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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2011 Oct 12;67(Pt 11):o2958–o2959. doi: 10.1107/S1600536811041870

1-[(4-{[(2-Oxo-1,2-dihydro­naphthalen-1-yl­idene)meth­yl]amino}­anilino)methyl­idene]naphthalen-2(1H)-one dihydrate

Anita Blagus a,*, Branko Kaitner b
PMCID: PMC3247366  PMID: 22219984

Abstract

The title compound, C28H20N2O2·2H2O, comprises a Schiff base mol­ecule with an imposed inversion centre in the middle of p-phenyl­enediamine unit and water mol­ecules of crystallization. In the structure, the Schiff base mol­ecule is present as the keto–amino tautomer with a strong intra­molecular N—H⋯O hydrogen bond. The Schiff base mol­ecules and water mol­ecules of crystallization create infinite [010] columns through O—H⋯O hydrogen bonds. Inter­molecular attractions within columns are through additional π–π inter­actions [centroid–centroid distance = 3.352 (1) Å] between parallel Schiff base mol­ecules. The columns are joined into infinite (011) layers through weak C—H⋯O hydrogen bonds. The layers pack in an assembly by van der Waals attractions, only being effective between bordering non-polar naphthalene ring systems.

Related literature

For general background to Schiff bases, see: Blagus et al. (2010). The stereochemistry of intrinsic Schiff bases differs significantly, see: Inabe et al. (1994). For the quinoid effect in 2-oxy-naphthaldimine Schiff base derivatives, see: Gavranić et al. (1996); Friščić et al. (1998). For the herringbone packing motif in fused aromatic systems, see: Desiraju & Gavezzotti (1989).graphic file with name e-67-o2958-scheme1.jpg

Experimental

Crystal data

  • C28H20N2O2·2H2O

  • M r = 452.49

  • Monoclinic, Inline graphic

  • a = 17.4222 (11) Å

  • b = 4.4686 (5) Å

  • c = 15.9374 (10) Å

  • β = 116.30 (1)°

  • V = 1112.3 (2) Å3

  • Z = 2

  • Mo Kα radiation

  • μ = 0.09 mm−1

  • T = 298 K

  • 0.5 × 0.2 × 0.1 mm

Data collection

  • Oxford Diffraction Xcalibur CCD diffractometer

  • 14006 measured reflections

  • 2423 independent reflections

  • 1351 reflections with I > 2σ(I)

  • R int = 0.054

Refinement

  • R[F 2 > 2σ(F 2)] = 0.061

  • wR(F 2) = 0.190

  • S = 1.05

  • 2423 reflections

  • 160 parameters

  • 3 restraints

  • H atoms treated by a mixture of independent and constrained refinement

  • Δρmax = 0.20 e Å−3

  • Δρmin = −0.27 e Å−3

Data collection: CrysAlis CCD (Oxford Diffraction, 2003); cell refinement: CrysAlis CCD; data reduction: CrysAlis RED (Oxford Diffraction, 2003); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: ORTEP-3 (Farrugia, 1997); software used to prepare material for publication: WinGX (Farrugia, 1999), PARST97 (Nardelli, 1995) and Mercury (Macrae et al., 2006).

Supplementary Material

Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536811041870/kp2357sup1.cif

e-67-o2958-sup1.cif (16.4KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811041870/kp2357Isup2.hkl

e-67-o2958-Isup2.hkl (119.1KB, hkl)

Supplementary material file. DOI: 10.1107/S1600536811041870/kp2357Isup3.cml

Additional supplementary materials: crystallographic information; 3D view; checkCIF report

Table 1. Hydrogen-bond geometry (Å, °).

D—H⋯A D—H H⋯A DA D—H⋯A
N1—H1⋯O1 0.86 1.86 2.560 (3) 138
O1W—H1B⋯O1 0.83 2.27 3.090 (4) 169
O1W—H1A⋯O1i 0.84 2.01 2.826 (4) 165
C13—H13⋯O1Wii 0.93 2.33 3.247 (5) 170

Symmetry codes: (i) Inline graphic; (ii) Inline graphic.

Acknowledgments

Financial support by the Ministry of Science, Education and Sport of the Republic of Croatia is gratefully acknowledged (grant No. 119–1193079–3069).

supplementary crystallographic information

Comment

Desiraju and Gavezzotti presented classification of packing arrangements for polynuclear aromatic hydrocarbons depending on the number and positions of C and H atoms in molecules (Desiraju & Gavezzotti, 1989). As a result of significant planarity, Schiff bases derived from p-phenylenediamine have significant aromatic-aromatic C···C interactions compared to the number of intermolecular C–H hydrogen bonds and usually show a herringbone motif of intermolecular assembly (Blagus et al., 2010).

We report here the crystal structure of the title compound (I) as a crystal hydrate. The stereochemistry of intrinsic 1,4-bis(2-hydroxy-1-naphthylmethylideneamino)benzene was earlier determined and reported (Inabe et al., 1994). Distinctively planar Schiff base molecule possesses crystallographic inversion centre in the middle of p-phenylenediamine moiety with anti arrangements of chelate rings (Fig. 1). Interplanar angle between naphthalene moiety and the central aromatic ring is 1.7 (2)°. Schiff base molecule does not deviate significantly from planarity in contrast to the structure by Inabe et al. with corresponding interplanar angle being 22.3°.In both structures molecules possess internal (molecular) symmetry with inversion centre in the middle of p-phenylenediamine moiety.

Bond distances C2–O1 [1.277 (4) Å] and C11–N1 [1.322 (4) Å] indicate keto-amino tautomeric form of (I). This is confirmed by a formation of strong intramolecular hydrogen bond N–H···O [N···O = 2.560 (3) Å]. Short C3-to-C4 bond distance [1.345 (5) Å] with O1 oxygen atom at C2 position of naphthalene core indicates the presence of quinoid effect (Gavranić et al., 1996; Friščić et al., 1998). Water molecules play crucial role in crystal packing: a) as bridging media pilling up Schiff base molecules at the separation characteristic for graphite in the form of infinite [010] columns and b) as bridging molecule connecting neighboring [010] columns into infinite (011) layers. Hydrogen bonds effective for columns formation are: a) O1W–H1A···O1i 2.826 (4) Å [(i): x, y + 1, z] and O1W–H1B···O1 3.090 (4) Å while for layers formation is effective b) C13–H13···OW1ii 3.247 (5) Å [(ii): x, – y + 3/2, z] (Fig. 2 and Table 1).

Along with intermolecular contacts via hydrogen bonds the linking between molecules amplifies through π–π interactions with offset (Fig. 2). Schiff base molecules arrange parallel to each other with their middle p-phenylenediamine moiety being separated at distances characteristic for layer separation in graphite. The shortest separations corresponding to the sum of van der Waals radii are: C12···C12iii 3.362 (3) Å [(iii): -x, -y + 1, -z] and C11···C13iv 3.374 (3) Å [(iv): x, y - 1, z]. π··· π interactions are also characterised by perpendicular Cgiii···Cgv distance 3.352 (1) Å [(v): -x, 3 - y, -z] and slippage of 2.955 Å. There is a space between each pair of neighboring columns large enough to accommodate water molecules (Fig. 3). Connection between neighboring parallel layers is accomplished through bordering non-polar naphthalene core by the standard van der Walls attractions. The rather planar Schiff base molecules of (I) reveal characteristic herringbone motif of packing arrangement (Fig. 4).

Experimental

The crystals of (I), (1,4-bis(2-hydroxy-1-naphthylmethylideneamino)benzene as crystal hydrate were obtained during an unsuccessful attempt to synthesise the nickel complex of corresponding Schiff base. Schiff base itself was prepared separately in standard way by condensation of 2-hydroxy-naphtaldehyde and p-phenylenediamine in ethanol solution in molar ratio 2:1 and used as a ligand in metal complex synthesis. The 1:1 mixture of 0.1 mmol DMSO solutions of Schiff base and 0.2 mmol nickel salt, NiCl2. 6H2O was stirred under reflux for two h at 373 K. Preparation of nickel complex failed. The crystals of title compound crystallised from mother liquor after cooling to RT and mechanically separated from nickel salt.

Refinement

Hydrogen atoms were refined in two different ways.

For hydrogen atoms bonded to C and N atoms benzene type riding mode was used with C-to-H and N-to-H bond distances taken as 0.93 and 0.86 Å, respectively.

Due to somewhat higher values of anisotropic thermal parameters of O1W oxygen atom, implying to certain disorder of water molecule, bond distances O1W to H1A and H1B, respectively, as well as bond distance H1A–H1B were restrained to the values accepted for water molecule. Bond distances O1W to H1A and H1B, respectively were fixed to 0.82 (1) Å and H1A to H1B to 1.30 (1) Å and the position of hydrogen atoms were re-calculated in consecutive refinement cycles. Isotropic thermal parameters for hydrogen atoms were estimated as 1.2 times of equivalent isotropic thermal parameter of corresponding C, N and O atoms.

Figures

Fig. 1.

Fig. 1.

A general overview of (I) showing numbering scheme with anisotropic thermal ellipsoids pictured at 30% probability level. Thin lines display intra N–H···O, and the two intermolecular hydrogen bonds O–H···O and C–H···O. Hydrogen atoms are drawn as spheres of arbitrary radius.

Fig. 2.

Fig. 2.

The display of three intermolecular contacts of water molecule with nearby Schiff base molecules. Two Schiff base molecules connected by π–π interactions are additionally bridged with a water molecule through two strong hydrogen bonds O1W–H1A···O1i [(i): x, y + 1, z] and O1W–H1B···O1, respectively. The third intermolecular contact of water molecule is via C13–H13···OW1ii 3.247 (5) Å [(ii): x, - y + 3/2, z] interaction.

Fig. 3.

Fig. 3.

Water molecules of crystallisation occupy the cylindrical voids formed by assembling Schiff base molecules into the [010] columns.

Fig. 4.

Fig. 4.

The display of herringbone packing arrangement of Schiff base molecules viewed down c-axes. Water molecules and all hydrogen atoms were omitted for clarity.

Crystal data

C28H20N2O2·2H2O F(000) = 476
Mr = 452.49 Dx = 1.351 Mg m3
Monoclinic, P21/c Mo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ybc Cell parameters from 2423 reflections
a = 17.4222 (11) Å θ = 4–27°
b = 4.4686 (5) Å µ = 0.09 mm1
c = 15.9374 (10) Å T = 298 K
β = 116.30 (1)° Prism, green
V = 1112.3 (2) Å3 0.5 × 0.2 × 0.1 mm
Z = 2

Data collection

Oxford Diffraction Xcalibur CCD diffractometer 1351 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tube Rint = 0.054
graphite θmax = 27.0°, θmin = 3.9°
ω scans h = −22→21
14006 measured reflections k = −5→5
2423 independent reflections l = −20→20

Refinement

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)] = 0.061 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.190 H atoms treated by a mixture of independent and constrained refinement
S = 1.05 w = 1/[σ2(Fo2) + (0.0914P)2 + 0.2128P] where P = (Fo2 + 2Fc2)/3
2423 reflections (Δ/σ)max = 0.009
160 parameters Δρmax = 0.20 e Å3
3 restraints Δρmin = −0.27 e Å3

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
O1 0.19806 (12) 0.2820 (4) 0.25053 (12) 0.0537 (6)
N1 0.12888 (13) 0.5855 (4) 0.09888 (14) 0.0420 (5)
H1 0.1321 0.5349 0.1524 0.050*
C1 0.24546 (15) 0.2518 (5) 0.13184 (17) 0.0383 (6)
C2 0.25000 (16) 0.1743 (5) 0.22164 (17) 0.0416 (6)
C3 0.31492 (17) −0.0329 (6) 0.27967 (18) 0.0486 (7)
H3 0.3186 −0.0853 0.3378 0.058*
C4 0.37040 (18) −0.1525 (6) 0.25139 (19) 0.0495 (7)
H4 0.4116 −0.2855 0.2910 0.059*
C5 0.36876 (15) −0.0839 (5) 0.16289 (18) 0.0427 (6)
C6 0.42800 (18) −0.2111 (6) 0.1358 (2) 0.0527 (7)
H6 0.4696 −0.3410 0.1764 0.063*
C7 0.42563 (19) −0.1479 (7) 0.0517 (2) 0.0583 (8)
H7 0.4654 −0.2326 0.0345 0.070*
C8 0.36356 (19) 0.0436 (6) −0.0084 (2) 0.0568 (8)
H8 0.3616 0.0850 −0.0665 0.068*
C9 0.30524 (18) 0.1733 (6) 0.01493 (19) 0.0498 (7)
H9 0.2643 0.3014 −0.0274 0.060*
C10 0.30542 (15) 0.1174 (5) 0.10235 (17) 0.0387 (6)
C11 0.18466 (15) 0.4573 (5) 0.07490 (17) 0.0399 (6)
H11 0.1832 0.5066 0.0175 0.048*
C12 0.06465 (15) 0.7953 (5) 0.04716 (18) 0.0396 (6)
C13 0.05037 (17) 0.8940 (6) −0.04079 (19) 0.0466 (7)
H13 0.0838 0.8227 −0.0685 0.056*
C14 −0.01402 (16) 1.0993 (6) −0.08723 (18) 0.0450 (6)
H14 −0.0233 1.1673 −0.1461 0.054*
O1W 0.1500 (2) 0.8211 (6) 0.3392 (2) 0.0919 (9)
H1A 0.160 (3) 0.978 (4) 0.317 (3) 0.110*
H1B 0.170 (3) 0.687 (5) 0.318 (3) 0.110*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
O1 0.0561 (12) 0.0580 (12) 0.0539 (12) 0.0074 (10) 0.0306 (10) 0.0081 (9)
N1 0.0396 (12) 0.0385 (11) 0.0463 (12) 0.0040 (10) 0.0177 (10) 0.0037 (10)
C1 0.0330 (13) 0.0333 (12) 0.0435 (14) −0.0026 (11) 0.0122 (11) −0.0004 (11)
C2 0.0396 (14) 0.0392 (14) 0.0462 (15) −0.0029 (12) 0.0193 (13) 0.0003 (12)
C3 0.0490 (16) 0.0481 (15) 0.0434 (15) 0.0008 (13) 0.0156 (13) 0.0080 (12)
C4 0.0414 (15) 0.0442 (15) 0.0511 (16) 0.0031 (13) 0.0097 (13) 0.0079 (13)
C5 0.0323 (13) 0.0402 (13) 0.0495 (15) −0.0007 (11) 0.0124 (12) −0.0009 (12)
C6 0.0394 (15) 0.0461 (16) 0.0653 (19) 0.0066 (12) 0.0166 (14) 0.0016 (14)
C7 0.0535 (18) 0.0555 (17) 0.074 (2) 0.0034 (15) 0.0361 (17) −0.0068 (16)
C8 0.0609 (19) 0.0574 (18) 0.0573 (18) 0.0021 (15) 0.0309 (16) −0.0027 (14)
C9 0.0511 (17) 0.0498 (16) 0.0480 (16) 0.0090 (13) 0.0214 (14) 0.0045 (12)
C10 0.0345 (13) 0.0333 (12) 0.0442 (14) −0.0025 (11) 0.0138 (11) −0.0025 (11)
C11 0.0373 (14) 0.0352 (13) 0.0449 (14) −0.0005 (11) 0.0162 (12) −0.0029 (11)
C12 0.0365 (14) 0.0328 (13) 0.0451 (14) 0.0008 (11) 0.0142 (12) −0.0017 (11)
C13 0.0433 (15) 0.0454 (14) 0.0536 (16) 0.0058 (13) 0.0238 (13) 0.0002 (13)
C14 0.0454 (15) 0.0457 (14) 0.0427 (14) 0.0052 (13) 0.0185 (13) 0.0039 (12)
O1W 0.113 (2) 0.0952 (18) 0.0958 (19) 0.0004 (18) 0.0719 (17) 0.0129 (17)

Geometric parameters (Å, °)

O1—C2 1.277 (3) C6—H6 0.9300
N1—C11 1.322 (3) C7—C8 1.378 (4)
N1—C12 1.412 (3) C7—H7 0.9300
N1—H1 0.8600 C8—C9 1.357 (4)
C1—C11 1.392 (3) C8—H8 0.9300
C1—C2 1.440 (3) C9—C10 1.414 (4)
C1—C10 1.452 (3) C9—H9 0.9300
C2—C3 1.437 (3) C11—H11 0.9300
C3—C4 1.345 (4) C12—C13 1.383 (4)
C3—H3 0.9300 C13—C14 1.383 (4)
C4—C5 1.431 (4) C13—H13 0.9300
C4—H4 0.9300 C14—H14 0.9300
C5—C6 1.404 (4) O1W—H1A 0.836 (10)
C5—C10 1.419 (3) O1W—H1B 0.831 (10)
C6—C7 1.353 (4)
C11—N1—C12 127.8 (2) C6—C7—C8 119.2 (3)
C11—N1—H1 116.1 C6—C7—H7 120.4
C12—N1—H1 116.1 C8—C7—H7 120.4
C11—C1—C2 119.8 (2) C9—C8—C7 121.9 (3)
C11—C1—C10 120.7 (2) C9—C8—H8 119.1
C2—C1—C10 119.5 (2) C7—C8—H8 119.1
O1—C2—C3 119.5 (2) C8—C9—C10 121.3 (3)
O1—C2—C1 122.1 (2) C8—C9—H9 119.4
C3—C2—C1 118.4 (2) C10—C9—H9 119.4
C4—C3—C2 121.2 (2) C9—C10—C5 116.3 (2)
C4—C3—H3 119.4 C9—C10—C1 123.9 (2)
C2—C3—H3 119.4 C5—C10—C1 119.8 (2)
C3—C4—C5 122.8 (2) N1—C11—C1 122.8 (2)
C3—C4—H4 118.6 N1—C11—H11 118.6
C5—C4—H4 118.6 C1—C11—H11 118.6
C6—C5—C10 120.3 (2) C13—C12—N1 122.9 (2)
C6—C5—C4 121.3 (2) C12—C13—C14 119.5 (2)
C10—C5—C4 118.4 (2) C12—C13—H13 120.2
C7—C6—C5 121.1 (3) C14—C13—H13 120.2
C7—C6—H6 119.4 C13—C14—H14 119.6
C5—C6—H6 119.4 H1A—O1W—H1B 103 (2)
C11—C1—C2—O1 2.0 (4) C8—C9—C10—C1 179.3 (2)
C10—C1—C2—O1 −178.9 (2) C6—C5—C10—C9 1.3 (4)
C11—C1—C2—C3 −178.5 (2) C4—C5—C10—C9 −178.7 (2)
C10—C1—C2—C3 0.6 (3) C6—C5—C10—C1 −178.9 (2)
O1—C2—C3—C4 179.6 (2) C4—C5—C10—C1 1.1 (3)
C1—C2—C3—C4 0.0 (4) C11—C1—C10—C9 −2.3 (4)
C2—C3—C4—C5 −0.1 (4) C2—C1—C10—C9 178.6 (2)
C3—C4—C5—C6 179.6 (3) C11—C1—C10—C5 177.9 (2)
C3—C4—C5—C10 −0.5 (4) C2—C1—C10—C5 −1.2 (3)
C10—C5—C6—C7 −0.7 (4) C12—N1—C11—C1 −179.9 (2)
C4—C5—C6—C7 179.3 (3) C2—C1—C11—N1 −0.9 (3)
C5—C6—C7—C8 −0.3 (4) C10—C1—C11—N1 −179.9 (2)
C6—C7—C8—C9 0.7 (4) C11—N1—C12—C13 1.3 (4)
C7—C8—C9—C10 −0.1 (4) N1—C12—C13—C14 179.8 (2)
C8—C9—C10—C5 −0.9 (4)

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
N1—H1···O1 0.86 1.86 2.560 (3) 138
O1W—H1B···O1 0.83 2.27 3.090 (4) 169
O1W—H1A···O1i 0.84 2.01 2.826 (4) 165
C13—H13···O1Wii 0.93 2.33 3.247 (5) 170

Symmetry codes: (i) x, y+1, z; (ii) x, −y+3/2, z−1/2.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: KP2357).

References

  1. Blagus, A., Cinčić, D., Friščić, T., Kaitner, B. & Stilinović, V. (2010). Maced. J. Chem. Chem. Eng. 29, 117–138.
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  5. Friščić, T., Kaitner, B. & Meštrović, E. (1998). Croat. Chem. Acta, 71, 87–98.
  6. Gavranić, M., Kaitner, B. & Meštrović, E. (1996). J. Chem. Crystallogr. 26, 23–28.
  7. Inabe, T., Luneau, I., Mitani, T., Maruyama, Y. & Takeda, S. (1994). Bull. Chem. Soc. Jpn, 67, 612–621.
  8. Macrae, C. F., Edgington, P. R., McCabe, P., Pidcock, E., Shields, G. P., Taylor, R., Towler, M. & van de Streek, J. (2006). J. Appl. Cryst. 39, 453–457.
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  10. Oxford Diffraction (2003). CrysAlis CCD and CrysAlis RED Oxford Diffraction Ltd, Wrocław, Poland.
  11. Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]

Associated Data

This section collects any data citations, data availability statements, or supplementary materials included in this article.

Supplementary Materials

Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536811041870/kp2357sup1.cif

e-67-o2958-sup1.cif (16.4KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811041870/kp2357Isup2.hkl

e-67-o2958-Isup2.hkl (119.1KB, hkl)

Supplementary material file. DOI: 10.1107/S1600536811041870/kp2357Isup3.cml

Additional supplementary materials: crystallographic information; 3D view; checkCIF report


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