Literature DB >> 21837068

Bis[(1-methyl-1H-tetra-zol-5-yl)sulfan-yl]ethane.

Chun-Rong Li, Tao Chen, Zheng-Qiang Xia.   

Abstract

The title compound, C(6)H(10)N(8)S(2), was prepared by the nucleophilic substitution reaction of 5-mercapto-1-methyl-tetra-zole and dichloro-ethane. In the crystal, the mol-ecule possesses an approximate non-crystallographic twofold symmetry axis. The crystal packing is stabilized by weak inter-molecular C-H⋯N and π-π inter-actions [centroid-centroid distances = 3.448 (6), 3.5085 (5) and 3.4591 (2) Å]. The two five-membered rings form a dihedral angle of 1.9 (2)°.

Entities:  

Year:  2011        PMID: 21837068      PMCID: PMC3151974          DOI: 10.1107/S1600536811021957

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


Related literature

For the synthesis and structures of closely related compounds, see: She et al. (2006 ▶); Wei et al. (2011 ▶). For the pharmacological activity of tetra­zole-containing compounds, see: Gilchrist (1992 ▶); Armour et al. (1996 ▶); Upadhayaya et al. (2004 ▶). For applications of tetra­zole derivatives in coordination chemistry and as energetic materials, see: Zhao et al. (2008 ▶); Wang et al. (2009 ▶).

Experimental

Crystal data

C6H10N8S2 M = 258.34 Triclinic, a = 7.5905 (17) Å b = 7.9958 (17) Å c = 10.398 (2) Å α = 95.206 (3)° β = 92.922 (3)° γ = 115.109 (2)° V = 566.3 (2) Å3 Z = 2 Mo Kα radiation μ = 0.46 mm−1 T = 296 K 0.31 × 0.27 × 0.04 mm

Data collection

Bruker APEXII CCD diffractometer Absorption correction: multi-scan (SADABS; Bruker, 2002 ▶) T min = 0.868, T max = 0.982 2874 measured reflections 1972 independent reflections 1454 reflections with I > 2σ(I) R int = 0.017

Refinement

R[F 2 > 2σ(F 2)] = 0.047 wR(F 2) = 0.135 S = 1.39 1972 reflections 147 parameters H-atom parameters constrained Δρmax = 0.26 e Å−3 Δρmin = −0.26 e Å−3 Data collection: SMART (Bruker, 2002 ▶); cell refinement: SAINT (Bruker, 2002 ▶); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: ORTEP-3 (Farrugia, 1997 ▶); software used to prepare material for publication: SHELXL97. Crystal structure: contains datablock(s) global, I. DOI: 10.1107/S1600536811021957/yk2010sup1.cif Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811021957/yk2010Isup2.hkl Supplementary material file. DOI: 10.1107/S1600536811021957/yk2010Isup3.cml Additional supplementary materials: crystallographic information; 3D view; checkCIF report
C6H10N8S2Z = 2
Mr = 258.34F(000) = 268
Triclinic, P1Dx = 1.515 Mg m3Dm = 1.515 Mg m3Dm measured by not measured
Hall symbol: -P 1Mo Kα radiation, λ = 0.71073 Å
a = 7.5905 (17) ÅCell parameters from 816 reflections
b = 7.9958 (17) Åθ = 3.0–24.3°
c = 10.398 (2) ŵ = 0.46 mm1
α = 95.206 (3)°T = 296 K
β = 92.922 (3)°Flake-like, colourless
γ = 115.109 (2)°0.31 × 0.27 × 0.04 mm
V = 566.3 (2) Å3
Bruker APEXII CCD diffractometer1972 independent reflections
Radiation source: fine-focus sealed tube1454 reflections with I > 2σ(I)
graphiteRint = 0.017
φ and ω scansθmax = 25.1°, θmin = 2.0°
Absorption correction: multi-scan (SADABS; Bruker, 2002)h = −8→9
Tmin = 0.868, Tmax = 0.982k = −9→9
2874 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)] = 0.047Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.135H-atom parameters constrained
S = 1.39w = 1/[σ2(Fo2) + (0.050P)2] where P = (Fo2 + 2Fc2)/3
1972 reflections(Δ/σ)max < 0.001
147 parametersΔρmax = 0.26 e Å3
0 restraintsΔρmin = −0.26 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
S10.09578 (12)0.84390 (12)0.77838 (9)0.0521 (3)
S20.09347 (12)0.29485 (12)0.68329 (10)0.0556 (3)
C30.1006 (5)0.5022 (4)0.7748 (3)0.0475 (8)
H3A−0.01860.46950.81710.071*
H3B0.20960.55070.84180.071*
C40.1213 (5)0.6503 (4)0.6906 (3)0.0462 (8)
H4A0.02240.59750.61690.069*
H4B0.24850.69520.65760.069*
N80.4054 (4)0.2801 (4)0.5763 (3)0.0453 (7)
N10.3945 (4)1.1385 (4)0.9194 (3)0.0508 (7)
N70.6021 (4)0.3722 (4)0.5857 (3)0.0553 (8)
C20.3378 (5)0.3691 (4)0.6618 (3)0.0416 (8)
N40.4956 (4)0.9965 (4)0.7756 (3)0.0593 (8)
N50.4887 (4)0.5150 (4)0.7245 (3)0.0560 (8)
N30.6501 (4)1.1452 (5)0.8422 (3)0.0673 (9)
C50.3392 (5)0.9955 (5)0.8249 (3)0.0463 (8)
N60.6500 (4)0.5133 (4)0.6750 (3)0.0611 (8)
C10.2987 (5)0.1146 (5)0.4834 (4)0.0571 (10)
H1A0.37720.11410.41400.086*
H1B0.17910.11510.44890.086*
H1C0.26930.00550.52600.086*
N20.5909 (5)1.2321 (4)0.9288 (3)0.0664 (9)
C60.2779 (6)1.1957 (6)1.0046 (4)0.0694 (12)
H6A0.19581.23440.95400.104*
H6B0.36311.29731.06750.104*
H6C0.19811.09291.04820.104*
U11U22U33U12U13U23
S10.0445 (5)0.0435 (5)0.0671 (6)0.0217 (4)0.0033 (4)−0.0113 (4)
S20.0421 (5)0.0364 (5)0.0800 (7)0.0130 (4)0.0051 (4)−0.0121 (5)
C30.046 (2)0.0407 (19)0.054 (2)0.0201 (16)0.0055 (15)−0.0083 (16)
C40.046 (2)0.0393 (19)0.0510 (19)0.0189 (16)0.0026 (15)−0.0081 (16)
N80.0426 (16)0.0439 (16)0.0483 (16)0.0188 (13)0.0039 (13)−0.0006 (13)
N10.0494 (18)0.0460 (17)0.0492 (16)0.0150 (15)0.0033 (13)−0.0037 (14)
N70.0469 (18)0.059 (2)0.0606 (18)0.0229 (16)0.0091 (14)0.0061 (16)
C20.0393 (18)0.0323 (17)0.0483 (18)0.0128 (15)−0.0012 (15)−0.0021 (15)
N40.0489 (19)0.057 (2)0.067 (2)0.0194 (16)0.0076 (15)−0.0027 (16)
N50.0457 (18)0.0510 (18)0.0647 (19)0.0192 (15)−0.0068 (15)−0.0098 (15)
N30.0475 (19)0.063 (2)0.075 (2)0.0088 (17)0.0081 (17)0.0056 (18)
C50.051 (2)0.0419 (19)0.0460 (19)0.0220 (17)−0.0010 (16)−0.0004 (16)
N60.0456 (18)0.055 (2)0.074 (2)0.0171 (15)−0.0039 (16)−0.0024 (17)
C10.064 (2)0.0388 (19)0.059 (2)0.0167 (18)0.0033 (18)−0.0145 (17)
N20.057 (2)0.057 (2)0.069 (2)0.0104 (17)−0.0027 (17)0.0026 (17)
C60.070 (3)0.074 (3)0.060 (2)0.034 (2)0.005 (2)−0.023 (2)
S1—C51.738 (4)N1—C61.457 (4)
S1—C41.812 (3)N7—N61.302 (4)
S2—C21.724 (3)C2—N51.323 (4)
S2—C31.814 (3)N4—C51.314 (4)
C3—C41.496 (5)N4—N31.362 (4)
C3—H3A0.9700N5—N61.357 (4)
C3—H3B0.9700N3—N21.299 (4)
C4—H4A0.9700C1—H1A0.9600
C4—H4B0.9700C1—H1B0.9600
N8—C21.342 (4)C1—H1C0.9600
N8—N71.349 (4)C6—H6A0.9600
N8—C11.456 (4)C6—H6B0.9600
N1—C51.340 (4)C6—H6C0.9600
N1—N21.348 (4)
C5—S1—C4100.94 (15)N5—C2—S2128.0 (3)
C2—S2—C3100.20 (15)N8—C2—S2123.6 (2)
C4—C3—S2112.2 (2)C5—N4—N3105.8 (3)
C4—C3—H3A109.2C2—N5—N6106.0 (3)
S2—C3—H3A109.2N2—N3—N4110.7 (3)
C4—C3—H3B109.2N4—C5—N1108.9 (3)
S2—C3—H3B109.2N4—C5—S1128.2 (3)
H3A—C3—H3B107.9N1—C5—S1122.9 (3)
C3—C4—S1111.8 (2)N7—N6—N5110.8 (3)
C3—C4—H4A109.3N8—C1—H1A109.5
S1—C4—H4A109.3N8—C1—H1B109.5
C3—C4—H4B109.3H1A—C1—H1B109.5
S1—C4—H4B109.3N8—C1—H1C109.5
H4A—C4—H4B107.9H1A—C1—H1C109.5
C2—N8—N7108.6 (3)H1B—C1—H1C109.5
C2—N8—C1129.7 (3)N3—N2—N1106.3 (3)
N7—N8—C1121.7 (3)N1—C6—H6A109.5
C5—N1—N2108.3 (3)N1—C6—H6B109.5
C5—N1—C6130.2 (3)H6A—C6—H6B109.5
N2—N1—C6121.5 (3)N1—C6—H6C109.5
N6—N7—N8106.2 (2)H6A—C6—H6C109.5
N5—C2—N8108.4 (3)H6B—C6—H6C109.5
D—H···AD—HH···AD···AD—H···A
C1—H1A···N4i0.962.493.413 (5)161
C6—H6B···N5ii0.962.433.355 (5)161
Table 1

Hydrogen-bond geometry (Å, °)

D—H⋯AD—HH⋯ADAD—H⋯A
C1—H1A⋯N4i0.962.493.413 (5)161
C6—H6B⋯N5ii0.962.433.355 (5)161

Symmetry codes: (i) ; (ii) .

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