supplementary materials


gk2112 scheme

Acta Cryst. (2008). E64, o374    [ doi:10.1107/S1600536807062149 ]

4-(5-Bromo-2-hydroxybenzylideneamino)-3-methyl-1H-1,2,4-triazole-5(4H)-thione

M. Wang, M. Cao, B. Hu, C. X. Cheng and X. G. Song

Abstract top

In the title compound, C10H9BrN4OS, the triazole ring forms a dihedral angle of 72.05 (14)° with the benzene ring. The conformation of the molecule is stabilized by intramolecular O-H...·N hydrogen bonding. The crystal packing is determined by intermolecular N-H...S interactions, a short Br...S contact of 3.4464 (13) Å and [pi]-[pi] stacking of the triazole rings and of the benzene rings (centroid-centroid distances of 3.4109 and 3.569 Å, respectively).

Comment top

Recently, compounds containing 1H-1,2,4-triazole group have attracted much interest because compounds containing this ring system are well known as efficient fungicides in pesticides and they exhibit good plant-growth regulatory activity for a wide variety of crops (Xu et al., 2002). In addition, amine- and thione-substituted triazoles have been studied as anti-inflamatory and antimicrobial agents (Eweiss et al., 1986; Awad et al., 1991). In a search for new triazole compounds with better biological activity, the title compound, (I), was synthesized and we report here its crystal structure.

The molecule of (I) exists in the thione tautomeric form, with the S==C distance of 1.681 (4) Å, which indicates a substantial double-bond character (Allen et al., 1987). The dihedral angle between the thione-substituted triazole ring and the benzene ring is 72.05 (14)°. The crystal packing is determined by intermolecular N–H···S interaction (Table 1), short Br···S contact of 3.4464 (13) Å and π-π stacking of the triazole rings (centroid-to-centrod distance of 3.410 Å) and π-π stacking of the benzene rings (centroid-to-centrod distance of 3.569 Å).

Related literature top

For related literature, see: Allen et al. (1987); Awad et al. (1991); Eweiss et al. (1986); Ji et al. (2002); Mohan (1983); Xu et al. (2002).

Experimental top

4-Amino-5-methyl-1,2,4-triazole-3-thione (0.02 mol in 15 ml e thanol), synthesized according to a reported method (Mohan, 1983), was added to a solution of 5-bromosalicylaldehyde (0.02 mol in 20 ml). Then several drops of concentrated sulfuric acid were added to the solution, which was then refluxed for 1 h. The mixture was filtered and crystallized from ethanol to afford the title compound (I). Yellow plates of (I) were obtained by recrystallization from ethanol at room temperature.

Refinement top

The N– and O-bound H atoms were located in difference maps and refined with distance restraints [N–H = 0.86 (2) Å, O–H = 0.82 (2) Å] and the constraints for Uiso(H) = 1.5Ueq(N, O).

The C-bound H atoms were geometrically placed in idealized positions [C–H = 0.96 Å (methyl), 0.96 Å (aromatic), 0.96 Å (methine)]. Isotropic displacement parameters of H atoms were: Uiso(H)=1.5Ueq(C, methyl), Uiso(H) = 1.2Ueq(C, aromatic and methine).

Computing details top

Data collection: SMART (Bruker, 2001); cell refinement: SAINT (Bruker, 2001); data reduction: SAINT (Bruker, 2001); program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: SHELXTL (Bruker, 2001); software used to prepare material for publication: SHELXTL (Bruker, 2001).

Figures top
[Figure 1] Fig. 1. View of the molecular structure of (I), showing 50% probability displacement ellipsoids for the non-hydrogen atoms.
[Figure 2] Fig. 2. Part of the crystal structure of (I) showing the formation of the two-dimensional network. Hydrogen bonds are shown as dashed lines.
4-(5-Bromo-2-hydroxylbenzylideneamino)-3-methyl-1H-1,2,4-triazole-5(4H)-thione top
Crystal data top
C10H9BrN4OSZ = 2
Mr = 313.18F000 = 312
Triclinic, P1Dx = 1.730 Mg m3
Hall symbol: -P 1Mo Kα radiation
λ = 0.71073 Å
a = 6.9780 (8) ÅCell parameters from 1728 reflections
b = 7.1529 (8) Åθ = 2.9–26.2º
c = 12.3119 (14) ŵ = 3.58 mm1
α = 83.561 (2)ºT = 293 (2) K
β = 88.820 (2)ºPlate, yellow
γ = 79.987 (2)º0.30 × 0.28 × 0.26 mm
V = 601.35 (12) Å3
Data collection top
Bruker SMART CCD
diffractometer
2560 independent reflections
Radiation source: fine-focus sealed tube1977 reflections with I > 2σ(I)
Monochromator: graphiteRint = 0.038
T = 293(2) Kθmax = 27.0º
ω scansθmin = 1.7º
Absorption correction: multi-scan
(Blessing; 1995)
h = 8→8
Tmin = 0.404, Tmax = 0.519k = 9→8
4340 measured reflectionsl = 13→15
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.040H atoms treated by a mixture of
independent and constrained refinement
wR(F2) = 0.111  w = 1/[σ2(Fo2) + (0.0416P)2 + 0.455P]
where P = (Fo2 + 2Fc2)/3
S = 1.10(Δ/σ)max = 0.001
2560 reflectionsΔρmax = 0.42 e Å3
161 parametersΔρmin = 0.58 e Å3
2 restraintsExtinction correction: none
Primary atom site location: structure-invariant direct methods
Crystal data top
C10H9BrN4OSγ = 79.987 (2)º
Mr = 313.18V = 601.35 (12) Å3
Triclinic, P1Z = 2
a = 6.9780 (8) ÅMo Kα
b = 7.1529 (8) ŵ = 3.58 mm1
c = 12.3119 (14) ÅT = 293 (2) K
α = 83.561 (2)º0.30 × 0.28 × 0.26 mm
β = 88.820 (2)º
Data collection top
Bruker SMART CCD
diffractometer
2560 independent reflections
Absorption correction: multi-scan
(Blessing; 1995)
1977 reflections with I > 2σ(I)
Tmin = 0.404, Tmax = 0.519Rint = 0.038
4340 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0402 restraints
wR(F2) = 0.111H atoms treated by a mixture of
independent and constrained refinement
S = 1.10Δρmax = 0.42 e Å3
2560 reflectionsΔρmin = 0.58 e Å3
161 parameters
Special details top

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.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
Br10.79546 (7)0.36351 (7)0.64076 (4)0.05088 (18)
C10.2803 (6)0.3219 (6)0.0688 (3)0.0386 (9)
C20.5585 (6)0.2362 (6)0.0218 (3)0.0383 (9)
C30.7615 (6)0.1524 (7)0.0409 (4)0.0500 (11)
H3A0.78320.14810.11780.075*
H3B0.78860.02530.00380.075*
H3C0.84570.22900.01340.075*
C40.5834 (6)0.2340 (6)0.2504 (3)0.0387 (9)
H40.55140.36630.23710.046*
C50.6609 (5)0.1469 (6)0.3552 (3)0.0350 (9)
C60.6983 (5)0.0480 (6)0.3857 (3)0.0377 (9)
C70.7585 (6)0.1188 (6)0.4911 (3)0.0415 (10)
H70.78070.25000.51140.050*
C80.7855 (6)0.0030 (6)0.5659 (3)0.0422 (10)
H80.82590.04560.63650.051*
C90.7521 (5)0.2008 (6)0.5355 (3)0.0356 (9)
C100.6892 (6)0.2752 (6)0.4322 (3)0.0384 (9)
H100.66540.40650.41260.046*
N10.4330 (5)0.3251 (5)0.0963 (3)0.0419 (8)
N20.2652 (5)0.3746 (5)0.0387 (3)0.0372 (8)
N30.4714 (5)0.2332 (4)0.0799 (3)0.0355 (8)
N40.5586 (5)0.1292 (5)0.1755 (3)0.0398 (8)
O10.6727 (5)0.1790 (4)0.3183 (3)0.0500 (8)
S10.10932 (16)0.35060 (17)0.16652 (9)0.0457 (3)
H20.161 (5)0.440 (6)0.069 (4)0.069*
H10.640 (8)0.123 (7)0.258 (2)0.069*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Br10.0587 (3)0.0552 (3)0.0373 (3)0.0031 (2)0.0109 (2)0.0079 (2)
C10.044 (2)0.037 (2)0.035 (2)0.0072 (18)0.0095 (18)0.0040 (18)
C20.043 (2)0.033 (2)0.041 (2)0.0098 (18)0.0050 (18)0.0098 (18)
C30.047 (3)0.047 (3)0.055 (3)0.004 (2)0.003 (2)0.005 (2)
C40.038 (2)0.040 (2)0.036 (2)0.0030 (18)0.0052 (17)0.0012 (18)
C50.0302 (19)0.041 (2)0.034 (2)0.0083 (17)0.0078 (16)0.0013 (18)
C60.0279 (19)0.033 (2)0.047 (2)0.0047 (16)0.0057 (17)0.0024 (19)
C70.039 (2)0.036 (2)0.045 (2)0.0042 (18)0.0069 (19)0.0075 (19)
C80.035 (2)0.050 (3)0.036 (2)0.0016 (19)0.0069 (17)0.010 (2)
C90.0286 (19)0.040 (2)0.038 (2)0.0015 (16)0.0091 (16)0.0059 (18)
C100.038 (2)0.033 (2)0.039 (2)0.0024 (17)0.0083 (18)0.0067 (18)
N10.046 (2)0.046 (2)0.0337 (18)0.0062 (17)0.0059 (16)0.0034 (16)
N20.0391 (19)0.0380 (19)0.0325 (18)0.0021 (15)0.0100 (15)0.0007 (15)
N30.0396 (18)0.0323 (18)0.0345 (18)0.0054 (15)0.0119 (14)0.0024 (14)
N40.0440 (19)0.0285 (17)0.0389 (19)0.0097 (14)0.0155 (15)0.0086 (15)
O10.062 (2)0.0376 (17)0.0481 (19)0.0034 (15)0.0136 (16)0.0005 (15)
S10.0458 (6)0.0541 (7)0.0325 (6)0.0015 (5)0.0055 (4)0.0006 (5)
Geometric parameters (Å, °) top
Br1—C91.898 (4)C5—C101.431 (5)
C1—N21.336 (5)C6—O11.356 (5)
C1—N31.375 (5)C6—C71.385 (6)
C1—S11.681 (4)C7—C81.373 (6)
C2—N11.312 (5)C7—H70.9300
C2—N31.381 (5)C8—C91.402 (6)
C2—C31.463 (6)C8—H80.9300
C3—H3A0.9600C9—C101.372 (5)
C3—H3B0.9600C10—H100.9300
C3—H3C0.9600N1—N21.370 (5)
C4—N41.285 (5)N2—H20.862 (19)
C4—C51.440 (5)N3—N41.409 (4)
C4—H40.9300O1—H10.821 (19)
C5—C61.383 (5)
N2—C1—N3102.6 (3)C8—C7—C6120.5 (4)
N2—C1—S1129.2 (3)C8—C7—H7119.7
N3—C1—S1128.2 (3)C6—C7—H7119.7
N1—C2—N3109.8 (4)C7—C8—C9119.9 (4)
N1—C2—C3126.3 (4)C7—C8—H8120.1
N3—C2—C3123.9 (4)C9—C8—H8120.1
C2—C3—H3A109.5C10—C9—C8120.8 (4)
C2—C3—H3B109.5C10—C9—Br1120.7 (3)
H3A—C3—H3B109.5C8—C9—Br1118.4 (3)
C2—C3—H3C109.5C9—C10—C5118.8 (4)
H3A—C3—H3C109.5C9—C10—H10120.6
H3B—C3—H3C109.5C5—C10—H10120.6
N4—C4—C5120.0 (4)C2—N1—N2104.2 (3)
N4—C4—H4120.0C1—N2—N1114.4 (3)
C5—C4—H4120.0C1—N2—H2123 (3)
C6—C5—C10119.7 (4)N1—N2—H2122 (3)
C6—C5—C4124.2 (4)C1—N3—C2109.0 (3)
C10—C5—C4116.0 (4)C1—N3—N4126.2 (3)
O1—C6—C5123.4 (4)C2—N3—N4124.1 (3)
O1—C6—C7116.3 (4)C4—N4—N3113.7 (3)
C5—C6—C7120.3 (4)C6—O1—H1109 (4)
N4—C4—C5—C65.4 (6)C3—C2—N1—N2179.5 (4)
N4—C4—C5—C10178.1 (4)N3—C1—N2—N10.2 (4)
C10—C5—C6—O1179.1 (3)S1—C1—N2—N1178.5 (3)
C4—C5—C6—O12.6 (6)C2—N1—N2—C10.5 (4)
C10—C5—C6—C71.5 (6)N2—C1—N3—C20.7 (4)
C4—C5—C6—C7174.9 (4)S1—C1—N3—C2178.0 (3)
O1—C6—C7—C8179.0 (4)N2—C1—N3—N4171.4 (3)
C5—C6—C7—C81.3 (6)S1—C1—N3—N47.3 (6)
C6—C7—C8—C90.0 (6)N1—C2—N3—C11.1 (4)
C7—C8—C9—C101.2 (6)C3—C2—N3—C1179.3 (4)
C7—C8—C9—Br1179.0 (3)N1—C2—N3—N4172.1 (3)
C8—C9—C10—C50.9 (6)C3—C2—N3—N48.4 (6)
Br1—C9—C10—C5179.2 (3)C5—C4—N4—N3176.5 (3)
C6—C5—C10—C90.4 (6)C1—N3—N4—C471.7 (5)
C4—C5—C10—C9176.3 (3)C2—N3—N4—C4118.9 (4)
N3—C2—N1—N20.9 (4)
Hydrogen-bond geometry (Å, °) top
D—H···AD—HH···AD···AD—H···A
N2—H2···S1i0.862 (19)2.44 (2)3.295 (3)173 (5)
O1—H1···N40.821 (19)1.97 (4)2.676 (4)144 (5)
O1—H1···N1ii0.821 (19)2.69 (5)3.178 (5)120 (5)
Symmetry codes: (i) −x, −y+1, −z; (ii) −x+1, −y, −z.
Table 1
Hydrogen-bond geometry (Å, °)
top
D—H···AD—HH···AD···AD—H···A
N2—H2···S1i0.862 (19)2.44 (2)3.295 (3)173 (5)
O1—H1···N40.821 (19)1.97 (4)2.676 (4)144 (5)
O1—H1···N1ii0.821 (19)2.69 (5)3.178 (5)120 (5)
Symmetry codes: (i) −x, −y+1, −z; (ii) −x+1, −y, −z.
Acknowledgements top

We thank Xianggao Meng for assistance with testing and refinement of the crystal structure.

references
References top

Allen, F. H., Kennard, O., Watson, D. G., Brammer, L., Orpen, A. G. & Taylor, R. (1987). J. Chem. Soc. Perkin Trans. 2, pp. S1–19.

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Eweiss, N., Bahajaj, A. & Elsherbini, E. (1986). J. Heterocycl. Chem. 23, 1451–1458.

b>Ji et al. (2002). PLEASE SUPPLY FULL REFERENCE

Mohan, J. A. G. (1983). Indian J. Chem. B22, 270–271.

Sheldrick, G. M. (1997). SHELXS97 and SHELXL97. University of Göttingen, Germany.

Xu, L. Z., Zhang, S. S., Li, H. J. & Jiao, K. (2002). J. Chem. Res. Chin. Univ. 18, 284–286.