JPS58100333A - Magnetron - Google Patents
MagnetronInfo
- Publication number
- JPS58100333A JPS58100333A JP19681581A JP19681581A JPS58100333A JP S58100333 A JPS58100333 A JP S58100333A JP 19681581 A JP19681581 A JP 19681581A JP 19681581 A JP19681581 A JP 19681581A JP S58100333 A JPS58100333 A JP S58100333A
- Authority
- JP
- Japan
- Prior art keywords
- gasket
- cylinder
- metal
- magnetron
- output terminal
- 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.)
- Granted
Links
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
- H01J23/00—Details of transit-time tubes of the types covered by group H01J25/00
Landscapes
- Microwave Tubes (AREA)
Abstract
Description
【発明の詳細な説明】
本斃明は、マグネトロンの導波管への取付は個所に用い
る電波漏洩防止用ガスケットの作用が確実に行なわれ、
かつガスケットのマグネトロンへの取付は作業も容易な
マグネトロンに関する。[Detailed Description of the Invention] The present invention is designed to ensure that the gaskets used to prevent radio wave leakage work properly when attaching the magnetron to the waveguide.
Furthermore, the present invention relates to a magnetron in which the gasket can be easily attached to the magnetron.
第1図は従来のマグネトロンの一例を示し、lはマグネ
トロン本体、1aは内側に複数の共振空胴な有する陽極
円筒、1bは陰極側金属封止部材。FIG. 1 shows an example of a conventional magnetron, where l is the magnetron main body, 1a is an anode cylinder having a plurality of resonant cavities inside, and 1b is a metal sealing member on the cathode side.
lcは陰極側絶縁物、ldは陰極フイラメン) 9−ド
、1eは出力側金属対止部材、1fは出力側絶縁物、1
gは出力端子、2m 、2bは永久磁石、3 a *
3 bは管外磁路をなすl−夕、4は真導電性かつ高弾
性の材料よりなるガスケット、7は円筒状金属部材、8
は孔あき金属円板である。第2図は第1図に示した従来
のマグネ)aンのガスケット近傍拡大図で、9は銀ろう
、その他の符号は第1IIの場合と同じである。第3図
は円筒状金属部材7の断面がL字状をなし、ガスケット
4を保持するよ5に1.た従来例を示す図である。lc is a cathode side insulator, ld is a cathode filament) 9-do, 1e is an output side metal stopper member, 1f is an output side insulator, 1
g is the output terminal, 2m, 2b is the permanent magnet, 3a*
3 b is an extra-tube magnetic path, 4 is a gasket made of a truly conductive and highly elastic material, 7 is a cylindrical metal member, and 8
is a perforated metal disk. FIG. 2 is an enlarged view of the vicinity of the gasket of the conventional magnet (a) shown in FIG. In FIG. 3, the cross section of the cylindrical metal member 7 is L-shaped and holds the gasket 4. FIG. 2 is a diagram showing a conventional example.
マグネトロンは通常出力端子igを下または横にし″C
@包輸送されるが、徊包時、輸送荷役時の振動、衝撃に
より、第2.3図に示した様な構造のマグネトロンでは
、ガスケット島蕎事故が生じ易い。The magnetron usually has the output terminal ig down or sideways.
When a package is transported, a magnetron with a structure like the one shown in Figure 2.3 is prone to gasket failure accidents due to vibrations and shocks during transport and cargo handling.
また!グネ)Elンは、第411に示す様な状態で導波
管20に接続され、導波管に6設され麩導波管受は部2
01がガスケツ)4K(いとみ嵐く接触して1イクロ波
の漏洩放射が生じないよ5KL。Also! The waveguide receiver is connected to the waveguide 20 in the state shown in No. 411, and six waveguide receivers are installed in the waveguide.
01 is the gasket) 4K (5KL) 4K (Itomi Arashi contacts tightly and leakage radiation of 1 microwave does not occur) 5KL.
である。しかし実際には、導波管受は部20mがガスケ
ツ)4#IC(いこんだ時の状態は、第5図に示すよ5
に、ガスケット4の上面が、このくいこみ現象により引
張られて浮上り、円筒状金属部材7とガスケット4の内
径側4mとの接触が悪化してしまうことが多い。この様
になると出力側金属封止部材1@1円筒状金属部材7.
ガスケット4゜導波管受け@Boaを流れるマイクロ波
電流によって、接触の悪化した部分が加熱され焼ける。It is. However, in reality, the waveguide receiver has a gasket on the part 20m of the 4#IC (the state when it is inserted is 5 as shown in Figure 5).
In addition, the upper surface of the gasket 4 is often pulled and floated due to this wedge-in phenomenon, resulting in poor contact between the cylindrical metal member 7 and the inner diameter side 4m of the gasket 4. In this case, the output side metal sealing member 1@1 cylindrical metal member 7.
The microwave current flowing through the gasket 4° waveguide support @Boa heats and burns the area where the contact has deteriorated.
第5図に示し例の場合は、ガスケット4と金属円板8の
外径部近くとが導波管受は部20alc押されて密着し
ているため、ガスケットが浮上ってガスケットの内径側
4畠近くの接触が悪くなっても、焼けて変色するel&
ですむ。しかし菖3#A&C示した構造の場合には、ガ
スケット4の内径側が浮上がると、マイクロ波エネルギ
ーが永久磁石2mの方にも伝搬するため、磁石2鳳が加
熱され磁束が減りたり極端な場合には割れたりする。な
お従来は、出力側金属封止部材1・に円筒状金属部材7
を、縞2図に示すよ5に、銀ろ59で固着する高価な構
造になっていた。In the case of the example shown in FIG. 5, since the gasket 4 and the part near the outer diameter of the metal disk 8 are pressed against the waveguide receiver 20alc and are in close contact with each other, the gasket floats up and Even if the contact near the field gets bad, the el& will burn and discolor.
That's fine. However, in the case of the structure shown in Iris 3#A&C, when the inner diameter side of the gasket 4 floats, the microwave energy also propagates toward the permanent magnet 2m, which heats the magnet 2 and reduces the magnetic flux, or in extreme cases. It may crack. Note that conventionally, a cylindrical metal member 7 is attached to the output side metal sealing member 1.
It had an expensive structure in which it was fixed to the stripe 5 with a silver foil 59 as shown in Figure 2.
上記の如き問題をさけるため、従来、ガスケット4の内
径を円筒状金属部材7の外径よりも小さくシ、かつガス
ケット4の外径な璽−り3mの穴の径よりも大きく設定
して、ガスケット脱落やガスケット焼けの対策をしてい
た。しかしこの場合は、ガスケットにカが加わり弾力性
が落ちて固くなるため、導波管受は部20mの平坦度が
悪いときには、くいこみの少ない部分で、マイクロ波エ
ネルギーが漏洩したり、!I触が悪くてその部分のガス
ケットが焼けるなどの不具合が生じた。またガスケット
をそれより狭い場所に押入れなければならないため工数
が増大してしまう0%にマグネトロン本体lとヨーク3
aの穴とが偏心している場合はガスケット4の挿入に工
数がかかり、また導波管受けm20mとガスケット4と
の接触が金屑にわたらないという不具合が発生する。In order to avoid the above-mentioned problems, conventionally, the inner diameter of the gasket 4 is set smaller than the outer diameter of the cylindrical metal member 7, and larger than the diameter of the 3 m-sized hole in the outer diameter of the gasket 4. Measures were taken to prevent gaskets from falling off and burning. However, in this case, force is added to the gasket, which reduces its elasticity and makes it hard, so if the flatness of the 20m part of the waveguide receiver is poor, microwave energy may leak in the part where there is little bite. I had problems such as the gasket in that area burning due to poor contact. Also, since the gasket has to be pushed into a narrower space, the number of man-hours increases.
If the hole a is eccentric, it will take a lot of man-hours to insert the gasket 4, and there will be a problem that the waveguide support m20m and the gasket 4 will not come into contact with the metal chips.
本発明の目的は、マグネトロンを導波管に接続するIn
c、上述した様な種々の不具合が生じないようKしたマ
グネトロンを提供することにある。The object of the present invention is to connect a magnetron to a waveguide.
c. To provide a magnetron that does not cause the various problems described above.
上記目的を達成するために本発@においては、出力側金
属封止部材の円筒状部k、つば付き金属円筒のつばのな
い端部を強制嵌合して固着させ、この円筒の他端すなわ
ち軸方陶出力端子寄り端部のつばと外**他部分の導電
部材とでガスケットの内径側を挾持させ、ガスケットの
脱落、浮上がりを防止するよう和した。In order to achieve the above object, in this invention, the cylindrical part k of the output side metal sealing member and the end part without a flange of the metal cylinder with a flange are forcibly fitted and fixed, and the other end of the cylinder, i.e. The inner diameter side of the gasket was sandwiched between the brim at the end near the axial ceramic output terminal and the conductive member on the outside** to prevent the gasket from falling off or rising.
第6〜9図は、本発明のそれぞれ異なる4実施例の要部
拡大図で、いずれの例でも、つば付き金属円筒6は、つ
ばのない端部5bを出力側金属封止部材1・の円筒状部
に強制嵌合により固着され、他端ではっば51がガスケ
ット4の内径側を上面(出力端子側)から押さえ、磁石
2畠またはN −り3暑の上面とでガスケット4を圧縮
挾持している。したがってガスケット4は輸送中などに
も確11!に保持され脱落事故は生じない。金属円筒5
は端部5bで出力側金属封止部材1eと強制嵌合され、
マイクロ波的にも安定した接続が得られており、しかも
この接続部には従来の如く高価な銀ろうを使用せず、工
数もわずかですむ。ガスケット4の外径は、目−り3m
の穴径と同じか、やや小さくしてもよく、またガスケッ
ト4の内径は、つば付き金属円筒5の5C部(第6゜7
図)の外径と同じか、大きく、ただしっぽ5mの外径よ
り小さければよいので、ガスケットの挿入は非常に容易
になり、工数が短縮され、しかもガプケット自体の重量
も減らすことができる。さらに、−vグネトロン本体1
とヨーク3mの穴とが偏心していても、金属円筒6の5
C部の外径よりガスケット4の内径を大きく設定するこ
とにより、ガスケット4はどの部分でも弾力性均一であ
り、また、導波管受は部20暑は冒−り3畠の穴と同心
なので、理想的な接続が可能となる。更に金属円筒5の
端部5bにマイクμ波接続を害さないStに短いスリッ
トを設けると嵌合が容易になる。金属円筒5を磁性材た
とえば亜鉛引き鉄板で作れば、11に永久磁石2aK吸
引されるので、端部5bの強制嵌合部は、マイクル技的
に*好な接触が得られる程度の嵌合度であれば、金属円
筒5がぬけ出す恐れは少ない。6 to 9 are enlarged views of main parts of four different embodiments of the present invention, and in each example, the flange metal cylinder 6 connects the non-flange end 5b to the output side metal sealing member 1. It is fixed to the cylindrical part by forced fitting, and at the other end, a flap 51 presses the inner diameter side of the gasket 4 from the upper surface (output terminal side), and compresses the gasket 4 with the upper surface of the magnet 2 or N-3. It's being held in place. Therefore, gasket 4 is reliable even during transportation! It is held securely and no accidents occur. metal cylinder 5
is forcibly fitted with the output side metal sealing member 1e at the end portion 5b,
A stable connection is obtained from a microwave point of view, and this connection does not require the use of expensive silver solder as in the past, requiring only a small number of man-hours. The outer diameter of gasket 4 is 3 m.
The inner diameter of the gasket 4 may be the same as or slightly smaller than the hole diameter of the flange metal cylinder 5.
The gasket needs to be the same as or larger than the outer diameter of the gasket (see figure), but smaller than the outer diameter of the 5m tail, making gasket insertion very easy, reducing man-hours, and reducing the weight of the gasket itself. Furthermore, -v Gnetron body 1
5 of the metal cylinder 6 even if the hole of the yoke 3m is eccentric.
By setting the inner diameter of the gasket 4 larger than the outer diameter of the C section, the elasticity of the gasket 4 is uniform in all parts, and since the waveguide receiver is concentric with the hole in the part 20 and the hole 3, , an ideal connection is possible. Furthermore, if a short slit is provided at the end 5b of the metal cylinder 5 at St that does not impede the microwave connection, fitting becomes easier. If the metal cylinder 5 is made of a magnetic material, such as a galvanized iron plate, the permanent magnet 2aK will be attracted to the 11, so the forced fitting part at the end 5b should be formed with a degree of fitting that allows for good contact in terms of Micro technology. If there is, there is little risk that the metal cylinder 5 will come out.
第7図に示した実施例では、ガスケット4を金属8曽5
と璽−夕31とで挾持するようKなっている。この例の
場合ガスケット4の内掻を小さ目に設定し【おけばガス
ケット4と金属円筒5とを別工楊で組合せて、組立て部
品として供給でき、一層工数が減る。嬉6図に示した実
施例でも同様にできる。In the embodiment shown in FIG.
It is designed so that it can be held between 31 and 31. In this example, if the internal clearance of the gasket 4 is set small, the gasket 4 and the metal cylinder 5 can be assembled separately and supplied as an assembled part, further reducing the number of man-hours. The same can be done with the embodiment shown in Figure 6.
マグネトロンの発振には比較的高調波成分が多いが、第
8.9図中のh寸法すなわち金属封止部材l・と金属円
筒5とに囲まれた空間の軸方向長さを、不要放射を抑制
したい特定^調波の波長(電気長)の#tばl/4
Kすることにより抑制効果が得られる。第9図の実施例
では強制嵌合させる端部5bが折返し構造罠なっている
ので挿入が容易となり工数が低減される。The oscillation of a magnetron has relatively many harmonic components, but the dimension h in Fig. 8.9, that is, the axial length of the space surrounded by the metal sealing member l and the metal cylinder 5, can be used to eliminate unnecessary radiation. #tbal/4 of the wavelength (electrical length) of the specific harmonic that you want to suppress
A suppressive effect can be obtained by adding K. In the embodiment shown in FIG. 9, the end portion 5b to be forcibly fitted has a folded trap structure, which facilitates insertion and reduces the number of man-hours.
以上説明したように本発明によれば、ガスケット脱落や
ガスケット焼け、磁石割れなどが生じなくなり、しかも
工数なども減少する。As explained above, according to the present invention, gasket falling off, gasket burning, magnet cracking, etc. do not occur, and the number of man-hours is also reduced.
第1図は従来のマグネトロンの一例を示す図、第2図は
そのガスケット近傍拡大図、第3図は異なったガスケッ
ト保持構造の従来例図、第4図はマグネトロンと導波管
との接続状態図、第5図は従来のマグネトロンの導波管
との接続時におけるガスケット浮上り説明図、第6〜9
図はそれぞれ異なる本発明実施例の要部拡大図である。
1・・・・出力側金属封止部材、1f・・・出力側絶縁
物、2m・・・永久磁石、3m・・・ヨーク、4・・・
ガスケット、5・・・つば付き金属円筒、5m・・・つ
ば、5b・・・強制嵌合する端部。Figure 1 is a diagram showing an example of a conventional magnetron, Figure 2 is an enlarged view of the vicinity of its gasket, Figure 3 is a diagram of a conventional example of a different gasket holding structure, and Figure 4 is a state of connection between the magnetron and waveguide. Figure 5 is an explanatory diagram of the gasket floating when connected to a conventional magnetron waveguide, Figures 6 to 9
The figures are enlarged views of main parts of different embodiments of the present invention. 1...Output side metal sealing member, 1f...Output side insulator, 2m...Permanent magnet, 3m...Yoke, 4...
Gasket, 5...Metal cylinder with flange, 5m...Brim, 5b...Forcibly fitted end.
Claims (1)
面導電部材と、導液管壁との間に、jIL導電性かつ高
弾性のガスケットを介在させて、導波管に取付けるよう
にしたマグネトロンにおいて、1IIi円筒端郁に封着
され、絶縁物を介して出力端子を支持する金属封止部材
の円筒状部に、つば付き金属円筒のつばのない端部な強
制嵌合して固着させ、この円筒の軸方崗出力端子寄り端
部のつばと、他の外表面導電部材とで、前記ガスケット
を挾持させたことを特徴とするマグネト窒ン。 i 餉記金属對止部材と前記金属円筒と<Sまれだ空間
の軸方内憂さを、不要放射を抑制すべき特定な電波の波
畏の捏ぼ1/4とした特許請求の範8第1項記載のマグ
ネトロン。[Claims] 1. A jIL electrically conductive and highly elastic gasket is interposed between the outer surface conductive member insulated with respect to the output terminal located in the waveguide and the liquid guide tube wall, and the In a magnetron that is attached to a wave tube, the cylindrical part of the metal sealing member that is sealed to the 1IIi cylinder end and supports the output terminal through an insulator is attached to the flangeless end of the flange-equipped metal cylinder. A magnetron nitrogen gasket, characterized in that the gasket is forcibly fitted and fixed, and the gasket is held between the collar at the end of the cylinder near the axial output terminal and another conductive member on the outer surface. i. Claim 8, in which the axial distance between the metal blocking member, the metal cylinder, and the rare space is equivalent to 1/4 of the fear of specific radio waves whose unnecessary radiation should be suppressed. The magnetron described in item 1.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP19681581A JPS58100333A (en) | 1981-12-09 | 1981-12-09 | Magnetron |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP19681581A JPS58100333A (en) | 1981-12-09 | 1981-12-09 | Magnetron |
Publications (2)
Publication Number | Publication Date |
---|---|
JPS58100333A true JPS58100333A (en) | 1983-06-15 |
JPH0216535B2 JPH0216535B2 (en) | 1990-04-17 |
Family
ID=16364114
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP19681581A Granted JPS58100333A (en) | 1981-12-09 | 1981-12-09 | Magnetron |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS58100333A (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS59187060U (en) * | 1983-05-31 | 1984-12-12 | 松下電子工業株式会社 | magnetron |
-
1981
- 1981-12-09 JP JP19681581A patent/JPS58100333A/en active Granted
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS59187060U (en) * | 1983-05-31 | 1984-12-12 | 松下電子工業株式会社 | magnetron |
JPH0310601Y2 (en) * | 1983-05-31 | 1991-03-15 |
Also Published As
Publication number | Publication date |
---|---|
JPH0216535B2 (en) | 1990-04-17 |
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