Source: http://www.patentsencyclopedia.com/app/20130175090
Timestamp: 2018-06-20 16:37:08
Document Index: 123379952

Matched Legal Cases: ['art 9000', 'art 9001', 'art 9000', 'art 9000', 'art 9000', 'art 9000', 'art 9001', 'art 9001', 'art 9001', 'art 9001', 'art 9001']

Patent application number: 20130175090
1. A high power laser drilling system for advancing a borehole comprising: a. a source of high power laser energy, the laser source capable of providing a laser beam having at least 5 kW of power; b. a tubing assembly, the tubing assembly having at least 1000 feet of tubing, having a distal end and a proximal; c. a source of fluid for use in advancing a borehole; d. the proximal end of the tubing being in fluid communication with the source of fluid, whereby fluid is transported in association with the tubing; e. the proximal end of the tubing being in optical communication with the laser source, whereby the laser beam can be transported in association with the tubing; f. the tubing comprising a high power laser transmission cable, the transmission cable having a distal end and a proximal end, the proximal end being in optical communication with the laser source, whereby the laser beam is transmitted by the cable from the proximal end to the distal end of the cable for delivery of the laser beam energy to the borehole; and, g. the power of the laser energy at the distal end of the cable when the cable is within a borehole being at least about 2 kW.
29. The system of claim 1 comprising: h. a means for advancing the tubing into the borehole; i. a bottom hole assembly; j. a blowout preventer; k. a diverter; l. the bottom hole assembly in fluid and optical communication with the distal end of the tubing; and, m. the tubing extending through the blowout preventer and the diverter and into the borehole, and being capable of advancement through the blowout preventer and the diverter into and out of the borehole by the advancing means; n. whereby the laser beam and fluid are directed by the bottom hole assembly to a surface in the borehole to advance the borehole.
53. A method of advancing a borehole using a laser, the method comprising: a. advancing a high power laser beam transmission means into a borehole; i. the borehole having a bottom surface, a top opening, and a length extending between the bottom surface and the top opening of at least about 1000 feet; ii. the transmission means comprising a distal end, a proximal end, and a length extending between the distal and proximal ends, the distal end being advanced down the borehole; iii. the transmission means comprising a means for transmitting high power laser energy; b. providing a high power laser beam to the proximal end of the transmission means; c. transmitting substantially all of the power of the laser beam down the length of the transmission means so that the beam exits the distal end; and, d. directing the laser beam to the bottom surface of the borehole whereby the length of the borehole is increased, in part, based upon the interaction of the laser beam with the bottom of the borehole.
57. A high power laser drilling system for advancing a borehole comprising: a. a source of high power laser energy, the laser source capable of providing a laser beam having at least 5 kW of power; b. a tubing assembly, the tubing assembly having at least 1000 feet of tubing, having a distal end and a proximal; c. the proximal end of the tubing being in optical communication with the laser source, whereby the laser beam can be transported in association with the tubing; d. the tubing comprising a high power laser transmission cable, the transmission cable having a distal end and a proximal end, the proximal end being in optical communication with the laser source, whereby the laser beam is transmitted by the cable from the proximal end to the distal end of the cable for delivery of the laser beam energy to the borehole; and, e. the power of the laser energy at the distal end of the cable when the cable is within a borehole being at least about 2 kW.
68. A high power laser drilling system for advancing a borehole comprising: a. a source of high power laser energy, the laser source capable of providing a laser beam having at least 5 kW of power; b. a tubing, the tubing assembly having at least 1000 feet of tubing, having a distal end and a proximal; c. a means for advancing the tubing into the borehole; d. a bottom hole assembly; e. a blowout preventer; f. a diverter; g. the proximal end of the tubing being in optical communication with the laser source, whereby the laser beam can be transported in association with the tubing; h. the tubing comprising a high power laser transmission cable, the transmission cable having a distal end and a proximal end, the proximal end being in optical communication with the laser source, whereby the laser beam is transmitted by the cable from the proximal end to the distal end of the cable for delivery of the laser beam energy to the borehole; and, i. the power of the laser energy at the distal end of the cable when the cable is within a borehole being at least about 2 kW.
69-86. (canceled)
[0004] The term borehole includes any opening that is created in the ground that is substantially longer than it is wide, such as a well, a well bore, a well hole, and other terms commonly used or known in the art to define these types of narrow long passages in the earth. Although boreholes are generally oriented substantially vertically, they may also be oriented on an angle from vertical, to and including horizontal. Thus, using a level line as representing the horizontal orientation, a borehole can range in orientation from 0° i.e., a vertical borehole, to 90°,i.e., a horizontal borehole and greater than 90° e.g., such as a heel and toe. Boreholes may further have segments or sections that have different orientations, they may be arcuate, and they may be of the shapes commonly found when directional drilling is employed. Thus, as used herein unless expressly provided otherwise, the "bottom" of the borehole, the "bottom" surface of the borehole and similar terms refer to the end of the borehole, i.e., that portion of the borehole farthest along the path of the borehole from the borehole's opening, the surface of the earth, or the borehole's beginning.
[0023] There is still further provided a system and a method for providing high power laser energy to the bottom of deep boreholes, the system and method comprising employing a high powered laser source, from for example about 1 kW to about 20 kW, which provides a high power laser beam, employing a means for transmitting the laser beam from the high power laser source to the bottom of a deep borehole, the employed transmitting means having a means for suppressing nonlinear scattering phenomena whereby, high power laser energy is delivered to the bottom of the borehole with sufficient power to advance the borehole.
[0035] FIG. 1 is a cross sectional view of the earth, a borehole and an example of a system of the present invention for advancing a borehole.
[0041] FIG. 7 is a schematic diagram of a laser fiber amplifier.
[0046] The spool of coiled tubing 1009 is rotated to advance and retract the coiled tubing 1012. Thus, the laser beam transmission means 1008 and the fluid conveyance means 1011 are attached to the spool of coiled tubing 1009 by means of rotating coupling means 1013. The coiled tubing 1012 contains a means to transmit the laser beam along the entire length of the coiled tubing, i.e., "long distance high power laser beam transmission means," to the bottom hole assembly, 1014. The coiled tubing 1012 also contains a means to convey the fluid along the entire length of the coiled tubing 1012 to the bottom hole assembly 1014.
[0057] For example, FIG. 5. Illustrates a frequency modulated phased array of lasers. Thus, there is provided a master oscillator than can be frequency modulated, directly or indirectly, that is then used to injection-lock lasers or amplifiers to create a higher power composite beam than can be achieved by any individual laser. Thus, there are provided lasers 5001, 5002, 5003, and 5004, which have the same wavelength. The laser beams are combined by a beam combiner 5005 and transmitted by an optical fiber 5006. The lasers 5001, 5002, 5003 and 5004 are associated with a master oscillator 5008 that is FM modulated. The combined beam having a spectrum show in 5007, where 6 is the frequency excursion of the FM modulation. Such lasers are disclosed in U.S. Pat. No. 5,694,408, the disclosure of which is incorporated here in reference in its entirety.
[0058] The laser source may be a low order mode source (M2<2) so it can be focused into an optical fiber with a mode diameter of <100 microns. Optical fibers with small mode field diameters ranging from 50 microns to 6 microns have the lowest transmission losses. However, this should be balanced by the onset of non-linear phenomenon and the physical damage of the face of the optical fiber requiring that the fiber diameter be as large as possible while the transmission losses have to be as small as possible.
TABLE-US-00001 TABLE 1 Optical Characteristics Characteristics Test conditions Symbol Min. Typ. Max Unit Operation Mode CW, QCW Polarization Random Nominal Output Power PNOM 20000* W Output Power Tuning Range 10 100 % Emission Wavelength POUT = 20 kW 1070 1080 nm Emission Linewidth POUT = 20 kW 3 6 nm Switching ON/OFF Time POUT = 20 kW 80 100 μsec Output Power Modulation Rate POUT = 20 kW 5.0 kHz Output Power Stability Over 8 hrs, TWATER = Const 1.0 2.0 % Feeding Fiber Core Diameter 200 μm Beam Parameter Product 200 μm BPP 12 14 mm*mrad Feeding Fiber Fiber Length L 10 m Fiber Cable Bend Radius: unstressed R 100 stressed 200 mm Output Termination IPG HLC-8 Connector (QBH compatible) Aiming Laser Wavelength 640 680 nm Aiming Laser Output Power 0.5 1 mW Parameters Test conditions Min. Typ. Max Unit Operation Voltage (3 phases) 440 V 480 520 VAC Frequency 50/60 Hz Power Consumption POUT = 20 kW 75 80 kW Operating Temperature Range +15 +40 ° C. Humidity: without conditioner T < 25° C. 90 % with built-in conditioner T < 40° C. 95 Storage Temperature Without water -40 +75 ° C. Dimensions, H × W × D NEMA-12; IP-55 1490 × 1480 × 810 mm Weight 1200 kg Plumbing NPT Threaded Stainless Steel and/or Plastic Tubing *Output power tested at connector at distance not greater than 50 meters from laser.
[0062] In addition to the configuration of FIG. 1, and the above preferred examples of lasers for use with the present invention other configurations of lasers for use in a high efficiency laser drilling systems are contemplated. Thus, Laser selection may generally be based on the intended application or desired operating parameters. Average power, specific power, irradiance, operation wavelength, pump source, beam spot size, exposure time, and associated specific energy may be considerations in selecting a laser. The material to be drilled, such as rock formation type, may also influence laser selection. For example, the type of rock may be related to the type of resource being pursued. Hard rocks such as limestone and granite may generally be associated with hydrothermal sources, whereas sandstone and shale may generally be associated with gas or oil sources. Thus by way of example, the laser may be a solid-state laser, it may be a gas, chemical, dye or metal-vapor laser, or it may be a semiconductor laser. Further, the laser may produce a kilowatt level laser beam, and it may be a pulsed laser. The laser further may be a Nd:YAG laser, a CO2 laser, a diode laser, such as an infrared diode laser, or a fiber laser, such as a ytterbium-doped multi-clad fiber laser. The infrared fiber laser emits light in the wavelengths ranges from 800 nm to 1600 nm. The fiber laser is doped with an active gain medium comprising rare earth elements, such as holmium, erbium, ytterbium, neodymium, dysprosium, praseodymium, thulium or combinations thereof. Combinations of one or more types of lasers may be implemented.
[0063] Fiber lasers of the type useful in the present invention are generally built around dual-core fibers. The inner core may be composed of rare-earth elements; ytterbium, erbium, thulium, holmium or a combination. The optical gain medium emits wavelengths of 1064 nm, 1360 nm, 1455 nm, and 1550 nm, and can be diffraction limited. An optical diode may be coupled into the outer core (generally referred to as the inner cladding) to pump the rare earth ion in the inner core. The outer core can be a multi-mode waveguide. The inner core serves two purposes: to guide the high power laser; and, to provide gain to the high power laser via the excited rare earth ions. The outer cladding of the outer core may be a low index polymer to reduce losses and protect the fiber. Typical pumped laser diodes emit in the range of about 915-980 nm (generally--940 nm). Fiber lasers are manufactured from IPG Photonics or Southhampton Photonics. High power fibers were demonstrated to produce 50 kW by IPG Photonics when multiplexed.
TABLE-US-00002 TABLE 2 Chiller PC400.01-NZ-DIS Technical Data for 60 Hz operation: IPG-Laser type Cooling capacity net YLR-15000, YLR-20000 Refrigerant 60.0 kW Necessary air flow R407C Installation 26100 m3/h Number of compressors Outdoor installation Number of fans 2 Number of pumps 3 2 Operation Limits Designed Operating Temperature 33° C. (92 F.) Operating Temperature min. (-) 20° C. (-4 F.) Operating Temperature max. 39° C. (102 F.) Storage Temperature min. (with empty water (-) 40° C. (-40 F.) tank) Storage Temperature max. 70° C. (158 F.) Tank volume regular water 240 Liter (63.50 Gallon) Tank volume DI water 25 Liter (6.61 Gallon) Electrical Data for 60 Hz operation: Designed power consumption without heater 29.0 kW Designed power consumption with heater 33.5 kW Power consumption max. 41.0 kW Current max. 60.5 A Fuse max. 80.0 A Starting current 141.0 A Connecting voltage 460 V/3 Ph/PE Frequency 60 Hz Tolerance connecting voltage +/-10% Dimensions, weights and sound level Weight with empty tank 900 KG (1984 lbs) Sound level at distance of 5 m 68 dB(A) Width 2120 mm (831/2 inches) Depth 860 mm (337/8 inches) Height 1977 mm (777/8 inches) Tap water circuit 0 Cooling capacity 56.0 kW Water outlet temperature 21° C. (70 F.) Water inlet temperature 26° C. (79 F.) Temperature stability +/-1.0 K Water flow vs. water pressure free available 135 l/min at 3.0 bar (35.71 GPM at 44 PSI) Water flow vs. water pressure free available 90 l/min at 1.5 bar (23.81 GPM at 21 PSI) De-ionized water circuit Cooling capacity 4.0 kW Water outlet temperature 26° C. (79 F.) Water inlet temperature 31° C. (88 F.) Temperature stability +/-1.0 K Water flow vs. water pressure free available 20 l/min at 1.5 bar (5.28 GPM at 21 PSI) Waterflow vs. water pressure free available 15 l/min at 4.0 bar (3.96 GPM at 58 PSI) Options (included) Bifrequent version: 400 V/3 Ph/50 Hz 460 V/3 Ph 60 Hz
[0077] For systems of the general type illustrated in FIG. 1, the spool of coiled tubing can contain the following exemplary lengths of coiled tubing: from 1 km (3,280 ft) to 9 km (29,528 ft); from 2 km (6,561 ft) to 5 km (16,404 ft); at least about 5 km (16,404 ft); and from about 5 km (16,404 ft) to at least about 9 km (29,528 ft). The spool may be any standard type spool using 2.875 steel pipe. For example commercial spools typically include 4-6 km of steel 27/8'' tubing, Tubing is available in commercial sizes ranging from 1'' to 27/8''.
[0078] Preferably, the Spool will have a standard type 27/8'' hollow steel pipe, i.e., the coiled tubing. As discussed in further herein, the coiled tubing will have in it at least one optical fiber for transmitting the laser beam to the bottom hole assembly. In addition to the optical fiber the coiled tubing may also carry other cables for other downhole purposes or to transmit material or information back up the borehole to the surface. The coiled tubing may also carry the fluid or a conduit for carrying the fluid. To protect and support the optical fibers and other cables that are carried in the coiled tubing stabilizers may be employed.
[0080] When using a spool the mechanical axis of the spool is used to transmit optical power from the input end of the optical fiber to the distal end. This calls for a precision optical bearing system (the fiber slip ring) to maintain a stable alignment between the external fiber providing the optical power and the optical fiber mounted on the spool. The laser can be mounted inside of the spool, or as shown in FIG. 1 it can be mounted external to the spool or if multiple lasers are employed both internal and external locations may be used. The internally mounted laser may be a probe laser, used for analysis and monitoring of the system and methods performed by the system. Further, sensing and monitoring equipment may be located inside of or otherwise affixed to the rotating elements of the spool.
[0081] There is further provided rotating coupling means to connect the coiled tubing, which is rotating, to the laser beam transmission means 1008, and the fluid conveyance means 1011, which are not rotating. As illustrated by way of example in FIG. 2, a spool of coiled tubing 2009 has two rotating coupling means 2013. One of said coupling means has an optical rotating coupling means 2002 and the other has a fluid rotating coupling means 2003. The optical rotating coupling means 2002 can be in the same structure as the fluid rotating coupling means 2003 or they can be separate. Thus, preferably, two separate coupling means are employed. Additional rotating coupling means may also be added to handle other cables, such as for example cables for downhole probes.
[0082] The optical rotating coupling means 2002 is connected to a hollow precision ground axle 2004 with bearing surfaces 2005, 2006. The laser transmission means 2008 is optically coupled to the hollow axle 2004 by optical rotating coupling means 2002, which permits the laser beam to be transmitted from the laser transmission means 2008 into the hollow axle 2004. The optical rotating coupling means for example may be made up of a QBH connector, a precision collimator, and a rotation stage, for example a Precitec collimator through a Newport rotation stage to another Precitec collimator and to a QBH collimator. To the extent that excessive heat builds up in the optical rotating coupling cooling should be applied to maintain the temperature at a desired level.
[0083] The hollow axle 2004 then transmits the laser beam to an opening 2007 in the hollow axle 2004, which opening contains an optical coupler 202010 that optically connects the hollow axle 2004 to the long distance high power laser beam transmission means 2025 that is located inside of the coiled tubing 2012. Thus, in this way the laser transmission means 2008, the hollow axle 2004 and the long distance high power laser beam transmission means 2025 are rotatably optically connected, so that the laser beam can be transmitted from the laser to the long distance high power laser beam transmission means 2025.
[0084] A further illustration of an optical connection for a rotation spool is provided in FIG. 6, wherein there is illustrated a spool 6000 and a support 6001 for the spool 6000. The spool 6000 is rotatably mounted to the support 6001 by load bearing bearings 6002. An input optical cable 6003, which transmits a laser beam from a laser source (not shown in this figure) to an optical coupler 6005. The laser beam exits the connector 6005 and passes through optics 6009 and 6010 into optical coupler 6006, which is optically connected to an output optical cable 6004. The optical coupler 6005 is mounted to the spool by a preferably non-load bearing bearing 6008, while coupler 6006 is mounted to the spool by device 6007 in a manner that provides for its rotation with the spool. In this way as the spool is rotated, the weight of the spool and coiled tubing is supported by the load bearing bearings 6002, while the rotatable optical coupling assembly allows the laser beam to be transmitted from cable 6003 which does not rotate to cable 6004 which rotates with the spool.
[0085] In addition to using a rotating spool of coiled tubing, as illustrated in FIGS. 1 and 2, another means for extending and retrieving the long distance high powered laser beam transmission means is a stationary spool or creel. As illustrated, by way of example, in FIGS. 3A and 3B there is provided a creel 3009 that is stationary and which contains coiled within the long distance high power laser beam transmission means 3025. That means is connected to the laser beam transmission means 3008, which is connected to the laser (not shown in this figure). In this way the laser beam may be transmitted into the long distance high power laser beam transmission means and that means may be deployed down a borehole. Similarly, the long distance high power laser beam transmission means may be contained within coiled tubing on the creel. Thus, the long distance means would be an armored optical cable of the type provided herein. In using the creel consideration should be given to the fact that the optical cable will be twisted when it is deployed. To address this consideration the bottom hole assembly, or just the laser drill head, may be slowly rotated to keep the optical cable untwisted, the optical cable may be pre-twisted, and the optical cable may be designed to tolerate the twisting.
[0086] The Fluid
[0087] The source of fluid may be either a gas, a liquid, a foam, or system having multiple capabilities. The fluid may serve many purposes in the advancement of the borehole. Thus, the fluid is primarily used for the removal of cuttings from the bottom of the borehole, for example as is commonly referred to as drilling fluid or drilling mud, and to keep the area between the end of the laser optics in the bottom hole assembly and the bottom of the borehole sufficiently clear of cuttings so as to not interfere with the path and power of the laser beam. It also may function to cool the laser optics and the bottom hole assembly, as well as, in the case of an incompressible fluid, or a compressible fluid under pressure. The fluid further provides a means to create hydrostatic pressure in the well bore to prevent influx of gases and fluids.
[0088] Thus, in selecting the type of fluid, as well as the fluid delivery system, consideration should be given to, among other things, the laser wavelength, the optics assembly, the geological conditions of the borehole, the depth of the borehole, and the rate of cuttings removal that is needed to remove the cuttings created by the laser's advancement of the borehole. It is highly desirable that the rate of removal of cuttings by the fluid not be a limiting factor to the systems rate of advancing a borehole. For example fluids that may be employed with the present invention include conventional drilling muds, water (provided they are not in the optical path of the laser), and fluids that are transmissive to the laser, such as halocarbons, (halocarbon are low molecular weight polymers of chlorotrifluoroethylene (PCTFE)), oils and N2. Preferably these fluids can be employed and preferred and should be delivered at rates from a couple to several hundred CFM at a pressure ranging from atmospheric to several hundred psi. If combinations of these fluids are used flow rates should be employed to balance the objects of maintaining the trasmissiveness of the optical path and removal of debris.
[0089] The Long Distance HPLB Transmission Means
[0090] Preferably the long distance high powered laser beam transmission means is an optical fiber or plurality of optical fibers in an armored casing to conduct optical power from about 1 kW to about 20 kW, from about 10 kW to about 20 kW, at least about 10 kW, and preferably about 20 or more kW average power down into a borehole for the purpose of sensing the lithology, testing the lithology, boring through the lithology and other similar applications relating in general to the creation, advancement and testing of boreholes in the earth. Preferably the armored optical fiber comprises a 0.64 cm (1/4'') stainless steel tube that has 1, 2, 1 to 10, at least 2, more than 2, at least about 50, at least about 100, and most preferably between 2 to 15 optical fibers in it. Preferably these will be about 500 micron core diameter baseline step index fibers
[0091] At present it is believed that Industrial lasers use high power optical fibers armored with steel coiled around the fiber and a polymer jacket surrounding the steel jacket to prevent unwanted dust and dirt from entering the optical fiber environment. The optical fibers are coated with a thin coating of metal or a thin wire is run along with the fiber to detect a fiber break. A fiber break can be dangerous because it can result in the rupture of the armor jacket and would pose a danger to an operator. However, this type of fiber protection is designed for ambient conditions and will not withstand the harsh environment of the borehole.
[0092] Fiber optic sensors for the oil and gas industry are deployed both unarmored and armored. At present it is believed that the currently available unarmored approaches are unacceptable for the high power applications contemplated by this application. The current manifestations of the armored approach are similarly inadequate, as they do not take into consideration the method for conducting high optical power and the method for detecting a break in the optical fiber, both of which are important for a reliable and safe system. The current method for armoring an optical fiber is to encase it in a stainless steel tube, coat the fiber with carbon to prevent hydrogen migration, and finally fill the tube with a gelatin that both cushions the fiber and absorbs hydrogen from the environment. However this packaging has been performed with only small diameter core optical fibers (50 microns) and with very low power levels <1 Watt optical power.
[0093] Thus, to provide for a high power optical fiber that is useful in the harsh environment of a borehole, there is provided a novel armored fiber and method. Thus, it is provided to encase a large core optical fiber having a diameter equal to or greater than 50 microns, equal to or greater than 75 microns and most preferably equal to or greater than 100 microns, or a plurality of optical fibers into a metal tube, where each fiber may have a carbon coating, as well as a polymer, and may include Teflon coating to cushion the fibers when rubbing against each other during deployment. Thus the fiber, or bundle of fibers, can have a diameter of from about greater than or equal to 150 microns to about 700 microns, 700 microns to about 1.5 mm, or greater than 1.5 mm.
[0094] The carbon coating can range in thicknesses from 10 microns to >600 microns. The polymer or Teflon coating can range in thickness from 10 microns to >600 microns and preferred types of such coating are acrylate, silicone, polyimide, PFA and others. The carbon coating can be adjacent the fiber, with the polymer or Teflon coating being applied to it. Polymer or Teflon coatings are applied last to reduce binding of the fibers during deployment.
[0095] In some non-limiting embodiments, fiber optics may send up to 10 kW per a fiber, up to 20 kW per a fiber, up to and greater than 50 kw per fiber. The fibers may transmit any desired wavelength or combination of wavelengths. In some embodiments, the range of wavelengths the fiber can transmit may preferably be between about 800 nm and 2100 nm. The fiber can be connected by a connector to another fiber to maintain the proper fixed distance between one fiber and neighboring fibers. For example, fibers can be connected such that the beam spot from neighboring optical fibers when irradiating the material, such as a rock surface are under 2'' and non-overlapping to the particular optical fiber. The fiber may have any desired core size. In some embodiments, the core size may range from about 50 microns to 1 mm or greater. The fiber can be single mode or multimode. If multimode, the numerical aperture of some embodiments may range from 0.1 to 0.6. A lower numerical aperture may be preferred for beam quality, and a higher numerical aperture may be easier to transmit higher powers with lower interface losses. In some embodiments, a fiber laser emitted light at wavelengths comprised of 1060 nm to 1080 nm, 1530 nm to 1600 nm, 1800 nm to 2100 nm, diode lasers from 800 nm to 2100 nm, CO2 Laser at 10,600 nm, or Nd:YAG Laser emitting at 1064 nm can couple to the optical fibers. In some embodiments, the fiber can have a low water content. The fiber can be jacketed, such as with polyimide, acrylate, carbon polyamide, and carbon/dual acrylate or other material. If requiring high temperatures, a polyimide or a derivative material may be used to operate at temperatures over 300 degrees Celsius. The fibers can be a hollow core photonic crystal or solid core photonic crystal. In some embodiments, using hollow core photonic crystal fibers at wavelengths of 1500 nm or higher may minimize absorption losses.
[0096] The use of the plurality of optical fibers can be bundled into a number of configurations to improve power density. The optical fibers forming a bundle may range from two at hundreds of watts to kilowatt powers in each fiber to millions at milliwatts or microwatts of power. In some embodiments, the plurality of optical fibers may be bundled and spliced at powers below 2.5 kW to step down the power. Power can be spliced to increase the power densities through a bundle, such as preferably up to 10 kW, more preferably up to 20 kW, and even more preferably up to or greater than 50 kW. The step down and increase of power allows the beam spot to increase or decrease power density and beam spot sizes through the fiber optics. In most examples, splicing the power to increase total power output may be beneficial so that power delivered through fibers does not reach past the critical power thresholds for fiber optics.
[0097] Thus, by way of example there is provided the following configurations set forth in Table 3 herein.
TABLE-US-00003 TABLE 3 Diameter of Number of bundle fibers in bundle 100 microns 1 200 microns-1 mm 2 to 100 100 microns-1 mm 1
[0098] A thin wire may also be packaged, for example in the 1/4'' stainless tubing, along with the optical fibers to test the fiber for continuity. Alternatively a metal coating of sufficient thickness is applied to allow the fiber continuity to be monitored. These approaches, however, become problematic as the fiber exceeds 1 km in length, and do not provide a practical method for testing and monitoring.
[0099] The configurations in Table 3 can be of lengths equal to or greater than 1 m, equal to or greater than 1 km, equal to or greater than 2 km, equal to or greater than 3 km, equal to or greater than 4 km and equal to or greater than 5 km. These configuration can be used to transmit there through power levels from about 0.5 kW to about 10 kW, from greater than or equal to 1 kW, greater than or equal to 2 kW, greater than or equal to 5 kW, greater than or equal to 8 kW, greater than or equal to 10 kW and preferable at least about 20 kW.
[0100] In transmitting power over long distances, such as down a borehole or through a cable that is at least 1 km, there are three sources of power losses in an optical fiber, Raleigh Scattering, Raman Scattering and Brillioun Scattering. The first, Raleigh Scattering is the intrinsic losses of the fiber due to the impurities in the fiber. The second, Raman Scattering can result in Stimulated Raman Scattering in a Stokes or Anti-Stokes wave off of the vibrating molecules of the fiber. Raman Scattering occurs preferentially in the forward direction and results in a wavelength shift of up to +25 nm from the original wavelength of the source. The third mechanism, Brillioun Scattering, is the scattering of the forward propagating pump off of the acoustic waves in the fiber created by the high electric fields of the original source light (pump). This third mechanism is highly problematic and may create great difficulties in transmitting high powers over long distances. The Brillioun Scattering can give rise to Stimulated Brillioun Scattering (SBS) where the pump light is preferentially scattered backwards in the fiber with a frequency shift of approximately 1 to about 20 GHz from the original source frequency. This Stimulated Brillioun effect can be sufficiently strong to backscatter substantially all of the incident pump light if given the right conditions. Therefore it is desirable to suppress this non-linear phenomenon. There are essentially four primary variables that determine the threshold for SBS: the length of the gain medium (the fiber); the linewidth of the source laser; the natural Brillioun linewidth of the fiber the pump light is propagating in; and, the mode field diameter of the fiber. Under typical conditions and for typical fibers, the length of the fiber is inversely proportional to the power threshold, so the longer the fiber, the lower the threshold. The power threshold is defined as the power at which a high percentage of incident pump radiation will be scattered such that a positive feedback takes place whereby acoustic waves are generated by the scattering process. These acoustic waves then act as a grating to incite further SBS. Once the power threshold is passed, exponential growth of scattered light occurs and the ability to transmit higher power is greatly reduced. This exponential growth continues with an exponential reduction in power until such point whereby any additional power input will not be transmitted forward which point is defined herein as the maximum transmission power. Thus, the maximum transmission power is dependent upon the SBS threshold, but once reached, the maximum transmission power will not increase with increasing power input.
[0101] Thus, as provided herein, novel and unique means for suppressing nonlinear scattering phenomena, such as the SBS and Stimulated Raman Scattering phenomena, means for increasing power threshold, and means for increasing the maximum transmission power are set forth for use in transmitting high power laser energy over great distances for, among other things, the advancement of boreholes.
[0102] The mode field diameter needs to be as large as practical without causing undue attenuation of the propagating source laser. Large core single mode fibers are currently available with mode diameters up to 30 microns, however bending losses are typically high and propagation losses are higher than desired. Small core step index fibers, with mode field diameters of 50 microns are of interest because of the low intrinsic losses, the significantly reduced launch fluence and the decreased SBS gain because the fiber is not polarization preserving, it also has a multi-mode propagation constant and a large mode field diameter. All of these factors effectively increase the SBS power threshold. Consequently, a larger core fiber with low Raleigh Scattering losses is a potential solution for transmitting high powers over great distances, preferably where the mode field diameter is 50 microns or greater in diameter.
[0103] The next consideration is the natural Brillioun linewidth of the fiber. As the Brillioun linewidth increases, the scattering gain factor decreases. The Brillioun linewidth can be broadened by varying the temperature along the length of the fiber, modulating the strain on the fiber and inducing acoustic vibrations in the fiber. Varying the temperature along the fiber results in a change in the index of refraction of the fiber and the background (kT) vibration of the atoms in the fiber effectively broadening the Brillioun spectrum. In down borehole application the temperature along the fiber will vary naturally as a result of the geothermal energy that the fiber will be exposed to as the depths ranges expressed herein. The net result will be a suppression of the SBS gain. Applying a thermal gradient along the length of the fiber could be a means to suppress SBS by increasing the Brillioun linewidth of the fiber. For example, such means could include using a thin film heating element or variable insulation along the length of the fiber to control the actual temperature at each point along the fiber. Applied thermal gradients and temperature distributions can be, but are not limited to, linear, step-graded, and periodic functions along the length of the fiber.
[0104] Modulating the strain for the suppression of nonlinear scattering phenomena, on the fiber can be achieved, but those means are not limited to anchoring the fiber in its jacket in such a way that the fiber is strained. By stretching each segment between support elements selectively, then the Brillioun spectrum will either red shift or blue shift from the natural center frequency effectively broadening the spectrum and decreasing the gain. If the fiber is allowed to hang freely from a tensioner, then the strain will vary from the top of the hole to the bottom of the hole, effectively broadening the Brillioun gain spectrum and suppressing SBS. Means for applying strain to the fiber include, but are not limited to, twisting the fiber, stretching the fiber, applying external pressure to the fiber, and bending the fiber. Thus, for example, as discussed above, twisting the fiber can occur through the use of a creel. Moreover, twisting of the fiber may occur through use of downhole stabilizers designed to provide rotational movement. Stretching the fiber can be achieved, for example as described above, by using support elements along the length of the fiber. Downhole pressures may provide a pressure gradient along the length of the fiber thus inducing strain.
[0105] Acoustic modulation of the fiber can alter the Brillioun linewidth. By placing acoustic generators, such as piezo crystals along the length of the fiber and modulating them at a predetermined frequency, the Brillioun spectrum can be broadened effectively decreasing the SBS gain. For example, crystals, speakers, mechanical vibrators, or any other mechanism for inducing acoustic vibrations into the fiber may be used to effectively suppress the SBS gain. Additionally, acoustic radiation can be created by the escape of compressed air through predefined holes, creating a whistle effect.
[0106] The interaction of the source linewidth and the Brillioun linewidth in part defines the gain function. Varying the linewidth of the source can suppress the gain function and thus suppress nonlinear phenomena such as SBS. The source linewidth can be varied, for example, by FM modulation or closely spaced wavelength combined sources, an example of which is illustrated in FIG. 5. Thus, a fiber laser can be directly FM modulated by a number of means, one method is simply stretching the fiber with a piezo-electric element which induces an index change in the fiber medium, resulting in a change in the length of the cavity of the laser which produces a shift in the natural frequency of the fiber laser. This FM modulation scheme can achieve very broadband modulation of the fiber laser with relatively slow mechanical and electrical components. A more direct method for FM modulating these laser sources can be to pass the beam through a non-linear crystal such as Lithium Niobate, operating in a phase modulation mode, and modulate the phase at the desired frequency for suppressing the gain.
[0107] Additionally, a spectral beam combination of laser sources which may be used to suppress Stimulated Brillioun Scattering. Thus the spaced wavelength beams, the spacing as described herein, can suppress the Stimulated Brillioun Scattering through the interference in the resulting acoustic waves, which will tend to broaden the Stimulated Brillioun Spectrum and thus resulting in lower Stimulated Brillioun Gain. Additionally, by utilizing multiple colors the total maximum transmission power can be increased by limiting SBS phenomena within each color. An example of such a laser system is illustrated in FIG. 4.
[0108] Raman scattering can be suppressed by the inclusion of a wavelength-selective filter in the optical path. This filter can be a reflective, transmissive, or absorptive filter. Moreover, an optical fiber connector can include a Raman rejection filter. Additionally a Raman rejection filter could be integral to the fiber. These filters may be, but are not limited to, a bulk filter, such as a dichroic filter or a transmissive grating filter, such as a Bragg grating filter, or a reflective grating filter, such as a ruled grating. For any backward propagating Raman energy, as well as, a means to introduce pump energy to an active fiber amplifier integrated into the overall fiber path, is contemplated, which, by way of example, could include a method for integrating a rejection filter with a coupler to suppress Raman Radiation, which suppresses the Raman Gain. Further, Brillioun scattering can be suppressed by filtering as well. Faraday isolators, for example, could be integrated into the system. A Bragg Grating reflector tuned to the Brillioun Scattering frequency could also be integrated into the coupler to suppress the Brillioun radiation.
[0109] To overcome power loss in the fiber as a function of distance, active amplification of the laser signal can be used. An active fiber amplifier can provide gain along the optical fiber to offset the losses in the fiber. For example, by combining active fiber sections with passive fiber sections, where sufficient pump light is provided to the active, i.e., amplified section, the losses in the passive section will be offset. Thus, there is provided a means to integrate signal amplification into the system. In FIG. 7 there is illustrated an example of such a means having a first passive fiber section 8000 with, for example, -1 dB loss, a pump source 8001 optically associated with the fiber amplifier 8002, which may be introduced into the outer clad, to provide for example, a +1 dB gain of the propagating signal power. The fiber amplifier 8002 is optically connected to a coupler 8003, which can be free spaced or fused, which is optically connected to a passive section 8004. This configuration may be repeated numerous times, for varying lengths, power losses, and downhole conditions. Additionally, the fiber amplifier could act as the delivery fiber for the entirety of the transmission length. The pump source may be uphole, downhole, or combinations of uphole and downhole for various borehole configurations.
[0110] A further method is to use dense wavelength beam combination of multiple laser sources to create an effective linewidth that is many times the natural linewidth of the individual laser effectively suppressing the SBS gain. Here multiple lasers each operating at a predetermined wavelength and at a predetermined wavelength spacing are superimposed on each other, for example by a grating. The grating can be transmissive or reflective.
[0111] The optical fiber or fiber bundle can be encased in an environmental shield to enable it to survive at high pressures and temperatures. The cable could be similar in construction to the submarine cables that are laid across the ocean floor and maybe buoyant if the hole is filled with water. The cable may consist of one or many optical fibers in the cable, depending on the power handling capability of the fiber and the power required to achieve economic drilling rates. It being understood that in the field several km of optical fiber will have to be delivered down the borehole. The fiber cables maybe made in varying lengths such that shorter lengths are used for shallower depths so higher power levels can be delivered and consequently higher drilling rates can be achieved. This method requires the fibers to be changed out when transitioning to depths beyond the length of the fiber cable. Alternatively a series of connectors could be employed if the connectors could be made with low enough loss to allow connecting and reconnecting the fiber(s) with minimal losses.
[0112] Thus, there is provided in Tables 4 and 5 herein power transmissions for exemplary optical cable configurations.
TABLE-US-00004 TABLE 4 Power Length Diameter of # of fibers Power in of fiber(s) bundle in bundle out 20 kW 5 km 500 microns 1 15 kW 20 kW 7 km 500 microns 1 13 kW 20 kW 5 km 200 microns-1mm 2 to 100 15 kW 20 kW 7 km 200 microns-1mm 2 to 100 13 kW 20 kW 5 km 100-200 microns 1 10 kW 20 kW 7 km 100-200 microns 1 8 kW
TABLE-US-00005 TABLE 5 (with active amplification) Power Length Diameter of # of fibers Power in of fiber(s) bundle in bundle out 20 kW 5 km 500 microns 1 17 kW 20 kW 7 km 500 microns 1 15 kW 20 kW 5 km 200 microns-1mm 2 to 100 20 kW 20 kW 7 km 200 microns-1mm 2 to 100 18 kW 20 kW 5 km 100-200 microns 1 15 kW 20 kW 7 km 100-200 microns 1 13 kW
[0113] The optical fibers are preferably placed inside the coiled tubing for advancement into and removal from the borehole. In this manner the coiled tubing would be the primary load bearing and support structure as the tubing is lowered into the well. It can readily be appreciated that in wells of great depth the tubing will be bearing a significant amount of weight because of its length. To protect and secure the optical fibers, including the optical fiber bundle contained in the, for example, 1/4'' stainless steel tubing, inside the coiled tubing stabilization devices are desirable. Thus, at various intervals along the length of the coiled tubing supports can be located inside the coiled tubing that fix or hold the optical fiber in place relative to the coiled tubing. These supports, however, should not interfere with, or otherwise obstruct, the flow of fluid, if fluid is being transmitted through the coiled tubing. An example of a commercially available stabilization system is the ELECTROCOIL System. These support structures, as described above, may be used to provide strain to the fiber for the suppression of nonlinear phenomena.
[0114] Although it is preferable to place the optical fibers within the tubing, the fibers may also be associated with the tubing by, for example, being run parallel to the tubing, and being affixed thereto, by being run parallel to the tubing and be slidably affixed thereto, or by being placed in a second tubing that is associated or not associated with the first tubing. In this way, it should be appreciated that various combinations of tubulars may be employed to optimize the delivery of laser energy, fluids, and other cabling and devices into the borehole. Moreover, the optical fiber may be segmented and employed with conventional strands of drilling pipe and thus be readily adapted for use with a conventional mechanical drilling rig outfitted with connectable tubular drill pipe.
[0115] Downhole Monitoring Apparatus and Methods.
[0116] During drilling operations, and in particular during deep drilling operations, e.g., depths of greater than 1 km, it may be desirable to monitor the conditions at the bottom of the borehole, as well as, monitor the conditions along and in the long distance high powered laser beam transmission means. Thus, there is further provided the use of an optical pulse, train of pulses, or continuous signal, that are continuously monitored that reflect from the distal end of the fiber and are used to determine the continuity of the fiber. Further, there is provided for the use of the fluorescence from the illuminated surface as a means to determine the continuity of the optical fiber. A high power laser will sufficiently heat the rock material to the point of emitting light. This emitted light can be monitored continuously as a means to determine the continuity of the optical fiber. This method is faster than the method of transmitting a pulse through the fiber because the light only has to propagate along the fiber in one direction. Additionally there is provided the use of a separate fiber to send a probe signal to the distal end of the armored fiber bundle at a wavelength different than the high power signal and by monitoring the return signal on the high power optical fiber, the integrity of the fiber can be determined.
[0117] These monitoring signals may transmit at wavelengths substantially different from the high power signal such that a wavelength selective filter may be placed in the beam path uphole or downhole to direct the monitoring signals into equipment for analysis. For example, this selective filter may be placed in the creel or spool described herein.
[0118] To facilitate such monitoring an Optical Spectrum Analyzer or Optical Time Domain Reflectometer or combinations thereof may be used. An AnaritsuMS9710C Optical Spectrum Analyzer having: a wavelength range of 600 nm-1.7 microns; a noise floor of 90 dBm @ 10 Hz, -40 dBm @ 1 MHz; a 70 dB dynamic range at 1 nm resolution; and a maximum sweep width: 1200 nm and an Anaritsu CMA 4500 OTDR may be used.
[0119] The efficiency of the laser's cutting action can also be determined by monitoring the ratio of emitted light to the reflected light. Materials undergoing melting, spallation, thermal dissociation, or vaporization will reflect and absorb different ratios of light. The ratio of emitted to reflected light may vary by material further allowing analysis of material type by this method. Thus, by monitoring the ratio of emitted to reflected light material type, cutting efficiency, or both may be determined. This monitoring may be performed uphole, downhole, or a combination thereof.
[0120] Moreover, for a variety of purposes such as powering downhole monitoring equipment, electrical power generation may take place in the borehole including at or near the bottom of the borehole. This power generation may take place using equipment known to those skilled in the art, including generators driven by drilling muds or other downhole fluids, means to convert optical to electrical power, and means to convert thermal to electrical power.
[0121] The Bottom Hole Assembly.
[0122] The bottom hole assembly contains the laser optics, the delivery means for the fluid and other equipment. Bottom hole assemblies are disclosed in detail in co-pending U.S. patent application Ser. No. ______, Attorney Docket 13938/10 Foro s2, Ser. No. ______, Attorney Docket 13938/6 Foro s2 and Ser. No. ______, Attorney Docket 13938/7 Foro s3, filed contemporaneously herewith, the disclosure of which is incorporated herein by reference in its entirety. In general the bottom hole assembly contains the output end, also referred to as the distal end, of the long distance high power laser beam transmission means and preferably the optics for directing the laser beam to the earth or rock to be removed for advancing the borehole, or the other structure intended to be cut.
[0123] The present systems and in particular the bottom hole assembly, may include one or more optical manipulators. An optical manipulator may generally control a laser beam, such as by directing or positioning the laser beam to spall material, such as rock. In some configurations, an optical manipulator may strategically guide a laser beam to spall material, such as rock. For example, spatial distance from a borehole wall or rock may be controlled, as well as the impact angle. In some configurations, one or more steerable optical manipulators may control the direction and spatial width of the one or more laser beams by one or more reflective mirrors or crystal reflectors. In other configurations, the optical manipulator can be steered by an electro-optic switch, electroactive polymers, galvonometers, piezoelectrics, and/or rotary/linear motors. In at least one configuration, an infrared diode laser or fiber laser optical head may generally rotate about a vertical axis to increase aperture contact length. Various programmable values such as specific energy, specific power, pulse rate, duration and the like maybe implemented as a function of time. Thus, where to apply energy may be strategically determined, programmed and executed so as to enhance a rate of penetration and/or laser/rock interaction, to enhance the overall efficiency of borehole advancement, and to enhance the overall efficiency of borehole completion, including reducing the number of steps on the critical path for borehole completion. One or more algorithms may be used to control the optical manipulator.
[0124] Thus, by way of example, as illustrated in FIG. 8 the bottom hole assembly comprises an upper part 9000 and a lower part 9001. The upper part 9000 may be connected to the lower end of the coiled tubing, drill pipe, or other means to lower and retrieve the bottom hole assembly from the borehole. Further, it may be connected to stabilizers, drill collars, or other types of downhole assemblies (not shown in the figure) which in turn are connected to the lower end of the coiled tubing, drill pipe, or other means to lower and retrieve the bottom hole assembly from the borehole. The upper part 9000 further contains the means 9002 that transmitted the high power energy down the borehole and the lower end 9003 of the means. In FIG. 8 this means is shown as a bundle of four optical cables. The upper part 9000 may also have air amplification nozzles 9005 that discharge a portion up to 100% of the fluid, for example N2. The upper part 9000 is joined to the lower part 9001 with a sealed chamber 9004 that is transparent to the laser beam and forms a pupil plane for the beam shaping optics 9006 in the lower part 9001. The lower part 9001 may be designed to rotate and in this way for example an elliptical shaped laser beam spot can be rotated around the bottom of the borehole. The lower part 9001 has a laminar flow outlet 9007 for the fluid and two hardened rollers 9008, 9009 at its lower end, although non-laminar flows and turbulent flows may be employed.
[0125] In use, the high energy laser beam, for example greater than 10 kW, would travel down the fibers 9002, exit the ends of the fibers 9003 and travel through the sealed chamber and pupil plane 9004 into the optics 9006, where it would be shaped and focused into an elliptical spot. The laser beam would then strike the bottom of the borehole spalling, melting, thermally dissociating, and/or vaporizing the rock and earth struck and thus advance the borehole. The lower part 9001 would be rotating and this rotation would cause the elliptical laser spot to rotate around the bottom of the borehole. This rotation would also cause the rollers 9008, 9009 to physically dislodge any material that was crystallized by the laser or otherwise sufficiently fixed to not be able to be removed by the flow of the fluid alone. The cuttings would be cleared from the laser path by the laminar flow of the fluid, as well as, by the action of the rollers 9008, 9009 and the cuttings would then be carried up the borehole by the action of the fluid from the air amplifier 9005, as well as, the laminar flow opening 9007.
[0126] The Mud Return and Handling System.
[0127] Thus, in general cutting removal system may be typical of that used in an oil drilling system. These would include by way of example a shale shaker. Further, desanders and desilters and then centrifuges may be employed. The purpose of this equipment is to remove the cuttings so that the fluid can be recirculated and reused. If the fluid, i.e., circulating medium is gas, than a water misting systems may also be employed.
[0128] To further illustrate the advantages, uses, operating parameters and applications of the present invention, by way of example and without limitation, the following suggested exemplary studies are proposed.
[0129] Test exposure times of 0.05 s, 0.1 s, 0.2 s, 0.5 s and 1 s will be used for granite and limestone. Power density will be varied by changing the beam spot diameter (circular) and elliptical area of 12.5 mm×0.5 mm with a time-average power of 0.5 kW, 1.6 kW, 3 kW, 5 kW will be used. In addition to continuous wave beam, pulsed power will also be tested for spallation zones.
[0130] The general parameters of Example 1 will be repeated using sandstone and shale.Experimental Setup Fiber Laser IPG Photonics 5 kW ytterbium-doped mufti-clad fiber laser Berea Gray (or Yellow) 12'' × 12'' × 5'' and 5'' × 5'' × 5'' Sandstone Shale 12'' × 12'' × 5'' and 5'' × 5'' × 5'' Beam Type CW/Collimated Beam Spot Size (or 0.0625'' (12.5 mm × 0.5 mm), 0.1'' diameter) Power 0.25 kW, 0.5 kW, 1.6 kW, 3 kW, 5 kW Exposure Times 1 s, 0.5 s. 0.1 s
[0131] The ability to chip a rectangular block of material, such as rock will be demonstrated in accordance with the systems and methods disclosed herein. The setup is presented in the table below, and the end of the block of rock will be used as a ledge. Blocks of granite, sandstone, limestone, and shale (if possible) will each be spalled at an angle at the end of the block (chipping rock around a ledge). The beam spot will then be moved consecutively to other parts of the newly created ledge from the chipped rock to break apart a top surface of the ledge to the end of the block. Chipping approximately 1''×1''×1'' sized rock particles will be the goal. Applied SP and SE will be selected based on previously recorded spallation data and information gleaned from Experiments 1 and 2 presented above. ROP to chip the rock will be determined, and the ability to chip rock to desired specifications will be demonstrated.
TABLE-US-00008 Experimental Setup Fixed: Fiber Laser IPG Photonics 5 kW ytterbium-doped multi-clad fiber laser Dolomite/Barre Granite 12'' × 12'' × 12'' and 12'' × 12'' × 24'' Rock Size Limestone 12'' × 12'' × 12'' and 12'' × 12'' × 24'' Berea Gray (or Yellow) 12'' × 12'' × 12'' and 12'' × 12'' × 24'' Sandstone Shale 12'' × 12'' × 12'' and 12'' × 12'' × 24'' Beam Type CW/Collimated and Pulsed at Spallation Zones Specific Power Spallation zones (920 W/cm2 at ~2.6 kJ/cc for Sandstone & 4 kW/cm2 at ~0.52 kJ/cc for Lime- stone) Beam Size 12.5 mm × 0.5 mm Exposure Times See Experiments 1 & 2 Purging 189 l/min Nitrogen Flow
[0132] Multiple beam chipping will be demonstrated. Spalling overlap in material, such as rock resulting from two spaced apart laser beams will be tested. Two laser beams will be run at distances of 0.2'', 0.5'', 1'', 1.5'' away from each other, as outlined in the experimental setup below. Granite, sandstone, limestone, and shale will each be used. Rock fractures will be tested by spalling at the determined spalling zone parameters for each material. Purge gas will be accounted for. Rock fractures will overlap to chip away pieces of rock. The goal will be to yield rock chips of the desired 1''×1''×1'' size. Chipping rock from two beams at a spaced distance will determine optimal particle sizes that can be chipped effectively, providing information about particle sizes to spall and ROP for optimization.
[0133] Spalling multiple points with multiple beams will be performed to demonstrate the ability to chip material, such as rock in a pattern. Various patterns will be evaluated on different types of rock using the parameters below. Patterns utilizing a linear spot approximately 1 cm×15.24 cm, an elliptical spot with major axis approximately 15.24 cm and minor axis approximately 1 cm, a single circular spot having a diameter of 1 cm, an array of spots having a diameter of 1 cm with the spacing between the spots being approximately equal to the spot diameter, the array having 4 spots spaced in a square, spaced along a line. The laser beam will be delivered to the rock surface in a shot sequence pattern wherein the laser is fired until spallation occurs and then the laser is directed to the next shot in the pattern and then fired until spallation occurs with this process being repeated. In the movement of the linear and elliptical patterns the spots are in effect rotated about their central axis. In the pattern comprising the array of spots the spots may be rotated about their central axis, and rotated about an axis point as in the hands of a clock moving around a face.
TABLE-US-00010 Experimental Setup Fiber Laser IPG Photonics 5 kW ytterbium-doped multi-clad fiber laser Dolomite/Barre Granite 12'' × 12'' × 12'' and 12'' × 12'' × 5'' Rock Size Limestone 12'' × 12'' × 12'' and 12'' × 12'' × 5'' Berea Gray (or Yellow) 12'' × 12'' × 12'' and 12'' × 12'' × 5'' Sandstone Shale 12'' × 12'' × 12'' and 12'' × 12'' × 5'' Beam Type CW/Collimated or Pulsed at Spallation Zones Specific Power Spallation zones {~920 W/cm2 at- 2.6 kJ/cc for Sandstone & 4 kW/cm2 at ~0.52 kJ/cc for Limestone Beam Size 12.5 mm × 0.5 mm Exposure Times See Experiments 1 & 2 Purging 189 l/min Nitrogen Flow
[0134] From the foregoing examples and detailed teaching it can be seen that in general one or more laser beams may spall, vaporize, or melt the material, such as rock in a pattern using an optical manipulator. Thus, the rock may be patterned by spalling to form rock fractures surrounding a segment of the rock to chip that piece of rock. The laser beam spot size may spall, vaporize, or melt the rock at one angle when interacting with rock at high power. Further, the optical manipulator system may control two or more laser beams to converge at an angle so as to meet close to a point near a targeted piece of rock. Spallation may then form rock fractures overlapping and surrounding the target rock to chip the target rock and enable removal of larger rock pieces, such as incrementally. Thus, the laser energy may chip a piece of rock up to 1'' depth and 1'' width or greater. Of course, larger or smaller rock pieces may be chipped depending on factors such as the type of rock formation, and the strategic determination of the most efficient technique.
[0135] There is provided by way of examples illustrative and simplified plans of potential drilling scenarios using the laser drilling systems and apparatus of the present invention.
[0136] Drilling Plan Example 1
TABLE-US-00011 Drilling type/Laser power down Depth Rock type hole Drill 171/2 Surface- Sand and Conventional inch hole 3000 ft shale mechanical drilling Run 133/8 Length inch casing 3000 ft Drill 121/4 inch 3000 ft- basalt 40 kW hole 8,000 ft (minimum) Run 95/8 inch Length casing 8,000 ft Drill 81/2 inch 8,000 ft- limestone Conventional hole 11,000 ft mechanical drilling Run 7 inch Length casing 11,000 ft Drill 61/4 inch 11,000 ft- Sand stone Conventional hole 14,000 ft mechanical drilling Run 5 inch Length liner 3000 ft
[0137] Drilling Plan Example 2
TABLE-US-00012 Drilling type/Laser power down Depth Rock type hole Drill 171/2 Surface-500 Sand and Conventional inch hole ft shale mechanical drilling Run 133/8 Length 500 ft casing Drill 12 1/4 500 ft-4,000 granite 40 kW hole ft (minimum) Run 95/8 inch Length 4,000 casing ft Drill 81/2 inch 4,000 ft- basalt 20 kW hole 11,000 ft (mimimum) Run 7 inch Length casing 11,000 ft Drill 61/4 inch 11,000 ft- Sand stone Conventional hole 14,000 ft mechanical drilling Run 5 inch Length 3000 ft liner
[0138] Moreover, one or more laser beams may form a ledge out of material, such as rock by spalling the rock in a pattern. One or more laser beams may spall rock at an angle to the ledge forming rock fractures surrounding the ledge to chip the piece of rock surrounding the ledge. Two or more beams may chip the rock to create a ledge. The laser beams can spall the rock at an angle to the ledge forming rock fractures surrounding the ledge to further chip the rock. Multiple rocks can be chipped simultaneously by more than one laser beams after one or more rock ledges are created to chip the piece of rock around the ledge or without a ledge by converging two beams near a point by spalling; further a technique known as kerfing may be employed.
[0139] In accordance with the teaching of the invention, a fiber laser or liquid crystal laser may be optically pumped in a range from 750 nm to 2100 nm wavelength by an infrared laser diode. A fiber laser or liquid crystal laser may be supported or extend from the infrared laser diode downhole connected by an optical fiber transmitting from infrared diode laser to fiber laser or liquid crystal laser at the infrared diode laser wavelength. The fiber cable may be composed of a material such as silica, PMMA/perfluirnated polymers, hollow core photonic crystals, or solid core photonic crystals that are in single-mode or multimode. Thus, the optical fiber may be encased by a coiled tubing or reside in a rigid drill-string. On the other hand, the light may be transmitted from the infrared diode range from the surface to the fiber laser or liquid crystal laser downhole. One or more infrared diode lasers may be on the surface.
[0140] A laser may be conveyed into the wellbore by a conduit made of coiled tubing or rigid drill-string. A power cable may be provided. A circulation system may also be provided. The circulation system may have a rigid or flexible tubing to send a liquid or gas downhole. A second tube may be used to raise the rock cuttings up to the surface. A pipe may send or convey gas or liquid in the conduit to another pipe, tube or conduit. The gas or liquid may create an air knife by removing material, such as rock debris from the laser head. A nozzle, such as a Laval nozzle may be included. For example, a Laval-type nozzle may be attached to the optical head to provide pressurized gas or liquid. The pressurized gas or liquid may be transmissive to the working wavelength of the infrared diode laser or fiber laser light to force drilling muds away from the laser path. Additional tubing in the conduit may send a lower temperature liquid downhole than ambient temperature at a depth to cool the laser in the conduit. One or more liquid pumps may be used to return cuttings and debris to the surface by applying pressure uphole drawing incompressible fluid to the surface.
[0141] The drilling mud in the well may be transmissive to visible, near-IR range, and mid-IR wavelengths so that the laser beam has a clear optical path to the rock without being absorbed by the drilling mud.
[0142] Further, spectroscopic sample data may be detected and analyzed. Analysis may be conducted simultaneously while drilling from the heat of the rock being emitted. Spectroscopic samples may be collected by laser-induced breakdown derivative spectroscopy. Pulsed power may be supplied to the laser-rock impingement point by the infrared diode laser. The light may be analyzed by a single wavelength detector attached to the infrared diode laser. For example, Raman-shifted light may be measured by a Raman spectrometer. Further, for example, a tunable diode laser using a few-mode fiber Bragg grating may be implemented to analyze the band of frequencies of the fluid sample by using ytterbium, thulium, neodymium, dysprosium, praseodymium, or erbium as the active medium. In some embodiments, a chemometric equation, or least mean square fit may be used to analyze the Raman spectra. Temperature, specific heat, and thermal diffusivity may be determined. In at least one embodiment, data may be analyzed by a neural network. The neural network may be updated real-time while drilling. Updating the diode laser power output from the neural network data may optimize drilling performance through rock formation type.
[0143] An apparatus to geo-navigate the well for logging may be included or associated with the drilling system. For example, a magnemometer, 3-axis accelerometer, and/or gyroscope may be provided. As discussed with respect to the laser, the geo-navigation device may be encased, such as with steel, titanium, diamond, or tungsten carbide. The geo-navigation device may be encased together with the laser or independently. In some embodiments, data from the geo-navigation device may direct the directional movement of the apparatus downhole from a digital signal processor.
[0144] A high power optical fiber bundle may, by way of example, hang from an infrared diode laser or fiber laser downhole. The fiber may generally be coupled with the diode laser to transmit power from the laser to the rock formation. In at least one embodiment, the infrared diode laser may be fiber coupled at a wavelength range between 800 nm to 1000 nm. In some embodiments, the fiber optical head may not be in contact with the borehole. The optical cable may be a hollow core photonic crystal fiber, silica fiber, or plastic optical fibers including PMMA/perfluorinated polymers that are in single or multimode. In some embodiments, the optical fiber may be encased by a coiled or rigid tubing. The optical fiber may be attached to a conduit with a first tube to apply gas or liquid to circulate the cuttings. A second tube may supply gas or liquid to, for example, a Laval nozzle jet to clear debris from the laser head. In some embodiments, the ends of the optical fibers are encased in a head composed of a steerable optical manipulator and mirrors or crystal reflector. The encasing of the head may be composed of sapphire or a related material. An optical manipulator may be provided to rotate the optical fiber head. In some embodiments, the infrared diode laser may be fully encased by steel, titanium, diamond, or tungsten carbide residing above the optical fibers in the borehole. In other embodiments, it may be partially encased.
[0145] Single or multiple fiber optical cables may be tuned to wavelengths of the near-IR, mid-IR, and far-IR received from the infrared diode laser inducement of the material, such as rock for derivative spectroscopy sampling. A second optical head powered by the infrared diode laser above the optical head drilling may case the formation liner. The second optical head may extend from the infrared diode laser with light being transmitted through a fiber optic. In some configurations, the fiber optic may be protected by coiled tubing. The infrared diode laser optical head may perforate the steel and concrete casing. In at least one embodiment, a second infrared diode laser above the first infrared diode laser may case the formation liner while drilling.
[0146] In accordance with one or more configurations, a fiber laser or infrared diode laser downhole may transmit coherent light down a hollow tube without the light coming in contact with the tube when placed downhole. The hollow tube may be composed of any material. In some configurations, the hollow tube may be composed of steel, titanium or silica. A mirror or reflective crystal may be placed at the end of the hollow tube to direct collimated light to the material, such as a rock surface being drilled. In some embodiments, the optical manipulator can be steered by an electro-optic switch, electroactive polymers, galvonometers, piezoelectrics, or rotary/linear motors. A circulation system may be used to raise cuttings. One or more liquid pumps may be used to return cuttings to the surface by applying pressure uphole, drawing incompressible fluid to the surface. In some configurations, the optical fiber may be attached to a conduit with two tubes, one to apply gas or liquid to circulate the cuttings and one to supply gas or liquid to a Laval nozzle jet to clear debris from the laser head.
[0147] In a further embodiment of the present inventions there is provided a drilling rig for making a borehole in the earth to a depth of from about 1 km to about 5 km or greater, the rig comprising an armored fiber optic delivery bundle, consisting of from 1 to a plurality of coated optical fibers, having a length that is equal to or greater than the depth of the borehole, and having a means to coil and uncoil the bundle while maintaining an optical connection with a laser source. In yet a further embodiment of the present invention there is provided the method of uncoiling the bundle and delivering the laser beam to a point in the borehole and in particular a point at or near the bottom of the borehole. There is further provided a method of advancing the borehole, to depths in excess of 1 km, 2 km, up to and including 5 km, in part by delivering the laser beam to the borehole through armored fiber optic delivery bundle.
[0148] The novel and innovative armored bundles and associated coiling and uncoiling apparatus and methods of the present invention, which bundles may be a single or plurality of fibers as set forth herein, may be used with conventional drilling rigs and apparatus for drilling, completion and related and associated operations. The apparatus and methods of the present invention may be used with drilling rigs and equipment such as in exploration and field development activities. Thus, they may be used with, by way of example and without limitation, land based rigs, mobile land based rigs, fixed tower rigs, barge rigs, drill ships, jack-up platforms, and semi-submersible rigs. They may be used in operations for advancing the well bore, finishing the well bore and work over activities, including perforating the production casing. They may further be used in window cutting and pipe cutting and in any application where the delivery of the laser beam to a location, apparatus or component that is located deep in the well bore may be beneficial or useful.
[0149] From the foregoing description, one skilled in the art can readily ascertain the essential characteristics of this invention, and without departing from the spirit and scope thereof, can make various changes and/or modifications of the invention to adapt it to various usages and conditions.
2013-09-26 Reaming shoe for increased borehole clearance