Limiting fiber extensibility as parameter for damage in venous wall Lukas Horny, Rudolf Zitny, Hynek Chlup, Tomas Adamek and Michal Sara Faculty of Mechanical.

Slides:



Advertisements
Similar presentations
Mini-Seminar Dr. James Throne, Instructor
Advertisements

Structural scales and types of analysis in composite materials
Mechanics of Composite Materials
Application of A Phenomenological Viscoplasticity Model to The Stress Relaxation Behavior of Unidirectional and Angle-ply Laminates at High Temperature.
Testing and Modeling Rate Dependent
1 Unsymmetrical and/or inhomogeneous cross sections | CIE3109 CIE3109 Structural Mechanics 4 Hans Welleman Module : Unsymmetrical and/or inhomogeneous.
Column Buckling - Inelastic
Modeling of Neo-Hookean Materials using FEM
Silly Putty Opening Question
A Constitutive Model Based on Meso and Micro Kinematics for Impregnated Woven Continuous Fibre Reinforced Composites P. Harrison M.J. Clifford A.C. Long.
Micromechanics Macromechanics Fibers Lamina Laminate Structure Matrix.
Basic Terminology • Constitutive Relation: Stress-strain relation
Namrata Gundiah University of California, San Francisco
Constitutive Relations in Solids Elasticity
APPLIED MECHANICS Lecture 10 Slovak University of Technology
Prof. Dr. Nenad Filipovic 1,2 1) Faculty of Mechanical Engineering, University of Kragujevac, Kragujevac, Serbia 2) Harvard School of Public Health, Boston,
Ali Jafry Teacher Pre Calculus & Pre AP Pre Calculus Carbon Nanotube-Epoxy Composites Dr. Dimitris Lagoudas, Dr. Daniel Davis, Patrick Klein & Lesley Weitz.
Mechanics of Materials II
Finite Element Method in Geotechnical Engineering
INTRODUCTION INTO FINITE ELEMENT NONLINEAR ANALYSES
Classical Laminated Plate Theory
Expectations after today’s lecture
MECHANICAL PROPERTIES OF MATERIALS.  Engineers are primarily concerned with the development and design of machines, structures etc.  These products.
© 2011 Autodesk Freely licensed for use by educational institutions. Reuse and changes require a note indicating that content has been modified from the.
Elastic Stress-Strain Relationships
© 2011 Autodesk Freely licensed for use by educational institutions. Reuse and changes require a note indicating that content has been modified from the.
Review (2 nd order tensors): Tensor – Linear mapping of a vector onto another vector Tensor components in a Cartesian basis (3x3 matrix): Basis change.
Effective Inelastic Response of Polymer Composites by Direct Numerical Simulations A. Amine Benzerga Aerospace Engineering, Texas A&M University With:
Rheology I. Rheology Part of mechanics that deals with the flow of rocks, or matter in general Deals with the relationship of the following: (in terms.
EXPERIMENTAL METHODS 2010 PROJECT CONSTITUTIVE EQUATIONS
School of Civil EngineeringSpring 2007 CE 595: Finite Elements in Elasticity Instructors: Amit Varma, Ph.D. Timothy M. Whalen, Ph.D.
MODELLING THE PULLOUT OF HOOKED STEEL FIBERS FROM CEMENTITIOUS MATRIX Edmunds Zīle, Olga Zīle Institute of Polymer Mechanics Riga, Latvia.
Mechanics of Materials – MAE 243 (Section 002) Spring 2008
Poisson’s Ratio For a slender bar subjected to axial loading:
Experimental methods E181101
Elastography for Breast Cancer Assessment By: Hatef Mehrabian.
Dr. Wang Xingbo Fall , 2005 Mathematical & Mechanical Method in Mechanical Engineering.
Thrust III: Structure-based assessment of renal artery mechanics Infrastructure for Biomechanical Experiments The program for Biomedical Engineering has.
Constitutive models Part 1 Background and terminology Elasticity.
STRESS-STRAIN RELATIONSHIP
A novel approach for thermomechanical analysis of stationary rolling tires within an ALE-kinematic framework A. Suwannachit and U. Nackenhorst Institute.
Copyright Kaplan AEC Education, 2005 Mechanics of Materials Outline Overview AXIALLY LOADED MEMBERS, p. 262 Modulus of Elasticity Poisson’s Ratio Thermal.
Stress and Strain ( , 3.14) MAE 316 – Strength of Mechanical Components NC State University Department of Mechanical & Aerospace Engineering Stress.
Strain energy density To eliminate the effects of size, evaluate the strain- energy per unit volume, The total strain energy density resulting from the.
Namas Chandra and Sirish Namilae
Z. Guo, R. De Vita A Probabilistic Constitutive Law For Damage in Ligaments Page 1 Z. Guo, R. De Vita A Probabilistic Constitutive Law For Damage in Ligaments.
Viscoelasticity - 2 BME 615 “It’s a poor sort of memory that only works backwards” - Lewis Carroll, Alice through the Looking Glass.
Soft Tissues Unlike bone, most solid tissues are soft –they can undergo large deformations without failing Soft tissues with obvious mechanical functions:
Boundary Value Problems in Elasticity
Strain Energy Density Hyperelasticity BME 615 University of Wisconsin.
Nonlinear Elasticity of Soft Tissues
Mechanical Properties and Active Remodeling of Blood Vessels Gross anatomy of systemic and pulmonary circulation Microscopic structure Mechanical properties.
Topic 5: Bone Mechanics Bone is a hard connective tissue
Finite Element Method in Geotechnical Engineering
Soft Tissues Unlike bone, most solid tissues are soft
Topic 10: Nonlinear Elasticity of Soft Tissues
Loss of elastic fiber integrity compromises common carotid artery function: Implications for vascular aging  J. Ferruzzi, M.R. Bersi, R.P. Mecham, F.
Influence of Flow-Independent Viscoelasticity
Date of download: 10/23/2017 Copyright © ASME. All rights reserved.
APPLICATION OF COHESIVE ELEMENT TO BIMATERIAL INTERFACE
Continuum Mechanics (MTH487)
Continuum Mechanics (MTH487)
From: Constitutive Modeling of Brain Tissue: Current Perspectives
Mechanics of Biomaterials
روش عناصر محدود غیرخطی II Nonlinear Finite Element Procedures II
Volume 107, Issue 11, Pages (December 2014)
Visco-plastic self-consistent modeling of high strain rate and
ME 323 Final Lecture – April 2012
Volume 107, Issue 11, Pages (December 2014)
Finite element analysis of the wrinkling of orthotropic membranes
Presentation transcript:

Limiting fiber extensibility as parameter for damage in venous wall Lukas Horny, Rudolf Zitny, Hynek Chlup, Tomas Adamek and Michal Sara Faculty of Mechanical Engineering Czech Technical University in Prague Czech Republic

Introduction  Constitutive modeling of a wall of human vena cava inferior.  Constitutive model is fundamental information about material behavior  Constitutive model is needed for every engineering simulation which includes displacements and deformations

Goals  Suggestion of new constitutive model incorporation of structural information possibility of clear interpretation for parameters  Description of mechanical response within elastic behavior within inelastic behavior

Blood vessel mechanics  Geometric nonlinearity ̶ large strains  Physical nonlinearity ̶ nonlinear stress – strain relationship large strain stiffening  Anisotropy

Blood vessel mechanics  Inelastic behavior  Preconditioning  Viscoelasticity  Pseudoelasticity Loading and unloading curves are always different

Constitutive equations  Stored energy function ψ  1 st law of Thermodynamics  Zero energy under reference configuration  Zero stress under reference configuration  Constitutive equation  Terms for stored energy

Limiting fiber extensibility Reference configuration Deformed configuration Limiting configuration stress stretch  Limiting fiber extensibility mimics idea of limiting chain extensibility in polymer physics  Limiting fiber extensibility can capture large strain stiffening Reference Deformed Limiting

Limiting chain extensibility  Gent model - isotropy AN Gent rubbers …material parameter - shear modulus …material parameter – limiting extensibility parameter …1st invariant of a deformation tensor stress I1I1 I 1 = J m + 3 Limiting

Limiting fiber extensibility  Suggested model – local orthotropy …shear modulus …limiting extensibility parameter …4th invariant of a deformation tensor …angle between fibers and circumferential axis Blood vessel wall as a fiber reinforced composite stress I4I4 I 4 = J m + 1 Limiting z t 

Material parameters estimation Material parameters must be identified experimentally  Inflation–extension test  Computational model  Thick walled – tube  Hyperelastic fiber reinforced material  Matrix + fibers  Incompressibility  No shear strains  No residual strains

Regression  Measured data  Model predictions  Radial displacement (image analysis of photographs)  Axial displacement (image analysis of photographs)  Internal pressure (pressure probe recording)  Axial force (defined weight + pressure onto bottom) p …internal pressure F …axial force r …deformed radius t, z …stretch – z axial; t circumferential

Results – vena cava inferior Internal pressure p [kPa] Circumferential and axial stretch t, z [1] Axial force F [N] 1 st overloading cycle 2 nd overloading cycle 3 rd overloading cycle 4 th overloading cycle  Axial force Internal pressure o Physiological loading Supra-physiological

Results – vena cava inferior Axial force F [N] Internal pressure p [kPa] Representative cycle of supra-physiological loading Circumferential and axial stretch t, z [1]  Axial force Internal pressure Model predictions

Damage evolution 1 st overloading cycle 2 nd overloading cycle 3 rd overloading cycle 4 th overloading cycle  Axial force Internal pressure Supra-physiological loading only Axial force F [N] Internal pressure p [kPa] Circumferential and axial stretch t, z [1] Model predictions

Conclusion  Stored energy function based on limiting fiber extensibility assumption fits experimental data (inflation –extension test) successfully  Damage can be related to evolution of the limiting extensibility parameter J m  The only history dependent parameter J m is capable to explain different trends of stretches in axial and circumferential directions

Limiting fiber extensibility as parameter for damage in venice walls The End