2.3.4
Application examples
Three application examples
are shown below:
Free
edge problem
The free edge problem deals
with a laminate subjected to a tensile load with free edges. In our case, it
is a symmetrical multi-layered material (q1,...,qn)5
made up of N =
2n layers of orthotropic materials. Keeping in mind the symmetries, the
problem can be reduced to the determination of the generalized fields in the
lower right fourth section of Figure 1.

Figure 1.
Free edge problem of a symmetrical multi-layered material simplified by symmetry.
Let us take
the example of a (0,90)S made up of a carbon-epoxy UD composite
material. The material properties in the orthotropy coordinates system are:
EL
= 150GPa, ET = 10GPa, EN =
10GPa
GLT = 5GPa, GLN = 5GPa, GTN
= 5GPa
nLT
= 0.3 y nLN
= 0.3
The layer
thickness value is 1mm, the laminate width value is 10mm
and the axial strain
e =
1%.
These stages
are to be followed for obtaining the generalized fields:
- Definition of the multi-layered
material. In main window of DEILAM, type 4 in the space for the total number
of layers. Next, enter in the table the properties of the previously defined
layers (see Figure 2).

Figure 2.
Definition of a carbon-epoxy (0,90)S laminate.
- Definition of the calculation
properties. Click on the DEILAM <<Option>> in the main window
menu (see Figure 3). In this window, uncheck the 2 options
in which thermal and hygroscopic strains are considered (see Figure
4). Select the option for all generalized displacements and stresses (see
Figure 4).

Figure 3.
Where to click so that the calculation properties can be defined?

Figure 4.
Definition of the calculation properties.
- Definition of loads.
Click on the button <<Loads>> in the DEILAM main window (see Figure
5). From the list of predetermined configurations shown in the window,
select the <<Tensile load with free edges>> option and type 1
in the space corresponding to the strain e
(see Figure 6). Finally, click on the button <<Read
the configurations>>.

Figure 5.
Where to click for defining the loads?

Figure 6.
Load configuration.
- Definition of the meshing.
Click on the <<Meshing of the width [0, b]>> button in
the main window (see Figure 7). Select, from the window
that appears, the <<Automatic>> option in the list of meshing
types (see Figure 8). In the space for the value of width
b (in our case, b equals the half of the laminate width as a
result of the simplification by symmetry), enter 5 (see Figure
8).

Figure 7.
Where to click for the definition of the meshing?

Figure 8.
Definition of the meshing.
- Execution of the calculations.
Click on the <<Analyze>> button in the DEILAM main window (see
Figure 9).

Figure 9.
Where to click for executing the calculations?
- Visualization
of the results. After the previous stage, a new window appears. Click on the
<<Fields to be displayed>> button in this window (see Figure
10), and, in the new window (see Figure 11), select
from the <<Fields to be displayed>> list, the <<In-plane
and out-of-plane forces per layer>> option. Check the box that corresponds
to the Niyy (membranar force: in-plane force)
field, and enter 1-2 (for plotting the membranar forces in layers 1 and 2:
layers at 0° and at 90°, respectively) in the corresponding space.
Then click on the <<Draw>> button. You will see a graph as the
one in Figure 12. To distinguish both curves, click on
the <<Chart properties>> button and select the colors and types
of line you wish in order to make a difference between the curves.

Figure 10.
Where to click for selecting the fields to be plotted in the chart?

Figure 11.
Configuration for plotting the graph.

Figure 12.
Plotting the curves of the selected fields.
- Visualization of other
fields. To visualize the plots of other fields such as interfacial stresses
or generalized displacements, just retake stage 6 and select
the desired fields.
Analysis
of stresses in an adhesive joint
Let us consider
the following adhesive joint:
Figure 13.
Adhesive joint.
We suppose that there is
a generalized plane strain e =
0 state. The linear force F value is 100MPa.mm. Taking
the symmetries into account, the problem may be reduced to the lower half of
the assembly (see Figure 13).
In order to perform the
stress analysis in this assembly with the help of DEILAM, follow these stages:
- Definition of the laminate
(see Figure 14). In the main window of DEILAM, in the
space of the total number of layers type 6. Then, in the table, enter the
properties of the layers defined in Figure 13. Since
these are isotropic material layers:
- " The Young's
moduli EL , ET and EN
value is E (the isotropic material Young's modulus)
- " The Poisson's
ratios nLT
and nLN
value are n (the isotropic
material Poisson's ratio>>
- " The shear
moduli GLT, GLN and GTN
value is
(the
isotropic material shear modulus).

Figure 14.
Defining the properties of the laminate.
- Definition of the calculation
properties. In the main window menu, click on <<Options>> of DEILAM.
In the window that will appear, uncheck the 2 options of taking into account
the thermal and hygroscopic strains (see Figure 15).
Select the option all the generalized forces and displacements (see Figure
15).

Figure 15.
Definition of the calculation properties.
- Loads definition. In
the main window of DEILAM, click on the button <<Loads>>. In the
window that appears (called <<Configuration of the hygrothermal and
mechanical loads>>), in the list of predetermined configurations select
<<None>> (see Figure 16). Now, in this window,
select in the configuration of the boundary conditions the options of the
forces and moments on the left and right sides. Then, type 0 in the strain
space e (see Figure
16). Then click on the button <<Values of the boundary conditions>>.
A new window (called <<Values of the boundary conditions>>. In
this new window, you define first the values at the left edge as follows (see
Figure 17):
In the type of data
input, select the option input per layer and select layer 1. In the options
of forces and displacements, select the <<Left>> edge and
write zeros everywhere except for FY = 100MPa.mm. Then click
on the button <<Save the values>> (you will see the input
values in the table below the window). For layers 2 and 3 at the left
edge, repeat the same operation without forgetting to specify the layer
number and to write zeros for all of the forces and moments.
For the right edge,
the same instructions are followed except that the edge to be selected is
the <<Right>> edge and you write zeros for all of the forces
and moments in every layer except for the force FY = 100MPa.mm
applied on layer 3.
Finally, click on the
button <<OK>> in order to validate the data and you will go
to the window called <<Configuration of mechanical and hygrothermal
load>>. You have to click on the button <<Read the configurations>>

Figure 16.
First stage in the loads configuration.

Figure 17.
Second stage in the loads configuration
- Meshing definition.
In the main window, click on the button <<Meshing of the width 0, b
>>. In the window that appears, in the list of meshing types, select
the option <<Automatic>>. In the space of the width value b,
type 30.
- Executing the calculations.
Click on the button <<Analyze>> of the DEILAM main window.
- Visualization of results.
After the last stage, a new window appears. In this window, click on the button
<<Fields to be displayed>>, and in the new window that appears,
select in the list <<Fields to be displayed>> the option <<Interlaminar
stresses>>. Check the box corresponding to the field
(normal
stresses) and put in the corresponding space 1-2 (in order to draw the stresses
in interfaces 1 and 2: interfaces steel/adhesive and adhesive/steel, respectively).
Then click on the button <<Draw>>. You will see a graphic similar
to the one in Figure 18: it is the normal stresses curve
at interfaces 1 and 2 vs. the position (y) on the interface. In order to distinguish
the two curves, you only have to click on the button <<Chart properties>>
and select the colors and types of lines you want for distinguishing the two
curves.

Figure 18.
First stage in the loads configuration.
- Visualization of other
fields. In order to visualize other fields such as membranar forces or rotations,
you have to retake stage 6.
Determining
the residual thermal stresses and displacements
Let us consider
a symmetrical multi-layered material (q1,...,qn)S
made up of N
= 2n layers of orthotropic materials. The multi-layered material is only
subjected to a temperature variation DT.
For this problem, there are no external forces applied to the laminate. So,
the axial strain e should be such
that the global force on the x direction:
is zero.
In this MAC
LAM version, it is not possible to give the value of the force F. Despite
this, it is possible to calculate the axial strain e
that would give a null force F. In order to do this, you just have to
follow these stages:
- Calculation of the global
stiffness R in the x axe (this stiffness takes into account
the edge effect). This rigidity is calculated by performing first a calculation
of the type <<free edge problem>> without considering
the temperature and with a non-zero arbitrary axial strain e1.
Then you save the results of the in-plane forces (membranar forces) Nixx
for all of the layers and integrate the sum of all of the fields Nixx
along the width [0,b]; the result of the integration is a non-zero
force F1. Finally, is calculated.
R
= F1 / e1
- Intermediary calculation
with a non-zero temperature variation DT
and a zero axial strain e2
= 0.
Do not forget to enter the thermal expansion coefficients. After having finished
the calculations, the results of the in-plane forces Nixx
are saved for all of the layers and the sum of all these fields Nixx
is integrated along the width [0,b]; the result of the integration
is a force F2.
- Calculation of axial
strain e which gives, for a temperature
variation DT,
a force F = 0. This strain is given by the formula:
e
= -F2 /
R
After having
determined the strain , the same stages are followed as in the case of the free
edge problem, but this time with:
- An axial load e
equal to the one calculated by means of the above-said formula and
- a temperature variation
DT
(do not forget to enter the thermal expansion coefficients).
The results obtained by
means of this last calculation are the residual fields due to a single temperature
variation.
Important
remarks

The
shear stresses at the interfaces in DEILAM do not verify the 3D boundary
condition:
tyz
= 0
In
order to verify this condition, we should enrich the M4-5N
model. Nevertheless, even if the 3D boundary condition is not verified,
the M4-5N makes a good description of the interlaminar shear
stress tyz
. The 3D finite elements near the edges and interfaces (between layers
of different materials) give results that depend on the meshing (there
are singularities). DEILAM gives finite values at the interfaces and
the results converge quickly. For certain materials, these finite
values proved to be capable of predicting delamination onset 7 .
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References
[1] A.
Diaz Diaz, J.F. Caron, R.P. Carreira, Software application for evaluating
interfacial stresses in inelastic symmetrical laminates with free edges,
Journal of Composite Structures, 58, 195-208, 2002
[2] CARREIRA
RP, CARON JF, DIAZ DIAZ A. Model of multi-layered materials for interface
stresses estimation and validation by finite element calculations, Mechanics
of Materials, 34, 217-230, 2002.
[3] CARON
JF, CARREIRA RP, DIAZ DIAZ A. Critère d'initiation de délaminage
dans les stratifiés. Comptes Rendus de l'Académie des Sciences,
327, 1291-1296, 1999
[4] CARON
JF, DIAZ DIAZ A, CARREIRA RP, CHABOT A, EHRLACHER A. Multi-particle modelling
for the prediction of delamination in multi-layered materials. Artículo
aceptado para publicación en la revista Composite Science and Technology,
2005.
[5] DIAZ
DIAZ A, CARON JF. Prediction of the onset of mode III delamination in
carbon-epoxy laminates. Artículo aceptado para publicación
en la revista Composite Structures, 2005.