4.7 Article

Insights into the Polymorphic Structures and Enantiotropic Layer-Slip Transition in Paracetamol Form III from Enhanced Molecular Dynamics

期刊

CRYSTAL GROWTH & DESIGN
卷 21, 期 2, 页码 886-896

出版社

AMER CHEMICAL SOC
DOI: 10.1021/acs.cgd.0c01250

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资金

  1. New York University Materials Research Science and Engineering Center (MRSEC) program of the National Science Foundation [DMR-1420073]
  2. National Science Foundation [CHE-1955381]
  3. Abbvie

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Reversible temperature-mediated solid phase changes, known as enantiotropic transformations, occur in many molecular crystals due to entropic contributions. Understanding and predicting these transformations are crucial, and molecular simulations were used in this study to elucidate the mechanism behind the enantiotropic layer-slip phase transformation in paracetamol form III. The results suggest that the transformation is driven by localized and dynamic disorder within the structure, rather than a perfect crystal-to-crystal transition. The orthorhombic form III-o structure exists as an entropy-stabilized collective ensemble average of various misaligned layer-slipped structures.
Y Reversible temperature-mediated solid phase changes, otherwise known as enantiotropic transformations, occur in many molecular crystals. These transformations take place as a result of the free-energy stabilization through entropic contributions at finite temperatures and can often have significant implications for the properties of crystalline solids. As such, understanding and predicting these transformations is of great importance. In this study, we utilize molecular simulations to elucidate the mechanism behind the enantiotropic layer-slip phase transformation between the orthorhombic and monoclinic versions of paracetamol form III (form III-m and III-o). Using standard molecular dynamics (MD) in addition to crystal adiabatic free-energy dynamics, an MD-based enhanced sampling approach for crystalline systems, we demonstrate that the transformation from the monoclinic form III-m to the orthorhombic form III-o is driven by localized and dynamic disorder within the structure rather than a perfect crystal-to-crystal transition. These results suggest that the orthorhombic form III-o structure does not exist as a perfect orthorhombic crystal with fully aligned layers, but rather, as an entropy-stabilized collective ensemble average of various misaligned layer-slipped structures. Overall, these simulation approaches, which explicitly treat dynamic structural disorder, allowed us to map out the free-energy landscape of this enantiotropic transformation as a function of temperature and extract critical insights into the underlying mechanism of the transformation.

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