JPS6322440B2 - - Google Patents
Info
- Publication number
- JPS6322440B2 JPS6322440B2 JP16446481A JP16446481A JPS6322440B2 JP S6322440 B2 JPS6322440 B2 JP S6322440B2 JP 16446481 A JP16446481 A JP 16446481A JP 16446481 A JP16446481 A JP 16446481A JP S6322440 B2 JPS6322440 B2 JP S6322440B2
- Authority
- JP
- Japan
- Prior art keywords
- heating chamber
- groove
- door
- chamber opening
- radio wave
- 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)
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.
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
にドア機構の低コスト化が要望されている。 Compact, multifunctional electronic components such as ICs and microcomputers are being actively incorporated into the control circuits of high-frequency heating equipment, and operation panels are becoming smaller and thinner. There is a demand for thin doors. Furthermore, there is a growing tendency to automate complex operations, and as electronic circuits become more expensive, there is a demand for lower costs for mechanical parts, especially door mechanisms.
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。 A proposal was made in the United States to increase the attenuation effect of the chiyoke groove as a radio wave propagation direction regulating device by periodically arranging conductor pieces of λ/4 length, so-called slits, on one side of the chiyoke groove, which has a depth of 1/4 of the used wavelength λ. Patent 2772402
(1956.11.27 patent) and 2850706 (1958.9.2 patent).
上記特許と同様な電波漏洩防止構造が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
対向金属面と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
熱室開口部周縁の間隙に入射する電波が多くな
り、基本波および高周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。 3767884 has a radio wave leakage prevention structure similar to the above patent.
(Japanese Patent Application Publication No. 48-81146, Japanese Patent 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 slot is opposite to the slit. This method forcibly maintains the distance between the metal surface and the metal surface 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, and its function as a radio wave propagation direction regulating device (electromagnetic energy mode sustaining structure) decreases. be. With this method, a large number of radio waves enter the gap between the door and the periphery of the heating chamber opening, and to prevent leakage of fundamental waves and high frequencies, it is necessary to add conductive rubber or to complicate the propagation path of the leaked radio waves, resulting in large attenuation. It is necessary to produce an effect, and it is not suitable for making doors thinner and lowering costs.
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. 51-22663, 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実体を複数
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 to the fundamental wave and harmonics by dividing the wall surface of the chiyoke groove into multiple corrugated plates and giving specific relationships to the shapes and dimensions of the 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
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。 Next, an embodiment of the present invention will be described with reference to the drawings. Fig. 1 is an external view showing an example of a 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および透明盤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高周波用チ
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19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19a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19b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15c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15
w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15w′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15
w′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内へ伝搬する電界成分を増し、電波減
衰空胴19内へ伝搬できない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
間を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
2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. The fundamental wave groove 19a for preventing radio wave leakage at a heating frequency of, for example, 2450 MHz, and the second high frequency wave groove 19b for preventing radio wave leakage at the second harmonic of the above frequency of 4900 MHz are arranged in opposite directions to each other. , forming one radio wave attenuation cavity 19 having one inlet 23. 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 one wall surface 16a of this groove 19a is used as a contact surface with the heating chamber opening periphery 18. In the second harmonic channel groove 19b, the L-shaped radio wave propagation path from the inlet 23 to the shorting surface 15b is approximately λo/8. The wall surface 15c of the second harmonic channel groove 19b is divided into a plurality of tapered corrugated plates 15w as shown in FIG.
The tips w have their tips at the entrance 23 of the radio wave attenuation cavity 19, and are arranged in the longitudinal direction with a gap dimension B larger than the entrance dimension A. The gap size B between adjacent corrugated plates 15w is larger than the entrance size A of the radio wave attenuation cavity 19 near the tip 15w' of the corrugated plate 15w.
The electric field tends to concentrate on w′. This is entrance 23
Although the electric field is discontinuous in the vicinity, this means that the corrugated plate 15w has the effect of increasing the electric field component that propagates into the radio wave attenuation cavity 19 and reducing the electric field component that cannot propagate into the radio wave attenuation cavity 19. 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 reduces the radio waves leaking to the outside. let 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. ing. The heating chamber opening periphery 18 and one wall surface 16a of the fundamental wave cheese yoke groove 19a come into plane contact when the door 2 is closed.
Since the gap between them is substantially small, the amount of leakage radio waves entering this contact portion is also small. 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. By the action of the matching posts of the corrugated plate 15w, these minute radio waves are efficiently guided into the radio wave attenuation cavity 19 and held as accumulated energy in the space inside the cavity 19, and some of it is consumed as power loss on the wall surface. Ru.
電波減衰空胴19内に入らず、入口23を通過
して加熱室開口部周縁18と波板15wとの間の
隙間に進入して外部へ向かう漏洩電波を、反射さ
せて加熱室11側へ戻すことにより、ドア2の電
波漏洩防止効果を一段と向上させることができ
る。そうするためには、周知のように、異なるイ
ンピーダンスを持つ二つの線路の接続点における
反射は両線路のインピーダンスの差が大きいほど
大きくなるという性質があるので、電波減衰空胴
19の入口23の高インピーダンスに対して加熱
室開口部周縁18と波板15wとの両導体間で形
成する近似的な平行板線路のインピーダンス(正
確には特性インピーダンス)を小さくすればよ
い。また、平行板線路では線路の幅を大きくする
ほどインピーダンスが小さくなるという性質が知
られている。 Leaked radio waves that do not enter the radio wave attenuation cavity 19 but pass through the inlet 23 and enter the gap between the heating chamber opening periphery 18 and the corrugated plate 15w and head to the outside are reflected to the heating chamber 11 side. By returning it, the effect of preventing radio wave leakage of the door 2 can be further improved. To do this, as is well known, the reflection at the connection point of two lines with different impedances increases as the difference in impedance between the two lines increases. For high impedance, the impedance (more precisely, the characteristic impedance) of the approximate parallel plate line formed between the conductors of the heating chamber opening periphery 18 and the corrugated plate 15w may be made small. Furthermore, it is known that the impedance of parallel plate lines decreases as the width of the line increases.
そこで、波板15wを、先端15w′では空隙
寸法B>入口寸法Aという寸法関係に保ち、その
根本15w′に向かうほど幅の広いテーパ状とす
ることにより、加熱室開口部周縁18と波板15
wとで形成する線路のインピーダンスを小さくす
る。すなわち、加熱室開口部周縁18と波板の両
導体間の低インピーダンスと上部入口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。したがつてフエライトや導電性ゴム等
が不要となり低コスト化がはかれる。 Therefore, by maintaining the dimensional relationship of gap size B>inlet size A at the tip 15w' of the corrugated plate 15w, and tapering the corrugated plate 15w so that the width becomes wider toward the base 15w', the heating chamber opening periphery 18 and the corrugated plate 15
The impedance of the line formed by w is reduced. That is, by increasing the reflection between the low impedance between the heating chamber opening periphery 18 and the conductors of the corrugated plate and the high impedance of the upper entrance 23, leakage radio waves passing through the entrance 23 and heading outside are further suppressed. . Therefore, ferrite, conductive rubber, etc. are not required, and costs can be reduced.
更に、ドア2を開く場合、第3図の黒丸をヒン
ジ側の回転軸24とすると、この回転軸24を中
心とする円孤状矢印で示したように、ドアカバー
端部14a、波板15wの根本15w″および先
端15w′が回転移動する。ドア2が開くとき、
ヒンジ側のドアカバー端部14aと波板15wの
根本15w″は加熱室開口部周縁18に接近する
が、波板15wの先端15w′は遠ざかる。した
がつて、ドアの回転軸24のあるヒンジ側におい
て、波板15wと加熱室開口部周縁18との間隙
を波板15wの根本15w″から先端15w′に向
かうほど小さくしても差し支えない。こうする
と、ドア2の開閉の際、波板15wが加熱室開口
部周縁18とぶつかることがなく、波板15wの
変形が防止できる。又、波板15wと加熱室開口
部周縁18との平均的な導体表面間距離を少なく
できるので、導体間インピーダンスが小さくな
る。そのため、ドア2の電波漏洩防止効果を十分
に発揮することができる。 Furthermore, when opening the door 2, assuming that the black circle in FIG. 3 is the rotation axis 24 on the hinge side, the door cover end 14a and the corrugated plate 15w move as shown by arc-shaped arrows centered on this rotation axis 24. The base 15w'' and the tip 15w' rotate. When the door 2 opens,
The door cover end 14a on the hinge side and the root 15w'' of the corrugated plate 15w approach the heating chamber opening periphery 18, but the tip 15w' of the corrugated plate 15w moves away. On the side, the gap between the corrugated plate 15w and the heating chamber opening periphery 18 may be made smaller from the base 15w'' of the corrugated plate 15w toward the tip 15w'. In this way, when the door 2 is opened and closed, the corrugated plate 15w does not collide with the heating chamber opening periphery 18, and deformation of the corrugated plate 15w can be prevented. Furthermore, since the average distance between the conductor surfaces between the corrugated plate 15w and the heating chamber opening periphery 18 can be reduced, the impedance between the conductors can be reduced. Therefore, the effect of preventing radio wave leakage of the door 2 can be fully exhibited.
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19b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 required 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 chock groove 19b in the direction parallel to the heating chamber opening periphery 18. Since the thickness of 2 may be thin, it is possible to achieve a desired appearance in terms of design that is in balance with a 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2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 including a door 2 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付近の拡大
断面図、第4図は電波減衰空胴19の入口23付
近での波板15wの作用を説明するための斜視図
である。
2…ドア、11…加熱室、15c…第2高調波
用チヨーク溝19bの壁面、15w…波板、15
w′…波板15wの先端、15w″…波板15wの
根本、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.
This figure is an enlarged sectional view of the vicinity of the radio wave attenuation cavity 19 in FIG. 2, and FIG. 4 is a perspective view for explaining the action of the corrugated plate 15w in the vicinity of the entrance 23 of the radio wave attenuation cavity 19. 2...Door, 11...Heating chamber, 15c...Wall surface of second harmonic chiyoke groove 19b, 15w...Corrugated plate, 15
w'... Tip of the corrugated plate 15w, 15w''... Root of the corrugated plate 15w, 16a... One wall surface of the fundamental wave chyo yoke groove 19a, 18... Heating chamber opening periphery, 19... Radio wave attenuation cavity, 19a... For the fundamental wave Chiyoke groove, 19b...2nd
Harmonic channel 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1
1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と加熱室開口部周縁
18との間隙をドア2の回転軸24のあるヒンジ
側において波板15wの根本から先端に向かうほ
ど小さく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 and the fundamental wave groove 19a is connected to the heating chamber 1.
1, one wall surface 16a of this groove 19a is brought into planar contact with the heating chamber opening periphery 18, and the wall surface 15c itself facing the heating chamber opening periphery 18 of the second harmonic chiyoke groove 19b is placed in planar contact with the heating chamber opening periphery 18. It is divided into a plurality of tapered corrugated plates 15w equivalent to alignment posts that efficiently introduce leakage radio waves into the radio wave attenuation cavity 19, and the gap between the corrugated plates 15w and the heating chamber opening periphery 18 is set at the door 2. A high-frequency heating device characterized in that the corrugated plate 15w becomes smaller from the root to the tip on the hinge side where the rotating shaft 24 is located.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP16446481A JPS5866285A (en) | 1981-10-15 | 1981-10-15 | High frequency heater |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP16446481A JPS5866285A (en) | 1981-10-15 | 1981-10-15 | High frequency heater |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5866285A JPS5866285A (en) | 1983-04-20 |
| JPS6322440B2 true JPS6322440B2 (en) | 1988-05-11 |
Family
ID=15793667
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP16446481A Granted JPS5866285A (en) | 1981-10-15 | 1981-10-15 | High frequency heater |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS5866285A (en) |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN108886845B (en) | 2016-03-25 | 2022-02-18 | 松下知识产权经营株式会社 | High-frequency heating device |
-
1981
- 1981-10-15 JP JP16446481A patent/JPS5866285A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5866285A (en) | 1983-04-20 |
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