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Where, f is the change in force, A is the cross-section of
the tensile specimen, x is the change in thickness of the
EVA film, and L is the original length of the film. The
Young’s Modulus can be finally expressed as:
The mechanical compliance of the tensile specimens was
measured:
where C is the compliance, x is the change in position,
and f is the change in force
It is important to note, that during the experiment, not only
did the EVA film was strained, but the rest of the specimen
(the glass, epoxy, tabs) and the testing apparatus strained
as well. To account for this artifact, a tensile specimen,
consisting of a very stiff epoxy instead of the EVA film
(otherwise identical to the previous specimens), was
prepared to measure its mechanical compliance, defined
as Cmachine
The compliance of the EVA film, CEVA, can be calculated
with
CEVA = C – Cmachine
Introduction Materials & Methods
Results
Conclusion
Acknowledgements
The Effect of Aging on the Stiffness of
Ethylene Vinyl Acetate
Vi Le, Fernando Novoa, Professor Reinhold Dauskardt
Materials Science and Engineering, Stanford University
Encapsulation specimens were prepared by bonding a
500-micron film of EVA (Ethylene Vinyl Acetate)
between two 0.006m glass substrates. One set of
specimens was left to age for one year at room
temperature while the other set was tested
immediately after lamination. Small square
specimens, 3.4 mm by 3.4 mm by 12.5 mm, were then
cut from the center with a high-precision glass saw as
shown in Figure 1.
Materials & Methods
Figure 5: Load(N) vs. time
(sec) of a mechanical test of a
new tensile specimen at 50˚C
over 10 cycles
The change in load remains at
approximately 0.825 N.
C =
x
f
Figure 4: Position (microns) vs.
time (sec) of a mechanical test
of a new tensile specimen at
50˚C over 10 cycles
The change in position was set
to 4.98 microns throughout.
EEVA =
σ
ε
σ =
f
A
ε =
x
L
EEVA =
f
A
x
L
EEVA =
f∙L
x∙A
EEVA =
L
CEVA∙A
Results
Figure 6: Stress (MPa) vs.
strain of new tensile
specimen at 50˚C and
40% RH. The slope of the
graph represents the
Young’s modulus.
Figure 1
Figure 4
Figure 5
Figure 6
Preservation of the mechanical integrity of the
encapsulation materials used in photovoltaic (PV)
modules, such as Ethylene Vinyl Acetate (EVA), is
essential to maintaining the long-term reliability of PV
applications. The effects of short-term aging under
aggressive laboratory environments (high
temperature, high humidity) on the properties of EVA
have been previously documented [1-3]. However, the
influence of long-term aging on the mechanical
properties of EVA have barely been explored.
In this study, we determine the change in the Young’s
Modulus of an EVA film after 1-year aging in a
laboratory environment (25C, 40%RH). We also
report the mechanical stress developed in the EVA
film during cyclical strain. The encapsulation
specimens were prepared by laminating a film of EVA
between two glass substrates. The mechanical
compliance of the testing apparatus was taken into
consideration for the strain measurements.
I would like to thank Kaye Storm and Judy Mckeon for
hosting the RISE Internship program. I would also like
to thank my mentor, Fernando Novoa, for guiding me
and introducing to me the reality of scientific research.
Lastly, I’d like to thank Professor Reinhold Dauskardt
for giving me the opportunity to work in his lab.
Figure 7: Young’s
Modulus (MPa) vs.
temperature of aged
and new tensile
specimens. At lower
temperatures, both
specimens have a high
Young’s Modulus
which then decreases
exponentially with temperature. Both the Young’s
Modulus of the aged and new specimens have the
same slope from 20˚C to approximately 50˚C. The
plateau, the region where the graph is constant, begins
at approximately 50˚C. Overall, aging of 1-year at 20C
and 40% RH increased the stiffness of the EVA ~10
fold at every temperature.
1 Shi, Xu‐Ming, et al. "Effect of damp‐heat aging on the
structures and properties of ethylene‐vinyl acetate
copolymers with different vinyl acetate contents."Journal
of Applied Polymer Science 112.4 (2009): 2358-2365.
2 Czanderna, A. W., and F. J. Pern. "Encapsulation of
PV modules using ethylene vinyl acetate copolymer as
a pottant: A critical review." Solar Energy Materials and
Solar Cells 43.2 (1996): 101-181.
3 Allen, Norman S., et al. "Aspects of the thermal
oxidation of ethylene vinyl acetate copolymer." Polymer
Degradation and Stability 68.3 (2000): 363-371.
Figure 7
Aged tensile
specimens
New tensile
specimens
-Tensile encapsulation specimens, prepared by
laminating an EVA film between two glass substrates,
were mechanically tested
-The mechanical stress developed in the EVA film was
measured with the mechanical compliance of the
testing apparatus considered.
-The Young’s Modulus of the EVA was measured in
aged (1-year) and new specimens. The modulus was
higher in the new tensile specimens (~10 fold) for all
the temperatures in range.
-The transition temperatures for aged and new EVA
specimens were the same, showing that aging
increases EVA stiffness but does not affect its the
temperature dependence.
Loading tabs were attached with a high-shear epoxy
to both sides of each specimen (Figure 2). The
loading tab was fixed to a mechanical testing system
consisting of a displacement-controlled actuator and a
mechanical load cell.
Figure 2
In order to compare the aged and new specimens, the
Young’s Modulus, which describes the stiffness of
materials, was measured:
Where E is the Young’s Modulus, and respectively, σ and ε
is tensile stress and tensile strain, also defined by:
The experiments were conducted in an
environmental chamber of controlled temperature and
relative humidity (RH). The testing system and the
specimen were stabilized for 30 minutes to reach
thermal
equilibrium before the mechanical test.
The developed mechanical load
(Figure 3) was measured as the
actuator position oscillated between
0.02 and 5.00 microns at 0.05
microns/sec in a triangle wave.
The experiment was conducted at
five selected temperatures of 30˚C,
40˚C, 50˚C, 60˚C, and 80˚C. The relative
Humidity was kept constant at 40%.
Figure 3
Load
Load
References

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RISE 2013 Poster - Vi - Fernando

  • 1. Where, f is the change in force, A is the cross-section of the tensile specimen, x is the change in thickness of the EVA film, and L is the original length of the film. The Young’s Modulus can be finally expressed as: The mechanical compliance of the tensile specimens was measured: where C is the compliance, x is the change in position, and f is the change in force It is important to note, that during the experiment, not only did the EVA film was strained, but the rest of the specimen (the glass, epoxy, tabs) and the testing apparatus strained as well. To account for this artifact, a tensile specimen, consisting of a very stiff epoxy instead of the EVA film (otherwise identical to the previous specimens), was prepared to measure its mechanical compliance, defined as Cmachine The compliance of the EVA film, CEVA, can be calculated with CEVA = C – Cmachine Introduction Materials & Methods Results Conclusion Acknowledgements The Effect of Aging on the Stiffness of Ethylene Vinyl Acetate Vi Le, Fernando Novoa, Professor Reinhold Dauskardt Materials Science and Engineering, Stanford University Encapsulation specimens were prepared by bonding a 500-micron film of EVA (Ethylene Vinyl Acetate) between two 0.006m glass substrates. One set of specimens was left to age for one year at room temperature while the other set was tested immediately after lamination. Small square specimens, 3.4 mm by 3.4 mm by 12.5 mm, were then cut from the center with a high-precision glass saw as shown in Figure 1. Materials & Methods Figure 5: Load(N) vs. time (sec) of a mechanical test of a new tensile specimen at 50˚C over 10 cycles The change in load remains at approximately 0.825 N. C = x f Figure 4: Position (microns) vs. time (sec) of a mechanical test of a new tensile specimen at 50˚C over 10 cycles The change in position was set to 4.98 microns throughout. EEVA = σ ε σ = f A ε = x L EEVA = f A x L EEVA = f∙L x∙A EEVA = L CEVA∙A Results Figure 6: Stress (MPa) vs. strain of new tensile specimen at 50˚C and 40% RH. The slope of the graph represents the Young’s modulus. Figure 1 Figure 4 Figure 5 Figure 6 Preservation of the mechanical integrity of the encapsulation materials used in photovoltaic (PV) modules, such as Ethylene Vinyl Acetate (EVA), is essential to maintaining the long-term reliability of PV applications. The effects of short-term aging under aggressive laboratory environments (high temperature, high humidity) on the properties of EVA have been previously documented [1-3]. However, the influence of long-term aging on the mechanical properties of EVA have barely been explored. In this study, we determine the change in the Young’s Modulus of an EVA film after 1-year aging in a laboratory environment (25C, 40%RH). We also report the mechanical stress developed in the EVA film during cyclical strain. The encapsulation specimens were prepared by laminating a film of EVA between two glass substrates. The mechanical compliance of the testing apparatus was taken into consideration for the strain measurements. I would like to thank Kaye Storm and Judy Mckeon for hosting the RISE Internship program. I would also like to thank my mentor, Fernando Novoa, for guiding me and introducing to me the reality of scientific research. Lastly, I’d like to thank Professor Reinhold Dauskardt for giving me the opportunity to work in his lab. Figure 7: Young’s Modulus (MPa) vs. temperature of aged and new tensile specimens. At lower temperatures, both specimens have a high Young’s Modulus which then decreases exponentially with temperature. Both the Young’s Modulus of the aged and new specimens have the same slope from 20˚C to approximately 50˚C. The plateau, the region where the graph is constant, begins at approximately 50˚C. Overall, aging of 1-year at 20C and 40% RH increased the stiffness of the EVA ~10 fold at every temperature. 1 Shi, Xu‐Ming, et al. "Effect of damp‐heat aging on the structures and properties of ethylene‐vinyl acetate copolymers with different vinyl acetate contents."Journal of Applied Polymer Science 112.4 (2009): 2358-2365. 2 Czanderna, A. W., and F. J. Pern. "Encapsulation of PV modules using ethylene vinyl acetate copolymer as a pottant: A critical review." Solar Energy Materials and Solar Cells 43.2 (1996): 101-181. 3 Allen, Norman S., et al. "Aspects of the thermal oxidation of ethylene vinyl acetate copolymer." Polymer Degradation and Stability 68.3 (2000): 363-371. Figure 7 Aged tensile specimens New tensile specimens -Tensile encapsulation specimens, prepared by laminating an EVA film between two glass substrates, were mechanically tested -The mechanical stress developed in the EVA film was measured with the mechanical compliance of the testing apparatus considered. -The Young’s Modulus of the EVA was measured in aged (1-year) and new specimens. The modulus was higher in the new tensile specimens (~10 fold) for all the temperatures in range. -The transition temperatures for aged and new EVA specimens were the same, showing that aging increases EVA stiffness but does not affect its the temperature dependence. Loading tabs were attached with a high-shear epoxy to both sides of each specimen (Figure 2). The loading tab was fixed to a mechanical testing system consisting of a displacement-controlled actuator and a mechanical load cell. Figure 2 In order to compare the aged and new specimens, the Young’s Modulus, which describes the stiffness of materials, was measured: Where E is the Young’s Modulus, and respectively, σ and ε is tensile stress and tensile strain, also defined by: The experiments were conducted in an environmental chamber of controlled temperature and relative humidity (RH). The testing system and the specimen were stabilized for 30 minutes to reach thermal equilibrium before the mechanical test. The developed mechanical load (Figure 3) was measured as the actuator position oscillated between 0.02 and 5.00 microns at 0.05 microns/sec in a triangle wave. The experiment was conducted at five selected temperatures of 30˚C, 40˚C, 50˚C, 60˚C, and 80˚C. The relative Humidity was kept constant at 40%. Figure 3 Load Load References