1983
DOI: 10.1016/0167-6105(83)90081-8
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Across-wind vibrations of structure of circular cross-section. Part II. Development of a mathematical model for full-scale application

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Cited by 86 publications
(19 citation statements)
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“…At the HDG it was not possible to simulate the turbulence of the atmospheric boundary layer. It is true that the lateral fluctuating component of the turbulent wind induces additional lift forces on the torque tube of circular cross-section (Basu and Vickery, 1983) and on the heliostat in all (Peterka and Derickson, 1992;Pfahl et al, 2011). Furthermore, by Cheung and Melbourne (2005) an increase of the span-wise force correlation with increased turbulence intensity was determined.…”
Section: Selection Of Toolmentioning
confidence: 95%
“…At the HDG it was not possible to simulate the turbulence of the atmospheric boundary layer. It is true that the lateral fluctuating component of the turbulent wind induces additional lift forces on the torque tube of circular cross-section (Basu and Vickery, 1983) and on the heliostat in all (Peterka and Derickson, 1992;Pfahl et al, 2011). Furthermore, by Cheung and Melbourne (2005) an increase of the span-wise force correlation with increased turbulence intensity was determined.…”
Section: Selection Of Toolmentioning
confidence: 95%
“…Different semi-empirical models have been used for describing VIV and lock-in phenomena, including wake oscillator models (Bishop and Hassan, 1963;Hartlen and Currie, 1970;Griffin et al, 1973;Skop and Griffin, 1973), SDOF models that use a single ordinary differential equation to describe the behavior of structural oscillator (Basu and Vickery, 1983;Simiu and Scanlan, 1986;Goswami et al, 1993), force decomposition models in which the lift force is decomposed into a fluid inertia force related to structure displacement and a fluid damping force related to structure velocity (Griffin, 1980;Griffin and Koopman, 1997), and variational approaches (McIver, 1973;Benaroya and Wei, 2000).…”
Section: Introductionmentioning
confidence: 99%
“…The first two most accepted models by the Wind Engineering community in the case of the circular section were developed in the 1980's. The first model (Vickery and Basu [2], [3], [4], Basu and Vickery [5]), was developed at the University of Western Ontario, Canada, and considers the effects of fluid-structure interaction, incorporating the concept of negative aerodynamic damping. The second model (Ruscheweyh,[6]), developed at the University of Aachen, Germany, considers that equivalent forces due to vortex shedding occur at a given correlation length.…”
Section: Introductionmentioning
confidence: 99%