Literature DB >> 21579425

4,6,7,9,10,12,13,15,16,18-Decahydro-1,3-dithiolo[4,5-l][1,4,7,10,15]trioxadithia-cyclo-hepta-decine-2-thione.

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

Abstract

The title compound, C(13)H(20)O(3)S(5), is bis-ected by a crystallographic twofold rotation axis, which relates the two halves of the mol-ecule to one another: one S, one C and one O atom lie on the axis. The thione S atom lies in the plane of the five-membered rings with an r.m.s. deviation of 0.0042 (5) Å. Parts of the 17-membered macrocycle were refined using a two-part disorder model [occupancies of 0.553 (14) and 0.447 (14)]. There are no noteworthy inter-molecular inter-actions.

Entities:  

Year:  2010        PMID: 21579425      PMCID: PMC2979504          DOI: 10.1107/S1600536810016946

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


Related literature

Thia­crown ether annulated 1,3-dithiol-2-thione is a key inter­mediate of the crown ether-bearing redox-active tetra­thia­fulvalene moiety, see: Moore et al. (2000 ▶). For details of the synthesis, see: Chen et al. (2005 ▶). For a related structure, see: Hou et al. (2009 ▶)

Experimental

Crystal data

C13H20O3S5 M = 384.59 Monoclinic, a = 14.040 (3) Å b = 13.616 (3) Å c = 10.004 (2) Å β = 110.89 (3)° V = 1786.6 (6) Å3 Z = 4 Mo Kα radiation μ = 0.65 mm−1 T = 290 K 0.13 × 0.13 × 0.12 mm

Data collection

Rigaku R-AXIS RAPID diffractometer Absorption correction: multi-scan (ABSCOR; Higashi, 1995 ▶) T min = 0.920, T max = 0.926 8683 measured reflections 2054 independent reflections 1795 reflections with I > 2σ(I) R int = 0.022

Refinement

R[F 2 > 2σ(F 2)] = 0.039 wR(F 2) = 0.103 S = 1.05 2054 reflections 116 parameters 31 restraints H-atom parameters constrained Δρmax = 0.38 e Å−3 Δρmin = −0.40 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/S1600536810016946/nk2030sup1.cif Structure factors: contains datablocks I. DOI: 10.1107/S1600536810016946/nk2030Isup2.hkl Additional supplementary materials: crystallographic information; 3D view; checkCIF report
C13H20O3S5F(000) = 808
Mr = 384.59Dx = 1.430 Mg m3
Monoclinic, C2/cMo Kα radiation, λ = 0.71073 Å
Hall symbol: -C 2ycCell parameters from 7120 reflections
a = 14.040 (3) Åθ = 3.0–27.5°
b = 13.616 (3) ŵ = 0.65 mm1
c = 10.004 (2) ÅT = 290 K
β = 110.89 (3)°Block, yellow
V = 1786.6 (6) Å30.13 × 0.13 × 0.12 mm
Z = 4
Rigaku R-AXIS RAPID diffractometer2054 independent reflections
Radiation source: fine-focus sealed tube1795 reflections with I > 2σ(I)
graphiteRint = 0.022
ω scansθmax = 27.5°, θmin = 3.0°
Absorption correction: multi-scan (ABSCOR; Higashi, 1995)h = −18→17
Tmin = 0.920, Tmax = 0.926k = −15→17
8683 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)] = 0.039Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.103H-atom parameters constrained
S = 1.05w = 1/[σ2(Fo2) + (0.0458P)2 + 1.730P] where P = (Fo2 + 2Fc2)/3
2054 reflections(Δ/σ)max < 0.001
116 parametersΔρmax = 0.38 e Å3
31 restraintsΔρmin = −0.40 e Å3
Experimental. (See detailed section in the paper)
Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds 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*/UeqOcc. (<1)
S10.0000−0.12281 (6)0.25000.0692 (3)
S20.05129 (4)0.06857 (4)0.14909 (6)0.04829 (17)
S30.17462 (5)0.26384 (5)0.11969 (8)0.0693 (2)
O10.17749 (17)0.40044 (19)0.3861 (3)0.1067 (8)
O20.00000.5091 (3)0.25000.1381 (16)
C10.0000−0.0016 (2)0.25000.0456 (6)
C20.02260 (13)0.18371 (13)0.2012 (2)0.0390 (4)
C30.04873 (15)0.27043 (15)0.1292 (2)0.0493 (5)
H3A0.04400.32950.18070.059*
H3B−0.00100.27570.03300.059*
C40.25511 (19)0.2730 (2)0.3037 (4)0.0816 (9)
H4A0.22780.23080.35940.098*
H4B0.32210.24810.31380.098*
C50.2672 (2)0.3743 (2)0.3658 (4)0.0896 (10)
H5A0.32380.37580.45640.108*
H5B0.28130.42050.30130.108*
C60.1737 (6)0.4901 (6)0.4396 (11)0.092 (2)0.553 (14)
H6A0.24090.51990.47530.111*0.553 (14)
H6B0.14730.48680.51690.111*0.553 (14)
C70.1044 (10)0.5461 (6)0.3178 (12)0.099 (3)0.553 (14)
H7A0.10040.61260.35010.118*0.553 (14)
H7B0.13510.54970.24510.118*0.553 (14)
C6'0.1649 (8)0.5194 (7)0.3562 (16)0.083 (3)0.447 (14)
H6'10.21300.55490.43600.100*0.447 (14)
H6'20.17850.53560.27030.100*0.447 (14)
C7'0.0574 (11)0.5476 (8)0.3385 (11)0.092 (3)0.447 (14)
H7'10.04590.53330.42660.110*0.447 (14)
H7'20.04910.61780.32190.110*0.447 (14)
U11U22U33U12U13U23
S10.0894 (6)0.0347 (4)0.0982 (7)0.0000.0513 (5)0.000
S20.0524 (3)0.0401 (3)0.0612 (3)0.00140 (19)0.0310 (2)−0.0020 (2)
S30.0700 (4)0.0671 (4)0.0918 (5)−0.0035 (3)0.0543 (4)0.0127 (3)
O10.0793 (14)0.1025 (17)0.142 (2)−0.0370 (13)0.0438 (14)−0.0511 (16)
O20.110 (3)0.067 (2)0.225 (5)0.0000.044 (3)0.000
C10.0432 (13)0.0374 (13)0.0576 (15)0.0000.0199 (12)0.000
C20.0321 (8)0.0354 (9)0.0478 (9)−0.0004 (6)0.0123 (7)0.0006 (7)
C30.0459 (10)0.0444 (10)0.0561 (11)−0.0011 (8)0.0165 (9)0.0090 (9)
C40.0423 (12)0.0699 (17)0.122 (2)−0.0026 (11)0.0168 (14)0.0213 (16)
C50.0518 (15)0.086 (2)0.115 (2)−0.0222 (13)0.0109 (15)0.0036 (18)
C60.109 (5)0.077 (4)0.080 (5)−0.023 (3)0.021 (3)−0.014 (3)
C70.112 (5)0.054 (3)0.126 (5)−0.018 (4)0.038 (5)−0.010 (3)
C6'0.092 (5)0.063 (5)0.100 (7)−0.029 (4)0.043 (5)−0.029 (5)
C7'0.108 (7)0.081 (5)0.094 (5)−0.003 (5)0.045 (5)−0.037 (4)
S1—C11.650 (3)C3—H3B0.9700
S2—C11.7231 (16)C4—C51.497 (4)
S2—C21.7440 (18)C4—H4A0.9700
S3—C41.788 (3)C4—H4B0.9700
S3—C31.806 (2)C5—H5A0.9700
O1—C61.342 (7)C5—H5B0.9700
O1—C51.391 (4)C6—C71.472 (14)
O1—C6'1.645 (12)C6—H6A0.9700
O2—C7'1.095 (11)C6—H6B0.9700
O2—C7'i1.095 (11)C7—H7A0.9700
O2—C71.467 (11)C7—H7B0.9700
O2—C7i1.467 (11)C6'—C7'1.506 (15)
C1—S2i1.7231 (16)C6'—H6'10.9700
C2—C2i1.340 (4)C6'—H6'20.9700
C2—C31.495 (3)C7'—H7'10.9700
C3—H3A0.9700C7'—H7'20.9700
C1—S2—C297.69 (10)O1—C5—H5B109.9
C4—S3—C3102.32 (13)C4—C5—H5B109.9
C6—O1—C5117.2 (4)H5A—C5—H5B108.3
C6—O1—C6'32.8 (4)O1—C6—C7104.4 (8)
C5—O1—C6'105.6 (4)O1—C6—H6A110.9
C7'—O2—C7'i122.7 (13)C7—C6—H6A110.9
C7'—O2—C730.3 (5)O1—C6—H6B110.9
C7'i—O2—C7122.3 (7)C7—C6—H6B110.9
C7'—O2—C7i122.3 (7)H6A—C6—H6B108.9
C7'i—O2—C7i30.3 (5)O2—C7—C6117.5 (8)
C7—O2—C7i139.8 (8)O2—C7—H7A107.9
S1—C1—S2i123.68 (8)C6—C7—H7A107.9
S1—C1—S2123.68 (8)O2—C7—H7B107.9
S2i—C1—S2112.65 (15)C6—C7—H7B107.9
C2i—C2—C3127.72 (11)H7A—C7—H7B107.2
C2i—C2—S2115.95 (6)C7'—C6'—O1108.1 (8)
C3—C2—S2116.30 (14)C7'—C6'—H6'1110.1
C2—C3—S3113.52 (14)O1—C6'—H6'1110.1
C2—C3—H3A108.9C7'—C6'—H6'2110.1
S3—C3—H3A108.9O1—C6'—H6'2110.1
C2—C3—H3B108.9H6'1—C6'—H6'2108.4
S3—C3—H3B108.9O2—C7'—C6'113.0 (9)
H3A—C3—H3B107.7O2—C7'—C7'i28.7 (6)
C5—C4—S3115.3 (2)C6'—C7'—C7'i125.7 (13)
C5—C4—H4A108.4O2—C7'—H7'1109.0
S3—C4—H4A108.4C6'—C7'—H7'1109.0
C5—C4—H4B108.4C7'i—C7'—H7'1118.7
S3—C4—H4B108.4O2—C7'—H7'2109.0
H4A—C4—H4B107.5C6'—C7'—H7'2109.0
O1—C5—C4108.8 (2)C7'i—C7'—H7'280.4
O1—C5—H5A109.9H7'1—C7'—H7'2107.8
C4—C5—H5A109.9
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