WO2010020796A1 - Conduit monitoring - Google Patents

Conduit monitoring Download PDF

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Publication number
WO2010020796A1
WO2010020796A1 PCT/GB2009/002058 GB2009002058W WO2010020796A1 WO 2010020796 A1 WO2010020796 A1 WO 2010020796A1 GB 2009002058 W GB2009002058 W GB 2009002058W WO 2010020796 A1 WO2010020796 A1 WO 2010020796A1
Authority
WO
WIPO (PCT)
Prior art keywords
conduit
fibre
pipeline
sensing
pipe
Prior art date
Application number
PCT/GB2009/002058
Other languages
French (fr)
Inventor
David John Hill
Magnus Mcewen-King
Original Assignee
Qinetiq Limited
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.)
Filing date
Publication date
Application filed by Qinetiq Limited filed Critical Qinetiq Limited
Priority to RU2011110518/28A priority Critical patent/RU2511228C2/en
Priority to CA2734820A priority patent/CA2734820C/en
Priority to US13/059,795 priority patent/US10900860B2/en
Priority to EP09784994.7A priority patent/EP2326932B1/en
Priority to CN200980141853.4A priority patent/CN102197294B/en
Publication of WO2010020796A1 publication Critical patent/WO2010020796A1/en

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Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01MTESTING STATIC OR DYNAMIC BALANCE OF MACHINES OR STRUCTURES; TESTING OF STRUCTURES OR APPARATUS, NOT OTHERWISE PROVIDED FOR
    • G01M3/00Investigating fluid-tightness of structures
    • G01M3/02Investigating fluid-tightness of structures by using fluid or vacuum
    • G01M3/04Investigating fluid-tightness of structures by using fluid or vacuum by detecting the presence of fluid at the leakage point
    • G01M3/24Investigating fluid-tightness of structures by using fluid or vacuum by detecting the presence of fluid at the leakage point using infrasonic, sonic, or ultrasonic vibrations
    • G01M3/243Investigating fluid-tightness of structures by using fluid or vacuum by detecting the presence of fluid at the leakage point using infrasonic, sonic, or ultrasonic vibrations for pipes
    • FMECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F17STORING OR DISTRIBUTING GASES OR LIQUIDS
    • F17DPIPE-LINE SYSTEMS; PIPE-LINES
    • F17D5/00Protection or supervision of installations
    • F17D5/02Preventing, monitoring, or locating loss
    • F17D5/06Preventing, monitoring, or locating loss using electric or acoustic means
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01DMEASURING NOT SPECIALLY ADAPTED FOR A SPECIFIC VARIABLE; ARRANGEMENTS FOR MEASURING TWO OR MORE VARIABLES NOT COVERED IN A SINGLE OTHER SUBCLASS; TARIFF METERING APPARATUS; MEASURING OR TESTING NOT OTHERWISE PROVIDED FOR
    • G01D5/00Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable
    • G01D5/48Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable using wave or particle radiation means
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01HMEASUREMENT OF MECHANICAL VIBRATIONS OR ULTRASONIC, SONIC OR INFRASONIC WAVES
    • G01H9/00Measuring mechanical vibrations or ultrasonic, sonic or infrasonic waves by using radiation-sensitive means, e.g. optical means
    • G01H9/004Measuring mechanical vibrations or ultrasonic, sonic or infrasonic waves by using radiation-sensitive means, e.g. optical means using fibre optic sensors
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01MTESTING STATIC OR DYNAMIC BALANCE OF MACHINES OR STRUCTURES; TESTING OF STRUCTURES OR APPARATUS, NOT OTHERWISE PROVIDED FOR
    • G01M3/00Investigating fluid-tightness of structures
    • G01M3/02Investigating fluid-tightness of structures by using fluid or vacuum
    • G01M3/04Investigating fluid-tightness of structures by using fluid or vacuum by detecting the presence of fluid at the leakage point
    • G01M3/042Investigating fluid-tightness of structures by using fluid or vacuum by detecting the presence of fluid at the leakage point by using materials which expand, contract, disintegrate, or decompose in contact with a fluid
    • G01M3/045Investigating fluid-tightness of structures by using fluid or vacuum by detecting the presence of fluid at the leakage point by using materials which expand, contract, disintegrate, or decompose in contact with a fluid with electrical detection means
    • G01M3/047Investigating fluid-tightness of structures by using fluid or vacuum by detecting the presence of fluid at the leakage point by using materials which expand, contract, disintegrate, or decompose in contact with a fluid with electrical detection means with photo-electrical detection means, e.g. using optical fibres
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01PMEASURING LINEAR OR ANGULAR SPEED, ACCELERATION, DECELERATION, OR SHOCK; INDICATING PRESENCE, ABSENCE, OR DIRECTION, OF MOVEMENT
    • G01P3/00Measuring linear or angular speed; Measuring differences of linear or angular speeds
    • G01P3/02Devices characterised by the use of mechanical means
    • G01P3/14Devices characterised by the use of mechanical means by exciting one or more mechanical resonance systems

Definitions

  • the present invention relates to conduit monitoring and inspection, and more particularly to subterranean pipeline monitoring.
  • Pipelines are the most economically viable method of transporting fluid assets, most commonly oil and gas, but other types of pipeline also exist.
  • a vast pipeline infrastructure exists today responsible for gathering, transporting and distributing these natural resources, with over three quarters of a million kilometers of oil and gas pipelines in the US alone.
  • the continuing proper operation of these pipelines is of paramount importance, and failures carry massive economic loss, environmental impact and potentially catastrophic physical damage also.
  • CCM computational pipeline monitoring
  • the present invention provides a method for monitoring a fluid carrying conduit comprising interrogating an optic fibre positioned along the path of said conduit to provide distributed acoustic sensing; introducing an acoustic pulse into the conduit; measuring by distributed acoustic sensing the response to said acoustic pulse at each of a plurality of discrete longitudinal sensing portions; and deriving from said plurality of measurements a conduit condition profile.
  • the acoustic pulse is introduced into the fluid contained in the pipe by a dedicated impulser or acoustic transducer.
  • a dedicated impulser or acoustic transducer This might typically take the form of a hydraulic ram, but other apparatus could be used to induce a pressure wave in the fluid carried by the conduit being monitored.
  • the impulser can be permanently installed in the pipeline, or can be applied at an existing valve station or junction. It has been found that such pressure pulses are capable of travelling large distances through pipelines with little attenuation, and therefore a single pulse source can provide sufficient input for monitoring 20, 30 or 40km or more of pipeline.
  • Pulses can be introduced into the fluid during normal operation, while normal flow conditions continue in the conduit, resulting in little or no downtime for monitoring operations. Pulses are introduced at intervals of 10 seconds in one embodiment, and intervals of between 5 and 20 seconds might be employed. A typical monitoring period might be 10 minutes, but other periods are possible, and continuous monitoring may be employed.
  • a pig travelling through a pipeline may be arranged to produce a series of pressure impulses.
  • the pig passes each girth weld in the pipe it encounters additional resistance and a slight overpressure builds behind the pig.
  • the pressure wave is released travelling in both directions down the pipe.
  • the frequency of the pulses depends on the spacing of the welds and the velocity of the pig. In such cases it will be understood that the position of the source of the pulses gradually moves along the pipe, however this does not affect the monitoring method adversely.
  • the pig may generate a higher acoustic signal as further constrictions or non-uniformities develop in the pipe over time, for example hydrocarbon build up or mechanical deformation. These can be identified in embodiments by looking for localised increases in generated acoustic signal over repeated pig passes.
  • a further possible source of an acoustic or pressure pulse in a conduit is a sudden crack or leak. The resulting pressure pulse can be detected and used to identify and/or locate the source and hence the location of the crack or leak.
  • a further aspect of the invention therefore provides a method for monitoring a fluid carrying conduit comprising interrogating an optic fibre positioned along the path of said conduit to provide distributed acoustic sensing; detecting an acoustic pulse at each of a plurality of discrete longitudinal sensing portions; and determining the source of said detected pulse.
  • condition profile of the pipe need not be explicitly analysed to determine corresponding physical characteristics (although this is possible). More use may be derived by monitoring a pipeline over a period of time to obtain one or more profiles, and comparing these profiles to determine changes in characteristics. Thus two pipeline profiles may be obtained corresponding to two dates having a known time separation. Differences in the profile can be determined using data analysis techniques to obtain information concerning which portions of the pipe have undergone physical changes, and hence the location of those changes. More complex statistical analysis of profiles can be undertaken if a set of multiple profiles is built up over time, and profiles will typically be obtained at regular intervals for this purpose. Additionally or alternatively profiles can be taken before or after planned maintenance or repair work to characterise known changes to the pipeline.
  • Changes in the pipe, (and possibly ground conditions surrounding the pipe) can therefore be monitored over time intervals, and the location and characterising information concerning those changes can be provided. This information may prompt further actions, such as maintenance, cleaning, physical inspection or repair.
  • the amplitude response to the acoustic pulse is measured. This may be performed by integrating across the available bandwidth for each channel. Further analysis of the data returned from distributed sensing however allows the spectral content of each channel to be provided in certain embodiments, enabling enhanced condition monitoring capability.
  • Distributed acoustic sensing in embodiments of the present invention senses seismic signals (both P pressure and S shear vibration waves) which are within a bandwidth from OHz - 5kHz. Higher frequencies are commonly strongly attenuated however, and the range from OHz to 1kHz is more commonly monitored.
  • the sensing fibre for distributed sensing may be located inside the conduit, on the exterior surface of the conduit, directly buried adjacent to the conduit or in a separate adjacent conduit, in various different embodiments.
  • the sensing fibre there is no prescribed position for the sensing fibre, provided its location is such that it is able to detect a sufficient response to the acoustic pulse. Because of the high sensitivities possible in fibre optic sensing, whereby induced phase differences can be measured using interferometric techniques, the potential scope for positioning the fibre, or the scope _ for selecting an existing fibre is large. Generally speaking however, it is preferable for the fibre to be located at or within approximately 3m of the fluid carrying conduit, and more preferably at or within approximately 1.5m from the centreline of the conduit to be monitored.
  • Fibre-optic distributed acoustic sensing is provided by interrogating the fibre with optical pulses at different frequencies in many embodiments.
  • the single length of fibre is typically single mode fibre, and is preferably free of any mirrors, reflectors, gratings, or change of optical properties along its length. This provides the advantage that an unmodified, substantially continuous length of standard fibre can be used, requiring little or no modification or preparation for use.
  • Such embodiments typically operate by detecting Rayleigh backscatted light from the sensing fibre and using the frequency relationship of the interrogating pulses to determine the acoustic signals incident on the fibre along its length. Any suitable distributed sensing technique may be employed however.
  • a suitable DAS system is described in GB 2442745 for example.
  • the length and arrangement of fibre sections corresponding to each channel is determined by the interrogation of the fibre. These can be selected according to the physical arrangement of the fibre, and also according to the type of monitoring required. In this way, the distance along the fibre, and the length of each fibre section, or channel resolution, can easily be varied with adjustments to the interrogator changing the input pulse width and input pulse duty cycle, without any changes to the fibre. Data from multiple channels can be provided substantially simultaneously in embodiments.
  • the spatial resolution of the distributed fibre optic sensing is less than or equal to 30m in many embodiments, and less than or equal to 20m or 10m in certain embodiments.
  • the optic fibre is interrogated to provide sensed data over a distance greater than or equal to 20km, and distances of greater than or equal to 30km or 40km are achievable in other embodiments.
  • a further aspect of the invention provides pipeline monitoring apparatus comprising an optic fibre interrogator adapted to interrogate an optic fibre and provide distributed fibre sensing; an impulser adapted to produce pressure pulses in a fluid contained in a pipeline; and a processor adapted to receive sensed data from said interrogator in response to said pressure pulses and to derive a conduit condition profile from said sensed data.
  • the invention also provides a computer program and a computer program product for carrying out any of the methods described herein and/or for embodying any of the apparatus features described herein, and a computer readable medium having stored thereon a program for carrying out any of the methods described herein and/or for embodying any of the apparatus features described herein
  • Figure 1 illustrates the basic component of a distributed fibre optic sensor
  • Figure 2 shows a fibre sensor arranged along a length of pipeline
  • Figure 3 is a cross section of a pipeline and sensing fibres
  • Figures 4 and 5 show pipeline monitoring data outputs.
  • Figure 1 shows a schematic of a distributed fibre optic sensing arrangement.
  • a length of sensing fibre 104 is connected at one end to an interrogator 106.
  • the output from interrogator 106 is passed to a signal processor 108 and optionally a user interface, which in practice may be realised by an appropriately specified PC.
  • the sensing fibre can be many kilometres in length, and in this example is approximately 40km long.
  • the interrogator launches an interrogating optical signal, which may for example comprise a series of pulses having a selected frequency pattern, into the sensing fibre.
  • the phenomenon of Rayleigh backscattering results in some fraction of the light input into the fibre being reflected back to the interrogator, where it is detected to provide an output signal which is representative of acoustic disturbances in the vicinity of the fibre.
  • the form of the optical input and the method of detection allow a single continuous fibre to be spatially resolved into discrete sensing lengths. That is, the acoustic signal sensed at one sensing length can be provided substantially independently of the sensed signal at an adjacent length.
  • the spatial resolution in the present example is approximately 10m, resulting in the output of the interrogator taking the form of 4000 independent data channels.
  • the single sensing fibre can provide sensed data which is analogous to a multiplexed array of adjacent sensors, arranged in a linear path.
  • Figure 2 shows an arrangement employing a method according to the present invention, whereby a sensing fibre 202 (and associated interrogator and/or processor 204) is arranged along the path of a pipeline 206.
  • An impulser 208 is arranged at a point along the pipeline, and adapted to introduce a pressure pulse into the fluid in the pipe.
  • Impulser 208 can take a variety of forms, but in this example comprises a hydraulic ram.
  • the pressure pulse generated travels in both directions down the pipe, away from the impulser.
  • the pipe acts as a waveguide and it has been found that the pulse can travel for tens of kilometres without being unduly attenuated.
  • Figure 3 shows a cross section of a pipe 302 with possible locations of a sensing fibre able to detect the response of the pulse in the pipe.
  • the pipe in the present example has an internal diameter of 1200mm and 50mm carbon steel walls, carrying natural gas at approximately 80bar.
  • the pipe may be buried approximately 1-2m below the surface which may be ground level or the seabed in certain situations.
  • Fibre 304 is located inside the interior bore of the pipe 302, resting on the bottom of the pipe.
  • Fibre 306 is bonded to the exterior of the pipe, while fibre 308 is located in a separate cable carrying conduit 310, located approximately 1.5m from the centreline of the gas transmission pipeline.
  • Conduit 310 is typically laid at the time of installing the pipeline to carry communication and/or SCADA lines.
  • Fibre 312 is directly buried in the ground alongside the pipeline, at approximately 1m from the pipe centreline.
  • the measured response to the pressure pulse in the pipe will be different, and will depend on different factors.
  • the signal sensed by fibre 308 will depend on the transfer characteristics of the ground between pipe 302 and conduit 310, for example, while sensing fibres 304 and 306 will be less affected. As will be explained below however, this does not adversely affect the present invention, and any fibre placement which produces a reliable response to the pressure pulse can be used.
  • Figure 4 shows a histogram and associated waterfall plot illustrating a distributed fibre sensor output in response to a series of pressure pulses introduced into an adjacent pipeline.
  • Data in Figure 4 was produced by a sensing fibre in a conduit.
  • the x-axis of the histogram and waterfall is the length of the sensing fibre which is this case is approximately 40km.
  • the histogram shows, at an instant in time the amplitude of the sensed acoustic signal returned from the sensing fibre. In order that all 4000 channels can be viewed, each bar in the diagram represents the peak amplitude from a group of 10m sections. Individual 10m could be viewed if desired.
  • the lower plot is a waterfall with an update rate of 0.05 seconds showing sound intensity against distance and time, time plotted along the y-axis of the waterfall, most recent data plotted at the top.
  • the first is an area of constant activity towards the left of the plot at 402, corresponding to a length of approximately 4000m of the sensing fibre. This is attributable to an industrial unit located over that section of fibre, producing a steady vibrational noise. Secondly distinct chevron patterns can be seen, most clearly in region 404, away from the constant noise of the industrial unit.
  • each chevron is located at point 406 along the fibre, corresponding to the location of an impulser.
  • the 1 V shape of the plot corresponds to the pressure pulse moving along the pipe in both directions away from the source of the pulse, and the slope of the 'V shape corresponds to the speed of sound in the pressurised gas contained within the pipe which in this case is approximately 400ms '1 . It can be seen that a series of pressure pulses are introduced into the gas, and multiple traces are formed. On the top histogram plot, the individual pulses appear in their respective positions at that instant, spaced along the fibre.
  • Figure 5 shows data in a similar form to that of Figure 4, but with the axes of both the histogram and the lower waterfall plot similarly rescaled.
  • the x-axis of the waterfall plot corresponds to a section of the sensing cable approximately 4km long (as opposed to 40km in Figure 4) and the update rate of Figure 5 is set to 2 seconds (as opposed to 0.05 sec in Figure 4).
  • Data for Figure 5 comes from the same pipe and fibre arrangement as in Figure 4, but taken during a pigging run, and the path of the pig is clearly visible as a diagonal trace 502 in the waterfall plot. Also visible in the waterfall plot of Figure 5 are a series of vertical lines having various intensities. The lines correspond to various locations along the length of the pipe, and can be considered as a fingerprint or barcode of the pipe, the pattern of lines corresponding to the physical characteristics or condition of the pipe, and to a certain extent its immediately surrounding environment (in this case the ground in which it is buried.
  • a pipe profile or barcode as explained above, additionally decomposed by frequency provides more detail to a user and allows more sophisticated analysis. For example different types of physical phenomena may be associated with particular frequency bands. For instance, changes in the higher frequency bands may be indicative of turbulent flow in the pipe caused by the build-up of wax deposits whereas changes in the lower frequency band may be indicative of changes to the ground condition in which the pipe is laid. The interpreted results may therefore provide a greater quantity and quality of information to a user.

Abstract

A method for monitoring a fluid carrying conduit by introducing an acoustic pulse into the conduit, and interrogating an optic fibre positioned along the path of said conduit to provide distributed acoustic sensing. By measuring the response at each of a plurality of locations, a conduit condition profile can be derived. A condition profile can be obtained quickly and easily with minimum disruption to the pipeline infrastructure and contained flow. Existing optic fibres running along the path of a pipe can be employed for sensing purposes, allowing relatively long spans of pipeline to be monitored with only limited access to the pipe.

Description

CONDUIT MONITORING
The present invention relates to conduit monitoring and inspection, and more particularly to subterranean pipeline monitoring.
Pipelines are the most economically viable method of transporting fluid assets, most commonly oil and gas, but other types of pipeline also exist. A vast pipeline infrastructure exists today responsible for gathering, transporting and distributing these natural resources, with over three quarters of a million kilometers of oil and gas pipelines in the US alone. The continuing proper operation of these pipelines is of paramount importance, and failures carry massive economic loss, environmental impact and potentially catastrophic physical damage also.
Significant efforts are therefore made to monitor and inspect pipelines. The sheer size of many pipeline networks however, and the fact that many kilometres of pipelines consist of underground or sub-sea installations makes effective and efficient monitoring a difficult problem.
The most common pipeline inspection technique is the use of smart pigs. Pigs travel down a pipeline, driven by the pressure of the product being transported, and perform tasks such as cleaning, profiling or inspecting pipeline walls. Alternative monitoring techniques include simply walking the pipeline and satellite inspection, where pipes are accessible. Computational pipeline monitoring (CPM) systems are also used whereby field gathered information such as pressure, temperature and flow rate are used to estimate the hydraulic behaviour of the product being transported.
It is an object of the present invention to provide improved conduit monitoring.
In a first aspect the present invention provides a method for monitoring a fluid carrying conduit comprising interrogating an optic fibre positioned along the path of said conduit to provide distributed acoustic sensing; introducing an acoustic pulse into the conduit; measuring by distributed acoustic sensing the response to said acoustic pulse at each of a plurality of discrete longitudinal sensing portions; and deriving from said plurality of measurements a conduit condition profile.
In this way a condition profile can be obtained quickly and easily with minimum disruption to the pipeline infrastructure and contained flow. Existing optic fibres running along the path of a pipe can be employed for sensing purposes, by connecting suitable interrogation and processing apparatus. A significant proportion of pipelines will have pre-existing lengths of optic fibre running along the path of the pipeline. These are typically communications cables and/or for SCADA (Supervisory Control and Data Acquisition) of the pipeline which were laid at the same time as the pipeline for obvious logistical reasons. In such cases, because existing cables can be made to form part of the monitoring apparatus, relatively long spans of pipeline can be monitored with only limited access to the pipe required.
In certain embodiments the acoustic pulse is introduced into the fluid contained in the pipe by a dedicated impulser or acoustic transducer. This might typically take the form of a hydraulic ram, but other apparatus could be used to induce a pressure wave in the fluid carried by the conduit being monitored. The impulser can be permanently installed in the pipeline, or can be applied at an existing valve station or junction. It has been found that such pressure pulses are capable of travelling large distances through pipelines with little attenuation, and therefore a single pulse source can provide sufficient input for monitoring 20, 30 or 40km or more of pipeline. Pulses can be introduced into the fluid during normal operation, while normal flow conditions continue in the conduit, resulting in little or no downtime for monitoring operations. Pulses are introduced at intervals of 10 seconds in one embodiment, and intervals of between 5 and 20 seconds might be employed. A typical monitoring period might be 10 minutes, but other periods are possible, and continuous monitoring may be employed.
As an alternative to a dedicated impulser it has been found that a pig travelling through a pipeline may be arranged to produce a series of pressure impulses. As the pig passes each girth weld in the pipe it encounters additional resistance and a slight overpressure builds behind the pig. As the pig subsequently passes the weld the pressure wave is released travelling in both directions down the pipe. The frequency of the pulses depends on the spacing of the welds and the velocity of the pig. In such cases it will be understood that the position of the source of the pulses gradually moves along the pipe, however this does not affect the monitoring method adversely. It is additionally noted that the pig may generate a higher acoustic signal as further constrictions or non-uniformities develop in the pipe over time, for example hydrocarbon build up or mechanical deformation. These can be identified in embodiments by looking for localised increases in generated acoustic signal over repeated pig passes. A further possible source of an acoustic or pressure pulse in a conduit is a sudden crack or leak. The resulting pressure pulse can be detected and used to identify and/or locate the source and hence the location of the crack or leak. A further aspect of the invention therefore provides a method for monitoring a fluid carrying conduit comprising interrogating an optic fibre positioned along the path of said conduit to provide distributed acoustic sensing; detecting an acoustic pulse at each of a plurality of discrete longitudinal sensing portions; and determining the source of said detected pulse.
The condition profile of the pipe need not be explicitly analysed to determine corresponding physical characteristics (although this is possible). More use may be derived by monitoring a pipeline over a period of time to obtain one or more profiles, and comparing these profiles to determine changes in characteristics. Thus two pipeline profiles may be obtained corresponding to two dates having a known time separation. Differences in the profile can be determined using data analysis techniques to obtain information concerning which portions of the pipe have undergone physical changes, and hence the location of those changes. More complex statistical analysis of profiles can be undertaken if a set of multiple profiles is built up over time, and profiles will typically be obtained at regular intervals for this purpose. Additionally or alternatively profiles can be taken before or after planned maintenance or repair work to characterise known changes to the pipeline.
Changes in the pipe, (and possibly ground conditions surrounding the pipe) can therefore be monitored over time intervals, and the location and characterising information concerning those changes can be provided. This information may prompt further actions, such as maintenance, cleaning, physical inspection or repair.
In some embodiments the amplitude response to the acoustic pulse is measured. This may be performed by integrating across the available bandwidth for each channel. Further analysis of the data returned from distributed sensing however allows the spectral content of each channel to be provided in certain embodiments, enabling enhanced condition monitoring capability. Distributed acoustic sensing in embodiments of the present invention senses seismic signals (both P pressure and S shear vibration waves) which are within a bandwidth from OHz - 5kHz. Higher frequencies are commonly strongly attenuated however, and the range from OHz to 1kHz is more commonly monitored. The sensing fibre for distributed sensing may be located inside the conduit, on the exterior surface of the conduit, directly buried adjacent to the conduit or in a separate adjacent conduit, in various different embodiments. There is no prescribed position for the sensing fibre, provided its location is such that it is able to detect a sufficient response to the acoustic pulse. Because of the high sensitivities possible in fibre optic sensing, whereby induced phase differences can be measured using interferometric techniques, the potential scope for positioning the fibre, or the scope _ for selecting an existing fibre is large. Generally speaking however, it is preferable for the fibre to be located at or within approximately 3m of the fluid carrying conduit, and more preferably at or within approximately 1.5m from the centreline of the conduit to be monitored.
Fibre-optic distributed acoustic sensing is provided by interrogating the fibre with optical pulses at different frequencies in many embodiments. The single length of fibre is typically single mode fibre, and is preferably free of any mirrors, reflectors, gratings, or change of optical properties along its length. This provides the advantage that an unmodified, substantially continuous length of standard fibre can be used, requiring little or no modification or preparation for use. Such embodiments typically operate by detecting Rayleigh backscatted light from the sensing fibre and using the frequency relationship of the interrogating pulses to determine the acoustic signals incident on the fibre along its length. Any suitable distributed sensing technique may be employed however. A suitable DAS system is described in GB 2442745 for example.
Since the fibre has no discontinuities, the length and arrangement of fibre sections corresponding to each channel is determined by the interrogation of the fibre. These can be selected according to the physical arrangement of the fibre, and also according to the type of monitoring required. In this way, the distance along the fibre, and the length of each fibre section, or channel resolution, can easily be varied with adjustments to the interrogator changing the input pulse width and input pulse duty cycle, without any changes to the fibre. Data from multiple channels can be provided substantially simultaneously in embodiments.
The spatial resolution of the distributed fibre optic sensing is less than or equal to 30m in many embodiments, and less than or equal to 20m or 10m in certain embodiments. In certain embodiments the optic fibre is interrogated to provide sensed data over a distance greater than or equal to 20km, and distances of greater than or equal to 30km or 40km are achievable in other embodiments.
A further aspect of the invention provides pipeline monitoring apparatus comprising an optic fibre interrogator adapted to interrogate an optic fibre and provide distributed fibre sensing; an impulser adapted to produce pressure pulses in a fluid contained in a pipeline; and a processor adapted to receive sensed data from said interrogator in response to said pressure pulses and to derive a conduit condition profile from said sensed data.
The invention also provides a computer program and a computer program product for carrying out any of the methods described herein and/or for embodying any of the apparatus features described herein, and a computer readable medium having stored thereon a program for carrying out any of the methods described herein and/or for embodying any of the apparatus features described herein
The invention extends to methods, apparatus and/or use substantially as herein described with reference to the accompanying drawings.
Any feature in one aspect of the invention may be applied to other aspects of the invention, in any appropriate combination. In particular, method aspects may be applied to apparatus aspects, and vice versa.
Furthermore, features implemented in hardware may generally be implemented in software, and vice versa. Any reference to software and hardware features herein should be construed accordingly.
Preferred features of the present invention will now be described, purely by way of example, with reference to the accompanying drawings, in which:
Figure 1 illustrates the basic component of a distributed fibre optic sensor Figure 2 shows a fibre sensor arranged along a length of pipeline Figure 3 is a cross section of a pipeline and sensing fibres Figures 4 and 5 show pipeline monitoring data outputs.
Figure 1 shows a schematic of a distributed fibre optic sensing arrangement. A length of sensing fibre 104 is connected at one end to an interrogator 106. The output from interrogator 106 is passed to a signal processor 108 and optionally a user interface, which in practice may be realised by an appropriately specified PC. The sensing fibre can be many kilometres in length, and in this example is approximately 40km long.
The interrogator launches an interrogating optical signal, which may for example comprise a series of pulses having a selected frequency pattern, into the sensing fibre. The phenomenon of Rayleigh backscattering results in some fraction of the light input into the fibre being reflected back to the interrogator, where it is detected to provide an output signal which is representative of acoustic disturbances in the vicinity of the fibre. The form of the optical input and the method of detection allow a single continuous fibre to be spatially resolved into discrete sensing lengths. That is, the acoustic signal sensed at one sensing length can be provided substantially independently of the sensed signal at an adjacent length. The spatial resolution in the present example is approximately 10m, resulting in the output of the interrogator taking the form of 4000 independent data channels.
In this way, the single sensing fibre can provide sensed data which is analogous to a multiplexed array of adjacent sensors, arranged in a linear path.
Figure 2 shows an arrangement employing a method according to the present invention, whereby a sensing fibre 202 (and associated interrogator and/or processor 204) is arranged along the path of a pipeline 206. An impulser 208 is arranged at a point along the pipeline, and adapted to introduce a pressure pulse into the fluid in the pipe. Impulser 208 can take a variety of forms, but in this example comprises a hydraulic ram. The pressure pulse generated travels in both directions down the pipe, away from the impulser. The pipe acts as a waveguide and it has been found that the pulse can travel for tens of kilometres without being unduly attenuated.
As the pulse passes through any particular length of pipe, it creates an acoustic disturbance which can be detected by the distributed fibre sensor 202. Figure 3 shows a cross section of a pipe 302 with possible locations of a sensing fibre able to detect the response of the pulse in the pipe.
The pipe in the present example has an internal diameter of 1200mm and 50mm carbon steel walls, carrying natural gas at approximately 80bar. The pipe may be buried approximately 1-2m below the surface which may be ground level or the seabed in certain situations. Fibre 304 is located inside the interior bore of the pipe 302, resting on the bottom of the pipe. Fibre 306 is bonded to the exterior of the pipe, while fibre 308 is located in a separate cable carrying conduit 310, located approximately 1.5m from the centreline of the gas transmission pipeline. Conduit 310 is typically laid at the time of installing the pipeline to carry communication and/or SCADA lines. Fibre 312 is directly buried in the ground alongside the pipeline, at approximately 1m from the pipe centreline.
It will be understood that for each different fibre placement, the measured response to the pressure pulse in the pipe will be different, and will depend on different factors. The signal sensed by fibre 308 will depend on the transfer characteristics of the ground between pipe 302 and conduit 310, for example, while sensing fibres 304 and 306 will be less affected. As will be explained below however, this does not adversely affect the present invention, and any fibre placement which produces a reliable response to the pressure pulse can be used.
Figure 4 shows a histogram and associated waterfall plot illustrating a distributed fibre sensor output in response to a series of pressure pulses introduced into an adjacent pipeline. Data in Figure 4 was produced by a sensing fibre in a conduit. The x-axis of the histogram and waterfall is the length of the sensing fibre which is this case is approximately 40km. The histogram shows, at an instant in time the amplitude of the sensed acoustic signal returned from the sensing fibre. In order that all 4000 channels can be viewed, each bar in the diagram represents the peak amplitude from a group of 10m sections. Individual 10m could be viewed if desired. The lower plot is a waterfall with an update rate of 0.05 seconds showing sound intensity against distance and time, time plotted along the y-axis of the waterfall, most recent data plotted at the top.
Two main features can be seen from the waterfall plot. The first is an area of constant activity towards the left of the plot at 402, corresponding to a length of approximately 4000m of the sensing fibre. This is attributable to an industrial unit located over that section of fibre, producing a steady vibrational noise. Secondly distinct chevron patterns can be seen, most clearly in region 404, away from the constant noise of the industrial unit.
The vertex of each chevron is located at point 406 along the fibre, corresponding to the location of an impulser. The 1V shape of the plot corresponds to the pressure pulse moving along the pipe in both directions away from the source of the pulse, and the slope of the 'V shape corresponds to the speed of sound in the pressurised gas contained within the pipe which in this case is approximately 400ms'1. It can be seen that a series of pressure pulses are introduced into the gas, and multiple traces are formed. On the top histogram plot, the individual pulses appear in their respective positions at that instant, spaced along the fibre.
Figure 5 shows data in a similar form to that of Figure 4, but with the axes of both the histogram and the lower waterfall plot similarly rescaled. In Figure 5, the x-axis of the waterfall plot corresponds to a section of the sensing cable approximately 4km long (as opposed to 40km in Figure 4) and the update rate of Figure 5 is set to 2 seconds (as opposed to 0.05 sec in Figure 4).
Data for Figure 5 comes from the same pipe and fibre arrangement as in Figure 4, but taken during a pigging run, and the path of the pig is clearly visible as a diagonal trace 502 in the waterfall plot. Also visible in the waterfall plot of Figure 5 are a series of vertical lines having various intensities. The lines correspond to various locations along the length of the pipe, and can be considered as a fingerprint or barcode of the pipe, the pattern of lines corresponding to the physical characteristics or condition of the pipe, and to a certain extent its immediately surrounding environment (in this case the ground in which it is buried.
Considering the condition profile provided by this barcode effect, it will be understood that this corresponds to the chevron effect of Figure 4, but viewed with a compressed time axis. The pressure pulses passing through the pipe can be thought of as acoustically 'illuminating' each portion of the pipe they pass through, eliciting a response from the pipe and its environment, whereby the response is detected by the distributed sensing fibre. By averaging over time, it can be seen that some sections of the pipe have a different response to the pulses than others. Possible causes of these differences include a local hydrocarbon build up on the pipe wall, a weakness in the pipe wall or variation in the wall profile, or variation in the ground composition in the vicinity of the pipe for example. In this way the plot provides a condition profile of the pipe at a given time or date.
It is noted that while the pressure pulses seen in Figure 4 are produced by a dedicated impulser, the pulses in Figure 5, which give rise to the condition profile of the pipe are created as the pig passes each girth weld in the pipe, as explained above. Although not illustrated the spectral content of the sensed data can be extracted and provided. This would add an extra dimension to the plots of Figures 4 and 5, and would enable enhanced condition monitoring capability. Seismic signals are typically dominant at frequencies below 500Hz due to the high attenuation of higher frequencies through the ground.
For example, by looking at a selected frequency band or bands, the 'noise' from the industrial plant in region 402 of Figure 4 could be filtered out. A pipe profile or barcode as explained above, additionally decomposed by frequency provides more detail to a user and allows more sophisticated analysis. For example different types of physical phenomena may be associated with particular frequency bands. For instance, changes in the higher frequency bands may be indicative of turbulent flow in the pipe caused by the build-up of wax deposits whereas changes in the lower frequency band may be indicative of changes to the ground condition in which the pipe is laid. The interpreted results may therefore provide a greater quantity and quality of information to a user.
It will be understood that the present invention has been described above purely by way of example, and modification of detail can be made within the scope of the invention.
Each feature disclosed in the description, and (where appropriate) the claims and drawings may be provided independently or in any appropriate combination.

Claims

1. A method for monitoring a fluid carrying conduit comprising:
interrogating an optic fibre positioned along the path of said conduit to provide distributed acoustic sensing;
introducing an acoustic pulse into the conduit;
measuring by distributed acoustic sensing the response to said acoustic pulse at each of a plurality of discrete longitudinal sensing portions; and
deriving from said plurality of measurements a conduit condition profile.
2. A method according to Claim 1, comprising deriving one or more further conduit profiles and comparing said profiles to determine a change in conduit characteristics.
3. A method according to Claim 2, comprising determining the longitudinal location of a change in conduit characteristics.
4. A method according to any preceding claim, wherein the amplitude of response to said acoustic pulse is measured.
5. A method according to any preceding claim, wherein the spectral content of the response to said acoustic pulse is measured.
6. A method according to any preceding claim, wherein the distributed acoustic fibre is located inside said conduit.
7. A method according to any preceding claim, wherein the distributed acoustic fibre is located adjacent to said conduit.
8. A method according to any preceding claim, wherein the spatial resolution of said distributed fibre optic sensor is less than or equal to 25m.
9. A method according to any preceding claim, wherein the length of said distributed fibre optic sensor is greater than or equal to 20km.
10. A method according to any preceding claim, wherein said pulse is introduced by a dedicated impulser.
11. A method according to any one of Claims 1-9, wherein said pulse is introduced by the passage of a pig through said pipeline.
12. Pipeline monitoring apparatus comprising:
an optic fibre interrogator adapted to interrogate an optic fibre and provide distributed acoustic sensing;
an impulser adapted to produce pressure pulses in a fluid contained in a pipeline; and
a processor adapted to receive sensed data from said interrogator in response to said pressure pulses and to derive a conduit condition profile from said sensed data.
PCT/GB2009/002058 2008-08-21 2009-08-20 Conduit monitoring WO2010020796A1 (en)

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EP09784994.7A EP2326932B1 (en) 2008-08-21 2009-08-20 Conduit monitoring
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Cited By (16)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2012175954A1 (en) 2011-06-20 2012-12-27 Optasense Holdings Limited Monitoring of conduits
US8505625B2 (en) 2010-06-16 2013-08-13 Halliburton Energy Services, Inc. Controlling well operations based on monitored parameters of cement health
US8584519B2 (en) 2010-07-19 2013-11-19 Halliburton Energy Services, Inc. Communication through an enclosure of a line
CN103492849A (en) * 2011-03-01 2014-01-01 光学感应器控股有限公司 Conduit monitoring
US8930143B2 (en) 2010-07-14 2015-01-06 Halliburton Energy Services, Inc. Resolution enhancement for subterranean well distributed optical measurements
US9170149B2 (en) 2010-09-01 2015-10-27 Schlumberger Technology Corporation Distributed fiber optic sensor system with improved linearity
WO2016010553A1 (en) * 2014-07-18 2016-01-21 Halliburton Energy Services, Inc. Determining locations of acoustic sources around a borehole
US9388686B2 (en) 2010-01-13 2016-07-12 Halliburton Energy Services, Inc. Maximizing hydrocarbon production while controlling phase behavior or precipitation of reservoir impairing liquids or solids
US9599272B2 (en) 2008-07-23 2017-03-21 Schlumberger Technology Corporation Monitoring of the position of a pipe inspection tool in a pipeline
US9739645B2 (en) 2009-11-13 2017-08-22 Optasense Holdings Limited Fibre optic distributed sensing
US9823373B2 (en) 2012-11-08 2017-11-21 Halliburton Energy Services, Inc. Acoustic telemetry with distributed acoustic sensing system
RU2642135C2 (en) * 2012-02-01 2018-01-24 Оптасенс Холдингз Лимитед Location indication
US10359302B2 (en) 2015-12-18 2019-07-23 Schlumberger Technology Corporation Non-linear interactions with backscattered light
CN110375840A (en) * 2019-06-25 2019-10-25 武汉理工光科股份有限公司 Pig tracing localization method based on distributing optical fiber sensing
US11543286B2 (en) * 2020-04-14 2023-01-03 Nec Corporation Distributed acoustic sensing based acoustic wave speed scanning and mapping of civil infrastructures
US11619542B2 (en) * 2020-04-14 2023-04-04 Nec Corporation Distributed acoustic sensing based natural frequency measurement of civil infrastructures

Families Citing this family (78)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US20110290477A1 (en) 2008-12-31 2011-12-01 Jaeaeskelaeinen Kari-Mikko Method for monitoring deformation of well equipment
AU2009339275B2 (en) 2009-02-09 2013-06-27 Shell Internationale Research Maatschappij B.V. Areal monitoring using distributed acoustic sensing
WO2010091404A1 (en) 2009-02-09 2010-08-12 Shell Oil Company Method of detecting fluid in-flows downhole
US20100200743A1 (en) * 2009-02-09 2010-08-12 Larry Dale Forster Well collision avoidance using distributed acoustic sensing
EP4174448A3 (en) 2009-05-27 2023-07-26 Silixa Ltd. Method and apparatus for optical sensing
CN104314552B (en) 2009-05-27 2017-09-26 光学感应器控股有限公司 Fracturing monitoring
GB2476449B (en) 2009-09-18 2013-12-11 Optasense Holdings Ltd Wide area seismic detection
US8425683B2 (en) * 2009-11-17 2013-04-23 Acoustic Systems, Inc. Method for tracking a scraper within a pipeline
US9109944B2 (en) 2009-12-23 2015-08-18 Shell Oil Company Method and system for enhancing the spatial resolution of a fiber optical distributed acoustic sensing assembly
WO2011079107A2 (en) 2009-12-23 2011-06-30 Shell Oil Company Detecting broadside and directional acoustic signals with a fiber optical distributed acoustic sensing (das) assembly
GB201008823D0 (en) 2010-05-26 2010-07-14 Fotech Solutions Ltd Fluid flow monitor
US8605542B2 (en) 2010-05-26 2013-12-10 Schlumberger Technology Corporation Detection of seismic signals using fiber optic distributed sensors
US9140815B2 (en) 2010-06-25 2015-09-22 Shell Oil Company Signal stacking in fiber optic distributed acoustic sensing
US20120020184A1 (en) * 2010-07-26 2012-01-26 Colin Wilson Using a distributed optical acoustic sensor to position an object
GB201013712D0 (en) * 2010-08-16 2010-09-29 Qinetiq Ltd Gunfire detection
GB201013704D0 (en) 2010-08-16 2010-09-29 Qinetiq Ltd Border monitoring
EP2656112A2 (en) 2010-12-21 2013-10-30 Shell Internationale Research Maatschappij B.V. Detecting the direction of acoustic signals with a fiber optical distributed acoustic sensing (das) assembly
CA2821583C (en) 2010-12-21 2019-09-24 Shell Internationale Research Maatschappij B.V. System and method for making distributed measurements using fiber optic cable
AU2012225422B2 (en) 2011-03-09 2015-07-02 Shell Internationale Research Maatschappij B.V. Integrated fiber optic monitoring system for a wellsite and method of using same
GB201109372D0 (en) 2011-06-06 2011-07-20 Silixa Ltd Method for locating an acoustic source
AU2012271016B2 (en) 2011-06-13 2014-12-04 Shell Internationale Research Maatschappij B.V. Hydraulic fracture monitoring using active seismic sources with receivers in the treatment well
US9091589B2 (en) 2011-06-20 2015-07-28 Shell Oil Company Fiber optic cable with increased directional sensitivity
GB201112154D0 (en) 2011-07-15 2011-08-31 Qinetiq Ltd Seismic geophysical surveying
GB201112161D0 (en) * 2011-07-15 2011-08-31 Qinetiq Ltd Portal monitoring
CA2844334C (en) 2011-08-09 2019-10-22 Shell Internationale Research Maatschappij B.V. Method and apparatus for measuring seismic parameters of a seismic vibrator
BR112014014565B1 (en) 2011-12-15 2022-06-28 Shell Internationale Research Maatschappij B.V. DISTRIBUTED FIBER OPTICS ACOUSTIC DETECTION SYSTEM
CN102588743B (en) * 2012-03-08 2013-08-07 东北大学 Device and method for real-time tracking and accurate positioning for internal detector in pipeline
GB2519009B (en) 2012-08-01 2017-09-13 Shell Int Research Cable comprising twisted sinusoid for use in distributed sensing
ITMI20122196A1 (en) 2012-12-20 2014-06-21 Eni Spa METHOD AND SYSTEM FOR REMOTE DETECTION OF THE POSITION OF A PIG DEVICE INSIDE A PRESSURE CONDUCT
US10048395B2 (en) * 2013-02-01 2018-08-14 Westerngeco L.L.C. Computing a gradient based on differences of plural pairs of particle motion sensors
US20140352442A1 (en) * 2013-06-03 2014-12-04 Macau University Of Science And Technology Vibration Detection System Based on Biconical Tapered Fiber and the Method thereof
GB2515564A (en) * 2013-06-28 2014-12-31 Optasense Holdings Ltd Improvements in fibre optic distributed sensing
US10408954B2 (en) 2014-01-17 2019-09-10 Westerngeco L.L.C. Seismic sensor coupling
US9535039B2 (en) 2014-04-30 2017-01-03 Control Devices, Inc. Acoustic transmitter and method for underwater pipeline inspection gauges
EA028210B1 (en) 2014-05-14 2017-10-31 Эни С.П.А. Method and system for the continuous remote monitoring of the position and advance speed of a pig device inside a pipeline
US10274381B2 (en) 2014-06-30 2019-04-30 Exxonmobil Upstream Research Company Pipeline constriction detection
ES2878002T3 (en) * 2015-07-17 2021-11-18 Univ Adelaide Method and system for the analysis of the state of pipes
US11530606B2 (en) 2016-04-07 2022-12-20 Bp Exploration Operating Company Limited Detecting downhole sand ingress locations
EP3670830B1 (en) 2016-04-07 2021-08-11 BP Exploration Operating Company Limited Detecting downhole events using acoustic frequency domain features
CN106051379B (en) * 2016-05-27 2018-01-16 沈阳鑫联石化设备有限公司 A kind of wiper remote monitoring instrument and monitoring method
US11015996B2 (en) * 2016-07-26 2021-05-25 Halliburton Energy Services, Inc. Electro acoustic technology (EAT) for real time intelligent pigging
WO2018022063A1 (en) 2016-07-28 2018-02-01 Halliburton Energy Services, Inc. Real-time plug tracking with fiber optics
US10317014B2 (en) * 2016-08-09 2019-06-11 Baker Hughes, A Ge Company, Llc Flow variation system
EP3583296B1 (en) 2017-03-31 2021-07-21 BP Exploration Operating Company Limited Well and overburden monitoring using distributed acoustic sensors
AU2018321150A1 (en) 2017-08-23 2020-03-12 Bp Exploration Operating Company Limited Detecting downhole sand ingress locations
WO2019056121A1 (en) * 2017-09-22 2019-03-28 University Of Saskatchewan Methods for detecting pipeline weakening
EP3695099A2 (en) 2017-10-11 2020-08-19 BP Exploration Operating Company Limited Detecting events using acoustic frequency domain features
WO2019126131A1 (en) 2017-12-20 2019-06-27 Kimberly-Clark Worldwide, Inc. System for intervening and improving the experience of the journey of an absorbent article change
WO2019126437A1 (en) 2017-12-20 2019-06-27 Kimberly-Clark Worldwide, Inc. System for documenting product usage by recognizing an acoustic signature of a product
CN108053477B (en) * 2017-12-20 2021-07-02 北京华航无线电测量研究所 Numerical processing method for deformation in pipeline
EP3514564B1 (en) * 2018-01-19 2023-05-31 Centre National D'etudes Spatiales Indoor positioning system
CN110107816A (en) * 2018-02-01 2019-08-09 北京声创新技术发展有限责任公司 Oil and gas pipeline pipe cleaner/detector infrasonic sound real-time tracking positioning system and method
US11181208B2 (en) 2018-05-24 2021-11-23 Tdw Delaware, Inc. Non-invasive pipeline pig signal using vibration sensors
US11132542B2 (en) * 2018-06-28 2021-09-28 Nec Corporation Time-space de-noising for distributed sensors
CN109298080B (en) * 2018-10-31 2023-12-15 江苏大学 Time-sharing excitation system and method of special array sensor for weld defect detection based on characteristic guided wave
RU2726440C2 (en) * 2018-11-26 2020-07-14 Публичное акционерное общество "Транснефть" (ПАО "Транснефть") Apparatus for determining location of cleaning device in pipeline
CN109306864A (en) * 2018-11-27 2019-02-05 美钻深海能源科技研发(上海)有限公司 Subsea pig operation real-time monitoring device based on fiber laser arrays
US20210389486A1 (en) 2018-11-29 2021-12-16 Bp Exploration Operating Company Limited DAS Data Processing to Identify Fluid Inflow Locations and Fluid Type
GB201820331D0 (en) 2018-12-13 2019-01-30 Bp Exploration Operating Co Ltd Distributed acoustic sensing autocalibration
CA3154435C (en) 2019-10-17 2023-03-28 Lytt Limited Inflow detection using dts features
EP4045766A1 (en) 2019-10-17 2022-08-24 Lytt Limited Fluid inflow characterization using hybrid das/dts measurements
CN110822292A (en) * 2019-10-29 2020-02-21 东莞新奥燃气有限公司 System and method for monitoring running position of gas pipeline through ball
WO2021093974A1 (en) 2019-11-15 2021-05-20 Lytt Limited Systems and methods for draw down improvements across wellbores
CN110987318B (en) * 2019-12-11 2021-11-05 北京华展汇元信息技术有限公司 Automatic detection device and detection method for gas leakage of high-pressure pipeline
GB2604489B (en) * 2019-12-13 2023-10-04 Halliburton Energy Services Inc Method and system to determine variations in a fluidic channel
US20230043381A1 (en) * 2020-01-24 2023-02-09 Lytt Limited Detecting flow obstruction events within a flow line using acoustic frequency domain features
CA3180595A1 (en) 2020-06-11 2021-12-16 Lytt Limited Systems and methods for subterranean fluid flow characterization
EP4168647A1 (en) 2020-06-18 2023-04-26 Lytt Limited Event model training using in situ data
CN111965693B (en) * 2020-08-21 2023-06-27 电子科技大学 Pipeline trend tracing method and system based on optical cable
EP3992600B1 (en) 2020-11-02 2023-02-15 Tata Consultancy Services Limited Method and system for inspecting and detecting fluid in a pipeline
CN112504969B (en) * 2021-02-03 2021-05-14 四川大学 Pipeline flange weld joint health detection device and method based on distributed acoustic sensing
RU2757682C1 (en) * 2021-03-25 2021-10-20 Федеральное государственное бюджетное образовательное учреждение высшего образования "Поволжский государственный университет телекоммуникаций и информатики" Method for monitoring the condition of a viewing device on the route of a fiber-optic cable line
RU2758340C1 (en) * 2021-04-13 2021-10-28 Федеральное государственное бюджетное образовательное учреждение высшего образования "Поволжский государственный университет телекоммуникаций и информатики" Method for non-destructive testing of optical fiber strength
CN113275341B (en) * 2021-05-19 2022-04-08 精仪监测科技(苏州)有限公司 Pipe cleaner tracking and positioning method based on distributed optical fiber vibration sensing
CN113447727B (en) * 2021-06-30 2022-12-09 武汉理工光科股份有限公司 Method and device for positioning lightning above oil and gas pipeline based on optical fiber vibration measurement system
CN113933002A (en) * 2021-08-12 2022-01-14 吉林大学 Method for identifying leakage point of long-distance large-scale water delivery pressure pipeline hydrostatic test
CN113883422B (en) * 2021-09-10 2023-06-02 江苏禹治流域管理技术研究院有限公司 Urban water supply network leakage on-line monitoring system
EP4202374A1 (en) 2021-12-22 2023-06-28 Universität Hamburg Device for fibre-optical measurement and transport of measurement signals

Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4747309A (en) 1980-10-02 1988-05-31 Imperial Chemical Industries Plc Structures and methods of testing them with linear microphones
US20060225507A1 (en) 2003-01-13 2006-10-12 Paulson Peter O Pipeline monitoring system
EP1912049A1 (en) * 2006-10-13 2008-04-16 AT&T Corp. Method and apparatus for acoustic sensing using multiple optical pulses

Family Cites Families (43)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US3949353A (en) * 1973-12-10 1976-04-06 Continental Oil Company Underground mine surveillance system
US4311391A (en) * 1979-12-27 1982-01-19 Westinghouse Electric Corp. Passive fiber optic sonar system
US4313185A (en) * 1979-12-31 1982-01-26 General Electric Company Acoustic vibration sensor and sensing system
US4363114A (en) * 1981-01-21 1982-12-07 The United States Of America As Represented By The Secretary Of The Navy Low noise remote optical fiber sound detector
US4927232A (en) * 1985-03-18 1990-05-22 G2 Systems Corporation Structural monitoring system using fiber optics
GB8307985D0 (en) * 1983-03-23 1983-04-27 British Gas Corp Pipeline pig tracking
US4541278A (en) * 1984-04-23 1985-09-17 Union Oil Company Of California Pipeline corrosion sensing device and method
EP0170736A1 (en) * 1984-07-09 1986-02-12 Amon, Glen C. Pipeline fault status monitoring system
US4918303A (en) * 1989-05-11 1990-04-17 Conoco Inc. Detecting disturbance with cross polarized fiber optic sensing
US5194847A (en) * 1991-07-29 1993-03-16 Texas A & M University System Apparatus and method for fiber optic intrusion sensing
JP2833932B2 (en) * 1992-06-18 1998-12-09 日本電気アイシーマイコンシステム株式会社 Non-linear emphasis circuit
US5417112A (en) * 1993-01-11 1995-05-23 Tdw Delaware, Inc. Apparatus for indicating the passage of a pig moving within an underground pipeline
GB9324333D0 (en) * 1993-11-26 1994-01-12 Sensor Dynamics Ltd Measurement of one or more physical parameters
CN2212773Y (en) * 1994-06-24 1995-11-15 刘达峰 Position finder for obstacle in pipeline
US5549000A (en) * 1994-06-27 1996-08-27 Texaco, Inc. Passive acoustic detection of pipeline pigs
JPH08233932A (en) 1995-02-28 1996-09-13 Tokyo Gas Co Ltd Running position monitoring means for pig
JPH08233564A (en) * 1995-02-28 1996-09-13 Tokyo Gas Co Ltd Traveling position detecting device for pig
GB9520387D0 (en) * 1995-10-06 1995-12-06 R S T Projects Ltd Debris monitoring system and apparatus
AU7275398A (en) * 1997-05-02 1998-11-27 Baker Hughes Incorporated Monitoring of downhole parameters and tools utilizing fiber optics
US6211964B1 (en) * 1997-10-09 2001-04-03 Geosensor Corporation Method and structure for incorporating fiber optic acoustic sensors in a seismic array
GB9802688D0 (en) 1998-02-06 1998-07-29 Marconi Gec Ltd Improvements in or relating to sound detection
JP2000088561A (en) * 1998-09-11 2000-03-31 Tokyo Gas Co Ltd Detecting method for running position of pig at inside of conduit
CA2412041A1 (en) * 2000-06-29 2002-07-25 Paulo S. Tubel Method and system for monitoring smart structures utilizing distributed optical sensors
US6993977B2 (en) * 2001-12-10 2006-02-07 Moe Momayez Remote structural material evaluation apparatus
US20040261547A1 (en) * 2002-10-01 2004-12-30 Russell David Alexander Method of deriving data
US20050034917A1 (en) * 2003-08-14 2005-02-17 Baker Hughes Incorporated Apparatus and method for acoustic position logging ahead-of-the-bit
GB0407982D0 (en) 2004-04-08 2004-05-12 Wood Group Logging Services In "Methods of monitoring downhole conditions"
US6847207B1 (en) * 2004-04-15 2005-01-25 Tdw Delaware, Inc. ID-OD discrimination sensor concept for a magnetic flux leakage inspection tool
RU2271446C1 (en) * 2004-07-27 2006-03-10 Общество с ограниченной ответственностью "ПетроЛайт" Vibroacoustic elongated object characteristics monitoring device
US7271884B2 (en) * 2004-08-06 2007-09-18 The United States Of America Represented By The Secretary Of The Navy Natural fiber span reflectometer providing a virtual phase signal sensing array capability
CN2758749Y (en) 2004-12-16 2006-02-15 何志强 Alarm with signal sampling for natural gas pipeline cleaner
KR20060084256A (en) 2005-01-19 2006-07-24 삼성전자주식회사 Lens compound of light emission diode device and led device, backlight unit and liquid crystal display comprising the same
US7397976B2 (en) * 2005-01-25 2008-07-08 Vetco Gray Controls Limited Fiber optic sensor and sensing system for hydrocarbon flow
RU2287131C1 (en) * 2005-09-06 2006-11-10 Общество с ограниченной ответственностью "ПетроЛайт" Method for monitoring status of extensive objects, primarily, product lines, and device for realization of said method
GB2442746B (en) * 2006-10-13 2011-04-06 At & T Corp Method and apparatus for acoustic sensing using multiple optical pulses
DE102007004104A1 (en) 2007-01-26 2008-07-31 Ksb Aktiengesellschaft Position detector for a part moved in a pipe
CN201034929Y (en) * 2007-04-04 2008-03-12 南京旭飞光电有限公司 Optical fiber gas sensors
RU68692U1 (en) * 2007-07-05 2007-11-27 Общество С Ограниченной Ответственностью "Проект-Ресурс" PIPELINE MONITORING SYSTEM
CN101135577A (en) * 2007-09-29 2008-03-05 中国科学院上海光学精密机械研究所 Automatic tuning control F-P fiber optic sensor
US7946341B2 (en) * 2007-11-02 2011-05-24 Schlumberger Technology Corporation Systems and methods for distributed interferometric acoustic monitoring
CN101226078A (en) * 2008-01-30 2008-07-23 广厦建设集团有限责任公司 Method for detecting long-distance linear organization abnormal vibration based on distributed optical fibre sensor
GB2462096A (en) * 2008-07-23 2010-01-27 Schlumberger Holdings Monitoring of a pipeline pig using external acoustic sensors
US8020616B2 (en) * 2008-08-15 2011-09-20 Schlumberger Technology Corporation Determining a status in a wellbore based on acoustic events detected by an optical fiber mechanism

Patent Citations (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4747309A (en) 1980-10-02 1988-05-31 Imperial Chemical Industries Plc Structures and methods of testing them with linear microphones
US20060225507A1 (en) 2003-01-13 2006-10-12 Paulson Peter O Pipeline monitoring system
EP1912049A1 (en) * 2006-10-13 2008-04-16 AT&T Corp. Method and apparatus for acoustic sensing using multiple optical pulses
GB2442745A (en) 2006-10-13 2008-04-16 At & T Corp Acoustic sensing using an optical fibre

Non-Patent Citations (1)

* Cited by examiner, † Cited by third party
Title
LI H-N ET AL: "Recent applications of fiber optic sensors to health monitoring in civil engineering", ENGINEERING STRUCTURES, BUTTERWORTH, GB, vol. 26, no. 11, 1 September 2004 (2004-09-01), pages 1647 - 1657, XP004567450, ISSN: 0141-0296 *

Cited By (23)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US9599272B2 (en) 2008-07-23 2017-03-21 Schlumberger Technology Corporation Monitoring of the position of a pipe inspection tool in a pipeline
US9739645B2 (en) 2009-11-13 2017-08-22 Optasense Holdings Limited Fibre optic distributed sensing
US9388686B2 (en) 2010-01-13 2016-07-12 Halliburton Energy Services, Inc. Maximizing hydrocarbon production while controlling phase behavior or precipitation of reservoir impairing liquids or solids
US8505625B2 (en) 2010-06-16 2013-08-13 Halliburton Energy Services, Inc. Controlling well operations based on monitored parameters of cement health
US8930143B2 (en) 2010-07-14 2015-01-06 Halliburton Energy Services, Inc. Resolution enhancement for subterranean well distributed optical measurements
US9003874B2 (en) 2010-07-19 2015-04-14 Halliburton Energy Services, Inc. Communication through an enclosure of a line
US8584519B2 (en) 2010-07-19 2013-11-19 Halliburton Energy Services, Inc. Communication through an enclosure of a line
US9170149B2 (en) 2010-09-01 2015-10-27 Schlumberger Technology Corporation Distributed fiber optic sensor system with improved linearity
US9594002B2 (en) 2011-03-01 2017-03-14 Optasense Holdings Limited Conduit monitoring
CN103492849A (en) * 2011-03-01 2014-01-01 光学感应器控股有限公司 Conduit monitoring
EA027707B1 (en) * 2011-06-20 2017-08-31 Оптасенс Холдингз Лимитед Method and apparatus for monitoring of a conduit
WO2012175954A1 (en) 2011-06-20 2012-12-27 Optasense Holdings Limited Monitoring of conduits
US9453821B2 (en) 2011-06-20 2016-09-27 Optasense Holdings Limited Monitoring of conduits
CN103733040A (en) * 2011-06-20 2014-04-16 光学感应器控股有限公司 Monitoring of conduits
GB2505849A (en) * 2011-06-20 2014-03-12 Optasense Holdings Ltd Monitoring of conduits
RU2642135C2 (en) * 2012-02-01 2018-01-24 Оптасенс Холдингз Лимитед Location indication
US9823373B2 (en) 2012-11-08 2017-11-21 Halliburton Energy Services, Inc. Acoustic telemetry with distributed acoustic sensing system
US9714566B2 (en) 2014-07-18 2017-07-25 Halliburton Energy Services, Inc. Determining locations of acoustic sources around a borehole
WO2016010553A1 (en) * 2014-07-18 2016-01-21 Halliburton Energy Services, Inc. Determining locations of acoustic sources around a borehole
US10359302B2 (en) 2015-12-18 2019-07-23 Schlumberger Technology Corporation Non-linear interactions with backscattered light
CN110375840A (en) * 2019-06-25 2019-10-25 武汉理工光科股份有限公司 Pig tracing localization method based on distributing optical fiber sensing
US11543286B2 (en) * 2020-04-14 2023-01-03 Nec Corporation Distributed acoustic sensing based acoustic wave speed scanning and mapping of civil infrastructures
US11619542B2 (en) * 2020-04-14 2023-04-04 Nec Corporation Distributed acoustic sensing based natural frequency measurement of civil infrastructures

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