WO2009023526A1 - High temperature downhole tool - Google Patents
High temperature downhole tool Download PDFInfo
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- WO2009023526A1 WO2009023526A1 PCT/US2008/072494 US2008072494W WO2009023526A1 WO 2009023526 A1 WO2009023526 A1 WO 2009023526A1 US 2008072494 W US2008072494 W US 2008072494W WO 2009023526 A1 WO2009023526 A1 WO 2009023526A1
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- Prior art keywords
- downhole
- gain
- light
- semiconductor device
- tool
- Prior art date
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- 239000004065 semiconductor Substances 0.000 claims abstract description 131
- 238000000034 method Methods 0.000 claims abstract description 43
- 239000000463 material Substances 0.000 claims description 37
- 239000012530 fluid Substances 0.000 claims description 34
- 239000000758 substrate Substances 0.000 claims description 25
- 230000015572 biosynthetic process Effects 0.000 claims description 17
- 238000005553 drilling Methods 0.000 claims description 17
- 238000001816 cooling Methods 0.000 claims description 14
- 238000012360 testing method Methods 0.000 claims description 12
- 238000004891 communication Methods 0.000 claims description 10
- 238000004519 manufacturing process Methods 0.000 claims description 9
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- 229910001218 Gallium arsenide Inorganic materials 0.000 claims description 7
- 239000002096 quantum dot Substances 0.000 claims description 7
- 230000002277 temperature effect Effects 0.000 claims description 7
- 230000001133 acceleration Effects 0.000 claims description 5
- 238000002835 absorbance Methods 0.000 claims description 4
- GYHNNYVSQQEPJS-UHFFFAOYSA-N Gallium Chemical compound [Ga] GYHNNYVSQQEPJS-UHFFFAOYSA-N 0.000 claims description 3
- 229910052782 aluminium Inorganic materials 0.000 claims description 3
- XAGFODPZIPBFFR-UHFFFAOYSA-N aluminium Chemical compound [Al] XAGFODPZIPBFFR-UHFFFAOYSA-N 0.000 claims description 3
- 229910052733 gallium Inorganic materials 0.000 claims description 3
- 229910052738 indium Inorganic materials 0.000 claims description 3
- APFVFJFRJDLVQX-UHFFFAOYSA-N indium atom Chemical compound [In] APFVFJFRJDLVQX-UHFFFAOYSA-N 0.000 claims description 3
- 150000004767 nitrides Chemical class 0.000 claims description 3
- 238000005755 formation reaction Methods 0.000 description 12
- 238000010586 diagram Methods 0.000 description 5
- 230000003287 optical effect Effects 0.000 description 4
- 238000005253 cladding Methods 0.000 description 3
- 229910000807 Ga alloy Inorganic materials 0.000 description 2
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- 229910000980 Aluminium gallium arsenide Inorganic materials 0.000 description 1
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Classifications
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- G—PHYSICS
- G01—MEASURING; TESTING
- G01V—GEOPHYSICS; GRAVITATIONAL MEASUREMENTS; DETECTING MASSES OR OBJECTS; TAGS
- G01V8/00—Prospecting or detecting by optical means
- G01V8/02—Prospecting
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N21/00—Investigating or analysing materials by the use of optical means, i.e. using sub-millimetre waves, infrared, visible or ultraviolet light
- G01N21/17—Systems in which incident light is modified in accordance with the properties of the material investigated
-
- 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
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01S—DEVICES USING THE PROCESS OF LIGHT AMPLIFICATION BY STIMULATED EMISSION OF RADIATION [LASER] TO AMPLIFY OR GENERATE LIGHT; DEVICES USING STIMULATED EMISSION OF ELECTROMAGNETIC RADIATION IN WAVE RANGES OTHER THAN OPTICAL
- H01S5/00—Semiconductor lasers
- H01S5/30—Structure or shape of the active region; Materials used for the active region
Definitions
- the present disclosure generally relates to well bore tools and in particular to apparatus and methods for conducting downhole operations.
- the apparatus includes a high-gain semiconductor device having a plurality of semiconductor layers forming an active region, the active region having a bandgap offset that provides device operation through at least the temperature environment of a downhole location, the high-gain semiconductor device being used at least in part to estimate a downhole parameter.
- a method for estimating a downhole parameter includes carrying a tool to a downhole location adjacent a subterranean formation using a carrier; and operating a high-gain semiconductor device and the tool together to estimate the downhole parameter, wherein the high-gain semiconductor includes a plurality of semiconductor layers forming an active region, the active region having a bandgap offset that provides device operation through at least the temperature environment of the downhole location.
- a method for manufacturing a downhole semiconductor includes providing a substrate, providing a plurality of materials selected based in part on temperature effect on the materials, and combining the materials on the substrate using a layering process to form a high-gain semiconductor device having a plurality of semiconductor layers forming an active region, the active region having a bandgap offset that provides device operation through at least the temperature environment of a downhole location.
- high temperatures cause stress on tools and reduce useful life without complex cooling systems designed into the tool used.
- Typical semiconductor devices are likewise subject to failure in high temperatures experienced in the downhole environment. Non-semiconductor devices may be larger and more susceptible to failure caused by drilling vibration, rough handling and tool impacts even in wireline operations.
- FIG. 1 is a cross section view of an exemplary high-gain semiconductor device that may be used in the several embodiments of the disclosure;
- FIG. 2 illustrates a non-limiting example of a high-gain semiconductor according to FIG. 1 where the semiconductor is configured as a laser device;
- FIG. 3 is a non-limiting example of a layered semiconductor structure that may be used to construct a Quantum Well device useful in the several embodiments disclosed herein;
- FIG. 4 is a non-limiting example of a layered semiconductor structure that may be used to construct a Quantum Dot device useful in the several embodiments disclosed herein;
- FIG. 5 is a non-limiting example of a layered semiconductor structure that may be used to construct a Quantum Wire device useful in the several embodiments disclosed herein;
- FIG. 6 illustrates a non-limiting example of a s a layered semiconductor structure that may be used to construct a Quantum Dash device useful in the several embodiments disclosed herein;
- FIG. 7 represents an energy diagram for an exemplary heterostructure semiconductor device
- FIG. 8 is an example an energy diagram showing the effect of temperature-based bandgap engineering
- FIG. 9 schematically represents a non-limiting example of a tool for conducting a downhole operation
- FIG. 10 is a non-limiting example of a well logging apparatus according to several embodiments of the disclosure.
- FIG. 11 is a non-limiting elevation view of an exemplary simultaneous drilling and logging system that incorporates several aspects of the disclosure.
- FIG. 12 is a non-limiting example of a method for constructing a high-gain semiconductor device.
- high temperature refers to a range of temperatures typically experienced in oil production well boreholes.
- high temperature and downhole temperature include a range of temperatures from about 100° C to about 200° C (about 212° F to about 390° F).
- high-gain means that the ratio of output over input that is at least higher than unity. Depending on the type of semiconductor device, gain may refer to any output/input ratio.
- Non-limiting examples include voltage, current, power and light (optic gain).
- the high-gain semiconductor device 100 includes a substrate 102 disposed on a bottom electrode 104.
- a high-gain media 106 is disposed on the substrate 102 and a top electrode 108 is disposed on the high-gain region 106.
- the terms top and bottom are merely references with respect to the non-limiting example shown in Fig. 1, and any other electrode position and/or orientation is within the scope of the disclosure.
- the high-gain media semiconductor 100 may be configured for any application where a high-gain region 106 is desirable, and application where more than one junction and more than two electrodes are desired are within the scope of the disclosure.
- the semiconductor device may be a diode, a transistor, a field effect transistor (FET), a laser diode or any other useful semiconductor device using a high-gain media.
- FET field effect transistor
- the following discussion will use the two-electrode example illustrated.
- the substrate 102 and high-gain media 106 of the present disclosure are selected and layered with respect to temperature that allows use with the temperature extremes of the well borehole environment.
- speed and bandwidth may be reduced by the selection of semiconductor materials and/or dimensions.
- thicker layering of the high-gain media materials and substrate will increase temperature tolerance and may decrease device speed and bandwidth.
- the high-temperature high-gain media semiconductor device 100 may used in any number of sensor, communication, switching, amplification and information handling applications.
- the semiconductor 100 may be laser device that may be used in a downhole tool.
- the laser device is a semiconductor laser where the high-gain media 106 will include an optical region sandwiched between the substrate 102 and the top electrode 108.
- FIG. 2 shows a cross section of the high-gain semiconductor of FIG. 1 in more detail and where the semiconductor is configured as a laser device 200.
- the laser device 200 includes an optical region 202.
- the optical region 202 includes layered semiconductors between a bottom mirror 204 and a top mirror 206.
- the semiconductor layers form an active region 208 between the top mirror 208 and the bottom mirror 206.
- the active region 210 is a region having a material (active material) that is excited by energy added to the materials.
- the active region 210 includes a light-emitting region 212 between cladding layers 214.
- the exemplary laser device 200 is that of a Vertical-Cavity Surface-Emitting Laser ("VCSEL") device that emits coherent light through a window 216 in a top electrode 218.
- the bottom mirror 206 in this VCSEL example is a fully reflective mirror, while the top mirror 208 allows some light to transmit through the electrode window 216.
- VCSEL Vertical-Cavity Surface-Emitting Laser
- the active region 210 includes a Ga alloy cladding, such as a combination of
- a substrate of InP or of GaAs may be used depending on the desired wavelength of the laser.
- Laser wavelength may be modified in GaAs substrates by adding N to Iri( 1 - x )Ga x Al y As( 1-y ) or Iri ⁇ i- X )Ga x Al y As (1-y) quantum dots.
- the high-gain media devices described above may be formed as herterostructure devices with layered semiconductor construction. Depending on the desired downhole application and particular performance requirements, the heterostructure device may take on several forms.
- FIGS. 3-6 schematically represent non-limiting examples of high-gain media heterostructure device configurations that may be used in the several embodiments disclosed herein as well as in other embodiments within the scope of the disclosure.
- FIG. 3 shows a non-limiting example of a layered semiconductor structure 300 that may be used to construct a Quantum Well device useful in the several embodiments disclosed herein.
- the structure 300 includes a layered active region 302 sandwiched between substrate layers 304.
- the active layer 302 may comprise any combination of semiconductor materials where the combination provides operation at downhole temperatures.
- FIG. 4 is another non-limiting example of a layered semiconductor structure 400 that may be used in a Quantum Dot device useful in the several embodiments disclosed herein.
- the structure 400 includes a layered active region 402 sandwiched between substrate layers 404.
- the active layer 402 may comprise any combination of semiconductor materials where the combination provides operation at downhole temperatures.
- additional semiconductor material is deposited in the active region 402 to form dot-like structures 406 providing the semiconductor device with Quantum Dash operating characteristics.
- FIG. 5 is a non-limiting example of a layered semiconductor structure 500 that may be used in a Quantum Wire device useful in the several embodiments disclosed herein.
- the structure 500 includes a layered active region 502 surrounded by substrate 504.
- the active layer 502 may comprise any combination of semiconductor materials where the combination provides operation at downhole temperatures.
- the active region 502 being relatively wire-like within the substrate 504 provides the device with Quantum Wire operating characteristics.
- FIG. 6 is another non-limiting example of a layered semiconductor structure 600 that may be used in a Quantum Dash device useful in the several embodiments disclosed herein.
- the structure 600 includes a layered active region 602 sandwiched between substrate layers 604 (only one being shown to illustrate the internal structure.).
- the active layer 602 may comprise any combination of semiconductor materials where the combination provides operation at downhole temperatures. During manufacture, additional semiconductor material is deposited in the active region 602 to form multiple ridge-like structures 606. These ridge-like structures provide the device with Quantum Dash operating characteristics.
- FIG. 7 represents an energy diagram 700 for an exemplary heterostructure semiconductor device similar to those devices disclosed herein.
- the diagram 700 shows a conduction band 710 and a valence band 712 representative of a quantum device such as a in a quantum well (QW) laser.
- An energy "potential well” 714 is created when one material is combined (sandwiched) between other materials of different composition. For example, ALGaAs layers sandwiching an InGaAs materials will produce potential well similar to the potential well 714.
- the valence band 712 in this example may be formed using materials oppositely-doped with respect to the materials in the conduction band 710.
- the quantum well 714 in the conduction band 710 may include any number of quantum energy levels C 1 , C 2 ... CN depending on the construction.
- the valence band 712 will include one or more hole potentials hhl.
- the energy potential between a given quantum level Cl and a hole potential hhl is the energy gap, and a barrier bandgap 702 exists between the top of the conduction band 710 and the bottom of the valence band 712.
- a conduction band offset exists between the top and bottom levels of the conduction band 710, and a valence band offset 706 exists between the top and bottom of the valence band 712.
- the operating characteristics of high-gain semiconductor devices are determined in part by the bad offsets 704,706 shown here.
- FIG. 8 illustrates the effect of bandgap engineering provided by the several examples in the disclosure where temperature effect is used to determine the bandgap offsets.
- the energy diagram 800 shows an adjusted bandgap 802, a larger conduction bandgap offset 804 and a larger valence bandgap offset 806.
- the changes depicted in FIG. 8 may be accomplished by any utilizing any of several techniques for adjusting the bandgap and associated offsets.
- FIG. 9 schematically represents a non-limiting example of a tool 900 for conducting a downhole operation.
- the tool 900 has a carrier 934 that carries the tool into a well borehole.
- the tool 900 may include any number of devices for conducting downhole operations, and several devices may include a high-gain semiconductor such as those described above and shown in FIGS. 1 through 6 that are selected for operation in the high temperatures typical of the downhole environment.
- the tool 900 may include a spectrometer 904.
- the tool 900 may include one or more of a temperature sensor 918, a pressure sensor 920, a stress sensor 922 and/ or a distance sensor 924.
- the stress sensor may also be acceleration and/or a vibration sensor.
- a downhole computing device 928 includes a processor 930 and a memory 932. The downhole computing device 928 may be coupled to the spectrometer 904 when included in the tool 900.
- the downhole computing device 928 may be in communication with other sensors 918, 920, 922, 925, when included, and may further be in communication with a high-gain semiconductor 906 used with the several sensors. Power and data may be conveyed to and from the sensors, spectrometer and computing device using an electrical conductor cable 936. hi some cases, an optical fiber 926 may be used for communicating information between tool components.
- a port 902 may be used to convey fluid into the tool 900 through a fluid conduit 912.
- a sample chamber 916 may be included for holding or transporting fluid samples. Fluids may be expelled from the tool when desired by including a port 914 for directing the fluids into the annulus out side of the tool 900.
- the exemplary spectrometer 904 may include a light source 906, a sample region
- the light source 906 includes a high-gain semiconductor used as a laser light source.
- the high-gain semiconductor may provide light having a broader emission band than that of a laser where such a light source is desired.
- the high-gain semiconductor may be selected for high-temperature operation by using a configuration as described above and shown in FIGS. 1-6.
- the several sensors 918, 920, 922, and 924 described above may also include a light source 906 emitting laser or other useful light.
- sensors or other tool devices may use a high-gain semiconductor device such as a FET, LED, MOSFET, transistor, diode or the like where the semiconductor includes the high- temperature structure described above and shown in FIGS. 1-6.
- the spectrometer 904 may be used for measuring refractive index of the formation fluid.
- the light detector 910 may be located so as to receive light after reflection and refraction from a fluid sample in the fluid sample region 908.
- the detector 910 may be placed such that light emitted from the light source 906 passes through the sample region 908 and is detected at the detector 910.
- the carrier 934 may be configured for conveying the tool 900 either on a while-drilling apparatus or on a wireline apparatus.
- the carrier 934 may include a jointed pipe, a wired pipe, a coiled tube or a wireline. Some or all of these carrier examples may be combined.
- cooling devices 938 may be utilized for cooling the semiconductor devices 906, other components such as the computing device 928 or other tool components without departing from the scope of the invention.
- cooling devices 938 may include sorption cooling devices, Dewar and thermoelectric cooling devices.
- FIG. 10 shows a non-limiting example of a well logging apparatus 1000 according to several embodiments of the disclosure.
- the well logging apparatus 1000 is shown disposed in a well borehole 1002 penetrating earth formations 1004 for making measurements of properties of the earth formations 1004.
- the borehole 1002 is typically filled with drilling fluid to prevent formation fluid influx.
- a string of logging tools 1006 is lowered into the well borehole 1002 by an armored electrical cable 1008.
- the cable 1008 can be spooled and unspooled from a winch or drum 1010.
- the tool string 1006 can be electrically connected to surface equipment 1012 by an optical fiber (not shown separately) forming part of the cable 1008.
- the surface equipment 1012 can include one part of a telemetry system 1014 for communicating control signals and data to the tool string 1006 and computer 1016.
- the computer can also include a data recorder 1018 for recording measurements made by the apparatus and transmitted to the surface equipment 1012.
- One or more logging devices 1020 form part of the tool string 1006.
- the tool string 1006 is preferably centered within the well borehole 1002 by a top centralizer 1022a and a bottom centralizer 1022b attached to the tool string 1006 at axially spaced apart locations.
- the centralizers 1022a, 1022b can be of types known in the art such as bowsprings.
- Circuitry for operating the logging tool 1020 may be located within the string
- the circuitry may further be connected to the tool 1020 through a connector 1026.
- the logging tool 1020 may incorporate a high-gain semiconductor device such as any of the devices described herein and shown in FIGS. 1 through 6.
- the tool 1020 may include any of the configurations as described above and shown in FIG. 9.
- FIG. 11 is an elevation view of a simultaneous drilling and logging system that may incorporate non-limiting embodiments of the disclosure.
- a well borehole 1102 is drilled into the earth under control of surface equipment including a drilling rig 1104.
- rig 1104 includes a drill string 1106.
- the drill string 1106 may be a coiled tube, jointed pipes or wired pipes as understood by those skilled in the art.
- a bottom hole assembly (BHA) 1108 may include a tool 1110 according to the disclosure.
- While-drilling tools will typically include a drilling fluid 1112 circulated from a mud pit 1114 through a mud pump 1116, past a desurger 1118, through a mud supply line 1120.
- the drilling fluid 1112 flows down through a longitudinal central bore in the drill string, and through jets (not shown) in the lower face of a drill bit 1122.
- Return fluid containing drilling mud, cuttings and formation fluid flows back up through the annular space between the outer surface of the drill string and the inner surface of the borehole to be circulated to the surface where it is returned to the mud pit.
- the system in FIG. 11 may use any conventional telemetry methods and devices for communication between the surface and downhole components.
- mud pulse telemetry techniques are used to communicate data from downhole to the surface during drilling operations.
- a surface controller 1124 may be used for processing commands and other information used in the drilling operations.
- the drill string 1106 can have a downhole drill motor 1126 for rotating the drill bit 1122.
- the while-drilling tool 1110 may incorporate a high-gain semiconductor device such as any of the devices described herein and shown in FIGS. 1 through 6.
- the tool 1110 may include any of the configurations as described above and shown in FIG. 9.
- a telemetry system 1128 may be located in a suitable location on the drill string
- the telemetry system 1128 may be used to receive commands from, and send data to, the surface via the mud pulse telemetry described above or by other communication techniques known in the art. For example, acoustic pipe telemetry and/or wired pipe telemetry may be used.
- the surface controller 1124 may include a processor, memory for storing data, data recorder and other peripherals.
- the surface controller 1124 may also respond to user commands entered through a suitable device, such as a keyboard.
- the BHA 1126 contains various sensors and logging- while-drilling (LWD) devices incorporating aspects of the disclosure to provide information about the formation, downhole drilling parameters and the mud motor.
- LWD logging- while-drilling
- FIG. 12 shows a non-limiting example of a method 1200 for forming a high- temperature semiconductor device for use in a downhole operation.
- the method includes selecting a substrate 1202, selecting a group of materials based on a combined temperature effect 1204 and combining and/or layering the selected materials on the substrate using a layer thickness selected based on temperature effect.
- the substrate may be selected from any suitable semiconductor material.
- the selected substrate includes a Ga alloy cladding, such as a combination of InGaAsP, AlGaAs, or InAsP.
- a substrate of InP or of GaAs may be used depending on the desired operating characteristics of the tool.
- Characteristics such as laser wavelength may be modified in GaAs substrates by adding N to InGaAlAs or InGaAlAs quantum dots.
- Selecting a group of materials based on combined temperature effect may include the selection of any suitable combination, which combination helps provide device operation in the downhole temperature environment.
- Combining the materials may include a layering process, a deposition process, wet etching, dry etching, and other known manufacturing processes suitable for combining semiconductor materials.
- the present disclosure includes combining the materials such that the combination characteristics are selected to increase operating temperature of the high-gain semiconductor device.
- the combination includes creating a heterostructure.
- the combining includes combining the materials to adjust the strain in the media, hi one example, the combining includes adjusting layer thickness to increase operating temperature.
- the selection and combining are performed such that operating speed is reduced while operating temperature is increased.
- a well tool includes a high-gain semiconductor device having a plurality of semiconductor layers forming an active region.
- the active region has a bandgap offset that provides device operation through at least the temperature environment of a downhole location.
- the high-gain semiconductor device being used at least in part to estimate a downhole parameter.
- a well tool includes a high-gain semiconductor device that comprises a light source.
- the light source may be a laser light source, while in other particular embodiments the light source may provide incoherent light.
- a downhole tool utilizing a high-gain semiconductor device may be used to estimate one or more of sample absorbance, sample reflectance, temperature, pressure, strain, acceleration, vibration and flow rate.
- the temperature environment at the downhole location may exceed 80° C, 100° C or may be within a range of about 100° C to about 200° C.
- Embodiments may include operating a high-gain semiconductor that is in direct thermal communication with the downhole temperature environment, or a cooling device may be used.
- a downhole tool includes a high-gain semiconductor that is constructed using layers of direct bandgap semiconductors.
- High-gain semiconductors disclosed herein may include semiconductor layers of direct bandgap semiconductors that include one or more of gallium, aluminum, arsenide, phosphide, indium and nitride.
- the high-gain semiconductor device may include a bandgap offset that is increased during manufacturing with respect to operating temperature.
- the bandgap offset is includes strain material at a heterojunction layer boundary, and in others a combination of direct bandgap semiconductor materials increases the bandgap offset.
- High-gain semiconductor devices disclosed herein may include a quantum well device, a quantum dot device, a quantum wire device, and/or a quantum dash device.
- a downhole tool includes a light transmitting member defining a fluid test volume, a photodetector responsive to light emitted from a high-gain semiconductor device laser after the light interacts with a formation fluid within the fluid test volume, and a processor in communication with the photodetector.
- an estimated parameter includes a pressure, and light emitted from a high-gain semiconductor device being responsive to pressure, is sensed by a transducer that converts the light to an electrical signal, and a processor receives the electrical signal and processes the signal for estimating the pressure
- an estimated parameter includes a temperature
- the tool includes a light receiving sensor that is responsive to light changes due to temperature, the light receiving sensor produces an electrical signal, and a processor receives the electrical for estimating the temperature.
- an estimated downhole parameter includes a strain
- a tool includes a light receiving sensor responsive to light changes due to strain, the light receiving sensor producing an electrical signal
- a processor receives the electrical for estimating the strain.
- an estimated parameter includes a fluid flow rate
- a tool includes a light transmitting member defining a fluid test volume
- a photodetector is responsive to light emitted from a laser after the light interacts with a formation fluid flowing within the fluid test volume and a processor in communication with the photodetector processes a photodetector output representative of fluid flow rate within the fluid test volume.
- One method includes carrying a tool to a downhole location adjacent a subterranean formation using a carrier, and operating a high-gain semiconductor device and the tool together to estimate the downhole parameter, wherein the high-gain semiconductor includes a plurality of semiconductor layers forming an active region, the active region having a bandgap offset that provides device operation through at least the temperature environment of the downhole location.
- a method for estimating a downhole parameter includes emitting a light from the light source that uses a high-gain semiconductor device.
- the high-gain semiconductor device comprises a laser light source, and the method includes emitting laser light from the light source, while in another particular embodiment a method includes emitting an incoherent light.
- methods for estimating a downhole parameter include estimating one or more of i) sample absorbance, ii) sample reflectance, iii) temperature, iv) pressure, v) strain, vi) acceleration, vii) vibration and viii) flow rate.
- methods for estimating a downhole parameter include operating a high- gain semiconductor comprises operating in a downhole temperature environment that exceeds 80° C, that exceeds 100° C and that includes a range of about 100° C to about 200° C.
- a method for manufacturing a downhole semiconductor includes providing a substrate, providing a plurality of materials selected based in part on temperature effect on the materials, and combining the materials on the substrate using a layering process to form a high-gain semiconductor device having a plurality of semiconductor layers forming an active region, the active region having a bandgap offset that provides device operation through at least the temperature environment of a downhole location.
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Abstract
Description
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Priority Applications (3)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
BRPI0816242A BRPI0816242A2 (en) | 2007-08-13 | 2008-08-07 | high temperature downhole tool |
GB1002586A GB2464431B (en) | 2007-08-13 | 2008-08-07 | High temperature downhole tool |
NO20100345A NO344094B1 (en) | 2007-08-13 | 2010-03-11 | High temperature borehole tool |
Applications Claiming Priority (2)
Application Number | Priority Date | Filing Date | Title |
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US11/837,692 US7638761B2 (en) | 2007-08-13 | 2007-08-13 | High temperature downhole tool |
US11/837,692 | 2007-08-13 |
Publications (1)
Publication Number | Publication Date |
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WO2009023526A1 true WO2009023526A1 (en) | 2009-02-19 |
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Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
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PCT/US2008/072494 WO2009023526A1 (en) | 2007-08-13 | 2008-08-07 | High temperature downhole tool |
Country Status (5)
Country | Link |
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US (1) | US7638761B2 (en) |
BR (1) | BRPI0816242A2 (en) |
GB (1) | GB2464431B (en) |
NO (1) | NO344094B1 (en) |
WO (1) | WO2009023526A1 (en) |
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WO2015051229A1 (en) | 2013-10-03 | 2015-04-09 | Baker Hughes Incorporated | Wavelength-selective, high temperature, near infrared photodetectors for downhole applications |
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US7720323B2 (en) * | 2004-12-20 | 2010-05-18 | Schlumberger Technology Corporation | High-temperature downhole devices |
US8952319B2 (en) * | 2010-03-04 | 2015-02-10 | University Of Utah Research Foundation | Downhole deployable tools for measuring tracer concentrations |
AU2011222514A1 (en) * | 2010-03-04 | 2012-09-20 | University Of Utah Research Foundation | Colloidal-crystal quantum dots as tracers in underground formations |
US8726725B2 (en) | 2011-03-08 | 2014-05-20 | Schlumberger Technology Corporation | Apparatus, system and method for determining at least one downhole parameter of a wellsite |
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US9249656B2 (en) | 2012-11-15 | 2016-02-02 | Baker Hughes Incorporated | High precision locked laser operating at elevated temperatures |
US10126433B2 (en) | 2014-11-10 | 2018-11-13 | Halliburton Energy Services, Inc. | Energy detection apparatus, methods, and systems |
US9885591B2 (en) * | 2016-03-18 | 2018-02-06 | Baker Hughes, A Ge Company, Llc | Low etendue light source for fiber optic sensors in high temperature environments |
US10620429B2 (en) * | 2017-08-30 | 2020-04-14 | Abl Ip Holding Llc | Electrowetting with compensation for force that may otherwise cause distortion or aberration |
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2008
- 2008-08-07 BR BRPI0816242A patent/BRPI0816242A2/en not_active IP Right Cessation
- 2008-08-07 GB GB1002586A patent/GB2464431B/en not_active Expired - Fee Related
- 2008-08-07 WO PCT/US2008/072494 patent/WO2009023526A1/en active Search and Examination
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US5406574A (en) * | 1991-10-23 | 1995-04-11 | Kabushiki Kaisha Toshiba | Semiconductor laser device |
US20040011950A1 (en) * | 2002-05-31 | 2004-01-22 | Harkins Gary O. | Parameter sensing apparatus and method for subterranean wells |
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Cited By (2)
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WO2015051229A1 (en) | 2013-10-03 | 2015-04-09 | Baker Hughes Incorporated | Wavelength-selective, high temperature, near infrared photodetectors for downhole applications |
EP3052758A4 (en) * | 2013-10-03 | 2017-05-31 | Baker Hughes Incorporated | Wavelength-selective, high temperature, near infrared photodetectors for downhole applications |
Also Published As
Publication number | Publication date |
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GB2464431B (en) | 2011-11-09 |
NO344094B1 (en) | 2019-09-02 |
GB2464431A (en) | 2010-04-21 |
BRPI0816242A2 (en) | 2016-07-19 |
NO20100345L (en) | 2010-05-14 |
GB201002586D0 (en) | 2010-03-31 |
US20090045814A1 (en) | 2009-02-19 |
US7638761B2 (en) | 2009-12-29 |
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