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首页> 外文期刊>High Pressure Research >Viscosity, relaxation time, glass temperature, melting temperature and fragile-to-strong transition parameterizations at extreme pressures in soft-matter systems
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Viscosity, relaxation time, glass temperature, melting temperature and fragile-to-strong transition parameterizations at extreme pressures in soft-matter systems

机译:在软物质系统中,在极端压力下的粘度,弛豫时间,玻璃温度,熔融温度和易碎到强烈的过渡参数设置

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摘要

This contribution presents the extended, pressure-related Vogel-Fulcher-Tammann equation applied to portray the pressure evolution of viscosity η(P) and the related dynamic properties, such as the primary relaxation time τ(P), in soft-matter systems as well as the modified Simon-Glatzel-type equation for describing pressure dependences of the glass temperature T_g(P), the melting temperature T_m(P) and the fragile-to-strong dynamical transition in confined water T_d(P). Both equations are capable of penetrating the negative pressure (isotropically stretched liquid) domain, and at very high pressures are capable of the inverse behavior. They have the following forms: (i) η(P) = η0 exp[D_PΔP/(p_0 - P)] = η0 exp[(D_P - D_PP_(SL))/(P_0 - P)], where P_0 is the estimate of the ideal glass temperature, P_(SL) is for the stability limit at negative pressures and D_P denotes the pressure fragility strength coefficient and (ii) T_(g,m,d)(P) = (T_(g,m,d))~0(1 + (P - (P_(g,m,d)~0/(π + (P_(g,m,d)~0))) exp(-(P - (P_(g,m,d))~0)/c), where (T_(g,m,d))~0 and (P_(g,m,d))~0 are the reference temperature and pressure, -π is the negative pressure asymptote and c is the damping coefficient responsible for the inversion phenomenon.
机译:该贡献提出了与压力有关的扩展的Vogel-Fulcher-Tammann方程,用于描述软物质系统中的粘度η(P)的压力演化以及相关的动力学特性,例如主弛豫时间τ(P),如下所示:以及用于描述玻璃温度T_g(P),熔融温度T_m(P)和承压水T_d(P)中的从弱到强的动力转变的压力依赖性的改进的Simon-Glatzel型方程。这两个方程都能够穿透负压(各向同性拉伸的液体)域,而在非常高的压力下则具有逆行为。它们具有以下形式:(i)η(P)=η0exp [D_PΔP/(p_0-P)] =η0exp [(D_P-D_PP_(SL))/(P_0-P)],其中P_0是估计值理想玻璃温度的P_(SL)是负压下的稳定性极限,D_P表示压力脆性强度系数,并且(ii)T_(g,m,d)(P)=(T_(g,m,d ))〜0(1 +(P-(P_(g,m,d)〜0 /(π+(P_(g,m,d)〜0)))exp(-(P-(P_(g, m,d))〜0)/ c),其中(T_(g,m,d))〜0和(P_(g,m,d))〜0为参考温度和压力,-π为负压力渐近线,c是引起反演现象的阻尼系数。

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