organic papers
Acta Cryst.(2007). E63, o1977–o1978 doi:10.1107/S1600536807012998 Gowdaet al. C
9H11NO
o1977
Acta Crystallographica Section E Structure Reports Online
ISSN 1600-5368
N
-(2-Methylphenyl)acetamide
B. Thimme Gowda,a* Jozef Kozˇı´sˇek,bMiroslav Tokarcˇı´kcand Hartmut Fuessd
aDepartment of Chemistry, Mangalore
University, Mangalagangotri 574 199, Mangalore, India,bDepartment of Physical
Chemistry, Slovak University of Technology, Radlinske´ho 9, SK-812 37 Bratislava, Slovak Republic,cDepartment of Chemical Physics, Slovak University of Technology, Radlinske´ho 9, 812 37 Bratislava, Slovak Republic, and
d
Institute of Materials Science, Darmstadt University of Technology, Petersenstrasse 23, D-64287, Darmstadt, Germany
Correspondence e-mail: [email protected]
Key indicators
Single-crystal X-ray study T= 298 K
Mean(C–C) = 0.005 A˚ Rfactor = 0.070 wRfactor = 0.177
Data-to-parameter ratio = 14.0
For details of how these key indicators were automatically derived from the article, see http://journals.iucr.org/e.
Received 4 March 2007 Accepted 19 March 2007
#2007 International Union of Crystallography All rights reserved
In the title compound, C9H11NO, the acetamide unit is slightly
twisted with respect to the 2-methylphenyl substituent. The structure is closely related to that of the unsubstituted N -phenylacetamide with slightly different bond parameters. The conformation of the N—H bond is antito the ortho-methyl substituent in the crystal structure of the title compound.
Comment
In the present work, the structure of N -(2-methylphenyl)-acetamide (2MPA), (I), has been determined as part of a study on the systematization of the crystal structures of acetanilides (Gowdaet al., 2004, 2006, 2007). 2MPA resembles closely the unsubstituted N-(phenyl)-acetamide (PA) and other substi-tuted amides (Brownet al., 1954, 1966; Gowdaet al., 2000a,b, 2001), with slightly different bond parameters. In fact, 2MPA and PA crystallize in the same space group, Pbca. In the structure of 2MPA, the conformation of the N—H bond isanti
to theortho-methyl substituent.
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 (375 K). It was characterized by recording its infrared and NMR spectra (Gowdaet al., 2003). Single crystals of the title compound were obtained by the slow evaporation of an ethanolic solution.
Crystal data
C9H11NO
Mr= 149.19
Orthorhombic,Pbca a= 8.9608 (10) A˚
b= 12.4784 (17) A˚
c= 15.012 (2) A˚
V= 1678.6 (4) A˚3
Z= 8
MoKradiation
= 0.08 mm 1
T= 298 (2) K 0.320.150.09 mm
Data collection
Oxford Diffraction Xcalibur diffractometer
Absorption correction: none 10081 measured reflections
1639 independent reflections 895 reflections withI> 2(I)
Refinement
R[F2> 2(F2)] = 0.070
wR(F2) = 0.177
S= 1.09 1639 reflections
117 parameters
H-atom parameters constrained
max= 0.18 e A˚ 3
min= 0.17 e A˚ 3
All H atoms were positioned geometrically and treated as riding with C—H = 0.93 A˚ (CH aromatic) or 0.96 A˚ (CH3) and N—H =
0.86 A˚ , and with Uiso(H) = 1.2Ueq(CH or NH) and Uiso(H) =
1.5Ueq(CH3).
Data collection: CrysAlis CCD (Oxford Diffraction, 2006); cell refinement: CrysAlis RED(Oxford Diffraction, 2006); data reduc-tion:CrysAlis RED; program(s) used to solve structure:SHELXS97
(Sheldrick, 1997); program(s) used to refine structure:SHELXL97
(Sheldrick, 1997); molecular graphics: ORTEP-3 for Windows
(Farrugia, 1997); software used to prepare material for publication:
SHELXL97(Sheldrick, 1997),PLATON(Spek, 2003) andWinGX
(Farrugia, 1999).
BTG thanks the Alexander von Humboldt Foundation, Bonn, Germany, for resumption of his research fellowship. JK and MT thank the Grant Agency of the Slovak Republic (Grant No. 1/2449/05).
References
Brown, C. J. (1966).Acta Cryst.21, 442–445.
Brown, C. J. & Corbridge, D. E. C. (1954).Acta Cryst.7, 711–715. Farrugia, L. J. (1997).J. Appl. Cryst.30, 565.
Farrugia, L. J. (1999).J. Appl. Cryst.32, 837–838.
Gowda, B. T., Kozisek, J. & Fuess, H. (2006).Z. Naturforsch. Teil A,61, 588– 594.
Gowda, B. T., Kozisek, J., Svoboda, I. & Fuess, H. (2007).Z. Naturforsch. Teil A,62, 91–100.
Gowda, B. T., Paulus, H. & Fuess, H. (2000a).Z. Naturforsch. Teil A,55, 711– 720.
Gowda, B. T., Paulus, H. & Fuess, H. (2000b).Z. Naturforsch. Teil A,55, 791– 800.
Gowda, B. T., Paulus, H. & Fuess, H. (2001).Z. Naturforsch. Teil A,56, 386– 394.
Gowda, B. T., Svoboda, I. & Fuess, H. (2004).Z. Naturforsch. Teil A,59, 845– 852.
Gowda, B. T., Usha, K. M. & Jayalakshmi, K. L. (2003).Z. Naturforsch. Teil A,
58, 801–806.
Oxford Diffraction (2006).CrysAlis CCD,CrysAlis RED. Oxford Diffraction Ltd, Abingdon, Oxfordshire, England.
Sheldrick, G. M. (1997). SHELXS97 and SHELXL97. University of Go¨ttingen, Germany.
[image:2.610.315.566.71.235.2]Spek, A. L. (2003).J. Appl. Cryst.36, 7–13.
Figure 1
supporting information
sup-1 Acta Cryst. (2007). E63, o1977–o1978
supporting information
Acta Cryst. (2007). E63, o1977–o1978 [https://doi.org/10.1107/S1600536807012998]
N
-(2-Methylphenyl)acetamide
B. Thimme Gowda, Jozef Ko
žíš
ek, Miroslav Tokar
čí
k and Hartmut Fuess
N-(2-Methylphenyl)acetamide
Crystal data
C9H11NO
Mr = 149.19
Orthorhombic, Pbca
Hall symbol: -P 2ac 2ab
a = 8.9608 (10) Å
b = 12.4784 (17) Å
c = 15.012 (2) Å
V = 1678.6 (4) Å3
Z = 8
F(000) = 640
Dx = 1.181 Mg m−3
Mo Kα radiation, λ = 0.71073 Å Cell parameters from 2695 reflections
θ = 2.3–30.0°
µ = 0.08 mm−1
T = 298 K Prism, colourless 0.32 × 0.15 × 0.09 mm
Data collection
Oxford Diffraction Xcalibur diffractometer
Graphite monochromator
Detector resolution: 8.4012 pixels mm-1
ω scans
10081 measured reflections 1639 independent reflections
895 reflections with I > 2σ(I)
Rint = 0.078
θmax = 26.0°, θmin = 4.2°
h = −5→11
k = −15→15
l = −18→18
Refinement
Refinement on F2
Least-squares matrix: full
R[F2 > 2σ(F2)] = 0.070
wR(F2) = 0.177
S = 1.09 1639 reflections 117 parameters 0 restraints
Primary atom site location: structure-invariant direct methods
Secondary atom site location: difference Fourier map
Hydrogen site location: inferred from neighbouring sites
H-atom parameters constrained
w = 1/[σ2(F
o2) + (0.0541P)2 + 1.0901P]
where P = (Fo2 + 2Fc2)/3
(Δ/σ)max = 0.015
Δρmax = 0.18 e Å−3
Δρmin = −0.17 e Å−3
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
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 0.0254 (4) 0.9605 (3) 0.1188 (2) 0.0745 (11) H1A −0.0774 0.9533 0.1358 0.089* H1B 0.0430 0.9211 0.0649 0.089* H1C 0.0480 1.0348 0.1092 0.089* C2 0.1220 (3) 0.9178 (2) 0.1908 (2) 0.0507 (8) O3 0.2570 (2) 0.91709 (19) 0.18313 (13) 0.0617 (7) N4 0.0523 (3) 0.8809 (2) 0.26354 (16) 0.0561 (7) H4N −0.0436 0.8820 0.2637 0.067* C5 0.1248 (3) 0.8402 (3) 0.3404 (2) 0.0515 (8) C6 0.2072 (4) 0.7471 (3) 0.3372 (2) 0.0626 (9) C7 0.2717 (5) 0.7132 (3) 0.4163 (3) 0.0850 (12) H7 0.3276 0.6505 0.4162 0.102* C8 0.2564 (4) 0.7683 (4) 0.4942 (3) 0.0851 (12) H8 0.3023 0.7433 0.5458 0.102* C9 0.1743 (4) 0.8595 (3) 0.4963 (2) 0.0754 (11) H9 0.1630 0.8974 0.5492 0.090* C10 0.1079 (3) 0.8953 (3) 0.4196 (2) 0.0606 (9) H10 0.0508 0.9575 0.4209 0.073* C11 0.2227 (5) 0.6830 (3) 0.2542 (3) 0.0935 (13) H11A 0.2584 0.6126 0.2687 0.112* H11B 0.2922 0.7175 0.2150 0.112* H11C 0.1273 0.6775 0.2254 0.112*
Atomic displacement parameters (Å2)
U11 U22 U33 U12 U13 U23
supporting information
sup-3 Acta Cryst. (2007). E63, o1977–o1978
Geometric parameters (Å, º)
C1—C2 1.483 (4) C6—C11 1.486 (5) C1—H1A 0.96 C7—C8 1.360 (6)
C1—H1B 0.96 C7—H7 0.93
C1—H1C 0.96 C8—C9 1.358 (5) C2—O3 1.215 (3) C8—H8 0.93 C2—N4 1.341 (4) C9—C10 1.369 (5) N4—C5 1.417 (4) C9—H9 0.93
N4—H4N 0.86 C10—H10 0.93
C5—C6 1.377 (4) C11—H11A 0.96 C5—C10 1.387 (4) C11—H11B 0.96 C6—C7 1.389 (5) C11—H11C 0.96
C2—C1—H1A 109.5 C6—C7—C8 122.8 (4) C2—C1—H1B 109.5 C6—C7—H7 118.7 H1A—C1—H1B 109.5 C8—C7—H7 118.7 C2—C1—H1C 109.5 C9—C8—C7 119.8 (4) H1A—C1—H1C 109.5 C9—C8—H8 120.1 H1B—C1—H1C 109.5 C7—C8—H8 120.1 O3—C2—N4 122.6 (3) C8—C9—C10 119.3 (4) O3—C2—C1 121.0 (3) C9—C10—C5 120.9 (4) N4—C2—C1 116.4 (3) C8—C9—H9 120.3 C2—N4—C5 125.0 (2) C10—C9—H9 120.3 C2—N4—H4N 117.5 C9—C10—H10 119.5 C5—N4—H4N 117.5 C5—C10—H10 119.5 C6—C5—C10 120.6 (3) C6—C11—H11A 109.5 C6—C5—N4 121.1 (3) C6—C11—H11B 109.5 C10—C5—N4 118.3 (3) H11A—C11—H11B 109.5 C5—C6—C7 116.6 (3) C6—C11—H11C 109.5 C5—C6—C11 122.2 (3) H11A—C11—H11C 109.5 C7—C6—C11 121.1 (3) H11B—C11—H11C 109.5