Due to the transient incident wind upon the mountain range, the flow undergoes a transition from the low-level blocking/flow-splitting regime into nonlinear and linear wave regimes as the cross-mountain flow increases; the inverse progression is found as the cross-mountain flow decelerates back to zero. At the early stage of the accelerating phase, the flow is nonlinear, with lee vortex generation, followed by wake formation, vortex shedding, and finally wake detachment. As the incident flow further increases, the flow becomes more linear, and unsteady mountain wave propagation is present. After the maximum incident wind passes by the mountain, a transition from the linear regime to the nonlinear regime is found. During the decelerating phase, the low-level flow is deflected by the mountain and wake formation and lee vortex generation are again present.
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