Wu K L, Lai S K
Complex Liquids Laboratory, Department of Physics, National Central University, Chungli 320, Taiwan, ROC.
Colloids Surf B Biointerfaces. 2007 Apr 15;56(1-2):290-5. doi: 10.1016/j.colsurfb.2006.11.017. Epub 2006 Nov 18.
Recent experimental studies [Z. Wu, B. Zhou, Z.B. Hu, Phys. Rev. Lett. 90 (2003) 048304] on an uncharged aqueous poly-N-isopropylacrylamide (PNIPAM) dispersion have shown that this microgel system is sensitive to temperature. This system was also experimentally found to be modeled quite well by microgel particles interacting via a hard-sphere repulsive plus an inverse power (temperature-dependent) attractive potential. To understand theoretically this thermally responsive PNIPAM dispersion, we apply a novel approach [G.F. Wang, S.K. Lai, Phys. Rev. E 70 (2004) 051402] to calculate its thermodynamic phase diagram. Differing from the conventional method in which the boundaries of the coexisting phases are the ultimate target, the present work places emphasis on crosshatching colloidal domains which include the homogeneous phase (gas, liquid or solid), two coexisting phases and perhaps also multi-phases in coexistence. Strategically, this was done by treating the coexisting phases as one composite system whose Helmholtz free energy density is written as the sum of constituent free energy densities each of which is weighed by its respective volume proportion. We show here that by minimizing the composite system's free energy density the phase-diagram domains can all be determined in addition to the phase boundaries customarily obtained by imposing the conditions of equal pressure and equal chemical potential. Also, we present the theoretically predicted phase diagram of PNIPAM dispersion and compare it with the one observed experimentally.
最近关于不带电的聚-N-异丙基丙烯酰胺(PNIPAM)水性分散体系的实验研究[Z. Wu, B. Zhou, Z.B. Hu,《物理评论快报》90 (2003) 048304]表明,这种微凝胶体系对温度敏感。实验还发现,该体系可以很好地用通过硬球排斥力加上反比幂(与温度有关)吸引力相互作用的微凝胶颗粒来建模。为了从理论上理解这种热响应性的PNIPAM分散体系,我们应用一种新方法[G.F. Wang, S.K. Lai,《物理评论E》70 (2004) 051402]来计算其热力学相图。与传统方法不同,传统方法将共存相的边界作为最终目标,而本研究重点关注交叉阴影胶体区域,其中包括均相(气体、液体或固体)、两个共存相以及可能同时共存的多相。从策略上讲,这是通过将共存相视为一个复合体系来实现的,该复合体系的亥姆霍兹自由能密度写成各组成部分自由能密度之和,每个部分自由能密度都由其各自的体积比例加权。我们在此表明,通过最小化复合体系的自由能密度,除了通过施加等压和等化学势条件通常得到的相边界外,还可以确定相图区域。此外,我们给出了PNIPAM分散体系的理论预测相图,并将其与实验观察到的相图进行比较。