JPH11283517A - Magnetron - Google Patents

Magnetron

Info

Publication number
JPH11283517A
JPH11283517A JP8362298A JP8362298A JPH11283517A JP H11283517 A JPH11283517 A JP H11283517A JP 8362298 A JP8362298 A JP 8362298A JP 8362298 A JP8362298 A JP 8362298A JP H11283517 A JPH11283517 A JP H11283517A
Authority
JP
Japan
Prior art keywords
anode cylinder
cathode
tube axis
vane
pole piece
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
Application number
JP8362298A
Other languages
Japanese (ja)
Inventor
Masayuki Aiga
正幸 相賀
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.)
Sanyo Electric Co Ltd
Original Assignee
Sanyo Electric Co Ltd
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Application filed by Sanyo Electric Co Ltd filed Critical Sanyo Electric Co Ltd
Priority to JP8362298A priority Critical patent/JPH11283517A/en
Publication of JPH11283517A publication Critical patent/JPH11283517A/en
Pending legal-status Critical Current

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Abstract

PROBLEM TO BE SOLVED: To suppress noise by forming asymmetrically with respect to a tube axis, a small diameter flat surface of at least one pole piece, arranged at each end of an anode cylinder, for guiding magnetic face into the acting space between a cathode and a vein. SOLUTION: A pole piece 21, arranged in an opening part at each end of an anode cylinder 1, has a large diameter flat part 22, a slanting part 23 projecting toward a vane 2 as approaching the center, and a small diameter flat part 24 in the central part of the slanting part 23. A circular through-hole 25 is formed in the eccentric position to the tube axis of the small diameter flat part 24. The eccentric positions of the through-holes 25 are arranged, so as to be about 180 degrees symmetric with respect to the tube axis in the pole pieces 21 on the upper side and the lower side. Magnetic field strength and the direction of a magnetic flux become asymmetric with respect to the tube axis, electron orbitaling motion on the end side in the tube axial direction of an acting space 5 becomes discontinuous, so that oscillation in this part is suppressed to prevent multiple oscillations, and only the main oscillation in the central part is generated.

Description

【発明の詳細な説明】DETAILED DESCRIPTION OF THE INVENTION

【0001】[0001]

【発明の属する技術分野】本発明は、電子レンジ等のマ
イクロ波加熱機器やレーダーなどに用いられるマグネト
ロンに関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a magnetron used for a microwave heating device such as a microwave oven, a radar, and the like.

【0002】[0002]

【従来の技術】従来の家庭用電子レンジなどに用いられ
るマグネトロンを図10に示す要部断面図に基づいて説
明すると、1は陽極筒体で、その内周面に放射状に配設
された複数枚のベイン2を有し、隣り合うベイン2と陽
極筒体1の内周壁とで囲まれる複数の共振空洞を形成し
ている。3は前記ベイン2を一つおきに連結するストラ
ップリングである。
2. Description of the Related Art A conventional magnetron used in a microwave oven for home use will be described with reference to a sectional view of a main part shown in FIG. 10. Reference numeral 1 denotes an anode cylinder, and a plurality of anode cylinders are arranged radially on the inner peripheral surface thereof. It has a plurality of vanes 2 and forms a plurality of resonance cavities surrounded by adjacent vanes 2 and the inner peripheral wall of the anode cylinder 1. Reference numeral 3 denotes a strap ring for connecting the vanes 2 alternately.

【0003】4は前記ベイン2で囲まれる空間に配設さ
れる陰極で、ベイン2との間に作用空間5が形成されて
いる。6は前記陰極4をリード端子7を介して支持固定
するステム構体、8は前記陽極筒体1の両開口端部に配
設されるポールピースで、大径平坦部9と、傾斜部10
と、傾斜部10の中央部に形成される小径平坦部11
と、小径平坦部11の中央部に形成される貫通穴12と
を有し、ベイン2と陰極4との間に印加される直流電圧
と併せて作用空間5に直交静電磁界を形成すべく、図示
しない磁石の磁力を作用空間5に導くようになってい
る。
Reference numeral 4 denotes a cathode disposed in a space surrounded by the vane 2, and a working space 5 is formed between the cathode 4 and the vane 2. Reference numeral 6 denotes a stem structure for supporting and fixing the cathode 4 via a lead terminal 7. Reference numeral 8 denotes a pole piece disposed at both open ends of the anode cylinder 1, a large-diameter flat portion 9 and an inclined portion 10.
And a small-diameter flat portion 11 formed at the center of the inclined portion 10.
And a through-hole 12 formed at the center of the small-diameter flat portion 11 so as to form an orthogonal electrostatic magnetic field in the working space 5 together with a DC voltage applied between the vane 2 and the cathode 4. The magnetic force of a magnet (not shown) is guided to the working space 5.

【0004】上記構成のマグネトロンにおいて、陰極4
から放射された電子は、直交静電磁界によって円周方向
に回転してベイン2に近づき、電子雲の形になって共振
空洞にエネルギー変換される。その結果、共振空洞内の
微弱マイクロ波が増幅され、ベイン2の1枚に電気的に
接続されたアンテナリード13から電子レンジ等の庫内
に放射される。
In the magnetron having the above structure, the cathode 4
The electrons radiated from are rotated in the circumferential direction by the orthogonal electrostatic magnetic field, approach the vane 2, and are converted into energy in the form of an electron cloud into a resonant cavity. As a result, the weak microwave in the resonance cavity is amplified and radiated from the antenna lead 13 electrically connected to one of the vanes 2 into a storage such as a microwave oven.

【0005】しかしながら、上述した構成のマグネトロ
ンにおいては、作用空間5での磁界強度がベイン2の軸
方向において不均一となっていた。即ち、ポールピース
6間の磁力線は、円弧を描いて一方のポールピース6か
ら他方のポールピース6に向かうため、磁力線は、ポー
ルピース6間の間隔の中心部では作用空間5からベイン
2側または陰極4側にそれる。そのため、作用空間5内
での磁界の強さをみると、図11に示すごとく、ベイン
2の軸方向端部側が中央部よりも約16%強い分布とな
っていた。
However, in the magnetron having the above-described configuration, the magnetic field intensity in the working space 5 is not uniform in the axial direction of the vane 2. That is, since the magnetic lines of force between the pole pieces 6 are drawn in an arc from one pole piece 6 to the other pole piece 6, the magnetic lines of force are located at the center of the interval between the pole pieces 6 from the action space 5 to the vane 2 side. Deviate to the cathode 4 side. As a result, the intensity of the magnetic field in the working space 5 was such that, as shown in FIG. 11, the distribution at the axial end of the vane 2 was about 16% stronger than that at the center.

【0006】この直交静電磁界中の電界強度Eと磁界強
度Bとの比E/Bの値により電子の回転速度が決まり、
磁界強度Bが管軸方向において不均一分布なため、電子
の回転速度も不均一となり、多重発振の原因となってい
る。この多重発振時の周波数偏差がマグネトロンの陰極
側端子から外部に漏洩する雑音となって、ラジオ、テレ
ビなどの受信に妨害を与えたり、多重発振の周波数その
ものが通信に妨害を与えるという問題がある。図12は
従来のマグネトロンの周波数特性を示しており、基本波
であるメインローブAの周辺に多重発振を示すサイドロ
ーブBが確認されている。
[0006] The value of the ratio E / B of the electric field strength E and the magnetic field strength B in the orthogonal electrostatic magnetic field determines the rotational speed of the electrons.
Since the magnetic field strength B is unevenly distributed in the tube axis direction, the rotational speed of the electrons is also uneven, which causes multiple oscillations. The frequency deviation at the time of the multiple oscillation becomes noise leaking from the cathode side terminal of the magnetron to the outside, and there is a problem that the reception of a radio or a television is disturbed, and the frequency of the multiple oscillation itself disturbs the communication. . FIG. 12 shows the frequency characteristics of a conventional magnetron, in which a side lobe B indicating multiple oscillation is confirmed around a main lobe A which is a fundamental wave.

【0007】[0007]

【発明が解決しようとする課題】本発明は、上記問題点
に鑑みなされたもので、低雑音のマグネトロンを提供す
ることを課題とする。
SUMMARY OF THE INVENTION The present invention has been made in view of the above problems, and has as its object to provide a low-noise magnetron.

【0008】[0008]

【課題を解決するための手段】本発明の第1の手段は、
陽極筒体と、該陽極筒体の管軸上に配置された陰極と、
前記陽極筒体の一端側に固着され陰極を支持固定するス
テム構体と、前記陽極筒体の内周面に放射状に配設され
る複数枚のベインと、前記ベインに接続されるアンテナ
リードと、前記陽極筒体の他端側に固着されアンテナリ
ードを囲繞する出力部と、前記陽極筒体の両端に配設さ
れ陰極とベインとの間の作用空間に磁力を導く小径平坦
面を有するポールピースとを備え、少なくとも一方のポ
ールピースの小径平坦面を、管軸に対して非対称形状に
形成したことを特徴とする。
A first means of the present invention is as follows.
An anode cylinder, and a cathode disposed on a tube axis of the anode cylinder,
A stem structure fixed to one end of the anode cylinder and supporting and fixing the cathode, a plurality of vanes radially arranged on an inner peripheral surface of the anode cylinder, and an antenna lead connected to the vane; An output portion fixed to the other end of the anode cylinder and surrounding the antenna lead, and a pole piece having a small-diameter flat surface disposed at both ends of the anode cylinder and guiding a magnetic force to a working space between the cathode and the vane. Wherein the small-diameter flat surface of at least one of the pole pieces is formed in an asymmetric shape with respect to the tube axis.

【0009】本発明の第2の手段は、陽極筒体と、該陽
極筒体の管軸上に配置された陰極と、前記陽極筒体の一
端側に固着され陰極を支持固定するステム構体と、前記
陽極筒体の内周面に放射状に配設される複数枚のベイン
と、前記ベインに接続されるアンテナリードと、前記陽
極筒体の他端側に固着されアンテナリードを囲繞する出
力部と、前記陽極筒体の両端に配設され陰極とベインと
の間の作用空間に磁力を導く小径平坦面を有する一対の
同形状のポールピースとを備え、前記ポールピースの小
径平坦面を管軸に対して非対称形状に形成すると共に、
一方のポールピースを、他方のポールピースに対し、管
軸に対して略180度回転させた位置に配置したことを
特徴とする。
A second means of the present invention comprises an anode cylinder, a cathode disposed on a tube axis of the anode cylinder, and a stem assembly fixed to one end of the anode cylinder for supporting and fixing the cathode. A plurality of vanes radially arranged on the inner peripheral surface of the anode cylinder, an antenna lead connected to the vane, and an output unit fixed to the other end of the anode cylinder and surrounding the antenna lead And a pair of pole pieces of the same shape having a small-diameter flat surface disposed at both ends of the anode cylinder and guiding a magnetic force to a working space between the cathode and the vane. While being formed asymmetrical with respect to the axis,
One pole piece is arranged at a position rotated by about 180 degrees with respect to the tube axis with respect to the other pole piece.

【0010】本発明の第3の手段は、陽極筒体と、該陽
極筒体の管軸上に配置された陰極と、前記陽極筒体の一
端側に固着され陰極を支持固定するステム構体と、前記
陽極筒体の内周面に放射状に配設される複数枚のベイン
と、前記ベインに接続されるアンテナリードと、前記陽
極筒体の他端側に固着されアンテナリードを囲繞する出
力部と、前記陰極とベインとの間の作用空間に磁力を導
くポールピースとを備え、前記ポールピースの略中心に
形成した貫通穴を、管軸に対して変位させて形成したこ
とを特徴とする。
A third means of the present invention comprises an anode cylinder, a cathode disposed on a tube axis of the anode cylinder, and a stem assembly fixed to one end of the anode cylinder for supporting and fixing the cathode. A plurality of vanes radially arranged on the inner peripheral surface of the anode cylinder, an antenna lead connected to the vane, and an output unit fixed to the other end of the anode cylinder and surrounding the antenna lead And a pole piece for guiding a magnetic force to the working space between the cathode and the vane, wherein a through hole formed substantially at the center of the pole piece is formed by being displaced with respect to a tube axis. .

【0011】本発明の第4の手段は、陽極筒体と、該陽
極筒体の管軸上に配置された陰極と、前記陽極筒体の一
端側に固着され陰極を支持固定するステム構体と、前記
陽極筒体の内周面に放射状に配設される複数枚のベイン
と、前記ベインに接続されるアンテナリードと、前記陽
極筒体の多端側に固着されアンテナリードを囲繞する出
力部と、前記陽極筒体の両端に配設され陰極とベインと
の間の作用空間に磁力を導く一対のポールピースとを備
え、前記ポールピースの略中心に形成した貫通穴を、管
軸に対して互いに逆方向に変位させたことを特徴とす
る。
According to a fourth aspect of the present invention, there is provided an anode cylinder, a cathode disposed on a tube axis of the anode cylinder, and a stem structure fixed to one end of the anode cylinder for supporting and fixing the cathode. A plurality of vanes radially arranged on the inner peripheral surface of the anode cylinder, an antenna lead connected to the vane, and an output unit fixed to a multi-end side of the anode cylinder and surrounding the antenna lead. A pair of pole pieces that are disposed at both ends of the anode cylinder and guide magnetic force to the working space between the cathode and the vane, and a through hole formed substantially at the center of the pole piece is formed with respect to the tube axis. It is characterized by being displaced in opposite directions.

【0012】[0012]

【実施の形態】本発明の実施の形態を図1乃至図5に基
づいて以下に詳述する。尚、上述した従来の技術と同一
部品は同一符号を付して説明を省略する。
DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS An embodiment of the present invention will be described below in detail with reference to FIGS. The same components as those in the above-described conventional technology are denoted by the same reference numerals, and description thereof will be omitted.

【0013】21は陽極筒体1の両端開口部に配設され
るポールピースで、大径平坦部22と、中心になるに従
ってベイン2に向かって突出する傾斜部23と、傾斜部
23の中央部に形成される小径平坦部24を有してお
り、小径平坦部24には、管軸に対して偏心した位置に
円形の貫通穴25が形成されている。前記ポールピース
21は貫通穴25の偏心した位置が管軸に対して約18
0度対称となるように陽極筒体1の両端開口部に配設さ
れる。
Reference numeral 21 denotes a pole piece disposed at the opening at both ends of the anode cylinder 1, a large-diameter flat portion 22, an inclined portion 23 protruding toward the vane 2 toward the center, and a center of the inclined portion 23. The small-diameter flat portion 24 is formed with a circular through hole 25 at a position eccentric with respect to the tube axis. The eccentric position of the through hole 25 is about 18
The anode cylinder 1 is disposed at both ends of the opening so as to be symmetric with respect to 0 degrees.

【0014】図4に本実施の形態を用いたマグネトロン
のベイン端面における管軸方向磁界強度差を示す。尚、
同実験に用いたマグネトロンは、材厚1.6mmのポールピ
ース21を用い、貫通穴25の直径を9.2mm、管軸に対
する貫通穴25の偏心量aを0.3mm、ベイン2の内接円
の直径Dを9.0mm、陰極4外径dを4.0mm、ベイン2高さ
hを9.0mmとしている。
FIG. 4 shows the difference in magnetic field strength in the tube axis direction at the vane end face of the magnetron using this embodiment. still,
The magnetron used in the experiment uses a pole piece 21 having a material thickness of 1.6 mm, the diameter of the through hole 25 is 9.2 mm, the eccentricity a of the through hole 25 with respect to the pipe axis is 0.3 mm, and the diameter of the inscribed circle of the vane 2 D is 9.0 mm, the outer diameter d of the cathode 4 is 4.0 mm, and the height h of the vane 2 is 9.0 mm.

【0015】図4に示されるとおり、本実施の形態を用
いたマグネトロンは、図11に示す従来のマグネトロン
と同様に、作用空間の管軸方向端部側の磁界強度が中央
部よりも約16%強い分布となっている。しかしなが
ら、従来のマグネトロンにおいては、作用空間5の管軸
方向端部側での磁界強度及び磁束の向きが管軸に対して
全周が軸対称となるのに対し、本実施の形態を用いたマ
グネトロンは、磁界強度及び磁束の向きが管軸に対して
非対称となることから、作用空間5の管軸方向端部側で
の電子周回運動も非連続となり、この部分での発振が抑
制されて多重発振が防止される。
As shown in FIG. 4, in the magnetron using this embodiment, the magnetic field strength at the end of the working space in the tube axis direction is about 16 times higher than that at the center, like the conventional magnetron shown in FIG. % Distribution is strong. However, in the conventional magnetron, the magnetic field strength and the direction of the magnetic flux at the end of the working space 5 in the tube axis direction are all axially symmetric with respect to the tube axis. In the magnetron, since the magnetic field strength and the direction of the magnetic flux are asymmetric with respect to the tube axis, the electron circulating motion at the end portion of the working space 5 in the tube axis direction also becomes discontinuous, and oscillation in this portion is suppressed. Multiple oscillations are prevented.

【0016】即ち、本発明のマグネトロンは、作用空間
5の管軸方向端部側での電子周回運動を抑制し、作用空
間5の中央部での主発振のみ発生させるようにすること
で多重発振を防止するものである。
That is, the magnetron of the present invention suppresses the electron orbital movement at the end of the working space 5 in the tube axis direction and generates only the main oscillation at the central portion of the working space 5 so that the multiple oscillation is achieved. It is to prevent.

【0017】上述した本実施の形態を用いたマグネトロ
ンの基本波周辺の周波数特性を図5に示す。図12に示
した従来のマグネトロンの周波数特性と比較し、多重発
振に起因したメインローブA周辺のサイドローブが抑制
されていることがわかる。
FIG. 5 shows the frequency characteristics around the fundamental wave of the magnetron using the above-described embodiment. Compared with the frequency characteristics of the conventional magnetron shown in FIG. 12, it can be seen that side lobes around the main lobe A due to multiple oscillation are suppressed.

【0018】尚、上述した実施の形態では、円形の貫通
穴25を中心線に対し偏心させる構成としたが、図6及
び図7に示す如く貫通穴25を楕円形状に形成してもよ
く、図8及び図9に示す如く小径平坦部24を管軸に対
して偏心させる構成としてもよい。
In the above-described embodiment, the circular through hole 25 is configured to be eccentric with respect to the center line. However, as shown in FIGS. 6 and 7, the through hole 25 may be formed in an elliptical shape. As shown in FIGS. 8 and 9, the small diameter flat portion 24 may be configured to be eccentric with respect to the tube axis.

【0019】また、両方のポールピース21の貫通穴2
5を偏心させる構成としたが、一方のポールピース21
の貫通穴25のみを偏心させてもよい。さらに、ポール
ピース21の貫通穴25縁の一部に面取りを施す構成、
あるいは貫通穴25縁の肉厚を変化させる構成としても
よく、要は、作用空間5の管軸方向端部の磁界の傾きに
変化を与えうる構成であればよいものである。
The through holes 2 of both pole pieces 21
5 is eccentric, but one pole piece 21
Only the through hole 25 may be eccentric. Furthermore, a configuration in which a part of the edge of the through hole 25 of the pole piece 21 is chamfered,
Alternatively, the configuration may be such that the thickness of the edge of the through hole 25 is changed. In short, any configuration may be used as long as it can change the gradient of the magnetic field at the end of the working space 5 in the tube axis direction.

【0020】[0020]

【発明の効果】本発明の構成によれば、簡単な構成で、
多重発振を軽減することができ、雑音の発生を低減する
ことができる等の効果を奏する。
According to the structure of the present invention, with a simple structure,
It is possible to reduce multiplex oscillation and to reduce noise generation.

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

【図1】本発明の実施の形態を示す断面図である。FIG. 1 is a sectional view showing an embodiment of the present invention.

【図2】同ポールピースの断面図である。FIG. 2 is a sectional view of the pole piece.

【図3】同ポールピースの平面図である。FIG. 3 is a plan view of the pole piece.

【図4】同磁界強度分布を示す図である。FIG. 4 is a diagram showing the same magnetic field intensity distribution.

【図5】同周波数波形を示す図である。FIG. 5 is a diagram showing the same frequency waveform.

【図6】同他の実施の形態を示すポールピースの断面図
である。
FIG. 6 is a sectional view of a pole piece according to another embodiment.

【図7】同ポールピースの平面図である。FIG. 7 is a plan view of the pole piece.

【図8】同他の実施の形態を示すポールピースの断面図
である。
FIG. 8 is a sectional view of a pole piece according to another embodiment.

【図9】同ポールピースの平面図である。FIG. 9 is a plan view of the pole piece.

【図10】従来のマグネトロンを示す断面図である。FIG. 10 is a sectional view showing a conventional magnetron.

【図11】同磁界強度分布を示す図である。FIG. 11 is a diagram showing the same magnetic field intensity distribution.

【図12】同周波数波形を示す図である。FIG. 12 is a diagram showing the same frequency waveform.

【符号の説明】[Explanation of symbols]

1 陽極筒体 2 ベイン 4 陰極 5 作用空間 21 ポールピース 24 小径平坦部 25 貫通穴 DESCRIPTION OF SYMBOLS 1 Anode cylinder 2 Bain 4 Cathode 5 Working space 21 Pole piece 24 Small diameter flat part 25 Through hole

Claims (4)

【特許請求の範囲】[Claims] 【請求項1】 陽極筒体と、該陽極筒体の管軸上に配置
された陰極と、前記陽極筒体の一端側に固着され陰極を
支持固定するステム構体と、前記陽極筒体の内周面に放
射状に配設される複数枚のベインと、前記ベインに接続
されるアンテナリードと、前記陽極筒体の他端側に固着
されアンテナリードを囲繞する出力部と、前記陽極筒体
の両端に配設され陰極とベインとの間の作用空間に磁力
を導く小径平坦面を有するポールピースとを備え、少な
くとも一方のポールピースの小径平坦面を、管軸に対し
て非対称形状に形成したことを特徴とするマグネトロ
ン。
1. An anode cylinder, a cathode disposed on a tube axis of the anode cylinder, a stem assembly fixed to one end of the anode cylinder to support and fix the cathode, and A plurality of vanes radially arranged on the peripheral surface, an antenna lead connected to the vane, an output portion fixed to the other end of the anode cylinder and surrounding the antenna lead, A pole piece disposed at both ends and having a small-diameter flat surface that guides magnetic force to the working space between the cathode and the vane, wherein the small-diameter flat surface of at least one of the pole pieces is formed asymmetrically with respect to the tube axis. A magnetron, characterized in that:
【請求項2】 陽極筒体と、該陽極筒体の管軸上に配置
された陰極と、前記陽極筒体の一端側に固着され陰極を
支持固定するステム構体と、前記陽極筒体の内周面に放
射状に配設される複数枚のベインと、前記ベインに接続
されるアンテナリードと、前記陽極筒体の他端側に固着
されアンテナリードを囲繞する出力部と、前記陽極筒体
の両端に配設され陰極とベインとの間の作用空間に磁力
を導く小径平坦面を有する一対の同形状のポールピース
とを備え、前記ポールピースの小径平坦面を管軸に対し
て非対称形状に形成すると共に、一方のポールピース
を、他方のポールピースに対し、管軸に対して略180
度回転させた位置に配置したことを特徴とするマグネト
ロン。
2. An anode cylinder, a cathode disposed on a tube axis of the anode cylinder, a stem assembly fixed to one end of the anode cylinder to support and fix the cathode, and A plurality of vanes radially arranged on the peripheral surface, an antenna lead connected to the vane, an output portion fixed to the other end of the anode cylinder and surrounding the antenna lead, A pair of pole pieces of the same shape having a small-diameter flat surface that is disposed at both ends and guides magnetic force to the working space between the cathode and the vane, wherein the small-diameter flat surface of the pole piece is asymmetric with respect to the tube axis. And forming one pole piece relative to the other pole piece at approximately 180
A magnetron characterized by being disposed at a position rotated by degrees.
【請求項3】 陽極筒体と、該陽極筒体の管軸上に配置
された陰極と、前記陽極筒体の一端側に固着され陰極を
支持固定するステム構体と、前記陽極筒体の内周面に放
射状に配設される複数枚のベインと、前記ベインに接続
されるアンテナリードと、前記陽極筒体の他端側に固着
されアンテナリードを囲繞する出力部と、前記陰極とベ
インとの間の作用空間に磁力を導くポールピースとを備
え、前記ポールピースの略中心に形成した貫通穴を、管
軸に対して変位させて形成したことを特徴とするマグネ
トロン。
3. An anode cylinder, a cathode disposed on a tube axis of the anode cylinder, a stem assembly fixed to one end of the anode cylinder to support and fix the cathode, and A plurality of vanes radially arranged on the peripheral surface, an antenna lead connected to the vane, an output unit fixed to the other end of the anode cylinder and surrounding the antenna lead, the cathode and the vane And a pole piece for guiding a magnetic force to a working space between the pole pieces, wherein a through hole formed substantially at the center of the pole piece is formed displaced with respect to a tube axis.
【請求項4】 陽極筒体と、該陽極筒体の管軸上に配置
された陰極と、前記陽極筒体の一端側に固着され陰極を
支持固定するステム構体と、前記陽極筒体の内周面に放
射状に配設される複数枚のベインと、前記ベインに接続
されるアンテナリードと、前記陽極筒体の多端側に固着
されアンテナリードを囲繞する出力部と、前記陽極筒体
の両端に配設され陰極とベインとの間の作用空間に磁力
を導く一対のポールピースとを備え、前記ポールピース
の略中心に形成した貫通穴を、管軸に対して互いに逆方
向に変位させたことを特徴とするマグネトロン。
4. An anode cylinder, a cathode disposed on a tube axis of the anode cylinder, a stem assembly fixed to one end of the anode cylinder to support and fix the cathode, and A plurality of vanes radially arranged on a peripheral surface, an antenna lead connected to the vane, an output portion fixed to a multi-end side of the anode cylinder and surrounding the antenna lead, and both ends of the anode cylinder And a pair of pole pieces for guiding a magnetic force to the working space between the cathode and the vane, and the through holes formed substantially in the center of the pole pieces are displaced in directions opposite to each other with respect to the tube axis. A magnetron, characterized in that:
JP8362298A 1998-03-30 1998-03-30 Magnetron Pending JPH11283517A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP8362298A JPH11283517A (en) 1998-03-30 1998-03-30 Magnetron

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP8362298A JPH11283517A (en) 1998-03-30 1998-03-30 Magnetron

Publications (1)

Publication Number Publication Date
JPH11283517A true JPH11283517A (en) 1999-10-15

Family

ID=13807592

Family Applications (1)

Application Number Title Priority Date Filing Date
JP8362298A Pending JPH11283517A (en) 1998-03-30 1998-03-30 Magnetron

Country Status (1)

Country Link
JP (1) JPH11283517A (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
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
KR100485725B1 (en) * 2001-08-22 2005-04-27 마쯔시다덴기산교 가부시키가이샤 Magnetron
US6921889B2 (en) * 2002-12-06 2005-07-26 Samsung Electronics Co., Ltd. Magnetron and microwave oven and high frequency heating apparatus each equipped with the same

Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
KR100485725B1 (en) * 2001-08-22 2005-04-27 마쯔시다덴기산교 가부시키가이샤 Magnetron
US6921889B2 (en) * 2002-12-06 2005-07-26 Samsung Electronics Co., Ltd. Magnetron and microwave oven and high frequency heating apparatus each equipped with the same
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
WO2004100353A3 (en) * 2003-04-17 2005-07-14 Univ 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

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