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Predicting disorder-order phase transitions in polymeric micelles

机译:预测聚合物胶束的无序相变

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The structure observed in concentrated polymeric micelles results from interactions between coronal chains that develop as micelles are brought to approach distances where the chains either compress or interdigitate. One powerful model for polymeric micelles comprises spherical particles with chains tethered to their core at a specified surface density. This treatment combined with self-consistent field theory provides an estimate of the pair interaction potential between micelles. These pair interaction potentials allow modeling of the structure and thermodynamic properties that depend on the overall micelle concentration. We perform neutron scattering experiments to measure the short-range correlations in the liquid, through the static structure factor S(q), and compare these results with models that rely on a solution of the Ornstein-Zernike equation subject to a Rogers-Young closure. A description of the homogeneous liquid serves as the basis for employing density functional theory (DFT) to estimate the free energy of the solid. In this investigation, we use the modified weighted density approximation of Denton and Ashcroft [Phys. Rev. A 39, 4701 (1989)] to estimate the free energy of the solid for each of our micellar systems to predict the liquid-solid phase transition. Although we experimentally observe transitions to face-centered-cubic (fcc) and body-centered-cubic (bcc) crystals depending on the length of the corona relative to the core, we only predict a simple liquid-fcc transition with the DFT method. The nature of the transition suggests a simple perturbation result using the hard sphere as the reference system. Despite the inability to predict the bcc lattice type, both DFT and hard-sphere models accurately predict coexistence over the entire range of our experiments.
机译:在浓缩的聚合物胶束中观察到的结构是由冠状链之间的相互作用产生的,该冠状链是随着胶束达到接近的距离而发展的,在该距离处链被压缩或相互交叉。一种有效的高分子胶束模型包括球形颗粒,其球形链在指定的表面密度下束缚在其核心上。结合自洽场理论的这种处理提供了胶束之间的成对相互作用潜力的估计。这些成对的相互作用电位允许对取决于总胶束浓度的结构和热力学性质进行建模。我们进行中子散射实验,通过静态结构因子S(q)来测量液体中的短程相关性,并将这些结果与依赖于受Rogers-Young封闭的Ornstein-Zernike方程解的模型进行比较。对均匀液体的描述是采用密度泛函理论(DFT)估算固体自由能的基础。在这项研究中,我们使用Denton和Ashcroft [Phys。 Rev. A 39,4701(1989)]来估计每个胶束系统的固体自由能,以预测液-固相变。尽管我们根据电晕相对于磁芯的长度实验性地观察到向面心立方(fcc)和体心立方(bcc)晶体的转变,但我们仅使用DFT方法预测了简单的液体-fcc转变。过渡的性质表明使用硬球体作为参考系统的简单摄动结果。尽管无法预测bcc晶格类型,但DFT模型和硬球模型都可以准确预测我们实验整个范围内的共存。

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