U.S. patent number 3,571,551 [Application Number 04/810,650] was granted by the patent office on 1971-03-23 for high frequency heating apparatus.
This patent grant is currently assigned to Furukawa Denki Kogyo Kabushiki Kaisha. Invention is credited to Takao Namiki, Naoyuki Ogasawara, Katsutoshi Sone.
United States Patent |
3,571,551 |
Ogasawara , et al. |
March 23, 1971 |
HIGH FREQUENCY HEATING APPARATUS
Abstract
An apparatus for noncontact heating of a continuously running
metal wire with microwave power, which consists of a high loss
transmission line such as coaxial line, strip line, or slab line,
or its resonator, with the wire serving as an inner conductor. A
bare or insulated wire to be heated and a conductor surrounding the
wire together constitute a high loss transmission line such as a
coaxial line, a strip line or a slab line. Such a transmission line
is shorted at both ends thereof to form a resonator. The
transmission line or resonator is fed with a high frequency power
from a high frequency power source such as magnetron through a
waveguide system connected to the transmission line or resonator in
noncontacting relationship to the wire. Heat that develops either
by the resistance loss in the wire or by the dielectric loss in the
insulation layer is used for annealing of the wire or curing of the
insulation layer.
Inventors: |
Ogasawara; Naoyuki (Tokyo,
JA), Namiki; Takao (Chiba-ken, JA), Sone;
Katsutoshi (Chiba-ken, JA) |
Assignee: |
Furukawa Denki Kogyo Kabushiki
Kaisha (Tokyo, JA)
|
Family
ID: |
27276424 |
Appl.
No.: |
04/810,650 |
Filed: |
March 26, 1969 |
Foreign Application Priority Data
|
|
|
|
|
Apr 3, 1968 [JA] |
|
|
43/21465 |
|
Current U.S.
Class: |
219/696;
219/750 |
Current CPC
Class: |
H05B
6/782 (20130101) |
Current International
Class: |
H05B
6/78 (20060101); H05b 009/06 (); H05b 005/00 () |
Field of
Search: |
;219/10.61 |
References Cited
[Referenced By]
U.S. Patent Documents
Foreign Patent Documents
|
|
|
|
|
|
|
1,452,124 |
|
Aug 1966 |
|
FR |
|
703,049 |
|
Feb 1965 |
|
CA |
|
Primary Examiner: Truhe; J. V.
Assistant Examiner: Bender; L. H.
Claims
We claim:
1. A high frequency heating apparatus comprising:
1. a high frequency coaxial transmission line wherein a running
wire to be heated, serves as an inner conductor, and an outer
conductor surrounding coaxially said inner conductor;
2. shorting elements which short the inner and outer conductors in
noncontacting relationship to each other near both ends of the
outer conductor of said coaxial;
3. a high frequency power source for feeding high frequency power
to said coaxial line; and
4. a waveguide system for coupling said coaxial line and said power
source with each other in noncontacting relationship to said inner
conductor, said coaxial line and said shorting elements together
constituting a high frequency coaxial resonator, said coaxial
resonator being immersed in a dielectric liquid.
2. A high frequency heating apparatus as claimed in claim 1,
wherein a bare copper wire, an enameled wire, or a synthetic resin
coated wire is used as an inner conductor.
3. A noncontact coaxial resonator type high frequency heating
apparatus for heating a running metal wire comprising:
1. a high frequency coaxial transmission line immersed in a
dielectric liquid wherein said running wire to be heated serves as
an inner conductor and a tubular outer conductor;
2. detuned cavity resonator elements for short circuiting said wire
and said outer conductor in a noncontacting relationship to each
other near the ends of said outer conductor;
3. a T-shaped junction for joining said coaxial transmission line
to a waveguide to excite said wire with a high frequency power in
noncontacting relationship to said wire; and
4. means for feeding a high frequency power to a noncontact type
coaxial resonator composed of said coaxial line, detuned cavity
resonator elements and T-shaped junction.
4. A high frequency heating apparatus as claimed in claim 3,
wherein a bare copper wire, an enameled wire, or a synthetic
resin-coated wire is used as an inner conductor.
Description
BACKGROUND OF THE INVENTION
The present invention relates to a high frequency heating
apparatus, and more particularly to an apparatus for noncontact
heating running object of continuous length hereinafter called
"heating object" such as a metal wire, an insulated electric wire,
tube or the like, for continuous annealing of metal wires or heat
treatment of insulating layers.
There have been several conventional methods of continuously
heating a running metal wire such as a bare copper wire, a
synthetic resin insulated electric wire, an enameled wire or the
like; that is, radiation heating using electric heaters or infrared
ray heater, conduction heating using heated liquids, heating by
direct passage of electric current, and induction heating. The
radiation heating and the conduction heating are defective in that
their thermal efficiency is very low because other objects than the
heating object must also be heated and that their thermal response
is slow because the heating furnace used has a large thermal
capacity. A large size heating apparatus will therefore be required
if such heating must be done at a high speed. The slow thermal
response means the impossibility of rapid temperature control and
therefore of uniform heating.
On the other hand, heating by direct passage of electric current
requires electrodes for power supply and the induction heating
requires contact members for constituting a secondary circuit.
Therefore, an object heated by these methods will be injured by
friction or spark discharge that develops between it and the
electrodes or contact members.
In the wood, synthetic fiber and food industries there has been
employed dielectric heating. For example, the so-called microwave
oven having a cavity resonator for generating microwaves, has been
put to practical use. Such technique, however, is based on the
dielectric loss and therefore unsuitable for heating a rapidly
running wire. It is also difficult to use such technique for
heating object with metallic conductors embedded therein such as
insulated electric wires.
The principal object of the present invention is to provide a novel
high frequency heating apparatus free from the above disadvantages
of the conventional heating apparatus.
Another object of the invention is to provide a high frequency
heating apparatus capable of continuously heating either or both of
a metallic conductor and a dielectric material provided
thereon.
A further object of the invention is to provide a high frequency
heating apparatus adapted for heating a metallic conductor covered
with a dielectric material such as an insulated electric wire,
which allows not only dielectric heating of the dielectric material
but heating of the conductor by ohmic loss at the same time,
utilizing the microwave technique.
A further object of the invention is to provide a high frequency
heating apparatus in which high frequency power is concentrated on
and absorbed by the heating object in noncontact relationship
thereto, without electrodes, contact members or the like for
feeding power.
A further object of the invention is to provide a high frequency
heating apparatus having a high power efficiency, with a high
concentration of high frequency power on the heating object and
little leakage of the power.
A further object of the invention is to provide a high frequency
heating apparatus, small in size and capable of rapid temperature
control with quick thermal response.
A further object of the invention is to provide a high frequency
heating apparatus in which a cavity resonator is made in the form
of coaxial line, strip line, or slab line with a heating object
serving as the inner conductor, the apparatus having a wideband
coupling with the cavity and being free from spark in the
cavity.
A further object of the invention is to provide a high frequency
heating apparatus that can be applied to foaming process in the
manufacture of an electric wire insulated with foamed synthetic
resin.
A still further object of the invention is to provide a high
frequency heating apparatus suitable for continuous annealing of a
metallic wire.
SUMMARY OF THE INVENTION
In accordance with the invention, there is provided a high
frequency heating apparatus comprising (1) a high loss, high
frequency transmission line composed of a running object, which
serves as an inner conductor, and an outer conductor surrounding
the running object, (2) a high frequency power source for feeding
high frequency power to the transmission line; and (3) a waveguide
system for coupling the transmission line and the power source with
each other in noncontacting relationship to said inner
conductor.
In accordance with another aspect of the invention, near the ends
of the outer conductor of the above transmission line there are
provided shorting elements in noncontacting relationship to the
object to be heated, both the shorting elements and the
transmission line together constituting a high frequency
resonator.
Other features and advantages of the invention will be apparent
from the following description taken in connection with the
accompanying drawings.
BRIEF DESCRIPTION OF THE DRAWINGS
In the drawings:
FIG. 1 illustrates a high frequency heating apparatus embodying the
invention;
FIG. 2 is a view, partly in section, of a feeder for feeding high
frequency power to a coaxial line in noncontacting relationship to
a heating object as an inner conductor;
FIG. 3 is a longitudinal sectional view of another embodiment of
the invention;
FIG. 4 is a longitudinal sectional view of another high frequency
heating apparatus;
FIG. 5 is a perspective view of the apparatus in FIG. 4;
FIG. 6 illustrates a further high frequency heating apparatus;
FIG. 7 is a view, partly in section, of a shorting element in
noncontacting relationship to a heating object as an inner
conductor;
FIG. 8a is a diagram showing the frequency of the shorting
element;
FIG. 8b is a schematic longitudinal view of a measuring apparatus
used for obtaining the characteristics shown in FIG. 8a;
FIG. 9 illustrates a lossy circuit structure;
FIG. 10 is a diagram showing input voltage standing wave ratio (as
function of frequency) of a cavity resonator with or without the
lossy circuit in FIG. 9;
FIG. 11 illustrates an application of the high frequency heating
apparatus of the invention to the manufacture of an electric wire
insulated with a foamed synthetic resin.
In the drawings the corresponding parts are designated with the
same reference numerals.
Referring now to FIG. 1, the reference number 1 designates a wire
to be heated, such as a bare copper wire, a synthetic resin coated
electric wire, an enameled wire or the like, which, driven by a
suitable device not shown, runs in the direction shown with an
arrow. A pipe-shaped outer conductor number 2 is arranged so as to
surround coaxially the wire 1, and both constitute a high loss
coaxial line 2'. Coupled with the outer conductor 2 is a power
feeder 3 in noncontacting relationship to the wire 1 as an inner
conductor. The feeder 3 is a coaxial line waveguide transducer with
the wire 1 as the center conductor of coaxial line. Its coupling
degree can be adjusted by means of a movable shorting plate 33 with
an adjusting screw 34 in a waveguide section 31 and matching stubs
36 screwed into another waveguide section 32. The waveguide section
32 is connected in series to a directional coupler 4 and an
isolator 5.
The isolator 5 in turn is connected to a magnetron mount consisting
of a magnetron tube 7, a waveguide 6, and a short plunger 61. The
feeder 3, directional coupler 4, isolator 5, and waveguide 6
together constitute a waveguide system for carrying high frequency
power from the power source 7 to the coaxial line 2'. The
directional coupler 4 is equipped with a detector and a
galvanometer (not shown), and serves to monitor the incident power
to the coaxial line 2' and the reflected power from the feeder 3.
The isolator 5 absorbs reflected power from the coaxial line to
keep power source stable.
Waveguide 6 is provided with a movable shorting plate (not shown)
actuated by an adjusting screw for matching the waveguide system
with the power source 7. As the high frequency power source 7 there
may be employed a microwave oscillator of high power such as
magnetron which oscillates microwave power, in frequency of 2,450
MHz.
In the above arrangement, the high frequency power which has been
generated in the power source 7 is excited in the waveguide 6 and
supplied to the coaxial line 2' through the waveguide system.
Almost all of the power from the power source 7 may be fed to the
coaxial line 2' by proper adjustment of the shorting plate 33 and
the matching elements 36. Since the coaxial line 2' is constructed
as high loss transmission line as described above, the high
frequency power fed thereto is well concentrated on the wire 1,
which is heated by ohmic loss in the case of bare wire and, in
addition, by dielectric loss in the case of insulated wire.
Furthermore if the inner wall of the outer conductor 2 is lined
with a appropriate lossy material such as ferrite or polyiron, the
wire will receive the radiant heat from the lining, in addition to
the heat generated by itself.
The microwave power of the coaxial TEM mode is most suitable for
concentrating high frequency power on the inner conductor and
dissipating it mostly therein. The TEM mode is also stable against
mechanical vibrations of the running wire 1.
The heating apparatus shown in FIG. 3 is provided with an electric
heater 20 wound on the outer conductor 2. The heater 20 is embedded
in a heat insulating material 21 such as asbestos and covered with
a protecting metal tube 22. In such a structure, the wire 1 may be
heated up not only by ohmic loss and dielectric loss but by
radiation heat supplied from the surrounding electric heater 20.
Such a structure of heating apparatus, especially when utilized for
the foaming process in the manufacture of foamed synthetic resin
insulated electric wires, as described later, permits high speed
production of foamed plastic insulated wires of good quality.
In FIGS. 4 and 5, the coaxial line system 2' is immersed in a
dielectric liquid 26 in which case high frequency power heats not
only the wire by its ohmic loss and dielectric loss but also the
liquid 26 by its dielectric loss. For this purpose, the outer
conductor 2 is internally lined with a heatproof dielectric tube 23
such as a fused quartz tube, which prevents the liquid 26 in the
coaxial line 2' from flowing out into the waveguide system 24. The
dielectric liquid 26 must have such permittivity and loss factor as
will permit it to be heated by dielectric loss to a predetermined
temperature. As such liquid, water or glycerine may be preferably
used. The wire 1 runs through the apertures 43 and 42, the tube 25
and apertures 42' and 43', and is heated in the coaxial line 2' by
its ohmic loss and dielectric loss and additionally by the heated
liquid 26. The liquid 26 is circulated by a pump 30 through a feed
pipe 41, receptacle chambers 44 and 44' having opening 42 and 42'
and return pipes 28 and 29. This heating apparatus may also be
utilized for foaming process in the manufacture of foamed synthetic
resin insulated electric wires, and permits high speed production
of foamed plastic insulated wire of good quality.
In order to ensure higher thermal efficiency of a high frequency
heating apparatus and less leakage of high frequency power
therefrom, a resonator is formed in the apparatus by shorting the
inner and outer conductors at both ends of the above high loss
transmission line. This helps reduce the overall size of the
heating apparatus. Since the wire 1 must be kept noncontact with
any part in an exciting section and other sections in the whole
apparatus, noncontact short elements and a noncontact exciting
section must be provided to make such a coaxial resonator. The
noncontact short elements may be constructed by utilizing the
effect of detuned short of a cavity resonator, which is a tunable
waveguide cavity provided with a couple of tubes to permit the wire
to run through as shown in FIG. 7. As regards the noncontacting
exciting, the coaxial line-waveguide transducer may be used as
shown in FIG. 2, where the movable shorting plunger serves not only
to adjust the coupling with a cavity but to adjust the resonant
frequency without changing the length of the coaxial cavity.
Such a heating apparatus of resonator type is illustrated in FIG.
6. Near the ends of the coaxial line 2, there are mounted
noncontact short elements 8 and 8'. The short element 8 and 8', as
shown in detail in FIG. 7, are each composed of (1) two waveguide
members 81 and 82 connected transversely to the outer conductor 2
of the coaxial line, (2) a metallic plate 83 for shorting the free
end of the waveguide member 82, and (3) a movable shorting plate 84
with an adjustment screw 85 mounted to the free end of the
waveguide 81. The noncontact short element 8 and 8' serve as a
cavity filter. FIG. 8a shows an example of the short characteristic
of noncontact short elements 8 and 8', ascertained by the use of a
measuring circuit shown in FIG. 8b. In FIG. 8a the abscissa
represents the frequency applied and the ordinate represents the
ratio of output to input level. As the short element shown in FIG.
8b, a rectangular waveguide having inner dimensions 34.0 mm.
.times. 72.1 mm. was used while the input and output lines 45 and
45' were each composed of a coaxial line having an inner conductor
of 16.9 mm. and an outer conductor of 38.8 mm. in diameter. The
reference numeral 47 designates a high frequency oscillator and 47
an output level detector line 45'. The input and output line 45
were matched with the oscillator 46 and the detector 47
respectively. As is evident from FIG. 8a, the short element in FIG.
8b has the shorting effect at the frequencies of 2,456 and 2,493
MHz. The shorting frequency may be changed by means of the movable
shorting plate 84 in a desired manner. The shorting frequency, of
course, must agree with the frequency of the high frequency power
source. The reference numerals 9 and 9' in FIG. 6 designate each a
monitor for power leakage from the coaxial resonator, in which a
loop of suitable form or a probe is inserted.
It is better to make Q.sub.o of the resonator somewhat smaller in
view of the spark discharge and the wideband coupling with the
resonator. The reduction of Q.sub.o may be easily achieved by
loading lossy materials such as polyiron or ferrite in the coaxial
cavity or by coupling lossy circuits with the coaxial cavity. The
lossy circuit used in one embodiment of the invention consists of a
noncontact coupler 103, an isolator 105, and a waveguide transducer
106 as shown in FIG. 9. The improvement of Q.sub.o is evident from
the graph in FIG. 10, in which the abscissa represents the
frequency applied while the ordinate represents the input voltage
standing wave ratio to the coaxial cavity.
In the foregoing, the description has been referred to a high loss
transmission line and a resonator of a coaxial line. Such a high
loss transmission line or a resonator may naturally be made of a
strip line or a slab line.
The application of the high frequency heating apparatus described
above to the foaming process in the manufacture of an electric wire
insulated with a foamed synthetic resin will be described with
reference to FIG. 11. A conductor wire 11 fed from a supplier 10 is
led into a coating tank 14 through a payoff capstan 12 and
preheating furnace 13, where it is coated at a high temperature
with a solution of crystalline synthetic resin melted in an organic
solvent. The conductor wire with the solution is then stored
temporarily in a wire stored temporarily in a wire storing machine
15, in which the crystalline resin in the coating while being
cooled and dried segregates from the solvent so that the coated
layer which has been transparent becomes cloudy. Such a step, which
is indispensable for foaming, will be referred to as "clouding"
hereinafter. The wire coated with such a cloudy resin layer will be
called as a clouded wire. The clouded wire is then led to a high
temperature foaming furnace in which the coated layer thereof is
foamed. When the high frequency apparatus of the present invention
is used as the foaming furnace 17, the coated layer is not only
heated by dielectric loss that develops in the layer itself but
heated from inside by the resistance loss of the conductor wire.
Additional heat is given from outside to the coated layer when the
heating apparatus as shown in FIG. 3 or 4 is used. The resin-coated
wire is finally wound up by a winding machine.
Several examples of the manufacture of a synthetic resin insulated
wire by the use of the heating apparatus of the invention will be
described in the following:
Now, when the high frequency heating apparatus shown in FIGS. 1, 3,
and 6 are given such construction as described in examples 1, 2,
and 3, the foamed synthetic resin insulated electric wires produced
by them have the characteristics as shown in the columns of
examples 1, 2, and 3 of table 1.
EXAMPLE 1
A heating furnace using a high loss coaxial line as shown in FIG. 1
was used. The outer conductor of the coaxial line was 53.5 mm. in
inner diameter and 6.6 mm. in length. A rectangular waveguide
having the inner dimensions 34.0 mm. .times. 72.1 mm. was employed
as the waveguide system for feeding high frequency power to the
coaxial line. The high frequency power source was a magnetron
having a power of 1.2 kw. at 2,450 MHz. The conductor wire was a
soft copper wire of 0.32 mm. in diameter. A coating solution was
made of one part by weight of high density polyethylene (density:
0.949, melt index: 0.32) mixed with two parts by weight of xylene
as a solvent. The solution at 130.degree. C. was coated on the
copper wire.
EXAMPLE 2
A heating furnace using a high loss coaxial line and a connectional
heater as shown in FIG. 3 was used. The outer conductor of the
coaxial line was 53.5 mm. in inner diameter and 3.3 m. in length.
The heater having a power of 10 kw. was wound on the outer
conductor. The heating temperature of the outer conductor was set
at 500.degree. C. The other conditions were the same as in example
1.
EXAMPLE 3
A heating furnace using a coaxial resonator as shown in FIG. 6 was
used. The outer conductor thereof was 53.5 mm. in inner diameter
and 2 m. in length. The short element was a rectangular waveguide
having inner dimensions 34.0 mm. .times. 72.1 mm. Other conditions
were the same as in example 1. ##SPC1##
As is evident from the above table, the foamed synthetic resin
insulated wire manufactured, using the heating apparatus of the
invention, has excellent features as enumerated below:
1. The insulation layer is uniformly foamed and well cured so that
the amount of residual solvent may be reduced.
2. Because the optimum foaming condition can easily be obtained,
the foaming degree is remarkably improved.
3. The insulation layer, which is well cured, has excellent
mechanical properties, that is, a good elongation and a high
mechanical strength.
4. Since a well-cured thin annular layer forms in contact with the
conductor, foamed cells never burst toward the conductor.
5. The insulation layer is well foamed near the conductor so that
the electric property thereof is improved. (In case of equal
foaming degree, the equivalent permittivity of the insulation layer
well foamed near the conductor is smaller than otherwise.)
6. The high speed and high efficiency production of the insulated
electric wire will be possible.
Although heating of the insulation of an insulated electric wire
has been described, the heating apparatus of the invention may be
applied to heating of a metal wire without insulation, for example,
to continuous annealing of a bare copper wire. Examples of
continuous annealing of a bare copper wire will be described in the
following:
EXAMPLE 4
An annealing furnace using a high loss coaxial line as shown in
FIG. 1 was employed. The outer conductor of the coaxial line was
53.5 mm. in inner diameter and 3.6 m. in length. The waveguide
system for feeding high frequency power to the coaxial line was a
rectangular waveguide having inner dimension 34.0 mm. .times. 72.1
mm. As the high frequency power source is used a magnetron having a
power of 1.2 kw. at 2,450 MHz. A hard copper wire was 0.4 mm. in
diameter.
EXAMPLE 5
An annealing furnace using a coaxial resonator as shown in FIG. 6
was used. The outer conductor thereof was 53.5 mm. in diameter and
2 m. in length. The short element was a rectangular waveguide
having inner dimensions 34.0 mm. .times. 72.1 mm. Other conditions
were the same as in example 4.
The results obtained are shown in table 2. ##SPC2##
The present invention may naturally be applied with advantage to
the using process of enameled wires or the vulcanizing process of
rubber- or plastic-insulated wires.
Further changes also may be made without departing the scope and
spirit of the invention as set forth in the appended claims.
* * * * *