 2ycCell parameters from 1595 reflections
a = 24.617 (3) Åθ = 2.8–68.1°
b = 4.7085 (3) ŵ = 4.81 mm1
c = 17.7866 (15) ÅT = 293 K
β = 116.571 (13)°Block, colourless
V = 1843.9 (3) Å30.18 × 0.15 × 0.07 mm
Z = 4
Oxford Diffraction Xcalibur Sapphire3 diffractometer1682 independent reflections
Radiation source: Enhance (Cu) X-ray Source1353 reflections with I > 2σ(I)
graphiteRint = 0.020
Detector resolution: 16.0855 pixels mm-1θmax = 68.1°, θmin = 2.8°
ω scansh = −29→25
Absorption correction: multi-scan (CrysAlis RED; Oxford Diffraction, 2005)k = −5→3
Tmin = 0.765, Tmax = 1.000l = −21→19
2930 measured reflections
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) = 0.129H-atom parameters constrained
S = 1.05w = 1/[σ2(Fo2) + (0.0876P)2] where P = (Fo2 + 2Fc2)/3
1682 reflections(Δ/σ)max = 0.001
114 parametersΔρmax = 0.27 e Å3
0 restraintsΔρmin = −0.25 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
C10.17154 (13)0.1689 (5)1.11310 (16)0.0505 (6)
C20.18584 (15)−0.0249 (6)1.17798 (17)0.0608 (7)
H20.2256−0.08601.20980.073*
C30.13924 (18)−0.1235 (7)1.1936 (2)0.0701 (8)
H30.1474−0.25681.23590.084*
C40.08011 (16)−0.0269 (8)1.1470 (2)0.0702 (8)
H40.0494−0.09541.15910.084*
C50.06625 (15)0.1676 (6)1.0837 (2)0.0614 (7)
H50.02660.23281.05340.074*
C60.11236 (12)0.2665 (6)1.06519 (15)0.0489 (6)
C70.15597 (12)0.4948 (6)0.99910 (14)0.0483 (6)
C80.09486 (13)0.8627 (6)0.86818 (16)0.0532 (6)
H8C0.07910.91990.90700.064*
H8B0.09951.03230.84060.064*
C90.05001 (13)0.6678 (5)0.80325 (17)0.0552 (6)
H9A0.06830.57690.77120.066*
H9B0.03700.52150.83000.066*
N10.10483 (10)0.4522 (5)1.00023 (13)0.0507 (5)
S10.21965 (3)0.32443 (16)1.07717 (4)0.0560 (2)
S20.16852 (3)0.69930 (17)0.92661 (4)0.0592 (3)
O10.00000.8363 (5)0.75000.0501 (6)
U11U22U33U12U13U23
C10.0535 (14)0.0516 (13)0.0422 (12)−0.0026 (11)0.0176 (11)−0.0037 (10)
C20.0671 (18)0.0625 (16)0.0465 (14)0.0052 (13)0.0197 (13)0.0058 (12)
C30.094 (2)0.0659 (17)0.0546 (16)−0.0017 (16)0.0364 (17)0.0077 (13)
C40.081 (2)0.076 (2)0.0661 (18)−0.0114 (16)0.0442 (17)−0.0024 (15)
C50.0579 (16)0.0686 (18)0.0606 (17)−0.0045 (13)0.0290 (14)−0.0061 (13)
C60.0530 (15)0.0504 (13)0.0395 (12)−0.0021 (11)0.0171 (11)−0.0063 (10)
C70.0454 (13)0.0524 (13)0.0387 (11)−0.0023 (10)0.0112 (10)−0.0007 (10)
C80.0561 (15)0.0484 (13)0.0442 (13)0.0012 (11)0.0127 (11)0.0024 (10)
C90.0528 (15)0.0482 (13)0.0482 (13)0.0051 (11)0.0078 (12)−0.0003 (11)
N10.0460 (11)0.0559 (12)0.0427 (10)−0.0030 (9)0.0132 (9)−0.0023 (9)
S10.0438 (4)0.0679 (5)0.0484 (4)0.0033 (3)0.0136 (3)0.0090 (3)
S20.0450 (4)0.0713 (5)0.0519 (4)−0.0050 (3)0.0132 (3)0.0131 (3)
O10.0485 (14)0.0462 (13)0.0436 (12)0.0000.0099 (11)0.000
C1—C21.387 (4)C7—N11.284 (4)
C1—C61.396 (4)C7—S21.744 (3)
C1—S11.739 (3)C7—S11.755 (3)
C2—C31.376 (5)C8—C91.501 (4)
C2—H20.9300C8—S21.810 (3)
C3—C41.390 (5)C8—H8C0.9700
C3—H30.9300C8—H8B0.9700
C4—C51.372 (5)C9—O11.414 (3)
C4—H40.9300C9—H9A0.9700
C5—C61.395 (4)C9—H9B0.9700
C5—H50.9300O1—C9i1.414 (3)
C6—N11.394 (4)
C2—C1—C6122.1 (3)N1—C7—S1116.8 (2)
C2—C1—S1128.4 (2)S2—C7—S1116.50 (15)
C6—C1—S1109.5 (2)C9—C8—S2112.65 (19)
C3—C2—C1117.7 (3)C9—C8—H8C109.1
C3—C2—H2121.1S2—C8—H8C109.1
C1—C2—H2121.1C9—C8—H8B109.1
C2—C3—C4121.0 (3)S2—C8—H8B109.1
C2—C3—H3119.5H8C—C8—H8B107.8
C4—C3—H3119.5O1—C9—C8107.0 (2)
C5—C4—C3121.1 (3)O1—C9—H9A110.3
C5—C4—H4119.4C8—C9—H9A110.3
C3—C4—H4119.4O1—C9—H9B110.3
C4—C5—C6119.1 (3)C8—C9—H9B110.3
C4—C5—H5120.4H9A—C9—H9B108.6
C6—C5—H5120.4C7—N1—C6110.1 (2)
N1—C6—C5125.7 (2)C1—S1—C788.23 (13)
N1—C6—C1115.3 (2)C7—S2—C8101.30 (13)
C5—C6—C1118.9 (3)C9—O1—C9i111.7 (3)
N1—C7—S2126.7 (2)
D—H···AD—HH···AD···AD—H···A
C4—H4···O1ii0.932.713.358 (3)128
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