Geophysical Abstracts 152 January-March 1953
Geophysical Abstracts 152 January-March 1953
Geophysical Abstracts 152 January-March 1953
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50 GEOPHYSICAL ABSTRACTS <strong>152</strong>, JANUARY-MARCH <strong>1953</strong><br />
to be the same as that of meteors, one-third iron, uranium, thorium, potassium,<br />
and actinouranium, and two-thirds stony material. As the basic premise the earth<br />
is assumed to have been formed by a cold process, so a homogenous distribution<br />
of radioactive substances in the initial phase of the process seems quite probable.<br />
Constant density and heat capacity of the earth, independent of the depth, are<br />
also assumed.<br />
The intensity of radioactive heat production computed from recent determina<br />
tions of decay constants, resulted in greater heat generation in the beginning of<br />
geologic history than at the present time. Applying the method of images, ex<br />
pressions were derived for the temperature in the center of the earth for the past<br />
time, for different assumed ages of the earth; for the variation of temperature<br />
with depth. The great thermal inertia of the earth, due to very low heat con<br />
ductivity, leads to conditions where the exterior surface is cooling, while near the<br />
center the temperature continues to rise. The computed quantities are presented<br />
in the form of rapidly converging series. S. T. V.<br />
14353. Bikitake, Tsuneji. Electrical conductivity and temperature in the earth :<br />
Tokyo Univ. Earthquake Research Inst. Bull., v. 30, pt. 1, p. 13-24, 1952.<br />
Eikitake's previous work on determining the temperature distribution within<br />
the earth from the distribution of electrical conductivity and the theory of<br />
ionic crystals is revised for greater accuracy and to take into account changes<br />
in physical conditions above and below the so-called 20° discontinuity. Consider<br />
ing the pressure-effect of the conductivity it is found that the temperature is<br />
probably 1,000 K just below the crust and then increases almost proportionally to<br />
depth, the rate being estimated as 1.4 K per km. This distribution is roughly<br />
consistent with the density and bulk modulus distribution determined by Bul-<br />
len. M. 0. R.<br />
INSTRUMENTS AND METHODS OF MEASUREMENT<br />
14354. Tavernier, Paul, and Prache, Pierre. Influence de la pression sur la re-<br />
sistivite" d'une thermistance [Effect of pressure on the resistivity of a<br />
thermistor] : Jour. Physique et Radium, tome 13, no. 7-S-9, p. 423-426,<br />
1952.<br />
Experiments indicate the variation in resistance expressed as the fractional<br />
change &R/Ro, of a thermistor subjected to pressures P up to 5,000 kg per cm2<br />
is given by &R/Ro= 4.6 XIO"6 P and is independent of temperature in the range<br />
between 30 and 70 C.' The correction to rough data is of the order of 0.01 de<br />
gree for pressure of 100 kg per cm2. Details of the experimental set up are<br />
given. M. G. R.<br />
OBSERVED TEMPERATURES IN THE CRUST AND HEAT FLOW<br />
14355. Revelle, Roger, Maxwell, Arthur E., and Bullard, E. C. Heat flow through<br />
the floor of the eastern North Pacific Ocean: Nature, v. 170, no. 4318, p.<br />
199, 1952.<br />
The thermal gradient at 6 places in the eastern north Pacific ocean floor was<br />
found to be about 1.2X10~6 cal/cm2/sec. This is the same order of magnitude as<br />
in continental areas. A possible explanation is that the heat is generated by<br />
radioactivity, the total amount beneath a unit area of continent or ocean being<br />
the same when summed to a depth of a few hundred kilometers. M. (7. R.