# Electrochemical and Oxidation Behavior of Yttria Stabilized Zirconia Coating on Zircaloy-4 Synthesized via Sol-Gel Process

Authors: S. Rezaee; Gh. R. Rashed; M. A. Golozar
Journal: International Journal of Corrosion
 (2013)

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## Abstract

Sol-gel 8 wt.% Yttria Stabilized Zirconia (YSZ) thin films were prepared on zirconium (zircaloy-4 alloy) by dip-coating technique followed by heat treating at various temperatures (200°C, 400°C, and 700°C) in order to improve both electrochemical corrosion and high temperature oxidation properties of the substrate. Differential thermal analysis and thermogravimetric analysis (DTA-TG) revealed the coating formation process. X-ray diffraction (XRD) was used to determine the crystalline phase structure transformation. The morphological characterization of the coatings was carried out using scanning electron microscopy (SEM). The electrochemical behavior of the coated and uncoated samples was investigated by means of open circuit potential, Tafel, and electrochemical impedance spectroscopy (EIS) in a 3.5 wt.% NaCl solution. The homogeneity and surface appearance of coatings produced was affected by the heat treatment temperature. According to the corrosion parameters, the YSZ coatings showed a considerable increase in the corrosion resistance, especially at higher heat treatment temperatures. The coating with the best quality, from the surface and corrosion point of view, was subjected to oxidation test in air at 800°C. The coated sample presented a 25% reduction in oxidation rate in comparison with bare substrate.


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## Body

## 1. Introduction

Because of many excellent bulk properties like low thermal neutron capture cross section, favorable mechanical properties and good corrosion resistance even at high temperatures, zirconium and its alloys are widely used in nuclear reactors as fuel cladding and as reactor structural elements, chemical engineering, and lately in biomedical applications. For fuel cladding applications, the alloys of choice are zircaloy-2 (Zr-2) and zircaloy-4 (Zr-4). In fuel deep geological repository, used fuel bundles and the associated Zr cladding are encapsulated in durable containers and the containers are sealed in an engineered vault at a depth of hundreds of meters in a stable low permeability rock mass. Ground water composition especially in crystalline and sedimentary rock types contains NaCl. In a failed container, zirconium is in contact with NaCl solution [1–4]. So, they are somehow subject to corrosion and their specific surface properties (e.g., corrosion, oxidation, etc.) should be improved [2, 4].Surface modification of materials permits independent optimization of bulk and surface properties. Among all surface modification techniques such as chemical vapor deposition [5, 6], physical vapor deposition [7], plasma [8], ion implantation [3, 4, 9, 10], and so forth, sol-gel processing has many advantages over other techniques. They include low processing temperature, chemically and physically uniform coatings, high purity, low capital investment, producing thin homogeneous films on large scale, easy controlling of film thickness, and practical in complex geometries effectively [11–14].Many sol-gel derived ceramic thin films like SiO2 [5, 15], ZrO2 [12, 16], CeO2-ZrO2 [17], ZrO2-SiO2 [11], TiO2, TiO2-SiO2 [18], and so forth have been produced on different substrates. Zirconia films have been used widely in recent years because it possesses more efficient anticorrosion ability, thermal protection, optical properties, easier sol preparation, and good erosion resistance accompanied by toughening strength and its close thermal expansion coefficient to many metals and alloys [11, 14, 17]. Yttria Stabilized Zirconia (YSZ) is the most common system because of its high ionic conductivity and thermal stability offering an improvement in adhesion and corrosion resistance properties [19].Cracking the film during drying stage is the main concern of sol-gel derived ceramic coatings. In recent years many researchers have tried to reduce these cracks and therefore changed many variables. López et al. [15] have found that the corrosion resistance is improved with increasing the number of deposited silica layers because they become free of cracks and porosities. Domínguez-Crespo et al. [19], Li et al. [20], and López et al. [15] found that denser and more crack-free zirconia and silica films were formed at higher temperatures because of the removal of organic substances. This also helps to increase the anticorrosive properties of the coatings. Baron and Ruiz [21] concluded that the basic catalysts were more effective in crack-free film production compared with acidic catalysts and denser films were produced in more diluted sols. Ugas-Carrión et al. [22] revealed that, by using an optimum acetylacetone concentration as a complexing agent, the porosities and defects of zirconia coatings could be reduced even at low temperatures. Nouri et al. [23] have studied the structural evolution and electrochemical behavior of sol-gel derived zirconia films on 304 stainless steel substrate. The best performance was obtained at 500°C. At temperatures higher or lower than 500°C, the coatings properties are reduced.Considering the above findings with regard to improve in protection against corrosion and high temperature oxidation, the YSZ coating is applied on top of zircaloy-4. In the present work it is focused on the preparation of the stable 8 wt.% Yttria Stabilized Zirconia sol and sol-gel dip coating using zirconium propoxide/yttrium chloride/acetylacetone/water system and ethanol as a solvent. We describe how Yttria Stabilized Zirconia coating can improve the corrosion and high temperature oxidation resistance of the zircaloy-4 and the effects of different heat treatment temperature on the coating quality and its corrosion rate will be discussed.


## 2. Material and Methods

### 2.1.  Sol and Coating Preparation

Zircaloy-4 samples were cut in the shape of plates of 20 mm × 10 mm surface area from a sheet of 1 mm in thickness. The elemental composition of the zircaloy-4 is represented in Table1. They are subjected to mechanical polishing with sand papers of 120 to 600 grade papers, cleaned in acetone, and then dried under air pressure. Sol of ZrO2-8 wt.% Y2O3 was obtained using zirconium (IV) propoxide (70 wt.% in 1-propanol, Merck), acetylacetone as complexing agent and distilled water in mole ratios of 1 : 1 : 10, respectively. Yttrium (III) chloride (99.99% anhydrous powder) is used as stabilizing agent and ethanol as solvent. The acetylacetone was added to zirconium propoxide to control the reactions; proper quantity of ethanol was well mixed with the previous solution using the magnetic stirrer. Then the precursor solution was added gradually to the proper amount of water while stirring continued. Finally, yttrium (III) chloride was mixed in the solution under continuous stirring. After about 30 minutes a yellow, stable, and transparent precursor sol was obtained. Zirconium concentration in final solution was 0.5 M. No precipitate was observed even after 6 months. The zircaloy-4 substrates were then coated by dip-coating technique with controlled immersion and withdrawal speed of 1 mm·s−1. The immersion time interval was 3 minutes. After each time of three depositions, the coatings were treated up to 200°C with 10°C·min−1, and at last, they were heated up to three different temperatures of 200°C, 400°C, and 700°C and then subjected to thermal annealing at that temperature for 1 hour to remove water and organic compounds.Table 1
Chemical composition of zircaloy-4.
Element
Sn
Fe
Cr
Ni
Zr
wt.%
1.55
0.15
0.1
0.05
Bal.
(Fe + Cr + Ni = 0.3 wt.%).


### 2.2. Characterization

The morphology of the films before electrochemical measurements is studied by Scanning Electron Microscopy (SEM, VEGA, TESCAN-LMU). X-ray diffraction (XRD) (Model Bruker, D8ADVANCE, Germany X-Ray Tube Anode: Cu, Wavelength: 1.5406 Å (CuKα)) was used to determine the chemical composition and the crystalline phase structure transformation of the dried gel powder at 3 different temperatures of 150°C, 400°C, and 700°C. The crystallite size of the films was determined from the half-height width of the XRD peaks using Scherrer’s equation. The process pathway like water or organic substances evaporation and phase transitions were studied by thermal analysis (TG-DTA) (Model L81, 1750, Linseis, Germany) of the samples heated from room temperature to 800°C in air at a heating rate of 10°C·min−1. Open circuit potential (OCP), electrochemical impedance spectroscopy (EIS), and potentiodynamic polarization tests were done to evaluate the effect of YSZ coatings on the corrosion performance of zircaloy-4 substrate in 3.5 wt.% aerated NaCl solution at room temperature. Measurements were done by Autolab device equipped with a computer; Model PGSTAT 302 N. Autolab GPES (general purpose electrochemical system) software was used for evaluating of polarization data in the potential range of ±1.5 V from OCP after the attainment of steady state at OCP conditions after about 30 minutes. The scan rate used was 0.5 mV/s. The standard electrochemical cell was arranged with saturated Ag/AgCl electrode as the reference electrode and platinum as the counter electrode. The exposed area of the samples was 1.8 cm2. Corrosion characteristics such as corrosion potential (Ecorr), corrosion current density (icorr), and anodic/cathodic Tafel slopes (βa and βc) were obtained from the intersection of cathodic and anodic Tafel curve tangents using Tafel extrapolation method. The polarization resistance (Rp) was determined using Stren-Geary equation (see [24]):
(1)Rp=βa·βc2.303icorr(βa+βc).The corrosion rate is calculated using the following equation (see [25]):
(2)rcorr=0.00327icorrMn·d,
where rcorr is corrosion rate in millimeter per year (mpy), n is charge number (4), M is molar mass (91.22 g·mol−1), and d is density of substrate (6.56 g·cm−3).The EIS measurements were carried out with FRA2 frequency response analyzer at open circuit potential after 1 hr immersion time with AC amplitude of 20 mV over a frequency range of 100 kHz to 1 mHz. Coating thickness was determined using SEM image of the cross section of the coated sample. High temperature oxidation resistance of the coating was evaluated by weight gain test.


## 2.1.  Sol and Coating Preparation

Zircaloy-4 samples were cut in the shape of plates of 20 mm × 10 mm surface area from a sheet of 1 mm in thickness. The elemental composition of the zircaloy-4 is represented in Table1. They are subjected to mechanical polishing with sand papers of 120 to 600 grade papers, cleaned in acetone, and then dried under air pressure. Sol of ZrO2-8 wt.% Y2O3 was obtained using zirconium (IV) propoxide (70 wt.% in 1-propanol, Merck), acetylacetone as complexing agent and distilled water in mole ratios of 1 : 1 : 10, respectively. Yttrium (III) chloride (99.99% anhydrous powder) is used as stabilizing agent and ethanol as solvent. The acetylacetone was added to zirconium propoxide to control the reactions; proper quantity of ethanol was well mixed with the previous solution using the magnetic stirrer. Then the precursor solution was added gradually to the proper amount of water while stirring continued. Finally, yttrium (III) chloride was mixed in the solution under continuous stirring. After about 30 minutes a yellow, stable, and transparent precursor sol was obtained. Zirconium concentration in final solution was 0.5 M. No precipitate was observed even after 6 months. The zircaloy-4 substrates were then coated by dip-coating technique with controlled immersion and withdrawal speed of 1 mm·s−1. The immersion time interval was 3 minutes. After each time of three depositions, the coatings were treated up to 200°C with 10°C·min−1, and at last, they were heated up to three different temperatures of 200°C, 400°C, and 700°C and then subjected to thermal annealing at that temperature for 1 hour to remove water and organic compounds.Table 1
Chemical composition of zircaloy-4.
Element
Sn
Fe
Cr
Ni
Zr
wt.%
1.55
0.15
0.1
0.05
Bal.
(Fe + Cr + Ni = 0.3 wt.%).


## 2.2. Characterization

The morphology of the films before electrochemical measurements is studied by Scanning Electron Microscopy (SEM, VEGA, TESCAN-LMU). X-ray diffraction (XRD) (Model Bruker, D8ADVANCE, Germany X-Ray Tube Anode: Cu, Wavelength: 1.5406 Å (CuKα)) was used to determine the chemical composition and the crystalline phase structure transformation of the dried gel powder at 3 different temperatures of 150°C, 400°C, and 700°C. The crystallite size of the films was determined from the half-height width of the XRD peaks using Scherrer’s equation. The process pathway like water or organic substances evaporation and phase transitions were studied by thermal analysis (TG-DTA) (Model L81, 1750, Linseis, Germany) of the samples heated from room temperature to 800°C in air at a heating rate of 10°C·min−1. Open circuit potential (OCP), electrochemical impedance spectroscopy (EIS), and potentiodynamic polarization tests were done to evaluate the effect of YSZ coatings on the corrosion performance of zircaloy-4 substrate in 3.5 wt.% aerated NaCl solution at room temperature. Measurements were done by Autolab device equipped with a computer; Model PGSTAT 302 N. Autolab GPES (general purpose electrochemical system) software was used for evaluating of polarization data in the potential range of ±1.5 V from OCP after the attainment of steady state at OCP conditions after about 30 minutes. The scan rate used was 0.5 mV/s. The standard electrochemical cell was arranged with saturated Ag/AgCl electrode as the reference electrode and platinum as the counter electrode. The exposed area of the samples was 1.8 cm2. Corrosion characteristics such as corrosion potential (Ecorr), corrosion current density (icorr), and anodic/cathodic Tafel slopes (βa and βc) were obtained from the intersection of cathodic and anodic Tafel curve tangents using Tafel extrapolation method. The polarization resistance (Rp) was determined using Stren-Geary equation (see [24]):
(1)Rp=βa·βc2.303icorr(βa+βc).The corrosion rate is calculated using the following equation (see [25]):
(2)rcorr=0.00327icorrMn·d,
where rcorr is corrosion rate in millimeter per year (mpy), n is charge number (4), M is molar mass (91.22 g·mol−1), and d is density of substrate (6.56 g·cm−3).The EIS measurements were carried out with FRA2 frequency response analyzer at open circuit potential after 1 hr immersion time with AC amplitude of 20 mV over a frequency range of 100 kHz to 1 mHz. Coating thickness was determined using SEM image of the cross section of the coated sample. High temperature oxidation resistance of the coating was evaluated by weight gain test.


## 3. Results and Discussion

### 3.1. Thermal Analysis Results

Thermal analysis (TGA-DTA) can vividly show what species of gel precursor is removed in each temperature range. Also the temperature that all organic solvents are evaporated and a dense and continuous coating is obtained will be found out by thermal analysis. The YSZ xerogel powder was first dried by 80°C for 1.5 hours in an oven and then heated from room temperature to 800°C in air at a heating rate of 10°C·min−1. As it can be seen from Figure 1, there is a continuous weight reduction in TGA curve during heating up to 730°C. No more weight loss is observed beyond 730°C. It is obvious that TGA curve displays three different slopes, and in this regard it could be divided into three different temperature ranges. The first range between 30–180°C shows a moderate slope attributing to disappearance of superficial and structural water in gel precursor. The DTA curve in this range shows two small endothermic peaks. One at 50°C ascribes to superficial water evaporation and the other one at 90°C belongs to structural water removal. The second part on TGA curve starts from 180°C to about 480°C with a sharp slope due to decomposition of a large amount of organic compounds. Beyond 480°C, the TGA slope is decreased by 730°C and then becomes a horizontal line. Slope reduction of the third temperature range in comparison with the second part asserts that the most amounts of organic species are vanished at 180–480°C. This behavior is also occurred in YSZ coatings and denser and more crack-free ones are expected at higher temperatures. In other words, the existence of water and organic solvents leads to produce discontinuities and porosities in coatings. The two exothermic peaks in the second temperature range should be considered. The results of works of Tiwari et al. [26] on sol-gel derived YSZ powder revealed that the weight loss between 330°C and 450°C is due to organic species removal by combustion. Soo et al. [27] ascribed two exothermic peaks near 350°C and 421°C during zirconia sol-gel derived powders in DTA curve to organic substances decomposition and crystallization of tetragonal structure of zirconia, respectively. The presence of sharp exothermic peak near 380°C refers to the crystallization transition of amorphous YSZ gel. XRD pattern in the next section shows that tetragonal phase is produced. As the temperature increases, the tetragonal crystals grow and a wide exothermic peak extending from 550°C to 725°C is resulted on DTA curve. This crystal growth is also verified by calculating the crystal size using Scherrer’s equation in XRD section. Finally, a dense gel powder weighted about 53% of its initial weight is remained.Figure 1
Thermal analysis (DTA-TGA) diagram for YSZ powder first dried at 80°C for 3 hrs in an oven.


### 3.2.  X-Ray Diffraction (XRD)

XRD analysis was done to determine which crystallized phases are in the coating at different temperatures. At low temperatures the gel is amorphous. As the temperature increases the amorphous gel transforms to tetragonal phase. Then the crystals of tetragonal phase grow, and at a critical crystal size, tetragonal to monoclinic phase transformation occurs. This transformation accompanied by a volume expansion which leads to crack emerging [12, 26]. The previous discussion verifies the importance of phase characterization.The gel powder was first thermally treated at three different temperatures of 150°C, 400°C, and 700°C, then their XRD patterns are obtained. Figure2(a) shows that the samples heated at low temperatures of 150°C are amorphous. The gel powder has crystalline structure at higher temperatures of 400°C and 700°C. The crystallization occurs near 400°C, and according to thermal analysis results, crystallization starts at 380°C. This indicates that the results of two analyses well satisfy each other. In addition, it is well compatible with other researcher’s works revealing the formation of crystallized YSZ above 300°C [19, 28, 29]. The patterns of Figures 2(b) and 2(c) belong to tetragonal zirconia crystals and the peaks at 700°C are sharper and stronger than 400°C due to both remaining of organic compounds and/or small crystal size at lower temperatures. No monoclinic phase was detected up to 700°C.Figure 2
XRD spectra of YSZ powders sintered at (a) 150°C, (b) 400°C, and (c) 700°C. The amorphous to crystalline transformation from 150°C to 400°C is clearly shown. The intensity of peaks increases from 400°C to 700°C.The crystal size (D) of YSZ crystals is measured using Scherrer’s equation (see [19, 23, 26]):
(3)Dhkl=kλBcosθ,
where Dhkl denotes the average crystallite size of the synthesized YSZ, k=0.94 is the shape factor, λ=0.15406 nm is the X-ray wavelength of CuKα, B is the full width of the peak measured at half maximum intensity (FWHM) in radians, and θ represents Bragg’s angle of the peak.The average crystal size of YSZ increases from 5.64 nm at 400°C to 10.22 nm at 700°C. This confirms that the wide peak at DTA curve between 550°C and 725°C is the consequence of crystal growth. In the presence of tetragonal stabilizer of yttria, the critical crystal size of zirconia increases and a higher temperature is needed to monoclinic phase being produced.


### 3.3. Surface Morphology

The scanning electron micrographs of the coatings heat treated at 200°C, 400°C, and 700°C are shown in Figures3(a)–3(c). The coatings dried at low temperatures reveal more cracks. As the drying temperature increases, the water and the organic compounds release and the coatings become denser. Li et al. [20] attributed the formation of these cracks to the internal stresses during heat treatment, but they are reduced as the temperature increased. In a sol-gel based coating the gel is made up of a solid network part and connected pores filled with liquid. In the first step of drying, the body shrinks at a constant rate equal to liquid evaporation rate. Due to the capillary forces, the pore sides of the gel are pulled together by the liquid. In the subsequent step, when the gel is too stiff to continue its shrinkage under capillary forces, the interface between liquid and air move into the film. This occurs because the top layers are shrinking quicker than the water and organic substances saturated bottom layers and evaporation is taking place from the liquid/air interface. This produces tensile stresses in the surface layer. It is at this point that cracking will occur. With further increasing in drying temperature, the remaining of organic substances will decompose and a dense and crack-free film is produced. Although such crack formation takes place in most of the films, in the thicker films the shrinkage, evaporation, and decomposition of the bottom layers create more stresses and more cracks [30, 31]. So it is found that the thickness of YSZ coatings is a crucial factor affecting the corrosion and oxidation behaviors; that is, a multilayer coating is much more effective than the single-layer one. At temperatures higher than tetragonal to monoclinic transformation temperature, the cracks again emerge due to a volume increase in the crystallization transformation. In the presence of stabilizers such as Y3+, Ca2+, and Mg2+, the transformation temperature shifts to higher values and more liquids are extracted and evaporated from the gel without additional volume changes [12, 26].(a)–(c) SEM images of the surface of coated samples with different sintering temperature (a) 200°C, (b) 400°C, (c) 700°C, and (d) SEM image of the cross section of coated sample (15 layers, 700°C).
(a)
(b)
(c)
(d)Domínguez Crespo et al. [19] have also obtained that the cracks of YSZ coatings on commercial carbon steel substrate are decreased due to the removal of organic compounds at higher temperatures.According to XRD results, there are no monoclinic phases up to 700°C heat treatment due to the presence of Y3+ stabilizer. As it can be seen in Figures 3(a)–3(c), the more crack-free and dense film is obtained at 700°C.


### 3.4. Film Thickness

The film thickness of the coatings was determined using SEM image of the cross section of 15 layers coating sintered at 700°C (Figure3(d)). The total thickness of the coating after 15 deposited layers is about 970 nm. Therefore each layer’s thickness would be about 64 nm.


### 3.5. Electrochemical Measurements

#### 3.5.1. Polarization Tests

It can be concluded from the results obtained by Tafel plots (Figure4) that the YSZ coatings show more noble corrosion potential (Ecorr) and less corrosion current density (icorr) when it is dried at higher temperatures. The corrosion current density decreases about 104 times and the corrosion potential shifts to positive direction more than 600 mV, when the drying temperature increases from 200°C to 700°C. The electrochemical performance of the YSZ coating dried at 200°C is even worse than the bare substrate. According to the results of thermal analysis, there are organic substances in the film at 200°C and this leads to electrolyte penetration onto the substrate surface. With increasing temperature the organic substances evaporation and decomposition increase the densification of the films.Figure 4
Polarization plots for (a) bare substrate, (b) 200°C, (c) 400°C, and (d) 700°C.López et al. have also concluded that the corrosion resistance of high temperature treatment silica layers produced by sol-gel process is better than the low temperature heat treated ones. Li et al. [20] attributed the lower corrosion resistance of zirconia coating on magnesium substrate at the low temperature in comparison with the high temperature, to the poor adhesion between the substrate and the zirconia coating. The electrochemical parameters of coated and uncoated samples for different drying temperature are reported in Table 2.Table 2
The electrochemical parameters of coated and uncoated samples for different sintering temperature.
Sintering temp. (°C)
i
corr (A·cm−2)
E
corr (V)
β
a (V/dec)
β
c (V/dec)
R
p (ohm·cm2)
Corr. rate (mm·yr−1)
Bare
9.80
E
-
07
−0.41
0.035
0.05
1.60
E
+
3
7.35
E
-
3
200
2.47
E
-
07
−0.44
0.070
0.03
2.62
E
+
3
2.91
E
-
3
400
1.21
E
-
10
−0.05
0.050
0.04
7.49
E
+
6
7.20
E
-
8
700
9.76
E
-
11
0.21
0.035
0.05
9.33
E
+
7
6.68
E
-
8


#### 3.5.2. Electrochemical Impedance Spectroscopy (EIS)

Figure5 shows the Nyquist plot representation of the electrochemical impedance measurements carried out in 3.5 wt.% NaCl solution for bare and coated samples at three different drying temperatures of 200°C, 400°C, and 700°C after about 1 hour immersion in order to obtain the evolution of the coating’s protective properties, also their corrosion mechanism.Figure 5
Nyquist plots for bare and coated samples dried at (a) 200°C (b) 400°C, and (c) 700°C, after 1 hour immersion in 3.5 wt.% NaCl electrolyte.It is possible to observe that the real part of impedance (X-axis) at low frequency is strongly increased with drying temperature. Since the real part of impedance at low frequency can be considered equal to the resistance correlated to the Faradic processes, this observation evidences that the barrier property tends to be increased as a function of drying temperature.The impedance spectra for Nyquist diagrams were analyzed by fitting the experimental data to equivalent circuit model in Figure6 by Zsim software. Figure 6(a) simulates the bare and coated samples dried at 700°C and Figure 6(b) was used for coated samples dried at 200°C and 400°C. In the equivalent circuits, Rs is the solution resistance, Rct is the charge transfer resistance, CPEdl is the double layer capacitance, and CPEcoat models the intact layer, while the resistance Rp is associated to large pores in the outer layer. The intermediate oxide is modeled with the constant phase element (CPEox) and the resistance Rox. CPEox describes a network of electrolyte resistances and double layer capacitors in the pores of the layer, while Rox is related to the barrier properties of the film. The parameter Rox is affected by nanopores in this layer. Therefore, this is the most important parameter of the equivalent circuit of Figure 6(b) as long as corrosion protection is concerned. In general, the charge transfer resistance could be compared in all cases to evaluate their corrosion performance. Here, a constant phase element (CPE) is commonly used to represent capacitance because it is hardly pure capacitance in the real electrochemical process [17].Equivalent circuits of samples after 1 hour immersion in 3.5 wt.% NaCl electrolyte: (a) bare and coated one dried at 700°C and (b) coated and dried at 200°C and 400°C.
(a)
(b)Parameters obtained from EIS tests are presented in Table3. Heat treatment at higher temperatures improves the coating resistance. This observation is well compatible with the Tafel results and again confirms that, at higher temperatures, the organic substances decompose more than lower temperatures and this leads to more densification of the coating.Table 3
Parameters of equivalent electrical circuit for sol-gel coated samples immersed in 3.5 wt.% NaCl electrolyte.
Sample
R
s (Ωcm2)
CPEox
R
ox (Ωcm2)
R
ct (Ωcm2)
CPEdl
Y
0 (F·cm2)
n
Y
0 (F·cm2)
n
Bare
32
—
—
—
1.68
E
+
5
3.00
E
-
6
1
a
16
2.00
E
-
4
0.98
1.00
E
+
5
902
8.20
E
-
6
0.52
b
21
1.00
E
-
9
0.93
6.3
E
+
7
1.90
E
+
5
5.40
E
-
9
0.95
c
27
—
—
—
1.90
E
+
8
6.00
E
-
9
0.96


### 3.6. High Temperature Corrosion (Oxidation Resistance)

According to the SEM results, the most homogeneous and crack-free coating was obtained at 700°C. This sample was subjected to weight gain test in air at 800°C for 110 minutes to evaluate YSZ coating resistance against high temperature oxidation. Figure7 shows the weight gain versus time curve of both bare and coated samples. This coating reduces the oxidation rate of coated zircaloy-4 about 25% when compared with the bare substrate. So the YSZ coating acts as a thermal barrier allowing the use of this kind of material at higher operational temperatures. Li et al. [32] have investigated high temperature oxidation of bare mild steel and ZrO2 coated samples in air at 450–550°C for 12 hours. They concluded that the oxidation resistance of mild steel at this temperature is about 6.5 times higher than that of uncoated substrates. Baron and Ruiz [21] have found that high temperature oxidation of 1.25Cr–0.5Mo steel is reduced in the presence of YSZ coating. This oxidation reduction was about 35% when the sol is prepared with acidic catalyst, and it is 62% with a basic catalyst during 96 hours at 700°C in air. The proposed mechanism was that the YSZ coating acts as a physical barrier making outward diffusion of iron difficult. However, once the stresses generated by the slow growing oxides break the continuity of the coating, the formation of vacancies-cations pair (the Zr4+ cations react with the growing iron oxides forming pairs with vacancies) keeps the oxidation rate lower than for uncoated samples. Such mechanism can be expected in the application of YSZ coating on the zircaloy-4 substrate.Figure 7
Weight gain versus time curves for (a) bare and (b) coated zircaloy-4 exposed to air at 800°C.


## 3.1. Thermal Analysis Results

Thermal analysis (TGA-DTA) can vividly show what species of gel precursor is removed in each temperature range. Also the temperature that all organic solvents are evaporated and a dense and continuous coating is obtained will be found out by thermal analysis. The YSZ xerogel powder was first dried by 80°C for 1.5 hours in an oven and then heated from room temperature to 800°C in air at a heating rate of 10°C·min−1. As it can be seen from Figure 1, there is a continuous weight reduction in TGA curve during heating up to 730°C. No more weight loss is observed beyond 730°C. It is obvious that TGA curve displays three different slopes, and in this regard it could be divided into three different temperature ranges. The first range between 30–180°C shows a moderate slope attributing to disappearance of superficial and structural water in gel precursor. The DTA curve in this range shows two small endothermic peaks. One at 50°C ascribes to superficial water evaporation and the other one at 90°C belongs to structural water removal. The second part on TGA curve starts from 180°C to about 480°C with a sharp slope due to decomposition of a large amount of organic compounds. Beyond 480°C, the TGA slope is decreased by 730°C and then becomes a horizontal line. Slope reduction of the third temperature range in comparison with the second part asserts that the most amounts of organic species are vanished at 180–480°C. This behavior is also occurred in YSZ coatings and denser and more crack-free ones are expected at higher temperatures. In other words, the existence of water and organic solvents leads to produce discontinuities and porosities in coatings. The two exothermic peaks in the second temperature range should be considered. The results of works of Tiwari et al. [26] on sol-gel derived YSZ powder revealed that the weight loss between 330°C and 450°C is due to organic species removal by combustion. Soo et al. [27] ascribed two exothermic peaks near 350°C and 421°C during zirconia sol-gel derived powders in DTA curve to organic substances decomposition and crystallization of tetragonal structure of zirconia, respectively. The presence of sharp exothermic peak near 380°C refers to the crystallization transition of amorphous YSZ gel. XRD pattern in the next section shows that tetragonal phase is produced. As the temperature increases, the tetragonal crystals grow and a wide exothermic peak extending from 550°C to 725°C is resulted on DTA curve. This crystal growth is also verified by calculating the crystal size using Scherrer’s equation in XRD section. Finally, a dense gel powder weighted about 53% of its initial weight is remained.Figure 1
Thermal analysis (DTA-TGA) diagram for YSZ powder first dried at 80°C for 3 hrs in an oven.


## 3.2.  X-Ray Diffraction (XRD)

XRD analysis was done to determine which crystallized phases are in the coating at different temperatures. At low temperatures the gel is amorphous. As the temperature increases the amorphous gel transforms to tetragonal phase. Then the crystals of tetragonal phase grow, and at a critical crystal size, tetragonal to monoclinic phase transformation occurs. This transformation accompanied by a volume expansion which leads to crack emerging [12, 26]. The previous discussion verifies the importance of phase characterization.The gel powder was first thermally treated at three different temperatures of 150°C, 400°C, and 700°C, then their XRD patterns are obtained. Figure2(a) shows that the samples heated at low temperatures of 150°C are amorphous. The gel powder has crystalline structure at higher temperatures of 400°C and 700°C. The crystallization occurs near 400°C, and according to thermal analysis results, crystallization starts at 380°C. This indicates that the results of two analyses well satisfy each other. In addition, it is well compatible with other researcher’s works revealing the formation of crystallized YSZ above 300°C [19, 28, 29]. The patterns of Figures 2(b) and 2(c) belong to tetragonal zirconia crystals and the peaks at 700°C are sharper and stronger than 400°C due to both remaining of organic compounds and/or small crystal size at lower temperatures. No monoclinic phase was detected up to 700°C.Figure 2
XRD spectra of YSZ powders sintered at (a) 150°C, (b) 400°C, and (c) 700°C. The amorphous to crystalline transformation from 150°C to 400°C is clearly shown. The intensity of peaks increases from 400°C to 700°C.The crystal size (D) of YSZ crystals is measured using Scherrer’s equation (see [19, 23, 26]):
(3)Dhkl=kλBcosθ,
where Dhkl denotes the average crystallite size of the synthesized YSZ, k=0.94 is the shape factor, λ=0.15406 nm is the X-ray wavelength of CuKα, B is the full width of the peak measured at half maximum intensity (FWHM) in radians, and θ represents Bragg’s angle of the peak.The average crystal size of YSZ increases from 5.64 nm at 400°C to 10.22 nm at 700°C. This confirms that the wide peak at DTA curve between 550°C and 725°C is the consequence of crystal growth. In the presence of tetragonal stabilizer of yttria, the critical crystal size of zirconia increases and a higher temperature is needed to monoclinic phase being produced.


## 3.3. Surface Morphology

The scanning electron micrographs of the coatings heat treated at 200°C, 400°C, and 700°C are shown in Figures3(a)–3(c). The coatings dried at low temperatures reveal more cracks. As the drying temperature increases, the water and the organic compounds release and the coatings become denser. Li et al. [20] attributed the formation of these cracks to the internal stresses during heat treatment, but they are reduced as the temperature increased. In a sol-gel based coating the gel is made up of a solid network part and connected pores filled with liquid. In the first step of drying, the body shrinks at a constant rate equal to liquid evaporation rate. Due to the capillary forces, the pore sides of the gel are pulled together by the liquid. In the subsequent step, when the gel is too stiff to continue its shrinkage under capillary forces, the interface between liquid and air move into the film. This occurs because the top layers are shrinking quicker than the water and organic substances saturated bottom layers and evaporation is taking place from the liquid/air interface. This produces tensile stresses in the surface layer. It is at this point that cracking will occur. With further increasing in drying temperature, the remaining of organic substances will decompose and a dense and crack-free film is produced. Although such crack formation takes place in most of the films, in the thicker films the shrinkage, evaporation, and decomposition of the bottom layers create more stresses and more cracks [30, 31]. So it is found that the thickness of YSZ coatings is a crucial factor affecting the corrosion and oxidation behaviors; that is, a multilayer coating is much more effective than the single-layer one. At temperatures higher than tetragonal to monoclinic transformation temperature, the cracks again emerge due to a volume increase in the crystallization transformation. In the presence of stabilizers such as Y3+, Ca2+, and Mg2+, the transformation temperature shifts to higher values and more liquids are extracted and evaporated from the gel without additional volume changes [12, 26].(a)–(c) SEM images of the surface of coated samples with different sintering temperature (a) 200°C, (b) 400°C, (c) 700°C, and (d) SEM image of the cross section of coated sample (15 layers, 700°C).
(a)
(b)
(c)
(d)Domínguez Crespo et al. [19] have also obtained that the cracks of YSZ coatings on commercial carbon steel substrate are decreased due to the removal of organic compounds at higher temperatures.According to XRD results, there are no monoclinic phases up to 700°C heat treatment due to the presence of Y3+ stabilizer. As it can be seen in Figures 3(a)–3(c), the more crack-free and dense film is obtained at 700°C.


## 3.4. Film Thickness

The film thickness of the coatings was determined using SEM image of the cross section of 15 layers coating sintered at 700°C (Figure3(d)). The total thickness of the coating after 15 deposited layers is about 970 nm. Therefore each layer’s thickness would be about 64 nm.


## 3.5. Electrochemical Measurements

### 3.5.1. Polarization Tests

It can be concluded from the results obtained by Tafel plots (Figure4) that the YSZ coatings show more noble corrosion potential (Ecorr) and less corrosion current density (icorr) when it is dried at higher temperatures. The corrosion current density decreases about 104 times and the corrosion potential shifts to positive direction more than 600 mV, when the drying temperature increases from 200°C to 700°C. The electrochemical performance of the YSZ coating dried at 200°C is even worse than the bare substrate. According to the results of thermal analysis, there are organic substances in the film at 200°C and this leads to electrolyte penetration onto the substrate surface. With increasing temperature the organic substances evaporation and decomposition increase the densification of the films.Figure 4
Polarization plots for (a) bare substrate, (b) 200°C, (c) 400°C, and (d) 700°C.López et al. have also concluded that the corrosion resistance of high temperature treatment silica layers produced by sol-gel process is better than the low temperature heat treated ones. Li et al. [20] attributed the lower corrosion resistance of zirconia coating on magnesium substrate at the low temperature in comparison with the high temperature, to the poor adhesion between the substrate and the zirconia coating. The electrochemical parameters of coated and uncoated samples for different drying temperature are reported in Table 2.Table 2
The electrochemical parameters of coated and uncoated samples for different sintering temperature.
Sintering temp. (°C)
i
corr (A·cm−2)
E
corr (V)
β
a (V/dec)
β
c (V/dec)
R
p (ohm·cm2)
Corr. rate (mm·yr−1)
Bare
9.80
E
-
07
−0.41
0.035
0.05
1.60
E
+
3
7.35
E
-
3
200
2.47
E
-
07
−0.44
0.070
0.03
2.62
E
+
3
2.91
E
-
3
400
1.21
E
-
10
−0.05
0.050
0.04
7.49
E
+
6
7.20
E
-
8
700
9.76
E
-
11
0.21
0.035
0.05
9.33
E
+
7
6.68
E
-
8


### 3.5.2. Electrochemical Impedance Spectroscopy (EIS)

Figure5 shows the Nyquist plot representation of the electrochemical impedance measurements carried out in 3.5 wt.% NaCl solution for bare and coated samples at three different drying temperatures of 200°C, 400°C, and 700°C after about 1 hour immersion in order to obtain the evolution of the coating’s protective properties, also their corrosion mechanism.Figure 5
Nyquist plots for bare and coated samples dried at (a) 200°C (b) 400°C, and (c) 700°C, after 1 hour immersion in 3.5 wt.% NaCl electrolyte.It is possible to observe that the real part of impedance (X-axis) at low frequency is strongly increased with drying temperature. Since the real part of impedance at low frequency can be considered equal to the resistance correlated to the Faradic processes, this observation evidences that the barrier property tends to be increased as a function of drying temperature.The impedance spectra for Nyquist diagrams were analyzed by fitting the experimental data to equivalent circuit model in Figure6 by Zsim software. Figure 6(a) simulates the bare and coated samples dried at 700°C and Figure 6(b) was used for coated samples dried at 200°C and 400°C. In the equivalent circuits, Rs is the solution resistance, Rct is the charge transfer resistance, CPEdl is the double layer capacitance, and CPEcoat models the intact layer, while the resistance Rp is associated to large pores in the outer layer. The intermediate oxide is modeled with the constant phase element (CPEox) and the resistance Rox. CPEox describes a network of electrolyte resistances and double layer capacitors in the pores of the layer, while Rox is related to the barrier properties of the film. The parameter Rox is affected by nanopores in this layer. Therefore, this is the most important parameter of the equivalent circuit of Figure 6(b) as long as corrosion protection is concerned. In general, the charge transfer resistance could be compared in all cases to evaluate their corrosion performance. Here, a constant phase element (CPE) is commonly used to represent capacitance because it is hardly pure capacitance in the real electrochemical process [17].Equivalent circuits of samples after 1 hour immersion in 3.5 wt.% NaCl electrolyte: (a) bare and coated one dried at 700°C and (b) coated and dried at 200°C and 400°C.
(a)
(b)Parameters obtained from EIS tests are presented in Table3. Heat treatment at higher temperatures improves the coating resistance. This observation is well compatible with the Tafel results and again confirms that, at higher temperatures, the organic substances decompose more than lower temperatures and this leads to more densification of the coating.Table 3
Parameters of equivalent electrical circuit for sol-gel coated samples immersed in 3.5 wt.% NaCl electrolyte.
Sample
R
s (Ωcm2)
CPEox
R
ox (Ωcm2)
R
ct (Ωcm2)
CPEdl
Y
0 (F·cm2)
n
Y
0 (F·cm2)
n
Bare
32
—
—
—
1.68
E
+
5
3.00
E
-
6
1
a
16
2.00
E
-
4
0.98
1.00
E
+
5
902
8.20
E
-
6
0.52
b
21
1.00
E
-
9
0.93
6.3
E
+
7
1.90
E
+
5
5.40
E
-
9
0.95
c
27
—
—
—
1.90
E
+
8
6.00
E
-
9
0.96


## 3.5.1. Polarization Tests

It can be concluded from the results obtained by Tafel plots (Figure4) that the YSZ coatings show more noble corrosion potential (Ecorr) and less corrosion current density (icorr) when it is dried at higher temperatures. The corrosion current density decreases about 104 times and the corrosion potential shifts to positive direction more than 600 mV, when the drying temperature increases from 200°C to 700°C. The electrochemical performance of the YSZ coating dried at 200°C is even worse than the bare substrate. According to the results of thermal analysis, there are organic substances in the film at 200°C and this leads to electrolyte penetration onto the substrate surface. With increasing temperature the organic substances evaporation and decomposition increase the densification of the films.Figure 4
Polarization plots for (a) bare substrate, (b) 200°C, (c) 400°C, and (d) 700°C.López et al. have also concluded that the corrosion resistance of high temperature treatment silica layers produced by sol-gel process is better than the low temperature heat treated ones. Li et al. [20] attributed the lower corrosion resistance of zirconia coating on magnesium substrate at the low temperature in comparison with the high temperature, to the poor adhesion between the substrate and the zirconia coating. The electrochemical parameters of coated and uncoated samples for different drying temperature are reported in Table 2.Table 2
The electrochemical parameters of coated and uncoated samples for different sintering temperature.
Sintering temp. (°C)
i
corr (A·cm−2)
E
corr (V)
β
a (V/dec)
β
c (V/dec)
R
p (ohm·cm2)
Corr. rate (mm·yr−1)
Bare
9.80
E
-
07
−0.41
0.035
0.05
1.60
E
+
3
7.35
E
-
3
200
2.47
E
-
07
−0.44
0.070
0.03
2.62
E
+
3
2.91
E
-
3
400
1.21
E
-
10
−0.05
0.050
0.04
7.49
E
+
6
7.20
E
-
8
700
9.76
E
-
11
0.21
0.035
0.05
9.33
E
+
7
6.68
E
-
8


## 3.5.2. Electrochemical Impedance Spectroscopy (EIS)

Figure5 shows the Nyquist plot representation of the electrochemical impedance measurements carried out in 3.5 wt.% NaCl solution for bare and coated samples at three different drying temperatures of 200°C, 400°C, and 700°C after about 1 hour immersion in order to obtain the evolution of the coating’s protective properties, also their corrosion mechanism.Figure 5
Nyquist plots for bare and coated samples dried at (a) 200°C (b) 400°C, and (c) 700°C, after 1 hour immersion in 3.5 wt.% NaCl electrolyte.It is possible to observe that the real part of impedance (X-axis) at low frequency is strongly increased with drying temperature. Since the real part of impedance at low frequency can be considered equal to the resistance correlated to the Faradic processes, this observation evidences that the barrier property tends to be increased as a function of drying temperature.The impedance spectra for Nyquist diagrams were analyzed by fitting the experimental data to equivalent circuit model in Figure6 by Zsim software. Figure 6(a) simulates the bare and coated samples dried at 700°C and Figure 6(b) was used for coated samples dried at 200°C and 400°C. In the equivalent circuits, Rs is the solution resistance, Rct is the charge transfer resistance, CPEdl is the double layer capacitance, and CPEcoat models the intact layer, while the resistance Rp is associated to large pores in the outer layer. The intermediate oxide is modeled with the constant phase element (CPEox) and the resistance Rox. CPEox describes a network of electrolyte resistances and double layer capacitors in the pores of the layer, while Rox is related to the barrier properties of the film. The parameter Rox is affected by nanopores in this layer. Therefore, this is the most important parameter of the equivalent circuit of Figure 6(b) as long as corrosion protection is concerned. In general, the charge transfer resistance could be compared in all cases to evaluate their corrosion performance. Here, a constant phase element (CPE) is commonly used to represent capacitance because it is hardly pure capacitance in the real electrochemical process [17].Equivalent circuits of samples after 1 hour immersion in 3.5 wt.% NaCl electrolyte: (a) bare and coated one dried at 700°C and (b) coated and dried at 200°C and 400°C.
(a)
(b)Parameters obtained from EIS tests are presented in Table3. Heat treatment at higher temperatures improves the coating resistance. This observation is well compatible with the Tafel results and again confirms that, at higher temperatures, the organic substances decompose more than lower temperatures and this leads to more densification of the coating.Table 3
Parameters of equivalent electrical circuit for sol-gel coated samples immersed in 3.5 wt.% NaCl electrolyte.
Sample
R
s (Ωcm2)
CPEox
R
ox (Ωcm2)
R
ct (Ωcm2)
CPEdl
Y
0 (F·cm2)
n
Y
0 (F·cm2)
n
Bare
32
—
—
—
1.68
E
+
5
3.00
E
-
6
1
a
16
2.00
E
-
4
0.98
1.00
E
+
5
902
8.20
E
-
6
0.52
b
21
1.00
E
-
9
0.93
6.3
E
+
7
1.90
E
+
5
5.40
E
-
9
0.95
c
27
—
—
—
1.90
E
+
8
6.00
E
-
9
0.96


## 3.6. High Temperature Corrosion (Oxidation Resistance)

According to the SEM results, the most homogeneous and crack-free coating was obtained at 700°C. This sample was subjected to weight gain test in air at 800°C for 110 minutes to evaluate YSZ coating resistance against high temperature oxidation. Figure7 shows the weight gain versus time curve of both bare and coated samples. This coating reduces the oxidation rate of coated zircaloy-4 about 25% when compared with the bare substrate. So the YSZ coating acts as a thermal barrier allowing the use of this kind of material at higher operational temperatures. Li et al. [32] have investigated high temperature oxidation of bare mild steel and ZrO2 coated samples in air at 450–550°C for 12 hours. They concluded that the oxidation resistance of mild steel at this temperature is about 6.5 times higher than that of uncoated substrates. Baron and Ruiz [21] have found that high temperature oxidation of 1.25Cr–0.5Mo steel is reduced in the presence of YSZ coating. This oxidation reduction was about 35% when the sol is prepared with acidic catalyst, and it is 62% with a basic catalyst during 96 hours at 700°C in air. The proposed mechanism was that the YSZ coating acts as a physical barrier making outward diffusion of iron difficult. However, once the stresses generated by the slow growing oxides break the continuity of the coating, the formation of vacancies-cations pair (the Zr4+ cations react with the growing iron oxides forming pairs with vacancies) keeps the oxidation rate lower than for uncoated samples. Such mechanism can be expected in the application of YSZ coating on the zircaloy-4 substrate.Figure 7
Weight gain versus time curves for (a) bare and (b) coated zircaloy-4 exposed to air at 800°C.


## 4. Conclusion

The present study shows that in the presence of yttria cations, the tetragonal phase in sol-gel YSZ coating can be stabilized even at 700°C. This stabilization prevents from tetragonal to monoclinic transformation and the crack formation resulting from volume expansion is not occurred. The surface quality and corrosion properties of the coatings strongly depend on the heat treatment temperature, because the process requires the condensation reaction and densification among the sols, which affects the diffusion of electrolytes at the metal/solution interface through coating. The higher corrosion protection was achieved with drying at 700°C. This coating also reduces the oxidation rate of the zircaloy-4 in about 25% when compared with the bare substrate.



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*Source: 453835-2013-12-17.xml*