A SIMPLE DERIVATION OF SEIGEL'S TIME DOMAIN INDUCED POLARIZATION FORMULA *
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It is advantageous to postulate the phenomenological equivalence of chargeability with a slight increase in resistivities rather than a similar reduction in the conductivities. Substitution of these increments in the expression for the total differential of apparent resistivity leads directly to Seigel's formula. Included also are (i) an equally simple demonstration that, for a homogeneously chargeable ground with arbitrary resistivity distribution, the apparent chargeability ma, equals the true homogeneous value m, and (ii) a direct derivation of the completely general resistivity relation
where the symbols have the usual meanings.
[1] D. Patella. A NEW PARAMETER FOR THE INTERPRETATION OF INDUCED POLARIZATION FIELD PROSPECTING (time‐domain) * , 1973 .
[2] F. S. Grant,et al. IP AND RESISTIVITY TYPE CURVES FOR THREE‐DIMENSIONAL BODIES , 1969 .
[3] H. Seigel. CHAPTER 2 – A THEORY OF INDUCED POLARIZATION EFFECTS (FOR STEP-FUNCTION EXCITATION) , 1959 .