• Aucun résultat trouvé

Full-field strain measurement and material

N/A
N/A
Protected

Academic year: 2022

Partager "Full-field strain measurement and material"

Copied!
51
0
0

Texte intégral

(1)

Centre for Biomedical and Healthcare Engineering CNRS UMR 5307

Mr Aaron Romo, Prof Stéphane Avril, Dr Pierre Badel, Dr Ambroise Duprey, Prof

Jean-Pierre Favre, Prof Sam Evans

Full-field strain measurement and material

identification in soft tissue biomechanics

(2)

2

BSSM Cardiff - 2013/09/05 - Stéphane AVRIL

Location

(3)

3

Center for Biomedical and Healthcare Engineering

Campus with hospital, medical school, prevention center, college of engineering and companies manufacturing

medical devices

BSSM Cardiff - 2013/09/05 - Stéphane AVRIL

(4)

4

4 topics

22 permanent staff 35 postgraduate

students and postdocs

Soft tissue

biomechanics

Biomaterials for bone

replacement Healthcare

engineering

Biotoxicity of inhaled

nanoparticules

BSSM Cardiff - 2013/09/05 - Stéphane AVRIL

(5)

5

BSSM Cardiff - 2013/09/05 - Stéphane AVRIL

Biomechanics of soft tissues

The aim is to employ biomechanical models to adapt the treatments of cardiovascular and osteoarticuar diseases to each patient

Orthèses fonctionnelles

Orthèses de rééducation

Orthèses prophylactiques

(6)

6

BSSM Cardiff - 2013/09/05 - Stéphane AVRIL

Today’s talk…

(7)

7

BSSM Cardiff - 2013/09/05 - Stéphane AVRIL

ascending aorta

descending aorta

(thoracic aorta and abdominal aorta)

arch of aorta ▶ a local dilation of the aorta

due to aortic wall weakening

a fatal medical emergency aneurysm rupture

Aortic aneurisms

(8)

8

BSSM Cardiff - 2013/09/05 - Stéphane AVRIL

Aortic aneurisms

(9)

9

BSSM Cardiff - 2013/09/05 - Stéphane AVRIL

PREVENTION OF ATAA RUPTURE FROM A

BIOMECHANICAL

POINT OF VIEW???

(10)

10

Quantify the risk of rupture for each patient…

BSSM Cardiff - 2013/09/05 - Stéphane AVRIL

[McGloughlin T. Biomechanics and mechanobiology of aneurysms. 2012, Springer

(11)

11

2 IMPORTANT QUESTIONS

What are the patient-specific material properties of the

tissue?

What is the patient-specific strength of the tissue?

BSSM Cardiff - 2013/09/05 - Stéphane AVRIL

(12)

12

BSSM Cardiff - 2013/09/05 - Stéphane AVRIL

BIOMECHANICAL EXPERIMENTAL

APPROACHES

(13)

13

Tensile rupture mode

BSSM Cardiff - 2013/09/05 - Stéphane AVRIL

[Duprey et. al., In-vitro characterisation of physiological and

maximum elastic modulus of ascending thoracic aortic aneurysms using uniaxial tensile testing, Eur. J. Vascular &

Endovascular Surgery, 2010]

(14)

14

BSSM Cardiff - 2013/09/05 - Stéphane AVRIL

Arteries: a complex structure and

behavior

(15)

15

Biomechanical comparison of aneurismal and healthy tissue

BSSM Cardiff - 2013/09/05 - Stéphane AVRIL

Vorp DA, Schiro BJ, Ehrlich MP, Juvonen TS, Ergin MA, Griffith BP. Effect of aneurysm on the tensile strength and biomechanical behaviour of the ascending thoracic aorta. Ann Thorac Surg 2003; 75(4):1210-4.

(16)

16

Need of biaxial tension

BSSM Cardiff - 2013/09/05 - Stéphane AVRIL

Sacks MS. Biaxial mechanical evaluation of planar biological materials. J. Elast. 61:199–246, 2000

(17)

17

BSSM Cardiff - 2013/09/05 - Stéphane AVRIL

W < 10 mJ/cm 2

Sommer G, Gasser TC, Regitnig P, Auer M., Holzapfel G.A. Dissection properties of the human aortic media: an experimental study. ASME J Biomech Eng 2008; 130:021007.

Delamination properties…

(18)

18

Lack of local analyses

Where and how does the rupture initiates?

BSSM Cardiff - 2013/09/05 - Stéphane AVRIL

(19)

19

BSSM Cardiff - 2013/09/05 - Stéphane AVRIL

MATERIALS AND

METHODS

(20)

20

BSSM Cardiff - 2013/09/05 - Stéphane AVRIL

Deformation gradient Lagrange strain

Aneurismal

aortic tissue Inflation test Optical Full-field measurement ( Full-field displacement)

Inverse procedure

Full-field

Stress reconstruction

Constitutive model

Calculation of stress at rupture

Methodology

(21)

21

BSSM Cardiff - 2013/09/05 - Stéphane AVRIL

Deformation gradient Lagrange strain

Aneurismal

aortic tissue Inflation test Optical Full-field measurement ( Full-field displacement)

Inverse procedure

Full-field

Stress reconstruction

Constitutive model

Calculation of stress at rupture

Methodology

(22)

22

BSSM Cardiff - 2013/09/05 - Stéphane AVRIL

Materials

(23)

23

BSSM Cardiff - 2013/09/05 - Stéphane AVRIL

Deformation gradient Lagrange strain

Aneurismal

aortic tissue Inflation test Optical Full-field measurement ( Full-field displacement)

Inverse procedure

Full-field

Stress reconstruction

Constitutive model

Calculation of stress at rupture

Methodology

(24)

24

BSSM Cardiff - 2013/09/05 - Stéphane AVRIL

inflation device cylinder

pressure gage

in vivo loading environments

(biaxial stress state due to internal pressure) can be generated

Inflation test

(25)

25

BSSM Cardiff - 2013/09/05 - Stéphane AVRIL

Deformation gradient Lagrange strain

Aneurismal

aortic tissue Inflation test Optical Full-field measurement ( Full-field displacement)

Inverse procedure

Full-field

Stress reconstruction

Constitutive model

Calculation of stress at rupture

Methodology

(26)

26

BSSM Cardiff - 2013/09/05 - Stéphane AVRIL

camera

Instron machine protector

Undeformed Deformed

x y

tracks the gray value pattern

in each subset during deformation

Digital image stereocorrelation

(27)

27

BSSM Cardiff - 2013/09/05 - Stéphane AVRIL

Deformation gradient Lagrange strain

Aneurismal

aortic tissue Inflation test Optical Full-field measurement ( Full-field displacement)

Inverse procedure

Full-field

Stress reconstruction

Constitutive model

Calculation of stress at rupture

Methodology

(28)

28

BSSM Cardiff - 2013/09/05 - Stéphane AVRIL

Theory of finite deformation

Deformation gradient F

Green-Lagrange strain tensor E = 1/2(C - I) right Cauchy-Green tensor C = F T F

Ux Uy Uz

from the undeformed and deformed

coordinates of each measurement data point

Assumption: plane stress

homogeneous initial thickness incompressibility

Measured displacement fields

(29)

29

BSSM Cardiff - 2013/09/05 - Stéphane AVRIL

Derivation of the strain fields

(30)

30

BSSM Cardiff - 2013/09/05 - Stéphane AVRIL

ℎ = ℎ 0

𝑭 𝟏𝟏 𝑭 𝟐𝟐 − 𝑭 𝟏𝟐 𝑭 𝟐𝟏 Thickness evolution

Incompressibility assumption:

(31)

31

BSSM Cardiff - 2013/09/05 - Stéphane AVRIL

Deformation gradient Lagrange strain

Aneurismal

aortic tissue Inflation test Optical Full-field measurement ( Full-field displacement)

Inverse procedure

Full-field

Stress reconstruction

Constitutive model

Calculation of stress at rupture

Methodology

(32)

32

BSSM Cardiff - 2013/09/05 - Stéphane AVRIL

Stress reconstruction

 Membrane elastostatics

(33)

33

Validation

BSSM Cardiff - 2013/09/05 - Stéphane AVRIL

(34)

34

BSSM Cardiff - 2013/09/05 - Stéphane AVRIL

Deformation gradient Lagrange strain

Aneurismal

aortic tissue Inflation test Optical Full-field measurement ( Full-field displacement)

Inverse procedure

Full-field

Stress reconstruction

Constitutive model

Calculation of stress at rupture

Methodology

S. Avril, P. Badel, A Duprey. Anisotropic and hyperelastic identification of in vitro human arteries from full-field

measurements. Journal of Biomechanics -2010, vol 43, N°15, pp 2978-2985.

J. Kim, S. Avril, A Duprey, JP Favre. Experimental characterization of rupture in human aortic aneurysms using full-field

measurement technique. Biomechanics and Modeling in Mechanobiology, 2012.

(35)

35

Incompressibility:

J =1

Constitutive model

BSSM Cardiff - 2013/09/05 - Stéphane AVRIL

(36)

36

Point-wise stress-strain curve fitting

BSSM Cardiff - 2013/09/05 - Stéphane AVRIL

(37)

37

BSSM Cardiff - 2013/09/05 - Stéphane AVRIL

RESULTS

(38)

38

BSSM Cardiff - 2013/09/05 - Stéphane AVRIL

Results

(39)

39

BSSM Cardiff - 2013/09/05 - Stéphane AVRIL

Local distribution of material

properties

(40)

40

BSSM Cardiff - 2013/09/05 - Stéphane AVRIL

Statistical analysis of the results

(14) (10)

(24)

(7)

(41)

41

BSSM Cardiff - 2013/09/05 - Stéphane AVRIL

Ultimate stresses

inflation device

(42)

42

BSSM Cardiff - 2013/09/05 - Stéphane AVRIL

Rupture modes

(43)

43

BSSM Cardiff - 2013/09/05 - Stéphane AVRIL

Rupture initiation

(44)

44

BSSM Cardiff - 2013/09/05 - Stéphane AVRIL

Conclusions

(45)

45

BSSM Cardiff - 2013/09/05 - Stéphane AVRIL

Modes of rupture???

The tissue thinning starts to localize very early before the rupture

-> presence of aneslatic response in very local areas

(46)

46

BSSM Cardiff - 2013/09/05 - Stéphane AVRIL

Conclusions

 The strength of the tissue is heterogeneous

 Existence of weaker zones in the tissue

 Damage develops in the weaker zones

 Damage leads to rupture when the pressure increases.

 What is the microstructural specificity of the weaker zone?

 Does it affect the elastic response in the

physiological domain?

(47)

47

BSSM Cardiff - 2013/09/05 - Stéphane AVRIL

Current questions…

inflation device

 Accurate measurement of the thickness distribution

 Validity of the incompressibility assumption

 Effect of loading conditions and environment

(48)

48

BSSM Cardiff - 2013/09/05 - Stéphane AVRIL

Future work

(49)

49

BSSM Cardiff - 2013/09/05 - Stéphane AVRIL

Microscopic analysis

Multiphoton-second harmonic generation (MP-SHG) microscope 600x

Intima Media

Smooth muscle cells Elastin fibers

Collagen fibers

Biologic sensor and filter

Adventitia Collagen fibers

(50)

50

BSSM Cardiff - 2013/09/05 - Stéphane AVRIL

In vivo imaging

S. Avril, F. Schneider, C. Boissier, ZY Li. In vivo velocity vector imaging and time-resolved strain rate measurements in the wall of blood vessels using MRI. Journal of Biomechanics, 2010, 44(5) pp 979-983.

US elastography

(51)

51

BSSM Cardiff - 2013/09/05 - Stéphane AVRIL

Acknowledgements

Références

Documents relatifs

Bottle bases construction in a circular zone around the injection point (PI) and visualization of the displacement field when bottles are under internal pressure: (c) VS base, (d)

The purpose of the identification problems is to retrieve some of mechanical parameters (known for the direct problem) from kinematic measurements, that is to find the description of

We present a polarization-sensitive full-field optical coherence tomography system that can produce high- resolution images of the linear retardance and reflectivity properties

Un banc d'essai de micro-traction est utilisé pour tester la traction de fibres élémentaires de lin. Les champs de déplacements de la fibre sont calculés en temps réel par

Although numerous distinct core cracks are clearly observed, it is proposed to identify the behavior of plaster- board through a homogenized continuum description where the

Progress in this problem can be envisioned along different directions, namely either by including the constitutive law hypothesis earlier in the identification procedure, so that

The measurement of the 8 first modes of a vibrating cantilever plate has been performed using a deflectometry setup composed of a single standard camera.. This fast expo- sure

Figures 4 shows en face tomographic images in the plane of the glass surface through the scattering layer, obtained with both cameras with the same detection sensitivity