Title: Chapter 1, page 1
1Chapter 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.
2An 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.
3SOLUTION 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.
4Common 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
5INTEGRAL 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. -
6Governing differential equation
The calculus of variations shows that the
equation giving the lowest value for p is the
solution of the differential equation
7Weighted 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
9For a simply supported beam with concentrated end
moments
EI
H
10Exact Solution
11Method
Collocation
Subdomain
Galerkin
Least squares
12In the example, the Galerkins method uses the
same function for wi(x) that was used in the
approximate solution.
.
13Integrating yields
Solving gives
and the approximate solution is
This solution is identical to the solution
obtained using the variational method.
1430
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?
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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.
15Structural 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.
17THE FINITE ELEMENT METHOD
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.