High-Temperature Lightweight Ceramics with Nano-sized Ferrites for EMI Shielding: Synthesis, Characterization, and Potential Applications

1. Introduction

Radiation fields from electronic devices like antennas, phones, and household appliances cause electromagnetic interference (EMI). Shielding sensitive electronics from EMI is challenging for aircraft, military, and communication system components [1]. Efforts to combat EMI involve developing shielding systems for intentional or unintentional interference. However, using metallic materials for EMI shielding is becoming difficult due to the trend toward smaller and lighter electronic packaging [2].

Industry traditionally use electrically conductive metals for EMI shielding, but their high density and susceptibility to corrosion lead to heavyweight shielding components. To address this, researchers have turned to low density materials like polymers, which have poor electrical conductivity and EMI shielding. Two approaches are used to prepare polymer shields: coating with conductive metals or blending with conductive fibers and particles [3]. Researchers have attempted to reinforce transparent polymers with conductive fillers like carbon nanofibers [4,5], carbon nanotubes [6], graphene [7,8], and metallic nanowires and particles [9,10]. Syntactic foams are lightweight composite materials with hollow particles dispersed in a polymer matrix that offer weight-saving potential and are being explored for their EMI shielding effectiveness [11].

The development of lightweight and mechanically robust porous or cellular materials is one of the current trends in modern materials design. In recent years, the use of cenospheres (CS) for manufacturing porous lightweight composite materials has been extensively investigated. CS is three-dimensional objects with a spherical shape that contains a cavity or empty spaces inside. These materials are chemically multicomponent systems with SiO₂-Al₂O₃-Fe₂O₃ content of about 90 wt.% [12,13,14]. Due to their low apparent density (0.40-0.72 g·cm^-3), low thermal conductivity (about 0.065 W·m^-1·K^-1), and excellent stability in alkaline solutions and at high temperatures, cenospheres are a promising raw material for the development of new porous materials. The particle size of cenospheres ranges from about 40 up to 500 µm [15,16].

The civil engineering industry widely applies CS in producing lightweight concrete with improved thermal insulation [14,17]. CS also takes filler and reinforcement roles in metal-matrix [18,19,20] and polymer-matrix [20,21] composites. However, researchers rarely report results of CS containing low-density ceramic-matrix composites. However, interest in ceramic-cement composites has gained in recent years, and researchers have reported some stunning results.

CS exhibit reliable sintering tendencies while maintaining their spherical shape, yet they do not possess the ability to form durable structures. Therefore, adding a second phase, which promotes the adhesion of the material, can improve its mechanical strength. In addition, various additives can promote sintering, e.g., metals, oxides, or other additives. For example, one way to enhance sintering could be using oxides, e.g., ferrite nanoparticles [22].

Cobalt ferrite (CoFe₂O₄) has excellent chemical stability, mechanical hardness, and electrical insulation. On the other hand, it is a hard magnetic material, and its magnetic properties exhibit size dependence. Therefore, using CoFe₂O₄ nanoparticles (NP) in composite production could have a positive effect. In addition, the spinel structure of CoFe₂O₄ allows the introduction of different metallic ions into its lattice, thus altering the structural, magnetic, electrical, and catalytic properties [23]. It has many applications, such as magnetic data storage, hybrid electric vehicles, transformer core, high-frequency integrated inductors, biocompatible magnetic fluids, magnetic resonance imaging, and controlled drug delivery. Other industries also implement CoFe₂O₄ in manufacturing microwave-absorbing paints, catalysis, hybrid supercapacitors, and products of different applications [24,25]. The remarkable magnetic properties, such as high coercivity (H_C), magneto crystalline anisotropy constant (K), Curie temperature ( T_C), moderate saturation magnetization (M_S) and remanent magnetization (Mr), high magnetostriction coefficient (λ), and low eddy current losses, along with excellent chemical and mechanical stability, electrical resistance, optical and dielectric properties, low toxicity [26,27,28,29], and impressive mechanical hardness, present CoFe₂O₄, as a good candidate for producing syntactic foams with CoFe₂O₄.

CoFe₂O₄ nanoparticles have been used as standalone materials and incorporated with other materials, such as polymers and carbon-based materials, to improve their magnetic properties. There is significant literature describing the various material design methods and applications of these materials, including EMI shielding, catalysts, and magnetism-related applications [30,31,32,33,34,35,36,37]. Spinel CoFe₂O₄ prepared by sol-gel assisted sintering at 1150 °C by Caldeira et. al. [38], exhibited Vicker’s hardness of 133.9. Hollow CoFe₂O₄ spheres on carbon template have been prepared for high wave absorption by Zhou et. al. [39]. A porous lightweight nano composite of CoFe₂O₄ and graphene oxide was prepared by Liu et. al. [40] that displayed high microwave absorption [23].

For use in real-life EMI shielding applications, it is necessary that the material has sufficient mechanical strength and low density. In the aerospace industry has additional requirements to the materials - is to withstand high-temperatures (up to 1000 °C). But most of the EMI shielding materials mainly made of (or contain) polymer materials [41] which decomposes at 250-350 °C, or contain graphite or graphene [41] which burn out at 350-450 °C.

In this study, the preliminary investigation into the formability and structural integrity of a novel CS-CoFe₂O₄ composite foam has been conducted. With the incorporation of CoFe₂O₄ nanoparticles in CS matrix, a lightweight, high-temperature ceramic material capable of electromagnetic wave absorption can be produced. Generally, a high-performance absorber must possess strong absorptivity, low density, broad absorption frequency, and thin thickness to satisfy the requirements of actual applications [42,43,44]. The effect of sintering temperature and Compaction Pressure (CP) on the mechanical properties is investigated. This article also demonstrates the effect of CoFe₂O₄ nanoparticles as an additive for the sintering of CS while improving magnetic properties [24,25]. The authors studied two ceramic types: pure CS and CS-based ceramics with CoFe₂O₄ addition. The following characterisation methods, materials, and sintering approach demonstrate the effect of applied compressive pressure, sintering temperature, and the amount of added ferrite on the density and properties of ceramics. This paper investigates and discusses material mechanical strength, porosity and density. Based on these observations, the recipe with the best properties combination will be used in further EMI absorber design and study.

2. Materials and Methods

2.1. Materials

The authors selected mullite-based CS (Biotecha SIA, Latvia) [15] with two different particle size distributions, 63 – 150 μm (CS2) and 150 – 250 μm (CS1). An optical image and the representative XRD spectrum of as received CS2 is shown in Figure 1a and 1b, respectively. The authors have provided a more detailed description of selected CS properties in one of their previous publications [15]. The mullite-based CS exhibit exceptional mineral mechanical strength and chemical corrosion resistance. Their robustness makes them ideal for applications requiring durability and resilience in high-temperature and corrosive environments. The specific sintering temperature and pressure required to maintain the hollow nature of mullite-based CS while sintering them into a single object can vary depending on various factors, including the composition of the cenospheres and the desired final properties. However, in general, a typical sintering temperature range for mullite-based CS is around 1200 to 1600 °C. The pressure applied during the sintering process can vary but is often conducted under atmospheric pressure or in a low-pressure environment to avoid collapsing the hollow structure.

CoFe₂O₄ nano powder with an average particle size of 40 nm was prepared by high-frequency plasma chemical synthesis [45]. This process produced nanoparticles of different sizes (Figure 2a) and their XRD spectrum (Figure 2b) matches the peaks of CoFe₂O₄ obtained using the chemical co-precipitation method [46].

These nanoparticles can be sintered completely at 1100-1200 °C [47], forming a compacted material. The electromagnetic properties of pure CoFe₂O₄ material are shown in Figure 3. A small additive of nanoparticles can create a connective network between the cenospheres, improving the strength of the structure. The ceramic engineer made compositions with CoFe₂O₄ content from 0 to 20 wt.%. Therefore, the authors expect the lowered required sintering temperature to produce CS-based ceramic materials with CoFe₂O₄ nanoparticle additives [15].

Table 1. Magnetic properties of CoFe₂O_4.

Ferrite	Magnetic properties
	Ms, emu/g	Mr, emu/g	Hc, Oe
CoFe2O4	75.4	32.0	780

Table 1. Magnetic properties of CoFe₂O_4.

Ferrite	Magnetic properties
	Ms, emu/g	Mr, emu/g	Hc, Oe
CoFe2O4	75.4	32.0	780

2.2. Sintering process

The flowchart of the methodology used for the research is shown in Figure 4. Sintering was performed at 1100–1300 °C in an LHT-08/18 furnace (Nabertherm GmbH) in an air atmosphere with a heating rate of 10 °C·min^-1 and a residence time at the maximum temperature of 1h. The CP of the samples was 25-125 bar. Cylindrical sample size ᴓ=12 mm and h=10 mm. Samples with dimensions of 65 x 65 x 9 mm were made for determining the mechanical properties.

2.3. Applied Characterization Methods

An operator employed an Advance D8, Bruker AXS X-ray diffraction (XRD) analysis system with Cu-Ka radiation, utilising the ICDD database PDF-4 + 2008, PDF-4/Organics 2008, and Sleve+2008 software, to characterise the phase composition of raw materials and sintering products. An operator used Hitachi S4800 and Mira/Tescan scanning electron microscopes (SEM) to evaluate the morphology and microstructure of CS and produced ceramic composites. In addition, researchers conducted optical imaging using a Keyence VHX-2000 digital optical microscope equipped with VH-Z20R/W and VH-Z500R/W lenses.

Furthermore, the TEM JEM-100S "JEOL" was employed to analyse the nanoparticle microstructure. The laboratory assistant used the Archimedes method to determine the bulk density, apparent porosity, water absorption, and apparent specific gravity of the sintered samples. The technician conducted compressive and bending strength tests using the ToniNorm Tinius Olsen 25ST apparatus. The magnetic properties of the manufactured materials were analysed using vibrating sample magnetometry (VSM) with Lake Shore Cryotronics Inc., model 7404 VSM.

Apparent density and porosity were determined by the Archimedes method at 20 °C, using a distilled water as liquid media for immersing.

3. Results and Discussion

Most of the studies have been carried out using cenospheres CS1 with sphere size in the range of 150-250 μm ((Figure 7, Figure 8, Figure 10, Figure 12 and Figure 13), as well as using cenosphere CS2 (Figure 5, Figure 9 and Figure 11). The results show that as the sintering temperature increases, the density of the material increases due to decrease in the content of moisture and apparent porosity by consolidation of material. Similar trend was observed with increasing CP used for producing of samples. In all sintering modes, regardless of the size of the ferrite nanoparticle additive, as the CP of the samples increases, the density of the material increases, and apparent porosity of the material decreases. Density of a cellular material has a positive impact on its mechanical response. Similar relationship between density and compressive strength was observed in this study as well. Various concentrations of ferrites were used in the composite material: 0 wt. % (CS1-0, CS2-0), 7.5 wt. % (CS1-7.5 and CS2-7.5), 10 wt. % (CS1-10, CS2-10) and 20 wt. % (CS1-20). In all these variants, it was seen that as the concentration of ferrite nanoparticles increases, the density of the material increases, irrespective of the sintering temperature. With increasing density (decreasing porosity) the compressive strength of the materials also increases.

For the range of sintering parameters used in the study (p = 50 bar to 125 bar, t = 1100 °C to 1300 °C, CoFe₂O₄ content from 0 to 20 wt.%), samples with density of 1.19-2.16 g·cm^-3 and a compressive strength of 1.5 – 125 MPa were obtained.

Composition CS2-0 (without CoFe₂O₄) sintered at 1100 °C and compacted at all studied CP range (25-125 Bar), has very low strength (below 1 MPa) (Figure 5).

This fact could be explained by low CS particles adhesion to each other due to low (1100 °C) temperature. As described in previous research [15], this type of CS has good thermal stability (no softening, no shrinkage below 1250 °C. This is clearly seen on the Figure 6, where is seen area’s cross section decrease of CS1, started from 1250 °C.

Figure 6. CS1 and CS2 high-temperature optical dilatometry curves in the 50-1325 °C temperatures interval, adopted from [15]. Reprint on CC BY, 4.0 Open Access licence from [15].

Figure 6. CS1 and CS2 high-temperature optical dilatometry curves in the 50-1325 °C temperatures interval, adopted from [15]. Reprint on CC BY, 4.0 Open Access licence from [15].

The same weak particles adhesion to each other noticed for specimens sintered at 1200 °C and CP 25 bar. At the same time, other specimens series: sintered at 1300 °C (CP=25 ÷ 125 bar), and at 1200 °C, (by except CP=25 bar) demonstrate significant enough mechanical strength. As can be seen on Figure 5, increasing sintering temperature from 1100 to 1200 °C, in average compressive strength increase for 20 MPa. It is interesting to note that density of the CS2 -0 sintered materials increase gradually (and porosity has reverse dependence, which is logically, but also gradually) in all studied sintering temperatures and CP. The mechanical properties increases drastically by increasing the sintering temperature from 1100 to 1200 and to 1300 °C - average increase for 20 MPa per 100 °C. This is could be explained by CS softening, as result a better compaction, what also supported by high-temperature optical dilatometry curves (Figure 6). But CP brings a much smaller contribution into mechanical properties for the samples CS2-0, comparing with the sintering temperature: 2-3 MPa for 1200 °C and 3-6 MPa for 1300 °C.

Composition CS1-0 demonstrate quite similar dependences, but demonstrate slightly higher compression strength of series sintered at 1100 °C, than the same series of CS2-0. Sintered at 1100 °C and compacted at all studied CP range (25-125 bar), has very low strength (below 3 MPa) (Figure 7). The same weak particles adhesion to each other noticed for specimens sintered at 1200 °C and CP 25 bar. At the same time, other specimens series: sintered at 1300 °C (CP=25 ÷ 125 bar), and at 1200 °C, (by except CP=25 bar) demonstrate significant enough mechanical strength.

Figure 7. Ceramic apparent density, apparent porosity and compressive strength depending on CP and sintering temperature for CS1-0.

Figure 7. Ceramic apparent density, apparent porosity and compressive strength depending on CP and sintering temperature for CS1-0.

Series with CoFe₂O₄ has lower porosity’s value for average 10% (for CS1) and 7% (for CS2) (Figure 8 and Figure 9). This is obvious, due to interparticle voids filling by CoFe₂O₄ NP. Filling the voids by NP also leads to increasing contact points spots of CS particles, which lead to increase of mechanical properties of the material. Specimens series CS1-7.5 and CS2-7.5 (with 7.5 wt.% of CoFe₂O₄) in all CP and sintering temperature studied ranges characterises by higher compressive strength average for 30 MPa in comparison without CoFe₂O₄ addition. The overall tendency of the influence of the of CP on the compressive strength is the same as for CS without NP it is gradually in-crease.

Figure 8. CS1-7.5 porous ceramics with 7.5 wt. % of CoFe₂O₄ apparent density, apparent porosity and compressive strength depending on CP and sintering temperature.

Figure 8. CS1-7.5 porous ceramics with 7.5 wt. % of CoFe₂O₄ apparent density, apparent porosity and compressive strength depending on CP and sintering temperature.

Figure 9. CS2-7.5 porous ceramics with 7.5 wt. % of CoFe₂O₄ apparent density, apparent porosity and compressive strength depending on CP and sintering temperature.

Figure 9. CS2-7.5 porous ceramics with 7.5 wt. % of CoFe₂O₄ apparent density, apparent porosity and compressive strength depending on CP and sintering temperature.

Similar regularities are also determined for materials with a ferrite content of 10 wt%. (Figure 10 and Figure 11). Comparing the results obtained using cenospheres with a size of 150-250 μm (CS1) and 63-150 μm (CS2), it can be concluded that the size of the cenospheres does not significantly affect the sintering results – bulk density and apparent porosity. As known from [15], at temperatures above 1200 °C, cenospheres begin to plastically deform (Figure 6), which can explain the significant increase in sample density for samples sintered at 1300 °C, compared to samples sintered at temperatures of 1100 or 1200 °C. The plastic deformation leads to consolidation of the material by reduction of inter particle voids without the particle getting broken.

Figure 10. CS1-10 porous ceramics with 10 wt.% of CoFe₂O₄ bulk density, apparent porosity and compressive strength depending on CP and sintering temperature.

Figure 10. CS1-10 porous ceramics with 10 wt.% of CoFe₂O₄ bulk density, apparent porosity and compressive strength depending on CP and sintering temperature.

Figure 11. CS2-10 porous ceramics with 10 wt.% of CoFe₂O₄ bulk density, apparent porosity and compressive strength depending on CP and sintering temperature.

Figure 11. CS2-10 porous ceramics with 10 wt.% of CoFe₂O₄ bulk density, apparent porosity and compressive strength depending on CP and sintering temperature.

The nature of the samples with 20% ferrite additives (Figure 12) is similar to the samples with a smaller amount of ferrite additives: the density and compressive strength of the samples increase with the increase of pressing pressure and sintering temperature. Higher ferrite addition increases both material density and compressive strength.

Figure 12. CS1-20 ceramics with 20 wt.% of CoFe₂O₄ bulk density, apparent porosity and compressive strength depending on CP and sintering temperature.

Figure 12. CS1-20 ceramics with 20 wt.% of CoFe₂O₄ bulk density, apparent porosity and compressive strength depending on CP and sintering temperature.

The relationship between ferrite NP content, CP, apparent density, and compressive strength for CS1 is shown in Figure 13. There is a clear relationship between the material's apparent density (red curves) and compressive strength (blue curves) and ferrite concentration - with the increase in ferrite concentration, the apparent density and compressive strength also increase. Apparent density and compressive strength increase monotonically as CP increases.

Figure 13. Effect of CoFe₂O₄ concentration on the apparent density and compressive strength of cenosphere CS1 ceramics (sintering temperature 1200 °C.

Figure 13. Effect of CoFe₂O₄ concentration on the apparent density and compressive strength of cenosphere CS1 ceramics (sintering temperature 1200 °C.

The relationship between ceramic apparent density (a), compressive strength (b) and CP and sintering temperature for CS1-7.5 and CS2 -7.5 is shown in Figure 14. As can be seen from Figure 14, the density of the samples grows monotonically with increasing com-paction pressure and does not depend on the size of the used cenospheres. In contrast to samples sintered at 1100 and 1200 °C, the density of samples sintered at 1300 °C is significantly higher, which could be related to the pronounced plastic deformation of ceno-spheres at this temperature. On the other hand, the compressive strength of samples sintered at 1300 °C is significantly higher for CS1 (150-250 μm) samples than for CS2 samples.

Figure 14. Ceramic relative density (a) and compressive strength (b) depending on CP and sintering temperature for CS1-7.5 and CS2 -7.5.

Figure 14. Ceramic relative density (a) and compressive strength (b) depending on CP and sintering temperature for CS1-7.5 and CS2 -7.5.

Analysis of X-ray phases (Figure 14) shows that in the case of cenospheres and CoFe₂O₄ ceramics, their partial interaction takes place - mullite partially decomposes: Al₂O₃ enters the structure of CoFe₂O₄, while SiO₂ precipitates as a separate phase. The presence of the SiO₂ phase in sintered samples can also be partly explained by the crystallization of amorphous SiO₂ on the cenospheres.

Figure 14. Phase composition of ceramic (a) CS1–10 sintered at 1200 °C and (b) CS1-20 sintered at 1300 °C.

Figure 14. Phase composition of ceramic (a) CS1–10 sintered at 1200 °C and (b) CS1-20 sintered at 1300 °C.

Scanning electron microscopy is used to study the structure of materials. To test the strength of the cenospheres, individual samples were pressed at a higher pressure (250 bars). SEM images (Figure 16 and Figure 17) show that in the case of pure cenosphere ceramics, the ce-nospheres are either partially or fully crushed. The formation of mullite needles on the surface of the cenospheres can be observed in the SEM images of the sintered samples of cenospheres (CS1 and CS2) (Figure 16). At a CP of 250 bars, almost all spheres are destroyed (Figure 17). In well-sintered (1300 °C) CS1 samples at low CPs (25-50 bar), many cenospheres are intact (Figure 18).

Figure 15. At a temperature of 1200 °C sintered CS1-0 cenospheres (CP 250 bar).

Figure 15. At a temperature of 1200 °C sintered CS1-0 cenospheres (CP 250 bar).

Figure 16. At a temperature of 1200 °C sintered CS1-0 cenospheres (CP 250 bar).

Figure 16. At a temperature of 1200 °C sintered CS1-0 cenospheres (CP 250 bar).

Figure 17. At a temperature of 1300 °C sintered CS1-0 cenospheres (CP 25 bar).

Figure 17. At a temperature of 1300 °C sintered CS1-0 cenospheres (CP 25 bar).

The addition of CoFe₂O₄ improves sintering and mechanical strength, so the spheres are less crushed (Figure 19). In compositions of cenospheres with CoFe₂O₄, most of the spheres are healthy (Figure 20. (the image was taken with an optical microscope)). Ferrite particles cover the cenospheres, thus increasing the density of the material and improving the mechanical properties

Figure 18. Microstructure of ceramic CS1–20 sintered at 1300 °C (CP 25 bar).

Figure 18. Microstructure of ceramic CS1–20 sintered at 1300 °C (CP 25 bar).

Figure 19. Magnetization hysteresis of CS1 nanocomposites with CoFe₂O₄ nanoparticles sintered at 1200 °C. CoFe₂O₄ = 7.5 (1), 10 (2), 20 (3).

Figure 19. Magnetization hysteresis of CS1 nanocomposites with CoFe₂O₄ nanoparticles sintered at 1200 °C. CoFe₂O₄ = 7.5 (1), 10 (2), 20 (3).

Figure 20. Microstructure of ceramic CS1 – 20 sintered at 1300 °C (CP 25 bar).

Figure 20. Microstructure of ceramic CS1 – 20 sintered at 1300 °C (CP 25 bar).

As a result of research, the optimal CP for samples of the given size is 25-75 bar.

The mechanical properties (compressive and bending strength) of some samples depending on CP, sintering temperature and concentration of ferrites are given in Table 2. For this purpose, plates 65x65x9 mm were made, from which samples were cut to determine compressive strength (10x10x9 mm) and bending strength (10x9x60 mm).

As can be seen from Table 2, a geometric factor can be observed - the density of cylindrical tablets obtained under the same conditions (temperature, CP) is higher than that of large plates. Compared to small-sized samples (in our case, the surface area of the small samples perpendicular to the compaction direction was 1 cm²), the surface area of the plates exceeds 40 cm². Therefore, in a small volume, the material compresses more and the initial density at the same CP is higher.

Figure 19 shows the hysteresis loop magnetization (σ) as a function of applied magnetic field (H) for the three CS1 samples sintered at 1200 °C. The values of saturation magnetization Ms, remanent magnetization Mr and coercivity Hc are listed in 3. The coercivity (H_c) of the ceramics with various ferrite content was 275 Oe. But as the ferrite content increases, the saturation magnetization (M_s) and remnant magnetization (M_r) of the ceramics also increase. The M_s value for ceramics with 7.5, 10, and 20 % ferrite was 6.93, 2.78, and 2.04 emu/g, respectively, and M_r values are 2.3, 1.0, and 0.65 Oe, respectively. It shows that the soft magnetic properties are improved with increasing ferrite content. Soft magnetism is indicative of low volume resistivity and better EMI shielding as observed in FeCoNi coated carbon fibers [48], and CI/Ti3C2Tx/PVDF multilayer structured composite films [49].

The coercivity of a material dictates its magnetization capacity. If it is high, the material stays magnetized for long and vice versa. For CoFe₂O₄ nanoparticles sintered at, the coercivity was reported to be 188.57 Oe at room temperature [50]. Compared to the pure CoFe₂O₄, the ceramic and ferrite material studied in this study had a higher value of coercivity of 275 Oe, which suggests that some hardening in the ferromagnetic properties of the material is detected. Although, it is important to note that while for CS1 ferrite, sintered at 1200 °C, the coercivity is the same, it is higher for CS2 at the same sintering temperature. Typically, it is the higher the coercivity of the materials does not.

The electromagnetic properties (saturation magnetization Ms, remanent magnetization Mr and coercivity Hc) of the material increase in direct proportion to the concentration of ferrite nanoparticles in the material (Table 3, Figure 21 and Figure 22).

Increasing the CP and sintering temperature contributes to the sintering of the material and the increase in mechanical strength, both in the case of pure cenosphere ceramics and in the composition with CoFe₂O₄. As SEM images show, in the case of pure cenosphere ceramics, the cenospheres are partially or completely destroyed, depending on the CP. Low CPs should be used to preserve the closed pore structure as much as possible. But then the mechanical strength of the material is not great. The addition of CoFe₂O₄ nanoparticles significantly improves the sinterability of ceramics even at low CPs, allowing to obtain highly porous ceramics with good mechanical strength. X-ray phase analysis (Figure 15.) shows that in the case of cenospheres - CoFe₂O₄ ceramics, there is a slight interaction between them - mullite partially decomposes: Al₂O₃ enters the structure of CoFe₂O₄, while SiO₂ precipitates as a separate phase.

The electromagnetic properties of the material are enhanced in direct proportion to the concentration of ferrite nanoparticles in the material.

4. Conclusions

Lightweight high-temperature ceramics material with an ferromagnetic shielding effect were obtained by conventional pressure-sintering method using cenosphere and CoFe₂O₄ nanoparticles. Additives of ferrite nanoparticles improve the sintering of cenospheres, increasing the density of the material and increasing the mechanical properties. The porous structure of the samples largely depends on the CP of the samples: at CPs of 25-75 bars, whole cenospheres are largely preserved in the sample; at higher CPs, there is significant crushing of cenospheres, a decrease in porosity and an increase in density. Depending on the sample CP and sintering temperature, samples with a density of 1.2-2.1 g/cm³ and a compressive strength of 1.5-125.0 MPa were obtained. The bending strength of the obtained samples is determined within 10 - 20 MPa. The magnetic properties of the samples change in proportion to the amount of CoFe₂O₄ in the sample.