JPH04306906A - Balance type microwave band amplifier - Google Patents
Balance type microwave band amplifierInfo
- Publication number
- JPH04306906A JPH04306906A JP7133491A JP7133491A JPH04306906A JP H04306906 A JPH04306906 A JP H04306906A JP 7133491 A JP7133491 A JP 7133491A JP 7133491 A JP7133491 A JP 7133491A JP H04306906 A JPH04306906 A JP H04306906A
- Authority
- JP
- Japan
- Prior art keywords
- harmonic
- line
- parallel
- resistor
- hybrid
- 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.)
- Granted
Links
- 238000010521 absorption reaction Methods 0.000 abstract description 13
- 239000003990 capacitor Substances 0.000 abstract description 5
- 239000000203 mixture Substances 0.000 abstract 1
- 238000010586 diagram Methods 0.000 description 8
- 240000001973 Ficus microcarpa Species 0.000 description 1
Landscapes
- Amplifiers (AREA)
- Microwave Amplifiers (AREA)
Abstract
Description
【0001】0001
【産業上の利用分野】本発明はバランス型マイクロ波帯
増幅器に関する。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a balanced microwave band amplifier.
【0002】0002
【従来の技術】マイクロ波帯増幅器の出力電力レベルを
高めるために、1対の単位増幅器を並列動作させるバラ
ンス型マイクロ波帯増幅器が用いられている。各単位増
幅器は、入力側および出力側のそれぞれで、90度ハイ
ブリッドにより互いに並列接続される。2. Description of the Related Art In order to increase the output power level of a microwave band amplifier, a balanced microwave band amplifier is used in which a pair of unit amplifiers are operated in parallel. Each unit amplifier is connected in parallel to each other by a 90 degree hybrid on each of the input side and output side.
【0003】0003
【発明が解決しようとする課題】この従来のバランス型
マイクロ波帯増幅器では、動作レベルが飽和領域に入る
と非線形動作となり、基本波周波数成分fの他に2倍波
2f,3倍波3f,…等高調波成分が生じる。[Problems to be Solved by the Invention] In this conventional balanced microwave band amplifier, when the operating level enters the saturation region, nonlinear operation occurs, and in addition to the fundamental frequency component f, the second harmonic 2f, the third harmonic 3f, ... Equal harmonic components are generated.
【0004】図5を参照すると、バランス型増幅器では
単位増幅器21の負荷である出力側のハイブリッド22
が基本波f,3倍波3f,…といった奇数次高調波成分
に対しては所要の50Ω負荷になるが、2倍波2f,4
倍波,…といった偶数次高調波成分に対しては50Ω負
荷にならない。そのために、偶数次高調波成分がハイブ
リッド22で反射されて単位増幅器21の出力側に戻り
、基本波fとミキシングし、例えば2倍波高調波成分2
fは2f−f=fという基本波fと同じ周波数の成分を
生じる。この成分は単位増幅器21で増幅された基本波
成分fと位相がずれている為に合成出力で周波数特性に
リップルが生じるという問題があった。Referring to FIG. 5, in a balanced amplifier, a hybrid 22 on the output side is a load of a unit amplifier 21.
is the required 50Ω load for odd harmonic components such as the fundamental wave f, the third harmonic 3f, ..., but the second harmonic 2f, 4
For even-order harmonic components such as harmonics, etc., the load does not become 50Ω. For this purpose, the even-order harmonic components are reflected by the hybrid 22 and returned to the output side of the unit amplifier 21, and mixed with the fundamental wave f, for example, the second harmonic component 2.
f produces a component of the same frequency as the fundamental wave f, 2f-f=f. Since this component is out of phase with the fundamental wave component f amplified by the unit amplifier 21, there is a problem in that ripples occur in the frequency characteristics of the combined output.
【0005】[0005]
【課題を解決するための手段】本発明のバランス型マイ
クロ波帯増幅器は、1対の単位増幅器の前後に90度ハ
イブリッドを有するバランス型マイクロ波帯増幅器にお
いて、前記単位増幅器の出力側の主線路と並列に接続し
た抵抗と、所要周波数の2倍波高調波成分に対し1/2
波長の長さであり一端を前記抵抗に接続し他端を高周波
的に短絡した線路とを含んでいる。Means for Solving the Problems The balanced microwave band amplifier of the present invention has a 90 degree hybrid before and after a pair of unit amplifiers, in which the main line on the output side of the unit amplifier is and a resistor connected in parallel with 1/2 for the double harmonic component of the required frequency.
The line has a wavelength length and has one end connected to the resistor and the other end short-circuited in terms of high frequency.
【0006】[0006]
【実施例】次に本発明について図面を参照して説明する
。DESCRIPTION OF THE PREFERRED EMBODIMENTS Next, the present invention will be explained with reference to the drawings.
【0007】図1は本発明の一実施例を示す回路図、図
2は図1における2倍波吸収回路9,10の構成を示す
図である。FIG. 1 is a circuit diagram showing one embodiment of the present invention, and FIG. 2 is a diagram showing the configuration of second harmonic absorption circuits 9 and 10 in FIG.
【0008】図1を参照すると、1対の単位増幅器5,
6の入力端がハイブリッド7により並列に接続されてい
る。単位増幅器5,6の出力側の主線路1はハイブリッ
ド8により並列に接続され、これら主線路には2倍波吸
収回路9,10がそれぞれ接続されている。Referring to FIG. 1, a pair of unit amplifiers 5,
The input terminals of 6 are connected in parallel by a hybrid 7. Main lines 1 on the output side of unit amplifiers 5 and 6 are connected in parallel by a hybrid 8, and double wave absorption circuits 9 and 10 are connected to these main lines, respectively.
【0009】2倍波吸収回路9,10は、図2に示すよ
うに、主線路1と並列に抵抗2を介し、基本波に対して
1/4波長,2倍波に対しては1/2波長となる長さの
線路3の一端を接続し、線路3の他端をコンデンサ4に
より高周波的に接地して2倍波高調波を抵抗2に吸収さ
せるしくみである。例えば、基本波周波数12GHzの
とき、抵抗2の抵抗値25Ω,線路3の特性インピーダ
ンス70Ω,コンデンサ3の容量値3.9pFを使用す
る。As shown in FIG. 2, the second harmonic absorption circuits 9 and 10 are connected in parallel with the main line 1 through a resistor 2, and have a wavelength of 1/4 for the fundamental wave and a wavelength of 1/4 for the second harmonic. One end of a line 3 having a length of two wavelengths is connected, and the other end of the line 3 is grounded at high frequency by a capacitor 4, so that the second harmonic is absorbed by the resistor 2. For example, when the fundamental wave frequency is 12 GHz, the resistance value of the resistor 2 is 25 Ω, the characteristic impedance of the line 3 is 70 Ω, and the capacitance value of the capacitor 3 is 3.9 pF.
【0010】図3は図2の線路3の受端短絡時の送端イ
ンピーダンスZAの変化を示したものである。波長をλ
、線路3の特性インピーダンス,長さをZ,Lとすると
、ZA=jZtanβL(ただし.β=2π/λ)であ
るから、基本波において1/4波長を持つ線路3の送端
からみたインピーダンスZAは無限大となり、2倍波吸
収回路9,10は基本波に対して動作しない。線路3は
2倍波成分では1/2波長を持つ線路となり、送端から
みたインピーダンスZAは0となり、2倍波高調波成分
は2倍波吸収回路9,10に流れ込み抵抗2に吸収され
る。故に基本波はそのまま主線路1を通るが、2倍波高
調波成分は2倍波吸収回路9,10に吸収され負荷とな
る出力側のハイブリッド8には流れない為に、基本波と
のミキシングが起こらない。従って非線形領域における
2倍波高調波成分の影響はなくなる。FIG. 3 shows a change in the transmitting end impedance ZA when the receiving end of the line 3 shown in FIG. 2 is short-circuited. The wavelength is λ
, when the characteristic impedance and length of the line 3 are Z and L, ZA=jZtanβL (however, β=2π/λ), so the impedance ZA seen from the sending end of the line 3 which has 1/4 wavelength in the fundamental wave becomes infinite, and the second harmonic absorption circuits 9 and 10 do not operate with respect to the fundamental wave. The line 3 becomes a line with a 1/2 wavelength for the second harmonic component, and the impedance ZA seen from the sending end becomes 0, and the second harmonic component flows into the second harmonic absorption circuits 9 and 10 and is absorbed by the resistor 2. . Therefore, the fundamental wave passes through the main line 1 as it is, but the second harmonic component is absorbed by the second harmonic absorption circuits 9 and 10 and does not flow to the hybrid 8 on the output side, which serves as a load, so mixing with the fundamental wave is required. does not occur. Therefore, the influence of the second harmonic component in the nonlinear region is eliminated.
【0011】図4は2倍波吸収回路9,10が2倍波を
吸収している説明図である。基本波成分,3倍波成分等
の奇数次高調波成分は出力側のハイブリッド8の方向に
流れて行くが、2倍波成分等の偶数次高調波成分は2倍
波吸収回路9,10に流れ、ハイブリッド8は流れない
。FIG. 4 is an explanatory diagram of the second harmonic absorption circuits 9 and 10 absorbing the second harmonic. Odd-numbered harmonic components such as the fundamental wave component and 3rd harmonic component flow toward the hybrid 8 on the output side, but even-numbered harmonic components such as the 2nd harmonic component flow to the 2nd harmonic absorption circuits 9 and 10. Flow, Hybrid 8 does not flow.
【0012】0012
【発明の効果】以上説明した様に本発明は、単位増幅器
の出力側の主線路と並列に、抵抗を介し、基本波におい
て1/4波長,2倍波高調波成分に対して1/2波長と
なる長さを持ち受端をコンデンサ等で高周波的に接地し
た線路を設ける事により、基本波には影響を与えること
なく2倍波高調波成分等の偶数次高調波成分を吸収させ
、非線形領域において周波数特性のリップルを押え、振
幅偏差や振幅傾斜を小さくする事ができるという効果を
有する。Effects of the Invention As explained above, the present invention provides a 1/4 wave wavelength for the fundamental wave and a 1/2 wave for the double wave harmonic component through a resistor in parallel with the main line on the output side of the unit amplifier. By providing a line with a length that corresponds to the wavelength and whose receiving end is grounded at high frequency with a capacitor, etc., even-order harmonic components such as second harmonic components are absorbed without affecting the fundamental wave. This has the effect of suppressing ripples in frequency characteristics in the nonlinear region and reducing amplitude deviations and amplitude slopes.
【図1】本発明の一実施例を示す回路図である。FIG. 1 is a circuit diagram showing one embodiment of the present invention.
【図2】図1における2倍波吸収回路9,10の構成を
示す図である。2 is a diagram showing the configuration of second harmonic absorption circuits 9 and 10 in FIG. 1. FIG.
【図3】図2の線路3の送端インピーダンスZAの長さ
Lに対する変化を示した図である。3 is a diagram showing a change in the sending end impedance ZA of the line 3 in FIG. 2 with respect to the length L. FIG.
【図4】図1の実施例における偶数次高調波成分の吸収
を説明するための図である。FIG. 4 is a diagram for explaining absorption of even harmonic components in the embodiment of FIG. 1;
【図5】従来のバランス型マイクロ波帯増幅器における
2倍波高調波成分と基本波とのミキシングを説明するた
めの図である。FIG. 5 is a diagram for explaining mixing of a second harmonic component and a fundamental wave in a conventional balanced microwave band amplifier.
1 主線路 2 抵抗 3 線路 4 コンデンサ 5,6 単位増幅器 7,8 ハイブリッド 9,10 2倍波吸収回路 1 Main line 2 Resistance 3 Railway 4 Capacitor 5, 6 unit amplifier 7,8 Hybrid 9,10 Second harmonic absorption circuit
Claims (1)
ブリッドを有するバランス型マイクロ波帯増幅器におい
て、前記単位増幅器の出力側の主線路と並列に接続した
抵抗と、所要周波数の2倍波高調波成分に対し1/2波
長の長さであり一端を前記抵抗に接続し他端を高周波的
に短絡した線路とを含むことを特徴とするバランス型マ
イクロ波帯増幅器。Claim 1. A balanced microwave band amplifier having a 90-degree hybrid before and after a pair of unit amplifiers, including a resistor connected in parallel with the main line on the output side of the unit amplifier, and a second harmonic of a desired frequency. A balanced microwave band amplifier comprising a line having a length of 1/2 wavelength relative to a wave component, one end of which is connected to the resistor, and the other end of which is short-circuited in terms of high frequency.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP3071334A JP2927981B2 (en) | 1991-04-04 | 1991-04-04 | Balanced microwave band amplifier |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP3071334A JP2927981B2 (en) | 1991-04-04 | 1991-04-04 | Balanced microwave band amplifier |
Publications (2)
Publication Number | Publication Date |
---|---|
JPH04306906A true JPH04306906A (en) | 1992-10-29 |
JP2927981B2 JP2927981B2 (en) | 1999-07-28 |
Family
ID=13457524
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP3071334A Expired - Lifetime JP2927981B2 (en) | 1991-04-04 | 1991-04-04 | Balanced microwave band amplifier |
Country Status (1)
Country | Link |
---|---|
JP (1) | JP2927981B2 (en) |
Cited By (6)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2009200911A (en) * | 2008-02-22 | 2009-09-03 | Toshiba Corp | Secondary harmonic suppression filter |
JP2009246871A (en) * | 2008-03-31 | 2009-10-22 | Mitsubishi Electric Corp | Second harmonic suppression circuit |
JP2010182683A (en) * | 2002-05-20 | 2010-08-19 | Mks Instruments Inc | Method and apparatus for vhf plasma processing with load mismatch reliability and stability |
JP2010199855A (en) * | 2009-02-24 | 2010-09-09 | Furukawa Electric Co Ltd:The | Filter circuit |
WO2014171033A1 (en) * | 2013-04-19 | 2014-10-23 | 株式会社村田製作所 | High-frequency module |
JP6399267B1 (en) * | 2018-02-09 | 2018-10-03 | 三菱電機株式会社 | amplifier |
Citations (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS61100011A (en) * | 1984-10-23 | 1986-05-19 | Toshiba Corp | Microwave power amplifier |
JPH0255721U (en) * | 1988-10-18 | 1990-04-23 | ||
JPH02134729U (en) * | 1989-04-14 | 1990-11-08 |
-
1991
- 1991-04-04 JP JP3071334A patent/JP2927981B2/en not_active Expired - Lifetime
Patent Citations (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS61100011A (en) * | 1984-10-23 | 1986-05-19 | Toshiba Corp | Microwave power amplifier |
JPH0255721U (en) * | 1988-10-18 | 1990-04-23 | ||
JPH02134729U (en) * | 1989-04-14 | 1990-11-08 |
Cited By (11)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2010182683A (en) * | 2002-05-20 | 2010-08-19 | Mks Instruments Inc | Method and apparatus for vhf plasma processing with load mismatch reliability and stability |
JP2009200911A (en) * | 2008-02-22 | 2009-09-03 | Toshiba Corp | Secondary harmonic suppression filter |
JP4643666B2 (en) * | 2008-02-22 | 2011-03-02 | 株式会社東芝 | Second harmonic suppression filter |
JP2009246871A (en) * | 2008-03-31 | 2009-10-22 | Mitsubishi Electric Corp | Second harmonic suppression circuit |
JP2010199855A (en) * | 2009-02-24 | 2010-09-09 | Furukawa Electric Co Ltd:The | Filter circuit |
WO2014171033A1 (en) * | 2013-04-19 | 2014-10-23 | 株式会社村田製作所 | High-frequency module |
US9413336B2 (en) | 2013-04-19 | 2016-08-09 | Murata Manufacturing Co., Ltd. | Multiband-support radio-frequency module |
JP6399267B1 (en) * | 2018-02-09 | 2018-10-03 | 三菱電機株式会社 | amplifier |
WO2019155601A1 (en) * | 2018-02-09 | 2019-08-15 | 三菱電機株式会社 | Amplifier |
CN111869102A (en) * | 2018-02-09 | 2020-10-30 | 三菱电机株式会社 | Amplifier with a high-frequency amplifier |
US11264951B2 (en) | 2018-02-09 | 2022-03-01 | Mitsubishi Electric Corporation | Amplifier |
Also Published As
Publication number | Publication date |
---|---|
JP2927981B2 (en) | 1999-07-28 |
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Legal Events
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A02 | Decision of refusal |
Free format text: JAPANESE INTERMEDIATE CODE: A02 Effective date: 19971111 |