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首页> 外文期刊>The journal of physical chemistry, B. Condensed matter, materials, surfaces, interfaces & biophysical >Phase Transition Behavior of a Series of Even n-Alkane C_n/C_(n+2) Mixtures Confined in Microcapsules: From Total Miscibility to Phase Separation Determined by Confinement Geometry and Repulsion Energy
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Phase Transition Behavior of a Series of Even n-Alkane C_n/C_(n+2) Mixtures Confined in Microcapsules: From Total Miscibility to Phase Separation Determined by Confinement Geometry and Repulsion Energy

机译:一系列限制在微胶囊中的偶数n-烷烃C_n / C_(n + 2)混合物的相变行为:从总混溶性到由约束几何和斥力确定的相分离

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The phase behaviors of binary consecutive even normal alkane (n-alkane) mixtures (n-C_nH_(2n+2)-C_(n+2)H_(2n+6), with mass ratios of 90/10 and 10/90) with different average carbon numbers n both in the bulk state (abbreviated as C_n/C_(n+2)) and in nearly monodisperse microcapsules (abbreviated as m-C_n/C_(n+2)), have been investigated by the combination of differential scanning calorimetry and temperature-dependent X-ray diffraction. The phase behavior of n-alkane mixtures gradually shifts from complete phase separation, partial miscibility to total miscibility in both bulk and microcapsules with the increase of average carbon numbers n. There are critical points for average carbon numbers of C_n/C_(n+2)), where the corresponding mixtures exhibit coexistence of a triclinic phase (formed by alkane with a longer chain) and an orthorhombic ordered phase (formed by the two components of mixtures). Due to the confinement from hard shells of microcapsules, the critical points of m-C_n/C_(n+2)) are smaller than those of C_n/C_(n+2)). Such a phase behavior originates from the delicate combined action of confinement and repulsion energy for the encapsulated n-alkane mixtures with different average carbon numbers n. When n is less than the critical point, the repulsion energy between the two kinds of molecules exceeds the suppression effect of confinement, and phase separation occurs in microcapsules. It is believed that the average carbon number is another important factor that exerts strong negative influence on the phase separation of m-C_n/C_(n+2)) systems.
机译:二元连续均匀正构烷烃(n-烷烃)混合物(n-C_nH_(2n + 2)-C_(n + 2)H_(2n + 6),质量比为90/10和10/90的相行为通过结合以下方法研究了在本体态(缩写为C_n / C_(n + 2))和几乎单分散的微胶囊(缩写为m-C_n / C_(n + 2))中具有不同平均碳数n的碳差示扫描量热法和温度相关的X射线衍射。随着平均碳原子数n的增加,正构烷烃混合物的相行为从完全相分离,部分可混溶性转变为在整体和微胶囊中的完全可混溶性。对于C_n / C_(n + 2)的平均碳原子数有一些临界点,其中相应的混合物表现出三斜晶相(由具有较长链的烷烃形成)和斜方晶有序相(由C的两个成分组成)共存混合物)。由于受限于微囊的硬壳,因此,m-C_n / C_(n + 2))的临界点小于C_n / C_(n + 2))的临界点。这种相行为源自具有不同平均碳原子数n的被封装的正构烷烃混合物的封闭和排斥能的微妙组合作用。当n小于临界点时,两种分子之间的斥力超过了约束的抑制作用,在微胶囊中发生了相分离。据信,平均碳数是对m-C_n / C_(n + 2))系统的相分离产生强烈负面影响的另一个重要因素。

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