3.1. FTIR Results
This FTIR spectrum corresponds to a polymeric blend composed of polylactic acid (PLA) and polycaprolactone (PCL) (see
Figure 2), showing the characteristic absorption bands associated with the functional groups of both polymers. In the region around 2994 cm
−1 and 2944 cm
−1, we observe stretching vibrations of the –CH
3 and –CH
2 groups, typical of the aliphatic chains present in both PLA and PCL. The peak at 2865 cm
−1 is also related to symmetric –CH
2 stretching. A strong and sharp peak at 1749 cm
−1 is attributed to the carbonyl (C=O) stretching vibration, which is prominent in both ester-based polymers. The band at 1453 cm
−1 is associated with bending vibrations of the –CH
2 and –CH
3 groups. The absorption near 1361 cm
−1 and 1295 cm
−1 corresponds to C–H bending, particularly from PLA. The peaks at 1179 cm
−1 and 1081 cm
−1 are due to C–O–C stretching vibrations, also indicative of ester linkages. The region between 959 cm
−1 and 756 cm
−1 shows complex deformation and bending modes associated with the skeletal vibrations of the polymer backbone. Notably, the bands at 867 cm
−1 and 786 cm
−1 are often related to PCL-specific modes. Finally, the band at 1043 cm
−1 corresponds to C–O stretching, further confirming the presence of ester functionalities in the blend. This spectral analysis confirms the coexistence of PLA and PCL within the blend through the identification of their characteristic functional groups.
The FTIR spectra obtained from the PLA-g-MA/PCL formulations revealed several characteristic absorption bands corresponding to the chemical structures of poly (lactic acid) (PLA), polycaprolactone (PCL), and maleic anhydride (MA) (see
Figure 3). Furthermore, a detailed examination was carried out to assess the possible presence of residual benzoyl peroxide (BPO), which was used as the radical initiator during reactive extrusion.
Firstly, the main peaks associated with the PLA structure were clearly observed across all spectra. The most prominent band appeared near 1750 cm
−1, corresponding to the C=O stretching of the ester group in PLA. Additionally, peaks were identified around 2995 cm
−1 and 2945 cm
−1, and were attributed to the C–H stretching vibrations of CH
3 and CH units, respectively. Bending vibrations were seen near 1455 cm
−1, 1385 cm
−1, and 1355 cm
−1, consistent with CH
3 and CH deformation modes [
25,
26].
In the region from 1185 to 1045 cm−1, several peaks were assigned to the asymmetric and symmetric stretching of C–O–C ester groups. A band at 865 cm−1 was also present, corresponding to C–COO deformation, commonly reported for PLA.
In addition to the PLA signals, characteristic PCL bands were also evident. The C=O stretching of PCL ester groups appeared near 1720–1730 cm−1, partially overlapping with the carbonyl signal of PLA. The C–H stretching from methylene groups in PCL was observed around 2945 cm−1 and 2865 cm−1. Vibrational modes near 1295 cm−1 and 1240 cm−1 were attributed to C–O and C–C stretching, while signals between 1160 and 1100 cm−1 reflected C–O–C bending, all of which are consistent with PCL’s aliphatic ester structure.
Regarding the grafting of maleic anhydride onto PLA, the presence of MA was inferred from subtle but distinct spectral features. In particular, the carbonyl region around 1750 cm−1 showed broadening and increased intensity in the PLA-g-MA samples when compared to neat PLA. This effect is due to the superimposition of the carbonyl bands from both PLA and the anhydride groups of MA. In some spectra, especially for PLA-g-3MA and PLA-g-5MA formulations, additional absorption bands were observed between 1885 and 1850 cm−1. These bands are attributed to asymmetric C=O stretching of anhydride functionalities, supporting the successful grafting of MA onto PLA chains. These findings are consistent with prior reports in the literature, such as the work of Orozco et al., who noted that the spectral features of MA are often subtle due to its low concentration, yet detectable through carbonyl shifts and minor absorptions in this range.
A critical part of the analysis focused on determining the presence of residual benzoyl peroxide (BPO), which would indicate incomplete decomposition during processing. BPO has several characteristic FTIR signals, most notably the O–O peroxide bond stretching near 880–890 cm−1. Aromatic ring vibrations appear at 1600 cm−1, 1500 cm−1, and 1450 cm−1, while aromatic C–H stretching is found in the 3100–3050 cm−1 region. Additionally, the C=O stretching of benzoate groups from BPO can overlap with PLA and PCL near 1720–1760 cm−1, making this region less definitive for BPO identification.
After carefully inspecting the FTIR spectra, no significant absorption was observed in the 880–890 cm−1 region, indicating the absence of the O–O bond and, therefore, no detectable residual BPO. Similarly, no peaks were observed around 1600, 1500, or 1450 cm−1 that could be attributed to the aromatic vibrations of BPO. The carbonyl band at 1750 cm−1 is consistent with the ester groups in PLA, PCL, and MA, and cannot by itself confirm the presence of BPO. However, in the absence of aromatic-related peaks, it is unlikely that BPO remains in formulation. These observations suggest that BPO was fully decomposed during melt processing at 180 °C, which is above the thermal decomposition range of BPO (typically between 80 and 100 °C).
In conclusion, the FTIR spectra confirmed the presence of key functional groups associated with PLA, PCL, and grafted MA, supporting the successful preparation of PLA-g-MA/PCL blends. No residual BPO was detected, as evidenced by the absence of characteristic peroxy and aromatic bands in all the spectra. These results indicate that the extrusion conditions applied (a temperature profile from 170 to 185 °C and a 100 rpm screw speed) were sufficient to promote the complete decomposition of BPO, ensuring clean grafting reactions without initiator residue. This aligns with findings in related studies where FTIR proved effective in monitoring MA grafting and confirming the elimination of peroxide residues after processing.
3.2. Thermal Properties
The glass transition temperature (T
g) can be used to assess thermal properties. Additionally, variations in cold crystallization temperature (T
cc), melting temperature (T
m), and the percentage of crystallinity (X
C) are often indicative of the interactions between different components [
27]. The DSC results obtained are summarized in
Table 3. To ensure accurate assessments, the thermal data was analyzed based on the second heating run, which eliminates any potential influence of process history.
The thermal behavior of the PLA/PCL blends modified with different concentrations and types of maleic anhydride (MA)-grafted PLA (PLA-g-MA) was studied using differential scanning calorimetry (DSC). The results reveal how varying the compatibilizer type and amount influences the thermal transitions and crystallinity of the blends.
The unmodified blend, composed of 80% PLA and 20% PCL (PLA 20PCL), exhibited a melting temperature (Tm) of 154.1 °C and a cold crystallization temperature (Tcc) of 127.1 °C. Despite showing moderate values for the enthalpy of cold crystallization (ΔHcc = 14.9 J/g) and melting enthalpy (ΔHm = 15.3 J/g), the degree of crystallinity (Xc) was extremely low (0.4%), suggesting poor crystallization under the experimental conditions.
Incorporating 5 wt.% of PLA-g-1MA into the PLA/PCL matrix led to a slight decrease in both T
m (151.1 °C) and T
cc (122.2 °C). However, a noticeable increase was observed in ΔH
m (20.3 J/g), resulting in a crystallinity of 5.5%, which suggests that PLA-g-1MA enhances the compatibility between PLA and PCL, promoting more effective crystallization [
8]. Similarly, the use of 5 wt.% PLA-g-3MA produced T
m and T
cc values of 151.5 °C and 123.3 °C, respectively. The crystallinity in this case reached 3.6%, indicating moderate improvement compared to the unmodified blend.
When PLA-g-5MA was added at 5 wt.%, the melting and crystallization temperatures were 151.9 °C and 123.5 °C, respectively. While the ΔH
cc (18.6 J/g) and ΔH
m (19.1 J/g) values were relatively high, the resulting X
c remained low (0.5%). This suggests that although energy input was sufficient for crystallization, the steric hindrance introduced by the higher MA content may have limited chain mobility and thus reduced crystalline structure formation [
8].
Increasing the content of PLA-g-1MA to 10 wt.% caused a further shift in thermal behavior. The melting temperature slightly decreased to 151.7 °C, while the Tcc remained stable at 122.1 °C. The higher ΔHm (22.5 J/g) and ΔHcc (19.7 J/g) values led to a crystallinity of 3.0%, which, although lower than the 5 wt.% version, still reflects the compatibilization effect. The use of 10 wt.% PLA-g-3MA showed similar thermal behavior (Tm = 151.5 °C, Tcc = 122.4 °C), with a ΔHm of 19.5 J/g and crystallinity at 2.5%, confirming a moderate enhancement in thermal transitions.
The sample containing 10 wt.% PLA-g-5MA exhibited the lowest Tm (150.4 °C) and Tcc (120.0 °C) of all the formulations. Despite showing the highest enthalpy values (ΔHcc = 21.2 J/g and ΔHm = 21.4 J/g), its crystallinity remained low (1.2%), reinforcing the idea that excessive MA functionalization may hinder efficient crystal formation due to reduced chain flexibility and potential crosslinking effects.
In conclusion, the addition of PLA-g-MA compatibilizers, particularly PLA-g-1MA, significantly modifies the thermal behavior of PLA/PCL blends. Moderate concentrations (5–10 wt.%) enhance compatibility and crystallinity, with PLA-g-1MA showing the most promising results. In contrast, excessive MA content, especially in PLA-g-5MA, appears to limit crystallization despite increased thermal energy absorption. These findings support the use of functionalized PLA to tailor the thermal properties of biodegradable polymer blends.
Thermogravimetric analysis (TGA) and its derivative (DTG) reveal the thermal behavior of PLA/PCL formulations with different concentrations of MA as a compatibilizer (see
Figure 4 and
Figure 5). In PLA 20PCL, the main degradation occurs between 350 and 400 °C, with a single well-defined stage, indicating typical thermal degradation of PLA. When incorporating PLA-g-MA, variations in thermal stability are observed, with a slight decrease in the initial degradation temperature, possibly due to the presence of modified bonds that influence the polymer’s decomposition. In the PLA/PLA-g-1MA/5PCL formulation, thermal degradation follows a similar pattern to PLA 20PCL, although with slight variations in the DTG curve; this suggests that compatibilization does not drastically alter thermal stability. However, when increasing the amount of MA to 3MA and 5MA, the DTG curves show a greater dispersion of degradation peaks, indicating a more thermally heterogeneous structure, likely due to interactions between MA and PCL. The PLA/PLA-g-5MA/5PCL formulation exhibits slightly higher thermal stability compared to the other modifications, suggesting that a higher concentration of MA may improve the thermal resistance of the material. In conclusion, the addition of MA modifies the thermal degradation of the PLA/PCL system, with a tendency to generate more complex structures and potentially enhance thermal stability when higher MA concentrations are used.
In the PLA 20PCL formulation, the main degradation occurs in the 350–400 °C range, indicating that the addition of 10% PCL does not drastically alter the thermal stability of PLA. However, the presence of multiple peaks in the DTG curve suggests the occurrence of multi-step degradation processes. Upon incorporating PLA-g-1MA, the degradation temperature does not vary significantly, and the DTG curve retains a profile comparable to that of PLA 20PCL, suggesting that the compatibilizer does not substantially modify the overall thermal degradation behavior. In contrast, when increasing the amount of MA to 3MA and 5MA, a broader distribution of degradation peaks is observed, which indicates a more complex interaction between PLA, PCL, and MA, likely associated with morphological changes in the blend that influence its thermal response.
In particular, in the PLA/PLA-g-3MA/10PCL formulation, the DTG curve shows a broadening of the peaks, indicating that degradation occurs less uniformly, likely due to improved compatibility between the phases, which generates regions with different thermal resistance. On the other hand, the PLA/PLA-g-5MA/10PCL formulation exhibits a slight improvement in thermal stability, with a DTG curve displaying multiple well-defined peaks, suggesting a greater homogenization of the polymeric system and better interactions between PLA and PCL in the presence of 5MA.
Overall, it can be concluded that increasing the amount of MA alters the thermal degradation process, promoting greater compatibilization between PLA and PCL, although with a possible impact on the uniformity of thermal decomposition. The formulation with 5MA appears to be the most thermally stable among the options analyzed, making it an interesting candidate for applications where a balance between compatibilization and thermal resistance is required.
3.3. Mechanical Properties
The analysis of mechanical properties is essential to understanding the structural behavior of polymeric materials and their suitability for specific applications. In this study, key parameters were evaluated, such as elongation at break, which reflects the material’s ability to deform before fracturing; maximum shear stress, which relates to the material’s resistance to mechanical loads; as well as impact strength and Shore D hardness, which provide insights into the material’s toughness and surface rigidity, respectively. These tests, together with the stress–strain graph shown below, allow for the assessment of how PLA modification with PCL and PLA-g-MA affects the mechanical performance of the system, offering a comprehensive view of its ductility, structural strength, and stability under impact deformation. The stress–strain graph is shown below (see
Figure 6).
Pure PLA exhibits a very low elongation at break (12.6% ± 5), indicating its brittle nature (see
Figure 7). In contrast, PLA 20PCL shows a significant improvement (40% ± 13), suggesting that the addition of PCL increases the material’s ductility.
In formulations containing PLA-g-MA, the elongation at break varies depending on the percentage used. The 5 PLA-g-MA formulation shows values of 46.2% ± 13, 40.7% ± 11, and 20.9% ± 20, indicating a general improvement in ductility compared to pure PLA, but with a high standard deviation, suggesting substantial variability in the results. In the case of 10 PLA-g-MA, values range between 20% ± 11 and 38.4% ± 12, with an intermediate value of 37% ± 17.6. This suggests that a higher PLA-g-MA content does not necessarily lead to a consistent increase in elongation at break and that the material may exhibit heterogeneous behavior.
Overall, the addition of PCL significantly improves ductility, while PLA-g-MA also increases elongation at break, although with greater variability, which could indicate inconsistencies in the material’s structure or in phase dispersion.
Pure PLA continues to show the highest maximum strength (76 MPa ± 1.8), while PLA 20PCL exhibits a significant reduction (59 MPa ± 1.7), suggesting a decrease in stiffness due to the addition of PCL (see
Figure 8).
In the formulations containing PLA-g-MA, variations in strength are observed depending on the percentage used. The 5 PLA-g-MA formulation shows values of 49.7 MPa ± 1.8, 52.8 MPa ± 2, and 52.7 MPa ± 5, indicating a decrease compared to pure PLA, although with relatively stable behavior across the different measurements. In the case of 10 PLA-g-MA, the values range from 53.8 MPa ± 2.8 to 50.3 MPa ± 3.5 and 50.77 MPa ± 2.5, suggesting that variability increases with a higher PLA-g-MA content.
Overall, the addition of PLA-g-MA reduces strength compared to pure PLA, although some values suggest a slight improvement over PLA 20PCL. Furthermore, the standard deviation increases with higher PLA-g-MA concentrations, indicating greater dispersion in the obtained values and possibly lower homogeneity in the material’s microstructure.
The impact test results show a clear trend in the resistance of PLA and its modifications (see
Figure 9). Pure PLA exhibits the highest impact strength value at 42.1 KJ/m
2, with a standard deviation of 7, indicating moderate variability in the results. However, when 20% PCL is added, the impact strength decreases significantly to 26.3 KJ/m
2, with a lower standard deviation of 3, suggesting a more homogeneous blend but with a lower impact absorption capacity. When 5% PLA-g-MA is introduced, an increase in impact strength to 34 KJ/m
2 is observed, with standard deviations of 5 and 6, indicating a partial recovery of the mechanical properties lost with the addition of PCL. This suggests that compatibilization with PLA-g-MA helps improve stress transfer between the material phases, although the original strength of pure PLA is still not reached. On the other hand, with 10% PLA-g-MA, impact values show greater variability, with records of 29 and 31 KJ/m
2 and standard deviations of 6.5 and 3. This dispersion indicates that phase interaction remains a determining factor and that compatibilization does not fully achieve homogeneity in impact resistance.
In general, it can be concluded that the incorporation of PCL significantly reduces the impact resistance of PLA, likely due to a decrease in the material’s stiffness. However, the introduction of PLA-g-MA partially improves resistance, indicating that it acts as a compatibilizing agent by enhancing phase adhesion. Despite this improvement, the dispersion in values suggests that compatibilization is not entirely effective and that there may be regions with differences in phase structure and distribution.
The Shore D hardness results obtained reflect relatively low variability in most measurements (see
Table 4), with values ranging from 72.0 to 75.5, indicating that the material maintains moderately consistent hardness. The average value is approximately 74.3, suggesting that the analyzed material exhibits relatively high hardness within this category of polymers. Looking at it in more detail, the lowest recorded value is 72.0, with a standard deviation of 2, implying lower hardness in that specific measurement, although still within an acceptable range. On the other hand, the highest value obtained is 75.5, with a deviation of 0.58, indicating high uniformity in that measurement and more stable hardness. The remaining samples show intermediate values, such as 73.5 with a deviation of 3, which suggests greater variability in that specific sample, and 74.7 with a deviation of 2.6, indicating a tendency to maintain hardness around that value, albeit with some dispersion in the results.
Overall, the material displays moderately high and stable hardness, with some variations in certain samples that may be attributed to differences in the internal structure of the material, testing methodology, or the distribution of its components.
3.5. Morphological Characterization
The SEM micrographs present the fractured surfaces of various PLA/PCL blends at two different magnifications (10 µm and 1 µm) (see
Figure 11). These images provide insight into the morphological characteristics and the degree of compatibility between the PLA matrix and PCL phase, especially when modified with maleic anhydride (MA).
The first sample (
Figure 11a), corresponding to the PLA/20PCL blend, shows a typical sea-island morphology, where discrete spherical PCL domains, with dimensions ranging between 1 and 3 μm, are dispersed in the PLA matrix. This morphology is characteristic of immiscible polymer blends, where one phase (in this case, PCL) is finely dispersed in the continuous phase (PLA). As reported in the literature [
28], the viscosity of PCL at 180 °C is significantly lower than that of PLA, which results in a high viscosity ratio. This high viscosity contrast contributes to the formation of spherical domains during melt blending, as the lower-viscosity PCL tends to form droplets rather than co-continuous structures. Also, a clear phase separation is observed with PCL appearing as spherical domains without adhesion to the PLA matrix; voids are evident at the interface.
In the second sample (
Figure 11b), PLA-(PLA-g-1MA)/5PCL, the size of the dispersed phase increases, but there is still no visible improvement in interfacial adhesion.
In the third sample (
Figure 11c), corresponding to PLA-(PLA-g-3MA)/5PCL, the morphology appears smoother and more continuous. The voids are more uniform and less pronounced, which reflects an improved level of compatibility. The higher amount of MA grafting (3MA) contributes to better phase adhesion and reduced interfacial tension between PLA and PCL. In this case, a reduction in the size of the PCL domains is not observed [
29]. However, when increasing the PLA-g-MA content to 3 wt.%, the appearance of certain filamentous structures is evident. These features are likely due to the increased ductility of the system, suggesting that although domain refinement is not clearly achieved, the morphological changes reflect the enhanced deformability of the dispersed phase.
In the fourth sample (
Figure 11d), PLA-(PLA-g-5MA)/5PCL, no distinct phase separation can be observed in the SEM micrographs. The morphology appears more homogeneous, with a continuous structure suggesting a high degree of compatibility between the PLA matrix and the PCL phase. The absence of visible domain boundaries indicates that the maleic anhydride grafting at 5 wt.% may have effectively enhanced the interfacial adhesion and molecular interactions between the two polymers. However, despite the lack of clear phase separation, the presence of discrete particles within the matrix is still noticeable. These particles are likely associated with the precipitation or phase segregation of excess maleic anhydride or unreacted grafting residues. This observation suggests that while compatibilization improves, there may be a limit beyond which additional grafting does not further refine the morphology and could instead lead to the formation of secondary structures or by-products.
Finally, upon analyzing the PLA-(PLA-g-1MA)/10PCL, PLA-(PLA-g-3MA)/10PCL, and PLA-(PLA-g-5MA)/10PC SEM images (
Figure 12), a morphology like the one described previously (
Figure 11d) is observed.