Abstract
The title compound, C9H20NO+·C2F3O2 −, is an important intermediate in the synthesis of hindered light stabilizers. The piperidinium ring adopts a chair conformation with the hydroxyl group in an equatorial position. The crystal packing is stabilized by O—H⋯O and N—H⋯O hydrogen bonds. The CF3 group is disordered over two positions with almost equal site occupancy factors.
Related literature
For general background, see: Borzatta & Carrozza (1991 ▶). For related structures, see: Nengfang et al. (2005 ▶).
Experimental
Crystal data
C9H20NO+·C2F3O2 −
M r = 271.28
Orthorhombic,
a = 7.6204 (8) Å
b = 9.8939 (10) Å
c = 18.099 (2) Å
V = 1364.6 (2) Å3
Z = 4
Mo Kα radiation
μ = 0.12 mm−1
T = 113 (2) K
0.22 × 0.20 × 0.16 mm
Data collection
Rigaku Saturn diffractometer
Absorption correction: multi-scan (CrystalClear; Rigaku/MSC, 2005 ▶) T min = 0.974, T max = 0.981
17989 measured reflections
2039 independent reflections
1993 reflections with I > 2σ(I)
R int = 0.057
Refinement
R[F 2 > 2σ(F 2)] = 0.057
wR(F 2) = 0.132
S = 1.23
2039 reflections
202 parameters
48 restraints
H-atom parameters constrained
Δρmax = 0.22 e Å−3
Δρmin = −0.21 e Å−3
Data collection: CrystalClear (Rigaku/MSC, 2005 ▶); cell refinement: CrystalClear; data reduction: CrystalClear; program(s) used to solve structure: SHELXS97 (Sheldrick, 1997 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997 ▶); molecular graphics: SHELXTL (Bruker, 1997 ▶); software used to prepare material for publication: CrystalStructure (Rigaku/MSC, 2005 ▶).
Supplementary Material
Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536807066305/bt2664sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536807066305/bt2664Isup2.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—H1B⋯O2 | 0.92 | 1.88 | 2.786 (3) | 169 |
| N1—H1A⋯O1i | 0.92 | 1.96 | 2.869 (3) | 171 |
| O1—H1⋯O3ii | 0.84 | 1.85 | 2.682 (3) | 171 |
Symmetry codes: (i)
; (ii)
.
supplementary crystallographic information
Comment
4-hydroxyl-2,2,6,6-tetramethylpiperidine is a very important intermediate in the synthesis of hindered light stabilizers (Borzatta & Carrozza, 1991; She et al., 2005). The piperidium ring adopts a chair conformation with the hydroxyl group in an equatorial position. The crystal packing is stabilized by O—H···O and N—H···O hydrogen bonds.
Experimental
An ethanol solution (10 ml) of 2,2,6,6-tetramethylpiperidin-4-ol (3.2 mmol, 0.5 g) was added dropwise to a stirred aqueous solution (6 ml) of trifluoroacetic acid (3.8 mmol, 0.43 g) at 293 K. Then the reaction mixture was filtered and the filtrate stood for about five days until colourless needle shaped crystals were obtained.
Refinement
In the absence of anomalous scatterers, Friedel pairs had been merged and the absolute structure was arbitrarily assigned. All H atoms were positioned geometrically with C—H ranging from 0.98Å to 1.00Å and refined as riding with Uiso(H)=1.2Ueq(C,N,O) or 1.5eq(Cmethyl). The CF3 group is disordered over two position with a ratio of occupancy factors of 0.459 (1)/0.541 (1). The atoms of the CF3 group were restrained to an isotropic behaviour.
Figures
Fig. 1.
A perspective view of the title compound. Displacement ellipsoids are drawn at the 30% probability level and H atoms are shown as small spheres of arbitrary radii. Only the major occupied site of the disordered CF3 group is shown.
Crystal data
| C9H20NO+·C2F3O2– | Dx = 1.320 Mg m−3 |
| Mr = 271.28 | Mo Kα radiation λ = 0.71070 Å |
| Orthorhombic, P212121 | Cell parameters from 4344 reflections |
| a = 7.6204 (8) Å | θ = 2.1–28.7º |
| b = 9.8939 (10) Å | µ = 0.12 mm−1 |
| c = 18.099 (2) Å | T = 113 (2) K |
| V = 1364.6 (2) Å3 | Needle, colourless |
| Z = 4 | 0.22 × 0.20 × 0.16 mm |
| F000 = 576 |
Data collection
| Rigaku Saturn diffractometer | 2039 independent reflections |
| Radiation source: rotating anode | 1993 reflections with I > 2σ(I) |
| Monochromator: confocal | Rint = 0.057 |
| Detector resolution: 14.63 pixels mm-1 | θmax = 28.7º |
| T = 113(2) K | θmin = 2.3º |
| ω scans | h = −10→10 |
| Absorption correction: multi-scan(CrystalClear; Rigaku/MSC, 2005) | k = −13→13 |
| Tmin = 0.974, Tmax = 0.981 | l = −24→24 |
| 17989 measured reflections |
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)] = 0.057 | H-atom parameters constrained |
| wR(F2) = 0.132 | w = 1/[σ2(Fo2) + (0.0506P)2 + 0.4132P] where P = (Fo2 + 2Fc2)/3 |
| S = 1.23 | (Δ/σ)max = 0.001 |
| 2039 reflections | Δρmax = 0.22 e Å−3 |
| 202 parameters | Δρmin = −0.21 e Å−3 |
| 48 restraints | Extinction correction: SHELXL, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4 |
| Primary atom site location: structure-invariant direct methods | Extinction coefficient: 0.028 (4) |
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 | Occ. (<1) | |
| O1 | 0.9028 (3) | −0.20835 (18) | 0.73102 (11) | 0.0271 (5) | |
| H1 | 0.8683 | −0.2769 | 0.7078 | 0.041* | |
| O2 | 0.6874 (3) | 0.4099 (2) | 0.58896 (13) | 0.0394 (6) | |
| O3 | 0.7885 (3) | 0.5590 (2) | 0.67201 (12) | 0.0398 (6) | |
| N1 | 0.8175 (3) | 0.1997 (2) | 0.67551 (12) | 0.0226 (5) | |
| H1A | 0.9012 | 0.2378 | 0.7056 | 0.027* | |
| H1B | 0.7631 | 0.2695 | 0.6510 | 0.027* | |
| C1 | 0.6801 (4) | 0.1339 (3) | 0.72563 (15) | 0.0244 (5) | |
| C2 | 0.7571 (4) | 0.0022 (3) | 0.75609 (14) | 0.0241 (5) | |
| H2A | 0.8503 | 0.0245 | 0.7922 | 0.029* | |
| H2B | 0.6639 | −0.0475 | 0.7827 | 0.029* | |
| C3 | 0.8336 (4) | −0.0893 (3) | 0.69685 (14) | 0.0233 (5) | |
| H3 | 0.7392 | −0.1152 | 0.6612 | 0.028* | |
| C4 | 0.9789 (4) | −0.0143 (3) | 0.65571 (15) | 0.0234 (5) | |
| H4A | 1.0300 | −0.0753 | 0.6181 | 0.028* | |
| H4B | 1.0729 | 0.0095 | 0.6911 | 0.028* | |
| C5 | 0.9142 (4) | 0.1151 (3) | 0.61754 (14) | 0.0241 (6) | |
| C6 | 0.6475 (4) | 0.2352 (3) | 0.78794 (18) | 0.0326 (7) | |
| H6A | 0.7557 | 0.2477 | 0.8164 | 0.049* | |
| H6B | 0.5549 | 0.2009 | 0.8205 | 0.049* | |
| H6C | 0.6110 | 0.3220 | 0.7668 | 0.049* | |
| C7 | 0.5089 (4) | 0.1126 (3) | 0.68236 (19) | 0.0335 (7) | |
| H7A | 0.4141 | 0.0899 | 0.7168 | 0.050* | |
| H7B | 0.5244 | 0.0387 | 0.6469 | 0.050* | |
| H7C | 0.4789 | 0.1958 | 0.6558 | 0.050* | |
| C8 | 1.0678 (4) | 0.2025 (3) | 0.59214 (16) | 0.0302 (6) | |
| H8A | 1.0229 | 0.2852 | 0.5691 | 0.045* | |
| H8B | 1.1384 | 0.1522 | 0.5562 | 0.045* | |
| H8C | 1.1408 | 0.2262 | 0.6348 | 0.045* | |
| C9 | 0.7963 (4) | 0.0851 (3) | 0.55106 (16) | 0.0331 (7) | |
| H9A | 0.7112 | 0.0149 | 0.5643 | 0.050* | |
| H9B | 0.8685 | 0.0536 | 0.5097 | 0.050* | |
| H9C | 0.7338 | 0.1675 | 0.5366 | 0.050* | |
| C10 | 0.7562 (4) | 0.5187 (3) | 0.60881 (16) | 0.0281 (6) | |
| C11 | 0.8356 (12) | 0.6096 (9) | 0.5496 (5) | 0.037 (3) | 0.459 (14) |
| F1 | 0.7559 (17) | 0.7299 (6) | 0.5473 (4) | 0.067 (3) | 0.459 (14) |
| F2 | 1.0045 (10) | 0.6341 (15) | 0.5611 (4) | 0.086 (4) | 0.459 (14) |
| F3 | 0.8194 (18) | 0.5655 (13) | 0.4799 (6) | 0.070 (4) | 0.459 (14) |
| C11' | 0.7828 (13) | 0.6165 (8) | 0.5453 (4) | 0.042 (3) | 0.541 (14) |
| F1' | 0.6352 (15) | 0.6809 (12) | 0.5291 (5) | 0.126 (4) | 0.541 (14) |
| F2' | 0.900 (2) | 0.7116 (8) | 0.5599 (3) | 0.099 (5) | 0.541 (14) |
| F3' | 0.8406 (14) | 0.5571 (12) | 0.4839 (5) | 0.070 (4) | 0.541 (14) |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| O1 | 0.0347 (11) | 0.0164 (8) | 0.0303 (10) | 0.0008 (8) | −0.0069 (9) | 0.0017 (8) |
| O2 | 0.0504 (13) | 0.0219 (10) | 0.0458 (12) | −0.0013 (10) | −0.0187 (11) | −0.0011 (9) |
| O3 | 0.0615 (15) | 0.0274 (10) | 0.0306 (11) | −0.0091 (11) | −0.0059 (11) | −0.0024 (9) |
| N1 | 0.0236 (11) | 0.0177 (10) | 0.0266 (10) | −0.0003 (9) | −0.0010 (9) | −0.0003 (9) |
| C1 | 0.0212 (12) | 0.0193 (11) | 0.0327 (14) | −0.0006 (10) | 0.0012 (11) | 0.0002 (10) |
| C2 | 0.0220 (12) | 0.0239 (12) | 0.0266 (12) | −0.0010 (11) | 0.0014 (10) | 0.0015 (10) |
| C3 | 0.0260 (13) | 0.0189 (11) | 0.0251 (12) | 0.0016 (10) | −0.0050 (10) | 0.0015 (10) |
| C4 | 0.0242 (12) | 0.0226 (12) | 0.0235 (12) | 0.0017 (11) | −0.0001 (10) | −0.0021 (10) |
| C5 | 0.0278 (13) | 0.0202 (12) | 0.0244 (12) | 0.0020 (11) | −0.0004 (11) | −0.0008 (10) |
| C6 | 0.0298 (15) | 0.0269 (14) | 0.0412 (16) | 0.0004 (12) | 0.0098 (13) | −0.0047 (13) |
| C7 | 0.0242 (13) | 0.0266 (13) | 0.0498 (18) | 0.0009 (11) | −0.0036 (13) | 0.0032 (14) |
| C8 | 0.0356 (16) | 0.0263 (14) | 0.0286 (14) | −0.0029 (13) | 0.0046 (12) | 0.0016 (12) |
| C9 | 0.0434 (18) | 0.0272 (14) | 0.0287 (14) | 0.0013 (13) | −0.0109 (13) | 0.0016 (11) |
| C10 | 0.0292 (13) | 0.0200 (12) | 0.0351 (14) | 0.0032 (11) | −0.0061 (12) | −0.0015 (11) |
| C11 | 0.048 (5) | 0.030 (5) | 0.033 (5) | −0.009 (4) | −0.006 (4) | −0.004 (4) |
| F1 | 0.132 (8) | 0.020 (3) | 0.049 (4) | 0.017 (4) | 0.014 (4) | 0.011 (2) |
| F2 | 0.064 (5) | 0.129 (9) | 0.065 (4) | −0.058 (5) | 0.007 (3) | 0.005 (5) |
| F3 | 0.136 (10) | 0.043 (6) | 0.030 (5) | −0.037 (6) | −0.025 (5) | 0.002 (4) |
| C11' | 0.063 (6) | 0.037 (4) | 0.026 (4) | 0.000 (4) | −0.010 (3) | −0.001 (3) |
| F1' | 0.123 (7) | 0.136 (7) | 0.120 (6) | 0.051 (6) | −0.004 (5) | 0.080 (5) |
| F2' | 0.198 (13) | 0.060 (5) | 0.039 (3) | −0.082 (7) | 0.013 (6) | −0.012 (3) |
| F3' | 0.105 (7) | 0.063 (7) | 0.042 (5) | −0.025 (5) | 0.042 (4) | −0.024 (4) |
Geometric parameters (Å, °)
| O1—C3 | 1.431 (3) | C6—H6A | 0.9800 |
| O1—H1 | 0.8400 | C6—H6B | 0.9800 |
| O2—C10 | 1.250 (3) | C6—H6C | 0.9800 |
| O3—C10 | 1.236 (3) | C7—H7A | 0.9800 |
| N1—C1 | 1.531 (3) | C7—H7B | 0.9800 |
| N1—C5 | 1.531 (3) | C7—H7C | 0.9800 |
| N1—H1A | 0.9200 | C8—H8A | 0.9800 |
| N1—H1B | 0.9200 | C8—H8B | 0.9800 |
| C1—C6 | 1.529 (4) | C8—H8C | 0.9800 |
| C1—C2 | 1.531 (4) | C9—H9A | 0.9800 |
| C1—C7 | 1.537 (4) | C9—H9B | 0.9800 |
| C2—C3 | 1.519 (4) | C9—H9C | 0.9800 |
| C2—H2A | 0.9900 | C10—C11' | 1.516 (7) |
| C2—H2B | 0.9900 | C10—C11 | 1.525 (8) |
| C3—C4 | 1.526 (4) | C11—F2 | 1.326 (9) |
| C3—H3 | 1.0000 | C11—F1 | 1.337 (8) |
| C4—C5 | 1.536 (4) | C11—F3 | 1.339 (8) |
| C4—H4A | 0.9900 | C11'—F2' | 1.324 (8) |
| C4—H4B | 0.9900 | C11'—F1' | 1.325 (8) |
| C5—C8 | 1.527 (4) | C11'—F3' | 1.333 (8) |
| C5—C9 | 1.530 (4) | ||
| C3—O1—H1 | 109.5 | H6A—C6—H6B | 109.5 |
| C1—N1—C5 | 120.2 (2) | C1—C6—H6C | 109.5 |
| C1—N1—H1A | 107.3 | H6A—C6—H6C | 109.5 |
| C5—N1—H1A | 107.3 | H6B—C6—H6C | 109.5 |
| C1—N1—H1B | 107.3 | C1—C7—H7A | 109.5 |
| C5—N1—H1B | 107.3 | C1—C7—H7B | 109.5 |
| H1A—N1—H1B | 106.9 | H7A—C7—H7B | 109.5 |
| C6—C1—N1 | 105.6 (2) | C1—C7—H7C | 109.5 |
| C6—C1—C2 | 110.8 (2) | H7A—C7—H7C | 109.5 |
| N1—C1—C2 | 108.2 (2) | H7B—C7—H7C | 109.5 |
| C6—C1—C7 | 109.1 (2) | C5—C8—H8A | 109.5 |
| N1—C1—C7 | 109.7 (2) | C5—C8—H8B | 109.5 |
| C2—C1—C7 | 113.1 (2) | H8A—C8—H8B | 109.5 |
| C3—C2—C1 | 113.6 (2) | C5—C8—H8C | 109.5 |
| C3—C2—H2A | 108.9 | H8A—C8—H8C | 109.5 |
| C1—C2—H2A | 108.9 | H8B—C8—H8C | 109.5 |
| C3—C2—H2B | 108.9 | C5—C9—H9A | 109.5 |
| C1—C2—H2B | 108.9 | C5—C9—H9B | 109.5 |
| H2A—C2—H2B | 107.7 | H9A—C9—H9B | 109.5 |
| O1—C3—C2 | 109.1 (2) | C5—C9—H9C | 109.5 |
| O1—C3—C4 | 110.1 (2) | H9A—C9—H9C | 109.5 |
| C2—C3—C4 | 109.5 (2) | H9B—C9—H9C | 109.5 |
| O1—C3—H3 | 109.4 | O3—C10—O2 | 128.9 (3) |
| C2—C3—H3 | 109.4 | O3—C10—C11' | 117.9 (4) |
| C4—C3—H3 | 109.4 | O2—C10—C11' | 112.8 (4) |
| C3—C4—C5 | 113.1 (2) | O3—C10—C11 | 112.4 (4) |
| C3—C4—H4A | 109.0 | O2—C10—C11 | 118.2 (4) |
| C5—C4—H4A | 109.0 | F2—C11—F1 | 106.4 (8) |
| C3—C4—H4B | 109.0 | F2—C11—F3 | 107.3 (8) |
| C5—C4—H4B | 109.0 | F1—C11—F3 | 102.6 (8) |
| H4A—C4—H4B | 107.8 | F2—C11—C10 | 112.5 (7) |
| C8—C5—C9 | 108.9 (2) | F1—C11—C10 | 111.5 (7) |
| C8—C5—N1 | 105.4 (2) | F3—C11—C10 | 115.7 (9) |
| C9—C5—N1 | 111.2 (2) | F2'—C11'—F1' | 106.0 (8) |
| C8—C5—C4 | 111.2 (2) | F2'—C11'—F3' | 104.8 (8) |
| C9—C5—C4 | 112.4 (2) | F1'—C11'—F3' | 107.9 (8) |
| N1—C5—C4 | 107.6 (2) | F2'—C11'—C10 | 113.2 (6) |
| C1—C6—H6A | 109.5 | F1'—C11'—C10 | 111.2 (6) |
| C1—C6—H6B | 109.5 | F3'—C11'—C10 | 113.3 (8) |
| C5—N1—C1—C6 | 165.7 (2) | O2—C10—C11—F2 | −121.8 (8) |
| C5—N1—C1—C2 | 47.0 (3) | C11'—C10—C11—F2 | 164 (3) |
| C5—N1—C1—C7 | −76.9 (3) | O3—C10—C11—F1 | −69.1 (8) |
| C6—C1—C2—C3 | −166.0 (2) | O2—C10—C11—F1 | 118.7 (8) |
| N1—C1—C2—C3 | −50.6 (3) | C11'—C10—C11—F1 | 45 (2) |
| C7—C1—C2—C3 | 71.2 (3) | O3—C10—C11—F3 | 174.2 (8) |
| C1—C2—C3—O1 | 179.6 (2) | O2—C10—C11—F3 | 2.0 (11) |
| C1—C2—C3—C4 | 59.1 (3) | C11'—C10—C11—F3 | −72 (2) |
| O1—C3—C4—C5 | −180.0 (2) | O3—C10—C11'—F2' | 25.7 (9) |
| C2—C3—C4—C5 | −60.1 (3) | O2—C10—C11'—F2' | −160.6 (8) |
| C1—N1—C5—C8 | −166.6 (2) | C11—C10—C11'—F2' | −47 (2) |
| C1—N1—C5—C9 | 75.6 (3) | O3—C10—C11'—F1' | −93.5 (8) |
| C1—N1—C5—C4 | −47.8 (3) | O2—C10—C11'—F1' | 80.2 (9) |
| C3—C4—C5—C8 | 167.3 (2) | C11—C10—C11'—F1' | −167 (3) |
| C3—C4—C5—C9 | −70.4 (3) | O3—C10—C11'—F3' | 144.8 (8) |
| C3—C4—C5—N1 | 52.4 (3) | O2—C10—C11'—F3' | −41.5 (10) |
| O3—C10—C11—F2 | 50.4 (9) | C11—C10—C11'—F3' | 72 (2) |
Hydrogen-bond geometry (Å, °)
| D—H···A | D—H | H···A | D···A | D—H···A |
| N1—H1B···O2 | 0.92 | 1.88 | 2.786 (3) | 169 |
| N1—H1A···O1i | 0.92 | 1.96 | 2.869 (3) | 171 |
| O1—H1···O3ii | 0.84 | 1.85 | 2.682 (3) | 171 |
Symmetry codes: (i) −x+2, y+1/2, −z+3/2; (ii) x, y−1, z.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: BT2664).
References
- Borzatta, V. & Carrozza, P. (1991). European Patent EP 0 462 069.
- Bruker (1997). SHELXTL Bruker AXS Inc., Madison, Wisconsin, USA.
- Rigaku/MSC (2005). CrystalClear and CrystalStructure Rigaku/MSC, The Woodlands, Texas, USA.
- Nengfang, S., Guo, H. Z., Yin, G. & Wu, A. (2005). Acta Cryst E61, o2902–o2903.
- Sheldrick, G. M. (1997). SHELXS97 and SHELXL97 University of Göttingen, Germany.
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/S1600536807066305/bt2664sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536807066305/bt2664Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report

