organic compounds
2-Benzyl-6-nitro-2H-indazole
aLaboratoire de Chimie Organique Hétérocyclique, Centre de Recherche des Sciences des médicaments, URAC 21, Pôle de Compétence Pharmacochimie, Av Ibn Battouta, BP 1014, Faculté des Sciences, Université Mohammed V, Rabat, Morocco, and bDepartment of Chemistry, Tulane University, New Orleans, LA 70118, USA
*Correspondence e-mail: jalilmostafa202@gmail.com
In the title compound, C14H11N3O2, the indazole portion is planar to within 0.022 (2) Å and subtends a dihedral angle of 65.87 (7)° with the pendant benzene ring. In the crystal, oblique stacks of molecules extending along the a-axis direction are generated by π–π stacking interactions between the five- and six-membered rings [centroid–centroid separation = 3.6743 (19) Å] and the stacks are cross-linked by C—H⋯O hydrogen bonds.
Keywords: crystal structure; indazole; hydrogen bond; π–π stacking.
CCDC reference: 1818813
Structure description
Although rare in nature (Liu et al., 2004; Ali et al., 2008), indazoles exhibit a variety of biological activities such as HIV protease inhibition (Patel et al., 1999), antiarrhythmic and analgesic activities (Mosti et al., 2000). As a continuation of our studies of indazole derivatives (Mohamed Abdelahi et al., 2017), we report the synthesis and structure of the title compound (Fig. 1).
The indazole portion is almost planar (r.m.s. deviation 0.017 Å) with the atoms farthest from the mean plane being C6 (0.018 (2) Å) and C5 (−0.022 (2) Å). The dihedral angle between the mean plane of the indazole unit and the benzene ring of the benzyl side chain is 65.87 (7)°. The crystal packing involves oblique stacks of molecules extending along the a-axis direction formed by π–π-stacking interactions between the five- and six-membered rings of the indazole units with a centroid–centroid distance of 3.6744 (19) Å and a dihedral angle of 1.63 (8)° (Fig. 2). The stacks are associated through C7—H7⋯O1, C8—H8B⋯O2 and C10—H10⋯O2 hydrogen bonds (Table 1 and Figs. 2 and 3).
Synthesis and crystallization
To a solution of 6-nitro-1H-indazole (1 g, 5 mmol) in tetrahydrofuran (30 ml) was added benzylchloride (0.8 g, 5 mmol), potassium carbonate (1.24 g, 9 mmol) and a catalytic quantity of tetra-n-butylammonium iodide. The mixture was stirred at room temperature for 48 h. The solution was filtered and the solvent removed under reduced pressure. The residue was recrystallized from ethanol solution to afford the title compound as colourless crystals (yield: 86%)
Refinement
Crystal data, data collection and structure . The crystal used contained a minor twin component (CELL_NOW; Sheldrick, 2008a), which was considered sufficiently small to be ignored in the final refinement.
details are summarized in Table 2Structural data
CCDC reference: 1818813
https://doi.org/10.1107/S2414314618001517/hb4206sup1.cif
contains datablocks global, I. DOI:Structure factors: contains datablock I. DOI: https://doi.org/10.1107/S2414314618001517/hb4206Isup2.hkl
Supporting information file. DOI: https://doi.org/10.1107/S2414314618001517/hb4206Isup3.cdx
Supporting information file. DOI: https://doi.org/10.1107/S2414314618001517/hb4206Isup4.cml
Data collection: APEX3 (Bruker, 2016); cell
SAINT (Bruker, 2016); data reduction: SAINT (Bruker, 2016); program(s) used to solve structure: SHELXT (Sheldrick, 2015a); program(s) used to refine structure: SHELXL2016 (Sheldrick, 2015b); molecular graphics: DIAMOND (Brandenburg & Putz, 2012); software used to prepare material for publication: SHELXTL (Sheldrick, 2008b).C14H11N3O2 | F(000) = 528 |
Mr = 253.26 | Dx = 1.427 Mg m−3 |
Monoclinic, P21/n | Mo Kα radiation, λ = 0.71073 Å |
a = 4.4890 (19) Å | Cell parameters from 9894 reflections |
b = 19.770 (8) Å | θ = 2.6–28.9° |
c = 13.308 (6) Å | µ = 0.10 mm−1 |
β = 93.608 (6)° | T = 100 K |
V = 1178.6 (9) Å3 | Column, colourless |
Z = 4 | 0.40 × 0.20 × 0.17 mm |
Bruker SMART APEX CCD diffractometer | 3223 independent reflections |
Radiation source: fine-focus sealed tube | 2210 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.056 |
Detector resolution: 8.3333 pixels mm-1 | θmax = 29.5°, θmin = 1.9° |
φ and ω scans | h = −6→6 |
Absorption correction: multi-scan (SADABS; Bruker, 2016) | k = 0→27 |
Tmin = 0.96, Tmax = 0.98 | l = −18→18 |
22904 measured reflections |
Refinement on F2 | Primary atom site location: structure-invariant direct methods |
Least-squares matrix: full | Secondary atom site location: difference Fourier map |
R[F2 > 2σ(F2)] = 0.059 | Hydrogen site location: inferred from neighbouring sites |
wR(F2) = 0.150 | H-atom parameters constrained |
S = 0.96 | w = 1/[σ2(Fo2) + (0.0959P)2] where P = (Fo2 + 2Fc2)/3 |
3223 reflections | (Δ/σ)max < 0.001 |
172 parameters | Δρmax = 0.54 e Å−3 |
0 restraints | Δρmin = −0.26 e Å−3 |
Experimental. The diffraction data were obtained from 3 sets of 400 frames, each of width 0.5° in ω, colllected at φ = 0.00, 90.00 and 180.00° and 2 sets of 800 frames, each of width 0.45° in φ, collected at ω = –30.00 and 210.00°. The scan time was 20 sec/frame. |
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. H-atoms attached to carbon were placed in calculated positions (C—H = 0.95 - 0.99 Å). All were included as riding contributions with isotropic displacement parameters 1.2 times those of the attached atoms. |
x | y | z | Uiso*/Ueq | ||
O1 | 1.1690 (3) | 0.27750 (6) | 0.70851 (9) | 0.0254 (3) | |
O2 | 1.1457 (3) | 0.17253 (6) | 0.66604 (9) | 0.0314 (3) | |
N1 | 0.1797 (3) | 0.36929 (6) | 0.39590 (9) | 0.0156 (3) | |
N2 | 0.3722 (3) | 0.38443 (6) | 0.47413 (9) | 0.0164 (3) | |
N3 | 1.0647 (3) | 0.23134 (6) | 0.65597 (10) | 0.0193 (3) | |
C1 | 0.5118 (3) | 0.32514 (7) | 0.49448 (11) | 0.0143 (3) | |
C2 | 0.7354 (3) | 0.31196 (7) | 0.57032 (11) | 0.0152 (3) | |
H2 | 0.813941 | 0.346431 | 0.614108 | 0.018* | |
C3 | 0.8331 (4) | 0.24708 (8) | 0.57749 (11) | 0.0163 (3) | |
C4 | 0.7253 (4) | 0.19377 (8) | 0.51450 (11) | 0.0189 (3) | |
H4 | 0.800949 | 0.149231 | 0.524440 | 0.023* | |
C5 | 0.5123 (4) | 0.20657 (8) | 0.43946 (11) | 0.0194 (3) | |
H5 | 0.440036 | 0.171504 | 0.395606 | 0.023* | |
C6 | 0.4017 (4) | 0.27289 (7) | 0.42839 (11) | 0.0153 (3) | |
C7 | 0.1870 (3) | 0.30481 (7) | 0.36564 (11) | 0.0171 (3) | |
H7 | 0.068645 | 0.284850 | 0.311847 | 0.020* | |
C8 | −0.0081 (3) | 0.42330 (8) | 0.35141 (11) | 0.0179 (3) | |
H8A | −0.088342 | 0.450603 | 0.405911 | 0.021* | |
H8B | −0.179168 | 0.402997 | 0.311612 | 0.021* | |
C9 | 0.1609 (3) | 0.46872 (7) | 0.28450 (11) | 0.0164 (3) | |
C10 | 0.1313 (4) | 0.46162 (8) | 0.18117 (12) | 0.0216 (4) | |
H10 | 0.006152 | 0.427191 | 0.151969 | 0.026* | |
C11 | 0.2830 (4) | 0.50439 (9) | 0.11997 (13) | 0.0275 (4) | |
H11 | 0.259724 | 0.499660 | 0.048866 | 0.033* | |
C12 | 0.4678 (4) | 0.55385 (8) | 0.16192 (13) | 0.0269 (4) | |
H12 | 0.572625 | 0.583060 | 0.119773 | 0.032* | |
C13 | 0.5007 (4) | 0.56093 (8) | 0.26501 (13) | 0.0247 (4) | |
H13 | 0.628790 | 0.594894 | 0.293986 | 0.030* | |
C14 | 0.3475 (4) | 0.51870 (7) | 0.32611 (12) | 0.0201 (3) | |
H14 | 0.369781 | 0.523851 | 0.397166 | 0.024* |
U11 | U22 | U33 | U12 | U13 | U23 | |
O1 | 0.0261 (7) | 0.0325 (7) | 0.0165 (6) | −0.0024 (5) | −0.0068 (5) | 0.0013 (5) |
O2 | 0.0377 (8) | 0.0312 (7) | 0.0244 (7) | 0.0144 (5) | −0.0048 (6) | 0.0036 (5) |
N1 | 0.0136 (7) | 0.0232 (7) | 0.0099 (6) | −0.0006 (5) | −0.0010 (5) | 0.0022 (5) |
N2 | 0.0166 (7) | 0.0223 (6) | 0.0099 (6) | 0.0001 (5) | −0.0024 (5) | −0.0003 (5) |
N3 | 0.0193 (8) | 0.0280 (7) | 0.0107 (6) | 0.0029 (5) | 0.0019 (5) | 0.0034 (5) |
C1 | 0.0155 (8) | 0.0184 (7) | 0.0091 (7) | −0.0018 (6) | 0.0014 (5) | 0.0005 (5) |
C2 | 0.0150 (8) | 0.0220 (7) | 0.0086 (7) | −0.0019 (6) | 0.0005 (5) | −0.0002 (5) |
C3 | 0.0153 (8) | 0.0257 (8) | 0.0079 (7) | 0.0010 (6) | 0.0017 (6) | 0.0026 (5) |
C4 | 0.0234 (9) | 0.0193 (7) | 0.0141 (7) | 0.0026 (6) | 0.0026 (6) | 0.0010 (5) |
C5 | 0.0232 (9) | 0.0216 (8) | 0.0135 (7) | −0.0023 (6) | 0.0023 (6) | −0.0035 (6) |
C6 | 0.0158 (8) | 0.0222 (8) | 0.0081 (7) | −0.0023 (6) | 0.0024 (5) | −0.0005 (5) |
C7 | 0.0168 (8) | 0.0220 (7) | 0.0124 (7) | −0.0034 (6) | 0.0011 (6) | −0.0010 (5) |
C8 | 0.0157 (8) | 0.0246 (8) | 0.0129 (7) | 0.0030 (6) | −0.0018 (6) | 0.0027 (5) |
C9 | 0.0154 (8) | 0.0191 (7) | 0.0146 (7) | 0.0049 (6) | −0.0006 (6) | 0.0007 (5) |
C10 | 0.0224 (9) | 0.0268 (8) | 0.0154 (8) | 0.0000 (6) | −0.0010 (6) | −0.0006 (6) |
C11 | 0.0294 (11) | 0.0384 (9) | 0.0148 (8) | 0.0023 (7) | 0.0029 (7) | 0.0054 (7) |
C12 | 0.0246 (10) | 0.0288 (9) | 0.0280 (10) | 0.0016 (7) | 0.0072 (7) | 0.0101 (7) |
C13 | 0.0240 (10) | 0.0188 (8) | 0.0312 (10) | 0.0001 (6) | −0.0004 (7) | 0.0008 (6) |
C14 | 0.0203 (9) | 0.0225 (8) | 0.0172 (8) | 0.0037 (6) | −0.0014 (6) | −0.0006 (6) |
O1—N3 | 1.2245 (17) | C6—C7 | 1.387 (2) |
O2—N3 | 1.2230 (17) | C7—H7 | 0.9500 |
N1—C7 | 1.3379 (19) | C8—C9 | 1.503 (2) |
N1—N2 | 1.3441 (17) | C8—H8A | 0.9900 |
N1—C8 | 1.4623 (19) | C8—H8B | 0.9900 |
N2—C1 | 1.3487 (19) | C9—C10 | 1.380 (2) |
N3—C3 | 1.460 (2) | C9—C14 | 1.388 (2) |
C1—C2 | 1.402 (2) | C10—C11 | 1.383 (2) |
C1—C6 | 1.425 (2) | C10—H10 | 0.9500 |
C2—C3 | 1.357 (2) | C11—C12 | 1.378 (3) |
C2—H2 | 0.9500 | C11—H11 | 0.9500 |
C3—C4 | 1.413 (2) | C12—C13 | 1.378 (2) |
C4—C5 | 1.362 (2) | C12—H12 | 0.9500 |
C4—H4 | 0.9500 | C13—C14 | 1.379 (2) |
C5—C6 | 1.406 (2) | C13—H13 | 0.9500 |
C5—H5 | 0.9500 | C14—H14 | 0.9500 |
C7—N1—N2 | 114.75 (12) | N1—C7—H7 | 126.8 |
C7—N1—C8 | 126.75 (13) | C6—C7—H7 | 126.8 |
N2—N1—C8 | 118.49 (12) | N1—C8—C9 | 112.12 (13) |
N1—N2—C1 | 103.29 (12) | N1—C8—H8A | 109.2 |
O2—N3—O1 | 123.07 (14) | C9—C8—H8A | 109.2 |
O2—N3—C3 | 118.31 (13) | N1—C8—H8B | 109.2 |
O1—N3—C3 | 118.61 (13) | C9—C8—H8B | 109.2 |
N2—C1—C2 | 127.49 (13) | H8A—C8—H8B | 107.9 |
N2—C1—C6 | 111.56 (14) | C10—C9—C14 | 119.19 (15) |
C2—C1—C6 | 120.95 (13) | C10—C9—C8 | 120.59 (14) |
C3—C2—C1 | 116.09 (13) | C14—C9—C8 | 120.22 (14) |
C3—C2—H2 | 122.0 | C9—C10—C11 | 120.31 (15) |
C1—C2—H2 | 122.0 | C9—C10—H10 | 119.8 |
C2—C3—C4 | 124.50 (14) | C11—C10—H10 | 119.8 |
C2—C3—N3 | 117.65 (13) | C12—C11—C10 | 120.11 (16) |
C4—C3—N3 | 117.85 (14) | C12—C11—H11 | 119.9 |
C5—C4—C3 | 119.65 (14) | C10—C11—H11 | 119.9 |
C5—C4—H4 | 120.2 | C13—C12—C11 | 119.97 (16) |
C3—C4—H4 | 120.2 | C13—C12—H12 | 120.0 |
C4—C5—C6 | 118.48 (14) | C11—C12—H12 | 120.0 |
C4—C5—H5 | 120.8 | C12—C13—C14 | 119.98 (16) |
C6—C5—H5 | 120.8 | C12—C13—H13 | 120.0 |
C7—C6—C5 | 135.61 (14) | C14—C13—H13 | 120.0 |
C7—C6—C1 | 104.05 (13) | C13—C14—C9 | 120.44 (15) |
C5—C6—C1 | 120.32 (14) | C13—C14—H14 | 119.8 |
N1—C7—C6 | 106.36 (13) | C9—C14—H14 | 119.8 |
C7—N1—N2—C1 | 0.19 (16) | N2—C1—C6—C5 | −177.95 (14) |
C8—N1—N2—C1 | −178.47 (12) | C2—C1—C6—C5 | 1.2 (2) |
N1—N2—C1—C2 | −179.58 (14) | N2—N1—C7—C6 | 0.16 (17) |
N1—N2—C1—C6 | −0.48 (16) | C8—N1—C7—C6 | 178.70 (14) |
N2—C1—C2—C3 | 177.76 (15) | C5—C6—C7—N1 | 177.76 (17) |
C6—C1—C2—C3 | −1.3 (2) | C1—C6—C7—N1 | −0.43 (16) |
C1—C2—C3—C4 | 0.1 (2) | C7—N1—C8—C9 | −101.09 (17) |
C1—C2—C3—N3 | −179.67 (13) | N2—N1—C8—C9 | 77.40 (16) |
O2—N3—C3—C2 | 176.93 (14) | N1—C8—C9—C10 | 101.16 (16) |
O1—N3—C3—C2 | −3.1 (2) | N1—C8—C9—C14 | −79.25 (17) |
O2—N3—C3—C4 | −2.9 (2) | C14—C9—C10—C11 | −0.8 (2) |
O1—N3—C3—C4 | 177.09 (14) | C8—C9—C10—C11 | 178.78 (15) |
C2—C3—C4—C5 | 1.2 (2) | C9—C10—C11—C12 | 0.8 (3) |
N3—C3—C4—C5 | −179.05 (14) | C10—C11—C12—C13 | −0.3 (3) |
C3—C4—C5—C6 | −1.2 (2) | C11—C12—C13—C14 | −0.3 (3) |
C4—C5—C6—C7 | −177.89 (17) | C12—C13—C14—C9 | 0.3 (2) |
C4—C5—C6—C1 | 0.1 (2) | C10—C9—C14—C13 | 0.2 (2) |
N2—C1—C6—C7 | 0.58 (17) | C8—C9—C14—C13 | −179.36 (14) |
C2—C1—C6—C7 | 179.75 (14) |
D—H···A | D—H | H···A | D···A | D—H···A |
C7—H7···O1i | 0.95 | 2.51 | 3.437 (2) | 164 |
C8—H8B···O2i | 0.99 | 2.53 | 3.407 (2) | 147 |
C10—H10···O2i | 0.95 | 2.56 | 3.431 (3) | 152 |
Symmetry code: (i) x−3/2, −y+1/2, z−1/2. |
Acknowledgements
JTM thanks Tulane University for support of the Tulane Crystallography Laboratory.
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