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Geophysical Abstracts 152 January-March 1953

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ELECTRICITY 25<br />

14252. Wait, James R. Transient coupling in grounded circuits: Geophysics,<br />

v. 18, no. 1, p. 13&-141,<strong>1953</strong>.<br />

The electrical field in an infinite isotropic medium caused by a step-function<br />

current flowing through a wire ground at both ends is considered. The problem<br />

is solved to determine the voltage which is induced in a second insulated circuit,<br />

also grounded at both ends, but having infinite resistance. The Solution is<br />

applied to electrical well logging when a commutated or square wave is used.<br />

The particular electrode configuration considered consists of a single current<br />

electrode in a drill hole and two potential electrodes in line with the current<br />

electrode at distances I and 21. The second current electrode is at the surface.<br />

In such a case, the voltage between the pickup electrodes reaches 97 percent<br />

of its maximum value in 10~5 a seconds, where o- is the conductivity of the<br />

medium. Gf. V. K.<br />

ELECTRICAL PROPERTIES OF ROCKS AND MINERALS<br />

14253. Cownie, A., and Palmer, L. S. The effect of moisture on the electrical<br />

properties of soil: Physical Soc. London Proc., sec. B, v. 65, no. 4,<br />

p. 295-301,1952.<br />

Measurements of the dielectric constant of soil containing different known<br />

percentages of moisture were made at a fixed frequency of 430 megacycles per<br />

second. The method adopted involved the use of a coaxial transmission line<br />

terminated with a sample of the soil under text. The line consisted of a central<br />

rod with a concentric tube about 2y2 meters in length. Measurements were<br />

made with soil samples containing from 4.1 to 47.7 percent moisture. The<br />

dielectric constant was found to vary from 4.0 to 31.4. The values are shown<br />

graphically and compared with those obtained by nine other authors. The<br />

conductivity could not be measured accurately with the method used, but it<br />

was estimated to vary from about 1.5X10 9 e. s. u. with 4 percent moisture to<br />

4 X10 10 e. s. u. with 50 percent moisture. Authors' Abstract<br />

14254. Keller, G. V. Effect of wettability on the electrical resistivity of sand:<br />

Oil and Gas Jour., v. 51, no. 34, p. 62-65,<strong>1953</strong>.<br />

Experiments show that for conditions which may conceivably be repre­<br />

sentative of rock in place, the exponent n of Archie's equation may vary from<br />

1.5 to 11.7 for the same rock sample and the form of the equation is inadequate<br />

to explain the resistivity of rock at the low water saturations in many oil<br />

reservoirs. Experiments show that for the same water saturation, resistivity<br />

can vary a thousandfold for different wetting conditions. M. C. R.<br />

14255. Sakuma, Shuzo. Earth-current potentials near boundaries of various<br />

geological formations: Tokyo Univ. Earthquake Research Inst Bull,,<br />

v. 30, p.t 1, p. 25-30,1952.<br />

Natural-potential measurements were made in several areas to determine the<br />

relations, if any, between geologic structures and earth-current potentials. Near<br />

the active Tanna fault, a zone of negative potentials was found along the fault<br />

line superposed on the general east-west earth current although rocks on both<br />

sides of the fault are petrologically similar. Similar disturbances of the earth<br />

current were noted near other faults. Earth-current potentials differed ob­<br />

viously among formations of strongly contrasting physical and chemical<br />

properties. M. C. R.

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