Modeling Flow and Deformation during Salt- Assisted Puffing of Single Rice Kernels. Tushar Gulati Cornell University 1

Size: px
Start display at page:

Download "Modeling Flow and Deformation during Salt- Assisted Puffing of Single Rice Kernels. Tushar Gulati Cornell University 1"

Transcription

1 Modeling Flow and Deformation during Salt- Assisted Puffing of Single Rice Kernels Tushar Gulati Cornell University 1

2 Puffing 2

3 Puffing: Salient Features Quick process and a complex interplay of mass, momentum and energy transport with Large Deformations Rapid evaporation of water to vapor Phase Transition from Glassy (brittle) to Rubbery (ductile) state Large volumetric expansion of the kernel due to Gas Pressure generation and Phase Transition Large Plastic (inelastic) deformation of the material 3

4 Transport Process in Deformable Porous Media E = EMT (, ) p f Multiphase, multicomponent transport Poromechanics, phase dependent properties ni,g = ni,s +c i vs,g 4

5 Transport Process Porous Media 1,2,3 Water bulk flow/convection capillary diffusion phase change Solid Porous material 1 Whitaker (1997) 2 Ni H et al., (1999) 3 Halder A et al., (2007) Gas (Vapor + Air) bulk flow binary diffusion phase change Element 5

6 Transport Process Porous Media Momentum Conservation Darcy Law c g t ( n g,g ) + = I kk = P g rg, n g,s ρg µ g v i kk i ri, = µ i P Darcy Velocity i = water, gas Mass Conservation Liquid Water phase change Water Vapor phase change bulk flow capillary flow bulk flow binary diffusion Energy Conservation Phase Change Thermal Balance for Mixture phase change Evaporation-Condensation convection conduction microwave source Non-Equilibrium Formulation 6

7 Deformation in Porous Media: Poromechanics 1,2,3 Average Stress in REV Porous material Stress due to solid skeleton σ = σ ' p I Balance of Linear Momentum: f Stress due to fluids inside pore σ ' = p Constitutive Model for the Solid Skeleton: f σ ' Solid ( D ε) = p f Gas p f Liquid pf = Sgpg + Swpw Elasto-Plastic 1 Perre & May (2001) 2 Kowalski (2000) 3 Coussy (2004) 7

8 Phase Transition Glassy Rubbery Textural Attributes Porosity & Bulk Density 10 7 Hard & rigid Modulus Glass Transition Soft & compliant Volume Shrinkage/Expansion Temperature/Moisture Stress Cracking 1 Roos, Y.H. (2010) 8

9 Puffing: Modeling Framework Salt-Assisted Puffing carried out at C for 15s Multiphase transport (Gas Pressure Driven) Large Deformations (Elastic, Perfectly-Plastic Material) Prediction of Key Quality Attributes Porosity Microstructure Volumetric Expansion Driving force of deformation: Expansion is driven by gas pressure gradients only, shrinkage due to moisture loss is neglected 9

10 Puffing: Mechanical Properties Temperature (K) 10 Hard & rigid Young s Modulus Mechanical Property Glass Transition Poisson s ratio

11 Model implementation Geometry & Boundary Conditions Numerical Solution using COMSOL 4.3b Rice kernel as prolate spheroid A highly-non linear coupled multi-physics problem, convergence issues 2D Axisymmetric b a Forced Convection Heat Transfer Moisture Loss through Evaporation Free Surfaces for Deformation a = 0.5 x 10-4 m b = 5.75 x 10-4 m No axial displacement Insulated for Energy and Moisture transfer Mesh inverts and leads to convergence problems Large strain plasticity adds additional level of numerical challenge, Need to play extensively with default solver features of the software

12 Puffing: Model validation Convective losses Moisture Content Moisture lost primarily by evaporation Volume Ratio Expansion due to Glass Transition and Evaporation Material is Glassy Dimension Changes Major Axis Minor Axis Expansion is more along the tip 12

13 Puffing: Actual and Simulated Expansion Actual volume expansion 0 s 3 s 6 s 9 s 12 s 15 s Simulated volume expansion 0 s 3 s 6 s 9 s 12 s 15 s 13

14 Puffing: Porosity and Microstructure Development Experiment 0.74 Model s 3 s 6 s 9 s 12 s 15 s 14

15 Puffing: Simulated Process Temperature Bulk Modulus Pressure Plastic Deformation 15

16 Puffing: Expansion Ratio as a Quality Parameter Salt preconditioning is done to increase volumetric expansion Addition of salt: Decreases the Glass Transition Temperature of the material Increases expansion ratio by at least 15% (found experimentally) Volume Expansion With salt Without salt 20% more predicted expansion Puffing time (s) 16

17 Puffing: Summary & Potential Applications Physics: High temperatures cause rapid evaporation of water generating large gas pressures within and, Rubbery-Glassy Phase Transition of the material. Key Observations: Rice puffs from the tip where it Glass Transitions. The expansion front moves inwards eventually causing the entire kernel to puff. Pore formation follows a similar trend Process Optimization: Salt preconditioning increases the expansion ratio of the kernel Model Extension: Other puffing type processes using hot oil, gun puffing, extrusion and microwave puffing. Starch based-foamed plastics in the chemical process industry 17

18 Acknowledgements USDA Grants Prof. Ashim Datta Prof. Alan Zehnder Prof. Shefford Baker Alex Warning Huacheng Zhu Peyman Taherkhani Porawon Nitjarunkul Dr. Swati Kadam 18

19 Thank You 19

Coupled Electromagnetics- Multiphase Porous Media Model for Microwave Combination Heating

Coupled Electromagnetics- Multiphase Porous Media Model for Microwave Combination Heating Presented at the COMSOL Conference 2008 Boston Coupled Electromagnetics- Multiphase Porous Media Model for Microwave Combination Heating Vineet Rakesh and Ashim Datta Biological & Environmental Engineering

More information

Thermal properties of Engineering Materials

Thermal properties of Engineering Materials Thermal properties of Engineering Materials Engineering materials are important in everyday life because of their versatile structural properties. Other than these properties, they do play an important

More information

Game Physics. Game and Media Technology Master Program - Utrecht University. Dr. Nicolas Pronost

Game Physics. Game and Media Technology Master Program - Utrecht University. Dr. Nicolas Pronost Game and Media Technology Master Program - Utrecht University Dr. Nicolas Pronost Soft body physics Soft bodies In reality, objects are not purely rigid for some it is a good approximation but if you hit

More information

I. Borsi. EMS SCHOOL ON INDUSTRIAL MATHEMATICS Bedlewo, October 11 18, 2010

I. Borsi. EMS SCHOOL ON INDUSTRIAL MATHEMATICS Bedlewo, October 11 18, 2010 : an : an (Joint work with A. Fasano) Dipartimento di Matematica U. Dini, Università di Firenze (Italy) borsi@math.unifi.it http://web.math.unifi.it/users/borsi porous EMS SCHOOL ON INDUSTRIAL MATHEMATICS

More information

Localization in Undrained Deformation

Localization in Undrained Deformation Localization in Undrained Deformation J. W. Rudnicki Dept. of Civil and Env. Engn. and Dept. of Mech. Engn. Northwestern University Evanston, IL 621-319 John.Rudnicki@gmail.com Fourth Biot Conference on

More information

Elmer :Heat transfert with phase change solid-solid in transient problem Application to silicon properties. SIF file : phasechange solid-solid

Elmer :Heat transfert with phase change solid-solid in transient problem Application to silicon properties. SIF file : phasechange solid-solid Elmer :Heat transfert with phase change solid-solid in transient problem Application to silicon properties 3 6 1. Tb=1750 [K] 2 & 5. q=-10000 [W/m²] 0,1 1 Ω1 4 Ω2 7 3 & 6. α=15 [W/(m²K)] Text=300 [K] 4.

More information

Mechanics of Earthquakes and Faulting

Mechanics of Earthquakes and Faulting Mechanics of Earthquakes and Faulting www.geosc.psu.edu/courses/geosc508 Standard Solids and Fracture Fluids: Mechanical, Chemical Effects Effective Stress Dilatancy Hardening and Stability Mead, 1925

More information

Finite Element Method in Geotechnical Engineering

Finite Element Method in Geotechnical Engineering Finite Element Method in Geotechnical Engineering Short Course on + Dynamics Boulder, Colorado January 5-8, 2004 Stein Sture Professor of Civil Engineering University of Colorado at Boulder Contents Steps

More information

20. Rheology & Linear Elasticity

20. Rheology & Linear Elasticity I Main Topics A Rheology: Macroscopic deformation behavior B Linear elasticity for homogeneous isotropic materials 10/29/18 GG303 1 Viscous (fluid) Behavior http://manoa.hawaii.edu/graduate/content/slide-lava

More information

Soft Bodies. Good approximation for hard ones. approximation breaks when objects break, or deform. Generalization: soft (deformable) bodies

Soft Bodies. Good approximation for hard ones. approximation breaks when objects break, or deform. Generalization: soft (deformable) bodies Soft-Body Physics Soft Bodies Realistic objects are not purely rigid. Good approximation for hard ones. approximation breaks when objects break, or deform. Generalization: soft (deformable) bodies Deformed

More information

Module 5: Failure Criteria of Rock and Rock masses. Contents Hydrostatic compression Deviatoric compression

Module 5: Failure Criteria of Rock and Rock masses. Contents Hydrostatic compression Deviatoric compression FAILURE CRITERIA OF ROCK AND ROCK MASSES Contents 5.1 Failure in rocks 5.1.1 Hydrostatic compression 5.1.2 Deviatoric compression 5.1.3 Effect of confining pressure 5.2 Failure modes in rocks 5.3 Complete

More information

Impact Simulation of Extreme Wind Generated Missiles on Radioactive Waste Storage Facilities

Impact Simulation of Extreme Wind Generated Missiles on Radioactive Waste Storage Facilities Impact Simulation of Extreme Wind Generated Missiles on Radioactive Waste Storage Facilities Gianluca Barbella Sogin S.p.A. Structural Design Department barbella@sogin.it Rotterdam - october 24, 2013 Outline

More information

Frequently Asked Questions

Frequently Asked Questions Frequently Asked Questions Why do we have to make the assumption that plane sections plane? How about bars with non-axis symmetric cross section? The formulae derived look very similar to beam and axial

More information

TIME-DEPENDENT BEHAVIOR OF PILE UNDER LATERAL LOAD USING THE BOUNDING SURFACE MODEL

TIME-DEPENDENT BEHAVIOR OF PILE UNDER LATERAL LOAD USING THE BOUNDING SURFACE MODEL TIME-DEPENDENT BEHAVIOR OF PILE UNDER LATERAL LOAD USING THE BOUNDING SURFACE MODEL Qassun S. Mohammed Shafiqu and Maarib M. Ahmed Al-Sammaraey Department of Civil Engineering, Nahrain University, Iraq

More information

Flow and Transport. c(s, t)s ds,

Flow and Transport. c(s, t)s ds, Flow and Transport 1. The Transport Equation We shall describe the transport of a dissolved chemical by water that is traveling with uniform velocity ν through a long thin tube G with uniform cross section

More information

MULTIPHASE TRANSPORT IN DEFORMABLE PHASE-CHANGING POROUS MATERIALS

MULTIPHASE TRANSPORT IN DEFORMABLE PHASE-CHANGING POROUS MATERIALS MULTIPHASE TRANSPORT IN DEFORMABLE PHASE-CHANGING POROUS MATERIALS A Dissertation Presented to the Faculty of the Graduate School of Cornell University in Partial Fulfillment of the Requirements for the

More information

Again we will consider the following one dimensional slab of porous material:

Again we will consider the following one dimensional slab of porous material: page 1 of 7 REVIEW OF BASIC STEPS IN DERIVATION OF FLOW EQUATIONS Generally speaking, flow equations for flow in porous materials are based on a set of mass, momentum and energy conservation equations,

More information

Research Article Nonequilibrium Thermal Dynamic Modeling of Porous Medium Vacuum Drying Process

Research Article Nonequilibrium Thermal Dynamic Modeling of Porous Medium Vacuum Drying Process Mathematical Problems in Engineering Volume, Article ID 347598, pages doi:5//347598 Research Article Nonequilibrium Thermal Dynamic Modeling of Porous Medium Vacuum Drying Process Zhijun Zhang and Ninghua

More information

Geology 229 Engineering Geology. Lecture 5. Engineering Properties of Rocks (West, Ch. 6)

Geology 229 Engineering Geology. Lecture 5. Engineering Properties of Rocks (West, Ch. 6) Geology 229 Engineering Geology Lecture 5 Engineering Properties of Rocks (West, Ch. 6) Common mechanic properties: Density; Elastic properties: - elastic modulii Outline of this Lecture 1. Uniaxial rock

More information

Sand Control Rock Failure

Sand Control Rock Failure Sand Control Rock Failure Why? A bit of Mechanics on rock failure How? Some choices that depend on the rock What is moving? Sand grains? Fines? 3/14/2009 1 Young s Modulus, E Young s Modulus is a material

More information

Salt Crystallization in Hydrophobic Porous Materials

Salt Crystallization in Hydrophobic Porous Materials Hydrophobe V 5 th International Conference on Water Repellent Treatment of Building Materials Aedificatio Publishers, 97-16 (28) Salt Crystallization in Hydrophobic Porous Materials H. Derluyn 1, A.S.

More information

2. Modeling of shrinkage during first drying period

2. Modeling of shrinkage during first drying period 2. Modeling of shrinkage during first drying period In this chapter we propose and develop a mathematical model of to describe nonuniform shrinkage of porous medium during drying starting with several

More information

Mathematical Modeling of Oil Shale Pyrolysis

Mathematical Modeling of Oil Shale Pyrolysis October, 19 th, 2011 Mathematical Modeling of Oil Shale Pyrolysis Pankaj Tiwari Jacob Bauman Milind Deo Department of Chemical Engineering University of Utah, Salt Lake City, Utah http://from50000feet.wordpress.com

More information

Supplementary Figure 1 Extracting process of wetting ridge profiles. a1-4, An extraction example of a ridge profile for E 16 kpa.

Supplementary Figure 1 Extracting process of wetting ridge profiles. a1-4, An extraction example of a ridge profile for E 16 kpa. Supplementary Figure 1 Extracting process of wetting ridge profiles. a1-4, An extraction example of a ridge profile for E 16 kpa. An original image (a1) was binarized, as shown in a2, by Canny edge detector

More information

Click to add title. Continuum mechanics of two-phase porous media

Click to add title. Continuum mechanics of two-phase porous media Click to add title Continuum mechanics of two-phase porous media Ragnar Larsson Division of Material and Computational Mechanics Department of Applied Mechanics Chalmers University of Technology S-412

More information

The Finite Element Method II

The Finite Element Method II [ 1 The Finite Element Method II Non-Linear finite element Use of Constitutive Relations Xinghong LIU Phd student 02.11.2007 [ 2 Finite element equilibrium equations: kinematic variables Displacement Strain-displacement

More information

3D simulations of an injection test done into an unsaturated porous and fractured limestone

3D simulations of an injection test done into an unsaturated porous and fractured limestone 3D simulations of an injection test done into an unsaturated porous and fractured limestone A. Thoraval *, Y. Guglielmi, F. Cappa INERIS, Ecole des Mines de Nancy, FRANCE *Corresponding author: Ecole des

More information

Lecture 8: Tissue Mechanics

Lecture 8: Tissue Mechanics Computational Biology Group (CoBi), D-BSSE, ETHZ Lecture 8: Tissue Mechanics Prof Dagmar Iber, PhD DPhil MSc Computational Biology 2015/16 7. Mai 2016 2 / 57 Contents 1 Introduction to Elastic Materials

More information

Finite Element Analysis of Permeation Tests on Articular Cartilage under Different Testing Conditions Using COMSOL Multiphysics.

Finite Element Analysis of Permeation Tests on Articular Cartilage under Different Testing Conditions Using COMSOL Multiphysics. Excerpt from the Proceedings of the COMSOL Conference 2010 Paris Finite Element Analysis of Permeation Tests on Articular Cartilage under Different Testing Conditions Using COMSOL Multiphysics. Grazia

More information

An Introduction to COMSOL Multiphysics v4.3b & Subsurface Flow Simulation. Ahsan Munir, PhD Tom Spirka, PhD

An Introduction to COMSOL Multiphysics v4.3b & Subsurface Flow Simulation. Ahsan Munir, PhD Tom Spirka, PhD An Introduction to COMSOL Multiphysics v4.3b & Subsurface Flow Simulation Ahsan Munir, PhD Tom Spirka, PhD Agenda Provide an overview of COMSOL 4.3b Our products, solutions and applications Subsurface

More information

Coalbed Methane Properties

Coalbed Methane Properties Coalbed Methane Properties Subtopics: Permeability-Pressure Relationship Coal Compressibility Matrix Shrinkage Seidle and Huitt Palmer and Mansoori Shi and Durucan Constant Exponent Permeability Incline

More information

Juan E. Santos a,b,c, Gabriela B. Savioli a and Robiel Martínez Corredor c a

Juan E. Santos a,b,c, Gabriela B. Savioli a and Robiel Martínez Corredor c a Juan E. Santos a,b,c, Gabriela B. Savioli a and Robiel Martínez Corredor c a Universidad de Buenos Aires, Fac. Ing., IGPUBA, ARGENTINA b Department of Mathematics, Purdue University, USA c Universidad

More information

Numerical Simulation of ES-SAGD Process in Athabasca Oil Sands with Top Water and Gas Thief Zones. Presented by Xia Bao

Numerical Simulation of ES-SAGD Process in Athabasca Oil Sands with Top Water and Gas Thief Zones. Presented by Xia Bao Numerical Simulation of ES-SAGD Process in Athabasca Oil Sands with Top Water and Gas Thief Zones Presented by Xia Bao 1 Outline Thermal simulation Optimization on the operating strategy ES-SAGD possibility

More information

Diffusion and Adsorption in porous media. Ali Ahmadpour Chemical Eng. Dept. Ferdowsi University of Mashhad

Diffusion and Adsorption in porous media. Ali Ahmadpour Chemical Eng. Dept. Ferdowsi University of Mashhad Diffusion and Adsorption in porous media Ali Ahmadpour Chemical Eng. Dept. Ferdowsi University of Mashhad Contents Introduction Devices used to Measure Diffusion in Porous Solids Modes of transport in

More information

Modeling as a tool for understanding the MEA. Henrik Ekström Utö Summer School, June 22 nd 2010

Modeling as a tool for understanding the MEA. Henrik Ekström Utö Summer School, June 22 nd 2010 Modeling as a tool for understanding the MEA Henrik Ekström Utö Summer School, June 22 nd 2010 COMSOL Multiphysics and Electrochemistry Modeling The software is based on the finite element method A number

More information

Mechanical properties of polymers: an overview. Suryasarathi Bose Dept. of Materials Engineering, IISc, Bangalore

Mechanical properties of polymers: an overview. Suryasarathi Bose Dept. of Materials Engineering, IISc, Bangalore Mechanical properties of polymers: an overview Suryasarathi Bose Dept. of Materials Engineering, IISc, Bangalore UGC-NRCM Summer School on Mechanical Property Characterization- June 2012 Overview of polymer

More information

Chapter 7. Highlights:

Chapter 7. Highlights: Chapter 7 Highlights: 1. Understand the basic concepts of engineering stress and strain, yield strength, tensile strength, Young's(elastic) modulus, ductility, toughness, resilience, true stress and true

More information

Drying shrinkage of deformable porous media: mechanisms induced by the fluid removal

Drying shrinkage of deformable porous media: mechanisms induced by the fluid removal Drying shrinkage of deformable porous media: mechanisms induced by the fluid removal L.B. Hu 1, H. Péron 2, T. Hueckel 1 and L. Laloui 2 1 Department of Civil and Environmental Engineering, Duke University,

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

OCR Physics Specification A - H156/H556

OCR Physics Specification A - H156/H556 OCR Physics Specification A - H156/H556 Module 3: Forces and Motion You should be able to demonstrate and show your understanding of: 3.1 Motion Displacement, instantaneous speed, average speed, velocity

More information

Enabling Technologies

Enabling Technologies Enabling Technologies Mechanical Modelling 1 Key Parameter Mineral System Exploration is reflected in scale-dependent translation A. Gradient in hydraulic potential B. Permeability C. Solubility sensitivity

More information

Modeling the Effect of Headspace Steam on Microwave Heating Performance of Mashed Potato

Modeling the Effect of Headspace Steam on Microwave Heating Performance of Mashed Potato Modeling the Effect of Headspace Steam on Microwave Heating Performance of Mashed Potato J. Chen, K. Pitchai, D. Jones, J. Subbiah University of Nebraska Lincoln October 9 th, 2014 Session : Electromagnetic

More information

D-MAVT Membrane Separation Processes

D-MAVT Membrane Separation Processes Membrane Separation Processes Federico Milella Rate Controlled Separation - Autumn 2017 Separation Processes Laboratory - Institute of Process Engineering Agenda Introduction Mass balances over a membrane

More information

Cellular solid structures with unbounded thermal expansion. Roderic Lakes. Journal of Materials Science Letters, 15, (1996).

Cellular solid structures with unbounded thermal expansion. Roderic Lakes. Journal of Materials Science Letters, 15, (1996). 1 Cellular solid structures with unbounded thermal expansion Roderic Lakes Journal of Materials Science Letters, 15, 475-477 (1996). Abstract Material microstructures are presented which can exhibit coefficients

More information

A thermo-hydro-mechanically coupled analysis of clay using a thermo-elasto-viscoplastic model

A thermo-hydro-mechanically coupled analysis of clay using a thermo-elasto-viscoplastic model JHUWS05 A thermo-hydro-mechanically coupled analysis of clay using a thermo-elasto-viscoplastic model by F. Oka, S. Kimoto, Y.-S. Kim, N. Takada Department of Civil & Earth Resources Engineering, Kyoto

More information

Fluid Flow Fluid Flow and Permeability

Fluid Flow Fluid Flow and Permeability and Permeability 215 Viscosity describes the shear stresses that develop in a flowing fluid. V z Stationary Fluid Velocity Profile x Shear stress in the fluid is proportional to the fluid velocity gradient.

More information

Calculation types: drained, undrained and fully coupled material behavior. Dr Francesca Ceccato

Calculation types: drained, undrained and fully coupled material behavior. Dr Francesca Ceccato Calculation types: drained, undrained and fully coupled material behavior Dr Francesca Ceccato Summary Introduction Applications: Piezocone penetration (CPTU) Submerged slope Conclusions Introduction Porous

More information

Mechanics of Earthquakes and Faulting

Mechanics of Earthquakes and Faulting Mechanics of Earthquakes and Faulting Lectures & 3, 9/31 Aug 017 www.geosc.psu.edu/courses/geosc508 Discussion of Handin, JGR, 1969 and Chapter 1 Scholz, 00. Stress analysis and Mohr Circles Coulomb Failure

More information

Module-4. Mechanical Properties of Metals

Module-4. Mechanical Properties of Metals Module-4 Mechanical Properties of Metals Contents ) Elastic deformation and Plastic deformation ) Interpretation of tensile stress-strain curves 3) Yielding under multi-axial stress, Yield criteria, Macroscopic

More information

Conservation of mass. Continuum Mechanics. Conservation of Momentum. Cauchy s Fundamental Postulate. # f body

Conservation of mass. Continuum Mechanics. Conservation of Momentum. Cauchy s Fundamental Postulate. # f body Continuum Mechanics We ll stick with the Lagrangian viewpoint for now Let s look at a deformable object World space: points x in the object as we see it Object space (or rest pose): points p in some reference

More information

Evaporation-driven soil salinization

Evaporation-driven soil salinization Evaporation-driven soil salinization Vishal Jambhekar 1 Karen Schmid 1, Rainer Helmig 1,Sorin Pop 2 and Nima Shokri 3 1 Department of Hydromechanics and Hydrosystemmodeling, University of Stuttgart 2 Department

More information

Reservoir Simulator Compaction Modelling: A Predictor for Accelerated Coupled Rock Mechanics -- Reservoir Simulation

Reservoir Simulator Compaction Modelling: A Predictor for Accelerated Coupled Rock Mechanics -- Reservoir Simulation Reservoir Simulator Compaction Modelling: A Predictor for Accelerated Coupled Rock Mechanics -- Reservoir Simulation by Øystein Pettersen Centre for Integrated Petroleum Research, Bergen, Norway ECMOR

More information

Prediction of geometric dimensions for cold forgings using the finite element method

Prediction of geometric dimensions for cold forgings using the finite element method Journal of Materials Processing Technology 189 (2007) 459 465 Prediction of geometric dimensions for cold forgings using the finite element method B.Y. Jun a, S.M. Kang b, M.C. Lee c, R.H. Park b, M.S.

More information

Lecture 7, Foams, 3.054

Lecture 7, Foams, 3.054 Lecture 7, Foams, 3.054 Open-cell foams Stress-Strain curve: deformation and failure mechanisms Compression - 3 regimes - linear elastic - bending - stress plateau - cell collapse by buckling yielding

More information

Gravity Tectonics Volcanism Atmosphere Water Winds Chemistry. Planetary Surfaces

Gravity Tectonics Volcanism Atmosphere Water Winds Chemistry. Planetary Surfaces Gravity Tectonics Volcanism Atmosphere Water Winds Chemistry Planetary Surfaces Gravity & Rotation Polar flattening caused by rotation is the largest deviation from a sphere for a planet sized object (as

More information

Cohesive band model: a triaxiality-dependent cohesive model for damage to crack transition in a non-local implicit discontinuous Galerkin framework

Cohesive band model: a triaxiality-dependent cohesive model for damage to crack transition in a non-local implicit discontinuous Galerkin framework University of Liège Aerospace & Mechanical Engineering Cohesive band model: a triaxiality-dependent cohesive model for damage to crack transition in a non-local implicit discontinuous Galerkin framework

More information

2D Liquefaction Analysis for Bridge Abutment

2D Liquefaction Analysis for Bridge Abutment D Liquefaction Analysis for Bridge Abutment Tutorial by Angel Francisco Martinez Integrated Solver Optimized for the next generation 64-bit platform Finite Element Solutions for Geotechnical Engineering

More information

Elements of Continuum Elasticity. David M. Parks Mechanics and Materials II February 25, 2004

Elements of Continuum Elasticity. David M. Parks Mechanics and Materials II February 25, 2004 Elements of Continuum Elasticity David M. Parks Mechanics and Materials II 2.002 February 25, 2004 Solid Mechanics in 3 Dimensions: stress/equilibrium, strain/displacement, and intro to linear elastic

More information

Thermal Analysis. with SolidWorks Simulation 2013 SDC. Paul M. Kurowski. Better Textbooks. Lower Prices.

Thermal Analysis. with SolidWorks Simulation 2013 SDC. Paul M. Kurowski. Better Textbooks. Lower Prices. Thermal Analysis with SolidWorks Simulation 2013 Paul M. Kurowski SDC PUBLICATIONS Schroff Development Corporation Better Textbooks. Lower Prices. www.sdcpublications.com Visit the following websites to

More information

CHAPTER 1 Fluids and their Properties

CHAPTER 1 Fluids and their Properties FLUID MECHANICS Gaza CHAPTER 1 Fluids and their Properties Dr. Khalil Mahmoud ALASTAL Objectives of this Chapter: Define the nature of a fluid. Show where fluid mechanics concepts are common with those

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

dynamics of f luids in porous media

dynamics of f luids in porous media dynamics of f luids in porous media Jacob Bear Department of Civil Engineering Technion Israel Institute of Technology, Haifa DOVER PUBLICATIONS, INC. New York Contents Preface xvii CHAPTER 1 Introduction

More information

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

Back Calculation of Rock Mass Modulus using Finite Element Code (COMSOL) Back Calculation of Rock Mass Modulus using Finite Element Code (COMSOL) Amirreza Ghasemi 1. Introduction Deformability is recognized as one of the most important parameters governing the behavior of rock

More information

Measurement of deformation. Measurement of elastic force. Constitutive law. Finite element method

Measurement of deformation. Measurement of elastic force. Constitutive law. Finite element method Deformable Bodies Deformation x p(x) Given a rest shape x and its deformed configuration p(x), how large is the internal restoring force f(p)? To answer this question, we need a way to measure deformation

More information

Bifurcation Analysis in Geomechanics

Bifurcation Analysis in Geomechanics Bifurcation Analysis in Geomechanics I. VARDOULAKIS Department of Engineering Science National Technical University of Athens Greece and J. SULEM Centre d'enseignement et de Recherche en Mecanique des

More information

MASS TRANSPORT Macroscopic Balances for Multicomponent Systems

MASS TRANSPORT Macroscopic Balances for Multicomponent Systems TRANSPORT PHENOMENA MASS TRANSPORT Macroscopic Balances for Multicomponent Systems Macroscopic Balances for Multicomponent Systems 1. The Macroscopic Mass Balance 2. The Macroscopic Momentum and Angular

More information

This paper was prepared for presentation at the Unconventional Resources Technology Conference held in Denver, Colorado, USA, August 2014.

This paper was prepared for presentation at the Unconventional Resources Technology Conference held in Denver, Colorado, USA, August 2014. URTeC: 1923960 Coupled Geomechanics and Pore Confinement Effects for Modeling Unconventional Shale Reservoirs Yi Xiong*, Philip. H. Winterfeld, Yu-Shu Wu, Colorado School of Mines; Zhaoqin Huang, China

More information

Chapter 1. Continuum mechanics review. 1.1 Definitions and nomenclature

Chapter 1. Continuum mechanics review. 1.1 Definitions and nomenclature Chapter 1 Continuum mechanics review We will assume some familiarity with continuum mechanics as discussed in the context of an introductory geodynamics course; a good reference for such problems is Turcotte

More information

THE PHYSICS OF FOAM. Boulder School for Condensed Matter and Materials Physics. July 1-26, 2002: Physics of Soft Condensed Matter. 1.

THE PHYSICS OF FOAM. Boulder School for Condensed Matter and Materials Physics. July 1-26, 2002: Physics of Soft Condensed Matter. 1. THE PHYSICS OF FOAM Boulder School for Condensed Matter and Materials Physics July 1-26, 2002: Physics of Soft Condensed Matter 1. Introduction Formation Microscopics 2. Structure Experiment Simulation

More information

3-D Finite Element Analysis of Instrumented Indentation of Transversely Isotropic Materials

3-D Finite Element Analysis of Instrumented Indentation of Transversely Isotropic Materials 3-D Finite Element Analysis of Instrumented Indentation of Transversely Isotropic Materials Abstract: Talapady S. Bhat and T. A. Venkatesh Department of Material Science and Engineering Stony Brook University,

More information

Introduction to Heat and Mass Transfer. Week 10

Introduction to Heat and Mass Transfer. Week 10 Introduction to Heat and Mass Transfer Week 10 Concentration Boundary Layer No concentration jump condition requires species adjacent to surface to have same concentration as at the surface Owing to concentration

More information

Developments in a Coupled Thermal- Hydraulic-Chemical-Geomechanical Model for Soil and Concrete

Developments in a Coupled Thermal- Hydraulic-Chemical-Geomechanical Model for Soil and Concrete Developments in a Coupled Thermal- Hydraulic-Chemical-Geomechanical Model for Soil and Concrete S.C. Seetharam * and D. Jacques 24 th October 2013 * suresh.seetharam@sckcen.be (Belgian Nuclear Research

More information

Mechanical Properties of Materials

Mechanical Properties of Materials Mechanical Properties of Materials Strains Material Model Stresses Learning objectives Understand the qualitative and quantitative description of mechanical properties of materials. Learn the logic of

More information

Estimating Permeability from Acoustic Velocity and Formation Resistivity Factor

Estimating Permeability from Acoustic Velocity and Formation Resistivity Factor 5th Conference & Exposition on Petroleum Geophysics, Hyderabad-2004, India PP 582-587 and Formation Resistivity Factor Majid Nabi-Bidhendi Institute of Geophysics, University of Tehran, P.O. Box 14155-6466,

More information

Multiphysics modelling of the Mandel-Cryer effect

Multiphysics modelling of the Mandel-Cryer effect Int. Jnl. of Multiphysics Volume 10 Number 1 2016 11 Multiphysics modelling of the Mandel-Cryer effect E Holzbecher* German University of Technology in Oman (GUtech) Muscat, Oman ABSTRACT In porous medium

More information

We may have a general idea that a solid is hard and a fluid is soft. This is not satisfactory from

We may have a general idea that a solid is hard and a fluid is soft. This is not satisfactory from Chapter 1. Introduction 1.1 Some Characteristics of Fluids We may have a general idea that a solid is hard and a fluid is soft. This is not satisfactory from scientific or engineering point of view. In

More information

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

Fig. 1. Circular fiber and interphase between the fiber and the matrix. Finite element unit cell model based on ABAQUS for fiber reinforced composites Tian Tang Composites Manufacturing & Simulation Center, Purdue University West Lafayette, IN 47906 1. Problem Statement In

More information

Unsaturated Flow (brief lecture)

Unsaturated Flow (brief lecture) Physical Hydrogeology Unsaturated Flow (brief lecture) Why study the unsaturated zone? Evapotranspiration Infiltration Toxic Waste Leak Irrigation UNSATURATAED ZONE Aquifer Important to: Agriculture (most

More information

Modeling and Simulation of the Consolidation Behaviour of Cemented Paste Backfill

Modeling and Simulation of the Consolidation Behaviour of Cemented Paste Backfill Modeling and Simulation of the Consolidation Behaviour of Cemented Paste Backfill Liang Cui and Mamadou Fall Presented by Liang Cui Department of Civil Engineering, University of Ottawa OUTLINE Introduction

More information

Appendix: Nomenclature

Appendix: Nomenclature Appendix: Nomenclature 209 Appendix: Nomenclature Chapter 2: Roman letters A amplitude of surface wave m A j (complex) amplitude of tidal component [various] a right ascension rad or a magnitude of tidal

More information

A Critical Plane-energy Model for Multiaxial Fatigue Life Prediction. of Homogeneous and Heterogeneous Materials. Haoyang Wei

A Critical Plane-energy Model for Multiaxial Fatigue Life Prediction. of Homogeneous and Heterogeneous Materials. Haoyang Wei A Critical Plane-energy Model for Multiaxial Fatigue Life Prediction of Homogeneous and Heterogeneous Materials by Haoyang Wei A Thesis Presented in Partial Fulfillment of the Requirements for the Degree

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

Using Thermal Boundary Conditions in SOLIDWORKS Simulation to Simulate a Press Fit Connection

Using Thermal Boundary Conditions in SOLIDWORKS Simulation to Simulate a Press Fit Connection Using Thermal Boundary Conditions in SOLIDWORKS Simulation to Simulate a Press Fit Connection Simulating a press fit condition in SOLIDWORKS Simulation can be very challenging when there is a large amount

More information

Liquid water is one of the

Liquid water is one of the Formanski 71 1/07/09 8:57 Page 71 V olume 5 - Number 7 - May 2009 (71-75) Abstract Liquid water is one of the agents responsible for damage of building materials. Therefore determination of its content

More information

UNIT I SIMPLE STRESSES AND STRAINS

UNIT I SIMPLE STRESSES AND STRAINS Subject with Code : SM-1(15A01303) Year & Sem: II-B.Tech & I-Sem SIDDHARTH GROUP OF INSTITUTIONS :: PUTTUR Siddharth Nagar, Narayanavanam Road 517583 QUESTION BANK (DESCRIPTIVE) UNIT I SIMPLE STRESSES

More information

Thermal and coupled THM analysis

Thermal and coupled THM analysis PLAXIS Thermal and coupled THM analysis 2015 TABLE OF CONTENTS TABLE OF CONTENTS 1 Features and limitations 5 2 Governing equations 7 2.1 Non isothermal unsaturated water flow 7 2.2 Mass balance equation

More information

Four Verification Cases for PORODRY

Four Verification Cases for PORODRY Four Verification Cases for PORODRY We designed four different verification cases to validate different aspects of our numerical solution and its code implementation, and these are summarized in Table

More information

Coupled Thermomechanical Contact Problems

Coupled Thermomechanical Contact Problems Coupled Thermomechanical Contact Problems Computational Modeling of Solidification Processes C. Agelet de Saracibar, M. Chiumenti, M. Cervera ETS Ingenieros de Caminos, Canales y Puertos, Barcelona, UPC

More information

1.8 Unconfined Compression Test

1.8 Unconfined Compression Test 1-49 1.8 Unconfined Compression Test - It gives a quick and simple measurement of the undrained strength of cohesive, undisturbed soil specimens. 1) Testing method i) Trimming a sample. Length-diameter

More information

Model of Heat and Mass Transfer with Moving Boundary during Roasting of Meat in Convection-Oven

Model of Heat and Mass Transfer with Moving Boundary during Roasting of Meat in Convection-Oven Presented at the COMSOL Conference 2009 Milan Model of Heat and Mass Transfer with Moving Boundary during Roasting of Meat in Convection-Oven COMSOL Conference October 15, 2009, Milan, ITALY Aberham Hailu

More information

Simulation Analysis of Microchannel Deformation during LTCC Warm Water Isostatic Pressing Process Lang Ping, Zhaohua Wu*

Simulation Analysis of Microchannel Deformation during LTCC Warm Water Isostatic Pressing Process Lang Ping, Zhaohua Wu* International Conference on Information Sciences, Machinery, Materials and Energy (ICISMME 2015) Simulation Analysis of Microchannel Deformation during LTCC Warm Water Isostatic Pressing Process Lang Ping,

More information

On measurement of mechanical properties of sound absorbing materials

On measurement of mechanical properties of sound absorbing materials On measurement of mechanical properties of sound absorbing materials Nicolas Dauchez, Manuel Etchessahar, Sohbi Sahraoui To cite this version: Nicolas Dauchez, Manuel Etchessahar, Sohbi Sahraoui. On measurement

More information

Thermal Analysis with SOLIDWORKS Simulation 2015 and Flow Simulation 2015

Thermal Analysis with SOLIDWORKS Simulation 2015 and Flow Simulation 2015 Thermal Analysis with SOLIDWORKS Simulation 2015 and Flow Simulation 2015 Paul M. Kurowski SDC PUBLICATIONS Better Textbooks. Lower Prices. www.sdcpublications.com Powered by TCPDF (www.tcpdf.org) Visit

More information

Modeling of Liquid Water Distribution at Cathode Gas Flow Channels in Proton Exchange Membrane Fuel Cell - PEMFC

Modeling of Liquid Water Distribution at Cathode Gas Flow Channels in Proton Exchange Membrane Fuel Cell - PEMFC Modeling of Liquid Water Distribution at Cathode Gas Flow Channels in Proton Exchange Membrane Fuel Cell - PEMFC Sandro Skoda 1*, Eric Robalinho 2, André L. R. Paulino 1, Edgar F. Cunha 1, Marcelo Linardi

More information

Fundamentals of Fluid Dynamics: Elementary Viscous Flow

Fundamentals of Fluid Dynamics: Elementary Viscous Flow Fundamentals of Fluid Dynamics: Elementary Viscous Flow Introductory Course on Multiphysics Modelling TOMASZ G. ZIELIŃSKI bluebox.ippt.pan.pl/ tzielins/ Institute of Fundamental Technological Research

More information

Numerical Analysis And Experimental Verification of a Fire Resistant Overpack for Nuclear Waste

Numerical Analysis And Experimental Verification of a Fire Resistant Overpack for Nuclear Waste Numerical Analysis And Experimental Verification of a Fire Resistant Overpack for Nuclear Waste Author P. Geraldini 1, Co-author A. Lorenzo 2 1,2 Sogin S.p.A., Rome, Italy Via Marsala 51/C 00185 Rome 1

More information

Chapter II: Reversible process and work

Chapter II: Reversible process and work Chapter II: Reversible process and work 1- Process Defined by change in a system, a thermodynamic process is a passage of a thermodynamic system from an initial to a final state of thermodynamic equilibrium.

More information

Semeniuk, B., Göransson, P. (2018) Modelling the Dynamic Viscous and Thermal Dissipation Mechanisms in a Fibrous Porous Material In:

Semeniuk, B., Göransson, P. (2018) Modelling the Dynamic Viscous and Thermal Dissipation Mechanisms in a Fibrous Porous Material In: http://www.diva-portal.org This is the published version of a paper presented at COMSOL Conference 2018 Lausanne. Citation for the original published paper: Semeniuk, B., Göransson, P. (2018) Modelling

More information

Mathematical Modeling of Displacements and Thermal Stresses in Anisotropic Materials (Sapphire) in Cooling

Mathematical Modeling of Displacements and Thermal Stresses in Anisotropic Materials (Sapphire) in Cooling Mathematical Modeling of Displacements and Thermal Stresses in Anisotropic Materials (Sapphire) in Cooling Timo Tiihonen & Tero Tuovinen September 11, 2015 European Study Group with Industry, ESGI 112,

More information

Hardened Concrete. Lecture No. 16

Hardened Concrete. Lecture No. 16 Hardened Concrete Lecture No. 16 Fatigue strength of concrete Modulus of elasticity, Creep Shrinkage of concrete Stress-Strain Plot of Concrete At stress below 30% of ultimate strength, the transition

More information