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JP5894864B2 - High frequency heating device - Google Patents
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JP5894864B2 - High frequency heating device - Google Patents

High frequency heating device Download PDF

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JP5894864B2
JP5894864B2 JP2012120372A JP2012120372A JP5894864B2 JP 5894864 B2 JP5894864 B2 JP 5894864B2 JP 2012120372 A JP2012120372 A JP 2012120372A JP 2012120372 A JP2012120372 A JP 2012120372A JP 5894864 B2 JP5894864 B2 JP 5894864B2
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long side
waveguide
rotating antenna
inner conductor
high frequency
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JP2013246999A (en
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窪田 哲男
哲男 窪田
佐知 田中
佐知 田中
小林 良一
良一 小林
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Hitachi Global Life Solutions Inc
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Hitachi Appliances Inc
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Description

本発明は、回転アンテナを用いてマイクロ波エネルギーを加熱室内に放射し、食品などを加熱する高周波加熱装置に関するものである。   The present invention relates to a high-frequency heating apparatus that uses a rotating antenna to radiate microwave energy into a heating chamber to heat food and the like.

特許文献1に記載の高周波加熱装置は、加熱室の底面に固着された誘電体からなる載置棚を備え、加熱室底面中央部に設けた導波管の励振口部分にホーン形状の回転アンテナを備え、導波管により導かれるマイクロ波エネルギーをホーン形状の回転アンテナで受けホーン先端よりマイクロ波を加熱室内に放射し、載置棚に載置された食品などを高周波加熱するものである。   A high-frequency heating device described in Patent Document 1 includes a mounting shelf made of a dielectric material fixed to the bottom surface of a heating chamber, and a horn-shaped rotating antenna at an excitation port portion of a waveguide provided at the center of the bottom surface of the heating chamber. The microwave energy guided by the waveguide is received by a horn-shaped rotary antenna, the microwave is radiated from the tip of the horn into the heating chamber, and the food placed on the mounting shelf is heated at high frequency.

また、特許文献2では、ホーン形状の受信アンテナを備えホーン部の長辺面に幅が一定でホーン入り口での高さを低く、ホーンと連結された導波管部に設けた平面回路検出器部で高くした楔形のリッジを設け、ホーン形状の受信アンテナで自由空間を伝送されているマイクロ波信号を受信し、受信したマイクロ波の電界強度をリッジを介することにより強め、平面回路検出器部入り口に導き検出しようとするものである。なお、リッジとは、マイクロ波伝送路である導波管の長辺面中央の内面側に管軸に沿って設けた直方体状の突起をさす。   Further, in Patent Document 2, a planar circuit detector provided in a waveguide portion connected to a horn, having a horn-shaped receiving antenna, having a constant width on the long side surface of the horn portion and a low height at the horn entrance. A wedge-shaped ridge that is raised at the center, receives a microwave signal transmitted through free space by a horn-shaped receiving antenna, and enhances the electric field strength of the received microwave by passing through the ridge. It is intended to be detected at the entrance. The ridge refers to a rectangular parallelepiped protrusion provided along the tube axis on the inner surface side of the center of the long side surface of the waveguide that is a microwave transmission path.

特開2010−199009号公報JP 2010-199209 A 特開平1−132108号公報JP-A-1-132108

特許文献1では、高周波供給室底面中央部に設けられた結合孔を貫通して、前記高周波供給室内へ略垂直に臨んで設けられ回転アンテナと結合された内導体の一端を導波管内に突出させ、これによりマグネトロンで発生し導波管内を伝送されてきたマイクロ波をホーン形の回転アンテナに結合してホーン先端から加熱室内に放射するようになっている。   In Patent Document 1, one end of an inner conductor that passes through a coupling hole provided in the center of the bottom surface of the high-frequency supply chamber and faces the vertical direction into the high-frequency supply chamber and is coupled to the rotating antenna protrudes into the waveguide. Thus, the microwave generated by the magnetron and transmitted through the waveguide is coupled to the horn-shaped rotating antenna and radiated from the tip of the horn into the heating chamber.

この場合、導波管を伝送されてきたマイクロ波を同じような導波管形状を持つ回転アンテナに結合させて伝送させれば、反射が少なく結合度も大きくとれ効率よく伝送できるが、上記の従来技術のように形状も特性インピーダンスも異なり、高次モードの発生するホーン形状の回転アンテナへ結合する場合は両者間で反射が大きくなり結合度も低くなるので、マグネトロンで発生し導波管内を伝送されてきたマイクロ波を効率よくホーン形状の回転アンテナに結合させて供給することができない。   In this case, if the microwave transmitted through the waveguide is coupled to a rotating antenna having a similar waveguide shape and transmitted, the reflection can be reduced and the degree of coupling can be increased. As in the prior art, the shape and characteristic impedance are different, and when coupled to a horn-shaped rotating antenna that generates higher-order modes, the reflection between them increases and the degree of coupling decreases. The transmitted microwaves cannot be efficiently coupled to the horn-shaped rotating antenna and supplied.

また、回転アンテナをホーン形状にすれば空間に幅広くマイクロ波電力が拡散放射されるので、従来技術で述べているようなホーン形状としたことにより指向性を高めたとする効果は少ない。さらにホーン形状の伝送路をもつ特許文献1の回転アンテナではマイクロ波は高次のTEモードの波として伝送され、自由空間を伝送されるマイクロ波の姿態であるTEMモードと特性インピーダンスが異なるので、加熱室空間に放射される時に反射が生じるという問題がある。   Also, if the rotating antenna is formed into a horn shape, microwave power is diffused and radiated in a wide space. Therefore, the effect of increasing the directivity by using the horn shape as described in the prior art is small. Furthermore, in the rotating antenna of Patent Document 1 having a horn-shaped transmission path, the microwave is transmitted as a high-order TE mode wave, and the characteristic impedance is different from the TEM mode, which is a form of microwave transmitted through free space. There is a problem that reflection occurs when radiated to the heating chamber space.

そのために導波管やホーン形状部にリッジを設けてTEモードの波からTEMモードの波に変換して自由空間に放射する手段が考えられ、従来例で示す特許文献2にはこれに類似した内容が示されているが、受信アンテナの特許でありリッジの高さをホーン形状部で低くして反射波を抑制し、導波管入り口で高くして電界強度を高めて平面回路検出器でとらえるのが目的の構成となっている。   For this purpose, a means for providing a ridge in the waveguide or horn-shaped portion to convert the TE mode wave into a TEM mode wave and radiating it into free space can be considered, which is similar to Patent Document 2 shown in the conventional example. Although the contents are shown, it is a patent of the receiving antenna, and the height of the ridge is lowered at the horn shape part to suppress the reflected wave, and the electric field strength is increased at the waveguide entrance to increase the electric field strength. The purpose is to capture.

これを回転アンテナに置き換えてリッジの効果を検証すると、ホーン形状の開放口でリッジの高さが低いためにTEMモードの波に変換されないので反射が大きくなりマイクロ波を効率よく放射できないばかりか、電界はリッジの高さが低いと集中しないのでホーン開放口での電界強度も弱くなり指向性を鋭くする効果もない。また、従来例ではリッジの高さが高い平面回路検出器部が回転アンテナではマイクロ波給電部となるので、給電部近傍に金属製の背の高い金属製リッジを設けることはその部分での反射が大きくなり整合がとれないという問題がある。   When this is replaced with a rotating antenna and the effect of the ridge is verified, since the height of the ridge is low at the horn-shaped opening, it is not converted into a TEM mode wave, so the reflection becomes large and microwaves can not be radiated efficiently, Since the electric field does not concentrate when the height of the ridge is low, the electric field strength at the opening of the horn becomes weak and there is no effect of sharpening the directivity. In addition, in the conventional example, the planar circuit detector portion having a high ridge height serves as a microwave feeding portion in the rotating antenna. Therefore, providing a metal tall metal ridge in the vicinity of the feeding portion reflects on that portion. There is a problem that it becomes large and cannot be matched.

なお、TEモードとはマイクロ波の進行方向Zに電界成分を持たない(磁界成分はあってもよく、電界成分はマイクロ波の進行方向Zに対して直角な面でのX方向、Y方向にある)波の姿態をさす。TEMモードとはマイクロ波の進行方向Zに電界成分も磁界成分も持たない波(電界成分や磁界成分はマイクロ波の進行方向Zに対して直角な面でのX方向、Y方向にある)の姿態をさす。高次モードとは伝送路において、マイクロ波の進行方向Zに対して直角な面でのX方向、Y方向に電界成分や磁界成分が複数個発生する波の姿態をさす。   The TE mode has no electric field component in the microwave traveling direction Z (there may be a magnetic field component, and the electric field component is in the X and Y directions on a plane perpendicular to the microwave traveling direction Z). (A)) The appearance of the wave. The TEM mode is a wave having neither an electric field component nor a magnetic field component in the microwave traveling direction Z (the electric field component and the magnetic field component are in the X direction and the Y direction on a plane perpendicular to the microwave traveling direction Z). Appear. The higher-order mode refers to a wave form in which a plurality of electric field components and magnetic field components are generated in the X and Y directions on a plane perpendicular to the microwave traveling direction Z in the transmission line.

本発明は上記の問題を解決するためになされたものであり、請求項1の高周波加熱装置では、被加熱物を収容する加熱室と、該加熱室の底面に設けた誘電体からなる被加熱物載置板と、この被加熱物載置板の下方で前記加熱室の底面略中央部に設けた高周波供給室と、マイクロ波エネルギーを発生するマグネトロンと、該マグネトロンを取り付ける導波管と、前記高周波供給室底面中央部に設けた結合孔と、該結合孔を貫通して前記高周波供給室内へ略垂直に臨んで設けた内導体と、該内導体の一端の前記高周波供給室内に略水平に連結した金属製で立体構造の回転アンテナと、前記内導体の前記導波管内で連結した誘電体軸と、該誘電体軸を回転駆動する駆動部とを備え、前記回転アンテナは、第1長辺、第2長辺、第1短辺、第2短辺で囲まれた矩形部と、前記第2長辺と略平行により長い第3長辺と、該第3長辺と前記第1短辺を結ぶ第1辺と、前記第3長辺と前記第2短辺を結ぶ第2辺と、前記第2長辺で台形部とを有し、前記第1長辺、前記第1短辺、前記第2短辺、前記第1辺、および、前記第2辺には下向きの垂直壁部を備え、前記内導体は、前記回転アンテナの矩形部の下面に接しており、前記第1長辺および第2長辺は、1/2λ(λはマイクロ波の波長)より長く、かつ、λより短く、前記矩形部の垂直壁の高さは、1/2λより短い構成とした。
The present invention has been made to solve the above problems, and in the high-frequency heating device according to claim 1, a heating chamber including a heating chamber for storing an object to be heated and a dielectric provided on a bottom surface of the heating chamber. An object mounting plate, a high-frequency supply chamber provided at a substantially central portion of the bottom surface of the heating chamber below the heated object mounting plate, a magnetron for generating microwave energy, a waveguide for attaching the magnetron, A coupling hole provided in a central portion of the bottom surface of the high-frequency supply chamber, an inner conductor provided through the coupling hole and facing the high-frequency supply chamber substantially vertically, and substantially horizontal in the high-frequency supply chamber at one end of the inner conductor comprising a rotating antenna conformational a metal linked, a dielectric shaft coupled with said waveguide in said conductor, and a drive unit for rotating the dielectric body axis, to said rotating antenna, the 1 long side, 2nd long side, 1st short side, 2nd short side An enclosed rectangular portion, a third long side that is substantially parallel to the second long side, a first side connecting the third long side and the first short side, the third long side, and the second long side A second side connecting the short sides, and a trapezoidal portion at the second long side, the first long side, the first short side, the second short side, the first side, and the second side. The side is provided with a downward vertical wall portion, the inner conductor is in contact with the lower surface of the rectangular portion of the rotating antenna, and the first long side and the second long side are 1 / 2λ (λ is the microwave The vertical wall height of the rectangular portion is shorter than 1 / 2λ .

本発明の高周波加熱装置の回転アンテナでは、矩形部の第1長辺および第2長辺は、1/2λ(λはマイクロ波の波長)より長く、かつλより短く、前記矩形部の垂直壁の高さは、1/2λより短くすることにより高次モードのマイクロ波を発生させることなく、前記導波管と同じTEモードの波の姿態で回転アンテナの導波路部に結合させることができるので反射が少なく結合度も大きくとれる効果があり、マグネトロンで発生させたマイクロ波エネルギーを効率よく回転アンテナの導波路に伝送できる。   In the rotary antenna of the high-frequency heating device of the present invention, the first long side and the second long side of the rectangular portion are longer than 1 / 2λ (λ is the wavelength of the microwave) and shorter than λ, and the vertical wall of the rectangular portion is Can be coupled to the waveguide portion of the rotating antenna in the same TE mode wave form as the waveguide without generating higher-order mode microwaves by making the height less than 1 / 2λ. Therefore, there is an effect that the reflection is small and the degree of coupling is large, and the microwave energy generated by the magnetron can be efficiently transmitted to the waveguide of the rotating antenna.

実施例1の高周波加熱装置の要部縦断面図。1 is a longitudinal sectional view of a main part of a high-frequency heating device according to Embodiment 1. FIG. 実施例1の回転アンテナの斜視図。1 is a perspective view of a rotary antenna according to Embodiment 1. FIG. 実施例2の回転アンテナの斜視図。FIG. 6 is a perspective view of a rotating antenna according to a second embodiment. 各実施例の回転アンテナの反射係数を解析により求めた図。The figure which calculated | required the reflection coefficient of the rotating antenna of each Example by analysis. 各実施例の回転アンテナの放射路前方での電界強度を解析により求めた図。The figure which calculated | required the electric field strength in the radiation path front of the rotating antenna of each Example by analysis. 実施例3の回転アンテナの斜視図。FIG. 6 is a perspective view of a rotating antenna according to a third embodiment. 実施例4の回転アンテナの斜視図。FIG. 6 is a perspective view of a rotating antenna according to a fourth embodiment. 実施例5の回転アンテナの斜視図。FIG. 10 is a perspective view of a rotating antenna according to a fifth embodiment.

以下、図1〜図7を参照して本発明の実施例を説明する。   Embodiments of the present invention will be described below with reference to FIGS.

図1は実施例1の高周波加熱装置の要部縦断面図で、図2、図3は回転アンテナの斜視図、図4A、図4Bはそれぞれ回転アンテナの凸部(リッジ)の違いによる結合度を評価するための反射係数と、指向性を評価するための電界強度の解析値を示している。   FIG. 1 is a longitudinal sectional view of a main part of the high-frequency heating device of Example 1, FIGS. 2 and 3 are perspective views of a rotating antenna, and FIGS. 4A and 4B are coupling degrees due to differences in convex portions (ridges) of the rotating antenna. 2 shows an analysis value of a reflection coefficient for evaluating the directivity and an electric field intensity for evaluating directivity.

図1の要部断面図に示すように、本実施例の高周波加熱装置は、被加熱物12を収容する加熱室1と、加熱室1の底面に設けられた誘電体からなる被加熱物載置板2と、この被加熱物載置板2の下方で加熱室1の底面略中央部に設けられた高周波供給室3と、マイクロ波エネルギーを発生するマグネトロン4と、マグネトロン4を取り付ける導波管5と、導波管5に導かれたマイクロ波エネルギーを高周波供給室3に放射するために高周波供給室底面中央部に設けられた結合穴6と、結合穴6を貫通して高周波供給室3内へ略垂直に臨んで設けられた内導体7と、内導体7の一端の高周波供給室3内に略水平に連結された金属製で立体構造の回転アンテナ8と、内導体7の導波管内で連結された誘電体軸9と、穴10を介して誘電体軸9を回転駆動する駆動部11とを備えており、回転アンテナ8は駆動部11により回転自在となっている。そして、マグネトロン4で発生したマイクロ波エネルギーは導波管5に導かれ、結合穴6を貫通する内導体7との同軸モード結合により上記回転アンテナ8に伝搬され、高周波供給室3、被加熱物載置板2を通して加熱室1内に放射される。   As shown in the cross-sectional view of the main part of FIG. 1, the high-frequency heating device of the present embodiment is mounted on a heated object 1 made of a heating chamber 1 that houses an object to be heated 12 and a dielectric provided on the bottom surface of the heating chamber 1. A mounting plate 2, a high-frequency supply chamber 3 provided at a substantially central portion of the bottom surface of the heating chamber 1 below the heated object mounting plate 2, a magnetron 4 that generates microwave energy, and a waveguide to which the magnetron 4 is attached. A tube 5, a coupling hole 6 provided in the center of the bottom surface of the high-frequency supply chamber for radiating microwave energy guided to the waveguide 5 to the high-frequency supply chamber 3, and a high-frequency supply chamber penetrating the coupling hole 6 3, an inner conductor 7 that is provided substantially vertically, and a metal three-dimensional rotating antenna 8 that is connected substantially horizontally to the high-frequency supply chamber 3 at one end of the inner conductor 7. The dielectric shaft 9 connected in the wave tube and the dielectric shaft 9 are rotated through the hole 10. And a drive unit 11 for driving the rotation antenna 8 is rotatable by a drive unit 11. Then, the microwave energy generated in the magnetron 4 is guided to the waveguide 5 and propagated to the rotating antenna 8 by coaxial mode coupling with the inner conductor 7 penetrating the coupling hole 6, and the high-frequency supply chamber 3, the object to be heated Radiated into the heating chamber 1 through the mounting plate 2.

図2(b)に示すように、回転アンテナ8は、導波路13となる矩形部8fと放射路14となる台形部8lとを一体に形成されたものであり、内導体7は、回転アンテナ8の矩形部8fの下面に接している。これにより、矩形部8fは、内導体7を介して伝わるマイクロ波エネルギーを台形部8lに導く導波路13となり、台形部8lは、矩形部8fを介して伝わるマイクロ波エネルギーを加熱室1に放射する放射路14となる。   As shown in FIG. 2 (b), the rotating antenna 8 is formed by integrally forming a rectangular portion 8f serving as the waveguide 13 and a trapezoidal portion 8l serving as the radiation path 14, and the inner conductor 7 includes the rotating antenna. 8 is in contact with the lower surface of the rectangular portion 8f. As a result, the rectangular portion 8f becomes the waveguide 13 that guides the microwave energy transmitted through the inner conductor 7 to the trapezoidal portion 8l, and the trapezoidal portion 8l radiates the microwave energy transmitted through the rectangular portion 8f to the heating chamber 1. The radiation path 14 is

図2(a)に示すように、矩形部8fは、第1長辺8a、第2長辺8b、第1短辺8c、第2短辺8dで囲まれており、さらに、第1長辺8a、第1短辺8c、第2短辺8dには下向きの垂直壁8eを備え、第2長辺8bは垂直方向に開口している。   As shown in FIG. 2A, the rectangular portion 8f is surrounded by a first long side 8a, a second long side 8b, a first short side 8c, and a second short side 8d, and further, the first long side 8a, the first short side 8c, and the second short side 8d are provided with downward vertical walls 8e, and the second long side 8b is open in the vertical direction.

また、台形部8lは、第2長辺8bと略平行で第2長辺8bより長い第3長辺8h、第2長辺8bと第3長辺8hを結ぶ第1辺8i、第2辺8jで囲まれており、第1辺8iおよび第2辺8jには下向きの垂直壁部8kを備え、第3長辺8hは垂直方向に開口している。   The trapezoidal portion 8l includes a third long side 8h that is substantially parallel to the second long side 8b and longer than the second long side 8b, a first side 8i that connects the second long side 8b and the third long side 8h, and a second side 8j, the first side 8i and the second side 8j are provided with downward vertical wall portions 8k, and the third long side 8h is open in the vertical direction.

本実施例の回転アンテナ8では、第1長辺8aと第2長辺8bの長さを、1/2λ(λはマイクロ波の波長)より長く、かつ、λより短くするとともに、矩形部8fの垂直壁8eの高さを、1/2λより短くした。   In the rotating antenna 8 of the present embodiment, the length of the first long side 8a and the second long side 8b is longer than 1 / 2λ (λ is the wavelength of the microwave) and shorter than λ, and the rectangular portion 8f. The height of the vertical wall 8e is shorter than 1 / 2λ.

以上で説明した本実施例の回転アンテナ8では、第1長辺8aと第2長辺8bの長さを、1/2λより長く、かつ、λより短くするとともに、矩形部8fの垂直壁8eの高さを、1/2λより短くすることにより、垂直壁8eの高さ方向には電界成分をもたず、第1長辺8aおよび第2長辺8bに一個の電界成分のみが表れるTEモードの波の基本モードTE10となり、高次モードのマイクロ波の発生を抑制し、導波管5と同じTE10モードの波の姿態で回転アンテナ8の導波路13に結合させることができ、反射が少なく結合度も大きくとることができる。   In the rotating antenna 8 of the present embodiment described above, the lengths of the first long side 8a and the second long side 8b are longer than 1 / 2λ and shorter than λ, and the vertical wall 8e of the rectangular portion 8f. Is made shorter than ½λ, there is no electric field component in the height direction of the vertical wall 8e, and only one electric field component appears on the first long side 8a and the second long side 8b. It becomes the fundamental mode TE10 of the mode wave, suppresses the generation of higher-order mode microwaves, can be coupled to the waveguide 13 of the rotating antenna 8 in the same TE10 mode wave form as the waveguide 5, and the reflection The degree of coupling can be increased with little.

実施例2の回転アンテナ8を図3に示す。なお、実施例1と共通する点は説明を省略する。実施例1との相違は、実施例2の回転アンテナ82では、その下面が平坦であるのに対し、図3の回転アンテナ8では、その下面に第2長辺8bと垂直な向きの凸部(リッジ)15を設けている。なお、図3から明らかなように、凸部(リッジ)15の高さと幅は一様としている。ここで、凸部(リッジ)15の幅、高さ寸法は、回転アンテナ8の導波路13の第1長辺8aおよび第2長辺8bの長さの約3/1以内、垂直壁8eの高さのおよそ1/2以内に選んでいる。   The rotating antenna 8 of Example 2 is shown in FIG. Note that the description of the points in common with the first embodiment will be omitted. The difference from the first embodiment is that the lower surface of the rotary antenna 82 of the second embodiment is flat, whereas the lower surface of the rotary antenna 8 of FIG. 3 has a convex portion oriented in the direction perpendicular to the second long side 8b. (Ridge) 15 is provided. As is apparent from FIG. 3, the height and width of the convex portion (ridge) 15 are uniform. Here, the width and height of the convex portion (ridge) 15 are within about 3/1 of the length of the first long side 8a and the second long side 8b of the waveguide 13 of the rotating antenna 8, and the vertical wall 8e. Selected within about 1/2 of the height.

本実施例の回転アンテナ8では、矩形部8fと台形部8lの下面に第2長辺8dと垂直な向きの凸部(リッジ)15を設けたことで、マグネトロン4から導波管5内を伝送されてきたTEモードのマイクロ波を導波路13、放射路14で加熱室内(自由空間)を伝送されるマイクロ波のモードであるTEMモードの波の姿態に変換することができる。   In the rotating antenna 8 of the present embodiment, a convex portion (ridge) 15 oriented in the direction perpendicular to the second long side 8d is provided on the lower surface of the rectangular portion 8f and the trapezoidal portion 8l. The transmitted TE mode microwave can be converted to a TEM mode wave form, which is a microwave mode transmitted through the heating chamber (free space) through the waveguide 13 and the radiation path 14.

具体的には、マグネトロンから導波管内を伝送されてきたTEモードのマイクロ波が矩形形状の導波路で同じTEモードの波の姿態で結合されたのち、凸部(リッジ)15の作用で導波路、放射路で平行線路や自由空間を伝送されるマイクロ波のモードであるTEMモードの波の姿態に変換され、放射路から加熱室空間に放射されるようになるので、回転アンテナから加熱室空間に放射される時の反射波の発生を抑制できる。   Specifically, TE mode microwaves transmitted through the waveguide from the magnetron are combined in the same TE mode wave form in a rectangular waveguide, and then guided by the action of the convex portion (ridge) 15. Since it is converted into a TEM mode wave form, which is a microwave mode transmitted through a parallel line or free space through a waveguide or radiation path, it is radiated from the radiation path to the heating chamber space. Generation of reflected waves when radiated into space can be suppressed.

実施例3の回転アンテナ8を図5に示す。なお、実施例2と共通する点は説明を省略する。実施例2との相違は、凸部(リッジ)15の形状にあり、本実施例では、凸部(リッジ)15の幅は一様であるが、高さは、矩形部8f側で小さく、台形部8l側で大きい、楔状としている。   The rotating antenna 8 of Example 3 is shown in FIG. Note that description of points in common with the second embodiment will be omitted. The difference from the second embodiment is the shape of the convex portion (ridge) 15. In this embodiment, the width of the convex portion (ridge) 15 is uniform, but the height is small on the rectangular portion 8f side, A large wedge shape is formed on the trapezoidal portion 8l side.

本実施例の回転アンテナ8では、導波路13の長辺面に垂直に設けられた内導体7近傍の凸部(リッジ)15の高さ寸法を短くして放射路14に向かって高さ寸法を長くした楔形で構成することで、内導体7近傍での反射が抑制される。一方、放射路14の下底部8−8の凸部(リッジ)15では高さ寸法が高くしているので、放射路14の第3長辺8h部近傍でTEモードの波の姿態が加熱室1内を伝送されるのと同じTEMモードの波の姿態に変換され易くなり、放射路と加熱室空間との整合がとれ、反射波の抑制に加えて電界強度を増すことができ、指向性も鋭くなる。   In the rotating antenna 8 of this embodiment, the height dimension of the convex portion (ridge) 15 near the inner conductor 7 provided perpendicularly to the long side surface of the waveguide 13 is shortened and the height dimension toward the radiation path 14 is reached. By making the wedge shape longer, reflection near the inner conductor 7 is suppressed. On the other hand, since the height dimension of the convex portion (ridge) 15 of the lower bottom portion 8-8 of the radiation path 14 is high, the TE mode wave appearance is near the third long side 8h portion of the radiation path 14 in the heating chamber. It is easy to be converted into the same TEM mode wave form that is transmitted through 1, the radiation path and the heating chamber space can be matched, the electric field strength can be increased in addition to the suppression of the reflected wave, and the directivity Also become sharper.

実施例4の回転アンテナ8を図6に示す。なお、実施例2と共通する点は説明を省略する。実施例2との相違は、凸部(リッジ)15の形状にあり、本実施例では、凸部(リッジ)15の高さと幅の両方が、矩形部8f側で小さく、台形部8l側で大きい、四角錐状としている。   The rotating antenna 8 of Example 4 is shown in FIG. Note that description of points in common with the second embodiment will be omitted. The difference from the second embodiment is the shape of the convex portion (ridge) 15. In this embodiment, both the height and width of the convex portion (ridge) 15 are small on the rectangular portion 8f side, and on the trapezoidal portion 8l side. It has a large, quadrangular pyramid shape.

本実施例の回転アンテナ8では、内導体7近傍の凸部(リッジ)15の高さ寸法、幅寸法を共に短くして内導体7近傍から放射路14に向かって凸部(リッジ)15の高さ寸法、幅寸法を共に長くした四角錐形にしているので、実施例3よりもさらに内導体7近傍での反射を抑制することができ、放射路下底部での電界強度が強くでき指向性も鋭くなるという効果がある。   In the rotating antenna 8 of the present embodiment, the height and width of the convex portion (ridge) 15 near the inner conductor 7 are shortened, and the convex portion (ridge) 15 of the convex portion (ridge) 15 from the vicinity of the inner conductor 7 toward the radiation path 14 is shortened. Since the height and width are both rectangular pyramids, the reflection near the inner conductor 7 can be further suppressed than in the third embodiment, and the electric field strength at the bottom of the radiation path can be increased and directed. It has the effect of improving sharpness.

実施例5の回転アンテナ8を図7に示す。なお、実施例2と共通する点は説明を省略する。実施例2との相違は、凸部(リッジ)15の形状、および、切り込み16、フランジ17を設けた点にある。   A rotating antenna 8 of Example 5 is shown in FIG. Note that description of points in common with the second embodiment will be omitted. The difference from the second embodiment is that the shape of the convex portion (ridge) 15 and the notch 16 and the flange 17 are provided.

本実施例の回転アンテナ8では、放射路14の台形部8lに切り込み16を設けることで、反射を抑制し整合性や指向性などを向上させることに加え、回転アンテナ8の真上に置かれた被加熱物12もむらなく効率よく加熱することができる。   In the rotating antenna 8 of the present embodiment, the notch 16 is provided in the trapezoidal portion 8 l of the radiation path 14, so that reflection is suppressed and consistency and directivity are improved. In addition, the rotating antenna 8 is placed directly above the rotating antenna 8. The heated object 12 can also be heated efficiently without unevenness.

また、導波路13や放射路14の垂直壁8e、垂直壁部8kには、これらと直角にフランジ17を設けることにより、垂直壁8e、垂直壁部8kとこれと対向する高周波供給口3の底面間でのスパーク発生の防止と、マイクロ波電力の伝送方向と垂直な側面からの漏洩電力を抑制し指向性を高めることができる。   In addition, the vertical wall 8e and the vertical wall portion 8k of the waveguide 13 and the radiation path 14 are provided with flanges 17 at right angles to the vertical wall 8e and the vertical wall portion 8k, and the high-frequency supply port 3 facing the vertical wall 8e and the vertical wall portion 8k. It is possible to increase the directivity by preventing the occurrence of sparks between the bottom surfaces and suppressing the leakage power from the side surface perpendicular to the transmission direction of the microwave power.

さらに、凸部15は丸みを帯びた円錐形状で絞り加工により一体加工した円錐形で構成し、直方体状や、楔形、四角錐形の凸部(リッジ)15の角部で発生しがちな電界集中による異常加熱やスパークを抑制することができる。   Further, the convex portion 15 is formed in a rounded conical shape and integrally formed by drawing, and an electric field that tends to be generated at a corner portion of a rectangular parallelepiped shape, a wedge shape, or a quadrangular pyramid shape convex portion (ridge) 15. Abnormal heating and sparks due to concentration can be suppressed.

〔参考例〕
図4を用いて、各実施例の回転アンテナ8の特性を従来の台形型回転アンテナと比較しながら説明する。なお、図4Aは、各実施例の回転アンテナの反射係数を解析により求めた図であり、縦軸は反射係数を横軸は周波数f(MHz)をとっている。また、図4Bは、各実施例の回転アンテナの放射路前方での電界強度をマグネトロン出力800ワットとして解析により求めた図であり、縦軸は電界強度E(V/m)をとっている。
[Reference example]
The characteristics of the rotating antenna 8 of each embodiment will be described using FIG. 4 in comparison with a conventional trapezoidal rotating antenna. FIG. 4A is a diagram obtained by analyzing the reflection coefficient of the rotating antenna of each example, where the vertical axis represents the reflection coefficient and the horizontal axis represents the frequency f (MHz). FIG. 4B is a diagram obtained by analysis with the electric field strength in front of the radiation path of the rotating antenna of each example as a magnetron output of 800 watts, and the vertical axis represents the electric field strength E (V / m).

図4Aに示すように、従来例と実施例1〜4の回転アンテナ8の反射係数を比べると、(実施例4)<(実施例3)<(実施例2)<(実施例1)<(従来例)となる。なお、実施例5は実施例4と実施例3の中間程度の特性となる。   As shown in FIG. 4A, when the reflection coefficient of the rotating antenna 8 of the conventional example and Examples 1 to 4 is compared, (Example 4) <(Example 3) <(Example 2) <(Example 1) < (Conventional example). In addition, Example 5 becomes a characteristic in the middle of Example 4 and Example 3.

一般に、結合度は反射係数の値から評価し、反射係数が小さいほど結合度が大きくなる。従って、矩形型の導波路13と台形型の放射路14を組み合わせた実施例1の回転アンテナ8の結合度が、従来の台形型の放射路からなる回転アンテナよりも大きくなるという効果や、それぞれの実施例の凸部(リッジ)15の形状違いによる結合度の違いがわかる。   In general, the degree of coupling is evaluated from the value of the reflection coefficient, and the degree of coupling increases as the reflection coefficient decreases. Therefore, the effect that the degree of coupling of the rotating antenna 8 of the first embodiment combining the rectangular waveguide 13 and the trapezoidal radiation path 14 is larger than that of the conventional rotating antenna composed of the trapezoidal radiation path, The difference in the degree of coupling due to the difference in the shape of the convex portion (ridge) 15 in the embodiment can be seen.

また、図4Bに示すように、従来例と実施例1〜4の回転アンテナ8の放射路前方での電界強度を比べると、(従来例)<(実施例1)<(実施例2)<(実施例3)<(実施例4)となる。なお、実施例5は実施例4と実施例3の中間程度の特性となる。   Moreover, as shown in FIG. 4B, when the electric field strength in the front of the radiation path of the rotating antenna 8 of Examples 1 to 4 is compared with that of the conventional example, (Conventional Example) <(Example 1) <(Example 2) < (Example 3) <(Example 4) In addition, Example 5 becomes a characteristic in the middle of Example 4 and Example 3.

一般に、指向性はアンテナ放射方向の電界強度の値から評価し、電界強度が大きいほど指向性が鋭くなる。従って、矩形型の導波路13と台形型の放射路を組み合わせた実施例1の回転アンテナの指向性が、従来の台形型の放射路からなる回転アンテナよりも鋭くなるという効果や、それぞれの凸部(リッジ)15の違いによる指向性の違いが分かる。   In general, the directivity is evaluated from the value of the electric field intensity in the antenna radiation direction, and the directivity becomes sharper as the electric field intensity increases. Therefore, the directivity of the rotating antenna according to the first embodiment, which is a combination of the rectangular waveguide 13 and the trapezoidal radiation path, is sharper than that of the conventional rotating antenna composed of the trapezoidal radiation path, and the respective convexities. The difference in directivity due to the difference in the portion (ridge) 15 can be seen.

なお、凸部(リッジ)15を設けることにより、放射方向の電界強度が強くなり、反射波の発生を抑制できるのは次の理由によるものである。すなわち、TEMモードの波の姿態で伝搬される自由空間や、TEモードの波の姿態で伝搬される導波管内では特性インピーダンスが異なる。自由空間での波の特性インピーダンスは伝搬される波の周波数に関係なく自由空間(真空中と見なせる)の誘電率εと透磁率μで決まり377Ωで、導波管の場合の特性インピーダンスは伝送する波の周波数と導波管の長辺寸法できまる。   In addition, by providing the convex part (ridge) 15, the electric field strength in the radial direction is increased, and the generation of reflected waves can be suppressed for the following reason. That is, the characteristic impedance differs in free space that propagates in a TEM mode wave form and in a waveguide that propagates in a TE mode wave form. The characteristic impedance of a wave in free space is determined by the dielectric constant ε and permeability μ of free space (which can be regarded as in a vacuum) regardless of the frequency of the propagated wave, and is 377Ω. The characteristic impedance in the case of a waveguide is transmitted. It can be determined by the wave frequency and the long dimension of the waveguide.

例えば、導波管の長辺長が85mmで周波数2450MHzのマイクロ波が伝送される場合は537Ωとなる。従って、導波管から加熱室の自由空間にマイクロ波が放射される時、マイクロ波のモードの違いで上記特性インピーダンスも異なるので、導波管出口から自由空間にマイクロ波が放射される時に両者境界面である導波管出口で不整合状態となり反射が生じる。そこで導波管内に凸部(リッジ)15を設けてTEMモードに変換して特性インピーダンスを自由空間の特性インピーダンスに近づけておけば導波管と自由空間の整合がとれて、導波管出口での反射が抑制され、電界強度も大きくとれる。このように導波管と類似した矩形型の導波路13や台形型の放射路14に凸部(リッジ)15を設けることで、TEモードの波がTEMモードの波の姿態に変換され、特性インピーダンスが低下し自由空間の特性インピーダンスに近づくからである。   For example, when a microwave having a long side length of 85 mm and a frequency of 2450 MHz is transmitted, it becomes 537Ω. Therefore, when microwaves are radiated from the waveguide to the free space of the heating chamber, the above characteristic impedance is also different depending on the mode of the microwaves. A mismatch occurs at the waveguide exit, which is the boundary surface, and reflection occurs. Therefore, if the convex portion (ridge) 15 is provided in the waveguide and converted into the TEM mode and the characteristic impedance is brought close to the characteristic impedance in the free space, the waveguide and the free space are matched, and the waveguide exit is obtained. Is suppressed, and the electric field strength can be increased. Thus, by providing the convex portion (ridge) 15 on the rectangular waveguide 13 or the trapezoidal radiation path 14 similar to the waveguide, the TE mode wave is converted into the TEM mode wave form, and the characteristics This is because the impedance decreases and approaches the characteristic impedance of free space.

なお、上記凸部(リッジ)15の幅、高さ寸法は回転アンテナ8の導波路13の長辺(第1長辺と第2長辺)の長さの約3/1以内、矩形部8fの垂直壁8eの高さのおよそ1/2以内に選んでいるのは、凸部(リッジ)15の幅寸法が長くなると電界集中が弱まりTEモードの波からTEMモードの波への変換効果が弱くなり、凸部(リッジ)15を設けたことによるモード変換と特性インピーダンスの変換効果が得られなくなるからである。また、凸部(リッジ)15高さ寸法が垂直壁8eの高さのおよそ1/2より長くなると、導波路13と放射路14内で反射が増大し回転アンテナ内をマイクロ波が伝搬されにくくなるのと、凸部(リッジ)15面と対向する高周波供給室3の底面間でのスパークが発生するからである。   The width and height of the convex portion (ridge) 15 are within about 3/1 of the length of the long side (first long side and second long side) of the waveguide 13 of the rotating antenna 8, and the rectangular portion 8f. The vertical wall 8e is selected within about 1/2 of the height of the vertical wall 8e because the electric field concentration is weakened when the width of the convex portion (ridge) 15 is increased, and the effect of conversion from the TE mode wave to the TEM mode wave is obtained. This is because the effect of mode conversion and characteristic impedance conversion due to the provision of the convex portion (ridge) 15 cannot be obtained. Further, when the height dimension of the convex portion (ridge) 15 becomes longer than about ½ of the height of the vertical wall 8e, reflection increases in the waveguide 13 and the radiation path 14, and the microwave is difficult to propagate through the rotating antenna. This is because a spark occurs between the bottom surfaces of the high-frequency supply chamber 3 facing the surface of the convex portion (ridge) 15.

1 加熱室
2 被加熱物載置板
3 高周波供給室
4 マグネトロン
5 導波管
6 結合穴
7 内導体
8 回転アンテナ
8a 第1長辺
8b 第2長辺
8c 第1短辺
8d 第2短辺
8e 垂直壁
8f 矩形部
8h 第3長辺
8i 第1辺
8j 第2辺
8k 垂直壁部
8l 台形部
9 誘電体軸
10 穴
11 駆動部
12 被加熱物
13 導波路
DESCRIPTION OF SYMBOLS 1 Heating chamber 2 To-be-heated object mounting plate 3 High frequency supply chamber 4 Magnetron 5 Waveguide 6 Coupling hole 7 Inner conductor 8 Rotating antenna 8a 1st long side 8b 2nd long side 8c 1st short side 8d 2nd short side 8e Vertical wall 8f Rectangular part 8h Third long side 8i First side 8j Second side 8k Vertical wall part 8l Trapezoid part 9 Dielectric shaft 10 Hole 11 Drive part 12 Heated object 13 Waveguide

Claims (3)

被加熱物を収容する加熱室と、該加熱室の底面に設けた誘電体からなる被加熱物載置板と、この被加熱物載置板の下方で前記加熱室の底面略中央部に設けた高周波供給室と、マイクロ波エネルギーを発生するマグネトロンと、該マグネトロンを取り付ける導波管と、前記高周波供給室底面中央部に設けた結合孔と、該結合孔を貫通して前記高周波供給室内へ略垂直に臨んで設けた内導体と、該内導体の一端の前記高周波供給室内に略水平に連結した金属製で立体構造の回転アンテナと、前記内導体の前記導波管内で連結した誘電体軸と、該誘電体軸を回転駆動する駆動部とを備え、
前記回転アンテナは、
第1長辺、第2長辺、第1短辺、第2短辺で囲まれた矩形部と、
前記第2長辺と略平行により長い第3長辺と、該第3長辺と前記第1短辺を結ぶ第1辺と、前記第3長辺と前記第2短辺を結ぶ第2辺と、前記第2長辺で台形部とを有し、
前記第1長辺、前記第1短辺、前記第2短辺、前記第1辺、および、前記第2辺には下向きの垂直壁部を備え、
前記内導体は、前記回転アンテナの矩形部の下面に接しており、
前記第1長辺および第2長辺は、1/2λ(λはマイクロ波の波長)より長く、かつ、λより短く、
前記矩形部の垂直壁の高さは、1/2λより短い
ことを特徴とする高周波加熱装置。
A heating chamber that accommodates an object to be heated, a heated object mounting plate made of a dielectric material provided on the bottom surface of the heating chamber, and provided at a substantially central portion of the bottom surface of the heating chamber below the heated object mounting plate. A high frequency supply chamber, a magnetron for generating microwave energy, a waveguide to which the magnetron is attached, a coupling hole provided at the center of the bottom surface of the high frequency supply chamber, and passing through the coupling hole into the high frequency supply chamber. An inner conductor facing substantially vertically, a metal three-dimensional rotating antenna connected substantially horizontally in the high-frequency supply chamber at one end of the inner conductor, and a dielectric connected in the waveguide of the inner conductor comprising a shaft, a driving unit for rotating the dielectric body axis, a,
The rotating antenna is
A rectangular portion surrounded by the first long side, the second long side, the first short side, and the second short side;
A third long side that is substantially parallel to the second long side, a first side connecting the third long side and the first short side, and a second side connecting the third long side and the second short side. And a trapezoidal portion on the second long side,
The first long side, the first short side, the second short side, the first side, and the second side include a downward vertical wall portion,
The inner conductor is in contact with the lower surface of the rectangular portion of the rotating antenna ;
The first long side and the second long side are longer than 1 / 2λ (λ is the wavelength of the microwave) and shorter than λ,
The high- frequency heating apparatus according to claim 1, wherein the height of the vertical wall of the rectangular portion is shorter than ½λ .
請求項1に記載の高周波加熱装置において、
前記矩形部は、前記内導体を介して伝わるマイクロ波エネルギーを前記第2長辺と前記第3長辺と前記第1辺および前記第2辺とからなる台形部に導く導波路であり、
前記台形部は、前記矩形部を介して伝わるマイクロ波エネルギーを前記加熱室に放射する放射路であることを特徴とする高周波加熱装置。
In the high frequency heating apparatus according to claim 1,
The rectangular portion is a waveguide that guides microwave energy transmitted through the inner conductor to a trapezoidal portion including the second long side, the third long side, the first side, and the second side,
The high frequency heating apparatus , wherein the trapezoidal portion is a radiation path that radiates microwave energy transmitted through the rectangular portion to the heating chamber .
請求項1又は2に記載の高周波加熱装置において、
前記矩形部と台形部の下面に前記第2長辺と垂直な向きの凸部(リッジ)を設けたことを特徴とする高周波加熱装置。
In the high frequency heating device according to claim 1 or 2 ,
A high-frequency heating apparatus , wherein convex portions (ridges) oriented in a direction perpendicular to the second long side are provided on the lower surfaces of the rectangular portion and the trapezoidal portion .
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