JPH065211A - Magnetron - Google Patents
MagnetronInfo
- Publication number
- JPH065211A JPH065211A JP16568992A JP16568992A JPH065211A JP H065211 A JPH065211 A JP H065211A JP 16568992 A JP16568992 A JP 16568992A JP 16568992 A JP16568992 A JP 16568992A JP H065211 A JPH065211 A JP H065211A
- Authority
- JP
- Japan
- Prior art keywords
- vane
- magnetron
- tube axis
- face
- peripheral edge
- 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
(57)【要約】
【目的】ベインの片側端面だけに均圧環を設置し、しか
も発振された基本波の周波数スペクトラムは、サイドロ
ーブやスプリアスが良く抑制されて雑音対策が容易な、
性能価格比の良好なマグネトロンを提供することにあ
る。
【構成】ベインの片側端面だけに均圧環を設置し、それ
による周波数対策としてベイン先端には張出し部を設け
た陽極を用い、そのマイクロ波出力取出部側のベイン端
面に最も近接する磁極の内周縁部の面を平坦にした。
(57) [Abstract] [Purpose] A pressure equalizing ring is installed only on one end face of the vane, and the frequency spectrum of the oscillated fundamental wave has well suppressed side lobes and spurious noise, making it easy to take noise countermeasures.
It is to provide a magnetron with a good performance price ratio. [Structure] An equalizer ring is installed only on one end face of the vane, and an anode with a bulge at the tip of the vane is used as a frequency countermeasure, and the magnetic poles closest to the vane end face on the microwave output extraction side are used. The peripheral surface was flattened.
Description
【0001】[0001]
【産業上の利用分野】本発明は、ベインのマイクロ波出
力取出部側端面のみに均圧環を配置して工数を低減さ
せ、所望共振周波数への合わせ込みを容易にし、しか
も、内蔵する空洞共振器群に励振されるマイクロ波の基
本波の周波数スペクトラムをサイドローブやスプリアス
の十分抑制されたものに改善した、外部へ放射されるノ
イズが少ない電子レンジ等に好適なマグネトロンに関す
る。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention reduces the number of steps by arranging a pressure equalizing ring only on the end face of the vane on the side of the microwave output extraction portion, facilitating adjustment to a desired resonance frequency, and further, incorporating a cavity resonance. The present invention relates to a magnetron suitable for a microwave oven or the like, in which the frequency spectrum of the fundamental wave of the microwave excited in the vessel group is improved to a side lobe or spurious that is sufficiently suppressed, and which has a small amount of noise radiated to the outside.
【0002】[0002]
【従来の技術】図2は従来のマグネトロンの一例の管軸
を通る平面による断面図である。陰極1の周囲を、円筒
状の作用空間を隔てて、陽極円筒2の内壁から放射状に
突出したベイン3の先端が取り囲んでいる。陽極円筒と
ベインとはホビングにより一体成形されたものも、両者
それぞれ別個に製作したものを、ろう付けしたものもあ
る。陽極円筒2の上下には、管軸方向に短い円環状の永
久磁石6が配置され、この磁石が起磁力源となって、永
久磁石6の外側面に接して管体外側を囲み外部磁気回路
となるヨーク7と、陽極円筒2の端部と永久磁石6の内
側面との間に挾まれた外周縁部、及び、作用空間の端部
近くに伸びた内周縁部を有する磁極4によって、作用空
間内に管軸方向に静磁界が形成されている。陽極円筒2
など真空外囲器となる部分は安全上から接地され、陰極
1には高い直流負電位が印加されている。陰極1から接
地電位にあるベイン3の先端の方へ電子が吸引される
が、作用空間には管軸方向に静磁界が形成されているた
め、電子には磁界と運動方向とに直交する力が作用し、
ベインの先端を円周方向に横切って陰極側へ戻ろうとす
る電子も現れ、作用空間内に電子密度の高い部分と疎な
部分が生じ、高電子密度の電子雲が作用空間内を高速周
回して陽極円筒と隣接ベインとで形成された空洞共振器
群内にマイクロ波電気振動が励振される。空洞共振器群
内の電気振動のうち、最も強く安定して発振されるの
は、隣接空洞間で逆位相となる所謂πモードの振動であ
る。このπモード振動で同電位(同位相)となる点を連
結して此の振動を一層安定させるために、ベインを一つ
おきに交互に接続する内側均圧環10と外側均圧環11
とが、ベインの管軸方向端面に設けた溝の内部に収納設
置されている。マイクロ波電気振動を、ベインの端面に
取付けたアンテナ5によってマイクロ波出力取出部8に
導いて、外部で、例えば電子レンジで食物加熱用に、利
用する。なお、陰極1は加熱用給電線を介して陰極ステ
ム9によって支持されている。2. Description of the Related Art FIG. 2 is a sectional view taken along a plane passing through a tube axis of an example of a conventional magnetron. The tip of a vane 3 radially protruding from the inner wall of the anode cylinder 2 surrounds the cathode 1 with a cylindrical working space. The anode cylinder and the vane may be integrally molded by hobbing, or may be separately manufactured and brazed. An annular permanent magnet 6 which is short in the tube axis direction is arranged above and below the anode cylinder 2, and this magnet serves as a magnetomotive force source that contacts the outer surface of the permanent magnet 6 and surrounds the outside of the tubular body to form an external magnetic circuit. And a magnetic pole 4 having an outer peripheral edge portion sandwiched between the end portion of the anode cylinder 2 and the inner side surface of the permanent magnet 6 and an inner peripheral edge portion extending near the end portion of the working space. A static magnetic field is formed in the working space in the tube axis direction. Anode cylinder 2
For safety reasons, the portion that serves as a vacuum envelope is grounded, and a high DC negative potential is applied to the cathode 1. Electrons are attracted from the cathode 1 toward the tip of the vane 3 at the ground potential, but since a static magnetic field is formed in the working space in the tube axis direction, the electrons have a force perpendicular to the magnetic field and the movement direction. Acts,
Electrons that cross the tip of the vane in the circumferential direction and try to return to the cathode side also appear, and a part with a high electron density and a sparse part are generated in the action space, and an electron cloud with a high electron density orbits in the action space at a high speed. The microwave electric vibration is excited in the cavity resonator group formed by the anode cylinder and the adjacent vane. Among the electric vibrations in the cavity resonator group, what is oscillated most strongly and stably is so-called π-mode vibration having an opposite phase between the adjacent cavities. In order to further stabilize this vibration by connecting points having the same potential (same phase) by this π-mode vibration, every other one of the vanes is alternately connected to the inner pressure equalizing ring 10 and the outer pressure equalizing ring 11.
And are housed and installed inside the groove provided on the end surface of the vane in the tube axial direction. The microwave electric vibration is guided to the microwave output extraction portion 8 by the antenna 5 attached to the end surface of the vane, and is used outside, for example, for heating food in a microwave oven. The cathode 1 is supported by the cathode stem 9 via the heating power supply line.
【0003】現在、数量的に最も大きなマグネトロンの
用途は電子レンジ用であるが、家庭用電気製品の場合、
性能と並んで重要なことは、価格低廉なことである。し
たがって、電子レンジ用マグネトロンの場合、価格低減
のために種々工夫が凝らされる。上記従来のマグネトロ
ンでは、ベインのマイクロ波出力取出部側端面と陰極ス
テム側端面の両方に均圧環が設置されていたが、これが
片側端面に設置するだけで済めば、工数、部品代とも削
減できる。At present, the largest quantity of magnetrons are used for microwave ovens, but for household electric appliances,
As important as performance is price. Therefore, in the case of a magnetron for a microwave oven, various measures are taken to reduce the price. In the above-mentioned conventional magnetron, pressure equalizing rings were installed on both the microwave output extraction side end surface and the cathode stem side end surface of the vane, but if this is installed on one side end surface, man-hours and parts cost can be reduced. .
【0004】しかし、ベインの片側端面だけに均圧環を
設置して其の他の部分を従来のままにしておくと、空洞
の共振周波数が高くなり過ぎてしまう。これは、内、外
均圧環同士や均圧環と(その均圧環が接続されずに収納
溝底面の上を通過する)ベインとの間の静電容量が共振
周波数に影響するのに、それらの静電容量がほぼ半分に
なってしまうからである。この周波数の上昇を抑制する
ために、特願平2−405641号には、各ベインのマ
イクロ波出力取出部側端面のみに管軸から等距離に溝を
刻設して内部にベインを1枚おきに交互に電気的に接続
する内、外均圧環を収納させ、各ベインの先端に両隣接
ベインの先端側へ対称に突出し隣接ベイン側と平行平面
で対向する張出部分を設けて、上記静電容量の不足を補
い、更に、ベインの陰極ステム側端面に上記張出部分と
管軸から更に遠い部分との境界に段差を設けて管軸から
遠い部分のベインの幅を狭くして、管軸から遠い部分の
ベインのインダクタンス分を大きくする技術が記載され
ている。この技術によれば、空洞共振器の静電容量は増
加し、インダクタンス分も増加するので、均圧環をベイ
ンの片側端面だけに設けても、周波数を従来のものと同
様にすることができる。図3(a)は上記技術によるマ
グネトロンの陽極円筒の平面図を、図3(b)はその断
面図を示す。図中、31はベイン3の先端の張出部分、
3aは均圧環収納溝で、3bは張出部分と管軸から更に
遠い部分との境界の段差である。図示のものはホビング
加工により一体成形したもので、符号を付けてないアン
テナ端部取付け用の溝は、実際は1枚のベインだけに必
要であるが、旋盤加工で形成するので全てのベインの端
面に形成されている。なお、このようなマグネトロン陽
極をホビング加工により一体成形することは、ホブの形
状は多少複雑になるが、材料ブランクの中央部分で、材
料が押出される量が減少するため、ホブに対する抵抗が
減少し、ホブの寿命は長くなる。However, if the pressure equalizing ring is installed only on one end face of the vane and the other part is left as it is, the resonance frequency of the cavity becomes too high. This is because the capacitance between the inner and outer pressure equalizing rings or between the pressure equalizing ring and the vane (which passes over the bottom surface of the storage groove without connecting the pressure equalizing ring) affects the resonance frequency. This is because the capacitance will be almost halved. In order to suppress this increase in frequency, Japanese Patent Application No. 2-405641 discloses that each vane is provided with a single vane inside by engraving grooves equidistant from the tube axis only on the end face on the microwave output extraction side. Alternately electrically connected every other, accommodating the outer pressure equalizing ring, provided at the tip of each vane symmetrically projecting to the tip side of both adjacent vanes, and providing an overhanging portion facing the adjacent vane side in a parallel plane, Compensating for the lack of electrostatic capacity, further, at the cathode stem side end surface of the vane, a step is provided at the boundary between the overhanging portion and the portion farther from the tube axis to narrow the width of the vane at the portion far from the tube axis, A technique for increasing the inductance of the vane in the portion far from the tube axis is described. According to this technique, the capacitance of the cavity resonator increases and the amount of inductance also increases. Therefore, even if the pressure equalizing ring is provided only on one end face of the vane, the frequency can be made similar to the conventional frequency. FIG. 3A is a plan view of the anode cylinder of the magnetron according to the above technique, and FIG. 3B is a sectional view thereof. In the figure, 31 is a protruding portion of the tip of the vane 3,
Reference numeral 3a denotes a pressure equalizing ring storage groove, and 3b denotes a step on the boundary between the overhanging portion and the portion further away from the pipe axis. The one shown in the figure is integrally formed by hobbing, and the groove for attaching the antenna end part without reference numeral is actually required for only one vane, but since it is formed by lathe, the end faces of all vanes are formed. Is formed in. Note that integrally forming such a magnetron anode by hobbing makes the shape of the hob somewhat complicated, but the amount of material extruded in the central portion of the material blank decreases, so the resistance to the hob decreases. However, the hob will have a longer life.
【0005】[0005]
【発明が解決しようとする課題】しかし、上記のような
マグネトロン陽極を用いた場合、実際に励振されるマイ
クロ波振動の基本波の周波数スペクトラムは、図4に示
すように、サイドローブの抑制が十分でなく、スプリア
スも目立ち、マグネトロンを機器たとえば電子レンジに
取付けて使用した場合に、外部に放射されるノイズが多
いという問題が生じた。However, when the magnetron anode as described above is used, the frequency spectrum of the fundamental wave of the microwave vibration actually excited is such that the side lobe is suppressed as shown in FIG. Not enough, spurious was also noticeable, and when the magnetron was attached to a device such as a microwave oven for use, a large amount of noise was emitted to the outside.
【0006】電子レンジでは、2450MHzのマイク
ロ波を使用することになっているが、その第5高調波が
外部に漏洩すると、近年非常に広範囲に利用されるよう
になって来た衛星放送の周波数帯にノイズとして現れて
問題になる。既に法規的に規制している国もある。従っ
て、均圧環をベインの片側端面だけで済むようにしたマ
グネトロンにとって、ノイズを抑制減少させることが課
題である。Microwave ovens are supposed to use microwaves of 2450 MHz, but if the fifth harmonic leaks to the outside, the frequency of satellite broadcasting has become very widespread in recent years. It appears as noise in the band and becomes a problem. Some countries are already legally regulated. Therefore, it is a problem to suppress and reduce noise in the magnetron in which the pressure equalizing ring is formed only on one end surface of the vane.
【0007】本発明は上記従来の課題を解決し、均圧環
の設置はベイン端面の片側だけで済ませながら、ノイズ
特に12GHz帯に現れるものを十分抑制できるように
した性能価格比の良好なマグネトロンを提供することを
目的とする。The present invention solves the above-mentioned problems of the prior art and provides a magnetron with a good performance-price ratio which can sufficiently suppress noise, especially that appearing in the 12 GHz band, while installing the pressure equalizing ring only on one side of the end face of the vane. The purpose is to provide.
【0008】[0008]
【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、ベインのマイクロ波出力取出部側
端面のみにベイン収納溝を設け、各ベインの先端に両隣
接ベインの先端側へ対称に突出し隣接ベイン側と平行平
面で対向する張出し部分を設け、ベインの陰極ステム側
端面に上記張出し部分と管軸から更に遠い部分との境界
に段差を設けて管軸から遠い部分のベインの幅を狭くし
たマグネトロンにおいて、マイクロ波出力取出部側ベイ
ン端面に最も近接する磁極内周縁部の面を平坦にした。In order to solve the above-mentioned problems, according to the present invention, a vane storage groove is provided only on the end face of the vane on the microwave output extraction side, and the tip of each vane is extended to the tip side of both adjacent vanes. Protruding symmetrically, providing an overhanging portion facing the adjacent vane side in a parallel plane, and providing a step at the boundary between the overhanging portion and the portion farther from the tube axis on the end surface of the vane on the cathode stem side, and the vane of the portion far from the tube axis In the magnetron with a narrow width, the surface of the inner peripheral edge of the magnetic pole closest to the end surface of the vane on the microwave output extraction side was flattened.
【0009】[0009]
【作用】本発明者は上記陽極構造を有するマグネトロン
のノイズを減少させるために、作用空間の端部の付近で
の磁界や電界の分布状態を変化させた場合について試
作、実験を重ねた結果、上記のようにマイクロ波出力取
出部側ベイン端面に最も近接する磁極内周縁部の面を平
坦にすることによって、マグネトロンが発生する基本波
の周波数スペクトラムがサイドローブやスプリアスの抑
制されたものになり、外部へ放射されるノイズが低減さ
れることを発見したのである。The present inventor repeated trial manufacture and experimentation in the case of changing the distribution state of the magnetic field and electric field near the end of the working space in order to reduce the noise of the magnetron having the above-mentioned anode structure. As described above, by flattening the surface of the inner peripheral edge of the magnetic pole that is closest to the end face of the vane on the microwave output extraction side, the frequency spectrum of the fundamental wave generated by the magnetron is one in which side lobes and spurs are suppressed. We have found that the noise radiated to the outside is reduced.
【0010】[0010]
【実施例】図1は本発明一実施例の要部である陽極円筒
や磁極を含む部分の側断面図である。図中、1は陰極、
2は陽極円筒、3はベイン、4は陽極円筒の陰極ステム
側に取付けた従来形の磁極、4aは陽極円筒のマイクロ
波出力取出部側に取付けた本発明に係る磁極、5はアン
テナで、従来形の磁極4はベインの端面に最も近接する
部分の面に突出部があるのに対し、本発明に係る磁極4
aのベイン端面に最も近接する部分の面は図示のように
平坦になっている。その結果、本発明マグネトロンの2
450MHzの基本波の周波数スペクトラムは図5に示
すようになり、従来のマグネトロンの場合には基本波の
スペクトラムが図4に示したようにマイクロ波応用装置
に割り当てられている2450MHzのISM帯の幅を
越えてはみ出していたのに対し、本発明マグネトロンの
場合は発振周波数スペクトラムのサイドローブやスプリ
アスが大幅に低減されている。従って、本発明マグネト
ロンをマイクロ波応用装置たとえば電子レンジに利用し
た場合、雑音電波漏洩対策が容易になる。1 is a side sectional view of a portion including an anode cylinder and a magnetic pole, which is a main part of one embodiment of the present invention. In the figure, 1 is a cathode,
2 is an anode cylinder, 3 is a vane, 4 is a conventional magnetic pole attached to the cathode stem side of the anode cylinder, 4a is a magnetic pole according to the present invention attached to the microwave output extraction side of the anode cylinder, and 5 is an antenna, Whereas the conventional magnetic pole 4 has a protrusion on the surface of the portion closest to the end face of the vane, the magnetic pole 4 according to the present invention.
The surface of the portion of a closest to the vane end surface is flat as shown. As a result, the magnetron of the present invention 2
The frequency spectrum of the fundamental wave of 450 MHz is as shown in FIG. 5, and in the case of the conventional magnetron, the spectrum of the fundamental wave is the width of the ISM band of 2450 MHz assigned to the microwave application device as shown in FIG. In contrast, in the magnetron of the present invention, side lobes and spurs of the oscillation frequency spectrum are significantly reduced. Therefore, when the magnetron of the present invention is used in a microwave application device such as a microwave oven, it is easy to take measures against noise radio wave leakage.
【0011】[0011]
【発明の効果】以上説明したように本発明によれば、製
作作業が容易で、しかも雑音電波の漏洩対策が容易な、
性能価格比の良好なマグネトロンが得られる。As described above, according to the present invention, the manufacturing work is easy, and the measures against the leakage of noise radio waves are easy.
A magnetron with a good performance price ratio can be obtained.
【図1】本発明一実施例の要部である陽極円筒や磁極を
含む部分の側断面図である。FIG. 1 is a side sectional view of a part including an anode cylinder and a magnetic pole, which is a main part of one embodiment of the present invention.
【図2】従来のマグネトロンの一例の管軸を通る平面に
よる断面図である。FIG. 2 is a sectional view taken along a plane passing through a tube axis of an example of a conventional magnetron.
【図3】図3(a)はベインのマイクロ波出力取出部側
端面のみに均圧環を設置し、ベインの先端に隣接ベイン
の先端側へ突出した張出し部分を設け、ベインの陰極ス
テム側端面に張出し部分と管軸から更に遠い部分との境
界に段差を設けて管軸から遠い部分のベインの幅を狭く
したマグネトロン陽極の平面図、図3(b)はその断面
図である。FIG. 3 (a) is a view showing that the pressure equalizing ring is installed only on the end surface of the vane on the side where the microwave output is taken out, and the end of the vane is provided with an overhanging portion protruding toward the end of the adjacent vane. FIG. 3 (b) is a plan view of the magnetron anode in which a step is provided at the boundary between the overhanging portion and the portion further away from the tube axis to narrow the width of the vane at the portion farther from the tube axis, and FIG.
【図4】従来のベインの片側端面だけに均圧環を設置し
たマグネトロンの2450MHz帯の基本波スペクトラ
ムを示す図である。FIG. 4 is a diagram showing a fundamental wave spectrum in a 2450 MHz band of a magnetron in which a pressure equalizing ring is installed only on one end surface of a conventional vane.
【図5】本発明実施例マグネトロンの2450MHz帯
の基本波スペクトラムを示す図である。FIG. 5 is a diagram showing a fundamental wave spectrum in a 2450 MHz band of a magnetron according to an embodiment of the present invention.
2…陽極円筒、 3…ベイン、 31…ベイン先端の張
出部分、 4…従来形の磁極、 4a…本発明に係る磁
極。2 ... Anode cylinder, 3 ... Vane, 31 ... Vane tip overhanging portion, 4 ... Conventional magnetic pole, 4a ... Magnetic pole according to the present invention.
Claims (1)
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空洞共振器群が囲み、作用
空間に管軸方向の静磁界を形成させるために、作用空間
の管軸方向端部近くに伸びた内周縁部、及び、陽極円筒
端部と環状永久磁石とに挾まれた外周縁部を夫々有する
2個の摺鉢状の磁極を設け、各ベインのマイクロ波出力
取出部側端面のみに管軸から等距離に溝を刻設して内部
にベインを1枚おきに交互に電気的に接続する内、外均
圧環を収納させ、各ベインの先端に両隣接ベインの先端
側へ対称に突出し隣接ベイン側と平行平面で対向する張
出し部分を設け、ベインの陰極ステム側端面に上記張出
し部分と管軸から更に遠い部分との境界に段差を設けて
管軸から遠い部分のベインの幅を狭くしたマグネトロン
において、マイクロ波出力取出部側ベイン端面に最も近
接する磁極の内周縁部の面を平坦にしたことを特徴とす
るマグネトロン。1. A cathode resonator arranged concentrically with a tube axis is surrounded by an anode cylinder and a cavity resonator group consisting of an even number of vanes radially projecting from an inner wall of the anode cylinder, with a cylindrical operating space being separated from each other. In order to form a static magnetic field in the tube axis direction, each has an inner peripheral edge portion extending near the end portion in the tube axial direction of the working space, and an outer peripheral edge portion sandwiched between the anode cylindrical end portion and the annular permanent magnet. Each pole is provided with a pole-shaped magnetic pole, and grooves are formed equidistantly from the tube axis only on the end surface of each vane on the microwave output extraction side to alternately electrically connect every other vane inside. , The outer pressure equalizing ring is housed, and a protruding portion is provided at the tip of each vane symmetrically projecting toward the tip side of both adjacent vanes and facing the adjacent vane side in a plane parallel to the vane. A portion further away from the pipe axis by providing a step on the boundary with the portion further away from In narrowed magnetron width of the vane, the magnetron, characterized in that the flat surface of the inner peripheral edge portion of the magnetic pole closest to the microwave output extraction portion side vane end face.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP16568992A JPH065211A (en) | 1992-06-24 | 1992-06-24 | Magnetron |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP16568992A JPH065211A (en) | 1992-06-24 | 1992-06-24 | Magnetron |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPH065211A true JPH065211A (en) | 1994-01-14 |
Family
ID=15817175
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP16568992A Pending JPH065211A (en) | 1992-06-24 | 1992-06-24 | Magnetron |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH065211A (en) |
Cited By (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US5635798A (en) * | 1993-12-24 | 1997-06-03 | Hitachi, Ltd. | Magnetron with reduced dark current |
| US6872929B2 (en) | 2003-04-17 | 2005-03-29 | The Regents Of The University Of Michigan | Low-noise, crossed-field devices such as a microwave magnetron, microwave oven utilizing same and method of converting a noisy magnetron to a low-noise magnetron |
| KR100863253B1 (en) * | 2002-12-06 | 2008-10-15 | 삼성전자주식회사 | Magnetron, Microwave and High Frequency Heater |
-
1992
- 1992-06-24 JP JP16568992A patent/JPH065211A/en active Pending
Cited By (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US5635798A (en) * | 1993-12-24 | 1997-06-03 | Hitachi, Ltd. | Magnetron with reduced dark current |
| KR100863253B1 (en) * | 2002-12-06 | 2008-10-15 | 삼성전자주식회사 | Magnetron, Microwave and High Frequency Heater |
| US6872929B2 (en) | 2003-04-17 | 2005-03-29 | The Regents Of The University Of Michigan | Low-noise, crossed-field devices such as a microwave magnetron, microwave oven utilizing same and method of converting a noisy magnetron to a low-noise magnetron |
| US6921890B2 (en) | 2003-04-17 | 2005-07-26 | The Regents Of The University Of Michigan | Low-noise, crossed-field devices such as a microwave magnetron having an azimuthally-varying axial magnetic field and microwave oven utilizing same |
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| EP0263491B1 (en) | Magnetron for microwave oven | |
| US5635798A (en) | Magnetron with reduced dark current | |
| KR20040008346A (en) | Magnetron | |
| US4891557A (en) | Magnetron device | |
| JP3193647B2 (en) | Magnetron | |
| US4074169A (en) | Magnetron with harmonic frequency output suppression | |
| JPH065211A (en) | Magnetron | |
| US3914644A (en) | Rotary tuner for circular electric mode crossed field tube | |
| US2447537A (en) | Coupled cavity resonator | |
| JP2557354B2 (en) | Magnetron for microwave oven | |
| EP1804269A2 (en) | Magnetron | |
| JP2582830Y2 (en) | Bottom shield fixing structure of magnetron cathode assembly | |
| KR100266604B1 (en) | Structure for preventing harmonic wave leakage in magnetron | |
| KR100351790B1 (en) | Structure and method of anode manufacturing for micro wave oven | |
| US20020008479A1 (en) | Double loop output system for magnetron | |
| JPH07230771A (en) | Magnetron | |
| JP3261726B2 (en) | Magnetron | |
| JP3448424B2 (en) | Magnetron | |
| US3290548A (en) | Reverse magnetron | |
| JPH0521014A (en) | Magnetron | |
| KR100451235B1 (en) | Input part sealing structure for magnetron | |
| KR200152107Y1 (en) | Magnetron bipolar vane structure | |
| GB2393570A (en) | Reducing unwanted emissions in a magnetron | |
| US2803773A (en) | High frequency diode magnetron | |
| JPH0652805A (en) | Magnetron |