Topology Optimization Mathematics for Design

Similar documents
Topology Optimization OPTISHAPE

Computational Analysis for Composites

Topology Optimization Using the SIMP Method

Mechanical Engineering Ph.D. Preliminary Qualifying Examination Solid Mechanics February 25, 2002

202 Index. failure, 26 field equation, 122 force, 1

Finite Element Method in Geotechnical Engineering

FEA A Guide to Good Practice. What to expect when you re expecting FEA A guide to good practice

Topology Optimization of Compliant Mechanism with Geometrical Advantage

Integration simulation method concerning speed control of ultrasonic motor

Structural Optimization. for Acoustic Disciplines

Verification of Shell Elements by Eigenanalysis of Vibration Problems

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

EQUIVALENT FRACTURE ENERGY CONCEPT FOR DYNAMIC RESPONSE ANALYSIS OF PROTOTYPE RC GIRDERS

University of Sheffield The development of finite elements for 3D structural analysis in fire

ME 475 Modal Analysis of a Tapered Beam

Lecture 8. Stress Strain in Multi-dimension

Composite Structures- Modeling, FEA, Optimization and Diagnostics

CHAPTER 5. Beam Theory

Finite Element Analysis Lecture 1. Dr./ Ahmed Nagib

Post Graduate Diploma in Mechanical Engineering Computational mechanics using finite element method

Laminated Composite Plates and Shells

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

Emerging Technology in Optimization An Image Based Approach for CAE

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

FEM Validation. 12th January David Schmid Teamleader Structural Analysis

Stresses Analysis of Petroleum Pipe Finite Element under Internal Pressure

Modelling the behaviour of plastics for design under impact

SEMM Mechanics PhD Preliminary Exam Spring Consider a two-dimensional rigid motion, whose displacement field is given by

Practice Final Examination. Please initial the statement below to show that you have read it

ME FINITE ELEMENT ANALYSIS FORMULAS

DEPARTMENT OF MECHANICAL ENIGINEERING, UNIVERSITY OF ENGINEERING & TECHNOLOGY LAHORE (KSK CAMPUS).

Content. Department of Mathematics University of Oslo

#SEU16. FEA in Solid Edge and FEMAP Mark Sherman

Elastoplastic Deformation in a Wedge-Shaped Plate Caused By a Subducting Seamount

Performance Evaluation of Various Smoothed Finite Element Methods with Tetrahedral Elements in Large Deformation Dynamic Analysis

Finite Element Method

Static and Modal Analysis of Telescope Frame in Satellite

3. Overview of MSC/NASTRAN

Stress Analysis of Radial and Non- Radial Nozzle Connections in Ellipsoidal Head Pressure Vessel

Interior-Point Method for the Computation of Shakedown Loads for Engineering Systems

Free-form Optimization Method for Designing Spatial Frame Structure

CHAPTER 4 DESIGN AND ANALYSIS OF CANTILEVER BEAM ELECTROSTATIC ACTUATORS

A Study on the Tube of Integral Propeller Shaft for the Rear-wheel Drive Automobile Using Carbon Composite Fiber

Discrete Analysis for Plate Bending Problems by Using Hybrid-type Penalty Method

3 2 6 Solve the initial value problem u ( t) 3. a- If A has eigenvalues λ =, λ = 1 and corresponding eigenvectors 1

Plates and Shells: Theory and Computation. Dr. Mostafa Ranjbar

Stress and Displacement Analysis of a Rectangular Plate with Central Elliptical Hole

ANALYSIS AND NUMERICAL MODELLING OF CERAMIC PIEZOELECTRIC BEAM BEHAVIOR UNDER THE EFFECT OF EXTERNAL SOLICITATIONS

Advanced Friction Modeling in Sheet Metal Forming

Experimental Modal Analysis of a Flat Plate Subjected To Vibration

Mechanical Properties

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

Eshan V. Dave, Secretary of M&FGM2006 (Hawaii) Research Assistant and Ph.D. Candidate. Glaucio H. Paulino, Chairman of M&FGM2006 (Hawaii)

Two Tier projects for students in ME 160 class

Tolerance Ring Improvement for Reducing Metal Scratch

SIZE EFFECTS IN THE COMPRESSIVE CRUSHING OF HONEYCOMBS

Aluminum shell. Brass core. 40 in

Stress analysis of a stepped bar

FREE VIBRATION ANALYSIS OF THIN CYLINDRICAL SHELLS SUBJECTED TO INTERNAL PRESSURE AND FINITE ELEMENT ANALYSIS

Strain Gages. Approximate Elastic Constants (from University Physics, Sears Zemansky, and Young, Reading, MA, Shear Modulus, (S) N/m 2

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

Topology Optimization of Low Frequency Structure with Application to Vibration Energy Harvester

MODELLING BAMBOO AS A FUNCTIONALLY GRADED MATERIAL

THE EFFECT OF GEOMETRY ON FATIGUE LIFE FOR BELLOWS

Characterization of MEMS Devices

DISPENSA FEM in MSC. Nastran

Dynamic (Vibrational) and Static Structural Analysis of Ladder Frame

Stress analysis of functionally graded discs under mechanical and thermal loads

ROBUST DESIGN OF A MECHANICAL LATCH

Thermal buckling and post-buckling of laminated composite plates with. temperature dependent properties by an asymptotic numerical method

LINEAR AND NONLINEAR BUCKLING ANALYSIS OF STIFFENED CYLINDRICAL SUBMARINE HULL

The Analysis of Aluminium Cantilever Beam with Piezoelectric Material by changing Position of piezo patch over Length of Beam

JEPPIAAR ENGINEERING COLLEGE

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

INFLUENCE OF FLANGE STIFFNESS ON DUCTILITY BEHAVIOUR OF PLATE GIRDER

VIBRATION CONTROL OF RECTANGULAR CROSS-PLY FRP PLATES USING PZT MATERIALS

DYNAMIC RESPONSE OF SYNTACTIC FOAM CORE SANDWICH USING A MULTIPLE SCALES BASED ASYMPTOTIC METHOD

FINITE ELEMENT APPROACHES TO MESOSCOPIC MATERIALS MODELING

The Rotating Inhomogeneous Elastic Cylinders of. Variable-Thickness and Density

EVALUATING RADIATION DAMPING OF SHALLOW FOUNDATIONS ON NONLINEAR SOIL MEDIUM FOR SOIL-STRUCTURE INTERACTION ANALYSIS OF BRIDGES

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

Design and Analysis of Various Microcantilever Shapes for MEMS Based Sensing

3D Elasticity Theory

Aircraft Stress Analysis and Structural Design Summary

HEALTH MONITORING OF PLATE STRUCTURE USING PIEZO ELECTRIC PATCHES AND CURVATURE MODE SHAPE

EMEA. Liudmila Feoktistova Engineer Atomenergoproekt

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

International Journal of Advanced Engineering Technology E-ISSN

Fracture Test & Fracture Parameters of Self Compacting Concrete using ANSYS. Zeel Vashi 1,Megha Thomas 2 I. INTRODUCTION

Mechanics of Materials II. Chapter III. A review of the fundamental formulation of stress, strain, and deflection

VIBRATION ANALYSIS OF AN AUTOMOTIVE SILENCER

Strain Gages. Approximate Elastic Constants (from University Physics, Sears Zemansky, and Young, Reading, MA, 1979

ANSYS Explicit Dynamics Update. Mai Doan

Lecture 15: Revisiting bars and beams.

ABHELSINKI UNIVERSITY OF TECHNOLOGY

VIBRATION PROBLEMS IN ENGINEERING

DYNAMIC MODELING OF SPOT WELDS USING THIN LAYER INTERFACE THEORY

An orthotropic damage model for crash simulation of composites

Design of in-plane piezoelectric sensors for static response by simultaneously optimizing the host structure and the electrode profile

Correction of local-linear elasticity for nonlocal residuals: Application to Euler-Bernoulli beams

Transcription:

Topology Optimization Mathematics for Design Homogenization Design Method (HMD) Why topology? Change in shape & size may not lead our design criterion for reduction of structural weight. 1

Structural Design 3 Sets of Problems Sizing Optimization thickness of a plate or membrane height, width, radius of the cross section of a beam Shape Optimization outer/inner shape Topology Optimization number of holes configuration Shape of the Outer Boundary hole 2 hole 1 thickness distribution Location of the Control Point of a Spline Sizing Optimization Starting of Design Optimization 1950s : Fully Stressed Design σ = σ allowable in a structure 1960s : Mathematical Programming ( L. Schmit at UCLA ) min σ σ u u allowable max Total Weight Design Sensitivity Analysis 2

Equilibrium : State Equation Design Sensitivity Ku = f Dg g u g = + Dd d d u Design Velocity Sensitivity Performance Functions g K u f Ku = f u + K = d d d Dg g 1 K f g = + K u+ Dd d d d u Typical Performance Functions Strain Energy Density For Structural Design (This must be constant!) Mises Equivalent Stress For Strength Design and Failure Analysis Mean Compliance & Maximum Displacement For Stiffness Design Maximum Strain For Formability Study of Sheet Metals 3

Hemp in 1950s Size to Topology Eliminate unnecessary bars by designing the cross sectional area. An Optimization Algorithm Ku= f σe σ u u E, A min i allowable max N max e= 1 ρ AL e e e P1 P2 Design Sensitivity K u K f = u + A A A σ DBu = DB u e e e e e = e e A A A e u i A e b e e e e u u = i i u A i e g e 4

Prager in 1960s Design Optimization Theory Maximizing the minimum total potential energy 1 Π= Π = Ne Ne T T e e e e e e e= 1 e= 1 2 d K d d f max design A e min Π de Leads Equilibrium Why Total Potential? Maximizing the Global Stiffness Minimizing the mean compliance (Prager) when forces are applied T min ufs design max design T s u f Maximizing the mean compliance when displacement is specified 5

Lagrangian Variation NE NE 1 T T L= de Kede de fe + λ ρeaele W 2 e= 1 e= 1 Total Potential Energy Weight Constraint NE T 1 T K e δl= δd ( K d f ) + d d λρ L δ A e= 1 2 Ae e e e e e e e e e NE + δλ ρeal e e W e= 1 Kd = f e e e Optimality Condition 1 d 2 N E e= 1 K T e e de e e Ae ρ AL e e e + λρ L = 0 W 0 1 T 1 de 2 ρ L Something must be Constant! K A e e e e d e = λ 6

Physical Meaning Strain Energy Density Must be Constant 1 T 1 de 2 ρ L K A e e e 1 T 1 d K d 2 ρeal e e e d e e e Weight Average of the Stiffness e = λ Prager s Condition = λ Example 1 7

Example 2 160 Design Domain 100 (a) Single Loading (b) Multiple Loading Example 3 200 Design Domain 100 Applying Torque 100 8

TOPODANUKI A Topology Optimization Soft Toyota Central R&D Labs. Making up a grand-structure 9

Set up support and load conditions Only a bending load is applied 10

Two Loads are applied Further Development First Order Analysis in Toyota Central R&D Microsoft EXCEL Based Software 11

12

13

14

Extension to Continuum Characteristic Function Ω Ω = unknown optimum domain D = specified fixed domain D χ Ω axf = RST 1 0 if x Ω if x Ω i.e. x D \ Ω What can we get from this? Optimal Material Distribution Strain Energy of a Body 1 T 1 T U = 2 ε DεdΩ= χ 2 D Ω dd Ω ε Dε Shape Design = σ Material Design = D new Find the best Ω Find the best D new 15

Homogenization Design Method Shape and Topology Design of Structures is transferred to Material Distribution Design (Bendsoe and Kikuchi, 1988) Homogenization Method : Mathematics t Γ t Y Unit cell Ω b Γ X Γ g Unit cell Review Under the assumption of periodic microstructures which can be represented by unit cells. Using the asymptotic expansion of all variables and the average technique to determine the homogenized material properties and constitutive relations of composite materials. 16

HDM Test Problem Design Domain 40 Nondesign Domain R10 P 20 15 support 20 55 Starting from Uniform Perforation 17

18

19

4.400 4.200 4.000 3.800 3.600 3.400 3.200 3.000 Design Process Structural Formation Process Convergence History of Iteration 2.800 0 10 20 30 40 50 Ieration 20

Mesh Refinement 21

22

Change Volumes 23

Design Constraint Displacement fixed along circle Design area Load case 1 No design area (Full material) Load case 3 Load case 2 100 Design area 20 2 10 40 No design area (Full material) (Same boundary condition) No design area (No material) 24

Result of Design Constraint Influence of Design Domain 12 2 2 1.25 Design Domain 5 1.25 Non-design Domain 1.25 Design Domain 5 1.25 0.5 12 0.5 25

Different Topology Shape Design Example 20 60 10 30 26

Shape to Topology Extension to Shells Rib Formation P 20 20 30 20 10 h 0 =0.1 h 1 =1.0 27

Commercialization of HMD From University to Industry Three-dimensional shaping of a structure for Optimum without any spline functions OPTISHAPE Development 1986~1989 Acceptance Topology Optimization Methods Commercial Codes have been developed in USA, Europe, and Pacific Regions OPTISHAPE@Quint Corporation, Tokyo, Japan, 1989 OPTISTRUCT@Altair Computing, Troy, USA, 1996 MSC/CONSTRUCT@MSC German, 1997 And Others (OPTICON, ANSYS,..) 28

MSC/NASTRAN-OPTISHAPE Quint/OPTISHAPE + MSC/NASTRAN Shape and Topology Optimization Static Global Stiffness Maximization Maximizing the Mean Eigenvalues Frequency Control for Free Vibration Increase of the Critical Load MSC/PATRAN integration Developed by MSC Japan and Quint Corp. Static/Dynamic Stiffness Maximization 29

MSC/PATRAN GUI Environment MSC/NASTRAN Solver Design Example by MSC.NASTRAN-OPTISHAPE 30

Integration with Shape Optimization Prof. Azegami s Method Initial Design Optimized Shape Design Optimization by MSC.NASTRAN-OPTISHAPE 31

Compliant Mechanism Design by QUINT/OPTISHAPE Application of QUINT/OPTISHAPE @ Kanto Automotive 32

Altair: Altair: Concept Concept Design Design Environment Environment Product Product Design Design Synthesis Synthesis System Level Requirements Package Space Topology Optimization Control Arm Development Example Surface Geometry Generation Size and Shape Optimization Parametric Shape Vectors Finite Element Modeling Altair/OptiStruct Input: FE model of design space Load cases, frequencies, constraints Mass target Output: Optimal material distribution via density plot CAD geometry interpretation : using OSSmooth Then use to create optimal design 33

OptiStruct Version 3.4 Expanded Objective function Minimize Mass, Stiffness or Frequency Constraints on Mass, Stiffness, Freq, Disp Now available on Windows NT FE improvements, faster solution time HTML/Windows on-line documentation Improved integration with HyperMesh3.0 OptiStruct Case Study Volkswagen Bracket Minimize Mass of Engine Bracket Subject to stiffness/frequency constraints 7 loadcases: operating, pulley, transport 34

OptiStruct Case Study Volkswagen Bracket Results Mass reduced by 23% Original mass 950g ; Final mass 730g Performance targets were met OptiStruct: Topography Design for Future Automotive Body Engineering 35

ALTAIR/OPTISTRUCT Results Extension of HDM Topology Optimization Method Structural Design Static and Dynamic Stiffness Design Control Eigen-Frequencies Design Impact Loading Elastic-Plastic Design Material Microstructure Design Young s and Shear Moduli, Poisson s Ratios Thermal Expansion Coefficients Flexible Body Design (MEMS application) Piezocomposite and Piezoelectric Actuator Design 36

QUINT/OPTISHAPE Application to Contro Frequencies Material Design Special Mechanism : Negative ν Special Mechanism 37

Compliant Mechanism Design Professor S. Kota @ UM Negative Thermal Expansion Bing-Chung Chen s Design β α H H 8.01 = 0 52.7 = 0 0 7.89 0 58.9 38

39