Abstract
In the title compound, C14H13NO2, the mean planes through the benzyl and 2-hydoxybenzamide units make a dihedral angle of 68.81 (7)°. There is an intramolecular O—H⋯O hydrogen bond involving the carbonyl O atom and the 2-hydroxy substituent. In the crystal structure, N—H⋯O hydrogen bonds link symmetry-related molecules into one-dimensional chains extending along the a-axis direction. These chains are further connected via C—H⋯O hydrogen bonds, forming a sheet-like structure
Related literature
For related literature, see: Agwade (1982 ▶); Allen et al. (1987 ▶).
Experimental
Crystal data
C14H13NO2
M r = 227.25
Monoclinic,
a = 12.478 (3) Å
b = 8.3503 (17) Å
c = 12.664 (3) Å
β = 118.02 (3)°
V = 1164.9 (6) Å3
Z = 4
Mo Kα radiation
μ = 0.09 mm−1
T = 290 (2) K
0.33 × 0.22 × 0.20 mm
Data collection
Rigaku R-AXIS RAPID diffractometer
Absorption correction: multi-scan (ABSCOR; Higashi, 1995 ▶) T min = 0.977, T max = 0.983
11112 measured reflections
2665 independent reflections
1648 reflections with I > 2σ(I)
R int = 0.037
Refinement
R[F 2 > 2σ(F 2)] = 0.043
wR(F 2) = 0.116
S = 1.03
2665 reflections
207 parameters
All H-atom parameters refined
Δρmax = 0.17 e Å−3
Δρmin = −0.14 e Å−3
Data collection: RAPID-AUTO (Rigaku, 1998 ▶); cell refinement: RAPID-AUTO; data reduction: CrystalStructure (Rigaku/MSC, 2002 ▶); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: SHELXTL (Sheldrick, 2008 ▶); software used to prepare material for publication: SHELXL97.
Supplementary Material
Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536808010453/su2048sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536808010453/su2048Isup2.hkl
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 |
|---|---|---|---|---|
| N1—HN1⋯O1i | 0.882 (18) | 2.083 (18) | 2.9191 (18) | 158.1 (18) |
| O1—HO1⋯O2 | 0.98 (3) | 1.56 (3) | 2.4886 (19) | 157 (2) |
| C2—H2⋯O1i | 0.956 (19) | 2.58 (2) | 3.507 (2) | 162.5 (15) |
Symmetry code: (i)
.
Acknowledgments
The authors gratefully acknowledge the financial support of the Education Office of Zhejiang Province (grant No. 20051316).
supplementary crystallographic information
Comment
Over a quater of a century ago (Agwade, 1982) published a thesis on Potential Central Nervous System Active Agents, which included the synthesis of aromatic N-benzyl amides. One of the compounds synthesized was N-benzyl-2-hydroxy-benzamide, (I), whose crystal structure has not been descibed until now.
The molecular structure of compound I is illustrated in Fig. 1. The bond lengths and angles are close to normal values (Allen et al., 1987). There is an intramolecular O-H···O hydrogen bond in the molecule involving the carbonyl O-atom and the 2-hydroxyl substituent (Table 1). The best planes through the benzyl (atoms C8,C9-C14) and the 2-hydoxybenzamide (atoms C1-C6,C7,N1,O1,O2) moieties are inclined to one another by 68.81 (7)°.
In the crystal structure of I symmetry related molecules are connected via an N-H···O hydrogen bond to form chains running along the a direction. These chains are further connected connected via C-H···O hydrogen bonds (Table 1) to form a sheet-like structure (Fig 2).
Experimental
Freshly prepared CuCO3 (0.310 g 2.50 mmol), [C6H4(COOC6H4CONHCH2ph)2](0.350 g 0.601 mmol), 2-chloro-benzoic acid (0.160 g 1.022 mmol), and 15 ml CH3OH/H2O (1:2,v/v) were mixed and stirred for ca. 1.5 h. The resulting suspension was heated in a 23 ml Teflon-lined stainless steel autoclave at 373 K for 7 days. After the autoclave was cooled to room temperature, and colorless block-like crystals, suitable for X-ray analysis, were obtained.
Refinement
All of the H atoms were located in difference Fourier syntheses and were freely refined: O-H = 0.98 (3), N-H = 0.882 (18), and C-H = 0.94 (2) - 1.010 (16) Å.
Figures
Fig. 1.
A view of the moleculecular structure of I, showing the atom-labelling scheme. Displacement ellipsoids are drawn at the 40% probability level.
Fig. 2.
The crystal packing diagram for compound I, viewed down the b axis. Dashed lines indicate N-H···O hydrogen bonds.
Crystal data
| C14H13NO2 | F000 = 480 |
| Mr = 227.25 | Dx = 1.296 Mg m−3 |
| Monoclinic, P21/n | Mo Kα radiation λ = 0.71073 Å |
| Hall symbol: -P 2yn | Cell parameters from 6913 reflections |
| a = 12.478 (3) Å | θ = 3.0–27.5º |
| b = 8.3503 (17) Å | µ = 0.09 mm−1 |
| c = 12.664 (3) Å | T = 290 (2) K |
| β = 118.02 (3)º | Block, colorless |
| V = 1164.9 (6) Å3 | 0.33 × 0.22 × 0.20 mm |
| Z = 4 |
Data collection
| Rigaku R-AXIS RAPID diffractometer | 2665 independent reflections |
| Radiation source: fine-focus sealed tube | 1648 reflections with I > 2σ(I) |
| Monochromator: graphite | Rint = 0.037 |
| Detector resolution: 10 pixels mm-1 | θmax = 27.5º |
| T = 290(2) K | θmin = 3.0º |
| ω scans | h = −15→16 |
| Absorption correction: multi-scan(ABSCOR; Higashi, 1995) | k = −10→10 |
| Tmin = 0.977, Tmax = 0.983 | l = −16→16 |
| 11112 measured reflections |
Refinement
| Refinement on F2 | Hydrogen site location: inferred from neighbouring sites |
| Least-squares matrix: full | All H-atom parameters refined |
| R[F2 > 2σ(F2)] = 0.043 | w = 1/[σ2(Fo2) + (0.0564P)2 + 0.0491P] where P = (Fo2 + 2Fc2)/3 |
| wR(F2) = 0.116 | (Δ/σ)max < 0.001 |
| S = 1.03 | Δρmax = 0.17 e Å−3 |
| 2665 reflections | Δρmin = −0.14 e Å−3 |
| 207 parameters | Extinction correction: SHELXL97 (Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4 |
| Primary atom site location: structure-invariant direct methods | Extinction coefficient: 0.011 (2) |
| Secondary atom site location: difference Fourier map |
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 esds are taken into account in the estimation of distances, angles and torsion angles |
| 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 | ||
| O1 | 0.29704 (10) | 0.74227 (17) | −0.23736 (9) | 0.0731 (4) | |
| O2 | 0.49480 (9) | 0.60089 (14) | −0.16419 (9) | 0.0600 (4) | |
| N1 | 0.64585 (9) | 0.63326 (15) | 0.02206 (11) | 0.0449 (4) | |
| C1 | 0.45255 (11) | 0.76116 (16) | −0.03318 (11) | 0.0396 (4) | |
| C2 | 0.48553 (14) | 0.82179 (19) | 0.07995 (14) | 0.0493 (5) | |
| C3 | 0.40715 (15) | 0.9140 (2) | 0.10230 (16) | 0.0592 (6) | |
| C4 | 0.29300 (15) | 0.9477 (2) | 0.01061 (17) | 0.0604 (6) | |
| C5 | 0.25762 (14) | 0.8909 (2) | −0.10172 (16) | 0.0576 (6) | |
| C6 | 0.33637 (12) | 0.79771 (18) | −0.12499 (13) | 0.0478 (5) | |
| C7 | 0.53270 (11) | 0.66022 (17) | −0.06264 (12) | 0.0412 (4) | |
| C8 | 0.73259 (14) | 0.5375 (2) | 0.00128 (16) | 0.0508 (5) | |
| C9 | 0.80422 (12) | 0.63678 (17) | −0.04347 (14) | 0.0460 (5) | |
| C10 | 0.92320 (15) | 0.6768 (3) | 0.03099 (19) | 0.0722 (7) | |
| C11 | 0.98716 (18) | 0.7699 (3) | −0.0108 (2) | 0.0875 (9) | |
| C12 | 0.9333 (2) | 0.8228 (3) | −0.1254 (2) | 0.0785 (9) | |
| C13 | 0.81540 (19) | 0.7850 (3) | −0.20000 (19) | 0.0721 (8) | |
| C14 | 0.75139 (16) | 0.6917 (2) | −0.15893 (16) | 0.0596 (6) | |
| HN1 | 0.6728 (14) | 0.6819 (19) | 0.0917 (16) | 0.059 (5)* | |
| H2 | 0.5651 (15) | 0.7995 (18) | 0.1431 (15) | 0.060 (5)* | |
| HO1 | 0.367 (2) | 0.681 (3) | −0.230 (2) | 0.106 (7)* | |
| H3 | 0.4331 (15) | 0.952 (2) | 0.1817 (17) | 0.078 (5)* | |
| H4 | 0.2386 (15) | 1.009 (2) | 0.0252 (15) | 0.071 (5)* | |
| H5 | 0.1770 (17) | 0.913 (2) | −0.1697 (16) | 0.081 (5)* | |
| H8A | 0.6833 (14) | 0.455 (2) | −0.0610 (14) | 0.062 (5)* | |
| H8B | 0.7896 (14) | 0.4913 (19) | 0.0805 (15) | 0.062 (5)* | |
| H10 | 0.9607 (17) | 0.633 (2) | 0.1088 (19) | 0.087 (6)* | |
| H11 | 1.070 (2) | 0.793 (3) | 0.042 (2) | 0.107 (7)* | |
| H12 | 0.9743 (19) | 0.887 (3) | −0.1597 (18) | 0.099 (7)* | |
| H13 | 0.7716 (18) | 0.825 (3) | −0.283 (2) | 0.098 (7)* | |
| H14 | 0.6696 (16) | 0.668 (2) | −0.2122 (15) | 0.070 (5)* |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| O1 | 0.0512 (6) | 0.1059 (10) | 0.0395 (6) | 0.0150 (7) | 0.0024 (5) | −0.0056 (6) |
| O2 | 0.0503 (6) | 0.0798 (8) | 0.0421 (6) | 0.0005 (5) | 0.0152 (5) | −0.0147 (5) |
| N1 | 0.0376 (6) | 0.0549 (8) | 0.0399 (7) | 0.0001 (5) | 0.0162 (5) | 0.0025 (6) |
| C1 | 0.0369 (6) | 0.0420 (8) | 0.0378 (7) | −0.0052 (6) | 0.0159 (5) | 0.0030 (6) |
| C2 | 0.0465 (8) | 0.0557 (10) | 0.0433 (8) | −0.0040 (7) | 0.0190 (7) | −0.0014 (7) |
| C3 | 0.0664 (10) | 0.0594 (10) | 0.0604 (11) | −0.0070 (8) | 0.0370 (9) | −0.0106 (8) |
| C4 | 0.0586 (10) | 0.0493 (10) | 0.0853 (13) | 0.0013 (8) | 0.0438 (9) | 0.0000 (9) |
| C5 | 0.0440 (8) | 0.0553 (10) | 0.0696 (11) | 0.0052 (7) | 0.0235 (8) | 0.0109 (8) |
| C6 | 0.0408 (7) | 0.0533 (9) | 0.0436 (8) | −0.0018 (7) | 0.0150 (6) | 0.0048 (7) |
| C7 | 0.0379 (7) | 0.0458 (8) | 0.0374 (8) | −0.0052 (6) | 0.0156 (5) | 0.0021 (6) |
| C8 | 0.0454 (8) | 0.0501 (9) | 0.0583 (10) | 0.0065 (7) | 0.0256 (7) | 0.0099 (8) |
| C9 | 0.0447 (7) | 0.0410 (8) | 0.0558 (9) | 0.0018 (6) | 0.0266 (6) | −0.0020 (7) |
| C10 | 0.0477 (9) | 0.0840 (14) | 0.0753 (13) | −0.0025 (9) | 0.0209 (8) | 0.0173 (11) |
| C11 | 0.0510 (11) | 0.0993 (17) | 0.1074 (18) | −0.0151 (11) | 0.0333 (11) | 0.0117 (13) |
| C12 | 0.0808 (13) | 0.0764 (14) | 0.1031 (17) | −0.0141 (11) | 0.0639 (13) | −0.0013 (12) |
| C13 | 0.0835 (13) | 0.0814 (14) | 0.0652 (12) | −0.0113 (10) | 0.0464 (10) | 0.0005 (10) |
| C14 | 0.0579 (10) | 0.0695 (11) | 0.0538 (10) | −0.0107 (8) | 0.0283 (8) | −0.0039 (8) |
Geometric parameters (Å, °)
| O1—C6 | 1.3506 (18) | C10—C11 | 1.385 (3) |
| O2—C7 | 1.2456 (17) | C11—C12 | 1.355 (3) |
| O1—HO1 | 0.98 (3) | C12—C13 | 1.360 (4) |
| N1—C7 | 1.3311 (19) | C13—C14 | 1.381 (3) |
| N1—C8 | 1.466 (2) | C2—H2 | 0.956 (19) |
| N1—HN1 | 0.882 (18) | C3—H3 | 0.954 (19) |
| C1—C7 | 1.483 (2) | C4—H4 | 0.94 (2) |
| C1—C6 | 1.401 (2) | C5—H5 | 0.99 (2) |
| C1—C2 | 1.387 (2) | C8—H8A | 1.010 (16) |
| C2—C3 | 1.375 (3) | C8—H8B | 0.995 (17) |
| C3—C4 | 1.379 (3) | C10—H10 | 0.94 (2) |
| C4—C5 | 1.361 (3) | C11—H11 | 0.95 (3) |
| C5—C6 | 1.389 (3) | C12—H12 | 0.97 (3) |
| C8—C9 | 1.511 (3) | C13—H13 | 0.99 (2) |
| C9—C14 | 1.370 (2) | C14—H14 | 0.94 (2) |
| C9—C10 | 1.375 (3) | ||
| O1···O2 | 2.4886 (19) | C9···H4iv | 3.034 (17) |
| O1···N1i | 2.9191 (18) | C14···H4iv | 2.989 (17) |
| O2···C14 | 3.260 (3) | HN1···C2 | 2.554 (19) |
| O2···O1 | 2.4886 (19) | HN1···H2 | 2.00 (3) |
| O1···H2i | 2.58 (2) | HN1···O1iii | 2.083 (18) |
| O1···HN1i | 2.083 (18) | H2···N1 | 2.597 (18) |
| O2···HO1 | 1.56 (3) | H2···HN1 | 2.00 (3) |
| O2···H8A | 2.416 (18) | H2···O1iii | 2.58 (2) |
| O2···H14 | 2.59 (2) | HO1···O2 | 1.56 (3) |
| O2···H5ii | 2.692 (19) | HO1···C7 | 2.16 (2) |
| N1···O1iii | 2.9191 (18) | HO1···H5ii | 2.50 (3) |
| N1···H2 | 2.597 (18) | H4···C9iv | 3.034 (17) |
| C1···C3iv | 3.554 (2) | H4···C14iv | 2.989 (17) |
| C1···C8v | 3.549 (2) | H5···O2vi | 2.692 (19) |
| C3···C1iv | 3.554 (2) | H5···HO1vi | 2.50 (3) |
| C6···C8v | 3.507 (2) | H8A···O2 | 2.416 (18) |
| C7···C7v | 3.400 (2) | H8A···H14 | 2.56 (2) |
| C7···C14 | 3.483 (3) | H8A···H13vii | 2.54 (3) |
| C8···C1v | 3.549 (2) | H8A···C1v | 3.075 (18) |
| C8···C6v | 3.507 (2) | H8A···C2v | 3.060 (18) |
| C14···C7 | 3.483 (3) | H8B···H10 | 2.32 (3) |
| C14···O2 | 3.260 (3) | H8B···C6v | 3.073 (17) |
| C1···H8Av | 3.075 (18) | H10···H8B | 2.32 (3) |
| C2···H8Av | 3.060 (18) | H13···H8Aviii | 2.54 (3) |
| C2···HN1 | 2.554 (19) | H14···O2 | 2.59 (2) |
| C6···H8Bv | 3.073 (17) | H14···C7 | 3.09 (2) |
| C7···H14 | 3.09 (2) | H14···H8A | 2.56 (2) |
| C7···HO1 | 2.16 (2) | ||
| C6—O1—HO1 | 102.3 (13) | C9—C14—C13 | 121.17 (19) |
| C7—N1—C8 | 122.74 (13) | C1—C2—H2 | 118.7 (11) |
| C7—N1—HN1 | 119.3 (12) | C3—C2—H2 | 119.8 (11) |
| C8—N1—HN1 | 117.7 (13) | C2—C3—H3 | 118.8 (12) |
| C6—C1—C7 | 118.17 (12) | C4—C3—H3 | 121.6 (12) |
| C2—C1—C6 | 117.83 (15) | C3—C4—H4 | 120.2 (11) |
| C2—C1—C7 | 124.00 (14) | C5—C4—H4 | 119.2 (11) |
| C1—C2—C3 | 121.50 (16) | C4—C5—H5 | 122.9 (12) |
| C2—C3—C4 | 119.62 (17) | C6—C5—H5 | 116.9 (12) |
| C3—C4—C5 | 120.55 (19) | N1—C8—H8A | 106.4 (11) |
| C4—C5—C6 | 120.15 (17) | N1—C8—H8B | 105.6 (11) |
| C1—C6—C5 | 120.35 (14) | C9—C8—H8A | 109.4 (10) |
| O1—C6—C1 | 121.46 (15) | C9—C8—H8B | 108.8 (11) |
| O1—C6—C5 | 118.19 (15) | H8A—C8—H8B | 114.1 (13) |
| O2—C7—C1 | 120.79 (13) | C9—C10—H10 | 117.9 (14) |
| O2—C7—N1 | 120.61 (14) | C11—C10—H10 | 121.6 (14) |
| N1—C7—C1 | 118.60 (12) | C10—C11—H11 | 118.5 (15) |
| N1—C8—C9 | 112.64 (13) | C12—C11—H11 | 121.0 (15) |
| C8—C9—C10 | 120.97 (16) | C11—C12—H12 | 123.9 (13) |
| C8—C9—C14 | 120.74 (16) | C13—C12—H12 | 116.2 (13) |
| C10—C9—C14 | 118.28 (18) | C12—C13—H13 | 122.5 (15) |
| C9—C10—C11 | 120.3 (2) | C14—C13—H13 | 117.6 (15) |
| C10—C11—C12 | 120.5 (2) | C9—C14—H14 | 120.7 (11) |
| C11—C12—C13 | 119.9 (2) | C13—C14—H14 | 118.2 (11) |
| C12—C13—C14 | 119.8 (2) | ||
| C8—N1—C7—O2 | 1.6 (2) | C2—C3—C4—C5 | −0.2 (3) |
| C8—N1—C7—C1 | −178.95 (14) | C3—C4—C5—C6 | 0.2 (3) |
| C7—N1—C8—C9 | 89.06 (18) | C4—C5—C6—O1 | 179.22 (16) |
| C6—C1—C2—C3 | 0.4 (2) | C4—C5—C6—C1 | 0.1 (2) |
| C7—C1—C2—C3 | −179.59 (16) | N1—C8—C9—C10 | 104.4 (2) |
| C2—C1—C6—O1 | −179.48 (15) | N1—C8—C9—C14 | −74.4 (2) |
| C2—C1—C6—C5 | −0.4 (2) | C8—C9—C10—C11 | −179.0 (2) |
| C7—C1—C6—O1 | 0.5 (2) | C14—C9—C10—C11 | −0.2 (3) |
| C7—C1—C6—C5 | 179.56 (15) | C8—C9—C14—C13 | 178.77 (18) |
| C2—C1—C7—O2 | 175.27 (15) | C10—C9—C14—C13 | −0.1 (3) |
| C2—C1—C7—N1 | −4.2 (2) | C9—C10—C11—C12 | 0.1 (4) |
| C6—C1—C7—O2 | −4.7 (2) | C10—C11—C12—C13 | 0.3 (4) |
| C6—C1—C7—N1 | 175.80 (14) | C11—C12—C13—C14 | −0.6 (4) |
| C1—C2—C3—C4 | −0.1 (3) | C12—C13—C14—C9 | 0.5 (3) |
Symmetry codes: (i) x−1/2, −y+3/2, z−1/2; (ii) −x+1/2, y−1/2, −z−1/2; (iii) x+1/2, −y+3/2, z+1/2; (iv) −x+1, −y+2, −z; (v) −x+1, −y+1, −z; (vi) −x+1/2, y+1/2, −z−1/2; (vii) −x+3/2, y−1/2, −z−1/2; (viii) −x+3/2, y+1/2, −z−1/2.
Hydrogen-bond geometry (Å, °)
| D—H···A | D—H | H···A | D···A | D—H···A |
| N1—HN1···O1iii | 0.882 (18) | 2.083 (18) | 2.9191 (18) | 158.1 (18) |
| O1—HO1···O2 | 0.98 (3) | 1.56 (3) | 2.4886 (19) | 157 (2) |
| C2—H2···O1iii | 0.956 (19) | 2.58 (2) | 3.507 (2) | 162.5 (15) |
| C14—H14···O2 | 0.94 (2) | 2.59 (2) | 3.260 (3) | 128.8 (14) |
Symmetry codes: (iii) x+1/2, −y+3/2, z+1/2.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: SU2048).
References
- Agwade, V. C. (1982). Chem. Eng. Data, 27, 479–481.
- Allen, F. H., Kennard, O., Watson, D. G., Brammer, L., Orpen, A. G. & Taylor, R. (1987). J. Chem. Soc. Perkin Trans. 2, pp. S1–19.
- Higashi, T. (1995). ABSCOR Rigaku Corporation, Tokyo, Japan.
- Rigaku (1998). RAPID-AUTO Rigaku Corporation, Tokyo, Japan.
- Rigaku/MSC (2002). CrystalStructure Rigaku Corporation, Tokyo, Japan.
- Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
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/S1600536808010453/su2048sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536808010453/su2048Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report


