3.1. Deposited Sample Morphology Analysis
Cylindrical samples were printed using CSAM technology with powders P1, P2, and C, as depicted in
Figure 7a,e,i. These samples, with heights ranging from 6 mm to 12 mm and diameters approximately 5.5 ± 0.5 mm, close to the nozzle diameter of 5 mm. The surface of the cylindrical samples exhibited a "wrinkled" structure, indicating instability during powder deposition and subsequently resulting in a change in deposition diameter. In addition, these parallel wrinkles suggest a consistent layer-by-layer deposition.
It is noteworthy that the deposition rates of powders P1, P2, and C in CSAM are 5%, 2.1%, and 3.5%, respectively, where the deposition rate is defined as the ratio of the mass of the powder material deposited on the substrate to the total mass of the powder spraying during the CSAM process. Due to the varying deposition rates of P1 and P2, spraying a mixture of these powders does not produce a deposited material in P1 and P2 proportions consistent with the original powder mixture. To mitigate the effects of these differences in deposition efficiency, this study utilized a compaction method to bond P1 and P2 relatively together to produce powder C.
Subsequently, the cylindrical samples were subjected to two distinct curing processes for curing. The first method was conducted by controlling the heating rate. As illustrated in
Figure 7b,f,j, the samples printed using P1, P2, and C experienced significant softening deformation at a high heating rate of 2 °C/min. Conversely, when the heating rate was reduced to 0.1 °C/min, as illustrated in
Figure 7c,g,k, the samples almost retained the cylindrical shape, although the heating duration extended to 16.7 h.
The second method utilized a stepwise isothermal curing process, as depicted in
Figure 6, to sequentially cure the components and manage the deformation.
Figure 7d,h illustrate that samples printed using P1 and P2 softened at their respective isothermal conditions of 85 °C and 150 °C. In contrast, the sample printed using C, as shown in
Figure 7l, did not display any softening deformation with the stepwise curing process. It retained the cylindrical shape and the wrinkled surface texture observed in the initial morphology depicted in
Figure 7i. Moreover, it is found that the corresponding stepwise curing process required only 1.5 h, significantly less than the time required by the low heating rate method (i.e., 16.7 h).
Therefore, employing composite powder material C for CSAM printing and combining with a stepwise curing process can significantly mitigate the deformation issue both during the 3D-printing and curing stages.
3.2. Deposition and Curing Mechanism Analysis
During the CSAM process, thermosetting powders P1, P2, and C can be successfully deposited at room temperature. At this temperature, P1, P2, and C are in a glassy state, exhibiting brittle characteristics. Traditionally, brittle materials have significant challenges for CSAM applications, primarily due to their tendency to fracture upon impact, which normally results in thin films rather than substantial deposits [
23,
24]. However, the CSAM samples printed using P1, P2, and C demonstrated the ability to form cylindrical structures, indicating their potential for additive manufacturing applications. Thus, the deposition mechanism of P1, P2 and C should be significantly different from that of other brittle materials.
To investigate the corresponding deposition mechanism of thermosetting powders during the CSAM process, the particle impact velocity was estimated firstly. The average particle velocity of P1, P2, and C powders at the nozzle exit was in the range of 378~387 m/s, as predicted with the one-dimensional steady gas-dynamic model [
25,
26]. This high velocity provided the necessary conditions for severe plastic deformation of the particles upon impact. The surface morphologies of the samples printed using P1, P2, and C were examined, as shown in
Figure 8. A number of sharp ridges and valleys were observed, indicating that the heat generated during impact was insufficient to cause complete melting of the whole particle.
Meanwhile, the fracture surface of the samples printed using P1 and P2 was observed, as shown in
Figure 9a,b. It can be seen that the original form of the powder particles was no longer recognizable, and the contact interface between particles was also indistinguishable, indicating severe plastic deformation had occurred during the powder deposition. Additionally, a number of pores were found throughout the fracture surface of the samples, which could be categorized into two types based on their shapes, i.e., irregular pores with diameters close to 20 μm and small round pores with diameters of a few micrometers. Similar to the cold spraying of metal powders [
27,
28], air could be trapped during the powder deposition process, leading to the formation of the large irregular pores. For the dense small circular pores, they should be generated during the impact of the particles. Our prior research indicates that particles deposited onto surfaces display lower melting peaks in DSC compared to the original powder particles [
29]. This observation suggests that local melting occurred during impact, activating latent curing agents and accompanying release of blocking agents, where gas was generated during the decomposition or volatilization of the blocking agent to form the small circular pores [
30]. Hence, the presence of these micro-sized pores implies that particle melting occurred at the impact surface.
Based on above observations, the deposition mechanism of P1, P2 and C is due to the severe plastic deformation caused by high-speed particle impact, accompanied by significant heat generation. This thermal effect leads to local melting of the particle impact zone and transition from glassy state to viscous flow dynamic. Consequently, fusion occurs at the contact surface of the particles, promoting a strong bond, while also leading to the formation of small pores on the fracture surface.
To analyze the changes of the two components P1 and P2 in composite materials C during stepwise isothermal curing, the fracture surface of the samples, printed using P1 and P2, before and after heating was observed.
Figure 9c,d display the fracture morphologies of the samples after the first stage of heating. After heating at 85 °C for 1 h, in addition to small circular pores, there are also large circular pores with diameters in the range of tens of microns for the samples printed using P1. This indicates that the latent curing agent decomposed during heating, releasing a significant amount of gas, which expanded the pores as the epoxy resin melted. In contrast, the number of large pores in the samples printed using P2 was significantly less than that in the samples printed using P1, and some of the pores are irregular in shape. This may be attributed to the fact that no significant curing reaction occurs in the samples printed using P2, and most of the curing agents had not decomposed to generate gas.
Figure 9e,f show the fracture morphologies of the samples printed using P1 and P2 after the second stage of heating. The fracture surface of the samples printed using P1 displayed more large pores compared with the first stage of heating. This could be attributed to that the latent curing agent further decomposed at higher temperatures, producing more gas and forming more large pores. Similarly, the fracture surface of the samples printed using P2 also exhibited more large pores after the second stage of heating.
In addition, to investigate the effect of stepwise isothermal curing on the thermal properties, DSC tests were conducted on the samples printed using P1 and P2. As shown in
Figure 10, the DSC curves of P1 and P2 before heating exhibited significant endothermic peaks at around 55 °C and 70 °C, indicating the existence of crystallization in the epoxy resin. In addition, significant exothermic peaks suggest that the samples did not complete the curing reaction during the CSAM process, indicating the need for post-heating curing treatment.
After heating at 85 °C for 1 h in the first stage, the endothermic peak of P1 disappeared, and the exothermic peak significantly decreased, indicating that the curing reaction of P1 had been essentially completed in the first heating stage. In contrast, the endothermic peak of P2 disappeared, while the exothermic peak only showed slight changes, suggesting that the curing of P2 was not significantly activated in the first stage. After heating at 150 °C for 30 mins in the second stage, the exothermic peak of P2 disappeared, indicating that the curing reaction of P2 was completed during the second stage of heating.
From above analysis, it can be confirmed that the stepwise curing process induces sequential curing reactions of P1 and P2. During these curing reactions, gas is generated, leading to the formation of a porous structure.
3.3. Mechanical Property Evaluation
To investigate the influence of stepwise isothermal heating on the mechanical properties of the printed samples, TMA was conducted by using the proposed heating program illustrated in
Figure 6.
Figure 11 presents the changes of the indentation depth ratio of the samples printed using P1, P2 and C during the stepwise isothermal heating process, where the indentation depth ratio is defined as the ratio of the indentation depth to the thickness of the tested sample, to evaluate the sample deformation.
From
Figure 11, it can be seen that the sample printed using P1 exhibited significant deformation in the first heating stage, and little deformation occurred in the second heating stage. In contrast, the sample printed using P2 displayed minimal deformation in the first heating stage, but underwent severe softening deformation in the second heating stage. For the sample printed using C, although it experienced noticeable softening deformation in both stages, its final deformation degree was significantly lower than that of the samples printed using P1 and P2.
The unique behavior of the sample printed using C can be ascribed to the composite structure. During the first heating stage, the P1 component melted, while most of the P2 component remained solid, acting as rigid particles and providing reinforcement. This structural characteristic effectively reduced the deformation rate, resulting in a significantly smaller deformation compared with the sample printed using pure P1, as presented in
Figure 11. Upon entering the second heating stage, the P1 component had already cured, and the P2 component began to melt. At this time, the cured P1 component played the role of reinforcing agent, leading to a smaller deformation at this stage compared with the sample printed using pure P2, as shown in
Figure 11. In general, the excellent resistance to softening deformation exhibited by the sample printed using C throughout the entire heating process is due to the structural support provided by the unmelted P2 component and the cured P1 component in the first and second heating stages, respectively.
To assess the evolution of mechanical properties throughout the forming process, Vickers hardness tests were employed, as presented in
Figure 12. Preliminary results showed no significant hardness differences between the samples printed using P1, P2, and C and their respective original powders. This observation suggests that although high-velocity particle impacted during the CSAM process leading to partial decomposition of latent curing agents, no substantial curing reaction was triggered.
During the subsequent stepwise heat treatment, the materials exhibited distinct behavioral patterns. After the first heating stage (85 °C, 1 h), P1 demonstrated a significant increase in Vickers hardness, indicating that the curing reaction effectively enhanced its mechanical properties. In contrast, P2 showed only a slight increase in hardness at this stage, suggesting that its primary curing reaction had not yet initiated. In the second heating stage (150 °C, 30 mins), the hardness of P1 increased marginally, indicating that its curing reaction was almost completed in the first stage. Conversely, P2 underwent a significant hardness enhancement during this stage, revealing the occurrence of its melting and curing processes. Notably, the hardness characteristics of the composite material C was gradually improved, correlated with the increase of the hardness of P1 and P2. This phenomenon reflects the gradual enhancement of mechanical properties in the composite material during the stepwise curing process. Ultimately, the hardness of composite material C after stepwise curing was comparable to that of samples cured using a low-rate heating process. It demonstrates that the stepwise curing technique not only obtains the same mechanical properties as the traditional low-rate heating methods, but also significantly reduces the heating time.