Literature DB >> 21583868

5-Isopropyl-idene-1,3-dithiolo[4,5-d][1,3]dithiole-2-thione.

Masaaki Tomura, Yoshiro Yamashita.   

Abstract

The title compound, C(7)H(6)S(5), contains a 5-yl-idene-1,3-dithiolo[4,5-d][1,3]dithiole-2-thione framework, which is an important synthetic precursor of multi-dimensional organic superconductors and conductors. The mol-ecular framework is planar with an r.m.s. deviation of 0.012 Å for the non-H atoms. In the crystal structure, mol-ecules are linked by short inter-molecular S⋯S inter-actions [3.501 (5) and 3.581 (4) Å], constructing a zigzag mol-ecular tape network along the c axis.

Entities:  

Year:  2009        PMID: 21583868      PMCID: PMC2977732          DOI: 10.1107/S160053680901335X

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


Related literature

For general background, see: Williams et al. (1992 ▶); Ishiguro et al. (1998 ▶). For the synthesis of the title compound, see: Misaki et al. (1992 ▶). For related structures with a 5-yl­idene-1,3-dithiolo[4,5-d][1,3]dithiole-2-thione framework, see: Bryce et al. (2000 ▶); Hock et al. (2002 ▶); Beck et al. (2006 ▶). For bond-length data, see: Allen et al. (1987 ▶). For values of van der Waals radii, see: Bondi (1964 ▶). For a description of the Cambridge Structural Database, see: Allen (2002 ▶).

Experimental

Crystal data

C7H6S5 M = 250.47 Triclinic, a = 7.082 (6) Å b = 7.126 (6) Å c = 10.534 (10) Å α = 86.12 (3)° β = 84.77 (3)° γ = 71.95 (2)° V = 502.9 (8) Å3 Z = 2 Mo Kα radiation μ = 1.09 mm−1 T = 291 K 0.09 × 0.02 × 0.01 mm

Data collection

Rigaku/MSC Mercury CCD diffractometer Absorption correction: none 4550 measured reflections 2643 independent reflections 785 reflections with I > 2σ(I) R int = 0.117

Refinement

R[F 2 > 2σ(F 2)] = 0.072 wR(F 2) = 0.246 S = 0.84 2643 reflections 112 parameters H-atom parameters constrained Δρmax = 0.46 e Å−3 Δρmin = −0.50 e Å−3 Data collection: CrystalClear (Rigaku/MSC, 2006 ▶); cell refinement: CrystalClear; data reduction: TEXSAN (Rigaku/MSC, 2004 ▶); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: PLATON (Spek, 2009 ▶) and Mercury (Macrae et al., 2006 ▶); software used to prepare material for publication: SHELXL97. Crystal structure: contains datablocks global, I. DOI: 10.1107/S160053680901335X/hg2498sup1.cif Structure factors: contains datablocks I. DOI: 10.1107/S160053680901335X/hg2498Isup2.hkl Additional supplementary materials: crystallographic information; 3D view; checkCIF report
C7H6S5Z = 2
Mr = 250.47F(000) = 256
Triclinic, P1Dx = 1.654 Mg m3
Hall symbol: -P 1Mo Kα radiation, λ = 0.71070 Å
a = 7.082 (6) ÅCell parameters from 843 reflections
b = 7.126 (6) Åθ = 3.0–29.7°
c = 10.534 (10) ŵ = 1.09 mm1
α = 86.12 (3)°T = 291 K
β = 84.77 (3)°Needle, brown
γ = 71.95 (2)°0.09 × 0.02 × 0.01 mm
V = 502.9 (8) Å3
Rigaku/MSC Mercury CCD diffractometer785 reflections with I > 2σ(I)
Radiation source: Rotating AnodeRint = 0.117
Confocalθmax = 31.1°, θmin = 3.0°
Detector resolution: 14.63 pixels mm-1h = −9→9
φ and ω scansk = −10→10
4550 measured reflectionsl = −10→15
2643 independent reflections
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.072H-atom parameters constrained
wR(F2) = 0.246w = 1/[σ2(Fo2) + (0.0747P)2] where P = (Fo2 + 2Fc2)/3
S = 0.84(Δ/σ)max < 0.001
2643 reflectionsΔρmax = 0.46 e Å3
112 parametersΔρmin = −0.50 e Å3
0 restraintsExtinction correction: SHELXL97 (Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methodsExtinction coefficient: 0.003 (3)
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
S10.1573 (3)1.3556 (3)−0.12379 (19)0.0502 (6)
S20.2864 (3)0.9827 (3)−0.25144 (18)0.0496 (6)
S30.1902 (3)1.1364 (3)0.13884 (18)0.0452 (6)
S40.3259 (3)0.7524 (3)0.00739 (18)0.0434 (6)
S50.1908 (4)1.3598 (4)−0.4066 (2)0.0710 (9)
C10.2089 (11)1.2401 (12)−0.2662 (7)0.048 (2)
C20.2080 (10)1.1425 (11)−0.0257 (7)0.0427 (19)
C30.2706 (10)0.8745 (11)0.1547 (7)0.0407 (18)
C40.2678 (9)0.9729 (12)−0.0871 (7)0.0385 (17)
C50.2896 (10)0.7741 (12)0.2681 (8)0.045 (2)
C60.2430 (11)0.8811 (12)0.3900 (7)0.056 (2)
H6A0.36020.84720.43650.084*
H6B0.13950.84390.44050.084*
H6C0.19941.02100.37110.084*
C70.3596 (11)0.5529 (11)0.2761 (7)0.049 (2)
H7A0.38180.50360.19170.073*
H7B0.26030.50560.32390.073*
H7C0.48160.50780.31790.073*
U11U22U33U12U13U23
S10.0512 (13)0.0409 (13)0.0522 (14)−0.0080 (10)−0.0035 (10)0.0126 (10)
S20.0551 (14)0.0473 (14)0.0417 (12)−0.0113 (11)0.0001 (9)0.0038 (10)
S30.0519 (13)0.0337 (12)0.0451 (12)−0.0077 (10)0.0010 (9)−0.0006 (9)
S40.0513 (13)0.0308 (12)0.0429 (12)−0.0058 (10)−0.0014 (9)0.0009 (9)
S50.0751 (18)0.078 (2)0.0561 (16)−0.0221 (15)−0.0135 (12)0.0300 (13)
C10.049 (5)0.044 (5)0.047 (5)−0.007 (4)−0.011 (4)0.012 (4)
C20.046 (5)0.031 (5)0.047 (5)−0.008 (4)−0.002 (4)−0.003 (4)
C30.040 (4)0.039 (5)0.040 (4)−0.010 (4)0.004 (3)−0.001 (3)
C40.032 (4)0.038 (4)0.040 (4)−0.004 (3)−0.006 (3)0.006 (3)
C50.039 (4)0.037 (5)0.058 (5)−0.014 (4)0.013 (4)−0.001 (4)
C60.066 (6)0.050 (6)0.051 (5)−0.016 (5)0.002 (4)−0.005 (4)
C70.056 (5)0.039 (5)0.049 (5)−0.016 (4)0.002 (4)0.014 (4)
S1—C11.716 (8)C3—C51.346 (10)
S1—C21.738 (8)C5—C61.496 (10)
S2—C41.723 (7)C5—C71.497 (10)
S2—C11.744 (8)C6—H6A0.9600
S3—C21.725 (8)C6—H6B0.9600
S3—C31.775 (8)C6—H6C0.9600
S4—C41.758 (7)C7—H7A0.9600
S4—C31.783 (7)C7—H7B0.9600
S5—C11.652 (7)C7—H7C0.9600
C2—C41.341 (10)
S1···S1i3.581 (4)S5···S5ii3.501 (5)
C1—S1—C296.7 (4)C3—C5—C6120.7 (8)
C4—S2—C194.9 (4)C3—C5—C7121.2 (7)
C2—S3—C394.4 (3)C6—C5—C7118.1 (7)
C4—S4—C394.3 (4)C5—C6—H6A109.5
S5—C1—S1123.5 (5)C5—C6—H6B109.5
S5—C1—S2122.1 (5)H6A—C6—H6B109.5
S1—C1—S2114.4 (4)C5—C6—H6C109.5
C4—C2—S3119.7 (6)H6A—C6—H6C109.5
C4—C2—S1115.0 (6)H6B—C6—H6C109.5
S3—C2—S1125.3 (5)C5—C7—H7A109.5
C5—C3—S3123.3 (6)C5—C7—H7B109.5
C5—C3—S4122.0 (6)H7A—C7—H7B109.5
S3—C3—S4114.6 (4)C5—C7—H7C109.5
C2—C4—S2118.9 (6)H7A—C7—H7C109.5
C2—C4—S4117.0 (6)H7B—C7—H7C109.5
S2—C4—S4124.1 (5)
C2—S1—C1—S5180.0 (5)S3—C2—C4—S2−179.5 (4)
C2—S1—C1—S2−0.9 (5)S1—C2—C4—S2−0.4 (8)
C4—S2—C1—S5179.9 (5)S3—C2—C4—S4−0.3 (8)
C4—S2—C1—S10.8 (5)S1—C2—C4—S4178.8 (3)
C3—S3—C2—C40.3 (6)C1—S2—C4—C2−0.2 (6)
C3—S3—C2—S1−178.7 (5)C1—S2—C4—S4−179.3 (5)
C1—S1—C2—C40.8 (6)C3—S4—C4—C20.1 (6)
C1—S1—C2—S3179.8 (5)C3—S4—C4—S2179.2 (4)
C2—S3—C3—C5179.6 (7)S3—C3—C5—C6−0.2 (10)
C2—S3—C3—S4−0.2 (4)S4—C3—C5—C6179.7 (5)
C4—S4—C3—C5−179.8 (7)S3—C3—C5—C7−179.5 (5)
C4—S4—C3—S30.1 (4)S4—C3—C5—C70.3 (10)
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