JPS6014533B2 - How to combine the output power of multiple oscillators - Google Patents
How to combine the output power of multiple oscillatorsInfo
- Publication number
- JPS6014533B2 JPS6014533B2 JP5200380A JP5200380A JPS6014533B2 JP S6014533 B2 JPS6014533 B2 JP S6014533B2 JP 5200380 A JP5200380 A JP 5200380A JP 5200380 A JP5200380 A JP 5200380A JP S6014533 B2 JPS6014533 B2 JP S6014533B2
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- Prior art keywords
- oscillator
- terminal
- oscillators
- output
- coupler
- Prior art date
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- Expired
Links
- 238000000034 method Methods 0.000 claims description 28
- 238000001308 synthesis method Methods 0.000 claims description 7
- 230000002194 synthesizing effect Effects 0.000 claims description 5
- 238000010168 coupling process Methods 0.000 description 35
- 238000005859 coupling reaction Methods 0.000 description 35
- 230000008878 coupling Effects 0.000 description 34
- 238000010586 diagram Methods 0.000 description 8
- 230000015572 biosynthetic process Effects 0.000 description 7
- 239000002184 metal Substances 0.000 description 7
- 229910052751 metal Inorganic materials 0.000 description 7
- 238000003786 synthesis reaction Methods 0.000 description 7
- 238000002347 injection Methods 0.000 description 4
- 239000007924 injection Substances 0.000 description 4
- 230000010355 oscillation Effects 0.000 description 4
- 238000002474 experimental method Methods 0.000 description 3
- 238000003780 insertion Methods 0.000 description 3
- 230000037431 insertion Effects 0.000 description 3
- 230000001360 synchronised effect Effects 0.000 description 3
- 239000002131 composite material Substances 0.000 description 2
- 230000007423 decrease Effects 0.000 description 2
- 201000003144 pneumothorax Diseases 0.000 description 2
- 241000972773 Aulopiformes Species 0.000 description 1
- 241000270295 Serpentes Species 0.000 description 1
- WYTGDNHDOZPMIW-RCBQFDQVSA-N alstonine Natural products C1=CC2=C3C=CC=CC3=NC2=C2N1C[C@H]1[C@H](C)OC=C(C(=O)OC)[C@H]1C2 WYTGDNHDOZPMIW-RCBQFDQVSA-N 0.000 description 1
- JBTHDAVBDKKSRW-UHFFFAOYSA-N chembl1552233 Chemical compound CC1=CC(C)=CC=C1N=NC1=C(O)C=CC2=CC=CC=C12 JBTHDAVBDKKSRW-UHFFFAOYSA-N 0.000 description 1
- 238000007796 conventional method Methods 0.000 description 1
- 230000001419 dependent effect Effects 0.000 description 1
- 229910052745 lead Inorganic materials 0.000 description 1
- 238000004519 manufacturing process Methods 0.000 description 1
- 235000019515 salmon Nutrition 0.000 description 1
Classifications
-
- H—ELECTRICITY
- H03—ELECTRONIC CIRCUITRY
- H03B—GENERATION OF OSCILLATIONS, DIRECTLY OR BY FREQUENCY-CHANGING, BY CIRCUITS EMPLOYING ACTIVE ELEMENTS WHICH OPERATE IN A NON-SWITCHING MANNER; GENERATION OF NOISE BY SUCH CIRCUITS
- H03B9/00—Generation of oscillations using transit-time effects
- H03B9/12—Generation of oscillations using transit-time effects using solid state devices, e.g. Gunn-effect devices
- H03B9/14—Generation of oscillations using transit-time effects using solid state devices, e.g. Gunn-effect devices and elements comprising distributed inductance and capacitance
- H03B9/143—Generation of oscillations using transit-time effects using solid state devices, e.g. Gunn-effect devices and elements comprising distributed inductance and capacitance using more than one solid state device
Landscapes
- Stabilization Of Oscillater, Synchronisation, Frequency Synthesizers (AREA)
Description
【発明の詳細な説明】
本発明は4端子父旧90o結合器を用いた複数発振器の
出力電力合成方法に関する。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a method for combining the output power of a plurality of oscillators using a four-terminal father-to-back 90o coupler.
複数のマイクロ波またはミリ波発振器等の出力を同相で
合成する技術が数多〈提案されている。Many techniques have been proposed for synthesizing the outputs of multiple microwave or millimeter wave oscillators in the same phase.
4端子3旧9び結合器を用いる方法として結合器の第1
の端子に受動インピーダンスを接続し第2、第3の端子
にそれぞれ合成すべき発振器の出力を結合し、第4の様
子に合成出力を得る方法を挙げることができる。As a method using a 4-terminal 3-9 coupler, the first coupler
A fourth method is to connect a passive impedance to the terminal of the oscillator and couple the outputs of the oscillators to be synthesized to the second and third terminals, respectively, to obtain the synthesized output.
この方法を実施する回路では、最適調整された場合、第
1の端子に出る電力はほぼゼロとなり、極めて微弱とな
る。In a circuit that implements this method, when optimally adjusted, the power output to the first terminal is almost zero, and is extremely weak.
この微弱な電力を受動インピーダンスで反射し、2等分
して注入同期信号として各発振器に注入するのであるか
ら注入同期信号が弱く、回路の同期動作の安定性に問題
がある。また前述の2発振器電力合成法をくり返し使っ
た2N発振器出力電力合成方法も知られている。しかし
この方法は、結合段数Nを増すと結合器のもつ損失のた
めに電力合成効率が低下する欠点があった。また従来、
発振器を従属あるいは直列に接続して発振器の出力電力
を合成する方法にはサーキュレータを用いる方法と結合
度が各段毎に異つた値の方向性結合器を用いる方法が知
られている。Since this weak power is reflected by a passive impedance, divided into two equal parts, and injected into each oscillator as an injection locking signal, the injection locking signal is weak and there is a problem in the stability of the circuit's locking operation. Also known is a 2N oscillator output power synthesis method that repeatedly uses the two-oscillator power synthesis method described above. However, this method has a drawback that as the number of coupling stages N increases, the power combining efficiency decreases due to the loss of the coupler. Also, conventionally,
Known methods for combining oscillator output power by connecting oscillators in a dependent or series manner include a method using a circulator and a method using a directional coupler in which the degree of coupling is different for each stage.
いずれの方法もサーキュレータや方向性結合器の損失の
ために、結合段数の増加と共に電力合成効率が急速に低
下する欠点があった。本発明の目的は前述した諸問題を
すべて解決することができる新規な複数発振器の出力電
力合成方法を提供することにある。Both methods have the disadvantage that the power combining efficiency rapidly decreases as the number of coupling stages increases due to losses in the circulators and directional couplers. SUMMARY OF THE INVENTION An object of the present invention is to provide a novel method for combining the output power of multiple oscillators, which can solve all of the above-mentioned problems.
前記目的を達成するために本発明による複数発振器の出
力合成方法は、4端子父旧900結合器の第1、第2、
第3の端子に相互に注入同期可能な関係にある略同程度
の出力の発振器出力を接続し、第4の端子から前記各発
振器出力の和に相当する合成された出力を得るように構
成されている。To achieve the above object, the present invention provides a method for combining the outputs of multiple oscillators by combining the first, second,
The third terminal is configured to connect oscillator outputs having substantially the same level of output that can be mutually injection-locked, and to obtain a combined output corresponding to the sum of the respective oscillator outputs from the fourth terminal. ing.
上記構成によれば、従来方法に比較して、注入同期が確
実であり効率的な電力合成が可能になる。According to the above configuration, compared to the conventional method, injection locking is reliable and efficient power synthesis is possible.
さらに、この3発振器出力合成の基本概念を拡大するこ
とにより、多数個の発振器出力の合成が可能となる。後
述するように調整も容易であり、容易に工業的に応用が
可能となる。なお本発明において発振器という用語は、
要素発振器と呼ぶ個々の発振器およびそれ等の出力を合
成した出力を発生する装置を含めた意味で用いることに
する。以下図面等を参照して本発明方法を、その原理、
および実施例の順に説明する。Furthermore, by expanding the basic concept of combining the outputs of three oscillators, it becomes possible to combine the outputs of a large number of oscillators. As will be described later, adjustment is easy, and industrial application is easily possible. Note that in the present invention, the term oscillator is
The term ``element oscillator'' is used to include individual oscillators called element oscillators and devices that generate an output that is a combination of their outputs. The method of the present invention will be described below with reference to the drawings, its principles, etc.
and examples will be explained in order.
第1図は3発振器出力合成方法の原理を説明するための
概略図である。FIG. 1 is a schematic diagram for explaining the principle of a three-oscillator output synthesis method.
第1図において、発振器aの発振周波数をねとし、その
出力電力をPaとする。電力Paは結合器の端子1から
結合器に入り、$旧900結合器Aの特性に従い、2等
分されてPa/2が端子2に、Pa/2が端子3に出、
しかも端子3に出る電力波の位相は端子2に出る電力波
の位相より90o遅れる。端子2と端子3に出た電力は
、それぞれ発振器aと発振器bに注入される。端子2に
おいて、発振器bの自走発振周波数8bが岬こ十分近い
場合、同期引込現象がおき、発振器aと発振器bは単一
周波数fで同期発振する。In FIG. 1, the oscillation frequency of oscillator a is assumed to be 0, and the output power thereof is assumed to be Pa. Power Pa enters the coupler from terminal 1 of the coupler, and according to the characteristics of the old $900 coupler A, it is divided into two, Pa/2 goes out to terminal 2, Pa/2 goes out to terminal 3,
Moreover, the phase of the power wave output from terminal 3 lags the phase of the power wave output from terminal 2 by 90 degrees. The power output to terminals 2 and 3 is injected into oscillators a and oscillators b, respectively. At terminal 2, when the free-running oscillation frequency 8b of oscillator b is sufficiently close to the cape, a synchronous pull-in phenomenon occurs, and oscillators a and oscillators oscillate synchronously at a single frequency f.
同期引込状態で動作している発振器bの出力はfの抗か
ら離調周波数f−fbに依存し、ある機認周波数で最大
値をとり、その値はほぼ発振器bの目走発振器の出力電
力Pbと注入電力Pa/2を加算した値となる。端子3
には発振器bと似た特性をもつ発振器cが接続されてい
るため、前述の現象と同じ現象が90oの位相遅れを伴
って様子3でもおきる。The output of oscillator b operating in the synchronous pull-in state depends on the detuning frequency f - fb from the resistance of f, and takes a maximum value at a certain oscillator frequency, and that value is approximately equal to the output power of the running oscillator of oscillator b. The value is the sum of Pb and the injection power Pa/2. terminal 3
Since oscillator c having characteristics similar to oscillator b is connected to oscillator b, the same phenomenon as described above occurs in case 3 with a phase delay of 90°.
その結果、結合器Aには端子2からPb十Pa/2の電
力を運ぶ鰭力波が、また端子3からPc+Pa/2の電
力を運ぶ電力波が9び の位相遅れをもって送り込まれ
る。ここで、Pcは発振器cの自走発振時の出力電力で
ある。発振器bと発振器cは似た特性をもつからPbニ
Pcである。これらの電力波は、それぞれ、前述の3旧
90o結合器の特性に従って、端子1と端子4へ送り出
される。端子1においては、端子2と端子3から送り込
まれた電力波の位相は1800の差をもち、互いに相殺
されて発振器aへ逆注入される電力はゼロとなる。一方
「端子4においては、端子2と端子3から送り込まれた
電力波は同相で加算され、負荷dへPa+Pb十PCに
近い値の合成電力が供給される。以上説明した本発明に
よる基本的な方法は多数の発振器の出力電力合成に拡張
できる三つの方法を示す。As a result, a fin force wave carrying a power of Pb+Pa/2 is sent from the terminal 2 to the coupler A, and a power wave carrying a power of Pc+Pa/2 is sent from the terminal 3 with a phase delay of 9 degrees. Here, Pc is the output power of the oscillator c during free-running oscillation. Since oscillators b and oscillators c have similar characteristics, they are Pb and Pc. These power waves are sent to terminals 1 and 4, respectively, according to the characteristics of the three old 90o couplers described above. At terminal 1, the phases of the power waves sent from terminals 2 and 3 have a difference of 1800 degrees, and they cancel each other out, so that the power injected back into the oscillator a becomes zero. On the other hand, at terminal 4, the power waves sent from terminals 2 and 3 are added in phase, and a composite power of a value close to Pa + Pb + PC is supplied to load d. The method presents three methods that can be extended to output power combination of multiple oscillators.
第一の方法は、第1図の発振器a,bycをそれぞれ次
段の3発振器結合回路で置き換える方法でN段の場合、
3N個発振器の出力を(3N−1)/2個の結合器によ
って電力合成できる。多=9発振器結合回路を第2図に
示す。第2図において、21〜29は電力合成される発
振器、20は負荷、A〜Dは結合器である。第二の方法
は第1図の発振器aを次段の3発振器結合回路で置き換
える方法で、N段の場合が十1発振器の出力をNコの結
合器によって電力合成できる。The first method is to replace oscillators a and byc in Figure 1 with three oscillator coupling circuits in the next stage, and in the case of N stages,
The outputs of 3N oscillators can be combined in power by (3N-1)/2 couplers. A multi=9 oscillator coupling circuit is shown in FIG. In FIG. 2, 21 to 29 are oscillators whose power is combined, 20 is a load, and A to D are couplers. The second method is to replace oscillator a in FIG. 1 with a three-oscillator coupling circuit in the next stage, and in the case of N stages, the outputs of eleven oscillators can be combined in power by N couplers.
2×4十1=9発振器結合回路を第3図に示す。A 2×41=9 oscillator coupling circuit is shown in FIG.
第3図で31〜39は発振器、30は負荷、A〜Dは結
合器である。第三の方法は第3図のび十1発振器結合回
路から発振器32と負荷30を除いた州発振器結合回路
M個をM分岐電力分配・合成器を介してマスター発振器
と負荷に接続して洲M+1発振器結合回路を構成する方
法である。In FIG. 3, 31 to 39 are oscillators, 30 is a load, and A to D are couplers. The third method is to connect M state oscillator coupling circuits, which are obtained by removing the oscillator 32 and load 30 from the Nobi 11 oscillator coupling circuit shown in FIG. This is a method of configuring an oscillator coupling circuit.
N=4、M=2の場合の2×4×2十1=17発振器結
合回路を第4図に示す。第4図で41と42は2×4=
8発振器結合回路、43と44は2分岐電力分配・合成
器、45はマスター発振器、46は負荷、47と48は
無反射整合終機器を表す。次に前記各方法を実施する具
体的構成を順次説明する。FIG. 4 shows a 2×4×21=17 oscillator coupling circuit in the case of N=4 and M=2. In Figure 4, 41 and 42 are 2 x 4 =
8 oscillator coupling circuits, 43 and 44 are two-branch power dividers/combiners, 45 is a master oscillator, 46 is a load, and 47 and 48 are non-reflection matching terminal devices. Next, specific configurations for implementing each of the above methods will be sequentially explained.
第5図は本発明方法で用いる結合器の一例であるショー
トスロット結合器の干既念を示す斜視図である。第5図
において51と52は方形導波管、53は共通狭壁を除
去して形成された結合窓である。ショートスロット結合
器は、結合回路を平面状に構成するに適した構造をもち
、構造が簡単で製作が容易であるばかりでなく、線路長
が短く低損失で広帯域特性をもち、本発明の電力合成回
路の結合器として適している。1個のショートスロット
結合器で3個の蛇Hz帯ガン発振器を結合した3発振器
結合回路の例を第6図に示す。FIG. 5 is a perspective view showing the state of a short slot coupler, which is an example of a coupler used in the method of the present invention. In FIG. 5, 51 and 52 are rectangular waveguides, and 53 is a coupling window formed by removing a common narrow wall. The short slot coupler has a structure suitable for configuring a coupling circuit in a planar shape, and not only has a simple structure and is easy to manufacture, but also has a short line length, low loss, and broadband characteristics. Suitable as a combiner for synthetic circuits. FIG. 6 shows an example of a three-oscillator coupling circuit in which three serpentine Hz band Gunn oscillators are coupled by one short slot coupler.
第6図では61は内寸が22.劫岬×10.2側の方形
導波管を示す。62は結合回路出力端子の導波管フラン
ジ、63は発振器部と結合器の結合窓の部分との接続フ
ランジ、64は結合窓、65a,65b,65c、はガ
ンダイオード装着用金属ポスト、66a,66b,66
cは直流バイアス端子兼用の金属ポスト、67a,67
b,67cはガンダイオード、68a,68b,68c
は導波管空胴の同調調整用誘電体棒を表す。In Figure 6, 61 has an inner dimension of 22. The rectangular waveguide on the Komisaki×10.2 side is shown. 62 is a waveguide flange of the coupling circuit output terminal, 63 is a connection flange between the oscillator section and the coupling window portion of the coupler, 64 is a coupling window, 65a, 65b, 65c are metal posts for mounting Gunn diodes, 66a, 66b, 66
c is a metal post that also serves as a DC bias terminal, 67a, 67
b, 67c are Gunn diodes, 68a, 68b, 68c
represents a dielectric rod for tuning the waveguide cavity.
調整時および使用時には、出力端子を単向管を介して負
荷に接続する。回路調整は次の手順で行なう。During adjustment and use, the output terminal is connected to the load via a unidirectional tube. Perform circuit adjustment as follows.
まず、発振器aだけを動作させ、ねが所望の周波数fに
近い値となるよう誘電体棒68aの挿入長を調整する。
次に、発振器bと発振器cを動作に加え、結合回路の動
作が単一周波数fの同期発振状態で、かつ、出力が最大
となるように誘電体榛68bと68cの挿入長を交互に
くり返し調整すれば、Pa十Pb+Pcに近い値の合成
出力電力が動作周波数fで得られる。第6図の構造の試
作回路に虹世帯のガンダィオードを装着し、fを973
3M批に設定して行なった電力合成実験5例の結果を発
明の詳細な説明の末尾に表1として示してある。表1中
、Pa,Pb,Pcは発振器a,b,c、を独立にfで
目走発振させた時に同一負荷に供尊信する電力(仇W)
、Pは合成出力電力(肌W)、りはPり=Pa+Pb+
PCX100(%)
で定義された電力合成効率を表わす。First, only the oscillator a is operated, and the insertion length of the dielectric rod 68a is adjusted so that the frequency becomes close to the desired frequency f.
Next, oscillators b and oscillators c are added to the operation, and the insertion lengths of the dielectric bars 68b and 68c are alternately repeated so that the operation of the coupling circuit is in a synchronous oscillation state with a single frequency f and the output is maximized. If adjusted, a composite output power having a value close to Pa+Pb+Pc can be obtained at the operating frequency f. A Niji household gun diode was installed on the prototype circuit with the structure shown in Figure 6, and f was set to 973.
The results of five power synthesis experiments conducted using the 3M standard settings are shown in Table 1 at the end of the detailed description of the invention. In Table 1, Pa, Pb, and Pc are the power (W) supplied to the same load when oscillators a, b, and c are independently oscillated at f.
, P is the combined output power (skin W), and P = Pa + Pb +
Represents power combining efficiency defined as PCX100 (%).
いずれの例でも、ほぼ100%の電力合成効率が得られ
ている。また各発振器の離調周波数△fi=fi−f、
i=a、b、cの値も示してある。結合窓の中央に容量
性ビスを挿入し結合器の位相角が正確に9ぴとなるよう
にその挿入長を調整す机よ、△ねニ0および△fb三△
にの結果が得られると考えられる。第7図は多=9発振
器結合回路の実施例を示す平面構造説明図である。In both examples, power synthesis efficiency of approximately 100% is obtained. Also, the detuning frequency of each oscillator △fi=fi−f,
The values of i=a, b, c are also shown. Insert a capacitive screw in the center of the coupling window and adjust its insertion length so that the phase angle of the coupler is exactly 9 pins.
It is thought that the following results can be obtained. FIG. 7 is a planar structural explanatory diagram showing an embodiment of a multi=9 oscillator coupling circuit.
発振器の構造は第6図に示したものと同様で、蛇世帯ガ
ンダィオードを使用している。第7図で71は方形導波
管、72は結合回路出力様子導波管フランジ、73は結
合窓、74はガンダイオード装着用金属ポスト、75は
導波管空眼同調調整用誘電体棒を表わす。この試作回路
を用いたf=962瓜MHzにおける電力合成実験で、
鰍.4%の電力合成効率(194mWの合成出力)が得
られている。第8図は2×4十1=9の発振器結合回路
の一例を示し、上から見た平面構造説明図である。The structure of the oscillator is similar to that shown in FIG. 6, using a snake diode. In Fig. 7, 71 is a rectangular waveguide, 72 is a coupling circuit output waveguide flange, 73 is a coupling window, 74 is a metal post for mounting a Gunn diode, and 75 is a dielectric rod for adjusting waveguide air-eye tuning. represent. In a power synthesis experiment at f = 962 MHz using this prototype circuit,
Salmon. A power combining efficiency of 4% (combined output of 194 mW) is obtained. FIG. 8 shows an example of a 2×41=9 oscillator coupling circuit, and is an explanatory diagram of the planar structure seen from above.
発振器の構造は第5図に示したものと同様で、的世帯ガ
ンダィオードを使用している。第8図で81は方形導波
管、82は結合回路出力端子導波管フランジ、83は発
振器部と結合器部の接続フランジ、84は結合窓、85
は結合器の位相角を9ぴに合わせるための調整用容量性
ビス、86はガンダィオード装着用金属ポスト、87は
導波管空朝岡同調調整用誘電体棒を表わす。この試作回
路を用いたf=961仰けHzにおける電力合成実験で
、95.3%の蟹力合成効率(182机Wの合成出力)
が得られている。なお、前述の実施例では、結合器とし
て全てショートスロット結合器を用いたが、4関口をも
ち、結合度紅B、共雛端子出力間の位相差90oの結合
器には種々ある。そのうち次の名称の結合器が本発明の
結合回路の結合器として、特に有用であると考えられる
。有用この順に【11 ショートスロット結合器(方形
導波管狭面ショートスロット結合器、別名RjWet結
合器)■ ストリップ線×旧方向性結合器‘31 広面
結合器(方形導波管広面ショートスロット結合器)‘4
} 多結合孔型筑B方向性結合器(方形導波管広面型及
び狭面型)また、前述の実施例では、発振器として、1
つの発振器空胸中に1個のガンダィオードを装着した1
空胴単素子型の発振器を用いたが、1空眼中に複数の素
子を装着した1空且同複素子型の発振器の出力電力合成
にも本発明は適用できる。The structure of the oscillator is similar to that shown in FIG. 5, using a standard Gun diode. In FIG. 8, 81 is a rectangular waveguide, 82 is a coupling circuit output terminal waveguide flange, 83 is a connecting flange between the oscillator section and the coupler section, 84 is a coupling window, and 85 is a coupling circuit output terminal waveguide flange.
Reference numeral 86 represents a capacitive screw for adjustment to adjust the phase angle of the coupler to 9 pins, 86 represents a metal post for mounting a Gunn diode, and 87 represents a dielectric rod for adjusting the waveguide cavity Asaoka tuning. In a power synthesis experiment using this prototype circuit at f = 961 Hz, a power synthesis efficiency of 95.3% (combined output of 182 W) was obtained.
is obtained. In the above-mentioned embodiments, all short slot couplers were used as couplers, but there are various types of couplers that have four gates, a coupling degree of red B, and a phase difference of 90 degrees between outputs of common terminals. Among them, the couplers with the following names are considered to be particularly useful as couplers in the coupling circuit of the present invention. Useful in this order: [11 Short slot coupler (rectangular waveguide narrow-surface short slot coupler, also known as RjWet coupler) ■ Strip line x old directional coupler '31 Wide-area coupler (rectangular waveguide wide-surface short slot coupler) )'4
} Multi-coupling hole type Chiku B directional coupler (rectangular waveguide wide surface type and narrow surface type) In addition, in the above-mentioned embodiment, as an oscillator, one
1 with 1 gun diode installed in 2 oscillator pneumothorax
Although a cavity single element type oscillator is used, the present invention can also be applied to output power synthesis of a single cavity complex element type oscillator in which a plurality of elements are mounted in one cavity.
この場合、電力合成される能動素子の数がいちじるしく
増すという利点に加えて、ある空胸中の1素子の故障が
全体の合成出力電力へ与える影響を軽減できるという利
点もある。表1
f=9733MHzIn this case, in addition to the advantage that the number of active elements whose power is combined increases significantly, there is also the advantage that the influence of a failure of one element in a certain pneumothorax on the overall combined output power can be reduced. Table 1 f=9733MHz
第1図は本発明による3発振器出力合成法の原理を説明
するための回路図、第2図は本発明による結合段数N段
の3N発振器出力合成法の原理を説明するための回路図
、第3図および第4図は本発明による(州+1)および
(州M十1)発振器出力合成方法の原理を説明するため
の回路図である。
第5図は本発明方法を実施するための結合器の構成例の
一つであるショートスロット結合器の概念を示す斜視図
、第6図は3発振器出力合成方法の実施例を示す図、第
7図は3N個発振器出力合成方法の実施例を示す図、第
8図は(州+1)個発振器の出力合成方法の実施例を示
す図である。a,b,c:発振器、d:負荷、1,2,
3,4:結合器の第1、第2、第3および第4の端子、
A,B,C,D:4端子幻B90o結合器、21,22
,・…・・29:(要素)発振器 20(d)負荷、3
1,32,…・・・39:(要素)発振器30(d)負
荷、41,42:2×4発振器結合回路、43,44:
2分岐電力分配合成器、45:マスター発振器、46:
負荷、47,48:無反射整合終端器、51,52:方
形導波管、53:結合窓、61:方形導波管、62,6
3:フランジ、64:結合窓、65a,65b,65c
:ガンダィオード装着用金属ポスト、67a,67b,
67c:ガンダイオード(要素発振器)、68a,68
b,68c:同調調整用誘電体棒、71:方形導波管、
72:フランジ、73:結合窓、74:ガンダィオ−ド
装着用金属ポスト、75:調整用誘電体綾、81:方形
導波管、82,83:フランジ、84:結合窓、85:
調整用容量性ビス、86:ガンダィオード装着用金属ポ
スト、87:調整用誘電体榛。
第1図
第2図
第3図
第4図
第5図
第6図
第7図
第8図FIG. 1 is a circuit diagram for explaining the principle of the 3-oscillator output synthesis method according to the present invention, and FIG. 2 is a circuit diagram for explaining the principle of the 3N oscillator output synthesis method with N coupling stages according to the present invention. 3 and 4 are circuit diagrams for explaining the principle of the (state+1) and (state M11) oscillator output synthesis method according to the present invention. FIG. 5 is a perspective view showing the concept of a short slot coupler which is one of the configuration examples of a coupler for carrying out the method of the present invention, FIG. FIG. 7 is a diagram showing an embodiment of a method for synthesizing the outputs of 3N oscillators, and FIG. 8 is a diagram showing an embodiment of the method of synthesizing the outputs of (state+1) oscillators. a, b, c: oscillator, d: load, 1, 2,
3, 4: first, second, third and fourth terminals of the coupler,
A, B, C, D: 4-terminal phantom B90o coupler, 21, 22
,...29: (Element) Oscillator 20 (d) Load, 3
1, 32,...39: (Element) Oscillator 30 (d) Load, 41, 42: 2x4 oscillator coupling circuit, 43, 44:
2-branch power distribution combiner, 45: Master oscillator, 46:
Load, 47, 48: Non-reflection matched terminator, 51, 52: Rectangular waveguide, 53: Coupling window, 61: Rectangular waveguide, 62, 6
3: Flange, 64: Combined window, 65a, 65b, 65c
: Metal post for mounting gun diode, 67a, 67b,
67c: Gunn diode (element oscillator), 68a, 68
b, 68c: dielectric rod for tuning adjustment, 71: rectangular waveguide,
72: Flange, 73: Coupling window, 74: Metal post for mounting gun diode, 75: Dielectric twill for adjustment, 81: Rectangular waveguide, 82, 83: Flange, 84: Coupling window, 85:
Capacitive screw for adjustment, 86: Metal post for mounting gun diode, 87: Dielectric bar for adjustment. Figure 1 Figure 2 Figure 3 Figure 4 Figure 5 Figure 6 Figure 7 Figure 8
Claims (1)
子に相互に注入同期可能な関係にある略同程度の出力の
発振器出力を接続し、第4の端子から前記各発振器出力
の和に相当する合成された出力を得る複数発振器の出力
電力合成方法。 2 前記結合器の第1、第2、第3の端子のうち、少な
くとも1個の端子には前記第1項記載の方法で合成され
た発振器出力が接続される第1項記載の複数発振器の出
力電力合成方法。 3 前記第1項記載の結合器の第1、第2、第3の端子
は、すべて下位の結合器の第4端子からの最終被合成出
力が接続され、前記下位の結合器の第1、第2、第3の
端子にはさらに下位の結合器の第4の端子からの被合成
出力が接続され、この接続をさらに下位の結合器につい
て繰り返し、3^N個の要素発振器の出力電力を合成す
る第1項記載の複数発振器の出力電力合成方法。 4 前記第1項記載の結合器の第1、第2、第3端子中
の第1の端子につき、下位の結合器の第4端子からの出
力電力を接続し、他の2端子については要素発振器の出
力を接続し、前記下位の結合器の第1、第2、第3の端
子中の第1の端子につきさらに下位の結合器の第4端子
からの出力電力を接続し、他の2端子につき発振器の出
力を接続するという繰り返し接続により(2N+1)個
の要素発振器の出力電力を合成する、第1項記載の複数
発振器の出力電力合成方法。[Claims] 1. Oscillator outputs of approximately the same level of output that are mutually injection-lockable are connected to the first, second, and third terminals of a four-terminal 3 dB 90° coupler, and the fourth terminal A method for synthesizing the output power of a plurality of oscillators to obtain a synthesized output corresponding to the sum of the outputs of the respective oscillators. 2. The plurality of oscillators according to item 1, wherein at least one terminal among the first, second, and third terminals of the coupler is connected to the oscillator outputs synthesized by the method described in item 1 above. Output power synthesis method. 3. The first, second, and third terminals of the coupler described in item 1 above are all connected to the final combined output from the fourth terminal of the lower coupler, and the first, The combined output from the fourth terminal of the lower coupler is connected to the second and third terminals, and this connection is repeated for the lower coupler to calculate the output power of the 3^N element oscillators. 2. A method for combining output powers of a plurality of oscillators according to claim 1. 4 Connect the output power from the fourth terminal of the lower coupler to the first terminal among the first, second, and third terminals of the coupler described in item 1 above, and connect the other two terminals to the element. The output of the oscillator is connected, and the output power from the fourth terminal of the further lower coupler is connected to the first terminal among the first, second, and third terminals of the lower coupler, and the output power from the fourth terminal of the lower coupler is connected. 2. The method for synthesizing the output power of a plurality of oscillators according to claim 1, wherein the output powers of (2N+1) element oscillators are synthesized by repeatedly connecting the outputs of the oscillators for each terminal.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP5200380A JPS6014533B2 (en) | 1980-04-18 | 1980-04-18 | How to combine the output power of multiple oscillators |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP5200380A JPS6014533B2 (en) | 1980-04-18 | 1980-04-18 | How to combine the output power of multiple oscillators |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS56147524A JPS56147524A (en) | 1981-11-16 |
| JPS6014533B2 true JPS6014533B2 (en) | 1985-04-13 |
Family
ID=12902640
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP5200380A Expired JPS6014533B2 (en) | 1980-04-18 | 1980-04-18 | How to combine the output power of multiple oscillators |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS6014533B2 (en) |
Families Citing this family (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS5852043U (en) * | 1981-10-02 | 1983-04-08 | 株式会社ユ−シン | Hazard warning lamp lighting device |
| JP5634343B2 (en) * | 2011-07-05 | 2014-12-03 | 三菱電機株式会社 | Injection-locked oscillator |
-
1980
- 1980-04-18 JP JP5200380A patent/JPS6014533B2/en not_active Expired
Also Published As
| Publication number | Publication date |
|---|---|
| JPS56147524A (en) | 1981-11-16 |
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