Literature DB >> 21578954

2,5-Dichloro-thio-phene 1,1-dioxide.

Jonathan B Briggs1, Wenling Jia, Mikaël D Jazdzyk, Glen P Miller.   

Abstract

The complete mol-ecule of the title compound, C(4)H(2)Cl(2)O(2)S, is generated by crystallographic twofold symmetry, with the S atom lying on the rotation axis. In the crystal, the molecules are linked by C-H⋯O hydrogen bonds..

Entities:  

Year:  2009        PMID: 21578954      PMCID: PMC2972006          DOI: 10.1107/S1600536809050776

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


Related literature

For a related thio­phene-1,1-dioxide structure, see: Douglas et al. (1993 ▶). For the synthetic utility and related applications of thio­phene-1,1-dioxides, see: Moiseev et al. (2006 ▶); Nakayama & Sugihara (1999 ▶); Shul’ts et al. (2003 ▶); Lou et al. (2002 ▶).

Experimental

Crystal data

C4H2Cl2O2S M = 185.02 Monoclinic, a = 7.588 (2) Å b = 10.584 (3) Å c = 8.745 (3) Å β = 90.275 (9)° V = 702.4 (3) Å3 Z = 4 Mo Kα radiation μ = 1.14 mm−1 T = 296 K 0.50 × 0.40 × 0.30 mm

Data collection

Bruker SMART X2S diffractometer Absorption correction: multi-scan (SADABS; Bruker, 2007 ▶) T min = 0.590, T max = 0.726 3352 measured reflections 622 independent reflections 549 reflections with I > 2σ(I) R int = 0.028

Refinement

R[F 2 > 2σ(F 2)] = 0.035 wR(F 2) = 0.094 S = 1.12 622 reflections 42 parameters H-atom parameters constrained Δρmax = 0.21 e Å−3 Δρmin = −0.31 e Å−3 Data collection: GIS (Bruker, 2007 ▶); cell refinement: SAINT (Bruker, 2007 ▶); data reduction: SAINT (Bruker, 2007 ▶); 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: SHELXTL. Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536809050776/fl2274sup1.cif Structure factors: contains datablocks I. DOI: 10.1107/S1600536809050776/fl2274Isup2.hkl Additional supplementary materials: crystallographic information; 3D view; checkCIF report
C4H2Cl2O2SF(000) = 368
Mr = 185.02Dx = 1.750 Mg m3
Monoclinic, C2/cMo Kα radiation, λ = 0.71073 Å
Hall symbol: -C 2ycCell parameters from 1863 reflections
a = 7.588 (2) Åθ = 3.3–24.8°
b = 10.584 (3) ŵ = 1.14 mm1
c = 8.745 (3) ÅT = 296 K
β = 90.275 (9)°Block, colourless
V = 702.4 (3) Å30.50 × 0.40 × 0.30 mm
Z = 4
Bruker SMART X2S diffractometer622 independent reflections
Radiation source: micro-focus sealed tube549 reflections with I > 2σ(I)
doubly curved silicon crystalRint = 0.028
ω scansθmax = 25.0°, θmin = 3.3°
Absorption correction: multi-scan (SADABS; Bruker, 2007)h = −9→8
Tmin = 0.590, Tmax = 0.726k = −12→12
3352 measured reflectionsl = −10→10
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.035Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.094H-atom parameters constrained
S = 1.12w = 1/[σ2(Fo2) + (0.0473P)2 + 0.6008P] where P = (Fo2 + 2Fc2)/3
622 reflections(Δ/σ)max = 0.013
42 parametersΔρmax = 0.21 e Å3
0 restraintsΔρmin = −0.31 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
Cl10.32276 (10)0.08665 (9)0.07774 (10)0.0906 (4)
S10.00000.15554 (8)0.25000.0529 (3)
O1−0.0844 (3)0.2242 (2)0.1299 (2)0.0779 (6)
C10.1415 (3)0.0379 (3)0.1743 (3)0.0582 (6)
C20.0827 (4)−0.0754 (3)0.2059 (3)0.0677 (8)
H20.1398−0.14900.17570.081*
U11U22U33U12U13U23
Cl10.0634 (5)0.1157 (8)0.0932 (6)0.0154 (4)0.0365 (4)0.0078 (5)
S10.0513 (5)0.0506 (5)0.0570 (5)0.0000.0174 (4)0.000
O10.0812 (13)0.0728 (12)0.0799 (13)0.0258 (11)0.0188 (10)0.0181 (10)
C10.0518 (14)0.0674 (15)0.0553 (14)0.0134 (12)0.0115 (11)0.0005 (12)
C20.0788 (19)0.0587 (15)0.0657 (17)0.0167 (14)0.0042 (14)−0.0020 (13)
Cl1—C11.698 (3)S1—C1i1.774 (2)
S1—O1i1.427 (2)C1—C21.310 (4)
S1—O11.427 (2)C2—C2i1.476 (6)
S1—C11.774 (2)C2—H20.9300
O1i—S1—O1118.8 (2)C2—C1—Cl1131.4 (2)
O1i—S1—C1111.19 (13)C2—C1—S1110.9 (2)
O1—S1—C1110.68 (12)Cl1—C1—S1117.74 (16)
O1i—S1—C1i110.68 (12)C1—C2—C2i113.68 (16)
O1—S1—C1i111.19 (13)C1—C2—H2123.2
C1—S1—C1i90.87 (18)C2i—C2—H2123.2
D—H···AD—HH···AD···AD—H···A
C2—H2···O1ii0.932.523.367 (4)152
X···Yπ···π
C1···C24.137 (4)
Table 1

Hydrogen-bond geometry (Å, °)

D—H⋯A D—HH⋯A DA D—H⋯A
C2—H2⋯O1i 0.932.523.367 (4)152

Symmetry code: (i) .

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