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In the title compound, C12H10FN7S, the dihedral angles made by the plane of the thione-substituted triazole ring with the planes of the other triazole ring and the benzene ring are 71.94 (3) and 40.10 (2)°, respectively. Inter- and intra­mol­ecular hydrogen-bond and π–π stacking inter­actions stabilize the structure.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536805029715/hg6247sup1.cif
Contains datablocks 50128B, I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536805029715/hg6247Isup2.hkl
Contains datablock I

CCDC reference: 287601

Key indicators

  • Single-crystal X-ray study
  • T = 294 K
  • Mean [sigma](C-C) = 0.004 Å
  • R factor = 0.044
  • wR factor = 0.111
  • Data-to-parameter ratio = 14.7

checkCIF/PLATON results

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Alert level C PLAT230_ALERT_2_C Hirshfeld Test Diff for S1 - C5 .. 5.30 su PLAT432_ALERT_2_C Short Inter X...Y Contact F1 .. C2 .. 2.92 Ang.
0 ALERT level A = In general: serious problem 0 ALERT level B = Potentially serious problem 2 ALERT level C = Check and explain 0 ALERT level G = General alerts; check 0 ALERT type 1 CIF construction/syntax error, inconsistent or missing data 2 ALERT type 2 Indicator that the structure model may be wrong or deficient 0 ALERT type 3 Indicator that the structure quality may be low 0 ALERT type 4 Improvement, methodology, query or suggestion

Comment top

Compounds containing the 1,2,4-triazole ring possess a broad pharmacological activity spectrum encompassing anti-inflammatory (Prasad et al., 1989), sedative, smooth-muscle relaxation (Gall et al., 1976), anticonvulsant (Kane et al., 1990), antituberculosis (Mir et al., 1970) and platelet-aggregation inhibitory activities (Lagorce et al., 1992). In search of better biological activity, the title compound, (I), was synthesized. We report here the crystal structure of (I).

The bond lengths and angles of the thione-substituted triazole ring and the other triazole ring (Table 1) are in agreement with the values quotes in previous reports (Li et al., 2005; Xu et al., 2005). The molecule exists in the thione tautomeric form, with an S C distance of 1.668 (2) Å, which indicates substantial double-bond character (Allen et al., 1987). The planes C1–C3/N1–N3 and C6–C12/N7/F1 make angles of 71.94 (3) and 40.10 (2)°, respectively, with the thione-substituted triazole plane C4/C5/N4–N6/S1. The crystal structure of (I) is stabilized by weak intra- and intermolecular hydrogen bonds and double ππ stacking interactions. The ππ stacking interactions invole the thione-substituted triazole ring (C4/C5/N4–N6/S1) R1 and the benzene ring (C7–C12) R2. The distance between the centroids of rings R1 and R2 are 3.589 (8) Å at (−1/2 + x, 1/2 − y, −z) and 3.857 (4) Å at (1/2 + x, 1/2 − y, −z).

Experimental top

A mixture of 4-amino-3-(1,2,4-triazol-1-yl)-1H-1,2,4-triazole-5(4H)-thione (0.02 mol) and 4-fluorobenzaldehyde (0.02 mol) were refluxed at 391 K for 15–20 min in glacial acetic acid to yield a yellow crystalline precitate which was re-crystallized from ethanol to afford yellow crystals of the title compound (5.45 g, yield 90%; m.p. 497–498 K). 1H NMR (DMSO, 600 MHz): δ 14.16 (s, 1H), 10.00 (s, 1H), 8.70 (s, 1H), 7.41–7.99 (m, 4H), 5.70 (s, 2H). IR (KBr, cm−1): 3437, 3109, 2889, 1600, 1509, 1273. Analysis calculated for C12H10FN7S (Mr = 303.3): C 47.52, H 3.32, N 32.32%; found C 47.53, H 3.30, N 32.33%. Single crystals suitable for X-ray measurements were obtained by recrystallization from ethanol at room temperature.

Refinement top

All C-bound H atoms were placed in calculated positions, with C—H = 0.93–0.97 Å, and included in the final cycles of refinement using a riding model, with Uiso(H) = 1.2Ueq(C). NH H atom treatment?

Computing details top

Data collection: SMART (Bruker, 1998); cell refinement: SAINT (Bruker, 1999); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: SHELXTL (Bruker, 1999); software used to prepare material for publication: SHELXTL.

Figures top
[Figure 1] Fig. 1. View of the title compound, (I), with displacement ellipsoids for non-H atoms drawn at the 40% probability level. H atoms are represented as spheres of arbitrary radii.
[Figure 2] Fig. 2. A packing diagram of the molecule of the title compound, viewed down the a axis. Hydrogen bonds are shown as dashed lines.
5-((1H-1,2,4-triazol-1-yl)methyl)-4-(4-fluorobenzylideneamino)-2H- 1,2,4-triazole-3(4H)-thione top
Crystal data top
C12H10FN7SF(000) = 1248
Mr = 303.33Dx = 1.452 Mg m3
Orthorhombic, PbcaMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ac 2abCell parameters from 2822 reflections
a = 7.146 (4) Åθ = 2.3–25.1°
b = 17.906 (9) ŵ = 0.25 mm1
c = 21.697 (11) ÅT = 294 K
V = 2776 (3) Å3Block, yellow
Z = 80.32 × 0.22 × 0.10 mm
Data collection top
Bruker SMART CCD area detector
diffractometer
2855 independent reflections
Radiation source: fine-focus sealed tube1673 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.064
ϕ and ω scansθmax = 26.5°, θmin = 1.9°
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
h = 86
Tmin = 0.910, Tmax = 0.971k = 1722
14610 measured reflectionsl = 2727
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.044Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.111H atoms treated by a mixture of independent and constrained refinement
S = 1.01 w = 1/[σ2(Fo2) + (0.0423P)2 + 0.939P]
where P = (Fo2 + 2Fc2)/3
2855 reflections(Δ/σ)max = 0.001
194 parametersΔρmax = 0.18 e Å3
0 restraintsΔρmin = 0.25 e Å3
Crystal data top
C12H10FN7SV = 2776 (3) Å3
Mr = 303.33Z = 8
Orthorhombic, PbcaMo Kα radiation
a = 7.146 (4) ŵ = 0.25 mm1
b = 17.906 (9) ÅT = 294 K
c = 21.697 (11) Å0.32 × 0.22 × 0.10 mm
Data collection top
Bruker SMART CCD area detector
diffractometer
2855 independent reflections
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
1673 reflections with I > 2σ(I)
Tmin = 0.910, Tmax = 0.971Rint = 0.064
14610 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0440 restraints
wR(F2) = 0.111H atoms treated by a mixture of independent and constrained refinement
S = 1.01Δρmax = 0.18 e Å3
2855 reflectionsΔρmin = 0.25 e Å3
194 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
S10.23628 (11)0.09151 (4)0.48858 (3)0.0593 (2)
F10.1853 (3)0.47698 (12)0.28040 (8)0.1076 (8)
N10.3211 (4)0.45649 (12)0.64024 (10)0.0556 (6)
N20.2937 (3)0.34949 (12)0.69400 (10)0.0535 (6)
N30.1566 (3)0.35474 (11)0.65073 (8)0.0408 (5)
N40.0901 (3)0.16373 (11)0.65095 (8)0.0425 (5)
N50.1469 (3)0.11142 (12)0.60851 (9)0.0434 (5)
N60.1253 (3)0.21347 (10)0.55896 (8)0.0367 (5)
N70.1476 (3)0.27395 (11)0.51807 (8)0.0412 (5)
C10.1769 (4)0.41843 (15)0.61978 (11)0.0513 (7)
H10.09910.43390.58790.062*
C20.3876 (4)0.41172 (15)0.68522 (13)0.0574 (7)
H20.49260.42400.70840.069*
C30.0112 (4)0.29788 (13)0.64484 (11)0.0430 (6)
H3A0.08650.31670.61790.052*
H3B0.04410.28920.68500.052*
C40.0808 (3)0.22546 (13)0.61986 (10)0.0359 (6)
C50.1705 (3)0.13854 (13)0.55131 (11)0.0401 (6)
C60.1001 (3)0.26136 (14)0.46212 (11)0.0423 (6)
H60.05080.21510.45120.051*
C70.1228 (3)0.31919 (14)0.41548 (10)0.0390 (6)
C80.0703 (4)0.30365 (16)0.35493 (11)0.0515 (7)
H80.02200.25690.34530.062*
C90.0889 (4)0.35663 (19)0.30910 (12)0.0630 (8)
H90.05300.34650.26880.076*
C100.1620 (4)0.42445 (18)0.32505 (12)0.0623 (8)
C110.2145 (4)0.44279 (16)0.38383 (11)0.0547 (7)
H110.26220.48990.39290.066*
C120.1948 (3)0.38969 (14)0.42907 (11)0.0443 (6)
H120.22990.40090.46930.053*
H50.156 (4)0.0618 (18)0.6218 (13)0.081 (10)*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
S10.0780 (5)0.0430 (4)0.0570 (4)0.0004 (4)0.0135 (4)0.0167 (3)
F10.170 (2)0.0931 (16)0.0593 (10)0.0086 (14)0.0064 (12)0.0396 (11)
N10.0808 (17)0.0315 (13)0.0544 (13)0.0061 (11)0.0022 (12)0.0023 (11)
N20.0733 (17)0.0336 (13)0.0535 (13)0.0017 (11)0.0156 (11)0.0009 (11)
N30.0594 (13)0.0255 (11)0.0376 (10)0.0034 (9)0.0032 (10)0.0030 (9)
N40.0587 (14)0.0295 (12)0.0393 (11)0.0026 (9)0.0014 (10)0.0001 (10)
N50.0585 (14)0.0253 (12)0.0465 (13)0.0007 (10)0.0032 (10)0.0005 (10)
N60.0500 (12)0.0250 (10)0.0350 (10)0.0007 (9)0.0024 (9)0.0019 (9)
N70.0551 (13)0.0300 (12)0.0386 (11)0.0008 (9)0.0031 (10)0.0042 (9)
C10.077 (2)0.0329 (15)0.0441 (14)0.0028 (14)0.0074 (14)0.0035 (12)
C20.071 (2)0.0352 (16)0.0659 (18)0.0003 (14)0.0135 (15)0.0106 (15)
C30.0528 (15)0.0333 (15)0.0430 (13)0.0011 (11)0.0018 (12)0.0060 (12)
C40.0453 (14)0.0277 (14)0.0348 (12)0.0035 (10)0.0016 (11)0.0000 (11)
C50.0452 (15)0.0278 (14)0.0474 (14)0.0032 (11)0.0002 (12)0.0001 (11)
C60.0458 (16)0.0389 (15)0.0422 (14)0.0007 (12)0.0000 (11)0.0029 (12)
C70.0417 (14)0.0409 (15)0.0344 (13)0.0043 (11)0.0014 (11)0.0002 (11)
C80.0596 (17)0.0527 (18)0.0424 (14)0.0029 (14)0.0034 (13)0.0055 (14)
C90.080 (2)0.077 (2)0.0320 (14)0.0017 (18)0.0095 (13)0.0004 (15)
C100.086 (2)0.062 (2)0.0387 (15)0.0091 (17)0.0040 (15)0.0166 (15)
C110.079 (2)0.0398 (16)0.0456 (15)0.0036 (14)0.0063 (14)0.0034 (13)
C120.0590 (17)0.0412 (16)0.0328 (12)0.0002 (12)0.0010 (11)0.0019 (11)
Geometric parameters (Å, º) top
S1—C51.668 (2)C2—H20.9300
F1—C101.361 (3)C3—C41.491 (3)
N1—C11.313 (3)C3—H3A0.9700
N1—C21.350 (3)C3—H3B0.9700
N2—C21.315 (3)C6—C71.457 (3)
N2—N31.360 (3)C6—H60.9300
N3—C11.331 (3)C7—C81.394 (3)
N3—C31.460 (3)C7—C121.395 (3)
N4—C41.297 (3)C8—C91.381 (4)
N4—N51.375 (3)C8—H80.9300
N5—C51.343 (3)C9—C101.366 (4)
N5—H50.94 (3)C9—H90.9300
N6—C41.376 (3)C10—C111.369 (4)
N6—C51.390 (3)C11—C121.374 (3)
N6—N71.409 (3)C11—H110.9300
N7—C61.280 (3)C12—H120.9300
C1—H10.9300
C1—N1—C2102.3 (2)N4—C4—C3124.7 (2)
C2—N2—N3102.1 (2)N6—C4—C3124.2 (2)
C1—N3—N2109.2 (2)N5—C5—N6102.07 (19)
C1—N3—C3129.1 (2)N5—C5—S1127.36 (19)
N2—N3—C3121.7 (2)N6—C5—S1130.57 (18)
C4—N4—N5104.34 (19)N7—C6—C7120.3 (2)
C5—N5—N4114.2 (2)N7—C6—H6119.9
C5—N5—H5128.2 (18)C7—C6—H6119.9
N4—N5—H5117.4 (18)C8—C7—C12118.6 (2)
C4—N6—C5108.61 (18)C8—C7—C6118.9 (2)
C4—N6—N7120.73 (18)C12—C7—C6122.5 (2)
C5—N6—N7129.80 (18)C9—C8—C7121.0 (3)
C6—N7—N6115.6 (2)C9—C8—H8119.5
N1—C1—N3111.1 (2)C7—C8—H8119.5
N1—C1—H1124.5C10—C9—C8117.7 (2)
N3—C1—H1124.5C10—C9—H9121.1
N2—C2—N1115.4 (2)C8—C9—H9121.1
N2—C2—H2122.3F1—C10—C9118.7 (3)
N1—C2—H2122.3F1—C10—C11117.6 (3)
N3—C3—C4113.6 (2)C9—C10—C11123.6 (3)
N3—C3—H3A108.8C10—C11—C12118.1 (3)
C4—C3—H3A108.8C10—C11—H11120.9
N3—C3—H3B108.8C12—C11—H11120.9
C4—C3—H3B108.8C11—C12—C7120.9 (2)
H3A—C3—H3B107.7C11—C12—H12119.6
N4—C4—N6110.8 (2)C7—C12—H12119.6
C2—N2—N3—C10.2 (3)N4—N5—C5—N60.2 (3)
C2—N2—N3—C3177.7 (2)N4—N5—C5—S1179.46 (18)
C4—N4—N5—C51.1 (3)C4—N6—C5—N50.8 (2)
C4—N6—N7—C6147.8 (2)N7—N6—C5—N5170.0 (2)
C5—N6—N7—C644.1 (3)C4—N6—C5—S1179.6 (2)
C2—N1—C1—N30.4 (3)N7—N6—C5—S110.4 (4)
N2—N3—C1—N10.1 (3)N6—N7—C6—C7178.08 (19)
C3—N3—C1—N1177.1 (2)N7—C6—C7—C8179.8 (2)
N3—N2—C2—N10.4 (3)N7—C6—C7—C120.4 (4)
C1—N1—C2—N20.5 (3)C12—C7—C8—C90.1 (4)
C1—N3—C3—C4112.5 (3)C6—C7—C8—C9179.9 (2)
N2—N3—C3—C470.5 (3)C7—C8—C9—C100.6 (4)
N5—N4—C4—N61.5 (3)C8—C9—C10—F1178.6 (3)
N5—N4—C4—C3175.2 (2)C8—C9—C10—C111.0 (5)
C5—N6—C4—N41.5 (3)F1—C10—C11—C12178.8 (2)
N7—N6—C4—N4171.89 (19)C9—C10—C11—C120.9 (5)
C5—N6—C4—C3175.3 (2)C10—C11—C12—C70.2 (4)
N7—N6—C4—C314.3 (3)C8—C7—C12—C110.3 (4)
N3—C3—C4—N4112.2 (3)C6—C7—C12—C11179.9 (2)
N3—C3—C4—N674.9 (3)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N5—H5···N1i0.94 (3)1.94 (3)2.867 (3)174 (3)
C6—H6···S10.932.703.244 (3)118
C9—H9···N4ii0.932.583.451 (4)157
C11—H11···S1iii0.932.763.519 (3)139
Symmetry codes: (i) x+1/2, y1/2, z; (ii) x, y+1/2, z1/2; (iii) x+1/2, y+1/2, z.

Experimental details

Crystal data
Chemical formulaC12H10FN7S
Mr303.33
Crystal system, space groupOrthorhombic, Pbca
Temperature (K)294
a, b, c (Å)7.146 (4), 17.906 (9), 21.697 (11)
V3)2776 (3)
Z8
Radiation typeMo Kα
µ (mm1)0.25
Crystal size (mm)0.32 × 0.22 × 0.10
Data collection
DiffractometerBruker SMART CCD area detector
diffractometer
Absorption correctionMulti-scan
(SADABS; Sheldrick, 1996)
Tmin, Tmax0.910, 0.971
No. of measured, independent and
observed [I > 2σ(I)] reflections
14610, 2855, 1673
Rint0.064
(sin θ/λ)max1)0.627
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.044, 0.111, 1.01
No. of reflections2855
No. of parameters194
H-atom treatmentH atoms treated by a mixture of independent and constrained refinement
Δρmax, Δρmin (e Å3)0.18, 0.25

Computer programs: SMART (Bruker, 1998), SAINT (Bruker, 1999), SAINT, SHELXS97 (Sheldrick, 1997), SHELXL97 (Sheldrick, 1997), SHELXTL (Bruker, 1999), SHELXTL.

Selected geometric parameters (Å, º) top
S1—C51.668 (2)N4—N51.375 (3)
N2—N31.360 (3)N6—N71.409 (3)
C6—N7—N6115.6 (2)N3—C3—C4113.6 (2)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N5—H5···N1i0.94 (3)1.94 (3)2.867 (3)174 (3)
C6—H6···S10.932.703.244 (3)117.8
C9—H9···N4ii0.932.583.451 (4)156.8
C11—H11···S1iii0.932.763.519 (3)139.2
Symmetry codes: (i) x+1/2, y1/2, z; (ii) x, y+1/2, z1/2; (iii) x+1/2, y+1/2, z.
 

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