ECIV 720 A Advanced Structural Mechanics and Analysis Lecture 10: Solution of Continuous Systems – Fundamental Concepts Mixed Formulations Intrinsic Coordinate.

Slides:



Advertisements
Similar presentations
MANE 4240 & CIVL 4240 Introduction to Finite Elements
Advertisements

AERSP 301 Finite Element Method
Isoparametric Elements Element Stiffness Matrices
Basic FEA Procedures Structural Mechanics Displacement-based Formulations.
Beams and Frames.
MANE 4240 & CIVL 4240 Introduction to Finite Elements
Some Ideas Behind Finite Element Analysis
By S Ziaei-Rad Mechanical Engineering Department, IUT.
Fundamentals of Elasticity Theory
ECIV 720 A Advanced Structural Mechanics and Analysis
ECIV 720 A Advanced Structural Mechanics and Analysis
ECIV 520 A Structural Analysis II
Materials Science & Engineering University of Michigan
Bars and Beams FEM Linear Static Analysis
MANE 4240 & CIVL 4240 Introduction to Finite Elements Introduction to 3D Elasticity Prof. Suvranu De.
Engineering Systems Lumped Parameter (Discrete) Continuous A finite number of state variables describe solution Algebraic Equations Differential Equations.
PAEN - 2nd Section Stability of structures Methods Initial Imperfections.
MANE 4240 & CIVL 4240 Introduction to Finite Elements
Outline Introduction to Finite Element Formulations
Finite Element Method in Geotechnical Engineering
MANE 4240 & CIVL 4240 Introduction to Finite Elements
ECIV 520 A Structural Analysis II Stiffness Method – General Concepts.
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.
One-Dimensional Problems
ECIV 720 A Advanced Structural Mechanics and Analysis Lecture 12: Isoparametric CST Area Coordinates Shape Functions Strain-Displacement Matrix Rayleigh-Ritz.
ECIV 720 A Advanced Structural Mechanics and Analysis
ECIV 720 A Advanced Structural Mechanics and Analysis Non-Linear Problems in Solid and Structural Mechanics Special Topics.
CST ELEMENT STIFFNESS MATRIX
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.
2005 February, 2 Page 1 Finite Element Analysis Basics – Part 2/2 Johannes Steinschaden.
CHAP 4 FINITE ELEMENT ANALYSIS OF BEAMS AND FRAMES
III Solution of pde’s using variational principles
CHAP 5 FINITE ELEMENTS FOR HEAT TRANSFER PROBLEMS
MANE 4240 & CIVL 4240 Introduction to Finite Elements
Finite Element: Theory, Applications & Implementation Presented By: Arthur Anconetani Barbara Gault Ryan Whitney.
2004 March, 4 Page 1 Finite Element Analysis Basics – Part 2/2 Johannes Steinschaden.
ME 520 Fundamentals of Finite Element Analysis
Section 2: Finite Element Analysis Theory
School of Civil EngineeringSpring 2007 CE 595: Finite Elements in Elasticity Instructors: Amit Varma, Ph.D. Timothy M. Whalen, Ph.D.
Finite Element Method.
Mechanics of Thin Structure Lecture 15 Wrapping Up the Course Shunji Kanie.
1 Variational and Weighted Residual Methods. 2 The Weighted Residual Method The governing equation for 1-D heat conduction A solution to this equation.
Chapter 6. Plane Stress / Plane Strain Problems
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.
Summer School for Integrated Computational Materials Education 2015 Computational Mechanics: Basic Concepts and Finite Element Method Katsuyo Thornton.
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
11 10-Jan-16 Last course Interpretations and properties of the stiffness matrix (cont’d) The DSM for plane and space trusses.
Variational and Weighted Residual Methods
1 Non-Linear Piezoelectric Exact Geometry Solid-Shell Element Based on 9-Parameter Model Gennady M. Kulikov Department of Applied Mathematics & Mechanics.
Finite Element: Theory, Applications & Implementation Presented By: Arthur Anconetani Barbara Gault Ryan Whitney.
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.
Finite Element Method in Geotechnical Engineering
1D OF FINITE ELEMENT METHOD Session 4 – 6
Continuum Mechanics (MTH487)
FEM : Finite Element Method 2017.
Introduction to Finite Elements
(برای دوره کارشناسی ارشد مکانیک سنگ) Finite Element Procedures
Materials Science & Engineering University of Michigan
1C9 Design for seismic and climate changes
Introduction to Finite Element Analysis for Skeletal Structures
ECIV 720 A Advanced Structural Mechanics and Analysis
Presentation transcript:

ECIV 720 A Advanced Structural Mechanics and Analysis Lecture 10: Solution of Continuous Systems – Fundamental Concepts Mixed Formulations Intrinsic Coordinate Systems

Last Time Weighted Residual Formulations Consider a general representation of a governing equation on a region V L is a differential operator eg. For Axial element

Last Time Weighted Residual Formulations Exact Approximate Objective: Define so that weighted average of Error vanishes NOT THE ERROR ITSELF !!

Last Time Weighted Residual Formulations Set Error relative to a weighting function  Objective: Define so that weighted average of Error vanishes

Weighted Residual Formulations   ERROR

Weighted Residual Formulations   ERROR

Last Time Weighted Residual Formulations  ERROR

Last Time Weighted Residual Formulations Assumption for approximate solution (Recall shape functions) Assumption for weighting function GALERKIN FORMULATION

Last Time Weighted Residual Formulations  i are arbitrary and  0

Last Time Galerkin Formulation Algebraic System of n Equations and n unknowns

Last Time Galerkin’s Method in Elasticity Governing equations Interpolated Displ Field Interpolated Weighting Function

Last Time Galerkin’s Method in Elasticity Integrate by part…

Last Time Galerkin’s Method in Elasticity Virtual Work Compare to Total Potential Energy Virtual Total Potential Energy

Last Time Galerkin’s Formulation More general method Operated directly on Governing Equation Variational Form can be applied to other governing equations Preffered to Rayleigh-Ritz method especially when function to be minimized is not available.

Mixed Formulation Displacement Based FE approximations –Combine subsidiary equations to obtain G.E. –G.E. in terms of displacements –Stresses, Strains etc enter as natural B.C. Mixed Formulation –Apply Galerkin directly on subsidiary relations –Nodal dof contain displacements AND other field quantities

Mixed Formulation Axial Equilibrium… Stress-Displacement…

Mixed Formulation

Galerkin Residual Equations Axial Equilibrium… Stress-Displacement…

Mixed Formulation Axial Equilibrium…

Mixed Formulation A

Stress-Displacement… B

Mixed Formulation kuku kuku k  A B

Mixed Formulation

Application Example

INTRINSIC COORDINATE SYSTEMS

Intrinsic Coordinate System  x1x1 x x2x2 x3x3  1 =-1 1  3  2 =1 2 Global C.S. Local C.S.

Intrinsic Coordinate System  x1x1 x x2x2 x3x3  1 =-1 1  3  2 =1 2 Linear Relationship Between GCS and LCS

Shape Functions wrt LCS  u(-1)=a 0 -a 1 +a 2 =u 1 u(1)=a 0 +a 1 +a 2 =u 2 u(0)=a 0 =u 3 … u(  )=a 0 +a 1  +a 2  2  1 =-1 1   2 =1 32

Shape Functions wrt Intrinsic Coordinate System  N1()N1() N2()N2() N3()N3()

 wrt 

Element Strain-Displacement Matrix Cast in Matrix Form  e  = B u e  e  = E B u e

Linear Stress Axial Element - In Summary  = B u  = E B u  1 =-1 1     2 =1 32

Linear Stress Axial Element - k e Stiffness Matrix

Linear Stress Axial Element - k e Stiffness Matrix  1 =-1 1     2 =

Linear Stress Axial Element – f e,T e  1 =-1 1     2 =1 32 Body Force Uniformly Distributed Force