supplementary materials


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Acta Cryst. (2008). E64, o768    [ doi:10.1107/S1600536808008076 ]

N'-(2-Hydroxynaphthylidene)-4-methoxybenzohydrazide

C.-B. Tang

Abstract top

The title Schiff base compound, C19H16N2O3, was derived from the condensation reaction of 2-hydroxy-1-naphthylaldehyde with 4-methoxybenzohydrazide. The dihedral angle between the benzene ring and the naphthyl ring system is 6.8 (2)°. In the crystal structure, molecules are linked through intermolecular N-H...O intermolecular hydrogen bonds, forming chains running along the c axis.

Comment top

Recently, the author has reported the structures of several Schiff base compounds (Tang, 2006, 2007a,b,c,d) and, in continuation of work in this area, reports herein the structure of the title compound, (I), Fig. 1, a new Schiff base compound.

In the title compound (Fig. 1), the dihedral angle between the benzene ring and the naphtyl ring is 6.8 (2)°. The torsion angles C1—C11—N1—N2, C11—N1—N2—C12, and N1—N2—C12—C13 are 1.3 (2), 17.0 (2), and 1.5 (2)°, respectively. All the bond lengths are within normal values (Allen et al., 1987).

In the crystal structure of the compound, molecules are linked through N—H···O intermolecular hydrogen bonds (Table 1), forming chains running along the c axis (Fig. 2).

Related literature top

For related structures, see: Tang (2006, 2007a,b,c,d). For reference structural data, see: Allen et al. (1987).

Experimental top

2-Hydroxy-1-naphtylaldehyde (0.1 mmol, 17.2 mg) and 4-methoxybenzohydrazide (0.1 mmol, 16.6 mg) were dissolved in an ethanol solution (20 ml). The mixture was stirred at reflux for 10 min to give a clear colorless solution. Colorless needle-like crystals of the compound were formed by slow evaporation of the solvent over several days.

Refinement top

H2 atom was located from a difference Fourier map and refined isotropically, with N—H distance restrained to 0.90 (1) Å. Other H atoms were constrained to ideal geometries, with C—H = 0.93–0.96 Å, O—H = 0.82 Å, and with Uiso(H) = 1.2Ueq(C), 1.5Ueq(C19 and O1).

Computing details top

Data collection: SMART (Bruker, 2002); cell refinement: SAINT (Bruker, 2002); data reduction: SAINT (Bruker, 2002); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: SHELXTL (Sheldrick, 2008); software used to prepare material for publication: SHELXL97 (Sheldrick, 2008).

Figures top
[Figure 1] Fig. 1. The molecular structure of the compound, showing the atom-numbering scheme. Displacement ellipsoids are drawn at the 30% probability level.
[Figure 2] Fig. 2. Molecular packing of (I) with hydrogen bonds drawn as dashed lines.
N'-(2-Hydroxynaphthylidene)-4-methoxybenzohydrazide top
Crystal data top
C19H16N2O3F000 = 672
Mr = 320.34Dx = 1.368 Mg m3
Monoclinic, P21/cMo Kα radiation
λ = 0.71073 Å
Hall symbol: -P 2ybcCell parameters from 1378 reflections
a = 11.159 (2) Åθ = 2.2–24.5º
b = 15.790 (3) ŵ = 0.09 mm1
c = 8.8300 (18) ÅT = 298 (2) K
β = 91.70 (3)ºCut from a needle, colorless
V = 1555.2 (5) Å30.32 × 0.32 × 0.30 mm
Z = 4
Data collection top
Bruker SMART CCD area-detector
diffractometer
3550 independent reflections
Radiation source: fine-focus sealed tube2161 reflections with I > 2σ(I)
Monochromator: graphiteRint = 0.052
T = 298(2) Kθmax = 27.5º
ω scansθmin = 1.8º
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
h = 14→14
Tmin = 0.971, Tmax = 0.972k = 20→20
13232 measured reflectionsl = 11→11
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.056H atoms treated by a mixture of
independent and constrained refinement
wR(F2) = 0.136  w = 1/[σ2(Fo2) + (0.0391P)2 + 0.168P]
where P = (Fo2 + 2Fc2)/3
S = 1.04(Δ/σ)max = 0.001
3550 reflectionsΔρmax = 0.18 e Å3
222 parametersΔρmin = 0.20 e Å3
1 restraintExtinction correction: none
Primary atom site location: structure-invariant direct methods
Crystal data top
C19H16N2O3V = 1555.2 (5) Å3
Mr = 320.34Z = 4
Monoclinic, P21/cMo Kα
a = 11.159 (2) ŵ = 0.09 mm1
b = 15.790 (3) ÅT = 298 (2) K
c = 8.8300 (18) Å0.32 × 0.32 × 0.30 mm
β = 91.70 (3)º
Data collection top
Bruker SMART CCD area-detector
diffractometer
3550 independent reflections
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
2161 reflections with I > 2σ(I)
Tmin = 0.971, Tmax = 0.972Rint = 0.052
13232 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0561 restraint
wR(F2) = 0.136H atoms treated by a mixture of
independent and constrained refinement
S = 1.04Δρmax = 0.18 e Å3
3550 reflectionsΔρmin = 0.20 e Å3
222 parameters
Special details top

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) top
xyzUiso*/Ueq
O10.44682 (14)0.12307 (9)0.77419 (16)0.0569 (4)
H10.40890.15840.72440.085*
O20.24817 (13)0.32717 (8)0.67361 (14)0.0515 (4)
O30.02184 (13)0.57256 (9)0.17402 (17)0.0602 (5)
N10.30518 (14)0.17750 (9)0.55897 (17)0.0415 (4)
N20.25139 (15)0.24056 (10)0.47098 (17)0.0423 (4)
C10.35505 (16)0.03145 (12)0.5862 (2)0.0362 (4)
C20.42732 (17)0.04559 (13)0.7145 (2)0.0431 (5)
C30.48691 (18)0.02246 (15)0.7874 (2)0.0520 (6)
H30.53700.01210.87150.062*
C40.47221 (19)0.10234 (14)0.7367 (2)0.0526 (6)
H40.51240.14620.78680.063*
C50.39740 (17)0.12109 (13)0.6096 (2)0.0434 (5)
C60.3824 (2)0.20495 (13)0.5558 (3)0.0561 (6)
H60.42300.24890.60510.067*
C70.3101 (2)0.22238 (14)0.4342 (3)0.0608 (6)
H70.30070.27790.40070.073*
C80.2498 (2)0.15638 (14)0.3591 (3)0.0586 (6)
H80.20050.16830.27500.070*
C90.26197 (18)0.07449 (12)0.4075 (2)0.0458 (5)
H90.21980.03180.35660.055*
C100.33734 (16)0.05348 (11)0.5331 (2)0.0371 (5)
C110.29956 (17)0.10221 (12)0.5053 (2)0.0388 (5)
H110.25940.09260.41310.047*
C120.22727 (17)0.31534 (11)0.5375 (2)0.0376 (5)
C130.17287 (17)0.38188 (11)0.4404 (2)0.0365 (4)
C140.18459 (18)0.46552 (12)0.4857 (2)0.0454 (5)
H140.22590.47780.57610.054*
C150.13651 (19)0.53130 (12)0.4000 (2)0.0493 (5)
H150.14660.58710.43170.059*
C160.07353 (17)0.51333 (12)0.2674 (2)0.0427 (5)
C170.05869 (18)0.43022 (12)0.2214 (2)0.0453 (5)
H170.01470.41800.13290.054*
C180.10864 (17)0.36569 (12)0.3058 (2)0.0406 (5)
H180.09950.31010.27250.049*
C190.0515 (2)0.65852 (13)0.2009 (3)0.0685 (7)
H19A0.02240.67550.29740.103*
H19B0.01530.69310.12270.103*
H19C0.13700.66520.20070.103*
H20.251 (2)0.2301 (14)0.3703 (12)0.080*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O10.0614 (11)0.0580 (10)0.0505 (10)0.0051 (8)0.0100 (8)0.0063 (8)
O20.0791 (11)0.0422 (8)0.0326 (8)0.0005 (7)0.0063 (7)0.0019 (6)
O30.0683 (11)0.0440 (9)0.0674 (11)0.0126 (7)0.0113 (8)0.0084 (8)
N10.0508 (11)0.0356 (9)0.0380 (9)0.0008 (8)0.0009 (8)0.0047 (7)
N20.0608 (11)0.0320 (9)0.0339 (9)0.0046 (8)0.0029 (9)0.0013 (7)
C10.0350 (10)0.0388 (11)0.0350 (11)0.0019 (8)0.0038 (8)0.0062 (8)
C20.0391 (11)0.0500 (13)0.0405 (12)0.0026 (10)0.0036 (9)0.0034 (10)
C30.0414 (12)0.0728 (16)0.0413 (13)0.0038 (11)0.0065 (10)0.0114 (11)
C40.0465 (13)0.0549 (14)0.0564 (14)0.0122 (10)0.0035 (11)0.0204 (11)
C50.0371 (11)0.0461 (12)0.0474 (12)0.0058 (9)0.0077 (9)0.0119 (10)
C60.0589 (15)0.0399 (13)0.0700 (16)0.0138 (11)0.0121 (12)0.0144 (11)
C70.0684 (16)0.0394 (13)0.0750 (17)0.0035 (11)0.0085 (14)0.0022 (12)
C80.0658 (16)0.0512 (14)0.0586 (15)0.0033 (11)0.0020 (12)0.0065 (11)
C90.0500 (13)0.0380 (11)0.0492 (13)0.0013 (9)0.0004 (10)0.0014 (9)
C100.0349 (11)0.0396 (11)0.0370 (11)0.0022 (9)0.0062 (9)0.0069 (9)
C110.0421 (12)0.0395 (11)0.0348 (11)0.0008 (9)0.0006 (9)0.0035 (9)
C120.0423 (11)0.0359 (11)0.0346 (11)0.0056 (8)0.0005 (9)0.0003 (8)
C130.0397 (11)0.0349 (10)0.0350 (11)0.0017 (8)0.0033 (8)0.0002 (8)
C140.0545 (13)0.0409 (12)0.0403 (12)0.0017 (10)0.0045 (10)0.0061 (9)
C150.0609 (14)0.0322 (11)0.0547 (14)0.0017 (10)0.0011 (11)0.0036 (10)
C160.0408 (11)0.0412 (12)0.0458 (12)0.0050 (9)0.0008 (9)0.0032 (9)
C170.0454 (13)0.0479 (13)0.0421 (12)0.0002 (10)0.0077 (10)0.0004 (10)
C180.0467 (12)0.0351 (11)0.0397 (11)0.0029 (9)0.0020 (9)0.0046 (9)
C190.0857 (19)0.0414 (13)0.0784 (18)0.0172 (12)0.0019 (14)0.0076 (12)
Geometric parameters (Å, °) top
O1—C21.347 (2)C7—C81.397 (3)
O1—H10.8200C7—H70.9300
O2—C121.231 (2)C8—C91.367 (3)
O3—C161.363 (2)C8—H80.9300
O3—C191.415 (2)C9—C101.411 (3)
N1—C111.281 (2)C9—H90.9300
N1—N21.388 (2)C11—H110.9300
N2—C121.350 (2)C12—C131.475 (3)
N2—H20.904 (9)C13—C141.385 (2)
C1—C21.389 (3)C13—C181.394 (3)
C1—C101.432 (2)C14—C151.384 (3)
C1—C111.455 (2)C14—H140.9300
C2—C31.409 (3)C15—C161.377 (3)
C3—C41.347 (3)C15—H150.9300
C3—H30.9300C16—C171.382 (3)
C4—C51.410 (3)C17—C181.371 (3)
C4—H40.9300C17—H170.9300
C5—C61.415 (3)C18—H180.9300
C5—C101.421 (3)C19—H19A0.9600
C6—C71.352 (3)C19—H19B0.9600
C6—H60.9300C19—H19C0.9600
C2—O1—H1109.5C9—C10—C5117.31 (18)
C16—O3—C19117.63 (17)C9—C10—C1123.40 (17)
C11—N1—N2116.28 (16)C5—C10—C1119.29 (18)
C12—N2—N1118.18 (15)N1—C11—C1121.04 (18)
C12—N2—H2126.4 (15)N1—C11—H11119.5
N1—N2—H2114.0 (15)C1—C11—H11119.5
C2—C1—C10119.24 (17)O2—C12—N2121.54 (17)
C2—C1—C11120.36 (18)O2—C12—C13121.46 (17)
C10—C1—C11120.39 (17)N2—C12—C13116.99 (16)
O1—C2—C1123.23 (18)C14—C13—C18117.57 (18)
O1—C2—C3116.45 (18)C14—C13—C12118.53 (17)
C1—C2—C3120.31 (19)C18—C13—C12123.89 (17)
C4—C3—C2120.7 (2)C15—C14—C13121.75 (19)
C4—C3—H3119.6C15—C14—H14119.1
C2—C3—H3119.6C13—C14—H14119.1
C3—C4—C5121.63 (19)C16—C15—C14119.34 (19)
C3—C4—H4119.2C16—C15—H15120.3
C5—C4—H4119.2C14—C15—H15120.3
C4—C5—C6121.66 (19)O3—C16—C15124.67 (18)
C4—C5—C10118.73 (19)O3—C16—C17115.39 (18)
C6—C5—C10119.6 (2)C15—C16—C17119.94 (18)
C7—C6—C5121.3 (2)C18—C17—C16120.17 (18)
C7—C6—H6119.4C18—C17—H17119.9
C5—C6—H6119.4C16—C17—H17119.9
C6—C7—C8119.5 (2)C17—C18—C13121.20 (18)
C6—C7—H7120.2C17—C18—H18119.4
C8—C7—H7120.2C13—C18—H18119.4
C9—C8—C7121.0 (2)O3—C19—H19A109.5
C9—C8—H8119.5O3—C19—H19B109.5
C7—C8—H8119.5H19A—C19—H19B109.5
C8—C9—C10121.29 (19)O3—C19—H19C109.5
C8—C9—H9119.4H19A—C19—H19C109.5
C10—C9—H9119.4H19B—C19—H19C109.5
Hydrogen-bond geometry (Å, °) top
D—H···AD—HH···AD···AD—H···A
O1—H1···N10.821.862.582 (2)146
N2—H2···O2i0.904 (9)1.957 (12)2.834 (2)163 (2)
Symmetry codes: (i) x, −y+1/2, z−1/2.
Table 1
Hydrogen-bond geometry (Å, °)
top
D—H···AD—HH···AD···AD—H···A
O1—H1···N10.821.862.582 (2)146
N2—H2···O2i0.904 (9)1.957 (12)2.834 (2)163 (2)
Symmetry codes: (i) x, −y+1/2, z−1/2.
Acknowledgements top

Financial support from the Jiaying University Research Fund is gratefully acknowledged.

references
References top

Allen, F. H., Kennard, O., Watson, D. G., Brammer, L., Orpen, A. G. & Taylor, R. (1987). J. Chem. Soc. Perkin Trans. 2, pp. S1–19.

Bruker (2002). SAINT (Version 5.62) and SMART (Version 6.02). Bruker AXS Inc., Madison, Wisconsin, USA.

Sheldrick, G. M. (1996). SADABS. University of Göttingen, Germany.

Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122.

Tang, C.-B. (2006). Acta Cryst. E63, m2629–m2630.

Tang, C.-B. (2007a). Acta Cryst. E63, m2654.

Tang, C.-B. (2007b). Acta Cryst. E63, m2785–m2786.

Tang, C.-B. (2007c). Acta Cryst. E63, o4545.

Tang, C.-B. (2007d). Acta Cryst. E63, o4841.