An Analysis of Transient Response Moments of a Linear System Subjected to Non-Gaussian Random Excitation Using Higher-Order Autocorrelation Functions of Excitation

H. Fukushima, T. Tsuchida
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Abstract

We present the analytical solutions of the second-, third-, and fourth-order response moments of a single-degree-of-freedom linear system subjected to a class of non-Gaussian random excitation. The non-Gaussian excitation is a zero-mean stationary stochastic process prescribed by an arbitrary probability density and a power spectrum whose peak is located at zero frequency. The excitation is described by an Itô stochastic differential equation in which the drift and diffusion coefficients are determined from the probability density and spectral density of the excitation. In order to obtain the analytical solutions of the response moments, first, we derive the third- and fourth-order autocorrelation functions of the non-Gaussian excitation using its Markov and detailed balance properties. The third-order correlation function is given by the same expression regardless of the difference in the probability density function of the excitation. On the other hand, the fourth-order correlation function is derived under the assumption that the excitation probability density belongs to the Pearson distribution family, which is one of the widest classes of probability distributions. Then, combining the autocorrelation functions of the excitation and the convolution representation of the response, we obtain the exact solutions of the response moments, and it is shown what kind of components the response moments are composed of. Finally, we investigate the dominant time-varying components of the response moments for several different excitation bandwidths.
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利用激励的高阶自相关函数分析非高斯随机激励下线性系统的瞬态响应矩
本文给出了一类非高斯随机激励下单自由度线性系统的二阶、三阶和四阶响应矩的解析解。非高斯激励是由任意概率密度和峰值位于零频率的功率谱规定的零均值平稳随机过程。该激励由Itô随机微分方程描述,其中漂移系数和扩散系数由激励的概率密度和谱密度确定。为了得到响应矩的解析解,首先利用非高斯激励的马尔可夫性和详细平衡性,推导了其三阶和四阶自相关函数。三阶相关函数由相同的表达式给出,而不考虑激励的概率密度函数的差异。另一方面,在假设激励概率密度属于皮尔逊分布族的情况下,推导出了四阶相关函数,皮尔逊分布族是最广泛的概率分布之一。然后,结合激励的自相关函数和响应的卷积表示,得到了响应矩的精确解,并给出了响应矩由哪些分量组成。最后,我们研究了几种不同激励带宽下响应矩的主导时变分量。
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