3.1. Scanning Electron Microscopy Analysis - SEM
The PLA filaments were characterized before and after the incorporation of Carbon Nanotubes through Scanning Electron Microscopy (SEM), and the results are presented in
Figure 6.
In
Figure 6 (a), the micrograph of the PLA surface prior to the incorporation of MWCNTs-COOH is presented. Upon analyzing the micrograph, the presence of PLA clusters (blue arrows) distributed throughout the surface is evident. Additionally, the existence of a pore (yellow arrow) permeating the material surface is identified. Furthermore, aligned PLA structures (red arrows) are observed, suggesting that PLA can form a microstructure with orientation through the extrusion process [
24].
In
Figure 6 (b), the morphology of PLA after the incorporation of 1.0 wt% Carbon Nanotubes is depicted. The notable presence of a Carbon Nanotube (yellow arrow) is emphasized, suggesting that CNTs may be dispersed in the PLA matrix through the extrusion method [
24]. The occurrence of crack phenomena (red arrows) deserves attention, as they manifest across the entire surface. These cracks, possibly resulting from the initiation of material decomposition during SEM analysis, can be attributed to the sample’s fragility under laser incidence. During this analysis, the Scanning Electron Microscope produces images by moving a focused beam of electrons across the sample’s surface while scanning, allowing for a more detailed study of the sample [
25].
In
Figure 6 (c), the micrograph of PLA with the addition of 2.0 wt% Carbon Nanotubes is presented. In this detailed analysis, the presence of pores (yellow arrows) and cracks (red arrows) distributed along the surface is identified. Additionally, clusters (orange arrows) are observed dispersed throughout the sample. It is noteworthy that, in micrograph 6 (c), the presence of MWCNTs-COOH is not discernible, which may be attributed to the quality of the polymer- nanofiller mixture [
26].
Figure 6.
(a) SEM of PLA before the incorporation of CNTs, (b) SEM of PLA with the incorporation of 1.0 wt% CNTs, and (c) SEM of PLA with the incorporation of 2.0 wt% CNTs.
Figure 6.
(a) SEM of PLA before the incorporation of CNTs, (b) SEM of PLA with the incorporation of 1.0 wt% CNTs, and (c) SEM of PLA with the incorporation of 2.0 wt% CNTs.
3.2. Characterization by X-ray Diffraction
The Carbon Nanotubes (CNTs), PLA, and nanocomposites (PLA/1.0%CNTs and PLA/2.0%CNTs) underwent characterization using X-ray Diffraction (XRD) technique, and the results are presented in the diffractogram of
Figure 7.
The XRD results show that Carbon Nanotubes exhibited diffractions at 2θ: 30.01° and 2θ: 50.03°, attributed, according to [
27], to the basal reflection peak and the graphitic crystalline lattice. As for PLA, both before and after 3D Printing, the results indicate the absence of crystallinity, revealing a slight curvature at 2θ: 8.2° and 2θ: 16.5°. Subsequently, the predominance of the amorphous phase of the polymer is observed, a behavior previously noted in studies by [
24], [
28], and [
29]. Regarding the nanocomposites, PLA/1.0%CNTs and PLA/2.0%CNTs did not show significant changes in their respective crystallinities, exhibiting the disappearance of the curvature at 2θ: 8.2° and a slight curvature at 2θ: 18.7°. The disappearance at 2θ: 8.2°, as well as the disappearance of characteristic CNTs diffractions, can be attributed, according to [
27], to the low dimensionality of MWCNTs clusters and their good dispersion in the matrix, resulting from the functionalization of carbon nanotubes.
Figure 7.
XRD of PLA, CNTs, and Nanocomposites.
Figure 7.
XRD of PLA, CNTs, and Nanocomposites.
3.3. Characterization by Raman Spectroscopy
Figure 8 presents the data obtained by Raman spectroscopy and treated by deconvolution into Lorentzian subbands for as-received carbon nanotube samples, the commercial PLA filament and the two nanocomposites produced respectively with 1.0 wt% and 2.0 wt% by mass of CNTs. The regions of interest were determined based on the main vibrational modes of the nanotubes, the first from 1200 to 1700 cm
-1 and the second from 2600 to 3050 cm
-1.
Figure 8.
Deconvolution of the Raman spectra of the as-received carbon nanotube samples, the commercial PLA filament and the nanocomposites with 1.0 wt% and 2.0 wt% of CNTs.
Figure 8.
Deconvolution of the Raman spectra of the as-received carbon nanotube samples, the commercial PLA filament and the nanocomposites with 1.0 wt% and 2.0 wt% of CNTs.
As can be seen in Figures 8(a) and 8(b), the Raman spectra of the nanocomposites are a superposition of vibrational modes associated with the PLA polymer and the carbon nanotubes, shown in Figures 8(c) and 8(d). For the as-received CNTs, the D band was deconvoluted in three subbands, two labeled D
L and one labeled D
R, associated with defects and functionalizations on nanotubes walls related to sp
3 hybridized carbon, respectively in 1305, 1347 and 1360 cm
-1 [
24,
30]. The subband D
LO in 1402 cm
-1 is associated with longitudinal optic phonons in the CNTs structure and the subband D
middle in 1492 cm
-1 has been used in literature as an indicator of the amorphous carbon degree on CNTs samples [
30]. The G band was deconvoluted in three subbands, G
out, G
inn and D’ respectively in 1580, 1605 and 1620 cm
-1. The G
out and G
inn subbands are associated with the vibrations sp
2 hybridized carbon atoms of the outermost and the innermost walls of the carbon nanotubes, respectively, while the D’ subband is associated with structural disorder-induced double resonance process of the D band projected in the G band [
24,
30].
In this region, there are several vibrational modes for PLA, associated with stretching and bending vibrations of single and double-bonded carbon atoms and bonds between carbon and hydrogen, but the spectrum show some divergences with literature [
24,
31,
32,
33] such as vibrational modes in the same region of the G band of CNTs, these could be due to the production process of the commercial PLA. Even so, the most prominent band associated with CH
3 symmetric deformation vibrations was identified and deconvoluted with two subbands in 1448 and 1460 cm
-1 and the the band associated with CH
3 asymmetric deformation vibrations was identified in 1387 cm
-1 [
31,
32,
33]. The spectra of the nanocomposites appeared as an overlap of these and the CNTs vibrational modes, as these same PLA modes were identified in 1447, 1456 and 1384 cm
-1. Furthermore, the signal from PLA showed an enhancement as it is closer to the literature, which can be due the nanocomposites preparation methodology.
In both nanocomposite’s spectra, the signal from PLA appeared with more intensity covering part of the signal from the CNTs. Although the D band isn’t clearly visible, its subbands were identified in 1311, 1343 and 1359 cm-1, but it is difficult to obtain information from these modes dislocations as they have low intensity and are in the same region of PLA modes. Similarly, the DLO, Dmiddle and D’ bands disappeared, but this can be due to the low signal intensity in comparison to the PLA spectrum. As a highlight, the Gout and Ginn subbands were identified respectively in 1585 and 1614 cm-1 for PLA/1.0%CNTs and in 1583 and 1610 cm-1 for PLA/2.0%CNTs, showing significant blueshift as shown in Figures 8 (a) and 8 (b). This indicates that the nanotubes are being compressed by the polymeric matrix, as they are distributed by its volume, which also could explain the lower signal of the CNTs. As they are randomly distributed, they could be subjected to different compressions and the region analyzed explains the higher blueshift in the sample with 1.0 wt% by mass of CNTs.
In Figures from 8 (e) to 8 (h) are shown the spectra in higher frequencies of the nanocomposites with 2. 0 wt% and 1.0 wt% by mass of CNTs, the commercial PLA and the as-received CNTs, respectively. The PLA spectrum also diverged from literature as shouldn’t exist vibrational modes in this region [
24,
31,
32,
33], on the other hand the second order vibrational modes of CNTs were identified, as de 2D band was deconvoluted in 2D
L and 2D
R subbands and the D+G band in D
L+G
out and D
R+G
inn subbands, respectively in 2695, 2729, 2891 and 2948 cm
-1 [
34,
35,
36]. For the nanocomposites, the D+G band wasn’t identified and the resulting spectra are attributed to the 2D band of the CNTs considering a split of both subbands, the redshift 2D
L and the blueshift 2D
R that resulted in the split of the 2D band itself. The 2D
L and 2D
R subbands are attributed to second order Raman scattering of the innermost and of the outermost tubes, respectively. For PLA/1.0%CNTs, the 2D
L1 and the 2D
L2 subbands were identified in 2660 and 2674 cm
-1, while for PLA/2.0%CNTs these subbands appeared in 2654 and 2678 cm
-1. Similarly, the 2D
R1 and the 2D
R2 subbands were identified in 2734 cm
-1 and 2747 cm
-1 for PLA/1.0%CNTs and in 2738 cm
-1 and 2756 cm
-1 for PLA/2.0%CNTs. For the 2D
R subbands the blueshift could indicate p-type doping of the outermost tubes and for the 2D
L subbands the redshift could indicate n-type doping of the innermost tubes. These results suggest that the doping effect can be due to the interaction between the CNTs and the polymeric matrix [
34,
35,
36].
3.4. Compression Testing: Shape Solid Sample Variations of Infill Patterns
The strength of solid 3D-printed PLA samples with variable infill patterns (concentric, hexagonal, and triangular) and same percentages of 90%, was analyzed by means of mechanical compression tests. The results are presented in the following
Table 1.
Table 1.
Average compressive strength behavior of printed parts with different infill patterns.
Table 1.
Average compressive strength behavior of printed parts with different infill patterns.
Types of Samples/Infill Patterns |
Filling Percentage |
Compressive Strength (MPa) |
PLA/Concentric |
90 % |
45.9 ± 6,5 |
PLA/Hexagon |
90 % |
48.5 ± 6,6 |
PLA/Triangle |
90 % |
52.8 ± 4,2 |
The results of the compression test show that there is a variation in the strength of the printed parts as the infill pattern changes. According to the results, it can be observed that the solid sample with a triangle infill pattern exhibits a higher average compression strength, followed by the hexagonal infill pattern. In addition, it is possible to observe that the infill pattern that presented the lowest mechanical performance was the concentric pattern. This behavior has already been observed in the study conducted by [
37] when investigating PLA printed parts with varying infill patterns. In their research, they achieved better compression performance for samples with a triangular infill pattern compared to line type infill. [
38] emphasize that the compressive properties of 3D-printed materials (such as PLA) depend on the infill patterns and infill percentages; these factors influence the mechanical properties of the parts.
Figure 9 (a) illustrates the comparisons of solid materials (patterns: triangular, hexagonal, and concentric) regarding their compression strengths. Upon analyzing the figure, it can be observed that the printed material exhibiting the highest average compression strength was the PLA sample with a triangular infill pattern, with an increase of 15.03% compared to the concentric, and 8.8% compared to the hexagonal. And,
Figure 9 (b) shows the percentage Stress x Strain behavior of the PLA with different infill patterns under mechanical compression loading.
Figure 9.
(a) Comparative analysis of compressive strength of 3D printed PLA samples with variations infill patterns and 9 (b) Deformation of the PLA with different infill patterns when subjected to mechanical analysis of compression.
Figure 9.
(a) Comparative analysis of compressive strength of 3D printed PLA samples with variations infill patterns and 9 (b) Deformation of the PLA with different infill patterns when subjected to mechanical analysis of compression.
3.5. Compression Test: Nanocomposites PLA with 1.0 wt% and 2.0 wt% CNTs
The evaluation of the mechanical strength of the nanocomposites of PLA and CNTs was conducted by performing compression tests, and the corresponding results are presented in
Table 2.
Table 2.
Average Compression Strength Behavior of Nanocomposites.
Table 2.
Average Compression Strength Behavior of Nanocomposites.
Types of Samples/Infill Patterns |
Filling Percentage |
Compressive Strength (MPa) |
PLA/Triangles |
90 % |
52.8 ± 4,2 |
PLA/1.0%CNTs/ Triangles |
90% |
61.7 ± 12,1 |
PLA/2.0%CNTs/Triangles |
90% |
73.5 ± 15,0 |
The results demonstrate that the addition of Carbon Nanotubes to the matrix enhances the compression strength of the nanocomposites. There is a noticeable 20.32% increase in compression strength for the nanocomposite containing 2.0 wt% CNTs compared to the nanocomposite with 1.0 wt% CNTs in its composition. All nanocomposites exhibited higher strength than the matrix with a triangular infill pattern.
The nanocomposite with 1.0 wt% of CNTs in its composition shows an increase in compression mechanical strength of 16.8% compared to the matrix. Furthermore, for the nanocomposite with 2.0 wt%, the increase is even more significant, reaching 39.2% compared to the matrix.
Contrary to what was observed in the study conducted by [
39], where the analysis of the influence of graphene in the PLA matrix didn’t result in an increase in compression strengths compared to the PLA matrix, this work reveals a significant contribution of carbon nanotubes (CNTs) to the mechanical compression performance. It is noteworthy that, to date, there are no records in the literature regarding PLA/CNTs nanocomposites under the specific conditions evaluated in this study.
The results regarding average compression strength are visualized in
Figure 10 (a), which illustrates the comparison between the matrix (configured with a triangular infill pattern) and the nanocomposites (PLA/1.0%CNTs and PLA/2.0%CNTs). In the figure, it is evident that the nanocomposites show significantly higher compression strengths when contrasted with the matrix. And 10 (b) graphically depicts the Stress-Strain behavior of PLA polymer and PLA/CNTs nanocomposites at concentrations of 1.0 wt% and 2.0 wt%, respectively.
Figure 10.
(a) Comparative Analysis of Compression Strength between PLA Matrix and PLA/CNTs Nanocomposites and (b) Stress-Strain Behavior of PLA and Nanocomposites under Compression Analysis.
Figure 10.
(a) Comparative Analysis of Compression Strength between PLA Matrix and PLA/CNTs Nanocomposites and (b) Stress-Strain Behavior of PLA and Nanocomposites under Compression Analysis.
3.6. Compression Testing: Honeycomb Shape with Variations of Infill Patterns
In the mechanical compression analysis, honeycomb structures with variations in infill patterns (concentric, hexagonal, and triangular) exhibited behaviors similar to the structures analyzed by [
40] and [
41]. Where, in their studies presented three distinct regions: Elastic, Plateau and densification.
According by [
42], the three regions of the stress-strain graph are associated with three different failure modes at each stage of compaction. Initially, the material is subjected to elastic bending, represented by the almost linear portion until the maximum crushing force. This is followed by elastic buckling and subsequent densification of cells during the final stages of loading.
However, in the scope of this study, we will delimit our analysis to compressive properties restricted to the elastic region. Thus, in the subsequent table, the results of the compression test of the honeycomb samples are presented, considering variations in the infill patterns (concentric, hexagonal and triangular).
Table 3.
Average Compression Strength Behavior of Printed Parts with Different Infill Patterns.
Table 3.
Average Compression Strength Behavior of Printed Parts with Different Infill Patterns.
Type of Samples/Infill Patterns |
Filling Percentage |
Compressive Strength (MPa) |
Honeycomb/Concentric |
90 % |
20.6 ± 1,9 |
Honeycomb/Hexagon |
90 % |
19.6 ± 4,6 |
Honeycomb/Triangles |
90 % |
20.8 ± 2,2 |
The results obtained from the compression test of honeycomb samples, considering variations in infill patterns (concentric, hexagonal, and triangular), demonstrate that the structures exhibit remarkably equivalent compression strength. It is noteworthy, however, that the Honeycomb/Triangles configuration exhibits superior compressive performance compared to the other analyzed forms.
Figures 11 (a) and 11 (b) illustrate, respectively, the average compression strength and the stress-strain behavior of honeycomb-printed structures with variations in infill patterns.
Figure 11.
(a) Comparative analysis of compression strength in honeycomb samples with different infill patterns and (b) Stress-Strain Behavior of honeycomb shape with different infill patterns.
Figure 11.
(a) Comparative analysis of compression strength in honeycomb samples with different infill patterns and (b) Stress-Strain Behavior of honeycomb shape with different infill patterns.
3.7. Compression Test: Honeycomb Samples with 1.0 wt% and 2.0 wt% Carbon Nanotubes
The results of the compression test for nanostructured honeycomb samples, containing carbon nanotubes (CNTs) at concentrations of 1.0 wt% and 2.0 wt%, and the matrix (triangular infill pattern), are presented in the table below.
Table 4.
Average Compression Strength of the Matrix and Nanocomposites.
Table 4.
Average Compression Strength of the Matrix and Nanocomposites.
Type of samples/Infill Patterns |
Filling Percentage |
Compressive Strength (MPa) |
Honeycomb/Triangles |
90 % |
20.8 ± 2,2 |
Honeycomb/1.0%CNTs |
90 % |
33.2 ± 2,2 |
Honeycomb/2.0%CNTs |
90 % |
20.9 ± 4,4 |
The results show a 59.6% increase in compressive strength for the nanocomposite sample (PLA/1.0%CNTs) compared to the sample without addition of CNTs. As for the nanocomposite sample (PLA/2.0%CNTs), the increase is 0.48%. However, contrary to what occurs in solid samples, where an increase in mean compressive resistance is observed with the increase in the percentage of CNTs in the matrix, there is reduction in resistance as the percentage of CNTs in the matrix increases.
It is noteworthy that, up to the present moment, there are no reports in the literature regarding investigative studies of nanostructured honeycomb structures PLA/CNTs under the specific conditions examined in this research.
Figures 12 (a) and 12 (b) represent, sequentially, the average compressive strength and stress-strain behavior of the structures printed in the honeycomb configuration, showing variations in percentages of CNTs.
Figure 12.
(a) Comparative analysis of compression strength in honeycomb samples with variations in percentages of CNTs and (b) Stress-Strain Behavior of the matrix and nanostructured honeycomb.
Figure 12.
(a) Comparative analysis of compression strength in honeycomb samples with variations in percentages of CNTs and (b) Stress-Strain Behavior of the matrix and nanostructured honeycomb.
3.8. Morphological Analysis via SEM After the Compression Test
The solid and honeycomb shaped PLA samples containing variations in infill patterns were subjected to Scanning Electron Microscopy (SEM) analysis, and the results obtained are illustrated in the figures below:
The results of the Scanning Electron Microscopy analysis shown in
Figure 13 reveal in (a) micrographs corresponding to the solid sample with a concentric infill pattern, highlighting highly compacted regions (blue arrows) that can be attributed to deformations resulting from the mechanical test. Additionally, the presence of folds in the structure is observed (yellow arrow), which could be associated with both the manufacturing process and the responses of the mechanical analysis.
In
Figure 13 (b), the micrograph of the honeycomb shape structure is presented, showing the presence of voids throughout the structure, which can be associated with the internally distributed honeycomb configuration.
Figure 13.
(a) Micrograph of the solid shape and (b) honeycomb with a concentric infill pattern.
Figure 13.
(a) Micrograph of the solid shape and (b) honeycomb with a concentric infill pattern.
In
Figure 14, micrographs corresponding to the solid test specimen with a hexagon infill patterns are displayed in (a), and those of the honeycomb shaped structure with the same infill pattern are shown in (b).
In 14 (a), the occurrence of structure ruptures is observed (yellow arrows), which can be attributed, as mentioned earlier, to the mechanical loading. Additionally, compacted structures are observed (red arrows), mechanisms already noted in the micrograph with concentric infill patterns.
In 14 (b), the micrograph of the honeycomb-shaped structure with hexagonal infill patterns is shown. Here, mechanisms such as structure folds (black arrows), layer stacking (orange arrows), and the presence of voids (blue arrows) are observed. The voids can be attributed to the arrangements of the hexagons within the structures.
Figure 14.
(a) Micrograph of the solid shape, and (b) honeycomb with hexagonal infill pattern.
Figure 14.
(a) Micrograph of the solid shape, and (b) honeycomb with hexagonal infill pattern.
Figure 15 displays micrographs corresponding to the shape solid (a) and the honeycomb (b) with triangle infill patterns.
In the micrograph of the solid test specimen with triangle infill patterns, as presented in 15 (a), the presence of compacted structures is noticeable (orange arrows), a mechanism observed in other solid structures analyzed in this study. Additionally, fractures in the structure are observed (blue arrows), which can be attributed to increased load during the mechanical analysis, leading to structural ruptures.
In
Figure 15 (b), the micrograph of the honeycomb-shaped structure with triangle infill patterns is illustrated. Here, well-compacted structures are noted (red arrows), and the presence of voids (yellow arrows) is observed again, associated with the honeycomb-like configuration of the structure.
Figure 15.
a) Micrograph of the solid shape, and (b) honeycomb shaped structure with triangular infill pattern.
Figure 15.
a) Micrograph of the solid shape, and (b) honeycomb shaped structure with triangular infill pattern.
The nanocomposite solid (PLA/1.0%CNTs) and (PLA/2.0%CNTs), subjected to the mechanical compression test, were microscopically analyzed by SEM, with the results presented in
Figure 16.
In 16 (a), layer rupture is observed (green arrow), which can be attributed to mechanical stresses during the compression test; additionally, the layers can be seen compacting onto each other (orange arrows). In 16 (b), voids (black arrows) in the structure are observed, along with cracks (red arrows) and detachment (white arrows). The mechanisms present in the fractures of the nanocomposites are similar to those exhibited in PLA samples without the addition of Carbon Nanotubes.
Figure 16.
Micrograph of the nanocomposite (PLA/1.0%CNTs) in (a) and (b) PLA/2.0%CNTs.
Figure 16.
Micrograph of the nanocomposite (PLA/1.0%CNTs) in (a) and (b) PLA/2.0%CNTs.
Figure 17 (a) illustrates the micrograph of the honeycomb nanostructure (PLA/1.0%CNTs) and (PLA/2.0%CNTs).
In micrograph (a), the presence of detachment (red arrows) and cracks (white arrows) is highlighted. In micrograph 17 (b), there is a widespread presence of cracks (white arrows) throughout the structure, along with compacted areas (black arrows). These deformations, including cracks and detachment, can be attributed to the applied forces during the mechanical compression analysis.
Figure 17.
a) Micrograph of the nanostructured honeycomb shape (PLA/1.0%CNTs) and (b) Nanostructured honeycomb shape (PLA/2.0%CNTs).
Figure 17.
a) Micrograph of the nanostructured honeycomb shape (PLA/1.0%CNTs) and (b) Nanostructured honeycomb shape (PLA/2.0%CNTs).