Home The influence of preparation of nano-ZrO2/α-Al2O3 gradient coating on the corrosion resistance of 316L stainless steel substrate
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The influence of preparation of nano-ZrO2/α-Al2O3 gradient coating on the corrosion resistance of 316L stainless steel substrate

  • Lianzhi Zhang EMAIL logo , Zhangyong Wu EMAIL logo , Tingyou Wang and Ziyong Mo
Published/Copyright: March 23, 2023

Abstract

Generally, 316L stainless steel instrumentation tubes working in a humid environment with a large amount of Cl all the year round have serious corrosion problems, so the stainless steel substrate should be gradiently coated with nano-ZrO2/α-Al2O3 slurry. In this article, the slender 316L stainless steel tube was first ground by magnetorheological fluid and then coated with the slurry, which can not only increase the contact area between the coating and the substrate but also prevent the generation of new substances that have adversely affected the adhesion of the coating. The properties of the samples were characterized and analyzed; the results showed that the substrate ground by magnetorheological fluid is more favorable for bonding with coating under the grinding conditions that the speed of the tube is 210 rpm, magnetic induction intensity is 40.83 mT, and mass ratio of micron and submicron magnetic particles is 2.3. The coating prepared under the above conditions has uniform thickness, flat surface, and can better inhibit the diffusion of Cr of the substrate to its surface. It can be obtained from corrosion resistance analysis that the coating has the highest self-corrosion potential of −0.016 V and the lowest corrosion current density of 0.491 μA/cm2, which indicate that the coating has the strongest corrosion resistance. According to the composition analysis of the coating, the composition of the corroded coating is similar to that of the coating itself, but accompanied by a small amount of Fe, which indirectly indicates that the coating is relatively compact, the coating is well bonded with the substrate, and the coating can protect the substrate; thus, the service life of 316L stainless steel instrumentation tubes is extended.

1 Introduction

Manufacturing is the main body of industry, one of the power sources of modernization, and it undertakes the important manufacturing tasks of transportation, living materials, and defense equipment; it is not only an essential carrier of emerging technologies but also a booster for its development. Therefore, its development level determines the lifeline of the entire national economy. Since the 1950s, due to the development demands of materials science, high technology, cutting-edge defense products, and scientific research, the update on new products has been accelerated, and products with high strength and cost performance are required. Therefore, products have been required to develop in the direction of high speed, high precision, high reliability, corrosion resistance, high temperature, high pressure, and high power [1,2,3,4,5]. However, machining as a part of manufacturing science and technology is very important for modern manufacturing industries [6], so machining faces a series of severe challenges [7,8]. The importance of nuclear power has become increasingly prominent with the decrease of fossil fuel reserves such as coal and oil [9,10]. Currently, lots of slender 316L stainless steel tubes are used in nuclear safety instruments, such as the pressure-inducing tubes in the built-in orifice flowmeter assembly used to measure the small flow of air. Stress corrosion cracks of 316L stainless steel instrumentation tubes are prone because the medium is wet and contains a large number of chloride ions [11,12,13,14], which seriously threatens the use safety of nuclear-grade instrumentation tubes. Therefore, nuclear-grade instrumentation tubes are required to have strong corrosion resistance, so manufacturing requirements for nuclear-grade instrumentation tubes are pretty strict.

At present, the internal surface of the 316L stainless steel tube is often processed by cold drawing, sandblasting, laser irradiation, etc. A cold-drawn stainless steel tube is formed by the plastic deformation of the pre-treated hot-rolled stainless steel tube when it goes through a mold having a particular shape and size under the action of drawing force of a hydraulic high-precision cold-drawing machine. Cold drawing is widely used because of its high production efficiency, chipless processing, and high material utilization rate. However, a large amount of plastic deformation is produced during cold drawing, which will cause significant lattice distortion, resulting in the increase of lattice energy, the increase of internal energy of the metal, and generation of residual stresses [15,16,17,18,19,20,21,22,23,24], and eventually the increase of hardness while the decrease of toughness. When the residual stresses reach a specific value, the metal will be torn along a specific grain interface, which will result in the cracking of the stainless steel tube. The blasting process enables roughing or smoothing out the inner surface of 316L stainless steel tube according to individual requirements, but the removal of the surface layers and the subsurface work hardening occurs together with changes in mechanical properties and surface activity [25]. In addition, laser beam micromachining (LBM) causes several phenomena that are variations in dislocations and residual stress distributions, formation of different carbide types, and size and shape modification of austenitic grains, and hardening effects [26]. Therefore, it is urgent to explore a suitable and high-quality processing method for the inner surface of the 316L stainless steel tube.

Magnetorheological grinding (MRF) is an emerging surface precision processing technology. Unlike traditional machining methods, the “tool” used in magnetorheological grinding is loose and free-moved magnetic particles, so its grinding has pretty good flexibility [27,28,29,30,31,32]. In addition, the interaction between magnetic poles and abrasives is noncontact. Therefore, slender tubes can be ground by magnetic abrasives, while that cannot be processed by the conventional method. Furthermore, a mathematical model that can more comprehensively predict the surface roughness value of the inner surface of the tube has not been found in the existing magnetorheological grinding theory, and the grinding is generally carried out with single particle-size magnetic particles. In this article, magnetic abrasives are prepared by high-energy ball milling of micron and submicron ferromagnetic particles and nano-abrasive particles, so magnetic abrasives with a larger shear yield stress, better fluidity, and large hardness can be obtained. Therefore, when constructing a surface roughness prediction model, in addition to considering the influences of the speed of the stainless steel tube and magnetic induction strength on it, the mass ratio of micron and submicron magnetic particles also needs to be taken into account. However, magnetorheological grinding can not change any chemical properties of the tube, so the corrosion resistance of the tube after grinding is poor. If the inner surface of the ground tube is coated with corrosion-resistant nanomaterials, the corrosion resistance of the stainless steel tube can be significantly improved [33,34,35,36].

Numerous techniques [37] have been applied to enhance the corrosion resistance of stainless steel. Coating is one of the most efficient surface treatment and modification techniques among them. Alumina is a cost-effective, heat resistant, and chemically durable material and has broad applications as protective coatings for stainless steel in the marine environment [38], but limitation for this ceramic coating results from the inevitable porous structure of alumina allowing oxygen or aqueous medium permeability. Betts [39] attempted to blow cladding Al2O3 powder in a 316 stainless steel substrate but received bad results. Tao et al. [40] conducted a continuous immersion test in 3.5 wt% NaCl solution on Al coatings on AZ91D magnesium alloy; the results measured by EIS revealed that the corrosion resistance decreased and the Warburg diffusive impedance increased sharply due to the pitting corrosion at the active sites which were later filled with solution and corrosion products. However, the Al/Al2O3 multilayers prepared by evaporation with ion beam-assisted deposition (IBAD) have been successfully applied on CK45 steel by Xue et al. [41], and good corrosion protection has been obtained. Yi’s study has shown that Al/Al2O3 bilayer coating with a graded interface layer can improve corrosion resistance and surface hardness [42]. However, the most prominent problem in preparing coating on the substrate surface is poor adhesion, which often leads to coating to crack and even spall in application [43,44,45]. Several techniques have been reported to facilitate the bond strength between resin cement and Y-TZP ceramic [46]. In addition, tribochemical silica coating was suggested as an effective method for bonding [47], but it has been recently criticized for possibility of subcritical crack propagation within zirconia [48]. In the relevant research [49], Al2O3 ceramic coating deposited on metallic substrates by plasma spraying has received considerable attention for good corrosion resistance. However, the single Al2O3 coating presents porous microstructures and poor bonding. Especially, it often obtained lower bond strength between Al2O3 ceramic and the metallic substrate due to their biggest difference in thermal expansion coefficient.

In conclusion, in order to improve the bonding strength between coating and substrate, on the one hand, the substrate needs to be ground in advance, and on the other hand, the coating needs to be gradiently prepared to reduce the stresses in the coating. Therefore, in this article, the slender 316L stainless steel tube was first ground by magnetorheological fluid and then gradiently coated with the prepared nano-ZrO2/α-Al2O3 slurry, which can not only increase the contact area between the coating and the substrate but also prevent the generation of new substances that have adversely affected the adhesion of the coating, eventually improving the bonding strength between the coating and the substrate and achieving the protection of the substrate. In addition, for the parts working in nuclear power plants, the selection of coating materials in terms of good corrosion resistance, and good high-temperature stability, α-Al2O3 is the preferred coating material because α-Al2O3 has not only good corrosion resistance, good thermal stability, high thermal conductivity, and low thermal expansion coefficient but also is cheap and rich in raw materials. Thermal expansion coefficient of ZrO2 is between that of 316L stainless steel and that of α-Al2O3. Moreover, ZrO2 has excellent corrosion resistance. Therefore, ZrO2 is used as transition layer material, which can relieve the generation of stresses during the preparation of coating, so the bonding strength between the coating and the substrate is increased, and eventually, corrosion resistance of the coated sample is improved.

Therefore, in this article, the slender 316L stainless steel tube was first ground by magnetorheological fluid and then gradiently coated with nano-ZrO2/α-Al2O3 slurry; finally, its corrosion resistance is significantly improved.

2 Establishment of surface roughness prediction model by multiple linear regression

The proper magnetic induction intensity is crucial for obtaining a high-precision and high-quality processing surface in magnetorheological grinding. Considering the actual situation of shearing and grinding of the magnetorheological fluid, magnetic particles should include both micron and submicron sizes, so mass ratio ε of micron and submicron magnetic particles has an important influence on the inner surface quality of the tube. In addition, it is also necessary to consider the influence of the speed of the slender tube on the surface quality. Therefore, a surface roughness prediction model can be constructed as shown in equation (1).

(1) S q = K n β 1 B ¯ β 2 ε β 3 ,

where S q is the evaluation value of three-dimensional surface roughness of the inner surface of the slender tube; K is the scale coefficient of the model; n is the speed of the slender tube; B is the magnetic induction intensity value; ε is the mass ratio of micron and submicron magnetic particles. The surface roughness values of inner surfaces of slender tubes (substrates) after magnetic grinding are shown in Table 1.

Table 1

Surface roughness values of substrates after magnetic grinding

Substrate Speed of tube magnetic induction intensity Mass ratio Surface roughness
n/(rpm) B /(mT) ε value S q / μ m
1# 105 96.07 1.5 5.385
2# 210 96.07 9.0 5.813
3# 132 96.07 2.3 5.897
4# 170 96.07 4.0 5.032
5# 210 59.12 4.0 6.799
6# 170 59.12 9.0 5.955
7# 132 59.12 1.5 5.195
8# 105 59.12 2.3 4.634
9# 210 40.83 2.3 6.778
10# 170 40.83 1.5 6.821
11# 132 40.83 9.0 6.510
12# 105 40.83 4.0 6.214
13# 210 29.06 1.5 7.526
14# 170 29.06 2.3 6.874
15# 132 29.06 4.0 6.914
16# 105 29.06 9.0 6.437

Formula (1) is a nonlinear function. A linear function model of Formula (2) can be obtained by linearizing Formula (1).

(2) lg S q = lg K + β 1 lg n + β 2 lg B ¯ + β 3 lg ε .

Let y = lg S q , β 0 = lg K , x 1 = lg n , x 2 = lg B ¯ , and x 3 = lg ε . The simplified linear regression model is shown in equation (3).

(3) y = β 0 + β 1 x 1 + β 2 x 2 + β 3 x 3 .

Multiple linear regression equations are constructed as follows:

(4) y 1 = β 0 + β 1 x 11 + β 2 x 12 + β 3 x 13 + δ 1 y 2 = β 0 + β 1 x 21 + β 2 x 22 + β 3 x 23 + δ 2 y 16 = β 0 + β 1 x 161 + β 2 x 162 + β 3 x 163 + δ 16 ,

where δ i is the random experimental error. Let

Y = y 1 y 2 y 16 X = 1 x 11 x 12 x 13 1 x 21 x 22 x 23 1 x 161 x 162 x 163 β = β 0 β 1 β 2 β 3 , a n d δ = δ 1 δ 2 δ 16

The regression model is

(5) Y = X β + δ ,

where Y is the matrix composed of values obtained after logarithmic transformation for each group of surface roughness values; X is the matrix composed of values obtained after logarithmic transformation for each process parameter; β is the matrix composed of the regression coefficients in the linear regression model; δ is the matrix composed of the random errors.

It is known from the principles of the method of least squares that the least-squares estimation vector B ˆ can be solved when the residual sum of squares in the linear regression model takes a minimal value.

(6) Q = i = 1 n δ i 2 = δ δ = ( Y X β ) ( Y X β ) .

Therefore, the partial derivative of the residual sum of squares with respect to the parameter β to be estimated is zero. That is

(7) Q β = 2 X Y + 2 X X β ˆ = 0 .

Assuming that the matrix X X exists, the formula (8) can be obtained from formula (7), as follows:

(8) β ˆ = ( X X ) 1 X Y .

Substituting the data in Table 1 into equation (8), the regression coefficients can be obtained as shown in equation (9).

(9) β ˆ = β ˆ 0 β ˆ 1 β ˆ 2 β ˆ 3 = 0.622 0.219 0.198 0.008 .

The regression equation can be determined by equation (9):

(10) y = 0.622 + 0.219 x 1 0.198 x 2 + 0.008 x 3 .

Then, the prediction model of surface roughness is:

(11) S q = 10 0.622 n 0.219 B ¯ 0.198 ε 0.008 .

From the index of each process parameter of the prediction model of surface roughness, it can be seen that the importance order of process parameters that affect the microscopic morphology of the inner surface of stainless steel tube is respectively speed of slender tube, magnetic induction intensity, and mass ratio of micron and submicron magnetic particles. The comparison results between the measured and predicted values of the inner surface roughness of the slender tube are shown in Table 2.

Table 2

Comparison results between the measured and predicted values of inner surface roughness of the slender tube

Substrate Measured value Predicted value Absolute error Relative error (%)
S q / μ m S q / μ m
1# 5.385 4.700 −0.685 −12.7
2# 5.813 5.569 −0.244 −4.2
3# 5.897 4.975 −0.922 −15.6
4# 5.032 5.280 0.248 4.9
5# 6.799 6.089 −0.710 −10.4
6# 5.955 5.853 −0.102 −1.71
7# 5.195 5.440 0.245 4.7
8# 4.634 5.211 0.577 12.5
9# 6.778 6.526 −0.252 −3.7
10# 6.821 6.187 −0.634 −9.3
11# 6.510 5.959 −0.551 −8.5
12# 6.214 5.629 −0.585 −9.4
13# 7.526 6.931 −0.595 −7.9
14# 6.874 6.664 −0.210 −3.1
15# 6.914 6.330 −0.584 −8.4
16# 6.437 6.063 −0.374 −5.8

It can be seen from Table 2 that the maximum absolute value of the absolute error of the prediction model is 0.922 μm, and the average value of absolute error is −0.34 μm; the maximum absolute value of relative error is 15.6%, and its average value is −4.96%, which indicate that prediction accuracy of the prediction model is good. The model can better reflect the influences of the various process parameters on the micromorphology of the inner surface of the slender tube after magnetic grinding and guide the selection of magnetic abrasive grinding process parameters.

3 Materials and method

The monoclinic ZrO2 (20 nm), α-Al2O3 (30 nm), Fe3O4 (80 mesh), Fe3O4 (800 mesh), cetyltrimethylammonium bromide (CTAB), sodium carboxymethyl cellulose (CMC) and other reagents used in the experiments are all analytically pure and were purchased from high-quality zirconium nanomaterials Co.,Ltd. in Suzhou.

3.1 Magnetorheological grinding of a slender 316L stainless steel tube

Fe3O4/ZrO2 magnetorheological fluid was prepared by a double planetary ball mill. The magnetic block supported by a self-made frame was fixed on the skateboard of the CY6140 ordinary lathe by the magnetic base. One end of the slender tube was sealed with a cap, and then, the magnetorheological fluid was injected into the slender tube with a syringe, and the other was sealed and clamped on the machine tool spindle. The tube was cut into half from the middle part with a wire electric discharge machine after magnetorheological grinding. Half of it was used to measure the surface roughness value of the sample. The other half was used for slurry coating experiments. The behavior of magnetic abrasive particles in a magnetic field is shown in Figure 1(a). The grinding schematic diagram of magnetic abrasive particles is shown in Figure 1(b).

Figure 1 
                  Grinding mechanism of magnetic abrasive particles: (a) behavior of magnetic abrasive particles in magnetic field, (b) grinding schematic diagram of magnetic abrasive particles.
Figure 1

Grinding mechanism of magnetic abrasive particles: (a) behavior of magnetic abrasive particles in magnetic field, (b) grinding schematic diagram of magnetic abrasive particles.

3.2 Preparation of nano-ZrO2/α-Al2O3 gradient coating

The ground substrate was first pretreated before the slurry was coated. The dust on the substrate surface was first removed with diluted alcohol, and the rust on the substrate surface was removed with diluted oxalic acid. After cleaning and drying the substrate, the coating of the slurry can be carried out. The CMC, ZrO2, and α-Al2O3 were mixed well using an electric stirrer. The slurry could be prepared after the mixed mixture of CMC, ZrO2, and α-Al2O3 was milled by a double planetary ball mill for some time. The slurry was gradiently coated on the substrate surface by the wetting method; a schematic diagram of gradient coating is shown in Figure 2. The slurry was further dried in a constant-temperature drying oven at 60°C for 30 min after being naturally dried and then held in a chamber resistance furnace at 310°C for 1 h, so nano-ZrO2/α-Al2O3 gradient coating could be prepared. The coated samples were cut into 10 mm in length with a wire electric discharge machine and used for corrosion test analysis in a CHI760e electrochemical workstation. The photo of the electrochemical workstation is shown in Figure 3. The green collet is connected to the working electrode, the red collet is connected to the platinum sheet counter electrode, and the white collet is connected to the silver/silver chloride reference electrode. Finally, the surface and cross-sectional morphologies of samples were observed using a high-resolution field emission scanning electron microscope (FESEM).

Figure 2 
                  Schematic diagram of ZrO2/α-Al2O3 gradient coating.
Figure 2

Schematic diagram of ZrO2/α-Al2O3 gradient coating.

Figure 3 
                  Photo of CHI760e electrochemical workstation.
Figure 3

Photo of CHI760e electrochemical workstation.

4 Results and discussions

4.1 Surface roughness analysis

The microscopic morphologies of substrates after magnetic grinding are shown in Figure 4. It can be seen that the surface roughness value of substrate 8# (Figure 4(h)) is 4.634 μm, which is the minimum value. The surface roughness value of substrate 13# (Figure 4(m)) is 7.526 μm, which is the maximum value. From the perspective of the fluctuation range of the surface roughness value, the fluctuation range of the surface roughness value of substrate 8# is the smallest in the range of −20.069 to 8.235 μm; in contrast, the fluctuation range of the surface roughness value of substrate 6# is the largest in the range of −61.793 to 7.625 μm; it can also be seen that substrates with smaller surface roughness values are 1#, 4#, 7#, 8#, and the fluctuation range of their surface roughness values is small, all fluctuating around −25 to 18 μm. Substrates with larger surface roughness values are 5#, 10#, 13#, 14#, 15#, and their fluctuation range is more extensive, fluctuating around −34–38 μm. Surface roughness values of substrate 2#, substrate 3#, substrate 6#, substrate 9#, substrate 11#, substrate 12#, and substrate 16# are neither too large nor too small; the fluctuation range is quite different. The surface quality of ground substrate 8# is the best, and its fluctuation range is the smallest under the grinding conditions that the speed of tube is 105 rpm, magnetic induction intensity is 59.12 mT, and mass ratio of micron and submicron magnetic particles is 2.3.

Figure 4 
                  Microscopic morphologies of substrates after magnetic grinding: (a) substrate 1#; (b) substrate 2#; (c) substrate 3#; (d) substrate 4#; (e) substrate 5#; (f) substrate 6#; (g) substrate 7#; (h) substrate 8#; (i) substrate 9#; (j) substrate 10#; (k) substrate 11#; (l) substrate 12#; (m) substrate 13#; (n) substrate 14#; (o) substrate 15#; (p) substrate 16#.
Figure 4

Microscopic morphologies of substrates after magnetic grinding: (a) substrate 1#; (b) substrate 2#; (c) substrate 3#; (d) substrate 4#; (e) substrate 5#; (f) substrate 6#; (g) substrate 7#; (h) substrate 8#; (i) substrate 9#; (j) substrate 10#; (k) substrate 11#; (l) substrate 12#; (m) substrate 13#; (n) substrate 14#; (o) substrate 15#; (p) substrate 16#.

The surface roughness effect curve is used to intuitively express the influence of key parameters on the ground surface roughness, as shown in Figure 5. It can be seen from Figure 5 that the surface roughness of the tube wall increases with the increase in speed of the tube because the grinding pressure of magnetic abrasives on the tube wall increases with the increase of speed of the tube, and finally, the scraping effect of magnetic abrasives is enhanced, the rougher cutting lines are left on the substrate surface while removing the convex and concave layers, so the surface roughness of the tube wall increases accordingly; the surface roughness is the minimum at 105 rpm. It can also be seen that the surface roughness of the tube wall decreases with the increase of magnetic induction intensity because the grinding pressure of magnetic abrasives increases with the increase of magnetic induction intensity, and finally grinding ability of magnetic abrasives is enhanced. However, an increase of low magnetic induction intensity will not produce excessive grinding pressure which will cause serious scratches on the tube wall, so the surface roughness of the tube wall decreases with the increase of magnetic induction intensity; the surface roughness is the minimum at 96.07 mT. In addition, it can also be seen that the surface roughness of the tube wall decreases first and then increases with the increase of the mass ratio of micron and submicron magnetic particles; the reason is that the increase of the mass ratio is equivalent to the increase of the number of larger-size magnetic particles, so grinding pressure of magnetic abrasives on tube wall increases under the effect of the magnetic field, and finally grinding ability of magnetic particles is enhanced, so the surface roughness shows a downward trend, but the scraping effect of magnetic abrasives on tube wall is too strong with the further increase of mass ratio, which will cause surface roughness of tube wall to increase. It can be seen that the surface roughness of the tube wall is minimum when the mass ratio of micron and submicron magnetic particles is 2.3.

Figure 5 
                  The surface roughness effect curve.
Figure 5

The surface roughness effect curve.

The surface morphologies of coated sample 2#, coated sample 8#, coated sample 9#, and coated sample 13# are shown in Figure 6. The surface roughness values of the coated samples were compared with that of substrates, respectively; the comparison results are shown in Table 3. The smaller the surface roughness value of the substrate, the smaller the surface roughness value of the corresponding coated sample. It can also be seen that the greater the surface roughness value of the substrate, the more significant the decrease of the surface roughness value of the corresponding coated sample, and the coating effect is better.

Figure 6 
                  Microscopic morphologies of the coated samples: (a) the coated sample 2#; (b) the coated sample 8#; (c) the coated sample 9#; (d) the coated sample 13#.
Figure 6

Microscopic morphologies of the coated samples: (a) the coated sample 2#; (b) the coated sample 8#; (c) the coated sample 9#; (d) the coated sample 13#.

Table 3

Comparison of surface roughness values of inner walls of slender 316L stainless steel tubes before and after coating

Sample Substrate The coated sample Sample Substrate The coated sample
Sq/μm Sq/μm Sq/μm Sq/μm
2# 5.813 4.381 9# 6.778 4.051
8# 4.634 3.758 13# 7.526 6.194

4.2 Morphological analyses in field emission scanning electron microscope

Surface morphologies of substrates obtained under different magnetic grinding conditions are shown in Figure 7. It can be seen from Figure 7 that the surface morphology of substrate 8# (Figure 7(b)) is the flattest compared with other substrates, which means magnetic abrasives have the best grinding effect on substrate 8#; that is, its surface quality is the best under the grinding conditions that speed of tube is 105 rpm, magnetic induction intensity is 59.12 mT, and mass ratio of micron and submicron magnetic particles is 2.3. It can also be seen from Figure 7 that the surface morphology of substrate 13# (Figure 7(d)) is the roughest compared with other substrates, which means magnetic abrasives have the worst grinding effect on substrate 13#; that is, its surface quality is the worst under the grinding conditions that speed of tube is 210 rpm, magnetic induction intensity is 29.06 mT, and mass ratio of micron and submicron magnetic particles is 1.5. The surface quality of substrate 8# is superior to that of substrate 2#, that of substrate 2# is superior to that of substrate 9#, and that of substrate 9# is superior to that of substrate 13# among the four substrates shown in Figure 7.

Figure 7 
                  FESEM photos of surface morphologies of substrates: (a) substrate 2#, (b) substrate 8#, (c) substrate 9#, (d) substrate 13#.
Figure 7

FESEM photos of surface morphologies of substrates: (a) substrate 2#, (b) substrate 8#, (c) substrate 9#, (d) substrate 13#.

The surface morphologies of the coated samples are shown in Figure 8. It can be seen that the coated sample 8# (Figure 8(b)) has the most severe cracks, while the coated sample 2# (Figure 8(a)) and the coated sample 9# (Figure 8(c)) have fewer cracks. The coated sample 13# (Figure 8(d)) has almost no cracks but a large number of holes. The reason is that the surface roughness value of substrate 8# is the smallest, that is 4.634 μm, so the contact area between the coating and substrate 8# is small, which will result in low bonding strength between the coating and the substrate. Therefore, coated sample 8# is prone to cracking during sintering. Surface roughness value of substrate 9# is more considerable, that is 6.778 μm, and the contact area between the coating and substrate 9# is larger, which makes the bond strength between the coating and the substrate significantly stronger; therefore, coated sample 9# rarely cracked after sintering. It can be seen from Table 3 that the surface roughness value of substrate13# is the largest, that is 7.526 μm, and the substrate surface is highly uneven; therefore, dirt and air bubbles can easily remain in concave areas, which will result in incomplete penetration of the slurry into the concave areas, so many holes exist.

Figure 8 
                  FESEM photos of surface morphologies of the coated samples: (a) coated sample 2#, (b) coated sample 8#, (c) coated sample 9#, and (d) coated sample 13#.
Figure 8

FESEM photos of surface morphologies of the coated samples: (a) coated sample 2#, (b) coated sample 8#, (c) coated sample 9#, and (d) coated sample 13#.

The cross-sectional morphologies of the coated samples are shown in Figure 9. It can be seen from Figure 9 that the bottom part of the coated sample 2# (Figure 9(a)) is a porous layer and the top part is a loose layer; the bonding between coating and substrate 2# is poor. Taking point A on the coating surface for spectrogram analysis, it can be seen that the atomic fractions of Zr and Al on the coating surface are low. The structure of coated sample 8# (Figure 9(c)) is loose and accompanied by spalling of the coating; its cross-sectional line scan EDS analysis is shown in Figure 9(d). From Figure 9(e), it can be seen that structure of the coated sample 9# is continuous and compact without defects such as holes, the coating thickness is uniform, the coating surface is flat, and the coating is well bonded with substrate 9#; its cross-sectional line scan EDS analysis is shown in Figure 9(f). It is shown in Figure 9(i) that the content of Cr on the surface of coated sample 9# is lower than that of coated sample 8#, which indirectly indicates that coated sample 9# is compacter, so coated sample 9# can better inhibit diffusion of Cr of the substrate to the coating surface. It can be seen from Figure 9(g) that the structure of coated sample 13# is not only rough and loose but also has a large number of holes, which are caused by the considerable surface roughness value of substrate13#. The spectral analysis of the G point on the surface of coated sample 13# is shown in Figure 9(h), which shows that atomic fractions of Zr and Al on the coating surface are high.

Figure 9 
                  FESEM photos of cross-sectional morphologies and EDS spectra of the coated samples: (a) FESEM photo of coated sample 2#, (b) EDS spectrogram of point A on the surface of coated sample 2#, (c) FESEM photo of coated sample 8#, (d) line scan graph of coated sample 8#, (e) FESEM photo of coated sample 9#, (f) line scan graph of coated sample 9#, (g) FESEM photo of coated sample 13#, (h) EDS spectrogram of point G on the surface of coated sample 13#, and (i) comparative analysis of line scan between coated sample 8# and coated sample 9#.
Figure 9

FESEM photos of cross-sectional morphologies and EDS spectra of the coated samples: (a) FESEM photo of coated sample 2#, (b) EDS spectrogram of point A on the surface of coated sample 2#, (c) FESEM photo of coated sample 8#, (d) line scan graph of coated sample 8#, (e) FESEM photo of coated sample 9#, (f) line scan graph of coated sample 9#, (g) FESEM photo of coated sample 13#, (h) EDS spectrogram of point G on the surface of coated sample 13#, and (i) comparative analysis of line scan between coated sample 8# and coated sample 9#.

4.3 The corrosion resistance analyses

The polarization curves of the substrates and the coated samples in 3.5% NaCl solution are shown in Figure 10. According to the curves shown in Figure 10, self-corrosion potential and corrosion current density of each sample can be calculated as shown in Table 4. It can be seen from Table 4 that the self-corrosion potential of the coated samples is significantly increased compared with the substrate, which indicates that the corrosion resistance of the sample can be greatly improved by coating gradiently with the prepared nano-ZrO2/α-Al2O3 slurry after magnetic grinding. Phosphating the surface of the substrate though resulted in crack-free sol–gel coatings, anodic polarization in NaCl solution revealed that current increases with the increase of potential [50,51]; generally speaking, larger corrosion current density usually means higher corrosion rate and worse corrosion resistance [52], so phosphating only offers limited protection for substrate. In addition, phosphating has serious environmental problems because of containing a large number of heavy metal ions such as phosphorus, zinc, manganese, and nickel that cannot be biodegradable, and its energy consumption is large and use cost is high. Therefore, there are many deficiencies in phosphating to improve the corrosion resistance of the substrate. In literature[53], the generation of iron oxides (Fe2O3/Fe3O4/FeO) on steel surfaces had adversely affected the adhesion of the coating during thermal and plasma sprayed coatings; in addition, thermal spraying will not only cause thermal deformation of the workpiece but also produce many harmful substances. However, in this article, the composition of the substrate will not be changed after magnetic grinding; therefore, the generation of new substances that have adversely affected the adhesion of the coating can be prevented. It can be seen from Table 4 that the self-corrosion potential of the coated sample 9# is the highest, that is −0.016 V. In the relevant research [54], the E corr value of Al2O3 coated stainless steel was −0.06 V, and its I corr value was 45.5 μA/cm2; it can be seen that the I corr value is too large, and obviously, the I corr of the single Al2O3 coating increased by 2 orders of magnitude higher than that of ZrO2/α-Al2O3 gradient coating in this article. In addition, in literature [55], sol–gel Al2O3 coatings on mild steel/plain carbon steel exhibited limited protection to the substrate. The above conclusions indicate that the corrosion resistance of single Al2O3 coating is poor because of a large number of loose structures such as pores caused by its low inherent compactness. The composition of ZrO2/α-Al2O3 gradient coating in this article changes gradiently from inside to outside; that is, the Al2O3 content increases gradually from inside to outside, and the thermal expansion coefficient of the coating is reduced gradually from inside to the outside, thus reducing thermal stress in the coating, making bonding strength stronger between the coating and the substrate, and making the coating has stronger corrosion resistance. Corrosion current density of the coated samples is generally smaller than that of the substrates according to corrosion current density calculation results. The corrosion current density of coated sample 9# is the smallest, that is 0.491 μA/cm2, which shows the lowest corrosion rate and indicates that the corrosion resistance of coated sample 9# is the best. However, the corrosion current density of the coated sample 13# is the highest, that is 1.4 μA/cm2, which indicates that the corrosion rate is the fastest and the corrosion resistance is the worst.

Figure 10 
                  Polarization curves of the substrates and the coated samples in 3.5% NaCl solution.
Figure 10

Polarization curves of the substrates and the coated samples in 3.5% NaCl solution.

Table 4

Electrochemical parameters of the substrates and the coated samples in 3.5% NaCl solution

Sample Self-corrosion Corrosion current Sample Self-corrosion Corrosion current
Potential/V density /(μA/cm2) Potential/V density/(μA/cm2)
substrate 2# −0.300 3.380 the coated sample 2# −0.106 0.881
substrate 8# −0.146 0.817 the coated sample 8# −0.126 0.526
substrate 9# −0.082 0.925 the coated sample 9# −0.016 0.491
substrate 13# −0.272 1.870 the coated sample 13# −0.231 1.400

The cross-sectional morphologies of the substrates and the coated samples after corroding in 3.5% NaCl solution are shown in Figure 11. It can be seen that the substrates are prone to cracks (Figure 11(a)) and holes (Figure 11(e)) after corroding; the corroded surface is rough (Figure 11(h)), and the corrosion is more severe. In comparison, the coated samples after corroding have fewer corrosion defects because of the substrates coated with more corrosion-resistant ZrO2/α-Al2O3 gradient coating. It can also be seen that coated sample 2# (Figure 11(b)), coated sample 8# (Figure 11(d)), and coated sample 13# (Figure 11(i)) after corroding have many dense microholes compared with coated sample 9# (Figure 11(f)), while the coated sample 9# after corroding has few defects. In addition, taking point F on the corroded surface of the coated sample 9# for spectrogram analysis (Figure 11(g)), the result showed that the composition of the corroded coating is similar to that of the coating itself, but accompanied by a small amount of Fe, which indirectly indicates that the coating is relatively compact, the coating is well bonded with substrate 9#, and the coating can protect the substrate.

Figure 11 
                  FESEM photos of the cross-sectional morphologies of the substrates and the coated samples after corroding: (a) substrate 2#, (b) the coated sample 2#, (c) substrate 8#, (d) the coated sample 8#, (e) substrate 9#, (f) the coated sample 9#, (g) EDS spectrogram of point F on the corroded surface of the coated sample 9#, (h) substrate 13#, and (i) the coated sample 13#.
Figure 11

FESEM photos of the cross-sectional morphologies of the substrates and the coated samples after corroding: (a) substrate 2#, (b) the coated sample 2#, (c) substrate 8#, (d) the coated sample 8#, (e) substrate 9#, (f) the coated sample 9#, (g) EDS spectrogram of point F on the corroded surface of the coated sample 9#, (h) substrate 13#, and (i) the coated sample 13#.

5 Conclusion

In this article, the inner wall of a slender 316L stainless steel tube was ground by magnetorheological fluid, and corrosion resistance of substrates and the coated samples in a salt environment was deeply studied. The research results are as follows:

  1. A surface roughness prediction model was constructed by multiple linear regression, and the maximum relative error between the predicted values of the prediction model and the experimental values is 15.6%, which indicates that the prediction accuracy of the prediction model is good and the prediction model can guide the selection of magnetic abrasive grinding process parameters.

  2. According to the surface roughness values of samples after magnetic grinding and the FESEM analysis, the surface roughness value of ground substrate 8# is the smallest, that is 4.634 μm; under the grinding conditions that the speed of tube is 105 rpm, magnetic induction intensity is 59.12 mT, and mass ratio of micron and submicron magnetic particles is 2.3.

  3. It can be obtained from the surface roughness effect curve that the surface roughness of the tube wall increases with the increase of speed of the tube, decreases with the increase of magnetic induction intensity, and decreases first and then increases with the increase of the mass ratio of micron and submicron magnetic particles.

  4. It can be seen from the cross-sectional morphologies of the coated samples that the structure of the coated sample 9# is continuous and compact, and the coating thickness is uniform, the coating surface is flat, the coating is well bonded with substrate 9#, which indirectly indicate that the substrate ground by magnetorheological fluid is more favorable for bonding with coating under the grinding conditions that speed of tube is 210 rpm, magnetic induction intensity is 40.83 mT, and mass ratio of micron and submicron magnetic particles is 2.3.

  5. It can be obtained from corrosion resistance analysis that the self-corrosion potentials of the coated samples are both significantly increased, and the corrosion current densities of the coated samples are generally reduced, which indicates that the corrosion resistance of the coated samples has been improved. Therein, the self-corrosion potential of coated sample 9# is the highest, that is −0.016 V, and the corrosion current density of the coated sample 9# is the smallest, which is 0.491 μA/cm2, which indicates that the corrosion resistance of the coated sample 9# is the best. The composition of the corroded surface of coated sample 9# is similar to that of the coating itself but accompanied by a small amount of Fe, which indirectly indicates that the coating is relatively compact, the coating is well bonded with substrate 9#, and the coating can protect the substrate.


# Lianzhi Zhang, researching mainly on nontraditional machining on magnetic composite materials.

## Zhangyong Wu, researching mainly on water-based hydraulic transmission technology and electrohydraulic digital control technology.


Acknowledgments

This work was financially supported by the Natural Science Foundation of China (51165012). The Analytical and Testing Centers at Kunming University of Science and Technology is appreciated.

  1. Conflict of interest: The authors declare no conflict of interest.

  2. Data availability statement: All data, models, and code generated or used during the study appear in the published article.

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Received: 2022-10-12
Revised: 2023-01-24
Accepted: 2023-02-01
Published Online: 2023-03-23

© 2023 the author(s), published by De Gruyter

This work is licensed under the Creative Commons Attribution 4.0 International License.

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