2006
DOI: 10.1016/j.jweia.2006.01.004
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Monte Carlo simulation of wind velocity fields on complex structures

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Cited by 99 publications
(39 citation statements)
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“…Several models were developed in the literature to give an analytical representation to S uj uj (x, n), for j = 1, 2, 3. Here, the model by Solari and Piccardo [23] is adopted for this purpose and Coh vivj (x, x , n) is expressed by means of the classic exponential law [11]. The imaginary part of the CPSD (called quadrature spectrum) introduces a time lag between the simulated velocities, which may become significant for points placed in the along-wind direction x 1 .…”
Section: Stochastic Wind Modelingmentioning
confidence: 99%
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“…Several models were developed in the literature to give an analytical representation to S uj uj (x, n), for j = 1, 2, 3. Here, the model by Solari and Piccardo [23] is adopted for this purpose and Coh vivj (x, x , n) is expressed by means of the classic exponential law [11]. The imaginary part of the CPSD (called quadrature spectrum) introduces a time lag between the simulated velocities, which may become significant for points placed in the along-wind direction x 1 .…”
Section: Stochastic Wind Modelingmentioning
confidence: 99%
“…, N. The complete characterization of the process u(t) is given by its power spectral density (PSD) matrix S u u (n) containing PSD and CPSD functions between turbulent velocities. Equivalently, the two-side PSD matrix G u u (ω) can also be utilized [11]. Having neglected the quadrature spectrum, both matrices S u u (n) and G u u (ω) are real and positive definite.…”
Section: Stochastic Wind Modelingmentioning
confidence: 99%
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