Literature DB >> 22590194

5-(Thio-phen-2-ylmeth-yl)-1,3,4-thia-diazol-2-amine.

Yavuz Köysal, Sadık Deniz, Ray J Butcher, Sema Oztürk Yildirim, Jerry P Jasinski, Amanda C Keeley.   

Abstract

In the title mol-ecule, C(7)H(7)N(3)S(2), the dihedral angle between the thio-phene and thia-diazole rings is 72.99 (5)°; the two rings are oriented so that the S atoms in each ring are on the same side. In the crystal, the three-dimensional network involves strong N-H⋯O hydrogen bonds, as well as C-H⋯π and π-π stacking inter-actions [centroid-centroid distances = 3.654 (1) and 3.495 (1) Å].

Entities:  

Year:  2012        PMID: 22590194      PMCID: PMC3344432          DOI: 10.1107/S1600536812013633

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


Related literature

For the anti­tumor activity of 2-amino-1,3,4-thia­diazole, 2-ethyl­amino-1,3,4-thia­diazole and 2,2′-(methyl­enediamino)­bis-1,3,4-thia­diazole, see: Olesan et al. (1955 ▶); Mishra et al. (1995 ▶). For their anti-HIV, anti­proliferative, germicidal and D2 dopamine­rgic activity, see: Mohareb et al. (2004 ▶). For the synthesis of the title compound, see: Sancak et al., (2007 ▶). For standard bond lengths, see: Allen et al. (1987 ▶).

Experimental

Crystal data

C7H7N3S2 M = 197.28 Monoclinic, a = 11.2970 (6) Å b = 6.6094 (3) Å c = 11.2480 (6) Å β = 97.243 (5)° V = 833.15 (7) Å3 Z = 4 Cu Kα radiation μ = 5.33 mm−1 T = 173 K 0.46 × 0.28 × 0.15 mm

Data collection

Agilent Xcalibur Eos Gemini diffractometer Absorption correction: multi-scan (CrysAlis PRO; Agilent, 2010 ▶) T min = 0.209, T max = 0.450 4375 measured reflections 1539 independent reflections 1497 reflections with I > 2σ(I) R int = 0.036

Refinement

R[F 2 > 2σ(F 2)] = 0.045 wR(F 2) = 0.120 S = 1.09 1539 reflections 110 parameters H-atom parameters constrained Δρmax = 0.64 e Å−3 Δρmin = −0.38 e Å−3 Data collection: CrysAlis PRO (Agilent, 2010 ▶); cell refinement: CrysAlis PRO; data reduction: CrysAlis PRO; 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 datablock(s) I, global. DOI: 10.1107/S1600536812013633/hg5202sup1.cif Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812013633/hg5202Isup2.hkl Supplementary material file. DOI: 10.1107/S1600536812013633/hg5202Isup3.cml Additional supplementary materials: crystallographic information; 3D view; checkCIF report
C7H7N3S2F(000) = 408
Mr = 197.28Dx = 1.573 Mg m3
Monoclinic, P21/cCu Kα radiation, λ = 1.54184 Å
Hall symbol: -P 2ybcCell parameters from 2744 reflections
a = 11.2970 (6) Åθ = 3.9–70.0°
b = 6.6094 (3) ŵ = 5.33 mm1
c = 11.2480 (6) ÅT = 173 K
β = 97.243 (5)°Chunk, colorless
V = 833.15 (7) Å30.46 × 0.28 × 0.15 mm
Z = 4
Agilent Xcalibur Eos Gemini diffractometer1539 independent reflections
Radiation source: Enhance (Cu) X-ray Source1497 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.036
Detector resolution: 16.1500 pixels mm-1θmax = 70.1°, θmin = 3.9°
ω scansh = −13→13
Absorption correction: multi-scan (CrysAlis PRO; Agilent, 2010)k = −5→8
Tmin = 0.209, Tmax = 0.450l = −12→13
4375 measured reflections
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.045H-atom parameters constrained
wR(F2) = 0.120w = 1/[σ2(Fo2) + (0.0928P)2 + 0.0849P] where P = (Fo2 + 2Fc2)/3
S = 1.09(Δ/σ)max = 0.001
1539 reflectionsΔρmax = 0.64 e Å3
110 parametersΔρmin = −0.38 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: 0.035 (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
S10.64166 (4)0.57641 (7)0.32224 (4)0.0210 (2)
S20.82410 (4)1.05521 (6)0.34150 (3)0.0182 (2)
N10.87197 (12)1.0981 (2)0.56747 (13)0.0175 (4)
N20.91662 (12)1.2714 (2)0.51908 (13)0.0179 (4)
N30.93579 (14)1.4168 (2)0.33358 (14)0.0251 (4)
H3A0.97321.51980.36650.030*
H3B0.92201.40850.25680.030*
C10.48911 (16)0.5889 (3)0.30609 (17)0.0216 (4)
H10.43950.53060.24300.026*
C20.44958 (15)0.6943 (3)0.39653 (16)0.0226 (4)
H20.36930.71600.40300.027*
C30.54422 (16)0.7680 (3)0.48045 (16)0.0206 (4)
H30.53230.84200.54830.025*
C40.65455 (15)0.7192 (2)0.45147 (15)0.0171 (4)
C50.77380 (16)0.7709 (3)0.51957 (16)0.0212 (4)
H5A0.83060.66680.50440.025*
H5B0.76670.76890.60460.025*
C60.82264 (14)0.9732 (3)0.48849 (14)0.0159 (4)
C70.89906 (14)1.2698 (3)0.40174 (15)0.0165 (4)
U11U22U33U12U13U23
S10.0161 (3)0.0215 (4)0.0250 (4)−0.00005 (14)0.0010 (2)−0.00692 (15)
S20.0184 (3)0.0192 (3)0.0158 (3)−0.00404 (13)−0.0027 (2)−0.00264 (13)
N10.0172 (7)0.0156 (7)0.0191 (7)−0.0010 (5)0.0000 (6)0.0004 (5)
N20.0170 (7)0.0175 (8)0.0184 (7)−0.0032 (5)−0.0012 (5)−0.0010 (5)
N30.0272 (9)0.0290 (9)0.0172 (8)−0.0138 (6)−0.0039 (6)0.0017 (6)
C10.0172 (8)0.0152 (8)0.0311 (9)−0.0020 (6)−0.0017 (7)0.0002 (7)
C20.0176 (8)0.0169 (9)0.0337 (10)0.0024 (6)0.0052 (7)0.0078 (7)
C30.0248 (9)0.0135 (9)0.0239 (9)0.0041 (6)0.0054 (7)0.0012 (6)
C40.0211 (8)0.0084 (8)0.0213 (9)−0.0011 (6)0.0007 (7)0.0000 (6)
C50.0236 (9)0.0130 (9)0.0251 (9)−0.0007 (6)−0.0039 (7)0.0016 (7)
C60.0139 (7)0.0152 (8)0.0179 (8)0.0022 (6)−0.0004 (6)−0.0003 (6)
C70.0100 (7)0.0184 (9)0.0199 (8)−0.0002 (6)−0.0025 (6)−0.0031 (6)
S1—C11.7119 (18)C1—C21.354 (3)
S1—C41.7237 (17)C1—H10.9300
S2—C61.7419 (17)C2—C31.420 (3)
S2—C71.7445 (17)C2—H20.9300
N1—C61.287 (2)C3—C41.366 (2)
N1—N21.390 (2)C3—H30.9300
N2—C71.310 (2)C4—C51.503 (2)
N3—C71.336 (2)C5—C61.505 (2)
N3—H3A0.8600C5—H5A0.9700
N3—H3B0.8600C5—H5B0.9700
C1—S1—C492.29 (9)C3—C4—C5127.66 (16)
C6—S2—C786.93 (8)C3—C4—S1110.36 (13)
C6—N1—N2113.90 (14)C5—C4—S1121.96 (13)
C7—N2—N1111.83 (14)C4—C5—C6114.53 (14)
C7—N3—H3A120.0C4—C5—H5A108.6
C7—N3—H3B120.0C6—C5—H5A108.6
H3A—N3—H3B120.0C4—C5—H5B108.6
C2—C1—S1111.59 (14)C6—C5—H5B108.6
C2—C1—H1124.2H5A—C5—H5B107.6
S1—C1—H1124.2N1—C6—C5123.32 (15)
C1—C2—C3112.57 (16)N1—C6—S2113.61 (13)
C1—C2—H2123.7C5—C6—S2123.00 (12)
C3—C2—H2123.7N2—C7—N3123.65 (16)
C4—C3—C2113.16 (16)N2—C7—S2113.71 (13)
C4—C3—H3123.4N3—C7—S2122.63 (13)
C2—C3—H3123.4
C6—N1—N2—C7−0.27 (19)N2—N1—C6—C5176.73 (15)
C4—S1—C1—C2−1.08 (14)N2—N1—C6—S2−0.36 (18)
S1—C1—C2—C30.4 (2)C4—C5—C6—N1136.56 (17)
C1—C2—C3—C40.7 (2)C4—C5—C6—S2−46.6 (2)
C2—C3—C4—C5−179.68 (15)C7—S2—C6—N10.64 (13)
C2—C3—C4—S1−1.50 (19)C7—S2—C6—C5−176.45 (15)
C1—S1—C4—C31.47 (14)N1—N2—C7—N3−178.55 (16)
C1—S1—C4—C5179.78 (14)N1—N2—C7—S20.78 (18)
C3—C4—C5—C6−87.1 (2)C6—S2—C7—N2−0.80 (13)
S1—C4—C5—C694.86 (17)C6—S2—C7—N3178.53 (16)
D—H···AD—HH···AD···AD—H···A
N3—H3B···N1i0.862.132.991 (2)175
N3—H3A···N2ii0.862.173.013 (2)167
C1—H1···Cgiii0.932.833.549 (2)135
Table 1

Hydrogen-bond geometry (Å, °)

Cg is the centroid of the S1/C1–C4 ring.

D—H⋯AD—HH⋯ADAD—H⋯A
N3—H3B⋯N1i0.862.132.991 (2)175
N3—H3A⋯N2ii0.862.173.013 (2)167
C1—H1⋯Cgiii0.932.833.549 (2)135

Symmetry codes: (i) ; (ii) ; (iii) .

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