1995
DOI: 10.1016/0266-8920(95)00018-6
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Surge response statistics of tension leg platforms under wind and wave loads: a statistical quadratization approach

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Cited by 29 publications
(5 citation statements)
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“…According to the linear wave theory, the current is modeled as an average current velocity U and a water-particle velocity u(t), which is modeled as a Gaussian random process with a given power spectral density S ( ) u ω . One specificity of this problem is that the typical shape of this spectral density is such that the center of gravity of the distribution α is usually much larger than the natural frequency ω of the linear unloaded oscillator [24]. Furthermore, commonly adopted power spectral densities such as the one resulting from the wave height in the Jonswap model [59] are negligible in the low-frequency range, precisely where the fundamental natural frequency of the linear unloaded oscillator is located.…”
Section: Problem 5: Response Of a Nonlinear Systemmentioning
confidence: 99%
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“…According to the linear wave theory, the current is modeled as an average current velocity U and a water-particle velocity u(t), which is modeled as a Gaussian random process with a given power spectral density S ( ) u ω . One specificity of this problem is that the typical shape of this spectral density is such that the center of gravity of the distribution α is usually much larger than the natural frequency ω of the linear unloaded oscillator [24]. Furthermore, commonly adopted power spectral densities such as the one resulting from the wave height in the Jonswap model [59] are negligible in the low-frequency range, precisely where the fundamental natural frequency of the linear unloaded oscillator is located.…”
Section: Problem 5: Response Of a Nonlinear Systemmentioning
confidence: 99%
“…limited to statistical order 2 or not, e.g. [11][12][13][14][15], (ii) the single degree-of-freedom (SDOF) and the multiple degree-of-freedom (MDOF) versions, the latter being well known for the second order [5,7] and theoretically established for higher order analysis [13,16], (iii) the steady-state response analysis, as in most common applications, but also with evolutionary stochastic analyses, a concept formalized by Priestley [17], but that still receives much interest [18], especially in seismic engineering [19,20] and (iv) although the concept of spectral analysis hinges on the underlying assumptions of linearity and of the superposition principle, both the stochastic linearization [21] (as well as its higher order generalizations [22][23][24]) and the Volterra series Contents lists available at ScienceDirect journal homepage: www.elsevier.com/locate/probengmech model [25][26][27] are interesting ways to extend its domain of applicability to systems with mild nonlinearities. In all these versions of the spectral analysis, a canonical form for the jth order spectrum of the response (or contribution thereof in the nonlinear case) is ( ) ( ) ( ) x ω respectively stand for the jth-order spectra of the loading and of the response.…”
mentioning
confidence: 99%
“…It is assumed that this process is zero-mean, stationary in time but possibly non Gaussian so that it is fully described by its spectra of various orders [14,24,25]. This assumption is justified as follows: (i) the case of a non-zero-mean process can be tackled similarly owing to the linearity of the problem and the superposition principle, (ii) stationarity in time is a common assumption for wind loads [4], wave and current loads [33], (iii) the non Gaussianity of the loading might arise from the nonlinear nature of the wind and wave loading processes [34,35].…”
Section: Second Order Stochastic Analysismentioning
confidence: 99%
“…[175][176][177] presented spectral densities of the drag force on rigid structures. Attempts to assess the response to the non-linear drag force on compliant structures in the frequency domain have been done by [178][179][180][181], who employed the Volterra series expansion technique.…”
Section: Frequency-domain Analysismentioning
confidence: 99%