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MECH593 Introduction to Finite Element Methods

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1 MECH593 Introduction to Finite Element Methods
Finite Element Analysis of 2D Problems Axisymmetric Problems Plate Bending

2 Axi-symmetric Problems
Definition: A problem in which geometry, loadings, boundary conditions and materials are symmetric about one axis. Examples:

3 Axi-symmetric Analysis
Cylindrical coordinates: quantities depend on r and z only 3-D problem D problem

4 Axi-symmetric Analysis

5 Axi-symmetric Analysis – Single-Variable Problem
Weak form: where

6 Finite Element Model – Single-Variable Problem
where Ritz method: Weak form where

7 Single-Variable Problem – Heat Transfer
Weak form where

8 3-Node Axi-symmetric Element
1 2

9 4-Node Axi-symmetric Element
h 4 3 b 1 2 x a z r

10 Single-Variable Problem – Example
z T(r,L) = T0 Step 1: Discretization R L T(R,z) = T0 r T(r,0) = T0 Step 2: Element equation Heat generation: g = 107 w/m3

11 Plate Bending

12 Governing Equations of Classical Plates
From force equilibrium --- Governing Equations for Classical Plates ----- (Distributed Transverse Loading) where Bending Stiffness (Flexural Rigidity) D = Eh3/12(1-n2)

13 Strain Energy of Classical Plates

14 Weak Form of Classical Plates
Governing equation: (isotropic, steady) Weak form: Note: w is the deflection of the mid-plane and u is the weight function.

15 Boundary Conditions of Classical Plates
Essential Boundary Conditions ----- Natural Boundary Conditions ----- Examples: Clamped : Simply connected free

16 4-Node Rectangular Plate Element
Since the governing eq. is 4th order, at each node, there should 2 EBCs and 2 NBCs in each direction (but specify just 2 of them). For displacement-based finite element formulation, the DoFs should be on generalized displacements. In total, there are 3 DoFs per node: where

17 Formulation of 4-Node Rectangular Plate Element
Let Pascal’s Triangle ----- (incomplete 4th order polynomial)

18 3-Node Triangular Plate Element
Let Pascal’s Triangle ----- (incomplete 3th order polynomial)


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