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      In the first part of this paper, literature survey on AAA biomechanics is reported including several aspects from experimental test, constitutive model, and ILT. Further, we presented our FE models, aimed at simulating and enhancing the computational study of the aneurismatic pathology. The combination of fluid and nonlinear structure modeling can give better understanding of the flow, pressure distribution, wall shear stress quantification, and effect of material properties and geometrical parameters. Computational methods have made patient‐specific analyses possible, a feature essential for understanding the progression of AAA in a particular patient. Finally, future clinical DSS is suggested by using DM approach. The main aim is to run predictive FSI model in order to estimate the risk of rupture and to use patient‐specific wall properties with calcium, tissue disease, and thrombus to overcome multiple level of uncertainties.

      During the last two decades, significant efforts have been made in order to define a computational model which includes biomechanical and biological approach, but still a lot of clinical studies are necessary in order to make these computational studies real in everyday clinical practice.

      Exercise 1.1 Modeling of Blood Flow Within the AAA

      The shape of AAA is very important. The severity of AAA is commonly estimated in clinical practice by considering the AAA maximal diameter. However, from the mechanical point of view, the hemodynamic effects and the mechanical stresses within the AAA tissue certainly are important in the process of the AAA rupture. Bulge diameter alone may not be a sufficient criterion for determination of rupture risk; therefore, an insight into the hemodynamic effects and the stress–strain quantification and distribution within the vessel wall are of great significance even in medical practice.

      Generation of the Finite Element Model

Schematic illustration of geometrical parameters of AAA.

      Boundary Conditions

      At the inflow aorta cross‐section, a fully developed parabolic flow is assumed, determined by a selected volume flux. The normal stress and tangential stress are set to be equal to zero (stress‐free condition) or they are prescribed at the outlet cross‐section.

Schematic illustration of a typical in-flow waveform at the aorta entry.

      Results

      Results for two examples of the symmetric AAA are given here: (i) case with rigid walls and (ii) AAA with deformable walls. Results not shown here and solutions for other model parameters can be obtained using Software on the web.

      Modeling of AAA Assuming Rigid Walls

      We analyze an aneurism at the straight aorta domain, where aorta proximal and distal to the AAA bulge is idealized as straight rigid tube and branching arteries are excluded. The model has ratio D/d = 2.75 and geometry generated according to Figure 1.5 (D and d are diameters of the bulge and aorta, respectively). The data are: blood density is ρ = 1.05 g/cm3; kinematic viscosity (Newtonian fluid) ν = 0.035 cm2/s, d = 12.7 mm. The inflow velocity is defined by the flux function given in Figure 1.6. The FE mesh consisted of approximately 8000 3D 8‐node brick elements.

Schematic illustration of velocity field (left panel) and pressure distribution (right panel) for peak systole t/T = 0.16 of AAA for the model with D/d = 2/75, d = 12.7 mm.

      Modeling AAA with Deformable Walls

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