GBT (GENERALISED BEAM THEORY)-BASED ELASTIC - PLASTIC POST-BUCKLING ANALYSIS OF STAINLESS STEEL THIN-WALLED MEMBERS

Size: px
Start display at page:

Download "GBT (GENERALISED BEAM THEORY)-BASED ELASTIC - PLASTIC POST-BUCKLING ANALYSIS OF STAINLESS STEEL THIN-WALLED MEMBERS"

Transcription

1 4 TH INTERNATIONAL EXERTS SEMINAR STAINLESS STEEL IN STRUCTURES ASCOT, UK, 6-7 DECEMBER 2012 (GENERALISED BEAM THEORY)-BASED ELASTIC - LASTIC OST-BUCKLING ANALYSIS OF STAINLESS STEEL THIN-WALLED MEMBERS TECHNICAL UNIVERSITY OF LISBON MIGUEL ABAMBRES, DINAR CAMOTIM, NUNO SILVESTRE

2 MOTIVATION STAINLESS STEEL HAS SEVERAL ATTRACTIVE FEATURES WHEN COMARED WITH CARBON STEEL: BETTER AEARANCE HIGHER CORROSION RESISTANCE MORE COST-EFFECTIVE AND LONGER LIFE CYCLE DISSEMINATION OF EASY-TO-USE DESIGN TOOLS IS NEEDED IN ORDER TO INCREASE THE STRUCTURAL USE OF STAINLESS STEEL SINCE SHELL FINITE ELEMENT ANALYSES ARE OFTEN RONE TO DATA INUT ERRORS, YIELD DIFFICULT-TO-INTERRET RESULTS, AND INVOLVE HIGH COMUTATIONAL COSTS CLOUD GATE, CHICAGO (USA) ADRE ARRUE FOOTBRIDGE, BILBAO (SAIN), HTT://

3 MOTIVATION A -BASED FORMULATION TO REDICT THE BEHAVIOUR AND COLLASE OF THIN-WALLED MEMBERS CONSTITUTED BY HIGHLY NON-LINEAR MATERIALS (e.g., STAINLESS STEEL) IS ROOSED SUMMARY BRIEF OVERVIEW OF THE FORMULATION ILLUSTRATIVE EXAMLES: NON-LINEAR BEHAVIOUR OF TWO LEAN DULEX SHS COLD-FORMED COLUMNS (THEOFANOUS & GARDNER 2009) 1999 mm mm 400 mm FIXED-ENDED LONG IN-ENDED STUB COLUMN

4 FORMULATION - ASSUMTIONS : BEAM THEORY INCLUDING CROSS - SECTION IN - LANE DEFORMATION q ds s (v) z (w) d t (u) σ = 0, ε = 0 zz iz ε ε ss γ s σ E Eν ν 1-ν e Eν E D = σ ss ν 1-ν σ s 0 0 G

5 FORMULATION DISLACEMENT FIELD LINEAR COMBINATION OF DEFORMATION MODES WHITH AMLITUDES VARYING ALONG THE MEMBER LENGTH ds d CROSS-SECTION ANALYSIS s (v) z (w) (u) u(,s) = u (s) ζ () k k, v(,s) = w(,s) = v (s) k w (s) k ζ () k ζ () k MEMBER ANALYSIS

6 FORMULATION - EQUILIBRIUM ds s (v) z (w) d (u) VIRTUAL WORK δw +δw = = 0 + σ δγ dv int FE AROXIMATION: HERMITE CUBIC et σ δε σssδεs s + s s L e b t ζ = Ψ d v, w = 0 k, H k γ s =u ε,s + v= u,, - 2zw -, +,s +u u,, +,s v, +, v w,s +, w, w,s ζ 1 2 = Ψ d v, w 0 k H k e INCREMENTAL-ITERATIVE SCHEME: CYLINDRICAL ARC-LENGTH Ktan j Δd = Δλf σ σ ε σ εss σmn γ = + + d ε d ε d γ d mn mn mn s pl pl ss pl s pl

7 LASTICITY - OVERVIEW THEORY: J 2 WITH ASSOCIATED FLOW RULE NUMERICAL INTEGRATION: MEAN-NORMAL STRESS - STRAIN CURVE: QUACH ET AL. (2008) BASED ON ONLY THREE ARAMETERS n σ σ ,0 σ σ0.2 E σ0.2 n2 σ * σ* ε = ε + + ε *, σ < σ σ 2p E0.2 σ* 1 σ - a, σ 2 < σ σu b σ

8 ILLUSTRATIVE EXAMLES STRESS-STRAIN CURVE RAMBERG - OSGOOD ARAMETERS OBTAINED FROM FLAT COUON TESTS (CORNER STRENGTH ENHANCEMENT NOT MODELLED) σ (N/mm 2 ) Fied-ended column ( ) in-ended column (80804) % 0% 0.2% 5% 0.4% 10% 0.6% 15% 0.8% 1.0% 20% ε

9 LONG IN-ENDED COLUMN LEAN DULEX (EN ): σ 0 y = N/mm 2, σ 0.2 =657 N/mm 2, E= N/mm 2, ν=0.3 z y F = λ N [mm] : S4 SFEs mm = d.o.f : 41 / 124 MODES + 48 FEs = 3909 d.o.f (18%) 2.5 δ y δ y t = KNIFE EDGES (THEOFANOUS & GARDNER, 2009 ) INITIAL GEOMETRICAL IMERFECTIONS 2.0 Δ = L/ λ b,glob = Δ = mm λ b,loc =5.76 L

10 EQUILIBRIUM ATH λ B Test (Theofanous and Gardner) A % & MODAL ARTICIATION λ u, = 1.04 λ u,test = 1.00 DIF 1.5% OTHERS 6 δ y z y F = λ δ y EX. OTHERS 75% 3 93% δ y 1

11 DISLACEMENTS λ z y A δ y LOCAL BUCKLING OVERSHADOWED 90 δ y BY GLOBAL BENDING A RECALL THE INITIAL IMERFECTION... δ y L L

12 STRESSES z y W3 λ B A W2 W1 δ y WHEREVER σ MISES > σ 0 y, THE DIAGRAM NON-LINEARITY REFLECTS THE NEUTRAL AXIS CROSSES THE CROSS-SECTION AT THE A STATE STAINLESS TENSILE STRESSES STEEL NON-LINEAR ONLY DEVELO HARDENING AFTER THE EAK LOAD σ (N / mm 2 ) σ MISES (N / mm 2 ) B A W1 W2 W A B W1 W2 W3

13 STRESSES z y W3 λ B A W2 W1 δ y WHEREVER σ MISES > σ 0 y, THE DIAGRAM NON-LINEARITY REFLECTS THE STAINLESS STEEL NON-LINEAR HARDENING A STATE () σ MISES (N / mm 2 ) A COMRESSION SIDE 600 LASTICITY ALSO IN TENSION ( BUT TO A LESSER EXTENT ) TENSION SIDE B W1 W2 W3

14 FIXED-ENDED STUB COLUMN LEAN DULEX (EN ): σ 0 y = N/mm 2, σ 0.2 =560 N/mm 2, E= N/mm 2, ν=0.3 z F = λ N t = [mm] : S4 SFEs 8 8 mm = d.o.f : 28 / 204 MODES + 16 FEs = 865 d.o.f (6%) INITIAL GEOMETRICAL IMERFECTION δ z Δ = t / L λ b,loc =

15 EQUILIBRIUM ATH & MODAL ARTICIATION λ B Test (Theofanous and Gardner) % CORNER STRENGTH ENHANCEMENT SHOULD BE MODELLED z 77.3% 166, DIF 4.9% 28% λ u, = λ u,test = % OTHERS 9, 14 19% A Δ Δ TWO DISTINCT BEHAVIOURS: EX GLOBAL DEFORMATION GOVERNS U TO THE EAK LOAD LOCAL BUCKLING EMERGES IN 1 THE OST-EAK STAGE F = λ Δ 9 14 OTHERS

16 MISES STRESSES λ AT THE EAK (), THE WHOLE COLUMN MID-SURFACE IS ALREADY YIELDED: σ MISES > N/mm A Δ THE HIGHEST A STRESSES OCCUR AT THE MID-SAN CORNER REGIONS (RED), DUE TO FROM TO A, THE COLUMN EXERIENCES UNLOADING (BLUE + GREEN) AND ALSO THE FURTHER REDISTRIBUTION LASTIC DEFORMATION CAUSED BY THE (YELLOW LOCAL + DEFORMATION RED) (EFFECTIVE WIDTH CONCET)

17 DISLACEMENTS z δ z λ B A δ 400 Δ AT AT OST-COLLASE, (A), THE THREE THE AXIAL HALF-WAVES STIFFNESS RETURN DRO AT DUE MID-SAN TO BOTH ROFILES DISLAY FIVE HALF-WAVES. THE INITIAL IMERFECTION HAD THREE... LOCALISED ASSOCIATED LASTIC WITH DEFORMATION THE INCREASING AT MID-SAN LOCAL(ISED) + ELASTIC DEFORMATION UNLOADING 1.2 δ z B L δ z A δ B A L L

18 CONCLUDING REMARKS A FORMULATION TO ERFORM OST-BUCKLING ANALYSES OF THIN-WALLED MEMBERS MADE OF ISOTROIC MATERIALS EXHIBITING NON-LINEAR HARDENING WAS DEVELOED AND IMLEMENTED THE ALICATION AND OTENTIAL OF THE FORMULATION WERE ILLUSTRATED THROUGH THE NON-LINEAR BEHAVIOUR AND COLLASE OF TWO LEAN DULEX SHS COLD-FORMED COLUMNS TESTED AT IMERIAL COLLEGE BY THEOFANOUS & GARDNER (2009) THE RESULTS WERE VALIDATED AGAINST SFEA VALUES - QUITE GOOD AGREEMENT WAS FOUND, EVEN IF THE ANALYSES INVOLVE ONLY 18% AND 6% OF THE D.O.F. NUMBERS REQUIRED BY THE SFEA

19 CONCLUDING REMARKS THE MODAL NATURE MAKES IT OSSIBLE TO ACQUIRE IN-DETH INSIGHT ON THE MECHANICAL FEATURES OF THE COLUMN BEHAVIOUR CORNER STRENGTH ENHANCEMENT AND MEMBRANE RESIDUAL STRESS EFFECTS WILL BE FAIRLY SOON INCORORATED IN THE ANALYSES (ALSO FOR OEN SECTIONS AND DISTORTIONAL BUCKLING ROBLEMS) ADDITIONAL SIMULATIONS, INVOLVING TESTS CARRIED OUT AT THE UNIV. OF SYDNEY, WILL BE REORTED IN THE NEAR FUTURE (FIFTH SEMC CONFERENCE SETEMBER 2013, CAE TOWN, S. AFRICA)

FE FORMULATIONS FOR PLASTICITY

FE FORMULATIONS FOR PLASTICITY G These slides are designed based on the book: Finite Elements in Plasticity Theory and Practice, D.R.J. Owen and E. Hinton, 1970, Pineridge Press Ltd., Swansea, UK. 1 Course Content: A INTRODUCTION AND

More information

8.7 Associated and Non-associated Flow Rules

8.7 Associated and Non-associated Flow Rules 8.7 Associated and Non-associated Flow Rules Recall the Levy-Mises flow rule, Eqn. 8.4., d ds (8.7.) The lastic multilier can be determined from the hardening rule. Given the hardening rule one can more

More information

A SIMPLE PLASTICITY MODEL FOR PREDICTING TRANSVERSE COMPOSITE RESPONSE AND FAILURE

A SIMPLE PLASTICITY MODEL FOR PREDICTING TRANSVERSE COMPOSITE RESPONSE AND FAILURE THE 19 TH INTERNATIONAL CONFERENCE ON COMPOSITE MATERIALS A SIMPLE PLASTICITY MODEL FOR PREDICTING TRANSVERSE COMPOSITE RESPONSE AND FAILURE K.W. Gan*, M.R. Wisnom, S.R. Hallett, G. Allegri Advanced Comosites

More information

Computational Solid Mechanics Computational Plasticity

Computational Solid Mechanics Computational Plasticity Comutational Solid Mechanics Comutational Plasticity Chater 3. J Plasticity Models C. Agelet de Saracibar ETS Ingenieros de Caminos, Canales y Puertos, Universidad Politécnica de Cataluña (UPC), Barcelona,

More information

Modified Quasi-Static, Elastic-Plastic Analysis for Blast Walls with Partially Fixed Support

Modified Quasi-Static, Elastic-Plastic Analysis for Blast Walls with Partially Fixed Support Article Modified Quasi-Static, Elastic-Plastic Analysis for Blast Walls with Partially Fixed Suort Pattamad Panedojaman Deartment of Civil Engineering, Faculty of Engineering, Prince of Songkla University,

More information

The effect of dynamic bending moments on the ratchetting behavior of stainless steel pressurized piping elbows

The effect of dynamic bending moments on the ratchetting behavior of stainless steel pressurized piping elbows International Journal of echanical Engineering and Alications 2014; 2(2): 31-37 Published online ay 30, 2014 (htt://www.scienceublishinggrou.com/j/ijmea) doi: 10.11648/j.ijmea.20140202.12 The effect of

More information

Finite Element Analysis of V-Bending of Polypropylene Using Hydrostatic-Pressure-Dependent Plastic Constitutive Equation*

Finite Element Analysis of V-Bending of Polypropylene Using Hydrostatic-Pressure-Dependent Plastic Constitutive Equation* Materials Transactions, Vol. 48, No. 1 (7). 6 to 664 #7 The Jaan Society for Technology of Plasticity Finite Element Analysis of V-Bending of Polyroylene Using Hydrostatic-Pressure-Deendent Plastic onstitutive

More information

The. Consortium. Continuum Mechanics. Original notes by Professor Mike Gunn, South Bank University, London, UK Produced by the CRISP Consortium Ltd

The. Consortium. Continuum Mechanics. Original notes by Professor Mike Gunn, South Bank University, London, UK Produced by the CRISP Consortium Ltd The C R I S P Consortium Continuum Mechanics Original notes b Professor Mike Gunn, South Bank Universit, London, UK Produced b the CRISP Consortium Ltd THOR OF STRSSS In a three dimensional loaded bod,

More information

Pressure-sensitivity Effects on Toughness Measurements of Compact Tension Specimens for Strain-hardening Solids

Pressure-sensitivity Effects on Toughness Measurements of Compact Tension Specimens for Strain-hardening Solids American Journal of Alied Sciences (9): 19-195, 5 ISSN 1546-939 5 Science Publications Pressure-sensitivity Effects on Toughness Measurements of Comact Tension Secimens for Strain-hardening Solids Abdulhamid

More information

A New Design Method for Stainless Steel Column Subjected to Flexural Buckling

A New Design Method for Stainless Steel Column Subjected to Flexural Buckling Stainless Steel in Structures: Fourth International xperts Seminar A New Design Method for Stainless Steel Column Subjected to Flexural Buckling Shu Ganping Zheng Baofeng School of Civil ngineering, Southeast

More information

Keywords: pile, liquefaction, lateral spreading, analysis ABSTRACT

Keywords: pile, liquefaction, lateral spreading, analysis ABSTRACT Key arameters in seudo-static analysis of iles in liquefying sand Misko Cubrinovski Deartment of Civil Engineering, University of Canterbury, Christchurch 814, New Zealand Keywords: ile, liquefaction,

More information

Chapter 5 Structural Elements: The truss & beam elements

Chapter 5 Structural Elements: The truss & beam elements Institute of Structural Engineering Page 1 Chapter 5 Structural Elements: The truss & beam elements Institute of Structural Engineering Page 2 Chapter Goals Learn how to formulate the Finite Element Equations

More information

Elio Sacco. Dipartimento di Ingegneria Civile e Meccanica Università di Cassino e LM

Elio Sacco. Dipartimento di Ingegneria Civile e Meccanica Università di Cassino e LM Elio Sacco Diartimento di Ingegneria Civile e Meccanica Università di Cassino e LM Uni-axial resonse E ε if ε < 0 = 0 if ε 0 stress-strain t ε = 0 = c 0 if ε < 0 = E ( ε δ) with δ = ε if ε 0 ε e δ elastic

More information

PLATE GIRDERS - I 1.0 INTRODUCTION

PLATE GIRDERS - I 1.0 INTRODUCTION 15 PLATE GIRDERS - I 1.0 INTRODUCTION A fabricated late girder shown diagrammatically in Fig. 1 is emloyed for suorting heavy loads over long sans. The bending moments and shear forces roduced in such

More information

SAMARIS. Draft report

SAMARIS. Draft report SAMARIS Work Package 5 - Performance based secifications Selection and evaluation of models for rediction of ermanent deformations of unbound granular materials in road avements Draft reort Pierre Hornych

More information

INTRODUCING THE SHEAR-CAP MATERIAL CRITERION TO AN ICE RUBBLE LOAD MODEL

INTRODUCING THE SHEAR-CAP MATERIAL CRITERION TO AN ICE RUBBLE LOAD MODEL Symosium on Ice (26) INTRODUCING THE SHEAR-CAP MATERIAL CRITERION TO AN ICE RUBBLE LOAD MODEL Mohamed O. ElSeify and Thomas G. Brown University of Calgary, Calgary, Canada ABSTRACT Current ice rubble load

More information

Flexible Pipes in Trenches with Stiff Clay Walls

Flexible Pipes in Trenches with Stiff Clay Walls Flexible Pies in Trenches with Stiff Clay Walls D. A. Cameron University of South Australia, South Australia, Australia J. P. Carter University of Sydney, New South Wales, Australia Keywords: flexible

More information

SHAPE OPTOMIZATION OF H-BEAM FLANGE FOR MAXIMUM PLASTIC ENERGY DISSIPATION

SHAPE OPTOMIZATION OF H-BEAM FLANGE FOR MAXIMUM PLASTIC ENERGY DISSIPATION The Fourth China-Jaan-Korea Joint Symosium on Otimization of Structural and Mechanical Systems Kunming, Nov. 6-9, 2006, China SHAPE OPTOMIZATION OF H-BEAM FLANGE FOR MAXIMUM PLASTIC ENERGY DISSIPATION

More information

International Journalof Fatigue

International Journalof Fatigue International Journal of Fatigue 29 (2007) 1634 1646 International Journalof Fatigue www.elsevier.com/locate/ijfatigue Variable amlitude fatigue crack growth, exerimental results and modeling R. Hamam

More information

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

Influence of residual stresses in the structural behavior of. tubular columns and arches. Nuno Rocha Cima Gomes October 2014 Influence of residual stresses in the structural behavior of Abstract tubular columns and arches Nuno Rocha Cima Gomes Instituto Superior Técnico, Universidade de Lisboa, Portugal Contact:

More information

Adam Paweł Zaborski. 8 Plasticity. reloading. 1. Bauschinger s effect. 2. unchanged yielding limit. 3. isotropic hardening

Adam Paweł Zaborski. 8 Plasticity. reloading. 1. Bauschinger s effect. 2. unchanged yielding limit. 3. isotropic hardening 8 lasticity Introduction Definitions loading/unloading/reloading words commonly used in lasticity lastic strain a ermanent strain that doesn t vanish after unloading, lastically assive rocess a rocess

More information

Geo-E2010 Advanced Soil Mechanics L Wojciech Sołowski. 07 March 2017

Geo-E2010 Advanced Soil Mechanics L Wojciech Sołowski. 07 March 2017 Geo-E2010 Advanced Soil Mechanics L Wojciech Sołowski 07 March 2017 Soil modeling: critical state soil mechanics and Modified Cam Clay model Outline 1. Refresh of the theory of lasticity 2. Critical state

More information

Hydrogen-assisted stress corrosion cracking simulation using the stress-modified fracture strain model

Hydrogen-assisted stress corrosion cracking simulation using the stress-modified fracture strain model Journal of Mechanical Science and Technology 26 (8) (2012) 2631~2638 www.sringerlink.com/content/1738-494x DOI 10.1007/s12206-012-0642-x Hydrogen-assisted stress corrosion cracking simulation using the

More information

Numerical and experimental investigation on shot-peening induced deformation. Application to sheet metal forming.

Numerical and experimental investigation on shot-peening induced deformation. Application to sheet metal forming. Coyright JCPDS-International Centre for Diffraction Data 29 ISSN 197-2 511 Numerical and exerimental investigation on shot-eening induced deformation. Alication to sheet metal forming. Florent Cochennec

More information

UNIVERSITY OF SASKATCHEWAN ME MECHANICS OF MATERIALS I FINAL EXAM DECEMBER 13, 2008 Professor A. Dolovich

UNIVERSITY OF SASKATCHEWAN ME MECHANICS OF MATERIALS I FINAL EXAM DECEMBER 13, 2008 Professor A. Dolovich UNIVERSITY OF SASKATCHEWAN ME 313.3 MECHANICS OF MATERIALS I FINAL EXAM DECEMBER 13, 2008 Professor A. Dolovich A CLOSED BOOK EXAMINATION TIME: 3 HOURS For Marker s Use Only LAST NAME (printed): FIRST

More information

Lower bound solutions for bearing capacity of jointed rock

Lower bound solutions for bearing capacity of jointed rock Comuters and Geotechnics 31 (2004) 23 36 www.elsevier.com/locate/comgeo Lower bound solutions for bearing caacity of jointed rock D.J. Sutcliffe a, H.S. Yu b, *, S.W. Sloan c a Deartment of Civil, Surveying

More information

COMPARISON OF FREQUENCY DEPENDENT EQUIVALENT LINEAR ANALYSIS METHODS

COMPARISON OF FREQUENCY DEPENDENT EQUIVALENT LINEAR ANALYSIS METHODS October 2-7, 28, Beijing, China COMPARISON OF FREQUENCY DEPENDENT EQUIVALENT LINEAR ANALYSIS METHODS Dong-Yeo Kwak Chang-Gyun Jeong 2 Duhee Park 3 and Sisam Park 4 Graduate student, Det. of Civil Engineering,

More information

Design of Isolated Bridges from the Viewpoint of Collapse under Extreme Earthquakes

Design of Isolated Bridges from the Viewpoint of Collapse under Extreme Earthquakes Design of Isolated Bridges from the Viewoint of Collase under Extreme Earthquakes D.W. Chang, Y.T. Lin, C.H. Peng, C.Y. Liou CECI Engineering Consultants, Inc., Taiwan T.Y. Lee National Central University,

More information

BENDING INDUCED VERTICAL OSCILLATIONS DURING SEISMIC RESPONSE OF RC BRIDGE PIERS

BENDING INDUCED VERTICAL OSCILLATIONS DURING SEISMIC RESPONSE OF RC BRIDGE PIERS BENDING INDUCED VERTICAL OSCILLATIONS DURING SEISMIC RESPONSE OF RC BRIDGE PIERS Giulio RANZO 1, Marco PETRANGELI And Paolo E PINTO 3 SUMMARY The aer resents a numerical investigation on the behaviour

More information

Predicting the constitutive behaviour of microsphere-filled elastomers: the influence of shell buckling and interaction

Predicting the constitutive behaviour of microsphere-filled elastomers: the influence of shell buckling and interaction Predicting the constitutive behaviour of microshere-filled elastomers: the influence of shell buckling and interaction William J. Parnell Professor of Alied Mathematics and EPSRC Research Fellow School

More information

The reciprocal effects of bending and torsion on springback during 3D bending of profiles

The reciprocal effects of bending and torsion on springback during 3D bending of profiles Available online at www.sciencedirect.com ScienceDirect Procedia Engineering 207 (2017) 2322 2327 International Conference on the Technology of Plasticity, ICTP 2017, 17-22 Setember 2017, Cambridge, United

More information

KEY ISSUES IN THE ANALYSIS OF PILES IN LIQUEFYING SOILS

KEY ISSUES IN THE ANALYSIS OF PILES IN LIQUEFYING SOILS 4 th International Conference on Earthquake Geotechnical Engineering June 2-28, 27 KEY ISSUES IN THE ANALYSIS OF PILES IN LIQUEFYING SOILS Misko CUBRINOVSKI 1, Hayden BOWEN 1 ABSTRACT Two methods for analysis

More information

ELASTO-PLASTIC BUCKLING BEHAVIOR OF H-SHAPED BEAM WITH LARGE DEPTH-THICKNESS RATIO UNDER CYCLIC LOADING

ELASTO-PLASTIC BUCKLING BEHAVIOR OF H-SHAPED BEAM WITH LARGE DEPTH-THICKNESS RATIO UNDER CYCLIC LOADING SDSS Rio STABILITY AND DUCTILITY OF STEEL STRUCTURES E. Batista, P. Vellasco, L. de Lima (Eds.) Rio de Janeiro, Brazil, Setember 8 -, ELASTO-PLASTIC BUCKLING BEHAVIOR OF H-SHAPED BEA WITH LARGE DEPTH-THICKNESS

More information

Adaptive Analysis of Bifurcation Points of Shell Structures

Adaptive Analysis of Bifurcation Points of Shell Structures First published in: Adaptive Analysis of Bifurcation Points of Shell Structures E. Ewert and K. Schweizerhof Institut für Mechanik, Universität Karlsruhe (TH), Kaiserstraße 12, D-76131 Karlsruhe, Germany

More information

GBTUL 1.0. Buckling and Vibration Analysis of Thin-Walled Members GBT THEORETICAL BACKGROUND. Rui Bebiano Nuno Silvestre Dinar Camotim

GBTUL 1.0. Buckling and Vibration Analysis of Thin-Walled Members GBT THEORETICAL BACKGROUND. Rui Bebiano Nuno Silvestre Dinar Camotim GBTUL 1.0 Buckling and Vibration Analysis of Thin-Walled Members GBT THEORETICAL BACKGROUND Rui Bebiano Nuno Silvestre Dinar Camotim Department of Civil Engineering and Architecture, DECivil/IST Technical

More information

G1RT-CT D. EXAMPLES F. GUTIÉRREZ-SOLANA S. CICERO J.A. ALVAREZ R. LACALLE W P 6: TRAINING & EDUCATION

G1RT-CT D. EXAMPLES F. GUTIÉRREZ-SOLANA S. CICERO J.A. ALVAREZ R. LACALLE W P 6: TRAINING & EDUCATION D. EXAMPLES 426 WORKED EXAMPLE I Flat Plate Under Constant Load Introduction and objectives Data Analysis Bibliography/References 427 INTRODUCTION AND OBJECTIVES During a visual inspection of a C-Mn flat

More information

A General Damage Initiation and Evolution Model (DIEM) in LS-DYNA

A General Damage Initiation and Evolution Model (DIEM) in LS-DYNA 9th Euroean LS-YNA Conference 23 A General amage Initiation and Evolution Model (IEM) in LS-YNA Thomas Borrvall, Thomas Johansson and Mikael Schill, YNAmore Nordic AB Johan Jergéus, Volvo Car Cororation

More information

Lecture 8. Stress Strain in Multi-dimension

Lecture 8. Stress Strain in Multi-dimension Lecture 8. Stress Strain in Multi-dimension Module. General Field Equations General Field Equations [] Equilibrium Equations in Elastic bodies xx x y z yx zx f x 0, etc [2] Kinematics xx u x x,etc. [3]

More information

Civil. Engineering INELASTIC BENDING CAPACITY IN COLD-FORMED STEEL MEMBERS Annual Stability Conference New Orleans, Louisiana

Civil. Engineering INELASTIC BENDING CAPACITY IN COLD-FORMED STEEL MEMBERS Annual Stability Conference New Orleans, Louisiana Civil Engineering at JOHNS HOPKINS UNIVERSITY at JOHNS HOPKINS UNIVERSITY INELASTIC BENDING CAPACITY IN COLD-FORMED STEEL MEMBERS 2007 Annual Stability Conference New Orleans, Louisiana April 2007 Y.Shifferaw

More information

Numerical Simulation of Orthogonal Cutting using the Material Point Method

Numerical Simulation of Orthogonal Cutting using the Material Point Method Numerical Simulation of Orthogonal Cutting using the Material Point Method John A. Nairn Wood Science and Engineering, Oregon State University, Corvallis, OR 97330, USA Tel: +-54-737-465 Fax: +-54-737-3385

More information

Churilova Maria Saint-Petersburg State Polytechnical University Department of Applied Mathematics

Churilova Maria Saint-Petersburg State Polytechnical University Department of Applied Mathematics Churilova Maria Saint-Petersburg State Polytechnical University Deartment of Alied Mathematics Technology of EHIS (staming) alied to roduction of automotive arts The roblem described in this reort originated

More information

Module 4. Analysis of Statically Indeterminate Structures by the Direct Stiffness Method. Version 2 CE IIT, Kharagpur

Module 4. Analysis of Statically Indeterminate Structures by the Direct Stiffness Method. Version 2 CE IIT, Kharagpur Module Analysis of Statically Indeterminate Structures by the Direct Stiffness Method Version CE IIT, Kharagur Lesson 9 The Direct Stiffness Method: Beams (Continued) Version CE IIT, Kharagur Instructional

More information

Chapter 5 Elastic Strain, Deflection, and Stability 1. Elastic Stress-Strain Relationship

Chapter 5 Elastic Strain, Deflection, and Stability 1. Elastic Stress-Strain Relationship Chapter 5 Elastic Strain, Deflection, and Stability Elastic Stress-Strain Relationship A stress in the x-direction causes a strain in the x-direction by σ x also causes a strain in the y-direction & z-direction

More information

Analysis of cold rolling a more accurate method

Analysis of cold rolling a more accurate method Analysis of cold rolling a more accurate method 1.1 Rolling of stri more accurate slab analysis The revious lecture considered an aroximate analysis of the stri rolling. However, the deformation zone in

More information

A Simple And Efficient FEM-Implementation Of The Modified Mohr-Coulomb Criterion Clausen, Johan Christian; Damkilde, Lars

A Simple And Efficient FEM-Implementation Of The Modified Mohr-Coulomb Criterion Clausen, Johan Christian; Damkilde, Lars Aalborg Universitet A Simle And Efficient FEM-Imlementation Of The Modified Mohr-Coulomb Criterion Clausen, Johan Christian; Damkilde, Lars Published in: Proceedings of the 9th Nordic Seminar on Comutational

More information

Design of Steel Structures Prof. S.R.Satish Kumar and Prof. A.R.Santha Kumar. Local buckling is an extremely important facet of cold formed steel

Design of Steel Structures Prof. S.R.Satish Kumar and Prof. A.R.Santha Kumar. Local buckling is an extremely important facet of cold formed steel 5.3 Local buckling Local buckling is an extremely important facet of cold formed steel sections on account of the fact that the very thin elements used will invariably buckle before yielding. Thinner the

More information

Chapter 3 Variational Formulation & the Galerkin Method

Chapter 3 Variational Formulation & the Galerkin Method Institute of Structural Engineering Page 1 Chapter 3 Variational Formulation & the Galerkin Method Institute of Structural Engineering Page 2 Today s Lecture Contents: Introduction Differential formulation

More information

NONLINEAR CONTINUUM FORMULATIONS CONTENTS

NONLINEAR CONTINUUM FORMULATIONS CONTENTS NONLINEAR CONTINUUM FORMULATIONS CONTENTS Introduction to nonlinear continuum mechanics Descriptions of motion Measures of stresses and strains Updated and Total Lagrangian formulations Continuum shell

More information

Damage Identification from Power Spectrum Density Transmissibility

Damage Identification from Power Spectrum Density Transmissibility 6th Euroean Worksho on Structural Health Monitoring - h.3.d.3 More info about this article: htt://www.ndt.net/?id=14083 Damage Identification from Power Sectrum Density ransmissibility Y. ZHOU, R. PERERA

More information

Nomenclature. Length of the panel between the supports. Width of the panel between the supports/ width of the beam

Nomenclature. Length of the panel between the supports. Width of the panel between the supports/ width of the beam omenclature a b c f h Length of the panel between the supports Width of the panel between the supports/ width of the beam Sandwich beam/ panel core thickness Thickness of the panel face sheet Sandwich

More information

Characteristics of Beam-Based Flexure Modules

Characteristics of Beam-Based Flexure Modules Shorya Awtar e-mail: shorya@mit.edu Alexander H. Slocum e-mail: slocum@mit.edu Precision Engineering Research Grou, Massachusetts Institute of Technology, Cambridge, MA 039 Edi Sevincer Omega Advanced

More information

Deformation Analysis of Ground Foundation Usage and theory of DACSAR

Deformation Analysis of Ground Foundation Usage and theory of DACSAR Deformation Analysis of Ground Foundation Usage and theory of DACSAR Visiting scholar in RCUSS of Kobe university Zhang Xiangxia 8-3-4 DACSARs: DACSAR (DACSAR-original) Oen to the ublic DACSAR-MC (DACSAR-udated)

More information

ENG2000 Chapter 7 Beams. ENG2000: R.I. Hornsey Beam: 1

ENG2000 Chapter 7 Beams. ENG2000: R.I. Hornsey Beam: 1 ENG2000 Chapter 7 Beams ENG2000: R.I. Hornsey Beam: 1 Overview In this chapter, we consider the stresses and moments present in loaded beams shear stress and bending moment diagrams We will also look at

More information

Computational Inelasticity FHLN05. Assignment A non-linear elasto-plastic problem

Computational Inelasticity FHLN05. Assignment A non-linear elasto-plastic problem Computational Inelasticity FHLN05 Assignment 2017 A non-linear elasto-plastic problem General instructions A written report should be submitted to the Division of Solid Mechanics no later than October

More information

VIBRATION ANALYSIS OF BEAMS WITH MULTIPLE CONSTRAINED LAYER DAMPING PATCHES

VIBRATION ANALYSIS OF BEAMS WITH MULTIPLE CONSTRAINED LAYER DAMPING PATCHES Journal of Sound and Vibration (998) 22(5), 78 85 VIBRATION ANALYSIS OF BEAMS WITH MULTIPLE CONSTRAINED LAYER DAMPING PATCHES Acoustics and Dynamics Laboratory, Deartment of Mechanical Engineering, The

More information

ANALYSIS OF ULTRA LOW CYCLE FATIGUE PROBLEMS WITH THE BARCELONA PLASTIC DAMAGE MODEL

ANALYSIS OF ULTRA LOW CYCLE FATIGUE PROBLEMS WITH THE BARCELONA PLASTIC DAMAGE MODEL XII International Conerence on Comutational Plasticity. Fundamentals and Alications COMPLAS XII E. Oñate, D.R.J. Owen, D. Peric and B. Suárez (Eds) ANALYSIS OF ULTRA LOW CYCLE FATIGUE PROBLEMS WITH THE

More information

INFLUENCE OF FLANGE STIFFNESS ON DUCTILITY BEHAVIOUR OF PLATE GIRDER

INFLUENCE OF FLANGE STIFFNESS ON DUCTILITY BEHAVIOUR OF PLATE GIRDER International Journal of Civil Structural 6 Environmental And Infrastructure Engineering Research Vol.1, Issue.1 (2011) 1-15 TJPRC Pvt. Ltd.,. INFLUENCE OF FLANGE STIFFNESS ON DUCTILITY BEHAVIOUR OF PLATE

More information

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

PURE BENDING. If a simply supported beam carries two point loads of 10 kn as shown in the following figure, pure bending occurs at segment BC. BENDING STRESS The effect of a bending moment applied to a cross-section of a beam is to induce a state of stress across that section. These stresses are known as bending stresses and they act normally

More information

97.398*, Physical Electronics, Lecture 8. Diode Operation

97.398*, Physical Electronics, Lecture 8. Diode Operation 97.398*, Physical Electronics, Lecture 8 Diode Oeration Lecture Outline Have looked at basic diode rocessing and structures Goal is now to understand and model the behavior of the device under bias First

More information

Finite Element Solutions for Geotechnical Engineering

Finite Element Solutions for Geotechnical Engineering Release Notes Release Date: June, 2017 Product Ver.: GTSNX 2017(v1.1) Integrated Solver Otimized for the next generation 64-bit latform Finite Element Solutions for Geotechnical Engineering 1. Analysis

More information

Implementation and Validation of Finite Volume C++ Codes for Plane Stress Analysis

Implementation and Validation of Finite Volume C++ Codes for Plane Stress Analysis CST0 191 October, 011, Krabi Imlementation and Validation of Finite Volume C++ Codes for Plane Stress Analysis Chakrit Suvanjumrat and Ekachai Chaichanasiri* Deartment of Mechanical Engineering, Faculty

More information

THEME IS FIRST OCCURANCE OF YIELDING THE LIMIT?

THEME IS FIRST OCCURANCE OF YIELDING THE LIMIT? CIE309 : PLASTICITY THEME IS FIRST OCCURANCE OF YIELDING THE LIMIT? M M - N N + + σ = σ = + f f BENDING EXTENSION Ir J.W. Welleman page nr 0 kn Normal conditions during the life time WHAT HAPPENS DUE TO

More information

Development of self-adaptively loading for planetary roller traction-drive transmission

Development of self-adaptively loading for planetary roller traction-drive transmission Available online www.jocr.com Journal of Chemical and Pharmaceutical Research, 013, 5(9):498-506 Research Article ISSN : 0975-7384 CODEN(USA) : JCPRC5 Develoment of self-adatively loading for lanetary

More information

PLASTIC COLLAPSE MECHANISMS IN COMPRESSED ELLIPTICAL HOLLOW SECTIONS

PLASTIC COLLAPSE MECHANISMS IN COMPRESSED ELLIPTICAL HOLLOW SECTIONS SDSS Rio 010 STABILITY AND DUCTILITY OF STEEL STRUCTURES E. Batista, P. Vellasco, L. de Lima (Eds.) Rio de Janeiro, Brazil, September 8-10, 010 PLASTIC COLLAPSE MECHANISMS IN COMPRESSED ELLIPTICAL HOLLOW

More information

Accordingly, the nominal section strength [resistance] for initiation of yielding is calculated by using Equation C-C3.1.

Accordingly, the nominal section strength [resistance] for initiation of yielding is calculated by using Equation C-C3.1. C3 Flexural Members C3.1 Bending The nominal flexural strength [moment resistance], Mn, shall be the smallest of the values calculated for the limit states of yielding, lateral-torsional buckling and distortional

More information

FEM simulation of a crack propagation in a round bar under combined tension and torsion fatigue loading

FEM simulation of a crack propagation in a round bar under combined tension and torsion fatigue loading FEM simulation of a crack roagation in a round bar under combined tension and torsion fatigue loading R.Citarella, M.Leore Det. of Industrial Engineering University of Salerno - Fisciano (SA), Italy. rcitarella@unisa.it

More information

Meshfree Inelastic Frame Analysis

Meshfree Inelastic Frame Analysis Theory & Results Louie L. Yaw, Sashi Kunnath and N. Sukumar University of California, Davis Department of Civil and Environmental Engineering Minisymposium 47 Recent Advances in Modeling of Engineering

More information

Load Capacity of Bodies and Structures

Load Capacity of Bodies and Structures Load Caacity of Bodies and Structures Reuven Segev Deartment of Mechanical Engineering Ben-Gurion University Structures of the Mechanics of Comlex Bodies October 27 Centro di Ricerca Matematica, Ennio

More information

A fatigue limit diagram for plastic rail clips

A fatigue limit diagram for plastic rail clips Computers in Railways XIV 839 A fatigue limit diagram for plastic rail clips S. Tamagawa, H. Kataoka & T. Deshimaru Department of Track Structures and Components, Railway Technical Research Institute,

More information

Engineering Fracture Mechanics

Engineering Fracture Mechanics Engineering Fracture Mechanics 90 (2012) 172 179 Contents lists available at SciVerse ScienceDirect Engineering Fracture Mechanics journal homeage: www.elsevier.com/locate/engfracmech Discussion of: Mode

More information

Characterization of Material Parameters

Characterization of Material Parameters Proceedings of the World Congress on Engineering 29 Vol II WCE 29, July 1-3, 29, London, U.K. Characterization of Material Parameters S. M. Humayun Kabir, Tae-In Yeo, Sang-Ho Kim Abstract The resent work

More information

Large inelastic deformation resistance of stiffened panels subjected to lateral loading

Large inelastic deformation resistance of stiffened panels subjected to lateral loading Large inelastic deformation resistance of stiffened anels subjected to lateral loading Zhaolong Yu a, b, Jørgen Amdahl a, b, Yanyan Sha a. Deartment of Marine Technology, oregian University of Science

More information

JEPPIAAR ENGINEERING COLLEGE

JEPPIAAR ENGINEERING COLLEGE JEPPIAAR ENGINEERING COLLEGE Jeppiaar Nagar, Rajiv Gandhi Salai 600 119 DEPARTMENT OFMECHANICAL ENGINEERING QUESTION BANK VI SEMESTER ME6603 FINITE ELEMENT ANALYSIS Regulation 013 SUBJECT YEAR /SEM: III

More information

FREE VIBRATION OF AXIALLY LOADED FUNCTIONALLY GRADED SANDWICH BEAMS USING REFINED SHEAR DEFORMATION THEORY

FREE VIBRATION OF AXIALLY LOADED FUNCTIONALLY GRADED SANDWICH BEAMS USING REFINED SHEAR DEFORMATION THEORY FREE VIBRATION OF AXIALLY LOADED FUNCTIONALLY GRADED SANDWICH BEAMS USING REFINED SHEAR DEFORMATION THEORY Thuc P. Vo 1, Adelaja Israel Osofero 1, Marco Corradi 1, Fawad Inam 1 1 Faculty of Engineering

More information

Composite bridge design (EN1994-2) Bridge modelling and structural analysis

Composite bridge design (EN1994-2) Bridge modelling and structural analysis EUROCODES Bridges: Background and applications Dissemination of information for training Vienna, 4-6 October 2010 1 Composite bridge design (EN1994-2) Bridge modelling and structural analysis Laurence

More information

ANALYSIS OF THE INTERACTIVE BUCKLING IN STIFFENED PLATES USING A SEMI-ANALYTICAL METHOD

ANALYSIS OF THE INTERACTIVE BUCKLING IN STIFFENED PLATES USING A SEMI-ANALYTICAL METHOD EUROSTEEL 2014, September 10-12, 2014, Naples, Italy ANALYSIS OF THE INTERACTIVE BUCKLING IN STIFFENED PLATES USING A SEMI-ANALYTICAL METHOD Pedro Salvado Ferreira a, Francisco Virtuoso b a Polytechnic

More information

PREDICTION MODEL FOR BURR FORMATION

PREDICTION MODEL FOR BURR FORMATION PREDICTION MODEL FOR BURR FORMATION Prof. Dr.-Ing. habil. Hans-Michael Beier FHTW Berlin Berlin, Germany dr.beier@beier-entgrattechnik.de Dil.-Ing. Reinhard Nothnagel Dr. Beier-Entgrattechnik Altlandsberg,

More information

Direct calculation of critical points in parameter sensitive systems

Direct calculation of critical points in parameter sensitive systems Direct calculation of critical points in parameter sensitive systems Behrang Moghaddasie a, Ilinca Stanciulescu b, a Department of Civil Engineering, Ferdowsi University of Mashhad, P.O. Box 91775-1111,

More information

Chapter 12 Elastic Stability of Columns

Chapter 12 Elastic Stability of Columns Chapter 12 Elastic Stability of Columns Axial compressive loads can cause a sudden lateral deflection (Buckling) For columns made of elastic-perfectly plastic materials, P cr Depends primarily on E and

More information

Flange Curling in Cold Formed Profiles

Flange Curling in Cold Formed Profiles Downloaded from orbit.dtu.dk on: Sep 4, 28 Flange Curling in Cold Formed Profiles Jönsson, Jeppe; Ramonas, Gediminas Published in: Proceedings of Nordic Steel Construction Conference 22 Publication date:

More information

A NUMERICAL MODEL OF FINITE DIFFERENCE (F.D) FOR DYNAMIC PILE DRIVING

A NUMERICAL MODEL OF FINITE DIFFERENCE (F.D) FOR DYNAMIC PILE DRIVING A NUMERICAL MODEL OF FINITE DIFFERENCE (F.D) FOR DYNAMIC PILE DRIVING *Amir Taban 1, Masoud Mirmohammad Sadeghi 2 and Mohammad Ali Roshan Zamir 3 1 Deartment of Civil Engineering, Isfahan (Khorasgan) Branch,

More information

Nonlinear Static Analysis of Cable Net Structures by Using Newton-Raphson Method

Nonlinear Static Analysis of Cable Net Structures by Using Newton-Raphson Method Nonlinear Static Analysis of Cable Net Structures by Using Newton-Rahson Method Sayed Mahdi Hazheer Deartment of Civil Engineering University Selangor (UNISEL) Selangor, Malaysia hazheer.ma@gmail.com Abstract

More information

Introduction to Continuous Systems. Continuous Systems. Strings, Torsional Rods and Beams.

Introduction to Continuous Systems. Continuous Systems. Strings, Torsional Rods and Beams. Outline of Continuous Systems. Introduction to Continuous Systems. Continuous Systems. Strings, Torsional Rods and Beams. Vibrations of Flexible Strings. Torsional Vibration of Rods. Bernoulli-Euler Beams.

More information

Nonlinear Thermo- Mechanics of Plates and Shallow Shells

Nonlinear Thermo- Mechanics of Plates and Shallow Shells Nonlinear Thermo- Mechanics of Plates and Shallow Shells Payam Khazaeinejad 1, Asif S. Usmani 1, Omar Laghrouche 1 IIE, School of Engineering, The University of Edinburgh IIE, School of the Built Environment,

More information

NON-LINEAR DYNAMIC BEHAVIOR OF THIN RECTANGULAR PLATES PARAMETRICALLY EXCITED USING THE ASYMPTOTIC METHOD, PART 2: COMPUTATION OF THE PHASE ANGLE

NON-LINEAR DYNAMIC BEHAVIOR OF THIN RECTANGULAR PLATES PARAMETRICALLY EXCITED USING THE ASYMPTOTIC METHOD, PART 2: COMPUTATION OF THE PHASE ANGLE Proceedings of the 9th WSEAS International Conference on Alied Mathematics, Istanbul, Turkey, May 7-9, 6 (9-99 NON-LINEAR DYNAMIC BEHAVIOR OF THIN RECTANGULAR PLATES PARAMETRICALLY EXCITED USING THE ASYMPTOTIC

More information

On Using FASTEM2 for the Special Sensor Microwave Imager (SSM/I) March 15, Godelieve Deblonde Meteorological Service of Canada

On Using FASTEM2 for the Special Sensor Microwave Imager (SSM/I) March 15, Godelieve Deblonde Meteorological Service of Canada On Using FASTEM2 for the Secial Sensor Microwave Imager (SSM/I) March 15, 2001 Godelieve Deblonde Meteorological Service of Canada 1 1. Introduction Fastem2 is a fast model (multile-linear regression model)

More information

Non-linear and time-dependent material models in Mentat & MARC. Tutorial with Background and Exercises

Non-linear and time-dependent material models in Mentat & MARC. Tutorial with Background and Exercises Non-linear and time-dependent material models in Mentat & MARC Tutorial with Background and Exercises Eindhoven University of Technology Department of Mechanical Engineering Piet Schreurs July 7, 2009

More information

DETERMINATION OF TRAIN SPEED LIMITS ON RENEWED TRACKS USING TAMPING MACHINE AND NUMERICAL OPTIMISATION

DETERMINATION OF TRAIN SPEED LIMITS ON RENEWED TRACKS USING TAMPING MACHINE AND NUMERICAL OPTIMISATION DETERMINATION O TRAIN SPEED LIMITS ON RENEWED TRACKS USING TAMPING MACHINE AND NUMERICAL OPTIMISATION V.L. Markine, C. Esveld Section of Road and Railway Engineering aculty of Civil Engineering, Delft

More information

Review of Strain Energy Methods and Introduction to Stiffness Matrix Methods of Structural Analysis

Review of Strain Energy Methods and Introduction to Stiffness Matrix Methods of Structural Analysis uke University epartment of Civil and Environmental Engineering CEE 42L. Matrix Structural Analysis Henri P. Gavin Fall, 22 Review of Strain Energy Methods and Introduction to Stiffness Matrix Methods

More information

THE USE OF DYNAMIC RELAXATION TO SOLVE THE DIFFERENTIAL EQUATION DESCRIBING THE SHAPE OF THE TALLEST POSSIBLE BUILDING

THE USE OF DYNAMIC RELAXATION TO SOLVE THE DIFFERENTIAL EQUATION DESCRIBING THE SHAPE OF THE TALLEST POSSIBLE BUILDING VII International Conference on Textile Composites and Inflatable Structures STRUCTURAL MEMBRANES 2015 E. Oñate, K.-U.Bletzinger and B. Kröplin (Eds) THE USE OF DYNAMIC RELAXATION TO SOLVE THE DIFFERENTIAL

More information

NONLOCAL PLASTICITY APPLIED TO BENDING OF BEAMS

NONLOCAL PLASTICITY APPLIED TO BENDING OF BEAMS IX International Conference on Computational Plasticity COMPLAS IX E. Oñate and D. R. J. Owen (Eds) CIMNE, Barcelona, 2007 NONLOCAL PLASTICITY APPLIED TO BENDING OF BEAMS L. Strömberg Div of Structural

More information

This is an author-deposited version published in: Eprints ID: 9322

This is an author-deposited version published in:   Eprints ID: 9322 Oen Archive Toulouse Archive Ouverte (OATAO) OATAO is an oen access reository that collects the work of Toulouse researchers and makes it freely available over the web where ossible. This is an author-deosited

More information

ELASTOPLASTIC STEEL BEAM BENDING ANALYSIS BY USING ABAQUS

ELASTOPLASTIC STEEL BEAM BENDING ANALYSIS BY USING ABAQUS 11 ELASTOPLASTIC STEEL BEAM BENDING ANALYSIS BY USING ABAQUS Biswajit Jena * * Corresponding author: biswa.tech88@gmail.com Abstract: In recent years tremendous efforts have been made in development of

More information

On the Prediction of Material Failure in LS-DYNA : A Comparison Between GISSMO and DIEM

On the Prediction of Material Failure in LS-DYNA : A Comparison Between GISSMO and DIEM 13 th International LS-YNA Users Conference Session: Constitutive Modeling On the Prediction of Material Failure in LS-YNA : A Comarison Between GISSMO and IEM Filie Andrade¹, Markus Feucht², Andre Haufe¹

More information

A consistent dynamic finite element formulation for a pipe using Euler parameters

A consistent dynamic finite element formulation for a pipe using Euler parameters 111 A consistent dynamic finite element formulation for a pipe using Euler parameters Ara Arabyan and Yaqun Jiang Department of Aerospace and Mechanical Engineering, University of Arizona, Tucson, AZ 85721,

More information

EMA 3702 Mechanics & Materials Science (Mechanics of Materials) Chapter 2 Stress & Strain - Axial Loading

EMA 3702 Mechanics & Materials Science (Mechanics of Materials) Chapter 2 Stress & Strain - Axial Loading MA 3702 Mechanics & Materials Science (Mechanics of Materials) Chapter 2 Stress & Strain - Axial Loading MA 3702 Mechanics & Materials Science Zhe Cheng (2018) 2 Stress & Strain - Axial Loading Statics

More information

Chapter 6: Cross-Sectional Properties of Structural Members

Chapter 6: Cross-Sectional Properties of Structural Members Chapter 6: Cross-Sectional Properties of Structural Members Introduction Beam design requires the knowledge of the following. Material strengths (allowable stresses) Critical shear and moment values Cross

More information

3. BEAMS: STRAIN, STRESS, DEFLECTIONS

3. BEAMS: STRAIN, STRESS, DEFLECTIONS 3. BEAMS: STRAIN, STRESS, DEFLECTIONS The beam, or flexural member, is frequently encountered in structures and machines, and its elementary stress analysis constitutes one of the more interesting facets

More information

AN EVALUATION OF A SIMPLE DYNAMICAL MODEL FOR IMPACTS BETWEEN RIGID OBJECTS

AN EVALUATION OF A SIMPLE DYNAMICAL MODEL FOR IMPACTS BETWEEN RIGID OBJECTS XIX IMEKO World Congress Fundamental and Alied Metrology Setember 6, 009, Lisbon, Portugal AN EVALUATION OF A SIMPLE DYNAMICAL MODEL FOR IMPACTS BETWEEN RIGID OBJECTS Erik Molino Minero Re, Mariano Lóez,

More information

MODELING OF MECHANICAL RESPONSE IN CFRP ANGLE-PLY LAMINATES

MODELING OF MECHANICAL RESPONSE IN CFRP ANGLE-PLY LAMINATES HE 9 H INERNAIONAL ONFERENE ON OMPOIE MAERIAL Introduction It is known that the failure rocess in angle-ly laminate involves matrix cracking and delamination and that they exhibit nonlinear stress-strain

More information