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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2008 Feb 29;64(Pt 3):o641. doi: 10.1107/S1600536808005369

4-Hydr­oxy-2,2,6,6-tetra­methyl­piperidinium trichloro­acetate

Peng-Wei Zhang a,b,*, Tong-Yun Zhang c, Li Zhang b, Yi Deng a
PMCID: PMC2960749  PMID: 21201972

Abstract

In the crystal structure of the title compound, C9H20NO+·Cl3CCOO, the cations and anions are connected via O—H⋯O, N—H⋯O, O—H⋯Cl and N—H⋯Cl hydrogen bonding. The six-membered ring adopts a chair conformation with the hydroxyl group in an equatorial position.

Related literature

For related literature, see: Borzatta & Carrozza (1991).graphic file with name e-64-0o641-scheme1.jpg

Experimental

Crystal data

  • C9H20NO+·C2Cl3O2

  • M r = 320.63

  • Monoclinic, Inline graphic

  • a = 6.3468 (13) Å

  • b = 14.450 (3) Å

  • c = 8.2175 (16) Å

  • β = 95.19 (3)°

  • V = 750.5 (3) Å3

  • Z = 2

  • Mo Kα radiation

  • μ = 0.61 mm−1

  • T = 113 (2) K

  • 0.12 × 0.10 × 0.08 mm

Data collection

  • Rigaku Saturn diffractometer

  • Absorption correction: multi-scan (CrystalClear; Rigaku/MSC, 2005) T min = 0.930, T max = 0.953

  • 5459 measured reflections

  • 2858 independent reflections

  • 2636 reflections with I > 2σ(I)

  • R int = 0.028

Refinement

  • R[F 2 > 2σ(F 2)] = 0.024

  • wR(F 2) = 0.060

  • S = 1.06

  • 2858 reflections

  • 179 parameters

  • 1 restraint

  • H atoms treated by a mixture of independent and constrained refinement

  • Δρmax = 0.21 e Å−3

  • Δρmin = −0.23 e Å−3

  • Absolute structure: Flack (1983), 996 Friedel pairs

  • Flack parameter: 0.04 (4)

Data collection: CrystalClear (Rigaku/MSC, 2005); cell refinement: CrystalClear; data reduction: CrystalClear; 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.

Supplementary Material

Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536808005369/hg2380sup1.cif

e-64-0o641-sup1.cif (17.9KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536808005369/hg2380Isup2.hkl

e-64-0o641-Isup2.hkl (140.3KB, hkl)

Additional supplementary materials: crystallographic information; 3D view; checkCIF report

Table 1. Hydrogen-bond geometry (Å, °).

D—H⋯A D—H H⋯A DA D—H⋯A
O1—H1⋯O3i 0.89 (3) 1.99 (3) 2.8095 (18) 152 (3)
O1—H1⋯Cl1i 0.89 (3) 2.92 (3) 3.6201 (16) 136 (2)
N1—H1A⋯O3ii 0.95 (3) 1.87 (3) 2.8085 (19) 170 (2)
N1—H1B⋯O2iii 0.94 (2) 1.87 (2) 2.796 (2) 165.1 (19)
N1—H1B⋯Cl2iii 0.94 (2) 2.94 (2) 3.5647 (16) 124.5 (16)

Symmetry codes: (i) Inline graphic; (ii) Inline graphic; (iii) Inline graphic.

supplementary crystallographic information

Comment

The title compound was obtained as a byproduct in the synthesis of hindered amine light stabilizers preventing the degradation of polyolefins in sunlight, in which 2,2,6,6-tetramethylpiperidin-4-ol is a very important intermediate (Borzatta & Carrozza,1991). We report here the crystal structure 4-hydroxy-2,2,6,6-tetramethylpiperidinium trichloroacetate (Fig. 1). Intermolecular O—H···O, N—H···O, O—H···Cl, N—H···Cl hydrogen bonds are observed which help to establish the crystal packing. The piperidine ring adopts a chair conformation.

Experimental

0.25 g (1.6 mmol) of 2,2,6,6-tetramethylpiperidin-4-ol was dissolved in 3.2 ml of trichloroacetate acid solution (1.6 mmol, 0.26 g). Colorless crystals of the title compound were obtained by slow evaporation of the solvent.

Refinement

All H atoms bound to C atoms were constrained; positioned geometrically (C—H = 0.96–0.98 Å) and refined as riding with Uiso(H)=1.2Ueq(carrier) or 1.5eq(methyl groups). H atoms of O—H and N—H were located from difference maps and then refined freely.

Figures

Fig. 1.

Fig. 1.

Crystal structure of the title compound with atom labeling and displacement ellipsoids drawn at the 30% probability level. H atoms are shown as small spheres of arbitrary radii.

Crystal data

C9H20NO+·C2Cl3O2 F000 = 336
Mr = 320.63 Dx = 1.419 Mg m3
Monoclinic, P21 Mo Kα radiation λ = 0.71073 Å
Hall symbol: P 2yb Cell parameters from 2559 reflections
a = 6.3468 (13) Å θ = 1.4–27.9º
b = 14.450 (3) Å µ = 0.61 mm1
c = 8.2175 (16) Å T = 113 (2) K
β = 95.19 (3)º Block, colorless
V = 750.5 (3) Å3 0.12 × 0.10 × 0.08 mm
Z = 2

Data collection

Rigaku Saturn diffractometer 2858 independent reflections
Radiation source: rotating anode 2636 reflections with I > 2σ(I)
Monochromator: confocal Rint = 0.028
T = 113(2) K θmax = 27.9º
ω and φ scans θmin = 2.5º
Absorption correction: multi-scan(CrystalClear; Rigaku/MSC, 2005) h = −8→8
Tmin = 0.930, Tmax = 0.953 k = −15→19
5459 measured reflections l = −10→10

Refinement

Refinement on F2 Hydrogen site location: inferred from neighbouring sites
Least-squares matrix: full H atoms treated by a mixture of independent and constrained refinement
R[F2 > 2σ(F2)] = 0.024   w = 1/[σ2(Fo2) + (0.0324P)2] where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.060 (Δ/σ)max = 0.001
S = 1.06 Δρmax = 0.21 e Å3
2858 reflections Δρmin = −0.23 e Å3
179 parameters Extinction correction: none
1 restraint Absolute structure: Flack (1983), 996 Friedel pairs
Primary atom site location: structure-invariant direct methods Flack parameter: 0.04 (4)
Secondary atom site location: difference Fourier map

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
Cl1 −0.04464 (7) 0.51471 (3) 0.10942 (5) 0.01980 (10)
Cl2 0.34863 (6) 0.41431 (3) 0.12885 (6) 0.02203 (11)
Cl3 −0.00077 (8) 0.35637 (3) −0.09864 (5) 0.02572 (11)
O1 0.7973 (2) 0.47566 (9) 0.51619 (17) 0.0227 (3)
H1 0.798 (4) 0.453 (2) 0.415 (4) 0.063 (10)*
O2 0.1032 (2) 0.27147 (9) 0.27469 (18) 0.0247 (3)
O3 −0.20242 (18) 0.34925 (9) 0.25644 (15) 0.0169 (3)
N1 0.4803 (2) 0.71305 (9) 0.64562 (18) 0.0111 (3)
C1 0.4608 (3) 0.62855 (12) 0.75507 (19) 0.0129 (3)
C2 0.6286 (3) 0.55858 (11) 0.7135 (2) 0.0139 (3)
H2A 0.7701 0.5832 0.7515 0.017*
H2B 0.6080 0.5005 0.7739 0.017*
C3 0.6235 (3) 0.53661 (11) 0.5324 (2) 0.0159 (4)
H3 0.4876 0.5051 0.4945 0.019*
C4 0.6475 (3) 0.62493 (13) 0.4346 (2) 0.0164 (3)
H4A 0.6371 0.6090 0.3170 0.020*
H4B 0.7905 0.6506 0.4638 0.020*
C5 0.4836 (3) 0.69993 (12) 0.46158 (19) 0.0135 (3)
C6 0.2366 (3) 0.58770 (13) 0.7353 (2) 0.0198 (4)
H6A 0.1327 0.6377 0.7379 0.030*
H6B 0.2191 0.5443 0.8248 0.030*
H6C 0.2149 0.5550 0.6306 0.030*
C7 0.5076 (3) 0.66393 (13) 0.9293 (2) 0.0189 (4)
H7A 0.6495 0.6912 0.9419 0.028*
H7B 0.5003 0.6124 1.0061 0.028*
H7C 0.4029 0.7110 0.9519 0.028*
C8 0.2629 (3) 0.67658 (13) 0.3825 (2) 0.0198 (4)
H8A 0.1595 0.7193 0.4228 0.030*
H8B 0.2266 0.6130 0.4104 0.030*
H8C 0.2609 0.6825 0.2636 0.030*
C9 0.5521 (3) 0.79290 (13) 0.3950 (2) 0.0213 (4)
H9A 0.4450 0.8399 0.4123 0.032*
H9B 0.5676 0.7871 0.2779 0.032*
H9C 0.6878 0.8113 0.4523 0.032*
C10 0.0700 (3) 0.40324 (12) 0.09850 (19) 0.0130 (3)
C11 −0.0172 (3) 0.33454 (11) 0.2249 (2) 0.0133 (3)
H1A 0.373 (4) 0.7546 (18) 0.674 (3) 0.037 (7)*
H1B 0.610 (4) 0.7410 (15) 0.683 (3) 0.025 (6)*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
Cl1 0.0227 (2) 0.01408 (19) 0.0232 (2) 0.00440 (16) 0.00505 (17) 0.00388 (16)
Cl2 0.01100 (19) 0.0235 (2) 0.0318 (3) −0.00221 (15) 0.00291 (17) 0.00920 (19)
Cl3 0.0321 (3) 0.0304 (3) 0.0149 (2) −0.0025 (2) 0.00289 (18) −0.00596 (17)
O1 0.0249 (7) 0.0194 (7) 0.0241 (7) 0.0108 (5) 0.0033 (6) −0.0052 (6)
O2 0.0147 (6) 0.0220 (7) 0.0377 (8) 0.0023 (5) 0.0044 (6) 0.0151 (6)
O3 0.0125 (6) 0.0160 (6) 0.0230 (7) −0.0007 (5) 0.0056 (5) −0.0007 (5)
N1 0.0114 (7) 0.0098 (7) 0.0124 (7) 0.0007 (5) 0.0033 (6) −0.0002 (5)
C1 0.0127 (8) 0.0130 (8) 0.0133 (8) 0.0010 (6) 0.0032 (6) 0.0029 (6)
C2 0.0137 (8) 0.0124 (8) 0.0156 (9) 0.0027 (6) 0.0014 (7) 0.0001 (6)
C3 0.0152 (8) 0.0131 (8) 0.0193 (9) 0.0035 (6) 0.0010 (7) −0.0028 (6)
C4 0.0164 (9) 0.0187 (8) 0.0149 (8) 0.0020 (6) 0.0049 (7) −0.0023 (7)
C5 0.0167 (8) 0.0153 (8) 0.0089 (7) 0.0010 (6) 0.0031 (6) 0.0010 (6)
C6 0.0152 (9) 0.0174 (9) 0.0276 (10) −0.0007 (7) 0.0059 (8) 0.0059 (7)
C7 0.0228 (9) 0.0215 (10) 0.0127 (8) 0.0047 (7) 0.0028 (7) 0.0000 (7)
C8 0.0196 (9) 0.0215 (9) 0.0176 (9) −0.0002 (7) −0.0023 (7) 0.0013 (7)
C9 0.0272 (11) 0.0164 (9) 0.0214 (10) −0.0001 (7) 0.0090 (8) 0.0043 (7)
C10 0.0118 (8) 0.0134 (8) 0.0141 (8) 0.0009 (6) 0.0021 (6) 0.0010 (6)
C11 0.0124 (8) 0.0145 (8) 0.0130 (8) −0.0019 (6) 0.0010 (6) −0.0006 (6)

Geometric parameters (Å, °)

Cl1—C10 1.7729 (17) C4—C5 1.532 (2)
Cl2—C10 1.7710 (17) C4—H4A 0.9900
Cl3—C10 1.7756 (17) C4—H4B 0.9900
O1—C3 1.427 (2) C5—C8 1.528 (2)
O1—H1 0.89 (3) C5—C9 1.529 (3)
O2—C11 1.235 (2) C6—H6A 0.9800
O3—C11 1.245 (2) C6—H6B 0.9800
N1—C5 1.526 (2) C6—H6C 0.9800
N1—C1 1.528 (2) C7—H7A 0.9800
N1—H1A 0.95 (3) C7—H7B 0.9800
N1—H1B 0.94 (2) C7—H7C 0.9800
C1—C7 1.524 (2) C8—H8A 0.9800
C1—C2 1.529 (2) C8—H8B 0.9800
C1—C6 1.535 (2) C8—H8C 0.9800
C2—C3 1.519 (2) C9—H9A 0.9800
C2—H2A 0.9900 C9—H9B 0.9800
C2—H2B 0.9900 C9—H9C 0.9800
C3—C4 1.523 (2) C10—C11 1.573 (2)
C3—H3 1.0000
C3—O1—H1 112.3 (19) C8—C5—C4 113.00 (15)
C5—N1—C1 119.53 (13) C9—C5—C4 110.55 (15)
C5—N1—H1A 113.1 (15) C1—C6—H6A 109.5
C1—N1—H1A 105.4 (15) C1—C6—H6B 109.5
C5—N1—H1B 106.5 (14) H6A—C6—H6B 109.5
C1—N1—H1B 105.4 (13) C1—C6—H6C 109.5
H1A—N1—H1B 106 (2) H6A—C6—H6C 109.5
C7—C1—N1 105.40 (13) H6B—C6—H6C 109.5
C7—C1—C2 110.56 (14) C1—C7—H7A 109.5
N1—C1—C2 107.56 (13) C1—C7—H7B 109.5
C7—C1—C6 109.16 (14) H7A—C7—H7B 109.5
N1—C1—C6 111.62 (14) C1—C7—H7C 109.5
C2—C1—C6 112.31 (14) H7A—C7—H7C 109.5
C3—C2—C1 113.80 (14) H7B—C7—H7C 109.5
C3—C2—H2A 108.8 C5—C8—H8A 109.5
C1—C2—H2A 108.8 C5—C8—H8B 109.5
C3—C2—H2B 108.8 H8A—C8—H8B 109.5
C1—C2—H2B 108.8 C5—C8—H8C 109.5
H2A—C2—H2B 107.7 H8A—C8—H8C 109.5
O1—C3—C2 105.80 (14) H8B—C8—H8C 109.5
O1—C3—C4 110.67 (14) C5—C9—H9A 109.5
C2—C3—C4 110.33 (14) C5—C9—H9B 109.5
O1—C3—H3 110.0 H9A—C9—H9B 109.5
C2—C3—H3 110.0 C5—C9—H9C 109.5
C4—C3—H3 110.0 H9A—C9—H9C 109.5
C3—C4—C5 114.51 (14) H9B—C9—H9C 109.5
C3—C4—H4A 108.6 C11—C10—Cl2 111.74 (11)
C5—C4—H4A 108.6 C11—C10—Cl1 111.69 (11)
C3—C4—H4B 108.6 Cl2—C10—Cl1 108.65 (9)
C5—C4—H4B 108.6 C11—C10—Cl3 106.67 (11)
H4A—C4—H4B 107.6 Cl2—C10—Cl3 109.25 (9)
N1—C5—C8 110.77 (14) Cl1—C10—Cl3 108.77 (9)
N1—C5—C9 105.97 (14) O2—C11—O3 128.65 (16)
C8—C5—C9 108.77 (14) O2—C11—C10 116.15 (14)
N1—C5—C4 107.55 (13) O3—C11—C10 115.14 (14)
C5—N1—C1—C7 168.77 (14) C1—N1—C5—C9 −167.95 (14)
C5—N1—C1—C2 50.78 (19) C1—N1—C5—C4 −49.69 (19)
C5—N1—C1—C6 −72.85 (19) C3—C4—C5—N1 50.25 (19)
C7—C1—C2—C3 −166.72 (14) C3—C4—C5—C8 −72.32 (19)
N1—C1—C2—C3 −52.12 (18) C3—C4—C5—C9 165.51 (16)
C6—C1—C2—C3 71.08 (18) Cl2—C10—C11—O2 −29.86 (19)
C1—C2—C3—O1 176.40 (14) Cl1—C10—C11—O2 −151.81 (14)
C1—C2—C3—C4 56.67 (19) Cl3—C10—C11—O2 89.47 (17)
O1—C3—C4—C5 −172.59 (14) Cl2—C10—C11—O3 152.80 (13)
C2—C3—C4—C5 −55.84 (19) Cl1—C10—C11—O3 30.85 (18)
C1—N1—C5—C8 74.25 (18) Cl3—C10—C11—O3 −87.87 (15)

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
O1—H1···O3i 0.89 (3) 1.99 (3) 2.8095 (18) 152 (3)
O1—H1···Cl1i 0.89 (3) 2.92 (3) 3.6201 (16) 136 (2)
N1—H1A···O3ii 0.95 (3) 1.87 (3) 2.8085 (19) 170 (2)
N1—H1B···O2iii 0.94 (2) 1.87 (2) 2.796 (2) 165.1 (19)
N1—H1B···Cl2iii 0.94 (2) 2.94 (2) 3.5647 (16) 124.5 (16)

Symmetry codes: (i) x+1, y, z; (ii) −x, y+1/2, −z+1; (iii) −x+1, y+1/2, −z+1.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: HG2380).

References

  1. Borzatta, V. & Carrozza, P. (1991). European Patent EP 0 462 069.
  2. Flack, H. D. (1983). Acta Cryst. A39, 876–881.
  3. Rigaku/MSC (2005). CrystalClear Rigaku/MSC, The Woodlands, Texas, USA.
  4. Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]

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/S1600536808005369/hg2380sup1.cif

e-64-0o641-sup1.cif (17.9KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536808005369/hg2380Isup2.hkl

e-64-0o641-Isup2.hkl (140.3KB, hkl)

Additional supplementary materials: crystallographic information; 3D view; checkCIF report


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