• 专利附录
  • 专利说明
  • 权利要求
  • 类似技术
  • 同族专利
  • 引用文献
  • 法律状态
  • 优先权
    • 专利摘要:
    In accordance with at least one aspect of this disclosure, a signal arithmetic processor includes a fiber optic cable including a fiber optic input and a fiber optic output and two or more electro-optical transducers coupled to the fiber optic cable between the fiber optic input and output and having at least a first electrode and second electrode, the two or more electro-optical transducers configured to modify an optical signal in the fiber optic cable based on a voltage between the first electrode and the second electrode of the two or more electro-optical transducers. The signal arithmetic processor can also include an interferometer coupled to the fiber optic cable and configured to sense a phase difference of a fiber optic signal between the fiber optic input and the fiber optic output.
    公开号:NL1042120A
    申请号:NL1042120
    申请日:2016-10-28
    公开日:2017-06-22
    发明作者:R Capoglu Ilker；Donderici Burkay
    申请人:Halliburton Energy Services Inc；
    IPC主号:
    专利说明:

    SENSOR SYSTEMS
    BACKGROUND 1. Field
    The present disclosure relates to electromagnetic (EM) and fiber optic (FO) sensors for reservoir monitoring. 2. Description of Related Art
    Permanently installed fiber optic-based electromagnetic (EM) reservoir monitoring systems can be used to monitor one or more conditions in a reservoir. Such systems can include EM sensors bonded to an optical fiber that are remotely interrogated.
    In certain systems, when there are multiple EM sensors operating independently on a sensor system (e.g., in a wireline array tool or a reservoir monitoring array), it may be necessary to perform arithmetic operations and linear combinations on the outputs of these sensors. A possible solution would require using complex active electronics (amplifiers, microprocessors, etc.) which are not capable of withstanding the high temperatures and pressures of the downhole environment.
    An alternative method is to measure each EM sensor output individually and combine them at the surface. This has the disadvantage of requiring either miles of extra fiber optic line (for each fiber optic sensor) or the implementation of complicated optical multiplexing schemes.
    Such conventional methods and systems have generally been considered less than satisfactory for their intended purpose. Thus, there is still a need in the art for improved sensor systems. The present disclosure provides a solution for this need. WO 2015/130298 A1 discloses optical electric field sensors having passivated electrodes for permanent electromagnetic monitoring of the regions around and between wells may employ a casing string positioned within a borehole through the subsurface formations of interest. At least two passivated electrodes are mounted on the casing string to sense electric fields in the formation. Though only capacitively coupled to the formation, the passivated electrodes nevertheless provide a potential difference to an electro-optical transducer, which in turn modifies a property of the light passing along an optical fiber attached to the casing string. An interface unit senses the modified property to derive a measure of the eletric field between each pair of passivated electrodes. The passivated electrodes have a contact surface that is conductive but for one or more layers of non-reactive (and thus electrically insulating) materials. Illustrative materials include metal oxides, polymers and ceramics, but the layers are preferably kept very thin to maximize the coupling capacitance with the formation. WO 2015/178876 A1 discloses electromagnetic measurement systems and methods for a downhole environment. An example system includes an optical fiber, an EM source to emit an EM field, and a magnetic induction sensor. The magnetic induction sensor comprises a coil and an electro-optical transducer coupled to the coil and the optical fiber. The electro-optical transducer generates a light beam or modulates a source light beam in the optical fiber in accordance with a voltage induced in the coil by the EM field. An example method includes positioning an optical fiber and magnetic induction sensor in the downhole environment, the magnetic induction sensor having a coil and an electro-optical transducer coupled to the coil and the optical fiber. The method also includes emitting an EM field and generating a light beam or modulating a source light beam, by the electro-optical transducer, in the optical fiber in accordance with a voltage induced in the coil by the EM field.
    BRIEF DESCRIPTION OF THE DRAWINGS A signal arithmetic processor according to the present invention is defined by the combination of features of claim 1. A sensor system according to the present invention is defined by the combination of features of claim 7. A well tool according to the present invention is defined by the combination of features of claim 11. Dependent claims relate to preferred embodiments.
    So that those skilled in the art to which the subject disclosure appertains will readily understand how to make and use the devices and methods of the subject disclosure without undue experimentation, embodiments thereof will be described in detail herein below with reference to certain figures, wherein:
    Fig. 1 is a schematic plan view of an embodiment of a signal arithmetic processor in accordance with this disclosure, showing a first, second, and third fiber optic transducers having first, second, and third voltage terminal pairs, and a single fiber passing through all transducers;
    Fig. 2 is a perspective view of an embodiment of an electro-optical transducer in accordance with this disclosure;
    Fig. 3 A shows an embodiment of a setup for interrogating total phase change in the signal arithmetic processor of Fig. 1 using an intrinsic Fabry-Perot interferometer (IFPI);
    Fig. 3B shows an embodiment of a setup for interrogating the total phase change in the signal arithmetic processor of Fig. 1 using Mach-Zehnder interferometer;
    Fig. 3C shows an embodiment of a setup for interrogating the total phase change in the signal arithmetic processor of Fig. 1 using a Michelson interferometer;
    Fig. 4 is a side elevational schematic view of an embodiment of a magnetic-field sensing system, shown with the outputs of two receiver coils connected to first and second voltage terminals of an arithmetic processing unit to subtract one output from the other for axial bucking;
    Fig. 5 is a perspective schematic view of an embodiment of an electric-field sensing system, shown with the outputs of two azimuthally-opposite electrodes and a metallic supporting tubular structure connected to a signal arithmetic processor which subtracts one from the other for azimuthal bucking; and
    Fig. 6 is a perspective schematic view of an embodiment of an electromagnetic (EM) ranging system, shown with two azimuthally-opposed EM sensors placed on a bottom-hole assembly (BHA) operatively connected to a signal arithmetic processor to subtract the outputs of the EM sensors for azimuthal differencing.
    DETAILED DESCRIPTION
    Reference will now be made to the drawings wherein like reference numerals identify similar structural features or aspects of the subject disclosure. For purposes of explanation and illustration, and not limitation, an illustrative view of an embodiment of a signal arithmetic processor in accordance with the disclosure is shown in Fig. 1 and is designated generally by reference character 100. Other embodiments and/or aspects of this disclosure are shown in Figs. 2-6. The systems and methods described herein can be used to process a plurality of sensor signals.
    In accordance with at least one aspect of this disclosure, a signal arithmetic processor 100 includes a fiber optic cable 101 including a fiber optic input 101a and a fiber optic output 101b. The fiber optic cable 101 can include one or more fibers and/or segments thereof for carrying a fiber optic signal therein. In certain embodiments, the fiber optic input 101a can be operatively connected to a fiber optic receiver (e.g., associated with a computer) for reading a fiber optic signal. One or both of the fiber optic input 101a and the fiber optic output 101b can be operatively connected to a fiber optic signal interrogator (not expressly shown) for measuring signal differences between the input 101a and the output 101b.
    Two or more electro-optical transducers 103 are coupled to the fiber optic cable 101 between the fiber optic input 101a and output 101b. Each transducer 103 has at least a first electrode 103 a and second electrode 103b. The two or more electro-optical transducers 103 are configured to modify an optical signal in the fiber optic cable 101 based on a voltage between the first electrode 103 a and the second electrode 103 b of each respective electro-optical transducers 103.
    In certain embodiments, the signal arithmetic processor 100 can include at least two (e.g., three as shown in Fig. 1) electro-optical transducers 103. In certain embodiments, each electro-optical transducer 103 can have a predetermined scale factor for controlling the effect of the voltage acting on each transducer 103 on the optical signal in the fiber optical cable 101.
    In certain embodiments, the predetermined scale factor of each electro-optical transducer 103 can be different. For example, each of the predetermined scale factors can be selected based on a characteristic of an associated sensor for each transducer 103. The characteristic of each transducer can include at least one of, for example, a location of the associated sensor, a sensor design, and/or any other suitable sensor characteristics.
    As shown in Fig. 1, a number of transducers 103 can be placed in a processor package 105, with a single common fiber optic cable 101 passing through each transducer 103. There may be N number of transducers 103 (e.g., N=3 as shown) in a given processor package 105. Although Fig. 1 shows three transducers 103 (e.g., labelled as 1,2, and 3), any suitable number of transducers 103 can be utilized. Each electrode pair 103a, 103b is exposed to an input voltage denoted in Fig. 1 by Vi, V2, and V3 for each transducer 103, respectively. Each of these voltages can be the output of a suitable sensor (e.g., as described below in Figs. 4, 5, and 6). In certain embodiments, each transducer 103 can convert the voltage applied to its electrodes 103a, 103b into a change in total phase of the light (e.g., a fiber optic signal) passing through the fiber optic cable 101. In certain cases, a positive/negative voltage corresponds to a positive/negative change in phase.
    The amount of change in the total phase is proportional to the amplitude of the applied voltage. Thus the total change of phase between points A and B on the fiber can be expressed by
    where ab α2, and α3 are scale factors (as described above) for each of the three transducers 103 of Fig. 1, respectively, and where Vi, V2, and V3 are voltages applied to each of the three transducers 103 of Fig. 1, respectively. As described above, the scale factors can be a function of physical characteristics of associated sensors (e.g., as shown in Figs. 4-6), which can be customized to for any desired arithmetic operation. For example, a negative scale factor can be realized by reversing the polarity of the associated electrodes 103a, 103b such that the input voltage is reversed.
    Referring to Fig. 2, one or more of the transducers 103 can include a piezoelectric body 201 operatively connected to the first and second electrode 103a, 103b. As shown, the fiber optic cable 101 can be wound around the piezo-electric body 201 such that any strain in the piezoelectric body 201 is effectively transferred to the fiber. The strain induced in the piezoelectric body 201 (and hence the strain transferred to the fiber) is proportional to the voltage applied across its electrodes 103a, 103b. The predetermined scale factors as described above can be a function of at least one of piezoelectric coefficient of the body 201 and/or the number of optic cable 101 windings around the body 201. Thus, for example, in certain embodiments, the scale factor can be doubled if the number of turns of the fiber optic cable 101 are doubled.
    While the body 201 is shown as cylindrical, any suitable shape is contemplated herein. While the fiber optic cable 101 is shown wound around a circumference of the body 201, it is contemplated that the cable 101 can be wound in longitudinal and/or any other suitable manner (e.g., with multiple layers of winding). While the electrodes 103a, 103b are often longitudinal plates, the electrodes 103a, 103b can have any suitable shape and can be placed at any suitable position on the body 201 (e.g., for exciting a certain piezoelectric resonance mode).
    In certain embodiments, one or more of the transducers 103 can include a lithium niobate (LiNb03) phase modulator. The voltage applied across the LiNb03 phase modulator causes a variation of the refractive index inside the LiNb03 phase modulator. This causes a modulation of optical phase change in the light travelling through the LiNb03 phase modulator.
    Referring to Figs. 3 A-3C, the optical phase change of the fiber optic signal between the input 101a and the output 101b can be remotely interrogated using well known interrogation techniques such as intrinsic Fabry-Perot with the interrogator located at the surface as shown in Fig. 3 A. In this case, two partially reflective mirrors (e.g., Fiber Bragg gratings (“FBG”)) are located at the input 101a and the output 101b. Similarly, other interrogating methods involving a Mach-Zehnder (see couplers) and/or Michelson (see Faraday rotator mirrors) interferometer can be applied as shown in Figs. 3B and 3C, respectively.
    In accordance with at least one aspect of this disclosure, a sensor system can include a plurality of sensors and a signal arithmetic processor as described above, wherein each electro-optical transducer 103 is configured to modify an optical signal in the fiber optic cable 101 based on a voltage from each sensor between the first electrode 103a and the second electrode 103 b of each electro-optical transducer 103. The plurality of sensors can include a magnetic field sensor. In certain embodiments, the plurality of sensors include an electric field sensor. Any suitable sensor is contemplated herein.
    Referring to Fig. 4, a portion of a magnetic-field sensing system 400 is illustrated. The system 400 has sensors that include two axial receiver coils 401a, 401b wrapped around a supporting structure 403 (e.g., a mandrel of a wireline tool, a bottom hole-assembly (BHA) of an LWD/MWD tool, or a casing of a reservoir monitoring system).
    The outputs of the receiver coils 401a, 401b are connected to electrodes 103a, 103b of a respective transducer 103 of a signal arithmetic processor 100.
    The system 400 is amenable to conventional axial receiver-side bucking, which is a way of canceling the direct signal from the transmitter (not shown in Fig. 4). However, by using the signal arithmetic processor 100 as described hereinabove, the voltage outputs of coil 401a can be subtracted from that of coil 401b inside the signal arithmetic processor 100 downhole without the need for complex electronics. Moreover, the winding orientations (clockwise vs. counter-clockwise) of the two receiver coils 401a, 401b are immaterial as long as the voltage inputs to the processor 100 are of the correct polarity.
    Referring to Fig. 5, a portion of an embodiment of an electric-field sensing system 500 is illustrated. Excitation current is shown flowing nearly azimuthally outward from a cylindrical metallic supporting structure 503 (e.g., a mandrel of a wireline tool, a bottom hole-assembly (BHA) of an LWD/MWD tool, or a casing of a reservoir monitoring system). The outward current can be collected far away at another metallic object (e.g., a ground stake). One or more receiver electrode pairs 501a, 501b can be placed around the structure 503 in any suitable azimuthal pattern on an insulating pad 505.
    In this embodiment, voltages Vi and V2 from each electrode 501a, 501b on the supporting structure 503 are input to the signal arithmetic processor 100 which subtracts
    Vi from V2, possibly with some scaling factors as described above. This embodiment corresponds to an azimuthal bucking scheme, which serves to cancel the baseline voltage without any formation inhomogeneities, but without the need for complex electronics. Any suitable number of receiver electrode pairs 501a, 501b could be placed around the supporting structure 503, and each pair 501a, 501b can be bucked using one or more signal arithmetic processors 100 (e.g., each pair 501a, 501b can have separate processors 100). More electrode pairs around the supporting structure 503 can provide more azimuthal sensitivity to formation inhomogeneity, for example.
    Referring to Fig. 6, an embodiment of an EM ranging system 600 is shown having a pair of EM sensors 601a, 601b (e.g., magnetometers or magnetometer arrays) placed in different azimuthal locations on a section 603 of a bottom-hole-assembly (BHA). The output voltages of the two EM sensors 601a, 601b can be connected as inputs to a signal arithmetic processor 100, which then takes the difference between the two voltages, possibly with some scaling factors as described above. This type of processing can be useful for determining the azimuthal direction to a current source. Any suitable number of sensor pairs 601a, 601b can be placed around the BHA section 603, and each pair can be differenced using one or more processors 100 (e.g., one for each pair). More sensor pairs around the BHA section 603 can provide better azimuthal ranging sensitivity, for example.
    It is contemplated that any other suitable well tool (e.g., with a tubular body) can include a plurality of sensors disposed on or within the tubular body and a signal arithmetic processor as described above disposed on or within the tubular body. As an example, embodiments can be used to process data from array tools on wireline logging devices, from array tools on logging-while-drilling (LWD) or measuring while-drilling (MWD) equipment, from array tools on permanent reservoir monitoring systems, from array tools on EM ranging systems, and from array tools on cement monitoring systems. Also, embodiments can be deployed on either metal (e.g., steel) casing or insulated (e.g., fiber glass) casing, deployed in either offshore or onshore wells, and/or operated in the presence of any formation fluid.
    Utilizing devices and systems as described above, when there are multiple EM sensors operating independently on a sensor system (such as in a wireline array tool or a reservoir monitoring array), it is possible to perform arithmetic operations and linear combinations of signals on the outputs of the sensors without using any complex active electronics (amplifiers, microprocessors, etc.). As a result, the reliability of the whole system is improved substantially.
    For example, embodiments remove the need for extra wires, fiber lines, and complicated multiplexing schemes for performing the same linear combination of EM sensor outputs. ASPECTS
    In accordance with at least one aspect of this disclosure, a signal arithmetic processor includes a fiber optic cable including a fiber optic input and a fiber optic output and two or more electro-optical transducers coupled to the fiber optic cable between the fiber optic input and output and having at least a first electrode and second electrode the two or more electro-optical transducers configured to modify an optical signal in the fiber optic cable based on a voltage between the first electrode and the second electrode of the two or more electro-optical transducers. The signal arithmetic processor can also include an interferometer coupled to the fiber optic cable and configured to sense a phase difference of a fiber optic signal between the fiber optic input and the fiber optic output.
    In certain embodiments, each electro-optical transducer can include a predetermined scale factor. The predetermined scale factor of each electro-optical transducer can be different from at least one other electro-optical transducer or the same. Each of the predetermined scale factors can be selected based on a characteristic of an associated sensor for each transducer. The characteristic of each electro-optical transducer can include at least one of a location of the associated sensor or a sensor design.
    The two or more electro-optical transducers can include a piezoelectric body operatively connected to the first and second electrode, wherein the fiber optic cable is wound around the piezo-electric body. The predetermined scale factors can be a function of at least one of piezoelectric coefficient or the number of cable windings.
    In certain embodiments, the interferometer can include at least one of an intrinsic Fabry-Perot interferometer, a Mach-Zehnder interferometer, or a Michelson interferometer. A sensor system can include a plurality of sensors and a signal arithmetic processor having a fiber optic cable including a fiber optic input and a fiber optic output and a plurality of electro-optical transducers coupled to the fiber optic cable between the fiber optic input and output and having at least a first electrode and second electrode electrically connected to each sensor, wherein each electro-optical transducer is configured to modify an optical signal in the fiber optic cable based on a voltage from each sensor between the first electrode and the second electrode of each electro-optical transducer. The signal arithmetic processor can also include an interferometer coupled to the fiber optic cable and configured to sense a phase difference of a fiber optic signal between the fiber optic input and the fiber optic output.
    In certain embodiments, the plurality of electro-optical transducers can include two electro-optical transducers. Each electro-optical transducer can include a predetermined scale factor. The predetermined scale factor of each electro-optical transducer can be different from at least one other electro-optical transducer.
    In certain embodiments, the predetermined scale factors can be selected based on a characteristic of an associated sensor for each electro-optical transducer. The characteristic of each electro-optical transducer can include at least one of a location of the associated sensor or a sensor design.
    The two or more electro-optical transducers can include a piezoelectric body operatively connected to the first and second electrode, wherein the fiber optic cable is wound around the piezo-electric body. In certain embodiments, the predetermined scale factors can be a function of at least one of piezoelectric coefficient or the number of cable windings.
    The plurality of sensors can include a magnetic field sensor. In certain embodiments, the plurality of sensors include and electric field sensor.
    In certain embodiments, the interferometer can include at least one of an intrinsic Fabry-Perot interferometer, a Mach-Zehnder interferometer, or a Michelson interferometer. A well tool can include a tubular body, a plurality of sensors disposed on or within the tubular body, and a signal arithmetic processor disposed on or within the tubular body, the signal arithmetic processor including features as described above.
    The methods and systems of the present disclosure, as described above and shown in the drawings, provide for sensor systems with superior properties including downhole signal arithmetic processing. While the apparatus and methods of the subject disclosure have been shown and described with reference to embodiments, those skilled in the art will readily appreciate that changes and/or modifications may be made thereto without departing from the spirit and scope of the subject disclosure.
    权利要求:
    Claims (11)
    [1]
    A signal-arithmetic processor (100), comprising: a fiber optic cable (101) including a fiber optic input (101a) and a fiber optic output (101b); and two or more electro-optical transducers (103) coupled to the fiber optic cable (101) between the fiber optic input (101a) and the fiber optic output (101b) and having at least a first electrode (103a) and second electrode (103b), wherein the two or more electro-optic transducers (103) are configured to change an optical signal in the fiber optic cable (101) based on a voltage between the first electrode (103a) and the second electrode (103b) of the two or a plurality of electro-optical transducers (103); and an interferometer coupled to the fiber optic cable (101) and configured to sense a phase difference of a fiber optic signal between the fiber optic input (101a) and the fiber optic output (101b), wherein each electro-optical transducer (103) includes a contains predetermined scale factor, wherein the predetermined scale factor of each electro-optical transducer (103) differs from at least one other electro-optical transducer.
    [2]
    The signal-computing processor of claim 1, wherein each of the predetermined scale factors is selected based on a characteristic of an associated sensor for each electro-optical transducer (103).
    [3]
    The signal-computing processor of claim 2, wherein the characteristic of an associated sensor for each transducer (103) includes at least one of a location of the associated sensor or a sensor design.
    [4]
    The signal-computing processor of any of the preceding claims, wherein the two or more electro-optical transducers (103) include a piezoelectric body (201) that is functionally connected to the first and second electrode (103a, 103b) and wherein the fiber optic cable (101) is wound around the piezoelectric body (201).
    [5]
    The signal-computing processor of claim 4, wherein the predetermined scale factors are a function of at least one of the piezoelectric coefficient or the number of cable windings.
    [6]
    The signal arithmetic processor of any of the preceding claims, wherein the interferometer includes at least one of an intrinsic Fabry-Perot interferometer, a Mach-Zehnder interferometer or a Michelson interferometer.
    [7]
    7. A sensor system consisting of: a plurality of sensors; and a signal-computing processor (101) according to any one of the preceding claims.
    [8]
    The system of claim 7, wherein the two or more electro-optical transducers (103) comprise two electro-optical transducers.
    [9]
    The system of claim 7 or 8, wherein the plurality of sensors comprises a magnetic field sensor.
    [10]
    The system according to any of claims 7 to 9, wherein the plurality of sensors comprises, inter alia, an electric field sensor.
    [11]
    A wellbore tool comprising: a tubular body; a plurality of sensors positioned on or within the tubular body; and a signal-computing processor (101) according to any of claims 1 to 10 positioned on or within the tubular body.
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    同族专利:
    公开号 | 公开日
    WO2017099733A1|2017-06-15|
    US11048011B2|2021-06-29|
    US20180321411A1|2018-11-08|
    FR3044780A1|2017-06-09|
    NL1042120B1|2017-07-03|
    引用文献:
    公开号 | 申请日 | 公开日 | 申请人 | 专利标题
    US4939447A|1987-11-13|1990-07-03|Bbc Brown Boveri Ag|Fiber-optic voltage sensor|
    US5675674A|1995-08-24|1997-10-07|Rockbit International|Optical fiber modulation and demodulation system|
    WO2015130298A1|2014-02-28|2015-09-03|Halliburton Energy Services, Inc.|Optical electric field sensors having passivated electrodes|
    WO2015178876A1|2014-05-19|2015-11-26|Halliburton Energy Services, Inc.|A magnetic induction sensor with an electro-optical transducer and related methods and systems|
    US5123065A|1991-06-17|1992-06-16|Tektronix, Inc.|Electro-optical transducer module|
    JP2002116087A|2000-10-10|2002-04-19|Fuji Electric Co Ltd|Wavelength-measuring apparatus|
    US7366055B2|2006-05-05|2008-04-29|Optoplan As|Ocean bottom seismic sensing system|
    WO2008091645A1|2007-01-24|2008-07-31|Davidson Energy|Transducer for measuring environmental parameters|
    US9273548B2|2012-10-10|2016-03-01|Halliburton Energy Services, Inc.|Fiberoptic systems and methods detecting EM signals via resistive heating|
    US20140139225A1|2012-11-16|2014-05-22|Halliburton Energy Services, Inc.|Well monitoring with optical electromagnetic sensors|
    US9091785B2|2013-01-08|2015-07-28|Halliburton Energy Services, Inc.|Fiberoptic systems and methods for formation monitoring|US10808525B2|2017-12-26|2020-10-20|Halliburton Energy Services, Inc.|Alternating polarity of casing-side antennas in a wellbore|
    法律状态:
    2021-06-02| MM| Lapsed because of non-payment of the annual fee|Effective date: 20201101 |
    优先权:
    申请号 | 申请日 | 专利标题
    PCT/US2015/064563|WO2017099733A1|2015-12-08|2015-12-08|Sensor systems|
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