Abstract
Crystals of the title compound, C15H12N4O·H2O, were obtained from a condensation reaction of isonicotinylhydrazine and 3-indolylformaldehyde. The molecule assumes an E configuration, with the isonicotinoylhydrazine and indole units located on the opposite sites of the C=N double bond. In the molecular structure the pyridine ring is twisted with respect to the indole ring system, forming a dihedral angle of 44.72 (7)°. Extensive classical N—H⋯N, N—H⋯O, O—H⋯O and O—H⋯N hydrogen bonding and weak C—H⋯O interactions are present in the crystal structure.
Related literature
For the applications of hydrazone derivatives in biology, see: Okabe et al. (1993 ▶). For general background to this work, see: Shan et al. (2003 ▶); Qiang et al. (2007 ▶). For the corresponding (E)-3-indolylformaldehyde isonicotinoylhydrazone methanol solvate, see: Tai et al. (2003 ▶), and (E)-3-indolylformaldehyde isonicotinoylhydrazone ethanol solvate, see: Jing et al. (2006 ▶).
Experimental
Crystal data
C15H12N4O·H2O
M r = 282.30
Monoclinic,
a = 7.1984 (11) Å
b = 25.327 (4) Å
c = 7.9811 (16) Å
β = 104.062 (12)°
V = 1411.5 (4) Å3
Z = 4
Mo Kα radiation
μ = 0.09 mm−1
T = 294 K
0.40 × 0.32 × 0.28 mm
Data collection
Rigaku R-AXIS RAPID IP diffractometer
Absorption correction: none
9235 measured reflections
2504 independent reflections
1575 reflections with I > 2σ(I)
R int = 0.048
Refinement
R[F 2 > 2σ(F 2)] = 0.055
wR(F 2) = 0.161
S = 1.07
2504 reflections
191 parameters
H-atom parameters constrained
Δρmax = 0.18 e Å−3
Δρmin = −0.20 e Å−3
Data collection: PROCESS-AUTO (Rigaku, 1998 ▶); cell refinement: PROCESS-AUTO; data reduction: CrystalStructure (Rigaku/MSC, 2002 ▶); program(s) used to solve structure: SIR92 (Altomare et al., 1993 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: ORTEP-3 for Windows (Farrugia, 1997 ▶); software used to prepare material for publication: WinGX (Farrugia, 1999 ▶).
Supplementary Material
Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536809027329/xu2554sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536809027329/xu2554Isup2.hkl
Table 1. Hydrogen-bond geometry (Å, °).
D—H⋯A | D—H | H⋯A | D⋯A | D—H⋯A |
---|---|---|---|---|
N1—H1N⋯N4i | 0.91 | 2.06 | 2.961 (3) | 171 |
N3—H3N⋯O1Wii | 0.89 | 2.11 | 2.939 (3) | 155 |
O1W—H1A⋯O1iii | 0.91 | 1.90 | 2.800 (3) | 168 |
O1W—H2A⋯N2 | 0.89 | 2.40 | 3.223 (3) | 152 |
C12—H12⋯O1Wii | 0.93 | 2.58 | 3.466 (3) | 159 |
Symmetry codes: (i) ; (ii) ; (iii) .
Acknowledgments
The work was supported by the Natural Science Foundation of Zhejiang Province, China (No. M203027).
supplementary crystallographic information
Comment
The hydrazone derivatives has attracted our much attention because they have shown to be potential DNA damaging and mutagenic agents (Okabe et al., 1993). As part of the ongoing investigation on the relationship between structure and property of hydrazone derivatives (Shan et al., 2003; Qiang et al., 2007) the title compound has recently been prepared in our laboratory and its crystal structure is reported here.
The molecular structure of the title compound is shown in Fig. 1. The pyridine ring is twisted with respect to the indole ring system by a dihedral angle of 44.72 (7)°. The N2—C9 bond distance of 1.293 (3) Å shows a typical C═N double bond. The isonicotinoylhydrazine and indole moieties are located on the opposite sites of the CN bond, thus the molecule assumes an E configuration, which agrees with those found in ethanol solvate compound (Jing et al., 2006) and methanol solvate compound (Tai et al., 2003).
The extensive classic hydrogen bonding and weak C—H···O hydrogen bonding are present in the crystal structure (Table 1).
Experimental
Isonicotinylhydrazine (1.37 g, 0.01 mol) was dissolved in ethanol (50 ml), the solution was heated at about 333 K for several minutes until the solution cleared. An ethanol solution (20 ml) containing 3-indolylformaldehyde (1.45 g, 0.01 mol) was dropped slowly into the above solution with continuous stirring, and the mixture solution was refluxed for 1.5 h. When the solution had cooled to room temperature, colorless powder crystals appeared. The powder crystals were separated from the solution and washed with cold water three times. Recrystallization was performed twice with a mixture solvent of 2-propanol-water (1:1 v/v), to obtain single crystals of the title compound.
Refinement
Water and imino H atoms were located in a difference Fourier map and were refined as riding in as-found relative positions, Uiso(H) = 1.5Ueq(N,O). Methyl H atoms were placed in calculated positions with C—H = 0.96 Å and torsion angle was refined to fit the electron density, Uiso(H) = 1.5Ueq(C). Other H atoms were placed in calculated positions with C—H = 0.93 Å, and refined in riding mode with Uiso(H) = 1.2Ueq(C).
Figures
Crystal data
C15H12N4O·H2O | F(000) = 592 |
Mr = 282.30 | Dx = 1.328 Mg m−3 |
Monoclinic, P21/c | Mo Kα radiation, λ = 0.71073 Å |
Hall symbol: -P 2ybc | Cell parameters from 3236 reflections |
a = 7.1984 (11) Å | θ = 2.8–25.0° |
b = 25.327 (4) Å | µ = 0.09 mm−1 |
c = 7.9811 (16) Å | T = 294 K |
β = 104.062 (12)° | Prism, colorless |
V = 1411.5 (4) Å3 | 0.40 × 0.32 × 0.28 mm |
Z = 4 |
Data collection
Rigaku R-AXIS RAPID IP diffractometer | 1575 reflections with I > 2σ(I) |
Radiation source: fine-focus sealed tube | Rint = 0.048 |
graphite | θmax = 25.2°, θmin = 2.8° |
Detector resolution: 10.0 pixels mm-1 | h = −8→8 |
ω scans | k = −30→28 |
9235 measured reflections | l = −9→9 |
2504 independent reflections |
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)] = 0.055 | H-atom parameters constrained |
wR(F2) = 0.161 | w = 1/[σ2(Fo2) + (0.0753P)2] where P = (Fo2 + 2Fc2)/3 |
S = 1.07 | (Δ/σ)max < 0.001 |
2504 reflections | Δρmax = 0.18 e Å−3 |
191 parameters | Δρmin = −0.20 e Å−3 |
0 restraints | Extinction correction: SHELXL97 (Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4 |
Primary atom site location: structure-invariant direct methods | Extinction coefficient: 0.022 (4) |
Special details
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)
x | y | z | Uiso*/Ueq | ||
N1 | 0.0721 (3) | 0.27145 (8) | 0.4661 (3) | 0.0532 (6) | |
H1N | 0.0189 | 0.2388 | 0.4518 | 0.080* | |
N2 | 0.2051 (3) | 0.44265 (8) | 0.6709 (3) | 0.0557 (6) | |
N3 | 0.1479 (3) | 0.48641 (8) | 0.7552 (3) | 0.0567 (6) | |
H3N | 0.0249 | 0.4904 | 0.7553 | 0.085* | |
N4 | 0.0958 (3) | 0.66448 (8) | 1.0414 (3) | 0.0585 (6) | |
O1 | 0.4458 (3) | 0.52331 (7) | 0.8055 (3) | 0.0778 (7) | |
O1W | 0.2725 (3) | 0.51295 (8) | 0.3543 (3) | 0.0717 (6) | |
H1A | 0.3680 | 0.5059 | 0.3000 | 0.108* | |
H2A | 0.2989 | 0.4927 | 0.4490 | 0.108* | |
C1 | 0.0052 (4) | 0.31058 (10) | 0.5519 (3) | 0.0524 (7) | |
H1 | −0.1042 | 0.3081 | 0.5940 | 0.063* | |
C2 | 0.1222 (4) | 0.35481 (10) | 0.5685 (3) | 0.0485 (7) | |
C3 | 0.4346 (4) | 0.36807 (10) | 0.4582 (3) | 0.0520 (7) | |
H3 | 0.4625 | 0.4023 | 0.4989 | 0.062* | |
C4 | 0.5486 (4) | 0.34271 (11) | 0.3671 (4) | 0.0603 (8) | |
H4 | 0.6518 | 0.3606 | 0.3429 | 0.072* | |
C5 | 0.5118 (4) | 0.29032 (12) | 0.3099 (4) | 0.0630 (8) | |
H5 | 0.5931 | 0.2741 | 0.2511 | 0.076* | |
C6 | 0.3582 (4) | 0.26257 (10) | 0.3389 (3) | 0.0546 (7) | |
H6 | 0.3348 | 0.2278 | 0.3019 | 0.066* | |
C7 | 0.2390 (4) | 0.28874 (9) | 0.4262 (3) | 0.0469 (6) | |
C8 | 0.2756 (3) | 0.34103 (9) | 0.4881 (3) | 0.0444 (6) | |
C9 | 0.0874 (4) | 0.40330 (10) | 0.6509 (3) | 0.0511 (7) | |
H9 | −0.0232 | 0.4063 | 0.6909 | 0.061* | |
C10 | 0.2762 (4) | 0.52496 (10) | 0.8150 (4) | 0.0539 (7) | |
C11 | 0.2053 (4) | 0.57134 (9) | 0.8990 (3) | 0.0483 (7) | |
C12 | 0.0156 (4) | 0.58804 (10) | 0.8584 (3) | 0.0587 (8) | |
H12 | −0.0785 | 0.5685 | 0.7835 | 0.070* | |
C13 | −0.0314 (4) | 0.63452 (10) | 0.9316 (4) | 0.0611 (8) | |
H13 | −0.1585 | 0.6454 | 0.9026 | 0.073* | |
C14 | 0.2765 (4) | 0.64680 (11) | 1.0837 (4) | 0.0629 (8) | |
H14 | 0.3666 | 0.6662 | 1.1632 | 0.076* | |
C15 | 0.3374 (4) | 0.60145 (10) | 1.0164 (4) | 0.0590 (8) | |
H15 | 0.4652 | 0.5913 | 1.0493 | 0.071* |
Atomic displacement parameters (Å2)
U11 | U22 | U33 | U12 | U13 | U23 | |
N1 | 0.0506 (13) | 0.0365 (12) | 0.0698 (15) | −0.0060 (10) | 0.0094 (11) | −0.0002 (11) |
N2 | 0.0574 (14) | 0.0399 (13) | 0.0711 (15) | 0.0061 (11) | 0.0184 (12) | −0.0088 (11) |
N3 | 0.0554 (13) | 0.0399 (13) | 0.0771 (16) | 0.0050 (11) | 0.0207 (12) | −0.0113 (11) |
N4 | 0.0716 (16) | 0.0416 (13) | 0.0618 (14) | 0.0087 (12) | 0.0153 (12) | −0.0015 (11) |
O1 | 0.0638 (14) | 0.0592 (13) | 0.1204 (18) | −0.0004 (11) | 0.0418 (13) | −0.0204 (12) |
O1W | 0.0577 (12) | 0.0756 (14) | 0.0845 (14) | 0.0109 (10) | 0.0221 (11) | −0.0006 (11) |
C1 | 0.0469 (15) | 0.0442 (15) | 0.0663 (17) | 0.0017 (13) | 0.0139 (13) | 0.0062 (13) |
C2 | 0.0488 (15) | 0.0374 (14) | 0.0575 (16) | 0.0058 (12) | 0.0093 (13) | 0.0040 (12) |
C3 | 0.0542 (16) | 0.0382 (14) | 0.0616 (17) | −0.0011 (13) | 0.0099 (14) | 0.0032 (12) |
C4 | 0.0524 (16) | 0.0555 (18) | 0.0711 (19) | 0.0016 (14) | 0.0111 (15) | 0.0059 (15) |
C5 | 0.0606 (18) | 0.0628 (18) | 0.0662 (19) | 0.0130 (16) | 0.0165 (15) | −0.0018 (15) |
C6 | 0.0597 (17) | 0.0408 (15) | 0.0580 (17) | 0.0048 (13) | 0.0039 (14) | −0.0042 (12) |
C7 | 0.0464 (15) | 0.0369 (14) | 0.0524 (15) | 0.0020 (12) | 0.0021 (12) | −0.0006 (12) |
C8 | 0.0454 (14) | 0.0339 (14) | 0.0491 (14) | 0.0025 (12) | 0.0021 (12) | 0.0007 (11) |
C9 | 0.0558 (16) | 0.0411 (15) | 0.0587 (16) | 0.0054 (13) | 0.0185 (13) | 0.0041 (12) |
C10 | 0.0569 (18) | 0.0396 (15) | 0.0677 (18) | 0.0069 (13) | 0.0203 (14) | 0.0001 (13) |
C11 | 0.0552 (16) | 0.0371 (14) | 0.0564 (16) | 0.0041 (12) | 0.0206 (13) | 0.0036 (12) |
C12 | 0.0615 (18) | 0.0461 (15) | 0.0633 (17) | 0.0100 (14) | 0.0048 (14) | −0.0080 (13) |
C13 | 0.0632 (18) | 0.0543 (17) | 0.0625 (18) | 0.0154 (15) | 0.0088 (15) | −0.0032 (14) |
C14 | 0.0634 (19) | 0.0478 (17) | 0.076 (2) | −0.0035 (15) | 0.0131 (16) | −0.0070 (14) |
C15 | 0.0500 (16) | 0.0466 (16) | 0.081 (2) | 0.0017 (13) | 0.0165 (15) | −0.0072 (14) |
Geometric parameters (Å, °)
N1—C1 | 1.358 (3) | C3—H3 | 0.9300 |
N1—C7 | 1.387 (3) | C4—C5 | 1.407 (4) |
N1—H1N | 0.9057 | C4—H4 | 0.9300 |
N2—C9 | 1.293 (3) | C5—C6 | 1.376 (4) |
N2—N3 | 1.409 (3) | C5—H5 | 0.9300 |
N3—C10 | 1.349 (3) | C6—C7 | 1.397 (3) |
N3—H3N | 0.8916 | C6—H6 | 0.9300 |
N4—C13 | 1.338 (3) | C7—C8 | 1.416 (3) |
N4—C14 | 1.339 (3) | C9—H9 | 0.9300 |
O1—C10 | 1.242 (3) | C10—C11 | 1.502 (3) |
O1W—H1A | 0.9147 | C11—C15 | 1.389 (3) |
O1W—H2A | 0.8945 | C11—C12 | 1.391 (4) |
C1—C2 | 1.388 (3) | C12—C13 | 1.392 (3) |
C1—H1 | 0.9300 | C12—H12 | 0.9300 |
C2—C9 | 1.444 (3) | C13—H13 | 0.9300 |
C2—C8 | 1.449 (3) | C14—C15 | 1.384 (4) |
C3—C4 | 1.380 (4) | C14—H14 | 0.9300 |
C3—C8 | 1.403 (3) | C15—H15 | 0.9300 |
C1—N1—C7 | 108.6 (2) | N1—C7—C6 | 129.5 (2) |
C1—N1—H1N | 122.6 | N1—C7—C8 | 108.3 (2) |
C7—N1—H1N | 128.5 | C6—C7—C8 | 122.2 (2) |
C9—N2—N3 | 114.0 (2) | C3—C8—C7 | 119.2 (2) |
C10—N3—N2 | 118.9 (2) | C3—C8—C2 | 134.4 (2) |
C10—N3—H3N | 120.8 | C7—C8—C2 | 106.4 (2) |
N2—N3—H3N | 119.7 | N2—C9—C2 | 122.1 (2) |
C13—N4—C14 | 116.3 (2) | N2—C9—H9 | 119.0 |
H1A—O1W—H2A | 105.0 | C2—C9—H9 | 119.0 |
N1—C1—C2 | 110.9 (2) | O1—C10—N3 | 123.6 (2) |
N1—C1—H1 | 124.6 | O1—C10—C11 | 119.9 (2) |
C2—C1—H1 | 124.6 | N3—C10—C11 | 116.5 (2) |
C1—C2—C9 | 124.2 (2) | C15—C11—C12 | 117.6 (2) |
C1—C2—C8 | 105.9 (2) | C15—C11—C10 | 118.6 (2) |
C9—C2—C8 | 130.0 (2) | C12—C11—C10 | 123.7 (2) |
C4—C3—C8 | 118.4 (2) | C11—C12—C13 | 119.0 (3) |
C4—C3—H3 | 120.8 | C11—C12—H12 | 120.5 |
C8—C3—H3 | 120.8 | C13—C12—H12 | 120.5 |
C3—C4—C5 | 121.4 (3) | N4—C13—C12 | 123.9 (3) |
C3—C4—H4 | 119.3 | N4—C13—H13 | 118.1 |
C5—C4—H4 | 119.3 | C12—C13—H13 | 118.1 |
C6—C5—C4 | 121.5 (3) | N4—C14—C15 | 124.0 (3) |
C6—C5—H5 | 119.3 | N4—C14—H14 | 118.0 |
C4—C5—H5 | 119.3 | C15—C14—H14 | 118.0 |
C5—C6—C7 | 117.2 (2) | C14—C15—C11 | 119.2 (3) |
C5—C6—H6 | 121.4 | C14—C15—H15 | 120.4 |
C7—C6—H6 | 121.4 | C11—C15—H15 | 120.4 |
Hydrogen-bond geometry (Å, °)
D—H···A | D—H | H···A | D···A | D—H···A |
N1—H1N···N4i | 0.91 | 2.06 | 2.961 (3) | 171 |
N3—H3N···O1Wii | 0.89 | 2.11 | 2.939 (3) | 155 |
O1W—H1A···O1iii | 0.91 | 1.90 | 2.800 (3) | 168 |
O1W—H2A···N2 | 0.89 | 2.40 | 3.223 (3) | 152 |
C12—H12···O1Wii | 0.93 | 2.58 | 3.466 (3) | 159 |
Symmetry codes: (i) −x, y−1/2, −z+3/2; (ii) −x, −y+1, −z+1; (iii) −x+1, −y+1, −z+1.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: XU2554).
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 I, global. DOI: 10.1107/S1600536809027329/xu2554sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536809027329/xu2554Isup2.hkl