Optimization Methods for Force and Shape Design of Tensegrity Structures. J.Y. Zhang and M. Ohsaki Kyoto University, Japan
|
|
- May Dorsey
- 5 years ago
- Views:
Transcription
1 Optimization Methods for Force and Shape Design of Tensegrity Structures J.Y. Zhang and M. Ohsaki Kyoto University, Japan
2 Contents Purpose Optimization techniques are effective for shape and force design of tensegrity structures. Concept & Applications Shape Design Energy Approach Direct Approach Minimum energy difference in cables and struts Minimum force deviation from target values Force Design Force & Stiffness Maximum stiffness Uniform forces Conclusions
3 Basics Tensegrity = Tension + Integrity (R.B. Fuller 1975) Assumptions Pin-jointed No external loads Struts (compression) + Cables (tension) No member failure Self-equilibrium Member forces Configuration Stiffness
4 Energy Approach? Cable Nets Cable nets: carry only tension.? Shape design problem: m 1 Minimize EA 2 Subject to? Variables: unstressed length, nodal locations? Stationary condition Equilibrium equation? Convex problem (Kanno & Ohsaki 2003) 2 0 i Li i 1 0 (1 i ) Li Bix di? Can specify member forces (or strain)
5 Energy Approach? Tensegrity Structures Tensegrity structures: tension + compression? Shape design problem: Minimize Subject to i Cable 1 1 EA L EA L i i i i i Strut 0 (1 i ) Li Bix di, i Cable 0 (1 i ) Li Bix di, i Strut? Variables: unstressed length, nodal locations? Stationary condition Equilibrium equation? Non-convex problem May not converge? Can specify member forces (or strain)? Unable to control member directions
6 Direct Approach? Objective & Idea? Direct assignment of member directions (Zhang et al. 2006) Fixed member Supported Free-standing Directed graph? Independent member directions? Difficulty for complicated structures
7 Direct Approach? Constraints? Two-step approach for form finding? Step 1: Find member directions (forces)? Step 2: Find nodal locations? Hard constraints (exactly satisfied) Hv = 0 Self-equilibrium equations Directions of fixed members Symmetry properties? Soft constraints (preferably satisfied) v cv Sv = 0 e.g., i j
8 Direct Approach? Member directions Step 1:? Minimize error from target values minimize subject to Hv = 0? Lagrangian? Stationary condition 1 T I 1 T II E( v) v v W v v ( Sv) W ( Sv) 2 2 L( v, ƒ) E( v) ƒ Hv I T II T I W S W S H v W v H O ƒ 0 T
9 Direct Approach? Nodal Coordinates Step 2:? Equilibrium equation w.r.t nodal coordinates FX 0? Rank of F < the number of unknown coordinates? Specify independent components of coordinates to obtain X
10 Direct Approach? Example 1 Top Side Perspective Hard constraints: Self-equilibrium equations Rotational symmetry Soft constraints: No 1 E ) T 1( v) ( vi vi ) ( vi vi 2 i K rank( F) 32 3n = 36 x, y, z, x ) (0, 0, 0,1.05) (
11 Direct Approach? Example 2 Soft constraint v 2v 7 19 Top Side Perspective Result v v 19 rank( F) 32 3n = 36 x, y, z, x ) (0, 0, 0,1.05) (
12 Force Design? Force Distribution Self-equilibrium Equation Ds 0 D? Equilibrium Matrix s? Member Force Configuration R: rank of D s f f f f i i m R m R fi? Force Mode Unknown Force Unknown Coefficient Force Deviation Stiffness Optimization Problem
13 Force Design? Stiffness Member Forces Configuration G E K K K E K M 0 stiffness Member Stiffness Q T G M K M M? mechanism Objective 1 Structure collapses in the weakest direction! Strengthen the Weakest Maximize the Minimum Eigenvalue of Q
14 Force Design? Force Deviation & Constraints Design Analysis Manufacture Construction Objective 2 Minimize deviation of member forces Constraints Positive force for cable Negative force for strut Given strain energy
15 Force Design? Formulation and Solution Objectives Maximize the Minimum Eigenvalue of Q Minimize deviation of member forces Constraints Positive force for cable Constraint Approach Negative force for strut Given strain energy Upper bound of force deviation
16 Force Design? Tensegrity Grid 38 Nodes 115 Members 8 Force Modes 1 Mechanism y x Top View Unit Cell Side View
17 Force Design? Pareto Optimality Maximum Stiffness Force Deviation Min. Force Deviation Pareto Optimality Target values: uniform distribution Maximum Stiffness
18 Conclusions? Optimization can be effectively used for shape and force design of tensegrity structures Shape Design Energy Difference Directed Graph Force Design? Specify member forces (strains)? Stationary condition satisfy self-equilibrium? Non-convex? Convergence problem? Direct assignment or force vectors? Member direction can be specified? Determine force components by optimization.? Shape and forces are controlled by modifying the target values and soft constraints.? Maximum stiffness? Minimum force deviation from target values? Pareto optimality to assist decision making
Simon D. GUEST Reader University of Cambridge Cambridge, UK.
Multi-stable Star-shaped Tensegrity Structures Jingyao ZHANG Lecturer Ritsumeikan University Kusatsu, Shiga, JAPAN zhang@fc.ritsumei.ac.jp Robert CONNELLY Professor Cornell University Ithaca, NY, USA rc46@cornell.edu
More informationTopology Optimization of Tensegrity Structures Based on Nonsmooth Mechanics. Yoshihiro Kanno. November 14, 2011 ACOMEN 2011
Topology Optimization of Tensegrity Structures Based on Nonsmooth Mechanics Yoshihiro Kanno November 14, 2011 ACOMEN 2011 tensegrity definition tension + integrity [Fuller 75] [Emmerich], [Snelson] pin-jointed
More informationSymmetric Prismatic Tensegrity Structures: Part II. Symmetry-adapted Formulations
Symmetric Prismatic Tensegrity Structures: Part II. Symmetry-adapted Formulations J.Y. Zhang a S.D. Guest b, M. Ohsaki a a Dept. of Architecture & Architectural Engineering, Kyoto University, Japan b Dept.
More informationOPTIMUM PRE-STRESS DESIGN FOR FREQUENCY REQUIREMENT OF TENSEGRITY STRUCTURES
Blucher Mechanical Engineering Proceedings May 2014, vol. 1, num. 1 www.proceedings.blucher.com.br/evento/10wccm OPTIMUM PRE-STRESS DESIGN FOR FREQUENCY REQUIREMENT OF TENSEGRITY STRUCTURES Seif Dalil
More information1.105 Solid Mechanics Laboratory Fall 2003
1.105 Solid Mechanics Laboratory Fall 200 Experiment 7 Elastic Buckling. The objectives of this experiment are To study the failure of a truss structure due to local buckling of a compression member. To
More informationPrestress stability. Lecture VI. Session on Granular Matter Institut Henri Poincaré. R. Connelly Cornell University Department of Mathematics
Prestress stability Lecture VI Session on Granular Matter Institut Henri Poincaré R. Connelly Cornell University Department of Mathematics 1 Potential functions How is the stability of a structure determined
More informationSTATIC LOADING TESTS AND A COMPUTATIONAL MODEL OF A FLEXIBLE NET
STATIC LOADING TESTS AND A COMPUTATIONAL MODEL OF A FLEXIBLE NET Jun FUJIWARA 1, Shinya SEGAWA 1, Kenshi ODA 1, Fumio FUJII, Makoto OHSAKI 3, Hirohisa NOGUCHI 4 1 Research Engineer, Advanced Structures
More informationInternational Journal of Solids and Structures
International Journal of Solids and Structures 7 (00) 75 79 Contents lists available at ScienceDirect International Journal of Solids and Structures journal homepage: www.elsevier.com/locate/ijsolstr Advanced
More informationUsing the finite element method of structural analysis, determine displacements at nodes 1 and 2.
Question 1 A pin-jointed plane frame, shown in Figure Q1, is fixed to rigid supports at nodes and 4 to prevent their nodal displacements. The frame is loaded at nodes 1 and by a horizontal and a vertical
More informationENGN1300: Structural Analysis
ENGN1300: Structural Analysis Homework 4 Due Wednesday, March 3, 2010 Division of Engineering Brown University 1. For the statically indeterminate structure shown below, all members have identical values
More informationFLEXIBILITY METHOD FOR INDETERMINATE FRAMES
UNIT - I FLEXIBILITY METHOD FOR INDETERMINATE FRAMES 1. What is meant by indeterminate structures? Structures that do not satisfy the conditions of equilibrium are called indeterminate structure. These
More informationKinestatic Analyses of Mechanisms with Compliant Elements
Kinestatic Analyses of Mechanisms with Compliant Elements Carl Crane How can such a simple mechanism have such a high order solution? Tensegrity structures comprised of struts in compression and ties in
More informationOn the determinacy of repetitive structures
Journal of the Mechanics and Physics of Solids 51 (2003) 383 391 www.elsevier.com/locate/jmps On the determinacy of repetitive structures S.D. Guest a;, J.W. Hutchinson b a Department of Engineering, University
More informationLecture 4: PRELIMINARY CONCEPTS OF STRUCTURAL ANALYSIS. Introduction
Introduction In this class we will focus on the structural analysis of framed structures. We will learn about the flexibility method first, and then learn how to use the primary analytical tools associated
More informationA MARCHING PROCEDURE FOR FORM-FINDING FOR TENSEGRITY STRUCTURES
JOURNAL OF MECHANICS OF MATERIALS AND STRUCTURES Vol., No., A MARCHING PROCEDURE FOR FORM-FINDING FOR TENSEGRITY STRUCTURES ANDREA MICHELETTI AND WILLIAM O. WILLIAMS We give an algorithm for solving the
More informationThere are three main types of structure - mass, framed and shells.
STRUCTURES There are three main types of structure - mass, framed and shells. Mass structures perform due to their own weight. An example would be a dam. Frame structures resist loads due to the arrangement
More informationCHAPTER 14 BUCKLING ANALYSIS OF 1D AND 2D STRUCTURES
CHAPTER 14 BUCKLING ANALYSIS OF 1D AND 2D STRUCTURES 14.1 GENERAL REMARKS In structures where dominant loading is usually static, the most common cause of the collapse is a buckling failure. Buckling may
More informationChapter 4 Deflection and Stiffness
Chapter 4 Deflection and Stiffness Asst. Prof. Dr. Supakit Rooppakhun Chapter Outline Deflection and Stiffness 4-1 Spring Rates 4-2 Tension, Compression, and Torsion 4-3 Deflection Due to Bending 4-4 Beam
More informationthree Point Equilibrium 1 and planar trusses ARCHITECTURAL STRUCTURES: FORM, BEHAVIOR, AND DESIGN DR. ANNE NICHOLS SUMMER 2014 lecture
ARCHITECTURAL STRUCTURES: FORM, BEHAVIOR, AND DESIGN DR. ANNE NICHOLS SUMMER 2014 lecture three point equilibrium http:// nisee.berkeley.edu/godden and planar trusses Point Equilibrium 1 Equilibrium balanced
More informationSTATICALLY INDETERMINATE STRUCTURES
STATICALLY INDETERMINATE STRUCTURES INTRODUCTION Generally the trusses are supported on (i) a hinged support and (ii) a roller support. The reaction components of a hinged support are two (in horizontal
More informationChapter 2 Examples of Optimization of Discrete Parameter Systems
Chapter Examples of Optimization of Discrete Parameter Systems The following chapter gives some examples of the general optimization problem (SO) introduced in the previous chapter. They all concern the
More informationBistable Regimes in an Elastic Tensegrity System
Bistable Regimes in an Elastic Tensegrity System Andrea Micheletti Department of Civil Engineering and Computer Science Engineering University of Rome Tor Vergata Via Politecnico 1, 00133, Rome, Italy
More informationthree point equilibrium and planar trusses Equilibrium Equilibrium on a Point Equilibrium on a Point
RHITETURL STRUTURES: FORM, EHVIOR, N ESIGN R. NNE NIHOLS SUMMER 2014 lecture three Equilibrium balanced steady resultant of forces on a particle is 0 X point equilibrium and planar trusses http:// nisee.berkeley.edu/godden
More informationChapter 14 Truss Analysis Using the Stiffness Method
Chapter 14 Truss Analsis Using the Stiffness Method Structural Mechanics 2 ept of Arch Eng, Ajou Univ Outline undamentals of the stiffness method Member stiffness matri isplacement and force transformation
More informationVector Mechanics: Statics
PDHOnline Course G492 (4 PDH) Vector Mechanics: Statics Mark A. Strain, P.E. 2014 PDH Online PDH Center 5272 Meadow Estates Drive Fairfax, VA 22030-6658 Phone & Fax: 703-988-0088 www.pdhonline.org www.pdhcenter.com
More informationResidual Force Equations
3 Residual Force Equations NFEM Ch 3 Slide 1 Total Force Residual Equation Vector form r(u,λ) = 0 r = total force residual vector u = state vector with displacement DOF Λ = array of control parameters
More informationStress analysis of a stepped bar
Stress analysis of a stepped bar Problem Find the stresses induced in the axially loaded stepped bar shown in Figure. The bar has cross-sectional areas of A ) and A ) over the lengths l ) and l ), respectively.
More informationIf the number of unknown reaction components are equal to the number of equations, the structure is known as statically determinate.
1 of 6 EQUILIBRIUM OF A RIGID BODY AND ANALYSIS OF ETRUCTURAS II 9.1 reactions in supports and joints of a two-dimensional structure and statically indeterminate reactions: Statically indeterminate structures
More informationImperfection sensitivity analysis of hill-top branching with many symmetric bifurcation points 1
Imperfection sensitivity analysis of hill-top branching with many symmetric bifurcation points 1 M. Ohsaki Department of Architecture and Architectural Engineering, Kyoto University Kyotodaigaku-Katsura,
More informationReview 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 informationThe AR OPF: an Exact Convex Formulation for the Optimal Power Flow in Radial Distribution Networks
Photo credit: Infineon The AR OPF: an Exact Convex Formulation for the Optimal Power Flow in Radial Distribution Networks Jean Yves Le Boudec and Mario Paolone EPFL LCA and DESL (joint work with Dr. Mostafa
More informationLIMIT LOAD OF A MASONRY ARCH BRIDGE BASED ON FINITE ELEMENT FRICTIONAL CONTACT ANALYSIS
5 th GRACM International Congress on Computational Mechanics Limassol, 29 June 1 July, 2005 LIMIT LOAD OF A MASONRY ARCH BRIDGE BASED ON FINITE ELEMENT FRICTIONAL CONTACT ANALYSIS G.A. Drosopoulos I, G.E.
More informationTruss Analysis Method of Joints. Steven Vukazich San Jose State University
Truss nalysis Method of Joints Steven Vukazich San Jose State University General Procedure for the nalysis of Simple Trusses using the Method of Joints 1. raw a Free Body iagram (FB) of the entire truss
More informationStructural Analysis of Truss Structures using Stiffness Matrix. Dr. Nasrellah Hassan Ahmed
Structural Analysis of Truss Structures using Stiffness Matrix Dr. Nasrellah Hassan Ahmed FUNDAMENTAL RELATIONSHIPS FOR STRUCTURAL ANALYSIS In general, there are three types of relationships: Equilibrium
More informationMEE224: Engineering Mechanics Lecture 4
Lecture 4: Structural Analysis Part 1: Trusses So far we have only analysed forces and moments on a single rigid body, i.e. bars. Remember that a structure is a formed by and this lecture will investigate
More informationTo show how to determine the forces in the members of a truss using the method of joints and the method of sections.
5 Chapter Objectives To show how to determine the forces in the members of a truss using the method of joints and the method of sections. To analyze the forces acting on the members of frames and machines
More informationLecture 28 Introduction to finite elements methods
Fall, 2017 ME 323 Mechanics of Materials Lecture 28 Introduction to finite elements methods Reading assignment: News: Instructor: Prof. Marcial Gonzalez Last modified: 10/27/17 10:56:52 AM Some announcements
More informationFinite Element Analysis Prof. Dr. B. N. Rao Department of Civil Engineering Indian Institute of Technology, Madras. Lecture - 06
Finite Element Analysis Prof. Dr. B. N. Rao Department of Civil Engineering Indian Institute of Technology, Madras Lecture - 06 In the last lecture, we have seen a boundary value problem, using the formal
More informationTruss Topology Optimization under Constraints. on Number of Different Design Variables
Truss Topology Optimization under Constraints on Number of Different Design Variables Yoshihiro Kanno (Tokyo Institute of Technology) (University of Tokyo) June 11, 2015 constraint on # of different design
More informationFlavors of Rigidity Flavor III - Universal Rigidity and Tensegrities
Flavors of Rigidity Flavor III - Universal Rigidity and Tensegrities Discrete Networks University of Pittsburgh Bob Connelly Cornell University October 2014 1 / 22 Stress-Energy Form Recall that a tensegrity
More informationPrestressed gridshell structures 1
25-28th September 2017, Hamburg, Germany Annette Bögle, Manfred Grohmann (eds.) restressed gridshell structures 1 Mats ANDER a, Alexander SEHLSTRÖM *, aul SHEHERD b, Chris J. K. WILLIAMS c * Department
More informationUniqueness and Symmetry of Optimal Thickness Distribution of Axisymmetric Shells
6 th China Japan Korea Joint Symposium on Optimization of Structural and Mechanical Systems June -5, 010, Kyoto, Japan Uniqueness and Symmetry of Optimal Thickness Distribution of Axisymmetric Shells Ryo
More informationMarch 24, Chapter 4. Deflection and Stiffness. Dr. Mohammad Suliman Abuhaiba, PE
Chapter 4 Deflection and Stiffness 1 2 Chapter Outline Spring Rates Tension, Compression, and Torsion Deflection Due to Bending Beam Deflection Methods Beam Deflections by Superposition Strain Energy Castigliano
More informationEquilibrium of a Particle
ME 108 - Statics Equilibrium of a Particle Chapter 3 Applications For a spool of given weight, what are the forces in cables AB and AC? Applications For a given weight of the lights, what are the forces
More informationFOAM TOPOLOGY BENDING VERSUS STRETCHING DOMINATED ARCHITECTURES
Acta mater. 49 (001) 1035 1040 www.elsevier.com/locate/actamat FOAM TOPOLOGY BENDING VERSUS STRETCHING DOMINATED ARCHITECTURES V. S. DESHPANDE, M. F. ASHBY and N. A. FLECK Cambridge University, Department
More informationChapter 2. Formulation of Finite Element Method by Variational Principle
Chapter 2 Formulation of Finite Element Method by Variational Principle The Concept of Variation of FUNCTIONALS Variation Principle: Is to keep the DIFFERENCE between a REAL situation and an APPROXIMATE
More informationIf you take CT5143 instead of CT4143 then write this at the first of your answer sheets and skip problem 4 and 6.
Delft University of Technology Faculty of Civil Engineering and Geosciences Structural Mechanics Section Write your name and study number at the top right-hand of your work. Exam CT4143 Shell Analysis
More information6.5 Cables: Concentrated Loads
6.5 ables: oncentrated Loads 6.5 ables: oncentrated Loads Procedures and Strategies, page 1 of 3 Procedures and Strategies for Solving Problems Involving ables With oncentrated Loads 1. Pass sections through
More informationMethods of Analysis. Force or Flexibility Method
INTRODUCTION: The structural analysis is a mathematical process by which the response of a structure to specified loads is determined. This response is measured by determining the internal forces or stresses
More informationSTATICS--AN INVESTIGATION OF FORCES
STTIS--N INVESTIGTION O ORES Two areas of study to investigate forces. Statics where the forces acting on a material are balanced so that the material is either stationary or in uniform motion. or fluid
More informationDiscretization Methods Exercise # 5
Discretization Methods Exercise # 5 Static calculation of a planar truss structure: a a F Six steps: 1. Discretization 2. Element matrices 3. Transformation 4. Assembly 5. Boundary conditions 6. Solution
More informationEDEXCEL NATIONAL CERTIFICATE/DIPLOMA MECHANICAL PRINCIPLES AND APPLICATIONS NQF LEVEL 3 OUTCOME 1 - LOADING SYSTEMS TUTORIAL 3 LOADED COMPONENTS
EDEXCEL NATIONAL CERTIICATE/DIPLOMA MECHANICAL PRINCIPLES AND APPLICATIONS NQ LEVEL 3 OUTCOME 1 - LOADING SYSTEMS TUTORIAL 3 LOADED COMPONENTS 1. Be able to determine the effects of loading in static engineering
More information3.032 Problem Set 1 Fall 2007 Due: Start of Lecture,
3.032 Problem Set 1 Fall 2007 Due: Start of Lecture, 09.14.07 1. The I35 bridge in Minneapolis collapsed in Summer 2007. The failure apparently occurred at a pin in the gusset plate of the truss supporting
More informationChapter 13. Simple Harmonic Motion
Chapter 13 Simple Harmonic Motion Hooke s Law F s = - k x F s is the spring force k is the spring constant It is a measure of the stiffness of the spring A large k indicates a stiff spring and a small
More informationLecture 2: Finite Elements
Materials Science & Metallurgy Master of Philosophy, Materials Modelling, Course MP7, Finite Element Analysis, H. K. D. H. Bhadeshia Lecture 2: Finite Elements In finite element analysis, functions of
More informationStatics. Phys101 Lectures 19,20. Key points: The Conditions for static equilibrium Solving statics problems Stress and strain. Ref: 9-1,2,3,4,5.
Phys101 Lectures 19,20 Statics Key points: The Conditions for static equilibrium Solving statics problems Stress and strain Ref: 9-1,2,3,4,5. Page 1 The Conditions for Static Equilibrium An object in static
More informationLecture 27 Introduction to finite elements methods
Fall, 2017 ME 323 Mechanics of Materials Lecture 27 Introduction to finite elements methods Reading assignment: News: Instructor: Prof. Marcial Gonzalez Last modified: 10/24/17 7:02:00 PM Finite element
More informationAbstract. 1 Introduction
Buckling force for deployable pantographic columns I. Raskin, J. Roorda Department of Civil Engineering, University of Waterloo, Waterloo, Ontario, Canada N2L SGI Abstract The method of calculating the
More informationDesign Sensitivity Analysis and Optimization for Nonlinear Buckling of Finite-Dimensional Elastic Conservative Structures 1
Design Sensitivity Analysis and Optimization for Nonlinear Buckling of Finite-Dimensional Elastic Conservative Structures 1 M. Ohsaki Department of Architecture and Architectural Engineering, Kyoto University
More informationPLATE GIRDERS II. Load. Web plate Welds A Longitudinal elevation. Fig. 1 A typical Plate Girder
16 PLATE GIRDERS II 1.0 INTRODUCTION This chapter describes the current practice for the design of plate girders adopting meaningful simplifications of the equations derived in the chapter on Plate Girders
More informationInstitute of Structural Engineering Page 1. Method of Finite Elements I. Chapter 2. The Direct Stiffness Method. Method of Finite Elements I
Institute of Structural Engineering Page 1 Chapter 2 The Direct Stiffness Method Institute of Structural Engineering Page 2 Direct Stiffness Method (DSM) Computational method for structural analysis Matrix
More informationA HIGHER-ORDER BEAM THEORY FOR COMPOSITE BOX BEAMS
A HIGHER-ORDER BEAM THEORY FOR COMPOSITE BOX BEAMS A. Kroker, W. Becker TU Darmstadt, Department of Mechanical Engineering, Chair of Structural Mechanics Hochschulstr. 1, D-64289 Darmstadt, Germany kroker@mechanik.tu-darmstadt.de,
More informationENGINEERING MECHANICS STATIC
Trusses Simple trusses The basic element of a truss is the triangle, three bars joined by pins at their ends, fig. a below, constitutes a rigid frame. The term rigid is used to mean noncollapsible and
More informationCHAPTER 5 Statically Determinate Plane Trusses
CHAPTER 5 Statically Determinate Plane Trusses TYPES OF ROOF TRUSS TYPES OF ROOF TRUSS ROOF TRUSS SETUP ROOF TRUSS SETUP OBJECTIVES To determine the STABILITY and DETERMINACY of plane trusses To analyse
More informationCHAPTER 5 Statically Determinate Plane Trusses TYPES OF ROOF TRUSS
CHAPTER 5 Statically Determinate Plane Trusses TYPES OF ROOF TRUSS 1 TYPES OF ROOF TRUSS ROOF TRUSS SETUP 2 ROOF TRUSS SETUP OBJECTIVES To determine the STABILITY and DETERMINACY of plane trusses To analyse
More information3.1 Limit Analysis and Design of Structures Formulated as LP Problems
Linear Programming 3 Mathematical programming is concerned with the extremization of a function f defined over an n-dimensional design space R n and bounded by a set S in the design space. The set S may
More informationChapter 12. Static Equilibrium and Elasticity
Chapter 12 Static Equilibrium and Elasticity Static Equilibrium Equilibrium implies that the object moves with both constant velocity and constant angular velocity relative to an observer in an inertial
More informationDrilling in tempered glass modelling and experiments
Drilling in tempered glass modelling and experiments Jens H. NIELSEN* * Department of Civil Engineering, Technical University of Denmark jhn@byg.dtu.dk Abstract The present paper reports experimentally
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 information3D problem: Fx Fy Fz. Forces act parallel to the members (2 5 ) / 29 (2 5 ) / 29
problem: x y z 0 t each joint a a a a 5a j i W k y z x x y z Equations:S x =S y =S z =0 at each joint () Unknowns: Total of : Member forces,,, () Reactions : x, y, z, x, y, z, x, y, z (9) y z x W orces
More informationCOLUMNS: BUCKLING (DIFFERENT ENDS)
COLUMNS: BUCKLING (DIFFERENT ENDS) Buckling of Long Straight Columns Example 4 Slide No. 1 A simple pin-connected truss is loaded and supported as shown in Fig. 1. All members of the truss are WT10 43
More informationA Framework for Comparing Form Finding Methods
A Framework for Comparing Form Finding Methods Diederik VEENENDAA Research Assistant ETH Zurich Zurich, Switzerland veenendaal@arch.ethz.ch Diederik Veenendaal, born 1982, received his civil engineering
More informationInstitute of Structural Engineering Page 1. Method of Finite Elements I. Chapter 2. The Direct Stiffness Method. Method of Finite Elements I
Institute of Structural Engineering Page 1 Chapter 2 The Direct Stiffness Method Institute of Structural Engineering Page 2 Direct Stiffness Method (DSM) Computational method for structural analysis Matrix
More informationthree Equilibrium 1 and planar trusses ELEMENTS OF ARCHITECTURAL STRUCTURES: FORM, BEHAVIOR, AND DESIGN DR. ANNE NICHOLS SPRING 2015 lecture ARCH 614
ELEMENTS OF ARCHITECTURAL STRUCTURES: FORM, BEHAVIOR, AND DESIGN DR. ANNE NICHOLS SPRING 2015 lecture three equilibrium and planar trusses Equilibrium 1 Equilibrium balanced steady resultant of forces
More informationCHAPTER 2: FORCES AND MOTION
CHAPTER 2: FORCES AND MOTION 2.1 Linear Motion Linear Motion is motion in a straight line with constant acceleration. Classification Scalar Vector Physical quantity with Magnitude only Magnitude and direction
More informationStatic Equilibrium. University of Arizona J. H. Burge
Static Equilibrium Static Equilibrium Definition: When forces acting on an object which is at rest are balanced, then the object is in a state of static equilibrium. - No translations - No rotations In
More informationPROBLEMS. m s TAC. m = 60 kg/m, determine the tension in the two supporting cables and the reaction at D.
1. he uniform I-beam has a mass of 60 kg per meter of its length. Determine the tension in the two supporting cables and the reaction at D. (3/62) A( 500) m (5 23) m m = 60 kg/m determine the tension in
More informationOBJECTIVES & ASSUMPTIONS
OBJECTIVES & ASSUMPTIONS Z Project Objectives: Construct a template for the 5-node pyramid element Conduct higher-order patch tests Verify element formulation Determine the optimal element in bending X
More informationREVIEW. Final Exam. Final Exam Information. Final Exam Information. Strategy for Studying. Test taking strategy. Sign Convention Rules
Final Exam Information REVIEW Final Exam (Print notes) DATE: WEDNESDAY, MAY 12 TIME: 1:30 PM - 3:30 PM ROOM ASSIGNMENT: Toomey Hall Room 199 1 2 Final Exam Information Comprehensive exam covers all topics
More informationEQUATIONS OF EQUILIBRIUM & TWO- AND THREE-FORCE MEMEBERS
EQUATIONS OF EQUILIBRIUM & TWO- AND THREE-FORCE MEMEBERS Today s Objectives: Students will be able to: a) Apply equations of equilibrium to solve for unknowns, and b) Recognize two-force members. In-Class
More informationActuation of kagome lattice structures
Actuation of kagome lattice structures A.C.H. Leung D.D. Symons and S.D. Guest Department of Engineering, University of Cambridge, Trumpington Street, Cambridge, CB2 1PZ, UK The kagome lattice has been
More informationLecture 4 Honeycombs Notes, 3.054
Honeycombs-In-plane behavior Lecture 4 Honeycombs Notes, 3.054 Prismatic cells Polymer, metal, ceramic honeycombs widely available Used for sandwich structure cores, energy absorption, carriers for catalysts
More informationMechanics Lab & Problem Sheet 2: Structures ( )
Mechanics Lab & Problem Sheet 2: Structures (2009-2010) Name (please print): P/1 Tutor (please print): Lab group Notes In the session you will be divided into small groups (about five per group). For the
More informationENT 151 STATICS. Contents. Introduction. Definition of a Truss
CHAPTER 6 Analysis ENT 151 STATICS Lecture Notes: Mohd Shukry Abdul Majid KUKUM of Structures Contents Introduction Definition of a Truss Simple Trusses Analysis of Trusses by the Method of Joints Joints
More informationChapter 5: Equilibrium of a Rigid Body
Chapter 5: Equilibrium of a Rigid Body Chapter Objectives To develop the equations of equilibrium for a rigid body. To introduce the concept of a free-body diagram for a rigid body. To show how to solve
More informationENGR-1100 Introduction to Engineering Analysis. Lecture 13
ENGR-1100 Introduction to Engineering Analysis Lecture 13 EQUILIBRIUM OF A RIGID BODY & FREE-BODY DIAGRAMS Today s Objectives: Students will be able to: a) Identify support reactions, and, b) Draw a free-body
More informationPhysics 125, Spring 2006 Monday, May 15, 8:00-10:30am, Old Chem 116. R01 Mon. 12:50 R02 Wed. 12:50 R03 Mon. 3:50. Final Exam
Monday, May 15, 8:00-10:30am, Old Chem 116 Name: Recitation section (circle one) R01 Mon. 12:50 R02 Wed. 12:50 R03 Mon. 3:50 Closed book. No notes allowed. Any calculators are permitted. There are no trick
More informationIntroduction to Simulation - Lecture 2. Equation Formulation Methods. Jacob White. Thanks to Deepak Ramaswamy, Michal Rewienski, and Karen Veroy
Introduction to Simulation - Lecture Equation Formulation Methods Jacob White Thanks to Deepak Ramaswamy, Michal Rewienski, and Karen Veroy Outline Formulating Equations rom Schematics Struts and Joints
More informationVibration characteristics analysis of a centrifugal impeller
Vibration characteristics analysis of a centrifugal impeller Di Wang 1, Guihuo Luo 2, Fei Wang 3 Nanjing University of Aeronautics and Astronautics, College of Energy and Power Engineering, Nanjing 210016,
More informationANALYSIS OF GATE 2018*(Memory Based) Mechanical Engineering
ANALYSIS OF GATE 2018*(Memory Based) Mechanical ME Industrial 4% General Aptitude 15% Mathematics 14% Mechanics 4% Manufacturing 14% Mechanics of Materials 14% Thermodynamics 10% Heat Transfer 2% Fluid
More informationThe analysis of trusses Mehrdad Negahban (1999)
The analysis of trusses Mehrdad Negahban (1999) A truss: A truss is a structure made of two force members all pin connected to each other. The method of joints: This method uses the free-body-diagram of
More informationPractice Final Examination. Please initial the statement below to show that you have read it
EN175: Advanced Mechanics of Solids Practice Final Examination School of Engineering Brown University NAME: General Instructions No collaboration of any kind is permitted on this examination. You may use
More informationAuthor(s) Okajima, Kenji; Tanaka, Tadatsugu; Symposium on Backwards Problem in G.
Title Backwards Analysis for Retaining Wa based upon ateral Wall Displacemen Author(s) Okajima, Kenji; Tanaka, Tadatsugu; Proceeding of TC302 Symposium Osaka Citation Symposium on Backwards Problem in
More informationEQUATIONS OF EQUILIBRIUM & TWO- AND THREE-FORCE MEMEBERS
EQUATIONS OF EQUILIBRIUM & TWO- AND THREE-FORCE MEMEBERS Today s Objectives: Students will be able to: a) Apply equations of equilibrium to solve for unknowns, and, b) Recognize two-force members. In-Class
More informationOn Nonlinear Buckling and Collapse Analysis using Riks Method
Visit the SIMULIA Resource Center for more customer examples. On Nonlinear Buckling and Collapse Analysis using Riks Method Mingxin Zhao, Ph.D. UOP, A Honeywell Company, 50 East Algonquin Road, Des Plaines,
More informationSection 5.4 (Systems of Linear Differential Equation); 9.5 Eigenvalues and Eigenvectors, cont d
Section 5.4 (Systems of Linear Differential Equation); 9.5 Eigenvalues and Eigenvectors, cont d July 6, 2009 Today s Session Today s Session A Summary of This Session: Today s Session A Summary of This
More informationThe case where there is no net effect of the forces acting on a rigid body
The case where there is no net effect of the forces acting on a rigid body Outline: Introduction and Definition of Equilibrium Equilibrium in Two-Dimensions Special cases Equilibrium in Three-Dimensions
More informationME 176 Final Exam, Fall 1995
ME 176 Final Exam, Fall 1995 Saturday, December 16, 12:30 3:30 PM, 1995. Answer all questions. Please write all answers in the space provided. If you need additional space, write on the back sides. Indicate
More informationPin-Jointed Frame Structures (Frameworks)
Pin-Jointed rame Structures (rameworks) 1 Pin Jointed rame Structures (rameworks) A pin-jointed frame is a structure constructed from a number of straight members connected together at their ends by frictionless
More informationChapter 1 Introduction- Concept of Stress
hapter 1 Introduction- oncept of Stress INTRODUTION Review of Statics xial Stress earing Stress Torsional Stress 14 6 ending Stress W W L Introduction 1-1 Shear Stress W W Stress and Strain L y y τ xy
More information