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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2012 Nov 10;68(Pt 12):o3335. doi: 10.1107/S1600536812045746

(S)-(−)-1-Phenyl­ethanaminium hexa­noate

Mary H Wood a,*, Stuart M Clarke a
PMCID: PMC3588937  PMID: 23476173

Abstract

A binary mixture of (S)-(−)-1-phenyl­ethanamine and hexa­noic acid was allowed to react to form the title salt, C8H12N+·C6H11O2 . This crystal contains a 1:1 stoichiometric mixture of the acid- and amine-derived species and displays a chiral structure with N—H⋯O hydrogen-bonded chains propagating along the c-axis direction.

Related literature  

For spectroscopic studies of acid–amine complexes, see: Karlsson et al. (2000); Paivarinta et al. (2000); Kohler et al. (1981); Smith et al. (2001, 2002); Klokkenburg et al. (2007). For recent diffraction studies of acid–amine complexes, see: Jefferson et al. (2011); Sun et al. (2011); Wood & Clarke (2012).graphic file with name e-68-o3335-scheme1.jpg

Experimental  

Crystal data  

  • C8H12N+·C6H11O2

  • M r = 237.33

  • Hexagonal, Inline graphic

  • a = 19.5845 (5) Å

  • c = 6.6307 (2) Å

  • V = 2202.49 (10) Å3

  • Z = 6

  • Mo Kα radiation

  • μ = 0.07 mm−1

  • T = 180 K

  • 0.46 × 0.05 × 0.05 mm

Data collection  

  • Nonius KappaCCD diffractometer

  • Absorption correction: multi-scan (SORTAV; Blessing, 1995) T min = 0.740, T max = 0.999

  • 11638 measured reflections

  • 1461 independent reflections

  • 1270 reflections with I > 2σ(I)

  • R int = 0.064

Refinement  

  • R[F 2 > 2σ(F 2)] = 0.040

  • wR(F 2) = 0.087

  • S = 1.06

  • 1461 reflections

  • 157 parameters

  • 1 restraint

  • H-atom parameters constrained

  • Δρmax = 0.11 e Å−3

  • Δρmin = −0.14 e Å−3

Data collection: COLLECT (Nonius, 1998); cell refinement: SCALEPACK (Otwinowski & Minor, 1997); data reduction: DENZO (Otwinowski & Minor, 1997) and SCALEPACK; program(s) used to solve structure: SIR92 (Altomare et al., 1994); program(s) used to refine structure: SHELXL97 (Sheldrick 2008); molecular graphics: Mercury (Macrae et al., 2008); software used to prepare material for publication: SHELXL97.

Supplementary Material

Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536812045746/mw2095sup1.cif

e-68-o3335-sup1.cif (17.1KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812045746/mw2095Isup2.hkl

e-68-o3335-Isup2.hkl (72.1KB, hkl)

Supplementary material file. DOI: 10.1107/S1600536812045746/mw2095Isup3.cml

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—H1A⋯O2i 0.91 1.84 2.753 (3) 176
N1—H1B⋯O1 0.91 1.87 2.768 (3) 167
N1—H1C⋯O1ii 0.91 1.82 2.714 (2) 168

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

Acknowledgments

The authors thank the Department of Chemistry, the BP Institute and the Oppenheimer Trust for financial and technical assistance and Dr J. E. Davies for collecting and analysing the X-ray data.

supplementary crystallographic information

Comment

The existence of stable acid:amine complexes formed from simple acid and amine reagents has been reported in the literature (Klokkenburg et al., 2007; Karlsson et al., 2000). Many examples adopt a 1:1 stoichiometry, although acid-rich complexes are not uncommon, with both 2:1 and 3:1 adducts observed in some cases (Sun et al., 2011; Kohler et al., 1981). Amine-rich complexes are thought to be inherently instable and thus unlikely to form (Paivarinta et al., 2000), although there is a report of a diamine complex formed between methylamine and dnsa (3,5-dinitrosalicyclic acid) due to deprotonation of the phenolic group in the acid (Smith et al., 2001; Smith et al., 2002).

The stability of complexes such as the title compound derives from the reactive exchange of a proton giving cations and anions with a strong electrostatic attraction. These ions subsequently interact via strong hydrogen-bond formation; each ammonium ion in the s-(-)-α-methylbenzylammonium hexanoate example is able to form three hydrogen bonds (shown in Figures 1, 2 and 3). For the acid-rich complexes, the hydrogen bonding is considered to extend over the three (or more) species involved.

This work follows previous findings of the formation of a 1:1 complex of octanoic acid and decylamine using the same method (Jefferson et al., 2011) as well as a 1:1 complex between benzylamine and hexanoic acid (Wood et al., 2012). This work focuses on the use of a chiral amine, s-(-)-α-methylbenzylamine.

Whilst spectroscopic studies identifying such acid:amine complexes are reasonably common, there still only a few examples of single-crystal X-ray data, as reported here. This may be attributed to the difficulty of growing suitable crystals as outlined in the experimental section.

Experimental

Hexanoic acid and s-(-)-methylbenzylamine, with purities of 99.5% and 99.8% respectively as determined by titration and GC, were purchased from Sigma Aldrich and used without further purification. The crystals were grown by pipetting a small volume (approximately 1 ml) of each into small vials and leaving within a larger vial along with a polypropylene nucleation surface under an inert atmosphere (to minimize amine reaction with atmospheric CO2 (Sun et al., 2011)). After several weeks abundant crystal growth on the polypropylene surface was observed and a sample selected for X-ray characterization.

Elemental analysis of the crystalline sample gave values of 70.64%, 5.98%, 9.72% and 13.66% for carbon, nitrogen, hydrogen and oxygen respectively. For a 1:1 acid: amine complex, the expected values are: 70.85%, 5.90%, 9.77% and 13.48%, in excellent agreement.

The experimental sample temperature 180 K represents a compromise of improved thermal factors but avoiding sample fracture.

Refinement

The absolute structure was assigned from the known configuration of the starting material. 1183 Friedel pairs were averaged for the refinement.

Hydrogen site location were inferred from neighbouring sites and H-atom parameters were constrained in the refinement.

Figures

Fig. 1.

Fig. 1.

Perspective view of the asymmetric unit showing one of the three N—H···O hydrogen bonds.

Fig. 2.

Fig. 2.

Illustration of the molecular packing - top view of a hydrogen bonded chain. Hydrogen bonds are shown by dashed red lines.

Fig. 3.

Fig. 3.

Illustration of the molecular packing - side view of a hydrogen bonded chain. Hydrogen bonds are shown by dashed red lines and form chains of molecules parallel to the c axis.

Crystal data

C8H12N+·C6H11O2 Dx = 1.074 Mg m3
Mr = 237.33 Mo Kα radiation, λ = 0.71073 Å
Hexagonal, P63 Cell parameters from 7677 reflections
Hall symbol: P 6c θ = 1.0–25.4°
a = 19.5845 (5) Å µ = 0.07 mm1
c = 6.6307 (2) Å T = 180 K
V = 2202.49 (10) Å3 Needle, colourless
Z = 6 0.46 × 0.05 × 0.05 mm
F(000) = 780

Data collection

Nonius KappaCCD diffractometer 1270 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tube Rint = 0.064
Thin slice ω and φ scans θmax = 25.4°, θmin = 3.6°
Absorption correction: multi-scan (SORTAV; Blessing, 1995) h = −23→22
Tmin = 0.740, Tmax = 0.999 k = −22→23
11638 measured reflections l = −7→7
1461 independent 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)] = 0.040 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.087 H-atom parameters constrained
S = 1.06 w = 1/[σ2(Fo2) + (0.0379P)2 + 0.3614P] where P = (Fo2 + 2Fc2)/3
1461 reflections (Δ/σ)max < 0.001
157 parameters Δρmax = 0.11 e Å3
1 restraint Δρmin = −0.14 e Å3

Special details

Experimental. multi-scan from symmetry-related measurements Sortav (Blessing, 1995)
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
N1 0.51079 (11) 0.94274 (11) 0.0797 (3) 0.0332 (4)
H1A 0.5437 0.9491 −0.0246 0.050*
H1B 0.5394 0.9618 0.1949 0.050*
H1C 0.4849 0.9695 0.0530 0.050*
C1 0.49217 (13) 0.81354 (13) 0.1884 (4) 0.0352 (5)
C2 0.46986 (15) 0.77731 (15) 0.3746 (4) 0.0442 (6)
H2 0.4295 0.7797 0.4483 0.053*
C3 0.50523 (17) 0.73764 (15) 0.4557 (5) 0.0530 (7)
H3 0.4899 0.7139 0.5850 0.064*
C4 0.56286 (17) 0.73265 (15) 0.3483 (5) 0.0534 (8)
H4 0.5871 0.7051 0.4027 0.064*
C5 0.58501 (16) 0.76781 (15) 0.1621 (5) 0.0497 (7)
H5 0.6246 0.7642 0.0879 0.060*
C6 0.55026 (14) 0.80857 (15) 0.0807 (4) 0.0415 (6)
H6 0.5662 0.8329 −0.0479 0.050*
C7 0.45226 (13) 0.85703 (14) 0.1056 (4) 0.0367 (6)
H7 0.4121 0.8522 0.2063 0.044*
C8 0.41036 (17) 0.82438 (18) −0.0939 (5) 0.0580 (8)
H8A 0.3859 0.8549 −0.1387 0.087*
H8B 0.3696 0.7690 −0.0765 0.087*
H8C 0.4486 0.8281 −0.1951 0.087*
O1 0.57647 (10) 0.99218 (11) 0.4586 (3) 0.0445 (5)
O2 0.60989 (10) 0.96859 (11) 0.7585 (3) 0.0492 (5)
C9 0.61695 (13) 0.97445 (13) 0.5718 (4) 0.0326 (5)
C10 0.67789 (14) 0.95875 (14) 0.4762 (4) 0.0360 (5)
H10A 0.6532 0.9013 0.4529 0.043*
H10B 0.7211 0.9736 0.5745 0.043*
C11 0.71404 (14) 1.00073 (15) 0.2782 (4) 0.0396 (6)
H11A 0.6714 0.9874 0.1792 0.047*
H11B 0.7414 1.0584 0.3008 0.047*
C12 0.77217 (14) 0.97868 (14) 0.1911 (4) 0.0396 (6)
H12A 0.8136 0.9902 0.2926 0.048*
H12B 0.7442 0.9212 0.1647 0.048*
C13 0.81090 (17) 1.02175 (16) −0.0018 (4) 0.0495 (7)
H13A 0.8426 1.0789 0.0267 0.059*
H13B 0.7695 1.0138 −0.1000 0.059*
C14 0.8639 (2) 0.99434 (19) −0.0959 (5) 0.0714 (10)
H14A 0.8851 1.0221 −0.2237 0.107*
H14B 0.8333 0.9374 −0.1208 0.107*
H14C 0.9075 1.0058 −0.0037 0.107*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
N1 0.0388 (10) 0.0438 (11) 0.0260 (9) 0.0273 (9) 0.0000 (9) −0.0005 (9)
C1 0.0343 (12) 0.0335 (12) 0.0342 (13) 0.0143 (10) −0.0028 (11) −0.0051 (12)
C2 0.0440 (14) 0.0454 (14) 0.0401 (15) 0.0202 (12) 0.0053 (12) 0.0048 (12)
C3 0.0592 (17) 0.0431 (15) 0.0479 (18) 0.0189 (14) −0.0035 (15) 0.0121 (14)
C4 0.0577 (18) 0.0333 (14) 0.070 (2) 0.0229 (13) −0.0176 (16) −0.0024 (15)
C5 0.0481 (15) 0.0459 (15) 0.0634 (19) 0.0297 (13) −0.0045 (15) −0.0113 (15)
C6 0.0441 (14) 0.0422 (14) 0.0392 (13) 0.0223 (12) 0.0030 (13) −0.0027 (12)
C7 0.0317 (12) 0.0433 (13) 0.0362 (14) 0.0195 (11) 0.0033 (11) 0.0028 (11)
C8 0.0509 (17) 0.0625 (18) 0.059 (2) 0.0272 (14) −0.0232 (15) −0.0104 (16)
O1 0.0534 (10) 0.0647 (11) 0.0333 (10) 0.0430 (9) −0.0058 (9) −0.0097 (9)
O2 0.0512 (11) 0.0703 (13) 0.0298 (11) 0.0331 (10) 0.0079 (9) 0.0073 (9)
C9 0.0327 (12) 0.0322 (12) 0.0300 (15) 0.0142 (10) −0.0018 (11) −0.0032 (11)
C10 0.0373 (13) 0.0420 (13) 0.0321 (13) 0.0223 (11) −0.0006 (11) −0.0004 (11)
C11 0.0427 (14) 0.0453 (14) 0.0339 (14) 0.0244 (12) 0.0017 (11) 0.0003 (12)
C12 0.0361 (13) 0.0390 (13) 0.0406 (14) 0.0164 (11) 0.0013 (12) −0.0020 (12)
C13 0.0524 (16) 0.0557 (16) 0.0407 (14) 0.0272 (14) 0.0092 (13) 0.0006 (14)
C14 0.084 (2) 0.0603 (19) 0.072 (2) 0.0374 (17) 0.0398 (19) 0.0078 (17)

Geometric parameters (Å, º)

N1—C7 1.496 (3) C8—H8C 0.9800
N1—H1A 0.9100 O1—C9 1.260 (3)
N1—H1B 0.9100 O2—C9 1.244 (3)
N1—H1C 0.9100 C9—C10 1.513 (3)
C1—C2 1.382 (4) C10—C11 1.522 (4)
C1—C6 1.387 (3) C10—H10A 0.9900
C1—C7 1.518 (3) C10—H10B 0.9900
C2—C3 1.382 (4) C11—C12 1.519 (3)
C2—H2 0.9500 C11—H11A 0.9900
C3—C4 1.378 (4) C11—H11B 0.9900
C3—H3 0.9500 C12—C13 1.511 (4)
C4—C5 1.374 (4) C12—H12A 0.9900
C4—H4 0.9500 C12—H12B 0.9900
C5—C6 1.391 (4) C13—C14 1.520 (4)
C5—H5 0.9500 C13—H13A 0.9900
C6—H6 0.9500 C13—H13B 0.9900
C7—C8 1.519 (4) C14—H14A 0.9800
C7—H7 1.0000 C14—H14B 0.9800
C8—H8A 0.9800 C14—H14C 0.9800
C8—H8B 0.9800
C7—N1—H1A 109.5 H8B—C8—H8C 109.5
C7—N1—H1B 109.5 O2—C9—O1 124.2 (2)
H1A—N1—H1B 109.5 O2—C9—C10 117.4 (2)
C7—N1—H1C 109.5 O1—C9—C10 118.4 (2)
H1A—N1—H1C 109.5 C9—C10—C11 116.9 (2)
H1B—N1—H1C 109.5 C9—C10—H10A 108.1
C2—C1—C6 118.9 (2) C11—C10—H10A 108.1
C2—C1—C7 119.5 (2) C9—C10—H10B 108.1
C6—C1—C7 121.6 (2) C11—C10—H10B 108.1
C1—C2—C3 121.2 (3) H10A—C10—H10B 107.3
C1—C2—H2 119.4 C12—C11—C10 112.7 (2)
C3—C2—H2 119.4 C12—C11—H11A 109.0
C4—C3—C2 119.8 (3) C10—C11—H11A 109.0
C4—C3—H3 120.1 C12—C11—H11B 109.0
C2—C3—H3 120.1 C10—C11—H11B 109.0
C5—C4—C3 119.5 (3) H11A—C11—H11B 107.8
C5—C4—H4 120.2 C13—C12—C11 113.7 (2)
C3—C4—H4 120.2 C13—C12—H12A 108.8
C4—C5—C6 120.9 (3) C11—C12—H12A 108.8
C4—C5—H5 119.5 C13—C12—H12B 108.8
C6—C5—H5 119.5 C11—C12—H12B 108.8
C1—C6—C5 119.6 (3) H12A—C12—H12B 107.7
C1—C6—H6 120.2 C12—C13—C14 113.0 (2)
C5—C6—H6 120.2 C12—C13—H13A 109.0
N1—C7—C1 110.52 (17) C14—C13—H13A 109.0
N1—C7—C8 108.8 (2) C12—C13—H13B 109.0
C1—C7—C8 113.6 (2) C14—C13—H13B 109.0
N1—C7—H7 107.9 H13A—C13—H13B 107.8
C1—C7—H7 107.9 C13—C14—H14A 109.5
C8—C7—H7 107.9 C13—C14—H14B 109.5
C7—C8—H8A 109.5 H14A—C14—H14B 109.5
C7—C8—H8B 109.5 C13—C14—H14C 109.5
H8A—C8—H8B 109.5 H14A—C14—H14C 109.5
C7—C8—H8C 109.5 H14B—C14—H14C 109.5
H8A—C8—H8C 109.5
C6—C1—C2—C3 1.0 (4) C6—C1—C7—N1 −63.3 (3)
C7—C1—C2—C3 −179.6 (2) C2—C1—C7—C8 −120.0 (3)
C1—C2—C3—C4 −1.1 (4) C6—C1—C7—C8 59.4 (3)
C2—C3—C4—C5 0.5 (4) O2—C9—C10—C11 −152.0 (2)
C3—C4—C5—C6 0.3 (4) O1—C9—C10—C11 28.2 (3)
C2—C1—C6—C5 −0.3 (4) C9—C10—C11—C12 −177.9 (2)
C7—C1—C6—C5 −179.7 (2) C10—C11—C12—C13 −178.0 (2)
C4—C5—C6—C1 −0.4 (4) C11—C12—C13—C14 −175.4 (3)
C2—C1—C7—N1 117.3 (2)

Hydrogen-bond geometry (Å, º)

D—H···A D—H H···A D···A D—H···A
N1—H1A···O2i 0.91 1.84 2.753 (3) 176
N1—H1B···O1 0.91 1.87 2.768 (3) 167
N1—H1C···O1ii 0.91 1.82 2.714 (2) 168

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

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: MW2095).

References

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Associated Data

This section collects any data citations, data availability statements, or supplementary materials included in this article.

Supplementary Materials

Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536812045746/mw2095sup1.cif

e-68-o3335-sup1.cif (17.1KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812045746/mw2095Isup2.hkl

e-68-o3335-Isup2.hkl (72.1KB, hkl)

Supplementary material file. DOI: 10.1107/S1600536812045746/mw2095Isup3.cml

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


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