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Wind Hazard Risk Assessment and Management for Structures

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Chapter 2. Structural Components <strong>and</strong> <strong>Wind</strong> Directionality 24<br />

University of Florida, 2009). The values of the parameters are listed in the caption of Figure<br />

2.3, which shows the simulated wind records. For comparison, the historical wind records<br />

(see Figure 2.4) are converted from 15-minute average to 3-second gust. The general trends<br />

of the simulated wind speed <strong>and</strong> wind angle time series match the historical record quite<br />

well. The magnitude of the wind velocity is also close to the historical data. Note that the<br />

absolute accuracy of this model is not the major focus in this study. Since the objective is<br />

to look at the effect of changing wind directionality in individual wind events, it is more<br />

important <strong>for</strong> the wind time series model to be capable to generate wind time series that<br />

have trends similar to those of the historical wind records, in terms of both wind speed <strong>and</strong><br />

wind angle.<br />

2.3 Alternative Approaches to <strong>Wind</strong>-Load <strong>and</strong> Reliability<br />

<strong>Assessment</strong><br />

Given the simulated tropical cyclone wind velocity time series described in the previous<br />

section, wind loads may be computed <strong>and</strong> structural reliability analysis may be carried out,<br />

<strong>for</strong> the two a<strong>for</strong>e-mentioned approaches, in the way explained below.<br />

2.3.1 <strong>Wind</strong> Load <strong>and</strong> Reliability Calculation<br />

Damage of envelope components, which is the major factor in insurance claims (Sparks<br />

et al., 1994), is mainly caused by wind loads during tropical cyclones (National Institute of<br />

St<strong>and</strong>ards <strong>and</strong> Technology, 2006b). Given a wind velocity time series over the time domain<br />

[0, tL] (with wind speed V (t) <strong>and</strong> θ(t)), from bluff-body aerodynamics, the wind pressure<br />

acting on a building envelope component at time t ∈ [0, tL] is given by (Holmes, 2007):<br />

S(t) = 1<br />

2 ρV (t)2 Cp(θ(t) − γ), (2.12)

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