JPS6372089A - Radio frequency heater - Google Patents

Radio frequency heater

Info

Publication number
JPS6372089A
JPS6372089A JP61215365A JP21536586A JPS6372089A JP S6372089 A JPS6372089 A JP S6372089A JP 61215365 A JP61215365 A JP 61215365A JP 21536586 A JP21536586 A JP 21536586A JP S6372089 A JPS6372089 A JP S6372089A
Authority
JP
Japan
Prior art keywords
wall surface
cavity resonator
shaped conductor
inlet
door
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Granted
Application number
JP61215365A
Other languages
Japanese (ja)
Other versions
JPH0569276B2 (en
Inventor
岩淵 康司
哲男 窪田
幸雄 田中
多和田 正春
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Hitachi Heating Appliances Co Ltd
Original Assignee
Hitachi Heating Appliances Co Ltd
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Hitachi Heating Appliances Co Ltd filed Critical Hitachi Heating Appliances Co Ltd
Priority to JP61215365A priority Critical patent/JPS6372089A/en
Priority to GB8718229A priority patent/GB2196520B/en
Priority to DE19873726002 priority patent/DE3726002A1/en
Priority to KR1019870008619A priority patent/KR900008074B1/en
Priority to US07/082,471 priority patent/US4868359A/en
Priority to FR8711322A priority patent/FR2602626B1/en
Publication of JPS6372089A publication Critical patent/JPS6372089A/en
Publication of JPH0569276B2 publication Critical patent/JPH0569276B2/ja
Granted legal-status Critical Current

Links

Abstract

(57)【要約】本公報は電子出願前の出願データであるた
め要約のデータは記録されません。
(57) [Abstract] This bulletin contains application data before electronic filing, so abstract data is not recorded.

Description

【発明の詳細な説明】 産業上の利用分野 本発明は高周波加熱装置のドア構造の改良に関する。[Detailed description of the invention] Industrial applications The present invention relates to an improvement in the door structure of a high frequency heating device.

従来の技術 高周波加熱装置のドア周縁に特性インピーダンスの異な
る溝を深さ方向に設け、この溝の深さ方向の特性インピ
ーダンスを不連続にすることにより実質的深さが使用波
長の4分の1より小さくしても、溝の入口でのインピー
ダンスが最大となり。
Conventional technology Grooves with different characteristic impedances are provided in the depth direction on the periphery of the door of a high-frequency heating device, and by making the characteristic impedance of the grooves discontinuous in the depth direction, the effective depth can be reduced to one-fourth of the wavelength used. Even if it is made smaller, the impedance at the entrance of the groove is maximum.

チョーク溝と同様に漏洩電波を少なくすることができる
という提案が特開昭60−25190号公報にある。こ
の従来例では、溝の深さ方向に幅の異なる溝を設けたり
、溝の周壁の形状を深さ方向に変形するなどかなり形状
が複雑である。また、特性インピーダンスの不連続部に
おける反射防止を考慮する必要がある。
There is a proposal in Japanese Patent Laid-Open No. 60-25190 that it is possible to reduce leakage radio waves in the same way as choke grooves. In this conventional example, the shape is quite complicated, such as providing grooves with different widths in the depth direction of the groove and deforming the shape of the peripheral wall of the groove in the depth direction. Furthermore, it is necessary to consider reflection prevention at discontinuous portions of characteristic impedance.

寸た。第7図で示すように、ドア5の外周に電波漏洩防
止用の空胴共振器12を屈曲形成して口字状断面とし、
空胴共振器12の一周壁である張出面11の端部切口と
空胴共振器12の他の壁面(第1の壁面8)とを対向さ
せた入口25を有する構造が実開昭61−795号公報
に示されている。この従来例では空胴共振器12の周壁
が複数の導体片に分割さ凡ているとは記載されていない
。したがって空胴共振器12内には進行方向がyz面以
外にも生じる高次モードの電波が入ってくるため、空胴
共振器12が共振状態から外れ、電波漏洩防止効果が小
さくなる。仮りに第7図の空胴共振器12の立ち上がり
面23と張出面11を長手方向(X方向)に使用波長の
−より小さい幅の導体片に分割したと考える。
Dimensions. As shown in FIG. 7, a cavity resonator 12 for preventing radio wave leakage is formed in a curved manner on the outer periphery of the door 5 to form a mouth-shaped cross section.
A structure having an entrance 25 in which the end cut of the protruding surface 11, which is one peripheral wall of the cavity resonator 12, and the other wall surface (first wall surface 8) of the cavity resonator 12 are opposed was developed in 1982. It is shown in Publication No. 795. This conventional example does not describe that the peripheral wall of the cavity resonator 12 is divided into a plurality of conductor pieces. Therefore, higher-order mode radio waves whose propagation direction is not in the yz plane enter the cavity resonator 12, so the cavity resonator 12 goes out of the resonant state and the radio wave leakage prevention effect becomes smaller. It is assumed that the rising surface 23 and the projecting surface 11 of the cavity resonator 12 shown in FIG. 7 are divided into conductor pieces each having a width smaller than the wavelength used in the longitudinal direction (X direction).

この場合、空胴共振器12を等価容量Cと等価イン′ダ
クタンスLとから成る並列共振素子をドア5の長手方向
(X方向)に複数個並べたものとみなせる。各並列共振
素子において、後述の(2)式で示すように、空胴共振
器12の入口25と空胴断面の面積tb丁 中心0の距離tMと、入口寸法Gとの比で−が大きいほ
ど等価容量Cが大きくなる。第7図の空胴共振器12で
はZM =t oで、後述する本発明のb≧G    
                   G1.5に比
べて等価容量Cが小さくなる。その分だけ後述の(3)
式より等価インダクタンスLを大きくして漏洩電波の周
波数に共振させるようにしなければならない。そのため
、後述の(1)式から明らかなように、空胴共振器12
の断面ABを大きくする必要があるので、従来例の空胴
共振器12は大形となり、ドアの小形化、低コスト化に
は不向きである。
In this case, the cavity resonator 12 can be regarded as a plurality of parallel resonant elements each having an equivalent capacitance C and an equivalent inductance L arranged in the longitudinal direction (X direction) of the door 5. In each parallel resonant element, as shown in equation (2) below, - is large in the ratio of the distance tM between the entrance 25 of the cavity resonator 12 and the center 0 of the cavity cross section, and the entrance dimension G. The equivalent capacitance C becomes larger. In the cavity resonator 12 of FIG. 7, ZM = t o, and b≧G of the present invention, which will be described later
The equivalent capacitance C is smaller than that of G1.5. For that reason, see (3) below.
According to the formula, the equivalent inductance L must be increased to resonate with the frequency of the leaked radio waves. Therefore, as is clear from equation (1) below, the cavity resonator 12
Since it is necessary to increase the cross section AB of the conventional cavity resonator 12, the conventional cavity resonator 12 becomes large, and is not suitable for downsizing and cost reduction of the door.

な2.第7図は実開昭61−795号公報の明細書の図
面の各部寸法を同一比率で示したものであり。
2. FIG. 7 shows the dimensions of each part of the drawings in the specification of Japanese Utility Model Application Publication No. 61-795 in the same proportions.

また、構成要素の名称および番号は本発明と対応する部
分は同じにしである。
Also, the names and numbers of the components corresponding to those of the present invention are the same.

発明が解決しようとする問題点 溝の深さ方向に、複雑な形状をした溝を設ける必要があ
り、また、特性インピーダンスの不連続部における反射
防止に手間が掛かったり、ドアの小形化に不向きな点で
ある。
Problems to be solved by the invention It is necessary to provide grooves with complicated shapes in the depth direction of the groove, and it takes time and effort to prevent reflections at discontinuous portions of characteristic impedance, making it unsuitable for miniaturizing doors. This is a point.

問題点を解決するだめの手段 ドア周囲に口字状断面を持つ漏洩電波防止用の空胴共振
器を設け、との空胴共振器の壁面の一部を多数のコ字状
導体片で形成し、又空胴共振器に漏洩電波を導びき入れ
る入口をコ字状導体片の一部と他の壁面の一部とで形成
し、かつこの入口と空胴断面の面積中心の距離AMと、
入口寸法GとのM 止子を1.5以上とし、更に又、入口両端部に2個の容
量調整素子を設け、他の壁面側の容量調整素子をコ字状
導体片側のものより大きくしたものである。
A workaround to the problem was to install a cavity resonator with a cross section around the door to prevent leakage radio waves, and form part of the wall of the cavity resonator with a large number of U-shaped conductor pieces. In addition, an entrance for introducing leakage radio waves into the cavity resonator is formed by a part of the U-shaped conductor piece and a part of the other wall surface, and the distance between this entrance and the center of area of the cavity cross section is AM. ,
The M stopper between the entrance dimension G was set to 1.5 or more, and two capacitance adjustment elements were provided at both ends of the entrance, and the capacitance adjustment element on the other wall side was made larger than the one on one side of the U-shaped conductor. It is something.

作用 上記のように構成することにより、コ字状導体片により
漏洩しようとする電波はTEM波として口字状断面の空
胴共振器内に導びき入れられる。
Operation With the above configuration, radio waves that are about to leak due to the U-shaped conductor piece are guided into the cavity resonator with the square-shaped cross section as TEM waves.

この空胴共振器は、近似的に1巻きの筒状コイルとして
空胴断面積に比例した等価インダクタンスLと、空胴の
入口付近の乱れ電界に基づく等価容量Cから成る並列共
振素子を形成する。空胴の入口を小さくし2個の容量調
整素子を設けるとCが大きくなり、その分だけLを小さ
くできる。すなわち空胴断面積を小さくできる。口字状
断面の各辺がそれぞれ使用波長の4分の1よりも小さい
寸法で、電波シール効果が最大となる。
This cavity resonator forms a parallel resonant element consisting of an equivalent inductance L proportional to the cross-sectional area of the cavity and an equivalent capacitance C based on the disturbed electric field near the entrance of the cavity as a cylindrical coil with approximately one turn. . If the entrance of the cavity is made smaller and two capacitance adjustment elements are provided, C becomes larger, and L can be made smaller by that amount. In other words, the cross-sectional area of the cavity can be reduced. The radio wave sealing effect is maximized when each side of the cross-section is smaller than one quarter of the wavelength used.

実施例 本発明の一実施例による高周波加熱装置の構成および使
用を図面とともに説明する。
Embodiment The structure and use of a high-frequency heating device according to an embodiment of the present invention will be explained with reference to the drawings.

第1図および第2図において、1は加熱室で。In Figures 1 and 2, 1 is a heating chamber.

2は加熱室1の開口部を取り囲む7ランジで、3は外箱
である。4は加熱室1内を覗くためにドア5の中央部に
できるだけ広範囲に設けた小穴群である。6はこの小穴
群4の周囲を取り囲む段部でこの段部6は小穴群4の内
面に固着した透光性のドア内カバー15の端部が清掃の
際などにはがれるのを防ぐと共に、ドア5閉成時にフラ
ンジ2と平面接触する封口面7の平面度を良くするもの
である。8は封口面7の端部より7ランジ2に対して略
直角に折り曲げた第1の壁面である。9は第1の壁面8
の端部よりフランジ2に対して略平行と延長した第2の
壁面である。10は第2の壁面9に溶接した多数のコ字
状導体片である。このコ字状導体片10は第2の壁面9
に溶接される取シ付け面19と、第1の壁面8にほぼ平
行に対向する立ち上がり面23と、端部切口を第1の壁
面8に対向させた張出面11との3面から成る。ドア5
の周囲の長手方向に対する各コ字状導体片10の幅D(
X方向)は使用波長の2分の1よりも小さくしている。
2 is seven lunges surrounding the opening of the heating chamber 1, and 3 is an outer box. Reference numeral 4 designates a group of small holes provided in the center of the door 5 as wide as possible to allow viewing into the heating chamber 1. Reference numeral 6 denotes a stepped portion that surrounds the small hole group 4. This stepped portion 6 prevents the edge of the translucent door inner cover 15 fixed to the inner surface of the small hole group 4 from peeling off during cleaning, etc. 5. This improves the flatness of the sealing surface 7 which makes plane contact with the flange 2 when closed. Reference numeral 8 denotes a first wall surface bent from the end of the sealing surface 7 at a substantially right angle to the 7 flange 2 . 9 is the first wall surface 8
This is a second wall surface extending substantially parallel to the flange 2 from the end thereof. 10 is a large number of U-shaped conductor pieces welded to the second wall surface 9. This U-shaped conductor piece 10 is connected to the second wall surface 9
It consists of three surfaces: a mounting surface 19 that is welded to the surface, a rising surface 23 that faces the first wall surface 8 in a substantially parallel manner, and an overhanging surface 11 that has an end cut facing the first wall surface 8. door 5
The width D of each U-shaped conductor piece 10 in the longitudinal direction around the
(X direction) is made smaller than half of the wavelength used.

第1の壁面8とコ字状導体片10とで囲まれた口字状断
面は狭小な入口25を有する空胴共振器12を形成する
。この空胴共振器12の入口25をふさぐ不透明の誘電
体カバー13から突き出した突起片14はコ字状導体片
10の立ち上がり面23に設けた取り付け穴18に引っ
掛かるようになっている。ドア5の前面を覆う透光性の
ドア外カバー13を保持するための誘電体製のドア外枠
24から突き出した突起片17は第2の壁面9の最外周
縁端部20に引っ掛かるようになっている。
The opening-shaped cross section surrounded by the first wall surface 8 and the U-shaped conductor piece 10 forms a cavity resonator 12 having a narrow entrance 25 . A projection piece 14 protruding from an opaque dielectric cover 13 that blocks an entrance 25 of this cavity resonator 12 is adapted to be caught in a mounting hole 18 provided in a rising surface 23 of the U-shaped conductor piece 10. A protruding piece 17 protruding from a dielectric door frame 24 for holding a translucent door outer cover 13 covering the front surface of the door 5 is hooked onto the outermost peripheral edge 20 of the second wall surface 9. It has become.

また、第5図のように張出面11の端部近傍および第1
の壁面8近傍それぞれに誘電体カバー13から突き出し
た容量調整素子26.27を設け、かつ第1の壁面8近
傍の容量調整素子27の突出寸法をもう一方の容量調整
素子26よりも大きくしている。
In addition, as shown in FIG.
Capacitance adjusting elements 26 and 27 protruding from the dielectric cover 13 are provided near the first wall surface 8, respectively, and the protruding dimension of the capacitance adjusting element 27 near the first wall surface 8 is made larger than that of the other capacitance adjusting element 26. There is.

次に上記のように構成した実施例の作用効果を説明する
。加熱室1開口部を取り囲むフランジ2と封口面7との
平面接触部に向かう入射電波に対して、第4図のような
簡易等価回路によって定性的に電波シール効果を説明す
る。21は7ランジ2と封口面7との平面接触部に対応
する容量で、一種のバイパスコンデンサとして作用する
。平面接触部は平行板線路と考えられ、この線路の容量
は平行板のキャップに比例するので容量21は、上記平
面接触部のキャップが小さいほど大きくなり。
Next, the effects of the embodiment configured as described above will be explained. The radio wave sealing effect will be qualitatively explained using a simple equivalent circuit as shown in FIG. 4 with respect to the incident radio waves directed toward the planar contact portion between the flange 2 surrounding the opening of the heating chamber 1 and the sealing surface 7. 21 is a capacitor corresponding to the planar contact portion between the 7 flange 2 and the sealing surface 7, and acts as a type of bypass capacitor. The planar contact portion is considered to be a parallel plate line, and since the capacitance of this line is proportional to the cap of the parallel plate, the capacitance 21 becomes larger as the cap of the planar contact portion is smaller.

電波イール効果が増す。コ字状導体片10の幅D(第3
図のX方向)を使用波長の2分の1より小さくしている
ので、第1の壁面8と各コ字状導体片10とで形成され
た口字状断面を持つ空胴共振器12の内部に入り込んだ
電波の進行方向は第3図のyz面内に限定される。張出
面11が無ければ第6図のように電界が分布し、平行板
線路の長さtが自由空間波長λの約4分の1で並列共振
を起こし。
Increases radio wave effect. Width D of U-shaped conductor piece 10 (third
(X direction in the figure) is made smaller than half of the wavelength used, so the cavity resonator 12 with a cross section formed by the first wall surface 8 and each U-shaped conductor piece 10 is The traveling direction of the radio waves that have entered the interior is limited to the yz plane in FIG. If there is no overhanging surface 11, the electric field will be distributed as shown in FIG. 6, and parallel resonance will occur when the length t of the parallel plate line is approximately one-fourth of the free space wavelength λ.

インピーダンスが最大となり、電波漏洩を防止すること
ができるが、  2450MHzの高周波加熱装置では
tは3[13mmで、これをドアに実装しようとすると
厚くなり、意匠的にもコスト的にも不利である。
Impedance is maximized and radio wave leakage can be prevented, but t is 3 [13 mm] for a 2450 MHz high frequency heating device, and if you try to mount this on a door, it will be thick, which is disadvantageous in terms of design and cost. .

本実施例のように、張出面11を設けて1口字状断面を
持ち狭小な入口25を有する空胴共振器12を形成した
場合は、第5図のような電界分布となる。
In the case where the cavity resonator 12 having the protruding surface 11 and having a single-shaped cross section and a narrow entrance 25 is formed as in this embodiment, the electric field distribution will be as shown in FIG.

この場合、張出面11の端部切口付近と第1の壁面8と
の間に電気力線の大部分が集まっている。空胴共振器1
2は第4図において等価インダクタンスLと等価容量C
とから成る並列共振素子として表わされている。等価イ
ンダクタンスLは、近似的に空胴共振器12と同じ断面
の1巻きの筒状コイルとして働き、そのコイルの定数と
しての等測的なインダクタンスを意味し、筒軸方向(X
方向)の単位長あたりの値は(11式のよってなる。ま
た1等価容量Cは空胴共振器12の入口25付近の乱れ
電界に基づくもので、近似的に(2)式で与えられる。
In this case, most of the electric lines of force are concentrated between the vicinity of the end cut of the overhanging surface 11 and the first wall surface 8. Cavity resonator 1
2 is equivalent inductance L and equivalent capacitance C in Figure 4.
It is expressed as a parallel resonant element consisting of. The equivalent inductance L works as a one-turn cylindrical coil with approximately the same cross section as the cavity resonator 12, and means the isometric inductance as a constant of the coil, and is expressed in the cylindrical axis direction (X
The value per unit length of (direction) is given by Equation 11. The 1-equivalent capacitance C is based on the disturbed electric field near the entrance 25 of the cavity resonator 12, and is approximately given by Equation (2).

L=μoAB・・・・・・・・・・・・・・・・・・・
・・・・・・・・・・・・・・・・・・・・・・・・・
・・・・・・・・・・(1)ここで AB:空胴共振器12の口字状断面の面積μ0 :空胴
共振器12内の媒質の透磁率e  :  2.72 tM:空胴共振器12の入口25と空胴断面の面積中心
Oとの距離 ε0 :空胴共振器12内の媒質の誘宣率K :入口2
5付近の形状に関係する補正項G :入口25の間隙(
入口寸法) 空胴共振器12の共振周波数f。は(3)式で表わせる
L=μoAB・・・・・・・・・・・・・・・・・・
・・・・・・・・・・・・・・・・・・・・・・・・
・・・・・・・・・・・・(1) Here, AB: Area μ0 of the cross-section of the cavity resonator 12: Permeability e of the medium inside the cavity resonator 12: 2.72 tM: Air Distance ε0 between the entrance 25 of the cavity resonator 12 and the center of area O of the cavity cross section: Induction coefficient K of the medium inside the cavity resonator 12: Inlet 2
Correction term G related to the shape around 5: Gap at the entrance 25 (
(inlet dimensions) resonant frequency f of the cavity resonator 12; can be expressed by equation (3).

(2)式より入口25の間隙Gを小さくするほど、ある
ことかわかる。共振周波数foを一定とすると。
From equation (2), it can be seen that the smaller the gap G of the inlet 25 is, the more this is true. Assuming that the resonant frequency fo is constant.

等価容量Cが大きくなるほど等価インダクタンスLが小
さくてよいことが(3)式かられかる。等価インダクタ
ンスLを小さくするには(11式より空胴共振器12の
口字状断面の面積ABを小さくすればよい。すなわち、
空胴共振器12を小形にするためにけ、入口25の間隙
Gを狭くして等価容量Cを太きくシ、その分だけ空胴面
積ABを小さくして等価インダクタンスLを小さくシ、
一定の共振周波数to (高周波加熱装置の加熱周波数
)で並列共振を起こさせて、入口25におけるインピー
ダンスヲ最大にし電波漏洩を防止すればよい。
It can be seen from equation (3) that the larger the equivalent capacitance C is, the smaller the equivalent inductance L is. In order to reduce the equivalent inductance L (from equation 11, the area AB of the mouth-shaped cross section of the cavity resonator 12 should be made smaller; that is,
In order to make the cavity resonator 12 smaller, the gap G of the inlet 25 is narrowed to increase the equivalent capacitance C, and the cavity area AB is correspondingly decreased to decrease the equivalent inductance L.
Parallel resonance may be caused at a certain resonance frequency to (heating frequency of the high-frequency heating device) to maximize the impedance at the inlet 25 and prevent radio wave leakage.

加熱周波数が2.450 MHz 、高周波出力が50
0Wの高周波加熱装置において、7ランジ2と封口面7
との間の間隙を2間、張出面11と封口面7との段差を
3調、コ字状導体片の幅りを15朋とし、水275m1
を加熱してドア5の周囲から50の距離で電波漏洩量を
測定してみた。その結果、G=5mmy−一 のときAB = 15.4 X 15.9咽、−2,1
で、電波漏洩量が0.1 m W//cA以下となり、
G=Bwmと犬きくすると、上記と同程度に少ない電波
漏洩量に抑えるためにはAB = 20.4 X 18
.4閣、ム=1.75というように口字状断面の面積も
大きくなる。このような実、験により、入口25の間隙
Gを4m8惰位と狭M 小にして了をt5以上にすることにより1口字状断面の
空胴共振器12の寸法Aおよび寸法Bをそれぞれ使用波
長λの4分の1である30.6mよりもかなり小さくで
きることが明らかとなっている。
Heating frequency is 2.450 MHz, high frequency output is 50 MHz
In a 0W high frequency heating device, 7 langes 2 and sealing surface 7
The gap between
I heated it and measured the amount of radio wave leakage at a distance of 50 degrees from the periphery of the door 5. As a result, when G = 5mmy-1, AB = 15.4 x 15.9mm, -2,1
Therefore, the amount of radio wave leakage is less than 0.1 mW//cA,
If we assume that G = Bwm, in order to suppress the amount of radio wave leakage to the same level as above, AB = 20.4 x 18
.. The area of the kuji-shaped cross section also becomes larger, as in the case of 4 kakus, mu = 1.75. Through these actual experiments, the dimensions A and B of the cavity resonator 12 with a single-shaped cross section can be respectively reduced by narrowing the gap G of the inlet 25 to 4 m8 and making the gap t5 or more. It has become clear that the wavelength can be made considerably smaller than 30.6 m, which is one quarter of the wavelength λ used.

また、容量調整素子26.27により等価容量Cを調整
して、並列共振を確実に生じるようにし、電波シール効
果を増す。さらに、第1の壁面8近傍の容量調整素子2
7の方が張出面11の端部近傍の容量調整素子26より
突出寸法が長いので、誘電体カバー15をはめこむとき
、まず容量調整素子27が第1の壁面8に沿って挿入さ
れ9位置決めされた後で、容量調整素子26が入口25
に入っていく。したがって容量調整素子26が張出面1
1をy方向から押して変形する恐れがない。なお容量調
整素子26は誘電体カバー13の固着状態において、Z
方向からの外力に対して張出面11の変形を最小限に抑
える役目も果たしている。
Further, the equivalent capacitance C is adjusted by the capacitance adjustment elements 26 and 27 to ensure parallel resonance and increase the radio wave sealing effect. Furthermore, the capacitance adjustment element 2 near the first wall surface 8
7 has a longer protruding dimension than the capacitance adjustment element 26 near the end of the projecting surface 11, so when the dielectric cover 15 is fitted, the capacitance adjustment element 27 is first inserted along the first wall surface 8 and the 9 positioning is performed. After the capacitance adjustment element 26 is connected to the inlet 25
going into. Therefore, the capacitance adjustment element 26
There is no risk of deformation by pushing 1 from the y direction. Note that the capacitance adjustment element 26 has a Z value when the dielectric cover 13 is fixed.
It also plays the role of minimizing deformation of the projecting surface 11 against external forces from directions.

発明の効果 以上のようンて本発明によると、多数のコ字状導体片と
第1の壁面とで囲まれた口字状断面の空胴共振器の入口
をコ字状導体片の張出面の端部切口と第1の壁面を対向
させた構成で狭小なものとし。
Effects of the Invention As described above, according to the present invention, the entrance of a cavity resonator having a square cross section surrounded by a large number of U-shaped conductor pieces and the first wall surface is connected to the overhanging surface of the U-shaped conductor piece. The end cut and the first wall face each other and are narrow.

e≧i、5のように寸法を選び、2個の容量調整素子に
よって並列共振をより確実に生じるようにすることによ
り空胴共振器の断面寸法AおよびBを使用波長λの4分
の1よりも小さくできるので。
By selecting the dimensions such that e≧i, 5, and ensuring that parallel resonance is generated by the two capacitance adjustment elements, the cross-sectional dimensions A and B of the cavity resonator can be reduced to a quarter of the wavelength λ used. Because it can be made smaller than.

共振空胴器の形状が簡単となり、ドアの小形化。The shape of the resonant cavity is simplified, making the door more compact.

薄形化が図れ9組立容易なコンパクトな高周波加熱装置
を提供でき、経済的波及効果も大なるものがある。
It is possible to provide a compact high-frequency heating device that is thin, easy to assemble, and has a large economic impact.

【図面の簡単な説明】[Brief explanation of the drawing]

第1図は本発明の一実施例による高周波加熱装置のドア
5の金属部だけを示す要部斜視図、第2図は同ドア周囲
の電波シール部を示す要部断面図。 第3図は同電界方向を示す図、第4図はドア5の電波シ
ール部の簡易等価回路図、第5図は同電波シール部の電
界分布図、第6図は同終端を短絡した平行板線路の電界
分布図、第7図は従来の電波シール構造を示す構成説明
図、第8図は同電界方向を示す図である。 1・・・加熱室  2・・・フランジ  4・・・小穴
群5・・・ドア   6・・・段部    7・・・封
口面8・・・第1の壁面  9・・・第2の壁面10・
・・コ字状導体片  11・・・張出面12・・・空胴
共振器  13・・・誘電体カバー19・・・取り付け
面  23・・・立ち上がり面25・・・入口  26
 、27・・・容量調整素子AM・・・空胴共振器12
の入口25と空胴断面の面積中心Oとの距離 G・・・入口寸法
FIG. 1 is a perspective view of a main part showing only the metal part of a door 5 of a high-frequency heating device according to an embodiment of the present invention, and FIG. 2 is a sectional view of a main part showing a radio wave seal part around the door. Fig. 3 is a diagram showing the direction of the electric field, Fig. 4 is a simplified equivalent circuit diagram of the radio wave seal part of the door 5, Fig. 5 is an electric field distribution diagram of the radio wave seal part, and Fig. 6 is a parallel diagram with the same termination short-circuited. An electric field distribution diagram of a board line, FIG. 7 is a configuration explanatory diagram showing a conventional radio wave seal structure, and FIG. 8 is a diagram showing the direction of the electric field. DESCRIPTION OF SYMBOLS 1... Heating chamber 2... Flange 4... Small hole group 5... Door 6... Step part 7... Sealing surface 8... First wall surface 9... Second wall surface 10・
... U-shaped conductor piece 11 ... Overhanging surface 12 ... Cavity resonator 13 ... Dielectric cover 19 ... Mounting surface 23 ... Rising surface 25 ... Inlet 26
, 27...Capacitance adjustment element AM...Cavity resonator 12
Distance G between the inlet 25 and the center of area O of the cavity cross section...Inlet dimension

Claims (1)

【特許請求の範囲】[Claims] 加熱室(1)開口部を開閉するドア(5)の周縁に位置
し、ドア(5)閉成時には加熱室(1)開口部のフラン
ジ(2)に平面接触する封口面(7)と、この封口面(
7)の端部よりフランジ(2)に対して略直角の第1の
壁面(8)と、この第1の壁面(8)と略直角の第2の
壁面(9)と、この第2の壁面(9)と略直角の立ち上
がり面(23)と、この立ち上がり面(26)と略直角
の張出面(11)とを備えた高周波加熱装置において、
第2の壁面(9)に端面が接した多数のコ字状導体片(
10)を設け、第1の壁面(8)とコ字状導体片(10
)とによりロ字状断面を持つと共に入口(25)を有す
る空胴共振器(12)を形成し、かつ入口(25)と空
胴断面の面積中心Oの距離lMと、入口寸法Gとの比l
M/Gを1.5以上とし第1の壁面(8)に向かって張
り出したコ字状導体片(10)の張出面(11)の端部
近傍および第1の壁面(8)近傍それぞれに入口(25
)をふさぐ誘電体カバー(13)から突き出した容量調
整素子(26)、(27)を設け、かつ第1の壁面(8
)近傍の容量調整素子(27)の突出寸法をもう一方の
容量調整素子(26)よりも大きくし、コ字状導体片(
10)は第2の壁面(9)に接する取り付け面(19)
と、第1の壁面(8)にほぼ平行に対向する立ち上がり
面(23)と、端部切口を第1の壁面(8)に対向させ
た張出面(11)との3面から成り、空胴共振器(12
)の入口(25)は張出面(11)の端部切口と第1の
壁面(8)を対向させて形成したことを特徴とする高周
波加熱装置。
a sealing surface (7) located at the periphery of a door (5) that opens and closes the opening of the heating chamber (1), and which makes plane contact with the flange (2) of the opening of the heating chamber (1) when the door (5) is closed; This sealing surface (
7), a first wall surface (8) substantially perpendicular to the flange (2), a second wall surface (9) substantially perpendicular to this first wall surface (8), and a second wall surface (9) substantially perpendicular to this first wall surface (8); In a high-frequency heating device including a rising surface (23) substantially perpendicular to the wall surface (9) and an overhanging surface (11) substantially perpendicular to the rising surface (26),
A large number of U-shaped conductor pieces (
10), and the first wall surface (8) and the U-shaped conductor piece (10
) forms a cavity resonator (12) having a square-shaped cross section and an inlet (25), and the distance lM between the inlet (25) and the center of area O of the cavity cross section and the inlet dimension G comparison
M/G is 1.5 or more, and near the end of the projecting surface (11) of the U-shaped conductor piece (10) projecting toward the first wall surface (8) and near the first wall surface (8), respectively. Entrance (25
) are provided with capacitance adjustment elements (26) and (27) protruding from the dielectric cover (13) that blocks the first wall (8).
) The protruding dimension of the capacitance adjustment element (27) near the other capacitance adjustment element (26) is made larger than that of the other capacitance adjustment element (26), and the U-shaped conductor piece (
10) is the mounting surface (19) in contact with the second wall surface (9)
It consists of three surfaces: a rising surface (23) facing substantially parallel to the first wall surface (8), and an overhanging surface (11) with an end cut facing the first wall surface (8). Body resonator (12
) The inlet (25) of the high-frequency heating device is characterized in that the end cut of the projecting surface (11) and the first wall surface (8) are opposed to each other.
JP61215365A 1986-08-07 1986-09-12 Radio frequency heater Granted JPS6372089A (en)

Priority Applications (6)

Application Number Priority Date Filing Date Title
JP61215365A JPS6372089A (en) 1986-09-12 1986-09-12 Radio frequency heater
GB8718229A GB2196520B (en) 1986-08-07 1987-07-31 Microwave heating apparatus
DE19873726002 DE3726002A1 (en) 1986-08-07 1987-08-05 DOOR GASKET FOR A MICROWAVE OVEN
KR1019870008619A KR900008074B1 (en) 1986-08-07 1987-08-06 Microwave sealing device
US07/082,471 US4868359A (en) 1986-08-07 1987-08-07 Radiation sealed door in a microwave heating apparatus
FR8711322A FR2602626B1 (en) 1986-08-07 1987-08-07 ELECTROMAGNETIC SEAL FOR MICROWAVE HEATING DEVICE DOOR, AND HEATING DEVICE HAVING SUCH AN ARRANGEMENT

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP61215365A JPS6372089A (en) 1986-09-12 1986-09-12 Radio frequency heater

Publications (2)

Publication Number Publication Date
JPS6372089A true JPS6372089A (en) 1988-04-01
JPH0569276B2 JPH0569276B2 (en) 1993-09-30

Family

ID=16671083

Family Applications (1)

Application Number Title Priority Date Filing Date
JP61215365A Granted JPS6372089A (en) 1986-08-07 1986-09-12 Radio frequency heater

Country Status (1)

Country Link
JP (1) JPS6372089A (en)

Citations (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS50142546U (en) * 1974-05-13 1975-11-25
JPS59230291A (en) * 1983-06-07 1984-12-24 松下電器産業株式会社 Radio wave sealing device
JPS6033596U (en) * 1983-08-12 1985-03-07 日立建機株式会社 Boom proximity warning device
JPS61160997A (en) * 1985-01-08 1986-07-21 松下電器産業株式会社 Radio wave sealing apparatus

Patent Citations (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS50142546U (en) * 1974-05-13 1975-11-25
JPS59230291A (en) * 1983-06-07 1984-12-24 松下電器産業株式会社 Radio wave sealing device
JPS6033596U (en) * 1983-08-12 1985-03-07 日立建機株式会社 Boom proximity warning device
JPS61160997A (en) * 1985-01-08 1986-07-21 松下電器産業株式会社 Radio wave sealing apparatus

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