Structures Matrix Analysis Introduction to Finite Element Analysis

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Structures Matrix Analysis Introduction to Finite Element Analysis Sina Askarinejad 1/1 7/8/2016 1

Structures Matrix Analysis Introduction to Finite Element Analysis Sina Askarinejad 1/1 7/8/2016 1

Hook’s Law. . • 2

Hook’s Law. . • 2

Application to elastic materials • 3

Application to elastic materials • 3

Structures and elements In order to analyze engineering structures, we divide the structure into

Structures and elements In order to analyze engineering structures, we divide the structure into small sections. F d 1=? Nodes Elements 1. Trusses 2. Beams 3. Plates 4. Shells 5. 3 -D solids 4

Truss • Truss is a slender member (length is much larger than the cross-section).

Truss • Truss is a slender member (length is much larger than the cross-section). • It is a two-force member i. e. it can only support an axial load and cannot support a bending load. • The cross-sectional dimensions and elastic properties of each member are constant along its length. • The element may interconnect in a 2 -D or 3 -D configuration in space. • The element is mechanically equivalent to a spring, since it has no stiffness against applied loads except those acting along the axis of the member. (Beam is a truss that can tolerate bending load with rotation) 5

Complex structures with simple elements 6

Complex structures with simple elements 6

Finite element method • Step 1: Divide the system into bar/truss elements connected to

Finite element method • Step 1: Divide the system into bar/truss elements connected to each other through the nodes • Step 2: Describe the behavior of each bar/truss element (i. e. derive its stiffness matrix and load vector in local AND global coordinate system) • Step 3: Describe the behavior of the entire system by assembling their stiffness matrices and load vectors • Step 4: Apply appropriate boundary conditions and solve 7

E, A, L Two nodes: 1, 2 Nodal displacements: Nodal forces: Spring constant: Element

E, A, L Two nodes: 1, 2 Nodal displacements: Nodal forces: Spring constant: Element stiffness matrix in local coordinates Element force vector Element stiffness matrix Element nodal displacement vector 8

y x At node 1: At node 2: 9

y x At node 1: At node 2: 9

y x Rewrite as 10

y x Rewrite as 10

In the global coordinate system, the vector of nodal displacements and loads Our objective

In the global coordinate system, the vector of nodal displacements and loads Our objective is to obtain a relation of the form Where k is the 4 x 4 element stiffness matrix in global coordinate system 11

Relationship between and for the truss element At node 1 At node 2 Putting

Relationship between and for the truss element At node 1 At node 2 Putting these together 12

Putting all the pieces together y x The desired relationship is Where is the

Putting all the pieces together y x The desired relationship is Where is the element stiffness matrix in the global coordinate system 13

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Assembly…. 15

Assembly…. 15

Same procedure for 3 -D trusses © 2002 Brooks/Cole Publishing / Thomson Learning™ 16

Same procedure for 3 -D trusses © 2002 Brooks/Cole Publishing / Thomson Learning™ 16

Transformation matrix T relating the local and global displacement and load vectors of the

Transformation matrix T relating the local and global displacement and load vectors of the truss element Element stiffness matrix in global coordinates 17

Global k for 3 -d trusses 18

Global k for 3 -d trusses 18

Solve the following problem with your previous knowledge about springs and the method that

Solve the following problem with your previous knowledge about springs and the method that you just learned E 1, A 1 E 2, A 2 F L 1 L 2 19