Literature DB >> 21579180

1-[(E)-(2-Phenoxy-anilino)methyl-ene]naphthalen-2(1H)-one.

Ersin Temel, Erbil Ağar, Orhan Büyükgüngör.   

Abstract

The mol-ecule of the title compound, C(23)H(17)NO(2), a Schiff base derived from 2-hydr-oxy-1-naphthaldehyde, crystallizes in the keto-amine tautomeric form. The dihedral angle between the aniline and hydroxy-benzene rings is 77.41 (17)°, whereas the planes of the naphthaldehyde and fused aniline benzene rings are nearly coplanar, making a dihedral angle of 8.29 (15)°. Intra-molecular N-H⋯O hydrogen bonding, a characteristic hydrogen bond for Schiff bases, helps to stabilize the mol-ecular structure. Weak inter-molecular C-H⋯π inter-actions are present in the crystal structure.

Entities:  

Year:  2010        PMID: 21579180      PMCID: PMC2979135          DOI: 10.1107/S1600536810013851

Source DB:  PubMed          Journal:  Acta Crystallogr Sect E Struct Rep Online        ISSN: 1600-5368


Related literature

For Schiff bases, see: Caligaris et al. (1972 ▶); Caligaris & Randaccio et al. (1987 ▶); Salman et al. (1990 ▶); Popović et al. (2001 ▶); Garnovskii et al. (1993 ▶); Pyrz et al. (1985 ▶); Hadjoudis et al. (1987 ▶). For the HOMA (harmonic oscillator model of aromaticity) index, see: Krygowski et al. (1993 ▶). For similar structures, see: Özek et al. (2004 ▶); Takano et al. (2009 ▶).

Experimental

Crystal data

C23H17NO2 M = 339.38 Monoclinic, a = 14.6428 (11) Å b = 5.6297 (3) Å c = 42.602 (3) Å β = 101.175 (6)° V = 3445.3 (4) Å3 Z = 8 Mo Kα radiation μ = 0.08 mm−1 T = 296 K 0.40 × 0.34 × 0.23 mm

Data collection

Stoe IPDSII diffractometer Absorption correction: integration (X-RED; Stoe & Cie, 2002 ▶) T min = 0.960, T max = 0.996 11832 measured reflections 2565 independent reflections 1522 reflections with I > 2σ(I) R int = 0.212 θmax = 23.6°

Refinement

R[F 2 > 2σ(F 2)] = 0.115 wR(F 2) = 0.331 S = 1.06 2565 reflections 236 parameters H-atom parameters constrained Δρmax = 0.30 e Å−3 Δρmin = −0.39 e Å−3 Data collection: X-AREA (Stoe & Cie, 2002 ▶); cell refinement: X-AREA; data reduction: X-RED32 (Stoe & Cie, 2002 ▶); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); 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 ▶). Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536810013851/si2256sup1.cif Structure factors: contains datablocks I. DOI: 10.1107/S1600536810013851/si2256Isup2.hkl Additional supplementary materials: crystallographic information; 3D view; checkCIF report
C23H17NO2F(000) = 1424
Mr = 339.38Dx = 1.309 Mg m3
Monoclinic, C2/cMelting point = 411–413 K
Hall symbol: -C 2ycMo Kα radiation, λ = 0.71073 Å
a = 14.6428 (11) ÅCell parameters from 2565 reflections
b = 5.6297 (3) Åθ = 2.8–24.1°
c = 42.602 (3) ŵ = 0.08 mm1
β = 101.175 (6)°T = 296 K
V = 3445.3 (4) Å3Long prismatic rod, yellow
Z = 80.40 × 0.34 × 0.23 mm
Stoe IPDSII diffractometer2565 independent reflections
Radiation source: fine-focus sealed tube1522 reflections with I > 2σ(I)
plane graphiteRint = 0.212
Detector resolution: 6.67 pixels mm-1θmax = 23.6°, θmin = 2.8°
rotation scansh = −16→16
Absorption correction: integration (X-RED; Stoe & Cie, 2002)k = −6→6
Tmin = 0.960, Tmax = 0.996l = −47→47
11832 measured reflections
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.115H-atom parameters constrained
wR(F2) = 0.331w = 1/[σ2(Fo2) + (0.1935P)2] where P = (Fo2 + 2Fc2)/3
S = 1.06(Δ/σ)max = 0.001
2565 reflectionsΔρmax = 0.30 e Å3
236 parametersΔρmin = −0.39 e Å3
0 restraintsExtinction correction: SHELXL97 (Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methodsExtinction coefficient: 0.0045 (17)
Experimental. 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.
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 > 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.
xyzUiso*/Ueq
C10.4850 (4)−0.3268 (11)0.56310 (14)0.0576 (16)
C20.4649 (5)−0.1907 (13)0.53616 (18)0.0748 (19)
H20.4969−0.04990.53450.090*
C30.3949 (5)−0.2683 (15)0.51107 (16)0.082 (2)
H30.3797−0.18000.49230.099*
C40.3489 (4)−0.4759 (13)0.51444 (17)0.075 (2)
H40.3040−0.53140.49760.090*
C50.3683 (4)−0.6017 (12)0.54216 (17)0.0704 (19)
H50.3345−0.73830.54450.084*
C60.4377 (4)−0.5276 (11)0.56682 (15)0.0641 (18)
H60.4517−0.61440.58570.077*
C70.6418 (3)−0.3294 (10)0.59332 (14)0.0513 (14)
C80.7060 (3)−0.2112 (10)0.61624 (13)0.0482 (14)
C90.7982 (4)−0.2933 (11)0.62192 (15)0.0581 (16)
H90.8429−0.21580.63690.070*
C100.8231 (4)−0.4821 (11)0.60609 (16)0.0622 (17)
H100.8845−0.53430.61060.075*
C110.7588 (4)−0.5997 (11)0.58329 (15)0.0627 (17)
H110.7767−0.72840.57220.075*
C120.6665 (4)−0.5216 (12)0.57725 (15)0.0639 (18)
H120.6220−0.60020.56230.077*
C130.7229 (4)0.1281 (10)0.65264 (13)0.0503 (14)
H130.78720.10900.65710.060*
C140.6860 (4)0.3109 (9)0.66784 (13)0.0487 (14)
C150.5865 (4)0.3495 (10)0.66058 (15)0.0571 (16)
C160.5513 (4)0.5463 (12)0.67467 (18)0.0716 (19)
H160.48760.57470.66990.086*
C170.6065 (4)0.6971 (12)0.69492 (18)0.0704 (19)
H170.57970.82350.70390.084*
C180.7048 (4)0.6642 (10)0.70262 (14)0.0548 (15)
C190.7619 (5)0.8288 (11)0.72230 (14)0.0647 (17)
H190.73470.95660.73080.078*
C200.8549 (5)0.8045 (12)0.72899 (16)0.0730 (19)
H200.89160.91370.74220.088*
C210.8956 (5)0.6163 (13)0.71618 (17)0.078 (2)
H210.95990.59760.72130.094*
C220.8435 (4)0.4567 (12)0.69608 (16)0.0691 (19)
H220.87280.33520.68700.083*
C230.7448 (4)0.4752 (9)0.68896 (12)0.0481 (14)
N10.6738 (3)−0.0213 (8)0.63234 (10)0.0493 (12)
H10.61460.00050.62850.059*
O10.5318 (2)0.2158 (8)0.64128 (11)0.0720 (14)
O20.5522 (2)−0.2386 (8)0.58887 (11)0.0755 (15)
U11U22U33U12U13U23
C10.031 (3)0.080 (4)0.055 (4)0.002 (3)−0.008 (3)−0.025 (3)
C20.060 (4)0.084 (4)0.075 (5)−0.016 (3)−0.001 (3)−0.005 (4)
C30.072 (5)0.116 (6)0.050 (4)−0.011 (4)−0.010 (3)0.007 (4)
C40.044 (3)0.098 (5)0.072 (5)−0.011 (3)−0.014 (3)−0.016 (4)
C50.045 (3)0.084 (4)0.075 (5)−0.010 (3)−0.005 (3)−0.007 (4)
C60.049 (3)0.074 (4)0.060 (4)0.001 (3)−0.013 (3)−0.002 (3)
C70.028 (3)0.066 (3)0.055 (3)0.000 (2)−0.003 (2)−0.011 (3)
C80.033 (3)0.068 (3)0.042 (3)−0.005 (2)0.003 (2)−0.006 (3)
C90.031 (3)0.075 (4)0.062 (4)−0.010 (3)−0.007 (3)0.001 (3)
C100.032 (3)0.077 (4)0.074 (4)−0.003 (3)0.003 (3)−0.008 (3)
C110.043 (3)0.080 (4)0.064 (4)0.001 (3)0.008 (3)−0.014 (3)
C120.033 (3)0.093 (4)0.061 (4)−0.007 (3)−0.002 (3)−0.022 (3)
C130.033 (3)0.071 (3)0.043 (3)0.000 (3)−0.003 (2)−0.001 (3)
C140.034 (3)0.062 (3)0.046 (3)−0.003 (2)−0.003 (2)0.001 (3)
C150.029 (3)0.069 (4)0.069 (4)−0.003 (3)0.000 (3)−0.001 (3)
C160.034 (3)0.090 (5)0.088 (5)0.006 (3)0.004 (3)−0.012 (4)
C170.048 (3)0.080 (4)0.083 (5)0.014 (3)0.012 (3)−0.004 (4)
C180.049 (3)0.061 (3)0.050 (3)0.004 (3)0.000 (3)0.000 (3)
C190.073 (4)0.065 (4)0.050 (3)0.008 (3)−0.001 (3)−0.008 (3)
C200.070 (4)0.082 (4)0.060 (4)−0.009 (4)−0.005 (3)−0.013 (3)
C210.045 (3)0.106 (5)0.075 (5)−0.004 (3)−0.007 (3)−0.021 (4)
C220.038 (3)0.093 (4)0.070 (4)0.003 (3)−0.007 (3)−0.034 (3)
C230.041 (3)0.058 (3)0.040 (3)0.003 (2)−0.004 (2)0.002 (2)
N10.027 (2)0.071 (3)0.045 (3)−0.006 (2)−0.0059 (19)−0.006 (2)
O10.0240 (19)0.097 (3)0.087 (3)−0.0049 (19)−0.009 (2)−0.018 (3)
O20.028 (2)0.106 (3)0.083 (3)0.004 (2)−0.013 (2)−0.047 (3)
C1—C61.351 (9)C12—H120.9300
C1—C21.364 (9)C13—N11.315 (6)
C1—O21.414 (6)C13—C141.381 (8)
C2—C31.400 (9)C13—H130.9300
C2—H20.9300C14—C151.447 (7)
C3—C41.370 (10)C14—C231.451 (7)
C3—H30.9300C15—O11.276 (7)
C4—C51.359 (10)C15—C161.404 (9)
C4—H40.9300C16—C171.359 (9)
C5—C61.377 (8)C16—H160.9300
C5—H50.9300C17—C181.425 (8)
C6—H60.9300C17—H170.9300
C7—C121.366 (8)C18—C231.395 (8)
C7—O21.387 (6)C18—C191.411 (8)
C7—C81.387 (7)C19—C201.344 (10)
C8—N11.400 (7)C19—H190.9300
C8—C91.403 (8)C20—C211.379 (10)
C9—C101.347 (9)C20—H200.9300
C9—H90.9300C21—C221.368 (8)
C10—C111.383 (8)C21—H210.9300
C10—H100.9300C22—C231.422 (8)
C11—C121.397 (8)C22—H220.9300
C11—H110.9300N1—H10.8600
C6—C1—C2122.4 (5)N1—C13—H13117.6
C6—C1—O2119.9 (6)C14—C13—H13117.6
C2—C1—O2117.4 (6)C13—C14—C15118.8 (5)
C1—C2—C3118.3 (7)C13—C14—C23121.8 (5)
C1—C2—H2120.9C15—C14—C23119.3 (5)
C3—C2—H2120.9O1—C15—C16120.3 (5)
C4—C3—C2119.2 (7)O1—C15—C14122.0 (5)
C4—C3—H3120.4C16—C15—C14117.7 (5)
C2—C3—H3120.4C17—C16—C15122.9 (5)
C5—C4—C3120.8 (6)C17—C16—H16118.6
C5—C4—H4119.6C15—C16—H16118.6
C3—C4—H4119.6C16—C17—C18120.9 (6)
C4—C5—C6120.3 (6)C16—C17—H17119.5
C4—C5—H5119.9C18—C17—H17119.5
C6—C5—H5119.9C23—C18—C19120.0 (5)
C1—C6—C5118.9 (6)C23—C18—C17119.4 (5)
C1—C6—H6120.5C19—C18—C17120.5 (6)
C5—C6—H6120.5C20—C19—C18121.3 (6)
C12—C7—O2124.0 (5)C20—C19—H19119.4
C12—C7—C8121.5 (5)C18—C19—H19119.4
O2—C7—C8114.4 (5)C19—C20—C21119.5 (6)
C7—C8—N1117.7 (5)C19—C20—H20120.2
C7—C8—C9117.5 (5)C21—C20—H20120.2
N1—C8—C9124.8 (5)C22—C21—C20121.4 (6)
C10—C9—C8121.3 (5)C22—C21—H21119.3
C10—C9—H9119.4C20—C21—H21119.3
C8—C9—H9119.4C21—C22—C23120.4 (6)
C9—C10—C11121.0 (6)C21—C22—H22119.8
C9—C10—H10119.5C23—C22—H22119.8
C11—C10—H10119.5C18—C23—C22117.3 (5)
C10—C11—C12118.8 (6)C18—C23—C14119.9 (5)
C10—C11—H11120.6C22—C23—C14122.8 (5)
C12—C11—H11120.6C13—N1—C8128.1 (4)
C7—C12—C11119.9 (5)C13—N1—H1115.9
C7—C12—H12120.1C8—N1—H1115.9
C11—C12—H12120.1C7—O2—C1118.3 (4)
N1—C13—C14124.8 (5)
C6—C1—C2—C3−2.5 (11)C14—C15—C16—C17−1.0 (11)
O2—C1—C2—C3−176.5 (6)C15—C16—C17—C181.0 (11)
C1—C2—C3—C40.3 (11)C16—C17—C18—C230.4 (10)
C2—C3—C4—C52.4 (12)C16—C17—C18—C19176.6 (7)
C3—C4—C5—C6−3.0 (11)C23—C18—C19—C20−1.8 (10)
C2—C1—C6—C51.9 (10)C17—C18—C19—C20−177.9 (7)
O2—C1—C6—C5175.7 (6)C18—C19—C20—C210.6 (11)
C4—C5—C6—C10.9 (10)C19—C20—C21—C221.7 (12)
C12—C7—C8—N1−177.8 (5)C20—C21—C22—C23−2.7 (12)
O2—C7—C8—N11.2 (8)C19—C18—C23—C220.7 (9)
C12—C7—C8—C91.2 (9)C17—C18—C23—C22176.9 (6)
O2—C7—C8—C9−179.8 (5)C19—C18—C23—C14−177.9 (5)
C7—C8—C9—C10−1.0 (9)C17—C18—C23—C14−1.7 (9)
N1—C8—C9—C10177.9 (6)C21—C22—C23—C181.5 (10)
C8—C9—C10—C111.0 (10)C21—C22—C23—C14−180.0 (6)
C9—C10—C11—C12−1.1 (10)C13—C14—C23—C18176.9 (5)
O2—C7—C12—C11179.8 (6)C15—C14—C23—C181.6 (8)
C8—C7—C12—C11−1.4 (10)C13—C14—C23—C22−1.6 (9)
C10—C11—C12—C71.3 (10)C15—C14—C23—C22−176.9 (6)
N1—C13—C14—C15−2.0 (9)C14—C13—N1—C8−179.5 (5)
N1—C13—C14—C23−177.4 (5)C7—C8—N1—C13−173.3 (5)
C13—C14—C15—O12.0 (9)C9—C8—N1—C137.7 (9)
C23—C14—C15—O1177.4 (6)C12—C7—O2—C1−9.5 (10)
C13—C14—C15—C16−175.8 (6)C8—C7—O2—C1171.6 (6)
C23—C14—C15—C16−0.3 (9)C6—C1—O2—C784.9 (8)
O1—C15—C16—C17−178.8 (7)C2—C1—O2—C7−101.0 (7)
Cg1 and Cg2 are the centroids of the C1–C6 and C18–C23 rings, respectively.
D—H···AD—HH···AD···AD—H···A
N1—H1···O10.861.872.561 (6)136
C11—H11···Cg1i0.932.873.664 (7)144
C19—H19···Cg2ii0.932.903.674 (7)142
Table 1

Hydrogen-bond geometry (Å, °)

Cg1 and Cg2 are the centroids of the C1–C6 and C18–C23 rings, respectively.

D—H⋯AD—HH⋯ADAD—H⋯A
N1—H1⋯O10.861.872.561 (6)136
C11—H11⋯Cg1i0.932.873.664 (7)144
C19—H19⋯Cg2ii0.932.903.674 (7)142

Symmetry codes: (i) ; (ii) .

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