A. Apparao et al., Depth of detection of highly conducting and volume polarizable targets using induced polarization, GEOPHYS PR, 48(5), 2000, pp. 797-813
We define the apparent frequency effect in induced polarization (IP) as the
relative difference between apparent resistivities measured using DC excit
ation on the one hand and high-frequency excitation (when the IP effect van
ishes) on the other. Assuming a given threshold for the minimum detectable
anomaly in the apparent frequency effect, the depth of detection of a targe
t by IP can be defined as that depth below which the target response is low
er than the threshold for a given electrode array. Physical modelling shows
that for the various arrays, the depth of detection of a highly conducting
and volume polarizable target agrees closely with the depth of detection o
f an infinitely conducting and non-polarized body of the same shape and siz
e. The greatest depth of detection is obtained with a two-electrode array,
followed by a three-electrode array, while the smallest depth of detection
is obtained with a Wenner array when the array spread is in-line (i.e. perp
endicular to the strike direction). The depth of detection with a Wenner ar
ray improves considerably and is almost equal to that of a two-electrode ar
ray when the array spread is broadside (i.e. along the strike direction).