JP2949965B2 - Radio wave sealing device - Google Patents
Radio wave sealing deviceInfo
- Publication number
- JP2949965B2 JP2949965B2 JP28265391A JP28265391A JP2949965B2 JP 2949965 B2 JP2949965 B2 JP 2949965B2 JP 28265391 A JP28265391 A JP 28265391A JP 28265391 A JP28265391 A JP 28265391A JP 2949965 B2 JP2949965 B2 JP 2949965B2
- Authority
- JP
- Japan
- Prior art keywords
- conductor
- radio wave
- groove
- door
- wall surface
- 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 - Fee Related
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)
- Electric Ovens (AREA)
Description
【発明の詳細な説明】DETAILED DESCRIPTION OF THE INVENTION
【0001】[0001]
【産業上の利用分野】本発明は高周波電波を供給する本
体とドアとの間から漏洩する恐れがある高周波電波を遮
断する電波シール装置に関する。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a radio wave sealing device for blocking a high frequency radio wave which may leak from a main body supplying a high frequency radio wave and a door.
【0002】[0002]
【従来の技術】近年、電子レンジなどの高周波により食
品を加熱して調理する機器はドアの厚さを薄くすること
が求められている。2. Description of the Related Art In recent years, it has been required to reduce the thickness of a door of a device such as a microwave oven that heats and cooks food by high frequency.
【0003】従来、この種の機器の電波シール装置は図
6〜図8に示すような構成が一般的であった。以下、そ
の構成について説明する。図に示すように、加熱室本体
1は食品を収納して高周波加熱するもので、この加熱室
本体1の食品出し入れの開口部をドア2により開閉自在
に覆うようにしており、加熱室本体1の高周波電磁波が
加熱室本体1外へ漏洩して人体に弊害を及ぼさないよう
に電波シール対策が施されている。従来の電波シールの
第一の方法としては、導体部だけを示すと図7に示すよ
うなインピーダンス反転を利用する方法があった。図7
(a)のようにドア2側の溝の深さA−B間の長さを加
熱室本体1内の電波の4分の1波長分の長さとして、電
波を減衰させるのである。すなわち、(以下、チョーク
部という)3の特性インピーダンスをZ0、深さをLと
し、終端部を短絡したときにチョーク部開口部Bでのイ
ンピーダンスZinは、 Zin=j・Z0・tan (2・χ・L/λ0)(λ0は自
由空間波長) となる。チョーク方式の電波減衰手段は、チョーク部3
の深さLを4分の1波長に選定することにより、 |Zin|=Z0・tan (π/2)=∞ を達成するという原理に基づいている。よって、図7
(a)をα側から見た図7(b)において、開放端の先
端部5に破線で示したようにインピーダンス無限大の領
域が発生し、電波が外部に出られなくなる。もし、チョ
ーク部3内に誘電体(比誘電率εr)を充填すると、電
波の波長λ’は、Conventionally, a radio wave sealing device for this type of equipment generally has a configuration as shown in FIGS. Hereinafter, the configuration will be described. As shown in the figure, a heating chamber main body 1 stores food and performs high-frequency heating, and the food chamber opening and closing opening of the heating chamber main body 1 is opened and closed by a door 2. In order to prevent the high frequency electromagnetic wave from leaking out of the heating chamber main body 1 and exerting an adverse effect on the human body, a radio wave sealing measure is taken. As a first method of a conventional radio wave seal, there has been a method using impedance inversion as shown in FIG. 7 when only a conductor portion is shown. FIG.
The radio wave is attenuated by setting the length between the depths A and B of the groove on the door 2 side as the length of a quarter wavelength of the radio wave in the heating chamber main body 1 as shown in FIG. That is, the characteristic impedance (hereinafter referred to as a choke portion) 3 is Z0, the depth is L, and when the terminal portion is short-circuited, the impedance Zin at the choke portion opening B is as follows: Zin = j · Z0 · tan (2 · χ · L / λ0) (λ0 is a free space wavelength). The choke type radio wave attenuating means includes a choke unit 3
Is selected to be a quarter wavelength to achieve | Zin | = Z0 · tan (π / 2) = ∞. Therefore, FIG.
In FIG. 7B in which FIG. 7A is viewed from the α side, an infinite impedance region is generated at the distal end 5 of the open end as shown by a broken line, and radio waves cannot be emitted to the outside. If the choke 3 is filled with a dielectric (relative permittivity εr), the wavelength λ ′ of the radio wave becomes
【0004】[0004]
【化1】 Embedded image
【0005】に圧縮される。この場合、チョーク部3の
深さL’は、[0005] In this case, the depth L 'of the choke 3 is
【0006】[0006]
【化2】 Embedded image
【0007】と短くなる。しかしながらL’がλ’の4
分の1であることに変わりはなく、チョーク方式におい
ては、深さを実質的に4分の1波長よりも小さくするこ
とができず、材料面から考えてチョーク部3の小型化
(すなわちドアを薄くすること)に限界があった。[0007] However, L 'is λ'4
In the choke method, the depth cannot be substantially reduced to less than a quarter wavelength, and the size of the choke portion 3 can be reduced from the viewpoint of the material (that is, the door may have a smaller size). Thinning) was limited.
【0008】また、電子レンジの軽量化にともないドア
2を薄くする試みとして生まれてきた電波シールの第二
の方法としては図8に示すような方法がある。図8
(a)では加熱室本体1とドア2の導体部の構成を示
し、図8(b)は図8(a)のドア部をα側から見た構
成である。チョーク構造が複雑ではあるが電波を減衰さ
せることができ、4分の1波長以下の深さが実現でき
た。FIG. 8 shows a second method of the radio wave seal which has been developed as an attempt to make the door 2 thinner with the reduction in the weight of the microwave oven. FIG.
8A shows the configuration of the conductors of the heating chamber main body 1 and the door 2, and FIG. 8B shows the configuration of the door of FIG. 8A as viewed from the α side. Although the choke structure is complicated, radio waves can be attenuated, and a depth of less than a quarter wavelength can be realized.
【0009】またマイクロストリップ線路技術を電波シ
ール装置に応用する例も過去にあった。これは本体もし
くはドアの片方をグランド面、他方を信号線路と考えて
いるため、前述のインピーダンス反転の理論を満たさな
い(すなわち、ショート面を確保できないためインピー
ダンス∞を作ることができない)物であり、電子レンジ
等にはとても利用できないものであった。(特開昭58
−9400号公報参照)In the past, there has been an example in which the microstrip line technology is applied to a radio wave sealing device. This is one that does not satisfy the above-mentioned theory of impedance inversion because one of the main body or the door is considered as the ground plane and the other as the signal line (that is, the impedance ∞ cannot be created because the short side cannot be secured). It could not be used for microwave ovens. (Japanese Patent Laid-Open No. 58
-9400)
【0010】[0010]
【発明が解決しようとする課題】このような従来の電波
シール装置では、簡単で作りやすい構成でかつドアを薄
くするということは実現できていなかった。たとえば、
電波シールの第二の方法の例として、図8に示すような
電波シール対策を施しており、ドアは薄いが、製造上一
つの導体部(たとえば板金)の折りまげだけでは作れ
ず、ドア2側の導体部(b)は第1のドア導体7と第2
のドア導体8とをスポット点9でスポット溶接して作る
などの複雑な構成となっており、作りづらく工数および
材料費の面で高価格となる課題があった。また、スポッ
ト溶接のやり方によってはばらつきが生じ、電波の漏洩
を抑え切れない場合や、抑えるにしても管理項目が多く
なるなど種種の問題を有していた。In such a conventional radio wave sealing device, it has not been possible to realize a simple and easy-to-manufacture structure and to make the door thin. For example,
As an example of the second method of the radio wave seal, a countermeasure against radio waves as shown in FIG. 8 is taken, and although the door is thin, it cannot be made only by folding one conductor portion (for example, a sheet metal) in manufacturing. The conductor part (b) on the side is composed of the first door conductor 7 and the second door conductor 7.
And the door conductor 8 is spot-welded at the spot point 9, which makes it difficult to manufacture the door conductor 8 and costs high in terms of man-hours and material costs. In addition, there is a variety of problems depending on the method of spot welding, such as the inability to suppress radio wave leakage and the increase in management items even if suppressed.
【0011】本発明は上記課題を解決するもので、ドア
を薄くしながら簡単な構成で、電波の外部への漏洩を抑
制し、安全な電波シール性能を提供することを目的とし
ている。SUMMARY OF THE INVENTION The object of the present invention is to solve the above-mentioned problems and to provide a safe radio wave sealing performance by suppressing leakage of radio waves to the outside with a simple structure while making the door thin.
【0012】[0012]
【課題を解決するための手段】本発明は上記目的を達成
するために、被加熱物の出し入れをする開口部を有し電
波が内部に供給される加熱室本体に設けた第1の導体部
と、前記加熱室本体の前記開口部を開閉自在に覆うドア
に設けた第2の導体部とを対向させ、前記第1の導体部
または第2の導体部の少なくとも一方に少なくとも一つ
の溝を設け、前記溝を形成する第1の導体壁面および溝
底面は連続的な導電性部材からなり、前記溝を形成する
第2の導体壁面は開放端から切り込み部を設けて溝の長
手方向に一定ピッチの導体片板が複数個並ぶ構成とし、
かつ前記各導体片板はそれぞれ前記溝底面と電気的に接
触し、前記第1の導体壁面との間にマイクロストリップ
線路を構成し、前記導体片板は2種類以上の異なった形
状のものを順次配列する構成としたことを課題解決手段
としている。SUMMARY OF THE INVENTION In order to achieve the above object, the present invention provides a first conductor section provided in a heating chamber main body having an opening through which an object to be heated is taken in and out, and into which a radio wave is supplied. And a second conductor provided on a door that opens and closes the opening of the heating chamber body so as to open and close, and at least one groove is formed in at least one of the first conductor and the second conductor. The first conductor wall surface and the groove bottom surface forming the groove are formed of a continuous conductive member, and the second conductor wall surface forming the groove is provided with a cutout from an open end to be constant in the longitudinal direction of the groove. A configuration in which a plurality of conductor strips of pitch are lined up,
Each of the conductor strips is in electrical contact with the bottom of the groove, and constitutes a microstrip line between the conductor strip and the first conductor wall. The conductor strips have two or more different shapes. The configuration for sequentially arranging them is a means for solving the problem.
【0013】[0013]
【作用】本発明は上記した課題解決手段により、導体片
板と第1の導体壁面の間で、溝内の媒質(空気)を基板
材料と考えマイクロストリップ線路とみなすことによ
り、導体片板の形状を自由に選べるため従来の方法に縛
られないインピーダンス反転が実現できる。すなわち、
深さ方向と溝の長手方向の合成長で4分の1波長を稼げ
ばよいことになり、深さ自身は4分の1波長より短くす
ることができる。さらに、2種類以上の異なった形状の
導体片板を順次配列するので、同じピッチ内に複数個の
マイクロストリップ線路を構成することができ、きわめ
て電波が漏れにくくできる。According to the present invention, the medium (air) in the groove is regarded as a substrate material between the conductor plate and the first conductor wall, and is regarded as a microstrip line. Since the shape can be freely selected, impedance inversion not restricted by the conventional method can be realized. That is,
It is only necessary to obtain a quarter wavelength with the combined length in the depth direction and the longitudinal direction of the groove, and the depth itself can be shorter than the quarter wavelength. Further, since two or more types of conductor strips having different shapes are sequentially arranged, a plurality of microstrip lines can be formed within the same pitch, so that radio waves can hardly leak.
【0014】[0014]
【実施例】以下、本発明の一実施例を電子レンジのドア
シールに応用した場合について図1を参照しながら説明
する。DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS An embodiment in which one embodiment of the present invention is applied to a door seal of a microwave oven will be described below with reference to FIG.
【0015】図に示すように、第1の導体部10は加熱
室本体1に設け、この第1の導体部と、ドア2に設けた
第2の導体部11とにより加熱室内空間12をふさぐよ
うにしている。第2の導体部11は、一つの導体(板
金)を折りまげるだけで作られており、第1の導体壁面
13と溝底面14と第2の導体壁面15とでチョーク部
16を形成している。また、図1(a)をα側から見た
図1(b)において、第2の導体壁面15は開放端が切
り込みが入り、溝の長手方向に一定ピッチの導体片板1
7、18が順次複数個並ぶ構成としており、第1の導体
壁面13がグラインドラインで導体片板17、18が信
号ラインと考えると、各導体片板17、18と第1の導
体壁面13の間でマイクロトスリップ線路を形成してい
ると考えることができる。ここで、第2の導体壁面15
の深さL1は、導体片板17、18の形状によって決ま
るが、これはドア2の厚みを決定するもっとも重要な要
因である。本実施例の場合、導体片板17、18は途中
から右方向に曲がっており、深さL1を4分の1波長以
下にしている。そのため、加熱室外へ漏れようとする電
波にとってのインピーダンス無限大の領域は、図7の従
来例とは少し異なった位置(開放端の先端部19に現れ
る。このとき、導体片板17、18の曲がる向きは、イ
ンピーダンス無限大が一定間隔で現れるよう右側で統一
されている。As shown in the figure, a first conductor portion 10 is provided in a heating chamber main body 1, and the first conductor portion and a second conductor portion 11 provided in a door 2 block a heating chamber space 12. Like that. The second conductor portion 11 is made by simply folding one conductor (sheet metal), and forms a choke portion 16 with the first conductor wall surface 13, the groove bottom surface 14, and the second conductor wall surface 15. I have. In FIG. 1B as viewed from the α side in FIG. 1A, the second conductor wall surface 15 has a notch at the open end, and the conductor plate 1 having a constant pitch in the longitudinal direction of the groove.
When the first conductor wall 13 is considered to be a grind line and the conductor plates 17 and 18 are considered to be signal lines, each of the conductor plates 17 and 18 and the first conductor wall 13 are arranged. It can be considered that a micro-toslip line is formed between them. Here, the second conductor wall 15
Is determined by the shapes of the conductor plates 17 and 18, and this is the most important factor that determines the thickness of the door 2. In the case of the present embodiment, the conductor pieces 17 and 18 are bent rightward from the middle, and the depth L1 is set to a quarter wavelength or less. Therefore, the region of infinite impedance for the radio wave to leak out of the heating chamber appears at a position slightly different from the conventional example in FIG. 7 (at the end portion 19 of the open end. The bending directions are unified on the right side so that infinite impedance appears at regular intervals.
【0016】ここで、導体片体17、18のピッチPに
ついて説明すると、導体片板17、導体片板18のいず
れもピッチPの間隔で並設しており、逆に言えば、一定
ピッチ内に2種類の導体片板17、18を並設してい
る。すなわち、インピーダンス無限大の位置が導体片板
17の先端と導体片板18の先端のそれぞれに現れるの
で二重に強調されることになり、電波シールの性能を向
上できる。なお、詳細は明らかでないが、ピッチPはお
およそ4分の1波長付近に最適値がある。Here, the pitch P of the conductor pieces 17 and 18 will be described. Both the conductor piece plates 17 and 18 are arranged side by side at intervals of the pitch P. , Two types of conductor piece plates 17 and 18 are arranged side by side. That is, since the position of the impedance infinity appears at each of the tip of the conductor plate 17 and the tip of the conductor plate 18, it is double-emphasized and the performance of the radio wave seal can be improved. Although the details are not clear, the pitch P has an optimum value near a quarter wavelength.
【0017】つぎに、導体片板17について図2を参照
しながら説明すると、インピーダンス無限大の領域を作
るために、マイクロストリップ線路の実行長を4分の1
波長にする必要があるが、線路幅Hの信号ラインについ
ては、センター長のトータルが実際の長さと考えられる
ので、第2の導体壁面15の深さL1と横方向の長さL
2を用いると、 L1+L2−H≒λ/4 を満たすように選ばなければならない。さらに、ピッチ
間隔P(L2と隙間Sの和)についてもおおよそ4分の
1波長を選んでいる。電子レンジの場合、発振周波数が
約2450MHz であり、波長が約120mmとなることを
考えて計算すると、H=5mm、L2=20mm、S=10
mmとすれば、L1≒15mmとなり、従来の30mmからす
れば2分の1の深さにすることができる。導体片板18
についても同様である。Next, the conductor plate 17 will be described with reference to FIG. 2. In order to create a region of infinite impedance, the effective length of the microstrip line is reduced by a quarter.
It is necessary to set the wavelength to the wavelength, but for the signal line having the line width H, since the total of the center lengths is considered to be the actual length, the depth L1 of the second conductor wall surface 15 and the lateral length L
If 2 is used, it must be selected so as to satisfy L1 + L2-H / λ / 4. Further, about the pitch interval P (the sum of L2 and the gap S), approximately a quarter wavelength is selected. In the case of a microwave oven, the oscillation frequency is about 2450 MHz and the wavelength is about 120 mm. Calculations are made to find that H = 5 mm, L2 = 20 mm, and S = 10 mm.
mm, L1 ≒ 15 mm, which can be reduced to a half of the conventional 30 mm. Conductor plate 18
The same applies to.
【0018】図3は、L1、L2を変化させた場合のド
ア部からの電波の漏洩電力の特性を示している。図3か
ら明らかなように、L2をパラメータとして極小値を与
えるL1があることがわかる。L2が大きいときは、特
性aのように極小値を与えるL1を小さくする(L1
a)ことができ、L2が小さいときは、特性bのように
極小値を与えるL1が大きくなる(L1b)ことがわか
る。FIG. 3 shows the characteristics of the leakage power of radio waves from the door when L1 and L2 are changed. As is clear from FIG. 3, it is found that there is L1 which gives a minimum value using L2 as a parameter. When L2 is large, L1 that gives the minimum value like characteristic a is reduced (L1
a) It can be seen that when L2 is small, L1 giving the minimum value like characteristic b becomes large (L1b).
【0019】つぎに、図4は、マイクロストリップ線路
を用いた場合のインピーダンスと電波漏洩の特性を示し
ている。図4(a)のように Zin=j・Z0・tan (2・χ・L/λ0)(λ0は自
由空間波長) |Zin|=Z0・tan (π/2)=∞ で与えられる通り、横軸に信号線路の実行長(L1+L
2−Hの長さ)をとると、さまざまなインピーダンスを
発生でき、実際に電波の通過のしやすさという点から絶
対値に置き換えると図4(b)のようになる。図4
(b)は、電波の通りにくさを示すものであり、逆に漏
洩する電力はというと図3で示したのと同様に図4
(c)のような特性が得られる。FIG. 4 shows characteristics of impedance and radio wave leakage when a microstrip line is used. As shown in FIG. 4A, Zin = j · Z0 · tan (2 · χ · L / λ0) (λ0 is a free space wavelength) | Zin | = Z0 · tan (π / 2) = ∞ On the horizontal axis, the execution length of the signal line (L1 + L
2−H), various impedances can be generated, and when they are replaced with absolute values from the viewpoint of easy passage of radio waves, the results are as shown in FIG. 4B. FIG.
FIG. 4B shows the degree of difficulty in passing radio waves. On the contrary, the amount of leaked power is similar to that shown in FIG.
The characteristic as shown in FIG.
【0020】また、実際のドア構成の場合には、図5の
ように第2の導体部11を裸のままにするのではなく、
樹脂や硝子などのカバー20、21を用いる場合が多
い。In the case of an actual door configuration, instead of leaving the second conductor 11 bare as shown in FIG.
In many cases, covers 20 and 21 made of resin or glass are used.
【0021】[0021]
【発明の効果】以上の実施例から明らかなように本発明
によれば、2種類以上の形状の異なる導体片板を用いて
おり、一定ピッチ内にインピーダンス無限大の部分を複
数箇所容易に作り出せるため、電波漏洩の抑制に優れき
わめて安全な電波シールを実現でき、また、マイクロス
トリップ線路技術の考え方に基づくので、導体片板の形
状が自由に選べるため、簡単な構成でドア部の厚みを薄
くでき、小型軽量化が図れる。As is apparent from the above embodiments, according to the present invention, two or more types of conductor pieces having different shapes are used, and a plurality of portions having infinite impedance can be easily formed within a fixed pitch. Therefore, it is possible to realize an extremely safe radio wave seal that is excellent in suppressing radio wave leakage, and because it is based on the concept of microstrip line technology, the shape of the conductor single plate can be freely selected, so the thickness of the door part is thin with a simple configuration. It can be made smaller and lighter.
【図1】(a)本発明の一実施例の電波シール装置の断
面図 (b)同電波シール装置の第2の導体壁面の正面図FIG. 1A is a sectional view of a radio wave sealing device according to an embodiment of the present invention. FIG. 1B is a front view of a second conductor wall surface of the radio wave sealing device.
【図2】同電波シール装置の第2の導体壁面の要部拡大
正面図FIG. 2 is an enlarged front view of a main part of a second conductor wall surface of the radio wave sealing device.
【図3】同電波シール装置の特性図FIG. 3 is a characteristic diagram of the radio wave sealing device.
【図4】(a)(c)マイクロストリップ線路技術に基
づくインピーダンス反転の特性図4A and 4C are characteristic diagrams of impedance inversion based on microstrip line technology.
【図5】本発明の他の実施例の電波シール装置の断面図FIG. 5 is a sectional view of a radio wave seal device according to another embodiment of the present invention.
【図6】一般の電子レンジの斜視図FIG. 6 is a perspective view of a general microwave oven.
【図7】(a)従来の一例の電波シール装置の断面図 (b)同電波シール装置の第2の導体壁面の正面図FIG. 7A is a cross-sectional view of an example of a conventional radio wave seal device. FIG. 7B is a front view of a second conductor wall surface of the radio wave seal device.
【図8】(a)従来の他の例の電波シール装置の断面図 (b)同電波シール装置の第2の導体壁面の正面図FIG. 8A is a cross-sectional view of another example of a conventional radio wave seal device. FIG. 8B is a front view of a second conductor wall surface of the radio wave seal device.
【符号の説明】 10 第1の導体部 11 第2の導体部 13 第1の導体壁面 14 溝底面 15 第2の導体壁面 16 チョーク部(溝) 17 導体片板 18 導体片板[Description of Signs] 10 First conductor portion 11 Second conductor portion 13 First conductor wall surface 14 Groove bottom surface 15 Second conductor wall surface 16 Choke (groove) 17 Conductor plate 18 Conductor plate
───────────────────────────────────────────────────── フロントページの続き (58)調査した分野(Int.Cl.6,DB名) H05B 6/76 F24C 7/02 501 ──────────────────────────────────────────────────続 き Continued on the front page (58) Field surveyed (Int.Cl. 6 , DB name) H05B 6/76 F24C 7/02 501
Claims (1)
波が内部に供給される加熱室本体に設けた第1の導体部
と、前記加熱室本体の前記開口部を開閉自在に覆うドア
に設けた第2の導体部とを対向させ、前記第1の導体部
または第2の導体部のどちらか一方に少なくとも一つの
溝を設け、前記溝を形成する第1の導体壁面および溝底
面は連続的な導電性部材からなり、前記溝を形成する第
2の導体壁面は開放端から切り込み部を設けて溝の長手
方向に一定ピッチの導体片板が複数個並ぶ構成とし、か
つ前記各導体片板はそれぞれ前記溝底面と電気的に接触
して前記第1の導体壁面との間にマイクロストリップ線
路を構成し、前記導体片板は2種類以上の異なった形状
のものを順次配列する構成とした電波シール装置。1. A first conductor provided in a heating chamber main body having an opening through which an object to be heated is taken in and out, to which radio waves are supplied, and the opening of the heating chamber main body is openably and closably covered. A second conductor portion provided in the door is opposed to the first conductor portion, and at least one groove is provided in one of the first conductor portion and the second conductor portion; a first conductor wall surface and the groove forming the groove; The bottom surface is made of a continuous conductive member, the second conductor wall surface forming the groove is provided with a cutout from an open end, and a plurality of conductor pieces having a constant pitch are arranged in the longitudinal direction of the groove, and Each of the conductor strips is in electrical contact with the bottom of the groove to form a microstrip line between the conductor strip and the first conductor wall, and the conductor strips are sequentially arranged in two or more different shapes. A radio wave seal device with a configuration.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP28265391A JP2949965B2 (en) | 1991-10-29 | 1991-10-29 | Radio wave sealing device |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP28265391A JP2949965B2 (en) | 1991-10-29 | 1991-10-29 | Radio wave sealing device |
Publications (2)
Publication Number | Publication Date |
---|---|
JPH05121166A JPH05121166A (en) | 1993-05-18 |
JP2949965B2 true JP2949965B2 (en) | 1999-09-20 |
Family
ID=17655316
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP28265391A Expired - Fee Related JP2949965B2 (en) | 1991-10-29 | 1991-10-29 | Radio wave sealing device |
Country Status (1)
Country | Link |
---|---|
JP (1) | JP2949965B2 (en) |
Families Citing this family (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
WO2011021368A1 (en) * | 2009-08-20 | 2011-02-24 | パナソニック株式会社 | Electromagnetic wave heating device |
-
1991
- 1991-10-29 JP JP28265391A patent/JP2949965B2/en not_active Expired - Fee Related
Also Published As
Publication number | Publication date |
---|---|
JPH05121166A (en) | 1993-05-18 |
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LAPS | Cancellation because of no payment of annual fees |