“…In an open flow, turbulence commences following a characteristic distance measured between the contact point of a fluid on a flat plate and the point at which the flow becomes turbulent [33]; however, this case requires all dimensions of the flow, including film depth, to be large compared to the characteristic distance. In the case of this flow, the meniscus defines the flow geometry; thus, the effect of rolling eddies alone are not responsible for the deposition patterns evidenced by Dowding and Lawrence [28], where debris distribution appeared to lie in ripple patterns downstream of the feature machined. Instead, large inertial, capillary, and viscous contributions complicated the flow path.…”