Maxwell-wagner effect and strong low-frequency dispersion

1 October 1983

conference paper
Published by Institute of Electrical and Electronics Engineers (IEEE)

p. 479-485
https://doi.org/10.1109/ceidp.1983.7736427

Abstract

The dielectric properties of dipolar materials are well understood in terms of the “universal” many-body approach developed by the Chelsea Group [1–4], with the characteristic power-law frequency dependence of the complex susceptibility above the loss peak frequency ωp given by: X(ω) = ∊(ω) − ∊∞ ∝ [1 + i cot(nπ/2)] ωⁿ⁻¹ (1) where the exponent falls generally in the range 0 < n < 1.

Keywords

DISPERSION
GLASS
MEDIA
DIELECTRIC LOSSES
FREQUENCY DEPENDENCE
RESISTANCE

This publication has 0 references indexed in Scilit: