Literature DB >> 21582961

4,6,7,9,10,12-Hexahydro-1,3-dithiolo[4,5-f][1,4,9]oxadithia-cyclo-undecine-2-thione.

Rui-Bin Hou, Bao Li, Bing-Zhu Yin, Li-Xin Wu.   

Abstract

In the title mol-ecule, C(9)H(12)S(5)O, the five-membered ring and attached S atom are essentially coplanar [mean deviation from the mean plane = 0.020 (1) Å]. The two S atoms belonging to the macrocycle deviate from this plane by 1.005 (1) and 1.337 (2) Å. In the crystal, π-π inter-actions link the mol-ecules into centrosymmetric dimers with a short distance of 3.753 (5) Å between the centroids of the five-membered rings.

Entities:  

Year:  2009        PMID: 21582961      PMCID: PMC2969415          DOI: 10.1107/S1600536809024003

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


Related literature

The title compound was prepared according to Chen et al. (2005 ▶). For background literature concerning crown-ether-annulated 1,3-dithiol-2-thione derivatives, see: Hansen et al. (1992 ▶); Trippé et al. (2002 ▶).

Experimental

Crystal data

C9H12OS5 M = 296.49 Triclinic, a = 8.3425 (17) Å b = 8.9611 (18) Å c = 9.820 (2) Å α = 98.10 (3)° β = 106.58 (3)° γ = 112.74 (3)° V = 622.2 (2) Å3 Z = 2 Mo Kα radiation μ = 0.90 mm−1 T = 291 K 0.15 × 0.12 × 0.12 mm

Data collection

Rigaku R-AXIS RAPID diffractometer Absorption correction: multi-scan (ABSCOR; Higashi, 1995 ▶) T min = 0.877, T max = 0.900 6141 measured reflections 2813 independent reflections 2560 reflections with I > 2σ(I) R int = 0.017

Refinement

R[F 2 > 2σ(F 2)] = 0.031 wR(F 2) = 0.106 S = 1.06 2813 reflections 136 parameters H-atom parameters constrained Δρmax = 0.41 e Å−3 Δρmin = −0.36 e Å−3 Data collection: RAPID-AUTO (Rigaku, 1998 ▶); cell refinement: RAPID-AUTO; data reduction: CrystalStructure (Rigaku/MSC, 2002 ▶); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: PLATON (Spek, 2009 ▶); software used to prepare material for publication: SHELXL97. Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536809024003/cv2573sup1.cif Structure factors: contains datablocks I. DOI: 10.1107/S1600536809024003/cv2573Isup2.hkl Additional supplementary materials: crystallographic information; 3D view; checkCIF report
C9H12OS5Z = 2
Mr = 296.49F(000) = 308
Triclinic, P1Dx = 1.583 Mg m3
Hall symbol: -P 1Mo Kα radiation, λ = 0.71073 Å
a = 8.3425 (17) ÅCell parameters from 5678 reflections
b = 8.9611 (18) Åθ = 3.4–27.0°
c = 9.820 (2) ŵ = 0.90 mm1
α = 98.10 (3)°T = 291 K
β = 106.58 (3)°Block, yellow
γ = 112.74 (3)°0.15 × 0.12 × 0.12 mm
V = 622.2 (2) Å3
Rigaku R-AXIS RAPID diffractometer2813 independent reflections
Radiation source: fine-focus sealed tube2560 reflections with I > 2σ(I)
graphiteRint = 0.017
ω scansθmax = 27.5°, θmin = 3.4°
Absorption correction: multi-scan (ABSCOR; Higashi, 1995)h = −10→10
Tmin = 0.877, Tmax = 0.900k = −11→11
6141 measured reflectionsl = −12→12
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.031Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.106H-atom parameters constrained
S = 1.06w = 1/[σ2(Fo2) + (0.0645P)2 + 0.2783P] where P = (Fo2 + 2Fc2)/3
2813 reflections(Δ/σ)max = 0.003
136 parametersΔρmax = 0.41 e Å3
0 restraintsΔρmin = −0.36 e Å3
Experimental. (See detailed section in the paper)
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
C10.3295 (3)0.6916 (3)0.4927 (2)0.0376 (4)
C20.2130 (3)0.8764 (2)0.3463 (2)0.0300 (4)
C30.1113 (3)0.9792 (2)0.3073 (2)0.0354 (4)
H3A0.11941.00510.21610.042*
H3B0.17241.08510.38480.042*
C4−0.2203 (3)0.6799 (3)0.1413 (3)0.0408 (5)
H4A−0.14450.62330.17460.049*
H4B−0.34690.60750.13150.049*
C5−0.2231 (3)0.6956 (3)−0.0092 (3)0.0486 (5)
H5A−0.29750.5852−0.08110.058*
H5B−0.28050.7677−0.03780.058*
C6−0.0193 (3)0.6766 (3)−0.1285 (3)0.0466 (5)
H6A−0.11080.6664−0.22080.056*
H6B−0.04230.5639−0.12110.056*
C70.1742 (3)0.7686 (3)−0.1276 (2)0.0439 (5)
H7A0.19910.8846−0.12290.053*
H7B0.17540.7190−0.22150.053*
C80.4004 (3)0.9279 (2)0.1782 (2)0.0367 (4)
H8A0.53281.00560.22430.044*
H8B0.33420.99200.14430.044*
C90.3363 (2)0.8552 (2)0.2922 (2)0.0294 (4)
O1−0.0377 (2)0.7650 (2)−0.0088 (2)0.0600 (5)
S10.43959 (7)0.73453 (6)0.36855 (5)0.03533 (15)
S20.36763 (14)0.58331 (12)0.60929 (8)0.0708 (3)
S30.17163 (8)0.77394 (7)0.48048 (6)0.03867 (15)
S4−0.13328 (7)0.87314 (7)0.28369 (6)0.04162 (16)
S50.36387 (8)0.77082 (7)0.01819 (6)0.04019 (15)
U11U22U33U12U13U23
C10.0448 (11)0.0454 (11)0.0277 (9)0.0247 (9)0.0138 (8)0.0110 (8)
C20.0293 (8)0.0333 (9)0.0239 (8)0.0121 (7)0.0089 (7)0.0061 (7)
C30.0375 (10)0.0361 (9)0.0347 (10)0.0190 (8)0.0136 (8)0.0087 (8)
C40.0313 (9)0.0420 (10)0.0486 (12)0.0163 (8)0.0140 (9)0.0140 (9)
C50.0318 (10)0.0615 (14)0.0431 (12)0.0164 (10)0.0121 (9)0.0057 (10)
C60.0439 (11)0.0526 (12)0.0361 (11)0.0199 (10)0.0127 (9)0.0023 (9)
C70.0506 (12)0.0565 (13)0.0329 (10)0.0266 (10)0.0214 (9)0.0172 (9)
C80.0388 (10)0.0339 (9)0.0361 (10)0.0107 (8)0.0200 (8)0.0097 (8)
C90.0283 (8)0.0289 (8)0.0276 (9)0.0101 (7)0.0105 (7)0.0059 (7)
O10.0356 (8)0.0692 (11)0.0481 (10)0.0048 (8)0.0198 (7)−0.0146 (8)
S10.0340 (3)0.0422 (3)0.0348 (3)0.0204 (2)0.0152 (2)0.0112 (2)
S20.1147 (7)0.0990 (6)0.0578 (4)0.0820 (6)0.0517 (4)0.0521 (4)
S30.0443 (3)0.0543 (3)0.0322 (3)0.0285 (2)0.0224 (2)0.0188 (2)
S40.0399 (3)0.0544 (3)0.0438 (3)0.0303 (2)0.0214 (2)0.0135 (2)
S50.0468 (3)0.0511 (3)0.0357 (3)0.0300 (2)0.0217 (2)0.0135 (2)
C1—S21.642 (2)C5—H5A0.9700
C1—S11.726 (2)C5—H5B0.9700
C1—S31.726 (2)C6—O11.402 (3)
C2—C91.346 (3)C6—C71.499 (3)
C2—C31.495 (3)C6—H6A0.9700
C2—S31.7471 (19)C6—H6B0.9700
C3—S41.814 (2)C7—S51.796 (2)
C3—H3A0.9700C7—H7A0.9700
C3—H3B0.9700C7—H7B0.9700
C4—C51.498 (3)C8—C91.497 (3)
C4—S41.802 (2)C8—S51.820 (2)
C4—H4A0.9700C8—H8A0.9700
C4—H4B0.9700C8—H8B0.9700
C5—O11.426 (3)C9—S11.747 (2)
S2—C1—S1124.30 (13)O1—C6—H6A109.7
S2—C1—S3123.21 (13)C7—C6—H6A109.7
S1—C1—S3112.49 (12)O1—C6—H6B109.7
C9—C2—C3127.67 (18)C7—C6—H6B109.7
C9—C2—S3115.53 (15)H6A—C6—H6B108.2
C3—C2—S3116.79 (14)C6—C7—S5117.34 (17)
C2—C3—S4112.96 (14)C6—C7—H7A108.0
C2—C3—H3A109.0S5—C7—H7A108.0
S4—C3—H3A109.0C6—C7—H7B108.0
C2—C3—H3B109.0S5—C7—H7B108.0
S4—C3—H3B109.0H7A—C7—H7B107.2
H3A—C3—H3B107.8C9—C8—S5114.07 (14)
C5—C4—S4116.74 (17)C9—C8—H8A108.7
C5—C4—H4A108.1S5—C8—H8A108.7
S4—C4—H4A108.1C9—C8—H8B108.7
C5—C4—H4B108.1S5—C8—H8B108.7
S4—C4—H4B108.1H8A—C8—H8B107.6
H4A—C4—H4B107.3C2—C9—C8127.63 (18)
O1—C5—C4110.55 (19)C2—C9—S1116.14 (15)
O1—C5—H5A109.5C8—C9—S1116.20 (14)
C4—C5—H5A109.5C6—O1—C5113.57 (18)
O1—C5—H5B109.5C1—S1—C997.73 (10)
C4—C5—H5B109.5C1—S3—C298.01 (10)
H5A—C5—H5B108.1C4—S4—C3102.59 (10)
O1—C6—C7109.68 (19)C7—S5—C8103.70 (11)
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