Dynamics of Uncrystallized Water, Ice, and Hydrated Protein in Partially Crystallized Gelatin–Water Mixtures Studied by Broadband Dielectric Spectroscopy

Динамика некристаллизованной воды, льда и гидратированного белка в частично кристаллизованных смесях желатин–вода, изученная широкополосной диэлектрической спектроскопией
Apostolos Kyritsis, P. Pissis, Kaito Sasaki, Άννα Παναγοπούλου, Rio Kita‬, Naoki Shinyashiki, Shin Yagihara
2016-12-14

Arrhenius to non-Arrhenius transitionbroadband dielectric spectroscopydielectric relaxation processesgelatin–water mixturesglass transitionhydration shellsice Ihuncrystallized water
The glass transition of partially crystallized gelatin-water mixtures was investigated using broadband dielectric spectroscopy (BDS) over a wide range of frequencies (10 mHz to 10 MHz), temperatures (113-298 K), and concentrations (10-45 wt %). Three dielectric relaxation processes (processes I, II, and III) were clearly observed. Processes I, II, and III originate from uncrystallized water (UCW) in the hydration shells of gelatin, ice, and hydrated gelatin, respectively. A dynamic crossover, called the Arrhenius to non-Arrhenius transition of UCW, was observed at the glass transition temperature of the relaxation process of hydrated gelatin for all mixtures. The amount of UCW increases with increasing gelatin content. However, above 35 wt % gelatin, the amount of UCW became more dependent on the gelatin concentration. This increase in UCW causes a decrease in the glass transition temperature of the cooperative motion of gelatin and UCW, which appears to result from a change in the aggregation structure of gelatin in the mixture at a gelatin concentration of approximately 35 wt %. The temperature dependence of the relaxation time of process II has nearly the same activation energy as pure ice made by slow crystallization of ice Ih. This implies that process II originates from the dynamics of slowly crystallized ice Ih.
1
A dynamic crossover (Arrhenius to non-Arrhenius transition) of UCW occurs at the glass transition temperature of the hydrated gelatin relaxation for all mixtures.
2
Broadband dielectric spectroscopy (10 mHz–10 MHz, 113–298 K, 10–45 wt%) revealed three distinct dielectric relaxation processes (I, II, III) in partially crystallized gelatin–water mixtures.
3
Increasing UCW lowers the glass transition temperature of the cooperative gelatin–UCW motion, likely due to a change in gelatin aggregation structure around 35 wt% concentration.
4
Process I originates from uncrystallized water (UCW) in gelatin hydration shells, process II from ice (slowly crystallized ice Ih), and process III from hydrated gelatin.
5
The activation energy of process II closely matches that of pure ice formed by slow crystallization as ice Ih, supporting assignment of process II to slowly crystallized ice Ih dynamics.
6
The amount of uncrystallized water increases with gelatin content, with a pronounced concentration dependence above ~35 wt% gelatin.

Partially crystallized gelatin–water mixtures with their constituent uncrystallized water, ice (ice Ih), and hydrated gelatin

Dynamics and glass-transition behavior of uncrystallized water (UCW), ice (process II), and hydrated protein (gelatin) probed via broadband dielectric relaxation (processes I–III), including Arrhenius-to-non‑Arrhenius crossover, UCW amount dependence on gelatin concentration, and effects on cooperative motion and aggregation structure around ~35 wt% gelatin

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2016-12-14
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Apostolos Kyritsis
P. Pissis
Kaito Sasaki
Άννα Παναγοπούλου
Rio Kita‬
Naoki Shinyashiki
Shin Yagihara
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