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THE SMOOTH SOUNDING GRAPH. A Manual for Field Work ... - BGR

THE SMOOTH SOUNDING GRAPH. A Manual for Field Work ... - BGR

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1. Basic rules<br />

4<br />

The first chapter deals with the fundamentals of direct current resistivity<br />

measurements. The attempt was made to give an elementary introduction<br />

into what really happens within the earth during a measurement. The<br />

physical process should be understood by the reader.<br />

Each physical parameter will be checked with respect to its influence on<br />

the measured data. This will be done by reducing mathematical <strong>for</strong>mulae<br />

to a minimum. A well-trained mathematician will sometimes have a bad<br />

feeling seeing the rigorous way of using mathematical "tools". But this<br />

manual is written <strong>for</strong> a field crew working with modern equipments on the<br />

earth’s surface. Going on step by step in recording data they should follow<br />

up in mind the subsurface process, i.e. they should know what they are<br />

really doing.<br />

One remark should be added: In the theoretical part of this chapter only<br />

one very simple integral appears. The authors would be very glad if read-<br />

ers could make any proposal to get rid of this integral in explaining the<br />

necessary background of direct current resistivity sounding.<br />

1.1. Ohm's Law<br />

Geo-electrical measurements are carried out on the earth's surface. The<br />

air space is assumed as an insulator and the earth's surface as a plane.<br />

The underground is an electrical conductor. A direct current is running<br />

from the surface through this conductive infinite half-space, limited above<br />

by the plane earth's surface. Which laws are valid <strong>for</strong> this current flow<br />

through the underground?<br />

Regarding electrical currents we generally are accustomed to think of a<br />

wire. A wire has a certain resistance which can be calculated from Ohm's<br />

law. We regard (see Fig.1) a wire of the length a, measured in meters [m]<br />

with a cross-section q, measured in [m 2 ]. Ohm's law then can be written<br />

as<br />

U<br />

I<br />

a<br />

= R = ρ<br />

(1)<br />

q

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