3. Results and Discussion
In the tests, fracture energies were first obtained, from which fracture values were derived. Both pure and composite samples were assessed for impact energy and impact strength values. Overall, examining the results table show that the highest impact energy was obtained from the pure PA6 sample, followed by the PA6 GF30 sample, while the lowest was observed in the PA CF15 sample. Literature reviews indicated that the sample were generally produced in orientation other than the critical ZX orientaiton. Each experiment was repeated three times under the same conditions, and the results were calculated as the arithmetic mean. To obtain impact energy values are listed in
Table 5.
At this step, the impact strength values for each sample and experimental condition have been calculated using Equation 2. And the results of impact strength are listed in
Table 6. It was observed that the highest impact strength value was achieved in the pure PA6 sample in experiment 8, with a value of 8.990 kJ/m
2. In the experimental condition, the parameters are A3B2C1D3, where these values correspond to a nozzle temperature of 275 °C, a layer thickness of 0.3mm, an outer wall count of 0, and a post heat treatment application duration of 160 minutes. It is noted in the manufacturer’s product datasheet that the impact strength in the ZX orientation printing during production is 3.2 kJ/m
2 in the notched impact test [
15]. The manufacturer has set the nozzle temperature at 245 °C for the produced samples in the testing process. In this study, a higher nozzle temperature and additional heat treatment process were applied. In another study, it was observed that the impact strength in the XY printing orientaiton, depending on nozzle temperature, is approximately around 6 kJ/m
2 [
1]. The reason for the effect of the printing orientation on mechanical properties is related to layer adhesion. In the ZX orientation, the load on the woven layers is applied parallel to the layers, resulting in lower mechanical properties. For example, a study conducted by F. Calignano et al. has shown significant differences in impact strength between the XY and ZX orientation [
6].
The highest second impact strength value in this study was obtained in the forth experiment produced with PA6 GF30 material, measuring 8.101 kJ/m
2. The sample was produced under the parameters of 260 C nozzle temperature, 0.15mm layer thickness, 1 outer wall count, and a post heat treatment duration of 160 minutes, labeled as A2B1C2D3. According to the product’s datasheet, a notched izod impact test in the ZX orientaiton yielded an impact strength of 2.6 kJ/m
2. In contrast, the same sample produced in the XY orientation under identical conditions had an impact strength of 38.4 kJ/m
2. The manufacturer’s datasheet also indicates that mechanical properties are orientation-dependent; for instance, while the tensile strength in the XY production direction is 78.3 MPa, it drops to 14.9 MPa in the ZX direction. When compared to pure PA6, these values are approximately 10% lower. However, literature studies show that the results for GF- reinforced PA materials in XY and XZ orientations are significantly higher than those for pure PA6. For example, in a study conducted by B.A. Moreno-Nunez et al., it was reported that in PA/CF materials, different production parameters and conditions achieved impact value of 113.4 kJ/m
2 in the XY orientaiton [
3].
In the carbon fiber (CF) reinforced PA6 material, the lowest impact strength value was obtained under the conditions of the seventh experiment, measuring 6.258 kJ/m
2. This value was achieved with a nozzle temperature of 275 °C, a layer thickness of 0.15 mm, 2 outer wall count, and an 80-minute post-heat treatment duration. When compared to pure PA6 material, this value is approximately 30% lower, while it is about 22% lower compared to PA6 GF30 material. However, according to the datasheet provided by the manufacturer, this value was initially 2.6 kJ/m
2, but experimental results reached 6.258 kJ/m
2, representing an increase of approximately 2.4 times [
17].
Mechanical properties indicate that if the products had been printed in the XY orientaiton, the expected ranking would be PA CF15 > PA6 GF30 > PA6. However, in the ZX orientaiton, which is the critical printing orientation, the ranking observed was PA6>PA6 GF30>PA6 CF15. The reason for this situation is explained in detail in the damage analysis section. For example, a study in the literature evaluated these three materials in term of the impact energy they absorbed. It was reported that the PA/GF composite stored 18.6% more energy than the PA/CF material and 210.56% more energy than the PA6 material. Thus, in this study, the ranking was also stated as PA6/GF>PA6/CF>PA6 [
14]. Mechanical properties vary depending on different production methods and the parameters associated with each method. For example, in a study conducted by Wang et al., PA-CF materials were produced using injection molding techniques varying additive ratios, and combinations of PA-30CF, PA-20CF, PA-10CF, and PA were tested. The PA-30CF material achieved a tensile strength of approximately 230 MPa, while the PA-20CF material reached around 200 MPa. In contrast, the PA-10CF material had a tensile strength of about 125 MPA. Pure PA material, on the other hand, exhibited a tensile strength of approximately 50 MPa [
9]. These values are significantly higher than those of samples produced with 3D printing techniques, especially for PA/CF combinations. However, the value for pure PA material is approximately similar when produced using 3D printing. In the literature, for example, a study reported that the tensile strength of PA/CF material produced via 3D printing reached values of 89.3 MPa [
10]. In at study focused on the production of PA6 material using a different manufacturing technique, Selecting Laser Sintering (SLS), materials with 30% glass bead and 10% glass fiber were produced. The highest tensile strength obtained was approximately 85 MPa [
18]. This indicates that comprehensive research and development efforts are necessary for products produced with 3D printing technology.
In the study, after obtaining the results, an analysis was conducted using the Taguchi method, which is one of the statistical experimental design methods widely used in engineering applications. Through the Taguchi analyis, the signal-to-noise (S/N) ratios for each experimental condition with different materials were calculated and graphed. The analyis was initially performed for the pure PA6 material. In the optimization of impact strength, the ‘Larger is better’ technique was used. In terms of S/N ratios, the experiment with the highest S/N ratio is considered the most significant. The S/N ratios obtained from the experimental results for the PA6 materials are presented in
Figure 3. As shown in the figure, for all factors expected parameter C, the impact strength values increase as a factor level are raised. When considering the effects, it is observed that factor A, and D are the most influential, while factor B is also effective, albeit to a lesser extent compared to A and D. Factor C shows minimal effect on the results. Regarding the outer wall count, it is evident that it has a weak effect on the impact strength of PA6 materials. In terms of S/N ratios, the optimal parameters for PA6 material are identified as A3B3C2D3, which correspond to a nozzle temperature of 275 °C, a layer thickness of 0.45 mm, 2 outer wall counts, and post-heat treatment duration of 160 minutes. For the worst-case scenario, it is observed that the A1B1C1D1 experiment corresponds to the lowest performance. Since a fractional factorial design method was used, 81 experiments were estimated using the Taguchi method's prediction technique. The predicted results are shown in
Figure 4. As seen in the figure, the difference between the highest and lowest value in the experimental design is 8.86 kJ/m
2, indicating the effect of the factors and levels used in the experiment. The values for the best and worst case are presented in
Table 7.
In the statistical experimental design, the 3D graphs of factor effects are crucial for interpreting results. For the impact strength of PA6 material, 3D effect graphs for A-B, A-C, B-C, B-D, and C-D were created and are presented in
Figure 5. Upon detailed examination of the graphs, it is observed that the peak point in the A-B effect graph occurs at the A3B2 level, while the peak in the A-C graph is at the A3C1 level, in the A-D graph at A3D3, in the B-C graph at B2C1, in the B-D graph at B2D3, and in the C-D graph at C1D3. For instance, in the AB graph, it can be seen that as a A parameter increases, the impact strength also increases. Additionally, in most graphs, an increase in the D parameter also leads to an increase in the impact strength. Overall, the graphs indicate that the effects of factors and their levels are significant.
S/N ratios for the PA CF15 material have been calculated and presented in
Figure 6. When evaluating the factors based on S/N ratios, it is observed that factor A is the most effective, followed by factor B. In the contrast to pure PA6 material, the C and D factors are seen to have minimal effect according to graph. When assessed in terms of optimal parameters, the configuration A3B1C2D2 has been identified. Particularly, compared to pure PA6, it is noted that increasing the layer thickness results in a decrease in impact strength values for PA CF15. Additionally, looking at the effect of post-heat treatment, it is observed that the impact strength level decreases after an 80-minute process.
3D effect graphs for the impact strength value of PA6 CF15 material have been created for A-B, A-C, A-D, B-C, B-D, and C-D, and are presented in
Figure 7. A detailed examination of the graphs shows that the peak point in the A-B effect graph occurs at the A3B1 level, while in the A-C graph, the peak is at the A3C3 level. In the A-D graph, the peak is at A3D2, in the B-C graph at B1C3, in the B-D graph at B1D2. And in the C-D graph at C3D2. For example, when looking at the AB graph, it is observed that as the A parameter increases, the impact strength value also increases. The factor D, however, shows an increase at level 1 and 2, while it decreases at level 3. Overall, the graphs indicate that the effects of the factor are significant.
S/N ratios for PA6 GF30 material have been calculated and are presented in
Figure 9. To determine the optimal parameters, the S/N ratios were considered. It is observed that factors A, B, and D are effective, while the effect of factor C is relatively low. Additionally, compared to pure PA6 material, the effect of the B parameter is the opposite; that is, as the value of the B parameter increases, the impact strength decreases, like the behavior observed in PA6 GF30 material. The A parameter shows variation when compared to PA6 CF15 material. It is anticipated that when the nozzle temperature exceeds 260 °C, the impact strength value decreases due to the embrittlement of the matrix. When evaluating the results in terms of optimal parameters, it is seen that the optimal configuration is A2B1C1D3. From the perspective of post-heat treatment, it is noted that the heat treatment duration of 160 minutes is effective for PA6 GF30 materials.
3D effect graphs for the impact strength value of PA6 GF30 material have been created for A-B, A-C, A-D, B-D, and C-D, and presented in
Figure 11. A detailed examination of the graphs reveals that the peak point in the A-B effect graph occur at the A2b1 level, while the peak in the A-C graph is at the A2C2 level. In the A-D graph, the peak is at A2D3, in the B-C graph at B2C2, in the B-D graph at B1D3, and in the C-D graph at C3D3. When comparing the factor effects with the S/N ratios, it is evident that they are suitable in terms of optimal values.
When examining the effects of factors on mechanical properties, it has been observed in the literature that, depending on different parameters in XY orientation weaving, the impact strength values are highest in PA/GF materials, followed by PA/CF materials. The effect of continuous carbon fiber allows the PA/CF value to reach 100 kJ/m
2, while the effect continuous glass fiber enables the PA/GF value to reach approximately 290 kJ/m
2. These results indicate that the type of fiber used has a significant effect on the mechanical properties [
13]. Although the continuous carbon fiber 3D printing technique provides values closest to those of PA/CF and PA/GF composites produced by the pressure injection technique, issues arise due to printing difficulties and the inability to produce desired complex surface geometries. However, with the FDM technique, it is possible to manufacture complex-shaped part using short fiber materials, indicating a need for R&D effort in this area.
In the final step of the optimization phase of the study, the best and worst experimental conditions were identified for each material group. To determine the accuracy of the technique used, these values were additionally produced a tested, and percentage error values were calculated. The values are presented in
Table 7. As seen in the table, the highest error value is 11%, while the lowest error value is 6%. The average error has been calculated as 9.51%. When considering the overall success of the prediction model, this high prediction rate is acceptable for such a complex model.
When evaluating the results overall, although the best conditions for nozzle temperature (A) are at level 3, specifically 275 °C, it is observed that for the PA6 GF30, this temperature is 260 °C. For the worst conditions, the lowest nozzle temperature is at level 1, which is 245 °C. In terms of layer thickness, it is noted that, expect for pure PA6, the best value in other material groups is provided by the lowest layer thickness of 0.15mm. However, pure PA6, the highest layer thickness yields the best results. When evaluating the number of outer walls (C), it is found that in optimal conditions, the wall-less structure performs best pure PA6 and PA6/GF, whereas for PA6/CF, the structure with 2 walls is the best. Regarding the post-heat treatment process time (D), it has determined that a duration of 160 minutes is optimal for pure PA6 and PA6 GF30 materials., while 80 minutes is optimal for PA6 CF156. The literature indicates that applying heat treatment as a post-processing step leads to a significant increase in mechanical properties. In a study by Xu et al, post-processing heat treatment was applied to carbon and nylon materials in various layered products. It was reported that the optimal effect of thermal treatment on the tensile strength in a 3D-printed layered composite structure occurs at a temperature of 140 -150 °C with a waiting period of 4 hours, which is also optimal for interlaminar shear strength at the same temperature [
18]. In this study, a post-processing heat treatment temperature of 80 °C was applied, and the result were examined. The lower temperature was chosen particularly due to reasons such as dimensional distortions and stability. In future studies, different temperatures and waiting times can be optimized based on dimensional distortions and stability characteristics.
Micro and Macro Damage Analyis
The fracture surfaces of samples are thoroughly examined using SEM for the damage analysis of composite products. In this context, various aspects such as the main matrix of the composite structure, fibers, fracture lines, fiber breakages, fiber structures, and matrix damages are analyzed in detail [
20,
21]. The macro damage images of the samples after impact are presented collectively in
Figure 12. When examining the fracture surfaces of the samples, it is observed that pure PA6 samples exhibit a brittle fracture surface, while fiber-reinforced samples show more ductile and rougher surface.
The SEM images of the damaged surfaces of the samples obtained from the impact tests are presented in detail and comparatively in
Figure 13,
Figure 14 and
Figure 15 for micro damage analyses. Upon examining
Figure 13, it can be clearly observed that the extruder width (EW)’s is evident in pure samples, especially at low temperatures. As the temperature increases, the formation of gaps between the EWs in pure samples is noteworthy (
Figure 2.a.). At is believed that this may due to contraction caused by rapid cooling during the printing of the first layer. In samples reinforced with glass and carbon fibers, although there are partially weak interfacial bonds between EWs at low temperatures (
Figure 13. b and c), it is observed that as the temperature increases, the fibers form bridging at the boundaries between the EWs (
Figure 13. k). During the production phase, it is believed that the flow of the liquid matrix facilitates the flow between the EWs, helping the structure to form more homogenously (
Figure 15. b, and c). Upon examining the facture surfaces, it is noted that in sample pure PA6 with 2th experiment, impact damages occur at the overlap surfaces of the EWs, while damage-free regions are identified at the boundary areas due to geometry (
Figure 13.j).
In fiber-reinforced samples (GF2, CF2), fiber pull-out, debonding, and matrix cracks have been observed (
Figure 13). Notably, intensive fiber pull-out damages have been identified in carbon fiber-reinforced samples. With the increase in temperature (
Figure 14 and
Figure 15), the changes in fracture surface morphology, particularly in pure PA6 samples, are striking.
On the damage surfaces of pure PA6 samples, damage such as textured microflow, toughened phase, and scarp have been particularly observed. It is believed that the changes in damage modes and fracture surface morphology are due to heat processing. In fiber-reinforced samples, particularly those reinforced with carbon fibers, a strong fiber-matrix interfacial bond has been observed. The smaller diameter and higher surface area of carbon fiber compared to glass fibers have contributed to the formation of a stronger fiber-matrix interfacial bond. In fiber-reinforced samples, toughness mechanisms such as debonding, pull-out, matrix cracks, and fiber bridging (
Figure 13,
Figure 14 and
Figure 15) have had a positive effect on the impact toughness of the samples.
When examining the SEM images in terms of voids, it was observed that in pure samples, large and non-homogeneous air voids formed between /in the EWs. In fiber-reinforced samples, voids appeared in certain shapes and more homogenous structures. Additionally, it was noted that in the fiber-reinforced samples, the EW line boundaries became less distinct due to fiber reinforcements, resulting in stronger boundaries compared to pure samples. This phenomenon was attributed to fibers remaining as protrusions outside the layer during the solidification of a lower layer, which became trapped in the melt during the formation of an upper layer. This situation facilitated the formation of a good interface between the layers, thereby improving the mechanical properties of the fiber-reinforced samples.