Surface mobility of molecular glasses and its importance in physical stability☆
Graphical abstract
Introduction
Glasses are amorphous materials that combine the mechanical strength of crystals and the spatial uniformity of liquids. Compared to crystals, glasses are more easily fabricated to be spatially homogeneous from macroscopic to nearly molecular dimensions. Such spatial uniformity is the basis for their wide applications in optics and contributes to the superior strength of metallic glasses [1], [2]. While better-known glasses are inorganic and polymeric, organic glasses of relatively low molecular weights (“molecular glasses”) are being explored for applications in drug delivery [3], [4], [5], bio-preservation [6], [7], and organic electronics [8], [9]. Pharmaceutical scientists take advantage of the high solubility of amorphous solids for the delivery of poorly soluble drugs.
An important subject in the study of molecular glasses is physical stability [5], [10], [11]. Glasses are non-equilibrium solids formed by cooling liquids, condensing vapors, or evaporating solutions while avoiding crystallization. A common feature of these processes is the kinetic arrest of a fluid structure. In glass formation by liquid cooling (Fig. 1), molecular motions slow down with falling temperature and eventually the system falls out of equilibrium at the so-called glass transition temperature Tg, forming a solid glass. Glasses are thermodynamically driven to crystallize and to “age” toward the equilibrium liquid state, both processes leading to changes in structure, properties, and performance.
A recent progress in understanding glass stability is the finding that molecular glasses have extremely high surface mobility and this property causes problems of poor stability and paradoxically, provides a tool for preparing glasses with vastly improved stability. Here we discuss this recent progress. Section 2 reviews recent measurements of surface diffusion on molecular glasses. Section 3 discusses the role of surface mobility in the physical stability of molecular glasses. We show that surface mobility is directly responsible for fast crystal growth on free surfaces, and may be involved in bulk crystal growth through the creation of voids and free surfaces. In vapor deposition, surface mobility allows efficient equilibration of newly deposited molecules and the formation of stable glasses with exceptionally low energy and high density. We also consider the methods for stabilizing molecular glasses against surface-facilitated transformations.
Section snippets
Surface mobility of molecular glasses
Recent experiments have shown that molecules on the free surface of an organic glass can be much more mobile than those in bulk. The experiments that led to this conclusion include the evolution of surface contours driven by surface tension [12], [13], [14], [15], [16] , the conductivity of ions implanted at different depths [17], the embedding of nano-particles [18], and the rotation of probe molecules [19]. The high mobility of surface molecules is qualitatively understood from their special
Surface mobility and its role in the stability of molecular glasses
If surface mobility is high, any process that requires molecular transport should be accelerated by a free surface. In this section, we consider the role of surface mobility in the crystallization of molecular glasses. Surface diffusion is directly linked to fast crystal growth at the free surface and may be partially responsible for fast crystal growth in the interior. We also consider the formation of stable glasses by vapor deposition as another consequence of surface mobility and briefly
Concluding remarks
Recent work has found that surface mobility can be extremely high on molecular glasses and play a key role in their physical stability. Surface mobility is directly linked to fast surface crystal growth and may be involved in bulk crystal growth through the creation of voids and free surfaces. Surface mobility is responsible for the formation of stable glasses by vapor deposition; in terms of density and energy, these glasses are equivalent to liquid-cooled glasses that have been aged for
Acknowledgment
I thank the National Science Foundation (DMR 1206724 and 1234320) for supporting this work and my coworkers for their contributions, including M. D. Ediger, Juan J. de Pablo, Lei Zhu, Ye Sun., Hanmi Xi, Caleb Brian, Wei Zhang, Tian Wu, Erica Gunn, Ting Cai, Mariko Hasebe, Danielle Musumeci, C. Travis Powell, and Yinshan Chen.
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This review is part of the Advanced Drug Delivery Reviews theme issue on “Amorphous pharmaceutical solids”.