Patent Grant
9545692
The present inventions relate to methods, apparatus and systems for the delivery of high power laser beams over a distance to a work surface to perform a laser operation on the work surface, such as, treating, fracturing, tunneling, weakening, welding, annealing, cutting, removing, drilling, penetrating, and combinations and variations of these. The work surfaces, for example, may be roads, the earth, bridge supports, dams, meat, animal and human tissue, food products, ice, rocks, rock faces, pipes, conduit, tubes, columns, wire, cables, girders, beams, buildings, concrete, reinforced concrete, rebar, metal, coal, ore, shale, tar sands, mineral containing materials, steel, tanks, and support structures.
As used herein the term “earth” should be given its broadest possible meaning, and includes, 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, tar sands, dolomite, sand, salt, limestone, ores, minerals, overburden, marble, rhyolite, quartzite and shale rock.
As used herein, unless specified otherwise, the terms “borehole,” “tunnel,” “shaft” and similar such terms should be given their broadest possible meaning and include any opening that is created in the earth, in a structure (e.g., building, protected military installation, nuclear plant, or ship), in a work surface, or in a structure in the ground, (e.g., foundation, roadway, airstrip, cave or subterranean structure) that is substantially longer than it is wide, such as a well, a tunnel, a hole, a well bore, a mine shaft, a well hole, a micro hole, slimhole and other terms commonly used or known in the arts to define these types of narrow long passages. Boreholes may further have segments or sections that have different orientations, they may have straight sections and arcuate sections and combinations thereof; and for example may be of the shapes commonly found when directional drilling is employed or when mining tunnels follow ore deposits. Thus, as used herein unless expressly provided otherwise, the terms “bottom”, “bottom surface” or “end,” and similar such terms, when used in relation to a borehole, tunnel or shaft, refer to the end of the borehole, tunnel or shaft, i.e., that portion that is farthest along the path from the opening, start, the surface of the earth, or the beginning.
As used herein, unless specified otherwise, the terms, “cut,” “cutting,” “sectioning” and similar such terms should be given their broadest possible meaning, and include the remove of material in a pattern that is longer than it is wide, which would include a pattern that is linear, substantially linear, curved, annular, geometric (such as a rectangle, square, trapezoid, etc.) or non-geometric (such as a trace of a natural structure like an ore seam, or other pattern that does not have a common geometric name). A cut may be continuous, such that the material is removed by the laser along the entirely of the pattern, or it may be staggered or partial, which could be viewed as a series of lands (where no material is removed) and cuts (where material is removed), stitches, perforations, spaced holes, etc. The use of the term “completed” cut, and similar such terms, includes severing a material into two sections, i.e., a cut that is all the way through the material, or removing sufficient material to meet the intended objective of the cut. A borehole, a tunnel, a hole, an opening, or any volumetric shape of removed material, may be made using cuts placed adjacent, or substantially adjacent one an another, as for example by delivering the laser beam in a raster scan pattern.
As used herein, unless specified otherwise “high power laser energy” means a laser beam having at least about 1 kW (kilowatt) of power. As used herein, unless specified otherwise “great distances” means at least about 500 m (meter). As used herein the term “substantial loss of power,” “substantial power loss” and similar such phrases, mean a loss of power of more than about 3.0 dB/km (decibel/kilometer) for a selected wavelength. As used herein the term “substantial power transmission” means at least about 50% transmittance.
There has been a long standing need for the delivery of high power laser beams over distances, and in particular through free space, to laser process materials. The present inventions, among other things, solve these and other needs by providing the articles of manufacture, devices and processes taught herein.
Thus, there is provided a method of shaped volumetric removal from a material using high power directed energy, by: applying high power directed energy having a power sufficient to penetrate the material in a predetermined three dimensional pattern, corresponding to a predetermined volumetric shape; removing the material along the three dimensional pattern; weakening material adjacent to the pattern, thereby creating directed energy affected areas of the material; the directed energy affected areas substantially occupying the predetermined volumetric shape; and, removing the material from the predetermined volumetric shape.
There is further provided methods of these shaped volumetric removals of materials in which one or more of the following may also be practiced: wherein the three dimensional pattern has a line; wherein the line forms a spiral; wherein the three dimensional pattern has a length, a width and a depth, and the depth is at least about 10 feet; wherein the three dimensional pattern has a plurality of lines; wherein at least two of the plurality of lines is interconnected; wherein the volumetric shape corresponds to a mineral deposit; wherein the depth of penetration is self-limiting; wherein the volumetric shape is a cube; wherein the volumetric shape is a cylinder; wherein the directed energy is a high power laser beam having at least about 1 kW of power; wherein the directed energy is a high power laser beam having at least about 1 kW of power; wherein the directed energy is a high power laser beam having at least about 1 kW of power; wherein the directed energy is a high power laser beam having at least about 1 kW of power; wherein the directed energy is a high power laser beam having at least about 10 kW of power; wherein the directed energy is a high power laser beam having at least about 10 kW of power; wherein the directed energy is a high power laser beam having at least about 10 kW of power; wherein the directed energy is a high power laser beam having at least about 10 kW of power; wherein the directed energy is a high power laser beam having at least about 50 kW of power; wherein the directed energy is a high power laser beam having at least about 60 kW of power; wherein the directed energy is a high power laser beam having at least about 80 kW of power.
Additionally there is provided a method of shaped volumetric removal from a material using high power laser energy, the method having the following steps: directing a high power laser beam having a power sufficient to penetrate the material in a predetermined three dimensional pattern, corresponding to a predetermined volumetric shape; removing the material along the three dimensional pattern; creating laser affected areas of material adjacent to the pattern; the laser affected areas substantially filling the predetermined volumetric shape; and, removing the material from the predetermined volumetric shape.
There is further provided methods of these shaped volumetric removals of materials in which one or more of the following may also be practiced: wherein the laser beam is a CW beam; wherein the laser beam is a pulsed beam; wherein the power is at least about 10 kW; wherein the power is at least about 20 kW; wherein the laser beam is applied from a high power laser cutting tool positioned at a stand off distance from a surface of the material; wherein the stand off distance is at least about 3 ft; wherein the stand off distance is at least about 10 ft; wherein the stand off distance is at least about 20 ft; wherein the stand off distance is at least about 30 ft; wherein the laser beam is applied from a high power laser cutting tool positioned at a stand off distance from a surface of the material; the laser beam has a spot size and spot shape along the laser beam, and a waist having a focal point and a distal end and a proximal end defining a waist length therebetween; wherein the spot size of the beam waste is less than about 2.5 cm2; wherein the spot size of the beam waste is less than about 2.5 cm2, and the waist length is at least about 2 ft; wherein the spot size of the beam waste is less than about 2.5 cm2, the waist length is at least about 2 ft, and the stand off distance is at least about 3 ft; wherein the spot size area at the beam waste is less than about 2.5 cm2, the waist length is at least about 2 ft, the stand off distance is at least about 3 ft, and the proximal end of the beam waist is at the surface of the material; wherein the beam shape is circular; wherein the beam shape is rectangular; wherein the beam shape is a linear; wherein the spot size of the beam waste is less than about 2.0 cm2; wherein the spot size of the beam waste is less than about 2.0 cm2, and the waist length is at least about 4 ft; wherein the spot size of the beam waste is less than about 2.0 cm2, the waist length is at least about 4 ft, and the stand off distance is at least about 10 ft;
Still further, there is provided methods of these shaped volumetric removals of materials in which one or more of the following may also be practiced: wherein the spot size of the beam waste is less than about 2.0 cm2, the waist length is at least about 4 ft, the stand off distance is at least about 10 ft, and the proximal end of the beam waist is at the surface of the material; wherein the spot size of the beam waste is less than about 2.0 cm2, the waist length is at least about 4 ft, the stand off distance is at least about 10 ft, and the distal end of the beam waist is at the surface of the material; wherein the spot size of the beam waste is less than about 2.0 cm2, the waist length is at least about 4 ft, the stand off distance is at least about 10 ft, and the proximal end of the focal point is at the surface of the material.
Moreover, there is provided methods of these shaped volumetric removals of materials in which one or more of the following may also be practiced: wherein the laser beam is directed at a beam angle of at least about 5°; wherein the laser beam is directed at a beam angle of at least about 10°; wherein the laser beam is directed at a beam angle of at least about 25°; wherein the laser beam is directed at a beam angle of at least about 30°; wherein the laser beam is directed at a beam angle of at least about 80°; wherein the laser beam is directed at a beam angle of at least about 5°; wherein the laser beam is directed at a beam angle of at least about 10°; wherein the laser beam is directed at a beam angle of at least about 30°; wherein the laser beam is directed at a beam angle of at least about 80°; wherein the laser beam is directed at a beam angle of at least about 5°; wherein the laser beam is directed at a beam angle of at least about 10°; wherein the laser beam is directed at a beam angle of at least about 25°.
Yet further, there is provided a high power laser tool for long stand off distance cutting of a material, the tool having: a source of high power laser energy, a source of a fluid, and an optics package; the optics package having a cooling means, and an optics assembly; the optics assembly configured to provide a laser beam from the tool, the beam having a focal length, a spot size, a spot shape, and a waist having a focal point and a distal end and a proximal end defining a waist length therebetween.
Still further, there is provided these tools for the removal of materials in which one or more of the following may also be present or practiced: wherein the spot size of the beam waste is less than about 2.5 cm2; wherein the spot size of the beam waste is less than about 2.5 cm2, and the waist length is at least about 2 ft; wherein the spot size of the beam waste is less than about 2.5 cm2, the waist length is at least about 2 ft; whereby the tool has a stand off distance of at least about 3 ft; wherein the beam shape is circular; wherein the beam shape is rectangular and has a length of about 2.0 cm and a width of about 0.5 cm; wherein the beam shape is rectangular and has a length of at least about 5 cm and a width of less than about 1 cm; the spot size of the beam is less than about 2.0 cm2; wherein the spot size of the beam is less than about 2.0 cm2; wherein the beam waist length is at least about 4 ft; wherein the spot size of the beam waste is less than about 2.0 cm2, the waist length is at least about 4 ft; whereby the tool has a stand off distance of at least about 10 ft; wherein the laser source has a power of at least about 5 kW; wherein the laser source has a power of at least about 10 kW; wherein the laser source has a power of at least about 40 kW; and wherein the laser source has a power of at least about 60 kW.
Furthermore, there is provided a method of removing material using high power laser energy, including: directing a high power laser beam having a power of at least about 1 kW and a beam angle of greater than about 2° toward a surface of a material; the laser beam creating a hole in the material having a bottom having molten material; and, advancing the hole by flowing the molten material back towards the laser beam, thereby exposing solid material for the laser beam to melt.
Furthermore, there is provided a method of removing material using high power laser energy, including: directing a high power laser beam having a power of at least about 1 kW and a beam angle of at least about 10° toward a surface of a material; the laser beam creating a hole in the material having a bottom having molten material; and, advancing the hole by flowing the molten material back towards the laser beam, thereby exposing solid material for the laser beam to melt.
Furthermore, there is provided a method of removing material using high power laser energy, including: directing a high power laser beam having a power of at least about 1 kW and a beam angle of at least about 30° toward a surface of a material; the laser beam creating a hole in the material having a bottom having molten material; and, advancing the hole by flowing the molten material back towards the laser beam, thereby exposing solid material for the laser beam to melt.
Furthermore, there is provided a method of removing material using high power laser energy, including: directing a high power laser beam having a power of at least about 1 kW and a beam angle of at least about 80° toward a surface of a material; the laser beam creating a hole in the material having a bottom having molten material; and, advancing the hole by flowing the molten material back towards the laser beam, thereby exposing solid material for the laser beam to melt.
Still additionally, there is provided a method of removing material using high power laser energy, by: directing a high power laser beam having a power of at least about 1 kW toward a surface of a material; the laser beam creating a hole in the material having a bottom having molten material; and, advancing the hole by flowing the molten material back towards the laser beam, thereby exposing solid material for the laser beam to melt.
In general, the present inventions relate to the delivery of high power laser beams over a distance to a work surface to perform a laser operation on the work surface. These distances, e.g., the stand off distance, may be greater, and may be substantially larger than typically occurs, or is obtainable, in laser cutting operations. Further, and preferably, the present inventions provide the ability to perform these distant cuts without the need for, with a minimum need for, or with a reduced need for a fluid jet to remove the laser effected material, e.g., dross, slag, or molten material, created by the laser operation. Thus, among other things, the longer stand off distances, alone or in conjunction with, minimizing the need for mechanical cleaning of the cut, e.g., fluid jet, provides the ability to perform laser operations in the field, including in hostile and remote locations, such as, a quarry, a tunnel, a pit, a mine, a well bore, or a nuclear reactor. The laser operations may include, for example, treating, fracturing, tunneling, weakening, melting, ablating, spalling, vaporizing, cooking, charring, welding, heating, annealing, cutting, removing, drilling, penetrating, perforating and combinations and various of these and other activities.
Turning to
In
The gas inlet section body 1005, has a gas inlet line 1009 and connector 1010, for securing the gas inlet line 1009 to the gas inlet section body 1005. The gas inlet section body 1005 has a back end piece 1018, which has a fitting 1011 for an optical fiber cable 1012. The back end piece 1018, also has an auxiliary fitting 1013 for data line 1014, and data line 1015.
Turning to
Generally, the various body sections of the tool may be separate components or they may be integral. They may be connected by any means available that meets the use requirements for the tool. Preferably, the tool, as assembled, should be sufficiently rigid to withstand anticipated vibration and mechanical shocks so that the optical components will remain in optical alignment. The tool body may be made from a single component or tube, it may be made from two, three or more components that are fixed together, such as by threaded connections, bolts, screws, flanges, press fitting, welding, etc. Preferably, the tool, as assembled, should meet the anticipated environmental conditions for an intended use, such as temperature, temperature changes, moisture, weather conditions, vibration, shock (e.g., being dropped) and dust and dirt conditions. The tool body, and body sections may be made from metal, composite materials, or similar types of materials that provide the requisite performance capabilities.
As used herein, unless specified otherwise, the terms front, and distal, are used to refer to the side or portion of a body, component, or structure that is the laser discharge side, is closer to the laser discharge end of the tool, or is further from the source of the laser beam, when the tool is assembled or operational. The terms back or proximal, as used herein and unless specified otherwise, are used to refer to the side or portion of a body, component, or structure that is the back side, is further from the laser discharge end of the tool, or is closer to the source of the laser beam, when the tool is assembled or is operational.
Returning to
Turning to
In this embodiment of the tool, the optics package 1024 has lenses that provided for a long focal length, e.g., greater than about 100 mm (3.94″), greater than about 150 mm (5.91″), greater than about 250 mm (9.84″), greater than about 500 mm (19.68″), greater than about 1,000 mm (39.37″), greater than about 1,500 mm (59.06″), greater than about 2,000 mm (78.74″), greater than about 22,860 mm (75′) and greater; and from about 250 mm to about 1,500 mm, and about 500 mm to about 1,000 mm.
Turning to
The stand off distance, which is the distance from the face or distal end 1030 of the laser tool 1000 to the work surface can be greater than about 0.5 feet, greater than about 1 foot, greater than about 3 feet, greater than about 4 feet, and greater. As laser power increases, and laser beam properties are selected, the stand off distance may be about 10 feet and greater. Further, as laser power increases, laser beam properties are selected, and, if needed, means for assisting the laser beam path from the tool to the work surface are used, e.g., a special atmosphere, a jet, or a means to keep the beam path clear, even greater stand off distances may be used, e.g., 50 feet, 75 feet, 100 feet, or more. Generally, across the stand off distance the laser beam path will be in free space, e.g., the laser beam would not be traveling through any solid components, e.g., an optical fiber core, a lens, a window. Thus, for example, the laser beam could be traveling through the atmosphere, e.g., the environmental conditions at a work site, upon exiting the tool at opening 1008 until it strikes the intended work surface.
Turning to
Having a laser beam path angle greater than zero, in conjunction with the laser beam power and other beam properties allows for the laser beam to penetrate deeply into a target material, e.g., the earth, rock, hard rock, and concrete. The laser beam can penetrate over 1 foot into a target material, e.g., hard rock, at least about 2 feet, at least about 5 feet, at least about 10 feet, at least about 50 feet and at least about 100 feet and more. Generally, the laser beam upon striking the work surface of the target material heats and melts that material (vaporization may also take place, and as discussed further below, spallation and thermal-mechanical cracking may also arise as a result of the laser heating of the target material, as well as other laser-thermal-mechanical phenomena, changes or transitions). Because the beam angle is greater than 0° the laser beam forms a hole in the target material that has a slope, i.e., down toward the work surface and up into the target material. Thus, the molten material can flow down and out of the hole, clearing the hole so that the laser beam is continually striking the bottom or end of the hole, melting and thus removing additional target material and lengthening the hole.
Turning to
In general it is preferred that the optimum portion of the laser beam, e.g., beam waist 1064 of
The beam waist in many applications is preferably in the area of the maximum depth of the cut. In this manner the hole opens up toward the face (from surface), which further helps the molten material to flow from the hole. This effect is further shown in
Turning to
Turning to
Turning now to
In general, the airflow within the tool preferably is sufficient to keep the distal end of the optics package and of the tool clear of debris and dirt from the environment. The airflow may also be used for cooling the optical package, optical components or other portions of the tool. A separate fluid, gas, or other type of cooling or thermal management system may be employed with the tool depending upon such factors as laser power, likely stand off distances, and environment temperatures, e.g., if the target material is a glacier in Antarctica compared to a rock face deep within an underground gold mine. For example, air flows of from about 15 scfm to about 50 scfm, about 20 scfm to about 40 scfm, about 20 scfm, and about 30 scfm can be utilized. Greater air flows may be used, but may not be necessary to cool and keep the optics clean. Ambient air from a compressor, bottled or compress air, nitrogen or other gasses may be used. Preferably the gas is clean, and substantially free from, or free from, any grease, oil or dirt that could adversely effect the optics when the laser beam is being propagated.
Turning to
It should be further noted that once this self limiting depth control has occurred, the laser tool can be moved closer to the material and then have the process continue to advance the hole until the new self limiting depth is reached, at which if desired the tool could be move close, and this may be repeated until the tool is essentially upon the face of the target material.
Turning to
The fractures 5090a, 5090b, 5090c and 5090d are merely schematic representation of the laser induced fractures that can occur in the target material, such as rock, earth, rock layer formations and hard rocks, including for example granite, basalt, sandstone, dolomite, sand, salt, limestone, ores, minerals, overburden, marble, rhyolite, quartzite and shale rock. In the target material, and especially in target materials that have a tendency, and a high tendency for thermal-mechanical fracturing, in a 10 foot section of laser cut hole there may be about 10, about 20, about 50 or more such fractures, and these fractures may be tortious, substantially linear, e.g., such as a crack along a fracture line, interconnected to greater and lessor extents, and combinations and variations of these. These laser fractures may also be of varying size, e.g., length, diameter, or distance of separation. Thus, they may vary from micro fractures, to hairline fractures, to total and extended separation of sections having considerable lengths.
The depth or length of the hole can be controlled by determining the rate, e.g., inches/min, at which the hole is advanced for a particular laser beam, configuration with respect to the work surface of the target material, and type of target material. Thus, based upon the advancement rate, the depth of the hole can be predetermined by firing the laser for a preset time.
The rate and extent of the laser fracturing, e.g., laser induced crack propagation, may be monitored by sensing and monitoring devices, such as acoustical devices, acoustical geological sensing devices, and other types of geological, sensing and surveying type devices. In this manner the rate and extent of the laser fracturing may be controlled real time, by adjusting the laser beam properties based upon the sensing data.
In doing assays of a formation, for example, to determine a mineral or precious metal content, a laser hole can be cut into the face of the formation and advanced into the formation to a predetermined depth, for example 100 feet. Samples of the molten material flowing from the hole can be taken at set time intervals, which would correspond to set distances from the face (based upon the advancement rate for the hole). The molten sample can be analyzed at the location or solidified and stored, for later analysis. In this manner, if a series of holes are laser cut into the rock face at predetermined intervals an analysis of the entire formation can be performed. For example, since the laser can be used to melt the target material, e.g., a rock, it is also possible to collect the molten rock in for example a crucible. By keeping the rock molten for a few minutes, (the laser may be used for this purpose, a second laser may be used, or conventional heaters, e.g., flame, electric, may be used) the heavier desired metal, e.g., gold, silver, copper, and other heavy metals can sink to the bottom of the crucible giving the operator a real time method for assaying the potential of the formation. The laser can also be used to melt a predetermined surface or volume of rock for the purpose of assaying the formation independent of any drilling or cutting process. The spectral emissions from the laser rock process may also be used to determine the presence of trace elements. In this example, preferably a sophisticated spectral analysis technique, known to those of skill in the spectral analysis arts, can be employed, to sort out the spectral signatures of the desired or sought after materials that may be buried in the background blackbody radiation signal.
Cuts in, sectioning of, and the volumetric removal of the target material can be accomplished by delivering the laser beam energy to the target material in preselected and predetermined energy distribution patterns. These patterns can be done with a single laser beam, or with multiple laser beams. For example, these patterns can be: a linear cut; a circular cut; a spiral cut; a pattern of connected cuts; a pattern of connected linear cuts, such as a grid pattern, a pattern of radially extending cuts, e.g., spokes on a wheel; a circle and radial cut pattern, e.g., cutting pieces of a pie and cutting around the pie pan; a pattern of spaced apart holes, such as in a line, in a circle, in a spiral, or other pattern, as well as other patterns and arrangements. The patterns, whether lines, staggered holes, others, or combinations thereof, can be traced along a feature of the target material, such as, a geologic feature of a formation, a boarder of an ore seam, or a joint in a structure. The patterns can be traced along a feature intended to be created in the target material, such as a side wall or roof of a tunnel or shaft. The forgoing are illustrative examples of the types and nature of laser cuts, sectionings and volumetric removals that the can be performed; and that additional, other, varied, as well as combinations and variations of the forgoing are contemplated. Additionally, the timing and sequence of the creation of the holes, cuts and volumetrically removed sections, can be predetermined to enhance, and take advantage, the laser fracturing of the target material, as well as the laser affected zones in the material. The predetermined timing sequence can also provide the ability to enhance other non-laser operations that may be taking place before, after or in conjunction with the laser operations.
Thus, for example, in determining a laser beam delivery pattern to provide a predetermined and preselected laser beam energy distribution pattern, the spacing of cut lines, or staggered holes, in the target material, preferably may be such that the laser affected zones are slightly removed from one another, adjacent to one another but do not overlap, or overlap only slightly. In this manner, the maximum volume of the target material will be laser affected, i.e., weakened, with the minimum amount of total energy.
It is further believed that when comparing the energy delivered from the present laser operations, as compared to conventional blasting using explosives, substantially less energy is being used. Further, the present laser operations avoid the peripheral environment damage, and structural damage to surround structures, e.g., homes and business, that may occur from the use of explosive in mining, quarrying, tunneling and construction activities. The present inventions provide a further benefit by eliminating risk to personnel from the use and handling of explosives; thus eliminating the need to vacate all personnel during the mining operation. Unlike explosive use, the use of the present laser operations may not require the clearing of large areas and the stopping of other operations, while the cutting and fracturing operations are ongoing.
Preferably, when the laser tool is configured for performing a laser operation on a target material the laser beam path from the front of the tool to the surface of target material should be isolated. This may be accomplished by the use of a barrier that prevents the laser light from escaping or from reaching the location where personnel may be present. For example the laser beam path may be isolated by using a light weight metal tube, having an internal diameter that is large enough to not interfere with the laser beam, that is optically sealed to the laser tool, i.e., no laser light can escape, and that extends from the laser tool to the work surface, where it is optically sealed to the work surface. It may be isolated by using a temporary, semi-permanent or permanent shielding structure, e.g., stands holding welding blankets or other light blocking materials, a scaffold supporting light blocking materials, a telescoping or extendable housing that is placed over the beam path or more preferably the tool and the beam path. It may also be isolated by constructing a temporary, semi-permanent or permanent barrier to optically isolate the beam path, and more preferably to isolate the tool, the work surface and the target material from personnel, e.g., a temporary barrier in a tunnel, optically sealing against the tunnel walls, behind the laser tool as it is advancing the tunnel face. The enclosure or shield may also be made from laser safe glass, e.g., glass that does not transmit, or substantially does not transmit light in the wavelength of the laser beam, or have window having such glass in them.
Turning to
A preferable configuration, and use, for an adjustable optics package will be for use with a 300 m optic system so that the beam waist can be driven, e.g., advanced forward by changing focal length, into the borehole as the borehole advances.
Turning to
In
In the embodiment of
Generally, the various body sections of the tool 9000 may be separate components or they may be integral. They may be connected by any means available that meets the use requirements for the tool. Preferably, the tool, as assembled, should be sufficiently rigid to withstand anticipated vibration and mechanical shocks so that the optical components will remain in optical alignment. The tool body, body section, the beam tube and the prism section may be made from a single component or tube, it may be made from two, three or more components that are fixed together, such as by threaded connections, bolts, screws, flanges, press fitting, welding, etc. Preferably, the tool, as assembled, should meet the anticipated environmental conditions for an intended use, such as temperature, temperature changes, moisture, weather conditions, and dust and dirt conditions. The tool body, body sections, and beam tube, and prism sections may be made from metal, composite materials, or similar types of materials that provide the requisite performance capabilities.
The optical fiber cable 9012 extends into the gas inlet section body 1005 and the gas flow passage 9019. The optical fiber cable 9012 is optically and mechanically associated with optical connector 9022, which is positioned in optical connector receptacle 9023. The optical connector receptacle has a plurality of fins, e.g., 9025, which extend into gas flow passage 9019, and which provide cooling for the optical connector 9022 and the optical connector receptacle 9023. The laser beam path is represented by dashed line 9026, and extends from within the core of the optical fiber cable 9012 to a potential target or work surface. (The totality of the optical path would start at the source of the laser beam, and extend through all optical components, and free space, that are in the intended path of the laser beam.) At the distal end 9022a of optical connector 9022, the laser beam path 9026 is in free space, e.g., no solid components are present, and travels from the distal connector end 9022a to the optics package 9024, where the laser beam is optically manipulated to predetermined laser beam parameters for providing long stand off distance capabilities. The laser beam path 9026 exits the distal end 9024a of the optics package 9024, and travels in free space in the flow carry over section 9020, in the front section of the optical section body 9028, and into beam path tube section 9003 which has beam tube 9003, and enters TIR prism 9050 where it is reflected at a right angle, exiting through opening 9008. In operation the laser beam 9027 would be propagated by a laser, e.g., a source of a laser beam, and travel along the laser beam path 9026. The TIR (total internal reflection) prism 9050 is of the type taught and disclose in U.S. Patent Application Ser. No. 61/605,434 the entire disclosure of which is incorporated herein by reference, and which can be configured to provide other angles in addition to 90°.
Other types of reflective mirrors may be used. Thus, the mirror may be any high power laser optic that is highly reflective of the laser beam wavelength, can withstand the operational pressures, and can withstand the power densities that it will be subjected to during operation. For example, the mirror may be made from various materials. For example, metal mirrors are commonly made of copper, polished and coated with polished gold or silver and sometime may have dielectric enhancement. Mirrors with glass substrates may often be made with fused silica because of its very low thermal expansion. The glass in such mirrors may be coated with a dielectric HR (highly reflective) coating. The HR stack as it is known, consists of layers of high/low index layers made of SiO2, Ta2O5, ZrO2, MgF, Al2O3, HfO2, Nb2O5, TiO2, Ti2O3, WO3, SiON, Si3N4, Si, or Y2O3 (All these materials would work for many wave lengths, including 1064 nm to 1550 nm). For higher powers, such as 50 kW actively cooled copper mirrors with gold enhancements may be used. It further may be water cooled, or cooled by the flow of the gas. Preferably, the mirror may also be transmissive to wavelengths other than the laser beam wave length. In this manner an optical observation device, e.g., a photo diode, a camera, or other optical monitoring and detection device, may be placed behind it.
In the embodiment of the tool in
The nozzles or distal end opening of the tools may have opens of about 1 cm diameter for a focusing optic with a short focal length to 40 cm diameter for the long focal length optics assemblies.
In addition to moving or scanning the laser beam, or the laser cutting head to create a pattern on the target material, the optics then self, or in combination with scanning or movement, can be used to create custom and predetermined patterns, such as, e.g., a matrix of spaced spots or a grid pattern.
The following examples are provide to illustrate various devices, tools, configurations and activities that may be performed using the high power laser tools, devices and system of the present inventions. These examples are for illustrative purposes, and should not be view as, and do not otherwise limit the scope of the present inventions.
A laser pattern is delivered to a target material from a stand off distance of about 30 feet. A laser cutting tool of the general type shown in
An embodiment of an optics assembly for providing a high power laser beam for cutting and drilling a target material from a stand off distance of 100 feet is provided in
Turning to
Turning to
In an example of an embodiment of this optical assembly, the fiber may have a core of about 200 μm, and the NA of the connector distal face is 0.22. The beam launch assembly (fiber 1410/connector) launches a high power laser beam, having 20 kW of power in a pattern shown by the ray trace lines, to a secondary mirror 1416. The diverging mirror 1416 is located 11 cm (as measured along the total length of the beam path) from the launch or distal face of the beam launch assembly. The secondary mirror 1416 has a diameter of 2″ and a radius of curvature 143 cm. For distances of about 100 feet the primary mirror 1418 has a diameter of 18″ and a radius of curvature of 135 cm. In this embodiment the primary mirror is shaped, based upon the incoming beam profile, to provide for a focal point 100 feet from the face of the primary mirror. This configuration can provided a very tight spot in the focal plain, the spot having a diameter of 1.15 cm. Moving in either direction from the focal plane, along the beam waist, for about 4 feet in either direction (e.g., an 8 foot optimal cutting length of the laser beam) the laser beam spot size is about 2 cm. For cutting rock, it is preferable to have a spot size of about ¾″ or less (1.91 cm or less) in diameter (for laser beam having from about 10 to 40 kW). In an example of an embodiment during use, the diverging mirror could have 2 kW/cm2 and the primary mirror could have 32 W/cm2 of laser power on their surfaces when performing a laser perforation operation.
In this embodiment a 20 kW laser beam is launched into the laser optics assembly of the embodiment of Example 2, the secondary mirror would have 1 kW/cm2 and the primary mirror would have 16 W/cm2.
In this embodiment a 40 kW laser beam is launched into the laser optics assembly of the embodiment of Example 2, the secondary mirror would have 2 kW/cm2 and the primary mirror would have 32 W/cm2.
In this embodiment a 40 kW laser beam is launched into the laser optics assembly of the embodiment of Example 2a, the diverging (secondary) mirror would have 2 kW/cm2 and the primary mirror would have 32 W/cm2.
In this embodiment 3 optical assemblies of the configuration of Example 2a are used, with a separate fiber each providing a 20 kW laser beam to the assemblies. The three assemblies are positioned to direct three laser beams into a 2 cm2 spot, having a combined power of about 60 kW at a distance of 100 feet from the tool.
In this embodiment 3 optical assemblies of the configuration of Example 2a are used, with a separate 200 μm core fiber, each providing a 40 kW laser beam to the assemblies. The three assemblies are positioned to direct three laser beams into a 2 cm2 spot, having a combined power of about 120 kW at a distance of 100 feet from the tool.
Turning to
Differing types of lens may be used, for example in an embodiment Lens 830 has a focal length of 500 mm and lens 840 has a focal length of 500 mm, which provide for a focal length for the optics assembly of 250 mm. The NA of the connector face is 0.22. Lens 810 is a meniscus (f=200 mm). Lens 820 is a plano-convex (f=200 mm). Lens 830 is a plano-convex (f=500 mm). Lens 840 is a menisus (f=500 mm).
In an embodiment of the assembly of
In an embodiment of the assembly of
The embodiment of
In this embodiment the lens configuration and types of the embodiment of
In an embodiment of the optics assembly of the
In this embodiment the lens configuration of
Turning to
A crosshatch laser beam delivery pattern having 100 essentially vertical planar cuts and 20 essentially horizontal planar cuts is delivered to the rock face of an open face mine. The laser beam has a focal point of 100 feet, a beam waist of about 2 cm and a depth of focus of about 8 feet. The laser beam has a beam angle of 10°. The laser beam has a power of 40 kW. The vertical planes of the pattern are cut first, by firing the laser at the top of the planar cut until the desired depth of the initial hole is achieved and then moving the laser beam down until the length of the cut, to depth has been completed. Once the vertical cuts have been done, the horizontal cuts are made.
A crosshatch laser beam delivery pattern having 300 essentially vertical planar cuts and 200 essentially horizontal planar cuts is delivered to the rock face in a subsurface mine. The laser beam has a focal point of 50 feet, a beam waste having a length of 5 feet, and a maximum spot size diameter of about 2 cm. The laser beam has a beam angle of 15°. The laser beam has a power of 50 kW. The vertical planes of the pattern are cut first, by firing the laser at the top of the planar cut until the desired depth of the initial hole is achieved and then moving the laser beam down until the length of the cut, to depth has been completed. Once the vertical cuts have been done, the horizontal cuts are made.
A crosshatch laser beam delivery pattern having 100 essentially vertical planar cuts and 20 essentially horizontal planar cuts is delivered to the rock face of an open pit mine. The laser beam has a focal point of 100 feet, a beam waste having a length of 8 feet, and a maximum spot size diameter of about 2 cm. The laser beam has a beam angle of 10°. The laser beam has a power of 40 kW. The horizontal planes of the pattern are cut first, by firing the laser at the top of the planar cut until the desired depth of the initial hole is achieved and then moving the laser beam across until the length of the cut, to depth has been completed. Once the horizontal cuts have been done, the vertical cuts are made.
A crosshatch laser beam delivery pattern having 300 essentially vertical planar cuts and 200 essentially horizontal planar cuts is delivered to the rock face in a subsurface mine. The laser beam has a focal point of 50 feet, a beam waste having a length of 5 feet, and a maximum spot size diameter of about 2 cm. The laser beam has a beam angle of 15°. The laser beam has a power of 50 kW. The horizontal planes of the pattern are cut first, by firing the laser at the top of the planar cut until the desired depth of the initial hole is achieved and then moving the laser beam across until the length of the cut, to depth has been completed. Once the horizontal cuts have been done, the vertical cuts are made.
A laser tool was used to cut perforations in rock samples. The laser power was 15.3 kW, the beam angle was 15°, the standoff distance was 3 feet, and a laser tool of the general type shown in
A laser tool was used to cut perforations in Brohm rock samples. The laser power was 15 kW, the beam angle was 15°, the standoff distances were varied, and a laser tool of the general type shown in
A laser tool was used to cut perforations in Brohm rock samples. The laser power was 15 kW, the beam angle was 15°, the standoff distances were varied, and a laser tool of the general type shown in
A laser tool was used to cut perforations in Brohm rock samples. The laser power was 15.3 kW, the beam angle was 30°, the standoff distance was 3 feet, and a laser tool of the general type shown in
A laser tool was used to cut perforations in limestone rock samples. The laser power was 15.3 kW, the beam angle was 15°, the standoff distance was 3 feet, and a laser tool of the general type shown in
A laser tool was used to cut perforations in limestone rock samples. The laser power was varied, the beam angle was 30°, the standoff distance was 3 feet, and a laser tool of the general type shown in
A laser tool was used to cut perforations in rock samples. The laser power was 15.3 kW, the beam angle was 15°, the standoff distance was 3 feet, and a laser tool of the general type shown in
A laser tool was used to cut perforations in rock samples. The laser power was varied, the beam angle was 30°, the standoff distance was 3 feet, and a laser tool of the general type shown in
In addition to these, examples, the high power laser systems, tools, devices and methods of the present inventions may find other uses and applications in activities such as: off-shore activities; subsea activities; decommissioning structures such as, factories, nuclear facilities, nuclear reactors, pipelines, bridges, ships, hazardous waste locations; contaminated structures, etc.; cutting and removal of structures in refineries; civil engineering projects and construction and demolitions; concrete repair and removal; mining; surface mining; deep mining; rock and earth removal; surface mining; tunneling; making small diameter bores; oil field perforating; oil field fracking; well completion; precise and from a distance, in-place milling and machining; heat treating; and combinations and variations of these and other activities and operations.
In addition to the foregoing Examples, figures and embodiments, other optics assemblies and configurations may be used to focus the laser beam and provide long stand off distance operations. Such optics assemblies would include zoom optics based on a moveable lens, zoom optics based on a movable mirror, zoom optics based on an adaptive optic, and combinations and variations of these.
For example, and preferably, gravity can be used as the motive force to remove the molten material by drilling the laser at a slight upward angle, this angle can be as small as a few degrees or as much as 90 degrees from horizontal, i.e., a vertical hole. In general, the greater the angle, the faster the flow rate of the molten rock. For example, the temperature for the melting point for quartz is about 2,100° C. This effect is shown in the chart of
However, for example, downward laser perforations have been made in rocks when the focus is before (or above) the rock face and the downward angel of the beam is about 4 degrees, without the need for assistance to clear the hole.
A single high power laser may be utilized in the system, tools and operations, or there may be two or three high power lasers, or more. High power solid-state lasers, specifically semiconductor lasers and fiber lasers are preferred, because of their short start up time and essentially instant-on capabilities. The high power lasers for example may be fiber lasers or semiconductor lasers having 10 kW, 20 kW, 50 kW or more power and, which emit laser beams with wavelengths in the range from about 455 nm (nanometers) to about 2100 nm, preferably in the range about 800 nm to about 1600 nm, about 1060 nm to 1080 nm, 1530 nm to 1600 nm, 1800 nm to 2100 nm, and more preferably about 1064 nm, about 1070-1080 nm, about 1360 nm, about 1455 nm, 1490 nm, or about 1550 nm, or about 1900 nm (wavelengths in the range of 1900 nm may be provided by Thulium lasers).
An example of this general type of fiber laser is the IPG YLS-20000. The detailed properties of which are disclosed in US patent application Publication Number 2010/0044106.
Examples of lasers, conveyance structures, high power laser fibers, high power laser systems, optics, optics housings to isolate optics from vibration and environment conditions, break detection and safety monitoring, control systems, connectors, cutters, and other laser related devices, systems and methods that may be used with, in, or in conjunction with, the various embodiments of devices systems, tools, activities and operations set forth in this specification are disclosed and taught in the following US patent application publications and US patent applications: Publication Number 2010/0044106; Publication Number 2010/0044105; Publication Number 2010/0044103; Publication Number 2010/0215326; Publication Number 2012/0020631; Publication Number 2012/0074110; Publication No. 2012/0068086; Publication No. 2012/0248078; Ser. No. 13/403,723; Ser. No. 13/403,509; Ser. No. 13/486,795; Ser. No. 13/565,345; Ser. No. 13/782,869; Ser. No. 61/605,429; Ser. No. 13/768,149; and Ser. No. 61/605,434, the entire disclosures of each of which are incorporated herein by reference.
In addition to the use of high power electromagnetic energy, such as high power laser beams, other forms of directed energy or means to provide the same, may be utilized in, in addition to, or in conjunction with the devices systems, tools, activities and operations set forth in this specification. Such directed energy could include, for example, non-optical stimulated emission electromagnetic energy, non-optical coherent electromagnetic energy, microwaves, sound waves, millimeter waves, plasma, electric arcs, flame, flame jets, steam and combinations of the foregoing, as well as, water jets and particle jets. It is noted, however, that each of these other such directed energies, has significant disadvantages when compared to high power laser energy. Nevertheless, the use of these other less desirable directed energy means is contemplated by the present inventions as directed energy means.
These tools, systems and operations provide a unique laser drilling and cutting methods for performing many activities such as prepping blast holes or cutting out the slope of a rock face, they also provide the ability to reduce the need for, if not to eliminate the need for the use of explosives in construction, demolition, decommissioning, mining, drilling and other types of activities where explosives and large equipment are utilized. It being understood, that precision activities of a very fine nature may also be performed, such as precision cutting of a part or component in a high hazardous environment, such as within a nuclear reactor containment structure. Additionally, a high power laser, of 1 kW or greater, can be used to drill a hole directly in a rock face. A laser, when drilling into a vertical wall or ceiling can penetrate to the maximum limit of the laser beam's intensity, as long as, fresh material is being exposed to the laser beams energy. Thus, by way of example, it is preferable that there is room for the melted rock to flow from the laser drilled hole, and if necessary and preferably that some means be employed to force or assist in the melted rock being removed from the laser drilled hole, or from the laser beam path as it progress into and advances the hole.
Depending upon the target material being cut, the location of the cutting, e.g., in a confined area or in the open, it may be advisable or preferable to have a system for handling, managing, processing and combinations and variation of these, the gases, fumes, and other air born or gaseous materials that are created during or by the laser operation. Thus, for example and preferably, a high volume vacuum system can be located near the exit of the drilling or cutting region to be able to remove any toxic fumes from the molten region.
The shape of the laser beam, the laser beam spot on the surface of the target material, and the resultant hole that is created by the laser beam in the target material may be circular, square, v-shaped, circular with a flat bottom, square with a rounded bottom, and other shapes and configurations that may be utilized and can be based upon the flow characteristics of the molten target material, and selected to maximize the removal of that material.
The various embodiments of devices systems, tools, activities and operations set forth in this specification may be used with various high power laser systems and conveyance structures and systems, in addition to those embodiments of the Figures and Examples in this specification. The various embodiments of devices systems, tools, activities and operations set forth in this specification may be used with: other high power laser systems that may be developed in the future: with existing non-high power laser systems, which may be modified, in-part, based on the teachings of this specification, to create a high power laser system; and with high power directed energy systems. Further, the various embodiments of devices systems, tools, activities and operations set forth in this specification may be used with each other in different and various combinations. Thus, for example, the configurations provided in the various embodiments of this specification may be used with each other; and the scope of protection afforded the present inventions should not be limited to a particular embodiment, configuration or arrangement that is set forth in a particular embodiment, example, or in an embodiment in a particular Figure.
The invention may be embodied in other forms than those specifically disclosed herein without departing from its spirit or essential characteristics. The described embodiments are to be considered in all respects only as illustrative and not restrictive.
This application: (i) claims, under 35 U.S.C. §119(e)(1), the benefit of the filing date of Nov. 15, 2012 of U.S. provisional application Ser. No. 61/727,096; (ii) is a continuation-in-part of Ser. No. 13/782,869, filed Mar. 1, 2013, which claims under 35 U.S.C. §119(e)(1), the benefit of the filing date of Mar. 1, 2012 of U.S. provisional application Ser. No. 61/605,429; (iii) is a continuation-in-part of Ser. No. 13/768,149, filed Feb. 15, 2013, which claims, under 35 U.S.C. §119(e)(1), the benefit of the filing date of Mar. 1, 2012 of U.S. provisional application Ser. No. 61/605,434; (iv) is a continuation-in-part of U.S. patent application Ser. No. 13/222,931 filed Aug. 31, 2011, which claims under 35 U.S.C. §119(e)(1), the benefit of the filing date of Aug. 31, 2010 of provisional application Ser. No. 61/378,910; (v) is a continuation-in-part of U.S. patent application Ser. No. 13/210,581, filed Aug. 16, 2011, which claims, under 35 U.S.C. §119(e)(1), the benefit of the filing date of Aug. 17, 2010 of provisional application Ser. No. 61/374,594; (vi) is a continuation-in-part of U.S. patent application Ser. No. 12/544,136, filed Aug. 19, 2009, which claims, under 35 U.S.C. §119(e)(1), the benefit of the filing date of Aug. 20, 2008 of provisional application Ser. No. 61/090,384, the benefit of the filing date of Oct. 3, 2008 of provisional application Ser. No. 61/102,730, the benefit of the filing date of Oct. 17, 2008 of provisional application Ser. No. 61/106,472, and the benefit of the filing date of Feb. 17, 2009 of provisional application Ser. No. 61/153,271; (vii) is a continuation-in-part of U.S. patent application Ser. No. 12/544,094, filed Aug. 19, 2009; (viii) is a continuation-in-part of U.S. patent application Ser. No. 12/706,576 filed Feb. 16, 2010; (ix) is a continuation-in-part of U.S. patent application Ser. No. 12/840,978 filed Jul. 21, 2010; and, (x) is a continuation-in-part of U.S. patent application Ser. No. 12/543,986, filed Aug. 19, 2009, the entire disclosures, of each, of which are incorporated herein by reference.
| Number | Name | Date | Kind |
|---|---|---|---|
| 3998281 | Salisbury et al. | Dec 1976 | A |
| 7802384 | Kobayashi | Sep 2010 | B2 |
| 8997894 | Zediker | Apr 2015 | B2 |
| 20030132029 | Parker | Jul 2003 | A1 |
| 20060237233 | Reed et al. | Oct 2006 | A1 |
| 20070068705 | Hosie et al. | Mar 2007 | A1 |
| 20070272407 | Lehman et al. | Nov 2007 | A1 |
| 20100044102 | Rinzler et al. | Feb 2010 | A1 |
| 20100044103 | Moxley et al. | Feb 2010 | A1 |
| 20100044104 | Zediker | Feb 2010 | A1 |
| 20100044105 | Faircloth | Feb 2010 | A1 |
| 20100044106 | Zediker | Feb 2010 | A1 |
| 20100215326 | Zediker | Aug 2010 | A1 |
| 20100258289 | Lynde et al. | Oct 2010 | A1 |
| 20100326659 | Schultz | Dec 2010 | A1 |
| 20110290563 | Kocis et al. | Dec 2011 | A1 |
| 20120020631 | Rinzler | Jan 2012 | A1 |
| 20120067643 | DeWitt | Mar 2012 | A1 |
| 20120068086 | DeWitt | Mar 2012 | A1 |
| 20120074110 | Zediker | Mar 2012 | A1 |
| 20120217015 | Zediker | Aug 2012 | A1 |
| 20120217017 | Zediker | Aug 2012 | A1 |
| 20120217018 | Zediker | Aug 2012 | A1 |
| 20120217019 | Zediker | Aug 2012 | A1 |
| 20120248078 | Zediker | Oct 2012 | A1 |
| 20120255774 | Grubb | Oct 2012 | A1 |
| 20120255933 | McKay | Oct 2012 | A1 |
| 20120261188 | Zediker | Oct 2012 | A1 |
| 20120266803 | Zediker | Oct 2012 | A1 |
| 20121267168 | Grubb | Oct 2012 | |
| 20120273269 | Rinzler | Nov 2012 | A1 |
| 20120273470 | Zediker | Nov 2012 | A1 |
| 20120275159 | Fraze | Nov 2012 | A1 |
| 20130011102 | Rinzler | Jan 2013 | A1 |
| 20130175090 | Zediker | Jul 2013 | A1 |
| 20130192893 | Zediker | Aug 2013 | A1 |
| 20130192894 | Zediker | Aug 2013 | A1 |
| 20130220626 | Zediker | Aug 2013 | A1 |
| 20130228372 | Linyaev | Sep 2013 | A1 |
| 20130228557 | Zediker | Sep 2013 | A1 |
| 20130266031 | Norton | Oct 2013 | A1 |
| 20130319984 | Linyaev | Dec 2013 | A1 |
| 20140000902 | Wolfe | Jan 2014 | A1 |
| 20140060802 | Zediker | Mar 2014 | A1 |
| 20140060930 | Zediker | Mar 2014 | A1 |
| 20140069896 | Deutch | Mar 2014 | A1 |
| 20140090846 | Deutch | Apr 2014 | A1 |
| 20140190949 | Zediker | Jul 2014 | A1 |
| 20140231085 | Zediker | Aug 2014 | A1 |
| 20140231398 | Land | Aug 2014 | A1 |
| 20140248025 | Rinzler | Sep 2014 | A1 |
| 20140345872 | Zediker | Nov 2014 | A1 |
| Entry |
|---|
| International Search Report and the Written Opinion of the International Searching Authority, PCT/US13/070321, mailed Jun. 13, 2014. |
| International Search Report and the Written Opinion of the International Searching Authority, PCT/US13/77614, mailed Nov. 3, 2014. |
| Number | Date | Country | |
|---|---|---|---|
| 20160221125 A1 | Aug 2016 | US |
| Number | Date | Country | |
|---|---|---|---|
| 61727096 | Nov 2012 | US | |
| 61605429 | Mar 2012 | US | |
| 61605434 | Mar 2012 | US | |
| 61378910 | Aug 2010 | US | |
| 61374594 | Aug 2010 | US | |
| 61090384 | Aug 2008 | US | |
| 61102730 | Oct 2008 | US | |
| 61106472 | Oct 2008 | US | |
| 61153271 | Feb 2009 | US |
| Number | Date | Country | |
|---|---|---|---|
| Parent | 13782869 | Mar 2013 | US |
| Child | 14080722 | US | |
| Parent | 13768149 | Feb 2013 | US |
| Child | 13782869 | US | |
| Parent | 13222931 | Aug 2011 | US |
| Child | 13768149 | US | |
| Parent | 13210581 | Aug 2011 | US |
| Child | 13222931 | US | |
| Parent | 12544136 | Aug 2009 | US |
| Child | 13210581 | US | |
| Parent | 12544094 | Aug 2009 | US |
| Child | 12544136 | US | |
| Parent | 12706576 | Feb 2010 | US |
| Child | 12544094 | US | |
| Parent | 12840978 | Jul 2010 | US |
| Child | 12706576 | US | |
| Parent | 12543986 | Aug 2009 | US |
| Child | 12840978 | US |
