JPH03238736A - Magnetron - Google Patents

Magnetron

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Publication number
JPH03238736A
JPH03238736A JP2035217A JP3521790A JPH03238736A JP H03238736 A JPH03238736 A JP H03238736A JP 2035217 A JP2035217 A JP 2035217A JP 3521790 A JP3521790 A JP 3521790A JP H03238736 A JPH03238736 A JP H03238736A
Authority
JP
Japan
Prior art keywords
output side
insulating cylinder
metal container
choke structure
higher harmonics
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
JP2035217A
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 JP2035217A priority Critical patent/JPH03238736A/en
Priority to US07/653,429 priority patent/US5180946A/en
Priority to GB9103033A priority patent/GB2243018B/en
Priority to KR1019910002408A priority patent/KR940006302B1/en
Publication of JPH03238736A publication Critical patent/JPH03238736A/en
Pending legal-status Critical Current

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Abstract

PURPOSE:To obtain sufficient effect of suppressing higher harmonics of short wavelength easily and surely be setting a higher harmonics suppressing choke structure electrically connected with a cylindrical metal container between an insulating cylinder in the output side and an antenna conductor. CONSTITUTION:To add higher harmonics suppressing choke, a choke structure 13 having circular grooves with a depth of 1/4 wavelength of any higher harmonics is set toward the inside space of an insulating cylinder 8 in the output side while its end part to be connected air-tightly with the insulating cylinder 8 in the output side of the metal container 7 being electrically connected. The insulating cylinder 8 having length (l) in the output side is thus covered with a metallic choke structure 13 to the extent of over 1/2 of the length (l), so that the length (l) of the insulating cylinder 8 in the output side which is regard as a space for high frequency is shortened to (l). As a result, sufficient effect of suppressing higher harmonics of short wavelength is obtained simply and surely.

Description

【発明の詳細な説明】 (イ)産業上の利用分野 本発明は、電子レンジなどに用いられるマグネトロンに
関する。
DETAILED DESCRIPTION OF THE INVENTION (a) Field of Industrial Application The present invention relates to a magnetron used in microwave ovens and the like.

(ロ) 従来の技術 一般に家庭用電子レンジに用いられるマグネトロンの基
本発振周波数は、国際電気通信連合(ITU)によって
2450±50MHzの範囲に決められているが、実際
のマグネトロンから発振されるマイクロ波には、第2、
第3高調波等多くの高調波が含まれ、更に基本波におい
ても上記範囲から外れた成分が含まれている。この高調
波は、例えば、電子レンジのキャビティ内に伝播される
と、この高調波の波長が短くなるほどシールドが困難と
なり、外部に漏洩しやすい。この漏洩電波はかなり微弱
であっても、電波障害をひき起こす場合がある。特に最
近は、第5高調波に相当する不要輻射が、SHF帯衛星
放送の12GHz帯と重なるため、問題視されている。
(b) Conventional technology The basic oscillation frequency of magnetrons generally used in household microwave ovens is determined by the International Telecommunication Union (ITU) to be in the range of 2450±50MHz. The second,
Many harmonics such as the third harmonic are included, and the fundamental wave also includes components outside the above range. For example, when this harmonic wave is propagated into the cavity of a microwave oven, the shorter the wavelength of this harmonic wave, the more difficult it is to shield it, and the more likely it is to leak to the outside. Even if these leaked radio waves are quite weak, they may cause radio interference. Particularly recently, unnecessary radiation corresponding to the fifth harmonic has been viewed as a problem because it overlaps with the 12 GHz band of SHF band satellite broadcasting.

ところで、従来からマグネトロン自身の不要輻射抑制技
術として、出力部にに波長形チョークを設けていること
はすでに知られている。例えば、特公昭54−6862
号公報、特開昭61−288347号公報などに開示さ
れている。このようなマグネトロンは、およそ第5図に
示すような構造である。同図で(7)は金属容器、(8
)は出力側絶縁筒、(9)はアンテナ導体である。そし
てアンテナ導体(9)をとり囲んで、金属容器(7〉内
に設けられたチョーク構体(12)の溝の深さdを高調
波波長の約%に設定して、その高調波に対するチョーク
構造としたものである。また、深さdを可変させること
により、任意の高調波を抑制することもできる。
Incidentally, it is already known that a wavelength choke is provided at the output section of the magnetron itself as a technique for suppressing unnecessary radiation. For example, Tokuko Sho 54-6862
This method is disclosed in Japanese Patent Application Laid-Open No. 61-288347, etc. Such a magnetron has a structure approximately as shown in FIG. In the figure, (7) is a metal container, (8
) is the output side insulating tube, and (9) is the antenna conductor. Then, the depth d of the groove of the choke structure (12) provided in the metal container (7) surrounding the antenna conductor (9) is set to approximately % of the harmonic wavelength, and the choke structure for the harmonics is constructed. Further, by varying the depth d, arbitrary harmonics can be suppressed.

しかし、かかる従来技術は、第2、第3高調波などの比
較的長波長の高調波抑制には効果を発揮するが、SHF
衛星放送の周波数帯である12GH2とほぼ一致するこ
とで問題となっている、電子レンジの第5高調波などの
ように短波長の高調波抑制には、充分な効果を得ること
ができない。その理由は、第5図に示す出力側絶縁筒の
長さlが、その高周波絶縁性から一般゛に約10mm程
度必要であるため、短波長の高調波にとっては、空間と
見なされ外部に放射されるためであると推定される。
However, although this conventional technology is effective in suppressing relatively long wavelength harmonics such as second and third harmonics, SHF
A sufficient effect cannot be obtained in suppressing harmonics of short wavelengths, such as the fifth harmonic of microwave ovens, which is a problem because it almost coincides with 12GH2, which is the frequency band of satellite broadcasting. The reason for this is that the length l of the output side insulating cylinder shown in Figure 5 is generally required to be about 10 mm due to its high frequency insulation properties, so for short wavelength harmonics, it is considered as space and radiated to the outside. It is presumed that this is because the

(ハ)発明が解決しようとする課題 そこで、本発明は、短波長の高調波抑制にも充分な効果
が、簡単、かつ、確実に得られるチョーク構体をもつマ
グネトロンを提供することを課題とする。
(c) Problems to be Solved by the Invention Therefore, an object of the present invention is to provide a magnetron having a choke structure that can easily and reliably obtain a sufficient effect to suppress harmonics of short wavelengths. .

(ニ)課題を解決するための手段 本発明は、出力側絶縁筒とアンテナ導体の間に、筒状金
属容器と電気的に結合された高調波抑制チョーク構体を
配したことを特徴とする。
(d) Means for Solving the Problems The present invention is characterized in that a harmonic suppression choke structure electrically coupled to the cylindrical metal container is disposed between the output-side insulating cylinder and the antenna conductor.

(ホ)作 用 本発明によれば、従来空間と見なされていた絶縁筒の内
側空間に、高調波抑制チョークを設けるため、空間と見
なされていた出力側絶縁筒の長さlが短縮されることか
ら、この部分よりの漏洩を抑制でき、チョーク効果を向
上させることができる。
(E) Function According to the present invention, since the harmonic suppression choke is provided in the inner space of the insulating cylinder, which was conventionally considered as a space, the length l of the output side insulating cylinder, which was considered as a space, is shortened. Therefore, leakage from this part can be suppressed and the choke effect can be improved.

(へ)実施例 第1図は本発明実施例のマグネトロンを示す。(f) Example FIG. 1 shows a magnetron according to an embodiment of the present invention.

(1)は筒状陽極体、(5)は該筒状陽極体の中心軸に
設置された陰極構体、(2)は筒状陽極体(1)の内面
に固着され、陰極(5)の囲りに放射状に配列された複
数の陽極ベイン、(6)は筒状陽極体(1)の一方の開
放端に固着されたポールピースである。(7)は筒状金
属容器、(8)は出力側絶縁筒、(10)は排気管で、
順次積み上げ固着され、筒状陽極体(1)内に連通ずる
気密空間を形成する。(9)は陽極ベイン(2)に一端
が固定され、気密空間内を延在した後、他端が排気管(
10)に固着指示されたアンテナ導体、(11)は排気
管(10)に被冠されたアンテナキャップである。
(1) is a cylindrical anode body, (5) is a cathode structure installed on the central axis of the cylindrical anode body, and (2) is fixed to the inner surface of the cylindrical anode body (1), and is attached to the cathode (5). A plurality of anode vanes (6) are arranged radially around the anode body, and a pole piece (6) is fixed to one open end of the cylindrical anode body (1). (7) is a cylindrical metal container, (8) is an output side insulating cylinder, (10) is an exhaust pipe,
They are sequentially stacked and fixed to form an airtight space communicating within the cylindrical anode body (1). (9) is fixed at one end to the anode vane (2), extends inside the airtight space, and then the other end is attached to the exhaust pipe (
10) is an antenna conductor fixedly attached, and (11) is an antenna cap capped on the exhaust pipe (10).

上記構成において、高調波抑制チョークを付加するため
に、金属容器(7)の出力側絶縁筒(8)と気密接合さ
れる側の端部と電気的に結合され、出力側絶縁筒(8)
の内側空間に向かって、任意の高調波の%波長の深さの
環状溝を有するチョーク構体(13)を配している。こ
のに波長チョーク構体は、一般的に電子レンジの電波漏
洩対策として用いられているドアシール等と同じ原理で
あり、チョーク構体(13)が空胴共振器の作用をする
ものである。チョーク構体(13)はプレスによる深絞
りで金属容器(7)と一体に形成されている。この時の
チョーク構体(13)の寸法は、2450MHzが基本
波の電子レンジ用マグネトロンの第5高調波抑制を目的
とするのであれば、第2図で示される深さdは、波長2
4.5画の約にで6.01111となる。
In the above configuration, in order to add a harmonic suppression choke, the output side insulating tube (8) is electrically coupled to the end of the metal container (7) on the side that is hermetically sealed to the output side insulating tube (8).
A choke structure (13) having an annular groove having a depth of % wavelength of an arbitrary harmonic is disposed toward the inner space of the harmonic. This wavelength choke structure has the same principle as a door seal or the like which is generally used as a countermeasure against radio wave leakage in microwave ovens, and the choke structure (13) acts as a cavity resonator. The choke structure (13) is formed integrally with the metal container (7) by deep drawing using a press. The dimensions of the choke structure (13) at this time are: If the purpose is to suppress the fifth harmonic of a microwave oven magnetron whose fundamental wave is 2450 MHz, the depth d shown in FIG.
Approximately 4.5 strokes equals 6.01111.

本実施例においては、第2図に示されるチョーク構体内
の寸法D1.g、チョーク構体外の寸法D2を、それぞ
れ、D1=11.0m1ll、  g”t、omnD2
=8.01+11に形成している。なお、このチョーク
構体(13)とアンテナ導体(9)とは、これらの間に
生じる高周波電界により放電が生じないための十分な距
離が保たれている。
In this embodiment, the dimension D1 within the choke structure shown in FIG. g, dimension D2 outside the choke structure, D1=11.0ml, g”t, omnD2, respectively.
=8.01+11. Note that a sufficient distance is maintained between the choke structure (13) and the antenna conductor (9) so that no discharge occurs due to the high frequency electric field generated between them.

本実施例と従来との実験したところ、本実施例は、一般
的に10閣の長さ1を有する出力側絶縁筒(8)が、そ
の長さlのに強が金属性のチョーク構体(13〉で覆わ
れるために、高周波的に空間と見なされる出力側絶縁筒
(8)の長さlが短縮されて1′となり、短波長の高次
高調波に対しても、第4図に示すように、従来のチョー
ク構成よりも優れた抑制効果を得ることができる。
An experiment between this embodiment and the conventional one revealed that in this embodiment, the output-side insulating tube (8), which generally has a length of 1, has a choke structure (8) made of strong metal, whose length is l. 13〉, the length l of the output side insulating tube (8), which is regarded as space in terms of high frequency, is shortened to 1′, and even for high-order harmonics with short wavelengths, As shown, a better suppression effect than the conventional choke configuration can be obtained.

本実施例においては、lが一定の場合、抑制しようとす
る波長が短ければ短いほどdが短縮され、l′が増加す
る。この場合は、先述の出力側絶縁筒(8)からの漏洩
の抑制をあまり期待できないので、第3図に示される第
2の実施例の構成の如く、1′を変えずに%λチョーク
構体を形成することが望ましい。
In this embodiment, when l is constant, the shorter the wavelength to be suppressed, the shorter d becomes and the more l' increases. In this case, it is not expected to suppress the leakage from the output-side insulating tube (8) to a great extent, so the %λ choke structure is constructed without changing 1', as in the configuration of the second embodiment shown in FIG. It is desirable to form a

(ト)発明の効果 本発明は短波長の高調波抑制にも充分な効果力釈簡単、
かつ、確実に得られるチョーク構体を、出力側絶縁筒の
内部に配置することにより、−段と電波漏洩の抑制効果
をあげることができ、SHF帯衛星放送等に対する電波
障害を抑制できる等の効果を奏する。
(g) Effects of the invention The present invention has sufficient effects for suppressing short wavelength harmonics.
Furthermore, by arranging the reliable choke structure inside the output side insulating cylinder, it is possible to suppress radio wave leakage to a greater extent, and it is possible to suppress radio wave interference to SHF band satellite broadcasting, etc. play.

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

第1図は本発明の一実施例によるマグネトロンの断面図
、第2図は同実施例の要部拡大断面図、第3図は他の実
施例の要部拡大断面図、第4図は従来と本発明の効果を
対比する高調波雑音特性図、第5図は従来の高調波抑制
マグネトロンの要部断面図である。 (1)・・・筒状陽極体、(5)・・・陰極構体、(7
)・・・筒状金属容器、(8)・・・出力側絶縁筒、ナ
導体、(12)(13)・・・チョーク構体。 (9)・・・アンチ
Fig. 1 is a sectional view of a magnetron according to an embodiment of the present invention, Fig. 2 is an enlarged sectional view of the main part of the same embodiment, Fig. 3 is an enlarged sectional view of the main part of another embodiment, and Fig. 4 is a conventional one. FIG. 5 is a sectional view of a main part of a conventional harmonic suppressing magnetron. (1)...Cylindrical anode body, (5)...Cathode structure, (7
)...Cylindrical metal container, (8)...Output side insulating tube, na conductor, (12) (13)...Choke structure. (9)...Anti

Claims (1)

【特許請求の範囲】[Claims] (1)陰極構体と該陰極構体の周囲に配置された複数の
ベインを有する筒状陽極体と、該筒状陽極体の一端に気
密空間を形成する筒状金属容器と、該筒状金属容器に気
密接合された出力側絶縁筒と、一端が前記ベインに電気
的に結合され、前記筒状金属容器、および、絶縁筒の内
側空間を通して延長されたアンテナ導体とを有するマグ
ネトロンにおいて、前記筒状金属容器に電気的に結合さ
れ、前記アンテナ導体をとりまく、高調波抑制用チョー
ク構体を、前記出力側絶縁筒の内側空間に配設したこと
を特徴とするマグネトロン。
(1) A cathode assembly, a cylindrical anode body having a plurality of vanes arranged around the cathode assembly, a cylindrical metal container forming an airtight space at one end of the cylindrical anode body, and the cylindrical metal container. In the magnetron, the magnetron has an output-side insulating tube hermetically sealed to the vane, and an antenna conductor having one end electrically coupled to the vane and extending through the inner space of the cylindrical metal container and the insulating tube. A magnetron characterized in that a harmonic suppressing choke structure electrically coupled to a metal container and surrounding the antenna conductor is disposed in an inner space of the output side insulating tube.
JP2035217A 1990-02-15 1990-02-15 Magnetron Pending JPH03238736A (en)

Priority Applications (4)

Application Number Priority Date Filing Date Title
JP2035217A JPH03238736A (en) 1990-02-15 1990-02-15 Magnetron
US07/653,429 US5180946A (en) 1990-02-15 1991-02-08 Magnetron having coaxial choke means extending into the output side insulating tube space
GB9103033A GB2243018B (en) 1990-02-15 1991-02-13 Magnetron
KR1019910002408A KR940006302B1 (en) 1990-02-15 1991-02-13 High harmonic frequency restraint structure of magnetron

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP2035217A JPH03238736A (en) 1990-02-15 1990-02-15 Magnetron

Publications (1)

Publication Number Publication Date
JPH03238736A true JPH03238736A (en) 1991-10-24

Family

ID=12435680

Family Applications (1)

Application Number Title Priority Date Filing Date
JP2035217A Pending JPH03238736A (en) 1990-02-15 1990-02-15 Magnetron

Country Status (1)

Country Link
JP (1) JPH03238736A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
KR19990015480A (en) * 1997-08-06 1999-03-05 구자홍 Microwave Magnetron

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
KR19990015480A (en) * 1997-08-06 1999-03-05 구자홍 Microwave Magnetron

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