KIT – University of the State of Baden-Wuerttemberg and National Research Center of the Helmholtz Association Institute for Applied Materials (IAM-WBM)

Slides:



Advertisements
Similar presentations
Chap.8 Mechanical Behavior of Composite
Advertisements

Deformation of Sediments via Grain-Scale Simulations: Variational Algorithm Ran Holtzman, Dmitriy Silin, Tad Patzek U.C. Berkeley
Failure Phenomenon Simulation by MPS-DEM Geotechnical Structure Elastic behavior: MPS Failure: DEM.
Validation of the plasticity models introduction of hardening laws
1 Volpe The National Transportation Systems Center Finite Element Analysis of Wood and Concrete Crossties Subjected to Direct Rail Seat Pressure U.S. Department.
Constitutive Equations CASA Seminar Wednesday 19 April 2006 Godwin Kakuba.
Multi-Physics Numerical Modeling and Experimental Characterization of Materials Vincent Y. Blouin Assistant Professor Materials Science and Engineering.
Elasticity by Ibrhim AlMohimeed
Chapter 3 Mechanical Properties of Materials
November 14, 2013 Mechanical Engineering Tribology Laboratory (METL) Benjamin Leonard Post-Doctoral Research Associate Third Body Modeling Using a Combined.
University of Minho School of Engineering Territory, Environment and Construction Centre (C-TAC) Uma Escola a Reinventar o Futuro – Semana da Escola de.
Soil Physics 2010 Outline Announcements Basic rheology Soil strength Triaxial test.
KIT – University of the State of Baden-Wuerttemberg and National Research Center of the Helmholtz Association M.H.H. Kolb, R. Knitter INSTITUTE FOR APPLIED.
Institute for Mechanics of Materials and Structures Vienna University of Technology Prediction of the early-age strength evolution of cement paste and.
Measuring segregation of inertial particles in turbulent flows by a Full Lagrangian approach E. Meneguz Ph.D. project: Rain in a box of turbulence Supervisor:
Modeling Static Friction of Rubber-Metal Contact
Introduction. Outline Fluid Mechanics in Chemical and Petroleum Engineering Normal Stresses (Tensile and Compressive) Shear stress General Concepts of.
Failure Theories Why do parts fail? What kind of stresses?
Mechanics of Materials II
Critical Scaling at the Jamming Transition Peter Olsson, Umeå University Stephen Teitel, University of Rochester Supported by: US Department of Energy.
BFC (Mechanics of Materials) Chapter 5: Compression Member
Critical Scaling at the Jamming Transition Peter Olsson, Umeå University Stephen Teitel, University of Rochester Supported by: US Department of Energy.
Lecture 26: Mechanical Properties I: Metals & Ceramics
Mechanics of Materials II
University of Stuttgart Institute of Construction Materials (IWB) 1/34 Discrete Bond Element for 3D Finite Element Analysis of RC Structures Steffen Lettow.
Lecture-8 Shear Strength of Soils
Current status and outlook of thermomechanics research and development for blanket pebble beds Jon Van Lew Ph.D. Student UCLA Fusion Science and Technology.
By Paul Delgado Advisor – Dr. Vinod Kumar Co-Advisor – Dr. Son Young Yi.
Vacuum, Surfaces & Coatings Group Technology Department Glassy Carbon Tests at HiRadMat 14 March 2014 C. Garion2 Outline: Introduction Context: Transparent.
P.B. Flemings (1), I. Song (2,3) and D.M. Saffer (3) (1) Jackson School of Geosciences, University of Texas, Austin, USA (2) Korea Institute of Geoscience.
Mechanical Properties
Random Finite Element Modeling of thermomechanical behavior of AGR bricks Jose David Arregui Mena, Louise Lever, Graham Hall, Lee Margetts, Paul Mummery.
Mechanical Properties
0 Laser Flash Method for Effective Thermal Diffusivity Measurement of Pebble Beds CBBI-16 Portland, OR, USA Sept. 9, 2011 Mu-Young Ahn 1, Duck Young Ku.
MODELLING THE PULLOUT OF HOOKED STEEL FIBERS FROM CEMENTITIOUS MATRIX Edmunds Zīle, Olga Zīle Institute of Polymer Mechanics Riga, Latvia.
November 14, 2013 Mechanical Engineering Tribology Laboratory (METL) Arnab Ghosh Ph.D. Research Assistant Analytical Modeling of Surface and Subsurface.
Class #1.2 Civil Engineering Materials – CIVE 2110
MAE 343-Intermediate Mechanics of Materials QUIZ No.1 - Thursday, Aug. 26, 2004 List three possible failure modes of a machine element (5points) List the.
Bilinear Isotropic Hardening Behavior MAE 5700 Final Project Raghavendar Ranganathan Bradly Verdant Ranny Zhao.
Lecture 8 – Viscoelasticity and Deformation
The Kinetic Theory of Gases Temperature as a measure of average kinetic energy of the particles.
Manufacturing process II. Sándor Pálinkás Ph. D
Numerical analysis of Concrete Face Rockfill Dams based on Lade’s model and gradient plasticity P. Dakoulas, E. Stavrotheodorou, A. Giannakopoulos University.
WEAR. Wear –Quantitative Measurement of Wear: A general description of adhesive wear is given by V = (kPx/3H), Where V is the volume of material worn.
DR KAFEEL AHMED Mechanical Behaviour Stress Strain Behaviour of Mild Steel.
Kinetic Molecular Theory Images taken from
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.
STRUCTURES Young’s Modulus. Tests There are 4 tests that you can do to a material There are 4 tests that you can do to a material 1 tensile This is where.
Topic 3: Constitutive Properties of Tissues
Today, we will study data obtained using three techniques: Micropipette aspiration Force range: 10 pN – 1000 nN soft cells hard cells Optical tweezers.
Capturing Size Effect in Unidirectional Fiber Composites Employing Stochastic Finite Element Simulations By Thomas Bilodeau Advisor: Dr. Fertig May 2,
SETTLEMENT ANALYSIS By: Engr. Hammad Akbar. Contents 1. Definition 2. Types & Modes of settlements 3. Primary and secondary consolidation settlements.
PLASTIC ANALYSIS OF BEAMS - SANDEEP DIGAVALLI. AT A GLANCE OF THIS TOPIC  BASIS OF PLASTIC THEORY  STRESS-STRAIN CURVE OF PLASTIC MATERIALS  STRESSES.
From: A Numerical Investigation Into Cold Spray Bonding Processes
APPLICATION OF COHESIVE ELEMENT TO BIMATERIAL INTERFACE
Continuum Mechanics (MTH487)
EML 4930/5930 Advanced Materials
Results and Discussion
“Hard to Deform” Grain Interior
Lecture 9 – Deformation and Damage
Lab #1 due TODAY!!!!!  HW#5 due Wednesday, 2/11
Lecture 8 Announcements
Volume 107, Issue 11, Pages (December 2014)
Lecture 8 – Viscoelasticity and Deformation
Lecture 9 – Deformation and Damage
Lecture 8 – Deformation and Damage
Lecture 9 – Deformation and Damage
Volume 107, Issue 11, Pages (December 2014)
Chap 11 Gas laws.
B. RISCOB et al., Institute for Plasma Research
Presentation transcript:

KIT – University of the State of Baden-Wuerttemberg and National Research Center of the Helmholtz Association Institute for Applied Materials (IAM-WBM) Crushing Analysis of Pebbles in a Pebble Assembly using DEM Ratna Kumar Annabattula, Shuo Zhao, Yixiang Gan and Marc Kamlah

CBBI-16 Meeting, Portland, OR, USA 8-10 September /09/11 Ratna Kumar Annabattula, Karlsruhe Institute of Technology Outline Introduction Model Results Summary Outlook

CBBI-16 Meeting, Portland, OR, USA 8-10 September /09/11 Ratna Kumar Annabattula, Karlsruhe Institute of Technology Introduction Pebble Assembly and Pebble-Pebble Interactions Assumptions: Pebble shape: spherical Pebble size: uniform, r s = r g = 0.25 mm Y. Gan et. Al, JMPS 2010 Idealizations: A unit cell of interest from a large assembly Periodic boundary conditions

CBBI-16 Meeting, Portland, OR, USA 8-10 September /09/11 Ratna Kumar Annabattula, Karlsruhe Institute of Technology Introduction Crush tests on single Li 2 SiO 4 pebbles F c – Crush load F u F Fitting Parameters m The fit parameters depend on plate material Phd Thesis, ShuoZhao, 2010 and FML at KIT Different contact states

CBBI-16 Meeting, Portland, OR, USA 8-10 September /09/11 Ratna Kumar Annabattula, Karlsruhe Institute of Technology Introduction Failure criterion for Osi Pebbles Failure criterion based on maximum stress in the pebble. Failure criterion based on the energy absorbed by the pebble. Failure criterion based on maximum stress in the pebble. Failure criterion based on the energy absorbed by the pebble. Phd Thesis, ShuoZhao, 2010 These parameters depend on the plate material

CBBI-16 Meeting, Portland, OR, USA 8-10 September /09/11 Ratna Kumar Annabattula, Karlsruhe Institute of Technology Model Macroscopic Average Stress Average normal contact force ( f ave ) and hydrostatic pressure ( p ) An assembly of 5000 pebbles in a box with periodic boundary conditions. Uni-axial compression to 3% strain and then unloading to stress-free state.

CBBI-16 Meeting, Portland, OR, USA 8-10 September /09/11 Ratna Kumar Annabattula, Karlsruhe Institute of Technology Model Damage Criterion and simulation flow chart Φ: Stored elastic energy Φ cr : Critical failure energy D: Damage variable E = (1-D)*E 0, if E >= 1 kPa E = 1 kPa if E < 1 kPa

CBBI-16 Meeting, Portland, OR, USA 8-10 September /09/11 Ratna Kumar Annabattula, Karlsruhe Institute of Technology Results Damaged Pebbles ε 33 = 0% ε 33 = 1.65 % ε 33 = 3 % No Damage Localization

CBBI-16 Meeting, Portland, OR, USA 8-10 September /09/11 Ratna Kumar Annabattula, Karlsruhe Institute of Technology Results Stress-Strain Response Effect of packing factorEffect of damage criterion

CBBI-16 Meeting, Portland, OR, USA 8-10 September /09/11 Ratna Kumar Annabattula, Karlsruhe Institute of Technology Results Damaged Pebbles Effect of random energy distribution Effect of packing factorEffect of damage criterion

CBBI-16 Meeting, Portland, OR, USA 8-10 September /09/11 Ratna Kumar Annabattula, Karlsruhe Institute of Technology Results Damaged Pebles: Effect of damage law

CBBI-16 Meeting, Portland, OR, USA 8-10 September /09/11 Ratna Kumar Annabattula, Karlsruhe Institute of Technology Results Damage Histograms: Effect of packing factor

CBBI-16 Meeting, Portland, OR, USA 8-10 September /09/11 Ratna Kumar Annabattula, Karlsruhe Institute of Technology Summary Crushing analysis of pebbles in the frame work of damage mechanics A mere 0.2% of failed pebbles in the assembly ceases the further load carrying capacity of the assembly. An assembly with high packing factor is prone to more total damage. A sudden damage law exhibits a higher flow stress than gradual damage. The fraction of critical pebbles to failure is independent of damage accumulation law. The stress plateau after the critical number of failed pebbles indicate a creep like behavior.

CBBI-16 Meeting, Portland, OR, USA 8-10 September /09/11 Ratna Kumar Annabattula, Karlsruhe Institute of Technology Outlook Implementation of pebble failure into small particles. The present damage law is heuristic and a damage law with a physical basis based on experiments to be developed. Extend the analysis to polydisperse pebble assembly.

CBBI-16 Meeting, Portland, OR, USA 8-10 September /09/11 Acknowledgments Regina Knitter for Pebbles and Crush load data. European Fusion Development Agreement (EFDA) for funding. Ratna Kumar Annabattula, Karlsruhe Institute of Technology

CBBI-16 Meeting, Portland, OR, USA 8-10 September /09/11 Ratna Kumar Annabattula, Karlsruhe Institute of Technology Thank you for your attention! Questions?

CBBI-16 Meeting, Portland, OR, USA 8-10 September /09/11 Backup slides Ratna Kumar Annabattula, Karlsruhe Institute of Technology

CBBI-16 Meeting, Portland, OR, USA 8-10 September /09/11 Backup Slides Ratna Kumar Annabattula, Karlsruhe Institute of Technology