JPH01307147A - Magnetron - Google Patents

Magnetron

Info

Publication number
JPH01307147A
JPH01307147A JP13653188A JP13653188A JPH01307147A JP H01307147 A JPH01307147 A JP H01307147A JP 13653188 A JP13653188 A JP 13653188A JP 13653188 A JP13653188 A JP 13653188A JP H01307147 A JPH01307147 A JP H01307147A
Authority
JP
Japan
Prior art keywords
anode body
vanes
magnetron
anode
cavity resonator
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
JP13653188A
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 JP13653188A priority Critical patent/JPH01307147A/en
Publication of JPH01307147A publication Critical patent/JPH01307147A/en
Pending legal-status Critical Current

Links

Abstract

PURPOSE:To prevent the characteristic of a magnetron from varying even though its anode structure is made in small size, by forming unevenness on the surface of a resonance cavity. CONSTITUTION:A cylindrical anode body 11 has radially oriented vanes 12 installed at the bore, and this anode body 11 and vanes 12 are formed by press from a blank of oxygen free copper through a hobbing process in such a way as consolidated. Undulate surfaces are provided on the bore of the anode body 11 and at the sides of vanes 12 so that the creeping length of a unitary cavity resonator 13 will be a length necessary to oscillate high frequency electric waves of fundamental frequency. This permits making the anode structure in small size without varying its characteristics to lead to accomplishment of a small-sized magnetron.

Description

【発明の詳細な説明】 a)産業上の利用分野 本発明はマグネトロンに係わり、特にその陽極構体の改
良に関する。
DETAILED DESCRIPTION OF THE INVENTION a) Field of Industrial Application The present invention relates to magnetrons, and more particularly to improvements in the anode structure thereof.

―) 従来の技術 一般にマグネトロンの陽極構体は第5図及び第6図に示
すように構成されている。;1)は筒状陽極体で、内周
面には陽極体(1)の中心軸に向って複数のベイン(2
)を放射状に配設しており、隣り合った2枚のベイン(
2)と陽極体(1)内周面とで囲まれた空間で空胴共振
器(3)を形成している。(4)(51は各ベイン(2
1の上下に夫々一つおきに連結された大小のストラップ
リングである。
--) Prior Art Generally, the anode structure of a magnetron is constructed as shown in FIGS. 5 and 6. ;1) is a cylindrical anode body, and the inner peripheral surface has a plurality of vanes (2) toward the central axis of the anode body (1).
) are arranged radially, and two adjacent vanes (
A cavity resonator (3) is formed in a space surrounded by the anode body (1) and the inner peripheral surface of the anode body (1). (4) (51 is each vane (2
These are large and small strap rings that are connected every other time to the top and bottom of 1.

マグネトロンを小型化するため、陽極構体を小径化する
ことが考えられるが、陽極体Il+の径を小さくすると
、単位空胴共振器(3)の沿面長lが短縮さnるため、
空胴共振−a(31のインダクタンスLが減少し、 2
450M)1gの基本周波数の高周波電波が得られなく
なる欠点があった。
In order to downsize the magnetron, it is conceivable to reduce the diameter of the anode structure, but if the diameter of the anode body Il+ is reduced, the creepage length l of the unit cavity resonator (3) will be shortened n.
Cavity resonance-a (inductance L of 31 decreases, 2
450M) had the disadvantage that high frequency radio waves with a fundamental frequency of 1g could not be obtained.

fl  発明が解決しようとする課題 本発明は上記欠点に鑑みなされたもので、陽極構体を小
型化しても特性が変化することのないマグネトロンを提
供することを課題とする。
fl Problems to be Solved by the Invention The present invention has been made in view of the above-mentioned drawbacks, and an object thereof is to provide a magnetron whose characteristics do not change even if the anode structure is downsized.

に)課題を解決するための手段 上記課題を解決するため、共振空胴器の表面を凹凸状に
形成する。
B) Means for solving the problem In order to solve the above problem, the surface of the resonant cavity is formed into an uneven shape.

(ホ)作 用 上述の如く構成したから、空胴共振器の沿面長を変える
ことなく、陽極体の内径及びベインの長さを小さくする
ことができる。
(E) Function Since the structure is configured as described above, the inner diameter of the anode body and the length of the vane can be reduced without changing the creeping length of the cavity resonator.

(へ)実施例 本発明の一実施例を第1図及び第2図に基づき以下に詳
述する(尚、従来と同一部品は同一符号を附して説明も
省略する)。
(F) Embodiment An embodiment of the present invention will be described in detail below with reference to FIGS. 1 and 2 (components that are the same as those in the prior art are given the same reference numerals and explanations will be omitted).

Uは筒状陽極体、ttaは前記陽極体αBの内周に陽極
体lIDの中心軸に向って放射状に複数設けられたベイ
ンで、陽極体ttU及びペインσ2は無酸素銅のブラン
クからホピンク゛加工によシ一体にプレス成形される。
U is a cylindrical anode body, tta is a plurality of vanes provided on the inner periphery of the anode body αB radially toward the central axis of the anode body lID, and the anode body ttU and the pane σ2 are made of a blank of oxygen-free copper by hopper processing. Press-molded into one piece.

前記陽極体ttUの内周面及びベインt121の側面は
波状の凹凸面に形成され、単位空胴共振器1131の沿
面長lが基本周波数2450MHzの高周波電波を発振
するのに必要な長さになるように形成されている。
The inner circumferential surface of the anode body ttU and the side surface of the vane t121 are formed into wave-like uneven surfaces, and the creepage length l of the unit cavity resonator 1131 is the length necessary to oscillate high-frequency radio waves with a fundamental frequency of 2450 MHz. It is formed like this.

即ち、空胴共振器+131をLC等価回路で考えると、
マイクロ波゛ぼ流iは表皮効果によシ空胴共振器の表面
を流れるため、空胴共振器の沿面長lがL分に、ペイン
1z相互間、ストラップリング+41(51間及びベイ
ン(2)とストラップリングf41(51間が0分に相
当する。基本周波数2450MHzの高周波電波を発振
する為には所定のL分と0分が必要であシ、従って、所
定の空胴共振器(13の沿面長lが必要となる。
That is, if cavity resonator +131 is considered as an LC equivalent circuit,
Since the microwave current i flows on the surface of the cavity resonator due to the skin effect, the creepage length l of the cavity resonator is L. ) and strap ring f41 (51 corresponds to 0 minutes. In order to oscillate high-frequency radio waves with a fundamental frequency of 2450 MHz, a predetermined L minute and 0 minutes are required. Therefore, a predetermined cavity resonator (13 A creepage length l is required.

本発明に依れば、陽極体αBの内周面及びペインu21
の側面を凹凸状に形成しているので、空胴共振器t13
1の沿面長lを所定の長さにすると、第5図及び第6図
に示した従来に比べ、陽極体aυの内径及びベイン11
21の長さが小さくなる。
According to the present invention, the inner peripheral surface of the anode body αB and the pane u21
Since the side surface of the cavity resonator t13 is formed into an uneven shape, the cavity resonator t13
When the creepage length l of 1 is set to a predetermined length, the inner diameter of the anode body aυ and the vane 11 are
21 becomes smaller.

尚、第6図に示す如く、陽極体aυ内周面のみを凹凸状
に形成してもよく、第4図に示す如く、ペイン(12+
側面のみを凹凸状に形成してもよい。
Incidentally, as shown in FIG. 6, only the inner peripheral surface of the anode body aυ may be formed into an uneven shape, and as shown in FIG.
Only the side surfaces may be formed into an uneven shape.

(ト)発明の効果 以上の如く本発明に依れば、陽極構体を小型化でき、マ
グネトロンを小型化することができる。
(G) Effects of the Invention As described above, according to the present invention, the anode structure can be downsized, and the magnetron can be downsized.

【図面の簡単な説明】[Brief explanation of the drawing]

第1図は本発明の一実施例の要部斜視図、第2図は同平
面図、第6図は他の実施例の平面図、第4図は更に他の
実施例の平面図、第5図は従来例の平面図、第6図は同
要部拡大図である。 ull・・・筒状陽極体、 α2・・・ペイン、(13
・・・空胴共振器。
FIG. 1 is a perspective view of essential parts of one embodiment of the present invention, FIG. 2 is a plan view of the same, FIG. 6 is a plan view of another embodiment, and FIG. 4 is a plan view of still another embodiment. FIG. 5 is a plan view of the conventional example, and FIG. 6 is an enlarged view of the main part. ul...Cylindrical anode body, α2...Pain, (13
...Cavity resonator.

Claims (1)

【特許請求の範囲】[Claims] (1)筒状陽極体の内周面に、前記陽極体の中心軸に向
って複数のベインを突設せしめ、空胴共振器を形成する
マグネトロンにおいて、前記空胴共振器の表面を凹凸状
に形成してなるマグネトロン。
(1) In a magnetron in which a plurality of vanes are provided on the inner circumferential surface of a cylindrical anode body protruding toward the central axis of the anode body to form a cavity resonator, the surface of the cavity resonator is made uneven. A magnetron formed by
JP13653188A 1988-06-02 1988-06-02 Magnetron Pending JPH01307147A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP13653188A JPH01307147A (en) 1988-06-02 1988-06-02 Magnetron

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP13653188A JPH01307147A (en) 1988-06-02 1988-06-02 Magnetron

Publications (1)

Publication Number Publication Date
JPH01307147A true JPH01307147A (en) 1989-12-12

Family

ID=15177366

Family Applications (1)

Application Number Title Priority Date Filing Date
JP13653188A Pending JPH01307147A (en) 1988-06-02 1988-06-02 Magnetron

Country Status (1)

Country Link
JP (1) JPH01307147A (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP1316984A2 (en) * 2001-11-09 2003-06-04 Matsushita Electric Industrial Co., Ltd. Magnetron apparatus
KR20040009855A (en) * 2002-07-26 2004-01-31 삼성전자주식회사 Vane of magnetron
JP2009146663A (en) * 2007-12-12 2009-07-02 Panasonic Corp Magnetron, and method of manufacturing magnetron anode vane

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP1316984A2 (en) * 2001-11-09 2003-06-04 Matsushita Electric Industrial Co., Ltd. Magnetron apparatus
EP1316984A3 (en) * 2001-11-09 2004-03-03 Matsushita Electric Industrial Co., Ltd. Magnetron apparatus
KR20040009855A (en) * 2002-07-26 2004-01-31 삼성전자주식회사 Vane of magnetron
JP2009146663A (en) * 2007-12-12 2009-07-02 Panasonic Corp Magnetron, and method of manufacturing magnetron anode vane

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