MANE 4240 & CIVL 4240 Introduction to Finite Elements

Slides:



Advertisements
Similar presentations
Finite Element Method CHAPTER 4: FEM FOR TRUSSES
Advertisements

SPECIAL PURPOSE ELEMENTS
MANE 4240 & CIVL 4240 Introduction to Finite Elements
Finite element method Among the up-to-date methods of stress state analysis, the finite element method (abbreviated as FEM below, or often as FEA for analyses.
AERSP 301 Finite Element Method
MANE 4240 & CIVL 4240 Introduction to Finite Elements
Beams and Frames.
Introduction to Finite Elements
LECTURE SERIES on STRUCTURAL OPTIMIZATION Thanh X. Nguyen Structural Mechanics Division National University of Civil Engineering
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
Physics Based Modeling II Deformable Bodies Lecture 2 Kwang Hee Ko Gwangju Institute of Science and Technology.
CST ELEMENT Constant Strain Triangular Element
By S Ziaei-Rad Mechanical Engineering Department, IUT.
APPLIED MECHANICS Lecture 10 Slovak University of Technology
VARIATIONAL FORMULATION OF THE STRAIN LOCALIZATION PHENOMENON GUSTAVO AYALA.
Section 4: Implementation of Finite Element Analysis – Other Elements
MANE 4240 & CIVL 4240 Introduction to Finite Elements
ECIV 720 A Advanced Structural Mechanics and Analysis
Copyright 2001, J.E. Akin. All rights reserved. CAD and Finite Element Analysis Most ME CAD applications require a FEA in one or more areas: –Stress Analysis.
ECIV 720 A Advanced Structural Mechanics and Analysis
MANE 4240 & CIVL 4240 Introduction to Finite Elements
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 Introduction to differential equations Prof. Suvranu De.
MANE 4240 & CIVL 4240 Introduction to Finite Elements Numerical Integration in 1D Prof. Suvranu De.
Copyright © 2002J. E. Akin Rice University, MEMS Dept. CAD and Finite Element Analysis Most ME CAD applications require a FEA in one or more areas: –Stress.
MANE 4240 & CIVL 4240 Introduction to Finite Elements
Finite Element Method in Geotechnical Engineering
Theory of Elasticity Theory of elasticity governs response – Symmetric stress & strain components Governing equations – Equilibrium equations (3) – Strain-displacement.
MANE 4240 & CIVL 4240 Introduction to Finite Elements
MECh300H Introduction to Finite Element Methods
MANE 4240 & CIVL 4240 Introduction to Finite Elements
ECIV 720 A Advanced Structural Mechanics and Analysis
MCE 561 Computational Methods in Solid Mechanics
ECIV 720 A Advanced Structural Mechanics and Analysis Lecture 7: Formulation Techniques: Variational Methods The Principle of Minimum Potential Energy.
CHAP 4 FINITE ELEMENT ANALYSIS OF BEAMS AND FRAMES
III Solution of pde’s using variational principles
MANE 4240 & CIVL 4240 Introduction to Finite Elements
MANE 4240 & CIVL 4240 Introduction to Finite Elements
Finite Element: Theory, Applications & Implementation Presented By: Arthur Anconetani Barbara Gault Ryan Whitney.
The Finite Element Method
ME 520 Fundamentals of Finite Element Analysis
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.
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
Illustration of FE algorithm on the example of 1D problem Problem: Stress and displacement analysis of a one-dimensional bar, loaded only by its own weight,
HEAT TRANSFER FINITE ELEMENT FORMULATION
MECH4450 Introduction to Finite Element Methods
Principles of Computer-Aided Design and Manufacturing Second Edition 2004 ISBN Author: Prof. Farid. Amirouche University of Illinois-Chicago.
CHAP 3 WEIGHTED RESIDUAL AND ENERGY METHOD FOR 1D PROBLEMS
11 10-Jan-16 Last course Interpretations and properties of the stiffness matrix (cont’d) The DSM for plane and space trusses.
1 HOW MANY ELEMENTS? How to choose element size? –Critically important in obtaining good results –Mesh refinement improves solution accuracy. –How small.
Finite Element: Theory, Applications & Implementation Presented By: Arthur Anconetani Barbara Gault Ryan Whitney.
CAD and Finite Element Analysis Most ME CAD applications require a FEA in one or more areas: –Stress Analysis –Thermal Analysis –Structural Dynamics –Computational.
1 Variational and Weighted Residual Methods. 2 Introduction The Finite Element method can be used to solve various problems, including: Steady-state field.
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 in Geotechnical Engineering
FE Exam Tutorial
MANE 4240 & CIVL 4240 Introduction to Finite Elements
CAD and Finite Element Analysis
Introduction to Finite Elements
Materials Science & Engineering University of Michigan
1C9 Design for seismic and climate changes
FEA convergence requirements.
FEA Simulations Boundary conditions are applied
ECIV 720 A Advanced Structural Mechanics and Analysis
Implementation of 2D stress-strain Finite Element Modeling on MATLAB
Presentation transcript:

MANE 4240 & CIVL 4240 Introduction to Finite Elements Prof. Suvranu De Convergence of analysis results

Reading assignment: Lecture notes Summary: Concept of convergence Criteria for monotonic convergence : completeness (rigid body modes + constant strain) + compatibility Incompatible elements and the patch test Rate of convergence

Errors that affect finite element solution results Type of error Source 1. Discretization error Use of FE interpolations for geometry and solution variables 2. Numerical integration Evaluation of FE element matrices and vectors using numerical integration 3. Round off This error is due to the finite precision arithmetic used in digital computers

What is “convergence”? “Convergence” of FE solution results to the exact solution of the mathematical model FE scheme exhibits convergence if the Discretization error →0 as the mesh is made infinitely fine (i.e., element size →0) Physical system Mathematical model FE model

Mesh refinement h-refinement p-refinement h=element size p=polynomial order

Convergence in energy and displacement u : exact displacement solution to a problem that makes the potential energy of the system a minimum corresponding stress and strain Exact strain energy of the body uh : FE solution (‘h’ refers to the element size) Approximate strain energy of the body

Calculation of strain energies Example: Consider a linear elastic bar with varying cross section 1 2 x The governing differential (equilibrium) equation P=3E/80 80cm Eq(1) E: Young’s modulus Boundary conditions Analytical solution

Note The exact strain energy of the system is If we discretize the problem using a single linear finite element, the stiffness matrix is The strain energy of the FE system is Note

Convergence in strain energy Monotonic convergence Nonmonotonic convergence

Convergence in displacement Monotonic convergence Nonmonotonic convergence

Criteria for monotonic convergence 1. COMPLETENESS 2. COMPATIBILITY © 2002 Brooks/Cole Publishing / Thomson Learning™

CONDITION 1. COMPLETENESS This requires that the displacement interpolation functions must be chosen so that the elements can represent 1. Rigid body modes 2. Constant strain states

Rigid body modes

The # of rigid body modes of an element = # of zero eigenvalues of the element stiffness matrix

Constant strain states Strain computed using linear finite elements Actual variation of strain e x

Mathematical implication of the two conditions (rigid body modes + constant strain state) Inside a finite element (of any order) in 1D but this is just a polynomial… Hence The requirement for completeness in 1D is that the displacement approximation be at least a linear polynomial of degree (k=1), ie any 2 node element and higher is complete

Mathematical implication of the two conditions (rigid body modes + constant strain state) Inside a finite element (of any order) in 2D but this is just a polynomial… Hence The requirement for completeness in 1D is that the displacement approximation be at least a linear polynomial of degree (k=1).

Mathematical implication of the two conditions (rigid body modes + constant strain state) The element displacement approximation must be at least a COMPLETE polynomial of degree one k=1 1D 2D

In 2D, the minimum displacement assumption needs to be Translation along x Translation along y Rigid body rotation about z-axis

CONDITION 2. COMPATIBILITY The assumed displacement variations are continuous within elements and across inter-element boundaries Ensures that strains are bounded within elements and across element boundaries. If ‘u’ is discontinuous across element boundaries then the strains blow up in-between elements and this leads to erroneous contributions to the potential energy of the structure Physical meaning: no gaps/cracks open up when the finite element assemblage is loaded

Nonconforming elements and the patch test Conforming = compatible Nonconforming = incompatible Ideal: Conforming elements Observation: Certain nonconforming elements also give good results, at the expense of nonmonotonic convergence Nonconforming elements: satisfy completeness do not satisfy compatibility result in at least nonmonotonic convergence if the element assemblage as a whole is complete, i.e., they satisfy the PATCH TEST

PATCH TEST: 1. A patch of elements is subjected to the minimum displacement boundary conditions to eliminate all rigid body motions 2. Apply to boundary nodal points forces or displacements which should result in a state of constant stress within the assemblage 3. Nodes not on the boundary are neither loaded nor restrained. 4. Compute the displacements of nodes which do not have a prescribed value 5. Compute the stresses and strains The patch test is passed if the computed stresses and strains match the expected values to the limit of computer precision.

NOTES: 1. This is a great way to debug a computer code 2. Conforming elements ALWAYS pass the patch test 3. Nodes not on the boundary are neither loaded nor restrained. 4. Since a patch may also consist of a single element, this test may be used to check the completeness of a single element 5. The number of constant stress states in a patch test depends on the actual number of constant stress states in the mathematical model (3 for plane stress analysis. 6 for a full 3D analysis)

CONVERGENCE RATE This is a measure of how fast the discretization error goes to zero a the mesh is refined Convergence rate depends on the order of the complete polynomial (k) used in the displacement approximation k=1 k=2 k=3

It can be shown that for (1) a sufficiently refined mesh and (2) for problems whose analytical solution does not contain singularities Convergence in strain energy : order 2k Convergence in displacements : order p=k+1 C and C1 are constants independent of ‘h’ but dependent on 1. the analytical solution 2. material properties 3. type of element used

Ex: for a domain discretized using 4 node plane stress/strain elements (k=1) Large C shifts curve up slope = 2

Important property of finite element solution: When the conditions of monotonic convergence are satisfied (compatibility and completeness) the finite element strain energy always underestimates the strain energy of the actual structure Strain energy of mathematical model Strain energy of FE model