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Introduction
Geomagnetic surveying is usually done nowadays to map a
geological feature mainly at exploration stages detections of mines.
The problem facing requires an inverse solution. The Gauss’ theorem
1
implies that if one knows the feld distribution on a bounding
surface, infnitely many equivalent sources distributions inside the
boundary can produce the known feld. Thus, any geomagnetic feld
measurement performed on the surface of the Earth can be reproduced
by an infnitesimally thin zone of magnetic dipoles beneath the
surface. From a mathematical perspective, this means there is no depth
resolution inherent in magnetic feld data. An approach for inverting
geomagnetic data is to divide the Earth into a large number of cells
of fxed size but of unknown susceptibility. Although the problem is
not unique, if we choose an objective function for the model to ft
the data using a global minimization technique such as,
2
minimization
of a weighted model norm for a reference model is considered. This
method allows the interpreter to guide the inversion by varying the
weighting according to the available information
3
choose to minimize
the total volume of the causative body so that the fnal model is
compact and structurally simple
4
minimized the moment of inertia
of the causative body for the centere of gravity or an axis passing
through it. Their inversion result is guided by the estimate of the
central depth and dip of the causative body. These approaches have
merit, but they are not fexible enough to handle problems we are
concerning. The
5
presented an inverting method for magnetic data to
recover 3-D susceptibility models. To allow the maximum fexibility
for the model to represent geologically realistic structures, they
discretized the 3-D model region into a set of rectangular cells, each
having a constant susceptibility. The number of cells is generally far
greater than the number of the data available, and thus they solved
an underdetermined problem. Solutions are obtained by minimizing
a global objective function composed of the model objective function
and data misft. The algorithm can incorporate a priori information
into the model objective function by using one or more appropriate
weighting functions. The inversion model can be either susceptibility
of its logarithm. If susceptibility is chosen, a positivity constraint
is imposed to reduce the nonuniqueness and to maintain physical
realizability. In this study, we use the
5
method to delineate the
magnetic ores in the study area. The study presented here is typical
and similar studies can be done to detect various ferrous mines.
Study area and data acquisition
The Chenar ferrous mine is located within the 5 km vicinity of
Chenar village placed in 16 km north of Asadabad city of Hamadan
Province of Iran. The access road to the mine is the road which
connects the Chenar village to Asadabad city. The geographical
location and the access road to Chenar ferrous mine are shown with
green colour in Figure 1 (A). The area of interest is shown in red
colour. A selected portion of Figure 1 (A) is shown in Figure 1 (B).
The black box indicated in Figure 1 (B) is the top view projection
of an imaginary box used to illustrate our analysis. The data was
acquired in 4300 pre-planned location using a Canadian GEM-GSM
19 T series magnetometer in 10 days. The spatial resolution of the data
in each line was 20 meters Figure 1 (C).
Figure 1 (A) Location of the study mine in the satellite image and the way
of green access to the mine. (B) The black box shows the top view of the
analysis cubes in the study area. (C) The data acquisition points where the
magnetometer was placed and recorded the magnetic value of the Earth.
Phys Astron Int J. 2020;4(5):172‒175. 172
©2020 Ala Amjadi et al. This is an open access article distributed under the terms of the Creative Commons Attribution License,
which permits unrestricted use, distribution, and build upon your work non-commercially.
Geomagnetic inversion for delineation of ore
deposits in chenar mine
Volume 4 Issue 5 - 2020
Ahmad Ala Amjadi,
1,2,3
Mohsen Kushki
1
1
GeoMine Company, No. 6, Block 37, West Shabnam Ave, Tehran,
Iran
2
North Drilling Company (NDC), No. 2127, Corner of Del
Afrooz St.,Valiasr St., Tehran, Iran
3
International Institute of Earthquake Engineering and
Seismology (IIEES), Iran
Correspondence: Ahmad Ala Amjadi, GeoMine Company,
No. 6, Block 37, West Shabnam Ave., 2nd Golha St., Entesarieh,
North Karegar, Tehran, Iran, P.O. Box: 14139-93317,
Email
Received: September 24, 2019 | Published: October 12, 2020
Abstract
In this manuscript, we have performed an applied geomagnetic inversion study in the
Chenar ferrous mine near Asadabad-Hamedan of Iran. The principal purpose of this study
was to depict and visualize the ore massif of the Chenar ferrous mine in details and to fnd
the suitable locations for geological drilling cores. In this study, 4300 Geomagnetic readings
were acquired over a ten-day data acquisition period with a Canadian-built 2019 GEM-
GSM19T magnetometer. The analyzes of the geomagnetic data in the Chenar ferrous mine
successfully identifed the susceptible zones in the area of study, and we have suggested the
location of six drilling points in the mining area for further investigation and verifying of
geophysical data. Our results depict four massifs which are extended as veins. According
to the dimensions of the magnetic halos, our geophysical result estimates the ore deposit
to be about two and a half million tons for three of the massifs in the Eastern part and 250
thousand tons for the fourth massif in the Western part of the study region.
Keywords: geomagnetic, geophysics, ferrous mines, exploration
Physics & Astronomy International Journal
Research Article
Open Access