Introduction

The increasing efficiency of advanced turbine engines requires higher operation temperatures for more complete combustion of fuels. At the high working temperature above 1000 °C, surface oxidation becomes the life limiting factor (Ref 1). Diffusive nickel aluminide coatings are widely used to protect nickel-based superalloys against oxidation (Ref 2). Aluminide coatings rely on formation of the β-NiAl phase on the surface of the alloys. Three major processes, by which aluminide can be deposited include: pack cementation, vapor phase aluminizing (VPA) and chemical vapor deposition (CVD). One of the steps, which is common in these three processes, is the generation of vapors containing aluminum or the other metallic constituents of the coatings. The vapor phase is transported to the chamber and reacts with the alloy which forms the aluminide coating. In the pack process, the component is embedded in, and therefore in intimate contact with a pack mix in a heated retort (Ref 3). The pack generates the halide vapors. In the vapor phase aluminizing process (VPA), the component to be coated is inside the retort but not in contact with the pack (Al-Cr alloy and Al2O3 filler). The halide vapors are plumbed on to the accessible internal and external surfaces of the component. In the CVD process, the halide vapor sources are external in individual generators and vapors are plumbed on to the component held inside a reactor in a heated retort (Ref 4, 5). The aluminum activity plays a critical role in determining the predominant diffusing species. Depending on the content of aluminum in the pack and the processing temperature, the coating process is termed a “low-activity” or “high activity” one. When the aluminum activity is low and the temperature is above 1000 °C, the predominant diffusing species is nickel, which diffuses out of the alloy, producing an ‘outward diffusion’ coating. If the aluminum activity is high and the temperature is below 950 °C, aluminum diffuses inwards, resulting in an “inward diffusion” coating. Aluminum is also the predominant diffusing species in the Ni2Al3 phase. In the low-activity process, nickel is a predominant diffusing species, which diffuses outwards and combines with aluminum to form the external NiAl zone. Near the interface, the internal zone, which is also called the interdiffusion zone, loses nickel. Many of the alloying constituents of the alloy have very low solubility in the NiAl phase formed in the inner zone. The total coating thickness includes both the external and the interdiffusion zones. Both of the zones consist of the NiAl phase, but only in the interdiffusion zone carbides are formed. Aluminum is the predominant diffusing species in the high-activity coating process. The consequence of the higher inward diffusion of aluminum to nickel is that the original surface becomes the external surface of the coating (Ref 6).

Aluminum in the coating combines with the oxygen which forms the protective α-Al2O3 oxide. When the oxide cracks and spalls due to thermal cycling, additional aluminum from the coating diffuses to the surface to reform the oxide. When the aluminum content in the coatings drops to about 4 or 5% at., the α-Al2O3 oxide can no longer be formed and rapid oxidation occurs (Ref 7).

Watanabe et al. (Ref 8) reported that the residual stress in the aluminide coatings caused by cooling from the manufacturing temperature facilitates, yielding of the coatings. It does so by interacting with the stress in the aluminide coating caused by the thermal expansion misfit with the thermally grown oxide. It causes an acceleration of the degradation of coated elements at high temperature. Therefore, there is a strong need of a thorough investigation of the correlation between residual stresses and degradation of coated elements.

This paper presents the results of the research performed on the aluminide coating deposited by the CVD and VPA methods on the turbine blade made of ŻS6K superalloy. The oxidation behavior of coated turbine blades was evaluated. Moreover, the residual stresses after aluminization and oxidation were investigated.

Experimental

The nickel-based turbine blades made of ŻS6K superalloy were used as a substrate. The chemical composition of this superalloy is: 0.14 wt.% C, 10.2 wt.% Cr, 5.2 wt.% W, 4.7 wt.% Co, 3.7 wt.% Mo, 5.3 wt.% Al, 2.8 wt.% Ti, 1.5 wt.% Fe, and the balance nickel (Ref 2).

Two kinds of coatings were produced on the turbine blades: namely deposited by the CVD and PVD processes.

The aluminized turbine blades were subjected to the oxidation test at 1100 °C in an air atmosphere for 1000 h. Samples were heated up to 1100 °C, kept at that temperature for 20 h and then cooled down in the air to the room temperature and then weighed with accuracy of 0.0001 g.

The microstructure of the surface of the synthesized coatings was investigated by the scanning electron microscope (SEM) Hitachi S-3400N and the energy dispersive spectroscope (EDS) (Ref 9-11).

Macroscopic residual stresses in as deposited aluminide coatings and after the oxidation test were determined using the Proto I XRD diffractometer. Asymmetric geometry was used to measure ωsin2ψ and interplanar spacing determined as a function of ψ tilt angle of x-rays to determine the strain of the specimen (Ref 12-15).

A mobile x-ray diffraction residual stress analyzer with a horizontal goniometer fixture was used to measure residual stress in the samples. The specimen axis for ψ tilt is vertical and the arrangement of the diffractometer is based on the Bragg-Bentano focusing principle.

Cobalt x-ray source with a spot diameter of 2 mm was used. X-ray tube operating parameters were 20 kV and 4 mA. Measurements were made by the diffraction of manganese K-alpha radiation from the (311) crystallographic planes with a peak position 2Θ = 149° with the exposure time of 2 s and number of 20 exposures. The depth of K-alpha radiation was about 10 μm.

Two position scintillation detectors were used to cover positive and negative ψ angles and the goniometer oscillated over 3° about the main position to obtain better signal-to-noise ratio.

Multiple channel x-ray diffraction data were acquired simultaneously using position sensitive scintillation detectors (PSSD).

Pearson VII peak-fitting algorithm was applied to the intensity data and Lorentz polarization and absorption corrections were used to determine the center of the diffraction peak. For residual stress determination at a given location, the diffraction peak position was determined at seven ψ tilt angles. These ψ values were in the ranges between −45.65° and 45.65°.

Measurements of the stress by scanning the sample in both orthogonal x and y directions revealed the distribution of the residual stress (Fig. 1).

Fig. 1
figure 1

A scheme of the turbine blade and places where residual stress measurement was performed: 1—lock of turbine blade, 2—suction side and 3—pressure side

The diffraction method applied in this research is based on the Bragg’s law i.e., lattice spacing is calculated on the basis of the diffraction angle 2θ and x-ray wavelength. Residual stress in the material causes the shift of the mean positions of diffraction peaks. Usually, it is less than one degree. The magnitude of this shift is proportional to the value of the strain The residual stress is calculated from the value of this strain. The x-rays can penetrate into material for not more than several μm. Therefore, it is assumed that the residual stress in the surface is biaxial. It may be described by principle stresses σ11 and σ22 in the plane of the surface with no stress σ33 perpendicular to the free surface. The shear stresses σ13 = σ31 and σ23 = σ32 are then equal to zero (Fig. 2).

Fig. 2
figure 2

The principal axes of the residual stresses σ. Ψ—angle between the normal to the surface and the normal to the family of diffracting planes {hkl} M, σ ϕ—stress in the measurement direction, ϕ—angle between the direction of the principal stress σ11 and the selected direction of the measurement

The lattice spacing values d ψϕ for a given family of lattice planes are determined as a function of sin2ψ. The slope \(\frac{{\partial d_{\phi \Psi } }}{{\partial \sin^{2} \Psi }}\) is determined on the basis of the linear fit to the recorded data points. Knowing the Young’s modulus and Poisson’s ratio the residual stress σ ϕ may be calculated according to the equation:

$$\sigma_{\upphi } = \left( {\frac{E}{1 + \nu }} \right)_{hkl} \frac{1}{{d_{0} }}\left( {\frac{{\partial d_{\upphi \Psi } }}{{\partial \sin^{2} \Psi }}} \right).$$
(1)

One should also know the unstressed lattice spacing d 0 for the analyzed family of lattice planes. As it usually remains unknown, d ϕ0 is applied instead of d 0. It is determined experimentally at ψ = 0. This procedure introduces an error which is negligible when compared to other errors.

Results

The turbine blades made of ŻS6K Ni-based superalloy were aluminized by the vapor deposition method and the low-activity CVD method. The obtained coating covered the turbine blades completely.

The cross-section of the turbine blade after aluminizing by the VPA method is shown in Fig. 3. The microstructural analysis on the cross-section revealed that the coating consisted of two layers: an additive layer and an interdiffusion layer (Fig. 3a). The total coating thickness is about 65 μm. The EDS analysis results showed that the top additive layer is composed of the β-NiAl phase [50.14 Al-2.87 Cr-0.31 Ti-4.23 Co-42.0 Ni-0.44 W (at.%)] (Fig. 3b). The interdiffusion layer contains precipitates rich in chromium, titanium, tungsten, and molybdenum that were in the substrate (Fig. 3c). The XRD pattern indicates the presence of the NiAl phase and MC, M23C6 carbides in the coating (Fig. 4).

Fig. 3
figure 3

The cross-section microstructure of the aluminide coating deposited by the VPA method on the ŻS6K Ni-base superalloy turbine blade (a), EDS spectrum of the additive layer (b), and EDS spectrum of the interdiffusion layer (c)

Fig. 4
figure 4

XRD pattern of the aluminide coating deposited by the VPA method

The microstructure analysis on the cross-section revealed that the CVD coating consists of two layers: an additive layer and interdiffusion layer (Fig. 5a). The total coating thickness is about 34 μm. The EDS analysis results showed that the top additive layer is composed of the β-NiAl phase (39.59 Al-2.15 Cr-5.16 Co-52.92 Ni-0.17W) (at.%) (Fig. 5b). The interdiffusion layer contains precipitates rich in chromium, titanium, tungsten, and molybdenum that diffused from the substrate (Fig. 5c). The XRD pattern indicates the presence of the NiAl phase in the coating (Fig. 6).

Fig. 5
figure 5

The microstructure of the cross-section of the aluminide coating deposited by the low-activity CVD method on the ŻS6K Ni-base superalloy turbine blade (a), EDS spectrum of the additive layer (b), and EDS spectrum of the interdiffusion layer (c)

Fig. 6
figure 6

XRD pattern of the aluminide coating deposited by the CVD method

It was found that the residual stress in the aluminide coating at the lock, suction side, and pressure side of the turbine blades was tensile (Table 1). Moreover, the values of the residual stress in the x and y directions do not differ significantly (Table 1).

Table 1 XRD residual stress results after the aluminizing process

Mass change curves of aluminide coatings during the cyclic oxidation test are shown in Fig. 7. The aluminide coating deposited by the low-activity CVD method showed better oxidation resistance in comparison to the aluminide coating deposited by the VPA method. The mass change of the ŻS6K turbine blade covered with the aluminide coating deposited by the VPA method is about −6.2 mg/cm2, while the mass change of the turbine blade covered with the aluminide coating deposited by the low-activity CVD method is about 0.5 mg/cm2 after 40 cycles of oxidation in the air atmosphere (Fig. 7).

Fig. 7
figure 7

Mass change curves of ŻS6K superalloy: 1—with the aluminide coating deposited by the low-activity CVD process; 2—with the aluminide coating deposited by the VPA process

After 10 cycles of oxidation, the turbine blade aluminized by the VPA process was covered with the green scale that spalled (Fig. 8a). The largest damage was revealed in the pressure side of the turbine blade. After 10 cycles of oxidation, the turbine blade aluminized by the low-activity CVD method was covered with the gray scale (Fig. 8b). The surface analysis did not reveal any fracturing nor cracking in the scale.

Fig. 8
figure 8

Turbine blades: (a) aluminized by the VPA process and (b) aluminized by the CVD process after 10 cycles of oxidation at 1100 °C

The XRD surface analysis results are presented in Table 2. Al2O3 + HfO2 + NiAlO4 phases were found in the aluminide coating deposited by the VPA method after 240 h oxidation, while Al2O3 + TiO2 phases were found in the aluminide coating deposited by the CVD method (Table 2). NiAl2O4 + NiO spinels were formed in the aluminide coating deposited by the VPA method after 720 h oxidation, while Al2O3 oxide still remains in the aluminide coating deposited by the CVD method after 720 h oxidation.

Table 2 XRD surface analysis results of the aluminide coating

The evident scale spallation was observed on the surface of the aluminide coating deposited by the VPA method after 10 cycles of oxidation. The oxides have nonuniform composition. The chemical composition of the oxides corresponds to NiAl2O4 [56.04O-29.61Al-1.81Ti-1.53Cr-1.11Co-9.48Ni (at.%)] and predominantly Al2O3 oxides [56.57O-38.95Al-0.36Ti-0.68Cr-0.63Co-1.21Ni-1.59Hf (at.%)] (Fig. 9). The digimap analysis of the coating after 10-cycles oxidation confirmed the presence of Hf-rich pegs inside Al2O3 oxides (Fig. 10 and 11).

Fig. 9
figure 9

SEM micrographs of the scales formed on the aluminide coating deposited by the VPA method after 10 cycles of oxidation at 1100 °C in the air atmosphere

Fig. 10
figure 10

The digimap analysis of the aluminide coating deposited by the VPA method after 10 cycles of oxidation at 1100 °C, HfO2 oxide surrounded by Al2O3 oxide

Fig. 11
figure 11

SEM micrographs of the Al2O3 and HfO2 oxides formed on the aluminide coating deposited by the VPA method after 10 cycles of oxidation at 1100 °C in the air atmosphere

Some scale spallation was observed on the surface of the aluminide coating deposited by the low-activity CVD process after 10 cycles of oxidation. Chemical composition of the scale corresponds to the presence of predominantly Al2O3 oxide [47.84O-46.42Al-1.14Ti-1.20Cr-0.14Fe-0.88Co-2.37Ni (at.%)] (Fig. 12). The TiO2 oxide was in some spots observed in place of alumina oxides (Fig. 13 and 14). After 30 cycles of oxidation, the whole surface of the turbine blade aluminized by the VPA process was covered with a green scale, while a blue scale was observed on the surface of the turbine blade aluminized by the CVD method. A mixture of oxides consisting of NiAl2O4 and NiO oxides was formed (Fig. 15). Some HfO2 oxide precipitates surrounded by Al2O3 oxide were found inside NiO oxide (Fig. 16). The mass change of the turbine blade aluminized by the VPA method is about −4.2 mg/cm2 after 30 cycles of oxidation.

Fig. 12
figure 12

SEM micrographs of oxides formed on the aluminide coating deposited by the CVD method after 10 cycles of oxidation at 1100 °C in the air atmosphere

Fig. 13
figure 13

SEM micrographs of Al2O3 and TiO2 oxides formed on the aluminide coating deposited by the CVD method after 10 cycles of oxidation at 1100 °C in the air atmosphere

Fig. 14
figure 14

SEM micrographs of TiO2 oxide formed on the aluminide coating deposited by the CVD method after 10 cycles of oxidation at 1100 °C in the air atmosphere

Fig. 15
figure 15

SEM micrographs of the oxides formed on the aluminide coating deposited by the VPA method after 30 cycles of oxidation at 1100 °C in the air atmosphere

Fig. 16
figure 16

SEM micrographs of Al2O3 and HfO2 oxides formed on the aluminide coating deposited by the VPA method after 30 cycles of oxidation at 1100 °C in the air atmosphere

A continuous and uniform Al2O3 scale without significant changes was found after 30 cycles of oxidation on the surface of the turbine blade aluminized by the low-activity CVD process (Fig. 17). The topology of the coating shows polygonal grains. The spallation occurs along grain boundaries. The chemical composition of this region corresponds to Al2O3 oxide. Some small regions of NiO oxide were also found on the surface of the coating after 30 cycles of oxidation (Fig. 17). The large portion of fine precipitates of HfO2 oxide was found on the surface of the coating. Precipitates were distributed both at grain boundaries and inside grains (Fig. 18).

Fig. 17
figure 17

SEM micrographs of oxides formed on the aluminide coating deposited by the CVD method after 30 cycles of oxidation at 1100 °C in the air atmosphere

Fig. 18
figure 18

SEM micrographs of oxides formed on the aluminide coating deposited by the CVD method after 30 cycles of oxidation at 1100 °C in the air atmosphere: Al2O3 and HfO2 oxides are visible

The residual stress measurements were performed after 30 cycles of oxidation. The results are presented in Table 3.

Table 3 XRD residual stress results after the aluminizing process and 30 cycles of oxidation

It was found that the residual stress in the aluminide coating after 30 cycles of oxidation at the lock, suction side, and pressure side of the turbine blade was compressive (Table 3). Moreover, the residual stress of the turbine blade after the low-activity CVD aluminizing was more compressive in comparison to the residual stress of the turbine blade after the VPA aluminizing.

Discussion

The above experimental results indicate that the aluminide coating deposited by the CVD method protects the turbine blade made of ŻS6K superalloy up to 50-cycles of oxidation at 1100 °C. Although the aluminide coatings deposited by the VPA method is thicker and the higher aluminum content in the aluminide coating was found in comparison to the coating deposited by the low-activity CVD method, the oxidation resistance of the turbine blade coated in the low-activity process was about seven times higher than the turbine blade coated by the VPA method. Warnes et al. (Ref 16) state that in the VPA process the aluminum source (Al-Cr alloy) contains a large sulfur concentration (about 22 ppm). Sulfur could react with hydrogen in either the pack or the aluminizing process to form the hydrogen sulfide gas. Sulfur (as H2S) is transported from the aluminum source (Al-Cr alloy) to the coating. The low-activity CVD aluminizing process takes place without the aluminum source (Al-Cr alloy). The surface is reduced by hydrogen before the aluminizing process. The hydrogen reduction removes sulfur from the surface. Therefore, there is less sulfur than in the coating deposited by the VPA process. The oxidation resistance and the purity of the aluminide coating are related. The removal of impurities from the coating by reactions with hydrogen chloride in the low-activity CVD process produces a “clean” additive layer. Pure aluminide coatings may form a ‘cleaner’ alumina scale that grows slower and is more resistant to oxidation.

It was found that the residual stresses in the aluminide coating deposited by the CVD method were more tensile than in the coating deposited by the VPA method. The different kind of stresses may be associated to different microstructures of coatings after aluminizing processes and different content of impurities. The XRD results indicate the presence of the NiAl phase and MC, M23C6 carbides in the coating deposited in the VPA process. While the XRD results indicate the presence of the NiAl phase in the coating deposited in the CVD process. Moreover, the literature data (Ref 16) report that aluminide coating deposited in the low-activity CVD process has less impurities than the coating deposited in the VPA process. The presence of the NiAl phase, MC and M23C6 carbides in the microstructure of the coating may lead to the increase of the volume of the coating and the decrease of the value of the tensile stresses.

The Al2O3, NiAl2O4 phases, and Hf-rich pegs inside Al2O3 oxides were found after 10 cycles of oxidation of the aluminide coating deposited by the VPA process. The formation of ‘pegs’ is apparently due to the difference of oxygen diffusivity in HfO2 and Al2O3 scales. The formation mechanism has been proposed as follows: Al2O3 scales are formed with embedded HfO2 particles on hafnium-rich areas, such as grain boundaries (Ref 17, 18). Since the diffusivity of oxygen in HfO2 is several orders of magnitude higher than in Al2O3, HfO2 particles along Hf-rich grain boundaries act as short circuit diffusion paths for the oxygen transport, leading to preferentially localized scale thickening in the neighborhood of these particles, causing a deep penetration of the formed HfO2 scales into the substrate (Ref 17, 18). The oxygen transported through this short circuit diffusion paths reacts with Al atoms in the surrounding areas to form Al2O3 scales. Therefore HfO2 ‘pegs’ surrounded by Al2O3 are formed. NiAl2O4 and NiO oxides were found after 30 cycles of oxidation.

The Al2O3 and TiO2 phases were found after 10 cycles of oxidation of aluminide coating deposited by the low-activity CVD process. According to Vialas (Ref 19), HfO2 oxide can also be visible on the surface of the aluminide coating after oxidation. TiO2 oxide probably grew by the fast Ti diffusion from the substrate to the external oxide surface where it can form TiO2 above the existing alumina scale. When an oxide forms at the metal/oxide interface, the volume changes because of the oxide formation. Pilling and Bedworth ratio (Ref 19) of Al2O3 and TiO2 grown on the NiAl phase can be calculated basing on the corresponding molar volumes. It was found that PBR (Al2O3/NiAl) = 1.8 and PBR (TiO2/NiAl) = 2.6. This huge difference means that TiO2 growth on the surface of the oxidized coating should cause large local compressive stresses in the oxide scale. These stresses add to the compressive thermal stress during cooling may promote local cracking or spallation. Al2O3 oxide remains after 30 cycles of oxidation.

The oxidation of the coatings involves the following steps: initial development of the continuous Al2O3 scale and its propagation inwards and scale spallation with subsequent formation of poorly—protective oxides containing Ni. The next step results in the rapid scale growth and increases the tendency to spallation. After just 10 cycles of oxidation, NiAl2O4 spinel appears on the surface of the VPA aluminide coating, which in turn spalls easily producing further catastrophic oxidation. Scale spallation of the aluminide coating deposited by the low-activity CVD method starts along grain boundaries. The scales on the grain boundaries contain larger amounts of substrate elements than within the grains. The difference in composition between boundaries and grains may induce higher stress concentrations and yield earlier spalling at these points, especially as a result of mismatch of thermal stresses during cooling. The residual stresses after aluminizing and 30 cycles of oxidation by both VPA and CVD process were compressive. Moreover, more compressive residual stresses were found in oxides formed on the surface of the aluminide coating deposited by the low-activity CVD process after 30 cycles of oxidation and Al2O3 protective oxide remained.

Conclusions

Aluminizing of the turbine blade by means of VPA and CVD methods lead to the formation of two layers (additive and interdiffusion) of the aluminide coatings. The additive and the interdiffusion layers obtained by the VPA method consists of the NiAl phase and some carbides, while the additive layer deposited by the CVD method consist of the NiAl phase only. It was found that residual stresses in the aluminide coating at the lock, suction side, and pressure side of the blade were tensile. The investigation of oxidation resistance revealed that the aluminide coating deposited by the CVD method is about 7 times better than that deposited by the VPA method. Al2O3 + HfO2 + NiAl2O4 phases were revealed on the surface of the aluminide coating deposited by the VPA method after 240 h oxidation. Meanwhile Al2O3 + TiO2 oxides were found on the surface of aluminide coating deposited by the CVD method after 240 h oxidation. Increasing the time of oxidation from 240 to 720 h led to the formation of the NiO oxide on the surface of the coating deposited by the VPA method. Al2O3 oxide is still visible on the surface of the coating deposited by the CVD method. The residual stresses in the aluminide coating after 30 cycles of oxidation at the lock, suction side, and pressure side of the turbine blade are compressive.