3d Stiffness Matrix
3d Stiffness Matrix
3d Stiffness Matrix
Lecture 2
Matrix Structural Analysis of Framed
Structures
Introduction
In this chapter, we shall derive the element
stiness matrix [k] of various one dimensional
elements. Only after this important step is well
understood, we could expand the theory and
introduce the structure stiness matrix [K] in its
global coordinate system.
Introduction
As will be seen later, there are two fundamentally
dierent approaches to derive the stiness
matrix of one dimensional element. The rst one,
which will be used in this chapter, is based on
classical methods of structural analysis (such as
moment area or virtual force method). Thus,
in deriving the element stiness matrix, we will be
reviewing concepts earlier seen.
Introduction
The other approach, based on energy
consideration through the use of assumed shape
functions, will be examined later. This second
approach, exclusively used in the nite element
method, will also be extended to two
dimensional continuum elements.
Influence Coefficients
In structural analysis an inuence coecient Cij
can be dened as the eect on d.o.f. i due to a unit
action at d.o.f. j for an individual element or a hole
structure. Examples of Inuence Coecients are
shown in Table 2.1.
It should be recalled that inuence lines are
associated with the analysis of structures subjected
to moving loads (such as bridges), and that the
exibility and stiness coecients are components
of matrices used in structural analysis.
Influence Coefficients
Flexibility Matrices
Flexibility Method
Stiffness Coefficients
Truss Element
Beam Elements
There are two major beam theories:
Euler-Bernoulli which is the classical
formulation for beams.
Timoshenko which accounts for transverse
shear deformation eects.
Grid Element
3D Frame Element
3D Frame Element