JPS5853767Y2 - power combiner - Google Patents
power combinerInfo
- Publication number
- JPS5853767Y2 JPS5853767Y2 JP12306978U JP12306978U JPS5853767Y2 JP S5853767 Y2 JPS5853767 Y2 JP S5853767Y2 JP 12306978 U JP12306978 U JP 12306978U JP 12306978 U JP12306978 U JP 12306978U JP S5853767 Y2 JPS5853767 Y2 JP S5853767Y2
- Authority
- JP
- Japan
- Prior art keywords
- characteristic impedance
- input
- transmission line
- output
- power
- 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
Links
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- Waveguides (AREA)
Description
【考案の詳細な説明】
本考案は通信用高周波電力合成器に関し、特に3個の入
力電力を合成する電力合成器に関する。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a high frequency power combiner for communication, and more particularly to a power combiner that combines three input powers.
従来、この種の電力合成器は、第1図及び第2図に示す
ような回路で、プリント基板上にスト、リンプラインを
形成したものであったが、各入力端子間の回り込みを防
止する目的で用いられている抵抗器は合成電力に比例し
で耐電力が大きい物を必、要とした。Conventionally, this type of power combiner has a circuit as shown in Figures 1 and 2, with struts and limp lines formed on a printed circuit board, but this type of power combiner is designed to prevent wrap-around between input terminals. The resistors used for this purpose needed to be proportional to the combined power and had a large withstand power.
しかし耐電力の大きい抵抗器は放熱効果を持たせる必要
上、接地面との間に絶縁板を介して抵抗素子を配置させ
る構造となり抵抗素子と接地面とで静電容量が形成され
、高周波電流が抵抗素子を介して接地面に流れ込み損失
となる欠点があった。However, resistors with high power resistance need to have a heat dissipation effect, so the structure is such that the resistance element is placed between the ground plane and an insulating plate, and capacitance is formed between the resistance element and the ground plane, and high-frequency current However, there was a drawback in that this flowed into the ground plane through the resistive element, resulting in loss.
第1図について説明すると、第1図はウィルキンソン型
の合成器で、1,2.3は入力端子、4は出力端子、8
,9.10は抵抗器、18は4分の1波長の伝送線路で
ある。To explain Fig. 1, Fig. 1 is a Wilkinson type synthesizer, 1, 2.3 are input terminals, 4 is an output terminal, 8
, 9.10 is a resistor, and 18 is a quarter wavelength transmission line.
周知の如く入出力インピーダンスをZ。As is well known, the input and output impedance is Z.
とすると伝送線路18の特性インピーダンスはr行へ、
抵抗器8゜9.100抵抗値はZoであり、入力端子1
のみ電力が印加された場合は抵抗器9に入力の9分の4
の電力が消費され抵抗器8と10には、それぞれ入力の
9分の1の電力が消費される。Then, the characteristic impedance of the transmission line 18 is to the r row,
Resistor 8゜9.100 resistance value is Zo, input terminal 1
When only power is applied, resistor 9 has 4/9 of the input power.
, and resistors 8 and 10 each consume one-ninth of the input power.
故に抵抗器はその電力に耐える物が必要である。Therefore, the resistor must be able to withstand that amount of power.
又、3個の入力端子に電力が印加され入力端子1,2.
3の箇所で、同電位、同相となるようにすれば、各抵抗
器には電流が流れないはずであるが3個の入力端子の入
力電力や位相が変れば各抵抗器に電流が流れてしまう。Also, power is applied to three input terminals, input terminals 1, 2 .
If the points 3 are at the same potential and phase, no current should flow through each resistor, but if the input power or phase of the three input terminals changes, current will flow through each resistor. Put it away.
また耐電力の大きな抵抗器は第3図に示す如く放熱を良
くした物を用いる必要がある。Furthermore, as shown in FIG. 3, it is necessary to use a resistor with good heat dissipation as shown in FIG.
第4図は第3図に示した抵抗器の側面図である。FIG. 4 is a side view of the resistor shown in FIG. 3.
この抵抗器は、抵抗素子23、絶縁板24、放熱板25
および入出力端子26を備えた構造の物で放熱板はきよ
う体等に接地し熱放散を良くして使用される。This resistor includes a resistance element 23, an insulating plate 24, and a heat sink 25.
It has a structure that includes an input/output terminal 26, and the heat dissipation plate is grounded to a body or the like to improve heat dissipation.
このため、抵抗素子と接地間に静電容量が形成され、耐
電力が大きい物はど、抵抗素子の面積が大きくなるので
静電容量も大となる。For this reason, a capacitance is formed between the resistive element and the ground, and the higher the withstand power, the larger the area of the resistive element, and the larger the capacitance.
また、第2図は端子1,2に供給される電力をまず合成
し、それから更に端子3に供給される電力を合成する電
力合成器である、同図で19,20゜21.22はτ波
長の伝送線路、11,19.12は抵抗器である。Also, Figure 2 shows a power combiner that first combines the power supplied to terminals 1 and 2, and then combines the power supplied to terminal 3. In the figure, 19,20°21.22 is τ Wavelength transmission lines 11, 19, and 12 are resistors.
本考案の目的は耐電力の小さい抵抗器を用い、しかも前
述の欠点を改良した電力合成器を提供することである。The object of the present invention is to provide a power combiner that uses resistors with low power resistance and that improves the above-mentioned drawbacks.
本考案によれば、第一の入力端子1に印加された電力を
ウィルキンソン型の分配回路で分配したのち第二および
第三の入力端子2,3に印加された電力とそれぞれウィ
ルキンソン型の合成回路で合成し、更にこれらをウィル
キンソン型の合成回路で合成することにより第1図の構
成より約5分の2又、第2図の構成より2分のlの耐電
力を有する抵抗器の使用が可能となった電力合成器が得
られる。According to the present invention, the power applied to the first input terminal 1 is distributed by a Wilkinson type distribution circuit, and then the power applied to the second and third input terminals 2 and 3 is combined with the Wilkinson type combining circuit. By further composing these using a Wilkinson-type synthesis circuit, it is possible to use a resistor with a power resistance that is approximately two-fifths that of the configuration shown in Figure 1 and one-half that of the configuration shown in Figure 2. A power combiner that has become possible is obtained.
次に本考案の一実施例を示した図面を参照して本考案を
詳細に説明する。Next, the present invention will be described in detail with reference to the drawings showing an embodiment of the present invention.
第5図は本考案の一実施例を示した図で入力端子1から
の電力は2つに分割され、分割された電力はそれぞれ端
子2,3からの電力と合成される。FIG. 5 is a diagram showing an embodiment of the present invention, in which power from input terminal 1 is divided into two, and the divided power is combined with power from terminals 2 and 3, respectively.
それぞれ合成された電力は最終的に)波長線路17で合
成され、出力端子4から出力される。The respective combined powers are finally combined in the wavelength line 17 and output from the output terminal 4.
ここで13,14,15゜16はτ波長線路であり、5
,6.7は抵抗器である。Here, 13, 14, 15°16 are τ wavelength lines, and 5
, 6.7 is a resistor.
表1は入出力インピーダンスzoとした場合の第1図、
第2図及び第5図の各伝送線路の特性インピーダンスと
各抵抗器の抵抗値を示している。Table 1 shows Figure 1 when the input/output impedance is zo,
The characteristic impedance of each transmission line and the resistance value of each resistor in FIGS. 2 and 5 are shown.
次に表2は各入力電力を300Wとし、3つの入力端子
の入力の有無によって各抵抗器の2゜当りの消費電力を
示す。Next, Table 2 shows the power consumption per 2° of each resistor depending on the presence or absence of input from the three input terminals, assuming that each input power is 300W.
本考案は、以上説明したように、第5図のように構成す
ることにより耐電力の小さな抵抗器の使用が可能になっ
たとともに損失の少ない合成器を製作出来る。As explained above, in the present invention, by configuring as shown in FIG. 5, it is possible to use a resistor with low power resistance, and it is also possible to manufacture a combiner with low loss.
表−2より本考案の回路が耐電力のより小さな抵抗器の
使用が可能である。Table 2 shows that the circuit of the present invention allows the use of resistors with smaller power resistance.
第1図及び第2図は従来の回路図を示す図、第3図は抵
抗器の平面図、第4図は第3図に示した抵抗器の側面図
、第5図は本考案の一実施例を示す図、
図において、1,2,3・・・・・・入力端子、4・・
・・・・出力端子、5,6,7,8,9,10,11
。
12・・・・・・抵抗器、13,14,15.16,1
7゜18.19,20・・・・・・T波長線路。Figures 1 and 2 are diagrams showing conventional circuit diagrams, Figure 3 is a plan view of the resistor, Figure 4 is a side view of the resistor shown in Figure 3, and Figure 5 is a diagram of the resistor of the present invention. In the figure, 1, 2, 3...input terminals, 4...
...Output terminal, 5, 6, 7, 8, 9, 10, 11
. 12...Resistor, 13,14,15.16,1
7゜18.19,20...T wavelength line.
Claims (1)
入力を受ける特性インピーダンスρジ丁Z。 (zの:電力合成器の入出力インピーダンス)の2つの
伝送線路を含み第一の入力を2つに分配するウィルキン
ソン型の分配回路と;第二の入力を受ける特性インピー
ダンスC1丁z。 の伝送線路と、特性インピーダンスへン〒zoの前記伝
送線路の出力端に接続される特性インピーダンスZ。 の伝送線路と、前記分配回路からの一方の出力を受ける
特性インピーダンス2Zoの伝送線路と、特性インピー
ダンスZ。 、2Zoの前記伝送線路の入力端に挿入される抵抗値2
zoの抵抗とを含み、特性インピーダンスzo、2Zo
の前記伝送路の出力端の接続点から合成出力を取り出す
ウィルキンソン型の第一の合成回路と:第三の入力を受
ける特性インピーダンスヘシ丁z oの伝送線路と、特
性インピーダンスペレ丁zoの前記伝送線路の出力端に
接続される特性インピーダンス2゜の伝送路と、前記分
配回路からの他方の出力を受ける特性インピーダンス2
Zoの伝送線路と、特性インピーダンスzo、2zOの
前記伝送線路の入力端に挿入される抵抗値2Zoの抵抗
とを含み、特性インピーダンスzo、2ZQの前記伝送
路の出力端の接続点から合成出力を取り出すウィルキン
ソン型の第二の合成回路と:前記第−、二合成回路の出
力をそれぞれ受ける特性インピーダンスfΣZ。 の2つの伝送線路と、特性インピーダンスaZ。 の前記2つの伝送線路の入力端に挿入される抵抗値2z
oの抵抗とを含み、特性インピーダンスhZoの前記2
つの伝送線路の出力端の接続点から合成出力を取り出す
ウィルキンソン型の第三の合成回路とを具備し、前記第
三の合成回路から前記3つの入力の合成電力を取り出す
ことを特徴とする電力合成器。[Claims for Utility Model Registration] A power combiner that combines three inputs; 1st (7)
Characteristic impedance ρjidingZ that receives input. A Wilkinson-type distribution circuit that includes two transmission lines (z: input/output impedance of the power combiner) and divides the first input into two; and a characteristic impedance C1 that receives the second input. and a characteristic impedance Z connected to the output end of the transmission line with characteristic impedance Z. a transmission line with a characteristic impedance 2Zo that receives one output from the distribution circuit, and a characteristic impedance Z. , 2Zo resistance value 2 inserted at the input end of the transmission line
zo resistance, and the characteristic impedance zo, 2Zo
a Wilkinson type first combining circuit that takes out a combined output from a connection point of the output end of the transmission line; a transmission line with a characteristic impedance of 0 to receive a third input; and the transmission line of characteristic impedance of 0 to 0; A transmission line with a characteristic impedance of 2° connected to the output end of the line, and a characteristic impedance 2 which receives the other output from the distribution circuit.
It includes a transmission line of Zo and a resistor of resistance value 2Zo inserted into the input end of the transmission line with characteristic impedance zo and 2zO, and outputs a composite output from the connection point of the output end of the transmission line with characteristic impedance zo and 2ZQ. A Wilkinson-type second synthesis circuit to be extracted: a characteristic impedance fΣZ receiving the outputs of the second and second synthesis circuits, respectively; two transmission lines and a characteristic impedance aZ. The resistance value 2z inserted at the input ends of the two transmission lines of
2 with a characteristic impedance hZo.
a Wilkinson-type third combining circuit that takes out a combined output from a connection point between output ends of two transmission lines, and takes out the combined power of the three inputs from the third combining circuit. vessel.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP12306978U JPS5853767Y2 (en) | 1978-09-06 | 1978-09-06 | power combiner |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP12306978U JPS5853767Y2 (en) | 1978-09-06 | 1978-09-06 | power combiner |
Publications (2)
Publication Number | Publication Date |
---|---|
JPS5539775U JPS5539775U (en) | 1980-03-14 |
JPS5853767Y2 true JPS5853767Y2 (en) | 1983-12-07 |
Family
ID=29081802
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP12306978U Expired JPS5853767Y2 (en) | 1978-09-06 | 1978-09-06 | power combiner |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS5853767Y2 (en) |
Families Citing this family (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
KR100362877B1 (en) * | 2000-08-09 | 2002-11-27 | 엘지이노텍 주식회사 | Power divider /combiner using 3 way chebyshev matching transformer |
-
1978
- 1978-09-06 JP JP12306978U patent/JPS5853767Y2/en not_active Expired
Also Published As
Publication number | Publication date |
---|---|
JPS5539775U (en) | 1980-03-14 |
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