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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2011 Mar 26;67(Pt 4):o961. doi: 10.1107/S1600536811010245

Ethane-1,2-diyl bis­(benzene­dithio­ate)

Daisuke Abe a, Yuji Sasanuma a,*, Hiroyasu Sato b
PMCID: PMC3099809  PMID: 21754225

Abstract

In the crystal structure, the title compound, C16H14S4, is located on an inversion center and exhibits a gauche+transgauche conformation in the S—CH2—CH2—S bond sequence. The S—C=S plane makes a dihedral angle of 30.63 (17)° with the phenyl ring. An inter­molecular C—H⋯π inter­action is observed.

Related literature

For crystal structures and conformations of related compounds with S—CH2—CH2—S bond sequences, see: for example, Takahashi et al. (1968); Deguire & Brisse (1988); Sasanuma & Watanabe (2006).graphic file with name e-67-0o961-scheme1.jpg

Experimental

Crystal data

  • C16H14S4

  • M r = 334.53

  • Monoclinic, Inline graphic

  • a = 11.5431 (7) Å

  • b = 8.74071 (16) Å

  • c = 8.93720 (16) Å

  • β = 122.3772 (7)°

  • V = 761.54 (5) Å3

  • Z = 2

  • Cu Kα radiation

  • μ = 5.60 mm−1

  • T = 93 K

  • 0.32 × 0.27 × 0.08 mm

Data collection

  • Rigaku R-AXIS RAPID diffractometer

  • Absorption correction: multi-scan (ABSCOR; Higashi, 1995) T min = 0.195, T max = 0.639

  • 8415 measured reflections

  • 1389 independent reflections

  • 1292 reflections with F 2 > 2σ(F 2)

  • R int = 0.054

Refinement

  • R[F 2 > 2σ(F 2)] = 0.030

  • wR(F 2) = 0.079

  • S = 1.14

  • 1389 reflections

  • 91 parameters

  • H-atom parameters constrained

  • Δρmax = 0.31 e Å−3

  • Δρmin = −0.39 e Å−3

Data collection: PROCESS-AUTO (Rigaku, 1998); cell refinement: PROCESS-AUTO; data reduction: CrystalStructure (Rigaku Americas & Rigaku, 2007); program(s) used to solve structure: SIR2004 (Burla et al., 2005); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: ORTEPII (Johnson, 1976); software used to prepare material for publication: CrystalStructure.

Supplementary Material

Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536811010245/is2686sup1.cif

e-67-0o961-sup1.cif (13.9KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536811010245/is2686Isup2.hkl

e-67-0o961-Isup2.hkl (68.6KB, hkl)

Additional supplementary materials: crystallographic information; 3D view; checkCIF report

Table 1. Hydrogen-bond geometry (Å, °).

Cg1 is the centroid of the C1–C6 phenyl ring.

D—H⋯A D—H H⋯A DA D—H⋯A
C8—H8ACg1i 0.99 2.65 3.451 (1) 138

Symmetry code: (i) Inline graphic.

Acknowledgments

This study was partly supported by a Grant-in-Aid for Scientific Research (C) (22550190) from the Japan Society for the Promotion of Science.

supplementary crystallographic information

Comment

The S—CH2—CH2—S part of crystallized poly(ethylene sulfide) (PES, [–CH2CH2S–]x) lies in the gauche+transgauche- (g+tg-) conformation (Takahashi et al., 1968); the two S—C bonds are in opposite gauche states, and dipole moments are formed along bisectors of the C—S—C angles. The dipole–dipole interaction was suggested to be the source of its high melting point (215–220 °C) in comparison with that (66–69 °C) of poly(ethylene oxide), [–CH2CH2O–]x (Sasanuma & Watanabe, 2006). Therefore, poly(thioethylenethioterephthaloyl) ([–SCH2CH2SCOC6H4CO–]x) and poly(thioethylenethiodithioterephthaloyl) ([–SCH2CH2SCSC6H4CS–]x), having the same S—CH2—CH2—S bond sequence as PES, are expected to be superior in some physical properties to their homologous polyester, poly(ethylene terephthalate) ([–OCH2CH2OCOC6H4CO–]x). Crystal conformations of polymers are requisite to derive their configurational properties and thermodynamic quantities. Because a polymer tends to have a crystal conformation similar to that of its small model compounds, the models provide the physicochemical information on the polymer. The crystal structure of 1,2-bis(benzoylthio)ethane (BBTE, C6H5C(=O)SCH2CH2SC(=O)C6H5), a model compound of poly(thioethylenethioterephthaloyl), was determined already (Deguire & Brisse, 1988); its S—CH2—CH2—S part also lies in the g+tg- state. We have investigated structure-property relationships of the above-mentioned polyester, polythioester, and polydithioester. As part of the work, this study has dealt with 1,2-bis(dithiobenzoyl)ethane (BDTBE, C6H5C(=S)SCH2CH2SC(=S)C6H5), a model compounds of poly(thioethylenethiodithioterephthaloyl); the crystal structure has been determined and compared with those of BBTE and PES.

Figure 1 shows the molecular structure of BDTBE. Its S—CH2—CH2—S bond sequence adopts the g+tg- conformation, as found for PES and BBTE. The g+tg- conformation renders the two phenyl rings parallel to each other; however, this is partly because the BDTBE molecule is located on the center of symmetry. The C6H5—C(=O)—S part of BBTE is essentially coplanar, whereas the C=S bond of BDTBE is out of the phenyl plane; the S–C═S plane makes a dihedral angle of 30.63 (17)° with the phenyl ring. This is probably due to the van der Waals radius (1.80 Å) of sulfur larger than that (1.52 Å) of oxygen.

The BBTE crystal seems to include intermolecular π–π interactions of a near vertical type (Deguire & Brisse, 1988). In addition, dipole moments, formed close to the O=C bonds, are either parallel or antiparallel to one another. The dipole-dipole interactions are known to stabilize the crystal structure (Sasanuma & Watanabe, 2006). On the other hand, Figure 2 shows that the C=S bonds of BDTBE do not have such clear orientations, because the small difference in electronegativity between C and S little polarizes the C=S bond. In the BDTBE crystal, instead, C—H···π interactions appear to exist between C8—H8A bond and its neighboring phenyl (Ph) ring, and the H···Ph spacing can be estimated to be 2.65 Å.

Experimental

Benzoyl chloride (19.5 g) was added dropwise into 1,2-ethanedithiol (6.2 g) and pyridine (11 ml) in a four-neck flask equipped with a mechanical stirrer and a reflux condenser, and the mixture was stirred at 0 °C for 30 m and, furthermore, at room temperature overnight. The reaction mixture was subjected to extraction with water and ether. The organic layer was washed three times with 8% sodium hydrogen carbonate solution, dried overnight over anhydrous magnesium sulfate, filtrated, and condensed on a rotary evaporator. The residue was recrystallized twice from ethanol and dried under reduced pressure. 1,2-Bis(benzoylthio)ethane (1.5 g) thus prepared, Lawesson's reagent (2.5 g), and toluene (10 ml) were mixed and refluxed for 5 h. The reaction mixture was condensed, dissolved in a mixed solvent (15 ml) of toluene and n-hexane (volume ratio 1:3), and fractionated by a silica-gel column chromatograph. The reddish fraction was collected, condensed, recrystallized twice from ethanol, and dried in vacuo.

Crystals for X-ray diffraction were prepared by slow evaporation of a dimethyl sulfoxide solution. Then, the solution was kept in an open vessel so that water vapor, a poor solvent, would be immixed and hasten the crystallization.

Refinement

All C—H hydrogen atoms were geometrically positioned with C—H = 0.95 and 0.99 Å for the aromatic and methylene groups respectively, and refined as riding by Uiso(H) = 1.2Ueq(C).

Figures

Fig. 1.

Fig. 1.

Molecular structure of 1,2-bis(dithiobenzoyl)ethane (BDTBE). Displacement ellipsoids are drawn at the 50% probability level. The asterisk corresponds to symmetry code -x, -y + 1, -z.

Fig. 2.

Fig. 2.

Packing diagram of BDTBE, viewed down (a) the b axis and (b) the c axis. Displacement ellipsoids are drawn at the 50% probability level. The dotted lines represent C–H···π interactions.

Crystal data

C16H14S4 F(000) = 348.00
Mr = 334.53 Dx = 1.459 Mg m3
Monoclinic, P21/c Cu Kα radiation, λ = 1.54187 Å
Hall symbol: -P 2ybc Cell parameters from 7723 reflections
a = 11.5431 (7) Å θ = 4.5–68.2°
b = 8.74071 (16) Å µ = 5.60 mm1
c = 8.93720 (16) Å T = 93 K
β = 122.3772 (7)° Prism, orange
V = 761.54 (5) Å3 0.32 × 0.27 × 0.08 mm
Z = 2

Data collection

Rigaku R-AXIS RAPID diffractometer 1292 reflections with F2 > 2σ(F2)
Detector resolution: 10.00 pixels mm-1 Rint = 0.054
ω scans θmax = 68.2°
Absorption correction: multi-scan (ABSCOR; Higashi, 1995) h = −13→13
Tmin = 0.195, Tmax = 0.639 k = −10→10
8415 measured reflections l = −10→10
1389 independent reflections

Refinement

Refinement on F2 Secondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.030 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.079 H-atom parameters constrained
S = 1.14 w = 1/[σ2(Fo2) + (0.0329P)2 + 0.4332P] where P = (Fo2 + 2Fc2)/3
1389 reflections (Δ/σ)max < 0.001
91 parameters Δρmax = 0.31 e Å3
0 restraints Δρmin = −0.39 e Å3
Primary atom site location: structure-invariant direct methods

Special details

Geometry. All e.s.d.'s (except that 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 was performed with all reflections. The weighted R-factor (wR) and goodness of fit (S) are based on F2, while the R-factor on F. The threshold expression of F2 > 2.0 σ(F2) was used only for calculating R-factor.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2)

x y z Uiso*/Ueq
S1 0.27738 (4) 0.43962 (5) 0.38957 (6) 0.01677 (15)
S2 0.03137 (4) 0.26716 (5) 0.11103 (6) 0.01529 (15)
C1 0.26047 (17) 0.1259 (2) 0.3631 (2) 0.0107 (3)
C2 0.35523 (17) 0.1069 (2) 0.5448 (2) 0.0132 (4)
C3 0.41019 (18) −0.0366 (2) 0.6127 (2) 0.0154 (4)
C4 0.37290 (18) −0.1615 (2) 0.4996 (2) 0.0174 (4)
C5 0.28006 (18) −0.1431 (2) 0.3188 (2) 0.0157 (4)
C6 0.22359 (18) −0.0005 (2) 0.2505 (2) 0.0134 (3)
C7 0.19836 (18) 0.2793 (2) 0.2954 (2) 0.0116 (3)
C8 −0.02347 (18) 0.4635 (2) 0.0565 (2) 0.0143 (4)
H2 0.3821 0.1924 0.6221 0.016*
H3 0.4733 −0.0493 0.7363 0.019*
H4 0.4109 −0.2594 0.5460 0.021*
H5 0.2552 −0.2285 0.2417 0.019*
H6 0.1596 0.0112 0.1269 0.016*
H8A −0.1248 0.4677 −0.0080 0.017*
H8B 0.0137 0.5229 0.1674 0.017*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
S1 0.0199 (2) 0.0102 (2) 0.0133 (2) −0.00211 (16) 0.0043 (2) −0.00110 (17)
S2 0.0121 (2) 0.0111 (2) 0.0152 (3) 0.00043 (15) 0.0024 (2) 0.00257 (17)
C1 0.0106 (7) 0.0115 (8) 0.0113 (9) 0.0003 (6) 0.0068 (7) 0.0013 (7)
C2 0.0112 (7) 0.0137 (9) 0.0129 (10) −0.0019 (6) 0.0053 (7) 0.0001 (7)
C3 0.0113 (8) 0.0176 (9) 0.0123 (10) −0.0007 (6) 0.0029 (7) 0.0027 (7)
C4 0.0150 (8) 0.0120 (9) 0.0236 (11) 0.0024 (6) 0.0092 (8) 0.0045 (8)
C5 0.0162 (8) 0.0118 (8) 0.0168 (10) −0.0003 (6) 0.0072 (8) −0.0021 (7)
C6 0.0127 (8) 0.0156 (9) 0.0098 (9) −0.0005 (6) 0.0045 (7) 0.0005 (7)
C7 0.0134 (8) 0.0137 (9) 0.0089 (9) 0.0001 (6) 0.0067 (7) 0.0002 (7)
C8 0.0143 (8) 0.0119 (8) 0.0153 (10) 0.0050 (6) 0.0070 (8) 0.0039 (7)

Geometric parameters (Å, °)

S1—C7 1.6376 (17) C5—C6 1.387 (2)
S2—C7 1.7436 (15) C8—C8i 1.519 (3)
S2—C8 1.8033 (17) C2—H2 0.950
C1—C2 1.400 (2) C3—H3 0.950
C1—C6 1.399 (2) C4—H4 0.950
C1—C7 1.488 (2) C5—H5 0.950
C2—C3 1.390 (2) C6—H6 0.950
C3—C4 1.389 (2) C8—H8A 0.990
C4—C5 1.390 (2) C8—H8B 0.990
S1···H4ii 2.990 H4···S1vi 2.990
C1···H8Aiii 2.866 H4···H2v 2.664
C2···H8Aiii 2.779 H5···H8Avii 2.763
C3···H8Aiii 2.903 H8A···C1viii 2.866
H2···H3iv 2.687 H8A···C2viii 2.779
H2···H4iv 2.664 H8A···C3viii 2.903
H3···H2v 2.687 H8A···H5vii 2.763
C7—S2—C8 104.35 (7) C3—C2—H2 119.9
C2—C1—C6 119.24 (15) C2—C3—H3 120.0
C2—C1—C7 119.06 (16) C4—C3—H3 120.0
C6—C1—C7 121.67 (14) C3—C4—H4 120.0
C1—C2—C3 120.25 (17) C5—C4—H4 120.0
C2—C3—C4 120.03 (16) C4—C5—H5 119.9
C3—C4—C5 120.03 (16) C6—C5—H5 119.9
C4—C5—C6 120.22 (17) C1—C6—H6 119.9
C1—C6—C5 120.22 (16) C5—C6—H6 119.9
S1—C7—S2 124.57 (10) S2—C8—H8A 109.1
S1—C7—C1 123.21 (11) S2—C8—H8B 109.1
S2—C7—C1 112.18 (11) C8i—C8—H8A 109.1
S2—C8—C8i 112.39 (16) C8i—C8—H8B 109.1
C1—C2—H2 119.9 H8A—C8—H8B 107.9
C7—S2—C8—C8i 83.65 (14) C6—C1—C7—S1 −152.1 (2)
C8—S2—C7—S1 0.8 (2) C6—C1—C7—S2 30.0 (3)
C8—S2—C7—C1 178.65 (18) C7—C1—C6—C5 −177.9 (2)
C2—C1—C6—C5 0.3 (3) C1—C2—C3—C4 1.1 (3)
C6—C1—C2—C3 −1.0 (3) C2—C3—C4—C5 −0.3 (3)
C2—C1—C7—S1 29.7 (3) C3—C4—C5—C6 −0.4 (3)
C2—C1—C7—S2 −148.13 (18) C4—C5—C6—C1 0.5 (3)
C7—C1—C2—C3 177.1 (2)

Symmetry codes: (i) −x, −y+1, −z; (ii) x, y+1, z; (iii) −x, y−1/2, −z+1/2; (iv) −x+1, y+1/2, −z+3/2; (v) −x+1, y−1/2, −z+3/2; (vi) x, y−1, z; (vii) −x, −y, −z; (viii) −x, y+1/2, −z+1/2.

Hydrogen-bond geometry (Å, °)

Cg1 is the centroid of the C1–C6 phenyl ring.
D—H···A D—H H···A D···A D—H···A
C8—H8A···Cg1viii 0.99 2.65 3.451 (1) 138

Symmetry codes: (viii) −x, y+1/2, −z+1/2.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: IS2686).

References

  1. Burla, M. C., Caliandro, R., Camalli, M., Carrozzini, B., Cascarano, G. L., De Caro, L., Giacovazzo, C., Polidori, G. & Spagna, R. (2005). J. Appl. Cryst. 38, 381–388.
  2. Deguire, S. & Brisse, F. (1988). Can. J. Chem. 66, 341–347.
  3. Higashi, T. (1995). ABSCOR. Rigaku Corporation, Tokyo, Japan.
  4. Johnson, C. K. (1976). ORTEPII. Report ORNL-5138. Oak Ridge National Laboratory, Tennessee, USA.
  5. Rigaku (1998). PROCESS-AUTO. Rigaku Corporation, Tokyo, Japan.
  6. Rigaku Americas & Rigaku (2007). CrystalStructure Rigaku Americas, The Woodlands, Texas, USA, and Rigaku Corporation, Tokyo, Japan.
  7. Sasanuma, Y. & Watanabe, A. (2006). Macromolecules, 39, 1646–1656.
  8. Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
  9. Takahashi, Y., Tadokoro, H. & Chatani, Y. (1968). J. Macromol. Sci. Phys. B2, 361–367.

Associated Data

This section collects any data citations, data availability statements, or supplementary materials included in this article.

Supplementary Materials

Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536811010245/is2686sup1.cif

e-67-0o961-sup1.cif (13.9KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536811010245/is2686Isup2.hkl

e-67-0o961-Isup2.hkl (68.6KB, hkl)

Additional supplementary materials: crystallographic information; 3D view; checkCIF report


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