Abstract
The title compound, C15H15NO3, adopts the enol–imine tautomeric form. The two rings are twisted with respect to each other, making a dihedral angle of 44.08 (5)°. The 3-methoxy-2-[(E)-(4-methoxyphenyl)-iminomethyl]phenol unit is almost planar, the largest deviation from the mean plane being 0.047 (2) Å. Such a planar conformation might be related to the occurrence of an intramolecular O—H⋯N hydrogen bond. In the crystal, intermolecular C—H⋯O hydrogen bonds link the molecules into sheets parallel to (010). These sheets are interconnected by weak C—H⋯π interactions.
Related literature
For background to the properties and uses of Schiff bases, see: Barton & Ollis (1979 ▶); Layer (1963 ▶); Ingold (1969 ▶); Cohen et al. (1964 ▶); Taggi et al. (2002 ▶). For hydrogen-bond motifs, see: Etter et al. (1990 ▶); Bernstein et al. (1995 ▶). For related structures, see: Özdemir Tarı et al. (2010 ▶); Şahin et al. (2005 ▶).
Experimental
Crystal data
C15H15NO3
M r = 257.28
Monoclinic,
a = 14.2658 (8) Å
b = 14.1553 (11) Å
c = 6.5893 (17) Å
β = 96.398 (9)°
V = 1322.3 (4) Å3
Z = 4
Mo Kα radiation
μ = 0.09 mm−1
T = 293 K
0.65 × 0.32 × 0.14 mm
Data collection
Stoe IPDS 2 diffractometer
Absorption correction: integration (X-RED32; Stoe, 2002) ▶ T min = 0.991, T max = 0.997
7244 measured reflections
2585 independent reflections
1622 reflections with I > 2σ(I)
R int = 0.032
Refinement
R[F 2 > 2σ(F 2)] = 0.053
wR(F 2) = 0.122
S = 1.04
2585 reflections
172 parameters
H-atom parameters constrained
Δρmax = 0.11 e Å−3
Δρmin = −0.19 e Å−3
Data collection: X-AREA (Stoe, 2002) ▶; cell refinement: X-AREA ▶; data reduction: X-RED32 (Stoe, 2002 ▶); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: ORTEPIII (Burnett & Johnson, 1996 ▶), ORTEP-3 for Windows (Farrugia, 1997 ▶) and PLATON (Spek, 2009 ▶); software used to prepare material for publication: SHELXL97.
Supplementary Material
Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536811000596/dn2646sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536811000596/dn2646Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report
Table 1. Hydrogen-bond geometry (Å, °).
Cg1 is the centroid of the C1—C6 ring.
| D—H⋯A | D—H | H⋯A | D⋯A | D—H⋯A |
|---|---|---|---|---|
| C13—H13⋯O2i | 0.93 | 2.60 | 3.428 (3) | 149 |
| C14—H14A⋯O1ii | 0.96 | 2.49 | 3.412 (3) | 162 |
| O2—H2A⋯N1 | 0.82 | 1.87 | 2.590 (2) | 146 |
| C5—H5⋯Cg1iii | 0.93 | 2.80 | 3.486 (2) | 132 |
Symmetry codes: (i)
; (ii)
; (iii)
.
Acknowledgments
The authors acknowledge the Faculty of Arts and Sciences, Ondokuz Mayıs University, Turkey, for the use of the Stoe IPDS 2 diffractometer (purchased under grant No. F279 of the University Research Fund).
supplementary crystallographic information
Comment
Schiff bases are used as starting materials in the synthesis of important drugs, such as antibiotics and antiallergic, antiphlogistic, and antitumor substances (Barton et al., 1979; Layer, 1963; Ingold 1969). On the industrial scale, they have a wide range of applications, such as dyes and pigments (Taggi et al., 2002). There are two characteristic properties of Schiff bases, viz. Photochromism and thermochromism (Cohen et al., 1964). In general, Schiff bases display two possible tautomeric forms, the phenol-imine (OH) and the keto-amine (NH) forms. Depending on the tautomers, two types of intramolecular hydrogen bonds are observed in Schiff bases: O—H···N in phenol-imine (Özdemir Tarı et al., 2010) and N—H···O in keto-amine tautomers (Şahin et al., 2005). Another form of the Schiff base compounds is also known as zwitterion having an ionic intramolecular hydrogen bond (N+—H···O-) and this form is rarely seen in the solid state (Özdemir Tarı et al., 2010).
The title compound, C15H15O3N1, adopts the enol-imine tautomeric form. The C7=N1 [1.278 (3) Å] and C8=N1 [1.419 (2) Å] bond distances are of double-bond character, whereas, C6—O2 [1.356 (2) Å] distance is single bond. These distances are similar to that reported in the literature [1.269 (8) Å] and [1.397 (7) Å] for C=N and [1.332 (8) Å] for C—O respectively (Özdemir Tarı et al., 2010).
The two phenyl rings are twisted with respect to each other making dihedral angle of 44.08 (5)° (Fig. 1). The 4-methoxyphenylimino)phenol moiety is planar with the largest deviation from the mean plane being 0.047 (2)Å at C7. Such planar conformation might be related to the occurrence of the O—H···N intramolecular hydrogen bond (Fig. 1, Table 1). This intramolecular N—H···O hydrogen bond results in the formation of an S(6) ring (Etter et al., 1990; Bernstein et al., 1995).
Intermolecular C—H···O hydrogen bonds link the molecules forming sheets parallel to the (0 1 0) plane (Fig. 2, Table 1). These sheets are interconnected by weak C—H···π interactions (Table 1, Cg1 is the centroid of the C1—C6 phenyl ring).
Experimental
(E)-3-methoxy-2-((4-methoxyphenylimino)methyl)phenol was prepared by refluxing a mixture of a solution containing 2-hydroxy-6- methoxybenzaldehyde (15.2 mg, o.1 mmol) in ethanol (30 ml) and a solution containing 4-methoxyaniline (12.3 mg, 0.1 mmol) in ethanol (20 ml). The reaction mixture was stirred for 2 h under reflux. Single crystals of the title compound for x-ray analysis were obtained by slow evaporation of an ethanol solution (yield 72%; m.p 346–348 K).
Figures
Fig. 1.
The molecular structure of the title compound, showing the atom-numbering scheme Displacement ellipsoids are drawn at the 30% probability level. H atoms are represented as small sphere of arbitrary radii. Intramolecular H bond is shown as dashed line.
Fig. 2.
The crystal packing of the title compound showing the formation of sheets parallel to the (0 1 0) plane. H bonds are shown as dashed lines. H atoms not involved in hydrogen bonding have been omitted for clarity.
Crystal data
| C15H15NO3 | F(000) = 544 |
| Mr = 257.28 | Dx = 1.292 Mg m−3 |
| Monoclinic, P21/c | Mo Kα radiation, λ = 0.71073 Å |
| Hall symbol: -P 2ybc | Cell parameters from 12079 reflections |
| a = 14.2658 (8) Å | θ = 1.4–27.2° |
| b = 14.1553 (11) Å | µ = 0.09 mm−1 |
| c = 6.5893 (17) Å | T = 293 K |
| β = 96.398 (9)° | Prism, brown |
| V = 1322.3 (4) Å3 | 0.65 × 0.32 × 0.14 mm |
| Z = 4 |
Data collection
| Stoe IPDS 2 diffractometer | 2585 independent reflections |
| Radiation source: fine-focus sealed tube | 1622 reflections with I > 2σ(I) |
| graphite | Rint = 0.032 |
| Detector resolution: 6.67 pixels mm-1 | θmax = 26.0°, θmin = 1.4° |
| φ scan rotation method | h = −16→17 |
| Absorption correction: integration (X-RED32; Stoe, 2002) | k = −17→17 |
| Tmin = 0.991, Tmax = 0.997 | l = −8→6 |
| 7244 measured reflections |
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)] = 0.053 | Hydrogen site location: inferred from neighbouring sites |
| wR(F2) = 0.122 | H-atom parameters constrained |
| S = 1.04 | w = 1/[σ2(Fo2) + (0.0524P)2 + 0.1038P] where P = (Fo2 + 2Fc2)/3 |
| 2585 reflections | (Δ/σ)max < 0.001 |
| 172 parameters | Δρmax = 0.11 e Å−3 |
| 0 restraints | Δρmin = −0.19 e Å−3 |
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 | ||
| C1 | 0.20529 (13) | 0.11619 (13) | 0.4013 (3) | 0.0443 (5) | |
| C2 | 0.29338 (14) | 0.10131 (14) | 0.3295 (3) | 0.0483 (5) | |
| H2 | 0.2959 | 0.0793 | 0.1972 | 0.058* | |
| C3 | 0.37566 (14) | 0.11898 (15) | 0.4526 (3) | 0.0516 (5) | |
| C4 | 0.37125 (16) | 0.15062 (15) | 0.6515 (3) | 0.0548 (6) | |
| H4 | 0.4268 | 0.1626 | 0.7353 | 0.066* | |
| C5 | 0.28635 (16) | 0.16440 (15) | 0.7254 (3) | 0.0542 (6) | |
| H5 | 0.2848 | 0.1854 | 0.8588 | 0.065* | |
| C6 | 0.20294 (15) | 0.14735 (14) | 0.6034 (3) | 0.0479 (5) | |
| C7 | 0.11923 (14) | 0.10451 (13) | 0.2639 (3) | 0.0481 (5) | |
| H7 | 0.1229 | 0.0900 | 0.1274 | 0.058* | |
| C8 | −0.04619 (13) | 0.11307 (14) | 0.1930 (3) | 0.0459 (5) | |
| C9 | −0.12676 (15) | 0.07751 (15) | 0.2668 (4) | 0.0544 (6) | |
| H9 | −0.1226 | 0.0522 | 0.3977 | 0.065* | |
| C10 | −0.21198 (15) | 0.07926 (15) | 0.1495 (4) | 0.0553 (6) | |
| H10 | −0.2648 | 0.0535 | 0.1995 | 0.066* | |
| C11 | −0.22005 (14) | 0.11941 (14) | −0.0446 (4) | 0.0512 (5) | |
| C12 | −0.14058 (15) | 0.15559 (16) | −0.1200 (4) | 0.0561 (6) | |
| H12 | −0.1452 | 0.1823 | −0.2497 | 0.067* | |
| C13 | −0.05435 (15) | 0.15172 (15) | −0.0012 (3) | 0.0537 (6) | |
| H13 | −0.0010 | 0.1755 | −0.0526 | 0.064* | |
| C14 | −0.3216 (2) | 0.1629 (2) | −0.3428 (5) | 0.0908 (9) | |
| H14A | −0.3868 | 0.1590 | −0.3970 | 0.136* | |
| H14B | −0.2837 | 0.1297 | −0.4310 | 0.136* | |
| H14C | −0.3026 | 0.2280 | −0.3338 | 0.136* | |
| C15 | 0.47450 (18) | 0.0772 (2) | 0.1985 (4) | 0.0881 (9) | |
| H15A | 0.5402 | 0.0742 | 0.1795 | 0.132* | |
| H15B | 0.4427 | 0.1196 | 0.1000 | 0.132* | |
| H15C | 0.4472 | 0.0153 | 0.1810 | 0.132* | |
| N1 | 0.03849 (12) | 0.11390 (12) | 0.3283 (3) | 0.0496 (4) | |
| O1 | 0.46496 (10) | 0.10987 (13) | 0.3953 (3) | 0.0752 (5) | |
| O2 | 0.12069 (11) | 0.16290 (11) | 0.6830 (2) | 0.0636 (5) | |
| H2A | 0.0763 | 0.1500 | 0.5975 | 0.095* | |
| O3 | −0.30930 (10) | 0.12168 (12) | −0.1453 (3) | 0.0662 (5) |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| C1 | 0.0417 (11) | 0.0426 (10) | 0.0480 (12) | −0.0004 (9) | 0.0020 (9) | −0.0004 (9) |
| C2 | 0.0481 (12) | 0.0525 (12) | 0.0439 (12) | 0.0043 (9) | 0.0032 (10) | −0.0031 (9) |
| C3 | 0.0418 (11) | 0.0593 (12) | 0.0524 (13) | 0.0040 (10) | 0.0000 (10) | 0.0011 (10) |
| C4 | 0.0537 (14) | 0.0603 (13) | 0.0475 (13) | −0.0011 (10) | −0.0073 (11) | −0.0002 (10) |
| C5 | 0.0630 (15) | 0.0575 (13) | 0.0412 (12) | 0.0010 (10) | 0.0017 (11) | −0.0042 (10) |
| C6 | 0.0494 (13) | 0.0472 (11) | 0.0487 (13) | 0.0010 (9) | 0.0117 (10) | 0.0013 (9) |
| C7 | 0.0468 (12) | 0.0484 (11) | 0.0494 (12) | 0.0000 (9) | 0.0059 (10) | −0.0025 (9) |
| C8 | 0.0401 (11) | 0.0430 (11) | 0.0551 (13) | −0.0016 (9) | 0.0075 (10) | −0.0027 (9) |
| C9 | 0.0480 (13) | 0.0570 (13) | 0.0586 (14) | −0.0036 (10) | 0.0080 (11) | 0.0085 (11) |
| C10 | 0.0406 (12) | 0.0562 (13) | 0.0706 (15) | −0.0078 (10) | 0.0127 (11) | 0.0063 (11) |
| C11 | 0.0404 (11) | 0.0493 (11) | 0.0632 (14) | −0.0021 (9) | 0.0025 (10) | −0.0071 (11) |
| C12 | 0.0519 (13) | 0.0645 (14) | 0.0516 (13) | −0.0045 (10) | 0.0046 (11) | 0.0036 (10) |
| C13 | 0.0402 (12) | 0.0667 (13) | 0.0548 (14) | −0.0061 (10) | 0.0086 (10) | 0.0042 (11) |
| C14 | 0.0623 (17) | 0.125 (3) | 0.079 (2) | −0.0102 (16) | −0.0186 (15) | 0.0173 (18) |
| C15 | 0.0519 (15) | 0.142 (3) | 0.0722 (18) | 0.0053 (15) | 0.0146 (14) | −0.0252 (18) |
| N1 | 0.0409 (10) | 0.0518 (10) | 0.0561 (11) | −0.0028 (8) | 0.0057 (8) | 0.0023 (8) |
| O1 | 0.0402 (9) | 0.1206 (15) | 0.0637 (11) | 0.0052 (9) | 0.0009 (8) | −0.0167 (10) |
| O2 | 0.0557 (9) | 0.0812 (11) | 0.0560 (10) | 0.0037 (8) | 0.0157 (8) | −0.0081 (8) |
| O3 | 0.0417 (9) | 0.0795 (11) | 0.0749 (11) | −0.0074 (7) | −0.0055 (8) | 0.0016 (9) |
Geometric parameters (Å, °)
| C1—C6 | 1.407 (3) | C9—H9 | 0.9300 |
| C1—C2 | 1.407 (3) | C10—C11 | 1.393 (3) |
| C1—C7 | 1.451 (3) | C10—H10 | 0.9300 |
| C2—C3 | 1.373 (3) | C11—O3 | 1.369 (2) |
| C2—H2 | 0.9300 | C11—C12 | 1.386 (3) |
| C3—O1 | 1.375 (3) | C12—C13 | 1.384 (3) |
| C3—C4 | 1.393 (3) | C12—H12 | 0.9300 |
| C4—C5 | 1.369 (3) | C13—H13 | 0.9300 |
| C4—H4 | 0.9300 | C14—O3 | 1.419 (3) |
| C5—C6 | 1.381 (3) | C14—H14A | 0.9600 |
| C5—H5 | 0.9300 | C14—H14B | 0.9600 |
| C6—O2 | 1.356 (2) | C14—H14C | 0.9600 |
| C7—N1 | 1.278 (3) | C15—O1 | 1.397 (3) |
| C7—H7 | 0.9300 | C15—H15A | 0.9600 |
| C8—C13 | 1.385 (3) | C15—H15B | 0.9600 |
| C8—C9 | 1.391 (3) | C15—H15C | 0.9600 |
| C8—N1 | 1.419 (2) | O2—H2A | 0.8200 |
| C9—C10 | 1.366 (3) | ||
| C6—C1—C2 | 118.79 (19) | C9—C10—H10 | 119.9 |
| C6—C1—C7 | 121.21 (19) | C11—C10—H10 | 119.9 |
| C2—C1—C7 | 119.91 (19) | O3—C11—C12 | 124.9 (2) |
| C3—C2—C1 | 120.7 (2) | O3—C11—C10 | 115.58 (18) |
| C3—C2—H2 | 119.6 | C12—C11—C10 | 119.5 (2) |
| C1—C2—H2 | 119.6 | C13—C12—C11 | 119.6 (2) |
| C2—C3—O1 | 125.3 (2) | C13—C12—H12 | 120.2 |
| C2—C3—C4 | 119.3 (2) | C11—C12—H12 | 120.2 |
| O1—C3—C4 | 115.40 (19) | C12—C13—C8 | 121.1 (2) |
| C5—C4—C3 | 121.0 (2) | C12—C13—H13 | 119.5 |
| C5—C4—H4 | 119.5 | C8—C13—H13 | 119.5 |
| C3—C4—H4 | 119.5 | O3—C14—H14A | 109.5 |
| C4—C5—C6 | 120.4 (2) | O3—C14—H14B | 109.5 |
| C4—C5—H5 | 119.8 | H14A—C14—H14B | 109.5 |
| C6—C5—H5 | 119.8 | O3—C14—H14C | 109.5 |
| O2—C6—C5 | 118.21 (18) | H14A—C14—H14C | 109.5 |
| O2—C6—C1 | 122.03 (19) | H14B—C14—H14C | 109.5 |
| C5—C6—C1 | 119.75 (19) | O1—C15—H15A | 109.5 |
| N1—C7—C1 | 120.8 (2) | O1—C15—H15B | 109.5 |
| N1—C7—H7 | 119.6 | H15A—C15—H15B | 109.5 |
| C1—C7—H7 | 119.6 | O1—C15—H15C | 109.5 |
| C13—C8—C9 | 118.6 (2) | H15A—C15—H15C | 109.5 |
| C13—C8—N1 | 123.71 (18) | H15B—C15—H15C | 109.5 |
| C9—C8—N1 | 117.54 (19) | C7—N1—C8 | 121.78 (19) |
| C10—C9—C8 | 120.9 (2) | C3—O1—C15 | 118.36 (18) |
| C10—C9—H9 | 119.6 | C6—O2—H2A | 109.5 |
| C8—C9—H9 | 119.6 | C11—O3—C14 | 117.85 (19) |
| C9—C10—C11 | 120.29 (19) | ||
| C6—C1—C2—C3 | −1.5 (3) | N1—C8—C9—C10 | 176.32 (19) |
| C7—C1—C2—C3 | 175.00 (19) | C8—C9—C10—C11 | −1.9 (3) |
| C1—C2—C3—O1 | −177.7 (2) | C9—C10—C11—O3 | −176.91 (19) |
| C1—C2—C3—C4 | 1.0 (3) | C9—C10—C11—C12 | 1.5 (3) |
| C2—C3—C4—C5 | −0.1 (3) | O3—C11—C12—C13 | 178.0 (2) |
| O1—C3—C4—C5 | 178.7 (2) | C10—C11—C12—C13 | −0.3 (3) |
| C3—C4—C5—C6 | −0.2 (3) | C11—C12—C13—C8 | −0.6 (3) |
| C4—C5—C6—O2 | −179.4 (2) | C9—C8—C13—C12 | 0.3 (3) |
| C4—C5—C6—C1 | −0.4 (3) | N1—C8—C13—C12 | −174.7 (2) |
| C2—C1—C6—O2 | −179.81 (18) | C1—C7—N1—C8 | 172.99 (18) |
| C7—C1—C6—O2 | 3.7 (3) | C13—C8—N1—C7 | −36.1 (3) |
| C2—C1—C6—C5 | 1.2 (3) | C9—C8—N1—C7 | 148.9 (2) |
| C7—C1—C6—C5 | −175.24 (19) | C2—C3—O1—C15 | −2.2 (4) |
| C6—C1—C7—N1 | −6.4 (3) | C4—C3—O1—C15 | 179.1 (2) |
| C2—C1—C7—N1 | 177.11 (18) | C12—C11—O3—C14 | 0.9 (3) |
| C13—C8—C9—C10 | 1.0 (3) | C10—C11—O3—C14 | 179.2 (2) |
Hydrogen-bond geometry (Å, °)
| Cg1 is the centroid of the C1—C6 ring. |
| D—H···A | D—H | H···A | D···A | D—H···A |
| C13—H13···O2i | 0.93 | 2.60 | 3.428 (3) | 149 |
| C14—H14A···O1ii | 0.96 | 2.49 | 3.412 (3) | 162 |
| O2—H2A···N1 | 0.82 | 1.87 | 2.590 (2) | 146 |
| C5—H5···Cg1iii | 0.93 | 2.80 | 3.486 (2) | 132 |
Symmetry codes: (i) x, y, z−1; (ii) x−1, y, z−1; (iii) x, −y−1/2, z−1/2.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: DN2646).
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/S1600536811000596/dn2646sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536811000596/dn2646Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report


