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I SG NUCLEAR w'ELL LOGGING 4 <br />(b) Clay type identification:~lot of thorium versus potassium will indica~at type <br />of clay is present as shown in Fig. 4.3. The thorium/potassium ratio can also be <br />used. <br />(c) Source rock potentiel of shale: A relation exists between the uranium-to-potassium <br />ratio and the organic carbon content. The source rock potential of shale can thus be <br />evaluated. <br />»m <br />Th <br />(GPm) <br />mm <br />~m <br />e4l <br />om <br />K(°f~ <br />Fig. 4.3. -Plot of thorium versus uranium. <br />(After W. H. Ferrt) <br />4.3. DIFFUSED GAMMA-RAY LOGS <br />Gamma rays interact with matter in three different ways: <br />(a) Pairs (electron + positron) are produced if the energy of the incident GR is greater <br />than 1.02 MeV. <br />(b) Compton diffusion by the electrons occurs in the entire gamma spectrum, and this is <br />used in density logging. The amount of Compton diffusion is related to the number of <br />electrons by the unit volume which in turn is linked to the specific gravity o(the <br />matter. <br />(c) Photoelectric absorption occurs (or low-energy gamma rays. This absorption <br />depends on the nucleus-electron bonding energy which in turn is linked to the <br />atomic number Z of the nucleus. This absorption is the basis (or another log, the <br />Litholog. <br /> ~ <br /> / <br />i <br />i~.,, <br />~~ m <br /> /%% ~j <br /> <br /> <br />~~/ ~// ; <br /> ~, ! <br />'j; <br />ououx~ <br />i:: c <br />~ <br />;ii <br />i <br />~.o+~•onuoYa! <br />Q <br />cuoR~rz <br /> o J <br /> cuuco+rtv <br />~~~ <br /> YVSCWR! 1lLpyiR <br /> <br />4 <br />4.3.1. Densil <br />As shown in Fi <br />mounted on the <br />the gamma rays <br />related [o the d~ <br />having undergo) <br />Pad ~ <br />So as to correc <br />an open hole, a <br />directly and is sc <br />equation: <br />i <br />where <br />p, is the bul <br />pm, is the den <br />pf is the den <br />~ is the por <br />