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Acta Cryst. (2008). E64, o559    [ doi:10.1107/S1600536808003516 ]

(R)-1-Phenylethanaminium (S)-4-chloromandelate

Q. He, M. C. Jennings, S. Rohani, J. Zhu and H. Gomaa

Abstract top

The absolute configuration of the title complex, C8H12N+·C8H6ClO3- or [R-C6H5C(H)CH3NH3][S-4-ClC6H4C(H)(OH)CO2], has been confirmed by the structure determination. In the crystal structure, intermolecular O-H...O and N-H...O hydrogen bonds form a two-dimensional network perpendicular to the c axis.

Comment top

In our previous work, phenylethylamine (PEA) has been proven to be an efficient resolving agent for resolution of racemic 4-chloromandelic acid. In order to further investigate the chiral recognition mechanism, the single-crystal structure of the corresponding more soluble salt, (R)-Phenylethylammonium (S)-4-chloromandelate, is reported here for comparison with that of the less soluble salt (R)-Phenylethylammonium (R)-4-chloromandelate (He et al., 2007).

The title complex consists of an ion pair; an amine cation and a carboxylate anion (see Fig. 1). The absolute stereochemistry of each ion has been confirmed by the structure determination [absolute structure parameter -0.03 (8); (Flack, 1983)]. All three H atoms of the –NH3 group and the H atom of the O—H group act as hydrogen bond donors in intermolecular O—H···O and N—H···O hydrogen bonds, forming a two-dimensional network perpendicular to the c axis. The hydrogen bond motif in the title compound is different to that observed in the room temperature structure of the R,R diastereomer (He et al., 2007).

Related literature top

For background information and the crystal structure of the R,R diastereomer of the title compound, see: He et al. (2007).

Experimental top

To a solution (S)-4-chloromandelate (2.0 g, 0.01 mol) in 10 ml 2-propanol, (1.3 mL, 0.01 mol), (R)-Phenylethylammonium, was added gradually. A white crystalline solid appeared. The crystals were collected and washed with 2-propanol twice to give the title compound (1.85 g), yield 56%. Single crystals were grown from a concentrated methanol solution of the title compound by slow evaporation at room temperature.

Refinement top

All H atoms were positioned geometrically and constrained as riding atoms with; C—H = 1.00Å and Uiso(H) = 1.2Ueq(C) for methyne H atoms, C—H = 0.98Å and Uiso(H) = 1.5Ueq(C) for methyl H atoms, C—H = 0.95Å and Uiso(H) = 1.2Ueq(C) for aromatic H atoms, O—H = 0.84Å and Uiso(H) = 1.5Ueq(C) for hydroxyl H atoms and N—H = 0.91Å and Uiso(H) = 1.5Ueq(C) for amine H atoms.

Computing details top

Data collection: COLLECT (Nonius, 1997); cell refinement: DENZO-SMN (Otwinowski & Minor, 1997); data reduction: DENZO-SMN (Otwinowski & Minor, 1997); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: SHELXTL/PC (Sheldrick, 2008); software used to prepare material for publication: SHELXTL/PC (Sheldrick, 2008).

Figures top
[Figure 1] Fig. 1. The molecular structure of the title compound with 30% probability displacement ellipsoids and the atom labelling scheme.
(R)-1-Phenylethanaminium (S)-4-chloromandelate top
Crystal data top
C8H12N+·C8H6ClO3–F000 = 324
Mr = 307.76Dx = 1.295 Mg m−3
Monoclinic, P21Mo Kα radiation
λ = 0.71073 Å
Hall symbol: P 2ybCell parameters from 11634 reflections
a = 10.4091 (7) Åθ = 2.0–27.5º
b = 5.7635 (4) ŵ = 0.25 mm−1
c = 13.2544 (10) ÅT = 150 (2) K
β = 96.831 (4)ºPlate, colourless
V = 789.52 (10) Å30.45 × 0.15 × 0.08 mm
Z = 2
Data collection top
Nonius KappaCCD
diffractometer		3431 independent reflections
Radiation source: fine-focus sealed tube2881 reflections with I > 2σ(I)
Monochromator: graphiteRint = 0.072
T = 150(2) Kθmax = 27.5º
φ scans, and ω scans with κ offsetsθmin = 2.4º
Absorption correction: multi-scan
(SORTAV; Blessing, 1995)		h = −13→13
Tmin = 0.787, Tmax = 0.984k = −7→7
7943 measured reflectionsl = −16→17
Refinement top
Refinement on F2Hydrogen site location: inferred from neighbouring sites
Least-squares matrix: fullH-atom parameters constrained
R[F2 > 2σ(F2)] = 0.044  w = 1/[σ2(Fo2) + (0.0565P)2 + 0.1172P]
where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.115(Δ/σ)max < 0.001
S = 1.05Δρmax = 0.26 e Å−3
3431 reflectionsΔρmin = −0.30 e Å−3
192 parametersExtinction correction: none
1 restraintAbsolute structure: Flack (1983), 1436 Fridel pairs
Primary atom site location: structure-invariant direct methodsFlack parameter: −0.03 (8)
Secondary atom site location: difference Fourier map
Crystal data top
C8H12N+·C8H6ClO3–V = 789.52 (10) Å3
Mr = 307.76Z = 2
Monoclinic, P21Mo Kα
a = 10.4091 (7) ŵ = 0.25 mm−1
b = 5.7635 (4) ÅT = 150 (2) K
c = 13.2544 (10) Å0.45 × 0.15 × 0.08 mm
β = 96.831 (4)º
Data collection top
Nonius KappaCCD
diffractometer		3431 independent reflections
Absorption correction: multi-scan
(SORTAV; Blessing, 1995)		2881 reflections with I > 2σ(I)
Tmin = 0.787, Tmax = 0.984Rint = 0.072
7943 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.044H-atom parameters constrained
wR(F2) = 0.115Δρmax = 0.26 e Å−3
S = 1.05Δρmin = −0.30 e Å−3
3431 reflectionsAbsolute structure: Flack (1983), 1436 Fridel pairs
192 parametersFlack parameter: −0.03 (8)
1 restraint
Special details top

Experimental. Absorption correction: multi-scan from symmetry-related measurements (SORTAV; Blessing, 1995). M.p. 140.8–142.5 K. The specific rotation was [α]25D = +50.5° (c=1, C1H3OH), determined using a Perkin Elmer Model 341 Digital Polarimeter; 1H-NMR (d6-DMSO/TMS): δ 1.424 (d, 3H, CH3), 4.300 (m, 1H, CHNH2), 4.536 (s, 1H, CHOH), 7.268–7.457 (m, 9H, C6H5 and C6H4Cl) measured using an INOVA 400 MHz NMR (Varian).

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
Cl10.62566 (7)0.61666 (16)1.01588 (5)0.0611 (3)
C20.6271 (2)0.5894 (5)0.88508 (17)0.0393 (6)
C30.5788 (3)0.7663 (5)0.82206 (19)0.0435 (6)
H3A0.54080.89900.84900.052*
C40.5863 (2)0.7484 (4)0.71887 (18)0.0368 (5)
H4A0.55290.87020.67510.044*
C50.64141 (18)0.5567 (4)0.67818 (16)0.0260 (4)
C60.6887 (2)0.3804 (4)0.74326 (19)0.0359 (5)
H6A0.72670.24730.71650.043*
C70.6815 (2)0.3952 (5)0.84688 (19)0.0422 (6)
H7A0.71370.27300.89090.051*
C80.64285 (18)0.5435 (3)0.56394 (15)0.0246 (4)
H8A0.65740.70330.53820.030*
O90.52152 (12)0.4619 (3)0.51580 (11)0.0287 (3)
H9A0.47010.57400.50530.043*
C100.74941 (19)0.3868 (4)0.53386 (15)0.0249 (4)
O110.72224 (14)0.1839 (3)0.50678 (13)0.0345 (4)
O120.86102 (13)0.4771 (3)0.53936 (11)0.0299 (3)
N130.87681 (16)−0.1239 (3)0.42117 (14)0.0269 (4)
H13A0.8657−0.25870.45480.040*
H13B0.8332−0.00760.44870.040*
H13C0.9625−0.08850.42670.040*
C140.6876 (2)−0.2471 (5)0.30409 (19)0.0395 (6)
H14A0.6898−0.40750.32880.059*
H14B0.6480−0.24300.23320.059*
H14C0.6366−0.15170.34580.059*
C150.8256 (2)−0.1521 (4)0.31099 (16)0.0296 (5)
H15A0.82230.00450.27830.035*
C160.91365 (19)−0.3052 (4)0.25701 (17)0.0278 (5)
C170.9388 (2)−0.2491 (4)0.15998 (17)0.0348 (5)
H17A0.9041−0.11030.12920.042*
C181.0142 (2)−0.3926 (5)0.10662 (18)0.0425 (6)
H18A1.0293−0.35360.03940.051*
C191.0672 (2)−0.5923 (5)0.15193 (19)0.0400 (6)
H19A1.1194−0.69030.11600.048*
C201.0443 (2)−0.6496 (4)0.24955 (19)0.0376 (6)
H20A1.0815−0.78590.28100.045*
C210.9671 (2)−0.5080 (4)0.30114 (17)0.0325 (5)
H21A0.9502−0.54950.36770.039*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Cl10.0659 (5)0.0910 (7)0.0280 (3)−0.0131 (4)0.0120 (3)−0.0052 (4)
C20.0348 (12)0.0566 (15)0.0273 (11)−0.0126 (12)0.0076 (9)−0.0033 (12)
C30.0474 (15)0.0465 (15)0.0389 (14)0.0067 (12)0.0141 (11)−0.0070 (13)
C40.0438 (13)0.0333 (12)0.0342 (12)0.0085 (11)0.0089 (10)−0.0005 (10)
C50.0202 (9)0.0275 (11)0.0311 (10)−0.0025 (8)0.0058 (8)−0.0028 (9)
C60.0376 (12)0.0329 (11)0.0383 (13)0.0040 (10)0.0094 (10)0.0050 (11)
C70.0415 (13)0.0485 (15)0.0366 (13)0.0003 (12)0.0048 (10)0.0083 (12)
C80.0202 (9)0.0239 (10)0.0299 (11)−0.0023 (8)0.0035 (8)−0.0004 (8)
O90.0199 (7)0.0278 (8)0.0376 (9)0.0015 (6)0.0000 (6)−0.0031 (7)
C100.0223 (9)0.0273 (11)0.0256 (10)0.0011 (8)0.0052 (8)0.0004 (9)
O110.0290 (8)0.0286 (8)0.0474 (10)−0.0002 (6)0.0104 (7)−0.0071 (7)
O120.0208 (7)0.0323 (8)0.0373 (8)−0.0001 (6)0.0067 (6)0.0026 (7)
N130.0233 (8)0.0258 (9)0.0325 (9)0.0003 (7)0.0066 (7)−0.0027 (8)
C140.0272 (11)0.0549 (15)0.0361 (13)0.0034 (11)0.0029 (9)−0.0099 (12)
C150.0290 (11)0.0321 (12)0.0284 (11)0.0066 (9)0.0063 (9)0.0001 (9)
C160.0226 (10)0.0298 (11)0.0314 (11)−0.0001 (8)0.0051 (8)−0.0043 (9)
C170.0373 (12)0.0359 (12)0.0320 (12)0.0035 (10)0.0070 (9)0.0021 (10)
C180.0429 (13)0.0526 (16)0.0344 (12)0.0052 (12)0.0145 (10)−0.0043 (12)
C190.0304 (11)0.0468 (15)0.0442 (14)0.0054 (10)0.0105 (10)−0.0116 (12)
C200.0338 (12)0.0358 (13)0.0432 (14)0.0078 (10)0.0040 (10)−0.0038 (11)
C210.0340 (11)0.0343 (12)0.0305 (12)0.0038 (10)0.0087 (9)0.0003 (10)
Geometric parameters (Å, °) top
Cl1—C21.743 (2)N13—H13B0.9100
C2—C31.375 (4)N13—H13C0.9100
C2—C71.378 (4)C14—C151.530 (3)
C3—C41.383 (3)C14—H14A0.9800
C3—H3A0.9500C14—H14B0.9800
C4—C51.384 (3)C14—H14C0.9800
C4—H4A0.9500C15—C161.512 (3)
C5—C61.385 (3)C15—H15A1.0000
C5—C81.518 (3)C16—C171.381 (3)
C6—C71.387 (3)C16—C211.393 (3)
C6—H6A0.9500C17—C181.390 (3)
C7—H7A0.9500C17—H17A0.9500
C8—O91.425 (2)C18—C191.382 (4)
C8—C101.520 (3)C18—H18A0.9500
C8—H8A1.0000C19—C201.383 (3)
O9—H9A0.8400C19—H19A0.9500
C10—O111.246 (3)C20—C211.382 (3)
C10—O121.267 (2)C20—H20A0.9500
N13—C151.503 (3)C21—H21A0.9500
N13—H13A0.9100
C3—C2—C7121.1 (2)H13A—N13—H13C109.5
C3—C2—Cl1119.5 (2)H13B—N13—H13C109.5
C7—C2—Cl1119.4 (2)C15—C14—H14A109.5
C2—C3—C4119.1 (2)C15—C14—H14B109.5
C2—C3—H3A120.5H14A—C14—H14B109.5
C4—C3—H3A120.5C15—C14—H14C109.5
C3—C4—C5121.3 (2)H14A—C14—H14C109.5
C3—C4—H4A119.3H14B—C14—H14C109.5
C5—C4—H4A119.3N13—C15—C16110.97 (17)
C4—C5—C6118.5 (2)N13—C15—C14108.59 (18)
C4—C5—C8118.86 (19)C16—C15—C14112.37 (19)
C6—C5—C8122.64 (19)N13—C15—H15A108.3
C5—C6—C7121.0 (2)C16—C15—H15A108.3
C5—C6—H6A119.5C14—C15—H15A108.3
C7—C6—H6A119.5C17—C16—C21118.5 (2)
C2—C7—C6119.1 (2)C17—C16—C15119.8 (2)
C2—C7—H7A120.4C21—C16—C15121.69 (19)
C6—C7—H7A120.4C16—C17—C18121.0 (2)
O9—C8—C5110.47 (15)C16—C17—H17A119.5
O9—C8—C10108.78 (16)C18—C17—H17A119.5
C5—C8—C10112.68 (16)C19—C18—C17119.6 (2)
O9—C8—H8A108.3C19—C18—H18A120.2
C5—C8—H8A108.3C17—C18—H18A120.2
C10—C8—H8A108.3C18—C19—C20120.1 (2)
C8—O9—H9A109.5C18—C19—H19A120.0
O11—C10—O12125.27 (19)C20—C19—H19A120.0
O11—C10—C8119.05 (17)C21—C20—C19119.8 (2)
O12—C10—C8115.68 (18)C21—C20—H20A120.1
C15—N13—H13A109.5C19—C20—H20A120.1
C15—N13—H13B109.5C20—C21—C16121.0 (2)
H13A—N13—H13B109.5C20—C21—H21A119.5
C15—N13—H13C109.5C16—C21—H21A119.5
C7—C2—C3—C4−0.5 (4)C5—C8—C10—O1198.5 (2)
Cl1—C2—C3—C4176.8 (2)O9—C8—C10—O12155.95 (17)
C2—C3—C4—C5−0.1 (4)C5—C8—C10—O12−81.2 (2)
C3—C4—C5—C60.4 (3)N13—C15—C16—C17−139.6 (2)
C3—C4—C5—C8178.0 (2)C14—C15—C16—C1798.6 (2)
C4—C5—C6—C7−0.2 (3)N13—C15—C16—C2142.8 (3)
C8—C5—C6—C7−177.7 (2)C14—C15—C16—C21−79.0 (3)
C3—C2—C7—C60.8 (4)C21—C16—C17—C180.9 (3)
Cl1—C2—C7—C6−176.52 (19)C15—C16—C17—C18−176.8 (2)
C5—C6—C7—C2−0.4 (3)C16—C17—C18—C19−1.3 (4)
C4—C5—C8—O9−81.8 (2)C17—C18—C19—C200.5 (4)
C6—C5—C8—O995.7 (2)C18—C19—C20—C210.8 (3)
C4—C5—C8—C10156.32 (19)C19—C20—C21—C16−1.2 (3)
C6—C5—C8—C10−26.2 (3)C17—C16—C21—C200.4 (3)
O9—C8—C10—O11−24.4 (3)C15—C16—C21—C20178.1 (2)
Hydrogen-bond geometry (Å, °) top
D—H···AD—HH···AD···AD—H···A
O9—H9A···O9i0.842.262.939 (2)139
O9—H9A···O11i0.842.092.826 (2)146
N13—H13A···O12ii0.911.892.798 (2)172
N13—H13B···O110.911.832.731 (2)169
N13—H13C···O12iii0.911.882.779 (2)171
Symmetry codes: (i) −x+1, y+1/2, −z+1; (ii) x, y−1, z; (iii) −x+2, y−1/2, −z+1.
Table 1
Hydrogen-bond geometry (Å, °) top
D—H···AD—HH···AD···AD—H···A
O9—H9A···O9i0.842.262.939 (2)139
O9—H9A···O11i0.842.092.826 (2)146
N13—H13A···O12ii0.911.892.798 (2)172
N13—H13B···O110.911.832.731 (2)169
N13—H13C···O12iii0.911.882.779 (2)171
Symmetry codes: (i) −x+1, y+1/2, −z+1; (ii) x, y−1, z; (iii) −x+2, y−1/2, −z+1.
Acknowledgements top

This work was supported by Ningbo Nature Science Fund (grant Nos. 2005B100085 and 2005 A620017)

references
References top

Blessing, R. H. (1995). Acta Cryst. A51, 33–38.

Flack, H. D. (1983). Acta Cryst. A39, 876–881.

He, Q., Jennings, M. C., Rohani, S., Zhu, J. & Gomaa, H. (2007). Acta Cryst. E63, o4199–?.

Nonius (1997). COLLECT. Nonius BV, Delft, The Netherlands.

Otwinowski, Z. & Minor, W. (1997). Methods in Enzymology, Vol. 276, Macromolecular Crystallography, Part A, edited by C. W. Carter Jr & R. M. Sweet, pp. 307–326. New York: Academic Press.

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