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The conventional methods for fabricating flexible dielectric materials with high electrical energy densities are introducing zero-, one-, and three-dimensional high-k inorganic nanofiller into a dielectric polymer matrix while less two-dimensional high-k nanofillers were included. Herein, two-dimensional 2D high-k titanium dioxide nanosheets prepared by a one-step hydrothermal reaction were utilized to boost the energy storage performance of dielectric polymer nanocomposites.

It was found that compared with the polymer matrix the nanocomposites not only exhibit an enhanced dielectric constant but also show suppressed dielectric loss, which is desirable for energy storage applications. Finite element simulation was conducted to study the electric field distribution in nanocomposites with different shapes of nanofillers. Furthermore, the comparison of the current nanocomposites and previous reported nanocomposites with 0D, 1D, and 3D nanofillers shows that the 2D high-k nanofiller exhibited superior potential in advancing the energy storage nature of polymer nanocomposites.

The new band at nm is observed after addition of SiO 2 with the decrease in the UV—visible regions with shift toward longer wavelength.

Dielectric Breakdown Strength of Polymer Nanocomposites-The Effect of Nanofiller Content

The investigation of the absorption spectra is a method to study and more data for the materials structure. The changes in the absorption radiation lower to higher energy state can decide kinds transitions of the electron. The optical energy gap E g for direct and indirect transitions can be calculated by equations as following [27,28] :.

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The optical gap E g. The estimated values of E g are decreased from 4. This behavior is a general trend of dielectrics materials as a polymer that can be understood by polarization which created related to the ionic exchange of the number of ions by locally displacing in the applied field direction. The dielectric constant for the polymer is created due to the dipolar, electronic, ionic, and interfacial polarizations. At lowest frequency, there is a charge accumulation at the interface causing contributions for various interfacial polarizations are watched.

The discussion of this behavior is that at a certain point, the space charges cannot support and comply with the outside field which causes a decrease in the polarization and there is no charge accumulation at the interface. At low frequencies, dielectric constant and dielectric loss depend on the presence of ion center type of polarization in the films and to the interfacial polarization.

The dielectric constant is high at the low frequency that might be because of space charge polarization. It is because obstructing of charge carriers at the electrodes due to confinement to their movement at the interface. Likewise, we can observe the dielectric dispersion at low frequencies.

Bibliographic Information

From the figure, the curves give a semicircular arc which deviate its movement with changes and variations occurring with increase of silica contents. The behavior of the semi-circular curve can be display and explain the kind of the electrical process existing in the samples where the impedance arc is bent to characterized by the formation of the curves.

The intersection with Z o axis represents the sample bulk resistance. The semicircles in the plot can be correlated with Debye type relaxation. The plots further show a decrease in impedance with the increase in silica content.. The blend of chitosan Cs and polyacrylamide PAM doped low concentrations of silica nanoparticles SiO 2 was prepared and investigated using different techniques.

No changes in the position of the IR bands after incorporation of SiO 2 nanoparticles. The UV—vis absorption spectra were measured as a function of wavelength. The optical band gap Eg was calculated using the indirect transition forbidden transition. At low content of SiO 2 , the onset of the semicircles indicates that the impedance is very high. The author declares no conflicts of interest.. Journal of Materials Research and Technology. Open Access Option. Previous article Next article. Issue 2. Pages April Download PDF.

Dielectric Polymer Nanocomposites

Laila Hussein Gaabour a , b ,. Corresponding author. This item has received. Under a Creative Commons license. Article information.

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  • Show more Show less. The got nanocomposites show improved, optical, mechanical, thermal, electrical and optoelectronic properties [2]. At the point when chitosan is mixed with other polymers, the miscibility between the polymers is an extremely critical factor particularly for a mechanical property of the blend [9,10].

    The blends between polyacrylamide with other polymers are studied [13—16]. All the measurements are done in an evacuated system to eliminate the effect of moisture. Scheme 1.

    Dielectric Polymer Nanocomposites | J. Keith Nelson | Springer

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    Fundamentals, Properties, and Applications of Polymer Nanocomposites

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    Feng, Y. Liu, B. Zhao, K. Characterization of half N-acetylated chitosan powders and films. Proc Eng, 27 , pp. Cheung, T. Ng, J. Wong, W. Chitosan: an update on potential biomedical and pharmaceutical applications. Mar Drugs, 13 , pp. Pakravan, M. Heuzey, A. Polymer Guildf , 52 , pp. Moura, J. Mano, M.

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    Paiva, N. Chitosan nanocomposites based on distinct inorganic fillers for biomedical applications. Sci Technol Adv Mater, 17 , pp. Hu, Z. Zhang, Z. Lu, P. Li, S. Chitosan-based composite materials for prospective hemostatic applications. Sakurai, T. Maegawa, T. Polymer Guildf , 41 , pp.