supplementary materials


fj2138 scheme

Acta Cryst. (2008). E64, o1763    [ doi:10.1107/S1600536808025300 ]

4,4'-(Propane-1,3-diyl)dipiperidinium sulfate monohydrate

E. Yang, X.-C. Song and R.-Q. Zhuang

Abstract top

In the title compound, C13H28N22+·SO42-·H2O, extensive hydrogen-bonding interactions between the protonated 4,4'-(propane-1,3-diyl)dipiperidinium ions, the sulfate anions and the water molecules lead to a three-dimensional pillared and layered structure with the 4,4'-(propane-1,3-diyl)dipiperidinium ions acting as the pillars.

Comment top

The asymmetric unit of the title compound, (I), consists of one protonated 4,4'-(propane-1,3-diyl)dipiperidinium ion, one deprotonated sulfate anion and one water molecule (Figure 1). Both protonated N ends of the 4,4'-(propane-1,3-diyl)dipiperidinium ion form N—H···O hydrogen bonds with the sulfate anion, as well as the water molecules form O—H···O hydrogen bonds with the sulfate anion, which leads to the formation of two-dimensional hydrogen-bonding layer parallel to the ac plane (Table 1 & Figure 2). The resulting layers are further pillared by the 4,4'-(propane-1,3-diyl)dipiperidinium ions to complete the three-dimensional structure.

Related literature top

Please supply any relevant related literature.

Experimental top

A solution of 4,4-trimethylenedipiperidine (1 mmol), sulfuric acid (1 mmol) and H2O (10 ml) was slowly evaporated at room temperature, giving colorless single crystals suitable for X-ray analysis.

Refinement top

The H atoms bonded to C and O atoms were placed at calculated positions, and refined with isotropic displacement parameters, using a riding model [C—H 0.93Å and Uiso(H) = 1.2Ueq(C); O—H 0.85Å and Uiso(H) = 1.5Ueq(C)]. The H atoms bonded to N atoms were refined freely.

Computing details top

Data collection: SMART (Siemens, 1996); cell refinement: SAINT (Siemens, 1996); data reduction: SAINT (Siemens, 1996); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: DIAMOND (Bergerhoff et al., 1999); software used to prepare material for publication: SHELXTL (Sheldrick, 2008).

Figures top
[Figure 1] Fig. 1. A view of the title compound, showing 30% probability displacement ellipsoids.
[Figure 2] Fig. 2. The three-dimensional structure of the title compound, showing the hydrogen bonding interactions (dashed lines).
4,4'-(Propane-1,3-diyl)dipiperidinium sulfate monohydrate top
Crystal data top
C13H28N22+·S1O42–·H2OF000 = 712
Mr = 326.45Dx = 1.315 Mg m3
Monoclinic, P21/nMo Kα radiation
λ = 0.71073 Å
Hall symbol: -P 2ynCell parameters from 99 reflections
a = 6.2019 (2) Åθ = 2.0–25.1º
b = 22.5110 (5) ŵ = 0.22 mm1
c = 12.0052 (3) ÅT = 293 (2) K
β = 100.439 (2)ºPrism, colorless
V = 1648.32 (8) Å30.22 × 0.14 × 0.09 mm
Z = 4
Data collection top
Siemens SMART 1K CCD area-detector
diffractometer
2932 independent reflections
Radiation source: fine-focus sealed tube2011 reflections with I > 2σ(I)
Monochromator: graphiteRint = 0.066
T = 293(2) Kθmax = 25.1º
φ and ω scansθmin = 2.0º
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
h = 7→7
Tmin = 0.927, Tmax = 0.98k = 26→26
13022 measured reflectionsl = 13→14
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.048H atoms treated by a mixture of
independent and constrained refinement
wR(F2) = 0.131  w = 1/[σ2(Fo2) + (0.0635P)2 + 0.5599P]
where P = (Fo2 + 2Fc2)/3
S = 1.03(Δ/σ)max < 0.001
2932 reflectionsΔρmax = 0.34 e Å3
202 parametersΔρmin = 0.39 e Å3
Primary atom site location: structure-invariant direct methodsExtinction correction: none
Crystal data top
C13H28N22+·S1O42–·H2OV = 1648.32 (8) Å3
Mr = 326.45Z = 4
Monoclinic, P21/nMo Kα
a = 6.2019 (2) ŵ = 0.22 mm1
b = 22.5110 (5) ÅT = 293 (2) K
c = 12.0052 (3) Å0.22 × 0.14 × 0.09 mm
β = 100.439 (2)º
Data collection top
Siemens SMART 1K CCD area-detector
diffractometer
2932 independent reflections
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
2011 reflections with I > 2σ(I)
Tmin = 0.927, Tmax = 0.98Rint = 0.066
13022 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.048202 parameters
wR(F2) = 0.131H atoms treated by a mixture of
independent and constrained refinement
S = 1.03Δρmax = 0.34 e Å3
2932 reflectionsΔρmin = 0.39 e Å3
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*/Ueq
S10.28582 (11)0.18642 (3)0.35885 (6)0.0255 (2)
O1W0.7186 (3)0.20465 (10)0.15532 (19)0.0458 (6)
H1WA0.60740.22740.14210.069*
H1WB0.81810.22790.14100.069*
O10.2335 (3)0.19986 (9)0.23718 (16)0.0346 (5)
O20.2510 (4)0.12374 (10)0.38116 (19)0.0489 (6)
O30.5164 (3)0.20349 (10)0.40084 (18)0.0431 (6)
O40.1467 (3)0.22203 (10)0.42124 (19)0.0493 (7)
N10.1395 (4)0.13893 (12)0.4911 (2)0.0310 (6)
H1NA0.026 (5)0.1498 (14)0.529 (3)0.046*
H1NB0.258 (6)0.1500 (14)0.533 (3)0.046*
N20.8705 (4)0.19250 (11)0.0746 (2)0.0279 (6)
H2NA0.986 (5)0.1962 (14)0.128 (3)0.042*
H2NB0.851 (5)0.2258 (14)0.029 (3)0.042*
C10.1335 (5)0.07379 (13)0.4752 (3)0.0328 (7)
H1A0.14820.05450.54840.039*
H1B0.00680.06240.43060.039*
C20.3159 (5)0.05304 (13)0.4160 (2)0.0279 (7)
H2A0.45550.05890.46610.033*
H2B0.29870.01080.40070.033*
C30.3192 (4)0.08591 (12)0.3044 (2)0.0249 (6)
H3A0.18590.07560.25070.030*
C40.3183 (5)0.15306 (12)0.3261 (2)0.0300 (7)
H4A0.30800.17390.25460.036*
H4B0.45540.16430.37390.036*
C50.1292 (5)0.17174 (14)0.3825 (2)0.0351 (8)
H5A0.00870.16340.33260.042*
H5B0.13690.21410.39720.042*
C60.5170 (5)0.06873 (12)0.2525 (2)0.0297 (7)
H6A0.52590.09570.19050.036*
H6B0.64830.07430.30920.036*
C70.5158 (4)0.00503 (12)0.2080 (3)0.0296 (7)
H7A0.39180.00010.14660.036*
H7B0.49640.02220.26810.036*
C80.7255 (5)0.01124 (13)0.1655 (3)0.0315 (7)
H8A0.84650.01120.22930.038*
H8B0.75490.01910.11290.038*
C90.6696 (5)0.18163 (13)0.1245 (3)0.0298 (7)
H9A0.54130.18200.06470.036*
H9B0.65360.21320.17740.036*
C100.6836 (4)0.12266 (12)0.1851 (2)0.0269 (7)
H10A0.54940.11600.21410.032*
H10B0.80420.12360.24910.032*
C110.7181 (4)0.07147 (12)0.1069 (2)0.0264 (7)
H11A0.59430.07120.04330.032*
C120.9259 (5)0.08438 (13)0.0598 (3)0.0332 (7)
H12A1.05080.08440.12150.040*
H12B0.94790.05300.00760.040*
C130.9149 (5)0.14331 (13)0.0008 (3)0.0346 (8)
H13A1.05280.15060.02580.042*
H13B0.79970.14200.06730.042*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
S10.0231 (4)0.0290 (4)0.0237 (4)0.0011 (3)0.0024 (3)0.0009 (3)
O1W0.0439 (13)0.0327 (13)0.0623 (16)0.0011 (10)0.0131 (12)0.0080 (11)
O10.0342 (11)0.0457 (14)0.0209 (12)0.0003 (9)0.0027 (9)0.0051 (9)
O20.0630 (16)0.0310 (14)0.0508 (16)0.0044 (11)0.0049 (12)0.0120 (11)
O30.0239 (11)0.0606 (15)0.0401 (14)0.0115 (10)0.0070 (10)0.0122 (11)
O40.0416 (13)0.0637 (17)0.0469 (15)0.0067 (12)0.0196 (11)0.0167 (12)
N10.0267 (13)0.0376 (16)0.0275 (16)0.0033 (11)0.0019 (12)0.0095 (12)
N20.0327 (14)0.0249 (15)0.0230 (14)0.0041 (11)0.0036 (11)0.0046 (11)
C10.0350 (16)0.0349 (19)0.0274 (17)0.0063 (14)0.0028 (13)0.0008 (14)
C20.0298 (15)0.0218 (16)0.0298 (17)0.0013 (12)0.0008 (13)0.0008 (13)
C30.0267 (14)0.0203 (15)0.0258 (16)0.0005 (12)0.0008 (12)0.0047 (12)
C40.0401 (17)0.0219 (17)0.0266 (17)0.0035 (13)0.0022 (14)0.0004 (13)
C50.0396 (18)0.0320 (18)0.0291 (18)0.0142 (14)0.0058 (14)0.0019 (14)
C60.0318 (16)0.0244 (17)0.0326 (18)0.0010 (12)0.0047 (13)0.0020 (13)
C70.0324 (15)0.0227 (16)0.0357 (18)0.0010 (12)0.0110 (13)0.0020 (13)
C80.0347 (16)0.0229 (17)0.0379 (19)0.0002 (13)0.0094 (14)0.0012 (13)
C90.0325 (16)0.0251 (17)0.0317 (18)0.0027 (12)0.0051 (13)0.0021 (13)
C100.0300 (15)0.0235 (17)0.0286 (17)0.0016 (12)0.0093 (13)0.0005 (13)
C110.0272 (15)0.0248 (17)0.0275 (17)0.0003 (12)0.0058 (13)0.0011 (12)
C120.0407 (17)0.0243 (17)0.0398 (19)0.0020 (13)0.0206 (15)0.0047 (14)
C130.0391 (17)0.0342 (19)0.0324 (19)0.0038 (14)0.0114 (15)0.0033 (14)
Geometric parameters (Å, °) top
S1—O21.459 (2)C4—H4B0.9700
S1—O11.469 (2)C5—H5A0.9700
S1—O41.477 (2)C5—H5B0.9700
S1—O31.478 (2)C6—C71.530 (4)
O1W—H1WA0.8501C6—H6A0.9700
O1W—H1WB0.8500C6—H6B0.9700
N1—C11.478 (4)C7—C81.525 (4)
N1—C51.489 (4)C7—H7A0.9700
N1—H1NA0.94 (3)C7—H7B0.9700
N1—H1NB0.85 (3)C8—C111.524 (4)
N2—C131.488 (4)C8—H8A0.9700
N2—C91.497 (4)C8—H8B0.9700
N2—H2NA0.88 (3)C9—C101.509 (4)
N2—H2NB0.92 (3)C9—H9A0.9700
C1—C21.515 (4)C9—H9B0.9700
C1—H1A0.9700C10—C111.526 (4)
C1—H1B0.9700C10—H10A0.9700
C2—C31.534 (4)C10—H10B0.9700
C2—H2A0.9700C11—C121.527 (4)
C2—H2B0.9700C11—H11A0.9800
C3—C61.523 (4)C12—C131.509 (4)
C3—C41.534 (4)C12—H12A0.9700
C3—H3A0.9800C12—H12B0.9700
C4—C51.516 (4)C13—H13A0.9700
C4—H4A0.9700C13—H13B0.9700
O2—S1—O1111.60 (13)C3—C6—C7115.3 (2)
O2—S1—O4108.18 (14)C3—C6—H6A108.4
O1—S1—O4110.38 (13)C7—C6—H6A108.4
O2—S1—O3110.79 (13)C3—C6—H6B108.4
O1—S1—O3108.13 (12)C7—C6—H6B108.4
O4—S1—O3107.69 (14)H6A—C6—H6B107.5
H1WA—O1W—H1WB100.7C8—C7—C6113.0 (2)
C1—N1—C5112.5 (2)C8—C7—H7A109.0
C1—N1—H1NA108.6 (19)C6—C7—H7A109.0
C5—N1—H1NA112.1 (19)C8—C7—H7B109.0
C1—N1—H1NB111 (2)C6—C7—H7B109.0
C5—N1—H1NB106 (2)H7A—C7—H7B107.8
H1NA—N1—H1NB107 (3)C11—C8—C7114.3 (2)
C13—N2—C9112.4 (2)C11—C8—H8A108.7
C13—N2—H2NA108 (2)C7—C8—H8A108.7
C9—N2—H2NA110 (2)C11—C8—H8B108.7
C13—N2—H2NB105.2 (19)C7—C8—H8B108.7
C9—N2—H2NB109.9 (19)H8A—C8—H8B107.6
H2NA—N2—H2NB111 (3)N2—C9—C10110.9 (2)
N1—C1—C2111.3 (2)N2—C9—H9A109.4
N1—C1—H1A109.4C10—C9—H9A109.4
C2—C1—H1A109.4N2—C9—H9B109.4
N1—C1—H1B109.4C10—C9—H9B109.4
C2—C1—H1B109.4H9A—C9—H9B108.0
H1A—C1—H1B108.0C9—C10—C11111.7 (2)
C1—C2—C3113.0 (2)C9—C10—H10A109.3
C1—C2—H2A109.0C11—C10—H10A109.3
C3—C2—H2A109.0C9—C10—H10B109.3
C1—C2—H2B109.0C11—C10—H10B109.3
C3—C2—H2B109.0H10A—C10—H10B107.9
H2A—C2—H2B107.8C8—C11—C10112.6 (2)
C6—C3—C2112.0 (2)C8—C11—C12112.5 (2)
C6—C3—C4110.4 (2)C10—C11—C12107.8 (2)
C2—C3—C4109.0 (2)C8—C11—H11A107.9
C6—C3—H3A108.5C10—C11—H11A107.9
C2—C3—H3A108.5C12—C11—H11A107.9
C4—C3—H3A108.5C13—C12—C11112.3 (2)
C5—C4—C3112.1 (2)C13—C12—H12A109.2
C5—C4—H4A109.2C11—C12—H12A109.2
C3—C4—H4A109.2C13—C12—H12B109.2
C5—C4—H4B109.2C11—C12—H12B109.2
C3—C4—H4B109.2H12A—C12—H12B107.9
H4A—C4—H4B107.9N2—C13—C12111.0 (2)
N1—C5—C4109.9 (2)N2—C13—H13A109.4
N1—C5—H5A109.7C12—C13—H13A109.4
C4—C5—H5A109.7N2—C13—H13B109.4
N1—C5—H5B109.7C12—C13—H13B109.4
C4—C5—H5B109.7H13A—C13—H13B108.0
H5A—C5—H5B108.2
Hydrogen-bond geometry (Å, °) top
D—H···AD—HH···AD···AD—H···A
O1W—H1WA···O4i0.851.982.819 (3)168
O1W—H1WB···O3ii0.851.972.799 (3)165
N1—H1NA···O4iii0.94 (3)2.09 (3)2.904 (3)144 (3)
N1—H1NB···O3iv0.85 (3)1.91 (3)2.711 (3)157 (3)
N2—H2NA···O1v0.88 (3)1.83 (3)2.704 (3)177 (3)
N2—H2NB···O4vi0.92 (3)2.02 (3)2.845 (4)149 (3)
Symmetry codes: (i) −x+1/2, y−1/2, −z+1/2; (ii) −x+3/2, y−1/2, −z+1/2; (iii) −x, −y, −z+1; (iv) −x+1, −y, −z+1; (v) x+1, y, z; (vi) x+1/2, −y+1/2, z−1/2.
Table 1
Hydrogen-bond geometry (Å, °)
top
D—H···AD—HH···AD···AD—H···A
O1W—H1WA···O4i0.851.982.819 (3)168
O1W—H1WB···O3ii0.851.972.799 (3)165
N1—H1NA···O4iii0.94 (3)2.09 (3)2.904 (3)144 (3)
N1—H1NB···O3iv0.85 (3)1.91 (3)2.711 (3)157 (3)
N2—H2NA···O1v0.88 (3)1.83 (3)2.704 (3)177 (3)
N2—H2NB···O4vi0.92 (3)2.02 (3)2.845 (4)149 (3)
Symmetry codes: (i) −x+1/2, y−1/2, −z+1/2; (ii) −x+3/2, y−1/2, −z+1/2; (iii) −x, −y, −z+1; (iv) −x+1, −y, −z+1; (v) x+1, y, z; (vi) x+1/2, −y+1/2, z−1/2.
Acknowledgements top

The authors acknowledge the financial support from Natural Science Foundation of Fujian Province (2006 F3042).

references
References top

Bergerhoff, G., Berndt, M. & Brandenburg, K. (1999). DIAMOND. Crystal Impact GbR, Bonn, Germany.

Sheldrick, G. M. (1996). SADABS. University of Göttingen, Germany.

Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122.

Siemens (1996). SMART and SAINT. Siemens Analytical X-ray Instruments Inc., Madison, Wisconsin, USA.