U.S. patent number 3,770,935 [Application Number 05/210,350] was granted by the patent office on 1973-11-06 for plasma jet generator.
This patent grant is currently assigned to Rikagaku Kenkyusho. Invention is credited to Torao Ichimiya, Haruo Tateno.
United States Patent |
3,770,935 |
Tateno , et al. |
November 6, 1973 |
PLASMA JET GENERATOR
Abstract
Disclosed is an improved plasma jet generator comprising at
least two plasma jet torches and a guide attachment integrally
connected to the torches with a view to fixing the anode foot of a
non-transferred type plasma jet. This special structure permits the
proper selection of the point of the anode foot of the plasma jet
with respect to the cathode spot of the plasma jet, thus realizing
a high voltage plasma jet. Also, the new structure prevents the
local erosion to the parts of the electrodes on which the anode
foot and the cathode spot stand by means of an inactive gas, thus
allowing the main arc column to directly heat a high concentrated
active gas.
Inventors: |
Tateno; Haruo (Tokyo,
JA), Ichimiya; Torao (Hayama-Machi, JA) |
Assignee: |
Rikagaku Kenkyusho (Wako-shi
Saitama-ken, JA)
|
Family
ID: |
26413474 |
Appl.
No.: |
05/210,350 |
Filed: |
December 21, 1971 |
Foreign Application Priority Data
|
|
|
|
|
Dec 25, 1970 [JA] |
|
|
45/118284 |
Sep 17, 1971 [JA] |
|
|
46/72338 |
|
Current U.S.
Class: |
219/121.47;
219/121.5; 219/121.52; 219/75; 219/121.51 |
Current CPC
Class: |
H05H
1/44 (20130101); H05H 1/26 (20130101) |
Current International
Class: |
H05H
1/44 (20060101); H05H 1/26 (20060101); B23k
009/00 () |
Field of
Search: |
;219/121P,121R,74,75
;315/231 |
References Cited
[Referenced By]
U.S. Patent Documents
Primary Examiner: Albritton; C. L.
Assistant Examiner: Peterson; Gale R.
Claims
What is claimed is:
1. A plasma jet generator comprising a plurality of plasma jet
torches, a hollow guide attached to said torches, said hollow guide
having an outlet and a plurality of inlets, said inlets being
disposed to receive and direct the gas streams from respective
torches to intersect at a given location within the guide to form a
combined plasma jet exiting the guide through said outlet, said
inlets and outlets being the only openings in said hollow guide,
one of said torches including a cathode rod and at least two
bushings which define a gas flow space, and said hollow guide being
electrically insulated from at least one of said torches by a body
of dielectric material.
2. A plasma jet generator according to claim 1 including two plasma
jet torches disposed to produce gas streams that are oriented
generally perpendicular to each other.
3. A plasma jet generator according to claim 1 including three
plasma jet torches disposed to produce gas streams, two of which
gas streams are oriented generally symmetrical with respect to the
third gas stream.
Description
This invention relates to a plasma jet generator including a
plurality of plasma jet torches which are capable of independently
functioning as the plasma jet torch of straight polarity.
Thus, the wall of the torch will be free from the damage which
would be caused by using the torch wall as the negative electrode
if the torch is used in the mode of reverse polarity. The plasma
jets ejected from those plasma jet torches will meet one another in
the inner space of a guide attachment which are integrally
connected with the torches. A main arc can be established in the
electrically conductive space by applying a voltage from a main
power supply with one electrode of each plasma jet torch used as
the positive or negative electrode, and the gas supplied will be
heated by the main arc and then properly directed by the guide
attachment.
A plasma jet generator (hereinafter abbreviated to P.J.G.) has been
widely used in cutting, welding, coating and other operations. The
basic structure of P.J.G. (see U.S. Pat. No. 2,806,124) was
originally developed by Union Carbide Corporation, and numerous
improvements have been proposed. In these P.J.G.'s, the factors to
determine the electric characteristics thereof are as, for
instance, follows: gas flow rate, gas compositions, size of
caliber, distance between the electrodes, and electric current
values. It should be noted that the arc voltage also depends on
these factors.
The efficiency of heating gas is usually given by the following
equation:
The efficiency of heating gas (.eta.) ##SPC1##
Provided that:
Torch Consumption(L.sub.t) = K .times. Electric Current(I) +
Thermal Conduction to Casing Wall(L.sub.w) (2)
where K is a constant.
By substituting Equation (2) for the corresponding term of Equation
(1) the following equation can be obtained:
.eta. = 1 - K/V - L.sub.w /VI (3)
the last term is negligible for its smallness, and therefore it is
apparent the efficiency will increase with the arc voltage.
A conventional method of increasing the arc voltage is to increase
the eddy component of the gas stream in passing through the
torch.
Another means to increase the arc voltage is to provide recessed
portions electrically isolated both from the anode and the cathode
in the flow path of gas. However, relaying on these means, the arc
voltage for given values of gas flow rate and electric current
cannot be raised beyond a certain critical value without
accompanying adverse effects such as double arcing, damage of the
throat aperture, and deviation or unstability of the arc column.
P.J.G.'s heretofore proposed still have defects such as
complicatedness in structure, difficulty in operation and narrow
range for varying electric current, gas flow rate and other
factors.
An object of this invention is to provide an improved P.J.G. which
is characteristic of the high arc voltage and hence the highly
improved efficiency of heating gas and little or no electrode
consumption.
Another object of this invention is to provide a new high-voltage
P.J.G. in which an active gas of high density can be heated
directly by the arc column. This direct heating of concentrated
active gas by means of the arc column was deemed as impossible in
the prior art.
This invention will be better understood from the following
description which is to be made with reference to the accompanying
drawings:
FIG. 1 shows an embodiment of the P.J.G. according to this
invention in section and an associated electric circuit;
FIG. 2 is a similar view to FIG. 1, but shows a different
embodiment suitable for a concentrated active gas and an associated
electric circuit;
FIGS. 3 - 8 show partly in section, different guide attachments
suitable for use in the P.J.G. given in FIG. 1;
FIG. 9 is a similar view to FIG. 2, except for the structure of the
guide attachment;
FIG. 10 shows in section an embodiment of this invention having two
positive plasma jet torches and one negative plasma jet torch, and
an associated circuit; and
FIG. 11 shows in cross-section, different shapes of the
white-bright portion of the plasma flame at the outlet.
Referring to FIG. 1 there is shown a primary P.J.G. according to
this invention which consists of a positive plasma jet torch A, a
negative plasma jet torch B and a guide attachment C. The positive
plasma jet torch A has a cathode rod 1 and at least two bushings 2,
3 mounted concentric with the cathode rod. The second bushing 3 has
an arc throttle aperture 4. A gas such as Argon, Helium and other
inactive gases is supplied in the form of stream 7 and 8 from the
inlets 5 and 6 to the annular space formed between the cathode and
the first bushing 2 and the one between the first bushing 2 and the
second bushing 3 respectively. The negative plasma jet torch B has
a cathode rod 9 and a bushing 11 positioned concentric with the
cathode. The bushing 11 has an arc throttle aperture 10. An
inactive gas 13 is supplied from the inlet 12 to the annular space
formed between the cathode 9 and the bushing 11.
The guide attachment C has two inlets 15 and 16 and one outlet 17.
These inlets are so positioned that when the guide attachment is
fixed to the positive and negative jet torches, these inlets
function to direct the gas streams from the torches to the
intersection of the center axis of these torches, whereas the
outlet is so positioned that it functions to allow the resultant
gas stream to flow from the intersection to the exterior.
It should be noted that the guide attachment is fixed to at least
one bushing (the bushing 3 of the positive plasma jet torch in FIG.
1) via an insulator 18 of a dielectric material, and that a gas 20
is supplied from the inlet 19 to the annular space formed by the
insulator 18 at the joint part. The cathode holders 50, 51 and the
bushings 2, 3, 11 and the guide attachment C are water-cooled by a
proper means (not shown), and are integrated via insulators 52 of,
for instance, Bakelite in a complete air-tight manner.
An auxiliary power supply 21 includes a high-frequency oscillator
for arc-establishment. The negative terminal of the power supply 21
is connected to the cathode 1 of the positive jet torch A via an
electric switch 22 whereas the positive terminal is connected to
the bushing 2 of the torch A.
Likewise, the negative terminal of the main power supply 23
containing a high-frequency oscillator for arc-establishment is
connected to the cathode 9 of the negative plasma jet torch B, and
the positive terminal of the main power supply is connected to the
bushing 2 of the torch A. The positive terminals of the power
supplies 21, 23 are connected to the bushing 11 via a switch 24.
The P.J.G. thus connected to the associated circuit will be
operated as follows:
1. Gas 7, 8 is supplied to the positive plasma jet torch A, and
then the high-frequency oscillator of the auxiliary power supply 21
is put into operation by closing the switch 22. As a result an
auxiliary arc 25 is established and finally a plasma jet flame is
formed and extends from the arc-throttle aperture 4 into the guide
attachment C.
2. gas 13 is supplied, and then the high-frequency oscillator of
the main power supply 23 is brought into operation by closing the
switch 24. As a result an arc 26 is established, and then a plasma
jet flame is formed and extends from the arc-throttle aperture 10
into the guide attachment C.
3. after the plasma jet flames of straight polarity are thus
established and meets one another at the intersection 14, the
switch 24 is opened. Then a hairpin shaped main arc is formed, and
the plasma jet flame 28 extends from the outlet 17 of the guide
attachment C to the exterior.
The supply of the gas stream 20 from the inlet 19 of the guide
attachment C may be begun before or after operation 3 above. The
hairpin-shaped arc happens to open wide, and as a result the curved
leg of the arc approaches one side of the inlet 15 of the
attachment to excessively heat the wall of the inlet 15. Partly
because of this and partly because of the injection of ions into
the inlet wall it is most likely that a cathode spot is formed on
the inlet wall. This is the cause for the formation of a double
arc. The supply of the gas stream 20 is useful to first, prevent
the "hairpin" arc from opening wide and second, prevent ions from
invading the inlet wall, thus finally eliminating the possibility
of establishing a double arc.
The high-voltage P.J.G. thus operated is capable of establishing a
stable arc whose arc-voltage is at least two times as high as the
arc-voltage of the conventional P.J.G. for given electric current
and gas flow rate.
EXAMPLE 1
The particulars of the apparatus according to the embodiment shown
in FIG. 1 are:
Diameter of the throttle aperture 4 of the bushing 3 -- 2 mm
Diameter of the inlet 15 of the guide attachment -- 3 mm
Diameter of the inlet 16 of the guide attachment -- 2 mm
Diameter of the passage 30 of the guide attachment -- 5 mm
Distance from the intersection 14 to the end of the bushing 2 -- 18
mm
Distance from the intersection 14 to the tip of the cathode 9 -- 27
mm
Flow rate of gas 7 (Argon) -- 0.2 l/min.
Flow rate of gas 8 (Argon) -- 0.4 l/min.
Flow rate of gas 13 (Argon) -- 3.0 l/min.
Flow rate of gas 20 (Argon) -- 0.2 l/min.
Arc current -- 20 A
A possible longest plasma jet flame was formed and the arc voltage
was as high as 76 volts. (The arc voltage in the conventional
plasma jet torch is 30 volts or less for the same current and flow
rate.)
Referring to FIG. 2, there is shown a P.J.G. according to this
invention which is capable of heating a concentrated (90 percent or
more) gas chemically active to the material of the electrode such
as oxygen or air directly by means of an arc column.
In spite of ever increasing demand for this capability of direct
heating an active gas in the fields of chemical reactions, coating,
cutting and other appliances since the appearance of the P.J.G., it
could not be attained before the completion of this invention.
In the apparatus of FIG. 2 the positive plasma jet torch A is
similar to that of the apparatus of FIG. 1. The negative plasma jet
torch B has an extra bushing 34 with a throttle aperture 34' and
extra inlets 35, 36 for gas 37, 38, compared with the negative
plasma jet torch B in FIG. 1. The guide attachment C is fixed to
the bushing 34 via an electric insulator 18. Complying with this
modification the positive terminal of the main power supply 23 is
connected to the bushings 11 and 34 and the guide attachment C.
This apparatus can be operated as
1. Argon is supplied in the form of gas stream 7, and then the
switch 22 is closed to start the operation of the high-frequency
oscillator of the auxiliary power supply 21 with a result of a
establishing an auxiliary arc 25. Then, the plasma jet flame is
ejected from the throttle aperture 4, and it extends into the main
passage 30. Additionally, argon is supplied in the form of the gas
streams 8 and 20.
2. Argon is supplied in the form of the gas streams 13, 37 and 38,
and then the switches 24, 24' and 24" are closed for the main power
supply 23 to apply a d.c. voltage and a high-frequency voltage to
the torch B and the guide attachment C with a result of
establishing the first non-transferred arc 26. Then, the switch 24
is opened, transforming the arc column into the second
non-transferred arc 26'. Next, the switch 24' is opened, thus again
transforming the arc column into the third non-transferred arc 26".
Then, the supply of gas 13 to the cathode is made to cease, and the
switch 24" is opened with a result of establishing the main arc
column 27.
3. The switch 22 is opened to extinguish the arc 25, and at the
same time the supply of gas 7 to the cathode is made to cease.
Finally, the gas streams 20 and 38 are switched from argon to air
or oxygen. Thus, a highly concentrated active gas plasma jet can be
obtained.
This operation can be reduced to a full automatic "on-off"
operation by using a piping system which includes pre-adjusted
needle valves and electromagnetic valves.
EXAMPLE 2
The particulars of the apparatus shown in FIG. 2 are:
Diameter of the inlet 15 or 16 of the guide attachment C 3 mm
Diameter of the gas channel of the guide attachment 5 mm
Diameter of throttle aperture 34' of the bushing 34 2 mm
Distance from the intersection 14 to the end surface of the bushing
2 18 mm
Distance from the intersection 14 of the tip of the cathode 9 34
mm
Flow rate of the gas stream 8 (Argon) 0.3 l/min.
Flow rate of the gas stream 20 (Oxygen) 0.2 l/min.
Flow rate of the gas stream 37 (Argon) 0.3 l/min.
Flow rate of the gas stream 38 (Oxygen) 5 l/min.
Arc current 20 A
A plasma flame of 90 percent oxygen concentration was obtained, and
the arc voltage was as high as 115 volts. The substitution of air
for oxygen caused the arc voltage to rise up to 135 volts.
A mixture of a higher active gas content can be used by enhancing
the cooling capability to the bushings and by increasing the arc
current.
With a view to improving the directional stability of the plasma
jet flame and at the same time with a view to increasing the
efficiency of heating gas the inventors carried out experiments on
a variety of guide attachments as follows:
The guide attachment shown in FIG. 3 is the same as the
corresponding part of the apparatus shown in FIG. 1 except for a
notched portion a at the downstream side thus making the terminal
end of the outlet 17 fairly close to the "hairpin" arc column. In
this modification the plasma jet flame 28 deviated apart from the
center axis 29 of the outlet 17, and the directionarity varied with
the gas flow rate and the value of electric current.
FIG. 4 shows further modification of the guide attachment of FIG. 3
in that the gas channel is enlarged around the intersection 14 at
the upstream side while still maintaining the cross-section of the
outlet equal to that of the outlet of the guide attachment shown in
FIG. 1 or 3. In this case the plasma jet flame 28 was positioned on
the center axis 29 of the outlet 17.
FIG. 5 shows a guide attachment shown in FIG. 1 modified in the
same manner as in FIG. 4. In this modification, likewise, the
plasma jet flame 28 was positioned on the center axis 29 of the
outlet 17, and what was better, the length of the white bright
portion of the laminated flow of the plasma jet flame was increased
approximately 50 percent. This indicates that the ejection of the
plasma jet flame was remarkably enhanced. A similar result was
obtained with regard to the guide attachment the gas channel of
which was modified as indicated by broken line 31.
FIG. 6 shows further modification of the guide attachment of FIG. 5
in that the part b indicated by broken line was removed. In this
case the laminar stream of the plasma jet flame 28 deviated with
respect to the center axis 29 of the outlet 17.
The guide attachments shown in FIGS. 3, 4, 5 and 6 were tested for
the same values of gas flow rate and electric current.
The results of these experiments indicate that:
1. The removal of the part a from the end of the attachment given
in FIG. 1 is useful to direct the plasma jet flame along the center
axis 29 of the guide channel.
2. The cross-sectional enlargement of the guide channel shown in
FIG. 4 endows the guide attachment with the directionality of the
plasma jet flame.
3. The enlargement of the guide channel in the guide attachment
free of the notched portion a as shown in FIG. 5 is useful to
reduce the loss of the plasma jet flame which otherwise would be
caused at the part corresponding to the notched portion a in FIG.
3.
4. if the cross-sectional enlargement extends far to the inlet of
the guide attachment as shown in FIG. 6, the effect of directing
the plasma jet flame on the center line will disappear. From the
results of the experiments above mentioned, the inventors reached
the conclusion as follows:
The structures of the guide attachments given in FIGS. 4 and 5 are
useful to throttle the disturbing fluid flow which results from the
two gas streams supplied from the two inlets of the guide
attachment so as to allow the resultant flow to align in the center
line of the guide attachment.
As seen from FIG. 6, the position of the outlet relative to the arc
column is critical, and it is necessary to allow a part of the
"hairpin" arc or at least the sharp bent portion of the "hairpin"
to appear in the throttle aperture for the following reasons:
First, the entrance of a part of the arc column into the throttle
aperture will cause the rise of the temperature of the gas in the
throttle aperture, and hence the increase of the cubic expansion of
the gas, finally resulting in the increase of the flow resistance
of the throttle, which is useful to improve the directing
capability of the throttle. Second, the directing effect realized
by the wall of the aperture at the sacrifice of the heat loss as is
the case with the device in FIG. 1, can be reduced, and the
ejection of the plasma jet flame will be improved because the
"hairpin" of the arc whose thermal energy is about half the total
energy of the arc column, is aligned in the central axis of the
throttle aperture for heating the gas.
FIGS. 7 and 8 show other modifications of the guide attachment. The
guide attachment of FIG. 7 is specifically designed for the cutting
operation. In this example the space 32 which the "hairpin" enters
is made larger than the outlet 17 of the guide attachment which is
for instance as small as 1.0 mm diameter across, because otherwise
the "hairpin" would not enter the throttle aperture.
FIG. 8 shows a modification of the guide attachment of FIG. 4. In
this modification a blind hole 33 is made on the wall of the guide
channel opposite to the inlet 15 of the guide attachment. Thus, the
directness of a laminar flow of plasma jet which is ejected from an
aperture 17 of relatively small diameter was substantially
improved.
As is apparent from the results of the experiments on the
modifications given in FIGS. 3 - 6, the directness of a plasma jet
flame can be improved, and at the same time the efficiency of
heating gas can be raised by enlarging the cross-section of the
guide channel over the length of the channel beyond the
intersection of the two center axes of the positive and negative
plasma jet torch towards the outlet.
FIG. 9 shows a P.J.G. which is equivalent to the embodiment of FIG.
2 modified by substituting the guide attachment of FIG. 4 or 5 for
the corresponding member of the apparatus of FIG. 2. This
modification was compared with the apparatus of FIG. 2 as
follows:
EXAMPLE 3
Operating condition:
Gas stream 8 -- Argon 0.3 l/min.
Gas stream 37 -- Argon 0.3 l/min.
Gas stream 7 -- none
Gas stream 13 -- none
Gas stream 38 -- Oxygen 4 l/min.
Gas stream 20 -- Oxygen 1 l/min.
Arc voltage -- 95 V
Arc current -- 50 A
P.j.g. of FIG. 2
Diameters d.sub.1, d.sub.2 of the inlets 15, 16 -- d.sub.1, d.sub.2
= 3.0 mm
Diameter d.sub.3 of the outlet 17 -- d.sub.3 = 5.0 mm
Distance l from the intersection 14 to the outlet 17 -- .about.l =
8.5 mm
The plasma jet flame extended 25 to 30 cm, and it deviated about
2.degree. apart from the center axis 29.
P.J.G. of FIG. 9
Diameters d.sub.1, d.sub.2 of the inlets 15, 16 d.sub.1, d.sub.2 =
3.0 mm. Diameter d.sub.3 of the outlet d.sub.3 = 5.0 mm Diameter
d.sub.4 of the guide channel d.sub.4 = 7.0 mm Distance l.sub.1 from
the intersection 14 14 to the outlet 17 l.sub.1 = 4.5 mm, l.sub.2 =
4.0 mm
The plasma jet flame extended 35 to 50 cm on the central axis
29.
The throttle part was modified into the two step form as shown in
FIG. 7.
The following arc voltages were realized for different diameters
d.sub.2 and d.sub.3 of the inlet 16 and the outlet 17, and the
ejection of the plasma jet flame suitable for the cutting operation
was substantially improved.
Pressure in the Guide d.sub.2 d.sub.4 Arc Voltage Attachment (Gauge
dia. dia. Pressure) 3.0 mm 3.0 mm 95 V 2.0 mm 1.5 mm 110 V 0.1
kg/cm.sup.2 2.0 mm 1.0 mm 120 V 1.0 kg/cm.sup.2
EXAMPLE 4
Operating Condition
Gas stream 38 -- Oxygen 12 l/min.
Gas stream 20 -- Oxygen 3 l/min
(The flow rates of the other gas streams were equal to those in
Example 3.)
Arc voltage -- 130 V
Arc current -- 50 A
P.j.g. of FIG. 2
The dimensions of the apparatus were identical with those of
Example 3. The incandescent part of the flame was composed of a
disturbed flow about 2 cm. long, and the plasma jet flame deviated
about 3.degree. or more apart from the central axis.
P.j.g. of FIG. 9
The particular dimensions of the apparatus were identical with
those of Example 3. The incandescent part of the flame was composed
of a disturbed stream about 3.5 cm long, and the plasma jet flame
was directed straight.
The deviation and the length of the plasma jet flame is a direct
measure for the efficiency of heating gas for a given condition. In
view of this it is apparent that the effect of the special
structure of the guide attachment given in FIG. 4 or 5 is
remarkable for improving the efficiency of heating gas.
Additionally, the capability for varying the flow rate of the gas
stream 20 over a wide range facilitates the operation of the
apparatus.
As seen from the above, the P.J.G. according to this invention has
a single throttle aperture and at least one anode electrode,
essentially different from a conventional P.J.G. using the inside
wall of the throttle aperture as the anode electrode.
The advantages attributable to the use of a plurality of positive
plasma jet torches are:
First, as a matter of course, the anode input power can be equally
divided into as many parts as the positive plasma jet torches, thus
avoiding the damage of the throttle aperture due to the local
concentration of heat as is the case with the conventional P.J.G.
Second, the adverse effect by the gas injection from the inlet 15
on the main arc column can be substantially reduced.
FIG. 10 shows a P.J.G. having a negative plasma jet torch and two
positive plasma jet torches positioned symmetrical to the negative
torch. This apparatus is identical with the apparatus of FIG. 1
except for the guide attachment. A single switch 24 is provided for
generating a plasma jet flame in each of the negative torches.
Although two auxiliary power supplies 21 are shown in the drawing,
a single power supply in place of these devices can be used by
properly modifying the relevant electrical connection because the
device is not used with regard to the positive plasma jet torches
at the same time.
In operation, a main arc is established by the positive plasma jet
torch to which the switch 24 is connected (right torch in the
drawing), in the same manner as in the apparatus of FIG. 1. With
the main arc thus established, an auxiliary arc is established by
the other positive plasma jet torch (left torch in the drawing),
and then a main arc is established therein. After the establishment
of the main arc at the left side the switch 22 is opened, and then
the supply of the gas stream 7 is made to cease. The flow rates of
the gas 7 and 8, such as argon are set to a proper value, for
instance 0.2 l/min. Thus, the main arc 27 is finally
established.
In a particular example of the apparatus the total electric current
was 40 A and the arc voltage was 73 V.
FIG. 11 shows the shapes of the cross-sections of the incandescent
cores of different plasma jet flames which are ejected from the
main channel 30 when the gas is supplied from either of the right
and left positive plasma jet torches at an equal pressure balancing
at the center of the main channel. In this drawing the outer circle
39 is the wall of the main channel of the guide attachment, and the
direction of the gas supplied by the positive plasma jet torch is
indicated by the arrow. The shaded part 40 is the cross-section of
the incandescent part or core of the plasma jet flame in the outlet
17.
FIG. 11-I pertaining the use of a single positive plasma jet torch
shows the "off-center" position of the incandescent core, the
cross-section of which is of an ellipse. This phenomenon is
observed in the plasma jet flame in a conventional torch.
FIG. 11-II pertaining to the use of two positive plasma jet torches
shows the "on-center" position of the incandescent core 40, the
cross-section of which is of an ellipse.
FIG. 11-III pertaining to the angular arrangement of three positive
plasma jet torches 120.degree. apart shows the "on-center" position
of the incandescent core 40, the cross-section of which is almost
circular.
FIG. 11-IV pertaining to the angular arrangement of four positive
plasma jet torches 90.degree. apart shows the "on-center" position
of the incandescent core, the cross-section of which approaches a
circle.
The positioning of the incandescent core on the exact center of the
throttle aperture as shown in FIGS. 11-II, III and IV means the
aligning of the plasma jet flame in the central axis of the main
channel, thus decreasing the thermal loss which would be caused if
the plasma jet flame approaches the channel wall apart from the
center. The centering of the plasma jet flame by means of a
plurality of positive plasma jet torches is useful to improve the
efficiency of the apparatus.
For the sake of simplicity this invention has been heretoabove
described with reference to the non-transferred type straight
polarity P.J.G., but it should be noted that the reverse polarity
P.J.G. according to this invention is equally useful. It is
commonly admitted that the use of oxygen or air in the transferred
type P.J.G. will increase the cutting speed for steel or aluminium
sheets. However, in order to avoid the damage to the electrode of a
conventional P.J.G. (more specifically in order to assure the life
of the apparatus as long as the apparatus using argon), it is
necessary to use an inactive gas in the mode of non-transferred
operation and then introduce oxygen or air as a substitute for the
inactive gas after the transition of the arc to the workpiece. This
operation is too inconvenient, and it makes the apparatus actually
useless. This defect is overcome by, according to this invention,
generating first non-transferred plasma jet with the aid of an
auxiliary power supply and second, a transferred plasma jet between
the cathode rod and the workpiece with the aid of the main power
supply.
This invention has been heretoabove described as using plasma jet
of straight polarity, but it is apparent to the skilled in the art
that a P.J.G. according to this invention can equally use plasma
jet of reverse polarity. In other words, a P.J.G. according to this
invention will not be deteriorated, which type of plasma jet may be
used. The embodiments herein disclosed have the axis of the
positive plasma jet torch and the axis of the negative plasma jet
torch transverse therewith. However, in cutting a workpiece of a
dielectric material, such as concrete in the mode of
non-transferred operation or in cutting a workpiece of a conductive
material, such as aluminium, iron and other metals in the mode of
transferred operation, two plasma jet torches were angularly
arranged 60.degree. , thus first allowing the "hairpin" arc to
approach the outlet with a result of increasing the thermal energy
to the workpiece and second, making the outlet accessible to the
workpiece because the plasma jet units causes little or no
hindrance against the workpiece. As a matter of course, the angle
at which the two plasma jet units arc arranged can be arbitrarily
determined to meet the requirements.
The P.J.G. has been widely used in numerous industrial fields since
it appeared in the world, and this invention enlarges the domain of
appliance to the possible extremity from the points of economical
and technical views.
* * * * *