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Chapter 1, page 1

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Collocation method impulse function. Subdomain method weighting functions = 1 ... Collocation - residual vanishes at points(Impulse function) ... – PowerPoint PPT presentation

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Title: Chapter 1, page 1


1
Chapter 1, Introduction
  • FEM numerical procedure for obtaining solutions
    to many engineering problems
  • Uses discrete elements for joint displacements
    and member forces
  • Uses continuum elements for field problems
    heat transfer, fluid mechanics, and solid
    mechanics problems.

2
An analytical solution best
  • Numerical methods must be used to obtain an
    approximate solution when an analytical solution
    can not be found, due to
  • Irregular shape
  • Impossible to describe the boundary
    mathematically
  • Composite materials
  • Anisotropic materials
  • Etc.

3
SOLUTION OF BOUNDARY VALUE PROBLEMS (Solving
physical problems governed by a differential
equation to obtain an approximate solution.)
  • Finite difference method approximates the
    derivatives in the differential equation.
  • Variational method integral of a function
    produces a number find the function that
    produces the lowest number (min.)
  • Weighted residual methods approximate solution
    is substituted into the differential equation.

4
Common Weighted Residual Methods
  • Collocation method impulse function
  • Subdomain method weighting functions 1
  • Galerkins method the approximating function
    is used for the weighting functions
  • Least squares method - uses the residuals as the
    weighting function you get a new error term,
    which must then be minimized
  • What we will use for the field problems

5
INTEGRAL FORMULATION FOR NUMERICAL SOLUTIONS
  • Variational Method
  • It is not applicable to a differential equation
    containing a first derivative
  • Based on Calculus of Variation
  • A functional appropriate for the differential
    equation is minimized with respect to
    undetermined coefficients in the approximate
    solution.

6
Governing differential equation
The calculus of variations shows that the
equation giving the lowest value for p is the
solution of the differential equation
7
Weighted Residual Methods
An approximate solution is substituted into the
governing differential equation for p.
THE RESIDUAL
So we require that
Where wi(x) is the weighting function an R(x) is
the residual. Note Write one residual equation
for every unknown
8
  • Common choices for the weighting functions

Method
Collocation - residual vanishes at points(Impulse
function)
Subdomain - residual vanishes over interval
Approx. function
Galerkins method - similar results to
variational method
Least Squares Method - error minimized with
respect to unknown coefficients in the
approximating solution
9
For a simply supported beam with concentrated end
moments
EI
H
10
Exact Solution
11
Method
Collocation
Subdomain
Galerkin
Least squares
12
In the example, the Galerkins method uses the
same function for wi(x) that was used in the
approximate solution.
.
13
Integrating yields
Solving gives
and the approximate solution is
This solution is identical to the solution
obtained using the variational method.
14
  • Comparison of Errors

30
?
?
?
20
Subdomain method
?
10
?
0.125
0.25
0.375
0.50
0
Percent error in deflection
?
?
?
Variational method Galerkins method Least
squares method
?
10
?
?
20
Collocation method
?
?
30
?
?
Collocation and subdomain method errors depend on
choice of collocation point/subdomain.
15
Structural and Solid Mechanics
Potential Energy Formulation
The displacements at the equilibrium position
occur such that the potential energy of a stable
system is a minimum value.
16
  • The Finite Element Method (FEM) is a numerical
    technique for obtaining approximate solutions to
    engineering problems.
  • Subdivisions
  • Discrete element formulation (Matrix Analysis of
    Structures) Utilizes discrete elements to
    obtain the joint displacements and member forces
    of a structural framework.
  • Continuum element formulation yields
    approximate values of the unknowns at nodes.
  • The FEM produce a system of linear or nonlinear
    equations.

17
THE FINITE ELEMENT METHOD
  • Basic Steps

1. Discretize the region gt nodes 2. Specify
the approximation equation (linear, quadratic) 3.
Develop the system of equations 4. Solve the
system 5. Calculate quantities of interest
derivative of the parameter
Galerkin - 1/node Potential Energy - 1/displ.
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