Open Access Short Communication

Enhancement of Microwave Absorption Property of Polymer Blend using MXene

Pritom J Bora and Daniel Q Tan*

Technion Israel Institute of Technology and Guangdong Technion Israel Institute of Technology Shantou, China

Corresponding Author

Received Date: January 13, 2020;  Published Date: January 21, 2020

Abstract

2D MXene significantly enhances the microwave absorption properties of a polymer blend (PVB- PEDOT:PSS or PVBPS). For various military and civilian applications such as X-band (8.2–12.4 GHz) and Ku-band (12.4–18 GHz) absorption these materials are very important. The minimum reflection loss (RL)-53 dB was obtained for optimally prepared PVBPS- Ti3C2Tx MXene nanocomposite for thickness of 1.5 mm. A single 2 mm thick layer of PVBPS- Ti3C2Tx MXene nanocomposite shows the most promising absorption bandwidth (RL≤-10 dB from 8.2 to 18 GHz). Mechanistically, dielectric loss and interfacial polarization contribute more efficiently, and the stored energy becomes predominant in Ti3C2Tx MXene contained PVBPS blend which enhances the microwave absorption bandwidth.

Keywords: Polymer blend; Polymer nanocomposite; Mxene; Microwave absorption

Introduction

At present, the cutting edge telecommunication, healthcare systems, detective systems, military applications, etc. predominantly use microwave frequency [1-3]. The lightweight polymer nanocomposite microwave absorbing materials is increasingly felt due to the presence of electromagnetic threat [3- 4]. Polyvinyl butyral (PVB) based blend and nanocomposite has drawn special attraction for organic nanoelectronics as well as for microwave absorption due to many advantages such as lightweight, weather resistive, solution processability (facile coating), lower cost [2-6]. Two-dimensional (2D) nano materials are among the most promising materials for electromagnetic/device applications due to the better control of their properties at the atomic scale with high surface to volume ratio. A large family of 2D metal carbides and nitrides, called MXenes, have been proposed as one of the attracting absorption predominant electromagnetic interference (EMI) shielding materials particularly in microwave regions due to its light weight, superior electrical property and microstructure [7- 8]. MXenes have a general formula of Mn+1XnTx, where M represents a transition metal such as Ti, Zr, Hf, V, Nb, Ta, Cr, Mo, and X is carbon or nitrogen, and n= 1–3. The surface terminations, such as oxygen, fluorine, hydroxyl, always present on MXene surface, and they can be shown as Tx in the Mn+1XnTx formula [7-8]. The objective of this short communication is to investigate the microwave absorption property of facile prepared dielectric polymer blend (PVBPEDOT: PSS) incorporated with Ti3C2Tx MXene.

Results and Discussion

The Ti3C2Tx MXene was synthesized by the standard synthesis method [8], as shown by the schematic of the process in Figure 1 (a). The recorded FESEM images were shown in the Figure 1(bc). The facile preparation of PVB-PEDOT:PSS (PVBPS) blend was reported in our previous article [9]. In order to prepare MXene loaded PVBPS, Ti3C2Tx MXene was first dispersed in deionized water with a concentration 1 mg/ml. The Ti3C2Tx MXene suspension was then optimally added (3 ml) to the PVBPS solution (10 ml) followed by casting on a PET mold and drying for 24 h in open air (Figure 2).

The microwave absorption is understood in terms of reflection loss (RL), as given by Refs. [4-6],

Where, Z0 (=377 Ω) is the free space intrinsic impedance and 𝑀𝑎𝑡𝑒𝑟𝑖𝑎𝑙 𝑖𝑚𝑝𝑒𝑑𝑎𝑛𝑐𝑒, *

Where, irispublishers-openaccess-modern-concepts-material-science is the relative permittivity and permeability respectively. f is the frequency; d is the thickness of the composite material and c is the velocity of light. The RL value of -10 dB, which corresponds to 90 % absorption, is adequate for practical applications [9]. The RL of PVBPS blend was shown in Figure 2(a). The bandwidth for RL ≤ -10 dB of PVBPS blend was not found to increase significantly until the thickness was increased to 2 mm. Better RL was observed for Ku-band (12.4– 18 GHz) for a thickness of 1.5 mm. On the other hand, outstanding RL value of -53 dB was achieved for the

irispublishers-openaccess-modern-concepts-material-science
irispublishers-openaccess-modern-concepts-material-science

PVBPS- Ti3C2Tx MXene nanocomposite for the thickness of 1.5 mm as shown in Figure 2 (b). For thickness of 1.8 mm, a broad absorption bandwidth of 8.5–18 GHz was achieved with minimum RL value -35 dB. When thickness was increased to 2 mm, the absorption bandwidth of PVBPS- Ti3C2Tx MXene nanocomposite was found to increase 8.2-18 GHz (entire X-band and Ku-band). Thus, this work clearly demonstrates the enhancement of microwave absorption properties of PVBPS blend (in a much broader bandwidth) with the presence of Ti3C2Tx MXene. Mechanistically, dielectric loss and interface polarizations contribute more efficiently. This is because the charges in the interfaces in PVBPS- Ti3C2Tx MXene (either heterogeneous or homogeneous interface) can generate aggregation and the rearrangement. As a result, the polarization loss takes place, which has a significant impact on dielectric loss [10-11]. In addition, the associated functional groups of Ti3C2Tx MXene could generate dipolar interactions at multiple interfaces, and form capacitor-like structures [10-11]. Thus, it gave rise to an excellent electromagnetic energy absorption performance.

Conclusion

In the development of microwave absorption material, the use of 2D materials as a component in optimized polymer blends is a promising approach, as demonstrated by enhanced microwave absorption bandwidth in PVBPS- Ti3C2Tx MXene nanocomposite. A large bandwidth, 8.2–18 GHz, was achieved for the optimally prepared PVBPS- Ti3C2Tx MXene nanocomposite for the single 2 mm thick layer. The minimum RL value of -53 dB was achieved for 1.5 mm thick PVBPS- Ti3C2Tx MXene nanocomposite. PVBPSTi 3C2Tx MXene nanocomposite may present a tangible pathway for developing extremely efficient microwave absorption material in future.

Acknowledgment

Authors would like to thank Prof. Praveen C Ramamurthy (Dept. of Materials Engineering, IISc) and Prof. KJ Vinoy (Dept. of Electrical and Communication Engineering, IISc, India) for providing the lab facilities for microwave measurements and characterizations.

Conflict of Interest

No conflict of interest.

References

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