Cardiovascular Fluid Mechanics - Lecture Notes 8W090

Total Page:16

File Type:pdf, Size:1020Kb

Cardiovascular Fluid Mechanics - Lecture Notes 8W090 Cardiovascular Fluid Mechanics - lecture notes 8W090 - F.N. van de Vosse (2013) Eindhoven University of Technology department of Biomedical Engineering Preface i Preface As cardiovascular disease is a major cause of death in the western world, knowledge of cardiovascular pathologies, including heart valve failure and atherosclerosis is of great importance. This knowledge can only be gathered after well understanding the circulation of the blood. Also for the development and usage of diagnostic tech- niques, like ultrasound and magnetic resonance assessment of blood flow and vessel wall displacement, knowledge of the fluid mechanics of the circulatory system is in- dispensable. Moreover, awareness of cardiovascular fluid mechanics is of great help in endovascular treatment of diseased arteries, the design of vascular prostheses that can replace these arteries when treatment is not successful, and in the development of prosthetic heart valves. Finally, development and innovation of extra-corporal systems strongly relies on insight into cardiovascular fluid mechanics. The lecture notes focus on fluid mechanical phenomena that occur in the human cardiovascular system and aim to contribute to better understanding of the circulatory system. ii Cardiovascular Fluid Mechanics - lecture notes In the introductory part of these notes a short overview of the circulatory system with respect to blood flow and pressure will be given. In chapter 1 a simple model of the vascular system will be presented despite the fact that the fluid mechanics of the cardiovascular system is complex due to the non-linear and non-homogeneous rheological properties of blood and arterial wall, the complex geometry and the pulsatile flow properties. An important part, chapter 2, is dedicated to the description of Newtonian flow in straight, curved and bifurcating, rigid tubes. With the aid of characteristic di- mensionless parameters the flow phenomena will be classified and related to specific physiological phenomena in the cardiovascular system. In this way difference be- tween flow in the large arteries and flow in the micro-circulation and veins and the difference between flow in straight and curved arteries will be elucidated. It will be shown that the flow in branched tubes shows a strong resemblance to the flow in curved tubes. Although flow patterns as derived from rigid tube models do give a good approx- imation of those that can be found in the vascular system, they will not provide information on pressure pulses and wall motion. In order to obtain this informa- tion a short introduction to vessel wall mechanics will be given and models for wall motion of distensible tubes as a function of a time dependent pressure load will be derived in chapter 3. The flow in distensible tubes is determined by wave propagation of the pressure pulse. The main characteristics of the wave propagation including attenuation and reflection of waves at geometrical transitions are treated in chapter 4, using a one- dimensional wave propagation model. As blood is a fluid consisting of blood cells suspended in plasma its rheological properties differ from that of a Newtonian fluid. In chapter 5 constitutive equations for Newtonian flow, generalized Newtonian flow, viscoelastic flow and the flow of suspensions will be dealt with. It will be shown that the viscosity of blood is shear and history dependent as a result of the presence of deformation and aggregation of the red blood cells that are suspended in plasma. The importance of non-Newtonian properties of blood for the flow in large and medium sized arteries will be discussed. Finally in chapter 6 the importance of the rheological (non-Newtonian) properties of blood, and especially its particulate character, for the flow in the micro-circulation will be elucidated. Velocity profiles as a function of the ratio between the vessel diameter and the diameter of red blood cells will be derived. In the appendix A, a short review of the equations governing fluid mechanics is given. This includes the main concepts determining the constitutive equations for both fluids and solids. Using limiting values of the non-dimensional parameters, simplifications of these equations will be derived in subsequent chapters. In order to obtain a better understanding of the physical meaning, many of the mathematical models that are treated are implemented in MATLAB. Descriptions of these implementations are available in a separate manuscript: ’Cardiovascular Fluid Mechanics - computational models’. Contents 1 General introduction 1 1.1 Introduction................................ 1 1.2 Thecardiovascularsystem. 2 1.2.1 Theheart............................. 3 1.2.2 Thesystemiccirculation. 7 1.3 Pressure and flow in the cardiovascular system . ... 9 1.3.1 Pressure and flow waves in arteries . 9 1.3.2 Pressure and flow in the micro-circulation . 13 1.3.3 Pressureandflowinthevenoussystem . 13 1.4 Simplemodelofthevascularsystem . 13 1.4.1 Periodic deformation and flow . 13 1.4.2 Thewindkesselmodel . 14 1.4.3 Vascularimpedance . 15 1.5 Summary ................................. 16 2 Newtonian flow in blood vessels 17 2.1 Introduction................................ 17 2.2 Steady and pulsatile Newtonian flow in straight tubes . ..... 18 2.2.1 Fully developed flow . 18 2.2.2 Entranceflow........................... 25 2.3 Steady and pulsating flow in curved and branched tubes . 27 2.3.1 Steadyflowinacurvedtube . 27 2.3.2 Unsteady fully developed flow in a curved tube . 33 2.3.3 Flowinbranchedtubes . 35 2.4 Summary ................................. 35 3 Mechanics of the vessel wall 37 3.1 Introduction................................ 37 3.2 Morphology................................ 38 3.3 Mechanicalproperties . .. .. .. .. .. .. .. 39 3.4 Incompressible elastic deformation . 42 3.4.1 Deformation of incompressible linear elastic solids ...... 42 3.4.2 Approximation for small strains . 43 3.5 Wallmotion................................ 45 3.6 Summary ................................. 47 iii iv Cardiovascular Fluid Mechanics - lecture notes 4 Wave phenomena in blood vessels 49 4.1 Introduction................................ 49 4.2 Pressureandflow............................. 50 4.3 Fluidflow................................. 51 4.4 Wavepropagation ............................ 53 4.4.1 Derivation of a quasi one-dimensional model . 53 4.4.2 Wave speed and attenuation constant . 56 4.5 Wavereflection .............................. 61 4.5.1 Wave reflection at discrete transitions . 61 4.5.2 Multiple wave reflection: effective admittance . 64 4.5.3 Vascular impedance and cardiac work . 67 4.6 Summary ................................. 68 5 Non-Newtonian flow in blood vessels 69 5.1 Introduction................................ 69 5.2 Mechanicalpropertiesofblood . 70 5.2.1 Morphology............................ 70 5.2.2 Rheological properties of blood . 72 5.3 Newtonianmodels ............................ 75 5.3.1 Constitutive equations . 75 5.3.2 Viscometricresults. 76 5.4 Generalized Newtonian models . 76 5.4.1 Constitutive equations . 76 5.4.2 Viscometricresults. 77 5.5 Viscoelasticmodels............................ 80 5.5.1 Constitutive equations . 80 5.5.2 Viscometricresults. 83 5.6 Rheologyofsuspensions . .. .. .. .. .. .. .. 86 5.6.1 Constitutive equations . 86 5.6.2 Viscometricresults. 88 5.7 Rheologyofwholeblood. .. .. .. .. .. .. .. 88 5.7.1 Experimental observations . 88 5.7.2 Constitutive equations . 90 5.8 Summary ................................. 91 6 Flow patterns in the micro-circulation 93 6.1 Introduction................................ 93 6.2 Flow in small arteries and small veins: Dv > 2Dc ........... 94 6.3 Velocityprofiles.............................. 94 6.3.1 Flow................................ 96 6.3.2 Effective viscosity . 96 6.3.3 Concentration........................... 97 6.3.4 Cellvelocity............................ 98 6.4 Flow in arterioles and venules : Dc < Dv < 2Dc ............ 98 6.4.1 Velocityprofiles. .. .. .. .. .. .. .. 98 6.4.2 Flow................................ 98 Contents v 6.4.3 Effective viscosity . 99 6.4.4 Concentration........................... 99 6.4.5 Cellvelocity............................ 100 6.5 Flow in capillaries: Dv < Dc ....................... 100 6.6 Summary ................................. 102 A Basic equations 103 A.1 Introduction................................ 103 A.2 Thestateofstressanddeformation. 104 A.2.1 Stress ............................... 104 A.2.2 Displacement and deformation . 104 A.2.3 Velocity and rate of deformation . 107 A.2.4 Constitutive equations . 108 A.3 Equationsofmotion . .. .. .. .. .. .. .. 109 A.3.1 Reynolds’transporttheorem . 109 A.3.2 Continuity equation . 110 A.3.3 The momentum equation . 111 A.3.4 Initial and boundary conditions . 112 A.4 Incompressibleviscousflow . 112 A.4.1 Newtonianflow.......................... 112 A.5 Incompressiblein-viscidflow. 113 A.5.1 Irotationalflow . 114 A.5.2 Boundaryconditions . 115 A.6 Incompressibleboundarylayerflow . 115 A.6.1 Newtonian boundary layer flow . 115 A.6.2 Initial and boundary conditions . 116 vi Cardiovascular Fluid Mechanics - lecture notes Chapter 1 General introduction 1.1 Introduction The study of cardiovascular fluid mechanics is only possible with some knowledge of cardiovascular physiology. In this chapter a brief introduction to cardiovascular physiology will be given. Some general aspects of the fluid mechanics of the heart, the arterial system, the micro-circulation and the venous system as well as the most important properties of the vascular tree that determine the pressure and
Recommended publications
  • Wall Thermal Inertia Effects of Pulsatile Flow in a Ribbed Tube: a Numerical Approach Amin Kardgar*,A, Davood Domiri Ganjib
    Journal of Heat and Mass Transfer Research 7 (2020) 85-94 Journal of Heat and Mass Transfer Research Journal homepage: http://jhmtr.semnan.ac.ir Semnan University Wall Thermal Inertia Effects of Pulsatile Flow in a Ribbed Tube: A Numerical Approach Amin Kardgar*,a, Davood Domiri Ganjib aDepartment of Mechanical Engineering, University of Mazandaran, Babolsar, Iran. bDepartment of Mechanical Engineering, Babol University of Technology, Babol, Iran. PAPER INFO ABSTRACT Paper history: In the present paper, the heat transfer of pulsatile flow in ribbed tube was investigated Received: 2020-02-24 numerically by considering the effect of thermal inertia of solid wall thickness. To this purpose, the CVFV technique with collocated grids arrangement was adopted to discretize Revised: 2020-07-01 momentum and energy equations. In order to avoid checker-board of pressure field in Accepted: 2020-10-16 numerical simulation, Chow and Rhie interpolation scheme was employed. The well- established SIMPLE (Semi-Implicit Method for Pressure Linked Equations) method was Keywords: utilized to handle velocity and pressure coupling in the momentum equation. Stone’s Strongly Pulsatile flow; Implicit Procedure (SIP) was used to solve the set of individual linear algebraic equations. Conjugate heat transfer; Womersley number, Reynolds number, velocity amplitude, and wall thickness ratio are four Womersley number; essential parameters that influence heat transfer and Nusselt number in pulsatile flow in a Wall thickness; ribbed tube. It was deduced by varying Womersley number Nu does not change. Nu enhances ribbed tube. almost 19% by augmentation of wall thickness ratio from 0.125 to 1. It was shown by increasing velocity amplitude from 0.1 to 0.8; Nu reduces almost 4.7%.
    [Show full text]
  • Effect of Dean Number on Heating Transfer Coefficients in an Flat Bottom Agitated Vessel
    IOSR Journal of Engineering May. 2012, Vol. 2(5) pp: 945-951 Effect of Dean Number on Heating Transfer Coefficients in an Flat Bottom Agitated Vessel 1*Ashok Reddy K 2 Bhagvanth Rao M 3 Ram Reddy P 1*..Professor Dept. of Mechanical Engineering ,Prof Rama Reddy College of Engineering & Technology Nandigoan(V) Pantacheru(M) Greater Hyderabad A P 2. Director CVSR College of Engineering Ghatkesar(M) R R Dist A P 3 .Director Malla Reddy College of Engineering Hyderbad A P ABSTRACT Experimental work has been reviewed using non- Newtonian and Newtonian fluids like Sodium Carboxymethal Cellulose with varying concentrations 0.05%,0.1%,0.15% and 0.2% with two different lengths (L=2.82m,L=2.362m) and outer diameter do=6.4mm,inner diameter di=4.0mm in an mixing vessel completely submerged helical coil. In our present study, the effect impeller speed, discharge ,flow behavior index(n) and consistency index (K) of test fluids with dimensionless curvature of the helical coil based on characteristic diameter were presented.. Keywords: Dean Number, Curvature, Heating Rates, Agitated Vessel I. Introduction To improve the performance of heat transfer rates, the fundamental aspect of flow patterns is an essential and important criteria in the helical coil design theory. The helical coil silent features consists of a inner diameter di and mean coil diameter Dm which is also known as pitch circle diameter of the coil. The ratio of coil pipe diameter to the mean coil diameter is known as dimensionless curvature .The ratio of pitch of the helical coil to the developed length of one turn is called non dimensional pitch .The angle which makes with plane geometry perpendicular to the axis of the one turn of the coil dimensions ic defined as helix angle.
    [Show full text]
  • Introduction to Biofluid Mechanics Portonovo S
    To protect the rights of the author(s) and publisher we inform you that this PDF is an uncorrected proof for internal business use only by the author(s), editor(s), reviewer(s), Elsevier and typesetter TNQ Books and Journals Pvt Ltd. It is not allowed to publish this proof online or in print. This proof copy is the copyright property of the publisher and is confidential until formal publication. CHAPTER 16 Introduction to Biofluid Mechanics Portonovo S. Ayyaswamy OUTLINE 16.1 Introduction e2 Exercises e71 16.2 The Circulatory System in the Acknowledgments e72 Human Body e2 Literature Cited e72 16.3 Modeling of Flow in Blood Vessels e18 Supplemental Reading e73 16.4 Introduction to the Fluid Mechanics of Plants e65 CHAPTER OBJECTIVES • To properly introduce the subject of biofluid • To review the parametric impact of the prop- mechanics including the necessary language erties of rigid, flexible, branched, and curved fl • To describe the components of the human cir- tubes on blood ow culation system and document their nominal • To provide an overview of fluid transport in characteristics plants • To present analytical results of relevant models of steady and pulsatile blood flow Fluid Mechanics http://dx.doi.org/10.1016/B978-0-12-405935-1.00016-2 e1 Copyright © 2016 Elsevier Inc. All rights reserved. To protect the rights of the author(s) and publisher we inform you that this PDF is an uncorrected proof for internal business use only by the author(s), editor(s), reviewer(s), Elsevier and typesetter TNQ Books and Journals Pvt Ltd. It is not allowed to publish this proof online or in print.
    [Show full text]
  • Extended Stokes Series for Dean Flow in Weakly Curved Pipes
    EXTENDED STOKES SERIES FOR DEAN FLOW IN WEAKLY CURVED PIPES A thesis presented for the degree of Doctor of Philosophy of Imperial College by Florencia Amalia Tettamanti Department of Mathematics Imperial College 180 Queen’s Gate, London SW7 2BZ June 24, 2012 2 I certify that this thesis, and the research to which it refers, are the product of my own work, and that any ideas or quotations from the work of other people, published or otherwise, are fully acknowledged in accordance with the standard referencing practices of the discipline. Signed: 3 Copyright Copyright in text of this thesis rests with the Author. Copies (by any process) either in full, or of extracts, may be made only in accordance with instructions given by the Author and lodged in the doctorate thesis archive of the college central library. Details may be obtained from the Librarian. This page must form part of any such copies made. Further copies (by any process) of copies made in accordance with such instructions may not be made without the permission (in writing) of the Author. The ownership of any intellectual property rights which may be described in this thesis is vested in Imperial College, subject to any prior agreement to the contrary, and may not be made available for use by third parties without the written permission of the University, which will prescribe the terms and conditions of any such agreement. Further information on the conditions under which disclosures and exploitation may take place is available from the Imperial College registry. 4 5 Abstract This thesis considers steady, fully-developed flows through weakly curved pipes using the extended Stokes series method.
    [Show full text]
  • (English Edition) a Review on the Flow Instability of Nanofluids
    Appl. Math. Mech. -Engl. Ed., 40(9), 1227–1238 (2019) Applied Mathematics and Mechanics (English Edition) https://doi.org/10.1007/s10483-019-2521-9 A review on the flow instability of nanofluids∗ Jianzhong LIN†, Hailin YANG Department of Mechanics, State Key Laboratory of Fluid Power and Mechatronic Systems, Zhejiang University, Hangzhou 310027, China (Received Mar. 22, 2019 / Revised May 6, 2019) Abstract Nanofluid flow occurs in extensive applications, and hence has received widespread attention. The transition of nanofluids from laminar to turbulent flow is an important issue because of the differences in pressure drop and heat transfer between laminar and turbulent flow. Nanofluids will become unstable when they depart from the thermal equilibrium or dynamic equilibrium state. This paper conducts a brief review of research on the flow instability of nanofluids, including hydrodynamic instability and thermal instability. Some open questions on the subject are also identified. Key words nanofluid, thermal instability, hydrodynamic instability, review Chinese Library Classification O358, O359 2010 Mathematics Subject Classification 76E09, 76T20 1 Introduction Nanofluids have aroused significant interest over the past few decades for their wide applica- tions in energy, machinery, transportation, and healthcare. For example, low concentration of particles causes viscosity changes[1–2], decreases viscosity with increasing shear rate[3], changes friction factors and pressure drops[4–6], and improves heat transfer[7–9]. Moreover, the unique flow properties of nanofluids are determined by the flow pattern. Heat transfer[10] and pressure drop[11] are also much lower and higher, respectively, in laminar flow than in turbulent flow. By adding particles to the fluid, the thermal entropy generation and friction are of the same order of magnitude as in turbulent flow, while the effect of heat transfer entropy generation strongly outweighs that of the friction entropy generation in laminar flow.
    [Show full text]
  • Blood Flow in Arteries
    November 8, 1996 13:58 Annual Reviews KUTEXT.DOC AR23-12 Annu. Rev. Fluid Mech. 1997. 29:399–434 Copyright c 1997 by Annual Reviews Inc. All rights reserved BLOOD FLOW IN ARTERIES David N. Ku G. W. Woodruff School of Mechanical Engineering, Georgia Institute of Technology, Atlanta, Georgia 30332-0405 ABSTRACT Blood flow in arteries is dominated by unsteady flow phenomena. The cardiovas- cular system is an internal flow loop with multiple branches in which a complex liquid circulates. A nondimensional frequency parameter, the Womersley num- ber, governs the relationship between the unsteady and viscous forces. Normal arterial flow is laminar with secondary flows generated at curves and branches. The arteries are living organs that can adapt to and change with the varying hemo- dynamic conditions. In certain circumstances, unusual hemodynamic conditions create an abnormal biological response. Velocity profile skewing can create pock- ets in which the direction of the wall shear stress oscillates. Atherosclerotic dis- ease tends to be localized in these sites and results in a narrowing of the artery lumen—a stenosis. The stenosis can cause turbulence and reduce flow by means of viscous head losses and flow choking. Very high shear stresses near the throat of the stenosis can activate platelets and thereby induce thrombosis, which can totally block blood flow to the heart or brain. Detection and quantification of by CAPES on 04/01/09. For personal use only. stenosis serve as the basis for surgical intervention. In the future, the study of arterial blood flow will lead to the prediction of individual hemodynamic flows in any patient, the development of diagnostic tools to quantify disease, and the design of devices that mimic or alter blood flow.
    [Show full text]
  • Secondary Flow Structures Under Stent-Induced Perturbations for Cardiovascular Flow in a Curved Artery Model
    SECONDARY FLOW STRUCTURES UNDER STENT-INDUCED PERTURBATIONS FOR CARDIOVASCULAR FLOW IN A CURVED ARTERY MODEL Autumn L. Glenn, Kartik V. Bulusu, and Michael W. Plesniak Department of Mechanical and Aerospace Engineering The George Washington University 801 22 nd Street, N.W, Washington, D.C. 20052 [email protected] Fangjun Shu Department of Mechanical and Aerospace Engineering New Mexico State University MSC 3450, P.O. Box 30001, Las Cruces, NM 88003-8001 [email protected] ABSTRACT by the complex geometry and inherent forcing functions, as Secondary flows within curved arteries with unsteady well as changes due to disease. Strong evidence linking forcing are well understood to result from amplified cellular biochemical response to mechanical factors such as centrifugal instabilities under steady-flow conditions and are shear stress on the endothelial cells lining the arterial wall has expected to be driven by the rapid accelerations and received considerable interest (Berger and Jou, 2000; Barakat decelerations inherent in such waveforms. They may also and Lieu, 2003; White and Frangos, 2007; Melchior and affect the function of curved arteries through pro-atherogenic Frangos, 2010). Secondary flow structures may affect the wall shear stresses, platelet residence time and other vascular wall shear stress in arteries, which is known to be closely response mechanisms. related to atherogenesis (Mallubhotla et al., 2001; Evegren et Planar PIV measurements were made under multi-harmonic al., 2010). non-zero-mean and physiological carotid artery waveforms at In curved tubes, secondary flow structures characterized various locations in a rigid bent-pipe curved artery model. by counter-rotating vortex pairs (Dean vortices) are well- Results revealed symmetric counter-rotating vortex pairs that understood to result from amplified centrifugal instabilities developed during the acceleration phases of both multi- under steady flow conditions.
    [Show full text]
  • CFD Modelling of Air Flow and Fine Powder Deposition in the Respiratory Tract
    CFD modelling of air flow and fine powder deposition in the respiratory tract Yun Hwan Kim A thesis in fulfilment of the requirements for the degree of Master of Philosophy School of Materials Science and Engineering Faculty of Science April 2017 THE UNIVERSITY OF NEW SOUTH WALES Thesis/Dissertation Sheet Surname or Family name: Kim First name: Yun Hwan Other name/s: Abbreviation for degree as given in the University calendar: M.Phil. School: School of Materials Science and Engineering Faculty: Science Title: CFD modelling of air flow and fine powder deposition in the respiratory tract Abstract This project was to investigate and observe characteristics of micro particles suspended in the ambient air or pharmaceutical aerosols with respect to the mechanisms of deposition in human airways under different inspiratory conditions. Such determination includes pattern observations of inspiratory flow-field of the air, particle trajectory during inspiratory conditions and particle deposition. Computational fluid dynamic (CFD) was employed to simulate above problems, aiming to observe flow-field of the inspiratory air and characteristic of flow turbulence in the respiratory tract as well as particle behaviour in the respiratory tract regarding to the particle deposition. In order to do so, three different airway models were employed for the simulations: two realistic airway models introduced by Kitaoka and Weibel airways model. The motion of micro-sized particles between 1~20 µm were simulated under the steady state two inlet- inspiratory conditions – inhalation condition (60 L/min) and breathing condition (18 L/min); to evaluate deposition efficiency. Inertial impaction was dominantly caused high density deposition of particles in upper tracheobronchial region, particularly in regions where daughter airways bifurcate.
    [Show full text]
  • On Dimensionless Numbers
    chemical engineering research and design 8 6 (2008) 835–868 Contents lists available at ScienceDirect Chemical Engineering Research and Design journal homepage: www.elsevier.com/locate/cherd Review On dimensionless numbers M.C. Ruzicka ∗ Department of Multiphase Reactors, Institute of Chemical Process Fundamentals, Czech Academy of Sciences, Rozvojova 135, 16502 Prague, Czech Republic This contribution is dedicated to Kamil Admiral´ Wichterle, a professor of chemical engineering, who admitted to feel a bit lost in the jungle of the dimensionless numbers, in our seminar at “Za Plıhalovic´ ohradou” abstract The goal is to provide a little review on dimensionless numbers, commonly encountered in chemical engineering. Both their sources are considered: dimensional analysis and scaling of governing equations with boundary con- ditions. The numbers produced by scaling of equation are presented for transport of momentum, heat and mass. Momentum transport is considered in both single-phase and multi-phase flows. The numbers obtained are assigned the physical meaning, and their mutual relations are highlighted. Certain drawbacks of building correlations based on dimensionless numbers are pointed out. © 2008 The Institution of Chemical Engineers. Published by Elsevier B.V. All rights reserved. Keywords: Dimensionless numbers; Dimensional analysis; Scaling of equations; Scaling of boundary conditions; Single-phase flow; Multi-phase flow; Correlations Contents 1. Introduction .................................................................................................................
    [Show full text]
  • Mass Transfer and Separation of Species in Oscillating Flows
    MASS TRANSFER AND SEPARATION OF SPECIES IN OSCILLATING FLOWS By AARON M. THOMAS A DISSERTATION PRESENTED TO THE GRADUATE SCHOOL OF THE UNIVERSITY OF FLORIDA IN PARTIAL FULFILLMENT OF THE REQUIREMENTS FOR THE DEGREE OF DOCTOR OF PHILOSOPHY UNIVERSITY OF FLORIDA 2001 Copyright 2001 by AARON M. THOMAS To Susan, Yesenia, and Dakota. ACKNOWLEDGMENTS guidance on this work I am most grateful to my advisor, Dr. Narayanan, for his and his counsel on a variety of topics that arose during our numerous conversations. some of I also thank Dr. Kurzweg and Dr. Jaeger for their help on understanding the aspects of this research. for a large part of my I am fortunate that Dr. Weaver has taken time to mentor me education. My parents and sisters have been very supportive of me in all of my work and decisions, and I know I can never repay everything that they have done for me. have made The friends that I have made both inside and outside this department my experience in Gainesville most memorable. Most importantly, my wife continually makes me realize that nothing has as much meaning without her by my side. My wife and my children properly balance my life and make me understand what is truly important. from under I gratefully acknowledge the support for this project received NASA grant number NAG3 2415 and for my financial support through an NSF Fellowship under grant number 9616053. IV TABLE OF CONTENTS page ACKNOWLEDGMENTS i v LIST OF TABLES viii LIST OF FIGURES « LIST OF SYMBOLS xiii 1.3 ABSTRACT xvii 1 INTRODUCTION OF THE PHYSICS 1 1.1 Physics of the
    [Show full text]
  • A Brief History of Arterial Blood Flow—From Harvey and Newton to Computational Analysis
    View metadata, citation and similar papers at core.ac.uk brought to you by CORE provided by Elsevier - Publisher Connector CLINICAL RESEARCH STUDIES From the Southern Association for Vascular Surgery Presidential address: A brief history of arterial blood flow—from Harvey and Newton to computational analysis Joseph P. Archie, Jr, PhD, MD, Raleigh, NC My education and interests have always pointed toward ships, and of fluids moving through vessels, like arterial fluid mechanics both as a researcher and as a clinical vascu- blood flow. The basis of solving these problems lies in lar surgeon trying to restore or maintain arterial blood accurately determining fluid flow patterns near solid walls. flow. In 1970 to 1971 I was a research fellow at the These problems are defined by physical laws represented Cardiovascular Research Institute of the University of by differential equations that have been known for cen- California Medical Center, San Francisco. The director of turies. Computational analysis, a numerical method of the Institute, Julius Comroe, wrote a small book entitled solving these equations, was developed years ago, awaiting Retrospectroscope: Insights Into Medical Discovery,1 in which the advent of high-speed computers to do the work. he makes a strong case for basic science research leading to When pulsatile flow in an arterial segment is smooth unexpected important findings, as opposed to targeted and undisturbed, the probability of myointimal hyperpla- research. The first correct description of human circulation sia, thrombosis, or atherosclerosis developing is low. The was given almost 400 years ago by William Harvey. During converse is true in segments that have disturbed flow.
    [Show full text]
  • A Computer Simulation of the Non-Newtonian Blood Flow at the Aortic Bifurcation
    Do21 9290/93 %S.W+.oO J. Biomechmics Vol. 26, NO. I, pp. 37-49. 1993. c#; 1992 Pergamon Press Ltd Pnnted m Great Britain A COMPUTER SIMULATION OF THE NON-NEWTONIAN BLOOD FLOW AT THE AORTIC BIFURCATION ZHENG Lou* and WEN-JEI YANG? *Transportation Research Institute, University of Michigan, Ann Arbor, MI 48109, U.S.A. and tMechanicil Engineering and Applied Mechanics, University of Michigan, Ann Arbor, MI 48109, U.S.A. Abstract-A two-dimensional numerical model was developed to determine the effect of the non-New- tonian behavior of blood on a pulsatile flow at the aortic bifurcation. The blood rheology was described by a weak-form Casson equation. The successive-over-relaxation (SOR) method was used to solve both the vorticity and Poisson equations numerically. It was disclosed that the non-Newtonian property of blood did not drastically change the flow patterns, but caused an appreciable increase in the shear stresses and a slightly higher resistance to both flow separations and the phase shifts between flow layers. NOMENCLATURE INTRODUCTION AR area ratio The curvatures, junctions and bifurcations of large D diameter and medium arteries are severely affected by athero- second invariant of the strain rate tensor Dll sclerosis. It has been suggested that fluid dynamics H half-width of a channel J, .i and J’ coordinate transformation coefficients may play a role in the genesis and progression of the I, reference length disease. The blood flows in these regions are disturbed Lb min minimum branch length and the arterial walls are exposed to either high or low parameter in the Papanastasiou’s weak form shear stresses.
    [Show full text]