U.S. patent application number 14/330980 was filed with the patent office on 2015-10-29 for method and system for advancement of a borehole using a high power laser.
This patent application is currently assigned to FORO ENERGY INC.. The applicant listed for this patent is Brian O. Faircloth, Yeshaya Koblick, Mark S. Land, Joel F. Moxley, Charles C. Rinzler, Mark S. Zediker. Invention is credited to Brian O. Faircloth, Yeshaya Koblick, Mark S. Land, Joel F. Moxley, Charles C. Rinzler, Mark S. Zediker.
Application Number | 20150308194 14/330980 |
Document ID | / |
Family ID | 41695291 |
Filed Date | 2015-10-29 |
United States Patent
Application |
20150308194 |
Kind Code |
A1 |
Moxley; Joel F. ; et
al. |
October 29, 2015 |
METHOD AND SYSTEM FOR ADVANCEMENT OF A BOREHOLE USING A HIGH POWER
LASER
Abstract
There is provided a system, apparatus and methods for the laser
drilling of a borehole in the earth. There is further provided with
in the systems a means for delivering 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, a laser bottom hole assembly, and fluid directing techniques
and assemblies for removing the displaced material from the
borehole.
Inventors: |
Moxley; Joel F.; (Highlands
Ranch, CO) ; Land; Mark S.; (Houston, TX) ;
Rinzler; Charles C.; (Boston, MA) ; Faircloth; Brian
O.; (Evergreen, CO) ; Koblick; Yeshaya;
(Sharon, MA) ; Zediker; Mark S.; (Castle Rock,
CO) |
|
Applicant: |
Name |
City |
State |
Country |
Type |
Moxley; Joel F.
Land; Mark S.
Rinzler; Charles C.
Faircloth; Brian O.
Koblick; Yeshaya
Zediker; Mark S. |
Highlands Ranch
Houston
Boston
Evergreen
Sharon
Castle Rock |
CO
TX
MA
MA
CO |
US
US
US
CO
US
US |
|
|
Assignee: |
FORO ENERGY INC.
Houston
TX
|
Family ID: |
41695291 |
Appl. No.: |
14/330980 |
Filed: |
July 14, 2014 |
Related U.S. Patent Documents
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Application
Number |
Filing Date |
Patent Number |
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12543986 |
Aug 19, 2009 |
8826973 |
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14330980 |
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61090384 |
Aug 20, 2008 |
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61102730 |
Oct 3, 2008 |
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61106472 |
Oct 17, 2008 |
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61153271 |
Feb 17, 2009 |
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Current U.S.
Class: |
175/16 |
Current CPC
Class: |
E21B 10/60 20130101;
E21B 43/11 20130101; E21B 7/15 20130101; E21B 7/14 20130101; E21B
21/00 20130101; E21B 29/00 20130101; E21B 21/08 20130101; E21B
21/103 20130101 |
International
Class: |
E21B 7/15 20060101
E21B007/15 |
Goverment Interests
[0002] This invention was made with Government support under Award
DE-AR0000044 awarded by the Office of ARPA-E U.S. Department of
Energy. The Govemment has certain rights in this invention.
Claims
1. A high power laser drilling system for use in association with a
drilling rig, drilling platform, drilling derrick, a snubbing
platform, or coiled tubing drilling rig for advancing a borehole in
hard rock, the system comprising: a. a source of high power laser
energy, the laser source capable of providing a laser beam having
at least 20 kW of power; b. a bottom hole assembly; i. the bottom
hole assembly having an optical assembly; ii. the optical assembly
configured to provide a predetermined energy deposition profile to
a borehole surface; and, iii. the optical assembly configured to
provide a predetermined laser shot pattern; c. a means for
advancing the bottom hole assembly into and down the borehole; d. a
downhole high power laser transmission cable, the transmission
cable having a length of at least about 1000 feet; e. the downhole
cable in optical communication with the laser source; and, f. the
downhole cable in optical communication with the bottom hole
assembly.
2. The system of claim 1 wherein the cable and bottom hole assembly
are capable of illuminating a borehole surface with a laser beam
having a power of at least about 5 kW.
3. The system of claim 1 wherein the cable and bottom hole assembly
are capable of illuminating a borehole surface with a laser beam
having a power of at least about 10 kW at the bottom hole
assembly.
4. The system of claim 1 wherein the cable and bottom hole assembly
are capable of illuminating a borehole surface with a laser beam
having a power of at least about 15 kW at the bottom hole
assembly.
5. The system of claim 1 wherein the cable and bottom hole assembly
are capable of illuminating a borehole surface with a laser beam
having a power of at least about 18 kW at the bottom hole
assembly
6. The system of claim 1 wherein the downhole cable is at least
1500 feet long.
7. The system of claim 1 wherein the downhole cable is at least
2000 feet long.
8. The system of claim 1 wherein the downhole cable is at least
3000 feet long.
9. A high power laser drilling system for use in association with a
drilling rig, drilling platform, snubbing platform, drilling
derrick, or coiled tubing drilling rig for advancing a borehole,
the system comprising: a. a source of high power laser energy; i.
the laser source capable of providing a laser beam having at least
10 kW of power; ii. the laser source comprising a laser; b. a
bottom hole assembly; i. configured to provide a predetermined
energy deposition profile of laser energy to a borehole surface;
ii. configured to provide a predetermined laser shot pattern; iii.
comprising an optical assembly; and, iv. comprising a means to
mechanically remove borehole material; c. a means for advancing the
bottom hole assembly into and down the borehole; d. a source of
fluid for use in advancing a borehole; e. a downhole high power
laser transmission cable, the transmission cable having a length of
at least about 1000 feet; f. the downhole cable in optical
communication with the laser source; g. the downhole cable in
optical communication with the optical assembly; and, h. the bottom
hole assembly in fluid communication with the fluid source; i.
whereby high power laser energy may be provided to a surface of a
borehole at locates within the borehole at least 1000 feet from the
borehole opening.
10. The system of claim 9 wherein the downhole cable is
unitary.
11. The system of claim 9 wherein the downhole cable comprises a
pair of optically connected cables.
12. The system of claim 9 wherein the downhole cable comprises a
plurality of optically connected cables.
13. The system of claim 9 wherein the downhole cable comprises at
least two cables optically connected end to end.
14. The system of claim 9 wherein the laser source comprises at
least two lasers.
15. The system of claim 9 wherein the laser source comprises a
plurality of lasers.
16. A high power laser drilling system for use in association with
a drilling rig, drilling platform, drilling derrick, a snubbing
platform, or coiled tubing drilling rig for advancing a borehole,
the system comprising: a. a source of high power laser energy; b. a
bottom hole assembly; i. the bottom hole assembly having an optical
assembly; ii. the optical assembly configured to provide an energy
deposition profile to a borehole surface; and, iii. the optical
assembly configured to provide a laser shot pattern; iv. comprising
a means for directing a fluid; c. a means for advancing the bottom
hole assembly into and down the borehole; d. a source of fluid for
use in advancing a borehole; e. a downhole high power laser
transmission cable; f. the downhole cable in optical communication
with the laser source; g. the downhole cable in optical
communication with the bottom hole assembly; and, h. the means for
directing in fluid communications with the fluid source; i. wherein
the system is capable of cutting, spalling, or chipping rock by
illuminating a surface of the borehole with laser energy and remove
waste material created from said cutting, spalling or chipping,
from the borehole and the area of laser illumination by the action
of the directing means.
17. The system of claim 16 wherein the directing means comprises a
fluid amplifier.
18. The system of claim 16 wherein the directing means comprises a
fluid amplifier and an outlet port.
19. The system of claim 16 wherein the directing means comprises a
gas directing means and a fluid directing means.
20. The system of claim 16 wherein the directing means comprises an
air knife.
21. The system of claim 16 wherein the directing means comprises a
plurality of outlet ports.
22. The system of claim 16 wherein the directing means comprises
two outlet ports, the outlet ports are configured to provide for
relative flows of the fluid in the ratio of about 1:1.
23. The system of claim 16 wherein the directing means comprises
two outlet ports, the outlet ports are configured to provide for
relative flows of the fluid in the ratio of about 1 to at least
about 100.
24. A high power laser drilling system for advancing a borehole
comprising: a. a source of high power laser energy, the laser
source capable of providing a laser beam having at least 5 kW of
power; b. a tubing assembly, the tubing assembly having at least
1000 feet of tubing, having a distal end and a proximal; c. a
source of fluid for use in advancing a borehole; d. the proximal
end of the tubing being in fluid communication with the source of
fluid, whereby fluid is transported in association with the tubing;
e. the proximal end of the tubing being in optical communication
with the laser source, whereby the laser beam can be transported in
association with the tubing; f. the tubing comprising a high power
laser transmission cable, the transmission cable having a distal
end and a proximal end, the proximal end being in optical
communication with the laser source, whereby the laser beam is
transmitted by the cable from the proximal end to the distal end of
the cable for delivery of the laser beam energy to the borehole;
and, g. the power of the laser energy at the distal end of the
cable when the cable is within a borehole being at least about 2
kW.
25. The system of claim 24 wherein the tubing assembly is a coiled
tubing rig having at least 4000 ft of coiled tubing.
26. The system of claim 24 comprising: a. a means for advancing the
tubing into the borehole; b. a bottom hole assembly; c. a blowout
preventer; d. a diverter; e. the bottom hole assembly in fluid and
optical communication with the distal end of the tubing; and, f.
the tubing extending through the blowout preventer and the diverter
and into the borehole, and being capable of advancement through the
blowout preventer and the diverter into and out of the borehole by
the advancing means; g. whereby the laser beam and fluid are
directed by the bottom hole assembly to a surface in the borehole
to advance the borehole.
27. The system of claim 24 wherein the high power laser energy
source provides a laser beam having at least about 10 kW of
power.
28. The system of claim 24 wherein the high power laser energy
source provides a laser beam having at least about 15 kW of
power
29. The system of claim 24 wherein the high power laser energy
source provides a laser beam having at least about 20 kW of
power.
30. The system of claim 27 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 3 kW.
31. The system of claim 27 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 5 kW.
32. The system of claim 27 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 7 kW.
33. A system for providing high power laser energy to the bottom of
deep boreholes, the system comprising: a. a source or high powered
laser energy capable of providing a high power laser beam; b. a
means for transmitting the laser beam from the high power laser to
the bottom of a deep borehole; and, c. the transmitting means
having a means to suppress SBS; d. whereby substantially all of the
high power laser energy is delivered to the bottom of the
borehole.
34. The system of claim 33 wherein the deep borehole is at least
1,000 feet.
35. The system of claim 33 wherein the deep borehole is at least
5,000 feet.
36. The system of claim 33 wherein the deep borehole is at least
10,000 feet.
37. The system of claim 33 wherein the source is at least 10
kW.
38. The system of claim 33 wherein the source is at least 1 kW.
39. The system of claim 33 wherein the source is at least 15
kW.
40. (canceled)
41. 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; 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; and, d.
whereby, high power laser energy is delivered to the bottom of the
borehole with sufficient power to advance the borehole.
42. The system of claim 41 wherein the laser source comprises a
single laser
43. The system of claim 41 wherein the laser source comprises two
lasers
44. The system of claim 41 wherein the laser source comprises a
plurality of lasers
45. A system for providing high power laser energy to the bottom of
deep boreholes, the system comprising: a. a high powered laser
capable of providing a high power laser beam; b. a means for
transmitting the laser beam from the high power laser to the bottom
of a deep borehole; and, c. the transmitting means having a means
for increasing the maximum transmission power; d. whereby, high
power laser energy is delivered to the bottom of the borehole with
sufficient power to advance.
46. A system for providing high power laser energy to the bottom of
deep boreholes, the system comprising: a. a high powered laser
capable of providing a high power laser beam; b. a means for
transmitting the laser beam from the high power laser to the bottom
of a deep borehole; and, c. the transmitting means having a means
for increasing power threshold; d. whereby high power laser energy
is delivered to the bottom of the borehole with sufficient power to
advance the borehole.
47. A method of advancing a borehole using a laser, the method
comprising: a. advancing a high power laser beam transmission means
into a borehole; i. the borehole having a bottom surface, a top
opening, and a length extending between the bottom surface and the
top opening of at least about 1000 feet; ii. the transmission means
comprising a distal end, a proximal end, and a length extending
between the distal and proximal ends, the distal end being advanced
down the borehole; iii. the transmission means comprising a means
for transmitting high power laser energy; b. providing a high power
laser beam to the proximal end of the transmission means; c.
transmitting substantially all of the power of the laser beam down
the length of the transmission means so that the beam exits the
distal end; and, d. directing the laser beam to the bottom surface
of the borehole whereby the length of the borehole is increased, in
part, based upon the interaction of the laser beam with the bottom
of the borehole.
48. 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; b. providing a high
power laser beam to the proximal end of the transmission means; 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.
49. 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 increasing the maximum transmission power; b. providing a high
power laser beam to the proximal end of the transmission means; 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.
50. 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 increasing power threshold; b. providing a high power laser
beam to the proximal end of the transmission means; 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.
51. A high power laser drilling system for advancing a borehole
comprising: a. a source of high power laser energy, the laser
source capable of providing a laser beam having at least 5 kW of
power; b. a tubing assembly, the tubing assembly having at least
1000 feet of tubing, having a distal end and a proximal; c. the
proximal end of the tubing being in optical communication with the
laser source, whereby the laser beam can be transported in
association with the tubing; d. the tubing comprising a high power
laser transmission cable, the transmission cable having a distal
end and a proximal end, the proximal end being in optical
communication with the laser source, whereby the laser beam is
transmitted by the cable from the proximal end to the distal end of
the cable for delivery of the laser beam energy to the borehole;
and, e. the power of the laser energy at the distal end of the
cable when the cable is within a borehole being at least about 2
kW.
52. A high power laser drilling system for advancing a borehole
comprising: a. a source of high power laser energy, the laser
source capable of providing a laser beam having at least 5 kW of
power; b. a tubing, the tubing assembly having at least 1000 feet
of tubing, having a distal end and a proximal; c. a means for
advancing the tubing into the borehole; d. a bottom hole assembly;
e. a blowout preventer; f. a diverter; g. the proximal end of the
tubing being in optical communication with the laser source,
whereby the laser beam can be transported in association with the
tubing; h. the tubing comprising a high power laser transmission
cable, the transmission cable having a distal end and a proximal
end, the proximal end being in optical communication with the laser
source, whereby the laser beam is transmitted by the cable from the
proximal end to the distal end of the cable for delivery of the
laser beam energy to the borehole; and, i. the power of the laser
energy at the distal end of the cable when the cable is within a
borehole being at least about 2 kW.
53-70. (canceled)
71. A laser bottom hole assembly comprising: a. a first rotating
housing; b. a second fixed housing; c. the first housing being
rotationally associated with the second housing; d. a fiber optic
cable for transmitting a laser beam, the cable having a proximal
end and a distal end, the proximal end adapted to receive a laser
beam from a laser source, the distal end optically associated with
an optical assembly; e. at least a portion of the optical assembly
fixed to the first rotating housing, whereby the fixed portion
rotates with the first housing; f. a mechanical assembly fixed to
the first rotating housing, whereby the assembly rotates with the
first housing and is capable of applying mechanical forces to a
surface of a borehole upon rotation; and, g. a fluid path
associated with first and second housings, the fluid path having a
distal and proximal opening, the distal opening adapted to
discharge the fluid toward the surface of the borehole, whereby
fluid for removal of waste material is transmitted by the fluid
path and discharged from the distal opening toward the borehole
surface to remove waste material from the borehole.
72. The assembly of claim 71, wherein the rotating portion of the
optics comprises a beam shaping optic.
73. The assembly of claim 71, wherein the rotating portion of the
optics comprises a scanner.
74. The assembly of claim 71, comprising a rotation motor.
75. The assembly of claim 74, wherein in the rotation motor is a
mud motor.
76. The assembly of claim 71, wherein the mechanical assembly
comprises a conical stand-off device.
77. The assembly of claim 71, wherein the mechanical assembly
comprises a drill bit.
78. The assembly of claim 71, wherein the mechanical assembly
comprises a three-cone drill bit.
79. The assembly of claim 71, wherein the mechanical assembly
comprises a PDC bit.
80. The assembly of claim 71, wherein the mechanical assembly
comprises a PDC tool.
81. The assembly of claim 71, wherein the mechanical assembly
comprises a PDC cutting tool.
82. The assembly of claim 71, wherein the fluid path is adapted to
reduce debris from a laser beam path.
83. A laser bottom hole assembly comprising: a. a first rotating
housing; b. a second fixed housing; c. the first housing being
rotationally associated with the second housing; d. an optical
assembly, the assembly having a first portion and a second portion;
e. a fiber optic cable for transmitting a laser beam, the cable
having a proximal end and a distal end, the proximal end adapted to
receive a laser beam from a laser source, the distal end optically
associated with the optical assembly; f. the fiber proximal and
distal ends fixed to the second housing; g. the first portion of
the optical assembly fixed to the first rotating housing; the
second portion of the optical assembly fixed to the second fixed
housing, whereby the first portion of the optical assembly rotates
with the first housing; h. a mechanical assembly fixed to the first
rotating housing, whereby the assembly rotates with the first
housing and is capable of apply mechanical forces to a surface of a
borehole upon rotation; and, i. a fluid path associated with first
and second housings, the fluid path having a distal and proximal
opening, the distal opening adapted to discharge the fluid toward
the surface of the borehole, the distal opening fixed to the first
rotating housing, whereby fluid for removal of waste material is
transmitted by the fluid path and discharged from the distal
opening toward the borehole surface to remove waste material from
the borehole; j. wherein upon rotation of the first housing the
optical assembly first portion, the mechanical assembly and
proximal fluid opening rotate substantially concurrently.
84. A laser bottom hole assembly comprising: a. a first rotating
housing; b. a second fixed housing; c. the first housing being
rotationally associated with the second housing; d. a motor for
rotating the first housing; e. a fiber optic cable for transmitting
a laser beam, the cable having a proximal end and a distal end, the
proximal end adapted to receive a laser beam from a laser source,
the distal end optically associated with an optical assembly; f. at
least a portion of the optical assembly fixed to the first rotating
housing, whereby the fixed portion rotates with the first housing;
g. a mechanical assembly fixed to the first rotating housing,
whereby the assembly rotates with the first housing and is capable
of apply mechanical forces to a surface of a borehole upon
rotation; and, h. a fluid path associated with first and second
housings, the fluid path having a distal and proximal opening, the
distal opening adapted to discharge the fluid toward the surface of
the borehole, whereby fluid for removal of waste material is
transmitted by the fluid path and discharged from the distal
opening toward the borehole surface to remove waste material from
the borehole.
85. A laser bottom hole assembly comprising: a. a housing; b. a
means for providing a high power laser beam; c. an optical
assembly, the optical assembly providing an optical path upon which
the laser beam travels; and, d. a means for creating an area of
high pressure along the optical path; and, e. a means for providing
aspiration pumping for the removal of waste material from the area
of high pressure.
86. A system for creating a borehole in the earth comprising: a. a
high power laser source; b. a bottom hole assembly; and, c. a fiber
optically connecting the laser source with the bottom hole
assembly, such that a laser beam from the laser source is
transmitted to the bottom hole assembly; d. the bottom hole
assembly comprising: i. a means for providing the laser beam to a
bottom surface of the borehole; ii. the providing means comprising
beam power deposition optics; e. wherein, the laser beam as
delivered from the bottom hole assembly illuminates the bottom
surface of the borehole with a substantially even energy deposition
profile.
87. A system for creating a borehole in the earth comprising: a. a
high power laser source; b. a bottom hole assembly; and, c. a fiber
optically connecting the laser source with the bottom hole
assembly, such that a laser beam from the laser source is
transmitted to the bottom hole assembly; d. the bottom hole
assembly comprising: i. a means for providing the laser beam to a
bottom surface of the borehole; ii. the providing means comprising
beam power deposition optics; and, iii. the means for providing the
laser beam to the bottom surface configured to provide a
predetermined energy deposition profile; e. wherein, the laser beam
as delivered from the bottom hole assembly illuminates the bottom
surface of the borehole with a predetermined energy deposition
profile.
88. The system of claim 87, wherein the predetermined energy
deposition profile is biased toward the outside area of the
borehole surface.
89. The system of claim 87, wherein the predetermined energy
deposition profile is biased toward the inside area of the borehole
surface.
90. The system of claim 87, wherein the predetermined energy
deposition profile is comprises at least two concentric areas
having different energy deposition profiles.
91. The system of claim 87, wherein the predetermined energy
deposition profile is provided by a series of laser shot
patterns.
92. The system of claim 87, wherein the predetermined energy
deposition profile is provided by a scattered laser shot
pattern.
93. The system of claim 87, comprising a mechanical removal
means.
94. The system of claim 93, where in the predetermined energy
deposition profile is based upon the mechanical stresses applied by
the mechanical removal means.
95. The system of claim 93, wherein the predetermined energy
deposition profile has at least two areas of differing energy and
the energies in the areas correspond inversely to the mechanical
forces applied by the mechanical means.
96. A system for creating a borehole in the earth comprising: a. a
high power laser source; b. a bottom hole assembly; and, c. a fiber
optically connecting the laser source with the bottom hole
assembly, such that a laser beam from the laser source is
transmitted to the bottom hole assembly; d. the bottom hole
assembly comprising: i. a means for providing the laser beam shot
pattern to a surface of the borehole in a predetermined shot
pattern and in a predetermined energy deposition profile.
97. A system for creating a borehole in the earth comprising: a. a
high power laser source; b. a bottom hole assembly; and, c. a fiber
optically connecting the laser source with the bottom hole
assembly, such that a laser beam from the laser source is
transmitted to the bottom hole assembly; d. the bottom hole
assembly comprising: i. a means for providing a substantially
elliptical shaped laser beam shot pattern to the bottom surface of
the borehole in a rotating manner to thereby provided a
predetermined shot pattern and a predetermined energy deposition
profile.
98. A method of advancing a borehole using a laser, the method
comprising: a. advancing a high power laser beam transmission means
into a borehole; i. the borehole having a bottom surface, a top
opening, and a length extending between the bottom surface and the
top opening of at least about 1000 feet; ii. the transmission means
comprising a distal end, a proximal end, and a length extending
between the distal and proximal ends, the distal end being advanced
down the borehole; iii. the transmission means comprising a means
for transmitting high power laser energy; b. providing a high power
laser beam to the proximal end of the transmission means; c.
transmitting substantially all of the power of the laser beam down
the length of the transmission means so that the beam exits the
distal end; d. transmitting the laser beam from the distal end to
an optical assembly in a laser bottom hole assembly, e. the laser
bottom hole assembly directing the laser beam to the bottom surface
of the borehole; and, f. providing a predetermined energy
deposition profile to the bottom of the borehole; g. whereby the
length of the borehole is increased, in part, based upon the
interaction of the laser beam with the bottom of the borehole.
99. 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; b. providing a high power laser beam to the
proximal end of the transmission means; c. transmitting the power
of the laser beam down the length of the transmission fiber so that
the beam exits the distal end and enters a laser bottom hole
assembly; and, d. directing the laser beam to the bottom surface of
the borehole in a substantially uniform energy deposition profile;
e. whereby the length of the borehole is increased, in part, based
upon the interaction of the laser beam with the bottom of the
borehole.
100. A method of removing debris from a borehole during laser
drilling of the borehole the method comprising: a. directing a
laser beam comprising a wavelength, and having a power of at least
about 10 kW, down a borehole and towards a surface of a borehole;
b. the surface being at least 1000 feet within the borehole; c. the
laser beam illuminating an area of the surface; d. the laser beam
displacing material from the surface in the area of illumination;
e. directing a fluid into the borehole and to the borehole surface;
f. the fluid being substantially transmissive to the laser
wavelength; g. the directed fluid having a first and a second flow
path; h. the fluid flowing in the first flow path removing the
displaced material from the area of illumination at a rate
sufficient to prevent the displaced material from interfering with
the laser illumination of the area of illumination; and, i. the
fluid flowing in the second flow path removing displaced material
form borehole.
101. The method of claim 100, wherein the illumination area is
rotated.
102. The method of claim 101, wherein the fluid in the first fluid
flow path is directed in the direction of the rotation.
103. The method of claim 101, wherein the fluid in the first fluid
flow path is directed in a direction opposite of the rotation.
104. The method of claim 101, comprising a third fluid flow
path.
105. The method of claim 104, wherein the third fluid low path, and
the first fluid flow path are in the direction of rotation.
106. The method of claim 104, wherein the third fluid low path, and
the first fluid flow path are in a direction opposite to the
direction of rotation.
107. The method of claim 100, wherein the fluid is directed
directly at the area of illumination.
108. The method of claim 101, wherein the fluid in the first flow
path is directed near the area of illumination.
109. The method of claim 101, wherein the fluid in the first fluid
flow path is directed near the area of illumination, which area is
ahead of the rotation.
110. A method of removing debris from a borehole during laser
drilling of the borehole the method comprising: a. directing a
laser beam having at least about 10 kW of power towards a borehole
surface; b. illuminating an area of the borehole surface; c.
displacing material from the area of illumination; d. providing a
fluid; e. directing the fluid toward a first area within the
borehole; f. directing the fluid toward a second area; g. the
directed fluid removing the displaced material from the area of
illumination at a rate sufficient to prevent the displaced material
from interfering with the laser illumination; and, h. the fluid
removing displaced material form borehole.
111. The method of claim 110, wherein the first area is the area of
illumination.
112. The method of claim 110, wherein the second area is on a
sidewall of a bottom hole assembly.
113. The method of claim 110, wherein the second area is near the
first area and the second area is located on a bottom surface of
the borehole.
114. The method of claim 111, wherein the second area is near the
first area and the second area is located on a bottom surface of
the borehole.
115. The method of claim 110, comprising directing a first fluid to
the area of illumination and directing a second fluid to the second
area.
116. The method of claim 115, wherein the first fluid is
nitrogen.
117. The method of claim 115, wherein the first fluid is a gas.
118. The method of claim 115, wherein the second fluid is a
liquid.
119. The method of claim 115, wherein the second fluid is an
aqueous liquid.
120. A method of removing debris from a borehole during laser
drilling of the borehole the method comprising: a. directing a
laser beam towards a borehole surface; b. illuminating an area of
the borehole surface; c. displacing material from the area of
illumination; d. providing a fluid; e. directing the fluid in a
first path toward a first area within the borehole; f. directing
the fluid in a second path toward a second area; g. amplifying the
flow of the fluid in the second path; h. the directed fluid
removing the displaced material from the area of illumination at a
rate sufficient to prevent the displaced material from interfering
with the laser illumination; and, i. the amplified fluid removing
displaced material form borehole.
121. A laser bottom hole assembly for drilling a borehole in the
earth comprising: a. a housing; b. optics for shaping a laser beam;
c. an opening for delivering a laser beam to illuminate the surface
of a borehole; d. a first fluid opening in the housing; e. a second
fluid opening in the housing; and, f. the second fluid opening
comprising a fluid amplifier.
Description
[0001] This application is a divisional application of U.S. patent
application Ser. No. 12/543,986 filed Aug. 19, 2009, which 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.
BACKGROUND OF THE INVENTION
[0003] The present invention relates to methods, apparatus and
systems for delivering advancing boreholes using high power laser
energy that is delivered 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.
[0004] The present invention is useful with and may be employed in
conjunction with the systems, apparatus and methods that are
disclosed in greater detail in co-pending U.S. patent application
Ser. No. 12/544,136, which as issued as U.S. Pat. No. 8,511,401,
titled Method and Apparatus for Delivering High Power Laser Energy
Over Long Distances, U.S. patent application Ser. No. 12/544,038,
titled Apparatus for Advancing a Wellbore using High Power Laser
Energy, U.S. patent application Ser. No. 12/544,094, which issued
as U.S. Pat. No. 8,424,617, titled Methods and Apparatus for
Delivering High Power Laser Energy to a Surface, and U.S. patent
application Ser. No. 12/543,868, which issued as U.S. Pat. No.
8,363,085, titled Methods and Apparatus for Removal and Control of
Material in Laser Drilling of a Borehole, filed contemporaneously
herewith, the disclosures of which are incorporate herein by
reference in their entirety.
[0005] 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.
[0006] 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.degree. i.e., a vertical borehole, to 90.degree.,i.e., a
horizontal borehole and greater than 90.degree. 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.
[0007] 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.
[0008] 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.
[0009] 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.
[0010] 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.
[0011] 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.
[0012] 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.
[0013] 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.
[0014] 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.
[0015] 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.
[0016] 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.
[0017] 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
[0018] 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.
[0019] Thus, there is provided a high power laser drilling system
for use in association with a drilling rig, drilling platform,
drilling derrick, a snubbing platform, or coiled tubing drilling
rig for advancing a borehole, in hard rock, the system comprising:
a source of high power laser energy, the laser source capable of
providing a laser beam having at least 10 kW of power, at least
about 20 kW of power or more; a bottom hole assembly, the bottom
hole assembly having an optical assembly, the optical assembly
configured to provide a predetermined energy deposition profile to
a borehole surface and the optical assembly configured to provide a
predetermined laser shot pattern; a means for advancing the bottom
hole assembly into and down the borehole; a downhole high power
laser transmission cable, the transmission cable having a length of
at least about 500 feet, at least about 1000 feet, at least about
3000 feet, at least about 4000 feet or more; the downhole cable in
optical communication with the laser source; and, the downhole
cable in optical communication with the bottom hole assembly.
[0020] There is further provided a high power laser drilling system
for use in association with a drilling rig, drilling platform,
snubbing platform, drilling derrick, or coiled tubing drilling rig
for advancing a borehole, the system comprising: a source of high
power laser energy; the laser source capable of providing a laser
beam having at least 5 kW, at least about 10 kW, at least about 15
kW and at least about 20 kW or more of power; the laser source
comprising at least one laser; a bottom hole assembly; configured
to provide a predetermined energy deposition profile of laser
energy to a borehole surface; configured to provide a predetermined
laser shot pattern; comprising an optical assembly; and, comprising
a means to mechanically remove borehole material; a means for
advancing the bottom hole assembly into and down the borehole; a
source of fluid for use in advancing a borehole; a downhole high
power laser transmission cable, the transmission cable having a
length of at least about 1000 feet; the downhole cable in optical
communication with the laser source; the downhole cable in optical
communication with the optical assembly; and, the bottom hole
assembly in fluid communication with the fluid source; whereby high
power laser energy may be provided to a surface of a borehole at
locates within the borehole at least 1000 feet from the borehole
opening.
[0021] Yet further there is provided a high power laser drilling
system for use in association with a drilling rig, drilling
platform, drilling derrick, a snubbing platform, or coiled tubing
drilling rig for advancing a borehole, the system comprising: a
source of high power laser energy; a bottom hole assembly; the
bottom hole assembly having an optical assembly; the optical
assembly configured to provide an energy deposition profile to a
borehole surface; and, the optical assembly configured to provide a
laser shot pattern; comprising a means for directing a fluid; a
means for advancing the bottom hole assembly into and down the
borehole; a source of fluid for use in advancing a borehole; a
downhole high power laser transmission cable; the downhole cable in
optical communication with the laser source; the downhole cable in
optical communication with the bottom hole assembly; and, the means
for directing in fluid communications with the fluid source;
wherein the system is capable of cutting, spalling, or chipping
rock by Illuminating a surface of the borehole with laser energy
and remove waste material created from said cutting, spalling or
chipping, from the borehole and the area of laser Illumination by
the action of the directing means. Wherein the means for directing
may be, one or more of and combinations thereof a fluid amplifier,
an outlet port, a gas directing means, a fluid directing means, and
an air knife.
[0022] Additionally, there is provided a laser bottom hole assembly
comprising: a first rotating housing; a second fixed housing; the
first housing being rotationally associated with the second
housing; a fiber optic cable for transmitting a laser beam, the
cable having a proximal end and a distal end, the proximal end
adapted to receive a laser beam from a laser source, the distal end
optically associated with an optical assembly; at least a portion
of the optical assembly fixed to the first rotating housing,
whereby the fixed portion rotates with the first housing; a
mechanical assembly fixed to the first rotating housing, whereby
the assembly rotates with the first housing and is capable of
applying mechanical forces to a surface of a borehole upon
rotation; and, a fluid path associated with first and second
housings, the fluid path having a distal and proximal opening, the
distal opening adapted to discharge the fluid toward the surface of
the borehole, whereby fluid for removal of waste material is
transmitted by the fluid path and discharged from the distal
opening toward the borehole surface to remove waste material from
the borehole.
[0023] There is further provided a laser bottom hole assembly
comprising: a first rotating housing; a second fixed housing; the
first housing being rotationally associated with the second
housing; an optical assembly, the assembly having a first portion
and a second portion; a fiber optic cable for transmitting a laser
beam, the cable having a proximal end and a distal end, the
proximal end adapted to receive a laser beam from a laser source,
the distal end optically associated with the optical assembly; the
fiber proximal and distal ends fixed to the second housing; the
first portion of the optical assembly fixed to the first rotating
housing; the second portion of the optical assembly fixed to the
second fixed housing, whereby the first portion of the optical
assembly rotates with the first housing; a mechanical assembly
fixed to the first rotating housing, whereby the assembly rotates
with the first housing and is capable of apply mechanical forces to
a surface of a borehole upon rotation; and, a fluid path associated
with first and second housings, the fluid path having a distal and
proximal opening, the distal opening adapted to discharge the fluid
toward the surface of the borehole, the distal opening fixed to the
first rotating housing, whereby fluid for removal of waste material
is transmitted by the fluid path and discharged from the distal
opening toward the borehole surface to remove waste material from
the borehole; wherein upon rotation of the first housing the
optical assembly first portion, the mechanical assembly and
proximal fluid opening rotate substantially concurrently.
[0024] Additionally there is provided a laser bottom hole assembly
comprising: a housing; a means for providing a high power laser
beam; an optical assembly, the optical assembly providing an
optical path upon which the laser beam travels; and, a an air flow
and chamber for creating an area of high pressure along the optical
path; and, a an air flow through a housing of the bottom hole
assembly with ports that function as an aspiration pumping for the
removal of waste material from the area of high pressure.
[0025] Furthermore, these systems and assemblies may further have
rotating laser optics, a rotating mechanical interaction device, a
rotating fluid delivery means, one or all three of these devices
rotating together, beam shaping optic, housings, a means for
directing a fluid for removal of waste material, a means for
keeping a laser path free of debris, a means for reducing the
interference of waste material with the laser beam, optics
comprising a scanner; a stand-off mechanical device, a conical
stand-off device, a mechanical assembly comprises a drill bit, a
mechanical assembly comprising a three-cone drill bit, a mechanical
assembly comprises a PDC bit, a PDC tool or a PDC cutting tool.
[0026] Still further, there is provided a system for creating a
borehole in the earth having a high power laser source, a bottom
hole assembly and, a fiber optically connecting the laser source
with the bottom hole assembly, such that a laser beam from the
laser source is transmitted to the bottom hole assembly the bottom
hole assembly comprising: a means for providing the laser beam to a
bottom surface of the borehole; the providing means comprising beam
power deposition optics; wherein, the laser beam as delivered from
the bottom hole assembly illuminates the bottom surface of the
borehole with a substantially even energy deposition profile.
[0027] There is yet further provided a method of advancing a
borehole using a laser, the method comprising: 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; transmitting the laser beam
from the distal end to an optical assembly in a laser bottom hole
assembly, the laser bottom hole assembly directing the laser beam
to the bottom surface of the borehole; and, providing a
predetermined energy deposition profile to the bottom 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.
[0028] Additionally, there is provided a method of removing debris
from a borehole during laser drilling of the borehole the method
comprising: directing a laser beam comprising a wavelength, and
having a power of at least about 10 kW, down a borehole and towards
a surface of a borehole; the surface being at least 1000 feet
within the borehole; the laser beam illuminating an area of the
surface; the laser beam displacing material from the surface in the
area of illumination; directing a fluid into the borehole and to
the borehole surface; the fluid being substantially transmissive to
the laser wavelength; the directed fluid having a first and a
second flow path; the fluid flowing in the first flow path removing
the displaced material from the area of illumination at a rate
sufficient to prevent the displaced material from interfering with
the laser illumination of the area of illumination; and, the fluid
flowing in the second flow path removing displaced material form
borehole. Additionally, the forging method may also have the
illumination area rotated, the fluid in the first fluid flow path
directed in the direction of the rotation, the fluid in the first
fluid flow path directed in a direction opposite of the rotation, a
third fluid flow path, the third fluid low path and the first fluid
flow path in the direction of rotation, the third fluid low path
and the first fluid flow path in a direction opposite to the
direction of rotation, the fluid directed directly at the area of
illumination, the fluid in the first flow path directed near the
area of illumination, and the fluid in the first fluid flow path
directed near the area of illumination, which area is ahead of the
rotation.
[0029] There is yet further provided a method of removing debris
from a borehole during laser drilling of the borehole the method
comprising: directing a laser beam having at least about 10 kW of
power towards a borehole surface; illuminating an area of the
borehole surface; displacing material from the area of
illumination; providing a fluid; directing the fluid toward a first
area within the borehole; directing the fluid toward a second area;
the directed fluid removing the displaced material from the area of
illumination at a rate sufficient to prevent the displaced material
from interfering with the laser Illumination; and, the fluid
removing displaced material form borehole. This further method may
additionally have the first area as the area of Illumination, the
second area on a sidewall of a bottom hole assembly, the second
area near the first area and the second area located on a bottom
surface of the borehole, the second area near the first area when
the second area is located on a bottom surface of the borehole, a
first fluid directed to the area of illumination and a second fluid
directed to the second area, the first fluid as nitrogen, the first
fluid as a gas, the second fluid as a liquid, and the second fluid
as an aqueous liquid.
[0030] Yet, further there is provided a method of removing debris
from a borehole during laser drilling of the borehole the method
comprising: directing a laser beam towards a borehole surface;
Illuminating an area of the borehole surface; displacing material
from the area of illumination; providing a fluid; directing the
fluid in a first path toward a first area within the borehole;
directing the fluid in a second path toward a second area;
amplifying the flow of the fluid in the second path; the directed
fluid removing the displaced material from the area of illumination
at a rate sufficient to prevent the displaced material from
interfering with the laser illumination; and, the amplified fluid
removing displaced material form borehole.
[0031] Moreover, there is provided a laser bottom hole assembly for
drilling a borehole in the earth comprising: a housing; optics for
shaping a laser beam; an opening for delivering a laser beam to
illuminate the surface of a borehole; a first fluid opening in the
housing; a second fluid opening in the housing; and, the second
fluid opening comprising a fluid amplifier.
[0032] Still further, a high power laser drilling system for
advancing a borehole is provided that comprises: a source of high
power laser energy, the laser source capable of providing a laser
beam; a tubing assembly, the tubing assembly having at least 500
feet of tubing, having a distal end and a proximal; a source of
fluid for use in advancing a borehole; the proximal end of the
tubing being in fluid communication with the source of fluid,
whereby fluid is transported in association with the tubing from
the proximal end of the tubing to the distal end of the tubing; 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; and, a laser bottom hole assembly in optical and fluid
communication with the distal end of the tubing; and, the laser
bottom hole assembly comprising; a housing; an optical assembly,
and, a fluid directing opening. This system may be supplemented by
also having the fluid directing opening as an air knife, the fluid
directing opening as a fluid amplifier, the fluid directing opening
is an air amplifier, a plurality of fluid directing apparatus, the
bottom hole assembly comprising a plurality of fluid directing
openings, the housing comprising a first housing and a second
housing; the fluid directing opening located in the first housing,
and a means for rotating the first housing, such as a motor,
[0033] There is yet further 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; a
tubing assembly, the tubing assembly having at least 500 feet of
tubing, having a distal end and a proximal; a source of fluid for
use in advancing a borehole; the proximal end of the tubing being
in fluid communication with the source of fluid, whereby fluid is
transported in association with the tubing from the proximal end of
the tubing to the distal end of the tubing; 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; and, a laser bottom
hole assembly in optical and fluid communication with the distal
end of the tubing; and, a fluid directing means for removal of
waste material.
[0034] Further such systems may additionally have the fluid
directing means located in the laser bottom hole assembly, the
laser bottom hole assembly having a means for reducing the
interference of waste material with the laser beam, the laser
bottom hole assembly with rotating laser optics, and the laser
bottom hole assembly with rotating laser optics and rotating fluid
directing means.
[0035] 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
[0036] 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.
[0037] FIG. 2 is a view of a spool.
[0038] FIGS. 3A and 3B are views of a creel.
[0039] FIG. 4 is schematic diagram for a configuration of
lasers.
[0040] FIG. 5 is a schematic diagram for a configuration of
lasers.
[0041] FIG. 6 is a perspective cutaway of a spool and optical
rotatable coupler.
[0042] FIG. 7 is a schematic diagram of a laser fiber
amplifier.
[0043] FIG. 8 is a perspective cutaway of a bottom hole
assembly.
[0044] FIG. 9 is a cross sectional view of a portion of an
LBHA.
[0045] FIG. 10 is a cross sectional view of a portion of an
LBHA
[0046] FIG. 11 is an LBHA.
[0047] FIG. 12 is a perspective view of a fluid outlet.
[0048] FIG. 13 is a perspective view of an air knife assembly fluid
outlet.
[0049] FIG. 14A is a perspective view of an LBHA.
[0050] FIG. 148 is a cross sectional view of the LBHA of FIG. 14A
taken along B-B.
[0051] FIGS. 15A and 15B, is a graphic representation of an example
of a laser beam basalt illumination.
[0052] FIGS. 16A and 16B illustrate the energy deposition profile
of an elliptical spot rotated about its center point for a beam
that is either uniform or Gaussian.
[0053] FIG. 17A shows the energy deposition profile with no
rotation.
[0054] FIG. 17B shows the substantially even and uniform energy
deposition profile upon rotation of the beam that provides the
energy deposition profile of FIG. 17A.
[0055] FIGS. 18A to 18D illustrate an optical assembly.
[0056] FIG. 19 illustrates an optical assembly.
[0057] FIG. 20 illustrates an optical assembly.
[0058] FIGS. 21A and 21 B Illustrate an optical assembly.
[0059] FIG. 22 illustrates a multi-rotating laser shot pattern.
[0060] FIG. 23 illustrates an elliptical shaped shot.
[0061] FIG. 24 illustrates a rectangular shaped spot.
[0062] FIG. 25 illustrates a multi-shot shot pattern.
[0063] FIG. 26 illustrates a shot pattern.
[0064] FIGS. 27 to 36 illustrate LBHAs.
DESCRIPTION OF THE DRAWINGS AND THE PREFERRED EMBODIMENTS
[0065] 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.
[0066] 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.
[0067] 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.
[0068] 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.
[0069] 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.
[0070] 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 retums 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.
[0071] 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.
[0072] 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.
[0073] 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.
[0074] 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.
[0075] 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.
[0076] 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 M.sup.2 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.
[0077] 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+.delta.1
microns, where .delta.1 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+.delta.1+.delta.2
microns and a fourth laser 4004 having a wavelength of
x+.delta.1+.delta.2+.delta.3 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.
[0078] 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 .delta. 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.
[0079] The laser source may be a low order mode source
(M.sup.2<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.
[0080] 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.
[0081] 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-US-00001 TABLE 1 Optical Characteristics Characteristics Test
conditions Symbol Min. Typ. Max Unit Operation Mode CW, QCW
Polarization Random Nominal Output Power P.sub.NOM 20000* W Output
Power Tuning Range 10 100 % Emission Wavelength P.sub.OUT = 20 kW
1070 1080 nm Emission Linewidth P.sub.OUT = 20 kW 3 6 nm Switching
ON/OFF Time P.sub.OUT = 20 kW 80 100 .mu.sec Output Power
Modulation Rate P.sub.OUT = 20 kW 5.0 kHz Output Power Stability
Over 8 hrs, 1.0 2.0 % T.sub.WATER = Const Feeding Fiber Core
Diameter 200 .mu.m Beam Parameter Product 200 .mu.m 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 P.sub.OUT = 20 kW 75 80 kW
Operating Temperature Range +15 +40 .degree. C. Humidity: without
conditioner T < 25.degree. C. 90 % with built-in conditioner T
< 40.degree. C. 95 Storage Temperature Without water -40 +75
.degree. C. Dimensions, H .times. W .times. D NEMA-12; IP-55 1490
.times. 1480 .times. 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.
[0082] 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.
[0083] 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 CO.sub.2
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.
[0084] 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.
[0085] 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.
[0086] 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.
[0087] 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.degree. C. to about 100.degree. C. For a fiber laser its
operating temperature may be between about 20.degree. C. to about
50.degree. 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.
[0088] 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 extemal coolant may also be used.
[0089] 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.
[0090] 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.
[0091] 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-US-00002 TABLE 2 Chiller PC400.01-NZ-DIS Technical Data for
60 Hz operation: IPG-Laser type Cooling capacity net YLR-15000,
YLR-20000 Refrigerant 60.0 kW Necessary air flow R407C Installation
26100 m.sup.3/h Number of compressors Outdoor installation Number
of fans 2 Number of pumps 3 2 Operation Limits Designed Operating
Temperature 33.degree. C. (92 F.) Operating Temperature min. (-)
20.degree. C. (-4 F.) Operating Temperature max. 39.degree. C. (102
F.) Storage Temperature min. (with empty water tank) (-) 40.degree.
C. (-40 F.) Storage Temperature max. 70.degree. 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.degree. C. (70 F.)
Water inlet temperature 26.degree. 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.degree. C. (79 F.) Water inlet temperature 31.degree. C. (88 F.)
Temperature stability +/-1.0 K Water flow vs. water pressure free
available 20 l/min at 1.5 bar (5.28 GPM at 21 PSI) Waterflow vs.
water pressure free available 15 l/min at 4.0 bar (3.96 GPM at 58
PSI) Options (included) Bifrequent version: 400 V/3 Ph/50 Hz 460
V/3 Ph 60 Hz
[0092] 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.
[0093] 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.
[0094] 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.
[0095] 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.
[0096] 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''.
[0097] 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.
[0098] 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.
[0099] 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.
[0100] 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.
[0101] 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.
[0102] The hollow axle 2004 then transmits the laser beam to an
opening 2007 in the hollow axle 2004, which opening contains an
optical coupler 2010 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.
[0103] 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.
[0104] 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.
[0105] 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.
[0106] 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 N.sub.2.
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.
[0107] 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
[0108] 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.
[0109] 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.
[0110] 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.
[0111] 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.
[0112] 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,
C0.sub.2 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
polylmide 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.
[0113] 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 10 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.
[0114] Thus, by way of example there is provided the following
configurations set forth in Table 3 herein.
TABLE-US-00003 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
[0115] 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.
[0116] 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.
[0117] 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.
[0118] 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.
[0119] 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.
[0120] 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.
[0121] 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.
[0122] 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.
[0123] The interaction of the source linewidth and the Brillioun
linewidth in part defines the gain function. Varying the Iinewidth
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.
[0124] 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.
[0125] 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.
[0126] 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.
[0127] 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.
[0128] 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 may be
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 may be 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.
[0129] Thus, there is provided in Tables 4 and 5 herein power
transmissions for exemplary optical cable configurations.
TABLE-US-00004 TABLE 4 Length Power of Diameter # of fibers Power
in fiber(s) of bundle in bundle out 20 kW 5 km 500 microns 1 15 kW
20 kW 7 km 500 microns 1 13 kW 20 kW 5 km 200 microns-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-US-00005 TABLE 5 (with active amplification) Length Power of
Diameter # of fibers Power in fiber(s) of bundle in bundle out 20
kW 5 km 500 microns 1 17 kW 20 kW 7 km 500 microns 1 15 kW 20 kW 5
km 200 microns-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
[0130] 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.
[0131] 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 being 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.
[0132] 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 retum signal on the high power optical fiber, the
integrity of the fiber can be determined.
[0133] 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.
[0134] 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.
[0135] 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.
[0136] 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.
[0137] The bottom hole assembly contains the laser optics, the
delivery means for the fluid and other equipment. 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.
[0138] The present systems and in particular the bottom hole
assembly, may Include one or more optical manipulators. An optical
manipulator may generally control a laser beam, such as by
directing or positioning the laser beam to spall material, such as
rock. In some configurations, an optical manipulator may
strategically guide a laser beam to spall material, such as rock.
For example, spatial distance from a borehole wall or rock may be
controlled, as well as the impact angle. In some configurations,
one or more steerable optical manipulators may control the
direction and spatial width of the one or more laser beams by one
or more reflective mirrors or crystal reflectors. In other
configurations, the optical manipulator can be steered by an
electro-optic switch, electroactive polymers, galvonometers,
plezoelectrics, 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 may be
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.
[0139] 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
N.sub.2. 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.
[0140] 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.
[0141] In general, the LBHA may contain an outer housing that is
capable of withstanding the conditions of a downhole environment, a
source of a high power laser beam, and optics for the shaping and
directing a laser beam on the desired surfaces of the borehole,
casing, or formation. The high power laser beam may be greater than
about 1 kW, from about 2 kW to about 20 kW, greater than about 5
kW, from about 5 kW to about 10 kW, preferably at least about 10
kW, at least about 15 kW, and at least about 20 kW. The assembly
may further contain or be associated with a system for delivering
and directing fluid to the desired location in the borehole, a
system for reducing or controlling or managing debris in the laser
beam path to the material surface, a means to control or manage the
temperature of the optics, a means to control or manage the
pressure surrounding the optics, and other components of the
assembly, and monitoring and measuring equipment and apparatus, as
well as, other types of downhole equipment that are used in
conventional mechanical drilling operations. Further, the LBHA may
incorporate a means to enable the optics to shape and propagate the
beam which for example would include a means to control the index
of refraction of the environment through which the laser is
propagating. Thus, as used herein the terms control and manage are
understood to be used in their broadest sense and would include
active and passive measures as well as design choices and materials
choices.
[0142] The LBHA should be construed to withstand the conditions
found in boreholes including boreholes having depths of about 1,640
ft (0.5 km) or more, about 3,280 ft (1 km) or more, about 9,830 ft
(3 km) or more, about 16,400 ft (5 km) or more, and up to and
including about 22,970 ft (7 km) or more. While drilling, i.e.
advancement of the borehole, is taking place the desired location
in the borehole may have dust, drilling fluid, and/or cuttings
present. Thus, the LBHA should be constructed of materials that can
withstand these pressures, temperatures, flows, and conditions, and
protect the laser optics that are contained in the LBHA. Further,
the LBHA should be designed and engineered to withstand the
downhole temperatures, pressures, and flows and conditions while
managing the adverse effects of the conditions on the operation of
the laser optics and the delivery of the laser beam.
[0143] The LBHA should also be constructed to handle and deliver
high power laser energy at these depths and under the extreme
conditions present in these deep downhole environments. Thus, the
LBHA and its laser optics should be capable of handling and
delivering laser beams having energies of 1 kW or more, 5 kW or
more, 10 kW or more and 20 kW or more. This assembly and optics
should also be capable of delivering such laser beams at depths of
about 1,640 ft (0.5 km) or more, about 3,280 ft (1 km) or more,
about 9,830 ft (3 km) or more, about 16,400 ft (5 km) or more, and
up to and including about 22,970 ft (7 km) or more.
[0144] The LBHA should also be able to operate in these extreme
downhole environments for extended periods of time. The lowering
and raising of a bottom hole assembly has been referred to as
tripping in and tripping out. While the bottom hole assembling is
being tripped in or out the borehole is not being advanced. Thus,
reducing the number of times that the bottom hole assembly needs to
be tripped in and out will reduce the critical path for advancing
the borehole, i.e., drilling the well, and thus will reduce the
cost of such drilling. (As used herein the critical path referrers
to the least number of steps that must be performed in serial to
complete the well.) This cost savings equates to an increase in the
drilling rate efficiency. Thus, reducing the number of times that
the bottom hole assembly needs to be removed from the borehole
directly corresponds to reductions in the time it takes to drill
the well and the cost for such drilling. Moreover, since most
drilling activities are based upon day rates for drilling rigs,
reducing the number of days to complete a borehole will provided a
substantial commercial benefit. Thus, the LBHA and its laser optics
should be capable of handling and delivering laser beams having
energies of 1 kW or more, 5 kW or more, 10 kW or more and 20 kW or
more at depths of about 1,640 ft (0.5 km) or more, about 3,280 ft
(1 km) or more, about 9,830 ft (3 km) or more, about 16,400 ft (5
km) or more, and up to and including about 22,970 ft (7 km) or
more, for at least about % hr or more, at least about 1 hr or more,
at least about 2 hours or more, at least about 5 hours or more, and
at least about 10 hours or more, and preferably longer than any
other limiting factor in the advancement of a borehole. In this way
using the LBHA of the present invention could reduce tripping
activities to only those that are related to casing and completion
activities, greatly reducing the cost for drilling the well.
[0145] Thus, in general the 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.
[0146] There is provided in FIG. 9 an illustration of an example of
a LBHA configuration with two fluid outlet ports shown in the
Figure. This example employees the use of fluid amplifiers and in
particular for this illustration air amplifier techniques to remove
material from the borehole. Thus, there is provided a section of an
LBHA 9101, having a first outlet port 9103, and a second outlet
port 9105. The second outlet port, as configured, provides a means
to amplify air, or a fluid amplification means. The first outlet
port 9103 also provides an opening for the laser beam and laser
path. There is provided a first fluid flow path 9107 and a second
fluid flow path 9109. There is further a boundary layer 9111
associated with the second fluid flow path 9109. The distance
between the first outlet 9103 and the bottom of the borehole 9112
is shown by distance y and the distance between the second outlet
port 9105 and the side wall of the borehole 9114 is shown by
distance x. Having the curvature of the upper side 9115 of the
second port 9105 is important to provide for the flow of the fluid
to curve around and move up the borehole. Additionally, having the
angle 9116 formed by angled surface 9117 of the lower side 9119 is
similarly important to have the boundary layer 9111 associate with
the fluid flow 9109. Thus, the second flow path 9109 is primarily
responsible for moving waste material up and out of the borehole.
The first flow path 9117 is primarily responsible for keeping the
optical path optically open from debris and reducing debris in that
path and further responsible for moving waste material from the
area below the LBHA to its sides and a point where it can be
carried out of the borehole by second flow 9105.
[0147] It is presently believed that the ratio of the flow rates
between the first and the second flow paths should be from about
100% for the first flow path, 1:1, 1:10, to 1:100. Further, the use
of fluid amplifiers are exemplary and it should be understood that
a LBHA, or laser drilling in general, may be employed without such
amplifiers. Moreover, fluid jets, air knives, or similar fluid
directing means many be used in association with the LBHA, in
conjunction with amplifiers or in lieu of amplifiers. A further
example of a use of amplifiers would be to position the amplifier
locations where the diameter of the borehole changes or the area of
the annulus formed by the tubing and borehole change, such as the
connection between the LBHA and the tubing. Further, any number of
amplifiers, jets or air knifes, or similar fluid directing devices
may be used, thus no such devices may be used, a pair of such
devices may be used, and a plurality of such devices may be use and
combination of these devices may be used. The cuttings or waste
that is created by the laser (and the laser-mechanical means
interaction) have terminal velocities that must be overcome by the
flow of the fluid up the borehole to remove them from the borehole.
Thus for example if cuttings have terminal velocities of for
sandstone waste from about 4 m/sec. to about 7 m/sec., granite
waste from about 3.5 m/sec. to 7 m/sec., basalt waste from about 3
m/sec. to 8 m/sec., and for limestone waste less than 1 m/sec these
terminal velocities would have to be overcome.
[0148] In FIG. 10 there is provided an example of a LBHA. Thus
there is shown a portion of a LBHA 100, having a first port 103 and
a second port 105. In this configuration the second port 105, in
comparison to the configuration of the example in FIG. 3, is moved
down to the bottom of the LBHA. There second port provides for a
flow path 109 that can be viewed has two paths; an essentially
horizontal path 113 and a vertical path 111. There is also a flow
path 107, which is primarily to keep the laser path optically clear
of debris. Flow paths 113 and 107 combine to become part of path
111.
[0149] There is provided in FIG. 12 an example of a rotating outlet
port that may be part of or associated with a LBHA, or employed in
laser drilling. Thus, there is provided a port 1201 having an
opening 1203. The port rotates in the direction of arrows 1205. The
fluid is then expelled from the port in two different angularly
directed flow paths. Both flow paths are generally in the direction
of rotation. Thus, there is provided a first flow path 1207 and a
second flow path 1209. The first flow path has an angle "a" with
respect to and relative to the outlet's rotation. The second flow
path has an angle "b" with respect to and relative to the outlet's
rotation. In this way the fluid may act like a knife or pusher and
assist in removal of the material.
[0150] The illustrative outlet port of FIG. 12 may be configured to
provide flows 1207 and 1209 to be in the opposite direction of
rotation, the outlet may be configured to provide flow 1207 in the
direction of the rotation and flow 1209 in a direction opposite to
the rotation. Moreover, the outlet may be configured to provide a
flow angles a and b that are the same or are different, which flow
angles can range from 90.degree. to almost 0.degree. and may be in
the ranges from about 80.degree. to 10.degree., about 70.degree. to
20, about 60.degree. to 30.degree., and about 50.degree. to
40.degree., including variations of these where "a" is a different
angle and/or direction than "b."
[0151] There is provided in FIG. 13 an example of an air knife
configuration that is associated with a LBHA. Thus, there is
provided an air knife 1301 that is associated with a LBHA 1313. In
this manner the air knife and its related fluid flow can be
directed in a predetermined manner, both with respect to angle and
location of the flow. Moreover, in additional to air knives, other
fluid directing and delivery devices, such as fluid jets may be
employed.
[0152] 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
[0153] 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.times.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.
TABLE-US-00006 Experimental Setup Fiber Laser IPG Photonics 5 kW
ytterbium-doped multi-clad fiber laser Dolomite/Barre Granite 12''
.times. 12'' .times. 5'' or and 5'' .times. 5'' .times. 5'' Rock
Size Limestone 12'' .times. 12'' .times. 5'' or and5'' .times. 5''
.times. 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
TABLE-US-00007 [0154] 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'' .times. 12'' .times. 5''and5'' .times. 5''
.times. 5'' Sandstone Shale 12'' .times. 12'' .times. 5''and 5''
.times. 5'' .times. 5'' Beam Type CW/Collimated Beam Spot Size (or
0.0625'' (12.5 mm .times. 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
[0155] 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''.times.1''.times.1'' sized
rock particles will be the goal. Applied SP and SE will be selected
based on previously recorded spallation data and information
gleaned from Experiments 1 and 2 presented above. ROP to chip the
rock will be determined, and the ability to chip rock to desired
specifications will be demonstrated.
TABLE-US-00008 Experimental Setup Fixed: Fiber Laser IPG Photonics
5 kW ytterbium-doped multi-clad fiber laser Dolomite/Barre 12''
.times. 12'' .times. 12'' and12'' .times. 12'' .times. 24'' Granite
Rock Size Limestone 12'' .times. 12'' .times. 12'' and12'' .times.
12'' .times. 24'' Berea Gray 12'' .times. 12'' .times. 12'' and12''
.times. 12'' .times. 24'' (or Yellow) Sandstone Shale 12'' .times.
12'' .times. 12''and12'' .times. 12'' .times. 24'' Beam Type
CW/CollimatedandPulsed 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 .times. 0.5
mm Exposure Times See Experiments 1 & 2 Purging 189 l/min
Nitrogen Flow
Example 4
[0156] 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''.times.1''.times.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 spell and ROP for optimization.
TABLE-US-00009 Experimental Setup Fiber Laser IPG Photonics 5 kW
ytterbium-doped multi- clad fiber laser Dolomite/Barre 5'' .times.
5'' .times. 5'' Granite Rock Size Limestone 5'' .times. 5'' .times.
5'' Berea Gray 5'' .times. 5'' .times. 5'' (or Yellow) Sandstone
Shale 5'' .times. 5'' .times. 5'' Beam Type CW/Collimated or Pulsed
atSpallation 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 .times. 0.5 mm Exposure Times See
Experiments 1 & 2 Purging 1891/min Nitrogen Flow Distance
between 0.2'', 0.5'', 1'', 1.5'' two laser beams
Example 5
[0157] 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.times.15.24 cm, an elliptical spot with
major axis approximately 15.24 cm and minor axis approximately 1
cm, a single circular spot having a diameter of 1 cm, an array of
spots having a diameter of 1 cm with the spacing between the spots
being approximately equal to the spot diameter, the array having 4
spots spaced in a square, spaced along a line. The laser beam will
be delivered to the rock surface in a shot sequence pattern wherein
the laser is fired until spallation occurs and then the laser is
directed to the next shot in the pattern and then fired until
spallation occurs with this process being repeated. In the movement
of the linear and elliptical patterns the spots are in effect
rotated about their central axis. In the pattern comprising the
array of spots the spots may be rotated about their central axis,
and rotated about an axis point as in the hands of a clock moving
around a face.
TABLE-US-00010 Experimental Setup Fiber Laser IPG Photonics 5 kW
ytterbium-doped multi-clad fiber laser Dolomite/Barre 12'' .times.
12'' .times. 12'' and12'' .times. 12'' .times. 5'' Granite Rock
Size Limestone 12'' .times. 12'' .times. 12'' and12'' .times. 12''
.times. 5'' Berea Gray 12'' .times. 12'' .times. 12'' and12''
.times. 12'' .times. 5'' (or Yellow) Sandstone Shale 12'' .times.
12'' .times. 12'' and12'' .times. 12'' .times. 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 .times. 0.5
mm Exposure Times See Experiments 1 & 2 Purging 189 l/min
Nitrogen Flow
[0158] From the foregoing examples and detailed teaching it can be
seen that in general one or more laser beams may spall, chip,
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.
[0159] 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
TABLE-US-00011 [0160] Drilling type/Laser Depth Rock type power
down hole Drill 171/2 Surface-3000 ft.sup. Sand and Conventional
inch hole shale mechanical drilling Run 133/8 Length 3000 ft inch
casing Drill 121/4 3000 ft-8,000 ft basalt 40 kW inch hole
(minimum) Run 95/8 Length 8,000 ft inch casing Drill 81/2 8,000
ft-11,000 ft limestone Conventional inch hole mechanical drilling
Run 7 Length 11,000 ft inch casing Drill 61/4 11,000 ft-14,000 ft
Sand stone Conventional inch hole mechanical drilling Run 5 Length
3000 ft inch liner
Drilling Plan Example 2
TABLE-US-00012 [0161] Drilling type/Laser Depth Rock type power
down hole Drill 171/2 Surface-500 ft .sup. Sand and Conventional
inch hole shale mechanical drilling Run 133/8 Length 500 ft casing
Drill 121/4 .sup. 500 ft-4,000 ft granite 40 kW hole (minimum) Run
95/8 Length 4,000 ft inch casing Drill 81/2 4,000 ft-11,000 ft
basalt 20 kW inch hole (minimum) Run 7 Length 11,000 ft inch casing
Drill 61/4 11,000 ft-14,000 ft Sand stone Conventional inch hole
mechanical drilling Run 5 Length 3000 ft inch liner
[0162] 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.
[0163] 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/perfluimated 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.
[0164] 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 retum cuttings and debris to the surface by applying
pressure uphole drawing incompressible fluid to the surface.
[0165] 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.
[0166] 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.
[0167] 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.
[0168] 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.
[0169] 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.
[0170] In accordance with one or more configurations, a fiber laser
or infrared diode laser downhole may transmit coherent light down a
hollow tube without the light coming in contact with the tube when
placed downhole. The hollow tube may be composed of any material.
In some configurations, the hollow tube may be composed of steel,
titanium or silica. A mirror or reflective crystal may be placed at
the end of the hollow tube to direct collimated light to the
material, such as a rock surface being drilled. In some
embodiments, the optical manipulator can be steered by an
electro-optic switch, electroactive polymers, galvonometers,
piezoelectrics, or rotary/linear motors. A circulation system may
be used to raise cuttings. One or more liquid pumps may be used to
return cuttings to the surface by applying pressure uphole, drawing
incompressible fluid to the surface. In some configurations, the
optical fiber may be attached to a conduit with two tubes, one to
apply gas or liquid to circulate the cuttings and one to supply gas
or liquid to a Laval nozzle jet to clear debris from the laser
head.
[0171] 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.
[0172] 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.
[0173] Thus, by way of example, an LBHA is illustrated in FIGS. 14A
and B, which are collectively referred as FIG. 14. There is
provided a LBHA 14100, which has an upper part 1400 and a lower
part 1401. The upper part 1400 has housing 1418 and the lower part
1401 has housing 1419. The LBHA 14100, the upper part 1400, the
lower part 1401 and in particular the housings 1418, 1419 should be
constructed of materials and designed structurally to withstand the
extreme conditions of the deep downhole environment and protect any
of the components that are contained within them.
[0174] The upper part 1400 may be connected to the lower end of the
coiled tubing, drill pipe, or other means to lower and retrieve the
LBHA 14100 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 LBHA 14100 from the borehole. The upper part 1400
further contains, is connect to, or otherwise optically associated
with the means 1402 that transmitted the high power laser beam down
the borehole so that the beam exits the lower end 1403 of the means
1402 and ultimately exits the LBHA 14100 to strike the intended
surface of the borehole. The beam path of the high power laser beam
is shown by arrow 1415. In FIG. 14 the means 1402 is shown as a
single optical fiber. The upper part 1400 may also have air
amplification nozzles 1405 that discharge the drilling fluid, for
example N.sub.2, to among other things assist in the removal of
cuttings up the borehole.
[0175] The upper part 1400 further is attached to, connected to or
otherwise associated with a means to provide rotational movement
1410. Such means, for example, would be a downhole motor, an
electric motor or a mud motor. The motor may be connected by way of
an axle, drive shaft, drive train, gear, or other such means to
transfer rotational motion 1411, to the lower part 1401 of the LBHA
14100. It is understood, as shown in the drawings for purposes of
illustrating the underlying apparatus, that a housing or protective
cowling may be placed over the drive means or otherwise associated
with it and the motor to protect it form debris and harsh down hole
conditions. In this manner the motor would enable the lower part
1401 of the LBHA 14100 to rotate. An example of a mud motor is the
CAVO 1.7'' diameter mud motor. This motor is about 7 ft long and
has the following specifications: 7 horsepower @110 ft-lbs full
torque; motor speed 0-700 rpm; motor can run on mud, air, N.sub.2,
mist, or foam; 180 SCFM, 500-800 psig drop; support equipment
extends length to 12 ft; 10:1 gear ratio provides 0-70 rpm
capability; and has the capability to rotate the lower part 1401 of
the LBHA through potential stall conditions.
[0176] The upper part 1400 of the LBHA 14100 is joined to the lower
part 1401 with a sealed chamber 1404 that is transparent to the
laser beam and forms a pupil plane 1420 to permit unobstructed
transmission of the laser beam to the beam shaping optics 1406 in
the lower part 1401. The lower part 1401 is designed to rotate. The
sealed chamber 1404 is in fluid communication with the lower
chamber 1401 through port 1414. Port 1414 may be a one way valve
that permits clean transmissive fluid and preferably gas to flow
from the upper part 1400 to the lower part 1401, but does not
permit reverse flow, or if may be another type of pressure and/or
flow regulating value that meets the particular requirements of
desired flow and distribution of fluid in the downhole environment.
Thus, for example there is provided in FIG. 14 a first fluid flow
path, shown by arrows 1416, and a second fluid flow path, shown by
arrows 1417. In the example of FIG. 14 the second fluid flow path
is a laminar flow although other flows including turbulent flows
may be employed.
[0177] The lower part 1401 has a means for receiving rotational
force from the motor 1410, which in the example of the figure is a
gear 1412 located around the lower part housing 1419 and a drive
gear 1413 located at the lower end of the axle 1411. Other means
for transferring rotational power may be employed or the motor may
be positioned directly on the lower part. It being understood that
an equivalent apparatus may be employed which provide for the
rotation of the portion of the LBHA to facilitate rotation or
movement of the laser beam spot while that the same time not
providing undue rotation, or twisting forces, to the optical fiber
or other means transmitting the high power laser beam down the hole
to the LBHA. In his way laser beam spot can be rotated around the
bottom of the borehole. The lower part 1401 has a laminar flow
outlet 1407 for the fluid to exit the LBHA 14100, and two hardened
rollers 1408, 1409 at its lower end. Although a laminar flow is
contemplated in this example, it should be understood that
non-laminar flows, and turbulent flows may also be employed.
[0178] The two hardened rollers may be made of a stainless steel or
a steel with a hard face coating such as tungsten carbide,
chromium-cobalt-nickel alloy, or other similar materials. They may
also contain a means for mechanically cutting rock that has been
thermally degraded by the laser. They may range in length, i.e.,
from about 1 in to about 4 in and preferably are about 2-3 in and
may be as large as or larger than 6 Inches. Moreover in LBHAs for
drilling larger diameter boreholes they may be in the range of
10-20 inches in diameter or greater.
[0179] Thus, FIG. 14 provides for a high power laser beam path 1415
that enters the LBHA 14100, travels through beam spot shaping
optics 1406, and then exits the LBHA to strike its intended target
on the surface of a borehole. Further, although it is not required,
the beam spot shaping optics may also provide a rotational element
to the spot, and if so, would be considered to be beam rotational
and shaping spot optics.
[0180] In use the high energy laser beam, for example greater than
15 kW, would enter the LBHA 14100, travel down fiber 1402, exit the
end of the fiber 1403 and travel through the sealed chamber 1404
and pupil plane 1420 into the optics 1406, where it would be shaped
and focused into a spot, the optics 1406 would further rotate the
spot. The laser beam would then illuminate, in a potentially
rotating manner, the bottom of the borehole spalling, chipping,
melting, and/or vaporizing the rock and earth Illuminated and thus
advance the borehole. The lower part would be rotating and this
rotation would further cause the rollers 1408, 1409 to physically
dislodge any material that was effected by the laser or otherwise
sufficiently fixed to not be able to be removed by the flow of the
drilling fluid alone.
[0181] The cuttings would be cleared from the laser path by the
flow of the fluid along the path 1417, as well as, by the action of
the rollers 1408, 1409 and the cuttings would then be carried up
the borehole by the action of the drilling fluid from the air
amplifiers 1405, as well as, the laminar flow opening 1407.
[0182] It is understood that the configuration of the LBHA is FIG.
14 is by way of example and that other configurations of its
components are available to accomplish the same results. Thus, the
motor may be located in the lower part rather than the upper part,
the motor may be located in the upper part but only turn the optics
in the lower part and not the housing. The optics may further be
located in both the upper and lower parts, which the optics for
rotation being positioned in that part which rotates. The motor may
be located in the lower part but only rotate the optics and the
rollers. In this later configuration the upper and lower parts
could be the same, i.e., there would only be one part to the LBHA.
Thus, for example the inner portion of the LBHA may rotate while
the outer portion is stationary or vice versa, similarly the top
and/or bottom portions may rotate or various combinations of
rotating and non-rotating components may be employed, to provide
for a means for the laser beam spot to be moved around the bottom
of the borehole.
[0183] The optics 1406 should be selected to avoid or at least
minimize the loss of power as the laser beam travels through them.
The optics should further be designed to handle the extreme
conditions present in the downhole environment, at least to the
extent that those conditions are not mitigated by the housing 1419.
The optics may provide laser beam spots of differing power
distributions and shapes as set forth herein above. The optics may
further provide a sign spot or multiple spots as set forth herein
above.
[0184] Drilling may be conducted in a dry environment or a wet
environment. An important factor is that the path from the laser to
the rock surface should be kept as clear as practical of debris and
dust particles or other material that would interfere with the
delivery of the laser beam to the rock surface. The use of high
brightness lasers provides another advantage at the process head,
where long standoff distances from the last optic to the work piece
are important to keeping the high pressure optical window clean and
Intact through the drilling process. The beam can either be
positioned statically or moved mechanically, opto-mechanically,
electro-optically, electromechanically, or any combination of the
above to illuminate the earth region of Interest.
[0185] In general, and by way of further example, the LBHA may
comprise a housing, which may by way of example, be made up of
sub-housings. These sub-housings may be integral, they may be
separable, they may be removably fixedly connected, they may be
rotatable, or there may be any combination of one or more of these
types of relationships between the sub-housings. The LBHA may be
connected to the lower end of the coiled tubing, drill pipe, or
other means to lower and retrieve the LBHA from the borehole.
Further, it may be connected to stabilizers, drill collars, or
other types of downhole assemblies, 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
LBHA has associated therewith a means that transmitted the high
power energy from down the borehole.
[0186] The LBHA may also have associated with, or in, it means to
handle and deliver drilling fluids. These means may be associated
with some or all of the sub-housings. There are further provided
mechanical scraping means, e.g. a PDC bit, to remove and/or direct
material in the borehole, although other types of known bits and/or
mechanical drilling heads by also be employed in conjunction with
the laser beam. These scrapers or bits may be mechanically
interacted with the surface or parts of the borehole to loosen,
remove, scrap or manipulate such borehole material as needed. These
scrapers may be from less than about 1 in to about 20 in. In use
the high energy laser beam, for example greater than 15 kW, would
travel down the fibers through optics and then out the lower end of
the LBHA to illuminate the intended part of the borehole, or
structure contained therein, spalling, melting and/or vaporizing
the material so illuminated and thus advance the borehole or
otherwise facilitating the removal of the material so
illuminated.
[0187] In FIGS. 15A and 15B, there is provided a graphic
representation of an example of a laser beam-borehole surface
interaction. Thus, there is shown a laser beam 1500, an area of
beam illumination 1501, i.e., a spot (as used herein unless
expressly provided otherwise the term "spot" Is not limited to a
circle), on a borehole wall or bottom 1502. There is further
provided in FIG. 1B a more detailed representation of the
interaction and a corresponding chart 1510 categorizing the stress
created in the area of Illumination. Chart 1510 provides von Mises
Stress in .sigma..sub.M 10.sup.8 N/m.sup.2 wherein the cross
hatching and shading correspond to the stress that is created in
the illuminated area for a 30 mill-second illumination period,
under down hole conditions of 2000 psi and a temperature of 150F,
with a beam having a fluence of 2 kW/cm.sup.2. Under these
conditions the compressive strength of basalt is about
2.6.times.10.sup.8 N/m.sup.2, and the cohesive strength is about
0.66.times.10.sup.8 N/m.sup.2. Thus, there is shown a first area
1505 of relative high stress, from about 4.722 to
5.211.times.10.sup.8 N/m.sup.2, a second area 1506 of relative
stress at or exceeding the compressive stress of basalt under the
downhole conditions, from about 2.766 to 3.255.times.10.sup.8
N/m.sup.2, a third area 1507 of relative stress about equal to the
compressive stress of basalt under the downhole conditions, from
about 2.276 to 2.766.times.10.sup.8 N/m.sup.2, a fourth area 1508
of relative lower stress that is below the compressive stress of
basalt under the downhole conditions yet greater than the cohesive
strength, from about 2.276 to 2.766.times.10.sup.8 N/m.sup.2, and a
fifth area 1509 of relative stress that is at or about the cohesive
strength of basalt under the downhole conditions, from about 0.320
to 0.899.times.10.sup.8 N/m.sup.2.
[0188] Accordingly, the profiles of the beam interaction with the
borehole to obtain a maximum amount of stress in the borehole in an
efficient manner, and thus, increase the rate of advancement of the
borehole can be obtained. Thus, for example if an elliptical spot
is rotated about its center point for a beam that is either uniform
or Gaussian the energy deposition profile is illustrated in FIGS.
16A and 16B. Where the area of the borehole from the center point
of the beam is shown as x and y axes 1601 and 1602 and the amount
of energy deposited is shown on the z axis 1603. From this it is
seen that inefficiencies are present in the deposition of energy to
the borehole, with the outer sections of the borehole 1605 and 1606
being the limiting factor in the rate of advancement.
[0189] Thus, it is desirable to modify the beam deposition profile
to obtain a substantially even and uniform deposition profile upon
rotation of the beam. An example of such a preferred beam
deposition profile is provided in FIGS. 17A and 17B, where FIG. 17A
shows the energy deposition profile with no rotation, and FIG. 17B
shows the energy deposition profile when the beam profile of 17A is
rotated through one rotation, i.e., 360 degrees; having x and y
axes 1701 and 1702 and energy on z axis 1703. This energy
deposition distribution would be considered substantially
uniform.
[0190] To obtain this preferable beam energy profile there are
provided examples of optical assemblies that may be used with a
LBHA. Thus, an example is Illustrated in FIGS. 18A to 18D, having x
and y axes 1801 and 1802 and z axis 1803, wherein there is provided
a laser beam 1805 having a plurality of rays 1807. The laser beam
1805 enters an optical assembly 1820, having a culminating lens
1809, having input curvature 1811 and an output curvature 1813.
There is further provided an axicon lens 1815 and a window 1817.
The optical assembly of Example 1 would provide a desired beam
intensity profile from an input beam having a substantially
Gaussian, Gaussian, or super-Gaussian distribution for applying the
beam spot to a borehole surface 1830.
[0191] A further example is illustrated in FIG. 19 and has an
optical assembly 1920 for providing the desired beam intensity
profile of FIG. 17A and energy deposition of FIG. 17B to a borehole
surface from a laser beam having a uniform distribution. Thus,
there is provided in this example a laser beam 1905 having a
uniform profile and rays 1907, that enters a spherical lens 1913,
which collimates the output of the laser from the downhole end of
the fiber, the beam then exits 1913 and enters a toroidal lens
1915, which has power in the x-axis to form the minor-axis of the
elliptical beam. The beam then exits 1915 and enters a pair of
aspherical toroidal lens 1917, which has power in the y-axis to map
the y-axis intensity profiles form the pupil plane to the image
plane. The beam then exits the lens 1917 and enters flat window
1919, which protects the optics from the outside environment.
[0192] A further example is illustrated in FIG. 20, which provides
a further optical assembly for providing predetermined beam energy
profiles. Thus, there is provided a laser beam 205 having rays 207,
which enters collimating lens 209, spot shape forming lens 211,
which is preferably an ellipse, and a micro optic array 213. The
micro optic array 213 may be a micro-prism array, or a micro lens
array. Further the micro optic array may be specifically designed
to provide a predetermined energy deposition profile, such as the
profile of FIG. 17.
[0193] A further example is illustrated in FIG. 21, which provides
an optical assembly for providing a predetermined beam pattern.
Thus, there is provided a laser beam 2105, exiting the downhole end
of fiber 2140, having rays 2107, which enters collimating lens
2109, a diffractive optic 2111, which could be a micro optic, or a
corrective optic to a micro optic, that provides pattern 2120,
which may but not necessary pass through reimaging lens 2113, which
provides pattern 2121.
[0194] There is further provided shot patterns for illuminating a
borehole surface with a plurality of spots in a multi-rotating
pattern. Accordingly in FIG. 22 there is provided a first pair of
spots 2203, 2205, which illuminate the bottom surface 2201 of the
borehole. The first pair of spots rotate about a first axis of
rotation 2202 in the direction of rotation shown by arrow 2204 (the
opposite direction of rotation is also contemplated herein). There
is provided a second pair of spots 2207, 2209, which illuminate the
bottom surface 2201 of the borehole. The second pair of shots
rotate about axis 2206 in the direction of rotation shown by arrow
2208 (the opposite direction of rotation is also contemplated
herein). The distance between the spots in each pair of spots may
be the same or different. The first and second axis of rotation
simultaneously rotate around the center of the borehole 2212 in a
rotational direction, shown by arrows 2212, that is preferably in
counter-rotation to the direction of rotation 2208, 2204. Thus,
preferably although not necessarily, if 2208 and 2204 are
clockwise, then 2212 should be counter-clockwise. This shot pattern
provides for a substantially uniform energy deposition.
[0195] There is illustrated in FIG. 23 an elliptical shot pattern
of the general type discussed with respect to the forgoing
illustrated examples having a center 2301, a major axis 2302, a
minor axis 2303 and is rotated about the center. In this way the
major axis of the spot would generally correspond to the diameter
of the borehole, ranging from any known or contemplated diameters
such as about 30, 20, 171/2, 133/8, 121/4, 95/8, 81/2, 7, and 6%
inches.
[0196] There is further illustrated in FIG. 24 a rectangular shaped
spot 2401 that would be rotated around the center of the borehole.
There is illustrated in FIG. 25 a pattern 2501 that has a plurality
of individual shots 2502 that may be rotated, scanned or moved with
respect to the borehole to provide the desired energy deposition
profile. The is further Illustrated in FIG. 26 a squared shot 2601
that is scanned 2601 in a raster scan matter along the bottom of
the borehole, further a circle, square or other shape shot may be
scanned.
[0197] In accordance with one or more aspects, one or more fiber
optic distal fiber ends may be arranged in a pattern. The
multiplexed beam shape may comprise a cross, an x shape, a
viewfinder, a rectangle, a hexagon, lines in an array, or a related
shape where lines, squares, and cylinders are connected or spaced
at different distances.
[0198] In accordance with one or more aspects, one or more
refractive lenses, diffractive elements, transmissive gratings,
and/or reflective lenses may be added to focus, scan, and/or change
the beam spot pattern from the beam spots emitting from the fiber
optics that are positioned in a pattern. One or more refractive
lenses, diffractive elements, transmissive gratings, and/or
reflective lenses may be added to focus, scan, and/or change the
one or more continuous beam shapes from the light emitted from the
beam shaping optics. A collimator may be positioned after the beam
spot shaper lens in the transversing optical path plane. The
collimator may be an aspheric lens, spherical lens system composed
of a convex lens, thick convex lens, negative meniscus, and
bi-convex lens, gradient refractive lens with an aspheric profile
and achromatic doublets. The collimator may be made of the said
materials, fused silica, ZnSe, SF glass, or a related material. The
collimator may be coated to reduce or enhance reflectivity or
transmission. Said optical elements may be cooled by a purging
liquid or gas.
[0199] It is readily understood in the art that the terms lens and
optic(al) elements, as used herein is used in its broadest terms
and thus may also refer to any optical elements with power, such as
reflective, transmissive or refractive elements,
[0200] In some aspects, the refractive positive lens may be a
microlens. The microlens can be steered in the light propagating
plane to increase/decrease the focal length as well as
perpendicular to the light propagating plane to translate the beam.
The microlens may receive incident light to focus to multiple foci
from one or more optical fibers, optical fiber bundle pairs, fiber
lasers, diode lasers; and receive and send light from one or more
collimators, positive refractive lenses, negative refractive
lenses, one or more mirrors, diffractive and reflective optical
beam expanders, and prisms.
[0201] In some aspects, a diffractive optical element beam splitter
could be used in conjunction with a refractive lens. The
diffractive optical element beam splitter may form double beam
spots or a pattern of beam spots comprising the shapes and patterns
set forth above.
[0202] There is additionally provided a system and method for
creating a borehole in the earth wherein the system and method
employ means for providing the laser beam to the bottom surface in
a predetermined energy deposition profile, including having the
laser beam as delivered from the bottom hole assembly illuminating
the bottom surface of the borehole with a predetermined energy
deposition profile, illuminating the bottom surface with an any one
of or combination of: a predetermined energy deposition profile
biased toward the outside area of the borehole surface; a
predetermined energy deposition profile biased toward the inside
area of the borehole surface; a predetermined energy deposition
profile comprising at least two concentric areas having different
energy deposition profiles; a predetermined energy deposition
profile provided by a scattered laser shot pattern; a predetermined
energy deposition profile based upon the mechanical stresses
applied by a mechanical removal means; a predetermined energy
deposition profile having at least two areas of differing energy
and the energies in the areas correspond inversely to the
mechanical forces applied by a mechanical means.
[0203] There is yet further provided a method of advancing a
borehole using a laser, the method comprising: 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; transmitting the laser beam
from the distal end to an optical assembly in a laser bottom hole
assembly, the laser bottom hole assembly directing the laser beam
to the bottom surface of the borehole; and, providing a
predetermined energy deposition profile to the bottom 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.
[0204] Moreover there is provided a method of advancing a borehole
using a laser, wherein the laser beam is directed to the bottom
surface of the borehole in a substantially uniform energy
deposition profile and thereby the length of the borehole is
increased, in part, based upon the interaction of the laser beam
with the bottom of the borehole.
[0205] In accordance with one or more aspects, a method for laser
drilling using an optical pattern to chip rock formations is
disclosed. The method may comprise irradiating the rock to spall,
melt, or vaporize with one or more lasing beam spots, beam spot
patterns and beam shapes at non-overlapping distances and timing
patterns to induce overlapping thermal rock fractures that cause
rock chipping of rock fragments. Single or multiple beam spots and
beam patterns and shapes may be formed by refractive and reflective
optics or fiber optics. The optical pattern, the pattern's timing,
and spatial distance between non-overlapping beam spots and beam
shapes may be controlled by the rock type thermal absorption at
specific wavelength, relaxation time to position the optics, and
interference from rock removal.
[0206] In some aspects, the lasing beam spots power is either not
reduced, reduced moderately, or fully during relaxation time when
repositioning the beam spot on the rock surface. To chip the rock
formation, two lasing beam spots may scan the rock surface and be
separated by a fixed position of less than 2'' and non-overlapping
in some aspects. Each of the two beam spots may have a beam spot
area in the range between 0.1 cm.sup.2 and 25 cm.sup.2. The
relaxation times when moving the two lasing beam spots to their
next subsequent lasing locations on the rock surface may range
between 0.05 ms and 2 s. When moving the two lasing beam spots to
their next position, their power may either be not reduced, reduced
moderately, or fully during relaxation time.
[0207] In accordance with one or more aspects, a beam spot pattern
may comprise three or more beam spots in a grid pattern, a
rectangular grid pattern, a hexagonal grid pattern, lines in an
array pattern, a circular pattern, a triangular grid pattern, a
cross grid pattern, a star grid pattern, a swivel grid pattern, a
viewfinder grid pattern or a related geometrically shaped pattern.
In some aspects, each lasing beam spot in the beam spot pattern has
an area in the range of 0.1 cm.sup.2 and 25 cm.sup.2. To chip the
rock formation all the neighboring lasing beam spots to each lasing
beam spot in the beam spot pattern may be less than a fixed
position of 2'' and non-overlapping in one or more aspects.
[0208] In some aspects, more than one beam spot pattern to chip the
rock surface may be used. The relaxation times when positioning one
or more beam spot patterns to their next subsequent lasing location
may range between 0.05 ms and 2 s. The power of one or more beam
spot patterns may either be not reduced, reduced moderately, or
fully during relaxation time. A beam shape may be a continuous
optical beam spot forming a geometrical shape that comprises of, a
cross shape, hexagonal shape, a spiral shape, a circular shape, a
triangular shape, a star shape, a line shape, a rectangular shape,
or a related continuous beam spot shape.
[0209] In some aspects, positioning one line either linear or
non-linear to one or more neighboring lines either linear or
non-linear at a fixed distance less than 2'' and non-overlapping
may be used to chip the rock formation. Lasing the rock surface
with two or more beam shapes may be used to chip the rock
formation. The relaxation times when moving the one or more beam
spot shapes to their next subsequent lasing location may range
between 0.05 ms and 2 s.
[0210] In accordance with one or more aspects, the one or more
continuous beam shapes powers are either not reduced, reduced
moderately, or fully during relaxation time. The rock surface may
be irradiated by one or more lasing beam spot patterns together
with one or more beam spot shapes, or one or two beam spots with
one or more beam spot patterns. In some aspects, the maximum
diameter and circumference of one or more beam shapes and beam spot
patterns is the size of the borehole being chipped when drilling
the rock formation to well completion.
[0211] In accordance with one or more aspects, rock fractures may
be created to promote chipping away of rock segments for efficient
borehole drilling. In some aspects, beam spots, shapes, and
patterns may be used to create the rock fractures so as to enable
multiple rock segments to be chipped away. The rock fractures may
be strategically patterned. In at least some aspects, drilling rock
formations may comprise applying one or more non-overlapping beam
spots, shapes, or patterns to create the rock fractures. Selection
of one or more beam spots, shapes, and patterns may generally be
based on the intended application or desired operating parameters.
Average power, specific power, timing pattern, beam spot size,
exposure time, associated specific energy, and optical generator
elements may be considerations when selecting one or more beam
spots, a shape, or a pattern. The material to be drilled, such as
rock formation type, may also influence the one or more beam spot,
a shape, or a pattern selected to chip the rock formation. For
example, shale will absorb light and convert to heat at different
rates than sandstone.
[0212] In accordance with one or more aspects, rock may be
patterned with one or more beam spots. In at least one embodiment,
beam spots may be considered one or more beam spots moving from one
location to the next subsequent location lasing the rock surface in
a timing pattern. Beam spots may be spaced apart at any desired
distance. In some non-limiting aspects, the fixed position between
one beam spot and neighboring beam spots may be non-overlapping. In
at least one non-limiting embodiment, the distance between
neighboring beam spots may be less than 2''.
[0213] In accordance with one or more aspects, rock may be
patterned with one or more beam shapes. In some aspects, beam
shapes may be continuous optical shapes forming one or more
geometric patterns. A pattern may comprise the geometric shapes of
a line, cross, viewfinder, swivel, star, rectangle, hexagon,
circular, ellipse, squiggly line, or any other desired shape or
pattern. Elements of a beam shape may be spaced apart at any
desired distance. In some non-limiting aspects, the fixed position
between each line linear or non-linear and the neighboring lines
linear or non-linear are in a fixed position may be less than 2''
and non-overlapping.
[0214] In accordance with one or more aspects, rock may be
patterned with a beam pattern. Beam patterns may comprise a grid or
array of beam spots that may comprise the geometric patterns of
line, cross, viewfinder, swivel, star, rectangle, hexagon,
circular, ellipse, squiggly line. Beam spots of a beam pattern may
be spaced apart at any desired distance. In some non-limiting
aspects, the fixed position between each beam spot and the
neighboring beam spots in the beam spot pattern may be less than
2'' and non-overlapping.
[0215] In accordance with one or more aspects, the beam spot being
scanned may have any desired area. For example, in some
non-limiting aspects the area may be in a range between about 0.1
cm.sup.2 and about 25 cm.sup.2. The beam line, either linear or
non-linear, may have any desired specific diameter and any specific
and predetermined power distribution. For example, the specific
diameter of some non-limiting aspects may be in a range between
about 0.05 cm.sup.2 and about 25 cm.sup.2. In some non-limiting
aspects, the maximum length of a line, either linear or non-linear,
may generally be the diameter of a borehole to be drilled. Any
desired wavelength may be used. In some aspects, for example, the
wavelength of one or more beam spots, a shape, or pattern, may
range from 800 nm to 2000 nm. Combinations of one or more beam
spots, shapes, and patterns are possible and may be
implemented.
[0216] In accordance with one or more aspects, the timing patterns
and location to chip the rock may vary based on known rock chipping
speeds and/or rock removal systems. In one embodiment, relaxation
scanning times when positioning one or more beam spot patterns to
their next subsequent lasing location may range between 0.05 ms and
2 s. In another embodiment, a camera using fiber optics or
spectroscopy techniques can image the rock height to determine the
peak rock areas to be chipped. The timing pattern can be calibrated
to then chip the highest peaks of the rock surface to lowest or
peaks above a defined height using signal processing, software
recognition, and numeric control to the optical lens system. In
another embodiment, timing patterns can be defined by a rock
removal system. For example, if the fluid sweeps from the left side
the rock formation to the right side to clear the optical head and
raise the cuttings, the timing should be chipping the rock from
left to right to avoid rock removal interference to the one or more
beam spots, shape, or pattern lasing the rock formation or
vice-a-versa. For another example, if the rocks are cleared by a
jet nozzle of a gas or liquid, the rock at the center should be
chipped first and the direction of rock chipping should move then
away from the center. In some aspects, the speed of rock removal
will define the relaxation times.
[0217] In accordance with one or more aspects, the rock surface may
be affected by the gas or fluids used to clear the head and raise
the cuttings downhole. In one embodiment, heat from the optical
elements and losses from the fiber optics downhole or diode laser
can be used to increase the temperature of the borehole. This could
lower the required temperature to induce spallation making it
easier to spall rocks. In another embodiment, a liquid may saturate
the chipping location, in this situation the liquid would be tumed
to steam and expand rapidly, this rapid expansion would thus create
thermal shocks improving the growth of fractures in the rock. In
another embodiment, an organic, volatile components, minerals or
other materials subject to rapid and differential heating from the
laser energy, may expand rapidly, this rapid expansion would thus
create thermal shocks improving the growth of fractures in the
rock. In another embodiment, the fluids of higher index of
refraction may be sandwiched between two streams of liquid with
lower index of refraction. The fluids used to clear the rock can
act as a wavelength to guide the light. A gas may be used with a
particular index of refraction lower than a fluid or another
gas.
[0218] By way of example and to further illustrate the teachings of
the present inventions, the thermal shocks can range from lasing
powers between one and another beam spot, shape, or pattern. In
some non-limiting aspects, the thermal shocks may reach 10
kW/cm.sup.2 of continuous lasing power density. In some
non-limiting aspects, the thermal shocks may reach up to 10
MW/cm.sup.2 of pulsed lasing power density, for instance, at 10
nanoseconds per pulse. In some aspects, two or more beam spots,
shapes, and patterns may have different power levels to thermally
shock the rock. In this way, a temperature gradient may be formed
between lasing of the rock surface.
[0219] By way of example and to further demonstrate the present
teachings of the inventions, there are provided examples of optical
heads, i.e., optical assemblies, and beam shot patterns, i.e.,
Illumination patterns, that may be utilized with, as a part of, or
provided by an LBHA. FIG. 27 illustrates chipping a rock formation
using a lasing beam shape pattern. An optical beam 2701 shape
lasing pattern forming a checkerboard of lines 2702 irradiates the
rock surface 2703 of a rock 2704. The distance between the beam
spots shapes are non-overlapping because stress and heat absorption
cause natural rock fractures to overlap inducing chipping of rock
segments. These rock segments 2705 may peel or explode from the
rock formation.
[0220] By way of example and to further demonstrate the present
teachings, FIG. 28 illustrates removing rock segments by sweeping
liquid or gas flow 2801 when chipping a rock formation 2802. The
rock segments are chipped by a pattern 1606 of non-overlapping beam
spot shaped lines 2803, 2804, 2805. The optical head 2807,
optically associated with an optical fiber bundle, the optical head
2807 having an optical element system irradiates the rock surface
2808. A sweeping from left to right with gas or liquid flow 2801
raises the rock fragments 2809 chipped by the thermal shocks to the
surface.
[0221] By way of example and to further demonstrate the present
teachings, FIG. 29 illustrates removing rock segments by liquid or
gas flow directed from the optical head when chipping a rock
formation 2901. The rock segments are chipped by a pattern 2902 of
non-overlapping beam spot shaped lines 2903, 2904, 2905. The
optical head 2907 with an optical element system irradiates the
rock surface 2908. Rock segment debris 2909 is swept from a nozzle
2915 flowing a gas or liquid 2911 from the center of the rock
formation and away. The optical head 2907 is shown attached to a
rotating motor 2920 and fiber optics 2924 spaced in a pattern. The
optical head also has rails 2928 for z-axis motion if necessary to
focus. The optical refractive and reflective optical elements form
the beam path.
[0222] By way of example and to further demonstrate the present
teachings, FIG. 30 illustrates optical mirrors scanning a lasing
beam spot or shape to chip a rock formation in the XY-plane. Thus,
there is shown, with respect to a casing 3023 in a borehole, a
first motor of rotating 3001, a plurality of fiber optics in a
pattern 3003, a gimbal 3005, a second rotational motor 3007 and a
third rotational motor 3010. The second rotational motor 3007
having a stepper motor 3011 and a mirror 3015 associated therewith.
The third rotational motor 3010 having a stepper motor 3013 and a
mirror 3017 associated therewith. The optical elements 3019
optically associated with optical fibers 3003 and capable of
providing laser beam along optical path 3021. As the gimbal rotates
around the z-axis and repositions the mirrors in the XY-plane. The
mirrors are attached to a stepper motor to rotate stepper motors
and mirrors in the XY-plane. In this embodiment, fiber optics are
spaced in a pattern forming three beam spots manipulated by optical
elements that scan the rock formation a distance apart and
non-overlapping to cause rock chipping. Other fiber optic patterns,
shapes, or a diode laser can be used.
[0223] By way of example and to further demonstrate the present
teachings, FIG. 31 illustrates using a beam splitter lens to form
multiple beam foci to chip a rock formation. There is shown fibers
3101 in a pattern, a rail 3105 for providing z direction movement
shown by arrow 3103, a fiber connector 3107, an optical head 3109,
having a beam expander 3119, which comprises a DOE/ROE 3115, a
positive lens 3117, a collimator 3113, a beam expander 3111. This
assembly is capable of delivering one or more laser beams, as spots
3131 in a pattern, along optical paths 3129 to a rock formation
3123 having a surface 3125. Fiber optics are spaced a distance
apart in a pattern. An optical element system composed of a beam
expander and collimator feed a diffractive optical element attached
to a positive lens to focus multiple beam spots to multiple foci.
The distance between beam spots are non-overlapping and will cause
chipping. In this figure, rails move in the z-axis to focus the
optical path. The fibers are connected by a connector. Also, an
optical element can be attached to each fiber optic as shown in
this figure to more than one fiber optics.
[0224] By way of example and to further demonstrate the present
teachings, FIG. 32 illustrates using a beam spot shaper lens to
shape a pattern to chip a rock formation. There is provided an
array of optical fibers 3201, an optical head 3209. The optical
head having a rail 3203 for facilitating movement in the z
direction, shown by arrow 3205, a fiber connector 3207, an optics
assembly 3201 for shaping the laser beam that is transmitted by the
fibers 3201. The optical head capable of transmitting a laser beam
along optical path 3213 to illuminate a surface 3219 with a laser
beam shot pattern 3221 that has separate, but intersection lines in
a grid like pattern. Fiber optics are spaced a distance apart in a
pattern connected by a connector. The fiber optics emit a beam spot
to a beam spot shaper lens attached to the fiber optic. The beam
spot shaper lens forms a line in this figure overlapping to form a
tick-tack-toe laser pattern on the rock surface. The optical fiber
bundle wires are attached to rails moving in the z-axis to focus
the beam spots.
[0225] By way of example and to further demonstrate the present
teachings, FIG. 33 illustrates using a F-theta objective to focus a
laser beam pattern to a rock formation to cause chipping. There is
provided an optical head 3301, a first motor for providing rotation
3303, a plurality of optical fibers 3305, a connector 3307, which
positions the fibers in a predetermined pattern 3309. The laser
beam exits the fibers and travels along optical path 3311 through
F-Theta optics 3315 and illuminates rock surface 3313 in shot
pattern 3310. There is further shown rails 3317 for providing
z-direction movement. Fiber optics connected by connectors in a
pattern are rotated in the z-axis by a gimbal attached to the
optical casing head. The beam path is then refocused by an F-theta
objective to the rock formation. The beam spots are a distance
apart and non-overlapping to induce rock chipping in the rock
formation. A rail is attached to the optical fibers and F-theta
objective moving in the z-axis to focus the beam spot size.
[0226] It is understood that the rails in these examples for
providing z-direction movement are provided by way of illustration
and that z-direction movement, i.e. movement toward or away from
the bottom of the borehole may be obtained by other means, for
example winding and unwinding the spool or raising and lowering the
drill string that is used to advance the LBHA into or remove the
LBHA from the borehole.
[0227] By way of example and to further demonstrate the present
teachings, FIG. 34 illustrates mechanical control of fiber optics
attached to beam shaping optics to cause rock chipping. There is
provided a bundle of a plurality of fibers 3401 first motor 3405
for providing rotational movement a power cable 3403, an optical
head 3406, and rails 3407. There is further provided a second motor
3409, a fiber connector 3413 and a lens 3421 for each fiber to
shape the beam. The laser beams exit the fibers and travel along
optical paths 3415 and illumate the rock surface 3419 in a
plurality of individual line shaped shot patterns 3417. Fiber
optics are connected by connectors in a pattern and are attached to
a rotating gimbal motor around the z-axis. Rails are attached to
the motor moving in the z-axis. The rails are structurally attached
to the optical head casing and a support rail. A power cable powers
the motors. In this figure, the fiber optics emit a beam spot to a
beam spot shaper lens forming three non-overlapping lines to the
rock formation to induce rock chipping.
[0228] By way of example and to further demonstrate the present
teachings, FIG. 35 illustrates using a plurality of fiber optics to
form a beam shape line. There is provided an optical assembly 3511
having a source of laser energy 3501, a power cable 3503, a first
rotational motor 3505, which is mounted as a gimbal, a second motor
3507, and rails 3517 for z-direction movement. There is also
provided a plurality of fiber bundles 3521, with each bundle
containing a plurality of individual fibers 3523. The bundles 3521
are held in a predetermined position by connector 3525. Each bundle
3521 is optically associated with a beam shaping optics 3509. The
laser beams exit the beam shaping optics 3509 and travel along
optical path 3515 to Illuminate surface 3519. The motors 3507, 3505
provide for the ability to move the plurality of beam spots in a
plurality of predetermined and desired patterns on the surface
3519, which may be the surface the borehole, such as the bottom
surface, side surface, or casing in the borehole. A plurality of
fiber optics are connected by connectors in a pattern and are
attached to a rotating gimbal motor around the z-axis. Rails are
attached to the motor moving in the z-axis. The rails are
structurally attached to the optical head casing and a support
rail. A power cable powers the motors. In this figure, the
plurality of fiber optics emits a beam spot to a beam spot shaper
lens forming three lines that are non-overlapping to the rock
formation. The beam shapes induce rock chipping.
[0229] By way of example and to further demonstrate the present
teachings, FIG. 36 illustrates using a plurality of fiber optics to
form multiple beam spot foci being rotated on an axis. There is
provided a laser source 3601, a first motor 3603, which is gimbal
mounted, a second motor 3605 and a means for z-direction movement
3607. There is further provided a plurality of fiber bundles 3613
and a connector 3609 for positioning the plurality of bundles 3613,
the laser beam exits the fibers and Illuminates a surface in a
diverging and crossing laser shot pattern. The fiber optics are
connected by connectors at an angle being rotated by a motor
attached to a gimbal that is attached to a second motor moving in
the z-axis on rails. The motors receive power by a power cable. The
rails are attached to the optical casing head and support rail
beam. In this figure, a collimator sends the beam spot originating
from the plurality of optical fibers to a beam splitter. The beam
splitter is a diffractive optical element that is attached to
positive refractive lens. The beam splitter forms multiple beam
spot foci to the rock formation at non-overlapping distances to
chip the rock formation. The foci is repositioned in the z-axis by
the rails.
[0230] By way of example and to further demonstrate the present
teachings, FIG. 11 illustrates scanning the rock surface with a
beam pattern and XY scanner system. There is provided an optical
path 1101 for a laser beam, a scanner 1103, a diffractive optics
1105 and a collimator optics 1107. An optical fiber emits a beam
spot that is expanded by a beam expander unit and focused by a
collimator to a refractive optical element. The refractive optical
element is positioned in front of an XY scanner unit to form a beam
spot pattern or shape. The XY scanner composed of two mirrors
controlled by galvanometer mirrors 1109 irradiate the rock surface
1113 to induce chipping.
[0231] 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.
* * * * *