Abstract
In this work, CeO2 nanoparticles were synthesized via the chemical precipitation method. With this objective, two distinct surface functionalization methodologies were applied: the first one uses anionic surfactant (SDS), and the second one uses hexadecanoic acid (C16H32O2). During the development of this work, nanostructured films were obtained via direct mixing and the solvent evaporation method (in situ and ex situ). This material was characterized via thermogravimetry (TGA), differential scanning calorimetry (DSC), field emission gun scanning electron microscopy (FEG-SEM), infrared absorption spectroscopy (FTIR), Raman spectroscopy and X-ray diffraction (XRD). By XRD, when there is adequate incorporation and dispersion of nanoparticles, the characteristic peaks of the CeO2 crystalline planes are observed in the nanocomposites, and by SEM, their microstructures are evaluated to verify the dispersion. The results obtained showed that the synthesis protocols tested for the intended nanocomposite, with in situ or ex situ functionalization, were satisfactory. According to these results, it was possible to observe the agglomeration of nanoparticles without functionalization and confirm the nanometric scale for CeO2 nanoparticles synthesized without functionalization and with in situ functionalization (SDS), and their diameters were between approximately 10 and 15 nm. Additionally, for the PMMA powder, the Tg was 114 °C, whereas for the nanocomposite films, it averaged 53 °C, suggesting that the solvent acts as a plasticizing agent in the studied samples, thus reducing the Tg value. However, when samples obtained from the ex situ protocol by phase transfer with palmitic acid were analyzed, uncertainties were found regarding the adequate dispersion of CeO2 nanoparticles in PMMA, with in situ functionalization by SDS being the most promising.
Keywords:
Nanocomposite; PMMA; CeO2; Surface Functionalization; Phase Transfer; Functional Coating
1. Introduction
In the last few years, many different materials have created a new generation of materials for the future1-3. Currently, nanocomposite materials represent new alternatives to overcome the application limitations of conventional materials, becoming materials of the near future, mainly owing to their advantages, such as high surface/volume ratios; good mechanical, thermal and electrical properties; and improved optical properties1-3. Inside this context, nanocomposite-functionalized coatings are the focus of several technological studies and developments, as they can present exclusive physical and chemical properties once selected nanoparticles can improve polymeric matrix properties4,5.
Nanocomposite materials stand out because of their excellent physicochemical properties, which arise from the synergy of their constituents. Owing to these properties, these materials have been widely used in various applications, such as dielectric ceramics, electrochromic devices, biosensors, corrosion protection, supercapacitors and optoelectronic devices, among others6-10.
Currently, industries in the offshore11, automotive and aerospace12 areas are interested in coatings involving acrylic nanocomposites, since these materials allow the production of artifacts with excellent properties involving low electrolyte permeation, strong adhesion to the substrate, thermal stability, mechanical resistance and high durability in aggressive environments13. In this context, the use of cerium-based compounds as a complement to organic‒inorganic hybrid materials has gained prominence, especially when anticorrosive coatings are used to prevent the access of aggressive species to the metallic interface of these components, owing to the cathodic protection generated by the presence of Ce3+ and Ce4+ ions11.
Among the available synthesis methods, such as hydrothermal, glycothermal, pyrolysis and precipitation methods, routes in solution are relatively low cost and easy to perform. The solution routes for cerium oxide (CeO2) synthesis have the advantage of controlling the size of the particles formed and are promising for the preparation of nanometric particles, in which the degree of agglomeration is significantly reduced because of the absence of extensive heat treatment14-16. Since the properties of dispersed particles less than 10 nm in diameter are governed by the quantum size effect, these properties are behind many applications of ceria14,17,18.
CeO2 NPs are characterized for their transparency in the visible region, with a refractive index of 2.2 at a wavelength of 632 nm. All these properties allow several applications for these nanocomposites, such as optical devices, solar cells, oxidation catalysis in fuels, antioxidant systems and several medical applications19-26.
In accordance with what was presented previously, the authors of this work consider the following results: optical properties, such as diffuse reflectance and Tauc’s plot of PMMA and PMMA/CeO2 nanocomposites; variation in the refractive index; real and imaginary parts of the optical permittivity (εʹ) and optical dielectric loss tangent (tan δ) of the PMMA and PMMA/CeO2 nanocomposites; dielectric studies of the PMMA and PMMA/CeO2 nanocomposites; and antimicrobial and antibiofilm studies of the PMMA and PMMA/CeO2 nanocomposites, which are of great interest in this area. However, this article will not address these points specifically since the objective of this publication is to characterize this material via thermogravimetry (TGA), differential scanning calorimetry (DSC), scanning electron microscopy (SEM), infrared absorption spectroscopy (FTIR), Raman spectroscopy and X-ray diffraction (XRD).
Polymerization with inorganic nanoparticles with modified surfaces can be performed through dispersion, suspension, and emulsion processes to form hybrid nanocomposites. Several synthesis parameters may influence the homogenization process for the formation of nanostructured composites27,28. Among these, the knowledge and control of the interaction between acrylic monomers and organic additives is highly important. Studies involving the coupling of molecules with inorganic groups linked to acrylic groups have been carried out to better understand the establishment of covalent bonds between these constituents, which can generate crosslinking in the structure. As a result of this interaction, these molecules improve the adhesion between the nanocomposite and the metal substrate since they prevent the aggregation of inorganic particles and generate covalent bonds between the silane groups and hydroxyl bonds28,29.
In this work, the main objective was to develop nanocomposite films based on a polymethyl methacrylate (PMMA) polymeric matrix filled with surface-modified cerium oxide nanoparticles. CeO2 nanoparticles were synthesized via a chemical precipitation route, and their surface functional groups, crystallinity, and morphology were characterized. The behavior of the PMMA/CeO2 nanocomposites was characterized via spectroscopic techniques, as their morphological and thermal stabilities were compared among the different samples produced, considering the nanoparticle functionalization protocols used.
2. Methodology
In this work, CeO2 nanoparticles were synthesized via chemical precipitation, a widely adopted method due to its cost efficiency and reproducibility. Surface functionalization was performed via two distinct strategies: (i) in situ functionalization, where the surfactant was introduced during nanoparticle synthesis, and (ii) ex situ functionalization, where surfactant modification occurred postsynthesis12.
For in situ functionalization, sodium dodecyl sulfate (SDS; C12H25SO4Na) was selected as the anionic surfactant owing to its affordability and commercial availability. For ex situ functionalization, palmitic acid (PA; C16H32O2) was employed; its long hydrocarbon chain promotes colloidal stability in organic solvents, whereas the terminal carboxylate group facilitates surface modification30-33.
PMMA/CeO2 nanocomposites were prepared by dispersing functionalized nanoparticles into PMMA dissolved in an appropriate solvent. The mixture was magnetically stirred for 48 h at room temperature until complete solvent evaporation, yielding homogeneous PMMA/CeO2 composite films.
2.1. Reagents, materials and equipment
The following high-purity reagents were employed without further purification: cerium precursor: cerium(III) nitrate hexahydrate (Ce(NO3)3·6H2O, 99%, Sigma‒Aldrich); precipitation reagent: ammonium hydroxide solution (NH4OH, 28–30% w/w, Êxodo Científica); surfactant: sodium dodecyl sulfate (SDS, C12H25NaO4S, 95%, Êxodo Científica) for in situ functionalization; palmitic acid (PA; C16H32O2, 99.5%, Neon) for ex situ modification; solvent: chloroform (CHCl3, 99.8%, ACS Científica) for polymer dissolution; and polymer matrix: commercial polymethyl methacrylate (PMMA, Acrigel ECL®) provided by Unigel Plásticos S.A.
2.2. CeO2 nanoparticle (in situ functionalized) synthesis
The functionalized nanoparticles were prepared through an aqueous precipitation route with concurrent surfactant stabilization. The precursor dissolution stage: A cerium source solution was prepared by dissolving 2.17 g of Ce(NO3)3·6H2O in 50 mL of deionized water under constant magnetic stirring until complete homogenization. Surfactant incorporation: The clear cerium solution was then mixed with 50 mL of an aqueous SDS solution (0.05 M) as a stabilizing agent. The mixture was stirred to allow precomplexation of cerium ions with the anionic surfactant. Precipitation and aging: Nanoparticle formation was initiated by the dropwise addition of 25 mL of NH4OH (1.0 M) as a precipitating agent, following alkaline hydrolysis principles reported in prior work34. The pH value was verified using pH-indicator strips, and all measurements were greater than 10. The resulting colloidal suspension was aged for 1 h to ensure complete particle growth. Purification and processing: The CeO2 NP_SDS precipitate was isolated by centrifugation (3,000 rpm), followed by three washing cycles with deionized water to remove ionic residues. The purified product was oven-dried (80 °C, 12 h) and mechanically homogenized via an agate mortar to obtain free-flowing powder.
2.3. PMMA/CeO2 (in situ functionalized) nanocomposite synthesis – NC-01
The synthesis of PMMA/CeO2 via the in situ method was initially carried out by solubilizing the polymer in powder form (as received) in the best-tested solvent, CHCl3, at a proportion of 10% (w/v). This reaction medium was maintained under slow magnetic stirring for 24 h to allow the formation of a highly homogeneous, bubble-free matrix prior to the addition of ceria nanoparticles. The incorporation of CeO2 NP_SDS (2 wt%) was carried out by direct mixing of the solid nanoparticles (section 2.3) with the PMMA solution, followed by magnetic stirring for 4 h to ensure homogeneous dispersion. The obtained product was dispersed in a mold for casting and left to dry at room temperature for 48 h to obtain the nanocomposite film.
2.4. PMMA/CeO2 (ex situ functionalized) nanocomposite synthesis – NC-02
The ex situ method for obtaining functionalized nanoparticles was carried out via the phase transfer methodology, taking advantage of the good interaction between the carbon chain of palmitic acid (PA) and the solvent. The method consists of (i) chemical precipitation; (ii) surface functionalization (ex situ); (iii) phase transfer; (iv) phase separation; (v) preparation of the polymer matrix; and (vi) incorporation of the nanoparticles.
The precursor dissolution and chemical precipitation steps were carried out in the same manner as that adopted for the in situ functionalization protocol. Briefly, 20 mL of Ce(NO3)3·6H2O solution was prepared by dissolving 2.17 g in deionized water until complete homogenization. The solution was then added to 25 mL of NH4OH (1 mol/L – pH > 10) and initially stirred with a glass rod for a few minutes. Subsequently, the mixture was heated to 80 °C and magnetically stirred for 50 min.
Surface functionalization (ex situ): Thereafter, 0.05 g of PA (3,75% mol/%) was added, and the mixture was stirred and heated for another 1 h. After that, the heat stopped and the mixture was cooled to room temperature under stirring. The mixture was then filtered to eliminate excess particulate material.
Phase transfer: 20 mL of chloroform was added (10% w/v), and magnetic stirring was resumed. Thus, owing to intermolecular forces, the functionalized nanoparticles should migrate to the organic phase. This process was experimentally monitored by light dispersion (Tyndall effect), a phenomenon in which light is scattered by colloidal or suspended particles, making the light beam visible as it passes through the suspension.
The phase transfer step, or liquid–liquid extraction—a separation process in which solutes are transferred between two immiscible liquid phases, typically aqueous and organic, based on the differential solubility of the target analyte—is essential for the incorporation of CeO2 into intrinsically hydrophobic PMMA. Phase separation: The organic phase, containing the functionalized nanoparticles after phase transfer, was collected using a separatory funnel.
Preparation of the polymer matrix: The polymer matrix was prepared as previously described in Section 2.3. PMMA was dissolved in chloroform and maintained under magnetic stirring for 24 h. Incorporation of the nanoparticles: However, in this protocol, the previously collected chloroform aliquot was added to the PMMA/CHCl3 solution under magnetic stirring for an additional 3 h. After this period, the mixture was transferred to a mold for solvent elimination and dried at room temperature for 48 hours to obtain a 2% (w/w) nanocomposite film.
2.5. Characterization
The following techniques were used for the characterization of CeO2 NPs: Fourier transform infrared spectroscopy (FTIR), Raman spectroscopy, X-ray powder diffraction (XRD), and scanning and transmission electron microscopy (SEM and TEM) were performed for some produced samples. To characterize the PMMA/CeO2 NP_SDS nanocomposites, FTIR, XRD, thermogravimetry (TGA/DTG), differential scanning calorimetry (DSC) and SEM analyses were performed on commercial and PMMA nanocomposites.
The infrared spectroscopy was run on a Spectrum 100 ATR FTIR spectrophotometer (PerkinElmer, Inc., United States) using an ATR accessory with germanium crystals. The FTIR spectra were recorded with 16 scans per spectrum and a resolution of 4 cm-1.
The Raman spectra were obtained via a Horiba LabRam HR Evolution confocal spectrophotometer (Horiba, Ltd., Japan), featuring a spectral resolution of 2 cm-1, an argon laser (λ = 514.5 nm), at room temperature, with a power of 10 mW.
The XRD powder patterns were obtained by using a Philips X’Pert MRD high-resolution diffractometer for nanoparticles (Philips Analytical, The Netherlands) as well as Bruker D8 Advance (Bruker Co., United States) for nanocomposites, in both cases employing Cu Kα radiation (λ = 1.5406 Å) and setting 40 kV and 20 mA.
Field emission scanning electron microscopy (SEM) was performed on a model MIRA 3 FEG-SEM (TESCAN USA, Inc. United States) using a 5 kV beam voltage. Images from transmission electron microscopy (TEM) were captured via a JEOL JEM-2100 microscope equipped with an energy-dispersive X-ray (EDS) spectrometer (JEOL Ltd., Japan) using an accelerating voltage of 200 kV.
The aggregate size analysis was performed using ImageJ by measuring at least 80 individual aggregates from representative microscopy images. The aggregate diameters were obtained using an ellipsoidal fitting approach, and the values reported correspond to the mean diameter calculated from these measurements.
TGA‒DTG curves were obtained via a SEIKO EXSTAR instrument, model TG/DTA 6200 (SII NanoTechnology Inc., Japan). The parameters used were as follows: flow rate of 100 mL min-1 for both purge gas atmospheres (synthetic dry air and N2); heating rate of 10 °C min-1 for all analyses; and sample mass of approximately 10 mg in an alumina crucible.
The DSC Q20 module (TA Instruments Co., United States) was used to record the DSC curves. The purge gas used was N2 with a flow rate of 40 mL min-1. The heating rate was 10 °C min-1, and the sample mass was approximately 10 mg. The heating cycles were carried out in the temperature range between 0 and 125 °C. Aluminum crucibles with perforated lids in the center were employed during the analysis.
3. Results and Discussions
3.1. CeO2 nanoparticles
3.1.1. FTIR and Raman spectroscopy
The infrared spectroscopic spectrum of the CeO2 NPs with no functionalization is presented in Figure 1a. A broad band in the range of 3349 cm-1 can be attributed to the stretching vibration of the O–H bond in the OH groups from residual water and the hydroxylic groups generated by the synthesis process. In their studies on the properties of CeO2 NPs, Jayakumar et al.34 attributed the band observed at 1630 cm-1 to the OH vibration mode of water molecules. They emphasized that for any synthesis method in an aqueous solution, there will always be residual water molecules and OH groups on the CeO2 NPs, which will be detected via FTIR spectroscopy.
The absorption peaks at 1325 and 1509 cm−1 can also be attributed to physically adsorbed water molecules. The bands located at approximately 1048 cm-1 can be related to C–O stretching. These bands are due to atmospheric carbon dioxide since cerium oxide readily absorbs atmospheric water and air. The FTIR spectra presented absorption peaks at 880 cm−1 and 650 cm-1, which are typical peaks of Ce–O bond stretching vibrations34-36.
Ramachandran et al.36 reported the influence of pH on the synthesis and characterization of cerium oxide nanoparticles and observed that the band around 2300 cm-1, associated with the C=O stretching vibration, appears only when the nanoparticles are obtained at pH values below 10. As shown in Figure 1a, this band is not observed, indicating that the reaction medium had a pH above 10. In contrast, the band at 880 cm-1 is assigned to a Ce–O stretching, which is characteristic of cubic CeO2.
Therefore, to complement the FTIR analysis, RAMAN spectroscopy analysis was performed, according to the results presented in Figure 1b. The results obtained from the Raman spectrum clearly revealed the characteristic band corresponding to the elongation vibration of the Ce-O bond at approximately 466 cm-1, similar to that reported in the literature34,37.
3.1.2. X-ray diffraction (XRD) patterns
XRD analyses were used to qualitatively evaluate the peak positions corresponding to the respective planes in the crystalline structure in the spectra of the CeO2 NPs and CeO2 NP_SDS (Figure 2). The sample diffractograms were indexed according to ICSD form 01-081-0792 as CeO2, a cubic crystalline system, with network parameters a = b = c = 5.4124 Å and space group Fm-3 m. Well-defined and narrow peaks can be observed, which indicate the good crystallinity of the samples.
The size of the crystallites (d) can be obtained via the Scherrer equation (presented in Equation 1), in which λ is the wavelength of the incident X-ray (0.15406 nm); θ is the angle of incidence of the X-ray; β is the FWHM (full width half maximum); and k is the Scherrer constant with an approximate value of 0.94. CeO2 NPs had crystallite sizes of approximately 14.8 nm, and CeO2 NP_SDS had crystallite sizes of approximately 12.7 nm38.
In the in situ functionalization protocol, nanoparticle formation and surface modification occur simultaneously. This approach is primarily employed to overcome the inherent instability of freshly synthesized nanoparticles, which are prone to rapid agglomeration and oxidation. As a result, this procedure generally yields smaller nanoparticles due to factors such as growth inhibition associated with reduced nucleation activity and adsorption onto developing nanocrystals. Furthermore, surface functionalization provides a protective layer that mitigates the effects of the high surface-area-to-volume ratio and magnetic attraction forces that typically lead to particle aggregation, thereby enhancing system stability.
3.1.3. Scanning electron microscopy (SEM) and transmission electron microscopy (TEM)
Scanning electron microscopy (SEM) was used to verify the morphology of the CeO2 nanoparticles synthesized without functionalization, as presented in Figure 3, where there was significant agglomeration.
SEM images of CeO2 NP microstructures (SEM) with magnifications of (a) 7,92 kx and (b) 19,1 kx. TEM images of CeO2 NPs (c) 20 nm, (d) 10 nm scale, and CeO2 NP_SDS (e) 20 nm, and (f) 10 nm scale.
Microstructures are essentially formed by the agglomeration of smaller particles with irregular shapes and contours. It is possible to observe the formation of gaps between the clusters, which gives rise to a highly porous structure. According to Zheng and collaborators39, these pores provide access to the internal part of the structure, enabling them to act as effective transport pathways. Additionally, the porous structure associated with the crystal facets significantly increases the surface area of the sample.
Furthermore, consistent with previous studies by Wang et al.40, the micrographs reveal a wide particle size distribution, with agglomerates of smaller particles exhibiting irregular shapes and sizes.
Transmission electron microscopy (TEM), which is typically used for the characterization of materials at the nanoscale, was used to verify the morphology of the synthesized CeO2 NPs and CeO2 NP_SDS, according to the images presented in Figures 3cf.
For both the micrographs obtained for CeO2 NPs and CeO2 NP_SDS, their diameters were in the range of 10–15 nm, and no significant difference in size was observed. The observed nanoparticle diameters confirmed the results obtained by calculating the crystallite sizes via X-ray diffraction (XRD) (14.8 nm for CeO2 NPs and 12.7 nm for CeO2 NP_SDS). These results are in accordance with those of Parlak and Demir41. This finding is similar to the results presented by Wang and Feng16, who reported a textured distribution of nanoparticles deposited on a substrate surface with a preferential orientation.
The micrographs of CeO2 NP_SDS have a more regular and orderly format than nanoparticles without functionalization, which indicates that the surfactant has a relevant ability to homogenize the morphology of the nanoparticles. This fact is corroborated by Paschalidou and Theocharis42 who reported that surfactants have the ability to involve nanoparticles, favoring the formation of specific phases and determining the shape of particles and their surface properties.
3.2. PMMA/CeO2 NPs
The FTIR results obtained for the characterization of the PMMA/CeO2 nanocomposite samples are presented in Figure 4 and are compared with the results obtained for a pure PMMA film. NC-01 is functionalized in situ (SDS surfactant), and NC-02 is functionalized ex situ (palmitic acid). It is possible to compare the spectra of the films obtained with the respective functionalizing reagents and the functionalized nanoparticles obtained via in situ (SDS) and ex situ (PA) procedures.
Comparison of the FTIR spectra of (a) PMMA, (b) NC-01, (c) CeO2 NP_SDS, (d) SDS, (e) NC-02, (f) CeO2 NP and (g) PA.
For PMMA (Fig. 4a), according to the literature43, there is a distinct absorption range between 1150 cm-1 and 1250 cm-1, which can be attributed to the C-O-C stretching vibration. The band at 1732 cm-1 corresponds to the presence of the carbonyl acrylate group. The two bands at 2997 cm-1 and 2952 cm-1 can be attributed to the stretching vibrations of the C‒H bonds of the -CH3 and -CH2 groups, respectively. The signal at 754 cm-1 can be attributed to the vibrations of the α-methyl group.
Due to the small amount of incorporated NPs and the strong intensity of the PMMA polymer matrix peaks, the characteristic peaks of CeO2 were suppressed and are not distinguishable. However, for NC-01 presented in Fig. 4b, the characteristic bands of the SDS surfactant used in nanoparticle functionalization became evident. Absorptions such as those located at 2849 cm-1 and 2917 cm-1 are related to aliphatic -C-H stretching frequencies; those at 1216 cm-1 are due to -S=O stretching; peaks originating from the -S-O-C group at 993 cm-1 and 828 cm-1; and bands at 1468 cm-1, 1377 cm-1 and 721 cm-1 refer to -C-H bending of methyl and methylene groups. Finally, the band at 1081 cm-1 represents the characteristic vibration of the SO42- Group35-39. Therefore, this confirms the incorporation of CeO2 NP-SDS into the polymer matrix.
As shown in Fig. 4e, the spectrum of PA-functionalized sample (NC-02) indicates that functionalization with PA was clearly less effective than with SDS. Only a weak signal corresponding to the band at 2847 cm−1, assigned to the symmetric stretching vibration of –CH2, and a slight shift of the band at 1719 cm−1, compared to those at 1732 cm−1 for PMMA and 1699 cm−1 for PA—both associated with the respective carbonyl groups—are observed. For both nanocomposites, the characteristic PMMA bands are clearly visible.
The nanoparticle X-ray diffraction patterns (Figure 5) were indexed as CeO2 based on the ICSD card No. 01-081-0792.
Only the NC-01 diffractogram, with CeO2 NP_SDS, presented peaks related to cerium oxide, suggesting the effective incorporation of the nanoparticles in the polymer (PMMA). In the NC-02 diffractogram, the peaks could not be well defined, which indicates that there were problems in the incorporation and/or dispersion of the nanoparticles in this sample. The NC-02 diffractogram has a similar profile as that of PMMA, which is characteristic of amorphous solids.
However, as reported by Parlak and Demir41, when the amorphous characteristic of PMMA stands out in relation to CeO2 peaks, the sample diffractogram has a smoother profile, which in fact occurs with the NC-02 diffractogram. In addition, the percentage of nanoparticles incorporated into the polymer matrix can be considered too low to be identified only by XRD.
For the TGA/DTG analyses, the atmosphere was varied, and the thermogravimetric curves obtained are presented in Figure 6a for the synthetic air atmosphere and Figure 6b for the N2 atmosphere.
TG‒DTG curves of the PMMA, NC-01 and NC-02 nanocomposites in (a) a synthetic air atmosphere and (b) a N2 atmosphere.
From the TGA/DTG curves presented in Figures 66b, at least two stages of thermal decomposition were identified for the PMMA film. The literature44-47 also reported the presence of 2 stages of thermal decomposition for PMMA, and they divided the first stage into two stages, as can be observed by the inflection of the curve at this stage.
The first stage of thermal decomposition of PMMA occurred at approximately T1onset = 119 °C and resulted in a mass loss (Δm1) of 17.51%. The second stage of thermal decomposition showed variation in the start temperature (T2onset) between 286 and 336 °C, but this resulted in a mass loss (Δm2) of 81.80% for the analyzed samples.
According to the Zheng et al.39, the thermal decomposition of PMMA is a process characterized by high monomer yields in the products of degradation and a slow decrease in the molar mass of the polymer. This characteristic explains why the main stage of degradation presented a mass loss greater than 80% when the C‒C bonds were split, which are the most stable bonds in the PMMA structure.
Additionally, from the TGA/DTG curves presented in Figures 66b, it is possible to observe that the PMMA/CeO2 nanocomposites maintain the same thermal behavior as the pure PMMA film, in which two stages of thermal decomposition of the material are identified.
In general, in a synthetic air atmosphere, the first stage of decomposition for the PMMA/CeO2 nanocomposites occurred at approximately 118 °C (T1onset) and resulted in an average mass loss (Δm1) of 19%, similar to that of the pure PMMA film (T1onset = 119 °C; Δm1 = 19%). The second thermal event showed a small variation in the starting temperature for NC01 (increase of 5%, starting at 286 °C), with an average mass loss (Δm2) of 79%, which was also similar to that of the pure PMMA film (Δm2 = 79%).
At 500 °C, the percentages of residues obtained in a synthetic air atmosphere for the pure PMMA and NC-02 films were very similar, which may indicate problems in the dispersion of nanoparticles in the synthesis protocol with functionalization with palmitic acid. For NC-01, an increase of 2.8 times the residue mass was obtained compared with that of the pure PMMA film, which indicates the effective presence of CeO2 nanoparticles.
In a nitrogen atmosphere, the first thermal event for the PMMA/CeO2 nanocomposites started at approximately 122 °C (T1onset) and resulted in an average mass loss (Δm1) of 17%, similar to that of the pure PMMA film (T1onset = 122 °C; Δm1 = 17%). The second stage of decomposition was maintained at approximately 331 °C (T1onset) and resulted in a mean mass loss (Δm2) of 83% for the samples of the nanocomposites analyzed, which was also similar to that of the pure PMMA film (T2onset = 327 °C; Δm2 = 83%).
At 500 °C, the percentage of residue obtained in a nitrogen atmosphere for the pure PMMA film of only 0.14% is probably due to impurities or mild contamination during the handling of the PMMA powder or during solvent solubilization of the film. On the other hand, the percentages of residues in the nanocomposites are significantly greater than those in the pure PMMA film: 11.8 times greater for NC-01 (1.65%) and 6.3 times greater for NC-02 (0.88%). This finding indicates the effective presence of CeO2 nanoparticles in the nanocomposites and suggests that the synthesis protocol for NC-01 probably provides better dispersion of CeO2 nanoparticles in the PMMA matrix than the NC-02 synthesis protocol does.
From the previous results, there is also a small influence of in situ functionalization with SDS at the beginning of the second stage of decomposition, corresponding to an increase of 5% in the temperature in a synthetic air atmosphere and 3% in a nitrogen atmosphere, compared to the beginning for the pure PMMA film sample.
The highest percentage of residue at 500 °C was obtained for the nanocomposite films in relation to the pure PMMA film, indicating that CeO2 nanoparticles were incorporated into the PMMA matrix.
The DSC curves are shown in Figure 7. In all the DSC curves, a characteristic glass transition event was observed. The occurrence of a single Tg was observed in each sample, and the melting phenomenon was not observed, which indicates that the sample material was amorphous. Moreover, there is an inflection point in the curves below the Tg between approximately 50 and 60 °C for the films and 120 °C for the powder, indicating that the thermal stress and enthalpic relaxation are associated with the Tg of the samples.
DSC curves of the PMMA powder (a), PMMA film (b), NC-01 (c) and NC-02 (d) nanocomposites in a N2 atmosphere.
The glass transition temperatures (onset) and the corresponding standard deviations for the nanocomposites, PMMA powder, and PMMA film were 43.4 ± 0.2 °C (NC-01), 43.7 ± 0.3 °C (NC-02), 111.4 ± 0.3 °C (powder), and 54.1 ± 0.4 °C (film), respectively. All DSC measurements were performed in triplicate, and the values reported correspond to mean values. According to the manufacturer’s specifications, the experimental uncertainty of the DSC equipment is in the range of 1-2 °C; therefore, the small differences observed among the Tg onset values for the nanocomposites should be interpreted with caution, as they fall within the instrumental uncertainty of the technique.
The main difference observed in the DSC results was between the Tg values for the powder and PMMA films, which suggests that the solvent used during film formation may influence the thermal properties of the material. For the PMMA powder, the Tg was 111.4 °C, whereas for the nanocomposite films, it averaged 43 °C, suggesting that the solvent acts as a plasticizing agent in the studied samples, thus reducing the Tg value. From the DSC curves presented in Figure 7, the PMMA/CeO2 nanocomposites exhibit thermal behavior similar to that of the pure PMMA film, characterized by a deviation from the baseline in the endothermic direction, associated with the Tg, followed by an enthalpic relaxation attributed to thermal stress.
A slight trend in Tg variation was observed regardless of the nanoparticle functionalization method. Specifically, in situ functionalization with SDS yielded marginally higher Tg values, while ex situ functionalization with palmitic acid resulted in slightly lower values. These results demonstrate that the functionalization route does not exert a significant influence on the glass transition behavior of the nanocomposites.
In the present study, the observed decrease in the glass transition temperature is primarily attributed to the plasticizing effect of residual CHCl3 used during PMMA solubilization. Eriksson et al.48 demonstrated that solvent-polymer interactions play a decisive role in Tg shifts, specifically, the acidic nature of chloroform promotes strong interactions with the basic sites of PMMA, hindering complete solvent removal even after drying.
This is a critical observation, as several reports in the literature attribute Tg depressions to nanoparticle-induced mobility changes, when they may, in fact, be experimental artifacts stemming from solvent retention. This interpretation is consistent with studies on rigid nanostructures where the intrinsic effect of the filler on Tg is expected to be negligible, further pointing to the processing solvent as the dominant factor. In addition, due to the small amount of NPs added, their impact on Tg may be minimal or even nonexistent48,49.
3.2.1. Scanning electron microscopy (SEM)
From the images obtained, by contrast and differentiated shape (possibly a cluster of spheres) in relation to the polymer matrix, it was observed that CeO2 nanoparticles are effectively present in the nanocomposites (NC-01 and NC-02), with a distribution similar to that obtained in studies in the literature50-56. The dispersion of the nanoparticles in the matrix was heterogeneous, and agglomeration points were observed at greater magnifications (25.0 kx and 50.0 kx). These nanoparticle agglomeration points were more prominent in NC-02, reaching approximately 400 nm, which was probably influenced by the parameters of their synthesis process, such as the type of surfactant, temperature, number of reagents, time and direct mixing speed. In NC01, the agglomeration points were smaller, up to approximately 200 nm.
Although the dispersion was heterogeneous, it is possible to recognize nanoparticles throughout the analyzed area of the samples of all the nanocomposites, which indicates that there was no preferential concentration in a given region or that the nanoparticles were completely clustered, which allowed them to spread through the structure of the polymer matrix, changing the texture of the analyzed surface.
Notably, although the diffractogram of NC-02 (depicted in Figure 5) did not indicate the presence of peaks related to CeO2, it was possible to effectively verify the presence of nanoparticles in the micrographs in Figure 8. This fact confirms that XRD is not a fully adequate technique for evaluating the incorporation of low-concentration nanoparticles in the polymer matrix used and that, in these situations, other techniques should be used to obtain the correct characterization.
SEM micrographs of PMMA-based films: (a,b) neat PMMA at magnifications of 1.00 kx and 25.0 kx, respectively; (c,d) NC-01 film at 1.00 kx and 25.0 kx; (e,f) NC-02 film at 1.00 kx and 25.0 kx.
In general, the micrographs in Figure 8 verify that the morphology of the structure of the obtained PMMA/CeO2 nanocomposites is irregular and presents pores, such as the structure of the pure PMMA film used in this work. The porosity of the structure may be related to both the raw materials and the parameters of the synthesis process, such as the time, speed, stirring temperature, and solvent used, which can be adjusted to enable a more regular morphology.
4. Conclusions
This work investigated the synthesis of PMMA/CeO2 nanocomposites using a commercially available PMMA matrix and CeO2 nanoparticles obtained via in situ and ex situ functionalization routes. The study focused on comparing the synthesis protocols and assessing their influence on nanoparticle dispersion, structural features, and thermal behavior, providing a fundamental basis for the development of polymer-based nanocomposites with potential relevance for future applications.
Microscopy analyses revealed pronounced nanoparticle agglomeration in the absence of surface functionalization, while nanometric CeO2 particles with diameters of approximately 10–15 nm were observed for both non-functionalized and in situ functionalized (SDS) samples. FTIR, XRD, and SEM results confirmed the successful incorporation of CeO2 nanoparticles into the PMMA matrix. The PMMA/CeO2 nanocomposite films exhibited thermal behavior similar to that of the pure PMMA film, indicating that the incorporation of nanoparticles did not significantly alter the characteristic features of the polymer matrix.
The results demonstrate that the slight variation in the glass transition temperature of the nanocomposites is predominantly influenced by solvent-polymer interactions from the film-casting process. The choice of nanoparticle functionalization route showed a negligible effect on Tg, suggesting that both methods preserve the same thermomechanical behavior of the polymer matrix. In general, both the nanocomposite films and the pure PMMA film exhibited irregular and porous structures.
Although the synthesis route influenced nanoparticle dispersion and interfacial characteristics, the present study did not evaluate functional properties associated with coating performance. Therefore, no definitive conclusions can be drawn regarding the superiority of one functionalization method over another in terms of final application performance. Future studies addressing specific functional properties—such as barrier behavior, corrosion resistance, mechanical performance, or durability—are required to establish the suitability of these nanocomposites for coating applications and to determine which synthesis route is more appropriate for a given application.
5. Acknowledgments
The authors are grateful for the financial support given by the Brazilian Funding Institutions: São Paulo Foundation Research (FAPESP) (2017/16970-0; 2017/04740-0, 2018/07867-3, and 2019/18691-6) and the National Council for Scientific and Technological Development (CNPq) (140852/2018-2, 306576/2020-1 and 304876/2020-8), and this study was financed in part by the Coordenação de Aperfeiçoamento de Pessoal de Nível Superior – Brazil (CAPES) Finance Code 001. Special thanks to Laboratório Multiusuário de Microscopia de Alta Resolução (LabMic/UFG) for the TEM analysis and Laboratório Associado de Sensores e Materiais (LAS) - Instituto Nacional de Pesquisas Espaciais (INPE) for the FEG-SEM analysis.
6. Data Availability
The data utilized to buttress the conclusions of this study are available from the corresponding author upon request.
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Edited by
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Associate Editor:
Rodrigo Orefice.
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Editor-in-Chief:
Luiz Antonio Pessan.
















