2. Materials and Methods
Several sheets of AISI 430 and AISI 304 SSs, having an initial BA and 2B surface finishing, respectively, were submitted to an industrial brushing operation towards the rolling direction, in order to produce different batches of both materials with the same final SB finishing, but different roughness. Usually, after this operation a polyethylene adhesive film is industrially applied on the SB finishing side of the SS sheets.
The different roughness of these batches was measured in terms of Rz parameter on the basis of UNI EN ISO 4287:2002 and UNI EN ISO 4288:2000 standards by means of a Mitutoyo SJ-210 equipment (Mitutoyo Italiana srl, Milano, Italy). The measurements were done three times on different areas of the sheets of each batch, in the orthogonal direction with respect to the almost linear scratches determined by the brushing process and for an evaluation length of 4 mm.
Table 1 reports the average values of Rz. This parameter was taken into account in this study in place of Ra because it is considered more related to the presence of more or less occluded sites, in correspondence of high peaks and deep valleys in the roughness profile.
The average chemical compositions of the studied SSs are reported in
Table 2; the analysis was performed by means of a Spark Analyser SPECTROLAB Mod. LAVFA A18A (SPECTRO Analytical Instruments GmbH, Kleve, Germany).
From the sheets of each batch, several samples 10 × 10 cm2 in size (thickness 0.7 mm) were obtained and used to characterize their localized corrosion resistance by means of anodic CPP curves at room temperature. Before each test, the polyethylene adhesive film was removed from the sample surfaces, which were gently degreased by using a paper soaked in n-hexane.
The electrochemical cell was obtained by gluing with an epoxy resin a plexiglass tube on the SB surface of the samples, which were used as working electrodes having an exposed area of 38.5 cm2. A three-electrode configuration cell was obtained using a saturated calomel electrode (SCE, 0.241 V vs. SHE) and a spiral of activated titanium as the reference electrode and counter electrode, respectively.
The anodic CPP tests were performed by means of an AMEL 5000 (AMEL srl, Milano, Italy) electrochemical workstation in two different solutions at different chloride concentrations (pH = 6.5): NaCl 0.35 wt % and 1.75 wt %. Before each test, 250 mL of the solution was poured into the plexiglass tube after being aerated by a magnetic stirrer for at least 30 min. The anodic CPP curves were all recorded following the approach used previously [
5,
22,
23,
24,
25]: the corrosion potential (E
corr) was monitored up to the achievement of stationary value (usually, within 30 min). Subsequently, the potential was increased at a scan rate of 0.166 mV/s toward the anodic direction, starting from the value E
corr−0.030 V until a current density threshold of 0.01 mA/cm
2 was achieved. The scan was then reversed and continued until the obtainment of the repassivation condition, where the protection or repassivation potential (E
prot) is determined [
25]. In those cases where the samples did not repassivate, the test was stopped in correspondence to the initial E
corr potential, and, in the data elaboration, E
prot was set equal to this last value. Some samples showed a close-loop hysteresis (E
prot > E
corr) of the anodic curve, whereas other ones showed an open-loop hysteresis (E
prot set equal to E
corr). During the forward scan, the pitting potential (E
pit) was determined in correspondence of a significant increase in current density and it was considered valid if the pits were visually observed on the sample surface. On the contrary, if the increase of the current density was determined by the crevice corrosion in correspondence of the internal borders of the plexiglass cell, the test was discarded.
For each examined SS batch, at least three samples were tested in both solutions. The average values of the potential parameters obtained from the anodic CPP curves (Ecorr, Eprot, Epit) were calculated and related to Rz.
Scanning electron microscopy (SEM) and optical microscopy (OM) observations were done in order to characterize the surface features of the different SS samples and for characterizing the pits formed at the end of CPP tests. Energy Dispersive X-ray analysis (EDX) was also performed to investigate the chemical composition in the areas outside and inside the pits. SEM and EDX observations were performed by means of Zeiss Supra 40 microscope (Carl Zeiss Microscopy GmbH, Jena, Germany) coupled with a Bruker Quantax serie 5000L N2-free XFlash (Bruker Nano GmbH, Berlin, Germany).
3. Results and Discussion
Figure 1 shows the SEM images of a sample surface for each of the two tested SSs, having the highest Rz value within the same material type (Series 3 and Series 6, respectively,
Table 1). The higher roughness of AISI 304 sample compared to AISI 430 sample is clear. Both SS surfaces show similar features, without any particular defects to highlight.
Figure 2 shows three examples of anodic CPP curves. A method for obtaining the characteristic E
corr, E
prot, and E
pit values has been reported in previous works [
5,
22,
23], but recently [
25], an analytical method has been specifically developed to obtain these parameters from anodic CPP curves.
The analytical method allows to trace the dotted grey oblique lines shown in
Figure 2 along the anodic curve, one for each significant slope variation, and thus to identify the fundamental inflection points. In particular, the first one at low potentials, close to E
corr, represents the starting point of the alloy passivity range, which ends to the second one at high potentials: this is the intersection point between the upward oblique straight line and the straight line in correspondence to a stable current density increase, which defines the pitting potential E
pit. By means of this geometrical construction, it is also possible to define a unique average passivation current density i
p within the current density passivity range (i
p,min-i
p,max) [
25] between the two described inflection points, as
Figure 2 shows. Finally, E
prot is determined in correspondence to the new achievement of passivity conditions, where the current density return into the passivity range (
Figure 2a,c; closed-loop hysteresis). If this condition is not met (
Figure 2b; open-loop hysteresis), E
prot has been set equal to the initial E
corr value, which is easily obtained in all cases in the point where the curve passes from the cathodic branch to the anodic one.
From these characteristic potential values, it is possible to define both the perfect passivity region (
ppr) between E
corr and E
prot, where the pitting cannot initiate and the existing pits cannot propagate and the imperfect passivity region (
ipr) between E
pit and E
prot, where pits cannot initiate but the existing ones can propagate [
22,
23,
24,
25]. In the case of mechanical damage of the passivity film, localized corrosion does not propagate in service applications if the SS shows a closed-loop hysteresis (
Figure 2a,c), with a more extended
ppr as possible. On the contrary, for a SS that gives an anodic CPP curve similar to that of the AISI 430 sample Series 3, shown in
Figure 2b, the risk of localized corrosion propagation is very high.
From the analysis of the AISI 430 and AISI 304 anodic curves in both NaCl solutions, the results shown in
Figure 3 have been obtained, where the E
corr, E
prot, and E
pit trends, the corresponding error bars and the extensions of
ppr and
ipr are reported as a function of Rz (
Table 1). The limited extension of the error bars shows the good reproducibility of the results obtained from the anodic CPP curves.
Considering E
pit, AISI 304 shows higher values compared to those of AISI 430 in both solutions, although the former has in general a significantly higher roughness with respect to the latter (
Table 1,
Figure 3). Only the E
pit of AISI 304 Series with the highest Rz gets closer to E
pit of AISI 430 Series (
Figure 3), showing a not negligible effect of the surface roughness. However, since on increasing the surface roughness, E
pit of SSs in chloride solutions is normally expected to decrease [
17,
18], from these results, it can be concluded that the chemical composition of the tested SSs (
Table 2) is a more important factor than the roughness on determining their localized corrosion resistance. Cr content of the examined SSs, sensibly higher in AISI 304 than in AISI 430 (
Table 2), is the important factor that determines the higher values of E
pit for the former compared to latter [
10,
26]. Ni, present only in AISI 304 SS, has been considered of scarce importance on influencing these potential values in the case of SS alloys [
26].
The effect of roughness increase on the decrease of E
pit is visible for AISI 304, in particular in NaCl 0.35 wt % (
Figure 3a). This result can be related to the fact that AISI 304 has the highest values of Rz and the differences of this parameter among the Series are significantly higher than those among the AISI 430 Series (
Table 1,
Figure 3). These results do not agree with the results of other authors [
12,
15], which reported a poor correlation between corrosion resistance and the surface roughness parameters, when they move towards relatively high values. However, it is necessary to consider that these literature results are relative to only one SS, with different roughness, whereas in the present work two different SSs with two different Rz ranges are compared.
On increasing the NaCl concentration, the aggressiveness of the solution is probably so high that it is does not allow the observation of a clear E
pit decrease as a function of Rz for AISI 304 (
Figure 3b).
In the case of AISI 430 Series, E
pit does not show a particular relationship with Rz in both NaCl solutions. This result can be related to the very low differences of Rz values among the AISI 430 Series (
Table 1).
As expected, the effect of chloride concentration increase is to decrease E
pit passing from NaCl 0.35 wt % (
Figure 3a) to NaCl 1.75 wt % (
Figure 3b): E
pit ranges from 0.267–0.348 to 0.235–0.294 V for AISI 304 and ranges from 0.226–0.265 to 0.199–0.223 V for AISI 430, respectively.
A particular effect of the roughness increase on E
prot seems to be present only on AISI 304 samples in NaCl 0.35 wt % (
Figure 3a) because this potential decreases and follows the same trend of E
pit vs. Rz. However, as reported by other authors [
8,
9,
10,
15,
16,
17,
18,
19,
20,
21], while the surface roughness influences E
pit values, it does not necessarily have the same influence on the repassivation characteristics (E
prot) of a given SS [
9].
From the plots of
Figure 3, it is visible the higher extension of
ppr of AISI 304 Series with respect to that of AISI 430 Series in both solutions. At the same time, for both SSs, the
ppr extension decreases on increasing NaCl concentration and it is practically absent for AISI 430 Series in NaCl 1.75 wt %.
These results indicate that the repassivation ability of both examined SSs decreases with the increase in the concentration of chlorides. Furthermore, the absence of
ppr in the case of AISI 430 in the more concentrated NaCl solution means that the main part of the anodic CPP curves for this SS showed the same characteristics of that of
Figure 2b, with an open-loop hysteresis. In such cases, E
prot was set equal to E
corr to make possible data elaboration, but it cannot correspond to a real protection potential, which can be found only at more cathodic potentials [
27]. Even for AISI 430 Series tested in the less concentrated NaCl solution, some anodic curves showed an open-loop hysteresis (
Figure 2b), while other ones showed a closed-loop hysteresis (
Figure 2a). However, a predominant number of anodic curves of this last type was obtained and therefore
Figure 3a shows the presence of a visible
ppr in NaCl 0.35 wt %, although of limited extension.
In order to quantify the repassivation ability of both SSs, in
Table 3 the percentage of the experimental curves which showed a closed-loop hysteresis (E
prot > E
corr) are reported as a function of NaCl concentration, independently from Rz. The results of
Table 3 show the poor ability of AISI 430 to repassivate, which becomes lower with the increase of NaCl concentration, confirming the information given by
Figure 3. Therefore, it can be considered that when the passivity film on AISI 430 is damaged, there is a very low possibility for this material to return passive and, at the same time, there is a high probability to show corrosion phenomena, independently from roughness.
In order to make an in depth study on the relationship between localized corrosion resistance of SSs and roughness parameters, some authors tried to correlate the E
pit−E
corr differences (as a measure of the “extension of passivity range”, in terms of potentials) with Ra and Rz, obtaining controversial results [
8,
10,
14]. In the present work, a different approach has been used following literature findings [
28], from which E
pit−E
prot differences were considered for measuring the extension of the hysteresis loops of the anodic CPP curves. These differences were analyzed to make predictions on the durability of SSs in halide media: the higher the difference E
pit−E
prot, the lower is the durability of SSs [
28]. In the present work, a low durability of a given SS in service conditions, in contact with chloride environments, means that the macroscopic visualization of localized corrosion on its surface takes shorter times.
Figure 4 shows the E
pit−E
prot values calculated from the potentials obtained in this work. In NaCl 0.35 wt %, an almost monotonic relationship between E
pit−E
prot and Rz can be noticed. On increasing Rz, for AISI 430, E
pit−E
prot remains stationary and subsequently increases, whereas for AISI 304, before E
pit−E
prot increases and after remains almost stationary. Essentially, the durability either remains unchanged or decreases for both SSs, within the corresponding Rz ranges. In principle, in order to increase the SS durability, it can be suggested to not excessively increase the roughness of the material during the brushing operation, necessary to obtain the SB surface finishing.
The comparison of E
pit−E
prot values between AISI 430 Series and AISI 304 Series in the less concentrated NaCl solution, independently from Rz, indicates a minor durability of the former with respect to the latter. In addition, for the particular case of AISI 430, it is necessary to consider that 62.5% of the anodic curves showed a closed-loop hysteresis (
Table 3), while, for the remaining ones (37.5% with open-loop hysteresis), E
prot can be found to more cathodic values than E
corr. The consequence is a general rise of E
pit−E
prot vs. Rz curve for AISI 430, as qualitatively indicated by the dotted orange arrow in
Figure 4. From these observations, it is clear that in NaCl 0.35 wt %, the durability of AISI 304 is considerably higher than that of AISI 430; this can be attributed to the significantly higher content of Cr of the former compared to the latter (
Table 2).
In NaCl 1.75 wt % solution, the relationship between E
pit−E
prot and Rz is less regular than that previously considered in the less concentrated solution. In particular, for AISI 304, at the lowest values of Rz, E
pit−E
prot seems comparable to the values obtained for AISI 430 Series (dark blue curves in
Figure 4). However, considering that for AISI 430, only 28.6% of the anodic CPP curves showed a closed-loop hysteresis (
Table 3), the E
prot values for the majority of these curves (71.4% with open-loop hysteresis) can be found to lower values than E
corr. The consequence is a more pronounced rise of the E
pit−E
prot vs. Rz curve in
Figure 4, as qualitatively indicated by the dark blue dotted arrow compared to the orange one. Therefore, even in concentrated NaCl solution, the durability of AISI 304 is considerably higher than that of AISI 430 and it can be concluded that the differences of composition between the two tested SSs is again the more important factor affecting their durability, favouring AISI 304 due to its high content of Cr (
Table 2).
Finally, on considering only AISI 304 data in
Figure 4, for which only closed-loop hystereses were found (
Table 3), a significantly high difference E
pit−E
prot can be observed only at the lowest value of Rz, where the durability of this SS in NaCl 1.75 wt % should be lower than that expected in NaCl 0.35 wt %. On increasing Rz, this difference becomes less important.
Figure 5 displays some SEM images of the pits observed on the studied SSs at the end of CPP tests: their width is in the range 100–300 µm and their depth, measured by OM, is in the range of 150–250 µm. These pits show a cavernous characteristic.
Table 4 reports the average results of EDX analyses, in terms of Cr and Ni percentages, as those shown on both sides of SEM images in
Figure 5. The analyses were performed both inside the pits, in the points marked by red asterisks, and in points outside the pits, far from their mouth. For all samples, the EDX analyses performed outside the pits slightly underestimate the Cr and Ni contents in SSs with respect to those obtained by means of spectroscopic analyses (
Table 2).
The analyses performed inside the pits (
Table 4) indicate a significant increase in Cr content both for AISI 430 and for AISI 304 samples showing anodic CCP curves with a closed-loop hysteresis. On the contrary, for the samples of AISI 430 showing the anodic curve with the open-loop hysteresis, the Cr content resulted again higher than that found outside the pits (
Table 4), but with a lower difference compared to the previously considered AISI 430 samples showing a closed-loop hysteresis. In the case of the austenitic AISI 304 SS, even a slight Ni content depletion was found inside the pits (
Table 4).
It is noteworthy that the values reported in
Table 4 can be considered only as a qualitative indication of the changes in SS composition induced by pitting corrosion and subsequent repassivation. This is due to the fact that in the particular case of EDX analysis inside the pits, the signals do not only involve the visible pit surface (
Figure 5), but also the material underneath it, which is not yet affected by the corrosion phenomenon. However, the results of
Table 4 indicate that the repassivation at an E
prot value higher than E
corr (closed-loop hysteresis) can be associated with a significant Cr enrichment on the pit surface, where this element is able to form a new passive film and does not dissolve further.
From these observations, it can be concluded that chromium plays in any case a fundamental role on the delay of pitting initiation of the examined SSs and in the obtainment of new passivity conditions.