3.1. Microstructure of Nitriding Layer Analysis
Figure 2 presents SEM micrographs and XRD patterns of the nitriding layer. The surface layer of the PN pre-treated sample exhibits a nitride compound layer approximately 25 μm thick, primarily composed of ε-Fe₂₋₃N and γ’-Fe₄N iron nitrides, along with a small amount of Mn₄N and Cr₂N alloy nitrides. The nitride layer can be divided into three distinct sub-layers: the outermost layer (~5 μm from the surface) consists mainly of nanoscale nitride particles forming a loose, porous, sponge-like structure (porosity decreases with depth); the intermediate layer (5–15 μm depth) is composed of columnar crystals oriented perpendicular to the surface, with numerous grain boundaries also perpendicular to the surface. This intermediate layer is brittle and hard, and some structural damage occurred during sample preparation. The innermost layer is denser and free of obvious pores. During the nitriding process, nitrogen atoms first dissolve into the α-Fe matrix. When the nitrogen concentration exceeds the equilibrium solid solubility limit of the α/γ′ phases, a dense γ’-Fe₄N layer forms on the sample surface. Because the diffusion rate of nitrogen within this nitride layer is very low, the nitrogen content in the γ’-Fe₄N phase increases rapidly. Once the nitrogen concentration in γ’-Fe₄N reaches the equilibrium level between the γ′ and ε phases, a harder and more brittle high-nitrogen ε - Fe2-3N phase forms at the outer surface of the nitride layer. Consequently, the outermost compound layer consists of this ε-Fe₂₋₃N phase, which corresponds to the material loss observed during sample preparation. In contrast, the inner portion of the compound layer is a strong, tough, low-nitrogen γ’-Fe₄N phase.
Figure 3 illustrates the change in surface morphology of the sample due to the PN pre-treatment. Compared to the untreated surface, the PN treatment sample surface is completely covered by nanoscale nitride particles. The original polishing marks become nearly indistinguishable, and numerous pores along with a few microcracks are present on the larger nitride particles. These features are attributed to the volume expansion caused by the aggregation and growth of nitrides during the nitriding process [
11,
15]. Studies have shown that such surface characteristics provide improved conditions for subsequent carburizing, facilitating the adsorption and diffusion of carbon atoms [
4,
5,
16].
Figure 4 and
Table 2 show the three-dimensional surface topography and the calculated surface area of the specimen, obtained using laser confocal microscopy. A comparison of the surface topography and area before and after pre-nitriding reveals that prior to pre-nitriding, the specimen’s surface had ridge- like protrusions mostly below 20 μm in height and about 0.5 μm in width. After pre-nitriding, the surface displays numerous uniformly distributed tree-like protrusions, with heights of around 30 μm. Surface area measurements before and after pre-nitriding are summarized in
Table 2. The results indicate that the surface area increased by about 70% after pre-nitriding, with a surface area ratio of 1.701 (compared to 1.044 before pre-nitriding). The dense, uniformly distributed tree-like protrusions on the pre-nitriding specimen’s surface significantly increase its surface area. This larger surface area enhances the contact between the steel and the carburizing atmosphere during treatment, thereby increasing the adsorption of active carbon atoms per unit area and consequently facilitating the absorption and diffusion of carbon atoms.
Changes in surface roughness due to PN pre-treatment were further evaluated by contact angle measurements.
Table 3 shows the measured contact angles. Here,
θdw and
θp represent the intrinsic contact angles of the surface for deionized water and propanetriol, respectively. According to Young [
17]and Wenzel [
18] theories, the following relationship holds:
where
θw is the equilibrium (apparent) contact angle in the Wenzel equation,
θY is the intrinsic contact angle in the Young equation, and γ is the roughness factor of the solid surface. The roughness factor γ is defined as the ratio of the actual solid-liquid contact area to the apparent (geometric) solid-liquid contact area of a rough surface and is always greater than 1 for a rough solid surface. The terms
γsa,
γsl, and
γla represent the solid-gas, solid-liquid, and liquid-gas interfacial tensions, respectively. From the above equation, it can be seen that when the intrinsic contact angle
θY is less than 90°, the apparent contact angle decreases as
θY increases; conversely, when
θY is greater than 90°, the apparent contact angle increases as
θY increases[
19].
The contact angles of both samples are greater than 90°, indicating that the surfaces are non-wetting (hydrophobic). The intrinsic contact angles (
θY) of the PN sample for both liquids are significantly larger than those of the sample without PN, suggesting a substantial increase in surface roughness due to the PN. This is because wetting is actually a composite process involving both liquid–solid and gas–solid interfaces. When the surface is populated by a large number of nanoscale nitride particles, the liquid cannot fully penetrate the asperities, leading to air entrapment and the formation of an air film on the surface. This air film impedes the wetting of the solid by the liquid. Therefore, a larger contact angle corresponds to poorer wetting, higher surface roughness, greater pore volume, and a larger gas–solid interfacial area [
20,
21]. The much higher contact angle observed for the PN sample indicates that its surface roughness is significantly enhanced, which greatly promotes the adsorption of carbon atoms during carburizing. This leads to a rapid increase in surface carbon concentration, accelerates inward diffusion, and consequently improves carburizing efficiency.
3.2. Microstructure of Carburized Layer Analysis
Figure 5 shows the microstructure of the carburized layer in the samples without and with PN. The sample without PN exhibits almost no carbide precipitation, and the martensite in the carburized layer is relatively coarse. In contrast, the PN sample shows finer martensite and a significant amount of carbide precipitation. The carbides precipitated in the surface layer are primarily located along prior austenite grain boundaries, appearing as coarse granular and angular blocks at a depth of about 50 μm from the surface. In the sub-surface layer, the precipitates are very fine (approximately 100–600 nm) and are found on grain boundaries and within the martensitic matrix. Both the volume fraction and size of these precipitates gradually decrease with increasing depth. These observations indicate that pre-nitriding not only refines the martensitic microstructure of the carburized layer but also promotes carbide precipitation.
XRD results for the two groups are presented in
Figure 6. In the sample without PN, the diffraction peaks of γ-Fe are very weak and no Fe
3C peaks are observed, indicating that the matrix consists primarily of martensite (α′-Fe) with a small amount of retained austenite (γ-Fe). In the sample with PN, however, diffraction peaks of Fe
3C and γ-Fe appear at both the surface and sub- surface, with much stronger peaks in the surface layer. This indicates that the matrix consists of α′-Fe and retained γ-Fe, and the content of γ-Fe decreases with depth. This is attributed to the high carbon content at the surface, which lowers the martensite finish temperature; consequently, after quenching, more austenite remains untransformed (retained austenite).
Figure 7 shows an EPMA elemental map near the surface of the PN pre-treated sample. As shown in the figure, the coarse, granular, and angular cementite precipitates along the surface grain boundaries are enriched in chromium (Cr). This is because carbide-forming elements such as Cr tend to segregate at grain boundaries, and the high carbon content at the surface promotes the nucleation and growth of carbides at these boundaries. Subsequently, Cr atoms diffuse into the cementite, replacing some of the iron (Fe) atoms to form alloyed cementite. In contrast, the fine granular cementite in the subsurface layer contains no Cr. Furthermore, a few pores are observed in the carburized layer at a depth of approximately 10 μm from the surface. These pores result from nitrogen atoms combining to form N₂ gas during the carburizing process; the gas escapes and leaves behind voids in the layer [
4,
13].
3.3. Hardness and Carbon Concentration Analysis
Figure 8 shows the hardness and carbon concentration profiles in the carburized layer for both sample groups. At the same depth, the hardness and carbon concentration of the PN sample are significantly higher than those of the sample without PN. The effective hardened layer depth and the hardness at equivalent depths in the carburized layer increased by approximately 0.15 mm (~18%) and 75 HV (~10%), respectively, with PN pre-treatment. Additionally, the hardness gradient in the layer became more uniform. In particular, the hardness variation within the top 0.55 mm was much smaller in the PN sample compared to the untreated sample. In the PN sample, the hardness increased from 771 HV at the surface to 816 HV at 0.1 mm, and then gradually decreased to 760 HV at 0.55 mm; in the sample without PN, the hardness increased from 722 HV to 748 HV at 0.1 mm, then dropped more rapidly to 640 HV by 0.55 mm. For carbon concentration, the sample without PN showed a steady decrease from 0.77% at the surface to 0.39% at 1.4 mm. In contrast, the PN sample exhibited a sharp drop from 1.65% at the surface to 0.95% at 0.2 mm, followed by a slower decline (similar to the untreated sample) from 0.2 mm to 1.4 mm. The higher carbon content at the surface increases the hardness of the carburized layer, which not only improves wear resistance but also suppresses the formation of surface cracks, thereby enhancing fatigue strength[
22,
23]. Furthermore, the greater effective case depth achieved with PN contributes to improved fatigue strength of the carburized steel.[
24] By increasing the carbon content in the carburized layer, PN refines the martensitic structure and promotes carbide precipitation, thereby amplifying the fine-grain strengthening and second-phase strengthening effects [
25]. As a result, both the maximum hardness and the effective case depth of the carburized layer are improved.
When carbon atoms diffuse in austenite, they preferentially migrate along crystal defects such as grain boundaries and sub-grain boundaries, because the activation energy for diffusion at these sites is about half that within the grains and the diffusion coefficient is correspondingly higher. This significantly accelerates carbon diffusion [
26]. Once the carbon concentration reaches a critical level, carbides begin to precipitate at the grain boundaries and continue to grow. Since the carbon concentration is highest at the surface, carbide growth is fastest at the surface [
27,
28]. This explains why the carbon concentration at the surface is much higher than in the sub-surface layer. This disparity can be reduced by increasing the diffusion time or the number of boost diffusion cycles in the vacuum carburizing process.
3.4. Diffusion of Nitrogen Atoms During Carburizing
Figure 9 shows the nitrogen concentration profile in the PN sample, before and after vacuum carburizing. Before carburizing, the nitride layer on the surface hinders nitrogen diffusion inward, resulting in a very high nitrogen concentration in the surface layer and a much lower concentration in the deeper diffusion layer. After carburizing, however, the nitrogen content near the surface is greatly reduced (for example, at ~0.1 mm depth) and it increases with depth in the carburized layer. This phenomenon occurs because the ε-Fe₂₋₃N and γ’-Fe₄N phases formed by pre-nitriding transform and decompose into nitrogen-rich austenite during the carburizing heat. Moreover, carbon and nitrogen atoms both occupy octahedral interstitial sites in austenite and mutually repel each other; thus, the inward diffusion of carbon during carburizing pushes nitrogen atoms deeper into the material. Consequently, after carburizing, the nitrogen content increases with depth in the carburized layer. In addition, some nitrogen atoms form N
2 gas during carburizing, creating small pores in the surface layer of the case. This outgassing also contributes to the marked reduction of nitrogen in the near-surface region after carburizing. Given that the steel contains only 0.056% Ti, only a small fraction of nitrogen atoms combined with Ti to form refractory TiN particles; thus, most nitrogen atoms remain in solid solution. In austenite, interstitial solute atoms cause lattice distortion and increase the lattice parameter. Therefore, nitrogen in solid solution expands the lattice and enlarges the interstitial sites [
29]. Carbon atoms diffuse in austenite via an octahedral–tetrahedral–octahedral pathway (octahedral gap → tetrahedral gap → octahedral gap → tetrahedral gap). The enlarged interstitial sites due to dissolved nitrogen reduce the diffusion resistance for carbon atoms [
30]. In other words, a small amount of nitrogen in solid solution facilitates carbon diffusion.
Figure 9.
Nitrogen concentration of samples.
Figure 9.
Nitrogen concentration of samples.
Figure 10.
Lattice distortion in interstitial solid solution.
Figure 10.
Lattice distortion in interstitial solid solution.
The above experimental results demonstrate that PN significantly improves both the carburizing efficiency and the quality of the carburized layer. There is a notable increase in the carbon content of the carburized layer, primarily due to enhanced carbon diffusion. Additionally, nitrogen atoms in solid solution induce lattice distortion, which provides some strengthening. The underlying mechanisms are as follows: first, the nitride compound layer formed on the sample surface introduces numerous nanoscale nitride particles, along with nanoscale cracks and pores, which increase surface roughness. This, in turn, greatly enlarges the surface area available for carbon atom adsorption, thereby enhancing the adsorption and inward diffusion of carbon. Second, in the subsurface layer, the presence of many grain boundaries oriented perpendicular to the surface, together with micro-pores formed by nitrogen escaping as N2, provides additional fast-diffusion paths. Finally, the nitrogen atoms introduced by PN into the austenite solid solution increase the lattice constant and the size of interstitial sites. The enlarged interstitial sites reduce the resistance to carbon diffusion, thereby promoting carbon diffusion.