“…The crack increment Δainormal′ for each crack growth step is adjusted to be the average between those in the previous step and the next step, that is, Δai=(normalΔai−1′,+normalΔai′,)/2, and thus the adjusted crack increments are Δ a 1 =0.175 mm, Δ a 2 =0.425 mm, Δ a 3 =2.25 mm, Δ a 4 =4.5 mm, Δ a 5 =6.5 mm, and Δ a 6 =4 mm, so that the stress intensity factor range at the start point or the end point of each step becomes nearly at the middle point of the adjusted step to represent the stress intensity factor in the whole crack increment more precisely, as shown in Figure 4(g).- (2) Suitable finite element sub-models for crack growth analysis are established and the wind loading time-histories with a duration of 50s (500 load steps) as shown in Figure 4(f) are exerted on the multi-scale FE model. The simulation of wind loading is detailed in the previous research by the authors (Fang et al, 2017, 2018). The equivalent stress intensity factor time-history at the crack tip within each adjusted crack increment i ( i = 1, 2, ..., 6, the crack growth step number), denoted as K eq i , is calculated based on equation (15) from the work of Gerstle (1986).
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