54
1 Theo Arts [email protected] Frits Prinzen, Tammo Delhaas*, Peter Bovendeerd**, J. Lumens, W. Kroon (Biophysics, Physiology, Pediatric Cardiology, Engineering) Maastricht University, *Maastricht University Hospital **University of Technology, Eindhoven The Netherlands IPAM Feb 06 Modeling of heart mechanics with adaptation of tissue to load

Modeling of heart mechanics with adaptation of tissue to load

  • Upload
    niyati

  • View
    26

  • Download
    0

Embed Size (px)

DESCRIPTION

Modeling of heart mechanics with adaptation of tissue to load. Theo Arts [email protected] Frits Prinzen, Tammo Delhaas*, Peter Bovendeerd**, J. Lumens, W. Kroon (Biophysics, Physiology, Pediatric Cardiology, Engineering) Maastricht University, *Maastricht University Hospital - PowerPoint PPT Presentation

Citation preview

Page 1: Modeling of heart mechanics with adaptation of tissue to load

1

Theo [email protected]

Frits Prinzen, Tammo Delhaas*, Peter Bovendeerd**, J. Lumens, W. Kroon (Biophysics, Physiology, Pediatric Cardiology, Engineering)

Maastricht University, *Maastricht University Hospital**University of Technology, Eindhoven

The Netherlands

IPAM Feb 06

Modeling of heart mechanics with adaptation of tissue to load

Page 2: Modeling of heart mechanics with adaptation of tissue to load

2

Modeling:- Finite Element Model Electro-Mechanics of the heart- CircAdapt = whole circulation model- Incorporation of adaptation with Self-structuring

Models

Page 3: Modeling of heart mechanics with adaptation of tissue to load

3

left+right ventricle movie:

sarcomere length & pV

FEM of LV+RV- paced, depolarization wave with pacing- full cardiac cycle(R. Kerckhoffs, 2003)

Page 4: Modeling of heart mechanics with adaptation of tissue to load

4

CircAdapt model of heart and circulation

lungs

RA

RV

LA

LV

aorta

system

Dynamic(t)CompliancesInertiasNon-linear

Page 5: Modeling of heart mechanics with adaptation of tissue to load

5

Modeling structure of myocardial wall with adaptation:- mechanical load determines

wall massfiber orientationsheet orientation

- size and shape of blood vessels

Enormous reduction of number of parameters

Especially in pathology: Generally 1 basic cause of pathology, followed by physiological adaptation processes.

Parameter reduction: Self-structuring by simulation of adaptation

Page 6: Modeling of heart mechanics with adaptation of tissue to load

6

gene expressionprotein formation

adaptation

Local tissue adaptation

(pump) function

pressure flow load

tissue propertiesstructuregeometry

tissuestress & strain

Whole organ function

Cardiovascular adaptation to mechanical load

Implication: Cell adaptation determines organ structure

Page 7: Modeling of heart mechanics with adaptation of tissue to load

7

Myofiber structure and hypertrophy

Result of local adaptation?

Page 8: Modeling of heart mechanics with adaptation of tissue to load

8

Cardiac fiber structure

F. Torrent-Guasp

LVRV

apical view, upper layers peeled off(randomly?)

Page 9: Modeling of heart mechanics with adaptation of tissue to load

9

Filling/Rest

Activation

Relaxation

Force/StretchSynchrony

Shortening

What signals to the cells can be used for adaptation?

Page 10: Modeling of heart mechanics with adaptation of tissue to load

10

fibroblast

extra-cellularmatrix

myocyte

deformation

(filling)

myocyte orientation

in myocyte optimum: - principal stress alingment - sarcomere shortening

(fiber structure)

tissue mass (wall mass)

stretch contractility

extra-cellular matrix strain

softening

Used adaptation rules of cardiac tissue

Arts, 1994, Biophys J. 66:953-961.

Page 11: Modeling of heart mechanics with adaptation of tissue to load

11

Page 12: Modeling of heart mechanics with adaptation of tissue to load

12

Diffusion Tensor ImagingMyofiber orientation components in cross-section

of the goat heart.

posterior

anterior

perpendicular

in plane Base to apex In plane

1/2

Page 13: Modeling of heart mechanics with adaptation of tissue to load

13

Transmural course of helix angle (goat)

L. GeertsAJP 2002

model predicted

Page 14: Modeling of heart mechanics with adaptation of tissue to load

14

15

10

5

0

midwall radius ( )

mm

baseapex-20 20(mm)

equator

0

model prediction

10o

0o

-10o

transverseangle ( )

Transverse angle, model experiment (pig)

leftventricle

L. Geerts, AJP 2002

Page 15: Modeling of heart mechanics with adaptation of tissue to load

15

Myofiber structure

Proposed adaptation rules for local tissue →

Realistic helical and transverse fiber structure

Page 16: Modeling of heart mechanics with adaptation of tissue to load

16

Sheet structure

Page 17: Modeling of heart mechanics with adaptation of tissue to load

17

Fiber-Sheet Structure

endocardium

midwall

epicardium

Page 18: Modeling of heart mechanics with adaptation of tissue to load

18

Sheets split on plane of maximum shear

Hypothesis

Find plane with maximum shear

45o directions of maximum shear,

2 planes

Fiber direction not in one of those planes

Constraint: Sheet planes also contain the fiber direction

Page 19: Modeling of heart mechanics with adaptation of tissue to load

19

Sheet Angles6 pooledexperiments BASE

rz rzrc rc

APEX

0o

45o

90o

135o

180o

0o

45o

90o

135o

180o

epi endo Arts, T, Am J Physiol. 280:H2222-H2229 (2001).

model predicted: 2 solutions with different likelyhood

Page 20: Modeling of heart mechanics with adaptation of tissue to load

20

Simulation of short axis sheet cross-sections

seems realistic

Page 21: Modeling of heart mechanics with adaptation of tissue to load

21

Sheets facilitate wall thickening and shortening by shear

(and rotation)

(J. Covell)

Page 22: Modeling of heart mechanics with adaptation of tissue to load

22

Unloading for shear by 90º sheet rotation has same macroscopic effect on mechanics, ab= ba ≈ 0

So, sheet orientation itself is quite irrelevant for modeling, as long as it unloads the major component of shear stress.

2 solutions for sheat orientation

Page 23: Modeling of heart mechanics with adaptation of tissue to load

23

Cross-sheet slice

Courtesy A. Young

Page 24: Modeling of heart mechanics with adaptation of tissue to load

24

Sheet structure

- Sheet plane contains myofiber direction

- Designed to facilitate cross fiber deformation, thus minimizing chamber stiffness

Page 25: Modeling of heart mechanics with adaptation of tissue to load

25

Application of predicted structure in analysis

Non-invasive determination of transmural difference in myofiber shortening with aortic stenosis

Page 26: Modeling of heart mechanics with adaptation of tissue to load

26

epi

Aortic stenosis

aortic stenosis

endo

region with high intramyocardial pressure,causing coronary flow obstruction

high left ventricular

pressure

Subendocardial dysfunction

Page 27: Modeling of heart mechanics with adaptation of tissue to load

27

- Torsion tuned to Shortening- IF Subendocardial TSR=( Torsion / Shortening )

Shortening & Torsioninner - - outer - -

outer

inner

Shortening onlyinner - - -outer -

Torsion onlyinner +outer -

Wall segment model (cylindrical)

Determination of transmural differences

Page 28: Modeling of heart mechanics with adaptation of tissue to load

28

Rotation and deformation of the heart can be quantified

ribs

LV wall

RV

cavity

lung

Magnetic Resonance Tagging (MRT)

Page 29: Modeling of heart mechanics with adaptation of tissue to load

29

MRTshortening

torsion

torsion

shortening = ln(Cavity Area)

Definitions

Torsion/Shortening measurement

Page 30: Modeling of heart mechanics with adaptation of tissue to load

30

Mri-Software: Midwall motion and circumferential strain

Normal human left ventricle

Page 31: Modeling of heart mechanics with adaptation of tissue to load

31

TSR in Control and AVS patients

Inner wall strain ln(L/LVc=Vw)

TSR=slope of torsion versus inner wall strain in systole:

- Dimensionless- Species independent- Expresses transmural difference in contractile function

Control= healthy young

AVSten= Aortic Valve Stenosis

AVRepl= 3 mo after aortic valve replacement

Page 32: Modeling of heart mechanics with adaptation of tissue to load

32

From TSR to TransDifModel:

Torsion/Shortening (TSR)↓

normalized transmural difference in myofiber shortening (TransDif)

TransDif=Difference/Mean

Van der Toorn A et al. Am J Physiol. 2002;283:H1609-1615

Stunned subendocardial

myocardium regains function

Page 33: Modeling of heart mechanics with adaptation of tissue to load

33

CircAdapt modela. Modeling of circulation

- Lumped model in modules:chambers, tubes, valves

b. Adaptation of modules to load

Search:

Google + keyword ‘CircAdapt’

hit ‘AJP’: Arts T et al. Am J Physiol. 2005;288:H1943-H1954hit ‘Biophysics’: MatLab source code

Page 34: Modeling of heart mechanics with adaptation of tissue to load

34

Circulation in modules

Page 35: Modeling of heart mechanics with adaptation of tissue to load

35

1-fiber model of a thick-walled cavity (chamber or blood vessel)

Vlv

plv

Vw

ventricle (LV)

wrapped in 1 myofiber

wlv3

1f

wlvlvf

VV31ln

VV31p

f= myofiber stressf= myofiber strainplv= LV pressureVlv= LV volumeVw= wall volume

FEM model confirms: Shape is practically irrelevant

Page 36: Modeling of heart mechanics with adaptation of tissue to load

36

Laws of adaptation

Adaptation of Blood vessel• Shear stress → Diameter ↑

• Wall stress → Wall thickness ↑

• Contractility+diastolic stretch → Hypertrophy

• Deformation → Dilatation

Adaptation of Cavity

Page 37: Modeling of heart mechanics with adaptation of tissue to load

37

Input to CircAdapt value SI-unit description

Page 38: Modeling of heart mechanics with adaptation of tissue to load

38

Simulations after adaptation

Page 39: Modeling of heart mechanics with adaptation of tissue to load

39

Pressure-Volume & Stress-Strain Loops

Page 40: Modeling of heart mechanics with adaptation of tissue to load

40

Calculated parameters= Result

Page 41: Modeling of heart mechanics with adaptation of tissue to load

41

Promising applications

1. Boundary conditions for FEM of heart

2. Patient specific modeling

3. “Non-invasive catheterization”Pressure difference over:

- membrane → pressure transducer

- valve with inertiadoppler velocity and accelerationmass ~ dynamic membrane

→ pressure transducer

Page 42: Modeling of heart mechanics with adaptation of tissue to load

42

Hypertrophy in12 wks myofiber

mechanics in AV-block

Systolic fiber stress is not the stimulus to hypertrophy.

More likely: end-diastolic stress

(Donker et al, Basic Res Cardiol, 2005).

Page 43: Modeling of heart mechanics with adaptation of tissue to load

43

Adaptation rules with‘deformation intervention’

Page 44: Modeling of heart mechanics with adaptation of tissue to load

44

fiber direction

torsion

fiber direction

torsion

Situs Solitus(normal)

Situs InversusTotalis (SIT) Hypothesis

SIT heart with mirrored fiber structure is an alternative solution satisfying adaptation rules of cardiac cells.

Test

SIT heart should have equal torsion but in opposite direction.

occurrence

8000 : 1

Page 45: Modeling of heart mechanics with adaptation of tissue to load

45

Situs Inversus Totalis Normal

(pig SIT heart)

Page 46: Modeling of heart mechanics with adaptation of tissue to load

46

Situs Solitus (normal) ?? Situs Inversus Totalis ??Torsion (rad)

-0.20 -0.10 0 0.10 0.20

Expected torsion in SIT

NOT TRUE !

Page 47: Modeling of heart mechanics with adaptation of tissue to load

47

-0.10

0.00

0.10

0.20Rotation

[rad]

-0.20

-0.10

0.00

0.10Torsion

5 base43

2

1 apex

d basecba apex

Situs Solitus(normal)

Situs InversusTotalis (n=14)

0.5 s

Human torsion

Page 48: Modeling of heart mechanics with adaptation of tissue to load

48

-0.20

Situs Solitus (normal) Situs Inversus Totalis

Torsion (rad)

Torsion in SIT

-0.10 0 0.10 0.20

Delhaas, T. et al. Ann N Y Acad Sci 1015: 190-201.

Page 49: Modeling of heart mechanics with adaptation of tissue to load

49

Myofiber structure in SITNormal adaptation rules

Start conditions for fiber structure:- normal apex- inverse base

Development to SIT structure

→ RESULT

Page 50: Modeling of heart mechanics with adaptation of tissue to load

50

Situs Inversus Totalis

A natural in vivo ‘experiment’ to investigate cell’s long term response to a variety of deformations

boundary conditions

Page 51: Modeling of heart mechanics with adaptation of tissue to load

51

inverse

Dualistic myofiber structure SIT

Helix angleendo - epi

inverse

normal

normal

Page 52: Modeling of heart mechanics with adaptation of tissue to load

52

Efficency

The structure of the SIT heart is different.

Because each cell optimizes generation of mechanical work (= adaptation rule), all cells work close to their optimum. Since the only escape of mechanical work is pump work, the SIT heart works about just as optimal as the normal heart.

stress-strain work

stress-strain work

stress-strain work

The only escape of work:

pump work (p-V)

Page 53: Modeling of heart mechanics with adaptation of tissue to load

53

General conclusion: Self-structuring by adaptation

“morphogenetic draft”

result

Self-adaptation until load is proper

growing brick

- works for cardiovascular modeling on all levels- adaptation can be modeled- should be used as prior knowledge in heart modeling

Page 54: Modeling of heart mechanics with adaptation of tissue to load

54

That ’SIT