JPH02302108A - Frequency modulation circuit - Google Patents
Frequency modulation circuitInfo
- Publication number
- JPH02302108A JPH02302108A JP1121357A JP12135789A JPH02302108A JP H02302108 A JPH02302108 A JP H02302108A JP 1121357 A JP1121357 A JP 1121357A JP 12135789 A JP12135789 A JP 12135789A JP H02302108 A JPH02302108 A JP H02302108A
- Authority
- JP
- Japan
- Prior art keywords
- circuit
- carrier
- frequency
- carrier wave
- wave
- 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.)
- Pending
Links
- 230000010355 oscillation Effects 0.000 claims abstract description 19
- 230000010363 phase shift Effects 0.000 claims description 6
- 239000013078 crystal Substances 0.000 abstract description 2
- 239000000969 carrier Substances 0.000 abstract 1
- 239000000872 buffer Substances 0.000 description 6
- 238000010586 diagram Methods 0.000 description 5
- 239000003990 capacitor Substances 0.000 description 4
- 238000000034 method Methods 0.000 description 2
- 230000010356 wave oscillation Effects 0.000 description 2
- 239000002253 acid Substances 0.000 description 1
- 230000005540 biological transmission Effects 0.000 description 1
- 239000003795 chemical substances by application Substances 0.000 description 1
- 238000004891 communication Methods 0.000 description 1
- 230000003111 delayed effect Effects 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 238000005516 engineering process Methods 0.000 description 1
- 238000001308 synthesis method Methods 0.000 description 1
Landscapes
- Oscillators With Electromechanical Resonators (AREA)
Abstract
Description
【発明の詳細な説明】
〔産業上の利用分野〕
本発明は、通信機器、テレビジ目ン受信機、ラジオ受信
機等に使用されている周波数変調(FM)回路に関し、
特に無調整で高度の安定化を図ることができるようにし
た周波数変調回路に関する。[Detailed Description of the Invention] [Industrial Application Field] The present invention relates to a frequency modulation (FM) circuit used in communication equipment, television receivers, radio receivers, etc.
In particular, the present invention relates to a frequency modulation circuit that can achieve a high degree of stability without adjustment.
周波数変調は、搬送波の周波数を信号波の振幅に応じて
中心周波数から偏移させる変調方式であり、その内の間
接周波数変調方式であるベクトル合成方式の周波数変調
回路は、第3図に示すように構成されている。Frequency modulation is a modulation method in which the frequency of a carrier wave is shifted from the center frequency according to the amplitude of a signal wave.The frequency modulation circuit of the vector synthesis method, which is an indirect frequency modulation method, is shown in Figure 3. It is composed of
1は搬送波発振回路でありコイルLとコンデンサCから
なるタンク回路2によりその搬送波fcの発振周波数が
決定される。3はこの搬送波fcを90度移相させる移
相回路で、抵抗とコンデンサで構成される。4はこの9
0度移相された搬送波f c−9゜と信号波fsとを乗
算して位相変調(PM)波を作成する平衡変調回路、5
はこの位相変調波を搬送波fcと加算させて周波数変調
波fF)1を得る加算回路である。1 is a carrier wave oscillation circuit, and the oscillation frequency of the carrier wave fc is determined by a tank circuit 2 consisting of a coil L and a capacitor C. 3 is a phase shift circuit that shifts the phase of this carrier wave fc by 90 degrees, and is composed of a resistor and a capacitor. 4 is this 9
a balanced modulation circuit that creates a phase modulated (PM) wave by multiplying a carrier wave fc-9° phase-shifted by 0 degrees and a signal wave fs; 5
is an adding circuit that adds this phase modulated wave to the carrier wave fc to obtain a frequency modulated wave fF)1.
この回路では、発振回路1で発振された搬送波fcが移
相回路3で90度位相されて平衡変調回路4において信
号波fsと乗算されると、fp+=A−f 5−rc−
’T。In this circuit, when the carrier wave fc oscillated by the oscillation circuit 1 is phased by 90 degrees in the phase shift circuit 3 and multiplied by the signal wave fs in the balanced modulation circuit 4, fp+=A−f 5−rc−
'T.
となり、加算回路5において搬送波fcと加算されて、
周波数変調波fFMとなる。Aは振幅である。is added to the carrier wave fc in the adder circuit 5, and
This becomes a frequency modulated wave fFM. A is the amplitude.
ところがこの回路では、平衡変調回路4の出力を発振回
路1の出力と加算する際、発振回路1に直接電流加算す
る以外に方法がなく、このため周波数偏移幅を広くとる
場合に、無調整の発振素子ではQが高いので、Qの低い
LCのタンク回路2を使用しなければならない。However, in this circuit, when adding the output of the balanced modulation circuit 4 to the output of the oscillation circuit 1, there is no other way than to add the current directly to the oscillation circuit 1. Therefore, when widening the frequency deviation width, it is difficult to add the current to the oscillation circuit 1 without adjustment. Since the oscillation element has a high Q, an LC tank circuit 2 with a low Q must be used.
従って、バラツキの問題が生じ、更に移相回路3におい
てもコンデンサを使用するのでここで得られる搬送波f
。−、。の振幅のバラツキが更に加わり、集積回路化し
た場合には周波数偏移幅のバラツキに直接影響が生じる
という問題があった。Therefore, a problem of variation occurs, and since a capacitor is also used in the phase shift circuit 3, the carrier wave f obtained here is
. -,. Further, there is a problem in that the variation in the amplitude is further added, and when integrated circuits are implemented, the variation in the frequency deviation width is directly affected.
本発明はこのような点に鑑みてなされたものであり、そ
の目的は無調整化、周波数の安定化、周波数偏移幅の安
定化を実現した周波数変調回路を提供することである。The present invention has been made in view of these points, and its purpose is to provide a frequency modulation circuit that eliminates adjustment, stabilizes the frequency, and stabilizes the frequency deviation width.
〔課題を解決するための手段]
このために本発明は、搬送波を90度移相してこの移相
波と信号波を乗算することにより位相変調信号を得、該
位相変調信号と上記搬送波とを加算して周波数変調波を
得る周波数変調回路において、
上記搬送波の2倍の周波数の搬送波を発振する発振回路
と、該発振回路からの出力搬送波を2分周すると共に9
0度位相差を持つ2種の搬送波を出力するFF回路と、
該FF回路の一方の出力1般送波と信号波を乗算する平
衡変調回路と、該平衡変調回路から得られる位相変調信
号と上記FF回路から得られる他方の出力搬送波とを加
算する加算回路とを具備するように構成した。[Means for Solving the Problems] For this purpose, the present invention obtains a phase modulated signal by shifting the phase of a carrier wave by 90 degrees and multiplying this phase shifted wave by a signal wave, and then combining the phase modulated signal and the carrier wave. In the frequency modulation circuit that obtains a frequency modulated wave by adding , an oscillation circuit that oscillates a carrier wave with a frequency twice that of the above-mentioned carrier wave, and an oscillation circuit that oscillates a carrier wave with a frequency twice that of the above-mentioned carrier wave, and divides the output carrier wave from the oscillation circuit into two and divides the frequency of the output carrier wave by 9.
An FF circuit that outputs two types of carrier waves with a 0 degree phase difference,
a balanced modulation circuit that multiplies one output general transmission wave of the FF circuit by a signal wave; and an addition circuit that adds the phase modulation signal obtained from the balanced modulation circuit and the other output carrier wave obtained from the FF circuit. It was configured to have the following.
以下、本発明の実施例について説明する。第1図はその
一実施例の周波数変調回路を示す図である。本実施例で
は、搬送波発振回路11の発振素子としてクリスタル1
2を使用し、これにより必要とする搬送波fcの2倍の
周波数の搬送波2fcを発振させている。13はECL
タイプのT−FF回路であり、ここにおいて入力した搬
送波2fcが2分周されて搬送波fc酸成分90度遅れ
た搬送波r C−9゜成分が得られる。14は平衡変調
回路、15は加算回路である。Examples of the present invention will be described below. FIG. 1 is a diagram showing a frequency modulation circuit of one embodiment. In this embodiment, a crystal 1 is used as the oscillation element of the carrier wave oscillation circuit 11.
2 is used, thereby oscillating a carrier wave 2fc having twice the frequency of the required carrier wave fc. 13 is ECL
This is a type of T-FF circuit, in which the frequency of the input carrier wave 2fc is divided by two to obtain a carrier wave rC-9° component delayed by 90 degrees from the carrier wave fc acid component. 14 is a balanced modulation circuit, and 15 is an adder circuit.
本実施例では、平衡変調回路14において信号波fsと
搬送波f c−9゜とが乗算されて、そこから従来と同
様の、
f pH= A−f S−f c−90なる位相変調信
号f工が得られる。この信号fP1.Iが加算回路15
において搬送波fcと加算されることにより周波数変調
信号f2.4が得られる。In this embodiment, the signal wave fs and the carrier wave f c-9° are multiplied in the balanced modulation circuit 14, and from there, the phase modulation signal f of f pH=A-f S-f c-90 is obtained as in the conventional case. can be obtained. This signal fP1. I is the adder circuit 15
A frequency modulated signal f2.4 is obtained by adding it to the carrier wave fc.
このような構成であるので、第3図における構成のよう
な発振回路本体で周波数を変動させる必要がなく、よっ
て高いQをもつ発振素子を使用しても広い周波数偏移を
実現することができ、またRCを使用した移相回路が必
要なくなるので、無調整で安定した周波数変調波を得る
ことができる。With this configuration, there is no need to vary the frequency in the oscillation circuit itself as in the configuration shown in Figure 3, and therefore a wide frequency shift can be achieved even if an oscillation element with a high Q is used. Moreover, since a phase shift circuit using RC is not required, a stable frequency modulated wave can be obtained without adjustment.
第2図はより具体化した周波数変調回路を示す図である
。ここでは、発振回路11からの出、力搬送波2fcを
バッファ16を介してT型FF回路13に取り込み、こ
こにおいて搬送波2fcを搬送波fc、搬送波f、。9
゜、搬送波f9゜1110 %搬送波f e、2’70
のように〃分周すると共に90度つづ位相の異なる搬送
波を得、その内の搬送波fc、搬送波f C41110
をバッファ17.18を介して加算回路15に送ってい
る。また搬送波f c−’l。、搬送波f c+27゜
はバッファ19を介して平衡変調回路14に送り、その
平衡変調回路14において信号波fsと乗算された信号
をバッファ20を介して加算回路15に送っている。よ
って、加算回路15では、上記バッファ18からの搬送
波と位相変調波とを加算するので、周波数変調信号fF
Mが得られる。なお、ここにおけるバッファ16〜20
はタイミング合わせ用である。FIG. 2 is a diagram showing a more specific frequency modulation circuit. Here, the output carrier wave 2fc from the oscillation circuit 11 is taken into the T-type FF circuit 13 via the buffer 16, where the carrier wave 2fc is converted into a carrier wave fc, a carrier wave f, and so on. 9
゜, carrier wave f9゜1110% carrier wave f e, 2'70
The frequency is divided as follows, and carrier waves with different phases of 90 degrees are obtained, among which carrier wave fc and carrier wave f C41110
is sent to the adder circuit 15 via buffers 17 and 18. Also, the carrier wave f c-'l. , carrier wave f c +27° are sent to the balanced modulation circuit 14 via the buffer 19, and a signal multiplied by the signal wave fs in the balanced modulation circuit 14 is sent to the addition circuit 15 via the buffer 20. Therefore, since the adder circuit 15 adds the carrier wave and the phase modulated wave from the buffer 18, the frequency modulated signal fF
M is obtained. Note that buffers 16 to 20 here
is for timing adjustment.
以上説明したように本発明によれば、発振回路に直接位
相変調波を加算することはないので周波数が安定し、ま
た抵抗やコンデンサを使用した移相回路を必要としない
ので調整工数が必要なく、更に集積回路化した際の周波
数偏移幅のバラツキも少なくなる等の利点がある。As explained above, according to the present invention, the frequency is stabilized because the phase modulated wave is not directly added to the oscillation circuit, and there is no need for a phase shift circuit using resistors or capacitors, so there is no need for adjustment man-hours. Furthermore, there are advantages such as less variation in frequency deviation width when integrated circuits are formed.
第1図は本発明の一実施例の周波数変調回路の回路図、
第2図はその回路を具体化した同回路図、第3図は従来
の同回路の回路図である。
代理人 弁理士 長 尾 常 明
第1図
信号波FIG. 1 is a circuit diagram of a frequency modulation circuit according to an embodiment of the present invention,
FIG. 2 is a circuit diagram embodying the circuit, and FIG. 3 is a conventional circuit diagram of the same circuit. Agent Patent Attorney Tsuneaki Nagao Figure 1 Signal Wave
Claims (1)
乗算することにより位相変調信号を得、該位相変調信号
と上記搬送波とを加算して周波数変調波を得る周波数変
調回路において、 上記搬送波の2倍の周波数の搬送波を発振する発振回路
と、該発振回路からの出力搬送波を1/2分周すると共
に90度位相差を持つ2種の搬送波を出力するFF回路
と、該FF回路の一方の出力搬送波と信号波を乗算する
平衡変調回路と、該平衡変調回路から得られる位相変調
信号と上記FF回路から得られる他方の出力搬送波とを
加算する加算回路とを具備することを特徴とする周波数
変調回路。(1) A frequency modulation circuit that obtains a phase modulation signal by shifting the phase of a carrier wave by 90 degrees and multiplying this phase shift wave by a signal wave, and obtains a frequency modulation wave by adding the phase modulation signal and the carrier wave. an oscillation circuit that oscillates a carrier wave with twice the frequency of the carrier wave; an FF circuit that divides the output carrier wave from the oscillation circuit into 1/2 and outputs two types of carrier waves having a 90 degree phase difference; A balanced modulation circuit that multiplies one output carrier wave of the FF circuit by a signal wave, and an addition circuit that adds the phase modulation signal obtained from the balanced modulation circuit and the other output carrier wave obtained from the FF circuit. A frequency modulation circuit characterized by:
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP1121357A JPH02302108A (en) | 1989-05-17 | 1989-05-17 | Frequency modulation circuit |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP1121357A JPH02302108A (en) | 1989-05-17 | 1989-05-17 | Frequency modulation circuit |
Publications (1)
Publication Number | Publication Date |
---|---|
JPH02302108A true JPH02302108A (en) | 1990-12-14 |
Family
ID=14809267
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP1121357A Pending JPH02302108A (en) | 1989-05-17 | 1989-05-17 | Frequency modulation circuit |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH02302108A (en) |
-
1989
- 1989-05-17 JP JP1121357A patent/JPH02302108A/en active Pending
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