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JPS602756B2 - High frequency heating device - Google Patents
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JPS602756B2 - High frequency heating device - Google Patents

High frequency heating device

Info

Publication number
JPS602756B2
JPS602756B2 JP5644780A JP5644780A JPS602756B2 JP S602756 B2 JPS602756 B2 JP S602756B2 JP 5644780 A JP5644780 A JP 5644780A JP 5644780 A JP5644780 A JP 5644780A JP S602756 B2 JPS602756 B2 JP S602756B2
Authority
JP
Japan
Prior art keywords
resonator
dielectric resonator
door
radio wave
mode
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
Application number
JP5644780A
Other languages
Japanese (ja)
Other versions
JPS56152192A (en
Inventor
美夫 安岡
茂 駒井
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Sanyo Electric Co Ltd
Original Assignee
Sanyo Electric Co Ltd
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Sanyo Electric Co Ltd filed Critical Sanyo Electric Co Ltd
Priority to JP5644780A priority Critical patent/JPS602756B2/en
Publication of JPS56152192A publication Critical patent/JPS56152192A/en
Publication of JPS602756B2 publication Critical patent/JPS602756B2/en
Expired legal-status Critical Current

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  • Constitution Of High-Frequency Heating (AREA)

Description

【発明の詳細な説明】 本発明は加熱室を有する高周波加熱装置に関し、特に、
上記加熱室関口周辺からの電波漏洩を簡単な構造にて有
効に抑止せんとするものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a high frequency heating device having a heating chamber, and in particular,
The purpose is to effectively suppress radio wave leakage from the vicinity of the heating chamber entrance with a simple structure.

従来この種電波漏洩を抑止する構造として、加熱室関口
周辺に入/4長(入は漏洩電波の実効波長)の共振空洞
からなるいわゆるチョーク構造を設けることが知られて
いる。
Conventionally, as a structure for suppressing this type of radio wave leakage, it is known to provide a so-called choke structure consisting of a resonant cavity with an input/4 length (input is the effective wavelength of the leaked radio waves) around the entrance of the heating chamber.

然るに斯るチョーク構造はかなりの空洞体積を要するの
で、たとえばそれを加熱室関口を開閉するドアに設けた
場合ドア厚が大になるという欠点がある。本発明は斯る
欠点に鑑みてなされたもので、加熱室閉口周辺の電波漏
洩通路に漏洩電波の共振寸法関係にある誘電体共振器構
造体を配置すると共に、該構造体を複数のTEモード誘
電体共振器から構成したことを特徴とするもので、本発
明に従えば従来の様なチョーク構造を用いることなく有
効に電波漏洩の抑止をなすことができ、又本発明による
誘電体共振器機造体をドアに設けた場合にもドア厚が大
きくなることはない。
However, since such a choke structure requires a considerable cavity volume, it has the disadvantage that, for example, when it is provided in a door for opening and closing a heating chamber entrance, the door thickness becomes large. The present invention has been made in view of these drawbacks, and includes arranging a dielectric resonator structure having a resonance dimension relationship with leakage radio waves in the radio wave leakage path around the closing of the heating chamber, and using the structure in a plurality of TE modes. According to the present invention, radio wave leakage can be effectively suppressed without using a conventional choke structure, and the dielectric resonator device according to the present invention is Even when the structure is provided on the door, the thickness of the door does not increase.

上記議電体共振器は、電波伝播路内に誘電体を配し、そ
の形状を電波の共振寸法関係になせば譲曙体自身が共振
器の作用をなすものである。
In the electromagnetic body resonator described above, a dielectric body is disposed within the radio wave propagation path, and if its shape is set in relation to the resonance dimensions of the radio waves, the dielectric body itself acts as a resonator.

斯る原理自体はマイクロ波通信技術の分野において既に
知られているが、この様なマイクロ波弱ェネルギを扱う
通信技術とは異なりマイクロ波強ェネルギを扱う高周波
加熱装置においてその電波漏洩抑止のために誘電体共振
器が有効に作用することは従釆全く認識されていない。
本発明の新規な思想は、高周波加熱装置の電波漏洩防止
のために誘電体共振器を適用し、従来のチョーク構造に
代わる電波漏洩防止効果を達成できたことである。
This principle itself is already known in the field of microwave communication technology, but unlike communication technology that handles weak microwave energy, it is used to prevent radio wave leakage in high-frequency heating equipment that handles strong microwave energy. It has not yet been recognized that dielectric resonators work effectively.
The novel concept of the present invention is that a dielectric resonator is applied to prevent radio wave leakage in a high-frequency heating device, and the radio wave leakage prevention effect can be achieved in place of the conventional choke structure.

一方誘電体共振器はTEモード又はTMモードの何れか
で共振するが高周波加熱装置の電波漏洩防止のためには
TEモ−ドが好適であることが判明した。
On the other hand, a dielectric resonator resonates in either the TE mode or the TM mode, and it has been found that the TE mode is suitable for preventing radio wave leakage in a high frequency heating device.

即ちTMモードの場合、ドアを開放するに従い誘電体共
振器の共振周波数が大きく変化し、従って電波漏洩防止
が不完全なものとなる。TMモードの場合共振周波数が
大きく変化する原因は詳らかではないが、このモードの
場合、共振状態での電気力線は共振器より外方にも存在
し、よって高周波加熱装置のドア開閉に伴って金属製の
ドア壁面と本体壁面との間隔が変化して誘電体共振器近
辺の導体配置が変化すると、特に電気力線がその影響を
受けて共振周波数が変化するものと考えられ、この点T
Eモードでは電気力線が共振器内部にとじ込ゆられてい
るのでドア開閉による共振周波数の変化は少ないと推論
される。第1図、第2図は実施例装置としての電子レン
ジを示し、1は加熱室、2は該加熱室を空間的に限定す
る金属製本体、3は加熱室1前面の方形状閉口を開閉す
るドアである。ドア3は中央透視窓を有する金属製ドァ
枠4と該ドア枠の中央透視窓に固着され、透視用紬孔を
多数有する金属製透視板40とを備えている。ドア3は
図では省略されているが、その右端側にヒンジを有し、
該ヒンジを中心に左端側が回動する。
That is, in the case of the TM mode, the resonant frequency of the dielectric resonator changes greatly as the door is opened, and therefore prevention of radio wave leakage becomes incomplete. The reason for the large change in the resonance frequency in the TM mode is not clear, but in this mode, the lines of electric force in the resonance state exist outside the resonator. When the distance between the metal door wall and the main body wall changes and the conductor arrangement near the dielectric resonator changes, it is thought that the electric lines of force will be particularly affected and the resonant frequency will change.
In E mode, the lines of electric force are confined and swayed inside the resonator, so it can be inferred that there is little change in the resonant frequency due to opening and closing of the door. Figures 1 and 2 show a microwave oven as an example device, where 1 is a heating chamber, 2 is a metal body that spatially limits the heating chamber, and 3 is a rectangular closure in front of the heating chamber 1 that opens and closes. This is the door that opens. The door 3 includes a metal door frame 4 having a central see-through window, and a metal see-through plate 40 fixed to the center see-through window of the door frame and having a large number of see-through holes. Although the door 3 is omitted in the figure, it has a hinge on its right end side,
The left end side rotates around the hinge.

第1図はドア開状態を、又第2図は同じく少量開放状態
を夫々示している。閉ドア時にはドア枠4の平坦部4a
が本体2の前面2aと対藤し、従って斯る対藤部に電波
漏洩通路が形成され、該通路に本発明の特徴となる誘電
体共振器機造体5が配されている。尚図では一部のみを
示しているが斯る配置は加熱室1の方形状関口の全周に
百つて同様である。誘電体共振器機造体5は個々の誘電
体共振器5a,5a,・・・・・・・・・を加熱室関口
の周辺に沿ってドァ枠の平坦部4aに複数個配列固着し
たものである。
FIG. 1 shows the door in the open state, and FIG. 2 shows the door in the slightly opened state. When the door is closed, the flat part 4a of the door frame 4
faces the front surface 2a of the main body 2, and therefore a radio wave leakage path is formed in this facing portion, and the dielectric resonator structure 5, which is a feature of the present invention, is disposed in the path. Although only a portion is shown in the figure, this arrangement is the same all around the rectangular entrance of the heating chamber 1. The dielectric resonator mechanism 5 has a plurality of individual dielectric resonators 5a, 5a, . It is.

具体的には各譲竜体共振器5aは高さA、幅B、長さC
の直方体状議電体板で構成され、その長さ方向が加熱室
開□縁方向と垂直な方向、即ち図中X方向に一致する配
置にて一定間隔で配列されている。重要なことは、上記
誘電体共振器は漏洩電波に対して、TEモードで共振す
べく上記各寸法A,B,Cが決められていることである
。第3図は高さ泌、幅B、長さCを有するTEモード型
誘導体共振器5aのTEm6モードでの共振状態におけ
る電気力線6及び磁力線7の分布状態を示し、図から明
らかな如く、伝搬してくる電波の磁界が共振モード‘こ
おける磁力線7の合成方向、即ち共振器の幅方向(図中
Y方向)に成分を有すれば漏洩電波は共振的に誘電体共
振器5aと結合しその進行ェネルギが大きく減衰する。
又共振モード‘こおける電気力線6は誘電体共振器5a
内部の垂直面内で閉じたループを形成し、、従ってイメ
ージ理論により共振器5aの半分の高さの水平面に導体
板8を挿入しても電気力線6は導体に垂直に交わるから
その分布に何ら影響がなく、従って導体板8上に誘電体
共振器5aを設置する場合には該共振器の高さは半分の
Aでよいことになる。こ)に本実施例における誘電体共
振器5aは、ドア枠平坦部4aが上記導体板8に相当し
、TEo,6モードで共振するものであり、漏洩電波が
加熱室関口縁方向、即ち図中Y方向に一致する磁界成分
を有すれば斯る漏洩電波は共振器5aの存在により大き
く減衰し、外部に達し得ない。
Specifically, each dragon body resonator 5a has a height A, a width B, and a length C.
The heating chamber is made up of rectangular parallelepiped-shaped electrical body plates, which are arranged at regular intervals so that the length direction thereof coincides with the direction perpendicular to the opening edge direction of the heating chamber, that is, the X direction in the figure. What is important is that the dimensions A, B, and C of the dielectric resonator are determined so that the dielectric resonator resonates in the TE mode against leakage radio waves. FIG. 3 shows the distribution of electric lines of force 6 and magnetic lines of force 7 in the TEm6 mode resonance state of the TE mode type dielectric resonator 5a having height, width B, and length C, and as is clear from the figure, If the magnetic field of the propagating radio wave has a component in the composite direction of the magnetic lines of force 7 in the resonance mode, that is, in the width direction of the resonator (Y direction in the figure), the leaked radio wave will be resonantly coupled to the dielectric resonator 5a. The traveling energy of the shinobi is greatly attenuated.
Also, the electric lines of force 6 in the resonance mode' are the dielectric resonator 5a.
A closed loop is formed in the internal vertical plane, and therefore, according to image theory, even if the conductor plate 8 is inserted in a horizontal plane at half the height of the resonator 5a, the lines of electric force 6 intersect perpendicularly to the conductor, so its distribution is Therefore, when the dielectric resonator 5a is installed on the conductor plate 8, the height of the resonator only needs to be half A. 2) In the dielectric resonator 5a of this embodiment, the door frame flat portion 4a corresponds to the conductor plate 8, and resonates in the TEo,6 mode, so that the leakage radio waves are directed toward the heating chamber entrance edge, that is, in the figure. If the magnetic field components match in the middle Y direction, such leakage radio waves will be greatly attenuated by the presence of the resonator 5a and will not be able to reach the outside.

上記議電体共振器5aとしては、列えば比護電率ごsが
90のチタン酸バリウムを主成分とする譲亀体で成形さ
れ、各寸法はA=7.5肋、8=6胸、C=11.5柳
であり、その取付は共振器裏面を予めメタラィズしてお
き、斯る裏面をドア枠平坦部4aにはんだ付けあるいは
ロー付けすることにより行なわれる。更に上記誘電体共
振器5a,5a………の配置間隔1を例えば30肋とす
ると共に「閉ドア時の本体前面2aとドア枠平坦部4a
との距離を例えば10.5柳とする。第4図及び第5図
は上記誘電体共振器5aの配列状態を変更した他の実施
例を示し、第2図に示山た座標系にて表わすと、第4図
の場合は各共振器5aをその長さ方向が×方向とY方向
とに交互になるべく配置しており、第5図の場合には同
じくその長さ方向を×、Y各方向に対しては)、45度
に配置している。
The electromagnetic body resonator 5a is formed of a compact body mainly composed of barium titanate with a specific electrical constant S of 90, and each dimension is A=7.5 ribs, 8=6 ribs. , C=11.5 willow, and its attachment is carried out by metallizing the back surface of the resonator in advance and soldering or brazing the back surface to the flat portion 4a of the door frame. Further, the arrangement interval 1 of the dielectric resonators 5a, 5a, .
For example, let the distance between the two points be 10.5 willows. 4 and 5 show other embodiments in which the arrangement state of the dielectric resonators 5a is changed, and when expressed in the coordinate system shown in FIG. 2, in the case of FIG. 4, each resonator 5a are arranged with their length directions alternately in the are doing.

このとき、第4図及び第5図において面間距離にて表わ
される共振器の配置間隔1は夫々2仇廠及び3仇奴とす
る。これらの場合にはY方向の磁界成分を有する漏洩電
波の他、×方向の磁界成分を有する漏洩電波も減衰され
より確実な電波漏洩抑止効果がある。以上の説明より明
らかな如く、本発明によればTEモード誘電体共振器を
複数個配列した頗る簡単な構造にて電波漏洩を有効に抑
止することができ、又従来の如きチョーク構造が不要と
なるのでドア厚も薄くできる。
At this time, the arrangement interval 1 of the resonators expressed by the inter-plane distance in FIGS. 4 and 5 is assumed to be 2 and 3, respectively. In these cases, in addition to leaked radio waves having a magnetic field component in the Y direction, leaked radio waves having a magnetic field component in the x direction are also attenuated, resulting in a more reliable radio wave leakage prevention effect. As is clear from the above explanation, according to the present invention, radio wave leakage can be effectively suppressed with a very simple structure in which a plurality of TE mode dielectric resonators are arranged, and the conventional choke structure is not required. Therefore, the door thickness can be made thinner.

尚本発明は従来の抑止構造と併用できることは勿論であ
り、又誘電体共振器機造体を本体側に設けても同等の効
果が得られる。
It goes without saying that the present invention can be used in combination with the conventional deterrent structure, and the same effect can be obtained even if the dielectric resonator mechanism is provided on the main body side.

【図面の簡単な説明】[Brief explanation of drawings]

第1図は本発明実施例の菱部断面図、第2図は同斜視図
、第3図は譲露体共振器の共振状態を示す斜視図、第4
図及び第6図は他の実施例における誘電体共振器配列を
示す平面図である。 5a・・・・・・謎電体共振器。 第1図 第2図 第3図 第4図 第5図
FIG. 1 is a cross-sectional view of the lozenge portion of an embodiment of the present invention, FIG. 2 is a perspective view thereof, FIG. 3 is a perspective view showing the resonant state of the resonator, and FIG.
This figure and FIG. 6 are plan views showing a dielectric resonator arrangement in another embodiment. 5a...Mysterious electric resonator. Figure 1 Figure 2 Figure 3 Figure 4 Figure 5

Claims (1)

【特許請求の範囲】[Claims] 1 加熱室開口周辺の電波漏洩通路に漏洩電波の共振寸
法関係にある誘電体共振器機造体を配置してなる高周波
加熱装置において、上記誘電体共振器機造体は複数のT
Eモード誘電体共振器からなる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 dielectric resonator structure having a resonance dimension for leakage radio waves is arranged in a radio wave leakage path around the opening of the heating chamber, the dielectric resonator structure has a plurality of T.
A high-frequency heating device comprising an E-mode dielectric resonator.
JP5644780A 1980-04-28 1980-04-28 High frequency heating device Expired JPS602756B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP5644780A JPS602756B2 (en) 1980-04-28 1980-04-28 High frequency heating device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP5644780A JPS602756B2 (en) 1980-04-28 1980-04-28 High frequency heating device

Publications (2)

Publication Number Publication Date
JPS56152192A JPS56152192A (en) 1981-11-25
JPS602756B2 true JPS602756B2 (en) 1985-01-23

Family

ID=13027341

Family Applications (1)

Application Number Title Priority Date Filing Date
JP5644780A Expired JPS602756B2 (en) 1980-04-28 1980-04-28 High frequency heating device

Country Status (1)

Country Link
JP (1) JPS602756B2 (en)

Also Published As

Publication number Publication date
JPS56152192A (en) 1981-11-25

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