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Glass transition and fragility in the simple molecular glassformer CS2 from CS2–S2Cl2 solution studies

机译:CS2–S2Cl2溶液研究中的简单分子玻璃形成剂CS2中的玻璃化转变和易碎性

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With an interest in finding the fragility for a simple, single component, molecular glassformer, we have determined the dielectric relaxation and glass transition behavior for a series of glasses in the CS2–S2Cl2 and CS2-toluene systems. Crystallization of CS2 can be completely avoided down to the composition 20 mol% second component, and the fragility proves almost independent of CS2 content in each system. Since the glass temperature Tg obtained from both thermal studies and from dielectric relaxation using Tg,diel=T=100 s is quite linear over the whole composition range in each system, and since relaxation time data for pure CS2 fall on the same master plot when scaled by the linearly extrapolated Tg value, we deduce that pure CS2 has the same high fragility as the binary solutions. The value is m=86, as for ortho-terphenyl OTP. Based on observations of independent studies for the vibrational density of states VDoS of inherent structures for OTP and instantaneous, at-temperature structures for CS2, we attribute the high fragility to an excess vibrational heat capacity defined by Cp vib, excess=dSvib, excess/d ln T originating in the behavior of the low frequency modes of the VDoS the boson peak modes. Both low frequency DoS and anharmonicity increase with increasing temperature, augmenting the configurational entropy drive to the top of the system energy landscape. The surprising implication is that fragility is determined in the vibrational, not configurational, manifold of microstates.
机译:为了发现简单的单组分分子玻璃形成剂的脆性,我们确定了CS2-S2Cl2和CS2-甲苯系统中一系列玻璃的介电弛豫和玻璃化转变行为。直到成分20摩尔%的第二组分,都可以完全避免CS2的结晶,而脆性几乎与每个系统中CS2的含量无关。由于从热研究和使用Tg的介电弛豫获得的玻璃温度Tg,在每个系统的整个组成范围内,diel = T = 100 s都是线性的,并且由于纯CS2的弛豫时间数据落在相同的主图中根据线性外推的Tg值换算,我们推论纯CS2具有与二元解相同的高脆性。对于邻三苯基OTP,该值是m = 86。基于对OTP固有结构和CS2瞬时温度结构的状态振动密度VDoS的独立研究的观察结果,我们将高脆性归因于由Cp vib定义的过大振动热容,excess = dSvib,excess / d ln T源于VDoS的低频模式的玻色子峰值模式。低频DoS和非谐波都随温度升高而增加,从而将配置熵驱动增大到系统能量格局的顶部。令人惊讶的含义是,脆性是由振动的,而不是构型的微状态决定的。

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