JPS62119836A - Magnetron - Google Patents
MagnetronInfo
- Publication number
- JPS62119836A JPS62119836A JP26041985A JP26041985A JPS62119836A JP S62119836 A JPS62119836 A JP S62119836A JP 26041985 A JP26041985 A JP 26041985A JP 26041985 A JP26041985 A JP 26041985A JP S62119836 A JPS62119836 A JP S62119836A
- Authority
- JP
- Japan
- Prior art keywords
- antenna conductor
- needless
- radiation
- dielectric resonator
- output antenna
- 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.)
- Pending
Links
Landscapes
- Microwave Tubes (AREA)
Abstract
Description
【発明の詳細な説明】
け)腫東上の利用分野
本発明はマグネトロンに関し、特にその不要輻射抑制技
術に向《すられてiる。DETAILED DESCRIPTION OF THE INVENTION Field of Application The present invention relates to magnetrons, and is particularly directed to techniques for suppressing unnecessary radiation thereof.
(ロ)従来の技術
一般にマグネトロンから発撮されるマイクロ波には,基
本波の他に第2)第3高一波等多くの高i1IrIIL
が含まれて8リ,それらほ不要輻射となる。(b) Conventional technology In general, microwaves emitted from a magnetron include many high-level i1IrIIL waves such as second, third, and first waves in addition to the fundamental wave.
8 ri are included, and those are unnecessary radiation.
最近では,特に第5高稠波に相当する不要輻射が。Recently, unnecessary radiation corresponding to the fifth harmonic wave has become particularly prevalent.
SL4F)47191星放送の12GH2帯と瓜なるの
で問題視されている。SL4F) It is viewed as a problem because it is similar to the 12GH2 band of 47191 Star Broadcasting.
従来,マグネトロンにお(する不要4射抑別技術として
、例えば特公昭57ー6781号公報に見られる如く,
出刃アンテナ導体にチョークキャビティを設Cj“るこ
とが提案されているが,正確な寸法のチョークキャビテ
ィを作ることが4しく,従って不要輻射のS度良い抑制
の友めにに未だ改善の余地がある。Conventionally, as an unnecessary four-shot suppression technology for magnetrons, for example, as seen in Japanese Patent Publication No. 57-6781,
It has been proposed to provide a choke cavity in the antenna conductor, but it is difficult to create a choke cavity with accurate dimensions, so there is still room for improvement in achieving good suppression of unwanted radiation. be.
(ハ)発明が解決しようとする問題点
本発明は、より簡単な構造で,確度の良い不要輻射抑制
効果の得られる技術上提供するものである。(c) Problems to be Solved by the Invention The present invention provides a technology that allows a more accurate unnecessary radiation suppression effect to be obtained with a simpler structure.
(ニ)問題点を解決する友めの手段
本発明のマグネトロンは、気密空間を延在する出力アン
テナ導体と、上記気′!!!全問内に配された不要輻射
抑制体とを補え、上記不要輻射抑制体に、上記出力アン
テナ導体に装着され之誘電体共振器と該共振器の、上記
出力アンテナ導体の延在方間に平行な表面を榎う金属壁
とからなることt峙偵とする。(d) Companion means for solving the problems The magnetron of the present invention includes an output antenna conductor extending in an airtight space, and the above-mentioned airtight space. ! ! Supplement the unnecessary radiation suppressor arranged in all questions, and add a dielectric resonator attached to the output antenna conductor to the unnecessary radiation suppressor and the direction in which the output antenna conductor of the resonator extends. It consists of a metal wall with parallel surfaces.
不発rye VCX−て、上記不要輻射抑制体は、上記
出刃アンテナ導体全量軸的に包囲して上記気密空間を形
成する封止金属体と上記出刃アンテナ導体とがd成する
同軸構造部に設Cすられるのが好−fしいO
更に本発明に3いて、上記誘電体共振器はアルミナで形
成されるのが好ましい。Unexploded rye VCX-, the unnecessary radiation suppressor is installed in a coaxial structure formed by the Deba antenna conductor and a sealing metal body that axially surrounds the entire Deba antenna conductor to form the airtight space. Furthermore, in the third aspect of the present invention, the dielectric resonator is preferably formed of alumina.
(ホ)作 用
本発明によれば、誘電体共振器とその表面tcIkり金
JIA壁との組合わせにより、顕著な帯域反射机尿が現
われ、従って誘電体共振器の共振寸法を適宜設定するこ
とにより、特定の不要輻射波がアンテナから外部へ放射
されるの′t−効果的に抑制し得る。(E) Function According to the present invention, a remarkable band-reflection effect appears due to the combination of the dielectric resonator and its surface tcIk alloy JIA wall, and therefore the resonance dimensions of the dielectric resonator are set appropriately. As a result, it is possible to effectively suppress specific unnecessary radiation waves from being radiated to the outside from the antenna.
(へ)夷 厖 力 第1図に本発明実施例のマグネトロン上*す。(to) Yi power FIG. 1 shows a magnetron according to an embodiment of the present invention.
(IJは陽極円筒体、(2)は該円筒体の中心軸に設置
されに陰極体、 (3)(3J・・・に陽極円筒不(1
)の内面に固層され、陰極体(2)の囲りに放射状に配
列されea数の陽極ベイン、(4)に陽極筒体(1)+
Z)一方の開放ジーに固着されたポールピースである。(IJ is an anode cylindrical body, (2) is a cathode body installed on the central axis of the cylinder, (3) (3J... is an anode cylindrical body (1
) are solidly layered on the inner surface of the cathode body (2), and are arranged radially around the cathode body (2), with the number of ea anode vanes;
Z) It is a pole piece fixed to one open gee.
(5バ6)及び(7)は。(5 bar 6) and (7).
夫々ポールピース(4)上に順次積み上げ固着された封
止金属体、絶縁円筒、第1金属帽子で、これらに陽極円
筒体iII内にのみ連通する気密空間(8)を形成する
。(9)は陽極ベイン(3)に一端が固定され、気密空
間(8)内vf−延在し7を後、他端が41金属帽子(
7)に固着支持された出力アンテナ導f+、QGに第1
金属帽子(7)に被冠され次第2金属帽子である。尚、
以上の構成自体に周知である。The sealing metal body, the insulating cylinder, and the first metal cap, which are stacked and fixed in sequence on the pole piece (4), respectively, form an airtight space (8) that communicates only with the inside of the anode cylinder iII. (9) is fixed at one end to the anode vane (3), extends VF- inside the airtight space (8) after 7, and has the other end fixed to the metal cap (41).
7), the output antenna conductor f+ is fixedly supported on the QG, and the first
Once it is put on the metal cap (7), it becomes a second metal cap. still,
The above configuration itself is well known.
仕りは1本発明実施例の特徴として存在する不要輻射抑
制体で、それに、気密空間(8)内に位置する。The end is an unnecessary radiation suppressor that exists as a feature of the embodiment of the present invention, and is located in an airtight space (8).
不要輻射抑制体συを詳細に示す第2図1cおいて。In FIG. 2c, the unnecessary radiation suppressor συ is shown in detail.
ttaは上記出力アンテナ導体+9)ic (111通
され次セラミックスかうなる円柱状誘電体共振器、(1
3に、その挿通方向に平行な表面を榎う金属壁である。tta is the above output antenna conductor +9)ic (111 passed through the cylindrical dielectric resonator made of ceramics, (1
3 is a metal wall whose surface is parallel to the insertion direction.
尚導体(9)に対する共蛋幸じの固定法は圧入又は鑞材
による〇
誘1!不共振器u4に、特定の不要輻射波に共振する寸
法を町しており、斯る共振器α4と金属壁0四とは、出
力アンテナ導体(9)t−伝播するマイクロ波のうち、
上配脣足の不要輻射波に対し、顕著な反射現象′(i−
%几うす。The best way to fix the conductor (9) is by press-fitting or soldering. The non-resonator u4 has a dimension that resonates with a specific unnecessary radiation wave, and the resonator α4 and the metal wall 04 are connected to the output antenna conductor (9) t-of the microwaves propagating.
A remarkable reflection phenomenon'(i-
% thin.
この反射現象につき説明するに、不要輻射抑制体(11
は、出刃アンテナ導体(9)と、この導体上聞軸的に包
囲する封止金属体(5)とが作る同軸伝播路構造品VC
位置することとなり、これと等価な実験構造として、第
6図A、B、Cに示す如く3種類の同軸伝播路が準備さ
れた。各伝播路において、(9a)は中心!犀、(!l
)にこの中心導体と同軸的に設けられた円筒状外部導体
、(12a)は中心導体(9a)に挿通され次回柱状の
m電体共振器、(13a)rl、共振器(12al)、
そノ伸通方向に平行な表面にメタライズ被着された金属
壁である。各伝播路の相違に、因より明らかな如く、外
部導体(5a)の内径’t D i 1m11L不共T
kx器(12&)の外径2diとすると、第3図Aの場
合、dl<L)t、第6図Bの場合、dz=Dz。To explain this reflection phenomenon, the unnecessary radiation suppressor (11
is a coaxial propagation path structure product VC made by a Deba antenna conductor (9) and a sealing metal body (5) that axially surrounds this conductor.
Three types of coaxial propagation paths were prepared as equivalent experimental structures as shown in FIG. 6A, B, and C. In each propagation path, (9a) is the center! Rhinoceros, (!l
) is a cylindrical external conductor provided coaxially with this central conductor, (12a) is inserted into the central conductor (9a) and is a columnar m electric resonator, (13a) rl, resonator (12al),
It is a metal wall whose surface parallel to its extension direction is metallized. Due to the difference in each propagation path, as is clear from the cause, the inner diameter of the outer conductor (5a) 'tD i 1m11L
If the outer diameter of the kx device (12&) is 2di, then in the case of Fig. 3A, dl<L)t, and in the case of Fig. 6B, dz=Dz.
第3図Cの場合、dl(D3でかつ金属壁(16a)が
存在する点にある。In the case of FIG. 3C, the point is dl (D3) and the metal wall (16a) is present.
今%D1=、Dz−Da=17sw、dt=sd3−6
1とし、又Jt体共振6(125L)i第5高調rBL
(12,25GHz )共振用トシテ、共振器(121
L)t−アルミナ−セラミックス(AI!203.εr
長) t 4.1 層とし次。共振器(1211)はセ
ラミックスの成型体で形成されるから、その寸法精度。Now %D1=, Dz-Da=17sw, dt=sd3-6
1, and Jt body resonance 6 (125L) i 5th harmonic rBL
(12,25GHz) Resonator, resonator (121
L) t-alumina ceramics (AI!203.εr
long) t 4.1 layer and next. Since the resonator (1211) is formed from a ceramic mold, its dimensional accuracy is important.
即ち共振周波数、ff簾は容易に高められる。That is, the resonant frequency and ff screen can be easily increased.
M4図A、B%Cに大々第3図A%B、Cの各伝播路の
伝送特性を示しており、この図から、第3図Co伝播路
は、はソ第5高調波(12゜25GHz)に対し、顕著
な反射性を示すことが明らかである。M4 Diagrams A and B%C show the transmission characteristics of each propagation path in Figure 3 A%B and C, and from this figure, it can be seen that the Co propagation path in Figure 3 has the fifth harmonic (12 25 GHz).
さて、!@1図vcおける不要輻射抑制体αυを含む同
軸伝播路構造を第3図Cの伝播路と同一条件にした場合
のマグネ)oンt*子レンジに組み込み。Now,! When the coaxial propagation path structure including the unnecessary radiation suppressor αυ in Fig. 1 vc is set to the same conditions as the propagation path in Fig. 3 C, magnet) ont* is incorporated into the child microwave oven.
斯る電子レンジから放射される不要輻射@Cl5PR規
格に基いて測定した結果を第5図において集線にて示す
。K5図中、破線に、第1図におCする不要輻射抑1f
lJ%1MのみtS去し、その他を全て$1図の場合と
同一条件としたマグネトロンを上記と同一の電子レンジ
に組み込み、同様の側足tし次結来を示す。#I5図よ
り本実施例マグネトロンVCおける不要4射抑制効果に
明らかである。尚。The results of measurement of unnecessary radiation emitted from such a microwave oven based on the @Cl5PR standard are shown in concentrated lines in FIG. In Figure K5, the dashed line indicates unnecessary radiation suppression 1f shown in Figure 1.
A magnetron with only 1J% 1M removed and all other conditions the same as in the $1 diagram was installed in the same microwave oven as above, and the same side legs were used to show the following results. #I5 shows the effect of suppressing unnecessary four shots in the magnetron VC of this embodiment. still.
本実施例マグネトロンは、第5高vIA波より上の高久
高11&につ−てt抑制効果が現われてgす、この理由
は詳らかではないが、第4図Cの特性にg−て、第5高
調波以上の周波数領域においてもかなりの反射効果が現
われている現象と関連があると思われる。In the magnetron of this example, a t suppression effect appears for the Takaku high 11 & above the 5th high vIA wave.The reason for this is not clear, but based on the characteristics shown in Fig. 4C, the t suppression effect appears. This seems to be related to the phenomenon in which a considerable reflection effect appears even in the frequency range of the fifth harmonic or higher.
第6図は上記不要輻射抑fllJ体μυの変更例を示し
。FIG. 6 shows an example of a modification of the unnecessary radiation suppressing fllJ body μυ.
この場合、メタライズ農に代えて金属円筒からなる金I
!4壁0に誘電体共振611′4が圧入されている。In this case, gold I made of metal cylinder instead of metallization
! A dielectric resonance 611'4 is press-fitted into the fourth wall 0.
金属壁u3の両端t1図の如く共振4α4の両端より若
干はみ出しておけば共振aUa両端からの放射慣を防止
することができる。If both ends of the metal wall u3 are slightly protruded from both ends of the resonance 4α4 as shown in the figure t1, radiation from both ends of the resonance aUa can be prevented.
第7図rc、i$611!gの更に変更例を示し、この
場合、金属円筒状の金属壁tta+に共振周波数の異な
る#域体共珈器(120)(121)が圧入され、これ
により複数の高iI4波に対する抑制効果を得ている。Figure 7 rc, i$611! A further modified example of g is shown. In this case, # area body resonators (120) (121) having different resonance frequencies are press-fitted into the metal cylindrical wall tta+, thereby suppressing the plurality of high iI4 waves. It has gained.
第1図の実施例においても、異なる共振周波数を何する
個々の誘電体共mat用意し、それら各共嶽器にメタラ
イズ農かうなる金属mv付けたものを出力アンテナ導体
(9)に取着することにより複数の高周tlLVc対す
る抑制効果が得られる。In the embodiment shown in Fig. 1 as well, individual dielectric components having different resonance frequencies are prepared, and each of these dielectric components is attached with a metal MV attached to the output antenna conductor (9). As a result, the effect of suppressing a plurality of high frequency tlLVc can be obtained.
上記各実施例に′M−て、誘電体共振器の材料としては
アルミナの他にチタン酸バリウム等、他の七うミックス
も便用可能であるが、″Vグネトロンの気密空間(8)
に十分余裕をもって収め得る共振器@t%たらす材料と
してアルミナが最適である。In each of the above embodiments, as the material for the dielectric resonator, other materials such as barium titanate can be used in addition to alumina.
Alumina is the most suitable material for creating a resonator @t% that can be accommodated with sufficient margin.
上記5A−例では、不要輻射抑制体αDは封止金属ゐ
(5Jと出力アンテナ導体(9)とからてJ同軸#!a
に設へ
けられたが、気密空間(8Jのその他の饋域で出力アン
テナ導不(9)に装着されてもかなりの不要輻射抑11
Jカ来が生じる。In the example 5A above, the unnecessary radiation suppressor αD is a sealing metal (5J and output antenna conductor (9), J coaxial #!a
However, even if the output antenna is installed in an airtight space (other areas of 8J), it will still significantly suppress unnecessary radiation (9).
J-Kara occurs.
(ト」発明の効果
本発明マグネトロンによれば、誘電体共振器とその表面
t−嶺つ金属壁との組合わせにより効果的な不要輻射抑
制がなされ、しか%縛電体共去器は、各員にその寸法精
成、!Itlち共振装置が高められるので、1度の艮−
不要輻射抑制t%たらす。(G) Effects of the Invention According to the magnetron of the present invention, effective suppression of unnecessary radiation is achieved by the combination of a dielectric resonator and a metal wall with a ridge on its surface. Each member refines its dimensions, and the resonant device is enhanced, so that it can be used once.
Add unnecessary radiation suppression t%.
第1図は本発明の実施例を示す断面図、第2図は同安部
斜視図、第6図は芙験II造を示す断面図。
!4図μ向実鏡の測定結果を示す特性曲線図、第5図σ
本発明冥jll11例の特性四巌図、第6図、第7図に
夫々異なる実施例を示す要部断面−である。
(5)・・・封止金属体、(8)・・・気密空間、 (
9)−・・出力アンテナ4体、liυ・・・不要輻射抑
制体、α4・・・誘電体共振器、 tlal・・・金属
壁。
出麩三洋電機株式会社FIG. 1 is a sectional view showing an embodiment of the present invention, FIG. 2 is a perspective view of the same part, and FIG. 6 is a sectional view showing the Fuken II structure. ! Figure 4: Characteristic curve diagram showing the measurement results of μ-oriented real mirror; Figure 5: σ
FIG. 6 and FIG. 7 are cross-sectional views of main parts showing different embodiments of the present invention. (5)...Sealing metal body, (8)...Airtight space, (
9) -...4 output antennas, liυ...unwanted radiation suppressor, α4...dielectric resonator, tlal...metal wall. Defu Sanyo Electric Co., Ltd.
Claims (3)
密空間内に配された不要輻射抑制体とを備え、上記不要
輻射抑制体は、上記出力アンテナ導体に装着された誘電
体共振器と該共振器の、上記出力アンテナ導体の延在方
向に平行な表面を覆う金属壁とからなることを特徴とす
るマグネトロン。(1) An output antenna conductor extending in an airtight space and an unnecessary radiation suppressor disposed in the airtight space, the unnecessary radiation suppressor including a dielectric resonator attached to the output antenna conductor. A magnetron comprising: a metal wall covering a surface of the resonator parallel to the extending direction of the output antenna conductor.
ナ導体を同軸的に包囲して上記気密空間を形成する封止
金属体と上記出力アンテナ導体とが構成する同軸構造部
に上記不要輻射抑制体が設けられていることを特徴とす
るマグネトロン。(2) In claim 1, the unnecessary radiation is suppressed in a coaxial structure formed by the output antenna conductor and a sealing metal body that coaxially surrounds the output antenna conductor to form the airtight space. A magnetron characterized by having a body.
誘電体共振器はアルミナで形成されていることを特徴と
するマグネトロン。(3) The magnetron according to claim 1 or 2, wherein the dielectric resonator is made of alumina.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP26041985A JPS62119836A (en) | 1985-11-20 | 1985-11-20 | Magnetron |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP26041985A JPS62119836A (en) | 1985-11-20 | 1985-11-20 | Magnetron |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS62119836A true JPS62119836A (en) | 1987-06-01 |
Family
ID=17347674
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP26041985A Pending JPS62119836A (en) | 1985-11-20 | 1985-11-20 | Magnetron |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS62119836A (en) |
Cited By (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
WO2002065504A1 (en) * | 2001-02-13 | 2002-08-22 | Marconi Applied Technologies Limited | Magnetron |
WO2003079394A1 (en) * | 2002-03-16 | 2003-09-25 | E2V Technologies (Uk) Limited | Magnetron |
GB2392004A (en) * | 2002-05-13 | 2004-02-18 | New Japan Radio Co Ltd | Magnetron device |
US7199525B2 (en) | 2001-02-13 | 2007-04-03 | E2V Technologies (Uk) Limited | Strapped magnetron with a dielectric resonator for absorbing radiation |
Citations (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS5418121U (en) * | 1977-07-08 | 1979-02-06 |
-
1985
- 1985-11-20 JP JP26041985A patent/JPS62119836A/en active Pending
Patent Citations (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS5418121U (en) * | 1977-07-08 | 1979-02-06 |
Cited By (5)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
WO2002065504A1 (en) * | 2001-02-13 | 2002-08-22 | Marconi Applied Technologies Limited | Magnetron |
US7199525B2 (en) | 2001-02-13 | 2007-04-03 | E2V Technologies (Uk) Limited | Strapped magnetron with a dielectric resonator for absorbing radiation |
WO2003079394A1 (en) * | 2002-03-16 | 2003-09-25 | E2V Technologies (Uk) Limited | Magnetron |
GB2392004A (en) * | 2002-05-13 | 2004-02-18 | New Japan Radio Co Ltd | Magnetron device |
GB2392004B (en) * | 2002-05-13 | 2006-01-18 | New Japan Radio Co Ltd | Magnetron device |
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