The document discusses the finite element method (FEM) for analyzing beam structures. FEM involves subdividing a structure into finite elements of simple shape and solving for the whole structure. Elements can be one-, two-, or three-dimensional, with accuracy increasing with more elements. Nodes are points where elements connect, and nodal displacements describe element deformation. FEM allows analyzing complex shapes like plates by treating them as assemblies of beams. A simple bar analysis example demonstrates deriving and solving the stiffness matrix to determine displacements and forces from applied loads.

1. TheFiniteElementMethod For Beam Analysis

2. The F.E.M. Defined In finite element method, the structure to be analyzed is subdivided into a mesh of finite-sized elements of simple shape, and then the whole structure is solved with quite easiness. Finite Sized Element Rectangular Body Circular Plate

3. Finite Sized Elements The rectangular panel in the rectangular body and triangular panel in the circular plate are referred to an ‘element’. There’re one-, two- and three-dimensional elements. The accuracy of the solution depends upon the number of the finite elements; the more there’re, the greater the accuracy.

4. Finite Element of a Bar If a uniaxial bar is part of a structure then it’s usually modeled by a spring element if and only if the bar is allowed to move freely due to the displacement of the whole structure. (One dimensional element) Bar Uniaxial bar of the structure Structure Spring element

5. Types of Elements Here goes the examples of two- and three-dimensional finite sized elements. Triangle Rectangle Hexahedron

6. Node The points of attachment of the element to other parts of the structure are called nodes. The displacement at any node due to the deformation of structure is known as the nodal displacement. Node

9. Simple Bar Analysis Consider a simple bar made up of uniform material with length L and the cross-sectional area A. The young modulus of the material is E. Since any bar is modeled as spring in FEM thus we’ve: L x2 k F1 F2 x1

10. Let us suppose that the value of spring constant is k. Now, we’ll evaluate the value of k in terms of the properties (length, area, etc.) of the bar: We know that: i.e. Also: i.e. And i.e. Simple Bar Analysis

11. Now substituting the values of x and F is the base equation of k, we’ll have: But Hence, we may write: Simple Bar Analysis

12. Simple Bar Analysis According to the diagram, the force at node x1 can be written in the form: Where x1 – x2is actually the nodal displacement between two nodes. Further: Similarly:

13. Simple Bar Analysis Now further simplification gives: These two equations for F1 and F2 can also be written as, in Matrix form: Or:

14. Simple Bar Analysis Here Ke is known as the Stiffness Matrix. So a uniform material framework of bars, the value of the stiffness matrix would remain the same for all the elements of bars in the FEM structure.

15. Similarly for two different materials bars joined together, we may write: ; Further Extension k1 k2 F1 F2 F3 x1 x2 x3

16. Numerical Problem With The Help Of FEM Analysis For Bars

17. Problem Three dissimilar materials are friction welded together and placed between rigid end supports. If forces of 50 kN and 100 kN are applied as indicated, calculate the movement of the interfaces between the materials and the forces exerted on the end support. Steel Rigid support 50 kN Brass Aluminium 100 kN

18. Given Data And Diagram k1 k2 k3 F1 F2 F3 F4 x1 x2 x3 x4

19. The system may be represented as the system of three springs. Hence, the spring are shown. Values of spring constant can be determined as: Analysis

20. From the extension of FEM, we can write the force-nodal equations for this system as: Solving this system and adding similar equations yields: Analysis

21. Now: From these equations we can easily determine the unknowns, but we’ll have to apply the boundary conditions first. Analysis

22. At point 1 and 4, the structure is fixed, and hence no displacement can be produced here. Thus, we’ll say that: And also, from the given data, we know that: Analysis

23. Now, simply putting these values in the equations, we get: And: And, that was the required. Analysis

24. The Last Word Complex Structure Analysis

25. Complex Structures Complex structures which contain the material continuum, are subdivided into the elements and are analyzed on the computers. Software packages are available for the determination of the Stiffness matrix of those structures. Some software packages also allow virtual subdivision on the computer as well i.e. computer automatically analyzes the shape, and gives the stress-strain values at any point of the structure.

26. Example Complex Structure FEM Structure

27. Inclined Bars Inclined bars are always analyzed by resolving them into their x- and y-components. The value of the inclined angle is always known and then the components are evaluated. Three-dimensional structures involve three dimensional elements i.e. elements with three dimensions (length, width, thickness).

28. Importance FEM has become very familiar in subdivision of continuum. It gives reliable and accurate results if the number of elements are kept greater. Modern computer technology had helped this analysis to be very easy and less time consuming. Large structures under loadings are now easily solved and stresses on each and every part are now being determined.

29. Thank YouVery Much Sheikh Haris Zia 08-ME-39 Ibrahim Azhar 08-ME-53 Muhammad Haris 08-ME-69