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MECH593 Introduction to Finite Element Methods

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MECH593 Introduction to Finite Element Methods. Finite Element Analysis of 2-D Problems. Dr. Wenjing Ye – PowerPoint PPT presentation

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Title: MECH593 Introduction to Finite Element Methods


1
MECH593 Introduction to Finite Element Methods
Finite Element Analysis of 2-D Problems Dr.
Wenjing Ye
2
2-D Discretization
Common 2-D elements
3
2-D Model Problem with Scalar Function- Heat
Conduction
  • Governing Equation

in W
  • Boundary Conditions

Dirichlet BC
Natural BC
Mixed BC
4
Weak Formulation of 2-D Model Problem
  • Weighted - Integral of 2-D Problem -----
  • Weak Form from Integration-by-Parts -----

5
Weak Formulation of 2-D Model Problem
  • Green-Gauss Theorem -----

where nx and ny are the components of a unit
vector, which is normal to the boundary G.
6
Weak Formulation of 2-D Model Problem
  • Weak Form of 2-D Model Problem -----

EBC Specify T(x,y) on G NBC Specify
on G
where
is the normal outward flux on
the boundary G at the segment ds.
7
FEM Implementation of 2-D Heat Conduction Shape
Functions
Step 1 Discretization linear triangular element
T1
Derivation of linear triangular shape functions
T2
Let
T3
Interpolation properties
Same
8
FEM Implementation of 2-D Heat Conduction Shape
Functions
linear triangular element area coordinates
T1
A2
A3
A1
T2
T3
9
Interpolation Function - Requirements
  • Interpolation condition
  • Take a unit value at node i, and is zero at all
    other nodes
  • Local support condition
  • fi is zero at an edge that doesnt contain node
    i.
  • Interelement compatibility condition
  • Satisfies continuity condition between adjacent
    elements over any element boundary that includes
    node i
  • Completeness condition
  • The interpolation is able to represent exactly
    any displacement field which is polynomial in x
    and y with the order of the interpolation
    function

10
Formulation of 2-D 4-Node Rectangular Element
Bi-linear Element
Let
Note The local node numbers should be arranged
in a counter-clockwise sense. Otherwise, the area
Of the element would be negative and the
stiffness matrix can not be formed.
f2
f4
f1
f3
11
FEM Implementation of 2-D Heat Conduction
Element Equation
  • Weak Form of 2-D Model Problem -----

Assume approximation and let w(x,y)fi(x,y) as
before, then
where
12
FEM Implementation of 2-D Heat Conduction
Element Equation
13
Assembly of Stiffness Matrices
14
Imposing Boundary Conditions
The meaning of qi
3
3
1
1
1
2
2
3
3
1
1
1
2
2
15
Imposing Boundary Conditions
Consider
Equilibrium of flux
FEM implementation
16
Calculating the q Vector
Example
17
2-D Steady-State Heat Conduction - Example
A
D
AB
CD convection
DA and BC
0.6 m
C
B
0.4 m
y
x
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