JPH0148687B2 - - Google Patents
Info
- Publication number
- JPH0148687B2 JPH0148687B2 JP57110656A JP11065682A JPH0148687B2 JP H0148687 B2 JPH0148687 B2 JP H0148687B2 JP 57110656 A JP57110656 A JP 57110656A JP 11065682 A JP11065682 A JP 11065682A JP H0148687 B2 JPH0148687 B2 JP H0148687B2
- Authority
- JP
- Japan
- Prior art keywords
- wave
- ssb
- amplifier
- power
- amplification
- 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
- 238000001514 detection method Methods 0.000 claims description 7
- 238000005070 sampling Methods 0.000 claims description 3
- 230000003321 amplification Effects 0.000 description 11
- 238000003199 nucleic acid amplification method Methods 0.000 description 11
- 238000010586 diagram Methods 0.000 description 4
- 230000005236 sound signal Effects 0.000 description 4
- 238000001816 cooling Methods 0.000 description 2
- 206010037660 Pyrexia Diseases 0.000 description 1
- 230000005669 field effect Effects 0.000 description 1
- 238000005259 measurement Methods 0.000 description 1
- 238000000034 method Methods 0.000 description 1
Landscapes
- Amplifiers (AREA)
- Transmitters (AREA)
- Amplitude Modulation (AREA)
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SSB(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 relates to a high efficiency linear amplifier suitable for SSB (single sideband) transmitters that require linear power amplification.
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
ている。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。
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輻を行う
のであるが、電力効率が悪いことが難点であつ
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
という欠点があつた。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。 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 traditionally been used only for DSB (double sideband) broadcasting.
It is well known that in DSB broadcasting, the carrier wave is always present and is only AMed with audio, but in the case of SSB broadcasting, the carrier wave is reduced or removed, and one side of the sideband is completely removed. There is. In an SSB transmitter, the SSB wave is usually generated in the low-level stage, and the waves are sequentially increased with good linearity, but the problem is that the power efficiency is poor, so for example, it is difficult to integrate the transmitter into an integrated circuit. However, it 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級増幅によつて行われている。
第1図は従来のSSB送信機の構成例図で、通常の
直線増幅器を用いた場合である。第1図において
AFは低周波入力信号、1はSSB発生回路、2は
平衡変調器、fs1,fs2は搬送周波入力、3はバン
ドパスフイルタ、4は前段増幅器、Q1,Q2は電
力増幅部を形成する電界効果トランジスタ
(FET)、5は整合回路、Zp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心cにバイアスをかけ
FET Q1,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
流によつて電力増幅器の電力効率が下がりQ1,
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%台であ
るが、歪率を良くするためにもつとA級増幅に近
付けると電力効率は30%台になつてしまう。すな
わち損失電力は70%近い値となり、Q1,Q2の冷
却装置も大きなものとなる。 First, in conventional SSB transmitters, SSB waves are amplified using class B or class AB amplification.
FIG. 1 shows an example of the configuration of a conventional SSB transmitter, using an ordinary linear amplifier. In Figure 1
AF is a low frequency input signal, 1 is an SSB generation circuit, 2 is a balanced modulator, f s1 and f s2 are carrier frequency inputs, 3 is a bandpass filter, 4 is a preamplifier, and Q 1 and Q 2 are power amplifiers. A field effect transistor (FET) is formed, 5 is a matching circuit, and Z p is an antenna load impedance. To perform linear amplification with this power amplifier circuit, bias is applied to the center c on the gate side.
A certain amount of idle current must flow through FETs Q 1 and Q 2 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, Q 1 ,
Q2 fever increases. Normally, when a small amount of idle current flows in class B amplification, the power efficiency is in the 40% range, but if you use it to improve the distortion rate and approach class A amplification, the power efficiency will drop to the 30% range. In other words, the power loss will be close to 70%, and the cooling devices for Q 1 and Q 2 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(スイツチング増幅)を用い、直
線的に信号を増幅すると共に電力効率を上げ、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, class D amplification (switching amplification) is used instead of conventional class B or A amplification to linearly amplify signals, increase power efficiency, reduce the number of amplification elements used, and downsize the cooling device. It is characterized by what it can do.
第2図は本発明を実施したSSB送信機の構成例
図である。図中の6はSSB発生回路で、音声周波
数AFを搬送周波数fc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つて始めて
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波をまずそのまゝ包絡線
検波し、この検波波形により位相変調された割当
周波数fs波(SSB波を制限増幅器13を通し位相
変調は残るが振幅一定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 is a diagram showing an example of the configuration of an SSB transmitter embodying the present invention. 6 in the figure is an SSB generation circuit, which performs balanced modulation of the audio frequency AF using the carrier frequency f c , and generates SSB from which the f c component and one sideband, in this example, the lower sideband (or upper sideband) have been removed. obtain. By the way, an SSB signal created from an audio signal has a waveform that is completely different from the original audio signal. Suppose that an SSB wave as shown in Fig. 3 is obtained.
The original audio signal cannot be obtained from this SSB wave 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 envelope-detected as it is, and the assigned frequency f s wave is phase-modulated by this detected waveform (the SSB wave is passed through the limiting amplifier 13 and the phase modulation remains, but it becomes a constant amplitude wave). (after amplifying the signal and then using it as a carrier wave) is amplitude-modulated and transmitted as a normal SSB wave. Fig. 2 will be explained below. FIG. 4 is a waveform diagram after envelope detection of the SSB wave in FIG. 3, which corresponds to the f input in FIG. 2.
第2図に戻つて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はローパスフイルタ(LPF)、12は
バンドパスフイルタ(BPF)、13は制限増幅
器、14は前段増幅器、Q1〜Q4はスイツチング
電力増幅を行うFET、Q5はスイツチングFET、
T1は出力変成器である。さてレベルシフト回路
7は第4図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hによつ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図に示してあるが、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100kHz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
よつて増幅されFET Q5のゲートに与えられる。
Q5は従つてパルス信号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によつて電源gをオン、
オフされた電力はLPF11によつてサンプリン
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Q1〜Q4に与えられる。 Returning to Figure 2, 7 is a level shift circuit, 8 is 3
Square 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), 13 is a limiting amplifier, 14 is a pre-stage amplifier, Q 1 to Q 4 are switching power amplifiers Q5 is a switching FET,
T1 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 is at zero level as shown in FIG. It is adjusted to zero by h. The pulse P modulated in pulse width by the comparator 9 is shown in Fig. 5, but this figure is an enlarged version of the waveform from a to b in Fig. 4 for ease of understanding, and the sampling frequency is usually around 100kHz. This shows how the waveform of the triangular wave B is compared and pulse width modulated, and the PWM wave P is obtained in this way. This pulse P is amplified by a pulse amplifier 10 and applied to the gate of FET Q5 .
Therefore, Q5 performs an on/off operation according to the pulse signal P. 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. Turn on power g by Q 5 ,
The sampling frequency component of the turned-off power is removed by the LPF 11, resulting in the original envelope waveform, which is applied to Q1 to Q4 as modulated power.
他方SSB発生回路6から出力され位相変調を受
けて割当周波数fs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(Q1とQ3は180゜、
Q2とQ4は180゜、Q1とQ2は180゜それぞれ位相が異
つている)でQ1〜Q4をスイツチングする。Q1〜
Q4はD級増幅器を形成するもので、例えばQ1と
Q4がオンのときはQ3とQ2がオフとなり、Q3とQ2
がオンのときはQ1とQ4がオフとなり、割当周波
数fsに従つて交互にオン、オフを繰返す。変成器
T1の1次側にはQ1〜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
スイツチングされた波形を持つため、バンドパス
フイルタ12によつて不要な成分が除去され、ア
ンテナ等の負荷Zp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。 On the other hand, the signal of assigned frequency f s 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 sent to the transformer T2,
Due to T3, the phase relationship as shown in the figure (Q 1 and Q 3 are 180°,
Q 1 to Q 4 are switched at a phase difference of 180 degrees between Q 2 and Q 4 , and a phase difference of 180 degrees between Q 1 and Q 2 . Q1 ~
Q 4 forms a class D amplifier, for example Q 1 and
When Q 4 is on, Q 3 and Q 2 are off, and Q 3 and Q 2
When is on, Q1 and Q4 are off and alternately turn on and off according to the assigned frequency fs. Since a current whose polarity is reversed as Q1 to Q4 are turned on and off flows through the primary side of the transformer T1, 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 original SSB shown in Figure 3 is applied to the load Zp such as the antenna.
Power is supplied with an envelope similar to a wave.
以上は特に直線性を要求されるSSB波の電力増
幅をD級増幅によつ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%近くまで
上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。 Above we have described a circuit that concretely performs power amplification of SSB waves, which particularly require linearity, using class D amplification, but actual measurements have confirmed that the power efficiency can be increased to nearly 80%. As a highly efficient linear amplifier, it is extremely effective in reducing the size of transmitters.
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
包絡線検波した波形図、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、3…
…BPF、4……前段増幅器、5……整合回路、
6……SSB発生回路、7……レベルシフト回路、
8……3角波発生器、9……コンパレータ、10
……パルス増幅器、11……LPF、12……
BPF、13……制限増幅器、14……前段増幅
器。
Figure 1 is an example of the configuration of a conventional SSB transmitter, Figure 2 is an example of the configuration of an SSB transmitter implementing the present invention, and Figure 3 is an example of the configuration of an SSB transmitter according to the present invention.
The figure is an example of an SSB wave, Figure 4 is a waveform diagram of the SSB wave in Figure 3 with envelope detection, and Figure 5 is a triangular wave and envelope-detected waveforms from a to b in Figure 4. It is an explanatory diagram for comparing and obtaining a PWM wave P. 1...SSB generation circuit, 2...Balanced modulator, 3...
...BPF, 4...Pre-stage amplifier, 5...Matching circuit,
6...SSB generation circuit, 7...Level shift circuit,
8... Triangular wave generator, 9... Comparator, 10
...Pulse amplifier, 11...LPF, 12...
BPF, 13...Limiting amplifier, 14...Pre-stage amplifier.
Claims (1)
れとサンプリング周波数の3角波とによつて得ら
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つて変調される上記シングル
サイドパンド波の振幅制限増幅出力でスイツチさ
れるスイツチング電力増輻器とを備えることを特
徴とするSSB用高効率直線増幅器。1 A circuit that performs envelope detection of a single sideband wave and obtains a pulse width modulated wave obtained by using this and a triangular wave of a sampling frequency, and the above single sideband wave that is modulated by the demodulated wave of the pulse width modulated wave. A high-efficiency linear amplifier for SSB, characterized by comprising a switching power intensifier that is switched by the amplitude-limited amplified output of a sidepan wave.
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 JPS594210A (en) | 1984-01-11 |
| JPH0148687B2 true 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) |
Families Citing this family (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS6480112A (en) * | 1987-09-22 | 1989-03-27 | Japan Broadcasting Corp | Matching circuit |
| JPH061879B2 (en) * | 1987-09-22 | 1994-01-05 | 日本放送協会 | Matching circuit |
-
1982
- 1982-06-29 JP JP57110656A patent/JPS594210A/en active Granted
Non-Patent Citations (1)
| Title |
|---|
| PROCEEDINGS OF THE I R E=1952 * |
Also Published As
| Publication number | Publication date |
|---|---|
| JPS594210A (en) | 1984-01-11 |
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