# Patent

## Title
Method and apparatus for delivering high power laser energy over long distances

## Abstract

Systems, devices and methods for the transmission of 1 kW or more of laser energy deep into the earth and for the suppression of associated nonlinear phenomena. Systems, devices and methods for the laser drilling of a borehole in the earth. These systems can deliver high power laser energy down a deep borehole, while maintaining the high power to advance such boreholes deep into the earth and at highly efficient advancement rates.

## Background
This application claims the benefit of priority of provisional applications: Ser. No. 61/090,384 filed Aug. 20, 2008, titled System and Methods for Borehole Drilling: Ser. No. 61/102,730 filed Oct. 3, 2008, titled Systems and Methods to Optically Pattern Rock to Chip Rock Formations; Ser. No. 61/106,472 filed Oct. 17, 2008, titled Transmission of High Optical Power Levels via Optical Fibers for Applications such as Rock Drilling and Power Transmission; and, Ser. No. 61/153,271 filed Feb. 17, 2009, title Method and Apparatus for an Armored High Power Optical Fiber for Providing Boreholes in the Earth, the disclosures of which are incorporated herein by reference.


This invention was made with Government support under Award DE-AR0000044 awarded by the Office of ARPA-E U.S. Department of Energy. The Government has certain rights in this invention.


BACKGROUND OF THE INVENTION
The present invention relates to methods, apparatus and systems for delivering high power laser energy over long distances, while maintaining the power of the laser energy to perform desired tasks. In a particular, the present invention relates to providing high power laser energy to create and advance a borehole in the earth and to perform other tasks in the borehole.
In general, boreholes have been formed in the earth's surface and the earth, i.e., the ground, to access resources that are located at and below the surface. Such resources would include hydrocarbons, such as oil and natural gas, water, and geothermal energy sources, including hydrothermal wells. Boreholes have also been formed in the ground to study, sample and explore materials and formations that are located below the surface. They have also been formed in the ground to create passageways for the placement of cables and other such items below the surface of the earth.
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.
Advancing a borehole means to increase the length of the borehole. Thus, by advancing a borehole, other than a horizontal one, the depth of the borehole is also increased. Boreholes are generally formed and advanced by using mechanical drilling equipment having a rotating drilling bit. The drilling bit is extending to and into the earth and rotated to create a hole in the earth. In general, to perform the drilling operation a diamond tip tool is used. That tool must be forced against the rock or earth to be cut with a sufficient force to exceed the shear strength of that material. Thus, in conventional drilling activity mechanical forces exceeding the shear strength of the rock or earth must be applied to that material. The material that is cut from the earth is generally known as cuttings, i.e., waste, which may be chips of rock, dust, rock fibers and other types of materials and structures that may be created by the thermal or mechanical interactions with the earth. These cuttings are typically removed from the borehole by the use of fluids, which fluids can be liquids, foams or gases.
In addition to advancing the borehole, other types of activities are performed in or related to forming a borehole, such as, work over and completion activities. These types of activities would include for example the cutting and perforating of casing and the removal of a well plug. Well casing, or casing, refers to the tubulars or other material that are used to line a wellbore. A well plug is a structure, or material that is placed in a borehole to fill and block the borehole. A well plug is intended to prevent or restrict materials from flowing in the borehole.
Typically, perforating, i.e., the perforation activity, involves the use of a perforating tool to create openings, e.g. windows, or a porosity in the casing and borehole to permit the sought after resource to flow into the borehole. Thus, perforating tools may use an explosive charge to create, or drive projectiles into the casing and the sides of the borehole to create such openings or porosities.
The above mentioned conventional ways to form and advance a borehole are referred to as mechanical techniques, or mechanical drilling techniques, because they require a mechanical interaction between the drilling equipment, e.g., the drill bit or perforation tool, and the earth or casing to transmit the force needed to cut the earth or casing.
It has been theorized that lasers could be adapted for use to form and advance a borehole. Thus, it has been theorized that laser energy from a laser source could be used to cut rock and earth through spalling, thermal dissociation, melting, vaporization and combinations of these phenomena. Melting involves the transition of rock and earth from a solid to a liquid state. Vaporization involves the transition of rock and earth from either a solid or liquid state to a gaseous state. Spalling involves the fragmentation of rock from localized heat induced stress effects. Thermal dissociation involves the breaking of chemical bonds at the molecular level.
To date it is believed that no one has succeeded in developing and implementing these laser drilling theories to provide an apparatus, method or system that can advance a borehole through the earth using a laser, or perform perforations in a well using a laser. Moreover, to date it is believed that no one has developed the parameters, and the equipment needed to meet those parameters, for the effective cutting and removal of rock and earth from the bottom of a borehole using a laser, nor has anyone developed the parameters and equipment need to meet those parameters for the effective perforation of a well using a laser. Further is it believed that no one has developed the parameters, equipment or methods need to advance a borehole deep into the earth, to depths exceeding about 300 ft (0.09 km), 500 ft (0.15 km), 1000 ft, (0.30 km), 3,280 ft (1 km), 9,840 ft (3 km) and 16,400 ft (5 km), using a laser. In particular, it is believed that no one has developed parameters, equipments, or methods nor implemented the delivery of high power laser energy, i.e., in excess of 1 kW or more to advance a borehole within the earth.
While mechanical drilling has advanced and is efficient in many types of geological formations, it is believed that a highly efficient means to create boreholes through harder geologic formations, such as basalt and granite has yet to be developed. Thus, the present invention provides solutions to this need by providing parameters, equipment and techniques for using a laser for advancing a borehole in a highly efficient manner through harder rock formations, such as basalt and granite.
The environment and great distances that are present inside of a borehole in the earth can be very harsh and demanding upon optical fibers, optics, and packaging. Thus, there is a need for methods and an apparatus for the deployment of optical fibers, optics, and packaging into a borehole, and in particular very deep boreholes, that will enable these and all associated components to withstand and resist the dirt, pressure and temperature present in the borehole and overcome or mitigate the power losses that occur when transmitting high power laser beams over long distances. The present inventions address these needs by providing a long distance high powered laser beam transmission means.
It has been desirable, but prior to the present invention believed to have never been obtained, to deliver a high power laser beam over a distance within a borehole greater than about 300 ft (0.09 km), about 500 ft (0.15 km), about 1000 ft, (0.30 km), about 3,280 ft (1 km), about 9,8430 ft (3 km) and about 16,400 ft (5 km) down an optical fiber in a borehole, to minimize the optical power losses due to non-linear phenomenon, and to enable the efficient delivery of high power at the end of the optical fiber. Thus, the efficient transmission of high power from point A to point B where the distance between point A and point B within a borehole is greater than about 1,640 ft (0.5 km) has long been desirable, but prior to the present invention is believed to have never been obtainable and specifically believed to have never been obtained in a borehole drilling activity.
A conventional drilling rig, which delivers power from the surface by mechanical means, must create a force on the rock that exceeds the shear strength of the rock being drilled. Although a laser has been shown to effectively spall and chip such hard rocks in the laboratory under laboratory conditions, and it has been theorized that a laser could cut such hard rocks at superior net rates than mechanical drilling, to date it is believed that no one has developed the apparatus systems or methods that would enable the delivery of the laser beam to the bottom of a borehole that is greater than about 1,640 ft (0.5 km) in depth with sufficient power to cut such hard rocks, let alone cut such hard rocks at rates that were equivalent to and faster than conventional mechanical drilling. It is believed that this failure of the art was a fundamental and long standing problem for which the present invention provides a solution.
Thus, the present invention addresses and provides solutions to these and other needs in the drilling arts by providing, among other things: spoiling the coherence of the Stimulated Brillioun Scattering (SBS) phenomenon, e.g. a bandwidth broadened laser source, such as an FM modulated laser or spectral beam combined laser sources, to suppress the SBS, which enables the transmission of high power down a long >1000 ft (0.30 km) optical fiber; the use of a fiber laser, disk laser, or high brightness semiconductor laser for drilling rock with the bandwidth broadened to enable the efficient delivery of the optical power via a >1000 ft (0.30 km) long optical fiber; the use of phased array laser sources with its bandwidth broadened to suppress the Stimulated Brillioun Gain (SBG) for power transmission down fibers that are >1000 ft (0.30 km) in length; a fiber spooling technique that enables the fiber to be powered from the central axis of the spool by a laser beam while the spool is turning; a method for spooling out the fiber without having to use a mechanically moving component; a method for combining multiple fibers into a single jacket capable of withstanding down hole pressures; the use of active and passive fiber sections to overcome the losses along the length of the fiber; the use of a buoyant fiber to support the weight of the fiber, laser head and encasement down a drilling hole; the use of micro lenses, aspherical optics, axicons or diffractive optics to create a predetermined pattern on the rock to achieve higher drilling efficiencies; and the use of a heat engine or tuned photovoltaic cell to reconvert optical power to electrical power after transmitting the power >1000 ft (0.30 km) via an optical fiber.
SUMMARY
It is desirable to develop systems and methods that provide for the delivery of high power laser energy to the bottom of a deep borehole to advance that borehole at a cost effective rate, and in particular, to be able to deliver such high power laser energy to drill through rock layer formations including granite, basalt, sandstone, dolomite, sand, salt, limestone, rhyolite, quartzite and shale rock at a cost effective rate. More particularly, it is desirable to develop systems and methods that provide for the ability to deliver such high power laser energy to drill through hard rock layer formations, such as granite and basalt, at a rate that is superior to prior conventional mechanical drilling operations. The present invention, among other things, solves these needs by providing the system, apparatus and methods taught herein.
Thus there is provided herein a high power laser drilling system for advancing a borehole the system having a source of high power laser energy, the laser source capable of providing a laser beam having at least 5 kW of power, the system further having a tubing assembly, the tubing assembly having at least 1000 feet of tubing and having a distal end and a proximal, the system further having a source of fluid for use in advancing a borehole. The components of the system are configured so that the proximal end of the tubing is in fluid communication with the source of fluid, whereby fluid is transported in association with the tubing, the proximal end of the tubing is in optical communication with the laser source, whereby the laser beam can be transported in association with the tubing, 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. In this manner, the power of the laser energy at the distal end of the cable when the cable is within a borehole is at least about 2 kW.
This system wherein the high power laser energy source provides a laser beam having at least about 10 kW of power and at least about 3 kW of power at the distal end of the cable within the borehole, this system wherein the high power laser energy source provides a laser beam having at least about 15 kW of power and at least about 5 kW of power at the distal end of the cable within the borehole, and this system wherein the high power laser energy source provides a laser beam having at least about 20 kW of power and at least about 7 kW of power at the distal end are provided.
These systems wherein the power of the laser energy at the distal end of the cable when the cable is within a borehole is at least about 4 kW, is at least about 14 kW and is at least about 19 kW are provided. These systems wherein the tubing assembly is a coiled tubing rig having at least 4000 ft of coiled tubing is provided. These systems wherein the tubing assembly comprises a spool of coiled tubing or a stationary spool of coiled tubing.
There is provided a further embodiment of these high power laser drilling systems for advancing a borehole the systems further having a means for advancing the tubing into the borehole, bottom hole assembly, a blowout preventer, and a diverter. Such further systems are configured so that the bottom hole assembly is in fluid and optical communication with the distal end of the tubing and the tubing extends through the blowout preventer and the diverter and into the borehole, and is capable of being advanced through the blowout preventer and the diverter into and out of the borehole by the advancing means. Thus, the laser beam and fluid are directed by the bottom hole assembly to a surface in the borehole to advance the borehole.
There is additionally provided a system for providing high power laser energy to the bottom of deep boreholes, the system comprising a source or high powered laser energy capable of providing a high power laser beam, a means for transmitting the laser beam from the high power laser to the bottom of a deep borehole, and, the transmitting means having a means to suppress SBS; whereby substantially all of the high power laser energy is delivered to the bottom of the borehole. This system may further be configured for use when the deep of borehole is at least 1,000 feet, at least 5,000 feet, is at least 10,000 feet, and still further when the laser source is at least 10 kW or greater.
There is yet further provided a spool assembly for rotatably coupling high power laser transmission cables for use in advancing boreholes, comprising base, a spool. Wherein, the spool is supported by the base through a load bearing bearing. The spool having coiled tubing having a first end and a second end, the coiled tubing comprising a means for transmitting a high power laser beam. The spool comprising an axle around which the coiled tubing is wound, the axle supported by the load bearing bearing, a first non-rotating optical connector for optically connecting a laser beam source to the axle, a rotatable optical connector optically associated with the first optical connector, whereby a laser beam is capable of being transmitted from the first optical connector to the rotatable optical connector. The assembly comprises a rotating optical connector optically associated with the rotatable optical connector, optically associated with the transmitting means and associated with the axle, whereby the spool is capable of transmitting a laser beam from the first optical connector through the rotatable optical connector and into the transmitting means during winding and unwinding of the tubing on the spool while maintaining sufficient power to advance a borehole.
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.
There is additionally provided a system for providing high power laser energy to the bottom of deep boreholes, the system comprising a high powered laser capable of providing a high power laser beam, a means for transmitting the laser beam from the high power laser to the bottom of a deep borehole, and the transmitting means having a means for increasing the maximum transmission power; whereby, high power laser energy is delivered to the bottom of the borehole with sufficient power to advance.
Moreover, there is provided a system for providing high power laser energy to the bottom of deep boreholes, the system comprising: a high powered laser capable of providing a high power laser beam; a means for transmitting the laser beam from the high power laser to the bottom of a deep borehole; and, the transmitting means having a means for increasing power threshold; whereby high power laser energy is delivered to the bottom of the borehole with sufficient power to advance the borehole.
Furthermore methods are provided herein such as a method of advancing a borehole using a laser, which method comprises: advancing a high power laser beam transmission means into a borehole; 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; 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; the transmission means comprising a means for transmitting high power laser energy; providing a high power laser beam to the proximal end of the transmission means; 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, 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.
Still further there is provided a method of advancing a borehole using a laser comprising: advancing a high power laser beam transmission fiber into a borehole; 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, the transmission fiber 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, the transmission fiber comprising a means for suppressing nonlinear scattering phenomena; providing a high power laser beam to the proximal end of the transmission means; transmitting the power of the laser beam down the length of the transmission fiber so that the beam exits the distal end; and, 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.
Yet further there is contemplated a method of advancing a borehole using a laser, the method having an advancing a high power laser beam transmission fiber into a borehole, where the borehole has a bottom surface, a top opening, and a length extending between the bottom surface and the top opening of at least about 1000 feet; the transmission fiber 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; the transmission fiber comprising a means for increasing the maximum transmission power; providing a high power laser beam to the proximal end of the transmission means; transmitting the power of the laser beam down the length of the transmission fiber so that the beam exits the distal end; and, 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.
Still additionally there is provided a method of advancing a borehole using a laser, the method comprising: advancing a high power laser beam transmission fiber into a borehole; 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; the transmission fiber 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; the transmission fiber comprising a means for increasing power threshold; providing a high power laser beam to the proximal end of the transmission means; transmitting the power of the laser beam down the length of the transmission fiber so that the beam exits the distal end; and, 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.
Additionally there is provided a high power laser drilling system for advancing a borehole comprising: a source of high power laser energy, the laser source capable of providing a laser beam having at least 5 kW of power, at least about 10 kW, at least about 15 kW, and at least about 29 kW; a tubing assembly, the tubing assembly having at least 1000 feet of tubing, having a distal end and a proximal; 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; 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, 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, at least about 3 kW of power at the distal end of the cable within the borehole, at least about 5 kW of power at the distal end of the cable within the borehole, at least about 7 kW of power at the distal end.
These systems and methods herein wherein the high power laser energy source provides a laser beam having at least about 10 kW of power and at least about 3 kW of power at the distal end of the cable within the borehole, this system wherein the high power laser energy source provides a laser beam having at least about 15 kW of power and at least about 5 kW of power at the distal end of the cable within the borehole, and this system wherein the high power laser energy source provides a laser beam having at least about 20 kW of power and at least about 7 kW of power at the distal end are provided.
These systems and methods herein wherein the power of the laser energy at the distal end of the cable when the cable is within a borehole is at least about 4 kW, is at least about 14 kW and is at least about 19 kW are provided. These systems wherein the tubing assembly is a coiled tubing rig having at least 4000 ft of coiled tubing is provided.
The systems and methods provided herein wherein the laser source comprises a single laser, comprises two lasers and comprises a plurality of lasers is provided
One of ordinary skill in the art will recognize, based on the teachings set forth in these specifications and drawings, that there are various embodiments and implementations of these teachings to practice the present invention. Accordingly, the embodiments in this summary are not meant to limit these teachings in any way.



BRIEF DESCRIPTION OF THE DRAWINGS
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.
FIG. 2 is a view of a spool.
FIGS. 3A and 3B are views of a creel.
FIG. 4 is schematic diagram for a configuration of lasers.
FIG. 5 is a schematic diagram for a configuration of lasers.
FIG. 6 is a perspective cutaway of a spool and optical rotatable coupler.
FIG. 7 is a schematic diagram of a laser fiber amplifier.
FIG. 8 is a perspective cutaway of a bottom hole assembly.



DESCRIPTION OF THE DRAWINGS AND THE PREFERRED EMBODIMENTS
In general, the present inventions relate to methods, apparatus and systems for use in laser drilling of a borehole in the earth, and further, relate to equipment, methods and systems for the laser advancing of such boreholes deep into the earth and at highly efficient advancement rates. These highly efficient advancement rates are obtainable because the present invention provides for a means to get high power laser energy to the bottom of the borehole, even when the bottom is at great depths.
Thus, in general, and by way of example, there is provided in FIG. 1 a high efficiency laser drilling system 1000 for creating a borehole 1001 in the earth 1002. As used herein the term “earth” should be given its broadest possible meaning (unless expressly stated otherwise) and would include, without limitation, the ground, all natural materials, such as rocks, and artificial materials, such as concrete, that are or may be found in the ground, including without limitation rock layer formations, such as, granite, basalt, sandstone, dolomite, sand, salt, limestone, rhyolite, quartzite and shale rock.
FIG. 1 provides a cut away perspective view showing the surface of the earth 1030 and a cut away of the earth below the surface 1002. In general and by way of example, there is provided a source of electrical power 1003, which provides electrical power by cables 1004 and 1005 to a laser 1006 and a chiller 1007 for the laser 1006. The laser provides a laser beam, i.e., laser energy, that can be conveyed by a laser beam transmission means 1008 to a spool of coiled tubing 1009. A source of fluid 1010 is provided. The fluid is conveyed by fluid conveyance means 1011 to the spool of coiled tubing 1009.
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.
Additionally, there is provided a support structure 1015, which holds an injector 1016, to facilitate movement of the coiled tubing 1012 in the borehole 1001. Further other support structures may be employed for example such structures could be derrick, crane, mast, tripod, or other similar type of structure or hybrid and combinations of these. As the borehole is advance to greater depths from the surface 1030, the use of a diverter 1017, a blow out preventer (BOP) 1018, and a fluid and/or cutting handling system 1019 may become necessary. The coiled tubing 1012 is passed from the injector 1016 through the diverter 1017, the BOP 1018, a wellhead 1020 and into the borehole 1001.
The fluid is conveyed to the bottom 1021 of the borehole 1001. At that point the fluid exits at or near the bottom hole assembly 1014 and is used, among other things, to carry the cuttings, which are created from advancing a borehole, back up and out of the borehole. Thus, the diverter 1017 directs the fluid as it returns carrying the cuttings to the fluid and/or cuttings handling system 1019 through connector 1022. This handling system 1019 is intended to prevent waste products from escaping into the environment and separates and cleans waste products and either vents the cleaned fluid to the air, if permissible environmentally and economically, as would be the case if the fluid was nitrogen, or returns the cleaned fluid to the source of fluid 1010, or otherwise contains the used fluid for later treatment and/or disposal.
The BOP 1018 serves to provide multiple levels of emergency shut off and/or containment of the borehole should a high-pressure event occur in the borehole, such as a potential blow-out of the well. The BOP is affixed to the wellhead 1020. The wellhead in turn may be attached to casing. For the purposes of simplification the structural components of a borehole such as casing, hangers, and cement are not shown. It is understood that these components may be used and will vary based upon the depth, type, and geology of the borehole, as well as, other factors.
The downhole end 1023 of the coiled tubing 1012 is connected to the bottom hole assembly 1014. The bottom hole assembly 1014 contains optics for delivering the laser beam 1024 to its intended target, in the case of FIG. 1, the bottom 1021 of the borehole 1001. The bottom hole assembly 1014, for example, also contains means for delivering the fluid.
Thus, in general this system operates to create and/or advance a borehole by having the laser create laser energy in the form of a laser beam. The laser beam is then transmitted from the laser through the spool and into the coiled tubing. At which point, the laser beam is then transmitted to the bottom hole assembly where it is directed toward the surfaces of the earth and/or borehole. Upon contacting the surface of the earth and/or borehole the laser beam has sufficient power to cut, or otherwise effect, the rock and earth creating and/or advancing the borehole. The laser beam at the point of contact has sufficient power and is directed to the rock and earth in such a manner that it is capable of borehole creation that is comparable to or superior to a conventional mechanical drilling operation. Depending upon the type of earth and rock and the properties of the laser beam this cutting occurs through spalling, thermal dissociation, melting, vaporization and combinations of these phenomena.
Although not being bound by the present theory, it is presently believed that the laser material interaction entails the interaction of the laser and a fluid or media to clear the area of laser illumination. Thus the laser illumination creates a surface event and the fluid impinging on the surface rapidly transports the debris, i.e. cuttings and waste, out of the illumination region. The fluid is further believed to remove heat either on the macro or micro scale from the area of illumination, the area of post-illumination, as well as the borehole, or other media being cut, such as in the case of perforation.
The fluid then carries the cuttings up and out of the borehole. As the borehole is advanced the coiled tubing is unspooled and lowered further into the borehole. In this way the appropriate distance between the bottom hole assembly and the bottom of the borehole can be maintained. If the bottom hole assembly needs to be removed from the borehole, for example to case the well, the spool is wound up, resulting in the coiled tubing being pulled from the borehole. Additionally, the laser beam may be directed by the bottom hole assembly or other laser directing tool that is placed down the borehole to perform operations such as perforating, controlled perforating, cutting of casing, and removal of plugs. This system may be mounted on readily mobile trailers or trucks, because its size and weight are substantially less than conventional mechanical rigs.
The Laser.
For systems of the general type illustrated in FIG. 1, having the laser located outside of the borehole, the laser may be any high powered laser that is capable of providing sufficient energy to perform the desired functions, such advancing the borehole into and through the earth and rock believed to be present in the geology corresponding to the borehole. The laser source of choice is a single mode laser or low order multi-mode laser with a low M2 to facilitate launching into a small core optical fiber, i.e. about 50 microns. However, larger core fibers are preferred. Examples of a laser source include fiber lasers, chemical lasers, disk lasers, thin slab lasers, high brightness diode lasers, as well as, the spectral beam combination of these laser sources or a coherent phased array laser of these sources to increase the brightness of the individual laser source.
For example, FIG. 4 Illustrates a spectral beam combination of lasers sources to enable high power transmission down a fiber by allocating a predetermined amount of power per color as limited by the Stimulated Brillioun Scattering (SBS) phenomena. Thus, there is provided in FIG. 4 a first laser source 4001 having a first wavelength of “x”, where x is less than 1 micron. There is provided a second laser 4002 having a second wavelength of x+δ1 microns, where δ1 is a predetermined shift in wavelength, which shift could be positive or negative. There is provided a third laser 4003 having a third wavelength of x+δ1+δ2 microns and a fourth laser 4004 having a wavelength of x+δ1+δ2+δ3 microns. The laser beams are combined by a beam combiner 4005 and transmitted by an optical fiber 4006. The combined beam having a spectrum show in 4007.
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 δ 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.
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.
Thus, the laser source should have total power of at least about 1 kW, 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. Moreover, combinations of various lasers may be used to provide the above total power ranges. Further, the laser source should have beam parameters in mm millirad as large as is feasible with respect to bendability and manufacturing substantial lengths of the fiber, thus the beam parameters may be less than about 100 mm millirad, from single mode to about 50 mm millirad, less than about 50 mm millirad, less than about 15 mm millirad, and most preferably about 12 mm millirad. Further, the laser source should have at least a 10% electrical optical efficiency, at least about 50% optical efficiency, at least about 70% optical efficiency, whereby it is understood that greater optical efficiency, all other factors being equal, is preferred, and preferably at least about 25%. The laser source can be run in either pulsed or continuous wave (CW) mode. The laser source is preferably capable of being fiber coupled.
For advancing boreholes in geologies containing hard rock formations such as granite and basalt it is preferred to use the IPG 20000 YB having the following specifications set forth in Table 1 herein.







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,


1.0
2.0
%



TWATER = Const














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.






For cutting casing, removal of plugs and perforation operations the laser may be any of the above referenced lasers, and it may further be any smaller lasers that would be only used for workover and completion downhole activities.
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.
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.
In use, one or more laser beams generated or illuminated by the one or more lasers may spall, vaporize or melt material, such as rock. The laser beam may be pulsed by one or a plurality of waveforms or it may be continuous. The laser beam may generally induce thermal stress in a rock formation due to characteristics of the material, such as rock including, for example, the thermal conductivity. The laser beam may also induce mechanical stress via superheated steam explosions of moisture in the subsurface of the rock formation. Mechanical stress may also be induced by thermal decompositions and sublimation of part of the in situ mineral of the material. Thermal and/or mechanical stress at or below a laser-material interface may promote spallation of the material, such as rock. Likewise, the laser may be used to effect well casings, cement or other bodies of material as desired. A laser beam may generally act on a surface at a location where the laser beam contacts the surface, which may be referred to as a region of laser illumination. The region of laser illumination may have any preselected shape and intensity distribution that is required to accomplish the desired outcome, the laser illumination region may also be referred to as a laser beam spot. Boreholes of any depth and/or diameter may be formed, such as by spalling multiple points or layers. Thus, by way of example, consecutive points may be targeted or a strategic pattern of points may be targeted to enhance laser/rock interaction. The position or orientation of the laser or laser beam may be moved or directed so as to intelligently act across a desired area such that the laser/material interactions are most efficient at causing rock removal.
One or more lasers may further be positioned downhole, i.e., down the borehole. Thus, depending upon the specific requirements and operation parameters, the laser may be located at any depth within the borehole. For example, the laser may be maintained relatively close to the surface, it may be positioned deep within the borehole, it may be maintained at a constant depth within the borehole or it may be positioned incrementally deeper as the borehole deepens. Thus, by way of further example, the laser may be maintained at a certain distance from the material, such as rock to be acted upon. When the laser is deployed downhole, the laser may generally be shaped and/or sized to fit in the borehole. Some lasers may be better suited than others for use downhole. For example, the size of some lasers may deem them unsuitable for use downhole, however, such lasers may be engineered or modified for use downhole. Similarly, the power or cooling of a laser may be modified for use downhole.
Systems and methods may generally include one or more features to protect the laser. This become important because of the harsh environments, both for surface units and downhole units. Thus, In accordance with one or more embodiments, a borehole drilling system may include a cooling system. The cooling system may generally function to cool the laser. For example, the cooling system may cool a downhole laser, for example to a temperature below the ambient temperature or to an operating temperature of the laser. Further, the laser may be cooled using sorption cooling to the operating temperature of the infrared diode laser, for example, about 20° C. to about 100° C. For a fiber laser its operating temperature may be between about 20° C. to about 50° C. A liquid at a lower temperature may be used for cooling when a temperature higher than the operating diode laser temperature is reached to cool the laser.
Heat may also be sent uphole, i.e., out of the borehole and to the surface, by a liquid heat transfer agent. The liquid transfer agent may then be cooled by mixing with a lower temperature liquid uphole. One or multiple heat spreading fans may be attached to the laser diode to spread heat away from the infrared diode laser. Fluids may also be used as a coolant, while an external coolant may also be used.
In downhole applications the laser may be protected from downhole pressure and environment by being encased in an appropriate material. Such materials may include steel, titanium, diamond, tungsten carbide and the like. The fiber head for an infrared diode laser or fiber laser may have an infrared transmissive window. Such transmissive windows may be made of a material that can withstand the downhole environment, while retaining transmissive qualities. One such material may be sapphire or other material with similar qualities. One or more infrared diode lasers or fiber lasers may be entirely encased by sapphire. By way of example, an infrared diode laser or fiber laser may be made of diamond, tungsten carbide, steel, and titanium other than the part where the laser beam is emitted.
In the downhole environment it is further provided by way of example that the infrared diode laser or fiber laser is not in contact with the borehole while drilling. For example, a downhole laser may be spaced from a wall of the borehole.
The Chiller.
The chiller, which is used to cool the laser, in the systems of the general type illustrated in FIG. 1 is chosen to have a cooling capacity dependent on the size of the laser, the efficiency of the laser, the operating temperature, and environmental location, and preferably the chiller will be selected to operate over the entirety of these parameters. Preferably, an example of a chiller that is useful for a 20 kW laser will have the following specifications set forth in Table 2 herein.








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)


Water flow 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









The Spool
For systems of the general type illustrated in FIG. 1, the laser beam is transmitted to the spool of coiled tubing by a laser beam transmission means. Such a transmittance means may be by a commercially available industrial hardened fiber optic cabling with QBH connectors at each end.
There are two basic spool approaches, the first is to use a spool which is simply a wheel with conduit coiled around the outside of the wheel. For example, this coiled conduit may be a hollow tube, it may be an optical fiber, it may be a bundle of optical fibers, it may be an armored optical fiber, it may be other types of optically transmitting cables or it may be a hollow tube that contains the aforementioned optically transmitting cables.
The spool in this configuration has a hollow central axis where the optical power is transmitted to the input end of the optical fiber. The beam will be launched down the center of the spool, the spool rides on precision bearings in either a horizontal or vertical orientation to prevent any tilt of the spool as the fiber is spooled out. It is optimal for the axis of the spool to maintain an angular tolerance of about +/−10 micro-radians, which is preferably obtained by having the optical axis isolated and/or independent from the spool axis of rotation. The beam when launched into the fiber is launched by a lens which is rotating with the fiber at the Fourier Transform plane of the launch lens, which is insensitive to movement in the position of the lens with respect the laser beam, but sensitive to the tilt of the incoming laser beam. The beam, which is launched in the fiber, is launched by a lens that is stationary with respect to the fiber at the Fourier Transform plane of the launch lens, which is insensitive to movement of the fiber with respect to the launch lens.
A second approach is to use a stationary spool similar to a creel and rotate the laser head as the fiber spools out to keep the fiber from twisting as it is extracted from the spool. If the fiber can be designed to accept a reasonable amount of twist along its length, then this would be the preferred method. Using the second approach if the fiber could be pre-twisted around the spool then as the fiber is extracted from the spool, the fiber straightens out and there is no need for the fiber and the drill head to be rotated as the fiber is played out. There will be a series of tensioners that will suspend the fiber down the hole, or if the hole is filled with water to extract the debris from the bottom of the hole, then the fiber can be encased in a buoyant casing that will support the weight of the fiber and its casing the entire length of the hole. In the situation where the bottom hole assembly does not rotate and the fiber is twisted and placed under twisting strain, there will be the further benefit of reducing SBS as taught herein.
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′′.
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.
The spool may have QBH fibers and a collimator. Vibration isolation means are desirable in the construction of the spool, and in particular for the fiber slip ring, thus for example the spool's outer plate mounts to the spool support using a Delrin plate, while the inner plate floats on the spool and pins rotate the assembly. The fiber slip ring is the stationary fiber, which communicates power across the rotating spool hub to the rotating fiber.
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.
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.
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.
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.
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.
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.
The Fluid
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.
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.
The Long Distance HPLB Transmission Means
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
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.
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.
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.
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.
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.
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.
Thus, by way of example there is provided the following configurations set forth in Table 3 herein.









TABLE 3






Diameter of bundle
Number of fibers in bundle








100 microns
1



200 microns-1 mm
2 to 100



100 microns-1 mm
1









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.
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.
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.
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.
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.
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.
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.
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.
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.
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.
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.
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.
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.
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.
Thus, there is provided in Tables 4 and 5 herein power transmissions for exemplary optical cable configurations.











TABLE 4





Power


# of fibers



in
Length of fiber(s)
Diameter of bundle
in bundle
Power 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-1 mm
2 to 100
15 kW


20 kW
7 km
200 microns-1 mm
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 5







(with active amplification)











Power


# of fibers



in
Length of fiber(s)
Diameter of bundle
in bundle
Power 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-1 mm
2 to 100
20 kW


20 kW
7 km
200 microns-1 mm
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









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.
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.
Downhole Monitoring Apparatus and Methods.
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.
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.
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.
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.
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.
The Bottom Hole Assembly.
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. 12/544,038, Ser. No. 12/544,094, and Ser. No. 12/543,968, 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.
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, galvanometers, 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.
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.
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.
The Mud Return and Handling System.
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.
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.
Example 1
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.










Experimental Setup
















Fiber Laser
IPG Photonics 5 kW ytterbium-doped



multi-clad fiber laser


Dolomite/Barre Granite
12′′ × 12′′ × 5′′ or and 5′′ × 5′′ × 5′′


Rock Size



Limestone
12′′ × 12′′ × 5′′ or and 5′′ × 5′′ × 5′′


Beam Spot Size (or
0.3585′′, 0.0625′′ (12.5 mm, 0.5 mm), 0.1′′,


diameter)



Exposure Times
0.05 s, 0.1 s, 0.2 s, 0.5 s, 1 s


Time-average Power
0.25 kW, 0.5 kW, 1.6 kW, 3 kW, 5 kW


Pulse
0.5 J/pulse to 20 J/pulse at 40 to 600 1/s









Example 2










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









Example 3
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.










Experimental Setup
















Fixed:



Fiber Laser
IPG Photonics 5 kW ytterbium-doped multi-clad



fiber laser


Dolomite/Barre
12′′ × 12′′ × 12′′ and 12′′ × 12′′ × 24′′


Granite



Rock Size



Limestone
12′′ × 12′′ × 12′′ and 12′′ × 12′′ × 24′′


Berea Gray
12′′ × 12′′ × 12′′ and 12′′ × 12′′ × 24′′


(or Yellow)



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 Limestone)


Beam Size
12.5 mm × 0.5 mm


Exposure Times
See Experiments 1 & 2


Purging
189 l/min Nitrogen Flow









Example 4
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.










Experimental Setup
















Fiber Laser
IPG Photonics 5 kW ytterbium-doped multi-



clad fiber laser


Dolomite/Barre Granite
5′′ × 5′′ × 5′′


Rock Size



Limestone
5′′ × 5′′ × 5′′


Berea Gray (or Yellow)
5′′ × 5′′ × 5′′


Sandstone



Shale
5′′ × 5′′ × 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
1891/min Nitrogen Flow


Distance between two
0.2′′, 0.5′′, 1′′, 1.5′′


laser beams









Example 5
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.










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









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.
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.
Drilling Plan Example 1
















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 3000 ft




inch casing





Drill 121⁄4 inch
3000 ft-8,000 ft
basalt
40 kW


hole


(minimum)


Run 95⁄8 inch
Length 8,000 ft




casing





Drill 81⁄2 inch
8,000 ft-11,000 ft
limestone
Conventional


hole


mechanical





drilling


Run 7 inch
Length 11,000 ft




casing





Drill 61⁄4 inch
11,000 ft-14,000 ft
Sand stone
Conventional


hole


mechanical





drilling


Run 5 inch
Length 3000 ft




liner









Drilling Plan Example 2
















Drilling





type/Laser





power down



Depth
Rock type
hole







Drill 171⁄2
Surface -
Sand and
Conventional


inch hole
500 ft
shale
mechanical





drilling


Run 133⁄8
Length 500 ft




casing





Drill 121⁄4 hole
500 ft-4,000 ft
granite
40 kW





(minimum)


Run 95⁄8 inch
Length 4,000 ft




casing





Drill 81⁄2 inch
4,000 ft-11,000 ft
basalt
20 kW


hole


(minimum)


Run 7 inch
Length 11,000 ft




casing





Drill 61⁄4 inch
11,000 ft-14,000 ft
Sand stone
Conventional


hole


mechanical





drilling


Run 5 inch
Length 3000 ft




liner









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.
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.
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.
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.
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.
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.
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.
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.
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, galvanometers, 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.
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.
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.
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.

## Claims

1. A system for providing high power laser energy to the bottom of deep boreholes, the system comprising:
a. a source for high powered laser energy capable of providing a high power laser beam having a power greater than about 1 kW;
b. an optical fiber for transmitting the laser beam from the high power laser to the bottom of a deep borehole; and,
c. the optical fiber having a means to suppress SBS arising from the transmission of the greater than about 1 kW laser beam;
d. whereby substantially all power of the high power laser beam is delivered to the bottom of the borehole.

2. The system of claim 1 wherein the deep borehole is at least 1,000 feet.

3. The system of claim 2 wherein the source is at least 10 kW.

4. The system of claim 1 wherein the deep borehole is at least 5,000 feet.

5. The system of claim 4 wherein the source is at least 10 kW.

6. The system of claim 1 wherein the deep borehole is at least 10,000 feet.

7. The system of claim 6 wherein the source is at least 10 kW.

8. A system for providing high power laser energy to the bottom of deep boreholes, the system comprising:
a. a high powered laser source capable of providing a high power laser beam having a power of at least about 10 kW;
b. a means for transmitting the laser beam from the high power laser source to the bottom of a deep borehole; and,
c. the transmitting means having a means for suppressing nonlinear scattering phenomena arising from the transmission of the laser beam having a power of at least about 10 kW; and,
d. whereby, the high power laser beam is delivered to the bottom of the borehole with sufficient power to form the borehole.

9. The system of claim 8 wherein the laser source comprises a single laser and the transmitting means having a length of at least about 3,000 feet.

10. The system of claim 8 wherein the laser source comprises two lasers and the transmitting means having a length of at least about 3,000 feet.

11. A method of advancing a borehole using a laser, the method comprising:
a. advancing a high power laser beam transmission fiber 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 fiber 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 fiber comprising a means for suppressing nonlinear scattering phenomena arising from the transmission of at least about a 1 kW laser beam within the transmission fiber;

b. providing a high power laser beam having a power of at least about 1 kW to the proximal end of the transmission fiber;
c. transmitting the power of the laser beam down the length of the transmission fiber 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.

12. A system for providing high power laser energy of 1 kW power or more over a long distance to a borehole, the system comprising:
a. a high powered laser source, capable of providing a high power laser beam, having at least about 1 kW of power;
b. a means for suppressing nonlinear scattering phenomena from the high power laser beam; and,
c. a means for transmitting the laser beam from the high power laser source to a location in the borehole;
d. whereby, the high power laser beam is delivered to the borehole.

13. The system of claim 12, wherein the nonlinear scattering phenomena is Stimulated Brillouin Scattering and the means for transmitting the laser beam has a length of at least about 1,000 feet.

14. The system of claim 13, wherein the means for suppressing comprises a means for spoiling the coherence of the Stimulated Brillouin Scattering.

15. The system of claim 13, wherein the means for suppressing comprises a means for varying a linewidth of the laser source, whereby a Brillouin gain factor is decreased.

16. The system of claim 13, wherein the means for suppressing comprises a means for increasing a Brillouin linewidth.

17. The system of claim 13, wherein the means for suppressing comprises a thin film heating element associated with the means for transmitting.

18. The system of claim 13, wherein the means for suppressing comprises a filter.

19. The system of claim 13, wherein the means for suppressing comprises a Faraday isolator.

20. The system of claim 13, wherein the means for suppressing comprises a Bragg Grating reflector.

21. The system of claim 12, wherein the nonlinear scattering phenomena is Stimulated Raman Scattering and the means for transmitting the laser beam has a length of at least about 1,000 feet.

22. The system of claim 12, wherein the means for suppressing comprises a means for spoiling the coherence of the nonlinear scattering phenomena and the means for transmitting the laser beam has a length of at least about 1,000 feet.

23. The system of claim 12, wherein the means for suppressing comprises a means for varying a linewidth of the laser source, whereby a Brillouin gain factor is decreased and the means for transmitting the laser beam has a length of at least about 1,000 feet.

24. The system of claim 12, wherein the means for suppressing comprises a means for increasing a Brillouin linewidth and the means for transmitting the laser beam has a length of at least about 1,000 feet.

25. The system of claim 12, wherein the means for suppressing comprises a means for suppressing Stimulated Brillouin Scattering and a means for suppressing Stimulated Raman Scattering.

26. The system of claim 12, wherein the high power laser source is a solid-state laser, capable of providing a high power laser beam characterized by a power of at least about 15 kW.

27. The system of claim 26, wherein the laser beam is characterized by a varying linewidth, wherein a gain function is suppressed, and whereby a nonlinear phenomena is suppressed.

28. The system of claim 27, wherein the nonlinear phenomena is Stimulated Brillouin Scattering.

29. The system of claim 12, wherein the high power laser source is a solid-state laser, capable of providing a high power laser beam characterized by a power of at least about 15 kW and a continuous wave mode.

30. The system of claim 29, wherein the laser source is characterized by a varying linewidth, wherein a gain function is suppressed, and whereby a nonlinear phenomena is suppressed.

31. The system of claim 30, wherein the nonlinear phenomena is Stimulated Brillouin Scattering.

32. The system of claim 12, wherein the high power laser source is a solid-state laser, capable of providing a high power laser beam characterized by a power of at least about 20 kW and a continuous wave mode and the means for transmitting the laser beam has a length of at least about 1,000 feet.

33. The system of claim 32, wherein the laser beam is characterized by a varying linewidth, wherein a gain function is suppressed, and whereby a nonlinear phenomena is suppressed.

34. The system of claim 33, wherein the nonlinear phenomena is Stimulated Brillouin Scattering.

35. The system of claim 12, wherein the high power laser source is a solid-state laser, capable of providing a high power laser beam characterized by a power of at least about 50 kW and a continuous wave mode and the means for transmitting the laser beam has a length of at least about 3,000 feet.

36. The system of claim 35, wherein the laser beam is characterized by a varying linewidth, wherein a gain function is suppressed, and whereby a nonlinear phenomena is suppressed.

37. The system of claim 36, wherein the nonlinear phenomena is Stimulated Brillouin Scattering.

38. The system of claim 37, wherein the high power laser source is a low order mode source.

39. The system of claim 37, wherein the high power laser source is a low order mode source characterized by an M2<2.

40. The system of claim 12, wherein the high power laser source is a solid-state laser, capable of providing a high power laser beam characterized by a power of at least about 15 kW and a pulsed mode.

41. The system of claim 40, wherein the laser beam is characterized by a varying linewidth, wherein a gain function is suppressed, and whereby a nonlinear phenomena is suppressed.

42. The system of claim 41, wherein the nonlinear phenomena is Stimulated Brillouin Scattering.

43. The system of claim 12, wherein the high power laser source comprises a combination of a plurality of laser sources, wherein each laser source of the combination is capable of providing a high power laser beam characterized by a power of at least about 15 kW and a linewidth, wherein the means for suppressing comprises a combination of the laser beams from the plurality of laser sources, and a combined laser beam characterized by an effective linewidth greater than the linewidth of a laser beam from a laser source from the plurality of laser sources.

44. The system of claim 43, wherein a laser source from the plurality of laser sources is characterized by a continuous wave mode.

45. The system of claim 43, wherein a laser source from the plurality of laser sources is characterized by a pulsed mode.

46. The system of claim 43, wherein a laser source from the plurality of laser sources is a solid-state laser.

47. The system of claim 43, wherein a laser source from the combination of a plurality of laser sources is a low order mode source.

48. The system of claim 43, wherein a laser source from the combination of a plurality of laser sources is a low order mode source characterized by an M2<2.

49. The system of claim 43, wherein the means for transmitting comprises an optical fiber and an armored casing.

50. The system of claim 49, wherein the armored casing comprises a metal tube having a diameter of about 1⁄4′′, and the fiber having a core having a diameter of at least about 500 microns.

51. The system of claim 43, wherein the means for transmitting has a means for break detection.

52. The system of claim 43, wherein the means for transmitting comprises a plurality of optical fibers.

53. The system of claim 43, wherein the means for transmitting comprises an optical fiber, the optical fiber having a core having a core diameter of at least about 100 microns, a first protective member and a second protective member, wherein the protective members are selected from the group consisting of a steel tube, a polymer coating, a Teflon coating, a polyimide, an acrylate, a carbon polyamide, and a carbon coating.

54. The system of claim 43, wherein the means for transmitting comprises a single mode optical fiber.

55. The system of claim 43, wherein the means for transmitting comprises a multimode optical fiber.

56. The system of claim 12, wherein the high power laser source comprises a combination of a plurality of solid-state laser sources, wherein each laser source of the combination is capable of providing a high power laser beam characterized by a power of at least about 20 kW and a linewidth, wherein the means for suppressing comprises a combination of the laser beams from the plurality of laser sources, and a combined laser beam characterized by an effective linewidth greater than the linewidth of a laser beam from a laser source from the plurality of laser sources.

57. The system of claim 12, wherein the high power laser source comprises a combination of a plurality of laser sources, wherein each laser source of the combination is capable of providing a high power laser beam characterized by a linewidth; wherein the means for suppressing comprises a combination of the laser beams from the plurality of laser sources, and a combined laser beam characterized by an effective linewidth greater than the linewidth of a laser beam from a laser source from the plurality of laser sources; and wherein the combined beam is characterized by having a power of at least about 40 kW.

58. The system of claim 57, wherein a laser source from the plurality of laser sources is a solid-state laser.

59. The system of claim 58, wherein the solid state laser is a low order mode source.

60. The system of claim 58, wherein the solid state laser a low order mode source characterized by an M2<2.

61. The system of claim 58, wherein the solid state laser is a bandwidth broadened laser source.

62. The system of claim 57, wherein each laser source from the plurality of laser sources is a solid-state laser.

63. The system of claim 12, wherein the means for suppressing comprises a thin film heating element associated with the means for transmitting and the means for transmitting the laser beam has a length of at least about 2,000 feet.

64. The system of claim 12, wherein the means for suppressing comprises a filter.

65. The system of claim 12, wherein the means for suppressing comprises a Faraday isolator.

66. The system of claim 12, wherein the means for suppressing comprises a Bragg Grating reflector and the means for transmitting the laser beam has a length of at least about 1,000 feet.

67. The system of claim 12, wherein the high power laser source comprises a combination of a plurality of laser sources capable of providing a combined high power laser beam characterized by a combined wavelength having a wavelength range; wherein each laser source from the plurality of laser sources is capable of providing a high power laser beam characterized by a source wavelength, having a source wavelength range, wherein a source wavelength is a different wavelength from another source wavelength; and wherein the means for suppressing comprises the combined wavelength range being broader than a source wavelength range and the means for transmitting the laser beam has a length of at least about 1.000 feet.

68. The system of claim 12, wherein the high power laser source comprises a combination of a plurality of laser sources capable of providing a combined high power laser beam characterized by a combined wavelength having a wavelength range; wherein each laser source from the plurality of laser sources is capable of providing a high power laser beam characterized by a source wavelength, having a source wavelength range; and wherein the means for suppressing comprises the combined wavelength range being broader than a source wavelength and the means for transmitting the laser beam has a length of at least about 1,000 feet.

69. The system of claim 68, wherein the means for transmitting comprises an optical fiber and an armored casing.

70. The system of claim 69, wherein the armored casing comprises a metal tube having a diameter of about 1⁄4′′, and the fiber having a core having a diameter of at least about 500 microns.

71. The system of claim 68, wherein the means for transmitting has a means for break detection.

72. The system of claim 68, wherein the means for transmitting comprises a plurality of optical fibers.

73. The system of claim 68, wherein the means for transmitting comprises an optical fiber, the optical fiber having a core having a core diameter of at least about 100 microns, a first protective member and a second protective member, wherein the protective members are selected from the group consisting of a steel tube, a polymer coating, a Teflon coating, a polyimide, an acrylate, a carbon polyamide, and a carbon coating.

74. The system of claim 68, wherein the means for transmitting comprises a single mode optical fiber.

75. The system of claim 68, wherein the means for transmitting comprises a multimode optical fiber.

76. The system of claim 12, wherein the high power laser source is a low order mode source.

77. The system of claim 12, wherein the high power laser source is a low order mode source characterized by an M2<2.

78. The system of claim 12, wherein the laser source is a bandwidth broadened laser source.

79. The system of claim 12, wherein the means for transmitting comprises an optical fiber and an armored casing.

80. The system of claim 79, wherein the armored casing comprises a metal tube having a diameter of about 1⁄4′′, and the fiber having a core having a diameter of at least about 500 microns.

81. The system of claim 79, wherein the armored casing comprises a metal tube having a diameter of about 1⁄4′′, and the fiber having a core having a diameter of at least about 500 microns.

82. The system of claim 12, wherein the means for transmitting has a means for break detection.

83. The system of claim 12, wherein the means for transmitting comprises a plurality of optical fibers.

84. The system of claim 12, wherein the means for transmitting comprises an optical fiber, the optical fiber having a core having a core diameter of at least about 100 microns, a first protective member and a second protective member, wherein the protective members are selected from the group consisting of a steel tube, a polymer coating, a Teflon coating, a polyimide, an acrylate, a carbon polyamide, and a carbon coating.

85. The system of claim 12, wherein the means for transmitting comprises a single mode optical fiber.

86. The system of claim 12, wherein the means for transmitting comprises a multimode optical fiber.

87. The system of claim 12, wherein the laser source has a linewidth of from 3 nm to 6 nm.

88. The system of claim 12, wherein the means for transmitting comprises an optical fiber and an armored casing.

89. The system of claim 12, wherein the high power laser source comprises a combination of a plurality of laser sources, wherein each laser source of the combination is capable of providing a high power laser beam characterized by a power of at least about 1 kW and a linewidth, wherein the means for suppressing comprises a combination of the laser beams from the plurality of laser sources, and a combined laser beam characterized by an effective linewidth greater than the linewidth of a laser beam from a laser source from the plurality of laser sources; and wherein the means for transmitting comprises an optical fiber and an armored casing.

90. The system of claim 12, wherein the high power laser source comprises a combination of a plurality of laser sources, wherein each laser source of the combination is capable of providing a high power laser beam characterized by a power of at least about 1 kW and a linewidth, wherein the means for suppressing comprises a combination of the laser beams from the plurality of laser sources, and a combined laser beam characterized by an effective linewidth greater than the linewidth of a laser beam from a laser source from the plurality of laser sources; wherein the means for transmitting comprises an optical fiber and an armored casing;
and wherein the armored casing comprises a metal tube, and the fiber having a core having a diameter of at least about 500 microns.

91. The system of claim 12, wherein the high power laser source comprises a combination of a plurality of laser sources, wherein each laser source of the combination is capable of providing a high power laser beam characterized by a power of at least about 1 kW and a linewidth, wherein the means for suppressing comprises a combination of the laser beams from the plurality of laser sources, and a combined laser beam characterized by an effective linewidth greater than the linewidth of a laser beam from a laser source from the plurality of laser sources; and wherein the means for transmitting has a means for break detection.

92. The system of claim 12, wherein the high power laser source comprises a combination of a plurality of laser sources, wherein each laser source of the combination is capable of providing a high power laser beam characterized by a power of at least about 1 kW and a linewidth, wherein the means for suppressing comprises a combination of the laser beams from the plurality of laser sources, and a combined laser beam characterized by an effective linewidth greater than the linewidth of a laser beam from a laser source from the plurality of laser sources; and wherein the means for transmitting comprises an optical fiber, the optical fiber having a core having a core diameter of at least about 100 microns, a first protective member and a second protective member, wherein the protective members are selected from the group consisting of a steel tube, a polymer coating, a Teflon coating, a polyimide, an acrylate, a carbon polyamide, and a carbon coating.

93. The system of claim 12, wherein the means for suppressing comprises having different temperatures along a length of the means for transmission.

94. The system of claim 12, wherein the means for suppressing comprises the means for transmission comprising an optical fiber and a means for providing a strain in the optical fiber.

95. The system of claim 12, wherein the means for suppressing comprises an acoustic generator.

96. The system of claim 12, wherein the nonlinear scattering phenomena is Stimulated Brillouin Scattering, the means for suppressing nonlinear scattering phenomena comprises a laser beam having a broad laser linewidth and a laser power; wherein the broad laser linewidth and the laser power in combination with the means for transmitting prevent the onset of Stimulated Brillouin Scattering.

97. The system of claim 12, wherein the nonlinear scattering phenomena is Stimulated Brillouin Scattering, the means for suppressing nonlinear scattering phenomena comprises a laser beam having a broad laser linewidth and a laser power; wherein the broad laser linewidth and the laser power in combination with the means for transmitting reduces Stimulated Brillouin Scattering.

98. A system for providing high power laser energy to a borehole, the system comprising:
a. a high powered laser, capable of providing a high power laser beam having at least about 1 kW of power;
b. a first means for suppressing nonlinear scattering phenomena arising from the transmission of the high power laser beam, in association with the high powered laser;
c. a means for transmitting the laser beam from the high power laser to a position in the borehole; and,
d. a second means for suppressing nonlinear scattering phenomena arising from the transmission of the high power laser beam, in association with the means for transmitting;
e. whereby, the high power laser energy is delivered to the borehole.

99. The system of claim 98, wherein the first means nonlinear scattering phenomena is Stimulated Brillouin Scattering.

100. The system of claim 98, wherein the second means nonlinear scattering phenomena is Stimulated Raman Scattering.

101. The system of claim 98, wherein the first or second means for suppressing comprises a means for spoiling the coherence of the nonlinear scattering phenomena.

102. The system of claim 98, wherein the high power laser is a solid-state laser, capable of providing a high power laser beam characterized by a power of at least about 15 kW and a continuous wave mode.

103. The system of claim 102, wherein the first means for suppression comprises a varying linewidth, wherein a gain function is suppressed, and whereby a nonlinear phenomena is suppressed.

104. The system of claim 103, wherein the first means nonlinear phenomena is Stimulated Brillouin Scattering.

105. The system of claim 98, wherein the high power laser source comprises a combination of a plurality of laser sources capable of providing a combined high power laser beam characterized by a combined wavelength having a wavelength range; wherein each laser source from the plurality of laser sources is capable of providing a high power laser beam characterized by a source wavelength, having a source wavelength range, wherein a source wavelength is a different wavelength from another source wavelength; and wherein the first means for suppressing comprises the combined wavelength range being broader than a source wavelength range.

106. The system of claim 98, wherein the high power laser source comprises a combination of a plurality of laser sources capable of providing a combined high power laser beam characterized by a combined wavelength having a wavelength range; wherein each laser source from the plurality of laser sources is capable of providing a high power laser beam characterized by a source wavelength, having a source wavelength range; and wherein the first means for suppressing comprises the combined wavelength range being broader than a source wavelength.

107. The system of claim 98, wherein the high power laser source comprises a combination of a plurality of laser sources, wherein each laser source of the combination is capable of providing a high power laser beam characterized by a linewidth; wherein the first means for suppressing comprises a combination of the laser beams from the plurality of laser sources, and a combined laser beam characterized by an effective linewidth greater than the linewidth of a laser beam from a laser source from the plurality of laser sources; and wherein the combined beam is characterized by having a power of at least about 40 kW.

108. The system of claim 107, wherein a laser source from the plurality of laser sources is a solid-state laser.

109. The system of claim 107, wherein each laser source from the plurality of laser sources is a solid-state laser.

110. The system of claim 98, wherein the first and the second nonlinear scattering phenomena are Stimulated Brillouin Scattering, the first and second means for suppressing nonlinear scattering phenomena comprises the laser beam having a broad laser linewidth and a laser power; wherein the broad laser linewidth and the laser power in combination with the means for transmitting prevent the onset of Stimulated Brillouin Scattering.

111. The system of claim 98, wherein the first and the second nonlinear scattering phenomena are Stimulated Brillouin Scattering, the first and second means for suppressing nonlinear scattering phenomena comprises the laser beam having a broad laser linewidth and a laser power; wherein the broad laser linewidth and the laser power in combination with the means for transmitting reduces Stimulated Brillouin Scattering.

112. A system for providing high power laser energy to a borehole, the system comprising:
a. a source of high power laser energy, the laser source capable of providing a laser beam having at least about 20 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 a fluid for use in the borehole;
d. the proximal end of the tubing being in fluid communication with the source of fluid;
e. the proximal end of the tubing being in optical communication with the laser source;
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;
g. a means for suppressing nonlinear scattering phenomena from the laser beam in associations with at least one of elements a, b, e, or f; and,
h. the power of the laser energy at the distal end of the cable when the cable is within the borehole being at least about 5 kW.

113. The system of claim 112, wherein the high power laser source comprises a combination of a plurality of laser sources, wherein each laser source of the combination is capable of providing a high power laser beam characterized by a linewidth; wherein the means for suppressing comprises a combination of the laser beams from the plurality of laser sources, and a combined laser beam characterized by an effective linewidth greater than the linewidth of a laser beam from a laser source from the plurality of laser sources; and wherein the combined beam is characterized by having a power of at least about 40 kW.

114. The system of claim 113, wherein a laser source from the plurality of laser sources is a solid-state laser.

115. The system of claim 113, wherein each laser source from the plurality of laser sources is a solid-state laser.

116. The system of claim 112, wherein the laser source has a linewidth of from 3 nm to 6 nm.

117. A method of providing high power laser energy to a borehole, the method comprising:
a. advancing a high power laser beam transmission fiber into a borehole having a depth of at least about 1,000 feet, the transmission fiber comprising a distal end, a proximal end, and a length extending between the distal and proximal ends, wherein the distal end is advanced into the borehole;
b. propagating a high power laser beam, having a power of at least about 1 kW, into the proximal end of the transmission fiber;
c. transmitting the laser beam down the length of the transmission fiber so that the beam exits the distal end;
d. a step for suppressing nonlinear scattering phenomena arising from the transmission of the high power laser beam; and,
e. directing the laser beam to a surface in the borehole.

118. The method of claim 117, wherein the nonlinear scattering phenomena is Stimulated Brillouin Scattering.

119. The method of claim 118, wherein the step for suppressing comprises spoiling the coherence of the Stimulated Brillouin Scattering.

120. The method of claim 118, wherein the step for suppressing comprises increasing a Brillouin linewidth.

121. The method of claim 117, wherein the nonlinear scattering phenomena is Stimulated Raman Scattering.

122. The method of claim 117, wherein the step for suppressing comprises spoiling the coherence of the nonlinear scattering phenomena.

123. The method of claim 117, wherein the step for suppressing comprises varying a linewidth of the laser source, and decreasing a Brillouin gain factor.

124. The method of claim 117, wherein the step for suppressing comprises suppressing Stimulated Brillouin Scattering and suppressing Stimulated Raman Scattering.

125. The method of claim 117, wherein the high power laser source is a solid-state laser, and the high power laser beam has a power of at least about 15 kW and a linewidth.

126. The method of claim 125, comprising varying the linewidth, suppressing a gain function, whereby a nonlinear phenomena is suppressed.

127. The method of claim 126, wherein the nonlinear phenomena is Stimulated Brillouin Scattering.

128. The method of claim 117, wherein the high power laser source is a solid-state laser, and the high power laser beam has a power of at least about 15 kW, and is propagated as a continuous wave.

129. The method of claim 128, wherein the nonlinear phenomena is Stimulated Brillouin Scattering.

130. The method of claim 117, wherein the high power laser source comprises a combination of a plurality of solid-state laser sources, wherein each source from the plurality of sources provides a high power laser beam having a power of at least about 15 kW and a linewidth, wherein the step for suppressing comprises combining the laser beams from the plurality of sources to provide a combined laser beam having an effective linewidth greater than the linewidth of a source from the plurality of sources.

131. The method of claim 117, wherein the transmission fiber has a means for break detection.

132. The method of claim 117, wherein the transmission fiber comprises a plurality of optical fibers.

133. The method of claim 117, wherein the transmission fiber comprises an optical fiber, the optical fiber having a core having a core diameter of at least about 100 microns, a first protective member and a second protective member, wherein the protective members are selected from the group consisting of a steel tube, a polymer coating, a Teflon coating, a polyimide, an acrylate, a carbon polyamide, and a carbon coating.

134. The method of claim 117, wherein the transmission fiber comprises a single mode optical fiber.

135. The method of claim 117, wherein the transmission fiber comprises a multimode optical fiber.

136. A method for providing high power laser energy to a borehole, the method comprising:
a. associating a high power optical fiber with a borehole;
b. propagating a high powered laser beam, having a power of at least about 5 kW, from a high power laser source into the high power optical fiber;
c. transmitting the laser beam through the high power optical fiber to a location associated with the borehole; and,
d. a step for suppressing nonlinear scattering phenomena arising from the transmission of the high powered laser beam.

137. The method of claim 136, wherein the nonlinear scattering phenomena is Stimulated Brillouin Scattering, wherein the borehole has a depth of at least about 1,000 feet and a location associated with the borehole is at a depth of at least about 1,000 feet.

138. The method of claim 137, wherein the step for suppressing comprises spoiling the coherence of the Stimulated Brillouin Scattering.

139. The method of claim 137, wherein the step for suppressing comprises varying a linewidth of the laser source, whereby a Brillouin gain factor is decreased.

140. The method of claim 137, wherein the step for suppressing comprises increasing a Brillouin linewidth.

141. The method of claim 137, wherein the step for suppressing comprises providing heat to the optical fiber from a heating element associated with the optical fiber.

142. The method of claim 137, wherein the step for suppressing comprises a filtering.

143. The method of claim 137, wherein the step for suppressing comprises propagating the laser beam through a Faraday isolator.

144. The method of claim 137, wherein the step for suppressing comprises propagating the laser beam through a Bragg Grating reflector.

145. The method of claim 136, wherein the nonlinear scattering phenomena is Stimulated Raman Scattering, wherein the borehole has a depth of at least about 1,000 feet and a location associated with the borehole is at a depth of at least about 1,000 feet.

146. The method of claim 136, wherein the step for suppressing comprises spoiling the coherence of the nonlinear scattering phenomena, wherein the borehole has a depth of at least about 1,000 feet and a location associated with the borehole is at a depth of at least about 1,000 feet.

147. The method of claim 136, wherein the step for suppressing comprises varying a linewidth of the laser source, whereby a Brillouin gain factor is decreased.

148. The method of claim 136, wherein the step for suppressing comprises increasing a Brillouin linewidth.

149. The method of claim 136, wherein the step for suppressing comprises suppressing Stimulated Brillouin Scattering and suppressing Stimulated Raman Scattering, wherein the borehole has a depth of at least about 1,000 feet and a location associated with the borehole is at a depth of at least about 1,000 feet.

150. The method of claim 136, wherein the high power laser source is a solid-state laser, and the high power laser beam has a power of at least about 15 kW and a linewidth, wherein the borehole has a depth of at least about 1,000 feet and a location associated with the borehole is at a depth of at least about 1,000 feet.

151. The method of claim 150, comprising varying the linewidth, suppressing a gain function, and whereby a nonlinear phenomena is suppressed.

152. The method of claim 151, wherein the nonlinear phenomena is Stimulated Brillouin Scattering.

153. The method of claim 136, wherein the high power laser source is a solid-state laser, and the high power laser beam has a power of at least about 15 kW, and is propagated as a continuous wave and has a linewidth, wherein the borehole has a depth of at least about 1,000 feet and a location associated with the borehole is at a depth of at least about 1,000 feet.

154. The method of claim 153, wherein the step for suppressing comprises varying the linewidth, suppressing a gain function, and whereby a nonlinear phenomena is suppressed.

155. The method of claim 154, wherein the nonlinear phenomena is Stimulated Brillouin Scattering.

156. The method of claim 136, wherein the high power laser source is a solid-state laser, and the high power laser beam has a power of at least about 15 kW, and is propagated in a pulsed mode, wherein the borehole has a depth of at least about 1,000 feet and a location associated with the borehole is at a depth of at least about 1,000 feet.

157. The method of claim 136, wherein the high power laser source comprises a combination of a plurality of solid-state laser sources, wherein each laser source from the plurality of sources provides a high power laser beam having a power of at least about 15 kW and a linewidth, wherein the step for suppressing comprises combining the laser beams from the plurality of sources to provide a combined laser beam into the fiber, the combined laser beam having an effective linewidth greater than the linewidth of a source from the plurality of sources, wherein the borehole has a depth of at least about 1,000 feet and a location associated with the borehole is at a depth of at least about 1,000 feet.

158. The method of claim 157, wherein the combined laser beam has an effective linewidth greater than the linewidth of each source from the plurality of sources.

159. The method of claim 157, wherein a laser beam from a source of the plurality of sources is propagated in a continuous wave mode.

160. The method of claim 157, wherein a laser beam from a source of the plurality of sources is propagated in a pulsed mode.

161. The method of claim 136, wherein the high power laser source comprises a combination of a plurality of laser sources, wherein each laser source from the plurality of sources is capable of providing a high power laser beam characterized by a power of at least about 20 kW and a linewidth, wherein the step for suppressing comprises combining the laser beams from the plurality of sources to provide a combined laser beam having an effective linewidth broader than the linewidth of a laser beam for a source from the plurality of sources, wherein the borehole has a depth of at least about 1,000 feet and a location associated with the borehole is at a depth of at least about 1,000 feet.

162. The method of claim 161, wherein a laser source from the plurality of laser sources is a solid-state laser.

163. The method of claim 162, wherein a laser source from the plurality of laser sources is a fiber laser.

164. The method of claim 162, wherein each of the laser sources from the plurality of laser sources is a solid state laser.

165. The method of claim 161, wherein the combined laser beam has an effective linewidth broader than the linewidth of each laser beam from each laser source from the plurality of sources.

166. The method of claim 136, wherein the high power laser source comprises a combination of a plurality of solid-state laser sources, wherein each laser source of the combination is capable of providing a high power laser beam characterized by a linewidth, wherein the step for suppressing comprises combining the laser beams from each source of the combination to provide a combined laser beam having an effective linewidth greater than the linewidth of each source of the combination; and wherein the combined beam is characterized by having a power of at least about 40 kW, wherein the borehole has a depth of at least about 1,000 feet and a location associated with the borehole is at a depth of at least about 1,000 feet.

167. The method of claim 136, wherein the step for suppressing comprises providing heat to the optical fiber from a thin film heating element associated with the optical fiber, wherein the borehole has a depth of at least about 1,000 feet and a location associated with the borehole is at a depth of at least about 1,000 feet.

168. The method of claim 136, wherein the step for suppressing comprises filtering, wherein the borehole has a depth of at least about 1,000 feet and a location associated with the borehole is at a depth of at least about 1,000 feet.

169. The method of claim 136, wherein the step for suppressing comprises propagating the laser beam through a Faraday isolator, wherein the borehole has a depth of at least about 1,000 feet and a location associated with the borehole is at a depth of at least about 1,000 feet.

170. The method of claim 136, wherein the step for suppressing comprises propagating the laser beam through a Bragg Grating reflector, wherein the borehole has a depth of at least about 1,000 feet and a location associated with the borehole is at a depth of at least about 1,000 feet.

171. The method of claim 136, wherein the high power laser source comprises a combination of a plurality of laser sources, wherein each source from the plurality of sources provides a high power laser beam characterized by a source linewidth; wherein the step for suppressing comprises combining the laser beams from the plurality of sources to provide a combined laser beam having a combined linewidth greater than a source linewidth; and wherein the combined beam is characterized by having a power of at least about 40 kW, wherein the borehole has a depth of at least about 1,000 feet and a location associated with the borehole is at a depth of at least about 1,000 feet.

172. The method of claim 136, wherein the high power laser source comprises a combination of a plurality of laser sources capable of providing a high power laser beam characterized by a combined wavelength, having a combined wavelength range, wherein each laser source of the combination is capable of providing a high power laser beam characterized by a source wavelength, having a source wavelength range;
wherein each source wavelength is different from the others; and wherein the step for suppressing comprises combining the laser beams into a combined beam having a combined wavelength range greater than a source wavelength range, wherein the borehole has a depth of at least about 1,000 feet and a location associated with the borehole is at a depth of at least about 1,000 feet.

173. The method of claim 136, wherein the step for suppressing nonlinear scattering phenomena comprises the laser beam having a broad laser linewidth and a laser power; wherein the broad laser linewidth and the laser power in combination with the optical fiber substantially prevents the onset of Stimulated Brillouin Scattering.

174. A system for providing high power laser energy over a long distance to a borehole, the system comprising:
a. a high powered laser source, capable of providing a high power combined laser beam, the high power laser source comprising a combination of a plurality of laser sources, wherein each laser source of the combination is capable of providing a high power laser beam characterized by a power of at least about 1 kW and a linewidth;
b. a means for suppressing nonlinear scattering phenomena arising from transmission of the high power laser beam, comprising the high power combined laser beam characterized by an effective linewidth greater than the linewidth of a laser beam from a laser source from the plurality of laser sources; and,
c. a means for transmitting the laser beam from the high power laser source to a location in the borehole;
d. whereby, the high power combined laser beam is delivered within the borehole and, whereby the combined laser beam has a power of at least about 15 kW.

175. A method for providing high power laser energy to a borehole, the method comprising:
a. associating a high power optical fiber with a borehole;
b. propagating a high powered laser beam, having a power of at least about 1 kW, from a high power laser source into the high power optical fiber;
c. transmitting the laser beam through the high power optical fiber to a location associated with the borehole; and,
d. suppressing a nonlinear scattering phenomena arising from the transmission of the high powered laser beam.

176. The method of claim 175, wherein the nonlinear scattering phenomena is Stimulated Brillouin Scattering.

177. The method of claim 175, wherein the nonlinear scattering phenomena is Stimulated Raman Scattering.

178. The method of claim 175, wherein the step for suppressing comprises spoiling the coherence of the nonlinear scattering phenomena.

179. A system for providing high power laser energy, having at least about 1 kW of power, over a long distance to a borehole, the system comprising:
a. a high powered laser source, capable of providing a high power laser beam having a power of at least about 1 kW and characterized by a linewidth;
b. a means for transmitting the laser beam from the high power laser source to a location in the borehole comprising an optical fiber; and,
c. a means for suppressing nonlinear scattering phenomena arising from the transmission of the high power laser beam, comprising a broad laser beam linewidth and a large diameter fiber core, whereby the linewidth in combination with the fiber prevent a Stimulated Brillouin Scattering threshold from being reached.