Abstract
In the structure of the title compound (NP2MBA), C14H13NO, the conformation of the C—O bond is syn to the ortho-methyl substituent in the benzoyl phenyl ring, while the N—H bond is anti to the ortho-methyl substituent. The structure of NP2MBA closely resembles that of 2-chloro-N-phenylbenzamide, with similar bond parameters. The dihedral angle between the phenyl and benzoyl rings is 88.05 (5)°. Molecules are linked into a chain through N—H⋯O hydrogen bonding.
Related literature
For related literature, see: Gowda et al. (2003 ▶, 2007 ▶, 2008 ▶).
Experimental
Crystal data
C14H13NO
M r = 211.25
Orthorhombic,
a = 14.404 (1) Å
b = 8.6824 (6) Å
c = 18.710 (1) Å
V = 2339.9 (3) Å3
Z = 8
Mo Kα radiation
μ = 0.08 mm−1
T = 100 (2) K
0.40 × 0.20 × 0.16 mm
Data collection
Oxford Diffraction Xcalibur diffractometer with Sapphire CCD detector
Absorption correction: multi-scan (SCALE3 ABSPACK; Oxford Diffraction, 2007 ▶) T min = 0.970, T max = 0.981
11005 measured reflections
2387 independent reflections
1686 reflections with I > 2σ(I)
R int = 0.029
Refinement
R[F 2 > 2σ(F 2)] = 0.038
wR(F 2) = 0.115
S = 1.05
2387 reflections
149 parameters
H atoms treated by a mixture of independent and constrained refinement
Δρmax = 0.24 e Å−3
Δρmin = −0.21 e Å−3
Data collection: CrysAlis CCD (Oxford Diffraction, 2004 ▶); cell refinement: CrysAlis RED (Oxford Diffraction, 2007 ▶); data reduction: CrysAlis RED; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: PLATON (Spek, 2003 ▶); software used to prepare material for publication: SHELXS97.
Supplementary Material
Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536807068821/dn2308sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536807068821/dn2308Isup2.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—H1N⋯O1i | 0.878 (17) | 2.012 (18) | 2.8751 (16) | 167.7 (15) |
Symmetry code: (i)
.
Acknowledgments
BTG thanks the Alexander von Humboldt Foundation, Bonn, Germany, for extensions of his research fellowship.
supplementary crystallographic information
Comment
As part of a study of the substituent effects on the structures of benzanilides, in the present work, the structure of 2-methyl-N-(phenyl)benzamide (NP2MBA) has been determined (Gowda, et al., 2003; 2007; 2008). In the structure of NP2MBA,(Fig. 1), the conformation of the C—O bond is syn to the ortho-methyl substituent in the benzoyl phenyl ring, while the N—H bond is anti to the ortho-methyl substituent. The bond parameters in NP2MBA are similar to those in 2-chloro-N-(phenyl)-benzamide (Gowda, et al.,2003), 2-chloro-N-(2-chlorophenyl)-benzamide (Gowda, et al.,2007), N-(4-methylphenyl)-benzamide (Gowda, et al.,2008) and other benzanilides. The dihedral angle between the phenyl and benzoyl rings in NP2MBA is 88.05 (5)°. The packing diagram of NP2MBA molecules showing the hydrogen bonds N1—H1N···O1 (Table 1) involved in the formation of molecular chain is shown in Fig. 2.
Experimental
The title compound was prepared according to the literature method (Gowda et al., 2003). The purity of the compound was checked by determining its melting point. It was characterized by recording its infrared and NMR spectra. Single crystals of the title compound were obtained from an ethanolic solution and used for X-ray diffraction studies at room temperature.
Refinement
The NH atom was located in difference map with N—H = 0.88 (2) %A. The other H atoms were positioned with idealized geometry using a riding model with C—H = 0.95–0.98 Å A l l H atoms were refined with isotropic displacement parameters (set to 1.2 times of the Ueq of the parent atom).
Figures
Fig. 1.
Molecular structure of the title compound, showing the atom labeling scheme. The displacement ellipsoids are drawn at the 50% probability level. H atoms are represented as small spheres of arbitrary radii.
Fig. 2.
Molecular packing of the title compound with hydrogen bonding shown as dashed lines.H atoms not involved in hydrogen bondings have been omitted for clarity. [Symmetry code: (i) 3/2 - x, 1/2 + y, z]
Crystal data
| C14H13NO | F000 = 896 |
| Mr = 211.25 | Dx = 1.199 Mg m−3 |
| Orthorhombic, Pbca | Mo Kα radiation λ = 0.71073 Å |
| Hall symbol: -P 2ac 2ab | Cell parameters from 3291 reflections |
| a = 14.404 (1) Å | θ = 1.5–26.9º |
| b = 8.6824 (6) Å | µ = 0.08 mm−1 |
| c = 18.710 (1) Å | T = 100 (2) K |
| V = 2339.9 (3) Å3 | Rod, colourless |
| Z = 8 | 0.40 × 0.20 × 0.16 mm |
Data collection
| Oxford Diffraction Xcalibur diffractometer with Sapphire CCD Detector | 2387 independent reflections |
| Radiation source: fine-focus sealed tube | 1686 reflections with I > 2σ(I) |
| Monochromator: graphite | Rint = 0.029 |
| T = 100(2) K | θmax = 26.4º |
| Rotation method data acquisition using ω and φ scans. | θmin = 2.6º |
| Absorption correction: multi-scan(SCALE3 ABSPACK; Oxford Diffraction, 2007) | h = −17→17 |
| Tmin = 0.970, Tmax = 0.981 | k = −10→10 |
| 11005 measured reflections | l = −23→23 |
Refinement
| Refinement on F2 | Secondary atom site location: difference Fourier map |
| Least-squares matrix: full | Hydrogen site location: inferred from neighbouring sites |
| R[F2 > 2σ(F2)] = 0.038 | H atoms treated by a mixture of independent and constrained refinement |
| wR(F2) = 0.115 | w = 1/[σ2(Fo2) + (0.0589P)2 + 0.6762P] where P = (Fo2 + 2Fc2)/3 |
| S = 1.05 | (Δ/σ)max = 0.007 |
| 2387 reflections | Δρmax = 0.24 e Å−3 |
| 149 parameters | Δρmin = −0.21 e Å−3 |
| Primary atom site location: structure-invariant direct methods | Extinction correction: none |
Special details
| 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. |
| 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 | ||
| C1 | 0.69394 (10) | 0.28490 (16) | 0.53783 (8) | 0.0226 (3) | |
| C2 | 0.60165 (11) | 0.32710 (18) | 0.52773 (9) | 0.0298 (4) | |
| H2 | 0.5740 | 0.4029 | 0.5575 | 0.036* | |
| C3 | 0.55046 (12) | 0.2578 (2) | 0.47398 (10) | 0.0395 (5) | |
| H3 | 0.4876 | 0.2869 | 0.4667 | 0.047* | |
| C4 | 0.59039 (14) | 0.1463 (2) | 0.43075 (10) | 0.0421 (5) | |
| H4 | 0.5544 | 0.0966 | 0.3950 | 0.051* | |
| C5 | 0.68238 (13) | 0.1079 (2) | 0.43987 (9) | 0.0360 (4) | |
| H5 | 0.7102 | 0.0334 | 0.4094 | 0.043* | |
| C6 | 0.73475 (11) | 0.17696 (18) | 0.49311 (8) | 0.0276 (4) | |
| H6 | 0.7983 | 0.1505 | 0.4990 | 0.033* | |
| C7 | 0.80898 (9) | 0.28653 (16) | 0.63583 (7) | 0.0197 (3) | |
| C8 | 0.85208 (9) | 0.38985 (16) | 0.69023 (8) | 0.0203 (3) | |
| C9 | 0.85849 (9) | 0.34624 (16) | 0.76232 (8) | 0.0231 (3) | |
| C10 | 0.90322 (10) | 0.44704 (19) | 0.80890 (9) | 0.0284 (4) | |
| H10 | 0.9075 | 0.4210 | 0.8581 | 0.034* | |
| C11 | 0.94171 (11) | 0.58472 (19) | 0.78533 (9) | 0.0323 (4) | |
| H11 | 0.9735 | 0.6498 | 0.8180 | 0.039* | |
| C12 | 0.93373 (11) | 0.62687 (18) | 0.71470 (9) | 0.0310 (4) | |
| H12 | 0.9590 | 0.7218 | 0.6986 | 0.037* | |
| C13 | 0.88876 (10) | 0.53029 (16) | 0.66721 (9) | 0.0248 (4) | |
| H13 | 0.8828 | 0.5597 | 0.6185 | 0.030* | |
| C14 | 0.81853 (11) | 0.19677 (19) | 0.78942 (8) | 0.0311 (4) | |
| H14A | 0.8571 | 0.1108 | 0.7730 | 0.037* | |
| H14B | 0.7552 | 0.1842 | 0.7711 | 0.037* | |
| H14C | 0.8172 | 0.1981 | 0.8418 | 0.037* | |
| N1 | 0.74373 (8) | 0.35464 (14) | 0.59463 (7) | 0.0220 (3) | |
| H1N | 0.7283 (11) | 0.448 (2) | 0.6078 (9) | 0.026* | |
| O1 | 0.83366 (7) | 0.15084 (11) | 0.62885 (6) | 0.0245 (3) |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| C1 | 0.0295 (8) | 0.0138 (7) | 0.0244 (7) | −0.0039 (6) | −0.0054 (6) | 0.0032 (6) |
| C2 | 0.0308 (8) | 0.0223 (8) | 0.0362 (9) | −0.0009 (7) | −0.0051 (7) | 0.0040 (7) |
| C3 | 0.0335 (9) | 0.0373 (10) | 0.0477 (10) | −0.0048 (8) | −0.0176 (8) | 0.0095 (9) |
| C4 | 0.0563 (12) | 0.0291 (9) | 0.0410 (10) | −0.0117 (9) | −0.0223 (9) | 0.0006 (9) |
| C5 | 0.0541 (11) | 0.0221 (8) | 0.0316 (9) | −0.0039 (8) | −0.0079 (8) | −0.0018 (8) |
| C6 | 0.0348 (8) | 0.0204 (8) | 0.0276 (8) | −0.0022 (7) | −0.0039 (7) | 0.0007 (7) |
| C7 | 0.0189 (7) | 0.0154 (7) | 0.0248 (7) | −0.0018 (5) | 0.0013 (6) | 0.0015 (6) |
| C8 | 0.0172 (7) | 0.0154 (7) | 0.0284 (8) | 0.0023 (5) | −0.0008 (6) | −0.0020 (6) |
| C9 | 0.0183 (7) | 0.0217 (7) | 0.0294 (8) | 0.0040 (6) | −0.0005 (6) | −0.0019 (7) |
| C10 | 0.0249 (8) | 0.0316 (9) | 0.0287 (8) | 0.0065 (7) | −0.0055 (7) | −0.0063 (8) |
| C11 | 0.0246 (8) | 0.0273 (8) | 0.0452 (10) | 0.0000 (7) | −0.0082 (7) | −0.0151 (8) |
| C12 | 0.0263 (8) | 0.0190 (8) | 0.0478 (10) | −0.0038 (6) | −0.0030 (7) | −0.0031 (8) |
| C13 | 0.0235 (7) | 0.0176 (7) | 0.0333 (8) | 0.0001 (6) | −0.0013 (6) | 0.0009 (7) |
| C14 | 0.0336 (9) | 0.0299 (9) | 0.0298 (8) | −0.0022 (7) | −0.0004 (7) | 0.0052 (8) |
| N1 | 0.0261 (6) | 0.0126 (6) | 0.0273 (7) | 0.0019 (5) | −0.0033 (6) | −0.0017 (6) |
| O1 | 0.0274 (5) | 0.0124 (5) | 0.0336 (6) | 0.0014 (4) | −0.0033 (5) | −0.0018 (5) |
Geometric parameters (Å, °)
| C1—C6 | 1.387 (2) | C8—C13 | 1.397 (2) |
| C1—C2 | 1.392 (2) | C8—C9 | 1.404 (2) |
| C1—N1 | 1.4180 (18) | C9—C10 | 1.393 (2) |
| C2—C3 | 1.385 (2) | C9—C14 | 1.507 (2) |
| C2—H2 | 0.9500 | C10—C11 | 1.390 (2) |
| C3—C4 | 1.387 (3) | C10—H10 | 0.9500 |
| C3—H3 | 0.9500 | C11—C12 | 1.376 (2) |
| C4—C5 | 1.377 (3) | C11—H11 | 0.9500 |
| C4—H4 | 0.9500 | C12—C13 | 1.383 (2) |
| C5—C6 | 1.386 (2) | C12—H12 | 0.9500 |
| C5—H5 | 0.9500 | C13—H13 | 0.9500 |
| C6—H6 | 0.9500 | C14—H14A | 0.9800 |
| C7—O1 | 1.2375 (17) | C14—H14B | 0.9800 |
| C7—N1 | 1.3516 (18) | C14—H14C | 0.9800 |
| C7—C8 | 1.492 (2) | N1—H1N | 0.878 (17) |
| C6—C1—C2 | 120.05 (14) | C10—C9—C8 | 117.51 (14) |
| C6—C1—N1 | 121.76 (13) | C10—C9—C14 | 120.47 (14) |
| C2—C1—N1 | 118.19 (13) | C8—C9—C14 | 122.01 (13) |
| C3—C2—C1 | 119.53 (16) | C11—C10—C9 | 121.78 (15) |
| C3—C2—H2 | 120.2 | C11—C10—H10 | 119.1 |
| C1—C2—H2 | 120.2 | C9—C10—H10 | 119.1 |
| C2—C3—C4 | 120.41 (16) | C12—C11—C10 | 120.01 (15) |
| C2—C3—H3 | 119.8 | C12—C11—H11 | 120.0 |
| C4—C3—H3 | 119.8 | C10—C11—H11 | 120.0 |
| C5—C4—C3 | 119.73 (16) | C11—C12—C13 | 119.66 (15) |
| C5—C4—H4 | 120.1 | C11—C12—H12 | 120.2 |
| C3—C4—H4 | 120.1 | C13—C12—H12 | 120.2 |
| C4—C5—C6 | 120.53 (17) | C12—C13—C8 | 120.56 (15) |
| C4—C5—H5 | 119.7 | C12—C13—H13 | 119.7 |
| C6—C5—H5 | 119.7 | C8—C13—H13 | 119.7 |
| C5—C6—C1 | 119.69 (15) | C9—C14—H14A | 109.5 |
| C5—C6—H6 | 120.2 | C9—C14—H14B | 109.5 |
| C1—C6—H6 | 120.2 | H14A—C14—H14B | 109.5 |
| O1—C7—N1 | 123.79 (13) | C9—C14—H14C | 109.5 |
| O1—C7—C8 | 121.65 (12) | H14A—C14—H14C | 109.5 |
| N1—C7—C8 | 114.53 (12) | H14B—C14—H14C | 109.5 |
| C13—C8—C9 | 120.44 (14) | C7—N1—C1 | 126.32 (12) |
| C13—C8—C7 | 118.16 (13) | C7—N1—H1N | 114.9 (11) |
| C9—C8—C7 | 121.37 (13) | C1—N1—H1N | 118.5 (11) |
| C6—C1—C2—C3 | 1.6 (2) | C13—C8—C9—C14 | 179.07 (13) |
| N1—C1—C2—C3 | −178.20 (14) | C7—C8—C9—C14 | −2.9 (2) |
| C1—C2—C3—C4 | 0.5 (3) | C8—C9—C10—C11 | −1.1 (2) |
| C2—C3—C4—C5 | −2.1 (3) | C14—C9—C10—C11 | 179.21 (14) |
| C3—C4—C5—C6 | 1.7 (3) | C9—C10—C11—C12 | 2.0 (2) |
| C4—C5—C6—C1 | 0.4 (2) | C10—C11—C12—C13 | −1.2 (2) |
| C2—C1—C6—C5 | −2.0 (2) | C11—C12—C13—C8 | −0.5 (2) |
| N1—C1—C6—C5 | 177.73 (14) | C9—C8—C13—C12 | 1.5 (2) |
| O1—C7—C8—C13 | 126.10 (15) | C7—C8—C13—C12 | −176.65 (13) |
| N1—C7—C8—C13 | −52.29 (17) | O1—C7—N1—C1 | −0.2 (2) |
| O1—C7—C8—C9 | −51.99 (19) | C8—C7—N1—C1 | 178.11 (13) |
| N1—C7—C8—C9 | 129.62 (14) | C6—C1—N1—C7 | −35.5 (2) |
| C13—C8—C9—C10 | −0.7 (2) | C2—C1—N1—C7 | 144.32 (15) |
| C7—C8—C9—C10 | 177.40 (13) |
Hydrogen-bond geometry (Å, °)
| D—H···A | D—H | H···A | D···A | D—H···A |
| N1—H1N···O1i | 0.878 (17) | 2.012 (18) | 2.8751 (16) | 167.7 (15) |
Symmetry codes: (i) −x+3/2, y+1/2, z.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: DN2308).
References
- Gowda, B. T., Foro, S., Sowmya, B. P. & Fuess, H. (2007). Acta Cryst. E63, o3789.
- Gowda, B. T., Jyothi, K., Paulus, H. & Fuess, H. (2003). Z. Naturforsch. Teil A, 58, 225–230.
- Gowda, B. T., Tokarčík, M., Kožíšek, J. & Sowmya, B. P. (2008). Acta Cryst. E64, o83. [DOI] [PMC free article] [PubMed]
- Oxford Diffraction (2004). CrysAlis CCD Version 1.171.26. Oxford Diffraction Ltd. Abingdon, Oxfordshire, England.
- Oxford Diffraction (2007). CrysAlis RED Version 1.171.32.5. Oxford Diffraction Ltd. Abingdon, Oxfordshire, England.
- Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
- Spek, A. L. (2003). PLATON J. Appl. Cryst.36, 7–13.
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/S1600536807068821/dn2308sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536807068821/dn2308Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report


