JPH0569277B2 - - Google Patents
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- Publication number
- JPH0569277B2 JPH0569277B2 JP61215371A JP21537186A JPH0569277B2 JP H0569277 B2 JPH0569277 B2 JP H0569277B2 JP 61215371 A JP61215371 A JP 61215371A JP 21537186 A JP21537186 A JP 21537186A JP H0569277 B2 JPH0569277 B2 JP H0569277B2
- Authority
- JP
- Japan
- Prior art keywords
- wall surface
- door
- cavity resonator
- shaped conductor
- 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.)
- Expired - Lifetime
Links
Landscapes
- Constitution Of High-Frequency Heating (AREA)
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 Field of the Invention 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、チヨーク溝と同様に漏洩電波を少なくするこ
とができるという提案が特開昭60−25190号公報
にある。この従来例では、溝の深さ方向に幅の異
なる溝を設けたり、溝の周壁の形状を深さ方向に
変形するなどかなり形状が複雑である。また、特
性インピーダンスの不連続部における反射防止を
考慮する必要がある。また、第7図で示すよう
に、ドア5の外周に電波漏洩防止用の空胴共振器
12を屈曲形成してロ字状断面とし、空胴共振器
12の一周壁である張出面11の端部切口と空胴
共振器12の他の壁面(第1の壁面8)とを対向
させた入口25を有する構造が実開昭61−795号
公報に示されている。この従来例では空胴共振器
12の周壁が複数の導体片に分割されているとは
記載されていない。したがつて空胴共振器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つてくるため、空胴共振
器12が共振状態から外れ、電波漏洩防止効果が
小さくなる。仮りに第7図の空胴共振器12の立
ち上がり面23と張出面11を長手方向(x方
向)に使用波長の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
容量Cと等価インダクタンスLとから成る並列共
振素子をドア5の長手方向(x方向)に複数個並
べたものとみなせる。各並列共振素子において、
後述の(2)式で示すように、空胴共振器12の入口
25と空胴断面の面積中心Oの距離lMと、入口寸
法Gとの比lM/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lM/G=1.0で、後
述する本発明のlM/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12の
断面ABを大きくする必要があるので、従来例の
空胴共振器12は大形となりドアの小形化、低コ
スト化には不向きである。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. There is a proposal in Japanese Patent Laid-Open No. 60-25190 that even if the diameter 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 chiyoke groove. 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. Further, as shown in FIG. 7, a cavity resonator 12 for preventing radio wave leakage is bent on the outer periphery of the door 5 to have a rectangle-shaped cross section, and a projecting surface 11 that is one peripheral wall of the cavity resonator 12 is bent. A structure having an inlet 25 in which the end cut 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. This conventional example does not describe that the peripheral wall of the cavity resonator 12 is divided into a plurality of conductor pieces. Therefore, higher-order mode radio waves that occur in a direction other than the yz plane as shown in FIG. 8 enter the cavity resonator 12, so the cavity resonator 12 comes out of the resonant state, preventing radio wave leakage. The effect becomes smaller. 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 each 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 C and an equivalent inductance L arranged in the longitudinal direction (x direction) of the door 5. In each parallel resonant element,
As shown in equation (2) below, the larger the ratio l M /G of the distance l M between the entrance 25 of the cavity resonator 12 and the center of area O of the cavity cross section to the entrance dimension G, the greater the equivalent capacitance C. growing. In the cavity resonator 12 of FIG. 7, when l M /G=1.0, the equivalent capacitance C is smaller than when l M /G≧1.5 in the present invention, which will be described later. Accordingly, the equivalent inductance L must be increased by that amount according to equation (3) described later, so that it resonates with the frequency of the leaked radio waves. Therefore, as is clear from equation (1) below, it is necessary to increase the cross section AB of the cavity resonator 12, so the conventional cavity resonator 12 is large, resulting in a smaller door and lower cost. It is not suitable for
なお、第7図は実開昭61−795号公報の明細書
の図面の各部寸法を同一比率で示したものであ
り、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てある。 In addition, FIG. 7 shows the dimensions of each part in the drawing of the specification of Utility Model Application Publication No. 61-795 in the same proportion, and the names and numbers of the components are the same for the parts corresponding to the present invention. There is.
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つたり、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 difficult to miniaturize the door. This is an unsuitable point.
問題点を解決するための手段
ドア周囲にロ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4面のうち
3面をドアの周囲の長手方向に設けた多数のコ字
状導体片で形成し、残りの一面とコ字状導体片の
端部切口とを互いに対向させて空胴共振器に漏洩
電波を導びき入れる入口とし、かつこの入口と空
胴断面の面積中心の距離lMと、入口寸法Gとの比
lM/Gを1.5以上とし、コ字状導体片の一端面を第2
の壁面に接触させる構成としたものである。Measures to solve the problem A cavity resonator with a rectangle-shaped cross section for preventing leakage radio waves is installed around the door, and three of the four sides of this cavity resonator are installed in the longitudinal direction around the door. The remaining surface and the end cut of the U-shaped conductor piece are made to face each other as an entrance for introducing leakage radio waves into the cavity resonator, and this entrance and the cavity Ratio of the distance l M between the center of area of the body cross section and the inlet dimension G
l M /G is set to 1.5 or more, and one end surface of the U-shaped conductor piece is in contact with the second wall surface.
コ字状導体片はドアとは別にベルト状金属板か
ら一体形成されたものである。 The U-shaped conductor piece is integrally formed from a belt-shaped metal plate separately from the door.
作 用
上記のように構成することにより、コ字状導体
片により漏洩しようとする電波は伝送モードのう
ち波長が最も短いTEM波としてロ字状断面の空
胴共振器内に導びき入れられる。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とから成る
並列共振素子を形成する。空胴の入口を小さくす
るほど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。ロ字
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。
さらに、コ字状金属片はドアと別に形成されるた
め、コ字状導体片とドアとは材質、板厚、加工工
程等をそれぞれコスト的に有利なものを選定する
ことができる。Operation With the above configuration, radio waves that are about to leak through the U-shaped conductor piece are guided into the cavity resonator with a square-shaped cross section as a TEM wave with the shortest wavelength among the transmission modes. 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. do. The smaller the entrance of the cavity, the larger C becomes, and L can be made smaller accordingly. In other words, the cross-sectional area of the cavity can be reduced. The radio wave sealing effect is maximized when each side of the square-shaped cross section is smaller than a quarter of the wavelength used.
Further, since the U-shaped metal piece is formed separately from the door, it is possible to select materials, plate thicknesses, processing steps, etc. of the U-shaped conductor piece and the door that are advantageous in terms of cost.
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。第1図およ
び第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。6は
この小穴群4の周囲を取り囲む段部で、この段部
6は小穴群4の内面に固着した透光性のドア内カ
バー15の端部が清掃の際などにはがれるのを防
ぐと共に、ドア5閉成時にフランジ2と平面接触
する封口面7の平面度を良くするものである。8
は封口面7の端部よりフランジ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はドア5とは別体で、
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
される取り付け面19と、第1の壁面8にほぼ平
行に対向する立ち上がり面23と、端部切口を第
1の壁面8に対向させた張出面11との3面から
成る。ドア5の周囲の長手方向に対する各コ字状
導体片10の幅D(第3図のx方向)は使用波長
の2分の1よりも小さくしている。又、第1の壁
面8とコ字状導体片10とで囲まれたロ字状断面
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の入口をふさぐ不透明
の誘電体カバー13から突き出した突起片14は
コ字状導体片10の立ち上がり面23に設けた取
り付け穴18に引つ掛かるようになつている。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2
0に引つ掛かるようになつている。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. 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. Reference numeral 6 denotes a stepped portion surrounding the small hole group 4, and this stepped portion 6 prevents the end portion of the translucent door inner cover 15 fixed to the inner surface of the small hole group 4 from peeling off during cleaning, etc. This improves the flatness of the sealing surface 7 that makes plane contact with the flange 2 when the door 5 is closed. 8
is 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 separate from door 5,
These are 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 that is welded to the second wall surface 9 , a rising surface 23 that faces the first wall surface 8 substantially parallel to it, and an end cut that faces the first wall surface 8 . It consists of three sides, including an overhanging surface 11. The width D (x direction in FIG. 3) of each U-shaped conductor piece 10 in the longitudinal direction of the periphery of the door 5 is made smaller than one-half of the wavelength used. Further, the square-shaped cross section surrounded by the first wall surface 8 and the U-shaped conductor piece 10 forms a cavity resonator 12 having a narrow entrance 25. A projection piece 14 protruding from an opaque dielectric cover 13 that blocks the entrance of the cavity resonator 12 is adapted to be hooked into a mounting hole 18 provided in a rising surface 23 of the U-shaped conductor piece 10. A protruding piece 17 protruding from a dielectric door frame 24 for holding a translucent door outer cover 16 covering the front surface of the door 5 is located at the outermost peripheral edge 2 of the second wall surface 9.
It seems to be stuck at 0.
次に上記のように構成した実施例の作用効果を
説明する。加熱室1開口部を取り囲むフランジ2
と封口面7との平面接触部に向かう入射電波に対
して、第4図のような簡易等価回路によつて定性
的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
は平行板のギヤツプに反比例するので容量21は
上記平面接触部のギヤツプが小さいほど大きくな
り、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とで形成されたロ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l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lは30.6mm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。 Next, the effects of the embodiment configured as described above will be explained. Flange 2 surrounding heating chamber 1 opening
The radio wave sealing effect will be qualitatively explained using a simple equivalent circuit as shown in FIG. 21 is a capacity corresponding to the planar contact portion between the flange 2 and the sealing surface 7;
It acts as a kind of bypass capacitor. The planar contact portion is considered to be a parallel plate line, and since the capacity of this line is inversely proportional to the gap of the parallel plates, the capacitance 21 becomes larger as the gap of the planar contact portion is smaller, and the radio wave sealing effect increases. Since the width D (x direction in FIG. 3) of the U-shaped conductor piece 10 is made smaller than one-half of the wavelength used, a The traveling direction of the radio waves entering the cavity resonator 12 having a rectangle-shaped cross section is limited to the yz plane of FIG. 3. If there is no overhanging surface 11, the electric field will be distributed as shown in Figure 6, and the length l of the parallel plate line will cause parallel resonance at about one quarter 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, l is 30.6 mm, and if you try to mount this on a door, it will be thick, which is disadvantageous both in terms of design and cost.
本実施例のように、張出面11を設けてロ字状
断面を持ち狭小な入口25を有する空胴共振器1
2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つて
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
子として表わされている。等価インダクタンスL
は、近似的に空胴共振器12と同じ断面の1巻き
の筒状コイルとして働き、そのコイルの定数とし
ての等価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。また、等価容量Cは空胴共振器12の入口2
5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。 As in this embodiment, a cavity resonator 1 is provided with an overhanging surface 11, has a square-shaped cross section, and has a narrow entrance 25.
2, the electric field distribution will be as shown in FIG. In this case, most of the electric lines of force are gathered between the vicinity of the end cut of the overhanging surface 11 and the first wall surface 8. Cavity resonator 12 is represented in FIG. 4 as a parallel resonant element consisting of an equivalent inductance L and an equivalent capacitance C. equivalent inductance L
acts as a one-turn cylindrical coil with approximately the same cross section as the cavity resonator 12, and means the equivalent inductance as a constant of the coil, and is the value per unit length in the cylindrical axis direction (x direction). becomes as shown in equation (1). In addition, the equivalent capacitance C is the inlet 2 of the cavity resonator 12.
It is based on the turbulent electric field around 5, and is approximately given by equation (2).
L=μ0AB ……(1)
C=(2/πloge√2elM/G−K)ε0 ……(2)
ここで
AB:空胴共振器12のロ字状断面の面積
μ0:空胴共振器12内の媒質の透磁率
e:2.72
lM:空胴共振器12の入口25と空胴断面の
面積中心Oとの距離
ε0:空胴共振器12内の媒質の誘電率
K: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0は(3)式で表わせ
る。 L=μ 0 AB ...(1) C=(2/πloge√2el M /G-K)ε 0 ...(2) where AB: Area of the square-shaped cross section of the cavity resonator 12 μ 0 : Magnetic permeability of the medium inside the cavity resonator 12 e: 2.72 l M : Distance between the entrance 25 of the cavity resonator 12 and the center of area O of the cavity cross section ε 0 : Permittivity of the medium inside the cavity resonator 12 K: Correction term related to the shape of the vicinity of the entrance 25 G: Gap of the entrance 25 (entrance dimension) The resonance frequency 0 of the cavity resonator 12 can be expressed by equation (3).
0=1/2π√LC ……(3)
(2)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0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)式からわかる。
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のロ字状断面の面積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G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を小さくし、一定
の共振周波数0(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。 0 = 1/2π√LC ...(3) From equation (2), the smaller the gap G of the inlet 25, the more
Alternatively, it can be seen that as l M /G increases, the equivalent capacitance C increases. Assuming that the resonance frequency 0 is constant, it can be seen from equation (3) that the larger the equivalent capacitance C is, the smaller the equivalent inductance L is.
In order to reduce the equivalent inductance L, the area AB of the rectangle-shaped cross section of the cavity resonator 12 can be reduced from equation (1). That is, in order to make the cavity resonator 12 smaller, the gap G between the entrances 25 is narrowed to increase the equivalent capacitance C, and the cavity area AB is correspondingly reduced to reduce the equivalent inductance L, which is constant. Resonant frequency 0 (heating frequency of high frequency heating device)
Then, by causing parallel resonance, the impedance at the entrance 25 can be maximized 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2mm、張出面11と封口面7との
段差を3mm、コ字状導体片の幅Dを15mmとし、水
275mlを加熱してドア5の周囲から5cm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AB=15.4×15.9mm、lM/G=2.1で、電波漏洩
量が0.1mW/cm2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=20.4×18.4mm、lM/G=1.75という
ようにロ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4〜8mm位と
狭小にしてlM/Gを1.5以上にすることにより、ロ字
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30.6mmより
もかなり小さくできることが明らかとなつてい
る。 In a high-frequency heating device with a heating frequency of 2450MHz and a high-frequency output of 500W, the flange 2 and the sealing surface 7
The gap between
I heated 275ml and measured the amount of radio wave leakage at a distance of 5cm from around Door 5. As a result, G=5mm
When AB = 15.4 x 15.9 mm, l M /G = 2.1, the amount of radio wave leakage is 0.1 mW/cm 2 or less, and if G = 8 mm, it is necessary to suppress the amount of radio wave leakage to the same level as above. The area of the square cross section is also large, as AB = 20.4 x 18.4 mm and l M /G = 1.75. Through such experiments, by narrowing the gap G of the inlet 25 to about 4 to 8 mm and increasing l M /G to 1.5 or more, the dimensions A and B of the cavity resonator 12 having a rectangular cross section can be respectively reduced. It has become clear that it can be made much smaller than 30.6 mm, which is a quarter of the wavelength λ used.
空胴共振器12の4辺のうち3辺を占めるコ字
状導体片10は、細いベルト状の金属板に周期的
な切り欠きを入れ、次に2か所の曲げ工程を行う
ことにより製作される。2箇所の曲げは同一方向
であるため、1工程で行うことができる。このよ
うにコ字状導体片10は形状が単純で、加工性が
よい。また、コ字状導体片10は取り付け面19
を除く他の2面に切り欠きがあるため、取り付け
面19を下部に置いたとき、重心の位置が低い。
そのため、第2の壁面9に安定して設置でき、隣
合う導体片10の間の切り欠きを通して溶接棒を
挿入し、第2の壁面9へ容易に溶接することがで
きる。1枚の金属板から一体形成したドア5と、
ベルト状金属板から形成したコ字状導体片10
は、材質、板厚加工工程等をそれぞれコスト的に
有利なものを選べる。たとえば、強度を大きくす
る必要のある大形のドアは板厚を0.8mmとし、誘
電体カバー13とドア外枠24で囲まれて外力か
ら保護されているコ字状導体片10は板厚を0.6
mmとして量産化が可能である。 The U-shaped conductor piece 10 that occupies three of the four sides of the cavity resonator 12 is manufactured by making periodic notches in a thin belt-shaped metal plate and then performing a bending process in two places. be done. Since the two locations are bent in the same direction, they can be performed in one step. As described above, the U-shaped conductor piece 10 has a simple shape and good workability. Further, the U-shaped conductor piece 10 is attached to the mounting surface 19.
Since there are notches on the other two sides, the center of gravity is low when the mounting surface 19 is placed at the bottom.
Therefore, it can be stably installed on the second wall surface 9, and a welding rod can be inserted through the notch between adjacent conductor pieces 10 to easily weld to the second wall surface 9. A door 5 integrally formed from a single metal plate,
U-shaped conductor piece 10 formed from a belt-shaped metal plate
The material, plate thickness processing process, etc. can be selected to be cost-effective. For example, a large door that requires increased strength should have a plate thickness of 0.8 mm, and the U-shaped conductor piece 10, which is surrounded by the dielectric cover 13 and door frame 24 and protected from external forces, should have a plate thickness of 0.8 mm. 0.6
Mass production is possible as mm.
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ロ字状断面の空胴
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lM/G≧1.5のように寸法を選びんだので、
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、更にコ字状導体片の一端面を第2の
壁面に接触させる構成としたので組立が容易とな
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。さらに、コ字状金属片は単純な
形状で、加工工数が少なくて済み、コスト的に有
利であり、溶接時の設置性がよいので、第2の壁
面への溶接作業が容易である。Effects of the Invention As described above, according to the present invention, the entrance of a cavity resonator having a rectangle-shaped cross section surrounded by a large number of U-shaped conductor pieces and the first wall surface is connected to the overhanging surface of the U-shaped conductor piece. Since the end cut and the first wall face each other and are narrow, and the dimensions are selected such that l M /G ≧ 1.5, the cross-sectional dimensions A and B of the cavity are set to the wavelength λ used. The resonant cavity can be made smaller than one-fourth of the original size, and the shape of the resonant cavity is simple.Furthermore, one end surface of the U-shaped conductor piece is in contact with the second wall surface, making it easy to assemble and making the door more compact. , it is possible to provide a thinner and more compact high-frequency heating device, and it also has great economic ripple effects. Further, the U-shaped metal piece has a simple shape, requires fewer processing steps, is advantageous in terms of cost, and is easy to install during welding, so welding to the second wall surface is easy.
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図は第1図におけるxyz方向を示す図、
第4図はドア5の電波シール部の簡易等価回路
図、第5図は同電波シール部の電界分布図、第6
図は同終端を短絡した平行板線路の電界分布図、
第7図は従来の電波シール構造を示す構成説明
図、第8図は同電界方向を示す図である。
1……加熱室、2……フランジ、4……小穴
群、5……ドア、6……段部、7……封口面、8
……第1の壁面、9……第2の壁面、10……コ
字状導体片、11……張出面、12……空胴共振
器、19……取り付け面、23……立ち上がり
面、25……入口、lM……空胴共振器12の入口
25と空胴断面の面積中心Oとの距離、G……入
口寸法。
FIG. 1 is a perspective view of a main part showing only the metal part of a door 5 of a high-frequency heating device according to an embodiment of the present invention;
The figure is a sectional view of the main part showing the radio wave seal part around the door, Figure 3 is a diagram showing the xyz direction in Figure 1,
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 a diagram of the electric field distribution of the radio wave seal part of the door 5.
The figure is an electric field distribution diagram of a parallel plate line with the same terminal short-circuited.
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. 1... Heating chamber, 2... Flange, 4... Small hole group, 5... Door, 6... Step, 7... Sealing surface, 8
... first wall surface, 9 ... second wall surface, 10 ... U-shaped conductor piece, 11 ... overhanging surface, 12 ... cavity resonator, 19 ... mounting surface, 23 ... rising surface, 25...Inlet, l M ...Distance between the inlet 25 of the cavity resonator 12 and the center of area O of the cavity cross section, G...Inlet dimension.
Claims (1)
洩電波防止用の空胴共振器12を設けた高周波加
熱装置において、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とを一枚の金属
板から一体形成し、この第2の壁面9にドア5の
周囲の長手方向に使用波長の2分の1よりも小さ
く分割した多数のコ字状導体片10を固着し、第
1の壁面8とコ字状導体片10とにより各辺がい
ずれも使用波長の4分の1よりも小さいロ字状断
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lMと、入口寸法Gとの距離の比(lM/
G)を1.5以上とし、コ字状導体片10はドア5
とは別にベルト状金属板から一体形成されたもの
で、第2の壁面に固着する取り付け面19と、第
1の壁面8にほぼ平行に対向する立ち上がり面2
3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面からなり、空胴共振器12の入口
25は張出面11の端部切口と第1の壁面8とを
対向させて形成したことを特徴とする高周波加熱
装置。1 In a high-frequency heating device in which a cavity resonator 12 for preventing leakage radio waves is provided at the periphery of a door 5 that opens and closes the opening of the heating chamber 1, the cavity resonator 12 is located at the periphery of the door 5 and when the opening of the heating chamber 1 is closed. a sealing surface 7 that is in planar contact with the flange 2; a first wall surface 8 that is approximately perpendicular to the flange 2 from the end of the sealing surface 7;
A second wall surface 9 that is substantially perpendicular to the wall surface 8 is integrally formed from a single metal plate, and this second wall surface 9 is divided in the longitudinal direction of the periphery of the door 5 into smaller parts than half of the wavelength used. A large number of U-shaped conductor pieces 10 are fixed together, and the first wall surface 8 and the U-shaped conductor pieces 10 form a rectangle-shaped cross section in which each side is smaller than one-fourth of the wavelength to be used. A cavity resonator 12 having an inlet 25 is formed, and the ratio of the distance l M between the inlet 25 and the center of area O of the cavity cross section to the inlet dimension G (l M /
G) is 1.5 or more, and the U-shaped conductor piece 10 is connected to the door 5.
Separately from this, it is integrally formed from a belt-shaped metal plate, and includes a mounting surface 19 that is fixed to the second wall surface, and a rising surface 2 that faces the first wall surface 8 substantially in parallel.
3 and an overhanging surface 11 whose end cut faces the first wall surface 8 . A high-frequency heating device characterized in that they are formed facing each other.
Priority Applications (6)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP61215371A JPS6372095A (en) | 1986-09-12 | 1986-09-12 | Radio frequency heater |
| GB8718229A GB2196520B (en) | 1986-08-07 | 1987-07-31 | Microwave heating apparatus |
| DE19873726002 DE3726002A1 (en) | 1986-08-07 | 1987-08-05 | DOOR GASKET FOR A MICROWAVE OVEN |
| KR1019870008619A KR900008074B1 (en) | 1986-08-07 | 1987-08-06 | Ultra High Frequency Heating Device |
| FR8711322A FR2602626B1 (en) | 1986-08-07 | 1987-08-07 | ELECTROMAGNETIC SEAL FOR MICROWAVE HEATING DEVICE DOOR, AND HEATING DEVICE HAVING SUCH AN ARRANGEMENT |
| US07/082,471 US4868359A (en) | 1986-08-07 | 1987-08-07 | Radiation sealed door in a microwave heating apparatus |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP61215371A JPS6372095A (en) | 1986-09-12 | 1986-09-12 | Radio frequency heater |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS6372095A JPS6372095A (en) | 1988-04-01 |
| JPH0569277B2 true JPH0569277B2 (en) | 1993-09-30 |
Family
ID=16671187
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP61215371A Granted JPS6372095A (en) | 1986-08-07 | 1986-09-12 | Radio frequency heater |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS6372095A (en) |
Family Cites Families (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS50142546U (en) * | 1974-05-13 | 1975-11-25 | ||
| JPS59230291A (en) * | 1983-06-07 | 1984-12-24 | 松下電器産業株式会社 | Radio wave seal device |
| JPS6343287A (en) * | 1986-08-07 | 1988-02-24 | 株式会社日立ホームテック | Radio frequency heater |
-
1986
- 1986-09-12 JP JP61215371A patent/JPS6372095A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS6372095A (en) | 1988-04-01 |
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