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包裹颗粒的随机流形的肿胀

Swelling of particle-encapsulating random manifolds.

作者信息

Haleva Emir, Diamant Haim

机构信息

School of Chemistry, Raymond & Beverly Sackler Faculty of Exact Sciences, Tel Aviv University, Tel Aviv 69978, Israel.

出版信息

Phys Rev E Stat Nonlin Soft Matter Phys. 2008 Aug;78(2 Pt 1):021132. doi: 10.1103/PhysRevE.78.021132. Epub 2008 Aug 22.

Abstract

We study the statistical mechanics of a closed random manifold of fixed area and fluctuating volume, encapsulating a fixed number of noninteracting particles. Scaling analysis yields a unified description of such swollen manifolds, according to which the mean volume gradually increases with particle number, following a single scaling law. This is markedly different from the swelling under fixed pressure difference, where certain models exhibit criticality. We thereby indicate when the swelling due to encapsulated particles is thermodynamically inequivalent to that caused by fixed pressure. The general predictions are supported by Monte Carlo simulations of two particle-encapsulating model systems: a two-dimensional self-avoiding ring and a three-dimensional self-avoiding fluid vesicle. In the former the particle-induced swelling is thermodynamically equivalent to the pressure-induced one, whereas in the latter it is not.

摘要

我们研究了一个封闭的随机流形的统计力学,该流形具有固定的面积和波动的体积,其中封装了固定数量的非相互作用粒子。标度分析给出了此类膨胀流形的统一描述,据此,平均体积随粒子数逐渐增加,遵循单一的标度律。这与在固定压差下的膨胀明显不同,在固定压差下某些模型会表现出临界性。由此我们指出,由于封装粒子导致的膨胀在热力学上何时与由固定压力导致的膨胀不等价。通用预测得到了两个封装粒子的模型系统的蒙特卡罗模拟的支持:二维自回避环和三维自回避流体囊泡。在前者中,粒子诱导的膨胀在热力学上等同于压力诱导的膨胀,而在后者中则不然。

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