organic compounds
Ethyl 5-amino-3-methylsulfanyl-1H-pyrazole-4-carboxylate
aSchool of Chemistry and Chemical Engineering, Shandong University, Jinan 250100, People's Republic of China
*Correspondence e-mail: yugp2005@yahoo.com.cn
In the title compound, C7H11N3O2S, bond lengths and angles are within normal ranges. The crystal packing is stabilized by intermolecular N—H⋯O hydrogen bonds, linking the molecules into infinite one-dimensional chains along the a axis.
Related literature
For the biological activity, see: Hanefeld et al. (1996). For a similar structure, see: Ren et al. (2004).
Experimental
Crystal data
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Refinement
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Data collection: SMART (Bruker, 2001); cell SAINT (Bruker, 2001); data reduction: SAINT; program(s) used to solve structure: SHELXTL (Sheldrick, 2008); program(s) used to refine structure: SHELXTL; molecular graphics: SHELXTL; software used to prepare material for publication: SHELXTL.
Supporting information
10.1107/S1600536808035095/hg2437sup1.cif
contains datablocks I, global. DOI:Structure factors: contains datablock I. DOI: 10.1107/S1600536808035095/hg2437Isup2.hkl
A round-bottomed flask fitted with a dropping funnel was charged with 11.2 g (0.2 mol) potassium hydroxide in 200 ml MeCN. The solution was cooled in an ice bath. Through the dropping funnel 22.7 g (0.2 mol) ethyl cyanoacetate was added gradually. After stirring at 273K for 0.5 h, 15.2 g(0.2 mol) carbon bisulfide was added while vigorous stirring. Keep stirring for 1 h, 50.4 g(0.4 mol) dimethyl sulfate was added through the drop funnel, then left overnight. The reaction mixture was filtered and filtrate evaporated on a rotary evaporator to remove the solvent. The mixture was dissolved in 50 ml ethanol, then through a drop funnel 12.5 g (0.2 mol) of hydrazine hydrate was added. The solution was evaporated in vacuo to afford crude product, which was purified by
to give the desired product 34.7 g, yield 86.3%. Crystals suitable for X-ray were obtained by slow evaporation of a methanol solution at room temperature for one week.All H atoms were placed in calculated positions, with C—H = 0.93 or 0.97 Å, N–H = 0.86 Å, and included in the final cycles of
using a riding model, with Uiso(H) = 1.2 (1.5 times for methyl) times Ueq(C,N).Data collection: SMART (Bruker, 2001); cell
SAINT (Bruker, 2001); data reduction: SAINT (Bruker, 2001); program(s) used to solve structure: SHELXTL (Sheldrick, 2008); program(s) used to refine structure: SHELXTL (Sheldrick, 2008); molecular graphics: SHELXTL (Sheldrick, 2008); software used to prepare material for publication: SHELXTL (Sheldrick, 2008).Fig. 1. View of the title compound (I), with displacement ellipsoids drawn at the 40% probability level. |
C7H11N3O2S | Z = 2 |
Mr = 201.25 | F(000) = 212 |
Triclinic, P1 | Dx = 1.437 Mg m−3 |
Hall symbol: -P 1 | Mo Kα radiation, λ = 0.71073 Å |
a = 7.0012 (7) Å | Cell parameters from 1750 reflections |
b = 7.5870 (8) Å | θ = 3.0–27.5° |
c = 10.1055 (10) Å | µ = 0.32 mm−1 |
α = 81.038 (2)° | T = 273 K |
β = 72.173 (2)° | Block, yellow |
γ = 65.643 (1)° | 0.10 × 0.10 × 0.05 mm |
V = 465.26 (8) Å3 |
Bruker SMART CCD area-detector diffractometer | 1624 independent reflections |
Radiation source: fine-focus sealed tube | 1488 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.013 |
ϕ and ω scans | θmax = 25.0°, θmin = 2.1° |
Absorption correction: multi-scan (SADABS; Sheldrick, 1996) | h = −8→8 |
Tmin = 0.969, Tmax = 0.984 | k = −8→9 |
2317 measured reflections | l = −5→11 |
Refinement on F2 | Primary atom site location: structure-invariant direct methods |
Least-squares matrix: full | Secondary atom site location: difference Fourier map |
R[F2 > 2σ(F2)] = 0.044 | Hydrogen site location: inferred from neighbouring sites |
wR(F2) = 0.127 | H-atom parameters constrained |
S = 1.08 | w = 1/[σ2(Fo2) + (0.0669P)2 + 0.2967P] where P = (Fo2 + 2Fc2)/3 |
1624 reflections | (Δ/σ)max < 0.001 |
118 parameters | Δρmax = 0.45 e Å−3 |
0 restraints | Δρmin = −0.24 e Å−3 |
C7H11N3O2S | γ = 65.643 (1)° |
Mr = 201.25 | V = 465.26 (8) Å3 |
Triclinic, P1 | Z = 2 |
a = 7.0012 (7) Å | Mo Kα radiation |
b = 7.5870 (8) Å | µ = 0.32 mm−1 |
c = 10.1055 (10) Å | T = 273 K |
α = 81.038 (2)° | 0.10 × 0.10 × 0.05 mm |
β = 72.173 (2)° |
Bruker SMART CCD area-detector diffractometer | 1624 independent reflections |
Absorption correction: multi-scan (SADABS; Sheldrick, 1996) | 1488 reflections with I > 2σ(I) |
Tmin = 0.969, Tmax = 0.984 | Rint = 0.013 |
2317 measured reflections |
R[F2 > 2σ(F2)] = 0.044 | 0 restraints |
wR(F2) = 0.127 | H-atom parameters constrained |
S = 1.08 | Δρmax = 0.45 e Å−3 |
1624 reflections | Δρmin = −0.24 e Å−3 |
118 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 | 0.46271 (10) | 0.72168 (10) | 0.13781 (7) | 0.0506 (3) | |
O1 | 0.3262 (3) | 0.7811 (3) | 0.61242 (17) | 0.0461 (4) | |
O2 | 0.1914 (3) | 0.7558 (3) | 0.44317 (18) | 0.0486 (5) | |
N2 | 0.8938 (3) | 0.7010 (3) | 0.3056 (2) | 0.0435 (5) | |
H2C | 1.0232 | 0.6889 | 0.3013 | 0.052* | |
C3 | 0.3414 (4) | 0.7574 (3) | 0.4801 (2) | 0.0383 (5) | |
N1 | 0.7639 (3) | 0.7355 (3) | 0.5482 (2) | 0.0510 (6) | |
H1D | 0.8881 | 0.7260 | 0.5535 | 0.061* | |
H1E | 0.6578 | 0.7515 | 0.6223 | 0.061* | |
C5 | 0.7355 (3) | 0.7256 (3) | 0.4242 (2) | 0.0368 (5) | |
C2 | 0.1246 (4) | 0.8045 (4) | 0.7109 (3) | 0.0418 (6) | |
H2A | 0.0903 | 0.6923 | 0.7138 | 0.050* | |
H2B | 0.0088 | 0.9182 | 0.6866 | 0.050* | |
C6 | 0.6221 (4) | 0.7165 (3) | 0.2425 (3) | 0.0387 (5) | |
N3 | 0.8282 (3) | 0.6970 (3) | 0.1904 (2) | 0.0450 (5) | |
C4 | 0.5518 (3) | 0.7352 (3) | 0.3906 (2) | 0.0360 (5) | |
C1 | 0.1484 (5) | 0.8274 (4) | 0.8514 (3) | 0.0542 (7) | |
H1A | 0.0146 | 0.8433 | 0.9215 | 0.081* | |
H1B | 0.1818 | 0.9392 | 0.8472 | 0.081* | |
H1C | 0.2638 | 0.7143 | 0.8740 | 0.081* | |
C7 | 0.6528 (5) | 0.7014 (5) | −0.0316 (3) | 0.0626 (8) | |
H7A | 0.5843 | 0.7025 | −0.1009 | 0.094* | |
H7B | 0.7777 | 0.5824 | −0.0347 | 0.094* | |
H7C | 0.6977 | 0.8085 | −0.0493 | 0.094* |
U11 | U22 | U33 | U12 | U13 | U23 | |
S1 | 0.0384 (4) | 0.0712 (5) | 0.0510 (4) | −0.0245 (3) | −0.0179 (3) | −0.0052 (3) |
O1 | 0.0381 (9) | 0.0649 (11) | 0.0429 (9) | −0.0248 (8) | −0.0141 (7) | −0.0026 (8) |
O2 | 0.0306 (9) | 0.0707 (12) | 0.0543 (11) | −0.0249 (8) | −0.0170 (8) | −0.0035 (9) |
N2 | 0.0280 (9) | 0.0626 (13) | 0.0486 (12) | −0.0232 (9) | −0.0139 (8) | −0.0029 (9) |
C3 | 0.0304 (11) | 0.0412 (12) | 0.0469 (13) | −0.0150 (9) | −0.0144 (10) | 0.0001 (10) |
N1 | 0.0336 (11) | 0.0840 (16) | 0.0477 (12) | −0.0301 (11) | −0.0154 (9) | −0.0060 (11) |
C5 | 0.0286 (11) | 0.0430 (12) | 0.0450 (12) | −0.0174 (9) | −0.0143 (9) | −0.0002 (10) |
C2 | 0.0311 (11) | 0.0468 (13) | 0.0547 (14) | −0.0174 (10) | −0.0189 (10) | −0.0003 (11) |
C6 | 0.0324 (11) | 0.0389 (12) | 0.0460 (13) | −0.0151 (9) | −0.0100 (10) | −0.0022 (9) |
N3 | 0.0335 (10) | 0.0597 (13) | 0.0463 (12) | −0.0218 (9) | −0.0105 (9) | −0.0043 (9) |
C4 | 0.0254 (10) | 0.0398 (11) | 0.0475 (13) | −0.0141 (9) | −0.0141 (9) | −0.0016 (9) |
C1 | 0.0513 (15) | 0.0736 (18) | 0.0446 (14) | −0.0320 (14) | −0.0093 (12) | −0.0064 (13) |
C7 | 0.0547 (17) | 0.095 (2) | 0.0483 (16) | −0.0347 (16) | −0.0180 (13) | −0.0050 (15) |
S1—C6 | 1.744 (2) | C5—C4 | 1.399 (3) |
S1—C7 | 1.801 (3) | C2—C1 | 1.522 (3) |
O1—C3 | 1.343 (3) | C2—H2A | 0.9700 |
O1—C2 | 1.415 (3) | C2—H2B | 0.9700 |
O2—C3 | 1.222 (3) | C6—N3 | 1.328 (3) |
N2—C5 | 1.336 (3) | C6—C4 | 1.435 (3) |
N2—N3 | 1.385 (3) | C1—H1A | 0.9600 |
N2—H2C | 0.8600 | C1—H1B | 0.9600 |
C3—C4 | 1.429 (3) | C1—H1C | 0.9600 |
N1—C5 | 1.346 (3) | C7—H7A | 0.9600 |
N1—H1D | 0.8600 | C7—H7B | 0.9600 |
N1—H1E | 0.8600 | C7—H7C | 0.9600 |
C6—S1—C7 | 100.66 (12) | N3—C6—C4 | 111.9 (2) |
C3—O1—C2 | 116.79 (18) | N3—C6—S1 | 122.18 (19) |
C5—N2—N3 | 113.11 (18) | C4—C6—S1 | 125.90 (17) |
C5—N2—H2C | 123.4 | C6—N3—N2 | 104.02 (19) |
N3—N2—H2C | 123.4 | C5—C4—C3 | 129.2 (2) |
O2—C3—O1 | 123.1 (2) | C5—C4—C6 | 103.93 (19) |
O2—C3—C4 | 125.2 (2) | C3—C4—C6 | 126.9 (2) |
O1—C3—C4 | 111.67 (19) | C2—C1—H1A | 109.5 |
C5—N1—H1D | 120.0 | C2—C1—H1B | 109.5 |
C5—N1—H1E | 120.0 | H1A—C1—H1B | 109.5 |
H1D—N1—H1E | 120.0 | C2—C1—H1C | 109.5 |
N2—C5—N1 | 122.8 (2) | H1A—C1—H1C | 109.5 |
N2—C5—C4 | 107.0 (2) | H1B—C1—H1C | 109.5 |
N1—C5—C4 | 130.2 (2) | S1—C7—H7A | 109.5 |
O1—C2—C1 | 106.85 (18) | S1—C7—H7B | 109.5 |
O1—C2—H2A | 110.4 | H7A—C7—H7B | 109.5 |
C1—C2—H2A | 110.4 | S1—C7—H7C | 109.5 |
O1—C2—H2B | 110.4 | H7A—C7—H7C | 109.5 |
C1—C2—H2B | 110.4 | H7B—C7—H7C | 109.5 |
H2A—C2—H2B | 108.6 | ||
C2—O1—C3—O2 | 0.2 (3) | N1—C5—C4—C3 | −0.4 (4) |
C2—O1—C3—C4 | −179.98 (19) | N2—C5—C4—C6 | −0.8 (2) |
N3—N2—C5—N1 | −179.3 (2) | N1—C5—C4—C6 | 179.9 (2) |
N3—N2—C5—C4 | 1.3 (3) | O2—C3—C4—C5 | −176.5 (2) |
C3—O1—C2—C1 | 179.7 (2) | O1—C3—C4—C5 | 3.6 (3) |
C7—S1—C6—N3 | −1.3 (2) | O2—C3—C4—C6 | 3.1 (4) |
C7—S1—C6—C4 | 177.5 (2) | O1—C3—C4—C6 | −176.7 (2) |
C4—C6—N3—N2 | 0.6 (3) | N3—C6—C4—C5 | 0.1 (3) |
S1—C6—N3—N2 | 179.63 (16) | S1—C6—C4—C5 | −178.88 (17) |
C5—N2—N3—C6 | −1.2 (3) | N3—C6—C4—C3 | −179.6 (2) |
N2—C5—C4—C3 | 178.9 (2) | S1—C6—C4—C3 | 1.4 (4) |
D—H···A | D—H | H···A | D···A | D—H···A |
N1—H1D···O2i | 0.86 | 2.16 | 2.914 (3) | 146 |
N2—H2C···O2i | 0.86 | 2.34 | 3.019 (3) | 137 |
Symmetry code: (i) x+1, y, z. |
Experimental details
Crystal data | |
Chemical formula | C7H11N3O2S |
Mr | 201.25 |
Crystal system, space group | Triclinic, P1 |
Temperature (K) | 273 |
a, b, c (Å) | 7.0012 (7), 7.5870 (8), 10.1055 (10) |
α, β, γ (°) | 81.038 (2), 72.173 (2), 65.643 (1) |
V (Å3) | 465.26 (8) |
Z | 2 |
Radiation type | Mo Kα |
µ (mm−1) | 0.32 |
Crystal size (mm) | 0.10 × 0.10 × 0.05 |
Data collection | |
Diffractometer | Bruker SMART CCD area-detector diffractometer |
Absorption correction | Multi-scan (SADABS; Sheldrick, 1996) |
Tmin, Tmax | 0.969, 0.984 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 2317, 1624, 1488 |
Rint | 0.013 |
(sin θ/λ)max (Å−1) | 0.595 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.044, 0.127, 1.08 |
No. of reflections | 1624 |
No. of parameters | 118 |
H-atom treatment | H-atom parameters constrained |
Δρmax, Δρmin (e Å−3) | 0.45, −0.24 |
Computer programs: SMART (Bruker, 2001), SAINT (Bruker, 2001), SHELXTL (Sheldrick, 2008).
D—H···A | D—H | H···A | D···A | D—H···A |
N1—H1D···O2i | 0.86 | 2.16 | 2.914 (3) | 146.0 |
N2—H2C···O2i | 0.86 | 2.34 | 3.019 (3) | 136.7 |
Symmetry code: (i) x+1, y, z. |
References
Bruker (2001). SMART and SAINT. Bruker AXS Inc., Madison, Wisconsin. Google Scholar
Hanefeld, U., Rees, C. W. & White, A. J. P. (1996). J. Chem. Soc., Perkin Trans. 1, pp. 1545–1552. Google Scholar
Ren, X. L., Wu, C., Hu, F. Z., Zou, X. M. & Yang, H. Z. (2004). Chin. J. Chem. 22, 194–198. CrossRef CAS Google Scholar
Sheldrick, G. M. (1996). SADABS. University of Göttingen, Germany. Google Scholar
Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. Web of Science CrossRef CAS IUCr Journals Google Scholar
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The title compound, is an important intermediate in synthesis of heterocyclic compounds (Hanfeld et al., 1996) in particular, in producing imidazo[1,2-b]pyrazole derivatives. Here, we report the crystal structure of (I).
In compound (I), all bond lengths and angles are normal and in a good agreement with those reported previously (Ren et al., 2004). The pyrazole ring C4/C5/C5/N2/N3 and bonded atoms N1, S1, C3, O1, C2 and C1 are coplanar, the largest deviation from the mean plane being 0.053 (2)Å for atom C3. The crystal packing is stabilized by intermolecular N—H···O hydrogen bonds, linking the molecules into infinite one-dimensional chain along the a axis.