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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2012 Oct 20;68(Pt 11):o3168. doi: 10.1107/S1600536812042262

4-Bromo-2-[(E)-{[4-nitro-2-(trifluoro­meth­yl)phen­yl]imino}­meth­yl]phenol

Mehmet Akkurt a,*, Alan R Kennedy b, Shaaban K Mohamed c, Antar A Abdelhamid c, Gary J Miller d
PMCID: PMC3515262  PMID: 23284482

Abstract

Except two F atoms of the –CF3 group, the title compound, C14H8BrF3N2O3, has an almost planar conformation, the dihedral angle between the aromatic rings being 3.60 (16)°. The mol­ecule adopts the enol–imine tautomeric form, with an intra­molecular O—H⋯N hydrogen bond, which generates an S(6) ring motif. In the crystal, face-to-face π–π stacking [centroid–centroid distances = 3.669 (2) and 3.732 (2) Å] between the aromatic rings of the mol­ecules, which lie in sheets parallel to (202), help to establish the packing.

Related literature  

For the biological activity of fluorine-containing compounds, see: Blair et al. (2000); Chawla et al. (2012); Bella et al. (2004); Chandra & Kumar (2005); Yang et al. (2000). For the synthesis of a similar azomethine compound, see: Mohamed et al. (2012). For the graph-set analysis of hydrogen bonding, see: Bernstein et al. (1995).graphic file with name e-68-o3168-scheme1.jpg

Experimental  

Crystal data  

  • C14H8BrF3N2O3

  • M r = 389.12

  • Monoclinic, Inline graphic

  • a = 7.3596 (5) Å

  • b = 16.4625 (10) Å

  • c = 11.2599 (6) Å

  • β = 94.955 (5)°

  • V = 1359.12 (14) Å3

  • Z = 4

  • Mo Kα radiation

  • μ = 3.08 mm−1

  • T = 123 K

  • 0.20 × 0.18 × 0.18 mm

Data collection  

  • Oxford Diffraction Xcalibur Eos diffractometer

  • Absorption correction: multi-scan (CrysAlis PRO; Oxford Diffraction, 2010) T min = 0.546, T max = 0.575

  • 6329 measured reflections

  • 3149 independent reflections

  • 2165 reflections with I > 2σ(I)

  • R int = 0.043

Refinement  

  • R[F 2 > 2σ(F 2)] = 0.050

  • wR(F 2) = 0.090

  • S = 1.02

  • 3149 reflections

  • 203 parameters

  • 1 restraint

  • H-atom parameters constrained

  • Δρmax = 0.51 e Å−3

  • Δρmin = −0.59 e Å−3

Data collection: CrysAlis PRO (Oxford Diffraction, 2010); cell refinement: CrysAlis PRO; data reduction: CrysAlis PRO; 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) and PLATON (Spek, 2009).

Supplementary Material

Crystal structure: contains datablock(s) global, I. DOI: 10.1107/S1600536812042262/xu5632sup1.cif

e-68-o3168-sup1.cif (23KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812042262/xu5632Isup2.hkl

e-68-o3168-Isup2.hkl (154.5KB, hkl)

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
O3—H1O⋯N1 0.84 1.88 2.623 (4) 146

Acknowledgments

Manchester Metropolitan University, Erciyes University and the University of Strathclyde are gratefully acknowledged for supporting this study.

supplementary crystallographic information

Comment

A great number of Schiff base complexes with metals have provoked wide interest because they possess a diverse spectrum of biological and pharmaceutical activities, such as antitumor and anti-oxidative activities, as well as the inhibition of lipid peroxidation (Bella et al., 2004; Chandra & Kumar, 2005; Yang et al., 2000). Fluorine can dramatically change the properties of biologically active compounds and can influence the metabolism and distribution of drug molecules in the body (Blair et al., 2000). Recently, SAR studies revealed that the presence of a fluoro group had a marked influence on the antibacterial activity (Chawla et al., 2012). Such facts and further to our studies on synthesis of bio-active molecules we herein report the synthesis and crystal structure of a new potential bio-active fluorinated azomethine compound (I).

Fig. 1 shows the title compound (I) with the enol-imine tautomeric form, which has an intramolecular O— H···N hydrogen bond forming an S(6) motif (Bernstein et al., 1995; Table 1). The C6—O3 single bond of 1.354 (4) Å and the C7═N1 double bond of 1.293 (4) Å verify the enol-imine form. These distances and the values of the other geometric parameters are in the normal range and are comparable with those of a similar compound reported previously (Mohamed et al., 2012). The two aromatic rings (C1–C6 and C8–C13) make a dihedral angle of 3.60 (16)° with each other. The C1—C7—N1—C8, O1—N2—C11—C10, O2—N2—C11—C10, C14–C9—C8—N1, C8—N1—C7—C1, C7—C1—C6—O3 and C1—C2—C3—Br1 torsion angles are 178.1 (3), 2.4 (4), 175.8 (3), -1.4 (5), -178.1 (3), 0.0 (6) and 179.2 (3) °, respectively. Therefore, the whole molecule of (I), except the F1 and F3 atoms of the –CF3 group, is almostly planar.

The crystal structure is stabilized by face-to-face π-π stacking interactions [Cg1···Cg2(1 - x, -y, 2 - z) = 3.669 (2) Å and Cg1···Cg2(2 - x, -y, 2 - z) = 3.732 (2) Å] between the Cg1 and Cg2 centroids of the C1–C6 and C8–C13 aromatic rings of the molecules to form two-dimensional sheets parallel to the (202) plane (Fig. 2 & Fig. 3).

Experimental

The title compound was unexpectedly obtained from a three component reaction of 0.01 mol 4-nitro-2-(trifluoromethyl)aniline, 0.01 mol 5-bromosalicyaldehyde and 0.01 mol 5-phenyl-1,3-cyclohexanedione in 50 ml ethanol. The reaction mixture was refluxed for 7 h at 350 K. The solid product that obtained on cooling was filtered off, washed with cold ethanol and dried. The crude product was recrystallized from a mixture of ethanol and acetone (10:1 vv) to afford a good quality crystals suitable for X-ray difraction after two days of slow evaporation at room temperature. [Yield 83%; Mp. 511 K].

Refinement

All H atoms were positioned geometrically [C—H = 0.95 Å and O—H = 0.84 Å] and refined as riding with Uiso(H) = 1.2Ueq(C) for aromatic H and Uiso(H) = 1.5Ueq(O) for hydroxyl H. The components of anisotropic displacement for N1 and C7 atoms were made equal using the EADP constraint.

Figures

Fig. 1.

Fig. 1.

The title compound with the atom numbering scheme. Displacement ellipsoids for non-H atoms are drawn at the 50% probability level.

Fig. 2.

Fig. 2.

View of the packing and hydrogen bonding of (I) down a axis. H atoms not involved in hydrogen bonding have been omitted for clarity.

Fig. 3.

Fig. 3.

View of the packing and hydrogen bonding of (I) down b axis. H atoms not involved in hydrogen bonding have been omitted for clarity.

Crystal data

C14H8BrF3N2O3 F(000) = 768
Mr = 389.12 Dx = 1.902 Mg m3
Monoclinic, P21/n Mo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2yn Cell parameters from 1836 reflections
a = 7.3596 (5) Å θ = 3.2–29.0°
b = 16.4625 (10) Å µ = 3.08 mm1
c = 11.2599 (6) Å T = 123 K
β = 94.955 (5)° Cut rod, yellow
V = 1359.12 (14) Å3 0.20 × 0.18 × 0.18 mm
Z = 4

Data collection

Oxford Diffraction Xcalibur Eos diffractometer 3149 independent reflections
Radiation source: Enhance (Mo) X-ray Source 2165 reflections with I > 2σ(I)
Graphite monochromator Rint = 0.043
Detector resolution: 16.0727 pixels mm-1 θmax = 29.0°, θmin = 3.2°
ω scans h = −9→8
Absorption correction: multi-scan (CrysAlis PRO; Oxford Diffraction, 2010) k = −18→22
Tmin = 0.546, Tmax = 0.575 l = −14→15
6329 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)] = 0.050 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.090 H-atom parameters constrained
S = 1.02 w = 1/[σ2(Fo2) + (0.0233P)2] where P = (Fo2 + 2Fc2)/3
3149 reflections (Δ/σ)max < 0.001
203 parameters Δρmax = 0.51 e Å3
1 restraint Δρmin = −0.59 e Å3

Special details

Geometry. Bond distances, angles etc. have been calculated using the rounded fractional coordinates. All su's are estimated from the variances of the (full) variance-covariance matrix. The cell e.s.d.'s are taken into account in the estimation of distances, angles and torsion angles
Refinement. Refinement on F2 for ALL reflections except those flagged by the user for potential systematic errors. Weighted R-factors wR and all goodnesses of fit S are based on F2, conventional R-factors R are based on F, with F set to zero for negative F2. The observed criterion of F2 > σ(F2) is used only for calculating -R-factor-obs 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
Br1 0.40760 (6) 0.10935 (3) 0.52512 (3) 0.0305 (2)
F1 0.7671 (3) 0.08414 (14) 1.28090 (17) 0.0313 (8)
F2 1.0022 (3) 0.05148 (15) 1.39501 (17) 0.0404 (9)
F3 1.0339 (3) 0.09587 (14) 1.21958 (18) 0.0321 (8)
O1 1.1326 (3) −0.22498 (18) 1.4389 (2) 0.0299 (9)
O2 1.0746 (4) −0.31205 (17) 1.2960 (2) 0.0286 (9)
O3 0.7242 (4) 0.17073 (17) 1.02757 (19) 0.0262 (9)
N1 0.7788 (4) 0.01384 (19) 1.0499 (2) 0.0168 (7)
N2 1.0692 (4) −0.2434 (2) 1.3380 (3) 0.0231 (11)
C1 0.6384 (5) 0.0741 (2) 0.8725 (3) 0.0160 (11)
C2 0.5635 (4) 0.0613 (2) 0.7551 (3) 0.0185 (11)
C3 0.5065 (5) 0.1256 (3) 0.6850 (3) 0.0192 (11)
C4 0.5184 (5) 0.2040 (3) 0.7277 (3) 0.0220 (12)
C5 0.5917 (5) 0.2182 (2) 0.8437 (3) 0.0210 (12)
C6 0.6520 (5) 0.1540 (2) 0.9156 (3) 0.0176 (11)
C7 0.6997 (4) 0.0045 (2) 0.9437 (3) 0.0168 (7)
C8 0.8434 (4) −0.0537 (2) 1.1180 (3) 0.0145 (11)
C9 0.9215 (5) −0.0375 (2) 1.2358 (3) 0.0158 (11)
C10 0.9916 (4) −0.1002 (2) 1.3070 (3) 0.0185 (11)
C11 0.9869 (4) −0.1777 (2) 1.2628 (3) 0.0165 (11)
C12 0.9119 (5) −0.1958 (2) 1.1491 (3) 0.0194 (12)
C13 0.8421 (5) −0.1338 (2) 1.0781 (3) 0.0190 (11)
C14 0.9282 (5) 0.0480 (3) 1.2828 (3) 0.0225 (12)
H1O 0.75720 0.12730 1.06220 0.0390*
H2 0.55230 0.00760 0.72440 0.0220*
H4 0.47670 0.24810 0.67820 0.0260*
H5 0.60030 0.27220 0.87360 0.0250*
H7 0.68160 −0.04870 0.91210 0.0200*
H10 1.04260 −0.08970 1.38590 0.0220*
H12 0.90880 −0.25020 1.12080 0.0230*
H13 0.79150 −0.14570 0.99960 0.0230*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
Br1 0.0418 (3) 0.0288 (3) 0.0189 (2) 0.0038 (2) −0.0083 (2) 0.0014 (2)
F1 0.0389 (14) 0.0225 (14) 0.0323 (13) 0.0074 (12) 0.0023 (10) −0.0076 (11)
F2 0.0708 (18) 0.0249 (16) 0.0215 (12) 0.0036 (15) −0.0195 (11) −0.0031 (11)
F3 0.0407 (14) 0.0180 (14) 0.0370 (13) −0.0091 (12) −0.0002 (10) −0.0010 (11)
O1 0.0367 (17) 0.0287 (18) 0.0221 (14) −0.0014 (15) −0.0098 (11) 0.0078 (14)
O2 0.0364 (17) 0.0168 (17) 0.0325 (15) 0.0032 (15) 0.0019 (12) 0.0047 (13)
O3 0.0387 (17) 0.0174 (16) 0.0206 (14) 0.0006 (15) −0.0082 (11) 0.0014 (12)
N1 0.0190 (12) 0.0145 (13) 0.0168 (11) −0.0024 (11) 0.0008 (9) 0.0019 (11)
N2 0.0215 (18) 0.023 (2) 0.0249 (18) 0.0009 (17) 0.0021 (13) 0.0074 (16)
C1 0.0146 (19) 0.017 (2) 0.0164 (18) −0.0012 (17) 0.0015 (14) 0.0063 (17)
C2 0.0190 (19) 0.015 (2) 0.021 (2) −0.0019 (18) −0.0007 (14) −0.0029 (17)
C3 0.0156 (19) 0.024 (2) 0.0178 (19) −0.0020 (18) −0.0004 (14) 0.0031 (17)
C4 0.020 (2) 0.023 (2) 0.023 (2) −0.0011 (19) 0.0022 (15) 0.0039 (18)
C5 0.025 (2) 0.013 (2) 0.025 (2) 0.0003 (18) 0.0022 (15) 0.0016 (17)
C6 0.0170 (19) 0.016 (2) 0.0198 (19) −0.0017 (18) 0.0014 (14) 0.0005 (17)
C7 0.0190 (12) 0.0145 (13) 0.0168 (11) −0.0024 (11) 0.0008 (9) 0.0019 (11)
C8 0.0136 (18) 0.016 (2) 0.0139 (18) 0.0001 (17) 0.0015 (13) 0.0036 (16)
C9 0.0169 (19) 0.016 (2) 0.0144 (18) −0.0003 (17) 0.0015 (14) 0.0020 (16)
C10 0.0168 (19) 0.025 (2) 0.0136 (18) −0.0014 (19) 0.0009 (13) 0.0002 (17)
C11 0.0138 (19) 0.018 (2) 0.0177 (18) 0.0029 (17) 0.0018 (14) 0.0057 (17)
C12 0.022 (2) 0.012 (2) 0.024 (2) −0.0020 (18) 0.0015 (15) −0.0028 (17)
C13 0.028 (2) 0.014 (2) 0.0139 (18) −0.0011 (18) −0.0037 (15) −0.0018 (16)
C14 0.029 (2) 0.017 (2) 0.020 (2) −0.001 (2) −0.0071 (16) 0.0025 (17)

Geometric parameters (Å, º)

Br1—C3 1.902 (3) C4—C5 1.389 (5)
F1—C14 1.325 (5) C5—C6 1.381 (5)
F2—C14 1.333 (4) C8—C13 1.393 (5)
F3—C14 1.352 (5) C8—C9 1.425 (5)
O1—N2 1.228 (4) C9—C10 1.379 (5)
O2—N2 1.227 (4) C9—C14 1.503 (6)
O3—C6 1.354 (4) C10—C11 1.369 (5)
O3—H1O 0.8400 C11—C12 1.382 (5)
N1—C7 1.293 (4) C12—C13 1.369 (5)
N1—C8 1.410 (4) C2—H2 0.9500
N2—C11 1.471 (5) C4—H4 0.9500
C1—C6 1.403 (5) C5—H5 0.9500
C1—C7 1.448 (5) C7—H7 0.9500
C1—C2 1.404 (5) C10—H10 0.9500
C2—C3 1.365 (5) C12—H12 0.9500
C3—C4 1.378 (7) C13—H13 0.9500
C6—O3—H1O 109.00 N2—C11—C10 118.7 (3)
C7—N1—C8 120.9 (3) C10—C11—C12 122.2 (3)
O1—N2—C11 117.1 (3) N2—C11—C12 119.1 (3)
O2—N2—C11 118.7 (3) C11—C12—C13 118.7 (3)
O1—N2—O2 124.2 (3) C8—C13—C12 121.7 (3)
C2—C1—C7 118.8 (3) F1—C14—F3 106.5 (3)
C6—C1—C7 122.8 (3) F1—C14—C9 114.4 (3)
C2—C1—C6 118.5 (3) F1—C14—F2 106.7 (3)
C1—C2—C3 120.3 (3) F2—C14—C9 111.9 (3)
Br1—C3—C2 120.8 (3) F3—C14—C9 111.3 (3)
Br1—C3—C4 118.0 (3) F2—C14—F3 105.5 (3)
C2—C3—C4 121.2 (3) C1—C2—H2 120.00
C3—C4—C5 119.6 (4) C3—C2—H2 120.00
C4—C5—C6 120.1 (3) C3—C4—H4 120.00
O3—C6—C5 118.1 (3) C5—C4—H4 120.00
C1—C6—C5 120.3 (3) C4—C5—H5 120.00
O3—C6—C1 121.6 (3) C6—C5—H5 120.00
N1—C7—C1 120.8 (3) N1—C7—H7 120.00
N1—C8—C13 125.4 (3) C1—C7—H7 120.00
C9—C8—C13 117.9 (3) C9—C10—H10 120.00
N1—C8—C9 116.7 (3) C11—C10—H10 120.00
C8—C9—C14 120.1 (3) C11—C12—H12 121.00
C10—C9—C14 119.8 (3) C13—C12—H12 121.00
C8—C9—C10 120.1 (3) C8—C13—H13 119.00
C9—C10—C11 119.3 (3) C12—C13—H13 119.00
C8—N1—C7—C1 −178.1 (3) C4—C5—C6—C1 −0.5 (6)
C7—N1—C8—C9 −177.4 (3) N1—C8—C9—C10 −178.5 (3)
C7—N1—C8—C13 4.8 (5) N1—C8—C9—C14 1.4 (5)
O1—N2—C11—C10 2.4 (4) C13—C8—C9—C10 −0.5 (5)
O1—N2—C11—C12 −179.2 (3) C13—C8—C9—C14 179.3 (3)
O2—N2—C11—C10 −175.8 (3) N1—C8—C13—C12 178.3 (3)
O2—N2—C11—C12 2.5 (5) C9—C8—C13—C12 0.5 (5)
C6—C1—C2—C3 0.3 (5) C8—C9—C10—C11 0.7 (5)
C7—C1—C2—C3 −179.2 (3) C14—C9—C10—C11 −179.2 (3)
C2—C1—C6—O3 −179.5 (3) C8—C9—C14—F1 57.2 (4)
C2—C1—C6—C5 0.4 (5) C8—C9—C14—F2 178.7 (3)
C7—C1—C6—O3 0.0 (6) C8—C9—C14—F3 −63.6 (4)
C7—C1—C6—C5 179.9 (3) C10—C9—C14—F1 −122.9 (3)
C2—C1—C7—N1 176.1 (3) C10—C9—C14—F2 −1.5 (5)
C6—C1—C7—N1 −3.4 (5) C10—C9—C14—F3 116.3 (4)
C1—C2—C3—Br1 179.2 (3) C9—C10—C11—N2 177.4 (3)
C1—C2—C3—C4 −0.9 (5) C9—C10—C11—C12 −0.8 (5)
Br1—C3—C4—C5 −179.3 (3) N2—C11—C12—C13 −177.5 (3)
C2—C3—C4—C5 0.8 (6) C10—C11—C12—C13 0.8 (5)
C3—C4—C5—C6 −0.1 (6) C11—C12—C13—C8 −0.6 (5)
C4—C5—C6—O3 179.3 (3)

Hydrogen-bond geometry (Å, º)

D—H···A D—H H···A D···A D—H···A
O3—H1O···N1 0.84 1.88 2.623 (4) 146
C10—H10···F2 0.95 2.35 2.685 (4) 100
C13—H13···O1i 0.95 2.50 3.134 (4) 125

Symmetry code: (i) x−1/2, −y−1/2, z−1/2.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: XU5632).

References

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  8. Mohamed, S. K., Abdelhamid, A. A., Akkurt, M., Fanwick, P. E. & Maharramov, A. M. (2012). Acta Cryst. E68, o1618. [DOI] [PMC free article] [PubMed]
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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 datablock(s) global, I. DOI: 10.1107/S1600536812042262/xu5632sup1.cif

e-68-o3168-sup1.cif (23KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812042262/xu5632Isup2.hkl

e-68-o3168-Isup2.hkl (154.5KB, hkl)

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


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