Due to their unique glass-forming tendency, carbohydrate-based solutions introduce certain challenges during desiccation. Depending on various factors such as their chemical properties, the glass transition temperature and the surface interactions nonhomogeneities within the drying solution arise. These effects range from the formation of very sharp concentration gradients within the processed product (the biopreservation solution containing the macromolecules, cells, etc. to be preserved) to cracking, which physically destroys the product. We are interested in engineering carbohydrate solutions to decrease the molecular mobility around proteins, membranes and in biological systems for preservation purposes.
Just to give a simple example to the instabilities encountered during drying of sessile droplets, let’s look at two droplets of identical initial volume (200 nl) and identical initial sugar concentration (Ci=15% w/w). The droplets are deposited on the surface of a quartz crystal and are being dried diffusively (please click on the images for the movies). As seen in the movies, the apex height of the trehalose droplet decreases gradually during desiccation, while for the dextran droplet the response is quite complicated (for detailed examination of the phenomena, see Aksan, et al. Langmuir, 2005).
Molecular Mobility
For a supersaturated solution, crystallization is the energetically most favorable path. However, if the concentration increases very rapidly (or the temperature drops very fast) a meta-stable “glassy” state can be reached. For a glass-forming system, the transition from a dilute to a concentrated solution diffusion mechanism is determined by the concentration corresponding to the cross-over temperature, Tc, predicted by the Mode Coupling Theory. At the cross-over temperature there is a transition from liquid-like to solid-like dynamics. Note that Tc~(1.14-1.6)Tg for most glass-forming solutions, where Tg is the glass-transition temperature. Diffusion in very high concentration solutions (close to glass transition temperature) is governed by the frequency of jumping between the cages surrounding the tagged molecule (either the solvent or a small solute) and is comparable to the time the molecule spends entrapped in the cage rattling (ß-relaxation). This is similar to the mechanism of diffusion in crystalline systems, where the diffusing molecule jumps between the crystal defects (vacancies). Frequency of jumping is inversely related to the structural relaxation (a-relaxation) time, of the matrix. Temperature dependence of distinguishes between the “fragile” and “strong” glasses, where the variation in with temperature is steeper in the former case.
We are interested in engineering carbohydrate solutions to decrease the molecular mobility around proteins, membranes and in biological systems for preservation solutions.
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