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JPS624815B2 - - Google Patents
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JPS624815B2 - - Google Patents

Info

Publication number
JPS624815B2
JPS624815B2 JP7352279A JP7352279A JPS624815B2 JP S624815 B2 JPS624815 B2 JP S624815B2 JP 7352279 A JP7352279 A JP 7352279A JP 7352279 A JP7352279 A JP 7352279A JP S624815 B2 JPS624815 B2 JP S624815B2
Authority
JP
Japan
Prior art keywords
vanes
cathode
strap
straps
vane
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
Application number
JP7352279A
Other languages
Japanese (ja)
Other versions
JPS55165549A (en
Inventor
Masahiro Kume
Norio Tashiro
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.)
Toshiba Corp
Original Assignee
Tokyo Shibaura 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 Tokyo Shibaura Electric Co Ltd filed Critical Tokyo Shibaura Electric Co Ltd
Priority to JP7352279A priority Critical patent/JPS55165549A/en
Publication of JPS55165549A publication Critical patent/JPS55165549A/en
Publication of JPS624815B2 publication Critical patent/JPS624815B2/ja
Granted legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01JELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
    • H01J23/00Details of transit-time tubes of the types covered by group H01J25/00
    • H01J23/16Circuit elements, having distributed capacitance and inductance, structurally associated with the tube and interacting with the discharge
    • H01J23/18Resonators
    • H01J23/22Connections between resonators, e.g. strapping for connecting resonators of a magnetron

Landscapes

  • Microwave Tubes (AREA)

Description

【発明の詳細な説明】 本発明は、マグネトロンの改良に関する。[Detailed description of the invention] The present invention relates to improvements in magnetrons.

従来のマグネトロン本体部は、第1図、第2図
に示されるように中央の円筒状の陰極11をとり
囲むように複数枚の板状陽極ベイン12が放射状
に配置され、ベイン12の外端は陽極円筒13に
固着されている。ベイン12の上下側端14a,
14bには、それぞれリング状の大小2本で一体
のストラツプ15a,15b,15c,15dが
交互にベイン12を1つおきに短絡するように接
続され、同一ベイン12の上端14aと下端14
bでは短絡するストラツプの大小関係は反対とな
る。隣り合つた2枚のベイン12と陽極円筒13
内壁とで囲まれ、一部が陰極11に向かつて開か
れた空間が空胴共振器16を形成し、ベイン先端
部17と陰極11の間の作用空間18を通じて結
合したこの空胴共振器16により、マグネトロン
の発振周波数が定まり、この発振周波数を不要モ
ードから分離し、安定させるのがストラツプであ
る。
As shown in FIGS. 1 and 2, in the conventional magnetron main body, a plurality of plate-shaped anode vanes 12 are arranged radially to surround a central cylindrical cathode 11, and the outer ends of the vanes 12 is fixed to the anode cylinder 13. Upper and lower ends 14a of the vane 12,
14b, two integrated ring-shaped straps 15a, 15b, 15c, and 15d are connected to alternately short-circuit every other vane 12.
In case b, the size relationship of the short-circuited straps is opposite. Two adjacent vanes 12 and anode cylinder 13
A space surrounded by an inner wall and partially open toward the cathode 11 forms a cavity resonator 16 , and this cavity resonator 16 is coupled through a working space 18 between the vane tip 17 and the cathode 11 . This determines the oscillation frequency of the magnetron, and the strap separates this oscillation frequency from unnecessary modes and stabilizes it.

しかし、ストラツプは、ベイン上下側端からベ
イン上下の端空間19へ漏れ出す高周波電界を変
形するために陰極11を軸方向に励振する成分が
生じ入力部20側へ高周波電磁界を漏洩させる大
きな原因となる。第3図はストラツプによる陰極
励振を示すために陰極11軸を中心とした円周上
で測定した端空間への漏洩電界分布を示してい
る。第3図aは第1図に示される陽極、陰極構造
を直線に展開した図であり、第3図b、同c、同
dにそれぞれ、内側ストラツプとベイン先端部の
中間部R1、外側ストラツプより少し外側R2、陽
極円筒13と外側ストラツプの中間部R3、を通
過するように測定した高周波電界の分布が示され
ている。縦軸は端空間19でのベイン端面14a
に垂直な方向の高周波電界強度E、横軸は陰極1
1軸を中心とした回転角Pである。第3図dよ
り、ストラツプから離れた所での漏洩高周波電界
はベインに対応した符号で振幅は正、負共ほぼ等
しい。しかし、ベイン先端近傍では、第3図bか
らわかるように、正負の振幅は大きく異なり、原
因は近くに反対電位のストラツプ15bが存在す
るベイン12は、ほとんどの電界がそのストラツ
プ15bへ向かうためである。このような状況で
は、陰極11の感ずる軸方向の高周波電界は打ち
消し合うことなく、第3図bの場合には、負の方
向の電界を感ずる。ここまではベイン12の一方
の側端14aのみを考えたが、他端14bでも大
小のストラツプの結合の順序が反転しているため
に同一方向に陰極11を励振する。上記の機構に
より励振された陰極11は、入力部20を通じて
第4図に示されるフイルターボツクス21に高周
波電磁界を放射し、低域フイルターを形成してい
るチヨークコイル22の焼損、放電等を引き起こ
すだけでなく、フイルターボツクス21内又は、
入力部20で反射し作用空間18に返つた高周波
電磁界エネルギーは陰極異常加熱、効率低下等マ
グネトロン特性を劣下させる原因となる場合があ
る。よつて、従来入力部20にλ/4チヨーク又
はコンデンサーを構成する方法、作用空間18か
ら見た入力側インピーダンスを調節する方法等に
より、漏洩電磁界に対する対策が行なわれてき
た。しかしこのような方法は、理論的予測が難し
く、主に試行錯誤により行なわれるため、時間
的、経済的無駄が非常に多く、又入力部20やフ
イルターボツクス21、チヨークコイル形状位置
が大きく規制されるため、低域フイルター部の十
分な効果が得られない場合がある等の欠点を有し
ていた。
However, since the strap deforms the high-frequency electric field leaking from the upper and lower ends of the vane to the upper and lower end spaces 19 of the vane, a component that excites the cathode 11 in the axial direction is generated, which is a major cause of leakage of the high-frequency electromagnetic field to the input section 20 side. becomes. FIG. 3 shows the leakage electric field distribution to the end space measured on the circumference centered on the axis of the cathode 11 to show cathode excitation by the strap. Fig. 3a is a linear development of the anode and cathode structures shown in Fig. 1 , and Figs. The distribution of the high-frequency electric field measured as it passes through R 2 slightly outside the strap and the intermediate portion R 3 between the anode cylinder 13 and the outside strap is shown. The vertical axis is the vane end surface 14a in the end space 19.
High-frequency electric field strength E in the direction perpendicular to , the horizontal axis is the cathode 1
This is the rotation angle P around one axis. From FIG. 3d, it can be seen that the leakage high-frequency electric field at a location away from the strap has a sign corresponding to Vane, and the amplitudes are almost equal in both positive and negative directions. However, as can be seen from Figure 3b, near the tip of the vane, the positive and negative amplitudes are greatly different. be. In such a situation, the high-frequency electric fields in the axial direction felt by the cathode 11 do not cancel each other out, and in the case of FIG. 3b, an electric field in the negative direction is felt. Up to this point, only one side end 14a of the vane 12 has been considered, but since the order of coupling of the large and small straps is also reversed at the other end 14b, the cathode 11 is excited in the same direction. The cathode 11 excited by the above mechanism radiates a high frequency electromagnetic field through the input section 20 to the filter box 21 shown in FIG. but inside the filter box 21 or
The high-frequency electromagnetic field energy reflected by the input section 20 and returned to the working space 18 may cause deterioration of magnetron characteristics such as abnormal heating of the cathode and reduction in efficiency. Therefore, countermeasures against leakage electromagnetic fields have conventionally been taken by configuring a λ/4 choke or a capacitor in the input section 20, adjusting the input side impedance as seen from the working space 18, and the like. However, such a method is difficult to predict theoretically and is carried out mainly by trial and error, resulting in a large amount of time and economic waste.In addition, the shape and position of the input section 20, filter box 21, and choke coil are greatly restricted. Therefore, the low-pass filter section has some drawbacks, such as not being able to provide a sufficient effect.

本発明は、陰極部の励振源を除去、又は減ずる
ことによりかかる欠点を除くことを目的としたも
のである。
The present invention aims to eliminate this drawback by eliminating or reducing the excitation source of the cathode section.

本発明の概要は、ベイン側端部に取り付けられ
たそれぞれ2本のストラツプの一部を、内側スト
ラツプと外側ストラツプが互いに接触することな
く交錯し入れ替わる形状とすることにより、陰極
励振成分を零とし上記欠点を解決するものであ
る。
The outline of the present invention is to reduce the cathode excitation component to zero by forming part of each of the two straps attached to the vane side end into a shape in which the inner strap and the outer strap intersect and replace each other without contacting each other. This solves the above drawbacks.

以下、図面に示した本発明の実施例に基づき、
詳細に説明を行なう。
Hereinafter, based on the embodiments of the present invention shown in the drawings,
I will explain in detail.

ストラツプ以外の図中の符号は従来例と同じも
のを用いる。ストラツプA30、ストラツプB3
1は管軸を通る直線C―C′の左右でベインを短
絡する順序が反転しており、直線C―C′と交差
する2点で右側で外側であつたストラツプは左側
の内側のストラツプと、又、右側で内側のもの
は、左側で外側のものと結合している。第5図を
展開して第6図aに示し、又、内側ストラツプと
ベイン先端部17の中間部R1上の端空間19へ
の漏洩高周波電界の分布を第6図bに示す。この
図からわかるように電界の負の部分が大となる領
域と正の部分とが大となる領域が等しく、全体と
して陰極11の軸方向への励振部分は相殺されて
零となり励振は起きない。
The symbols in the figures other than the straps are the same as in the conventional example. Strap A30, Strap B3
In 1, the order in which the vanes are shorted on the left and right sides of the straight line C-C' passing through the tube axis is reversed, and at the two points that intersect with the straight line C-C', the outer strap on the right side is connected to the inner strap on the left side. , and the inner one on the right side is combined with the outer one on the left side. FIG. 5 is expanded and shown in FIG. 6a, and the distribution of the leakage high-frequency electric field to the end space 19 above the intermediate portion R1 between the inner strap and the vane tip 17 is shown in FIG. 6b. As can be seen from this figure, the region where the negative part of the electric field is large and the region where the positive part is large are equal, and as a whole, the excitation part in the axial direction of the cathode 11 cancels out and becomes zero, and no excitation occurs. .

以上のように本発明は陰極11励振の大きな原
因であるストラツプ30,31による端空間19
への漏洩高周波電界は、全体として打ち消され、
そのため入力部20及びフイルターボツクス21
内部の設計は、作用空間18内から見た入力部側
インピーダンスの調節という厳しい規制を受ける
ことなく行なうことができ、マグネトロンの性能
の向上にも有効である。
As described above, the present invention is designed to improve the end space 19 due to the straps 30 and 31, which is a major cause of excitation of the cathode 11.
The high-frequency electric field leaking to the
Therefore, the input section 20 and the filter box 21
The internal design can be done without being subject to strict regulations such as adjusting the impedance on the input section side as seen from inside the working space 18, and is also effective in improving the performance of the magnetron.

第5図の実施例で大小ストラツプの交点が2点
のものを示したがこの交点数はベイン数以内の任
意の偶数個を選ぶことができる。そしてそれら交
差する位置は、管軸に対称な位置関係になつてい
る。又、交点でのストラツプ形状は、全交点を考
えた場合2本のストラツプが同等であること、つ
まりストラツプAがストラツプBの上方で交差す
る回数とその反対の場合の数が同一であることが
望ましい。
In the embodiment shown in FIG. 5, the large and small straps have two intersections, but the number of intersections can be any even number within the number of vanes. The positions where these intersect are symmetrical with respect to the tube axis. In addition, the shape of the strap at the intersection point is such that the two straps are equivalent when considering all the intersection points, that is, the number of times that strap A crosses above strap B and the number of times that the strap crosses over strap B are the same. desirable.

ストラツプ交差部の他の実施例を第7,8,9
図に示す。第7図は交差部でストラツプが互いに
接触するのを防ぎ組立精度を緩和するように、両
ストラツプの一部を切除したものであり、又、第
8図は、一方のストラツプを上下方向に曲げ、他
方のストラツプを避ける形状となつている。又、
第9図は、交点近くにストラツプの上下にズレた
切れ目をつくり、ベインを通じて接続したもので
あり、ストラツプ自体が交差していないため、製
造が簡単となる。
Other examples of strap intersections are shown in Nos. 7, 8, and 9.
As shown in the figure. Fig. 7 shows a part of both straps cut out to prevent the straps from coming into contact with each other at the intersection and reduce assembly precision, and Fig. 8 shows one strap bent in the vertical direction. , the shape is such that it avoids the other strap. or,
In FIG. 9, cuts are made at the top and bottom of the straps near the intersection, and the straps are connected through vanes, and the straps themselves do not intersect, which simplifies manufacturing.

以上のように、ストラツプの交差点がベインと
ベインの間にあるもの以外に、交点がベイン上に
あつてもよく、その実施例を第10図に示す。
As described above, in addition to the case where the intersection of the straps is located between the vanes, the intersection may be located on the vane, and an embodiment thereof is shown in FIG. 10.

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

第1図は従来構造の横断面図、第2図はその縦
断面図、第3図aないしdは端空間への漏洩電界
の分布を示す図、第4図はマグネトロンの外装を
含む断面図、第5図は本発明の一実施例を示す要
部横断面図、第6図a,bはその動作図、第7
図、第8図、第9図、第10図は各々他の実施例
を示す要部斜視図である。 11……陰極、12……ベイン、14a,14
b……ベイン側端部、30,31……一対のスト
ラツプ。
Figure 1 is a cross-sectional view of the conventional structure, Figure 2 is its longitudinal cross-section, Figures 3 a to d are diagrams showing the distribution of the leakage electric field to the end space, and Figure 4 is a cross-sectional view including the exterior of the magnetron. , FIG. 5 is a cross-sectional view of essential parts showing one embodiment of the present invention, FIGS. 6 a and b are operational diagrams, and FIG.
8, 9, and 10 are perspective views of main parts showing other embodiments. 11... cathode, 12... vane, 14a, 14
b... Vane side end, 30, 31... A pair of straps.

Claims (1)

【特許請求の範囲】[Claims] 1 中央部の陰極と、前記陰極をとり囲み放射状
に配置された複数個の陽極ベインと、前記ベイン
の外端部が固着されている陽極円筒と、前記ベイ
ンの側端部にあり前記ベインと1つおきに交互に
接続された2本一対のリング状ストラツプとを有
するマグネトロンにおいて、2本一対の前記スト
ラツプが前記ベイン間又は前記ベイン上にて互い
に接触することなく交差する部分を、管軸に対称
な位置関係で偶数個有することを特徴とするマグ
ネトロン。
1 a central cathode, a plurality of anode vanes surrounding the cathode and arranged radially, an anode cylinder to which the outer ends of the vanes are fixed, and a plurality of anode vanes located at side ends of the vanes. In a magnetron having two pairs of ring-shaped straps connected alternately to each other, the portion where the two pairs of straps intersect between the vanes or on the vanes without contacting each other is defined as the tube axis. A magnetron characterized by having an even number of magnetrons in a symmetrical positional relationship.
JP7352279A 1979-06-13 1979-06-13 Magnetron Granted JPS55165549A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP7352279A JPS55165549A (en) 1979-06-13 1979-06-13 Magnetron

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP7352279A JPS55165549A (en) 1979-06-13 1979-06-13 Magnetron

Publications (2)

Publication Number Publication Date
JPS55165549A JPS55165549A (en) 1980-12-24
JPS624815B2 true JPS624815B2 (en) 1987-02-02

Family

ID=13520646

Family Applications (1)

Application Number Title Priority Date Filing Date
JP7352279A Granted JPS55165549A (en) 1979-06-13 1979-06-13 Magnetron

Country Status (1)

Country Link
JP (1) JPS55165549A (en)

Also Published As

Publication number Publication date
JPS55165549A (en) 1980-12-24

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