JPH0546677B2 - - Google Patents
Info
- Publication number
- JPH0546677B2 JPH0546677B2 JP60241948A JP24194885A JPH0546677B2 JP H0546677 B2 JPH0546677 B2 JP H0546677B2 JP 60241948 A JP60241948 A JP 60241948A JP 24194885 A JP24194885 A JP 24194885A JP H0546677 B2 JPH0546677 B2 JP H0546677B2
- Authority
- JP
- Japan
- Prior art keywords
- door
- slit plate
- slit
- sides
- leakage
- 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 - Lifetime
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
産業上の利用分野
本発明は電子レンジ等の高周波加熱装置におけ
る開閉自在の扉の漏洩高周波シール構成に関する
ものである。
従来の技術
一般に電子レンジ等の高周波加熱装置における
扉の構成には次の3つの方式がある。
第1には、金属製扉体の周辺枠部に使用高周波
の波長の1/4の長さに等しい深さをもつ金属製壁
面を有するチヨーク溝を設け、これに加熱室側に
設けた開口から漏洩する高周波を導いて減衰させ
るものである。
第2は、上記と同様の構造においてフエライト
等の電波吸収体を併設したものである。
第3は、上記第1ならび第2の例としばしば組
合せて使用することが多いが、前記チヨーク溝内
に扉枠長手方向に平行して連続的な周期をもつて
スリツトを設けた金属板を埋設し、スリツトチヨ
ーク構成として減衰効果を高めたものである。
上記第3の方式の構成の中でも、連続的なスリ
ツトを有する金属板(以下スリツト板と称する)
を種々の形状に加工して、加熱装置の個々の特性
に対する最適化をはかつているが、チヨーク溝の
深さは使用高周波の1/4波長の長さを基本とする
ものが主であつた。
最近になつて、前記チヨーク溝の深さを1/4波
長より小さくしたものが現れ、更にチヨーク溝の
外壁を即ち扉の枠部最外周をスリツト板そのもの
で代用する方式のものが現われるようになつた。
(PCT特許国際公報W084−01083参照)
この小形チヨーク方式の採用によつて扉体の大
きさを小さく、かつ薄くできる利点があり、装置
全体の大きさもそれに伴なつて小形化し、軽量化
できるという利点を有する。
発明が解決しようとする問題点
ところが上記の構成においても、上辺ならび下
辺と左辺ならび右辺とのスリツト板同志の突合せ
部における減衰性能については期待された効果を
あげていないし、また漏波のメカニズムについて
理論的にも解明されているとはいい難い。
扉を開いてゆく過程で、通常高周波の発生装置
を停止させるスイツチが設けられているが、少く
とも前記スイツチが作動するまでの過程では扉周
辺からの漏波は増加するが、このときに最大の漏
波は扉の角部に集中する傾向がある。漏波測定器
の検出プローブの先端を扉の角部に当てたときに
常に最大値を示すのではなく、角部もしくは角部
近傍、経験的には角部より1/4波長離れた点がピ
ークを示すことが多い。なお、扉のヒンジ側にお
ける角部の漏波も同条件ではあるものの扉の開閉
に伴なう加熱室前面との〓間変化が少ないためほ
とんど問題とならない。即ち、扉の開き側の2つ
の隈部の漏波の減衰に対して十分な対策がとれて
いないのが現状である。ただし扉の閉成時におい
ては、ヒンジ側隈部も同様に漏波が大きいという
問題はある。
問題点を解決するための手段
上記問題を解決するため本発明の高周波加熱装
置の扉装置においては、扉枠部中に設けたスリツ
ト板の形状は、断面は略7字状をなし、その断面
の短辺を扉の四辺のそれぞれにおいて扉の内方向
に向かうようにし、スリツトと角穴とを交互に後
述する一定の周期寸法をもつている長辺を扉枠部
の最外周に配置して、前記長辺と扉本体の内周壁
とで加熱室側に開口を有するチヨーク溝を形成し
たものであつて、かつ前記チヨーク溝の内周壁面
と近接対向するスリツト板短辺の長手方向の延長
線同志が扉の隈部において直角に交差するが、そ
の際に縦もしくは横のいずれか一方の延長線が横
もしくは縦のいずれか他方のスリツト板に直接ぶ
つかることのないようにするとともに、前記延長
線とこれに直角なスリツト板との間の水平ならび
垂直方向の〓間を、スリツト板のスリツトの幅と
同等もしくはそれより小さくなるよう構成したも
のである。
またスリツト板の長手方向のスリツトと角穴と
が形成される周期、すなわちスリツトの一端から
隣のスリツトの一端まで、もしくは角穴の一端か
ら隣の角穴の一端までの寸法を、使用高周波の1/
4波長以下とし、その両端部はスリツトならびに
角穴部の長手方向寸法を他の部分と異なつた周期
をもつものとして構成している。
作 用
上記のような構成による扉装置は、加熱室から
漏洩する高周波、特に隈部からの漏洩量減衰に効
果がある。即ち、扉の隈部からの漏波は加熱室前
面開口のコーナ部もしくはその近傍から漏洩する
ものである。この部分からの漏波の性質と中央付
近からの漏波の性質とは若干異なつた点が考えら
れ、この差にそれぞれ応じたチヨーク構造が必要
である。
周期構造体をなすチヨーク構造の高周波域減衰
効果は、この周期構造体の長手方向(x方向とす
る)へ伝播する高周波エネルギーの減衰と、これ
に直角方向(y方向とする)へ進行する高周波エ
ネルギーの減衰との組合せにより得られるものと
考えられる。今チヨーク装置の任意の点における
高周波漏出を考えたとき、これが波長λ、電力密
度Wでx方向に対してθなる角度をもつて進行す
るとすれば、そのx方向ならびにy方向への見か
け上の成分は各々λx=λcosθ,Wx=Wcosθ,λy=
λsinθ,Wy=Wsinθとみなすことができる。チヨ
ーク溝の長手方向中央付近(縦でも横でも同じ)
における高周波の漏出進行は、x方向とy方向の
ほとんどあらゆる角度にわたるものとしなければ
ならない。そしてこれら180°の角度にわたる全方
向の漏洩高周波に対するスリツト板の寸法形状の
最適化は、θ=0°からθ=90°にわたる範囲にお
けるλx,λy,Wx,Wyに対して行なわれることに
なる。通常チヨーク溝の位置は加熱室開口より少
くとも外側に配設されているためθ=0°の場合は
ありえないが、θ≒0°とすると、このときx方向
の高周波のエネルギーが最も高く、y方向が0で
あり、またθ=90°のときにy方向のエネルギー
が最大でx方向が0となる。
これに対しコーナ部分の漏出進行波はθ=45°
を中心とした±45°の角度の範囲にわたるものと
みなすことができる。また加熱室内における定在
波は開口角部に集中することは考えにくく、開口
角部に近い点での定在波の存在は角部より1/4波
長離れた点が最も近いと想定する方が妥当であ
り、この点から外側に向かつて進行する漏波の減
衰をスリツト板の端部ならび縦横のスリツト板の
突合せ部分が受けもつと考えなければならない。
そして45°方向の進行波がエネルギー的に最も高
いレベルにあるとしなけれならない。
以上のように扉の隈部からの漏洩高周波の性質
は中央部分と異なつた性質を有しており、スリツ
ト板の隈部の処理ならびにその近傍におけるスリ
ツト板寸法は中央部分と異なる周期性をもつ構成
によつて対応することが可能となり、その組合せ
によつて扉周辺部からの漏洩量を少くすることが
可能となる。
実施例
以下本発明一実施例の高周波加熱装置の扉装置
を図面を参照して説明する。
第1図、第2図において金属製扉本体1は加熱
室前板開口2(一点鎖線にて示す)のやや外側に
位置する扉内周壁3と、断面略7字状のスリツト
板4,5とによつてチヨーク溝を形成している。
スリツト板断面における短辺6,7は前記チヨー
ク溝の中間に位置し、扉内周壁3と対向して設け
られ、この短辺6,7と内周壁3との間〓が高周
波の該チヨーク溝への導入開口となる。図示して
いないが通常この部分に樹脂製のカバーを設け
る。
スリツト板4,5は長手方向にスリツト8と角
穴9を交互にかつ一定の周期をもつて設けてい
る。スリツト8の下端と角穴9の下端とは長手方
向に一線上にあり、かつ角穴9の上端と短辺6,
7の下端とを一致させている。
扉は横開きであり本体片側上下にヒンジ部1
0,11を備えている。扉の開き側にあるスリツ
ト板5の外側のスペース12はドアスイツチ等を
作動させるキー等を取付けるために用いられる。
縦横のスリツト板4,5のコーナ部分の〓間寸
法、即ち図における水平方向の〓間Hと垂直方向
の〓間Vを限りなく小さくすることによつてコー
ナ部分からの漏波を少なくすることができる。た
だし第3図にH′寸法として示すように一方のス
リツト板の端部に他本のスリツト板がオーバーラ
ツプする位置まで伸びる形は望ましくない。これ
らの〓間寸法H,Vを変化させた場合の漏洩電力
密度の実測値を次に示す。
INDUSTRIAL APPLICATION FIELD The present invention relates to a leakage high frequency seal structure for a door that can be opened and closed in a high frequency heating device such as a microwave oven. 2. Description of the Related Art Generally, there are the following three types of door configurations in high-frequency heating devices such as microwave ovens. First, a chiyoke groove with a metal wall surface having a depth equal to 1/4 of the wavelength of the high frequency used is provided in the peripheral frame of the metal door body, and an opening is provided in this on the heating chamber side. It guides and attenuates high frequency waves leaking from the source. The second type has the same structure as above, but also includes a radio wave absorber such as ferrite. The third method, which is often used in combination with the first and second examples above, is a metal plate in which slits are provided at continuous intervals parallel to the longitudinal direction of the door frame in the cheese yoke groove. The damping effect is enhanced by the slit yoke structure. Among the configurations of the third method above, a metal plate having continuous slits (hereinafter referred to as a slit plate)
are processed into various shapes to optimize the individual characteristics of the heating device, but the depth of the chiyoke groove is mainly based on the length of 1/4 wavelength of the high frequency used. . Recently, a system has appeared in which the depth of the cheese yoke groove is smaller than 1/4 wavelength, and a system in which the outer wall of the cheese yoke groove, that is, the outermost periphery of the door frame, is replaced with the slit plate itself has appeared. Summer.
(Refer to PCT Patent International Publication W084-01083) Adoption of this compact chiyoke system has the advantage that the door body can be made smaller and thinner, and the overall size of the device can also be made smaller and lighter. has advantages. Problems to be Solved by the Invention However, even with the above configuration, the expected effect on the damping performance at the butt portions of the slit plates between the upper and lower sides and the left and right sides has not been achieved, and the mechanism of leakage waves has not been achieved. It is difficult to say that it has been explained theoretically. In the process of opening the door, there is usually a switch that stops the high-frequency generator, but at least in the process until the switch is activated, leakage waves from around the door increase; Leakage waves tend to concentrate at the corners of the door. The maximum value is not always shown when the tip of the detection probe of the leakage meter is placed against the corner of the door, but it is measured at the corner or near the corner, empirically at a point 1/4 wavelength away from the corner. It often shows a peak. Note that although the same conditions apply to the leakage of waves at the corners of the hinge side of the door, this is hardly a problem because there is little change in distance from the front of the heating chamber when the door is opened and closed. That is, the current situation is that no sufficient measures have been taken to attenuate the leakage waves at the two corners on the opening side of the door. However, when the door is closed, there is a problem in that the leakage of waves from the side edges of the hinge is also large. Means for Solving the Problems In order to solve the above-mentioned problems, in the door device of the high frequency heating device of the present invention, the shape of the slit plate provided in the door frame portion is approximately 7-shaped in cross section; The short sides of the door face toward the inside of the door on each of the four sides of the door, and the long sides with slits and square holes having a certain periodic dimension as described later are arranged on the outermost periphery of the door frame. , wherein the long side and the inner circumferential wall of the door body form a cheese groove having an opening on the heating chamber side, and an extension in the longitudinal direction of the short side of the slit plate that closely opposes the inner peripheral wall surface of the cheese groove. The lines intersect at right angles at the edge of the door, but in doing so, ensure that either the vertical or horizontal extension line does not directly collide with the other horizontal or vertical slit plate, and The horizontal and vertical spacing between the line and the slit plate perpendicular to the line is configured to be equal to or smaller than the width of the slit in the slit plate. In addition, the period in which the slits and square holes are formed in the longitudinal direction of the slit plate, that is, the dimension from one end of a slit to one end of an adjacent slit, or from one end of a square hole to one end of an adjacent square hole, is determined based on the high frequency used. 1/
The length is 4 wavelengths or less, and the longitudinal dimensions of the slits and square holes at both ends are configured to have a period different from that of the other parts. Effect The door device configured as described above is effective in attenuating the amount of high frequency leaking from the heating chamber, especially the amount of leakage from the corners. That is, the leakage waves from the corner of the door leak from the corner of the front opening of the heating chamber or the vicinity thereof. It is thought that the characteristics of the leakage waves from this part and the characteristics of the leakage waves from around the center are slightly different, and it is necessary to have a chain structure that corresponds to each of these differences. The high-frequency attenuation effect of the chi-yoke structure, which is a periodic structure, is the attenuation of high-frequency energy propagating in the longitudinal direction (x direction) of the periodic structure, and the high-frequency energy propagating in the direction perpendicular to this (y direction). This is thought to be obtained in combination with energy attenuation. Now, when considering high-frequency leakage at any point in the yoke device, if it travels at a wavelength λ, a power density W, and an angle θ with respect to the x direction, then the apparent leakage in the x and y directions is The components are λ x = λcosθ, W x = Wcosθ, λ y =
It can be regarded as λsinθ, W y =Wsinθ. Near the longitudinal center of the chiyoke groove (same both vertically and horizontally)
The radio frequency leakage progression in must span almost all angles in the x and y directions. Optimization of the dimensions and shape of the slit plate for leakage high frequencies in all directions over these 180° angles was performed for λ x , λ y , W x , W y in the range from θ = 0° to θ = 90°. It will be. Normally, the position of the cheese yoke groove is located at least outside the heating chamber opening, so it is impossible for θ = 0°, but if θ = 0°, then the high frequency energy in the x direction is the highest, and the y When the direction is 0 and θ=90°, the energy in the y direction is maximum and the energy in the x direction is 0. On the other hand, the leakage traveling wave at the corner part is θ=45°
It can be considered as covering an angle range of ±45° centered on . In addition, it is unlikely that standing waves in the heating chamber will be concentrated at the aperture corners, and it is best to assume that the presence of standing waves at a point close to the aperture corner is closest at a point 1/4 wavelength away from the corner. is reasonable, and it must be considered that the end portions of the slit plates and the abutting portions of the vertical and horizontal slit plates are responsible for attenuating the leakage waves that proceed outward from this point.
And it must be assumed that the traveling wave in the 45° direction is at the highest energy level. As mentioned above, the properties of the high-frequency waves leaking from the edges of the door are different from those at the center, and the processing of the edges of the slit plate and the dimensions of the slit plate in the vicinity are structured to have a periodicity different from that of the center. Therefore, it becomes possible to deal with the problem, and by the combination thereof, it becomes possible to reduce the amount of leakage from the area around the door. Embodiment Hereinafter, a door device for a high-frequency heating device according to an embodiment of the present invention will be described with reference to the drawings. In FIGS. 1 and 2, the metal door body 1 consists of a door inner circumferential wall 3 located slightly outside the heating chamber front plate opening 2 (indicated by a dashed line), and slit plates 4 and 5 each having an approximately 7-shaped cross section. A chiyoke groove is formed by this.
The short sides 6 and 7 in the cross section of the slit plate are located between the cheese grooves and are provided facing the inner peripheral wall 3 of the door, and the area between the short sides 6 and 7 and the inner peripheral wall 3 is the high frequency cheese groove. It becomes an introduction opening to. Although not shown, a resin cover is usually provided at this portion. The slit plates 4 and 5 are provided with slits 8 and square holes 9 alternately and at regular intervals in the longitudinal direction. The lower end of the slit 8 and the lower end of the square hole 9 are on a line in the longitudinal direction, and the upper end of the square hole 9 and the short side 6,
7 is aligned with the lower end. The door opens horizontally, and there are hinge parts 1 on the top and bottom of one side of the main body.
0,11. A space 12 outside the slit plate 5 on the opening side of the door is used for attaching a key or the like for operating a door switch or the like. To reduce leakage waves from the corner portions by minimizing the distance between the corner portions of the vertical and horizontal slit plates 4 and 5, that is, the horizontal distance H and the vertical distance V in the figure. I can do it. However, as shown by dimension H' in FIG. 3, it is not desirable that the end of one slit plate extends to a position where the other slit plate overlaps. The actual measured values of the leakage power density when these dimensions H and V are changed are shown below.
【表】
この表において上段の数値は、扉が正常に閉じ
ている状態で寸法公差の組合せが最悪の場合(即
ち〓間が一番大きい状態)であり、下段の数値は
高周波発生装置を停止させるためのスイツチが作
動する直前まで扉を開いた状態のいずれも最高ピ
ーク値を示す。また測定対象は高周波出力500W
の電子レンジで水道水275mlを負荷とした場合で
ある。なおヒンジ側でのスリツト板4,5の突合
せ寸法の組合せは前述したように寸法変化に対す
る漏波の変化がほとんどないので省略し、上表の
値は全て扉の開き側のコーナについての値であ
る。
この実測結果からスリツト板4,5のコーナ部
の突合せ寸法が小さくなるほど漏波が減少してい
ることがわかる。ただH=−40mmの時の値がH=
5.0mmの時の値よりも一部漏波が大きくなる傾向
を示している。これはスリツト板4,5の長手方
向に伝播して減衰してゆく高周波が互に干渉し合
い減衰効果を乱すためと思われる。
H,V寸法の大きさはスリツト板4,5の長手
方向のスリツトの幅寸法A(本測定の場合は10mm)
を越えた場合にはほとんど実用に供しない値とな
るので、この幅寸法Aが一つの目安となり、少く
ともこの値より小さくすることが適切な効果を期
待できる条件と考えられる。
一方スリツト板のスリツト8のA寸法とスリツ
トとスリツトとの間の寸法Bとは長手方向に規則
正しい間隔をもつて設定した場合には、上記コー
ナ寸法の最適化がはかれない場合がある。即ち縦
方向のスリツト板5は丁度良いが横方向のスリツ
ト板4が寸法不足(あるいは寸法過大)になつた
り、あるいはその逆になつたり、あるいは一方が
寸法不足で他方が寸法過大であつたりすることが
多い。ところが長手方向の周期性は縦横とも同じ
周期を備えることが漏波の点がは望ましい。これ
ら相反する条件に対してスリツト板4,5の両端
部と最外側のスリツトの幅A,B寸法を0.5〜1
mmの範囲内で中央付近の寸法と異なるものとし、
従つて両端近傍において非周期性としている。こ
れは上述したように加熱室開口のコーナ近辺から
へ向かう漏波の性質が他の部分の漏波と異なると
いう点に着目し、前記周期を高周波の1/4波長と
し、スリツト板4,5の長手方向の端部の一周期
即ち最大でも1/4波長の長さ分だけを非周期性と
するもので、「作用」の項でも述べたように加熱
室開口角部から1/4波長以上離れた点でないと加
熱室内の定在波の存在が考えにくいという点から
考え、このスリツト板の非周期部分が受けもつ漏
波の減衰は前記定在波存在部分から外方向に向か
う他とやや性質の異なる高周波漏洩分だけを対象
とすることができる。
発明の効果
以上のように本発明のチヨーク装置における縦
と横のスリツト板のコーナ部における水平、垂直
方向の〓間を、少くともスリツトの幅より小さく
するとともに、互にオーバーラツプのない値に設
定し、同時にスリツト板の両端部の一周期分の長
さを中央部分の他の周期と異なる周期をもたせる
ことにより、扉のシール性能におけるコーナ部分
での漏洩量を確実に減少させうる効果が得られ
る。[Table] In this table, the numbers in the upper row are for the worst combination of dimensional tolerances when the door is closed normally (i.e., the largest gap), and the numbers in the lower row are for stopping the high-frequency generator. The highest peak value is shown in both cases when the door is open until just before the switch is activated. The measurement target is a high frequency output of 500W.
This is the case when 275ml of tap water is loaded in a microwave oven. Note that the combination of the butt dimensions of the slit plates 4 and 5 on the hinge side is omitted because, as mentioned above, there is almost no change in leakage due to the change in dimensions, and the values in the table above are all values for the corner on the opening side of the door. be. From this actual measurement result, it can be seen that the smaller the abutting dimension of the corner portions of the slit plates 4 and 5, the more the leakage of waves decreases. However, the value when H=-40mm is H=
There is a tendency for some wave leakage to become larger than the value at 5.0 mm. This seems to be because the high frequency waves that propagate in the longitudinal direction of the slit plates 4 and 5 and are attenuated interfere with each other and disturb the attenuation effect. The H and V dimensions are the width dimension A of the slit in the longitudinal direction of the slit plates 4 and 5 (10 mm in this measurement)
If it exceeds this value, it becomes a value that is hardly of practical use, so this width dimension A serves as a guideline, and making it smaller than this value is considered to be a condition under which appropriate effects can be expected. On the other hand, if dimension A of the slits 8 of the slit plate and dimension B between the slits are set at regular intervals in the longitudinal direction, the corner dimensions may not be optimized. That is, the vertical slit plate 5 may be just right, but the horizontal slit plate 4 may be undersized (or oversized), or vice versa, or one may be undersized and the other may be oversized. There are many things. However, from the viewpoint of wave leakage, it is desirable that the periodicity in the longitudinal direction be the same in both the vertical and horizontal directions. For these contradictory conditions, the widths A and B of both ends of the slit plates 4 and 5 and the outermost slit are set to 0.5 to 1.
It shall be different from the dimension near the center within the range of mm,
Therefore, it is assumed to be non-periodic near both ends. This is done by focusing on the fact that the nature of the leakage waves from the vicinity of the corner of the heating chamber opening is different from the leakage waves from other parts, as described above, and the period is set to 1/4 wavelength of the high frequency, and the slit plates 4, 5 It is non-periodic for only one period of the length of the longitudinal end, that is, a length of 1/4 wavelength at the maximum. Considering that it is difficult to imagine the existence of standing waves in the heating chamber unless the point is more far away, we believe that the attenuation of the leakage waves carried by the non-periodic portion of the slit plate is directed outward from the portion where the standing waves exist. It is possible to target only high-frequency leakage components with slightly different properties. Effects of the Invention As described above, in the cheese yoke device of the present invention, the distances in the horizontal and vertical directions at the corners of the vertical and horizontal slit plates are made at least smaller than the width of the slits, and are set to values that do not overlap with each other. At the same time, by making the length of one cycle at both ends of the slit plate different from the other cycles at the center, it is possible to reliably reduce the amount of leakage at the corners of the door sealing performance. It will be done.
第1図は本発明実施例の扉のチヨーク装置の一
部切欠斜視図、第2図は同扉の裏面図、第3図は
同扉のコーナ部分の組合せの一例を示す部分裏面
図である。
3……扉内周壁、4……(横の)スリツト板、
5……(縦の)スリツト板、6,7……短辺、8
……スリツト。
Fig. 1 is a partially cutaway perspective view of a chiyoke device of a door according to an embodiment of the present invention, Fig. 2 is a back view of the door, and Fig. 3 is a partial back view showing an example of a combination of corner portions of the door. . 3... Inner peripheral wall of the door, 4... (horizontal) slit plate,
5... (vertical) slit plate, 6, 7... short side, 8
...Slit.
Claims (1)
用チヨーク装置において、切り欠き部と角穴部と
を交互に、かつ使用高周波の波長の1/4以下の寸
法となる一定周期で形成した断面略7字状のスリ
ツト板を前記チヨーク内に配し、扉の上下辺の前
記スリツト板の各一端と、これに直角に対応する
扉の左右辺のスリツト板の7字状断面の短辺を長
手方向に延長したときの見掛け上の水平方向の間
〓、ならびに扉の左右辺の前記スリツト板の各一
端と、これに直角に対応する扉の上下辺のスリツ
ト板の7字状断面の短辺を長手方向に延長したと
きの見掛け上の垂直方向の間〓を、0より大き
く、かつ前記スリツト板の切り欠き部の幅寸法よ
り小さく設定する構成とした高周波加熱装置の扉
装置。 2 左右上下各4辺のスリツト板の切り欠き部と
角穴部の長手方向寸法を、各々の端部においての
み他の一定周期寸法と異なる寸法とした特許請求
の範囲第1項記載の高周波加熱装置の扉装置。[Scope of Claims] 1. In a high-frequency sealing device provided on the four surrounding frames of a metal door body, the cutout portions and square hole portions are arranged alternately, and the dimensions are 1/4 or less of the wavelength of the high frequency used. A slit plate with a cross section of approximately 7-shape formed at regular intervals is arranged in the cheese yoke, and one end of each slit plate on the upper and lower sides of the door and a 7-shaped slit plate on the left and right sides of the door that corresponds at right angles to the slit plate are arranged in the cheese yoke. The apparent horizontal distance when the short sides of the shaped cross section are extended in the longitudinal direction, as well as the distance between each end of the slit plates on the left and right sides of the door and the slit plates on the top and bottom sides of the door corresponding at right angles thereto. A high-frequency heating device configured such that the apparent vertical distance when the short sides of the figure-7 cross section are extended in the longitudinal direction is set to be larger than 0 and smaller than the width dimension of the notch of the slit plate. door device. 2. High-frequency heating according to claim 1, in which the longitudinal dimensions of the notch and the square hole of the slit plate on each of the four sides of the left, right, top, and bottom are different from other constant periodic dimensions only at each end. Device door device.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP60241948A JPS62100987A (en) | 1985-10-29 | 1985-10-29 | Door of radio frequency heater |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP60241948A JPS62100987A (en) | 1985-10-29 | 1985-10-29 | Door of radio frequency heater |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS62100987A JPS62100987A (en) | 1987-05-11 |
| JPH0546677B2 true JPH0546677B2 (en) | 1993-07-14 |
Family
ID=17081949
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP60241948A Granted JPS62100987A (en) | 1985-10-29 | 1985-10-29 | Door of radio frequency heater |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS62100987A (en) |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2007317607A (en) * | 2006-05-29 | 2007-12-06 | Mitsubishi Electric Corp | High frequency heating device |
-
1985
- 1985-10-29 JP JP60241948A patent/JPS62100987A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS62100987A (en) | 1987-05-11 |
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