Papafaklis Michail_Blood Flow Simulation in Coronary Arteries

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    Computational Fluid Dynamics

    A new research tool for assessing

    coronary physiology

    Michail I. Papafaklis MD, PhD

    Michailideion Cardiac Centre

    Medical School, University of Ioannina

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    Summary

    Physiology and Hemodynamics

    Computational analysis of blood flow and

    blood flow simulation in coronary arteries

    The role of hemodynamic forces incoronary artery disease

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    Physiology

    Cardiology Is FlowCardiology Is Flow

    The primary aim of the cardiovascular system is to drive, control andmaintain blood flow to all parts of the body

    Complexity of the circulatory system

    The heart is an intermittent pump blood flow in the arterial

    circulation is pulsatile

    The blood vessels are branched, distensible tubes of various

    dimensions The blood is a complex suspension

    Richter and Edelman Circulation2006

    Despite this complexity, the function of the circulatory

    system can be explained by the principles of basic

    fluid mechanics that apply to non-biologic systems,

    such as household plumbing systems

    http://upload.wikimedia.org/wikipedia/en/f/f9/Waterpipes.jpeg
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    Hemodynamics

    The term hemodynamicshemodynamics describes the physicalprinciples governing pressure, flow and resistance as

    they relate to the cardiovascular system, and the flow ofblood in the vessels

    Blood flow is determined by two factors: A pressure difference between the two ends of a vessel or group

    of vessels

    The resistance that blood must overcome as it moves throughthe vessel or vessels

    Pressure (P) = Flow (Q) Resistance (R)1 peripheral resistance unit (PRU)=100mmHg/100mlsec-1

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    Fluid Mechanics

    Stress (Pa) = Force (Nt)/Surface (m2)

    Shear stress (tangential component)

    Normal stress (vertical component)

    Angular deformation

    (strain) of fluids is

    caused by shear stresses

    Newtonian fluidsShear stress = viscosity Strain rate

    Non-Newtonian fluids

    Viscosity is not constant, but depends on the strain rate

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    Hemodynamics

    Components of hemodynamic stress

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    Hemodynamics

    Rheological properties of blood Whole blood is a

    concentrated suspension

    of blood cells in plasma

    (electrolytic solution of

    inorganic and organic

    molecules, and proteins)

    Viscometric properties of

    whole blood Depend on Hct

    Depend on the strain rate

    (non-Newtonian fluid)mainly in low strain rates

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    Hemodynamics

    Poiseuille flowQ=(/128)Pd4/L w

    = 32Q/d3

    Assumptions

    Blood is considered to behave as a Newtonian fluid

    The vessel is considered to be a straight tube withrigid walls and constant circular cross-section

    Blood flow is considered

    to be steady, laminar andfully-developed

    Jean Louis Marie Poiseuille (1799-1869)Gotthilf Heinrich Ludwig Hagen (1797-1884)

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    Coronary circulation

    The coronary circulation net is the denser

    capillary net in the human body The resting coronary blood flow is

    about 225 ml/min or about 0.8 ml/g

    of the heart muscle During exercise conditions the

    coronary blood supply can increase

    by 4 to 10 times the resting bloodflow rate

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    Coronary circulation

    Arteries Coronary arteries are tubes with a non-circular

    cross-section, which is progressively reduced in size

    going distally (tapering) Several bifurcations and branches are present

    The arterial wall is distended in every heartbeat(pressure wave)

    Coronary arteries are situated on the epicardium andfollow its curvature

    The geometry of the system is dynamic because of the

    constant movement of the heart during every cardiaccycle

    Coronary blood flow is pulsatile

    Most flow (mainly for the left coronary artery) occurs

    during the diastolic phase of the cardiac cycle

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    Hemodynamics

    Differential analysis Detailed description of the flow field and accurate computation of

    hemodynamic parameters in all flow situations

    Cartesian coordinates

    Continuity equation Navier-Stokes equation

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    Computational Fluid Dynamics

    Computational techniques (use of computers) applied for

    the numerical solution of the differential flow equations,since a direct analytic solution for complex flow fields isnot feasible

    A practical and reliable tool for studying the time-varying,3D blood flow patterns in complex arterial geometries

    CFD computations are based on a much more complexflow model compared to Poiseuille flow and provide

    useful info on spatial and temporal changes ofhemodynamic parameters (e.g. flow velocity near thevessel wall and shear stress)

    CFD allows the simulation of the hemodynamicenvironment under controlled conditions

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    Computational Fluid Dynamics

    General Principles of the method

    In CFD modelling a complex geometry is

    discretized into a large number of smallerbut regular (typically, tetrahedral orhexahedral) elements computational

    mesh Numerical solution of the differential equations

    of motion at the nodes connecting these

    elements after applying certain boundaryconditions

    Computation of hemodynamic quantities

    (pressure, velocity components, shear stress)

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    Computational Fluid Dynamics

    Application in human vessel models

    CFD was initially applied in theoretical idealized

    computer models of various vessels (aorta, carotids,coronary arteries, aorto-coronary bypass grafts)

    These idealized computer vessel models were based onmean measurements from cadaver specimens or

    angiographic data However, normal anatomic differences from one person

    to another cause great variations in terms ofhemodynamics and necessitate the incorporation of the

    detailed arterial characteristics of every person in CFDmodelling

    In order to achieve blood flow simulation for every vesseland every patient, the most important element is real 3D

    reconstruction of the lumen vessel patientpatient--specificspecificarterial models

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    Computational Fluid Dynamics

    3D coronary artery reconstruction Anatomic characteristics of coronary arteries

    Small dimension (mean diameter 3mm)

    3D complex (epicardial curvature) and time-dependent geometry

    (heart movement)

    Fusion of coronary angiography and intravascular

    ultrasound (IVUS) data

    Coronary angiography

    Geometry of coronary artery lumen

    Position and geometry of IVUS catheter in the arterial lumen

    IVUS

    Detailed geometry of the lumen and arterial wall (atheromatic

    plaque) in every cross-section

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    Computational Fluid Dynamics

    3D coronary artery reconstruction

    +

    Point cloud of the lumen

    Point cloud of the

    outer vessel wall

    Bourantas et al. Comput Med Imaging Graph2005

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    Computational Fluid Dynamics

    3D coronary artery reconstruction

    Point clouds of the

    lumen &&outer vessel wall

    3D lumen && outer

    vessel wall

    reconstructionLAO view

    3D lumen && outer

    vessel wall

    reconstructionRAO view

    Papafaklis

    MI. PhD Thesis 2008

    Bourantas et al. Comput Med Imaging Graph2005

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    Computational Fluid Dynamics

    Mesh Generation Discretization of the

    complex arterial

    lumen intohexahedrons, whosesize and distributionlargely govern theaccuracy of thecomputed velocityfield

    Papafaklis MI. PhD Thesis 2008

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    Computational Fluid Dynamics

    Fluid properties & boundary conditions Definition of fluid properties (blood)

    Homogeneous Newtonian / non-Newtonian fluid Density (): 1050 kg/m3

    Dynamic viscosity (): 0,0035 Pasec Boundary conditions

    Laminar flow

    Steady (e.g. Q=1ml/sec) /Pulsatile flow

    Velocity profile (flat / parabolic) at the inlet of the

    artery

    Non-slip condition at the arterial wall

    Pressure condition at the outlet of the artery

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    Computational Fluid Dynamics

    Numerical Solution Discretization of the

    equations for each

    control volume

    (hexahedron)

    Initial approximate

    solution at each node ofthe computational mesh

    Continuous iterations of

    the solution

    Error minimization and

    convergence to the

    exact solution

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    Computational Fluid Dynamics

    Blood flow simulation

    3D lumen

    reconstructionand

    blood particle

    tracking in aright coronary

    artery

    Papafaklis MI. PhD Thesis 2008

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    Computational Fluid Dynamics

    Blood flow simulation Streamlines in a right coronary artery lumen

    Papafaklis MI. PhD Thesis 2008

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    Computational Fluid Dynamics

    Blood flow simulation Velocity profiles in lumen cross-sections

    Papafaklis MI. PhD Thesis 2008

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    Computational Fluid Dynamics

    Blood flow simulation 3D colour map of shear stress distribution

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    Computational Fluid Dynamics

    Blood flow simulation Angioscopic view

    Wahle et al. SPOIE Proceedings 2001

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    CFD is a technological tool which in combinat ionw ith imaging modalities can accurately simulate the

    hemodynamic environment in human arteries

    Why do we need to

    simulate blood

    flow in the

    arteries ?

    Because it

    is fancy ! ? !

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    Hemodynamic forces &

    Atherosclerosis

    Chronic, inflammatory and fibroproliferative disease mainly of large-

    and medium-sized arteries Remains the leading cause of death in the developed world

    Despite the systemic nature of its associated risk factors (i.e.hypertension, smoking, hyperlipidemia, diabetes mellitus, social

    stress), atherosclerosis is a site specific disease and itsmanifestations are focal and eccentric

    Specific regions are affected: branch points (outer edges of bloodvessel bifurcations) and the inner walls of curved arteries

    Within each patient, each coronary obstruction progresses,regresses, or remains quiescent in an independent manner

    Local factors (hemodynamic forces) play a major role in the regionallocalization of atherosclerosis

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    Hemodynamic forces &

    Localization of atheromatic plaques

    A i i f l h i h

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    Association of low shear stress w ithatherosclerosis

    in coronary arterial segments

    Van Langenhove et al. Circulation2000

    A i ti f l h t ith

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    Association of low shear stress w ithatherosclerosis

    in coronary arterial segments

    Stone et al. Eur Heart J2007

    Serial intracoronary study (3D anatomy and CFD) inpatients with stable angina revealed plaque progression

    in areas with low shear stress

    A i ti f l h t ith

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    Association of low shear stress w ithatherosclerosis

    in left main coronary artery bifurcation

    In vivo study using 3Dreconstruction and CFDdemonstrated anassociation of disturbedflow and low shearstress with increased

    plaque thickness Plaque thickness was

    found to be inverselyrelated to shear stress in

    five patients

    Papafaklis

    et al. Int

    J Cardiol

    2007

    Papafaklis et al. (abstr) Heart2007

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    Shear stress and

    Vulnerable plaques Low SS has been lately found in a serial IVUS study (coupled with

    CFDanalysis) in swines to be an independent predictor of plaquelocation, development and progression to a high-risk plaque with:

    Intense lipid accumulation

    Inflammation

    Thin fibrous cap

    Internal elastic lamina fragmentation

    Media thinning

    Excessive expansive remodelling

    The magnitude of low SS at baseline was associated with theseverity of high-risk plaque characteristics

    Low SS

    IntenseinflammationExcessiveexpansiveremodelling

    TCFA

    Chatzizisis et al. Circulation2008

    Role of shear stress in

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    Role of shear stress inin-stent restenosis

    Bare metal stents Neointima thickness is inversely related to shear stress

    Low shear stress areas

    must be considered as

    areas with a higher

    probability for neointimalhyperplasia to be present

    and more prominent

    Adjunctive brachytherapy was found to reduce the effect of shear

    stress on neointimal hyperplasia

    Areas with sufficient irradiation and thus, minimal neointimal thickness

    minimal effect of SS on in-stent restenosis because of brachytherapyinduced cell death

    Wentzel

    et al. Circulation2001

    Papafaklis et al. (abstr)J Am Coll Cardiol2006

    Papafaklis et al. Int J Cardiol2008

    Role of shear stress in

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    Role of shear stress inneointima distribution

    Drug-eluting stents Low shear stress is associated with neointimal hyperplasia

    Shear stress does not seem to play a role in tissue regression and

    lumen enlargement which occur after drug-eluting stent implantation

    Gijsen

    et al.Am J Cardiol 2003

    Papafaklis et al. (abstr)

    J Am Coll

    Cardiol

    2008

    Papafaklis et al.

    Heart Vessels 2007

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    Clinical Implications

    Detection of vulnerable plaques at an earlier stage by

    adding CFD techniques to current imaging methods:

    invasive (IVUS-based virtual histology and palpography,

    thermography, intravascular MRI, angioscopy)

    noninvasive (MSCT, MRI, PET)

    Assess the vulnerability risk of a vessel or patient Selective invasive treatment (use of stents to stabilize

    high-risk plaques ? ? ?)

    Limitation: vulnerable plaques are not single localized lesionsrestricted to one coronary artery only

    Prognosis of probable locations of restenosis after stent

    implantation

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    Conclusions

    Low shear stress explains the focal susceptibility of thearterial system to atherosclerosis and neointima

    distribution following stent implantation

    Incorporation ofin vivoin vivohemodynamic measurements by

    using CFD in current diagnostic methods may increaseour knowledge on the pathobiology of coronary arterydisease with beneficial implications for the vulnerablepatient

    Future: Create a prognostic model for vulnerableplaques based on hemodynamic parameters

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    Thank you