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Transient integral boundary layer method to calculate the ...

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BioMedical Engineering OnLine 2006, 5:42http://www.biomedical-engineering-online.com/content/5/1/42(a)(b)u (x, t)Coronary Figure 1 angiogram of two myocardial bridges in <strong>the</strong> LADCoronary angiogram of two myocardial bridges in <strong>the</strong> LAD. (a) Coronary angiogram of two myocardial bridges in <strong>the</strong>left anterior descending (LAD) branch (arrows) in dias<strong>to</strong>le (left) and sys<strong>to</strong>le (right). Compression of <strong>the</strong> artery during <strong>the</strong>hearts contraction phase, i.e. sys<strong>to</strong>le, is a characteristic finding in myocardial bridging (see text and [6] for details), (b) Dias<strong>to</strong>liclumen dimensions and flow velocity are normal, while sys<strong>to</strong>lic flow velocities are increased within <strong>the</strong> bridged segments.tthirdly <strong>the</strong>re is evidence for flow separation in post stenoticregions [43,44] and finally at severe deformations (orelevated flow velocities) <strong>the</strong> artery may temporally collapse[32].ObjectiveTo ascertain <strong>the</strong> severity of <strong>the</strong> disease it is often desirable<strong>to</strong> have simple models <strong>to</strong> predict <strong>the</strong> pressure drop characteristics.A review of <strong>the</strong> available literature reveals thata few models exist, which are able <strong>to</strong> predict pressure drop(or friction fac<strong>to</strong>r) in non-circular ducts [45] (and references<strong>the</strong>rein). However, <strong>the</strong> available models are for fullydeveloped flow in non-circular ducts with fixed walls andmostly require tabulated coefficients.In this study we intend <strong>to</strong> investigate physiological relevantcases of developing blood flow through a myocardialbridge located in <strong>the</strong> middle segment of <strong>the</strong> LAD. A priormodel with similar geometry [46], but based on <strong>the</strong>assumption of fully developed Hagen-Poiseuille flow, wasused <strong>to</strong> determine <strong>the</strong> influence of severity, length anddegree of deformation and vascular termination on <strong>the</strong>flow. The results, however, indicated that <strong>the</strong> pressuredrop was not realistic, which we assume is mainly due <strong>to</strong>negligence of entrance and separation losses. The systemstudied herein is <strong>the</strong> developing flow of an incompressible,viscous fluid through a network of elastic tubes inresponse <strong>to</strong> <strong>the</strong> aortic pressure. The tube characteristicsand fluid properties are known, <strong>the</strong> developing flow conditions,<strong>the</strong> pressure response and mean FFR are desiredquantities. We primarily substantiate <strong>the</strong> influence of frictionallosses and separation losses on <strong>the</strong> translesionalpressure drop and we <strong>calculate</strong> <strong>the</strong> mean fractional flowreserve <strong>to</strong> determine <strong>the</strong> haemodynamic relevance of <strong>the</strong>myocardial bridge. Fur<strong>the</strong>r, we examine <strong>the</strong> consequenceof external deformation on <strong>the</strong> wall shear stress distributionalong <strong>the</strong> vessel.MethodsThe fluid mechanics involved in flow through a myocardialbridge is complex, because of <strong>the</strong> three dimensionalityof <strong>the</strong> deformations, coupling of <strong>the</strong> fluid with <strong>the</strong>arterial wall and flow separation. To understand <strong>the</strong> complicatedbehaviour of <strong>the</strong> tube flow, it is convenient <strong>to</strong>Page 3 of 25(page number not for citation purposes)

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