The resistance to current flow of minerals and partial-melts is a freq
uency dependent electrical property. Measurements of the frequency dep
endent electrical impedance of single crystal olivine, polycrystalline
olivine, dunites, metapelites, and partial-melts, between 10(-4) and
10(5) Hz, when plotted in the complex impedance plane, reveal arcs tha
t correspond to different conduction mechanisms in the material being
studied. In polycrystalline materials, two impedance arcs related to m
aterial properties (as opposed to electrode properties or electrode-sa
mple interactions) are observed. Each impedance arc is activated over
a distinct range of frequency, that is, the mechanisms occur in series
. Based on experiments comparing single and polycrystalline impedance
spectra, experiments on samples with different electrode configuration
s, and on samples of varying dimension, the mechanisms responsible for
these impedance arcs are interpreted as grain interior conduction (si
gma(gi)), grain boundary conduction (in polycrystalline materials; sig
ma(gb)), and sample-electrode interface effects, from highest to lowes
t frequency, respectively. Impedance spectra of natural dunitic rocks
reveal analogous behavior. that is, sigma(gb) and sigma(gi) add in ser
ies. The grain boundaries do not enhance the conductivity of any of th
e materials studied (a direct result of the observed series electrical
behavior) and, under certain conditions, limit the total conductivity
of the grain interior-grain boundary system. By examining the frequen
cy dependence of the electrical properties of partial-melts, it is pos
sible to gain information about microstructure and the distribution of
the melt phase and to determine the conditions under which the presen
ce of melt enhances the total conductivity. Impedance spectra of olivi
ne-basalt partial-melts indicate that at least two conduction mechanis
ms occur in series over the frequency range 10(-4)-10(5) Hz, similar t
o the observed electrical response of melt-absent polycrystalline mate
rials. In a sample containing isolated melt pockets the intermediate f
requency grain boundary impedance arc is modified by the presence of m
elt indicating series conduction behavior. In a sample with an interco
nnected melt phase the high frequency grain interior impedance arc is
modified by the melt phase, indicating the initiation of parallel cond
uction behavior. Because-field EM response versus frequency curves are
used to derive conductivity versus depth profiles, it is important to
perform laboratory experiments to understand the frequency-dependent
electrical behavior of Earth materials. Activation energies determined
from studies that measure conductivity at a single frequency may be e
rroneous because of the shift of the dominant conduction mechanism wit
h frequency as temperature is varied.