Miami, FL September 11-15, 2012

Size: px
Start display at page:

Download "Miami, FL September 11-15, 2012"

Transcription

1 TBI Assessment Based on Biomechanical Modeling of Brain Tissue at the Cellular Level Under Blast Loading Mariusz Ziejewski, Ph.D., Inż and Ghodrat Karami, Ph.D. North American Brain Injury Society Presenter Mariusz Ziejewski, Ph.D., Inż Professor Director of Impact Biomechanics Laboratory, College of Engineering Director of Automotive Systems Laboratory, College of Engineering Mechanical Engineering Department North Dakota State University and Adjunct Associate Professor Department of Neuroscience, School of Medicine University of North Dakota Miami, FL September 11-15, 2012

2 Involvement with Department of Defense Researcher: 1. Armstrong Aerospace Medical Laboratory, Wright Patterson Air Force Base 2. ~900 tests analyzed with humans male/female 3. Seven (7) research contracts, Current, $600,000 grant, Blast Pressure Gradients and Fragments on Ballistic Helmets and the Head and Brain Injury Simultaneous Multiscale Modeling with Experimental Validation, Department of the Army, US Army Research, Development and Engineering Command ( ) 5. Current, $500,000 grant, Blast and the Consequences on Traumatic Brain Injury Mulitscale Mechanical Modeling of Brain Air Force Office of Scientific Research, ( ) Chair: 1. Chairman, Scientific Peer Review Panel, Proposals, Integrated Eye Tracking and Neural Monitoring for Enhanced Assessment of Mild TBI, United States Medical Research and Materiel Command (USARMC), DoD Psychological Health, Polytrauma, and Operational Health (PHPOH) Program. (2012) 2. Chairman, Scientific Peer Review Panel, Physics of Blast as it relates to Brain Injury, Intramural proposals, DoD PTSD/TBI Research Program, Congressionally Directed Medical Research Program (CDMRP). (2007) 3. Chairman, Scientific Peer Review Panel, Physics of Blast as it relates to Brain Injury, Extramural proposals, DoD PTSD/TBI Research Program, CDMRP. (2007) Reviewer: 1. Reviewer, Proposals for United States Army Medical Research and Materiel Command (USARMC) Psychological Health, Polytrauma, and Operational Health (PHPOH) Program (2012) 2. Reviewer, Proposals for United States Medical Research and Materiel Command (USARMC) Warrior Injury Assessment Manikin (WIAMan) Program (2012) 3. Reviewer, Proposals for United States Medical Research and Materiel Command (USAMRMC) Military Medical Research and Development Grant Program (2010, 2011) 4. Reviewer, Intramural Proposals for the Department of Defense (DoD) Defense Medical Research and Development Program, Intramural Applied Research and Advanced Technology Development Award (2009) 5. Reviewer, Proposals for the Military Operational Medical Research Program, US Army Materiel Research Command (USAMRMC).(2008) 6. Reviewer, Intramural Proposals for the Department of Defense (DoD) Intramural War Supplement Program.(2008) 7. Reviewer, Scientific Peer Review Panels, Concept Proposals related to brain injuries caused by blasts for the DoD (PTSD/TBI) Research Program, CDMRP. (2007) 8. Reviewer, Scientific Peer Review Panels, Intramural Proposals on Clinical Diagnosis related to brain injuries caused by blasts for the DoD (PTSD/TBI) Research Program, CDMRP. (2007) Invited Faculty: 1. Invited Faculty, Invited by former US Air Force Surgeon General P.K. Carlton to make a presentation on the Physics of Blast Injury to a special conference/think tank session on allocation of Department of Defense (DoD) funding for TBI/blast injuries. 2. Invited Faculty, National Veteran s Health Administration/Department of Defense (VHA/DoD) Conference: Visual Consequences of Traumatic Brain Injury. 3. Invited Faculty, National Veteran s Health Administration/Department of Defense (VHA/DoD) Conference: Sensory Impairment Issues in Traumatic Brain Injury.

3 Direction of Our Research (Sponsored by DoD) Multiscale modeling method proposed for brain cell adhesion modeling: (a) MD (molecular dynamics)simulation of Cell-ECM (extracellular matrix)interaction (b) Average traction-separation data from MD simulation (c) Axon- ECM continuum modeling of the interface (d) Undulated RUC (repeating cell unit) of brain material and fiber reinforced composite modeling of the tissue (e) Micromechanics modeling of RUC under different load cases for material characterization

4 Invisible Injury macro scale (mm) (10-3 m) MRI detection limit Fig. A, B, C Diffusion Tensor Imaging (DTI) 1x1x5 mm 3 Susceptibility Weighted Imaging (SWI) 0.2x0.2x0.2 mm 3 micro scale (μm) (10-6 m) the cell Fig. D MR Microscopy (MRM) 100 μm 3, Tesla Performed only on autopsied brain nano scale (nm) (10-9 m) the axon neural filaments Fig. E Electron microscope to visualize Carpenter, M., Human Neuroanatomy. Baltimore, MD: Williams and Wilkins, 1976 Williams TH, Gluhbegovic N. Jew JY. The human brain: dissections of the real brain. Virtual Hospital, University of Iowa, 1997; and [21/10/22] Callot, et. al, Short-scan-time multi-slice diffusion MRI of the mouse cervical spinal cord using echo planar imaging, NMR in Biomedicine, 2008

5 BIOMECHANICS the application of the principles and techniques of mechanics to the structure, functions and capabilities of living organisms. Webster s New World Dictionary of the American Language Ed. David B. Guralnik. 2 nd College Ed. New York: World Pub. Co., 1970

6 IMPACT NEUROTRAMA (Traumatic Brain Injuries) APPLICATION OF FORCE RAPID HEAD VELOCITY CHANGE LINEAR ANGULAR BRAIN DEFORMATION BRAIN DAMAGE CHANGE TO SHAPE CHANG E TO VOLUME NEURONAL (DAI) VASCULAR CYTOSKELERAL STRUCTURE

7 Accelerometer

8 TYPES OF ACCELERATION Linear Acceleration Rotational Acceleration Z Y X A x = Linear Acceleration, Forward-Backward Direction Ay = Linear Acceleration, Side to Side Direction A z = Linear Acceleration, Vertical Direction a x = Rotational Acceleration, About Forward-Backward Axis a y = Rotational Acceleration, About Side to Side Axis a z = Rotational Acceleration, About Vertical Axis

9 TYPES OF ACCELERATION Linear Acceleration Rotational Acceleration Z Y X A x = Linear Acceleration, Forward-Backward Direction Ay = Linear Acceleration, Side to Side Direction A z = Linear Acceleration, Vertical Direction a x = Rotational Acceleration, About Forward-Backward Axis a y = Rotational Acceleration, About Side to Side Axis a z = Rotational Acceleration, About Vertical Axis

10 TYPES OF ACCELERATION Linear Acceleration Rotational Acceleration Z Y X A x = Linear Acceleration, Forward-Backward Direction A y = Linear Acceleration, Side to Side Direction A z = Linear Acceleration, Vertical Direction a x = Rotational Acceleration, About Forward-Backward Axis a y = Rotational Acceleration, About Side to Side Axis a z = Rotational Acceleration, About Vertical Axis

11 TYPES OF ACCELERATION Linear Acceleration Rotational Acceleration Z Y X A x = Linear Acceleration, Forward-Backward Direction A y = Linear Acceleration, Side to Side Direction A z = Linear Acceleration, Vertical Direction a x = Rotational Acceleration, About Forward-Backward Axis a y = Rotational Acceleration, About Side to Side Axis a z = Rotational Acceleration, About Vertical Axis

12 TYPES OF ACCELERATION Linear Acceleration Rotational Acceleration Z Y X A x = Linear Acceleration, Forward-Backward Direction A y = Linear Acceleration, Side to Side Direction A z = Linear Acceleration, Vertical Direction a x = Rotational Acceleration, About Forward-Backward Axis a y = Rotational Acceleration, About Side to Side Axis a z = Rotational Acceleration, About Vertical Axis

13 TYPES OF ACCELERATION Linear Acceleration Rotational Acceleration Z Y X A x = Linear Acceleration, Forward-Backward Direction A y = Linear Acceleration, Side to Side Direction A z = Linear Acceleration, Vertical Direction a x = Rotational Acceleration, About Forward-Backward Axis a y = Rotational Acceleration, About Side to Side Axis a z = Rotational Acceleration, About Vertical Axis

14 TYPES OF ACCELERATION Linear Acceleration Rotational Acceleration Z Y X A x = Linear Acceleration, Forward-Backward Direction A y = Linear Acceleration, Side to Side Direction A z = Linear Acceleration, Vertical Direction a x = Rotational Acceleration, About Forward-Backward Axis a y = Rotational Acceleration, About Side to Side Axis a z = Rotational Acceleration, About Vertical Axis

15 TYPES OF ACCELERATION Linear Acceleration Rotational Acceleration Z Y X A x = Linear Acceleration, Forward-Backward Direction Ay = Linear Acceleration, Side to Side Direction A z = Linear Acceleration, Vertical Direction a x = Rotational Acceleration, About Forward-Backward Axis a y = Rotational Acceleration, About Side to Side Axis a z = Rotational Acceleration, About Vertical Axis

16 Human Head Model

17 FE Modeling of the Human Helmeted Head Head Components: Scalp Skull Dura Mater CSF Pia mater Falx Brain Tentorium Mechanical Properties: Facial bone Head component Young s modulus (GPa) Density Element type Number of elements Neck Skull E-6 Solid element 8305 Dura mater E-6 Shell element 2125 Tentorium E-6 Shell element 230 Falx E-6 Shell element 235 Pia mater 1.150E E-6 Shell element 2754 Facial bone E-6 Solid element 1124 Neck E-6 Solid element 3772 Scalp E-6 Solid element 5938 CSF E-6 Solid element 3354

18 Mechanical Properties of Brain Tissue Incompressible (High resistance to change in size, high bulk modulus) Deformable (Low resistance to change in shape, low shear modulus)

19 B.R. Donnelly and J. Medige, Shear Properties of Human Brain Tissue, Journal of Biomechanical Engineering, Nov. 1997, Vol. 119, Shames, I.H. and Cozzarelli, F.A., 1992, Elastic and Inelastic Stress Analysis, New Jersey: Prentice Hall, Englewood Cliffs, NJ Incompressible/Deformable Bulk modulus is approximately 10 5 (100,000) times larger than shear modulus. Deformation of brain tissue can be assumed to depend on shear modulus only. This behavior is common with viscoelastic materials (Shames and Cozzarelli, 1992)

20 Mechanical Properties of Brain Tissue Heterogeneous (Different properties within the brain) Anisotropic (Different properties in different directions)

21 Repeating Unit Cell - Homogenization Method The distribution of undulated axons inside the extracellular matrix for a guinea optic nerve microstructure (Meaney, 2003) simulated periodic sinusoidal undulated distribution of axons, with the corresponding periodic unit cell RUC representing undulated periodic microstructure of the composite tissue N. Abolfathi, M. Sotudeh, A. Naik, G. Karami and M. Ziejewski, A micromechanical procedure for the anisotropic modeling of mechanical properties of brain white matter, Computer Methods in Biomechanics and Biomedical Engineering 2009;12(3),

22 Axon-ECM Stress Distribution Results (c) (d) (b) (a) Illustration of the tensile stresses (S 11 ) developed in the (a) axons; (b) matrix and; the (c) tissue unit cell (d) The deformed shape of the axon with respect to its original shape is also shown in. Abolfathi N., Naik A., Sotudeh M., Karami G. and Ziejewski M. A micromechanical procedure for characterization of the mechanical properties of brain white matter Computer Methods in Biomechanics and Biomedical Engineering, 2009 (in press, available online, DOI: / ).

23 Repeating Unit Cell - Homogenization Method (a) Approximation of axons distribution inside the histology slide showing typical cross-section of the adult porcine brainstem (Abrogast and Margulies, 1999) (b) (b) Approximated random distribution (c) Hexagonal distribution (c) (d) Simulated square distribution (a) (d) Venkata Dirisala, Ghodrat Karami and Mariusz Ziejewski, A Biomechanical Investigation Of Primary Blast Head Injury Using Finite Element Methods, Annals of Biomedical Engineering (submitted) N. Abolfathi, M. Sotudeh, A. Naik, G. Karami and M. Ziejewski, A micromechanical procedure for the anisotropic modeling of mechanical properties of brain white matter, Computer Methods in Biomechanics and Biomedical Engineering 2009;12(3),

24 Mechanical Properties of Brain Tissue Viscoelastic (Time dependent properties: magnitude, duration, rate of change)

25 Viscoelastic Materials: Exhibit both viscous and elastic characteristics

26 Demonstration Slow Application of Force Rapid Application of Force

27 Visualization of INTERNAL Damage Test # 1 Impact severity ~7.5 J Low velocity (2.2 mph) Large mass (39.5 lb) Low Velocity Test # 2 Impact severity ~7.5 J High velocity (69 mph) Small mass (0.03 lb) High Velocity

28 Visualization of INTERNAL Damage Test # 1 Impact severity ~7.5 J Low velocity (2.2 mph) Large mass (39.5 lb) Low Velocity Test # 2 Impact severity ~7.5 J High velocity (69 mph) Small mass (0.03 lb) High Velocity

29 (kpa) Uniqueness of the Loading Conditions μs Supersonic overpressurization shockwave Timescale in μs (microseconds) 1atm 100 kpa

30 (kpa) Uniqueness of the Loading Conditions μs Supersonic overpressurization shockwave Timescale in μs (microseconds) 1atm 100 kpa

31 Relative Motion of the Brain

32 Coup and Counter-Coup Phenomena at the early stage (a) (b)

33 Coup and Counter-Coup Phenomena at the early stage Countercoup (C, D) Coup (A, B) (a) (b)

34 Blast Brain Trauma Countercoup (C, D) Coup (A, B) (a).0002s (b) Extremely Dynamic Oscillation of the Brain Tissue Ziejewski, M. and Karami, G., Biomechanical Perspective on Blast Injury, in Concussive Brain Trauma: Neurobehavioral Impairment and Maladaptation by Dr. Rolland Parker, Taylor & Francis Group, Boca Raton, FL, 2012

35 Properties Comparison Silicon Gel & Brain Tissue Brands, D., P. Bovendeered, G. Peter, et al. Comparison of the Dynamic Behaviour of Brain Tissue and Two Model Materials, SAE 99C21, Society of Automotive Engineers, Inc

36 Skull/Gel Model Testing Test Conditions (per ATB Simulation) : Severity of Impact (X = 10.10g, Y = 14.09g, Z = 4.02) Tested at Y = 10.55g Position of Head (Yaw 75º, Pitch 7º, Roll 6º) Video Parameters: Capture rate: 10,000 frames/sec Slow motion (1/60th of actual velocity)

37 Skull/Gel Model Testing Test Conditions (per ATB Simulation) : Severity of Impact (X = 10.10g, Y = 14.09g, Z = 4.02) Tested at Y = 10.55g Position of Head (Yaw 75º, Pitch 7º, Roll 6º) Video Parameters: Capture rate: 10,000 frames/sec Slow motion (1/60th of actual velocity) Transformed MRI Data Source of Original Data: Dr. Orrison, Nevada Imaging Centers

38 Skull/Gel Model Testing Test Conditions (per ATB Simulation) : Severity of Impact (X = 10.10g, Y = 14.09g, Z = 4.02) Tested at Y = 10.55g Position of Head (Yaw 75º, Pitch 7º, Roll 6º) Video Parameters: Capture rate: 10,000 frames/sec Slow motion (1/60th of actual velocity) Transformed MRI Data Source of Original Data: Dr. Orrison, Nevada Imaging Centers Dynamic Pattern at Impact Approach Rebound

39 (kpa) Uniqueness of the Loading Conditions μs Supersonic overpressurization shockwave Timescale in μs (microseconds) 1atm 100 kpa

40 (kpa) Cavitation Automotive Blast Supersonic overpressurization shockwave (>300m/s) Pressure increased to MPa (1atm 100 kpa) Timescale in μs (microseconds)

41 Cavitation Liquid Jet Scanning Electron Micrograph Brass Plate ~ 1 mm Crater

42 Cavitation Liquid Jet Scanning Electron Micrograph Brass Plate ~ 1 mm Crater

43 CAVITATION DAMAGE Macroscale Bubble Collapse (Classical Approach) A. Spherical Bubble Collapse Nanoscale Bubble Inception (New Brain Injury Mechanism) Mass Spring Fracture Point Mass Spring B. Non-Spherical Bubble Collapse Liquid Jet Recoil pressure waves

44 Shear Strain Response Taber, k.h. et al., J Neuropsychiatry Clin Neurosci 18: , May 2006 Area of Damage: Cortical surface Central core region Cerebellum Brain stem

45 Shear Stress Response Taber, k.h. et al., J Neuropsychiatry Clin Neurosci 18: , May 2006 Area of Damage: Brain stem Max. Shear stress distribution on sagittal section (1 lb TNT)

46 Thank You

EXAMINATION OF THE IMPACT OF HELMETS ON THE LEVEL OF TRANSFERRED LOADS TO THE HEAD UNDER BALLISTIC AND BLAST LOADS

EXAMINATION OF THE IMPACT OF HELMETS ON THE LEVEL OF TRANSFERRED LOADS TO THE HEAD UNDER BALLISTIC AND BLAST LOADS EXAMINATION OF THE IMPACT OF HELMETS ON THE LEVEL OF TRANSFERRED LOADS TO THE HEAD UNDER BALLISTIC AND BLAST LOADS A Dissertation Submitted to the Graduate Faculty of the North Dakota State University

More information

Wave Propagation Through Soft Tissue Matter

Wave Propagation Through Soft Tissue Matter Wave Propagation Through Soft Tissue Matter Marcelo Valdez and Bala Balachandran Center for Energetic Concepts Development Department of Mechanical Engineering University of Maryland College Park, MD 20742-3035

More information

Validating Critical Limits of the Universal Brain Injury Criterion

Validating Critical Limits of the Universal Brain Injury Criterion Validating Critical Limits of the Universal Brain Injury Criterion Igor Szczyrba 1, Martin Burtscher 2, and Rafał Szczyrba 3 1 School of Mathematical Sciences, University of Northern Colorado, Greeley,

More information

Development of Rotational Brain Injury Criterion (BRIC) Human Injury Research Division

Development of Rotational Brain Injury Criterion (BRIC) Human Injury Research Division Development of Rotational Brain Injury Criterion (BRIC) Human Injury Research Division Procedure Develop validated human brain FE model (SIMon) Use CSDM as a biomechanical rotational injury criterion Use

More information

MODELLING THE SHAKEN BABY SYNDROME

MODELLING THE SHAKEN BABY SYNDROME MODELLING THE SHAKEN BABY SYNDROME I.C. Howard, E.A. Patterson, J. Langley Structural Integrity Research Institute of the University of Sheffield (SIRIUS) Introduction Physical child abuse is common. For

More information

The UCD community has made this article openly available. Please share how this access benefits you. Your story matters!

The UCD community has made this article openly available. Please share how this access benefits you. Your story matters! Provided by the author(s) and University College Dublin Library in accordance with publisher policies., Please cite the published version when available. Title Finite element analysis of the effect of

More information

Composites: Part B 43 (2012) Contents lists available at SciVerse ScienceDirect. Composites: Part B

Composites: Part B 43 (2012) Contents lists available at SciVerse ScienceDirect. Composites: Part B Composites: Part B 43 (2012) 3160 3166 Contents lists available at SciVerse ScienceDirect Composites: Part B journal homepage: www.elsevier.com/locate/compositesb The influence of heterogeneous meninges

More information

ROLE OF ROTATIONAL ACCELERATION AND DECELERATION PULSES ON BRAIN STRAINS IN LATERAL IMPACT

ROLE OF ROTATIONAL ACCELERATION AND DECELERATION PULSES ON BRAIN STRAINS IN LATERAL IMPACT ROLE OF ROTATIONAL ACCELERATION AND DECELERATION PULSES ON BRAIN STRAINS IN LATERAL IMPACT ABSTRACT Jianrong Li, Jiangyue Zhang, Narayan Yoganandan, Frank A. Pintar, Thomas A. Gennarelli Department of

More information

FINITE ELEMENT ANALYSIS OF COMPOSITE MATERIALS

FINITE ELEMENT ANALYSIS OF COMPOSITE MATERIALS FINITE ELEMENT ANALYSIS OF COMPOSITE MATERIALS Ever J. Barbero Department of Mechanical and Aerospace Engineering West Virginia University USA CRC Press Taylor &.Francis Group Boca Raton London New York

More information

MECHANICAL CHARACTERIZATION OF BRAIN TISSUE

MECHANICAL CHARACTERIZATION OF BRAIN TISSUE ROLE OF MOISTURE CONTENT IN MECHANICAL CHARACTERIZATION OF BRAIN TISSUE HENRY W. HASLACH, JR. DEPARTMENT OF MECHANICAL ENGINEERING CENTER for ENERGETICS CONCEPTS DEVELOPMENT UNIVERSITY OF MARYLAND COLLEGE

More information

MODELLING AND ANALYSIS OF SOCCER HEADING AND PROTECTIVE HEADGEAR TO UNDERSTAND AND PREVENT MILD TRAUMATIC BRAIN INJURY

MODELLING AND ANALYSIS OF SOCCER HEADING AND PROTECTIVE HEADGEAR TO UNDERSTAND AND PREVENT MILD TRAUMATIC BRAIN INJURY MODELLING AND ANALYSIS OF SOCCER HEADING AND PROTECTIVE HEADGEAR TO UNDERSTAND AND PREVENT MILD TRAUMATIC BRAIN INJURY MOHD HASNUN ARIF HASSAN DOCTOR OF PHILOSOPHY UNIVERSITI MALAYSIA PAHANG UNIVERSITI

More information

The mechanical response of the midbrain to indentation

The mechanical response of the midbrain to indentation Technische Universiteit Eindhoven Mechanical Engineering Section, Mechanics of Materials Group, Materials Technology Eindhoven, September 27, 2009 The mechanical response of the midbrain to indentation

More information

Finite Element Analysis of Head Impacts in Contact Sports

Finite Element Analysis of Head Impacts in Contact Sports Finite Element Analysis of Head Impacts in Contact Sports Eyal Bar-Kochba 1, Mark Guttag 1, Subham Sett 2, Jennifer A. Franck 1, Kyle McNamara 1, Joseph J. Crisco 3, Janet Blume 1, and Christian Franck

More information

INVESTIGATION ON THE INFLUENCE. OF THE INCLUSION GEOMETRY ON ORIENTATED BRAIN TISSUE DAMAGE G.G. Melpignano MT 10.20

INVESTIGATION ON THE INFLUENCE. OF THE INCLUSION GEOMETRY ON ORIENTATED BRAIN TISSUE DAMAGE G.G. Melpignano MT 10.20 INVESTIGATION ON THE INFLUENCE OF THE INCLUSION GEOMETRY ON ORIENTATED BRAIN TISSUE DAMAGE G.G. Melpignano MT 10.20 1 INVESTIGATION ON THE INFLUENCE OF THE INCLUSION GEOMETRY ON ORIENTATED BRAIN TISSUE

More information

On the Role of a Nonlinear Stress-Strain Relation in Brain Trauma

On the Role of a Nonlinear Stress-Strain Relation in Brain Trauma On the Role of a Nonlinear Stress-Strain Relation in Brain Trauma Igor Szczyrba School of Mathematical Sciences University of Northern Colorado Greeley, CO 80639, U.S.A. Martin Burtscher Center for Grid

More information

MESH MODELING OF ANGLE-PLY LAMINATED COMPOSITE PLATES FOR DNS AND IPSAP

MESH MODELING OF ANGLE-PLY LAMINATED COMPOSITE PLATES FOR DNS AND IPSAP 16 TH INTERNATIONAL CONFERENCE ON COMPOSITE MATERIALS MESH MODELING OF ANGLE-PLY LAMINATED COMPOSITE PLATES FOR DNS AND IPSAP Wanil Byun*, Seung Jo Kim*, Joris Wismans** *Seoul National University, Republic

More information

Dynamic Response of Brain Subjected to Blast Loadings: Influence of Frequency Ranges

Dynamic Response of Brain Subjected to Blast Loadings: Influence of Frequency Ranges University of Nebraska - Lincoln DigitalCommons@University of Nebraska - Lincoln Mechanical & Materials Engineering Faculty Publications Mechanical & Materials Engineering, Department of 2011 Dynamic Response

More information

Multi-scale mechanics of traumatic brain injury

Multi-scale mechanics of traumatic brain injury Multi-scale mechanics of traumatic brain injury Cloots, R.J.H. DOI: 10.6100/IR719431 Published: 01/01/2011 Document Version Publisher s PDF, also known as Version of Record (includes final page, issue

More information

Analysis of high loss viscoelastic composites

Analysis of high loss viscoelastic composites Analysis of high loss viscoelastic composites by C. P. Chen, Ph.D. and R. S. Lakes, Ph.D. Department of Engineering Physics Engineering Mechanics Program; Biomedical Engineering Department Materials Science

More information

Skull Shape Affects Susceptibility to Traumatic Brain Injury

Skull Shape Affects Susceptibility to Traumatic Brain Injury Washington University in St. Louis Washington University Open Scholarship Mechanical Engineering and Materials Science Independent Study Mechanical Engineering & Materials Science 12-19-2016 Skull Shape

More information

Natural Frequency Analysis of the Human Head in Normal models

Natural Frequency Analysis of the Human Head in Normal models Bulletin of Environment, Pharmacology and Life Sciences Bull. Env. Pharmacol. Life Sci., Vol 5 [1] December 2015: 37-41 2015 Academy for Environment and Life Sciences, India Online ISSN 2277-1808 Journal

More information

MECHANICAL PROPERTIES OF POLYTETRAFLOUROETHYLENE ELASTOMER MEMBRANE FOR DYNAMIC CELL CULTURE TESTING ABSTRACT INTRODUCTION

MECHANICAL PROPERTIES OF POLYTETRAFLOUROETHYLENE ELASTOMER MEMBRANE FOR DYNAMIC CELL CULTURE TESTING ABSTRACT INTRODUCTION MECHANICAL PROPERTIES OF POLYTETRAFLOUROETHYLENE ELASTOMER MEMBRANE FOR DYNAMIC CELL CULTURE TESTING Carolyn Hampton 1, Gregory D. Webster 1, Beverly Rzigalinski 2, Hampton C. Gabler 1 1 Virginia Tech

More information

EVALUATION OF MICROSTRUCTURE RESPONSE UNDER VARIOUS LOADING AND BOUNDARY CONDITIONS TO AID IN THE ESTABLISHMENT OF A THRESHOLD CRITERION

EVALUATION OF MICROSTRUCTURE RESPONSE UNDER VARIOUS LOADING AND BOUNDARY CONDITIONS TO AID IN THE ESTABLISHMENT OF A THRESHOLD CRITERION EVALUATION OF MICROSTRUCTURE RESPONSE UNDER VARIOUS LOADING AND BOUNDARY CONDITIONS TO AID IN THE ESTABLISHMENT OF A THRESHOLD CRITERION FOR MILD TRAUMATIC BRAIN INJURY BY WILLIAM MATTHEW TAYLOR W. STEVE

More information

Intracranial Response in Helmet Oblique Impacts

Intracranial Response in Helmet Oblique Impacts Intracranial Response in Helmet Oblique Impacts M. Ghajari 1, U. Galvanetto 2, L. Iannucci 3, R. Willinger 4 Abstract The purpose of this work was to investigate the influence of the presence of the body

More information

Journal of Biomechanics, 47 (5):

Journal of Biomechanics, 47 (5): Provided by the author(s) and University College Dublin Library in accordance with publisher policies. Please cite the published version when available. Title The influence of acceleration loading curve

More information

Influence of Impact Velocity and Angle in a Detailed Reconstruction of a Bicycle Accident

Influence of Impact Velocity and Angle in a Detailed Reconstruction of a Bicycle Accident Influence of Impact Velocity and Angle in a Detailed Reconstruction of a Bicycle Accident Madelen Fahlstedt, Katrien Baeck, Peter Halldin, Jos Vander Sloten, Jan Goffin, Bart Depreitere, Svein Kleiven

More information

Multi-scale mechanics and structure of semi-hard cheese

Multi-scale mechanics and structure of semi-hard cheese Multi-scale mechanics and structure of semi-hard cheese T.J. Faber a,b, P.J.Schreurs b, J.M.J.G. Luyten a, H.E.H.Meijer b a FrieslandCampina Research, Deventer, The Netherlands (timo.faber@frieslandcampina.com))

More information

Quantitative Metrics for White Matter Integrity Based on Diffusion Tensor MRI Data. Stephanie Lee

Quantitative Metrics for White Matter Integrity Based on Diffusion Tensor MRI Data. Stephanie Lee Quantitative Metrics for White Matter Integrity Based on Diffusion Tensor MRI Data Stephanie Lee May 5, 2005 Quantitative Metrics for White Matter Integrity Based on Diffusion Tensor MRI Data ABSTRACT

More information

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

Full-field measurements and identification for biological soft tissues: application to arteries in vitro Centre for Health Engineering CNRS UMR 5146 INSERM IFR 143 Prof. Stéphane Avril Full-field measurements and identification for biological soft tissues: application to arteries in vitro using single-gage

More information

Micromechanical analysis of FRP hybrid composite lamina for in-plane transverse loading

Micromechanical analysis of FRP hybrid composite lamina for in-plane transverse loading Indian Journal of Engineering & Materials Sciences Vol. 15, October 2008, pp. 382-390 Micromechanical analysis of FRP hybrid composite lamina for in-plane transverse loading K Sivaji Babu a *, K Mohana

More information

06 - kinematic equations kinematic equations

06 - kinematic equations kinematic equations 06 - - 06-1 continuum mechancis continuum mechanics is a branch of physics (specifically mechanics) that deals with continuous matter. the fact that matter is made of atoms and that it commonly has some

More information

THE INFLUENCE OF IN-PLANE DENSITY VARIATION ON ENGINEERING PROPERTIES OF ORIENTED STRANDBOARD: A FINITE ELEMENT SIMULATION

THE INFLUENCE OF IN-PLANE DENSITY VARIATION ON ENGINEERING PROPERTIES OF ORIENTED STRANDBOARD: A FINITE ELEMENT SIMULATION Proceedings of McMat5: 5 Joint ASME/ASCE/SES Conference on Mechanics and Materials June 1-3, 5, Baton Rouge, Louisiana, USA 255 THE INFLUENCE OF IN-PLANE DENSITY VARIATION ON ENGINEERING PROPERTIES OF

More information

Mechanical properties 1 Elastic behaviour of materials

Mechanical properties 1 Elastic behaviour of materials MME131: Lecture 13 Mechanical properties 1 Elastic behaviour of materials A. K. M. B. Rashid Professor, Department of MME BUET, Dhaka Today s Topics Deformation of material under the action of a mechanical

More information

A Neurosurgeon s Perspectives of Diffusion Tensor Imaging(DTI) Diffusion Tensor MRI (DTI) Background and Relevant Physics.

A Neurosurgeon s Perspectives of Diffusion Tensor Imaging(DTI) Diffusion Tensor MRI (DTI) Background and Relevant Physics. A Neurosurgeon s Perspectives of Diffusion Tensor Imaging(DTI) Kalai Arasu Muthusamy, D.Phil(Oxon) Senior Lecturer & Consultant Neurosurgeon. Division of Neurosurgery. University Malaya Medical Centre.

More information

Dynamics of Transient Liquid Injection:

Dynamics of Transient Liquid Injection: Dynamics of Transient Liquid Injection: K-H instability, vorticity dynamics, R-T instability, capillary action, and cavitation William A. Sirignano University of California, Irvine -- Round liquid columns

More information

Importance of Windscreen Modelling Approach for Head Injury Prediction. Victor S. Alvarez, Svein Kleiven

Importance of Windscreen Modelling Approach for Head Injury Prediction. Victor S. Alvarez, Svein Kleiven Importance of Windscreen Modelling Approach for Head Injury Prediction. Victor S. Alvarez, Svein Kleiven Abstract The objective of this study is to evaluate the capability of two modelling approaches in

More information

Archetype-Blending Multiscale Continuum Method

Archetype-Blending Multiscale Continuum Method Archetype-Blending Multiscale Continuum Method John A. Moore Professor Wing Kam Liu Northwestern University Mechanical Engineering 3/27/2014 1 1 Outline Background and Motivation Archetype-Blending Continuum

More information

Entropic methods to study the evolution of damage and degradation of materials

Entropic methods to study the evolution of damage and degradation of materials Entropic methods to study the evolution of damage and degradation of materials Mohammad Modarres Presented at 14th International Conference on Fracture Rhodes, Greece, June 18-23, 2017 20 JUNE 2017 Department

More information

Cortical diffusion imaging

Cortical diffusion imaging Cortical diffusion imaging Alard Roebroeck Maastricht Brain Imaging Center (MBIC) Dept. of Cognitive Neuroscience Faculty of Psychology & Neuroscience Maastricht University Diffusion MRI In vivo & Ex vivo

More information

Alternative numerical method in continuum mechanics COMPUTATIONAL MULTISCALE. University of Liège Aerospace & Mechanical Engineering

Alternative numerical method in continuum mechanics COMPUTATIONAL MULTISCALE. University of Liège Aerospace & Mechanical Engineering University of Liège Aerospace & Mechanical Engineering Alternative numerical method in continuum mechanics COMPUTATIONAL MULTISCALE Van Dung NGUYEN Innocent NIYONZIMA Aerospace & Mechanical engineering

More information

Investigating the dynamic response of a punch to human head using finite element analysis

Investigating the dynamic response of a punch to human head using finite element analysis Engineering Solid Mechanics 3 (2015) 177-186 Contents lists available at GrowingScience Engineering Solid Mechanics homepage: www.growingscience.com/esm Investigating the dynamic response of a punch to

More information

Skull Flexure from Blast Waves: A Mechanism for Brain Injury with Implications for Helmet Design *

Skull Flexure from Blast Waves: A Mechanism for Brain Injury with Implications for Helmet Design * LLNL-JRNL-412717 1 Skull Flexure from Blast Waves: A Mechanism for Brain Injury with Implications for Helmet Design * William C. Moss 1, Michael J. King 1, and Eric G. Blackman 2 1 Lawrence Livermore National

More information

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

Theory at a Glance (for IES, GATE, PSU) 1. Stress and Strain Theory at a Glance (for IES, GATE, PSU) 1.1 Stress () When a material is subjected to an external force, a resisting force is set up within the component. The internal resistance force

More information

1. A pure shear deformation is shown. The volume is unchanged. What is the strain tensor.

1. A pure shear deformation is shown. The volume is unchanged. What is the strain tensor. Elasticity Homework Problems 2014 Section 1. The Strain Tensor. 1. A pure shear deformation is shown. The volume is unchanged. What is the strain tensor. 2. Given a steel bar compressed with a deformation

More information

Nanoindentation of Fibrous Composite Microstructures: Experimentation and Finite Element Investigation. Mark Hardiman

Nanoindentation of Fibrous Composite Microstructures: Experimentation and Finite Element Investigation. Mark Hardiman Nanoindentation of Fibrous Composite Microstructures: Experimentation and Finite Element Investigation Mark Hardiman Materials and Surface Science Institute (MSSI), Department of Mechanical and Aeronautical

More information

Multiscale modeling and simulation of shock wave propagation

Multiscale modeling and simulation of shock wave propagation University of Iowa Iowa Research Online Theses and Dissertations Spring 2013 Multiscale modeling and simulation of shock wave propagation Cory Nelsen University of Iowa Copyright 2013 Cory Nelsen This

More information

Computational Analysis for Composites

Computational Analysis for Composites Computational Analysis for Composites Professor Johann Sienz and Dr. Tony Murmu Swansea University July, 011 The topics covered include: OUTLINE Overview of composites and their applications Micromechanics

More information

Microstructural Randomness and Scaling in Mechanics of Materials. Martin Ostoja-Starzewski. University of Illinois at Urbana-Champaign

Microstructural Randomness and Scaling in Mechanics of Materials. Martin Ostoja-Starzewski. University of Illinois at Urbana-Champaign Microstructural Randomness and Scaling in Mechanics of Materials Martin Ostoja-Starzewski University of Illinois at Urbana-Champaign Contents Preface ix 1. Randomness versus determinism ix 2. Randomness

More information

1 Introduction. This brief chapter introduces the subject of Solid Mechanics and the contents of this book

1 Introduction. This brief chapter introduces the subject of Solid Mechanics and the contents of this book 1 Introduction This brief chapter introduces the subject of Solid Mechanics and the contents of this book 1 2 Section 1.1 1.1 What is Solid Mechanics? Solid mechanics is the study of the deformation and

More information

S Kleiven. doi: /ijcr

S Kleiven. doi: /ijcr Evaluation of head injury criteria using a finite element model validated against experiments on localized brain motion, intracerebral acceleration, and intracranial pressure S Kleiven CTV Centre for Technology

More information

MICROMECHANICAL ANALYSIS OF FRP COMPOSITES SUBJECTED TO LONGITUDINAL LOADING

MICROMECHANICAL ANALYSIS OF FRP COMPOSITES SUBJECTED TO LONGITUDINAL LOADING MICROMECHANICAL ANALYSIS OF FRP COMPOSITES SUBJECTED TO LONGITUDINAL LOADING N. Krishna Vihari 1, P. Phani Prasanthi 1, V. Bala Krishna Murthy 2* and A. Srihari Prasad 3 1 Mech. Engg. Dept., P. V. P. Siddhartha

More information

An Atomistic-based Cohesive Zone Model for Quasi-continua

An Atomistic-based Cohesive Zone Model for Quasi-continua An Atomistic-based Cohesive Zone Model for Quasi-continua By Xiaowei Zeng and Shaofan Li Department of Civil and Environmental Engineering, University of California, Berkeley, CA94720, USA Extended Abstract

More information

ME 176 Final Exam, Fall 1997

ME 176 Final Exam, Fall 1997 Tuesday, December 16, 5:00 8:00 PM, 1997. Answer all questions for a maximum of 100 points. Please write all answers in the space provided. If you need additional space, write on the back sides. Indicate

More information

D : SOLID MECHANICS. Q. 1 Q. 9 carry one mark each. Q.1 Find the force (in kn) in the member BH of the truss shown.

D : SOLID MECHANICS. Q. 1 Q. 9 carry one mark each. Q.1 Find the force (in kn) in the member BH of the truss shown. D : SOLID MECHANICS Q. 1 Q. 9 carry one mark each. Q.1 Find the force (in kn) in the member BH of the truss shown. Q.2 Consider the forces of magnitude F acting on the sides of the regular hexagon having

More information

Chapter 1 Fluid Characteristics

Chapter 1 Fluid Characteristics Chapter 1 Fluid Characteristics 1.1 Introduction 1.1.1 Phases Solid increasing increasing spacing and intermolecular liquid latitude of cohesive Fluid gas (vapor) molecular force plasma motion 1.1.2 Fluidity

More information

Fatigue in osteoporotic human trabecular bone Comparison between genders

Fatigue in osteoporotic human trabecular bone Comparison between genders loading to the load corresponding to a normalized stress level (Δσ/E 0 ). Fatigue in osteoporotic human trabecular bone Comparison between genders André do Carmo Saraiva Abstract In the present work, the

More information

N o n l i n e a r M u l t i - S c a l e M o d e l i n g o f A e r o s p a c e C o m p o s i t e s M a t e r i a l s & S t r u c t u r e s

N o n l i n e a r M u l t i - S c a l e M o d e l i n g o f A e r o s p a c e C o m p o s i t e s M a t e r i a l s & S t r u c t u r e s N o n l i n e a r M u l t i - S c a l e M o d e l i n g o f A e r o s p a c e C o m p o s i t e s M a t e r i a l s & S t r u c t u r e s R o g e r A. A s s a k e r C E O, e - X s t r e a m e n g i n e

More information

Module 7: Micromechanics Lecture 34: Self Consistent, Mori -Tanaka and Halpin -Tsai Models. Introduction. The Lecture Contains. Self Consistent Method

Module 7: Micromechanics Lecture 34: Self Consistent, Mori -Tanaka and Halpin -Tsai Models. Introduction. The Lecture Contains. Self Consistent Method Introduction In this lecture we will introduce some more micromechanical methods to predict the effective properties of the composite. Here we will introduce expressions for the effective properties without

More information

Bending a slab of neural tissue

Bending a slab of neural tissue arxiv:q-bio/0510034v1 [q-bio.to] 17 Oct 2005 Bending a slab of neural tissue Partha P. Mitra Cold Spring Harbor Laboratory, NY 11724 March 2, 2008 Abstract In comparative and developmental neuroanatomy

More information

DIFFUSION MAGNETIC RESONANCE IMAGING

DIFFUSION MAGNETIC RESONANCE IMAGING DIFFUSION MAGNETIC RESONANCE IMAGING from spectroscopy to imaging apparent diffusion coefficient ADC-Map anisotropy diffusion tensor (imaging) DIFFUSION NMR - FROM SPECTROSCOPY TO IMAGING Combining Diffusion

More information

Injury tolerances for oblique impact helmet testing

Injury tolerances for oblique impact helmet testing 1 2 3 4 5 Injury tolerances for oblique impact helmet testing M Aare, S Kleiven and P Halldin Division of Neuronic Engineering, CTV Centre for Technology within Healthcare, Royal Institute of Technology

More information

Diffusion Tensor Imaging (DTI): An overview of key concepts

Diffusion Tensor Imaging (DTI): An overview of key concepts Diffusion Tensor Imaging (DTI): An overview of key concepts (Supplemental material for presentation) Prepared by: Nadia Barakat BMB 601 Chris Conklin Thursday, April 8 th 2010 Diffusion Concept [1,2]:

More information

EE 5344 Introduction to MEMS CHAPTER 6 Mechanical Sensors. 1. Position Displacement x, θ 2. Velocity, speed Kinematic

EE 5344 Introduction to MEMS CHAPTER 6 Mechanical Sensors. 1. Position Displacement x, θ 2. Velocity, speed Kinematic I. Mechanical Measurands: 1. Classification of main types: EE 5344 Introduction MEMS CHAPTER 6 Mechanical Sensors 1. Position Displacement x, θ. Velocity, speed Kinematic dx dθ v =, = ω 3. Acceleration

More information

Diffusion Tensor Imaging I: The basics. Jennifer Campbell

Diffusion Tensor Imaging I: The basics. Jennifer Campbell Diffusion Tensor Imaging I: The basics Jennifer Campbell Diffusion Tensor Imaging I: The basics Jennifer Campbell Diffusion Imaging MRI: many different sources of contrast T1W T2W PDW Perfusion BOLD DW

More information

Lectures on. Constitutive Modelling of Arteries. Ray Ogden

Lectures on. Constitutive Modelling of Arteries. Ray Ogden Lectures on Constitutive Modelling of Arteries Ray Ogden University of Aberdeen Xi an Jiaotong University April 2011 Overview of the Ingredients of Continuum Mechanics needed in Soft Tissue Biomechanics

More information

Mechanical Properties of Polymers. Scope. MSE 383, Unit 3-1. Joshua U. Otaigbe Iowa State University Materials Science & Engineering Dept.

Mechanical Properties of Polymers. Scope. MSE 383, Unit 3-1. Joshua U. Otaigbe Iowa State University Materials Science & Engineering Dept. Mechanical Properties of Polymers Scope MSE 383, Unit 3-1 Joshua U. Otaigbe Iowa State University Materials Science & Engineering Dept. Structure - mechanical properties relations Time-dependent mechanical

More information

Lecture 8 Viscoelasticity and Deformation

Lecture 8 Viscoelasticity and Deformation Read: pg 130 168 (rest of Chpt. 4) 1 Poisson s Ratio, µ (pg. 115) Ratio of the strain in the direction perpendicular to the applied force to the strain in the direction of the applied force. For uniaxial

More information

Mechanics PhD Preliminary Spring 2017

Mechanics PhD Preliminary Spring 2017 Mechanics PhD Preliminary Spring 2017 1. (10 points) Consider a body Ω that is assembled by gluing together two separate bodies along a flat interface. The normal vector to the interface is given by n

More information

Engineering Solid Mechanics

Engineering Solid Mechanics }} Engineering Solid Mechanics 1 (2013) 1-8 Contents lists available at GrowingScience Engineering Solid Mechanics homepage: www.growingscience.com/esm Impact damage simulation in elastic and viscoelastic

More information

Lecture 3. Properties of Fluids 11/01/2017. There are thermodynamic properties of fluids like:

Lecture 3. Properties of Fluids 11/01/2017. There are thermodynamic properties of fluids like: 11/01/2017 Lecture 3 Properties of Fluids There are thermodynamic properties of fluids like: Pressure, p (N/m 2 ) or [ML -1 T -2 ], Density, ρ (kg/m 3 ) or [ML -3 ], Specific weight, γ = ρg (N/m 3 ) or

More information

Simulation and Test Validation of Windscreen Subject to Pedestrian Head Impact

Simulation and Test Validation of Windscreen Subject to Pedestrian Head Impact 12 th International LS-DYNA Users Conference Occupant Safety Simulation and Test Validation of Windscreen Subject to Pedestrian Head Impact Qi Liu, Junyong Liu, Qiang Miao, Dazhi Wang, Xiaodong Tang SAIC

More information

Mechanics of Biomaterials

Mechanics of Biomaterials Mechanics of Biomaterials Lecture 7 Presented by Andrian Sue AMME498/998 Semester, 206 The University of Sydney Slide Mechanics Models The University of Sydney Slide 2 Last Week Using motion to find forces

More information

Supplementary Information: Nanoscale heterogeneity promotes energy dissipation in bone

Supplementary Information: Nanoscale heterogeneity promotes energy dissipation in bone Supplementary Information: Nanoscale heterogeneity promotes energy dissipation in bone KUANGSHIN TAI, * MING DAO, * SUBRA SURESH,, AHMET PALAZOGLU, & AND CHRISTINE ORTIZ Department of Materials Science

More information

N = Shear stress / Shear strain

N = Shear stress / Shear strain UNIT - I 1. What is meant by factor of safety? [A/M-15] It is the ratio between ultimate stress to the working stress. Factor of safety = Ultimate stress Permissible stress 2. Define Resilience. [A/M-15]

More information

International Journal of Scientific & Engineering Research Volume 8, Issue 12, December-2017 ISSN

International Journal of Scientific & Engineering Research Volume 8, Issue 12, December-2017 ISSN 362 Study of the Effects of Random Inclusions in Composite Construction with Isotropic Negative Poisson s Ratio [Kundan Singh Deshwal1, a and Dr. Satyendra Singh2, b] 1 Assistant Professor, Department

More information

Nonlinear Modeling of Fiber-Reinforced Elastomers and the Response of a Rubber Muscle Actuator

Nonlinear Modeling of Fiber-Reinforced Elastomers and the Response of a Rubber Muscle Actuator Nonlinear Modeling of Fiber-Reinforced Elastomers and the Response of a Rubber Muscle Actuator Larry D. Peel, Ph.D.* Department of Mechanical & Industrial Engineering Texas A&M Univ. - Kingsville David

More information

VISCOELASTIC PROPERTIES OF POLYMERS

VISCOELASTIC PROPERTIES OF POLYMERS VISCOELASTIC PROPERTIES OF POLYMERS John D. Ferry Professor of Chemistry University of Wisconsin THIRD EDITION JOHN WILEY & SONS New York Chichester Brisbane Toronto Singapore Contents 1. The Nature of

More information

Mechanics of Solids. Mechanics Of Solids. Suraj kr. Ray Department of Civil Engineering

Mechanics of Solids. Mechanics Of Solids. Suraj kr. Ray Department of Civil Engineering Mechanics Of Solids Suraj kr. Ray (surajjj2445@gmail.com) Department of Civil Engineering 1 Mechanics of Solids is a branch of applied mechanics that deals with the behaviour of solid bodies subjected

More information

Final Project: Indentation Simulation Mohak Patel ENGN-2340 Fall 13

Final Project: Indentation Simulation Mohak Patel ENGN-2340 Fall 13 Final Project: Indentation Simulation Mohak Patel ENGN-2340 Fall 13 Aim The project requires a simulation of rigid spherical indenter indenting into a flat block of viscoelastic material. The results from

More information

Strain Direct Mapping by Using Carbon Nanotube Strain Sensor

Strain Direct Mapping by Using Carbon Nanotube Strain Sensor TOMODACHI STEM @ Rice University FinalPresentation (March 18, 016) Strain Direct Mapping by Using Carbon Nanotube Strain Sensor Shuhei Yoshida (University of Tokyo) Supervisor: Professor Bruce Weisman

More information

Fluid Properties and Units

Fluid Properties and Units Fluid Properties and Units CVEN 311 Continuum Continuum All materials, solid or fluid, are composed of molecules discretely spread and in continuous motion. However, in dealing with fluid-flow flow relations

More information

ENGN2210 CONTINUUM MECHANICS

ENGN2210 CONTINUUM MECHANICS School of Engineering Brown University ENGN2210 CONTINUUM MECHANICS Allan Bower Fall 2016 What is continuum mechanics? Boeing Dreamliner Chevy Volt What is continuum mechanics? A continuum idealized form

More information

CHEM-C2410: Materials Science from Microstructures to Properties Composites: basic principles

CHEM-C2410: Materials Science from Microstructures to Properties Composites: basic principles CHEM-C2410: Materials Science from Microstructures to Properties Composites: basic principles Mark Hughes 14 th March 2017 Today s learning outcomes To understand the role of reinforcement, matrix and

More information

Numerical modeling of diffusion within composite media

Numerical modeling of diffusion within composite media Numerical modeling of diffusion within composite media Miljan Milosevic To cite this version: Miljan Milosevic. Numerical modeling of diffusion within composite media. 2nd ECCOMAS Young Investigators Conference

More information

Constitutive model of brain tissue suitable for finite element analysis of surgical procedures

Constitutive model of brain tissue suitable for finite element analysis of surgical procedures Journal of Biomechanics 32 (1999 531 537 Technical Note Constitutive model of brain tissue suitable for finite element analysis of surgical procedures Karol Miller* Department of Mechanical and Materials

More information

Design and Analysis of Various Microcantilever Shapes for MEMS Based Sensing

Design and Analysis of Various Microcantilever Shapes for MEMS Based Sensing ScieTech 014 Journal of Physics: Conference Series 495 (014) 01045 doi:10.1088/174-6596/495/1/01045 Design and Analysis of Various Microcantilever Shapes for MEMS Based Sensing H. F. Hawari, Y. Wahab,

More information

MEG 741 Energy and Variational Methods in Mechanics I

MEG 741 Energy and Variational Methods in Mechanics I MEG 741 Energy and Variational Methods in Mechanics I Brendan J. O Toole, Ph.D. Associate Professor of Mechanical Engineering Howard R. Hughes College of Engineering University of Nevada Las Vegas TBE

More information

Computer Modeling in Bioengineering

Computer Modeling in Bioengineering Computer Modeling in Bioengineering Theoretical Background, Examples and Software Milos Kojic Harvard School of Public Health, USA University of Kragujevac, Serbia University of Texas Health Science Center

More information

Copyright Warning & Restrictions

Copyright Warning & Restrictions Copyright Warning & Restrictions The copyright law of the United States (Title 17, United States Code) governs the making of photocopies or other reproductions of copyrighted material. Under certain conditions

More information

KINK BAND FORMATION OF FIBER REINFORCED POLYMER (FRP)

KINK BAND FORMATION OF FIBER REINFORCED POLYMER (FRP) KINK BAND FORMATION OF FIBER REINFORCED POLYMER (FRP) 1 University of Science & Technology Beijing, China, niukm@ustb.edu.cn 2 Tsinghua University, Department of Engineering Mechanics, Beijing, China,

More information

Elastic parameters prediction under dynamic loading based on the. unit cell of composites considering end constraint effect

Elastic parameters prediction under dynamic loading based on the. unit cell of composites considering end constraint effect Elastic parameters prediction under dynamic loading based on the unit cell of composites considering end constraint effect Wang Meng 1,, Fei Qingguo 1,, Zhang Peiwei 1, (1. Institute of Aerospace Machinery

More information

A FULLY COUPLED MULTISCALE SHELL FORMULATION FOR THE MODELLING OF FIBRE REINFORCED LAMINATES

A FULLY COUPLED MULTISCALE SHELL FORMULATION FOR THE MODELLING OF FIBRE REINFORCED LAMINATES ECCM-6 TH EUROPEAN CONFERENCE ON COMPOSITE MATERIALS, Seville, Spain, 22-26 June 24 A FULLY COUPLED MULTISCALE SHELL FORMULATION FOR THE MODELLING OF FIBRE REINFORCED LAMINATES J. Främby, J. Brouzoulis,

More information

Multiscale analyses of the behaviour and damage of composite materials

Multiscale analyses of the behaviour and damage of composite materials Multiscale analyses of the behaviour and damage of composite materials Presented by Didier BAPTISTE ENSAM, LIM, UMR CNRS 8006 151 boulevard de l hôpital l 75013 PARIS, France Research works from: K.Derrien,

More information

NMR Imaging in porous media

NMR Imaging in porous media NMR Imaging in porous media What does NMR give us. Chemical structure. Molecular structure. Interactions between atoms and molecules. Incoherent dynamics (fluctuation, rotation, diffusion). Coherent flow

More information

Measuring the anisotropy of the cerebrum in the linear regime

Measuring the anisotropy of the cerebrum in the linear regime Measuring the anisotropy of the cerebrum in the linear regime L. Tang MT 06.26 Coaches: Dr.Ir. J.A.W. van Dommelen Ing. M. Hrapko June 20, 2006 2 Abstract In this report the anisotropy is measured of the

More information

Name :. Roll No. :... Invigilator s Signature :.. CS/B.TECH (CE-NEW)/SEM-3/CE-301/ SOLID MECHANICS

Name :. Roll No. :... Invigilator s Signature :.. CS/B.TECH (CE-NEW)/SEM-3/CE-301/ SOLID MECHANICS Name :. Roll No. :..... Invigilator s Signature :.. 2011 SOLID MECHANICS Time Allotted : 3 Hours Full Marks : 70 The figures in the margin indicate full marks. Candidates are required to give their answers

More information

Finite Element Modeling of an Aluminum Tricycle Frame

Finite Element Modeling of an Aluminum Tricycle Frame Finite Element Modeling of an Aluminum Tricycle Frame A. Rodríguez, B. Chiné*, and J. A. Ramírez Costa Rica Institute of Technology, School of Materials Science and Engineering, Cartago, Costa Rica *Corresponding

More information

Experimentally Calibrating Cohesive Zone Models for Structural Automotive Adhesives

Experimentally Calibrating Cohesive Zone Models for Structural Automotive Adhesives Experimentally Calibrating Cohesive Zone Models for Structural Automotive Adhesives Mark Oliver October 19, 2016 Adhesives and Sealants Council Fall Convention contact@veryst.com www.veryst.com Outline

More information

Reducing effect of softball-to-head impact by incorporating slip-surface in helmet

Reducing effect of softball-to-head impact by incorporating slip-surface in helmet Available online at www.sciencedirect.com Procedia Engineering 13 (2011) 415 421 5 th Asia-Pacific Congress on Sports Technology (APCST) Reducing effect of softball-to-head impact by incorporating slip-surface

More information

An Anisotropic Material Model for Image Guided Neurosurgery

An Anisotropic Material Model for Image Guided Neurosurgery An Anisotropic Material Model for Image Guided Neurosurgery Corey A. Kemper 1, Ion-Florin Talos 2, Alexandra Golby 2, Peter M. Black 2, Ron Kikinis 2, W. Eric L. Grimson 1, and Simon K. Warfield 2 1 Massachusetts

More information