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US3350634A - Electromagnetic investigation for salt webs interconnecting spaced salt domes - Google Patents

Electromagnetic investigation for salt webs interconnecting spaced salt domes
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US3350634A
US3350634AUS420259AUS42025964AUS3350634AUS 3350634 AUS3350634 AUS 3350634AUS 420259 AUS420259 AUS 420259AUS 42025964 AUS42025964 AUS 42025964AUS 3350634 AUS3350634 AUS 3350634A
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salt
domes
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Jr Gustave L Hoehn
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Mobil Oil AS
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Oct. 31, 1967 s. L. HOEHN. JR v 3,
TIC INVESTIGATION FOR SALT WEBS ELECTROMAGNE IN-IEZRCONNECTING SPACED SALT DOMES Filed Dec. 22, 1964 2 Sheets-Sheet l GUSTAVE L. HOEHN, JR.
INVENTOR BY MWJW ATTORNEY Oct. 31, 1967 G. L. HO EHN. JR 3,350,634 ELECTROMAGNETIC INVESTIGATION FOR SALT WEBS I INTERCONNECTING SPACED SALT DOMES Filed Dec. 22, 1964 2 Sheets-Sheet z GUSTAVE L. HOEHN, JR.
INVENTOR- ATTORNEY United States Patent ELECTROMAGNETIC INVESTIGATION FOR SALT WEBS INTERCONNECTING SPACED SALT DOMES Gustave L. Hoehn, Jr., Dallas, Tern, assignor to Mobil Oil Corporation, a corporation of New York Filed Dec. 22, 1964, Ser. No. 420,259
2 Claims. (Cl. 3246) ABSTRACT OF THE DHSCLOSURE The specification discloses a method of determining the presence or the absence of a salt Web interconnecting spaced salt domes at a level substantially higher than the lever of the mother salt bed from which the domes arise. A transmitter of electromagnetic energy is located within one salt dome and a receiver is located within the other salt dome. The transmitter is operated to produce pulses of electromagnetic energy and the receiver is employed for sensing for electromagnetic energy passing to the other salt dome by way of an interconnecting salt web.
This invention relates to a method of utilizing salt dome structures to obtain useful information and more particularly to a method of investigating salt dome regions to determine the presence or absence of salt structure interconnecting adjacent salt domes.
In certain applications, particularly in the petroleum industry, salt dome structures have been utilized for various purposes and thus are of special interest. For example, in the exploration of petroleum, boundary conditions of salt domes are investigated since knowledge thereof allows one to obtain information as to the possible location of dipping or inclined formations which have been found to surround salt domes and further to provide for the entrapment of oil and gas deposits.
As has been reported in the literature, geologists have suspected that the salt domes have grown from a mother salt bed lying deep below the earths surface. Duringthe growth period, the domes apparently have pushed upward into overlying sediments, thereby resulting in the inclined position of the above-mentioned subsurface formations.
In some areas, the salt domes are found relatively close together, that is to say from to 20 miles apart, and further appear to be located along a pronounced contour line. Thus, it appears that these salt domes have grown out of the same mother salt bed and hence are coupled together by a common salt structure.
In certain applications, it is desirable to establish communication between adjacent salt domes by way of the common salt structure in order to obtain useful information. In geophysical prospecting, the information of interest is the presence or absence of a salt web which may connect adjacent salt domes together at a level substantially higher than the level of the mother salt bed. More particularly, if adjacent salt domes have grown out of the same mother salt bed, there is a distinct possibility that the salt domes in their growth have pulled up an intermediate connecting web. It is desirable to determine the presence or absence of such a web, since the existence thereof may influence or alter the position of subsurface formations between adjacent salt domes and hence alfect the potential of these formations for providing traps for oil or gas.
In accordance with one aspect of the present invention,
a technique is provided for investigating salt dome regions containing adjacent salt domes by generating and applying electromagnetic energy to one salt dome and sensing for electromagnetic energy passing to an adjacent salt dome by way of interconnecting salt structure. Elec 3,350,634 Patented Oct. 31, 1967 ice tromagnetic energy detected at the second salt dome is recorded and analyzed to determine the presence or absence of a common salt structure interconnectingthe adjacent salt domes.
Since salt has a very high resistivity, it is a very good medium for transmitting electromagnetic energy. The other subsurface formations, however, generally have lower resistivities. Thus, there is little likelihood that the electromagnetic energy will be transmitted from one salt to the other by way of the low resistivity subsurface formations adjacent to the salt domes. Electromagnetic energy detected thus will be due at least in part to that passing to the detector by way of the common salt structure.
In a more specific aspect, electromagnetic energy is generated in pulses spaced in time and measurements made of the amplitude of the received electromagnetic energy as well as the time of detection following each generated pulse. In this manner, electromagnetic energy passing to the detector by way of the common salt structure may be distinguished from that passing to the detector by way of a leakage path extending above the earths surface. Discrimination is possible since the latter signal will exhibit the first arrival time as well as the largest amplitude. The amplitude and time of arrival of the remainder of the signal may be analyzed to obtain information about the presence or absence of interconnecting salt webs.
For a more complete understanding of the present invention and for further objects and advantages thereof, reference may be now had to the following description taken in conjunction with the accompanying drawings wherein:
FIGURE 1 illustrates a system for carrying out the present invention in adjacent salt domes of a salt dome region;
FIGURE 2 illustrates a modified System for carrying out the method of the present invention.
As illustrated in FIGURE 1, two salt domes 10 and 11, which may be spaced apart a distance of the order of miles, are shown extending from a commonmother salt bed 12. Also shown connecting the two salt domes in a thin interconnecting salt web 13 which may have been pulled up and formed between the two salt domes 10 and 11 during their initial growth period. As mentioned previously, in geophysical prospecting it is desirable to determine the presence or absence of this connecting web since it may have influenced intermediate subsurface formations, for example, those illustrated at 14 or those on either side of the web, and hence their probability of providing traps for oil and gas.
The presence or absence of this interconnecting web is determined by generating and applying to the salt dome 10 electromagnetic energy transmitted to the salt dome 11 by way of a path whichextends through the interconnect ing web 13. The system illustrated for generating the electromagnetic energy comp-rises atransmitter 15 coupled to a long antenna 16 extending into borehole 17 while the system for detecting the electromagnetic energy comprises a long antenna 18 located in borehole 19 and coupled toreceiver 20. The receiver in turn is coupled to areadout 21 which may be an oscilloscope? The path of electromagnetic energy through the interconnecting web 13 may be that illustrated at 22. As mentioned previously, since theformations 14 have a relatively low resistivity, there is little likelihood that electromagnetic energy will be transmitted through these formations. If the web exists, the electromagnetic energy transmitted to the detector or antenna 18 by way of the interconnecting salt structure is expected predominantly to be by way of the web since the path length therethrough is the shortest.
Preferably, thetransmitter 15 is pulsed to generate bursts of electromagnetic energy spaced in time whereby the amplitude of the received electromagnetic energy may be measured as well as the time required for the electromagnetic energy to travel to antenna 18. More particularly, the pulse generating system comprises a highfrequency crystal oscillator 23, asealer 24 for obtaining the desired repetition pulse rate, and apulse generator 25 for producing pulses of desired width for triggering thetransmitter 15. The output of thescaler 24 also is applied, by way ofconductor 26, to the sweep circuit of theoscilloscope 21. Thus, at the beginning of each pulse the sweep circuit of the oscilloscope is actuated whereby the signal received will be displayed in accordance with time following each pulse generated.
The signal illustrated on the scope of the oscilloscope comprises ahigh amplitude pulse 27 which comprises leakage electromagnetic energy received first and traveling by way of path illustrated at 28. Following thepulse 27 is a lower amplitude signal illustrated at 29 and which indicates the reception of electromagnetic energy by way of interconnecting salt structure. The presence of an interconnecting salt structure hence is determined by the presence ofsignal 29. The depth of the upper surface of the salt structure may be determined by resolving thesignal 29 by well-known mathematical techniques into a distribution of travel time paths necessary to provide the particular signal received. For example, the time of arrival of the signal, as well as its amplitude, are influenced by the path taken as well as the electrical properties of the salt at various depths. These properties may be determined by measuring temperature variations in existing wells in the salt structure to obtain a temperature gradient. From the measurements obtained, the gradient expected deep into the salt structure may then be approximated by extrapolation. Salt samples in the structure may be extracted and their electrical properties measured as a function of pressure and temperature. Of particular importance is the resistivity, dielectric properties, and permeability. After these properties have been measured and calculated, the salt structure may be treated as a plurality of subsurface layers each having different dielectric and resistivity values. By knowing the limits of these values, one maydetermine mathematically the probable paths of the electromagnetic energy through the formations to antenna 18. Of particular importance in the calculations is the determination of the direction of reflected and refracted components of the electromagnetic energy through the layers; the corresponding velocity of the components through the layers and hence the time of propagation; and, in addition, the strength of each signal component propagated through each layer. The time of propagation and the signal amplitudes as calculated for each path may then be correlated with the signal shown by theoscilloscope 21 to determine the depth of the upper surface of the interconnecting salt structure.
In the embodiment shown in FIGURE 1, the antenna 16 may comprise a coaxial cable having an insulated shield and a central conductor 41 extending therethrough and to a point below the shield a desired distance. The antenna is wound and unwound upondrum 42 driven by power means not shown. Thetransmitter 15 is coupled to conductor 41 by way ofbrush 43 andslip ring 44. Similarly, the antenna 18 may be a coaxial cable comprising aninsulated shield 45 and acentral conductor 46 wound and unwound upon adrum 47 driven by power means not shown.Receiver 20 is coupled toconductor 46 by way ofbrush 49 andslip ring 50. The signals applied to theoscilloscope 21 fromreceiver 20 may be filtered and rectified to give the pulselike signals shown.
Preferably, the antennas 16 and 13 are lowered deep into boreholes 17 and 19 to increase the probability of receiving signals transmitted by way of salt web 13. In the operation of the system, each pulse of radiation generated may have a time width of about 100 microseconds. The pulse repetition period may be of the order of 10,000
microseconds.Transmitter 15 may be operated at a frequency of the order of one megacycle.
Referring now to FIGURE 2, there is described a modification whereby the antennas may be positioned in balloons having reflecting surfaces to obtain increased directivity of the electromagnetic signals generated and received.
More particularly, aninflated balloon 60 encompassing adipole 61 is shown located in a large cavity 62 formed insalt dome 63. Thedipole 61 comprises coaxial rods mounted in acentral mandrel 64 of high dielectric material. The balloon is formed of a nonconductive material but has a conductive reflectingfilm 65 lining one half of the interior, as iilustrated. Thus, radiation from thedipole 61 is directed primarily alongpath 66.
In the embodiment of FIGURE 2, the cavity 62 is formed in asalt dome 63 fromborehole 67 by wellknown leaching techniques. After the cavity has been formed, all of the fluid may be displaced with another fluid such as oil. After this operation,tube 68 supporting themandrel 64 anddipole 61 and having theballoon 60 clamped at the lower end thereof by suitable means, not shown, is inserted in the borehole into the cavity. During the insertion operation, the ballon may be suitably folded around themandrel 64. In the inflation of the balloon, pump 69 is operable by way ofvalve 70 andcoupling 71 to introduce fluid, such as oil, into the balloon. In the alternative, the balloon may be inflated by the use of a small pump (not shown) attached totube 68 at the lower end to pump the fluid in the cavity into the balloon.
In the system illustrated, thetube 68 is supported at the well head on slips 72. The support is of such a nature that it may be rotated as onturntable 73. After the balloon has been inflated, thecoupling 71 may be disconnected andturntable 72 rotated to the desired direction to carry out the investigation technique. Suitable orientating system (not shown) may be employed to determine the orientation of the reflectingsurface 65.
Although a transmitter is shown in FIGURE 2, it is to 'be understood that a similar system may be employed with a receiver to carry out the receiving operations. Connection of the transmitter or receiver with the dipole is4by way ofconductors 74 extending through the mandrel A suitable transmitter for carrying out the present invention may be of the type manufactured by Arenberg Ultrasonic Laboratories Inc., Boston, Mass, Model No.PG 65 0-C.
Having described the invention in connection with specific embodiments thereof, it is to be understood that further modifications may suggest themselves to those sltilled in the art and it is intended to cover such modifications which fall within the scope of the appended claims.
I claim:
1. A method of investigating a salt dome region to determine the presence of subsurface salt structure interconnecting spaced subsurface salt domes and extending substantially above the base of said domes, comprising the steps of:
locating a source of electromagnetic energy in one of said salt domes,
locating a receiver of electromagnetic energy in the other of said salt domes,
periodically generating a control signal,
applying said control signal to said source to generate pulses of electromagnetic energy spaced in time, detecting at said receiver the electromagnetic energy resulting from said generated pulses and passing to said other salt dome by way of said salt structure, and periodically employing said control signal to initiate the recording of the output of said receiver to obtain a measurement as a function of time of the electromagnetic energy detected by said receiver following each pulse of electromagnetic energy generated.
5 2. The method of claim 1 wherein: said source and said receiver are lowered into openings extending into said salt domes, respectively, for carrying out said electromagnetic pulse generating and detecting operations.
' References Cited UNITED STATES PATENTS Barret 324-6 Hawley 3241 Athy et a1. 1-81.5 Bays 325-28 Lehan 324-6 X Holser et a1. 3246 0 G. R. STRECKER, Assistant Examiner.
UNITED STATES PATENT OFFICE CERTIFICATE OF CORRECTION Patent No. 3,350,634 October 31, 1967 Gustave L. Hoehn, Jr.
It is hereby certified that error appears in the above numbered patent requiring correction and that the said Letters Patent should read as corrected below.
Column 2, line 9, after "salt" insert dome line 41, for 1n" read 1s line 53, after "energy" insert and sens ng for electromagnetic energy Signed and sealed this 12th day of November 1968.
(SEAL) Attest:
EDWARD J. BRENNER Commissioner of Patents Edward M. Fletcher, Jr.
Attesting Officer

Claims (1)

1. A METHOD OF INVESTIGATING A SALT DOME REGION TO DETERMINE THE PRESENCE OF SUBSURFACE SALT STRUCTURE INTERCONNECTING SPACED SUBSURFACE SALT DOMES AND EXTENDING SUBSTANTIALLY ABOVE THE BASE OF SAID DOMES, COMPRISING THE STEPS OF: LOCATING A SOURCE OF ELECTROMAGNETIC ENERGY IN ONE OF SAID SALT DOMES, LOCATING A RECEIVER OF ELECTROMAGNETC ENERGY IN THE OTHER OF SAID SALT DOMES, PERIODICALLY GENERATING A CONTROL SIGNAL, APPLYING SAID CONTROL SIGNAL TO SAID SOURCE TO GENERATE PULSES OF ELECTROMAGNETIC ENERGY SPACED IN TIME, DETECTING AT SAID RECEIVER THE ELECTROMAGNETIC ENERGY RESULTING FROM SAID GENERATED PULSES AND PASSING TO SAID OTHER SALT DOME BY WAY OF SAID SALT STRUCTURE, AND PERIODICALLY EMPLOYING SAID CONTROL SIGNAL TO INITIATE THE RECORDING OF THE OUTPUT OF SAID RECEIVER TO OBTAIN A MEASUREMENT AS A FUNCTION OF TIME OF THE ELECTROMAGNETIC ENERGY DETECTED BY SAID RECEIVER FOLLOWING EACH PULSE OF ELECTROMAGNETIC ENERGY GENERATED.
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Cited By (17)

* Cited by examiner, † Cited by third party
Publication numberPriority datePublication dateAssigneeTitle
US3412815A (en)*1966-11-141968-11-26Chevron ResElectromagnetic radiation method for guiding the drilling of oil wells after the borehole has entered a massive earth formation of chemically deposited material, by a mistake, accident, or the like
US3440523A (en)*1965-04-021969-04-22Inst Francais Du PetroleMethod and apparatus for electromagnetic determination of the position of boundaries of and discontinuities in a geological formation
US3690164A (en)*1968-06-241972-09-12Inst Francais Du PetroleProcess for prospecting of the ground layers surrounding a borehole
US3978396A (en)*1968-11-061976-08-31Trw Inc.Method and apparatus for measuring electromagnetic conductivity of a medium and for detecting anomalies therein
US4161687A (en)*1977-09-121979-07-17The United States Of America As Represented By The United States Department Of EnergyMethod for locating underground anomalies by diffraction of electromagnetic waves passing between spaced boreholes
US4308499A (en)*1978-05-261981-12-29Kali Und Salz A.G.Method utilizing electromagnetic wave pulses for determining the locations of boundary surfaces of underground mineral deposits
US4446433A (en)*1981-06-111984-05-01Shuck Lowell ZApparatus and method for determining directional characteristics of fracture systems in subterranean earth formations
FR2561395A1 (en)*1984-03-191985-09-20Prakla Seismos GmbhMeasuring device in drilling
US4639669A (en)*1983-09-261987-01-27Lockheed Missiles & Space Company, Inc.Pulsed electromagnetic nondestructive test method for determining volume density of graphite fibers in a graphite-epoxy composite material
US4691166A (en)*1985-05-061987-09-01Stolar, Inc.Electromagnetic instruments for imaging structure in geologic formations
US5485089A (en)*1992-11-061996-01-16Vector Magnetics, Inc.Method and apparatus for measuring distance and direction by movable magnetic field source
US5512830A (en)*1993-11-091996-04-30Vector Magnetics, Inc.Measurement of vector components of static field perturbations for borehole location
US20030158669A1 (en)*2000-05-252003-08-21Davidson John KennethMethod for detecting direction and relative magnitude of maximum horizontal stress in earth's crust
US20040059511A1 (en)*2000-10-102004-03-25Exxonmobil Upstream Research CompanyMethod for borehole measurement of formation properties
US20120139748A1 (en)*2009-07-022012-06-07Halliburton Energy Services, Inc.Borehole Array for Ranging and Crosswell Telemetry
US9010461B2 (en)2009-06-012015-04-21Halliburton Energy Services, Inc.Guide wire for ranging and subsurface broadcast telemetry
US9581718B2 (en)2010-03-312017-02-28Halliburton Energy Services, Inc.Systems and methods for ranging while drilling

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US1240328A (en)*1914-04-021917-09-18Submarine Signal CoMethod and apparatus for locating ore-bodies.
US1724794A (en)*1925-02-201929-08-13Walter W DavisMethod of detecting ore deposits
US2172688A (en)*1937-08-191939-09-12Engineering Res CorpElectrical apparatus and method for geologic studies
US2183565A (en)*1938-05-271939-12-19Stanolind Oil & Gas CoTwo-well method of electrical logging and apparatus therefor
US2207281A (en)*1938-04-161940-07-09Continental Oil CoSeismic method of logging boreholes
US2653220A (en)*1949-10-211953-09-22Carl A BaysElectromagnetic wave transmission system
US2992325A (en)*1959-06-011961-07-11Space Electronics CorpEarth signal transmission system
US3286163A (en)*1963-01-231966-11-15Chevron ResMethod for mapping a salt dome at depth by measuring the travel time of electromagnetic energy emitted from a borehole drilled within the salt dome

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* Cited by examiner, † Cited by third party
Publication numberPriority datePublication dateAssigneeTitle
US1240328A (en)*1914-04-021917-09-18Submarine Signal CoMethod and apparatus for locating ore-bodies.
US1724794A (en)*1925-02-201929-08-13Walter W DavisMethod of detecting ore deposits
US2172688A (en)*1937-08-191939-09-12Engineering Res CorpElectrical apparatus and method for geologic studies
US2207281A (en)*1938-04-161940-07-09Continental Oil CoSeismic method of logging boreholes
US2183565A (en)*1938-05-271939-12-19Stanolind Oil & Gas CoTwo-well method of electrical logging and apparatus therefor
US2653220A (en)*1949-10-211953-09-22Carl A BaysElectromagnetic wave transmission system
US2992325A (en)*1959-06-011961-07-11Space Electronics CorpEarth signal transmission system
US3286163A (en)*1963-01-231966-11-15Chevron ResMethod for mapping a salt dome at depth by measuring the travel time of electromagnetic energy emitted from a borehole drilled within the salt dome

Cited By (21)

* Cited by examiner, † Cited by third party
Publication numberPriority datePublication dateAssigneeTitle
US3440523A (en)*1965-04-021969-04-22Inst Francais Du PetroleMethod and apparatus for electromagnetic determination of the position of boundaries of and discontinuities in a geological formation
US3412815A (en)*1966-11-141968-11-26Chevron ResElectromagnetic radiation method for guiding the drilling of oil wells after the borehole has entered a massive earth formation of chemically deposited material, by a mistake, accident, or the like
US3690164A (en)*1968-06-241972-09-12Inst Francais Du PetroleProcess for prospecting of the ground layers surrounding a borehole
US3978396A (en)*1968-11-061976-08-31Trw Inc.Method and apparatus for measuring electromagnetic conductivity of a medium and for detecting anomalies therein
US4161687A (en)*1977-09-121979-07-17The United States Of America As Represented By The United States Department Of EnergyMethod for locating underground anomalies by diffraction of electromagnetic waves passing between spaced boreholes
US4308499A (en)*1978-05-261981-12-29Kali Und Salz A.G.Method utilizing electromagnetic wave pulses for determining the locations of boundary surfaces of underground mineral deposits
US4446433A (en)*1981-06-111984-05-01Shuck Lowell ZApparatus and method for determining directional characteristics of fracture systems in subterranean earth formations
US4639669A (en)*1983-09-261987-01-27Lockheed Missiles & Space Company, Inc.Pulsed electromagnetic nondestructive test method for determining volume density of graphite fibers in a graphite-epoxy composite material
FR2561395A1 (en)*1984-03-191985-09-20Prakla Seismos GmbhMeasuring device in drilling
US4691166A (en)*1985-05-061987-09-01Stolar, Inc.Electromagnetic instruments for imaging structure in geologic formations
US5485089A (en)*1992-11-061996-01-16Vector Magnetics, Inc.Method and apparatus for measuring distance and direction by movable magnetic field source
USRE36569E (en)*1992-11-062000-02-15Vector Magnetics, Inc.Method and apparatus for measuring distance and direction by movable magnetic field source
US5512830A (en)*1993-11-091996-04-30Vector Magnetics, Inc.Measurement of vector components of static field perturbations for borehole location
US20030158669A1 (en)*2000-05-252003-08-21Davidson John KennethMethod for detecting direction and relative magnitude of maximum horizontal stress in earth's crust
US6885944B2 (en)*2000-05-252005-04-26Petrecon Australia Pty LtdMethod for detecting direction and relative magnitude of maximum horizontal stress in earth's crust
US20040059511A1 (en)*2000-10-102004-03-25Exxonmobil Upstream Research CompanyMethod for borehole measurement of formation properties
US9010461B2 (en)2009-06-012015-04-21Halliburton Energy Services, Inc.Guide wire for ranging and subsurface broadcast telemetry
US20120139748A1 (en)*2009-07-022012-06-07Halliburton Energy Services, Inc.Borehole Array for Ranging and Crosswell Telemetry
US8912915B2 (en)*2009-07-022014-12-16Halliburton Energy Services, Inc.Borehole array for ranging and crosswell telemetry
US10190405B2 (en)2009-07-022019-01-29Halliburton Energy Services, Inc.Borehole array for ranging and crosswell telemetry
US9581718B2 (en)2010-03-312017-02-28Halliburton Energy Services, Inc.Systems and methods for ranging while drilling

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