Mechanical Properties of Thoracic and. Abdominal Arteries of Sheep

Similar documents
Full-field measurements and identification for biological soft tissues: application to arteries in vitro

NORMAL STRESS. The simplest form of stress is normal stress/direct stress, which is the stress perpendicular to the surface on which it acts.

Lectures on. Constitutive Modelling of Arteries. Ray Ogden

IN VITRO DEGRADATION AND EROSION OF DEGRADABLE LACTATE SEGMENTED POLYURETHANES

MECE 3321 MECHANICS OF SOLIDS CHAPTER 3

Activity Tensile Testing SIM

Numerical study of blood fluid rheology in the abdominal aorta

Computer Modeling in Bioengineering

ME 2570 MECHANICS OF MATERIALS

Stress-Strain Analysis of Abdominal Aortic Wall: A Case of 3D Geometry Simulation

Pharmaceutical compounding I Colloidal and Surface-Chemical Aspects of Dosage Forms Dr. rer. nat. Rebaz H. Ali

Engineering Solid Mechanics

ME 243. Mechanics of Solids

4.MECHANICAL PROPERTIES OF MATERIALS

Mathematical Models and Numerical Simulations for the Blood Flow in Large Vessels

Physics 207 Lecture 22. Lecture 22

AN ANISOTROPIC PSEUDO-ELASTIC MODEL FOR THE MULLINS EFFECT IN ARTERIAL TISSUE

Sean Carey Tafe No Lab Report: Hounsfield Tension Test

Finite Element Modeling of the Pulse Wave propagation in the aorta for simulation of the Pulse Wave Imaging (PWI) method

Lab Exercise #3: Torsion

Multiscale modeling of failure in ABS materials

A PROTOCOL FOR DETERMINATION OF THE ADHESIVE FRACTURE TOUGHNESS OF FLEXIBLE LAMINATES BY PEEL TESTING: FIXED ARM AND T-PEEL METHODS

PATHOLOGICAL conditions often induce changes in biological

Effects of Aging on the Mechanical Behavior of Human Arteries in Large Deformations

Tensile stress strain curves for different materials. Shows in figure below

Mathematical Model of Blood Flow in Carotid Bifurcation

COMPARISON OF COHESIVE ZONE MODELS USED TO PREDICT DELAMINATION INITIATED FROM FREE-EDGES : VALIDATION AGAINST EXPERIMENTAL RESULTS

How Should We Measure and Report Elasticity in Aortic Tissue?

MOLECULAR, CELLULAR, & TISSUE BIOMECHANICS

TINIUS OLSEN Testing Machine Co., Inc.

PULSE WAVE PROPAGATION IN LARGE BLOOD VESSELS BASED ON FLUID-SOLID INTERACTIONS METHODS

1.103 CIVIL ENGINEERING MATERIALS LABORATORY (1-2-3) Dr. J.T. Germaine Spring 2004 LABORATORY ASSIGNMENT NUMBER 6

Outline. Tensile-Test Specimen and Machine. Stress-Strain Curve. Review of Mechanical Properties. Mechanical Behaviour

Module-4. Mechanical Properties of Metals

Finite Element Method Analysis of the Deformation of Human Red Blood Cells

This chapter is concerned with the mechanical behavior of blood vessels. under static loading conditions and the methods required to analyze this

Identification of Hyperelastic Anisotropic Properties in Vascular Biomechanics Based on In- Vivo and In- Vitro Measurements

4.4 Tensegrity model for the cytoskeleton

Stress Analysis Lecture 3 ME 276 Spring Dr./ Ahmed Mohamed Nagib Elmekawy

Medical Biomaterials Prof. Mukesh Doble Department of Biotechnology Indian Institute of Technology, Madras. Lecture - 04 Properties (Mechanical)

Chapter Two: Mechanical Properties of materials

Experimentally Calibrating Cohesive Zone Models for Structural Automotive Adhesives

BioMechanics and BioMaterials Lab (BME 541) Experiment #5 Mechanical Prosperities of Biomaterials Tensile Test

The objective of this experiment is to investigate the behavior of steel specimen under a tensile test and to determine it's properties.

NE 125 L. Title Page

MATERIALS FOR CIVIL AND CONSTRUCTION ENGINEERS

Back Calculation of Rock Mass Modulus using Finite Element Code (COMSOL)

Mechanical Properties of Materials

9 MECHANICAL PROPERTIES OF SOLIDS

A Numerical Model of Atherosclerotic Lesions in Human Arteries

Vessel Wall Models for Simulation of Atherosclerotic Vascular Networks

COMPUTATION OF EIGENSTRESSES IN THREE-DIMENSIONAL PATIENT-SPECIFIC ARTERIAL WALLS

Fig. 1. Different locus of failure and crack trajectories observed in mode I testing of adhesively bonded double cantilever beam (DCB) specimens.

The science of elasticity

Elastic Properties of Solid Materials. Notes based on those by James Irvine at

Influence of residual stresses in the structural behavior of. tubular columns and arches. Nuno Rocha Cima Gomes

Tensile Properties of Ag Alloy Clad Bi-2212 Round Wires

Samantha Ramirez, MSE. Stress. The intensity of the internal force acting on a specific plane (area) passing through a point. F 2

EFFECTS OF MOLECULAR STRUCTURE ON MACROSCOPIC MECHANICAL PROPERTIES OF AN ADVANCED POLYMER (LARC -SI)

TOUGHNESS OF PLASTICALLY-DEFORMING ASYMMETRIC JOINTS. Ford Research Laboratory, Ford Motor Company, Dearborn, MI 48121, U.S.A. 1.

N = Shear stress / Shear strain

Elasticity. A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University Modified by M.

Laboratory 4 Bending Test of Materials

Laboratory 4 Topic: Buckling

Theory at a Glance (for IES, GATE, PSU)

Propagation of dissection in a residually-stressed artery model

Instrumented Impact Testing

Materials and Structures. Indian Institute of Technology Kanpur

UNIT I SIMPLE STRESSES AND STRAINS

Supplementary Figures

Stress-Strain Behavior

6.4 A cylindrical specimen of a titanium alloy having an elastic modulus of 107 GPa ( psi) and

Mechanical properties 1 Elastic behaviour of materials

Elastic Properties of Solids (One or two weights)

Modeling of Fiber-Reinforced Membrane Materials Daniel Balzani. (Acknowledgement: Anna Zahn) Tasks Week 2 Winter term 2014

Constitutive Modeling of Biological Soft Tissues

Statics Principles. The laws of motion describe the interaction of forces acting on a body. Newton s First Law of Motion (law of inertia):

Arterial Macrocirculatory Hemodynamics

Numerical Model of the Influence of Shear Stress on the Adaptation of a Blood Vessel BMT 03-35

Mechanics of Materials Primer

THEME IS FIRST OCCURANCE OF YIELDING THE LIMIT?

THE S-S CURVE APPROXIMATION FOR GFRP TENSILE SPECIMEN BY USING INVERSE METHOD AND OPTIMIZATION

Numerical Study of the Behaviour of Wall Shear Stress in Pulsatile Stenotic Flows

PURE BENDING. If a simply supported beam carries two point loads of 10 kn as shown in the following figure, pure bending occurs at segment BC.

Mechanical Properties of Biological Materials M.Richetta and R.Montanari

Slow crack growth in polycarbonate films

Lecture 17: Cell Mechanics

Fig. 1. Circular fiber and interphase between the fiber and the matrix.

There are three main types of structure - mass, framed and shells.

ME 207 Material Science I

5. STRESS CONCENTRATIONS. and strains in shafts apply only to solid and hollow circular shafts while they are in the

INTRODUCTION TO STRAIN

Objectives: After completion of this module, you should be able to:

A Performance Modeling Strategy based on Multifiber Beams to Estimate Crack Openings ESTIMATE in Concrete Structures CRACK

Biomaterial Scaffolds

Discontinuous Galerkin methods for nonlinear elasticity

MAGNETIC FLUX LEAKAGE INVESTIGATION OF INTERACTING DEFECTS: COMPETITIVE EFFECTS OF STRESS CONCENTRATION AND MAGNETIC SHIELDING

Material Characterization of Carbon Fiber Reinforced Polymer Laminate Using Virtual Fields Method

CTC 460 kcmil ACCC Conductor Stress Strain Tests

7.4 The Elementary Beam Theory

Transcription:

Adv. Theor. Appl. Mech., Vol. 5, 2012, no. 4, 173-178 Mechanical Properties of Thoracic and Abdominal Arteries of Sheep Kadri Salim Laboratory of Industrial Mechanic, (LMI) Department of Mechanical Engineering Badji Mokhtar University BP12, Annaba-Algeria salim.kadri@yahoo.fr Bouchelaghem Abdelaziz Mahmoud Laboratory of Industrial Mechanic, (LMI) Department of Mechanical Engineering Badji Mokhtar University BP12, Annaba-Algeria Lemouchi Karim Department of Electronics Badji Mokhtar University BP12, Annaba-Algeria Abstract An accretion dalliance is accorded by biotechnology, in general, and biomaterials, in particular, in determining the mechanical properties of different biological tissues comprising or composing the living creatures bodies. Their microscopic and macroscopic structures are complex and mechanical tests can be of a major in studying their mechanical properties [1] [8] [7]. During operation, any blood circulation system is subject to an alternating blood pressure and the constituent organs behave differently. Amongst the rudimentary mechanical tests to characterize thoracic and abdominal arteries, and soft tissues as well - vital components of the blood circulatory system we find the traction test. This work focuses on the characterization of thoracic and abdominal arteries, located on the same trunk of a sheep, precisely determining Young s modulus, elasticity constraints, and deformations and break strain.

174 K. Salim, B. A. Mahmoud and L. Karim Keywords: Mechanical testing, biomaterials, mechanical properties of soft tissues. 1Introduction Any soft tissues pathologies are usually accompanied by an alteration in their mechanical properties [7] [8]. Mechanical properties of the arterial wall ensue from its characteristics of elasticity and contractility. These two factors are tightly correlated to the organization and the state of degeneration of cells and macromolecules that compose the vascular tissue [3] [6]. Due to the fact that tissue pathologies give raise to localized changes in the mechanical properties of the affected tissue, the alteration arterial wall s mechanical properties can be regarded as a parameter for the characterization of vascular tissue. This is what happens in atherosclerotic lesions cases, where the arterial wall thickens and loses its elasticity. Knowing the mechanical properties of blood vessels has been, for long lasting, recognized as a chief aspect of understanding the cardiovascular system behavior. In 1808, Thomas Young described a relationship between the elasticity of blood vessels and circulatory hemodynamic. Grand part of Young s researches are based on the nature of the elasticity and[7], in particular, the relationship between the elastic properties of arteries and the arterial wave propagation speed. His work on the elasticity nature led to the development of elasticity modulus concept that bears his name, however. The elastic behavior of the arterial wall plays an important role in determining the speed of the pressure wave propagation. The benefit of mechanical tests is to identify the mechanical properties and characteristics of any material in such a fashion, diseases and issues like deformation, rupture and sudden swelling of the artery are averted. 2Testing Methodology The tensile (traction) test can precisely determine the targeted mechanical properties: Young's modulus E, the elastic limit σ élast and breaking stress σr. To accomplish that, deformation and strain curves must be drawn. Deformation (Strain) measurements will be carried out by means of extensometer which comprises two blades where the gap between them constitutes the basis of measurement (useful length L). Tensile tests on biological tissue will be made in a in-vitro way (inactive tissue) [2] [4] [5]. Three samples of a sheep thoracic artery will enable us to carry out three tests.

Mechanical properties of thoracic and abdominal arteries of sheep 175 3Test conditions - Room temperature (ambient temperature): 20 0 C - Constant Test speed: 100 mm / min - Zero clamp slippage. - Sample specimen-artery tissue from a sheep, shape and dimensions are shown below. Figure 1. Sample form Effective specimen length L 0 = 100mm Length between the jaws L = 80mm Width b 0 = 20mm Thickness of the specimen a 0 = 1mm - Machine and features: brand ZWICK 1120, "power of 2.5 KN, jaws maximum displacement 1140 mm, displacement speed 100 mm / min. - Software used: Test Expert Version 1.9 4 Results Figure 2. Stress-strain curves

176 K. Salim, B. A. Mahmoud and L. Karim N a 0 b 0 E σ elast σ max ε max ε c σ c σ r testing Mm mm N/mm 2 N/mm 2 N/mm 2 % % N/mm 2 N/mm 2 1 1 20 1.22 0.125 0.76 68.41 118.08 0.054 6.43 2 1 20 1.31 0.130 0.84 71.15 122.80 0.060 7.428 3 1 20 1.28 0.127 0.81 69.78 120.44 0.060 7.2864 Table 1. Mechanical properties obtained E (N/mm 2 ) σ elast (N/mm 2 ) σ max (N/mm 2 ) average 1.27 0.12733 0.8033 Variance 0.0021 0.0000063 0.00958 standard deviation 0.0458 0.00251 0.09787 Table 2. Statistical Characteristics Figure 3. Working curve in Joule versus displacement 5 Concluding remarks The shape of the obtained curve corresponds to the classic one of Euler. We perfectly can distinguish (discriminate) three parts: the elastic, almost straight, is characterized by stress and relatively low deformations, the curved section (portion) is featured by fairly high deformations and stresses, the third portion, as it is concerned, is characterized by an abrupt drop of effort corresponding to the

Mechanical properties of thoracic and abdominal arteries of sheep 177 maximum stress or tensile strength of the tissue. The peaks and ranges of the curve imply a reorganization of the structure during the elongation process, because the tissue is made up of three layers (intima, media and adventitia). The identified and measured features of the tests show that the stresses and deformations are low in the elastic region (ε <15%, up to 0127 N/mm2 σ) and significant in the other two zones (up 71.15 ε % σ 0.803N/mm2 up). The dispersion (diffusion/ spread) found is rather significant, despite the short test. It is due to the nature of samples which are soft tissues with high contractility. The activity (work) at the beginning of the displacement is almost nil, it begins to rise from a certain value, thence it finally stabilizes. The deformation and the recorded activity on the sheep s artery show that the soft type tissue is a non-elastic material. 6. Nomenclature L 0 : effective specimen Length L: Length between jaws b 0 : Width a 0 : Thickness of the specimen E: Young's Modulus σ: Stress σ c : Conventional Stress σ r : Accurate Tensile stress σ elast : Elasticity stress σ max : Maximum stress ε: Deformation ε c : Conventional Deformation ε max : Maximum deformation References [1] N. Assoul, P. Flaud, M. Chaouat, D. Letourneur, I. Battle, Mechanical properties of rat thoracic and abdominal Aortas, Journal of Biomechanics, 8p, 2008. [2] F. Mc Cunntock and A. Argon, Mechanical Behavior of Materials, Addison Wesley (1966). [3] D. Francois, Technical engineering, Part I: Mechanical testing of materials, CNRS, Paris.

178 K. Salim, B. A. Mahmoud and L. Karim [4] P. Laurent, Experimental Methods for Materials Testing cold, cf. p17. [5] D. Mc Lean, Mechanical properties of metal, John Wiley, 1967. [6] L. Soualmi, Characterizing the elastic properties of the arterial wall by endovascular ultrasonography, PhD (Biomedical Engineering), Polytechnique School of Montreal, October 1998. [7] J. J. Wang, K. H. Parker, Wave Propagation in a Model of the arterial circulation, Journal of Biomechanics, 10 p, 2003. [8] D. Zelmati, Study of mechanical properties and toughness of HDPE for the gas pipeline coatings, Thesis of magister, Annaba, 2005. Received: January, 2012