U.S. patent number 3,830,428 [Application Number 05/334,555] was granted by the patent office on 1974-08-20 for plasma torches.
This patent grant is currently assigned to The Electricity Council. Invention is credited to Gordon Thomas Dyos.
United States Patent |
3,830,428 |
Dyos |
August 20, 1974 |
PLASMA TORCHES
Abstract
A method of cooling the nozzle of a plasma torch by forcing
water through the porous wall of the constrictor tube of the
nozzle. This method results in a number of advantages over the use
of a transpiring gas, including, no radiation shield being required
to protect the constrictor tube; the energy density of the plasma
arc is higher, the boundary of the plasma arc is better defined;
and there is less acoustic and ultra-violet radiation from the
plasma arc. A plasma torch is described having a porous constrictor
tube and means for supplying water for transpiration-cooling.
Inventors: |
Dyos; Gordon Thomas
(Capenhurst, EN) |
Assignee: |
The Electricity Council
(London, EN)
|
Family
ID: |
9849919 |
Appl.
No.: |
05/334,555 |
Filed: |
February 22, 1973 |
Foreign Application Priority Data
|
|
|
|
|
Feb 23, 1972 [GB] |
|
|
8302/72 |
|
Current U.S.
Class: |
239/11;
219/121.52; 239/13; 219/121.49; 219/121.5; 219/121.59;
239/132.5 |
Current CPC
Class: |
H05H
1/28 (20130101) |
Current International
Class: |
H05H
1/28 (20060101); H05H 1/26 (20060101); B23k
009/00 () |
Field of
Search: |
;239/13,11,128,132,132.1,132.3,132.5,424,429,431 ;219/121P |
References Cited
[Referenced By]
U.S. Patent Documents
Primary Examiner: Wood, Jr.; M. Henson
Assistant Examiner: Mar; Michael Y.
Attorney, Agent or Firm: Browne, Beveridge, DeGrandi &
Kline
Claims
I claim:
1. A method of cooling the nozzle of a plasma torch, comprising the
steps of providing a plasma torch having a constrictor tube formed
of porous material, providing a supply of working medium for the
plasma torch, operating the plasma torch in a manner to produce a
constricted plasma arc jet, and forcing water through the porous
constrictor tube into the bore of the tube whereby the plasma arc
column in the constrictor tube becomes highly constricted and of
increased energy density.
2. In a plasma torch including a constrictor tube formed of a
porous material and a means for providing a supply of working fluid
to the torch to produce a plasma arc jet, the improvement
comprising means for providing a supply of water to the outside of
said constrictor tube and pumping means for raising the pressure of
the water so supplied to a predetermined value to force the water
through the walls of said porous constrictor tube into the bore
thereof whereby the plasma arc column in the constrictor tube
becomes further constricted and of increased energy density.
3. A plasma torch as claimed in claim 2 wherein the porous material
is a ceramic material.
4. A plasma torch as claimed in claim 2 wherein the pore size of
the porous material lies in the range from 1.5 to 1500 microns.
5. A plasma torch as claimed in claim 4 wherein the pore size is 15
microns.
6. A plasma torch provided with a nozzle having a constrictor tube
formed of a porous material, and comprising means for supplying
water to the outside of the constrictor tube, pumping means for
raising the pressure of the water so supplied to a predetermined
value, and having a sleeve fitting coaxially around the nozzle and
wherein the nozzle has a throat portion removably sealed within the
sleeve and having a peripheral recess which forms, with the inside
surface of the sleeve, a cavity for the flow therethrough of
cooling water.
7. A plasma torch as claimed in claim 6 wherein the constrictor
tube is removable, and wherein the throat portion is formed having
a first part and a second part, the second part being disposed
between the first part and the constrictor tube and being
removeably sealed to the first part and removable from the torch,
and the first part being formed with the peripheral recess and
being removably sealed within the sleeve.
8. A plasma torch provided with a nozzle having a throat portion
and a porous ceramic constrictor tube, and including: a sleeve
fitting around the nozzle, the throat portion having an O-ring seal
at each of two axially-spaced positions on the peripheral surface
thereof, the O-ring seals engaging the inside surface of the
sleeve, the throat portion also having a peripheral recess disposed
between the O-ring seals; an inlet tube and an outlet tube
communicating through the sleeve with the peripheral recess for
flow and return of a coolant thereto; an annular groove in the
inside surface of the sleeve disposed below the throat portion, a
retaining ring fitting within the annular groove and retaining the
throat portion within the sleeve; a stop within the sleeve above
the throat portion for limiting the upward movement thereof, a
screw cap mounted for axial movement relative to the sleeve and
having a coaxial central aperture corresponding to the bore of the
constrictor tube; a seal between the screw cap and the lower end of
the constrictor tube; a seal between the upper end of the
constrictor tube and the lower end of the throat portion; an
annular cavity around the constrictor tube, a passageway
communicating with said annular cavity, an inlet pipe for
introducing transpiring water into the passageway, and means for
controlling the pressure of water supplied to the passageway.
9. A plasma torch as claimed in claim 8 wherein the throat portion
is formed having a first part and a second part, the second part
being disposed between the first part and the constrictor tube and
being removeably sealed to the first part, and the first part being
formed with the peripheral recess and carrying the O-ring seals.
Description
This invention relates to plasma torches and to a method of cooling
the nozzles of a plasma torch.
Plasma torches are known in which the nozzle is cooled by the flow
of a cooling fluid (usually water) through an annular chamber
surrounding the bore of the nozzle. The same chamber may serve to
cool the throat of the nozzle, or a separate chamber may be used.
The material of the nozzle is impervious to the cooling fluid, and
an arc produced by a torch having such an arrangement is known as a
"water-cooled arc."
The nozzle of a plasma torch is formed to provide a throat leading
to a bore. That part of the nozzle in which the bore is formed is
known as, a constrictor tube.
It is also known, for example from the following articles,
"Transpiration cooling of a constricted Electric-arc Heater" by J.
E. Anderson and E. R. G. Eckert, AIAA Journal, April 1967;
"Experimental Investigation of a Transpiration-Cooled, Constricted
Arc" by E. Pfender, G. Gruber and E. R. G. Eckert, Proceedings of
the Third International Symposium on High Temperature Technology,
held September 1967;
"Study of a Transpiration-Cooled, Constricted Arc" by J. Heberlein,
E. Pfender, and E. R. G. Eckert, ARL Technical Documentrary Report
70-0007, January 1970 published Aerospace Research Laboratories,
Office of Aerospace Research, United States Air Force; and
"Transpiration-Cooling of the Constrictor Walls of an Electric
High-Intensity Arc," by J. Heberlein and E. Pfender, Transactions
of the ASME, May 1971, to form the constrictor tube of a plasma
torch of a porous material and to feed a transpiring gas, usually
argon or nitrogen, through the walls of the tube while the torch is
in use. The arc produced by a torch having this arrangement is
known as a "transpiration-cooled arc."
SUMMARY
According to one aspect of the present invention, a method of
cooling the nozzle of a plasma torch, which nozzle has a
constrictor tube formed of a porous material, comprises the step of
forcing water through the porous material into the bore of the
nozzle while the plasma torch is in use.
According to another aspect of the present invention, a plasma
torch, provided with a nozzle having a porous constrictor tube,
comprises means for supplying water to the outside of the
constrictor tube, and pumping means for raising the pressure of the
water so supplied to a predetermined value.
The pore size of the material is preferably in the range of 1.5 to
1500 microns and more preferably is 15 microns. The constrictor
tube may be formed from a ceramic material.
The throat portion may be removably sealed within a sleeve of the
torch and have a peripheral recess which forms, with the inside
surface of the sleeve, a cavity for the flow therethrough of
cooling water. By this means cooling water may pass through the
wall of the sleeve via inlet and outlet pipes for circulation
around the peripheral recess, and the throat portion may be removed
from the sleeve without any disturbance of the cooling system.
Preferably the constrictor tube is removable and the throat portion
is formed having a first part and a second part, the second part
being disposed between the first part and the constrictor tube and
being separable from the first part and removable from the torch,
and the first part being formed with the peripheral recess and
being removably sealed within the sleeve. Thus if it is required to
change the bore size of the nozzle, the constrictor tube can be
replaced by a tube of the required bore size, and the second part
of the throat portion can be replaced by a corresponding part
having an appropriate configuration for matching the first part to
the replacement constrictor tube.
When the plasma torch is in use transpiring water is forced through
the wall of the porous constrictor tube and becomes partially
vaporized as it emerges from the pores on the inside surface of the
tube. This use of water as the transpiring medium results in a
number of advantages over the use of a gas as the transpiring
medium. Such advantages include:
a. More of the heat energy radiated from the plasma arc is absorbed
by the partially vaporized water than would be absorbed by a
transpiring gas and therefore when using water it may not be
necessary to use an auxiliary means for reducing the amount of
radiant heat energy incident upon the wall of the constrictor
tube.
b. The large change of volume which occurs when the water vaporizes
results in a greater constriction of the arc, and thus a higher
energy density, than can be achieved using a transpiring gas.
c. The boundary between the plasma arc and surrounding layer of
partially vaporized water is more sharply defined than when using a
transpiring gas.
d. There is less acoustic radiation from the plasma arc external to
the constrictor tube. This is thought to be due to less turbulence
in the partially vaporized water surrounding the plasma arc than is
experienced using a transpiring gas, the flow being more
streamlined because of the higher density of the vapour and water
droplets.
e. The partially vaporized water absorbes ultra-violet radiation
from the plasma arc more strongly than a transpiring gas.
The increased power density of the arc resulting from the
constriction by the transpiring water (partially vaporized) enables
the torch to be used to obtain an improved quality of cut compared
with conventional water-cooled arcs and gas transpiration-cooled
arcs. Also, the maximum linear rate of cutting at which acceptable
cut quality is achieved is greater than that for such arcs.
DESCRIPTION OF THE DRAWINGS
FIG. 1 is a partly cut-away schematic representation of a plasma
torch;
FIG. 2 is a partly schematic longitudinal section in the region of
the nozzle assembly of the torch of FIG. 1; and
FIG. 3 is a corresponding section showing a modification of the
nozzle of FIG. 2.
DETAILED DESCRIPTION
In FIG. 1 a plasma torch, indicated generally at 10, comprises a
torch body 11 within which is mounted a water-cooled cathode 12.
The cooling of the cathode is by conventional water-cooling, water
being supplied via inlet pipe 13 and being returned via outlet pipe
14, disposed at the top of the plasma torch. The cathode has a
conical portion 15 ending in a radiussed tip 16. The conical
portion 15 is disposed within a conical throat portion 17 of a
nozzle assembly of the plasma torch. The conical throat leads into
a cylindrical bore in a constrictor tube portion 18 which is
coaxial with the throat portion 17.
The throat portion 17 is formed of copper and includes an internal
annular cavity 19 for the flow of water to cool the cathode in a
conventional manner.
The constrictor tube portion 18 is formed from a tube of porous
ceramic material around which is an annular cavity 20 connected via
an inlet pipe 21 to a pump 22 for controlling the supply of water
at a pressure in the region of 300 lbs/sq. in for transpiration
cooling of the constrictor tube portion.
In FIG. 2, which shows the nozzle assembly and surrounding
components more clearly, the throat portion 17 basically comprises
an upper horizontal disc having a large central hole therein, a
lower horizontal disc of the same radius as the upper disc and
having a small central hole therein, and a conical wall which joins
the periphery of the large central hole to the periphery of the
small central hole.
The throat portion 17 is mounted within a sleeve 23 being sealed to
the inside surface thereof by means of an upper O-ring 24 fitted in
a peripheral groove in the rim of the upper disc, and by means of a
lower O-ring 25 fitted in a peripheral groove in the rim of the
lower disc. The upper and lower discs and the conical wall form a
peripheral recess which becomes the cavity 19 when bounded by the
inside surface of the sleeve 23. An inlet pipe 26 and an outlet
pipe 27 sealed to the sleeve 23 communicate with the cavity 19 for
the flow and return of cooling water. By this means the throat
portion 17 can be removed from the sleeve while leaving the pipes
26 and 27 in place.
The body 11 has a short downwardly extending annular wall 28
fitting within the sleeve 23 and forming an abutment for defining
the uppermost position of the throat portion 17. The throat portion
17 is retained within sleeve 23 by means of a retaining ring 29
fitting in a recess extending around the inside surface of the
sleeve 23.
An insulating sleeve 30 fits around the outside of sleeve 23 and
has at its lower edge an inwardly directed flange 31 with a central
circular aperture of slightly less diameter than the inside
diameter of sleeve 23. A cap 32 is screwed to the insulating sleeve
30. A retaining cap 33 is screwed into cap 32 and maintains the
tube of porous ceramic material, forming the constrictor tube 18,
pressed upwardly against the lower surface of the throat portion 17
which is in turn pressed upwardly against wall 28. A seal 34 is
provided at the upper surface of the tube 18, and also between the
lower surface and the retaining cap 33. The diameter of the small
central hole in the lower horizontal disc of the throat portion 17
is the same as the diameter of the bore of the constrictor tube 18,
and the retaining cap 33 has an exit hole 35 coaxial with, and of
the same diameter as the bore of the constrictor tube 18, and
having its lower peripheral edge flared.
Inlet pipe 21 communicates with the top of a vertical channel 37 in
the wall of sleeve 23. The top of channel 37 is otherwise blind and
its bottom opens into a shallow annular recess 38 in the upper
surface of the flange 31. A series of small bores 39 lead from the
recess 38 into the annular cavity 20 between the constrictor tube
18 and the flange 31. The bores 39 are angled at 60.degree. to the
longitudinal axis of the plasma torch.
FIG. 3 shows a modification of the arrangement of FIG. 2 in which
the throat portion 17 is formed of upper and lower parts 17a and
17b respectively, and has a different throat configuration. The
upper throat portion 17a is formed basically as the throat portion
17 shown in FIG. 2 but differs in that the aperture at the lower
end is larger and is threaded to receive the lower throat portion
17b and in that the wall joining the upper and lower discs extends
axially and turns inwardly at its lower end to form with a
corresponding portion of the lower throat portion 17b, an inwardly
directed shoulder 40 which leads into the conical throat 41 of the
lower throat portion 17b. The conical throat 41 corresponds to the
lower part of the throat portion 17. An O-ring seal 42 is provided
between throat portions 17a and 17b.
By utilizing the above arrangement of FIG. 3, the bore size of a
plasma torch may readily be changed by the replacement of the lower
throat portion 17b, the constrictor tube 18 and the retaining cap
33, by the equivalent items for the different bore size.
The porosity of the ceramic material is selected not so small as to
require too high a supply pressure for the transpiring water, yet
not so large as to introduce too much water into the constrictor
bore. A preferred range of pore size is from 1.5 to 1500 microns.
The most preferred pore size is 15 microns at which a suitable flow
rate for the transpiring water is 100 ml/min for a bore diameter of
5 mm, and under these conditions the constriction ratio is in the
region of 3 to 1, in other words the arc becomes constricted by the
partially vaporized water and its effective diameter is
approximately one-third of the diameter of the bore of the
constrictor tube.
By forming the constrictor tube from a ceramic material, any
tendency of the plasma torch to produce a double arc is greatly
reduced. However, if it is not required to take advantage of this
feature of the ceramic constrictor tube, then the tube may be
formed from another porous material, for example, a sintered
metal.
The bore of the constrictor tube may be profiled in order to obtain
a degree of focussing such that the arc diameter is reduced in the
region at, or adjacent, the exit of the bore.
* * * * *