Higher-Order Finite-Element Analysis for Fuzes Subjected to High-Frequency Environments
|
|
- Lucy Dawson
- 5 years ago
- Views:
Transcription
1 Higher-Order Finite-Element Analysis for Fuzes Subjected to High-Frequency Environments Stephen Beissel Southwest Research Institute (210) Presented at: The 60 th Annual Fuze Conference 9-11 May, 2017 Cincinnati, OH Approved for Public Release 1
2 Outline Background Comparison of first-order and higher-order elements in explicit solid dynamics Finite-deformation plasticity Wave propagation Summary and Conclusions 2
3 Background Fuze components subjected to high-frequency waves steel case Al housing Reflections disrupt wave front fuze circuit boards electronics Impact generates wave front potting target 3
4 Background Lagrangian finite-element codes are industry standard for analysis of wave propagation Explicit time integration by central differences First-order elements Computations often can t resolve high-frequency modes, resulting in spurious oscillations (Gibbs phenomenon) Artificial viscosity damps oscillations and high-frequency modes Objective is to improve the accuracy of Lagrangian computations of wave propagation Systematic survey of numerical methods uncovered advantages of higher-order ( > 2 nd order) elements Higher-Order elements formulated and added to the EPIC code 4
5 Background Higher-order elements used successfully for years in CFD Higher-order elements not used for solid mechanics because: Computational efficiency of explicit schemes historically equated to minimizing the floating-point operations (FLOPS) in evaluation of internal-force term, and FLOPs increase with element order. Greater complexity of curved-surface contact algorithms Decades of research invested in various formulaic tradeoffs between locking and zero-energy modes of first-order elements Mass lumping of 2 nd -order serendipity elements yields vertex nodes with zero or negative: Masses Nodal forces due to uniform external traction Lack of meshing and visualization software for higher orders 5
6 Finite-deformation plasticity Square copper rod impacting a rigid surface at 200 m/s plastic strain symmetric order-1 tetrahedra non-symmetric order-1 tetrahedra order-1 hexahedra (Flanagan-Belytschko) 6
7 Finite-deformation plasticity Square copper rod impacting a rigid surface at 200 m/s plastic strain order-2 hexahedra order-3 hexahedra order-4 hexahedra 7
8 Finite-deformation plasticity No volumetric locking 8
9 Wave propagation in 2-D axisymmetry Baseline mesh of simple part loaded by a pulse monitored node near top 16 cm element size: 1x1 cm monitored node in base 4340 steel: c 1 = 5845 m/s c 2 = 4451 m/s 7 cm 5 m/s v z t pulse 2 ms t 9
10 Wave propagation in 2-D axisymmetry t = 5 µs 10 µs 15 µs 20 µs 25 µs 30 µs 35 µs 40 µs 45 µs 50 µs 55 µs 60 µs 65 µs 70 µs 75 µs 80 µs 85 µs 90 µs 95 µs 100 µs 10
11 Wave propagation in 2-D axisymmetry Velocities of node in base at equal mesh refinement 11
12 Wave propagation in 2-D axisymmetry Velocities of node in base at equal mesh refinement 12
13 Wave propagation in 2-D axisymmetry Velocities of node in base at equal mesh refinement 13
14 Wave propagation in 2-D axisymmetry Summary of errors at node in base (0-12 µs) 5x 10x 20x order = 5 40x 80x
15 Wave propagation in 2-D axisymmetry Convergence of top-node velocity with element order 15
16 Wave propagation in 2-D axisymmetry Convergence of top-node velocity with element order 16
17 Wave propagation in 2-D axisymmetry Convergence of top-node velocity with element order 17
18 Wave propagation in 2-D axisymmetry Convergence of top-node velocity with element order 18
19 Wave propagation in 2-D axisymmetry Convergence of top-node velocity with element order 19
20 Wave propagation in 2-D axisymmetry Convergence of top-node velocity with refinement of first-order quads 20
21 Wave propagation in 2-D axisymmetry Convergence of top-node velocity with refinement of first-order quads 21
22 Wave propagation in 2-D axisymmetry Convergence of top-node velocity with refinement of first-order quads 22
23 Wave propagation in 2-D axisymmetry Convergence of top-node velocity with refinement of first-order quads 23
24 Wave propagation in 2-D axisymmetry Convergence of top-node velocity with refinement of first-order quads 24
25 Wave propagation in 2-D axisymmetry Convergence of top-node velocity with refinement of first-order quads 25
26 Wave propagation in 2-D axisymmetry Convergence of top-node velocity with refinement of first-order quads 26
27 Wave propagation in 2-D axisymmetry Convergence of top-node velocity with refinement of first-order quads 27
28 Wave propagation in 2-D axisymmetry Convergence of top-node velocity with refinement of first-order triangles 28
29 Wave propagation in 2-D axisymmetry Convergence of top-node velocity with refinement of first-order triangles 29
30 Wave propagation in 2-D axisymmetry Convergence of top-node velocity with refinement of first-order triangles 30
31 Wave propagation in 2-D axisymmetry Convergence of top-node velocity with refinement of first-order triangles 31
32 Wave propagation in 2-D axisymmetry Convergence of top-node velocity with refinement of first-order triangles 32
33 Wave propagation in 2-D axisymmetry Convergence of top-node velocity with refinement of first-order triangles 33
34 Wave propagation in 2-D axisymmetry Convergence of top-node velocity with refinement of first-order triangles 34
35 Wave propagation in 2-D axisymmetry Comparison of velocity convergence with order and refinement 35
36 Wave propagation in 2-D axisymmetry Comparison of velocity convergence with order and refinement 36
37 Wave propagation in 2-D axisymmetry Comparison of velocity convergence with order and refinement 37
38 Wave propagation in 2-D axisymmetry Comparison of velocity convergence with order and refinement 38
39 (1) Wave propagation in 2-D axisymmetry Summary of errors in velocity at node near top 3x first-order quads 5x 3x 10x 7x 4x 15x 8x first-order triangles order = 3 20x 30x 12x 15x higher-order elements 4 40x 20x 5 80x 40x (1) Errors relative to data from 20 th - order elements for t = µs 39
40 (1) Wave propagation in 2-D axisymmetry Summary of errors in velocity at node near top 3x 3x 5x 4x 7x 10x 3 8x 15x 4 12x 20x order = x 10 30x (2) 20x (1) Errors relative to data from 20 th - order elements for t = µs (2) Intel Core i7: 2.93 GHz 15 GB RAM 40
41 (1) Wave propagation in 2-D axisymmetry Summary of errors in velocity at node near top 8x 3 15x 20x 12x 4 15x 30x order = 5 20x 40x (1) Errors relative to data from 20 th - order elements for t = µs 41
42 Wave propagation in 3D Baseline mesh of simple part loaded by a pulse monitored node (same location as 2D) mesh on plane of symmetry identical to 2-D mesh 5 m/s v z t v z t model differs from 2D due to facets along hoop direction 2 ms t 42
43 Wave propagation in 3D Comparison of 2-D and 3-D node velocities 43
44 Wave propagation in 3D Convergence of top-node velocity with element order 44
45 Wave propagation in 3D Convergence of top-node velocity with element order 45
46 Wave propagation in 3D Convergence of top-node velocity with element order 46
47 Wave propagation in 3D Convergence of top-node velocity with element order 47
48 Wave propagation in 3D Convergence of top-node velocity with refinement of first-order hexes 48
49 Wave propagation in 3D Convergence of top-node velocity with refinement of first-order hexes 49
50 Wave propagation in 3D Convergence of top-node velocity with refinement of first-order hexes 50
51 Wave propagation in 3D Convergence of top-node velocity with refinement of first-order hexes 51
52 Wave propagation in 3D Convergence of top-node velocity with refinement of first-order hexes 52
53 Wave propagation in 3D Convergence of top-node velocity with refinement of first-order hexes 53
54 Wave propagation in 3D Convergence of top-node velocity with refinement of first-order hexes 54
55 Wave propagation in 3D Convergence of top-node velocity with refinement of first-order hexes 55
56 Wave propagation in 3D Comparison of convergence with order and refinement 56
57 Wave propagation in 3D Comparison of convergence with order and refinement 57
58 Wave propagation in 3D Comparison of convergence with order and refinement 58
59 (1) Wave propagation in 3D Summary of velocity errors at monitored node 3x first-order hexahedra 7x 5x 4x 15x 12x 10x first-order quads order = 3 20x 3-D higher-order elements D higher-order elements (1) Errors relative to data from 7 th - order elements for t = µs 59
60 (1) Wave propagation in 3D Summary of velocity errors at monitored node 3x 4x 5x 2 7x 10x 12x order = (2) 6 (1) Errors relative to data from 7 th - order elements for t = µs (2) AMD Opteron: 2.31 GHz 15.7 GB RAM 60
61 (1) Wave propagation in 3D Summary of velocity errors at monitored node 3x 4x 5x 2 7x 10x 12x order = 3 15x (1) Errors relative to data from 7 th - order elements for t = µs 61
62 Summary and conclusions Analysis of wave propagation is essential to fuze design 1D, 2D and 3D higher-order elements have been formulated and implemented in EPIC The higher-order elements show no signs of volumetric locking Accuracy of higher-order elements is compared to standard first-order elements in simulations of wave propagation. Higher-order elements provide much greater accuracy at equal: Mesh refinement Computing time Allocated memory 62
63 Acknowledgment This work was funded by the DoD Joint Fuze Technology Program. 63
Simulation in Computer Graphics Elastic Solids. Matthias Teschner
Simulation in Computer Graphics Elastic Solids Matthias Teschner Outline Introduction Elastic forces Miscellaneous Collision handling Visualization University of Freiburg Computer Science Department 2
More informationCAEFEM v9.5 Information
CAEFEM v9.5 Information Concurrent Analysis Corporation, 50 Via Ricardo, Thousand Oaks, CA 91320 USA Tel. (805) 375 1060, Fax (805) 375 1061 email: info@caefem.com or support@caefem.com Web: http://www.caefem.com
More informationComputation Time Assessment of a Galerkin Finite Volume Method (GFVM) for Solving Time Solid Mechanics Problems under Dynamic Loads
Proceedings of the International Conference on Civil, Structural and Transportation Engineering Ottawa, Ontario, Canada, May 4 5, 215 Paper o. 31 Computation Time Assessment of a Galerkin Finite Volume
More informationTransactions on Engineering Sciences vol 1, 1993 WIT Press, ISSN
A contact algorithm for explicit dynamic FEM analysis E. Anderheggen", D. Ekchian", K. Heiduschke", P. Bartelt^ "Swiss Federal Institute of Technology, Honggerberg, CH-8093 Zurich, Switzerland %2 AG,
More informationDrop Test Simulation of a BGA Package: Methods & Experimental Comparison
Drop Test Simulation of a BGA Package: Methods & Experimental Comparison Chris Cowan, Ozen Engineering, Inc. Harvey Tran, Intel Corporation Nghia Le, Intel Corporation Metin Ozen, Ozen Engineering, Inc.
More informationNumerical Simulation and Experimental Study of Electromagnetic Forming
11 th International LS-DYNA Users Conference Metal Forming Numerical Simulation and Experimental Study of Electromagnetic Forming Jianhui Shang 1, Pierre L Eplattenier 2, Larry Wilkerson 1, Steve Hatkevich
More informationAbstract. 1 Introduction
Contact analysis for the modelling of anchors in concrete structures H. Walter*, L. Baillet** & M. Brunet* *Laboratoire de Mecanique des Solides **Laboratoire de Mecanique des Contacts-CNRS UMR 5514 Institut
More informationTowards Efficient Finite Element Model Review Dr. Richard Witasse, Plaxis bv (based on the original presentation of Dr.
Towards Efficient Finite Element Model Review Dr. Richard Witasse, Plaxis bv (based on the original presentation of Dr. Brinkgreve) Journée Technique du CFMS, 16 Mars 2011, Paris 1/32 Topics FEA in geotechnical
More informationCoupled 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 informationParticle Dynamics with MBD and FEA Using CUDA
Particle Dynamics with MBD and FEA Using CUDA Graham Sanborn, PhD Senior Research Engineer Solver 2 (MFBD) Team FunctionBay, Inc., S. Korea Overview MFBD: Multi-Flexible-Body Dynamics Rigid & flexible
More informationNUMERICAL MODELING OF ROCKET WARHEAD DETONATION AND FRAGMENTATION
NUMERICAL MODELING OF ROCKET WARHEAD DETONATION AND FRAGMENTATION Joseph D. Baum 1, G. Daniel Williams 1, G. Daniel Williams,Orlando A. Soto 1, Fumiya Togashi, and Rainald Löhner 2, 1 SAIC, 1710 SAIC Drive,
More informationSimulation of Impact Proof Testing of Electronic Sub- Systems
12 th International LS-DYNA Users Conference Blast/Impact(3) Simulation of Impact Proof Testing of Electronic Sub- Systems Paul Glance, PhD ME Naval Air Warfare Center Weapons Division China Lake, California
More informationUsing MATLAB and. Abaqus. Finite Element Analysis. Introduction to. Amar Khennane. Taylor & Francis Croup. Taylor & Francis Croup,
Introduction to Finite Element Analysis Using MATLAB and Abaqus Amar Khennane Taylor & Francis Croup Boca Raton London New York CRC Press is an imprint of the Taylor & Francis Croup, an informa business
More informationFinite Element Modeling and Analysis. CE 595: Course Part 2 Amit H. Varma
Finite Element Modeling and Analysis CE 595: Course Part 2 Amit H. Varma Discussion of planar elements Constant Strain Triangle (CST) - easiest and simplest finite element Displacement field in terms of
More informationCD40174BC CD40175BC Hex D-Type Flip-Flop Quad D-Type Flip-Flop
Hex D-Type Flip-Flop Quad D-Type Flip-Flop General Description The CD40174BC consists of six positive-edge triggered D- type flip-flops; the true outputs from each flip-flop are externally available. The
More informationCOMPUTATIONAL FLUID DYNAMICS (CFD) FOR THE OPTIMIZATION OF PRODUCTS AND PROCESSES
THE INTERNATIONAL CONFERENCE OF THE CARPATHIAN EURO-REGION SPECIALISTS IN INDUSTRIAL SYSTEMS 7 th EDITION COMPUTATIONAL FLUID DYNAMICS (CFD) FOR THE OPTIMIZATION OF PRODUCTS AND PROCESSES Franz, Haas DI
More informationChapter 2 Finite Element Formulations
Chapter 2 Finite Element Formulations The governing equations for problems solved by the finite element method are typically formulated by partial differential equations in their original form. These are
More informationSSNA109 - Tensile test with the model VISC_CIN2_CHAB
Titre : SSNA109 Essai de traction avec le modèle VISC_CI[...] Date : 03/08/2011 Page : 1/6 SSNA109 - Tensile test with the model VISC_CIN2_CHAB Summary: This test of nonlinear quasi-static mechanics makes
More informationMAE 323: Chapter 6. Structural Models
Common element types for structural analyis: oplane stress/strain, Axisymmetric obeam, truss,spring oplate/shell elements o3d solid ospecial: Usually used for contact or other constraints What you need
More informationModified Symmetry Cell Approach for Simulation of Surface Enhancement Over Large Scale Structures
Modified Symmetry Cell Approach for Simulation of Surface Enhancement Over Large Scale Structures T. Spradlin 1, R. Grandhi 2, and K. Langer 3 1 Doctoral Candidate, Wright State University, USA 2 Distinguished
More informationNumerical Simulations of the Mars Science! Laboratory Supersonic Parachute!
Numerical Simulations of the Mars Science! Laboratory Supersonic Parachute! Graham V. Candler! Vladimyr Gidzak! William L. Garrard! University of Minnesota! Keith Stein! Bethel University! Supported by
More informationUsing 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 informationAn Assessment of the LS-DYNA Hourglass Formulations via the 3D Patch Test
5 th European LS-DYNA Users Conference Code Developments An Assessment of the LS-DYNA Hourglass Formulations via the 3D Patch Test Authors Leonard E. Schwer, Schwer, Engineering & Consulting Services Samuel
More informationLevel 7 Postgraduate Diploma in Engineering Computational mechanics using finite element method
9210-203 Level 7 Postgraduate Diploma in Engineering Computational mechanics using finite element method You should have the following for this examination one answer book No additional data is attached
More informationThe following syntax is used to describe a typical irreducible continuum element:
ELEMENT IRREDUCIBLE T7P0 command.. Synopsis The ELEMENT IRREDUCIBLE T7P0 command is used to describe all irreducible 7-node enhanced quadratic triangular continuum elements that are to be used in mechanical
More informationINTRODUCCION AL ANALISIS DE ELEMENTO FINITO (CAE / FEA)
INTRODUCCION AL ANALISIS DE ELEMENTO FINITO (CAE / FEA) Title 3 Column (full page) 2 Column What is Finite Element Analysis? 1 Column Half page The Finite Element Method The Finite Element Method (FEM)
More informationPerformance Evaluation of Various Smoothed Finite Element Methods with Tetrahedral Elements in Large Deformation Dynamic Analysis
Performance Evaluation of Various Smoothed Finite Element Methods with Tetrahedral Elements in Large Deformation Dynamic Analysis Ryoya IIDA, Yuki ONISHI, Kenji AMAYA Tokyo Institute of Technology, Japan
More informationWeld Fracture. How Residual Stresses Affect Prediction of Brittle Fracture. Outline. Residual Stress in Thick Welds
How Residual Stresses ffect Prediction of Brittle Fracture Michael R. Hill University of California, Davis Tina L. Panontin NS-mes Research Center Weld Fracture Defects provide location for fracture initiation
More informationGame 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 informationINTRODUCTION TO THE EXPLICIT FINITE ELEMENT METHOD FOR NONLINEAR TRANSIENT DYNAMICS
INTRODUCTION TO THE EXPLICIT FINITE ELEMENT METHOD FOR NONLINEAR TRANSIENT DYNAMICS SHEN R. WU and LEI GU WILEY A JOHN WILEY & SONS, INC., PUBLICATION ! PREFACE xv PARTI FUNDAMENTALS 1 1 INTRODUCTION 3
More informationContent. Department of Mathematics University of Oslo
Chapter: 1 MEK4560 The Finite Element Method in Solid Mechanics II (January 25, 2008) (E-post:torgeiru@math.uio.no) Page 1 of 14 Content 1 Introduction to MEK4560 3 1.1 Minimum Potential energy..............................
More informationPREDICTIVE SIMULATION OF UNDERWATER IMPLOSION: Coupling Multi-Material Compressible Fluids with Cracking Structures
PREDICTIVE SIMULATION OF UNDERWATER IMPLOSION: Coupling Multi-Material Compressible Fluids with Cracking Structures Kevin G. Wang Virginia Tech Patrick Lea, Alex Main, Charbel Farhat Stanford University
More informationJEPPIAAR 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 informationBilinear Quadrilateral (Q4): CQUAD4 in GENESIS
Bilinear Quadrilateral (Q4): CQUAD4 in GENESIS The Q4 element has four nodes and eight nodal dof. The shape can be any quadrilateral; we ll concentrate on a rectangle now. The displacement field in terms
More informationBenchmark problems for wave propagation in elastic materials
DOI 10.1007/s00466-008-0346-3 ORIGINAL PAPER Benchmark problems for wave propagation in elastic materials A. Idesman H. Samajder E. Aulisa P. Seshaiyer Received: 13 May 2008 / Accepted: 20 October 2008
More informationFinite Element Modeling of Ultrasonic Transducers for Polymer Characterization
Excerpt from the Proceedings of the COMSOL Conference 2009 Milan Finite Element Modeling of Ultrasonic Transducers for Polymer Characterization Serena De Paolis *, Francesca Lionetto and Alfonso Maffezzoli
More informationGeometric nonlinear sensitivity analysis for nonparametric shape optimization with non-zero prescribed displacements
0 th World Congress on Structural and Multidisciplinary Optimization May 9-24, 203, Orlando, Florida, USA Geometric nonlinear sensitivity analysis for nonparametric shape optimization with non-zero prescribed
More informationNumerical Studies of Supersonic Jet Impingement on a Flat Plate
Numerical Studies of Supersonic Jet Impingement on a Flat Plate Overset Grid Symposium Dayton, OH Michael R. Brown Principal Engineer, Kratos/Digital Fusion Solutions Inc., Huntsville, AL. October 18,
More information6.4 A cylindrical specimen of a titanium alloy having an elastic modulus of 107 GPa ( psi) and
6.4 A cylindrical specimen of a titanium alloy having an elastic modulus of 107 GPa (15.5 10 6 psi) and an original diameter of 3.8 mm (0.15 in.) will experience only elastic deformation when a tensile
More informationMeshfree 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 informationCS470: Computer Architecture. AMD Quad Core
CS470: Computer Architecture Yashwant K. Malaiya, Professor malaiya@cs.colostate.edu AMD Quad Core 1 Architecture Layers Building blocks Gates, flip-flops Functional bocks: Combinational, Sequential Instruction
More informationThe Green Index (TGI): A Metric for Evalua:ng Energy Efficiency in HPC Systems
The Green Index (TGI): A Metric for Evalua:ng Energy Efficiency in HPC Systems Wu Feng and Balaji Subramaniam Metrics for Energy Efficiency Energy- Delay Product (EDP) Used primarily in circuit design
More informationME751 Advanced Computational Multibody Dynamics
ME751 Advanced Computational Multibody Dynamics October 24, 2016 Antonio Recuero University of Wisconsin-Madison Quote of the Day If a cluttered desk is a sign of a cluttered mind, of what, then, is an
More informationUniversity of Sheffield The development of finite elements for 3D structural analysis in fire
The development of finite elements for 3D structural analysis in fire Chaoming Yu, I. W. Burgess, Z. Huang, R. J. Plank Department of Civil and Structural Engineering StiFF 05/09/2006 3D composite structures
More informationChapter 5: Ball Grid Array (BGA)
Chapter 5: Ball Grid Array (BGA) 5.1 Development of the Models The following sequence of pictures explains schematically how the FE-model of the Ball Grid Array (BGA) was developed. Initially a single
More informationCreating Axisymmetric Models in FEMAP
Creating Axisymmetric Models in FEMAP 1. Introduction NE/Nastran does not support 2-d axisymmetric elements. 3-d axisymmetric models are supported, and can be generated with a few additional steps. The
More informationStresses Analysis of Petroleum Pipe Finite Element under Internal Pressure
ISSN : 48-96, Vol. 6, Issue 8, ( Part -4 August 06, pp.3-38 RESEARCH ARTICLE Stresses Analysis of Petroleum Pipe Finite Element under Internal Pressure Dr.Ragbe.M.Abdusslam Eng. Khaled.S.Bagar ABSTRACT
More informationNUMERICAL AND EXPERIMENTAL STUDY OF FAILURE IN STEEL BEAMS UNDER IMPACT CONDITIONS
Blucher Mechanical Engineering Proceedings May 2014, vol. 1, num. 1 www.proceedings.blucher.com.br/evento/10wccm NUMERICAL AND EXPERIMENTAL STUDY OF FAILURE IN STEEL BEAMS UNDER IMPACT CONDITIONS E. D.
More informationBack Matter Index The McGraw Hill Companies, 2004
INDEX A Absolute viscosity, 294 Active zone, 468 Adjoint, 452 Admissible functions, 132 Air, 294 ALGOR, 12 Amplitude, 389, 391 Amplitude ratio, 396 ANSYS, 12 Applications fluid mechanics, 293 326. See
More informationANSYS Explicit Dynamics Update. Mai Doan
ANSYS Explicit Dynamics Update Mai Doan Mai.Doan@ansys.com +1 512 687 9523 1/32 ANSYS Explicit Dynamics Update Outline Introduction Solve Problems that were Difficult or Impossible in the Past Structural
More informationBasics of Finite Element Analysis. Strength of Materials, Solid Mechanics
Basics of Finite Element Analysis Strength of Materials, Solid Mechanics 1 Outline of Presentation Basic concepts in mathematics Analogies and applications Approximations to Actual Applications Improvisation
More informationNon-Linear Finite Element Methods in Solid Mechanics Attilio Frangi, Politecnico di Milano, February 17, 2017, Lesson 5
Non-Linear Finite Element Methods in Solid Mechanics Attilio Frangi, attilio.frangi@polimi.it Politecnico di Milano, February 17, 2017, Lesson 5 1 Politecnico di Milano, February 17, 2017, Lesson 5 2 Outline
More informationNumerical Study: Time-Reversed Reciprocal Method and Damage Detection Method for Weld Fracture
Chapter 4 Numerical Study: Time-Reversed Reciprocal Method and Damage Detection Method for Weld Fracture A numerical study is performed to gain insight into applying the proposed method of detecting high-frequency
More informationSTRUCTURAL ANALYSIS OF A WESTFALL 2800 MIXER, BETA = 0.8 GFS R1. By Kimbal A. Hall, PE. Submitted to: WESTFALL MANUFACTURING COMPANY
STRUCTURAL ANALYSIS OF A WESTFALL 2800 MIXER, BETA = 0.8 GFS-411519-1R1 By Kimbal A. Hall, PE Submitted to: WESTFALL MANUFACTURING COMPANY OCTOBER 2011 ALDEN RESEARCH LABORATORY, INC. 30 Shrewsbury Street
More informationGeneral Guidelines for Crash Analysis in LS-DYNA. Suri Bala Jim Day. Copyright Livermore Software Technology Corporation
General Guidelines for Crash Analysis in LS-DYNA Suri Bala Jim Day Copyright Livermore Software Technology Corporation Element Shapes Avoid use of triangular shells, tetrahedrons, pentahedrons whenever
More informationAnalysis and Optimization of a Hybrid Fan Blade
Analysis and Optimization of a Hybrid Fan Blade Permas Users Conference 27.04.06 28.04.06 Strassbourg DLR German Aerospace Center, Stuttgart Institute of Structures and Design J. Ehrmanntraut, F. Kocian,
More informationBHAR AT HID AS AN ENGIN E ERI N G C O L L E G E NATTR A MPA LL I
BHAR AT HID AS AN ENGIN E ERI N G C O L L E G E NATTR A MPA LL I 635 8 54. Third Year M E C H A NICAL VI S E M ES TER QUE S T I ON B ANK Subject: ME 6 603 FIN I T E E LE ME N T A N A L YSIS UNI T - I INTRODUCTION
More information3. Numerical integration
3. Numerical integration... 3. One-dimensional quadratures... 3. Two- and three-dimensional quadratures... 3.3 Exact Integrals for Straight Sided Triangles... 5 3.4 Reduced and Selected Integration...
More informationEXTENDED ABSTRACT. Dynamic analysis of elastic solids by the finite element method. Vítor Hugo Amaral Carreiro
EXTENDED ABSTRACT Dynamic analysis of elastic solids by the finite element method Vítor Hugo Amaral Carreiro Supervisor: Professor Fernando Manuel Fernandes Simões June 2009 Summary The finite element
More informationN = 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 informationAnalysis of forming Upper bound analysis
Analysis of forming Upper bound analysis Slip line field analysis has limited application in forming in view of its applicability to plane strain deformation only. A more accurate and general analysis
More informationDue Monday, November 16 th, 12:00 midnight
Due Monday, November 16 th, 12:00 midnight This homework is considering the finite element analysis of transient and dynamic FEM analysis. You are asked to include transient and/dynamic effects to MatLab
More informationFINITE ELEMENT SIMULATION OF ROLL FORMING OF HIGH STRENGTH STEEL
FINITE ELEMENT SIMULATION OF ROLL FORMING OF HIGH STRENGTH STEEL Author: Joakim Lempiäinen Roll forming of high strength sheet steel, using explicit FE simulations has been analyzed in terms of the state
More informationFinite 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 informationValidation of LS-DYNA MMALE with Blast Experiments
12 th International LS-DYNA Users Conference Blast/Impact(3) Validation of LS-DYNA MMALE with Blast Experiments Yuli Huang and Michael R. Willford Arup, San Francisco, CA 94116 Leonard E. Schwer Schwer
More informationThe Finite Element Method for Mechonics of Solids with ANSYS Applicotions
The Finite Element Method for Mechonics of Solids with ANSYS Applicotions ELLIS H. DILL 0~~F~~~~"P Boca Raton London New Vork CRC Press is an imprint 01 the Taylor & Francis Group, an Informa business
More informationInterpolation Functions for General Element Formulation
CHPTER 6 Interpolation Functions 6.1 INTRODUCTION The structural elements introduced in the previous chapters were formulated on the basis of known principles from elementary strength of materials theory.
More informationPost Graduate Diploma in Mechanical Engineering Computational mechanics using finite element method
9210-220 Post Graduate Diploma in Mechanical Engineering Computational mechanics using finite element method You should have the following for this examination one answer book scientific calculator No
More informationNUMERICAL ANALYSIS OF PASSIVE EARTH PRESSURES WITH INTERFACES
III European Conference on Computational Mechanics Solids, Structures and Coupled Problems in Engineering C.A. Mota Soares et.al. (eds.) Lisbon, Portugal, 5-8 June 2006 NUMERICAL ANALYSIS OF PASSIVE EARTH
More informationMultiscale modeling and simulation of shock wave propagation
University of Iowa Iowa Research Online Theses and Dissertations Spring 2013 Multiscale modeling and simulation of shock wave propagation Cory Nelsen University of Iowa Copyright 2013 Cory Nelsen This
More informationFEA A Guide to Good Practice. What to expect when you re expecting FEA A guide to good practice
FEA A Guide to Good Practice What to expect when you re expecting FEA A guide to good practice 1. Background Finite Element Analysis (FEA) has transformed design procedures for engineers. Allowing more
More informationStudy of the hydrodynamic flow around a 70m sailing boat for powering, wave pattern and propeller efficiency prediction
Study of the hydrodynamic flow around a 70m sailing boat for powering, wave pattern and propeller efficiency prediction Romain Baudson Supervisor: Prof. Dario Boote (UNIGE) External Reviewer: Prof. Pierre
More informationA FINITE ELEMENT STUDY OF ELASTIC-PLASTIC HEMISPHERICAL CONTACT BEHAVIOR AGAINST A RIGID FLAT UNDER VARYING MODULUS OF ELASTICITY AND SPHERE RADIUS
Proceedings of the International Conference on Mechanical Engineering 2009 (ICME2009) 26-28 December 2009, Dhaka, Bangladesh ICME09- A FINITE ELEMENT STUDY OF ELASTIC-PLASTIC HEMISPHERICAL CONTACT BEHAVIOR
More informationfield using second order edge elements in 3D
The current issue and full text archive of this journal is available at http://www.emerald-library.com using second order edge elements in 3D Z. Ren Laboratoire de GeÂnie Electrique de Paris, UniversiteÂs
More informationPresentation Outline
Parallel Multi-Zone Methods for Large- Scale Multidisciplinary Computational Physics Simulations Ding Li, Guoping Xia and Charles L. Merkle Purdue University The 6th International Conference on Linux Clusters
More informationDynamic Analysis Contents - 1
Dynamic Analysis Contents - 1 TABLE OF CONTENTS 1 DYNAMIC ANALYSIS 1.1 Overview... 1-1 1.2 Relation to Equivalent-Linear Methods... 1-2 1.2.1 Characteristics of the Equivalent-Linear Method... 1-2 1.2.2
More informationSTAR-CCM+: NACA0012 Flow and Aero-Acoustics Analysis James Ruiz Application Engineer January 26, 2011
www.cd-adapco.com STAR-CCM+: NACA0012 Flow and Aero-Acoustics Analysis James Ruiz Application Engineer January 26, 2011 Introduction The objective of this work is to prove the capability of STAR-CCM+ as
More informationStatic and Modal Analysis of Telescope Frame in Satellite
Abstract Static and Modal Analysis of Telescope Frame in Satellite Sun Libin Department of Mechanical Engineering Tsinghua University Feng Hui School of Material Science and Engineering University of Science
More information3D Observations of Electromagnetic Ion Cyclotron Wave Propagation. in a Laboratory Plasma Column
3D Observations of Electromagnetic Ion Cyclotron Wave Propagation in a Laboratory Plasma Column Stephen T. Vincena and Walter N. Gekelman University of California, Los Angeles Department of Physics LAPD
More informationAnalysis of a Casted Control Surface using Bi-Linear Kinematic Hardening
Analysis of a Casted Control Surface using Bi-Linear Kinematic Hardening Abdul Manan Haroon A. Baluch AERO, P.O Box 91, Wah Cantt. 47040 Pakistan Abstract Control Surfaces or Fins are very essential parts
More informationNUMERICAL SIMULATION OF BLAST RESISTANT STEEL PLATE STRENGTHENED WITH COMPOSITE
Journal of KONES Powertrain and Transport, Vol. 18, No. 3 2011 NUMERICAL SIMULATION OF BLAST RESISTANT STEEL PLATE STRENGTHENED WITH COMPOSITE Krzysztof Kosiuczenko, Tadeusz Niezgoda, Wies aw Barnat, Robert
More informationDevelopment and Validation of the FAT Finite Element Model for the Side Impact Dummy EUROSID-1
Development and Validation of the FAT Finite Element Model for the Side Impact Dummy EUROSID-1 Thomas Pyttel* *ESI GmbH, 65760 Eschborn, Frankfurter Str. 13-15, Germany ABSTRACT A new deformable model
More informationAn Energy Dissipative Constitutive Model for Multi-Surface Interfaces at Weld Defect Sites in Ultrasonic Consolidation
An Energy Dissipative Constitutive Model for Multi-Surface Interfaces at Weld Defect Sites in Ultrasonic Consolidation Nachiket Patil, Deepankar Pal and Brent E. Stucker Industrial Engineering, University
More informationIMPACT PROPERTY AND POST IMPACT VIBRATION BETWEEN TWO IDENTICAL SPHERES
ICSV4 Cairns Australia 9- July, 7 IMPACT PROPERTY AND POST IMPACT VIBRATION BETWEEN TWO IDENTICAL SPHERES Hirofumi MINAMOTO, Keisuke SAITOH and Shozo KAWAMURA Toyohashi University of Technology Dept. of
More information2. Polynomial interpolation
2. Polynomial interpolation Contents 2. POLYNOMIAL INTERPOLATION... 1 2.1 TYPES OF INTERPOLATION... 1 2.2 LAGRANGE ONE-DIMENSIONAL INTERPOLATION... 2 2.3 NATURAL COORDINATES*... 15 2.4 HERMITE ONE-DIMENSIONAL
More informationStructural Dynamics. Spring mass system. The spring force is given by and F(t) is the driving force. Start by applying Newton s second law (F=ma).
Structural Dynamics Spring mass system. The spring force is given by and F(t) is the driving force. Start by applying Newton s second law (F=ma). We will now look at free vibrations. Considering the free
More informationHigh Order Discontinuous Galerkin Methods for Aerodynamics
High Order Discontinuous Galerkin Methods for Aerodynamics Per-Olof Persson Massachusetts Institute of Technology Collaborators: J. Peraire, J. Bonet, N. C. Nguyen, A. Mohnot Symposium on Recent Developments
More informationParticles Removal from a Moving Tube by Blowing Systems: A CFD Analysis
Engineering, 2013, 5, 268-276 http://dx.doi.org/10.4236/eng.2013.53037 Published Online March 2013 (http://www.scirp.org/journal/eng) Particles Removal from a Moving Tube by Blowing Systems: A CFD Analysis
More informationProceedings of the ASME th International Conference on Ocean, Offshore and Arctic Engineering OMAE2016 June 19-24, 2016, Busan, South Korea
Proceedings of the ASME 26 35th International Conference on Ocean, Offshore and Arctic Engineering OMAE26 June 9-24, 26, Busan, South Korea OMAE26-54554 LOCAL STRAIN AND STRESS CALCULATION METHODS OF IRREGULAR
More informationLHC Collimators for Phase 1
The LHC Collimation project LHC Collimators for Phase 1 Effects of the 450GeV accident case (TT40 experiment) on the jaw metal support (preliminary report) 71st Collimator design meeting 01/09/2005 Alessandro
More informationExample 37 - Analytical Beam
Example 37 - Analytical Beam Summary This example deals with the use of RADIOSS linear and nonlinear solvers. A beam submitted to a concentrated load on one extremity and fixed on the other hand is studied.
More informationConstitutive models. Constitutive model: determines P in terms of deformation
Constitutive models Constitutive model: determines P in terms of deformation Elastic material: P depends only on current F Hyperelastic material: work is independent of path strain energy density function
More informationmidas NFX 2015 R1 Release Note
Total Solution for True Analysis-driven Design midas NFX 2015 R1 Release Note 1 midas NFX R E L E A S E N O T E 2 0 1 5 R 1 Accurate whenever you Need Be more efficient by focusing on the right details
More informationLab 5: Post Processing and Solving Conduction Problems. Objective:
Lab 5: Post Processing and Solving Conduction Problems Objective: The objective of this lab is to use the tools we have developed in MATLAB and SolidWorks to solve conduction heat transfer problems that
More informationTheoretical Manual Theoretical background to the Strand7 finite element analysis system
Theoretical Manual Theoretical background to the Strand7 finite element analysis system Edition 1 January 2005 Strand7 Release 2.3 2004-2005 Strand7 Pty Limited All rights reserved Contents Preface Chapter
More informationNon-linear fracture mechanics in LS-DYNA and LS-PrePost
Non-linear fracture mechanics in LS-DYNA and LS-PrePost Per Lindström 1,, Anders Jonsson 3, Anders Jernberg 3, Erling Østby 1 Department of Engineering Science, University West, Trollhättan, Sweden DNV
More informationFlow-Induced Vibration Modeling
Flow-Induced Vibration Modeling Bin Zhu, Hector H. Mireles, and Aqib Qureshi Baker Hughes Abstract: The current work pertains to a re-closeable annular flow valve oil completion tool (X- AFV) with high
More informationSimulation of Piezoelectric Induced Lamb Waves in Plates
Simulation of Piezoelectric Induced Lamb Waves in Plates C. WILLBERG, J. M. VIVAR-PEREZ, Z. AHMAD and U. GABBERT ABSTRACT The use of Lamb waves for damage detection and non-destructive evaluation have
More informationFluid-Structure Interaction Problems using SU2 and External Finite-Element Solvers
Fluid-Structure Interaction Problems using SU2 and External Finite-Element Solvers R. Sanchez 1, D. Thomas 2, R. Palacios 1, V. Terrapon 2 1 Department of Aeronautics, Imperial College London 2 Department
More informationInterpretation of Pile Integrity Test (PIT) Results
Annual Transactions of IESL, pp. 78-84, 26 The Institution of Engineers, Sri Lanka Interpretation of Pile Integrity Test (PIT) Results H. S. Thilakasiri Abstract: A defect present in a pile will severely
More information