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    Equivalent Stochastic Systems

    Source: Journal of Applied Mechanics:;1988:;volume( 055 ):;issue: 004::page 918
    Author:
    Y. K. Lin
    ,
    G. Q. Cai
    DOI: 10.1115/1.3173742
    Publisher: The American Society of Mechanical Engineers (ASME)
    Abstract: Equivalent stochastic systems are defined as randomly excited dynamical systems whose response vectors in the state space share the same probability distribution. In this paper, the random excitations are restricted to Gaussian white noises; thus, the system responses are Markov vectors, and their probability densities are governed by the associated Fokker-Planck equations. When the associated Fokker-Planck equations are identical, the equivalent stochastic systems must share both the stationary probability distribution and the transient nonstationary probability distribution under identical initial conditions. Such systems are said to be stochastically equivalent in the strict (or strong) sense. A wider class, referred to as the class of equivalent stochastic systems in the wide (or weak) sense, also includes those sharing only the stationary probability distribution but having different Fokker-Planck equations. Given a stochastic system with a known probability distribution, procedures are developed to identify and construct equivalent stochastic systems, both in the strict and in the wide sense.
    keyword(s): Stochastic systems , Probability , Equations , Random excitation , Noise (Sound) AND Dynamic systems ,
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      Equivalent Stochastic Systems

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    contributor authorY. K. Lin
    contributor authorG. Q. Cai
    date accessioned2017-05-08T23:26:23Z
    date available2017-05-08T23:26:23Z
    date copyrightDecember, 1988
    date issued1988
    identifier issn0021-8936
    identifier otherJAMCAV-26299#918_1.pdf
    identifier urihttp://yetl.yabesh.ir/yetl/handle/yetl/103447
    description abstractEquivalent stochastic systems are defined as randomly excited dynamical systems whose response vectors in the state space share the same probability distribution. In this paper, the random excitations are restricted to Gaussian white noises; thus, the system responses are Markov vectors, and their probability densities are governed by the associated Fokker-Planck equations. When the associated Fokker-Planck equations are identical, the equivalent stochastic systems must share both the stationary probability distribution and the transient nonstationary probability distribution under identical initial conditions. Such systems are said to be stochastically equivalent in the strict (or strong) sense. A wider class, referred to as the class of equivalent stochastic systems in the wide (or weak) sense, also includes those sharing only the stationary probability distribution but having different Fokker-Planck equations. Given a stochastic system with a known probability distribution, procedures are developed to identify and construct equivalent stochastic systems, both in the strict and in the wide sense.
    publisherThe American Society of Mechanical Engineers (ASME)
    titleEquivalent Stochastic Systems
    typeJournal Paper
    journal volume55
    journal issue4
    journal titleJournal of Applied Mechanics
    identifier doi10.1115/1.3173742
    journal fristpage918
    journal lastpage922
    identifier eissn1528-9036
    keywordsStochastic systems
    keywordsProbability
    keywordsEquations
    keywordsRandom excitation
    keywordsNoise (Sound) AND Dynamic systems
    treeJournal of Applied Mechanics:;1988:;volume( 055 ):;issue: 004
    contenttypeFulltext
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