JPH0446492B2 - - Google Patents

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Publication number
JPH0446492B2
JPH0446492B2 JP5442284A JP5442284A JPH0446492B2 JP H0446492 B2 JPH0446492 B2 JP H0446492B2 JP 5442284 A JP5442284 A JP 5442284A JP 5442284 A JP5442284 A JP 5442284A JP H0446492 B2 JPH0446492 B2 JP H0446492B2
Authority
JP
Japan
Prior art keywords
wave
output
frequency
converted
interference
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
Application number
JP5442284A
Other languages
Japanese (ja)
Other versions
JPS60198926A (en
Inventor
Shigeru Yamazaki
Hiroo Arata
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.)
Japan Broadcasting Corp
Original Assignee
Japan Broadcasting Corp
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 Japan Broadcasting Corp filed Critical Japan Broadcasting Corp
Priority to JP5442284A priority Critical patent/JPS60198926A/en
Publication of JPS60198926A publication Critical patent/JPS60198926A/en
Publication of JPH0446492B2 publication Critical patent/JPH0446492B2/ja
Granted legal-status Critical Current

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Description

【発明の詳細な説明】 技術分野 本発明は、例えばテレビジヨン放送波など所望
の受信振幅変調信号波に異常伝搬等により混入し
たFM放送波等の周波数変調あるいは位相変調な
どの角度変調を施した妨害波を除去する妨害角度
変調波除去受信方式に関し、所望の受信振幅変調
信号波をほとんど損傷することなく妨害角度変調
波をほぼ完全に除去し得るようにしたものであ
る。
[Detailed Description of the Invention] Technical Field The present invention is directed to frequency modulation or angle modulation such as phase modulation of FM broadcast waves mixed into a desired received amplitude modulated signal wave such as television broadcast waves due to abnormal propagation. The present invention relates to a reception method for removing interference angle modulated waves that removes interference waves, and is capable of almost completely removing interference angle modulation waves without substantially damaging a desired received amplitude modulated signal wave.

従来技術 従来、この種妨害角度変調波を除去して所望の
受信振幅変調信号波を受信するには、専らノツチ
フイルタを用いて妨害角度変調波の主要成分を帯
域除去する受信方式が用いられていた。かくし
て、周波数帯域の拡がりを有する妨害角度変調波
を十分に除去するようにすれば、同じ帯域内の所
望信号成分も同時に除去されるために受信信号に
副次的な歪みが生じ、総合的に受信信号の品位を
低下させる結果となる欠点があつた。かかる所望
信号成分の欠除を伴わずに妨害角度変調波のみを
相殺除去し得るようにするために、適切に離隔配
置した複数本のアンテナからのアンテナ出力をレ
ベルおよび位相を適切に調整して合成することに
よりアンテナ指向性にヌル点を設け、そのヌル点
の方向を妨害角度変調波の到来方向に一致させる
ようにした受信方式も従来用いられていたが、元
来、異常伝搬等によつて混入するFM放送波等の
妨害角度変調波はその到来方向がふらついたりす
るので、常時、上述したアンテナヌル点の方向の
再調整を必要とする欠点があり、さらに、複数の
この種妨害波が同時に到来した場合には対処し切
れない、という欠点もあつた。
Prior Art Conventionally, in order to remove this type of interference angle modulated wave and receive a desired received amplitude modulated signal wave, a receiving method was used in which a notch filter was used exclusively to remove the main components of the interference angle modulated wave in the band. . In this way, if the interfering angle modulated wave with a spread frequency band is sufficiently removed, the desired signal component within the same band will also be removed at the same time, causing secondary distortion in the received signal, and the overall There was a drawback that resulted in a reduction in the quality of the received signal. In order to cancel out and remove only the interfering angle modulated wave without eliminating the desired signal component, the levels and phases of the antenna outputs from a plurality of appropriately spaced antennas are adjusted appropriately. Conventionally, a receiving method has been used in which a null point is provided in the antenna directivity through synthesis, and the direction of the null point is made to match the arrival direction of the interfering angle modulated wave. The direction of arrival of interfering angle-modulated waves such as FM broadcast waves that are mixed in with the antenna may fluctuate, so there is a drawback that the direction of the antenna null point needs to be readjusted all the time. Another drawback was that it would not be possible to fully deal with the situation if they arrived at the same time.

発明の要点 本発明の目的は、上述した従来の欠点を除去
し、所望の受信信号波には何ら実質的な損傷を与
えることなく、しかも、無調整にて妨害角度変調
波を常時ほぼ完全に受信信号波から除去し得るよ
うにした妨害角度変調波除去受信方式を提供する
ことにある。
SUMMARY OF THE INVENTION An object of the present invention is to eliminate the above-mentioned conventional drawbacks, to eliminate any substantial damage to the desired received signal waves, and to eliminate the interfering angle modulated waves almost completely without any adjustment. An object of the present invention is to provide a reception method for removing interference angle modulated waves that can be removed from received signal waves.

すなわち、本発明妨害角度変調波除去受信方式
は、受信信号波に混入した妨害角度変調波を積極
的に受信して復調し、その復調出力を負帰還して
受信信号波全体に逆変調を施し、妨害角度変調波
を周波数偏移の小さい帯域圧縮した信号にして復
元受信信号から除去するようにしたものであり、
妨害角度変調波が混入した受信振幅変調信号波を
電圧制御局部発振器の発振出力によりそれぞれ周
波数変換して第1および第2の変換出力波を形成
し、前記第1の変換出力波を、当該変換出力波の
前記妨害角度変調波が混入した側波帯成分の帯域
を通過帯域とするバンドパスフイルタを介し、前
記電圧制御局部発振器の発振出力により周波数逆
変換した逆変換出力波について角度復調検波して
得た復調出力を負帰還して前記電圧制御局部発振
器の発振出力周波数を制御することにより前記第
1および前記第2の変換出力波に混入した前記妨
害角度変調波の占有帯域を圧縮するとともに、前
記第2の変換出力波の当該占有帯域が圧縮された
妨害角度変調波が混入した側波帯成分を前記バン
ドパスフイルタに対応するフイルタを介して抽出
し、前記占有帯域が圧縮された妨害角度変調波の
帯域を通過帯域通過とする狭帯域通過フイルタを
介して前記第1の変換出力波を前記第2の変換出
力波に等振幅逆位相合成することにより前記第2
の変換出力波の前記フイルタを介して抽出した周
波数変換出力側波帯成分から前記占有帯域が圧縮
された妨害角度変調波を前記第1および前記第2
の変換出力波間で相殺して除去した後に、その除
去して得た出力波を前記電圧制御局部発振器の発
振出力により周波数逆変換して前記妨害角度変調
波が混入しない受信振幅変調信号波に復元するよ
うにしたことを特徴とするものである。
That is, the interfering angle modulated wave removal reception method of the present invention actively receives and demodulates the interfering angle modulated wave mixed into the received signal wave, and negative-feeds back the demodulated output to apply inverse modulation to the entire received signal wave. , the interfering angle modulated wave is converted into a band-compressed signal with a small frequency deviation and removed from the restored received signal,
A received amplitude modulated signal wave mixed with a disturbance angle modulated wave is frequency-converted by the oscillation output of a voltage-controlled local oscillator to form first and second converted output waves, and the first converted output wave is converted into the first converted output wave. Angle demodulation detection is performed on the inversely converted output wave whose frequency has been inversely converted by the oscillation output of the voltage controlled local oscillator through a bandpass filter whose passband is the band of the sideband component mixed with the interference angle modulated wave of the output wave. By controlling the oscillation output frequency of the voltage-controlled local oscillator by negative feedback of the demodulated output obtained by , extracting the sideband component mixed with the interference angle modulated wave in which the occupied band of the second converted output wave is compressed through a filter corresponding to the bandpass filter, and extracting the sideband component mixed with the interference angle modulated wave in which the occupied band is compressed; The first converted output wave is equal-amplitude and anti-phase synthesized with the second converted output wave through a narrow band pass filter whose pass band is the band of the angle modulated wave.
A disturbance angle modulated wave in which the occupied band is compressed is obtained from the frequency conversion output sideband component extracted through the filter of the conversion output wave of the first and second
After canceling and eliminating the converted output waves of It is characterized by the fact that it is made to do so.

なお、ここにいう復元は、入力信号に対し、同
一局部発振出力により、周波数の変換を施した後
に逆変換してもとの周波数に戻すことを指す。
Note that restoration here refers to converting the frequency of the input signal using the same local oscillation output, and then inversely converting the input signal to return it to the original frequency.

実施例 以下に図面を参照して実施例につき本発明を詳
細に説明する。
EXAMPLES The present invention will be explained in detail below using examples with reference to the drawings.

本発明妨害角度変調波除去受信方式は、妨害波
自体の変調により帯域の拡がりを有する妨害角度
変調波を受信信号中から除去するに当つて、ま
ず、妨害波の帯域を圧縮して、その除去に伴い所
望信号成分の欠除が生ずるにしても、信号成分欠
除が生ずる帯域幅をできるだけ局限したうえで、
狭い帯域幅の妨害波を除去するようにするのであ
るが、本発明方式による妨害波除去の起点をなす
角度変調波の帯域圧縮に関しては、第1図に示す
回路方式が従来知られている。図示の構成による
角度変調波帯域圧縮回路装置においては、FM放
送波等の入力角度変調波を乗算器1に導いて、電
圧制御発振器6の発振出力との乗算を行なうこと
によりその発振出力を局部発振とする周波数変換
を施し、バンドパスフイルタ3を介して取出した
上下いずれかの側波帯の変換出力を乗算器2に導
き、電圧制御発振器6の上述と同じ発振出力を局
部発振として上述とは逆の周波数変換を施し、同
じくバンドパスフイルタ20を介して入力角度変
調波を復元し、かかる周波数変換とその逆変換と
により復元した角度変調波をリミツタ4および
FM検波回路5に順次に導いて復調し、その復調
出力をローパスフイルタ7を介して電圧制御発振
器6に負帰還し、復調出力信号、したがつて、入
力角度変調波の周波数偏移に追従して局部発振周
波数を変化させることにより、乗算器1および2
からそれぞれ得られる変換出力波および逆変換出
力波の帯域幅を圧縮して、負帰還率を増大させれ
ば中心搬送波周波数成分のみに局限し得るように
なつている。
The interference angle modulated wave removal reception method of the present invention first compresses the band of the interference wave and removes it when removing the interference angle modulation wave whose band is expanded by modulating the interference wave itself from the received signal. Even if deletion of the desired signal component occurs due to
The purpose is to remove interference waves with a narrow bandwidth, and the circuit system shown in FIG. 1 is conventionally known for band compression of angle modulated waves, which is the starting point of interference wave removal by the method of the present invention. In the angle modulated wave band compression circuit device having the configuration shown in the figure, an input angle modulated wave such as an FM broadcast wave is guided to the multiplier 1, and multiplied by the oscillation output of the voltage controlled oscillator 6, thereby localizing the oscillation output. Frequency conversion is applied as oscillation, and the converted output of either the upper or lower sideband taken out via the bandpass filter 3 is led to the multiplier 2, and the same oscillation output as described above of the voltage controlled oscillator 6 is used as the local oscillation. performs reverse frequency conversion, similarly restores the input angle modulated wave via the bandpass filter 20, and transmits the angle modulated wave restored by such frequency conversion and its inverse conversion to the limiter 4 and
The signal is sequentially guided to the FM detection circuit 5 for demodulation, and the demodulated output is negatively fed back to the voltage controlled oscillator 6 via the low-pass filter 7 to follow the demodulated output signal and therefore the frequency deviation of the input angle modulated wave. multipliers 1 and 2 by changing the local oscillation frequency.
By compressing the bandwidth of the converted output wave and the inversely converted output wave respectively obtained from , and increasing the negative feedback rate, it is possible to localize only to the center carrier frequency component.

すなわち、入力端子8に供給する受信入力信号
波の周波数をi+Δとしてその周波数偏移Δに
よつて決まる帯域幅を圧縮するに当つて、電圧制
御発振器6の発振周波数をlとし、乗算器1およ
び2の変換出力および逆変換出力の周波数をそれ
ぞれ1および2とすると、例えば、 (i+Δ)−l1 (1) 1l2 (2) なる関係が成立つ。これらの式(1)および(2)から i+Δ=2 (3) となる。したがつて、乗算器2の逆変換出力周波
2は、局部発振周波数lの如何に拘わりなく、
つねに受信入力信号周波数i+Δに等しく、逆変
換出力として受信入力信号波が復元される。この
復元受信入力信号波の復調出力を電圧制御発振器
に印加して局部発振周波数lを負帰還制御する
と、帰還係数をαとし、電圧制御発振周波数の負
帰還制御に伴う変化範囲の中心周波数をpとし
て、局部発振周波数lは、 lp+α・Δ (4) となる。この式(4)を式(1)に代入して整理すると、
つぎの式(5)が得られる。
That is, when the frequency of the received input signal wave supplied to the input terminal 8 is i + Δ and the bandwidth determined by the frequency deviation Δ is compressed, the oscillation frequency of the voltage controlled oscillator 6 is l , and the multiplier 1 When the frequencies of the conversion output and the inverse conversion output of 2 and 2 are respectively 1 and 2 , the following relationship holds true, for example: ( i + Δ) − l = 1 (1) 1 + l = 2 (2). From these equations (1) and (2), i + Δ= 2 (3). Therefore, regardless of the local oscillation frequency l , the inverse conversion output frequency 2 of the multiplier 2 is
The received input signal wave is always equal to the received input signal frequency i + Δ, and the received input signal wave is restored as the inversely transformed output. When the demodulated output of this restored received input signal wave is applied to the voltage controlled oscillator and the local oscillation frequency l is controlled by negative feedback, the feedback coefficient is set to α, and the center frequency of the change range due to the negative feedback control of the voltage controlled oscillation frequency is set to p. , the local oscillation frequency l is l = p + α・Δ (4). Substituting this equation (4) into equation (1) and organizing it, we get
The following equation (5) is obtained.

ip)+(1−α)・Δ=1 (5) したがつて、帰還係数α=0のときには、受信
入力信号波の周波数偏移Δがそのままバンドパ
スフイルタ3に加わることになり、また、帰還係
数α=1のときには受信入力信号波の周波数偏移
Δが圧縮除去されて、バンドパスフイルタ3に
は変換出力搬送周波数成分のみが加わることにな
る。すなわち、受信入力信号波の搬送周波数i
変換出力中心周波数1に変換されて、周波数偏移
を伴わない単一の搬送波として変換出力に現われ
ることになり、したがつて、出力端子10にはか
かる無変調搬送波信号が現われる。
( i + p ) + (1-α)・Δ= 1 (5) Therefore, when the feedback coefficient α=0, the frequency deviation Δ of the received input signal wave is directly applied to the bandpass filter 3. When the feedback coefficient α=1, the frequency deviation Δ of the received input signal wave is compressed and removed, and only the converted output carrier frequency component is applied to the bandpass filter 3. That is, the carrier frequency i of the received input signal wave is converted to the conversion output center frequency 1 , and appears in the conversion output as a single carrier wave with no frequency deviation. An unmodulated carrier signal appears.

本発明方式の妨害角度変調波除去の一実施例に
おいては、上述した角度変調波帯域圧縮を受信信
号波に混入している妨害角度変調波に施して、妨
害波を無変調搬送波の状態にして抽出するととも
に、受信信号波全体に同一信号処理を施して妨害
波混入帯域を圧縮し、双方を等振幅逆位相合成す
ることにより、無変調搬送波の状態にした妨害波
を相殺除去するように妨害波除去用受信回路を構
成する。
In one embodiment of the interference angle modulated wave removal method of the present invention, the above-mentioned angle modulated wave band compression is applied to the interference angle modulated wave mixed in the received signal wave, so that the interference wave becomes an unmodulated carrier wave. At the same time, the same signal processing is applied to the entire received signal wave to compress the interference wave mixed band, and by combining both with equal amplitude and antiphase, the interference wave is canceled out and removed in the state of an unmodulated carrier wave. Configure a receiving circuit for wave removal.

本発明方式のかかる妨害波除去用受信回路の構
成例を第2図に示す。第2図示の回路構成におい
て破線枠により囲んで示した回路部分は第1図示
の回路構成と全く同一に構成してあり、この回路
部分によつて、まず、受信信号波に混入している
妨害角度変調波を、第1図につき上述したように
して、無変調妨害搬送波の状態にする。
FIG. 2 shows an example of the configuration of a receiving circuit for removing interference waves according to the method of the present invention. In the circuit configuration shown in the second diagram, the circuit part shown surrounded by a broken line frame is configured exactly the same as the circuit configuration shown in the first diagram, and this circuit part first allows interference to be mixed into the received signal wave. The angle modulated wave is brought into the state of an unmodulated interfering carrier as described above with respect to FIG.

一方、第2図示の回路構成において、破線枠外
に付加した回路部分は、前述したように受信信号
波全体に同様の信号処理を施したうえで、破線枠
の内と外とにおいて無変調妨害搬送波を等振幅逆
位相合成して相殺除去するように構成してある。
なお、破線枠内の回路部分における電圧制御発振
器6に接続してある中心周波数制御回路16は、
電圧制御発振周波数の前述した負帰還制御に伴う
変化範囲の中心周波数pを制御するための回路部
分である。すなわち、入力端子8からの受信入力
信号波を乗算器11に導き、電圧制御発振器6の
発振出力との乗算を行なつて、発振器6の発振出
力を局部発振とした周波数変換を施し、バンドパ
スフイルタ12により破線枠内におけると同じ側
波帯に位置する側の変換出力を取出して減算回路
14に供給すれば、その変換出力に含まれている
妨害波成分は、破線枠内においてバンドパスフイ
ルタ3から取出した妨害波成分と同じ無変調妨害
搬送波の状態になつている。破線枠内の無変調妨
害搬送波成分を、その妨害搬送波周波数近傍のみ
を通過帯域とする狭帯域バンドパスフイルタ18
および破線枠の内外における信号レベルおよび信
号遅延時間の相違を修正除去するためのレベル・
遅延時間調整回路13を介して同じく減算回路1
4に導き、上述した変換出力信号波より減算する
ことにより、妨害波の相殺除去を行なう。このよ
うにして妨害波成分を相殺除去した変換出力信号
波を乗算器15に導いて、電圧制御発振器6から
の同一局部発振によつて乗算器11におけるとは
逆の周波数変換を施し、バンドパスフイルタ17
を介し、受信入力信号波と同一帯域の逆変換出力
信号波を抽出して出力端子19から取出す。
On the other hand, in the circuit configuration shown in the second diagram, the circuit portion added outside the dashed line frame performs the same signal processing on the entire received signal wave as described above, and then generates unmodulated interference carriers inside and outside the dashed line frame. The configuration is such that equal amplitude and antiphase are combined to cancel each other out.
Note that the center frequency control circuit 16 connected to the voltage controlled oscillator 6 in the circuit portion within the broken line frame is as follows.
This is a circuit portion for controlling the center frequency p of the range of change of the voltage controlled oscillation frequency due to the above-mentioned negative feedback control. That is, the received input signal wave from the input terminal 8 is guided to the multiplier 11, where it is multiplied by the oscillation output of the voltage controlled oscillator 6, frequency conversion is performed using the oscillation output of the oscillator 6 as a local oscillation, and a bandpass signal is generated. If the filter 12 extracts the converted output located in the same sideband as that within the dashed line frame and supplies it to the subtraction circuit 14, the interference wave component contained in the converted output will be filtered through the bandpass filter within the dashed line frame. It is now in the state of an unmodulated interference carrier wave, which is the same as the interference wave component extracted from No. 3. A narrowband bandpass filter 18 whose pass band is only near the frequency of the unmodulated interfering carrier wave within the dashed line frame.
and level and
Similarly, the subtraction circuit 1 is connected to the subtraction circuit 1 via the delay time adjustment circuit 13.
4 and subtracted from the above-mentioned converted output signal wave to cancel and remove the interference wave. The converted output signal wave whose interference wave components have been canceled out and removed in this way is guided to the multiplier 15, where it is subjected to frequency conversion opposite to that in the multiplier 11 by the same local oscillation from the voltage controlled oscillator 6, and is passed through the bandpass. Filter 17
, the inversely transformed output signal wave having the same band as the received input signal wave is extracted and taken out from the output terminal 19 .

すなわち、所望の受信入力信号波の搬送波周波
数をdとし、妨害波の周波数を前述したようにi
+Δとすると、帰還係数α=1のときには乗算
器11の変換出力中における妨害波成分の周波数
3は、破線枠内におけると同様に、周波数偏移
Δがなくなり、局部発振周波数lはその変化範囲
の中心周波数pとなるので、 3ip (6) となる。一方、乗算器11の変換出力中における
受信信号波は、局部発振とする電圧制御発振器6
の発振周波数lが妨害波復調出力による負帰還制
御を受けた結果であるから、妨害角度変調波にお
けるとは逆に、周波数偏移Δの周波数変調を受
け、その周波数d′は、 d′=(d−Δ)−do (7) となる。しかして、式(6)の妨害波周波数3は破線
枠内の端子10に現われた無変調妨害搬送波周波
数と同一であるから、その端子10から狭帯域バ
ンドパスフイルタ18およびレベル・遅延時間調
整回路13を介して取出した無変調妨害搬送波と
上述したバンドパスフイルタ12からの変換出力
信号波中に混入している周波数3の妨害波とを減
算回路14に供給して減算すなわち等振幅逆位相
合成による相殺除去を行なえば、式(7)による周波
d′の変換出力信号波成分のみが得られること
になる。その変換出力信号波成分を乗算器15に
導いて電圧制御発振器6からの式(4)においてα=
1とした局部発振周波数lp+Δの局部発振に
より周波数逆変換を施すと、式(7)を援用して d′+l=〔a−Δ)−p〕 +(p+Δ)=d (8) なる周波数の逆変換出力信号波が得られ、受信入
力信号波が混入妨害波成分を除いて完全に復元さ
れることになる。なお、狭帯域バンドパスフイル
タ18は、無変調妨害搬送波のみを波抽出する
ためのものであるから、波出力の無変調妨害搬
送波の振幅情報が損なわれないフイルタであれ
ば、如何なる狭帯域通過フイルタをも使用し得
る。
That is, the carrier frequency of the desired received input signal wave is d , and the frequency of the interference wave is i as described above.
+Δ, when the feedback coefficient α=1, the frequency of the interference wave component in the conversion output of the multiplier 11
3 , the frequency deviation Δ disappears and the local oscillation frequency l becomes the center frequency p of its range of change, as in the broken line frame, so 3 = ip (6). On the other hand, the received signal wave in the converted output of the multiplier 11 is generated by the voltage controlled oscillator 6 which generates local oscillation.
Since the oscillation frequency l is the result of negative feedback control by the interference wave demodulation output, it is subjected to frequency modulation with a frequency deviation Δ, contrary to the interference angle modulated wave, and its frequency d ′ is d ′= ( d −Δ)−do (7). Therefore, since the interference wave frequency 3 in equation (6) is the same as the unmodulated interference carrier frequency appearing at the terminal 10 within the broken line frame, the interference wave frequency 3 from the terminal 10 is connected to the narrowband bandpass filter 18 and the level/delay time adjustment circuit. The unmodulated interfering carrier wave taken out through the filter 13 and the interfering wave of frequency 3 mixed in the converted output signal wave from the bandpass filter 12 described above are supplied to the subtracting circuit 14 for subtraction, that is, equal amplitude and antiphase synthesis. If cancellation is removed by , only the converted output signal wave component of frequency d ′ according to equation (7) will be obtained. The converted output signal wave component is guided to the multiplier 15, and in equation (4) from the voltage controlled oscillator 6, α=
When inverse frequency conversion is performed by local oscillation with a local oscillation frequency l = p + Δ set to 1, using equation (7), d ′+ l = [ a − Δ) − p ] + ( p + Δ) = d ( 8) An inversely converted output signal wave with a frequency of Note that since the narrow band band pass filter 18 is for extracting only the unmodulated interfering carrier wave, any narrow band pass filter may be used as long as it does not damage the amplitude information of the unmodulated interfering carrier wave output. can also be used.

また、妨害波の搬送波周波数iが変化した場合
には、前述した中心周波数制御回路16により、
その妨害波周波数iの変化に応じて電圧制御発振
器6の発振周波数変化範囲の中心周波数pを変化
させることのみにより、他のバンドパスフイルタ
については、いずれも、その通過帯域を固定した
ままで、妨害搬送波周波数iの変化に追随して上
述したとおりの妨害波相殺除去を遂行することが
できる。
In addition, when the carrier frequency i of the interference wave changes, the center frequency control circuit 16 described above
By simply changing the center frequency p of the oscillation frequency change range of the voltage controlled oscillator 6 in accordance with the change in the interference wave frequency i , all other bandpass filters can maintain their passbands fixed. The above-described interference cancellation and cancellation can be performed following the change in the interference carrier frequency i .

また、破線枠内のバンドパスフイルタ3の通過
帯域は妨害角度変調波のスペクトル分布帯域幅と
ほぼ同じにし、破線枠外のバンドパスフイルタ1
2の通過帯域は、乗算器11の変換出力として得
られる周波数偏移Δの周波数変調受信信号波の
(7)式に基づく信号帯域のうち、局部発振周波数l
を中心とした上下両側波帯の一方の不要側波帯成
分を除去し得れば足りるので、上下いずれの側の
周波数変換出力側波帯を使用するかに応じてロー
パスフイルタあるいはハイパスフイルタを代替使
用することができる。なお、妨害波の相殺除去に
支障を生じると見られる狭帯域バンドパスフイル
タ18による位相シフトなどは、レベル・遅延時
間調整回路13により一括して補正すれば、以後
再調整の必要はない。
Furthermore, the passband of the bandpass filter 3 within the dashed line frame is approximately the same as the spectral distribution bandwidth of the interfering angle modulated wave, and the passband of the bandpass filter 3 outside the dashed line frame is
The passband of No. 2 is the frequency modulated received signal wave with a frequency deviation Δ obtained as the conversion output of the multiplier 11.
Local oscillation frequency l of the signal band based on equation (7)
It is sufficient to remove unnecessary sideband components from one of the upper and lower sidebands centered on can be used. It should be noted that if the phase shift caused by the narrowband bandpass filter 18, which seems to interfere with the cancellation and removal of interference waves, is corrected all at once by the level/delay time adjustment circuit 13, there is no need for readjustment thereafter.

つぎに、第2図示の構成例における中心周波数
制御回路16を妨害搬送波周波数に関連した制御
情報に応動させることにより、妨害搬送波周波数
の変化等に自動的に追従して混入妨害波成分零の
状態に収斂させるようにした場合の本発明方式に
よる受信回路の概略構成の例を第3図に示す。図
示の構成例は、異常伝搬等により周波数割当ての
領域を超えてテレビジヨン放送波に混入したFM
放送波の妨害を自動的に除去するように構成した
ものである。すなわち、第2図示の構成における
復元受信信号出力端子19に接続したテレビジヨ
ン受信機内の映像検波回路21の検波出力映像信
号に含まれた妨害波周波数と映像搬送波周波数と
の差に相当するビート周波数成分を、その検波出
力映像信号を増幅回路22を介して供給したビー
ト検出回路23によつて検出する。なお、このビ
ート検出回路23には増幅回路22からの映像信
号を供給した同期分離回路24により分離抽出し
た同期信号を印加して、映像内容の影響を受けな
い妨害搬送波周波数のみに依存した正確なビート
周波数を同期信号区間に検出する。その検出出力
のビート周波数に比例した電圧を得て、前述した
中心周波数制御回路16に供給し、そのビート周
波数の変動には拘わりなく、乗算器1からの変換
妨害搬送波の周波数が所定の値となるように局部
発振周波数変化範囲の中心周波数pを自動制御す
れば、妨害波の自動追尾除去を行なうことができ
る。
Next, by making the center frequency control circuit 16 in the configuration example shown in the second figure respond to the control information related to the interfering carrier frequency, it is possible to automatically follow changes in the interfering carrier frequency and achieve a state where the mixed interfering wave component is zero. FIG. 3 shows an example of a schematic configuration of a receiving circuit according to the method of the present invention in which the signals are converged. The illustrated configuration example shows FM that has crossed the frequency allocation range and mixed into television broadcast waves due to abnormal propagation, etc.
It is configured to automatically remove interference from broadcast waves. That is, the beat frequency corresponds to the difference between the interference wave frequency included in the detected output video signal of the video detection circuit 21 in the television receiver connected to the restored received signal output terminal 19 in the configuration shown in the second diagram and the video carrier frequency. The component is detected by a beat detection circuit 23 to which the detected output video signal is supplied via an amplifier circuit 22. The beat detection circuit 23 is supplied with a synchronization signal separated and extracted by the synchronization separation circuit 24 that has supplied the video signal from the amplifier circuit 22, and is used to detect accurate synchronization signals that depend only on the interfering carrier frequency, which is not affected by the video content. Detect the beat frequency in the synchronization signal section. A voltage proportional to the beat frequency of the detection output is obtained and supplied to the center frequency control circuit 16 described above, so that the frequency of the converted interfering carrier wave from the multiplier 1 is set to a predetermined value, regardless of fluctuations in the beat frequency. If the center frequency p of the local oscillation frequency change range is automatically controlled so that the interference wave can be automatically tracked and removed.

なお、第2図示の構成例においては、説明の便
宜上、破線枠の枠内と枠外とに全く同様に構成し
て全く同様に作用する乗算器1および乗算器11
よりなる2個の周波数変換段をそれぞれ別個に設
けたが、周波数変換段は、そのいずれか一方のみ
を設けて、その変換出力を枠内と枠外とに分岐し
て使用するように変更し得ること勿論である。
In the configuration example shown in the second diagram, for convenience of explanation, the multiplier 1 and the multiplier 11 are configured in exactly the same manner and operate in the same way inside and outside the broken line frame.
Although two frequency conversion stages consisting of Of course.

効 果 以上の説明から明らかなように、本発明によれ
ば、一般の受信入力信号波に混入した妨害角度変
調波のスペクトル分布範囲を著しく局限し、究極
的には単一の妨害搬送波に変換して混入妨害波を
除去するので、原帯域のままの混入妨害波を除去
した場合に比して所望信号波成分に及ぼす悪影
響、特に、前述の実施例に述べたように相殺除去
の手法を用いた場合には位相歪みや映像信号成分
の損傷を実質的に無視して妨害波除去を行ない得
るという格別の効果が得られる。しかも、特に精
密調整を要することなく、低廉な回路部品による
簡単な構成の回路装置によつて安定確実に妨害角
度変調波の除去を行なうことができる。
Effects As is clear from the above explanation, according to the present invention, the spectral distribution range of the interfering angle modulated wave mixed into the general received input signal wave is significantly localized, and ultimately converted into a single interfering carrier wave. Since the interfering interference waves are removed by using the cancellation method described in the previous embodiment, there is no adverse effect on the desired signal wave component than when interfering interfering waves are removed in the original band. When used, a special effect can be obtained in that interference waves can be removed while substantially ignoring phase distortion and damage to video signal components. In addition, the interfering angle modulated wave can be removed stably and reliably using a simple circuit device using inexpensive circuit components without requiring particularly precise adjustment.

なお、本発明受信方式を例えばテレビジヨン放
送波の受信信号中に混入したFM放送波除去に適
用した場合には、第1図に示したFM検波回路5
により復調したFM放送波信号中に映像信号成分
が混入して復調FM放送波信号のS/Nを劣化さ
せることになるが、相殺除去すべき妨害波の方が
角度変調波であるがために、かかる復調FM放送
波信号のS/N劣化はいわゆるFM改善度だけ軽
減されており、妨害波の強度が大なるほど、映像
信号成分によるS/N劣化の程度は軽減される。
Note that when the receiving method of the present invention is applied to, for example, removing FM broadcast waves mixed in the received signal of television broadcast waves, the FM detection circuit 5 shown in FIG.
The video signal component will mix into the demodulated FM broadcast wave signal and degrade the S/N of the demodulated FM broadcast wave signal, but since the interference wave that should be canceled out is the angle modulated wave. The S/N deterioration of such a demodulated FM broadcast wave signal is reduced by the so-called FM improvement degree, and as the intensity of the interference wave increases, the degree of S/N deterioration due to the video signal component is reduced.

また、本発明方式による妨害角度変調波除去受
信回路を異なる妨害搬送波周波数iにそれぞれ対
応させて複数段縦続接続すれば、受信信号波に混
入した複数種類の妨害角度変調波をそれぞれ確実
に除去することができ、さらに、局部発振器とす
る電圧制御発振器の発振周波数変化範囲の中心周
波数pを適切に制御すれば、無調整にて広い周波
数範囲内の妨害角度変調波を自動的に追跡して除
去することもでき、混入妨害波の自動追尾除去回
路装置を実現することができる。
Furthermore, by cascading multiple stages of interference angle modulated wave removal receiving circuits according to the present invention, each corresponding to a different interference carrier frequency i , multiple types of interference angle modulation waves mixed in the received signal wave can be reliably removed. Furthermore, if the center frequency p of the oscillation frequency variation range of the voltage controlled oscillator used as a local oscillator is appropriately controlled, the interfering angle modulated wave within a wide frequency range can be automatically tracked and removed without adjustment. It is also possible to realize an automatic tracking and removal circuit device for mixed interference waves.

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

第1図は本発明妨害角度変調波除去受信方式の
根幹をなす角度変調波帯域圧縮回路装置の構成を
示すブロツク線図、第2図は本発明方式による妨
害角度変調波除去受信回路の詳細構成例を示すブ
ロツク線図、第3図は同じくその妨害波除去受信
回路の一部の他の構成例を示すブロツク線図であ
る。 1,2,11,15…乗算器、3,12,1
7,20…バンドパスフイルタ、4…リミツタ、
5…FM検波回路、6…電圧制御発振器、7…ロ
ーパスフイルタ、8…入力端子、9,10,19
…出力端子、13…レベル・遅延時間調整回路、
14…減算回路、16…中心周波数制御回路、1
8…狭帯域バンドパスフイルタ、21…映像検波
回路、22…増幅回路、23…ビート検出回路、
24…同期分離回路。
Fig. 1 is a block diagram showing the configuration of the angle modulated wave band compression circuit device which forms the basis of the interference angle modulated wave removal reception method of the present invention, and Fig. 2 is the detailed configuration of the interference angle modulated wave removal reception circuit according to the invention method. FIG. 3 is a block diagram showing another example of the structure of a part of the interference wave removal receiving circuit. 1, 2, 11, 15...multiplier, 3, 12, 1
7, 20...Band pass filter, 4...Limiter,
5...FM detection circuit, 6...Voltage controlled oscillator, 7...Low pass filter, 8...Input terminal, 9, 10, 19
...Output terminal, 13...Level/delay time adjustment circuit,
14... Subtraction circuit, 16... Center frequency control circuit, 1
8...Narrowband bandpass filter, 21...Video detection circuit, 22...Amplification circuit, 23...Beat detection circuit,
24...Synchronization separation circuit.

Claims (1)

【特許請求の範囲】 1 妨害角度変調波が混入した受信振幅変調信号
波を電圧制御局部発振器の発振出力によりそれぞ
れ周波数変換して第1および第2の変換出力波を
形成し、前記第1の変換出力波を、当該変換出力
波の前記妨害角度変調波が混入した側波帯成分の
帯域を通過帯域とするバンドパスフイルタを介
し、前記電圧制御局部発振器の発振出力により周
波数逆変換した逆変換出力波について角度復調検
波して得た復調出力を負帰還して前記電圧制御局
部発振器の発振出力周波数を制御することにより
前記第1および前記第2の変換出力波に混入した
前記妨害角度変調波の占有帯域を圧縮するととも
に、前記第2の変換出力波の当該占有帯域が圧縮
された妨害角度変調波が混入した側波帯成分を前
記バンドパスフイルタに対応するフイルタを介し
て抽出し、前記占有帯域が圧縮された妨害角度変
調波の帯域を通過帯域とする狭帯域通過フイルタ
を介して前記第1の変換出力波を前記第2の変換
出力波に等振幅逆位相合成することにより前記第
2の変換出力波の前記フイルタを介して抽出した
周波数変換出力側波帯成分から前記占有帯域が圧
縮された妨害角度変調波を前記第1および第2の
変換出力波間で相殺して除去した後に、その除去
して得た出力波を前記電圧制御局部発振器の発振
出力により周波数逆変換して前記妨害角度変調波
が混入しない受信振幅変調信号波に復元するよう
にしたことを特徴とする妨害角度変調波除去受信
方式。 2 特許請求の範囲第1項記載の受信方式におい
て、前記復調出力により負帰還制御する前記電圧
制御局部発振器の発振周波数範囲の中心周波数を
前記受信振幅変調信号波の搬送波と前記妨害角度
変調波との混合波の振幅検波によつて前記受信振
幅変調信号波の検波出力に生ずるビート周波数に
応じて前記負帰還制御をするようにしたことを特
徴とする妨害角度変調波除去受信方式。
[Claims] 1. A received amplitude modulated signal wave mixed with a disturbing angle modulated wave is frequency-converted by the oscillation output of a voltage controlled local oscillator to form first and second converted output waves, Inverse conversion in which the frequency of the converted output wave is inversely converted by the oscillation output of the voltage controlled local oscillator through a bandpass filter whose pass band is the band of the sideband component mixed with the disturbance angle modulated wave of the converted output wave. By controlling the oscillation output frequency of the voltage controlled local oscillator by negative feedback of the demodulated output obtained by angle demodulation detection of the output wave, the interfering angle modulated wave mixed into the first and second converted output waves is generated. compressing the occupied band of the second conversion output wave, and extracting sideband components mixed with the jamming angle modulated wave in which the occupied band of the second converted output wave is compressed, through a filter corresponding to the bandpass filter, The first converted output wave is equal-amplitude and anti-phase synthesized with the second converted output wave through a narrow band pass filter whose pass band is the band of the jamming angle modulated wave whose occupied band has been compressed. After the interference angle modulated wave whose occupied band has been compressed is canceled and removed between the first and second converted output waves from the frequency conversion output sideband component extracted through the filter of the second converted output wave. , the output wave obtained by removing the interference is inversely frequency-converted by the oscillation output of the voltage controlled local oscillator to restore the received amplitude modulated signal wave in which the interference angle modulated wave is not mixed. Modulated wave removal reception method. 2. In the receiving system according to claim 1, the center frequency of the oscillation frequency range of the voltage controlled local oscillator which is subjected to negative feedback control by the demodulated output is set to the carrier wave of the received amplitude modulated signal wave and the interference angle modulated wave. An interfering angle modulated wave removal receiving system characterized in that the negative feedback control is performed in accordance with a beat frequency generated in the detected output of the received amplitude modulated signal wave by amplitude detection of the mixed wave.
JP5442284A 1984-03-23 1984-03-23 Reception system for eliminating disturbing angular modulation wave Granted JPS60198926A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP5442284A JPS60198926A (en) 1984-03-23 1984-03-23 Reception system for eliminating disturbing angular modulation wave

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP5442284A JPS60198926A (en) 1984-03-23 1984-03-23 Reception system for eliminating disturbing angular modulation wave

Publications (2)

Publication Number Publication Date
JPS60198926A JPS60198926A (en) 1985-10-08
JPH0446492B2 true JPH0446492B2 (en) 1992-07-30

Family

ID=12970270

Family Applications (1)

Application Number Title Priority Date Filing Date
JP5442284A Granted JPS60198926A (en) 1984-03-23 1984-03-23 Reception system for eliminating disturbing angular modulation wave

Country Status (1)

Country Link
JP (1) JPS60198926A (en)

Also Published As

Publication number Publication date
JPS60198926A (en) 1985-10-08

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