1. Field of the Invention
This invention generally relates to exploration for hydrocarbons involving electrical investigations of a borehole penetrating an earth formation. More specifically, this invention relates to highly localized borehole investigations of multifrequency focusing of survey currents injected into the wall of a borehole by capacitive coupling of electrodes on a tool moved along the borehole with the earth formation.
2. Background of the Art
Electrical earth borehole logging is well known and various devices and various techniques have been described for this purpose. Broadly speaking, there are two categories of devices used in electrical logging devices. In the first category, a measure electrode (current source or sink) are used in conjunction with a diffuse return electrode (such as the tool body). A measure current flows in a circuit that connects a current source to the measure electrode, through the earth formation to the return electrode and back to the current source in the tool. In inductive measuring tools, an antenna within the measuring instrument induces a current flow within the earth formation. The magnitude of the induced current is detected using either the same antenna or a separate receiver antenna. The present invention belongs to the first category.
There are several modes of operation. In one, the current at the measuring electrode is maintained constant and a voltage is measured, while in the second mode, the voltage of the electrode is fixed and the current flowing from the electrode is measured. Ideally, it is desirable that if the current is varied to maintain at a constant value the voltage between measure and return electrodes, the current is inversely proportional to the resistivity of the earth formation being investigated. Conversely, it is desirable that if this current is maintained constant, the voltage measured between monitor electrodes is proportional to the resistivity of the earth formation being investigated. Ohm's law teaches that if both current and voltage vary, the resistivity of the earth formation is proportional to the ratio of the voltage to the current.
Birdwell (U.S. Pat. No. 3,365,658) teaches the use of a focused electrode for determination of the resistivity of subsurface formations. A survey current is emitted from a central survey electrode into adjacent earth formations. This survey current is focused into a relatively narrow beam of current outwardly from the borehole by use of a focusing current emitted from nearby focusing electrodes located adjacent the survey electrode and on either side thereof. Ajam et al (U.S. Pat. No. 4,122,387) discloses an apparatus wherein simultaneous logs may be made at different lateral distances through a formation from a borehole by guard electrode systems located on a sonde which is lowered into the borehole by a logging cable. A single oscillator controls the frequency of two formation currents flowing through the formation at the desired different lateral depths from the borehole. The armor of the logging cable acts as the current return for one of the guard electrode systems, and a cable electrode in a cable electrode assembly immediately above the logging sonde acts as the current return for the second guard electrode system. Two embodiments are also disclosed for measuring reference voltages between electrodes in the cable electrode assembly and the guard electrode systems.
Techniques for investigating the earth formation with arrays of measuring electrodes have been proposed. See, for example, the U.S. Pat. No. 2,930,969 to Baker, Canadian Patent No. 685727 to Mann et al., U.S. Pat. No. 4,468,623 to Gianzero, and U.S. Pat. 5,502,686 to Dory et al. The Baker patent proposed a plurality of electrodes, each of which was formed of buttons which are electrically joined by flexible wires with buttons and wires embedded in the surface of a collapsible tube. The Mann patent proposes an array of small electrode buttons either mounted on a tool or a pad and each of which introduces in sequence a separately measurable survey current for an electrical investigation of the earth formation. The electrode buttons are placed in a horizontal plane with circumferential spacings between electrodes and a device for sequentially exciting and measuring a survey current from the electrodes is described.
The Gianzero patent discloses tool mounted pads, each with a plurality of small measure electrodes from which individually measurable survey currents are injected toward the wall of the borehole. The measure electrodes are arranged in an array in which the measure electrodes are so placed at intervals along at least a circumferential direction (about the borehole axis) as to inject survey currents into the borehole wall segments which overlap with each other to a predetermined extent as the tool is moved along the borehole. The measure electrodes are made small to enable a detailed electrical investigation over a circumferentially contiguous segment of the borehole so as to obtain indications of the stratigraphy of the formation near the borehole wall as well as fractures and their orientations. In one technique, a spatially closed loop array of measure electrodes is provided around a central electrode with the array used to detect the spatial pattern of electrical energy injected by the central electrode. In another embodiment, a linear array of measure electrodes is provided to inject a flow of current into the formation over a circumferentially effectively contiguous segment of the borehole. Discrete portions of the flow of current are separately measurable so as to obtain a plurality of survey signals representative of the current density from the array and from which a detailed electrical picture of a circumferentially continuous segment of the borehole wall can be derived as the tool is moved along the borehole. In another form of an array of measure electrodes, they are arranged in a closed loop, such as a circle, to enable direct measurements of orientations of resistivity of anomalies. U.S. Pat. No. 6,714,014 to Evans et al, having the same assignee as the present invention and the contents of which are incorporated herein by reference, teaches the use of capacitive coupling with the formation through both oil-based mud and water-based mud.
The Dory patent discloses the use of an acoustic sensor in combination with pad mounted electrodes, the use of the acoustic sensors making it possible to fill in the gaps in the image obtained by using pad mounted electrodes due to the fact that in large diameter boreholes, the pads will necessarily not provide a complete coverage of the borehole.
The prior art devices, being contact devices, are sensitive to the effects of borehole rugosity: the currents flowing from the electrodes depend upon good contact between the electrode and the borehole wall. If the borehole wall is irregular, the contact and the current from the electrodes are irregular, resulting in inaccurate imaging of the borehole. A second drawback is the relatively shallow depth of investigation caused by the use of measure electrodes at the same potential as the pad and the resulting divergence of the measure currents. U.S. Pat. No. 6,809,521 to Tabarovsky et al. discloses a multi-frequency method for determination of formation resistivity. The assumption made in Tabarovsky is that
where the σ's are conductivities, the ε's are dielectric constant, ω is the operating frequency, the subscript 1 refers to the mud and the subscript 2 refers to the formation. The first of the two inequalities is easily satisfied with oil based mud where the mud conductivity is extremely small. However, if the mud has a finite conductivity, the condition is hard to satisfy. It would be desirable to have an apparatus and method of determination of formation resistivity that is relatively insensitive to borehole rugosity and can be used with either water based or with oil-based muds for a wide range of formation resistivities. The present invention satisfies this need.
U.S. patent application Ser. No. 11/209,532 of Bespalov et al., having the same assignee as the present disclosure and the contents of which are incorporated herein by5 reference, discloses a dual frequency apparatus and method for borehole resistivity imaging. There are a number of technically challenging issues that still remain. One of these is the elimination of “galvanic” cross-talk between sensor electrodes through non-conductive mud and a conductive formation. This error becomes more pronounced in the presence of borehole rugosity when the sensor experience uneven standoff from the formation. Another problem with multi-electrode imaging tools is the presence of mutual inductive coupling between circuits defined by the individual button electrodes. Most importantly, while prior art methods recognize the need for methods and hardware for maintaining the buttons at equipotential using, for example, focusing electrodes, this still remains a difficult technical problem at elevated frequencies (in the MHz range). In addition, multifrequency methods require that each of the amplifiers be maintained at proper tuning at a plurality of frequencies.
One embodiment of the disclosure is a method of imaging a resistivity property of a subsurface material. The method includes conveying a logging tool having a plurality of measure electrodes into a borehole and reducing a mutual coupling between at least one pair of the plurality of measure electrodes. A first measure current having a first frequency is conveyed through a first one of the at least one pair of measure electrodes and a second measure current at the first frequency is conveyed through a second one of the at least one pair of measure electrodes. A 2-D image of the resistivity property of the subsurface material is produced using a value of the first measure current and a value of the second measure current. The mutual coupling between the at least one pair of measure electrodes may be reduced introducing a series impedance with each of the at least one pair of measure electrodes. The series impedance may be a resistance, a capacitance, and/or an inductance. The mutual coupling may be reduced by increasing a spacing between the at least one pair of measure electrodes. The mutual coupling maybe reduced by floating the second one of the at least one pair of measure electrodes while conveying the measure current through the first one of the at least one pair of measure electrodes, and floating the first one of the at least one pair of measure electrodes while conveying the measure current through the second one of the at least one pair of measure electrodes. The method may include using a return electrode to return the first measure current and the second measure current. Floating any of the plurality of electrodes may be done by disconnecting an electrical connection, and/or disabling an input to an amplifier. The method may include conveying the logging tool on a bottomhole assembly on a drilling tubular, or a downhole logging string conveyed on a wireline.
Another embodiment is an apparatus for imaging a resistivity property of a subsurface material. The apparatus includes a logging tool having a plurality of measure electrodes configured to be into a borehole, the logging tool including circuitry configured to reduce a mutual coupling between at least one pair of the plurality of measure electrodes. The apparatus also includes at least one processor configured to convey a first measure current having a first frequency through a first, single one of the at least one pair of measure electrodes, convey a second measure current at the first frequency through a second, single one of the at least one pair of measure electrodes; and produce an image of the borehole wall of the resistivity property of the subsurface material using a value of the first measure current and a value of the second measure current. The circuitry may include a series impedance with each of the at least one pair of measure electrodes. The series impedance may be a resistance, a capacitance, and/or an inductance. The apparatus circuitry may further include a processor configured to float the second one of the at least one pair of measure electrodes while conveying the measure current through the first one of the at least one pair of measure electrodes, and a processor configured to float the first one of the at least one pair of measure electrodes while conveying the measure current through the second one of the at least one pair of measure electrodes. The apparatus may include a return electrode configured to return the first measure current and the second measure current. The processor may be further configured to float any of the plurality of electrodes by disconnecting an electrical connection, and/or disabling an input to an amplifier. The apparatus may include a conveyance device configured to convey the logging tool into the borehole, the conveyance device being a drilling tubular configured to convey a bottomhole assembly, or a wireline configured to convey a logging string.
Another embodiment is a computer-readable medium for use with an apparatus for imaging a resistivity property of a subsurface material. The apparatus includes a logging tool having a plurality of measure electrodes configured to be into a borehole the logging tool including circuitry configured to reduce a mutual coupling between at least one pair of the plurality of measure electrodes. The medium includes instructions that enable at least one processor to convey a first measure current having a first frequency through a first single one of the at least one pair of measure electrodes, convey a second measure current at the first frequency through a second single one of the plurality of measure electrodes produce an image of the borehole wall of the resistivity property of the subsurface material using a value of the first measure current and a value of the second measure current. The computer-readable medium may be a ROM, an EPROM, an EAROM, a flash memory, and/or an optical disk.
The present invention is best understood with reference to the accompanying figures in which like numerals refer to like elements and in which:
Also shown in
The approximate imaging schematic circuit diagram for an ideal two-electrode case (single sensor electrode and return electrode) is presented in
In case of a conductive formation (with a resistivity less than 10 Ω-m) and oil-based mud, the contribution of the formation into the effective impedance becomes small Rf<<<ZT+ZG which results in a reduction of the sensitivity of the measured impedance to the resistivity of formation. The gap impedance ZG, which depends on the mud properties and the receiver standoff, becomes a major contributor to the effective impedance. Typically, ZT is negligible and could be excluded from considerations for on-pad oil-based imagers.
Notice that there the current flow through a button follows a path that typically includes transmitter (return) electrode—formation—mud—button—electronics and back to transmitter electrode. The path has complex impedance which is dominated by the gap capacitive reactance in oil-based mud. Some inductive reactance might also be present due to path length. However, the locality of measurements in the current disclosure makes it negligible. See, for example, U.S. Pat. No. 6,714,014 to Evans et al.
An effect that can not be ignored is the mutual magnetic coupling between these current paths and particularly in the areas where current paths become separated. This happens when currents leave a conductive formation and then flow through mud to buttons. This is illustrated in
The currents in the two electrodes are denoted by 407a, 407b. The current 407b produces a magnetic field denoted by 409 that, in turn, crosses the conduction path of the neighboring electrode 405a, thus inducing a current denoted by 411 in the first electrode 405a.
The equivalent circuit for this is depicted in
Referring to
Generalizing the discussion to a plurality of electrodes, we conclude that:
Another resistivity imaging problem associated with current re-distribution in the formation has been noted before in oil-based imagers. See, for example, U.S. Pat. No. 6,714,014 to Evans et al. Conventionally it has been called as a “defocusing” of the high frequency button current if a neighboring conductive pad structure is presented. See, for example, U.S. patent application Ser. No. 11/758,875 of Itskovich et al., filed on Jun. 6, 2007, having the same assignee as the present disclosure and the contents of which are incorporated herein by reference. As disclosed therein, the button and pad body are kept under the same potential as the sensor.
The simplified physics of this effect could be seen through example is based on equivalent Wheatstone bridge presentation and includes two neighboring buttons. As one can see from the
Providing for a high level of button equipotentiality has remained a challenge at higher frequencies. The sensor current has to be measured while entering the button and at elevated frequencies (10 MHz and above) mutual coupling of the button with associated electronics and rest of pad structure becomes an issue. Moreover, electronics itself could create unwanted biases coupled to the buttons and thus driving currents between them.
The principles of the present disclosure are illustrated by
An important aspect of the present disclosure is that only one of the electrodes (805a, 805b) is connected to a power source at a time. This means that if a measure current is flowing through one of the electrodes, 805a for example, there is no current flowing through any of the adjacent electrodes. The data are acquired sequentially by the individual electrodes rather than the prior art methods of simultaneous acquisition. Consequently, there is no need to use focusing or guard electrodes to prevent leakage current between the electrodes.
There are a number of ways by which the sequentially acquisition can be carried out. This could be done by sequentially connecting and disconnecting the switches 809a, 809b under control of the processor 821, or by disabling input circuits of preamplifiers 807a, 807b under the control of the processor 821.
Besides simplifying the hardware, the method disclosed above also eliminates the galvanic cross-talk between the channels. Based on the discussion above, when there is no current flowing through the other electrodes, the effect of mutual coupling is eliminated.
Referring now to
The disclosure above was directed towards a method and apparatus for eliminating the effects of mutual magnetic coupling between currents flowing through different electrodes. In an alternate embodiment of the disclosure, instead of completely eliminating the mutual magnetic coupling, the coupling is mitigated by introducing series impedance at each and every sense electrode. This acts to suppress the differences between the signals at each electrode, thereby reducing the relative magnitude of the cross-coupling. The series impedance can be achieved using a resistor, capacitor or inductor, or by adding an ‘impeding material’ in the current path, such as an insulator in front of the electrodes. While it is obviously not desirable to have a soft material in contact with the borehole wall, such a configuration might be acceptable for imaging a fluid. Mitigation can also be achieved by attempting to calibrate the response in an environment that is substantially similar to the measurement environment, although this is generally much less practical. Reduction of mutual coupling can also be accomplished by increasing the spacing between the electrodes.
A point to note with the present disclosure is that many of the prior art processing methods may also be applied to data acquired using the method of the present invention. This includes, for example, dual frequency focusing (U.S. patent application Ser. No. 11/209,531 of Bespalov et al.).
The invention has further been described by reference to logging tools that are intended to be conveyed on a wireline. However, the method of the present invention may also be used with measurement-while-drilling (MWD) tools, or logging while drilling (LWD) tools, either of which may be conveyed on a drillstring or on coiled tubing. An example of a resistivity imaging tool for MWD use is discloses in U.S. Pat. No. 6,600,321 to Evans, having the same assignee as the present invention and the contents of which are incorporated herein by reference.
Implicit in the processing of the data is the use of a computer program implemented on a suitable machine readable medium that enables the processor to perform the control and processing. The term processor as used in this application is intended to include such devices as field programmable gate arrays (FPGAs). The machine readable medium may include ROMs, EPROMs, EAROMs, Flash Memories and Optical disks. As noted above, the processing may be done downhole or at the surface, by using one or more processors. In addition, results of the processing, such as an image of a resistivity property, can be stored on a suitable medium.
While the foregoing disclosure is directed to the preferred embodiments of the invention, various modifications will be apparent to those skilled in the art. It is intended that all variations within the scope and spirit of the appended claims be embraced by the foregoing disclosure.