Ansys 14.5 Magnitude

Ansys 14.5 Magnitude



 
 
 
 
 
 
 

Ansys 14.5 Magnitude

as shown in fig 10, re = 570 is already sufficiently low to result in a steady state flow and the secondary flow velocity is even larger than the axial flow velocity. in addition, the pressure gradient in the graft is much smaller than the systolic pressure gradient in the host artery (see fig 11). as a result, there are only minor interactions between the flow patterns in the host artery and the graft. the fact that the secondary velocity magnitude is actually larger than the axial velocity in the host artery indicates that the flow is actually recirculating in a larger section of the graft.

next, the effects of changing the graft angle (α = 0, 60°) on the flow patterns were investigated. the results are shown in fig 12 and fig 13. as shown, the flow patterns and the secondary velocity distributions on the host artery are relatively unaffected by graft angle. with an increasing angle, the secondary velocity magnitude decreases, but the regions where secondary flow is present are generally larger. the recirculation region in the graft is also shifted away from the graft wall in a non-linear manner. this is because, with increasing graft angle, the recirculation region is pushed away from the graft wall and consequently, the host artery flow-roung areas (cf. the shear layer regions in fig 13) become larger.

the results of the unsteady flow simulations conducted at re = 570 are shown in fig 14 and fig 15. compared to the flow patterns in the previous unsteady flow simulations at re = 570, the secondary velocity magnitude is higher and the recirculation region is wider. in addition, the secondary flow moves slightly away from the wall towards the centre of the host artery, rather than moving towards the wall. this can be attributed to the fact that the high secondary velocity in the lumen causes the flow to move towards the centre of the graft.

while ansoft continuum solver technology is exciting and exciting, the larger strategic goal of customers to use hfss as an integral part of their entire design and simulation process remains unchanged. ansys is committed to transforming design into engineering as early as possible in the design process, giving engineers and researchers quick and useful results with the ultimate goal of delivering shorter design cycles and faster designs.
for completeness, the wss map for the triple-ridge case is below. you can see that the triple ridge case is qualitatively different from the single and double ridge cases. a high shear zone is visible on the arterial floor, distal to the stagnation point, where the maximum normalised wss magnitude is approximately 85% and 50% higher than that in the single and double ridge cases, respectively. higher number of ridges, however, would reduce the cross-sectional area and consequently increase the resistance against the flow. they may also result in an increase of pressure at the leading edge of the ridges, which can lead to deposition of cholesterol, calcium, cellular debris and fatty substances [46].
geometry scale presents yet another challenge. with todays higher frequency content, ignoring em coupling of an ic to its packaging can no longer be safely ignored. but in such complex em systems, geometry detail scales from microns to millimeters presenting challenges with mesh tolerance. creating a finite element mesh that scales up through orders of magnitude in feature size across multiple types of designs while maintaining a faithful representation of the geometry everywhere is extremely challenging and a barrier to engineering simulation.
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