The understanding of valvular opening is a central issue in cardiac flows, whose analysis is often prohibited by the unavailability of (in vivo) data about tissue properties. Asymptotic or approximate representations of fluid-structure interaction are thus sought. The dynamics of an accelerated stream, in a two-dimensional channel initially closed by a rigid inertialess movable leaflet, is studied as a simple model problem aimed at demonstrating the main phenomena contributing to the fluidstructure interaction. The problem is solved by the coupled numerical solution of equations for the flow and solid. The results show that the leaflet initially opens in a no-shedding regime, driven by fluid mass conservation and a predictable dynamics. Then the leaflet motion jumps, after the saturation of a very rapid intermediate vortex-shedding phase, to the asymptotic slower regime with a stable self-similar wake structure.
IntroductionThe interaction between a fluid stream and a moving boundary is common in several contexts; numerous examples can be found in the cardiovascular system where flows inside deformable vessels and through cardiac valves are of primary physiological relevance. The original motivation for this work is our interest in the flow through the mitral valve that controls the blood motion from the left atrium to the left ventricle of the heart. More generally, similar phenomena can be found in technological devices when valves are used to control the fluid motion through orifices and possibly to avoid back-flow. Despite the applied background this work is a theoretical one, on the interaction of the flow and a leaflet under ideal conditions. It represents a step towards the understanding of phenomena in a fluid-structure interaction of potentially high applied relevance.When a closed valve is forced to open by a stream, the (typically thin) leaflets rapidly move with the fluid with only a weak resistance to it. A rigorous mathematical model of the flow-structure dynamics should be based on the fluid and solid equations, for the flow and the tissue, respectively, and on the proper coupling relations. Along these lines, a simplified approach, developed for a thin solid without bending stiffness, was introduced by Peskin & McQueen (1989). However, in our experience, the numerical implementation of this mathematically attractive model has several disadvantages, such as the lack of resolution close to the body and unrealistic stress distributions on it. A major difficulty in studying the fluid-solid interaction is the rapidity of the leaflet response to the action of the incoming fluid, and its large movement within the flow domain. A complete numerical solution of the fluid-solid system has been presented for the flow in models of the aortic valve (De Hart et al. 2003; Stijnen et al.