Widely used equations for the analysis of dispersive relaxation data f
or conducting materials, developed by Moynihan and associates more tha
n two decades ago, are shown to be require correction. Corrected equat
ions which can differ appreciably in their consequences from those of
Moynihan et al. are derived and used to justify the empirical Barton,
Nakajima, Namikawa (BNN) formula satisfied by much frequency-response
data for disordered materials. The conductive-system frequency-respons
e analysis described in the paper and the corrected Moynihan approach
both allow arbitrary fitting models to be used. It is shown that, for
one class of models, the two fitting approaches are identical and yiel
d maximum information while, for other models, the fit information is
intrinsically more limited and inaccurate. Improved methods for invert
ing transient-response data to yield the associated distribution of re
laxation times and frequency response are compared with the approach M
oynihan et al. used for the fractional-exponential fitting model (KWW)
, and a misconception in their work is corrected. Correct and incorrec
t ways to invert frequency-response data that include the effects of a
high-frequency-limiting dielectric constant are illustrated for KWW r
esponse. The conventional KWW model yields physically unrealizable tim
e and frequency responses, but a modification which restores realizabi
lity is developed. Analysis approaches are described which allow one t
o identify the type of dispersed behavior present in the data: either
conductive- or dielectric-system response. Weighted, complex-non-linea
r-least-squares analyses of frequency-response data for Li2O-Al2O3-2Si
O(2) glass at 24 degrees C using an approximate KWW fitting model are
compared with earlier fitting results of the same data obtained by Moy
nihan and others using the Moynihan et al. equations and fitting appro
ach. Excellent fits were obtained over the entire measured frequency r
ange when the fitting model included elements accounting for electrode
polarization effects in the data. These effects are shown to make non
-negligible contributions at both extremes of the frequency-response r
ange. Such contributions, and the past use of the Moynihan approach, p
robably explain most previously unexplained excess losses found presen
t in the high frequency region, ones which Moynihan and associates cha
racterized as endemic to the vitreous state.