JPS6345794A - Radio frequency heater - Google Patents

Radio frequency heater

Info

Publication number
JPS6345794A
JPS6345794A JP18927686A JP18927686A JPS6345794A JP S6345794 A JPS6345794 A JP S6345794A JP 18927686 A JP18927686 A JP 18927686A JP 18927686 A JP18927686 A JP 18927686A JP S6345794 A JPS6345794 A JP S6345794A
Authority
JP
Japan
Prior art keywords
wall surface
cavity resonator
door
inlet
cavity
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.)
Pending
Application number
JP18927686A
Other languages
Japanese (ja)
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 JP18927686A priority Critical patent/JPS6345794A/en
Publication of JPS6345794A publication Critical patent/JPS6345794A/en
Pending legal-status Critical Current

Links

Landscapes

  • Constitution Of High-Frequency Heating (AREA)

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、チミ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60−25
190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。
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 is reduced to a quarter of the wavelength used. A proposal was made in JP-A-60-25 that even if the value is smaller than 1, the impedance at the entrance of the groove is maximized, and leakage radio waves can be reduced in the same way as the Chimique groove.
It is in Publication No. 190. 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.

また、第7図で示すように、l−′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、空調共振器12の一周壁である張8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
公報に示さ些ている。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れていることは記載されて
いない、したがって空胴共振器12内には第8図に示す
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の立上り面23と張出面11を長手方向(X方向
)に使用波長の1/2より小さい幅の導体片に分割した
と考える。この場合、空胴共振器12を等価容tc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と空胴断面の面積中心0の距
離QMと、入口寸法Gとの比AM/G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am
/G=1.0で、後述する本発明のQx/G≧1.5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1
2の断面ABを大きくする必要があるので。
In addition, as shown in FIG. 7, a cavity resonator 12 for preventing radio wave leakage is bent on the outer periphery of the l-'a 5 to have a cross-section shaped like an opening. A structure having an inlet 25 in which the end cut of the surface 11 and the other wall surface (first wall surface 8) of the cavity resonator 12 are opposed to each other is shown in Japanese Utility Model Application Publication No. 61-795. In this conventional example, there is no description that the peripheral wall of the cavity resonator 12 is divided into a plurality of conductor pieces.Therefore, inside the cavity resonator 12, the traveling direction shown in FIG. Since the generated higher-order mode radio waves enter, the cavity resonator 12 is removed from the resonant state, and the radio wave leakage prevention effect is reduced. Assume that the rising surface 23 and the projecting surface 11 of the cavity resonator 12 shown in FIG. 7 are divided into conductor pieces having a width smaller than 1/2 of the wavelength used in the longitudinal direction (X direction). In this case, the cavity resonator 12 can be regarded as a plurality of parallel resonant elements each having an equivalent capacitance tc 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,
The larger the ratio AM/G between the distance QM between the entrance 25 of the cavity resonator 12 and the center of area 0 of the cavity cross section and the entrance dimension G, the larger the equivalent capacitance C becomes. In the cavity resonator 12 of FIG.
When /G=1.0, the equivalent capacitance C becomes smaller than when Qx/G≧1.5 of the present invention, which will be described later. For that reason, see (3) below.
) According to the equation, 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 1
Because it is necessary to increase the cross section AB of 2.

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。
The cavity resonator 12 of the conventional example is large, and the door is made smaller.
It is not suitable for cost reduction.

なお、第7図は実開昭61−795号公報の明細書の図
面の各部首法を同一比率で示したものであり、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。
In addition, FIG. 7 shows each radical in the drawings of the specification of Utility Model Publication No. 61-795 in the same proportion, and the names and numbers of the constituent elements are the same as those in the present invention. It's Nishide.

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 a groove with a complicated shape in the depth direction of the groove, and it takes time and effort to prevent reflections at discontinuous parts of the characteristic impedance, and it is not suitable for downsizing the door. It is a point.

問題点を解決するための手段 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、こ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き入れる
入口を設け、かつこの入口と空胴断面の面積中心の距離
QMと、入口寸法Gとの比12M/Gを1.5以上とし
、入口に容量調整素子を設けたものである。
Means for solving the problem: A cavity resonator with a square-shaped cross section for preventing leakage radio waves was installed around the door, and a part of the wall of this cavity resonator was formed with a large number of U-shaped conductor pieces. In addition, an inlet is provided in the cavity resonator to introduce leakage radio waves, and the ratio 12M/G between the distance QM between this inlet and the center of area of the cross section of the cavity and the inlet dimension G is set to be 1.5 or more, and a capacitance is provided at the inlet. It is equipped with an adjustment element.

作用 上記のように構成することによ、す、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
空胴共振器内に導き入れられる。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容量素子を設けると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0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。     。
Operation With the above configuration, radio waves that are about to leak through the U-shaped conductor piece are introduced into the cavity resonator with the square-shaped cross section as TEM waves. 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 a capacitive element is provided, C becomes larger, and L can be made smaller by that amount. That is, the radio wave sealing effect is maximized when each side of the 0-shaped cross section, which can reduce the cross-sectional area of the cavity, is smaller than one-fourth 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作
用を図面とともに説明する。
Embodiment The structure and operation 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、第2図において、1は加熱室で、2は加熱室1
の開口部を取り囲むフランジで、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。
In Figures 1 and 2, 1 is a heating chamber, and 2 is a heating chamber 1.
3 is the 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.

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6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。
Reference numeral 6 denotes a step surrounding this small hole group 4;
is a translucent door cover 15 fixed to the inner surface of the small hole group 4.
This prevents the end portion of the door from being peeled off during cleaning, etc., and improves the flatness of the sealing surface 7 that makes plane contact with the flange 2 when the door 5 is closed.

8は封口面7の端部よりフランジ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に対して略平行に延長した第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
れる取り付は面19と、第1の壁面8にほぼ平行に対向
する立ち害がり面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。
Reference numeral 8 denotes a first wall surface bent from the end of the sealing surface 7 at a substantially right angle to the flange 2. Reference numeral 9 denotes a second wall surface extending substantially parallel to the flange 2 from the end of the first wall surface 8. 10 is a large number of U-shaped conductor pieces welded to the second wall surface 9. This U-shaped conductor piece 10 has a mounting surface 19 which is welded to the second wall surface 9, a standing edge surface 23 that faces substantially parallel to the first wall surface 8, and an end cut that is attached to the first wall surface. 8 and an overhanging surface 11 facing each other. Width D of each U-shaped conductor piece 10 in the longitudinal direction around the door 5 (X direction)
is 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に設けた取り付は穴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16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。また、誘
電体カバー13の裏面から空胴共振器12の内部に向か
って容量調整素子26を突き出している。
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 the opaque dielectric cover 13 that blocks the entrance 25 of the cavity resonator 12 is attached to a hole 18 provided on the 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 16 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. Further, a capacitance adjustment element 26 protrudes from the back surface of the dielectric cover 13 toward the inside of the cavity resonator 12.

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関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質に電波シール効果を説明す
る。21はフランジ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
は平行板のギャップに比例するので容量21は上記平面
接触部のギ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 incident radio waves directed toward the planar contact portion between the flange 2 surrounding the entrance portion of the heating chamber 1 and the sealing surface 7. 21 is a capacitor corresponding to the planar contact portion between the 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 the capacity of this line is proportional to the gap between the parallel plates, so the capacitance 21 becomes larger as the gap of the planar contact portion is smaller.

電波シール効果が増す、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
線路の長さ党が自由空間波長λの約4分の1で並列共振
を起こし、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Qは30.61m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。
The width D (third width) of the U-shaped conductor piece 10 increases the radio wave sealing effect.
(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 Figure 6, and the length of the parallel plate line will cause parallel resonance at about one-fourth of the free space wavelength λ, and the impedance will be maximum, preventing radio wave leakage. However, in the case of a 2450 MHz high frequency heating device, the Q is 30.61 m, and if it is attempted to be mounted on a door, it will be thick, which is disadvantageous both in terms of design and cost.

本発明のように、張出面11を設けて、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。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12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
共振素子として表されている0等価インダクタンスLは
When the cavity resonator 12 is formed by providing the projecting surface 11 and having a mouth-shaped cross section and a narrow entrance 25 as in the present invention, an electric field distribution as shown in FIG. 5 is obtained. 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. The cavity resonator 12 is represented in FIG. 4 as a parallel resonant element consisting of an equivalent inductance L and an equivalent capacitance C, where the equivalent inductance L is 0.

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(1)式のようになる。
It 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 the value per unit length in the cylinder axis direction (X direction) is It becomes as shown in equation (1).

また、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
Further, the 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).

1=、。AB            ・・・(1)こ
こで AB:空胴共振器12の口字状断面の面積μ。:空胴共
振器12内の媒質の透磁率e:2.72 ΩM:空胴共振器12の入口25と空胴断面の面積中心
0との距離 ε。:空胴共振器12内の媒質の誘電率に:入口25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f0は(3)式で表せる。
1=. AB... (1) where AB: area μ of the mouth-shaped cross section of the cavity resonator 12. : Permeability e of the medium in the cavity resonator 12: 2.72 ΩM: Distance ε between the entrance 25 of the cavity resonator 12 and the center of area 0 of the cavity cross section. : To the permittivity of the medium in the cavity resonator 12 : A correction term related to the shape of the vicinity of the inlet 25 G : Gap of the inlet 25 (inlet dimension) The resonant frequency f0 of the cavity resonator 12 can be expressed by equation (3). .

(η式より入口25の間隙Gを小さくするほど、あるい
はlM/Gを大きくするほど等価容量Cが大きくなるこ
とがわかる。共振周波数f、を一定とすると、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0等価インダクタンスLを
小さくするには(1)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は、入口25の間隙すを狭く
して等価容量Cを大きくし、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。
(From the η equation, it can be seen that the smaller the gap G of the inlet 25 or the larger lM/G, the larger the equivalent capacitance C becomes.If the resonant frequency f is constant, the larger the equivalent capacitance C is, the more the equivalent inductance L It can be seen from equation (3) that the zero equivalent inductance L can be reduced by reducing the area AB of the mouth-shaped cross section of the cavity resonator 12 from equation (1), that is, the cavity In order to make the resonator 12 smaller, the gap between the inlet 25 is narrowed to increase the equivalent capacitance C, and the cavity area AB is correspondingly reduced to reduce the equivalent inductance L.

一定の共振周波数f、C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
ンスを最大にし電波漏洩を防止すればよい。
Constant resonance frequency f, C heating frequency of high frequency heating device)
Parallel resonance may be caused in the inlet 25 to maximize the impedance at the inlet 25 to prevent radio wave leakage.

加熱周波数が2450MHz、高周波出力が500wの
高周波加熱装置において、フランジ2と封口面7との間
の間隙を2m!+、張出面11と封口面7との段差を3
m、コ字状導体片の幅りを15mmとし、水275 m
 Qを加熱してドア5の周囲から5afiの距離で電波
漏洩量を測定してみた。その結果、G=5mmのときA
 B = 15 、4 X 15 、9 m、fix/
G=2.1で、電波漏洩量がO,1mw/d以下となり
、G=8mmと大きくすると、上記と同程度に少ない電
波漏洩量に抑えるためにはAB=20.4X18.4+
a、QM/G=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4〜8LII11位と狭小にしてfiM/Gを1.
5以上にすることにより、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30.6−よりもかなり小さくできることが明ら
かとなっている。
In a high-frequency heating device with a heating frequency of 2450 MHz and a high-frequency output of 500 W, the gap between the flange 2 and the sealing surface 7 is 2 m! +, the difference in level between the protruding surface 11 and the sealing surface 7 is 3
m, the width of the U-shaped conductor piece is 15 mm, and the water is 275 m.
I heated the Q and measured the amount of radio wave leakage at a distance of 5afi from around the door 5. As a result, when G=5mm, A
B = 15, 4 x 15, 9 m, fix/
When G = 2.1, the amount of radio wave leakage is less than O,1 mw/d, and if G = 8 mm, in order to suppress the amount of radio wave leakage to the same small amount as above, AB = 20.4 x 18.4 +
a, QM/G=1.75, so the area of the mouth-shaped cross section also increases. Through such experiments, the gap G of the inlet 25 was narrowed to about 4 to 8 LII11, and fiM/G was reduced to 1.
By setting the number to 5 or more, the cavity resonator 12 with a cross-sectional shape
Dimension A and dimension B of are each a quarter of the wavelength λ used.
It has become clear that it can be made considerably smaller than 30.6-.

また、誘電体カバー13の裏面から空胴共振器12の内
部に向かって容量調整素子26を突き出しているので、
入口25の電気力線の集中したところへ誘電体が挿入さ
れることになるので、等価容量Cが大きくなり、その分
だけ等価インダクタンスLが小さくてよい。すなわち容
量調整素子26を設けることにより、空胴共振器12を
一層小形化できるようになる。
Furthermore, since the capacitance adjustment element 26 protrudes from the back surface of the dielectric cover 13 toward the inside of the cavity resonator 12,
Since the dielectric is inserted into the inlet 25 where the lines of electric force are concentrated, the equivalent capacitance C increases, and the equivalent inductance L can be reduced accordingly. That is, by providing the capacitance adjustment element 26, the cavity resonator 12 can be further downsized.

発明の効果 以上のように本発明によると、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、かつ2M / G≧1.5
のように寸法を選び、かつ誘電体カバーの裏面から空胴
共振器の内部に向がって容量調整素子を突き出すように
したので、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、共振空胴器の形状が簡
単となり、ドアの小形化、薄形化が図れ、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。
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 projecting surface of the U-shaped conductor piece. The end cut and the first wall face each other to make it narrow, and 2M/G≧1.5.
Since we selected the dimensions as shown below and made the capacitance adjustment element protrude from the back side of the dielectric cover toward the inside of the cavity resonator, we determined that the cross-sectional dimensions A and B of the cavity resonator correspond to the wavelength λ used. It can be made smaller than one quarter, the shape of the resonant cavity is simple, the door can be made smaller and thinner, a compact high frequency heating device can be provided, and the economic ripple effect is also large.

【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。
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, FIG. 2 is a cross-sectional view of a main part showing a radio wave seal around the door, and FIG. Figure 4 is a simplified equivalent circuit diagram of the radio wave seal part of the door 5, Figure 5 is an electric field distribution diagram of the radio wave seal part, and Figure 6 is the electric field of the parallel plate line with the same termination short-circuited. A distribution diagram, 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.

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(23)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(1
0)を設け、第1の壁面(8)とコ字状導体片(10)
とにより口字状断面を形成すると共に入口(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(l_M)と、入口寸
法(G)との比l_M/Gを1.5以上とし、かつ入口
(25)をふさぐ誘電体カバー(13)の裏面から空胴
共振器(12)の内部に向かって容量調整素子(26)
を突き出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 the door (5) that opens and closes the opening of the heating chamber (1) and in planar contact with the flange (2) of the opening of the heating chamber (1) when the door (5) is closed; Sealing side (7
), a first wall surface (8) substantially perpendicular to the flange (2), a second wall surface (9) substantially perpendicular to the first wall surface (8), and a second wall surface (9) substantially perpendicular to the first wall surface (8); (9), a rising surface (23) substantially perpendicular to the rising surface (23), and a projecting surface (11) substantially perpendicular to the high-frequency heating device, the end surface of which is in contact with the second wall surface (9). Many U-shaped conductor pieces (1
0), and the first wall surface (8) and the U-shaped conductor piece (10)
A cavity resonator (12) having a mouth-shaped cross section and an inlet (25) is formed by and, and the distance (l_M) between the inlet (25) and the center of area (O) of the cavity cross section, and the inlet. The ratio l_M/G with the dimension (G) is 1.5 or more, and the capacitance adjustment element (26 )
A high-frequency heating device characterized by protruding.
JP18927686A 1986-08-12 1986-08-12 Radio frequency heater Pending JPS6345794A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP18927686A JPS6345794A (en) 1986-08-12 1986-08-12 Radio frequency heater

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP18927686A JPS6345794A (en) 1986-08-12 1986-08-12 Radio frequency heater

Publications (1)

Publication Number Publication Date
JPS6345794A true JPS6345794A (en) 1988-02-26

Family

ID=16238607

Family Applications (1)

Application Number Title Priority Date Filing Date
JP18927686A Pending JPS6345794A (en) 1986-08-12 1986-08-12 Radio frequency heater

Country Status (1)

Country Link
JP (1) JPS6345794A (en)

Similar Documents

Publication Publication Date Title
US4254318A (en) Door seal arrangement for high-frequency heating apparatus
US4868359A (en) Radiation sealed door in a microwave heating apparatus
JPS6345794A (en) Radio frequency heater
JP2717401B2 (en) High frequency heating equipment
JPS6345793A (en) Radio frequency heater
JPS6345795A (en) Radio frequency heater
JPS6343287A (en) Radio frequency heater
JP2673347B2 (en) High frequency heating equipment
JPS6345791A (en) Radio frequency heater
JPS6345792A (en) Radio frequency heater
JPS6380496A (en) Radio frequency heater
JPS6372090A (en) Radio frequency heater
JPS6372095A (en) Radio frequency heater
JPS6372089A (en) Radio frequency heater
JPH10241855A (en) Microwave oven door
JPH08316679A (en) Electromagnetic shielding box and electric equipment having this case
JPS6343288A (en) Radio frequency heater
JPS6372094A (en) Radio frequency heater
JPS62249386A (en) Radio frequency heater
JPS6372092A (en) Radio frequency heater
JPS6372093A (en) Radio frequency heater
JPS62249389A (en) Radio frequency heater
JPS6372091A (en) Radio frequency heater
JPS62249388A (en) Radio frequency heater
JPS6343291A (en) Radio frequency heater