organic compounds
N,4-Dimethylbenzamide
aCollege of Chemical and Biological Engineering, Yancheng Institute of Technology, Yinbing Road No. 9 Yancheng, Yancheng 224051, People's Republic of China, and bDepartment of Chemical Engineering, Yancheng College of Textile Technology, Yancheng 224051, People's Republic of China
*Correspondence e-mail: xujiaying-1984@163.com
In the crystal of the title compound, C9H11NO, molecules are connected via intermolecular N—H⋯O hydrogen bonds, forming a one-dimensional network in the b-axis direction. The dihedral angle between the amide group and the benzyl ring is 13.8 (2)°.
Related literature
For the synthetic procedure, see: Lee et al. (2009). For bond-length data, see: Allen et al. (1987). ?show [softreturn]>
Experimental
Crystal data
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Refinement
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Data collection: CAD-4 Software (Enraf–Nonius, 1985); cell CAD-4 Software; data reduction: XCAD4 (Harms & Wocadlo,1995); 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: SHELXTL.
Supporting information
10.1107/S1600536811003527/vm2076sup1.cif
contains datablocks I, global. DOI:Structure factors: contains datablock I. DOI: 10.1107/S1600536811003527/vm2076Isup2.hkl
The title compound, (I) was prepared by a method reported in literature (Lee et al. (2009)). Crystals were obtained by dissolving (I) (0.2 g, 1.34 mmol) in ethanol (25 ml) and evaporating the solvent slowly at room temperature for about 7 d.
All H atoms were positioned geometrically and constrained to ride on their parent atoms, with C—H = 0.93 Å for aromatic H, 0.96 Å for methyl H and 0.86 Å for N—H, respectively. The Uiso(H) = xUeq(C), where x = 1.2 for aromatic H and N—H, and x = 1.5 for methyl H.
Data collection: CAD-4 Software (Enraf–Nonius, 1985); cell
CAD-4 Software (Enraf–Nonius, 1985); data reduction: XCAD4 (Harms & Wocadlo,1995); 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: SHELXTL (Sheldrick, 2008).C9H11NO | F(000) = 320 |
Mr = 149.19 | Dx = 1.205 Mg m−3 |
Monoclinic, P21/n | Mo Kα radiation, λ = 0.71073 Å |
Hall symbol: -P 2yn | Cell parameters from 25 reflections |
a = 6.7670 (14) Å | θ = 9–13° |
b = 9.946 (2) Å | µ = 0.08 mm−1 |
c = 12.229 (2) Å | T = 293 K |
β = 92.63 (3)° | Block, colourless |
V = 822.2 (3) Å3 | 0.30 × 0.20 × 0.10 mm |
Z = 4 |
Enraf–Nonius CAD-4 diffractometer | 1062 reflections with I > 2σ(I) |
Radiation source: fine-focus sealed tube | Rint = 0.033 |
Graphite monochromator | θmax = 25.4°, θmin = 2.6° |
ω/2θ scans | h = 0→8 |
Absorption correction: ψ scan (North et al., 1968) | k = −11→11 |
Tmin = 0.977, Tmax = 0.992 | l = −14→14 |
3362 measured reflections | 3 standard reflections every 200 reflections |
1510 independent reflections | intensity decay: 1% |
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)] = 0.050 | H-atom parameters constrained |
wR(F2) = 0.166 | w = 1/[σ2(Fo2) + (0.1P)2 + 0.080P] where P = (Fo2 + 2Fc2)/3 |
S = 1.01 | (Δ/σ)max < 0.001 |
1510 reflections | Δρmax = 0.20 e Å−3 |
103 parameters | Δρmin = −0.15 e Å−3 |
0 restraints | Extinction correction: SHELXL97 (Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4 |
Primary atom site location: structure-invariant direct methods | Extinction coefficient: 0.028 (8) |
C9H11NO | V = 822.2 (3) Å3 |
Mr = 149.19 | Z = 4 |
Monoclinic, P21/n | Mo Kα radiation |
a = 6.7670 (14) Å | µ = 0.08 mm−1 |
b = 9.946 (2) Å | T = 293 K |
c = 12.229 (2) Å | 0.30 × 0.20 × 0.10 mm |
β = 92.63 (3)° |
Enraf–Nonius CAD-4 diffractometer | 1062 reflections with I > 2σ(I) |
Absorption correction: ψ scan (North et al., 1968) | Rint = 0.033 |
Tmin = 0.977, Tmax = 0.992 | 3 standard reflections every 200 reflections |
3362 measured reflections | intensity decay: 1% |
1510 independent reflections |
R[F2 > 2σ(F2)] = 0.050 | 0 restraints |
wR(F2) = 0.166 | H-atom parameters constrained |
S = 1.01 | Δρmax = 0.20 e Å−3 |
1510 reflections | Δρmin = −0.15 e Å−3 |
103 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. |
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. |
x | y | z | Uiso*/Ueq | ||
O | 0.2041 (3) | 0.99892 (14) | 0.23558 (16) | 0.0773 (6) | |
N | 0.2849 (2) | 0.78998 (15) | 0.28900 (14) | 0.0514 (5) | |
H0A | 0.2554 | 0.7059 | 0.2868 | 0.062* | |
C1 | −0.5644 (4) | 0.6995 (3) | 0.0146 (2) | 0.0766 (8) | |
H1A | −0.6295 | 0.6353 | 0.0592 | 0.115* | |
H1B | −0.5367 | 0.6591 | −0.0543 | 0.115* | |
H1C | −0.6485 | 0.7763 | 0.0023 | 0.115* | |
C2 | −0.3742 (3) | 0.7431 (2) | 0.07191 (17) | 0.0550 (6) | |
C3 | −0.2949 (4) | 0.8698 (2) | 0.05499 (19) | 0.0652 (7) | |
H3A | −0.3599 | 0.9283 | 0.0062 | 0.078* | |
C4 | −0.1226 (3) | 0.9106 (2) | 0.10867 (18) | 0.0591 (6) | |
H4A | −0.0750 | 0.9968 | 0.0969 | 0.071* | |
C5 | −0.0184 (3) | 0.82556 (17) | 0.18015 (15) | 0.0440 (5) | |
C6 | −0.0961 (3) | 0.69834 (18) | 0.19627 (17) | 0.0530 (6) | |
H6A | −0.0291 | 0.6387 | 0.2434 | 0.064* | |
C7 | −0.2701 (3) | 0.6593 (2) | 0.14374 (18) | 0.0581 (6) | |
H7A | −0.3195 | 0.5738 | 0.1569 | 0.070* | |
C8 | 0.1657 (3) | 0.87739 (18) | 0.23661 (16) | 0.0479 (5) | |
C9 | 0.4623 (3) | 0.8321 (2) | 0.3494 (2) | 0.0613 (6) | |
H9A | 0.5168 | 0.7575 | 0.3904 | 0.092* | |
H9B | 0.4309 | 0.9034 | 0.3987 | 0.092* | |
H9C | 0.5571 | 0.8637 | 0.2993 | 0.092* |
U11 | U22 | U33 | U12 | U13 | U23 | |
O | 0.0747 (11) | 0.0273 (8) | 0.1272 (15) | −0.0054 (7) | −0.0245 (10) | 0.0023 (8) |
N | 0.0498 (10) | 0.0296 (8) | 0.0737 (12) | −0.0025 (7) | −0.0084 (8) | −0.0006 (7) |
C1 | 0.0590 (15) | 0.0951 (19) | 0.0743 (16) | −0.0004 (13) | −0.0132 (12) | −0.0086 (14) |
C2 | 0.0481 (12) | 0.0610 (13) | 0.0555 (12) | 0.0047 (10) | −0.0017 (10) | −0.0086 (10) |
C3 | 0.0654 (15) | 0.0563 (13) | 0.0721 (15) | 0.0125 (11) | −0.0159 (12) | 0.0065 (11) |
C4 | 0.0631 (14) | 0.0396 (11) | 0.0739 (14) | 0.0040 (10) | −0.0038 (12) | 0.0083 (10) |
C5 | 0.0446 (11) | 0.0321 (9) | 0.0552 (11) | 0.0050 (8) | 0.0007 (9) | −0.0030 (8) |
C6 | 0.0531 (12) | 0.0351 (10) | 0.0695 (13) | 0.0000 (9) | −0.0108 (10) | 0.0047 (9) |
C7 | 0.0547 (13) | 0.0463 (12) | 0.0724 (14) | −0.0055 (9) | −0.0068 (11) | −0.0010 (10) |
C8 | 0.0503 (12) | 0.0288 (9) | 0.0647 (12) | 0.0016 (8) | 0.0017 (9) | −0.0024 (8) |
C9 | 0.0537 (13) | 0.0506 (12) | 0.0783 (15) | −0.0037 (10) | −0.0122 (11) | −0.0019 (11) |
O—C8 | 1.237 (2) | C3—H3A | 0.9300 |
N—C8 | 1.330 (2) | C4—C5 | 1.386 (3) |
N—C9 | 1.442 (3) | C4—H4A | 0.9300 |
N—H0A | 0.8600 | C5—C6 | 1.388 (3) |
C1—C2 | 1.501 (3) | C5—C8 | 1.489 (3) |
C1—H1A | 0.9600 | C6—C7 | 1.372 (3) |
C1—H1B | 0.9600 | C6—H6A | 0.9300 |
C1—H1C | 0.9600 | C7—H7A | 0.9300 |
C2—C7 | 1.381 (3) | C9—H9A | 0.9600 |
C2—C3 | 1.389 (3) | C9—H9B | 0.9600 |
C3—C4 | 1.373 (3) | C9—H9C | 0.9600 |
C8—N—C9 | 121.90 (17) | C4—C5—C6 | 117.46 (19) |
C8—N—H0A | 119.0 | C4—C5—C8 | 118.17 (17) |
C9—N—H0A | 119.0 | C6—C5—C8 | 124.35 (17) |
C2—C1—H1A | 109.5 | C7—C6—C5 | 120.96 (19) |
C2—C1—H1B | 109.5 | C7—C6—H6A | 119.5 |
H1A—C1—H1B | 109.5 | C5—C6—H6A | 119.5 |
C2—C1—H1C | 109.5 | C6—C7—C2 | 121.9 (2) |
H1A—C1—H1C | 109.5 | C6—C7—H7A | 119.0 |
H1B—C1—H1C | 109.5 | C2—C7—H7A | 119.0 |
C7—C2—C3 | 117.0 (2) | O—C8—N | 121.39 (19) |
C7—C2—C1 | 121.6 (2) | O—C8—C5 | 120.36 (18) |
C3—C2—C1 | 121.4 (2) | N—C8—C5 | 118.24 (16) |
C4—C3—C2 | 121.5 (2) | N—C9—H9A | 109.5 |
C4—C3—H3A | 119.2 | N—C9—H9B | 109.5 |
C2—C3—H3A | 119.2 | H9A—C9—H9B | 109.5 |
C3—C4—C5 | 121.2 (2) | N—C9—H9C | 109.5 |
C3—C4—H4A | 119.4 | H9A—C9—H9C | 109.5 |
C5—C4—H4A | 119.4 | H9B—C9—H9C | 109.5 |
C7—C2—C3—C4 | −1.1 (3) | C3—C2—C7—C6 | −0.1 (3) |
C1—C2—C3—C4 | 178.9 (2) | C1—C2—C7—C6 | 179.9 (2) |
C2—C3—C4—C5 | 1.5 (4) | C9—N—C8—O | 1.5 (3) |
C3—C4—C5—C6 | −0.7 (3) | C9—N—C8—C5 | −177.53 (18) |
C3—C4—C5—C8 | −179.17 (19) | C4—C5—C8—O | 13.1 (3) |
C4—C5—C6—C7 | −0.4 (3) | C6—C5—C8—O | −165.2 (2) |
C8—C5—C6—C7 | 177.91 (18) | C4—C5—C8—N | −167.81 (18) |
C5—C6—C7—C2 | 0.8 (3) | C6—C5—C8—N | 13.8 (3) |
D—H···A | D—H | H···A | D···A | D—H···A |
N—H0A···Oi | 0.86 | 2.10 | 2.912 (2) | 158 |
Symmetry code: (i) −x+1/2, y−1/2, −z+1/2. |
Experimental details
Crystal data | |
Chemical formula | C9H11NO |
Mr | 149.19 |
Crystal system, space group | Monoclinic, P21/n |
Temperature (K) | 293 |
a, b, c (Å) | 6.7670 (14), 9.946 (2), 12.229 (2) |
β (°) | 92.63 (3) |
V (Å3) | 822.2 (3) |
Z | 4 |
Radiation type | Mo Kα |
µ (mm−1) | 0.08 |
Crystal size (mm) | 0.30 × 0.20 × 0.10 |
Data collection | |
Diffractometer | Enraf–Nonius CAD-4 diffractometer |
Absorption correction | ψ scan (North et al., 1968) |
Tmin, Tmax | 0.977, 0.992 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 3362, 1510, 1062 |
Rint | 0.033 |
(sin θ/λ)max (Å−1) | 0.603 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.050, 0.166, 1.01 |
No. of reflections | 1510 |
No. of parameters | 103 |
H-atom treatment | H-atom parameters constrained |
Δρmax, Δρmin (e Å−3) | 0.20, −0.15 |
Computer programs: CAD-4 Software (Enraf–Nonius, 1985), XCAD4 (Harms & Wocadlo,1995), SHELXS97 (Sheldrick, 2008), SHELXL97 (Sheldrick, 2008), SHELXTL (Sheldrick, 2008).
D—H···A | D—H | H···A | D···A | D—H···A |
N—H0A···Oi | 0.86 | 2.10 | 2.912 (2) | 158 |
Symmetry code: (i) −x+1/2, y−1/2, −z+1/2. |
Acknowledgements
The authors thank the Center of Testing and Analysis, Nanjing University, for the data collection.
References
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. CrossRef Web of Science Google Scholar
Enraf–Nonius (1985). CAD-4 Software. Enraf–Nonius, Delft, The Netherlands. Google Scholar
Harms, K. & Wocadlo, S. (1995). XCAD4. University of Marburg, Germany. Google Scholar
Lee, S., Song, K. H., Choe, J., Ju, J. & Jo, Y. (2009). J. Org. Chem. 74, 6358–6361. Web of Science PubMed Google Scholar
North, A. C. T., Phillips, D. C. & Mathews, F. S. (1968). Acta Cryst. A24, 351–359. CrossRef IUCr Journals Web of Science Google Scholar
Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. Web of Science CrossRef CAS IUCr Journals Google Scholar
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Benzamide derivatives exhibit interesting biological activities such as antibacterial and antifungal effects (Lee et al., 2009) We report here the crystal structure of the title compound N,4-dimethylbenzamide (I), an important organic intermediate (Fig. 1). Bond lengths and angles are within normal ranges (Allen et al., 1987).
In the crystal packing of (I) the molecules are connected together via N—H···O intermolecular hydrogen bonds to form a one-dimensional network in the b direction (Table 1, graph set C1,1(4)), which seems to be very effective in the stabilization of the crystal structure.