Jadhao Vikram, Solis Francisco J, de la Cruz Monica Olvera
Department of Materials Science and Engineering, Northwestern University, Evanston, Illinois 60208, USA.
Phys Rev E Stat Nonlin Soft Matter Phys. 2013 Aug;88(2):022305. doi: 10.1103/PhysRevE.88.022305. Epub 2013 Aug 12.
In simulating charged systems, it is often useful to treat some ionic components of the system at the mean-field level and solve the Poisson-Boltzmann (PB) equation to get their respective density profiles. The numerically intensive task of solving the PB equation at each step of the simulation can be bypassed using variational methods that treat the electrostatic potential as a dynamic variable. But such approaches require the access to a true free-energy functional: a functional that not only provides the correct solution of the PB equation upon extremization, but also evaluates to the true free energy of the system at its minimum. Moreover, the numerical efficiency of such procedures is further enhanced if the free-energy functional is local and is expressed in terms of the electrostatic potential. Existing PB functionals of the electrostatic potential, while possessing the local structure, are not free-energy functionals. We present a variational formulation with a local free-energy functional of the potential. In addition, we also construct a nonlocal free-energy functional of the electrostatic potential. These functionals are suited for employment in simulation schemes based on the ideas of dynamical optimization.
在模拟带电系统时,将系统的一些离子成分在平均场水平上进行处理,并求解泊松 - 玻尔兹曼(PB)方程以获得它们各自的密度分布通常是很有用的。使用将静电势视为动态变量的变分方法,可以绕过在模拟的每个步骤中求解PB方程这一数值密集型任务。但是,这种方法需要获得一个真正的自由能泛函:一个在求极值时不仅能提供PB方程的正确解,而且在其最小值处能评估为系统真实自由能的泛函。此外,如果自由能泛函是局部的并且以静电势表示,那么这些过程的数值效率会进一步提高。现有的静电势PB泛函虽然具有局部结构,但不是自由能泛函。我们提出了一种具有势的局部自由能泛函的变分公式。此外,我们还构造了一种静电势的非局部自由能泛函。这些泛函适用于基于动态优化思想的模拟方案。