organic compounds
N-Cyclohexyl-3-fluorobenzamide
aDepartment of Chemistry, Quaid-I-Azam University, Islamabad 45320, Pakistan, and bDepartment Chemie, Fakultät für Naturwissenschaften, Universität Paderborn, Warburgerstrasse 100, D-33098 Paderborn, Germany
*Correspondence e-mail: aamersaeed@yahoo.com
In the title molecule, C13H16FNO, the amide (N—C=O) plane is oriented at an angle of 29.9 (2)° with respect to the aromatic ring. The cyclohexane ring adopts the usual chair conformation. In the intermolecular N—H⋯O hydrogen bonds link the molecules into chains along [100]. A weak C—H⋯F interaction is also observed. The F atom is disordered over two positions with occupancy factors of 0.873 (3) and 0.127 (3).
Experimental
Crystal data
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Refinement
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Data collection: SMART (Bruker, 2002); cell SAINT (Bruker, 2002); data reduction: SAINT; 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/S1600536808034478/ci2689sup1.cif
contains datablocks global, I. DOI:Structure factors: contains datablock I. DOI: 10.1107/S1600536808034478/ci2689Isup2.hkl
3,5-Difluorobenzoyl chloride (5.4 mmol) in CHCl3 was treated with cyclohexylamine (21.6 mmol) under a nitrogen atmosphere at reflux for 4 h. Upon cooling, the reaction mixture was diluted with CHCl3 and washed consecutively with aq 1 M HCl and saturated aq NaHCO3. The organic layer was dried over anhydrous sodium sulfate and concentrated under reduced pressure. Crystallization of the residue in CHCl3 afforded the title compound (84%). Analysis calculated for C13H15F2NO: C 65.26, H 6.32, N 5.85%; found: C 65.31, H 6.39, N 5.77%.
The F atom is disordered over two positions (F1 and F2) with site occupation factors of 0.873 (3) for F1 and 0.127 (3) for F2. H atoms were initially located in difference syntheses, but were then included in the
at calculated positions, in the riding-model approximation, with N—H = 0.88 Å and C—H = 0.95–1.00 Å. The isotropic displacement parameters were set equal to 1.2Ueq of the In the absence of significant effects, the Friedel pairs were merged.Data collection: SMART (Bruker, 2002); cell
SAINT (Bruker, 2002); data reduction: SAINT (Bruker, 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: SHELXTL (Sheldrick, 2008).C13H16FNO | F(000) = 236 |
Mr = 221.27 | Dx = 1.262 Mg m−3 |
Monoclinic, P21 | Mo Kα radiation, λ = 0.71073 Å |
Hall symbol: P 2yb | Cell parameters from 796 reflections |
a = 5.267 (3) Å | θ = 2.4–28.3° |
b = 6.599 (4) Å | µ = 0.09 mm−1 |
c = 16.755 (9) Å | T = 120 K |
β = 90.090 (17)° | Prism, colourless |
V = 582.4 (6) Å3 | 0.45 × 0.40 × 0.21 mm |
Z = 2 |
Bruker SMART APEX diffractometer | 1492 independent reflections |
Radiation source: sealed tube | 1420 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.034 |
ϕ and ω scans | θmax = 27.9°, θmin = 2.4° |
Absorption correction: multi-scan (SADABS; Sheldrick, 2004) | h = −6→6 |
Tmin = 0.962, Tmax = 0.978 | k = −8→8 |
5071 measured reflections | l = −22→19 |
Refinement on F2 | Primary atom site location: structure-invariant direct methods |
Least-squares matrix: full | Secondary atom site location: difference Fourier map |
R[F2 > 2σ(F2)] = 0.035 | Hydrogen site location: difference Fourier map |
wR(F2) = 0.098 | H-atom parameters constrained |
S = 1.05 | w = 1/[σ2(Fo2) + (0.0686P)2 + 0.0394P] where P = (Fo2 + 2Fc2)/3 |
1492 reflections | (Δ/σ)max = 0.001 |
150 parameters | Δρmax = 0.25 e Å−3 |
1 restraint | Δρmin = −0.17 e Å−3 |
C13H16FNO | V = 582.4 (6) Å3 |
Mr = 221.27 | Z = 2 |
Monoclinic, P21 | Mo Kα radiation |
a = 5.267 (3) Å | µ = 0.09 mm−1 |
b = 6.599 (4) Å | T = 120 K |
c = 16.755 (9) Å | 0.45 × 0.40 × 0.21 mm |
β = 90.090 (17)° |
Bruker SMART APEX diffractometer | 1492 independent reflections |
Absorption correction: multi-scan (SADABS; Sheldrick, 2004) | 1420 reflections with I > 2σ(I) |
Tmin = 0.962, Tmax = 0.978 | Rint = 0.034 |
5071 measured reflections |
R[F2 > 2σ(F2)] = 0.035 | 1 restraint |
wR(F2) = 0.098 | H-atom parameters constrained |
S = 1.05 | Δρmax = 0.25 e Å−3 |
1492 reflections | Δρmin = −0.17 e Å−3 |
150 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 | Occ. (<1) | |
F1 | 0.9633 (3) | 0.6562 (2) | 0.49344 (8) | 0.0376 (4) | 0.873 (3) |
F2 | 0.249 (2) | 0.9837 (17) | 0.3846 (6) | 0.043 (3)* | 0.127 (3) |
O1 | 0.2561 (2) | 0.2922 (2) | 0.25636 (8) | 0.0316 (3) | |
N1 | 0.6841 (3) | 0.2208 (2) | 0.25218 (8) | 0.0206 (3) | |
H1A | 0.8356 | 0.2505 | 0.2710 | 0.025* | |
C1 | 0.4794 (3) | 0.3278 (2) | 0.27778 (10) | 0.0208 (3) | |
C2 | 0.5341 (3) | 0.5002 (2) | 0.33504 (9) | 0.0198 (3) | |
C3 | 0.7409 (3) | 0.4971 (3) | 0.38818 (10) | 0.0229 (3) | |
H3A | 0.8556 | 0.3860 | 0.3894 | 0.027* | |
C4 | 0.7720 (3) | 0.6615 (3) | 0.43877 (10) | 0.0269 (4) | |
H4A | 0.9080 | 0.6591 | 0.4760 | 0.032* | 0.127 (3) |
C5 | 0.6128 (4) | 0.8300 (3) | 0.43745 (10) | 0.0288 (4) | |
H5A | 0.6419 | 0.9416 | 0.4721 | 0.035* | |
C6 | 0.4084 (4) | 0.8306 (3) | 0.38366 (11) | 0.0295 (4) | |
H6A | 0.2973 | 0.9439 | 0.3817 | 0.035* | 0.873 (3) |
C7 | 0.3671 (3) | 0.6659 (3) | 0.33314 (10) | 0.0253 (4) | |
H7A | 0.2265 | 0.6658 | 0.2976 | 0.030* | |
C8 | 0.6571 (3) | 0.0567 (2) | 0.19365 (9) | 0.0195 (3) | |
H8A | 0.4853 | −0.0054 | 0.2003 | 0.023* | |
C9 | 0.6786 (4) | 0.1391 (3) | 0.10784 (10) | 0.0275 (4) | |
H9A | 0.5431 | 0.2403 | 0.0984 | 0.033* | |
H9B | 0.8445 | 0.2074 | 0.1011 | 0.033* | |
C10 | 0.6542 (4) | −0.0336 (3) | 0.04667 (10) | 0.0299 (4) | |
H10A | 0.4813 | −0.0920 | 0.0497 | 0.036* | |
H10B | 0.6781 | 0.0216 | −0.0078 | 0.036* | |
C11 | 0.8501 (4) | −0.2007 (3) | 0.06182 (11) | 0.0291 (4) | |
H11A | 1.0228 | −0.1466 | 0.0524 | 0.035* | |
H11B | 0.8212 | −0.3136 | 0.0240 | 0.035* | |
C12 | 0.8313 (4) | −0.2802 (3) | 0.14799 (11) | 0.0272 (4) | |
H12A | 0.6653 | −0.3480 | 0.1555 | 0.033* | |
H12B | 0.9664 | −0.3818 | 0.1573 | 0.033* | |
C13 | 0.8582 (3) | −0.1078 (3) | 0.20882 (11) | 0.0232 (3) | |
H13A | 1.0299 | −0.0476 | 0.2047 | 0.028* | |
H13B | 0.8379 | −0.1624 | 0.2635 | 0.028* |
U11 | U22 | U33 | U12 | U13 | U23 | |
F1 | 0.0405 (8) | 0.0402 (7) | 0.0322 (7) | −0.0017 (6) | −0.0107 (5) | −0.0067 (6) |
O1 | 0.0177 (6) | 0.0310 (7) | 0.0460 (8) | 0.0009 (5) | −0.0028 (5) | −0.0113 (6) |
N1 | 0.0172 (6) | 0.0198 (6) | 0.0247 (7) | 0.0003 (5) | −0.0015 (5) | −0.0024 (5) |
C1 | 0.0197 (8) | 0.0181 (7) | 0.0246 (7) | 0.0002 (6) | 0.0004 (6) | −0.0004 (6) |
C2 | 0.0197 (8) | 0.0180 (7) | 0.0217 (7) | −0.0015 (6) | 0.0045 (6) | 0.0002 (6) |
C3 | 0.0231 (8) | 0.0221 (7) | 0.0235 (7) | 0.0014 (6) | 0.0018 (6) | 0.0010 (6) |
C4 | 0.0270 (9) | 0.0306 (9) | 0.0229 (8) | −0.0040 (7) | 0.0018 (6) | −0.0012 (7) |
C5 | 0.0314 (9) | 0.0259 (9) | 0.0292 (8) | −0.0041 (7) | 0.0075 (7) | −0.0081 (8) |
C6 | 0.0268 (9) | 0.0233 (8) | 0.0385 (9) | 0.0044 (7) | 0.0076 (7) | −0.0052 (8) |
C7 | 0.0214 (8) | 0.0253 (8) | 0.0293 (8) | 0.0023 (7) | 0.0013 (6) | −0.0015 (7) |
C8 | 0.0169 (7) | 0.0173 (7) | 0.0243 (8) | −0.0005 (6) | −0.0003 (6) | −0.0017 (6) |
C9 | 0.0376 (10) | 0.0205 (8) | 0.0242 (8) | 0.0018 (7) | −0.0026 (7) | 0.0000 (6) |
C10 | 0.0367 (10) | 0.0281 (9) | 0.0250 (8) | −0.0007 (8) | −0.0034 (7) | −0.0043 (7) |
C11 | 0.0290 (9) | 0.0249 (8) | 0.0334 (9) | −0.0032 (8) | 0.0051 (7) | −0.0085 (8) |
C12 | 0.0284 (9) | 0.0177 (8) | 0.0356 (9) | 0.0023 (7) | −0.0016 (7) | −0.0027 (7) |
C13 | 0.0221 (8) | 0.0192 (8) | 0.0285 (8) | 0.0014 (6) | −0.0010 (6) | −0.0003 (6) |
F1—C4 | 1.361 (2) | C8—C13 | 1.538 (2) |
F2—C6 | 1.315 (11) | C8—C9 | 1.541 (2) |
O1—C1 | 1.252 (2) | C8—H8A | 1.00 |
N1—C1 | 1.359 (2) | C9—C10 | 1.538 (2) |
N1—C8 | 1.468 (2) | C9—H9A | 0.99 |
N1—H1A | 0.88 | C9—H9B | 0.99 |
C1—C2 | 1.515 (2) | C10—C11 | 1.531 (3) |
C2—C7 | 1.404 (2) | C10—H10A | 0.99 |
C2—C3 | 1.406 (2) | C10—H10B | 0.99 |
C3—C4 | 1.386 (3) | C11—C12 | 1.540 (3) |
C3—H3A | 0.95 | C11—H11A | 0.99 |
C4—C5 | 1.393 (3) | C11—H11B | 0.99 |
C4—H4A | 0.95 | C12—C13 | 1.534 (2) |
C5—C6 | 1.403 (3) | C12—H12A | 0.99 |
C5—H5A | 0.95 | C12—H12B | 0.99 |
C6—C7 | 1.394 (3) | C13—H13A | 0.99 |
C6—H6A | 0.95 | C13—H13B | 0.99 |
C7—H7A | 0.95 | ||
C1—N1—C8 | 121.23 (14) | C13—C8—H8A | 108.4 |
C1—N1—H1A | 119.4 | C9—C8—H8A | 108.4 |
C8—N1—H1A | 119.4 | C10—C9—C8 | 110.76 (15) |
O1—C1—N1 | 123.89 (15) | C10—C9—H9A | 109.5 |
O1—C1—C2 | 120.02 (14) | C8—C9—H9A | 109.5 |
N1—C1—C2 | 116.09 (14) | C10—C9—H9B | 109.5 |
C7—C2—C3 | 120.72 (15) | C8—C9—H9B | 109.5 |
C7—C2—C1 | 116.85 (14) | H9A—C9—H9B | 108.1 |
C3—C2—C1 | 122.42 (15) | C11—C10—C9 | 111.55 (14) |
C4—C3—C2 | 117.78 (16) | C11—C10—H10A | 109.3 |
C4—C3—H3A | 121.1 | C9—C10—H10A | 109.3 |
C2—C3—H3A | 121.1 | C11—C10—H10B | 109.3 |
F1—C4—C3 | 118.55 (17) | C9—C10—H10B | 109.3 |
F1—C4—C5 | 118.43 (16) | H10A—C10—H10B | 108.0 |
C3—C4—C5 | 123.00 (16) | C10—C11—C12 | 110.90 (15) |
C3—C4—H4A | 118.5 | C10—C11—H11A | 109.5 |
C5—C4—H4A | 118.5 | C12—C11—H11A | 109.5 |
C4—C5—C6 | 118.30 (16) | C10—C11—H11B | 109.5 |
C4—C5—H5A | 120.9 | C12—C11—H11B | 109.5 |
C6—C5—H5A | 120.9 | H11A—C11—H11B | 108.0 |
F2—C6—C7 | 120.5 (5) | C13—C12—C11 | 111.33 (15) |
F2—C6—C5 | 119.0 (5) | C13—C12—H12A | 109.4 |
C7—C6—C5 | 120.42 (16) | C11—C12—H12A | 109.4 |
C7—C6—H6A | 119.8 | C13—C12—H12B | 109.4 |
C5—C6—H6A | 119.8 | C11—C12—H12B | 109.4 |
C6—C7—C2 | 119.75 (15) | H12A—C12—H12B | 108.0 |
C6—C7—H7A | 120.1 | C12—C13—C8 | 110.55 (13) |
C2—C7—H7A | 120.1 | C12—C13—H13A | 109.5 |
N1—C8—C13 | 110.16 (13) | C8—C13—H13A | 109.5 |
N1—C8—C9 | 110.86 (13) | C12—C13—H13B | 109.5 |
C13—C8—C9 | 110.58 (13) | C8—C13—H13B | 109.5 |
N1—C8—H8A | 108.4 | H13A—C13—H13B | 108.1 |
C8—N1—C1—O1 | 2.5 (2) | F2—C6—C7—C2 | −177.6 (5) |
C8—N1—C1—C2 | −177.01 (13) | C5—C6—C7—C2 | −1.2 (3) |
O1—C1—C2—C7 | −29.1 (2) | C3—C2—C7—C6 | 0.9 (2) |
N1—C1—C2—C7 | 150.37 (15) | C1—C2—C7—C6 | −179.27 (15) |
O1—C1—C2—C3 | 150.71 (16) | C1—N1—C8—C13 | −148.28 (15) |
N1—C1—C2—C3 | −29.8 (2) | C1—N1—C8—C9 | 89.00 (18) |
C7—C2—C3—C4 | 0.6 (2) | N1—C8—C9—C10 | 179.17 (14) |
C1—C2—C3—C4 | −179.20 (14) | C13—C8—C9—C10 | 56.69 (18) |
C2—C3—C4—F1 | 176.62 (15) | C8—C9—C10—C11 | −55.8 (2) |
C2—C3—C4—C5 | −1.9 (3) | C9—C10—C11—C12 | 55.0 (2) |
F1—C4—C5—C6 | −176.95 (16) | C10—C11—C12—C13 | −55.56 (19) |
C3—C4—C5—C6 | 1.6 (3) | C11—C12—C13—C8 | 56.76 (19) |
C4—C5—C6—F2 | 176.4 (6) | N1—C8—C13—C12 | 179.90 (13) |
C4—C5—C6—C7 | 0.1 (3) | C9—C8—C13—C12 | −57.21 (18) |
D—H···A | D—H | H···A | D···A | D—H···A |
N1—H1A···O1i | 0.88 | 2.25 | 3.050 (2) | 152 |
C5—H5A···F1ii | 0.95 | 2.58 | 3.310 (3) | 134 |
Symmetry codes: (i) x+1, y, z; (ii) −x+2, y+1/2, −z+1. |
Experimental details
Crystal data | |
Chemical formula | C13H16FNO |
Mr | 221.27 |
Crystal system, space group | Monoclinic, P21 |
Temperature (K) | 120 |
a, b, c (Å) | 5.267 (3), 6.599 (4), 16.755 (9) |
β (°) | 90.090 (17) |
V (Å3) | 582.4 (6) |
Z | 2 |
Radiation type | Mo Kα |
µ (mm−1) | 0.09 |
Crystal size (mm) | 0.45 × 0.40 × 0.21 |
Data collection | |
Diffractometer | Bruker SMART APEX diffractometer |
Absorption correction | Multi-scan (SADABS; Sheldrick, 2004) |
Tmin, Tmax | 0.962, 0.978 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 5071, 1492, 1420 |
Rint | 0.034 |
(sin θ/λ)max (Å−1) | 0.658 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.035, 0.098, 1.05 |
No. of reflections | 1492 |
No. of parameters | 150 |
No. of restraints | 1 |
H-atom treatment | H-atom parameters constrained |
Δρmax, Δρmin (e Å−3) | 0.25, −0.17 |
Computer programs: SMART (Bruker, 2002), SAINT (Bruker, 2002), SHELXS97 (Sheldrick, 2008), SHELXL97 (Sheldrick, 2008), SHELXTL (Sheldrick, 2008).
D—H···A | D—H | H···A | D···A | D—H···A |
N1—H1A···O1i | 0.88 | 2.25 | 3.050 (2) | 152 |
C5—H5A···F1ii | 0.95 | 2.58 | 3.310 (3) | 134 |
Symmetry codes: (i) x+1, y, z; (ii) −x+2, y+1/2, −z+1. |
Acknowledgements
NA is grateful to the Higher Education Commission of Pakistan for financial support for a PhD programme.
References
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Chopra, D. & Guru Row, T. N. (2005). Cryst. Growth Des. 5, 1679–1681. Web of Science CSD CrossRef CAS Google Scholar
Saeed, A., Abbas, N., Hussain, S. & Flörke, U. (2008a). Acta Cryst. E64, o773. Web of Science CSD CrossRef IUCr Journals Google Scholar
Saeed, A., Khera, R. A., Batool, M., Shaheen, U. & Flörke, U. (2008b). Acta Cryst. E64, o1625. Web of Science CSD CrossRef IUCr Journals Google Scholar
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This is an open-access article distributed under the terms of the Creative Commons Attribution (CC-BY) Licence, which permits unrestricted use, distribution, and reproduction in any medium, provided the original authors and source are cited.
The background to this study has been described in an earlier paper (Saeed et al., 2008b).
The molecular structure of the title compound is related to that of the 2,4-dichloro compound (Saeed et al., 2008a). The cyclohexane ring is in the most stable chair conformation. In general, bond lengths and angles are within normal ranges. The aromatic ring C2–C7 is oriented with respect to the N1/O1/C1 plane at a dihedral angle of 29.9 (2)°. The N1–C1–C2–C7 torsion angle is 150.37 (15)°, for the reported dichloro compound the corresponding angle is 130.16 (18)°.
In the crystal structure, intermolecular N—H···O hydrogen bonds (Table 1) link the molecules into infinite chains along the [100] direction (Fig. 2), in which they may be effective in the stabilization of the structure. Another intermolecular interaction is C—H···F (Table 1), as found in 4-fluoro-N-(2-fluorophenyl)benzamide (Chopra & Row, 2005).