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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2011 Apr 7;67(Pt 5):o1051. doi: 10.1107/S1600536811011226

Penta­decyl­ammonium methyl sulfate

Lijun Zhang a, Youying Di a,*, Wenyan Dan a
PMCID: PMC3089230  PMID: 21754378

Abstract

In the crystal of the title compound, C15H34N+·CH3SO4 −, the cations and anions are joined together via strong N—H⋯O hydrogen bonds into layers parallel to (001).

Related literature

Long-chain n-alkyl­ammonium halides are widely used as surfacta­nts (Aratono et al., 1998 ▶; Tornblom et al., 2000 ▶) and as models for biological membranes (Ringsdorf et al., 1988 ▶). For solid-solid phase transitions in n-alkyl­ammonium chlorides, see: Terreros et al. (2000 ▶).graphic file with name e-67-o1051-scheme1.jpg

Experimental

Crystal data

  • C15H34N+·CH3O4S−

  • M r = 339.53

  • Monoclinic, Inline graphic

  • a = 5.4260 (5) Å

  • b = 7.4981 (6) Å

  • c = 24.376 (2) Å

  • β = 93.557 (1)°

  • V = 989.83 (15) Å3

  • Z = 2

  • Mo Kα radiation

  • μ = 0.18 mm−1

  • T = 298 K

  • 0.31 × 0.30 × 0.28 mm

Data collection

  • Siemens SMART CCD area-detector diffractometer

  • Absorption correction: multi-scan (SADABS; Sheldrick, 1996 ▶) T min = 0.946, T max = 0.951

  • 5243 measured reflections

  • 1880 independent reflections

  • 1025 reflections with I > 2σ(I)

  • R int = 0.062

Refinement

  • R[F 2 > 2σ(F 2)] = 0.074

  • wR(F 2) = 0.228

  • S = 1.06

  • 1880 reflections

  • 130 parameters

  • H-atom parameters constrained

  • Δρmax = 0.43 e Å−3

  • Δρmin = −0.24 e Å−3

Data collection: SMART (Siemens, 1996 ▶); cell refinement: SAINT (Siemens, 1996 ▶); data reduction: SAINT; 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/S1600536811011226/ru2002sup1.cif

e-67-o1051-sup1.cif (17KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536811011226/ru2002Isup2.hkl

e-67-o1051-Isup2.hkl (92.5KB, 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—H1A⋯O2i 0.89 2.03 2.857 (6) 155
N1—H1B⋯O3ii 0.89 2.03 2.911 (3) 169

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

Acknowledgments

We acknowledge the National Natural Science Foundation of China (20973089) for financial support.

supplementary crystallographic information

Comment

Long-chain n–alkylammonium halides are widely used as surfactants (Aratono et al., 1998; Tornblom et al., 2000) and as models for biological membranes (Ringsdorf et al., 1988). They exhibit polymorphism at room temperature; solid-solid phase transitions occurred in n–alkylammonium chlorides (Terreros et al., 2000). As a part of the studies on novel potential phase transition materials with the thermochemical properties such as n–alkylammonium chlorides, we report the crystal structure of the title compound (Fig. 1).

Atoms N1–C15 are coplanar in the title compound. The Space group of the title compound is P2(1)/m, however, the space group is P2(1)/c (Melanie Rademeyer,2009). The title compound has a symmetry plane, similarly, the n-pentadecylammonium bromide monohydrates has a symmetry axis. Furthermore, the S, O1, O2 and C16 are coplanar in the title compound.

The crystal packing (Fig. 2) is stabilized by one intermolecular N—H···O hydrogen bonds forming ionic pairs, and two other intramolecular N—H···O hydrogen bonds (Table 1).

Experimental

n–Pentadecylammonium methyl sulfate was prepared by the addition of sulfuric acid to an methanol solution of n–pentadecylamine. The mixture was heated and stirred under reflux for 6 h. Single crystals suitable for X–ray diffraction were prepared by evaporation of the resulting solutionat room temperature. Analysis, calculated for C16H37NSO4 (Mr =339.53): C 56.60, H 10.98, N 4.13%; found: C 56.59, H 10.99, N 4.12%.

Refinement

All the H atoms were placed in geometrically idealized positions and constrained to ride on their parent atoms, with methylene C—H distances of 0.97 Å, methyl C—H distances of 0.96 Å, N—H 0.89 Å and refined as riding on their parent atoms. TheUiso(H) values were set at 1.2Ueq for the methylene H atoms and at 1.5Ueq for other H atoms.

Figures

Fig. 1.

Fig. 1.

The molecular structure of the title compound with the atom numbering scheme. Displacement ellipsoids are drawn at the 30% probability level. H atoms are presented as a small spheres of arbitrary radius.

Fig. 2.

Fig. 2.

N—H···O interactions and intramolecular (dotted lines) in the crystal structure of the title compound. [Symmetry codes: (i) -x + 1, -y + 1, -z; (ii) x + 1, y, z]

Crystal data

C15H34N+·CH3O4S− F(000) = 376
Mr = 339.53 Dx = 1.139 Mg m−3
Monoclinic, P21/m Mo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2yb Cell parameters from 823 reflections
a = 5.4260 (5) Å θ = 2.5–26.3°
b = 7.4981 (6) Å µ = 0.18 mm−1
c = 24.376 (2) Å T = 298 K
β = 93.557 (1)° Acicular, colourless
V = 989.83 (15) Å3 0.31 × 0.30 × 0.28 mm
Z = 2

Data collection

Siemens SMART CCD area-detector diffractometer 1880 independent reflections
Radiation source: fine-focus sealed tube 1025 reflections with I > 2σ(I)
graphite Rint = 0.062
Detector resolution: 10 pixels mm-1 θmax = 25.0°, θmin = 2.5°
phi and ω scans h = −6→6
Absorption correction: multi-scan (SADABS; Sheldrick, 1996) k = −8→8
Tmin = 0.946, Tmax = 0.951 l = −26→28
5243 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)] = 0.074 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.228 H-atom parameters constrained
S = 1.06 w = 1/[σ2(Fo2) + (0.1131P)2] where P = (Fo2 + 2Fc2)/3
1880 reflections (Δ/σ)max = 0.001
130 parameters Δρmax = 0.43 e Å−3
0 restraints Δρmin = −0.24 e Å−3

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
S1 0.3365 (3) 0.7500 0.07723 (6) 0.0623 (6)
O1 0.3834 (8) 0.7500 0.14136 (16) 0.0806 (13)
O2 0.0747 (8) 0.7500 0.07105 (18) 0.1042 (16)
O3 0.4507 (5) 0.5923 (3) 0.05732 (12) 0.0784 (10)
N1 1.2215 (8) 0.2500 0.03004 (18) 0.0562 (12)
H1A 1.1749 0.2500 −0.0056 0.084*
H1B 1.3113 0.3469 0.0381 0.084*
C1 0.9998 (10) 0.2500 0.0626 (2) 0.0559 (14)
H1 0.9012 0.3544 0.0527 0.067*
C2 1.0542 (10) 0.2500 0.1226 (2) 0.0582 (14)
H2 1.1521 0.3545 0.1327 0.070*
C3 0.8258 (10) 0.2500 0.1545 (2) 0.0601 (14)
H3 0.7285 0.3543 0.1437 0.072*
C4 0.8663 (11) 0.2500 0.2159 (2) 0.0702 (16)
H4 0.9641 0.3542 0.2265 0.084*
C5 0.6433 (11) 0.2500 0.2481 (2) 0.0720 (17)
H5 0.5458 0.3541 0.2374 0.086*
C6 0.6793 (13) 0.2500 0.3087 (3) 0.087 (2)
H6 0.7782 0.3539 0.3190 0.104*
C7 0.4670 (12) 0.2500 0.3429 (2) 0.0811 (19)
H7 0.3682 0.3538 0.3325 0.097*
C8 0.5000 (14) 0.2500 0.4025 (3) 0.098 (2)
H8 0.5995 0.3537 0.4127 0.117*
C9 0.2936 (12) 0.2500 0.4378 (2) 0.085 (2)
H9 0.1941 0.3538 0.4277 0.102*
C10 0.3271 (14) 0.2500 0.4972 (3) 0.101 (2)
H10 0.4269 0.3537 0.5072 0.122*
C11 0.1238 (13) 0.2500 0.5329 (3) 0.089 (2)
H11 0.0241 0.3537 0.5228 0.106*
C12 0.1563 (14) 0.2500 0.5919 (3) 0.106 (2)
H12 0.2565 0.3536 0.6018 0.127*
C13 −0.0447 (14) 0.2500 0.6282 (3) 0.092 (2)
H13 −0.1449 0.3536 0.6184 0.111*
C14 −0.0117 (16) 0.2500 0.6873 (3) 0.116 (3)
H14 0.0882 0.3537 0.6973 0.139*
C15 −0.2143 (16) 0.2500 0.7228 (3) 0.113 (3)
H15C −0.1514 0.2500 0.7605 0.169*
H15D −0.3134 0.3545 0.7157 0.169*
C16 0.6344 (14) 0.7500 0.1633 (3) 0.096 (2)
H16A 0.6379 0.7500 0.2028 0.144*
H16B 0.7168 0.8545 0.1510 0.144*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
S1 0.0630 (10) 0.0772 (11) 0.0489 (9) 0.000 0.0208 (7) 0.000
O1 0.077 (3) 0.116 (3) 0.050 (3) 0.000 0.015 (2) 0.000
O2 0.066 (3) 0.177 (5) 0.071 (3) 0.000 0.021 (2) 0.000
O3 0.096 (2) 0.0590 (16) 0.083 (2) −0.0101 (15) 0.0296 (18) −0.0184 (14)
N1 0.054 (3) 0.056 (3) 0.060 (3) 0.000 0.017 (2) 0.000
C1 0.052 (3) 0.063 (3) 0.054 (4) 0.000 0.017 (3) 0.000
C2 0.057 (3) 0.065 (3) 0.054 (4) 0.000 0.012 (3) 0.000
C3 0.060 (3) 0.065 (3) 0.057 (4) 0.000 0.018 (3) 0.000
C4 0.072 (4) 0.081 (4) 0.060 (4) 0.000 0.020 (3) 0.000
C5 0.074 (4) 0.087 (4) 0.056 (4) 0.000 0.023 (3) 0.000
C6 0.083 (5) 0.112 (5) 0.067 (4) 0.000 0.026 (3) 0.000
C7 0.080 (5) 0.104 (5) 0.063 (4) 0.000 0.028 (3) 0.000
C8 0.089 (5) 0.136 (6) 0.071 (5) 0.000 0.027 (4) 0.000
C9 0.082 (5) 0.111 (5) 0.064 (5) 0.000 0.027 (4) 0.000
C10 0.095 (6) 0.139 (6) 0.073 (5) 0.000 0.030 (4) 0.000
C11 0.090 (5) 0.115 (5) 0.064 (5) 0.000 0.026 (4) 0.000
C12 0.104 (6) 0.143 (7) 0.074 (5) 0.000 0.034 (4) 0.000
C13 0.100 (5) 0.116 (6) 0.064 (5) 0.000 0.029 (4) 0.000
C14 0.121 (7) 0.152 (7) 0.077 (6) 0.000 0.041 (5) 0.000
C15 0.128 (7) 0.135 (7) 0.081 (6) 0.000 0.043 (5) 0.000
C16 0.110 (6) 0.106 (5) 0.072 (5) 0.000 0.013 (4) 0.000

Geometric parameters (Å, °)

S1—O2 1.419 (5) C7—C8 1.453 (8)
S1—O3i 1.434 (3) C7—H7 0.9700
S1—O3 1.434 (3) C8—C9 1.454 (8)
S1—O1 1.568 (4) C8—H8 0.9700
O1—C16 1.432 (8) C9—C10 1.450 (8)
N1—C1 1.481 (6) C9—H9 0.9700
N1—H1A 0.8900 C10—C11 1.445 (8)
N1—H1B 0.8900 C10—H10 0.9700
C1—C2 1.474 (7) C11—C12 1.439 (9)
C1—H1 0.9700 C11—H11 0.9700
C2—C3 1.503 (7) C12—C13 1.447 (9)
C2—H2 0.9700 C12—H12 0.9700
C3—C4 1.500 (7) C13—C14 1.440 (8)
C3—H3 0.9700 C13—H13 0.9700
C4—C5 1.483 (7) C14—C15 1.441 (9)
C4—H4 0.9700 C14—H14 0.9700
C5—C6 1.478 (8) C15—H15C 0.9600
C5—H5 0.9700 C15—H15D 0.9600
C6—C7 1.462 (8) C16—H16A 0.9600
C6—H6 0.9700 C16—H16B 0.9600
O2—S1—O3i 114.50 (15) C8—C7—H7 107.0
O2—S1—O3 114.50 (15) C6—C7—H7 107.1
O3i—S1—O3 111.2 (2) C7—C8—C9 122.7 (7)
O2—S1—O1 101.8 (3) C7—C8—H8 106.7
O3i—S1—O1 106.91 (15) C9—C8—H8 106.6
O3—S1—O1 106.91 (15) C10—C9—C8 122.6 (6)
C16—O1—S1 117.7 (4) C10—C9—H9 106.7
C1—N1—H1A 109.4 C8—C9—H9 106.7
C1—N1—H1B 109.5 C11—C10—C9 123.2 (7)
H1A—N1—H1B 109.5 C11—C10—H10 106.5
C2—C1—N1 114.3 (4) C9—C10—H10 106.5
C2—C1—H1 108.6 C12—C11—C10 123.4 (7)
N1—C1—H1 108.7 C12—C11—H11 106.5
C1—C2—C3 113.1 (4) C10—C11—H11 106.4
C1—C2—H2 109.0 C11—C12—C13 124.2 (7)
C3—C2—H2 108.9 C11—C12—H12 106.3
C4—C3—C2 116.2 (5) C13—C12—H12 106.3
C4—C3—H3 108.3 C14—C13—C12 124.1 (7)
C2—C3—H3 108.2 C14—C13—H13 106.3
C5—C4—C3 117.0 (5) C12—C13—H13 106.3
C5—C4—H4 108.0 C13—C14—C15 123.2 (8)
C3—C4—H4 108.0 C13—C14—H14 106.5
C6—C5—C4 117.9 (5) C15—C14—H14 106.5
C6—C5—H5 107.8 C14—C15—H15C 109.6
C4—C5—H5 107.8 C14—C15—H15D 109.4
C7—C6—C5 120.6 (6) H15C—C15—H15D 109.5
C7—C6—H6 107.2 O1—C16—H16A 109.5
C5—C6—H6 107.2 O1—C16—H16B 109.5
C8—C7—C6 121.1 (6) H16A—C16—H16B 109.5
O2—S1—O1—C16 180.000 (1) C5—C6—C7—C8 180.000 (3)
O3i—S1—O1—C16 −59.57 (14) C6—C7—C8—C9 180.000 (3)
O3—S1—O1—C16 59.57 (14) C7—C8—C9—C10 180.000 (4)
N1—C1—C2—C3 180.0 C8—C9—C10—C11 180.000 (3)
C1—C2—C3—C4 180.000 (1) C9—C10—C11—C12 180.000 (4)
C2—C3—C4—C5 180.000 (1) C10—C11—C12—C13 180.000 (5)
C3—C4—C5—C6 180.000 (2) C11—C12—C13—C14 180.000 (6)
C4—C5—C6—C7 180.000 (2) C12—C13—C14—C15 180.000 (6)

Symmetry codes: (i) x, −y+3/2, z.

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
N1—H1A···O2ii 0.89 2.03 2.857 (6) 155.
N1—H1B···O3iii 0.89 2.03 2.911 (3) 169.

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

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: RU2002).

References

  1. Aratono, M., Villeneuve, M., Takiue, T., Ikeda, N. & Iyota, H. (1998). J. Colloid Interface Sci. 200, 161–171.
  2. Ringsdorf, H., Schlarb, B. & Venzmer, J. (1988). Angew. Chem. Int. Ed. Engl. 27, 113–158.
  3. Sheldrick, G. M. (1996). SADABS University of Göttingen, Germany.
  4. Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
  5. Siemens (1996). SMART and SAINT Siemens Analytical X-Ray Systems, Inc., Madison, Wisconsin, USA.
  6. Terreros, A., Galera-Gomez, P. J. & Lopez-Cabarcos, E. (2000). J. Therm. Anal. Calorim. 61, 341–350.
  7. Tornblom, M., Sitnikov, R. & Henriksson, U. (2000). J. Phys. Chem. B, 104, 1529–1538.

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/S1600536811011226/ru2002sup1.cif

e-67-o1051-sup1.cif (17KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536811011226/ru2002Isup2.hkl

e-67-o1051-Isup2.hkl (92.5KB, hkl)

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


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