Literature DB >> 21203120

3-Ethyl-4-[(E)-2-methyl-benzyl-idene-amino]-1H-1,2,4-triazole-5(4H)-thione.

Shan-Heng Wang1, Ying-Li Xu, Pei-Jin Xie, Wen-Long Wang, Shang Shan.   

Abstract

Crystals of the title compound, C(12)H(14)N(4)S, were obtained from a condensation reaction of 4-amino-3-ethyl-1H-1,2,4-triazole-5(4H)-thione and 2-methyl-benzaldehyde. In the mol-ecular structure, there is a short N=C double bond [1.255 (2) Å], and the benzene and triazole rings are located on opposite sites of this double bond. The two rings are approximately parallel to each other, the dihedral angle being 1.75 (11)°. A partially overlapped arrangement is observed between the nearly parallel triazole and benzene rings of adjacent mol-ecules; the perpendicular distance of the centroid of the triazole ring from the benzene ring is 3.482 Å, indicating the existence of π-π stacking in the crystal structure.

Entities:  

Year:  2008        PMID: 21203120      PMCID: PMC2962033          DOI: 10.1107/S1600536808019867

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


Related literature

For general background, see: Okabe et al. (1993 ▶); Shan et al. (2003 ▶). For related structures, see: Fan et al. (2008 ▶); Shan et al. (2004 ▶, 2008 ▶). For the thickness of the aromatic ring, see: Cotton & Wilkinson (1972 ▶).

Experimental

Crystal data

C12H14N4S M = 246.33 Monoclinic, a = 7.7255 (15) Å b = 15.411 (3) Å c = 10.685 (2) Å β = 101.032 (12)° V = 1248.7 (4) Å3 Z = 4 Mo Kα radiation μ = 0.24 mm−1 T = 295 (2) K 0.32 × 0.28 × 0.24 mm

Data collection

Rigaku R-AXIS RAPID IP diffractometer Absorption correction: none 12354 measured reflections 2860 independent reflections 1777 reflections with I > 2σ(I) R int = 0.061

Refinement

R[F 2 > 2σ(F 2)] = 0.047 wR(F 2) = 0.120 S = 1.03 2860 reflections 156 parameters H-atom parameters constrained Δρmax = 0.18 e Å−3 Δρmin = −0.21 e Å−3 Data collection: PROCESS-AUTO (Rigaku, 1998 ▶); cell refinement: PROCESS-AUTO; data reduction: CrystalStructure (Rigaku/MSC, 2002 ▶); program(s) used to solve structure: SIR92 (Altomare et al., 1993 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: ORTEP-3 for Windows (Farrugia, 1997 ▶); software used to prepare material for publication: WinGX (Farrugia, 1999 ▶). Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536808019867/xu2434sup1.cif Structure factors: contains datablocks I. DOI: 10.1107/S1600536808019867/xu2434Isup2.hkl Additional supplementary materials: crystallographic information; 3D view; checkCIF report
C12H14N4SF000 = 520
Mr = 246.33Dx = 1.310 Mg m3
Monoclinic, P21/nMo Kα radiation λ = 0.71073 Å
Hall symbol: -P 2ynCell parameters from 4278 reflections
a = 7.7255 (15) Åθ = 2.8–24.5º
b = 15.411 (3) ŵ = 0.24 mm1
c = 10.685 (2) ÅT = 295 (2) K
β = 101.032 (12)ºPrism, yellow
V = 1248.7 (4) Å30.32 × 0.28 × 0.24 mm
Z = 4
Rigaku R-AXIS RAPID IP diffractometer2860 independent reflections
Radiation source: fine-focus sealed tube1777 reflections with I > 2σ(I)
Monochromator: graphiteRint = 0.061
Detector resolution: 10.00 pixels mm-1θmax = 27.6º
T = 295(2) Kθmin = 2.6º
ω scansh = −9→10
Absorption correction: nonek = −20→16
12354 measured reflectionsl = −13→13
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.047H-atom parameters constrained
wR(F2) = 0.121  w = 1/[σ2(Fo2) + (0.0463P)2 + 0.2633P] where P = (Fo2 + 2Fc2)/3
S = 1.03(Δ/σ)max < 0.001
2860 reflectionsΔρmax = 0.18 e Å3
156 parametersΔρmin = −0.21 e Å3
Primary atom site location: structure-invariant direct methodsExtinction correction: none
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
S0.70986 (7)−0.00644 (3)0.39484 (6)0.0542 (2)
N10.9437 (2)0.12184 (11)0.47565 (18)0.0453 (5)
H1N1.03200.08260.50950.068*
N20.9697 (2)0.20996 (11)0.47450 (18)0.0449 (5)
N30.70093 (19)0.17368 (10)0.37970 (15)0.0356 (4)
N40.5343 (2)0.19429 (11)0.31007 (17)0.0424 (5)
C10.7829 (3)0.09601 (13)0.4175 (2)0.0388 (5)
C20.8200 (3)0.24045 (13)0.4152 (2)0.0387 (5)
C30.7750 (3)0.33278 (13)0.3886 (2)0.0486 (6)
H3A0.67600.34820.42790.058*
H3B0.73910.34080.29730.058*
C40.9288 (3)0.39305 (14)0.4383 (3)0.0627 (7)
H4A0.96240.38680.52910.094*
H4B0.89420.45200.41800.094*
H4C1.02700.37840.39910.094*
C50.4118 (3)0.13985 (14)0.3022 (2)0.0443 (6)
H50.43300.08560.34020.053*
C60.2346 (3)0.16241 (14)0.2325 (2)0.0412 (5)
C70.1079 (3)0.09783 (15)0.1958 (2)0.0484 (6)
C8−0.0589 (3)0.1238 (2)0.1313 (2)0.0631 (7)
H8−0.14540.08200.10640.076*
C9−0.0980 (3)0.2091 (2)0.1040 (3)0.0688 (8)
H9−0.21050.22450.06180.083*
C100.0279 (3)0.27235 (18)0.1386 (2)0.0621 (7)
H100.00190.33020.11820.074*
C110.1935 (3)0.24901 (15)0.2038 (2)0.0502 (6)
H110.27830.29160.22880.060*
C120.1452 (3)0.00349 (16)0.2212 (3)0.0700 (8)
H12A0.2246−0.01690.16870.105*
H12B0.0369−0.02870.20190.105*
H12C0.1978−0.00450.30940.105*
U11U22U33U12U13U23
S0.0374 (3)0.0352 (3)0.0829 (5)−0.0002 (2)−0.0066 (3)−0.0011 (3)
N10.0309 (9)0.0361 (9)0.0641 (12)0.0015 (7)−0.0027 (8)0.0017 (9)
N20.0339 (9)0.0374 (10)0.0598 (12)−0.0031 (7)−0.0003 (8)0.0001 (9)
N30.0273 (8)0.0326 (8)0.0443 (10)0.0001 (7)0.0000 (7)0.0000 (7)
N40.0305 (9)0.0416 (10)0.0507 (11)0.0016 (8)−0.0031 (8)0.0013 (8)
C10.0304 (10)0.0400 (11)0.0444 (12)0.0025 (8)0.0028 (9)0.0000 (9)
C20.0333 (11)0.0368 (11)0.0449 (12)−0.0042 (8)0.0042 (9)−0.0016 (9)
C30.0468 (12)0.0380 (12)0.0586 (14)−0.0010 (10)0.0044 (11)0.0004 (11)
C40.0662 (16)0.0398 (13)0.0762 (18)−0.0139 (11)−0.0015 (14)0.0007 (12)
C50.0336 (11)0.0393 (11)0.0568 (14)0.0026 (9)0.0011 (10)0.0017 (10)
C60.0297 (10)0.0505 (12)0.0423 (12)0.0011 (9)0.0042 (9)0.0005 (10)
C70.0349 (11)0.0594 (15)0.0493 (14)−0.0029 (10)0.0042 (10)−0.0021 (11)
C80.0336 (12)0.090 (2)0.0625 (17)−0.0080 (13)0.0014 (12)−0.0046 (15)
C90.0353 (13)0.104 (2)0.0637 (17)0.0157 (15)−0.0003 (12)0.0089 (16)
C100.0513 (14)0.0725 (17)0.0615 (16)0.0261 (13)0.0086 (13)0.0125 (14)
C110.0413 (12)0.0545 (14)0.0538 (14)0.0100 (10)0.0069 (11)0.0033 (11)
C120.0550 (15)0.0620 (17)0.089 (2)−0.0124 (13)0.0029 (14)−0.0045 (15)
S—C11.679 (2)C5—C61.469 (3)
N1—C11.338 (2)C5—H50.9300
N1—N21.373 (2)C6—C111.393 (3)
N1—H1N0.9314C6—C71.399 (3)
N2—C21.296 (2)C7—C81.398 (3)
N3—C11.378 (2)C7—C121.497 (3)
N3—C21.384 (2)C8—C91.369 (4)
N3—N41.395 (2)C8—H80.9300
N4—C51.255 (2)C9—C101.376 (4)
C2—C31.479 (3)C9—H90.9300
C3—C41.522 (3)C10—C111.382 (3)
C3—H3A0.9700C10—H100.9300
C3—H3B0.9700C11—H110.9300
C4—H4A0.9600C12—H12A0.9600
C4—H4B0.9600C12—H12B0.9600
C4—H4C0.9600C12—H12C0.9600
C1—N1—N2114.48 (16)N4—C5—H5120.2
C1—N1—H1N122.2C6—C5—H5120.2
N2—N1—H1N123.2C11—C6—C7120.14 (19)
C2—N2—N1104.15 (15)C11—C6—C5119.32 (19)
C1—N3—C2108.74 (15)C7—C6—C5120.53 (19)
C1—N3—N4132.83 (15)C8—C7—C6117.7 (2)
C2—N3—N4118.30 (15)C8—C7—C12119.6 (2)
C5—N4—N3119.38 (17)C6—C7—C12122.71 (19)
N1—C1—N3102.21 (16)C9—C8—C7121.7 (2)
N1—C1—S127.10 (15)C9—C8—H8119.2
N3—C1—S130.66 (14)C7—C8—H8119.2
N2—C2—N3110.40 (17)C8—C9—C10120.5 (2)
N2—C2—C3126.69 (18)C8—C9—H9119.8
N3—C2—C3122.91 (17)C10—C9—H9119.8
C2—C3—C4112.41 (18)C9—C10—C11119.3 (2)
C2—C3—H3A109.1C9—C10—H10120.3
C4—C3—H3A109.1C11—C10—H10120.3
C2—C3—H3B109.1C10—C11—C6120.7 (2)
C4—C3—H3B109.1C10—C11—H11119.6
H3A—C3—H3B107.9C6—C11—H11119.6
C3—C4—H4A109.5C7—C12—H12A109.5
C3—C4—H4B109.5C7—C12—H12B109.5
H4A—C4—H4B109.5H12A—C12—H12B109.5
C3—C4—H4C109.5C7—C12—H12C109.5
H4A—C4—H4C109.5H12A—C12—H12C109.5
H4B—C4—H4C109.5H12B—C12—H12C109.5
N4—C5—C6119.54 (19)
D—H···AD—HH···AD···AD—H···A
N1—H1N···Si0.932.373.2899 (19)169
C5—H5···S0.932.543.239 (2)132
Table 1

Hydrogen-bond geometry (Å, °)

D—H⋯AD—HH⋯ADAD—H⋯A
N1—H1N⋯Si0.932.373.2899 (19)169
C5—H5⋯S0.932.543.239 (2)132

Symmetry code: (i) .

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