Introduction

Metallic glasses possess an excellent combination of properties, which include high mechanical strength, high wear resistance and high corrosion resistance. These properties originate from a lack of the long-range order in the atomic structure of the glasses (Ref 1,2,3). Fe-based metallic glasses are promising materials for developing protective coatings to withstand corrosive environments and wear (Ref 4,5,6). Recently, efforts have been made to produce Fe-based metallic glass coatings by thermal spraying, such as, high-velocity oxy-fuel (HVOF) (Ref 7), plasma (Ref 8), detonation (Ref 9) spraying, as well as by laser cladding (Ref 10). The advantages of detonation spraying over other deposition techniques are a high productivity and a pulse nature of the deposition process. Xie et al. (Ref 11) showed that detonation coatings obtained from the Fe48Mo14Cr15Y2C15B6 powder provide better mechanical properties than coatings produced by plasma spraying and HVOF. In our studies (Ref 12, 13), parameters of the detonation spraying process were determined for depositing Fe66Cr10Nb5B19 coatings. Dense coatings with amorphous structure and high bonding strength to steel substrates were obtained.

Due to a limited ductility, metallic glass coatings can exhibit low fracture resistance and toughness, which reduce the scope of their application in industry (Ref 14). Laminated structures or metallic glass matrix composites with a crystalline second phase can be designed to increase the fracture toughness of the coatings. The essence of the first approach is to form multilayer structures with alternating amorphous and crystalline layers. As reported by Zhang et al. (Ref 15), Fe-based amorphous alloy/NiCrAl multilayer structure possess a much higher toughness than the monolithic amorphous alloy coating. The second approach is to form a coating from a mixture of a Fe-based alloy and second-phase particles. Fe-based amorphous alloy coatings containing 8 vol.% of stainless steel particles showed an improved fracture resistance relative to the monolithic amorphous coatings (Ref 16). It was shown that the stainless steel particles could effectively absorb the fracture energy. However, the addition of the stainless steel powder decreases the corrosion resistance of the composite coatings, as pitting corrosion preferentially occurs at the interface between the crystalline particles and the amorphous matrix (Ref 17). In-situ crystallization resulting in the formation of second-phase particles in the coatings upon deposition is an alternative route (Ref 18, 19). However, the forming crystals can become enriched in Cr, creating Cr-depleted interfaces, which suffer localized corrosion in case of excessive crystallization (Ref 20, 21).

The tribological properties and corrosion resistance of amorphous alloy coatings can be considerably influenced by the presence of embedded particles, such as particles of amorphous carbon (Ref 22), WC-Co alloys (Ref 23), or nitrides (Ref 24). The amorphous matrix ensures a high corrosion resistance of the coatings. The crystalline particles of ceramic nature may increase the wear resistance of the amorphous coatings.

Yoon et al. (Ref 25) reported the properties of Fe-based amorphous alloy-B4C composite coatings. As the B4C content in the composite coatings increases, their wear resistance tends to improve relative to that of B4C-free coatings. It was shown that boron carbide particles play an important role, acting as solid “lubricants” during the sliding friction wear tests. As shown in ref. (Ref 26), the modification of Fe-based amorphous alloy coatings with ceramic particles does not usually affect the corrosion resistance of the coatings, as no galvanic coupling occurs. It should also be noted that the introduction of ceramic particles into an amorphous alloy matrix does not lead to the formation of Cr-depleted interfaces. The addition of Al2O3 particles into Fe-based amorphous alloy coatings improves the toughness of the material owing to crack blockage and deflection by the particles, and the microcrack formation inside the Al2O3 particles (Ref 27). The literature overview shows that the formation mechanisms and microstructural features of Fe-based amorphous alloy composite coatings have not been extensively studied. Further research in this area would allow developing coatings with novel sets of properties.

In the present study, Fe66Cr10Nb5B19 metallic glass coatings modified with Al2O3 particles were fabricated by detonation spraying. The effect of the Al2O3 content (in the 20–60 wt.% range) in the initial powder mixture on the phase composition and microstructure of the composite coatings was investigated by X-ray diffraction (XRD) and scanning electron microscopy (SEM). Vickers hardness, bonding strength (pin test method) and tribological behavior (reciprocating ball-on-flat sliding test) of the composite coatings were examined. The wear resistance of the composite coatings was compared with that of Al2O3-free amorphous alloy coatings and stainless steel.

Materials and Methods

The Fe66Cr10Nb5B19 powder was obtained by gas atomization using a HERMIGA 75/5VI gas atomizer (Phoenix Scientific Industries Ltd., UK). The powder was sieved to separate the 20–40 µm fraction. The starting Al2O3 powder had a purity of > 99.5 wt.% and particles in the 20–45 μm range (GTV Wear Protection GmbH, Germany). The metallic glass powder was mixed with the Al2O3 powder. The Al2O3 content in mixture was 20, 40 or 60 wt.%. The mixtures were prepared in a mortar; the duration of mixing was 15 min.

Detonation spraying of the powder mixtures was performed using a computer-controlled detonation spraying (CCDS2000) system (Ref 28). The barrel had a variable cross section (Ref 29). The total length of the barrel was 1000 mm. The diameter of the combustion chamber and the acceleration section was 20 and 16 mm, respectively. The spraying distance was 200 mm. Coatings were deposited at an O2/C2H2 molar ratio of 1.1 and an explosive charge of 50%. (A fraction of the barrel volume was filled with the gas mixture.) Nitrogen was used as a carrier gas. Previous studies have shown that, under such conditions, spraying allows obtaining high-quality coatings in terms of the amorphous phase content, adhesion, porosity and hardness (Ref 12). The composite coatings were deposited on carbon steel substrates (carbon steel, Grade St3, GOST 380-2005, analog to ASTM A570). The thickness of the deposited coatings was 250–300 µm. Before spraying, the substrates were sandblasted to ensure better adhesion of the coatings. The temperatures and velocities of the particles at the exit of the barrel were calculated using LIH software developed at Lavrentyev Institute of Hydrodynamics SB RAS (Ref 30, 31).

XRD analysis of the powders and coatings was carried out using a Bruker D8 ADVANCE diffractometer (Bruker AXS, Germany). The crystalline phase content of the starting Fe66Cr10Nb5B19 powder was determined by the Rietveld method using TOPAS 4.2 software (Bruker AXS, Germany). XRD patterns were taken from the polished surfaces of the coatings.

The morphology of the powders and microstructure of the coatings were studied by SEM in the secondary electron (SE) imaging mode using an EVO50 XVP microscope (Carl Zeiss, Germany) coupled with an energy-dispersive spectroscopy (EDS) X-Act system (Oxford Instruments, UK). The distribution of Al2O3 particles in the composite coatings was determined by elemental mapping.

The porosity of the coatings and the content of alumina particles in the coatings were determined using OLYMPUS Stream Image Analysis Software “Stream Essentials 1.9.1” (OLYMPUS, Japan). Optical images of the samples were recorded on an OLYMPUS GX-51 Optical Microscope (OLYMPUS, Japan). The fracture surface of the coatings was studied on a TM-1000 Tabletop microscope (Hitachi, Japan) in the back-scattered electron (BSE) imaging mode.

The hardness of the coatings was measured on polished cross sections using a Vickers hardness testing device (402MVD, Wolpert Wilson Instruments, Germany) under a load of 1 kg with a dwell time of 15 s. The average values of hardness were determined from 10 measurements.

The wear behavior of the coatings and stainless steel (grade 12Cr18Ni10Ti, GOST 2590-2006, analog to ASTM 321) was investigated by a standard test method for linearly reciprocating ball-on-flat sliding wear (ASTM G133-05) using a UMT-2 wear machine (Bruker Nano GmbH, Germany) (Ref 32). This test method uses a hard WC-6Co ball 6.35 mm in diameter. The ball was sliding against a flat specimen. Before the wear tests, the coatings and stainless steel surfaces were polished to a mirror finish. The ball and the sample were degreased with acetone and dried before testing to ensure nominal dry sliding conditions (40–60% relative humidity).

The normal load (25 N) was applied vertically downward through the ball against a flat coating mounted horizontally. The sliding speed was 5 mm s−1, and the stroke length was 5 mm. The total sliding distance was 100 m. An analytical balance, with an accuracy of 0.1 mg, was used for weighing the coating samples before and after each test. After the wear test, a Contour GT-K1 3D optical measurement system (Bruker Nano GmbH, Germany) was used to determine the worn volume of the coatings and stainless steel. The specific wear rate (κ) of the coatings and stainless steel was calculated by the following equation (Ref 33):

$$ k = V_{w} N^{ - 1} S^{ - 1} , $$
(1)

where Vw is the worn volume, N is the applied load, and S is the sliding distance. Afterward, the worn surfaces and the debris from the coatings were examined by SEM/EDS for gaining a better understanding of the wear mechanism of the coatings under dry sliding conditions.

The bonding strength of the coatings was determined by the pin test method (Ref 34,35,36). A conical pin with a flat end (1.5–1.8 mm in diameter) was placed into the conical hole of the matrix. After that, the end of the pin and the surface of the matrix were coated simultaneously. The bonding strength was determined by applying a force to the pin. The bonding strength was calculated by Eq 2:

$$ \sigma = F \, \left( {\pi r^{2} } \right)^{ - 1} , $$
(2)

where F is force and r is the radius of the flat end. The reported values of the bonding strength are averaged from five measurements. The standard deviation is also reported.

Results and Discussion

Characteristics of the Starting Powders and Fe66Cr10Nb5B19-Al2O3 Powder Mixtures

The XRD analysis revealed the predominance of an amorphous phase in the starting Fe66Cr10Nb5B19 powder (Fig. 1a). The crystalline phase content in this powder was ~ 5%. The glass transition Tg and crystallization Tx temperatures of the Fe66Cr10Nb5B19 alloy were determined in our previous work: Tg = 794 K, Tx = 846 K. A supercooled liquid region of 52 °C is an indicator of high glass-forming ability (Ref 13).

Fig. 1
figure 1

Characteristics of the feedstock powders: (a) XRD pattern and (b) SEM image of the Fe66Cr10Nb5B19 powder; (c) SEM image of the Al2O3 powder. Micrographs were taken in the SE imaging mode

SEM images of the Fe66Cr10Nb5B19 and alumina powders are shown in Fig. 1(b) and (c). The Fe-based alloy particles are spherical. This shape is characteristic of gas-atomized powders. The Al2O3 particles possess an irregular shape. Figure 2(a) shows the XRD patterns of the Fe66Cr10Nb5B19-Al2O3 feedstock powder mixtures. Narrow reflections in the patterns correspond to α-Al2O3.

Fig. 2
figure 2

XRD patterns of the feedstock powder mixtures (a) and coatings obtained by detonation spraying (b)

The calculated velocities and temperatures of the Fe66Cr10Nb5B19 and Al2O3 particles 20, 30 and 40 μm in size are presented in Table 1. The solidus temperature of the Fe66Cr10Nb5B19 alloy was determined as 1442 K (Ref 13). The melting point of alumina is 2319 K. A difference between the densities of the Fe-based alloy (7.58 g cm−3) and alumina (3.96 g cm−3) leads to differences in the particle velocities: The velocities of Al2O3 particles are higher than those of Fe66Cr10Nb5B19 particles. Alumina particles with a size of 20 μm, 30 μm and 40 μm reach velocities of 771, 717 and 631 m s−1, respectively. Under the selected spraying conditions, the Fe-based 30-µm alloy particles start melting, while Al2O3 particles of the same size remain in the solid state (heated up to 681 K). Since the Al2O3 particles are still solid, some particles can ricochet off the substrate or a previously deposited layer. The ricocheting events reduce the concentration of Al2O3 particles in the deposited coatings relative to the feedstock powder mixture. In addition, high velocities of brittle alumina particles create conditions for particles’ crushing upon impact.

Table 1 Calculated temperatures and velocities of Al2O3 and Fe66Cr10Nb5B19 particles at an explosive charge of 50% and an O2/C2H2 molar ratio of 1.1 for the particles with the diameter of 20, 30 and 40 μm

Microstructure and XRD Analysis of the Coatings

Figure 2(b) shows the XRD patterns of detonation coatings obtained by spraying the Fe66Cr10Nb5B19 powder and Fe66Cr10Nb5B19-Al2O3 mixtures. A halo in the patterns (2θ = 40–50°) indicates the presence of an amorphous phase in the composite coatings. The content of Al2O3 in the composite coatings was significantly lower than in the corresponding feedstock mixtures (Table 2). Because of a low concentration, it was rather difficult to detect Al2O3 in the coating by the XRD analysis. However, peaks of alumina were identified in the XRD pattern of the composite coating obtained from the feedstock powder mixture containing 60 wt.% of Al2O3.

Table 2 Concentration of Al2O3, porosity, Vickers hardness and bonding strength of detonation coatings

The cross sections of the Al2O3-free coating and coatings modified with Al2O3 particles are shown in Fig. 3 and 4, respectively. The coatings exhibit a dense lamellar structure (the porosity is below 3%) typical of coatings obtained by thermal spray. The coatings demonstrate a greater number of pores and microcracks as the alumina content in the initial powder mixtures increases (Fig. 4a, b, and c). The detonation coatings were formed by molten (partially molten) particles of the Fe-based alloy and solid Al2O3 particles. It should be emphasized that effective densification upon deposition is favored when the sprayed particles reach the substrate in a partially molten state. A concentration of alumina of 60 wt.% in the feedstock powder corresponds to 74 vol.%. So, in this mixture, the content of Fe66Cr10Nb5B19 powder is only 26 vol.%. Such a low concentration of the alloy does not allow forming a defect-free coating. Fe and Al elemental maps are presented in Fig. 5. The maps were recorded from selected areas of the cross sections of the coatings with different alumina concentrations. A coating obtained from the mixture containing 20 wt.% of Al2O3 showed alumina inclusions in an amorphous matrix, but the number of particles was low (Fig. 5a). Spraying of mixtures containing 40 and 60 wt.% of alumina resulted in the formation of coatings with a relatively uniform distribution of the ceramic particles in an amorphous matrix (Fig. 5b and c). It is seen that, despite significant Al2O3 losses during spraying, the higher is the alumina content in the feedstock powder, the higher is the concentration of alumina in the coatings. As the Al2O3 particles crush upon impact onto the previously deposited layers, the inclusions in the coatings are smaller than the Al2O3 particles in the starting mixture. The Al2O3 particles tend to form thin interlayers (with thicknesses of 5–10 μm) between the layers of an amorphous matrix (Fig. 5b and c).

Fig. 3
figure 3

Cross-sectional images of the Fe66Cr10Nb5B19 detonation coating (different magnifications). Micrographs were taken in the SE imaging mode

Fig. 4
figure 4

Cross-sectional images of the detonation coatings obtained by spraying the powder mixtures with different Al2O3 concentrations: (a) 20 wt.% of Al2O3; (b) 40 wt.% of Al2O3; and (c) 60 wt.% of Al2O3. Micrographs were taken by SEM in the SE imaging mode

Fig. 5
figure 5

SEM images and elemental Al and Fe distribution maps obtained from selected areas of the cross section of the composite coatings fabricated by spraying the powder mixture with 20 wt.% Al2O3 (a), 40 wt.% Al2O3 (b) and 60 wt.% Al2O3 (c). Micrographs were taken in the SE imaging mode

As the temperature of the alumina particles is relatively low (Table 1), the cohesion between those and the amorphous matrix is weak. The reaction products at the amorphous matrix/alumina particle interface are absent, as concluded from results of the EDS line analysis (Fig. 6). Investigations of the fracture surface morphology of the coating obtained from the powder mixture containing 20 wt.% of Al2O3 confirm that the coating has a dense structure (Fig. 7). The alumina inclusions (indicated by arrow in Fig. 7a) are located between the layers of an amorphous matrix. The amorphous alloy layers show high cohesion (to each other), as no signs of matrix delamination were found.

Fig. 6
figure 6

SEM image of an area containing an Al2O3 particle (a) and the results of the EDS line scanning analysis (b). Micrograph was taken by SEM in the SE imaging mode

Fig. 7
figure 7

SEM image of the fracture surface of the detonation coating obtained by spraying the powder mixture containing 20 wt.% of Al2O3 (a) and a magnified image of an Al2O3 particle (b). Micrographs were taken in the BSE imaging mode

Hardness, Bonding Strength and Wear Resistance of the Coatings

The experimentally measured characteristics of the coatings (the concentration of Al2O3, porosity, hardness, bonding strength to the substrate) are presented in Table 2. The hardness values of the composite and Al2O3-free coatings did not differ significantly (considering the given values of standard deviation). The coatings in the studied series showed close values of bonding strength (130 MPa).

In Fig. 8, the coefficient of friction (COF) measured under dry reciprocating sliding conditions is plotted against the sliding distance for samples of the Fe66Cr10Nb5B19 coating, composite coatings and stainless steel. The wear process can be divided into a running-in stage and a steady-state stage. Fluctuations of COF at the steady-state stage are indicative of high wear rates. Detonation coatings showed relatively stable COFs at the steady-state stage, which was reached after a sliding distance of less than 30 m. The COF measured for the stainless steel sample was very unstable after a distance of 30 m: It increased from 0.5 to 0.6. (The average value was 0.56.) This can be attributed to a low hardness (~ 200 HV) and a high ductility of stainless steel.

Fig. 8
figure 8

The coefficient of friction versus the sliding distance. The plots were obtained for the stainless steel, Fe-based alloy coating and composite coatings (with different concentrations of Al2O3) sample under dry linearly reciprocating wear conditions under a normal load of 25 N. The concentration of Al2O3 in the feedstock powder mixtures is given on the plot

At the steady-state stage, the unmodified coating and the composite coating produced from the mixture containing 20 wt.% of Al2O3 showed high COF; the average value was equal to 0.69 and 0.70, respectively. The average COF measured for coatings obtained from mixtures containing 40 and 60 wt.% of Al2O3 was 0.66 and 0.64, respectively. A reduction in COF is accompanied by an increase in the specific wear rate of the coatings, as shown in Table 3. This correlation was also reported in Zhang et al. (Ref 37) for spark plasma sintered materials.

Table 3 Weight loss and specific wear rate of stainless steel, unmodified Fe66Cr10Nb5B19 coating and composite coatings

The weight losses and specific wear rate of the Fe66Cr10Nb5B19 coating and composite coatings are given in Table 3. The Fe66Cr10Nb5B19 coating and composite coatings obtained from mixtures containing 20 and 40 wt.% of Al2O3 demonstrated close values of weight losses and specific wear rates. The coatings obtained from the powder mixture containing 60 wt.% of Al2O3 showed an increased specific wear rate. A general conclusion from the data presented in Table 3 is that the specific wear rate of the coatings is significantly lower than that of stainless steel.

Figure 9 shows the worn surface of composite coatings obtained from mixtures containing 20 and 60 wt.% of Al2O3. The observed morphology of the worn surface is typical of brittle fracture with detached lamellae (Ref 25, 38). It was shown that, under a high cyclic load, the coating lamellae may experience delamination (Ref 39). The detected lamellae indicate that fatigue wear is one of the main wear mechanisms of the composite coatings. The main reason for delamination could be a relatively low temperature developing in the coating-ball contact zone (not reaching Tg of the Fe66Cr10Nb5B19 alloy).

Fig. 9
figure 9

Worn surfaces of the composite coatings fabricated from the powder mixtures containing (a, b) 20 wt.% Al2O3; (c, d) 60 wt.% Al2O3. SEM images were obtained in the SE imaging mode at different magnifications. Rectangles in (b) and (d) are the areas selected for the EDS analysis, the results of which are summarized in Fig. 10

The number of delaminated lamellae was insignificant on the worn surface of the composite coating obtained from the powder mixture containing 20 wt.% Al2O3 (Fig. 9a). A larger number of delaminated particles on the worn surface of the coating obtained from the powder mixture containing 60 wt.% Al2O3 (Fig. 9c) can be explained by low cohesion between the ceramic and the matrix layers. The results of the elemental analysis of the worn surface prove this assumption (Fig. 10). As shown in Fig. 10(b), a higher concentration of aluminum was detected on the worn surface of the coating obtained from the powder mixture containing 60 wt.% Al2O3 (rectangle in Fig. 9d) than on the worn surface of the coating obtained from the mixture containing 20 wt.% Al2O3 (rectangle in Fig. 9b). The presence of tungsten on the worn surface was due to material transfer from the WC-6Co ball to the sample surface. The transfer was possible because of the difference in the nature of chemical bonding in the coating material and WC (Ref 40).

Fig. 10
figure 10

Results of the elemental analysis of the worn surfaces of the composite coatings obtained from powder mixtures containing 20 wt.% Al2O3 (a) and 60 wt.% Al2O3 (b). The areas selected for the analysis are shown in Fig. 9

During the wear tests, the delaminated particles did not leave the friction surface and acted as abrasive particles, contributing to microcutting (Fig. 9) and increasing the specific wear rate. The delaminated particles were of flaky shape and had diameters in the 20–80 µm range. Similar flaky debris was observed when a Fe41Co7Cr15Mo14C15B6Y2 bulk metallic glass and plasma-sprayed Fe68.8C7Si3.5B5P9.6Cr2.1Mo2Al2 amorphous alloy coatings were tested (Ref 25, 41). During the wear tests, the energy dissipation causes heating of the contact zone and oxidation of the sliding surface. In addition to fatigue and abrasion wear by delaminated particles, oxidation wear can be suggested to play a role (Ref 42). However, the main wear mechanisms of the coatings tested in the present work are assumed to be fatigue and abrasion wear. It should be noted that the results of wear investigations are in agreement with refs. (Ref 22).

Conclusion

Composite coatings were fabricated by detonation spraying of Fe66Cr10Nb5B19 metallic glass-(20–60 wt.%) Al2O3 powder mixtures. The structural features and tribological properties of the coatings were investigated. The structural analysis has not revealed crystallization or oxidation of the amorphous matrix in the sprayed coatings. The alumina particles acquired high velocities during the detonation spraying process and crushed upon impact. Furthermore, the ricocheting events of the alumina particles did not allow maintaining the concentration of alumina in the coatings equal to that in the feedstock mixture. The specific wear rate of the coatings modified with 1.5 and 4 vol.% of Al2O3 was about one-fifth of the specific wear rate of stainless steel. Fatigue and abrasion appeared to be the dominant wear mechanisms of the composite coatings. Incorporating Al2O3 particles into an alloy matrix forming composite particles (agglomerates, composite feedstock) is possible by co-injection during gas atomization or through high-energy milling of the mixtures. The use of composite feedstock may be beneficial for reducing the intensity of ricocheting events upon deposition.