JPS588537B2 - magnetron - Google Patents
magnetronInfo
- Publication number
- JPS588537B2 JPS588537B2 JP13895378A JP13895378A JPS588537B2 JP S588537 B2 JPS588537 B2 JP S588537B2 JP 13895378 A JP13895378 A JP 13895378A JP 13895378 A JP13895378 A JP 13895378A JP S588537 B2 JPS588537 B2 JP S588537B2
- Authority
- JP
- Japan
- Prior art keywords
- magnetic pole
- magnet
- tube axis
- magnet structure
- pole surface
- 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
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- Microwave Tubes (AREA)
Description
【発明の詳細な説明】 本発明はマグネトロンに関する。[Detailed description of the invention] The present invention relates to magnetrons.
近来、小形の永久磁石を真空容器の内部に封入して全体
を小形、軽量化したマグネトロンが実用になっている。Recently, magnetrons have been put into practical use that are made smaller and lighter by enclosing a small permanent magnet inside a vacuum container.
このマグネトロンは磁石を管軸上で作用空間に近接配置
する構造であるため出力アンテナ端子及びアンテナフィ
ーダは管軸からずらして突設するのが最も単純な構造と
なる点で採用されている。Since this magnetron has a structure in which the magnet is placed close to the working space on the tube axis, the output antenna terminal and the antenna feeder are protruded from the tube axis, which is the simplest structure.
しかし一方、出力アンテナ端子が管軸からずれているた
め電子レンジ等に取り付ける場合には取り付け方法が限
定されてしまう不都合があり、またアノードシリンダー
外周にとりつけるラジエータを一方向に片寄せて固定す
る必要があるなどの不都合がある。However, since the output antenna terminal is offset from the tube axis, there is an inconvenience that the mounting method is limited when installing it in a microwave oven, etc., and the radiator that is attached to the outer periphery of the anode cylinder needs to be fixed in one direction. There are some inconveniences such as:
そこで、出力アンテナ端子を管軸上に一致させる発明が
すでに提案されている。Therefore, an invention has already been proposed in which the output antenna terminal is aligned with the tube axis.
その1つは特開昭50−147277号公報に示される
もので、これは出力側の永久磁石に結合された磁性端板
の外方に空間部をつくり、アンテナフィーダをこの空間
部でクランク状に折り曲げ、管軸上のアンテナ端子に接
続する構成である。One of them is disclosed in Japanese Patent Application Laid-Open No. 50-147277, in which a space is created outside a magnetic end plate coupled to a permanent magnet on the output side, and an antenna feeder is mounted in a crank shape in this space. It is configured to be bent and connected to the antenna terminal on the tube axis.
しかしながらこれは管軸方向の全長が長大化するばかり
でなくアンテナフイーダがむやみに長くなり、負荷との
整合がとりにくくなってしまう欠点があり、実用性に乏
しい。However, this has the drawback that not only does the total length in the tube axis direction become long, but also the antenna feeder becomes unnecessarily long, making it difficult to match the load, and is therefore impractical.
また、実開昭53=2158号公報に開示されたものは
、永久磁石に斜め方向の切溝あるいは貫通孔を設けてこ
こをアンテナフィーダが通るようにしたものである。Furthermore, the magnet disclosed in Japanese Utility Model Application Publication No. 53/2158 is one in which a permanent magnet is provided with an oblique cut groove or a through hole through which an antenna feeder passes.
しかしながらこれは切溝や貫通孔を加工するというきわ
めてやっかいな工程を要し、また磁石材を切り取る分だ
け増量しなげればならず、きわめて実用性に乏しいもの
である。However, this requires an extremely troublesome process of cutting grooves and through holes, and requires an increase in the amount of magnet material to be cut out, making it extremely impractical.
本発明は以上のような従来技術の諸欠点をなくし、管軸
方向の全長をほとんど長大化することなく、しかも磁石
に複雑な加工を施すことなく管軸上に出力アンテナを位
置させたマグネトロンを提供するものである。The present invention eliminates the drawbacks of the prior art as described above, and creates a magnetron in which the output antenna is positioned on the tube axis without increasing the total length in the tube axis direction and without performing complicated processing on the magnet. This is what we provide.
すなわちその特徴とするところは永久磁石、又は永久磁
石と磁極片との組合せからなる磁石構体を管軸に対して
斜めに配設し、アンテナフイーダをこの磁石構体に沿い
側方を通して管軸上に導びき、アンテナ端子に接続する
ようにした構成である。In other words, the feature is that a magnet structure consisting of a permanent magnet or a combination of a permanent magnet and a magnetic pole piece is arranged obliquely to the tube axis, and the antenna feeder is passed laterally along this magnet structure and placed on the tube axis. The antenna terminal is connected to the antenna terminal.
以下図面を参照しながらその実施例を説明する。Examples thereof will be described below with reference to the drawings.
第1図ないし第3図に示す実施例は次の構造を有する。The embodiment shown in FIGS. 1 to 3 has the following structure.
軟鉄のような磁性体のアノードシリンダー11は、真空
容器の機能を有し、一端は磁性端板12、出力側封着リ
ング13、及び出力アンテナ端子14によって閉じられ
、他端はもう一方の磁性端板及びカソード入力端子(い
ずれも図示せず)によって閉じられている。An anode cylinder 11 made of a magnetic material such as soft iron has the function of a vacuum container, and one end is closed by a magnetic end plate 12, an output side sealing ring 13, and an output antenna terminal 14, and the other end is closed by a magnetic end plate 12, an output side sealing ring 13, and an output antenna terminal 14. It is closed by an end plate and a cathode input terminal (both not shown).
このアノードシリンダー11の内側には銅のような良導
電性の円筒15及び多数のアノードベイン16からなる
共振空胴構造体が設けられ、管軸C上に電子放射カソー
ド17がカソードリード18によって保持されている。Inside this anode cylinder 11, a resonant cavity structure consisting of a highly conductive cylinder 15 such as copper and a large number of anode vanes 16 is provided, and an electron emitting cathode 17 is held on the tube axis C by a cathode lead 18. has been done.
カソードリード18は図示しないカソード入力端子に固
定されている。The cathode lead 18 is fixed to a cathode input terminal (not shown).
カンード17とアノードベイン16との間は電子相互作
用空間19を構成している。An electron interaction space 19 is formed between the canard 17 and the anode vane 16 .
そこで、この作用空間19に管軸と平行な方向の磁束を
供給するために、作用空間をはさみ近接してそれぞれ磁
石構体20,20を配置してある。Therefore, in order to supply magnetic flux in a direction parallel to the tube axis to the working space 19, magnet assemblies 20, 20 are respectively arranged close to each other across the working space.
一方の磁石構体20は、円筒状永久磁石22と軟鉄のよ
うなリング状磁極片23とからなり、カンードリード1
8のまわりに同軸的に配置され、エンドシールドを兼ね
る保持円板24によって固定されている。One magnet structure 20 consists of a cylindrical permanent magnet 22 and a ring-shaped magnetic pole piece 23 made of soft iron.
8 and is fixed by a retaining disk 24 which also serves as an end shield.
さて出力側の磁石構体21は、第4図a+bに示すよう
に円柱状の磁石材25を側面と磁極面26a,26bと
の角度θを90°以外の角度で斜め方向に切断して得ら
れる永久磁石26と、その一端面26aに結合した円板
状磁極片27とから構成されている。Now, the magnet structure 21 on the output side is obtained by cutting the cylindrical magnet material 25 diagonally at an angle other than 90° between the side surface and the magnetic pole faces 26a and 26b, as shown in FIG. 4 a+b. It is composed of a permanent magnet 26 and a disc-shaped magnetic pole piece 27 coupled to one end surface 26a of the permanent magnet 26.
磁極片27の磁極面27aには中央に凹みがある。The magnetic pole face 27a of the magnetic pole piece 27 has a recess in the center.
磁石26の一方の切断面26a及び磁極片2γすなわち
この磁石構体の磁極面は管軸Cに一致1て位置され、他
方の切断面26bすなわち磁石構体の磁極面は管軸Cよ
りも図の岩側にずらして位置され磁性端板12に結合さ
れている。One cut surface 26a of the magnet 26 and the magnetic pole piece 2γ, that is, the magnetic pole face of this magnet structure, are aligned with the tube axis C, and the other cut surface 26b, that is, the magnetic pole surface of the magnet structure is positioned closer to the rock in the figure than the tube axis C. It is located offset to the side and is coupled to the magnetic end plate 12.
こうして磁石構体21は長手方向が事実上管軸Cに対し
て斜め方向になるように配置される。In this way, the magnet assembly 21 is arranged so that its longitudinal direction is substantially oblique to the tube axis C.
この磁石構体ス1は端板12に設けた位置決め用のプレ
ス成形突起28、及びエンドシールドを兼ねる保持円板
29により機械的に保持固定されている。This magnet structure S1 is mechanically held and fixed by a press-molded projection 28 for positioning provided on the end plate 12 and a holding disc 29 which also serves as an end shield.
そしてアンテナ端子14は管軸Cに一致して位置され、
端板12を覆いアノードシリンダー11の端部に気密接
合された封着リング13及び誘電体円筒30を介して外
方に突設されている。The antenna terminal 14 is positioned in line with the tube axis C,
It protrudes outward through a dielectric cylinder 30 and a sealing ring 13 that covers the end plate 12 and is hermetically sealed to the end of the anode cylinder 11 .
封着リング13の外周には導電体ガスケットリング31
がはめられている。A conductive gasket ring 31 is provided on the outer periphery of the sealing ring 13.
is fitted.
磁性端板12、保持円板29にはそれぞれ貫通孔12a
,29aが形成されており、これらの貫通孔を通して出
力アンテナフイーダ32が配置されている。The magnetic end plate 12 and the holding disk 29 each have a through hole 12a.
, 29a are formed, and the output antenna feeder 32 is arranged through these through holes.
このアンテナフイーダ32は一端が共振空胴の一部すな
わちアノードベインの外方端部近《に結合され、中間部
32aが磁石構体21に沿って側方を斜めに導かれ、他
端が管軸Cに一致して延長されたうえアンテナ端子14
に結合されている。One end of this antenna feeder 32 is coupled to a part of the resonant cavity, that is, near the outer end of the anode vane, an intermediate part 32a is guided laterally along the magnet structure 21, and the other end is connected to a tube. The antenna terminal 14 is extended in line with the axis C.
is combined with
なお磁石構体20,21は以上のように組み立てられた
状態で管軸方向の平行磁界により同時に着磁される。The magnet assemblies 20 and 21, assembled as described above, are simultaneously magnetized by a parallel magnetic field in the direction of the tube axis.
またアノードシリンダー11の外周には放熱フイン33
が固着されている。Furthermore, a heat dissipation fin 33 is provided on the outer periphery of the anode cylinder 11.
is fixed.
以上の本発明マグネトロンは、出力側磁石構体が事実上
管軸に対して斜めに配設され、これに沿ってアンテナフ
イーダが導出されて管軸上のアンテナ端子に結合されて
いるので、マグネトロンの管軸方向の全長を長大化する
ことなく管軸に一致したアンテナ端子をもつマグネトロ
ンを実現できる。In the above-described magnetron of the present invention, the output side magnet structure is arranged substantially obliquely to the tube axis, and the antenna feeder is led out along this and coupled to the antenna terminal on the tube axis. A magnetron having an antenna terminal aligned with the tube axis can be realized without increasing the total length in the tube axis direction.
そしてこれはアンテナフイーダを不所望に長大化しなく
てよく、負荷との整合特性や高周波損失をきたさない。This eliminates the need to make the antenna feeder undesirably long, and does not cause problems in matching characteristics with the load or high frequency losses.
また永久磁石は第4図に示したようにきわめて簡単な切
断加工のみで構成でき、作業性及び磁石材利用効率を何
ら阻害しない。Further, as shown in FIG. 4, the permanent magnet can be constructed by only a very simple cutting process, and does not impede workability or the efficiency of magnet material utilization.
このようにきわめて実用性の高いものである。In this way, it is extremely practical.
第5図及び第6図に示す実施例は、磁石26の磁極面2
6aに接続した磁極片27のの形状を、磁石の小さい切
断角となる隅26c側を厚くしてテーパ状の磁極面27
aを形成するようにしたものである。In the embodiment shown in FIGS. 5 and 6, the magnetic pole face 2 of the magnet 26 is
The shape of the magnetic pole piece 27 connected to 6a is made thicker on the corner 26c side, which is the small cutting angle of the magnet, so that the magnetic pole face 27 is tapered.
It is designed to form a.
これによって作用空間19中の磁束は一層管軸に平行に
なるように矯正される。As a result, the magnetic flux in the working space 19 is corrected so that it becomes more parallel to the tube axis.
もちろんテーパ面27aの角度及び面形状は発振特性が
最良となるように設計できる。Of course, the angle and surface shape of the tapered surface 27a can be designed to provide the best oscillation characteristics.
第7図に示す実施例は、磁石構体21として、切断面が
直角θな円柱状永久磁石26と、この磁石の両側に一方
の面がテーパ状に形成した磁極片27及び導磁性体41
(いずれも軟鉄のような磁性体でつ《られる)を結合し
て構成したものである。In the embodiment shown in FIG. 7, the magnet structure 21 includes a cylindrical permanent magnet 26 whose cut surface is at a right angle θ, magnetic pole pieces 27 with one surface tapered on both sides of the magnet, and a magnetic conductive material 41.
(Both are made of a magnetic material such as soft iron) bonded together.
この場合も磁石構体21の一方の磁極面すなわち磁極片
270作用空間対向磁極面27aを管軸Cに一致させ、
他方の磁極面すなわち導磁体41の裏面を管軸に対して
アンテナフイーダ32の位置と反対側にずらして端板1
2に結合させてある。Also in this case, one magnetic pole surface of the magnet structure 21, that is, the magnetic pole surface 27a facing the working space of the magnetic pole piece 270, is aligned with the tube axis C,
The end plate 1 is moved by shifting the other magnetic pole surface, that is, the back surface of the magnetic conductor 41 to the side opposite to the position of the antenna feeder 32 with respect to the tube axis.
It is combined into 2.
この実施例は、永久磁石を最も単純な円板形状とするこ
とができるので、一層低コストの磁石を使用しうる。In this embodiment, the permanent magnet can be made into the simplest disk shape, so a lower cost magnet can be used.
第9図に示す実施例は、第7図に示す導磁体41を使用
せず、磁性端板12自体を裏側から斜めに押し出して斜
めの磁石結合部42を形成したものである。In the embodiment shown in FIG. 9, the magnetic conductive body 41 shown in FIG. 7 is not used, and the magnetic end plate 12 itself is extruded obliquely from the back side to form an oblique magnet coupling portion 42.
これは磁気閉回路中の磁気抵抗を高めることもなく、ま
たそれほど加工性の困難を伴わず、組み立ても容易にな
り実用性が高いものとなる。This does not increase the magnetic resistance in the magnetic closed circuit, does not involve much difficulty in machining, and is easy to assemble, making it highly practical.
第10図a,b,cに示す実施例は、永久磁石の形状に
係わるもので、同図aに示すように横断面が楕円状の柱
状磁石材25を用い、切断面すなわち磁極面26a(又
は26b)の平面形状が同図Cに示すように真円となる
ように楕円短軸方向の側面と切断面すなわち磁極面との
角度θを定めて切断加工したものである。The embodiments shown in FIGS. 10a, b, and c relate to the shape of a permanent magnet, and as shown in FIG. Alternatively, 26b) is cut by setting an angle θ between the side surface in the short axis direction of the ellipse and the cut surface, that is, the magnetic pole surface, so that the planar shape of 26b is a perfect circle as shown in FIG.
これによって永久磁石の磁極面を真円にすることができ
、しかもこの磁石を用いると長軸方向がアンテナフイー
ダと直角方向になるため、アンテナフイーダと磁石との
間隔を縮めることなく磁石材の断面積を増しη眞力を高
めることができ、従って軸方向の長さが短かく体積の大
きい磁石を使用しうる。This allows the magnetic pole surface of the permanent magnet to be made into a perfect circle, and since the long axis direction of this magnet is perpendicular to the antenna feeder, the magnetic pole surface can be made into a perfect circle without reducing the distance between the antenna feeder and the magnet. The cross-sectional area of the magnet can be increased to increase the force, and therefore a magnet with a short axial length and a large volume can be used.
なお、本発明において磁石構体は永久磁石のみで構成さ
れる場合も含むものであり、また永久磁石は円筒状のも
のや、断面が多角形状のものでもよく、またアルニコ磁
石のような金属質のもののほかセラミノク磁石のように
粉末を圧縮成形したも島も使用しうる。In addition, in the present invention, the magnet structure may be composed of only permanent magnets, and the permanent magnets may be cylindrical or polygonal in cross section, or may be made of metal such as alnico magnets. In addition to magnets, it is also possible to use compression-molded powder such as Ceraminok magnets.
さらに、作用空間に対向する磁極面はその中心が管軸と
完全に一致している場合に限られず、少しずれている場
杏でも当然含まれる。Further, the center of the magnetic pole face facing the working space is not limited to a case where it completely coincides with the tube axis, but it is naturally possible to have a case where the center is slightly deviated from the tube axis.
以上のように本発明はマグネトロンの全長を長大化する
ことな《管軸とアンテナ端子軸とを一致させたマグネト
ロンを実現しうる。As described above, the present invention can realize a magnetron in which the tube axis and the antenna terminal axis are aligned without increasing the overall length of the magnetron.
第1図は本発明の一実施例を示す縦断面図、第2図は警
1図の2−2における横断面図、第3図ほそめ磁石を示
す斜視図、第4図は第3図の磁石の形成方法を説明する
図で、同aは上面図、同bは側面図、第5図は本発明の
他の実施例を示す要部断面図、第6図はその磁極片を示
す斜視図、第7図は本発明のさらに他の実施例を示す要
部断面図、第8図はその磁石を示す斜視図、第9図はさ
らに他の実施例を示す要部断面図、第10図はさらK他
の実施例の磁石形状及びその形成方法を示す図で、同a
は上面図、同bは側面図、同。
は切断面の展開図である。
11・・・・・・アノート5シリンダー、12・・・・
・・磁性端板、16・・・・・・アノードベイン、17
・・・・・・カソード、14・・・・・・出力アンテナ
端子、32・・・・・・アンテナフイーダ、20.21
・・・・・・磁石構体、C・・・・・・管軸、26・・
・・・・永久磁石、27・・・・・・磁極片、26a,
26b,27a・・・・・・磁極面。Fig. 1 is a longitudinal sectional view showing one embodiment of the present invention, Fig. 2 is a transverse sectional view taken at 2-2 in Fig. Figures illustrating a method of forming a magnet; Figure 5A is a top view, Figure 5B is a side view, Figure 5 is a cross-sectional view of main parts showing another embodiment of the present invention, and Figure 6 is a perspective view showing the magnetic pole pieces. 7 is a sectional view of a main part showing still another embodiment of the present invention, FIG. 8 is a perspective view showing the magnet, FIG. 9 is a sectional view of a main part showing still another embodiment, and FIG. The figure is a diagram showing the magnet shape and its formation method in another embodiment.
is a top view, b is a side view, and b is a side view. is a developed view of the cut surface. 11...Anote 5 cylinder, 12...
...Magnetic end plate, 16...Anode vane, 17
...Cathode, 14...Output antenna terminal, 32...Antenna feeder, 20.21
...Magnet structure, C...Tube shaft, 26...
...Permanent magnet, 27...Magnetic pole piece, 26a,
26b, 27a...Magnetic pole surface.
Claims (1)
て配設された永久磁石を含む磁石構体と、この磁石構体
の外方磁極面に接続された磁性端板と、この磁性端板よ
りも外方であって管軸上に設けられたアンテナ端子と、
上記アノードベインからなる共振空胴とアンテナ端子と
を接続するように設けられたアンテナフイーダとを具備
し、上記磁石構体は一方の磁極面を管軸上において作用
空間に近接対向させ他方の磁極面を管軸より上記アンテ
ナフイーダの位置と反対側にずらして上記磁性端板に接
続し実質的に管軸に対して斜めに配設されており、上記
アンテナフイーダは上記磁石構体の側方を通って上記ア
ンテナ端子に接続されてなるマグネトロン。 2 磁石構体は、磁極面が側面に対して傾斜した形状の
柱状又は筒状永久磁石を有してなる特許請求の範囲第1
項記載のマグネトロン。 3 磁石構体は、側面に対し垂直な磁極面を有する柱状
又は筒状永久磁石と、この磁石の磁極面に結合されたテ
ーパ状磁極片とを有してなる特許請求の範囲第1項記載
のマグネトロンっ 4 磁石構体は、外周が概して楕円状になった柱状又は
筒状磁石材からなり磁極面が円形状となるように短軸方
向の側面に対し傾斜した磁極面をもつ形状の永久磁石を
有してなる特許請求の範囲第2項記載のマグネトロン。[Claims] 1. A magnet structure including a permanent magnet disposed close to the working space between the cathode and the anode vane, a magnetic end plate connected to the outer magnetic pole surface of the magnet structure, and a magnetic end plate connected to the outer magnetic pole surface of the magnet structure. an antenna terminal provided on the tube axis outside the magnetic end plate;
An antenna feeder is provided to connect the resonant cavity made of the anode vane and the antenna terminal, and the magnet structure has one magnetic pole surface facing closely to the working space on the tube axis, and the other magnetic pole surface facing closely to the working space. The antenna feeder is connected to the magnetic end plate with its surface shifted from the tube axis to the side opposite to the position of the antenna feeder, and is arranged substantially obliquely to the tube axis, and the antenna feeder is located on the side of the magnet structure. The magnetron is connected to the above antenna terminal through the antenna terminal. 2. The magnet structure has a columnar or cylindrical permanent magnet whose magnetic pole surface is inclined with respect to the side surface.
Magnetron described in section. 3. The magnet structure according to claim 1, wherein the magnet structure includes a columnar or cylindrical permanent magnet having a magnetic pole surface perpendicular to the side surface, and a tapered magnetic pole piece coupled to the magnetic pole surface of this magnet. Magnetron 4 The magnet structure is a permanent magnet made of a columnar or cylindrical magnet material whose outer periphery is generally elliptical, and has a magnetic pole surface that is inclined with respect to the side surface in the short axis direction so that the magnetic pole surface is circular. A magnetron according to claim 2 comprising:
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP13895378A JPS588537B2 (en) | 1978-11-13 | 1978-11-13 | magnetron |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP13895378A JPS588537B2 (en) | 1978-11-13 | 1978-11-13 | magnetron |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5566834A JPS5566834A (en) | 1980-05-20 |
| JPS588537B2 true JPS588537B2 (en) | 1983-02-16 |
Family
ID=15234011
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP13895378A Expired JPS588537B2 (en) | 1978-11-13 | 1978-11-13 | magnetron |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS588537B2 (en) |
-
1978
- 1978-11-13 JP JP13895378A patent/JPS588537B2/en not_active Expired
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5566834A (en) | 1980-05-20 |
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