U.S. patent number 3,788,703 [Application Number 05/243,961] was granted by the patent office on 1974-01-29 for method of rock cutting employing plasma stream.
This patent grant is currently assigned to Humphreys Corporation. Invention is credited to Merle L. Thorpe.
United States Patent |
3,788,703 |
Thorpe |
January 29, 1974 |
**Please see images for:
( Certificate of Correction ) ** |
METHOD OF ROCK CUTTING EMPLOYING PLASMA STREAM
Abstract
A method especially useful for cutting and breaking hard rock
such as granite from the face of a tunnel is disclosed. A pattern
of slots are cut into the rock face by directing a high velocity
plasma jet on the rock face to melt a portion of the rock face and
produce a molten film and applying electrical power to the
plasma-jet and a cooperating electrode to flow electric current
through the molten film to further heat the molten film and melt
additional rock to form a slot. After the pattern of slots are
formed, spaced plasma streams are introduced into the slots and
electrical power of a frequency effective to produce dielectric
heating in the rock is applied through the plasma streams to
produce a heated region within the rock mass which thermally
stresses and severs that rock mass portion into fragments.
Inventors: |
Thorpe; Merle L. (Hopkington,
NH) |
Assignee: |
Humphreys Corporation (Bow,
NH)
|
Family
ID: |
22920811 |
Appl.
No.: |
05/243,961 |
Filed: |
April 14, 1972 |
Current U.S.
Class: |
299/14; 175/16;
219/75 |
Current CPC
Class: |
E21C
37/18 (20130101); E21C 37/16 (20130101) |
Current International
Class: |
E21C
37/00 (20060101); E21C 37/16 (20060101); E21C
37/18 (20060101); E21c 037/18 () |
Field of
Search: |
;299/14 ;175/16,13
;219/75 |
References Cited
[Referenced By]
U.S. Patent Documents
Primary Examiner: Purser; Ernest R.
Attorney, Agent or Firm: Ertman; Willis M.
Claims
What is claimed is:
1. The method of extending a tunnel face through a rock mass
comprising the steps of
cutting a pattern of slots into said tunnel face, each slot being
cut by a method including
directing a primary plasma stream from a primary plasma torch to
impinge on the tunnel face,
melting with said primary plasma stream portion of rock of the
tunnel face to produce a molten film thereon,
contacting said molten film with a cooperating electrode, and
applying electrical power to said torch and cooperating electrode
to cause current to flow along a path that includes said primary
plasma stream, said molten film, and said cooperating electrode to
further heat said molten film and melt additional rock underlying
said film to form a cut in the tunnel face, and
breaking off from the tunnel face fragments of rock between said
slots, said fragment being broken off by a method including
directing a first plasma stream against a first region of said rock
mass at the bottom of a first slot cut in said tunnel face to make
electrical contact between said first plasma stream and a first
rock surface,
directing a second plasma stream against a second region of said
rock mass at the bottom of a second slot spaced from said first
slot to make electrical contact between said second plasma stream
and a second rock surface,
and applying a voltage of a frequency effective for producing
dielectric heating in said rock across said first and second plasma
streams to said first and second rock faces to dielectrically heat
a portion of said rock mass between said first and second rock
faces to thermally stress and sever said rock mass portion into
fragments.
2. The method as claimed in claim 1 wherein said primary plasma
stream has a velocity in the order of at least three thousand feet
per second.
3. The method as claimed in claim 1 wherein said cooperating
electrode is a gaseous plasma stream.
4. The method as claimed in claim 3 wherein the velocity of said
cooperating plasma stream is less than about 10% of the velocity of
said primary plasma stream.
5. The method as claimed in claim 1 wherein said primary plasma
stream has a velocity substantially greater than the velocities of
said first and second plasma streams.
6. The method as claimed in claim 1 wherein the voltage applied
across said first and second plasma streams and said rock mass
portion has a gradient in the range of 750-7,500 volts/inch.
7. The method as claimed in claim 1 and further including the step
of subjecting said molten film to a fluid jet to remove material
from said cut.
8. The method as claimed in claim 1 and further including the step
of introducing an additive to said molten film to modify the
characteristics thereof.
9. The method as claimed in claim 8 wherein said additive is
introduced to said molten film via a plasma stream.
10. The method for cutting rock comprising the steps of
energizing a primary plasma torch to generate an elongated plasma
stream,
directing said elongated plasma stream to impinge on the rock,
melting a portion of the rock with said elongated plasma stream to
produce a molten film thereon,
providing cooperating electrode means adjacent said molten film and
in said elongated plasma stream at a point beyond said molten film
so that said plasma stream extends along said molten film between
said primary torch and said cooperating electrode means, and
applying electrical power to said elongated plasma stream and
cooperating electrode means to estalish a transferred are through
said plasma stream between said primary torch and said cooperating
electrode means to cause electrical current to flow along a path
between said primary torch and said cooperating electrode means
through said plasma stream to further heat said molten film and and
additional rock underlying said molten film to form a cut in the
rock.
11. The method as claimed in claim 10 wherein said cooperating
electrode means is a gaseous plasma stream and said cooperating
plasma stream is directed to impinge on said molten film.
12. The method as claimed in claim 10 wherein said primary plasma
stream has a velocity in the order of at least three thousand feet
per second.
13. The method as claimed in claim 10 and further including the
step of subjecting said molten film to a fluid jet to remove
material from said cut.
14. The method as claimed in claim 10 and further including the
step of advancing said primary plasma torch and said cooperating
electrode means in a fixed relationship to one another to extend
said cut and form a slot through said rock.
15. The method as claimed in claim 10 and further including the
step of introducing an additive to said molten film to modify the
characteristics thereof.
16. The method as claimed in claim 15 wherein said additive is
introduced to said molten film via a plasma stream.
17. The method as claimed in claim 16 wherein said primary plasma
stream has a velocity in the order of at least three thousand feet
per second, said cooperating electrode means is a gaseous plasma
stream and said cooperating plasma stream is directed to impinge on
said molten film and the velocity of said cooperating plasma stream
is less than about 10 percent of the velocity of said primary
plasma stream.
18. The method as claimed in claim 17 and further including the
step of subjecting said molten film to a fluid jet to remove
material from said cut.
19. The method as claimed in claim 17 and further including the
step of advancing said primary plasma torch and said cooperating
electrode means in a fixed relationship to one another to extend
said cut and form a slot through said rock.
20. The method of breaking off rock fragments from a mass of rock
comprising the steps of
directing a first plasma stream from a first torch against the
surface of a first region of said rock mass to make electrical
contact through said first plasma stream between said first torch
and said first region,
directing a second plasma stream from a second torch against the
surface of a second region of said rock mass to make electrical
contact through said second plasma stream between said second torch
and said second region, said first and second regions being spaced
one from another,
and applying AC voltage of a frequency effective for producing
dielectric heating in said rock across said first and second plasma
streams and the rock mass between said spaced regions to
dielectrically heat a portion of said rock mass between said spaced
regions to thermally stress and sever fragments from said rock
mass.
21. The method as claimed in claim 20 wherein the voltage applied
across said first and second plasma streams and said rock mass
portion has a gradient in the range of 750-7,500 volts/inch.
22. The method as claimed in claim 20 wherein the velocity of each
of said plasma streams is in excess of 20 feet per second.
Description
SUMMARY OF INVENTION
This invention relates to methods for cutting and breaking hard
rock and more particularly to methods especially useful for cutting
and breaking hard rock such as granite from the face of tunnel.
Boring a tunnel through hard rock has been done conventionally by
drilling a number of holes into the tunnel face with percussive
tools and then fragmenting the tunnel face by the detonation of
explosives inserted into the drilled holes. The operation has been
slow and has required expensive capital equipment. A technique has
been developed for fragmenting rocks by dielectric heating, but it
has been difficult to establish reliable electrical contact with
the rock mass with the electrodes used and the positioning of the
electrodes has been slow and cumbersome. Objects of the invention
include the provision of methods permitting more rapid tunnelling
and less expensive tunnelling through hard rock.
Another object of the invention is to provide novel and improved
methods for cutting rock.
Another object of the invention is to provide a reliable, high
speed method for hard rock cutting.
One aspect of the invention features the method of rock cutting,
e.g. for extending a tunnel face through a rock face comprising the
steps of cutting a pattern of slots into the rock face, each slot
being cut by directing a plasma-jet on the rock face to melt a
portion of the rock face and produce a molten film thereon, and
applying electrical power to the plasma-jet and a cooperating
electrode to cause electric current along a path that includes the
plasma-jet, the molten film, and the cooperating electrode, thus
further heating the molten film and melting additional rock
underlying the molten film to form a cut in the tunnel face. The
plasma-jet provides a gaseous contact electrode that facilitates
maintaining the electrically conductive path between the power
supply and the film of molten rock. The cooperating electrode may
take a number of forms, for example it may be a graphite rod, a
conductive metal rod, or a second plasma-jet may be employed. The
nature of the power supply is a function of the characteristics of
the rock to be cut and may be DC or AC or DC with a superimposed AC
signal. It is preferred that the plasma-jet have a velocity in the
order of at least three thousand feet per second. The dynamic
erosive effects of this high velocity jet facilitates the cutting
operation. When the cooperating electrode is formed by a second
plasma-jet, that jet in a particular embodiment has a substantially
lower velocity, preferably less than about 10 percent of the
velocity of the other plasma-jet. It may also be desirable in
particular cutting operations to modify the characteristics of the
molten film by use of an additive such as an alkaline flux (e.g.
sodium carbonate) with rock such as granite or an acid flux (e.g.
potassium pyrosulfate) with rock such as basalt and such additive
may be introduced to the molten film by means of the plasma stream.
An auxiliary quench or ejection jet may be employed to facilitate
removal of debris from the cut. Still another object of the
invention is to provide novel and improved methods for fragmenting
rock.
Another aspect of the invention features breaking off fragments of
rock by directing a plurality of plasma streams into holes or slots
spaced apart in a region of the rock mass to make electrical
contact between the plasma streams and the rock faces contacted by
the plasma streams, and then applying electrical power of a
frequency effective for producing dielectric heating in the rock
through said plasma streams to heat dielectricly the rock mass
between the rock faces to produce a heated region within the rock
mass and thermal stress cracks that sever the rock mass into
fragments.
The plasma streams employed in this aspect of the invention are
preferably of low velocity so that a large electrical contact area
is provided at the bases of the spaced slots or holes. The applied
dielectric heating power creates a heated core a substantial
distance below the face of the rock mass so that greater amounts of
rock are removed than would be the case where the heated core was
nearer the surface.
The invention provides efficient methods for cutting and breaking
rock. Other objects, features and advantages of the invention will
be seen as the following description of particular embodiments
progresses in conjunction with the drawings in which:
FIG. 1 shows the invention applied to extending a tunnel face;
FIG. 2 shows, at larger scale, cutting according to the invention
with a pair of plasma streams being used to cut a slot into the
rock of the tunnel face;
FIG. 3 shows a fragmenting operation according to the invention
employing the application of plasma streams to the tunnel face;
and
FIG. 4 shows a cross-section view through the center of a slot to
reveal in greater detail aspects of the cutting method shown in
FIG. 2.
DESCRIPTION OF PARTICULAR EMBODIMENTS
As shown in the drawing, tunnelling equipment 10 is brought up to
face 12 of tunnel 14. Conventional support mechanism 16 supports
torch holder 18 in position before tunnel face 12. According to the
invention the advance of the tunnel face is accomplished in two
operations successively applied. The first of these is a cutting
operation shown more particularly in FIGS. 2 and 4. During the
cutting operation, torch holder 18 supports primary plasma torch 20
and secondary plasma torch 22 in fixed relationship to each other
with the plasmas 24, 26 from each torch directed against the rock
face 12 to form an elongated slot 28.
A suitable primary plasma torch 20 is shown diagrammatically in
FIG. 4 and has a central tungsten cathode 32 supported by insulator
34 in cavity 36 within housing 38 that carries anode electrode 40.
Anode 40 is water cooled and defines a nozzle passage 42. A conduit
44 connected to a supply 46 of inert gas such as argon communicates
with cavity 36 to admit gas symmetrically thereto for flow past
cathode 32 and out through nozzle 42. Pilot arc DC power supply 48
(which optionally may have a super-imposed high frequency, e.g. 10
kHz) is connected with its negative pole to cathode 32 and its
positive pole to anode 40. One or more ports 50 into nozzle passage
42 provide a means for introducing an additive into plasma-jet 24.
Conduit 52 is connected to ports 50 to deliver the additive to
torch 30.
A suitable secondary plasma torch 22 is also shown diagrammatically
in FIG. 4 and has housing structure 60 enclosing chamber 62 with a
water cooled electrode 64 that defines an outlet orifice 66.
Central electrode 68 is supported within chamber 62. Inert gas is
supplied through passage 70 to chamber 62 for flow around electrode
68 and out through orifice 66. A DC power supply 72 similar to
power supply 48 is connected to electrodes 64 and 68. A variety of
other plasma torch configurations may also be used. For example, a
porous anode torch of the type shown in U.S. Pat. No. 3,214,623 may
be employed in particular applications as the secondary plasma
torch.
A cutting operation is initiated by turning on the flow of inert
gas (i.e. argon) which enters chamber 36 of torch 20 through
conduit 44 and then passes out through orifice 42. DC power supply
48 is turned on, causing pilot arc 54 to form between cathode 32
and anode 40. The gas issuing from orifice is ionized by arc 54 to
form a plasma. The gas pressure in chamber 36 is maintained at
sufficient pressure so that a high velocity plasma-jet 24 issues
from orifice 42. Typical velocities are in the range of 5,000
ft./sec. and above and preferably above 10,000 ft./sec. Plasma-jet
24 is initially directed at the rock face 12 until a portion of the
rock is melted to form a molten film 80. The electrical
conductivity of this molten rock is higher than that of the solid
rock. Secondary torch 22 is put in operation by flowing argon gas
through the torch and applying electric power from the power supply
72. Pilot arc 74 is established between the central electrode 68
and the electrode wall of orifice 66. The diameter of orifice
passage 66 is greater than the diameter of orifice 42, passage 66
has greater length, and the pressure in chamber 62 is less than
that in chamber 36 of primary torch 20 so that a relatively low
velocity plasma stream 26 issues from torch 22. The plasma stream
26 from torch 22 is directed against and makes electrocal contact
with a portion of molten film 80 formed by the plasma jet 24 from
primary torch 20. Power supply 84, which in a particular embodiment
is a DC power supply of the welding type with a drooping
characteristic, but which may provide AC or AC superimposed on DC
depending on the particular application, is switched on and a
transferred arc path 86 is established with the current passing
along plasma arc 24, the molten rock 80 and plasma stream 26 which
provides a return electrode for the current, conducting it back to
torch 22 and to the power supply 84. A magnetic field usefully may
be employed on electrode 64 to rotate the contact point of the main
current carrying arc 86 in particular applications. The electric
current passing through the film 80 of molten rock strongly heats
the film so that additional rock underlying the current path is
melted. The high velocity jet 24 from torch 20 blows away material
and thus enhances the rock cutting. Jet 88 (e.g. compressed air or
a quench liquid) may be employed to facilitate removal of debris
from the slot 28. After the rock cutting operation has been
initiated, torches 20 and 22 are advanced in fixed relationship to
each other by mechanism 16 across the face 12 of the tunnel to form
the slot 28 in the face. Further slots are cut in the same manner
to produce a pattern of slots penetrating into the face a distance
which may typically be in the order of one foot or more.
After a pattern of slots is cut into the tunnel face as described
above, the blocks of rock are fragmented off the face. This is done
with a pair of plasma torches 90, 92 as shown diagrammatically in
FIG. 3. Apparatus for the cracking operation is shown in FIG. 3.
Torches 90 and 92 are similar to torch 20 described above except
they are constructed for lower velocity operation to produce a long
gaseous plasma column that extends to the base of the hole or slot
in the rock face. As the resistance of an argon column is in the
range of 0.1 ohm cm., little power is dissipated in the gaseous
electrode column. In particular applications, it may be
advantageous to use more than two gaseous electrodes.
When in operation, torches 90 and 92 are supported in front of rock
face 12 by torch holder 18. Suitable gas supplies, and power
sources (diagrammatically indicated at 94) are connected to torches
90 and 92. Each of the torches 90 and 92 is put into operation in a
manner essentially identical with that described above for torch
20. The plasma streams 96, 98 issuing from torches 90 and 92 are
directed into two spaced slots of the pattern. Each of the plasma
streams establishes electrical contact on the rock face of the slot
along which it flows and its low velocity maintains an enlarged
plasma environment at the base of the slot. The velocities of these
streams should be in excess of twenty feet per second and
velocities in the range of 100-200 feet per secnd are satisfactory
in a particular embodiment. Electrical power of a frequency
effective for dielectricly heating rock (e.g. a frequency in the
general range of 0.5 to 20 MHz) is applied across the two torches
90, 92 and through the plasma stream conductors 96, 98 to the rock
face adjacent to the plasma stream. The electric field applied
across the rock (preferably at a voltage gradient in the range of
750-7,500 volts/inch) produces a thermal "nugget" 100 in the center
of the rock blocks which creates thermal stress and fragments rock
from the face of the tunnel. The fragmenting process is repeated at
new locations in the slot pattern, thus extending the tunnel face
into the rock mass. After the face has been cleared by the
fragmenting process, the cutting process is resumed to further
advance the tunnel face.
As an example of the principle of transferred arc cutting of rock,
a standard TAFA Model 51 torch was connected to a 40 kW DC, 160
volt open circuit power supply. The torch had a nozzle diameter of
one-quarter inch and was located approximately 3/8 inch above the
face of a granite rock mass. A graphite rod was employed as the
secondary or return electrode. Once the non-transferred arc was
turned on and the rock became molten, the arc appeared to conduct
through the molten material to the graphite rod. Typical operating
parameters were:
DC volts 90 DC amps 400 Argon, gas flow (SCFH) 110
the jet velocity used during these tests was in the range of 5,000
fps. The cutting speed was about 2 inches per minute and over 5
cubic inches of rock were removed per kWH consumed
Thus it will be seen that the invention provides techniques
employing one or more gaseous electrodes for cutting and/or
breaking hard rock. While particular embodiments of the invention
have been shown and described, various modifications thereof will
be apparent to those skilled in the art and it is not intended that
the invention be limited to the disclosed embodiments or to details
thereof, and departures may be made therefrom within the spirit and
scope of the invention as defined in the claims.
* * * * *