2021
DOI: 10.1155/2021/1823596
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Response of Cantilever Model with Inertia Nonlinearity under Transverse Basal Gaussian Colored Noise Excitation

Abstract: Considering the curvature nonlinearity and longitudinal inertia nonlinearity caused by geometrical deformations, a slender inextensible cantilever beam model under transverse pedestal motion in the form of Gaussian colored noise excitation was studied. Present stochastic averaging methods cannot solve the equations of random excited oscillators that included both inertia nonlinearity and curvature nonlinearity. In order to solve this kind of equations, a modified stochastic averaging method was proposed. This … Show more

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Cited by 1 publication
(2 citation statements)
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“…where 𝑚(𝐴) denotes the drift coefficient, 𝜎 (𝐴) denotes the diffusion coefficient, 𝑊(𝑡) is standard unit Brownian motion (see reference [29,30]). The operator ⟨•⟩ = ∫ • 𝑑𝜃 does averaging with respect to time, 𝑅(𝜏) denotes the noise correlation function, 2D is the noise strength, 𝜆 is the time delay coefficient:…”
Section: Stochastic Averagingmentioning
confidence: 99%
See 1 more Smart Citation
“…where 𝑚(𝐴) denotes the drift coefficient, 𝜎 (𝐴) denotes the diffusion coefficient, 𝑊(𝑡) is standard unit Brownian motion (see reference [29,30]). The operator ⟨•⟩ = ∫ • 𝑑𝜃 does averaging with respect to time, 𝑅(𝜏) denotes the noise correlation function, 2D is the noise strength, 𝜆 is the time delay coefficient:…”
Section: Stochastic Averagingmentioning
confidence: 99%
“…( 1) is infinitely large, the colored noise will decrease to be a Gaussian with noise. G. Falsone and I. Elishakoff [29] developed a stochastic linearization technique for colored noise excited Duffing oscillator. After that, Bo Li et.al.…”
Section: Introductionmentioning
confidence: 99%