| Literature DB >> 29850066 |
Lee Chin Lai1, Che Nursarah Binti Che Abdul Rahman1, M Ibrahim M Tahir1, Thahira B S A Ravoof1, Mukesh M Jotani2, Edward R T Tiekink3.
Abstract
The title disubstituted thio-urea derivative, C10H14N4S, features an almost planar imine (E configuration, C3N) core flanked by thio-urea (CN2S) and methyl-pyridyl (C5N) residues (each plane has a r.m.s. deviation of the respective fitted atoms of 0.0066 Å). The dihedral angles between the core and the thio-urea and pyridyl residues are 20.25 (8) and 7.60 (9)°, respectively, indicating twists in the mol-ecule; the dihedral angle between the outer planes is 13.62 (7)°. There is an anti-disposition of the amine-N-H atoms which allows for the formation of an intra-molecular amine-N-H⋯N(imine) hydrogen bond that closes an S(5) loop. In the crystal, amine-N-H⋯N(pyrid-yl) hydrogen bonds lead to zigzag (glide symmetry) supra-molecular chains along the c-axis direction. These are connected into a supra-molecular layer propagating in the bc plane by thio-amide-N-H⋯S(thione) hydrogen bonds via eight-membered thio-amide {⋯HNCS}2 synthons.Entities:
Keywords: Hirshfeld surface analysis; crystal structure; hydrogen bonding; thiourea derivative
Year: 2018 PMID: 29850066 PMCID: PMC5956349 DOI: 10.1107/S2056989018001305
Source DB: PubMed Journal: Acta Crystallogr E Crystallogr Commun
Figure 1The molecular structure of (I) showing the atom-labelling scheme and displacement ellipsoids at the 70% probability level.
Hydrogen-bond geometry (Å, °)
Cg1 is the centroid of the (N4,C5–C9) ring.
|
|
| H⋯ |
|
|
|---|---|---|---|---|
| N1—H1 | 0.88 (2) | 2.23 (2) | 2.6148 (18) | 106 (1) |
| N1—H1 | 0.88 (2) | 2.33 (2) | 3.0714 (18) | 142 (1) |
| N2—H2 | 0.87 (1) | 2.55 (1) | 3.3955 (13) | 168 (2) |
| C10—H10 | 0.98 | 2.89 | 3.7546 (18) | 147 |
Symmetry codes: (i) ; (ii) .
Figure 2Molecular packing in (I): (a) a view of the supramolecular layer propagating normal to the a-axis direction sustained by thioamide-N—H⋯S(thione) and amine-N—H⋯N(pyridyl) hydrogen bonds shown as orange and blue dashed lines, respectively. Non-participating hydrogen atoms have been omitted for reasons of clarity, and (b) a view of the unit-cell contents shown in projection down the c axis. One layer is highlighted in space-filling mode to emphasize the jagged topology.
Figure 3Two views of the Hirshfeld surface mapped over d norm for (I) in the range −0.110 to +1.348 au, highlighting N—H⋯N and N—H⋯S hydrogen bonds through yellow dashed lines and short interatomic C⋯S/S⋯C contacts through black dashed lines.
Summary of short interatomic contacts (Å) in (I)
| Contact | Distance | Symmetry operation |
|---|---|---|
| H2 | 2.23 | 2 − |
| H9⋯N4 | 2.54 |
|
| H7⋯S1 | 2.83 | −1 + |
| C3⋯H4 | 2.84 |
|
| C4⋯S1 | 3.4545 (15) | 2 − |
Figure 4Two views of the Hirshfeld surface mapped over the electrostatic potential for (I) in the range −0.103 to +0.104 au. The red and blue regions represent negative and positive electrostatic potentials, respectively.
Figure 5(a) The full two-dimensional fingerprint plot for (I) and fingerprint plots delineated into (b) H⋯H, (c) C⋯H/H⋯C, (d) S⋯H/H⋯S and (e) N⋯H/H⋯N contacts.
Relative percentage contributions of close contacts to the Hirshfeld surface of (I)
| H⋯H | 50.4 |
| C⋯H/H⋯C | 16.7 |
| S⋯H/H⋯S | 16.5 |
| N⋯H/H⋯N | 14.9 |
| C⋯C | 0.7 |
| C⋯S/S⋯C | 0.6 |
| S⋯N/N⋯S | 0.2 |
Experimental details
| Crystal data | |
| Chemical formula | C10H14N4S |
|
| 222.31 |
| Crystal system, space group | Monoclinic, |
| Temperature (K) | 100 |
|
| 8.8108 (3), 14.9044 (4), 9.3583 (3) |
| β (°) | 113.391 (4) |
|
| 1127.93 (7) |
|
| 4 |
| Radiation type | Cu |
| μ (mm−1) | 2.33 |
| Crystal size (mm) | 0.15 × 0.13 × 0.03 |
| Data collection | |
| Diffractometer | Rigaku Oxford Diffraction Gemini E |
| Absorption correction | Multi-scan ( |
|
| 0.852, 1.000 |
| No. of measured, independent and observed [ | 21767, 2184, 1995 |
|
| 0.034 |
| (sin θ/λ)max (Å−1) | 0.614 |
| Refinement | |
|
| 0.035, 0.097, 1.02 |
| No. of reflections | 2184 |
| No. of parameters | 145 |
| No. of restraints | 2 |
| H-atom treatment | H atoms treated by a mixture of independent and constrained refinement |
| Δρmax, Δρmin (e Å−3) | 0.41, −0.23 |
Computer programs: CrysAlis PRO (Agilent, 2011 ▸), SHELXS97 (Sheldrick, 2008 ▸), SHELXL2014 (Sheldrick, 2015 ▸), ORTEP-3 for Windows (Farrugia, 2012 ▸), DIAMOND (Brandenburg, 2006 ▸) and publCIF (Westrip, 2010 ▸).
| C10H14N4S | |
| Monoclinic, | Cu |
| Cell parameters from 9894 reflections | |
| θ = 3.0–71.2° | |
| µ = 2.33 mm−1 | |
| β = 113.391 (4)° | |
| Plate, brown | |
| 0.15 × 0.13 × 0.03 mm |
| Rigaku Oxford Diffraction Gemini E diffractometer | 2184 independent reflections |
| Radiation source: Enhance X-ray source | 1995 reflections with |
| Mirror monochromator | |
| Detector resolution: 16.1952 pixels mm-1 | θmax = 71.3°, θmin = 5.5° |
| ω scan | |
| Absorption correction: multi-scan (CrysAlis PRO; Agilent, 2011) | |
| 21767 measured reflections |
| Refinement on | Primary atom site location: structure-invariant direct methods |
| Least-squares matrix: full | Hydrogen site location: mixed |
| H atoms treated by a mixture of independent and constrained refinement | |
| (Δ/σ)max = 0.001 | |
| 2184 reflections | Δρmax = 0.41 e Å−3 |
| 145 parameters | Δρmin = −0.23 e Å−3 |
| 2 restraints |
| 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. |
| S1 | 1.01197 (4) | 0.43326 (2) | 0.80392 (4) | 0.01660 (14) | |
| N1 | 0.78625 (16) | 0.52040 (9) | 0.56429 (14) | 0.0167 (3) | |
| H1N | 0.728 (2) | 0.5689 (9) | 0.527 (2) | 0.020* | |
| N2 | 0.85960 (15) | 0.58621 (8) | 0.80403 (14) | 0.0151 (3) | |
| H2N | 0.908 (2) | 0.5811 (12) | 0.9041 (11) | 0.018* | |
| N3 | 0.73527 (15) | 0.64746 (8) | 0.73280 (14) | 0.0151 (3) | |
| N4 | 0.57917 (15) | 0.85680 (9) | 0.79338 (14) | 0.0169 (3) | |
| C1 | 0.87633 (17) | 0.51659 (10) | 0.71665 (16) | 0.0142 (3) | |
| C2 | 0.7888 (2) | 0.45156 (11) | 0.45507 (18) | 0.0206 (3) | |
| H2A | 0.9018 | 0.4289 | 0.4860 | 0.031* | |
| H2B | 0.7508 | 0.4772 | 0.3502 | 0.031* | |
| H2C | 0.7155 | 0.4022 | 0.4554 | 0.031* | |
| C3 | 0.73564 (17) | 0.72169 (10) | 0.80323 (16) | 0.0137 (3) | |
| C4 | 0.86453 (18) | 0.75205 (10) | 0.95558 (17) | 0.0176 (3) | |
| H4A | 0.8263 | 0.7403 | 1.0389 | 0.026* | |
| H4B | 0.8841 | 0.8165 | 0.9508 | 0.026* | |
| H4C | 0.9676 | 0.7192 | 0.9768 | 0.026* | |
| C5 | 0.59425 (17) | 0.78267 (10) | 0.71764 (16) | 0.0144 (3) | |
| C6 | 0.45183 (19) | 0.91141 (11) | 0.71570 (19) | 0.0201 (3) | |
| H6 | 0.4387 | 0.9638 | 0.7675 | 0.024* | |
| C7 | 0.33818 (18) | 0.89648 (11) | 0.56488 (18) | 0.0198 (3) | |
| H7 | 0.2515 | 0.9381 | 0.5154 | 0.024* | |
| C8 | 0.35303 (17) | 0.81950 (10) | 0.48712 (16) | 0.0168 (3) | |
| C9 | 0.48424 (17) | 0.76211 (10) | 0.56638 (16) | 0.0153 (3) | |
| H9 | 0.4989 | 0.7089 | 0.5175 | 0.018* | |
| C10 | 0.23240 (19) | 0.79716 (11) | 0.32435 (18) | 0.0205 (3) | |
| H10A | 0.2929 | 0.7874 | 0.2576 | 0.031* | |
| H10B | 0.1546 | 0.8470 | 0.2830 | 0.031* | |
| H10C | 0.1714 | 0.7426 | 0.3267 | 0.031* |
| S1 | 0.0203 (2) | 0.0138 (2) | 0.0143 (2) | 0.00414 (13) | 0.00545 (15) | 0.00082 (13) |
| N1 | 0.0217 (6) | 0.0131 (6) | 0.0134 (6) | 0.0032 (5) | 0.0050 (5) | 0.0000 (5) |
| N2 | 0.0174 (6) | 0.0140 (6) | 0.0111 (6) | 0.0029 (5) | 0.0028 (5) | 0.0006 (5) |
| N3 | 0.0158 (6) | 0.0148 (6) | 0.0144 (6) | 0.0029 (5) | 0.0057 (5) | 0.0017 (5) |
| N4 | 0.0178 (6) | 0.0160 (7) | 0.0171 (6) | 0.0018 (5) | 0.0072 (5) | −0.0005 (5) |
| C1 | 0.0152 (7) | 0.0125 (7) | 0.0161 (7) | −0.0017 (5) | 0.0073 (5) | 0.0008 (5) |
| C2 | 0.0278 (8) | 0.0167 (8) | 0.0158 (7) | 0.0015 (6) | 0.0072 (6) | −0.0027 (6) |
| C3 | 0.0158 (7) | 0.0143 (7) | 0.0126 (7) | 0.0000 (5) | 0.0073 (5) | 0.0008 (5) |
| C4 | 0.0193 (7) | 0.0141 (7) | 0.0166 (7) | 0.0020 (6) | 0.0042 (6) | −0.0023 (6) |
| C5 | 0.0161 (7) | 0.0134 (7) | 0.0156 (7) | −0.0002 (5) | 0.0082 (6) | 0.0013 (5) |
| C6 | 0.0216 (7) | 0.0157 (8) | 0.0228 (8) | 0.0035 (6) | 0.0086 (6) | −0.0022 (6) |
| C7 | 0.0174 (7) | 0.0185 (8) | 0.0223 (8) | 0.0043 (6) | 0.0067 (6) | 0.0022 (6) |
| C8 | 0.0162 (7) | 0.0189 (8) | 0.0158 (7) | 0.0000 (6) | 0.0069 (6) | 0.0033 (6) |
| C9 | 0.0182 (7) | 0.0143 (7) | 0.0149 (7) | 0.0005 (6) | 0.0081 (6) | 0.0000 (5) |
| C10 | 0.0204 (7) | 0.0221 (8) | 0.0166 (7) | 0.0028 (6) | 0.0050 (6) | 0.0028 (6) |
| S1—C1 | 1.6920 (15) | C4—H4A | 0.9800 |
| N1—C1 | 1.3295 (18) | C4—H4B | 0.9800 |
| N1—C2 | 1.4547 (19) | C4—H4C | 0.9800 |
| N1—H1N | 0.873 (9) | C5—C9 | 1.396 (2) |
| N2—C1 | 1.3649 (19) | C6—C7 | 1.386 (2) |
| N2—N3 | 1.3776 (17) | C6—H6 | 0.9500 |
| N2—H2N | 0.864 (9) | C7—C8 | 1.392 (2) |
| N3—C3 | 1.2872 (19) | C7—H7 | 0.9500 |
| N4—C5 | 1.3474 (19) | C8—C9 | 1.392 (2) |
| N4—C6 | 1.342 (2) | C8—C10 | 1.508 (2) |
| C2—H2A | 0.9800 | C9—H9 | 0.9500 |
| C2—H2B | 0.9800 | C10—H10A | 0.9800 |
| C2—H2C | 0.9800 | C10—H10B | 0.9800 |
| C3—C5 | 1.4923 (19) | C10—H10C | 0.9800 |
| C3—C4 | 1.4971 (19) | ||
| C1—N1—C2 | 123.66 (13) | H4A—C4—H4C | 109.5 |
| C1—N1—H1N | 117.9 (13) | H4B—C4—H4C | 109.5 |
| C2—N1—H1N | 118.3 (13) | N4—C5—C9 | 122.66 (13) |
| C1—N2—N3 | 117.92 (12) | N4—C5—C3 | 116.91 (12) |
| C1—N2—H2N | 117.3 (12) | C9—C5—C3 | 120.42 (13) |
| N3—N2—H2N | 122.4 (12) | N4—C6—C7 | 124.37 (14) |
| C3—N3—N2 | 118.81 (12) | N4—C6—H6 | 117.8 |
| C5—N4—C6 | 116.62 (12) | C7—C6—H6 | 117.8 |
| N1—C1—N2 | 116.71 (13) | C6—C7—C8 | 118.98 (14) |
| N1—C1—S1 | 123.75 (11) | C6—C7—H7 | 120.5 |
| N2—C1—S1 | 119.50 (11) | C8—C7—H7 | 120.5 |
| N1—C2—H2A | 109.5 | C7—C8—C9 | 117.28 (13) |
| N1—C2—H2B | 109.5 | C7—C8—C10 | 122.34 (14) |
| H2A—C2—H2B | 109.5 | C9—C8—C10 | 120.38 (14) |
| N1—C2—H2C | 109.5 | C8—C9—C5 | 120.08 (14) |
| H2A—C2—H2C | 109.5 | C8—C9—H9 | 120.0 |
| H2B—C2—H2C | 109.5 | C5—C9—H9 | 120.0 |
| N3—C3—C5 | 114.63 (12) | C8—C10—H10A | 109.5 |
| N3—C3—C4 | 126.45 (13) | C8—C10—H10B | 109.5 |
| C5—C3—C4 | 118.89 (12) | H10A—C10—H10B | 109.5 |
| C3—C4—H4A | 109.5 | C8—C10—H10C | 109.5 |
| C3—C4—H4B | 109.5 | H10A—C10—H10C | 109.5 |
| H4A—C4—H4B | 109.5 | H10B—C10—H10C | 109.5 |
| C3—C4—H4C | 109.5 | ||
| C1—N2—N3—C3 | −167.44 (13) | N3—C3—C5—C9 | −6.6 (2) |
| C2—N1—C1—N2 | −179.61 (13) | C4—C3—C5—C9 | 171.34 (13) |
| C2—N1—C1—S1 | 2.5 (2) | C5—N4—C6—C7 | −0.5 (2) |
| N3—N2—C1—N1 | 9.20 (19) | N4—C6—C7—C8 | 1.0 (2) |
| N3—N2—C1—S1 | −172.80 (10) | C6—C7—C8—C9 | −0.8 (2) |
| N2—N3—C3—C5 | −178.98 (11) | C6—C7—C8—C10 | 178.57 (15) |
| N2—N3—C3—C4 | 3.2 (2) | C7—C8—C9—C5 | 0.1 (2) |
| C6—N4—C5—C9 | −0.3 (2) | C10—C8—C9—C5 | −179.24 (13) |
| C6—N4—C5—C3 | 179.94 (13) | N4—C5—C9—C8 | 0.4 (2) |
| N3—C3—C5—N4 | 173.16 (12) | C3—C5—C9—C8 | −179.77 (13) |
| C4—C3—C5—N4 | −8.85 (19) |
| H··· | ||||
| N1—H1 | 0.88 (2) | 2.23 (2) | 2.6148 (18) | 106 (1) |
| N1—H1 | 0.88 (2) | 2.33 (2) | 3.0714 (18) | 142 (1) |
| N2—H2 | 0.87 (1) | 2.55 (1) | 3.3955 (13) | 168 (2) |
| C10—H10 | 0.98 | 2.89 | 3.7546 (18) | 147 |