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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2009 Sep 16;65(Pt 10):m1219. doi: 10.1107/S1600536809036587

4-(2-Methyl­piperidin-1-ylcarbon­yl)pyridinium hexachloridoantimonate(V)

Bo Wang a,*
PMCID: PMC2970264  PMID: 21577742

Abstract

In the hexa­chlorido­animonate anion of the title compound, (C12H17N2O)[SbCl6], the Sb5+ion is in a slightly distorted octa­hedral coordination. In the 4-(2-methyl­piperidine-1-carbon­yl) pyridinium cation, the dihedral angle between the mean planes of the pyridine and piperzine rings is 66.3 (3)°. The mean plane of the carbonyl group is twisted by 80.5 (7)° and 42.7 (4)° relative to the mean planes of the pyridine and piperzine rings, respectively. The methyl group is in an R configuration relative to the piperidine ring which is in a slightly distorted chair conformation. The crystal packing is stabilized by N—H⋯O hydrogen bonds between cations, which form infinite zigzag chains parallel to [010].

Related literature

For the use of halogenidoanti­monate salts in the study of phase transitions in dielectric–ferroelectric materials, see: Jakubas et al. (2005); Bednarska-Bolek et al. (2000). For related structures, see: Chen (2009); Clemente & Marzotto (2003); Kulicka et al. (2006). For puckering parameters, see: Cremer & Pople (1975).graphic file with name e-65-m1219-scheme1.jpg

Experimental

Crystal data

  • (C12H17N2O)[SbCl6]

  • M r = 539.73

  • Monoclinic, Inline graphic

  • a = 8.1067 (16) Å

  • b = 12.700 (3) Å

  • c = 19.677 (4) Å

  • β = 99.06 (3)°

  • V = 2000.6 (7) Å3

  • Z = 4

  • Mo Kα radiation

  • μ = 2.18 mm−1

  • T = 298 K

  • 0.20 × 0.20 × 0.20 mm

Data collection

  • Rigaku SCXmini diffractometer

  • Absorption correction: multi-scan (CrystalClear; Rigaku, 2005) T min = 0.638, T max = 0.646

  • 17300 measured reflections

  • 3918 independent reflections

  • 2731 reflections with I > 2σ(I)

  • R int = 0.065

Refinement

  • R[F 2 > 2σ(F 2)] = 0.072

  • wR(F 2) = 0.178

  • S = 1.06

  • 3918 reflections

  • 199 parameters

  • 8 restraints

  • H-atom parameters constrained

  • Δρmax = 1.08 e Å−3

  • Δρmin = −0.82 e Å−3

Data collection: CrystalClear (Rigaku 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: PRPKAPPA (Ferguson, 1999).

Supplementary Material

Crystal structure: contains datablocks I, New_Global_Publ_Block. DOI: 10.1107/S1600536809036587/jj2004sup1.cif

e-65-m1219-sup1.cif (18.3KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536809036587/jj2004Isup2.hkl

e-65-m1219-Isup2.hkl (192.1KB, 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
N1—H1B⋯O1i 0.86 1.87 2.689 (9) 159

Symmetry code: (i) Inline graphic.

Acknowledgments

The authors are grateful to the starter fund of Southeast University for financial support to buy the X-ray diffractometer.

supplementary crystallographic information

Comment

Halogenidoantimonate salts are used to study phase transitions in dielectric-ferroelectric materials (Jakubas et al., 2005; Bednarska-Bolek et al., 2000). In support of this work, crystal structures of pyridinium hexachloridoantimonate, (Clemente & Marzotto, 2003),4-aminopyridinium hexachloridoantimonate (Kulicka et al., 2006) and diisonicotinium pentachloridoantimonate monohydrate (Chen, 2009) have beenreported. In continuation of our studies on halogenoantimonate salts, we report the crystal structure of the title compound, C12H17N2O+. SbCl6-, (I).

In the cation (4-(2-methylpiperidine-1-carbonyl) pyridinium), the pyridine N atom is protonated. The piperidine ring (N2/C7—C11) adopts a slightly distorted chair conformation (Cremer & Pople, 1975) with puckering parameters Q, θ and φ of 0.564 (4) Å, 177.0 (6)° and 177.084 (5)°, respectively (Fig. 1). For an ideal chair θ has a value of 0 or 180°. The mean plane of the carbonyl group is twisted relative to the mean planes of the pyridine and piperzine rngs by 80.5 (7)° and 42.7 (4)°, respectively. The dihedral angle between the mean planes of pyridine and piperzine rings is 66.3 (3)°. In the anion the Sb atom is hexacoordinated with Cl atoms in a slightly distorted octahedral conformation. The Sb—Cl bond lengths (2.330 (3) to 2.348 (3) Å) are similar to that observed in pyridinium hexachlorido-antimony(V) (2.32 (1)–2.35 (5) Å; Clemente & Marzotto, 2003) and slightly shorter than that reported for 4-aminopyridinium hexachloridoantimonate (2.3608 (8)–2.3912 (7) Å; Kulicka et al.,2006). Crystal packing is stabilized by N1–H1B···O1 hydrogen bonds between cations which form infinite zigzag chains parallel to [010] (Fig. 2).

Experimental

A mixture of 4-(2-methylpiperidine-1-carbonyl)pyridine(1 mmol), SbCl5 (1 mmol), ethanol(8 ml) and a few drops of HCl (6 mol/L) was stirred in a beaker. There were many solid powders produced and the solution was filtered. Colorless single crystals of the title compound suitable for X-ray analysis were obtained on slow evaporation of the solvents over a period of 48 h.

Refinement

Positional parameters of all the H atoms were calculated geometrically and were allowed to ride on the C atoms to which they are bonded, with Uiso(H) = 1.2Ueq(C).

Figures

Fig. 1.

Fig. 1.

The molecular structure of the title compound, with the atomic numbering scheme. Displacement ellipsoids are drawn at the 30% probability level, and all H atoms have been omitted for clarity.

Fig. 2.

Fig. 2.

A view of the crystal packing of the title compound, Dashed lines indicate N–H···O hydrogen bonds which form infinite, one-dimensional chains along the (011) plane of the unit cell.

Crystal data

(C12H17N2O)[SbCl6] F(000) = 1056
Mr = 539.73 Dx = 1.792 Mg m3
Monoclinic, P21/n Mo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2yn Cell parameters from 7472 reflections
a = 8.1067 (16) Å θ = 3.0–27.7°
b = 12.700 (3) Å µ = 2.18 mm1
c = 19.677 (4) Å T = 298 K
β = 99.06 (3)° Prism, colourless
V = 2000.6 (7) Å3 0.20 × 0.20 × 0.20 mm
Z = 4

Data collection

Rigaku SCXmini diffractometer 3918 independent reflections
Radiation source: fine-focus sealed tube 2731 reflections with I > 2σ(I)
graphite Rint = 0.065
Detector resolution: 13.6612 pixels mm-1 θmax = 26.0°, θmin = 3.0°
ω scans h = −9→9
Absorption correction: multi-scan (CrystalClear; Rigaku, 2005) k = −15→15
Tmin = 0.638, Tmax = 0.646 l = −24→24
17300 measured reflections

Refinement

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)] = 0.072 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.178 H-atom parameters constrained
S = 1.06 w = 1/[σ2(Fo2) + (0.0594P)2 + 10.7201P] where P = (Fo2 + 2Fc2)/3
3918 reflections (Δ/σ)max < 0.001
199 parameters Δρmax = 1.08 e Å3
8 restraints Δρmin = −0.82 e Å3

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
C1 0.5950 (13) 0.2859 (8) 0.2451 (5) 0.092 (3)
H1A 0.5293 0.2434 0.2685 0.110*
C2 0.6745 (15) 0.3710 (9) 0.2774 (6) 0.107 (4)
H2A 0.6625 0.3868 0.3226 0.129*
C3 0.7859 (12) 0.4104 (8) 0.1821 (6) 0.089 (3)
H3A 0.8534 0.4541 0.1604 0.107*
C4 0.7082 (13) 0.3263 (7) 0.1474 (5) 0.076 (3)
H4A 0.7221 0.3128 0.1022 0.091*
C5 0.6107 (9) 0.2626 (6) 0.1797 (4) 0.0474 (18)
C6 0.5366 (10) 0.1615 (6) 0.1476 (4) 0.055 (2)
C7 0.2968 (10) 0.2610 (6) 0.0863 (6) 0.067 (3)
H7A 0.3572 0.3219 0.1069 0.080*
H7B 0.2776 0.2704 0.0368 0.080*
C8 0.1374 (15) 0.2526 (9) 0.1110 (6) 0.094 (3)
H8A 0.0691 0.3133 0.0955 0.113*
H8B 0.1566 0.2531 0.1610 0.113*
C9 0.0415 (15) 0.1501 (9) 0.0851 (7) 0.102 (4)
H9A −0.0581 0.1434 0.1064 0.123*
H9B 0.0074 0.1538 0.0356 0.123*
C10 0.1563 (13) 0.0526 (8) 0.1035 (5) 0.084 (3)
H10A 0.1810 0.0446 0.1530 0.100*
H10B 0.0998 −0.0105 0.0843 0.100*
C11 0.3164 (11) 0.0675 (7) 0.0745 (5) 0.068 (3)
H11A 0.3906 0.0087 0.0906 0.081*
C12 0.2905 (13) 0.0667 (7) −0.0031 (5) 0.079 (3)
H12A 0.3957 0.0775 −0.0187 0.119*
H12B 0.2148 0.1221 −0.0204 0.119*
H12C 0.2446 0.0001 −0.0196 0.119*
Cl1 0.3262 (6) 0.7906 (3) 0.19673 (17) 0.1303 (14)
Cl2 0.3231 (4) 0.7842 (2) 0.03045 (15) 0.0970 (9)
Cl3 0.0105 (4) 0.6753 (4) 0.0955 (2) 0.1479 (18)
Cl4 0.2771 (8) 0.5277 (3) 0.19805 (19) 0.192 (3)
Cl5 0.5929 (5) 0.6406 (5) 0.1308 (3) 0.199 (3)
Cl6 0.2773 (6) 0.5279 (2) 0.02829 (18) 0.1324 (15)
N1 0.7664 (10) 0.4296 (6) 0.2450 (5) 0.075 (2)
H1B 0.8162 0.4831 0.2658 0.091*
N2 0.3972 (9) 0.1656 (5) 0.1039 (4) 0.0623 (19)
O1 0.6169 (8) 0.0811 (5) 0.1647 (4) 0.082 (2)
Sb1 0.30206 (7) 0.65548 (4) 0.11435 (3) 0.0571 (2)

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
C1 0.122 (9) 0.096 (8) 0.059 (6) −0.040 (7) 0.024 (6) −0.011 (6)
C2 0.165 (13) 0.102 (9) 0.048 (6) −0.028 (9) −0.004 (7) −0.014 (6)
C3 0.089 (8) 0.075 (7) 0.110 (9) −0.023 (6) 0.036 (7) −0.017 (6)
C4 0.105 (8) 0.055 (6) 0.074 (6) −0.022 (5) 0.035 (6) −0.021 (5)
C5 0.047 (4) 0.050 (4) 0.040 (4) −0.001 (3) −0.008 (3) 0.004 (3)
C6 0.056 (5) 0.044 (4) 0.059 (5) 0.005 (4) −0.010 (4) 0.005 (4)
C7 0.048 (5) 0.036 (4) 0.110 (7) 0.007 (4) −0.008 (5) 0.001 (4)
C8 0.095 (9) 0.093 (8) 0.091 (8) 0.013 (7) 0.003 (6) −0.014 (6)
C9 0.083 (8) 0.107 (10) 0.121 (10) 0.009 (7) 0.030 (7) 0.004 (8)
C10 0.094 (8) 0.078 (7) 0.076 (7) −0.011 (6) 0.003 (6) −0.005 (5)
C11 0.068 (6) 0.046 (5) 0.080 (6) −0.011 (4) −0.015 (5) −0.006 (4)
C12 0.082 (7) 0.059 (6) 0.093 (8) −0.001 (5) 0.004 (6) −0.015 (5)
Cl1 0.184 (4) 0.121 (3) 0.083 (2) −0.041 (3) 0.011 (2) −0.042 (2)
Cl2 0.147 (3) 0.0595 (15) 0.0860 (19) −0.0035 (16) 0.0231 (18) 0.0139 (13)
Cl3 0.0633 (18) 0.239 (5) 0.145 (3) −0.026 (2) 0.0295 (19) −0.056 (3)
Cl4 0.368 (8) 0.126 (3) 0.080 (2) −0.056 (4) 0.026 (3) 0.043 (2)
Cl5 0.076 (2) 0.262 (6) 0.243 (6) 0.065 (3) −0.019 (3) 0.038 (5)
Cl6 0.251 (5) 0.0584 (17) 0.102 (2) −0.001 (2) 0.069 (3) −0.0125 (16)
N1 0.069 (5) 0.056 (5) 0.091 (6) −0.011 (4) −0.020 (5) −0.017 (4)
N2 0.056 (4) 0.035 (3) 0.087 (5) 0.000 (3) −0.018 (4) −0.002 (3)
O1 0.086 (5) 0.050 (4) 0.095 (5) 0.009 (3) −0.032 (4) 0.012 (3)
Sb1 0.0608 (4) 0.0543 (4) 0.0552 (4) −0.0006 (3) 0.0061 (2) 0.0038 (3)

Geometric parameters (Å, °)

C1—C5 1.347 (12) C9—C10 1.557 (15)
C1—C2 1.364 (15) C9—H9A 0.9700
C1—H1A 0.9300 C9—H9B 0.9700
C2—N1 1.291 (15) C10—C11 1.509 (14)
C2—H2A 0.9300 C10—H10A 0.9700
C3—N1 1.295 (13) C10—H10B 0.9700
C3—C4 1.367 (13) C11—N2 1.481 (10)
C3—H3A 0.9300 C11—C12 1.508 (13)
C4—C5 1.355 (11) C11—H11A 0.9800
C4—H4A 0.9300 C12—H12A 0.9600
C5—C6 1.514 (10) C12—H12B 0.9600
C6—O1 1.229 (9) C12—H12C 0.9600
C6—N2 1.309 (10) Cl1—Sb1 2.347 (3)
C7—C8 1.455 (14) Cl2—Sb1 2.348 (3)
C7—N2 1.470 (9) Cl3—Sb1 2.348 (3)
C7—H7A 0.9700 Cl4—Sb1 2.343 (3)
C7—H7B 0.9700 Cl5—Sb1 2.336 (4)
C8—C9 1.560 (15) Cl6—Sb1 2.330 (3)
C8—H8A 0.9700 N1—H1B 0.8600
C8—H8B 0.9700
C5—C1—C2 120.7 (10) C9—C10—H10A 109.8
C5—C1—H1A 119.6 C11—C10—H10B 109.8
C2—C1—H1A 119.6 C9—C10—H10B 109.8
N1—C2—C1 119.6 (10) H10A—C10—H10B 108.3
N1—C2—H2A 120.2 N2—C11—C12 112.6 (8)
C1—C2—H2A 120.2 N2—C11—C10 108.1 (8)
N1—C3—C4 120.6 (10) C12—C11—C10 113.0 (8)
N1—C3—H3A 119.7 N2—C11—H11A 107.6
C4—C3—H3A 119.7 C12—C11—H11A 107.6
C5—C4—C3 119.3 (9) C10—C11—H11A 107.6
C5—C4—H4A 120.4 C11—C12—H12A 109.5
C3—C4—H4A 120.4 C11—C12—H12B 109.5
C1—C5—C4 117.8 (8) H12A—C12—H12B 109.5
C1—C5—C6 119.6 (8) C11—C12—H12C 109.5
C4—C5—C6 122.2 (7) H12A—C12—H12C 109.5
O1—C6—N2 125.3 (7) H12B—C12—H12C 109.5
O1—C6—C5 115.6 (7) C2—N1—C3 122.1 (9)
N2—C6—C5 119.0 (6) C2—N1—H1B 119.0
C8—C7—N2 110.4 (8) C3—N1—H1B 119.0
C8—C7—H7A 109.6 C6—N2—C7 125.2 (7)
N2—C7—H7A 109.6 C6—N2—C11 120.4 (6)
C8—C7—H7B 109.6 C7—N2—C11 114.0 (6)
N2—C7—H7B 109.6 Cl6—Sb1—Cl5 90.8 (2)
H7A—C7—H7B 108.1 Cl6—Sb1—Cl4 91.26 (14)
C7—C8—C9 112.0 (9) Cl5—Sb1—Cl4 92.5 (2)
C7—C8—H8A 109.2 Cl6—Sb1—Cl1 177.11 (13)
C9—C8—H8A 109.2 Cl5—Sb1—Cl1 89.5 (2)
C7—C8—H8B 109.2 Cl4—Sb1—Cl1 91.60 (16)
C9—C8—H8B 109.2 Cl6—Sb1—Cl3 89.46 (16)
H8A—C8—H8B 107.9 Cl5—Sb1—Cl3 178.1 (2)
C10—C9—C8 109.8 (10) Cl4—Sb1—Cl3 89.4 (2)
C10—C9—H9A 109.7 Cl1—Sb1—Cl3 90.17 (15)
C8—C9—H9A 109.7 Cl6—Sb1—Cl2 88.89 (11)
C10—C9—H9B 109.7 Cl5—Sb1—Cl2 88.32 (18)
C8—C9—H9B 109.7 Cl4—Sb1—Cl2 179.19 (19)
H9A—C9—H9B 108.2 Cl1—Sb1—Cl2 88.24 (13)
C11—C10—C9 109.3 (9) Cl3—Sb1—Cl2 89.84 (16)
C11—C10—H10A 109.8
C5—C1—C2—N1 −0.4 (11) C9—C10—C11—C12 −66.8 (11)
N1—C3—C4—C5 −0.3 (14) C1—C2—N1—C3 0.1 (13)
C2—C1—C5—C4 0.3 (13) C4—C3—N1—C2 0.2 (15)
C2—C1—C5—C6 173.5 (7) O1—C6—N2—C7 176.7 (9)
C3—C4—C5—C1 0.1 (14) C5—C6—N2—C7 −4.7 (14)
C3—C4—C5—C6 −173.0 (8) O1—C6—N2—C11 4.7 (15)
C1—C5—C6—O1 −77.7 (11) C5—C6—N2—C11 −176.7 (8)
C4—C5—C6—O1 95.2 (11) C8—C7—N2—C6 −112.8 (10)
C1—C5—C6—N2 103.5 (10) C8—C7—N2—C11 59.6 (11)
C4—C5—C6—N2 −83.6 (12) C12—C11—N2—C6 −123.4 (10)
N2—C7—C8—C9 −53.9 (12) C10—C11—N2—C6 111.1 (10)
C7—C8—C9—C10 53.4 (13) C12—C11—N2—C7 63.8 (11)
C8—C9—C10—C11 −55.2 (12) C10—C11—N2—C7 −61.8 (11)
C9—C10—C11—N2 58.5 (10)

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
N1—H1B···O1i 0.86 1.87 2.689 (9) 159

Symmetry codes: (i) −x+3/2, y+1/2, −z+1/2.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: JJ2004).

References

  1. Bednarska-Bolek, B., Pietraszko, A., Jakubas, R., Bator, G. & Kosturek, B. (2000). J. Phys. Condens. Mat.12, 1143–1159.
  2. Chen, L. Z. (2009). Acta Cryst. E65, m689. [DOI] [PMC free article] [PubMed]
  3. Clemente, D. A. & Marzotto, A. (2003). Acta Cryst. B59, 43–50. [DOI] [PubMed]
  4. Cremer, D. & Pople, J. A. (1975). J. Am. Chem. Soc.97, 1354–1358.
  5. Ferguson, G. (1999). PRPKAPPA University of Guelph, Canada.
  6. Jakubas, R., Bednarska-Bolek, B., Zaleski, J., Medycki, W., Hołderna-Natkaniec, K., Zieliński, P. & Gała˛zka, M. (2005). Solid State Sci.7, 381–390.
  7. Kulicka, B., Jakubas, R., Pietraszko, A., Medycki, W. & Świergiel, J. (2006). J. Mol. Struct.783, 88–95.
  8. Rigaku (2005). CrystalClear Rigaku Corporation, Tokyo, Japan.
  9. 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, New_Global_Publ_Block. DOI: 10.1107/S1600536809036587/jj2004sup1.cif

e-65-m1219-sup1.cif (18.3KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536809036587/jj2004Isup2.hkl

e-65-m1219-Isup2.hkl (192.1KB, hkl)

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


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