This
paper examines
the pressure effect on the crystallization
rate of the pharmaceutically active enantiomerically pure S-enantiomer
and the racemic mixture of the well-known drug ibuprofen. Performed
experimental studies revealed that at ambient pressure
S
-ibuprofen crystallizes faster than the racemic mixture. When the
pressure increases, the crystallization rate slows down for both systems,
but interestingly it is more apparent in the case of the S-enantiomer.
It is found that this experimentally observed trend can be understood
based on the predictions of the classical nucleation theory. We suggest
that the solid–liquid interfacial free energy is the main reason
for the observed variations in
S
- and
RS
-ibuprofen’s stability behaviors. Employing a special method
of computational studies, i.e., the capillary fluctuation method,
we show that the increase in pressure affects the solid–liquid
interfacial free energy for
S
- and
RS
-ibuprofen in an entirely different way. Importantly, the detected
differences correspond to the experimentally observed variations in
the overall crystallization rates.
In this paper, we examine the crystallization tendency for two quasi-real systems, which differ exclusively in the dipole moment's value. The main advantage of the studied system is the fact that despite that their structures are entirely identical, they exhibit different physical properties. Hence, the results obtained for one of the proposed model systems cannot be scaled to reproduce the results for another corresponding system, as it can be done for simple model systems, where structural differences are modeled by the different parameters of the intermolecular interactions. Our results show that both examined systems exhibit similar stability behavior below the melting temperature. This finding is contrary to the predictions of the classical nucleation theory, which suggests a significantly higher crystallization tendency for a more polar system. Our studies indicate that the noted discrepancies are caused by the kinetic aspect of the classical nucleation theory, which overestimates the role of diffusion in the nucleation process.
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