高斯有色噪声激励下动力系统的概率响应:非马尔可夫理论的基础

K. Mamis, Κωνσταντίνος Ι. Μαμής
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引用次数: 4

摘要

本博士论文的主题是推导概率密度函数(pdf)的演化方程,该方程描述了高斯彩色(平滑相关)噪声下动力系统的非马尔可夫响应。这些pdf演化方程来源于随机Liouville方程(SLEs), SLEs通过将pdf表示为平均随机函数来表示。SLEs是精确的但非封闭的,因为它们包含通过高阶pdf表示的平均项。这些平均项通过使用Novikov-Furutsu (NF)定理的推广得到进一步的评估。在NF定理之后,SLE平均根据响应的整个历史(在某些情况下,也取决于激励的历史)等效地表示为非局部项。然后,利用响应的适当矩(或联合响应-激励矩)的历史,用一种新颖的闭包格式逼近非局部项。应用该格式得到了一组新的pdf演化方程。这些方程是非线性的,保留了可处理的SLEs的原始非局域性,也是封闭形式和可解的。最后,对Ornstein-Uhlenbeck激励下的标量双稳随机微分方程进行了数值求解,并与Monte Carlo (MC)模拟结果进行了比较。结果表明,即使在高噪声强度和大相关次数的激励下,即远离白噪声极限的情况下,所建立的演化方程也能很好地与MC模拟吻合,这是现有文献中发现的pdf演化方程所不能达到的。值得注意的是,求解新的pdf进化方程的计算工作量与求解相应的经典Fokker-Planck-Kolmogorov方程所需的计算工作量相当。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Probabilistic responses of dynamical systems subjected to gaussian coloured noise excitation: foundations of a non-markovian theory
The topic of this PhD thesis is the derivation of evolution equations for probability density functions (pdfs) describing the non-Markovian response to dynamical systems under Gaussian coloured (smoothly-correlated) noise. These pdf evolution equations are derived from the stochastic Liouville equations (SLEs), which are formulated by representing the pdfs as averaged random delta functions. SLEs are exact yet non-closed, since they contain averaged terms that are expressed via higher-order pdfs. These averaged terms are further evaluated by employing generalizations of the Novikov-Furutsu (NF) theorem. After the NF theorem, SLE averages are expressed equivalently as nonlocal terms depending on the whole history of the response (in some cases, on the history of excitation too). Then, nonlocal terms are approximated by a novel closure scheme, employing the history of appropriate moments of the response (or joint response-excitation moments). Application of this scheme results in a family of novel pdf evolution equations. These equations are nonlinear and retain a tractable amount of the original nonlocality of SLEs, being also in closed form and solvable. Last, the new evolution equations for the one-time response pdf are solved numerically and their results are compared to Monte Carlo (MC) simulations, for the case of a scalar bistable random differential equation under Ornstein-Uhlenbeck excitation. The results show that the novel evolution equations are in very good agreement with the MC simulations, even for high noise intensities and large correlation times of the excitation, that is, away from the white noise limit, where the existing pdf evolution equations found in literature fail. It should be noted that the computational effort for solving the new pdf evolution equations is comparable to the effort required for solving the respective classical Fokker-Planck-Kolmogorov equation.
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