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Equations of motion for position-dependent coarse-grain mappings obtained with Mori-Zwanzig theory

机译:用Mori-Zwanzig理论获得的位置依赖性粗粒映射的运动方程

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A position-dependent transformation is introduced for mapping a system of atomistic particles to a system of coarse-grained (CG) variables, which under some circumstances might be considered particles. This CG mapping allows atomistic particles to simultaneously contribute to more than a single CG particle and to change in time the CG particle they are associated with. That is, the CG mapping is dynamic. Mori-Zwanzig theory is then used to obtain the equations of motion for this CG mapping, resulting in conservative, dissipative, and random force terms in generalized, non-Markovian Langevin equations. In addition to the usual forces arising from the effective CG potential derived from atomistic interactions, new forces arise from the dynamic changes in the CG mapping itself. These new forces effectively account for changes arising from fluxes of atomistic particles into and out of CG ones as time progresses. Several examples are given showing the range of problems that can be addressed with this new CG mapping. These range from the usual case where atomistic particles are grouped into large molecular-like chunks, with mappings that remain fixed in time and for which an atomistic particle is part of only a single CG one, to the case where CG particles resemble fluid elements, containing many hundreds of independent atomistic particles. The new CG mapping also allows for hybrid descriptions, in which a part of the system remains atomistic or molecular-like and a part is highly coarse-grained to mesoscopic fluid element-like particles, for example. In the latter case, the equations of motion then provide the correct formalism for determining the forces, beyond the usual conservative ones. This provides a theoretical foundation upon which approximate equations of motion can be formulated to thus build numerical algorithms for expanded applications of accurate CG molecular dynamics. Published under license by AIP Publishing.
机译:引入位置依赖性变换,用于将原子颗粒的系统映射到粗粒(CG)变量的系统,这在某些情况下可能被认为是粒子。该CG映射允许原子颗粒同时有助于多于单个CG颗粒并随时间变化,它们与它们相关的CG粒子。也就是说,CG映射是动态的。然后使用Mori-Zwanzig理论来获得该CG映射的运动方程,导致广义的非马铃志朗文方程中的保守,耗散和随机力术语。除了从原始相互作用的有效CG潜力产生的通常的力量之外,新力来自CG映射本身的动态变化。随着时间的推移,这些新力量有效地解释了由原子颗粒的助熔剂引起的变化,因为时间进入CG系列。给出了几个例子,示出了可以通过这种新的CG映射解决的问题范围。从通常情况下将原子颗粒分成大分子样块的情况下的这些范围,其中映射保持在时间和原子颗粒是仅单个CG一的一部分,在CG颗粒类似于流体元件的情况下,包含数百个独立原子颗粒。新的CG映射还允许混合描述,其中系统的一部分仍然是原子或分子样的,并且部分是高度粗糙的粒度,例如脱模流体元件状颗粒。在后一种情况下,动作方程然后提供正确的形式主义来确定超出通常保守的力量。这提供了一种理论基础,可以配制出的近似运动方程,从而构建用于扩展的CG分子动力学的扩展应用的数值算法。通过AIP发布在许可证下发布。

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