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Characterization of the Adhesion Integrity in Photovoltaic
Panels using Various Thermomechanical Blister Tests
Scott Julien1, David Miller2, Xiaohong Gu3, and Kai-tak Wan1
1 Mechanical Engineering, Northeastern University, Boston, MA
2 National Renewable Energy Laboratory, Golden, CO
3 National Institute of Standards and Technology, Gaithersburg, MD
We are grateful to Len Magara, an undergraduate engineering student at Northeastern, and Hongdang
Zhang, a visiting scholar at Northeastern, for their invaluable help in performing the experimental work. We
are also grateful to the Department of Energy PREDICTS 2 program for providing grant funding.
1. M Quintana, et al, “Commonly Observed Degradation in Field-aged Photovoltaic Modules”, Photovoltaic
Spec Conf, Conf Record 29th IEEE, 2002 May: 1436–1439.
2. S Guo, KT Wan, and D Dillard, “A bending-to-stretching analysis of the blister test in the presence of tensile
residual stress,” Int J Solids Struct, 2005 May, 42 (9-10): 2771–2784.
3. KT Wan, “A novel blister test to investigate thin film delamination at elevated temperature,” Int J Adhes
Adhes 2001 Apr, 20 (2): 141-143.
4. S Julien, KT Wan, “An investigation of delamination in the shaft-loaded blister test.” Future publication.
Glass
EVA
Backsheet
Figure 3. Example of a blister test sample (here, a backsheet-thick glass sample).
(a) Glass-face view (b) Backsheet-face view
(d) Layering
Figure 2. Variations of the blister test used in our study.
(a) Thermal blister test (TBT). At room temperature,
the rear of the hole is covered with a plate, trapping
air in the blister cavity. Heat is then applied, causing
the air to expand, and driving delamination. Side
and top cameras are used to measure the blister
radius, a, and blister height, w. These two
parameters, along with the pressure of the
entrapped air, p, are used to calculate the adhesion
energy, G, of the film-substrate interface.
(b) Shaft-loaded blister test (SLBT). A shaft
(either flat- or spherically-ended), is driven into
the freestanding film, causing delamination. The
applied force, F, punch radius, R, blister radius,
a, and blister height, w, are used to calculated
the interfacial adhesion energy, G.
Our group’s focus is in characterizing the adhesion between the layers in photovoltaic
(PV) solar panels, using the thermomechanical blister test. Characterization of the adhesion
in PV panels is important because adhesive failure is a common mode of failure (see Fig. 1,
below). Delamination of the layers can lead to reduced optical transparency, heat
dissipation, and protection from outside elements [1]. We are interested in developing the
blister test as an accelerated testing method for predicting the long-term adhesive reliability
of PV modules.
There are several variations of the blister test, including the pressurized blister test,
the shaft-loaded blister test [2], and the thermal blister test [3]. Our focus is currently on the
thermal blister test and the shaft-loaded blister test (see Fig. 2, below).
(a) 40 oC
(b) 50 oC
(c) 60 oC
(d) 70 oC
(e) 80 oC
Figure 5. Results of a thermal blister test on
an EVA-glass sample. The water was heated
in intervals of 10 oC, starting at 40 oC.
Between each increase, the sample was
allowed to thermally equilibrate for 45
minutes. The photographs show the blister
“ballooning”—i.e. deforming mechanically,
significantly—while the blister grew slightly.
This seems to indicate that the EVA-glass
adhesion was strong, compared to the
stiffness of the EVA.
Figure 4. Sampling of sideview and bottom-
view photographs from a spherical-ended
shaft-loaded blister test on a backsheet-thick
glass sample. The figures show, qualitatively,
the evolution of the deformation/delamination
process, from initial indentation to final rupture
0
20
40
60
80
100
120
140
160
180
200
10 11 12 13 14 15 16
AppliedForce,F(N)
Blister Radius, a (mm)
Applied Force vs. Blister Radius
Bottom View
Side View
0
1
2
3
4
5
6
10 11 12 13 14 15 16
PunchDisplacement,w(mm)
Blister Radius, a (mm)
Punch Displacement vs. Blister Radius
Bottom View
Side View
Figure 6 (left and below). Example of
quantitative data from a flat-ended shaft-
loaded blister test. Note that, as we are
still developing the testing method, the
results are only preliminary and
approximate. Only nine datapoints are
shown in Figures (b) and (c)—explaining
the non-linearity of the curves (the “bends”
do not correlate with noteworthy events
during the test).
(a) Punch applied force, F, vs.
displacement, w. The blue arrow shows
the approximate onset of delamination,
prior to which the film simply stretched and
deformed. The green arrow shows a
sudden “jump” in delamination. The red
arrow shows rupture, where the punch
broke through the film.
(b) A plot of the punch displacement, w, vs.
blister radius, a, shows that both increase,
as the punch-driven delamination
progresses.
(c) Punch applied force, F, vs. blister
radius, a, showing the concomitant
increase in both as delamination is driven.
0
20
40
60
80
100
120
140
160
180
200
0 1 2 3 4 5 6
AppliedForce,F(N)
Punch Displacement, w (mm)
Applied Force vs. Punch Displacement
Figure 9. Custom apparatus for blister-testing real, field-weathered PV panel sections, currently being built.
The device features an articulating arm that will position a probe for performing shaft-loaded blister tests,
anywhere on the panel. Slated completion: QI, 2016.
Equation 1. A new analytical model for the flat-ended shaft-loaded blister test, currently being developed. It will
allow extraction of the interfacial adhesion energy, G, from our experimental results. The model will relate G to: (i)
the properties of the film—the thickness, h, elastic modulus, E, Poisson’s ratio, ν, and initial pre-stress, N0 — (ii)
the size of the punch—the radius, R — and (iii) the experimentally measured variables—the applied force, F,
blister height, w0, and blister radius, a. Slated completion: QI, 2016.
(c) Side view
𝐺𝐺 = Φ(ℎ, 𝐸𝐸, 𝜈𝜈, 𝑁𝑁0, 𝑅𝑅, 𝑤𝑤0) �
𝐹𝐹 � 𝑤𝑤0
𝜋𝜋𝑎𝑎2
Figure 1. Examples
of adhesive
delamination in PV
panels.
Introduction
Method
Results Ongoing Work
References
Acknowledgements
Figure 7 (above). Custom thermal-shock testing
apparatus, currently being built. The device will
interchange a set of thermal blister test samples
between temperature-controlled hot- and cold-water
baths, to simulate the thermal cycles experienced by
PV materials in the field. Slated completion: Q1, 2016.
Figure 8 (below). Custom acoustic emissions blister
test apparatus, currently being built. The apparatus
will record high-frequency acoustic emissions,
generated from sudden delamination events during a
shaft-loaded blister test, to give further insight into
the physics of the delamination process. Slated
completion: QIV, 2015.
Onset of
Delamination
Sudden Jump in
Delamination
Rupture
h
2a
r
W0
Delamination
Edge
F
Load Cell
Cold Spray
FilmSubstrate

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Characterization-of-the-Adhesion-Integrity-in-Photovoltaic-Panels-using-Various-Thermomechanical-Blister-Tests-Northeastern-U

  • 1. Characterization of the Adhesion Integrity in Photovoltaic Panels using Various Thermomechanical Blister Tests Scott Julien1, David Miller2, Xiaohong Gu3, and Kai-tak Wan1 1 Mechanical Engineering, Northeastern University, Boston, MA 2 National Renewable Energy Laboratory, Golden, CO 3 National Institute of Standards and Technology, Gaithersburg, MD We are grateful to Len Magara, an undergraduate engineering student at Northeastern, and Hongdang Zhang, a visiting scholar at Northeastern, for their invaluable help in performing the experimental work. We are also grateful to the Department of Energy PREDICTS 2 program for providing grant funding. 1. M Quintana, et al, “Commonly Observed Degradation in Field-aged Photovoltaic Modules”, Photovoltaic Spec Conf, Conf Record 29th IEEE, 2002 May: 1436–1439. 2. S Guo, KT Wan, and D Dillard, “A bending-to-stretching analysis of the blister test in the presence of tensile residual stress,” Int J Solids Struct, 2005 May, 42 (9-10): 2771–2784. 3. KT Wan, “A novel blister test to investigate thin film delamination at elevated temperature,” Int J Adhes Adhes 2001 Apr, 20 (2): 141-143. 4. S Julien, KT Wan, “An investigation of delamination in the shaft-loaded blister test.” Future publication. Glass EVA Backsheet Figure 3. Example of a blister test sample (here, a backsheet-thick glass sample). (a) Glass-face view (b) Backsheet-face view (d) Layering Figure 2. Variations of the blister test used in our study. (a) Thermal blister test (TBT). At room temperature, the rear of the hole is covered with a plate, trapping air in the blister cavity. Heat is then applied, causing the air to expand, and driving delamination. Side and top cameras are used to measure the blister radius, a, and blister height, w. These two parameters, along with the pressure of the entrapped air, p, are used to calculate the adhesion energy, G, of the film-substrate interface. (b) Shaft-loaded blister test (SLBT). A shaft (either flat- or spherically-ended), is driven into the freestanding film, causing delamination. The applied force, F, punch radius, R, blister radius, a, and blister height, w, are used to calculated the interfacial adhesion energy, G. Our group’s focus is in characterizing the adhesion between the layers in photovoltaic (PV) solar panels, using the thermomechanical blister test. Characterization of the adhesion in PV panels is important because adhesive failure is a common mode of failure (see Fig. 1, below). Delamination of the layers can lead to reduced optical transparency, heat dissipation, and protection from outside elements [1]. We are interested in developing the blister test as an accelerated testing method for predicting the long-term adhesive reliability of PV modules. There are several variations of the blister test, including the pressurized blister test, the shaft-loaded blister test [2], and the thermal blister test [3]. Our focus is currently on the thermal blister test and the shaft-loaded blister test (see Fig. 2, below). (a) 40 oC (b) 50 oC (c) 60 oC (d) 70 oC (e) 80 oC Figure 5. Results of a thermal blister test on an EVA-glass sample. The water was heated in intervals of 10 oC, starting at 40 oC. Between each increase, the sample was allowed to thermally equilibrate for 45 minutes. The photographs show the blister “ballooning”—i.e. deforming mechanically, significantly—while the blister grew slightly. This seems to indicate that the EVA-glass adhesion was strong, compared to the stiffness of the EVA. Figure 4. Sampling of sideview and bottom- view photographs from a spherical-ended shaft-loaded blister test on a backsheet-thick glass sample. The figures show, qualitatively, the evolution of the deformation/delamination process, from initial indentation to final rupture 0 20 40 60 80 100 120 140 160 180 200 10 11 12 13 14 15 16 AppliedForce,F(N) Blister Radius, a (mm) Applied Force vs. Blister Radius Bottom View Side View 0 1 2 3 4 5 6 10 11 12 13 14 15 16 PunchDisplacement,w(mm) Blister Radius, a (mm) Punch Displacement vs. Blister Radius Bottom View Side View Figure 6 (left and below). Example of quantitative data from a flat-ended shaft- loaded blister test. Note that, as we are still developing the testing method, the results are only preliminary and approximate. Only nine datapoints are shown in Figures (b) and (c)—explaining the non-linearity of the curves (the “bends” do not correlate with noteworthy events during the test). (a) Punch applied force, F, vs. displacement, w. The blue arrow shows the approximate onset of delamination, prior to which the film simply stretched and deformed. The green arrow shows a sudden “jump” in delamination. The red arrow shows rupture, where the punch broke through the film. (b) A plot of the punch displacement, w, vs. blister radius, a, shows that both increase, as the punch-driven delamination progresses. (c) Punch applied force, F, vs. blister radius, a, showing the concomitant increase in both as delamination is driven. 0 20 40 60 80 100 120 140 160 180 200 0 1 2 3 4 5 6 AppliedForce,F(N) Punch Displacement, w (mm) Applied Force vs. Punch Displacement Figure 9. Custom apparatus for blister-testing real, field-weathered PV panel sections, currently being built. The device features an articulating arm that will position a probe for performing shaft-loaded blister tests, anywhere on the panel. Slated completion: QI, 2016. Equation 1. A new analytical model for the flat-ended shaft-loaded blister test, currently being developed. It will allow extraction of the interfacial adhesion energy, G, from our experimental results. The model will relate G to: (i) the properties of the film—the thickness, h, elastic modulus, E, Poisson’s ratio, ν, and initial pre-stress, N0 — (ii) the size of the punch—the radius, R — and (iii) the experimentally measured variables—the applied force, F, blister height, w0, and blister radius, a. Slated completion: QI, 2016. (c) Side view 𝐺𝐺 = Φ(ℎ, 𝐸𝐸, 𝜈𝜈, 𝑁𝑁0, 𝑅𝑅, 𝑤𝑤0) � 𝐹𝐹 � 𝑤𝑤0 𝜋𝜋𝑎𝑎2 Figure 1. Examples of adhesive delamination in PV panels. Introduction Method Results Ongoing Work References Acknowledgements Figure 7 (above). Custom thermal-shock testing apparatus, currently being built. The device will interchange a set of thermal blister test samples between temperature-controlled hot- and cold-water baths, to simulate the thermal cycles experienced by PV materials in the field. Slated completion: Q1, 2016. Figure 8 (below). Custom acoustic emissions blister test apparatus, currently being built. The apparatus will record high-frequency acoustic emissions, generated from sudden delamination events during a shaft-loaded blister test, to give further insight into the physics of the delamination process. Slated completion: QIV, 2015. Onset of Delamination Sudden Jump in Delamination Rupture h 2a r W0 Delamination Edge F Load Cell Cold Spray FilmSubstrate