JPS594210A - High efficiency linear amplifier for SSB - Google Patents

High efficiency linear amplifier for SSB

Info

Publication number
JPS594210A
JPS594210A JP57110656A JP11065682A JPS594210A JP S594210 A JPS594210 A JP S594210A JP 57110656 A JP57110656 A JP 57110656A JP 11065682 A JP11065682 A JP 11065682A JP S594210 A JPS594210 A JP S594210A
Authority
JP
Japan
Prior art keywords
ssb
wave
amplifier
linear amplifier
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.)
Granted
Application number
JP57110656A
Other languages
Japanese (ja)
Other versions
JPH0148687B2 (en
Inventor
Yoshimasa Tsunoda
角田 義正
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.)
Kokusai Denki Electric Inc
Original Assignee
Kokusai 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 Kokusai Electric Co Ltd filed Critical Kokusai Electric Co Ltd
Priority to JP57110656A priority Critical patent/JPS594210A/en
Publication of JPS594210A publication Critical patent/JPS594210A/en
Publication of JPH0148687B2 publication Critical patent/JPH0148687B2/ja
Granted legal-status Critical Current

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  • Transmitters (AREA)
  • Amplitude Modulation (AREA)
  • Amplifiers (AREA)

Abstract

(57)【要約】本公報は電子出願前の出願データであるた
め要約のデータは記録されません。
(57) [Summary] This bulletin contains application data before electronic filing, so abstract data is not recorded.

Description

【発明の詳細な説明】 本発明は直線的に電力増幅することが要求される5SB
(シングルサイドバンド)送信機に適する高効率直線増
幅器に関するものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention applies to 5SB which requires linear power amplification.
(single sideband) transmitter.

さてパルス幅変調(以下PWMと略記)方式の振幅変調
(以下AMと略記)による放送機は既に実用化され、主
として中波ラジオ放送に用いられテイル。このパルス幅
変調方式は従来DSB(ダブルサイドバンド)放送のみ
を対象としてきた。
Now, broadcasters using pulse width modulation (hereinafter abbreviated as PWM) and amplitude modulation (hereinafter abbreviated as AM) have already been put into practical use, and are mainly used for medium wave radio broadcasting. This pulse width modulation method has conventionally been used only for DSB (double sideband) broadcasting.

DSB放送では搬送波が常時存在しこれを音声にてAM
するのみ゛であるが、SSB放送の場合では搬送波は低
減または除去され、サイドバンドの片側は完全に取除か
れていることはよく知られている。SSB送信機におい
てSSB波は通常低レベル段にて作られ、これを順次直
線性良好の増幅を行うのであるが、電力効率が悪いこと
が難点であって、たとえば送信機を集積回路化するのに
その最大出力を次に説明するように上げることが難しい
という欠点があった。本発明はこの問題を解決するため
に行われたものである。
In DSB broadcasting, a carrier wave is always present, and this is transmitted as AM using audio.
However, it is well known that in the case of SSB broadcasts, the carrier wave is reduced or removed, and one side of the sideband is completely removed. In an SSB transmitter, the SSB wave is usually generated in a low-level stage, and the wave is sequentially amplified with good linearity. However, the problem is that the power efficiency is poor, and it is difficult to integrate the transmitter into an integrated circuit. had the disadvantage that it was difficult to increase its maximum output as explained below. The present invention has been made to solve this problem.

まず従来のSSB送信機ではSSB波を増幅するにはB
級またはAB級増幅によって行われている。第1図は従
来のSSB送信機の構成側図で、通常の直線増幅器を用
いた場合である。第1図においてAPは低周波入力信号
、1はSSB発生回路、2は平衡変調器、fst  f
s。は搬送周波入力、3はバンドパスフィルタ、4は前
段増幅器、Q1Q2 は゛市力増幅部を形成する電界効
果トランジスタ(F E ’l” )、5は整合回路、
Zo はアンテナ負荷インピーダンスである。この電力
増幅回路で直線増幅を行うにはゲート側の中点Cにバイ
アスをかけF E ’I’ Q、  Q2 には無 信
号時においてもある程度のアイドル電流を流す必要があ
る。この電流は大きい程直線性の良い出力が得られるが
、他方この電流によって電力増幅器の電力効率が下がり
Q4.Q2  の発熱が大きくなる。通常B級増幅でア
イドル電流を僅か流す程度では電力効率は40チ台であ
るが、歪率を良くするためにもっとA級増幅に近付ける
と電力効率は30%台になってしまう。すなわち損失電
力は70%近い値となり、QIQ2 の冷却装置も大き
なものとなる。
First, with conventional SSB transmitters, B
Class or AB amplification is used. FIG. 1 is a side view of the configuration of a conventional SSB transmitter, in which a normal linear amplifier is used. In Figure 1, AP is a low frequency input signal, 1 is an SSB generation circuit, 2 is a balanced modulator, fst f
s. is a carrier frequency input, 3 is a bandpass filter, 4 is a pre-stage amplifier, Q1Q2 is a field effect transistor (F E 'l'') forming a power amplifier section, 5 is a matching circuit,
Zo is the antenna load impedance. In order to perform linear amplification with this power amplifier circuit, it is necessary to apply a bias to the center point C on the gate side and to allow a certain amount of idle current to flow through F E 'I' Q and Q2 even when there is no signal. The larger this current is, the more linear the output can be obtained, but on the other hand, this current reduces the power efficiency of the power amplifier, Q4. Q2 heat generation increases. Normally, when a small amount of idle current is passed through a class B amplifier, the power efficiency is in the 40s, but if it is made closer to a class A amplification in order to improve the distortion rate, the power efficiency drops to the 30% range. That is, the power loss will be close to 70%, and the QIQ2 cooling device will also be large.

本発明においては従来のB級またはA級増幅の代りにD
級増幅(スイッチング増幅)を用い、直線的に信号を増
幅すると共に電力効率を上け、使用する増幅素子を少く
し冷却装置を小形化できることが特徴である。
In the present invention, instead of conventional class B or class A amplification, D
It is characterized by using class amplification (switching amplification) to linearly amplify signals, improve power efficiency, reduce the number of amplification elements used, and downsize the cooling device.

第2図は本発明を実施したSSB送信機の構成側口であ
る。図中の6はSSB発生回路で、音声周波数AFを搬
送周波数f。により平衡変調し、fC成分と一方のサイ
ドバンド、この例では下サイドバンド(または上サイド
バンド)が除去されたSSBを得る。ところである音声
信号から作られたSSB信号はもとの音声信号とは全く
異なる波形となる。いま第3図に示すようなSSB波が
得られたとする。このSSB波は単純に包絡線検波して
ももとの音声信号を得ることはできず、通常はSSB信
号と搬送波成分を合成したのち包絡線検波を行って始め
て音声信号が得られることはよく知られている。本発明
回路においてはSSB波をまずそのま5包絡線検波し、
この検波波形により位相変調された割当周波数T5波(
SSB波を制限増幅器13を通し位相変調は残るが振幅
−電波としたものを増幅したのち搬送波として使用)を
振幅変調することにより通常のSSB波として送信する
もので、第2図について以下に説明する。第4図は第3
図のSSB波を包絡線検波した後の波形図で、第2図の
f入力に当るものである。
FIG. 2 shows the configuration side of an SSB transmitter embodying the present invention. 6 in the figure is an SSB generation circuit, which converts the audio frequency AF to the carrier frequency f. Balanced modulation is performed by , and an SSB is obtained in which the fC component and one sideband, in this example, the lower sideband (or upper sideband) are removed. By the way, an SSB signal created from an audio signal has a waveform completely different from that of the original audio signal. Assume now that an SSB wave as shown in FIG. 3 is obtained. The original audio signal of this SSB wave cannot be obtained simply by envelope detection; normally, the audio signal can only be obtained by combining the SSB signal and carrier component and then performing envelope detection. Are known. In the circuit of the present invention, the SSB wave is first detected by 5 envelopes,
The assigned frequency T5 wave (
The SSB wave is passed through the limiting amplifier 13, and the phase modulation remains, but the amplitude-radio wave is amplified and used as a carrier wave.) It is amplitude-modulated and transmitted as a normal SSB wave. Fig. 2 is explained below. do. Figure 4 is the third
This is a waveform diagram after envelope detection of the SSB wave shown in the figure, and corresponds to the f input in FIG. 2.

第2図に戻って7はレベルシフト回路、8は3角波発生
器、9はコンパレータ、10はパルス増幅器、11はロ
ーパスフィルタ(LPF)、12はバンドパスフィルタ
(BPF)、13は制限増幅器、14は前段増幅器、Q
1〜Q4はスイッチング電力増幅を行うFET、Q5 
はスイッチングFE’l”S’l”lは出力変成器であ
る。さてレベルシフト回路7は第4図の包絡線検波信号
が零レベルのとき3角波発生器8からの信号Bと包絡線
検波信号Aとを比較出力するコンパレータ9の出力Pの
パルス幅をシフト電圧りによって零に調整するものであ
る。コンパレータ9にてパルス幅変調されたパルスPは
第5図に示しであるが、この図は理解し易いように第4
図のaからbまでの波形を拡大し通常1. OOkHz
近辺のサンプリング周波数をとる3角波Bの波形と比較
されてパルス幅変調される様子を示したもので、PWM
波Pはこのようにして得られている。このパルスPはパ
ルス増幅器10によって増幅されFETQ5のゲートに
与えられる。Q5は従ってパルス信号Pに応じてオン、
オフの動作を行う。このQ5のオン、オフ動作による電
力損失は活性領域で動作する場合より格段に少ないこと
は自明である。Q5によって電#gをオン、オフされた
電力はLPFzによってサンプリング周波数成分が除去
されて、もとの包絡線波形となり変調電力として−Q、
1,7 Q4に与えられる。
Returning to Figure 2, 7 is a level shift circuit, 8 is a triangular wave generator, 9 is a comparator, 10 is a pulse amplifier, 11 is a low pass filter (LPF), 12 is a band pass filter (BPF), and 13 is a limiting amplifier. , 14 is the front stage amplifier, Q
1 to Q4 are FETs that perform switching power amplification, Q5
is the switching FE'l"S'l"l is the output transformer. Now, the level shift circuit 7 shifts the pulse width of the output P of the comparator 9 which compares and outputs the signal B from the triangular wave generator 8 and the envelope detection signal A when the envelope detection signal shown in FIG. 4 is at zero level. It is adjusted to zero by adjusting the voltage. The pulse P modulated in pulse width by the comparator 9 is shown in FIG.
The waveforms from a to b in the figure are enlarged and are usually 1. OOkHz
This shows how the pulse width is modulated by comparing it with the waveform of triangular wave B that takes a nearby sampling frequency.
The wave P is obtained in this way. This pulse P is amplified by a pulse amplifier 10 and applied to the gate of FETQ5. Q5 is therefore turned on in response to pulse signal P.
Perform the off action. It is obvious that the power loss due to the on/off operation of Q5 is much smaller than when it operates in the active region. The sampling frequency component of the power turned on and off by Q5 is removed by LPFz, and the original envelope waveform becomes -Q, as modulated power.
1,7 Given to Q4.

他方SSB発生回路6から出力され位相変調を受けてい
る割当周波数f5の信号は、制限増幅器13を経た後前
段増幅器14にて増幅されて変成器T2、T3により図
のような位相関係(QlとQ3は180、%とQ4は1
80、QlとQ2は180 それぞれ位相が異っている
)でQ□〜Q4をスイッチングする。Q1〜Q4はD級
増幅器を形成するもので、例えばQ□と鵠がオンのとき
はQ3と喝がオフとなり、Q3とQ2がオンのときはQ
□とへかオフとなり、割当周波数f、に従って交互にオ
ン、オフを繰返す。変成器T1の1次側にはQ□〜Q4
のオン、オフに従い極性が反転した電流が流れるため、
T1の2次側にはこの合成された誘導電流が流れる。こ
の電流はスイッチングされた波形を持つため、バンドパ
スフィルタ12によって不要な成分が除去され、アンテ
ナ等の負荷Z。
On the other hand, the signal of assigned frequency f5 outputted from the SSB generation circuit 6 and subjected to phase modulation passes through the limiting amplifier 13, is amplified by the front stage amplifier 14, and is converted into a phase relationship (Ql and Q3 is 180, % and Q4 are 1
80, and Ql and Q2 have different phases by 180) to switch Q□ to Q4. Q1 to Q4 form a class D amplifier; for example, when Q□ and Mouse are on, Q3 and Mouse are off, and when Q3 and Q2 are on, Q
□ and then off, and alternately turn on and off according to the assigned frequency f. Q□~Q4 on the primary side of transformer T1
As the current flows, the polarity is reversed as the switch turns on and off.
This combined induced current flows through the secondary side of T1. Since this current has a switched waveform, unnecessary components are removed by the bandpass filter 12 and the load Z such as an antenna is removed.

には第3図に示したもとのSSB波と同様の包絡線をも
つ電力が供給される。
is supplied with power having an envelope similar to the original SSB wave shown in FIG.

以上は特に直線性を要求されるSiB波の電力増幅をD
級増幅によって具体的に実行する回路を説明したが、電
力効率は実測によれば80多近くまで」二げられること
が確められ、高効率直線増幅器として送信機の小形化に
著しく有効である。
The above describes the power amplification of SiB waves, which requires particularly linearity.
Although we have explained the circuit specifically executed by class amplification, it has been confirmed that the power efficiency can be increased to nearly 80% according to actual measurements, and it is extremely effective in reducing the size of transmitters as a high-efficiency linear amplifier. .

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

第1図は従来のSSB送信機の構成例図、第2図は本発
明を実施したSSB送信機の構成例図、第3図はSSB
波の一例図、第4図は第3図のSSB波を包結線検波し
た波形図、第5図は3角波と包絡線検波された第4図の
aからbまでの波形を比較し、PWM波Pを得る説明図
である。 1・・・・SSB発生回路、 2・・・・平衡変調器、 30・・BPF、 4・・・・前段増幅器、 5・・・・整合回路、 6・・・・SSB発生回路、 71−拳レベルシフト回路、 8・・・・3角波発生器、 9■・・コンパレータ 】0・・・・パルス増幅器、 11・・・・L P Ii” 12・・・・BPP 13・・・・制限増幅器、 14・・・・前段増幅器。 特許出願人  国際電気株式会社
Fig. 1 is an example of the configuration of a conventional SSB transmitter, Fig. 2 is an example of the configuration of an SSB transmitter implementing the present invention, and Fig. 3 is an example of an SSB transmitter.
An example of the wave, Figure 4 is a waveform diagram of the SSB wave in Figure 3 with envelope detection, Figure 5 is a comparison of the triangular wave and the envelope-detected waveforms from a to b in Figure 4. FIG. 3 is an explanatory diagram for obtaining a PWM wave P. DESCRIPTION OF SYMBOLS 1...SSB generation circuit, 2...Balanced modulator, 30...BPF, 4...Pre-stage amplifier, 5...Matching circuit, 6...SSB generation circuit, 71- Fist level shift circuit, 8... triangular wave generator, 9 ■... comparator] 0... pulse amplifier, 11... L P Ii" 12... BPP 13... Limiting amplifier, 14...Pre-stage amplifier. Patent applicant Kokusai Denki Co., Ltd.

Claims (1)

【特許請求の範囲】[Claims] シングルサイドバンド波を包絡線検波し、これとサンプ
リング周波数の3角波とによって得られるパルス幅変調
波を得る回路と、そのパルス幅変調波の復調波によって
変調される上記シングルサイドバンド波の振幅制限増幅
出力でスイクチされるスイッチング電力増幅器とを備え
ることを特徴とするSSB用高効率直線増幅器。
A circuit that performs envelope detection of a single sideband wave and obtains a pulse width modulated wave obtained by this and a triangular wave of a sampling frequency, and an amplitude of the single sideband wave that is modulated by a demodulated wave of the pulse width modulation wave. A high-efficiency linear amplifier for SSB, comprising a switching power amplifier that is switched at a limited amplification output.
JP57110656A 1982-06-29 1982-06-29 High efficiency linear amplifier for SSB Granted JPS594210A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP57110656A JPS594210A (en) 1982-06-29 1982-06-29 High efficiency linear amplifier for SSB

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP57110656A JPS594210A (en) 1982-06-29 1982-06-29 High efficiency linear amplifier for SSB

Publications (2)

Publication Number Publication Date
JPS594210A true JPS594210A (en) 1984-01-11
JPH0148687B2 JPH0148687B2 (en) 1989-10-20

Family

ID=14541174

Family Applications (1)

Application Number Title Priority Date Filing Date
JP57110656A Granted JPS594210A (en) 1982-06-29 1982-06-29 High efficiency linear amplifier for SSB

Country Status (1)

Country Link
JP (1) JPS594210A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6480112A (en) * 1987-09-22 1989-03-27 Japan Broadcasting Corp Matching circuit
JPS6480111A (en) * 1987-09-22 1989-03-27 Japan Broadcasting Corp Matching circuit

Non-Patent Citations (1)

* Cited by examiner, † Cited by third party
Title
PROCEEDINGS OF THE I R E=1952 *

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6480112A (en) * 1987-09-22 1989-03-27 Japan Broadcasting Corp Matching circuit
JPS6480111A (en) * 1987-09-22 1989-03-27 Japan Broadcasting Corp Matching circuit

Also Published As

Publication number Publication date
JPH0148687B2 (en) 1989-10-20

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