E ﬀ ect of Modiﬁed Hexagonal Boron Nitride Nanoparticles on the Emulsion Stability, Viscosity and Electrochemical Behavior of Nanostructured Acrylic Coatings for the Corrosion Protection of AISI 304 Stainless Steel

: In this study, the e ﬀ ect of pure and modiﬁed hexagonal boron nitride (h-BN) nanosheet incorporation on the stability, viscosity, and electrochemical behavior of a waterborne emulsion acrylic coating was studied. The functionalization of h-BN nanoplatelets with polyacrylic acid (PAA) plasma polymerization was performed, and the successful surface modiﬁcation was determined through water dispersion testing, Fourier transform infrared spectroscopy and thermogravimetric analysis, X-ray photoelectron spectroscopy, and also by transmission electronic microscopy. Later, the stability and viscosity properties of emulsion nanostructured acrylic coatings, which were previously prepared by an ultrasound-assisted mixing system, were analyzed using zeta potential and rheometry testing, respectively. The electrochemical behavior was analyzed by electrochemical impedance spectroscopy. The results prove an e ﬀ ective deposition of PAA ﬁlms on the h-BN surfaces, which enhanced the stability and viscosity acrylic of nanostructured coatings due to the interactions between the h-BN nanoplatelets surface and emulsion acrylic paint and also with the thickener additives. On the other hand, the electrochemical analysis demonstrated a signiﬁcant increase (two orders of magnitude) in corrosion resistance in the acrylic nanostructured coatings with 1 wt.% of unmodiﬁed and modiﬁed h-BN nanoplatelets concerning pure acrylic paint due to a barrier protection mechanism of corrosion inhibition. Therefore, the results demonstrate that the surface modiﬁcation of h-BN by plasma polymerization (green technology) helped to solve the low dispersibility issue of BN nanosheet surfaces in a waterborne polymer matrix to obtained green nanostructured acrylic coatings with the right balance in in-can properties and corrosion inhibition of AISI 304 stainless steel.

modification of the nanoparticles can directly affect this interaction, modifying the anticorrosive properties of the nanocomposite coatings.
One of the most promising technologies for the surface modification of nanoparticles has been the plasma polymerization due the fact that it is simple, fast, dry, and free of organic solvents. For example, this technology has been used in our research group for modifying different nanoparticles, such as carbon nanofibers, graphene, clay, copper, and titanium oxide with several monomers (e.g., ethylene, acrylic acid, methyl methacrylate, etc.) [26][27][28][29][30][31][32], to mainly improve the dispersion and compatibility between the nanoparticles and a polymer matrix.
Therefore, the main aim of this study is to understand the effect of surface modification of hexagonal boron nitride (h-BN), by the solvent-free plasma polymerization (green technology), on the stability and viscosity of waterborne acrylic coating (green coating) and its posterior influence on its corrosion protection efficiency and mechanism on 304 stainless steel substrates. The surface modification of nanoparticles was analyzed by Fourier transform infrared spectroscopy (FTIR), thermogravimetric analysis (TGA), X-ray photoelectron spectroscopy (XPS), and transmission electron microscopy (TEM), while the aqueous coatings were characterized by zeta potential and apparent viscosity behavior. The electrochemical behavior of the acrylic nanostructured coatings deposited on 304 stainless steel substrates was studied using electrochemical impedance spectroscopy (EIS).

Materials
In the present study, h-BN nanoplatelets with a purity of 99%, an average size of 70 nm and a density of 2.29 g/cm 3 were purchased from Lower Friction (M. K. Impex, Mississauga, ON, Canada). Acrylic acid (AA) monomer with a purity of 99% and an Mw of 77.02 kg/mol was acquired from Sigma-Aldrich (St Louis, MO, USA), a commercial water-based acrylic resin with a density of 1.02-1.04 g/cm 3 and pH 8-10 was purchase from Berel (Santa Catarina, Nuevo Leon, Mexico) and a surfactant Eumulgin W-1000 was purchased from Henkel Mexicana (Huixquilucan, Estado de Mexico, Mexico). The substrates used for the purpose of coating were 304 stainless steel (SS-304) with the next chemical composition (C: 0.06%, Cr: 17.87%, Ni: 7.70%, Mn: 1.05%, Cu: 0.20%, Si: 0.035%, N: 0.045%, P: 0.025% and S: 0.001%) and were cut to a dimension of 50 mm × 50 mm × 1 mm and 25 mm × 25 mm × 1 mm for corrosion studies and mechanical tests, respectively.

Surface Modification of Nanoparticles
The surface modification process was carried out into a plasma reactor, as previously reported [22,25,27]. It consisted mainly of a power controller coupled to a radiofrequency generator of 13.56 MHz, a vacuum pump, a gas flux control valve, and a 250 mL Erlenmeyer flask held over a magnetic stirring rack. The deposition of polyacrylic acid (PAA) onto the h-BN was achieved as follows: 1.1 g of nanoparticles was introduced in the Erlenmeyer flask under vacuum conditions. The initial internal pressure was 30 Pa. AA monomer flow was fixed to maintain a constant pressure of 45 Pa. The h-BN was treated for 30 min with 50 W of plasma power, maintaining a constant agitation during the exposure of the particles to the plasma.
The untreated and plasma-treated nanoparticles were tested for dispersion in water as follows: 1 mg was immersed in 10 mL of solvent and sonicated for 10 min. After a given time, photographs were taken, and the degree of dispersion, which indirectly indicated the degree of the h-BN modification, was established. Infrared spectroscopy by Fourier transform (FTIR) analysis, to determine the functional groups on h-BN after the treatment, was carried out in a Nicolet™ iS™ 5 spectrometer (Thermo Scientific, Madison, WI, USA) using the attenuated total reflectance technique (ATR). The spectra were obtained at 100 scans and a resolution of 4 cm −1 between 400 and 4000 cm −1 with automatic atmosphere suppression. The thermogravimetric analysis (TGA) was used to determine the thermal stability of unmodified and modified nanoparticles, using a thermo-analyzer TA Q500. TGA curves were obtained according to the following conditions: temperature range of 30 to 600 • C, a heating rate of 10 • C/min, and an atmosphere of N 2 . Transmission electron microscopy (TEM) morphology analysis was performed in an equipment model FEI-TITAN 80-300 KV (Thermo Fisher Scientific, Waltham, MA, USA) with a field emission gun microscope. Aiming to understand the chemical interactions produced by the plasma treatment in the nanoparticles, the samples were analyzed by X-ray photoelectron spectroscopy (XPS) in a PHI 5000 Versa Probe II spectrometer (Physical Electronics, Inc., Chanhassen, MN, USA). The analysis consisted of obtaining the spectra in an energy scan of 0-1400 eV to quantify the chemical elements present in the surface; the samples were bombarded by a monochromatic aluminum X-ray source (Al Kα) with an energy of 1486.6 eV.

Preparation of Acrylic Nanostructured Coatings
The formulation procedure of the nanostructured coatings consisted of the incorporation of unmodified and modified nanoparticles into a commercial waterborne acrylic resin, with 0.1 wt.%, 0.5 wt.%, and 1 wt.% of h-BN. As a first step, the nanoparticles were dispersed in a mixture of water and a certain amount of Eumulgin W-1000 surfactant using an ultrasound bath for 10 min; then, this aqueous dispersion was incorporated into the acrylic resin. The mixture was exposed to mechanical agitation for 30 min at 250 rpm. After that, each mixture was stirred in an ultrasound semi-continuous system for 30 min.
The zeta potential is an effective way to evaluate the electrostatic behavior of the system since it indicates changes in the potential of the surface and in the forces of repulsion/attraction between particles. This potential value was determined in a Microtrac Zeta-Check potential analyzer (Microtrac-MRB, Osaka, Japan) that has a cylindrical polytetrafluoroethylene (PTFE) beaker with a capacity of 1-10 mL and an oscillating displacement piston to agitate and push the sample towards the electrodes and thus determine the level of electrostatic repulsion between the particles. The viscosity behavior of the formulations was studied in an Physica MCR-501 oscillating rheometer (Anton Paar, Graz, Austria) with a cone-plate measurement system of 50 mm diameter and a 2 • angle, the choice of geometry was based on the viscosity of the sample. All measurements were carried out at shear rates of 0.001 to 1000 s −1 at a temperature of 25 ± 0.05 • C with 20 measurements every 10 s.

Substrate Preparation and Deposition
The steel substrates were polished with silicon carbide abrasive paper (SiC), cleaned in an ultrasound bath with deionized water, degreased with ethanol and acetone, and dried for further use. Subsequently, the coatings were deposited by spray coating. In this procedure, the substrates were sprayed with a high-volume low pressure (HVLP) spray gun with the prepared formulations and dried in an oven at a temperature of 50 • C for 30 min. This process was repeated again to generate a dry film of homogeneous coating with a thickness of 70 ± 10 µm.
The electrochemical measurements were carried out in a conventional three-electrode flat cell using an Autolab PGSTAT204 electrochemical system (Metrohm, Herisau, Switzerland) to evaluate the corrosion behavior of the coatings. The coated 304-SS was used as a working electrode, and the test cell included an Ag/AgCl reference electrode and a 316 stainless steel auxiliary electrode. The samples were immersed in 3.5 wt.% NaCl solution for 2 h to establish a steady open circuit potential (OCP) before the measurements. Electrochemical impedance tests were performed at the OCP over a frequency range of 100 kHz and 100 mHz, with applied 10 mV sinusoidal perturbations. NOVA 2.1 software was used for analyzing the EIS results.  Figure 1 shows the comparison of the dispersion stability of unmodified (h-BN) and plasma-modified (mh-BN) nanoparticles at different times of storage in water. It could be seen that after the sonication of nanoparticles, both samples were suspended in the aqueous solution, despite being a hydrophobic material. This behavior is due to the exfoliation of h-BN sheets, basically by the hydrolysis during sonication, which provides the capacity to be dispersed in water, even without any surfactant or organic functionalization [33,34]. On the other hand, after standing for 168 h, the agglomerates and precipitation of the dispersion of h-BN could be found, whereas the dispersion of mh-BN was stable, and no visible precipitation was observed. This behavior was attributed to the hydroxyl and carbonyl functional groups corresponding to PAA that were deposited on the surface of the particles and resulting in a better interaction with water molecules.

Surface Modification of h-BN Nanoparticles with Plasma Functionalization
Coatings 2020, 9, x FOR PEER REVIEW 5 of 17 surfactant or organic functionalization [33,34]. On the other hand, after standing for 168 h, the agglomerates and precipitation of the dispersion of h-BN could be found, whereas the dispersion of mh-BN was stable, and no visible precipitation was observed. This behavior was attributed to the hydroxyl and carbonyl functional groups corresponding to PAA that were deposited on the surface of the particles and resulting in a better interaction with water molecules. The results of the FTIR analysis of unmodified and plasma-modified h-BN are shown in Figure  2. The spectra for both samples presented two strong characteristic peaks located at 1370 and 776 cm −1 . The peak at 1370 cm −1 has been assigned to the in-plane B-N stretching vibration of the sp 2bonded h-BN, while the one at 776 cm −1 is associated with the B-N-B out-of-plane bending vibrations [35][36][37]. In the case of mh-BN, spectra showed the presence of two additional signals at 1712 and 2800-3000 cm −1 , which were attributed to stretching vibrations of C=O and CH2/CH groups related to PAA, respectively [30,38].
The thermal decomposition behavior of the organic film deposited by plasma was measured through the weight loss, as depicted in Figure 3. The thermogram of h-BN suggested a typical thermal decomposition behavior and a marginal weight loss of 0.49 wt.% at a temperature of 600 °C, attributable to the loss of humidity. mh-BN showed a weight loss of 3.84 wt.%, which was associated with the decomposition (chain scission reaction of the PAA chains and the degradation of the PAA chains into monomers) of the organic film deposited on the surface of h-BN [38][39][40]. The results of the FTIR analysis of unmodified and plasma-modified h-BN are shown in Figure 2. The spectra for both samples presented two strong characteristic peaks located at 1370 and 776 cm −1 . The peak at 1370 cm −1 has been assigned to the in-plane B-N stretching vibration of the sp 2 -bonded h-BN, while the one at 776 cm −1 is associated with the B-N-B out-of-plane bending vibrations [35][36][37]. In the case of mh-BN, spectra showed the presence of two additional signals at 1712 and 2800-3000 cm −1 , which were attributed to stretching vibrations of C=O and CH 2 /CH groups related to PAA, respectively [30,38].
Coatings 2020, 9, x FOR PEER REVIEW 5 of 17 surfactant or organic functionalization [33,34]. On the other hand, after standing for 168 h, the agglomerates and precipitation of the dispersion of h-BN could be found, whereas the dispersion of mh-BN was stable, and no visible precipitation was observed. This behavior was attributed to the hydroxyl and carbonyl functional groups corresponding to PAA that were deposited on the surface of the particles and resulting in a better interaction with water molecules. The results of the FTIR analysis of unmodified and plasma-modified h-BN are shown in Figure  2. The spectra for both samples presented two strong characteristic peaks located at 1370 and 776 cm −1 . The peak at 1370 cm −1 has been assigned to the in-plane B-N stretching vibration of the sp 2bonded h-BN, while the one at 776 cm −1 is associated with the B-N-B out-of-plane bending vibrations [35][36][37]. In the case of mh-BN, spectra showed the presence of two additional signals at 1712 and 2800-3000 cm −1 , which were attributed to stretching vibrations of C=O and CH2/CH groups related to PAA, respectively [30,38].
The thermal decomposition behavior of the organic film deposited by plasma was measured through the weight loss, as depicted in Figure 3. The thermogram of h-BN suggested a typical thermal decomposition behavior and a marginal weight loss of 0.49 wt.% at a temperature of 600 °C, attributable to the loss of humidity. mh-BN showed a weight loss of 3.84 wt.%, which was associated with the decomposition (chain scission reaction of the PAA chains and the degradation of the PAA chains into monomers) of the organic film deposited on the surface of h-BN [38][39][40].   The thermal decomposition behavior of the organic film deposited by plasma was measured through the weight loss, as depicted in Figure 3. The thermogram of h-BN suggested a typical thermal decomposition behavior and a marginal weight loss of 0.49 wt.% at a temperature of 600 • C, attributable to the loss of humidity. mh-BN showed a weight loss of 3.84 wt.%, which was associated with the decomposition (chain scission reaction of the PAA chains and the degradation of the PAA chains into monomers) of the organic film deposited on the surface of h-BN [38][39][40].
Coatings 2020, 9, x FOR PEER REVIEW 6 of 17 The high-resolution transmission electron microscopy (HR-TEM) images shown in Figure 4 correspond to unmodified and plasma-modified nanoparticles. Figure 4a presents the micrograph of h-BN, where the nanoparticle shows an irregular surface, possibly due to its synthesis method. In Figure 4b the micrograph of mh-BN is shown, where a thin surface layer can be noticed on the edge of h-BN50, which corresponds to a thin polyacrylic acid layer deposited via plasma treatment. The thickness of this heterogeneous superficial nanolayer was less than 5 nm. Furthermore, XPS was used to investigate the chemical surface of unmodified and plasmamodified nanoparticles. Figure 5a shows the XPS survey spectrums obtained for both samples, which consisted mainly of nitrogen (N 1s), boron (B 1s), oxygen (O 1s) and carbon (C 1s), with peaks corresponding to bonding energies of 398.5, 190.8, 284.8, 534.9 eV, respectively. These values are consistent with the values reported for h-BN [41,42]. The additional oxygen and carbon from h-BN could result from the exposure of nanoparticles to air before the XPS measurement, while for h-BN50 the intensity of these peaks was increased due to the plasma polyacrylic acid deposited during the treatment. The high-resolution transmission electron microscopy (HR-TEM) images shown in Figure 4 correspond to unmodified and plasma-modified nanoparticles. Figure 4a presents the micrograph of h-BN, where the nanoparticle shows an irregular surface, possibly due to its synthesis method. In Figure 4b the micrograph of mh-BN is shown, where a thin surface layer can be noticed on the edge of h-BN50, which corresponds to a thin polyacrylic acid layer deposited via plasma treatment. The thickness of this heterogeneous superficial nanolayer was less than 5 nm. The high-resolution transmission electron microscopy (HR-TEM) images shown in Figure 4 correspond to unmodified and plasma-modified nanoparticles. Figure 4a presents the micrograph of h-BN, where the nanoparticle shows an irregular surface, possibly due to its synthesis method. In Figure 4b the micrograph of mh-BN is shown, where a thin surface layer can be noticed on the edge of h-BN50, which corresponds to a thin polyacrylic acid layer deposited via plasma treatment. The thickness of this heterogeneous superficial nanolayer was less than 5 nm. Furthermore, XPS was used to investigate the chemical surface of unmodified and plasmamodified nanoparticles. Figure 5a shows the XPS survey spectrums obtained for both samples, which consisted mainly of nitrogen (N 1s), boron (B 1s), oxygen (O 1s) and carbon (C 1s), with peaks corresponding to bonding energies of 398.5, 190.8, 284.8, 534.9 eV, respectively. These values are consistent with the values reported for h-BN [41,42]. The additional oxygen and carbon from h-BN could result from the exposure of nanoparticles to air before the XPS measurement, while for h-BN50 the intensity of these peaks was increased due to the plasma polyacrylic acid deposited during the treatment. Furthermore, XPS was used to investigate the chemical surface of unmodified and plasma-modified nanoparticles. Figure 5a shows the XPS survey spectrums obtained for both samples, which consisted mainly of nitrogen (N 1s), boron (B 1s), oxygen (O 1s) and carbon (C 1s), with peaks corresponding to bonding energies of 398.5, 190.8, 284.8, 534.9 eV, respectively. These values are consistent with the values reported for h-BN [41,42]. The additional oxygen and carbon from h-BN could result from the exposure of nanoparticles to air before the XPS measurement, while for h-BN50 the intensity of these peaks was increased due to the plasma polyacrylic acid deposited during the treatment.     [43][44][45][46][47].
On the other hand, Figure 5d shows the B 1s spectrum of h-BN50, where the signals of B-N and B-O are appreciated detected and a new one at 191.9 eV associated with the B-C bond, where the carbon comes from the PAA coating. During plasma treatment, the reactive species (electrons, free radical ions, etc.) of the plasma attack the surface of the nanoparticles by breaking the B-N bonds to increase B-O and form B-C bindings [43,48]. Figure

Effect of h-BN Surface Modification on Acrylic Resin Stability and Rheological Behavior
Zeta potential or Z potential measurements are a good quantitative measure to determine the stability level of acrylic resin at different concentrations of untreated and plasma-treated nanoparticles [52]. The results are shown in Table 2. Regarding the values of the zeta potential, it has been reported that values >30 mV indicate very stable positive micelles and that values <−30 mV correspond to stable values of micelles [53]. According to the zeta potential data obtained at pH = 8, the coating formulations had negative micelles in all cases. The acrylic resin showed the highest value of Z potential (−216.8 mV) due to the charges coming from the anionic stabilization of acrylic resin, which indicates its high degree of dispersion among their micelles. However, the Z potential values of the formulations with untreated nanoparticles (h-BNx) presented a considerable decrease with respect to acrylic resin (e.g., the h-BN0.1 sample presented a value of −73.5 mV), indicating that the particles disturbed the micelles of the acrylic resin due to a weak attraction between the nanoplatelet clusters and the micellar systems. Conversely, the potential values of the formulations with plasma-treated nanoparticles (mh-BNx) presented a slight decrease with respect to acrylic resin due to a low but better attraction with the acrylic resin emulsion, reveling the existence of greater compatibility between the h-BN50 nanoparticles with the acrylic resin micelles due to their modification with acrylic acid plasma.
In Figure 6, a scheme about the possible interactions between negative micelles of the pure latex particle is shown, with unmodified (positive charged) and modified (negative charged) h-BN nanoplatelet clusters. In Figure 6a, it can be appreciated that the positive counter-ions first wrap to the negatively charged micelle, forming the Stern layer. The micelle continues to attract more counter-ions, which could be repelled by neighbored counter-ions (diffuse layer), and by the Stern layer itself [54]. Both layers have been referred to as the double layer. The slip plane is developed where the Stern layer and diffuse layer join. The electrical potential at this point is named the zeta potential. Basically, at a higher absolute value of the zeta potential, the dispersion is more stable (particles are repelling each other). In accordance with the zeta potential value, these micelles had a highly repulsive behavior that allows the high stability of the paint. Figure 6b,c corresponds to the emulsion with mh-BN and h-BN nanoplatelets, respectively. In the case of mh-BN, the micelles had a low attraction between itself, while the h-BN had a weak attraction. Therefore, the micelles with h-BN were modified to allow for better stability between them and correspond with the zeta potential values obtained in all the concentrations.

Effect of h-BN Surface Modification on Viscosity Behavior
The coatings and emulsions require a complex rheology, in which the viscosity depends on the wide range of shear rate to which they are exposed during its manipulation [55]. The effect of concentration of unmodified (h-BN) and plasma-modified (mh-BN) nanoplatelets on the apparent viscosity of the acrylic resin is shown in Figure 7a. The viscosity profiles of the acrylic resin and the formulations with nanoparticles exhibited a rheological behavior of pseudoplastic type in which the viscosity value decreased as the shear rate increased [56]. The first step consisted of a constant viscosity at a low shear rate, known as the "first Newtonian plateau", followed by a drop-in viscosity due to the shear rate exceeding the molecular relaxation of the crosslinked chains so that the viscosity was reduced. There was also a stable low viscosity at a high shear rate; this is known as the "second Newtonian plateau", due to the Brownian movement that tries to give the original conformation to the acrylic resin molecules, but, as the shear rate continues to increase, these forces that were overcome again and continued the decrease in viscosity [56,57]. In the case of h-BNx and mh-BNx formulations, these samples presented a decrease in the viscosity behavior respect to the acrylic resin.
repelling each other). In accordance with the zeta potential value, these micelles had a highly repulsive behavior that allows the high stability of the paint. Figure 6b,c corresponds to the emulsion with mh-BN and h-BN nanoplatelets, respectively. In the case of mh-BN, the micelles had a low attraction between itself, while the h-BN had a weak attraction. Therefore, the micelles with h-BN were modified to allow for better stability between them and correspond with the zeta potential values obtained in all the concentrations.

Effect of h-BN Surface Modification on Viscosity Behavior
The coatings and emulsions require a complex rheology, in which the viscosity depends on the wide range of shear rate to which they are exposed during its manipulation [55]. The effect of concentration of unmodified (h-BN) and plasma-modified (mh-BN) nanoplatelets on the apparent viscosity of the acrylic resin is shown in Figure 7a. The viscosity profiles of the acrylic resin and the formulations with nanoparticles exhibited a rheological behavior of pseudoplastic type in which the viscosity value decreased as the shear rate increased [56]. The first step consisted of a constant viscosity at a low shear rate, known as the "first Newtonian plateau", followed by a drop-in viscosity due to the shear rate exceeding the molecular relaxation of the crosslinked chains so that the viscosity was reduced. There was also a stable low viscosity at a high shear rate; this is known as the "second Newtonian plateau", due to the Brownian movement that tries to give the original conformation to the acrylic resin molecules, but, as the shear rate continues to increase, these forces that were overcome again and continued the decrease in viscosity [56,57]. In the case of h-BNx and mh-BNx formulations, these samples presented a decrease in the viscosity behavior respect to the acrylic resin. In contrast, the formulations h-BNx manifested a pronounced drop in viscosity from low to high shear rate than formulations mh-BNx. It is inferred that this behavior was due to the interruption of the weak intermolecular unions existing mainly between the unmodified nanoplatelets with the micelles of acrylic resin with the increase of the shear rate [58]. This result indicates that the modification by plasma offer to the h-BN particles better compatibility with the acrylic resin molecules and in turn improve the in-can properties.
An essential aspect to take into consideration, due to the constant growth of the market of high specialty coatings, is the degree of compatibility that exists between the different additives that structure the coatings, mainly when nanometric additives are used. [59]. Figure 7b shows a scheme with the interaction of unmodified and modified h-BN nanoplatelets with the latex and the thickening of acrylic paint. In the case of Figure 7bi, it can be appreciated that the latex is surrounded In contrast, the formulations h-BNx manifested a pronounced drop in viscosity from low to high shear rate than formulations mh-BNx. It is inferred that this behavior was due to the interruption of the weak intermolecular unions existing mainly between the unmodified nanoplatelets with the micelles of acrylic resin with the increase of the shear rate [58]. This result indicates that the modification by plasma offer to the h-BN particles better compatibility with the acrylic resin molecules and in turn improve the in-can properties.
An essential aspect to take into consideration, due to the constant growth of the market of high specialty coatings, is the degree of compatibility that exists between the different additives that structure the coatings, mainly when nanometric additives are used. [59]. Figure 7b shows a scheme with the interaction of unmodified and modified h-BN nanoplatelets with the latex and the thickening of acrylic paint. In the case of Figure 7bi, it can be appreciated that the latex is surrounded by associative thickening, which consists of a water-soluble polymer backbone that contains two or more hydrophobic groups that warranty an excellent control of the rheology and simplify the handling and the application of the coating [59,60]. In Figure 7bii,iii, it can be observed when nanoparticles are incorporated into the resin; the thickening molecules were displaced from the latex surface caused by the hydrophobic nature of the h-BN. In the case of the incorporation of mh-BN, the viscosity behavior might be due to the hydrophilic surface of these particles holding weakly interactions with the hydrophobic groups of the thickening molecules. In summary, the interactions between the latex and the h-BN can be improved by the plasma modification, which could provide a repulsion of the micelles to keep the stability on the emulsion. Figure 8 shows the results of the impedance measurements. Figure 8a presents the Nyquist diagram for the 304-SS and the coating with the acrylic resin. In the case of 304-SS, a characteristic curve line for this type of steel is presented [61], while the acrylic resin presented two semicircles with different diameters. This behavior indicates the existence of two-time constants [62]. On the other hand, Figure 8b shows the Nyquist diagrams of nanostructured coatings with only a semicircle with different diameters. In Figure 8c, the results of the Bode-impedance show, and it is observed that 304-SS in the whole frequency range has the lowest impedance value. In the case of coatings with h-BN without treatment, it is observed that their impedance at low frequencies is slightly higher than coatings with modified nanoparticles.

Anticorrosive Performance of Acrylic/h-BN Coatings
Coatings 2020, 9, x FOR PEER REVIEW 11 of 17 interactions with the hydrophobic groups of the thickening molecules. In summary, the interactions between the latex and the h-BN can be improved by the plasma modification, which could provide a repulsion of the micelles to keep the stability on the emulsion. Figure 8 shows the results of the impedance measurements. Figure 8a presents the Nyquist diagram for the 304-SS and the coating with the acrylic resin. In the case of 304-SS, a characteristic curve line for this type of steel is presented [61], while the acrylic resin presented two semicircles with different diameters. This behavior indicates the existence of two-time constants [62]. On the other hand, Figure 8b shows the Nyquist diagrams of nanostructured coatings with only a semicircle with different diameters. In Figure 8c, the results of the Bode-impedance show, and it is observed that 304-SS in the whole frequency range has the lowest impedance value. In the case of coatings with h-BN without treatment, it is observed that their impedance at low frequencies is slightly higher than coatings with modified nanoparticles.

Anticorrosive Performance of Acrylic/h-BN Coatings
The resulting Bode-phase angle is shown in Figure 8d. It is observed that 304-SS exhibits resistive behavior at high frequencies and capacitive behavior at low frequencies. While the acrylic resin sample, showed a phase angle behavior with two-time constants, in similar form to Nyquist diagram. The appearance of two-time constants suggests that the electrolyte penetrated through the coating and reached the metal substrate, initiating the corrosion reaction of the steel. The time constant at a high-frequency range represents the characteristics of corrosion resistance or barrier properties of the coating, and the time constant at low frequencies corresponds to the properties of the coating-metal interface, that is, the controlled diffusion of the corrosion reaction [62,63].
On the contrary, all nanostructured coatings presented only a time constant, which indicates that the barrier property is improved by incorporating any of these nanoparticle systems. It was observed that for pure and modified nanoparticle coatings had the highest impedance value at low frequencies compared to acrylic resin and presented phase angles close to 90° in the region of high frequencies with a time constant, which represents an excellent barrier property of the coating at an initial time of immersion. It should be noted that when the concentration of the nanoparticles embedded in the acrylic resin decreased, the properties of resistance to load transfer of the coatings decreased. The resulting Bode-phase angle is shown in Figure 8d. It is observed that 304-SS exhibits resistive behavior at high frequencies and capacitive behavior at low frequencies. While the acrylic resin sample, showed a phase angle behavior with two-time constants, in similar form to Nyquist diagram. The appearance of two-time constants suggests that the electrolyte penetrated through the coating and reached the metal substrate, initiating the corrosion reaction of the steel. The time constant at a high-frequency range represents the characteristics of corrosion resistance or barrier properties of the coating, and the time constant at low frequencies corresponds to the properties of the coating-metal interface, that is, the controlled diffusion of the corrosion reaction [62,63].
On the contrary, all nanostructured coatings presented only a time constant, which indicates that the barrier property is improved by incorporating any of these nanoparticle systems. It was observed that for pure and modified nanoparticle coatings had the highest impedance value at low frequencies compared to acrylic resin and presented phase angles close to 90 • in the region of high frequencies with a time constant, which represents an excellent barrier property of the coating at an initial time of immersion. It should be noted that when the concentration of the nanoparticles embedded in the acrylic resin decreased, the properties of resistance to load transfer of the coatings decreased. Table 3 shows the results of the impedance |Z| at a low frequency that reflects the corrosive process. The impedance |Z| of all the resins is higher than the SS-304, implying a proper protection of the steel. Moreover, we can see that when increasing the h-BN content, the impedance |Z| value increases when it is not treated with plasma. The equivalent circuits, as shown in Figure 9, were used to fit the EIS results of bare SS-304, the acrylic coating (two-time constants), and nanostructured coatings (one-time constants), respectively [21,25,64]. In the equivalent circuits, R s was the resistance of solution, for SS-304 R st was the resistance of metal characteristics, and Q st means the constant phase element used to simulate the capacitive response. For all the coated SS-304 samples, R 1 was the resistance of the coating, Q 1 was the double electrode layer capacitance of coating, R 2 was the charge transfer resistance of corrosion electrochemical reaction in the metal/coating interface, Q 2 was the double electrode layer capacitance in the interface and W was the impedance of Warburg associated to the diffusion phenomena of ions from the solution through the coating.
Experimental data were compared with the model, and the results are shown in Table 4, showing a good correlation between the fit to the measured data, despite the approximations made. The impedance elements of the acrylic coating suggest that the electrochemical processes might be controlled by the active species diffusing to the metal surface of corrosion products diffusing away from the metal surface through the coating film. In contrast, the acrylic/h-BN coatings maintain their high capacitive behavior. For the solution resistance, it decreases with the presence of all the coatings, mainly when the acrylic coating contained 1% of h-BN, which suggested that the coating has high superficial defects. The coating resistance (R 1 ) is an important parameter that shows an increase with the content of h-BN, which results in the positive effect of these nanoparticles to incorporate into the acrylic resin. These high values of resistances show that the coating provided adequate corrosion protection. In general, when the electrolyte permeates the polymer film, Q 1 may be observed to increase, which is related to an increase in dielectric constant ε, due to the increased water absorption. For W exhibits an increase while the h-BN nanoplatelets concentration increased being even higher for the modified nanoparticles, indicating that the diffusion influence of corrosive electrolyte was lower at the highest content (i.e., 1.0 wt.%) of h-BN (9.30 × 10 7 Ω/s (1/2) ) and mh-BN (5.32 × 10 8 Ω/s (1/2) ) [64][65][66]. Similar impedance spectroscopy results were recently reported for plasma-treated boron nitride nanoflakes as barriers to enhance anticorrosion of acrylic coating on steel [67], where the authors observed that the plasma modification of h-BN nanoflakes with Ar + NH 3 enhanced the corrosion resistance of acrylic coatings, resulting in an even a lower corrosion current density (I corr ) value than pristine h-BN. This behavior was because plasma treatment can enlarge the interlayer distance and increase the formation of NH/OH groups on the h-BN surface, enhancing the storage of Fe 2+ ion and preventing its migration and the subsequent formation of Fe 2 O 3 .

SS-304
3.86 × 10 4 Resin 8.40 × 10 6 h-BN0. 1 1.00 × 10 8 h-BN0. 5 7.49 × 10 8 h-BN1 1.52 × 10 9 mh-BN0. 1 7.55 × 10 5 mh-BN0. 5 1.39 × 10 7 mh-BN1 5.75 × 10 8 The equivalent circuits, as shown in Figure 9, were used to fit the EIS results of bare SS-304, the acrylic coating (two-time constants), and nanostructured coatings (one-time constants), respectively [21,25,64]. In the equivalent circuits, Rs was the resistance of solution, for SS-304 Rst was the resistance of metal characteristics, and Qst means the constant phase element used to simulate the capacitive response. For all the coated SS-304 samples, R1 was the resistance of the coating, Q1 was the double electrode layer capacitance of coating, R2 was the charge transfer resistance of corrosion electrochemical reaction in the metal/coating interface, Q2 was the double electrode layer capacitance in the interface and W was the impedance of Warburg associated to the diffusion phenomena of ions from the solution through the coating. Experimental data were compared with the model, and the results are shown in Table 4, showing a good correlation between the fit to the measured data, despite the approximations made. The impedance elements of the acrylic coating suggest that the electrochemical processes might be controlled by the active species diffusing to the metal surface of corrosion products diffusing away from the metal surface through the coating film. In contrast, the acrylic/h-BN coatings maintain their high capacitive behavior. For the solution resistance, it decreases with the presence of all the coatings, mainly when the acrylic coating contained 1% of h-BN, which suggested that the coating has high superficial defects. The coating resistance (R1) is an important parameter that shows an increase with   Additionally, the corrosion rate results (Table S1) corroborated the significant increase in the corrosion resistance of SS-304 (1.42 × 10 −4 mm/year) coated with the waterborne acrylic nanostructured coatings prepared with 0.5% and 1.0% by the weight of unmodified (h-BN) and plasma-modified (mh-BN) boron nitride nanolayers, in comparison to the pure acrylic coating (1.15 × 10 −6 mm/year) being the highest for the h-BN1 sample (4.48 × 10 −9 mm/year).

Conclusions
In summary, h-BN nanoparticles pure and modified by plasma were used as reinforcement in acrylic matrix composite coatings. This study demonstrates that the plasma modification of the h-BN improves the dispersion and stability of the nanoplatelets, mainly at a concentration of 1% by weight, in the acrylic resin by the formation of a PAA film over the nanoplatelets' surface, which generated electrical interactions to provide the repulsion of the micelles and keep the stability on the emulsion.
Additionally, the electrochemical studies indicate that waterborne acrylic/h-BN nanostructured coatings acted as an excellent corrosion protection of AISI 304 stainless steel. In particular, the EIS and corrosion rate results suggest that the acrylic coatings with the highest concentration (1% by weight) of pure h-BN could provide the best corrosion inhibition effect for the AISI 304 stainless steel, although the electrochemical behavior of acrylic/mh-BN nanostructured coatings, with the same nanoplatelet concentration, suggests a similar corrosion inhibition grade. Therefore, it was demonstrated that the surface modification of h-BN by plasma polymerization helped to obtained green nanostructured acrylic coatings with the right balance in in-can properties and as a barrier protection coating for the corrosion inhibition of AISI 304 stainless steel.