Supporting information
Crystallographic Information File (CIF) https://doi.org/10.1107/S205322961402244X/sk3568sup1.cif | |
Structure factor file (CIF format) https://doi.org/10.1107/S205322961402244X/sk3568Isup2.hkl | |
Chemical Markup Language (CML) file https://doi.org/10.1107/S205322961402244X/sk3568Isup3.cml |
CCDC reference: 1028769
Isothiourea derivatives exhibit a range of biological behaviour, including pharmacological activity on the central nervous system (Harada et al., 2004; Witkin & Nelson, 2004; Montes et al., 2005) and action as potent inhibitors of various enzyme systems (Di Giacomo et al., 2003; Witkin & Nelson, 2004), including nitric oxide synthase (Di Giacomo et al., 2003; Basaran et al., 2005; Oliveira et al., 2011). S-Alkylisothioureas, such as S-methylisothiourea and S-(3-dimethylaminopropyl)isothiourea (dimaprit) are two of the inhibitors most commonly used against nitric oxide synthase (Basaran et al., 2005; Oliveira et al., 2011), while the N,S-dialkylisothiourea clobenpropit (Harada et al., 2004) can be used as an anticonvulsant. In synthesis, pyrazolylisothioureas have been used as intermediates in the preparation of pyrazolo[1,5-a][1,3,5]triazines (Insuasty, Estrada, Cobo et al., 2006; Insuasty, Estrada, Cortés et al., 2006; Insuasty et al., 2012), which are important as analogues of known antidepressant (Gilligan et al., 2009; Saito et al., 2011), anti-inflammatory (Raboisson et al., 2008), antitumoural (Popowycz et al., 2009) and antiviral agents (Gudmundsson et al., 2009). With these considerations in mind, we have now prepared 2-ethyl-1-[5-(4-methylphenyl)pyrazol-3-yl]-3-(thiophen-2-carbonyl)isothiourea, (I) (see Scheme 1) whose structure we report here.
A mixture of S,S-diethyl 2-thenoylimidothiocarbonate (0.015 mol) and 5-amino-3-(4-methylphenyl)-1H-pyrazole (0.015 mol) was subjected to microwave irradiation in the absence of solvent (maximum power 300 W, for 3 min at a temperature of 433 K), using a focused microwave reactor (CEM Discover). When the reaction was complete, as indicated by thin-layer chromatography, the crude product was dissolved in chloroform (3.0 ml) and purified by column chromatography on silica gel, using a mixture of hexanes and ethyl acetate (4:1 v/v) as eluent to give the title compound, (I). After removal of the solvent under reduced pressure, crystallization from ethyl acetate, at ambient temperature and in the presence of air, provided colourless crystals suitable for single-crystal X-ray diffraction (yield 51%, m.p. 404 K).
Crystal data, data collection and structure refinement details are summarized in Table 1. H atoms were located in difference maps. H atoms bonded to C atoms were subsequently treated as riding atoms in geometrically idealized positions, with C—H = 0.95 (aromatic and heterocyclic), 0.98 (CH3) or 0.99 Å (CH2), and with Uiso(H) = kUeq(C) where k = 1.5 for the methyl groups, which were permitted to rotate but not to tilt, and 1.2 for all other H atoms bonded to C atoms. For H atoms bonded to N atoms, the atomic coordinates were refined with Uiso(H) = 1.2Ueq(N), giving the N—H distances shown in Table 3. Four low-angle reflections (011, 110, 110 and 111), which had been attenuated by the beam stop, were omitted from the refinements. Examination of the refined structure at this stage revealed some unsatisfactory interatomic distances in the thiophene unit: the two C—C double-bond distances were very different [1.511 (6) Å for C32—C33 and 1.357 (7) Å for C34—C35] and the former of these appeared to be significantly larger than the formal single-bond distance [C33—C34 = 1.490 (6) Å]. In addition, the largest peak in the difference map was close to atom C33 and the deepest hole was close to atom S31. Accordingly, the thiophene unit was modelled using two sets of atomic sites, related to one another by a rotation of approximately 180° around the C31—C32 bond. For the minor-disorder component, the bonded distances and the one-angle non-bonded distances were restrained to be the same as the corresponding distances in the major component, subject to uncertainties of 0.005 Å and 0.01 Å, respectively. The H atoms of the minor component were included in the refinement in calculated positions, with C—H = 0.95 Å and Uiso(H) = 1.2Ueq(C), and the anisotropic displacement parameters for pairs of atoms occupying approximately the same regions of space were constrained to be identical. Subject to these conditions, the site occupancies of the two components refined to 0.814 (4) and 0.286 (4), respectively, with a dihedral angle between their mean planes of 4.4 (14)°.
The title isothiourea, (I), was synthesized by the reaction between S,S-diethyl thenoylimidodithiocarbonate, (A) (see Scheme 1), and 5-amino-3-(4-methylphenyl)-1H-pyrazole, (B), using a brief period of microwave irradiation under solvent-free conditions. The reaction proceeds by elimination of ethanethiol which is a gas under the reaction conditions employed (b.p. 308 K), and the formation of this volatile by-product and its loss from the reaction system undoubtedly provides an effective entropic driver for the formation of (I). The aims of this study were not only the confirmation of the molecular constitution of compound (I) but also the determination of its conformation and the mode of supramolecular assembly. The structure analysis found no indication whatever of the presence of any of the other possible conformations, in particular the conformation (Ib) (see Scheme 2) or of any of its tautomers, which would be a necessary precursor for the formation of the potential condensation product, the pyrazolo[1,5-a][1,3,5]triazine, (II), although such bicyclic products are readily obtained when solutions of N-substituted S,S-diethyl imidodithiocarbonates and 5-amino-1H-pyrazoles in N,N-dimethylformamide are heated under reflux (Insuasty, Estrada, Cobo et al., 2006; Insuasty, Insuasty et al., 2012).
The central spacer unit between atoms C13 and C32 is very nearly planar, as indicated by the relevant torsion angles (Table 2). For the atoms forming the spacer unit, the maximum deviation from their mean plane is 0.025 (2) Å for atom N1, with an r.m.s. deviation of 0.014 Å. Associated with this near planarity, the structure contains an intramolecular N—H···O hydrogen bond (Table 3), forming an S(6) motif (Bernstein et al., 1995). The dihedral angles between the plane of the spacer unit and the pyrazole ring, and the major component of the disordered thiophene ring are 58.82 (13) and 10.0 (6)°, respectively, while that between the pyrazole and phenyl rings is 19.96 (18)°. Accordingly, molecules of (I) exhibit no internal symmetry and so they are conformationally chiral: the centrosymmetric space group accommodates equal numbers of the two conformational enantiomers, although the conformational chirality has no chemical significance. It seems likely that the conformation is influenced by the presence of the intramolecular hydrogen bond, as this is likely to be absent from conformations such as (Ib) (see Scheme 2).
The bond distances in the molecule of (I) (Table 2) present some interesting features. In the central spacer unit, the distances for N1—C2 and C2—N3, which are formally single and double bonds, respectively, differ by less than 0.025 Å, while the formal single bond N3—C31 is somewhat shorted than the single bond N1—C13, and the carbonyl bond C31—O31 is typical of those in simple amides [mean value (Allen et al., 1987) 1.231 Å, upper quartile value 1.238 Å], where considerable electronic delocalization can occur. These observations, taken together, indicate that the polarized form (Ia) (see Scheme 1) is a significant contributor to the overall electronic structure in addition to the classical form (I), and that the intramolecular N—H···O hydrogen bond should be regarded as charge-assisted (Gilli et al., 1994). Within the pyrazole ring, the distances (Table 2) for N11—C15 and N12—C1, which are formally single and double bonds, respectively, differ by less than 0.02 Å, as do those for C13—C14 and C14—C15, which again are formally single and double bonds. These observations indicate a significant degree of aromatic type delocalization within the pyrazole ring, cf. (Ia), although the large dihedral angle between the pyrazole ring and the central spacer unit effectively rules out the possibility of any more extended conjugation.
The supramolecular assembly in compound (I) is fairly simple and depends upon only two hydrogen bonds, one each of the N—H···N and N—H···O types (Table 3). An inversion-related pair of molecules is linked by N—H···N hydrogen bonds to form a centrosymmetric dimer, centred at (1/2, 1/2, 1/2) and characterized by an R22(6) motif (Fig. 2). The N1—H1 bond participates in an almost-planar charge-assisted three-centre N—H···(O)2 system, where one component is the intramolecular hydrogen bond mentioned above and where the other component links an inversion-related pair of molecules in a centrosymmetric R22(4) motif centred at (1/2, 0, 1/2) and flanked by an inversion-related pair of S(6) rings (Fig. 2). The combination of these motifs generates a molecular ribbon, or chain of rings, in which the R22(4) centred at (1/2, n, 1/2) alternate with the R22(6) rings centred at (1/2, n+1/2, 1/2), where n represents an integer in each case (Fig. 2). One ribbon of this type passes through each unit cell, but there are no significant direction-specific interactions between adjacent ribbons.
There are, however, three intermolecular C—H···π contacts in the structure of (I) (Table 3), but none of them can be regarded as structurally significant. One of them involves an aliphatic C—H bond of low acidity, while the C—H bonds in the other two contacts are components of the disordered thiophene unit. The contacts involving atoms C21 and C44 have very long H···centroid and C···centroid distances, while that involving atom C32 has a very narrow C—H···centroid angle (cf. Wood et al., 2009).
It is of interest briefly to compare both the conformation and the supramolecular assembly in compound (I) with the corresponding behaviour of the tris-substituted isothiourea compound (III) (Sudha et al., 1996) (see Scheme 2). In compound (III), the orientation of both N-aryl substituents differs from the N-substituents in (I) and this may, in part, be a consequence of the intramolecular N—H···N contact. However, in view of the rather small N—H···N angle here, 123 (2)°, this contact would probably not now be regarded as an effective hydrogen bond (cf. Wood et al., 2009). On the other hand, the structure of (III) contains a fairly short C—H···π(arene) hydrogen bond, unremarked in the original structure report (Sudha et al., 1996), with dimensions H···Cg = 2.68 (3) Å, C···Cg = 3.600 (3) Å and C—H···Cg 162 (3)° (Cg is the centroid of the arene ring [addition OK?]), which links molecules related by a 21 screw axis into chains running parallel to the [010] direction (Fig. 3). There are, however, no N—H···O hydrogen bonds or intermolecular N—H···N hydrogen bonds in the structure of compound (III); neither (I) nor (III) contains and aromatic π–π stacking interactions, possibly because these are effectively prevented by the methyl substituents on the aryl rings.
For related literature, see: Allen et al. (1987); Basaran et al. (2005); Bernstein et al. (1995); Di Giacomo, Sorrenti, Salerno, Cardile, Guerrera, Siracusa, Avitabile & Vanella (2003); Gilli et al. (1994); Gilligan et al. (2009); Gudmundsson et al. (2009); Harada et al. (2004); Insuasty et al. (2012); Insuasty, Estrada, Cobo, Low & Glidewell (2006); Insuasty, Estrada, Cortés, Quiroga, Insuasty, Abonía, Nogueras & Cobo (2006); Montes et al. (2005); Oliveira et al. (2011); Popowycz et al. (2009); Raboisson et al. (2008); Saito et al. (2011); Sudha et al. (1996); Witkin & Nelson (2004); Wood et al. (2009).
Data collection: COLLECT (Hooft, 1999); cell refinement: DIRAX/LSQ (Duisenberg et al., 2000); data reduction: EVALCCD (Duisenberg et al., 2003); program(s) used to solve structure: SIR2011 (Burla et al., 2012); program(s) used to refine structure: SHELXL2014 (Sheldrick, 2008, 2014); molecular graphics: PLATON (Spek, 2009); software used to prepare material for publication: SHELXL2014 (Sheldrick, 2008, 2014) and PLATON (Spek, 2009).
C18H18N4OS2 | Z = 2 |
Mr = 370.48 | F(000) = 388 |
Triclinic, P1 | Dx = 1.366 Mg m−3 |
a = 7.998 (2) Å | Mo Kα radiation, λ = 0.71073 Å |
b = 11.085 (3) Å | Cell parameters from 4118 reflections |
c = 11.696 (2) Å | θ = 3.1–27.5° |
α = 61.92 (2)° | µ = 0.31 mm−1 |
β = 84.921 (18)° | T = 120 K |
γ = 79.928 (19)° | Block, colourless |
V = 900.8 (4) Å3 | 0.36 × 0.32 × 0.22 mm |
Bruker–Nonius KappaCCD diffractometer | 4114 independent reflections |
Radiation source: Bruker-Nonius FR591 rotating anode | 2350 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.097 |
Detector resolution: 9.091 pixels mm-1 | θmax = 27.5°, θmin = 3.5° |
ϕ and ω scans | h = −10→10 |
Absorption correction: multi-scan (SADABS; Sheldrick, 2003) | k = −14→14 |
Tmin = 0.835, Tmax = 0.934 | l = −14→15 |
12759 measured reflections |
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)] = 0.057 | Hydrogen site location: mixed |
wR(F2) = 0.119 | H atoms treated by a mixture of independent and constrained refinement |
S = 1.02 | w = 1/[σ2(Fo2) + (0.0281P)2 + 0.6991P] where P = (Fo2 + 2Fc2)/3 |
4114 reflections | (Δ/σ)max < 0.001 |
247 parameters | Δρmax = 0.30 e Å−3 |
10 restraints | Δρmin = −0.37 e Å−3 |
C18H18N4OS2 | γ = 79.928 (19)° |
Mr = 370.48 | V = 900.8 (4) Å3 |
Triclinic, P1 | Z = 2 |
a = 7.998 (2) Å | Mo Kα radiation |
b = 11.085 (3) Å | µ = 0.31 mm−1 |
c = 11.696 (2) Å | T = 120 K |
α = 61.92 (2)° | 0.36 × 0.32 × 0.22 mm |
β = 84.921 (18)° |
Bruker–Nonius KappaCCD diffractometer | 4114 independent reflections |
Absorption correction: multi-scan (SADABS; Sheldrick, 2003) | 2350 reflections with I > 2σ(I) |
Tmin = 0.835, Tmax = 0.934 | Rint = 0.097 |
12759 measured reflections |
R[F2 > 2σ(F2)] = 0.057 | 10 restraints |
wR(F2) = 0.119 | H atoms treated by a mixture of independent and constrained refinement |
S = 1.02 | Δρmax = 0.30 e Å−3 |
4114 reflections | Δρmin = −0.37 e Å−3 |
247 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. |
x | y | z | Uiso*/Ueq | Occ. (<1) | |
N1 | 0.3279 (3) | 0.2082 (3) | 0.4701 (3) | 0.0225 (6) | |
H1 | 0.368 (4) | 0.135 (3) | 0.461 (3) | 0.027* | |
C2 | 0.1951 (4) | 0.1888 (3) | 0.5529 (3) | 0.0213 (7) | |
N3 | 0.1319 (3) | 0.0718 (3) | 0.6188 (3) | 0.0218 (6) | |
N11 | 0.5020 (3) | 0.5098 (3) | 0.3601 (2) | 0.0206 (6) | |
H11 | 0.536 (4) | 0.567 (3) | 0.386 (3) | 0.025* | |
N12 | 0.4531 (3) | 0.3925 (3) | 0.4597 (2) | 0.0219 (6) | |
C13 | 0.3919 (4) | 0.3340 (3) | 0.3977 (3) | 0.0202 (7) | |
C14 | 0.4022 (4) | 0.4109 (3) | 0.2628 (3) | 0.0211 (7) | |
H14 | 0.3681 | 0.3892 | 0.1997 | 0.025* | |
C15 | 0.4728 (4) | 0.5251 (3) | 0.2411 (3) | 0.0188 (6) | |
C151 | 0.5089 (4) | 0.6473 (3) | 0.1196 (3) | 0.0210 (7) | |
C152 | 0.6171 (4) | 0.7337 (3) | 0.1179 (3) | 0.0240 (7) | |
H152 | 0.6769 | 0.7104 | 0.1939 | 0.029* | |
C153 | 0.6378 (4) | 0.8549 (3) | 0.0045 (3) | 0.0253 (7) | |
H153 | 0.7113 | 0.9132 | 0.0053 | 0.030* | |
C154 | 0.5537 (4) | 0.8929 (3) | −0.1101 (3) | 0.0239 (7) | |
C155 | 0.4511 (4) | 0.8038 (3) | −0.1086 (3) | 0.0297 (8) | |
H155 | 0.3959 | 0.8249 | −0.1859 | 0.036* | |
C156 | 0.4272 (4) | 0.6840 (4) | 0.0040 (3) | 0.0292 (8) | |
H156 | 0.3540 | 0.6258 | 0.0025 | 0.035* | |
C157 | 0.5691 (5) | 1.0279 (3) | −0.2324 (3) | 0.0321 (8) | |
H17A | 0.6452 | 1.0786 | −0.2163 | 0.048* | |
H17B | 0.4567 | 1.0842 | −0.2565 | 0.048* | |
H17C | 0.6154 | 1.0077 | −0.3030 | 0.048* | |
S21 | 0.10176 (10) | 0.33474 (8) | 0.57279 (9) | 0.0270 (2) | |
C21 | −0.0845 (4) | 0.2748 (3) | 0.6694 (3) | 0.0296 (8) | |
H21A | −0.1734 | 0.3556 | 0.6521 | 0.035* | |
H21B | −0.1290 | 0.2145 | 0.6421 | 0.035* | |
C22 | −0.0503 (5) | 0.1948 (4) | 0.8151 (3) | 0.0372 (9) | |
H22A | 0.0272 | 0.1087 | 0.8345 | 0.056* | |
H22B | −0.1576 | 0.1730 | 0.8622 | 0.056* | |
H22C | 0.0013 | 0.2513 | 0.8420 | 0.056* | |
C31 | 0.1990 (4) | −0.0419 (3) | 0.6018 (3) | 0.0226 (7) | |
O31 | 0.3184 (3) | −0.0511 (2) | 0.5300 (2) | 0.0288 (6) | |
S31 | −0.0260 (2) | −0.16440 (14) | 0.80208 (15) | 0.0293 (4) | 0.814 (4) |
C32 | 0.1148 (4) | −0.1636 (3) | 0.6839 (3) | 0.0220 (7) | 0.814 (4) |
C33 | 0.1415 (18) | −0.2895 (10) | 0.6845 (11) | 0.0244 (14) | 0.814 (4) |
H33 | 0.2155 | −0.3091 | 0.6252 | 0.029* | 0.814 (4) |
C34 | 0.0486 (16) | −0.3870 (8) | 0.7817 (13) | 0.0351 (15) | 0.814 (4) |
H34 | 0.0508 | −0.4784 | 0.7942 | 0.042* | 0.814 (4) |
C35 | −0.0448 (8) | −0.3341 (5) | 0.8557 (6) | 0.0302 (16) | 0.814 (4) |
H35 | −0.1121 | −0.3852 | 0.9281 | 0.036* | 0.814 (4) |
S41 | 0.155 (2) | −0.3061 (11) | 0.6610 (13) | 0.0244 (14) | 0.186 (4) |
C42 | 0.1148 (4) | −0.1636 (3) | 0.6839 (3) | 0.0220 (7) | 0.186 (4) |
C43 | −0.007 (4) | −0.179 (2) | 0.778 (3) | 0.0293 (4) | 0.186 (4) |
H43 | −0.0481 | −0.1090 | 0.8034 | 0.035* | 0.186 (4) |
C44 | −0.065 (4) | −0.308 (2) | 0.833 (3) | 0.0302 (16) | 0.186 (4) |
H44 | −0.1553 | −0.3323 | 0.8944 | 0.036* | 0.186 (4) |
C45 | 0.024 (8) | −0.393 (3) | 0.787 (6) | 0.0351 (15) | 0.186 (4) |
H45 | 0.0139 | −0.4874 | 0.8198 | 0.042* | 0.186 (4) |
U11 | U22 | U33 | U12 | U13 | U23 | |
N1 | 0.0217 (14) | 0.0204 (14) | 0.0265 (15) | −0.0055 (11) | 0.0088 (11) | −0.0126 (12) |
C2 | 0.0187 (15) | 0.0241 (17) | 0.0220 (17) | −0.0037 (12) | 0.0021 (13) | −0.0115 (14) |
N3 | 0.0197 (13) | 0.0194 (14) | 0.0258 (15) | −0.0045 (10) | 0.0038 (11) | −0.0103 (12) |
N11 | 0.0242 (14) | 0.0200 (14) | 0.0201 (14) | −0.0081 (11) | 0.0053 (11) | −0.0107 (12) |
N12 | 0.0235 (13) | 0.0204 (14) | 0.0224 (14) | −0.0088 (11) | 0.0085 (11) | −0.0099 (12) |
C13 | 0.0156 (14) | 0.0215 (17) | 0.0263 (17) | −0.0049 (12) | 0.0054 (13) | −0.0137 (14) |
C14 | 0.0225 (15) | 0.0254 (17) | 0.0189 (16) | −0.0059 (13) | 0.0026 (13) | −0.0127 (14) |
C15 | 0.0157 (14) | 0.0223 (17) | 0.0196 (16) | −0.0041 (12) | 0.0027 (12) | −0.0108 (13) |
C151 | 0.0201 (15) | 0.0263 (17) | 0.0197 (16) | −0.0033 (12) | 0.0045 (13) | −0.0140 (14) |
C152 | 0.0253 (16) | 0.0264 (18) | 0.0213 (17) | −0.0067 (13) | −0.0008 (14) | −0.0108 (14) |
C153 | 0.0267 (17) | 0.0271 (18) | 0.0239 (18) | −0.0103 (13) | 0.0029 (14) | −0.0116 (15) |
C154 | 0.0241 (16) | 0.0284 (18) | 0.0181 (16) | −0.0020 (13) | 0.0036 (13) | −0.0112 (14) |
C155 | 0.0327 (18) | 0.036 (2) | 0.0186 (17) | −0.0100 (15) | −0.0045 (14) | −0.0086 (15) |
C156 | 0.0294 (18) | 0.036 (2) | 0.0278 (19) | −0.0176 (15) | 0.0033 (15) | −0.0156 (16) |
C157 | 0.039 (2) | 0.030 (2) | 0.0221 (18) | −0.0072 (15) | 0.0002 (16) | −0.0074 (15) |
S21 | 0.0248 (4) | 0.0202 (4) | 0.0355 (5) | −0.0048 (3) | 0.0100 (4) | −0.0138 (4) |
C21 | 0.0186 (16) | 0.0303 (19) | 0.038 (2) | −0.0041 (13) | 0.0111 (15) | −0.0164 (16) |
C22 | 0.037 (2) | 0.043 (2) | 0.038 (2) | −0.0151 (17) | 0.0150 (17) | −0.0230 (19) |
C31 | 0.0222 (16) | 0.0235 (17) | 0.0234 (17) | −0.0043 (13) | −0.0010 (14) | −0.0115 (14) |
O31 | 0.0290 (12) | 0.0270 (13) | 0.0348 (14) | −0.0087 (10) | 0.0134 (11) | −0.0187 (11) |
S31 | 0.0265 (6) | 0.0287 (6) | 0.0332 (8) | −0.0109 (5) | 0.0107 (5) | −0.0143 (5) |
C32 | 0.0169 (15) | 0.0246 (17) | 0.0260 (18) | −0.0049 (12) | −0.0005 (13) | −0.0122 (14) |
C33 | 0.024 (2) | 0.024 (2) | 0.034 (4) | −0.0034 (19) | 0.007 (2) | −0.0220 (15) |
C34 | 0.033 (5) | 0.022 (2) | 0.050 (3) | −0.0098 (16) | −0.003 (2) | −0.014 (2) |
C35 | 0.028 (3) | 0.020 (3) | 0.030 (3) | −0.009 (2) | 0.000 (3) | 0.000 (3) |
S41 | 0.024 (2) | 0.024 (2) | 0.034 (4) | −0.0034 (19) | 0.007 (2) | −0.0220 (15) |
C42 | 0.0169 (15) | 0.0246 (17) | 0.0260 (18) | −0.0049 (12) | −0.0005 (13) | −0.0122 (14) |
C43 | 0.0265 (6) | 0.0287 (6) | 0.0332 (8) | −0.0109 (5) | 0.0107 (5) | −0.0143 (5) |
C44 | 0.028 (3) | 0.020 (3) | 0.030 (3) | −0.009 (2) | 0.000 (3) | 0.000 (3) |
C45 | 0.033 (5) | 0.022 (2) | 0.050 (3) | −0.0098 (16) | −0.003 (2) | −0.014 (2) |
N1—C2 | 1.347 (4) | C157—H17A | 0.9800 |
N1—H1 | 0.87 (3) | C157—H17B | 0.9800 |
C2—N3 | 1.323 (4) | C157—H17C | 0.9800 |
C2—S21 | 1.768 (3) | S21—C21 | 1.811 (3) |
N3—C31 | 1.377 (4) | C21—C22 | 1.530 (5) |
C31—O31 | 1.238 (3) | C21—H21A | 0.9900 |
N1—C13 | 1.408 (4) | C21—H21B | 0.9900 |
N11—N12 | 1.368 (3) | C22—H22A | 0.9800 |
N11—H11 | 0.91 (3) | C22—H22B | 0.9800 |
N12—C13 | 1.343 (4) | C22—H22C | 0.9800 |
C13—C14 | 1.399 (4) | C31—C32 | 1.477 (4) |
C14—C15 | 1.381 (4) | S31—C32 | 1.701 (3) |
C15—N11 | 1.357 (4) | C32—C33 | 1.370 (8) |
C14—H14 | 0.9500 | C33—C34 | 1.410 (10) |
C15—C151 | 1.480 (4) | C33—H33 | 0.9500 |
C151—C152 | 1.392 (4) | C34—C35 | 1.364 (5) |
C151—C156 | 1.402 (5) | C35—S31 | 1.710 (5) |
C152—C153 | 1.397 (4) | C34—H34 | 0.9500 |
C152—H152 | 0.9500 | C35—H35 | 0.9500 |
C153—C154 | 1.399 (5) | S41—C45 | 1.711 (7) |
C153—H153 | 0.9500 | C43—C44 | 1.410 (11) |
C154—C155 | 1.384 (4) | C43—H43 | 0.9500 |
C154—C157 | 1.522 (4) | C44—C45 | 1.365 (7) |
C155—C156 | 1.390 (4) | C44—H44 | 0.9500 |
C155—H155 | 0.9500 | C45—H45 | 0.9500 |
C156—H156 | 0.9500 | ||
C2—N1—C13 | 125.3 (3) | H17A—C157—H17B | 109.5 |
C2—N1—H1 | 113 (2) | C154—C157—H17C | 109.5 |
C13—N1—H1 | 122 (2) | H17A—C157—H17C | 109.5 |
N3—C2—N1 | 125.5 (3) | H17B—C157—H17C | 109.5 |
N3—C2—S21 | 118.9 (2) | C2—S21—C21 | 101.66 (15) |
N1—C2—S21 | 115.5 (2) | C22—C21—S21 | 113.5 (2) |
C2—N3—C31 | 120.0 (2) | C22—C21—H21A | 108.9 |
C15—N11—N12 | 113.5 (3) | S21—C21—H21A | 108.9 |
C15—N11—H11 | 132 (2) | C22—C21—H21B | 108.9 |
N12—N11—H11 | 114 (2) | S21—C21—H21B | 108.9 |
C13—N12—N11 | 102.9 (2) | H21A—C21—H21B | 107.7 |
N12—C13—C14 | 112.6 (3) | C21—C22—H22A | 109.5 |
N12—C13—N1 | 119.5 (3) | C21—C22—H22B | 109.5 |
C14—C13—N1 | 127.9 (3) | H22A—C22—H22B | 109.5 |
C15—C14—C13 | 105.2 (3) | C21—C22—H22C | 109.5 |
C15—C14—H14 | 127.4 | H22A—C22—H22C | 109.5 |
C13—C14—H14 | 127.4 | H22B—C22—H22C | 109.5 |
N11—C15—C14 | 105.9 (3) | O31—C31—N3 | 127.6 (3) |
N11—C15—C151 | 122.8 (3) | O31—C31—C32 | 119.7 (3) |
C14—C15—C151 | 131.3 (3) | N3—C31—C32 | 112.7 (2) |
C152—C151—C156 | 117.9 (3) | C32—S31—C35 | 92.3 (2) |
C152—C151—C15 | 121.2 (3) | C33—C32—C31 | 127.9 (5) |
C156—C151—C15 | 120.9 (3) | C33—C32—S31 | 110.8 (4) |
C151—C152—C153 | 120.1 (3) | C31—C32—S31 | 121.3 (2) |
C151—C152—H152 | 119.9 | C32—C33—C34 | 113.4 (5) |
C153—C152—H152 | 119.9 | C32—C33—H33 | 123.3 |
C152—C153—C154 | 122.0 (3) | C34—C33—H33 | 123.3 |
C152—C153—H153 | 119.0 | C35—C34—C33 | 111.7 (5) |
C154—C153—H153 | 119.0 | C35—C34—H34 | 124.2 |
C155—C154—C153 | 117.4 (3) | C33—C34—H34 | 124.2 |
C155—C154—C157 | 120.2 (3) | C34—C35—S31 | 111.7 (4) |
C153—C154—C157 | 122.4 (3) | C34—C35—H35 | 124.1 |
C154—C155—C156 | 121.2 (3) | S31—C35—H35 | 124.1 |
C154—C155—H155 | 119.4 | C44—C43—H43 | 123.4 |
C156—C155—H155 | 119.4 | C45—C44—C43 | 111.6 (8) |
C155—C156—C151 | 121.3 (3) | C45—C44—H44 | 124.2 |
C155—C156—H156 | 119.3 | C43—C44—H44 | 124.2 |
C151—C156—H156 | 119.3 | C44—C45—S41 | 111.3 (8) |
C154—C157—H17A | 109.5 | C44—C45—H45 | 124.3 |
C154—C157—H17B | 109.5 | S41—C45—H45 | 124.3 |
N1—C2—N3—C31 | −2.4 (5) | C14—C15—C151—C156 | 19.5 (5) |
C2—N3—C31—O31 | 0.7 (5) | C156—C151—C152—C153 | 1.8 (4) |
C2—N3—C31—C32 | 179.3 (3) | C15—C151—C152—C153 | −174.5 (3) |
N3—C2—N1—C13 | 178.2 (3) | C151—C152—C153—C154 | −0.6 (5) |
C13—N1—C2—S21 | −2.0 (4) | C152—C153—C154—C155 | −1.6 (5) |
C2—N1—C13—N12 | 61.4 (4) | C152—C153—C154—C157 | 177.1 (3) |
N3—C31—C32—S31 | −9.3 (4) | C153—C154—C155—C156 | 2.5 (5) |
N11—C15—C151—C152 | 18.3 (4) | C157—C154—C155—C156 | −176.2 (3) |
N1—C2—S21—C21 | 172.1 (3) | C154—C155—C156—C151 | −1.3 (5) |
C2—S21—C21—C22 | 85.9 (3) | C152—C151—C156—C155 | −0.9 (5) |
S21—C2—N3—C31 | 177.9 (2) | C15—C151—C156—C155 | 175.4 (3) |
C15—N11—N12—C13 | 0.2 (3) | N3—C2—S21—C21 | −8.1 (3) |
N11—N12—C13—C14 | 0.4 (3) | O31—C31—C32—C33 | −6.3 (9) |
N11—N12—C13—N1 | −179.9 (2) | N3—C31—C32—C33 | 175.0 (8) |
C2—N1—C13—C14 | −118.9 (4) | O31—C31—C32—S31 | 169.4 (3) |
N12—C13—C14—C15 | −0.8 (3) | C35—S31—C32—C33 | 1.6 (7) |
N1—C13—C14—C15 | 179.5 (3) | C35—S31—C32—C31 | −174.7 (4) |
N12—N11—C15—C14 | −0.7 (3) | C31—C32—C33—C34 | 175.6 (9) |
N12—N11—C15—C151 | 177.3 (3) | S31—C32—C33—C34 | −0.4 (14) |
C13—C14—C15—N11 | 0.8 (3) | C32—C33—C34—C35 | −1.4 (18) |
C13—C14—C15—C151 | −176.9 (3) | C33—C34—C35—S31 | 2.6 (15) |
C14—C15—C151—C152 | −164.3 (3) | C32—S31—C35—C34 | −2.5 (9) |
N11—C15—C151—C156 | −158.0 (3) | C43—C44—C45—S41 | −9 (7) |
D—H···A | D—H | H···A | D···A | D—H···A |
N1—H1···O31 | 0.87 (4) | 1.93 (4) | 2.632 (4) | 137 (3) |
N1—H1···O31i | 0.87 (4) | 2.51 (3) | 3.052 (4) | 121 (3) |
N11—H11···N12ii | 0.91 (4) | 2.07 (3) | 2.857 (4) | 145 (3) |
C21—H21A···Cg1iii | 0.99 | 2.90 | 3.879 (4) | 169 |
C33—H33···Cg1i | 0.95 | 2.80 | 3.481 (14) | 129 |
C44—H44···Cg2iv | 0.95 | 3.00 | 3.82 (3) | 147 |
Symmetry codes: (i) −x+1, −y, −z+1; (ii) −x+1, −y+1, −z+1; (iii) −x, −y+1, −z+1; (iv) x−1, y−1, z+1. |
Experimental details
Crystal data | |
Chemical formula | C18H18N4OS2 |
Mr | 370.48 |
Crystal system, space group | Triclinic, P1 |
Temperature (K) | 120 |
a, b, c (Å) | 7.998 (2), 11.085 (3), 11.696 (2) |
α, β, γ (°) | 61.92 (2), 84.921 (18), 79.928 (19) |
V (Å3) | 900.8 (4) |
Z | 2 |
Radiation type | Mo Kα |
µ (mm−1) | 0.31 |
Crystal size (mm) | 0.36 × 0.32 × 0.22 |
Data collection | |
Diffractometer | Bruker–Nonius KappaCCD diffractometer |
Absorption correction | Multi-scan (SADABS; Sheldrick, 2003) |
Tmin, Tmax | 0.835, 0.934 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 12759, 4114, 2350 |
Rint | 0.097 |
(sin θ/λ)max (Å−1) | 0.650 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.057, 0.119, 1.02 |
No. of reflections | 4114 |
No. of parameters | 247 |
No. of restraints | 10 |
H-atom treatment | H atoms treated by a mixture of independent and constrained refinement |
Δρmax, Δρmin (e Å−3) | 0.30, −0.37 |
Computer programs: COLLECT (Hooft, 1999), DIRAX/LSQ (Duisenberg et al., 2000), EVALCCD (Duisenberg et al., 2003), SIR2011 (Burla et al., 2012), PLATON (Spek, 2009), SHELXL2014 (Sheldrick, 2008, 2014) and PLATON (Spek, 2009).
N1—C2 | 1.347 (4) | C13—C14 | 1.399 (4) |
C2—N3 | 1.323 (4) | C14—C15 | 1.381 (4) |
C2—S21 | 1.768 (3) | C15—N11 | 1.357 (4) |
N3—C31 | 1.377 (4) | S31—C32 | 1.701 (3) |
C31—O31 | 1.238 (3) | C32—C33 | 1.370 (8) |
N1—C13 | 1.408 (4) | C33—C34 | 1.410 (10) |
N11—N12 | 1.368 (3) | C34—C35 | 1.364 (5) |
N12—C13 | 1.343 (4) | C35—S31 | 1.710 (5) |
N1—C2—N3—C31 | −2.4 (5) | C2—N1—C13—N12 | 61.4 (4) |
C2—N3—C31—O31 | 0.7 (5) | N3—C31—C32—S31 | −9.3 (4) |
C2—N3—C31—C32 | 179.3 (3) | N11—C15—C151—C152 | 18.3 (4) |
N3—C2—N1—C13 | 178.2 (3) | N1—C2—S21—C21 | 172.1 (3) |
C13—N1—C2—S21 | −2.0 (4) | C2—S21—C21—C22 | 85.9 (3) |
D—H···A | D—H | H···A | D···A | D—H···A |
N1—H1···O31 | 0.87 (4) | 1.93 (4) | 2.632 (4) | 137 (3) |
N1—H1···O31i | 0.87 (4) | 2.51 (3) | 3.052 (4) | 121 (3) |
N11—H11···N12ii | 0.91 (4) | 2.07 (3) | 2.857 (4) | 145 (3) |
C21—H21A···Cg1iii | 0.99 | 2.90 | 3.879 (4) | 169 |
C33—H33···Cg1i | 0.95 | 2.80 | 3.481 (14) | 129 |
C44—H44···Cg2iv | 0.95 | 3.00 | 3.82 (3) | 147 |
Symmetry codes: (i) −x+1, −y, −z+1; (ii) −x+1, −y+1, −z+1; (iii) −x, −y+1, −z+1; (iv) x−1, y−1, z+1. |
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