1994
DOI: 10.1016/0266-8920(94)90017-5
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Probability distribution applicable to non-Gaussian random processes

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Cited by 45 publications
(10 citation statements)
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“…This energy augmentation, therefore, provides the difference between the bare and the dressed spectra as originally introduced and discussed in [6]. The difference between bare and dressed spectra as given in (8) can also be assimilated with the bicoherence function of phase coupling as introduced by [7] and utilized by [8]. Indeed, energy of phase coupling to second order is another manifestation of the bispectrum defined as the Fourier transform of the skewness function using a third order cumulant.…”
Section: B Temporal and Statistical Modulationmentioning
confidence: 96%
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“…This energy augmentation, therefore, provides the difference between the bare and the dressed spectra as originally introduced and discussed in [6]. The difference between bare and dressed spectra as given in (8) can also be assimilated with the bicoherence function of phase coupling as introduced by [7] and utilized by [8]. Indeed, energy of phase coupling to second order is another manifestation of the bispectrum defined as the Fourier transform of the skewness function using a third order cumulant.…”
Section: B Temporal and Statistical Modulationmentioning
confidence: 96%
“…being the number of points of the series in and we have (9) Discretized pdfs are obtained this way. We associate this excess spectrum in (8) with terms added to the bare spectrum as contributing to the energy increase at higher frequencies due to the nonlinearities or mode coupling. This energy augmentation, therefore, provides the difference between the bare and the dressed spectra as originally introduced and discussed in [6].…”
Section: B Temporal and Statistical Modulationmentioning
confidence: 99%
See 1 more Smart Citation
“…This energy augmentation therefore provides the difference between the bare and the dressed spectra as discussed in [Elfouhaily et al, 1999]. The difference can also be assimilated with the bicoherence function of phase coupling as introduced by Kim and Powers [1979] and utilized by Ochi and Ahn [1994]. Indeed, energy of phase coupling to second order is another manifestation of the bispectrum defined as the Fourier transform of the skewness function using a third order cumulant.…”
Section: Temporal and Statistical Modulationmentioning
confidence: 99%
“…Different strategies to choose the function g have been proposed and studied in [8][9][10] and [11]. An advantage with the transformed Gaussian models is that they are easy to simulate from and that the fatigue damage can be related to Gaussian loads where a lot of results are known.…”
Section: Introductionmentioning
confidence: 99%