US2636975A

US2636975A - High-frequency heating apparatus

Info

Publication number: US2636975A
Authority: US
Publication date: 1953-04-28
Anticipated expiration: 1970-04-28

Description

April 28, 1953 R. M. BAKER ET AL HIGH-FREQUENCY HEATING APPARATUS 2 SHEETS-SHEET 1 Filed June 26, 1948 INVENTOR 5 EoerfMBa/(er and 0p0/7ne//,

ATTORNEY WITNESSES: 54%,?

April 1953 R. M. BAKER ET AL HIGH-FREQUENCY HEATING APPARATUS 2 SHEETS SHEET 2 Filed June 26, 1948 3/ mmw m M n .N E r 0 W WW 0 T aw M 5 MJ f x M g Patented Apr. 28, 1953 UNITED STATES PATENT OFFICE HIGH-FREQUENCY HEATING APPARATUS Robert M. Baker, Catonsville, and Robert J.

ODonnell, Baltimore, Md., assignors to Westinghouse Electric Corporation, East Pittsburgh, Pa., a corporation of Pennsylvania Application June 26, 1948, Serial No. 35,314

6 Claims. 1

This invention relates to high frequency electrical apparatus and particu arly to apparatus for transferring high frequency electrical energy from a source to a load.

Ultra high frequency energy can be caused to flow along a hollow duct called a wave guide. The energy flowing in such a wave guide is manifested by electric and magnetic fields having a distribution and orientation depending on the mode of transmisison. Such fields produce molecular friction in certain dielectric materials disposed in them, thereby heating the material. The energy in a wave guide may therefore be used for heating materials. In accordance with the teaching of the prior art of which we are aware, the material to be heated is in serted directly in the guide through a door in the end of the guide. provided in such a guide, for matching the im pedance presented by the load material to the impedance of the generator which supplies the energy flowing through the guide.

We have found that such prior art heaters are unsatisfactory for heating certain materials, particularly those dielectric materials which. have relatively low loss factors, to the high tem perature required in the industries in which the materials are used. The high frequency fields in a wave guide can also be impressed on a web of dielectric material drawn through the field to heat the web. We have found that such a web drawn through a wave guide must be moved relatively slowly to be properly heated.

1 His accordingly an object of our invention to provide improved high frequency heating apparatus for heating materials to high temperatures.

It is also an object of our invention to provide a-high frequency heating apparatus for quickly heating materials to high temperatures.

It is another object of our invention to provide a high frequency heating apparatus for quickly heating dielectric materials to high temperatures.

It is a further object of our invention to provide a high frequency heating apparatus for heating a web of material moved at high speed to high temperatures.

Our invention arises from the realization that the heat produced in dielectric material results from displacement current set up in the material by an electric field which varies with time. This displacement current increases as the electric field across the material is increased. In the practice-of our invention a field having a Suitable tuning stubs are 2 high amplitude is accordingly impressed across the material to be heated.

In accordance with the broad aspect of our invention the material to be heated is disposed in a cavity coupled to a wave guide. The cavity is so coupled that the electric field produced in it is higher in amplitude than the field in the wave guide. The material to be heated is disposed in the strong portion of this higher amplitude field.

We have found that couplers in the prior art of which we are aware are not satisfactory for coupling a wave guide to a resonant cavity, due to difiiculties encountered in tuning the coupler and arcing across the coupler parts, particularly whereas in the dielectric heating art, relatively large amounts of high frequency energy are involved.

It is therefore an ancillary object of our invention to provide an apparatus for efliciently couplin a wave guide to a resonant cavity.

It is also an ancillary object of our invention to provide a coupling arrangement between a wave guide and a resonant cavity wherein the cavity shall be driven at a voltage much higher than that in the wave guide.

Another ancillary object of our invention is to provide a coupler which can be mounted in its working position without the use of insulator .upports.

Another ancillary object of our invention is to provide a high frequency coupler that can be conveniently tuned to half wave resonance.

A further ancillary object of our invention is to provide an improved coupler which shall be capable of handling relatively large amounts of high frequency energy.

, A still further ancillary object of our invention is to provide an improved coupler construc-- tion wherein the effective inductance of the coupler loops shall be reduced to a value such that the coupler circuit can be conveniently tuned by an extended line.

In its specific aspects, our invention embraces two concepts First, the coupling of a. wave guide to a resonant cavity by means of a tunable coupler which is capable of transferring relatively large amounts of high frequency electrical energy of the order in excess of one kilowatt and which is tunable to half wave resonance so as to provide an efficient magnetic coupling between the wave guide and the resonant cavity, and obviate the use of insulator coupler mounting supports.

Second, the arrangement of a coupler befrom the following description of one embodi-' ment thereof when read in connection with the accompanying drawings, in which 1' Figure 1 is a. diagrammatic view in perspective showing a preferred embodiment of our invention.

Fig. 2 is a diagrammatic view in perspective showing in detail a portion of the apparatus shown in Fig. 1;

Fig. 3 is a graph showing the distribution of the maximum transverse electric field vector in a wave guide used in the practice of our invention; and

Fig. 4 is a sectional view taken on a horizontal plane through the apparatus of Fig. 2 showing magnetic field distribution.

The apparatus shown in Figs. 1 and 2 includes a rectangular wave guide, a resonant cavity, and a coupler, which are generally indicated by the reference numerals I, 3 and I? respectively. The

wave guide I is of conventional construction and is connected to a suitable oscillator (not shown) such as a magnetron and is so coupled to this oscillator that the mode of propagation in the wave guide is TEo,1. The wave guide I may be any convenient length and is closed at the end opposite the oscillator.

The resonant cavity 3 is a rectangular metal box preferably of the same width and height as the wave guide I, and is closed by a tuning piston 5 at its end nearest to the wave guide power source. The other end of the resonant cavity 3 is closed by a door I to permit insertion and removal of certain materials to be heated. Openings I I are provided in the top I3 and bottom I5 of the cavity 3 to allow passage of materials or articles 9 to be heated through the resonant cavity 3 when the apparatus is used in continuous treatment operation. In the specific embodiment shown in Fig. 1 these openings are in the form of elongated slots II and the material 9 being heated is shown passing through the slots II in the cavity 3 in web or ribbon form.

The coupler I'I comprises a pair of loop portions I9 and 2i and an extended line portion 23. The loop portions I 9 and 2! may be made by bending a, piece of a conductor in the form of two substantially horseshoe-shaped loops having a pair of spaced terminals as shown in Fig. 2. The extended line portion 23 includes a pair of parallel conducting rods 27 which are attached at one end to the loop terminals 25 and supported near the other end by a metal bar 29. A

short-circuiting bar Si is slidably mounted upon,

the parallel conducting rods 2?. A threaded shaft 33 having a tuning knob 35 on one end is rotatably mounted between the parallel conducting rods 27 so that its threaded portion engages a threaded hole 377 in the center of the short-circuiting bar 3 I. The position of the short circuiting bar 3! may be varied by turning the tuning knob 35. A cylindrical metal housing 39 is provided to shield and support the extended line portion 23 of the coupler H.

The resonant cavity 3 and the wave guide i are juxtaposed as shown in Fig. 2. Corresponding V-shaped slots II are cut in the adjacent sides of the wave guide I and cavity 3 and corresponding semicircular portions are cut away from their tops. The coupler I l is placed symmetrically between the wave guide I and the resonant cavity 3 so that its loops I9 and 2| and extended line 23 are in a plane which passes through the vertex of the V-shaped slots 4! and is transverse to the axis of the wave guide I. The extended line portion 23 of the coupler I'I extends up through the hole formed by the semicircular portions cut away from the tops of the wave guide I and cavity 3, and is covered by the cylindrical metal shield 39. The loop end of the coupler I? is secured to cavity 3 so that the field in the cavity 3 is high Fig. 4 shows at a particular time the magnetic field intensity distributions in the wave guide I and the resonant cavity 3 in the vicinity of the coupler IT. The magnetic field it in the wave guide I is at a maximum intensity in the regionnear the side 8 and a quarter wave length from the end 2 of the wave guide I. In order to make it possible to set up a maximum current in the coupler circuit, the loop of the coupler which extends into the-wave guide must be located in the maximum magnetic field intensity region of the wave guide; therefore the vertex of the V- shaped slot 4! in the wave guide I is located at a point approximately a quarter wave length from the end of the guide I and the coupler I! is mounted in the slot 4| as has been previously described. I

The magnetic field in the wave guide induces a voltage in the wave guide coupling p and causes alternating current to fiow through the loop. This same alternating current flows around through the cavity loop and sets up a magnetic field at the cavity loop which is equal in intensity to that magnetic field at the loop in the wave guide. The magnetic field 42 in the resonant cavity 3 is at maximum intensity in the regions of the midpoints of the sides and ends of the cavity 3. The magnetic field intensity in the cavity 3 is at a minimum in the regions of the corners of the cavity. 'We mount the resonant cavity 3 in a position longitudinally of the wave guide I such that the door I of the cavity 3'is .just under a quarter wave length from the end This locates the coupler loop in the cavity 3 in a region of low magnetic field in-' of the guide I.

tensity in the cavity 3. The magnetic field intensity in the plane of the wave guide coupling loop I9 is of the same value as'the magnetic field intensity in the plane of the cavity coupling loop 2I. Proceeding from the cavity coupling loop to a distance one quarter wave from the end of the cavity it is found that the magnetic field inten- An electric field proportional to the magneticfield occurs during that part of the cycle when magnetic energy has been transformed to electrical energy. Accordingly, an electric field is set up in the region of the center of the cavity '3 which is much greater than the electric field in;

the wave guide l. The heating effect in a material disposed in an electric field depends upon the intensity of that field. Thus by using the apparatus in accordance with the teaching of our invention it is possible to heat materials more quickly and to higher temperatures than has been possible prior to our invention.

Referring now to Fig. 2, we will point out the specific features of the improved coupler which is used in the practice of our invention. In order to get an cflicient transfer of energy from a wave guide to a cavity, there must be proper coupling between the wave guide and the cavity. To take care of variations in the frequency of the energy source it is desirable that the coupler be tunable. But in the field of dielectric heating, where quantitles of high frequency electrical energy of the order in excess of one kilowatt are involved, peculiar problems arise in the construction of a satisfactory tunable coupler. We have found that a coupler comprising a pair of loops and an extended line is the most desirable. But in order to get a large amount of current induced in the coupler circuit it is necessary to make the loop in the wave guide large so that it links a large area of the magnetic field of the wave guide. However in making the loop large, its effective inductance would ordinarily be increased to a value such that it could not be tuned by a reasonable length of extended line. However, we overcome this difficulty by specially constructing the loops in a manner which will be hereinafter described. A maximum transfer of energy between the wave guide I and the cavity 3 is obtained when the circuit consisting of the coupler loops l9 and 2!, the extended line 23, and the short-circuiting bar 3| is tuned to half-wave resonance. In other Words, when there are voltage nodes at the point 43 where the loops I9 and 2 I are attached to the wave guide I and cavity 3, and at another point an effective half wave length in either direction from the first point. Now if the effective inductance of the loop 59 in the wave guide i is so large that it takes a length of extended line 23 the same length or longer than the physical length of the loop E9 to tune it, a voltage antinode in the coupler circuit will appear near the loop terminal 25 or out on the extended line 23 and arcing will occur at the loop terminals 25 or on the extended line 23. sary to construct a coupler loop l9 which has a large area and at the same time an effective inductance low enough to be tunable by a section of extended line 23 whose length is shorter than that of the loop IS, in order that the voltage peak of the coupler circuit will not occur near the loop terminal 25 or out on the extended line 23. To decrease the efiective inductance of the coupler loop [9 to a value which is tunable by a section of extended line 23 shorter than the loop 19, and at the same time keep the loop area large, We make the width of the loop large in comparison to its thickness. A loop width of the order of 16 times the thickness is satisfactory.

When the coupler loops l9 and 2! are made the same size and the coupler circuit is tuned to half wave resonance, voltage nodes will occur at the point where the loops l9 and 2! are attached to the wave guide I and cavity 3 and near the center of the short-circuiting bar 3!. This means that the portion of the extended line 23 which is above the short-circuiting b-ar may be directly attached to the cylindrical housing 39, whereby the coupler is supported entirely without the use of insulators which may be destroyed by being Therefore it is necesoil subjected toithe dielectric heating effectsof theintense electric fields encountered during the use of the coupler. Thus we have constructed a coupler capable of transferring large amounts of high frequency energy without arcing and tunable to half-wave resonance so as to get a maximum energy transfer between a wave guide and a resonant cavity, and obviate the use of lossy dielectricinsulators in mounting the coupler.

In the operation of the apparatus, the material S to be lo ated is placed in the center of the resonant cavity 3, and electrical energy at a suitable high frequency, for example 430 1nc., is fed into the wave guide 5. Then the cavity 3 is tuned to resonance by means of its tuning piston 5, and

he coupler circuit is tuned to half-wave resonance means of the coupler tuning knob 35.

The operating frequency or the arrangement of the material a to be heated in the cavity 3 may be varied to suit the purpose at hand.

Although we to make the coupler loops is and 2! the same their relative sizes may be varied somewhat without departing from the scope of our invention. The relative position of o the cavity 3 with respect to its coupler loop 2! may be varied so as to get the desired increase in electric field intensity over that in the wave guide l.

Although we have described the operation of our invention as it is applied in the dielectric heating art, We do not wish to be limited to that application.

Our invention be applied wherever it is desired to transfer appreciable amounts of high frequency electrical energy from a wave guide to a resonant cavity.

By the expression cavity resonator we intend to. mean a cavity, usually metallic and having conductive walls, in which ultra. high frequency electromagnetic oscillations can exist when the cavity is properly excited; its resonant frequency is determined by its physical dimensions. By the expression coupler or coupling element we intend to mean apparatus or means by which en ergy is transferred from one circuit to another; the common impedance necessary for effecting such coupling' By the expression Wave guide we intend to mean a hollow pipe-like conductor of electromagnetic energy which is used as a radio frequency transmission line; its dimensions are determined by the Wave length of the electromagnetic energy to be transmitted.

Our invention, therefore, is not to be restricted except in so far as is necessitated by the prior art and by the spirit of the appended claims.

We claim as our invention:

1. For heatin a dielectric material, a wave guide, a resonant cavity adapted to receive a dielectric material to be heated and a coupler tunable to half wave resonance comprising an extended line portion and two loop portions, said coupler being placed. longitudinally of the Wave guide so that one of said loop portions links the magnetic field. of the wave guide, said resonant cavity being placed adjacent the wave guide in a position longitudinally of the wave guide such that the other of said loop portions links less than the maximum magnetic field of the said resonant cavity.

2. For heating dielectric material, a rectangular wave guide havin common openings in its side and top, a resonant cavity having like openings in its side and top and placed adjacent the wave guide so that said openings are aligned, a coupler comprising two loop portions and an extended line :portion and. placed, between the. wave guide and the cavity so thatsaid loop portions are attached to the bottom of the said side. openings and the extended line portion extends up through the said top openings, and a metal housing placed over said top openings so as to shield and support said extended line.

3. For heating dielectric material, a rectangular wave guide having a V-shaped slot in its side and a, semicircular slot whose diameter is in the plane of the V-shaped slot in its top, a resonant cavity having like slots in its side and top and placed adjacent the Wave guide so that said V-shaped slots are aligned, a coupler comprising a pair of loops and an extended line which is bridged by a slidable short-circuiting bar, said coupler being attached at its loop end to the vertex of said V-shaped slots so that one loop extends into the wave guide and the other loop extends into the resonant cavity and the extended line protrudes up through the opening formed by said semicircular slots, a shielding housing placed oversaid opening toenclose and support said extended line, and a threaded shaft extending through the top of said housing and engaging the s lidable short-circuiting bar of said extended line, said threaded shaft being rotatable by means of an external knob to tune said coupler.

4. For coupling a hollow wave guide to a structure forming a resonant cavity, a coupler circuit tunable to half Wave resonance comprising that portion of an adjustable extended line which consists of two conducting rods bridged by a slider bar, and a pair of loops, adapted to be inserted one into the wave guide and the other into the cavity, joined at one of their ends and having their other ends spaced apart, said conducting rods being connected to the spaced ends of the loops, the width of said loops being large as compared to their thickness, whereby their effective inductance is reduced toa value which can be tuned by a section of extended line whose length is. less than the physical length of one of said loops.

5. A coupling device for use between a resonant cavity and a load and tunable to half wave resonance and'capable of handling amounts of high frequency electrical energy of the order in excess 8 of one kilowatt, comprising a pair, of oppositely disposed 10w inductance loops having one of their ends'joined and the other of their ends spaced, one of. said loops being positioned to be responsive to electrical energy in said cavity and the other of said loops being positioned to feed electrical energy to said load, an extended line section attached tosaid spaced ends, a short-circuiting slider mounted upon said extended line for tuning the circuit composed of the loops, the extended line and theslider to half wave resonance. 7

6. For use in heating materials, a wave guide, a resonant cavity adapted to receive material'to be heated, and a coupler tunable'to half wave resonance comprising a pair of oppositely dis: posed loops having one of their ends joined and the other of their ends spaced, and parallel con'-. ducting rods bridged by a short-circuiting slider bar attached to said spaced ends, said coupler beingplaced so that one of its loops extends into the wave guide and the other of its loops extends into the cavity, said coupler being supported be?- tween the wave guide and the cavity from its por-;; tion where the loop ends are joined and its portion which is above-the short-circuiting-slider; each of said supporting portions of the coupler, being attached to its supporting member.

ROBERT M. BAKER. i ROBERT J. ODONNELL.

References Cited in the file of this patent UNITED STATES PATENTS Number Name Date 2,311,658 Hansen Feb. 23, 19;;3 2,357,313 Carter Sept-5,1944 2,373,233 Dow Apr. 10, 1945 2,404,279 Dow July 16, 194 2,404,568 Dow July 23,1946 2,419,557 Friis Apr. 29,1947