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Mass Properties of Sedimentary Rocks and Gravimetric Effects of ...

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GRAVIMETRIC EFFECTS OF PETROLEUM AND NATURAL-GAS RESERVOIRS A5<br />

Foundation fpr financial assistance to permirt contributory<br />

studies in the Po basin <strong>of</strong> Italy.<br />

ROCK DENSITY IN SITU<br />

A widespread practical technique has not yet been<br />

devised for determining the density <strong>of</strong> rock in situ<br />

underground without direct or indirect dependence<br />

upon laboratory volume measurements <strong>of</strong> core samples.<br />

Core-sample analysis provides the calibration<br />

<strong>and</strong> control data needed for interpretation <strong>of</strong> gammagamma<br />

<strong>and</strong> velocity logs in terms <strong>of</strong> density (Pickell<br />

<strong>and</strong> Heacock, 1960). Until a praotical borehole gravimeter,<br />

or some other sensitive device capable <strong>of</strong> producing<br />

detailed <strong>and</strong> precise density logs, has become<br />

a reality, we will remain dependent on core analysis.<br />

Expressed in terms <strong>of</strong> parameters partly measurable<br />

in a core sample <strong>of</strong> rock, the density in situ Cuts) is:<br />

(I)<br />

where<br />

u,a=the density <strong>of</strong> the rock saturated with :fluid<br />

in its natural condition underground,<br />

u11=the dry-bulk density <strong>of</strong> the rock, including<br />

its pores,<br />

u1=the average density <strong>of</strong> the :fluid (or :fluids)<br />

filling the pores under natural conditions,<br />

=the total porosity expressed as a fraction,<br />

<strong>and</strong> is equal to 1-u 11 ,<br />

O"g<br />

where<br />

ug=the average density <strong>of</strong> the solid mineral<br />

grains composing the rock. .<br />

Other equivalent expressions for density in situ<br />

obtained by substitution <strong>of</strong> various <strong>of</strong> the foregoing<br />

terms in equation 1 are:<br />

<strong>and</strong><br />

+<br />

(2)<br />

O"fO"b ( )<br />

O"is=O"b u,-- 3<br />

Consideration <strong>of</strong> the terms in equations 2 <strong>and</strong> 3 reveals<br />

that knowledge <strong>of</strong> the densities <strong>of</strong> underground<br />

rocks in situ from core analysis depends on evaluation<br />

<strong>of</strong> the volume compressibilities-under low to moderate<br />

pressures <strong>and</strong> ·a range <strong>of</strong> temperatures like those found<br />

in nature-<strong>of</strong> the crystalline solid <strong>and</strong> the interstitial<br />

fluid constituents <strong>of</strong> such rocks, <strong>and</strong> also depends on<br />

the porosity or dry-bulk volume. The question <strong>of</strong><br />

whether core samples provide a satisfactory basis for<br />

evruluating these factors has never been fully <strong>and</strong> satisfactorily<br />

answered <strong>and</strong> is therefore examined here.<br />

The first step in such an examination is consideration<br />

<strong>of</strong> subsurface temperature <strong>and</strong> pressure gradients.<br />

239-675-67-· -2<br />

Ug<br />

SUBSURFACE TEMPERATURE AND PRESSURE<br />

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