organic compounds
2,8-Dimethyl-5,11-bis[3-(methylsulfanyl)propyl]-1H,7H-diimidazo[c,h][1,6]diazecine
aFacultad de Química, Universidad Nacional Autónoma de México, Ciudad Universitaria, 04510 México D.F., Mexico, and bInstituto de Física, Benemérita Universidad Autónoma de Puebla, Av. San Claudio y 18 Sur, 72570 Puebla, Pue., Mexico
*Correspondence e-mail: sylvain_bernes@hotmail.com
The 20H34N6S2, was challenging, as a consequence of three issues: crystals are twinned, disordered, and include large empty voids corresponding to ca 8% of the unit-cell volume. A satisfactory model was obtained using data collected at 153 K. The diazecine ring is centrosymmetric, and displays the expected boat–chair–boat conformation. The 3-(methylsulfanyl)propyl chain is disordered over two sites with equal occupancies, and different conformations, i.e. trans–gauche–gauche for the first chain [Ndiaz—Cmeth—Cmeth—Cmeth torsion angles: 169.9 (4), 66.8 (5), 62.4 (5)°; diaz = diazecine and meth = methylene] and trans–trans–gauche for the second component [torsion angles: 169.9 (4), −177.6 (4), 64.4 (5)°]. In the crystal, N—H⋯N hydrogen bonds between imidazole rings are evident; weak intermolecular C—H⋯S contacts are also noted. The crystal studied was modelled as a two-component twin.
of the of the title compound, CKeywords: crystal structure; diazecine; twinning; disorder; SQUEEZE algorithm.
CCDC reference: 1907206
Structure description
The chemistry of [1,6]diazecine derivatives bearing imidazole rings started in the 1990′s, through a collaboration between groups from Mexico and The Netherlands (Mendoza-Díaz et al., 1996), when a suitable methodology was established for their preparation, based on the Mannich reaction. Here, the one-pot reaction between propylamine, formaldehyde and 2-methylimidazole resulted in the double addition of formaldehyde on the imidazole, followed by condensation with propylamine, to afford the ten-membered ring characterizing the diazecines. Some other related structures were characterized by X-ray diffraction, upon modification of the group substituting the N sites in positions 1 and 6 in the ring (Mendoza-Díaz et al., 2002, 2010). On the other hand, the coordination chemistry of CuII with these molecules was studied, which has been relevant towards bioinorganic topics, including the modelling of the active site of catecholases (Mendoza-Díaz et al., 2002; Mendoza-Quijano et al., 2012; Zerón et al., 2017).
Although the bioinorganic chemistry has grown steadily for this class of compound, it is clear that the chemical crystallography of the corresponding free ligands is rather poor, with very few structures deposited in the Cambridge Structural Database (Groom et al., 2016). The reason probably stems in part from the fact that the of these crystal structures is not always routine. In the case of the title compound, three issues made the challenging: (i) crystals are systematically twinned, a rather common feature for the tetragonal system. In the present case, a rotation axis about (110) is swapping vectors a and b in the 4/m (class I of twins by merohedry), to form an almost perfect twin; for the studied crystal, fractional contributions for the two-component twin were k1 = 0.486 (2) and k2 = 0.514 (2). (ii) A disorder is observed for the lateral 3-(methylsulfanyl)propyl chain, involving the S atom, which is the main scatterer in the crystal (see Fig. 1, inset). Indeed, this disorder could not be solved using room-temperature diffraction data. (iii) The packing efficiency of the molecules in the crystal is very poor, leaving ca 8% of the cell empty (Fig. 2). Apparently, each individual void of ca 100 Å3 is not filled with disordered solvent (ethanol or water), as evidenced by unsuccessful attempts to include the contribution of disordered solvents to structure factors using the SQUEEZE tool in PLATON (Spek, 2015); a non-significant density of 12 e− per was recovered, corresponding to 1.5 e−/molecule.
Although these issues are decreased dramatically the scattering power of the crystals, data collected on a large sample at 153 K were suitable for refining the structure satisfactorily. The ). Atoms C10/S1/C11 belonging to the lateral chain are disordered over two sites, with occupancies equal to 0.5 for each part (sites A and B, Fig. 1, inset). The conformation of this chain is different for each disordered part: trans–gauche–gauche for part A [torsion angles starting from N7: 169.9 (4), 66.8 (5), 62.4 (5)°] and trans–trans–gauche for part B [torsion angles starting from N7: 169.9 (4), −177.6 (4), 64.4 (5)°]. The diazecine ten-membered ring adopts the skewed boat-chair-boat conformation, invariably found in other related derivatives (idealized symmetry: C2h). In the imidazole ring, π-bonds are localized, with normal bond lengths C2=N3 [1.320 (3) Å] and C3=C4 [1.369 (3) Å]. As a consequence, the imidazolic H atom is localized on N1. This group serves as donor group for the formation of N1—H1⋯N3 hydrogen bonds with a symmetry-related imidazole ring. Other potentially stabilizing hydrogen bonds are weak intermolecular C—H⋯S contacts (Table 1).
contains half the formula, with the molecule lying on an inversion centre (Fig. 1Synthesis and crystallization
2-Methylimidazole (20 mmol, 1.64 g) was dissolved in water (100 ml). To this solution, with vigorous stirring, 3(methylthio)propylamine (20 mmol, 2.1 g) was added dropwise. This mixture formed an emulsion which was broken with the addition of EtOH (ca 20 ml). Without pausing the agitation, formaldehyde (60 mmol, 37% aqueous solution) was added dropwise. This mixture was allowed to react at 333 K for approximately two days when the appearance of a white precipitate indicated the presence of the product. Analysis calculated (%) for C20H34N6S2: C, 56.37; H, 8.11; N, 19.88; S, 15.17. Found: C, 57.15; H, 8.25; N, 19.68, S, 15.30. 1H-NMR (400 MHz, CD3OD, p.p.m.) δ: 2.34 (s, 6H, CH3-Im), 3.36 (s, 8H, Im–CH2–N—R), 1.93 (q, 4H, –CH2-CH2-CH2—S—CH3), 2.12 (s, 6H, CH3-S–), 2.92 (t, 4H, –CH2—CH2–CH2–N–), 2.66 (t, 4H, –S–CH2–CH2—CH2—N–). Crystalline samples were obtained from the slow evaporation of ethanolic solutions of the compound.
Refinement
Crystal data, data collection and structure . The crystal was modelled as a two-component twin, using the twin matrix (0 1 0, 1 0 0, 0 0 ) and one batch scale factor, which converged to 0.486 (2) (Sheldrick, 2015b). Occupancies for disordered sites A and B (atoms C10/S1/C11) were first refined, and since they converged towards a value very close to 1/2, they were fixed to 0.5 in the last cycles of refinement.
details are summarized in Table 2Structural data
CCDC reference: 1907206
https://doi.org/10.1107/S2414314619004413/tk4057sup1.cif
contains datablock I. DOI:Structure factors: contains datablock I. DOI: https://doi.org/10.1107/S2414314619004413/tk4057Isup2.hkl
Supporting information file. DOI: https://doi.org/10.1107/S2414314619004413/tk4057Isup3.cml
Data collection: X-AREA (Stoe & Cie, 2018); cell
X-AREA (Stoe & Cie, 2018; data reduction: X-AREA (Stoe & Cie, 2018; program(s) used to solve structure: SHELXT2018 (Sheldrick, 2015a); program(s) used to refine structure: SHELXL2018 (Sheldrick, 2015b); molecular graphics: XP in SHELXTL-Plus (Sheldrick, 2008) and Mercury (Macrae et al., 2008); software used to prepare material for publication: publCIF (Westrip, 2010).C20H34N6S2 | Dx = 1.114 Mg m−3 |
Mr = 422.65 | Ag Kα radiation, λ = 0.56083 Å |
Tetragonal, I41/a | Cell parameters from 29151 reflections |
a = 16.8114 (6) Å | θ = 2.3–25.6° |
c = 17.8288 (6) Å | µ = 0.12 mm−1 |
V = 5038.8 (4) Å3 | T = 153 K |
Z = 8 | Prism, yellow |
F(000) = 1824 | 0.30 × 0.25 × 0.25 mm |
Stoe Stadivari diffractometer | 2943 independent reflections |
Radiation source: Sealed X-ray tube, Axo Astix-f Microfocus source | 2296 reflections with I > 2σ(I) |
Graded multilayer mirror monochromator | Rint = 0.098 |
Detector resolution: 5.81 pixels mm-1 | θmax = 21.5°, θmin = 2.3° |
ω scans | h = −21→21 |
Absorption correction: multi-scan (X-AREA; Stoe & Cie, 2018) | k = −21→21 |
Tmin = 0.326, Tmax = 1.000 | l = −23→19 |
50278 measured reflections |
Refinement on F2 | Primary atom site location: dual |
Least-squares matrix: full | Secondary atom site location: difference Fourier map |
R[F2 > 2σ(F2)] = 0.048 | Hydrogen site location: mixed |
wR(F2) = 0.138 | H atoms treated by a mixture of independent and constrained refinement |
S = 0.97 | w = 1/[σ2(Fo2) + (0.0946P)2] where P = (Fo2 + 2Fc2)/3 |
2943 reflections | (Δ/σ)max < 0.001 |
159 parameters | Δρmax = 0.39 e Å−3 |
0 restraints | Δρmin = −0.19 e Å−3 |
0 constraints |
Refinement. Refined as a 2-component twin, rotation axis (1 1 0). TWIN 0 1 0 1 0 0 0 0 -1 2 BASF 0.48572 All C-bound H atoms were placed in calculated positions and refined as riding to their carrier C atoms with isotropic displacement parameters. The atomic coordinates for the N-bound H atom were refined; Uiso = 1.2Ueq(N). |
x | y | z | Uiso*/Ueq | Occ. (<1) | |
C10A | 0.5232 (4) | 0.5267 (4) | 0.3420 (3) | 0.0508 (13) | 0.5 |
H10A | 0.559442 | 0.480455 | 0.338174 | 0.061* | 0.5 |
H10B | 0.482368 | 0.515233 | 0.380508 | 0.061* | 0.5 |
S1A | 0.57758 (8) | 0.61513 (10) | 0.36542 (7) | 0.0531 (4) | 0.5 |
C11A | 0.5021 (6) | 0.6863 (5) | 0.3722 (7) | 0.126 (4) | 0.5 |
H11A | 0.525322 | 0.737967 | 0.385065 | 0.189* | 0.5 |
H11B | 0.474258 | 0.690329 | 0.324065 | 0.189* | 0.5 |
H11C | 0.464325 | 0.670403 | 0.411337 | 0.189* | 0.5 |
C10B | 0.5452 (3) | 0.5766 (5) | 0.3314 (3) | 0.0541 (14) | 0.5 |
H10C | 0.557718 | 0.633326 | 0.322144 | 0.065* | 0.5 |
H10D | 0.595553 | 0.546074 | 0.329966 | 0.065* | 0.5 |
S1B | 0.49849 (9) | 0.56555 (13) | 0.42257 (7) | 0.0728 (5) | 0.5 |
C11B | 0.4927 (5) | 0.4626 (7) | 0.4248 (4) | 0.099 (3) | 0.5 |
H11D | 0.467977 | 0.445643 | 0.471933 | 0.149* | 0.5 |
H11E | 0.460470 | 0.443912 | 0.382466 | 0.149* | 0.5 |
H11F | 0.546275 | 0.439992 | 0.421161 | 0.149* | 0.5 |
N1 | 0.33547 (11) | 0.45749 (11) | −0.05949 (9) | 0.0340 (4) | |
H1 | 0.3217 (17) | 0.4482 (17) | −0.0945 (15) | 0.041* | |
C2 | 0.28871 (13) | 0.49400 (12) | −0.00916 (11) | 0.0337 (4) | |
N3 | 0.32672 (11) | 0.50618 (11) | 0.05457 (9) | 0.0342 (4) | |
C3 | 0.40212 (12) | 0.47426 (12) | 0.04372 (11) | 0.0308 (4) | |
C4 | 0.40840 (12) | 0.44355 (12) | −0.02712 (11) | 0.0316 (4) | |
C5 | 0.47564 (13) | 0.40230 (13) | −0.06585 (12) | 0.0369 (5) | |
H5A | 0.516715 | 0.390068 | −0.027772 | 0.044* | |
H5B | 0.455497 | 0.350876 | −0.085133 | 0.044* | |
C6 | 0.46077 (13) | 0.47487 (14) | 0.10598 (10) | 0.0361 (5) | |
H6A | 0.437275 | 0.447824 | 0.150050 | 0.043* | |
H6B | 0.508375 | 0.444327 | 0.090521 | 0.043* | |
N7 | 0.48549 (11) | 0.55613 (12) | 0.12799 (8) | 0.0373 (4) | |
C8 | 0.53467 (15) | 0.5544 (2) | 0.19642 (12) | 0.0559 (8) | |
H8A | 0.564999 | 0.604701 | 0.200290 | 0.067* | |
H8B | 0.573358 | 0.510160 | 0.192816 | 0.067* | |
C9 | 0.48435 (19) | 0.5437 (2) | 0.26668 (12) | 0.0732 (10) | |
H9A | 0.452184 | 0.592605 | 0.272717 | 0.088* | 0.5 |
H9B | 0.446619 | 0.499762 | 0.256607 | 0.088* | 0.5 |
H9C | 0.470416 | 0.487153 | 0.274937 | 0.088* | 0.5 |
H9D | 0.435047 | 0.575808 | 0.264417 | 0.088* | 0.5 |
C12 | 0.20352 (15) | 0.51376 (16) | −0.02429 (14) | 0.0481 (6) | |
H12A | 0.184832 | 0.552542 | 0.012768 | 0.072* | |
H12B | 0.171306 | 0.465312 | −0.020832 | 0.072* | |
H12C | 0.198561 | 0.536381 | −0.074737 | 0.072* |
U11 | U22 | U33 | U12 | U13 | U23 | |
C10A | 0.052 (3) | 0.072 (4) | 0.028 (2) | −0.006 (3) | −0.007 (2) | −0.006 (2) |
S1A | 0.0488 (7) | 0.0725 (9) | 0.0379 (6) | 0.0006 (7) | −0.0083 (5) | −0.0032 (6) |
C11A | 0.088 (6) | 0.083 (6) | 0.206 (10) | 0.033 (5) | −0.044 (7) | −0.028 (7) |
C10B | 0.042 (3) | 0.089 (5) | 0.031 (2) | −0.013 (3) | −0.009 (2) | −0.020 (3) |
S1B | 0.0529 (8) | 0.1376 (17) | 0.0279 (5) | 0.0111 (9) | 0.0017 (5) | −0.0087 (7) |
C11B | 0.060 (4) | 0.187 (10) | 0.051 (3) | 0.018 (5) | 0.011 (3) | 0.024 (4) |
N1 | 0.0360 (9) | 0.0387 (10) | 0.0274 (8) | −0.0039 (8) | −0.0013 (7) | −0.0085 (7) |
C2 | 0.0360 (11) | 0.0316 (10) | 0.0334 (10) | −0.0034 (8) | 0.0016 (8) | −0.0043 (8) |
N3 | 0.0362 (9) | 0.0382 (9) | 0.0282 (8) | −0.0026 (7) | 0.0042 (7) | −0.0056 (7) |
C3 | 0.0361 (11) | 0.0300 (10) | 0.0262 (8) | −0.0025 (8) | 0.0028 (8) | −0.0002 (7) |
C4 | 0.0349 (10) | 0.0305 (10) | 0.0295 (9) | −0.0045 (8) | 0.0016 (7) | −0.0035 (8) |
C5 | 0.0379 (12) | 0.0345 (11) | 0.0384 (10) | −0.0016 (9) | 0.0009 (8) | −0.0108 (9) |
C6 | 0.0398 (12) | 0.0459 (12) | 0.0227 (8) | −0.0001 (9) | 0.0014 (8) | 0.0035 (8) |
N7 | 0.0384 (10) | 0.0520 (12) | 0.0216 (7) | −0.0023 (8) | −0.0016 (7) | −0.0124 (7) |
C8 | 0.0432 (13) | 0.099 (2) | 0.0256 (10) | 0.0152 (13) | −0.0079 (9) | −0.0217 (12) |
C9 | 0.0659 (18) | 0.131 (3) | 0.0225 (10) | 0.0355 (19) | −0.0047 (11) | −0.0117 (13) |
C12 | 0.0383 (13) | 0.0531 (14) | 0.0529 (13) | 0.0028 (11) | −0.0022 (10) | −0.0120 (11) |
C10A—C9 | 1.520 (5) | N3—C3 | 1.390 (3) |
C10A—S1A | 1.795 (7) | C3—C4 | 1.369 (3) |
C10A—H10A | 0.9900 | C3—C6 | 1.485 (3) |
C10A—H10B | 0.9900 | C4—C5 | 1.495 (3) |
S1A—C11A | 1.748 (8) | C5—N7i | 1.464 (3) |
C11A—H11A | 0.9800 | C5—H5A | 0.9900 |
C11A—H11B | 0.9800 | C5—H5B | 0.9900 |
C11A—H11C | 0.9800 | C6—N7 | 1.481 (3) |
C10B—C9 | 1.639 (6) | C6—H6A | 0.9900 |
C10B—S1B | 1.815 (6) | C6—H6B | 0.9900 |
C10B—H10C | 0.9900 | N7—C8 | 1.474 (3) |
C10B—H10D | 0.9900 | C8—C9 | 1.522 (4) |
S1B—C11B | 1.734 (11) | C8—H8A | 0.9900 |
C11B—H11D | 0.9800 | C8—H8B | 0.9900 |
C11B—H11E | 0.9800 | C9—H9A | 0.9900 |
C11B—H11F | 0.9800 | C9—H9B | 0.9900 |
N1—C2 | 1.341 (3) | C9—H9C | 0.9900 |
N1—C4 | 1.375 (3) | C9—H9D | 0.9900 |
N1—H1 | 0.68 (3) | C12—H12A | 0.9800 |
C2—N3 | 1.320 (3) | C12—H12B | 0.9800 |
C2—C12 | 1.495 (3) | C12—H12C | 0.9800 |
C9—C10A—S1A | 105.6 (4) | N7i—C5—C4 | 117.74 (18) |
C9—C10A—H10A | 110.6 | N7i—C5—H5A | 107.9 |
S1A—C10A—H10A | 110.6 | C4—C5—H5A | 107.9 |
C9—C10A—H10B | 110.6 | N7i—C5—H5B | 107.9 |
S1A—C10A—H10B | 110.6 | C4—C5—H5B | 107.9 |
H10A—C10A—H10B | 108.8 | H5A—C5—H5B | 107.2 |
C11A—S1A—C10A | 102.3 (4) | N7—C6—C3 | 113.01 (18) |
S1A—C11A—H11A | 109.5 | N7—C6—H6A | 109.0 |
S1A—C11A—H11B | 109.5 | C3—C6—H6A | 109.0 |
H11A—C11A—H11B | 109.5 | N7—C6—H6B | 109.0 |
S1A—C11A—H11C | 109.5 | C3—C6—H6B | 109.0 |
H11A—C11A—H11C | 109.5 | H6A—C6—H6B | 107.8 |
H11B—C11A—H11C | 109.5 | C5i—N7—C8 | 112.67 (19) |
C9—C10B—S1B | 109.0 (4) | C5i—N7—C6 | 111.42 (14) |
C9—C10B—H10C | 109.9 | C8—N7—C6 | 111.0 (2) |
S1B—C10B—H10C | 109.9 | N7—C8—C9 | 111.8 (2) |
C9—C10B—H10D | 109.9 | N7—C8—H8A | 109.3 |
S1B—C10B—H10D | 109.9 | C9—C8—H8A | 109.3 |
H10C—C10B—H10D | 108.3 | N7—C8—H8B | 109.3 |
C11B—S1B—C10B | 98.5 (3) | C9—C8—H8B | 109.3 |
S1B—C11B—H11D | 109.5 | H8A—C8—H8B | 107.9 |
S1B—C11B—H11E | 109.5 | C10A—C9—C8 | 120.7 (3) |
H11D—C11B—H11E | 109.5 | C8—C9—C10B | 101.1 (3) |
S1B—C11B—H11F | 109.5 | C10A—C9—H9A | 107.2 |
H11D—C11B—H11F | 109.5 | C8—C9—H9A | 107.2 |
H11E—C11B—H11F | 109.5 | C10A—C9—H9B | 107.2 |
C2—N1—C4 | 108.65 (16) | C8—C9—H9B | 107.2 |
C2—N1—H1 | 121 (2) | H9A—C9—H9B | 106.8 |
C4—N1—H1 | 130 (2) | C8—C9—H9C | 111.6 |
N3—C2—N1 | 111.29 (19) | C10B—C9—H9C | 111.6 |
N3—C2—C12 | 125.80 (19) | C8—C9—H9D | 111.6 |
N1—C2—C12 | 122.85 (19) | C10B—C9—H9D | 111.6 |
C2—N3—C3 | 105.19 (17) | H9C—C9—H9D | 109.4 |
C4—C3—N3 | 110.15 (18) | C2—C12—H12A | 109.5 |
C4—C3—C6 | 129.9 (2) | C2—C12—H12B | 109.5 |
N3—C3—C6 | 119.93 (17) | H12A—C12—H12B | 109.5 |
C3—C4—N1 | 104.72 (18) | C2—C12—H12C | 109.5 |
C3—C4—C5 | 131.3 (2) | H12A—C12—H12C | 109.5 |
N1—C4—C5 | 124.00 (17) | H12B—C12—H12C | 109.5 |
C9—C10A—S1A—C11A | 62.4 (5) | C2—N1—C4—C5 | 178.75 (19) |
C9—C10B—S1B—C11B | 64.4 (5) | C3—C4—C5—N7i | −111.7 (3) |
C4—N1—C2—N3 | 0.9 (3) | N1—C4—C5—N7i | 69.1 (3) |
C4—N1—C2—C12 | −176.4 (2) | C4—C3—C6—N7 | 117.0 (2) |
N1—C2—N3—C3 | −0.8 (2) | N3—C3—C6—N7 | −65.4 (2) |
C12—C2—N3—C3 | 176.4 (2) | C3—C6—N7—C5i | −61.5 (2) |
C2—N3—C3—C4 | 0.4 (2) | C3—C6—N7—C8 | 172.04 (17) |
C2—N3—C3—C6 | −177.72 (19) | C5i—N7—C8—C9 | 156.2 (3) |
N3—C3—C4—N1 | 0.2 (2) | C6—N7—C8—C9 | −78.0 (3) |
C6—C3—C4—N1 | 178.0 (2) | S1A—C10A—C9—C8 | 66.8 (5) |
N3—C3—C4—C5 | −179.1 (2) | N7—C8—C9—C10A | 169.9 (4) |
C6—C3—C4—C5 | −1.3 (4) | N7—C8—C9—C10B | −159.8 (3) |
C2—N1—C4—C3 | −0.6 (2) | S1B—C10B—C9—C8 | −177.6 (4) |
Symmetry code: (i) −x+1, −y+1, −z. |
D—H···A | D—H | H···A | D···A | D—H···A |
N1—H1···N3ii | 0.68 (3) | 2.15 (3) | 2.825 (2) | 169 (3) |
C6—H6B···S1Aiii | 0.99 | 2.93 | 3.837 (3) | 153 |
C12—H12A···S1Aiv | 0.98 | 3.01 | 3.926 (3) | 156 |
C11B—H11D···S1Bv | 0.98 | 1.97 | 2.767 (6) | 137 |
Symmetry codes: (ii) y−1/4, −x+3/4, z−1/4; (iii) −y+5/4, x−1/4, z−1/4; (iv) x−1/2, y, −z+1/2; (v) −x+1, −y+1, −z+1. |
Funding information
Funding for this research was provided by: Consejo Nacional de Ciencia y Tecnología (grant No. 268178).
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