C W Cryer

P P Lunkenheimer

Mathematical Mo delling of the

Cardiovascular System   

Mathematical Mo delli ng

of the

Cardiovascular System

Version

Septemb er



Colin Walker Cryer Paul Peter Lunkenheimer

Abstract

We describ e the problem of mo delling the cardiovascular system and give current refer

ences

AMS Sub ject Classication Z C C C

Keywords Mo delling ventricular mechanics biomechanics cardiovascular system

mathematics

Institut fur Numerische und instrumentelle Mathematik Westfalische WilhelmsUniversitat Einste

instrae Munster email cryermathunimuensterde



Exp erimentelle Thorax Herz und Gefachirurgie Domagkstr Munster

Contents

Prologue

I Biomechanics

The Human Machine

Energetics

Mechanics

II The Heart

Intro duction

The

The Heart

Visualization

Disease and Pathology

ComparativePhysiology

History of Cardiology

The Cardiac Cycle

Intro duction

The Cardiac Cycle

Ventricular lling

Isovolumetric contraction

Ejection

Isovolumetric Relaxation

Global Motion of the Heart

The

Heart Sounds and Murm urs

Concluding Remarks

The Structure of the Myo cardium

Intro duction

Connective Tissue

Previous Mathematical Mo dels

The Pericardium Endo cardium and Epicardium

Exp erimental Observations

The Ventricular Function Curve

In Vivo Stress Measurements

In Vivo Strain Measurements

Coronary

Intramyo cardial Pressure

Other Exp erimental Observations

Pericardial Eusion

Hyp ervolemia

Oligemia

Arterial Hyp ertension

Aortic Coarctation

Aortic Stenosis

Pulmonary Stenosis

Idoventricular Rhythms

Coronary Occlusion Myo cardial

Cardiac Valves

Aortic Regurgitation

Mitral Insuciency

Mitral Stenosis

III Mathematical Mo delling of the Heart

In tro duction

The Field Equations

The Constitutive Equations

The Goal of Mo delling

Diastolic Expansion

Ventricular Blo o d Pressure

Myo cardial stress

Elastic Recoil

Residual Stress

Ventricular Geometry

Muscle Mechanics

Intro duction

The Phenomological Approach

The Fenn eect

Feng eect

Classic Results

Molecular Muscle Mechanics

Ventricular Interaction

PassiveMyo cardium

Exp erimental Metho ds and Results

Constitutive Equations

StrainEnergy Functions

Bovendeerd

Smaill and Hunter

Inverse Metho ds for Parameter Estimation

Cardiac Mechanics

Intro duction

The Comp onents of the Hearts Wall

Exp erimental StressStrain Measurements

ConstitutiveLaws

Hydraulic Eects

Myo cytes

Mo delling the Fibre Architecture of the Myo cardium

Foliations

Top ology

Geo desics

Mo dels with Spherical Geometry

The Law of Laplace

Spherical Mo dels

Analytical Work

Comparison of Mo dels

Mo dels with Cylindrical Geometry

Mo dels with Spheroidal Geometry

Mo dels with Additional Features

The Pericardium

Fibres

Hydrostatic Skeletons and Muscular Hydrostats

FluidFibre Mo dels

Systolic Contraction

Fibres

Treatment of the Band Structure

Poro elastic Mo dels

Other Factors

Numerical Mo dels

Numerical Metho ds

Prop erties of Blo o d

Fluid Flow in the heart

Intro duction

Numerical Metho ds

The ImmersedBoundary Metho d

EulerLagrangian Formulation

Vortex and whirl ows

Mo delling the Heart Valves

Intro duction

The Mitral Valve

The Aortic Valve

Architecture of the Aortic Valve Leaets

Articial Valves

Valve Vibration

Mo delling other Ventricular Pro cesses

Electrical and Electrophysiological Activity

Oxygen Diusion

Heat Flow

ComparativePhysiology of the Heart

Intro duction

Sources of Data

Allometric Equations

Dierences Between Mammalian

Concluding Remarks

Mo delling the Global Motion of the Heart

The Heart as a Mechanical Pump

Cardiac Energetics

Growth

Miscellaneous Topics

Heart Sounds

The IntervalForce Relationship

Assistance and Replacement

Anrep Eect

Gregg Eect

IV Mathematical Mo delling of the Circulatory System

Intro duction

The Arterial System

Intro duction

The Pulmonary Circulation

Intro duction

The V enous System

The

The Micro circulation

V Mathematical Mo delling of the Entire Cardiovascular Sys

tem

Intro duction

Mo dels of the Cardiovascular System

Control

Design Principles of the Cardiovascular System

Optimization of Biological Structures

A The SI System

A Physical Units

A Units

A Useful conversion factors

A Physical Quantities

B Dimensional Analysis

B Dimensional Analysis

C Elementary Concepts from Physical Chemistry

DPhysiology

E Cardiovascular Data

E Man

E Woman

E Dog

F Mathematical Tools

F Dierential geometry

F Geo desics

F Geometric Measure Theory

F Top ology

F Knots

F Partial Dierential Equations

F Singularities

F Chaos

G Mechanics

G Applied Mechanics

G Thermo dynamics

G Contiuum Mechanics

G Elasticity

G Fibrereinforced Materials

G Elastic Solids with Microstructure

H Biomechanics

H General References

H Biomaterials

H Mathematical Biology

H Pattern Formation

H Bio energetics

H Kinesiology

I Computer Graphics

J Numerical Metho ds

J Finite Elements

K Sources

K Sources of Preserved Hearts

K Bo oks Rep orts Theses

K Journals

K So cieties

K Deutsche Literatur

K DeutschEnglischVerzeichnis

K Diplomthemen

L Worksheets

L Questions

L Availability of Journals etc in Munster

L Literature Searched

L PhD Theses

L Corresp ondance

M Biomathematics

Prologue

App endix

References

Concepts

List of Figures

The simplied circulatory system

The plumbing of the normal heart

The lo cation of the heart

Crosssections of the heart

The cardiac cycle

Simplied diagram of isolated dog heartlung preparation of Starling

The ventricular function curve

Horts Mo del for elastic recoil

Contractile b ehaviour of isolated myo cardial muscle

Stressextension relations for left ventricular midwall sp ecimen during st

th and th cycles of equibiaxial loading Cycle p erio d sec and sp eci

men thickness mm The solid lines indicate the order of loading in the

crossb er direction for clarity these are omitted in the b er direction

The Law of Laplace

Blo o d ow a

Blo o d ow b

Chapter

Prologue

The human heart is a pump which converts metab olic energy to mechanical work and

generates the pressure that drives the blo o d throughout the b o dys circulation system It

can do so for years or more with a rate varying from ab out litresmin in an adult

human male at rest to litresmin in Olympic athletes For an organ which is ab out the

size of a st this is a remarkable achievement

In we b egan a longterm pro ject to examine ways of mo delling the heart sp ecically

its mechanical prop erties This requires several steps

The relevant features of the heart must b e formulated

Quantitative exp erimental data must b e obtained

Appropriate mathematical mo dels must b e constructed

As far as p ossible the mo dels should b e analyzed mathematically

Numerical metho ds must b e used to obtain quantitative results

After comparing theory and exp eriment the mo dels must if necessary b e mo died

There is an extensive literature on this sub ject Nevertheless we hop ed to b e able to make

a meaningful contribution by taking advantage of the combined physiological morpho

logical and mathematical knowledge of the authors Particular emphasis was to b e placed

on the bre architecture of the myo cardium and its inuence on ventricular mechanics

Since the mathematician amongst us CWC was a newcomer to the eld it was natural to

b egin by reading the literature and making notes As the breadth of the sub ject b ecame

apparent the notes evolved into the present text whichmay therefore b e particularly

useful to applied mathematicians who wish to contribute to a fascinating area While our

principal in terest lies in the mechanics of the heart this cannot b e considered in isolation

and we include descriptions sometimes extremely brief of the often fascinating problems

connected with other parts of the cardiovascular system

The text is intended for use in a course on the mathematical mo delling of the cardio

vascular system for mathematics students with little knowledge of physiologyphysics

or chemistry Hence some basic background information with references to additional

sources is given in app endices In the course of acquainting himself with the sub ject

CWC found information such as the addresses of cardiovascular so cieties sources of ma

terials etc to b e very useful and this is also included In this waywehopetohave

provided not just a textb o ok but also a sourceb o ok for anyone entering the eld

The mo delling of the cardiovascular system is the sub ject of several recent b o oks for

engineers and physicists Here we emphasize the mathematical asp ects

By giving sp ecic examples which can then b e sub jected to mathematical and nu

merical analysis

By drawing attention to op en problems

By drawing attention to p otentially useful mathematics

The text diers from many b o oks on mathematical mo delling in that we assume an

adequate knowledge of partial dierential equations such as could b e provided bya two

semester course on the theory of partial dierential equations and their numerical solution

In the past mathematicians have contributed relatively little to the sub ject and one may

very well ask whether there is anything that they can do which could not b e done b etter

by the physicists biomechanical engineers etc already working in the eld Wewould

like to think so and hop e that this b o ok will help to bring this ab out One source of

encouragement is our exp erience that given the opp ortunity and appropriate help many

mathematics students welcome the opp ortunity to mo del biological pro cesses

We are grateful to Butterworth and Heinemann Ltd for gran ting p ermission to repro duce

several gures and short pieces of text from An Introduction to Cardiovascular Physiology

by JR Levick Lev

The present text would never have b een conceived and written had it not b een for the

enthusiasm of the second author Paul Peter Lunkenheimer who sp entmany hours ex

plaining and demonstrating the workings of the heart to his mathematical colleague

Part I

Biomechanics

Chapter

The Human Machine

In this text we will primarily b e concerned with mo delling one asp ect of the human b o dy

the cardiovascular system and in particular the heart The approach used mathematical

mo delling is in principle straightforward We consider the individual comp onents of the

human b o dyFor each comp onent for example the lungs we seek to set up a set of math

ematical equations whichemb o dy the physical pro cesses within the comp onent These

equations which are usually a combination of algebraic ordinary and partial dierential

equations provide a mathematical mo del which can b e used for analysis and prediction

In practice mathematical mo delling is often dicult This is certainly the case in mo d

elling the human b o dy where as one moves from the macroscopic to the microscopic and

then to the molecular level new structures are revealed

This intro ductory part of the text serves two purp oses

To discuss some of the general features of man considered as a machine

Tointro duce the mathematical reader to some basic ideas and to give him or her a

feel for the size of some relevantphysiological quantities

There are some wellwritten nonmathematical intro ductions to biomechanics and physi

ology

Lifes Devices bySteven Vogel Vog

The Human Machine by Alexander Alea

There are also several excellent texts on mathematical biology which include sections on

mo delling the human machine

Hopp ensteadt and Peskin Mathematics in Medicine and the Life Sciences HP

Murray Mathematical Biology Mur

Mazumdar An Introduction to Mathematical Physiology and Biology Maz

And now without more ado let us turn to the task in hand

Chapter

Energetics

We b egin by recalling some basic facts ab out the human b o dy considered as a mechanical

device the human machineItmay b e noted here that there app ears to b e a fundamen

tal dierence b etween mathematical mo dellers and most physiologists A mo deller needs

mo del problems that is problems whcih embody typical features In the presentcontext

the mo deller would liketohave model man or model human machine There is of course no

such thing and physiologists seem to have little need to create it The normal or average

data given b elowhave had to b e extracted by us from several sources

A normal young man weighs W kg Corresp onding to a normal height H

H cm m



His b o dy surface area is ab out m Approximately of the b o dys weight is made

up of water

A normal young man has an oxygen consumption of

V ml O min

O 

breathing on average of ml of air twelve times p er minute

Rasch cite p uses examples from weight lifting to illustrate the p ower and

strength of athletes He also quotes the following maxima for the output of a human

b eing

hp kW kW for a single movement lasting less than second

tohp to kW for exercise lasting b etween and minutes

tohp tokW for steadystate work for min to min or more

hp kW for longterm work

The b o ok The Fire of Life by Kleib er Kle is a wellknown intro duction to animal

energetics which contains various interesting details but is also somewhat incoherent

For more details and references see App endix E where the average woman is also describ ed

Chapter

Mechanics

Part II

The Heart

Chapter

Intro duction

The heart is the pump in the cardiovascular system In this chapter the general features of

this system are describ ed In subsequentchapters more detailed information is provided

Wehave drawn heavily on standard texts including Cardiovascular Physiology byJR

Levick Lev Cardiovascular Physiology by RM Berne and MN Levy BL Cardio

vascular Physiology by Milnor Mil and The Cardiovascular System The Heart edited

by R M Berne Ber

Many exp erimental results are only available for nonhumans and it is in any case often

useful to compare results for dierent animals When discussing nonhuman physiology

this will b e explicitly stated

The Circulatory System

The mammalian cardiovascular system consists of the heart and blo o d vessels The basic

function of this system is to transp ort blo o d In this pro cess oxygen and other pro ducts

are conveyed to the tissues and waste pro ducts such as carb on dioxide and urea are re

moved

The heart consists of two adjacentintermittantmuscular pumps the rightventricle and

left Each pump is lled from a reservoir the right or left atrium

resp ectively The designation left or right is from the p ersp ectiv e of the patientthe left

ventricle is on the left side of the patients body Since the heart lies across the chest in a

human the rightventricle and atrium are towards the front anterior while the left ven

tricle and are towards the rear p osterior The rightventricle pumps blo o d through

the lungs to the left atrium the pulmonary circulation while the left ventricle simul

taneously pumps blo o d through the rest of the b o dy and back to the right atrium the

systemic circulation The blo o d is comp elled to follow a circular pathwayby oneway

valves lo cated in the heart and as was rst established by the London physician

William Harvey and published in Har Harb see Figure

In the pulmonary circulatory system venous blo o d enters the right atrium from

the two ma jor veins the sup erior vena cava and inferior vena cava and the

coronary sinusthenows through a valveinto the rightventricle This ventricle

which is comp osed mainly of receives the blo o d while it is in a

state of relaxation called diastole Contraction or systole then forces part of the

blo o d out through the pulmonary and into the lungs at a low pressure Gases

exchange by diusion in the lung air sacs raising the blo o d oxygen content from

approximately mll venous blo o d to mll The oxygenated blo o d returns

through the pulmonary veins to the left atrium and left ventricle

In the systemic circulatory system the left ventricle contracts virtually simultane

ously with the right and ejects approximately the same volume of blo o d but at a

much higher pressure The blo o d ows through the aorta and the branching arterial

system into ne thinwalled tub es called capillaries Here the dissolved gases and

nutrients diuse b etween the capillary blo o d and the tissue cells The circulation of

the blo o d is completed bythevenous system which conducts blo o d back to the

venae cavae

See App endix C for a discussion of the relevantphysical chemistry The statement that the oxygen

contentofvenous blo o d is mll means that litre of venous blo o d contains the equivalent of ml

of Oxygen O at STPD Standard Temp erature and Pressure that is C and atmospheric pressure

 BRAIN

HEAD and ARMS

S A V O C R LUNGS BRONCHI T A

RIGHT RIGHT LEFT LEFT ATRIUM VENTRICLE ATRIUM VENTRICLE

CORONARY SINUSHEART CORONARY ARTERY A MUSCLE O LIVER R SPLEEN T I GUT A V

C TUBULES GLOMERULUS

TRUNK and LEGS

Figure The simplied circulatory system

The ow of blo o d in the cardiovascular system is shown in simplied form in Figure

There are four circuits the pulmonary circuit where blo o d ows from the rightventri

cle through the lungs to the left atriumthe upp er or sup erior circuit where blo o d o ws

through the aorta to the head and arms returning via the sup erior vena cava SVCthe

lower or inferior circuit where blo o d ows through the aorta to the lower b o dy return

ing via the inferior vena cavaIVCand the coronary circuit where blo o d o ws through

the coronary artery to the heart muscle returning via the coronary sinus Together the

sup erior inferior and coronary circuits make up the systemic circuits The return of blo o d

from the bronchii is anomalous since it ows into the left atrium Under normal condi

tions the bronchial blo o d ow constitutes at most of the venous return to the heart

In certain pathological states the bronchial circulation may b ecome substantial See Berne

and Levy BL page RIGHT RIGHT VENTRICLE ATRIUM TRISCUPID VALVE PULMONARY VALVE

CORONARY SINUS

HEART LUNGS MUSCLE

CORONARY ARTERY

LEFT LEFT AORTIC VENTRICLE MITRAL ATRIUM

VALVE VALVE

Figure The plumbing of the normal heart

The ow of blo o d through the normal heart can b e represented functionally as in Figure

Eachventricle has an inlet valve the mitral and tricuspid valves resp ectively and an

outlet valve the aortic and pulmonary valves resp ectively These valves op en and close

at appropriate times during the cardiac cycle as describ ed in Section

In Figure the supply of blo o d to the heart muscles through the coronary artery

and coronary sinus is shown separately b ecause this blo o d supply is inuenced by the

pressures in the heart wall and is of imp ortance for the mo delling of the heart

The Heart

In an adult male weighing kg the heart weighs ab out grams and roughly o ccupies

a cub e with sides of length cm The lo cation of the heart is shown in Figure

Figure The lo cation of the heart

The heart lies obliquely across the chest The brotendinous ring black forms the base of

the heart It contains the tricuspid t mitral m aortic and pulmonary valves group ed

in an oblique plane b eneath the sternum The ap ex of the heart is formed by the left

ventricle LV and the anterior surface is formed by the rightventricle RV and right

atrium RA The inferior surface of the heart and the p ericardium not shown rest on the

central tendon of the diaphragm From JR Levick An Introduction to Cardiovascular

Physiologyby p ermission

As is shown in Figure a the heart consists of two adjacent pumps the left ventri

cle and rightventricle Blood ows into eachventricle from an antechamb er the left

atrium right atrium through a valve the mitral valve tricuspid valve Blo o d

leaves the left right ventricle through another valve the aortic valve pulmonary

valve The edges of each inow valve are tethered by strings the chordae tendineae

to twomuscles the papillary muscles which bulge from the ventricles walls

The wall dividing the left ventricle and atrium from the rightventricle and atrium is

called the septum The four heart valves lie approximately in a plane the intersection

of which with the heart is called the brotendinous ring see Figure

The rightventricle only pumps blo o d to the lungs and back to the left atrium while the

left ventricle must pump blo o d through the whole b o dy As to b e exp ected the outer

wall of the rightventricle is much thinner ab out cm than the outer wall of the left

ventricle ab out cm This is illustrated in Figure b which shows a view of the

lower part of the twoventricles

Visualization

Since the heart is threedimensional it is quite dicult to visualizefor a nonmedical

reader it may help to use a plastic mo del such as can b e obtained from medical b o ok

shops or even b etter the prepared heart of an animal Recently videos showing the



motion of the heart havebecomeavailable



See App endix K for the names and addresses of some suppliers

Figure Crosssections of the heart

a Schematic diagram of an oblique section b Section across the ventricles to illustrate

mo de of emptying c Arrangementofmuscle bres in the ventricle wall RA LA right

and left atrium The op ening just b elow the lab el RA is the coronary sinus RV LV right

and left ventricleT M tricuspid and mitral v alvesP papillary muscle with chordae

tendineaeA aorta P A PV and veinsSV C IVC sup erior and in

ferior venae cavae From JR Levick An Introduction to Cardiovascular Physiologyby

p ermission

Several b o oks provide extensivedrawings and photographs

Anderson and Becker The Heart Structure in Health and Disease AB

M J Davies Colour Atlas of Cardiovascular Pathology Dav

Thomas Geb ert and Hombach Grundlagen der klinischen Medizin Anatomie

Physiologie Pathologie Mikrobiologie Klinik Band Herz und Gefaesse

TGH

Vesalius The Illustrations from the Works of Andreas Vesalius of Brussels

Vesb

For the text of Anderson and Becker an accompanying set of slides is available

Disease and Pathology

An imp ortant justication for mo delling the cardiovascular system is that it may suggest

ways to improve the treatment of illness Examples of this approach are given in McDon

alds Blood Flow in the pages NO

An immense variety of pathological situations is observed in practice Every part of the

heart can b e aected either through congenital defects or disease

See

Anderson and Becker The Heart Structure in Health and Disease AB

Acierno The History of Cardiology Aci

Braunwald Heart Disease Bra

Davies Colour A tlas of Cardiovascular Pathology Dav

Julian and Cowan Cardiology JC

Lilly Pathophysiology of Heart Disease Lil

Thomas Geb ert and Hombach Grundlagen der klinischen Medizin Anatomie

Physiologie Pathologie Mikrobiologie Klinik Band Herz und Gefaesse

TGH

White Heart Disease Whi

Pathological situations presentachallenge to mathematical mo delling A mo del should

b e able to correctly repro duce the eects of any pathologySuchamodelwould b e a

valuable diagnostic to ol No current mo dels have such capabilities We b elieve that this

represents a tremendous opp ortunity

In this connection we observe that the following discuss changes in heart function caused

by disease

Grant Architectonics of the heart Gra

ComparativePhysiology

A great deal can b e learnt ab out the human cardiovascular system by considering the

cardiovascular systems of other animals

Some measurements are more easily made on certain animals

For the development and testing of a go o d theory it is of imp ortance to b e able to

vary parameters eg the size of the heart

The prime purp ose of a cardiovascular system is to transp ort oxygen within the b o dy

Twophysical pro cesses are involved

Diusion which is only eectiveover short distances b ecause the average time t

required for a particle to diuse a distance x is given by



t x D

where D is a constant the diusion co ecient For example for a solution of glucose

 

in water at D cm s so that the time required to diuse cm is



s s h t

that is hours and minutes

Even over short distances nature comp ensates for the slowness of diusion by pro

viding large surfaces



The lungs have a surface of ab out m in a normal adult Guyton

Guy page



The blo o d capillaries oer a surface of m Guyton Guy page

See Cameron Cam and Weib el Wei

Convection which is eected through the circulatory system and is eectiveover

long distances

Each animal has its own system of oxygen distribution and nature has provided a mar

vellous range of alternatives some of which are listed b elow

No circulatory system

Op en circulatory systems in which blo o d is pump ed by the heart through a system

of blood vessels but then moves freely b etween the tissues of the b o dy

Closed circulatory systems in which the blo o d is pump ed by the heart through a

system of blo o d vessels which it never leaves

In circulatory systems many p ossible arrangements of the hearts o ccur

One pump eg the frog

One bidirectional pump eg in tunicates see SchmidtNielsen SN page

Two pumps in one heart mammals and birds

Three separate pumps eg the o ctopus see Steven Vogel Vog page

The great range of cardiovascular mechanisms is clearly reviewed in Chapter of Scheer

Sch while in Chapter of Prosser Pro more details are given including tables of

blood volumes and blo o d pressures in various animals

Other references include

Comparative Animal Physiology by Prosser Pro

Comparative Physiology by Bradley T Scheer Sch

Animal Physiology byKnut SchmidtNielsen SN

Vital Circuits bySteven Vogel Vog

Biologie in Zahlen by Flindt Fli

History of Cardiology

The history of cardiology is a fascinating topic For the interested reader we can whole

heartedly recommend the translation of Harveys The Circulation of the Blood Harb

which is b eautifully clear even for to days reader Fosters Lectures on the History of

Physiology MF is interesting but alas long out of print The recent b o ok The History

by Acierno Aciiswellwritten and describ es not only historical contri of Cardiology

butions but also quite recentdevelopments Other currently or until recently available

references are

Giovanni Alphonso Borelli On the Movement of Animals Bor

Clendening SourceBook of Medical History Cle

Harris The Heart and Vascular System in Ancient Greece Har

Leib owitz The History of Coronary Heart Disease Lei

Andreas Vesalius EpitomeVesb

Andreas Vesalius The Il lustrations from the Works of Andreas Vesalius of Brussels

Vesa

Willius and KeysClassics of Cardiology previously cal led Cardiac Classics WK

Further references are given by

Acierno Aci

It is of interest to lo ok at old textb o oks such as

Braun Diagnose und Therapie der Herzkrankheiten Bra

Evans Starlings Principles of Human Physiology Eva

Grollman The Cardiac Output of Man in Health and Disease Gro

Tigerstedt Die Physiologie des Kreislaufes Tig

Chapter

The Cardiac Cycle

Intro duction

The basic facts ab out the cardiac cycle are describ ed Some standard texts are

Braunwald Ross jr and SonnenblickMechanisms of Contraction of the Normal

and Failing Heart BRS

Baan Arntzenius and Yellin Cardiac Dynamics BAY

Burton Physiology and Biophysics of the Circulation AnIntroductory Text Bur

Berne Handbook of Physiology Section The Cardiovascular System Vol I The

Heart Ber

Frank Zur Dynamik des HerzmuskelsFra

Katz Physiology of the Heart Kat

Noble The Cardiac Cycle Nob

Opie The Heart Physiology and Metabolism Opi

Rushmer Cardiovascular Dynamics Rus This textb o ok for medical students was

a standard reference

ter Keurs and Tyb erg Mechanics of the Circulation tKT

The Cardiac Cycle

The cardiac cycle corresp onding to one full b eat of the human heart lasts ab out sec

onds for a resting p erson The cycle comprises four parts during which the inlet valves

mitral and tricuspid and outlet valves aortic and pulmonary op en and close as appro

priate

The four parts of the cardiac cycle describ ed ab ove are traditionally divided into two

phases systole and diastole During the systolic phase isovolumetric contraction and

ejection the heart is actively pumping blo o d and the heart muscles are tensed During

the diastolic phase isovolumetric relaxation and ventricular lling the heart muscles are

relatively passive However this terminology is somewhat confusing since see eg Mc

Cullo ch and Omens MO p the heart muscle is not fully relaxed even during the

diastolic phase

Typical measurements of pressure and ow on the left side of the human heart adult

resting supine are shown in Figure The following description of events is based on

the b o ok of Levick Lev pages w ehave added some comments in fo otnotes

Figure The cardiac cycle

Diagram of pressure and outow on the left side of the human heart based on data

from intracardiac catheters and velo city measurements at the aortic ro ot dP dt is

max

the maximum rate of rise of ventricular pressure a measure of myo cardial contractility

The stippled region highlights the pressure gradient which decelerates outow during the

late ejection phase Note the slight reversal of aortic owataorticvalve closure The

waveforms in the right heart are of similar shap e but the pressures are lower From JR

Levick An Introduction to Cardiovascular Physiologyby p ermission

Ventricular lling

Duration s

Inlet valves tricuspid and mitral op en

Outlet valves pulmonary and aortic closed

Initially the atria are in diastole and blo o d ows passively from the great veins through

the op en atrioventricular valves into the ventricles There is an initial phase of rapid ll

ing lasting ab out s which has a curious featureev en though ventricular volume is

increasing ventricular pressure is falling The reason is that the ventricle wall is recoiling

elastically from the deformation of systole and is in eect sucking blo o d into the chamb er

As the ventricle reaches its natural volume lling slows down and further lling requires

distension of the ventricle by the pressure of the venous blo o dv entricular pressure now

b egins to rise In the nal third of the lling phase the atria contact and force some addi

tional blo o d into the ventricle PPL fragen In resting sub jects this atrial b o ost is quite

small During exercise however when the time available for passiveventricular lling is

curtailed the atrial b o ost b ecomes imp ortant The volume of blo o d in a ventricle at the

end of the lling phase is called the enddiastolic volumeor EDV and is typically

around ml in an adult human The corresp onding enddiastolic pressureor EDP

is a few mmHg

Isovolumetric contraction

Duration s

Inlet valv es tricuspid and mitral closed

Outlet valves pulmonary and aortic closed

Ventricular systole lasts s and is divided into a brief isovolumetric phase and a longer

ejection phase As so on as ventricular pressure rises fractionally ab ove atrial pressure the

atrioventricular valves are forced shut by the reversed pressure gradient Backow during

closure is minimal b ecause the cusps are already approximated byvortices b ehind them



in the late lling phase The ventricle is now a closed chamb er and the growing wall

tension causes a steep rise in the pressure of the trapp ed blo o d

The atrioventricular valves are the tricuspid and mitral valves which link the atria and ventricles



Although the ow around the tricuspid and mitral valves has b een extensively studied we are not

aware of a precise justication for this assertion Discussed in Section

Ejection

Duration s

Inlet valves tricuspid and mitral closed

Outlet valves pulmonary and aortic op en

When ventricular pressure exceeds arterial pressure the outowvalves are forced op en

and ejection b egins Three quarters of the strokevolume are ejected in the rst half of

the ejection phase s and at rst blo o d is ejected faster than it can escap e out of the

arterial tree As a result much of it has to b e accommo dated by distension of the large

elastic arteries and this drives arterial pressure up to its maximum or systolic level

Vortices b ehind the cusps of the op en aortic valve prevent the cusps from blo cking the



adjacent op enings of the

As systole weakens and the rate of ejection slows down the rate at which blo o d ows

away through the arterial system b egins to exceed the ejection rate and pressure b egins

to fall Activeventricular contraction actually ceases ab out twothirds of the way through

the ejection phase but a slow outowcontinues for a while owing to the momentum

of the blo o d As the ventricle b egins to relax ventricular pressure falls b elow arterial

pressure but the outward momentum of the blo o d prevents immediate valve closure Fi

nally a brief backow comprising less than of strokevolume closes the outowvalve

Valve closure creates a brief pressure rise in the arterial pressure called the dicrotic wave

The ventricle do es not empty completelythe a verage ejection fraction in man is

corresp onding to a strokevolume of ml in adults The residual endsystolic vol

ume of ab out ml acts as a reserve which can b e utilized to increase strokevolume in

exercise



As of December we do not know of a reference for this statement

Isovolumetric Relaxation

Duration s

Inlet valves tricuspid and mitral closed

Outlet valves pulmonary and aortic closed

With closure of the aortic and pulmonary valves eachventricle once again b ecomes a

closed chamb er Ventricular pressure falls very rapidly owing to the mechanical recoil

of collagen bres within the myo cardium whichwere tensed and deformed by the con

tracting myo cytes When ventricular pressure has fallen just b elow atrial pressure the

atrioventricular valves op en and blo o d o o ds in from the atria whichhave b een relling

during ventricular systole

Global Motion of the Heart

The heart is not stationary but moves relative to the rest of the b o dy during each cardiac

cycle The rotation of the left ventricular ap ex has b een measured by Buchalter Weiss et

al BWR

The Pericardium

When the chest is op ened the motion of the heart is largely hidden from view b ecause

of the p ericardium a brous uidlled sac in the thoraic cavitywhich encloses and

restrains the heart The p ericardium reduces friction b etween the heart and surrounding

organs and provides a barrier against infection

The p ericardium consists of twolayers a strong outer layer of tough brous tissue the

brous p ericardium and an inner doublelayer sac the serous p ericardium The

brous p ericardium is rmly attached within the b o dy The serous p ericardium is normally

lled with uid

The inuence of the p ericardium on the motion of the heart has b een discussed by several

authors see McCullo ch and Omens MO p The consensus of opinion seems to b e

that the p ericardium only plays a small role for normal hearts under normal conditions

Indeed humans with no p ericardium as a result of a congenital defect do not usually

showanyunusual symptoms see Bra p However Braunwald Bra p

lists three roles for the p ericardium which deserve consideration by mo dellers

The distribution of hydrostatic forces on the heart

The prevention of acute cardiac dilation

Diastolic coupling of the twoventricles

In the case of illness or injury the p ericardium probably plays an imp ortantroleinre

straining the heart see Braunwald Bra Over a p erio d of time the p ericardium can

adapt to changes in the size of the heart

In health the p ericardium may b e unobtrusive but there are several illnesses asso ciated

with the p ericardium including see Chapter of Braunwald Bra

p ericarditis acute caused by inammation of the p ericardium

p ericardial eusion caused by an increase in the amount of uid in the p ericardial



space According to Braunwald Bra p the p ericardial space in humans

normally contains b etween and ml of uid If additional uid increases slowly

the p ericardium can stretch and can accommo date up to l of uid without appar

ent discomfort If the uid increases rapidly or the p ericardium is not suciently

exible then a marked rise of intrap ericardial pressure will o ccur This can lead to

cardiac tamp onade whichischaracterized Braunwald Bra p by

Elevation of intracardiac pressures

Progressive limitation of ventricular diastolic lling

Reduction of strokevolume and cardiac output

p ericarditis constrictive which o ccurs when a brotic thickened and adherent

p ericardium restricts diastolic lling of the heart

Rowell Row p and pages discusses the role of the p ericardium It has b een

demonstrated exp erimentallyRowell Row Figure p that p ericardectomy

the surgical removal of the p ericardium leads to a substantial increase in stroke

volume for exercising dogs Rowell Row p comments on anecdotes that racing dogs

have had the p ericardium cut to improve their p erformance Blomqvist and Salting BS

have suggested that physical conditioning may alter apparentven tricular compliance by

mo difying right and left ventricular p ericardial interactions see Rowell Row p

Tyb erg Misbach Parmley and Glantz TMPG discuss the role of the p ericardium

They suggest see p with conrming exp erimenta data that the p ericardium has a

dominant role in the mechanism of acute shifts in the left ventricular diastolic pressure

volume relationship The authors suggest that the observations can b e explained bya

simple hydraulic mo del As long as the volume of the heart is less than the unstressed

volume of the p ericardium the diastolic pressure in the left ventricle is the same whether

the p ericardium is op en or closed However when the volume of the heart exceeds the

unstressed volume of the p ericardium the ventricular diastolic pressure equals the trans

mural pressure necessary to distend the ventricle plus the p ericardial pressure This implies

that changes in the left ventricular diastolic pressure whenever the unstressed volume of

the p ericardium has b een exceeded The authors p oint out that such shifts in the pressure

volume curve are imp ortant in explaining the resp onse of patients with cardiac failure to

vaso dilators

Heart Sounds and Murmurs

During the cardiac cycle a variety of sounds clicks murmurs etc is pro duced and pro

vides valuable diagnostic information The generation of some of these noises has also

b een analyzed mathematically as will b e discussed later see Peskin Pes p Ped

ley Ped page and page



The terms pericardial space and pericardial sac are used interchangeably

Some common heart sounds are listed b elow For more details and descriptions of other

sounds see Lilly Lil Chapter Luisada Luia LuibLuisada and P ortaluppi

LP Guyton Guy Chapter No veyPencak and Stang NPS

Heart Sounds There are four recognized heart sounds of whichtwo are easily

heard

S The rst heart sound is caused by the closure of the tricuspid and mitral valves

S The second heart sound is caused by the closure of the aortic and pulmonary



valves The mechanism of heart sounds as observed in exp eriments is consid

ered by Luisada and Portaluppi LP p

Heart Murmurs

Heart murmurs are abnormal sounds caused by turbulence which is normally absent

Typically this turbulence is caused bytwotyp es of valve defects see Levick Lev

page

Stenosis isanarrowing of a valve so that a highpressure gradient is needed

to force blo o d through a stenosed valve

Incomp etence is failure of a valve to close tightlythus allowing a regurgi

tation of blood

Korotko Sounds

Korotko sounds are heard when blo o d pressure is measured in the usual way

by placing a cu containing an inatable bag around the upp er arm If the cu

is rst inated and then the pressure is gradually reduced there comes a p oint

when the blo o d b egins to ow through the brachial artery again at this p oin t the

Korotko sounds can b e heard in a stethoscop e placed against the artery

Concluding Remarks

In this c hapter wehave describ ed the basic observations of the mammalian heart Some

such as the Korotko sounds or the maximum blo o d pressure can b e made by elemen

tary noninvasive means and form part of the diagnostic techniqes of every do ctor Oth

ers such as the measurement of the blo o d pressure at the aortic ro ot require the use of

sophisticated invasivetechniques All these observations have b een made and recorded

innumerable times

It is the job of the mo deller to predict and explain these observations To do so requires

much more detailed knowledge In the remainder of this Part we attempt to summa

rize what is known It will b ecome apparent that there are often surprising gaps in this

knowledge

Chapter

The Structure of the Myo cardium

Intro duction

The myo cardium is a complex brous continuum whichcontains not only the muscle

cells or myocytes but also an extensive network of connective tissue We refer to Levick

Lev Chapter for a description of individual myo cytes and their function and to

Lunkenheimer Lunkenheimer and Torrent Guasp LLG Chapter for photographs of

sp ecimens

Connective Tissue

The myo cardium is a complex brous continuum which contains not only the muscle cells

but also an extensivenetwork of connective tissue It is reasonable to supp ose that this

tissue can contribute to the expansion of the ventricles during diastole

This idea has a very long history see Lunkenheimer Lunkenheimer and Torrent Guasp

LLG pages but much more detailed information has now b ecome available

through microscopic analysis

Hunter and Smaill HS review recent ndings and consider the formulation of consti

tutivelaws A Horowitz Y Lanir FCP Yin M Perl I Sheinman and R K Strumpf

HLY consider constitutivelaws for the passivemyo cardium

The individual myocytes have a denite direction and together form muscle bres which

are clearly visible after preparatory treatment such as b oiling The determination of the

direction of the bres has b een the sub ject of investigation and sp eculation for many

centuries Inuential contributions were made byLo wer Pettigrew

MacCullum Mall Flett Fle and Thomas Tho Flett Fle

includes as complete a bibliography a p ossible of the literature as of

The earlier workers recorded their ndings in often very attractivedrawings To our

knowledge the rst detailed quantitative measurements are due to Hort Hor and Hort

Hor Although the individual myo cytes are joined together the determination of the

direction eld of the bres is not easy The literature has therefore tended to split

I On the one hand there are many classical descriptions of the complicated twisted form

taken by the bres As describ ed by Borelli in Bor p

The bres of the heart are not straight and parallel to each other but curved

and coiled They are amazingly intricate Their texture is not similar to that of

a wickerbasket as Vesalius b elieved but they are arranged in a more sophis

ticated wayImmediately underneath the p ericardium from the basis of the

heart and from the circular tendinous orices of the vena cava and pulmonary

auricle and from the origins of the aorta and pulmonary arteries a layer of

eshy bres spreads These bres are parallel to each other and they are orien

tated from the basis straight to the ap ex of the heart where they are diversely

curved and intertwined reecting towards the cavities of the ventricles This

layer is followed by other layers of bres oblique and descending in spirals

They are more and more inclined and orientated also towards the ap ex of the

heart Before reaching the ap ex they intersect and cover each other and other

ordinary bres Hence they are deviated to the inside and partly reected in

oblique and transverse spirals like scythes towards the base of the heart Part

of them seem to comp ose internal columns to which the strings of the tricuspid

and mitral valves are attached and others are intertwined transversally and

form the cavity of the rightventricle

Grant Gra briey and succintly summarizes earlier work on the muscular architecture

of the left v entricle He describ es the work of Lower and Mall and p oints out that Lower

drew attention to the twisting of the bres Grant p compares this with reserva

tions to a twisted rop e Grant also discusses the p ossible role of embryonic development

in the structure of the ventricle see Grant Gra page

Greenbaum Ho Gibson Becker and Anderson GHG briey summarized previous

work on the bre architecture and rep ort the outcome of a study using dissection and

histology on normal p ostmortem human hearts They conclude p Mo dels based

on uniform myo cardial bre structure cannot explain wall movement in normal sub jects

and are likely to have signicant limitations if used to investigate left ventricular function

in disease

Lunkenheimer Lunkenheimer and Torrent Guasp LLG and LW have extensive dis

cussions of the bre architecture The latter reference in particular contains a detailed

evaluation of current knowledge

As participants of this conference are well aware Torrent Guasp Gua has extended

this work and p ostulated a mo del based on these observations of twisting bres

II On the other hand many mo dels assume that

The bre directions vary smo othly through the heart wall

The bres run parallel to the inner and outer surfaces

The innermost endo cardial and outermost epicardial bres run longitudinally

from the base to the ap ex the central bres run circumferentially and the other

bres run obliquely

These assumptions are usually justied by reference to the pap ers of Streeter and Basset

SB who measured bre orientation in pig heart and Streeter Sp otnitz Patel Ross

and Sonnenblick SSP who measured bre orientation in canine hearts See also

the PhD thesis of Streeter Str and the article by Streeter Str However this is

an oversimplication of the results of Streeter who was well aware of the earlier work

Streeter did measure transmural bre directions but asserted that the asso ciated angle

which he called the imbro cation anglewas smaller than ab out



The measurements of Streeter were based on a small numb er of samples at nonrandom

sites The actual situation is much more complex as can b e seen from the pictures of

treated hearts in Lunkenheimer Lunkenheimer and Torrent Guasp LLG pages

Several authors have commented on the shortcomings of the results of Streeter For ex

ample Hunter and Smaill HS page comment

However despite the large numb er of studies there is still a dearth of

quantitative information on ventricular muscle bre orientation No studies

app ear to have measured the muscle bre orientation at more than sites on

a single heart

As rep orted byLunkenheimer p ersonal communication the bres frequently dip into the

surface with an angle of as muchas contradicting assumptions and ab ove

As McLean and Prothero MPb p state

Wehave no a priori reason to assume that the global largescale organization

of the myob ers in the heart can b e inferred with condence from a study

restricted to the lo cal organization at one or a few sites in the developing or

adult heart wall

At present several studies are under way which should provide much more detailed infor

mation ab out the bre orientation McLean Ross and Prothero MRP have mapp ed

bre directions in the mouse heart and rep ort that they apparently dier signicantly

from those in the human heart Nielsen Nie and Nielsen Le Grice Smaill and Hunter

NLSH have made detailed measurements of bre orientation in the canine heart See

also McLean Ross and Prothero MRP

Previous Mathematical Mo dels

Until recently only a few mo dels to ok account of the bre direction A few authers have

considered uidbre mo dels in which the myo cardium is treated as a uid with an

emb edded bre matrix Such mo dels thus ignore the elasticity of the myo cardium but

b ecause of their simplicity can sometimes b e solved analytically See

Caisch Caf

Fung Fun p

Unfortunately this work has b een discontinued

Skalak Ska

Chadwick und Cha Cha

It seems clear that the results should b e incorp orated into mo dels See

Bovendeerd Huyghe Arts van Camp en and Reneman Inuenceofendocardial

epicardial crossover of muscle bers on left ventricular wal l mechanics BHA

Bovendeerd Arts Huyghe van Camp en and Reneman Dendenceoflocal left ven

tricular wal l mechanics on myocardial ber orientation A model study BAH

Yang Tab er and Clark YTC page briey mention observations on bre orientation

in embryonic chick hearts which they incorp orate into their mo del

Grant Gra briey and succintly summarizes earlier workonthemuscular architec

ture of the left ventricle He describ es the work of Lower Low and Mall Mal and

p oints out that already Lower had drawn attention to the twisting of the bres Grant

compares this with reservationstoatwisted rop e page Grant also discusses the

p ossible role of embryonic development see Grant Gra Finally Grant page also

observes that on its outer surface epicardium the left ventricle has twovortices which

merge b elow the surface The rightven tricle has its own vortex

See also

Pu Puf

Flett Fle

Mall Mal

MacCullum Mac

Thomas Tho

Streeter and Ramon SR

Streeter Daniel Powers Ross and Torrent Guasp SPRG

The Pericardium Endo cardium and Epicardium

For observations on the p ericardium endo cardium and epicardium see

Faller Fal

Chapter

Exp erimental Observations

It is obviously dicult to obtain observations of the heart The layman maywell feel

that direct measurementmust b e nigh to p ossible However the heart is in some ways

remarkably robust as one author CWC rst realized when holding a b eating pig heart

with one hand There is a substantial and rapidly growing b o dy of knowledge which serves

both as a challenge and a guide for mo delling There seems to b e a denite need to design

exp eriments so as to conrm confound theoretical and numerical predictions

The Ventricular Function Curve

The measurements in Figure refer to a normal working heart However the heart

continues to function outside the b o dy In Otto Frank Fra studied the frog ven

tricle and measured the relation b etween pressure and volume see Knowlton and Starling

KS Markwalder and Starling MS Patterson and Starling PS Patterson Pip er

and Starling PPS as well as Starlings Principles of Human Physiolog Evans Eva

and Levick Lev page This work was extended by Starling and his collab orators

around Figure from Levick p Lev shows the exp erimental setup The

Starling resistor shown in Figure a device to maintain constant arterial pressure is

discussed in detail byFung Fun page

The results of this classical exp eriment are shown in Figure where the strokevolume

is plotted against the lling pressure for an isolated dog heart

A graph whose ordinate is strokevolume or any other measure of contractile energy and

whose abscissa is lling pressure or any other index of resting bre length is called a

ventricular function curve orStarling curve

The upward part of the curve is the basis of the celebrated FrankStarlingLaw or

Starlings Law of the Heart which asserts that the greater the stretchofthe

ventricle in diastole the greater the strokevolume This law explains a basic control

mechanism of the heart

The frog heart has two atria but only one ventricle

Figure Simplied diagram of isolated dog heartlung preparation of Starling

The height of the venous reservoir and the screwclamp regulated central venous pressure

CVP CVP and arterial pressure AP were measured by manometers and AP was held

constantbya variable resistance equivalent to the total p eripheral resistance TPR

Ventricular volume was measured by Hendersons b ell cardiometer an inverted glass

b ell which is attached to the atrioventricular gro oveby a rubb er diaphragm Beatby

b eat volume changes were recorded on a rotating smoked drum Mean cardiac output was

measured directly by collecting blo o d in a measuring cylinder b eyond the resistor After

Knowlton and Starling KS From JR Levick An Introduction to Cardiovascular

Physiologyby p ermission

Figure The ventricular function curve

Eect of lling pressure on the strokevolume of an isolated dog heart pumping against a

constant arterial pressure The solid line shows Starlings data for left ventricular stroke

volume LV and left atrial pressure The dashed line shows how the rightventricle has

a similar shap ed curve but a slightly lower lling pressure From J R Levick An Intro

duction to Cardiovascular Physiologyby p ermission Lev p

The results of exp eriments such as Starlings are of considerable imp ortance when mo d

elling ventricular mechanics b ecause they provide data ab out the heart as a mechanical

pump when isolated from the atria and the rest of the circulatory system In particular

the eects due to the elasticity of the aorta are eliminated

Some of Starlings smokeddrum recordings are repro duced by Levick Lev p It is

interesting to note that when the lling pressure is changed suddenly the heart adjusts to

the new conditions b oth quickly and smo othly In Figure the strokevolume p eaks at a

pressure of ab out mmHg and then falls This is an abnormal region sometimes called

the descending limb and there may b e exp erimental errors due to leakage through

the atrioventricular valves see Levick Lev p but it would still b e of interest to

repro duce this b ehaviour with a mo del since it is a challenging test for a mo del Katz

Kat p suggests that in some chronically ill patients the heart may op erate up on

this descending limb

For discussions of Starlings Law see

The Physiological Basis of Starlings Law of the Heart by the Ciba Foundation Sta

Sym

Starlings L aw of the Heart Revisited by Keurs and Noble tKN

In Vivo Stress Measurements

In the past various devices have b een implanted in the heart wall and used to measure the

stress but it is dicult to allow for the inevitable eects of the intrusion Lunkenheimer

Lunkenheimer and Torrent Guasp LLG pages summarize a variety of such

metho ds The stress vector has six comp onents and it is dicult to measure all of these

See also

Huisman Hui

Huisman Sipkema Westerhof and Elzinga HSWE

Huisman Sipkema Westerhof and Elzinga HSWE quoted byHunter and

Smaill HS p

Muss ergaenzt werden PPL fragen

Left ventricular wall motion has b een observed by Greenbaum and Gibson GG

who give further references

Rightventricular wall motion in dogs has b een measured byChuong Sacks Temple

ton Schwiep and Johnson CST

In Vivo Strain Measurements

Avariety of metho ds has also b een used to measure strains in the heart wall Less in

trusion is necessary and recent developments in promise that accurate

measurements of movements of the surfaces will so on b e available See

Lunkenheimer Lunkenheimer and Torrent Guasp LLG p

Hunter and Smaill HS pages

Waldman Wal

McCullo ch McC

Muss ergaenzt werden PPL fragen

Coronary Perfusion

The suggestion that changes of pressure and ow in the coronary vessels alter the passive

prop erties of the left ventricle has b een studied bymanyworkers Some references are

given by McCullo ch in his PhD thesis McC p

The term coronary p erfusion refers to the intro duction by normal or articial means



of additional blo o d in the coronary arteries This is related to the garden hose eect

Intramyo cardial Pressure

The extravascular forces in the myo cardium are commonly referred to as the intramy

o cardial pressure

See

PhDthesis of Rabbany Rab



CWCcheck this denition

Other Exp erimental Observations

In Chapter of Circulatory Dynamics by Wiggers Wig a varietyof in vivo exp eriments

are describ ed

Pericardial Eusion

Wiggers Wig pages discusses the eect of changes in p ericardial eusion that

is PPL fragen

He quotes several pap ers including

Kuno Kun

Fineb erg Fin

Wiggers Wig

Wiggers Wig Fig p shows graphically the eect of increasing the p ericardial

pressure the minimum ventricular pressure increases but the maximum ventricular pres

sure decreases For instance if the p ericardial pressure is increased to mmHg the

minimum ventricular pressure rises to mmHg while the maximum ventricular pressure

falls to mmHg PPL fragen

Hyp ervolemia

Oligemia

Arterial Hyp ertension

Aortic Coarctation

Aortic Stenosis

Pulmonary Stenosis

Idoventricular Rhythms

Coronary Occlusion Myo cardial Ischemia

Cardiac Valves

Aortic Regurgitation

Mitral Insuciency

Mitral Stenosis

Part III

Mathematical Mo delli ng of the

Heart

Chapter

Intro duction

The mo delling of the heart has a long history Already in the seventeenth century Borelli

Bor sketched the arrangementofmuscle bres on the surface of the heart and consid

ered how these could contract

At the end of the nineteenth centuryWoods Wo o applied the results of Laplace to

relate the pressure in a ventricle to the stress in the heart wall

The Law of Laplace which is derived in section is often quoted in medical texts

One conclusion from this law which nds medical application is that if a diseased heart

increases in size its eciency drops since R and R increase For a recent discussion



of the Law of Laplace see Moriarty Mor Any realistic mo del must of necessitybe

far more complicated Fortunately mo dern computer developments make it p ossible to

present the results of such mo dels in a readily accessible manner

The longterm goal of mathematical mo delling of the cardiovascular system is to predict

features such as

The blo o d pressure and other characteristics of the blo o d ow

The stresses in and motion of the comp onents of the heart

The general approach is to set up a system of equations which describ es the underlying

physical and biological pro cesses This system of equations will include partial dierential

equations for stresses in the heart wall and blo o d velo cities but may also include ordi

nary dierential equations and algebraic equations This system of equations must then

b e considered b oth mathematically to try to derive general features and numericallyto

obtain quantitative results

There are several excellent general references The threevolume workofFung Fun

tly app eared as a second edition is a broad Fun Fun one volume of which has recen

and leisurely intro duction to biomechanics The lecture notes of Peskin Pes are often

quoted and emphasize the uid mechanical and mathematical asp ects of mo delling the

heart asp ects which are often somewhat neglected in the literature There has recently

b een a surge of activity in the mo delling of the heart in part owing to the rapid improve

ments in computing facilities The pro ceedings TheoryofHeart edited by Glass Hunter

and McCullo ch GHM is an excellentintro duction to mo dels currently b eing develop ed

and used There is also an extensive review article by Hunter and Smaill HS which

discusses many asp ects of mo delling the heart using continuum mechanics Yin Yin

compares numerical results for dierent geometries and constitutivelaws

Antaki Ant has a lengthyintro ductory section of pages in which mo dels of the

heart are critically discussed and questions such as bre direction p p and p

and compressibility p are addressed with extensive references

Other references include

Part II Ventricular and Myocardial MechanicsinCardiovascular Dynamics and

Models by Brun et al BCL

Cardiovascular Biomechanics by Chandran Cha

Chapter Circulatory System Dynamics by No ordergraaf No o

The Mechanics of the Circulation by Caro PedleySchroter and Seed CPSS

This is an excellentintro duction to crdiovascular mechanics which tries wherever

p ossible to supply numerical data but also avoids mathematical formulations and

presents mechanics in readily comprehensible terms

The Physics of He art and Circulation by Strackee and Westerhof SW

Engineering Design of the Cardiovascular System of Mammals byDawson Daw

Noble The Cardiac Cycle Nob

Dinnar Cardiovascular Fluid Dynamics Din

Fung A First Course in Continuum MechanicsFun

Sagawa Maughan Suga and Sunagawa Cardiac Contraction and the Pressure

Volume Relationship SMSS

Sideman and Beyar Analysis and Simulation of the Cardiac SystemIschemia SB

Ghista Van Vollenhoven Yang Reul and Bleifeld Cardiovascular Engineering Part

I Model ling GVY

Hopp ensteadt and Peskin Mathematics in Medicine and the Life Sciences HP

The rst step in the mo delling pro cess is to decide whichvariables parameters and pro

cesses signicantly inuence the problem This decision is partly heuristic and is strongly

inuenced by the need to reduce the complexity to manageable prop ortions In mo delling

the mechanics of the heart twotypical assumptions are

To assume a simplied geometry

To assume that heat ow in the heart walls do es not inuence the mechanics of the

heart

Once the signicantvariables have b een chosen it is necessary to formulate the eld

equations governing these variables There are twotyp es of equations Firstly there are

the equations which represent general physical laws such as conservation of momentum

Secondly there are the constitutivelaws whichembody physical prop erties of the

medium In some cases these can b e simple and uncontroversial as when one can as

sume that heat ow is linearly prop ortional to the temp erature gradient In other cases

the formulation of suitable constitutivelaws is dicult This is the case in ventricular me

chanics where the relationship b etween stress and strain in the heart walls is extremely

complex One frequent cause of diculty is that mo dels nearly always use only one geo

metric scalethe constitutiv elaws must reect pro cesses at smaller scales The dilemma

facing the mo dellist is illustrated bytheLaw of Laplace This law is a useful sim

plication but is based on a great numb er of assumptions

The rst mo dels of the hearts wall were develop ed ab out thirtyyears ago and used lin

ear elasticity andor simplied geometry While these assumptions were justied at the

time the myo cardium is certainly nonlinear and the deformations are so large that the

assumptions of linear elasticity are not tenable With current computing facilities it is

feasible to handle nonlinear material prop erties

The Field Equations

We assume that the myo cardium is incompressible and satises the nonlinear elasticity

equations

d

div r p for x in

det F

F r

d

Here F denotes the deformation gradient tensor the deviatoric Cauchy stress tensor

and p the pressure These equations are formulated in the deformed b o dy When

solved they must rst b e transformed backonto the undeformed b o dy

The Constitutive Equations

There is a considerable literature on the form of the constitutive equations Following

Bovendeerd Bovwe assume the following constitutive equations

S S ES l l t

p a s c

where S represents the passive stress and S represents the active stress created by the

p a

activation of the muscle The terms l and l represent the lengths of the c ontractile ele

c s

ment and sarcomere resp ectively

S is the second PiolaKirchho stress tensor which is related to the Cauchy stress tensor

d

via

 d T

S detF F F

It is assumed that the material is hyp erelastic that is that a function W exists the

stored energy function such that

W

S

p

E

where

h i

   

W EC expa I a II a E a E E

 E  

E   

and

I E E E

E  

  

II E E E E E E E E E

E     

 

The active stress S is dened as

a

l T E T l

c a a max s

T T Al B t B t l

max c r s d s s

where the functions T Al B t and B t l are explicitly dened and l satises

c r s d s s c

the ordinary dierential equation

dl T T

c a max

v T T

 a max

dt T T

a 

T T T dl

a max a c

v exp a T T

 T a max

dt T T T

a  

It is a feature of nonlinear elasticity that standard puretraction tractiondisplacement

and puredisplacement problems mayhave more than one solution and this is indeed

desirable see Ciarlet Mathematical Elasticity Vol I ThreeDimensional Elasticity Cia

page An example see Gurtin Gur p shows that if an incompressible isotropic

homogeneous cub e is loaded uniformly and the constitutive equation is of the form

T

T I FF

where is a real numb er and is a given constant then there may b e up to dierent

solutions of the tension problem

As shown by Ball see Ciarlet Cia p the displacementtraction problem has a

solution if among other conditions the storedenergy function W is p olyconvex that

is

W E W x F CofF det F

where W is convex

In the accompanying talk we will try p erhaps provo catively to stimulate discussion on

several questions

Which mo del is appropriate

Whichnumerical metho ds are b est

What should b e the goal of mo delling

The Goal of Mo delling

We conclude with a numb er of questions

Which if any of the following should b e included in a mo del

Fibre direction

Porous ow

Residual stress

Restoring forces

Arteries veins

Inertia

Epicardium Endo cardium Pericardium

Is it true to say that current mo dels can predict global relationships such as the

pressurevolume curve reasonably well

Is the next goal the prediction of lo cal variables particularly in diseased hearts If

so how should one approach this task

Should some standard problems b e develop ed for use in comparing software

Diastolic Expansion

As describ ed in the section the ventricles are closed for a short time ab out s

during which the pressure falls isovolumetric relaxation Then the tricuspid and mitral

valves op en and the ventricles ll with blo o d from the atria ab out s

The mechanisms underlying the motion of the ventricles during diastole have b een the sub

ject of conjecture for manycenturies Lunkenheimer Lunkenheimer and Torrent Guasp

LLG pages summarize the developmentofvarious explanations from Aristotle

to the presentday Gilb ert and Glantz GG give a recent review as do McCullo ch

and Omens MO p Fung Fun p quotes the Chinese b o ok Internal Classic

written ab out BC but the ideas seem very imprecise

wn in Figure In par The variation of blo o d pressure with time during diastole is sho

ticular it can b e seen that initially the blo o d pressure continues to fall From this and

from direct measurements Meesmann Mee and Robinson Factor and Sonnenblick

RFS it is usually concluded that diastolic suction takes place that is that the heart

walls expand and suck blo o d in While this is quite likely it do es not seem to b e essential

one could imagine a system in which the pressure decrease arose b ecause the ventricles

expanded and the pressure dropp ed in accordance with the Law of Laplace see Equation

on page

To explain the observations two basic mechanisms suggest themselves

Ventricular Blo o d Pressure

In Harvey asserted that the blo o d pressure is the sole driving force during diastole

and that the ventricle muscles play no role While this is not completely true the blo o d

pressure is certainly an imp ortant factor Towards the end of the ventricular lling phase

the atria contract thereby forcing more blo o d into the ventriclesthis is called the atrial

b o ost and is of imp ortance during exercise when the time for passiveventricular lling

is reduced see Levick Lev page

The role of the lling blo o d pressure seems to us to have b een somewhat neglected in

the literature on mo delling So far as weareaware only Peskin and his coworkers have

mo delled the ow of blo o d in the atria and ventricles see PMb These results are

signicant but they do not so far as we can see provide values for the blo o d pressure

which can b e compared with the observations in Figure

Myo cardial stress

Although the heart is relaxed during diastole the heart walls are not stress free For

example in PPL fragen Dr James Johnson see Philip Phi p found that the

freshly excised heart of a turtle continues to b eat and prop els itself forward when placed

in water where the eect of lling pressure is absent Three sources of stress have b een

considered

Elastic Recoil

It has b een known but at times forgotten PPL fragen since the work of Vieussenius in

see Vie that the relaxed heart recoils It is p ossible to observe this an empty

ventricle expands after b eing compressed manually see Lunkenheimer Lunkenheimer

and Torrent Guasp LLG p In the past various mechanical mo dels have b een

prop osed to explain the elastic recoil For example in Figure a mechanical mo del for

wn Hort suggests that the intramyo cardial tissue elastic recoil due to Hort Hor sho

between the myo cytes is twisted during systole and then recoils during diastole

Recently scanning electron microscop es have b een used to reveal the detailed structure of

the connective tissue in the myo cardium However this has not yet led to an acceptable

constitutivelaw see Hunter and Smaill HS p

Hort Hor considers the question of reorientation of the bres during systole and di

astole Thus Hort Hor p Aus der Ueb ereinstimmung des Faserverlaufes in

kontrahierenden und dilatierenden Herzen geht hervor dass es in der Herzmuskulatur

eine Mechanismus geb en muss der es den einzelnen Muskelschichten ermoglicht sichver

schiedenen Kammerfuellungen durch Aenderungen der Schichtdicke und Flaechengro esse

anzupassen

Hort Hor p also discusses the idea that energy is stored during systole for release

during diastole and quotes FeneisF ennBenningho Rushmer Chrystal and W agner

See Lunkenheimer There is a mistake here since neither Hort Hor nor Hort Hor has this

gure

Figure Horts Mo del for elastic recoil

Residual Stress

Fung Fun p vigorously argues the case that at the end of systole the heart has a

residual stress distribution stress in the absence of external forces This idea has b een

develop ed by Omens Ome and McCullo ch and Omens MO p Fung p oints

out that residual stress is wellknown and used in engineering Both Fung Fun p

and McCullo ch and Omens MO p show examples of living tissue which relaxes

when cut thus proving the existence of residual stress

The dierence b etween residial stress and elastic recoil app ears to b e as follows Resid

ual stress can arise in statically indeterminate elastic b o dies even when the constitutive

equations are linear Elastic recoil presupp oses that while the myo cyte bres are con

tracting during systole other comp onents are b eing compressedin other w ords elastic

recoil presupp oses a nonlinear mechanism in which dierent elastic comp onents act during

systole and diastole CWC check

Residual stress mayplay a role in several ways

If the constitutivelaws are nonlinear then the relationship b etween incremental

stress and incremental strain dep ends up on the total stress and is thus aected by

any residual stress

If residual stress is included then the total stress distribution is found to b e smaller

as would b e exp ected in an organ which has develop ed b oth through growth and

through evolution The PhDthesis of Omens see Ome contains a very clear

description of residual stress and its measurement

Residual stress may aect the coronary blo o d ow and hence inuence the onset of

ischaemia reduced blo o d supply see Ome page

The relationship b etween residual stress and cardiac hyp ertrophy enlargement

of the myo cytes due to an increased workload is investigated by Omens in

Chap er V Ome

Yang Tab er and Clark YTC allow for residual stress in their mo del of the embryonic

chick heart

Ventricular Geometry

As is clear from Figure the heart is a complicated threedimensional ob ject In

Woods Wo o mo delled the left ventricle as a thinwalled sphere Later thinwalled

ellipsoidal geometry was used by several authors Since the left ventricular wall is of com

parable thickness to the ventricular radius thickwalled mo dels were intro duced For

references see Hunter and Smaill HS p

Only comparatively recently have fully threedimensional measurements b egun to b ecome

available The fully threedimensional ventricular geometry of the dog heart was measured

mechanically by Nielsen Nie and Nielsen Le Grice Smaill and Hunter NLSH The

present authors intend to provide similar information for the human heart in the near

future PPL fragen

So far as we are aware Octob er no workers haveasyet used mo dels with full

threedimensional geometry for the human heart

A large numb er of p ossible factors can b e considered

Geometry

Cylindrical

Spherical

Woods W oo

Ellipsoidal

Wong and Rautaharju WR

Prolate Spheroidal

Mirsky Mir

Shell Theory

Thin

Wo o ds Wo o

Thick

Mirsky Mir

Wong and Rautaharju WR

Constitutive StressStrainEquations

Linear Elasticity

The symp osium The Physiological Basis of Starlings Law of the Heart Sym page

contains interesting articles and discussions on general topics such as the eect

of geometry

Chapter

Muscle Mechanics

Intro duction

A muscle is any one of the contractile brous band or bundles that pro duce movement

in animal b o dies A muscle is therefore biological tissue which can b e either relaxed or

activein the latter state force can b e generated F or our purp oses weareinterested in

muscle mechanics the study of the motion of and forces generated bymuscles

The two basic typ es of muscle striated muscle and smo oth muscle dier in their

organization Striated muscle cells are organized very systematically and when viewed

under a microscop e have a denite banded structure Smo oth muscle cells are organized

much less regularly

Striated muscles o ccur as

skeletal muscles which make up approximately p er cent of the human b o dy

byweight As the name suggests the skeletal muscles are attached to the skeletal

structure of the b o dy and are resp onsible for the movement of arms legs etc

cardiovascular muscles which make up ab out p er centCWCcheck of the

human b o dy byweight and are the source of the forces in the heart Although similar

in structure to skeletal muscles they also dier in imp ortantways

Approximately p er cent of the human b o dy is smo oth muscle which is found in the

inner organs the eye the blood vessels etc There are two ma jor typ es Guyton Guy

p

Multiunit smo oth muscle which is comp osed of discrete smo oth muscle bres

each of which can contract indep endently of the others

Singleunit smo oth muscle which consists of hundreds or millions of muscle bres

that contract together as a single unit This typeofsmoothmuscle is also known

as synctial smo oth muscle or visceral smo oth muscle

The ab ove classication of muscles is very broad within eachtyp e of muscle there are

many sp ecial varieties each one adapted to its particular role

For our purp oses we wish to characterize the motion of and the forces generated bymus

cles so that these can b e incorp orated into mathematical mo dels Two basic approaches

can b e followed

The phenomological or engineering approach in which the elastic prop erties

of muscles are measured in the lab oratory and used to formulate constitutivelaws

Under this heading we include the the classical exp eriments on muscles of Blix

Bli Hill Hil

The molecular approach With the development of highp owered electron mi

croscop es and sophisticated chemical metho ds it has b ecome p ossible to elucidate

the structure and mechanisms of individual muscle cells to the extent that one can

for example say that a particular typ e of cell has ab out myosin heads p er m

which form crosslinks with the adjacent actin molecules

Of the two appproaches mentioned ab ove the molecular approach is clearly the more

fundamental However for the forseeable future this approach cannot by itself provide

all the information needed by the mo deller

The molecular approach has concentrated on the contractile units the sarcomeres

But one must also take account of the elastic prop erties of other comp onents of the

muscle

Even when the mechanism of the sarcomere is fully understo o d this is not the end

of the story b ecause the activation is caused by calcium ions whose densitymust

b e mo delled

On the other hand the phenomological approach is also not without diculties

The preparation and testing of sp ecimens is dicult

The stressstrain resp onse is highly nonlinear It is not clear how the strain energy

function should b e chosen In at least one case Smaill and Hunter SH p the

b estt material parameters havephysically unacceptable values

The mo deller should therefore combine the information from b oth the phenomological

and the molecular approach The situation is wellsummarizedby the following quotation

from Smaill and Hunter SH pages

Wehave already stated that any realistic constitutive formulation for pas

sivemyo cardium must incorp orate microstructural information It is worth re

iterating that an appropriate constitutivelaw should b e compact with unique

material parameters Wehave demonstrated that the last of these require

ments cannot easily b e met by phenomenological constitutive formulations

that use highly nonlinear functions However it is unlikely that the rst re

quirement could b e satised by a constitutivelaw based completely on cardiac

mircostructure Thus a constitutive formulation that incorp orates the most

advantageous features of b oth phenomenologically and microstructurebased

approaches app ears the b est option at present

In the reminder of this chapter we rst summarize these two approaches and then conclude

with some typical mo dels of cardiac muscle

Some general references include

R McNeill Alexander Elastic Mechanisms in Animal Movement Ale

A V Hill First and Last Experiments in Muscle Mechanics Hil

Z He Mathematical models in muscle by periodic stimuli He

Thomas A McMahon Muscles Reexes and Locomotion McM

Rob ert M Miura Lectures on Mathematics in the Life Science Vol Some Math

ematical Questions in Biology Muscle Physiology Miu

ter Keurs and Noble Starlings Law of the Heart Revisited tKN

Hopp ensteadt and Peskin Mathematics in Medicine and the Life Sciences HP

Daniel J Schneck Mechanics of Muscle Sch an engineering approach

Yuancheng Fung Biomechanics Mechanical Properties of Living Tissues Fun

Chapter Skeletal Muscle Chapter Heart Muscle and Chapter Smo oth

Muscle

The b o ok of McMahon Muscles Reexes and Loc omotion McM is an excellentintro

duction

The Phenomological Approach

Muscle in particular cardiac muscle is a biological material which can b e either relaxed

or passive during diastole or active during systole It is usual to consider these states

separately

Early in this century the term new elastic b o dy was coined to convey the idea that

excitation of muscle instantly changes its elastic state from a compliant level into a sti

level The excited muscle thus b ecomes a new elastic b o dy

Hill and other physiologists likened contracted skeletal muscle to a co cked

spring sp eculating that the amount of energy released by contraction dep ends only on

the preloaded lengththis w as disproved by the discovery of the Fenn eect byFenn

Fen see Sagawa Maughan Suga and Sunagawa SMSS p

The Fenn eect

The Fenn eect was rst observed byOFenn in in a skeletal muscle isotonically

contracting at a constant preload the total heat generation plus external work signicantly

increased and then decreased as the extent of shortening was increased by decreasing the

afterload force from isometric force to nearly zero Sagawa Maughan Suga and Sunagawa

SMSS p See Rall Ral

Feng eect

Concerning the Feng eect see

Ciba Foundation The Physiological Basis of Starlings Law of the Heart Symp

Feng The eect of length on the resting metabolism of muscleFen

Classic Results

For the purp oses of biomechanics it is necessary to determine the force generated bya

muscle It turns out that in cardiac muscle these is a complicated relationship b etween

the force develop ed the length of the muscle the velo city of shortening and the time see

eg Brutsaert Bru

To a growing extent this relationship can b e explained at the molecular level as briey

discussed in Section Here we describ e some classical results

Some brief remarks on early workonmuscle mechanics with esp ecial reference to car

diac muscle are given by Guz Guz and Jewell Jew It was shown bySchwann in

that muscles contract more forcibly when stretched A famous pap er by Blix in

Bli studied the relation b etween length and tension in muscle Early exp erimental

work on the heart is due to Roy Martin Howell and Donaldson

and Roy and Adani The most widely quoted pap ers are those of Otto Frank

Fra on the frog heart and Patterson Pip er and Starling PPS the latter pap er

presenting work p erformed at University College London and the University of Berlin

It is interesting that these work ers b egin their pap ers by quoting work on isolated muscles

and using this as a guideline for their own work on the heart

Atypical exp erimental setup for a single muscle is shown in Fig The muscle is rst

xed at one end and then stretched using a small weight w the preloadThemuscle is

then stimulated electrically As it shortens it picks up a second weight W the afterload

Some basic mo des of testing are

isotonic Here the muscle is allowed to shorten the b earing afterload W The force

is thus known The length of the muscle and sp eed of shortening are measured See

ii and iii in Fig

isometric loading Here the muscle length is kept xed The tension is measured

See i in Fig

As can b e seen from Fig an increase in the initial length of the muscle leads to an

increase of tension velo city and shortening Several comments are due here

Avery plausible explanation of the

In Fig the dep endency on time is not shown

In Fig the lengthtension curveonlygoesuptothemm ordinate

Mo dels

Wehave not consulted these early pap ers

Figure Contractile b ehaviour of isolated myo cardial muscle

Left Simplied diagram of arrangement used to study the contraction of isolated cat

papillary muscle The arrangement shown allows isotonic contraction to o ccur the weight

lab elled afterload b eing picked up as so on as shortening b egins The weight lab elled

preload sets the resting length If the preload is clamp ed in place contraction b ecomes

isometric Right Three fundamental relations i shows isometric contraction at increas

ing lengths ii and iii show isotonic contractions b eginning from two dierent resting

lengths mm and mm Contractile force velo city and shortening are all increased

by stretching the relaxed muscle See Sonnenblick Son From JR Levick An In

troduction to Cardiovascular Physiologyby p ermission

Molecular Muscle Mechanics

In Hugh Huxley and J Hanson HH and Huxley and Niedergerke HN inde

p endently prop osed a mo del on the molecular level for

Ventricular Interaction

So far as we are aware February no workers haveasyet mo delled ventricular

interaction The inuence of the rightventricle is discussed by McCullo ch and Omens

MO p and Antaki Ant p who give further references Since the

twoventricles share muscle bres and adjoin one another one must exp ect a signicant

iteraction see SG and SGL Inuence of epicardium etc see Hunter and Smaill

SH p and Fung Fun p and Humphrey and Yin HY

PassiveMyo cardium

Passivemyo cardium is an inert biological material whichcanin principle b e tested in

the lab oratorysothatin principle constitutivelaws can b e exp erimentally determined

There are however many diculties some of which are mentioned b elow

Exp erimental Metho ds and Results

General references on the testing of biological materials will b e found in App endix H

We are not concerned here with hte sp ecic techniques but do wish to draw attention to

some of the diculties see also Smaill and Hunter SH p

Soft biological material can b e damaged on excision It is also necessary to a buer

solution and to keep the sp ecimen in control the temp erature See also Fung Fun

p

o cardium is threedimensional but so far to our knowledge as of April The my

only onedimensional uniaxial and twodimensional biaxial tests have b een car

ried out



Almost all tests have b een carried out on papillary muscle and trab eculae carnae

But the myo cardium is far from b eing homogenous as observed for example by

Feneis Fen and shown in recent electron micrographs see eg Figures A to

D in Smaill and Hunter SH

The elastic prop erties of the passivemyo cardium have b een measured byseveral workers

including Pinto and Fung PF terKeurs Rijnsburger v an Heuningen and Nagelsmit

tKRvHNYin Strumpf Chew and Zeger YSCZ In Figure w e repro duce the

representative results of Smaill and Hunter SH

Figure illustrates several p oints

The stressstrain curves are monotone and convex



We remind the reader that the papillary muscles bulge from the endo cardium and are attached to

the chordae tendineae see Figure Crosssections The trab eculae carnae also bulge from the inner

wall but are not as conspicuous as the papillary muscles

Figure Stressextension relations for left ventricular midwall sp ecimen during st

th and th cycles of equibiaxial loading Cycle p erio d sec and sp ecimen thickness

mm The solid lines indicate the order of loading in the crossb er direction for

clarity these are omitted in the b er direction

There is a p ointbeyond which the material do es not stretch

For the same strains the stress in the bre direction is far higher than that in the

crossbre direction

The crude estimates of Youngs mo dulus E are quite low For the bre direction

an extension ratio of corresp onds to a stress of kPa That is

stress kP a

E kP a

strain



For comparison

Material Youngs mo dulus E

Steel

stainless steel GPa

Tendon

wet tendon GPa

Thuswet tendon is ab out







times stier than the passivemyo cardium The great discrepancy b etween tendons

and muscles is simply explained a tendon is a relatively simple material which

must only transmit tension In the context of the heart one sees that relatively thin



chordae tendineae suce to transmit the forces develop ed by the papillary muscles

Constitutive Equations

Given exp erimental data such as that in Figure one must construct corresp onding

constitutive equations which express the stress as a function of the strain and p ossibly

other prop erties

StrainEnergy Functions

Although the stress is known to b e dep endent on time relaxation past history a la

Bowditch and frequency of stimulation see section the ma jorityofworkers have



See Kaye and Laby Physical and Chemical Constants KL and Bennet Ker Dimery and Alexan

der Regional deformation and contractile function in canine right ventricular freewallBKDA Dry

tendon has substantically dierent prop erties see Vincent Structural Biomaterials Vin



We are not aware of measurements of the elastic prop erties of the chordae tendineae and are assuming

that they are mimilar to those of other tendons

chosen to formulate the constitutive equations using a strainenergy function That is

W E

S

E



where S is a stress tensor E is a strain tensor and W is a strainenergy function

Bovendeerd

Bovendeerd Bov page suggested the following strainenergy function

W E

S

E

where S is the second PiolaKirchho stress tensor based on the deviatoric Cauchy stress

tensor and E is the GreenLagrange strain tensor

The myo cardial tissue is assumed to b e transversely isotropic with resp ect to the bre

direction With resp ect to an orthonormal co ordinate system with direction e parallel to



the bre direction and crossbre directions e and e the strain tensor E is written as the



strain matrix E with comp onents E The strainenergy function WE for a material that

ij

is transversely isotropic with resp ect to e can b e expressed as a single valued function



of the following set of scalars Malvern Mal Green and Adkins GA page

I E E E

E  

  

II E E E E E E E E E

E     

 

III det E

E



I E



E

  

II E E

E  

ischosen so that W is zero in the unstrained state The functional form of W E

stress is an exp onential function of strain and no stresses are predicted in the unde

formed situation The following strainenergy function is consistent with these conditions

h i

   

W E C expa I a II a E a E E

 E  

E   

Because of the additional condition of incompressibility of the cardiac tissue the scalar

III is left out of this strainenergy function The values of the material parameters are

E

estimated from tting this function to exp erimentally obtained data Firstly according to

the exp erimental ndings of Yin Strumpf Chew and Zeger YSCZ the ratio of second

PiolaKirchho bre to crossbre stress is required to equal under conditions of equal

bre and crossbre stretch This condition is satised by setting

a a a

 

Secondly it is required that the uniaxial stressstrain data obtained by ter Keurs Rijns

b erger van Heuningen and Nagelsmit tKRvHN are describ ed reasonably well Thirdly

a is set at zero b ecause of the lack of exp erimental data on the mechanical b ehaviour of



cardiac tissue under conditions of shear stress The resulting parameter values are listed

in table



See App endix G

parameter C a a a a

  

value

unit kPa

Smaill and Hunter

Smaill and Hunter SH p adapt a suggestion of Fung and use the following strain

energy function for passivemyo cardium

Q Q 



W C e C e



where

  

Q C E C E E

 

 

and

 

Q C E E C E E E

      



It is hereby assumed that the material is transversely isotropic direction is aligned with

the bre axis The stress is given by

W W

p

ij ij

E E

ij ji

where p is the hydrostatic pressure The b estt parameters for four left ventricular mid



wall sp ecimens are given in Table

C C C C C C

    



mean

n

Table Bestt material parameters for left ventricular midwall sp ecimens

Inverse Metho ds for Parameter Estimation

Given the diculty of direct measurement some authors have constructed mo dels and

then estimated the parameters so as to t the observations

Guccione McCullo ch and Waldman GMW

Sideman



where wehave corrected apparent errors in the mean and standard deviation for C



Chapter

Cardiac Mechanics

Intro duction

The myo cardium is a complex structure containing see Robinson and Kinne RK

Smaill and Hunter HS Horowitz Hor and Lunkenheimer et al LRC b

myo cytes The myo cyte is the hearts muscle cell In shap e it resembles an ellip

soidal cylinder with a diameter of m and length of m The cell is

branched and is attached to adjacent cells in an endtoend fashion Eachmyocyte

is connected with several others to form a threedimensional network of cells The

interface b etween adjacent cells is called an intercalated disk

coronary blo o d vessels Within the heart wall is a dense network of coronary

blood vessels One or more capillaries run along the b oundary of eachmyo cyte

parallel to the long axis The coronary arteries and veins act muchlikerivets within

the wall

collagen matrix Individual myo cytes and bundles of myo cytes are connected by

a collagen matrix which consists of a dense network of struts of collagen typ e I

and typ e I I I predominate

connective tissue Additional connective tissue consists of collagen elastin gly

coaminoglycans and glycoproteins

The interstitial space or interstitium between cells is lled by interstitial uid

Since the p ores are so small the uid moves mainly through diusion

The monograph edited by Robinson and Kinne RK Cardiac MyocyteConnective Tis

sue Interactions in Health and Disease Issues Biomed provides a very readable overview

of the structure of the myo cardium Topics considered include

The bio chemistry of the myo cardium

The structure of the connective tissue

The elastic prop erties of myo cytes

In particular Covell Cov discusses the functional dynamics of the myo cardial tissue

Robinson Rob summarizes results obtained using scanning electron microscopy the

light microscopyhighvoltage transmission electron microscopyantib o dy lo calization

and in situ hybridization For our purp oses the following observations are of particular

interest

Robinson see page rep orts on signicant dierences on collagen contentinrats

see Table

Young adults Aged rats

Left ventricle

Rightventricle

Table Collagen content

Robinson Rob p summarizes the o ccurrence of four selfsimilar patterns frac

tal analysis of structures weave branced bre bilt and heliv These patterns o ccur

at several levels

Robinson Rob p sp eculates on the transfer of information b etween myocyte

and broblast

Robinson Rob p raises the question of the relativemechanical strengths of

dierent networks

Robinson Rob p refers to ma jor dierences in cases of stunned myo cardium

or infarct

For mo delling purp oses it is necessary to set up constitutivelaws which mo del the my

o cardium on a larger scale but it is of course imp ortant to take account of the microscopie

structure We therefore briey describ e the comp onents of the hearts wall in somewhat

greater detail b efore moving on to describ e p ossible constitutivelaws

The Comp onents of the Hearts Wall

Exp erimental StressStrain Measurements

ConstitutiveLaws

There is an extensive literature on the mechanical prop erties of isolated cardiac muscle

The rst exp eriments were apparently p erformed by Sonnenblick Son who measured

the b ehaviour of isolated myo cardial cat muscle His results are shown in Figure

These results show that stretching the muscle enhances its subsequent contractile energy

in agreement with the FrankStarlingLaw Levick Lev p discusses the physiologi

cal mechanisms underlying this b ehaviour

This seems very late PPL fragen

Hydraulic Eects

Living tissue is bathed in liquid PPL fragen In addition the heart is crisscrossed by

a network of blo o d vessels As a result one may regard the myo cardium as a structure

of bres and blo o d vessels surrounded by uid The pressure in coronary blo o d vessels

is called the p erfusion pressure or coronary p erfusion pressure PPL fragen and

provides a mechanism to explain the expansion of the ventricles There is an analogy with

a hosepip e which straightens as it is lled with water For this reason hydraulic eects are

sometimes called the garden hose eect See Lunkenheimer Lunkenheimer and Torrent

Guasp LLG p for further references See McCullo ch and Omens MO pages

and pages and Hunter and Smaill HS pages for an evaluation

of the inuence of coronary p erfusion

McCullo ch McC rep orts on measurement on the eect of coronary p erfusion on left

ventricle mechanics The pressure in uid outside the myo cardial bres and blo o d vessels

is called the intramyo cardial pressure See Rabbany Rab

Several mo dels take account of the uid in the myo cardium A theory for an elastic struc

ture lled with a uid think of a sp onge was rst formulated by Biot Bio It was

later extended to the case of nite deformations by Biot Bio and was further gen

eralized to a theory of mixtures byBowen Bow Bow These ideas have b een

used CWC check by Bogen see Boga and Bogb to mo del the swelling of tissue

Huyghe van Camp en Arts and Heethar HvCAH use a p orous medium nite element

mo del to mo del the diastolic left ventricle

Bogen Boga Bogb considers strain energy descriptions of biological swelling In

the second article multiple uid compartment mo dels are considered together with their

application to cardiac muscle The mo dels are visualized as constisting of networks of

springs or elastic tub es For the case of a single uid with two elastic networks a and b

Bogen Bogb equ suggests the strain energy function

k k k

k  k 

a a a a

a a

s

 

s s

k

a

k  k  k 

a a a 

k k a

 

a s

K

a

k k k

k  k 

b b b

b

b b

s

 

s s

k

b

k k  k  k 



b b b

k

b

 

b s

K

b

Bogen draws some general conclusions but do es not give sp ecic applications to the heart

He also considers the puzzling observation byPogatsa Koltai and Grosz PKG that

the ventricular stiness increase when myo cardial water content is either increased ab ove

or reduced b elow the normal water content PPL fragen

In the rst article Bogen considers various p ossible laws and shows that some are imp os

sible Boga p

Myo cytes

Concerning myocytes see

RabbanyFunai and No ordergraaf RFN

Chapter

Mo delli ng the Fibre Architecture of

the Myo cardium

In Part I the observations of the brous structure of the myo cardium have b een describ ed

In this chapter we attempt to use geometrical and top ological metho ds to describ e this

structure There seem to b e several p ossibly useful to ols

Foliations

In various works eg Krehl Kre Pettigrew Pet Streeter Str Figure Torrent

Guasp Gua the heart and in particular the left ventricle is depicted as consisting of

nested shells

Mathematically this corresp onds to a twodimensional foliation of the heart or left

ventricle the individual shells b eing called leaves

Top ology

The analysis of threedimensional structures is treated by Winfree Win pages

Chapter and and pages References given include

Bouligand Bou

Gordon and Winfree GW

Thursten and Weeks TW

Delbruck Del

Fuller Ful

Fuller Ful

See App endix Foliations

Winfree Win

Winfree and Strogatz WS

Geo desics

Concerning geo desics see

Thompson On Growth and Form Tho p

Chapter

Mo dels with Spherical Geometry

The Law of Laplace

We b egin the Law of Laplace whichwas rst stated byWoods Wo o can b e derived

with the help of Figure see Fung Fun page

Figure The Law of Laplace

Consider a thickwalled hemisp erical shell with inner radius r thickness t and outer

radius r t Let the pressure acting on the outside b e p pressure from p ericardium



Consider the equilibrium of forces in the vertical direction One obtains

   

r t r p r p r t

i 

where is the average circumferential wall stress

Hence

 

p r p r t

i 

 

r r t

When p and t is small we obtain in the limit as t the equation



p r

i

t

for the stress which can also b e written in the form

t

p

i

r

For applications see Woods Wo o Moriartiy Mor and Grossman Gro

The equation is the simplest form of a relation known as the Law of LaplaceIt

shows that the pressure created by a thin shell is prop ortional to the thickness t prop or

tional to the circumferential stress and inversely prop ortional to the radius r

Laplaces Law is often used to compute the stress in the left ventricular wallin fact the

curvature of the left ventricular is often negative see Greenbaum and Gibson GG

If we wish to obtain expressions for the pressure p the circumferential stress and the

i

thickness t as functions of r it is necessary to derive additional equations

Let the original shell have radius R and thickness T Since the volume of the heart wall

remains nearly constant wehave

   

R T R r t r

so that

   

r t r R T R

For small t we obtain

 

r t R T

Next we need a relationship b etween the wall stretch and the wall stress We use

the relationship prop osed byValanis and Landel VL

C H

where C and H are constants and tting this to the data for rat papillary muscle it is

found Moriarty Mor page that



C

with

The value for C seems to dier greatly from values given byFung Mechanical Properties pages

and

and



C g cm

Pa

Pa

The equations and comprise a system of three equations from which t

and p can b e determined as functions of the radius r or equivalently as functions of the

i





left ventricular volume v r



Spherical Mo dels

We summarize the predictions for the pressurevolume P V and pressurestress P S

relations predicted byseveral mathematical mo dels in which the left ventricle LV is

mo delled as a spherically symmetric sphere Wedraw heavily on the article of Moriarty

Mor Chapter of the b o ok of Mazumdar Maz contains a short description of some

mo dels apparently also based on the pap er of Moriarty

Analytical Work

There is clearly relatively little scop e for analytical work Nevertheless suchworkisof

ten valuable since it provides guidelines and viewp oints in a way that numerical results

cannot do

The sort of results which one might hop e to establish analytically would b e of the form

To show that for a certain class of mo dels particular a eg variable the circumfer

ential wall stress increases monotonically from epicardium to endo cardium

To show that for a certain class of mo dels a particular variable e g the wall stress

is maximized for axially symmetric geometry

In greater generalitytheLaw of Laplace can b e stated as follows

Let P denote the normal force exerted by the heart wall on the blo o d in the ventricle

the Let S b e the tangential stress in the wall w the thickness of the wall and R and R





principal curvatures Then the Law of Laplace states that

P Sw

R R



Woods Woo veried this formula exp erimentally Authors using the formula to com

pute the stress in the hearts wall include

Sandler and Do dge SD for patients with heart disease using b oth R and R





Sometimes called the LaplaceYoung equation since it was discovered indep endently by the Marquis

de Laplace and Thomas Young

Comparison of Mo dels

References in whichvarious mo dels are compared include

Huisman Sipkema Westerhof and Elzinga HSWE

Sandler and Do dge SD use Laplaces Law to estimate wall stress They quote references

to show that the dierence b etween thinwalled and thickwalled mo dels is of the order

of Sandler and Do dge SD p

Chapter

Mo dels with Cylindrical Geometry

Theo Arts A Mathematical Model of the Dynamics of the Left Ventricle and the

Coronary Circulation Art mo del the left ventricle as a cylinder comp osed of

concentric cylindrical shells

Arts Reneman and Veenstra Amodel of the mechanics of the left ventricle ARV

To ezeren Static analysis of the left ventricle To e

Feit Diastolic pressurevolume relations and distribution of pressureandber ex

tension across the wal l of a model left ventricle Fei

Chadwick The myocardium as a uidber continuum passive equilibrium congu

rations Cha and Chadwick Mechanics of the left ventricle Cha

Caisch Strukturgerechte Analyse der Myokardfaserspannungen Caf

Pelle Ohayon Oddou and Brun Theoretical models in mechanics of the left ventri

cle POOB

Skalak Approximate formulas for myocardial ber stresses Ska

Costa Hunter Wayne Waldman Guccione and McCullo ch A threedimensional

nite element method for large elastic deformations of ventricular myocardium Part

II Prolate spheroidal coordinates CHW

Guccione McCullo ch and Waldman GMW Passive material properties of intact

ventricular myocardium determinedfrom a cylindrical mode construct a cylindrical

mo del which they use to estimate material prop erties

In their second pap er Arts Veenstra and Reneman AVR compare their theoretical

results with exp erimental data for four dogs and obtain go o d agreementCWC check

Chapter

Mo dels with Spheroidal Geometry

Beyar and Sidemean Spatial energy balance within a structural model of the left

ventricle BS

Bovendeerd Huyghe Arts van Camp en and Reneman Inuenceofendocardial

epicardial crossover of muscle bers on left ventricular wal l mechanics BHA

also incorp orate transversal bres

Bovendeerd Arts Huyghe van Camp en and Reneman Dependenceoflocal left ven

tricular wal l mechanics on myocardial ber orientation A model study BAH

Beyar and Sideman Acomputer study of the left ventricular performancebased

on the ber structure sarcomere dynamics and transmural electrical propagation

velocity incorporate bres and electrical propagation BSa

Bovendeerd PhD thesis The Mechanics of the Normal and Ischemic Left Ventricle

During the Cardiac Cycle A Numerical and Experimental Analysis Bov

ter Rogers Guccione Waldman and McCullo ch A threedimensional Costa Hun

nite element method for large elastic deformations of ventricular myocardium

Part I Cylindrical and Spherical Polar Coordinates CHR and Costa Hunter

Wayne Waldman Guccione and McCullo ch A threedimensional nite element

method for large elastic deformations of ventricular myocardium Part II Prolate

Spheroidal Coordinates CHW

Chapter

Mo dels with Additional Features

The Pericardium

Only a few workers have mo delled the p ericardium

Misra and Singh MS incorp orate the p ericardial pressure in their mo del and con

clude MS page that the eect of the p ericardial pressure which is assumed

to b e onetenth of the left ventricular pressure is quite prominent

Humphrey and Yin HY discuss the eect of the p ericardium Fung Fun p

also comments on the role of the p ericardium

Fibres

Hydrostatic Skeletons and Muscular Hydrostats

A hydrostatic skeleton see Kier Kie is a uid mechanism that provides a means by

which contractile elements maybeantagonized Hydrostatic skeletons o ccur in a remark

able variety of organisms with examples from not only invertebrates but also vertebrates

Ahydrostatic skeleton is typically considered to include a liquidlled cavity surrounded

byamuscular wall reinforced with connective tissue bres

A muscular hydrostat is a hydrostatic skeleton that consists of a tightly packed three

dimensional arrayofmuscle bres Examples include the tentacles of the o ctopus the

tongues of many animals and the trunk of an elephant

There are obvious similaritiesbetween muscular hydrostats and the brous structure of

the heart wall Thus Lunkenheimer and Whimster LW section use the structure

of the uvular muscle and the tongue to illustrate p ossible mechanisms during diastolic

unfolding

There are some interesting mathematical problems in this area For example Kier Kie

page considers helical muscles wrapp ed around a circular cylinder and claims that

there is a torsional force with no longitudinal force only if the angle of the muscles is

exactly

See also

Johnson and Kier JK

Alexander in Chapter Fibrewound animals of Elastic Mechanisms in Animal

Movement Ale

See also Alexander Ale Clark and Cowey CC and Harris and Crofton HC

For a brief useful accountofvarious biological structures see Chapters and of Lifes

DevicesbyVogel Vog

FluidFibre Mo dels

Several authers have considered uidbre mo dels in whichthemyo cardium is treated

as a uid with an emb edded bre matrix Such mo dels thus ignore the elasticity of the

myo cardium but b ecause of their simpicitiy can sometimes b e solved analytically See

Caisch Caf

Fung Fun p

Skalak Ska

Chadwick und Cha Cha

For example Chadwick Cha considers the bre direction as a given function of x

The Cauchy stress tensor  takes the form

p T

ij ij i j

where T is the magnitude of the bre tension The equation of equilibrium is

div 

If ux denotes the displacement

xx ux

then since the material is assumed to b e incompressible

div u

Finally the equations are completed by an equation which expresses the relationship

between the bre tension T the time t and the bre deformation

ru



T tE tE tT





where the constants E and E represent the passive and active elasticity mo duli T is a



constant and tisa given function of time reecting the transition b etween active and

passive states

Systolic Contraction

As describ ed in the section the ventricles are closed for a short time ab out

s during which the pressure rises and the ventricles deform isovolumetric contraction

This is followed by a p erio d lasting ab out s during which the blo o d is ejected

The contraction of the heart muscles is iniated by electrical impulses the propagation of

which is discussed in Section The literature on systolic contraction involving active

muscles seems to b e much smaller than the literature on diastolic expansion involving

passive muscles

Relatively early calculations were p erformed by Ghista and Hamid GH and Chadwick

Cha while Waldman Wal discussed the coupling of the heart to the circulatory

system

Beyar and Sideman BSb consider systolic contraction under the following hyp otheses

The LV left ventricle is a thickwalled prolate spheroid with time indep endent

shap e ie constant axis ratio

The LV is incompressible

The bre angle acros the myo cardium varies linearly from to in the un

stressed reference conguration and do es not change during systole

The sarcomere length distribution is uniform at the reference conguration

The electrical activation propagates radially from endo cardium to epicardium

The mechanical activation function is half a sinusoidal wave

The stressstrain relationship for the muscle bre is linear

The active stresssarcomere length relationship is linear

The passive stresssarcomere length relationship is exp onential

Transbre stresses are not included

The afterload aortic pressure is mo delled

Beyar and Sideman BSb givea owchart for their Fortran program which calculated

the various variables through out systole Although their work contains a great many

approximations these are clearly stated The parameters used in the mo del are given and

compared with rep orted values The sensitivity with resp ect to various parameters is also

studied

Fibres

The following include bres in their mo del

Bovendeerd Bov

Yang Tab er and Clark YTC mo delling the chick heart

Beyar and Sideman BSb

Authors using more complex mo dels and allowing for bres parallel to the surface include

Costa Hunter Rogers Guccione Waldman and McCullo ch A threedimensional

nite element method for large elastic deformations of ventricular myocardium Part

I Cylindrical and spherical polar coordinates CHR

Costa Hunter Wayne Waldman Guccione and McCullo ch A threedimensional

nite element method for large elastic deformations of ventricular myocardium Part

II Prolate spheroidal coordinates CHW

Recently in his PhD thesis Bovendeerd Bov used a mo del which allowed transmural

bres This work has b een extended See

Bovendeerd Huyghe Arts van Camp en and Reneman Inuenceofendocardial

epicardial crossover of muscle bers on left ventricular wal l mechanics BHA

Bovendeerd Arts Huyghe van Camp en and Reneman Dependenceoflocal left ven

tricular wal l mechanics on myocar dial ber orientation A model study BAH

Yang Tab er and Clark YTC page briey mention observations on bre orientation

in embryonic chick hearts which they incorp orate into their mo del as torsion

Treatment of the Band Structure

The incorp oration of a bandlike structure into a mo del of the heart requires the following

A more detailed description of the orientation of the bres than is currently available

In particular the bandlike structure implies the existence of a twisted structure

which is more complicated than the usual Streeter structure This in turn will

require the use of much greater numb er of nite elements

The bandlike structure explicitly involves the rightventricle which should therefore

b e included in the mo del

Poro elastic Mo dels

Several mo dels take account of the uid in the myo cardium and use p oro elastic mo dels

A theory for an elastic structure lled with a uid think of a sp onge was rst formulated

by Biot Bio It was later extended to the case of nite deformations by Biot Bio

and was further generalized to a theory of mixtures byBowen Bow Bow These

ideas have b een used CWC check by Bogen see Boga and Bogb to mo del

the swelling of tissue Huyghe van Camp en Arts and Heethar HvCAH use a p orous

medium nite element mo del to mo del the diastolic left ventricle Simon and Gaballa

SGa use a p oro elastic nite element mo del to mo del the repsonse of large arteries

See also

Kenyon Ken

For the mathematical theory of p orous ow see Douglas and Hornung DH See also

Sorek and Sideman SSb

Sorek and Sideman SSa

The thesis of Huyghe Huy is extensive The myo cardium is mo delled using a combina

tion of a deformation mo del and a p erfusion mo del CWCmust lo ok further into this

The full cardiac cycle is also mo delled

In his PhD thesis Huyghe Huy mo dels the myo cardium using a p orous medium nite

deformation theory of blo o d p erfused soft tissue He then derives two sp ecial mo dels

A deformation mo del of the b eating left ventricle

A p erfusion mo del of the left ventricular coronary circulation

Numerical results are given and a complete cycle is simulated

Yang Tab er and Clark YTC mo del the embryonic heart of a chick stage

using a p oro elastic mo del This is a reasonable mo del for the chick heart at this stage of

development

Other Factors

In this pap er we are primarily interested in the role played by the bre direction and have

chosen to neglect a variety of other factors

the p ericardium which encloses the heart and restrains the motion of the heart

particularly during certain abnormal conditions Braunwald Bra comments that

whereas the p ericardial space normally contains at most ml of uid this can

increase to litres in severe cases of p ericardial eusion

So far no mo dels have directly considered the role of the endo cardium and epi

cardium whichmay p ossibly b e signicant One reference on this is Humphrey

and Yin Biaxial mechanical behaviour of excised epicardium HY

The heart wall contains a large amount of uid in the form of interstitial uid

and blood The ow of this uid has b een mo delled using the equations of Biot by

Huyghe and coauthors

The PhD thesis of Huyghe Huy

Huyghe Arts van Camp en and Reneman Porous medium nite element model

of the beating left ventricle HAvCR

van Camp en Huyghe Bovendeerd and Arts Biomechanics of the heart muscle

vCHBA

Howeverit should b e noted that in this work the eects of p orosity and elasticity

are uncoupled

In the literature it is customary to neglect the eects of inertia the pap er of

Moskowitz Mos b eing quoted in justication However the pap er of Moskowitz

compares solutions with and without the eects of inertia in a very simple case In

the opinion of the authors this needs further investigation

Residual stress See eg McCullo ch and Omens MO

As observed by Hort Feneis and other authors the myo cardium is not homogeneous

and there are gaps which can b e interpreted as sliding planes If we accept this

how can it b e mo delled

Chapter

Numerical Mo dels

In preceding chapters wehave considered mo dels classied according to their geometry

Here we briey summarize the developmentofnumerical mo dels See

In his PhD thesis McCullo ch Deformation and Stress in the Passive Heart McC

develop ed sp ecial nite elements

Yin Yin

Costa Hunter Rogers Guccione Waldman and McCullo ch CHR

Costa Hunter Wayne Waldman Guccione and McCullo ch CHW

Interesting recentwork includes

Authors using more complex mo dels and allowing for bres parallel to the surface include

Costa Hunter Rogers Guccione Waldman and McCullo ch A threedimensional

nite element method for large elastic deformations of ventricular myocardium Part

I Cylindrical and spherical polar coordinates CHR

Costa Hunter Wayne Waldman Guccione and McCullo ch A threedimensional

nite element method for large elastic deformations of ventricular myocardium Part

II Prolate spheroidal coordinates CHW

Recently in his PhD thesis Bovendeerd Bov used a mo del which allowed transmural

bres This work has b een extended See

Bovendeerd Huyghe Arts van Camp en and Reneman Inuenceofendocardial

epicardial crossover of muscle bers on left ventricular wal l mechanics BHA

Bovendeerd Arts Huyghe van Camp en and Reneman Dependenceoflocal left ven

tricular wal l mechanics on myocardial ber orientation A model study BAH

Yang Tab er and Clark YTC page briey mention observations on bre orientation

in embryonic chick hearts which they incorp orate into their mo del as torsion

Numerical Metho ds

It is prop osed to initially solve the equations using nite elements in particular using the

no de brick element for the displacements and the no de brick element for the pressure

Preliminary calculations were made using the NAG Finite ElementPackage but future

work will probably use Dipack

Chapter

Prop erties of Blood

See

Chapter Biological Fluid Dynamics of An Introduction to Mathematical Physiol

ogy and Biology by Mazumdar Maz

Chapter

Fluid Flow in the heart

Intro duction

See

Sugawara Ka jiya Kitabatake and Matsuo Blood Flow in the Heart and Large Blood

Vessels SKKM

Numerical Metho ds

The ImmersedBoundary Metho d

In a series of pap ers Peskin and collab orators used the immersedb oundary metho d

to compute twodimensional ow in the heart Applications included ow patterns around

heart valves Pes Pes blo o d ow in the heart and the design of cardiac valves An

improved version of the metho d which improves the conservation of mass was recently

describ ed byPeskin and Printz PP who give further references Peskin and Printz

PP illustrate the immersedb oundary metho d by considering a twodimensional mo del

of the heart which includes a left atrium a left ventricle and a mitral valve The aortic

valve is mo delled as a sink The entire left heart is mo delled as though it were oating

in a uid The b oundary p oints are mo delled using a mechanical analogue consisting of

elastic plastic and contractile comp onents see McQueen Peskin and Yellin MPY

This mo del is clearly somewhat outofdate However it also has interesting features It

is used to mo del the entire cardiac cycle and is run until a p erio dic solution is obtained

There is an interesting discussion of these results and comparisons with exp eriments in

Sugawara Ka jiya Kitabatake and Matsuo SKKM p

Yoganathan Lemmon Kim Walk er Levine and Vesier YLK have used the immersed

b oundary metho d to mo del threedimensional early systolic motion Fluid velo cities in

the outow tract matched NMR data to within The aortic valvewas not simulated

physiologically The connection of the papillary muscles to the mitral valveby the chordae

tendinea was simulated

See the related work on immersed interface problems of Adams A multigrid algorithm

for immersed interfaceproblems Ada

The authors comment page on deciencies of the immersedb oundary metho d In

eect the cardiac tissue is mo delled as an innitely thin layer page Unfortunately

one of the consequences of a thinwalled left ventricle is its tendency to b ecome spherical

at a physiologic left ventricular pressure The other consequence is that a thinwalled

structure must pro duce much larger stresses than a thickwalled structure to supp ort

the same pressure Toovercome these deciencies it was articcially assumed that all

structural p oints representing muscle tissue were tethered to the ventricular centerline

See also the PhD thesis of Vesier Ves and Vesier and Yoganathan VY

Adams Ada presentsamultigrid algorithm for immersed interface problems See also

LeVeque and Li LL

EulerLagrangian Formulation

RecentlyPeskin and McQueen PMb haveintro duced a mixed EulerianLagrangian

formulation of the interaction of a viscous incompressible uid with an elastic and p os

sibly active material The elastic part of the system is treated using the Lagrangian

equations while the uid part is treated using the Eulerian equations The use of La

grangian equations for the elastic part is based on ideas of Ebin and Saxton ES ES

Peskin and McQueen PMb use this approach to mo del the threedimensional owof

blo o d in the heart The mo del heart contains the left and rightventriclesthe left and

right atriathe mitral tricuspid aortic and pulmonary v alvesand segmen ts of the aorta

main pulmonary artery sup erior and inferior vena cavae and the four pulmonary veins

The authors sp ecify a stressstrain law for the m uscle bres and assume that the elastic

energy density dep ends only on the strain in the bre direction To complete the mo del

the paths of the bres are sp ecied

Several computational results are shown graphically Coloured plates are shown in an

article byPeskin and McQueen PMa Tu and Peskin TP and Mayo and Peskin

MP discuss the stability merits of implicit versus explicit metho ds for computing the

elastic force density from the conguration of the elastic material

The results of Peskin and McQueen PMb are impressive Unfortunately the geometry

is only shown graphically so that the reader cannot repro duce the results

Taylor Okino and Yamaguchi TOY describ e the use of a commercial software package

SCRYU using a nite volume integration of the threedimensional NavierStokes equa

tions based on the SIMPLE algorithm with a b o dytted BFC co ordinate system The

time variation of the left ventricle wall was assumed as given

A spherical mo del was used but fully threedimensional computations are planned

That is the material can exert force as for example when muscle bres contract

Vortex and whirl ows

The ow of blood into the left ventricle during diastole is closely connected with the mo

tion of the mitral valve Blo o d entering the ventricle through the mitral valve is directed

towards the ap ex and maybelikened to a jet It is deected by the ap ex and takes on

the form of a vortex see Fig This vortexlike motion plays an imp ortant role in

the closure of the mitral valve see Section In the case of a dilated left ventricle a

whirl ow can b e observed see Figure

Figure Blo o d ow from Strackee and Westerhof The Physics of Heart and Circulation

Figure p SW

Figure Blo o d ow a

Figure Blo o d ow b

See the Bots PhD thesis Mathematical Models of Diastolic Blood Flow Patterns in the

Human Left Ventricle Bot and Verburg Bot Strackee and Delemaire VBSD

See also

Bellhouse Bel

Bellhouse and Bellhouse BB

Chapter

Mo delli ng the Heart Valves

Intro duction

The heart has four valves the tricuspid mitral pulmonary and aortic valves The tricus

pid and mitral valves are called atrioventricular valves b ecause they lie b etween the

atria and the ventricles The pulmonary and aortic valves are called arterioventricu

lar valves b ecause they lie b etween the arteries and the ventricles or alternatively the

semilunar valves b ecause their leaets have the shap e of a half mo on The op eration of

the heart valves has aroused considerable interest since the valves are aps of connective

tissue and are largely or wholly passive

The op eration of the heart valves has nearly always b een considered separately in the

literature The problem was considered by Leonardo da Vinci see Peskin Pesp

Henderson and Johnson HJ probably gave the rst correct explanation Fung Fun

pages describ es the op eration of the dierentvalves

Peskin has made several contributions to the sub ject He rst considered the topic in his

PhDthesis Pes There is a further discussion in his lecture notes Pes p

Numerical results were later published Pes

For a general discussion of the op eration of the valves see

Section of Fluid Mechanics of Large BloodVessels byPedley Ped

Section of Biodynamics Circulation byFung Fun

Swanson and Clark SC

The Mitral Valve

See

Bellhouse and Bellhouse BB

In German Taschenklapp en ie Pocket valves

Bellhouse Bel

The PhDthesis of Lee Lee

For measurements see

Sugawara Kagijiya Kitabatake and Matsuo SKKM

The Aortic Valve

The op eration of the mitral valvewas considered by Lee and Talb ot LT Some of their

results are repro duced byFung Fun page See also

Section of Fluid Mechanics of Large BloodVessels byPedley Ped

The Aortic Valve byThubrikar Thu

Section of Fluid Mechanics of Large BloodVessels byPedley Ped

Section of Biodynamics Circulation byFung Fun

The aortic valve consists of three leaets and three sinuses The leaets are the mobile

parts of the valve The sinuses are cavities b ehind the leaets on the aortic downstream

side of the valve Each leaet is p o cketshap ed When the ventricle is lling and the

pressure in the aorta is greater than in the ventricle the p o ckets billow out and together

tricle increases and exceeds that in the aorta close the valve When the pressure in the ven

the leaets are forced op en

There is a plausible explanation of why three leaets are used Consider a circular op ening

of radius r closed by n equal leaets The free edges of the leaets have the length r

while the length of the circumferential part of the leaet is rnIfn or then

the free edge is to o short to fold back If n the free edge is excessively long and will

crease If n the free edge can fold back easily without creasing It may b e noted in

this connection that the aortic valve do es not normally op en completely the area when

op en is approximately of the total area

Architecture of the Aortic Valve Leaets

Peskin and McQueen PMb consider the structure of the aortic valveIt is assumed

that the function of the closed valve is to supp ort a uniform pressure load p It is further



assumed that this load is transfered to the aortic wall by a oneparameter family of bres

under tension

Let u v b e co ordinates on the surface of the leaet chosen in sucha way that the curves

v constant are the bres with v b eing the free edge of the leaet The co ordinate

u measures arc length along the bres with u along the midline of the leaet The

leaet is given by

x Xu v

Let T u v b e the bre tension chosen in sucha waythat T u v dv is the force trans

mitted by the group of bres in the interv al v v dv Let p b e the uniform pressure



applied to the leaet

For the equilibrium of a patch of surface u u v v we obtain

 

Z Z

u v

X X X

T p dudv



u v

 

u u u v

It is p ossible to derive certain consequences from equation

The torsion T u v is indep endentofu so that the tension is constantoneach bre

v

X

with equation To see this form the scalar pro duct of

u



X X X X X X T X

T p



u u u u u u v

u

Since

X X

u u

wehave by dierentiation



X X



u

n

Also for general vectors a and b

aa b

We conclude that

T

n

The bres are geo desics on the valve leaet surface

This yields the equation of equilibrium

X X X

T p



u u u v

Equation can b e integrated numerically Because of a singularity at the centre of

the aortic valve the computed bre architecture has a fractal nature

The resulting computed architecture agrees well with the true architecture PPL fragen

Some questions on these results of Peskin and McQueen as of July

To what extent do the assumptions lead to the consequences that

The bre length is constant

The bres are geo desics

Supp ose wehave a cylinder with circular bres supp orting an internal pressure p



Are there transformations dierential geometric which transform this surface into

a leaet preserving the prop erties

What do the numerical results really mean

Do we really just have a problem with inextensible cords

For what classes of surfaces do es a family of geo desics have constant curvature

Articial Valves

Concerning ariticial valves see

Chapter und Chapter in Cardiovascular Biomechanics by Chandran Cha

The Aortic Valve byThubrikar Thu

Blood Flow in Articial Organs and Cardiovascular Prostheses by Barb enel Fisher

Gaylor et al BFG

Unsteady ow through prosthetic heart valves Anintegral approach coupled with a

vortex method In Boundary Elements X Vol Heat Transfer Fluid Flow and

Electrical Applications by Cassot Morvan and Tonietto CMT

Valve Vibration

Concerning valve vibration see

Chapter Analysis and Applications of Vibrations of An Introduction

to Mathematical Physiology ad Biology by Mazumdar Maz

Chapter

Mo delli ng other Ventricular

Pro cesses

The mechanical events in the heart are accompanied by electrical chemical and thermal

pro cesses In general it is assumed that the coupling is not very strong so that the

mechanical events can b e treated separately but it is necessary to b e aware of the other

pro cesses It maywell b e that in diseased hearts the eects of coupling are signicant

PPL fragen

Electrical and Electrophysiological Activity

The contraction of the heart is activated by electrical impulses These spread rapidly along

the endo cardium inner surface via the Purkinje bre network and more slowly towards

the epicardium outer surface via muscle cell conduction The propagation is complete

after ab out ms Hunter and Smaill HS pages describ e exp erimental re

sults and compare these to numerical mo dels

Sofaraswe are aware Novemb er the electrical activation has not b een mo delled

in conjunction with ventricular mechanics It seems reasonable to assume that the two

asp ects can b e considered separatelyItwould however p erhaps b e of interest to deter

mine whether it is of signicance that most of the endo cardium is activated rst in other

words that a pressure pulse moves outward This might for instance aect the blo o d

ow in the myo cardium One surprising fact is that a small part of the left ventricular

endo cardium is activated relatively late see Fung Fun p The plot of iso chronal

contours on the epicardium given by Hunter and Smaill HS Figure page also

shows interesting features PPL fragen

The energy for the contraction of heart muscle is provided bychemical reactions Potential

ed to the ow of ionic currents In turn a rise dierences across cell membranes are link

in calcium ion concentration with in a cell activates the contractile proteins in the cell

The electrophysiological activity of the heart is considered in several of the later chapters

in the collection Theory of Heart HSHY to whichwe refer

The underlying mathematical equations are related to the wellknown Ho dgkinHuxley

equations for conduction and exitation in nerves Much of the emphasis in the mo delling

is on phenomena suchas brillation which are distinct from ventricular mechanics The

equations are also the sub ject of active mathematical research See

Peskin Pes p

Peskin Pes

The intro ductory text of Grinro d Gri

Fife Fif

It has recently b een suggested by Lab and Holden LH that mechano electric feedback

may o ccur

See

Rogers and McCullo ch RM

Frese Fre

In the b o ok When Time Breaks Down The ThreeDimensional Dynamics of Electrochem

ical Waves and Cardiac Arrhythmias by Winfree Win there are interesting gures and

ideas with reference to cardiac arrhythmias or arrhythmias

See also

Glass and Mackey From Clocks to Chaos The Rhythms of Life GM

Cohen and Hirsch Mathematical developments in HodgkinHuxley theory and its

approximations CH

Murray Mathematical Biology Mur p

Winfree The Ge ometry of Biological Time Win

Kaplan Ph D Thesis Kap

Winfree Puzzles about excitable media and sudden death Win

Scott Oscil lations waves and chaos in chemical kinetics Sco

Oxygen Diusion

The heart needs a steady supply of oxygen without which misfunction o ccurs the extreme

example b eing a heart attack The demands placed on the coronary circulation system

are high and the uptakeofoxygen from the blo o d in the myo cardium is ab out three times

higher than in the rest of the b o dy Lev Figure and Section The owof

blo o d is inuenced by the pressure in the heart walls During isovolumetric contraction

the coronary blo o d ow ceases and even reverses see Levick Lev p At the time

of writing Novemb er we are not aware of mo delling in this area

Heat Flow

Hunter and Smaill HS pages describ e the mo delling of heat ow in the

heart

According to Ghista Ghi pages the heart pro duces heat at the rate of ab out

kcalday and so pro duces ab out of the b o dys heat

This gure seems doubtful since a human uses ab out kcalday see Guyton Guy

p Schmidt and Thews ST p and p SchmidtNielsen SN p CWC

January

One night exp ect the temp erature of the heart to inuence the hearts output since the

following are certainly temp erature dep endent

The blo o ds viscosity and hence the ow of blo o d in the myo cardium

The elasticity parameters of the myo cardium For instance collagen b ecomes pliant

when heated CWCgive reference According to Guyton Guy page

Chapter

Comparative Physiology of the

Heart

Intro duction

It is of interest to compare the p erformance of hearts in dierent sp ecies

Out of scientic curiosity

Since exp eriments on animals are used to obtain information ab out humans

Since a go o d mo del should b e able to predict the p erformance of the hearts of

dierent sp ecies

Nature oers a great range of circulatory systems and asso ciated pumps Two distinct

groups of animals the mammals and the birds have develop ed closed circulatory systems

with two separate pumps in one unit the heart It is reasonable to assume that this

arrangement has advantages and to try to nd them It is for instance not immediately

obvious whythetwo pumps should b e in the same unit For example Woods Woo

page suggested that it would follow from the Law of Laplace that it would b e

mechanically more ecienttohavetwo separate pumps

Sources of Data

The basis of any comparison of the hearts of dierent sp ecies must b e the systematic

accumulation of data

At the time of writing April weareaware of the following sources of information

Biology Data Book volume III by Altman and Dittmer AD

Comparative Physiology of the Heart by Clark Cla

Merck Veterinary Journal byFraser Fra

The Ecological Implications of Body Size byPeters Pet

Comparative Animal Physiology by Prosser Pro

Animal Physiology byScheer Sch

Scaling Why is Animal Size so Important bySchmidtNielsen SN

SchmidtNielsen SN page lists further references

Allometric Equations

Despite the great range of diversity in nature there are also considerable similarities For

example for the mammalian heart the following equation relates the mass of the heart

M in kilograms to the b o dy mass M in kilograms SN page

h b



M M

h

b

Equation is valid over the full range of mammals from shrews with a b o dy weightof

grams to elephants with a b o dy weight of kg Equation states that in general

the mass of the mammalian heart is approximately of the b o dy mass

Equation is an example of an equation of the form

b

y ax

or equivalently

log y loga b log x

with y M and x M

h b

Equations of the form frequently with x equal to the b o dy weight M are called

b

allometric equations in biology In the b o ok The Ecological Implications of Body Size

by RH Peters Pet a large numb er of allometric equations are given

For the study of the cardiovascular system the following allometric equations are of sp e

cial interest

If P denotes the metab olic rate for animals at rest in kcalday then the wellknown

met

mousetoelephantcurve is expressed by

 

P M

met

b

This was given by Max Kleib er in but similar equations had long b een known see

Cla Kleib er subsequently suggested that the equation

 

P M

met

b

would b e equally reasonable

The heartb eat frequency f b eats p er minute is given by K SchmidtNielsen SN

h

page

 

f M

h

b

The cardiac output Q ml p er minute is given by SchmidtNielsen SN page

h



Q M

h

b

Finally the blo o d volume V ml is given by SchmidtNielsen SN page

b



V M

b

b

so that the blo o d volume accounts for b etween and of the b o dy mass In the b o ok

Engineering Design of the Cardiovascular System of MammalsDawson Daw system

atically applies scaling laws

The foregoing allometric equations are intrinsically interesting but must b e treated with

some caution Clark Cla quotes many such formulas but often has dierentvalues for

the constants b Clark also gives several graphs which illustrate the not inconsiderable

scatter of the data

Dierences Between Mammalian Hearts

While there are farreaching similarities b etween all mammalian hearts there are also

dierences

Allometric equations represent trends and there are substantial deviations for some

animals For example the masked shrew which has a body weight of grams has

a heart which is times larger than is predicted by equation

There are some qualitative dierences whichmay b e masked by allometric equations

The structure of the myo cardium of the dog heart may b e dierent from that

of man Lunkenheimer p ersonal communication

There may b e qualitative dierences in the bre geometry b etween the mouse

heart and the human heart McLean Rross and Prothero MRP as quoted

byHorowitz Hor page

Pedley Ped page comments on a signicant dierence b etween the coronary

circulation in the horse and the dog

It has b een suggested see SchmidtNielsen SN page that the large size of

the shrew heart may arise b ecause there is a physical upp er limit to the frequency

of heart b eats As it is the shrew heart can b eat over times a minute that is

one b eat every milliseconds

SchmidtNielson SN page comments on a dierence b etween birds and mam

mals For reasons which are not clear some birds have blo o d pressures ab ove

mmHg

Rowell Row p emphasizes the fact that for uprighthumans of the blo o d

volume is b elow the heart level whereas for many animals of the blo o d volume

is at or ab ove heart level

During the Alicante conference dierences b etween human and pig hearts were

rep orted

Concluding Remarks

In summary it seems to one of us CWC at the time of writing April that with

the p ossible exception of very small hearts there are no signicant qualitative dierences

between mammalian hearts which could b e used to test dierent mathematical mo dels

of the heart

What conclusions can b e drawn which are relevant to the mo delling of the cardiovascular

system

Chapter

Mo delli ng the Global Motion of the

Heart

As mentioned in section the heart as a whole moves quite dramatically during a single

heart b eat This motion has apparently only b een considered by a few authors

Figure b illustrates the motion of the heart walls during systole the ap ex of the

heart moves towards the base the outer walls contract the septum b ecomes more convex

with resp ect to the left ventricle PPL fragen At the same time the ap ex moves forward

and taps against the chest see Figure

Until quite recentlyitwas not p ossible to accurately measure the motion of the heart

since one had to rely on visual observation in much the same way as William Harvey who

made some of his observations on dying animals whose heartb eat was reduced Harvey

Har chapter

Robinson Factor and Sonnenblick RFS p comment on its implications and refer to

the early technique of ballistic cardiography in which a sub ject lay on a wheeled table

while the motions of the table in resp onse to the motions of the heart were recorded

Related references are Son and YSF The lighthearted b o ok Vital Circuits by

Steven Vogel also contains a brief reference to this sub ject Vog page So far as we

are aware April quantitative estimates of the eect of the hearts motion on its

p erformance have not b een made

See also

Pedley Ped pages considers momentum

Bo oks on ballistic cardiography see Starr and No ordergraafNo ordergraaf No o

Acierno Aci pages

Rushmer Rus pages

Buchalter Weiss et al BWR measure the rotation of the left ventricular ap ex

using MRI tagging

Beyer and Sideman BSb app endix B consider the eect of twisting on bre extension

The Heart as a Mechanical Pump

Many authors have considered the heart as a mechanical pump

Burton Bur

Burch Ray and Cronvich BRC

Beyar and Sideman Spatial energy balance within a structural model of the left ven

tricle BS

Peters and Visscher The energy metabolism of the heart failure and the inuenceof

drugs upon it PV

Robinson Factor Sonneblick RFS

Wong Some proposals in cardiac muscle mechanics and energetics Won

Moskowitz Mos estimates inertial eects

The determinants of myo cardial oxygen consumption M V have b een considered by

O

many authors

Kahler Braunwald Kelminson Kedes Chidsey and Segal Eect of alterations of

coronary blood ow on the oxygen consumption of the nonworking heart KBK

The work W done by the heart is usually estimated as the sum of the mechnical work

external work or volumepressurework and the kinetic energy



W P V mv

where P is the pressure dierence mean ejection pressure minus mena l ling pressure

V is the mass of blo o d ejected and v is the mean ejection velo city of the blo o d see eg

Levick Lev p

For comparison with ordinary mechanical pumps see

Rogers and Mayhew Engineering Thermodynamics Work and Heat Transfer RM

Ryder and Bennett

Cardiac Energetics

Concerning cardiac energetics see

Gibbs Cardiac energetics Gib

Kleib er The Fire of Life Kle

Ryder and Bennett

Chapter

Growth

The human heart likemany other parts of the b o dy grows while maturing but also in

resp onse to changes in loading conditions It is a challenge to determine the mechanisms

which control this growth The study of the embryonic heart is relevantheregrowth

and remo delling

Wol s Law see

WolDas Gesetz der Transformation der Knochen

See

Thompson Tho

Lin and Tab er LT

Ro driguez Hoger and McCullo ch RHM

Yang Tab er and Clark YTC

Currey The Mechanical Adaptation of Bones Cur

Lin and Tab er LT mo del the growth of embryonic chickventricles They use the passive

strainenergy function

a

bQ

W e

b





Q I I



where

     

I

r z

     

I



r z

are strain invariants intro duced byYang Tab er and Clark YTC

The study of the growth adaptation remo delling and repair of living tissue raises inter

esting questions some of whichhave mathematical counterparts

In the present context one may ask whether knowledge ab out the stress distribution in

an overloaded heart can b e used to explain the developmentofhyp ertrophy see Fung

Fun page See

In Chapter of The Mechanical Adaptations of Bones Currey Cur critically

discusses p ossible mechanisms

The book On Growth and From by DArcy Thompson Tho is a classic in this

eld

Huxley Hux

Wol

Chapter

Miscellaneous Topics

Heart Sounds

Concerning heart sounds see

The Guide to Heart Sounds Normal and Abnormal NPS

Concerning Korotko sounds see

Pedley Ped pages and

The IntervalForce Relationship

Concerning the intervalforce relationship or forcefrequency relationship or force

interval relationship or intervalstrength relationship asso ciated with the name of

Bowditch See

Noble and Seed The IntervalForceRelationship of the Heart Bowditch Revisited

NSb

Wiggers Circulatory Dynamics Wig

Ciba Foundation The Physiological Basis of Starlings Law of the Heart Sym

Bowditch Ueber die Eigenthuemlichkeite n der Reizbarkeit welche die Muskelfasern

des Herzens zeigen Bow and Bowditch On the pecularities of excitability

which the bres of cardiac muscle show Translation of paper of Bow

Assistance and Replacement

See

Chapter Circulatory System Dynamics by No o dergraaf No o

Chapter and Chapter in Cardiovascular Biomechanics by Chandran Cha

Anrep Eect

Concerning the Anrep eect see

Ciba Foundation The Physiological Basis of Starlings Law of the Heart Sym

Gregg Eect

Concerning the Gregg eect see

Livingston Halp ering and Yin LHY

Gregg Gre

Part IV

Mathematical Mo delli ng of the

Circulatory System

Chapter

Intro duction

In this Part we attempt to provide an overview of the circulatory system other than the

heart As usual we emphasize the asso ciated mathematical problems

As Lighthill JL p comments

Many of the most imp ortant problems in this eld even if the uid dynamics

in them is considered in isolation are found to raise questions which in the

whole pro ceding history of research on uid dynamics have totally failed to

b e answered or in some cases even to b e asked

Some references include

Circulatory System Dynamics by No ordergraaf No o This is a readible and useful

description of the sub ject with problems and solutions at the end of eachchapter

One drawback is that the mathematics is often only briey describ ed

Cardiovascular Fluid Dynamics vols edited by Bergel Bera Berb

Blood Flow in the Heart and Large BloodVesselsby Sugawara Ka jiya Kitabataka

and Matsuo SKKM which describ es many exp erimental techniques and results

Circulation byFolkow and Neil FN

They also discuss the measurement of abnormal ows caused by defects such as

aortic regurgitation in which blo o d reenters the left ventricle from the aorta See

also Braunwald Bra p

shunts involving alternative paths for the circulation of blo o d See Braunwald

Bra p

stenosis the narrowing of a passage in the b o dy eg aortic stenosis See Braun

wald Bra p

Chapter

The Arterial System

The standard reference is McDonalds Blood Flow in Arteries the latest edition of which

is by Nichols and ORourke NO

Other references include

Part IV Wave Propagation and Arterial Dynamicsof Cardiovascular Dynamics

and Models by Brun et al BCL

The Fluid Mechanics of Large BloodVessels byPedley Ped

Chapter of Circulatory System Dynamics by No ordergraaf No o

Arterial System Dynamics by Li Li

Rubinow Rub

Chapter Analysis and Applications of Arterial Flow Dynamics of An Introduction

to Mathematical Physiology and Biology by Mazumdar Maz

Chapter and of Mathematical Biouiddynamics by Lighthill JL

Chapter of Biodynamics Circulation byFung Fun

Intro duction

The folw of blo o d through the arteries represents an interesting mathematical challenge

Blo o d is a complex nonNewtonian uid

The arterial walls are thick elastic containers

The arterial walls are often curved

The arteries branch rep eatedly

The ow is timedep endent

Since the pulsatile ow of the blo o d in the arteries is readily observed it aroused early

interest Early contributors included

Stephen Hales a clergyman who among other contributions rst measured arterial

pressure Hal

Thomas Young physicist and physician who rst calculated the wavevelo city for

thinwalled arteries You and You

Poiseuille physician and physicist who studied steadystate viscous ow

The brothers W Web er physicist and E H Web er physician WW and

Web

Womersley Wom and Witzig Wit

There are brief historical intro ductions in

McDonalds BloodFlowinArteries Nichols and ORourke NO pages

Biodynamics Circulation byFung Fun Chapter Fung also includes Table

pages a tabular summary of the contributions of dierent authors

Imp ortant results include the following

The Poiseuille ow of a viscous uid in laminar ow through a circular tub e of radius

a The velo city prole is

dp

 

u a r

dx

and the mean velo cityis



a dp

u

m

dx

Turbulentow in a circular tub e The transition to turbulence is governed by the

Reynolds number

UL

R

where U isatypical velo city L atypical length and the kinematic viscosity

For ow in tub es the ow b ecomes turbulentif R exceeds the critical value

RR

cr it

Surprisingly in the ascending and escending aorta of man and dog Reynolds numb ers

greater than can o ccur Fung Fun p

In Murray Mur used Poiseuilles formula to analyse the optimum design of blo o d

vessel bifurcation Murray found that if a blo o d vessel of radius a splits symmetrically



into twovessels of diameter a making angle with the original blo o d vessel then

a



a





cos





so that a a and These results known as Murrays formula are



roughly in agreement with measurements in the human b o dy

For owinathinwalled elastic tub e with Youngs mo dulus E of inner radius a and

i

wall thickness h the wave sp eed is found to b e Fung Fun p

s

Eh

c

a

i

This formula was derived byYoung in You but is called the Mo ensKorteweg

formula

More complicated ows were investigated by Witzig Wit and Womersley Wom

The Womersley number

r

D

play an imp ortant role

For numerical computations for ow in curved tub es eg the aorta see Chang and Tar

b ell CT

There are interesting clinical applications of the ab ove results McDonalds Blo o d Flow

in Arteries NO contains numerous examples

The ow of blo o d is inuenced by the stiening of arteries with age in man and

woman see NO p

It has b een p ostulated that turbulence increases the haemolysis loss of haemoglobin

of red blo o d cells see NO p

Chapter

The Pulmonary Circulation

Intro duction

The pulmonary circulation ist that part of the cardiovascular system in which blood

is pump ed from the rightventricle through the pulmonary artery to the lungs returning

through the pulmonary veins to the left artrium

See

Kowalczyk and Kleib er Model ling and numerical analysis of stresses and strains in

the human lung including tissuegas interaction KK

Berne and Levy BL pages

Pedley The Fluid Mechanics of Large BloodVessels Ped pages and

Nichols and ORourke in Chapter in McDonalds Blood Flow in Arteries NO

Levick An Introduction to Cardiovascular Physiology Lev

Handbook of Physiology Section Cardiovascular System vol Peripheral Cir

culation

Section Circulatory System Dynamics by No ordergraaf No o

Chapter IV Mathematical Aspects of Heart Physiology byPeskin Pes

The Respiratory Physiology of Animals by Cameron Cam

Chapter Mathematics in Medicine and the Life Sciences by Hopp ensteadt and

Peskin HP

Chapter Respiratory FlowPatterns of Mathematical Biouiddynamics by Lighthill

JL

Chapter

The Venous System

The venous system has b een studied comparatively little there is no equivalentof Mc

Donalds Blood Flow in the Arteries

References include

Chapter Flow in Col lapsible TubesofThe Fluid Mechanics of Large BloodVessels

byPedley Ped

Chapter The VeinsofBiodynamics Circulation byFung Fun

Chapter Circulatory System Dynamics by No ordergraaf No o

Amo ore and Santamore AS

Chapter

The Coronary Circulation

Some references on the coronary circulation are

Part I Myocardial Blood Flow of Cardiovascular Dynamics and Models by Brun et

al BCL

Fluid Mechanics of Large BloodVessels byPedley Ped contains scattered results

An interesting observation is that oscillations have b een observed in the coronary

artery of the horse which are not observed in a dog Ped page

Chapter of McDonalds Blood Flow in Arteries by Nichols and ORourke NO

Mechanics of the Coronary Circulation by Mates Nerem and Stein MNS

Fulton Ful

Microcirculation of the Heart Theoretical and Clinical Problems by Tillmanns

Kubler and Zeb e TKZ

A series of pap ers on the eects or coronary owwas

Kahler Braunwald Kelminson Kedes Chidsey and Segal Eect of alterations of

coronary blood ow on the oxygen consumption of the nonworking heart KBK

Ross Klo ck e Kaiser Braunwald Eect of alterations of coronary blood ow on the

oxygen consumption of the working heart RKKB

Sarno Gilmore Skinner Wallace Mitchell Relation between coronary blood ow

and myocardial oxygen consumption SGS

Weisb erg Katz and Boyd Inuenceofcoronary ow upon oxygen consumption and

cardiac performance WKB

In his PhD thesis Huyghe Huy gives a careful discussion of the inuence of myo car

dial mechanics on the coronary blo o d ow pages to and the inuence of the

coronary blo o d owonmyo cardial mechanics pages to

Huyghe Huy briey mentions the garden hose eect or erectile prop erties of

the coronary microvasculature and quotes Vogel Apstein Briggs Gaasch and Ahn

VAB

Chapter

The Micro circulatio n

See

Chapter Microcirculation in Biodynamics Circulation byFung Fun

Chapter Mathematical Biouiddynamics by Lighthill JL

Part V

Mathematical Mo delli ng of the

Entire Cardiovascular System

Chapter

Intro duction

The ultimate goal of mo delling the cardiovascular system is of course to mo del the entire

system as a whole This goal is far from b eing achieved

Some references are

Chapter of McDonalds Blood Flow in the Arteries NO

The conference pro ceedings edited by Yin Yin

The thesis of Waldman Wal

The b o ok of No ordergraaf Circulatory System Dynamics No o esp ecially Chapter

Control and Chapter The Closed Cardiovascular System

No ordergraaf No o quotes work in which mo dels containing hundreds of equations have

b een set up and solved by computer He makes the following comments No o page

The nature of the problems under scrutiny contains a temptation to write

massive systems of equations easily reaching into the hundreds Yet to date

mo dels of the entire circulation have neither answered the questions p osed

ab ove nor many of the other questions whichwere realistically the motivation

for developing the mo dels in the rst place

Chapter

Mo dels of the Cardiovascular

System

A few authors have considered the complete cardiovascular cycle by combining a mo del

of the heart with a simple mo del of the circulatory system load

See

Arts Veenstra and Reneman AVR

Arts Reneman and Veenstra ARV

Huyghe Huy

Chadwick Cha

In two pap ers Perl Horowitz and Sideman PHS and Horowitz Perl Sideman and

Ritman HPSR a complete canine cardiac cycle was mo delled using nite elements

The authors used threedimensional isoparametric elements The left ventricle was

treated as twolayers the ap ex elementshaving no des the reminder having no des

The bres were mo delled as truss elements The mo del allows for large deformations and

nonlinear constitutive equations However the active forces are treated as unknowns and

are chosen during each time step so that the exp erimentally observed ventricular volume

is obtained

An interesting feature of this work is that the authors attempt to assess the imp ortance

of four factors anisotropy geometric nonlinearity material nonlinearitymechanical ac

tivation They do so by dropping each one of these factors in turn and comparing the

results They conclude Horowitz Perl Sideman and Ritman HPSR p that all

factors play a role but the material nonlinearity is most signicant

Chapter

Control

See

Chapter Circulatory System Dynamics by No ordergraaf No o

Kapp el and Peer KP Based on the four compartment mo del of Gro dins Kapp el

and Peer develop a mo del for the resp onse of the cardiovascular to a short term

submaximal load Basic mechanisms included in the mo del are Starlings lawofthe

heart the Bowditch eect and autoregulation in the p eripheral regions The mo del

provides a description of data obtained in bicycle ergometer tests

Chapters and Cardiovascular Physiology by Berne and Levy BL

Human Circulation Regulation During Physical Stress byRowell Row

Human Cardiovascular Control byRowell Row Discusses circulatory adjustment

to upright p osture orthostasis and dynamic exercise Detailed but do es not treat

meathematical mo dels

Chapter VI Mathematical Aspects of Heart Physiology byPeskin Pes

Biomechanics and Exercise Physiology by Johnson Joh

Chapter

Design Principle s of the

Cardiovascular System

Almost everyone who studies the cardiovascular system comes to the conclusion that the

system must b e optimal See

Fung

Weib el The Pathway for Oxygen p discusses the question AreAnimals Built

Resonably Wei and intro duces the concept symmorphosis on p and

Weib el Wei Chapter reviews the respiratory system and particular the small

est mammal the Etruscan shrew see p

Talk in Alicante

Optimization of Biological Structures

There are several b o oks in which the optimal design of biological structure is considered

Gordon The New Science of Strong Materials or Why You Dont Fal l Through the

Floor Gor

Vogel Lifes Devices The Physical World of Animals and Plants Vog

Wainwright Biggs Currey and Gosline Mechanical Design in Organisms WBCG

Epilogue

In this text wehave attempted to survey the present state of mathematical mo delling of

cardiovascular mechanics

CWC Find a suitable quotation E g Weib el p

A great deal has b een achieved but many questions await denitive answers At the risk

of arousing criticism and demonstrating ignorance weventure to make some general and

p erhaps provo cative comments

In most numerical work in the literature the results are shown graphically and it is

very dicult for the reader to repro duce the results since neither the data nor the

programs are available A praiseworthy exception is provided byPeter Hunter and

his colleagues NLSH who have made their data available b oth on diskette and

by ftp

During the past few years muchwork has concentrated on mo delling the my

o cardium and the overall view has b een less emphasized Whereas Chadwick Cha

ventured to predict the pressurevolume cycle of the left ventricle recentworkers

have taken a muchnarrower view

There is little work whichcombines the computations of the stress in the heart walls

with computations of the blo o d owintheventricles

There seems to b e a need for greater interaction b etween physiological and morpho

logical observation and mathematical mo delling

The cardiovascular system is extremely complex At present most mo delling is

carried out by small groups PhD students etc Fullscale mo delling will require

co ordination of these eorts

We conclude with an optimistic quotation from Kovacs Kov p

It is extremly likely that in the years to come diagnosis therapy and followup

of cardiac patients will critically dep end on developments achieved through or

motivated by current mathematical and theoretical metho ds

App endix A

The SI System

A Physical Units

There is a b ewildering range of physical units Here we use with very few exceptions the

SI system

There are a numb er of b o oks which list conversion factors Wehave used Co ok Co o

The following intro duction to units is along the lines of that given bySchmidtNielsen

SN

See also

Goldman and Bell GB

Mechtly Mec

Symb ols Committee of the Royal So ciety otRS

Physical quantity SI base unit Symbol

length metre m

mass kilogram kg

time second s

thermo dynamic temp erature kelvin K

amount of substance mole mol

electric current amp ere A

luminous intensity candela cd

Table A Base units

This app endix provides names of units and their symb ols a brief list of conversion

factors and a list of some physical quantities and the recommended symb ols for their

designation

A Units

The SI system uses seven base units for seven dimensionally indep endent basic physical

quantitieseac h base unit is represented bya symbol Use of these symbols is mandatory

see table A The SI System recognizes several derived units as well as some supple

mentary units Although some of these have sp ecial symb ols they are derived from and

dened in terms of the base units A few of particular interest in physiology are listed in

Table A The following should b e noted ab out the use of these units and symb ols

Physical quantity SI derived unit Symb ol for unit Denition in

terms of base units



force newton N mkgs

 

energywork quantity of heat joule J Nm m kg s

 

power watt W JS m kg s

  

pressure pascal PaNm m kg s

   

viscosity p oise P Nsm m kg s

  

electric p otential dierence volt WA V m kg s A

  

electric resistance ohm VA m kg s A

electric charge coulomb C sA



frequency hertz Hz s

Table A Derived units

The symb ols are printed in roman upright letters The symb ols are not abbreva

tions and are not followed by a p erio d except at the end of a sentence

The plural form of a symb ol is unchanged and the ending s should not b e used

Certain units are derived from prop er names eg Voltthe sym b ols for these units

are capital roman upright letters V but the unit names are not capitalized volt

Prex Symbol Equivalent



tera T



giga G



mega M



kilo k



deci d



centi c



milli m



micro



nano n



pico p



femto f



atto a

Table A Prexes

There is frequent need for smaller and larger decimal multiples of the units These are

obtained by the use of the prexes listed in Table A These prexes may b e attached to

any SI base or derived unit Large multiples of seconds however are rarely expressed this

way The combination of prex and symb ol is regarded as a single symb ol and comp ound

prexes are not allowed The decimal sign is usually printed as a p oint in English but

as a comma in French and German In the SI system a p oint or comma should b e used

only for the decimal design To facilitate the reading of long numb ers the digits maybe

divided into groups of three but not separated by commas

Example not

When the decimal sign is placed b efore the rst digit of a numb er a zero should always

b e placed b efore the decimal sign

Example not

Pro ducts or quotients of two or more units are treated according to the rules of math

ematics Note that the use of more than one solidus is ambiguous Thus a sp ecic

  

rate of oxygen consumption can b e written ml k g sorml kg s or ml k g s or

 

ml kg s or ml kg s not ml k g s

A Useful conversion factors

Traditional units are commonly used in those elds of physiology that concern energy

eg in the area of metab olic rates and pressure eg in the area of gas exchange

Force

kgf kilogramforce N

newton kgf

Energywork force distance

cal J

joule cal

litre O at C mm Hg when used in oxidative metab olism is often equated



with kcalth us liter O kJ



Power work p er unit time

 

cal s J s W



kcal h W

  

watt cal s cal min cal h

Pressure force p er unit area

   

atm standard atmosphere N m kPa

 

at metric atmosphere kgf Nm kPkamm

 

Hg at C torr N m Pa

 

kNm mm Hg atm

Volume

  

litre is since dened as exactly equal to dm m th us ml cm



and l mm

Length



inch mm



foot m

Mass

poundavoirdup ois kg

ounce avoirdup ois kg

Temp erature

The temp erature unit of degree Celsius C equals the temp erature unit of

kelvin K

The Celsius temp erature is dened as the excess of the thermo dynamic temp erature

over K

A Physical Quantities

Physical quantities Symbol Dimensions

Length l L

Height h length

Radius r length



Area A L



Volume V L

Mass m M



Density mV ML

 

Pressure p ML T

Time t T



Velo city u v LT



Frequency f T



Force F MLT

Work W energy

 

Energy E W ML T

 

Power P ML T

Temp erature T

Table A Physical quantities recommended symb ols and dimensions Alternative sym

b ols are separated by commas

The names of some physical quantities and recommended symb ols are given in Table A

The symbolforaphysical quantity should b e a single letter of the Latin or Greek al

phab et and should b e printed in sloping italic typ e When necessary subscripts and

or sup erscripts are used to indicate a sp ecic meaning of a symb ol For example b o dy

temp erature T blood v olume V rate of o xygen consumption V

b bl O

Equations that representphysical or physiological relationships use these and similar

symb ols for physical quantities Symb ols for units m kg s etc should never b e used in

such equations

Also incorrectly known as centigrade

App endix B

Dimensional Analysis

B Dimensional Analysis

When a physical phenomenon is observed exp erimentally and the results are then repre

sented by an equation or law then the measurements must b e made in terms of physical

units such as metres or feet seconds or years but the particular physical units used are

clearly of secondary imp ortance and one may reasonably exp ect to b e able to express the

law in a form which is indep endent of the actual physical units used This can b e achieved

byintro ducing dimensionless variables and constants Dimensional analysis provides a

to ol to do this

Dimensional analysis brings additional b enets

In simple cases it is p ossible to deduce the general form whichanylawmust take

By ensuring that the dimensionless parameters are not changed one can scale a

problem without changing the form of the solution

As an example with biological applications the nature of the ow of a uid with velo city

u density and dynamic viscosity in a straight tub e of diameter d is determined by

the Reynolds number

ud

Re

For small values of Re the ow is laminar smo oth but if Re the ow can b ecome

turbulent

In animals one would exp ect that laminar ow in blood vessels would b e favoured by

natural selection but in fact the Reynolds numb er is often close to turbulentow

can o ccur YC Fung Fun p Fun p K SchmidtNielsen SN page

Dimensional analysis can b e systematized as follows

Determine all variables and parameters which o ccur in a problem

Determine a complete set of dimensionless pro ducts

Apply Buckinghams Theorem

Theorem An equation is dimensionally homogenous if and only if it can b e ex

pressed in the form F where f g is a complete set

 n  n

of dimensionless pro ducts

To illustrate the approach consider the pulsating ow of blo o d in an artery As determin

ing variables we take

r radius of artery L



f frequency T



density of blood ML

 

dynamic viscosity of blood ML T

To determine a complete set of dimensionles pro ducts we consider the pro duct

a b c d

r f

which has the dimensions

a b c c d d d

L T M L M L T

For this pro duct to b e dimensionless wemust have

acd L

bd T

cd M

from which it follows that

c d

b d

a c d d

Taking for convenience d we see that f g is a base with

s

f

r

is called the Womersley parameter

It is often denoted by

s

f

r

where is the kinematic viscosity

It follows from Buckinghams theorem that any solution must b e of the form

F

In his book Lifes Devices Vogel Vog page discusses several examples of scaling

when analysing biological problems

References on dimensional analysis include

Dimensional Analysis byP W Bridgman Bri

Dimensional Analysis in the Biomedical Sciences byBSchepartz Scha

Chapter in Eects of Scale in Muscles Reexes and Locomotion by Thomas A

McMahon McM

Chapter in AnIntroduction to Mathematical Physiology and Biology by J Mazum

dar Maz

Dimensional Analysis and Theory of Models by Langhaar Lan

Dimensional analysis is a sp ecial case of applications of the mathematical concept of

Lie Group to dierential equations Recent references to this sub ject include PJ Olver

Olv and GW Bluman and S Kumei BK

Some applications of dimensional analysis to biological problems are

In his PhD thesis Peskin Pes pages the ow patterns in the hearts of

dierent mammals are compared

Fung Fun page uses dimensional analysis to consider micro circulation in

the b o dy

Holmes Hol quoted by GW Bluman and S Kumei BK p uses dimen

sional analysis in the mo delling of soft tissue

Pritchard Pria Prib has p ointed out that most allometric equations violate

the rules of dimensional analysis He has suggested some new equations which con

form to dimensional analysis These might nd application in the mo delling of the

cardiovascular system

Lee Lee in Chapter discusses applications to hemo dynamics

Gunther Gue quoted byPeters Pet

In Chapter of Elastic Mechanisms in Animal Movement by Alexander Ale uses

dimensional analysis to discuss elastic similarity and dynamic similarity

App endix C

Elementary Concepts from Physical

Chemistry

See

Mo ore Physical Chemistry Mo o

Atkins Physical ChemistryAtk

Fenn Engines Energy and EntropyFen

Atkins Elements of Physical Chemistry Atk

Atkins Physical Chemistry th edition Atk

App endix D

Physiology

See

Guyton Textbook of Medical Physiolog Guy

Glaser Biophysik Gla

Schmidt and Thews Physiologie des Menschen Auage ST

Le Gros The Tissues of the Body WELGC

Duerr and Uehlinger unbek Sau

App endix E

Cardiovascular Data

E Man

We consider a normal young adult man weighing

W kg

The corresp onding normal heigth is

H cm m

If we assume a normal height of H m then according to the formula of DuBois

and DuBois DD he has a b o dy surface area of

    

S W H m

This formula is quoted by Dinnar Din but do es not app ear in Dub ois and Dub ois

DD See Kleib er Kle p

According to the formula of Carp enter he has a basal metab olic rate BMR of

BMR W H Age kcalh

for a man of age But Dinnar Din quotes kcalh as typical

See

Altman and Dittmer Biology Data Book vol III AD

Altman Dittmer and Greb e Handbook of Circulation ADG

Milnor Cardiovascular Physiology Mil

E Woman

E Dog

See Dinnar Din p

App endix F

Mathematical To ols

See

Mathematical Techniques for Biology and Medicine by Simon Sim

F Dierential geometry

Peskin see eg Peskin Pes has applied dierential geometry in several cases

See

Modern Dierential Geometry of Curves and Surfaces by Gray Gra

Tensor Analysis on Manifolds by Bishop and Goldb erg BG

Dierential Geometry of Curves and Surfaces by do Carmo dC

Riemannian Geometry by do Carmo dC

Dierential Forms with Applications to the Physical Sciences by Flanders Fla

Dierential Geometry by Kreyszig Kre

Dierential Geometry by Stoker Sto

Lectures on Classical Dierential Geometry by Struik Str

An Introduction to Dierential Topology Wil

Schweitzer Hurder dos Santos and Arraut Dierential Top ology Foliations and

Group Actions SHdSA

Eisenhart Introduction to Dierential Geometry with Use of the Tensor Calculus

Eis

Eisenhart Riemannian Geometry Eis

Abraham Marsden and Ratiu Manifolds Tensor Analysis and Applications RAR

Conlon Dierentiable Manifolds A First Course Con

Kosinski Dierential Manifolds Kos

Klingenb erg Riemannian Geometry Kli

F Geo desics

The concept of a geo desic has b een used in several areas

Fibres in the heart Peskin

Chapter Fibrewound animals in Elastic Mechanisms in Animal Movement by

Alexander Ale See also Alexander Ale

Horowitz Perl and Sideman HPS

F Geometric Measure Theory

Concerning geometric measure theory see

Geometric Measure Theory A Beginners Guide by Morgan Mor

F Top ology

The translation of Tamuras b o ok Tam contains a list of recent references on foliations

See

Abraham and Marsden Foundations of MechanicsAM

Armstrong Basic Topology Arm

Arnold Catastrophe Theory Arn

Arnold Singularity Theory Arn

H Blaine Lawson The Quantitative Theory of Foliations Law

Conlon Dier entiable Manifolds A First Course Con

Fuller The writhing number of a space curveFul

Fuller Decomposition of the linking number of a closedribbon A problem from

molecular biologyFul

Gordon Moriah and Wa jnryb Geometric Topology GMW

Hemp el Manifolds Hem

Lawson The Quantitative Theory of Foliations Law

Nash and Sen Topology and Geometry for Physicists NSa

Schwarz Topology for Physicists Sch

Tamura Topology of Foliations AnIntroduction Tam

Thurston and Weeks The mathematics of threedimensional manifolds TW

Weeks The ShapeofSpaceWee

F Knots

If we regard the bres in the heart wall as twisted then wemaywell ask whether they

form knots See

Adams The Knot Book Ada

Livingston Knot theory Liv

F Partial Dierential Equations

See

Renardy and Rogers RRb

F Singularities

See

Arnold Catastrophe Theory Arn

F Chaos

Some b o oks treating chaos include

Strogatz Singular laments organize chemical waves in three dimensions Wave

Taxonomy WS

App endix G

Mechanics

References on mechanics are

Chetaev Theoretical Mechanics Che

Goldstein Classical Mechanics Gol

Whittaker ATreatise on the Analytical Dynamics of Particles Rigid Bodies Whi

G Applied Mechanics

Under applied mechanics we understand elementary mechanis applied to practical en

gineering problems See

Hillier AppliedMechanics HH

Hibb eler Engineering Mechanics Statics and Dynamics Hib

Meriam and Kraige Engineering Mechanics Dynamics MK

Ryder and Bennet

G Thermo dynamics

Concerning thermo dynamics see

Rogers and Mayhew Engineering Thermodynamics Work and Heat Transfer RM

G Contiuum Mechanics

Standard classical references on continuum mechanics are

Truesdell and Noll The NonLinear Field Theories of Mechanics Handbuch der

Physik TN

Truesdell and Toupin The Classical Field Theories Handbuch der Physik vol III

TT

Truesdell The Elements of Rational Mechanics Tru

Mo delling using continuum mechanics is discussed by

Fung A First Course in Continuum Mechanics Fun

Allen Herrera and Pinder Numerical Modeling in Science and Engineering IHP

Bowen Introduction to Continuum Mechanics for Engineers Bow

Malvern Introduction to the Mechanics of a Continuous Medium Mal

Truesdell A First Course in Rational Continuum Mechanics Tru

Fung Foundations of Solid Mechanics Fun

Smith Constitutive Equations for Anisotropic and Isotropic Materials Smi

G Elasticity

References on elasticity include

Antman Nonlinear Problems of Elasticity Ant

Ciarlet Mathematical Elasticity vol I Cia The standard intro duction for math

ematicians

Ciarletta and Iesan Nonclassical Elastic Solids CI

Crandall Dahl and Lardner An Introduction to the Mechanics of Solids CDL

Gordon The New Science of Strong Materials or Why You Dont Fal l Through the

Floor Gor

Green and Adkins Large Elastic Deformations and NonLinear Continuum Mechan

ics GA

Green and Zerna Theoretical Elasticity GZ

Gurtin Topics in Finite Elasticity Gur

Love ATreatise on the Mathematical Theory of Elasticity Lov

Malvern Introduction to the Mechanics of a Continuous Medium Mal

Marsden and Hughes Mathematical Foundations of Elasticity MH

Maugin Material in homogeneities in Elasticity Mau

Sp encer Continuum Mechanics Sp e

Stoker Nonlinear Elasticity Sto

Timoshenko and Goodier Theory of Elasticity TG

ory of Anisotropic Elasticity and Applications Wu Ting and Barnett Modern The

WTB

G Fibrereinforced Materials

See

Mallick Fiberreinforced Composites Mal

Derek Hull AnIntroduction to Composite Materials Hul

Green and Adkins chapter VI I Reinforcementby Inextensible Cords Large Elastic

Deformations and NonLinear Continuum Mechanics GA

Christensen Mechanics of Composite Materials Chr

G Elastic Solids with Microstructure

See

Ciarletta and Iesan Nonclassical Elastic Solids CI

Kunin Elastic Media with MicrostructureIKun and Kunin Elastic Media with

MicrostructureIIKun

Capriz Continua with Microstructure Cap

Nowacki Theory of Asymmetric Elasticity Now

See also literature on p orous solids Hornung DH

App endix H

Biomechanics

H General References

See

Alexander Animal Mechanics Ale

Alexander Elastic Mechanisms in Animal Movement Ale

Alexander Mechanics of Animal Locomotion Alea

Biewener Biomechanics Structures and Systems A Practical Approach Bie

Currey The Mechanical Adaptation of Bones Cur

Fung A First Course in Continuum MechanicsFun

Flindt Biologie in Zahlen Fli

Gans Biomechanics An Approach to Vertebrate Biology Gan

Johnson Biomechanics and Exercise Physiology Joh

McMahon Muscles Reexes and Locomotion McM

Valenta BiomechanicsVal

Vincent Structural Biomaterials Vin

Vincent Biomechanics Materials A Practical Approach Vin

Vincent and Currey The Mechanical Properties of Biological Materials Symp Soc

Exp Biol VC

Vogel Steven Lifes Devices The Physical World of Animals and PlantsVog

Wainwright Axis and CircumferenceWai

Wainwright Biggs Currey and Gosline Mechanical Design in Organisms WBCG

H Biomaterials

See

Brown Structural Materials in Animals Bro

Fung Biomechanics Mechanical Properties of Living Tissues Fun

Silver Biological Materials Structure Mechanical Properties and Modeling of Soft

Tissues Sil

Vincent Structural Biomaterials Vin

Vincent Biomechanics Materials A Practical Approach Vin

Vogel Lifes Devices The Physical World of Animals and Plants Vog

Yamada Strength of Biological Materials Yam

H Mathematical Biology

See

Harrison Kinetic Theory of Living Pattern Hara

Levin Lectures on Mathematics in the Life Science Vol Some Mathematical

Questions in Biology Lev

Levin Frontiers in Mathematical Biology Lev

Mathematical Biology Mur Murray

Levin Frontiers in Mathematical Biology Lev

H Pattern Formation

Concerning pattern formation see

Harrison Kinetic Theory of Living Pattern Hara

Murray Mathematical Biology Mur

Concerning phyllotaxis see

Jean Phyl lotaxis A systemic study in plant morphogenesis Jea

Thompson On Growth and Form Tho

The phenomenon of phyllotaxis refers to the arrangement of leaf or oret primordia in

plants according to the Fib onacci sequence f g as seen in more than

of plants

H Bio energetics

See

Kleib er The FireofLifeKle

H Kinesiology

The science of the movement of the b o dy is called kinesiology See

Rasch

App endix I

Computer Graphics

Concerning computer graphics see

Foleyvan Dam Feiner and Hughes Computer Graphics Principles and Practice

FvDFH

Glassner Graphics GEMS Gla

Holden Reconstructing the heart Hol

Ho ehne DComputergrak in der Medizin Diagnose glasklar Ho e

ORourke Computational Geometry in C OR

WickhamJones MathematicaGraphics Techniques and Applications WJ

App endix J

Numerical Metho ds

Concerning numerical metho ds see

Adams MUDPACK Multigrid portable FORTRAN software for the ecient solu

tion of linear el liptic partial dierential equations Ada

Allen Herrera and Pinder Numerical Modeling in Science and Engineering IHP

Bank PLTMG A Software Package for Solving El liptic Partial Dierential Equa

tions Users Guide Ban

Brebbia and Dominguez Boundary Elements An Introductory Course nd edition

BD

Burkett Numerical methods for viscoelasticity Bur

Szab o and Babuska Finite Element Analysis SB

Smith and Criths Programming the Finite Element Method SGb

CriseldNonlinear Finite Element Analysis of Solids and Structures Crib

Zafrany El Techniques of the Boundary Element Method El

Kim and Karrila Microhydrodynamics KK

Hirsch Numerical Computation of Internal and External Flows Vol Computa

tional Methods for Inviscied and Viscous Flows Hir

Glowinski and Le TallecAugmentedLagrangian and OperatorSplitting Methods in

Nonlinear Mechanics GT

Grossmann and Ro os Numerik partiel ler Dierentialgleichungen GR

Langtangen and Nielsen Getting started with Dipack The Dipack Report Series

LN

J Finite Elements

Concerning nite elements see

Dhatt and Touzot The Finite Element Method Displayed DT

MacNeal Finite Elements Their Design and Performance Mac

Reddy AnIntroduction to the Finite Element Method Red

Schwarz Methode der niten Elemente Schb

Schwarz FORTRANProgramme zur Methode der niten Elemente Sch

Zienkiewicz and Taylor The Finite Element Method Vol Basic Formulation and

Linear Problems ZTa

Zienkiewicz and Taylor The Finite Element Method Vol Solid and Fluid Me

chanics Dynamics and NonLinearity ZTb

App endix K

Sources

K Sources of Preserved Hearts

The following information ab out suppliers of mo dels of hearts is taken from Vogel Vog

page

All of these vendors oer embalmed cow or calf sheep or lamb and pig hearts They

all have horribly exp ensive anatomical mo dels but Fisher and Wards have less costly

ones as well For nonfondlers NASCO has a reasonably priced sheep heart sliced op en

an emb edded in plastic and Wards has freeze dried whole and bisected as opp osed to

dissected sheep hears Addresses

Carolina Biological Supply Co

Burlington NC

NASCO

Janesville Ave Box

Ft Atkinson WI

Fisher Scientic Company

Educational Materials Division

W LeMoyne Street

Chicago IL

Wards Natural Science

Establishment

PO Box

Ro chester NY

A go o d source for inexp ensive mo dels but whose catalog maybedangeroustoyour

nancial security is

Edmund Scientic Co

E Glouchester Pike

Barrington NJ

K Bo oks Rep orts Theses

BMJ Bo okshop POBox London WCH TE England

Carries sto ck of medical b o oks

National Technical Information Service NTIS

Can provide copies of almost all ocial technical rep orts published in the USA

University Microlm UMI

Can provide copies of all PhD theses listed in the journal

K Journals

The following journals frequently contain information on the cardiovascular system

Cardiovascular Research

K So cieties

Cardiovascular System Dynamics So ciety

The so ciety holds a biannual conference the pro ceedings of which are published

Address

J Yasha Kresh PhD

Liko Cardiovascular Institute

Hahnemann University Ro om NCB

Broad Vine Streets Mail Stop

Philadelphia PA

Tel

Fax

email kreshcvihahnemannedu

Europ ean So ciety for Noninvasive Cardiovascular Dynamics

The Europ ean So ciety for Noninvasive Cardiovascular Dynamics ESNICVD was

initiated bythephysicist Prof AC Burger in the Netherland The main goal

tists and professionals whose of the ESNICVD is to unite and to keep together scien

common interest is to promote the knowledge and understanding of cardiovascular

dynamics with noninvasive metho ds in researchaswell as in medical practice The

congresses whichhave b een held all over Europ e for the past decades serve

to keep the scientists from this eld together despite the movementtowards ever

greater sp ecialization

DutchFoundation for Biophysics Verenigung vo or Biofysica This has a subsection

for the Heart and Circulation

Verenigung vo or Biofysika Kring Hart en Circulatie

British Heart Group

K Deutsche Literatur

Bauereisen Physiologie des Kreislaufs Bau

Bowditch Ueber die Eigenthuemlichkeite n der Reizbarkeit welche die Muskelfasern

des Herzens zeigen Bow

Braun Diagnose und Therapie der Herzkrankheiten Bra

Burton Physiologie und Biophysik des Kreislaufs Bur

Caisch Strukturgerechte Analyse der Myokardfaserspannungen Caf

Culclasure Anatomie und Physiologie des Menschen Lehrprogramme Band

Herz und Kreislaufsystem Cul

do Carmo Dierentialgeometrie von Kurven und Flaechen dC

Dierb erger FiniteElemente Simulat ion der Herzdynamik Das HerzgroessenSchlagvolumen

Konzept Die

Do err et al Pathologische Anatomie des Herzens und seiner Huel len I DSU

Faller Der Faserverlauf im Bindegewebe des Epikards menschlicher Herzen und

funktionel le Deutung Fal

Feneis Das Gefuege des Herzmuskels bei Systole und Diastole Fen

Flindt Biologie in Zahlen Fli

Frese Chaos Theorie und ploetzlicher Herztod Fre

Frank Zur Dynamik des Herzmuskels Fra

Glaser Biophysik Gla

Grossmann and Ro os Numerik partiel ler Dierentialgleichungen GR

Ho ehne DComputergrak in der Medizin Diagnose glasklar Ho e

Hort Untersuchungen ueber die Muskelfaserdehnung und das Gefuege des Myokards

in der rechten Herzkammerwand des Meerschweinchens Hor

Hort Untersuchungen zur funktionel len Morphologie des Bindegewebsgerue stes und

der Blutgefaesse der linken Herzkammerwand Hor

Horvath Physikalische Uebungsaufgaben fuer Biologen und Mediziner Hor

Krehl Beitraege zur Kenntniss der Fuel lung und Entleerung des Herzen Kre

Leonhardt Taschenatlas der Anatomie Band InnereOrgane Auage KLP

Lunkenheimer et al Kardiodynamik Wege zur strukturgerechten Analyse der Myokard

funktion LLG

Mattheck Design in der Natur Mat

Meesmann Nachweis der diastolischen Sogwirkung der Herzkammern und deren

Einuss auf die intrakardialen Druckablaeufe Mee

Meinzer Raeumliche Bilder des Koerperinneren Mei

Pu Der funktionel le Bau der Herzkammern Puf

Schmidt und Thews Physiologie des Menschen ST

Schwarz Methode der niten Elemente Schb

Schwarz FORTRANProgramme zur Methode der niten Elemente Sch

Thomas et al Grund lagen der klinischen Medizin Anatomie Physiologie Patholo

gie Mikrobiologie Klinik Band Herz und Gefaesse TGH

Tigerstedt Die Physiologie des Kreislaufes Tig

Torrent Guasp Lunk enheimer Intensivkurs Funktionel le Anatomie des Herzens

Vom bei Dr TorrentGuasp in Spanien Denia Alicante Gesprarchsnotizen

GL

Trost Analysis eines raeumlichen Model ls vom Herzmuskel Tro

Wol Das Gesetz der Transformation der Knochen

K DeutschEnglischVerzeichnis

K Diplomthemen

See

Adams A multigrid algorithm for immersed interfaceproblems Ada

Cameron The Respiratory Physiology of Animals Cam

Costa Hunter Rogers Guccione Waldman and McCullo ch A threedimensional

nite element method for large elastic deformations of ventricular myocardium Part

I Cylindrical and Sherical Polar Coordinate CHR

Costa Hunter Wayne Waldman Guccione and McCullo ch A threedimensional

nite element method for large elastic deformations of ventricular myocardium Part

II Prolate spheroidal coor dinates CHW

Harrison Kinetic Theory of Living Pattern Hara

Kowalczyk and Kleib er Model ling and numerical analysis of stresses and strains in

the human lung including tissuegas interaction KK

LeVeque and Li Immersed interface methods for Stokes ow with elastic boundaries

or surface tension LL

Lin and Tab er AModel for StressInducedGrowth in the Developing Heart LT

Moskowitz

Rogers and McCullo ch Acol locationGalerkin nite element model of cardiac action

potential propagation RM

Yang Tab er and Clark A Nonlinear Poroelastic Model for the Trabecular Embryonic

Heart YTC

App endix L

Worksheets

L Questions

This section contains various questions some of which are p oints to b e discussed with

PPL and some of which are p ossible research topics

Synchronisation of left and rightventricles

It is usually stated that the left and rightventricles work at the same time Is this

true If there is a small time dierence is there an explanation for this

Angular Momentum

The heart swivels during each b eat Is this caused by the angular momentum pro

duced by the outow of blo o d from the ventricles into the arteries

Global balance

Can one derive information from the global balance of forces See HSHY page

section and Mor

Law of Laplace

The inner wall of the left ventricle the septum is concave see Lev Levickg

c page Can the law of Laplace still apply See Mor

Peskins Formula

Peskin Comm P Appl Math page compares his theory with results of

Streeter et al Is this correct

Peskins crosssectional assumption

Peskin Comm P Appl Math page assumes that every bre tub e has

constant crosssectional area Correct

Inuence of the p ericardium The p ericardium restrains the heart What is its

role According to Fung Circulation p op ening of the p ericardium has an

imp ortant eect on the shap e and size of the heart He mentions also p the

dierence b etween surgery carried out with the p ericardium op en and closed

Heart oscillation PPL mentioned the measurement of heart b eats by placing pa

tients on a table

Flowintheventricle How is the ow in the left ventricle inuenced by the papil

lary muscles and by the clearly visible ridges on the inner surface the endo cardium

Stirlings law time dep endence In Stirlings exp eriments the pressure was

changed and the transitionary data were recorded see Lev p The system

is apparently damp ed Can one mo del this

Myo cardial activation In Hunter and Smaill p HS exp erimental and

numerical activation times are compared It would b e interesting to try to analyze

some of the features such as the closed contours in Figure

Heart deformation Are there any results in the literature which mo del the heart

deformation and blo o d pressure as functions of time assuming simple contraction

Systole expansion During diastole the ventrical wall recoils Lev p line

Why

Electrical activity Can the upwards movement of the heart b e explained by the

fact that the muscle is activated at slightly dierent times

Rightventricle and atrium These have not b een considered as extensivelyeven

though they handle the same amountofblood

Biots equations

Co ordination of veins and right atrium PPL fragen

T ectronic compartments of heart walls PPL fragen

The septum do es not distort but acts as though it were hinged

Wo o ds Role of t

Why

Do surface bres stay on surface

Where do cross bres come from go to

What are the trabi muscles

Are there bre lo ops

Do chordae tendae really do work

What ab out separate hearts

What ab out unrolling

What ab out ap ex

Magnetism

Magnets N S

rotating earth

Can one think up b etter constitutive equations for passivemyocardium What ab out

rational functions

Howdothechorae tendineae transmit the force to the tricuspid and mitral valves

Do the papillary muscles valves distend Are the chordae tendineae optimally

distributed

L Availability of Journals etc in Munster

Amer Heart J

Vol to date MED ZQ

Amer J Physiol

Split up into Series G H etc

MED ZD ie

Institut fr Physiologie

Rob ertKo chStr a

Annual Review of Physiology

MED

Anat Rec

MED ZD

Biophysical Journal

Vol to date Zo ologische Institute

Badestr MS

Vol to date UB ZD

Bull math Biology

ZD

Circulation

Vol ZQu

Vol date

Vol date

Vol

Circulation Research

Vol to date Med Klinik Innere Medizin AC

Alb ertSchweizerStr Munster ZC

Vol to date Institute Physiologie I I

Rob ertKo chStr Munster

Computer Programs in Biomedicine

Vol Continued as Computer Metho ds and Programs in

Biomedicine NotinM unster

CRC Crit Rev Biomed Eng

Chemical Rubb er Co Not available in Munster

Journal of Biomechanical Engineering

Not available in Munster

Journal of Biomechanics

Vol to date Institut fur

exp Biomechanik

Domagkstr Munster

J Fluid Mechanics

ZD

Journal of Thoracic Surgery

Klinik und Poliklinik fr

Thorax Herz Gefchirurgie

Alb ertSchweizerStr

Literatur Medizin

WG Kardiovaskulares System in der UB

Math Bioscience

Not in Munster

Progress in Biophysics and molecular biology

Vol to date Zo ologische Institute Badestr Munster

Scand J Thoracic and Cardiov Surg

either ZD all

or b

Scientic American

ZC

Virchows Archiv

Vol Vol UB ZD

Vol Vol GerhardDomagk

MED ZD

Institut fur Pathologie

Domagkstr MS

Z fuer Biologie

Vol Vol

Gegenbauers morph J

MED ZD

Journal of Physiology London

MED Z and UB

L Literature Searched

Bull Math Biology

ZD

Cardiovascular Research

Jan June

Circulation Research

JanJune

all

Must copy these pages

p

Dissertation Abstracts DA

No No No No

DA all

Index to Theses UK

Part Part Part

Am J Physiology

Am J Physiology

No Jan

NO Feb

No March

all

L PhD Theses

The following theses have not b een ordered as yet

Finite analytic numerical solution of laminar and turbulentowinatwodimensional

articial heart mo del

S H Kim Sang Hyun Kim

UniversityofIowa No p B DA

Advisor K B Chandran

The eects of right heart loading on left ventricular p erformance of in situ ejecting

hearts

EB Lankford

Johns Hopkins p No p B DA

Advisor not given

Hemo dynamics and wall shear rate measurements in the ab dominal aorta of dogs

K C White

Penn State No p B p DA

Advisor John M Tarb ell

Mo dels of cardiac muscle contraction and relaxation

J L Palladino

UniversityofPennsylvania No p B p DA

Advisor Abraham No ordergraaf

Reconstructing uid ow inside the heart from multiple xray image sequences

N H Cornelius

Carnegie Mellon No p B p DA

Advisor not given

Mathematical mo dels of comp onents of the cardiovascular system Arterial barore

ceptors and heart rate control

T F Itani Northwestern Nov No p B p DA

Advisor not given

Lo ok if theses by following are available

Costa Kevin D

Tab er Larry A

Burkett D A DA No

LeGrice Ian J A Finite Element Model of Myocardial Structur e Implications for

Electrical Activation in the Heart LeG

Rustum Choksi not in DAvol

L Corresp ondance

Prof Dr Charles Samuel Peskin

Professor Dr Charles Samuel Peskin

Courant Institute of Mathematical Sciences

New York University

email p eskincimsnyuedu

Prof Dr Peter J Hunter

Prof Dr Peter J Hunter

Department of Engineering Science

Scho ol of Engineering

University of Auckland

NewZealand

Tel

Fax

email hunteresvlaukuniacnz

Prof Dr Karl Heinz Hohne

Prof Dr Karl Heinz Hohne

Universitat Hamburg

Fachb ereich Medizin

Institut fur Mathematik und

Datenverarb eitung in der Medizin

Martinistr

Hamburg

Tel

Prof Dr Udupa

Prof Dr Jayaram K Udupa

UniversityofPennsylvania

Chief Section and

Asso ciate Professor

Medical Image Pro cessing Group

Department of Radiology

Blo ckley Hall Fourth Flo or

Service Drive

Philadelphia PA

email jayjaymipgup ennedu

Prof Dr Poul Michael Fnss Nielsen

Biomedical Engineering

Tel

Prof Dr Andrew D McCullo ch

Prof Dr Andrew D McCullo c h

Institute for Biomedical Engineering

Cardiac Mechanics Lab oratory

University of California San Diego

Gilman Drive

La Jolla California

Tel

FAX

email mccullo cheartucsdedu

Prof Dr Ruegsegger

Tel

FAX

Jennifer Rogers

email jarogersaucklandacnz

Professor William Kier

Department of Biology

The University of North Carolina at Chap el Hall

Coker Hill CB

Chap el Hill NC

Tel

Fax

Professor Abraham No ordergraaf

email ano orcardio dynseasup ennedu

App endix M

Biomathematics

General references on Biomathematics are

Winter On the Stem curve of a tal l palm in a strong wind Win

Biblio graphy

AB Rob ert H Anderson and Anton E Becker The orientation of bres within

the ventricular mass In Churchill Livingstone editor Cardiac anatomy

chapter Gowes Medical Publishing London Quoted by

Greenbaum Ho Gibson Becker and Anderson Get

AB Rob ert H Anderson and Anton E Becker The Heart StructureinHealth

and DiseaseGower Medical Publishing London ISBN

Have OK Also have set of slides

Aci Louis J Acierno The History of Cardiology Parthenon Publishers Cast

erton Hall Carnforth Lancs Ordered Blackwells for cwc

Have OK ISBN

AD Philip L Altman and Dorothy S Dittmer editors Biology Data Book

volume I I I Federation of American So cieties for Exp erimental Biol

ogy Bethesda Maryland second edition In Zo ologie Not in BIP

No chmal anschauen

Ada J C Adams MUDPACK Multigrid p ortable FORTRAN software for the

ecient solution of linear elliptic partial dierential equations Appl Math

Comput Get

Ada Loyce Adams Amultigrid algorithm for immersed interface problems

T echnical rep ort Dept of Applied Mathematics UniversityofWashington

Havecwc OK

Ada Colin Conrad Adams The Knot BookWHFreeman New York

ISBN X Havecwc

Ada Adam editor Physikalische Chemie und Biophysik SpringerVerlag

From Springer Catalog Lo ok at

ADG Philip L Altman Dorothy S Dittmer and Rudolph M Greb e Handbook

of Circulation WB Saunders Philadelphia In PHYSIOLOGIE I

Not in BIP No chmal anschauen

Ale Rob ert McNeill Alexander Animal MechanicsBlackwell Scientic Publi

cations Oxford nd edition Quoted in A A Biewener Biomechanics

Structures and Systems A Practical Approach Get In BIP

Not in MED In Whitaker X Ordered Kruep er

Vergrien laut Kruep er vom Vergrien lt Blackwells

Ordered Order UB

Ale Rob ert McNeill Alexander Bending of cylindrical animals with helical

bres in their skin or cuticle Journal of theoretical Biology

Quoted by R McNeill Alexander p Get

Ale Rob ert McNeill Alexander Elastic Mechanisms in Animal Movement

Cambridge University Press Cambridge p Quoted bySchmidt

Nielson Animal Physiology Adaptation and Environment page

Not in MED ISBN HaveOK

Alea Rob ert McNeill Alexander editor Comparative and Environmental Phys

iology Mechanics of Animal Locomotion SpringerVerlag ISBN

Have OK

Aleb Rob ert McNeill Alexander The Human Machine Natural History Museum

Publications Have ISBN Havecwc

Ale Rob ert McNeill Alexander Bones The Unity of Form and Function

Macmillan ISBN In BP LC Ordered

Kruep er

AM Ralph Abraham and Jerrold E Marsden Foundations of Mechanics Ben

jaminCummings nd edition In Math Bibl

AM Roy M Anderson and Rob ert M May Infectious Diseases of Humans

Oxford University Press Have O K

Ant James Francis Antaki An Experimental and Theor etical Model for the Pas

sive Biomechanical Properties of the Intact Heart Volumes I and II PhD

thesis University of Pittsburgh Have UMI No cheinmal

grundlic h lesen Hat mehrere interessante Zitate

Ant Stuart S Antman Nonlinear Problems of Elasticity SpringerVerlag

Have ISBN

AR Theo Arts and Rob ert S Reneman The imp ortance of geometry of the

heart to the pump In Henk E D J ter Keurs and Mark I M Noble

editors Starlings Law of the Heart Revisited pages Kluwer

Academic Publishers Have

Arm M A Armstrong Basic Topology SpringerVerlag Go o d Intro duc

tion Get In Math Lib

Arm A Armenti Jr editor Physics of Sports AIP Get AMR ISBN

Order for cwc privat Ordered Kruep er

Arn V I Arnold Catastrophe Theory SpringerVerlag ISBN

Get

Arn V I Arnold Singularity Theory Cambridge University Press Cambridge

Collection of pap ers including some generating concept of index to

manifolds with b oundary Get

Art Theo Arts A Mathematical Model of the Dynamics of the Left Ventricle and

the Coronary Circulation PhD thesis University of Limburg Maastricht

The Netherlands Ordered UB Wrote Jan to Theo Arts

NL Ordered UB No ch nichts erhalten UB

ARV Theo Arts Rob ert S Reneman and Pieter C Veenstra A mo del of the

mechanics of the left ventricle Annals of Biomedical Engineering

Have

AS John N Amo ore and William P Santamore Venous collapse and the res

piratory variability in systemic venous return Cardiovascular Research

Have OK

Ask Michael J Askew Advances in Bioengineering American So ciety of Me

chanical Engineers New York Have ISBN

Ata Fatihcan M Atay A dierentialdelay equation arising in the model ling of

the pupil light reex PhD thesis Brown University Rho de Island

Get

Atk Peter William Atkins Elements of Physical Chemistry Oxford University

Press Oxford ISBN X Have

Atk Peter William Atkins Physical Chemistry th edition Oxford University

Press Oxford Have ISBN

Atl SatyaNAtluri Alternate stress and conjugate strain measures and mixed

variational formulations involving rigid rotations for computational anal

yses of nitely deformed solids with applications to plates and shells I

Theory Computers and Structures Quoted byYang

Tab er and Clark Have OK

AVR Theo Arts Pieter C Veenstra and Rob ert S Reneman Epicardial defor

mation and left ventricular wall mechanics during ejection in the dog Amer

ican Journal on Physiology Heart and Circulatory Physiology H

H Have OK

AY Loyce Adams and Z Yang editors Acomparison of techniques for solving

il lconditionedproblems arising from the immersedboundary method Pro

ceedings of Symp osia in Applied Mathematics Vancouver CA Aug

Get Quoted byLoyce Adams

Baa Jan Baan editor Ventricular Function and PressureVolume Analysis

the Role of Conductance in Car diology Pro ceedings Conference in Nuern

b erg August Europ ean Heart J vol Suppl E Academic

Press London Not in BIP In MED Lesesaal MED ZD No chmal

anschauen

BAH Peter Hermanus Marie Bovendeerd Theo Arts Jacques Maria R J

Huyghe DickHvan Camp en and Rob ert S Reneman Dep endence of lo

cal left ventricular wall mechanics on myo cardial b er orientation A mo del

study Journ Biomech Have

Ban Randolph E Bank PLTMG A Software Package for Solving El liptic Par

tial Dierential Equations Users Guide So ciety for Industrial and

Applied Mathematics Philadelphia Have ISBN

Bau E Bauereisen Physiologie des Kreislaufs Band und SpringerVerlag

Berlin In PHYSIOLOGIE I Not in print

BAY Jan Baan Alexander C Arntzenius and Edward L Yellin editors Car

diac Dynamics Proc rd International Conference Cardiovascular System

Dynamic Society Kluwer Academic Press Dordrecht p

ISBN Have OK

BB B J Bellhouse and F H Bellhouse Fluid mechanics of a mo del mitral

valve and left ventricle Circulation Research In MED

ZC Checkvol year

BB R D Bauer and R Busse The Arterial System Dynamics Control Theory

and Regulation SpringerVerlag New York Get Not in BIP Ordered

UB Zurueck Vorh in MS UB G o der G

BCL Philipp e Brun Richard S Chadwick and Bernard I Levy editors Cardio

vascular Dynamics and Models Proceedings of NIHINSERM workshops

Bethesda September Paris volume of Col loques INSERM

Les Editions INSERM Paris Have ISBN

BD C A Brebbia and J Dominguez Boundary Elements An Introductory

Course nd edition Computational Mechanics Publications and McGraw

Hill Bo ok Company Have

BE D Bluestein and S Einav Transition to turbulence in pulsatile ow

through heart valves a mo died stability approach Transactions of the

ASME Journal of Biomechanical Engineering Have

Bel B J Bellhouse The uid mechanics of heart valves In D H Bergel

editor Cardiovascular Fluid Dynamicsvolume pages Academic

Publishers New York Have

Ben Jan E W Beneken Some computer mo dels in cardiovascular research

In D H Bergel editor Cardiovascular Fluid Dynamicsvolume pages

Academic Publishers New York Have

Bera D H Bergel editor Cardiovascular Fluid Dynamicsvolume Aca

demic Press New York ISBN Ordered Kruep er

Rep orted out of Print Dillons Not available Have Xerox

copy

Berb D H Bergel editor Cardiovascular Fluid Dynamicsvolume Academic

Press New York Have Xerox copy ISBN

Ber Rob ert M Berne editor Handbook of Physiology Section The Car

diovascular System Vol I The Heart American Physiological So ciety

Bethesda distributed by Oxford University Press Oxford Have

OK ISBN Not in MED In PHYSIOLOGIE I I Weitere

Baende Galloway

BFG J C Barb enel A C Fisher J D S Gaylor W J Angerson and C D

Sheldon editors Blood Flow in Articial Organs and Cardiovascular Pros

thesesvolume of OxfordMedical Engineering Series Clarendon Press

Oxford p ISBN Have Xeroxcopy OK

BG Richard L Bishop and Samuel I Goldb erg Tensor Analysis on Manifolds

Dover Have O K

BHA Peter Hermanus Marie Bovendeerd Jacques Maria R J Huyghe Theo

Arts DickHvan Camp en and Rob ert S Reneman Inuence of

endo cardialepicardial crossover of muscle b ers on left ventricular wall

mechanics Journ Biomech Have

Bie A A Biewener editor Biomechanics Structures and Systems A Practical

Approach Oxford University Press Have ISBN

Bio M A Biot unb ek J Anat Physiol Get Medizin ZD

MED

Bio M A Biot Theory of nite deformations of p orous solids Indiana Univ

Math J Have OK

Bio M A Biot Ho dograph metho d of nonlinear stress analysis of thickwalled

cylinders and spheres including p orous materials Int J Solids Structures

Quoted byAntman p Get Order UB

BK Paul J Blatz and William L Ko Application of nite elasticity to the

deformation of rubb ery materials Transactions of the Society of Rheology

Quoted byYang Tab er and Clark Have OK

BK George W Bluman and Sukeyuki Kumei Symmetries and Dierential

Equations SpringerVerlag New York Have

BKDA M B Bennet R F Ker N J Dimery and Rob ert McNeill Alexander

Mechanical prop erties of various mammalian tendons J of ZoologyA

Get UB ZD

BL Rob ert M Berne and Matthew Levy Cardiovascular Physiology Mosby

Year Bo ok St Louis sixth edition Have OK

Bli Blix Get Volume I I I p Volume IV p

Bli Blix Get Volume V pp and Volume VI p

BN L F Bishop and J Neilson Jr editors History of Cardiology Medical

Life Press New York Ordered UB Get Not in BIP Not in MED

Not available in Germany

BNR Jan Baan A No ordergraaf and J Raines editors Cardiovascular System

usetts Institute of Technology Cambridge Dynamics MIT Press Massach

Have OK

Boga Daniel K Bogen Strain energy descriptions of biological swelling I Single

uid compartment mo dels Transactions of the ASME Journal of Biome

chanical Engineering Have UB OK

Bogb Daniel K Bogen Strain energy descriptions of biological swelling I I Mul

tiple uid compartment mo dels Transactions of the ASME Journal of

Biomechanical Engineering Have UB OK

Bol L Bolis editor Comparative physiology Locomotion respiration transport

and blood Proc Intern Congress Aquasparta Elsevier Out

of Print Kruep er Get ISBN Not in MED Not in

UB Dillons Not available Order UB

Bor Giovanni Alfonso Borelli On the Movement of Animals Translated

by P Maquet SpringerVerlag New York Quoted byFung A rst

course in continuum mechanics pages and ISBN

Have OK

Bos Amitabha K Bose Existence and stability of travel ling waves for couples

nerve axon equations PhD thesis Brown University Rho de Island

Get

Bot Hans Bot Mathematical Mo dels of Diastolic Blood Flow Patterns in the

Human Left Ventricle PhD thesis University of Amsterdam Have

current address Have

Bou Y Bouligand Twisted brous arrangements in biological materials and

cholesteric mesophases Tissue and Cel l Quoted by Win

free Get ZOOLOG

Bov Peter Hermanus Marie Bovendeerd The Mechanics of the Normal and

Ischemic Left Ventricle During the Cardiac Cycle A Numerical and Ex

perimental Analysis PhD thesis Rijksuniversiteit Limburg te Maastricht

Have

Bow H PBowditch Ueb er die Eigenthuemlichkeiten der Reizbarkeit welche

die Muskelfasern des Herzens zeigen Abhand lungen der mathematisch

physischen Classe der Koeniglich Saechsischen Gesel lschaft der Wis

senschaften Leipzig Have

Bow RayMBowen Theory of mixtures In Ahmed Cemal Eringen editor

Continuum Physicsvolume pages Academic Press Get

UB G Lesesaal

Bow RayMBow en Incompressible p orous media mo dels by use of the theory

of mixtures Int J Enging Sci Have UB OK

Bow RayMBowen Introduction to Continuum Mechanics for Engineers

Plenum Press Have OK ISBN

Bow H PBowditch On the p ecularities of excitability which the bres of

cardiac muscle show translation of pap er of In Mark I M No

ble and W A Seed editors The IntervalForceRelationship of the Heart

Bowditch Revisited pages Cambridge University Press Cambridge

Have

Bra Ludwig Braun Diagnose und Therapie der Herzkrankheiten Urban und

Schwarzenb erg Berlin nd edition Havecwc

Bra A J BradyPassive elastic prop erties of cardiac myo cytes relative to in

tact cardiac tissues In T F Robinson and R K H Kinne editors Car

diac MyocyteConnective Tissue Interactions in Health and Disease Issues

Biomedvolume Karger Basel Have OK

Bra Eugene Braunwald editor Heart Disease WB Saunders Philadelphia

th edition Available as or vols ISBN A

standard reference for clinicians Excellentvalue for moneyHave OK

BRC G E Burch C T Ray and J A Cronvich Certain mechanical p eculiari

ties of the human cardiac pump in normal and diseased states Circulation

Hav e OK

Bre C A Brebbia editor Boundary Elements X Vol Heat transfer uid

ow and electrical applications Computational Mechanics Publications and

SpringerVerlag Have

Bri Percy Williams Bridgman Dimensional AnalysisYale Press New Haven

revised edition Have Xerox copy

Bro C H Brown Structural Materials in Animals Pitman Publishing

Havecwc OK ISBN

BRS Eugene Braunwald John Ross Jr and Edmund H Sonnenblick Mecha

nisms of Contraction of the Normal and Failing Heart Little Brown and

Company Boston second edition Quoted by Braunwald in Hand

book of physiology The heart page Have Xeroxcopy Excellent and

detailed OK

Bru Brutsaert See Sagawa b o ok for other pap ers Get

BS J R Bo oker and J C Small An investigation of the stabilityofnumeri

cal solution of Biots equations of consolidation Int J Solids Structures

Quoted by Huyghe Order UB Get

BS C Gunnar Blomqvist and Bengt Saltin Cardiovascular adaptations to

physical training Annual R ev Physiology Quoted by

Rowell p Have

BSa Rafael Beyar and Samuel Sideman A computer study of the left ventricular

p erformance based on the b er structure sarcomere dynamics and trans

mural electrical propagation velo city Circulation Research

Have OK

BSb Rafael Beyar and Samuel Sideman A mo del for left ventricular contraction

combining the force length velo city relationship with the time varying elas

tance theory Biophys Journ Get Quoted by BSa ZOOLOG

UB ZD

BS Rafael Beyar and Samuel Sideman Spatial energy balance within a struc

tural mo del of the left ventricle Annals of Biomedical Engineering

Have OK

BS O O Blumenfeld and S Seifter Bio chemistry of connective tissue with sp e

cial emphasis on the heart In T F Robinson and R K H Kinne editors

Cardiac MyocyteConnective Tissue Interactions in Health and Disease Is

sues Biomedvolume Karger Basel Have OK

BS Susanne C Brenner and L Ridgway Scott The Mathematical Theory of

Finite Element Methods SpringerVerlag Have ISBN

BT T K Borg and L Terracio Interaction of the extracellular matrix with

cardia myo cytes during development and disease In T F Robinson and

R K H Kinne editors Cardiac MyocyteConnective Tissue Interactions

in Health and Disease Issues Biomedvolume Karger Basel

Have OK

Bur Alan C Burton The imp ortance of the shap e and size of the heart Amer

ican Heart Journal Have OK

Bur Alan C Burton Physiologie und Biophysik des Kreislaufs Schattauer

Verlag Stuttgart In PHYSIOLOGIE

Bur Alan C Burton Physiology and Biophysics of the Circulation An Intro

ductory Text Bo oks on Demand nd edition Year Bo ok Medical

Publishers Chicago Available from LC ISBN

pap er Have OK

Bur Daniel Andrew Burkett Numerical methods for viscoelasticity PhD thesis

Carnegie Mellon UniversityPennsylvania Get DA B Order

UMI

BWR Maurice B Buchalter James L Weiss Walter J Rogers Elias A Zer

houni Myron L Weisfeld Rafael Beyar and Edward P Shapiro Non

invasivequantication of left ventricular rotational deformation in normal

humans using magnetic resonance imaging myo cardial tagging Circulation

Have OK

Caf Amadeo Caisch Strukturgerechte Analyse der Myokardfaserspannungen

Have Seite fehlt OK

Cam James N Cameron The Respiratory Physiology of Animals Oxford Uni

versity Press Have ISBN OK

Cap G Capriz Continua with microstructure In C Truesdell editor Springer

Tracts in Natural Philosophy SpringerVerlag New York Get

Quoted by Ciarletta and Iesan Nonclassical Elastic Solids Pitman Re

search Notes in Mathematics UB b estellen

Car Gail A Carp enter editor Lectures on Mathematics in the Life Science Vol

Some Mathematical Questions in Biology Circadian Rhythms Ameri

can Mathematical So ciety Providence Have

CB James B Cauleld and T K Borg The collagen network of the heart

Laboratory Investigation Have OK

CC R B Clark and J B CoweyFactors controlling the change of shap e of

certain nemertean and turb ellarian worms Journal of experimental Biology

Quoted by R McNeill Alexander p Get ZQu

UB XEROX

CC GillJeong Cheon and K B Chandran Transientbehavior analysis of a

mechanical monoleaet heart valve prosthesis in the closing phase Trans

actions of the ASME Journal of Biomechanical Engineering

Have

CCMH H J Chiel P Crago J M Mansour and K Hathi Biomechanismsofa

muscular hydrostat a mo del of lapping by a reptilian tongue Biological

Cybernetics Quoted by Johnson and Keir ZC

ZS ALL Get UB XEROX

CCPC P S Chen Y M Cha B B Peters and L S Chen Eects of my

o cardial b er orientation on the electrical induction of v entricular brilla

tion American Journal on Physiology Heart and Circulatory Physiology

HH Get Have Medline abstract

CDL Stephen H Crandall Norman C Dahl and Thomas J Lardner editors

An Introduction to the Mechanics of Solids McGrawHill Have O

K ISBN

CF C J Chuong and Yuancheng Fung Three dimensional stress distribution

in arteries Transactions of the ASME Journal of Biomechanical Engi

neering Quoted by JH Omens p Have

OK

CF C J Chung and Yuancheng Fung Residual stress in arteries In GW

SchmidtScho enb ein SL Wo o and BW Zweifach editors Frontiers in

Biomechanics SpringerVerlag New York Have Check

CH Cohen and Hirsch Mathematical developments in Ho dgkinHuxley theory

and its approximations In Simon A Levin editor Some Mathematical

Questions in Biologyvolume pages American Mathematical So

ciety Providence Have

Cha Richard S Chadwick The myo cardium as a uidb er continuum passive

equilibrium congurations Advances in Bioengineering pages

Have OK

Cha Richard S Chadwick Mechanics of the left ventricle Journ Biomech

Have OK

Cha Eric L Charnov Life history invariants Get ISBN X

Order Kruep er

Cha K B Chandran Cardiovascular BiomechanicsNewYork University Press

New York Ordered Heers ISBN Have

OK Text for use in course Emphasizes blo o d ow but also discusses imag

ing myo cardial mechanics and assist devices Tends to summarize results

and refer to literature Has some exercises no solutions

Che Nikolai G Chetaev Theoretical Mechanics SpringerVerlag Have

O K

Chh R P Chhabra Bubbles Drops and Particles in NonNewtonian Flu

idsCRC Press Get ISBN Ordered Kruep er

Cho Rustum Choksi Two topics on the equations of solid mechanics The in

compressible limit in nonlinear elasticity and conservation laws in bre

reinforced materials PhD thesis Brown University Rho de Island

Get Not in DAVol Order UMI

Chr Richard M Christensen Mechanics of Composite Materials Krieger Mal

abar Have OK ISBN

CHR Kevin D Costa Peter J Hunter Jack M Rogers Julius M Guccione Jr

Lewis K Waldman and Andrew M McCullo ch A threedimensional nite

element metho d for large elastic deformations of v entricular myo cardium

Part I Cylindrical and spherical p olar co ordinates Transactions of the

ASME Journal of Biomechanical Engineering Have

CHW Kevin D Costa Peter J Hunter Jennifer S Wayne Lewis K Waldman

Julius M Guccione Jr and Andrew M McCullo ch A threedimensional

nite element metho d for large elastic deformations of ventricular my

o cardium Part I I Prolate spheroidal co ordinates Transactions of the

ASME Journal of Biomechanical Engineering Have preprint

CI M Ciarletta and D Iesan Nonclassical Elastic Solidsvolume of

Pitman Research Notes in Mathematics Longman Scientic Technical

Have ISBN X

Cia Philipp e G Ciarlet Mathematical Elasticity Vol I ThreeDimensional

Elasticity NorthHolland Amsterdam Havecwc OK ISBN

X

Cia Philipp e G Ciarlet Mathematical Elasticity Vol II Lower Dimensional

Theories of Plates and Rods NorthHolland Amsterdam Ordered

Cia Philipp e G Ciarlet Mathematical Shel l Theory Wiley Get OK

ISBN Ordered Kruep er Publication Dec

CKK John A Callahan Thomas E Keys and JackDKey editors Classics

of Cardiology former title Cardiac Classicsvolume Krieger

Have ISBN

CKT Kenneth B Campb ell Rob ert D Kirkpatrick Anthony H Tobias

Hesameddin Taheri and Sanjeev G Shro Series coupled noncontractile

elements are functionally unimp ortant in the isolated heart Cardiovascular

Research Have OK

Cla A J Clark Comparative Physiology of the Heart Cambridge University

Press Comment A clear summary of the state of knowledge in

Includes references to earlier work Has numerous tables and graphs Two

chapters are of particular relevances Chapter The work of the Heart

and Chapter The Inuence of Chemical Environment Not in ZOOL

Have Xeroxcopy OK

Cle Logan Clendening SourceBook of Medical History Dover New York

Quoted by Acierno page re Vesalius ISBN Have

cwc OK

CMK John A Callahan Dwight C McGo on and JackDKey editors Classics

of Cardiology former title Cardiac Classicsvolume parts Krieger

Have ISBN

CMMR Jose E Castillo Greg McDermott Marc McEachern and John Richardson

A comparative analysis of numerical techniques applied to a mo del of the

otolith membrane Compters Math Applic Have OK

CMT F Cassot D Morvan and G Tonietto Unsteady ow through pros

thetic heart valvesAnintegral approach coupled with a vortex metho d In

Boundary Elements X Vol Heat Transfer Fluid Flow and Electrical

Applications pages Computational Mechanics Publications and

SpringerVerlag Have OK

Con Lawrence Conlon Dierentiable Manifolds A First Course Birkhaeuser

Boston ISBN Havecwc OK

Co o James L Co ok Conversion Factors Oxford University Press Have

cwc

Cou Coussy Mechanics of Porous Continua Wiley Get ISBN

Order Kruep er

Cov James W Covell Functional dynamics of the myo cyteconnective tissue

unit In T F Robinson and R K H Kinne editors Cardiac Myocyte

Connective Tissue Interactions in He alth and Disease Issues Biomedvol

ume Karger Basel Have OK

CPSS Colin Gerald Caro T J PedleyRCSchroter and W A Seed The

Mechanics of the Circulation Oxford University Press Have Xerox

copy ISBN OK

Cria Criseld NonLinear Finite Element Analysis Wiley Get ISBN

Ordered Kruep er

Crib M A Criseld Nonlinear Finite Element Analysis of Solids and Struc

tures Vol Essentials Wiley ISBN Get

Cry Colin Walker Cryer A comparison of the threedimensional consolidation

theories of Biot and Terzaghi Quarterly Journal of Mechanics and Applied

Mathematics Part Have

CST C J Chuong M S Sacks G Templeton F Schwiep and R L John

son Regional deformation and contractile function in canine rightventric

ular free wall Am J Physiol Heart and Circulatory Physiology

H Have Medline abstract

CT L J Chang and John M Tarb ell Numerical simulation of fully develop ed

sinusoidal and pulsatile physiological ow in curved tub es J Fluid Mech

Have OK

Cul David F Culclasure Anatomie und Physiologie des Menschen Lehrpro

gramme Band Herz und Kreislaufsystem VCH Verlagsgesellschaft

Weinheim ISBN Have OK

Cur John D Currey The Me chanical Adaptation of Bones Princeton University

Press Princeton Quoted by Biewener Biomechanics Structures and

Systems A Practical Approach Have pap er copy Not in BIP

OK

Cus J H Cushman editor Dynamics of Fluids in Hierarchial Porous Media

Academic Press San Diego Get AMR ISBN

CvD Angela Y Cheer and Cornelis Pvan Dam editors Fluid Dynamics in Biol

ogy Proceedings of an AMSIMSSIAM Joint Summer Research Conference

held July with support from the National ScienceFoundation and

NASA Headquartersvolume of Contemporary Mathematics American

Mathematical So ciety Providence Have ISBN

CW Carleton B Chapman and Eugene Wasserman On the dynamics of cardiac

muscle American Heart Journal Translation Otto Frank Zur

Dynamik des Herzmuskels

CW James W Covell and Lewis K Waldman Ventricular wall motion In Henk

E D J ter Keurs and J V Tyb erg editors Mechanics of the Circulation

chapter pages Martinus Nijho Publishers Have

Dav M J Davies Colour Atlas of Cardiovascular Pathology Oxford University

Press Have OK ISBN

Dav Paul Davis The art of the heart valve SIAM News Have

O K

Daw Thomas H Dawson Engineering Design of the Cardiovascular System of

Mammals Prentice Hall Ordered Heers p

ISBN Have

dC Manfredo P do Carmo Dierentialgeometrie von Kurven und Flaechen

Vieweg Braunschweig corrected edition Abbreviated translation

ISBN X Havecwc OK

dC Manfredo Perdigao do Carmo Riemannian Geometry Birkhaeuser

ISBN Have OK

dC Manfredo Perdigao do Carmo Dierential Geometry of Curves and Sur

faces Prentice Hall Englewo o d Clis Get Order Kruep er for

cwc

DD Delaeld DuBois and Eugene F DuBois Clinical calorimetry V The mea

surement of the surface area of man Archivs of internal Medicine

Quoted by Dinnar in b o ok edited by Ghista as source of formula

of DuBois and Dub ois Have OK

DD Delaeld DuBois and Eugene F DuBois Clinical calorimetry a formula

to estimate the approximate surface area if height and weightbeknown

Archivs of internal Medicine Get

Del M Delbruck Knotting problems in biology mathematical problems in the

biological sciences Proc Symp Appl Math Quoted by

Winfree Get Math

DF John Kenneth Dickinson and PAForsyth Preconditioned conjugate gra

dient metho ds for three dimensional linear elasticity Tec hnical rep ort

Department of Computer Science UniversityofWaterlo o Obtained

by ftp from Waterlo o Rep ort CS Have

DH Jim Douglas Jr and Ulrich Hornung editors Flow in Porous Media

Proceedings of the Oberwolfach Conference June Birkhaeuser

Verlag Basel Have OK ISBN

DHN Angela J DrakeHolland and Mark I M Noble editors Cardiac

Metabolism Wiley Interscience LC pap ISBN

Bks Demand Not in MED Ordered Kruep er

Nachfragen b ei Kruep er

DHW A S Douglas W C Hunter and MD Wiseman Inhomogeneous defor

mation as a source of error in strain measurements derived from implanted

markers in the canine left ventricle Journ Biomech

Get OK XEROX Biomech

Dic John Kenneth Dickinson Preconditioned conjugate gradient metho ds for

three dimensional linear elasticityTechnical rep ort Department of Com

puter Science UniversityofWaterlo o Obtained by ftp from Water

lo o Rep ort CS Have

Die Bernhard Dierb erger FiniteElemente Simulation der Herzdynamik

Das HerzgroessenSchlagvolumen Konze pt PhD thesis Eb erhardKarls

Universitaet Tuebingen Have

Din Uri Dinnar Cardiovascular Fluid Dynamics CRC Press p

ISBN Not in MED Have pap er copy

DMT Sid DeutschandEvangelia MicheliTzanakou Neuroelectric Systems New

York University Biomedical Engineering Series New York University Press

From K B Chandran Cardiovascular Biomechanics Ordered

Kruep er

DROH A S Douglas Edward K Ro driguez W ODell and W C Hunter Unique

strain history during ejection in canine left ventricle American Journal on

Physiology Heart and Circulatory Physiology HH

Have OK

DS Paul Doucet and Peter B Slo ep Mathematical Modeling in the Life Sci

ences Ellis Horwo o d in Mathematics and its Applications Ellis Horwood

Have ISBN X

DSLT Jean G Dumesnil Rashad M Shoucri JeanLouis Laurenceau and Jules

Turcot A mathematical mo del of the dynamic geometry of the intact left

ventricle und its application to clinical data Circulation

Have OK

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Eis Luther Pfahler Eisenhart Introduction to Dierential Geometry with Use

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Vergrien lt Kruep er

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ETvdBW Gijs Elzinga G PTo orop G C van den Bos and Nicolaas Westerhof

Ventricular pump function and arterial resistance In Henk E D J ter

Keurs and J V Tyb erg editors Mechanics of the circulationchapter

pages Martinus Nijho Publishers Have

Eul L Euler Principia pro motu sanguins p er arterias determinadeo Opera

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I M Noble editors Starlings Law of the Heart Revisited pages

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Mechanics of active contraction in cardiac muscle Part I I Cylindrical

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search Have

HH Hugh E Huxley and J Hanson Changes in the crossstriations of muscle

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Symposiumvolume ASME Have

HKT Hideyuki Honda Yoshiro Koiwa KazuhikoTakagi JunIchi Kikuchi

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left ventricular segment length in acute regional ischaemia in the in situ

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passivemyo cardium Transactions of the ASME Journal of Biomechanical

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In Rob ert L Spilker and Bruce R Simon editors Computational Methods

in Bioengineering BED volume pages American So cietyof

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to myo cardial activation and ventricular mechanics In Theo C Pilkington

Bruce Loftis Jo e F Thompson Savio LYWo o Thomas C Palmer and

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Kardio dynamik Wege zur strukturgerechten Analyse der Myokardfunktion

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dimensional nite element analysis of stresses and strains in the intact

heart Comput Biomed Res Quoted byPerl Horowitz

and Sideman Get

HPS Arie Horowitz M Perl and Samuel Sideman Geo desics as a mechanically

optimal b er geometry for the left vetnricle Basic Res Cardiol

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prehensive mo del for the simulation of left ventricle mechanics Part Im

plementation and results analysis Medical and Biological Engineering and

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Part see Perl Horowitz and Sideman

HS Peter J Hunter and Bruce H Smaill The analysis of cardiac function a

contin uum approach Prog Biophys mol Biol Have

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HSHY Jay D Humphrey Rob ert K Strumpf Henry R Halp erin and Frank

C P Yin Toward a stress analysis in the heart In Leon Glass Peter J

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HSWE Ro elof Martinus Huisman Pieter Sipkema Nicolaas Westerhof and Gijs

Elzinga Wall stress measurements in nonb eating canine hearts appli

cation of a metho d tested in rubb er mo dels Cardiovascular Research

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Elzinga Comparison of mo dels used to calculate left ventricular wall force

Medical Biolo gical Engineering Computing Have

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HTRR William P Ho o d Jr Walter J Thomson Charles E Rackley and Ellis L

Rolett Comparison of calculations of left ventricular wall stress in man

from thinwalled and thickwalled ellipsoidal mo dels Circulation Research

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Hui Ro elof Martinus Huisman Forces in the Wal l of the Left Ventricle

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Hul Derek Hull An Introduction to Composite MaterialsCambridge University

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Hun Peter Hunter Finite element analysis of cardiac muscle mechanics PhD

thesis Oxford University Get Quoted byPedley in Fluid Mechanics

of Large Blo o d Vessels p

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sity Press Havecwc ISBN Ordered Kruep er

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Beating Left Ventricle and the Intramyo cardial Coronary Circulation PhD

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Rob ert M Heethaar The constitutive b ehaviour of passive heart muscle

tissue A quasilinear visco elastic formulation Journ Biomech

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mo del of the diastolic left ventricle

HvCW R Huiskes DickHvan Camp en and J R De Wijn Biomechanics Prin

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HW Gab or T Herman and Dallas Webster editors Surfaces of organs in dis

crete threedimensional spacevolume of Lect Notes Med Inf Ob erwol

fach Pro c Have Summary

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HY Jay D Humphrey and F rank C P Yin Biaxial mechanical b ehaviour of

excised epicardium Transactions of the ASME Journal of Biomechani

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cardium

HY Jay D Humphrey and Frank C P Yin Constitutive relations and nite

deformations of passive cardiac tissue I I Stress analysis in the left ventricle

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HYMW Anna R Hashima Alistair A Young Andrew D McCullo ch and Lewis K

Waldman Nonhomogeneous analysis of epicardial strain distributions dur

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Ib e A S Ib erall Growth form and function on mammals Ann N Y Acad

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IHP Myron B Allen I I I Ismael Herrera and George F Pinder Numerical

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Ile A Ileb ekk Mechanics of the interventricular septum In Henk E D J ter

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pages Martinus Nijho Publishers Hav e

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Jac William Jaco Lectures on threemanifold top ology American Mathemat

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Jal Jose Jalife Mathematical Approaches to Cardiac Arrhythmias Annals of

the New York Academy of Sciences Have OK Only the table

of contents

JC Desmond G Julian and J Campb ell Cowan Cardiology Bailliere Tindall

London th edition Have OK ISBN

Jea Roger V Jean Phyl lotaxis A systemic study in plant morphogenesis Cam

bridge University Press Have OK

Jew B R Jewell Intro duction The changing face of the lengthtension relation

In Ciba Foundation Sta editor The Physiological Basis of Starlings Law

of the Heart pages Elsevier Amsterdam Have

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tion Lectures and communications Workshop on Cardiovascular Dynam

ics Tainach Tinje October Europ ean So ciety for Noninva

ve sive Cardiovascular Dynamics Ljubljana Medicinski Razgledi Ha

YU ISSN

JK S Johnson and William M Kier Intramuscular crossed connective tissue

bres Skeletal supp ort in the lateral ns of squid and cuttle sh Mollusca

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and Applied Mathematics Philadelphia Havecwc OK ISBN

JM Christopher R Johnson and Rob ert S MacLeo d Nonuniform spatial mesh

adaptation using a p osteriori error estimates applications to forward and

inverse problems Applied Numerical Mathematics Have

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Computational medicine Bio electric eld problems IEEE October pages

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links Contemporary Mathematics In MathBibl Have

Kap Daniel Theo dore Kaplan The Dynamics of Cardiac Electrical Instability

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Kat Arnold M Katz The descending limb of the Starling curve and the failing

heart Circulation Have OK

Kat Arnold M Katz Physiology of the HeartRaven Press New York second

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drew A Biewener editor Biomechanics Structures and Systems A Prac

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KP F Kapp el and R O Peer A mathematical mo del for fundamental regu

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LG M Lorange and R M Gulranjani A computer heart mo del incorp orating

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James W Co vell Contribution of collagen matrix to passiveleftventricular

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Mor Thomas F Moriarty The law of Laplace Its limitations as a relation for

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Measurement of strain and analysis of stress in resting rat left ventricular

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otRS Symb ols Committee of the Royal So ciety Quantities Units and Sym

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HighPerformance Computing in Biomedical ResearchCRC Press Inc

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Wol Julius Wol Das Gesetz der Transformation der Knochen Hirschwald

Berlin Reprinted Schattauer Verlag Stuttgart ISBN

An english translation is also available yHave OK

Wom J R Womersley The mathematical analysis of the arterial circulation in a

state of oscillatory motion Wright Air Development Center

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Won Alan Y K Wong Some prop osals in cardiac muscle mechanics and ener

getics Bul letin of Mathematical Biology Get ZD

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Wo o Rob ert H Wo o ds A few applications of a physical theorem to membranes

in the human b o dy in a state of tension J Anat Physiol

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WR Alan Y K Wong and P M Rautaharju Stress distribution within the left

ventricular wall approximated as a thick ellipsoidal shell American Heart

Journal Have ZQu OK

WS Arthur T Winfree and S H Strogatz Singular laments organize chemical

waves in three dimensions WaveTaxonomy Physica D

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WTB Julian J Wu T C T Ting and David M Barnett Modern Theory of

Anisotropic Elasticity and Applications So ciety for Industrial and Applied

Mathematics Philadelphia Have ISBN

WW E H Web er and W Web er Wel lenlehre auf experimente begruendet o der

Ueber die Wel len tropfbarer uessigkeiten mit Anwendung auf die Schal l

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Yam Hiroshi Yamada Strength of Biological Materials Williams Wilkins

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Yan Ming Yang Application of Nonlinear Porosity to the Analysis of Cardiac

Muscle PhD thesis UniversityofRochester DA Diss

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YGG A L Yettram B S Grewal and D G Gibson Mo deling the left ventricle

for determination of the elasticity of the myo cardiuml J Eng Med

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Yin Frank C P Yin Applications of the niteelement metho d to ventricular

mechanics CRC Critical Reviews in Biomedical Engineering

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Yin Frank C P Yin editor Ventricularvascular Coupling Clinical Physio

logical and Engineering Aspects SpringerVerlag New York Get

WG Out of Print MED

YLK Ajit PYoganathan Jack D Lemmon Jr Young H Kim Peter G Walker

Rob ert A Levine and Carol C Vesier A computational study of a thin

walled threedimensional left ventricle during early systole Transactions

of the ASME Journal of Biomechanical Engineering

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You Thomas Young Hydraulic investigations subservienttoanintended cro o

nian lecture on the motion of the blo o d Phil Trans Roy Soc London

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You Thomas Young On the function of the heart and arteries Philosophical

Transactions Royal So ciety London Get In UB ZC

YSBL Hitoshi Yaku Bryan K Slinker Stephen P Bell and Martin M LeWinter

Eects of free wall ischemia and bundle branch blo ck on systolic ventricular

interaction in dog hearts American Journal on Physiology Heart and

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YSCZ Frank C P Yin Rob ert K Strumpf Paul H Chew and Scott L Zeger

Quantication of the mechanical prop erties of noncontracting canine my

o cardium under simultaneous biaxial loading Journ Biomech

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YSF Edward L Yellin Edmund H Sonnenblick and Rob ert W M Frater Dy

namic determinants of left ventricular lling An overview In Jan Baan

Alexander C Arntzenius and Edward L Yellin editors Cardiac Dynam

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Factor and Sonnenblick Have OK

YTC Ming Yang Larry A Tab er and E B Clark A nonlinear p oro elastic mo del

for the trab ecular embryonic heart T ransactions of the ASME Journal of

Biomechanical Engineering Have

YVG A L Yettram C A Vinson and D G Gibson Eect of myo cardial

b er architecture on the b ehaviour of the human left ventricle in diastole

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ZLL Conrad M Zapanta Edward G Liszka Jr Theo dore C Lamson David R

Stinebring Steve Deutsch David B Geselowitz and John M Tarb ell A

metho d for realtime in vitro observation of cavitation on prosthetic heart

valves Transactions of the ASME Journal of Biomechanical Engineering

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ZTa Olgierd Cecil Zienkiewicz and R L Taylor The Finite Element Method

Vol Basic Formulation and Linear Problems McGrawHill London th

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ZZZ ZZZ Coronary circulation Transactions of the ASME Journal of Biome

chanical Engineering Nov Get AMR A

ZZZ ZZZ Inuence of endo cardialepicardial crossover of muscle b ers on left

ventricular wall mechanics Journ Biomech Get

A

Index

endo cardium

afterload

epicardium

allometric equations

erectile prop erties of the coronary microvas

Anrep eect

culature

aortic regurgitation

external work

aortic stenosis

aortic valve

Feng eect

applied mechanics

Fenn eect

ariticial valves

brillation

arrhythmias

brotendinous ring

arterioventricular valves

eld equations

atrioventricular valves

nite elements

uidbre mo dels

ballistic cardiography

foliation

basal metab olic rate

forcefrequency relationship

b o dy surface area

forceinterval relationship

Bowditch

formula of DuBois and DuBois

Buckinghams Theorem

fractal analysis

capillaries

FrankStarlingLaw

cardiac arrhythmias

garden hose eect cardiac energetics

geo desics

cardiac tamp onade

geometric measure theory

cardiovascular muscles

Gregg eect

chaos

growth chordae tendineae

collagen matrix

heart as a mechanical pump

computer graphics

Heart Murmurs

constitutivelaws

Heart Sounds

continuum mechanics

heart sounds

coronary artery

Ho dgkinHuxley equations

coronary circulation

hydraulic mo del

coronary p erfusion

hydrostatic skeleton

coronary p erfusion pressure

coronary sinus

immersed interface problems

immersedb oundary metho d

descending limb

Incomp etence

diastole

inferior vena cava

dicrotic wave

intercalated disk

Dimensional analysis

intervalforce relationship

dynamic similarity

intervalstrength relationship

EDP

intramyo cardial pressure

EDV

isometric loading

ejection fraction

elastic similarity

elasticity

embryonic heart

enddiastolic pressure

enddiastolic volume

isotonic

rightventricle

Rightventricular wall motion

jet

sarcomeres

kinesiology

semilunar valves

knots

septum

Korotko sounds

ts shun

Singleunit smo oth muscle

Law of Laplace

skeletal muscles

left atrium

smo oth muscle

left ventricle

Starling curve

Left ventricular wall motion

Starlings Law of the Heart

Lie Group

Stenosis

stenosis

mechanics

striated muscle

mitral valve

strokevolume

Mo ensKorteweg formula

sup erior vena cava

mousetoelephant curve

symmorphosis

Multiunit smo oth muscle

synctial smo oth muscle

Murrays formula

systemic circulation

muscle

systole

muscle mechanics

muscular hydrostat

thermo dynamics

myo cardial oxygen consumption

trab eculae carnae

myo cyte

tricuspid valve

myo cytes

Turbulentow

new elastic b o dy

valve vibration

numerical metho ds

vaso dilators

venous system

optimal design

ventricular function curve

orthostasis

ventricular interaction

papillary muscles

visceral smo oth muscle

pattern formation

volumepressurework

p erfusion pressure

vortex

p ericardectomy

whirl ow

p ericardial eusion

Wol s Law

p ericarditis acute

Womersley numb er

p ericarditis constrictive

Womersley parameter

p ericardium

phyllotaxis

Poiseuille ow

p oro elastic mo dels

preload

pulmonary circulation

pulmonary valve

regurgitation

remo delling

Reynolds numb er

right atrium