Summary
Focused resistivity logging tools, such as Laterolog 7, have been used extensively, because they record large deflections—as compared with those for the unfocused normal and lateral sondes—against highly resistive thin formations. These large deflections, however, do not signify any inherent superiority of these tools, but are the result of using a set of fictitious and genetically unrelated currents in the apparent resistivity formulae—currents that do not exist in the ground at the time of measurement, do not ensure the necessary condition for null or near-null of potential, and do not generate the measured potential. When the real currents are used, the apparent superiority disappears altogether. By a suitable manipulation of the apparent resistivity formulae, even the normal or the lateral device can be made to yield large deflections.
It is also demonstrated that (i) the unfocused two-electrode normal sonde has a far larger radius of investigation than the ‘focused’ seven-electrode Laterolog 7 of equal spacing; (ii) the response of any sonde, focused or unfocused, can be synthesised exactly from that of a normal device of suitable spacings; (iii) Laterolog interpretation charts, published by different companies or by the same company at different times, exhibit very wide variations; and (iv) the extraordinarily high refinement of present-day resistivity log interpretation is inconsistent with the drastic simplifications, idealisations and other ambient factors governing the complex logging problems.
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© 1982 Applied Science Publishers Ltd
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Roy, A. (1982). Focused Resistivity Logs. In: Fitch, A.A. (eds) Developments in Geophysical Exploration Methods—3. Springer, Dordrecht. https://doi.org/10.1007/978-94-009-7349-7_3
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DOI: https://doi.org/10.1007/978-94-009-7349-7_3
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