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Lecture+7

Course: BIM 106, Winter 2012
School: UC Davis
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Valves 3-4 2/1/12 Heart cm2 4-6 cm2 Calcified heart valve. Rosenhek et al. (2000) NEJM www.heartcenteronline.com 1 2/1/12 St. Louis University School of Medicine www.echobyweb.com Mark Kittleson, UCD VMTH Ball and cage valve Bjork-Shiley valve Carpentier Edwards stented porcine valve Leeds polyurethane valve All images from Leeds University School of Mechanical Engineering 2 2/1/12 AXIAL VELOCITY...

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Valves 3-4 2/1/12 Heart cm2 4-6 cm2 Calcified heart valve. Rosenhek et al. (2000) NEJM www.heartcenteronline.com 1 2/1/12 St. Louis University School of Medicine www.echobyweb.com Mark Kittleson, UCD VMTH Ball and cage valve Bjork-Shiley valve Carpentier Edwards stented porcine valve Leeds polyurethane valve All images from Leeds University School of Mechanical Engineering 2 2/1/12 AXIAL VELOCITY PROFILES at systolic peak flow Native valve Valve prosthesis Native valve: "blunted" velocity profiles; Prosthetic valve: "two jet" velocity profiles Native valve Valve prosthesis Axial WSS is higher downstream of the aortic valve prosthesis when compared to the native configuration (note the difference is measurement scales!) 3 2/1/12 Velocity profile of flow through normal healthy heart valve Velocity profile of flow through mechanical heart valve Images courtesy of BIDMC, Boston, MA Blood vessels arent just tubes! 4 2/1/12 Dynamics of flow in the heart 5 2/1/12 Curved Vessels Curved Vessels a = R De = Re A scaling of the Re by the ratio of the tube radius (a) to the radius of curvature (R). velocity profile 6 2/1/12 Curved Vessels For De<34 and <<1: v De 2 cos rz r =a = 1 + and 4a 73728 r r =a = v De sin 4a 72 The wall shear stress rz due to the primary flow is greatest at the outer wall and lowest at the inner wall. r arises from the secondary flow and is smaller than the value for the main component. 7 2/1/12 Changes in flow at branches Flow separation areas that diverge from fully-developed flow, often presenting as regions in which some of the fluid moves in a reverse direction. Separation point the location at which flow first reverses direction. Conversely, the reattachment point is the location where all of the fluid again moves in the same direction. Flow through carotid 70% of flow from common carotid goes into internal carotid! 32% of area of CCA 50% of area of CCA 120% of area of CCA 8 2/1/12 David Steinman Univ. of Toronto Pulsatile flow in an idealized normal carotid bifurcation In this animation, particles shaded blue represent blood flowing to the left, highlighting the region of recirculating blood in the carotid bulb. This is where atherosclerotic plaques commonly occur, suggesting a link between hemodynamics and vascular disease. David Steinman Univ. of Toronto Computational imaging of pulsatile flow in a normal human carotid bifurcation Magnetic resonance imaging (MRI) of a live subject provides the boundary conditions (i.e. geometry and flow rates) for a computational fluid dynamic (CFD) simulation of the blood flow patterns. In this animation, streak length and color intensity are proportional to the blood velocity. Color distinguishes particles exiting the external and internal branches. Note the complex swirling flow patterns and mixing of red and blue particles. 9 2/1/12 Putative profiles in endothelial gene expression Atheroprotective: Anti-inflammatory Anti-thrombotic Anti-oxidative Anti-proliferative Nonadhesive Atherosusceptible: Pro-inflammatory Pro-thrombotic Oxidative Proliferative Adhesive David Steinman Univ. of Toronto Image-based CFD of a mildly diseased carotid bifurcation Particle path animation of pulsatile flow in a mildly diseased carotid bifurcation CFD model reconstructed from black blood MRI. 10 2/1/12 David Steinman Univ. of Toronto Pulsatile flow in two models of the stenosed carotid bifurcation Different patterns of post-stenotic recirculation can be observed in models having the same stenosis severity but different stenosis geometries. Investigators are currently investigating whether geometric or hemodynamic information can help to better identify patients at risk of stroke, since such flow patterns may provide ideal conditions for the formation of the blood clots that cause many strokes. David Steinman Univ. of Toronto Computational imaging of pulsatile flow in a canine aneurysm This aneurysm model was reconstructed from an MR angiogram of a dog with an implanted vein-pouch aneurysm. 11 2/1/12 ECs responsive Sato are M et al. in Tissue Engineering for Therapeutic Use 4, Ikada Y, Shimizu Y, eds., 2000, p. 123. ECs are responsive Butcher, J. T. et al. Arterioscler Thromb Vasc Biol 2004;24:1429-1434 Images of PAECs (A, C, E, and G) and PAVECs (B, D, F, and H) in static and steady fluid flow environments 12 2/1/12 Spatial scaling of endothelial phenotypes Davies et al. Biorheology 39 (2002), 299-306. Passerini et al. PNAS 101 (2004), 2482-2487. Davies et al. Biorheology 39 (2002), 299-306. Davies et al. Circ Res 92 (2003), 359-370. Helmke et al. Circ Res 86 (2000), 745-752. ECs are responsive Disturbed flow Undisturbed flow NFB (p65) GPX3 Ab Passerini et al. (2004) PNAS 101:2482-2487 13 2/1/12 Progression of atherosclerosis ECs are responsive Nerem RM et al. Am J Med Sci 1998; 316:169-175. 14 2/1/12 Increased WSS increased NO Increased NO increased dilation/ diameter Fluid ow applied perpend icular to the direc3on of collagen bril orienta3on. (A) Sheared, unstrained. (B) Sheared, strained. (C) Unsheared, unstrained sample. Imber3 et al., The Response of Endothelial Cells to Fluid Shear Stress Using a CoCulture Model of the Arterial Wall. Endothelium (2002). 15 2/1/12 ECs are responsive Endothelial cell migra0on assay Peter Lelkes, Drexel Revzan et al., Steady Unidirec0onal Laminar Flow Inhibits Monolayer Forma0on by Human and Rat Microvascular Endothelial Cells, Endothelium (2004). ECs are responsive Kenneth Barbee, Drexel The three-dimensional surface topography of an endothelial monolayer aligned by flow in vitro. The surface geometry was measured by AFM on living cells. Computational Fluid Dynamics was used to calculate the shear stress distribution on the endothelial surface due to flow over the surface. Shear stress values, shown in pseudocolor, vary from the nominal wall shear stress by +/29%. 16 2/1/12 ECs are responsive h = 3.5 m h = 1.8 m = 1 + (h havg ) w where, is the local shear stress w is the wall shear stress in the absence of the cell h-havg is the variation in surface height about the mean over a single cell is a constant 0.120 m-1 for cells not exposed to flow 0.08 m-1 after a 24-h exposure of cells to flow Determine the maximum shear stress acting on a cultured endothelial cell exposed to a shear stress of 15 dyne/cm2 when (1) the cell has not been exposed to flow in culture (2) after exposure to flow for 24 hours. = 1 + (h havg ) w dyne cm 2 CASE 1 CASE 2 = 0.12 m 1 = 0.08m -1 h = 3.5m dyne = 21.3 2 cm h = 1.8m dyne = 18.2 2 cm w = 15 17 2/1/12 Therapeutic intervention and device failure Therapeutic intervention and device failure 18 2/1/12 hLp://www.biouids.net/media.html Implications of Responsive ECs in Tissue Engineering Tangential pressure Normal pressure Biomimetic conditions accelerated adaptation at 28 days compared to static conditions demonstrated by: 1. Improved bursting strength 2. Reduced losses in wall thickness and suture strength Hoerstrup et al., Eur J Card Surg 2001; 20:164-169. 19 2/1/12 Implications of Responsive ECs in Tissue Engineering xenograft autologous/preimplantation Niklason et al., Science (1999) 284:489 - 493 autologous/ postimplantation 24 d 20 2/1/12 EXAM 1 Topics covered Chapter 1: Introduc3on to Biotransport Transport in the body (types, deni3ons) Chapter 2: Conserva3on Rela3ons and Momentum Balances Fluid sta3cs (cor3cal & surface tension) Using mass, momentum, and force balances to nd velocity prole, Q, and shear stress for various geometries Newtons Law of Viscosity; Poiseuilles Law Rheology of blood Chapter 3: Conserva3on Rela3ons for Fluid Transport Equa3on of con3nuity (conserva3on of mass) Equa3ons of mo3on (NavierStokes) Dimensional analysis (Buckingham Pi Theorem) Chapter 4: Approximate Methods for Analysis of Complex Flow Bernoulli equa3on (simplied) Chapter 5: Fluid Flow in the Circula3on and Tissues Flow in Curved Vessels Responsiveness of ECs to ow 21
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