3.2. Results of Surface Roughness Evaluation
The measured values of selected roughness parameters of the surfaces of the base materials in the delivered state and after surface treatments are shown in
Table 5.
Abbot–Firestone material ratio curves for initial and treated materials are shown in
Figure 7 and
Figure 8.
The roughness of the evaluated materials was assessed by parameters that would describe the differences in the surfaces.
Table 4 shows that the value of the parameter Ra does not change significantly for materials and their surface treatments. It varies for DC material from 0.93 to 0.96 µm and for HX material from 0.69 to 1.02 µm. A similar finding applies to the Rz parameter, as its value ranges from 4.54 to 5.61 µm for DC material and from 3.98 to 4.96 µm for HX material. The differences between the individual surfaces were more pronounced in the RSm and RPc parameters. The number of peaks per centimetre of surface length increased for DC material compared to the original, most obviously on the surface modified by passivation and slightly also on the surface with organosilane.
For HX material, both surface treatments led to an increase in the number of peaks, mostly after the application of the organosilane layer. This fact, specifically the increased number of peaks per centimetre of length, induces an increase in the surface area of the treated surfaces, and thus also an increase in the contact area between the adhesive and the surface-treated material. This could lead to an increase in bond strength.
Differences in surface morphology can be seen in HX materials from profilograms, in
Figure 8. This material showed an increase in the number of peaks for both surface treatments compared to the untreated state. However, it is necessary to take into account the fact that the number of peaks in the HX material was double even in its original state compared to DC material, and after modifications the number of peaks is still significantly higher in this HX material compared to DC material with the same modifications (
Table 4). The Abbot–Firestone curve is different for both materials in their original state, even though the surfaces have almost the same value for the Ra and Rz parameters. From the mentioned measurements, it can be concluded that from the point of view of microgeometry and the shape of the Abbot–Firestone curve, the HX material and its modified variants are more likely to create a bonded joint with a high load-bearing capacity.
3.3. Load-Bearing Capacity of Joints Formed by Adhesive Bonding
Figure 9 and
Figure 10 show the load–displacement curves for adhesive bonding joints formed using equal (DC-DC, HX-HX) and dissimilar (DC-HX) materials, as-joined and also after climate test.
RB adhesive joints are characterized by failure occurring after a relatively short displacement (up to 1.5 mm). Joints with EP adhesive fail after deformation of the substrate, after a displacement of 2–13 mm, depending on the joint material combination and surface finish.
The load-carrying capacity of HX-HX joints is almost always the highest, confirming previous considerations about the more appropriate microgeometry of HX surfaces for bonding. The load capacity of DC-DC joints is always the lowest among all material combinations evaluated, again reflecting the influence of the microgeometry of this material. The load capacity of DC-HX mixed joints lies logically between that of HX-HX and DC-DC joints, with its Fmax value being closer to that of DC-DC joints. Hence the observation that the load-carrying capacity of joints of dissimilar materials will be significantly affected by the presence of less suitable surface microgeometry.
The limit state of the bonded joint is not only its failure but also the onset of plastic deformation of one of the substrates. When the bonded joint is working properly, plastic deformation of the substrates should not occur. If we evaluate even the weakest joints (DC-DC) made with RB adhesive from this point of view, their load-bearing capacity is just below 4000 N, which is very close to the force corresponding to the onset of DC yielding (3940 N), which we have determined on the basis of the yield strength of the DC steel (Re
DC = 197 MPa) and the cross-section of the DC substrate (0.8 × 25 mm). This shows that the properties of the RB adhesive are utilized as efficiently as possible in the joint; DC-DC joints with RB adhesive fail when the stress in the substrate reaches the yield stress and the substrate strengthening phase begins. The exception is DC-DC joints without surface treatment, which had significantly lower load-carrying capacity. The DC-HX joints behaved similarly, as one of the substrates in the mixed joint is DC and this substrate limits the load-carrying capacity of the joint. The HX-HX joints with RB adhesive have a load capacity very similar to both DC-DC and DC-HX, failing at approximately the same load and displacement value; thus, the load capacity is significantly lower than the yield strength of the HX substrate, which is 8280 N, for Re
HX = 414 MPa and substrate cross-section 0.8 × 25 mm. This implies that the joint load capacity of all material combinations (DC-DC, HX-HX, and DC-HX) is approximately the same because it is determined by the cohesion of the RB adhesive itself. If we consider that the shear strength of the RB adhesive itself is >15 MPa (see
Table 3) and the overlap area of the joint is 12.5 × 25 mm, the joint should fail at a load of 4680 N or more. Thus, the load-carrying capacity of real joints, which have many imperfections in the performance, actually lies between 3940 N and 4680 N, thus avoiding the onset of plastic deformation of the DC substrate and maximizing the utilization of the RB adhesive properties (in particular, internal cohesion). In the case of the RB adhesive, both surface modifications positively affected the adhesion of the adhesive to the DC substrate. The effect of the surface modification will become more apparent once the absorbed energy of the joints has been quantified.
DC-DC joints with EP adhesive had a higher load capacity compared with RB adhesive, in that all joints failure occurred only after significant plastic deformation of the substrates. Logically, in this case, there is no point in trying to increase the adhesion of the adhesive to the substrates by some surface treatment. However, for completeness, both surface treatments were also applied and tested with this adhesive (EP). The load-carrying capacity of the HX-HX joints was highest, above the yield strength of the HX material and significantly higher than that of the DC-DC and DC-HX joints. Failure of the HX-HX joints also occurred at a significantly higher displacement value, over a wide region of Luders deformation of the substrate, after the onset of the strain-hardening phase of the HX substrate. The loading behaviour of the DC-DC and DC-HX joints was controlled by the properties of the substrate with lower mechanical properties and less favourable microgeometry, i.e., the DC substrate. These joints failed again in the strain-hardening phase of the DC material, indicating a higher cohesion of the EP adhesive. An EP adhesive with a shear strength > 30MPa and with an overlapped area of 12.5 × 25 mm should fail at a load of 9375 MPa or more, which was never achieved. This means that the joints must necessarily have failed at least partially adhesively (see appearance of joint failure,
Figure 11 and
Figure 12).
Surface preparation by chromate-free zirconia passivation had a negative effect on the failure of the joint in terms of a significantly low value of displacement at failure, indicating adhesive failure or disconnection of the passivation layer from the substrate. Mixed DC-HX joints always have a slightly higher load carrying capacity than DC-DC joints, but fail on a slightly shorter displacement path. In terms of dissipated energy there is probably not much difference between them.
Corrosion exposure of the joints with EP adhesive in all cases resulted in a reduction of the displacement value at joint failure.
Table 6 summarizes the joint load-carrying capacity Fmax, displacement at joint failure sFmax, and dissipated energy at joint failure W, for both adhesives and all material combinations, during exposure in the climate chamber.
Figure 11 and
Figure 12 show the fracture surfaces of the tested joints, where the type of failure can be noticed: adhesive (between the adhesive and the substrate; one of the substrates is exposed), cohesive (failure in the adhesive layer; the adhesive remains on both substrates involved), or mixed (adhesive–cohesive).
The joint failure surfaces (
Figure 11 and
Figure 12) confirm the above considerations. The uncoated DC steel has a problem to establish a good bond of the RB adhesive to the substrate. After the DC-DC joint failure, some of the DC substrate remains naked. Both chromate-free zirconia passivation and application of organosilane functional molecules improved the adhesion of the adhesive to the substrate, which was manifested by cohesive bond failure. The HX-HX joints had good adhesion to the substrate independent of surface treatment. For the mixed DC-HX joints, adhesion of the adhesive to HX was excellent regardless of the surface treatment, and adhesion to DC was improved by application of both surface treatments, which was manifested by cohesive failure of the adhesive at the joints with the surface treatment.
The situation is different for the joints formed with EP adhesive; the joints failed at relatively high loads, reaching the plastic deformation region of the DC material when the irregular distribution of shear and peel stress along the bondline became more pronounced. Both of these stresses reach their maximum values at both ends of the bondline, which, together with the higher modulus of elasticity of the EP adhesive (compared to RB), resulted in adhesive failure in at least part of the joint area. But again, weaker adhesion of the adhesive to the DC substrate and better adhesion to the HX substrate is evident. For the EP adhesive, the effect of both surface treatments was not significantly more pronounced.
After exposure of the joints with RB adhesive in the climatic chamber, the joints without surface treatment failed similarly to as-bonded. The effect of surface treatment with chromium-free zirconate passivation decreased in the climatic chamber environment and the joints with this treatment failed adhesively, while the joints with organosilane substrate treatment failed cohesively even after exposure in the corrosive environment. This indicates a very strong bonding of the RB adhesive to the substrate surface (especially DC) via functional groups that prevent moisture penetration and corrosion-induced disbonding.
For the EP adhesive joints after the climatic test, the joints failed in a similar manner to the as-bonded joints; no significant improvement in adhesion was observed due to the surface treatments applied. This only confirms the above observation that for EP adhesive, due to its high load capacity above the yield strength of both substrates, surface modification is of no practical significance to improve adhesive adhesion and increase the load capacity of the joint.
Based on
Figure 9,
Figure 10,
Figure 11 and
Figure 12 and
Table 5, after considering the relationships between fracture mechanism, post fracture energy, and post fracture behaviour, we can draw a number of conclusions, outlined below.
The energy dissipated by joints performed on treated substrates upon testing is around 2 J, regardless of the type of failure. Approximately the same value of dissipated energy for both adhesion and cohesion failure means that the adhesion of the adhesive to the treated substrates and the internal cohesion of RB adhesive are approximately the same. So, the surface modifications used only changed the failure mechanism of the joint from adhesive (DC substrate exposure) to cohesive. They did not lead to an increase in the load-bearing capacity or dissipated energy of the joints, but improved the resistance of the joints against corrosion-induced disbonding when exposed in a corrosive environment.
Regarding the joints made with EP adhesive on chemically treated substrates, the adhesion of the adhesive to both types of substrate as well as the cohesion of the epoxy adhesive itself were high, far exceeded the yield strength of the weaker substrate in the joints.
The high cohesion of the epoxy adhesive was most pronounced in the HX-HX joints with good conditions for mechanical and chemical bonding with the adhesive, which was stronger than the cohesion of the adhesive and thus the joints failed by the cohesive mechanism. This was reflected by the highest energy dissipated when the HX-HX joints failed. Since the adhesion of the EP adhesive to the DC substrate was lower, this was evident for all the joints with DC substrate (DC-DC and DC-HX). Pretreatment with zirconate passivation for the DC steel joints resulted in lower Fmax values and earlier onset of failure (displacement value) and thus the dissipated energy is relatively small, compared to organosilane surface preparation. Preparation with organosilane provided higher energy dissipated in DC-DC and DC-HX joints under load, although the limiting factor in mixed joints still remained the adhesion to the DC substrate, which was manifested by the adhesive failure mechanism.
EDX analysis of the fracture surfaces of DC-HX joints and analysis of the adhesive failure mechanism are shown in
Table 7 and
Table 8.
From
Table 7 it can be seen on the DC substrate without surface treatment that both exposed (with only a very thin layer of adhesive) and adhesive-covered areas are present; the joint failure is adhesive–cohesive. After treatment with both BP and organosilane the adhesion was improved; the DC substrate remained firmly bonded to the adhesive after the bond failure. The substrate HX without treatment and with the tested treatments is not exposed; RB adhesive is found on it in different thicknesses. The joint failure with the coated substrates is cohesive.
The only exception is the HX substrate, which also contains an exposed site (high Zn content in spectrum 14).
From
Table 8 it is clear that DC substrate is revealed in all cases (proved by high Fe content in spectra 19, 2, and 12), but still with a thin adhesive layer (high C content in the same spectra). On the HX steel, there are regions with both thicker and thinner adhesive layers. The small concentration of Fe and Zn in spectra 20, 3, and 10 indicates the presence of an HX substrate under the thin adhesive layer, but no HX substrate was revealed. The bond failure is adhesive–cohesive.
A summary graphical representation of the individual joint characteristics is given in
Figure 13.
Figure 13a shows that surface modification of the substrates to form bonded joints with RB adhesive improved the adhesion of the adhesive to the DC substrate and thus brought all the investigated joints (DC-DC, HX-HX, and DC-HX) into the region of optimum utilization of the RB adhesive properties (all Fmax values with surface modification lie between the green and red lines). Joints with RB adhesive and with surface modification fail in the region between the yield strength of the DC substrate and the cohesive shear strength of the adhesive. This improvement in adhesion is maintained even after exposure in corrosive environments.
Figure 13c shows that the surface modification of the substrates was not significant for the formation of bonded joints with EP adhesive, in several cases even leading to a reduction in the load-carrying capacity of the joints, both in terms of Fmax and dissipated energy W; however, all joints, with and without surface modification, lie in the plastic deformation region of the weaker DC substrate in terms of load-carrying capacity, which thus becomes the limiting factor in mixed joints.
Figure 13b,d show the relationship of direct proportionality between the displacement values at Fmax and the dissipated energy at failure W, i.e., the higher the sFmax value, the larger the W value, and vice versa.