M. Bitencourt, et al.
International Journal of Pharmaceutics 589 (2020) 119840
of the solvent (Beckmann, 2013; Gao et al., 2017). The most suitable
single crystals were removed from the crystallization solution and sto-
rage in coin capsules. To avoid evaporation of the solvent and conse-
quently amorphization of the crystals, they are covered by a thin layer
of vegetable oil. The coin capsules were kept at room temperature
protected from the light. Attempts to obtain sufficient pure poly-
data reduction and multi-scan method absorption correction. The
structures were solved by direct methods and refined by full-matrix
2
least squares on F using the SHELXL-2018/3 software (Sheldrick,
2015). All non-hydrogen atoms were found from the electronic density
map constructed by Fourier synthesis and refined with anisotropic
thermal parameters. All hydrogen atoms (with exception of the water
hydrogen atoms) were placed in idealized positions in a riding model
with fixed C—H (or N—H) bond lengths of 0.98, 0.93, 0.96, 0.97 and
crystalline BCZHCl·H
2
O for the characterization part and the com-
parative physicochemical studies were unsuccessful.
0
.98 Å for the amino, aromatic, methyl, methylene and methine groups,
2
.2.3. Buclizine monohydrochloride (BCZHCl)
respectively. The isotropic thermal parameters of all hydrogens (except
the water hydrogens) depended on the equivalent isotropic thermal
displacements of the atoms bonded to them [Uiso(H) = 1.2Ueq(N-
amino, C-aromatic, C-methylene, C-methine) or 1.5Ueq(C-methyl)]. In
To obtain BCZHCl polycrystalline material, 1.0 g of the raw material
(
BCZH
2
Cl ) was solubilized at room temperature (25 °C) in 500 mL of a
2
methanol:water mixture (1:1, v:v). The solution was sonicated for
-
1
1
0 min followed by neutralization with drops of 1.0 mol L NaOH
the low temperature (150 K) structure of BCZHCl·H O, electron density
2
solution until it became cloudy, which took place at approximately pH
peaks corresponding to positions of the water hydrogen atoms were
identified and assigned at approximately 1 Å from the oxygen atom
(O1). Their positions (distances) nonetheless were restrained using
DFIX (O1-H1/O1-H2 = 0.84(2) Å) and DANG (H1-H2 = 1.34(4) Å)
instructions (Sheldrick, 2015), with Uiso(H1/H2) values = 1.5Ueq
(O1). For the room temperature (293 K) dataset, one of the water hy-
drogens is shared between the water oxygen and the amino nitrogen
(assigned in accordance with residual peaks without distance re-
straints), giving a final model after occupancy refinement of 23%
water/77% buclizine monohydrochloride and 77% hydroxide ion/23%
buclizine dihydrochloride. As previously observed for BCZ analogous
structures (Deb et al, 2015; Mohanty et al., 2015; Song et al, 2012), the
chlorine atom (Cl1) of 1-[(4-chlorophenyl)(phenyl)methyl]piper-
azinediium moiety was disordered over the two-symmetric benzene
carbon atoms (C1 and C11, Scheme 1). In all structures, the chlorine
atom was disordered over the Cl1-C1/Cl1-C11′ positions, with refined
site-occupation factors of 0.835(4)/0.165(4) (BCZHCl), 0.889(6)/
4
.8. As expected, this pH is at the middle of the pH range between the
two calculated BCZ pKa values (pKa1 = 2.12 and pKa2 = 6.55, See
section 3.3). The solution flask was capped with a parafilm layer
(
punctured with small holes) and stored without the direct incidence of
light. It is important to emphasize that the precipitate formed soon after
the BCZH Cl neutralization was amorphous (Figure S1, Supplementary
2
2
material). Crystalline BCZHCl without the presence of an amorphous
halo in the PXRD experiment was obtained by leaving the precipitate to
stand in contact with the stock solution for at least 10 days. In this way,
after 13 days, the precipitate on the flask bottom was separated from
the solution and dried in a desiccator containing silica for 24 h. The
generation of the BCZHCl form was confirmed by PXRD data (See
Discussion) and its chemical purity (99.6% +/- 0.3) attested by HPLC
analysis. The BCZHCl polycrystalline material was stored without the
direct incidence of light for the further analysis. The freshly prepared
BCZHCl polycrystalline material was also used in recrystallization
procedures in order to grow BCZHCl single-crystals that were good
enough for the single crystal X-ray experiment. After several attempts,
single-crystals were successfully obtained by vapor diffusion crystal-
lization method (Beckmann, 2013; Gao et al., 2017) as follow: ap-
proximately 2.0 mg of the BCZHCl form was dissolved in 0.5 mL of
acetone within a small open container (beaker of 10 mL), which was
placed in a larger container (vial of 50 mL) containing 2.5 mL of
chloroform. The outer container was sealed and the vapor chloroform
solution diffusion process into the acetone container was performed at
0
.111(6) (BCZHCl·H
2
O at 150 K) and 0.940(4)/0.060(4) (BCZHCl·H O
2
at 293 K). The occupancy factors were assigned using the free variables
and restraining the sum of them equal to 1.000 (FVAR SHELXL-2018/3
instruction) (Sheldrick, 2015). The Flack parameter for BCZHCl dataset
(
Cu radiation dataset) was reliably refined (Flack, 2003, 1983; Cianci
et al, 2005; Parsons and Flack, 2004) to 0.04(3) ((R)-isomer) using the
BASF/TWIN SHELXL-2018/3 instruction (Sheldrick, 2015). Refinement
of the Flack parameter for BCZHCl·H O datasets (both Mo radiation
2
datasets) at 150 K and 293 K was 0.08(16) and −0.03(10) respectively,
giving an inconclusive indication of the absolute structure, since the
standard uncertainty values are above 0.10. A favorable outcome was
obtained from the Bijvoet analysis reported by Hooft et al. (Hooft et al.,
2
5 °C. Plate-shaped colorless crystals were obtained after 15 days.
2
.2.4. Buclizine free-base (BCZ-FB)
2
008, 2010) and implemented in the PLATON program (Spek, 2009).
To obtain BCZ-FB polycrystalline material, 1.0 g of the raw material
was solubilized at 25 °C in 500 mL of ethanol:water (1:1, v:v) mixture.
However, due to the low Friedel coverage, this analysis was incon-
clusive for the low temperature dataset. The probability that the (R)-
isomer had been correctly assigned was 1.00 for either P2 (probability
assuming two possibilities, i.e. one enantiomer or the other) or P3
(probability assuming three possibilities, including the two possible
enantiomers plus the third option of a racemic twin). The resulting
value of the Hooft parameter y was 0.03(3). Therefore, since BCZHCl
-
1
After sonication for 10 min, 1.0 mol L NaOH solution was trickled into
the vial until pH 5.8 was reached (optimized value to produce BCZ-FB
absent of BCZHCl), which produced a significant amount of a white
colloidal precipitate. The remaining procedures were the same as those
applied to obtain the polycrystalline BCZH
2
2
Cl sample. The generation
of BCZ-FB was confirmed by HPLC (chemical purity of 99.5% +/-
and BCZHCl·H
2
O were solved respectively in the Pna2
1
and Pca2 polar
1
0
.01), PXRD, IR, DSC, and TGA data (See Discussion). Unfortunately,
several attempts using different crystal growth protocols to obtain BCZ-
FB single crystals that were good enough for a single-crystal X-ray
diffraction experiment were unsuccessful. Attempts to determine the
crystal structure of BCZ-FB from powder X-ray diffraction data were
also unsuccessful.
space groups (non-centrosymmetric space group containing mirror
planes), both are racemic crystals, so it obviously makes no sense to
establish the BCZ absolute configuration from the absolute structure.
The MERCURY (version 3.9) software program was used for crystal-
lographic analysis and artwork representations, in which the disorder
was omitted for the sake of clarity, i.e. only the chlorine atom with
highest site-occupation factors -linked to C1- was included. The crystal
data and details of data collection and refinement are shown in Table 1.
2.3. Single crystal X-ray diffraction analysis (SCXRD)
CCDC 1,912,183 (BCZHCl), CCDC 1,912,184 (BCZHCl·H O at 293 K)
2
Suitable BCZHCl·H O and BCZHCl single-crystals were previously
2
selected for the X-ray measurements. The data collections were per-
and CCDC 2,008,948 (BCZHCl·H O at 150 K) contain the supplemen-
2
TM
tary crystallographic data for this paper. The data can be obtained free
of charge from The Cambridge Crystallographic Data Centre (CCDC) via
www.ccdc.cam.ac.uk/getstructures. (Allen, 2002).
formed on an Agilent SuperNova diffractometer, equipped with dual
source of radiation (Cu and Mo) and an Atlas S2 CCD detector at 293
and 150 K (only for BCZHCl·H O crystal). The CrysalisPro software
2
(
Agilent, 2010) was used for data collection, unit cell determination,
3