Abstract
The title compound, C14H12FNO, crystallizes as the trans phenol–imine tautomer. The two benzene rings are essentially coplanar, being inclined to one another by 9.28 (7)°. This is at least in part due to the intramolecular O—H⋯N hydrogen bond between the hydroxy O atom and the imine N atom. The crystal structure is stabilized by an array of weak C—H⋯O and C—H⋯F interactions, which link the molecules into a stable three-dimensional network.
Related literature
For related structures, see: Karakaş et al. (2004 ▶); Arod et al. (2005 ▶); Cheng et al. (2005 ▶); Brink et al. (2009 ▶). For related rhenium tricarbonyl complexes containing salicylaldimines, see: Brink et al. (2011 ▶). For related N,O-bidentate ligands coordinated to a rhenium tricarbonyl core, see: Schutte et al. (2011 ▶).
Experimental
Crystal data
C14H12FNO
M r = 229.25
Monoclinic,
a = 10.2655 (6) Å
b = 4.6738 (2) Å
c = 12.3561 (8) Å
β = 112.331 (3)°
V = 548.37 (5) Å3
Z = 2
Mo Kα radiation
μ = 0.10 mm−1
T = 100 K
0.19 × 0.1 × 0.06 mm
Data collection
Bruker X8 APEXII 4K Kappa CCD diffractometer
Absorption correction: multi-scan (SADABS; Bruker, 2004 ▶) T min = 0.981, T max = 0.994
7009 measured reflections
1319 independent reflections
1203 reflections with I > 2σ(I)
R int = 0.028
Refinement
R[F 2 > 2σ(F 2)] = 0.034
wR(F 2) = 0.095
S = 1.06
1319 reflections
156 parameters
2 restraints
H-atom parameters constrained
Δρmax = 0.19 e Å−3
Δρmin = −0.19 e Å−3
Data collection: APEX2 (Bruker, 2005 ▶); cell refinement: SAINT-Plus (Bruker, 2004 ▶); data reduction: SAINT-Plus and XPREP (Bruker, 2004 ▶); program(s) used to solve structure: SIR92 (Altomare et al., 1999 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: DIAMOND (Brandenburg & Putz, 2004 ▶); software used to prepare material for publication: WingGX (Farrugia, 1999 ▶).
Supplementary Material
Crystal structure: contains datablock(s) global, I. DOI: 10.1107/S1600536812010513/sj5208sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812010513/sj5208Isup2.hkl
Supplementary material file. DOI: 10.1107/S1600536812010513/sj5208Isup3.cml
Additional supplementary materials: crystallographic information; 3D view; checkCIF report
Table 1. Hydrogen-bond geometry (Å, °).
| D—H⋯A | D—H | H⋯A | D⋯A | D—H⋯A |
|---|---|---|---|---|
| O1—H1B⋯N1 | 0.84 | 1.85 | 2.601 (2) | 147 |
| C1—H1A⋯O1i | 0.95 | 2.6 | 3.467 (3) | 151 |
| C16—H16⋯O1i | 0.95 | 2.65 | 3.495 (3) | 149 |
| C13—H13⋯F1ii | 0.95 | 2.6 | 3.472 (3) | 153 |
| C231—H23A⋯F1iii | 0.98 | 2.73 | 3.321 (3) | 119 |
| C231—H23C⋯F1iv | 0.98 | 2.67 | 3.193 (2) | 114 |
Symmetry codes: (i)
; (ii)
; (iii)
; (iv)
.
Acknowledgments
Financial assistance from the University of the Free State (UFS), the UFS Advanced Biomolecular Cluster, SASOL and the South African National Research Foundation (SA-NRF/THRIP) is gratefully acknowledged. Part of this material is based on work supported by the SA-NRF/THRIP under grant No. GUN 2068915. Opinions, findings, conclusions or recommendations expressed in this material are those of the authors and do not necessarily reflect the views of the SA-NRF.
supplementary crystallographic information
Comment
Schiff-base ligands have played a significant role in the development of coordination chemistry as stable organometallic complexes are readily formed with a variety of transition metals. In continuation of our research on the coordination of various bifunctional chelate systems on the fac-[M(CO)3]+ moiety (M = Re(I), Tc(I)) (Brink et al., 2011; Schutte et al., 2011) the title compound was synthesized and is reported here.
The title compound (Figure 1) is essentially co-planar with a dihedral angle of 9.28 (7)° between the aromatic rings. The bond distances and angles in the title compound are in accord with those reported for related salicylaldimine-based ligand systems (Karakaş et al., 2004; Arod et al., 2005; Cheng et al., 2005; Brink et al., 2009).
The compound crystallizes as the trans phenol-imine tautomer. A strong intramolecular hydrogen bond occurs between the O—H···N atoms in each unique molecule. The crystal structure is stabilized by an array of weak C—H···O and C—H···F interactions. The bifurcated acceptor, O1, experiences weak hydrogen bond interactions with H16 and H1A. As a result, the two independent molecules pack nearly perpendicular to each other with a dihedral angle of 88.01 (5)° between planes drawn through the C1 aromatic ring systems (Figures 2 and 3). All the interactions serve to link the molecules into a stable three-dimensional supramolecular network. The molecular packing, viewed along the c-axis, illustrates the cube-like tunnel formation resulting from the various interactions (Figure 4).
Experimental
The reaction was performed under Schlenk conditions using a nitrogen atmosphere. To a solution of 5-fluorosalicylaldehyde (0.50 g, 3.57 mmol) in methanol, a solution of m-toluidine (0.382 g, 3.57 mmol) was added. The reaction was refluxed at 80°C for 3 h. The solvent was removed under reduced pressure. The product was obtained as an orange solid which was washed with cold methanol and filtered. Crystals suitable for X-ray diffraction were grown from the filtrate. Yield 82.1%. 1H NMR [acetone-d6, 600 MHz, δ (p.p.m.)] 13.04 (s, 1H), 8.90 (s, 1H), 7.40 (dd, 1H, J = 3.1, 8.7 Hz), 7.35 (t, 1H, J = 7.7 Hz), 7.25 (s, 1H), 7.24–7.20 (m, 2H), 7.16 (d, 1H, J = 7.7 Hz), 6.96 (dd, 1H, J = 4.5, 9.1 Hz), 2.39 (s, 3H, CH3).
Refinement
The aromatic H atoms and hydroxy H atom were placed in geometrically idealized positions and constrained to ride on their parent atoms with Uiso(H) = 1.2Ueq(C) and 1.5eq(O).The aliphatic H atoms were placed in geometrically idealized positions and constrained to ride on their parent atoms with Uiso(H) = 1.2Ueq(C) and 1.5eq(C), respectively for the methylene and methyl carbon atoms. The methyl groups were generated to fit the difference electron density and the groups were then refined as rigid rotors. The absolute structure parameter is meaningless and has been removed from the CIF. The Friedel opposites have been merged as the compound is a weak anomalous scatterer.
Figures
Fig. 1.
Representation of the molecular structure of the title compound, showing the numbering scheme and displacement ellipsoids drawn at the 50% probability level.
Fig. 2.
Representation of the hydrogen-bond interactions (only relevant H atoms are shown).
Fig. 3.
Representation of the perpendicular orientation of molecules.
Fig. 4.
Molecular packing of the unit cell illustrating the cube-like formation as viewed along the c-axis.
Crystal data
| C14H12FNO | F(000) = 240 |
| Mr = 229.25 | Dx = 1.388 Mg m−3 |
| Monoclinic, Pc | Mo Kα radiation, λ = 0.71073 Å |
| Hall symbol: P -2yc | Cell parameters from 2573 reflections |
| a = 10.2655 (6) Å | θ = 3.4–28.3° |
| b = 4.6738 (2) Å | µ = 0.10 mm−1 |
| c = 12.3561 (8) Å | T = 100 K |
| β = 112.331 (3)° | Cuboid, orange |
| V = 548.37 (5) Å3 | 0.19 × 0.1 × 0.06 mm |
| Z = 2 |
Data collection
| Bruker X8 APEXII 4K Kappa CCD diffractometer | 1319 independent reflections |
| Graphite monochromator | 1203 reflections with I > 2σ(I) |
| Detector resolution: 512 pixels mm-1 | Rint = 0.028 |
| ω and φ scans | θmax = 28.0°, θmin = 3.4° |
| Absorption correction: multi-scan (SADABS; Bruker, 2004) | h = −13→13 |
| Tmin = 0.981, Tmax = 0.994 | k = −5→6 |
| 7009 measured reflections | l = −16→16 |
Refinement
| Refinement on F2 | 2 restraints |
| Least-squares matrix: full | H-atom parameters constrained |
| R[F2 > 2σ(F2)] = 0.034 | w = 1/[σ2(Fo2) + (0.0597P)2 + 0.0513P] where P = (Fo2 + 2Fc2)/3 |
| wR(F2) = 0.095 | (Δ/σ)max < 0.001 |
| S = 1.06 | Δρmax = 0.19 e Å−3 |
| 1319 reflections | Δρmin = −0.19 e Å−3 |
| 156 parameters |
Special details
| Experimental. Intensity data was collected on a Bruker X8 Apex II 4 K Kappa CCD diffractometer using an exposure time of 55 s/frame. A total of 1495 frames were collected with a frame width of 0.5° covering up to θ = 28.0° with 99.6% completeness accomplished |
| 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. |
Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2)
| x | y | z | Uiso*/Ueq | ||
| N1 | 0.51676 (18) | 0.7931 (4) | 0.51611 (15) | 0.0170 (4) | |
| O1 | 0.62483 (16) | 0.5330 (3) | 0.71672 (14) | 0.0229 (4) | |
| H1B | 0.571 | 0.6442 | 0.666 | 0.034* | |
| F1 | 0.95777 (14) | −0.0665 (3) | 0.54083 (13) | 0.0276 (3) | |
| C1 | 0.5962 (2) | 0.6410 (4) | 0.47953 (19) | 0.0178 (4) | |
| H1A | 0.5897 | 0.6626 | 0.4012 | 0.021* | |
| C11 | 0.6955 (2) | 0.4372 (4) | 0.55563 (18) | 0.0161 (4) | |
| C12 | 0.7069 (2) | 0.3900 (4) | 0.67131 (18) | 0.0183 (4) | |
| C13 | 0.8048 (2) | 0.1934 (5) | 0.74184 (18) | 0.0211 (5) | |
| H13 | 0.8132 | 0.1637 | 0.8203 | 0.025* | |
| C14 | 0.8897 (2) | 0.0416 (5) | 0.6980 (2) | 0.0219 (5) | |
| H14 | 0.9567 | −0.0919 | 0.7458 | 0.026* | |
| C15 | 0.8756 (2) | 0.0873 (4) | 0.5839 (2) | 0.0195 (5) | |
| C16 | 0.7817 (2) | 0.2812 (5) | 0.51227 (19) | 0.0181 (4) | |
| H16 | 0.7753 | 0.3092 | 0.4343 | 0.022* | |
| C21 | 0.4220 (2) | 0.9970 (4) | 0.44138 (18) | 0.0168 (4) | |
| C22 | 0.3265 (2) | 1.1211 (4) | 0.48298 (18) | 0.0171 (4) | |
| H22 | 0.3286 | 1.0669 | 0.5577 | 0.021* | |
| C23 | 0.2280 (2) | 1.3232 (5) | 0.41733 (18) | 0.0189 (4) | |
| C24 | 0.2290 (2) | 1.4038 (5) | 0.30877 (18) | 0.0209 (5) | |
| H24 | 0.163 | 1.541 | 0.2625 | 0.025* | |
| C25 | 0.3257 (2) | 1.2853 (5) | 0.26779 (19) | 0.0223 (5) | |
| H25 | 0.3258 | 1.3445 | 0.1943 | 0.027* | |
| C26 | 0.4219 (2) | 1.0818 (4) | 0.33261 (19) | 0.0205 (5) | |
| H26 | 0.4871 | 1.0008 | 0.3036 | 0.025* | |
| C231 | 0.1250 (2) | 1.4526 (5) | 0.4626 (2) | 0.0227 (5) | |
| H23A | 0.1367 | 1.3641 | 0.5377 | 0.034* | |
| H23B | 0.0289 | 1.4194 | 0.4063 | 0.034* | |
| H23C | 0.1422 | 1.6588 | 0.4736 | 0.034* |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| N1 | 0.0165 (8) | 0.0168 (8) | 0.0174 (9) | −0.0004 (6) | 0.0061 (7) | 0.0005 (6) |
| O1 | 0.0264 (8) | 0.0271 (8) | 0.0181 (7) | 0.0081 (6) | 0.0116 (7) | 0.0032 (6) |
| F1 | 0.0278 (7) | 0.0264 (7) | 0.0320 (7) | 0.0092 (5) | 0.0154 (6) | 0.0010 (6) |
| C1 | 0.0200 (10) | 0.0174 (8) | 0.0165 (10) | −0.0022 (8) | 0.0075 (8) | 0.0011 (8) |
| C11 | 0.0166 (10) | 0.0141 (9) | 0.0164 (10) | −0.0015 (7) | 0.0050 (8) | −0.0008 (8) |
| C12 | 0.0190 (10) | 0.0193 (10) | 0.0170 (10) | −0.0024 (8) | 0.0074 (9) | −0.0012 (8) |
| C13 | 0.0228 (11) | 0.0231 (10) | 0.0157 (10) | −0.0005 (9) | 0.0053 (9) | 0.0034 (8) |
| C14 | 0.0201 (11) | 0.0207 (10) | 0.0212 (11) | 0.0009 (8) | 0.0036 (9) | 0.0019 (8) |
| C15 | 0.0166 (10) | 0.0191 (10) | 0.0244 (12) | 0.0003 (8) | 0.0096 (9) | −0.0018 (8) |
| C16 | 0.0194 (10) | 0.0192 (10) | 0.0178 (10) | −0.0010 (8) | 0.0095 (8) | −0.0006 (7) |
| C21 | 0.0171 (10) | 0.0154 (9) | 0.0177 (10) | −0.0020 (8) | 0.0063 (8) | −0.0010 (7) |
| C22 | 0.0184 (10) | 0.0163 (9) | 0.0165 (10) | −0.0023 (7) | 0.0066 (8) | −0.0006 (8) |
| C23 | 0.0168 (10) | 0.0188 (10) | 0.0200 (11) | −0.0025 (8) | 0.0059 (8) | −0.0034 (8) |
| C24 | 0.0181 (11) | 0.0193 (10) | 0.0219 (11) | 0.0017 (8) | 0.0039 (9) | 0.0011 (8) |
| C25 | 0.0240 (12) | 0.0248 (11) | 0.0186 (10) | 0.0027 (8) | 0.0086 (9) | 0.0038 (8) |
| C26 | 0.0206 (10) | 0.0217 (10) | 0.0209 (11) | 0.0022 (8) | 0.0098 (9) | 0.0001 (8) |
| C231 | 0.0192 (10) | 0.0244 (10) | 0.0247 (11) | 0.0015 (8) | 0.0086 (9) | −0.0019 (9) |
Geometric parameters (Å, º)
| N1—C1 | 1.287 (3) | C21—C22 | 1.395 (3) |
| N1—C21 | 1.422 (3) | C21—C26 | 1.401 (3) |
| O1—C12 | 1.353 (3) | C21—N1 | 1.422 (3) |
| O1—H1B | 0.84 | C22—C23 | 1.396 (3) |
| F1—C15 | 1.361 (2) | C22—H22 | 0.95 |
| C1—C11 | 1.450 (3) | C23—C24 | 1.397 (3) |
| C1—H1A | 0.95 | C23—C231 | 1.499 (3) |
| C11—C16 | 1.401 (3) | C24—C25 | 1.389 (3) |
| C11—C12 | 1.407 (3) | C24—H24 | 0.95 |
| C12—C13 | 1.396 (3) | C25—C26 | 1.386 (3) |
| C13—C14 | 1.385 (3) | C25—H25 | 0.95 |
| C13—H13 | 0.95 | C26—H26 | 0.95 |
| C14—C15 | 1.377 (3) | C231—H23A | 0.98 |
| C14—H14 | 0.95 | C231—H23B | 0.98 |
| C15—C16 | 1.373 (3) | C231—H23C | 0.98 |
| C16—H16 | 0.95 | ||
| C1—N1—C21 | 120.69 (16) | C26—C21—N1 | 124.30 (18) |
| C12—O1—H1B | 109.5 | C22—C21—N1 | 116.25 (17) |
| N1—C1—C11 | 121.23 (18) | C26—C21—N1 | 124.30 (18) |
| N1—C1—H1A | 119.4 | C21—C22—C23 | 121.53 (18) |
| C11—C1—H1A | 119.4 | C21—C22—H22 | 119.2 |
| C16—C11—C12 | 119.11 (19) | C23—C22—H22 | 119.2 |
| C16—C11—C1 | 118.98 (18) | C22—C23—C24 | 118.16 (18) |
| C12—C11—C1 | 121.91 (18) | C22—C23—C231 | 120.94 (18) |
| O1—C12—C13 | 118.70 (18) | C24—C23—C231 | 120.90 (19) |
| O1—C12—C11 | 121.31 (19) | C25—C24—C23 | 120.63 (19) |
| C13—C12—C11 | 119.99 (19) | C25—C24—H24 | 119.7 |
| C14—C13—C12 | 120.27 (19) | C23—C24—H24 | 119.7 |
| C14—C13—H13 | 119.9 | C26—C25—C24 | 120.94 (19) |
| C12—C13—H13 | 119.9 | C26—C25—H25 | 119.5 |
| C15—C14—C13 | 118.9 (2) | C24—C25—H25 | 119.5 |
| C15—C14—H14 | 120.5 | C25—C26—C21 | 119.3 (2) |
| C13—C14—H14 | 120.5 | C25—C26—H26 | 120.4 |
| F1—C15—C16 | 118.91 (19) | C21—C26—H26 | 120.4 |
| F1—C15—C14 | 118.57 (19) | C23—C231—H23A | 109.5 |
| C16—C15—C14 | 122.5 (2) | C23—C231—H23B | 109.5 |
| C15—C16—C11 | 119.17 (19) | H23A—C231—H23B | 109.5 |
| C15—C16—H16 | 120.4 | C23—C231—H23C | 109.5 |
| C11—C16—H16 | 120.4 | H23A—C231—H23C | 109.5 |
| C22—C21—C26 | 119.44 (19) | H23B—C231—H23C | 109.5 |
| C22—C21—N1 | 116.25 (17) | ||
| N1—N1—C1—C11 | 0.0 (6) | N1—N1—C21—C22 | 0.0 (6) |
| C21—N1—C1—C11 | 178.58 (17) | C1—N1—C21—C22 | 171.08 (18) |
| N1—C1—C11—C16 | −178.66 (18) | N1—N1—C21—C26 | 0.0 (7) |
| N1—C1—C11—C12 | 1.9 (3) | C1—N1—C21—C26 | −10.4 (3) |
| C16—C11—C12—O1 | −179.24 (18) | C1—N1—C21—N1 | 0E1 (10) |
| C1—C11—C12—O1 | 0.2 (3) | C26—C21—C22—C23 | 1.7 (3) |
| C16—C11—C12—C13 | 1.1 (3) | N1—C21—C22—C23 | −179.74 (17) |
| C1—C11—C12—C13 | −179.45 (19) | N1—C21—C22—C23 | −179.74 (17) |
| O1—C12—C13—C14 | 179.49 (19) | C21—C22—C23—C24 | −1.3 (3) |
| C11—C12—C13—C14 | −0.8 (3) | C21—C22—C23—C231 | 179.38 (19) |
| C12—C13—C14—C15 | −0.2 (3) | C22—C23—C24—C25 | 0.0 (3) |
| C13—C14—C15—F1 | −178.87 (18) | C231—C23—C24—C25 | 179.33 (19) |
| C13—C14—C15—C16 | 1.0 (3) | C23—C24—C25—C26 | 0.9 (3) |
| F1—C15—C16—C11 | 179.14 (17) | C24—C25—C26—C21 | −0.5 (3) |
| C14—C15—C16—C11 | −0.8 (3) | C22—C21—C26—C25 | −0.7 (3) |
| C12—C11—C16—C15 | −0.3 (3) | N1—C21—C26—C25 | −179.19 (19) |
| C1—C11—C16—C15 | −179.79 (18) | N1—C21—C26—C25 | −179.19 (19) |
Hydrogen-bond geometry (Å, º)
| D—H···A | D—H | H···A | D···A | D—H···A |
| O1—H1B···N1 | 0.84 | 1.85 | 2.601 (2) | 147 |
| C1—H1A···O1i | 0.95 | 2.6 | 3.467 (3) | 151 |
| C16—H16···O1i | 0.95 | 2.65 | 3.495 (3) | 149 |
| C13—H13···F1ii | 0.95 | 2.6 | 3.472 (3) | 153 |
| C231—H23A···F1iii | 0.98 | 2.73 | 3.321 (3) | 119 |
| C231—H23C···F1iv | 0.98 | 2.67 | 3.193 (2) | 114 |
Symmetry codes: (i) x, −y+1, z−1/2; (ii) x, −y, z+1/2; (iii) x−1, y+1, z; (iv) x−1, y+2, z.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: SJ5208).
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 datablock(s) global, I. DOI: 10.1107/S1600536812010513/sj5208sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812010513/sj5208Isup2.hkl
Supplementary material file. DOI: 10.1107/S1600536812010513/sj5208Isup3.cml
Additional supplementary materials: crystallographic information; 3D view; checkCIF report




