Abstract

The freezing of aqueous solutions and reciprocal distribution of ice and a freeze-concentrated solution (FCS) are poorly understood in spite of their importance in fields ranging from biotechnology and life sciences to geophysics and climate change. Using an optical cryo-miscroscope and differential scanning calorimetry, we demonstrate that upon cooling of citric acid and sucrose solutions a fast freezing process results in a continuous ice framework (IF) and two freeze-concentrated solution regions of different concentrations, FCS1 and FCS2. The FCS1 is maximally freeze-concentrated and interweaves with IF. The less concentrated FCS2 envelops the entire IF/FCS1. We find that upon further cooling, the FCS1 transforms to glass, whereas the slow freezing of FCS2 continues until it is terminated by a FCS2-glass transition. We observe the resumed slow freezing of FCS2 upon subsequent warming. The net thermal effect of the resumed freezing and a reverse glass-FCS1 transition produces the Ttr2-transition which before has only been observed upon warming of frozen hydrocarbon solutions and which nature has remained misunderstood for decades.

Highlights

  • The freezing of aqueous solutions and reciprocal distribution of ice and a freeze-concentrated solution (FCS) are poorly understood in spite of their importance in fields ranging from biotechnology and life sciences to geophysics and climate change

  • Using an optical cryo-miscroscope and differential scanning calorimetry, we demonstrate that upon cooling of citric acid and sucrose solutions a fast freezing process results in a continuous ice framework (IF) and two freeze-concentrated solution regions of different concentrations, FCS1 and FCS2

  • We find that upon further cooling, the FCS1 transforms to glass, whereas the slow freezing of FCS2 continues until it is terminated by a FCS2-glass transition

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Summary

Introduction

The freezing of aqueous solutions and reciprocal distribution of ice and a freeze-concentrated solution (FCS) are poorly understood in spite of their importance in fields ranging from biotechnology and life sciences to geophysics and climate change. Upon freezing aqueous solutions separate into pure ice and a FCS which vitrifies[2,3,4,5,6,7,8,9,10,11,12] or freezes[13,14] upon further cooling This phase separation and FCS distribution within the ice play an important role in various natural, industrial and biotechnological processes. It is www.nature.com/scientificreports believed that freezing produces ice crystals embedded and dispersed in a matrix of glassy and/or crystallized FCS2,3,33–37 Such seeming picture of ice/FCS morphology cannot account for the appearance of two transitions, Ttr[1] and Ttr[2], calorimetrically observed upon warming of frozen carbohydrate solutions[9,10,11,12,29,30,31,38,39]. The obtained OC-M and DSC results are mutually complementary and give a clear picture of the freezing process and formed ice/FCS morphology

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