Impact of thermal treatment and magnetic field on the dynamic mechanical behavior of polyacrylonitrile nanofibers with embedded magnetic ferrite nanoparticles†

Baran Sarac^ab, Viktor Soprunyuk^c, Eray Yüce^ad, Selin Gümrükçü^e, Wilfried Schranz*^c and A. Sezai Sarac^f
aAustrian Academy of Sciences (ÖAW), Erich Schmid Institute of Materials Science, 8700 Leoben, Austria
^bChair of Casting Research, Montanuniversität Leoben, 8700 Leoben, Austria
^cFaculty of Physics, Physics of Functional Materials, University of Vienna, 1090 Vienna, Austria. E-mail: wilfried.schranz@univie.ac.at
^dDepartment of Materials Science, Chair of Materials Physics, Montanuniversität Leoben, 8700 Leoben, Austria
^eDepartment of Chemistry, Istanbul Technical University, 34469 Istanbul, Turkey
^fPolymer Science and Technology, Istanbul Technical University, 34469 Istanbul, Turkey

First published on 23rd June 2025

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1. Introduction

Ferrite is a ceramic compound containing iron oxide, known for its ferrimagnetic properties, making it attractive to magnets and magnetizable itself. It is typically hard, brittle, a poor electrical conductor, and resistant to high temperatures. Ferrites are cost-effective, have high resistivity, and are versatile, making them a valuable material in many industries.¹ Iron oxide nanoparticles (NPs) in small sizes exhibit superparamagnetic properties, where the magnetic moment of iron oxide nanoparticles can be improved, and the surface of ferrite nanoparticles can be modified by surfactants and polymers to increase their stability in solution.² Nanoferrites are extensively utilized as advanced oxides in biomedical applications, particularly for magnetic hyperthermia treatments, owing to their unique biocompatibility, persistent magnetic behavior and exceptional ability to generate localized heating for the destruction of tumor cells.³ However, their use in cancer treatments demands specific characteristics, including biocompatibility, low toxicity, a high specific absorption rate (SAR), rapid attainment of the target hyperthermia temperature, nanoscale crystalline size compatible with biological systems, and minimal dosage requirements to achieve therapeutic efficacy.⁴

Among various ferrite materials, cobalt ferrite with the chemical composition of CoFe₂O₄ (CoO·Fe₂O₃), stands out, where the material falls between soft and hard magnetic categories and is typically classified as semi-hard.⁵ Its magnetostrictive properties can be adjusted by applying a magnetic uniaxial anisotropy, which is achieved by raising the crystal to an appropriate temperature and applying magnetization for several minutes by an external magnetic field.⁶ The generated magnetic anisotropy in cobalt ferrite also provides advantages in enhancing the magnetoelectric effect in a composite.⁷ Cobalt ferrite, a prominent member of the spinel ferrite family, exhibits an inverse spinel structure. In its ideal configuration, all Co²⁺ ions are located at the B sites, while Fe³⁺ ions are evenly distributed between the A and B sites. This material has garnered significant acclaim owing to its outstanding electromagnetic performance (i.e., strong anisotropy, high coercivity, moderate saturation magnetization), exceptional chemical stability even at high temperatures, and mechanical hardness. These properties make cobalt ferrite an excellent candidate for applications in electronic parts, such as computer systems, recording devices, and magnetic cards.⁸

Fig. 1 illustrates the various applications of cobalt ferrites across different fields. Aside from its appealing magnetic properties, cobalt ferrite is a versatile material with applications in energy storage and conversion. It can serve as an electrocatalyst for the oxygen evolution reaction (OER) and is also used in the fabrication of electrodes for electrochemical capacitors (supercapacitors), enhancing their energy storage capabilities. For example, a simple electrospinning-based synthesis of CoFe₂O₄ spinel nanofibers exhibiting excellent electrocatalytic performance for both oxygen evolution and hydrogen peroxide reduction reactions.⁹ Cobalt ferrite prepared with controlled morphology and size to enhance the surface area, and thus the number of active sites, has been published.¹⁰ The evolution of their magnetic properties was systematically analyzed in terms of particle size and shape, emphasizing characteristics that optimize performance as permanent magnets. Notably, both saturation magnetization and remanent magnetization increase consistently with particle size, ultimately stabilizing at a constant value for sizes above 20 nm.¹¹ Cobalt ferrite particle (core)–polymer (shell) NPs can be incorporated into a polymer host matrix to generate mostly transparent polymer-based magneto-optic components.¹² A proof-of-concept all-optical magnetometer has been developed utilizing a nanocomposite material composed of a cobalt ferrite core encapsulated in a polymer shell. This magnetometer achieves a noise-equivalent magnetic field sensitivity of 50 nT √Hz⁻¹, demonstrating the potential of these highly transparent and magneto-optically responsive materials for applications in magnetic field sensing systems requiring high sensitivity. Traditional ferrite cores, often used in high-inductance coils and transformers, are brittle, rigid, and bulky, and their performance is heavily affected by external factors, i.e., temperature, pressure, electromagnetic fields, and frequency. In contrast, Flexible printed circuits (FPCs) offer a more versatile alternative, capable of being processed into injection-molded parts or thin, flexible films. These materials can function at high temperatures (up to 200 °C) and are available in self-adhesive formats with thicknesses between 0.2 and 0.4 mm. FPCs are particularly effective in electromagnetic compatibility (EMC) applications, where they shield coils from metallic interference or absorb high-frequency disturbances above 500 MHz.¹³

In terms of biomedical uses, CoFe₂O₄ NPs can be utilized as an efficient magnetic resonance imaging contrast agent, which possesses higher magnetic susceptibility than iron oxide.¹⁴ It can also be utilized as controlled and localized drug release, which is often coated with biocompatible polymers and targeting ligands.¹⁵ In another study, the dressing's cellulose component was magnetized by developing magnetic cellulose through the grafting of CoFe₂O₄ NPs onto cellulose fibers using a layer-by-layer deposition method. This method effectively integrates magnetic functionality into the cellulose structure, offering potential applications in wound healing and temperature-responsive medical materials.¹⁶ Cobalt ferrite NPs have a superior heating efficiency behavior with increased saturation magnetization when doped with other compounds. Also, it has a prominent measure of SAR parameters and thus makes a substantial pathway for hyperthermia treatments.¹⁷

Polyacrylonitrile (PAN), a widely recognized polymer known for its stability and mechanical properties. The properties of PAN are strongly influenced by its crystalline structures and the arrangement of its unit cells. However, the intrinsic properties of some PAN-based materials are often inadequate for specific applications. Nanoparticle fillers effectively modify the rheological behavior of PAN and its composite formulations, improving their processability. Moreover, when compared to microparticles of the same volume fraction, NPs significantly enhance the electrical, mechanical and chemical behavior of PAN, offering a more efficient solution for advanced material applications.¹⁸

The enhanced properties of PAN-based nanocomposite fibers, including those with carbon nanotubes, graphene, and inorganic NPs, are primarily attributed to the interfacial bonding between the nitrile groups in the polymer and the nanofillers. The enhanced properties of PAN nanofibers are linked to several factors, including the interfacial bonding of nitrile groups with nanofillers, their chemical composition, hydrophobicity, porosity, and wettability. Electrospun PAN nanofibers embedded with inorganic NPs, graphene nanosheets, graphene oxide, and carbon nanotubes are proposed for a broad range of advanced applications, such as supercapacitors, high-power batteries, filtration membranes, electromagnetic interference shielding, and strain sensors.^19,20 Surface-localized and homogenously dispersed magnetic particles on electrospun nanofibers offer significant advantages for sensing, actuation, and smart material applications due to their enhanced interfacial reactivity and stimulus responsiveness. For example, exposed ferrite or plasmonic NPs improve sensitivity and selectivity by facilitating direct interactions with target analytes, as demonstrated in gas sensors²¹ and biosensors.²² For actuation, magnetic NPs (e.g., Fe₃O₄) on fiber surfaces enable rapid and precise deformation under external magnetic fields for actuators with programmable deformation.²³ In smart materials, stimuli-responsive particles such as thermoresponsive polymers²⁴ or metal oxide-containing hydrogel films²⁵ allow dynamic property modulation for adaptive textiles and drug delivery systems.²⁶

Nanocomposite fibers composed of PAN incorporating carbon nanotubes (CNTs) and cobalt ferrite NPs were fabricated by electrospinning. Transmission electron microscopy reported the internal dispersion of the CNTs and CoFe₂O₄ NPs, and fibers exhibited electromagnetic interference shielding attenuation of about 3.9 dB.²⁷ Cobalt ferrite/PAN and cobalt ferrite/carbon nanofibers were synthesized through the electrospinning technique, and fiber magnetic properties measured by vibrating sample magnetometry indicate that CoFe₂O₄/PAN nanofibers have the saturation magnetization of 45 emu g⁻¹.²⁸ Incorporation of Fe-based nanofillers for the optimization of the polyacrylonitrile matrix was conducted to fabricate PAN nanofibers blended with iron oxide and MnZn Ferrite NPs through the introduction of an external magnetic field during dynamic mechanical measurements under tension.²⁹ For the PAN/MnZn Ferrite nanofibers, a relatively larger shift in T_g (10 K towards larger temperatures) is observed, emphasizing that, in comparison to Fe₂O₃, Mn²⁺ ions, in particular, enhance the material's magnetic response in MnZn Ferrite.

This paper presents a novel approach to synthesizing nearly monodisperse cobalt ferrite nanoparticles and their integration into polymer nanofibers, with a focus on their morphologic, spectroscopic, and thermodynamic properties. The superparamagnetic characteristics of cobalt ferrite NPs and their polymer-based nanocomposites are largely impacted by the particle size and distribution within the polymer matrix. The synthesis method for polymer nanocomposites doped with cobalt ferrite fillers, engineered as nanofibers, was detailed. We also compare their thermodynamic properties under varying magnetic fields to those of Fe₂O₃. Additionally, the morphological and spectroscopic attributes of the resulting materials are thoroughly investigated, highlighting the interplay between synthesis conditions and material performance. Distinct from prior studies focusing on other metal oxides, the novelty herein is the homogeneous dispersion of cobalt ferrite (CoFe₂O₄) nanoparticles within PAN nanofibers, which yields a quantifiable enhancement in thermal stability through an elevated glass transition temperature and a significant increase in stiffness around T_x, linked to the relatively less interaction of NPs with CN groups of PAN with minimum oxide surrounding NPs.

2. Materials and methods

2.1. Material

Polyacrylonitrile (PAN, molecular weight average of 150000, CAS No.: 25014-41-9) and N,N′-dimethylformamide (DMF, purity ≥99.8%, CAS No.: 68-12-2) were procured from Sigma Aldrich. Iron oxide nanopowder (γ-Fe₂O₃, purity 99.9%, average particle diameter 10 nm, laser synthesized, near-spherical morphology, CAS No.: 1309-37-1) and cobalt ferrite nanoparticles (CoFe₂O₄, purity 99.9%, average particle diameter 30 nm, synthesized by chemical reagants, spherical morphology, CAS No.: 12052-28-7) were sourced by US Research Nanomaterials, Inc. All reagents used were of analytical grade and were employed without additional purification.

2.2. Preparation of PAN/metal oxide nanoparticle composite fibers

The electrospinning device consists of a syringe pump, a grounded aluminum collector, and a high-voltage DC power supply capable of delivering positive voltages up to 50 kV. The syringe pump allowed precise control of the polymer solution feed rate, adjustable between 5.5 μL h⁻¹ and 20 mL h⁻¹. A syringe fitted with a needle (outer diameter: 0.7 mm) connected to a positive electrode was used to eject the polymer solution. Electrospinning was performed horizontally under ambient conditions, with an applied voltage ranging between 10 and 15 kV. The polymer solutions were ejected at a constant feed rate of 1 mL h⁻¹, and the separation between the collector and needle tip was kept at approximately 15 cm to ensure consistent nanofiber formation. Co ferrite microparticles (5 wt%) were mixed with 10 mL of 10% PAN solution in a cup horn sonicator via stirring overnight, which enables the PAN/CoFe₂O₄ to be dissolved in a dimethyl formamide solution. Nanofibers were successfully produced through continuous electrospinning for 3 hours, with no evidence of sedimentation in the polymer nanofiller solution throughout the process. Following each electrospinning trial, no visible sedimentation was detected within the syringe, indicating stable dispersion of the nanofillers in the solution.

2.3. Characterization methods

Dynamic mechanical analysis (DMA) was performed using a PerkinElmer DMA-8000 instrument over a temperature range of 300–800 K at a controlled 5 K min⁻¹ heating rate. Measurements were performed in tension mode under sinusoidal forces at frequencies of 0.5, 5, and 15 Hz. Test specimens were fabricated in sheet geometry with dimensions approximately 10 mm × 7.5 mm × 0.13 mm to suit the tension testing configuration. Thermogravimetric analysis (TGA, TA Instruments) was performed by heating scans from room temperature to 800 °C at a rate of 20 °C min⁻¹ under inert nitrogen atmosphere. X-ray diffraction (XRD) was conducted in Bragg–Brentano (θ–2θ) geometry by means of a Bruker D2 Phaser diffractometer equipped with a LYNXEYE-2 detector. Measurements were carried out over an angular range of 5° to 100°, utilizing Co Kα radiation (wavelength, λ = 0.17902 nm) with a step size of 0.005°. Data smoothing was performed using the Savitzky–Golay filter with a 20-point window and a second-order polynomial to enhance the signal quality. Imaging was performed using a TESCAN MAGNA scanning electron microscope (SEM), which offers ultra-high resolution and high-contrast capabilities. To enhance conductivity and achieve a high signal-to-noise ratio, the samples were sputtered with a 1–2 nm layer of graphite via sputtering. Magnifications ranging from 500× to 100000× were employed. SEM imaging was conducted at an acceleration voltage of 20 keV, a beam current of 1 nA, an aperture size of 30 μm, and a working distance of ∼12.5 mm. The same device was used at 20 kV acceleration voltage for the subsequent energy dispersive X-ray (EDX) mapping on the same samples using Quanta FEG 250 with an attached EDX detector. The information was processed using the software AZtec (OXFORD INSTRUMENTS). Average diameter and standard deviation of the nanofibers were measured from 50 single nanofibers through ImageJ Software. Attenuated total reflectance Fourier-transform infrared (ATR-FTIR) spectroscopy was implemented through a Bruker Vertex 70 ATR spectrometer covering the wavenumber range of 600–4000 cm⁻¹. The room temperature magnetic properties were assessed by alternating gradient field magnetometer (AGFM) within a ±10 kOe magnetic field range.

3. Results and discussion

3.1. Morphological and compositional characterization

The homogenous distribution of the nanofibers was ensured by low-magnification SEM imaging (Fig. 2a). White round-looking spots corresponding to the CoFe₂O₄ agglomerates were observed and accounted for the minimization of the high surface energy of the NPs within the PAN matrix.²⁹ The PAN matrix encapsulates these particle agglomerates, leading to round-looking morphologies.³⁰ The magnified imaging displays that particles (shown by the red arrows) join nanofibers (Fig. 2b) as well as are embedded within the nanofibers upon electrospinning (Fig. 2c). The average size of the PAN/CoFe₂O₄ nanofibers measured from the SEM images is 310 ± 40 nm. This value is much smaller than pure PAN (970 ± 110 nm) and PAN/Fe₂O₃ (520 ± 50 nm) nanofibers. Visible surface roughness is observed for all sample types, which can be attributed to the inherent nature of the electrospinning process, where the rapid solidification of polymer jets leads to the formation of irregular fiber deposition and topographical variations. The compositional analysis of a representative region (Fig. 2d) identifies the existence of Fe (Fig. 2e) and Co (Fig. 2f) dispersed throughout the nanofibers as well as within the agglomerated regions. The SEM imaging of the PAN/Fe₂O₃ nanofibers shows a similar nanoparticle dispersion (Fig. S1a, ESI†). The EDX imaging (Fig. S1b, ESI†) and the corresponding qualitative elemental analysis confirm that the bright particles correspond to Fe₂O₃ NPs (Fig. S1c and d, ESI†).

3.2. Structural characterization

X-ray diffraction can reveal the type of crystalline within an semi-crystalline PAN polymer. Fig. 3a presents a comparative XRD analysis of the PAN, PAN/CoFe₂O₄ and PAN/Fe₂O₃ samples over the 5° and 100° 2θ range. The diffuse peaks at ∼19.5° correspond to the orthorhombic PAN (110) reflection.³¹ This peak shifts towards larger values, i.e., ∼19.8°, with the inclusion of NPs, indicating that the average unit lattice becomes smaller. The broad and less intense peak between 23–33° corresponds to the (002) reflection of PAN.³² As confirmed formerly by the nanopowder diffraction analysis of Fe₂O₃ and PAN/Fe₂O₃ composite,²⁹ the peaks at ∼35.5°, ∼41.8°, ∼51.0°, ∼67.7°, and ∼74.8° corresponds to (220), (311), (400), (511) and (440) reflections of the nanopowders, respectively (Fig. 3b). For the PAN/CoFe₂O₄ nanofiber, compared to PAN/Fe₂O₃, there is a slight shift of the peak towards larger angles, i.e., ∼0.3° shift of the (311) peak.

3.3. FTIR-ATR spectroscopic analysis

Fig. 4a shows the FTIR-ATR comparison of the PAN/CoFe₂O₄, PAN/Fe₂O₃ and PAN reference samples. The significant broadening of the peak at ∼3620 cm⁻¹ may suggest interactions between the hydroxyl groups on the ferrite phase and the cyanoethyl groups (–CN triple bond) of PAN. Additionally, the spectra exhibited a wide absorption band between 3100–3600 cm⁻¹, which validates the interaction between the nitrile groups and Co²⁺ ions.³³ The peak observed around 2920 cm⁻¹ and a shoulder peak at ∼2860 cm⁻¹ accounts for the stretching vibrations of the –C–H bonds within the CH₂ groups of the PAN structure.³⁴ The FTIR spectrum of PAN reveals characteristic peaks at 2240 cm⁻¹, associated with the stretching vibrations of the –CN triple bond, indicating potential interactions between ferrite and polyacrylonitrile. The peak intensity decreases when Co₂Fe₂O₄ is added instead of Fe₂O₃, referring to the high interaction of this type of blend. PAN is polymerized in the presence of cobalt(II) salts. The peaks detected at approximately 1660 cm⁻¹ and 1450 cm⁻¹ are characteristic of pristine PAN nanofibers, corresponding to the –CO group in the amide structure and the –CN stretching vibrations, respectively.³⁵ C–H bending and CH₂ wagging are recorded at 1360 cm⁻¹, C–H wagging is at 1256 cm⁻¹, and C–C stretching of PAN polymer chain at 1070 cm⁻¹, and CH₂ rocking at 777 cm⁻¹.³⁶ The band at 538 cm⁻¹ is linked to the oscillation of Fe–O bonds.³⁷

New peaks are detected at 1540 and 1577 cm⁻¹ for the Co₂Fe₂O₄ interaction with the PAN compared to PAN itself and PAN/Fe₂O₃ nanofibers, clearly indicating above mentioned interaction of CN group, especially with cobalt (Fig. 4b). Table 1 indicates the comparison of the FTIR peaks 1450 cm⁻¹ to 2920 cm⁻¹ and 1662 cm⁻¹ to 2920 cm⁻¹. The areal ratio of absorbances of FTIR peaks (FTIR (A₂/A₁) CN/C–H) decreases in the order of PAN/CoFe₂O₄ < PAN/Fe₂O₃ < PAN owing to the varying extent of interaction of NPs with CN groups of PAN.

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C–H functionalization/activation reactions within a range of polymers using Fe₂O₃ or MFe₂O₄ (M: metal) containing oxide NPs were reported.³⁸ The Fe–O bonds in the NPs can participate in hydrogen bonding with the C–H bonds next to the cyanide (CN) bonds in PAN (see Fig. 6), where such non-covalent bonds are interactions between molecules or atoms that do not involve sharing electrons. Their importance lies in their ability to form weak yet specific interactions between molecules, which are crucial for many functions in living systems and materials. This type of interaction can contribute to forming a network between the NPs and PAN, decreasing the fiber dimensions and quenching their strength and elasticity.

3.4. Dynamic mechanical analysis

DMA results indicate the differences between the pure PAN sample at 0 mT and PAN/CoFe₂O₄ samples at 0, 40 and 100 mT externally applied field under 0.5 Hz (Fig. 5a). Even though no remarkable difference between the glass transition T_g points is observed for the PAN and PAN/CoFe₂O₄ samples at 0 mT, a large T_g shift by ∼15 K towards larger temperatures is observed by the application of an external magnetic field. The largest change is observed for the crystallization temperature T_x (from ∼587 K); there is a gradual rise in the storage modulus Y′ for the pure PAN sample, whereas a very steep rise from 50 MPa to 750 MPa was observed for the PAN/CoFe₂O₄ sample. The enhanced storage modulus observed in metal oxide-PAN fibers at high temperatures compared to pure PAN fibers is a result of the integration of metal oxide NPs. These NPs act as reinforcing agents, remarkably enhancing the mechanical properties of the composite material until 750 K, and the key factors contributing to this enhancement. Strong interfacial bonding facilitates the effective transfer of load from the polymer matrix to the NPs, thereby enhancing the overall stiffness of the composite.

Metal oxides can also enhance the thermomechanical stability of the PAN fibers. This increased thermal resistance can help sustain the mechanical attributes of the composite at higher temperatures (in the studied range) in comparison to the absence of metal oxide in PAN nanofiber, in contrast to our previous TGA data of PAN polymer and PAN NF under an inert (nitrogen) atmosphere.³⁹ The steepness of this rise attenuates to 350 MPa by the application of a 40 mT external field, but with a clear shift in T_x to 610 K. An early rupture of the sample below T_x was recorded for the PAN/CoFe₂O₄ sample under a 120 mT external field. The largest losses in modulus Y′′ are observed at T_g and T_x for the PAN/CoFe₂O₄ sample without the application of an external field, which is pronouncedly lower for the pure PAN sample. Compared to PAN/Fe₂O₃ at 0 mT reaching 800 K, the PAN/Fe₂O₃ under 120 mT is broken at 665 K before reaching the maximum Y′′ value. A clear comparison of the PAN (Fig. 5b) and PAN/CoFe₂O₄ (Fig. 5c) samples for three different frequencies of 0.5, 5 and 15 Hz was drawn. The activation energy E_a of each sample found from the T_g measurements at frequencies of 0.5, 5 and 15 Hz show distinct differences (Fig. 5d). A remarkable increase in E_a for the PAN/CoFe₂O₄ sample with the influence of magnetic field (from 299 ± 38 to 573 ± 62 kJ mol⁻¹) was recorded, meaning that the field can cause particle rearrangement or stiffening, restricting molecular motion and increasing E_a. This is also understood by the sharp stiffening observed for the magnetic nanoparticle containing PAN samples after T_x, except for the virgin PAN sample. The influence of homogenously dispersing only 5 wt% of ferrite-based NPs within PAN was also reflected in reaching full magnetic saturation with a well-defined sigmoidal shape, indicating a smooth magnetization reversal.^40,41

Fig. S2 (ESI†) shows the thermogravimetric analysis (TGA) of the electrospun PAN nanofibers produced in this study. The crystallization peak is at 561 K, where the crystallization leads to a weight loss of ∼37%. The second small peak at 704 K is related to the onset of degradation, as also confirmed by the onset of decrease in storage modulus in Fig. 5, with a further weight loss of ∼24%. The weight loss persists until the end of the measurement (1073 K), where compared to the initial state, a total weight loss of ∼70% was recorded.

In the former study, it was shown that PAN/MnZn Ferrite nanofibers show a more pronounced shift in T_g and T_x compared to PAN/Fe₂O₃, linked to the complex spinel structure of MnZn Ferrites with enhanced response to external magnetic field. PAN/CoFe₂O₄ shows a very similar increase in T_g (∼15 K) but with an earlier rupture with an applied magnetic field (120 mT). On the contrary, the molecular motions of PAN chains are more hindered or constrained in the presence of CoFe₂O₄ NPs than with MnZn ferrite (MnZn–Fe₂O₄), evidenced by the higher stiffness after exceeding the T_x when no external field was applied.²⁹

Along with the homogenous particle dispersion, finer nanofibers typically provide a higher surface area-to-volume ratio, leading to increased interfacial interactions within the matrix, which can enhance stiffness. Additionally, as also observed here, smaller fiber diameters restrict polymer chain mobility more effectively, which can lead to higher storage modulus and a shift in the glass transition temperature (T_g) toward higher values. Conversely, larger or irregularly distributed nanofibers may introduce defects or weak interfaces, reducing mechanical reinforcement and thermomechanical stability.^42,43

3.5. Magnetic property analysis

Alternative gradient field magnetometer (AGFM) shows a gradual and smooth magnetization with a complete magnetic saturation at 10 kOe. Table 2 depicts the magnetic property comparison of PAN/Fe₂O₃ and PAN/CoFe₂O₄. PAN/CoFe₂O₄ shows a lower saturation magnetization (M_s) and higher coercivity (H_c) accounted for by the stronger magnetocrystalline anisotropy.⁴⁴ In polymer composites, saturation magnetization (M_s) decreases for both CoFe₂O₄ and Fe₂O₃ due to magnetic dilution and spin disorder, while coercivity (H_c) generally decreases as well, though CoFe₂O₄ tends to retain higher Hc than Fe₂O₃ probably due to its intrinsic anisotropy.

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3.6. Possible interaction of ferrite nanoparticles with PAN

Ferrites can interact with PAN and undergo redox reactions with the CN group of PAN at possibly high temperatures. The CN groups in the polymer might act as reducing agents, reducing Fe₂O₃ to a lower oxidation state (i.e., FeO or Fe).⁴⁵ Within composite metal oxide layers, the interaction of molecules containing the CN group involves two primary mechanisms. Firstly, the π-electron system of the CN group can interact with the π-electron systems present in metal oxide clusters,⁴⁶ such as nanoparticles or nanowires. This interaction is favored by the electron-rich nature of the triple bond in the CN group, and these molecules can participate in redox reactions with species that have acquired electrons from the surrounding polymer matrix (Fig. 6). The mechanism of electron “capture” from the polymer matrix can vary and may involve processes like charge transfer complexes or electron transfer reactions. The specific characteristics of these interactions, including the type of metal oxide, the size and morphology of the clusters, and the properties of the polymer matrix, considerably impact the overall behavior of the composite material.

Stabilization (cyclization) of PAN during thermomechanical treatment in the presence of Fe₂O₃ NPs in PAN Nanofiber matrix was reported previously by our group.²⁹ Furthermore, the nanocatalytic behavior of iron nanoparticles is reported for reduction reactions.⁴⁷ A key step during this process was the association structures generated by the interaction of hydrogen bonds under heat treatment and the cyclization structures composed of CN bonds. The heat treatment process for PAN based carbon fibers critically relies on a chemical transformation known as the cyclization reaction, i.e., the cyclization reaction of PAN/Fe₂O₃ nanofiber (and for the PAN/Co Ferrite nanofibers as well), is promoted by the catalytic effect of Fe₂O₃ recorded during thermomechanical measurements.

4. Conclusion

The incorporation of metal oxide nanoparticles into PAN nanofibers significantly enhances their high-temperature properties, making them suitable for various advanced applications. These composite fibers exhibit improved thermomechanical stability, mechanical reinforcement in composites, and enhanced insulation properties due to the interaction between metal oxides and the CN groups in PAN ascertained by FTIR spectroscopy. The redox interactions between ferrites and PAN facilitate structural modifications, including cyclization, which is catalyzed by (cobalt) ferrites during thermomechanical processing.

Characterization techniques such as HRSEM, XRD, spectroscopy, and thermomechanical analysis confirm the well-dispersed nanoparticle distribution and strong interfacial interactions within the polymer matrix. Compared to Fe₂O₃, the globally and homogeneously dispersed Co-ferrite NPs ensured by XRD and SEM-EDX imaging demonstrate superior thermomechanical stability by shifting the glass transition temperature towards higher values, thereby improving the overall thermal performance of the nanocomposite.

Furthermore, PAN/CoFe₂O₄ NFs exhibit promising electrochemical properties, making them viable for energy storage applications, including supercapacitors and oxygen evolution reaction (OER) electrocatalysis. Optimizing the morphology and surface area of cobalt ferrite NPs can further enhance their electrochemical activity by increasing the density of active sites.

These findings underline the multifunctional potential of PAN/CoFe₂O₄ nanofibers, which makes them strong candidates for integration into next-generation energy storage systems, flexible electronic devices, and high-temperature composite materials. Future work should focus on tailoring the NP architecture—through size control, doping strategies, or template-assisted synthesis—to further improve performance. Additionally, scaling up fabrication methods and assessing long-term operational stability will be essential steps toward translating these materials into practical, industrial applications.

Conflicts of interest

There are no conflicts to declare.

Data availability

The data supporting this article have been included as part of the ESI.†

Acknowledgements

This article is based upon work from COST Action NanoSpace CA21126 and COST Action COSY CA21101, supported by COST (European Cooperation in Science and Technology).

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Footnote

† Electronic supplementary information (ESI) available. See DOI: https://doi.org/10.1039/d5ma00349k

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