如何定义时间分数相场方程的保耗散能量

IF 0.9 Q2 MATHEMATICS, APPLIED
Chaoyu Quan, T. Tang, Jiang Yang
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引用次数: 34

摘要

经典相场方程存在一个定义良好的能量,满足耗散规律,即能量随时间不增加。然而,如何将能量定义推广到时间分数相场方程中,以满足相应的耗散规律,目前尚不清楚。在这项工作中,我们将尝试通过将非局部能量定义为具有时间相关权函数的经典能量的平均值来解决具有卡普托时间分数阶导数的相场方程的这个问题。由于控制方程具有非局部和非线性特性,因此耗散分析具有挑战性。为了解决这个问题,我们提出了一个新的判断对称函数正定性的定理,该定理是由一个特殊的Cholesky分解导出的。然后,在一个简单的权函数限制下,证明了非局部能量是耗散的。在相同的框架下,可以证明时间分数相场模型的经典能量的时间分数导数总是非正的。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
How to Define Dissipation-Preserving Energy for Time-Fractional Phase-Field Equations
There exists a well defined energy for classical phase-field equations under which the dissipation law is satisfied, i.e., the energy is non-increasing with respect to time. However, it is not clear how to extend the energy definition to time-fractional phase-field equations so that the corresponding dissipation law is still satisfied. In this work, we will try to settle this problem for phase-field equations with Caputo time-fractional derivative, by defining a nonlocal energy as an averaging of the classical energy with a time-dependent weight function. As the governing equation exhibits both nonlocal and nonlinear behavior, the dissipation analysis is challenging. To deal with this, we propose a new theorem on judging the positive definiteness of a symmetric function, that is derived from a special Cholesky decomposition. Then, the nonlocal energy is proved to be dissipative under a simple restriction of the weight function. Within the same framework, the time fractional derivative of classical energy for time-fractional phase-field models can be proved to be always nonpositive.
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CiteScore
2.70
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