Literature DB >> 21579158

Redetermination of 1-cyclo-hexyl-3-(2-furo-yl)thio-urea.

J Duque, O Estévez, V Jancik, H Yee-Madeira.   

Abstract

The title compound, C(12)H(16)N(2)O(2)S, was synthesized from furoyl isothio-cyanate and cyclo-hexyl-amine in dry acetone, and the crystal structure redetermined. The thio-urea group is in the thio-amide form. The structure [Otazo-Sánchez et al. (2001 ▶). J. Chem. Soc. Perkin Trans. 2, pp. 2211-2218] has been redetermined in order to establish the intra- and inter-molecular inter-actions. The trans-cis geometry of the thio-urea group is stabilized by intra-molecular hydrogen bonding between the carbonyl and cis-thio-amide groups, resulting in a pseudo-S(6) planar ring which makes a dihedral angle of 3.24 (6)° with the 2-furoyl group and a torsion angle of -84.3 (2)° with the cyclo-hexyl group. There is also an intra-molecular hydrogen bond between the furan O atom and the other thio-amide H atom. In the crystal structure, mol-ecules are linked by inter-molecular N-H⋯O hydrogen bonds, forming chains along [010].

Entities:  

Year:  2010        PMID: 21579158      PMCID: PMC2979067          DOI: 10.1107/S1600536810013693

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


Related literature

For general background to the applications of aroylthio­ureas in coordination chemistry and mol­ecular electronics, see: Aly et al. (2007 ▶); Koch (2001 ▶); Duque et al. (2009 ▶); Estévez-Hernández et al. (2006 ▶). For related structures, see: Estévez-Hernández et al. (2008 ▶). For the synthesis, see: Otazo-Sánchez et al. (2001 ▶).

Experimental

Crystal data

C12H16N2O2S M = 252.33 Orthorhombic, a = 7.2667 (5) Å b = 10.2058 (7) Å c = 34.239 (3) Å V = 2539.3 (3) Å3 Z = 8 Mo Kα radiation μ = 0.25 mm−1 T = 100 K 0.37 × 0.34 × 0.23 mm

Data collection

Bruker APEXII CCD diffractometer Absorption correction: multi-scan (SADABS; Sheldrick, 2008 ▶) T min = 0.914, T max = 0.946 30412 measured reflections 2232 independent reflections 2175 reflections with I > 2σ(I) R int = 0.019

Refinement

R[F 2 > 2σ(F 2)] = 0.033 wR(F 2) = 0.072 S = 1.20 2232 reflections 160 parameters H atoms treated by a mixture of independent and constrained refinement Δρmax = 0.25 e Å−3 Δρmin = −0.22 e Å−3 Data collection: APEX2 (Bruker, 2007 ▶); cell refinement: SAINT (Bruker, 2007 ▶); 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 for Windows (Farrugia, 1997 ▶) and Mercury (Macrae et al., 2008 ▶); software used to prepare material for publication: WinGX (Farrugia, 1999 ▶). Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536810013693/bq2204sup1.cif Structure factors: contains datablocks I. DOI: 10.1107/S1600536810013693/bq2204Isup2.hkl Additional supplementary materials: crystallographic information; 3D view; checkCIF report
C12H16N2O2SF(000) = 1072
Mr = 252.33Dx = 1.32 Mg m3
Orthorhombic, PbcaMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ac 2abCell parameters from 9926 reflections
a = 7.2667 (5) Åθ = 2.9–25.1°
b = 10.2058 (7) ŵ = 0.25 mm1
c = 34.239 (3) ÅT = 100 K
V = 2539.3 (3) Å3Prism, colourless
Z = 80.37 × 0.34 × 0.23 mm
Bruker APEXII CCD diffractometer2232 independent reflections
Radiation source: fine-focus sealed tube2175 reflections with I > 2σ(I)
graphiteRint = 0.019
Detector resolution: 8.333 pixels mm-1θmax = 25.0°, θmin = 2.4°
φ and ω scansh = −8→8
Absorption correction: multi-scan (SADABS; Sheldrick, 2008)k = −12→12
Tmin = 0.914, Tmax = 0.946l = −40→40
30412 measured reflections
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.033Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.072H atoms treated by a mixture of independent and constrained refinement
S = 1.20w = 1/[σ2(Fo2) + (0.0145P)2 + 2.5358P] where P = (Fo2 + 2Fc2)/3
2232 reflections(Δ/σ)max = 0.001
160 parametersΔρmax = 0.25 e Å3
0 restraintsΔρmin = −0.22 e Å3
Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes.
xyzUiso*/Ueq
S10.02582 (6)0.83305 (4)0.380695 (12)0.01791 (12)
O10.23646 (16)0.91176 (11)0.51723 (3)0.0176 (3)
O20.20639 (16)1.18582 (10)0.45356 (3)0.0175 (3)
N10.15353 (19)0.96757 (14)0.44114 (4)0.0150 (3)
N20.0950 (2)1.08928 (14)0.38546 (4)0.0166 (3)
C10.2661 (2)1.03689 (15)0.50384 (5)0.0145 (3)
C20.3595 (2)1.10760 (16)0.53071 (5)0.0179 (4)
H2A0.39781.19630.52840.022*
C30.3890 (2)1.02359 (17)0.56302 (5)0.0188 (4)
H3A0.44991.04510.58670.023*
C40.3138 (2)0.90723 (17)0.55358 (5)0.0194 (4)
H4A0.31450.83210.570.023*
C50.2064 (2)1.07079 (15)0.46440 (5)0.0142 (3)
C60.0933 (2)0.97236 (16)0.40230 (5)0.0149 (3)
C70.0241 (2)1.11541 (16)0.34625 (5)0.0158 (3)
H7A−0.08591.05840.34180.019*
C80.1656 (2)1.08560 (17)0.31451 (5)0.0195 (4)
H8A0.27621.14080.31840.023*
H8B0.20350.99260.31620.023*
C90.0824 (3)1.11309 (17)0.27440 (5)0.0213 (4)
H9A−0.0231.05350.26990.026*
H9B0.17561.09560.2540.026*
C100.0172 (2)1.25554 (18)0.27119 (5)0.0223 (4)
H10A0.12471.31490.27260.027*
H10B−0.04341.2690.24560.027*
C11−0.1176 (2)1.28941 (17)0.30388 (5)0.0218 (4)
H11A−0.23261.23890.30020.026*
H11B−0.14861.38380.30250.026*
C12−0.0375 (2)1.25877 (16)0.34414 (5)0.0175 (4)
H12A−0.13161.27560.36440.021*
H12B0.06891.31680.34930.021*
H10.167 (3)0.894 (2)0.4510 (5)0.021*
H20.139 (3)1.1503 (19)0.3985 (6)0.021*
U11U22U33U12U13U23
S10.0206 (2)0.0144 (2)0.0188 (2)−0.00266 (17)−0.00123 (16)−0.00125 (16)
O10.0224 (6)0.0128 (6)0.0175 (5)−0.0014 (5)−0.0014 (5)0.0024 (5)
O20.0222 (6)0.0114 (6)0.0190 (6)0.0007 (5)−0.0007 (5)0.0007 (5)
N10.0179 (7)0.0112 (7)0.0159 (7)0.0005 (6)−0.0013 (6)0.0024 (6)
N20.0196 (7)0.0143 (7)0.0158 (7)−0.0012 (6)−0.0026 (6)−0.0005 (6)
C10.0139 (8)0.0112 (8)0.0185 (8)0.0022 (6)0.0037 (7)0.0011 (6)
C20.0188 (8)0.0137 (8)0.0213 (8)0.0013 (7)0.0014 (7)−0.0031 (7)
C30.0172 (8)0.0234 (9)0.0159 (8)0.0036 (7)−0.0010 (7)−0.0028 (7)
C40.0219 (9)0.0221 (9)0.0141 (8)0.0032 (7)−0.0005 (7)0.0036 (7)
C50.0101 (8)0.0145 (8)0.0179 (8)0.0013 (6)0.0026 (6)−0.0013 (6)
C60.0105 (8)0.0167 (8)0.0174 (8)0.0009 (6)0.0005 (6)0.0001 (6)
C70.0157 (8)0.0159 (8)0.0159 (8)−0.0002 (7)−0.0018 (7)−0.0002 (6)
C80.0195 (8)0.0181 (8)0.0211 (8)0.0036 (7)0.0016 (7)0.0005 (7)
C90.0236 (9)0.0216 (9)0.0187 (8)0.0011 (7)0.0032 (7)−0.0021 (7)
C100.0257 (9)0.0244 (9)0.0169 (8)0.0026 (8)−0.0001 (7)0.0038 (7)
C110.0251 (9)0.0207 (8)0.0196 (8)0.0057 (7)−0.0019 (7)0.0019 (7)
C120.0191 (8)0.0170 (8)0.0165 (8)0.0029 (7)−0.0002 (7)−0.0006 (6)
S1—C61.6760 (16)C7—C81.527 (2)
O1—C41.3665 (19)C7—C121.532 (2)
O1—C11.3739 (19)C7—H7A1
O2—C51.2313 (19)C8—C91.527 (2)
N1—C51.376 (2)C8—H8A0.99
N1—C61.401 (2)C8—H8B0.99
N1—H10.83 (2)C9—C101.533 (2)
N2—C61.325 (2)C9—H9A0.99
N2—C71.462 (2)C9—H9B0.99
N2—H20.83 (2)C10—C111.527 (2)
C1—C21.352 (2)C10—H10A0.99
C1—C51.460 (2)C10—H10B0.99
C2—C31.416 (2)C11—C121.529 (2)
C2—H2A0.95C11—H11A0.99
C3—C41.346 (2)C11—H11B0.99
C3—H3A0.95C12—H12A0.99
C4—H4A0.95C12—H12B0.99
C4—O1—C1105.71 (13)C9—C8—C7109.70 (14)
C5—N1—C6127.62 (14)C9—C8—H8A109.7
C5—N1—H1115.0 (13)C7—C8—H8A109.7
C6—N1—H1117.2 (13)C9—C8—H8B109.7
C6—N2—C7124.08 (14)C7—C8—H8B109.7
C6—N2—H2116.5 (13)H8A—C8—H8B108.2
C7—N2—H2119.4 (13)C8—C9—C10111.18 (14)
C2—C1—O1110.36 (14)C8—C9—H9A109.4
C2—C1—C5130.70 (15)C10—C9—H9A109.4
O1—C1—C5118.84 (13)C8—C9—H9B109.4
C1—C2—C3106.52 (15)C10—C9—H9B109.4
C1—C2—H2A126.7H9A—C9—H9B108
C3—C2—H2A126.7C11—C10—C9111.13 (14)
C4—C3—C2106.57 (15)C11—C10—H10A109.4
C4—C3—H3A126.7C9—C10—H10A109.4
C2—C3—H3A126.7C11—C10—H10B109.4
C3—C4—O1110.83 (15)C9—C10—H10B109.4
C3—C4—H4A124.6H10A—C10—H10B108
O1—C4—H4A124.6C10—C11—C12111.76 (14)
O2—C5—N1123.74 (15)C10—C11—H11A109.3
O2—C5—C1120.34 (14)C12—C11—H11A109.3
N1—C5—C1115.92 (14)C10—C11—H11B109.3
N2—C6—N1116.20 (14)C12—C11—H11B109.3
N2—C6—S1125.06 (12)H11A—C11—H11B107.9
N1—C6—S1118.74 (12)C11—C12—C7110.44 (13)
N2—C7—C8112.33 (13)C11—C12—H12A109.6
N2—C7—C12108.69 (13)C7—C12—H12A109.6
C8—C7—C12110.71 (13)C11—C12—H12B109.6
N2—C7—H7A108.3C7—C12—H12B109.6
C8—C7—H7A108.3H12A—C12—H12B108.1
C12—C7—H7A108.3
C4—O1—C1—C20.37 (17)C7—N2—C6—S15.0 (2)
C4—O1—C1—C5177.02 (14)C5—N1—C6—N23.2 (2)
O1—C1—C2—C3−0.65 (18)C5—N1—C6—S1−176.93 (13)
C5—C1—C2—C3−176.78 (16)C6—N2—C7—C8−84.29 (19)
C1—C2—C3—C40.68 (19)C6—N2—C7—C12152.86 (15)
C2—C3—C4—O1−0.47 (19)N2—C7—C8—C9179.24 (14)
C1—O1—C4—C30.08 (18)C12—C7—C8—C9−59.05 (18)
C6—N1—C5—O20.4 (3)C7—C8—C9—C1057.79 (19)
C6—N1—C5—C1−179.07 (15)C8—C9—C10—C11−55.4 (2)
C2—C1—C5—O2−14.7 (3)C9—C10—C11—C1253.9 (2)
O1—C1—C5—O2169.45 (14)C10—C11—C12—C7−55.05 (19)
C2—C1—C5—N1164.83 (17)N2—C7—C12—C11−178.47 (13)
O1—C1—C5—N1−11.0 (2)C8—C7—C12—C1157.71 (18)
C7—N2—C6—N1−175.11 (14)
D—H···AD—HH···AD···AD—H···A
N1—H1···O10.83 (2)2.329 (19)2.7342 (17)110.8 (16)
N1—H1···O2i0.83 (2)2.32 (2)3.0799 (18)153.0 (18)
N2—H2···O20.83 (2)1.983 (19)2.6574 (18)138.0 (18)
Table 1

Hydrogen-bond geometry (Å, °)

D—H⋯AD—HH⋯ADAD—H⋯A
N1—H1⋯O10.83 (2)2.329 (19)2.7342 (17)110.8 (16)
N1—H1⋯O2i0.83 (2)2.32 (2)3.0799 (18)153.0 (18)
N2—H2⋯O20.83 (2)1.983 (19)2.6574 (18)138.0 (18)

Symmetry code: (i) .

  3 in total

1.  A short history of SHELX.

Authors:  George M Sheldrick
Journal:  Acta Crystallogr A       Date:  2007-12-21       Impact factor: 2.290

2.  Novel CdCl2 and HgCl2 complexes with 3-monosubstituted and 3,3-disubstituted 1-furoylthioureas: IR and Raman spectra.

Authors:  O Estévez-Hernández; E Otazo-Sánchez; J L Hidalgo-Hidalgo de Cisneros; I Naranjo-Rodríguez; E Reguera
Journal:  Spectrochim Acta A Mol Biomol Spectrosc       Date:  2005-12-05       Impact factor: 4.098

3.  1-Furfuryl-3-furoylthio-urea.

Authors:  O Estévez-Hernández; J Duque; J Ellena; Rodrigo S Corrêa
Journal:  Acta Crystallogr Sect E Struct Rep Online       Date:  2008-05-24
  3 in total

北京卡尤迪生物科技股份有限公司 © 2022-2023.