organic compounds
5-(Thiophen-2-ylmethyl)-1,3,4-thiadiazol-2-amine
aYeşilyurt Demir Çelik Vocational School, Ondokuz Mayıs University, Samsun, Turkey, bDepartment of Chemistry, Karadeniz Technical Universty, 61080 Trabzon, Turkey, cDepartment of Chemistry, Howard University, 525 College Street, NW, Washington, DC 2059, USA, dDepartment of Physics, Faculty of Sciences, Erciyes University, 38039 Kayseri, Turkey, and eDepartment of Chemistry, Keene State College, 220 Main Street, Keene, NH 03435-2001, USA
*Correspondence e-mail: rbutcher99@yahoo.com
In the title molecule, C7H7N3S2, the dihedral angle between the thiophene and thiadiazole 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 interactions [centroid–centroid distances = 3.654 (1) and 3.495 (1) Å].
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
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Refinement
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Data collection: CrysAlis PRO (Agilent, 2010); cell 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.
Supporting information
10.1107/S1600536812013633/hg5202sup1.cif
contains datablocks I, global. DOI:Structure factors: contains datablock I. DOI: 10.1107/S1600536812013633/hg5202Isup2.hkl
Supporting information file. DOI: 10.1107/S1600536812013633/hg5202Isup3.cml
The amine H atoms were seen in a difference Fourier map and then idealized with Uiso(H) = 1.2Ueq(N) with N–H bond length of 0.86 Å. The C-bound H-atoms were positioned geometrically with C—H = 0.93 and 0.97 Å, for aromatic and CH2 H-atoms, respectively, and constrained to ride on their parent atoms, with Uiso(H) = 1.2Ueq(C). During the
it was noticed that for the strongest reflections (Fc/Fc(max) close to 1.00) the observed value (Fo) was much smaller than the calculated value (Fc) indicating detector saturation problems. These reflections were omitted from the refinement.Data collection: CrysAlis PRO (Agilent, 2010); cell
CrysAlis PRO (Agilent, 2010); data reduction: CrysAlis PRO (Agilent, 2010); 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 (Sheldrick, 2008).C7H7N3S2 | F(000) = 408 |
Mr = 197.28 | Dx = 1.573 Mg m−3 |
Monoclinic, P21/c | Cu Kα radiation, λ = 1.54184 Å |
Hall symbol: -P 2ybc | Cell parameters from 2744 reflections |
a = 11.2970 (6) Å | θ = 3.9–70.0° |
b = 6.6094 (3) Å | µ = 5.33 mm−1 |
c = 11.2480 (6) Å | T = 173 K |
β = 97.243 (5)° | Chunk, colorless |
V = 833.15 (7) Å3 | 0.46 × 0.28 × 0.15 mm |
Z = 4 |
Agilent Xcalibur Eos Gemini diffractometer | 1539 independent reflections |
Radiation source: Enhance (Cu) X-ray Source | 1497 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.036 |
Detector resolution: 16.1500 pixels mm-1 | θmax = 70.1°, θmin = 3.9° |
ω scans | h = −13→13 |
Absorption correction: multi-scan (CrysAlis PRO; Agilent, 2010) | k = −5→8 |
Tmin = 0.209, Tmax = 0.450 | l = −12→13 |
4375 measured reflections |
Refinement on F2 | Secondary atom site location: difference Fourier map |
Least-squares matrix: full | Hydrogen site location: inferred from neighbouring sites |
R[F2 > 2σ(F2)] = 0.045 | H-atom parameters constrained |
wR(F2) = 0.120 | w = 1/[σ2(Fo2) + (0.0928P)2 + 0.0849P] where P = (Fo2 + 2Fc2)/3 |
S = 1.09 | (Δ/σ)max = 0.001 |
1539 reflections | Δρmax = 0.64 e Å−3 |
110 parameters | Δρmin = −0.38 e Å−3 |
0 restraints | Extinction correction: SHELXL97 (Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4 |
Primary atom site location: structure-invariant direct methods | Extinction coefficient: 0.035 (3) |
C7H7N3S2 | V = 833.15 (7) Å3 |
Mr = 197.28 | Z = 4 |
Monoclinic, P21/c | Cu Kα radiation |
a = 11.2970 (6) Å | µ = 5.33 mm−1 |
b = 6.6094 (3) Å | T = 173 K |
c = 11.2480 (6) Å | 0.46 × 0.28 × 0.15 mm |
β = 97.243 (5)° |
Agilent Xcalibur Eos Gemini diffractometer | 1539 independent reflections |
Absorption correction: multi-scan (CrysAlis PRO; Agilent, 2010) | 1497 reflections with I > 2σ(I) |
Tmin = 0.209, Tmax = 0.450 | Rint = 0.036 |
4375 measured reflections |
R[F2 > 2σ(F2)] = 0.045 | 0 restraints |
wR(F2) = 0.120 | H-atom parameters constrained |
S = 1.09 | Δρmax = 0.64 e Å−3 |
1539 reflections | Δρmin = −0.38 e Å−3 |
110 parameters |
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. |
x | y | z | Uiso*/Ueq | ||
S1 | 0.64166 (4) | 0.57641 (7) | 0.32224 (4) | 0.0210 (2) | |
S2 | 0.82410 (4) | 1.05521 (6) | 0.34150 (3) | 0.0182 (2) | |
N1 | 0.87197 (12) | 1.0981 (2) | 0.56747 (13) | 0.0175 (4) | |
N2 | 0.91662 (12) | 1.2714 (2) | 0.51908 (13) | 0.0179 (4) | |
N3 | 0.93579 (14) | 1.4168 (2) | 0.33358 (14) | 0.0251 (4) | |
H3A | 0.9732 | 1.5198 | 0.3665 | 0.030* | |
H3B | 0.9220 | 1.4085 | 0.2568 | 0.030* | |
C1 | 0.48911 (16) | 0.5889 (3) | 0.30609 (17) | 0.0216 (4) | |
H1 | 0.4395 | 0.5306 | 0.2430 | 0.026* | |
C2 | 0.44958 (15) | 0.6943 (3) | 0.39653 (16) | 0.0226 (4) | |
H2 | 0.3693 | 0.7160 | 0.4030 | 0.027* | |
C3 | 0.54422 (16) | 0.7680 (3) | 0.48045 (16) | 0.0206 (4) | |
H3 | 0.5323 | 0.8420 | 0.5483 | 0.025* | |
C4 | 0.65455 (15) | 0.7192 (2) | 0.45147 (15) | 0.0171 (4) | |
C5 | 0.77380 (16) | 0.7709 (3) | 0.51957 (16) | 0.0212 (4) | |
H5A | 0.8306 | 0.6668 | 0.5044 | 0.025* | |
H5B | 0.7667 | 0.7689 | 0.6046 | 0.025* | |
C6 | 0.82264 (14) | 0.9732 (3) | 0.48849 (14) | 0.0159 (4) | |
C7 | 0.89906 (14) | 1.2698 (3) | 0.40174 (15) | 0.0165 (4) |
U11 | U22 | U33 | U12 | U13 | U23 | |
S1 | 0.0161 (3) | 0.0215 (4) | 0.0250 (4) | −0.00005 (14) | 0.0010 (2) | −0.00692 (15) |
S2 | 0.0184 (3) | 0.0192 (3) | 0.0158 (3) | −0.00404 (13) | −0.0027 (2) | −0.00264 (13) |
N1 | 0.0172 (7) | 0.0156 (7) | 0.0191 (7) | −0.0010 (5) | 0.0000 (6) | 0.0004 (5) |
N2 | 0.0170 (7) | 0.0175 (8) | 0.0184 (7) | −0.0032 (5) | −0.0012 (5) | −0.0010 (5) |
N3 | 0.0272 (9) | 0.0290 (9) | 0.0172 (8) | −0.0138 (6) | −0.0039 (6) | 0.0017 (6) |
C1 | 0.0172 (8) | 0.0152 (8) | 0.0311 (9) | −0.0020 (6) | −0.0017 (7) | 0.0002 (7) |
C2 | 0.0176 (8) | 0.0169 (9) | 0.0337 (10) | 0.0024 (6) | 0.0052 (7) | 0.0078 (7) |
C3 | 0.0248 (9) | 0.0135 (9) | 0.0239 (9) | 0.0041 (6) | 0.0054 (7) | 0.0012 (6) |
C4 | 0.0211 (8) | 0.0084 (8) | 0.0213 (9) | −0.0011 (6) | 0.0007 (7) | 0.0000 (6) |
C5 | 0.0236 (9) | 0.0130 (9) | 0.0251 (9) | −0.0007 (6) | −0.0039 (7) | 0.0016 (7) |
C6 | 0.0139 (7) | 0.0152 (8) | 0.0179 (8) | 0.0022 (6) | −0.0004 (6) | −0.0003 (6) |
C7 | 0.0100 (7) | 0.0184 (9) | 0.0199 (8) | −0.0002 (6) | −0.0025 (6) | −0.0031 (6) |
S1—C1 | 1.7119 (18) | C1—C2 | 1.354 (3) |
S1—C4 | 1.7237 (17) | C1—H1 | 0.9300 |
S2—C6 | 1.7419 (17) | C2—C3 | 1.420 (3) |
S2—C7 | 1.7445 (17) | C2—H2 | 0.9300 |
N1—C6 | 1.287 (2) | C3—C4 | 1.366 (2) |
N1—N2 | 1.390 (2) | C3—H3 | 0.9300 |
N2—C7 | 1.310 (2) | C4—C5 | 1.503 (2) |
N3—C7 | 1.336 (2) | C5—C6 | 1.505 (2) |
N3—H3A | 0.8600 | C5—H5A | 0.9700 |
N3—H3B | 0.8600 | C5—H5B | 0.9700 |
C1—S1—C4 | 92.29 (9) | C3—C4—C5 | 127.66 (16) |
C6—S2—C7 | 86.93 (8) | C3—C4—S1 | 110.36 (13) |
C6—N1—N2 | 113.90 (14) | C5—C4—S1 | 121.96 (13) |
C7—N2—N1 | 111.83 (14) | C4—C5—C6 | 114.53 (14) |
C7—N3—H3A | 120.0 | C4—C5—H5A | 108.6 |
C7—N3—H3B | 120.0 | C6—C5—H5A | 108.6 |
H3A—N3—H3B | 120.0 | C4—C5—H5B | 108.6 |
C2—C1—S1 | 111.59 (14) | C6—C5—H5B | 108.6 |
C2—C1—H1 | 124.2 | H5A—C5—H5B | 107.6 |
S1—C1—H1 | 124.2 | N1—C6—C5 | 123.32 (15) |
C1—C2—C3 | 112.57 (16) | N1—C6—S2 | 113.61 (13) |
C1—C2—H2 | 123.7 | C5—C6—S2 | 123.00 (12) |
C3—C2—H2 | 123.7 | N2—C7—N3 | 123.65 (16) |
C4—C3—C2 | 113.16 (16) | N2—C7—S2 | 113.71 (13) |
C4—C3—H3 | 123.4 | N3—C7—S2 | 122.63 (13) |
C2—C3—H3 | 123.4 | ||
C6—N1—N2—C7 | −0.27 (19) | N2—N1—C6—C5 | 176.73 (15) |
C4—S1—C1—C2 | −1.08 (14) | N2—N1—C6—S2 | −0.36 (18) |
S1—C1—C2—C3 | 0.4 (2) | C4—C5—C6—N1 | 136.56 (17) |
C1—C2—C3—C4 | 0.7 (2) | C4—C5—C6—S2 | −46.6 (2) |
C2—C3—C4—C5 | −179.68 (15) | C7—S2—C6—N1 | 0.64 (13) |
C2—C3—C4—S1 | −1.50 (19) | C7—S2—C6—C5 | −176.45 (15) |
C1—S1—C4—C3 | 1.47 (14) | N1—N2—C7—N3 | −178.55 (16) |
C1—S1—C4—C5 | 179.78 (14) | N1—N2—C7—S2 | 0.78 (18) |
C3—C4—C5—C6 | −87.1 (2) | C6—S2—C7—N2 | −0.80 (13) |
S1—C4—C5—C6 | 94.86 (17) | C6—S2—C7—N3 | 178.53 (16) |
Cg is the centroid of the S1/C1–C4 ring. |
D—H···A | D—H | H···A | D···A | D—H···A |
N3—H3B···N1i | 0.86 | 2.13 | 2.991 (2) | 175 |
N3—H3A···N2ii | 0.86 | 2.17 | 3.013 (2) | 167 |
C1—H1···Cgiii | 0.93 | 2.83 | 3.549 (2) | 135 |
Symmetry codes: (i) x, −y+5/2, z−1/2; (ii) −x+2, −y+3, −z+1; (iii) −x+1, y−1/2, −z+1/2. |
Experimental details
Crystal data | |
Chemical formula | C7H7N3S2 |
Mr | 197.28 |
Crystal system, space group | Monoclinic, P21/c |
Temperature (K) | 173 |
a, b, c (Å) | 11.2970 (6), 6.6094 (3), 11.2480 (6) |
β (°) | 97.243 (5) |
V (Å3) | 833.15 (7) |
Z | 4 |
Radiation type | Cu Kα |
µ (mm−1) | 5.33 |
Crystal size (mm) | 0.46 × 0.28 × 0.15 |
Data collection | |
Diffractometer | Agilent Xcalibur Eos Gemini diffractometer |
Absorption correction | Multi-scan (CrysAlis PRO; Agilent, 2010) |
Tmin, Tmax | 0.209, 0.450 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 4375, 1539, 1497 |
Rint | 0.036 |
(sin θ/λ)max (Å−1) | 0.610 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.045, 0.120, 1.09 |
No. of reflections | 1539 |
No. of parameters | 110 |
H-atom treatment | H-atom parameters constrained |
Δρmax, Δρmin (e Å−3) | 0.64, −0.38 |
Computer programs: CrysAlis PRO (Agilent, 2010), SHELXS97 (Sheldrick, 2008), SHELXL97 (Sheldrick, 2008), SHELXTL (Sheldrick, 2008).
Cg is the centroid of the S1/C1–C4 ring. |
D—H···A | D—H | H···A | D···A | D—H···A |
N3—H3B···N1i | 0.86 | 2.13 | 2.991 (2) | 174.6 |
N3—H3A···N2ii | 0.86 | 2.17 | 3.013 (2) | 166.7 |
C1—H1···Cgiii | 0.93 | 2.83 | 3.549 (2) | 135 |
Symmetry codes: (i) x, −y+5/2, z−1/2; (ii) −x+2, −y+3, −z+1; (iii) −x+1, y−1/2, −z+1/2. |
Acknowledgements
RJB acknowledges the NSF–MRI program (grant No. CHE-0619278) for funds to purchase the diffractometer.
References
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The antitumor activites of 2-amino-1,3,4-thiadiazole (ATDA, NSC-4728) and the related compounds: 2-ethylamino-1,3,4-thiadiazole (EATDA), 2,2'-(methylene-diamino) bis-1,3,4-thiadiazole (NSC-143019) were found in several experimental tumor systems about 50 years ago (Olesan et al., 1955). 2-Amino-1,3,4-thiadiazole (ATDA), as the most promising compound, was used in phase II clinical trials in patients with different tumors: renal, colon, ovarian, and others. Recently new derivatives with the 1,3,4-thiadiazole nucleus as well as Fe(II) / Fe (III) complexes of 2-amino-1,3,4-thiadiazoles have been synthesized and evaluated for their antiproliferative activity against a panel of human cancer cell lines (Mishra et al., 1995). Over recent years, there has been an increasing interest in the chemistry of thiophenes because of their biological significance. Many of them have been widely investigated for therapeutic uses, especially as antifungal, antibacterial, anti-inflammatory, anticonvulsant, antiasthmatic, and analgesic agents. They also were known to show anti-HIV, antiproliferative, germicidal, and D2 dopaminergic activities (Mohareb et al., 2004). In view of these facts, the aim of this present study is to obtain a structure of 1,3,4-oxadiazole incorporating the thiophene ring.
In the molecule of the title compound (Fig 1), the bond lengths are within normal ranges (Allen et al., 1987). In the molecule of (I) atom S1 is oriented towards the thiadiazol ring, Fig. 1. The dihedral angle between the planar thiophene (r.m.s. deviation = 0.007 Å) and planar thiadiazol (r.m.s. deviation = 0.004 Å) rings of 72.99 (5)° indicates a twist between planes as seen in the S1–C4–C5–C6 torsion angle of 94.86 (17) °. The amine group is effectively co-planar with the thiadiazol ring to which it is attached as seen in the N3–C7–S2–C6 torsion angle of 178.53 (16) °.
In the crystal structure, there are strong intermolecular N–H···N hydrogen bonds which lead to the formation of centrosymmetric dimers in the crystal. In addition there are C—H···π and π-π stacking interactions [Cg1···Cg1(1 - x, -y, -z) = 3.654 (1) Å and Cg2···Cg2(-x, 1 - y, -z) = 3.495 (1) Å, Cg1(S1/C1—C4) and Cg2(S2/N1/N2/C6/C7) are the centroids of the thiophene and thiadiazol rings]. This pattern is the primary supramolecular structure for this compound (Fig. 2).