TY - JOUR
T1 - A Passive Natural-Source Twin-Purpose Borehole Technique
T2 - Vertical Gradient Magnetometry (VGM)
AU - Jones, Alan G.
PY - 1983
Y1 - 1983
N2 - Two major factors hinder mineral exploration at this present time: (1) a conventional resistivity borehole log is often more indicative of the resistivity of the pore-filled fractured rock in the close locale (< 1 m) of the borehole than the actual resistivity of the layer in which the probe is located; and (2) ground-based em techniques, both natural and controlled source, are often unable to locate a mineralized zone beneath another mineralized zone. In this paper, the theory is presented for the basis of a conceptually new type of borehole technique based on the ratio of the measurement of the natural horizontal magnetic field variation to its gradient with depth, down the hole, viz. [formula omitted]. Defining the “downhole apparent resistivity”, ρa(ω, d) by it is shown that, for a 1D earth structure, as ω tends to infinity, then ρa(ω,d) tends to the actual resistivity of the layer in which the probe is located. Also, ρa(ω,d) is independent, in the 1D case, of any structure above it, and weakly dependent in the 2D case. The technique has the benefit of most borehole methods of being far superior at resolving structure at depth below it, e.g., a second good-conducting zone, than equivalent ground-based methods (e.g., MT and /or GDS). Application of the technique to some theoretical 1D and 2D structures is presented, as well as a discussion of the feasibility of constructing the necessary sensor for the proposed technique.
AB - Two major factors hinder mineral exploration at this present time: (1) a conventional resistivity borehole log is often more indicative of the resistivity of the pore-filled fractured rock in the close locale (< 1 m) of the borehole than the actual resistivity of the layer in which the probe is located; and (2) ground-based em techniques, both natural and controlled source, are often unable to locate a mineralized zone beneath another mineralized zone. In this paper, the theory is presented for the basis of a conceptually new type of borehole technique based on the ratio of the measurement of the natural horizontal magnetic field variation to its gradient with depth, down the hole, viz. [formula omitted]. Defining the “downhole apparent resistivity”, ρa(ω, d) by it is shown that, for a 1D earth structure, as ω tends to infinity, then ρa(ω,d) tends to the actual resistivity of the layer in which the probe is located. Also, ρa(ω,d) is independent, in the 1D case, of any structure above it, and weakly dependent in the 2D case. The technique has the benefit of most borehole methods of being far superior at resolving structure at depth below it, e.g., a second good-conducting zone, than equivalent ground-based methods (e.g., MT and /or GDS). Application of the technique to some theoretical 1D and 2D structures is presented, as well as a discussion of the feasibility of constructing the necessary sensor for the proposed technique.
UR - http://www.scopus.com/inward/record.url?scp=0020864420&partnerID=8YFLogxK
U2 - 10.5636/jgg.35.473
DO - 10.5636/jgg.35.473
M3 - Article
AN - SCOPUS:0020864420
VL - 35
SP - 473
EP - 490
JO - Journal of geomagnetism and geoelectricity
JF - Journal of geomagnetism and geoelectricity
SN - 0022-1392
ER -