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Lightweight and high-strength polyarylene ether nitrile-based composites for efficient electromagnetic interference shielding

  • Jianfei Qin , Lifen Tong EMAIL logo , Liang He , Xiaobo Liu and Xiran Tang EMAIL logo
Published/Copyright: December 31, 2023
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Abstract

The proliferation of electronic devices and the widespread adoption of microwave-based technologies have resulted in a notable rise in electromagnetic radiation pollution. In present work, a novel flexible lightweight polyarylene ether nitrile (PEN)-based composite for efficient electromagnetic interference (EMI) shielding was prepared by introducing dual-loss hybrid material (PKMWCNT@Fe3O4) into PEN via non-solvent induce phase separation method and assembling it layer-by-layer with carbon fiber (CF) fabric. The porous morphology of the PEN layer, the electrical conductivity of the CF fabric, and the dual-loss property of the filler enable the material to reflect and absorb electromagnetic waves multiple times, resulting in superior electromagnetic shielding performance. With the addition of PKMWCNT@Fe3O4 at a mass fraction of 50%, the EMI SE T and specific shielding effectiveness SSE/t can reach up to 47.08 dB and 617 dB cm2/g, respectively, indicating absorption dominated shielding mechanism. Furthermore, the material exhibits a lightweight nature with a density of 0.55 g/cm3, and excellent mechanical properties, including a tensile strength of 43.98 MPa and elongation at break of 43.32%. This work presents a new approach to prepare high-performance composites that are both lightweight and resistant to secondary contamination by electromagnetic waves.

Graphical abstract

1 Introduction

Electromagnetic shielding functional materials play a vital role in addressing the issue of electromagnetic wave pollution in both military and civilian sectors [14]. As electronic devices and telecommunication systems continue to advance rapidly, electromagnetic interference (EMI) has become increasingly significant [5,6]. To mitigate the harmful effects of EMI, various shielding techniques have been developed, among which electromagnetic shielding materials offer an effective solution [7,8]. These materials are designed to attenuate or redirect electromagnetic waves, preventing them from interfering with nearby electronic devices. They have extensive applications in industries such as aerospace, telecommunications, automotive, and medical, where the reliable operation of electronic equipment is of utmost importance [911].

Electromagnetic shielding materials can be categorized based on their shielding mechanisms, including reflective shielding materials, absorptive shielding materials, scattering shielding materials, and multilayer composite shielding materials. Reflective shielding materials are conductive materials that achieve shielding by reflecting electromagnetic waves [12,13]. When electromagnetic waves interact with these materials, the free electrons within the material are excited by the electromagnetic field, generating opposing currents to counteract the energy of the incident waves [14,15]. Absorptive shielding materials absorb electromagnetic waves by converting their energy into other forms [1619]. These materials typically have good electromagnetic wave absorption capabilities, such as high dielectric loss or conversion of electromagnetic waves into heat energy [2023]. Scattering shielding materials utilize their unique structures and shapes to cause multiple reflections and scattering of electromagnetic waves on the material surface, achieving shielding through interference effects [24,25]. Multilayer composite shielding materials consist of a combination of different types of shielding materials in a layered structure [2628]. By designing different layers of material combinations, multiple mechanisms such as reflection, absorption, and scattering can be utilized to achieve better shielding effects [29,30].

Traditional metals and their alloys have limitations in electromagnetic shielding due to factors such as high weight, high cost, and poor corrosion resistance [31,32]. Therefore, polymer-based or carbon-based electromagnetic shielding materials are receiving increasing academic attention [3337]. Gao et al. presented a comprehensive review on graphene-based materials for electromagnetic shielding applications [24]. The authors discuss various design strategies at different scales, ranging from molecular to macroscopic levels, aiming to enhance the electromagnetic shielding performance of graphene-based materials. These design strategies encompass the incorporation of graphene at the molecular scale, the utilization of micro/nanostructures, the development of macrostructures, and the integration of design approaches for multiscale assemblies. Kong et al. conducted a study on the development of an electromagnetic shielding shape memory polyimide material [38]. In their research, they synthesized the material by incorporating 5% short carbon fibers (CFs) and 4% carbon black into a shape memory polyimide matrix. As a result, this composite material achieved an impressive average EMI shielding effect of 23.9 dB in the X-band, despite having a relatively thin thickness of 0.35 mm. Zhang et al. successfully fabricated flexible composite films comprising Ti3C2T x nanosheets embedded in an aramid nanofiber/polyvinyl alcohol (PVA) matrix [39]. This composite material exhibited an exceptional EMI shielding effectiveness of 70 dB, highlighting its remarkable capability to attenuate and block electromagnetic radiation. Zheng et al. innovatively created a lightweight polyurethane (PU) composite foam designed specifically for EMI shielding purposes [40]. Fe3O4@PVA and graphene oxide@silver were incorporated into a PU matrix, which facilitated the formation of an excellent network structure within the PU foam skeleton. This enhanced network structure significantly contributed to the overall EMI shielding effectiveness and mechanical performance of the composite foams.

Polyarylene ether nitrile (PEN) is a leading special engineering plastic that finds extensive applications in both civil and military sectors due to its favorable characteristics, including exceptional high-temperature resistance, impressive strength, elevated modulus, and remarkable corrosion resistance, etc. [4146]. In view of the excellent properties and processability of polyarylether nitrile, researchers have developed a series of functional composites. In view of the excellent properties and processability of PEN, researchers have developed a series of functional composites. Wang et al. fabricated an anti-bacterial robust Ag@PDA/PEN electrospinning nanofibrous membrane for oil–water separation by combining PEN with polydopamine (PDA) and Ag nanoparticles (NPs) [47]. He et al. prepared high-performance thermally conductive composites by introducing boron nitride nanosheets and benzocyclobutene into PEN [48]. In the present work, PEN is used as a carrier for electromagnetic shielding fillers, and a novel electric/magnetic dual-loss nanomaterials of multi-walled carbon nanotubes (MWCNT)@Fe3O4 hybrid material and CF are used as functional fillers. First, the MWCNT@Fe3O4 hybrid material was prepared using a co-precipitation method, which effectively suppresses the reflection of electromagnetic waves, thus enhancing the reliability and durability of the shielding system. Subsequently, the MWCNT@Fe3O4 hybrid material was introduced into PEN matrix, and assembled with CF fabric layer-by-layer. Lastly, the composites of PEN/MWCNT@Fe3O4/CF fabric were prepared with non-solvent induced phase separation method. The influence of different filler contents on structural morphology and comprehensive properties was studied, and the shielding mechanism of the PEN/MWCNT@Fe3O4/CF fabric composites was investigated, which will provide reference for the suitable designs of multifunctional PEN/CF fabric composites with adjustable structure and properties and provide a theoretical basis for the realization of a more efficient shielding effectiveness for the next-generation new composites.

2 Experimental

2.1 Materials

PEN was synthesized from our labs [42]. The carboxylated carbon nanotubes (MWCNT-COOH), dopamine hydrochloride, tris (hydroxy) aminomethane, N,N-dimethylacetamide (DMAc), FeCl2·4H2O, FeCl3·6H2O, NH3·H2O, KH550, glycerol, and anhydrous ethanol were purchased from Chengdu Kelong Chemical Reagents Co., Ltd (Chengdu China). The CF fabric used in the study was obtained from Yixing Zhongfu Carbon Fiber Products Co.

2.2 Preparation of PEN/CF electromagnetic shielding composites

2.2.1 Synthesis of PKMWCNT@Fe3O4 hybrid nanomaterials

PKMWCNT@Fe3O4 hybrid nanomaterials were synthesized as shown in Figure 1(a). First, dissolve FeCl2·4H2O (0.373 g) and FeCl3·6H2O (1.014 g) into 300 mL deionized water under the protection of N2 to form a homogeneous solution. Then, carboxylated carbon nanotubes (MWCNT-COOH, 0.3 g) was added under mechanical stirring at 300 rpm with ultrasonic treatment. After MWCNT-COOH was completely dispersed in the solution, the water bath was warmed up to 80°C and ammonia was added drop by drop until pH = 11. After reaction for 2 h, the MWCNT@Fe3O4 hybrid filler was collected with magnet, washed repeatedly with deionized water, and then freeze-dried for 48 h to obtain MWCNT@Fe3O4. Next, MWCNT@Fe3O4 (0.1 g), dopamine (DA, 40 mg), and KH550 (8 mg) were dispersed in 100 mL deionized water and adjusted the solution with Tris until pH = 8.5. The reaction was reacted at 300 rpm for 8 h under mechanical agitation and sonicated at room temperature. After completion of the reaction, these functionalized fillers were separated in a centrifuge, and were freeze-dried for 48 h after several washes and named as PKMWCNT@Fe3O4.

Figure 1 
                     Preparation of (a) hybridized nanomaterial PKMWCNT@Fe3O4 and (b) PEN/PKMWCNT@Fe3O4/CF composites.
Figure 1

Preparation of (a) hybridized nanomaterial PKMWCNT@Fe3O4 and (b) PEN/PKMWCNT@Fe3O4/CF composites.

2.2.2 Preparation of PEN/PKMWCNT@Fe3O4/CF composites

The preparation process of PEN/PKMWCNT@Fe3O4/CF composites is shown in Figure 1(b). About 0.18 g of PEN, 0.005 g of glycerol, and 1.8 ml of DMAc were mechanically stirred at 300 rpm for 5 h until completely dissolved and a homogeneous solution was formed, and then left to stand for 5 h to completely eliminate the air bubbles, and is named as solution A. Meanwhile, PKMWCNT@Fe3O4 nanomaterials were dispersed into 10 mL DMAc to form a homogeneous solution B with mechanical stirring at 300 rpm and ultrasonic treatment, and the concentrations were 0, 12.5, 25, and 50 wt%, respectively. Solution B was then mixed with solution A for 5 h to form solution C. Pour an appropriate amount of the above solution onto a flat and clean glass plate and use a wet film preparation apparatus to push out a 600 μm liquid film, followed by placing a washed 1 cm × 1 cm square CF fabric lightly on it and pouring an appropriate amount of solution to push out the liquid film again, changing the amount of CF fabric and solution according to actual needs. The glass plate and the liquid/solid multi-phase mixture were immersed in a deionized water coagulation bath. The sample fell off from the glass plate by themselves. Then it was continued to be immersed in deionized water for 24 h to displace solvents and obtain the wet state PEN/PKMWCNT@Fe3O4/CF complex. The above obtained wet state complexes were dried at 60°C for 24 h to obtain PEN/MWCNT@Fe3O4/CF composites. The samples were named as P mPKCFx C n , where m and n represent the number of layers of PEN and CF, respectively, PKCF represents PKMWCNT@Fe3O4 and x represents the mass percentage of PKMWCNT@Fe3O4 in the PEN layer.

2.3 Characterization

The structure of filler was characterized by infrared spectroscopy (Fourier transform infrared [FTIR]) using a Shimadzu 8400S infrared spectrometer with a wavelength of 4,000–400 cm−1. Field emission scanning electron microscopy (FE-SEM; Hitachi SU8010) was employed to characterize the microscopic morphology of the dual-loss filler and PEN/PKMWCNT@Fe3O4/CF composites. The EMI shielding effectiveness (SE) of the multilayered films was evaluated in the X-band frequency range of 8.2–12.4 GHz using a Keysight PNA Network Analyzer N5224B, which operated based on the coaxial method. By analyzing the scattering parameters (S11 and S21) obtained directly from the vector network analyzer, it was possible to calculate various EMI shielding parameters. Specifically, the power coefficients of reflectivity (R), transmissivity (T), and absorptivity (A) were calculated from the scattering parameters. Based on these values, the total EMI shielding effectiveness (SE T ), reflection (SE R ), absorption (SE A ), and multiple reflections (SE M ) were determined using the relevant equations [49]:

(1) R = | S 11 | 2 ,

(2) T = | S 21 | 2 ,

(3) A = 1 ( T + R ) ,

(4) SE T = 10 log ( 1 / T ) ,

(5) SE R = 10 log ( 1 / 1 R ) ,

(6) SE A = 10 log [ ( 1 R ) / T ] ,

(7) SE T = SE R + SE A + SE M .

Typically, the contribution of SE M can be disregarded when the SE T is equal to or greater than 15 dB [50]. The conductivity of composites was measured on a four-point probe resistivity determiner (RTS-8). The magnetic properties of the samples were evaluated using a vibrating sample magnetometer from Riken Denshi (BHV-525, USA). The mechanical properties of all samples were tested by a universal testing machine with a crosshead speed of 1 mm/min. Thermogravimetric analysis was performed on a TA-Q50 in a nitrogen atmosphere with a ramp rate of 20°C/min.

3 Results and discussion

3.1 PKMWCNT@Fe3O4 hybrids materials

The successful preparation of the hybrid CNT is verified using FTIR analysis. In Figure 2(a), all curves have a small peak at 1,565 cm−1, corresponding to the carbon skeleton of the carbon nanotubes [51]. Curve (a) shows a faint peak at 3,550 cm−1, which corresponds to the −OH of the carboxylate group on the MWCNT-COOH [52], and the small peak at 1,767 cm−1 corresponds to C═O. Curve (b) displays a distinct absorption peak at 611 cm−1, which represents the stretching vibration peak of Fe–O in Fe3O4 [53]. Curve (c) corresponds to the PKMWCNT@Fe3O4 nanomaterials, where the broad peak at 3,421 cm−1 corresponds to the stretching vibration of –OH and –NH–, and the absorption peak at 1,505 cm−1 corresponds to the bending vibration of –NH–. The characteristic peaks at 2,918 and 2,852 cm−1 correspond to the asymmetric stretching vibration and symmetric stretching vibration of methylene, respectively [54]. Based on these results, it is reasonable to infer that PKMWCNT@Fe3O4 and cross-linked core–shell structure PKMWCNT@ Fe3O4 nanohybrid materials have been successfully prepared. Figure 2(b) shows the XRD pattern of PKMWCNT@ Fe3O4. The diffraction peaks at 2θ = 18.7°, 30.3°, 35.8°, 43.4°, 53.8°, 57.2°, and 63.0° are attributed to (111), (220), (311), (400), (422), (511), and (440) (JCPDS No. 19-0629) crystal planes of spinel Fe3O4.

Figure 2 
                  (a) FTIR curves of MWCNT-COOH, MWCNT@Fe3O4, and PKMWCNT@Fe3O4. (b) XRD pattern of PKMWCNT@Fe3O4.
Figure 2

(a) FTIR curves of MWCNT-COOH, MWCNT@Fe3O4, and PKMWCNT@Fe3O4. (b) XRD pattern of PKMWCNT@Fe3O4.

The SEM images demonstrate the microscopic morphology of the hybridized particles. Specifically, Figure 3(a)–(c) shows the morphologies of pristine MWCNT-COOH, MWCNT@Fe3O4, and PKMWCNT@Fe3O4, respectively, at a magnification of 160,000. From Figure 3(b), it is evident that carbon nanotubes are grown with nearly spherical particles, which is precisely Fe3O4 microspheres grown in situ on active sites of carbon tubes, and these microspheres have diameters ranging from 30 to 50 nm. Also, Figure 3(c) shows the microscopic morphology of the PKMWCNT@Fe 3 O 4 , and it can be seen that the spherical particles on these carbon nanotubes are slightly fuller and the surface is also slightly rougher compared to MWCNT@Fe3O4. This difference is attributed to the cross-linking reaction between DA and KH550 on the surface of MWCNTs, leading to the wrapping of PKMWCNT@Fe3O4. Hence, the SEM results can further demonstrate the successful preparation of hybrid PKMWCNTs fillers.

Figure 3 
                  SEM images of (a) MWCNT-COOH, (b) MWCNT@Fe3O4, and (c) PKMWCNT@Fe3O4.
Figure 3

SEM images of (a) MWCNT-COOH, (b) MWCNT@Fe3O4, and (c) PKMWCNT@Fe3O4.

Figure 4 is the hysteresis loops of hybrid materials. It can be seen that both are typical soft magnetic materials. The saturation magnetization intensity (Ms) of the MWCNT@Fe3O4 nanomaterial is higher than that of the PKMWCNT@Fe3O4. The Ms of former is 34.03 emu/g, while the latter is 24.80 emu/g. Since dopamine hydrochloride and KH550 cross-link on the surface of magnetic carbon nanotubes to form a polymer shell, the mass share of Fe3O4 in the whole PKMWCNT@Fe3O4 is reduced.

Figure 4 
                  Hysteresis loops of MWCNT@Fe3O4 and PKMWCNT@Fe3O4.
Figure 4

Hysteresis loops of MWCNT@Fe3O4 and PKMWCNT@Fe3O4.

3.2 PEN/PKMWCNT@Fe3O4/CF composites

The chemical structure of P4PKCFx C3 composites is investigated using FTIR. As depicted in Figure 5, an absorption peak with weak intensity is identified at 2,230 cm−1 in all the samples’ structures, corresponding to the stretching vibration of –CN of PEN [42,44]. Stronger absorption peaks are present at 1,457 and 1,576 cm−1, corresponding to vibrations of the inner backbone of the PEN, while a prominent absorption peak observed at approximately 1,206 cm−1 can be attributed to the stretching vibration of the aryl ether bond (Ar–O–Ar) present in the backbone structure [44]. With the exception of P4PKCF0C3, the other three materials show a small shoulder peak at 1,626 cm−1, indicating the presence of both C═N stretching vibration and aromatic ring vibration overlap [55]. The presence of C═N is evidence of a Schiff base or Michell addition reaction between dopamine and KH550.

Figure 5 
                  FTIR curves of P4PKCFx
                     C3 composite materials.
Figure 5

FTIR curves of P4PKCFx C3 composite materials.

Due to the characteristics of high strength of CF, there are some difficulties in studying the microscopic morphology of PEN/PKMWCNT@Fe3O4/CF composites cross-section, and only the PPKCFx layer was investigated. Figure 6(a)–(d) shows SEM images of PPKCFx layers at filler ratios of 0, 12.5, 25, and 50 wt%, in turn, at a scale rule of 200 μm. It is observed that the PEN films obtained using the method of non-solventogenic phase separation have finger-like pores with a pore diameter of about 20 μm, which promotes the advantage of light-weight and low-density. With the increase of filler content, the shape and diameter of the pores does not change significantly. However, the increase in filler content leads to a decrease in the compatibility of the phases within the porous membrane, and agglomeration of the PKMWCNT@Fe3O4 is observed inside the pores, which was particularly evident at 50 wt% addition.

Figure 6 
                  The SEM images of the PPKCFx. (a) PPKCF0; (b) PPKCF12.5; (c) PPKCF25; (d) PPKCF50; (e) PPKCF0; (f) PPKCF12.5; (g) PPKCF25; (h) PPKCF50.
Figure 6

The SEM images of the PPKCFx. (a) PPKCF0; (b) PPKCF12.5; (c) PPKCF25; (d) PPKCF50; (e) PPKCF0; (f) PPKCF12.5; (g) PPKCF25; (h) PPKCF50.

Fe3O4 is introduced into the composite material to impart magnetic properties to the material, which facilitates the absorption of electromagnetic waves, thereby improving the electromagnetic shielding effectiveness of the material. The magnetic properties of the P PKCFx layer and the P4PKCFx C3 composite are tested separately. From Figure 7(a), the saturation magnetization intensity of P PKCFx layer increases with the increase of magnetic filler content, and the saturation magnetization intensity of P PKCF12.5, P PKCF25, and P PKCF50 are 3.10, 5.46, and 8.15 emu/g, respectively. Also, the trend of composites is consistent with P PKCFx layer, and the M s of P4PKCF12.5C3, P4PKCF25C3, and P4PKCF50C3 are 0.47, 0.92, and 1.37 emu/cm3, respectively (Figure 7b). These findings suggest that incorporating PKMWCNT@Fe3O4 into the composites imparts magnetic properties to them. Additionally, the inclusion of a magnetic polymer layer can enhance magnetic loss, leading to improved electromagnetic shielding effectiveness. This contributes to the development of an absorption-based shielding mechanism, which effectively reduces secondary electromagnetic pollution.

Figure 7 
                  (a) and (b) Hysteresis loops of PPKCFx
                      and P4PKCFx
                     C3, (c) electrical conductivity of P4PLCFx
                     C3 composite, and (d) thickness and density of P4PkCFx
                     C3 composites.
Figure 7

(a) and (b) Hysteresis loops of PPKCFx and P4PKCFx C3, (c) electrical conductivity of P4PLCFx C3 composite, and (d) thickness and density of P4PkCFx C3 composites.

The conductivity of the four composites are presented in Figure 7(c). When the PEN matrix resin is not introduced in the modified carbon nanotubes, the composite exhibits a conductivity of 1.10 S/cm. Compared with the pure PEN matrix resin, this increase in electrical conductivity is mainly attributed to the asymmetric conductive network built by the CF in the composite, which leads to a significant improvement in electrical properties. When the functionalized carbon nanotubes are introduced, the PEN layer also forms a corresponding conductive network and the electrical properties of the composites are further improved. With the increase of the conductive filler content, P4PKCF12.5C3, P4PKCF25C3, and P4PKCF50C3 exhibit a gradual increase of electrical conductivity. The conductivity values are 1.44, 1.67 and 1.90 S/cm, respectively. This result highlights a significant positive correlation between the electrical conductivity of the composites and the amount of conductive filler doping, which is closely linked to the excellent electrical conductivity of PKMWCNT@Fe3O4. The increased presence of PKMWCNT@Fe3O4 in the material leads to a higher interconnection of conductive particles within the matrix, further improving the electrical conductivity network and resulting in a gradual increase in electrical conductivity [56]. The increase in conductivity of the composite material contributes to more dielectric loss of electromagnetic waves in the interior, which is crucial for the large improvement of shielding performance.

From Figure 7(d), the thicknesses of P4PKCF0C3, P4PKCF12.5C3, P4PKCF25C3, and P4PKCF50C3 are all around 0.128 cm with negligible variations, which is consistent with the SEM results above: the pore size and thickness of the PEN layer are not significantly related to the filler content, which again proves that the material prepared by this method has a high macroscopic morphology. Meanwhile, the density of these samples slightly increases to 0.542, 0.544, 0.546, and 0.550 g/cm3, respectively. This indicates that a lightweight composite material was successfully prepared.

The electromagnetic shielding effectiveness is determined by the frequency of electromagnetic waves and the electromagnetic properties of the shielding material. Therefore, studying the effect of filler content on the electromagnetic shielding performance of composites is crucial. Figure 8(a)–(c) shows the SE T , SE R , and SE A curves for the four materials, respectively. It is clear that except for P4PKCF0C3, the EMI SE T (Figure 8a) of the other three materials remains basically stable throughout the X-band without any significant fluctuation. The maximum SE T of P4PKCF0C3 in this X-band is 18.5 dB, which is a great improvement in shielding efficiency compared with the almost completely wave-transparent pure PEN film, which is the result of the introduction of carbon fabric into the substrate. Besides, the content of PKMWCNT@Fe3O4 is an important factor in determining its electromagnetic shielding performance. With the increase in nanoparticles, the shielding effectiveness of the material also increases. The SE T values of P4PKCF12.5C3, P4PKCF25C3, and P4PKCF50C3 in this band are up to 34.04, 42.56, and 47.08 dB, respectively, which fully meet the requirements of commercial shielding materials. It can be attributed to the enhancement of electrical and magnetic properties caused by the addition of this double loss type of filler, resulting in more conductive losses within the material to dissipate the electromagnetic waves. Figure 8(b) shows that although the SE T of P4PKCF0 is the lowest, its SE R is not lower than the other three materials, and is even higher than the other three materials when the frequency is higher than 10.5 GHz. The changes of SE A values of the four materials (Figure 8c) are consistent with the trends of SE T values. The highest SE A value of P4PKCF50C3 is 45.54 dB, and the SE R value at the corresponding frequency is only 1.57 dB.

Figure 8 
                  EMI SE data of P4PKCFx
                     C3 composites: (a) SE
                        T
                     , (b) SE
                        R
                     , (c) SE
                        A
                     , (d) SE
                        A
                     /SE
                        R
                     , (e) A(eff), and (f) A, R coefficient percentage.
Figure 8

EMI SE data of P4PKCFx C3 composites: (a) SE T , (b) SE R , (c) SE A , (d) SE A /SE R , (e) A(eff), and (f) A, R coefficient percentage.

The SE A /SE T , A(eff), and the percentage values of A and R coefficients are calculated to further investigate the electromagnetic screening mechanism. Figure 8(d) displays that the SE A /SE T ratio of composites increased with the content of PKMWCNT@Fe3O4 hybrid materials increasing, and values of P4PKCF0C3, P4PKCF12.5C3, P4PKCF25C3, and P4PKCF50C3 are 0.53, 0.78, 0.92, and 0.97, respectively, which represents that the introduction of magnetoelectric dual-loss nanoparticles helps to enhance the overall performance of the material and strengthen the interaction with the incident waves, thus facilitating the absorption of electromagnetic waves inside the material and improving the absorption efficiency to reduce the secondary pollution of electromagnetic waves. Meanwhile, the results of A(eff) also show that the increase in filler content increases the absorption and shielding efficiency of the materials (Figure 8e). The A(eff) of the four materials is 0.797, 0.996, 1.000, and 1.000, respectively. It means that when A(eff) is close to 1 the content of PKMWCNT@Fe3O4 in the PEN layer is 25 wt%. This is a reflection of the high absorption efficiency of this type of shielding material. In addition, the large A and R percent ratios calculated results are recorded in Figure 8(f). It shows that the influence of filler content on the shielding effect is also well illustrated by the A and R ratios calculated, where the material A-factor percentage increases and the R-factor percentage decreases with the increasing content of PKMWCNT@Fe3O4. When the filler content is 50 wt%, the A/R ratio of the material is 73/27. This reveals the difference between the reflective and absorptive efficiency of the material and proves its absorption-driven shielding mechanism in P4PKCF50C3 sample.

To sum up, the above data indicate that the electromagnetic shielding effectiveness can be effectively adjusted by the content of this magnetoelectric dual-loss PKMWCNT@Fe3O4 nanoparticle. Also, the conductivity as well as magnetic properties of the material are improved due to the increase of fillers. This is mainly due to the conductive losses caused by the interaction of a large number of free electrons in the matrix with electromagnetic waves, while eddy current losses due to the magnetic properties of this type of carbon nanotubes can also enhance the shielding effectiveness of the material. Specifically, a large number of free electrons within the composites form electrical energy under the action of incident electromagnetic waves, which is then converted into thermal energy. Second, due to the in situ growth of Fe3O4 particles on the carbon nanotubes, very small interfaces are formed between them. The introduction of Fe3O4 particles into PEN layer causes the formation of more interfaces in the porous layer, which helps to enhance the interfacial polarization and thus energy dissipation.

Figure 9 shows the trend of electrical conductivity, saturation magnetization strength, and shielding effectiveness of P4PKCFx C3 composite materials. It can be seen that EMI SE increases continuously with the increase of conductivity. This change is mainly due to the presence of a large number of free electrons in the material that interact with electromagnetic waves and dissipate the electromagnetic waves. The EMI SE of the composite also increases with its saturation magnetization strength. The variation trend shows a certain correlation with the saturation magnetization intensity. The results indicate that the hybridized PKMWCNT@Fe3O4 plays an important role in enhancing both conductivity and magnetism, proving that it is a double-loss type of filler, which contributes to the improvement of electromagnetic shielding performance in the composites. In this work, the porous morphology of the PEN layer, the electrical conductivity of the CF cloth, and the dual-loss property of the filler make the material reflect and absorb the electromagnetic wave many times, so that the material has superior electromagnetic shielding performance. The introduction of magnetic fillers allows the material to have a high shielding effectiveness even at low conductivity value.

Figure 9 
                  Trend of electrical conductivity, saturation magnetization strength, and shielding effectiveness of P4PKCFx
                     C3 composite materials.
Figure 9

Trend of electrical conductivity, saturation magnetization strength, and shielding effectiveness of P4PKCFx C3 composite materials.

Based on the provided information, the mechanism of the material can be summarized as shown in Figure 10. The PEN and CF layers have distinct roles in the process. Electromagnetic waves are dissipated within the PEN magnetic layer through hysteresis loss, eddy current loss, and interface polarization [57,58]. Between the CF layers, the dissipation of electromagnetic waves mainly occurs through conductive losses and interfacial polarization. In addition, the unique structure of the material contributes to enhanced shielding effectiveness in several ways. The magnetic PEN layer’s dielectric constant near the air allows electromagnetic waves to smoothly enter the material and be effectively consumed. Additionally, the porous structure of the PEN layer generates interfacial polarization, which further aids in dissipating electromagnetic waves. Furthermore, the impedance mismatches within the alternating multilayers of PEN and CF lead to multiple reflections of electromagnetic waves [59]. As a result, the PEN layer experiences hysteresis and eddy current losses, while the CF layer incurs conductive losses. These characteristics enable the composites to effectively follow an absorption-based shielding mechanism.

Figure 10 
                  Diagram of the electromagnetic shielding mechanism of P4PKCFx
                     C3 composite materials.
Figure 10

Diagram of the electromagnetic shielding mechanism of P4PKCFx C3 composite materials.

Figure 11 shows the calculated SSE/t values for the P4PKCFx C3 composites. This value increases with filler content increasing, and the SSE/t values for P4PKCF0C3, P4PKCF12.5C3, P4PKCF25C3, and P4PKCF50C3 are 177, 446, 534, and 617 dB cm2 g−1, respectively. It is clear that these composites have lower density and better SSE/t.

Figure 11 
                  SSE/t data of P4PKCFx
                     C3 composite materials.
Figure 11

SSE/t data of P4PKCFx C3 composite materials.

Table 1 presents key parameters of the P4PKCFx C3 composite. Results confirm that the composite has a stable thickness with the advantages of low density and high efficiency. This favorable performance can be primarily attributed to the ideal combination of the multilayer and porous structure of the PEN and the magnetoelectric double-loss type filler. Furthermore, the utilization of low-cost CF fabric as the conductive framework not only meets the standards set by the commercial industry but also offers excellent cost-effectiveness. This is in contrast to carbon/polymer composites prepared with alternative fillers like monolayer graphene, which tend to be more expensive.

Table 1

Critical data of P4PKCFx C3 composite materials

Sample Thickness (mm) Density (g/cm3) EMI-SE (dB) SSE/t (dB cm2 g−1)
P4PKCF0C3 1.283 0.542 12 177
P4PKCF12.5C3 1.282 0.544 31 446
P4PKCF25C3 1.282 0.546 37 534
P4PKCF50C3 1.282 0.550 44 617

To be practical, composite materials also need to have excellent mechanical strength. The mechanical strength of the material directly affects the life and reliability of the material. Table 2 lists the mechanical properties of P4PKCFx C3 varied as a function of filler content. Specifically, the tensile strength of P4PKCF0C3 is 42.54 MPa, which is 3,198% higher than that of the pure porous PEN film [60]. In addition, as the PKMWCNT@Fe3O4 content gradually increases from 12.5 to 50 wt%, the composites exhibit tensile strengths of 46.62, 44.57, and 43.98 MPa, respectively. This is the advantage of the good inherent properties of the CF. When the porous PEN structure is damaged during stretching, the interwoven strong CF are not affected and the composite can be further stretched until the interwoven structure of the CF is broken. Even if the original interwoven structure is destroyed, the composite still can be extended, so the material shows a large elongation at break. Take for instances, the elongation at break of P4PKCF12.5C3 is as high as 46.62%. Therefore, the inclusion of CF not only imparts high mechanical strength to the composite but also greatly improves its toughness.

Table 2

Critical mechanical data of P4PKCFx C3 composite materials

Sample Elongation at break (%) Tensile strength (MPa) Tensile modulus (GPa)
P4PKCF0C3 44.82 42.54 4.778
P4PKCF12.5C3 46.62 46.62 4.869
P4PKCF25C3 44.57 44.57 4.687
P4PKCF50C3 43.32 43.98 4.749

4 Conclusion

This work studied the effect of magnetoelectric double-loss PKMWCNT@Fe3O4 and CF on the electromagnetic shielding performance of PEN composites. The homogeneous distribution of PKMWCNT@Fe3O4 within the PEN phase, combined with the alternating multilayer structure formed by CF, effectively creates a continuous conductive network. As a result, the material exhibits high conductivity (1.90 S/cm) and good saturation magnetization strength (M s = 1.37 emu/cm3), synergistically enhancing the shielding effectiveness with a high SE T value of 47.08 dB. Furthermore, the SE A /SE T is 97%, indicating that the material predominantly follows an absorption-dominated shielding mechanism. At the same time, the use of NIPs imparts a porous structure to PEN layer in the material, significantly reducing the density of the material down to 0.54 g/cm3. Even with the addition of high content of PKMWCNT@Fe3O4, the functional PEN composites maintain high mechanical properties. Therefore, this lightweight and high-performance PEN composite material is anticipated to find extensive applications in the electromagnetic shielding field.

  1. Funding information: This project was supported by the National Natural Science Foundation of China (Grant no. 52073039).

  2. Author contributions: All authors have accepted responsibility for the entire content of this manuscript and approved its submission.

  3. Conflict of interest: The authors state no conflict of interest.

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Received: 2023-09-18
Revised: 2023-11-05
Accepted: 2023-11-14
Published Online: 2023-12-31

© 2023 the author(s), published by De Gruyter

This work is licensed under the Creative Commons Attribution 4.0 International License.

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  96. Solid lipid nanoparticles for targeted natural and synthetic drugs delivery in high-incidence cancers, and other diseases: Roles of preparation methods, lipid composition, transitional stability, and release profiles in nanocarriers’ development
  97. Critical review on experimental and theoretical studies of elastic properties of wurtzite-structured ZnO nanowires
  98. Polyurea micro-/nano-capsule applications in construction industry: A review
  99. A comprehensive review and clinical guide to molecular and serological diagnostic tests and future development: In vitro diagnostic testing for COVID-19
  100. Recent advances in electrocatalytic oxidation of 5-hydroxymethylfurfural to 2,5-furandicarboxylic acid: Mechanism, catalyst, coupling system
  101. Research progress and prospect of silica-based polymer nanofluids in enhanced oil recovery
  102. Review of the pharmacokinetics of nanodrugs
  103. Engineered nanoflowers, nanotrees, nanostars, nanodendrites, and nanoleaves for biomedical applications
  104. Research progress of biopolymers combined with stem cells in the repair of intrauterine adhesions
  105. Progress in FEM modeling on mechanical and electromechanical properties of carbon nanotube cement-based composites
  106. Antifouling induced by surface wettability of poly(dimethyl siloxane) and its nanocomposites
  107. TiO2 aerogel composite high-efficiency photocatalysts for environmental treatment and hydrogen energy production
  108. Structural properties of alumina surfaces and their roles in the synthesis of environmentally persistent free radicals (EPFRs)
  109. Nanoparticles for the potential treatment of Alzheimer’s disease: A physiopathological approach
  110. Current status of synthesis and consolidation strategies for thermo-resistant nanoalloys and their general applications
  111. Recent research progress on the stimuli-responsive smart membrane: A review
  112. Dispersion of carbon nanotubes in aqueous cementitious materials: A review
  113. Applications of DNA tetrahedron nanostructure in cancer diagnosis and anticancer drugs delivery
  114. Magnetic nanoparticles in 3D-printed scaffolds for biomedical applications
  115. An overview of the synthesis of silicon carbide–boron carbide composite powders
  116. Organolead halide perovskites: Synthetic routes, structural features, and their potential in the development of photovoltaic
  117. Recent advancements in nanotechnology application on wood and bamboo materials: A review
  118. Application of aptamer-functionalized nanomaterials in molecular imaging of tumors
  119. Recent progress on corrosion mechanisms of graphene-reinforced metal matrix composites
  120. Research progress on preparation, modification, and application of phenolic aerogel
  121. Application of nanomaterials in early diagnosis of cancer
  122. Plant mediated-green synthesis of zinc oxide nanoparticles: An insight into biomedical applications
  123. Recent developments in terahertz quantum cascade lasers for practical applications
  124. Recent progress in dielectric/metal/dielectric electrodes for foldable light-emitting devices
  125. Nanocoatings for ballistic applications: A review
  126. A mini-review on MoS2 membrane for water desalination: Recent development and challenges
  127. Recent updates in nanotechnological advances for wound healing: A narrative review
  128. Recent advances in DNA nanomaterials for cancer diagnosis and treatment
  129. Electrochemical micro- and nanobiosensors for in vivo reactive oxygen/nitrogen species measurement in the brain
  130. Advances in organic–inorganic nanocomposites for cancer imaging and therapy
  131. Advancements in aluminum matrix composites reinforced with carbides and graphene: A comprehensive review
  132. Modification effects of nanosilica on asphalt binders: A review
  133. Decellularized extracellular matrix as a promising biomaterial for musculoskeletal tissue regeneration
  134. Review of the sol–gel method in preparing nano TiO2 for advanced oxidation process
  135. Micro/nano manufacturing aircraft surface with anti-icing and deicing performances: An overview
  136. Cell type-targeting nanoparticles in treating central nervous system diseases: Challenges and hopes
  137. An overview of hydrogen production from Al-based materials
  138. A review of application, modification, and prospect of melamine foam
  139. A review of the performance of fibre-reinforced composite laminates with carbon nanotubes
  140. Research on AFM tip-related nanofabrication of two-dimensional materials
  141. Advances in phase change building materials: An overview
  142. Development of graphene and graphene quantum dots toward biomedical engineering applications: A review
  143. Nanoremediation approaches for the mitigation of heavy metal contamination in vegetables: An overview
  144. Photodynamic therapy empowered by nanotechnology for oral and dental science: Progress and perspectives
  145. Biosynthesis of metal nanoparticles: Bioreduction and biomineralization
  146. Current diagnostic and therapeutic approaches for severe acute respiratory syndrome coronavirus-2 (SARS-COV-2) and the role of nanomaterial-based theragnosis in combating the pandemic
  147. Application of two-dimensional black phosphorus material in wound healing
  148. Special Issue on Advanced Nanomaterials and Composites for Energy Conversion and Storage - Part I
  149. Helical fluorinated carbon nanotubes/iron(iii) fluoride hybrid with multilevel transportation channels and rich active sites for lithium/fluorinated carbon primary battery
  150. The progress of cathode materials in aqueous zinc-ion batteries
  151. Special Issue on Advanced Nanomaterials for Carbon Capture, Environment and Utilization for Energy Sustainability - Part I
  152. Effect of polypropylene fiber and nano-silica on the compressive strength and frost resistance of recycled brick aggregate concrete
  153. Mechanochemical design of nanomaterials for catalytic applications with a benign-by-design focus
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