Abstract
In the title compound, C13H30N+·Cl−·H2O, the C13H27 alkyl chain is in an all-trans conformation. In the crystal, intermolecular N—H⋯Cl, N—H⋯O and O—H⋯Cl hydrogen bonds connect the components into layers parallel to (010), with the alkyl chains oriented approximately perpendicular to these layers.
Related literature
For applications of long-chain n-alkylammonium halides, see: Aratono et al. (1998 ▶); Tornblom et al. (2000 ▶); Ringsdorf et al. (1988 ▶). For details of phase transitions in n-alkylammonium chlorides, see: Terreros et al. (2000 ▶). For related structures, see: Rademeyer et al. (2009 ▶); Lundén (1974 ▶); Clark & Hudgens (1950 ▶).
Experimental
Crystal data
C13H30N+·Cl−·H2O
M r = 253.85
Monoclinic,
a = 4.7420 (5) Å
b = 45.250 (3) Å
c = 7.8191 (9) Å
β = 106.332 (2)°
V = 1610.1 (3) Å3
Z = 4
Mo Kα radiation
μ = 0.22 mm−1
T = 298 K
0.34 × 0.33 × 0.03 mm
Data collection
Siemens SMART CCD area-detector diffractometer
Absorption correction: multi-scan (SADABS; Sheldrick, 1996 ▶) T min = 0.928, T max = 0.993
8230 measured reflections
2845 independent reflections
1379 reflections with I > 2σ(I)
R int = 0.077
Refinement
R[F 2 > 2σ(F 2)] = 0.067
wR(F 2) = 0.124
S = 1.03
2845 reflections
147 parameters
H-atom parameters constrained
Δρmax = 0.25 e Å−3
Δρmin = −0.18 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/S1600536811006246/lh5197sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536811006246/lh5197Isup2.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⋯Cl1 | 0.89 | 2.44 | 3.303 (3) | 162 |
| N1—H1B⋯Cl1i | 0.89 | 2.36 | 3.236 (2) | 170 |
| N1—H1C⋯O1ii | 0.89 | 2.05 | 2.901 (4) | 159 |
| O1—H1H⋯Cl1 | 0.85 | 2.45 | 3.290 (3) | 170 |
| O1—H1I⋯Cl1iii | 0.85 | 2.39 | 3.228 (2) | 170 |
Symmetry codes: (i)
; (ii)
; (iii)
.
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). It has been shown that phase transitions occur in n-alkylammonium chlorides (Terreros et al., 2000). As a part of our studies on novel potential phase transition materials with thermochemical properties, we report herein the crystal structure of the title compound (Fig. 1).
Atoms C2–C13 are essentially co-planar with a maximum deviation of 0.048 (3)Å for atom C2. The alkyl chain in related compounds is typically in the extended conformation e.g. in the isostructural n-tridecylamine bromide monohydrate compound (Rademeyer et al., 2009), n–dodecylammonium bromide (Lundén, 1974) and n–tridecylamine chloride (Clark & Hudgens, 1950). Although the methylene chain has the extended all–trans conformation, it is slightly bent in the vicinity of the ammonium group possibly to accommodate the hydrogen–bonding interactions. Only the C1–C2–C3–C4 torsion angle deviates significantly from 180 °, with a value of 169.84 (3)°. The crystal packing (Fig. 2) is stabilized by intermolecular N—H···Cl, N—H···O and O—H···Cl hydrogen bonds (Table 1 and Fig.2).
Experimental
n–Tridecylamine chloride monohydrate was prepared by the addition of hydrochloric acid to an ethanolic solution of n–tridecylamine. 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 solution at room temperature. Analysis, calculated for C13H32ClNO (Mr =253.85): C 61.51, H 12.71, N 5.52, Cl 13.96%; found: C 61.50, H 12.72, N 5.51, Cl 13.95%.
Refinement
All H atoms were placed in geometrically idealized positions and constrained to ride on their parent atoms, with methylene C—H = 0.97 Å, methyl C—H = 0.96 Å, N—H = 0.89 Å, O-H = 0.85 Å and refined as riding on their parent atoms. TheUiso(H) values were set at 1.2Ueq(Cmethylene, O) at 1.5Ueq(Cmethyl,N).
Figures
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.
Part of the crystal structure with hydrogen bonds shown as dashed lines.
Crystal data
| C13H30N+·Cl−·H2O | F(000) = 568 |
| Mr = 253.85 | Dx = 1.047 Mg m−3 |
| Monoclinic, P21/c | Mo Kα radiation, λ = 0.71073 Å |
| Hall symbol: -P 2ybc | Cell parameters from 817 reflections |
| a = 4.7420 (5) Å | θ = 2.7–20.8° |
| b = 45.250 (3) Å | µ = 0.22 mm−1 |
| c = 7.8191 (9) Å | T = 298 K |
| β = 106.332 (2)° | Acicular, colourless |
| V = 1610.1 (3) Å3 | 0.34 × 0.33 × 0.03 mm |
| Z = 4 |
Data collection
| Siemens SMART CCD area-detector diffractometer | 2845 independent reflections |
| Radiation source: fine-focus sealed tube | 1379 reflections with I > 2σ(I) |
| graphite | Rint = 0.077 |
| Detector resolution: 10 pixels mm-1 | θmax = 25.0°, θmin = 2.7° |
| φ and ω scans | h = −5→5 |
| Absorption correction: multi-scan (SADABS; Sheldrick, 1996) | k = −53→46 |
| Tmin = 0.928, Tmax = 0.993 | l = −7→9 |
| 8230 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)] = 0.067 | Hydrogen site location: inferred from neighbouring sites |
| wR(F2) = 0.124 | H-atom parameters constrained |
| S = 1.03 | w = 1/[σ2(Fo2) + (0.0256P)2] where P = (Fo2 + 2Fc2)/3 |
| 2845 reflections | (Δ/σ)max = 0.001 |
| 147 parameters | Δρmax = 0.25 e Å−3 |
| 0 restraints | Δρmin = −0.18 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 | ||
| Cl1 | 0.77004 (19) | 0.727389 (19) | 0.54882 (12) | 0.0578 (3) | |
| N1 | 0.2908 (5) | 0.72396 (5) | 0.1504 (4) | 0.0486 (8) | |
| H1A | 0.4378 | 0.7281 | 0.2466 | 0.073* | |
| H1B | 0.1648 | 0.7390 | 0.1270 | 0.073* | |
| H1C | 0.3618 | 0.7210 | 0.0578 | 0.073* | |
| O1 | 0.3848 (5) | 0.70538 (5) | 0.8156 (3) | 0.0690 (8) | |
| H1H | 0.5034 | 0.7102 | 0.7566 | 0.083* | |
| H1I | 0.2125 | 0.7103 | 0.7554 | 0.083* | |
| C1 | 0.1369 (7) | 0.69683 (6) | 0.1834 (4) | 0.0462 (9) | |
| H1D | −0.0396 | 0.6941 | 0.0856 | 0.055* | |
| H1E | 0.0779 | 0.6994 | 0.2915 | 0.055* | |
| C2 | 0.3263 (7) | 0.66944 (6) | 0.2017 (4) | 0.0445 (9) | |
| H2A | 0.5028 | 0.6722 | 0.2995 | 0.053* | |
| H2B | 0.3852 | 0.6668 | 0.0935 | 0.053* | |
| C3 | 0.1677 (7) | 0.64186 (6) | 0.2355 (4) | 0.0467 (9) | |
| H3A | −0.0251 | 0.6412 | 0.1498 | 0.056* | |
| H3B | 0.1397 | 0.6431 | 0.3534 | 0.056* | |
| C4 | 0.3305 (7) | 0.61334 (6) | 0.2221 (4) | 0.0444 (9) | |
| H4A | 0.5222 | 0.6140 | 0.3090 | 0.053* | |
| H4B | 0.3616 | 0.6123 | 0.1049 | 0.053* | |
| C5 | 0.1730 (7) | 0.58533 (6) | 0.2526 (4) | 0.0471 (9) | |
| H5A | 0.1495 | 0.5860 | 0.3718 | 0.056* | |
| H5B | −0.0219 | 0.5851 | 0.1691 | 0.056* | |
| C6 | 0.3292 (7) | 0.55675 (6) | 0.2317 (4) | 0.0440 (9) | |
| H6A | 0.3543 | 0.5562 | 0.1128 | 0.053* | |
| H6B | 0.5234 | 0.5569 | 0.3159 | 0.053* | |
| C7 | 0.1722 (7) | 0.52882 (6) | 0.2603 (4) | 0.0450 (9) | |
| H7A | −0.0231 | 0.5288 | 0.1773 | 0.054* | |
| H7B | 0.1496 | 0.5292 | 0.3798 | 0.054* | |
| C8 | 0.3260 (6) | 0.50019 (6) | 0.2369 (4) | 0.0440 (9) | |
| H8A | 0.3473 | 0.4997 | 0.1171 | 0.053* | |
| H8B | 0.5218 | 0.5003 | 0.3193 | 0.053* | |
| C9 | 0.1705 (7) | 0.47222 (6) | 0.2666 (4) | 0.0448 (9) | |
| H9A | −0.0251 | 0.4721 | 0.1839 | 0.054* | |
| H9B | 0.1485 | 0.4727 | 0.3862 | 0.054* | |
| C10 | 0.3245 (7) | 0.44364 (6) | 0.2439 (4) | 0.0438 (9) | |
| H10A | 0.3458 | 0.4431 | 0.1242 | 0.053* | |
| H10B | 0.5204 | 0.4438 | 0.3263 | 0.053* | |
| C11 | 0.1702 (7) | 0.41561 (6) | 0.2745 (4) | 0.0448 (9) | |
| H11A | 0.1479 | 0.4162 | 0.3940 | 0.054* | |
| H11B | −0.0253 | 0.4154 | 0.1917 | 0.054* | |
| C12 | 0.3236 (7) | 0.38729 (6) | 0.2530 (5) | 0.0522 (10) | |
| H12A | 0.5194 | 0.3876 | 0.3355 | 0.063* | |
| H12B | 0.3452 | 0.3867 | 0.1333 | 0.063* | |
| C13 | 0.1688 (8) | 0.35920 (7) | 0.2844 (5) | 0.0703 (12) | |
| H13A | 0.1532 | 0.3591 | 0.4042 | 0.105* | |
| H13B | 0.2798 | 0.3423 | 0.2668 | 0.105* | |
| H13C | −0.0242 | 0.3584 | 0.2021 | 0.105* |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| Cl1 | 0.0520 (5) | 0.0590 (6) | 0.0612 (6) | −0.0052 (5) | 0.0137 (4) | −0.0036 (5) |
| N1 | 0.0485 (16) | 0.0358 (17) | 0.061 (2) | 0.0041 (15) | 0.0145 (14) | 0.0002 (14) |
| O1 | 0.0659 (17) | 0.0752 (17) | 0.0683 (19) | 0.0036 (15) | 0.0230 (13) | 0.0100 (14) |
| C1 | 0.044 (2) | 0.034 (2) | 0.062 (3) | 0.0005 (18) | 0.0178 (17) | 0.0039 (16) |
| C2 | 0.046 (2) | 0.035 (2) | 0.053 (2) | −0.0022 (18) | 0.0152 (17) | −0.0021 (16) |
| C3 | 0.052 (2) | 0.039 (2) | 0.053 (2) | −0.0043 (19) | 0.0209 (18) | 0.0011 (17) |
| C4 | 0.050 (2) | 0.036 (2) | 0.050 (2) | −0.0033 (18) | 0.0191 (18) | 0.0020 (16) |
| C5 | 0.053 (2) | 0.041 (2) | 0.049 (2) | −0.005 (2) | 0.0189 (18) | 0.0004 (17) |
| C6 | 0.048 (2) | 0.039 (2) | 0.048 (2) | −0.0014 (19) | 0.0177 (17) | 0.0012 (16) |
| C7 | 0.048 (2) | 0.039 (2) | 0.050 (2) | −0.0024 (19) | 0.0178 (17) | 0.0029 (17) |
| C8 | 0.047 (2) | 0.040 (2) | 0.047 (2) | −0.003 (2) | 0.0170 (17) | 0.0042 (16) |
| C9 | 0.051 (2) | 0.037 (2) | 0.049 (2) | −0.0035 (19) | 0.0190 (18) | −0.0009 (16) |
| C10 | 0.048 (2) | 0.040 (2) | 0.047 (2) | −0.0014 (19) | 0.0194 (17) | −0.0011 (16) |
| C11 | 0.050 (2) | 0.039 (2) | 0.048 (2) | −0.0033 (19) | 0.0167 (17) | 0.0026 (16) |
| C12 | 0.062 (2) | 0.041 (2) | 0.054 (3) | 0.004 (2) | 0.0163 (19) | 0.0000 (17) |
| C13 | 0.094 (3) | 0.043 (2) | 0.076 (3) | −0.005 (2) | 0.026 (2) | 0.001 (2) |
Geometric parameters (Å, °)
| N1—C1 | 1.487 (3) | C6—H6B | 0.9700 |
| N1—H1A | 0.8900 | C7—C8 | 1.523 (4) |
| N1—H1B | 0.8900 | C7—H7A | 0.9700 |
| N1—H1C | 0.8900 | C7—H7B | 0.9700 |
| O1—H1H | 0.8499 | C8—C9 | 1.515 (4) |
| O1—H1I | 0.8499 | C8—H8A | 0.9700 |
| C1—C2 | 1.513 (4) | C8—H8B | 0.9700 |
| C1—H1D | 0.9700 | C9—C10 | 1.520 (4) |
| C1—H1E | 0.9700 | C9—H9A | 0.9700 |
| C2—C3 | 1.518 (4) | C9—H9B | 0.9700 |
| C2—H2A | 0.9700 | C10—C11 | 1.517 (4) |
| C2—H2B | 0.9700 | C10—H10A | 0.9700 |
| C3—C4 | 1.523 (4) | C10—H10B | 0.9700 |
| C3—H3A | 0.9700 | C11—C12 | 1.506 (4) |
| C3—H3B | 0.9700 | C11—H11A | 0.9700 |
| C4—C5 | 1.524 (4) | C11—H11B | 0.9700 |
| C4—H4A | 0.9700 | C12—C13 | 1.522 (4) |
| C4—H4B | 0.9700 | C12—H12A | 0.9700 |
| C5—C6 | 1.522 (4) | C12—H12B | 0.9700 |
| C5—H5A | 0.9700 | C13—H13A | 0.9600 |
| C5—H5B | 0.9700 | C13—H13B | 0.9600 |
| C6—C7 | 1.515 (4) | C13—H13C | 0.9600 |
| C6—H6A | 0.9700 | ||
| C1—N1—H1A | 109.5 | C6—C7—C8 | 114.8 (3) |
| C1—N1—H1B | 109.5 | C6—C7—H7A | 108.6 |
| H1A—N1—H1B | 109.5 | C8—C7—H7A | 108.6 |
| C1—N1—H1C | 109.5 | C6—C7—H7B | 108.6 |
| H1A—N1—H1C | 109.5 | C8—C7—H7B | 108.6 |
| H1B—N1—H1C | 109.5 | H7A—C7—H7B | 107.5 |
| H1H—O1—H1I | 108.1 | C9—C8—C7 | 114.9 (2) |
| N1—C1—C2 | 112.7 (3) | C9—C8—H8A | 108.5 |
| N1—C1—H1D | 109.1 | C7—C8—H8A | 108.5 |
| C2—C1—H1D | 109.1 | C9—C8—H8B | 108.5 |
| N1—C1—H1E | 109.1 | C7—C8—H8B | 108.5 |
| C2—C1—H1E | 109.1 | H8A—C8—H8B | 107.5 |
| H1D—C1—H1E | 107.8 | C8—C9—C10 | 115.0 (3) |
| C1—C2—C3 | 112.3 (3) | C8—C9—H9A | 108.5 |
| C1—C2—H2A | 109.1 | C10—C9—H9A | 108.5 |
| C3—C2—H2A | 109.1 | C8—C9—H9B | 108.5 |
| C1—C2—H2B | 109.1 | C10—C9—H9B | 108.5 |
| C3—C2—H2B | 109.1 | H9A—C9—H9B | 107.5 |
| H2A—C2—H2B | 107.9 | C11—C10—C9 | 115.1 (3) |
| C2—C3—C4 | 113.5 (3) | C11—C10—H10A | 108.5 |
| C2—C3—H3A | 108.9 | C9—C10—H10A | 108.5 |
| C4—C3—H3A | 108.9 | C11—C10—H10B | 108.5 |
| C2—C3—H3B | 108.9 | C9—C10—H10B | 108.5 |
| C4—C3—H3B | 108.9 | H10A—C10—H10B | 107.5 |
| H3A—C3—H3B | 107.7 | C12—C11—C10 | 115.1 (3) |
| C3—C4—C5 | 114.5 (3) | C12—C11—H11A | 108.5 |
| C3—C4—H4A | 108.6 | C10—C11—H11A | 108.5 |
| C5—C4—H4A | 108.6 | C12—C11—H11B | 108.5 |
| C3—C4—H4B | 108.6 | C10—C11—H11B | 108.5 |
| C5—C4—H4B | 108.6 | H11A—C11—H11B | 107.5 |
| H4A—C4—H4B | 107.6 | C11—C12—C13 | 115.0 (3) |
| C6—C5—C4 | 114.5 (3) | C11—C12—H12A | 108.5 |
| C6—C5—H5A | 108.6 | C13—C12—H12A | 108.5 |
| C4—C5—H5A | 108.6 | C11—C12—H12B | 108.5 |
| C6—C5—H5B | 108.6 | C13—C12—H12B | 108.5 |
| C4—C5—H5B | 108.6 | H12A—C12—H12B | 107.5 |
| H5A—C5—H5B | 107.6 | C12—C13—H13A | 109.5 |
| C7—C6—C5 | 114.8 (3) | C12—C13—H13B | 109.5 |
| C7—C6—H6A | 108.6 | H13A—C13—H13B | 109.5 |
| C5—C6—H6A | 108.6 | C12—C13—H13C | 109.5 |
| C7—C6—H6B | 108.6 | H13A—C13—H13C | 109.5 |
| C5—C6—H6B | 108.6 | H13B—C13—H13C | 109.5 |
| H6A—C6—H6B | 107.6 | ||
| N1—C1—C2—C3 | 180.0 (3) | C6—C7—C8—C9 | 179.6 (3) |
| C1—C2—C3—C4 | 169.9 (3) | C7—C8—C9—C10 | −179.8 (3) |
| C2—C3—C4—C5 | −179.1 (3) | C8—C9—C10—C11 | 179.7 (3) |
| C3—C4—C5—C6 | 177.6 (3) | C9—C10—C11—C12 | −179.7 (3) |
| C4—C5—C6—C7 | −179.5 (3) | C10—C11—C12—C13 | 179.8 (3) |
| C5—C6—C7—C8 | 179.2 (3) |
Hydrogen-bond geometry (Å, °)
| D—H···A | D—H | H···A | D···A | D—H···A |
| N1—H1A···Cl1 | 0.89 | 2.44 | 3.303 (3) | 162 |
| N1—H1B···Cl1i | 0.89 | 2.36 | 3.236 (2) | 170 |
| N1—H1C···O1ii | 0.89 | 2.05 | 2.901 (4) | 159 |
| O1—H1H···Cl1 | 0.85 | 2.45 | 3.290 (3) | 170 |
| O1—H1I···Cl1iii | 0.85 | 2.39 | 3.228 (2) | 170 |
Symmetry codes: (i) x−1, −y+3/2, z−1/2; (ii) x, y, z−1; (iii) x−1, y, z.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: LH5197).
References
- Aratono, M., Villeneuve, M., Takiue, T., Ikeda, N. & Iyota, H. (1998). J. Colloid Interface Sci. 200, 161–171.
- Clark, G. L. & Hudgens, C. R. (1950). Science, 112, 309. [DOI] [PubMed]
- Lundén, B.-M. (1974). Acta Cryst. B30, 1756–1760.
- Rademeyer, M., Kruger, G. J. & Billing, D. G. (2009). CrystEngComm, 11, 1926–1933.
- Ringsdorf, H., Schlarb, B. & Venzmer, J. (1988). Angew. Chem. Int. Ed. Engl. 27, 113–158.
- Sheldrick, G. M. (1996). SADABS University of Göttingen, Germany.
- Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
- Siemens (1996). SMART and SAINT Siemens Analytical X-ray Instruments Inc., Madison, Wisconsin, USA.
- Terreros, A., Galera-Gomez, P. J. & Lopez-Cabarcos, E. (2000). J. Therm. Anal. Calorim. 61, 341–350.
- 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/S1600536811006246/lh5197sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536811006246/lh5197Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report


