1. Introduction
Polymer nanocomposites (PNCs) are considered hybrid materials composed of a synergetic combination of nanoparticles (NPs) and a polymer matrix
[1-8]. The constructions of polymers are formed by the combination of monomers, while NPs contribute to enhancing mechanical strength, thermal stability, and electrical conductivity. This combination results in superior physicochemical properties, providing PNCs with a significant advantage over conventional materials due to their higher strength-to-weight ratio, easily customizable product properties, flexible manufacturing processes, and high corrosion resistance. Consequently, PNCs offer multifaceted benefits, including greater efficiency, sustainability, and performance
[9]. PNCs are designed based on the principles of size and surface area, forming a unified system with higher reactivity. The enhanced surface-to-volume ratio of nanofillers enables improved interactions with the polymer matrix, leading to superior overall performance
[10]. There are two types of polymers available: natural and synthetic. Natural polymers are water-based and naturally occurring materials that are extracted for use, such as silk, wool, DNA, cellulose, and proteins. In contrast, synthetic polymers are artificially synthesized materials such as nylon, polyethylene, polyester, Teflon, and epoxy. The selection of the polymer type in PNCs significantly influences their final properties and application scope.
[11] For example, natural polymers like chitosan-based nanocomposites are often used in biomedical applications due to their biocompatibility and antibacterial properties, making them suitable for wound dressings and drug delivery systems,
[12] whereas synthetic polymers like polypropylene (PP)-based nanocomposites offer excellent chemical resistance and durability, making them ideal for structural components in automotive and packaging industries. Over the past decade, recent breakthroughs have been made in this field, stimulating new insights and methodologies, as depicted in
Fig. 1.
In this review, we comprehensively discuss the relationship between chemistry and physics, fabrication routes, and a multitude of characterization techniques across PNCs as outlined in
Fig. 2.
2. Chemical and Physical Properties of PNCs
Based on the interfacial interactions that occur in PNCs, two are classified into filler-polymer and filler-filler interactions. The nature of these interactions plays a critical role in defining the dispersion, mechanical reinforcement-these are a large aspect ratio; good dispersion; alignment; and interfacial stress transfer, and overall stability of the nanocomposite system. This is crucial in order to optimize composite strength and stiffness.
[13] Interfacial stress transfer is a key factor influencing the mechanical properties of PNCs, as it governs the efficiency with which an applied load is transferred from the polymer matrix to the dispersed nanofillers. This process depends on the surface chemistry of the fillers, polymer-filler adhesion, and interfacial bonding strength. Functionalization of nanofillers, such as grafting with compatible polymer chains or incorporating chemical linkers, enhances adhesion and promotes efficient load transfer, reducing stress concentrations and improving durability.
[14] Furthermore, the overall stability of PNCs is influenced by a combination of thermodynamic compatibility, interfacial energy, and processing conditions. Strong interfacial interactions prevent phase separation and ensure long-term structural integrity, which is essential for maintaining consistent mechanical performance under varying environmental conditions. The interplay between these factors determines the final properties of PNCs, making precise control of interfacial interactions a crucial aspect of material design and optimization.
[15]From a physical perspective, PNCs demonstrate improved mechanical properties, including increased tensile strength, modulus, and impact resistance, attributed to strong interfacial interactions between the polymer matrix and the dispersed nanofillers. Additionally, their enhanced thermal properties, such as higher thermal conductivity and stability, make them suitable for applications in extreme environments. The electrical properties of PNCs can also be tuned by selecting appropriate nanofillers, allowing them to function as conductive materials for energy storage and electronic devices. Moreover, their barrier properties, crucial for packaging and protective coatings, are significantly improved due to the incorporation of nanoscale reinforcements. Chemically, PNCs offer remarkable chemical resistance to aggressive solvents, oxidation, and environmental degradation. The chemical stability of PNCs is largely influenced by the nature of nanofillers and their interaction with the polymer matrix. Functionalization of nanofillers further enhances interfacial adhesion, dispersion, and reactivity, leading to tailored chemical performance. This controlled modification enables applications that require specific chemical functionalities, such as biomedical coatings, drug delivery systems, and chemical sensors.
PNCs have garnered significant attention for their ability to bridge intrinsic material properties with a wide range of practical applications. They are extensively utilized across diverse fields, including energy storage and conversion, environmental sustainability, biomedical engineering, and biosensing. In the energy sector, PNCs are utilized in lithium-ion batteries, supercapacitors, and fuel cells due to their excellent electrical conductivity and mechanical integrity. Their potential in environmental applications includes water purification membranes, air filtration systems, and biodegradable polymers, which address sustainability challenges. Furthermore, in the biomedical field, PNCs are widely employed in drug delivery systems, tissue engineering scaffolds, and antimicrobial surfaces, benefiting from their biocompatibility and controlled release properties. Lastly, their enhanced sensitivity, selectivity, and stability make them highly effective materials for biosensor development, enabling precise detection of biomarkers and contaminants.
As research in PNCs continues to progress, advances in nanofiller integration and polymer engineering are expected to further enhance their tunability, unlocking new applications across a broad range of disciplines. This review provides a comprehensive overview of the physical and chemical properties of PNCs and their impact on emerging technologies in energy, environmental, biomedical, and biosensor applications.
[16] PNCs exhibit superior performance enhancements, including improved mechanical strength, thermal stability, and barrier properties, due to the nanoscale interactions between the polymer matrix and nanofillers. However, their fabrication often requires precise processing techniques and incurs higher costs. In contrast, conventional polymer composites are typically more cost-effective and easier to manufacture but offer comparatively limited property enhancements, as indicated in
Table 1.[10]3. Synthesis Routes and Fabrication of PNCs
The synthesis and fabrication of PNCs involve a variety of techniques designed to ensure optimal dispersion of nanofillers within the polymer matrix, leading to enhanced properties and performance. The choice of synthesis method significantly influences the interfacial interactions, structural integrity, and functional properties of the final material. Several well-established approaches are commonly employed, including
in situ polymerization, solution blending, melt compounding, and electrospinning.
[17]In situ polymerization is a widely used fabrication technique in which monomers and nanofillers are simultaneously polymerized, ensuring a strong interfacial adhesion and homogeneous distribution of NPs. The primary advantage of
in situ synthesis is its ability to achieve highly uniform dispersion of nanofillers within the polymer matrix, enhancing compatibility and promoting strong interfacial interactions. This method involves polymerizing monomers in the presence of nanofillers, ensuring their uniform incorporation during polymer chain formation. The high level of control over filler distribution enables superior mechanical and functional properties in the final composite material.
[18] Nanocomposites of poly (anilineboronic acid) (PABA)-hybrid structure of DNA-functionalized carbon nanostructures (DNA-CNT-NEG) fabrication using in-situ polymerization achieved a highly-ordered and polyconjugated structure with superior electrical conductivity (14300 Sm
−1 at 3.0 wt% filler content).
[19] In addition, nanocomposite polymethyl methacrylate (PMMA)-noble metal nanoparticles (Pt, Pd, Cu, and Au) have uniform distribution using
in situ polymerization and achieve in increasing of tensile strength 18.8% on Pd nanoparticles/PMMA.
[20] Solution blending involves dissolving both the polymer and nanofillers in a common solvent, followed by solvent evaporation to form a well-dispersed nanocomposite structure.
[21] Solution mixing is a simple, time-efficient, and cost-effective approach for PNC fabrication. It does not require complex instrumentation or extensive chemical processing, making it an attractive option for producing thin films, coatings, and nanostructured materials with tailored functionalities.
[22] Titanium dioxide (TiO
2) and α-Vanadyl phosphate (VOP) were mixed with polyaniline (PANI), polypyrrole (PPy), polyindole (PIn), and polycarbazole (PCz) to produce nanocomposite semiconductor with conductivity 1.0028 × 10
₋4 Sm
−1 for PANI/VOP.
[23] Melt compounding is an environmentally friendly, solvent-free process that involves mixing polymer and nanofillers at elevated temperatures to achieve uniform dispersion. This approach is widely adopted in industrial applications due to its scalability, cost-effectiveness, and compatibility with conventional polymer processing techniques.
[24], [25] Polycarbonate (PC)/alumina nanocomposites using melt compounding method obtain good optical properties for coating application. The 1 wt% PC nanocomposites has good transmittance at 350 nm that approximately the transmittance of pure PC.
[26]The electrospinning method has emerged as a promising technique for fabricating nanofiber-based PNCs, offering high surface area and tunable porosity, which are crucial for applications in filtration, sensors, and biomedical scaffolds. Electrospinning is a highly versatile method for fabricating nanofiber-based PNCs. It involves applying an electric field to a polymer solution containing dispersed nanofillers, resulting in the formation of ultrafine fibers with a high surface-area-to-volume ratio.
[27] For example, Hartati et al. outlines PAN/TiO
2/Ag nanofibers membrane that performs well as air filtration media and simultaneously acts as photocatalyst for self-cleaning performance.
[28] The composite scaffold collagen/nanohydroxyapatite nanofibers increased the ultimate strength to 5 ± 0.5 MPa and the modulus increased to 230 ± 30 MPa.
[29] In addition, poly(ester urethane urea) (PHH) and poly(dioxanone) (PDO) showed an elastic modulus (~5 MPa) with a combination of the ultimate tensile strength (2±0.5 MPa), and maximum elongation (150%±44%) in hydrated condition. Adhikari et. al reported that PHH/PDO composite is comparable to the materials currently being used for soft tissue applications such as skin, native arteries, and cardiac muscles applications.
[30]Other example of PNC synthesis is illustrated in the fabrication of ZnO/FG/chitosan composites using a simple spray-coating method. This study introduced an innovative approach to deposit zinc oxide (ZnO) onto one side of a fiberglass substrate while applying chitosan on the opposite side through spray coating.
[31] Spray coating is a technique in which printing ink is propelled through a nozzle to generate a fine aerosol.
[32] This method holds significant potential for large-scale production, as it is not restricted by substrate size and requires minimal polymer usage, making it a promising alternative to conventional spin coating.
[33] Additionally, spray coating can accommodate a wide range of liquid formulations with diverse rheological properties.
[34]The selection of synthesis and fabrication techniques depends on the desired properties and application requirements of PNCs. Understanding the fundamental mechanisms governing these methods allows researchers to design nanocomposites with improved efficiency, durability, and multifunctionality. This section explores the key synthesis and fabrication strategies, highlighting their advantages, limitations, and potential advancements in the field of PNCs.
3.1 DFT calculations
In the past decades, first-principles calculations based on DFT and molecular dynamics (MD) are the two integral parts that are essentially versatile tools for understanding the behavior of PNCs. Since its early development in the 1990s, DFT has been considered a powerful approach in both quantum and classical theoretical and computational physics to describe the equilibrium morphologies, interfacial interactions, electronic properties, and material design of PNCs.
[35] MD simulations complement DFT by introducing a model based on the time-dependent behavior of atoms and molecules, considering the interatomic forces, and offering molecular-level insights into adsorption processes. MD can uncover interactions such as hydrogen bonds, van der Waals (vdW) forces, and electrostatics, critical in assessing adsorbent-adsorbate behavior. In this section, we will also revisit the versatility of such calculation methods towards data-driven high-throughput screening.
Recent breakthroughs related to energy applications are mainly aimed at overcoming the limitations of DFT in handling large-scale systems, complex microstructures, and dynamic processes. Several efforts have shown that highly efficient predictive models with good accuracy for energy-related properties like dielectric breakdown strength and electronic band gaps are pursued extensively.
[36]-[38] The significant emerging developments within the past decade are to investigate the optimum interface engineering, high-throughput phase-field modeling, and ultrahigh energy density storage devices.
[36] To address these challenges, machine learning (ML) has emerged as a powerful complement approach to DFT, offering a synchronous pathway to overcome its limitations in computational cost and scalability. In combination of DFT-generated datasets and experimental results, the impact of ML models can capture uncovered physical correlations and extend predictive capabilities beyond the reach of conventional simulations. This integration not only accelerates property prediction with high accuracy but also provides a framework for linking quantum-scale calculations to mesoscopic structures and device-level performance. For instance, ML is being integrated with DFT to bridge the gap between quantum-scale calculations and macroscopic material properties.
[39]-[43] Shen et al. introduce the integrated phase-field model to simulate the dielectric response, charge transport, and breakdown process of PNCs.
[38] The incorporated ML strategy on 6615 high-throughput calculation on the composite of P(VDF-HFP)/Ca
2Nb
3O
10 to display prominent discharged energy density nearly doubles to 35.9Jcm
−3 compared with the pristine polymer. This, in turn, is governed by the improved breakdown strength of 853MVm
−1.
[38]In terms of understanding the impact of nanofiller effects, a representative case of a microstructural diagram on the breakdown process of the PNCs is illustrated in
Fig. 3a-h. To rationalize the finding, the proposed electron avalanche model is presented for random NPs and vertical nanofibers (v-nf) in
Fig. 3i and
3j, respectively. DFT is also useful to unveil the interaction mechanism between filler and its corresponding polymer, for instance, the case of carbon nanotube (CNT)-modified nanocomposite and pyrolyzed polyacrylonitrile (PPAN) studied by Zaporotskova et al. The finding indicated that strong sorption interaction between the CNT and PPAN matrix enhances tensile strength, electrical conductivity, and thermal stability.
[44] Their DFT calculations are performed based on the Becker-Lee-Yang-Parr (B3LYP) function and the 6-31G basis. Zhu et al. reported that the impact of hydrogen bonding interaction arose between polylactic acid-graphene-microcrystalline cellulose PLA-GN-MCC and PANI composite (
Fig. 3k) contributed to the interface affinity enhancement and simultaneously total surface energy reduction, achieving superior electrochemical capacitance increased from 2.72 to 3.72 up to 221.64 mF/cm
2.
[45] The Perdew-Burke-Ernzerhof (PBE) generalized gradient approximation (GGA) functional is used to optimized the geometric structures taken into account the Grime long-range dispersion correction. This is in turn governed by the core-shell structure illustrated in
Fig. 3l. and the generation of hydrogen bonding (
Fig. 3m).
The ML algorithms could also serve as a versatile tool to identify the optimal nanofiller concentrations, dispersion patterns, and polymer matrices to achieve emerging enhanced thermal conductivity or mechanical properties. Qu et al. reported that anionic polyacrylic acid (PAA) nanocomposites exhibited the strongest adsorption affinity among various tested polymers.
[12] In this study, nonionic polyacrylamide (PAM) displayed the amide groups and hydrogen bond donor are pointing downward and upwards, respectively (
Fig. 3n). Such short amide surface distance (0.4 nm) was associated to the substantial contributions from vdW forces (
Fig. 3o). Liu et al. proposed that thermal conductivity of single-filler polymer composites can be modelled using four ML regression algorithms: random forest regression (RFR), gradient boosting decision tree (GBDT), extreme gradient boosting (XGBoost), and Gaussian process regression (GPR). The finding showed that filler volume fraction and polymer matrix thermal conductivity contributed to the outcome of thermal conductivity of PNCs, while the thermal conductivity of the filler agent had a lesser contribution.
[42] Champa-Bujaico et al. displayed that accurate prediction of mechanical properties can be realized with low computational effort in a multiscale poly(3-hydroxybutyrate) (P3HB)-based nanocomposite reinforced with different concentrations of multiwalled carbon nanotubes (MWCNTs), WS
2 nanosheets (NSs), and sepiolite (SEP) nanoclay. For instance, the mechanical stiffness was enhanced up to 132% upon addition of 1:2:2 wt% SEP:MWCNTs:WS
2.
[40]In the aspect of environmental remediation, DFT plays a role in estimating theoretical band structures, charge-density distributions, and adsorption energies in predicting the pollutant interactions on PNC membranes. For example, Reis et al. focused on the study of polymer-cellulose and cellulose acetate-based adsorbents for metal ions (Cd
2+, Cu
2+, and Cr
3+).
[47] The findings indicated that strong interactions occurred in which cellulose-Cr
3+ showed the shortest interaction distances with the highest interaction energies. Chen et al. used DFT to investigate the adsorption and degradation of ronidazole on TiO
2 surfaces.
[48] The optimized geometric structure is simulated using the B3LYP functional and subsequently treated by van der Waals corrections. It turns out that the corresponding study revealed that stable adsorption configurations and structural changes promoted the chemical adsorption and hydrogen bonding. Moreover, the activation of C-N bond in the imidazole ring facilitated photocatalytic degradation. In recent literature, integrated computational and experimental studies have successfully demonstrated how polymer functional groups modulate pollutant adsorption performance. For example, Hernández et al. investigated chitosan cross-linked with 1, 3-dichlorocetone and showed that its -NH₂ and -OH functional groups markedly enhance the removal of heavy metals (Pb, Zn, Cr). Experimentally, metal concentrations were reduced to below 0.05 mg/L, while DFT modeling revealed reduced HOMO-LUMO energy gaps and enhanced dipole moments (0.01485 eV gap for Pb) that explain the high binding affinity.
[49] Another noteworthy example is the study by Meshkat et al., who combined DFT calculations and adsorption experiments to explore arsenite (As³⁺) removal by nitrogen-doped carbon nanotube composites.
[50] Townsend et al. carried out MD simulations to examine the pollutant adsorption onto microplastics, highlighting that hydrocarbon pollutants such as PFAS and PPCPs primarily adhered via noncovalent interactions in saline environments.
[51] ML recently emerged as a powerful approach in the development and optimization of polymeric nanocomposites for water purification. By employing algorithms like artificial neural networks (ANNs), ML enables predictive modeling of nanocomposite behavior under varying conditions. Syah et al. demonstrated an ML-based model using layered double hydroxide/ metal organic frameworks (LDH/MOF) nanocomposites to predict molecular separation during adsorption processes. The ANN model achieved outstanding predictive accuracy with determination coefficients (R
2) exceeding 0.99 in both training and validation stages, outperforming traditional modeling methods.
[52]The implementation of the theoretical approach in hydrogel composites has shown their tremendous contribution in the past decade.
[53], [54] Moghadam et al. conducted a gelation experiment on incorporated nanoclay polymer gel (PG). The analysis of variance (ANOVA) was implemented to evaluate the quadratic model and depicted an R-Squared value of 0.99 when compared with actual results. This indicates that nanoclay has proven as a decisive component that could affect the gelation time significantly.
[54] In a similar approach, Mohammadi et al. conducted a swelling experiment on conventional and nanocomposite gels. The validated ANOVA suggested a promising statistical significance (P ≤ 0.0001). In addition, by increasing nanoclay concentration, the swelling degree of the gel was reduced. Recent findings by Wang et al. outlined the importance of central composite design in copolymerized acrylamide, acrylic acid, and cross-linker into a self-degradable hydrogel by free radical polymerization. It turns out that gel strength is heavily influenced during the degradation process. Wang et al used the second order polynomial and fitting the response model degradation time. The results are represented by coded values (A, B, C, and D) where A is the copolymer, B is the cross-linker, C is the ammonium persulfate as the initiator, D is the reaction temperature, and AB, AC, AD, BC, BD, and CD are the interaction terms between the factors, respectively. The results of the fitting statistics have 154.37 of mean, 10.56 standard deviation, 6.84 coefficient of variation and R2 = 0.9902. In addition, the ANOVA results is presented in
Table 2.
[55] Further analysis of three-dimensional (3D) surface plots as a response of surface methodology represents the effect of each experimental factor on the response depicted in
Fig. 4a. The degradation time of the gel prolongs as the copolymer content increases, leading to densely populated hydrogels. This is exemplified by the 3D surface plots and contour plots between degradation time depicted in
Fig. 4b and
4c, respectively. A recent review highlighted the fabrication of nanocomposite hydrogel provide a standing point into this subject, covering fundamental aspects and state-of-the-art in enhanced oil recovery.
[55]Other study by Youssef et.al investigates the mechanical behavior of PEO/SiO
2 polymer nanocomposites through atomistic MD simulations, focusing on temperature and strain rate affect the elastic properties, including Young’s modulus and Poisson’s ratio. The tensile deformations were performed under different thermal conditions, spanning temperatures from 150 K to 400 K, using two different strain rates, 1.0 × 10
−5 fs
−1 and 1.0 × 10
−6 fs
−1. In this study, the standard deviation is used to quantify the variation in local strain distributions within the PEO/SiO
2 nanocomposite under different strain rates and temperatures. The probability distribution function P(ε) of local strain is computed for specific global strain values (0.03, 0.06, 0.09) and shifting from narrow peaks that broaden as global strain increases, indicating increased the heterogeneity. Lower strain rates and higher temperatures lead to higher standard deviation values, reflecting greater variability in local strain, while higher strain rates and lower temperatures result in smaller standard deviations, indicating more uniform strain distributions.
[57]DFT in biomedical research serves as a theoretical tool to unravel detailed atomic-level insights into material and molecular interactions. In drug delivery, DFT predicts binding affinities, adsorption sites, and electronic properties of drug-carrier complexes, enabling improved loading efficiency, stability, and controlled release.
[56]-[59] In tissue engineering and wound healing, DFT elucidates the chemical behavior, biocompatibility, and reaction mechanisms of biomaterials while assessing mechanical properties, structural stability, and binding interactions critical for therapeutic performance.
[60]-[63] Furthermore, in bioimaging, DFT investigates and optimizes the structural, electronic, and optical properties of NPs, revealing molecular interactions, band gap modifications, and charge transfer processes that enhance fluorescence, photostability, and imaging resolution.
[64], [65] For example, Adekoya et al. incorporated graphene oxide (GO) into poly(ethylene glycol) (PEG) to form a GO/PEG nanocomposite as a drug delivery substrate for the antibiotic drug cephalexin (CEX).
[60] The GO and PEG structures are modelled based on B3LYP exchange−correlation with the DNP basis set. Upon CEX adsorption, the variation in terms of the pristine reduced density gradient (RDG)
[66] isosurface is quite distinct compared to the GO/PEG−CEX complex (
Fig. 4d), depicting strong hydrogen bonding that governs the binding of the drug to the nanocarrier at three different binding sites (
Fig. 4e). In terms of biosensing applications, Kumar et al. proposed that theoretical results on poly(3, 4-ethylenedioxythiophene) (PEDOT) composites (MoS
2/PEDOT: PSS) composites unveiled the adsorption feasibility of volatile organic compounds (VOCs). The integration onto predefined electrodes acting as sensors and corresponding layered structures is shown in
Fig. 4f. The interaction dynamics profile between these compounds and the substrate implies that acetone does not strongly bound compared to ethanol, however, the adsorption profile is still favorable, making it a viable candidate for gas sensing such as propanol, toluene, and hexane is summarized in
Figure (4g-i).
In summary, DFT and advanced simulations provide a theoretical foundation to essentially predict not only the optimal polymer structure but also how the polymer and filler interact. These interdisciplinary strategies highlight a shift toward computational and data-driven methods in advancing PNCs towards next-generation optic or electronic-based devices with high performance and scalability. While DFT calculations able to provide molecular-level insights into the electronic structure, interfacial interactions, and energetics of polymer-nanofiller systems, these predictions must be complemented by experimental characterization techniques, which reveal the corresponding structural, morphological, and functional properties of PNCs at the macroscopic scale.
4. Characterization Tools
A comprehensive understanding of PNCs requires advanced characterization techniques beyond conventional methods such as scanning electron microscopy (SEM) and X-ray diffraction (XRD). Emerging analytical tools offer deeper insights into the nanoscale morphology, dispersion states, interfacial interactions, and dynamic behavior of PNCs, enabling a more precise correlation between structure and their physicochemical properties. This section explores unique and sophisticated techniques that provide a multidimensional perspective on PNC architecture and functionality.
[69] The advanced characterization techniques are classified not only based on X-ray and optical operations, but also as a comprehensive approach to analyze the structural, chemical, and morphological properties of PNCs
in situ or
ex situ.
4.1 In Situ Characterizations
Several in-situ approaches are indispensable towards the multi-scale, real-time, and chemically sensitive characterization of PNCs, providing insights into their structure-property relationships and deformation mechanisms. These cover a multitude of advanced microscopies, spectroscopies, and X-ray-based techniques, namely, high-resolution transmission electron microscopy (TEM), atomic force microscopy-infrared (AFM-IR), in-situ simultaneous small and wide-angle X-ray scatterings (SAXS and WAXS), In-situ SEM with tensile stages. The following section provides a concise overview of these techniques and their relevance in PNCs research.
4.1.1 High-Resolution TEM
TEM provides detailed atomistic imaging of the PNC’s microstructure at very high spatial resolution, allowing direct visualization of individual nanofillers and their dispersion within the polymer matrix at the sub-nanometer scale. TEM offers reveals fine morphological features and internal interfaces but requires complex sample preparation and operates under vacuum conditions. Recent advancements in TEM instrumentation have focused on enhancing its spatial resolution, 3D imaging, and real-time analysis of interfacial dynamics. To name a few of the breakthroughs: Site-specific glass transition using fluorescence-based TEM of polymer-nanofiller interphases. By localizing fluorescent dyes within adsorbed polymer layers, researchers correlated
Tg variations with layer thickness in polystyrene-silica nanocomposites.
[70]-[72] This technique revealed how nanoparticle (NP) interfaces alter local polymer dynamics, providing insights into mechanical and thermal properties. To some extent, the combination of electron tomography with TEM enables the projection of 3D and four-dimensional (4D) or visualization of complex polymer morphologies, such as block copolymer gyroid structures and semicrystalline polymer lamellae. This approach overcomes limitations of two-dimensional (2D) imaging, resolving nanoscale spatial distributions critical for understanding mechanical and gas-barrier properties.
[73]-[75] Though more common in inorganic nanocomposites,
in situ TEM nanomechanical testing has been applied to study mechanical behavior enhancements, such as toughness improvements due to NP encapsulation or structural changes under mechanical stress. This method provides real-time observation of deformation mechanisms at the nanoscale in polymer-based composites. Cryogenic-TEM protocols are adapted to minimize radiation damage in soft PNCs. This enabled high-resolution imaging of organic-inorganic interfaces in hydrated or thermally sensitive systems, preserving delicate morphologies. Low-dose focal series reconstruction is considered a further extension of TEM mode that achieves submolecular resolution imaging associated with defects, grain boundaries, and distortions in the crystalline lattice of PNCs.
[76]In dealing with polymer-based samples, the major limitation of in-situ TEM technique is mainly related to the weak contrast originating from the low atomic number of light element (carbon or nitrogen).
[73] A weak interaction at the interfaces resulted the minimum difference in electron scattering between polymer matrix and filler materials. This could even worse if the bond breakage or undesired cross-linking and led to the composition alteration or breaking the polymer chains during the experiment. Consequently, the reduced capability to identify the precise interfacial width or the extent of polymer-filler interaction zones creates an intricate challenge, in particular, when the corresponding fillers are contained low atomic number or fully-dispersed. To minimize dose for imaging, one alternative is to use focused ion beam for site-specific imaging capability.
[75]4.1.2 In Situ Scanning Electron Microscopy
Conventional SEM is typically able to monitor dynamic processes (deformation, crack propagation) at micro/nano scales of PNC under mechanical/thermal stimuli. To date, further development in SEM allows for the combination of in-situ tensile stages examination that is capable of demonstrating real-time observation of morphological and structural changes in PNC under mechanical loading.
[77] These specific stages are incorporated with SEM and other imaging methods to correlate mechanical properties with microstructural evolution during deformation. A study by Delp et al. on electrospun polycaprolactone (PCL) fiber scaffolds investigated using advanced
in situ tensile testing inside an SEM. This work successfully demonstrates tensile deformation in real-time within the SEM to understand fiber response at the nanoscale.
[78] In addition, in-situ SEM combined with electron backscatter diffraction (EBSD) and electron channeling contrast imaging (ECCI) can monitor deformation-induced phase changes, dislocation activities, mechanical twinning, mapping strain localization, and texture evolution in PNCs.
[79], [80]4.1.3 Atomic Force Microscopy-Infrared Spectroscopy
AFM-IR, a scanning probe-based technique that combines chemical analysis at the nanoscale with resolutions down to 10 nm. This combined technique is potentially appealing towards the complementary investigation of nano- and microscale biological processes. In-situ AFM nanomechanical methods enable direct visualization of micromechanical behaviors and stress distributions at the nanoscale during deformation, revealing local reinforcement mechanisms, heterogeneity, and degradation in PNCs.
[81]-[85] Such technical integration promotes the high-resolution chemical mapping at the nanoscale, revealing spatial variations in filler distribution, polymer crystallinity, and interfacial bonding. Photothermal AFM-IR combines the high spatial resolution of AFM with infrared absorption spectroscopy, enabling chemical characterization at nanometer precision.
[86] This technique is particularly valuable for analyzing interfacial interactions and phase distributions in complex PNC architectures. Initially, high-resolution analysis using AFM was limited to samples that were intrinsically smooth or could be processed using a restricted range of techniques to achieve damage-free, smooth surfaces. This study presents a novel approach for nanoscale characterization of PNCs using surface techniques, which is crucial for understanding the structure-property correlations in these complex material systems. A PNC was prepared using a gas cluster ion beam (GCIB), consisting of PMMA or polystyrene (PS) confined within 7 nm diameter pores of an organosilicate matrix. After GCIB preparation, the exposed nanocomposite surface exhibited an average roughness of 0.3 nm, comparable to spin-coated films, making it well-suited for high-resolution AFM characterization. AFM-IR spectroscopy revealed no significant chemical damage to the polymer composite after GCIB etching, while nanomechanical analysis confirmed that the measured mechanical properties aligned with expectations from bulk measurements. Furthermore, AFM-IR successfully identified extensive hydrogen bonding between the carbonyl groups of PMMA and the surface silanol groups of hydroxylated organosilicate.
[87] The key limitations of AFM-IR when probing polymer nanocomposites that needs to consider: Tedious measurement time and undesired artefacts, substrate effects, sample preparation constraint, complexity in data interpretation. For instance, the spatial resolution of the technique is limited by the AFM tip size and thermal sensitivity, which can limit probing of very small nanoscale features. Another consideration is that chemical characterization related to the phase separation, and crystallization at the nanoscale require careful interpretation due to overlapping signals and complex microstructures.
[88]-[92]4.1.4 Small, Wide, and Ultra-small Angle X-ray scattering
Small-angle X-ray scattering
(SAXS), wide-angle X-ray scattering
(WAXS), and ultra-small-angle X-ray scattering
(USAXS) provide statistical and structural information on NPs and their aggregates over a broad range of length scales within a representative volume of the material. These in-situ techniques reveal particle size distribution, filler network structure, and hierarchical organization in nanocomposites, complementing microscopy data for a comprehensive characterization of PNCs.
[93], [94] SAXS and USAXS enable the characterization of structures across multiple length scales, from nanoscale filler dispersion to mesoscale aggregation. This understanding is essential for optimizing nanocomposite properties, such as mechanical reinforcement, thermal stability, and transport behavior, by tailoring filler distribution and interfacial interactions.
[95] In general, SAXS technique provides useful information regarding the structure of heterogeneous substances on the micro- or nanometer scale, irrespective of sample shape, such as solid, liquid, or any two-phase sample. In other words, the actual particle size distribution of nanofillers can be deduced, while WAXS assesses the crystalline state of the sample or phase transitions in real time (for example, during heating or mechanical loading).
[96], [97] Two respective cases Kamal et al.
[98] and Giuntini et al.
[99] outlines the success of in-situ simultaneous SAXS and WAXS to determine the evolution of dispersion of nano-fillers upon uniaxial deformation. The latter demonstrated strains within the NPs of the order of ~0.1% probed by WAXS, and the SAXS found mesoscale strains in the superlattice of ~1−3%, indicating the organic phase encounters larger deformations (~10%).
[99] Another case on thermal and mechanical loading of 15 % w/w polyvinylidene fluoride (PVDF)-Fe
3O
4 NP nanocomposite yielded the incremental changes in terms of the PVDF fibers orientation being greater than that in the nanocomposites, due to the fact that the NPs prohibit the orientation of the polymer chains.
[100]A complement approach is crucially important to fairly compare computational results and actual performances, we therefore present several studies associated to the ML applications and their experimental validations. Wang Chen et al. propose a non-negative matrix factorization-based pan-sharpening (PSNMF) machine learning method to interpret noise found in TEM energy dispersive X-ray spectroscopy data in PNC, improving phase separation and quantification.
[101] Wang et al. developed ML-driven interfacial modeling and dielectric property prediction in PNCs in which experimental data collected in TEM and SAXS can be used for validation and interpretation.
[102] Biran et al. used transmission electron microtomography (TEMT) for 3D structural observations of PNCs with sub-nanometer resolution. This technique successfully combined ML-based image analysis that enables quantitative 3D morphology characterization, including hierarchical structures and phase separations.
[76] Röding et al. introduce ML-accelerated small-angle X-ray scattering analysis of disordered two- and three-phase materials" develops a machine learning framework using Gaussian Random Fields to model materials and predicts microstructural parameters from SAXS data.
[103]It is largely understood that SAXS is a powerful and statistically relevant technique for characterizing nanoparticle size, distribution, and hierarchical structure in PNCs, its main limitations are the need for model-based data interpretation, inability to provide local structural details, signal attenuation at high temperature, reduced sensitivity to low contrast systems, necessitating complementary use of microscopy and other methods for comprehensive analysis. For instance, the image contrast limitation is heavily influenced by the differences in electron density (electron contrast) between nanofillers and the surrounding polymer matrix. In the scenario when the electron density difference is very low, then the nanofillers and polymer share similar scattering length densities. Thus, the scattering intensity becomes weak, making it difficult to detect or distinguish the nanofillers. This can obscure the filler core in SAXS patterns, complicating size and distribution analysis.
4.1.5 X-ray Photoelectron Spectroscopy with Depth Profiling
X-ray Photoelectron Spectroscopy (XPS) combined with ion-etching depth profiling enables precise chemical analysis of polymer-nanofiller interfaces. This method is particularly useful for understanding surface functionalization, interfacial bonding, and elemental distribution across multilayered PNC structures. The light-matter process works by irradiating a sample with specific monochromatic X-rays with the soft X-ray range (200 eV to 2 keV).
Fig. 5 illustrates the preparation and characterization of cellulose nanocrystal (CNC)-crosslinked shape-memory PNCs. The nanocomposites were synthesized through the condensation reaction of PCL and PEG-based prepolymers with CNCs. The hydroxyl groups on the CNC surface participated in the condensation process, leading to either physical or chemical crosslinking with polyurethane chains. To analyze the nanocomposites, XPS was used to examine the main chain elements and carbon-based bonds. As expected, carbon and oxygen were the primary elements detected. The high-resolution C1s spectra revealed that the chemically crosslinked sample had a higher O-C=O content than the physically crosslinked one, confirming the successful condensation reaction between CNCs and the prepolymers.
[104] This results in the emission of photoelectrons whose energies are characteristic of the elements within the sampling volume.
[105] 4.1.6 Neutron Scattering Techniques
Small-angle neutron scattering (SANS) and neutron spin echo (NSE) provide high sensitivity in analyzing nanostructure evolution, polymer chain dynamics, and the spatial distribution of nanofillers.
[106] It can provide information on the size, shape, and structure of polymers as well as associated thermodynamic quantities. These methods are particularly useful for investigating self-assembled architectures and filler-polymer interfacial behavior in soft matter systems.
[107] SANS has been widely used to study the structural evolution of various materials, including polymers, PNCs, alloys, and biological systems. A notable application of SANS was in confirming Paul John Flory’s theory on the Gaussian coil conformation of polymer chains, contributing to his Nobel Prize in 1974.
[108] SANS has been applied in PNCs to investigate microstructure-property relationships, such as in filled silicone rubber, where contrast variation and time-resolved Rheo-SANS revealed interactions between the matrix, interface, and filler networks.
[109] Additionally, SANS has been used to analyze hydrogels, providing insights into microstructural evolution under temperature changes and aiding in the design of functional materials. Other studies have employed SANS to confirm surface fractal structures in hydrogels and to examine phase homogeneity.
[110] More recently, SANS has been instrumental in studying the structural evolution of lithium anodes in advanced battery technologies.
[111]4.2 Ex-situ Characterizations
Several conventional ex-situ methods offer a multitude of aspects to complement the previous discussion. The overview focused on nuclear magnetic resonance (NMR) spectroscopy, fluorescence lifetime imaging microscopy (FLIM), tip-enhanced Raman spectroscopy (TERS), positron annihilation lifetime spectroscopy (PALS), and gas chromatography (GC).
4.2.1 Solid-state nuclear magnetic resonance spectroscopy
The high sensitivity of the solid-state NMR spectrum, along with relaxation factors affecting the polymer chain, promotes solid-state NMR as an efficient technique for analyzing polymer filler interfaces. This spectrum differentiates the polymer interactions at the interface compared to the bulk phase. In both pristine polymers and their nanocomposites, the relaxation period exhibits a two-component decay. However, in the case of pristine polymers, the longer component is directly related to temperature, as the motion of polymer chains is strongly influenced by temperature. In contrast, for nanocomposites, temperature has a lesser effect on chain mobility compared to uncontaminated polymers. This is due to the interaction between the filler and the polymer chain, which restricts the movement of the polymer chains.
[112]Solid-state NMR is useful for investigating the effects of temperature and nanocomposite composition on the dynamic performance of ionic species (i.e., the inorganic phase) and polymer chains (i.e., the organic phase). Souza et al. utilized solid-state NMR to optimize the synthesis conditions for lithium-doped siloxane-poly(propylene glycol) nanocomposites and to obtain insights into their microscopic molecular performance. The study revealed that the thermal and electrical performance of solid electrolytes depends on the movement of these species, and conductivity is facilitated through the segmental motion of polymer chains.
[113] Additionally, NMR has found extensive applications in the characterization of liquid polymer electrolytes,
[114], [115] solid polymer electrolytes,
[116] and PNC electrolytes for lithium-based energy sources developed in recent years.
[117]4.2.2 Fluorescence Lifetime Imaging Microscopy
Fluorescence microscopy and FLIM are powerful microscopy techniques for investigating and uncovering information on micro- and nanometer length scales. FLIM is an advanced optical technique that maps fluorescence decay kinetics, providing insights into molecular interactions, polymer degradation, and filler dispersion. Its ability to monitor dynamic changes in PNCs makes it valuable for studying material response under mechanical or environmental stress.
[118]-[120] FLIM allows for determining the fluorescence decay lifetime of dyes covalently attached to polymer chains, which varies with polymer chain mobility and confinement within the nanocomposite matrix. For example, Vu et al. discussed the CNC polymer composites, where distinct fluorescence lifetimes corresponded to regions of differing polymer chain dynamics, reflecting variations in local polymer mobility and interfacial interactions. This allowed differentiation of PNCs based on how the polymer chains interact with nanofillers and the degree of confinement.
[119]4.2.3 Raman Imaging & Tip-Enhanced Raman Spectroscopy (TERS)
Raman imaging is a non-destructive surface technique that offers spatially resolved chemical composition analysis, while TERS enhances Raman signal detection at the nanoscale using a localized electromagnetic enhancement at the apex of a sharp metallic tip. TERS achieves spatial resolution down to approximately 10-30 nm, which is about an order of magnitude superior to the diffraction-limited resolution (~200-300 nm) of normal Raman microscopy.
[121]-[123] The tip is scanned across the sample surface in a raster pattern, generating Raman maps with nanoscale chemical contrast that reveal local composition, molecular orientation, and nanoscale heterogeneities in PNCs. This technique provides crucial insights into polymer-filler interactions, molecular orientation, and stress-induced structural modifications in PNCs.
[124]-[130]4.2.4 Positron Annihilation Lifetime Spectroscopy (PALS)
A positron is the antiparticle of an electron, possessing the same mass but carrying a positive charge. In materials science, positrons can be used as probes to study atomic-scale defects and free volume, which refers to unoccupied spaces between polymer chains or at interfaces within nanocomposites. These free volume regions play a crucial role in determining the mechanical, thermal, and transport properties of PNCs. PALS is a unique technique for probing free volume characteristics in PNCs, which directly influence mechanical strength, gas permeability, and thermal stability. By analyzing positron lifetimes, this method provides insights into polymer chain mobility and nanofiller-induced structural modifications.
[131], [132]4.2.5 Gas Chromatography
Gas chromatography (GC) is used in studies to identify the fundamental elements responsible for the inherent characteristics of carbon, cellulose, and their PNCs. The properties of the PNCs can easily be adjudged by identifying these elements. A blend is separated into its additives using GC, which are analyzed by one of the detectors.
[133], [134] By leveraging these advanced characterization tools, researchers can achieve a more profound understanding of the structural and functional aspects of PNCs, ultimately enabling the precise design of next-generation materials with tailored performance characteristics.
To further enhance the performance of PNCs, surface functionalization of nanofillers is often employed. Modifying the surface chemistry of nanofillers improves their compatibility with the polymer matrix, enhances dispersion, and tailors the composite’s mechanical, electrical, and thermal properties. Advanced fabrication strategies, including layer-by-layer assembly, 3D printing, and self-assembly techniques, are also being explored to develop next-generation PNCs with superior functionalities. To summarize,
Table 3 displays a comparison of several techniques used for PNC characterization.
5. Emerging PNC Applications
5.1 Energy Sectors
PNCs have emerged as a game-changing class of materials, revolutionizing next-generation energy technologies with their exceptional electrical, mechanical, and thermal properties. By integrating nanoscale reinforcements into polymer matrices, these advanced materials offer unprecedented improvements in conductivity, stability, and energy storage efficiency, making them highly promising for cutting-edge energy applications.
[135] Their versatility and tunability position them as key enablers in the development of high-performance solar cells,
[136] Lithium-ion batteries (LIBs),
[137], [138] fuel cells,
[135] and supercapacitors.
[139], [140] This review explores the latest advancements in PNC-based energy systems, highlighting their role in enhancing device efficiency, durability, and sustainability for future energy solutions.
In the early development towards fuel cell applications, a pioneering work by Brutti et al. outlines the utilization of PNCs comprising sulfonated polymers with inorganic compounds of metal oxides and solid proton conductors, such as the composition of SnO
2-Nafion nanocomposite.
[141] This study revealed that by incorporating nanosized SnO
2 particles with acidic properties into Nafion polymer membranes successfully enhanced proton conductivity and its energy harvester performance under low relative humidity conditions. Another early work on SPEEK/SWCNT/fly ash nanocomposites exhibited a proton conductivity of 0.027 S cm⁻¹ for fuel cell membranes.
[142] These early efforts laid the groundwork for optimizing nanocomposite membranes to address the anticipated challenges, to name a few: Fuel crossover, humidity dependence, and thermal stability in fuel cell device architecture. Several earlier reviews have mentioned that PNCs serve as a versatile active material in these emerging fields.
[143]-[149]In term of accelerated aging tests in assessing PNC performance, a real-world degradation simulation commonly carried out by subjecting the composites to extreme conditions: Elevated temperatures, humidity, and UV radiation. By analyzing the changes in their mechanical, thermal, and electrical properties, one could unravel the potential of PNCs towards real-time aging, long-term response and shelf-life and device performance. The remarkable role of dielectric properties of PNCs in the advancement electronic and high-power systems requires an appreciable input on their stability profile under operational conditions. Xinhui Li et al.
[150] outline the implication of high-temperature capacitive energy storage in PNCs can be achieved via laminated polyetherimide (PEI) polymer under nanoconfinement. With an improved thermal-mechanical-electrical stability in such constriction, the unchanged discharged energy density and its efficiency remains stable up to 100 thermal cycles between 25 to 200°C and unaffected by the relative humidity variation. In the work of Fengwan Zhao et al.
[151] PNC containing P(VDF-HFP)-based triple-layer film displays ultra-low fraction (
< 1.0 wt.%) of nanofillers, the nanocomposites demonstrate excellent stability in energy storage performance after 10,000 bending fatigue cycles. Third case related to the composite with a sandwhich structure of PVDF&PMMA)-HfO
2/PEI-BNNS, exhibiting its high thermal stability in a wide temperature range (25 to 150°C) with minor fluctuations of energy density and efficiency (~1%).
[152]5.1.1 Fuel Cells
Berber et al. utilized the conductive polymer of polybenzimidazole and Nafion to be incorporated as a catalyst in carbon black (CB), schematically shown in
Fig. 6a, with the typical power density of 130-170 mW/cm
2 under different humidity levels.
[153] The corresponding chemical structure of the polymers is depicted in
Fig. 6b. Low-dimensional materials such as MWCNTs are wrapped by distinct polymers could be applicable in high-temperature proton exchange membrane fuel cells (PEMFCs) applications.
[154] The general mechanism shown in
Fig. 6c shows that the synergistic effect can be realized between the polymer, platinum (Pt) surfaces, and the targeted polymer. Here, the incorporated polymer (polybenzimidazole, Nafion, polytetrafluoroethylene (PTFE)) is expected to minimize Pt catalyst agglomeration and undesired Pt detachment from the supporting material due to physical force. Hence, this facilitates the proton transfer in the membrane electrode assemblies (MEAs) system during the electrochemical reactions. In addition, the implementation of regulating the supramolecular interactions and topological structures is quite popular within the timeframe of the study. For example,
Fig. 6d nanostructured polymer composite membranes with multiplex proton transport channels of sulfonated poly(ether-ether-ketone) (SPEEK), poly(ether-ether-ketone)-grafted-poly(vinyl-pyrrolidone) (PGP) and polyoxometalate H
3PW
12O
40 (PW) is reported by Wang et al.
[155]In terms of low-temperature applications, Hu et al. successfully formed multilayered microstructures of poly(vinyl alcohol) and chitosan which was combined with the electrospun SPEEK nanofibers to produce proton conductivities of (0.951 ± 0.138) × 10
-2 S/cm at −30 °C and (7.32 ± 0.37) × 10
-2 S/cm at 160 °C with a long-term stability test.
[156] The molecular weight regulation of polymer is harnessed to achieve FC high efficiency and good proton conductivity, as outlined by Berber and Nakashima.
[157] A recent ternary composite is introduced containing a sulfonated poly(ether ether ketone) (SPEEK) membrane with phosphotungstic acid-ionic liquid (HPW-IL) and mesoporous graphite phase carbon nitride (mpg-C
3N
4) with antifreeze capability with a wide proton conductivity range from −40°C (7.2 × 10
-4 S cm
-1, ambient humidity) to 85°C (2.2 × 10
-1 S cm
-1, 95% RH).
[158] Further development on high-temperature polybenzimidazole-based polymer electrolyte membrane fuel cells can be found in the work of Harilal et al.
[159] and existing review.
[160] The effort of Fan et al.
[161] introducing the functionalization of GO NSs with 5-amino-1H-tetrazole (5-AT@GO) prepared by amination reaction led to promising proton conductivity (163.21 mS cm
-1 at 80°C), making it possible to reach a 65-h durability test.
Recent contribution by Zhang et al.
[162] reported that the formation of multi-hydrogen bond networks could facilitate proton conduction enhancement via imidazole moieties, as schematically shown in
Fig. 6e. Furthermore, to fairly evaluate the protonation, the under-study membrane was compared before and after the process at 80°C as outlined in
Fig. 6f. Since the conductivity possesses a linear response as a function of temperature, then
Fig. 6g implies the proton conductivity of PEMs is increasingly driven by the enhanced diffusion and thermal mobility of protons across the networks. To accommodate a higher proton conduction efficiency in high-temperature proton exchange membranes (HT-PEMs), several works
[159], [163]-[165] indicate this is related to the rational design. Sterical hindrance across the blending polyimidazolium (P-Im) and dihydrogen phosphate can be used to enhance proton conductivity that could reach 0.149 S cm
−1 at 200°C.
[163] The incorporation of synthetic and natural polymer-based materials into well-defined nanocomposites towards direct alcohol-oriented fuel cells has emerged extensively over the past years.
[148], [166]-[177] To name a few, recent breakthroughs in particular chitosan/graphene-based PNCs have inspired high-performance proton conductivity of the membrane. Gorgieva et al.
[166] proposed chitosan/N-doped reduced graphene oxide (rGO) composites with a 68% increase in power density (3.7mW/cm
2) compared to pristine chitosan membranes (2.2 mW/cm
2) in direct ethanol fuel cells. Such improvement originates from a synergistic effect triggered by N-doped rGO which enhances ionic conductivity via π-π interactions and hydrogen bonding with chitosan.
5.1.2 Solar Cells
Energy is the most fundamental and universal metric governing all natural and human-driven activities. In the face of rapid population growth and accelerating industrialization, the global energy demand has surged to unprecedented levels, placing immense pressure on conventional energy resources.
[178] As a result, the transition to renewable energy systems has become imperative, offering a more efficient and sustainable solution by harnessing naturally occurring energy flows such as wind, water, geothermal, solar, and biomass. Among these, solar energy stands out as an inevitable, clean, and sustainable alternative with immense potential to replace fossil fuels in an environmentally friendly manner.
[179]-[183] By leveraging photovoltaic systems, solar energy can be effectively harvested and converted into electricity, paving the way for a greener and more resilient energy future.
[184]-[186]Michael Grätzel and B.O. Regan are widely recognized as the pioneers of dye-sensitized solar cells (DSSCs), achieving an initial efficiency of 7.1%. Their groundbreaking work introduced a cost-effective and versatile material, marking a significant milestone in photovoltaic technology. This innovation opened new avenues for extensive research on DSSCs, driven by their unique advantages in cost efficiency, environmental friendliness, and ease of fabrication. However, challenges remain in commercializing DSSCs, including replacing noble metal Pt with more affordable alternatives and developing solid-state electrolytes to enhance cell stability.
[187]Initially, DSSCs were composed of TiO
2, N
3 dye, and a Pt counter electrode. As a counter electrode, Pt exhibits exceptional qualities, including strong catalytic activity, high stability, and excellent electrical conductivity.
[188], [189] However, the high cost of Pt and the instability of the electrolyte medium have driven the development of alternative materials with comparable properties. Carbon allotropes and conductive polymer composites have emerged as promising substitutes for Pt. The integration of carbon allotropes compatible with conductive polymers enhances the catalytic characteristics of conjugated/conductive polymers.
[136], [190] Ahmad et al. employed polythiopene (Pth) and MWCNTs nanocomposites as counter electrodes to accelerate the reduction reaction in DSSCs. The MWCNTs/Pth nanocomposites (
Fig. 7a) were synthesized via in-situ polymerization, and the newly developed electrocatalyst was deposited onto a conductive glass substrate. Notably, the performance of MWCNTs/PTh-based DSSCs outperformed Pt-based solar cells, particularly at an optimal composition of 30% MWCNTs/PTh.
[191]TiO
2 is widely used as a photoanode in DSSCs due to its high surface area, good power conversion efficiency (PCE), and low cost. However, TiO
2 NPs suffer from random electron transport caused by grain boundaries and surface traps.
[192]-[195] With a wide band gap of 3.2 eV, TiO
2 only absorbs UV light (< 387 nm), limiting solar harvesting and increasing charge recombination losses. To enhance its performance, various modifications have been explored, including nanocomposite passivation, core-shell structures, and metal ion doping.
[196]-[200] TiO
2/CdS nanocomposites stand out for their broad visible-UV light response and improved photocatalytic stability.
[201]-[203] CdS improves charge separation due to its more negative conduction band, enabling photoexcited electrons to transfer from CdS to TiO
2 while holes remain in CdS—suppressing recombination.
[204], [205] In a study by Ullah et al., a TiO
2/CdS nanocomposite photoanode doped with Ba, Ho, and Cd was synthesized via sol-gel and hydrothermal methods. Doping induced a red shift in the TiO
2 band gap, enabling visible light absorption and enhancing free electron generation. CdS also acted as a passivation layer, promoting efficient electron transport. This system reduced the TiO
2 band gap from 3.10 eV to 2.16 eV in the case of 3% holmium doping of TiO
2 coupled with CdS
(Fig. 7b). The Cd-doped TiO
2/CdS, sensitized with Pyrocatechol Violet dye, achieved a PCE of 2.68%, with V
oc of 0.41 V and J
sc of 16.97 mA/cm
2, outperforming the undoped version (0.82%).
[206] Interestingly, the same strategies that improve charge separation and electron transport in TiO
2/CdS photoanodes for solar energy harvesting are also central to environmental photocatalysis. As further discussed in Section 4.3, embedding TiO
2 nanocomposites in functional membranes applies these principles to pollutant degradation, demonstrating how energy-related innovations can be translated into environmental remediation.
[207]-[212]Sadegh et al. introduced an eco-friendly synthesis method to fabricate superparamagnetic Fe
3O
4@PANI nanocomposites with a well-defined core-shell architecture, as shown in
Fig. 7c. This innovative material was specifically designed to enhance triplet state population and overall solar cell efficiency. Fe
3O
4, known for its superparamagnetic behavior, facilitates charge transfer through an intrinsic magnetic field effect. In the context of solar cells, this property significantly aids in electron-hole pair separation while minimizing recombination, thereby improving charge collection efficiency.
Fig. 7d describes the working principle of solar cells, which begins with light exposure to a p-n junction. This exposure generates electron-hole pairs that are separated by a potential barrier, resulting in a voltage that drives current through an external circuit. In organic semiconductors, these photoexcited electron-hole pairs, known as excitons, exist in either singlet or triplet spin states. Spin states play a key role in solar cell performance, and improving efficiency requires prolonging the lifetime of excitons.
[213] PANI, a widely studied conductive polymer, contributes high charge mobility and strong absorption in the visible light spectrum. It also enables efficient electron transport, complementing the role of Fe
3O
4 in accelerating charge movement toward the electrode.
[217], [218] The core-shell configuration of Fe
3O
4@PANI creates an active interfacial region that supports triplet state transitions. These triplet states possess longer lifetimes than singlet states, allowing for more stable and efficient charge transfer before recombination occurs. The resulting Fe
3O
4@PANI nanocomposite exhibited strong superparamagnetic properties with a saturation magnetization of 44.09 emu/g and a distinct core-shell structure. When applied in polymer solar cells (PSCs), the system achieved a maximum PCE of 1.53%, with an open-circuit voltage (V
oc) of 0.4 V, short-circuit current density (J
sc) of 4.24 mA/cm
2, and a fill factor of 0.47 under AM 1.5 G illumination at 60 mW/cm
2. This nanocomposite effectively enhances photogeneration and charge transport within PSCs, which are key factors in boosting solar cell performance. Furthermore, the active layer synthesis and device fabrication were carried out via solvent-free, solid-state in-situ polymerization, a green, simple, cost-effective, and high-yield approach. Overall, the Fe
3O
4@PANI nanocomposite demonstrates significant promise as a next-generation material for scalable, solid-state polymer solar cell technologies.
[214]Compared to the traditional silicon-based solar cells, low PCE of PNC-based solar cells is mainly originate from structural degradation, high bandgap, poor thermal management, and inefficient charge transport. To provide a stable PNCs with suitable band alignment and doping remains difficult objective, limiting achievable performance compared to conventional silicon-based solar cells. In particular, the fundamental challenge driven by their intrinsic nature of polymer-nanofillers composition causing less efficient exciton dissociation, charge transfer, and poor charge carrier mobility, alongside challenges in morphology control and light absorption.
[219]-[221]5.1.3 Lithium-ion Batteries (LIBs)
LIBs have emerged as a revolutionary class of energy storage systems founded on lithium metal chemistry.
[222], [223] Renowned for their high energy density, long cycle life, high average output voltage, and environmental friendliness, LIBs have become indispensable for a wide range of modern applications-ranging from handheld electronics and electric vehicles to large-scale energy storage systems.
[137], [138], [224], [225] A typical LIB consists of an anode (negative electrode), a cathode (positive electrode), a non-aqueous electrolyte, and a separator. Among these, the electrolyte plays a pivotal role in determining the battery’s capacity, operational temperature range, and cycling stability by facilitating efficient ion transport while ensuring safety. The separator, placed between the electrodes, enables effective charge transfer while preventing short circuits.
[226], [227]Recently, high entropy oxides (HEOs) such as (CrMnCoNiZn)
3O
4 have garnered significant interest as potential anode materials for LIBs due to their exceptionally high theoretical capacity.
[228] However, their practical application is hindered by intrinsic limitations such as low electrical conductivity and considerable volume changes during charge-discharge cycles. To address these challenges,
[229]-[231] Jin et al. synthesized spinel-structured (CrMnCoNiZn)
3O
4 NPs via the solution combustion method and further developed a core-shell (CrMnCoNiZn)
3O
4@PPy nanocomposite through in-situ polymerization.
Fig. 7e illustrates the distinct core-shell morphology of the nanocomposite, with PPy shells approximately 15 nm thick. The Fig. indicates that PPy nucleated heterogeneously on the HEO substrate (PPyB), while some PPy particles aggregated separately and did not adhere to the HEO surface (PPyA and PPyC). The resulting nanocomposite delivered an impressive specific capacity of 802 mAh/g at 100 mA/g after 100 cycles. Additionally, it demonstrated excellent cycling stability with a capacity of 416 mAh/g at 1 A/g after 1000 cycles and superior rate performance, achieving 360 mAh/g at 2 A/g. These outstanding electrochemical performances highlight the potential of (CrMnCoNiZn)
3O
4@PPy nanocomposites as advanced anode materials. The conductive and flexible nature of PPy effectively accommodates volume expansion, enhances electrical conductivity, and suppresses unwanted side reactions, contributing to the overall stability of the system.
[215] In parallel, Silicone (Si) has attracted intense research interest as a next-generation anode material due to its extraordinarily high theoretical specific capacity of 3579 mAh/g.
[232] One promising approach involves the development of SiO
2/C nanocomposite-based anodes, supported by carbon films derived from rGO, synthesized via a mixed polymerization strategy (see
Fig. 7f). This design aims to enhance both energy storage capacity and cycling stability, leveraging cycle-dependent size reduction effects. As particles become smaller with each cycle, improved electrode contact and charge transfer efficiency are achieved, leading to better electrochemical performance.
[233]-[239] The porous architecture and conductive support structure further contribute to high-capacity retention and robust cycling behavior, as confirmed through charge/discharge and electrochemical impedance spectroscopy measurements. Overall, the GO-based SiO
2/C nanocomposite film emerges as a highly promising candidate for next-generation energy storage devices, offering a pathway to high-performance, durable lithium-ion batteries.
[216] Recent work on PI/MXene nanofiber composite displays a good combination of high thermal stability of PI with the superior electrolyte wettability of MXene resulted high tensile strength of 19.6 MPa, low bulk resistance (2.5 Ω), and low interfacial resistance (174 Ω). This in turn a discharge specific capacity of 126.7 mAh g
−1 and a capacity retention rate of 91%.
[240] An investigation on the ionic liquid (IL) grafted onto the surface of MXene is successfully enhance the electrochemical performance of PEO-based solid composite polymer electrolyte with high ionic conductivity (7.19 × 10
−4 S cm
−1) and exceptional capacity of 154.8 mAh g
−1 over 120 cycles with an impressive 95.3 % capacity retention at 0.5 C.
[241]5.1.4 Supercapacitors
Supercapacitors, also known as ultracapacitors or electrochemical capacitors, are energy storage devices that have a higher energy storage capacity compared to conventional capacitors.
[7], [139], [140], [242]-[245]. These devices offer high power density, fast charge and discharge capabilities, and long cycle life, making them essential components for applications that require rapid bursts of energy, such as electric vehicles, renewable energy systems, and portable electronics.
[246]-[248] The study by Chakraborty et al. explores the use of styrene maleic anhydride (SMA) polymer modified with thiadiazole groups and reinforced with approximately 20 nm flake-structured ZnO NPs. The electrochemical performance of the nanocomposite demonstrates a remarkable specific capacitance of 268.5 F/g at a current of 0.1 A/g, surpassing that of pure ZnO NPs and unmodified SMA polymer. Furthermore, the nanocomposite exhibits excellent cyclic stability with maximum capacity retention, indicating an enhancement in the intrinsic conductivity of the modified SMA polymer. These promising results highlight the significant potential of SMA-ZnO nanocomposites as eco-friendly and efficient electrode materials for supercapacitors in future energy storage applications.
[249]The highest energy density reported for PNC in supercapacitor applications is 561 Wh/kg and 86% capacitance retention after 5,000 cycles, achieved by a PANI/rGO/ZnO nanocomposite in a symmetric tandem supercapacitor configuration.
[250] In regards of their cyclic electrochemical stability, PANI composite with 2% composition displays an appreciable 96.67% capacitance retention. In addition, two respective cases by Boro et al.
[251] and Goodwin Jr. et al.
[252] on the aspect of active nanofiller ZnO dissolutions in PNC are discussed. Boro and coworkers suggest the presence of ZnO nanoparticles in polymer matrices could catalyze chain scission of the polymer matrix, leading to lower molecular weight polymer fragments. This chain scission causes a lowering of both glass transition and melting temperatures, indicating degradation. Based on their Thermal analysis, the incorporation of ZnO decreased the maximum degradation temperature of PLA from 363.1 °C to about 296.8°C for the highest ZnO loading, indicating catalyzed degradation. Moreover, this study specifically covered PLA/ZnO PNC where ZnO nanoflowers formed hydrogen bonds with the PLA matrix, enhancing nucleation rate but also initiating polymer degradation through chain scission. This presents a mechanism of degradation related to ZnO dissolution and such interaction causing polymer matrix breakdown and cycle stability challenges. Another article by Goodwin Jr. et al.
[252] outlines the epoxy PNC with ZnO nanofillers accelerated the photodegradation under UV light exposure. This in turns leads to polymer chain scission and formation of carbonyl groups. Such undesired degradation contributed to the loss of mechanical integrity and thereby nanofiller release.
Recent reports indicated that the highest specific capacitance reported for PNC in supercapacitor applications is 1136.4 F/g, achieved in PANI/GO composite synthesized via electro-polymerization.
[253] Another two examples utilized a self-dispersion method to integrate MWCNTs with PANI, resulting in a composite with 1017 F/g
[242] and PANI/GO/h-BN ternary nanocomposite (946 F/g).
[254] PVDF-HFP/LiBOB electrical-ionic hybrid nanocomposite produced specific energy of 30 Wh/kg and volumetric energy density of 6.64 mWh/cm
3, inferring a good promise in flexible solvent-free supercapacitors.
[255] In the case of PEDOT-based, Z. H. Wang
et al. outlines the high areal capacitance (251.4 mF/cm
2), volumetric capacitance (723.8 F/cm
3) and long cycling life (a capacity retention of 107 % after 10,000 cycles) are attainable. Recent breakthroughs in the utilization of 2D materials beyond graphene, such as MXenes
[256]-[262] or rare-earth oxides
[263], [264] are promising to enhance the energy storage capacity of PNCs as a supercapacitor. Recent work by Shaobo Tu et al. on the molten salt etched MXene incorporated into a poly(vinylidene fluoride-trifluoroethylene-chlorofluoroethylene) (P(VDF-TrFE-CFE))/PMMA hybrid matrix induces strong interfacial interactions.
[265]5.2 In situ hydrogel nanocomposites in upstream oil and gas sector
In the upstream oil and gas industry, PG has been used as a blocking or shutoff agent to prevent unwanted production of fluid, which can incur extra cost for treatment.
[266], [267] Recently, researchers have focused on improving the conventional PG by incorporating nanomaterials in the gels’ composition, hence PNCs. Many authors have reported success in developing different nanocomposite systems from different base gel systems and nanomaterials.
[268] This section focuses on the effect of nanomaterials addition in the conventional gel on gelation time, rheology/gel strength, swelling, and plugging ability.
5.2.1 Effect of Nanomaterials on Gelation Time of PNCs Gels
One of the most important parameters during the application of PG in the subsurface is gelation time. The gelation time determines when the gel, which is originally liquid, becomes more rigid and successfully blocks a channel. Different studies showed how nanomaterials affect the gelation time differently. Several studies reported that nanomaterials can shorten gelation time. For example, Liu et al.
[269] reported faster gelation in PAM/Hydroquinone(HQ)-Hexamethylenetetramine(HMTA) gels with increasing SiO
2 NPs concentration. Their result is depicted in
Fig. 8a where they determined the inflection point of the viscosity measurement as gelation time. The NPs, they argued, are doped in polymer coils and form microscopic arrangements that improve the viscosity and, hence, faster gelation. Liu et al
[270] reported shorter gelation time with increasing concentration of TiO
2 and SiO
2 in hydrolysed polyacrilamide (HPAM)/ polyethyleneimine (PEI) gels through Sydansk’s
[271] inverted bottle test method, as shown in
Fig. 8b. Ilavya et al.
[272] also reported acceleration in partially hydrolyzed polyacrilamide (PHPA) /HQ-HMTA gels with the addition of GO NPs, which bridged polymer chains, increasing crosslinking efficiency. Similarly, Reena et al.
[273] reported shorter gelation time when ZnO NPs were introduced to polyvinylpyrrolidone (PVP)/resorcinol-formaldehyde (RF) based hydrogel and attributed this to the crosslinking effect of the NPs. Pérez-Robles et al.
[274] tested Al
2O
3, MgO, SiO
2, and Cr
2O
3 in PAM/RF gels and reported that Al
2O
3, MgO, and Cr
2O
3 NPs reduced the gelation time, with Al
2O
3 showing the fastest gelation due to NPs interaction with polymer chains. However, in a subsequent study, Pérez-Robles et al.
[275] tested similar NPs in different gel systems of acrylamide sodium acrylate copolymer/chromium (III) and reported that only Al
2O
3 and MgO shorten gelation time. This shows that the base gel system also plays an important role in determining the effectiveness of NP addition.
Conversely, there are authors who reported longer gelation when nanomaterials were introduced to gel systems. Moghadam et al.
54 and Aalaie et al.
[276] reported longer gelation time in sulfonated PAM/Cr(III) acetate gels with sodium montmorillonite (Na-MMT) nanoclay, as the nanoclay particles blocked crosslinker access to polymer chains. Pérez-Robles et al.
[274] reported that SiO
2 NPs increased gelation time compared to other metal oxides, possibly due to weaker interactions with the polymer. In another study with a different gel system, Pérez-Robles et al.
[275] also reported that Cr
2O
3 NPs delayed gelation along with SiO
2 in some cases. Ma et al.
[277] added SiO
2 NPs to HPAM/PEI gel system and observed more than two times longer gelation than the conventional gel. On the other hand, Shehbaz & Bera et al.
[278] incorporated Al
2O
3 and SiO
2 NPs in PHPA/hexamine/HQ gels and observed that gelation time remains constant with the increase in NPs. Similarly, Yudhowijoyo et al.
[279] also tested Al
2O
3 and SiO
2 addition into Xanthan gum/chromium (III) gel system and reported that there was no significant change in the gelation time even at different nanomaterials concentration.
5.2.2 Effect of Nanomaterials on PG Strength and Rheology
The addition of nanomaterials to a PG system is mainly intended to improve the mechanical strength of the gel. One of the methods of quantifying gel strength is through the measurement of rheological properties, especially the storage modulus (G’), which indicates the gel’s elasticity.
[283], [284] Many authors have performed an investigation of nanocomposites through such method. The improved crosslinking density by incorporating nanomaterials is shown by Tongwa et al.
[285] and Okay and Opperman
[286] who tested Laponite XLG and RDS clay nanomaterials, respectively, and improved the G’ of the nanocomposite. Moreover, the PNC can be formed even in the absence of a conventional crosslinker as they showed a transition from liquid-like to solid-like viscoelastic behavior with increasing nanomaterials concentration. The crosslinking capability of the nanomaterials contributes to the increased gel strength. Similarly, Xu et al.
[287] also reported increased G’ when montmorillonite nanomaterials were added. This was governed by the interaction between nanomaterials and polymer chains, facilitating the reinforced gel networks. Aguiar et al.
[288] and Pereira et al.
[289] who worked with bentonite also reported increased gel strength.
Sun et al.
[280], [290] conducted rheological study on HPAM/Chromium(III) gel systems with the addition of SiO
2 NPs. It is shown that the elastic modulus G’ of the nanocomposite increases with increasing concentration of the NPs. According to environmental SEM (ESEM) (shown in
Fig. 8c), the NPs adsorbed on the gel’s networks, reduced the spacing between network chains, and filled the pores of the gel. This strengthened the micro network structure of the gel, and in turn, improved the macro strength of the gel.
Pérez-Robles et al.
[274] studied the effect of different NPs (SiO
2, Al
2O
3, MgO, and Cr
2O
3) in PAM/RF gels, and they reported increasing G’ with increasing NPs concentration, with Al
2O
3 showing the highest improvement. In their next publication
[275] they tested the same NPs in acrylamide sodium acrylate copolymer/chromium (III) and reported that SiO
2 addition results in the highest G’ at 8000 mg/L polymer, followed by Al
2O
3, MgO, and Cr
2O
3, respectively. At 4000 mg/L polymer, the order was different. SiO
2 addition caused the highest G’ followed by MgO, Al
2O
3, and Cr
2O
3, respectively. The graphical comparison between the two polymer concentrations is shown in Fig.
8d. When the amount of NPs was halved, weaker gels were formed, and the order became different once again. This time, Cr
2O
3 showed to cause the highest G’ followed by MgO, Al
2O
3, and SiO
2, respectively. This behavior implies that NPs can be considered as nucleation points that also act as crosslinkers. It is interesting to note that Yang et al.
[291] observed that silica NPs improve the viscoelasticity of HPAM only above a critical polymer concentration of 0.8 wt%, where NPs bridged polymer chains effectively. Below this threshold, the NPs were not able to bridge the polymer network and weaken the gel structure. Moreover, at higher silica concentration, the NPs would aggregate and disrupt crosslinking. These reports suggest that polymer chemistry dictates nanomaterials efficacy.
Other factors also influence the rheological behavior of the gel. Dijvejin et al.
[292] tested different sizes of SiO
2 NPs on SPAM/chromium gels. It turns out 20-30 nm NPs showed the highest G’ in comparison with 7-10 nm and 60-70 nm NPs. They argued that decreasing the NPs size would enhance the interaction between the increased NPs surface with the polymer. Decreasing the size further, however, would cause a higher aggregation level in the nanocomposite. Pereira et al.
[293] studied the effect of ZnO and Al
2O
3 NPs in HPAM/PEI gels. While they reported increased gel strength in both cases, the smaller ZnO NPs increased G’ better than Al
2O
3. They argued that larger Al
2O
3 NPs have a greater tendency to agglomerate. Reena et al.
[273] who introduced ZnO NPs to PVP/resorcinol-formaldehyde gels discovered that there is a threshold concentration of 0.8 wt%. Beyond this point, G’ would diminish due to the aggregation of NPs.
In contrast, few reports of decreasing G’ with the addition of nanomaterials led to different outcomes. Aalaie and Rahmatpour
[294] observed decreasing G' with increasing Na-MMT nanoclay concentration in HPAM/chromium(III) acetate. Some of the polymer chains would adsorb on the nanoclay, and there is interaction between the positive chromium ion and the negative layers of the nanoclay. In another publication, Aalaie et al.
[276] further increased the concentration of the nanoclay and discovered that beyond 1000 ppm, they became effective junction points and increased G’. Liu et al.
[270] reported increased G’ with increasing concentration of TiO
2 and SiO
2 only until 0.02%. Beyond this point, they reported a small reduction in G’ due to insufficient crosslinking between polymer and NPs. Contrary to this, Yudhowijoyo et al.
279 reported an initial reduction in G’ at 1000 ppm SiO
2 and Al
2O
3 NPs, followed by an increase in G’ at higher concentrations. Hence, to achieve the desired result, there should be an optimum combination between different components of the nanocomposite. Different nanomaterials should be carefully tested with different gel systems prior to utilization in subsurface conditions.
5.2.3 Effect of Nanomaterials Swelling Behavior of PNCs Gels
A number of publications have studied the effect of nanomaterials addition in PG on the swelling behavior of the gel. Almost all worked with clay-based nanomaterials, and the majority of them reported a decreased degree of swelling (DS) with nanomaterials. Mohammadi et al.
[295] and Aalaie et al.
[276] investigated the effect of Na-MMT clay nanomaterials on the swelling behavior of sulfonated PAM/chromium gel systems and reported decreasing DS. In another study, Aalaie and Rahmatpour
[294] changed the polymer to HPAM and reported a similar trend. Investigation on laponite nanoclays by Aalaie and Youssefi
[296] also showed decreasing DS with increased nanomaterials. This finding was also supported by the work of Ren et al.
[281] who used Laponite XLG nanoclays on a different gel system and reported a similar trend.
According to some authors
[294]-[296], the introduced nanomaterials contributed to the nonuniform distribution of electric potential within the gel system. This is because the counterions are ionically trapped by the anionic surface charge of the clay nanomaterials, making them osmotically passive and unable contribute to swelling.
[297] Asadizadeh et al.
[298] investigated the effect of increasing SiO
2 NPs concentration in HPAM gels and also reported a decreasing trend. They observe this trend in both seawater and formation water. They also attributed their finding to the same mechanism of ionic trapping by the nanomaterials. In addition to this, Mohammadi et al.
[295] suggested that the nanomaterials also act as a crosslinker, which contributed negatively to the total osmotic pressure.
Ren et al.
[281] reported swelling-deswelling behavior of the nanocomposite with laponite XLG concentration. As seen in
Fig. 8e, such behavior was not observed at the lower amount of clay. However, the nanocomposite exhibits swelling followed by deswelling at later times at higher amounts. When the samples eventually equilibrate, they reported decreasing DS with increasing nanomaterial concentration. In another study with laponite as a crosslinker, Abdurrahmanoglu et al.
[299] tested three different polymers and observed decreasing DS in PNIPA and PDMA nanocomposites but different behavior in PAM systems, where DS initially increased before decreasing at higher laponite concentrations. This is because the clay interacts strongly with PNIPA and PDMA, creating a more effective crosslinking density compared to PAM. Once again, this highlights the importance of the interaction between each component making up the gel/nanocomposite systems.
Further reduction of DS can be done by altering the hydrophilicity of the nanofillers. Lee and Fu
[300] worked with organic montmorillonite that is intercalated with methyl, tallow, and bis-2-hydroxyethyl quaternary ammonium salt (MT2EtOH) in the gel system of NIPA/MBA and reported a reduction in DS. This is because the originally hydrophilic MMt has become hydrophobic, and increasing the number of hydrophobic nanomaterials would expel water from the gel and cause shrinkage.
5.2.4 Effect of Nanomaterials on Plugging Ability of PNCs Gels
Singh and Mahto
[301] reported that adding Na-MMT nanoclay to PAM/chromium (III) acetate gels improved their permeability reduction in sandpack tests compared to conventional versions. In a subsequent work, Singh and Mahto
53 changed the polymer to PAM graft starch while keeping the other components the same and performed the investigation in sandpack media. This work also shows the superiority of nanocomposite gels over conventional gels in reducing the permeability of the porous media. It is suggested that increasing gel strength would improve the permeability reduction impacted by the gels. Similarly, Chen et al.
[302] also reported better plugging performance with the addition of nanosilica due to improved stability and absorption to the rock surface. In another study, Singh et al.
[303] also, notice improved plugging capability when fly ash NPs were used. Reena et al.
[273] also reported improved percentage permeability reduction (PPR) and residual resistance factor (RRF) after ZnO NPs addition, as shown in
Fig. 8f. Improvement in both PPR and RRF is an indicator of good plugging of the nanocomposite.
Almoshin et al.
[304] introduced graphene-based zirconium oxide NSs (Zr
2O/rGO) as both crosslinker and filler to low molecular weight PAM and reported increased pressure resistance when tested in Berea sandstone cores. They noticed the nanocomposite’s endurance against 2000 psi water. Similarly, Yang et al.
[282] reported that SiO
2 NPs enhanced the rupture resistance of PAM /chromium gels, allowing them to withstand higher mechanical stresses during fluid injection. Moreover, as presented in
Fig. 8g, with 2% nano silica nanocomposite, they noticed that in the presence of pressure, water would permeate gradually through the gels instead of causing rupture at lower pressure for the conventional gel. According to Ilavya et al.
[272] who worked with nano graphene oxide, the addition of the nanomaterials improved the plugging ability of conventional gels by enhancing the gels' adhesion to pore throats, which in turn formed a tight seal.
The suitability of nanocomposite gels for subsurface application was shown by Pérez-Robles et al., who reported the degradation of conventional gel against saline solution. By introducing Al
2O
3 NPs to the gel system, they reported increased resistance to saline conditions and washout. In addition to this, Mohammadi et al.
[295] who worked with Na-MMT nanomaterials noticed better performance for permeability reduction in the presence of water and oil. The nanocomposite gels successfully reduced the water permeability more than the oil permeability compared to conventional gels. Jia et al.
[305] conducted a pilot test and reported that introducing SiO
2 NPs resulted in better performance than conventional gels, as it showed better thermal stability, permeability reduction, and pressure resistance. The nanocomposite was reported to effectively seal fractures and vugular pores.
5.3 Environmental Remediation
The vast growth of industry reveals the undesired side effect, namely, the volume of wastewater is increasing substantially. Hence, PNCs are contributed to tackle various outcome ranging from chemical manufacturers to household productions. In this section we intend to derive several implications of PNC as active agent in wastewater treatment and water purification.
5.3.1 The role of PNCs in Wastewater Treatment Technology and Water Purification
PNCs have emerged as a promising and multifunctional platform for wastewater treatment technology, offering mechanisms such as catalytic degradation, adsorption, and membrane filtration to target a broad spectrum of organic pollutants effectively.
[306], [307] These composite materials enhance contaminant removal and address limitations of conventional methods through improved charge separation, suppressed recombination of charge carriers, and the promotion of synergistic interactions between the composite components.
[308], [309] The diversity of pollutants, including pharmaceuticals,
[310]-[312] heavy metal ions,
[313]-[315] dyes,
[207], [316], [317] polychlorinated biphenyls,
[318], [319] brominated flame retardant,
[320] and pesticides
[321] demands tedious effort in discriminating suitable active polymers with high removal rates and tunable selectivity.
5.3.2 Working Mechanism of PNCs in Wastewater Treatment
Among the mechanisms employed by PNCs, heterogeneous photocatalysis stands out for its remarkable efficiency in degrading persistent organic pollutants under light irradiation. As a subset of catalytic degradation, this process exemplifies how nanocomposite design can drive advanced oxidation reactions. Notably, heterogeneous photocatalysis is considered one of the most promising advanced oxidation processes (AOPs) for industrial wastewater treatment, largely because of its cost-effectiveness, eco-friendliness, minimal harmful by-products generation, and high pollutant removal efficiency. However, traditional inorganic semiconductor photocatalysts often suffer from limitations such as rapid electron-hole recombination, low surface activity, and NP agglomeration, which limit their performance.
[322], [323]Recent research has focused on engineering nanocomposite structures by integrating conductive polymers with active photocatalytic components to overcome these barriers. For instance, Kanwal et al. synthesized AgCl@PANI nanocomposite, as shown in
Fig. 9a, demonstrating how polymer-inorganic hybrids can improve photocatalytic behavior. In this system, the intercalation of AgCl into the PANI matrix not only increases the degree of protonation but also enhances the electrical conductivity of the composite.
[316]Under ultraviolet (UV) light, PANI undergoes a π-π* transition from the highest occupied molecular orbital to its lowest unoccupied molecular orbital, requiring low energy due to its superior light absorption,
[324] resulting in high photoresponsiveness. This transition promotes efficient charge transfer and separation of electron-hole pairs, while the nanostructured morphology of the composite minimizes recombination. Furthermore, AgCl enhances the formation of reactive oxygen species (ROS), such as hydroxyl radicals, critical for degrading dyes like methylene blue (MB).
[316]The photocatalytic behavior of TiO₂-based nanocomposites, already exploited in energy devices such as DSSCs (Section 4.1)
[206] can be extended beyond energy harvesting. In environmental remediation, these same properties, band gap tuning, charge separation, and electron mobility, are harnessed to design multifunctional membranes for pollutant removal. Building on this conceptual framework, further innovations have focused on integrating photocatalysis with membrane filtration towards multifunctional nanocomposite membranes. As shown in
Fig. 9b, embedding photocatalytic materials directly into membrane structures enables simultaneous pollutant filtration and degradation.
[207] While standalone photocatalysts are effective, their performance often declines at high concentrations due to the aggregation of NPs and limited active sites. Additionally, recovering dispersed catalysts from treated water is technically challenging and costly.
[325] Nanocomposite membranes address these issues by uniformly dispersing and stabilizing the photocatalyst within a polymer matrix, maintaining permeability, and minimizing catalyst loss.
[326] A notable example of PNC innovation is the integration of TiO
2 with GO in a nanocomposite membrane for degrading methyl orange
(MO) dye. This system combines physical filtration with photocatalytic oxidation: MO is first retained on the membrane surface, followed by UV irradiation that activates TiO
2. Upon excitation, TiO
2 generates electron-hole pairs, oxidizes water to hydroxyl radicals, and electrons reduce oxygen to form additional ROS. The presence of GO enhances electron transport, reducing charge carrier recombination and boosting photocatalytic efficiency.
[207]-[212]Expanding the multifunctionality of PNCs,
Fig. 9c illustrates a synergistic approach combining adsorption and photocatalysis to treat cationic dyes such as rhodamine B (RB) and malachite green (MG). While adsorption is simple and effective, it only transfers pollutants from liquid to solid phase, raising secondary pollution concerns. In contrast, photocatalytic AOPs offer a more sustainable solution, enabling not only decolorization but also promoting the breakdown and mineralization of dye molecules. Under near-neutral pH, a functionalized photocatalyst with hydroxyl and amine groups acquires a negative surface charge, promoting selective adsorption of positively charged dyes.
[317], [327] These concentrate pollutants at the catalyst surface, enhancing photo-induced degradation. Upon light exposure, the adsorbed dyes form radical cations, which react with oxygen to generate ROS. Advanced photocatalysts like PAM/NZP or Ni-doped zinc ZnO improve charge separation and hydroxyl radical production, accelerating the breakdown of dye structures and enabling efficient degradation.
[317]5.3.3 Towards high-efficiency of PNCs in Treating Wastewater
The efficiency of PNCs in wastewater treatment is typically assessed by two key parameters: pollutant removal percentage and material reusability over multiple cycles. These parameters are essential in evaluating the long-term practicality and sustainability of nanocomposites for environmental remediation. A study by Samadder et al. highlighted the selective dye removal performance of polymer-based adsorbents using a binary dye system: MB, a cationic dye, and MO, an anionic dye,
[328] monitored at wavelengths of approximately 665 nm and 464 nm, respectively, under neutral pH conditions.
[329], [330] A novel nanocomposite was synthesized by integrating magnetic 3D crosslinkers (M3D) with cellulosic material via
in situ polymerization. These M3D crosslinkers, formed by functionalizing Fe
3O
4 NPs with acrylic groups, enabled robust covalent bonding with PAA, enhancing the nanocomposite’s mechanical strength and stability.
[331] PAA, rich in carboxyl groups, provides a strong binding affinity toward cationic dyes,
[332] while the 3D crosslinkers offered more active sites than traditional linear or planar structures.
[333] The modification of the composite with carboxylated cellulose nanocrystals (CCN) forming the M3D-PAA-CCN nanocomposite improves dispersibility and reduces excessive stickiness.
[328] As shown in
Fig. 9d, this nanocomposite exhibited significantly higher adsorption capacity for MB compared to MO, driven by electrostatic attraction between the negatively charged surface and cationic MB molecules. This selective adsorption enhances treatment efficiency, allowing targeted removal of pollutants based on their ionic nature
[328].
Beyond initial adsorption performance, the recyclability of adsorbents plays a crucial role in determining their practical applicability.
Fig. 9e presents the results of five successive adsorption-desorption cycles conducted at pH 7. Both M3D-PAA-CCN and its counterpart, M3D-PAA, exhibited excellent recyclability. Although a modest decline in dye removal efficiency was observed, from 75% to 68% for M3D-PAA-CCN and from 50% to 37% for M3D-PAA, the materials retained substantial adsorption capacity across multiple cycles.
[328] In addition to adsorption, recent reviews have invoked a systematic foundation to increase the performance of incorporated PNC in photocatalysis. For example, Bhattacharyya et al. demonstrated a synergistic TiO
2-GO nanocomposite embedded within a membrane for MO degradation, shown in
Fig. 9f. A pristine membrane, lacking any photocatalyst, achieved only 13.3% MO degradation after 120 minutes, primarily due to physical sieving and limited electrostatic interactions.
[326], [334] In contrast, membranes containing 0.05 wt% TiO
2-GO nanocomposites (PM2) exhibited a significantly improved degradation efficiency of 68.5%, attributed to enhanced charge separation and electron transfer between TiO
2 and GO. Interestingly, when the concentration of TiO
2GO was increased to 0.1 wt% (PM3 membrane), a decline in photocatalytic performance was observed, likely due to catalyst clustering. This clustering reduces the effective number of active sites, thereby diminishing the overall photocatalytic activity. Control experiments with membranes incorporating only GO (PM-GO) or only TiO
2 (PM-TiO
2) yielded lower degradation efficiencies of 43.5% and 48%, respectively, further confirming the superior performance of the synergistic TiO
2-GO system.
[207]Fig. 9g illustrates the dual functionality of PAM/NZP composites in both adsorption and photocatalytic dye removal. This study was designed to investigate the sequential mechanism of dye removal, beginning with adsorption and followed by photocatalysis. Results showed that, during the dark adsorption phase, 29.5% of MG and 31.35% of RB were adsorbed onto the PAM/NZP composite. Upon solar light exposure, removal efficiencies increased to 55.9% for MG and 43.6% for RB. The enhanced performance is attributed to the adsorptive characteristics of the cross-linked PAM gel,
[327], [335] which provides abundant surface-active sites and a porous structure that facilitates pollutant capture. Moreover, the interconnected porous network promotes efficient mass transfer and supports light scattering within the framework, further improving photocatalytic activity.
[317] 5.3.4 Surface Properties of PNCs for Wastewater Treatment
Surface characterization is essential for evaluating PNCs in wastewater treatment as it reveals key changes in morphology, roughness, and chemical interactions upon nanomaterial incorporation. Ali et al. investigated polyamide thin-film nanocomposites (TFNs) embedded with TiO
2 NSs for fluoride removal from drinking water.
[336] Through FE-SEM
, they observed distinct surface morphology changes induced by the interfacial polymerization (IP) process.
[337], [338] Specifically, the incorporation of TiO
2 NSs resulted in a leaf-like, denser surface structure on the TFN membrane (
Fig. 10a), compared to the traditional nodular surface of the Thin Film Composite (TFC) membrane (
Fig. 10b), attributed to TiO
2 interaction with monomers during IP. This altered morphology enhances membrane compactness and performance.
[339]AFM images (
Fig. 10c-
10d) revealed lower roughness in TFN, likely due to TiO
2 disrupting nodular growth and promoting uniform surface formation, beneficial for antifouling and permeability.
[340], [341] In addition
, XPS was employed to analyze the elemental composition and chemical states present on the membrane surface. The O1s spectrum (
Fig. 10e) revealed distinct peaks around 532.4 eV and 533.8 eV
, corresponding to C=O and C-O bonds, respectively, indicating the presence of carbonyl and ether groups.
[342], [343] The C1s spectrum (
Fig. 10f) exhibited three peaks: around 284.85 eV (C-C/C=C), 286.85 eV (C-O/C=N),
[344], [345], and 287.81 eV (O=C/O=C-N),
[346] reflecting the complexity of the polyamide structure and its interactions with TiO
2 NSs.Ti 2p spectrum provided evidence for the presence of titanium species. Peaks at 447.2 eV (Ti 2p
3/2) and 458.5 eV (Ti 2p
1/2) (
Fig. 10g) confirmed successful incorporation of TiO
2 into the polyamide matrix.
[347], [348] The increase in intensity of these peaks was directly proportional to the concentration of TiO
2 NSs in the MPD monomer solution, signifying a strong correlation between TiO
2 loading and surface composition. Additionally, an increased oxygen signal in the O1s spectrum (
Fig. 10h) further verified the enrichment of oxygen-containing species due to TiO
2 integration. In addition to confirming the successful incorporation of nanofillers via XPS analysis, it is essential to evaluate the potential detachment and leaching of nanoparticles from polymer nanocomposites under operational conditions, as these processes may pose environmental risks. Nanoparticle release is strongly influenced by particle type, size, and the interactions with the surrounding polymer matrix. Wen et al. (2021) outlined four major mechanisms of polymer matrix degradation—UV radiation, temperature extremes, mechanical abrasion, and chemical erosion—which can accelerate nanoparticle release. Furthermore, Wen et al. (2019) described two principal pathways for engineered nanoparticle release: (i) direct detachment from the intact polymer matrix and (ii) release from a degraded polymer matrix.
[349] Kajau et al. (2021) investigated the leaching of CuO nanoparticles from polyethersulfone (PES) ultrafiltration membranes in different cleaning solutions (NaCl, HCl, NaOH, and NaClO). The highest leaching rate occurred in HCl solution, attributed to the susceptibility of the polymer matrix to chlorine-induced degradation.
[350] Similarly, Zodrow et al. (2009) observed approximately 10% loss of silver nanoparticles from a nanocomposite membrane after a relatively short filtration period, resulting in a notable decline in antifouling and antibacterial performance due to Ag⁺ release.
[351] In contrast, Hu et al. (2017) reported that embedding nanosized Ag particles into a polymer matrix significantly reduced leaching compared with micro- and macrosized counterparts.
[352] Moreover, Wan et al. (2017) demonstrated that the incorporation of polyacrylic acid into poly(vinylidene fluoride) membranes effectively minimized Fe/Pd bimetallic nanoparticle leaching, thereby enhancing the long-term stability of the composite material.
[353]Beyond surface tuning, PNCs also show strong potential for heavy metal removal. Mishra et al. developed mixed matrix membranes by incorporating ferrous sulfide and carboxyl-functionalized ferroferric oxide (CFFO) NPs into a PVDF matrix, achieving high removal efficiencies for Cr(VI) (88%), Cd
2+ (99%), Pb
2+ (99%), and As (95%) from industrial groundwater
[315].
Ding et al. fabricated multifunctional PVDF/PANI ultrafiltration membranes that enhanced Pb
2+ removal through combined sieving and adsorption mechanisms, outperforming pure PVDF membranes.
[314] Additionally, Bubela et al. reported that surface-modified PVDF/Fe
3O
4 membranes effectively removed excess Fe(II), reducing its concentration in permeate from 20 ppm to below WHO (0.3 ppm) and EU (0.2 ppm) limits, with rejection rates of 97.1% and 99.4% at pH 8.
[313]5.4 Biomedical Applications
PNCs have attracted significant attention in biomedical research since the early 2000s due to their potential to advance various healthcare applications.
[354]-[357] These composite materials are designed to interact directly with biological systems, including cells, tissues, and organs. They must exhibit excellent biocompatibility to ensure safety in medical settings.
[358] Additionally, the stimuli-responsive, conductive, magnetic, bioactive, and regenerative properties of PNCs must be tailored to meet the specific requirements of each biomedical application. Polymers, particularly those derived from natural sources, are widely used in biomedical applications due to their superior biocompatibility and biodegradability.
[359]-[362] Furthermore, the incorporation of NPs into the polymer matrices enhances several key properties, including stimuli responsiveness, electrical conductivity, optical and magnetic characteristics, bioactivity, and regenerative potential.
[363]-[367] This section highlights recent advancements in PNCs for biomedical applications, specifically in drug delivery, tissue engineering, biomedical imaging, and wound healing. A visual summary is provided in
Fig. 11. 5.4.1 Drug Delivery
Luanda et al.
[368] developed a nanocomposite hydrogel using locust bean gum (LBG), poly(4-acryloylmorpholine) (PAcM), and Ag NPs for the targeted delivery of 5-fluorouracil (5-FU), an anticancer drug, in the gastrointestinal tract. Drug release efficiency was assessed under simulated gastric (pH 1.2) and intestinal (pH 7.4) conditions at 37°C, as shown in
Figs.11a and
11b. The results demonstrated a pH-dependent release profile, with significantly higher release at pH 1.2 due to the protonation of acryloylmorpholine units and electrostatic repulsions, which facilitated polymer chain relaxation. These findings suggest the nanocomposite hydrogel is particularly well-suited for stomach cancer treatment. Furthermore, the nanocomposite exhibited enhanced drug release efficiency, achieving 72.11% release at pH 1.2 within 3 hours, compared to 44.21% for the neat gel. The incorporation of Ag-NPs played a crucial role in improving release behavior, as the nanocomposite structure was more porous, promoting better diffusion and drug release kinetics.
Similar pH-responsive behavior has been observed in other PNCs systems designed for cancer therapy. Pooresmaeil et al.
[373] reported a carboxymethyl starch-based nanocomposite incorporating Bio-MOF(Zn) and graphene quantum dots (GQDs) for co-delivery of curcumin and doxorubicin (DOX), which demonstrated enhanced drug release at pH 5.0 and reduced cancer cell viability to 23.5%. Likewise, Aslani et al.
[374] developed a PAA/PEG hydrogel embedded with hydroxyapatite (HAP) NPs for DOX delivery, resulting in over two-fold higher release at acidic pH and greater cytotoxicity against HeLa cells compared to free DOX. In addition to pH sensitivity, PNCs have also demonstrated potential in temperature-responsive drug delivery. Colli et al.
[375] designed thermoresponsive nanocomposites by embedding iron oxide nanocrystals into zwitterionic NPs. This system achieved 98% drug release at 43°C within 2 hours, whereas only ~5% was released at 37 °C after 8 hours. Moreover, PNCs have further evolved to exhibit dual-responsive behavior, responding to both pH and temperature. Dashti et al.
[376] reported a chitosan-PNIPAAm@ZIF-8 nanocomposite for breast cancer therapy that demonstrated dual-responsive drug release. Carboplatin release was primarily pH-dependent (92% at pH 5.5), while DOX release was temperature-sensitive, with nearly 100% released at 40°C. Similarly, Huang et al.
[377] developed a luminescent dual-responsive nanocomposite based on mesoporous silica and PNIPAAm-chitosan, which showed efficient DOX release (~70% in 24 h) under tumor-mimicking conditions (pH 5.0 and 42°C), along with significant cytotoxicity against HeLa cells.
Thi et al.
[369] developed a nanocomposite composed of Ag-NPs coated with a hyaluronic acid (HA) shell (Ag-NPs@HA) for intracellular delivery of DOX. The nanocomposite exhibited both pH-responsive and tumor-targeting capabilities. In an in vivo study using a HeLa-xenografted mouse model, Ag-NPs@HA/DOX demonstrated superior tumor suppression with minimized systemic toxicity compared to free DOX. As shown in
Fig. 11c, tumor volume in the control group (PBS) increased by 165% during the treatment period, while treatment with free DOX and Ag-NPs@HA/DOX reduced tumor volumes by 30% and 15%, respectively. Remarkably, 50% of mice treated with Ag-NPs@HA/DOX achieved complete tumor ablation. Moreover, severe inflammation and necrosis were observed at injection sites in the free DOX group, indicating its systemic toxicity
(Fig. 11d). In contrast, Ag-NPs@HA significantly mitigated these adverse effects, reinforcing its promise as a PNCs for targeted anticancer drug delivery.
5.4.2 Tissue Engineering
Xue et al.
[370] developed a guided bone regeneration membrane composed of a double-layer PCL/collagen (PCL/Col) structure modified with ZIF-8 NPs (PCL/Col/ZIF-8). The resulting PCL/Col/ZIF-8 membrane exhibited a combination of high porosity, stable tensile modulus, and pH-responsive zinc ion (Zn
2+) release. It effectively prevented fibroblast infiltration while promoting the osteogenic differentiation of rat bone marrow mesenchymal stem cells and angiogenesis of human umbilical vein endothelial cells in vitro. In vivo analysis using a rat calvarial defect model
(Fig. 11e) revealed newly formed bone, with 3D reconstructed images showing the greatest bone healing in the PCL/Col/ZIF-8 composite group, followed by the Col group, PCL/Col group, and the blank group. This was further supported by the highest bone volume to tissue volume ratio in the PCL/Col/ZIF-8 composite group (48.03% ± 4.48%)
(Fig. 11f). Additionally, newly formed bone under this membrane was uniformly distributed and exhibited the highest bone mineral density (152.79 ± 12.84 mg/cc)
(Fig. 11g).
Several other studies have explored PNCs to support bone regeneration. Soltani et al.
[378] incorporated metal oxide NPs (FeO and CuO) into a chitosan/alginate hydrogel, resulting in significantly enhanced osteogenic differentiation of ovine BM-MSCs. The nanocomposite demonstrated superior performance in alkaline phosphatase (ALP) activity, calcium deposition, and osteogenic gene expression, with CuO-NPs outperforming FeO-NPs. Fazeli et al.
[379] modified 3D-printed PCL scaffolds with HAP and bioglass NPs, leading to increased mineralization, higher osteoblast and osteocyte counts, and upregulated osteogenic markers such as ALP, Col1, and osteocalcin, supported by favorable modulation of osteogenic microRNAs. Similarly, Cidonio et al.
[380] developed a Laponite (LAP)-gellan gum (GG) nanocomposite hydrogel that enhanced C2C12 cell proliferation and promoted early osteogenic differentiation, as indicated by stronger ALP expression. LAP-GG also demonstrated improved angiogenesis, with enhanced blood vessel formation when combined with VEGF. Furthermore, Li et al.
[381] engineered a multifunctional PPEMA/GelMA hydrogel incorporated with dexamethasone-loaded ZIF-8 NPs for bone regeneration in periodontitis. The nanocomposite not only promoted osteogenesis by increasing the expression of osteogenic markers but also reduced osteoclast activity, inflammation, and alveolar bone loss in a rat periodontitis model.
PNCs are also gaining attention in neural tissue engineering, where they facilitate nerve repair and functional restoration. Hung et al.
[382] developed chitosan-gold NPs (chitosan-Au) nanocomposites that enhanced MSC neural differentiation, as indicated by upregulated neural markers and reduced CD44 expression. Chitosan-Au implantation decreased inflammation and fibrosis while promoting endothelialization. Hong et al.
[383] incorporated iron oxide NPs into a fibrin hydrogel, promoting neurogenesis and angiogenesis through upregulation of nerve growth factor and vascular endothelial growth factor. In vivo studies, axonal maturation and motor recovery were improved, with outcomes comparable to autografts. Similarly, Karimi et al.
[384] showed that SPION-loaded gelatin hydrogels improved osteo-endothelial mesenchymal stem cell (OE-MSC) proliferation and induced neural-like differentiation. Zhang et al.
[385] designed ZIF-8-modified chitosan conduits that enhanced Schwann cell function, reduced inflammation, and improved axonal regeneration, myelination, and muscle recovery. Furthermore, Sang et al.
[386] introduced ZnO quantum dot-decorated MXene hydrogels that suppressed oxidative stress and mitochondrial damage, promoted autophagy, improved neural repair and angiogenesis, while facilitating motor function recovery in spinal cord injury.
PNCs can also enhance conductivity properties, making them suitable for muscle and cardiac tissue engineering. Srinivasan et al.
[387] designed an electroconductive cardiac patch using bacterial nanocellulose (BC) incorporated with PPy NPs. The conductivity increased with the addition of pyrrole, reaching 0.02 ± 0.01 S/cm, comparable to native myocardial tissue (~10⁻³ S/cm). The BC-Ppy nanocomposite improved cardiomyoblast attachment, cell elongation, and differentiation into a cardiomyocyte-like phenotype, and upregulated cardiac markers. Similarly, Boularaoui et al.
[388] developed GelMA-based hydrogels incorporating AuNPs or MXene NSs to enhance electrical conductivity for skeletal muscle tissue engineering. Both AuNPs and MXene significantly increased conductivity, mimicking the native extracellular matrix environment. Upon differentiation, C2C12 cells encapsulated in GelMA-AuNPs and GelMA-MXene exhibited higher fusion indices, greater myotube length and diameter, with AuNPs yielding superior results.
5.4.3 Biomedical Imaging
Arias-Ramos et al.
[371] developed conjugated polymer NPs incorporating NiFe
2O
4 magnetic cores (CPNiNPs) using the nanoprecipitation method. These CPNiNPs were evaluated in vivo in glioblastoma-bearing mice using both orthotopic and heterotopic tumor models. In the orthotopic model
(Fig. 11h), tumor regions showed a strong decrease in signal variation (%), confirming high NP accumulation compared to the contralateral healthy brain. This suggests effective tumor targeting, likely due to the enhanced permeability and retention effect. In the heterotopic model
(Fig. 11i), a strong signal decrease in the liver and kidneys indicated that CPNiNPs were primarily cleared via hepatic and renal pathways, with minimal accumulation in other organs. T2-weighted MRI scans revealed a sustained signal intensity reduction for at least 30 minutes post-intravenous injection, confirming CPNiNPs as an effective contrast agent for tumor visualization. Intratumoral injection led to hypointense MRI regions due to the magnetic properties of NiFe
2O
4 (Fig. 11j). The signal remained stable over time, indicating good retention and minimal diffusion, making them suitable for long-term imaging. Whba et al.
[389] further developed a dual-mode MRI contrast agent by incorporating CNC with PEG, NaOH, and gadolinium oxide NPs (CNC-PEG/NaOH/Gd
2O
3). The nanocomposite enhanced T1- and T2-weighted MRI signals in a concentration-dependent manner, exhibited high relativity values (r
1 = 21.694 mM
-1s
-1, r
2 = 43.799 mM
-1s
-1), and a favorable r
2/r
1 ratio of 2.02, outperforming commercial agents.
Several polymer-based nanocomposites have been engineered as bimodal imaging agents by integrating multiple imaging modalities. Dong et al.
[390] designed Her2-targeted gold-nanoshelled PLGA hybrid NPs for dual ultrasound and magnetic resonance imaging, demonstrated strong tumor-specific contrast in both modalities and high transverse relativity (r
2 = 441.47 mM
-1s
-1). Similarly, Jin et al.
[391] developed magnetic nanobubbles encapsulating SPIONs and DOX in PLGA-PEG-FA, which enhanced US signal intensity by 64% and demonstrated an r
2 relativity of 109.18 mM
-1s
-1 in MR imaging. In vivo biodistribution revealed improved tumor accumulation through folic acid targeting. Wang et al.
[392] constructed nanocomposites from luminescent up conversion NPs and vanadium disulfide (VS
2), modified with PEG, for dual UCL and MR imaging. These nanocomposites exhibited sustained cytosolic luminescence signals and favorable T1-weighted contrast (r
1 = 2.31 mM
-1s
-1). Hassani et al.
[393] introduced a chitosan-coated iron oxide/graphene quantum dot nanocomposite for dual-mode MRI and fluorescence imaging. The nanocomposite retained sufficient transverse relativity and magnetic responsiveness for targeted MR imaging, while fluorescence studies confirmed strong, stable, and long-term photoluminescence properties. Furthermore, other nanocomposites have shown potential in applications such as cell tracking and SPECT/CT imaging. Dutta et al.
[394] developed a polymeric hydrogel with TEMPO-oxidized nanocellulose (T-CNCs) and carbon dots (CDs) for tissue regeneration, demonstrating enhanced fluorescence retention for non-invasive cell tracking. Zhu et al.
[395] created
[131]I-labeled gold NPs (APAS-Au PNPs) for dual-mode SPECT/CT imaging, showing improved tumor targeting and enhanced imaging signals.
5.4.4 Wound Healing
Lin et al.
[372] introduced self-assembled nanocomposite hydrogels (SANHs) by incorporating Puerarin-loaded NPs (Pue-NPs) into PAA hydrogel for diabetic wound healing. The efficacy of SANHs was evaluated in streptozotocin-induced diabetic mice, where wound healing analysis
(Fig. 11k and 11l) demonstrated that SANHs significantly accelerated wound closure. By day 7, wound contraction in the SANHs group reached 81.54%, compared to 65.19% in the disease model and 73.58% in the PAA-Gel group. By day 14, the SANHs group exhibited near-complete wound healing, while the disease model still showed 15.83% of the wound area remaining. In addition, SANHs promoted scab exfoliation and hair regrowth. SANHs also demonstrated potent antibacterial activity against
E. coli (Fig. 11m, 11o), with 92.22% bactericidal activity after 4 hours. SEM imaging
(Fig. 11n) confirmed severe bacterial membrane damage, suggesting superior antibacterial efficacy compared to the Pue solution and PAA-Gel. Complementing this, Tang et al.
[396] developed a hydrogel based on astragalus polysaccharide, chitosan, and sodium alginate, embedded with conductive PPy-PDA-MnO
2 NPs. This nanocomposite exhibited enhanced fibroblast migration, improved electrical conductivity, reduced expression of inflammatory cytokines (IL-6, TNF-α), and increased angiogenesis markers (VEGF, CD31). These features contributed to significantly faster wound closure with only ~9.3% residual wound area on day 21. In addition, Manjit et al.
[397] fabricated polyvinyl alcohol (PVA)/chitosan nanofibers co-loaded with AgNPs and luliconazole (LZNPs) for diabetic foot ulcer treatment. This nanocomposite displayed superior antifungal and antibiofilm activity, enhanced collagen deposition, and improved blood perfusion. Among all tested groups, the nanocomposite achieved the highest wound closure rate, with only 1.30 ± 0.32% residual area remaining by day 18.
Beyond diabetic wound management, PNCs have also shown promising therapeutic effects in burn wound treatment. Valadi et al.
[398] developed an alginate-chitosan hydrogel incorporated with green-synthesized ZnO NPs, which exhibited concentration-dependent antioxidant activity and strong antibacterial effects against
E. coli and
S. aureus. In vivo studies demonstrated enhanced wound healing, with wound size reduced to 0.38 ± 0.05 cm
2 by day 21, alongside improved re-epithelialization, collagen deposition, and neovascularization. Similarly, Maghsoudi et al.
[399] engineered an alginate-gelatin hydrogel loaded with zeolitic imidazolate framework-8 (ZIF-8) NPs. The nanocomposite achieved 99% bacterial inhibition against
E. coli and
S. aureus, promoted fibroblast proliferation, and significantly accelerated wound closure, reaching 89.40% by day 21. Histological analysis confirmed enhanced epidermal regeneration, neovascularization, and elevated TGF-β expression, indicating active tissue remodeling.
Aside from specific wound types, PNCs have also shown broad applicability in enhancing general wound healing. Tang et al.
[400] encapsulated CuO NPs within PEG-b-PCL polymersomes and Pluronic F127. Compared to free CuO NPs, the nanocomposite effectively scavenged ROS, reduced proinflammatory cytokines, boosted fibroblast proliferation, and upregulated growth factors. In vivo studies showed that the nanocomposite promoted the fastest wound closure, enhanced collagen deposition, and elevated angiogenesis markers. Moreover, it demonstrated superior antimicrobial efficacy, eradicating nearly 100% of
E. coli and
S. aureus, and outperformed commercial Silvercel™. Similarly, Leng et al.
[401] incorporated curcumin NPs into a collagen-PVA film (CPCF), enhancing its antibacterial activity and reducing inflammation. The CPCF film achieved a wound healing rate of 98.03% by day 15, supported by denser collagen networks, organized fibroblast alignment, complete re-epithelialization, and elevated TGF-β1 expression, confirming accelerated tissue remodeling.
Cytotoxicity assessments of PNCs in biomedical applications varied considerably across fields. In drug delivery, evaluations were largely confined to single immortalized cell lines (e.g., IEC-6
[332], HepG2
[337], MCF-7
[338], HeLa
[341]), with only a few studies employing primary dermal fibroblasts
[333], [339] and none extending to in vivo models, leaving a major gap in confirming biocompatibility. Tissue engineering studies employed broader strategies, ranging from immortalized cell lines (e.g., C2C12
[344], [352], PC12
[347]) to primary cultures such as mesenchymal stem cells
[334], [342], [343], [346], [348], dermal fibroblasts
[345], and Schwann cells
[349], and in some cases in vivo rodent implantation with histological and biochemical analyses
[334], [346], [347], thereby providing stronger evidence of compatibility. By contrast, most biomedical imaging studies focused on cancer-derived cell lines (e.g., HeLa
[353], [356], MDA-MB-231
[354], A549
[357]), with only limited assessment in healthy cells
[358] and occasional in vivo biodistribution studies
[355], [359], thus reflecting anticancer effects rather than general safety in normal tissues. Wound healing studies primarily relied on immortalized cell lines (e.g., L929
[360], [363], HUVEC
[360], NIH-3T3
[364]), with some inclusion of keratinocytes
[361] and skin fibroblasts
[365]. Although many incorporated in vivo rodent models, these were typically designed to evaluate therapeutic efficacy rather than systematic toxicity. Collectively, these findings highlight that while tissue engineering provides the most comprehensive cytotoxicity evaluations, most other applications remain constrained by their reliance on basic cell models and the scarcity of robust in vivo validation.
Beyond direct cytotoxicity, potential risks arising from material release and degradation also warrant careful consideration. Several metal and magnetic nanoparticles, including CuO
[342], [364], Gd₂O₃
[353], Fe
[335], and Ni NPs
[335], pose notable biosafety concerns at high concentrations. Prolonged exposure has been linked to their accumulation in organs such as the liver, kidney, bone, skin, and even the gray matter of the brain
[335], [357], [364]. Incorporation of these NPs into PNCs has improved acute biocompatibility in both in vitro and in vivo models. However, their long-term safety, particularly with respect to clearance pathways and the accumulation of degradation byproducts, remains poorly understood. Addressing these gaps in knowledge is essential to enable safe and clinically relevant translation.
5.5 Chemical and Biosensor Applications
Polymer has been used as a sensor that utilizes good chemical and physical properties to detect and respond to various parameters, including temperature,
[402]-[404] pressure,
[405]-[408] pH,
[409]-[412] humidity,
[413]-[417] or specific chemical
[418]-[423] and biological
[424]-[427] agents. Chemical sensors are devices designed to detect specific chemical substances in the environment, converting chemical information into a readable signal. The chemical sensors need to be developed as detectors to recognize the hazardous chemicals, both liquid and gaseous, from various fields, including environmental monitoring, industrial safety, medical diagnostics, and food quality control. Chemical sensors typically consist of a recognition element, which interacts with the chemical target, and a transducer that converts this interaction into an electrical, optical, or thermal signal. Depending on their design and application, chemical sensors can detect gases, ions, or biomolecules with high sensitivity and selectivity.
[428] Meanwhile, biosensors have a function to detect biological substances or changes in biological systems. Biosensors typically combine the biological element, such as enzymes, proteins, lipids, antibodies, polysaccharides, or nucleic acids, including viruses and bacteria. It also has a transducer that converts the biological response into an electrical or optical signal. Biosensors are widely used in medical diagnostics, environmental monitoring, food safety, and biotechnology. In healthcare, for instance, biosensors can be used to detect glucose levels in diabetic patients, cholesterol, pathogens in water supplies, or even biomarkers for cancer.
[429]By engineering the specific polymers, the sensitivity and selectivity of these sensors can be tailored for targeted applications, particularly in chemical and biological components. Conducting polymers are commonly used with other components in these sensors since they have a good response as the sensing materials. They can respond to chemical, physical, or biological stimuli through changes in their electrical conductivity, color, or other measurable properties. When exposed to a target analyte, such as a gas, ion, or biomolecule, the polymer undergoes a redox reaction or physical interaction that alters its electronic structure. This change can be detected and quantified by simple electronic or optical systems. Conducting polymers can conduct electricity that is generated from a system of conjugated double bonds along the polymer backbone, allowing for the movement of charge carriers. Popular examples include PANI, PPy, PEG, PVA, and Pth. These materials can be easily synthesized, processed into various forms (films, fibers, or composites), and chemically modified to enhance their properties, making them highly recommended for sensor applications. Another advantage of conducting polymers is their tunable selectivity. By incorporating functional groups or blending them with other materials (e.g., metal NPs or enzymes), these polymers can be tailored to detect specific analytes with high accuracy. For instance, a PANI-based sensor can be engineered to detect ammonia gas, while a PPy composite might be optimized for glucose sensing. Furthermore, their compatibility with flexible substrates enables the development of wearable sensors and other portable diagnostic devices.
[422], [428], [430]-[432] Surface modifications on polymer-based biosensors can promote covalent bonding or adsorption of biological recognition elements, enhancing the sensitivity and specificity of the biosensor. Conducting polymers like PANI and PPy are highly attractive due to their ability to transduce biological interactions into measurable electrical signals. When an analyte interacts with the biosensor, it induces changes in the electrical conductivity, potential, or capacitance of the polymer layer, which can be easily detected and quantified.
[433]Fig. 12a shows a schematic detection of the micro-ring resonator biosensor, a polysiloxane-based polymer for Staphylococcal Protein A (PA). Protein can be absorbed on the surface via intermolecular forces based on the physicochemical properties of the surface. The hydrophobicity of the surface should be at a medium level to facilitate the stable attachment between the material surface and the proteins. PA has good affinity coupled with human Immunoglobulin G that has been used as a biosensing process of polymer resonators. increase of resonant wavelength.
[434] Protein can also be detected by investigating its interaction with Poly(N-isopropylacrylamide) (PNIPAM). The sensing binding of Immunoglobulin G molecules to the immobilized PA layer could be detected by an abrupt detection uses the diffusion level based on the Stokes-Einstein fitting model.
[439] It is different from the protein detection; the bacteria could be detected using electrochemical (EC) detection as depicted in
Fig. 12b. An EC biosensor based on surface-imprinted polydopamine-
E.coli -modified electrodes and polyclonal antibody with nitrogen-doped GQDs (pAb-N-GQDs) was developed for sensitive and selective detection of
E.coli through antigen-antibody interactions. Optimal conditions were determined to be pH 8.0 and a two-hour incubation time, which yielded the highest EC signal due to efficient antibody binding. Under these conditions, EC intensity increased proportionally with bacterial concentration from 10
1 to 10
7 CFU mL
-1, achieving a detection limit of 8 CFU mL
-1 and a strong correlation (R = 0.998).
The sensor demonstrated high specificity, with no significant response to
Salmonella or other bacteria, and interference tests confirmed minimal impact from common ions and amino acids. Additionally, the biosensor showed excellent recovery rates (0.994-1.02) in spiked water samples and outperformed existing methods with its broader linear range and lower detection limit, confirming its reliability and practicality for real
E. coli detection.
[427] EC is also used as an amino detection through the diffusion process on the modified surface of Pth-NH
2-g-PEG as depicted in
Fig. 12c. Pth-NH
2-g-PEG exhibits good detection features with the concentration of 2.5 μM catechol and reaches the highest sensitivity at 132.45 μAmM
−1. Along with 12.5 μM catechol, a number of substrates, including ethanol, acetamidophenol (10 μM), ascorbic acid, and uric acid, were introduced to the reaction medium in order to investigate the interference effects on the biosensor response.
Fig. 12d shows that the signal of catechol with different concentrations was similar. Meanwhile, the other interfering components show no significant change in the current responses.
[435] On the branched-chain amino acids (BCAAs) detection, the resistance responses enlarged gradually until the BCAAs became stable along with the increasing concentration from 0.001 to 100.0 μg/mL of analytes. The resistance changes (ΔR/R0, %) responded dynamically linearly with the logarithm values of concentrations from 0.001 to 10.0 μg/mL. BCAAs detection on EC methods based on molecular imprinted polymer (MIP) biosensors achieved lower limit of detection (LOD) and exhibited stronger practical application. MIP biosensors demonstrated remarkable
in situ recognition and regeneration capabilities through appropriate EC techniques and excellent capacity to detect complex human sweat samples.
[440]Fig. 12e, demonstrates the detection of microRNA using PVP and PVA hydrogel-based. The copper nanoclusters (Cu NCs) were introduced to the hydrogel with dihydrolipoic acid (DLHA), showing the highest EC intensity (13055 a.u.) due to DHLA’s dual binding sites enhancing stability. Incorporation into a PVP−PVA hydrogel further boosted EC performance and stability by limiting non-radiative relaxation, preventing oxidation, and increasing local Cu NCs concentration. The resulting DHLA-Cu NCs@(PVP−PVA) hydrogel composite exhibited good and stable EC response with a maximum emission at 500 nm. The biosensor was tested with breast adenocarcinoma cells (MCF-7) and HeLa cell lysates to detect miRNA-21. EC intensity increased significantly with MCF-7 cell concentration, indicating high miRNA-21 expression, while only slight changes were observed with HeLa cells, reflecting low expression.
[436] Additionally, other polymers could be used for miRNA detection, including carboxyl-functionalized poly[(9, 9-dioctylfluorenyl-2, 7-diyl)-co-(1, 4-benzo-{2, 1′-3}-thia-diazole)] (PFBT-COOH)-based to detect miRNA-155,
[441] and nanostructured coordination polymers (Ce−Ru−NCPs)-AuNPs modified based to detect miRNA-141.
[442] It shows good potential for miRNA detection in cancer diagnostics. Other polymers that can be used for tumor/cancer detection include terbium complex-doped epoxy cellulose polymer for cancer antigen 125 detection,
[443] and PEDOT for MCF-7 detection.
[444] On the other hand, DNA detection can also be performed by polymer-based biosensors such as poly(ethylene terephthalate) (PET)-based, using the electroacoustic resonance phenomenon at ~30 MHz, which is promising for the integration of electroacoustic sensors toward biochips as schemes of QCM miniaturization in microsize
[445] and poly(dimethylsiloxane) (PDMS)-based with a detection limit of ~200 target copies in a probed volume of 150 µL (1.4 copies/µL) for a DNA sequence specific to Candida albicans.
[425] Besides, PDMS could also be used as bovine serum albumin (BSA)
[446] and enzyme detections
[426] combining with other polymer-based such as phospholipid 1, 2-diacyl-sn-glycero-3-phospho-(1-rac glycerol),
[447] PAA and poly(1-vinyl imidazole).
[431].
Fig. 12f shows the schematic detection by optical fiber coated with polymerized dopamine and beta-cyclodextrin (β-CD). A polymerized dopamine-based biosensor can detect cholesterol concentrations in the range of 0.001 to 1 mM that has a sensitivity of 12.7 nm/mM in the concentration range of 0.001 to 0.05 mM and can respond rapidly in the concentration range of 0.001 to 1 mM.
[437] β-CD can be mixed with other polymers such as poly(2-(2-octyldodecyl)-4, 7-di-(selenoph-2-yl)-2H-benzo[d][
1,
2,
3]triazole)) to detect the cholesterol. This composite has responses at −0.7 V vs Ag/AgCl in phosphate buffer (pH 7.0), a maximum current (I
max) of 12.1 μA, LOD at 0.005 μM, and sensitivity values at 5.77 μA/μMcm
2.
[443] Other biological parameters that influence human health can also be detected by composite polymer-based. Stress detection using PEI and PEG,
[424] cortisol detection using hydrogel poly(styrene)-block-PAA,
[448] antibiotic residual detection using PVA-graphene oxide-aptamer,
[449] blood pressure using polylactide (PLA),
[450] glutamate detection using polytetrafluoroethylene (Teflon),
[451], [452] and glucose detection using acrylic acid, PEG diacrylate (PEGD), and microbial bioflocculant polymers.
[453], [454] In general, these detectors use the EC detection method; however, it is possible to use the fluorometric methods for cyanide detection, which is lethal to humans, as shown in
Fig. 12g.
[438].
In addition, polymer-based sensors could also be used as chemical detectors, particularly for gases and volatile organic compound (VOC) detection. The release of VOCs, especially halogenated VOCs (X-VOCs), poses serious environmental and health risks. X-VOCs, containing fluorine or chlorine (HF or HC), are widely used in industry but are highly toxic, persistent, and difficult to degrade, contributing to ozone depletion, difficult to detect due to their thermal stability, chemical inertness, and poisoning effect on gas sensors at high temperatures. Wu et al. used 1-ethyl-3-methylimidazolium bis (trifluoromethylsulfonyl)imide-based ionic gel film and successfully detected X-VOC with high selectivity and high response time.
[460] Toluene and benzene are other VOCs that are categorized as harmful to human health. Sensor-based polyimide fiber, polyacrylate, and tetraphenylethylene functionalized UiO-66 have excellent fluorescence to detect them.
[461], [462] Other VOCs and gas detections are shown in
Table 4. Generally, in the gas schematic sensors, gas or VOC molecules will interact with the polymer matrix as depicted in
Fig. 13a. The interaction between molecules and polymer, particularly the Poly (3-hexyl thiophene) (P3HT), derives from two kinds of aggregation, including H-aggregation (i.e., face-to-face arrangement). It is preferred by P3HT chains with a high degree of torsional disorder, whereas J-aggregation (i.e., end-to-end arrangement) is more favorable for P3HT chains with a high degree of planarity in the thiophene rings, as shown in
Fig. 13b.
[455] The response output of gas and VOC detection could be in various forms, including the EC or I-V signal, colorimetric, or the fluorescence output. The fluorescence output is commonly operated by detecting changes in the optical properties of a fluorescent material upon exposure to specific gas molecules. The polymer doped with fluorescent molecules, e.g., β-cyano-appended oligo(p-phenylenevinylene) (β-COPV) as shown in
Fig. 13c, induces changes in fluorescence intensity, wavelength, or lifetime.[
456] Besides the EC methods, the response outputs are commonly displayed by the graph as depicted in
Fig. 13 (d-f).
PNC-based sensors improve detection limits and selectivity for pesticides in environmental samples by combining nanoscale materials with conductive polymers, which enhances the electrode surface properties. This modification increases sensitivity and stability, allowing for lower detection limits and better selectivity. For example, sensors fabricated via free radical polymerization using functional monomers and cross-linking agents have demonstrated linear detection ranges with low limits of detection (e.g., 6 nM) and high recovery rates (97-110%) in real samples like cabbage and apple peel. These improvements arise from the synergistic effects of the polymer matrix and nanomaterials, which facilitate efficient electron transfer and specific interactions with pesticide molecules. [
463], [
464] In addition, PNC sensors can be fabricated via cost-effective methods such as solution mixing, melt blending, and 3D printing, which potentially lowers production costs compared to high-temperature and complex fabrication processes needed for metal oxide sensors.[
465] Polymers are also widely varied from high-cost raw materials to cheap raw materials. It can be an alternative for researcher to develop low-cost material sensor using polymers. However, high-performance nanofillers like graphene may increase cost, but overall polymer-based sensors hold economic advantages in scalability and fabrication.[
428]
6. Challenges, future directions, and outlooks
In the past decade, PNCs have made remarkable progress across multiple fields, driven by their tunable properties and multifunctional capabilities. However, these emerging composite materials face intricate challenges in material performance, scalability, and sustainability. Several key hurdles and emerging opportunities that should be anticipated in the energy sectors: Material limitations, such as high dielectric loss and energy dissipation, limit energy storage efficiency, and thermal instability. Secondly, processing complexities cover dispersibility issues and scalability constraints. The shortcomings, such as commercialization barriers due to the utilization of NP toxicity, complicate its economic expansion. Despite their outstanding performance at the laboratory scale, the industrial feasibility of PNC fabrication remains a central challenge. Techniques such as electrospinning, while effective for tailoring nanoscale morphology, are often constrained by low throughput, high energy demand, and costly equipment requirements, which limit large-scale deployment. Addressing these bottlenecks requires systematic evaluation of process economics and sustainability, including energy consumption and production yield. Recent developments in scalable methods, such as phase inversion casting, melt compounding, and additive manufacturing, offer more promising routes for mass production, as they align better with existing industrial infrastructure.
[486]-[488] Integration of green chemistry principles, solvent recovery, and continuous-flow processing could further improve cost-effectiveness and environmental compatibility. These considerations are crucial to ensure that PNCs not only achieve high performance but also remain viable for widespread industrial adoption. To some extent, recent advances of PNC application in petroleum engineering and environmental remediation have led to several issues to be addressed: good performance under harsh conditions (thermal and salt stability, mechanical durability), uniform dispersion and long-term performance, and sustainability. Concerning the biomedical and biosensor applications, several significant challenges must be addressed for their successful clinical translation and widespread adoption. This would anticipate the upsurge in interest in enhancing biocompatibility and toxicity, for instance, PNCs are non-toxic and biocompatible both
in vitro and
in vivo, which remains a central challenge.
Future direction in the advancement of PNC as active materials in energy research is to prioritize the realization of membranes with higher proton conductivity that can survive under extreme conditions (e.g., low humidity, high temperatures). In particular, emerging low-dimensional materials spanning from carbon quantum dots,
[489] MXenes,
[490]-[492] metal-organic frameworks,
[493] and hybrid organic-inorganic perovskites
[494] could play a pivotal role as nanofillers toward high-performance PNC for energy applications. Such extensive material innovations in nanofiller functionalization and polymer matrix design might enhance their durability to mitigate the possibility of fuel crossover. A substitutional rational design with robust and cost-effective alternatives, such as carbon-based PNCs, is promising, while maintaining efficiency is expected to reveal a good intimacy that leads to good interfacial interaction between fillers and polymer matrix. In terms of batteries and supercapacitors investigations, one should aim to enhance the EC stability and energy density of PNC-based electrodes. High performance of self-healing PNCs to mitigate degradation during charge/discharge cycles is a promising avenue. The current trend in PNCs for environmental remediation aims for a multifunctionality, combining adsorption, photocatalysis, and membrane filtration in a single system. Scalable synthesis methods and recyclability of PNCs must be optimized to reduce environmental impact. In addition, PNC-based sensors with high selectivity and sensitivity for emerging contaminants (e.g., microplastics, pharmaceuticals) are needed. A summary of future directions in the PNC development is presented in
Fig. 14.
As an outlook, PNCs promote a promising roadmap to bridge the gap between laboratory-scale innovations and real-world applications. In the coming year, the current technical limitations of highly anticipated PNCs designed with unique structural heterogeneity are expected to play a transformative role in advancing energy sustainability, environmental protection, healthcare, and smart sensing systems. ML and artificial intelligence (AI) are identified as the workforce towards key descriptors governing the high performance of PNCs. This culminates in a step closer to miniaturization and integration of PNCs with multipurpose features, such as conducting wearable nanocomposite devices in the coming years. A long-standing partnership between fundamental research and industrial partnerships is a stimulating progression toward unlocking their full potential. Such platforms are aimed at the next-generation PNC-based materials as a transformative role in advancing energy sustainability, environmental protection, healthcare, and smart sensing systems.
Abbreviations
DFT: Density functional theory
MD: molecular dynamics
NPs: nanoparticles
NP: nanoparticle
PANI: polyaniline
PAA: poly(acrylic acid)
PAM: polyacrylamide
PABA: poly(anilineboronic acid)
vdW: van der Waals
RFR: random forest regression
GDBT: gradient boosting decision tree
XGBoost: extreme gradient boosting
GPR: Gaussian process regression
SEM: scanning electron microscopy
XRD: X-ray Diffraction
TEM: Transmission Electron Microscopy
AFM: Atomic Force Microscopy-Infrared
SAXS: Small Angle X-ray Scatterings
WAXS: Wide Angle X-ray Scatterings
PCL: polycaprolactone
P3HB: poly(3-hydroxybutyrate)
PEDOT: poly(3, 4-ethylenedioxythiophene)
NSs: Nanosheets
SEP: sepiolite
CNC: cellulose nanocrystal
PEG: poly(ethylene glycol)
SANS: Small-angle neutron scattering
NSE: neutron spin echo
NMR: nuclear magnetic resonance
FLIM: fluorescence lifetime imaging microscopy
TERS: tip-enhanced Raman spectroscopy
PALS: positron annihilation lifetime spectroscopy
GC: gas chromatography
LIBs: Lithium-ion batteries
GO: graphene oxide
rGO: reduced graphene oxide
DSSCs: dye-sensitized solar cells
Pth: Polythiophene
Pt: platinum
PPy: Polypyrrole
Si: Silicone
SMA: styrene maleic anhydride
PCE: power conversion efficiency
PG: polymer gel
HQ: Hydroquinone
HMTA: Hexamethylenetetramine
HPAM: hydrolysed polyacrilamide
PEI: polyethyleneimine
PHPA: partially hydrolyzed polyacrilamide
PVP: polyvinylpyrrolidone
RF: resorcinol-formaldehyde
Na-MMT: sodium montmorillonite
G’: storage modulus
ESEM: environmental SEM
DS: degree of swelling
PPR: percentage permeability reduction
RRF: residual resistance factor
AOPs: advanced oxidation processes
UV: ultraviolet
ROS: reactive oxygen species
MB: methyl blue
MO: methyl orange
RB: rhodamine B
MG: malachite green
M3D: magnetic 3D crosslinkers
CCN: carboxylated cellulose nanocrystals
TFNs: thin-film nanocomposites
IP: interfacial polymerization
TFC: Thin Film Composite
LBG: locust bean gum
PAcM: poly(4-acryloylmorpholine)
GQDs: graphene quantum dots
DOX: doxorubicin
HAP: hydroxyapatite
HA: hyaluronic acid
ALP: alkaline phosphatase
LAP-GG: Laponite-gellan gum
CPNiNPs: conjugated polymer nanoparticles incorporating NiFe2O4 magnetic cores
SANHs: self-assembled nanocomposite hydrogels (SANHs)
PVA: polyvinyl alcohol
CPCF: collagen-PVA film
PA: Protein A
PNIPAM: Poly(N-isopropylacrylamide)
EC: electrochemical
BCAAs: branched-chain amino acids
MIP: molecular imprinted polymer
DLHA: dihydrolipoic acid
MCF-7: breast adenocarcinoma cells
HeLa: human cervical cancer
LOD: limit of detection
β-CD: beta-cyclodextrin
VOC: volatile organic compound
X-VOCs: especially halogenated VOCs
P3HT: Poly (3-hexyl thiophene)
CRediT authorship contribution statement
Geolita Ihsantia Ning Asih: Writing-original draft (equal); Ande Fudja Rafryanto: Writing-original draft (equal), review and editing (equal); Sri Hartati: Writing-original draft (equal), review and editing (equal); Xiaoyi Jiang: Review and editing (supporting); Alinda Anggraini: Writing-original draft (equal), review and editing (equal); Azis Yudhowijoyo: Writing-original draft (equal), review and editing (equal); Jizhou Jiang: Conceptualization (supporting), review and editing (equal); Arramel: Conceptualization (lead), formal analysis (lead), review and editing (equal), supervision (lead). All authors have given approval to the final version of the manuscript.
Declaration of competing interest
The authors declare that they have no known competing financial interests or personal relationships that could have appeared to influence the work reported in this article. Jizhou Jiang is the Editor-in-Chief, and Xiaoyi Jiang, Arramel are Editorial Board Members of this journal and they were not involved in the editorial review or the decision to publish this article.
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