Literature DB >> 23476605

2-Methyl-sulfanyl-1,2,4-triazolo[1,5-a]quinazoline-5(4H)-thione.

Rashad Al-Salahi1, Mohamed Marzouk, Mohamed A Al-Omar, Abd El-Galil E Amr, Seik Weng Ng, Edward R T Tiekink.   

Abstract

In the title compound, C10H8N4S2, comprising fused six-, six- and five-membered rings, the mol-ecule is close to being planar (r.m.s. deviation of the non-H atoms = 0.041 Å). The S-bound methyl group is folded away from the single N atom of the triazole ring and the NH group of the six-membered ring, allowing for the formation of centrosymmetric eight-membered {⋯HNCN}2 synthons in the crystal. The resulting inversion dimers are connected into supra-molecular stacks aligned along the b-axis direction by π-π inter-actions [centroid-centroid distances = 3.6531 (12) and 3.7182 (12) Å].

Entities:  

Year:  2013        PMID: 23476605      PMCID: PMC3588520          DOI: 10.1107/S1600536813004881

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


Related literature

For background to the biological activity of triazoloquinazolines, see: Pierce et al. (2004 ▶); Al-Salahi & Geffken (2010 ▶, 2011 ▶); Al-Salahi et al. (2011 ▶, 2013 ▶).

Experimental

Crystal data

C10H8N4S2 M = 248.32 Monoclinic, a = 10.5414 (11) Å b = 4.9335 (6) Å c = 20.0943 (19) Å β = 99.127 (10)° V = 1031.79 (19) Å3 Z = 4 Mo Kα radiation μ = 0.49 mm−1 T = 295 K 0.30 × 0.15 × 0.05 mm

Data collection

Agilent SuperNova Dual diffractometer with an Atlas detector Absorption correction: multi-scan (CrysAlis PRO; Agilent, 2011 ▶) T min = 0.864, T max = 1.000 5096 measured reflections 2389 independent reflections 1667 reflections with I > 2σ(I) R int = 0.035

Refinement

R[F 2 > 2σ(F 2)] = 0.040 wR(F 2) = 0.098 S = 0.93 2389 reflections 149 parameters 1 restraint H atoms treated by a mixture of independent and constrained refinement Δρmax = 0.28 e Å−3 Δρmin = −0.29 e Å−3 Data collection: CrysAlis PRO (Agilent, 2011 ▶); cell refinement: CrysAlis PRO; data reduction: CrysAlis PRO; 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, 2012 ▶) and DIAMOND (Brandenburg, 2006 ▶); software used to prepare material for publication: publCIF (Westrip, 2010 ▶). Click here for additional data file. Crystal structure: contains datablock(s) global, I. DOI: 10.1107/S1600536813004881/hb7045sup1.cif Click here for additional data file. Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536813004881/hb7045Isup2.hkl Click here for additional data file. Supplementary material file. DOI: 10.1107/S1600536813004881/hb7045Isup3.cml Additional supplementary materials: crystallographic information; 3D view; checkCIF report
C10H8N4S2F(000) = 512
Mr = 248.32Dx = 1.599 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ybcCell parameters from 1314 reflections
a = 10.5414 (11) Åθ = 3.1–27.5°
b = 4.9335 (6) ŵ = 0.49 mm1
c = 20.0943 (19) ÅT = 295 K
β = 99.127 (10)°Prism, yellow
V = 1031.79 (19) Å30.30 × 0.15 × 0.05 mm
Z = 4
Agilent SuperNova Dual diffractometer with an Atlas detector2389 independent reflections
Radiation source: SuperNova (Mo) X-ray Source1667 reflections with I > 2σ(I)
Mirror monochromatorRint = 0.035
Detector resolution: 10.4041 pixels mm-1θmax = 27.6°, θmin = 3.1°
ω scanh = −13→12
Absorption correction: multi-scan (CrysAlis PRO; Agilent, 2011)k = −5→6
Tmin = 0.864, Tmax = 1.000l = −22→26
5096 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)] = 0.040Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.098H atoms treated by a mixture of independent and constrained refinement
S = 0.93w = 1/[σ2(Fo2) + (0.0452P)2] where P = (Fo2 + 2Fc2)/3
2389 reflections(Δ/σ)max = 0.001
149 parametersΔρmax = 0.28 e Å3
1 restraintΔρmin = −0.29 e Å3
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.
xyzUiso*/Ueq
S10.57415 (5)0.09061 (12)0.69579 (3)0.03633 (18)
S20.69330 (6)1.14441 (14)0.43364 (3)0.0455 (2)
N10.63890 (16)0.7597 (4)0.51388 (8)0.0334 (4)
H10.5735 (15)0.728 (5)0.4828 (9)0.052 (7)*
N20.75333 (14)0.6491 (3)0.61961 (8)0.0288 (4)
N30.74549 (16)0.4772 (3)0.67308 (8)0.0309 (4)
N40.57690 (15)0.4139 (4)0.58757 (8)0.0325 (4)
C10.72154 (19)0.9632 (4)0.50311 (10)0.0316 (5)
C20.83231 (19)1.0021 (4)0.55680 (10)0.0306 (5)
C30.92564 (19)1.1992 (5)0.55164 (11)0.0363 (5)
H30.91691.31020.51380.044*
C41.0296 (2)1.2317 (5)0.60125 (11)0.0403 (6)
H41.09061.36400.59700.048*
C51.04387 (19)1.0665 (5)0.65804 (11)0.0385 (5)
H51.11511.08830.69140.046*
C60.95443 (19)0.8723 (4)0.66552 (10)0.0358 (5)
H60.96440.76260.70360.043*
C70.84829 (18)0.8415 (4)0.61517 (10)0.0292 (5)
C80.65228 (18)0.6076 (4)0.57102 (9)0.0294 (5)
C90.63785 (18)0.3432 (4)0.65066 (10)0.0296 (5)
C100.6908 (2)0.0885 (5)0.77103 (11)0.0474 (6)
H10A0.6676−0.04560.80160.071*
H10B0.69350.26370.79200.071*
H10C0.77380.04610.75990.071*
U11U22U33U12U13U23
S10.0370 (3)0.0390 (4)0.0320 (3)−0.0018 (3)0.0023 (2)0.0034 (3)
S20.0496 (4)0.0525 (4)0.0330 (3)−0.0007 (3)0.0019 (3)0.0110 (3)
N10.0337 (9)0.0388 (11)0.0247 (9)−0.0014 (9)−0.0046 (8)0.0023 (8)
N20.0291 (8)0.0321 (10)0.0237 (8)0.0019 (8)−0.0006 (7)0.0006 (8)
N30.0339 (9)0.0321 (10)0.0256 (9)0.0011 (8)0.0015 (7)0.0028 (8)
N40.0328 (9)0.0369 (11)0.0266 (9)0.0011 (9)0.0007 (7)0.0016 (8)
C10.0351 (11)0.0320 (12)0.0285 (11)0.0054 (10)0.0070 (9)−0.0012 (9)
C20.0329 (10)0.0314 (12)0.0282 (11)0.0062 (10)0.0069 (9)−0.0035 (9)
C30.0380 (11)0.0367 (13)0.0354 (12)−0.0001 (11)0.0091 (10)−0.0006 (10)
C40.0366 (12)0.0394 (14)0.0457 (13)−0.0061 (11)0.0090 (10)−0.0064 (12)
C50.0306 (11)0.0436 (14)0.0387 (12)0.0001 (11)−0.0024 (10)−0.0089 (11)
C60.0363 (11)0.0380 (13)0.0313 (11)0.0050 (10)−0.0007 (9)−0.0009 (10)
C70.0287 (10)0.0304 (11)0.0283 (11)0.0020 (9)0.0044 (8)−0.0040 (9)
C80.0316 (10)0.0316 (12)0.0234 (10)0.0038 (10)−0.0007 (8)−0.0027 (9)
C90.0310 (10)0.0302 (12)0.0270 (10)0.0044 (10)0.0029 (9)−0.0020 (9)
C100.0511 (14)0.0587 (17)0.0299 (12)−0.0044 (13)−0.0007 (10)0.0097 (12)
S1—C91.738 (2)C2—C31.399 (3)
S1—C101.791 (2)C2—C71.403 (3)
S2—C11.645 (2)C3—C41.369 (3)
N1—C81.360 (2)C3—H30.9300
N1—C11.369 (3)C4—C51.391 (3)
N1—H10.868 (10)C4—H40.9300
N2—C81.342 (2)C5—C61.369 (3)
N2—N31.381 (2)C5—H50.9300
N2—C71.392 (2)C6—C71.393 (3)
N3—C91.329 (2)C6—H60.9300
N4—C81.319 (3)C10—H10A0.9600
N4—C91.372 (2)C10—H10B0.9600
C1—C21.471 (3)C10—H10C0.9600
C9—S1—C10100.05 (10)C6—C5—C4120.89 (19)
C8—N1—C1123.68 (17)C6—C5—H5119.6
C8—N1—H1118.3 (16)C4—C5—H5119.6
C1—N1—H1118.0 (16)C5—C6—C7119.0 (2)
C8—N2—N3109.51 (16)C5—C6—H6120.5
C8—N2—C7123.58 (17)C7—C6—H6120.5
N3—N2—C7126.91 (15)C6—C7—N2122.05 (19)
C9—N3—N2101.24 (15)C6—C7—C2121.4 (2)
C8—N4—C9101.80 (16)N2—C7—C2116.50 (17)
N1—C1—C2115.51 (18)N4—C8—N2111.57 (18)
N1—C1—S2119.93 (15)N4—C8—N1128.80 (17)
C2—C1—S2124.56 (17)N2—C8—N1119.63 (19)
C3—C2—C7117.51 (18)N3—C9—N4115.88 (18)
C3—C2—C1121.46 (19)N3—C9—S1124.04 (15)
C7—C2—C1121.0 (2)N4—C9—S1120.09 (15)
C4—C3—C2121.2 (2)S1—C10—H10A109.5
C4—C3—H3119.4S1—C10—H10B109.5
C2—C3—H3119.4H10A—C10—H10B109.5
C3—C4—C5119.9 (2)S1—C10—H10C109.5
C3—C4—H4120.0H10A—C10—H10C109.5
C5—C4—H4120.0H10B—C10—H10C109.5
C8—N2—N3—C90.5 (2)C3—C2—C7—C6−1.4 (3)
C7—N2—N3—C9179.49 (18)C1—C2—C7—C6178.41 (19)
C8—N1—C1—C22.8 (3)C3—C2—C7—N2179.17 (17)
C8—N1—C1—S2−177.27 (16)C1—C2—C7—N2−1.0 (3)
N1—C1—C2—C3178.67 (19)C9—N4—C8—N21.2 (2)
S2—C1—C2—C3−1.3 (3)C9—N4—C8—N1−178.6 (2)
N1—C1—C2—C7−1.2 (3)N3—N2—C8—N4−1.2 (2)
S2—C1—C2—C7178.89 (16)C7—N2—C8—N4179.82 (17)
C7—C2—C3—C40.9 (3)N3—N2—C8—N1178.65 (17)
C1—C2—C3—C4−178.9 (2)C7—N2—C8—N1−0.4 (3)
C2—C3—C4—C50.1 (3)C1—N1—C8—N4177.7 (2)
C3—C4—C5—C6−0.6 (3)C1—N1—C8—N2−2.1 (3)
C4—C5—C6—C70.1 (3)N2—N3—C9—N40.3 (2)
C5—C6—C7—N2−179.68 (19)N2—N3—C9—S1179.79 (14)
C5—C6—C7—C21.0 (3)C8—N4—C9—N3−0.9 (2)
C8—N2—C7—C6−177.57 (19)C8—N4—C9—S1179.53 (15)
N3—N2—C7—C63.6 (3)C10—S1—C9—N30.4 (2)
C8—N2—C7—C21.8 (3)C10—S1—C9—N4179.93 (17)
N3—N2—C7—C2−177.02 (18)
D—H···AD—HH···AD···AD—H···A
N1—H1···N4i0.87 (1)2.07 (1)2.931 (2)171 (2)
Table 1

Hydrogen-bond geometry (Å, °)

D—H⋯A D—HH⋯A DA D—H⋯A
N1—H1⋯N4i 0.87 (1)2.07 (1)2.931 (2)171 (2)

Symmetry code: (i) .

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