JPH0418661B2 - - Google Patents

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Publication number
JPH0418661B2
JPH0418661B2 JP60296807A JP29680785A JPH0418661B2 JP H0418661 B2 JPH0418661 B2 JP H0418661B2 JP 60296807 A JP60296807 A JP 60296807A JP 29680785 A JP29680785 A JP 29680785A JP H0418661 B2 JPH0418661 B2 JP H0418661B2
Authority
JP
Japan
Prior art keywords
magnetron
horizontal
magnetic pole
yoke
cylindrical portion
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 - Lifetime
Application number
JP60296807A
Other languages
Japanese (ja)
Other versions
JPS62176027A (en
Inventor
Takeshi Ito
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.)
Panasonic Holdings Corp
Original Assignee
Matsushita Electronics Corp
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 Matsushita Electronics Corp filed Critical Matsushita Electronics Corp
Priority to JP29680785A priority Critical patent/JPS62176027A/en
Priority to US06/945,881 priority patent/US4794304A/en
Publication of JPS62176027A publication Critical patent/JPS62176027A/en
Publication of JPH0418661B2 publication Critical patent/JPH0418661B2/ja
Granted legal-status Critical Current

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Description

【発明の詳細な説明】 産業上の利用分野 本発明は、電子レンジ等に用いられる強制空冷
型のマグネトロン装置に関するものである。
DETAILED DESCRIPTION OF THE INVENTION Field of Industrial Application The present invention relates to a forced air-cooled magnetron device used in microwave ovens and the like.

従来の技術 一般に、電子レンジ等に用いられる強制空冷型
のマグネトロン装置は、マグネトロンの陽極筒体
の外周面に多数の放熱翼板を多段にとりつけてな
り、放熱翼板間に強制空冷用の気流を流通させる
構成となしている。このため、動作時におけるマ
グネトロンの温度上昇が緩和され、マグネトロン
が異常高温となることによる動作不能や励磁用永
久磁石の高温減磁を防止することができる。
BACKGROUND TECHNOLOGY In general, a forced air-cooled magnetron device used in a microwave oven, etc. has a large number of heat dissipation vanes attached in multiple stages to the outer peripheral surface of the anode cylinder of the magnetron, and forced air cooling air flows between the heat dissipation vanes. It is configured to distribute. Therefore, the temperature rise of the magnetron during operation is alleviated, and it is possible to prevent the magnetron from becoming inoperable due to abnormally high temperatures and from high-temperature demagnetization of the excitation permanent magnet.

発明が解決しようとする問題点 ところで、マグネトロン装置の一層の小型・軽
量化およびコストの低減を図るためには、空冷効
率の改善が必要となる。第5図は従来のマグネト
ロン装置における強制空冷用気流の流通路を示し
たもので、放熱翼板1の板間を流通する強制空冷
用気流2が、マグネトロンの陽極筒体3の付近で
両側方へ大きく分流してしまうことから、もつと
も高温となる陽極筒体を効率よく空冷し難いとい
う問題点があつた。なお、図中の6は放熱翼板1
の陽極筒体貫通用円筒部、5は枠状継鉄の側壁部
を示す。
Problems to be Solved by the Invention Incidentally, in order to further reduce the size, weight, and cost of magnetron devices, it is necessary to improve air cooling efficiency. FIG. 5 shows the flow path of the forced air cooling airflow in a conventional magnetron device, where the forced air cooling airflow 2 flowing between the plates of the heat dissipation vanes 1 flows on both sides in the vicinity of the anode cylinder 3 of the magnetron. There was a problem in that it was difficult to efficiently air cool the anode cylinder, which is naturally hot. In addition, 6 in the figure is the heat dissipation vane plate 1.
The cylindrical part for penetrating the anode cylinder body, 5 indicates the side wall part of the frame-shaped yoke.

また、陽極筒体3の外周面上に圧入等の方法で
とりつけられた放熱翼板1の円筒部14上に、次
いでとりつけられた放熱翼板1の円筒部4が経時
変化等で重なりやすく、このようなことが起こる
と、放熱翼板間隔に不同を生じるりみならず、円
筒部4を陽極筒体3に広い面積で密着させ得なく
なり、良好な放熱効果を得ることが困難になる。
Furthermore, the cylindrical portion 14 of the heat dissipating vane 1 attached to the outer peripheral surface of the anode cylinder 3 by a method such as press-fitting tends to overlap with the cylindrical portion 4 of the heat dissipating vane 1 that is subsequently attached due to changes over time. If this happens, not only will the spacing between the heat dissipation vanes vary, but the cylindrical portion 4 will not be able to be brought into close contact with the anode cylinder 3 over a wide area, making it difficult to obtain a good heat dissipation effect.

問題点を解決するための手段 本発明によると、マグネトロンの一方の磁極部
上に同軸的に積み重ねられた環状永久磁石の外側
磁極が、前記マグネトロンの他方の磁極部に枠状
継鉄を介して磁気的に結合され、前記マグネトロ
ンの陽極筒体の外周面にとりつけられたラジエー
タが、強制空冷用気流の流通路を介して多段に配
設された水平翼部と、この水平翼部同士を橋絡す
る垂直翼部とを有し、前記水平翼部が前記陽極筒
体を貫通させる円筒部と、前記継鉄の両側壁に接
する両端部とを有してなるマグネトロン装置にお
いて、前記垂直翼部を前記水平翼部と一体に成型
する。この垂直翼部は、前記水平翼部の相互間隔
を前記円筒部の軸方向長以上の寸度に確保するた
めに、前記継鉄の両側壁と前記円筒部との各間に
おいて前記両側壁に沿つた隔壁を形成する。
Means for Solving the Problems According to the present invention, the outer magnetic pole of the annular permanent magnet coaxially stacked on one magnetic pole part of the magnetron is connected to the other magnetic pole part of the magnetron via a frame-shaped yoke. A radiator that is magnetically coupled and attached to the outer circumferential surface of the anode cylinder of the magnetron bridges the horizontal blade sections arranged in multiple stages through a flow passage for forced air cooling. In the magnetron device, the vertical wing section has a cylindrical section through which the horizontal wing section penetrates the anode cylinder, and both end sections contact both side walls of the yoke. is integrally molded with the horizontal wing portion. In order to ensure that the mutual spacing between the horizontal wing parts is greater than or equal to the axial length of the cylindrical part, the vertical wing parts are provided on both side walls between each side wall of the yoke and the cylindrical part. Forms parallel partition walls.

また、ラジエータを主として押し出し成型法に
よつて能率よく製造できるのみならず、ラジエー
タの円筒部にマグネトロンを一挙に圧入ことが可
能となる。そのうえ、前記円筒部が相互に重なり
合うことがなくなるので、ラジエータをマグネト
ロンの陽極筒体に広い面積で密着させることがで
きる。
Furthermore, not only can the radiator be efficiently manufactured mainly by extrusion molding, but also the magnetron can be press-fitted into the cylindrical portion of the radiator all at once. Furthermore, since the cylindrical portions do not overlap each other, the radiator can be brought into close contact with the anode cylindrical body of the magnetron over a wide area.

実施例 つぎに本発明を図面に示した実施例とともに詳
しく説明する。
Embodiments Next, the present invention will be described in detail with reference to embodiments shown in the drawings.

第1図において、マグネトロン6の陽極筒体の
外周面にとりつけられているラジエータ7は、ア
ルミニウムまたはその合金からなり、第2図に示
すような断面形状を有している。ラジエータ7の
各水平翼部8は強制空冷用気流の流通路を介して
多段に配設されており、各水平翼部8にはマグネ
トロン6の陽極筒体を貫通させるための円筒部9
が形成されている。また、水平翼部間には水平翼
部8を相互に橋絡する一対の垂直翼部10が一体
に設けられており、この垂直翼部10によつて水
平翼部8の相互間隔が規制される。すなわち、水
平翼部の相互間隔は垂直翼部10によつて円筒部
9の軸方向長以上の寸度に確保される。円筒部9
と垂直翼部10との最短間隔Aは、円筒部9の外
径Bの10〜30%となされている。
In FIG. 1, a radiator 7 attached to the outer peripheral surface of an anode cylinder of a magnetron 6 is made of aluminum or an alloy thereof, and has a cross-sectional shape as shown in FIG. Each horizontal blade part 8 of the radiator 7 is arranged in multiple stages via a forced air cooling air flow path, and each horizontal blade part 8 has a cylindrical part 9 for penetrating the anode cylinder of the magnetron 6.
is formed. Further, a pair of vertical wing sections 10 that bridge the horizontal wing sections 8 to each other are integrally provided between the horizontal wing sections, and the mutual spacing of the horizontal wing sections 8 is regulated by the vertical wing sections 10. Ru. That is, the mutual spacing between the horizontal wing sections is ensured by the vertical wing section 10 to a dimension equal to or longer than the axial length of the cylindrical section 9. Cylindrical part 9
The shortest distance A between the vertical wing portion 10 and the vertical wing portion 10 is set to 10 to 30% of the outer diameter B of the cylindrical portion 9.

このようなラジエータ7は、押し出し成型によ
つて形成された長尺のものを所定寸度で切断した
のち、円筒部9をプレス加工で形成することによ
つて比較的廉価に得ることができる。なお、マグ
ネトロン6の一方の磁極部11上には図外の円環
状永久磁石が同軸的に積み重ねられ、この磁石の
外側磁極が枠状継鉄12を通じていま一つの環状
永久磁石13の外側磁極に磁気的に結合されるの
であり、磁石13の内側磁極はマグネトロン6の
他方の磁極部に磁気的に結合される。
Such a radiator 7 can be obtained relatively inexpensively by cutting a long piece formed by extrusion molding to a predetermined size and then forming the cylindrical part 9 by press working. Note that an annular permanent magnet (not shown) is coaxially stacked on one magnetic pole portion 11 of the magnetron 6, and the outer magnetic pole of this magnet is connected to the outer magnetic pole of another annular permanent magnet 13 through a frame-shaped yoke 12. The inner magnetic pole of the magnet 13 is magnetically coupled to the other magnetic pole portion of the magnetron 6.

第3図に示すように、ラジエータ7の水平翼部
8間を流通する強制空冷用気流14のうち、一対
の垂直翼部10,10間に入つたものは、マグネ
トロン6の陽極筒体の近傍で両側方へ分流する
が、一対の垂直翼部10,10による隔壁作用の
ために両側方へ大きく偏向せず、陽極筒体と垂直
翼部10との間の狭小部を高密度で進行したのち
内方へ大きく向きを変える。このため、マグネト
ロン6の陽極筒体の全周およびその近傍のラジエ
ータ部分をよりよく空冷することができる。ま
た、垂直翼部10と枠状継鉄12の側壁との間を
流通する空冷用気流は垂直翼部10に沿つて直進
し、この領域におけるラジエータ部分も適度に空
冷されるのであつて、垂直翼部10による放熱面
積の拡大と相まつて良好な放熱効果を得ることが
できる。
As shown in FIG. 3, of the forced air cooling airflow 14 flowing between the horizontal blades 8 of the radiator 7, the air that enters between the pair of vertical blades 10, 10 is near the anode cylinder of the magnetron 6. However, due to the partitioning effect of the pair of vertical wing sections 10, 10, the flow was not deflected significantly to both sides, and instead proceeded at a high density in the narrow part between the anode cylinder and the vertical wing section 10. Later, it turns drastically inward. Therefore, the entire circumference of the anode cylinder of the magnetron 6 and the radiator portion in the vicinity can be better air-cooled. Further, the air cooling air flowing between the vertical wing section 10 and the side wall of the frame-shaped yoke 12 travels straight along the vertical wing section 10, and the radiator section in this region is also appropriately air-cooled. In combination with the expansion of the heat radiation area by the wing portion 10, a good heat radiation effect can be obtained.

円筒部9と垂直翼部10との最短間隔Aが円筒
部9の外径Bの10%未満になると、最短間隔Aに
おける空気抵抗が増し、一対の垂直翼部10,1
0間に流入する空冷用気流に減少をきたす。ま
た、最短間隔Aが外径Bの30%を越えると、陽極
筒体の背面側へ回り込む気流が減少してしまう。
When the shortest distance A between the cylindrical portion 9 and the vertical wing portion 10 becomes less than 10% of the outer diameter B of the cylindrical portion 9, air resistance at the shortest distance A increases, and the pair of vertical wing portions 10, 1
This causes a decrease in the airflow for cooling that flows in between zero and zero. Furthermore, if the shortest interval A exceeds 30% of the outer diameter B, the airflow that goes around to the back side of the anode cylinder will decrease.

第4図は実験結果に基づくA/B値−陽極筒体
温度特性を示すもので、これより、A/B=10〜
30%(たとえばA=40mmに於けるB値が4mm〜12
mm)のとき、従来のもの(B=約25mm)に比べて
陽極筒体温度を15〜25℃下げ得、A/B=15〜25
%のときには約25℃下げ得ることがわかる。
Figure 4 shows the A/B value vs. anode cylinder temperature characteristics based on the experimental results, and from this, A/B = 10 ~
30% (for example, B value at A = 40 mm is 4 mm to 12
mm), the anode cylinder temperature can be lowered by 15 to 25 degrees Celsius compared to the conventional one (B = approximately 25 mm), and A/B = 15 to 25
%, it can be seen that the temperature can be lowered by about 25℃.

発明の効果 以上のように本発明によると、ラジエータに垂
直翼部を付加するだけの簡単な改造によつて効率
のよい空冷効果を得ることができるのであり、し
かも、かかるラジエータは押し出し成型とプレス
加工とによつて比較的安価に得ることができる。
そのうえ、陽極筒体にラジエータを圧入等の方法
でとりつける作業が簡素化されるという利点もあ
る。
Effects of the Invention As described above, according to the present invention, an efficient air cooling effect can be obtained by simply modifying the radiator by adding vertical blades. It can be obtained relatively inexpensively by processing.
Furthermore, there is also the advantage that the work of attaching the radiator to the anode cylinder by a method such as press fitting is simplified.

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

第1図は本発明を実施したマグネトロン装置の
一部破断斜視図、第2図は同装置のラジエータの
側断面図、第3図は同装置の空冷用気流の流通路
を示す平面図、第4図は本発明の効果を説明する
ためのA/B値−陽極筒体温度特性図、第5図は
従来のマグネトロン装置の空冷用気流の流通路を
示す平面図である。 6……マグネトロン、7……ラジエータ、8…
…水平翼部、9……円筒部、10……垂直翼部。
FIG. 1 is a partially cutaway perspective view of a magnetron device embodying the present invention, FIG. 2 is a side sectional view of a radiator of the device, FIG. FIG. 4 is an A/B value-anode cylinder temperature characteristic diagram for explaining the effects of the present invention, and FIG. 5 is a plan view showing a flow path of air cooling air in a conventional magnetron device. 6... Magnetron, 7... Radiator, 8...
...Horizontal wing section, 9... Cylindrical section, 10... Vertical wing section.

Claims (1)

【特許請求の範囲】[Claims] 1 マグネトロンの一方の磁極部上に同軸的に積
み重ねられた環状永久磁石の外側磁極が、前記マ
グネトロンの他方の磁極部に枠状継鉄を介して磁
気的に結合され、前記マグネトロンの陽極筒体の
外周面にとりつけられたラジエータが、強制空冷
用気流の流通路を介して多段に配設された水平翼
部と、この水平翼部同士を橋絡する垂直翼部とを
有し、前記水平翼部が前記陽極筒体を貫通させる
円筒部と、前記継鉄の両側壁に接する両端部とを
有してなるマグネトロン装置において、前記垂直
翼部は前記水平翼部と一体に成型されていて、前
記水平翼部の相互間隔を前記円筒部の軸方向長以
上の寸度に確保するために、前記継鉄の両側壁と
前記円筒部との各間において前記両側壁に沿つた
隔壁を形成していることを特徴とするマグネトロ
ン装置。
1. The outer magnetic pole of an annular permanent magnet coaxially stacked on one magnetic pole part of the magnetron is magnetically coupled to the other magnetic pole part of the magnetron via a frame-shaped yoke, and the anode cylindrical body of the magnetron A radiator attached to the outer circumferential surface of the horizontal blade has horizontal blade sections arranged in multiple stages via forced air cooling air flow passages, and a vertical blade section that bridges the horizontal wing sections. In the magnetron device, the wing portion has a cylindrical portion that penetrates the anode cylinder, and both end portions contacting both side walls of the yoke, wherein the vertical wing portion is integrally molded with the horizontal wing portion. , in order to ensure that the mutual spacing between the horizontal wing portions is greater than or equal to the axial length of the cylindrical portion, partition walls are formed between both side walls of the yoke and the cylindrical portion along the both side walls; A magnetron device characterized by:
JP29680785A 1985-12-27 1985-12-27 Magnetron device Granted JPS62176027A (en)

Priority Applications (2)

Application Number Priority Date Filing Date Title
JP29680785A JPS62176027A (en) 1985-12-27 1985-12-27 Magnetron device
US06/945,881 US4794304A (en) 1985-12-27 1986-12-24 Magnetron with cooling fin structure

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP29680785A JPS62176027A (en) 1985-12-27 1985-12-27 Magnetron device

Publications (2)

Publication Number Publication Date
JPS62176027A JPS62176027A (en) 1987-08-01
JPH0418661B2 true JPH0418661B2 (en) 1992-03-27

Family

ID=17838397

Family Applications (1)

Application Number Title Priority Date Filing Date
JP29680785A Granted JPS62176027A (en) 1985-12-27 1985-12-27 Magnetron device

Country Status (1)

Country Link
JP (1) JPS62176027A (en)

Family Cites Families (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5460453U (en) * 1977-10-05 1979-04-26

Also Published As

Publication number Publication date
JPS62176027A (en) 1987-08-01

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