organic compounds
5-Fluoro-1H-indole-2-carbohydrazide
aDepartment of Chemistry, University of Aberdeen, Meston Walk, Aberdeen AB24 3UE, Scotland, bDepartment of Studies in Chemistry, University of Mysore, Manasagangotri, Mysore 570 006, India, and cDepartment of Chemistry, Mangalore University, Mangalagangotri 574 199, India
*Correspondence e-mail: w.harrison@abdn.ac.uk
The geometric parameters for the essentially planar molecule of the title compound, C9H8FN3O, are normal. A network of N—H⋯O and N—H⋯N hydrogen bonds helps to establish the crystal packing.
Comment
As part of our ongoing research into indole carboxylic acid derivatives (Harrison et al., 2006), the synthesis and of the title compound, (I) (Fig. 1), are now presented.
The geometric paramaters for (I) fall within their expected ranges (Allen et al., 1987). The indole ring system is essentially flat (r.m.s. deviation from the mean plane = 0.005 Å). The mean plane of atoms C9, O1, N2 and N3 of the carbohydrazide side chain is slightly twisted away from the indole mean plane [dihedral angle = 5.27 (9)°]. The bond angle sum about N2 is 359°, suggesting sp2-hybridization for this atom. Conversely, the average bond angle for N3 of 108° suggests sp3-hybridization.
The crystal packing in (I) is influenced by N—H⋯O and N—H⋯N hydrogen bonds (Table 1). Inversion-generated dimeric pairs of molecules are linked by a pair of N3—H3⋯O1iii hydrogen bonds (Fig. 2). Adjacent molecules are then linked into ribbons by a combination of the N2—H2⋯O1ii and N1⋯H1—N3i bonds. In terms of graph theory (Bernstein et al., 1995) these two hydrogen-bonding motifs result in R22(10) and R22(8) loops, respectively. Combining the two results in (001) sheets of molecules. Atom H4, attached to N3, does not participate in hydrogen bonds. A PLATON (Spek, 2003) analysis of (I) indicated a short C—H⋯F contact that may also help to consolidate the crystal packing. In the packing of (I), a zigzag stacking of molecules with respect to the c direction is seen (Fig. 3). Any π–π stacking interactions in (I) must be very weak, the shortest intermolecular ring-centroid separation being 4.08 Å.
Experimental
Methyl-5-fluoroindole-2-carboxylate (2.34 g, 0.01 mol) (Harrison et al., 2006) in 25 ml of absolute ethanol was refluxed with 1.0 ml of hydrazine hydrate for 2 h, with the reaction progress monitored by Upon completion, the mixture was cooled to room temperature. The separated solid was filtered off and washed with cold ethanol; cubes of (I) were recrystallized from ethanol (m.p. 505–507 K). Analysis found (calculated) for C9H8FN3O: C 55.70 (55.96), H 4.12 (4.17), N 21.65 (21.75)%.
Crystal data
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Refinement
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The N-bound H atoms were located in difference maps and their positions were freely refined with Uiso(H) set equal to 1.2Ueq(N). The C-bound H atoms were placed in idealized locations (C—H = 0.95 Å) and refined as riding with Uiso(H) = 1.2Ueq(C).
Data collection: COLLECT (Nonius, 1998); cell HKL SCALEPACK (Otwinowski & Minor 1997); data reduction: HKL DENZO and SCALEPACK (Otwinowski & Minor 1997), and SORTAV (Blessing, 1995); program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: ORTEP-3 (Farrugia, 1997); software used to prepare material for publication: SHELXL97.
Supporting information
https://doi.org/10.1107/S1600536806040943/bt2203sup1.cif
contains datablocks I, global. DOI:Structure factors: contains datablock I. DOI: https://doi.org/10.1107/S1600536806040943/bt2203Isup2.hkl
Data collection: Collect (Nonius, 1998); cell
HKL SCALEPACK (Otwinowski & Minor 1997); data reduction: HKL DENZO and SCALEPACK (Otwinowski & Minor 1997), and SORTAV (Blessing, 1995); program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: ORTEP-3 (Farrugia, 1997); software used to prepare material for publication: SHELXL97.C9H8FN3O | F(000) = 800 |
Mr = 193.18 | Dx = 1.452 Mg m−3 |
Orthorhombic, Pbca | Mo Kα radiation, λ = 0.71073 Å |
Hall symbol: -P 2ac 2ab | Cell parameters from 1996 reflections |
a = 10.0451 (3) Å | θ = 1.0–26.0° |
b = 9.4978 (2) Å | µ = 0.11 mm−1 |
c = 18.5293 (6) Å | T = 120 K |
V = 1767.81 (9) Å3 | Cube, colourless |
Z = 8 | 0.20 × 0.20 × 0.20 mm |
Nonius KappaCCD diffractometer | 1733 independent reflections |
Radiation source: fine-focus sealed tube | 1497 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.029 |
φ and ω scans | θmax = 26.1°, θmin = 3.7° |
Absorption correction: multi-scan (SADABS; Bruker, 2003) | h = −12→12 |
Tmin = 0.978, Tmax = 0.978 | k = −11→10 |
11208 measured reflections | l = −22→18 |
Refinement on F2 | Secondary atom site location: difference Fourier map |
Least-squares matrix: full | Hydrogen site location: difmap (N-H) and geom (others) |
R[F2 > 2σ(F2)] = 0.032 | H atoms treated by a mixture of independent and constrained refinement |
wR(F2) = 0.089 | w = 1/[σ2(Fo2) + (0.0434P)2 + 0.7328P] where P = (Fo2 + 2Fc2)/3 |
S = 1.06 | (Δ/σ)max = 0.001 |
1733 reflections | Δρmax = 0.25 e Å−3 |
140 parameters | Δρmin = −0.19 e Å−3 |
0 restraints | Extinction correction: SHELXL97, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4 |
Primary atom site location: structure-invariant direct methods | Extinction coefficient: 0.015 (2) |
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. |
x | y | z | Uiso*/Ueq | ||
C1 | 0.48589 (12) | 0.44387 (13) | 0.63425 (6) | 0.0181 (3) | |
C2 | 0.41098 (13) | 0.34193 (14) | 0.67046 (7) | 0.0217 (3) | |
H2A | 0.3166 | 0.3410 | 0.6676 | 0.026* | |
C3 | 0.47908 (13) | 0.24262 (14) | 0.71057 (7) | 0.0228 (3) | |
H3A | 0.4319 | 0.1713 | 0.7358 | 0.027* | |
C4 | 0.61805 (13) | 0.24800 (13) | 0.71369 (7) | 0.0216 (3) | |
C5 | 0.69439 (13) | 0.34626 (13) | 0.67917 (7) | 0.0211 (3) | |
H5 | 0.7887 | 0.3462 | 0.6829 | 0.025* | |
C6 | 0.62640 (12) | 0.44730 (13) | 0.63784 (6) | 0.0179 (3) | |
C7 | 0.66864 (12) | 0.56243 (13) | 0.59462 (7) | 0.0192 (3) | |
H7 | 0.7578 | 0.5914 | 0.5863 | 0.023* | |
C8 | 0.55545 (12) | 0.62391 (13) | 0.56713 (7) | 0.0179 (3) | |
C9 | 0.54006 (11) | 0.74680 (14) | 0.51939 (7) | 0.0175 (3) | |
N1 | 0.44498 (10) | 0.55295 (11) | 0.59124 (6) | 0.0186 (3) | |
H1 | 0.3600 (16) | 0.5719 (15) | 0.5798 (8) | 0.022* | |
N2 | 0.65387 (10) | 0.80349 (11) | 0.49559 (6) | 0.0208 (3) | |
H2 | 0.7311 (16) | 0.7653 (16) | 0.5037 (8) | 0.025* | |
N3 | 0.65712 (11) | 0.91675 (12) | 0.44592 (6) | 0.0209 (3) | |
H3 | 0.6249 (15) | 0.9963 (17) | 0.4682 (8) | 0.025* | |
H4 | 0.6008 (16) | 0.8927 (16) | 0.4082 (9) | 0.025* | |
O1 | 0.42915 (8) | 0.79502 (10) | 0.50288 (5) | 0.0217 (2) | |
F1 | 0.67988 (8) | 0.14679 (8) | 0.75401 (4) | 0.0297 (2) |
U11 | U22 | U33 | U12 | U13 | U23 | |
C1 | 0.0176 (6) | 0.0185 (6) | 0.0182 (6) | 0.0013 (5) | 0.0000 (5) | −0.0022 (5) |
C2 | 0.0170 (6) | 0.0236 (7) | 0.0244 (7) | −0.0007 (5) | 0.0022 (5) | −0.0002 (5) |
C3 | 0.0228 (7) | 0.0216 (7) | 0.0240 (7) | −0.0022 (5) | 0.0043 (5) | 0.0014 (5) |
C4 | 0.0234 (7) | 0.0199 (6) | 0.0216 (6) | 0.0042 (5) | −0.0017 (5) | 0.0022 (5) |
C5 | 0.0168 (6) | 0.0237 (7) | 0.0229 (6) | 0.0013 (5) | −0.0006 (5) | −0.0007 (5) |
C6 | 0.0172 (6) | 0.0182 (6) | 0.0185 (6) | 0.0007 (5) | 0.0000 (5) | −0.0029 (5) |
C7 | 0.0154 (6) | 0.0205 (6) | 0.0216 (6) | −0.0009 (5) | 0.0004 (5) | −0.0014 (5) |
C8 | 0.0161 (6) | 0.0181 (6) | 0.0196 (6) | −0.0007 (5) | 0.0008 (5) | −0.0024 (5) |
C9 | 0.0154 (6) | 0.0171 (6) | 0.0200 (6) | 0.0000 (5) | −0.0007 (5) | −0.0035 (5) |
N1 | 0.0139 (5) | 0.0197 (6) | 0.0223 (6) | 0.0003 (4) | 0.0001 (4) | 0.0013 (4) |
N2 | 0.0139 (5) | 0.0206 (6) | 0.0280 (6) | 0.0011 (4) | −0.0002 (4) | 0.0060 (5) |
N3 | 0.0191 (6) | 0.0178 (6) | 0.0258 (6) | −0.0006 (4) | −0.0007 (4) | 0.0039 (5) |
O1 | 0.0140 (4) | 0.0213 (5) | 0.0297 (5) | 0.0008 (3) | −0.0009 (4) | 0.0023 (4) |
F1 | 0.0259 (4) | 0.0281 (5) | 0.0352 (5) | 0.0030 (3) | −0.0019 (3) | 0.0124 (4) |
C1—N1 | 1.3702 (17) | C7—C8 | 1.3759 (17) |
C1—C2 | 1.3978 (18) | C7—H7 | 0.9500 |
C1—C6 | 1.4133 (18) | C8—N1 | 1.3730 (16) |
C2—C3 | 1.3820 (19) | C8—C9 | 1.4727 (18) |
C2—H2A | 0.9500 | C9—O1 | 1.2428 (14) |
C3—C4 | 1.3981 (19) | C9—N2 | 1.3384 (16) |
C3—H3A | 0.9500 | N1—H1 | 0.898 (16) |
C4—F1 | 1.3667 (14) | N2—N3 | 1.4161 (15) |
C4—C5 | 1.3667 (18) | N2—H2 | 0.870 (16) |
C5—C6 | 1.4050 (17) | N3—H3 | 0.920 (16) |
C5—H5 | 0.9500 | N3—H4 | 0.927 (17) |
C6—C7 | 1.4203 (17) | ||
N1—C1—C2 | 129.90 (12) | C8—C7—C6 | 106.77 (11) |
N1—C1—C6 | 108.02 (11) | C8—C7—H7 | 126.6 |
C2—C1—C6 | 122.08 (11) | C6—C7—H7 | 126.6 |
C3—C2—C1 | 117.67 (12) | N1—C8—C7 | 109.83 (11) |
C3—C2—H2A | 121.2 | N1—C8—C9 | 119.98 (11) |
C1—C2—H2A | 121.2 | C7—C8—C9 | 130.19 (11) |
C2—C3—C4 | 119.44 (12) | O1—C9—N2 | 122.44 (12) |
C2—C3—H3A | 120.3 | O1—C9—C8 | 122.27 (11) |
C4—C3—H3A | 120.3 | N2—C9—C8 | 115.28 (10) |
F1—C4—C5 | 118.76 (11) | C1—N1—C8 | 108.54 (10) |
F1—C4—C3 | 116.78 (11) | C1—N1—H1 | 125.0 (9) |
C5—C4—C3 | 124.46 (12) | C8—N1—H1 | 126.4 (9) |
C4—C5—C6 | 116.66 (12) | C9—N2—N3 | 122.64 (10) |
C4—C5—H5 | 121.7 | C9—N2—H2 | 122.5 (10) |
C6—C5—H5 | 121.7 | N3—N2—H2 | 114.1 (10) |
C5—C6—C1 | 119.69 (11) | N2—N3—H3 | 108.9 (9) |
C5—C6—C7 | 133.47 (12) | N2—N3—H4 | 106.8 (10) |
C1—C6—C7 | 106.84 (11) | H3—N3—H4 | 109.0 (14) |
N1—C1—C2—C3 | 179.90 (12) | C1—C6—C7—C8 | 0.22 (13) |
C6—C1—C2—C3 | −0.06 (18) | C6—C7—C8—N1 | 0.14 (14) |
C1—C2—C3—C4 | 0.29 (19) | C6—C7—C8—C9 | 179.73 (12) |
C2—C3—C4—F1 | −179.81 (11) | N1—C8—C9—O1 | 4.26 (19) |
C2—C3—C4—C5 | −0.1 (2) | C7—C8—C9—O1 | −175.31 (13) |
F1—C4—C5—C6 | 179.40 (11) | N1—C8—C9—N2 | −176.29 (11) |
C3—C4—C5—C6 | −0.27 (19) | C7—C8—C9—N2 | 4.1 (2) |
C4—C5—C6—C1 | 0.49 (17) | C2—C1—N1—C8 | −179.38 (12) |
C4—C5—C6—C7 | −179.26 (13) | C6—C1—N1—C8 | 0.58 (14) |
N1—C1—C6—C5 | 179.69 (11) | C7—C8—N1—C1 | −0.45 (15) |
C2—C1—C6—C5 | −0.35 (18) | C9—C8—N1—C1 | 179.90 (11) |
N1—C1—C6—C7 | −0.49 (13) | O1—C9—N2—N3 | −4.4 (2) |
C2—C1—C6—C7 | 179.47 (11) | C8—C9—N2—N3 | 176.16 (11) |
C5—C6—C7—C8 | 180.00 (13) |
D—H···A | D—H | H···A | D···A | D—H···A |
N1—H1···N3i | 0.898 (16) | 2.096 (16) | 2.9864 (15) | 171.3 (13) |
N2—H2···O1ii | 0.870 (16) | 2.073 (16) | 2.9193 (14) | 163.9 (14) |
N3—H3···O1iii | 0.920 (16) | 2.124 (16) | 3.0241 (15) | 165.8 (13) |
C3—H3A···F1iv | 0.95 | 2.55 | 3.2082 (15) | 127 |
Symmetry codes: (i) x−1/2, −y+3/2, −z+1; (ii) x+1/2, −y+3/2, −z+1; (iii) −x+1, −y+2, −z+1; (iv) x−1/2, y, −z+3/2. |
Acknowledgements
The authors thank the EPSRC National Crystallographic Service (University of Southampton) for data collection. ABV thanks Mangalore University for provision of research facilities.
References
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