Mechanical Adhesion in Adhesively Bonded Metal-Joints with Retentive Laser-Structured Adherends

Mechanical Adhesion in Adhesively Bonded Metal-Joints with Retentive
Laser-Structured Adherends
Paul Ludwig Geiss and Sascha Gramsch-Kempkes
University of Kaiserslautern, Faculty Mechanical and Process Engineering,
Workgroup Materials and Surface Technologies (AWOK)
Kaiserslautern, 67663, Germany
[email protected]
Introduction
The Ciba Laser Pretreatment process (CLP) [1] is one
of the earlier examples for using environmentally friendly
laser technologies to clean and modify adherend’s surfaces
prior to adhesive bonding. Laser-structured base retention
brackets have been used successfully in orthodontic applications for several years to enhance the durability of the
brackets adhesion under the detrimental service conditions
of the oral cavity. In this specific area of application the
goal of the laser structuring process is to create beads of
molten and resolidified metal, protruding from the adherend’s surface and thus facilitating a strong mechanical
interlocking between the dental adhesive and the brackets
base plate. The objective of this research study is to investigate the structure property relationship between the shape
and geometrical alignment of individual laser retentions
and their ability to increase the peel strength and durability
of structural adhesive joints.
The T-peel specimen were made of X5CrNi18-10 stainless
steel with a thickness of 1 mm.
Laser structuring was done in pulsed mode operation with
a pulse frequency of 17.500 Hz and an average pulse duration of 5 µs. Non isotropic surface patterns (Fig. 2) were
placed at different angles on the specimen’s surfaces to be
able to differentiate between the influence of the dimensions of the retentive structures perpendicular to the surface and their orientation in relation to the direction of
peeling (Fig. 3).
100 mm
Experimental
100 mm
Figure 2. Example of a non-isotropic surface pattern.
Laser structuring was done with a Trumpf TruMark™
3020 Nd:YAG laser. Fig. 1 illustrates the dimensions of
the T-peel specimen that were used in this study. The size
was chosen to take account for the maximum working area
of the laser unit.
s
r
L2
La
LK
L1
L2
L
b
L = 106 mm
L1 = 10 mm
L2 = 12,75 mm
La = 59,5 mm
LK = 85 mm
b = 15 mm
Figure 1. Size of the T-peel specimen.
d = 3 mm
r = 3 mm
s = 1 mm
Figure 3. Orientation of anisotropic laser patterns on the
surface of the T-peel specimen.
The variation of laser patterns was mainly governed by the
number of pulses per cavity and the pitch clearance B (125
µm and 175 µm) (Fig. 4). Additional parameter variations
included the choice of shielding gases (At=air, Ar=Arcal™,
La=Lasal™ and Va=Varigon™) (Fig. 5) and the application
of an electrochemical anodic treatment (EP) prior to adhesive bonding of the specimen.
Pm,5%
-fractile [N/mm]
pm,5%-Fraktil
[N/mm]
150 mm
B=125 µm
8
B=175 µm
7
6
5
4
3
2
1
0
Figure 4: Examples and denotation of laser patterns with
different pitch clearances B.
2R
milled
surface
Edelkorund
grit
blasted
Figure 6. Influence of the type of shielding gas on the peel
resistance of T-peel specimen.
50 mm
50 mm
Arcal (Ar)
Figure 5. Influence of the type of shielding gas (At=air,
Ar=Arcal™) on the shape of the laser patterns.
All T-peel specimen were bonded with a two component
epoxy based adhesive and cured at 80 °C in a convection
chamber. Testing was done at a separation speed of 50
mm/min.
Results and Discussion
In Figure 6 the peel resistance of T-peel specimen bonded
in the initial condition without further surface preparation
(milled surface, 2R) and after grit blasting with corundum
is given as a reference. The peel resistance is expressed as
the 5% p-fractile probabilistic distribution of the average
peel resistance.
8
7
Pm,5%
-fractile [N/mm]
pm,5%-Fraktil
[N/mm]
Air (At)
Figure 7 illustrates the influence of the type of shielding
gas on the 5% p-fractile probabilistic distribution of the
average peel resistance values.
Although the employment of shielding gas increases the
expansion of the individual retentions perpendicular to the
surface, the peel resistance of the T-peel specimen prepared at ambient atmospheric conditions is superior.
6
5
4
3
2
1
0
BAt125
BAr125
BLa125
BVa125
Figure 7. Influence of the type of shielding gas on the peel
resistance of T-peel specimen.
Accelerated corrosive aging according to DIN EN ISO
9227 leads to a significant reduction of the peel resistance
in Fig. 8. Again the specimen that had been laser-treated
under atmospheric condition with a pitch clearance of 125
µm exhibit a superior performance indicated by a residual
strength after aging of almost 75 % of the initial peel resistance. The specimen with the denotation BAt125EP and
BAt175EP had been subjected to an electrochemical anodic polishing procedure after laser treatment.
initial
Ppm,5%
-fractile [N/mm]
[N/mm]
m,5%-Fraktil
9
4 weeks
strength
ungealtert
4 saltspray
Wochen SST
8 weeks
16 weeks
8 saltspray
Wochen SST
16saltspray
Wochen SST
8
7
6
5
4
3
2
1
BAt175 EP
BAt125 EP
BAr175
BAr125
BAt175
BAt125
2R EP
0
Figure 8. Influence of aging under salt spray conditions on
the peel resistance of T-peel specimen.
The electro-polishing treatment of specimens BAt125EP
and BAt175EP after laser structuring serves to unify the
chemical properties of the adherent surface in reference to
the initial condition without significantly changing the size
and shape of the laser pattern.
Conclusions
Environmentally friendly single step surface pretreatment methods prior to adhesive bonding are of increasing
importance for a variety of industrial applications. In this
study the generation of retentions by laser surfacestructuring has led to adhesive joints with a high level of
peel resistance and excellent durability under corrosive
aging conditions. The main reason for their good performance is assigned to the mechanical interlocking of structures consisting of molten and resolidified metal, protruding from the adherend’s surface. Electrochemical posttreatment causes a slight reduction of the initial strength
and durability of the laser-structured peel specimen. This
indicates that the sub-micron-scale morphology of the surfaces and their chemical properties caused by the laser
treatment carries an accessory effect on the performance of
adhesive joints which will be a subject of subsequent research studies.
References
1.
2.
2. R. Broad, J. French, J., Int. J. of Adhesion and
Adhesives, 1999, 2-3, pp 193-198.
DIN EN ISO 9227, corrosion tests in artificial atmospheres - salt spray tests (ISO 9227:2012)