JPS6237564B2 - - Google Patents

Info

Publication number
JPS6237564B2
JPS6237564B2 JP7317482A JP7317482A JPS6237564B2 JP S6237564 B2 JPS6237564 B2 JP S6237564B2 JP 7317482 A JP7317482 A JP 7317482A JP 7317482 A JP7317482 A JP 7317482A JP S6237564 B2 JPS6237564 B2 JP S6237564B2
Authority
JP
Japan
Prior art keywords
frequency
variable
narrow band
series
output
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
JP7317482A
Other languages
Japanese (ja)
Other versions
JPS58190114A (en
Inventor
Teruhisa Fujino
Kenichi Chiwaki
Sadatoshi Narasaki
Hideki Wachi
Jushi Nezu
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.)
Koden Electronics Co Ltd
Original Assignee
Koden Electronics 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 Koden Electronics Co Ltd filed Critical Koden Electronics Co Ltd
Priority to JP7317482A priority Critical patent/JPS58190114A/en
Priority to NO830937A priority patent/NO157560C/en
Priority to DK122883A priority patent/DK122883A/en
Publication of JPS58190114A publication Critical patent/JPS58190114A/en
Publication of JPS6237564B2 publication Critical patent/JPS6237564B2/ja
Granted legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H03ELECTRONIC CIRCUITRY
    • H03HIMPEDANCE NETWORKS, e.g. RESONANT CIRCUITS; RESONATORS
    • H03H7/00Multiple-port networks comprising only passive electrical elements as network components
    • H03H7/01Frequency selective two-port networks
    • H03H7/06Frequency selective two-port networks including resistors
    • H03H7/07Bridged T-filters
    • HELECTRICITY
    • H03ELECTRONIC CIRCUITRY
    • H03HIMPEDANCE NETWORKS, e.g. RESONANT CIRCUITS; RESONATORS
    • H03H7/00Multiple-port networks comprising only passive electrical elements as network components
    • H03H7/01Frequency selective two-port networks
    • H03H7/17Structural details of sub-circuits of frequency selective networks
    • H03H7/1741Comprising typical LC combinations, irrespective of presence and location of additional resistors
    • H03H7/1758Series LC in shunt or branch path

Description

【発明の詳細な説明】 この発明は例えばロランC受信機において受信
帯域内又はその近くに存在するデツカ電波のよう
な妨害波を除去するために用いられ、かつその除
去周波数、つまり阻止周波数を変化させることが
できるようにされた可変狭帯域阻止波器に関す
る。
DETAILED DESCRIPTION OF THE INVENTION This invention is used, for example, in a Loran C receiver to remove interference waves such as Detsuka radio waves existing within or near the receiving band, and the removal frequency, that is, the blocking frequency, is changed. The present invention relates to a variable narrow band stop waver which can be used to

受信周波数帯域が比較的広い受信機などにおい
て、その受信帯域内、またはその近傍に存在する
単一周波数の妨害波を除去するために、第1図に
示すような、いわゆるノツチフイルタが用いられ
ていた。この波器は同一容量のコンデンサ1
1,12が直列に接続され、この直列接続と並列
に抵抗素子13が接続され、この並列接続の両端
は端子14,15とされ、コンデンサ11,12
の接続点はインダクタンス素子16、可変抵抗素
子17の直列回路を通じて接地され、つまり共通
電位点に接続されている。端子14より入力され
た信号中のコンデンサ11,12及びインダクタ
ンス素子16で共振したものと、これと同一成分
で抵抗素子13を通過したものとが端子15で互
に打消されると、その周波数成分は阻止されるこ
とになる。これらの打消が行われるように可変抵
抗素子17により前記共振成分のレベルが調整さ
れる。
In receivers with relatively wide receiving frequency bands, so-called notch filters, as shown in Figure 1, were used to remove single-frequency interference waves existing within or near the receiving band. . This wave generator is a capacitor of the same capacity 1
1 and 12 are connected in series, a resistance element 13 is connected in parallel with this series connection, both ends of this parallel connection are terminals 14 and 15, and capacitors 11 and 12 are connected in series.
The connection point is grounded through a series circuit of an inductance element 16 and a variable resistance element 17, that is, connected to a common potential point. When the signal input from terminal 14 that resonates with capacitors 11, 12 and inductance element 16 and the same component that has passed through resistance element 13 cancel each other out at terminal 15, the frequency component will be blocked. The level of the resonance component is adjusted by the variable resistance element 17 so that these cancellations occur.

可変狭帯域阻止波器においてはコンデンサ1
1,12の容量又はインダクタンス素子16のイ
ンダクタンスの何れかを調整して阻止周波数を変
化させている。この場合その阻止周波数の可変範
囲の中心などの一点で可変抵抗素子17を調整
し、阻止周波数を変化させても可変抵抗素子17
の調整は行つていなかつた。
In the variable narrow band stopper, capacitor 1
The blocking frequency is changed by adjusting either the capacitors 1 and 12 or the inductance of the inductance element 16. In this case, even if the variable resistance element 17 is adjusted at one point such as the center of the variable range of the stopping frequency, and the stopping frequency is changed, the variable resistance element 17
No adjustments were made.

この従来の可変狭帯域阻止波器においては、
特にその阻止周波数の可変範囲を広くする場合
は、その可変範囲の端部において必ずしも充分な
阻止(減衰)が得られなかつた。即ち例えば可変
阻止帯域の中心周波数f0で最大減衰量になるよう
に可変抵抗素子17の抵抗値を調整し、その可変
抵抗素子17の抵抗値をそのままにした状態で、
阻止周波数のみを中心周波数f0に対して±△fだ
け変化させた場合の阻止周波数における減衰量は
第2図に示すように阻止周波数が中心周波数f0
ら離れるに従つて小さくなる。そのため阻止周波
数の変化範囲を広げると、その可変範囲の両端部
では所望の減衰量が得られなくなる。
In this conventional variable narrow band stopper,
Particularly when the variable range of the blocking frequency is widened, sufficient blocking (attenuation) cannot always be obtained at the ends of the variable range. That is, for example, the resistance value of the variable resistance element 17 is adjusted so that the amount of attenuation is maximum at the center frequency f 0 of the variable stop band, and the resistance value of the variable resistance element 17 is left unchanged.
When only the stopping frequency is changed by ±Δf with respect to the center frequency f 0 , the amount of attenuation at the stopping frequency becomes smaller as the stopping frequency moves away from the center frequency f 0 as shown in FIG. Therefore, if the range of variation of the stopping frequency is widened, the desired amount of attenuation cannot be obtained at both ends of the variable range.

この原因を追究した結果、周波数に応じてイン
ダクタンス素子16、例えばコイルの実効抵抗が
第3図に示すように変化するため、中心周波数f0
から離れるに従つて第1図においてコンデンサ1
1,12を共振により通過した周波数成分と、こ
れと同一成分で抵抗素子13を通過したものとの
レベル差が大きくなるためであることがわかつ
た。従つて阻止周波数を変化させるごとに可変抵
抗素子17の抵抗値の調整をやりなおせば広い周
波数帯にわたり減衰量が充分大きい可変狭帯域
波器が得られるが、そのような調整をいちいち行
うことは繁雑である。
As a result of investigating the cause of this, it was found that the effective resistance of the inductance element 16, such as a coil, changes depending on the frequency as shown in FIG .
As the distance from capacitor 1 increases in Fig. 1,
It was found that this is because the level difference between the frequency component that passed through the resistor element 13 due to resonance and the same frequency component that passed through the resistor element 13 becomes large. Therefore, by re-adjusting the resistance value of the variable resistance element 17 each time the stopping frequency is changed, a variable narrowband transducer with sufficiently large attenuation over a wide frequency band can be obtained, but it is cumbersome to make such adjustments each time. It is.

この発明の目的は阻止周波数を変化させるごと
に可変抵抗素子をいちいち調整するような繁雑な
操作を行うことなく、可変阻止周波数帯域で充分
な減衰量が得られる可変狭帯域阻止波器を提供
することにある。
An object of the present invention is to provide a variable narrow band stopper that can obtain sufficient attenuation in the variable stop frequency band without having to perform complicated operations such as adjusting variable resistance elements each time the stop frequency is changed. There is a particular thing.

この発明によれば従来の狭帯域阻止波器に対
し、そのインダクタンス素子と直列に補償用コン
デンサを挿入し、この補償用コンデンサのインピ
ーダンスは阻止周波数に影響を与えないように充
分小さい値とされ、かつインダクタンス素子の実
効抵抗の周波数特性とほゞ逆の周波数特性とされ
る。つまり補償用コンデンサのインピーダンスと
インダクタンス素子の実効抵抗との和は阻止周波
数の変化範囲でほゞ一定になるようにされる。
According to the present invention, a compensating capacitor is inserted in series with the inductance element of a conventional narrow band stopper, and the impedance of the compensating capacitor is set to a sufficiently small value so as not to affect the stopping frequency. Moreover, the frequency characteristic is almost opposite to the frequency characteristic of the effective resistance of the inductance element. In other words, the sum of the impedance of the compensation capacitor and the effective resistance of the inductance element is made to be approximately constant within the range of change in the blocking frequency.

例えば第4図に第1図と対応する部分に同一符
号を付けて示すように、可変抵抗素子17と直列
に補償用コンデンサ18を接続する。この補償用
コンデンサ18のインピーダンスはコンデンサ1
1,12の各インピーダンスと比較して充分小さ
いものとされ、つまりコンデンサ11,12、イ
ンダクタンス素子16よりなる共振回路の共振周
波数特性に実質的に影響を与えないようにされ
る。また補償用コンデンサ18のインピーダンス
の周波数特性曲線19は第5図に示すように、イ
ンダクタンス素子16の実効抵抗の周波数特性曲
線21とほゞ逆に変化し、これらインピーダンス
及び抵抗の和は周波数軸とほゞ平行するようにさ
れる。補償用コンデンサ18の周波数特性は一般
に直線ではなく曲線であるため、この曲線19は
実効抵抗の周波数特性曲線21が第5図に示すよ
うに二点で交叉し、これら交叉点が阻止周波数の
可変範囲の両端f0−△f、f0+△f附近となるよ
うにし、その一方の交叉点において可変抵抗素子
17を調整してその周波数で減衰量が最大になる
ようにすることが好ましい。
For example, as shown in FIG. 4 with the same reference numerals assigned to parts corresponding to those in FIG. 1, a compensating capacitor 18 is connected in series with the variable resistance element 17. The impedance of this compensation capacitor 18 is the capacitor 1
The impedances of the capacitors 11 and 12 are sufficiently small compared to the impedances of the capacitors 11 and 12, and the resonant frequency characteristics of the resonant circuit made up of the capacitors 11 and 12 and the inductance element 16 are not substantially affected. Furthermore, as shown in FIG. 5, the frequency characteristic curve 19 of the impedance of the compensation capacitor 18 changes almost inversely to the frequency characteristic curve 21 of the effective resistance of the inductance element 16, and the sum of these impedances and resistances changes along the frequency axis. They are made to be almost parallel. Since the frequency characteristic of the compensation capacitor 18 is generally not a straight line but a curve, this curve 19 intersects the frequency characteristic curve 21 of the effective resistance at two points as shown in FIG. It is preferable to set the frequency to be near both ends of the range f 0 −Δf and f 0 +Δf, and adjust the variable resistance element 17 at one of the crossing points so that the amount of attenuation becomes maximum at that frequency.

この構成によれば阻止周波数の可変範囲内にお
いて、コンデンサ11,12、インダクタンス素
子16の共振回路を通過した周波数成分と、これ
と同一周波数成分で抵抗素子13を通過した成分
とのレベルがほゞ一致し、この可変周波数帯域に
おいて阻止周波数に対して大きな減衰量が得られ
る。例えば第1図、第2図に示した条件と同一の
場合に補償用コンデンサ18を用いることにより
阻止周波数における減衰量特性は第6図に示すよ
うになり、可変帯域においてほゞ40dB以上の減
衰量が得られ第2図の場合より約10dB改善され
た。
According to this configuration, within the variable range of the blocking frequency, the level of the frequency component that has passed through the resonant circuit of the capacitors 11 and 12 and the inductance element 16 and that of the same frequency component that has passed through the resistance element 13 are approximately the same. A large amount of attenuation can be obtained with respect to the stop frequency in this variable frequency band. For example, if the compensation capacitor 18 is used under the same conditions as shown in Figs. 1 and 2, the attenuation characteristics at the stop frequency will become as shown in Fig. 6, resulting in an attenuation of approximately 40 dB or more in the variable band. The amount was improved by about 10 dB compared to the case shown in Figure 2.

このようにこの発明によれば可変帯域において
いちいち可変抵抗素子の調整をすることなく、大
きな減衰量が得られるため、この帯域において不
要周波数成分を充分除去することができる。また
変化できる阻止周波数の帯域を広くすることがで
きる。
As described above, according to the present invention, a large amount of attenuation can be obtained without adjusting the variable resistance element each time in the variable band, so that unnecessary frequency components can be sufficiently removed in this band. Furthermore, the range of changeable stopping frequencies can be widened.

このような特徴があるからこの発明の可変狭帯
域阻止波器は例えばロランC受信機においてデ
ツカ電波を除去することを自動的に行う場合に適
用することができる。その例を第7図を参照して
説明する。
Because of these features, the variable narrow band stopper of the present invention can be applied, for example, to automatically remove deep radio waves in a Loran C receiver. An example will be explained with reference to FIG.

第7図において受信信号は入力端子31より前
段増幅器32を通じて増幅され、この発明の狭帯
域阻止波器33により妨害波が除去され、その
妨害波が除去された出力は後段増幅器34で増幅
され、出力端子35を通じて例えばロランC信号
処理装置のような処理装置36に供給される。狭
帯域阻止波器33の入力側と出力側の信号が分
岐されて制御回路37に供給される。制御回路3
7において狭帯域阻止波器33の阻止中心周波
数と目的とする妨害波の周波数とのずれが検出さ
れる。この検出されたずれはスイツチ38を通じ
て保持回路39に供給されて保持される。その保
持信号は狭帯域阻止波器33にその阻止中心周
波数制御信号として与えられる。
In FIG. 7, the received signal is amplified from the input terminal 31 through the preamplifier 32, the interference wave is removed by the narrow band rejection filter 33 of the present invention, and the output from which the interfering wave has been removed is amplified by the postamplifier 34. Via an output terminal 35 it is supplied to a processing device 36, such as a Loran C signal processing device. The signals on the input side and output side of the narrow band stop filter 33 are branched and supplied to the control circuit 37 . Control circuit 3
At step 7, a deviation between the blocking center frequency of the narrow band blocking filter 33 and the frequency of the target interference wave is detected. This detected deviation is supplied to a holding circuit 39 through a switch 38 and held there. The holding signal is given to the narrowband rejection filter 33 as its rejection center frequency control signal.

狭帯域阻止波器33は第4図に示したものと
同一構成とされ、そのコンデンサ11,12とし
て可変容量ダイオードが用いられ、これら可変容
量ダイオード11,12が保持回路39よりの制
御信号によつて制御されて阻止中心周波数が制御
される。この制御電圧は可変抵抗素子17及び補
償用コンデンサ18の接続点に与えられてダイオ
ード11,12に印加される。
The narrow band blocking filter 33 has the same configuration as shown in FIG. 4, and variable capacitance diodes are used as the capacitors 11 and 12. and the blocking center frequency is controlled. This control voltage is applied to the connection point between the variable resistance element 17 and the compensation capacitor 18, and is applied to the diodes 11 and 12.

制御回路37においては、例えば狭帯域阻止
波器33の入力側の信号と出力側の信号とがそれ
ぞれ帯域通過波器41,42を通じてとり出さ
れ、これら帯域通過波器41,42の出力が位
相比較器43で位相比較され、その位相比較出力
が制御回路37の出力とされる。帯域通過波器
41,42はその通過中心周波数が狭帯域阻止
波器33の阻止中心周波数とほゞ一致され、かつ
これら帯域通過波器41,42は互にほゞ等し
い波特性とされる。この狭帯域阻止波器33
の阻止中心周波数が保持回路39の出力で制御さ
れると共に、帯域通過波器41,42の中心周
波数も制御されるように、これら帯域通過波器
41,42の例えばその構成要素の一部に可変容
量ダイオードが使用され、その可変容量ダイオー
ドは保持回路39の出力によつて制御され、かつ
その制御信号に対する中心周波数の変化特性は狭
帯域阻止波器33の特性と同様とされる。
In the control circuit 37, for example, the input side signal and the output side signal of the narrowband rejection filter 33 are taken out through the bandpass waveformers 41 and 42, respectively, and the outputs of these bandpass waveformers 41 and 42 are outputted in phase. The comparator 43 compares the phases, and the phase comparison output is used as the output of the control circuit 37. The pass center frequencies of the band pass wave generators 41 and 42 are made to substantially match the rejection center frequency of the narrow band stop wave generator 33, and the wave characteristics of these band pass wave generators 41 and 42 are approximately equal to each other. . This narrow band stopper 33
For example, some of the components of the bandpass waveforms 41 and 42 may be controlled so that the rejection center frequency of the bandpass waveforms 41 and 42 is controlled by the output of the holding circuit 39 and the center frequencies of the bandpass waveforms 41 and 42 are also controlled. A variable capacitance diode is used, and the variable capacitance diode is controlled by the output of the holding circuit 39, and the change characteristics of the center frequency with respect to the control signal are similar to the characteristics of the narrow band stop filter 33.

狭帯域阻止波器33の位相周波数特性は第8
図の曲線66として示すように、その阻止中心周
波数f0よりも高い周波数側においては位相は急激
にほゞ90゜すすみ、中心周波数f0よりも低い周波
数においては位相は急激に90゜おくれる。つまり
f0−△f〜f0+△fの範囲内において位相が急激
に変化している。一方帯域通過波器41,42
は例えばコイルとコンデンサの同調回路より成る
単峰同調型として構成され、その位相周波数特性
は第8図の曲線67で示すように中心周波数f0
り低い側において徐々に進み位相となり、高い側
において徐々におくれ位相となる。従つて周波数
f0−△fないしf0+△fの間においては、波器
41,42の出力の位相は曲線66の特性でほぼ
決まつてしまう。よつてこれら波器41,42
の出力の位相を位相比較器43で検出することに
よつて狭帯域阻止波器33の中心周波数f0と妨
害波の周波数とのずれを検出することができる。
つまり妨害波の周波数の方が阻止中心周波数f0
りも高い場合は波器42の出力がすすみ位相と
なり、妨害波周波数の方が低い場合は波器41
の出力の方がすすみ位相となる。
The phase frequency characteristic of the narrow band stopper 33 is as follows:
As shown by curve 66 in the figure, the phase rapidly advances by approximately 90 degrees at frequencies higher than the center frequency f0 , and the phase rapidly lags 90 degrees at frequencies lower than the center frequency f0 . . In other words
The phase changes rapidly within the range of f 0 −Δf to f 0 +Δf. On the other hand, bandpass waveforms 41 and 42
For example, it is constructed as a single-peak tuning type consisting of a tuning circuit of a coil and a capacitor, and its phase frequency characteristics gradually advance in phase on the side lower than the center frequency f 0 and as shown by curve 67 in Figure 8, and on the higher side The phase gradually lags. Therefore the frequency
Between f 0 -△f and f 0 +△f, the phase of the outputs of wave generators 41 and 42 is almost determined by the characteristics of curve 66. Therefore, these wave devices 41, 42
By detecting the phase of the output with the phase comparator 43, it is possible to detect the deviation between the center frequency f 0 of the narrowband rejection filter 33 and the frequency of the interference wave.
In other words, if the frequency of the interference wave is higher than the blocking center frequency f 0 , the output of the wave generator 42 will be in forward phase, and if the frequency of the interference wave is lower than the blocking center frequency f 0 , the output of the wave generator 42 will be in forward phase.
The output of is in the forward phase.

狭帯域阻止波器33の入力側及び出力側の信
号が分岐されてレベル検出器でそれぞれのレベル
が検出される。即ち帯域通過波器41,42の
出力はそれぞれレベル検出器44,45に供給さ
れてそれぞれのレベルが検出され、レベル検出器
44,45の出力は比較器46で大小が比較さ
れ、その比較器46の比較出力によつてスイツチ
38が制御される。
The signals on the input side and output side of the narrowband rejection filter 33 are branched, and their respective levels are detected by a level detector. That is, the outputs of the bandpass waveformers 41 and 42 are respectively supplied to level detectors 44 and 45 to detect their respective levels, and the outputs of the level detectors 44 and 45 are compared in magnitude by a comparator 46. A switch 38 is controlled by the comparison output of 46.

ところで狭帯域阻止波器33の中心周波数f0
が妨害波の周波数と一致すると、狭帯域阻止波
器33の出力は入力に比べて充分小さくなる。従
つてレベル検出器44の出力は大きく、レベル検
出器45の出力は著しく小さくなる。この状態に
おいて比較器46の出力が高レベルとなつてスイ
ツチ38がオンとされ、制御回路37の出力は保
持回路39へ供給される。しかし妨害波が遮断さ
れると、狭帯域阻止波器33には雑音が入力さ
れていると同様の状態となり、入力側と出力側と
はほゞ同一レベルとなり、このためレベル検出器
26,27の出力レベルがほゞ同一となり、この
状態においては入力側の検出器44の検出レベル
の方が出力側の検出器45の検出レベルよりも小
さくなるようにされる。この結果スイツチ38は
オフとされ、制御回路37の出力は保持回路39
に供給されない。従つて妨害波が遮断された状態
においては制御回路37の検出信号は信頼できる
ものとならないが、このような誤つた制御信号は
保持回路39へ供給されることなく、保持回路3
9はそれまでの制御状態を保持しており、再び妨
害波が入力されるとその妨害波を狭帯域阻止波
器33で確実に阻止することが可能である。
By the way, the center frequency f 0 of the narrow band stop filter 33
When the frequency of the interference wave matches the frequency of the interference wave, the output of the narrow band stop filter 33 becomes sufficiently small compared to the input. Therefore, the output of level detector 44 is large, and the output of level detector 45 is significantly small. In this state, the output of the comparator 46 becomes high level, the switch 38 is turned on, and the output of the control circuit 37 is supplied to the holding circuit 39. However, when the interference wave is blocked, the narrowband blocker 33 enters the same state as if noise had been input, and the input side and the output side are at almost the same level, so that the level detectors 26, 27 The output levels of the detector 44 on the input side are made to be smaller than the detection level of the detector 45 on the output side in this state. As a result, the switch 38 is turned off, and the output of the control circuit 37 is transferred to the holding circuit 39.
is not supplied. Therefore, the detection signal of the control circuit 37 is not reliable in a state where the interference waves are blocked, but such an erroneous control signal is not supplied to the holding circuit 39 and is sent to the holding circuit 39.
9 maintains the previous control state, and when a disturbance wave is inputted again, it is possible to reliably block the disturbance wave by the narrow band rejection filter 33.

このようにロランC受信機においてその帯域又
は近傍の単一周波妨害波を、この発明の狭帯域阻
止波器で除去でき、かつ第7図に示したように
自動的にその阻止周波数を妨害波に一致させるこ
とができるが、その場合に可変抵抗素子17をい
ちいち調整する必要がなく、かつ広い可変帯域で
阻止周波数を変化させても所望の阻止減衰量を得
ることができる。なお第7図の例では補償用コン
デンサ18は制御信号に対する直流遮断コンデン
サとしての作用も兼ねており、ロランC受信機で
は第4図中の抵抗器13を150Ω、コンデンサ1
1,12をそれぞれ100〜400pF、インダクタン
ス素子16を6mH、可変抵抗器17を約10Ωと
した場合、補償用コンデンサ18として容量が
0.01〜0.022μF程度のポリエステルコンデンサ
が好ましい。
In this way, in the Loran C receiver, single-frequency interference waves in or near the band can be removed by the narrow band rejection device of the present invention, and the rejection frequency can be automatically changed to the interference wave as shown in FIG. In this case, it is not necessary to adjust the variable resistance element 17 one by one, and the desired amount of rejection attenuation can be obtained even if the rejection frequency is changed over a wide variable band. In the example shown in Fig. 7, the compensation capacitor 18 also functions as a DC cutoff capacitor for the control signal, and in the Loran C receiver, the resistor 13 in Fig. 4 is 150Ω, and the capacitor 1
1 and 12 are each 100 to 400 pF, the inductance element 16 is 6 mH, and the variable resistor 17 is approximately 10 Ω, the capacitance of the compensation capacitor 18 is
A polyester capacitor of about 0.01 to 0.022 μF is preferable.

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

第1図は従来の狭帯域阻止波器を示す回路
図、第2図は第1図の波器の阻止減衰量の周波
数特性図、第3図はインダクタンス素子の実効抵
抗周波数特性図、第4図はこの発明による可変狭
帯域阻止波器の一例を示す回路図、第5図は補
償用コンデンサ18のインピーダンス周波数特性
図、第6図は第4図の波器の阻止減衰器の周波
数特性図、第7図はこの発明の波器を用いた妨
害波除去装置の例を示すブロツク図、第8図は
波器33の周波数特性図である。 11,12:第1、第2コンデンサ、16:イ
ンダクタンス素子、17:可変抵抗素子、18:
補償用コンデンサ。
Figure 1 is a circuit diagram showing a conventional narrow band blocking filter, Figure 2 is a frequency characteristic diagram of the blocking attenuation of the wave generator in Figure 1, Figure 3 is an effective resistance frequency characteristic diagram of an inductance element, and Figure 4 The figure is a circuit diagram showing an example of a variable narrow band blocking device according to the present invention, FIG. 5 is an impedance frequency characteristic diagram of the compensation capacitor 18, and FIG. 6 is a frequency characteristic diagram of the blocking attenuator of the wave device shown in FIG. 4. 7 is a block diagram showing an example of an interference wave removal device using the wave generator of the present invention, and FIG. 8 is a frequency characteristic diagram of the wave generator 33. 11, 12: first and second capacitors, 16: inductance element, 17: variable resistance element, 18:
Compensation capacitor.

Claims (1)

【特許請求の範囲】[Claims] 1 第1、第2コンデンサが直列に接続され、そ
の直列接続と並列に第1抵抗素子が接続され、そ
の並列接続の両端は第1、第2端子とされ、上記
第1、第2コンデンサの接続点と、共通端子との
間に、インダクタンス素子及び可変抵抗素子の直
列回路が接続され、上記第1、第2コンデンサ及
び上記インダクタンス素子の一方はそのインピー
ダンスを変化することができるようにされた可変
狭帯域阻止波器において、上記可変抵抗素子と
直列に補償用コンデンサが挿入され、その補償用
コンデンサは、上記狭帯域阻止波器の可変周波
数帯域内において充分小さいインピーダンスをも
ち、かつその周波数特性は上記インダクタンス素
子の実効抵抗の周波数特性とほゞ逆の変化特性に
選定されていることを特徴とする可変狭帯域阻止
波器。
1. The first and second capacitors are connected in series, a first resistance element is connected in parallel to the series connection, and both ends of the parallel connection are used as first and second terminals, and the first and second capacitors are connected in series. A series circuit of an inductance element and a variable resistance element is connected between the connection point and the common terminal, and the impedance of one of the first and second capacitors and the inductance element can be changed. In the variable narrow band stopper, a compensation capacitor is inserted in series with the variable resistance element, and the compensation capacitor has a sufficiently small impedance within the variable frequency band of the narrow band stopper, and has a frequency characteristic. is selected to have a change characteristic that is substantially opposite to the frequency characteristic of the effective resistance of the inductance element.
JP7317482A 1982-03-29 1982-04-28 Variable narrow band stop filter Granted JPS58190114A (en)

Priority Applications (3)

Application Number Priority Date Filing Date Title
JP7317482A JPS58190114A (en) 1982-04-28 1982-04-28 Variable narrow band stop filter
NO830937A NO157560C (en) 1982-03-29 1983-03-16 DEVICE FOR DISPOSAL OF INTERRUPTIONS.
DK122883A DK122883A (en) 1982-03-29 1983-03-17 DEVICE FOR REJECTING A NOISE

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP7317482A JPS58190114A (en) 1982-04-28 1982-04-28 Variable narrow band stop filter

Publications (2)

Publication Number Publication Date
JPS58190114A JPS58190114A (en) 1983-11-07
JPS6237564B2 true JPS6237564B2 (en) 1987-08-13

Family

ID=13510509

Family Applications (1)

Application Number Title Priority Date Filing Date
JP7317482A Granted JPS58190114A (en) 1982-03-29 1982-04-28 Variable narrow band stop filter

Country Status (1)

Country Link
JP (1) JPS58190114A (en)

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
GB2310104A (en) * 1996-02-12 1997-08-13 Yang Yi Fu Loud speaker enclosure and tunable audio reproduction apparatus
IT1401799B1 (en) 2010-09-29 2013-08-28 Firex S R L MACHINE FOR MIXING OR CUTTING, PARTICULARLY FOR THE PROCESSING OF FOOD, AGENT WITH PLANETARY MOVEMENT SHAFT

Also Published As

Publication number Publication date
JPS58190114A (en) 1983-11-07

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