Finite Element Analysis

Slides:



Advertisements
Similar presentations
Finite Element Method Monday, 11/11/2002 Equations assembling Displacement boundary conditions Gaussian elimination.
Advertisements

Element Loads Strain and Stress 2D Analyses Structural Mechanics Displacement-based Formulations.
MANE 4240 & CIVL 4240 Introduction to Finite Elements Practical considerations in FEM modeling Prof. Suvranu De.
MANE 4240 & CIVL 4240 Introduction to Finite Elements
Some Ideas Behind Finite Element Analysis
Section 4: Implementation of Finite Element Analysis – Other Elements
Matrix Methods (Notes Only)
MECh300H Introduction to Finite Element Methods Finite Element Analysis (F.E.A.) of 1-D Problems – Applications.
MANE 4240 & CIVL 4240 Introduction to Finite Elements Introduction to 3D Elasticity Prof. Suvranu De.
FEA Simulations Usually based on energy minimum or virtual work Component of interest is divided into small parts – 1D elements for beam or truss structures.
MANE 4240 & CIVL 4240 Introduction to Finite Elements
MESF593 Finite Element Methods HW #2 Solutions. Prob. #1 (25%) The element equations of a general tapered beam with a rectangular cross- section are given.
MANE 4240 & CIVL 4240 Introduction to Finite Elements
ECIV 720 A Advanced Structural Mechanics and Analysis Lecture 10: Solution of Continuous Systems – Fundamental Concepts Mixed Formulations Intrinsic Coordinate.
MECh300H Introduction to Finite Element Methods
MANE 4240 & CIVL 4240 Introduction to Finite Elements
Isoparametric elements and solution techniques. Advanced Design for Mechanical System - Lec 2008/10/092.
ECIV 720 A Advanced Structural Mechanics and Analysis Lecture 12: Isoparametric CST Area Coordinates Shape Functions Strain-Displacement Matrix Rayleigh-Ritz.
CHAP 6 FINITE ELEMENTS FOR PLANE SOLIDS
CST ELEMENT STIFFNESS MATRIX
ECIV 720 A Advanced Structural Mechanics and Analysis Lecture 7: Formulation Techniques: Variational Methods The Principle of Minimum Potential Energy.
2005 February, 2 Page 1 Finite Element Analysis Basics – Part 2/2 Johannes Steinschaden.
CHAP 4 FINITE ELEMENT ANALYSIS OF BEAMS AND FRAMES
MECH593 Introduction to Finite Element Methods
MANE 4240 & CIVL 4240 Introduction to Finite Elements
CHAP 5 FINITE ELEMENTS FOR HEAT TRANSFER PROBLEMS
1 THERMAL STRESSES Temperature change causes thermal strain Constraints cause thermal stresses Thermo-elastic stress-strain relationship (a) at T = T.
MANE 4240 & CIVL 4240 Introduction to Finite Elements
Finite Element: Theory, Applications & Implementation Presented By: Arthur Anconetani Barbara Gault Ryan Whitney.
General Procedure for Finite Element Method FEM is based on Direct Stiffness approach or Displacement approach. A broad procedural outline is listed.
2004 March, 4 Page 1 Finite Element Analysis Basics – Part 2/2 Johannes Steinschaden.
ME 520 Fundamentals of Finite Element Analysis
School of Civil EngineeringSpring 2007 CE 595: Finite Elements in Elasticity Instructors: Amit Varma, Ph.D. Timothy M. Whalen, Ph.D.
An introduction to the finite element method using MATLAB
Mechanics of Thin Structure Lecture 15 Wrapping Up the Course Shunji Kanie.
1 20-Oct-15 Last course Lecture plan and policies What is FEM? Brief history of the FEM Example of applications Discretization Example of FEM softwares.
The Finite Element Method A Practical Course
Chapter 6. Plane Stress / Plane Strain Problems
MECH593 Finite Element Methods
11/11/20151 Trusses. 11/11/20152 Element Formulation by Virtual Work u Use virtual work to derive element stiffness matrix based on assumed displacements.
Last course Bar structure Equations from the theory of elasticity
HEAT TRANSFER FINITE ELEMENT FORMULATION
MECH4450 Introduction to Finite Element Methods
CHAP 3 WEIGHTED RESIDUAL AND ENERGY METHOD FOR 1D PROBLEMS
1 CHAP 5 FINITE ELEMENTS FOR HEAT TRANSFER PROBLEMS FINITE ELEMENT ANALYSIS AND DESIGN Nam-Ho Kim Audio by Raphael Haftka.
11 10-Jan-16 Last course Interpretations and properties of the stiffness matrix (cont’d) The DSM for plane and space trusses.
1/61/6 M.Chrzanowski: Strength of Materials SM1-08: Continuum Mechanics: Stress distribution CONTINUUM MECHANICS (STRESS DISTRIBUTION)
Finite Element: Theory, Applications & Implementation Presented By: Arthur Anconetani Barbara Gault Ryan Whitney.
Variational formulation of the FEM Principle of Stationary Potential Energy: Among all admissible displacement functions u, the actual ones are those which.
STIFFNESS MATRIX METHOD
1 CHAP 3 WEIGHTED RESIDUAL AND ENERGY METHOD FOR 1D PROBLEMS FINITE ELEMENT ANALYSIS AND DESIGN Nam-Ho Kim.
Our task is to estimate the axial displacement u at any section x
Finite Element Method Weak form Monday, 11/4/2002.
Overview of Finite Element Methods
Continuum Mechanics (MTH487)
Introduction to Finite Elements
AAE 556 Aeroelasticity Lecture 6 – Multi-DOF systems
Chapter 1 Stress and Strain.
FEA Simulations Boundary conditions are applied
Introduction to Finite Element Analysis for Skeletal Structures
Implementation of 2D stress-strain Finite Element Modeling on MATLAB
FEM Steps (Displacement Method)
CHAPTER 2 BASIC CONCEPTS OF DISPLACEMENT OR STIFFNESS METHOD:
Review for Mid-Term Exam
CHAPTER 1 Force Analysis. Deformation Analysis.
FINITE ELEMENT METHOD (INTRODUCTION)
F = 10,000 lb A = 2 in2 E = 30 x 106 psi L = 10 ft θ = 45°
Plane Trusses (Initial notes are designed by Dr. Nazri Kamsah)
FINITE ELEMENT METHOD (INTRODUCTION)
Presentation transcript:

Finite Element Analysis MEEN 5330 Dustin Grant Kamlesh Borgaonkar Varsha Maddela Rupakkumar Patel Sandeep Yarlagadda

Introduction What is finite element analysis, FEA? What is FEA used for? 1D Rod Elements, 2D Trusses

Basic Concepts Loads Equilibrium Boundary conditions

Development of Theory Rayleigh-Ritz Method Galerkin’s Method Total potential energy equation Galerkin’s Method

1D Rod Elements To understand and solve 2D and 3D problems we must understand basic of 1D problems. Analysis of 1D rod elements can be done using Rayleigh-Ritz and Galerkin’s method To solve FEA problems same are modified in the Potential-Energy approach and Galerkin’s approach

1D Rod Elements Loading consists of three types : body force f , traction force T, point load Pi Body force: distributed force , acting on every elemental volume of body i.e. self weight of body. Traction force: distributed force , acting on surface of body i.e. frictional resistance, viscous drag and surface shear Point load: a force acting on any single point of element

1D Rod Elements Element strain energy Element stiffness matrix Element -1 Element-2 Element strain energy Element stiffness matrix Load vectors Element body load vector Element traction-force vector

Example 1D Rod Elements Example 1 Problem statement: (Problem 3.1 from Chandrupatla and Belegunda’s book) Consider the bar in Fig.1, determine the following by hand calculation: 1) Displacement at point P 2) Strain and stress 3) Element stiffness matrix 4) strain energy in element Given:

2D Truss 2 DOF Transformations Modified Stiffness Matrix Methods of Solving

2D Truss Transformation Matrix Direction Cosines

2D Truss Element Stiffness Matrix

Methods of Solving Elimination Approach Penalty Approach Eliminate Constraints Penalty Approach Will not discuss Today

Elimination Method Set defection at the constraint to equal zero

Elimination Method Modified Equation DOF’s 1,2,4,7,8 equal to zero

2D Truss Element Stresses Element Reaction Forces

2D Truss Development of Tables Coordinate Table Connectivity Table Direction Cosines Table

2D Truss Coordinate Table

2D Truss Connectivity Table

2D Truss Direction Cosines Table

Example 2D Truss

MATLAB Program TRUSS2D.M

3D Truss Stiffness Matrix 3D Transformation Matrix Direction Cosines

3D Truss Stiffness Matrix 3D Stiffness Matrix

Conclusion Good at Hand Calculations, Powerful when applied to computers Only limitations are the computer limitations

References

Homework