# Pitting Suppression of AISI 316 Stainless Steel Plates in Conditions of Ultrasonic Vibration

Authors: Georgii S. Vasyliev; Oleg M. Kuzmenko
Journal: International Journal of Chemical Engineering
 (2020)

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## Abstract

Plate heat exchangers are widespread type of equipment that suffers from pitting corrosion in chloride containing solutions. Anodic behaviour of AISI 316 stainless steel was tested in 3.5% NaCl solution in conditions of ultrasound vibration (27 kHz, 10 W). The potentiodynamic sweep, potentiostatic technique, and galvanostatic technique were used coupled with surface morphology investigation after polarization. The pitting potential increased from 0.26 ± 0.02 V/SSCE to 0.42 ± 0.05 V/SSCE, and repassivation potential increased from 0.03 ± 0.01 V/SSCE to 0.18 ± 0.04 V/SSCE when vibration was applied. The anodic current at applied potential in pitting region was two orders of magnitude lower in conditions of ultrasound vibration. A possible mechanism of vibration influence on pitting is proposed, which is the elimination of pit covers from the vibrating surface, vibration-induced electrolyte motion in and out of the pits, and repassivation of active metal inside the pits.


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## Body

## 1. Introduction

Pitting corrosion is a major problem of metals in passive state operating in chloride containing solutions [1–4]. Surface defects and inclusions are the most common sites for pit initiation [5, 6], and pitting corrosion resistance is reduced at high flow rates [7]. The high corrosion rate, nonuniform pitting distribution, and high corrosion rate inside the pit cavity make this type of corrosion extremely dangerous, especially for thin metal parts. One of the examples of such equipment is plate heat exchangers. Thin stainless plates of 0.2–0.5 mm are assembled in one pack and the heat carrier pass between the plates at high velocity. The pitting corrosion of the steel can shorten the operation time of the heat exchanger to 1-2 years instead of a planned period of 25 years.Pitting corrosion usually undergoes several consecutive stages, from pit initiation to stable pitting growth. The metal impurities, grain boundaries, and mechanical defects of the passive film are known to be pit initiation sites. Recent works showed that MnS inclusions play significant role in pit initiation. The pit initiates at the boundary between the MnS inclusion and steel matrix and grows with time [8–10]. Under applied stress, the dissolution of MnS inclusions and sensitized grain boundaries is accelerated [11]. Laser surface melting was found to significantly reduce the size of the sulphide inclusions and thus improve the pitting resistance of austenitic steel [12].Different approaches were developed to reduce the pitting corrosion of stainless steel [13–18]. Recent investigations revealed that the application of ultrasound (US) cavitation is an efficient tool to suppress pitting corrosion of stainless steels. Wang studied the pitting suppression of SUS304 stainless steel in 3.5% NaCl solution and found three times reduction of electric charge passing through the steel when it was under the influence of ultrasound cavitation [19]. When the influence of ultrasound on pitting initiation, growth, and repassivation was investigated, it was established that lower potentials at constant currents and higher currents at constant potential responded to ultrasound [20]. In further work, it was shown that US intensity, as well as the distance between the vibrator and the steel specimen significantly, influences the efficiency of pitting suppression. When the distance was equal to US wavelength, the pitting suppression efficiency was proportional to the intensity. At a constant intensity, the increase in distance resulted in the reduction of efficiency [21].The mechanism of pitting suppression with the application of ultrasound is based on the removal of the corrosion products cover over the nucleated pit. Once the pit is initiated, its further growth depends greatly on the stability of the cover over the pit mouth [22–24]. Ultrasound cavitation produces collapsing bubbles that bring about high collapse power. This promotes a cleaning effect on the surface; thus, the corrosion products covering the metastable pits are removed from the surface and pits are passivated [20, 21, 25, 26].However, high intensity ultrasound is able to remove not only the partially damaged passive film but also the regular film, thus accelerating the corrosion rate. The simultaneous action of high intensity ultrasound and corrosive environment accelerates steel degradation [27–29]. The ultrasonic cavitation makes the outer layer of the passive film damaged, and the corrosion rate is accelerated [30]. Lavigne observed that passive films formed for 1 h under potentiostatic polarization and under ultrasonic conditions have more defects compared with those formed under silent conditions, which leads to a considerable decrease in the corrosion resistance of the sample [31]. Wan used 250 W ultrasound and found that cavitation accelerated the erosion of the ferrite in the corroded surface layer, resulting in the degradation of the nanomechanical properties of the corroded surface layer on stainless steel under cavitation [32]. The pitting corrosion was found to reduce fatigue behaviour of metals reducing the fatigue life by a factor of 10–100 [33].Practical application of ultrasound to reduce pitting corrosion of stainless steel is limited by a short radius of cavitation field around the horn [34]. This work is aimed at the investigation of the anodic behaviour of AISI 316 stainless steel in conditions of ultrasound vibration instead of cavitation and possible mechanism of pitting suppression is proposed.


## 2. Materials and Methods

Commercially supplied AISI 316 steel plate of 0.5 mm thick was used in all the experiments. The steel composition was: C, 0.08 mass%; Mn, 1.08; Si, 0.28; S, 0.02; P, 0.04; Cr, 16.1; Ni, 10.8; Mo, 2, 15; Fe balance. The steel sheet was cut into plates 20 × 200 mm. The plate was insulated, leaving a working area of 1 cm2 on one side of the plate. The surface of the plate was degreased with organic solvent and washed in flowing and distilled water.The corrosion tests were carried out in a three-electrode cell connected to the potentiostat (Figure1) [35, 36]. The working electrode was attached to the piezoelectric ultrasound transducer and connected to the ultrasound generator. A piece of glass (3 mm thick) was placed between the transducer and the steel plate to exclude any electrical contact. The input power of the ultrasound generator was 10 W, and the ultrasound intensity was 0.35 W/cm2 and US frequency 27 kHz. The low frequency ultrasound is widely used in industry to clean heat exchanging equipment from scale. Low intensity ultrasound was used to prevent any mechanical degradation of material due to erosion or fatigue. The ultrasound pressure was two orders of magnitude lower than the stress needed to cause fatigue fracture of the stainless steel [37]. The solution used in all the experiments was 3.5 mass% NaCl, and the temperature was maintained at 25° C using a water bath. A platinum plate was used as a counter electrode, and a saturated silver chloride electrode (SSCE) was used as a reference one.Figure 1
The scheme of laboratory set-up for corrosion testing in conditions of ultrasound vibration.Potentiodynamic polarization technique was used to determine the pitting potentialEpit and repassivation potential Erep. The polarization started from the OCP to the anodic direction with the scan rate of 0.2 mV/s. The nucleation of pits resulted in sharp current rise, and when the current value reached 100 μA/cm2, the polarization was reversed. The Epit was determined as a potential, where the current starts to increase. The Erep was determined in the reverse (cathodic) scan as a potential where the current in the reverse scan became lower than in the forward scan. In the tests with ultrasound, the steel plate was vibrated during the polarization. The tests were repeated five times to ensure data convergence. The experimental data in this work are presented by typical curves, and the values of Epit and Erep were averaged among five tests.OnceEpit was determined, the potentiostatic polarization technique was applied to compare the anodic current density with and without the application of ultrasound. The polarization started at the OCP and continued up to 0.3 V/SSCE with the scan rate of 0.2 mV/s. At 0.3 V/SSCE, the scan was stopped; potential was kept constant for 1 h and the anodic current was recorded. The holding potential of 0.3 V/SSCE was selected, because in potentiodynamic polarization tests it was established that pitting is already initiated for the nonvibrated sample, while the vibrated one remains passive at this potential.In the galvanostatic polarization method, the potential was determined as a function of time when a constant current was applied. The specimen was placed into the solution and held until the corrosion potential was established. Afterwards, a constant current density of 30μA/cm2 was applied for 1800 sec and the potential was recorded vs time. Every 1800 sec the current density was increased in 30 μA/cm2, to constitute 60, 90, and finally 120 μA/cm2. The same procedure was performed in conditions of ultrasound vibration. The current density values for the galvanostatic test were selected in the range, where stable pitting corrosion occurs on the surface of the nonvibrated steel according to the potentiodynamic test.After potentiostatic and galvanostatic polarizations, the working area of the steel surface was observed with the optical microscope to analyse the developed pits. The pit depth was measured using double focusing technique when the image is focused on the top of the surface and on the bottom of the pit. The difference in the focus distance is equal to the pit depth.


## 3. Results and Discussion

### 3.1. Potentiodynamic Polarization

Potentiodynamic polarization is used to determine the values of pitting potentialEpit and repassivation potential Erep. The first one refers to the breakdown of the passive film, while the second one characterizes the total passivation of the pits formed above this potential. Typical potentiodynamic curves are given in Figure 2, and the Epit and Erep values, obtained in all the tests, are presented in Table 1.Figure 2
Potentiodynamic sweep of AISI 316 stainless steel in 3.5% NaCl solution. 1: nonvibrated; 2: vibrated. Sweep rate: 0.2 mV/s. Ultrasound parameters: frequency 27 kHz, power 10 W.Table 1
The pitting potentialEpit and repassivation potential Erep of the AISI 316 steel in 3.5% NaCl in vibrated and nonvibrated conditions.
Test numberNonvibratedVibratedEpit, V/SSCEErep, V/SSCEEpit, V/SSCEErep, V/SSCE10.260.030.410.1520.260.040.450.1930.280.020.350.1540.250.040.470.2250.260.040.40.18Average0.26 ± 0.020.03 ± 0.010.42 ± 0.050.18 ± 0.04In the absence of ultrasound vibration, the steel remains passive until the potential is below 0.1 V/SSCE. After this potential, several current fluctuations are observed that led to the steady current growth once the potential reaches 0.2 V/SSCE. When the current density reached 0.1 mA/cm2, the polarization direction was shifted from anodic to cathodic. However, the current continued to grow as pitting was initiated. At the maximum, the current density values reached 0.3 mA/cm2. In the reverse scan, after the potential of 0.16 V/SSCE, the current decreased and the Erep was reached at 0.03 ± 0.01 V/SSCE.Another situation is observed for the vibrating specimen. The current below 1μA/cm2 is observed until the potential is below 0.42 ± 0.05 V/SSCE. After this potential, the current starts to grow rapidly, even when the scan direction is reversed. The maximum current value is reached at 0.35 V/SSCE. There are several current peaks below this potential, but each following peak was lower showing the current tendency to decrease. Finally, the steel passivated at 0.18 ± 0.04 V/SSCE.Comparing the pitting potentialsEpit and repassivation potentials Erep with and without ultrasound, it is clearly seen that US vibration increased the Epit in 0.16 V from 0.26 ± 0.02 V/SSCE to 0.42 ± 0.05 V/SSCE and Erep in 0.15 V from 0.03 ± 0.01 V/SSCE to 0.18 ± 0.04 V/SSCE to the anodic side. Thus, ultrasound vibration appeared to be a strong pitting suppression factor.


### 3.2. Potentiosatic Polarization

Potentiostaic polarization was performed to compare the anodic behaviour of vibrated and nonvibrated steel (Figure3). For the nonvibrated steel, the current appeared at 0.24 V/SSCE and raised slowly to reach the value of 0.25 mA/cm2. After this, a sharp increase occurred, and the current reached the value of 5 mA/cm2 and remained at this level.Figure 3
Potentiostatic polarization of AISI 316 stainless steel in 3.5% NaCl solution. 1: nonvibrated; 2: vibrated. Applied potential 0.3 V/SSCE. Ultrasound parameters: frequency 27 kHz; power 10 W.For the vibrating steel, the current-time dependence shows a slow rise when the potential was scanned in the anodic direction. The current value stabilized at 0.03 mA/cm2 when the potential becomes stable. Due to the vibration of the steel, current fluctuations were observed. Comparing the current values of vibrated and nonvibrated specimens, it can be clearly seen that ultrasound vibration reduces anodic current in the pitting region at least in 100 times.


### 3.3. Galvanostatic Polarization

During galvanostatic polarization, the minimum galvanostatic potential of pitting corrosionEpc was determined when constant current was applied. In this test, a total of four current densities were tested, ranging from 30 to 120 µA/cm2 applied for 1800 sec each.The potential-time dependences are given in Figure4. The current density of 30 µA/cm2 does not cause any significant changes in Epc potential between the vibrated and nonvibrated specimens. At higher current densities, the Epс value of nonvibrated steel is 0.02 ± 0.02 V/SSCE. Significantly more positive values were obtained for the vibrated steel. At the applied current density of 90 µA/cm2, the Epс is 0.1 ± 0.02 V/SSCE.Figure 4
Galvanostatic polarization of AISI 316 stainless steel in 3.5% NaCl solution. 1: nonvibrated; 2: vibrated. Applied current density 30–120µA/cm2. Ultrasound parameters: frequency 27 kHz; power 10 W.Comparing the results of potentiodynamic and galvanostatic polarization, theEpit values obtained in the potentiodynamic test are much higher, meaning the pitting initiation process is slower than the potential scan rate. However, the Erep values in potentiodynamic test are close to the value of Epc in galvanostatic test for vibrated and nonvibrated specimens.The micrographs of both vibrated and nonvibrated steel surfaces are given in Figure5. For each sample, all the surfaces were analysed, and typical pitting regions are presented. Figure 5(a) shows the pit developed on nonvibrated steel during galvanostatic polarization. The corresponding potential-time dependence is shown in Figure 4. On the contrary, a series of much smaller defects was found on the surface of the vibrated steel after polarization in the same conditions (Figure 5(b)).Figure 5
The surface of AISI 316 steel after galvanostatic (a, b) and potentiostatic (c, d) polarization in conditions of ultrasound vibration (b, d) and without vibration (a, c). Ultrasound parameters: frequency 27 kHz; power 10 W.The same results were obtained in the potentiostatic polarization test. A pit of 1 mm in diameter and 20μm in depth was formed after 1 h of polarization at 0.3 V/SSCE (Figure 5(c)). On the contrary, the surface of the vibrated steel shows no signs of dissolution. The results agree well with the current-time dependences, and higher anodic current values correspond to higher number of pits and the pits are deeper.Pit morphology is known to be dependent on its growing conditions [38, 39]. The higher anodic potential results in the opened pit with no pit cover [40]. In potentiostatic test at the applied potential of +0.3 V/SSCE, the 600 µm diameter pits are formed, with no covers, and are not dish-shaped (Figure 5(c)). Similar pit morphology was observed in galvanostatic test, but pit diameter was smaller –300 µm (Figure 5(a)). In conditions of ultrasound vibration, several tiny pits are formed with the diameters 10–20 µm (Figure 5(b)) and they are dish-shaped, meaning ultrasound vibration removes the lacy covers over pit mouth.


### 3.4. Mechanism of Pitting Suppression

The possible mechanism of ultrasonic vibration influence on the local dissolution of stainless steel can be explained with the following scheme (Figure6). According to the modern views, the pitting corrosion of metals in the passive state occurs in three consecutive stages [22]. The first one is pit nucleation (Figure 6(a)). Not all the nucleated pits can survive; only surviving pits enter the second stage, the metastable growth (Figure 6(b)). At this stage, the pitting growth is diffusion-controlled. The continued survival depends on the maintenance of a cover over the pit that acts as a diffusion barrier. The cover may be formed by corrosion products of undermined passive film. The breakdown of this cover results in repassivation. All the pits that survive the metastable stage enter the third stage, stable growth (Figure 6(c)). Here, the diffusion barrier is formed inside the deep and narrow pit, where no solution stirring occurs, so the pit progress into the metal.Figure 6
The scheme of pitting suppression with the application of ultrasound vibration: (a) pit nucleation; (b) metastable pitting; (c) stable pitting growth; (d, e) influence of vibration.Several works were dedicated to the influence of pit cover removal on the repassivation of metastable pits [23]. In numerous studies in conditions of ultrasound cavitation, it was established that collapsing bubbles can ruin the pit cover, thus enhancing pit repassivation [20, 21, 25, 26]. Therefore, the mechanism of pitting suppression, when ultrasound is applied to the solution, is cavitation erosion of the pit covers.In conditions of ultrasound vibration, the cavitation is not the key factor. Ultrasound vibration is known to be widely used to clean the surface from any deposits [41–43]. Ultrasound vibration produces accelerations of 104 g. When the particle is attached to the vibrating surface, it is influenced by the vibration force originating from the piezoelectric transmitter, adhesion force, and inertia force. When the vibration is directed towards the solution (Figure 6(d)), the inertia force coincides with the adhesion force and the particle remains on the surface. However, when the vibration goes in the reverse direction, the inertia force is directed against the adhesion force. Therefore, any particles attached to the surface spall off once the inertia force exceeds the adhesion force (Figure 6(e)). For the stainless steel during pitting corrosion, such particles are lacy covers of undermined passive film over the formed pits. Moreover, continuous vibration may lead to the fatigue fracture of the corrosion cover. Once the protective cover over the metastable pits is removed, they passivate. The inertia force depends on the mass of the corrosion products and the vibration acceleration. In the present study, the mass of the cover over the pit appeared to be enough to be removed with ultrasound vibration at 27 kHz and the power of 10 W.Another important part of pits repassivation under the influence of ultrasound vibration is related to the vibration induced electrolyte motion on the surface of the steel. The electrolyte contains constant oxygen concentration and when the surface is vibrating, fresh electrolyte moves in and out of the pits favouring fast repassivation of the inner surface of the pits. Any defects of the passive film breaking are recovered by rapid reaction of active metal with an oxygen saturated electrolyte. Moreover, fast and vigorous electrolyte movement near the surface facilitates the removal of lacy cover over the metastable pits. Moreover, the detached particles in the preelectrode layer, when moving with the electrolyte, act as an additional abrasive that cleans the surface from both newly formed pit covers and nonmetallic inclusions located at the surface that are known to be promoting the pitting corrosion.


## 3.1. Potentiodynamic Polarization

Potentiodynamic polarization is used to determine the values of pitting potentialEpit and repassivation potential Erep. The first one refers to the breakdown of the passive film, while the second one characterizes the total passivation of the pits formed above this potential. Typical potentiodynamic curves are given in Figure 2, and the Epit and Erep values, obtained in all the tests, are presented in Table 1.Figure 2
Potentiodynamic sweep of AISI 316 stainless steel in 3.5% NaCl solution. 1: nonvibrated; 2: vibrated. Sweep rate: 0.2 mV/s. Ultrasound parameters: frequency 27 kHz, power 10 W.Table 1
The pitting potentialEpit and repassivation potential Erep of the AISI 316 steel in 3.5% NaCl in vibrated and nonvibrated conditions.
Test numberNonvibratedVibratedEpit, V/SSCEErep, V/SSCEEpit, V/SSCEErep, V/SSCE10.260.030.410.1520.260.040.450.1930.280.020.350.1540.250.040.470.2250.260.040.40.18Average0.26 ± 0.020.03 ± 0.010.42 ± 0.050.18 ± 0.04In the absence of ultrasound vibration, the steel remains passive until the potential is below 0.1 V/SSCE. After this potential, several current fluctuations are observed that led to the steady current growth once the potential reaches 0.2 V/SSCE. When the current density reached 0.1 mA/cm2, the polarization direction was shifted from anodic to cathodic. However, the current continued to grow as pitting was initiated. At the maximum, the current density values reached 0.3 mA/cm2. In the reverse scan, after the potential of 0.16 V/SSCE, the current decreased and the Erep was reached at 0.03 ± 0.01 V/SSCE.Another situation is observed for the vibrating specimen. The current below 1μA/cm2 is observed until the potential is below 0.42 ± 0.05 V/SSCE. After this potential, the current starts to grow rapidly, even when the scan direction is reversed. The maximum current value is reached at 0.35 V/SSCE. There are several current peaks below this potential, but each following peak was lower showing the current tendency to decrease. Finally, the steel passivated at 0.18 ± 0.04 V/SSCE.Comparing the pitting potentialsEpit and repassivation potentials Erep with and without ultrasound, it is clearly seen that US vibration increased the Epit in 0.16 V from 0.26 ± 0.02 V/SSCE to 0.42 ± 0.05 V/SSCE and Erep in 0.15 V from 0.03 ± 0.01 V/SSCE to 0.18 ± 0.04 V/SSCE to the anodic side. Thus, ultrasound vibration appeared to be a strong pitting suppression factor.


## 3.2. Potentiosatic Polarization

Potentiostaic polarization was performed to compare the anodic behaviour of vibrated and nonvibrated steel (Figure3). For the nonvibrated steel, the current appeared at 0.24 V/SSCE and raised slowly to reach the value of 0.25 mA/cm2. After this, a sharp increase occurred, and the current reached the value of 5 mA/cm2 and remained at this level.Figure 3
Potentiostatic polarization of AISI 316 stainless steel in 3.5% NaCl solution. 1: nonvibrated; 2: vibrated. Applied potential 0.3 V/SSCE. Ultrasound parameters: frequency 27 kHz; power 10 W.For the vibrating steel, the current-time dependence shows a slow rise when the potential was scanned in the anodic direction. The current value stabilized at 0.03 mA/cm2 when the potential becomes stable. Due to the vibration of the steel, current fluctuations were observed. Comparing the current values of vibrated and nonvibrated specimens, it can be clearly seen that ultrasound vibration reduces anodic current in the pitting region at least in 100 times.


## 3.3. Galvanostatic Polarization

During galvanostatic polarization, the minimum galvanostatic potential of pitting corrosionEpc was determined when constant current was applied. In this test, a total of four current densities were tested, ranging from 30 to 120 µA/cm2 applied for 1800 sec each.The potential-time dependences are given in Figure4. The current density of 30 µA/cm2 does not cause any significant changes in Epc potential between the vibrated and nonvibrated specimens. At higher current densities, the Epс value of nonvibrated steel is 0.02 ± 0.02 V/SSCE. Significantly more positive values were obtained for the vibrated steel. At the applied current density of 90 µA/cm2, the Epс is 0.1 ± 0.02 V/SSCE.Figure 4
Galvanostatic polarization of AISI 316 stainless steel in 3.5% NaCl solution. 1: nonvibrated; 2: vibrated. Applied current density 30–120µA/cm2. Ultrasound parameters: frequency 27 kHz; power 10 W.Comparing the results of potentiodynamic and galvanostatic polarization, theEpit values obtained in the potentiodynamic test are much higher, meaning the pitting initiation process is slower than the potential scan rate. However, the Erep values in potentiodynamic test are close to the value of Epc in galvanostatic test for vibrated and nonvibrated specimens.The micrographs of both vibrated and nonvibrated steel surfaces are given in Figure5. For each sample, all the surfaces were analysed, and typical pitting regions are presented. Figure 5(a) shows the pit developed on nonvibrated steel during galvanostatic polarization. The corresponding potential-time dependence is shown in Figure 4. On the contrary, a series of much smaller defects was found on the surface of the vibrated steel after polarization in the same conditions (Figure 5(b)).Figure 5
The surface of AISI 316 steel after galvanostatic (a, b) and potentiostatic (c, d) polarization in conditions of ultrasound vibration (b, d) and without vibration (a, c). Ultrasound parameters: frequency 27 kHz; power 10 W.The same results were obtained in the potentiostatic polarization test. A pit of 1 mm in diameter and 20μm in depth was formed after 1 h of polarization at 0.3 V/SSCE (Figure 5(c)). On the contrary, the surface of the vibrated steel shows no signs of dissolution. The results agree well with the current-time dependences, and higher anodic current values correspond to higher number of pits and the pits are deeper.Pit morphology is known to be dependent on its growing conditions [38, 39]. The higher anodic potential results in the opened pit with no pit cover [40]. In potentiostatic test at the applied potential of +0.3 V/SSCE, the 600 µm diameter pits are formed, with no covers, and are not dish-shaped (Figure 5(c)). Similar pit morphology was observed in galvanostatic test, but pit diameter was smaller –300 µm (Figure 5(a)). In conditions of ultrasound vibration, several tiny pits are formed with the diameters 10–20 µm (Figure 5(b)) and they are dish-shaped, meaning ultrasound vibration removes the lacy covers over pit mouth.


## 3.4. Mechanism of Pitting Suppression

The possible mechanism of ultrasonic vibration influence on the local dissolution of stainless steel can be explained with the following scheme (Figure6). According to the modern views, the pitting corrosion of metals in the passive state occurs in three consecutive stages [22]. The first one is pit nucleation (Figure 6(a)). Not all the nucleated pits can survive; only surviving pits enter the second stage, the metastable growth (Figure 6(b)). At this stage, the pitting growth is diffusion-controlled. The continued survival depends on the maintenance of a cover over the pit that acts as a diffusion barrier. The cover may be formed by corrosion products of undermined passive film. The breakdown of this cover results in repassivation. All the pits that survive the metastable stage enter the third stage, stable growth (Figure 6(c)). Here, the diffusion barrier is formed inside the deep and narrow pit, where no solution stirring occurs, so the pit progress into the metal.Figure 6
The scheme of pitting suppression with the application of ultrasound vibration: (a) pit nucleation; (b) metastable pitting; (c) stable pitting growth; (d, e) influence of vibration.Several works were dedicated to the influence of pit cover removal on the repassivation of metastable pits [23]. In numerous studies in conditions of ultrasound cavitation, it was established that collapsing bubbles can ruin the pit cover, thus enhancing pit repassivation [20, 21, 25, 26]. Therefore, the mechanism of pitting suppression, when ultrasound is applied to the solution, is cavitation erosion of the pit covers.In conditions of ultrasound vibration, the cavitation is not the key factor. Ultrasound vibration is known to be widely used to clean the surface from any deposits [41–43]. Ultrasound vibration produces accelerations of 104 g. When the particle is attached to the vibrating surface, it is influenced by the vibration force originating from the piezoelectric transmitter, adhesion force, and inertia force. When the vibration is directed towards the solution (Figure 6(d)), the inertia force coincides with the adhesion force and the particle remains on the surface. However, when the vibration goes in the reverse direction, the inertia force is directed against the adhesion force. Therefore, any particles attached to the surface spall off once the inertia force exceeds the adhesion force (Figure 6(e)). For the stainless steel during pitting corrosion, such particles are lacy covers of undermined passive film over the formed pits. Moreover, continuous vibration may lead to the fatigue fracture of the corrosion cover. Once the protective cover over the metastable pits is removed, they passivate. The inertia force depends on the mass of the corrosion products and the vibration acceleration. In the present study, the mass of the cover over the pit appeared to be enough to be removed with ultrasound vibration at 27 kHz and the power of 10 W.Another important part of pits repassivation under the influence of ultrasound vibration is related to the vibration induced electrolyte motion on the surface of the steel. The electrolyte contains constant oxygen concentration and when the surface is vibrating, fresh electrolyte moves in and out of the pits favouring fast repassivation of the inner surface of the pits. Any defects of the passive film breaking are recovered by rapid reaction of active metal with an oxygen saturated electrolyte. Moreover, fast and vigorous electrolyte movement near the surface facilitates the removal of lacy cover over the metastable pits. Moreover, the detached particles in the preelectrode layer, when moving with the electrolyte, act as an additional abrasive that cleans the surface from both newly formed pit covers and nonmetallic inclusions located at the surface that are known to be promoting the pitting corrosion.


## 4. Conclusions

Application of ultrasound vibration is an efficient technique to reduce the pitting corrosion of AISI 316 steel in chloride containing solution, and this can be a promising approach to reduce the pitting corrosion of stainless steel parts in industrial plate heat exchangers. In addition, low amplitude ultrasound vibration is safe and does not cause fatigue fracture of the equipment.The potentiodynamic polarization showed that the pitting potential was shifted to the anodic direction in 0.16 V from 0.26 ± 0.02 V/SSCE to 0.42 ± 0.05 V/SSCE and repassivation potential in 0.15 V from 0.03 ± 0.01 V/SSCE to 0.18 ± 0.04 V/SSCE in conditions of ultrasound vibration. Potentiostatic polarization of the steel in the pitting region showed two orders of magnitude current reduction when ultrasound vibration was applied. Surface analysis revealed practically no signs of dissolution for the vibrated steel, which confirms efficient pitting suppression with ultrasound vibration.Possible mechanism of pitting suppression is the elimination of corrosion product covers over the pits. The detachment of corrosion products occurs when the inertia force appears under vibration and exceeds the adhesion force. Vibration-induced electrolyte motion leads to the further weakening of corrosion covers adhesion and promotes penetration of fresh oxygen-saturated electrolyte inside the pits that leads to the fast repassivation of the active metal.



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*Source: 6697227-2020-12-04.xml*