Abstract
In the title compound, C8H8N4, the dihedral angle between the triazole ring [maximum deviation = 0.003 (1) Å] and the benzene ring is 34.57 (7)°. In the crystal, molecules are linked into sheets lying parallel to the ac plane via intermolecular N—H⋯N and C—H⋯N hydrogen bonds. Aromatic π–π [centroid–centroid distance = 3.6750 (8) Å] stacking and N—H⋯π interactions are also observed.
Related literature
For general background to and the biological activity of triazole derivatives, see: Isloor et al. (2000 ▶, 2009 ▶); Soliman et al. (2001 ▶); Holla et al. (2000 ▶); Sunil et al. (2009 ▶). For bond-length data, see: Allen et al. (1987 ▶). For a related structure, see: Fun et al. (2010 ▶).
Experimental
Crystal data
C8H8N4
M r = 160.18
Monoclinic,
a = 5.5488 (1) Å
b = 7.3656 (2) Å
c = 19.5477 (5) Å
β = 99.416 (2)°
V = 788.15 (3) Å3
Z = 4
Mo Kα radiation
μ = 0.09 mm−1
T = 296 K
0.50 × 0.42 × 0.14 mm
Data collection
Bruker SMART APEXII CCD diffractometer
Absorption correction: multi-scan (SADABS; Bruker, 2009 ▶) T min = 0.957, T max = 0.988
8036 measured reflections
2160 independent reflections
1722 reflections with I > 2σ(I)
R int = 0.030
Refinement
R[F 2 > 2σ(F 2)] = 0.044
wR(F 2) = 0.118
S = 1.05
2160 reflections
110 parameters
H atoms treated by a mixture of independent and constrained refinement
Δρmax = 0.23 e Å−3
Δρmin = −0.17 e Å−3
Data collection: APEX2 (Bruker, 2009 ▶); cell refinement: SAINT (Bruker, 2009 ▶); data reduction: SAINT; program(s) used to solve structure: SHELXTL (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXTL; molecular graphics: SHELXTL; software used to prepare material for publication: SHELXTL and PLATON (Spek, 2009 ▶).
Supplementary Material
Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536810052025/hb5764sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536810052025/hb5764Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report
Table 1. Hydrogen-bond geometry (Å, °).
Cg2 is the centroid of the C3–C8 phenyl ring.
| D—H⋯A | D—H | H⋯A | D⋯A | D—H⋯A |
|---|---|---|---|---|
| N4—H2N4⋯N1i | 0.871 (16) | 2.208 (16) | 3.0709 (18) | 171.1 (15) |
| C1—H1A⋯N2ii | 0.93 | 2.50 | 3.4035 (16) | 166 |
| N4—H1N4⋯Cg2iii | 0.87 (2) | 2.58 (2) | 3.3929 (16) | 156.0 (17) |
Symmetry codes: (i)
; (ii)
; (iii)
.
Acknowledgments
HKF and CKQ thank Universiti Sains Malaysia (USM) for the Research University Grant (No. 1001/PFIZIK/811160). CKQ also thanks USM for the award of a USM fellowship. AMI is thankful to the Director of the National Institute of Technology for providing research facilities and also thanks the Board for Research in Nuclear Sciences, Department of Atomic Energy, Government of India, for a Young Scientist Award.
supplementary crystallographic information
Comment
Compounds incorporating heterocyclic ring systems continue to attract considerable interests due to the wide range of biological activities they possess (Isloor et al., 2000). Triazoles are a class of heterocyclic compounds having a five-membered ring of two carbon atoms and three nitrogen atoms (Soliman et al., 2001). They have wide range of applications. In last few decades, triazoles have received much significant attention in the field of medicinal chemistry because of their diversified biological properties like antibacterial (Isloor et al., 2009) and antifungal (Holla et al., 2000) activities. In recent years, 1,2,4-triazole derivatives have been found to associate with anticancer properties (Sunil et al., 2009). It is also observed that incorporation of aryl constituent into the triazoles ring systems augments the biological activities considerably.
In the title molecule (Fig. 1), the triazol-1-yl ring (N1-N3/C1/C2, maximum deviation = 0.003 (1) Å at atom N3) is inclined at angle of 34.57 (7)° with phenyl (C3-C8) ring. Bond lengths (Allen et al., 1987) and angles are within normal ranges and are comparable to a related structure (Fun et al., 2010).
In the crystal packing (Fig. 2), the molecules are linked into two-dimensional sheets parallel to the ac-plane via intermolecular N4–H2N4···N1 and C1–H1A···N2 hydrogen bonds. π-π stacking interactions between the centroids of N1-N3/C1/C2 triazol-1-yl rings (Cg1), with Cg1···Cg1i distance of 3.6750 (8) Å [symmetry code: (i) 1-X, -Y, 2-Z] are observed. The crystal structure is further consilidated by N4–H1N4···Cg2 (Table 1) interactions, where Cg2 is the centroid of C3-C8 phenyl ring.
Experimental
1,2,4-Triazole (2 g, 0.02 mol) was added lot-wise to a suspension of sodium hydride (60%, 1.47 g, 0.0308 mol) in dry DMF (20 ml) at 0°C. After the addition, the reaction mixture was stirred at the same temperature for 30 min. A solution of 4-fluoro nitrobenzene (2.82 g, 0.02 mol) in dry DMF (20 ml) was then added and the reaction mixture was stirred at room temperature for 18 h. The reaction mixture was then quenched with ice water and extracted with ethyl acetate. The organic layer was concentrated to afford a yellow solid as a nitro compound intermediate (3 g). This nitro compound was taken in methanol (30 ml) and hydrogenated using 10% palladium on carbon (0.2 g) at 3-kg pressure of hydrogen. After the reaction was over, the catalyst was filtered, the filtrate was concentrated to afford the title compound as a yellow solid. Yellow blocks were recrystallised from ethanol. Yield : 2.8g, 60 %. M.p. 433-435K.
Refinement
H1N4 and H2N4 were located in a difference Fourier map and allowed to refined freely. The remaining H atoms were positioned geometrically and refined using a riding model with C–H = 0.93 Å and Uiso(H) = 1.2 Ueq(C). The highest residual electron density peak is located at 0.67 Å from C3 and the deepest hole is located at 1.27 Å from C8.
Figures
Fig. 1.
The molecular structure of the title compound showing 50% probability displacement ellipsoids for non-H atoms.
Fig. 2.
The crystal structure of the title compound, viewed along the b axis. H atoms not involved in hydrogen bonds (dashed lines) have been omitted for clarity.
Crystal data
| C8H8N4 | F(000) = 336 |
| Mr = 160.18 | Dx = 1.350 Mg m−3 |
| Monoclinic, P21/c | Mo Kα radiation, λ = 0.71073 Å |
| Hall symbol: -P 2ybc | Cell parameters from 3245 reflections |
| a = 5.5488 (1) Å | θ = 3.0–29.1° |
| b = 7.3656 (2) Å | µ = 0.09 mm−1 |
| c = 19.5477 (5) Å | T = 296 K |
| β = 99.416 (2)° | Block, yellow |
| V = 788.15 (3) Å3 | 0.50 × 0.42 × 0.14 mm |
| Z = 4 |
Data collection
| Bruker SMART APEXII CCD diffractometer | 2160 independent reflections |
| Radiation source: fine-focus sealed tube | 1722 reflections with I > 2σ(I) |
| graphite | Rint = 0.030 |
| φ and ω scans | θmax = 29.4°, θmin = 2.1° |
| Absorption correction: multi-scan (SADABS; Bruker, 2009) | h = −7→7 |
| Tmin = 0.957, Tmax = 0.988 | k = −10→10 |
| 8036 measured reflections | l = −26→24 |
Refinement
| Refinement on F2 | Secondary atom site location: difference Fourier map |
| Least-squares matrix: full | Hydrogen site location: inferred from neighbouring sites |
| R[F2 > 2σ(F2)] = 0.044 | H atoms treated by a mixture of independent and constrained refinement |
| wR(F2) = 0.118 | w = 1/[σ2(Fo2) + (0.0509P)2 + 0.1531P] where P = (Fo2 + 2Fc2)/3 |
| S = 1.05 | (Δ/σ)max = 0.001 |
| 2160 reflections | Δρmax = 0.23 e Å−3 |
| 110 parameters | Δρmin = −0.17 e Å−3 |
| 0 restraints | Extinction correction: SHELXTL (Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4 |
| Primary atom site location: structure-invariant direct methods | Extinction coefficient: 0.042 (5) |
Special details
| 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. |
| 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 > 2sigma(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)
| x | y | z | Uiso*/Ueq | ||
| N1 | 0.3298 (2) | 0.17124 (18) | 1.08332 (6) | 0.0542 (3) | |
| N2 | 0.58582 (19) | 0.24895 (17) | 1.00992 (6) | 0.0498 (3) | |
| N3 | 0.34993 (17) | 0.26004 (14) | 0.97774 (5) | 0.0378 (3) | |
| N4 | 0.0895 (3) | 0.4820 (2) | 0.70184 (6) | 0.0597 (4) | |
| C1 | 0.2029 (2) | 0.2126 (2) | 1.02227 (7) | 0.0480 (3) | |
| H1A | 0.0334 | 0.2092 | 1.0117 | 0.058* | |
| C2 | 0.5611 (3) | 0.1960 (2) | 1.07255 (7) | 0.0533 (4) | |
| H2A | 0.6948 | 0.1768 | 1.1072 | 0.064* | |
| C3 | 0.2865 (2) | 0.31773 (16) | 0.90734 (6) | 0.0360 (3) | |
| C4 | 0.4336 (2) | 0.27300 (17) | 0.85909 (6) | 0.0411 (3) | |
| H4A | 0.5752 | 0.2056 | 0.8724 | 0.049* | |
| C5 | 0.3691 (2) | 0.32893 (18) | 0.79107 (6) | 0.0432 (3) | |
| H5A | 0.4686 | 0.2986 | 0.7589 | 0.052* | |
| C6 | 0.1573 (2) | 0.43007 (17) | 0.76988 (6) | 0.0404 (3) | |
| C7 | 0.0123 (2) | 0.47403 (17) | 0.81966 (6) | 0.0434 (3) | |
| H7A | −0.1296 | 0.5415 | 0.8068 | 0.052* | |
| C8 | 0.0763 (2) | 0.41891 (17) | 0.88743 (6) | 0.0415 (3) | |
| H8A | −0.0218 | 0.4496 | 0.9200 | 0.050* | |
| H2N4 | 0.171 (3) | 0.447 (2) | 0.6697 (8) | 0.065 (5)* | |
| H1N4 | −0.029 (3) | 0.560 (3) | 0.6921 (9) | 0.078 (6)* |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| N1 | 0.0549 (7) | 0.0658 (8) | 0.0435 (6) | 0.0049 (6) | 0.0124 (5) | 0.0063 (5) |
| N2 | 0.0340 (5) | 0.0681 (8) | 0.0452 (6) | −0.0015 (5) | 0.0006 (4) | 0.0051 (5) |
| N3 | 0.0318 (5) | 0.0448 (5) | 0.0367 (5) | 0.0009 (4) | 0.0052 (4) | −0.0009 (4) |
| N4 | 0.0711 (8) | 0.0683 (9) | 0.0406 (6) | 0.0212 (7) | 0.0116 (6) | 0.0085 (6) |
| C1 | 0.0392 (6) | 0.0616 (8) | 0.0447 (7) | 0.0024 (6) | 0.0115 (5) | 0.0042 (6) |
| C2 | 0.0485 (7) | 0.0650 (9) | 0.0439 (7) | 0.0014 (6) | −0.0002 (6) | 0.0047 (6) |
| C3 | 0.0324 (5) | 0.0396 (6) | 0.0355 (6) | −0.0019 (4) | 0.0043 (4) | −0.0023 (4) |
| C4 | 0.0313 (5) | 0.0480 (7) | 0.0445 (7) | 0.0041 (5) | 0.0074 (5) | −0.0005 (5) |
| C5 | 0.0388 (6) | 0.0518 (7) | 0.0412 (6) | 0.0008 (5) | 0.0133 (5) | −0.0019 (5) |
| C6 | 0.0427 (6) | 0.0395 (6) | 0.0386 (6) | −0.0027 (5) | 0.0051 (5) | −0.0006 (5) |
| C7 | 0.0388 (6) | 0.0453 (7) | 0.0451 (7) | 0.0081 (5) | 0.0042 (5) | −0.0005 (5) |
| C8 | 0.0375 (6) | 0.0468 (7) | 0.0413 (6) | 0.0053 (5) | 0.0096 (5) | −0.0049 (5) |
Geometric parameters (Å, °)
| N1—C1 | 1.3183 (17) | C3—C4 | 1.3842 (16) |
| N1—C2 | 1.3468 (19) | C3—C8 | 1.3851 (16) |
| N2—C2 | 1.3134 (18) | C4—C5 | 1.3821 (17) |
| N2—N3 | 1.3587 (14) | C4—H4A | 0.9300 |
| N3—C1 | 1.3332 (16) | C5—C6 | 1.3957 (17) |
| N3—C3 | 1.4284 (14) | C5—H5A | 0.9300 |
| N4—C6 | 1.3758 (16) | C6—C7 | 1.3987 (17) |
| N4—H2N4 | 0.871 (18) | C7—C8 | 1.3755 (16) |
| N4—H1N4 | 0.87 (2) | C7—H7A | 0.9300 |
| C1—H1A | 0.9300 | C8—H8A | 0.9300 |
| C2—H2A | 0.9300 | ||
| C1—N1—C2 | 102.04 (11) | C8—C3—N3 | 119.62 (10) |
| C2—N2—N3 | 102.11 (11) | C5—C4—C3 | 119.72 (11) |
| C1—N3—N2 | 109.16 (10) | C5—C4—H4A | 120.1 |
| C1—N3—C3 | 128.78 (10) | C3—C4—H4A | 120.1 |
| N2—N3—C3 | 122.06 (10) | C4—C5—C6 | 121.17 (11) |
| C6—N4—H2N4 | 121.5 (11) | C4—C5—H5A | 119.4 |
| C6—N4—H1N4 | 118.2 (12) | C6—C5—H5A | 119.4 |
| H2N4—N4—H1N4 | 120.1 (16) | N4—C6—C5 | 121.27 (12) |
| N1—C1—N3 | 111.01 (12) | N4—C6—C7 | 120.72 (12) |
| N1—C1—H1A | 124.5 | C5—C6—C7 | 118.00 (11) |
| N3—C1—H1A | 124.5 | C8—C7—C6 | 120.95 (11) |
| N2—C2—N1 | 115.69 (12) | C8—C7—H7A | 119.5 |
| N2—C2—H2A | 122.2 | C6—C7—H7A | 119.5 |
| N1—C2—H2A | 122.2 | C7—C8—C3 | 120.16 (11) |
| C4—C3—C8 | 120.00 (11) | C7—C8—H8A | 119.9 |
| C4—C3—N3 | 120.38 (10) | C3—C8—H8A | 119.9 |
| C2—N2—N3—C1 | −0.42 (15) | C8—C3—C4—C5 | −0.32 (19) |
| C2—N2—N3—C3 | 178.65 (11) | N3—C3—C4—C5 | 179.64 (11) |
| C2—N1—C1—N3 | −0.25 (16) | C3—C4—C5—C6 | 0.0 (2) |
| N2—N3—C1—N1 | 0.44 (16) | C4—C5—C6—N4 | −178.34 (13) |
| C3—N3—C1—N1 | −178.55 (12) | C4—C5—C6—C7 | 0.26 (19) |
| N3—N2—C2—N1 | 0.29 (17) | N4—C6—C7—C8 | 178.50 (13) |
| C1—N1—C2—N2 | −0.04 (18) | C5—C6—C7—C8 | −0.11 (19) |
| C1—N3—C3—C4 | −146.03 (13) | C6—C7—C8—C3 | −0.3 (2) |
| N2—N3—C3—C4 | 35.09 (17) | C4—C3—C8—C7 | 0.48 (19) |
| C1—N3—C3—C8 | 33.93 (19) | N3—C3—C8—C7 | −179.49 (11) |
| N2—N3—C3—C8 | −144.95 (12) |
Hydrogen-bond geometry (Å, °)
| Cg2 is the centroid of the C3–C8 phenyl ring. |
| D—H···A | D—H | H···A | D···A | D—H···A |
| N4—H2N4···N1i | 0.871 (16) | 2.208 (16) | 3.0709 (18) | 171.1 (15) |
| C1—H1A···N2ii | 0.93 | 2.50 | 3.4035 (16) | 166 |
| N4—H1N4···Cg2iii | 0.87 (2) | 2.58 (2) | 3.3929 (16) | 156.0 (17) |
Symmetry codes: (i) x, −y+1/2, z−1/2; (ii) x−1, y, z; (iii) −x, y+1/2, −z+3/2.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: HB5764).
References
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Associated Data
This section collects any data citations, data availability statements, or supplementary materials included in this article.
Supplementary Materials
Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536810052025/hb5764sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536810052025/hb5764Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report


