organic compounds\(\def\hfill{\hskip 5em}\def\hfil{\hskip 3em}\def\eqno#1{\hfil {#1}}\)

Journal logoCRYSTALLOGRAPHIC
COMMUNICATIONS
ISSN: 2056-9890

4-Hydr­­oxy-2,2,6,6-tetra­methyl­piperidinium chloride–hydroxonium chloride (3/1)

aDepartment of Pharmaceutics, Medical College of the Chinese People's Armed Police Force, Tianjin 300162, People's Republic of China, and bSchool of Pharmaceutical Science & Technology, Tianjin University, Tianjin 300072, People's Republic of China
*Correspondence e-mail: zpw0803@gmail.com

(Received 9 January 2008; accepted 21 January 2008; online 25 January 2008)

The crystal structure of the title compound, C9H20NO+·Cl·0.33(H3O+·Cl), is composed of 4-hydr­oxy-2,2,6,6-tetra­methyl­piperidinium cations, hydroxonium cations and chloride anions, which are connected via O—H⋯O, O—H⋯Cl and N—H⋯Cl hydrogen bonding. The 4-hydr­oxy-2,2,6,6-tetra­methyl­piperidinium cation and one of the two crystallographically independent chloride anions are located on a mirror plane. The hydroxonium cation is located on a threefold axis and the second crystallographically independent chloride anion is located on a sixfold rotoinversion axis. Due to symmetry, the hydroxonium cation is disordered over two positions.

[Scheme 1]

Experimental

Crystal data
  • C9H20NO+·Cl·0.33(H3O+·Cl)

  • Mr = 211.87

  • Hexagonal, P 63 /m

  • a = 13.4460 (19) Å

  • c = 11.528 (2) Å

  • V = 1804.9 (5) Å3

  • Z = 6

  • Mo Kα radiation

  • μ = 0.36 mm−1

  • T = 113 (2) K

  • 0.10 × 0.10 × 0.04 mm

Data collection
  • Rigaku Saturn diffractometer

  • Absorption correction: multi-scan (CrystalClear; Rigaku/MSC, 2005[Rigaku/MSC (2005). CrystalClear and CrystalStructure. Rigaku/MSC, The Woodlands, Texas, USA.]) Tmin = 0.968, Tmax = 0.989

  • 14051 measured reflections

  • 1513 independent reflections

  • 1424 reflections with I > 2σ(I)

  • Rint = 0.075

Refinement
  • R[F2 > 2σ(F2)] = 0.051

  • wR(F2) = 0.130

  • S = 1.08

  • 1513 reflections

  • 68 parameters

  • H-atom parameters constrained

  • Δρmax = 0.33 e Å−3

  • Δρmin = −0.26 e Å−3

Table 1
Hydrogen-bond geometry (Å, °)

D—H⋯A D—H H⋯A DA D—H⋯A
O1—H1⋯Cl2i 0.85 2.15 2.991 (2) 172
N1—H1B⋯Cl2ii 0.92 2.22 3.139 (2) 175
N1—H1C⋯Cl1iii 0.92 2.25 3.166 (2) 176
O2—H2⋯O1iv 0.85 1.63 2.475 (2) 175
Symmetry codes: (i) -y, x-y, z; (ii) -x+y+1, -x+1, z; (iii) -x+1, -y+1, -z+1; (iv) x+1, y, z.

Data collection: CrystalClear (Rigaku/MSC, 2005[Rigaku/MSC (2005). CrystalClear and CrystalStructure. Rigaku/MSC, The Woodlands, Texas, USA.]); cell refinement: CrystalClear; data reduction: CrystalClear; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008[Sheldrick, G. M. (2008). Acta Cryst. A64, 112-122.]); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008[Sheldrick, G. M. (2008). Acta Cryst. A64, 112-122.]); molecular graphics: SHELXTL (Sheldrick, 2008[Sheldrick, G. M. (2008). Acta Cryst. A64, 112-122.]); software used to prepare material for publication: SHELXTL.

Supporting information


Comment top

The title compound was obtained as a byproduct in the synthesis of hindered light stabilizer. For the characterization of this compound a crystal structure analysis was performed. The crystal structure of this compound consists of 4-hydroxy-2,2,6,6-tetramethylpiperidinium cations, hydroxonium cations and chloride anions, all of them located in special positions (Fig. 1). The cations and the anions are connected via O—H···O, O—H···Cl and N—H···Cl hydrogen bonding (Table 1). The isolated water oxygen atom, which is located on a 3-fold axis is disordered in two positions because of symmetry. For charge balance it must be protonated. However, the corresponding H atom was clearly located in difference map.

Experimental top

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

Refinement top

The C—H and N—H H atoms were positioned with idealized geometry (methyl allowed to rotate but not to tip) and refined isotropic with Uiso(H)=1.2 Ueq(carrier atom; 1.5 for methyl H atoms) using a riding model with C—H = 0.98 - 1.00Å and N—H = 1.00 Å. The O—H H atoms were located in different map, their bond length were set to 0.85Å and afterwards they were refined isotropic (Uiso(H)=1.2Ueq(carrier atom)) using a riding model.

Computing details top

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

Figures top
[Figure 1] Fig. 1. Crystal structure of the title compound with labeling and displacement ellipsoids drawn at the 30% probability level. H atoms are shown as small spheres of arbitrary radii. Symmetry codes: A = x,y,0.5 - z.
4-Hydroxy-2,2,6,6-tetramethylpiperidinium chloride–hydroxonium chloride (3/1) top
Crystal data top
C9H20NO+·Cl·0.33(H3O+·Cl)Dx = 1.170 Mg m3
Mr = 211.87Mo Kα radiation, λ = 0.71073 Å
Hexagonal, P63/mCell parameters from 4368 reflections
a = 13.4460 (19) Åθ = 1.8–27.9°
c = 11.528 (2) ŵ = 0.36 mm1
V = 1804.9 (5) Å3T = 113 K
Z = 6Block, colorless
F(000) = 6920.10 × 0.10 × 0.04 mm
Data collection top
Rigaku Saturn
diffractometer
1513 independent reflections
Radiation source: rotating anode1424 reflections with I > 2σ(I)
Confocal monochromatorRint = 0.075
Detector resolution: 7.31 pixels mm-1θmax = 27.9°, θmin = 2.5°
ω scansh = 1317
Absorption correction: multi-scan
(CrystalClear; Rigaku/MSC, 2005)
k = 1716
Tmin = 0.968, Tmax = 0.989l = 1415
14051 measured reflections
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.051Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.130H-atom parameters constrained
S = 1.08 w = 1/[σ2(Fo2) + (0.0699P)2 + 0.5807P]
where P = (Fo2 + 2Fc2)/3
1513 reflections(Δ/σ)max < 0.001
68 parametersΔρmax = 0.33 e Å3
0 restraintsΔρmin = 0.26 e Å3
Crystal data top
C9H20NO+·Cl·0.33(H3O+·Cl)Z = 6
Mr = 211.87Mo Kα radiation
Hexagonal, P63/mµ = 0.36 mm1
a = 13.4460 (19) ÅT = 113 K
c = 11.528 (2) Å0.10 × 0.10 × 0.04 mm
V = 1804.9 (5) Å3
Data collection top
Rigaku Saturn
diffractometer
1513 independent reflections
Absorption correction: multi-scan
(CrystalClear; Rigaku/MSC, 2005)
1424 reflections with I > 2σ(I)
Tmin = 0.968, Tmax = 0.989Rint = 0.075
14051 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0510 restraints
wR(F2) = 0.130H-atom parameters constrained
S = 1.08Δρmax = 0.33 e Å3
1513 reflectionsΔρmin = 0.26 e Å3
68 parameters
Special details top

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) top
xyzUiso*/UeqOcc. (<1)
O10.13431 (15)0.43006 (16)0.25000.0420 (6)
H10.09860.50310.25000.050*
N10.16134 (16)0.39830 (16)0.25000.0174 (4)
H1B0.20190.35980.25000.021*
H1C0.21450.47550.25000.021*
C10.0587 (2)0.3833 (2)0.25000.0283 (6)
H1A0.10630.29760.25000.034*
C20.01605 (15)0.42088 (15)0.35766 (18)0.0260 (4)
H2A0.03390.39650.42710.031*
H2B0.06250.50580.35870.031*
C30.09668 (15)0.37155 (15)0.36468 (16)0.0213 (4)
C40.03335 (16)0.24188 (16)0.38919 (18)0.0279 (4)
H4A0.03620.20370.34150.042*
H4B0.01230.22840.47140.042*
H4C0.08360.21080.37020.042*
C50.18849 (18)0.43315 (17)0.45708 (17)0.0302 (4)
H5A0.24380.40600.45420.045*
H5B0.15230.41700.53380.045*
H5C0.22830.51610.44260.045*
Cl10.66670.33330.75000.0219 (3)
Cl20.71701 (5)0.03169 (5)0.25000.0244 (2)
O20.66670.33330.3252 (4)0.0276 (10)0.50
H20.73520.37040.29990.041*0.50
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O10.0168 (9)0.0200 (9)0.091 (2)0.0103 (8)0.0000.000
N10.0169 (9)0.0186 (9)0.0159 (11)0.0083 (8)0.0000.000
C10.0176 (12)0.0170 (11)0.052 (2)0.0096 (9)0.0000.000
C20.0239 (9)0.0212 (8)0.0318 (11)0.0105 (7)0.0114 (8)0.0049 (7)
C30.0232 (8)0.0232 (8)0.0173 (9)0.0114 (7)0.0050 (7)0.0036 (6)
C40.0278 (9)0.0248 (9)0.0313 (11)0.0133 (8)0.0075 (8)0.0092 (8)
C50.0376 (10)0.0329 (10)0.0162 (10)0.0146 (9)0.0007 (8)0.0022 (8)
Cl10.0202 (3)0.0202 (3)0.0254 (6)0.01012 (16)0.0000.000
Cl20.0251 (3)0.0203 (3)0.0295 (4)0.0125 (2)0.0000.000
O20.0243 (14)0.0243 (14)0.034 (3)0.0121 (7)0.0000.000
Geometric parameters (Å, º) top
O1—C11.438 (3)C2—H2B0.9900
O1—H10.8500C3—C51.524 (3)
N1—C31.523 (2)C3—C41.536 (2)
N1—C3i1.523 (2)C4—H4A0.9800
N1—H1B0.9200C4—H4B0.9800
N1—H1C0.9200C4—H4C0.9800
C1—C21.516 (2)C5—H5A0.9800
C1—C2i1.516 (2)C5—H5B0.9800
C1—H1A1.0000C5—H5C0.9800
C2—C31.530 (2)O2—O2i1.733 (10)
C2—H2A0.9900O2—H20.8501
C1—O1—H1113.0N1—C3—C5105.47 (14)
C3—N1—C3i120.43 (18)N1—C3—C2107.23 (15)
C3—N1—H1B107.2C5—C3—C2111.00 (16)
C3i—N1—H1B107.2N1—C3—C4110.77 (15)
C3—N1—H1C107.2C5—C3—C4109.09 (15)
C3i—N1—H1C107.2C2—C3—C4113.01 (14)
H1B—N1—H1C106.9C3—C4—H4A109.5
O1—C1—C2110.50 (13)C3—C4—H4B109.5
O1—C1—C2i110.51 (13)H4A—C4—H4B109.5
C2—C1—C2i109.9 (2)C3—C4—H4C109.5
O1—C1—H1A108.6H4A—C4—H4C109.5
C2—C1—H1A108.6H4B—C4—H4C109.5
C2i—C1—H1A108.6C3—C5—H5A109.5
C1—C2—C3113.23 (16)C3—C5—H5B109.5
C1—C2—H2A108.9H5A—C5—H5B109.5
C3—C2—H2A108.9C3—C5—H5C109.5
C1—C2—H2B108.9H5A—C5—H5C109.5
C3—C2—H2B108.9H5B—C5—H5C109.5
H2A—C2—H2B107.7O2i—O2—H269.9
O1—C1—C2—C3178.55 (15)C3i—N1—C3—C474.5 (2)
C2i—C1—C2—C359.2 (2)C1—C2—C3—N151.7 (2)
C3i—N1—C3—C5167.57 (14)C1—C2—C3—C5166.46 (16)
C3i—N1—C3—C249.2 (2)C1—C2—C3—C470.6 (2)
Symmetry code: (i) x, y, z+1/2.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O1—H1···Cl2ii0.852.152.991 (2)172
N1—H1B···Cl2iii0.922.223.139 (2)175
N1—H1C···Cl1iv0.922.253.166 (2)176
O2—H2···O1v0.851.632.475 (2)175
Symmetry codes: (ii) y, xy, z; (iii) x+y+1, x+1, z; (iv) x+1, y+1, z+1; (v) x+1, y, z.

Experimental details

Crystal data
Chemical formulaC9H20NO+·Cl·0.33(H3O+·Cl)
Mr211.87
Crystal system, space groupHexagonal, P63/m
Temperature (K)113
a, c (Å)13.4460 (19), 11.528 (2)
V3)1804.9 (5)
Z6
Radiation typeMo Kα
µ (mm1)0.36
Crystal size (mm)0.10 × 0.10 × 0.04
Data collection
DiffractometerRigaku Saturn
diffractometer
Absorption correctionMulti-scan
(CrystalClear; Rigaku/MSC, 2005)
Tmin, Tmax0.968, 0.989
No. of measured, independent and
observed [I > 2σ(I)] reflections
14051, 1513, 1424
Rint0.075
(sin θ/λ)max1)0.658
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.051, 0.130, 1.08
No. of reflections1513
No. of parameters68
H-atom treatmentH-atom parameters constrained
Δρmax, Δρmin (e Å3)0.33, 0.26

Computer programs: CrystalClear (Rigaku/MSC, 2005), SHELXS97 (Sheldrick, 2008), SHELXL97 (Sheldrick, 2008), SHELXTL (Sheldrick, 2008).

Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O1—H1···Cl2i0.852.152.991 (2)172.0
N1—H1B···Cl2ii0.922.223.139 (2)174.6
N1—H1C···Cl1iii0.922.253.166 (2)175.7
O2—H2···O1iv0.851.632.475 (2)174.8
Symmetry codes: (i) y, xy, z; (ii) x+y+1, x+1, z; (iii) x+1, y+1, z+1; (iv) x+1, y, z.
 

References

First citationRigaku/MSC (2005). CrystalClear and CrystalStructure. Rigaku/MSC, The Woodlands, Texas, USA.  Google Scholar
First citationSheldrick, G. M. (2008). Acta Cryst. A64, 112–122.  Web of Science CrossRef CAS IUCr Journals Google Scholar

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.

Journal logoCRYSTALLOGRAPHIC
COMMUNICATIONS
ISSN: 2056-9890
Follow Acta Cryst. E
Sign up for e-alerts
Follow Acta Cryst. on Twitter
Follow us on facebook
Sign up for RSS feeds