Literature DB >> 29765714

Synthesis, crystal structure and computational studies of a new Schiff base compound: (E)-4-bromo-2-eth-oxy-6-{[(2-meth-oxy-phen-yl)imino]meth-yl}phenol.

Arzu Özek Yıldırım1, Murat Gülsu1, Çiğdem Albayrak Kaştaş2.   

Abstract

The title compound, C16H16BrNO3, which shows enol-imine tautomerism, crystallizes in the monoclinic P21/c space group. All non-H atoms of the mol-ecule are nearly coplanar, with a maximum deviation of 0.274 (3) Å. In the crystal, mol-ecules are held together by weak C-H⋯O, π-π and C-H⋯π inter-actions. The E/Z isomerism and enol/keto tautomerism energy barriers of the compound have been calculated by relaxed potential energy surface scan calculations with DFT methods. To observe the changes in the aromatic ring, HOMA aromaticity indexes were calculated during the scan process. Total energy and HOMA change curves were obtained to visualize results of the scan calculations.

Entities:  

Keywords:  2-meth­oxy­aniline; 5-bromo-3-eth­oxy-2-hy­droxy­benzaldehyde; DFT; Schiff bas; crystal structure

Year:  2018        PMID: 29765714      PMCID: PMC5947794          DOI: 10.1107/S2056989018002062

Source DB:  PubMed          Journal:  Acta Crystallogr E Crystallogr Commun


Chemical context

The synthesis and chemistry of Schiff bases have received considerable attention over the last several decades, primarily owing to their remarkable potential pharmacological (Hu et al., 2012 ▸), anti-tumor (Kamel et al., 2010 ▸) and biological properties (Lozier et al., 1975 ▸). Furthermore, Schiff bases can display photo-chromic and thermo-chromic effect (Hadjoudis & Mavridis, 2004 ▸). These effects depend on the prototropic tautomerism and mol­ecular planarity in Schiff bases (Moustakali-Mavridis et al., 1978 ▸; Hadjoudis et al., 1987 ▸). Prototropic tautomerism emerges from the intra­molecular H-atom transfer between an enolimine (Özdemir Tarı et al., 2016 ▸) and a keto–amine tautomer (Özek et al., 2006 ▸). The present work is part of our ongoing studies on Schiff bases (Özek Yıldırım et al., 2016 ▸, 2017 ▸; Albayrak et al., 2012 ▸). We report herein the synthesis, crystal structure and computational studies of the title compound, (E)-4-bromo-2-eth­oxy-6-{[(2-meth­oxy­phen­yl)imino]­meth­yl}phenol, obtained from the condensation of 5-bromo-3-eth­oxy-2-hy­droxy­benzaldehyde with 2-meth­oxy­aniline.

Structural commentary

Fig. 1 ▸ represents the mol­ecular structure of the title compound. All non-H atoms lie in the plane formed by the aromatic rings with a maximum deviation of 0.274 (3) Å. The dihedral angle between the aromatic rings C1–C6 and C10–C15 is 2.25 (13)°. In the chelate moiety, which comprises atoms C1, C2, O1, H1, N1 and C9, C9=N1 [1.281 (3)] is a typical double bond while C2—O1 [1.333 (3)] is a typical single bond; these are similar to those in related structures (Petek et al., 2010 ▸; Gül et al., 2007 ▸). The harmonic oscillator model of aromaticity (HOMA; Kruszewski & Krygowski, 1972 ▸) values were calculated [0.88 for C1–C6 and 0.98 for the C10–C15 ring] to observe the effect of substituent groups on the rings. There are no significant deformations of the rings when compared to those in (E)-2-eth­oxy-6-[(2-meth­oxy­phenyl­imino)­meth­yl]phenol (Petek et al., 2010 ▸). The chelate moiety forms an S(6) graph-set motif through a strong intra­molecular O1—H1⋯N1 hydrogen bond (Table 1 ▸).
Figure 1

The mol­ecular structure of the title compound, with atom labels and 50% probability displacement ellipsoids for non-H atoms. The dashed line indicates the intra­molecular hydrogen bond.

Table 1

Hydrogen-bond geometry (Å, °)

Cg1 and Cg2 are the centroids of the C1–C6 and C10–C15 rings, respectively.

D—H⋯A D—HH⋯A DA D—H⋯A
O1—H1⋯N10.81 (5)1.80 (5)2.566 (3)157 (5)
C16—H16A⋯O1i 0.962.553.293 (3)135
C7—H7ACg1ii 0.972.803.662 (3)149
C13—H13⋯Cg2iii 0.932.793.629 (3)150

Symmetry codes: (i) ; (ii) ; (iii) .

Supra­molecular features

In the crystal, inversion dimers with an motif are generated by the weak C16—H16A⋯O1(−x + 1, −y, −z + 1) hydrogen bonds (Table 1 ▸). As shown in Fig. 2 ▸, these dimers are connected to each other by π–π inter­actions [Cg1⋯Cg2(x, y + 1, z) = 3.6237 (16) Å; Cg1 and Cg2 are the centroids of the C1–C6 and C10–C15 rings, respectively]. C—H⋯π inter­actions (Table 1 ▸) generate zigzag chains along the [100] direction as shown in Fig. 3 ▸.
Figure 2

View of the inversion dimers, which are connected by π–π inter­actions, propagating along the c-axis direction. [Symmetry codes: (i) −x + 1, −y, −z + 1; (ii) x, y + 1, z; (iii) x, y − 1, z; (iv) −x + 1, −y + 1, −z + 1; (v) −x + 1, −y + 2, −z + 1.]

Figure 3

The packing, viewed down the c axis, showing mol­ecules connected by C—H⋯π inter­actions [Symmetry codes: (i) −x + , y + , −z + ; (ii) −x + , y − , −z + ; (iii) −x + , y + , −z + ; (iv) x, y + 1, z; (v) x − 1, y, z; (vi) −x + , y − , −z + ; (vii) x + 1, y, z.]

Computational Studies

Relaxed potential energy surface scan calculations were performed using the DFT/B3LYP/6-311G++(d,p) method with Gaussian 09W software (Frisch et al., 2009 ▸) to investigate the connection between the mol­ecular conformation and physical properties of a Schiff base. The results of a torsional angle scan and a proton-transfer scan on the O—H⋯N pathway are given in Fig. 4 ▸. The torsional barrier between the E/Z isomers was found to be 1.94 kcal mol−1 and the enol–keto tautomerism barrier was 1.92 kcal mol−1. The effects of the conformational changes on the aromatic ring can be visualized by calculating HOMA values during the scan calculations. Fig. 5 ▸ a shows that changes in the HOMA indices are very limited with an average fluctuation of 2%. As can be seen in Fig. 5 ▸ b, the aromaticity of the C1–C6 ring depends strongly on the prototropic tautomerism.
Figure 4

The potential energy curves for the torsional scan (a) and the O—H bond scan (b). Relative energies are calculated with respect to the global minimum of each curve.

Figure 5

Graphics showing the variation of HOMA values with scan coordinate.

Database survey

A survey of the Cambridge Structural Database (CSD, Version 5.37, update May 2017; Groom et al., 2016 ▸) for the (E)-4-bromo-2-eth­oxy-6-[(methyl­imino)­meth­yl]phenol unit of the title compound reveals five compounds, viz. OCOVEK (Kaştaş et al., 2017a ▸), OCOVIO (Kaştaş et al., 2017b ▸), OCOVOU (Kaştaş et al., 2017c ▸), OCOVUA (Kaştaş et al., 2017d ▸) and LUWZIO (Özek Yıldırım et al., 2016 ▸). The mol­ecular structures of the latter two compounds are planar, in which they are similar to the title compound, while the others are not planar.

Synthesis and crystallization

The title compound was prepared by refluxing a mixture of a solution containing 5-bromo-3-eth­oxy-2-hy­droxy­benzaldehyde (0.5 g, 2 mmol) in 20 ml ethanol and a solution containing 2-meth­oxy­aniline (0.25 g, 2 mmol) in 20 ml ethanol. The reaction mixture was stirred for 1 h under reflux. Crystals suitable for X-ray analysis were obtained from an ethanol solution by slow evaporation (yield 70%).

Refinement

Crystal data, data collection and structure refinement details are summarized in Table 2 ▸. The hydroxyl atom H1 was refined freely. All the other H atoms were located geometrically and refined using a riding model with C—H = 0.93–0.97 Å U iso(H) = 1.2U eq(C).
Table 2

Experimental details

Crystal data
Chemical formulaC16H16BrNO3
M r 350.21
Crystal system, space groupMonoclinic, P21/n
Temperature (K)296
a, b, c (Å)15.3405 (8), 6.5204 (2), 15.3612 (10)
β (°)98.716 (5)
V3)1518.78 (14)
Z 4
Radiation typeMo Kα
μ (mm−1)2.72
Crystal size (mm)0.56 × 0.28 × 0.05
 
Data collection
DiffractometerStoe IPDS 2
Absorption correctionIntegration (X-RED32; Stoe & Cie, 2002)
T min, T max 0.437, 0.893
No. of measured, independent and observed [I > 2σ(I)] reflections18156, 3491, 2754
R int 0.042
(sin θ/λ)max−1)0.650
 
Refinement
R[F 2 > 2σ(F 2)], wR(F 2), S 0.042, 0.091, 1.06
No. of reflections3491
No. of parameters194
H-atom treatmentH atoms treated by a mixture of independent and constrained refinement
Δρmax, Δρmin (e Å−3)0.28, −0.38

Computer programs: X-AREA and X-RED32 (Stoe & Cie, 2002 ▸), SHELXS97 (Sheldrick, 2015 ▸), SHELXL2018 (Sheldrick, 2015 ▸), ORTEP-3 for Windows and WinGX (Farrugia, 2012 ▸) and PLATON (Spek, 2009 ▸).

Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S2056989018002062/xu5918sup1.cif Structure factors: contains datablock(s) I. DOI: 10.1107/S2056989018002062/xu5918Isup2.hkl Click here for additional data file. Supporting information file. DOI: 10.1107/S2056989018002062/xu5918Isup3.cml CCDC reference: 1457124 Additional supporting information: crystallographic information; 3D view; checkCIF report
C16H16BrNO3F(000) = 712
Mr = 350.21Dx = 1.532 Mg m3
Monoclinic, P21/nMo Kα radiation, λ = 0.71073 Å
a = 15.3405 (8) ÅCell parameters from 3491 reflections
b = 6.5204 (2) Åθ = 2.0–28.1°
c = 15.3612 (10) ŵ = 2.72 mm1
β = 98.716 (5)°T = 296 K
V = 1518.78 (14) Å3Prism, orange
Z = 40.56 × 0.28 × 0.05 mm
Stoe IPDS 2 diffractometer3491 independent reflections
Radiation source: sealed X-ray tube, 12 x 0.4 mm long-fine focus2754 reflections with I > 2σ(I)
Detector resolution: 6.67 pixels mm-1Rint = 0.042
rotation method scansθmax = 27.5°, θmin = 2.0°
Absorption correction: integration (X-RED32; Stoe & Cie, 2002)h = −19→19
Tmin = 0.437, Tmax = 0.893k = −8→8
18156 measured reflectionsl = −19→19
Refinement on F20 restraints
Least-squares matrix: fullHydrogen site location: mixed
R[F2 > 2σ(F2)] = 0.042H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.091w = 1/[σ2(Fo2) + (0.0398P)2 + 0.5265P] where P = (Fo2 + 2Fc2)/3
S = 1.06(Δ/σ)max = 0.001
3491 reflectionsΔρmax = 0.28 e Å3
194 parametersΔρmin = −0.38 e Å3
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.
xyzUiso*/Ueq
C10.44857 (16)0.3446 (4)0.18253 (15)0.0403 (5)
C20.42497 (17)0.3902 (4)0.26511 (16)0.0417 (5)
C30.37588 (17)0.5714 (4)0.27491 (17)0.0440 (6)
C40.35124 (17)0.6978 (4)0.20324 (18)0.0469 (6)
H40.3184140.8156700.2089190.056*
C50.37596 (17)0.6473 (4)0.12266 (17)0.0456 (6)
C60.42285 (18)0.4758 (4)0.11072 (16)0.0457 (6)
H60.4377770.4456190.0556740.055*
C70.3190 (2)0.7984 (4)0.3743 (2)0.0574 (7)
H7A0.2600450.8094070.3412910.069*
H7B0.3544880.9096690.3567340.069*
C80.3155 (2)0.8097 (5)0.4713 (2)0.0640 (8)
H8A0.2900870.9382480.4847270.077*
H8B0.2801270.6991940.4878960.077*
H8C0.3741710.7990320.5032740.077*
C90.50092 (17)0.1655 (4)0.17069 (16)0.0442 (5)
H90.5164280.1382170.1156200.053*
C100.57777 (16)−0.1337 (4)0.22892 (16)0.0406 (5)
C110.59676 (16)−0.2499 (4)0.30608 (16)0.0420 (5)
C120.64681 (19)−0.4279 (4)0.30608 (19)0.0513 (6)
H120.659509−0.5056560.3571940.062*
C130.67759 (18)−0.4892 (5)0.2304 (2)0.0550 (7)
H130.711082−0.6082170.2308570.066*
C140.6594 (2)−0.3766 (5)0.1542 (2)0.0552 (7)
H140.680358−0.4190050.1034320.066*
C150.60944 (19)−0.1994 (4)0.15371 (18)0.0508 (6)
H150.596978−0.1232320.1021300.061*
C160.5727 (2)−0.2971 (5)0.45460 (19)0.0622 (8)
H16A0.546330−0.2273720.4990900.075*
H16B0.544000−0.4268400.4418080.075*
H16C0.634215−0.3191900.4753760.075*
N10.52630 (14)0.0438 (3)0.23498 (13)0.0423 (5)
O10.44838 (15)0.2719 (3)0.33548 (12)0.0536 (5)
O20.35740 (14)0.6041 (3)0.35724 (12)0.0546 (5)
O30.56318 (14)−0.1756 (3)0.37679 (12)0.0558 (5)
Br10.34398 (2)0.82939 (5)0.02613 (2)0.06603 (13)
H10.479 (3)0.186 (8)0.316 (3)0.119 (18)*
U11U22U33U12U13U23
C10.0405 (12)0.0374 (12)0.0424 (12)−0.0003 (11)0.0041 (10)0.0031 (10)
C20.0433 (13)0.0374 (13)0.0443 (12)0.0007 (10)0.0064 (10)0.0027 (10)
C30.0429 (14)0.0415 (13)0.0483 (13)0.0002 (11)0.0092 (11)0.0009 (11)
C40.0441 (14)0.0383 (14)0.0583 (15)0.0045 (11)0.0081 (11)0.0060 (11)
C50.0446 (14)0.0415 (14)0.0493 (13)−0.0018 (11)0.0021 (11)0.0109 (11)
C60.0492 (14)0.0476 (15)0.0403 (12)0.0025 (12)0.0070 (11)0.0067 (11)
C70.0640 (18)0.0433 (16)0.0674 (18)0.0125 (13)0.0184 (14)0.0005 (13)
C80.074 (2)0.0519 (17)0.0698 (19)0.0103 (15)0.0230 (16)−0.0074 (15)
C90.0514 (14)0.0430 (13)0.0387 (12)−0.0004 (12)0.0087 (10)0.0010 (11)
C100.0404 (13)0.0363 (13)0.0458 (12)−0.0001 (10)0.0089 (10)0.0016 (10)
C110.0392 (13)0.0422 (13)0.0450 (12)−0.0001 (11)0.0080 (10)0.0031 (10)
C120.0491 (15)0.0465 (15)0.0576 (15)0.0062 (12)0.0061 (12)0.0089 (13)
C130.0458 (15)0.0433 (15)0.0764 (19)0.0074 (12)0.0106 (14)−0.0017 (14)
C140.0555 (17)0.0534 (17)0.0607 (16)0.0041 (13)0.0217 (13)−0.0073 (13)
C150.0580 (16)0.0498 (16)0.0475 (14)0.0037 (13)0.0170 (12)0.0037 (12)
C160.070 (2)0.070 (2)0.0473 (15)0.0027 (16)0.0107 (13)0.0152 (14)
N10.0467 (12)0.0375 (11)0.0436 (10)0.0035 (9)0.0092 (9)0.0030 (9)
O10.0730 (14)0.0473 (11)0.0425 (10)0.0160 (10)0.0152 (9)0.0081 (8)
O20.0703 (13)0.0445 (10)0.0519 (10)0.0137 (9)0.0184 (9)0.0025 (8)
O30.0709 (13)0.0559 (11)0.0434 (9)0.0145 (10)0.0176 (9)0.0106 (9)
Br10.0763 (2)0.05858 (19)0.06202 (19)0.01265 (16)0.00668 (14)0.02361 (15)
C1—C21.403 (3)C9—N11.281 (3)
C1—C61.405 (3)C9—H90.9300
C1—C91.444 (4)C10—C151.387 (4)
C2—O11.333 (3)C10—C111.400 (3)
C2—C31.421 (4)C10—N11.412 (3)
C3—O21.354 (3)C11—O31.360 (3)
C3—C41.381 (4)C11—C121.392 (4)
C4—C51.388 (4)C12—C131.379 (4)
C4—H40.9300C12—H120.9300
C5—C61.356 (4)C13—C141.373 (4)
C5—Br11.905 (2)C13—H130.9300
C6—H60.9300C14—C151.386 (4)
C7—O21.438 (3)C14—H140.9300
C7—C81.500 (4)C15—H150.9300
C7—H7A0.9700C16—O31.423 (3)
C7—H7B0.9700C16—H16A0.9600
C8—H8A0.9600C16—H16B0.9600
C8—H8B0.9600C16—H16C0.9600
C8—H8C0.9600O1—H10.81 (5)
C2—C1—C6120.0 (2)N1—C9—H9119.5
C2—C1—C9120.7 (2)C1—C9—H9119.5
C6—C1—C9119.3 (2)C15—C10—C11118.9 (2)
O1—C2—C1122.4 (2)C15—C10—N1125.3 (2)
O1—C2—C3118.5 (2)C11—C10—N1115.8 (2)
C1—C2—C3119.1 (2)O3—C11—C12125.0 (2)
O2—C3—C4125.4 (2)O3—C11—C10115.3 (2)
O2—C3—C2114.8 (2)C12—C11—C10119.7 (2)
C4—C3—C2119.8 (2)C13—C12—C11120.1 (3)
C3—C4—C5119.4 (2)C13—C12—H12120.0
C3—C4—H4120.3C11—C12—H12120.0
C5—C4—H4120.3C14—C13—C12120.8 (3)
C6—C5—C4122.6 (2)C14—C13—H13119.6
C6—C5—Br1119.2 (2)C12—C13—H13119.6
C4—C5—Br1118.23 (19)C13—C14—C15119.5 (3)
C5—C6—C1119.2 (2)C13—C14—H14120.3
C5—C6—H6120.4C15—C14—H14120.3
C1—C6—H6120.4C14—C15—C10121.1 (3)
O2—C7—C8107.6 (2)C14—C15—H15119.5
O2—C7—H7A110.2C10—C15—H15119.5
C8—C7—H7A110.2O3—C16—H16A109.5
O2—C7—H7B110.2O3—C16—H16B109.5
C8—C7—H7B110.2H16A—C16—H16B109.5
H7A—C7—H7B108.5O3—C16—H16C109.5
C7—C8—H8A109.5H16A—C16—H16C109.5
C7—C8—H8B109.5H16B—C16—H16C109.5
H8A—C8—H8B109.5C9—N1—C10124.4 (2)
C7—C8—H8C109.5C2—O1—H1102 (3)
H8A—C8—H8C109.5C3—O2—C7117.3 (2)
H8B—C8—H8C109.5C11—O3—C16118.0 (2)
N1—C9—C1120.9 (2)
C6—C1—C2—O1−179.4 (2)N1—C10—C11—O3−0.2 (3)
C9—C1—C2—O1−0.7 (4)C15—C10—C11—C120.1 (4)
C6—C1—C2—C3−0.7 (4)N1—C10—C11—C12179.7 (2)
C9—C1—C2—C3177.9 (2)O3—C11—C12—C13180.0 (3)
O1—C2—C3—O2−0.3 (4)C10—C11—C12—C130.1 (4)
C1—C2—C3—O2−179.0 (2)C11—C12—C13—C14−0.1 (4)
O1—C2—C3—C4179.5 (2)C12—C13—C14—C150.0 (5)
C1—C2—C3—C40.8 (4)C13—C14—C15—C100.1 (5)
O2—C3—C4—C5179.0 (2)C11—C10—C15—C14−0.2 (4)
C2—C3—C4—C5−0.9 (4)N1—C10—C15—C14−179.8 (3)
C3—C4—C5—C60.9 (4)C1—C9—N1—C10−179.8 (2)
C3—C4—C5—Br1−178.1 (2)C15—C10—N1—C91.3 (4)
C4—C5—C6—C1−0.7 (4)C11—C10—N1—C9−178.3 (2)
Br1—C5—C6—C1178.21 (19)C4—C3—O2—C7−8.4 (4)
C2—C1—C6—C50.7 (4)C2—C3—O2—C7171.4 (2)
C9—C1—C6—C5−178.0 (2)C8—C7—O2—C3−172.8 (2)
C2—C1—C9—N10.6 (4)C12—C11—O3—C16−6.0 (4)
C6—C1—C9—N1179.3 (2)C10—C11—O3—C16173.9 (2)
C15—C10—C11—O3−179.8 (2)
D—H···AD—HH···AD···AD—H···A
O1—H1···N10.81 (5)1.80 (5)2.566 (3)157 (5)
C16—H16A···O1i0.962.553.293 (3)135
C7—H7A···Cg1ii0.972.803.662 (3)149
C13—H13···Cg2iii0.932.793.629 (3)150
  8 in total

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7.  Structure validation in chemical crystallography.

Authors:  Anthony L Spek
Journal:  Acta Crystallogr D Biol Crystallogr       Date:  2009-01-20

8.  The Cambridge Structural Database.

Authors:  Colin R Groom; Ian J Bruno; Matthew P Lightfoot; Suzanna C Ward
Journal:  Acta Crystallogr B Struct Sci Cryst Eng Mater       Date:  2016-04-01
  8 in total

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