Abstract:
The dispersion of dielectric permittivity in nanocrystalline cellulose–triglycine sulfate composites is studied in the range of frequencies from 10$^{-3}$ to 10$^6$ Hz, at temperatures varying from room temperature to the temperature of phase transition in this composite (54$^{\circ}$C), in weak electric fields (1 V cm$^{-1}$). Two behaviors for the dielectric dispersion are identified in the studied frequency range: at ultralow frequencies (10$^{-3}$–10 Hz), the dispersion is due to Maxwell–Wagner polarization, while at higher frequencies (10–10$^6$ Hz), the dispersion is due to the movement of domain walls in the embedded triglycine sulfate crystallites. An additional peak in the temperature-dependent profiles of dielectric permittivity is detected at lower temperatures in freshly prepared samples of the considered composite; we associate it with the presence of residual water in these samples.
Citation:
N. H. Thu'O'Ng, A. S. Sidorkin, S. D. Milovidova, “Dispersion of dielectric permittivity in a nanocrystalline cellulose–triglycine sulfate composite at low and ultralow frequencies”, Fizika Tverdogo Tela, 60:3 (2018), 553–559; Phys. Solid State, 60:3 (2018), 559–565
\Bibitem{ThuSidMil18}
\by N.~H.~Thu'O'Ng, A.~S.~Sidorkin, S.~D.~Milovidova
\paper Dispersion of dielectric permittivity in a nanocrystalline cellulose--triglycine sulfate composite at low and ultralow frequencies
\jour Fizika Tverdogo Tela
\yr 2018
\vol 60
\issue 3
\pages 553--559
\mathnet{http://mi.mathnet.ru/ftt9278}
\crossref{https://doi.org/10.21883/FTT.2018.03.45561.256}
\elib{https://elibrary.ru/item.asp?id=32739819}
\transl
\jour Phys. Solid State
\yr 2018
\vol 60
\issue 3
\pages 559--565
\crossref{https://doi.org/10.1134/S1063783418030320}
Linking options:
https://www.mathnet.ru/eng/ftt9278
https://www.mathnet.ru/eng/ftt/v60/i3/p553
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