Geometric Misfitting in Structures An Interval-Based Approach

Similar documents
Interval Finite Element Methods for Uncertainty Treatment in Structural Engineering Mechanics Rafi L. Muhanna Georgia Institute of Technology USA

Sharp Interval Estimates for Finite Element Solutions with Fuzzy Material Properties

Uncertainty is unavoidable in engineering system. Probabilistic approach is the traditional approach

Stress analysis of a stepped bar

4 Finite Element Method for Trusses

Level 7 Postgraduate Diploma in Engineering Computational mechanics using finite element method

Finite Element Analysis Prof. Dr. B. N. Rao Department of Civil Engineering Indian Institute of Technology, Madras. Lecture - 06

Structural Analysis of Truss Structures using Stiffness Matrix. Dr. Nasrellah Hassan Ahmed

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

Finite Element Structural Analysis using Imprecise Probabilities Based on P-Box Representation

Design of 2D Elastic Structures with the Interval Parameters

D : SOLID MECHANICS. Q. 1 Q. 9 carry one mark each. Q.1 Find the force (in kn) in the member BH of the truss shown.

Finite Element Method in Geotechnical Engineering

Interval Finite Element Analysis of Thin Plates

Multi-Point Constraints

Development of Truss Equations

IV B.Tech. I Semester Supplementary Examinations, February/March FINITE ELEMENT METHODS (Mechanical Engineering) Time: 3 Hours Max Marks: 80

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

INTRODUCTION TO STRAIN

JEPPIAAR ENGINEERING COLLEGE

CHAPTER 14 BUCKLING ANALYSIS OF 1D AND 2D STRUCTURES

2 marks Questions and Answers

The University of Melbourne Engineering Mechanics

Investigation of thermal effects on analyses of truss structures via metaheuristic approaches

Truss Structures: The Direct Stiffness Method

CHAPTER 5 Statically Determinate Plane Trusses

CHAPTER 5 Statically Determinate Plane Trusses TYPES OF ROOF TRUSS

GEOSYNTHETICS ENGINEERING: IN THEORY AND PRACTICE

Chapter 3 Variational Formulation & the Galerkin Method

Interval-Based Parameter Identification for Structural Static Problems

Lecture 8: Flexibility Method. Example

Analysis of Planar Truss

Sensitivity and Reliability Analysis of Nonlinear Frame Structures

The Plane Stress Problem

A two-dimensional FE truss program

Finite Element Method-Part II Isoparametric FE Formulation and some numerical examples Lecture 29 Smart and Micro Systems

FLEXIBILITY METHOD FOR INDETERMINATE FRAMES

Indeterminate Analysis Force Method 1

P.E. Civil Exam Review:

Methods of Analysis. Force or Flexibility Method

Using the finite element method of structural analysis, determine displacements at nodes 1 and 2.

STATICALLY INDETERMINATE STRUCTURES

J. Harish* and R.P. Rokade + *Graduate scholar Valliammai Engineering College, Kattankulathur, India + Principal Scientist

Formulation of the displacement-based Finite Element Method and General Convergence Results

14. *14.8 CASTIGLIANO S THEOREM

A Simple Problem Which Students Can Solve and Check Using an Inexpensive Calculator

CAAM 335 Matrix Analysis Planar Trusses

VORONOI APPLIED ELEMENT METHOD FOR STRUCTURAL ANALYSIS: THEORY AND APPLICATION FOR LINEAR AND NON-LINEAR MATERIALS

Due Tuesday, September 21 st, 12:00 midnight


CHAPTER 5. Beam Theory

NORMAL STRESS. The simplest form of stress is normal stress/direct stress, which is the stress perpendicular to the surface on which it acts.

Finite Element Structural Analysis using Imprecise Probabilities Based on P-Box Representation


Basic Energy Principles in Stiffness Analysis

Mechanics of Irregular Honeycomb Structures

Mechanical Models with Interval Parameters

Nondeterministic Linear Static Finite Element Analysis: An Interval Approach. Hao Zhang

CHAPTER OBJECTIVES CHAPTER OUTLINE. 4. Axial Load

Mechanical Properties of Materials

External Work. When a force F undergoes a displacement dx in the same direction i as the force, the work done is

Chapter 2: Deflections of Structures

Structural Analysis. For. Civil Engineering.

Chapter Two: Mechanical Properties of materials

Worst case analysis of mechanical structures by interval methods

Module 2. Analysis of Statically Indeterminate Structures by the Matrix Force Method

1.103 CIVIL ENGINEERING MATERIALS LABORATORY (1-2-3) Dr. J.T. Germaine Spring 2004 LABORATORY ASSIGNMENT NUMBER 6

GEO E1050 Finite Element Method Autumn Lecture. 9. Nonlinear Finite Element Method & Summary

Finite Element Analysis Prof. Dr. B. N. Rao Department of Civil Engineering Indian Institute of Technology, Madras. Module - 01 Lecture - 13

Institute of Structural Engineering Page 1. Method of Finite Elements I. Chapter 2. The Direct Stiffness Method. Method of Finite Elements I

ME 1401 FINITE ELEMENT ANALYSIS UNIT I PART -A. 2. Why polynomial type of interpolation functions is mostly used in FEM?

Ph.D. Preliminary Examination Analysis

Introduction to Finite Element Analysis Using Pro/MECHANICA Wildfire 5.0

Plane Trusses Trusses

MECE 3321 MECHANICS OF SOLIDS CHAPTER 3

Back Analysis of Measured Displacements of Tunnels

Chapter 11. Displacement Method of Analysis Slope Deflection Method

PRACTICE 2 PROYECTO Y CONSTRUCCIÓN DE PUENTES. 1º Máster Ingeniería de Caminos. E.T.S.I. Caminos, canales y puertos (Ciudad Real) 01/06/2016

Using MATLAB and. Abaqus. Finite Element Analysis. Introduction to. Amar Khennane. Taylor & Francis Croup. Taylor & Francis Croup,

KINGS COLLEGE OF ENGINEERING DEPARTMENT OF MECHANICAL ENGINEERING QUESTION BANK. Subject code/name: ME2254/STRENGTH OF MATERIALS Year/Sem:II / IV

Delhi Noida Bhopal Hyderabad Jaipur Lucknow Indore Pune Bhubaneswar Kolkata Patna Web: Ph:

ε t increases from the compressioncontrolled Figure 9.15: Adjusted interaction diagram

Module 4 : Deflection of Structures Lecture 4 : Strain Energy Method

Analyses of Truss Structures under Thermal Effects

Samantha Ramirez, MSE. Stress. The intensity of the internal force acting on a specific plane (area) passing through a point. F 2

Reg. No. : Question Paper Code : B.Arch. DEGREE EXAMINATION, APRIL/MAY Second Semester AR 6201 MECHANICS OF STRUCTURES I

BAR ELEMENT WITH VARIATION OF CROSS-SECTION FOR GEOMETRIC NON-LINEAR ANALYSIS

Due Monday, September 14 th, 12:00 midnight

Stiffness Matrices, Spring and Bar Elements

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

The Finite Element Method for the Analysis of Non-Linear and Dynamic Systems. Prof. Dr. Eleni Chatzi Lecture 1-20 September, 2017

If the number of unknown reaction components are equal to the number of equations, the structure is known as statically determinate.

1 Nonlinear deformation

CHAPTER 3 THE EFFECTS OF FORCES ON MATERIALS

five Mechanics of Materials 1 ARCHITECTURAL STRUCTURES: FORM, BEHAVIOR, AND DESIGN DR. ANNE NICHOLS SUMMER 2017 lecture

Topic 5: Finite Element Method

Mechanics of Structures (CE130N) Lab 6. 2 Principle of stationary potential energy

4.MECHANICAL PROPERTIES OF MATERIALS

MECh300H Introduction to Finite Element Methods. Finite Element Analysis (F.E.A.) of 1-D Problems

Biaxial Analysis of General Shaped Base Plates

Transcription:

Geometric Misfitting in Structures An Interval-Based Approach M. V. Rama Rao Vasavi College of Engineering, Hyderabad - 500 031 INDIA Rafi Muhanna School of Civil and Environmental Engineering Georgia Institute of Technology, Atlanta, GA 30332-0355, USA Robert L. Mullen Department of Civil and Environmental Engineering University of South Carolina, Columbia, SC 29208 USA REC 2014, May 25-28, 2014, IIT Chicago, USA

Outline Misfit of truss members Geometric Uncertainty Earlier work Present work Uncertainty of geometric, load and stiffness properties Interval FEM Sharpness of derived quantities Mixed IFEM formulation Iterative Enclosure Example Problems Conclusions

Misfit of Structural Members Due to fabrication errors and/or thermal changes certain bars can have improper length. In practice, the bar is forced into its position between two joints by applying some initial extension or compression. Under such a condition, some axial forces are introduced in the bars in the absence of external loads.

Geometric uncertainty Uncertainty in the bar length as the range between the lower and upper bounds on the nominal length of the bar. L L, L L = [L o L, L o + L] [ L, L]: { L R L L L} Geometric uncertainty is defined by specifying the percentage variation of the misfit of a member about the value of the nominal length of member.

Earlier Work.. Muhanna, Erdolen and Mullen (2006) addressed the problem of geometric uncertainty by considering a linear interval system of equations with interval right hand side in the form K U P Misfit forces were Solution vector of interval 1 displacements was obtained as U K P However, sharp bounds to interval axial forces could not be obtained then owing to the problem of overestimation.

Outline Misfit of truss members Geometric Uncertainty Earlier work Present work Uncertainty of geometric, load and stiffness properties Interval FEM Sharpness of derived quantities Mixed IFEM formulation Elimination of overestimation Example Problems Conclusions

Present work The present work obtains sharp bounds to interval displacements and axial forces by adapting the mixed finite element formulation developed by the authors. Truss structures with uncertainty in misfit, external loading and stiffness solved to illustrate the approach.

Interval Finite Element Method Error in secondary quantities Conventional finite element method gives 1 T T U K U U P 2 subject to the conditions 0 Secondary quantities such as force/ stress/ strain calculated from interval displacements show significant overestimation of interval bounds. U

Mixed interval finite element formulation The potential energy functional is rewritten as Unknowns associated with coincident nodes are forces to have identical values. Thus we have C U 0 T T T U KU U P ( CU V ) 2 * 1 Equating the first variation of * to zero,

Mixed interval finite element formulation T T T U KU U P ( CU V ) 2 * 1 where is the vector of Lagrange multipliers, is the vector of applied interval loads and contains interval multiples of additional loads due to misfit K C T U P M 0 C 0 λ 0 0 0 0 P

Mixed interval finite element formulation 2 2 Element (m) F 2m, u 2m 1 1 u Y F 1m, u 1m 2 1 1 2 Free node (n) u X P Y

Elimination of overestimation Overestimation is eliminated by Keeping individual elements separate and connected to free nodes and applying constraints on displacements of element nodes coincident with each free node Applying misfit forces along element local axes and thus avoiding their transformation from local axes to global axes Obtaining sharp enclosure to solution using Neumaier s algorithm Secondary variables are part of solution vector and thus are obtained at the same level of sharpness as the primary variables

Outline Misfit of truss members Geometric Uncertainty Earlier work Present work Uncertainty of geometric, load and stiffness properties Interval FEM Sharpness of derived quantities Mixed IFEM formulation Elimination of overestimation Example Problems Conclusions

Example Problem-1 Six bar truss P 3 3 4 5 6 4 2 5m 4 1 1 5m 2

Six bar truss - displacements for 0.2 percent geometric uncertainty alone U 3 10-3 (m) V 3 10-3 (m) U 4 10-3 (m) Lower Upper Lower Upper Lower Upper Combinatorial approach -3.41421 3.41421-1.49999 1.49999-3.20710 3.20710 Present approach -3.41421 3.41421-1.50000 1.50000-3.20710 3.20710 Error %(bounds) 0.00 0.00 0.00 0.00 0.00 0.00

Six bar truss axial forces for 0.2 percent geometric uncertainty alone N 2 (kn) N 3 (kn) N 6 (kn) Combinatorial approach Present approach Error %(bounds) Lower Upper Lower Upper Lower Upper -200.0 200.0-141.42 141.42-141.42 141.42-200.0 200.0-141.42 141.42-141.42 141.42 0.0 0.0 0.0 0.0 0.0 0.0

Six bar truss - displacements for 0.2 percent geometric uncertainty and 10 percent load uncertainty U 3 10-3 (m) V 3 10-5 (m) U 4 10-5 (m) Lower Upper Lower Upper Lower Upper Combinatorial approach -2.26746 4.68167-1.26250 1.76249-2.29785 4.21206 Present approach -2.26746 4.68167-1.26250 1.76250-2.29785 4.21206 Error %(bounds) 0.00 0.00 0.00 0.0005 0.00 0.00

Six bar truss axial forces for 0.2 percent geometric uncertainty and 10 percent load uncertainty N 2 (kn) N 3 (kn) N 6 (kn) Combinatorial approach Present approach Error %(bounds) Lower Upper Lower Upper Lower Upper -274.24 132.82-193.92 93.92-93.92 193.92-274.24 132.82-193.92 93.92-93.92 193.92 0.0 0.0 0.0 0.0 0.0 0.0

Six bar truss - displacements for 0.2 percent geometric uncertainty,10 percent load uncertainty and 1 percent uncertainty in modulus of Elasticity (E) U 3 10-3 (m) V 3 10-5 (m) U 4 10-5 (m) Lower Upper Lower Upper Lower Upper Combinatorial approach -2.28453 4.69874-1.26999 1.76999-2.31389 4.22810 Present approach -2.35837 4.77259-1.29639 1.79639-2.38431 4.29853 Error %(bounds) 3.23 1.57 2.07 1.49 3.04 1.66

Six bar truss forces for 0.2 percent geometric uncertainty,10 percent load uncertainty and 1 percent uncertainty in modulus of Elasticity (E) N2 (kn) N3 (kn) N6 (kn) Combinatorial approach Present approach Error %(bounds) Lower Upper Lower Upper Lower Upper -275.91 134.45-194.96 94.94-94.94 194.96-279.57 138.15-197.89 97.89-97.68 197.68 1.32 2.74 1.50 3.10 2.88 1.39

Example problem 2- Thirteen bar Truss 3 4 4 9 7 2 3 5 7 10 11 13 4.5m 1 1 2 6 5 8 6 12 8 4.5mm 4.5m 4.5m 4.5m P

Thirteen bar truss - displacements for 0.2 percent geometric uncertainty alone U 3 10-2 (m) V 5 10-3 (m) V 6 10-2 (m) Lower Upper Lower Upper Lower Upper Combinatorial approach -4.91421 4.91421 Present approach Error %(bounds) -4.91421 4.91421-8.82842 8.82842-8.82842 8.82842-5.62132 5.62132-6.12132 6.12132 0.0 0.0 0.0 0.0 0.0 0.0

Thirteen bar truss - displacements for 0. 2 percent geometric uncertainty and 10 percent load uncertainty U 3 10-2 V 5 10-3 V 6 10-2 Lower Upper Lower Upper Lower Upper Combinatorial approach 0.79107 1.90892-5.89350-3.65061-2.93409-1.48869 Present approach Error %(bounds) 0.79107 1.90892-5.89350-3.65061-2.93409-1.48869 0.0 0.0 0.0 0.0 0.0 0.0

Thirteen bar truss axial forces for 0.2 percent geometric uncertainty and10 percent load uncertainty N 2 (kn) N 5 (kn) N 6 (kn) Combinatorial approach Present approach Error %(bounds) Lower Upper Lower Upper Lower Upper -148.49-134.35-148.49-134.35 190.00 210.00-148.49-134.35-148.49-134.35 190.00 210.00 0.0 0.0 0.0 0.0 0.0 0.0

Thirteen bar truss - displacements for 0.2 percent geometric uncertainty,10 percent load uncertainty and 1 percent uncertainty in modulus of Elasticity (E) U 3 10-2 (m) V 5 10-3 (m) V 6 10-2 (m) Lower Upper Lower Upper Lower Upper Combinatorial approach 0.79140 1.90859-5.89285-3.65125-2.93377-1.48901 Present approach 0.78004 1.91995-5.91647-3.62763-2.94518-1.47760 Error %(bounds) 1.43 0.594 0.400 0.646 0.389 0.766

Thirteen bar truss axial forces for 2 percent geometric uncertainty,10 percent load uncertainty and 1 percent uncertainty in modulus of Elasticity (E) N2 (kn) N3 (kn) N6 (kn) Lower Upper Lower Upper Lower Upper Combinatorial approach -148.492-134.350 95.000 105.000 190.000 210.000 Present approach -148.918-133.923 94.698 105.301 189.263 210.737 Error %(bounds) 0.287 0.317 0.317 0.287 0.387 0.350

Outline Misfit of truss members Geometric Uncertainty Earlier work Present work Uncertainty of geometric, load and stiffness properties Interval FEM Sharpness of derived quantities Mixed IFEM formulation Iterative Enclosure Results Summary

Summary A method based on the use of a mixed finite element formulation for the analysis of structures with geometric, load and stiffness uncertainties is presented. Axial forces are obtained at the same level of sharpness as displacements in the simultaneous presence of geometric, stiffness and load uncertainties. Exact enclosure on the deformed geometry is obtained

Let us all be together. Let us share everything together. Let us carry out tasks with collective effort. Let our minds work together to acquire knowledge. Let us not harm each other. Let peace pervade Universe. -(Shanti Mantra ~3000 BC - INDIA)