GB1588865A - Creación de Inventos y Patentes con Inteligencia Artificial

GB1588865A – Electromagnetic wave propagation well logging utilizing multiple phase shift measurement
– Google Patents

GB1588865A – Electromagnetic wave propagation well logging utilizing multiple phase shift measurement
– Google Patents
Electromagnetic wave propagation well logging utilizing multiple phase shift measurement

Download PDF
Info

Publication number
GB1588865A

GB1588865A
GB1942778A
GB1942778A
GB1588865A
GB 1588865 A
GB1588865 A
GB 1588865A
GB 1942778 A
GB1942778 A
GB 1942778A
GB 1942778 A
GB1942778 A
GB 1942778A
GB 1588865 A
GB1588865 A
GB 1588865A
Authority
GB
United Kingdom
Prior art keywords
borehole
coils
signal
signals
frequency
Prior art date
1978-05-13
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)

Expired

Application number
GB1942778A
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)

Texaco Development Corp

Original Assignee
Texaco Development Corp
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
1978-05-13
Filing date
1978-05-13
Publication date
1981-04-29

1978-05-13
Application filed by Texaco Development Corp
filed
Critical
Texaco Development Corp

1978-05-13
Priority to GB1942778A
priority
Critical
patent/GB1588865A/en

1981-04-29
Publication of GB1588865A
publication
Critical
patent/GB1588865A/en

Status
Expired
legal-status
Critical
Current

Links

Espacenet

Global Dossier

Discuss

Classifications

G—PHYSICS

G01—MEASURING; TESTING

G01V—GEOPHYSICS; GRAVITATIONAL MEASUREMENTS; DETECTING MASSES OR OBJECTS; TAGS

G01V3/00—Electric or magnetic prospecting or detecting; Measuring magnetic field characteristics of the earth, e.g. declination, deviation

G01V3/18—Electric or magnetic prospecting or detecting; Measuring magnetic field characteristics of the earth, e.g. declination, deviation specially adapted for well-logging

G01V3/26—Electric or magnetic prospecting or detecting; Measuring magnetic field characteristics of the earth, e.g. declination, deviation specially adapted for well-logging operating with magnetic or electric fields produced or modified either by the surrounding earth formation or by the detecting device

G01V3/28—Electric or magnetic prospecting or detecting; Measuring magnetic field characteristics of the earth, e.g. declination, deviation specially adapted for well-logging operating with magnetic or electric fields produced or modified either by the surrounding earth formation or by the detecting device using induction coils

Description

(54) ELECTROMAGNETIC WAVE PROPAGATION WELL LOGGING
UTILIZING MULTIPLE PHASE SHIFT MEASUREMENT
(71) We, TEXACO DEVELOPMENT CORPORATION, a corporation organised and existing under the laws of the State of Delaware, United States of America, of 135 East 42nd Street, New York, New York 10017, United States of America, do hereby declare the invention, for which we pray that a patent may be granted to us, and the method by which it is to be performed, to be particularly described in and by the following statement::
The present invention relates to methods and apparatus for determining the characteristics of material surrounding an open hole well bore and in particular, relates to methods and apparatus for radio frequency resistivity well logging in which the true formation resistivity, flushed zone resistivity and invasion diameter are uniquely determinable by means of in situ measurements taken in a well borehole.
It has been conventional practice to log the electrical characteristics of earth formations in the vicinity of a well borehole in order to determine location of oil-bearing strata. There are only three material parameters which affect an electromagnetic wave, whether the wave gets from one point to another by induction or by propagation. They are conductivity (resistivity), magnetic susceptibility and dielectric constant. Conductivity provides an indication of the energy absorbing characteristics of the medium, while magnetic susceptibility and dielectric constant give a measure of the energy storing capacity of a material. The magnetic susceptibility of most earth materials has relatively little effect on electromagnetic waves and is of very little use in electrical logging techniques.Dielectric constant has considerable variation in the earth and has a large influence on high-frequency propagation but very little influence at low frequencies. It is well known that conductivity or resistivity has wide variation in value for earth materials and strongly affects all electromagnetic waves.
A propagating electromagnetic wave has two fundamental characteristics, amplitude and phase. By comparing the amplitude and phase of an electromagnetic wave as it passes receivers, propagation characteristics due to the formation may be studied. Measurement of these two characteristics in terms of wave travel time and attenuation may be used to determine the dielectric constant and/or the resistivity of the media through which the wave is propagated.
Study has indicated that four general frequency ranges exist which allow measurement of the formation effects. These four frequency regions are induction, low radio frequency propagation, high radio frequency propagation, and ultra high radio frequency propagation. The relative influence of resistivity (Rt) and dielectric constant (Et) in these four ranges is shown in the following table (where Rt = 20Qm and Et = 20::
RELATIVE INFLUENCE
Approx. wavelength
Type of log Resistivity Dielectric in earth formation
Induction 3.4 k Meter
(20 to 50 kHz) 1.0 0.0004 (11,000 ft.)
Low Radio Frequency
Propagation 1.0 0.004 34 meter
Resistivity (110 ft.)
(2 MHz)
High Radio Frequency
Dielectric and 1.0 0.7 2.2 meter
Resistivity (7.2 ft.)
(30 MHz)
Ultra-High Radio
Frequency Dielectric 1.0 22.0 .061 meter
(1 to 3 GHz) (0.2 ft.)
From the table, it can be seen that resistivity is the only parameter that materially influences the measurements in the induction and low radio frequency propagation range.
The resistivity and dielectric constant have about the same magnitude of influence in the high radio frequency propagation region. In the ultra high radio frequency region, the dielectric constant dominates the wave travel time while the resistivity influences wave attenuation.
Electrical induction logging has been practiced for many years. In conventional induction logging, a well logging sonde is provided having a transmitter coil (or array of coils) and a receiver coil (or array of coils) at longitudinally spaced intervals from the receiver coil.
Usually, an alternating current. in a range of 20 to 50 kilohertz, is passed through the transmitter coil. The resulting electric fields produced by this alternating current in the earth formation surrounding a well bore are detected at a spaced receiver coil by sensing the induced current or voltage in the receiver coil. Induction logging has been principally used with oil-base drilling mud or drilling fluids having high resistivities but, in recent years, has come to be used even with highly conductive (low resistivity) drilling fluids.
In low radio frequency wave propagation, as already pointed out, the dielectric constant has practically no effect on the propagating wave. Since both the travel time and attenuation are affected in this region essentially only by the formation resistivity, measurements of these propagation parameters in low radio frequency regions yields essentially only resistivity information.
Various problems have arisen in the interpretation of either induction logging or low radio frequency wave propagation logging methods where relatively non-conductive fresh water bearing formations are encountered. Such fresh water bearing sands or formations exhibit high resistivity much the same as those encountered in hydrocarbon bearing formations. However, since hydrocarbons have a characteristically low dielectric constant and fresh water has a relatively high dielectric constant, high radio frequency propagation logs have been found to be useful in such applications. In United States Patent No.
3,893,021, a solution to this problem is described utilizing a radio frequency electromagnetic field in the frequency range of 20 to 40 megahertz. At these high radio frequencies, the dielectric properties of the media surrounding the well bore influence the electro-magnetic field together with the conductivity or resistivity characteristics of a material. By providing apparatus to measure both phase shift (travel time) and amplitude change (attenuation) of the signal, both the dielectric and resistivity characteristics of the earth formation in the vicinity of the borehole may be determined.
In ultra-high radio frequency logging, above 300 megahertz. wave travel time is essentially dependent only on the dielectric constant. This region is characterized by very short wave lengths and very high wave attenuation. Because of these factors, the ultra-high radio frequency logging system requires very close source to receiver spacing and hence has a very shallow depth of investigation.
Commercial DC or very low frequency AC (such as 60 Hertz) electrical resistivity logs require direct contact with the surrounding well bore by contacting electrodes. This creates problems in providing a sonde which can be easily pulled through the well bore yet make the necessary contact with the well bore. For this reason, induction logging, which does not depend on such direct contact, is more desirable. However, as earlier mentioned commercial induction electrical logging systems now available are principally used with oil-based drilling muds or drilling fluids having high resistivity and are adversely affected by brine filled or highly conductive drilling fluid filled well bores.Furthermore, commercial induction electrical logs are generally not accurate in high resistivity formations and both electrical resistivity and electrical induction logging systems commercially available have relatively poor thin-bed response; i.e. they do not give accurate resistivity values for beds thinner than four feet. It would therefore be beneficial to provide a well logging system which could provide an accurate measurement of true formation resistivity, flushed zone resistivity and invasion diameter, whether used in well bores having highly resistive drilling fluids (such as oil-base drilling muds) or higher conductive drilling fluids, and regardless of whether the formations are highly resistive or of thin beds.
Accordingly, it is an object of the present invention to provide a well logging system which is capable of accurate measurement of true formation resistivity, flushed zone resistivity and invasion diameter by means of low radio frequency electromagnetic wave propagation. The flushed zone is that portion of the formation immediately adjacent to the well bore and extending outwardly to a limited extent wherein all the formation water and most of the formation hydrocarbons have been displaced by the drilling fluids. The invaded zone includes the flushed zone and extends further outwardly to the extent, at the invasion diameter, at which the formation fluids are found to be unaffected by any invasion by the drilling fluids.
According to the present invention there is provided apparatus for investigating earth formations in the vicinity of a borehole, comprising:
means for generating, in said borehole, an alternating electromagnetic field at a frequency in the range of from substantially 2 megahertz to substantially 4 megahertz;
detection means, including a plurality of receiver coils responsive to the total electromagnetic field generated by said generating means, said coils being arranged to provide first, second and third pairs at successively greater longitudinal distances from said generating means;;
and signal generating means connected to said detection means to generate first, second and third signals respectively representative of the phase difference in said field at the two coils of said first, second and third said pairs of coils, whereby said signals embody information concerning electromagnetic characteristics of said earth formations.
In another aspect the invention provides a method of investigating earth formations in the vicinity of a borehole, comprising the steps of:
generating, in said borehole, an alternating electromagnetic field at a frequency in the range of from substantially 2 megahertz to substantially 4 megahertz;
detecting, in said borehole, said generated electromagnetic field;
and generating first, second and third signals respectively representative of the phase difference in said field at the two locations of a pair of spaced locations at each of first, second and third successively greater longitudinal distances from where said field is generated, whereby said signals embody information concerning electromagnetic characteristics of said earth formations.
An embodiment of the invention will now be described, by way of example, with reference to the accompanying drawings, in which:
Figure 1 is a block diagram illustrating the overall layout of a radio frequency logging system in accordance with the present invention
Figure 2 is a schematic block diagram illustrating the downhole electronics portion of the system of Figure 1
Figure 3 is a theoretically derived plot of the phase difference for relatively short, medium and long phase shift measurements of the apparatus of Figure 1 plotted against earth formation resistivity;
Figure 4 is the plot of an actual well log obtained by a radio frequency logging system in accordance with the present invention, indicating phase difference for short, medium and long spaced measurements plotted against borehole depth; ;
Figure 5 is a plot of true formation resistivity and invasion zone diameter for particular phase differences for short, medium and long spaced measurements; and
Figure 6 is a plot of invaded zone resistivity for true formation resistivity derived from
Figure 5, against short spaced phase difference measurement.
Referring now to Figure 1, a low radio-frequency resistivity well logging system in accordance with concepts of the present invention is illustrated schematically. The well logging sonde 10 is made up of a cylindrical coil mandrel and associated electronics which can be placed inside a pressure-tight case formed of a non-conducting material such as fiberglass. The sonde 10 is shown suspended by well logging cable 11 in an uncased well borehole 12. The borehole 12 is filled with a borehole or drilling fluid 13 and is surrounded by earth formations whose conductivity properties are to be measured.
The lower portion of the well logging sonde 10 comprises an electronic transmitter section 15 to be more fully described hereafter, and associated transmitter coil 16 and battery pack 17. The transmitter section 15 is connected to the power of the battery pack 17 through a slip ring arrangement 18. The transmitter coil 16 is operated at a frequency of 2 megahertz and will be described subsequently in more detail.
Spaced at longitudinal intervals from the transmitter coil 16 are first, second, third and fourth receiver coils 19, 20, 21 and 22, respectively. These coils are spaced 10 inches, 22 inches, 34 inches and 46 inches, respectively from the transmitter coil 16. The receiver coils are used in pairs. Coils 19 and 20 are used for making a short-spaced measurement, coils 20 and 21 for making an intermediate spaced measurement and coils 21 and 22 for making a long-spaced measurement. It will be appreciated that while these transmitter and receiver coil spacings have been found useful in practicing the concepts of the present invention, they are intended as being illustrative only.It may be practical to utilize other than the disclosed spacing distances between the transmitter and receiver coils or a different number of receiver coils to make up three pairs thereof, such as six coils comprising the three separated pairs. Such variations are considered to be within the scope of the invention.
As will be appreciated, the radial depth of investigation of a coil pair of the logging system of the present invention is influenced by the spacing distance between the transmitting and receiving coils. The radial depth of investigation for the pairs of receiver coils increases from short spaced pair 19 and 20, to intermediate spaced pair 20 and 21, and to long spaced pair 21 and 22.
A conventional winch arrangement (not shown) may be used at the surface of the borehole 12 for moving the cable 11 and attached sonde through the borehole during a well logging operation. The winch arrangement may be provided with a conventional electrical or mechanical coupling linkage for recording well depth as a reference against which recorded signals from the downhole sonde 10 is recorded. Power for operation of the downhole receiver electronics section 23 is provided on the conductor of the well logging cable 11 by a surface power supply 24. Such power supplies may comprise conventional AC or DC supplies as known in the art.
Referring now to Figure 2, the downhole electronic portion of the system is illustrated in the form of a block diagram. The battery pack 17, which is connectible to the transmitter electronics by a slip ring assembly 18 as illustrated in Figure 1, may comprise rechargeable nickle cadmium batteries or the like. The slip ring method of connection allows the battery power to be easily turned on in the field and provides a means of inserting a fresh battery pack while the discharged batteries are being recharged. The transmitter electronics further comprises a crystal-controlled 2 megahertz, three-stage class C device 25 which uses standard RF circuits. The transmitter coil 16 may comprise fourteen turns of No. 12 enamel copper wire wound close spaced on the coil support mandrel.
The four receiver coils, 19, 20, 21 and 22 are identical single-turn electrostatically shielded coils. The electrostatic shielding reduces the chance of capacitive coupling with the transmitter, so that only propagating wave fields will be sensed by the coil pairs. As already mentioned, receiver coils 19 and 20 are used to make a short-spaced measurement, 20 and 21 to make an intermediate measurement and 21 and 22 to make a long-spaced measurement.
The signal from each receiver coil is fed to a signal-conversion, 2 megahertz receiver 26, 27, 28 and 29 which amplifies and converts, by mixing, the signals to 4.0 kilohertz. One 2.004 megahertz crystal oscillator 30 is used for mixing in all four receivers 26, 27, 28 and 29. This allows all phase information present in the 2 megahertz propagated signals to be maintained in the 4.0 kilohertz converted signal.
In the receivers, each 4.0 kilohertz signal is fed to an automatic gain control amplifier 31, 32, 33, and 34, respectively. resulting in a constant output amplitude. The signals from the
AGC amplifiers are then fed to Schmidt trigger circuits 35, 36, 37 and 38 which generate square waves which are precisely in phase with the received signals. These square waves are applied to exclusive-NOR logic gates 39, 40, and 41, which provide output pulses whose widths are proportional to the phase difference between the two inputs, gate 39 being for the short-spaced measurement. gate 40 for the intermediate spaced measurement and gate 41 for the long-spaced measurement. Thus, the square wave signals to the gates 39, 40 and 41, present a measurement of the phase difference or wave propagation velocity, between coils 19 and 20, 20 and 21, and 21 and 22, respectively.
The output of each of the three exclusive-NOR gates 39, 40 and 41 is integrated by single resistance capacitance filters 42, 43, and 44, respectively, to provide a DC voltage. The three DC voltages are then applied to respective voltage control oscillators 45, 46 and 47, each having a different center frequency. This action converts the respective DC signals to a
VCO frequency. As each DC voltage varies the voltage controlled oscillator (VCO) frequency varies. The three VCO outputs are passed through a summing amplifier 48 and cable driver 49 which sends the composite signal along the logging cable 11 to the surface electronics to be more fully described hereinafter with further reference to Figure 1.
Since the measurement of phase difference is dependent on the amplitude of the signals going from the AGC amplifiers 31, 32, 33 and 34 to their respective Schmidt triggers 35, 36, 37 and 38, it is important to known when the AGC amplifiers are no longer keeping the signal amplitude constant. The AGC voltage of the longest spaced receiver 29 (since this receiver coil will have the weakest signal) gives a measure of this important information.
The AGC voltage is applied to a fourth voltage controlled oscillator (VCO) 50 and summed along with the three phase signals.
Referring again to Figure 1, at the surface, the composite signal is taken from the logging cable 11 by coupling capacitor 51 and supplied to an input buffer amplifier 52. The output from the buffer amplifier 52 is separated by band pass filter circuits 53, 54, 55 and 56 into the four original frequency modulated signals. Each signal is then applied to phase locked loop demodulators 57, 58, 59 and 60. The demodulators 57, 58, 59 and 60 lock onto the input signal tracking its frequency changes and providing DC output voltage proportional to the input signal frequency.
Output signals from the phase locked loop demodulators 57-60 are supplied to differential amplifiers 61, 62, 63 and 64 for further amplication amplification prior to input to conventional well logging recorders (not shown). Recorder amplifiers 65, 66, 67 and 68 further amplify the signals and use them to control the motion of strip chart recorder pins or the grids of cathode ray tubes if this type of recorder is used.
Referring now to Figure 4, a strip chart recorder display for four traces; s (phase shift for short spaced measurement); m (phase shift for intermediate spaced measurement); Oi (phase shift for long spaced measurement); and AGC (AGC voltage from voltage controlled oscillator 50) is shown. The three phase traces 05, m and Oi may be set up for 50/inch sensitivity. These three phase traces may be used along with theoretical computer derived relationships to obtain Rt, Rxo and dj by the solving of three simultaneous non-linear equations which relate these quantities.Although these values are preferably solved by a computer program, their solution will be illustrated in Figures 5 and 6 which will be described hereafter.
As already mentioned, since the measurement of phase differences is dependent on the amplitude of the signals going from AGC amplifiers 31, 32 and 33, to their respective
Schmidt triggers 35, 36 and 37, it is important to know when the AGC amplifiers are no longer keeping the signal amplitude constant. The AGC trace, such as shown in Figure 4, is for this important indication. If the signal amplitude is being maintained constant the trace will appear as a straight line as shown in Figure 4. However, in regions where the signal is not sufficient to make a measurement, the AGC trace will depart from a straight line to so indicate.
Figure 3 is shown merely to illustrate the relationship of phase shift to true formation resistivity for short, intermediate and long radii measurements into the earth surrounding a borehole. The theoretically derived plot of Figure 3 is for a megahertz electromagnetic field, assuming no invasion of drilling fluids.
Referring now to Figures 5 and 6, solution of the three simultaneous non-linear equations necessary for determination of Rt, Rxo and di will be illustrated. For purposes of illustration, it will be assumed that O equals 11″ for which two families of curves for R, and dj can be plotted against variable m and 0,. In Figure 5, curves for Rt are shown as solid lines. Merely for purposes of illustration, it will be assumed that from the recording chart, when Hs equals 11″, m and 0 will be 9.3 and 8.7 , respectively.By entering the chart of
Figure 5, these readings intersect at point a. At this point, Rt equals 20Qm and dj equals 0.8M. Thus, true, resistivity Rt is determined to be 20Qm and dj is determined to be 0.8 meters. These figures may now be used in the chart of Figure 6 to determine the resistivity of the flushed zone, Rxo.
Assuming true resistivity to be a constant figure (Rt equals 2OQm in the present case) a family of curves can be drawn for flushed zone resistivity Rxo for variable short-spaced phase shift O and invaded zone diameters dj. Now using the short-spaced phase shift 11″ and the invaded zone diameter d = 0.8 meters, determined from Figure 5, point b is read on the chart of Figure 6. From this, it can be determined that Rxo = 3.95 ohm-meters. Thus, for the phase shift measurements 09 = 11″, Orn = 9.3 , 0 = 8.7 , the following determinations are made for true resistivity, invaded zone diameter and flushed zone resistivity: Rt = 20, dj = 0.8, Rxo = 3.95. As already mentioned, these graphical solutions are merely for purposes of illustration. In practice, graphical solutions could be generated on a computer program and the simultaneous solutions made by computer. A small general purpose computer such as the Model PDP-11 of the Digital Equipment Corp. can be properly programmed in a computer language such as FORTRAN for this purpose when provided with the graphical relationships of Figures 5 and 6.
To summarize the operation of the well logging system of the present invention, a downhole transmitter 15 is used to excite the earth formation in the vicinity of the well bore with 2.0 megahertz radio frequency energy. Four spaced receiver coils 19-22, receive voltages induced therein by the 2 megahertz signal. These receivers acting in pairs, 19 and 20, 20 and 21 and 21 and 22, measure respectively, the relative phase shift for short, medium and long-spaced radial distances from the borehole. These measurements are transmitted to the surface as multiplexed frequency modulated data. At the surface, the signals are demodulated and supplied to a data recorder (not shown) providing a trace or continuous log of phase shift as a function of borehole depth similar to the one shown in
Figure 4.This information may then be utilized in a computer program to determine R5, dj and R2x,.
The Rt, dj and Rxo so determined can be used to interpret earth formations surrounding the borehole being logged. The information can also be combined with other information determined by other logging methods, for example, those which require determination of the dielectric constant to distinguish fresh water zones from oil zones.
WHAT WE CLAIM IS:
1. Apparatus for investigating earth formations in the vicinity of a borehole, comprising:
means for generating, in said borehole, an alternating electromagnetic field at a frequency in the range of from substantially 2 megahertz to substantially 4 megahertz;
detection means, including a plurality of receiver coils responsive to the total electromagnetic field generated by said generating means, said coils being arranged to provide first, second and third pairs at successively greater longitudinal distances from said generating means;;
and signal generating means connected to said detection means to generate first, second and third signals respectively representative of the phase difference in said field at the two coils of said first, second and third said pairs of coils, whereby said signals embody information concerning electromagnetic characteristics of said earth formations.
2. Apparatus as claimed in claim 1 wherein said detection means comprises first, second, third and fourth said receiver coils, said first and second, said second and third and said third and fourth receiver coils providing said first, second, and third pairs of receiver coils, respectively.
3. Apparatus as claimed in claim 1 wherein said detection means comprises first, second, third, fourth, fifth and sixth said receiver coils, said first and second, said third and fourth and said fifth and sixth receiver coils providing said first, second and third pairs of receiver coils, respectively.
4. Apparatus as claimed in any one of claims 1 to 3 including means responsive to said first, second and third phase difference signals to determine the true formation resistivity (Rt), the flushed zone resistivity (rio) and the invasion diameter (dj) of said earth formation in the vicinity of said borehole.
5. Apparatus as claimed in any one of claims 1 to 4 wherein said signal generating means comprises signal converter means for converting the signal from each individual said coil into a signal of a second frequency and of substantially constant output amplitude.
6. Apparatus as claimed in claim 5 wherein said receiver signal converter means includes a crystal controlled oscillator common to said coils, said oscillator having an operating frequency equal to said first field frequency plus said second frequency.
7. Apparatus as claimed in claim 5 or claim 6 wherein said signal generating means includes means for converting said signals of constant output amplitude to first, second and third output pulses whose widths are proportional to the phase difference at the two coils of said first, second and third pairs of coils, respectively.
8. Apparatus as claimed in any one of claims 5 to 7 wherein said signal generating means includes means for detecting deviations in amplitude of said second frequency signal and providing a deviation signal.
9. Apparatus as claimed in claim 7 or claim 8 wherein said signal generating means includes means for integrating and summing said first, second, and third output pulse signals, and said deviation signal when present, into a composite signal for transmission to the earth’s surface.
10. A method of investigating earth formations in the vicinity of a borehole, comprising the steps of:
**WARNING** end of DESC field may overlap start of CLMS **.

Claims (13)

**WARNING** start of CLMS field may overlap end of DESC **. resistivity: Rt = 20, dj = 0.8, Rxo = 3.95. As already mentioned, these graphical solutions are merely for purposes of illustration. In practice, graphical solutions could be generated on a computer program and the simultaneous solutions made by computer. A small general purpose computer such as the Model PDP-11 of the Digital Equipment Corp. can be properly programmed in a computer language such as FORTRAN for this purpose when provided with the graphical relationships of Figures 5 and 6. To summarize the operation of the well logging system of the present invention, a downhole transmitter 15 is used to excite the earth formation in the vicinity of the well bore with 2.0 megahertz radio frequency energy. Four spaced receiver coils 19-22, receive voltages induced therein by the 2 megahertz signal. These receivers acting in pairs, 19 and 20, 20 and 21 and 21 and 22, measure respectively, the relative phase shift for short, medium and long-spaced radial distances from the borehole. These measurements are transmitted to the surface as multiplexed frequency modulated data. At the surface, the signals are demodulated and supplied to a data recorder (not shown) providing a trace or continuous log of phase shift as a function of borehole depth similar to the one shown in Figure 4.This information may then be utilized in a computer program to determine R5, dj and R2x,. The Rt, dj and Rxo so determined can be used to interpret earth formations surrounding the borehole being logged. The information can also be combined with other information determined by other logging methods, for example, those which require determination of the dielectric constant to distinguish fresh water zones from oil zones. WHAT WE CLAIM IS:

1. Apparatus for investigating earth formations in the vicinity of a borehole, comprising:
means for generating, in said borehole, an alternating electromagnetic field at a frequency in the range of from substantially 2 megahertz to substantially 4 megahertz;
detection means, including a plurality of receiver coils responsive to the total electromagnetic field generated by said generating means, said coils being arranged to provide first, second and third pairs at successively greater longitudinal distances from said generating means;;
and signal generating means connected to said detection means to generate first, second and third signals respectively representative of the phase difference in said field at the two coils of said first, second and third said pairs of coils, whereby said signals embody information concerning electromagnetic characteristics of said earth formations.

2. Apparatus as claimed in claim 1 wherein said detection means comprises first, second, third and fourth said receiver coils, said first and second, said second and third and said third and fourth receiver coils providing said first, second, and third pairs of receiver coils, respectively.

3. Apparatus as claimed in claim 1 wherein said detection means comprises first, second, third, fourth, fifth and sixth said receiver coils, said first and second, said third and fourth and said fifth and sixth receiver coils providing said first, second and third pairs of receiver coils, respectively.

4. Apparatus as claimed in any one of claims 1 to 3 including means responsive to said first, second and third phase difference signals to determine the true formation resistivity (Rt), the flushed zone resistivity (rio) and the invasion diameter (dj) of said earth formation in the vicinity of said borehole.

5. Apparatus as claimed in any one of claims 1 to 4 wherein said signal generating means comprises signal converter means for converting the signal from each individual said coil into a signal of a second frequency and of substantially constant output amplitude.

6. Apparatus as claimed in claim 5 wherein said receiver signal converter means includes a crystal controlled oscillator common to said coils, said oscillator having an operating frequency equal to said first field frequency plus said second frequency.

7. Apparatus as claimed in claim 5 or claim 6 wherein said signal generating means includes means for converting said signals of constant output amplitude to first, second and third output pulses whose widths are proportional to the phase difference at the two coils of said first, second and third pairs of coils, respectively.

8. Apparatus as claimed in any one of claims 5 to 7 wherein said signal generating means includes means for detecting deviations in amplitude of said second frequency signal and providing a deviation signal.

9. Apparatus as claimed in claim 7 or claim 8 wherein said signal generating means includes means for integrating and summing said first, second, and third output pulse signals, and said deviation signal when present, into a composite signal for transmission to the earth’s surface.

10. A method of investigating earth formations in the vicinity of a borehole, comprising the steps of:
generating, in said borehole, an alternating electromagneticm field at a frequency in the range of from substantially 2 megahertz to substantially 4 megahertz;
detecting, in said borehole, said generated electromagnetic field;
and generating first, second and third signals respectively representative of the phase difference in said field at the two locations of a pair of spaced locations at each of first, second and third successively greater longitudinal distances from where said field is generated, whereby said signals embody information concerning electromagnetic characteristics of said earth formations.

11. A method as claimed in claim 10 including determining from said signals the true formation resistivity (Rt), the flushed zone resistivity (rio), and the invasion diameter (dj) of said earth formations in the vicinity of the borehole.

12. A method as claimed in claim 10 and substantially as described herein with reference to the accompanying drawings.

13. Apparatus for investigating earth formations in the vicinity of a borehole, substantially as described herein with reference to the accompanying drawings.

GB1942778A
1978-05-13
1978-05-13
Electromagnetic wave propagation well logging utilizing multiple phase shift measurement

Expired

GB1588865A
(en)

Priority Applications (1)

Application Number
Priority Date
Filing Date
Title

GB1942778A

GB1588865A
(en)

1978-05-13
1978-05-13
Electromagnetic wave propagation well logging utilizing multiple phase shift measurement

Applications Claiming Priority (1)

Application Number
Priority Date
Filing Date
Title

GB1942778A

GB1588865A
(en)

1978-05-13
1978-05-13
Electromagnetic wave propagation well logging utilizing multiple phase shift measurement

Publications (1)

Publication Number
Publication Date

GB1588865A
true

GB1588865A
(en)

1981-04-29

Family
ID=10129211
Family Applications (1)

Application Number
Title
Priority Date
Filing Date

GB1942778A
Expired

GB1588865A
(en)

1978-05-13
1978-05-13
Electromagnetic wave propagation well logging utilizing multiple phase shift measurement

Country Status (1)

Country
Link

GB
(1)

GB1588865A
(en)

Cited By (1)

* Cited by examiner, † Cited by third party

Publication number
Priority date
Publication date
Assignee
Title

EP1269222A1
(en)

2000-03-03
2003-01-02
Baker Hughes Incorporated
Method of interpreting induction logs in horizontal wells

1978

1978-05-13
GB
GB1942778A
patent/GB1588865A/en
not_active
Expired

Cited By (2)

* Cited by examiner, † Cited by third party

Publication number
Priority date
Publication date
Assignee
Title

EP1269222A1
(en)

2000-03-03
2003-01-02
Baker Hughes Incorporated
Method of interpreting induction logs in horizontal wells

EP1269222A4
(en)

2000-03-03
2008-10-01
Baker Hughes Inc
Method of interpreting induction logs in horizontal wells

Información de contacto