CHEMPLUSCHEM
COMMUNICATIONS
according to the P2 and P3 Hooft parameters (see Ta-
ble SI1). Using the same procedure, the five confor-
mations of (+)-MQ-2 have an absolute configuration
of (11S, 12R) with the same probability (x=À0.03(13)
and y=0.03(4)).
In the two (À)-MQ-1 and (+)-MQ-2 bases, mole-
cules A to E possess nearly identical conformations,
the main difference being in the rotation of the pi-
peridine ring about the C11ÀC12 bond (see Fig-
ure SI1). The quinoline fragments of each MQ mole-
cule are approximately planar (RMSD from 0.016 to
0.030 ꢂ), with carbon C3A, C3B, C4C, C3D, and C4E
showing the maximum deviations from planarity of
the quinolone rings, in the range from 0.030(4) to
0.051(4) ꢂ. The piperidine ring assumes a chair con-
formation with atoms N13, C17, C16, and C14 copla-
nar such that the root mean square deviations from
the average plane through these four atoms are of
0.0016/0.0037, 0.0095/0.00134, 0.0010/0.0008, 0.0040/
0.0004, and 0.0090/0.0144 ꢂ for molecules A, B, C, D,
and E, for (À)-MQ-1 and (+)-MQ-2, respectively. The
aryl group lies equatorial to the piperidine ring, with
the angle between the average plane of the quino-
line ring and the average plane of the piperidine ring
Figure 2. Chromatogram illustrating the enantiomeric purity of the two erythro enantio-
mers of mefloquine after chromatographic purification. Column: Chiralpak IA
(250ꢃ4.6 mm); mobile phase: heptane/isopropanol/diethylamine (70:30:0.1); detection:
280 nm; flow rate: 1.0 mLminÀ1; retention times: (À)-(11R, 12S)-erythro-MQ-1: 4.77 min
and the (+)-(11S, 12R)-erythro-MQ-2: 9.02 min.
ranging from 79.3(2) to 92,4(2)8 for (À)-MQ-1 and from 79.3(2)
to 88.9(2)8 for (+)-MQ-2. The À58.6(4) to À72.0(4)8 range of
torsion angles for the atoms comprising O1-C11-C12-N13 dem-
onstrates that (À)-MQ-1 is gauche about the C12ÀC13 bond,
whereas the same torsion angles in (+)-MQ-2 were found
ranging from 58.2(4) to 72.5(5)8. The C4-C11-C12-N13 torsion
angles of 164.5(3)8, 179.2(3)8, 168.1(3)8, 171.7(3)8, and 177.7(3)8
for the five conformers of (À)-MQ-1 place the amine group
nearly as far away as possible from the quinoline ring. In
(+)-MQ-2, the same C4-C11-C12-N13 torsion angles were ob-
served at À163.6(4)8, À179.7(4)8, À168.5(4)8, À172.(4)8, and
À177.0(3)8 leading to the same observations.
The main role in the packing of MQ molecules in the two
structures studied is played by OÀH···N intermolecular hydro-
gen bonds (see Table SI2). There are no solvent-accessible
voids in the crystal lattice of the MQ molecules. Crystal cohe-
sion is ensured by a monodimensional network of hydrogen
bonds within the 010 crystallographic direction completed by
van der Waals interactions in other directions that essentially
involve the fluorine atoms.
Figure 3. ORTEP views of the molecular structure of (a) (À)-MQ-1 and
(b) (+)-MQ-2 bases with our numbering Scheme for one of the five mole-
cules in the asymmetric unit (molecule A). The numbering scheme for the
other four molecules is the same but the suffix is b, c, d, and e for B, C, D,
and E molecules, respectively. Displacement ellipsoids are drawn at the 30%
probability level.
Geometry optimizations along with frequency calculations
were performed in the gas phase on the two MQ molecules at
the B3LYP/6-31+G* level of theory using the structures ob-
tained by X-ray crystallography as starting points. For both MQ
molecules, the optimized geometries are very close to their
corresponding crystallographic states, indicating local minima.
Moreover, the energies of the two structures are identical im-
plying that the two MQ are “true” enantiomers, as shown in
Figure 5. To check whether these obtained structures are
global minima, additional analyses including conformational
search were carried out. Results show that the crystallographic
structure of (+)-MQ-2 is the actual global minimum of the
(11S, 12R) enantiomer, whereas calculations indicate that the
structures are given in the Table SI1 (see the Supporting Infor-
mation).
The absolute configurations of (À)-1 and (+)-MQ-2 were es-
tablished through single-crystal X-ray crystallography. The ab-
solute configuration of (À)-MQ-1 was determined by observing
and calculating the F(+)/F(À) ratios of Bijvoet pairs with the
mean F value of each independent reflection, and by determin-
ing the Flack factor value (x=0.08(11)).[11] In addition, the
Hooft parameter was determined by using Bayesian statistics
on Bijvoet differences (y=0.04(5)).[12] Based on these results,
the absolute configurations at C11 and C12 were determined
to be R and S, respectively, with a probability close to 100%
ꢁ 2013 Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim
ChemPlusChem 2013, 78, 642 – 646 643