r
LOCATION OF ABANDONED WELLS
WITH GEOPHYSICAL METHODS
by
F. C. Frischknecht
P. V. Raab
U.S. Geological Survey
Geological Division
Denver, CO 80225
Interagency Agreement No. DW 149 30473-01-0
Project Officer
Jeff van Ee
Aquatic and Subsurface Monitoring Branch
Environmental Monitoring Systems Laboratory
Las Vegas, NV 89114
This study was conducted in cooperation with the
U.S. Geological Survey, Department of Interior
ENVIRONMENTAL MONITORING SYSTEMS LABORATORY
OFFICE OF RESEARCH AND DEVELOPMENT
U.S. ENVIRONMENTAL PROTECTION AGENCY
LAS VEGAS, NEVADA 89114

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NOTICE
The information in this document has been funded wholly or in part by the
United States Environmental Protection Agency under interagency agreement number
DW 149 30473-01-0 to the U.S. Geological Survey, it has been subjected to the
Agency's peer and administrative review, and it has been approved for publica-
tion. Mention of trade names or conmercial products does not constitute
endorsement or recommendation for use.

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PREFACE
The Environmental Monitoring Systems Laboratory of the U.S. Environmental
Protection Agency (EPA) provided funding for the research on geophysical meth-
ods described in this report. The cooperative effort between EPA and the U.S.
Geological Survey (USGS) is part of a larger effort to provide local, state,
and Federal agencies with guidance methodologies to determine if abandoned
wells exist in an area where the underground injection of wastes is contemplated.
Besides geophysical surveys, record-searches, as conducted by the University of
Oklahoma, and photographic searches have proven to be useful in locating
abandoned wells.
This summary of the geophysical studies and the results was written for
persons who are not familiar with the terminology and methodology of geo-
physics. The reader who is interested in more technical details, including
all of the results, may refer to the USGS open-file reports that are listed
among the references.
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ABSTRACT
Abandoned wells are sometimes an Important element 1n the contamination
of fresh underground water supplies. If a well is not properly plugged and
the casing is leaky, it may serve as a conduit for brines or other pollutants
to reach a fresh water aquifer. This study was made to determine the feasi-
bility of using geophysical methods to locate abandoned wells which contain
steel casing. Preliminary considerations Indicated that magnetic and, perhaps,
electrical methods should be useful.
Detailed measurements of the Earth's magnetic field in the vicinity of a
number of wells showed large disturbances or anomalies 1n the field. Using a
. mathematical model developed to represent the effect of a steel casing, 1t was
possible to predict from ground magnetic measurements the anomalies which would
be observed by a magnetometer placed in an aircraft. Although magnetic anomal-
ies caused by a casing diminish rapidly as the height is Increased, 1t appeared
that wells could be detected from a low flying aircraft.
From the model study, a survey was designed with an aircraft height of
60 m and a spacing between flight lines, or tracks, of 100 m. Aeromagnetlc
surveys were made over one test area in Colorado and four test areas in Oklahoma
where there are many known wells. Supplemental Information was obtained with a
ground magnetometer. The aeromagnetlc results agreed well with those obtained
by a records search and by Interpretation of aerial photographs. These methods
are complementary 1n that each provides information which the others do not.
Most wells In Oklahoma produced anomalies with magnitudes far exceeding
the threshold for recognition. In a few cases the anomalies were small; but,
with careful analysis, most of them were recognized. When wells occurred in
close proximity, it was difficult to determine how many there were from the
aeromagnetlc results. Anomalies due to other manmade features, such as pipe-
lines and transmission line towers, were a minor problem In Interpreting the
aeromagnetlc results. In the Colorado test area, sharp anomalies resulting
from variations in the magnetization of near-surface sedimentary rocks caused
difficulty in interpretation of the aeromagnetlc results. However, questions
1n Interpretation were resolved by selective ground magnetometer measurements.
Overall it was estimated that 95-98 percent of the wells 1n the areas surveyed
were detected. Thus, the results of the study show that the magnetic method is
an effective means of locating abandoned wells. However, most agencies or
organizations which have the responsibility for finding wells will require
technical assistance in designing and carrying out magnetic surveys.
Electrical methods which were tested were the dipole-dlpole resistivity/
Induced polarization (IP), self-potential, and loop-loop electromagnetic
methods. Substantial self-potential anomalies were observed over some but not
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all wells. The results of a few resistivity/IP and electromagnetic tests did
not indicate the presence of wells. There are some other potentially useful
electrical methods which were not tested. However, it appears that electrical
methods have only limited uses in locating abandoned wells. Unless more promis-
ing electrical results become available, use of only the magnetic method is
recommended.
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CONTENTS
Page
Preface	iii
Abstract		iv
Figures	viii
Introduction		1
Conclusions and Recommendations 		3
Principles of Magnetic and Electrical Methods 		5
Magnetic Fields		5
Magnetic Properties of Materials 		5
Magnetometers		6
Magnetic Survey Procedures and Data Processing 		9
Electrical Properties of Materials 		11
Electrical Methods 		11
Ground Magnetic Measurements		14
Inversion of Ground Magnetic Measurements and Modeling		22
Airborne Magnetic Measurements and Results		24
Electrical Measurements and Results 		39
Planning and Management of Geophysical Investigations
for Locating Abandoned Wells 		41
References		45
Appendix: Costs for Geophysical Equipment and Services 		47
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FIGURES
Number	Page
1	Sketch of magnetic field lines for a magnetized object and
their Interaction with the Earth's magnetic field lines .... 7
2	Portable proton magnetometer in use in Colorado 	 8
3	Location of the P1ney Creek test area	 16
4	Observed and calculated north-south magnetic
profile over well No. 4, Piney Creek test area	 17
5	Observed and calculated east-west magnetic
profile over well No. 4, Piney Creek test area	 18
6	Location of the Oklahoma test areas 	 19
7	Observed and calculated north-south magnetic
profile over well No. 17, Horseshoe Lake test area	 20
8	Observed and calculated east-west magnetic profile
over well No. 17, Horseshoe Lake test area	 21
9	Calculated isopleth map of total intensity (gammas) at
a height of 200 ft above a well	 23
10	Fairchild Porter aircraft used in this study		25
11	Map of Arcadia, Oklahoma area, sections 3, 10, 11, and 14 ... .	28
12	Airborne profile data from Arcadia area 		29
13	Total intensity isopleth map for part of Arcadia area 		30
14	Map of Piney Creek, Colorado, area		31
15	Aeromagnetlc profiles at different aircraft heights
over well No. 4, Piney Creek area	 32
16	Total intensity gamma Isopleth map for part of
Piney Creek area	 35
17	Self-potential profiles over well No. 7, Piney
Creek, Colorado, area	 40
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INTRODUCTION
The Underground Injection Control (UIC) regulations promulgated by the
Environmental Protection Agency regulate injection wells for the protection of
actual or potential underground sources of drinking water as required by the
Safe Drinking Water Act. One-provision of the UIC regulations establishes a
radius of review around proposed new injection wells, based on the hydrogeologic
properties of the subsurface. Within this radius a search must be made for
possible conduits, such as abandoned wells, from the injection stratum to
overlying aquifers containing potable water.
It was estimated in 1979 that there were some 500,000 municipal, indus-
trial, commercial, agricultural and domestic wells injecting fluids below the
surface, and that at least 5,000 new injection wells were being constructed
each year (Federal Register, 1979). Due to differential pressures, dormant or
abandoned wells sometimes serve as conduits between aquifers containing brine
or other pollutants and fresh water aquifers. Location of such existing wells
is an important task; it was estimated in 1979 that there were as many as
1,800,000 producing, dormant, and abandoned wells in the United States (Federal
Register, 1979). The problem presented by abandoned or unknown wells is espe-
cially acute in petroleum producing regions where the total number of wells
may reach densities as high as 2,000 per square mile. Particularly in the
early days of petroleum production, the locations of wells were not always
recorded. Some recorded locations were erroneous, or described only in broad
terms, and many old records are not readily available.
Geophysical methods originally developed for resource exploration may be
useful in locating abandoned wells. The "classical" methods of exploration
geophysics are (1) the seismic method, depending on the propagation of mechani-
cal or seismic waves through the Earth; (2) the gravity method, depending on
changes in the force of gravity due to variations in density from region to
region; (3) the magnetic method, depending on disturbances in the magnetic
field of the Earth caused by magnetic materials; and (4) electrical methods,
depending on the the electrical resistivity and other electrical properties of
the Earth. The objectives of this research were to study the feasibility of
locating wells using geophysical methods and to test and demonstrate the most
promising methods.
Throughout the history of petroleum production, steel casings and other
steel pipes have been used in almost all petroleum wells; and, until recently,
steel casings were used in most drilled water wells. A steel casing causes a
relatively large disturbance, which may persist to distances of a few hundred
feet from the end of the casing, in the magnetic field of the Earth. Instru-
ments called magnetometers, which measure magnetic fields, can be used to
locate the magnetic disturbances or "anomalies" caused by steel casings.
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Magnetometers can be operated in low-flying aircraft, thereby offering a rapid
means for magnetic surveys of large areas. Although a type of simple handheld
magnetometer is sometimes used by construction and maintenance personnel to
locate iron and steel pipes, apparently magnetometers have not been systemati-
cally used for location of wells.
Steel casings are very good conductors of electricity, relative to the
surrounding Earth, and electrochemical reactions may take place between a
buried steel object and the Earth. Therefore, some of the electrical methods
of exploration geophysics may be useful in locating steel casings. However, in
some instances, all or part of the casing and other pipe has been removed from
abandoned wells; neither the magnetic nor electrical method would be useful in
locating uncased drill holes.
The change in gravity due to the presence of a cased or uncased hole is
too small to warrant considering the use of gravity techniques. Seismic meth-
ods might be of some use, but the range of detection would be rather short and
the method is costly to employ. Remote sensing methods which employ microwave,
infrared, or other high frequency electromagnetic radiation may be useful, theo-
retically, in detecting disturbances of the soil which mark a well site, but
' were deemed to have little chance for success in practice. Due to these con-
siderations, it appeared that the magnetic and electrical methods were the only
ones likely to be effective in the location of casings, and it was decided that
primary emphasis should be placed on magnetic methods.
In the first phase of this study, Frischknecht and others (1983) developed
a simple mathematical model for the magnetic field of a casing. To apply this
model to specific casings, the magnetic parameters of the casing must be deter-
mined experimentally. Magnetic parameters for a number of nonproducing or dry
wells near Denver, Colorado, were determined from measurements made with a
ground-based magnetometer. The model was then used to predict the results
which would be obtained with a magnetometer placed in a low-flying aircraft.
Since results of this study indicated that it was feasible to locate casings
from airborne measurements, the parameters of an airborne survey were designed
(Frischknecht and others, 1983).
In the second phase of the study (Frischknecht, and others, 1984), aero-
magnetic surveys of a small test area near Denver and four small areas near
Oklahoma City, Oklahoma, were made. The test areas near Oklahoma City were
selected by the University of Oklahoma (Fairchild and others, 1983). Ground
magnetic measurements were made at many localities to aid in the evaluation of
the aeromagnetic data. The data were processed and evaluated to arrive at
conclusions and recommendations for the use of the magnetic method.
The use of electrical methods was considered and self-potential and
inductive electromagnetic methods were tested (Frischknecht and others, 1983).
During the second phase of the study, the dipole-dipole resistivity/IP method
was tested near one casing (Washburne, 1984).
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CONCLUSIONS AND RECOMMENDATIONS
The results of this study show that steel well casings generally produce
large and distinctive magnetic anomalies. Although these anomalies diminish
rapidly with distance from the wells, modeling indicated that wells could be
detected by magnetometer measurements made on the ground or from low-flying
aircraft. The results of aeromagnetic surveys in Oklahoma agreed well with
those obtained by interpretation of aerial photographs and by a search of
available records. Since these other methods are not completely reliable, there
is no way of knowing exactly how many wells there are in the test areas, but it
was estimated that 95-98 percent of them were detected by the aeromagnetic
survey. Although the location of abandoned wells is basically a new application
for the magnetic method, this study demonstrates that ground and airborne
magnetic surveys are effective for this purpose.
Some of the advantages of the magnetic method in locating casings are:
1)	The method can be readily used to accurately locate buried casings
where there has been no surface evidence of the well for many years.
2)	By use of an aircraft, large areas can be surveyed rapidly without
need for access to the property.
3)	With the use of a ground magnetometer, the horizontal position of a
casing can be located within one or two meters and the results are immedi-
ately available.
Some of the disadvantages of magnetic methods and problems in their use are:
1)	Wells which do not contain near-surface casing or other pipes cannot be
detected at all, and it may be impractical to locate wells containing only a
small amount of casing due to the large number of close-spaced measurements
which is then required.
2)	The magnetic method may be relatively costly compared with other
methods, particularly if the areas are small and few in number.
3)	In some areas, magnetic disturbances due to manmade objects, such as
pipelines and steel buildings or anomalies due to naturally occurring
magnetic minerals in near-surface rocks, interfere with the recognition of
anomalies caused by casings.
4)	Most conmerical and public institutions which have a need to search
for abandoned wells will, at least initially, require technical assistance
from outside their organizations.
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Theory suggests that it may be possible to detect steel casings with
electrical methods of geophysical exploration. There are many reports of
distortion of resistivity/IP measurements caused by wells. However, the re-
sults of one res1stivity/IP test made as part of this study did not indicate
the well. Some casings produced substantial electrical self-potential
anomalies; but, most did not. Two standard electromagnetic methods which were
tested did not yield useful results. While more study is needed to completely
evaluate the use of all electrical methods in locating wells, it appears that
electrical methods are generally less effective and more costly than magnetic
methods.
The results of this study do not indicate that further research is re-
quired before the magnetic method should be applied in the search for abandoned
wells. Most of the questions that can be addressed in a modest research effort
have been answered. In considering the application of the magnetic method in
the search for abandoned wells in a new area, the most important questions are:
(1) what size magnetic anomalies are the casings likely to produce, and (2) how
much magnetic interference will there be from other manmade sources and from
natural sources? These questions can never be completely answered, since each
new area will be somewhat different than those already investigated. However,
' we believe that our test areas in Colorado and Oklahoma are representative of
conditions in many oil fields, and that our results can be used in planning and
conducting work in other areas.
The results of any new surveys designed to locate wells could be valuable
guides to further work, and they should be published as soon as possible.
After experience has been gained in a number of new areas, it would be very
worthwhile to carefully evaluate the effectiveness of the magnetic method,
compared with other approaches, and to identify continuing problems in the
application of the magnetic method. Such a review might lead to new recommen-
dations on how to best use the method, and it might lead to recommendations for
further study of particular problems or techniques.
The results of this study indicate that it is very useful to employ three
methods: records-search, photointerpretation, and magnetic surveys, in locating
wells. All three methods are recommended for use in new areas. However, since
each method has deficiencies, there is the possibility that in particular areas
one or more of the methods will not be applicable. Also, in some areas, it is
likely that wells can be located by use of only one or two methods.
There are a number of different circumstances in which the use of
magnetic methods to locate wells should be considered. Sometimes there are
requirements to physically locate buried wells which are known from records;
ground magnetic methods are most useful for this purpose. Regulations require
a search for abandoned wells within a certain radius, sometimes specified to be
1/4 mile, of proposed new injection wells (Federal Register, 1979). Ground or
airborne magnetic methods might be used for this purpose; but, if a search is
to be made around the location of several proposed injection wells in the same
general area, airborne methods will probably be least expensive. Finally, an
agency or firm may have a need to search for wells over large areas to find
potential sites for injection wells which are the prescribed distance from any
abandoned wells.
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PRINCIPLES OF MAGNETIC AND ELECTRICAL METHODS
MAGNETIC FIELDS
The Earth possesses a magnetic field which has roughly the same form as
that which would result from a large bar magnet placed near the Earth's center.
Both the intensity and direction of the Earth's magnetic field vary with loca-
tion. Such a field that possesses a direction as well as intensity is called
a vector field. The Earth's field is customarily described in terms of three
quantities: declination, inclination or dip, and intensity or "total field."
Declination is the difference between true or geographic north and the direc-
tion in which the needle of a magnetic compass points. Inclination is the
difference between the direction of the field and the horizontal plane. In-
tensity is a measure of the strength of the field or the force which it exerts
on magnetic objects. Declination and inclination are measured in degrees, and
intensity is expressed in gammas (1 gamma = 10"^ oersted) or in S.I. units as
nanoteslas. Numerically, the gamma and the nanotesla are the same; the former
unit is still used by most geophysicists. Over the coterminous United States,
average values of declination, inclination, and intensity vary systematically
between about 20° west of north to 20° east of north, 52° to 76° from the
horizontal plane, and 48,000 to 60,000 gammas, respectively (Fabiano, and
others, 1983). Locally, the values of the field may fall far outside these
ranges.
The interaction between the Earth's field and changing amounts of radi-
ation from the sun causes the intensity and direction of the field to vary with
time. Of most concern in magnetic surveying are a more or less regular daily
variation of the field and irregular changes which take place over time periods
varying from a few minutes to hours during "magnetic storms." In making mag-
netic surveys, it is generally necessary to monitor these time variations and
to remove their effect from survey data.
MAGNETIC PROPERTIES OF MATERIALS
Magnetization is a phenomenon which some materials exhibit that causes
objects made of the material to behave as magnets. For purposes of this re-
port, two kinds of magnetization should be recognized: induced magnetization
and permanent or remanent magnetization. Induced magnetization in a material
depends on the intensity and direction of the surrounding or inducing magnetic
fields; in our case, this is the Earth's field. If the Earth's field is
removed by placing the material inside a magnetic shield, the induced magnet-
ization in the object becomes zero. The degree to which a material is magnet-
ized by an inducing field depends on a parameter called magnetic susceptibility.
Permanent or remanent magnetization is the property of some materials such as
those used in household magnets, that causes them to retain magnetization in the
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absence of a magnetic field. Permanent magnetization in an object depends on
the original inducing field and a material property called coercive force.
The total magnetization of an object is the sum of the induced and permanent
magnetization.
The magnetic field near a magnetized object is the sum of the local field
due to the object and the Earth's field. It is sometimes convenient to think
of these fields in terms of imaginary lines along the direction of the field.
In Figure 1, the Earth's field locally is shown by a set of nearly parallel
lines whereas the field of the magnetized object is shown by a set of curved
lines. In summing the two fields, their directions as well as intensities must
be considered. Thus, the total field near a magnetized object may be greater
or less than the Earth's field.
Most iron and steel objects exhibit some degree of both kinds of magne-
tization. A few naturally occurring minerals, such as the iron oxide magnet-
ite, can be magnetized. Rocks containing even a small percentage of these
minerals are weakly magnetic and variations in the distribution of magnetic
rocks cause perturbations or anomalies in the Earth's field. Most oil or gas
fields are found in regions where the near-surface rocks are sedimentary.
¦ Generally, sedimentary rocks are only very weakly magnetic, but there are
notable exceptions to this rule (Donovan, and others, 1979). Igneous and
metamorphic rocks, which occur beneath sedimentary rocks and, in many regions,
at the surface, are often sources of substantial magnetic anomalies. Magnetic
surveys are useful in exploration for mineral deposits and in studies of sub-
surface geology. But, in using magnetic methods to locate casings, anomalies
due to rocks are a source of interference.
MAGNETOMETERS
The magnetometer is a sensitive instrument which can be used to map vari-
ations in the Earth's magnetic field. Some magnetometers are highly portable
instruments which are operated manually. Other magnetometers are designed to
be mounted in aircraft or other vehicles, and more or less continuous record-
ings are made as the vehicle moves. Some magnetometers measure the directions
of the field and others measure the intensity of the field in a particular
direction such as the vertical direction. The intensity of the field along a
particular direction is usually called the "component" of the field in that
direction. The component of a field in the direction perpendicular to the
direction of the field is zero, and the component in the direction parallel to
the field is the maximum value, or total intensity, of the field. Measurement
of the direction or of a component of the field is generally either very time
consuming or inaccurate or both. Most magnetic surveys are made with instru-
ments which measure only the total intensity. Currently, the proton precession
magnetometer is most commonly used for total intensity measurements. It con-
sists of a sensor containing a coil of wire immersed in a fluid rich in protons
and a separate box containing electronic circuits and a display. The protons
in the fluid collectively wobble like spinning tops at a rate which depends on
the intensity of the magnetic field. By measuring the rate of wobble, the
intensity of the field is determined. Use of a portable proton magnetometer in
the field is illustrated in Figure 2.
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FIELD LINES

REGION A
cs
REGIONS^
OF OBJECT
\	v^FIELD LINES
[ED ^ OF EARTH
Figure 1. Sketch of magnetic field lines for a magnetized object and
their interaction with the Earth's magnetic field lines. The
two fields directly reinforce each other in regions such
as A, and they oppose each other in regions such as B.
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Figure 2. Portable proton magnetometer in use in Colorado.
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The proton magnetometer cannot provide continuous measurements. However,
in airborne operation, it can sample once or twice a second or faster, depend-
ing on its sensitivity. Nominal sensitivity of a proton magnetometer is about
one gamma. Some handheld units have a sensitivity of only 10 gammas; other
more expensive systems have a sensitivity of 0.1 gamma or greater. Ground
magnetometer measurements are recorded in a notebook by the operator or, with
newer instruments, directly in a solid state memory. Airborne magnetometer
readings are usually recorded on magnetic tape.
For special purposes, changes in the field or "magnetic gradients" are
sometimes measured. In practical terms, the gradient is the difference in the
field measured at two points divided by the distance between the points. The
gradient of a component of the field can be determined, but most often the
gradient of the total intensity is measured. Typically, a gradiometer consists
of two proton magnetometer sensors and an electronic instrument which measures
the field at both sensors and the difference in fields between the sensors.
The sensors can be placed one above the other to measure the vertical gradient
or at the same height to measure the horizontal gradient in the direction of
the line joining the two sensors. Compared with total intensity measurements,
gradient measurements provide better resolution of nearby sources, and they are
insensitive to time variations in the field.
MAGNETIC SURVEY PROCEDURES AND DATA PROCESSING
Ground magnetic measurements are usually made with portable instruments at
regular intervals along straight parallel lines which cover the survey area.
Often the interval between measurement locations (stations) along the lines is
less than the spacing between lines. Ordinary land surveying methods are used
to establish stations at which measurements are made; high accuracy is not
usually required. Continuously recording instruments are sometimes mounted on
trucks (Hildenbrand, 1982); measurements can be made along road networks and in
areas where it is possible to drive off roads.
Most magnetic surveys are done from aircraft. Airborne measurements are
made along parallel flight lines that, for geologic investigations, are nor-
mally spaced 0.2 km (1/8 mile) to 9.7 km (6 miles) or more apart.1 For some
purposes, aeromagnetic surveys are made at a fixed altitude above sea level; for
other purposes they are flown at a fixed height above the ground. The pilot
may navigate visually to fly along lines drawn on maps or aerial photographs or
some type of electronic navigation system may be used for guidance. A tracking
camera or a video camera and recorder are commonly used to obtain a continuous
visual record of the flight path. In data processing, the location of the
aircraft is plotted at locations where common points on the base map and on the
tracking film are recognized; the locations for each measured value of the
field are then adjusted to the flight path by assuming that the speed and
direction of the aircraft were constant between identified locations. Errors
^English units or mixed English and S.I. units were used in making field
surveys reported here and, where appropriate, quantities are given in both
sets of units.
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in location are on the order of several tens of feet at low altitues and sever-
al hundreds of feet or more at high altitude. Where flights are over feature-
less terrain or water, the flight path cannot be recovered at all using the
photographic method and electronic navigation systems such as Doppler radar,
VLF, Loran-C, or inertia! navigation must be used for both pilot guidance and
recovery of the flight path. Use of these systems improves the accuracy of the
flight path determination, but in general, does not provide the degree of
accuracy needed for purposes such as the location of abandoned wells. Microwave
navigation systems can provide locations accurate to several meters or better.
These systems employ two or more radio transmitter-receivers (transponders)
placed at accurately surveyed sites. A transmitter-receiver and computer on
the aircraft measures the distance or range to each transponder and then com-
putes the position of the aircraft. The chief disadvantage of these systems is
that a line-of-site path between the aircraft and at least two transponders is
required at all times. Height of the aircraft above ground is usually measured
with a device called a radar altimeter. This instrument functions by measuring
the time between transmission of a pulse and its reception after being reflected
from the ground.
To make accurate anomaly maps, changes with time in the Earth's field
during the period of the survey must be considered. During severe magnetic
storms, which occur infrequently, magnetic surveys should not be made. Normal
changes during the day, sometimes called diurnal drift, are a few tens of
gammas and can be accounted for in processing the data. There are a number of
methods of correcting surveys for time variations. For ground surveys, one
method is to establish a base or reference station in the survey area and to
repeat measurements at this base at frequent intervals. Measurements at field
stations are then corrected by assuming that the field changed at a constant
rate over the survey area during the time interval between repeat base station
readings. This method works well, provided the field is relatively "quiet." In
airborne surveying, the traditional method is to fly "tie" lines across the
rows of parallel flight lines during a quiet period. The points or intersec-
tions at which the regular flight lines cross tie lines are determined and the
differences in intensity between the two sets of measurements at these points
are calculated. The flight line data are then adjusted to fit the tie line
data by assuming that the field changed at a constant rate between the inter-
sections. Usually, continuously recording magnetometers are employed at fixed
base sites to monitor temporal changes. If time is accurately recorded at both
base site and field location, the field data can be corrected by subtraction of
the variations at the base site. This method works well for surveys of small
areas, provided the base site is in or near the area. It does not work well
for surveys of large areas having dimensions on the order of tens of kilometers
since, over large areas, variations of the field with time are not uniform.
After all corrections are made, magnetic survey data are usually displayed
in the form of isopleths. Such a map shows lines of constant magnetic
intensity in the same way that a topographic map shows lines of constant ele-
vation. Survey data are also presented in the form of profiles in which the
magnetic intensity is plotted against a distance along the flight line. Vari-
ous mathematical operations are sometimes used to enhance certain features in
the data and suppress others. Geologic interpretation of magnetic anomalies is
carried out by comparison of the actual results with theoretical results
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calculated for idealized geologic models and by comparison of the results with
anomalies over known geologic features. Identification of anomalies caused by
steel casings is generally quite easy since the anomalies have a characteristic
shape. However, the problem becomes difficult when the anomaly due to the
casing is weak and there are stronger nearby anomalies caused by other cultural
and geologic sources.
For further information on the principles of the magnetic method and
survey techniques, the reader may wish to consult some of the many papers and
textbooks on the subject. The pamphlet by Breiner (1973) is a good introduc-
tion to the subject. The textbooks by Nettleton (1976), Parasnis (1975), and
Telford and others (1976) give good treatments of the subject without being
highly mathematical. For a review of more recent developments, including the
use of gradiometers, the reader might wish to consult the papers by Hood and
others (1979), and Emerson and others (1979).
ELECTRICAL PROPERTIES OF MATERIALS
Soils and rocks can conduct electricity, although not as easily as metals
such as steel. The intrinsic property of materials which determines the degree
of difficulty of driving electrical currents through the material is called
resistivity and is measured in the unit, ohm-meter. The resistivity of most
rocks is in the range of 1-10,000 ohm-m. In contrast, the resistivity of steel
is typically less than 0.000001 ohm-m. The flow of constant or direct current
through the Earth depends only on the resistivity. The flow of time-varying or
alternating current depends on other properties as well, including the di-
electric constant, which determines the way a material behaves in the presence
of electrical charges, and the magnetic susceptibility, which was discussed
previously in the section on magnetic properties. In practice, the influence
of magnetic susceptibility on the flow of alternating currents in the Earth is
usually negligible. Also, at the frequencies which are ordinarily employed in
geophysical exploration, the influence of the dielectric constant is negligible
for most Earth materials. However, some Earth materials, when excited by very
low frequency alternating currents, become electrically "polarized." As a
result, the resistance of the ground, or more properly the "impedance" of the
ground, varies with frequency. Strong polarization effects are often observed
when electrical currents flow between metallic objects and the Earth.
Electrochemical reactions between metallic objects and surrounding rocks
and soil generate electrical forces, called electrical potentials, which drive
electrical currents through the Earth. These self-potentials or spontaneous
potentials change only very slowly with time. A number of other processes,
such as the flow of ground water, can also generate self-potentials, voltages,
and currents.
ELECTRICAL METHODS
Five electrical methods, which may be of some interest in location of
steel casings, are resistivity, low frequency electromagnetic, ground pene-
trating radar, self-potential, and induced polarization. In the resistivity
method, electrical connections are made to the ground through use of metal
11

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stakes or other devices called electrodes. An extremely low frequency electri-
cal current is driven through the Earth using two electrodes, and the resultant
difference in electrical potential or voltage, which is established between
points on the surface of the Earth, is measured, usually by use of two other
electrodes. By taking the current and electrodes spacings into account, the
results are commonly expressed as "apparent resistivity" in ohm-m. The appar-
ent resistivity would be the same as the true or intrinsic resistivity if the
Earth were homogeneous. To make a resistivity map, the array of electrodes is
moved about the area of interest.
In the low frequency electromagnetic method, the source of energy is a
current flowing through a loop of wire or a current flowing through a length of
wire connected or grounded to the Earth through an electrode at either end.
The current in the wire causes a magnetic field about the wire which alternates
at the same rate as the current. Associated with this magnetic field is an
electric field that, when it passes through conductive materials such as the
Earth, causes or induces an electrical current to flow in the material. These
electrical currents flowing in the material produce a "secondary" magnetic
field which perturbs the original or "primary" field. When a grounded wire is
used, there is also a magnetic field associated with the current that is direc-
' tly injected into the Earth. The induced current in the Earth and its secondary
magnetic field depend on the resistivity of the Earth. An induction coil or
other special type of magnetometer is used to measure components of the alter-
nating magnetic field. The results of the measurements are usually expressed
as the ratio of the secondary field to the primary field and sometimes the
apparent resistivity is also computed.
From theoretical considerations and experience, we expect electromagnetic
methods using only a loop or induction source to be effective in the location
of horizontal pipelines and similar features and to be ineffective in the
location of vertical pipes. Methods which use grounded wires as sources are
expected to be much more effective in location of vertical pipes. At very
close range, currents induced directly in a casing or other metal object can be
detected with "metal detectors" (Johnston and others, 1973). However, at long
range the only hope for detection of a casing is to observe the distortion
caused by the casing in the normal flow of current in the Earth.
In the ground penetrating radar method, a very high frequency electromag-
netic wave is radiated into the ground. When the wave encounters the boundary
of a region where the velocity with which the wave propagates changes, some of
the energy is reflected to the surface where it is detected. If the velocity
of propagation is determined from other measurements, the depth of the reflector
beneath the surface can be computed from the difference between the time when
the transmitted wave left the antenna and the time when the reflected signal
was received. To map an area, the antenna is moved along the surface while the
system is operating; a display is thus obtained which resembles a cross section
of the Earth. The method is effective only when the resistivity of the rocks
is relatively high; it is not likely to be useful in most oil fields where near
surface rocks are sedimentary and have low resistivities. The method might be
useful in locating wells in igneous and metamorphic rocks and in glacial
deposits.
12

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The basis of the self-potential (SP) method is measurement of spontaneous
electrical potentials. The equipment consists of two non polarizable elec-
trodes, connecting wires and a sensitive voltmeter which presents a very high
resistance to the electrodes. Measurements of the electrical potential are
made with respect to an arbitrary fixed point in the survey area.
In the induced polarization (IP) method, very low frequency alternating
or time-varying current is driven through the Earth using two electrodes.
Potential differences are measured with two other electrodes as in resistivity
measurements. Usually, the "dipole-dipole" electrode configuration is employed
and resistivity measurements are made in conjunction with the IP measurements.
In one variant of the IP method the quantity measured is the apparent resis-
tivity at two or more frequencies. In other variations, the degree to which
the Earth becomes electrically charged (chargeability) or equivalent quantities
are measured. Rocks containing metallic minerals and some types of clay are
highly polarizable. Buried metallic objects often give large IP responses when
one or more of the electrodes is nearby (Nelson, 1977, Holladay and West,
1984).
For further information in the principles of electrical methods, the
reader may wish to consult the general textbooks by Parasnis (1975) and Telford
and others (1976). For more detailed information, the reader can consult the
textbooks by Keller and Frischknecht (1966) and Wait (1982) or many other books
and papers which deal with this subject.
13

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GROUND MAGNETIC MEASUREMENTS
In the first part of this study, ground magnetic measurements were made
near a number of known wells to obtain data that were used to evaluate the use
of both ground and airborne magnetic methods 1n locating wells. Later, addi-
tional ground magnetic measurements were made to help evaluate the results of
the airborne surveys. The first measurements were made near a number of wells
In two oil fields in Colorado. One of the fields 1s east of Denver and In-
cludes the area later used for an aeromagnetic test (Figure 3). This field
contains a number of producing and dry wells drilled during the 1970*s. The
second field 1s north of Denver near Boulder (Frlschknecht and others, 1983)
and contains many abandoned and a few producing wells.
To obtain data for use in analysis and modelling, measurements were gener-
ally made along radial lines or traverses 1n the magnetic north, south, east,
and west directions with the well at the center. The total Intensity of the
field was determined using proton magnetometers with the sensor placed on a
staff 2.4 m (8.0 ft) above the surface of the ground. Repeat readings were
made at a base station, and the results were used to correct the data for
diurnal drift. At most well sites a recording proton magnetometer was operated
to monitor the diurnal drift. Before making readings, all visible steel trash
such as oil drums, valves, and pipes was removed from the immediate vicinity of
the traverses. Some of the traverses were over buried or partly burled steel
trash which could not be readily removed. In the immediate vicinity of some of
the wells the magnetic gradients were so large the proton magnetometers were
not capable of making reliable measurements, but the loss of this data was
generally not a serious problem. In addition to the total intensity measure-
ments, vertical and horizontal gradients of the Intensity and the inclination
of the field were measured at a number of wells In both Colorado test areas.
Initial processing and plotting of data were done on a desk top computer, and
then the data were transferred to a larger computer for further analysis.
In evaluating airborne surveys, the ground magnetometer was used to
quickly determine the sources of aeromagnetic anomalies. Aerial photographs
and maps were used to locate the site of the anomaly on the ground. Measure-
ments were then made on a very rough grid established by pacing. Readings were
taken every 6-10 m (20-30 ft) but generally were not recorded. Usually it
required only a few minutes to find the casing, 1f it existed, or a little
longer to rule out the existence of a casing 1f none was found. When a casing
was found, a few readings directly over or near the well were generally
recorded.
This summary report includes only a few examples of the data which were
collected and analyzed; the complete set of data Is contained 1n the reports by
Frischknecht and others (1983, 1984). An example of ground magnetometer data

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near well No. 4, in the Piney Creek, Colorado, area (Figure 3) is shown in
Figures 4 and 5. The circles indicate the measured values of the intensity, F,
of the field and the solid line is calculated from a theoretical model de-
scribed in the next section. As predicted by theory, the experimental results
show that north-south profiles over a well are asymmetrical; the peak value of
the field is a little south of the well and then it drops to slightly less than
its normal value in a small region north of the well. East-west profiles are
symmetric except for disturbances due to sources other than the well. Well No.
4 produced one of the largest ground and airborne anomalies in the Piney Creek
area. A small disturbance, which is due to an unknown object, occurs about
20 m (60 ft) east of the well (Figure 4).
As another example, data .for PIW well No. 17 in the Horseshoe Lake,
Oklahoma, area (Figure 6) are shown in Figures 7 and 8. The anomaly is much
smaller in amplitude and narrower than in the previous example. The airborne
anomaly is only about one gamma for well No. 17, which is near the threshold of
detection. A secondary feature, perhaps caused by a buried piece of pipe,
occurs at about 20 m (70 ft) along the east-west traverse (Figure 8).
The anomalies illustrated in Figures 4 and 5 and 7 and 8 diminish rapidly
with distance from the well. To be certain of locating a well with a ground
magnetometer, the distance interval between measurements must be small. From
study of the results in Colorado, Frischknecht and others (1983) suggested that
a suitable grid for locating wells with a total intensity ground magnetometer
should consist of stations spaced at 10-m (30 ft) intervals along traverse
lines spaced 16-m (50 ft) apart. The results did not indicate that gradient
measurements would be more useful than total intensity measurements.
15

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104*45'
104*30'
yp

~r~

Ife-

BENNETT
+ °-

WATK1NS

©
A R E AJ^jt



*
Pinty Cr««k


nT
mm
N
1

i
-S
- +


-
5 0 5
MILES
10 15

	20
5 ' o a l~To iT 20 *25 30
i i i i i i	'	*	'	'i	'	'
KILOMETERS
Figure 3. Location of the Piney Creek test area.
16

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N
60000
i »
O O Observed
	 Calculated
. OBflOO
IL.
06000
ooo
00000,
o
o
(M
DISTANCE (feet)
Figure 4. North-south ground magnetic profile over well no. 4.

-------
O O Observed
¦	Calculated
0I6TANCE (feet)
Figure 5. East-west ground magnetic profile over well No. 4.
¦}

-------
97*30'
ARCADIA
JONES
illiiil
» &.
97*15'
Arcadia Test Area
S
LUTHER
Horaashoe Lake
Taat Areag^
'////////A
V///A
g Oklahoma City
Taat Area
23 Moora Taat Araa
VTTfr

HARRAH
0
¦ ¦ * ¦
MILES
10
15
20
5 0
	
10
i
15
20
25
30
KILOMETERS
Figure 6. Location of the Oklahoma test area.
19

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ro
o
¦MM.
M4N.
¦IIM.
•MN.
BUN.
611N.
BUM.
¦MM.
e—9 o o—
O O Obuned
¦	Calculated
• o
J	1	1	.	I	i	I	i	I	.	L
J	.	L
S
T
• •
2 S
8
7
8
• • • •
8 5 5 £
DISTANCE I roll
Figure 7. Observed and calculated north-south magnetic profile over
well No. 17, Horseshoe Lake test area.

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Observed
Calculated
m
¦MM,
BMM,
m
DISTANCE ir««ll
Figure 8. Observed and calculated east-west magnetic profile over
well No. 17, Horseshoe Lake test area.

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INVERSION OF GROUND MAGNETOMETER RESULTS AND MODELING
There is no simple and direct way to predict the results of airborne
surveys from ground results. Also, it is difficult to make a qualitative
comparison of the results from different wells if only the magnitude and shape
of the anomaly are used. To circumvent some of these problems, a mathematical
model of the well was employed. In its most simple form, this model consists
of a north and a south magnetic pole separated so that they are approximately
at the ends of a casing. Through a process called inversion, sets of magnetic
poles which would produce essentially the same anomaly as the one observed
were determined; the comparison between the observed data and the calculated
data for theoretical models is illstrated in Figures 4 and 5 and 7 and 8.
Using the pole strengths and distances found by inversion, it is a simple
' matter to compute estimates of the airborne results for various wells from
their theoretical models.
Estimated airborne anomalies were calculated at various heights and
horizontal distances for several Colorado wells. Total intensity as well as
horizontal and vertical gradients of the total intensity as well as the total
intensity were determined. When viewed in isopleth form, total intensity
anomalies are almost circular in shape (Figure 9). To detect such an anomaly,
one or more flight lines must pass close enough to the center of the anomaly
that a detectable response is observed. The size of the anomaly which can be
detected depends on: (1) the sensitivity of the magnetometer used, and (2)
anomalies or "noise" due to geologic sources and cultural features other than
the target. After considering the sensitivities of existing magnetometer and
magnetic gradiometer systems, it appeared that the range over which a casing
can be detected is greater for total intensity measurements than for gradient
measurements.
From the model studies, it was decided to use a height of 61 m (200 ft)
and a spacing between lines of 100 m (328 ft) for the experimental airborne
surveys. The use of a greater height and line spacing would have decreased
the cost of the surveys but increased the probability of not detecting wells.
Use of a substantially smaller height and line spacing is impractical with a
fixed wing aircraft.
22

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400
300
200
100
100
200
300
400
100 200 300 400
400 -300 -200 -100
0
Distance (feet)
Figure 9. Calculated isopleths of total intensity (gammas) at a height of 200
feet above a well. The lines show spacing of north-south or east-west flight
lines necessary to measure a two-gamma anomaly in the worst case.
23

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AIRBORNE MAGNETIC MEASUREMENTS AND RESULTS
Airborne surveys were made in one test area near Denver, Colorado (Figure
3) and in four test areas near Oklahom City, Oklahoma (Figure 6). The aircraft
used was a Fairchild Porter (Figure 10) which has a single turbine engine and
is designed for short take-offs and landings (STOL). Its high rate of climb,
low stalling speed, and the reliability of the turbine engine make this air-
craft suitable for very low-level surveying. The main parts of the geophysical
system were a high sensitivity proton magnetometer, a microwave navigation
system to determine the horizontal position of the aircraft, a radar altimeter
to determine the height above ground, and a data acquisition and recording
system. Ancillary equipment included sensors for monitoring roll, pitch, and
yaw of the aircraft and a 35-nrn tracking camera. Since the anomaly from a
casing can be very small, high resolution of the field was required. There are
many potential sources of noise in making high resolution airborne magnetometer
measurements. In particular, some of the component parts of aircraft have both
induced and permanent magnetization and when the altitude of the aircraft
changes the magnetic field changes at the position of the magnetometer sensor.
The sensor was placed at the end of a boom or stinger attached to the tail of
the US6S aircraft to remove it as far as possible from the magnetic parts.
Various measures were taken to reduce the fields of the aircraft, and compen-
sating fields were introduced to cancel the remaining fields. Nevertheless, a
small amount of noise, caused chiefly by electrical currents induced in the
airframe (eddy currents) when it rotates in the Earth's field, was introduced
into the data. By recording the motions of the aircraft, much of this motion
induced noise was later removed through computer processing. Also, there was a
slight error termed "heading effect" which depended on the direction of the
aircraft and which was a result of imperfect cancellation of the aircraft's
field.
The principal concern in setting up the microwave navigation system was to
maintain a clear, or line-of-sight, transmission path and suitable angles
between the aircraft antenna and the transponders. Topographic maps were used
to select tentative transponder sites, preferably in clearings on tops of
hills. Final selection of the sites was made after field examination. Contact-
ing and obtaining permission from landowners for temporary use of their land
was an important but time-consuming part of this process. Once the sites were
selected, land surveys were made to accurately measure the direction and
distance between sites and to locate the sites relative to roads and other
landmarks. The transponders, which are small, light-weight, battery-powered
units, were placed on top of temporary, 9.1 m (30 ft) high, steel masts; in the
areas surveyed, this generally placed the transponders above the level of
nearby treetops. After completing the surveying for each area, the data were
reduced and the grid for the aeromagnetic survey was planned. Each grid con-
tained a flight line along a rural road or other straight-line landmark. This
24

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Figure 10. Fairchild Porter aircraft used in this study.
25

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line was flown at the beginning of the survey to make certain there were no
serious discrepancies between the aircraft location, as indicated by the naviga-
tion system, and the position as determined visually.
To avoid excessive turbulence, flights were made either early in the
morning or late in the afternoon. The transponders were placed in operation on
the preceding day or on the day of the flight and the base station magnetometer
was placed at its site shortly before the flight began. In general, each area
was completed during a single flight.
Several weeks before field operations began, the project was discussed
with the Federal Aviation Administration's General Aviation District Office in
Oklahoma City and a request to make the necessary low-level flights was
submitted. Immediately before beginning flight operations, a press release
describing the operations was distributed to local newspapers and radio and
television stations. The primary reason for the press release at that time was
to inform the public of operations by a low-flying aircraft; otherwise, avia-
tion and law enforcement agencies might have been deluged with many reports
about a low-flying aircraft.
Most of the data processing was done by a private contractor. The first
step was to edit the field tapes to eliminate data taken in turns and other
extraneous data. Next, the actual flight path of the aircraft was calculated
from the results provided by the microwave navigation system. This was accom-
plished without any particular difficulty with a relative accuracy estimated at
±5 meters (±16 ft) (Frischknecht, and others, 1984). The results for each
line were plotted on a map at a scale of 1:6,000 (1 cm = 60 m).
The magnetic field was corrected for diurnal variations using the tie line
method. In making diurnal corrections it was necessary to consider differences
in elevation between the tie lines and the traverse lines at their intersec-
tions; elevation data were available from the record of radar altimeter output.
Corrections for a small amount of heading error were made simultaneously with
the diurnal corrections. The average mistie error after the adjustment was 0.2
gammas. Next, the magnetic data were gridded; that is, values of the field
were estimated at points spaced about 25 meters apart in both the north-south
and east-west directions. The gridded data were used to prepare isopleth maps
at a scale of 1:6,000 using an interval between isopleths of two gammas.
Profiles of the data along the flight lines contain much more detail than
can be displayed on isopleth maps. Consequently, it was important to remove as
much noise as possible from the profile data. Maneuvers were made during a
calibration flight at high altitude where the magnetic field changes very
gradually with distance. Analysis of this data showed that only roll maneuvers
caused significant errors in the magnetometer measurements. A step-by-step
procedure was used to find the relationship between roll and the sources of
error due to rotation of the sensor and the induced, permanent, and eddy
current fields of the aircraft. Once these relationships were established, the
information from the roll sensor was used to estimate the maneuver noise. The
noise, which was usually less than one gamma, was then subtracted from the
magnetometer measurements and the final results, along with auxiliary informa-
tion, were plotted at a scale of 1:6,000.
26

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As an example of typical profile data from Oklahoma, part of flight line 4
for the Arcadia test area (Figure 11) is shown in Figure 12. The bottom plot,
which shows the corrected magnetic field, is "folded"; that is, when the trace
goes off the top of the plot it reappears at the bottom. The quantity shown in
Figure 12 is the actual field less about 53,000 gammas. The traces for the
radar altimeter and the barometric altimeter give the height of the aircraft
above ground and above sea level, respectively. The differential roll, pitch,
and heading traces give the maneuvers or motions of the aircraft in degrees.
The maneuver noise correction was calculated from these maneuvers and has been
used to determine the corrected magnetic field. In this example, the maneuver
noise is small; in other extreme cases, it exceeds one gamma. The residual
noise in the corrected magnetic profile is about 0.2 gamma or less in this
example. The magnetic field peaks, numbered 37, 33, and 26, correspond to
anomalies with the same numbers on the magnetic isopleth map of the area (Figure
13). The peaks, which are caused by wells, are superimposed on a small, more or
less uniform magnetic feature in which the field decreases from south to north.
Aircraft flights were made over well No. 4 in the Piney Creek, Colorado,
test area (Figure 14) at nominal heights of 30.5, 45.7, 61 and 76.2 m (100, 150,
200, and 250 ft) to determine how the anomaly weakens with height above the
ground (Figure 15). Earlier, Frischknecht and others (1983) estimated the
anomaly at these heights from the ground data in Figures 4 and 5. Well No. 4
is not an ideal selection for this study because its anomaly is distorted by
variations in the magnetization of nearby rocks making it difficult to estimate
the magnitude of the anomaly. However, comparison of Figure 15 with Figures
93-99 in the report by Frischknecht and others (1983) indicates that the magni-
tude of the anomaly was underestimated by about 21% at 29.7 m (97.5 ft) and by
about 23% at 76.2 m (250 ft). Underestimation of the anomaly is not surprising
since the calculated results for the model do not fit the shoulders of the
observed curve (Figures 4 and 5) as well as is desirable. In any case the
agreement between predicted and actual results is good. There are enough other
uncertainties in the design of surveys so that an error of 23% in prediction of
the size of anomalies is not important.
One of two sheets of the isopleth map for the Arcadia test area (Figure 11) •
is shown as an example of airborne data where there are many wells (Figure 13).
The isopleth interval of the map is 2 gammas; an arbitrary value has been sub-
tracted from the field. On this sheet, 40 distinct aeromagnetic features have
been labelled. The map is dominated by these features, although there is a
subtle regional trend with the field generally increasing eastward. Some of
the anomalies cover a larger area than typical anomalies caused by only one
well; these have multiple designations, for example 15, 15a, 15b. The
following list shows the association of numbered anomalies with photograph-
ically identified wells (PIW's) (Stout and Sitton, 1983) and with the results of
ground checking.
Anomaly Number	Association or Probable Source
6, 9, 10, 11, 12, 13, 14, 16, Associated with one PIW.
18, 20, 22, 23, 25, 26, 28,
29, 30, 32, 33, 34, 35, 36,
38, 39, 40
27

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97"ir30"	R1W
T15N
T14N
OKLAHOMA CO.
N
10 STUDY AREA 11
N
' MILE
0
Figure 11. Map of Arcadia, Oklahoma, area, sections 3, 10, 11, and
The hachure pattern shows the area included in Figure 13.
28

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MANEUV. NOISE
OOftr-GAMMAS
DIFFERENTIAL
ROLL-DEG.
DIFFERENTIAL
PITCH-DEG.
DIFFERENTIAL
HE ADING-DEG.
BARO. ALTMTR
METERS
RADAR ALTMTR
METERS
o.ro
-».ri
4«20
	1	
44*0
	1	
4440
COR. MAS
FELD-GAMMAS
-•

•oo
at
-3
-3
'100
f 6
0
»-
H MILE
Figure 12. Airborne profile data from Arcadia area. The numbers at top
and bottom are identification numbers associated with each reading,
and the numbered anomalies correspond with those on Figure 13.
29

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Figure 13. Total intensity gammas isopleth map for part of Arcadia area.
30

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104*37'30*
R«5W
CO
N
I
Figure 14. Hap of the Piney Creek, Colorado, area. The
hachure pattern shows the area included in Figure 16.
31

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s
N
200-
100-
Height of Plane
250 feet
200 feet
150 feet
100 feet
0	5000	10000 feet
1	I	I
Figure 15. Aeromagnetic profiles for different aircraft heights
over well No. 4, Piney Creek area.
32

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Anomaly Number
Association or Probable Source
8-8a, 21-21a,	Each complex anomaly is associated with two
27, 27a, 27b	or three PIW's.
3f 17	Outside section where photointerpretation
was done; but are probably due to wells.
2	Outside section where photointerpretation
was done; probably due to a horizontal
pipeline and perhaps a well.
4, 5	Outside section where photointerpretation was
done. Anomaly 4 is associated with a well and
derrick and 5 is associated with a large pipe
of recent origin observed during field check.
24-24a	Anomaly 24a is associated with a PIW and 24 is
associated with a feature located during field
checking which may be a capped well or the
terminous of a pipeline; the characteristics of
the anomaly suggest a well.
31_31a	Associated with one PIW, two buildings, and a
tank. The anomaly suggests that there might be
another wel1.
19, 37	Apparently caused by wells which were not
identified from photos; anomalies were not
field checked.
7_7a	Apparently caused by one PIW plus tanks
and other facilities.
15-15a-15b	Associated with one PIW and another well and
other facilities.
There are three PIW's which are not associated with easily recognizable
anomalies; they are labelled with Roman numerals. Field checking and
examination of the aeromagnetic profiles yields the following information:
Well No.	Comments
I	Anomaly 15b is too far south to be caused by
well I. The profile for flight line 10 shows a
change in slope probably due to I but generally
the aeromagnetic expression of I is masked by
the large anomaly 15-15a. A distinct ground
magnetic anomaly over I was observed.
33

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Well No.
Comments
II (identified as
a possible well)
Ground checking showed a cleared area and a few
pieces of small pipe which produced small
anomalies but no anomaly typical of a casing
was found. This probably represents a site
which was abandoned before a casing was placed.
Ill
Examination of the aeromagnetic profiles shows
distinct anomalies of 5 and 4 gammas on flight
lines 6 and 7, respectively; they are no doubt
caused by well III but have been suppressed on
the isopleth map by gridding and smoothing.
The site was not field checked.
Considering only section 3 (Figure 11), which encompasses most of this
sheet, 36 wells were identified from photos; one of these sites does not con-
tain a casing. The records search by Fairchild and others (1983) identified 41
wells in section 3; Stout (oral communication, 1984) has interpreted the ex-
istence of 37 wells from a comparison of aerial photos and the original records.
' Magnetic contour or profile anomalies correlate with all 35 original PIW's.
There are two other anomalies, 19 and 15b, which are thought, by Stout, to be
wells plus two more, 24 and 31a, which may be wells. All wells for which
information is available have at least 76 m (250 ft) of surface casing and many
have more than 122 m (400 ft). Diameters of the surface casing are 21.9, 24.4,
and 32.8 cm (8-5/8, 9-5/8, and 10-3/4 in). Part of the smaller casing, usually
14.0 or 17.8 cm (5-1/2 or 7 in) diameter, has been removed at many of the wells.
As a generalization, the density of wells is greater and the anomalies are
larger and more uniform in magnitude for this area than for the rest of Arcadia
and the Horseshoe Lake area. The regional trend of the Earth's field is gener-
ally steeper in some of the other areas such as Horseshoe Lake. In the Moore
test area there is evidence for variations in the magnetization of the near
surface rocks, but anomalies due to geologic sources are not a serious problem
in interpretation of any of the Oklahoma data. The Horseshoe Lake area has
fewer anomalies due to manmade (cultural) sources than Arcadia, sheet 1, but
the other Oklahoma areas probably have more such features. In some cases shape
and extent of anomalies was very helpful in distinguishing between those due to
casings and those due to other cultural sources. Probable sources of cultural
anomalies, such as transmission line towers, bends in pipelines, and steel
buildings were sometimes identified from aerial photographs and topographic
maps. When used, ground checks with a magnetometer usually revealed the sources
of anomalies; but, in one or two instances, large ground magnetic anomalies
from multiple sources such as tanks, pipelines, and steel buildings may have
masked a weak anomaly from a casing.
In the Piney Creek, Colorado, test area (Figure 14) there are many sharp
anomalies which are due to variations in the magnetization of the near-surface
rocks (Figure 16). Some of these anomalies have the same appearance as anom-
alies caused by casings. Study of the airborne profiles was helpful but not
always definitive in determining the source of the anomalies. A considerable
amount of ground checking was necessary in this area to distinguish between
34

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Figure 16. Total intensity gamma isopleth map for part of Piney Creek
area. Triangles indicate locations of known wells.
35

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anomalies caused by casings and those caused by geologic sources; the geologic
anomalies are not a serious problem in interpreting ground magnetometer results.
The airborne method would be somewhat more effective in an area such as this if
the flight height and line spacing were decreased.
Considering all four test areas in Oklahoma, there is good agreement
between the results from the magnetic surveys and those from photointerpre-
tation. Most PIW's produce aeromagnetic anomalies and most magnetic anomalies
which are not due to other obvious cultural sources are associated with PIW's.
Following are three categories of exceptions to this generalization:
Category 1: PIW's that are isolated from other wells or other sources of
anomalies, and that produce no aeromagnetic anomaly.
Category 2: PIW's which may produce weak anomalies but which are located so
close to the source of a strong anomaly that the weak anomaly is
masked by the strong anomaly.
Category 3: Aeromagnetic anomalies not associated with PIW's where ground
checking has indicated a casing type anomaly and also, in some
cases, physical evidence of a well.
A summary of the numbers of these three categories of PIW's and anomalies
follows:
Area
Category 1. PIW's
Isolated From Other
Sources
Category 2. PIW's
Near Other
Sources
Categroy 3.
Casing Type
Anomalies
Without PIW
Arcadia
Horseshoe Lake
Moore
Oklahoma City
2-	one was checked
and has no ground
magnetic anomaly
3-	two were checked
and have no ground
magnetic anomaly
2- both were checked
and have no ground
magnetic anomaly
4
1
Caution must be used in evaluating the overall significance of category 3
anomalies; there would, no doubt, have been many more had all of the aero-
magnetic anomalies been ground checked. However, according to Stout (oral
communication, 1983, there is weak or inconclusive evidence in aerial photo-
graphs for the existence of wells associated with some of the anomalies in
category 3. Most of the PIW's in category 1 were identified as possible wells
36

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or dry holes, and some of them probably represent sites which were prepared for
drilling but where casing was either never emplaced or has been removed.
In some cases specific PIW's and magnetic anomalies were correlated with
particular wells listed in the records search. Generally, there was some
difficulty in establishing one-to-one correspondence between the data sets
because the locations given in the records are not sufficiently accurate and
because of other problems with the records. However, comparisons were made
between the total numbers of wells found in each section from the records and
the probable number of wells found from photointerpretation and magnetic
surveys. With the exception of one section in the Horseshoe Lake area, the
number of wells which were photographically identified and which have magnetic
anomalies is generally less than the number found from the records. However,
in all Oklahoma areas except Moore, the total number of magnetic anomalies
which may be caused by casings equals or exceeds the number of wells found from
the records.
In the Piney Creek, Colorado, test area there are 17 wells which are known
from records or from ground magnetic measurements or visual evidence. Two of
these did not cause recognizable aeromagnetic anomalies. A weak anomaly from
one of these wells is probably obscured by a strong anomaly of geologic origin;
there is no apparent reason for the failure to detect the other well. In the
Piney Creek area there are a number of anomalies which look like they could be
caused by wells but which are not associated with known wells. Several of
these anomalies were ground checked but no casings were found.
Due to the limitations of the other data sets the exact number of wells
within the areas covered by the aeromagnetic surveys is unknown. However, from
the evidence we concluded:
1.	Considering all five test areas, aeromagnetic anomalies are probably
associated with 95-98 percent of the wells.
2.	More wells were detected by the aeromagnetic surveys than by the
initial photointerpretation.
3.	More features which are not wells were identified as possibly being
wells from the aeromagnetic data than from the photograph evidence.
The anomalies over most wells in the Oklahoma test areas were much larger
than required to be easily recognizable; typically, anomalies over the wells in
Colorado were smaller. In general, the magnitude of the anomalies depends on
the amount and size of the casings, but there are many exceptions to this rule.
A few wells in both regions, which according to the records should have enough
casing to produce substantial anomalies, produced only weak anomalies. The
reasons for this are not known; the records may be inaccurate, the properties
of the steel may be different from the norm, or the casings may have been
selectively corroded away. Anomalies due to sources in near-surface rocks
cause difficulty in interpretation of the Colorado data, but they are only a
minor problem in interpretation of the Oklahoma results. Anomalies of cultural
origin are present in all test areas, but usually they are easily recognized.
We conclude that most wells containing on the order of 60 m (200 ft) or more of
37

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21.9 cm (8-5/8 in) diameter or larger surface casing can be detected by air-
borne measurements. Much smaller amounts of pipe can be found with a ground
magnetometer; however, very closely spaced measurements are then required.
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ELECTRICAL MEASUREMENTS AND RESULTS
Electromagnetic measurements using two different instruments with loop
sources showed no indication of wells (Frischknecht and others, 1983).
Dipole-dipole resistivity/IP measurements made near well No. 2 in the Piney
Creek, Colorado, test area showed little indication of the casing (Washburne,
J., 1984); this was somewhat surprising since theory (Holladay and West, 1984)
and experience in industry indicate that casings often cause resistivity or IP
anomalies at distances which may be greater than the detection ranges for
ground magnetometer surveys.
SP measurements were made in the vicinity of 11 wells using a fixed base
electrode and a roving electrode of lead-lead chloride construction. Distinct
and fairly large anomalies were found in the vicinity of four of the wells.
Small anomalies were observed in the vicinity of most of the other wells. As
an example, the results obtained near well No. 7 in the Piney Creek, Colorado,
area are shown in Figure 17. A distinct but rather narrow anomaly occurs
directly over the well. However, the profiles show a number of other small
anomalies of unknown origin. Such anomalies would cause difficulty in the
interpretation of SP results when searching for concealed wells. The SP method
might be useful to a limited extent in verification of the presence of
suspected wells.
Electrical methods are generally more expensive and more cumbersome to use
than magnetic methods. From this limited study of electrical methods it
appears that they are not nearly as reliable as magnetic methods in locating
casings.
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A ad ^ si sd iifriifri«ififliaa2bb
• XtfU
1 a U & ikibibikik'ik
X(FU
Figure 17. Self-potential profiles over well No. 7,
Piney Creek, Colorado, area.
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PLANNING AND MANAGEMENT OF GEOPHYSICAL INVESTIGATIONS
FOR LOCATING ABONDONED WELLS
The possibility of using geophysical methods should be considered
whenever there is a need to search for abandoned wells. Unless the problems
are very unusual, the magnetic method is the only geophysical method which
should be considered. Depending on the problem, there are several different
ways and levels at which magnetic methods should be applied, including:
1.	In some cases there may be a need to confirm the existence of a casing
or to pinpoint the location of a known but concealed well. If the
search area is only a few acres, a casing may be identified and located
very accurately by a rapid and inexpensive ground magnetometer survey.
An experienced person can make the measurements and interpret the
results immediately in the field. Less experienced technicians can
make the field measurements and plot the data for later interpretation
by an experienced person. An organization which has considerable need
for this type of work should probably develop an "in-house" capability.
2.	In some cases, such as in searching an area of review around a site
for a proposed injection well, it may be appropriate to use the ground
magnetometer to systematically search for wells. If access to the
property is not a problem, ground surveys generally will be cheaper
than airborne surveys for areas of a few square kilometers or less.
We recommend that such surveys be designed and progress and results be
evaluated by a competent geophysicist or by someone else who has been
properly trained and has had experience in doing this kind of work.
3.	Airborne magnetic methods are more cost effective than ground magnetic
methods for surveys of areas greater than several square kilometers or
for surveys of several smaller areas in the same general area. How-
ever, if access to the property is difficult or impossible, it may
also be worthwhile to use an aircraft for a small area. A specialist
should design the survey, monitor data acquisition and processing, and
evaluate the interpretation of the results.
To locate or verify the existence of suspected casings, very little
equipment is required. A proton magnetometer with a sensitivity of one gamma
is adequate; solid state memory is not required because it will not be
necessary to record very many readings. If aerial photographs or very
detailed maps are not available to locate the site, some sort of surveying
aids are necessary. If the site is not far from a known landmark, a compass
and a hip (thread) chain or other simple means of measuring distances can be
used. If the site is several hundred meters from a known landmark, it may be
necessary to use more accurate surveying instruments. The personnel performing
the work should have some knowledge of surveying practices and should be
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experienced in using aerial photographs or surveying equipment, as required.
The necessary skills to operate the magnetometer can be learned from reading
instrument manuals and textbooks, supplemented by a brief period of working
with someone with more formal training and experience.
To carry out systematic ground surveys on a preplanned grid to detect and
locate abandoned wells, the use of a magnetometer with a memory is recommended.
This will increase the rate of progress and decrease the likelihood of recording
data incorrectly. At a minimum, a suitable interface and a printer or a micro-
computer with printer are needed to copy the contents of the magnetometer
memory and make a permanent record of the data. Preferably a microcomputer with
a disk or tape drive to store the data and a plotter to present the data in
graphical form should be used. As in checking sites, if the survey lines are
relatively short, they can be established with a compass and hip chain. If the
lines are more than a few hundred meters long, it will probably be necessary to
use a theodolite or other more accurate means of establishing directions.
Persons without previous geophysical experience can be trained to make the
measurements and process the data. However, we recommend that a competent
geophysicist design the survey, periodically monitor the work, and review the
interpretation of the results. There are potential pitfalls and problems, even
' in "routine" work, and assistance from a geophysicist is likely to increase the
cost-effectiveness of the work.
The necessary equipment for airborne surveys is considerably more complex
than that required for ground surveys. The aircraft can be either fixed-wing
or rotary-wing. Federal Aviation Administration requirements are less stringent
for rotary-wing than for fixed-wing aircraft in operating over populated areas.
However, hourly costs for operating a small fixed-wing aircraft are usually much
less than for operating a rotary-wing aircraft. The magnetometer should have a
sensitivity better than one gamma and should take readings at a rate of about
two per second or faster. Considerable care must be taken to properly install
the magnetometer in the aircraft. If a fixed-wing aircraft is employed, the
fields of the aircraft must be properly reduced and compensated and maneuvers
should be monitored. If a helicopter is used, the sensor can be towed beneath
the aircraft to remove it from the influence of the helicopter.
In terrain where there are many landmarks, it may be possible to navigate
a helicopter visually and to recover the flight path adequately with a tracking
camera. If there are not enough good landmarks or if a fixed-wing aircraft is
used, it will be necessary to use an electronics navigation system for pilot
guidance and recovery of the flight path. Under ideal circumstances, this
might be a system such as Doppler radar or Loran C, which does not require
local transponders; but, in most cases it will probably be advisable to use a
microwave, transponder based, system. A radar altimeter is necessary for pilot
guidance and to furnish a record of the vertical position of the aircraft. A
means for formatting the information from all of the sensors and storing it on
magnetic tapes or disks is required and substantial computer capability is
necessary to process and display the data after it is collected.
Only well trained and experienced specialists should attempt to carry out
aeromagnetic surveys. An experienced interpreter should review the results of
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the interpretation. In most cases it will be desirable or necessary to ground
check some of the aeromagnetic results before a final interpretation is made.
While the results obtained in this study should be useful in planning
surveys in other areas, specific information on each new area should be obtained,
if possible. The most important questions are:
1.	What size anomalies are expected from wells in the area? This ques-
tion may be answered by making measurements near a few known wells,
provided those wells are representative of others in the area. If
this is not possible, rough estimates of the expected anomalies can be
made from the length and size of the casing in typical wells, provided
this information is available from records.
2.	Will anomalies due to geologic sources interfere with recognition of
anomalies due to casings? This question may be addressed by study of
existing geologic and magnetic maps of the area and by making a few
ground magnetic traverses.
3.	Will anomalies due to cultural sources interfere with interpretation
of the results? Most manmade objects which may cause interference can
be recognized by inspection of the area from roads or from an aircraft
and from a study of aerial photographs and maps.
Selection of persons and organizations to provide needed technical advice
and services is critical particularly if airborne surveys are to be made.
Surveys which are not adequately designed and carried out will not be effective.
On the other hand, a survey can be overdesigned and implemented in such a
fashion that, although effective, it costs much more than necessary. Great
caution should be exercised in dealing with anyone who is marketing a radically
new device or method, particularly if the principles of the device or method
must be kept secret.
It is common practice for petroleum and mining companies to obtain needed
geophysical data from geophysical contractors and to maintain a staff of geo-
physicists who design surveys, manage contracts, and interpret the results.
Companies who do not have an inhouse staff often rely on consultants or con-
sulting firms for managing their contracts and interpreting survey results.
Some geophysical contracting companies have the capability to design surveys
and interpret the results as well as to conduct surveys.
Unless the agency or company requiring geophysical services has had previ-
ous experience with geophysics, we recommend the use of a consultant, at least
initially. The consultant(s) should be trained and experienced in geophysics.
Engineers or physicists usually are untrained in geology and they may make
mistakes by ignoring geological conditions or by misinterpreting them. Geolo-
gists often lack training in geophysics and physics and they may make mistakes
regarding physical aspects of the problem. Most geophysicists have had adequate
training and experience to deal with any problems encountered in making ground
magnetic surveys. However, few geophysicists have had the necessary experience
to enable them to critically monitor and evaluate the acquisition and processing
of high resolution aeromagnetic data. The qualifications and experience of
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prospective consultants and contractors should be carefully considered. If
possible, evaluations of the contractors' previous performance should be ob-
tained from other clients.
Lists of consultants, consulting companies, service companies, instrument
manufacturers, and companies which use geophysical services are published
annually in The Geophysical Directory by the Geophysical Directory, Inc., P.O.
Box 13508, Houston, Texas 77219, and in The Leading Edge. Advertisements for
geophysical services, consultants, and equipment and professional directories
are carried in several journals, generally available in technical libraries,
including:
Geophysics
The Leading Edge
Geophysical Prospecting
First Break
Mining Engineering
Geotimes
The Departments of Earth science or geology and geophysics at many uni-
versities are potential sources of advice and help. Faculty members may be
available for consulting; advanced students may be available in the summer to
carry out and interpret ground magnetometer surveys.
We suggest that the technical personnel who are responsible for the design
and conduct of geophysical surveys and the interpretation of the results should
consult the USGS open-file reports by Frischknecht and others (1983, 1984).
Public agencies that have a need to locate wells may, in some cases, be
able to obtain help from other public agencies. Several states have agencies
concerned with natural resources and geology which have expertise in geophysics.
Several Federal agencies, including the U.S. Geological Survey and the Bureau
of Mines, have programs in geophysics. In some cases there may be a possibility
for cooperative work between agencies.
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REFERENCES
Breiner, S., 1973, Applications manual for portable magnetometers:
Geometries, Palo Alto, Ca., 58 p.
Donovan, T. J., R. L. Forgey, .and A. A. Roberts, 1979, Aeromagnetic detection
of diagenetic magnetite over oil fields: American Association of Pet.
Geologist Bull., V. 63, No. 2, p. 245-248.
Emerson, D. W., and others, 1979, Applied interpretation symposium open
session: Bull. Aust. Soc. of Expl. Geoph., V. 10, No. 1, p. 120-136.
Fabiano, E. B., N. W. Peddie, D. R. Barraclough, and A. K. Zunde, 1983,
International Geomagnetic Reference Field 1980 - Charts and Grid Values
(IAGA Bulletin No. 47): U.S. Geological Survey Circular 873, 142 p.
Fairchild, D. M., C. M. Hull, and L. W. Canter, 1983, Selection of flight
paths for magnetometer survey of wells: University of Oklahoma, 264 p.
Federal Register, 1979, Proposed Rules—Notices: Federal Register, V. 44, No.
78, p. 23738, 23744, 23746, 23754, 23755.
Frischknecht, F. C., L. Muth, R. Grette, T. Buckley, and B. Kornegay, 1983,
Geophysical methods for locating abandoned wells: U.S. Geological Survey
Open-File Report No. 83-702, 54 p., 151 figs.
Frischknecht, F. C., P. V. Raab, R. Grette, and J. Meredith, 1984,
Aeromagnetic surveys for locating abandoned wells: U.S. Geological Survey
unpublished report.
Hildenbrand, T. G., 1982, Models of the southeastern margin of the Mississippi
Valley graben near Memphis, Tennessee from interpretation of truck-
magnetometer data: Geology, V. 10, p. 476-480.
Holladay, J. S., and G. F. West, 1984, Effect of well casings on surface
electrical surveys: Geophysics, V. 49, No. 2, p. 177-188.
Hood, P. J., M. T. Holroyd, and P. H. McGrath, 1979, Magnetic methods applied
to base metal exploration: Geol. Sur. of Canada Econ. Geol. Rep. 31,
p. 77-104.
Johnston, K. H., H. B. Carroll, R. J. Heemstra, and F. E. Armstrong, 1973, How
to find abandoned oil and gas wells: U.S. Bureau of Mines Information
Circular 8578, 46 p.
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Keller, G. V., and F. C. Frischknecht, 1966, Electrical methods in geophysical
prospecting: New York, Pergamon Press, 519 p.
Nelson, P. H., 1977, Induced-polarization effects from grounded structures:
Geophysics, V. 42, No. 6, p. 1241-1253.
Nettleton, L. L., 1976, Gravity and magnetics in oil prospecting: New York,
McGraw-Hill, 464 p.
Parasnis, D. S., 1975, Mining Geophysics (2nd ed.): New York, Elsevier, 395 p.
Stout, K. and M. Sitton, 1983, Abandoned well study Oklahoma and Cleveland
counties Oklahoma: Report no. TS-PIL-83051, U.S. Environmental Protection
Agency.
Telford, W. M., L. P. Geldart, R. E. Sheriff, and D. A. Keys, 1976, Applied
Geophysics, New York, Cambridge University Press, 860 p.
Time Magazine, 1984, Big stink, scandal over "sniffer planes": Time Magazine,
V. 123, No. 5, p. 27.
Wait, J. R., 1982, Geoelectromagnetism, New York, Academic Press, 268 p.
Washburne, J., 1984, Well casing study for U. S. Geological Survey: Phoenix
Geophysics unpublished report.
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APPENDIX
COSTS FOR GEOPHYSICAL EQUIPMENT AND SERVICES
The cost of the equipment necessary for making ground magnetic surveys is
relatively modest whereas a complete airborne system is expensive. The follow-
ing information was compiled from the winter 1984 price lists of three of
several manufacturers of magnetometers; we did not consider all models or the
several options that are available in some models. Prices for other equipment
are nominal and could vary considerably.
Epuipment	Cost
Proton field magnetometer--l-gamma sensitivity no memory $3,300-4,000
Proton field magnetometer—0.1-gamma sensitivity and solid
state memory (can be used as a base station magnetometer) $5,100-6,500
Proton field magnetometer and gradiometer with solid
state memory	$8,200-8,900
Recording proton base station and airborne magnetometer $10,500
Airborne magnetometer with 0.2-gamma sensitivity or better
at 2 samples per second or faster	$37,000-40,000
Microcomputer and printer for reading out and	storing
contents of memory magnetometer	$2,500-3,700
Plotter for plotting ground magnetic profiles	$1,100
Compass and hip chain for rough surveying	$280
Microwave navigation system for aircraft	$60,000
Data acquisition and recording system for aircraft	$7,500-40,000
Radar altimeter for aircraft	$10,000
35-mm tracking camera for aircraft	$7,500
Equipment can often be rented at a cost of 10-20% of the purchase price
per month. The first-time installation of a system in a fixed-wing aircraft
including a tail stinger for the magnetometer sensor but not including equipment
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listed above will cost $20,000-40,000 or more. A temporary system with the
sensor in a towed "bird'1 can be placed in a helicopter at much lower cost.
It is impossible to provide accurate costs for making magnetic surveys to
locate wells because rates of production are likely to vary widely, depending
on local conditions. Nevertheless, the following information should be useful
in planning.
If accurate surveying is not required and if land access is easy, a crew
of two persons can ground check 10-30 sites per day to verify the existence of
casings and pinpoint their locations. On a regular grid with a station
spacing of 8 meters (26 feet) and using a memory magnetometer, one person can
measure about four stations per minute or cover about 1.9 km/hr (6,300
ft/hr). The man hours required for surveying in the grid will be at least
equal to those required for making the magnetic measurements. Assuming the
spacing between traverses is 16 meters (52.5 ft), a two-man crew could survey
and process data along 40-70 kilometers of line (line-km) (24.8-43.5 line-mi)
or cover an area of 0.64-1.12 km2 2 (0.25-0.43 miz) per week. Production would
be slower if the crew had to spend much time obtaining permission for access
to the land or to pinpoint the locations of casings as they are detected. The
cost per week including salaries, living expenses away from home, equipment
rental or amortization, supplies, and overhead, but not including mobilization
to the site, would be on the order of $2,200-3,000 per week. Excluding
mobilization or pre-survey expenses such as obtaining aerial photographs, unit
costs would be on the order of:
Checking individual sites	$15-60/site
Systematic surveys on a grid	$31-75/1ine-km
1150-121/1 ine-mi
!;2,000-4,700/km2
:;3,100-12,100/mi2
Costs for a routine aeromagnetic survey using small fixed-wing aircraft
are on the order of $5.60-9.30/1ine km ($9-15 line mi), including data pro-
cessing provided: (1) at least several thousand line-km are flown in one
block, (2) the lines are at least 20-30 km long, and (3) Doppler radar and a
tracking camera are used for flight path recovery. The costs for similar work
done with a rotary-wing aircraft are about $15.50-21.75/1ine-km ($25-35/1ine
mi). In making such surveys, rates of production during good weather will be
roughly 1,000 line-km/day for fixed-wing aircraft and perhaps half as much for
rotary wing aircraft. The costs for aeromagnetic surveys designed to locate
abandoned wells are much greater.
In surveying the Arcadia test area near Oklahoma City, where the lines
were 3.22 km (2 mi) long, the actual time required to do 114 line-km (71 line-
mi) with the Fairchild Porter was 1.72 hours so the rate of production was 66.4
line-km/hr (41.3 line-mi/hr). This does not include the time required for the
round trip between the airport and the area, which in this case was an addi-
tional hour. The rate of production with a rotary-wing aircraft would probably
be comparable; it would probably be operated at a lower speed, but the distance
flown in turning around between lines would be much less. Precision low-level

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1
flying is extremely demanding, and it would be unreasonable to expect a crew to
fly survey lines more than about three hours per day.
Following are rough estimates of costs for surveying using a rotary-wing
aircraft and assuming that 4 flights of 4 hours total duration are made per
week in areas similar to the Arcadia test area.
Helicopter and pi1ot—16 hours at $500/hr	$ 8,000
Equipment (without microwave navigation system) and
crew $10,000/week	$10,000
Data processing and display at $3.00/1ine-km for 750
line-km/week (466 line-mi) (assuming computer programs
already exist)	$ 2,250
Surveying and placement of microwave transponders at
$2,500/week	$ 2,500
Total weekly costs $22,750
There are a number of other fixed costs which must be considered:
Installation and removal of system from aircraft	$11,000
Helicopter standby time during installation and
removal of equipment	$ 2,000
Mobilization from helicopter base to and from area,
estimated 10 hours at $500/hr	$ 5,000
Rent of microwave navigation system, one month
minimum at $5,000/month	$5.000
Fixed costs $23,000
Production is assumed to be 750 1ine-km or 75 km2 per week.
Using these numbers, a summary for cost of airborne surveys is:
One-week survey from one base	$61/1ine-km
!>98 or 100/1 ine-mi
N610/km2
!;i,580/mi2
Four-week survey from one base	£38/1ine-km
! 161/1 ine-mi
:,380/km2
N984/mi2
Field costs would be somewhat less if it were not necessary to use a
microwave navigation system. Data processing costs would be substantially
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greater if a tracking camera rather than a navigation system were used for
flight path recovery. Field expenses for doing the same amount of work with a
fixed-wing aircraft would be considerably less. However, the one-time cost for
developing a system such as the one we used is very high and use of a fixed-wing
aircraft may be practical only if a large amount of work is required.
The cost of interpreting the results will be highly variable, depending on
the number of anomalies in the area and the degree of interference from sources
other than wells. In difficult areas a geophysicist may complete interpretation
of only a few km* per day.
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