Supporting information
Crystallographic Information File (CIF) https://doi.org/10.1107/S2056989015006374/hb7370sup1.cif | |
Structure factor file (CIF format) https://doi.org/10.1107/S2056989015006374/hb7370Isup2.hkl |
CCDC reference: 1005919
Key indicators
- Single-crystal X-ray study
- T = 293 K
- Mean (C-C) = 0.003 Å
- R factor = 0.050
- wR factor = 0.130
- Data-to-parameter ratio = 15.8
checkCIF/PLATON results
No syntax errors found
Alert level C PLAT029_ALERT_3_C _diffrn_measured_fraction_theta_full Low ....... 0.974 Note PLAT911_ALERT_3_C Missing # FCF Refl Between THmin & STh/L= 0.600 51 Report PLAT913_ALERT_3_C Missing # of Very Strong Reflections in FCF .... 1 Note
Alert level G PLAT002_ALERT_2_G Number of Distance or Angle Restraints on AtSite 4 Note PLAT172_ALERT_4_G The CIF-Embedded .res File Contains DFIX Records 2 Report PLAT199_ALERT_1_G Reported _cell_measurement_temperature ..... (K) 293 Check PLAT200_ALERT_1_G Reported _diffrn_ambient_temperature ..... (K) 293 Check PLAT309_ALERT_2_G Single Bonded Oxygen (C-O > 1.3 Ang) ........... O1 Check PLAT860_ALERT_3_G Number of Least-Squares Restraints ............. 2 Note PLAT910_ALERT_3_G Missing # of FCF Reflection(s) Below Th(Min) ... 1 Report PLAT912_ALERT_4_G Missing # of FCF Reflections Above STh/L= 0.600 19 Note
0 ALERT level A = Most likely a serious problem - resolve or explain 0 ALERT level B = A potentially serious problem, consider carefully 3 ALERT level C = Check. Ensure it is not caused by an omission or oversight 8 ALERT level G = General information/check it is not something unexpected 2 ALERT type 1 CIF construction/syntax error, inconsistent or missing data 2 ALERT type 2 Indicator that the structure model may be wrong or deficient 5 ALERT type 3 Indicator that the structure quality may be low 2 ALERT type 4 Improvement, methodology, query or suggestion 0 ALERT type 5 Informative message, check
N-substituted imines, also known as Schiff bases represent one of the most widely used families of organic compounds. Schiff bases have been intensively used as synthetic intermediates and as ligands for coordinating transition and inner transition metal ions, and recently also for coordinating anions. Schiff base ligands may contain a variety of substituents with different electron-donating or electron-withdrawing groups, and therefore may have interesting chemical properties. They have attracted particular interest due to their biological activities acting as radiopharmaceuticals for cancer targeting.They have also been used as model systems for biological macromolecules . Besides the biological activity, solid-state thermochromism and photochromism are an another characteristic of these compounds leading to their application in various areas of materials science such as the control and measurement of radiation intensity, display systems and optical memory devices . Schiff bases derived from o-hydroxyaromatic aldehydes and ketones are excellent models for the study of keto-enol tautomerism both in solution and in the solid state (Blagus et al., 2010).
The structure of the title compound is as shown in Fig.1 is described in terms of three planar subunits,namely two terminal benzene rings and their substituents bridged by a C=N moiety. The molecule has adopted E-configuration about the C8—N1 double bond (1.301 (2)Å) with a C9—N1—C8—C4 torsion angle of 179.90 (16)°. The C4—C8 and N1—C9 bond distances [1.410 (2) and 1.404 (2)Å] confirm π-electron delocalisation between the phenyl rings. The N1—C8—C4[123.26 (15)°] is greater than the normal value of 120°. This may be due to interaction of iminium H with phenolate O atom. The C6—C5—C4 [116.51 (15)°] is smaller than the normal value of 120° which is due to lengthening of the phenolate C5—O1 [1.304 (2)Å] bond. All other bond distances and bond angles are within the normal range (Eltayeb et al., 2010).
The iminium H atom is engaged in a strong intramolecular hydrogen bond with the O atom of the phenolate (N+ —H···O ) to form a S(6) motif. The crystal structure is stabilised by both intramolecular N1—H1···O1 and intermolecular O2—H4···O1 hydrogen bonding linking the molecules into infinite one-dimensional chains as shown in the figure.2, table.2, extending along the b-axis of the unit cell.
o-Aminophenol (5.45g, 0.01mole) was taken in 100mL round bottom flask. Salicylaldehyde (6.10g, 0.01mole) was added to the round bottom flask in methanol medium. The resulting mixture was refluxed for about 30 min. The resulting Schiff base was separated as orange crystals. The product was filtered, washed and recrystallized from methanol (M.P.134-135 0C, Yield 75%). Single crystals of the compound were grown by slow evaporation method using ethanol as solvent at room temperature.
N-substituted imines, also known as Schiff bases represent one of the most widely used families of organic compounds. Schiff bases have been intensively used as synthetic intermediates and as ligands for coordinating transition and inner transition metal ions, and recently also for coordinating anions. Schiff base ligands may contain a variety of substituents with different electron-donating or electron-withdrawing groups, and therefore may have interesting chemical properties. They have attracted particular interest due to their biological activities acting as radiopharmaceuticals for cancer targeting.They have also been used as model systems for biological macromolecules . Besides the biological activity, solid-state thermochromism and photochromism are an another characteristic of these compounds leading to their application in various areas of materials science such as the control and measurement of radiation intensity, display systems and optical memory devices . Schiff bases derived from o-hydroxyaromatic aldehydes and ketones are excellent models for the study of keto-enol tautomerism both in solution and in the solid state (Blagus et al., 2010).
The structure of the title compound is as shown in Fig.1 is described in terms of three planar subunits,namely two terminal benzene rings and their substituents bridged by a C=N moiety. The molecule has adopted E-configuration about the C8—N1 double bond (1.301 (2)Å) with a C9—N1—C8—C4 torsion angle of 179.90 (16)°. The C4—C8 and N1—C9 bond distances [1.410 (2) and 1.404 (2)Å] confirm π-electron delocalisation between the phenyl rings. The N1—C8—C4[123.26 (15)°] is greater than the normal value of 120°. This may be due to interaction of iminium H with phenolate O atom. The C6—C5—C4 [116.51 (15)°] is smaller than the normal value of 120° which is due to lengthening of the phenolate C5—O1 [1.304 (2)Å] bond. All other bond distances and bond angles are within the normal range (Eltayeb et al., 2010).
The iminium H atom is engaged in a strong intramolecular hydrogen bond with the O atom of the phenolate (N+ —H···O ) to form a S(6) motif. The crystal structure is stabilised by both intramolecular N1—H1···O1 and intermolecular O2—H4···O1 hydrogen bonding linking the molecules into infinite one-dimensional chains as shown in the figure.2, table.2, extending along the b-axis of the unit cell.
For a related structure, see: Eltayeb et al. (2010). For background to Schiff bases and their applications, see: Blagus et al. (2010).
o-Aminophenol (5.45g, 0.01mole) was taken in 100mL round bottom flask. Salicylaldehyde (6.10g, 0.01mole) was added to the round bottom flask in methanol medium. The resulting mixture was refluxed for about 30 min. The resulting Schiff base was separated as orange crystals. The product was filtered, washed and recrystallized from methanol (M.P.134-135 0C, Yield 75%). Single crystals of the compound were grown by slow evaporation method using ethanol as solvent at room temperature.
Crystal data, data collection and structure refinement details are summarized in Table 1.
Data collection: APEX2 (Bruker, 2009); cell refinement: SAINT (Bruker, 2009); data reduction: SAINT (Bruker, 2009); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL2014 (Sheldrick, 2015); molecular graphics: ORTEP-3 for Windows (Farrugia, 2012) and PLATON (Spek, 2009); software used to prepare material for publication: SHELXL2014 (Sheldrick, 2015) and PLATON (Spek, 2009).
C14H13NO2 | Dx = 1.313 Mg m−3 |
Mr = 227.25 | Melting point: 355 K |
Orthorhombic, Pbca | Mo Kα radiation, λ = 0.71073 Å |
a = 12.9474 (18) Å | Cell parameters from 500 reflections |
b = 9.0660 (13) Å | θ = 5.0–50.0° |
c = 19.583 (3) Å | µ = 0.09 mm−1 |
V = 2298.7 (6) Å3 | T = 293 K |
Z = 8 | Block, colorless |
F(000) = 960 | 0.3 × 0.25 × 0.20 mm |
Bruker APEXII CCD diffractometer | 1810 reflections with I > 2σ(I) |
Radiation source: graphite monochromator | Rint = 0.059 |
OMEGA–PHI scans | θmax = 27.6°, θmin = 2.6° |
Absorption correction: multi-scan (SADABS; Bruker, 2009) | h = −16→16 |
Tmin = 0.875, Tmax = 1.000 | k = −11→8 |
29481 measured reflections | l = −25→25 |
2583 independent reflections |
Refinement on F2 | 2 restraints |
Least-squares matrix: full | Hydrogen site location: mixed |
R[F2 > 2σ(F2)] = 0.050 | H atoms treated by a mixture of independent and constrained refinement |
wR(F2) = 0.130 | w = 1/[σ2(Fo2) + (0.0467P)2 + 1.0454P] where P = (Fo2 + 2Fc2)/3 |
S = 1.05 | (Δ/σ)max = 0.015 |
2583 reflections | Δρmax = 0.21 e Å−3 |
163 parameters | Δρmin = −0.20 e Å−3 |
C14H13NO2 | V = 2298.7 (6) Å3 |
Mr = 227.25 | Z = 8 |
Orthorhombic, Pbca | Mo Kα radiation |
a = 12.9474 (18) Å | µ = 0.09 mm−1 |
b = 9.0660 (13) Å | T = 293 K |
c = 19.583 (3) Å | 0.3 × 0.25 × 0.20 mm |
Bruker APEXII CCD diffractometer | 2583 independent reflections |
Absorption correction: multi-scan (SADABS; Bruker, 2009) | 1810 reflections with I > 2σ(I) |
Tmin = 0.875, Tmax = 1.000 | Rint = 0.059 |
29481 measured reflections |
R[F2 > 2σ(F2)] = 0.050 | 2 restraints |
wR(F2) = 0.130 | H atoms treated by a mixture of independent and constrained refinement |
S = 1.05 | Δρmax = 0.21 e Å−3 |
2583 reflections | Δρmin = −0.20 e Å−3 |
163 parameters |
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. |
x | y | z | Uiso*/Ueq | ||
H1 | 0.6541 (13) | 0.138 (3) | 0.2650 (11) | 0.063 (7)* | |
H4 | 0.5002 (18) | 0.378 (3) | 0.1982 (14) | 0.099 (9)* | |
N1 | 0.71804 (10) | 0.16956 (16) | 0.25537 (7) | 0.0328 (3) | |
C8 | 0.78912 (12) | 0.1022 (2) | 0.29051 (8) | 0.0345 (4) | |
H8 | 0.8579 | 0.1254 | 0.2819 | 0.041* | |
O1 | 0.58630 (9) | 0.00525 (16) | 0.31990 (7) | 0.0465 (4) | |
C9 | 0.73191 (11) | 0.2767 (2) | 0.20440 (8) | 0.0315 (4) | |
O2 | 0.55197 (9) | 0.31121 (17) | 0.20963 (7) | 0.0494 (4) | |
C14 | 0.64308 (12) | 0.3480 (2) | 0.18036 (9) | 0.0350 (4) | |
C5 | 0.66350 (13) | −0.0477 (2) | 0.35492 (9) | 0.0358 (4) | |
C10 | 0.82779 (13) | 0.3143 (2) | 0.17751 (9) | 0.0389 (4) | |
H10 | 0.8872 | 0.2685 | 0.1937 | 0.047* | |
C4 | 0.76708 (12) | −0.0042 (2) | 0.34097 (8) | 0.0335 (4) | |
C2 | 0.83378 (15) | −0.1684 (2) | 0.42880 (10) | 0.0451 (5) | |
C13 | 0.65167 (14) | 0.4516 (2) | 0.12897 (9) | 0.0415 (5) | |
H13 | 0.5928 | 0.4982 | 0.1124 | 0.050* | |
C6 | 0.64951 (14) | −0.1513 (2) | 0.40786 (9) | 0.0441 (5) | |
H6 | 0.5830 | −0.1815 | 0.4191 | 0.053* | |
C11 | 0.83474 (14) | 0.4189 (2) | 0.12694 (10) | 0.0462 (5) | |
H11 | 0.8990 | 0.4445 | 0.1094 | 0.055* | |
C3 | 0.84905 (13) | −0.0673 (2) | 0.37804 (9) | 0.0418 (5) | |
H3 | 0.9163 | −0.0390 | 0.3676 | 0.050* | |
C7 | 0.73159 (15) | −0.2085 (2) | 0.44311 (9) | 0.0461 (5) | |
H7 | 0.7190 | −0.2763 | 0.4778 | 0.055* | |
C12 | 0.74692 (16) | 0.4864 (2) | 0.10209 (9) | 0.0457 (5) | |
H12 | 0.7520 | 0.5554 | 0.0671 | 0.055* | |
C1 | 0.92146 (18) | −0.2371 (3) | 0.46830 (12) | 0.0691 (7) | |
H1A | 0.9742 | −0.2687 | 0.4372 | 0.104* | |
H1B | 0.8963 | −0.3205 | 0.4935 | 0.104* | |
H1C | 0.9497 | −0.1658 | 0.4994 | 0.104* |
U11 | U22 | U33 | U12 | U13 | U23 | |
N1 | 0.0232 (6) | 0.0327 (9) | 0.0425 (8) | −0.0010 (6) | −0.0004 (6) | −0.0013 (6) |
C8 | 0.0243 (7) | 0.0355 (11) | 0.0437 (9) | −0.0001 (7) | −0.0016 (7) | −0.0035 (8) |
O1 | 0.0253 (6) | 0.0571 (10) | 0.0572 (8) | −0.0049 (6) | −0.0043 (5) | 0.0051 (7) |
C9 | 0.0267 (8) | 0.0304 (10) | 0.0372 (8) | −0.0001 (7) | −0.0005 (6) | −0.0027 (7) |
O2 | 0.0249 (6) | 0.0582 (10) | 0.0651 (9) | 0.0050 (6) | 0.0004 (6) | 0.0148 (7) |
C14 | 0.0271 (8) | 0.0381 (11) | 0.0398 (9) | 0.0005 (7) | −0.0008 (7) | −0.0029 (8) |
C5 | 0.0305 (8) | 0.0360 (11) | 0.0410 (9) | −0.0041 (7) | 0.0000 (7) | −0.0059 (8) |
C10 | 0.0281 (8) | 0.0410 (12) | 0.0477 (10) | 0.0032 (7) | 0.0011 (7) | −0.0013 (8) |
C4 | 0.0289 (8) | 0.0332 (10) | 0.0383 (8) | −0.0017 (7) | −0.0016 (7) | −0.0022 (7) |
C2 | 0.0450 (10) | 0.0474 (13) | 0.0429 (10) | 0.0017 (9) | −0.0054 (8) | 0.0043 (9) |
C13 | 0.0381 (9) | 0.0443 (12) | 0.0423 (10) | 0.0050 (8) | −0.0062 (8) | 0.0023 (8) |
C6 | 0.0378 (9) | 0.0485 (13) | 0.0459 (10) | −0.0095 (8) | 0.0057 (8) | 0.0001 (9) |
C11 | 0.0377 (10) | 0.0494 (13) | 0.0516 (11) | −0.0049 (9) | 0.0109 (8) | 0.0016 (9) |
C3 | 0.0288 (8) | 0.0483 (13) | 0.0482 (10) | 0.0004 (8) | −0.0034 (7) | 0.0044 (9) |
C7 | 0.0528 (11) | 0.0463 (13) | 0.0392 (9) | −0.0045 (9) | 0.0019 (8) | 0.0038 (9) |
C12 | 0.0516 (11) | 0.0447 (13) | 0.0408 (9) | −0.0021 (9) | 0.0033 (9) | 0.0053 (9) |
C1 | 0.0560 (13) | 0.085 (2) | 0.0662 (14) | 0.0045 (12) | −0.0112 (11) | 0.0278 (14) |
N1—C8 | 1.301 (2) | C2—C3 | 1.367 (3) |
N1—C9 | 1.404 (2) | C2—C7 | 1.400 (3) |
N1—H1 | 0.895 (16) | C2—C1 | 1.508 (3) |
C8—C4 | 1.410 (2) | C13—C12 | 1.377 (3) |
C8—H8 | 0.9300 | C13—H13 | 0.9300 |
O1—C5 | 1.304 (2) | C6—C7 | 1.369 (3) |
C9—C10 | 1.391 (2) | C6—H6 | 0.9300 |
C9—C14 | 1.401 (2) | C11—C12 | 1.380 (3) |
O2—C14 | 1.353 (2) | C11—H11 | 0.9300 |
O2—H4 | 0.932 (17) | C3—H3 | 0.9300 |
C14—C13 | 1.381 (3) | C7—H7 | 0.9300 |
C5—C6 | 1.410 (3) | C12—H12 | 0.9300 |
C5—C4 | 1.424 (2) | C1—H1A | 0.9600 |
C10—C11 | 1.374 (3) | C1—H1B | 0.9600 |
C10—H10 | 0.9300 | C1—H1C | 0.9600 |
C4—C3 | 1.407 (2) | ||
C8—N1—C9 | 127.59 (14) | C12—C13—C14 | 120.40 (17) |
C8—N1—H1 | 113.3 (15) | C12—C13—H13 | 119.8 |
C9—N1—H1 | 119.1 (15) | C14—C13—H13 | 119.8 |
N1—C8—C4 | 123.26 (15) | C7—C6—C5 | 121.52 (17) |
N1—C8—H8 | 118.4 | C7—C6—H6 | 119.2 |
C4—C8—H8 | 118.4 | C5—C6—H6 | 119.2 |
C10—C9—C14 | 119.50 (16) | C10—C11—C12 | 120.41 (17) |
C10—C9—N1 | 123.55 (15) | C10—C11—H11 | 119.8 |
C14—C9—N1 | 116.95 (14) | C12—C11—H11 | 119.8 |
C14—O2—H4 | 111.4 (18) | C2—C3—C4 | 122.59 (17) |
O2—C14—C13 | 123.12 (15) | C2—C3—H3 | 118.7 |
O2—C14—C9 | 117.36 (16) | C4—C3—H3 | 118.7 |
C13—C14—C9 | 119.52 (15) | C6—C7—C2 | 122.30 (18) |
O1—C5—C6 | 122.24 (16) | C6—C7—H7 | 118.9 |
O1—C5—C4 | 121.25 (16) | C2—C7—H7 | 118.9 |
C6—C5—C4 | 116.51 (16) | C13—C12—C11 | 120.12 (18) |
C11—C10—C9 | 120.02 (16) | C13—C12—H12 | 119.9 |
C11—C10—H10 | 120.0 | C11—C12—H12 | 119.9 |
C9—C10—H10 | 120.0 | C2—C1—H1A | 109.5 |
C3—C4—C8 | 119.13 (15) | C2—C1—H1B | 109.5 |
C3—C4—C5 | 119.91 (16) | H1A—C1—H1B | 109.5 |
C8—C4—C5 | 120.96 (15) | C2—C1—H1C | 109.5 |
C3—C2—C7 | 117.15 (17) | H1A—C1—H1C | 109.5 |
C3—C2—C1 | 122.77 (18) | H1B—C1—H1C | 109.5 |
C7—C2—C1 | 120.08 (18) | ||
C9—N1—C8—C4 | 179.90 (16) | O2—C14—C13—C12 | 178.77 (18) |
C8—N1—C9—C10 | 8.4 (3) | C9—C14—C13—C12 | −0.9 (3) |
C8—N1—C9—C14 | −171.45 (17) | O1—C5—C6—C7 | 178.47 (18) |
C10—C9—C14—O2 | −177.89 (16) | C4—C5—C6—C7 | −1.0 (3) |
N1—C9—C14—O2 | 2.0 (2) | C9—C10—C11—C12 | −0.6 (3) |
C10—C9—C14—C13 | 1.8 (3) | C7—C2—C3—C4 | 0.1 (3) |
N1—C9—C14—C13 | −178.31 (16) | C1—C2—C3—C4 | 179.5 (2) |
C14—C9—C10—C11 | −1.1 (3) | C8—C4—C3—C2 | 178.41 (19) |
N1—C9—C10—C11 | 179.06 (17) | C5—C4—C3—C2 | −1.3 (3) |
N1—C8—C4—C3 | −177.72 (17) | C5—C6—C7—C2 | −0.2 (3) |
N1—C8—C4—C5 | 2.0 (3) | C3—C2—C7—C6 | 0.7 (3) |
O1—C5—C4—C3 | −177.76 (17) | C1—C2—C7—C6 | −178.8 (2) |
C6—C5—C4—C3 | 1.7 (3) | C14—C13—C12—C11 | −0.8 (3) |
O1—C5—C4—C8 | 2.5 (3) | C10—C11—C12—C13 | 1.5 (3) |
C6—C5—C4—C8 | −177.99 (17) |
D—H···A | D—H | H···A | D···A | D—H···A |
O2—H4···O1i | 0.93 (2) | 1.65 (2) | 2.5756 (18) | 176 (3) |
N1—H1···O2 | 0.90 (2) | 2.32 (2) | 2.6598 (19) | 102 (2) |
N1—H1···O1 | 0.90 (2) | 1.84 (2) | 2.5933 (19) | 141 (2) |
Symmetry code: (i) −x+1, y+1/2, −z+1/2. |
D—H···A | D—H | H···A | D···A | D—H···A |
O2—H4···O1i | 0.932 (17) | 1.645 (17) | 2.5756 (18) | 176 (3) |
N1—H1···O2 | 0.896 (18) | 2.32 (2) | 2.6598 (19) | 102.2 (19) |
N1—H1···O1 | 0.896 (18) | 1.84 (2) | 2.5933 (19) | 141 (2) |
Symmetry code: (i) −x+1, y+1/2, −z+1/2. |