Numerical analisys of discontinuities in beam structures.
Stan, Florina ; Grozea, Marius-Alexandru ; Dobrescu, Corina 等
1. INTRODUCTION
Beam structures are widespreaded, representing efficient and safe
solutions in civil and industrial structures, as well as in mechanical
engineering. In many types of activities, a great variety of lifting and
transport installations are used, which may execute lifting, moving,
transport, bringing down, loading, discharging, assembling, turning,
overturning operations etc. It is the case of the rolling bridges,
cranes, elevators, waggons, spinning towers etc. The modelling and
analisys of these structures as ensembles are quite simple due to the
variety of the high-performance computer codes based on: displacement
method, finite element method (Cioata, 2008) or algorythm based
analytical methods.
Beam structures (Boiangiu & Alecu, 2008) have geometrical and
constructive discontinuities and their calculus becomes difficult when
referring to the junctions between the beams.
The paper presents the calculus with finite elements of a junction
which is considered submodel and is isolated from the assembly of a
complex structure.
The substructuring technique (Constantinescu & Sorohan, 2003)
represents the sole method to get results close to reality, but the
working methodologies are not developed enough.
The problem of discontinuities in the beam structures nodes
presented in this paper involves deep investigations and the use of
special calculus methods like the finite element method and some proper
working methodologies because in these zones important stress
concentrations often appear.
The working methodology used in this paper may be extended to any
type of junction, no matter how complex.
[FIGURE 1 OMITTED]
[FIGURE 2 OMITTED]
2. MODELLING OF FOUR STRAIGHT BEAM JUNCTION
The rectangular junction between two circular section beams (pipes)
and two rectangular section beams was taken into consideration. The
general view of the junction is shown in figure 1.
This junction is a substructure or a submodel and it is obtained
from the structure ensemble by "cutting" at a certain distance
from the center of the node. In the cutting sections, the efforts and
displacements which were determined in a first stage for the structure
ensemble may be introduced in the submodel. The dimensions of the
submodel are shown in figure 2. The pipe with circular section broke
through the one with rectangular section, the two components of the
junction being assembled with 10 mm corner soldering.
[FIGURE 3 OMITTED]
[FIGURE 4 OMITTED]
The submodel was meshed with 21376 three dimensional brick finite
elements, with eight nodes and three degrees of freedom per node,
defined on a network of 28850 nodes. The submodel configuration and the
meshing are presented in figure 3.
The XYZ global coordinate system, to which the model is related, is
also figured.
The loads applied to the submodel are concentrated forces applied
in nodes, on the circular section beam, as follows:
--a [F.sub.X] = 2 kN resultant force, applied on the face of the
model with Z = 120 mm, on the X direction;
--a [F.sub.Z] = 2 kN resultant force applied on the face of the
model with Z = 120 mm, on the Z direction;
--a [F.sub.Y] = -4.2 kN resultant force applied on the exterior
face of the pipe, on a 50 mm length and a 30 mm width, on the Y
direction.
The constraints of the submodel were defined by null displacements
on the X, Y, Z directions in the inferior surface nodes of the
rectangular section pipe (Y = 110 mm).
The measuring units for all the calculations were Newtons and
Milimeters.
The elastic constants of the material (construction steel) were
considered with the following values:
--the Young's modulus E = 2.1 x [10.sup.5] MPa;
--the shear modulus G = 8.1x [10.sup.4] N/[mm.sup.2];
--the Poisson's ratio v = 0.3.
3. RESULTS OF THE JUNCTION ANALISYS
The finite element analyses (Ghionea et al., 2008) yielded a great
volume of information, from which only a small part is presented in a
simple and suggestive form. In figure 4, the configuration of the
deformed junction (with a multiplication factor of 300) as well as the
map of the resultant (total) displacement values, are presented.
The general configuration of the stress state and the zone with the
maximum equivalent stress are shown in figure 5. In figure 6, the
variation of the von Mises equivalent stress along a part of the
soldering between the two components of the junction is graphically
represented.
Because the model of the analyzed junction is three dimensional and
the meshing was realized with brick finite elements it is impossible to
directly estimate the stress state in the model. To obtain an image of
it, some sections with several planes are made, preferable with parallel
planes with the global coordinate system of the model.
[FIGURE 5 OMITTED]
[FIGURE 6 OMITTED]
4. CONCLUSIONS
1. Even if the analyzed junction is quite simple--geometrically and
constructive--it required a great volume of work, to create the finite
element model, to postprocess the results and to present them clearly.
2. The values of the stresses reveal phenomenon of stress
concentration and important values of local stresses (Hadar et al.,
2007) which in certain circumstances can be determined for correct
estimations of the safety coefficient and of the reliability of the beam
structure from which the analyzed junction was "detached".
3. The stress state configurations are clearly nonlinear, which
motivates the interest and the engineering importance of the steps like
the one shown above.
5. ACKNOWLEDGEMENT
The paper is conceveid in the frame of P.O.S.D.R.U.
Programme--University POLITEHNICA of Bucharest.
6. REFERENCES
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