WO2016044675A1 - Distributed seismic source array - Google Patents
Distributed seismic source array Download PDFInfo
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- WO2016044675A1 WO2016044675A1 PCT/US2015/050824 US2015050824W WO2016044675A1 WO 2016044675 A1 WO2016044675 A1 WO 2016044675A1 US 2015050824 W US2015050824 W US 2015050824W WO 2016044675 A1 WO2016044675 A1 WO 2016044675A1
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- wellbore
- original
- seismic sources
- seismic
- orbital
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Classifications
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- G—PHYSICS
- G01—MEASURING; TESTING
- G01V—GEOPHYSICS; GRAVITATIONAL MEASUREMENTS; DETECTING MASSES OR OBJECTS; TAGS
- G01V1/00—Seismology; Seismic or acoustic prospecting or detecting
- G01V1/40—Seismology; Seismic or acoustic prospecting or detecting specially adapted for well-logging
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01V—GEOPHYSICS; GRAVITATIONAL MEASUREMENTS; DETECTING MASSES OR OBJECTS; TAGS
- G01V1/00—Seismology; Seismic or acoustic prospecting or detecting
- G01V1/40—Seismology; Seismic or acoustic prospecting or detecting specially adapted for well-logging
- G01V1/52—Structural details
-
- B—PERFORMING OPERATIONS; TRANSPORTING
- B06—GENERATING OR TRANSMITTING MECHANICAL VIBRATIONS IN GENERAL
- B06B—METHODS OR APPARATUS FOR GENERATING OR TRANSMITTING MECHANICAL VIBRATIONS OF INFRASONIC, SONIC, OR ULTRASONIC FREQUENCY, e.g. FOR PERFORMING MECHANICAL WORK IN GENERAL
- B06B1/00—Methods or apparatus for generating mechanical vibrations of infrasonic, sonic, or ultrasonic frequency
- B06B1/10—Methods or apparatus for generating mechanical vibrations of infrasonic, sonic, or ultrasonic frequency making use of mechanical energy
- B06B1/16—Methods or apparatus for generating mechanical vibrations of infrasonic, sonic, or ultrasonic frequency making use of mechanical energy operating with systems involving rotary unbalanced masses
- B06B1/161—Adjustable systems, i.e. where amplitude or direction of frequency of vibration can be varied
- B06B1/162—Making use of masses with adjustable amount of eccentricity
- B06B1/164—Making use of masses with adjustable amount of eccentricity the amount of eccentricity being automatically variable as a function of the running condition, e.g. speed, direction
-
- B—PERFORMING OPERATIONS; TRANSPORTING
- B06—GENERATING OR TRANSMITTING MECHANICAL VIBRATIONS IN GENERAL
- B06B—METHODS OR APPARATUS FOR GENERATING OR TRANSMITTING MECHANICAL VIBRATIONS OF INFRASONIC, SONIC, OR ULTRASONIC FREQUENCY, e.g. FOR PERFORMING MECHANICAL WORK IN GENERAL
- B06B1/00—Methods or apparatus for generating mechanical vibrations of infrasonic, sonic, or ultrasonic frequency
- B06B1/10—Methods or apparatus for generating mechanical vibrations of infrasonic, sonic, or ultrasonic frequency making use of mechanical energy
- B06B1/16—Methods or apparatus for generating mechanical vibrations of infrasonic, sonic, or ultrasonic frequency making use of mechanical energy operating with systems involving rotary unbalanced masses
- B06B1/167—Orbital vibrators having masses being driven by planetary gearings, rotating cranks or the like
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01V—GEOPHYSICS; GRAVITATIONAL MEASUREMENTS; DETECTING MASSES OR OBJECTS; TAGS
- G01V1/00—Seismology; Seismic or acoustic prospecting or detecting
- G01V1/02—Generating seismic energy
- G01V1/143—Generating seismic energy using mechanical driving means, e.g. motor driven shaft
- G01V1/153—Generating seismic energy using mechanical driving means, e.g. motor driven shaft using rotary unbalanced masses
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- G—PHYSICS
- G01—MEASURING; TESTING
- G01V—GEOPHYSICS; GRAVITATIONAL MEASUREMENTS; DETECTING MASSES OR OBJECTS; TAGS
- G01V1/00—Seismology; Seismic or acoustic prospecting or detecting
- G01V1/40—Seismology; Seismic or acoustic prospecting or detecting specially adapted for well-logging
- G01V1/44—Seismology; Seismic or acoustic prospecting or detecting specially adapted for well-logging using generators and receivers in the same well
- G01V1/46—Data acquisition
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01V—GEOPHYSICS; GRAVITATIONAL MEASUREMENTS; DETECTING MASSES OR OBJECTS; TAGS
- G01V2210/00—Details of seismic processing or analysis
- G01V2210/10—Aspects of acoustic signal generation or detection
- G01V2210/12—Signal generation
- G01V2210/127—Cooperating multiple sources
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01V—GEOPHYSICS; GRAVITATIONAL MEASUREMENTS; DETECTING MASSES OR OBJECTS; TAGS
- G01V2210/00—Details of seismic processing or analysis
- G01V2210/10—Aspects of acoustic signal generation or detection
- G01V2210/12—Signal generation
- G01V2210/129—Source location
- G01V2210/1299—Subsurface, e.g. in borehole or below weathering layer or mud line
Definitions
- the invention relates generally to downhole seismic sources that are used in conjunction with acoustic receivers for determining the lithology and for acoustic imaging of the subsurface of the earth.
- Seismic sources are used to introduce controlled acoustic waves into the subsurface such that the direct and/or reflected waves can be detected by sensitive sensors at the surface or downhole.
- the detected energy is typically collected and processed and used to develop images of the subsurface.
- Geophysicists acknowledge that they experience as much as a 99 percent attenuation of the energy produced by surface sources (i.e., vibroseis trucks) as it passes through the unconsolidated near surface (top 100-200 feet) layers. "Bypassing the attenuation of the near-surface layer can reduce the power needed by two to three orders of magnitude, i.e., 30-300 kW for a surface source to -300 W for a downhole source.” (ref: P.C. Leary and LA. Walter - Geophysical Journal International, Aug 2005). In addition, the near surface layers absorb much of the higher frequency signals, limiting their useful frequencies to approximately 50 Hz and below.
- GPUSA's non-impulsive or distributed energy downhole seismic source can quadruple the spatial/temporal resolution, based upon a 4X increase (50 Hz to 200 Hz) in received frequency.
- Current downhole seismic sources are typically deployed via wireline into a wellbore as a single element, and are designed to be moved to multiple locations within the wellbore, as needed for a particular seismic survey. At each location, the source is typically clamped inside the wellbore prior to activation of the seismic source to achieve good coupling with the earth for best performance. Alternatively, the source can hang freely within the wellbore (i.e., fluid coupled) but transmission beyond the wellbore will be somewhat degraded. Each time a survey is performed, a wireline truck and crew is required at a significant expense. The major advantage of using downhole sources and sensors (as compared to surface seismic) is much higher resolution of the subsurface lithology.
- the present invention is generally directed to using multiple seismic sources held within a linear array and it is especially preferred that the seismic sources are orbital vibrators which have a primary acoustic radiation pattern which is orthogonal to a wellbore.
- the linear array may be cemented within the wellbore (and the cementing process can benefit from energizing the linear array during said process) or it may be secured within the wellbore by low friction rollers while a radial clamping force (such as a spring force) maintains the plurality of low friction rollers against sides of the wellbore.
- a radial clamping force such as a spring force
- the linear array of orbital vibrators (which can include two or more orbital vibrators co-located at each location in the linear array) can be held within drill pipe and tubing or interconnected strengthened cable and the linear array is connected inside a protected structure at or near the surface of the wellhead where a separable topside electronics unit provides power, control electronics, timing, as well as a means for synchronization with at least one other oilfield system used in conjunction with the linear array in a seismic survey.
- Topside electronics can include an AC generator which is used to provide a true, clean sinusoidal variable frequency signal to the linear array orbital vibrators.
- Fig. 1 illustrates a typical ORBITAL VIBRATOR DSS array in accordance with the present invention cemented inside a wellbore while Fig. 1 A is a blown-up illustration of one source within the ORBITAL VIBRATOR DSS of Fig. 1 .
- Fig. 2 illustrates an ORBITAL VIBRATOR DSS array employed inside a vertical wellbore.
- Figs. 3, 3A and 3B illustrate an ORBITAL VIBRATOR DSS array employed inside either a vertical wellbore (Fig. 3A) or a horizontal wellbore (Fig. 3B) and how it might be inserted through use of a coiled tubing rig (Fig. 3).
- Fig. 4 illustrates an alternative invention in which a single ORBITAL VIBRATOR DSS source (configured as shown in Fig. 13) is located at the bottom of one or more shallow wells to focus acoustic radiation downwardly into the earth from the bottom of the well(s).
- a single ORBITAL VIBRATOR DSS source (configured as shown in Fig. 13) is located at the bottom of one or more shallow wells to focus acoustic radiation downwardly into the earth from the bottom of the well(s).
- Fig. 5 illustrates an example tubing centralizers that incorporate rollers that an ORBITAL VIBRATOR DSS can be placed inside to allow it to move inside a wellbore with lo friction while also providing good acoustic coupling to the wellbore.
- Fig. 6 illustrates a typical system that might be used to drive a downhole orbital vibrator.
- Fig. 7 illustrates that the output of a variable frequency driver is not a true sine wave.
- Fig. 8 illustrates an alternative in which a generator used in
- Fig. 9 illustrates a preferred embodiment of the present invention useful in marine seismic applications.
- Fig. 10 illustrates an ORBITAL VIBRATOR DSS as rotating point source radiating energy omnidirectionally.
- Fig. 1 1 illustrates an ORBITAL VIBRATOR DSS placed inside a cylindrical vessel filled with an appropriate acoustic coupling to reduce cavitation while Fig. 12 illustrates a solid acoustic coupling material that serves the same function.
- Fig. 13 illustrates an ORBITAL VIBRATOR DSS system in accordance with the present invention modified by placing two single axis orbital vibrators on a rigid frame with each turning in the opposite direction while Fig. 14 shows a modified version in which the two single axis orbital vibrators can be mounted on an interior surface of an air-filled box such that vibration is imparted in one direction.
- Fig. 15 illustrates an ORBITAL VIBRATOR DSS deployed on a sea bottom.
- Fig. 1 6 is a chart which graphs force versus frequency for a typical orbital vibrator.
- Fig. 17 illustrates the eccentric mass of an orbital vibrator at rest according to the present invention while Fig. 18 illustrates a change of mass caused by rotation.
- ORBITAL VIBRATOR DSS Distributed Seismic Source
- the present invention uses linear arrays 1 of downhole vibratory seismic sources 1 A interconnected and deployed via drill pipe/tubing or high strength flexible cable.
- drill pipe/tubing the drill
- pipe/tubing encloses both the individual seismic sources and the
- drill pipe/tubing also provides the mechanical strength (in tension) holding the downhole system together such that the power/control cables see minimal tension during installation and operation.
- Using drill pipe/tubing has many advantages because it is standard equipment used every day in the oilfield; it is designed for the downhole environment, it is inexpensive, and it is readily available.
- ORBITAL VIBRATOR DSS can be permanently cemented in either a cased or uncased hole as shown in Fig. 1 A where downhole well 6 has been filled with cement 5.
- a surface vault 7 provides access to a connector at or near the top of the wellbore as well as protection when it is not in use.
- a separate power/control electronics chassis is connected to the ORBITAL VIBRATOR DSS system via the connector in the surface vault.
- the outside diameter of a cable section 3 of the drill pipe/tubing can vary from approximately 1 inch to approximately 2 inches.
- the outside diameter of an individual seismic source section 4 can vary from approximately 1 inch to approximately 5 inches.
- Seismic surveys are increasingly being used in the today's oilfield for monitoring/enhancing production vs. exploration. As such, there will be an increased demand for both permanent seismic sources and sensors. This will allow operators to perform seismic surveys on demand without the need to call in outside resources. And it will provide much more detailed
- an orbital vibrator is used as the downhole source 1 A.
- an orbital vibrator basically consists of a drive motor with
- the frequency can be designed to ramp up over time, ramp down over time, combined ramp up/down, or be held at a constant frequency (i.e., at frequency that provides the best performance for a given subsurface structure).
- ORBITAL VIBRATOR DSS Because the preferred embodiment calls for the ORBITAL VIBRATOR DSS to be permanently installed, it is envisioned that the ORBITAL VIBRATOR DSS will be installed in instrumentation, observation, or wells previously used for production that are no longer producing.
- the present invention includes, but is not limited to, the following combinations of equipment and/or methods:
- a multitude of seismic sources forming a linear array designed to be permanently deployed in a wellbore where the drill pipe/tubing is in separable sections with all wires/cables inside.
- a multitude of seismic sources forming a linear array designed to be permanently deployed in a wellbore where separable sections of drill pipe/tubing is used for deep wells to connect the top of the seismic source array to the surface connection.
- a multitude of seismic sources forming a linear array designed to be permanently deployed in a wellbore with a separable topside electronics unit that provides power, control electronics, timing, as well as a means for synchronization with other oilfield systems being used in conjunction such as data recorders and processing equipment.
- a multitude of seismic sources forming a linear array designed to be permanently deployed in a wellbore where the array is cemented inside the wellbore.
- a multitude of seismic sources forming a linear array designed to be permanently deployed in a wellbore where the sections of drill pipe/tubing are designed to be coupled together during the installation process with water tight, pressure proof connections
- a multitude of seismic sources forming a linear array designed to be permanently deployed in a wellbore, and designed to operate at elevated downhole temperatures, i.e., 150 degrees Celsius and higher.
- a multitude of seismic sources forming a linear array, designed to be permanently deployed in a wellbore the separable sections of drill pipe/tubing used for interconnection between the individual sources and/or to connect the top of the seismic source array to the surface connection is made of a plastic material.
- a multitude of seismic sources forming a linear array, designed to be permanently deployed in a wellbore the separable sections of drill pipe/tubing used for interconnection between the individual sources and/or to connect the top of the seismic source array to the surface connection is made of a reinforced composite material.
- a multitude of seismic sources forming a linear array designed to be permanently deployed in a wellbore where coiled tubing (with all wires inside) is used for deep wells to connect the top of the seismic source array to the surface connection, and can be used to provide a means for pushing the array for horizontal well applications.
- a multitude of seismic sources forming a linear array designed to be deployed in a wellbore on a temporary basis where the drill pipe, tubing, and/or coiled tubing (with wires inside) provide the means for insertion and extraction.
- a traditional method of deploying tools into a wellbore is via an armored cable.
- the armor surrounds the insulated conductors and or optical fibers, providing physical protection to the interior elements as well as longitudinal strength in tension.
- the armor is typically made of multiple strands of solid steel wire wrapped around the cable core with a lay angle that is consistent with the bend radius of the cable.
- the armor can be in a single layer or in multiple layers to provide specific performance features, however, those performance features are beyond the scope of the discussion at hand. So, the additional embodiment is added: A multitude of seismic sources forming an array, designed to be permanently deployed in wellbore(s) where the connecting element 3 between the individual sources 4 is an armored cable and the connecting element 6 between the top of the seismic
- the source/array to the surface is also an armored cable. It also includes a means of connecting the armored cable to the individual seismic sources via a termination that captures the armor to provide a pull-out strength
- Rotary vibrators are used to consolidate freshly placed concrete by helping entrapped air to escape. As the concrete subsides, large air voids between coarse aggregate particles fill with mortar. This consolidation enhances the concrete's performance, i.e., the concrete's density, strength, and the bond with reinforcing steel are improved.
- An additional claim of the present invention is that we can energize our downhole vibrator during the cementing process to ensure a good cement job; good compaction, elimination of air gaps, uniform density, good bonding between our source's outer body and the cement, and good bonding between the cement and the borehole walls.
- a single downhole vibratory seismic source is positioned at the bottom of each well so as to direct acoustic radiation downwardly from the bottom of the well into the earth as is illustrated in Fig. 4.
- Such wells can include shallow holes in the ground (on the order of 20 feet or less) with the source placed at the bottom and refilled with earth.
- Such wells can be arranged in patterns, such as an X or a cross, in which a single downhole vibratory seismic source 1 A is placed in a shallow hole (which can be dug without the need for expensive equipment) 20 and then power/control cables 22 are brought up to a shallow vault 23 which can be connected by trenches 24 with other vaults, one or more of which may contain electronics for controlling the entire array (but each seismic source 1 A will not necessarily need its own electronics).
- the orbital vibrators described so far have a primary acoustic radiation pattern that is orthogonal or perpendicular to the wellbore in which it is installed. In some applications it is desired to have acoustic energy from the source radiate in a direction downwardly from a bottom of a wellbore in which it is installed. In such an embodiment, as illustrated in Fig. 4, using orbital vibrators configured as in Fig. 13 where the primary direction of the useful energy generated by the source will be downwardly from the bottom of the well into the earth (which is ninety degrees different in direction from a previously described ORBITAL VIBRATOR DSS array put in a well).
- a single seismic source located in a bottom of a well might be oriented so as to generate a radiation pattern that is perpendicular to the wellbore, instead of being directed ninety degrees differently in a direction heading into the earth away from the well (and the ground surface).
- the acoustic sources described above may include orbital vibrators, combinations of orbital vibrators that when combined provide a desired directionality, or electromagnetic vibrators.
- a downhole clamping method that allows the sources to be lowered into the well with the clamps retracted, and once the sources are in the desired position, activating the clamps via the vibration of the source.
- non-armored cable for example a cable with a polymer
- Kevlar such as Kevlar, Vectran, or aramid fiber.
- Passive clamps are widely used (such as bow springs or magnets); however, since they are always “on” their clamping force is relatively low to allow them to slide down the wellbore during deployment.
- the source(s) can hang freely in the fluid column of the well when the source is energized causing the energy to be transmitted to the fluid and then to the well casing. This does not provide as much coupling efficiency as the cement; however, the source(s) are retrievable.
- ORBITAL VIBRATOR DSS Another means proposed here is a more novel passive clamping system for the distributed seismic source (ORBITAL VIBRATOR DSS).
- the ORBITAL VIBRATOR DSS is unique in that it generates acoustic energy in the radial direction only, with virtually no energy in the longitudinal direction of the wellbore. Because traditional downhole sources generate energy in all directions and traditional downhole sensors detect energy in all three axes (i.e., x, y, z) they require clamps that are rigid in all three axes.
- the ORBITAL VIBRATOR DSS requires the clamp be rigid in the radial direction only.
- the ORBITAL VIBRATOR DSS clamp requires no rigidity in the longitudinal direction, it can employ low friction rollers to allow the ORBITAL VIBRATOR DSS to more easily slide in the borehole (i.e., during deployment and retrieval) while still providing a high radial clamping force.
- the clamp can be similar to tubing centralizers (see Fig. 5) that incorporate rollers to centralize production tubing for example, inside a larger well casing.
- the passive ORBITAL VIBRATOR DSS clamps may also incorporate some kind of spring force that maintains the rollers against sides of the wellbore.
- the force should be high enough to remain stiff under the vibratory forces imparted from the source to the wellbore.
- the spring force also serves to maintain contact with the wellbore due to variations in wellbore diameter. Methods to adjust the passive clamps to fit various well diameters are also envisioned.
- the low friction rollers can incorporate ball bearings, needle bearings, or any other kind bearing that provides low rolling friction.
- Another alternative approach is to combine the rollers with a downhole activated mechanical means to clamp each of the sources to the wellbore.
- Using rollers to contact the wellbore upon activation prevents them from becoming stuck in the well, which is a large problem with clamping arms that engage directly against the wellbore.
- the seismic sources are lowered into the well in the undamped position (allows them to move freely) and clamped once they are at the desired depth.
- pipe clamps or an equivalent can be used to keep the spring force that maintains the rollers against sides of the wellbore compressed until a source is inserted into the wellbore and once the source is inserted, the pipe clamp or its equivalent can be removed.
- Mechanically activated clamps are usually very complicated, i.e., requiring additional power, electronics, motors and/or hydraulics.
- This embodiment requires no additional active downhole electronics or motors. It engages the clamps passively, i.e., simply energizing the source creates strong vibrational forces causing the clamps to "unlock” thereby coupling them to the wellbore. Whereas it is difficult to "push” the array down a wellbore even with minimal friction (i.e., requires sinker weight bars) it is relatively easy to pull an array out if it employs low friction rollers. It
- the forces generated by an orbital vibrator are proportional to the rotating mass, the distance the mass is from the centerline (i.e., the
- each orbital vibrator can provide optimum output at a different frequency range.
- An ORBITAL VIBRATOR DSS complete with control electronics can be installed at each wellhead at or near the surface exit point.
- a means of remote wireless activation can be added to allow activation from another location, or from anywhere around the world via an internet connection. This will allow operators to conduct seismic surveys without having to leave the office.
- a cable with synthetic strength members can be used.
- the possible synthetic strength member materials include Vectran, Kevlar, aramid fiber or any other suitable high strength material.
- a further addition to the above disclosure is a unique method of providing a frequency variable sinusoidal (3 phase) signal to drive a downhole source that may be 1000 or more feet away from the surface electronics. It allows speed control of a three phase induction motor without sending a PWM AC signal through a long downhole cable.
- the orbital vibrator consists of a motor (typically an AC electric 3 phase induction motor) that spins an off-center or eccentric weight resulting in vibration (the speed of the motor determines the frequency of the vibration).
- the speed of the AC motor is related to the frequency of the supplied AC voltage. The formula for calculating the speed of an AC
- Synchronous Speed 120 * Frequency/ Number of Poles
- VFDs Frequency Drives
- Most VFDs are designed for use with 3 phase induction motors.
- Fig. 6 shows a typical system that could be used to drive a downhole orbital vibrator.
- 240V or 480V three phase 60 Hz power is supplied to the VFD.
- the VFD converts the fixed 60 Hz input into a 240/480V variable frequency output signal, typically with a range from 0 to about 600 Hz.
- VFDs specify a maximum distance (typically 100 feet or so) between the VFD and the motor that is being controlled. The reason for this limit is because the output of a VFD is not a true sine wave but rather a pulse width modulation (PWM) approximating a sine wave (see Fig. 7).
- PWM pulse width modulation
- the PWM signal can become corrupted. This distance limit is acceptable for most industrial applications, however, for the downhole vibrator application, the separation distance can be 1000 feet or more.
- Various electronic modifications can be made to the downhole vibrator unit to minimize the effect described above; however, they add cost/complexity and do not completely eliminate the problem.
- Another feature of a PWM signal is that the voltage pulses can be significantly higher than the 240/480 modulated sine wave.
- the downhole cable and the downhole electric motor insulation would have to be rated for up to 1000 volts even though they will be running at 240/480 volts. This adds complexity, expense, and reduces reliability, another negative for the downhole application.
- Fig. 8 An alternative that eliminates the problems described above is depicted in Fig. 8.
- the VFD drives a 3 phase induction motor mounted in very close proximity.
- the 3 phase AC motor is directly coupled to a 3 phase AC generator.
- the VFD controls the speed of the motor which in turn controls the speed of the generator.
- the generator produces a true sine wave output (variable frequency) that does not degrade with distance and is free of the high voltage pulses.
- the key here is providing a true, clean sinusoidal variable frequency signal to the downhole orbital vibrator via the use of an AC generator.
- the means to drive and control the speed of the AC generator are numerous and not necessarily limited to the use of a VFD/AC induction motor.
- a The GPUSA marine vibrator solution (using orbital vibrators as the source) is small, reliable, simple, and inexpensive.
- the photo in Fig. 9 shows an orbital vibrator along with the motor generator set used to provide a clean variable frequency AC drive signal to the source module in accordance with the present invention (hereinafter referred to as "the GPUSA orbital vibrator solution").
- the GPUSA orbital vibrator solution produces useable vibratory signals from 30 Hz to 200 Hz.
- the main difference is that rather than being placed in a well, for this application it is placed in a body of water such as the Gulf of Mexico, North Sea or any other body of water where subsea oil may be present.
- the cavitation threshold is a function of the energy intensity of the source per unit area (i.e., watts per square inch) and the ambient water pressure. For a given amount of power, the cavitation threshold may be increased by increasing the ambient pressure (deeper depth) or increasing the surface area (reducing the energy intensity), or both.
- the ORBITAL VIBRATOR DSS it can be placed inside a cylindrical vessel filled with an appropriate acoustic coupling fluid (preferably with a higher cavitation threshold than water; see Fig. 1 1 ) such that the energy intensity at the outer surface of the source/projector is below the cavitation threshold.
- an appropriate acoustic coupling fluid preferably with a higher cavitation threshold than water; see Fig. 1 1
- Such acoustic coupling fluids are well known within the sonar industry. If needed, the pressure of the acoustic coupling fluid inside the cylindrical vessel may be increased also.
- the ORBITAL VIBRATOR DSS can be covered with a solid acoustic coupling material that serves the same function (see Fig. 12).
- the acoustic coupling may be cast/molded over the ORBITAL VIBRATOR DSS or it may be split and bolted and/or adhesively bonded to the ORBITAL VIBRATOR DSS.
- the two primary desired properties of the solid acoustic coupling material are that it provide a good acoustic match with the
- Dipole projector design The existing ORBITAL VIBRATOR DSS system can be modified by placing two single axis orbital vibrators OV on a rigid plate/frame RP by mounting M with each turning in the opposite direction (see Fig. 13). In this case the omnidirectional energy from each vibrator cancels out with the exception of the linear motion. The resultant energy will radiate in only two directions (i.e. dipole). 3.
- Half dipole projector design For some applications it is desired to have the energy radiate in one direction only.
- the two single axis orbital vibrators OV from the dipole design can be mounted to a flexing plate FP on the inside of an otherwise stiff, air filled enclosure E (see Fig. 14). Here the linear motion will cause the plate it is mounted on to move up and down, imparting the energy into the water in one direction only.
- the marine ORBITAL VIBRATOR DSS array can be towed behind a ship, tethered from an offshore oil platform at a depths anywhere from just below the surface to the sea bottom, or it can be trenched (buried) beneath the sea floor (see Fig. 15). If placed on the sea floor bottom a cover may be placed over the ORBITAL VIBRATOR DSS (omni or dipole versions) to direct the acoustic energy into the sea bottom and limit acoustic energy from entering the seawater above (minimizing harm to sea creatures).
- the half dipole projector can be placed on the sea floor directing all energy into the ocean bottom for maximum efficiency and minimal radiation in the seawater above minimizing possible harm to marine life.
- the other end can be attached to a small craft such that it can be easily repositioned (rotated) during a seismic survey. It can also be positioned (tethered) between two boats.
- tow depth can be maintained by flotation devices, depth control birds, or similar means.
- the half dipole projector may also be mounted to the underside of a boat with the source projecting energy downward.
- the downhole array does not have to be clamped, but can be fluid coupled inside the wellbore.
- the vibrator imparts an acoustic wave in the borehole fluid and the acoustic wave front travels radially to the borehole wall and exits as seismic waves.
- the orbital vibrator works by rotating an eccentric (off center from the axis of rotation) mass that results in cyclical vibration.
- the frequency of the vibration is directly
- Fig. 17 represents the eccentric mass of an orbital vibrator at rest incorporating the current invention.
- mass A is firmly attached to the motor shaft and the mass B is moveable however it is being held in place by springs S while the motor is at rest.
- Both masses are designed to rotate with the motor shaft.
- centrifugal force will tend to force the mass B away from the center of the motor shaft, providing more counterbalancing of the mass A, thus reducing the overall eccentricity.
- Preferred means for achieving linear motion from two orbital vibrators As disclosed previously, two orbital vibrators can be placed side by side and if the rotors are counter-rotating (see Fig. 13), the side forces cancel each other out and the resultant force is a linear motion only. Whereas the traditional method of achieving this linear motion is by placing two complete orbital vibrators (two individual motors with eccentric weights operating in synchrony) side by side, this is inefficient because it requires two separate drive motors and also synchronization between them is an added concern. Alternatively, a single drive motor can be used to drive two separate rotating shafts, each with eccentric weights attached. Gears or belt drives can be used to drive the two separate counter-rotating shafts from the single motor.
- ORBITAL VIBRATOR DSS Distributed Seismic Source
- While the most common mode of operation will be to vibrate the plate in an up and down motion against the earth's surface, sometimes it is desired to impart some side to side movement into the plate to impart shear waves into the earth. This can be performed by allowing a means to orient the axis of the vibrator away from normal to the plate/earth's surface.
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- Life Sciences & Earth Sciences (AREA)
- Engineering & Computer Science (AREA)
- Physics & Mathematics (AREA)
- Remote Sensing (AREA)
- Acoustics & Sound (AREA)
- Geology (AREA)
- Environmental & Geological Engineering (AREA)
- General Life Sciences & Earth Sciences (AREA)
- General Physics & Mathematics (AREA)
- Geophysics (AREA)
- Mechanical Engineering (AREA)
- Geophysics And Detection Of Objects (AREA)
- Building Environments (AREA)
Abstract
Description
Claims
Priority Applications (2)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
CA2961732A CA2961732A1 (en) | 2014-09-19 | 2015-09-17 | Distributed seismic source array |
GB1704858.8A GB2545594A (en) | 2014-09-19 | 2015-09-17 | Distributed seismic source array |
Applications Claiming Priority (12)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
US201462052879P | 2014-09-19 | 2014-09-19 | |
US62/052,879 | 2014-09-19 | ||
US201462077123P | 2014-11-07 | 2014-11-07 | |
US62/077,123 | 2014-11-07 | ||
US201562104025P | 2015-01-15 | 2015-01-15 | |
US62/104,025 | 2015-01-15 | ||
US201562111974P | 2015-02-04 | 2015-02-04 | |
US62/111,974 | 2015-02-04 | ||
US201562159820P | 2015-05-11 | 2015-05-11 | |
US62/159,820 | 2015-05-11 | ||
US14/857,778 US10139513B2 (en) | 2014-09-19 | 2015-09-17 | Distributed seismic source array |
US14/857,778 | 2015-09-17 |
Publications (1)
Publication Number | Publication Date |
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WO2016044675A1 true WO2016044675A1 (en) | 2016-03-24 |
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ID=55533881
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
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PCT/US2015/050824 WO2016044675A1 (en) | 2014-09-19 | 2015-09-17 | Distributed seismic source array |
Country Status (3)
Country | Link |
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CA (1) | CA2961732A1 (en) |
GB (1) | GB2545594A (en) |
WO (1) | WO2016044675A1 (en) |
Citations (12)
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GB1193295A (en) * | 1967-06-09 | 1970-05-28 | Albert George Bodine Jr | Fluid Resonator for Use with Sonically Driven Apparatus |
US4383308A (en) * | 1980-12-29 | 1983-05-10 | Mobil Oil Corporation | Acoustic well logging device for detecting shear and compressional waves |
US4874061A (en) * | 1988-01-19 | 1989-10-17 | Conoco Inc. | Downhole orbital seismic source |
US5954169A (en) * | 1997-10-24 | 1999-09-21 | Lord Corporation | Adaptive tuned vibration absorber, system utilizing same and method of controlling vibration therewith |
US20020171560A1 (en) * | 1997-06-02 | 2002-11-21 | Schlumberger Technology Corporation | Reservoir management system and method |
US20060096380A1 (en) * | 2004-11-11 | 2006-05-11 | Novascone Stephen R | Apparatus and methods for determining at least one characteristic of a proximate environment |
US20080068928A1 (en) * | 2006-09-15 | 2008-03-20 | Microseismic Inc. | Method for passive seismic emission tomography |
US20090003131A1 (en) * | 2007-06-28 | 2009-01-01 | Robert Jay Meyer | Enhanced oil recovery using multiple sonic sources |
US20110222368A1 (en) * | 2010-03-10 | 2011-09-15 | VCable, LLC | Detecting Seismic Data in a Wellbore |
US20120327742A1 (en) * | 2010-03-02 | 2012-12-27 | David John Kusko | Borehole Flow Modulator and Inverted Seismic Source Generating System |
US20130317630A1 (en) * | 2012-05-22 | 2013-11-28 | GM Global Technology Operations LLC | Methods, systems and apparatus for implementing dithering in motor drive system for controlling operation of an electric machine |
US20130343156A1 (en) * | 2012-06-25 | 2013-12-26 | Steve Allan Horne | Devices, Systems and Methods for Measuring Borehole Seismic Wavefield Derivatives |
-
2015
- 2015-09-17 WO PCT/US2015/050824 patent/WO2016044675A1/en active Application Filing
- 2015-09-17 GB GB1704858.8A patent/GB2545594A/en not_active Withdrawn
- 2015-09-17 CA CA2961732A patent/CA2961732A1/en not_active Abandoned
Patent Citations (12)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
GB1193295A (en) * | 1967-06-09 | 1970-05-28 | Albert George Bodine Jr | Fluid Resonator for Use with Sonically Driven Apparatus |
US4383308A (en) * | 1980-12-29 | 1983-05-10 | Mobil Oil Corporation | Acoustic well logging device for detecting shear and compressional waves |
US4874061A (en) * | 1988-01-19 | 1989-10-17 | Conoco Inc. | Downhole orbital seismic source |
US20020171560A1 (en) * | 1997-06-02 | 2002-11-21 | Schlumberger Technology Corporation | Reservoir management system and method |
US5954169A (en) * | 1997-10-24 | 1999-09-21 | Lord Corporation | Adaptive tuned vibration absorber, system utilizing same and method of controlling vibration therewith |
US20060096380A1 (en) * | 2004-11-11 | 2006-05-11 | Novascone Stephen R | Apparatus and methods for determining at least one characteristic of a proximate environment |
US20080068928A1 (en) * | 2006-09-15 | 2008-03-20 | Microseismic Inc. | Method for passive seismic emission tomography |
US20090003131A1 (en) * | 2007-06-28 | 2009-01-01 | Robert Jay Meyer | Enhanced oil recovery using multiple sonic sources |
US20120327742A1 (en) * | 2010-03-02 | 2012-12-27 | David John Kusko | Borehole Flow Modulator and Inverted Seismic Source Generating System |
US20110222368A1 (en) * | 2010-03-10 | 2011-09-15 | VCable, LLC | Detecting Seismic Data in a Wellbore |
US20130317630A1 (en) * | 2012-05-22 | 2013-11-28 | GM Global Technology Operations LLC | Methods, systems and apparatus for implementing dithering in motor drive system for controlling operation of an electric machine |
US20130343156A1 (en) * | 2012-06-25 | 2013-12-26 | Steve Allan Horne | Devices, Systems and Methods for Measuring Borehole Seismic Wavefield Derivatives |
Also Published As
Publication number | Publication date |
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CA2961732A1 (en) | 2016-03-24 |
GB201704858D0 (en) | 2017-05-10 |
GB2545594A (en) | 2017-06-21 |
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