JPS59941B2 - magnetron device - Google Patents
magnetron deviceInfo
- Publication number
- JPS59941B2 JPS59941B2 JP52046283A JP4628377A JPS59941B2 JP S59941 B2 JPS59941 B2 JP S59941B2 JP 52046283 A JP52046283 A JP 52046283A JP 4628377 A JP4628377 A JP 4628377A JP S59941 B2 JPS59941 B2 JP S59941B2
- Authority
- JP
- Japan
- Prior art keywords
- anode cylinder
- output antenna
- magnetron
- center
- waveguide
- 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
Links
Landscapes
- Microwave Tubes (AREA)
Description
【発明の詳細な説明】
本発明は主として電子レンジ用に使用されるマグネトロ
ンの改良に関するものである。DETAILED DESCRIPTION OF THE INVENTION The present invention relates primarily to improvements in magnetrons used in microwave ovens.
従来電子レンジ用マグネトロンは電子放射をする陰極と
、その周囲に位置して空胴を形成する陽極円筒と、この
陽極円筒の内壁に固定された複数個のベインと、陽極円
筒両端部に配置された磁極とから構成されており、陽極
円筒外部に配置した永久磁石により前記磁極を通して前
記ベインによって周まれでなる作用空間に磁界が供給さ
れている。Conventional microwave oven magnetrons consist of a cathode that emits electrons, an anode cylinder located around the cathode to form a cavity, multiple vanes fixed to the inner wall of the anode cylinder, and placed at both ends of the anode cylinder. A permanent magnet placed outside the anode cylinder supplies a magnetic field through the magnetic poles to the working space surrounded by the vanes.
このような従来のマグネトロンに対し、第1図に示すよ
うに永久磁石1a、1bを陽極円筒5の内側に配置し、
磁気利用効率を上げることにより小型で安価なマグネト
ロンが実用化されつつある。In contrast to such a conventional magnetron, permanent magnets 1a and 1b are arranged inside an anode cylinder 5 as shown in FIG.
Small and inexpensive magnetrons are being put into practical use by increasing the efficiency of magnetic utilization.
永久磁石1a、Ibを陽極円筒5の内側に配置したこの
種のマグネトロンは陽極円筒5の中心軸に近接して永久
磁石1bを配置しているため、従来のように陽極円筒5
の中心軸上に出力アンテナ4を設けることができない。In this type of magnetron in which the permanent magnets 1a and Ib are arranged inside the anode cylinder 5, the permanent magnet 1b is arranged close to the central axis of the anode cylinder 5.
It is not possible to provide the output antenna 4 on the central axis of the antenna.
従って従来この種のマグネトロンは、陽極円筒5を放熱
板9の中心に従って放熱板9を取り囲んでなる継鉄8の
出力アンテナ側の中心に、そして出力アンテナ4を陽極
円筒の中心軸を通り通風軸a−a’に垂直な線上に配し
た第2図のような構造が取られている。Therefore, in the conventional magnetron of this kind, the anode cylinder 5 is placed at the center of the output antenna side of the yoke 8 which surrounds the heat sink 9 along the center of the heat sink 9, and the output antenna 4 is placed along the ventilation axis passing through the central axis of the anode cylinder. A structure as shown in FIG. 2, which is arranged on a line perpendicular to a-a', is adopted.
しかし、このような構造のマグネトロンはアンテナ4と
継鉄8との関係が非対称なために、マグネトロンを導波
管あるいはオープンに継鉄8上の4ケ所にもうけられた
ビス穴12を通じて装着した場合、出力アンテナ4と同
心円上に設けられているガスケット部10と導波管ある
いはオープンとの締めつけが不均衡になり、部分的な接
触不良が発生して放電、電波もれ、さらには不要輻射の
漏洩が生ずるという問題があった。However, in a magnetron with such a structure, the relationship between the antenna 4 and the yoke 8 is asymmetrical, so when the magnetron is mounted through a waveguide or through the open screw holes 12 made at four locations on the yoke 8, , the tightening of the gasket part 10, which is provided concentrically with the output antenna 4, and the waveguide or open circuit becomes unbalanced, resulting in a partial contact failure, resulting in discharge, radio wave leakage, and even unnecessary radiation. There was a problem that leakage occurred.
又、導波管に装着する場合に限ってみれば、締め付は位
置の関係から第3図に示すように通風軸に対して左右対
称にして導波管13の両側で締め付けるのがもつとも容
易で確実な方法である。Also, when mounting it on a waveguide, it is easier to tighten it on both sides of the waveguide 13 by making it symmetrical with respect to the ventilation axis, as shown in Fig. 3, due to the positional relationship. This is a reliable method.
しかるにこの場合、マグネトロンの出力アンテナ4が導
波管13の中心軸から大巾に離れた位置にくるため、出
力アンテナ4により導波管13内に反射無く電波を励起
することが困難となる。However, in this case, since the output antenna 4 of the magnetron is located at a position far away from the central axis of the waveguide 13, it becomes difficult for the output antenna 4 to excite radio waves into the waveguide 13 without reflection.
なぜなら電磁気宇の教えるところによると導波管内に最
も有効に電波を励起しようとする場合、導波管内に伝播
する電波の電界分布すの最大点、すなわち導波管13の
中心線上に出力アンテナ4を位置させなければならない
からである。This is because electromagnetism teaches that in order to most effectively excite radio waves within a waveguide, the output antenna 4 should be located at the maximum point of the electric field distribution of the radio waves propagating within the waveguide, that is, on the center line of the waveguide 13. This is because it must be located.
そこで本発明は簡単な構成により上記従来の欠点を解消
するものである。Therefore, the present invention solves the above-mentioned conventional drawbacks with a simple configuration.
なお第1図〜第4図において共通部分は同一符号で説明
する。Note that common parts in FIGS. 1 to 4 are designated by the same reference numerals.
すなわち、la、1bは永久磁石、2はベイン、3はベ
イン2と出力アンテナを結ぶ導電体、4は出力アンテナ
、5は陽極円筒、6は陰極7を支え電圧を供給する陰極
リード、Iは電子を放射する陰極、8は放熱板9を囲ん
で通風路と永久磁石の帰還磁路を形成すると共にマグネ
トロンをオープン等に取り付けるための支持外体の役割
をする継鉄、9は放熱板、10はマグネトロンの陽極と
マグネトロンを装着する導波管等との電気的接触をはか
るガスケット、11は陶板側からの電波漏洩を防止する
シールドケース、12は取り付は用のビス穴、13は導
波管 a/は通風軸、bは導波管内の電界分布である
。That is, la and 1b are permanent magnets, 2 is a vane, 3 is a conductor connecting the vane 2 and the output antenna, 4 is the output antenna, 5 is an anode cylinder, 6 is a cathode lead that supports the cathode 7 and supplies voltage, and I is a cathode lead. A cathode that emits electrons, 8 a yoke that surrounds the heat sink 9 to form a ventilation path and a return magnetic path for the permanent magnet, and also serves as a supporting body for mounting the magnetron in an open manner; 9 a heat sink; 10 is a gasket that makes electrical contact between the magnetron anode and the waveguide etc. on which the magnetron is attached, 11 is a shield case that prevents radio wave leakage from the ceramic plate side, 12 is a screw hole for mounting, and 13 is a guide. Waveguide a/ is the ventilation axis and b is the electric field distribution within the waveguide.
第4図において、マグネトロンは出力アンテナ4と陽極
円筒5の中心軸が通風軸a−a’上にあり、さらに出力
アンテナ4が冷却板9の略中央、従って継鉄8の略中央
に位置し、陽極円筒5を中央からはずれた位置にくる構
造になっている。In FIG. 4, in the magnetron, the central axes of the output antenna 4 and the anode cylinder 5 are located on the ventilation axis a-a', and the output antenna 4 is located approximately at the center of the cooling plate 9, and therefore approximately at the center of the yoke 8. , the anode cylinder 5 is located at a position offset from the center.
以上のような構造を採用することにより、出力アンテナ
4及びガスケット部10がマグネトロンの略中央の位置
にくるため、導波管あるいはオープンに装着する場合の
ガスケット部10の締め付けが均一になり、接触不良に
よる放電、電波漏れ不要輻射の漏洩等の発生を大巾に低
減することができる。By adopting the above structure, the output antenna 4 and the gasket part 10 are located approximately at the center of the magnetron, so the tightening of the gasket part 10 is uniform when the magnetron is installed in a waveguide or in the open. The occurrence of electrical discharges due to defects, radio wave leakage, unnecessary radiation leakage, etc. can be greatly reduced.
又導波管13に装着する場合においても、マグネトロン
をそのまま左右対称に取り付ければ導波管13の中心線
上に出力アンテナ4が来るため、容易にいわゆるインピ
ーダンス整合が取れ、マグネトロンから出た電波を10
0%近く導波管13内へ導くことができるものである。Also, when installing the magnetron in the waveguide 13, if the magnetron is installed symmetrically, the output antenna 4 will be on the center line of the waveguide 13, so impedance matching will be easily achieved, and the radio waves emitted from the magnetron will be
It is possible to guide nearly 0% into the waveguide 13.
一方、陽極円筒5が冷却板9に対して通風軸a−a’上
を片方に偏った位置にあるので、通風路の2つの開口部
のうち陽極円筒5が近い側(a側)から空冷ファンによ
り冷却風を通風路に送り込むと、陽極円筒5が冷却板9
の中央にある場合よりも陽極円筒5の周囲の空気を強制
的に除去する効果が犬になる。On the other hand, since the anode cylinder 5 is located at a position biased to one side on the ventilation axis a-a' with respect to the cooling plate 9, the air is cooled from the side (a side) nearer to the anode cylinder 5 of the two openings of the ventilation passage. When cooling air is sent into the ventilation passage by a fan, the anode cylinder 5 is moved to the cooling plate 9.
The effect of forcibly removing the air around the anode cylinder 5 is greater than when it is in the center of the anode cylinder.
従ってマグネトロンの陽極円筒5の冷却が増進すること
が実験的にも認められる。Therefore, it has been experimentally confirmed that the cooling of the anode cylinder 5 of the magnetron is enhanced.
以上のように本発明によれば通風軸の一直線上に陽極円
筒と出力アンテナの中心軸を設けるとともに、アンテナ
を冷却板の中心に設け、陽極円筒を通風路の入口側に設
けたので、マグネトロンの取付状態においてアンテナ周
辺のガスケット部の締めつけが安定し放電、電波もれ、
不要輻射の漏洩が少ない。As described above, according to the present invention, the central axes of the anode cylinder and the output antenna are provided on a straight line with the ventilation axis, the antenna is provided in the center of the cooling plate, and the anode cylinder is provided on the entrance side of the ventilation path, so that the magnetron When installed, the tightening of the gasket around the antenna is stable, preventing electrical discharge, radio wave leakage,
Less leakage of unnecessary radiation.
又、陽極円筒はよく冷却される効果をも備えるものであ
る。Furthermore, the anode cylinder also has the effect of being well cooled.
第1図は従来のマグネトロンの横断面図、第2図は同マ
グネトロンの下面図、第3図は同マグネトロンを導波管
に装着した状態の断面図、第4図は本発明の一実施例を
示すマグネトロン装置の下面図である。
1a、1b・・・・・・永久磁石、2・・・・・・ベイ
ン、4・・・・・・出力アンテナ、5・・・・・・陽極
円筒、6・・・・・・陰極リード、7・・・・・・陰極
、8・・・・・・継鉄、9・・・・・・放熱板。Fig. 1 is a cross-sectional view of a conventional magnetron, Fig. 2 is a bottom view of the magnetron, Fig. 3 is a sectional view of the magnetron attached to a waveguide, and Fig. 4 is an embodiment of the present invention. FIG. 2 is a bottom view of the magnetron device. 1a, 1b...Permanent magnet, 2...Vane, 4...Output antenna, 5...Anode cylinder, 6...Cathode lead , 7... cathode, 8... yoke, 9... heat sink.
Claims (1)
体で接続されかつ前記陽極円筒と同心軸上にない出力ア
ンテナと、前記陽極円筒の中心軸に対して垂直平面上に
設けられかつ外周が略長方形をなした複数の冷却板と、
前記冷却板の相対する二つの長辺側を通風路の出入口と
なるように開口した空気ガイド構成としてなる冷却器と
を備え、前記陽極円筒と前記出力アンテナの中心軸を前
記冷却器の通風軸の一直線上に配置するとともに、前記
陽極円筒の中心軸を前記冷却板の中央からずらせること
により、前記出力アンテナを前記冷却板の略中央に配置
したマグネトロン装置。1. A plurality of vanes, an anode cylinder, an output antenna connected to the vane by a conductor and not on a concentric axis with the anode cylinder, and an output antenna that is provided on a plane perpendicular to the central axis of the anode cylinder and has an outer periphery. a plurality of cooling plates each having a substantially rectangular shape;
a cooler having an air guide configuration with openings on two opposing long sides of the cooling plate to serve as entrances and exits of ventilation passages, the center axis of the anode cylinder and the output antenna being aligned with the ventilation axis of the cooler. The output antenna is arranged on a straight line, and the central axis of the anode cylinder is shifted from the center of the cooling plate, so that the output antenna is arranged approximately at the center of the cooling plate.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP52046283A JPS59941B2 (en) | 1977-04-20 | 1977-04-20 | magnetron device |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP52046283A JPS59941B2 (en) | 1977-04-20 | 1977-04-20 | magnetron device |
Publications (2)
Publication Number | Publication Date |
---|---|
JPS53130964A JPS53130964A (en) | 1978-11-15 |
JPS59941B2 true JPS59941B2 (en) | 1984-01-09 |
Family
ID=12742887
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP52046283A Expired JPS59941B2 (en) | 1977-04-20 | 1977-04-20 | magnetron device |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS59941B2 (en) |
Citations (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS4979163A (en) * | 1972-12-04 | 1974-07-31 | ||
JPS49118360A (en) * | 1973-03-14 | 1974-11-12 |
-
1977
- 1977-04-20 JP JP52046283A patent/JPS59941B2/en not_active Expired
Patent Citations (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS4979163A (en) * | 1972-12-04 | 1974-07-31 | ||
JPS49118360A (en) * | 1973-03-14 | 1974-11-12 |
Also Published As
Publication number | Publication date |
---|---|
JPS53130964A (en) | 1978-11-15 |
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