10.07.2015 Views

Transient integral boundary layer method to calculate the ...

Transient integral boundary layer method to calculate the ...

Transient integral boundary layer method to calculate the ...

SHOW MORE
SHOW LESS

Create successful ePaper yourself

Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.

BioMedical Engineering OnLine 2006, 5:42http://www.biomedical-engineering-online.com/content/5/1/42 Deformation Figure 3 cross-sectionDeformation cross-section. This figure illustrates <strong>the</strong> deformation geometry of a circular, linear elastic tube neglecting <strong>the</strong>bending stress inside <strong>the</strong> wall. Cross-section B - B (left) shows circular expansion under pressure and <strong>the</strong> cross-section C - Cillustrates <strong>the</strong> geometry under external deformation (right). The equilibrium cross-sectional area A d is shaded in light grey,while <strong>the</strong> perturbation area A' is shaded in dark grey. The dashed lines indicate expansion under pressure.ity in axial direction. The volume flux across a given section<strong>the</strong>refore is q (x, t) = A u.As shown in <strong>the</strong> angiography 1 and Figure 2 <strong>the</strong> coronaryarteries in myocardial bridges are structured by severalwall deformations. Their number, degree and extensionmay independently vary with time, so that <strong>the</strong> axial curvatureof <strong>the</strong> arterial wall for each of <strong>the</strong> n = 1...N myocardialbridges in series is characterised by N functions. Thedeformation is specified by a parameter ζ, defined as ζ =R d /R 0 , which is chosen in <strong>the</strong> stenosis n <strong>to</strong> vary with timeas( ) +1ζn ( t) = ζdias<strong>to</strong>le −ζsys<strong>to</strong>le ( gn 1)+ ζsys<strong>to</strong>le,( 1)2where g n (t) are periodic functions describing <strong>the</strong> temporalcontraction of <strong>the</strong> muscle fibres. ζ sys<strong>to</strong>le and ζ dias<strong>to</strong>le are fixedgeometrical parameters between 0 and 1, specifying <strong>the</strong>degree of sys<strong>to</strong>lic and dias<strong>to</strong>lic deformation respectively.We note that in <strong>the</strong> centre of <strong>the</strong> deformation ζ (x = x s2 ) =ζ 0 = R d /R 0 , i.e. <strong>the</strong> degree of deformation increases withdecreasing ζ 0 and consequently ζ sys<strong>to</strong>le

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!