JPS6262435B2 - - Google Patents
Info
- Publication number
- JPS6262435B2 JPS6262435B2 JP16446681A JP16446681A JPS6262435B2 JP S6262435 B2 JPS6262435 B2 JP S6262435B2 JP 16446681 A JP16446681 A JP 16446681A JP 16446681 A JP16446681 A JP 16446681A JP S6262435 B2 JPS6262435 B2 JP S6262435B2
- Authority
- JP
- Japan
- Prior art keywords
- groove
- door
- radio wave
- heating chamber
- chiyoke
- 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.)
- Expired
Links
Classifications
-
- H—ELECTRICITY
- H05—ELECTRIC TECHNIQUES NOT OTHERWISE PROVIDED FOR
- H05B—ELECTRIC HEATING; ELECTRIC LIGHT SOURCES NOT OTHERWISE PROVIDED FOR; CIRCUIT ARRANGEMENTS FOR ELECTRIC LIGHT SOURCES, IN GENERAL
- H05B6/00—Heating by electric, magnetic or electromagnetic fields
- H05B6/64—Heating using microwaves
- H05B6/76—Prevention of microwave leakage, e.g. door sealings
- H05B6/763—Microwave radiation seals for doors
Landscapes
- Physics & Mathematics (AREA)
- Electromagnetism (AREA)
- Constitution Of High-Frequency Heating (AREA)
- Shielding Devices Or Components To Electric Or Magnetic Fields (AREA)
Description
【発明の詳細な説明】
本発明は高周波エネルギーによつて食品などの
被加熱物を加熱処理する高周波加熱装置に係り、
特に電波漏洩防止用チヨーク溝を備えたドアに関
するものである。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a high-frequency heating device that heats an object to be heated such as food using high-frequency energy.
In particular, the present invention relates to a door equipped with a chiyoke groove for preventing radio wave leakage.
従来、IC、マイコンなど小形で多機能を持つ
電子部品が高周波加熱装置の制御回路に積極的に
とり入れられ、操作パネルの小形化、薄形化が進
んでおり、こういつた操作パネルと釣合のとれた
薄形ドアが要望されている。また複雑な操作を自
動化する傾向が多くなつており、電子回路関係に
コストが掛かるようになつてきているので、機械
部品特にドア構造の低コスト化が要望されてい
る。 Conventionally, small, multifunctional electronic components such as ICs and microcomputers have been actively incorporated into the control circuits of high-frequency heating equipment, and operation panels have become smaller and thinner, making it difficult to balance these types of operation panels. A thin door with a flat profile is requested. In addition, there is a growing tendency to automate complex operations, which increases the cost of electronic circuits, so there is a demand for lower costs for mechanical parts, especially door structures.
従来のドアとしては、チヨーク溝と電波吸収材
のフエライトを併用したものが多いが、フエライ
トをドア全周にとりつけるためコスト的に不利で
あつた。さらにチヨーク溝自体の減衰効果を増
し、フエライトを除去しようとする提案がなされ
ている。この提案は次に述べる通りである。 Conventional doors often use a combination of chiyolk grooves and ferrite, which is a radio wave absorbing material, but this is disadvantageous in terms of cost because ferrite is attached to the entire circumference of the door. Furthermore, proposals have been made to increase the damping effect of the chiyoke groove itself and to remove ferrite. This proposal is as follows.
使用波長λの1/4の深さを持つチヨーク溝の一
面をλ/4の長さの導体片、いわゆるスリツトを周
期的に並べて電波伝搬方向規制装置として、チヨ
ーク溝の減衰効果を増す提案が米国特許2772402
(1956・11・27特許)や同2850706(1958・9・2
特許)においてなされている。又、上記特許と同
様な電波漏洩防止構造が同3767884(日本特開昭
48−81146、日本特公昭53−4660)に提案されて
いるが、この提案ではスリツト(スロツト)がチ
ヨーク溝に入る前の電波伝搬経路の一面となつて
おり、スリツトと対向する金属面との間隔を誘電
体を充てんすることにより強制的にとつている方
式である。これはスリツトが部分的に対向金属面
を接触すると実質的にスリツトの長さがλ/4より
短かくなり、電波伝搬方向規制装置(電磁エネル
ギーモード維持構造物)としての作用が低下する
ためである。この方式ではドアと加熱室開口部周
縁の隙間に入射する電波が多くなり、基本波およ
び高調波の漏洩を防止するには導電性ゴムを追加
したり、漏洩電波の伝搬経路を複雑にして大きな
減衰効果を出す必要があり、ドアの薄形化、低コ
スト化には不向きである。 A proposal has been made to increase the attenuation effect of the chiyoke groove by periodically arranging λ/4 length conductor pieces, so-called slits, on one side of the chiyoke groove, which has a depth of 1/4 of the used wavelength λ, as a radio wave propagation direction regulating device. US Patent 2772402
(1956/11/27 patent) and 2850706 (1958/9/2 patent)
patent). In addition, the radio wave leakage prevention structure similar to the above patent is patented in 3767884 (Japanese Unexamined Patent Publication No. 3767884).
48-81146, Japan Patent Publication Publication No. 53-4660), but in this proposal, the slit is one side of the radio wave propagation path before entering the chiyoke groove, and the slit and the opposing metal surface are This is a method in which the spacing is forcibly maintained by filling it with dielectric material. This is because when the slit partially contacts the opposing metal surface, the length of the slit becomes substantially shorter than λ/4, which reduces its function as a radio wave propagation direction regulating device (electromagnetic energy mode maintenance structure). be. With this method, a large number of radio waves enter the gap between the door and the heating chamber opening, and to prevent leakage of fundamental waves and harmonics, it is necessary to add conductive rubber or to complicate the propagation path of leaked radio waves. It is necessary to produce a damping effect, and it is not suitable for making doors thinner and lower in cost.
また、約λ/4のスリツトを有する金属壁でチヨ
ーク溝を二つに分割して減衰効果を増すことが英
国特許1392498、日本特公昭51−22663等多数提案
されているが、この方式では実質的にチヨーク溝
が大形化し、ドアの薄形化、低コスト化には不向
きである。 In addition, many proposals have been made, such as British Patent No. 1392498 and Japanese Patent Publication No. 1983-22663, to increase the damping effect by dividing the choke groove into two with a metal wall having a slit of approximately λ/4, but this method does not However, the yoke groove becomes large, making it unsuitable for making doors thinner and lower in cost.
さらに、チヨーク溝内に上記のようなスリツト
でない別の周期構造体を入れたものが、日本特公
昭54−21574、日本特公昭52−40461に提案されて
いるが、チヨーク溝を形成する面そのものでなく
別のものを追加する必要があり、さらに高調波に
対しては考慮されていないので、実用にするため
にはフエライト等の追加も必要となり、コスト的
に不利である。 Furthermore, a structure in which a periodic structure other than the above-mentioned slits is inserted into the chiyoke groove has been proposed in Japan Patent Publication No. 54-21574 and Japanese Patent Publication Publication No. 52-40461, but the surface forming the chiyoke groove itself Moreover, since harmonics are not taken into account, it is also necessary to add ferrite etc. for practical use, which is disadvantageous in terms of cost.
上記のように従来のドアは薄形化、低コスト化
には不向きであつた。 As mentioned above, conventional doors are not suitable for thinning and cost reduction.
そこで、本発明は基本波用チヨーク溝と第2高
調波用チヨーク溝とを逆向きに対向させて、一つ
の入口を持つ一つの電波減衰空胴をドアの周縁に
設け、第2高調波用チヨーク溝の壁面自体を複数
の波板に分割し、この波板の形状、寸法に特定の
関係を与えることにより、基本波および高調波に
対する電波漏洩を極力抑えるというように簡単な
電波漏洩防止構造を持ち、薄形化、低コスト化が
はかれるドアを備えた高周波加熱装置を提供する
ことを目的とする。 Therefore, in the present invention, one radio wave attenuation cavity with one entrance is provided at the periphery of the door by arranging the fundamental wave groove and the second harmonic wave groove in opposite directions, A simple radio wave leakage prevention structure that minimizes radio wave leakage of fundamental waves and harmonics by dividing the wall surface of the chiyoke groove itself into multiple corrugated plates and giving specific relationships to the shapes and dimensions of these corrugated plates. An object of the present invention is to provide a high-frequency heating device equipped with a door that can be made thinner and lower in cost.
次に本発明の一実施例を図面とともに説明す
る。 Next, one embodiment of the present invention will be described with reference to the drawings.
第1図は本発明の高周波加熱装置の一例を示す
外観図である。1は外箱で、2はドア、3はドア
2の厚さと釣合のとれた厚みの操作パネルであ
る。操作パネル3は用途によつて種々様々に変え
られるが、自動加熱の場合を例にして説明する。
4は高周波出力、残留加熱時間などを示す表示装
置、5はメニユーごとの最適加熱パターンを決め
るメニユー選定ボタン、6は仕上りの程度を好み
に合わせて選ぶ仕上り調節つまみ、7は加熱を開
始するときに押す加熱ボタン、8はドアを開ける
ためのドア開ボタンである。 FIG. 1 is an external view showing an example of the high frequency heating device of the present invention. 1 is an outer box, 2 is a door, and 3 is an operation panel whose thickness is balanced with the thickness of the door 2. Although the operation panel 3 can be changed in various ways depending on the application, the case of automatic heating will be explained as an example.
4 is a display device that shows high frequency output, residual heating time, etc., 5 is a menu selection button that determines the optimal heating pattern for each menu, 6 is a finish adjustment knob that allows you to select the degree of finish according to your preference, and 7 is when to start heating. 8 is the heating button to press, and 8 is the door open button to open the door.
第2図は第1図に対応する本発明の高周波加熱
装置の要部断面略図である。9は高周波エネルギ
ーを発生する高周波発振器で、10は高周波発振
器9からの高周波エネルギーを加熱室11に伝送
するための導波管である。12は均一加熱を行な
うためのターンテーブルで、この上に被加熱物を
置く。均一加熱装置としてはターンテーブル12
以外にもスターラ、回転アンテナ、固定アンテナ
などがあり、いずれを用いてもよい。13はドア
2の前面に取付けられた透明板で、透明板13は
ドアカバー14によつてドア前板15に固着され
ている。ドア前板15にはドア後板16がネジ1
7によつて取付けられている。ドア前板15とド
ア後板16とはともに金属板から成り、加熱室開
口部周縁18に対向した電波減衰空胴19を形成
する。20は加熱室11に面した透明板で、21
は金網(あるいは穴あき金属板)である。透明板
13、金網21および透明板20を通して加熱室
11内が覗けるようになつている。22はドア2
をとり囲むサツシである。 FIG. 2 is a schematic sectional view of a main part of the high-frequency heating device of the present invention corresponding to FIG. 1. 9 is a high frequency oscillator that generates high frequency energy, and 10 is a waveguide for transmitting the high frequency energy from the high frequency oscillator 9 to the heating chamber 11. 12 is a turntable for uniform heating, on which the object to be heated is placed. A turntable 12 is used as a uniform heating device.
In addition, there are stirrers, rotating antennas, fixed antennas, etc., and any of them may be used. Reference numeral 13 denotes a transparent plate attached to the front surface of the door 2, and the transparent plate 13 is fixed to the door front plate 15 by a door cover 14. The door front plate 15 is attached to the door rear plate 16 with screw 1.
It is attached by 7. Both the door front plate 15 and the door rear plate 16 are made of metal plates, and form a radio wave attenuation cavity 19 facing the heating chamber opening periphery 18. 20 is a transparent plate facing the heating chamber 11;
is wire mesh (or perforated metal plate). The inside of the heating chamber 11 can be seen through the transparent plate 13, the wire mesh 21, and the transparent plate 20. 22 is door 2
It is Satsushi that surrounds.
第3図は第2図で示した電波減衰空胴19付近
の拡大図である。加熱周波数たとえば2450MHに
対する電波漏洩を防止するための基本波用チヨー
ク溝19aと、上記周波数の第2高調波4900MHz
に対する電波漏洩を防止するための第2高調波用
チヨーク溝19bを、互いに逆向きに対向させ
て、一つの入口23を持つ一つの電波減衰空胴1
9を形成している。基本波用チヨーク溝19aで
は入口23から短絡面15aまでのL字形の電波
伝搬経路を加熱周波数の自由空間波長λoに対し
て約λo/4としている。基本波用チヨーク溝19a
を加熱室11に近い側に配置すると共にこの溝1
9aの一壁面16aを加熱室開口部周縁18との
接触面としている。第2高調波用チヨーク溝19
bでは入口23から短絡面15bまでのL字形の
電波伝搬経路を約λo/8としている。第2高調波用
チヨーク溝19bの壁面15を第4図に示すよう
に複数のテーパ状の波板15wに分割し、この波
板15wは電波減衰空胴19の入口23に先端を
持つと共に、入口寸法Aより大きい空隙寸法Bを
あけて長手方向に並べられている。隣り合う波板
15wの間の空隙寸法Bは波板15wの先端15
w′付近において、電波減衰空胴19の入口寸法
Aより大きくとつているので、波板15wの先端
15w′に電界が集中し易くなる。これは、入口
23付近において電界は不連続状態にあるが、電
波減衰空胴19内へ伝搬する方向の電界成分を増
し、電波減衰空胴19内へ伝搬できない方向の電
界成分を減らす作用を波板15wが持つことを意
味する。つまり、波板15wは加熱室開口部周縁
18とドア2との間に漏洩するあらゆる高次モー
ドの電波を電波減衰空胴19内に能率よく入れる
整合ポストの作用を持ち、外部へ漏洩する電波を
減少させる。さらに、第3図で示したように電波
減衰空胴19内の二方向の電波伝搬経路長を約
λo/4と約λo/8にして、基本波および第2高調波
に対
してそれぞれ高インピーダンスにしている。加熱
室開口部周縁18と基本波用チヨーク溝19aの
一壁面16aとがドア2の閉成時に平面接触する
ようになつており、実質的にその相互間の間隙は
少ないので、この接触部に入り込む漏洩電波自体
も少ない。また、接触部は低インピーダンス(伝
送線路としての特性インピーダンス)で、上記入
口23の高インピーダンスとの反射が大きいの
で、波板15wに達する電波も微少になつてい
る。この微少電波を波板15wの整合ポストの作
用により、電波減衰空胴19内へ能率よく導き入
れ、この空胴19内の空間の蓄積エネルギーとし
て保持し、一部は壁面での損失電力として消費さ
れる。 FIG. 3 is an enlarged view of the vicinity of the radio wave attenuation cavity 19 shown in FIG. A fundamental wave groove 19a for preventing radio wave leakage at a heating frequency of, for example, 2450 MHz, and a second harmonic of the above frequency of 4900 MHz.
One radio wave attenuation cavity 1 having one inlet 23 has second harmonic channel grooves 19b facing each other in opposite directions to prevent radio wave leakage.
9 is formed. In the fundamental wave channel groove 19a, the L-shaped radio wave propagation path from the inlet 23 to the short-circuit surface 15a is approximately λo/4 with respect to the free space wavelength λo of the heating frequency. The fundamental wave chiyoke groove 19a is arranged on the side closer to the heating chamber 11, and this groove 1
One wall surface 16a of the heating chamber opening 16a is used as a contact surface with the heating chamber opening periphery 18. Chiyoke groove 19 for second harmonic
In b, the L-shaped radio wave propagation path from the inlet 23 to the short-circuit surface 15b is approximately λo/8. The wall surface 15 of the second harmonic channel groove 19b is divided into a plurality of tapered corrugated plates 15w as shown in FIG. They are arranged in the longitudinal direction with a gap size B larger than the entrance size A. The gap size B between adjacent corrugated plates 15w is the tip 15 of the corrugated plates 15w.
Since the entrance dimension A of the radio wave attenuation cavity 19 is larger near w', the electric field tends to concentrate at the tip 15w' of the corrugated plate 15w. Although the electric field is in a discontinuous state near the entrance 23, this has the effect of increasing the electric field component in the direction that propagates into the radio wave attenuation cavity 19 and reducing the electric field component in the direction that cannot propagate into the radio wave attenuation cavity 19. This means that the plate 15w has it. In other words, the corrugated plate 15w has the function of a matching post that efficiently introduces all high-order mode radio waves leaking between the heating chamber opening periphery 18 and the door 2 into the radio wave attenuation cavity 19, and the radio waves leaking to the outside. decrease. Furthermore, as shown in FIG. 3, the radio wave propagation path lengths in the two directions within the radio wave attenuation cavity 19 are set to approximately λo/4 and approximately λo/8 to provide high impedance for the fundamental wave and the second harmonic, respectively. I have to. The peripheral edge 18 of the opening of the heating chamber and the wall surface 16a of the fundamental wave channel 19a come into plane contact when the door 2 is closed, and since there is substantially little gap between them, this contact portion There are also fewer leakage radio waves entering. Further, since the contact portion has a low impedance (characteristic impedance as a transmission line) and is largely reflected from the high impedance of the inlet 23, the radio waves reaching the corrugated plate 15w are also very small. This minute radio wave is efficiently introduced into the radio wave attenuation cavity 19 by the action of the matching post of the corrugated plate 15w, and is retained as energy stored in the space inside this cavity 19, and a part of it is consumed as power loss on the wall surface. be done.
一方、空隙寸法B>入口寸法Aという寸法関係
を保ち、かつ加熱室開口部周縁18に対向する波
板18wの導体面を多くして、両導体間のインピ
ーダンスを低くするために、波板15wは根本1
5w″が幅が広く、先端15w′で幅の狭いテーパ
状にしている。この両導体間の低インピーダンス
と上記入口23の高インピーダンスとの反射を大
きくして、入口23を通過して外部へ向かう漏洩
電波をさらに少なく抑えている。 On the other hand, in order to maintain the dimensional relationship of gap dimension B>inlet dimension A and to increase the conductor surface of the corrugated plate 18w facing the heating chamber opening periphery 18 to lower the impedance between both conductors, the corrugated plate 15w is root 1
5w'' has a wide width, and the tip 15w' has a narrow taper shape.The reflection between the low impedance between these two conductors and the high impedance of the inlet 23 is increased, and the conductor passes through the inlet 23 to the outside. This further reduces the amount of leaked radio waves.
第5図はドア2のコーナ2aにおける波板15
wの相互間の寸法関係を示す。コーナ2aにおい
て、隣り合う波板15wの根本15w″間の空隙
寸法Cをλo/4以下にしている。この寸法制限は第
2高調波用チヨーク溝19bに入つた第2高調波
の波長に対しては1/2波長に対応し、しや断領域
となり、一旦溝19bに入つた第2高調波が再び
溝19bの外部へ出るのを防ぐために必要な条件
である。さらに、コーナ2a以外の波板15wの
先端15w′どうしの空隙寸法Bも、上記と同じ
理由でλo/4以下にすると、第2高調波用チヨーク
溝19bの減衰効果を良好にする。ドア2のコー
ナ2aを含む全周において、空隙寸法Bは入口寸
法Aより大きく、λo/4以下ということになる。 FIG. 5 shows a corrugated plate 15 at the corner 2a of the door 2.
The dimensional relationship between w is shown. At the corner 2a, the gap size C between the bases 15w'' of adjacent corrugated plates 15w is set to λo/4 or less. This corresponds to 1/2 wavelength and becomes a shearing region, which is a necessary condition to prevent the second harmonic that once entered the groove 19b from exiting the groove 19b again. If the gap size B between the tips 15w' of the corrugated plates 15w is also set to λo/4 or less for the same reason as above, the damping effect of the second harmonic tooth yoke groove 19b will be improved. At the circumference, the gap size B is larger than the entrance size A and is less than λo/4.
上記のような電波減衰空胴19は基本波、第2
高調波に対して十分な減衰効果を持つので、実用
上フエライトや導電性ゴムの補助手段が不要とな
り、低コスト化をはかる上で有利となる。 The radio wave attenuation cavity 19 as described above is for the fundamental wave, the second
Since it has a sufficient attenuation effect against harmonics, it is practically unnecessary to use auxiliary means such as ferrite or conductive rubber, which is advantageous in terms of cost reduction.
さらに、電波減衰空胴19は基本波用チヨーク
溝19a、第2高調波用チヨーク溝ともに加熱室
開口部周縁18と平行な方向の深さを適宜選定す
ることにより必要寸法が得られ、ドア2の厚さが
薄くてもよいので、電子化された薄形の操作パネ
ルと釣合のとれたデザイン上望ましい外観に仕上
げることができる。 Furthermore, the necessary dimensions of the radio wave attenuation cavity 19 can be obtained by appropriately selecting the depths of both the fundamental wave chock groove 19a and the second harmonic wave groove in the direction parallel to the heating chamber opening periphery 18. Since the thickness may be thin, it is possible to create a desirable appearance in terms of design that is in balance with the thin electronic operation panel.
以上のように、本発明によると、電波漏洩を少
なくすることができ、かつ薄形化、低コスト化に
適するドアを備えた高周波加熱装置を提供するこ
とができる。 As described above, according to the present invention, it is possible to provide a high-frequency heating device equipped with a door that can reduce radio wave leakage and is suitable for reduction in thickness and cost.
第1図は本発明の高周波加熱装置の一例を示す
外観図、第2図は第1図に対応する本発明の高周
波加熱装置の一実施例を示す要部断面略図、第3
図は第2図における電波減衰空胴19の拡大断面
図、第4図および第5図は電波減衰空胴19の入
口23付近での波板15wの寸法関係、作用を説
明するための斜視図である。
2……ドア、2a……ドア2のコーナ、11…
…加熱室、15c……第2高調波用チヨーク溝1
9bの壁面、15w……波板、15w′……波板
15wの先端、15w″……波板15wの根元、
16a……基本波用チヨーク溝19aの一壁面、
18……加熱室開口部周縁、19……電波減衰空
胴、19a……基本波用チヨーク溝、19b……
第2高調波用チヨーク溝、23……電波減衰空胴
19の入口、24……ドア2のヒンジ側の回転
軸。
FIG. 1 is an external view showing an example of the high-frequency heating device of the present invention, FIG. 2 is a schematic cross-sectional view of essential parts showing an example of the high-frequency heating device of the present invention corresponding to FIG. 1, and FIG.
The figure is an enlarged sectional view of the radio wave attenuation cavity 19 in FIG. 2, and FIGS. 4 and 5 are perspective views for explaining the dimensional relationship and function of the corrugated plate 15w near the entrance 23 of the radio wave attenuation cavity 19. It is. 2...door, 2a...corner of door 2, 11...
...Heating chamber, 15c...Chiyoke groove 1 for second harmonic
Wall surface of 9b, 15w...corrugated plate, 15w'...tip of corrugated plate 15w, 15w''...root of corrugated plate 15w,
16a... One wall surface of the fundamental wave chiyoke groove 19a,
18...Heating chamber opening periphery, 19...Radio wave attenuation cavity, 19a...Fundamental wave chiyoke groove, 19b...
Second harmonic chiyoke groove, 23... Entrance of the radio wave attenuation cavity 19, 24... Rotating shaft on the hinge side of the door 2.
Claims (1)
平行な方向の深さを適宜選定して得られる基本波
用チヨーク溝19aと第2高調波用チヨーク溝1
9bとを設け、この両溝を互いに逆向きに対向さ
せて一つの入口23を持つ一つの電波減衰空胴1
9を構成し、基本波用チヨーク溝19aを加熱室
11に近い側に配置すると共に、この溝19aの
一壁面16aを加熱室開口部周縁18と平面接触
させ、第2高調波用チヨーク溝19bの加熱室開
口部周縁18と対向する壁面15c自体を上記電
波減衰空胴19に漏洩電波を能率よく導き入れる
整合ポストと等価なテーパ状の複数の波板15w
に分割し、かつこの波板15wの根本どうしの空
隙寸法Cをドア2のコーナ2aにおいて加熱周波
数の自由空間波長の1/4以下としたことを特徴と
する高周波加熱装置。1. Fundamental wave chiyoke groove 19a and second harmonic chiyoke groove 1 obtained by appropriately selecting the depth in the direction parallel to the heating chamber opening peripheral edge 18 at the periphery of the door 2.
9b, and these two grooves face each other in opposite directions to form one radio wave attenuation cavity 1 having one inlet 23.
9, the fundamental wave channel groove 19a is arranged on the side closer to the heating chamber 11, one wall surface 16a of this groove 19a is brought into plane contact with the heating chamber opening periphery 18, and the second harmonic channel channel 19b is arranged. A plurality of tapered corrugated plates 15w, which are equivalent to alignment posts that efficiently guide leaked radio waves into the radio wave attenuation cavity 19, are formed by a wall surface 15c facing the heating chamber opening periphery 18.
A high-frequency heating device characterized in that the corrugated plate 15w is divided into two parts, and the gap size C between the roots of the corrugated plate 15w is set to 1/4 or less of the free space wavelength of the heating frequency at the corner 2a of the door 2.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP16446681A JPS5866287A (en) | 1981-10-15 | 1981-10-15 | High frequency heater |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP16446681A JPS5866287A (en) | 1981-10-15 | 1981-10-15 | High frequency heater |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5866287A JPS5866287A (en) | 1983-04-20 |
| JPS6262435B2 true JPS6262435B2 (en) | 1987-12-26 |
Family
ID=15793708
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP16446681A Granted JPS5866287A (en) | 1981-10-15 | 1981-10-15 | High frequency heater |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS5866287A (en) |
Families Citing this family (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH0526717Y2 (en) * | 1986-06-17 | 1993-07-06 | ||
| WO2017163799A1 (en) | 2016-03-25 | 2017-09-28 | パナソニックIpマネジメント株式会社 | High frequency heating device |
-
1981
- 1981-10-15 JP JP16446681A patent/JPS5866287A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5866287A (en) | 1983-04-20 |
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