organic compounds
2-(3,3,4,4-Tetrafluoropyrrolidin-1-yl)aniline
aSchool of Chemistry and Environment, South China Normal University, Guangzhou 510006, People's Republic of China, and bKey Laboratory of Organofluorine Chemistry, Shanghai Institute of Organic Chemistry, Chinese Academy of Sciences, Shanghai, 200032, People's Republic of China
*Correspondence e-mail: zhuosioc@yahoo.com.cn
In the title fluorinated pyrrolidine derivative, C10H10F4N2, the dihedral angle between the best planes of the benzene and pyrrolidine rings is 62.6 (1)°. The crystal packing features intermolecular N—H⋯F hydrogen bonds.
Related literature
For applications of fluorinated pyrrolidine derivatives, see: Hulin et al. (2005); Kerekes et al. (2011); Marson (2005); Santora et al. (2008).
Experimental
Crystal data
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Refinement
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Data collection: APEX2 (Bruker, 2008); cell SAINT (Bruker, 2008); 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: SHELXL97.
Supporting information
10.1107/S1600536811030339/ld2018sup1.cif
contains datablocks global, I. DOI:Structure factors: contains datablock I. DOI: 10.1107/S1600536811030339/ld2018Isup2.hkl
Supporting information file. DOI: 10.1107/S1600536811030339/ld2018Isup3.cml
A mixture of trifluoromethanesulfonic acid 2,2,3,3,-tretrafluoro-1,4-butanediyl ester(1 mmol), o-phenylenediamine (1.5 mmol), Et3N (3 mmol) and ethanol(15 ml) was placed in a round-bottomed flask fitted with a reflux condenser, and then heated at reflux for 30 h. After cooling, the organic solvent was removed under reduced pressure and to the residue was solved in dichloromethane then washed with water, and the organic layer was dried over anhydrous Na2SO4. After the solvent was removed, the residue was purified by flash
on silica gel to afford a purple solid (164 mg), yield 70%. Crystals suitable for X-ray structural analysis were grown from CH3CN solution at room temperature.H-atoms were placed in calculated positions with C—H = 0.93 Å; the H atoms of amino group were refined freely.
Since this is a light-atom structure (it does not contain any atoms heavier than F) and since the data collection was carried out using Mo radiation, it was not possible to unambiguously determine the
of this molecule. In the absence of significant effects, Friedel pairs have been merged.Data collection: APEX2 (Bruker, 2008); cell
SAINT (Bruker, 2008); data reduction: SAINT (Bruker, 2008); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: SHELTLX (Sheldrick, 2008); software used to prepare material for publication: SHELXL97 (Sheldrick, 2008).Fig. 1. View of the title compound showing the atom-labelling scheme. Ellipsoids are drawn at the 50% probability level. | |
Fig. 2. Perspective view of the crystal packing. |
C10H10F4N2 | F(000) = 480 |
Mr = 234.20 | Dx = 1.500 Mg m−3 |
Orthorhombic, P212121 | Mo Kα radiation, λ = 0.71073 Å |
a = 6.791 (13) Å | µ = 0.14 mm−1 |
b = 8.185 (16) Å | T = 298 K |
c = 18.66 (4) Å | Block, purple |
V = 1037 (3) Å3 | 0.30 × 0.28 × 0.22 mm |
Z = 4 |
Bruker SMART APEXII CCD area-detector diffractometer | 1342 independent reflections |
Radiation source: fine-focus sealed tube | 748 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.061 |
ϕ and ω scans | θmax = 27.0°, θmin = 2.2° |
Absorption correction: multi-scan (SADABS; Sheldrick, 1996) | h = −8→7 |
Tmin = 0.959, Tmax = 0.970 | k = −8→10 |
6022 measured reflections | l = −23→23 |
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)] = 0.041 | Hydrogen site location: inferred from neighbouring sites |
wR(F2) = 0.112 | H atoms treated by a mixture of independent and constrained refinement |
S = 1.02 | w = 1/[σ2(Fo2) + (0.038P)2 + 0.0935P] where P = (Fo2 + 2Fc2)/3 |
1342 reflections | (Δ/σ)max < 0.001 |
153 parameters | Δρmax = 0.14 e Å−3 |
0 restraints | Δρmin = −0.15 e Å−3 |
C10H10F4N2 | V = 1037 (3) Å3 |
Mr = 234.20 | Z = 4 |
Orthorhombic, P212121 | Mo Kα radiation |
a = 6.791 (13) Å | µ = 0.14 mm−1 |
b = 8.185 (16) Å | T = 298 K |
c = 18.66 (4) Å | 0.30 × 0.28 × 0.22 mm |
Bruker SMART APEXII CCD area-detector diffractometer | 1342 independent reflections |
Absorption correction: multi-scan (SADABS; Sheldrick, 1996) | 748 reflections with I > 2σ(I) |
Tmin = 0.959, Tmax = 0.970 | Rint = 0.061 |
6022 measured reflections |
R[F2 > 2σ(F2)] = 0.041 | 0 restraints |
wR(F2) = 0.112 | H atoms treated by a mixture of independent and constrained refinement |
S = 1.02 | Δρmax = 0.14 e Å−3 |
1342 reflections | Δρmin = −0.15 e Å−3 |
153 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. Since this is a light atom structure (does not contain any atoms heavier than Si) and since the data collection was carried out using Mo radiation, it is not possible to unambiguously determine the absolute configuration of this molecule. |
x | y | z | Uiso*/Ueq | ||
F2 | 0.5502 (4) | 0.9533 (4) | 0.28755 (12) | 0.0946 (9) | |
F4 | 0.9856 (4) | 0.9465 (4) | 0.22927 (13) | 0.0938 (9) | |
F3 | 0.7878 (4) | 1.1542 (3) | 0.23004 (13) | 0.0903 (9) | |
F1 | 0.7058 (4) | 0.7458 (3) | 0.24699 (12) | 0.0897 (8) | |
C5 | 0.5124 (5) | 0.9963 (4) | 0.04139 (17) | 0.0451 (8) | |
C6 | 0.3393 (5) | 1.0854 (4) | 0.02680 (18) | 0.0491 (9) | |
C3 | 0.8125 (6) | 1.0019 (5) | 0.2037 (2) | 0.0608 (10) | |
C2 | 0.6375 (6) | 0.8962 (5) | 0.22754 (19) | 0.0595 (11) | |
C10 | 0.6062 (6) | 0.9131 (5) | −0.01323 (19) | 0.0575 (10) | |
H10 | 0.7199 | 0.8541 | −0.0031 | 0.069* | |
C7 | 0.2663 (6) | 1.0832 (5) | −0.0431 (2) | 0.0605 (11) | |
H7 | 0.1501 | 1.1383 | −0.0536 | 0.073* | |
C8 | 0.3635 (7) | 1.0009 (5) | −0.0966 (2) | 0.0688 (12) | |
H8 | 0.3133 | 1.0027 | −0.1430 | 0.083* | |
C9 | 0.5346 (7) | 0.9155 (5) | −0.0827 (2) | 0.0716 (13) | |
H9 | 0.6004 | 0.8608 | −0.1192 | 0.086* | |
C4 | 0.7993 (5) | 0.9997 (5) | 0.12353 (18) | 0.0583 (10) | |
H4A | 0.8623 | 1.0946 | 0.1025 | 0.070* | |
H4B | 0.8569 | 0.9013 | 0.1036 | 0.070* | |
C1 | 0.5016 (6) | 0.8845 (5) | 0.16406 (19) | 0.0665 (12) | |
H1A | 0.5021 | 0.7752 | 0.1440 | 0.080* | |
H1B | 0.3679 | 0.9136 | 0.1771 | 0.080* | |
N1 | 0.5854 (4) | 1.0035 (4) | 0.11341 (14) | 0.0466 (7) | |
N2 | 0.2447 (6) | 1.1710 (5) | 0.0805 (2) | 0.0653 (10) | |
H2A | 0.312 (7) | 1.201 (6) | 0.116 (3) | 0.091 (19)* | |
H2B | 0.171 (9) | 1.254 (9) | 0.068 (3) | 0.17 (3)* |
U11 | U22 | U33 | U12 | U13 | U23 | |
F2 | 0.093 (2) | 0.123 (2) | 0.0670 (14) | 0.0049 (17) | 0.0166 (15) | −0.0149 (14) |
F4 | 0.0610 (15) | 0.127 (2) | 0.0934 (19) | 0.0073 (16) | −0.0274 (15) | 0.0235 (16) |
F3 | 0.118 (2) | 0.0611 (15) | 0.0915 (17) | −0.0124 (16) | −0.0215 (16) | −0.0148 (13) |
F1 | 0.111 (2) | 0.0665 (15) | 0.0915 (17) | 0.0003 (16) | −0.0187 (16) | 0.0234 (14) |
C5 | 0.041 (2) | 0.047 (2) | 0.0470 (18) | −0.0033 (19) | −0.0009 (17) | 0.0050 (16) |
C6 | 0.047 (2) | 0.046 (2) | 0.054 (2) | −0.0019 (18) | −0.0030 (19) | 0.0006 (18) |
C3 | 0.056 (3) | 0.058 (3) | 0.068 (2) | 0.007 (2) | −0.016 (2) | 0.004 (2) |
C2 | 0.069 (3) | 0.062 (3) | 0.048 (2) | 0.006 (2) | −0.002 (2) | 0.008 (2) |
C10 | 0.058 (2) | 0.055 (2) | 0.059 (2) | 0.004 (2) | 0.003 (2) | −0.0032 (19) |
C7 | 0.057 (3) | 0.061 (2) | 0.064 (2) | 0.000 (2) | −0.016 (2) | 0.009 (2) |
C8 | 0.090 (3) | 0.069 (3) | 0.047 (2) | −0.013 (3) | −0.013 (2) | 0.000 (2) |
C9 | 0.087 (4) | 0.069 (3) | 0.058 (3) | −0.005 (3) | 0.005 (2) | −0.011 (2) |
C4 | 0.044 (2) | 0.070 (3) | 0.061 (2) | −0.004 (2) | −0.0026 (19) | 0.010 (2) |
C1 | 0.064 (3) | 0.074 (3) | 0.061 (2) | −0.017 (2) | −0.005 (2) | 0.017 (2) |
N1 | 0.0369 (16) | 0.0548 (18) | 0.0480 (16) | −0.0026 (15) | −0.0024 (14) | 0.0073 (15) |
N2 | 0.052 (2) | 0.073 (2) | 0.071 (2) | 0.011 (2) | 0.001 (2) | −0.004 (2) |
F2—C2 | 1.350 (5) | C7—C8 | 1.374 (6) |
F4—C3 | 1.347 (5) | C7—H7 | 0.9300 |
F3—C3 | 1.350 (5) | C8—C9 | 1.380 (6) |
F1—C2 | 1.365 (5) | C8—H8 | 0.9300 |
C5—C10 | 1.382 (5) | C9—H9 | 0.9300 |
C5—C6 | 1.409 (5) | C4—N1 | 1.465 (5) |
C5—N1 | 1.434 (5) | C4—H4A | 0.9700 |
C6—N2 | 1.381 (5) | C4—H4B | 0.9700 |
C6—C7 | 1.395 (5) | C1—N1 | 1.472 (5) |
C3—C4 | 1.498 (6) | C1—H1A | 0.9700 |
C3—C2 | 1.536 (6) | C1—H1B | 0.9700 |
C2—C1 | 1.505 (6) | N2—H2A | 0.84 (5) |
C10—C9 | 1.384 (6) | N2—H2B | 0.87 (7) |
C10—H10 | 0.9300 | ||
C10—C5—C6 | 119.8 (3) | C7—C8—C9 | 121.1 (4) |
C10—C5—N1 | 123.5 (3) | C7—C8—H8 | 119.5 |
C6—C5—N1 | 116.6 (3) | C9—C8—H8 | 119.5 |
N2—C6—C7 | 121.3 (4) | C8—C9—C10 | 118.6 (4) |
N2—C6—C5 | 120.7 (3) | C8—C9—H9 | 120.7 |
C7—C6—C5 | 118.1 (3) | C10—C9—H9 | 120.7 |
F4—C3—F3 | 106.8 (3) | N1—C4—C3 | 100.8 (3) |
F4—C3—C4 | 113.7 (3) | N1—C4—H4A | 111.6 |
F3—C3—C4 | 111.6 (3) | C3—C4—H4A | 111.6 |
F4—C3—C2 | 112.5 (3) | N1—C4—H4B | 111.6 |
F3—C3—C2 | 108.6 (3) | C3—C4—H4B | 111.6 |
C4—C3—C2 | 103.7 (3) | H4A—C4—H4B | 109.4 |
F2—C2—F1 | 103.9 (3) | N1—C1—C2 | 103.1 (3) |
F2—C2—C1 | 113.9 (4) | N1—C1—H1A | 111.2 |
F1—C2—C1 | 111.1 (3) | C2—C1—H1A | 111.2 |
F2—C2—C3 | 112.7 (4) | N1—C1—H1B | 111.2 |
F1—C2—C3 | 108.8 (3) | C2—C1—H1B | 111.2 |
C1—C2—C3 | 106.4 (3) | H1A—C1—H1B | 109.1 |
C5—C10—C9 | 121.5 (4) | C5—N1—C4 | 117.6 (3) |
C5—C10—H10 | 119.3 | C5—N1—C1 | 116.2 (3) |
C9—C10—H10 | 119.3 | C4—N1—C1 | 106.7 (3) |
C8—C7—C6 | 121.0 (4) | C6—N2—H2A | 117 (3) |
C8—C7—H7 | 119.5 | C6—N2—H2B | 118 (4) |
C6—C7—H7 | 119.5 | H2A—N2—H2B | 107 (5) |
C10—C5—C6—N2 | −179.2 (4) | C6—C7—C8—C9 | 1.1 (6) |
N1—C5—C6—N2 | −1.6 (5) | C7—C8—C9—C10 | 0.6 (6) |
C10—C5—C6—C7 | 1.3 (5) | C5—C10—C9—C8 | −1.3 (6) |
N1—C5—C6—C7 | 178.9 (3) | F4—C3—C4—N1 | 159.5 (3) |
F4—C3—C2—F2 | 93.9 (4) | F3—C3—C4—N1 | −79.6 (4) |
F3—C3—C2—F2 | −24.1 (4) | C2—C3—C4—N1 | 37.0 (4) |
C4—C3—C2—F2 | −142.8 (3) | F2—C2—C1—N1 | 115.4 (4) |
F4—C3—C2—F1 | −20.8 (4) | F1—C2—C1—N1 | −127.7 (4) |
F3—C3—C2—F1 | −138.8 (3) | C3—C2—C1—N1 | −9.4 (4) |
C4—C3—C2—F1 | 102.5 (3) | C10—C5—N1—C4 | 31.8 (5) |
F4—C3—C2—C1 | −140.6 (4) | C6—C5—N1—C4 | −145.8 (4) |
F3—C3—C2—C1 | 101.4 (4) | C10—C5—N1—C1 | −96.3 (4) |
C4—C3—C2—C1 | −17.3 (4) | C6—C5—N1—C1 | 86.2 (4) |
C6—C5—C10—C9 | 0.3 (5) | C3—C4—N1—C5 | −177.7 (3) |
N1—C5—C10—C9 | −177.1 (4) | C3—C4—N1—C1 | −45.2 (4) |
N2—C6—C7—C8 | 178.5 (4) | C2—C1—N1—C5 | 167.3 (3) |
C5—C6—C7—C8 | −2.0 (6) | C2—C1—N1—C4 | 34.1 (4) |
D—H···A | D—H | H···A | D···A | D—H···A |
N2—H2A···F1i | 0.84 (5) | 2.59 (5) | 3.295 (8) | 142 (4) |
Symmetry code: (i) −x+1, y+1/2, −z+1/2. |
Experimental details
Crystal data | |
Chemical formula | C10H10F4N2 |
Mr | 234.20 |
Crystal system, space group | Orthorhombic, P212121 |
Temperature (K) | 298 |
a, b, c (Å) | 6.791 (13), 8.185 (16), 18.66 (4) |
V (Å3) | 1037 (3) |
Z | 4 |
Radiation type | Mo Kα |
µ (mm−1) | 0.14 |
Crystal size (mm) | 0.30 × 0.28 × 0.22 |
Data collection | |
Diffractometer | Bruker SMART APEXII CCD area-detector diffractometer |
Absorption correction | Multi-scan (SADABS; Sheldrick, 1996) |
Tmin, Tmax | 0.959, 0.970 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 6022, 1342, 748 |
Rint | 0.061 |
(sin θ/λ)max (Å−1) | 0.639 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.041, 0.112, 1.02 |
No. of reflections | 1342 |
No. of parameters | 153 |
H-atom treatment | H atoms treated by a mixture of independent and constrained refinement |
Δρmax, Δρmin (e Å−3) | 0.14, −0.15 |
Computer programs: APEX2 (Bruker, 2008), SAINT (Bruker, 2008), SHELXS97 (Sheldrick, 2008), SHELXL97 (Sheldrick, 2008), SHELTLX (Sheldrick, 2008).
D—H···A | D—H | H···A | D···A | D—H···A |
N2—H2A···F1i | 0.84 (5) | 2.59 (5) | 3.295 (8) | 142 (4) |
Symmetry code: (i) −x+1, y+1/2, −z+1/2. |
Acknowledgements
The authors gratefully acknowledge the support of the Department of Science and Technology, Guangdong Province (grant No. 2010 A020507001–76, 5300410, FIPL-05–003).
References
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Fluorinated pyrrolidine derivatives have attracted much attention due to their potential applications as dipeptidyl peptidase IV inhibitors (Hulin et al., 2005), asymmetric synthesis catalysts (Marson, 2005), aurora kinase inhibitors (Kerekes et al., 2011), and H3 receptor antagonists (Santora et al., 2008). Herein, we report the crystal structure of the title compound (Fig. 1), obtained by the reaction of o-phenylenediamine with trifluoromethanesulfonic acid 2,2,3,3-tretrafluoro-1,4-butanediyl ester.
The dihedral angle between the plane of phenyl ring and the least-squares plane of pyrrolidine ring is 62.63 (14)°. The pyrrolidine ring adopts a distorted N1-envelope conformation with folding angle 40.6 (2)°. The crystal packing (Fig. 2) is characterized by intermolecular N—H···F—C bonds linking molecules in zigzag chains along b.