JPH0754669B2 - Vane magnetron with pressure equalizing ring - Google Patents
Vane magnetron with pressure equalizing ringInfo
- Publication number
- JPH0754669B2 JPH0754669B2 JP62144743A JP14474387A JPH0754669B2 JP H0754669 B2 JPH0754669 B2 JP H0754669B2 JP 62144743 A JP62144743 A JP 62144743A JP 14474387 A JP14474387 A JP 14474387A JP H0754669 B2 JPH0754669 B2 JP H0754669B2
- Authority
- JP
- Japan
- Prior art keywords
- anode
- pressure equalizing
- equalizing ring
- pieces
- magnetron
- 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
Links
- 230000008859 change Effects 0.000 description 14
- 238000005219 brazing Methods 0.000 description 13
- 238000004519 manufacturing process Methods 0.000 description 5
- 230000008646 thermal stress Effects 0.000 description 5
- 238000005452 bending Methods 0.000 description 4
- 230000000694 effects Effects 0.000 description 4
- 230000000452 restraining effect Effects 0.000 description 4
- 230000010355 oscillation Effects 0.000 description 3
- 230000001419 dependent effect Effects 0.000 description 2
- 238000009826 distribution Methods 0.000 description 2
- 230000009471 action Effects 0.000 description 1
- 238000007796 conventional method Methods 0.000 description 1
- 230000009467 reduction Effects 0.000 description 1
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
- H01J23/00—Details of transit-time tubes of the types covered by group H01J25/00
- H01J23/16—Circuit elements, having distributed capacitance and inductance, structurally associated with the tube and interacting with the discharge
- H01J23/18—Resonators
- H01J23/22—Connections between resonators, e.g. strapping for connecting resonators of a magnetron
Landscapes
- Microwave Tubes (AREA)
Description
【発明の詳細な説明】 [産業上の利用分野] 本発明は、クロス・フィールド・デバイスとしてのマグ
ネトロンに関し、特に、複数の陽極片(ベーン)を均圧
環で継いだ均圧環付ベーン形マグネトロンに関するもの
である。TECHNICAL FIELD The present invention relates to a magnetron as a cross field device, and more particularly to a vane magnetron with a pressure equalizing ring in which a plurality of anode pieces (vanes) are connected by a pressure equalizing ring. It is a thing.
[従来の技術] 従来一般に、均圧環付ベーン形マグネトロンは、第3図
(A),(B)に示すように、陽極筒1の内面から中心
に向け半径方向に延出する複数の陽極片2〜19と、各陽
極片2〜19の一方の面側(表面)に同心的に配された内
側均圧環20及び外側均圧環21と、他方の面側(裏面)に
同心的に配された内側均圧環22及び外側均圧環23とから
なり、表面側の内側均圧環20及び裏面側の外側均圧環23
は1つ置きの陽極片2,4,6,8,10,12,14,16,18にロウ付け
によって接続されており、表面側の外側均圧環21及び裏
面側の内側均圧環22は残る陽極片3,5,7,9,11,13,15,17,
19にロウ付けによって接続されているものである。な
お、均圧環20〜23が接続されない陽極片には、非接触用
の逃げ溝(図示せず)が夫々形成されている。[Prior Art] Conventionally, a vane type magnetron with a pressure equalizing ring is generally provided with a plurality of anode pieces extending radially from the inner surface of the anode cylinder 1 toward the center as shown in FIGS. 3 (A) and 3 (B). 2 to 19, inner pressure equalizing ring 20 and outer pressure equalizing ring 21 concentrically arranged on one surface side (front surface) of each anode piece 2 to 19, and concentrically arranged on the other surface side (rear surface). An inner pressure equalizing ring 22 and an outer pressure equalizing ring 23, and a front side inner pressure equalizing ring 20 and a back side outer pressure equalizing ring 23.
Is connected to every other anode piece 2,4,6,8,10,12,14,16,18 by brazing, and the outer pressure equalizing ring 21 on the front surface side and the inner pressure equalizing ring 22 on the back surface side remain. Anode piece 3,5,7,9,11,13,15,17,
It is connected to 19 by brazing. In addition, non-contact escape grooves (not shown) are formed in the anode pieces to which the pressure equalizing rings 20 to 23 are not connected.
また、別の均圧環付ベーン形マグネトロンとして、特開
昭56−15534号に開示の如く、陽極筒の中心から異なる
直径の3個の均圧環を備え、中央の均圧環は1つ置きの
陽極片へ接続されており、内側と外側の均圧環は残りの
陽極片に接続されているものが知られている。Further, as another vane type magnetron with a pressure equalizing ring, as disclosed in JP-A-56-15534, three pressure equalizing rings having different diameters from the center of the anode cylinder are provided, and the center pressure equalizing rings are every other anode. It is known that the inner and outer pressure equalizing rings are connected to the remaining anode pieces.
[解決すべき問題点] しかしながら、上記各マグネトロンにあっては、次の問
題がある。[Problems to be Solved] However, each magnetron has the following problems.
前者のマグネトロンにおいては、複数の陽極片の両
面に内側均圧環20,22及び外側均圧環21,23を備えた構造
であるため、高い周波数のマグネトロンに適用すること
が極めて困難である。即ち、そのマグネトロンの製作方
法は、まず、組立治具に陽極筒1と一方の均圧環22,23
を載置位置決めした後、ロウ付面を合せながら陽極片2
〜19を順次挿入し、放射状に整列された陽極片2〜19の
上に他方の均圧環20,21を置くものであるが、例えば周
波数9.5GHzのマグネトロンにおいては、陽極片2〜19の
厚さ寸法が0.4mmであり、表裏の均圧環20,23の厚さが夫
々0.2mmとなり、高周波数のマグネトロンになればなる
ほど、陽極筒1,陽極片2〜19及び均圧環20,23を僅小寸
法とせざるを得ないので、陽極片2〜19と両面の均圧環
20〜23のロウ付面合致作業が著しく困難であるばかり
か、陽極片2〜19及び均圧環20〜23の高い寸法精度が要
求される。上記9.5GHzのマグネトロンの場合、各寸法に
対して±0.01mmの高精度が必要とされ、製造コスト高を
招く。Since the former magnetron has a structure in which the inner pressure equalizing rings 20 and 22 and the outer pressure equalizing rings 21 and 23 are provided on both surfaces of a plurality of anode pieces, it is extremely difficult to apply it to a high frequency magnetron. That is, the manufacturing method of the magnetron is as follows. First, the anode jig 1 and one of the pressure equalizing rings 22, 23 are used in the assembly jig.
After placing and positioning, place the anode piece 2 while matching the brazing surfaces.
-19 are sequentially inserted, and the other equalizing rings 20 and 21 are placed on the anode pieces 2 to 19 which are radially arranged. For example, in a magnetron with a frequency of 9.5 GHz, the thickness of the anode pieces 2 to 19 is increased. The size is 0.4 mm, the thickness of the pressure equalizing rings 20 and 23 on the front and back sides is 0.2 mm, and the higher the frequency of the magnetron, the smaller the anode cylinder 1, the anode pieces 2 to 19 and the pressure equalizing rings 20 and 23. Since the size must be small, the anode pieces 2 to 19 and pressure equalizing rings on both sides
Not only is it extremely difficult to match the brazed surfaces of 20 to 23, but high dimensional accuracy of the anode pieces 2 to 19 and the pressure equalizing rings 20 to 23 is required. In the case of the above 9.5 GHz magnetron, a high precision of ± 0.01 mm is required for each dimension, resulting in high manufacturing cost.
後者のマグネトロンにおいては、3つの均圧環を陽
極片に配置した構造であるため、中央の均圧環と接続す
る陽極片の組のロウ付面は1箇所であるが、内側及び外
側の均圧環と接続する陽極片の組のロウ付け面は2箇所
となり、異なる陽極片によってロウ付面の数が異なるの
で、熱応力の違いによって陽極片の変形などを起すおそ
れが強い。Since the latter magnetron has a structure in which three pressure equalizing rings are arranged on the anode piece, the brazing surface of the set of anode pieces connected to the central pressure equalizing ring is at one location, but the inner and outer pressure equalizing rings are There are two brazing surfaces of the set of anode pieces to be connected, and the number of brazing surfaces is different for different anode pieces. Therefore, there is a strong possibility that the anode pieces may be deformed due to the difference in thermal stress.
[発明の目的] 本発明は、上記各従来例の問題点を解決するものであ
り、その目的は、容易な製造作業によって製造可能であ
ると共に、陽極片の熱応力による変形などのおそれがな
く、高い周波数のマグネトロンに適用し得る構造の均圧
環付ベーン形マグネトロンを提供することにある。[Object of the Invention] The present invention solves the problems of the above-mentioned conventional examples, and an object of the present invention is that the anode piece can be manufactured by an easy manufacturing operation and there is no fear of deformation due to thermal stress of the anode piece. To provide a vane type magnetron with a pressure equalizing ring having a structure applicable to a high frequency magnetron.
「問題点の解決手段] 上記目的を達成するため、本発明に係る均圧環付ベーン
形マグネトロンは、中心に向け半径方向に延出する複数
の陽極片を有する陽極筒と、その陽極筒の一方の面側に
おいて配され、その中心に対して異なる直径で同心円の
4個又はそれ以上の偶数個の均圧環とからなり、中心か
ら奇数番目の均圧環は1つおきの陽極片に接続されてい
ると共に、その中心から偶数番目の均圧環は残りの陽極
片に接続されていることを特徴とする。[Means for Solving Problems] In order to achieve the above object, a vane magnetron with a pressure equalizing ring according to the present invention has an anode cylinder having a plurality of anode pieces extending in a radial direction toward the center, and one of the anode cylinders. Of four or more even pressure-equalizing rings arranged concentrically with respect to the center and having different diameters with respect to the center, and the odd-numbered pressure-equalizing rings from the center are connected to every other anode piece. In addition, the even pressure rings from the center are connected to the remaining anode pieces.
かかる構成によれば次の作用効果を奏するものである。 According to this structure, the following operational effects are obtained.
陽極片の片面のみに均圧環を有するものであるか
ら、その両面にそれぞれ均圧環がある場合に比し、マグ
ネトロンの組付作業がすこぶる簡便となるので、僅小寸
法の陽極片及び均圧環の組付精度を高くでき、高い周波
数のベーン形マグネトロンを実現できる。Since the equalizing ring is provided on only one side of the anode piece, it is much easier to assemble the magnetron than when there are equalizing rings on both sides of the anode piece. Assembling accuracy can be improved and a high frequency vane magnetron can be realized.
2個又は3個の均圧環ではなく、4個以上の偶数の
均圧環を片面に配した構造であるから、周波数設定のた
めの容量負荷を2個,3個の場合に比して分散化させるこ
とができるので、同一周波数の場合には均圧環の太さ
(幅)を細くすることができる。陽極片は中心側(陰極
側)が高温であり陽極筒側が低温となっているため、強
い温度勾配を持っている。従って、均圧環の内側の方が
外側の方に比べて遥に熱膨張が盛んである。マグネトロ
ンの周波数変化は均圧環の幅に比例するから、熱膨張の
大きな内側の均圧環が周波数変化に支配的ないし優性的
となる。本発明では、内側の均圧環の幅が小さくなって
いるので周波数変化を優性的に抑制できると共に、外側
に追加された均圧環は周波数変化に劣勢的であってまた
僅小幅であることから、結果として、また実証的にも周
波数変化の温度依存特性を顕著に改善することができ
る。Since it has a structure in which four or more even pressure-equalizing rings are arranged on one side instead of two or three equalizing rings, the capacity load for frequency setting is distributed compared to the case of two or three. Therefore, the thickness (width) of the pressure equalizing ring can be reduced in the case of the same frequency. The anode piece has a strong temperature gradient because the center side (cathode side) has a high temperature and the anode cylinder side has a low temperature. Therefore, the inner side of the pressure-equalizing ring has much higher thermal expansion than the outer side. Since the frequency change of the magnetron is proportional to the width of the pressure equalizing ring, the inner pressure equalizing ring with large thermal expansion becomes dominant or dominant in the frequency change. In the present invention, since the width of the pressure equalizing ring on the inner side is small, it is possible to suppress the frequency change dominantly, and the pressure equalizing ring added to the outside is inferior to the frequency change and is also a very small width. As a result, and empirically, it is possible to significantly improve the temperature-dependent characteristics of the frequency change.
陽極片の均圧環が接続された面側は均圧環による拘
束面となっているため、陽極筒から半径方向に延出する
複数の陽極片は自由面側が自由膨張するので拘束面側へ
撓み、陽極片全体としては太鼓皮の様に片面側に膨れた
状態になる。ここで、1つおきの陽極片(第1組)が最
内側の均圧環と最外側均圧環に接続されており、残る陽
極片(第2組)が内側から2番目の均圧環と3番目の均
圧環に接続しているとすれば、第1組の陽極片の接続点
は両端に離れ過ぎであるのに対し、第2組の陽極片の中
央に近接し過ぎているので、第1組の陽極片と第2組の
陽極片とでは撓み状態が異なるため、周波数変化にバラ
ツキが生じる。本発明のように、第1組の陽極片が1番
目と3番目に、第2組の陽極片が2番目と4番目にそれ
ぞれ接続されている場合には、第1組の陽極片も第2組
の陽極片も接続箇所の分布が近似しているので、第1組
の陽極片と第2組の陽極片との撓み状態の差が少なくな
り、周波数変化のバラツキを抑制できる。Since the surface side of the anode piece to which the pressure equalizing ring is connected is a restraining surface due to the pressure equalizing ring, the plurality of anode pieces extending in the radial direction from the anode cylinder flex toward the restraining surface side because the free surface side expands freely. The entire anode piece is in a state of bulging to one side like a drum skin. Here, every other positive electrode piece (first set) is connected to the innermost pressure equalizing ring and the outermost pressure equalizing ring, and the remaining positive electrode pieces (second set) are the second equalizing ring and the third from the inner side. If it is connected to the pressure equalizing ring of the first set, the connecting points of the first set of anode pieces are too far away from both ends, while they are too close to the center of the second set of anode pieces. Since the bending state is different between the anode pieces of the set and the anode pieces of the second set, variations occur in the frequency change. As in the present invention, when the first set of anode strips is connected to the first and third sides and the second set of anode strips is connected to the second and fourth sides, respectively, the first set of anode strips is also connected to the first set. Since the distribution of the connection points is similar in the two sets of anode pieces, the difference in the bending state between the first set of anode pieces and the second set of anode pieces is reduced, and variation in frequency change can be suppressed.
各陽極片の接続箇所が偶数箇所で皆等しくなってい
るので、上記、の利点と相まって、高温下における
熱応力がいずれの陽極片及び均圧環についても均等化さ
れる傾向にあり、発振安定性の良好なマグネトロンを実
現できる。Since the connection points of each anode piece are equal at all even-numbered points, combined with the above advantages, thermal stress at high temperature tends to be equalized for any anode piece and pressure equalizing ring, and oscillation stability It is possible to realize a good magnetron.
[実施例] 次に、本発明に係る均圧環付ベーン形マグネトロンの一
実施例を添付図面に基づいて説明する。[Embodiment] Next, an embodiment of a vane type magnetron with a pressure equalizing ring according to the present invention will be described with reference to the accompanying drawings.
第1図(A),(B)は、本発明に係る均圧環付ベーン
形マグネトロンの一実施例を示す平面図、背面図であ
る。なお、第3図に示す部分と同一部分には同一参照符
号を付し、その説明を省略する。1 (A) and 1 (B) are a plan view and a rear view showing an embodiment of a vane type magnetron with a pressure equalizing ring according to the present invention. The same parts as those shown in FIG. 3 are designated by the same reference numerals, and the description thereof will be omitted.
陽極筒1の内側には中心に向け半径方向に延出する複数
の陽極片2〜19が設けられている。複数の陽極片2〜19
は同一寸法で等角度毎に放射状に配列されており、本実
施例では周波数9.5GHzのマグネトロンを得るために、陽
極片2〜19の厚さ寸法を0.4mmに設定してある。放射状
に配列された陽極片2〜19の一方の面(表面)には4つ
の均圧環30,31,32,33が設けられている。均圧環30〜33
は夫々異なる径を有し、陰極(図示せず)が位置する陽
極筒1の中心に対して同心円上に位置決めされており、
中心から第1番目の均圧環30及び第3番目の均圧環32は
1つ置きに陽極片2,4,6,8,10,12,14,16,18(以下、第1
組の陽極片という)にロウ付を以て接続されており、中
心から第2番目の均圧環31及び第4番目の均圧環33は残
りの陽極片3,5,7,9,11,13,15,17,19(以下、第2組の陽
極片という)にロウ付を以て接続されている。本実施例
では均圧環30〜33の厚さを0.2mmとしてある。Inside the anode cylinder 1, a plurality of anode pieces 2 to 19 extending in the radial direction toward the center are provided. Multiple anode pieces 2-19
Have the same size and are radially arranged at equal angles. In this embodiment, the thickness of the anode pieces 2 to 19 is set to 0.4 mm in order to obtain a magnetron having a frequency of 9.5 GHz. Four pressure equalizing rings 30, 31, 32, 33 are provided on one surface (surface) of the anode pieces 2 to 19 which are radially arranged. Pressure equalizing ring 30-33
Have different diameters and are positioned concentrically with respect to the center of the anode cylinder 1 where the cathode (not shown) is located,
The 1st pressure equalizing ring 30 and the 3rd pressure equalizing ring 32 from the center are the anode pieces 2,4,6,8,10,12,14,16,18 (although every other one)
The second equalizing ring 31 and the fourth equalizing ring 33 from the center are connected to the other positive electrode pieces 3,5,7,9,11,13,15 by brazing. , 17, 19 (hereinafter referred to as the second set of anode pieces) are connected by brazing. In this embodiment, the pressure equalizing rings 30 to 33 have a thickness of 0.2 mm.
奇数番目の均圧環30,32が接続される第1組の陽極片
は、夫々第2図(A)に示す如く、均圧環30,32がロウ
付固着されるロウ付段部30a,32aを有すると共に、奇数
番目の均圧環31,33に対して非接触とすべき逃げ溝31b,3
3bを有している。また、第2組の陽極片は、第2図
(B)に示す如く、奇数番目の均圧環30,32に対して非
接触とすべき逃げ溝30b,32bを有しており、均圧環31,33
に対するロウ付段部31a,33aを有している。The first set of anode pieces to which the odd-numbered pressure equalizing rings 30 and 32 are connected have brazing step portions 30a and 32a to which the pressure equalizing rings 30 and 32 are fixed by brazing, as shown in FIG. 2 (A). Relief grooves 31b, 3 which should have no contact with the odd-numbered pressure equalizing rings 31, 33
Has 3b. Further, as shown in FIG. 2 (B), the second set of anode pieces has escape grooves 30b and 32b which should be in non-contact with the odd-numbered pressure equalizing rings 30 and 32. , 33
It has brazing step portions 31a and 33a.
かかるマグネトロンは、組立治具に陽極筒1を置き、ロ
ウ付面を合せながら陽極片2〜19を挿入して放射線状に
配置し、それらの上にロウ付面を合せながら4つの均圧
環30〜33を同心的に配置することによって作成される。
この作成工程においては、陽極片2〜19の片面に4つの
均圧環30〜33を入念に位置決めするだけであるから、従
来に比し、製造の容易化を図ることができる。均圧環30
〜33の間隔や逃げ溝30b〜33bの隙間に形成される容量負
荷によって周波数調整が行なわれるが、4つの均圧環30
〜33が陽極片2〜19の片面に配されているので、上記間
隔及び隙間の調整作業を首尾よく行ない得る。また従来
の如く陽極片の両面に均圧環を配する場合に比べて、4
つの均圧環30〜33を以て容量負荷を分散させてあるの
で、均圧環30〜33の厚さを0.2mm程度で陽極片の厚さに
比し薄くでき、陽極片の支持力軽減に寄与する。更に、
均圧環30〜33に対する各陽極片2〜19のロウ付面はすべ
て2箇所であるから、上記支持力軽減の効果と相まっ
て、熱応力が均等化し、均圧環30〜33の熱変形などを有
効に防止でき、発振安定性を図れる。In such a magnetron, the anode cylinder 1 is placed on an assembling jig, the anode pieces 2 to 19 are inserted while aligning the brazed surfaces and arranged radially. Created by placing ~ 33 concentrically.
In this manufacturing process, the four pressure equalizing rings 30 to 33 are carefully positioned on one surface of the anode pieces 2 to 19, so that the manufacturing can be facilitated as compared with the conventional method. Pressure equalizing ring 30
The frequency adjustment is performed by the capacitive load formed in the intervals of 33 to 33 and the clearances of the escape grooves 30b to 33b.
Since .about.33 are arranged on one side of the anode pieces 2 to 19, it is possible to successfully carry out the work of adjusting the intervals and gaps. Compared with the conventional case where pressure equalizing rings are arranged on both sides of the anode piece,
Since the capacity load is distributed by two pressure equalizing rings 30 to 33, the thickness of the pressure equalizing rings 30 to 33 can be reduced to about 0.2 mm as compared with the thickness of the anode piece, which contributes to the reduction of the supporting force of the anode piece. Furthermore,
Since there are two brazing surfaces on each of the anode pieces 2 to 19 with respect to the pressure-equalizing rings 30 to 33, the thermal stress is equalized in combination with the effect of reducing the supporting force described above, and thermal deformation of the pressure-equalizing rings 30 to 33 is effective. Can be prevented, and oscillation stability can be achieved.
なお、上記実施例においては、4つの均圧環を陽極片の
片面のみに配して、高い周波数のマグネトロンを構成し
たが、4以上(6,8,10…)の偶数個の均圧環を片面に同
心的に配することによって、一層高い周波数のマグネト
ロンを構成することも可能である。In the above embodiment, four equalizing rings were arranged only on one side of the anode piece to form a high frequency magnetron, but an even number of equalizing rings of 4 or more (6,8,10 ...) Is provided on one side. It is also possible to construct a magnetron with a higher frequency by arranging them concentrically with each other.
[発明の効果] 以上説明したように、本発明に係る均圧環付ベーン形マ
グネトロンは、均圧環を4個用いながら、1つおきの陽
極片(第1組)が最内側の均圧環と最外側均圧環に接続
すると共に、残る陽極片(第2組)が内側から2番目の
均圧環と3番目の均圧環に接続して成るものではなく、
1つおきの陽極片(第1組)を奇数番目の均圧環に接続
すると共に、残る陽極片(第2組)を偶数番目の均圧環
に接続して成る点を特徴としている。従って、本願発明
は次のような独特な効果を有している。[Effects of the Invention] As described above, in the vane-type magnetron with a pressure equalizing ring according to the present invention, while using four pressure equalizing rings, every other positive electrode piece (first set) has the innermost pressure equalizing ring and the other. Not only is it connected to the outer pressure equalizing ring, but the remaining anode pieces (second set) are not connected to the second pressure equalizing ring and the third pressure equalizing ring from the inside,
It is characterized in that every other positive electrode piece (first set) is connected to the odd-numbered pressure equalizing ring, and the remaining anode pieces (second set) are connected to the even-numbered equalizing ring. Therefore, the present invention has the following unique effects.
2個又は3個の均圧環ではなく、4個以上の偶数の
均圧環を片面に配した構造であることから、周波数設定
のための容量負荷を2個,3個の場合に比して分散化させ
ることができるので、同一周波数の場合には均圧環の太
さ(幅)を細くすることができる。陽極片は中心側(陰
極側)が高温であり陽極筒側が低温となっているため、
強い温度勾配を持っている。従って、均圧環の内側の方
が外側の方に比べて遥に熱膨張が大きい。マグネトロン
の周波数変化は均圧環の幅に比例するから、熱膨張の大
きな内側の均圧環が周波数変化に優性的なる。本発明で
は、内側の均圧環の幅が小さくなっているので周波数変
化を優性的に抑制できると共に、外側に追加された均圧
環は周波数変化に劣勢的であってまた僅小幅であること
から、結果として、また実証的にも周波数変化の温度依
存特性を顕著に改善することができる。Since there is a structure in which four or more even pressure-equalizing rings are arranged on one side instead of two or three equalizing rings, the capacitive load for frequency setting is distributed compared to the case of two or three. Since the pressure equalizing ring can be made uniform, the thickness (width) of the pressure equalizing ring can be reduced in the case of the same frequency. Since the center side (cathode side) of the anode piece is hot and the anode cylinder side is cold,
Has a strong temperature gradient. Therefore, the inner side of the pressure-equalizing ring has a much larger thermal expansion than the outer side. Since the frequency change of the magnetron is proportional to the width of the pressure equalizing ring, the inner pressure equalizing ring with large thermal expansion becomes dominant in the frequency change. In the present invention, since the width of the pressure equalizing ring on the inner side is small, it is possible to suppress the frequency change dominantly, and the pressure equalizing ring added to the outside is inferior to the frequency change and is also a very small width. As a result, and empirically, it is possible to significantly improve the temperature-dependent characteristics of the frequency change.
陽極片の均圧環が接続された面側は均圧環による拘
束面となっているため、陽極筒から半径方向に延出する
複数の陽極片は自由面側が自由膨張するので拘束面側へ
撓み、陽極片全体として太鼓皮の様に片面側に膨れた状
態になる。ここで、1つおきの陽極片(第1組)が最内
側の均圧環と最外側均圧環に接続されており、残る陽極
片(第2組)が内側から2番目の均圧環と3番目の均圧
環に接続しているとすれば、第1組の陽極片の接続点は
両端に離れ過ぎであるのに対し、第2組の陽極片の中央
に近接し過ぎているので、第1組の陽極片と第2組の陽
極片とでは撓み状態が異なるため、周波数変化にバラツ
キが生じる。本発明のように、第1組の陽極片が1番目
と3番目に、第2組の陽極片が2番目と4番目にそれぞ
れ接続されている場合には、第1組の陽極片も第2組の
陽極片も接続箇所の分布が近似しているので、第1組の
陽極片と第2組の陽極片との撓み状態の差が少なくな
り、周波数変化のバラツキを抑制できる。Since the surface side of the anode piece to which the pressure equalizing ring is connected is a restraining surface due to the pressure equalizing ring, the plurality of anode pieces extending in the radial direction from the anode cylinder flex toward the restraining surface side because the free surface side expands freely. The anode piece as a whole bulges to one side like a drum skin. Here, every other positive electrode piece (first set) is connected to the innermost pressure equalizing ring and the outermost pressure equalizing ring, and the remaining positive electrode pieces (second set) are the second equalizing ring and the third from the inner side. If it is connected to the pressure equalizing ring of the first set, the connecting points of the first set of anode pieces are too far away from both ends, while they are too close to the center of the second set of anode pieces. Since the bending state is different between the anode pieces of the set and the anode pieces of the second set, variations occur in the frequency change. As in the present invention, when the first set of anode strips is connected to the first and third sides and the second set of anode strips is connected to the second and fourth sides, respectively, the first set of anode strips is also connected to the first set. Since the distribution of the connection points is similar in the two sets of anode pieces, the difference in the bending state between the first set of anode pieces and the second set of anode pieces is reduced, and variation in frequency change can be suppressed.
各陽極片の接続箇所が偶数箇所で皆等しくなってい
るので、上記、の利点と相まって、高温下における
熱応力がいずれの陽極片及び均圧環についても均等化さ
れる傾向にあり、発振安定性の良好なマグネトロンを実
現できる。Since the connection points of each anode piece are equal at all even-numbered points, combined with the above advantages, thermal stress at high temperature tends to be equalized for any anode piece and pressure equalizing ring, and oscillation stability It is possible to realize a good magnetron.
第1図(A)は、本発明に係る均圧環付ベーン形マグネ
トロンの一実施例を示す平面図である。 第1図(B)は、同実施例を示す背面図である。 第2図(A)は、同実施例における第1組の陽極片の縦
断面図である。 第2図(B)は、同実施例における第2組の陽極片の縦
断面図である。 第3図(A)は、従来の均圧環付ベーン形マグネトロン
の一例を示す平面図で、第3図(B)はその背面図であ
る。 1……陽極筒、2〜19……陽極片、2,4,6,8,10,12,14,1
6,18……第1組の陽極片、3,5,7,9,11,13,15,17,19……
第2組の陽極片、30……第1番目の均圧環、31……第2
番目の均圧環、32……第3番目の均圧環、33……第4番
目の均圧環、30a,31a,33a……ロウ付段部、30b,31b,32
b,33b……逃げ溝。FIG. 1 (A) is a plan view showing an embodiment of a vane type magnetron with a pressure equalizing ring according to the present invention. FIG. 1 (B) is a rear view showing the same embodiment. FIG. 2A is a vertical cross-sectional view of the first set of anode pieces in the example. FIG. 2B is a vertical cross-sectional view of the second set of anode pieces in the same example. FIG. 3 (A) is a plan view showing an example of a conventional vane type magnetron with a pressure equalizing ring, and FIG. 3 (B) is a rear view thereof. 1 …… Anode cylinder, 2-19 …… Anode piece, 2,4,6,8,10,12,14,1
6,18 …… 1st set of anode pieces, 3,5,7,9,11,13,15,17,19 ……
Second set of anode strips, 30 ... first pressure equalizing ring, 31 ... second
Th pressure equalizing ring, 32 …… third pressure equalizing ring, 33 …… fourth pressure equalizing ring, 30a, 31a, 33a …… brazing step, 30b, 31b, 32
b, 33b ... Escape groove.
Claims (1)
片を有する陽極筒と、該陽極筒の一方の面側において配
され、該中心に対して異なる直径で同心円の4個又はそ
れ以上の偶数個の均圧環とからなり、該中心から奇数番
目の均圧環は1つおきの陽極片に接続されていると共
に、該中心から偶数番目の均圧環は残りの陽極片に接続
されていることを特徴とする均圧環付ベーン形マグネト
ロン。1. An anode cylinder having a plurality of anode pieces extending in a radial direction toward a center, and four or more concentric circles arranged on one surface side of the anode cylinder and having different diameters with respect to the center. The above-mentioned even numbered pressure-equalizing rings are connected from the center to odd-numbered pressure-equalizing rings to every other positive electrode piece, and the even-numbered pressure-equalizing rings from the center are connected to the remaining positive electrode pieces. A vane type magnetron with a pressure equalizing ring.
Priority Applications (3)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP62144743A JPH0754669B2 (en) | 1987-06-10 | 1987-06-10 | Vane magnetron with pressure equalizing ring |
| GB8811674A GB2206991B (en) | 1987-06-10 | 1988-05-17 | Strapped vane-type magnetron |
| KR88006523A KR960011850B1 (en) | 1987-06-10 | 1988-05-31 | Strapped vane-type magnetron |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP62144743A JPH0754669B2 (en) | 1987-06-10 | 1987-06-10 | Vane magnetron with pressure equalizing ring |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS63308847A JPS63308847A (en) | 1988-12-16 |
| JPH0754669B2 true JPH0754669B2 (en) | 1995-06-07 |
Family
ID=15369328
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP62144743A Expired - Lifetime JPH0754669B2 (en) | 1987-06-10 | 1987-06-10 | Vane magnetron with pressure equalizing ring |
Country Status (3)
| Country | Link |
|---|---|
| JP (1) | JPH0754669B2 (en) |
| KR (1) | KR960011850B1 (en) |
| GB (1) | GB2206991B (en) |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| GB9723478D0 (en) | 1997-11-07 | 1998-01-07 | Eev Ltd | Magnetrons |
Family Cites Families (6)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US2808538A (en) * | 1952-10-02 | 1957-10-01 | Bell Telephone Labor Inc | Magnetron oscillator |
| GB729583A (en) * | 1952-11-18 | 1955-05-11 | British Thomson Houston Co Ltd | Improvements in and relating to magnetrons |
| US2808568A (en) * | 1954-03-31 | 1957-10-01 | Rca Corp | Magnetron |
| US3121822A (en) * | 1960-10-28 | 1964-02-18 | Gen Electric | Circuits for unimoding crossed field devices |
| US3176188A (en) * | 1960-10-28 | 1965-03-30 | Gen Electric | Mixed lines crossed fields oscillator or amplifier |
| GB2054256B (en) * | 1979-07-14 | 1983-03-30 | English Electric Valve Co Ltd | Magnetron strapping |
-
1987
- 1987-06-10 JP JP62144743A patent/JPH0754669B2/en not_active Expired - Lifetime
-
1988
- 1988-05-17 GB GB8811674A patent/GB2206991B/en not_active Expired - Lifetime
- 1988-05-31 KR KR88006523A patent/KR960011850B1/en not_active Expired - Lifetime
Also Published As
| Publication number | Publication date |
|---|---|
| GB2206991A (en) | 1989-01-18 |
| KR960011850B1 (en) | 1996-09-03 |
| GB8811674D0 (en) | 1988-06-22 |
| JPS63308847A (en) | 1988-12-16 |
| GB2206991B (en) | 1992-01-22 |
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