JP3261726B2 - Magnetron - Google Patents

Magnetron

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Publication number
JP3261726B2
JP3261726B2 JP06454092A JP6454092A JP3261726B2 JP 3261726 B2 JP3261726 B2 JP 3261726B2 JP 06454092 A JP06454092 A JP 06454092A JP 6454092 A JP6454092 A JP 6454092A JP 3261726 B2 JP3261726 B2 JP 3261726B2
Authority
JP
Japan
Prior art keywords
output
magnetron
cavity
harmonic
choke
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
Application number
JP06454092A
Other languages
Japanese (ja)
Other versions
JPH05266812A (en
Inventor
守 黒葛原
清二 北風
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.)
Hitachi Ltd
Original Assignee
Hitachi Ltd
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Filing date
Publication date
Application filed by Hitachi Ltd filed Critical Hitachi Ltd
Priority to JP06454092A priority Critical patent/JP3261726B2/en
Publication of JPH05266812A publication Critical patent/JPH05266812A/en
Application granted granted Critical
Publication of JP3261726B2 publication Critical patent/JP3261726B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

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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、不要高調波とくに第5
高調波の低減に有効なチョークをマイクロ波出力部に挿
入した電子レンジ用などに好適なマグネトロンに関す
る。
BACKGROUND OF THE INVENTION The present invention relates to an unnecessary harmonic, especially a fifth harmonic.
The present invention relates to a magnetron suitable for use in a microwave oven in which a choke effective for reducing harmonics is inserted into a microwave output unit.

【0002】[0002]

【従来の技術】マグネトロンでは、陽極内周に形成され
た空洞共振器群に、所謂πモードの基本波のみならず、
第2、第3、第4、第5、第6、第7高調波等の高調波
も同時に発生される。これら高調波が基本波と共に外部
へ電波として放射されると、基本波以外はいわゆる不要
波であって、雑音電波として通信障害を生じる。マグネ
トロンは、極力、上記不要高調波の放射が少なくなるよ
うに設計され、かかる不要高調波が放射されるのを抑制
するために、従来から、同軸構造の出力部に特定の不要
高調波の伝搬を抑制するためのチョークを取付けてい
た。
2. Description of the Related Art In a magnetron, not only a fundamental wave of a so-called π mode but also a group of cavity resonators formed on an inner periphery of an anode are provided.
Harmonics such as the second, third, fourth, fifth, sixth, and seventh harmonics are also generated at the same time. When these harmonics are radiated to the outside together with the fundamental wave, other than the fundamental wave are so-called unnecessary waves, which cause communication failure as noise radio waves. Magnetrons are designed to minimize the emission of the unwanted harmonics as much as possible.In order to suppress the emission of such unwanted harmonics, the propagation of specific unwanted harmonics to the output of the coaxial structure has been conventionally required. Chokes to control

【0003】図2は従来のマグネトロンの一例の管軸を
含む平面による断面図で、図中、1は陰極、2は陽極円
筒、3は陽極円筒内壁から放射状に突出したベイン、4
は陰極1とベイン3の先端とに挾まれた円筒状の作用空
間に管軸方向の静磁界を形成させるための磁極、5は上
記磁界形成のための起磁力源となる円環状の永久磁石、
6は組立の便宜上、上下二部分に分割され管外磁気回路
を形成するヨーク、7は出力部、8は出力部を接地電位
の陽極やそれと同電位のヨーク等から直流的に絶縁する
アルミナセラミックス円筒よりなる出力側絶縁体、9は
一端が陽極円筒とベインとで陽極内周に形成された空洞
共振器群の一つのベインの上端面に接続され他端が出力
部に接続されている出力導体、10は一端が陽極円筒2
の上端部に固着され他端が出力側絶縁体8に固着された
封着金属体、11、12は周辺部が封着金属体10にろ
う付け固着され高調波チョークを形成する金属片、13
は内部を通る出力導体9と共に圧切して封止切られた金
属製排気管の端部、14は内部の孔の周囲が排気管の端
部13の外面に固着され高調波チョークを形成するカッ
プ状の金属片(金属製排気管の端部13と金属片14の
外部に金属カバーを被せて出力部7を形成)、15、1
6はそれぞれ封着金属体10と金属片11、12により
形成された高調波チョーク(これらの部材に囲まれた部
分が何れも特定高調波(ここでは、第5高調波)に対す
る1/4波長の空洞共振器を形成している)、17は金
属線を編組しプレス成形したガスケット、18は封着金
属体10に固着され上端部がガスケット17に電気的に
接触している金属円筒、19は其の中央の孔の周辺の短
い円筒部が陽極円筒の外側に嵌合固着されヨーク側端部
も短く折り曲げて接触面を設けた冷却フィンである。出
力部の出力導体9と封着金属体10とでいわゆる同軸構
造を形成しており、封着金属体10は同軸構造の外導体
を、また出力導体9は内導体の役割をする。ガスケット
17は封着金属体10に固着された金属円筒18の外側
に密着して電気的に接続され、出力部からの電波洩れを
防止する。なお、上記高調波チョークを形成する金属片
11、12の円環状の底面は従来は同軸構造の軸方向に
対して直交するように形成されていた。
FIG. 2 is a sectional view taken along a plane including a tube axis of an example of a conventional magnetron. In the figure, 1 is a cathode, 2 is an anode cylinder, 3 is a vane projecting radially from the inner wall of the anode cylinder, 4
Are magnetic poles for forming a static magnetic field in the tube axis direction in a cylindrical working space sandwiched between the cathode 1 and the tip of the vane 3, and 5 is an annular permanent magnet serving as a magnetomotive force source for forming the magnetic field. ,
Reference numeral 6 denotes a yoke that is divided into upper and lower parts for convenience of assembly to form an extra-tube magnetic circuit, 7 denotes an output unit, and 8 denotes an alumina ceramic that insulates the output unit from an anode at a ground potential or a yoke at the same potential. An output-side insulator 9 consisting of a cylinder, an output having one end connected to the upper end surface of one vane of a group of cavity resonators formed on the inner periphery of the anode by the anode cylinder and the vane, and the other end connected to the output section One end of the conductor 10 is an anode cylinder 2
A metal piece which is fixed to the upper end portion and has the other end fixed to the output side insulator 8;
Is an end of a metal exhaust pipe cut off and sealed together with an output conductor 9 passing through the inside, and 14 is a cup around an inner hole is fixed to the outer surface of the end 13 of the exhaust pipe to form a harmonic choke. Metal pieces (the output section 7 is formed by covering a metal cover over the end 13 and the metal piece 14 of the metal exhaust pipe), 15, 1
Numeral 6 is a harmonic choke formed by the sealing metal body 10 and the metal pieces 11 and 12 (each of the portions surrounded by these members has a quarter wavelength with respect to the specific harmonic (here, the fifth harmonic). , 17 is a gasket formed by braiding a metal wire and press-molding, 18 is a metal cylinder fixed to the sealing metal body 10 and having an upper end in electrical contact with the gasket 17, 19 Is a cooling fin in which a short cylindrical portion around the center hole is fitted and fixed to the outside of the anode cylinder and the yoke side end is also bent short to provide a contact surface. The output conductor 9 of the output portion and the sealing metal body 10 form a so-called coaxial structure. The sealing metal body 10 functions as an outer conductor having a coaxial structure, and the output conductor 9 functions as an inner conductor. The gasket 17 is in close contact and electrically connected to the outside of the metal cylinder 18 fixed to the sealing metal body 10 to prevent the electric wave from leaking from the output unit. The annular bottom surfaces of the metal pieces 11 and 12 forming the harmonic choke are conventionally formed so as to be orthogonal to the axial direction of the coaxial structure.

【0004】陽極円筒2など、マグネトロンの外面をな
す部分は安全のため接地され、これに対して陰極には大
きな負電圧が印加されている。陰極から放出され陽極に
向けて加速された電子は作用空間内の管軸方向静磁界と
運動方向とに直交するローレンツの力により作用空間内
を電子雲をなして周回運動し、陽極円筒とベインとで陽
極円筒内周に形成された空洞共振器群内に高周波振動を
形成させる。定常状態では、隣接する空洞共振器内の振
動が丁度逆位相のπモード振動が基本波となって圧倒的
に強いが、それ以外に第2、第3、第4、第5、第6、
第7高調波等の高調波も同時に発生される。これらの所
謂不要高調波が外部に放射されると、それと同じ周波数
帯を使用する通信装置にとっては雑音電波となるため、
法規的にも規制されている。そのため、従来から、上記
のように、マイクロ波電力を空洞共振器から出力部へ導
く出力導体の途中に、それを囲む特定高調波用空洞共振
器を設置して、そこに出力導体を通る当該高調波に同調
した共振振動を発生させ、出力導体のその部分が上記不
要高調波に対して高いインピーダンスを呈し、出力部か
ら外部へ放射される当該不要高調波の電波強度を弱める
チョークあるいはトラップとして作用するようにしてい
る。
A portion forming the outer surface of the magnetron, such as the anode cylinder 2, is grounded for safety, whereas a large negative voltage is applied to the cathode. The electrons emitted from the cathode and accelerated toward the anode orbit around the working space in an electron cloud due to the static magnetic field in the axial direction of the tube in the working space and the Lorentz force orthogonal to the direction of movement, and the anode cylinder and the vane With this, a high-frequency vibration is formed in the cavity resonator group formed on the inner periphery of the anode cylinder. In the steady state, the vibration in the adjacent cavity resonators is overwhelmingly strong with the π-mode vibration having just the opposite phase as the fundamental wave, but the second, third, fourth, fifth, sixth, and
Harmonics such as the seventh harmonic are also generated at the same time. When these so-called unnecessary harmonics are radiated to the outside, they become noise radio waves for communication devices using the same frequency band.
It is also regulated by law. Therefore, conventionally, as described above, in the middle of the output conductor that guides microwave power from the cavity resonator to the output unit, a specific harmonic cavity resonator that surrounds the output conductor is provided, and the output conductor passes therethrough. As a choke or trap that generates a resonant vibration tuned to the harmonics, that part of the output conductor presents a high impedance to the unnecessary harmonics and weakens the radio wave intensity of the unnecessary harmonics radiated from the output unit to the outside It works.

【0005】上記のようなチョークに類似した構造は、
例えば、特開昭63−131438号公報等に記載され
ている。
[0005] The structure similar to the above-mentioned chalk is
For example, it is described in JP-A-63-131438.

【0006】[0006]

【発明が解決しようとする課題】近年、テレビジョンの
衛星放送が開始されるようになったが、その放送周波数
帯12GHzは、一般家庭に広く普及している電子レン
ジなどに用いる2450MHz用マグネトロンの第5高
調波に該当し、電子レンジ用マグネトロンに対して第5
高調波抑制対策が強く求められるようになった。そのた
め、既に図2に示したような空洞共振器を設けたマグネ
トロンが生産され、12GHz帯の第5高調波が出力部
から放射されるのを抑制する効果を挙げてきたが、波長
の短い第5高調波用チョークは寸法が小さく高い精度で
製作することが必要で、かつ抑止すべき周波数帯域は実
質的に11.75〜12.75GHzと広いので、図2
に示したような従来の構造においても、チョークを1
5、16と二つに別け、各々の共振周波数をずらして広
い周波数帯域に対応しようとしている。
In recent years, satellite broadcasting of television has started, and its broadcasting frequency band of 12 GHz is a 2450 MHz magnetron used for microwave ovens widely used in ordinary households. Corresponds to the 5th harmonic and the 5th harmonic
Harmonic suppression measures have been strongly required. Therefore, a magnetron having a cavity resonator as shown in FIG. 2 has already been produced, and the effect of suppressing the emission of the fifth harmonic in the 12 GHz band from the output unit has been obtained. Since the five-harmonic choke needs to be manufactured with small dimensions and high accuracy, and the frequency band to be suppressed is substantially as wide as 11.75 to 12.75 GHz, FIG.
In the conventional structure as shown in FIG.
It is divided into 5 and 16, and it is trying to correspond to a wide frequency band by shifting each resonance frequency.

【0007】上記チョーク15、16などの共振周波数
には、その断面の深さ(円環状の底面の最低部から内側
円筒面の上端まで)が大きく影響するので、具体的に寸
法を設定する時には概算の狙い値に対し数種類の寸法の
金属片を準備して試作、実験して確認している。その
際、図2のチョーク15において、共振周波数が一層低
くなるように調整したい場合、金属片11の内円筒部の
高さを増して共振周波数を下げようとしても、チョーク
のもう一方の構成要素である封着金属体10の外円筒部
の高さが固定されており、上記内円筒部の高さを伸ばす
だけでは共振周波数を下げることはできない(チョーク
は外円筒面と環状の底面と内円筒面で形成されるが、内
円筒面と外円筒面が対向していない個所は有効に作用せ
ず、内円筒面だけ高さを伸ばしても出力側絶縁体と対向
している部分は役に立たない)。
Since the depth of the cross section (from the lowest part of the annular bottom surface to the upper end of the inner cylindrical surface) greatly affects the resonance frequency of the chokes 15 and 16 and the like, when the dimensions are specifically set, Several types of metal pieces are prepared for the estimated target value, and prototypes are made and tested. At that time, in the choke 15 of FIG. 2, if it is desired to adjust the resonance frequency to be lower, the other component of the choke may be used even if the resonance frequency is lowered by increasing the height of the inner cylindrical portion of the metal piece 11. The height of the outer cylindrical portion of the sealing metal body 10 is fixed, and the resonance frequency cannot be lowered only by increasing the height of the inner cylindrical portion (the choke is formed between the outer cylindrical surface and the annular bottom surface. It is formed of a cylindrical surface, but the part where the inner cylindrical surface and the outer cylindrical surface do not face each other does not work effectively, and even if the inner cylindrical surface is extended, the part facing the output side insulator is useful. Absent).

【0008】尤も封着金属体10の外円筒部の高さも増
せば良いのであるが、そうするとマグネトロンの出力部
全長を変えることになり、マイクロ波出力の位相や負荷
との結合度が変化してしまい、同一の封着金属体10を
有するマグネトロンと動作特性上の互換性が無くなって
しまうという問題が生ずる。
It is possible to increase the height of the outer cylindrical portion of the sealing metal body 10, but this would change the total length of the output portion of the magnetron, changing the phase of the microwave output and the degree of coupling with the load. As a result, there arises a problem that compatibility with a magnetron having the same sealing metal body 10 in operating characteristics is lost.

【0009】本発明は上記従来の課題を解決し、チョー
クの共振周波数の調整を容易にしたマグネトロンを提供
することを目的とする。
An object of the present invention is to provide a magnetron which solves the above-mentioned conventional problems and facilitates adjustment of the choke resonance frequency.

【0010】[0010]

【課題を解決するための手段】上記課題を解決するため
に本発明においては、空洞共振器群に発生したマイクロ
波電力を取り出すために、空洞共振器のベインに接続し
た内導体と陽極円筒端部や磁極を覆う金属真空外囲器の
延長である外導体で形成した同軸構造の出力部内に、周
縁が前記外導体に密着した円環状底面部とその内側円周
から前記内導体に同軸に延在する円筒部よりなり前記マ
イクロ波電力の基本波の特定高調波に対し空洞共振器を
形成して該高調波の伝搬を阻止するチョークを複数個配
設したマグネトロンにおいて、前記チョークの円環状底
面部を前記同軸構造出力部の軸方向に対して傾斜させて
円錐面状に形成させることにした。
In order to solve the above-mentioned problems, according to the present invention, in order to extract microwave power generated in a group of cavity resonators, an inner conductor connected to a vane of the cavity resonator and an anode cylindrical end are provided. In the output portion of the coaxial structure formed of an outer conductor that is an extension of the metal vacuum envelope that covers the portion and the magnetic pole, the periphery is coaxial with the inner conductor from the annular bottom portion and the inner circumference thereof that are in close contact with the outer conductor. In a magnetron having a plurality of chokes each including a cylindrical portion extending and forming a cavity resonator for a specific harmonic of the fundamental wave of the microwave power to prevent propagation of the harmonic, the ring of the choke is provided. The bottom portion is formed in a conical shape by inclining with respect to the axial direction of the coaxial structure output portion.

【0011】[0011]

【作用】マグネトロンの同軸構造出力部の途中に、その
内導体すなわち出力導体を囲んで配置するチョークを上
記のようにすれば、例えば、チョークを形成する金属片
の内円筒の高さを増し、同時にその円環状底面を軸方向
に対して傾斜させて円錐状にしぼり込む形にすれば実質
的にチョーク寸法が大きくなる(Lが大きくなる)ので
共振周波数が低くなり、また、チョークを形成する金属
片の円環状底面を上記と逆方向に傾斜させ(封着金属体
側の位置を変えずに底面から内円筒面に移る位置を上
げ)れば、チョークの金属片の内円筒の上端が封着金属
体と出力側絶縁体の封着部を越えて上に行き、金属片の
内円筒の出力側絶縁体と対向する部分が長くなるが、既
述のようにこの部分は共振周波数に影響せず、実質的に
内円筒の高さを減らしたことになってLが小さくなり共
振周波数が高くなる。
If the choke arranged around the inner conductor, that is, the output conductor is arranged in the middle of the coaxial structure output part of the magnetron as described above, for example, the height of the inner cylinder of the metal piece forming the choke is increased, At the same time, if the annular bottom surface is inclined with respect to the axial direction and formed into a conical shape, the choke size is substantially increased (L is increased), so that the resonance frequency is reduced and a choke is formed. By inclining the annular bottom surface of the metal piece in the opposite direction (raising the position from the bottom surface to the inner cylindrical surface without changing the position of the sealing metal body side), the upper end of the inner cylinder of the metal piece of the chalk is sealed. The portion of the inner cylinder of the metal piece facing the output side insulator becomes longer, but this portion affects the resonance frequency as described above. Without substantially reducing the height of the inner cylinder L is the resonance frequency increases smaller supposed to have.

【0012】[0012]

【実施例】図1は本発明一実施例の、出力部の高調波チ
ョーク設置個所の近傍を拡大して示す断面図である。出
力部7では、内導体すなわち出力導体9をマグネトロン
の管軸上に配置して金属排気管13の中に通し、管内を
真空に排気してから排気管13と共に封止切ってある。
排気管13にはカップ状の金属片14が、その頂面の孔
の周囲で封止され、また金属片14の下端はアルミナセ
ラミックスなどからなる円筒状の出力側絶縁体8の上端
に封着してあり、これらの外側に図示のように排気管1
3の圧切した端部を保護する金属カバーが圧入されてい
る。出力側絶縁体8の下端には真空外囲器となる封着金
属体10が同軸に接合されている。この出力側絶縁体8
の下部外側を、図示してないガスケット(図2中の1
7)と電気的に接触して電波漏洩を防止し下方で封着金
属体10に嵌合する金属円筒18が囲んでいる。封着金
属体10の上部の内周面に、第5高調波漏洩防止用のチ
ョーク15、16を構成する金属片11、12の外周部
が接合されている。ここで、チョーク15の底面を形成
する金属片11の平板部11aは管軸に対して傾斜させ
円錐状に成形されているので、金属片11の内円筒部1
1bのチョークとしての有効な高さは大きくなり、チョ
ーク15の共振周波数は、従来(平板部11aが管軸に
直交)よりも低くなっている。本実施例ではチョーク1
5に対してのみ共振周波数の調整を行っているが、チョ
ーク16に対しても同様にして共振周波数の調整ができ
ることは明らかである。
FIG. 1 is an enlarged sectional view showing the vicinity of a place where a harmonic choke is installed in an output section according to an embodiment of the present invention. In the output section 7, the inner conductor, that is, the output conductor 9, is disposed on the tube axis of the magnetron, passes through the metal exhaust pipe 13, and the inside of the pipe is evacuated to vacuum.
A cup-shaped metal piece 14 is sealed around the hole on the top surface of the exhaust pipe 13, and the lower end of the metal piece 14 is sealed to the upper end of a cylindrical output-side insulator 8 made of alumina ceramics or the like. The exhaust pipe 1 is located outside these as shown in the figure.
The metal cover for protecting the pressed-off end of No. 3 is press-fitted. A sealing metal body 10 serving as a vacuum envelope is coaxially joined to the lower end of the output side insulator 8. This output side insulator 8
The lower outside of the gasket (not shown in FIG. 2).
7), a metal cylinder 18 fitted to the sealing metal body 10 at the lower side to prevent radio wave leakage and to surround the metal cylinder 18 is surrounded. The outer peripheral portions of the metal pieces 11 and 12 constituting the chokes 15 and 16 for preventing the fifth harmonic leakage are joined to the inner peripheral surface of the upper part of the sealing metal body 10. Here, the flat plate portion 11a of the metal piece 11 forming the bottom surface of the choke 15 is formed in a conical shape by being inclined with respect to the tube axis.
The effective height of the choke 1b is increased, and the resonance frequency of the choke 15 is lower than that of the related art (the flat portion 11a is orthogonal to the tube axis). In this embodiment, the chalk 1
Although the resonance frequency is adjusted only for No. 5, it is apparent that the resonance frequency can be similarly adjusted for the choke 16.

【0013】[0013]

【発明の効果】以上説明したように本発明によれば、同
軸構造の出力部内に設けた不要高調波が放射されるのを
防止するための複数のチョークの共振周波数を不要高調
波の帯域に対して容易に調整できるようになるため、低
雑音性能良好なマグネトロンが得られる。
As described above, according to the present invention, the resonance frequencies of a plurality of chokes provided in the output portion of the coaxial structure for preventing unnecessary harmonics from being radiated are set within the unnecessary harmonic band. In this case, the magnetron can be easily adjusted, so that a magnetron having good low noise performance can be obtained.

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

【図1】本発明一実施例の要部、すなわち出力部の高調
波チョーク設置個所の近傍を拡大して示す断面図であ
る。
FIG. 1 is an enlarged sectional view showing a main part of an embodiment of the present invention, that is, a vicinity of a place where a harmonic choke is installed in an output part.

【図2】従来のマグネトロンの一例の管軸を含む平面に
よる断面図である。
FIG. 2 is a sectional view of a plane including a tube axis of an example of a conventional magnetron.

【符号の説明】[Explanation of symbols]

1…陰極、 2…陽極円筒、 3…ベイン、 4…磁
極、 5…永久磁石、6…ヨーク、 7…出力部、 8
…出力側絶縁体、 9…出力導体、 10…封着金属
体、 11、12…金属片、 13…排気管の端部、1
4…カップ状の金属片、 15、16…チョーク、 1
7…ガスケット、 18…金属円筒、 19…冷却フィ
ン。
DESCRIPTION OF SYMBOLS 1 ... Cathode, 2 ... Anode cylinder, 3 ... Vane, 4 ... Magnetic pole, 5 ... Permanent magnet, 6 ... Yoke, 7 ... Output part, 8
... output side insulator, 9 ... output conductor, 10 ... sealing metal body, 11, 12 ... metal piece, 13 ... end of exhaust pipe, 1
4: cup-shaped metal piece, 15, 16: chalk, 1
7 gasket, 18 metal cylinder, 19 cooling fin.

Claims (1)

(57)【特許請求の範囲】(57) [Claims] 【請求項1】管軸に同心の陰極を、管軸方向に静磁界が
形成された作用空間を隔てて、陽極円筒とその内壁から
放射状に突出した偶数枚のベインよりなる偶数個の空洞
共振器が同心に囲み、空洞共振器群に発生したマイクロ
波電力を取り出すために空洞共振器のベインに接続した
内導体と陽極円筒端部や磁極を覆う金属真空外囲器の延
長である外導体で形成した同軸構造の出力部を備え、更
にこの出力部内に、周縁が前記外導体に密着した円環状
底面部とその内側円周から前記内導体に同軸に延在する
円筒部よりなり前記マイクロ波電力の基本波の特定高調
波に対し空洞共振器を形成して該高調波の伝搬を阻止す
るチョークを複数個配設したマグネトロンにおいて、前
記チョークの円環状底面部を前記同軸構造出力部の軸方
向に対して傾斜させて円錐面状に形成したことを特徴と
するマグネトロン。
A cathode concentric with a tube axis and an even number of cavity resonances composed of an anode cylinder and an even number of vanes radially protruding from an inner wall of the anode cylinder across a working space in which a static magnetic field is formed in the tube axis direction. The inner conductor is concentrically surrounded by the inner conductor connected to the cavities of the cavity to extract the microwave power generated in the cavity, and the outer conductor is an extension of the metal vacuum envelope that covers the anode cylindrical end and the magnetic pole. The output portion having a coaxial structure formed by the above, further comprising, in the output portion, an annular bottom surface portion whose peripheral edge is in close contact with the outer conductor, and a cylindrical portion extending coaxially from the inner circumference to the inner conductor. In a magnetron in which a plurality of chokes for forming a cavity for a specific harmonic of a fundamental wave of wave power and preventing the propagation of the harmonic are arranged, an annular bottom portion of the choke is used as an output of the coaxial structure output portion. Inclined with respect to the axial direction Magnetron, characterized in that formed in the conical shape Te.
JP06454092A 1992-03-23 1992-03-23 Magnetron Expired - Fee Related JP3261726B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP06454092A JP3261726B2 (en) 1992-03-23 1992-03-23 Magnetron

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP06454092A JP3261726B2 (en) 1992-03-23 1992-03-23 Magnetron

Publications (2)

Publication Number Publication Date
JPH05266812A JPH05266812A (en) 1993-10-15
JP3261726B2 true JP3261726B2 (en) 2002-03-04

Family

ID=13261162

Family Applications (1)

Application Number Title Priority Date Filing Date
JP06454092A Expired - Fee Related JP3261726B2 (en) 1992-03-23 1992-03-23 Magnetron

Country Status (1)

Country Link
JP (1) JP3261726B2 (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
KR19990001481A (en) * 1997-06-16 1999-01-15 구자홍 magnetron

Also Published As

Publication number Publication date
JPH05266812A (en) 1993-10-15

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