JPH0117289B2 - - Google Patents

Info

Publication number
JPH0117289B2
JPH0117289B2 JP56124910A JP12491081A JPH0117289B2 JP H0117289 B2 JPH0117289 B2 JP H0117289B2 JP 56124910 A JP56124910 A JP 56124910A JP 12491081 A JP12491081 A JP 12491081A JP H0117289 B2 JPH0117289 B2 JP H0117289B2
Authority
JP
Japan
Prior art keywords
signal
output
amplitude
delay
delayed
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
JP56124910A
Other languages
Japanese (ja)
Other versions
JPS5825707A (en
Inventor
Keiji Murakami
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.)
Mitsubishi Electric Corp
Original Assignee
Mitsubishi Electric 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 Mitsubishi Electric Corp filed Critical Mitsubishi Electric Corp
Priority to JP12491081A priority Critical patent/JPS5825707A/en
Publication of JPS5825707A publication Critical patent/JPS5825707A/en
Publication of JPH0117289B2 publication Critical patent/JPH0117289B2/ja
Granted legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H04ELECTRIC COMMUNICATION TECHNIQUE
    • H04BTRANSMISSION
    • H04B3/00Line transmission systems
    • H04B3/02Details
    • H04B3/04Control of transmission; Equalising
    • H04B3/14Control of transmission; Equalising characterised by the equalising network used
    • H04B3/142Control of transmission; Equalising characterised by the equalising network used using echo-equalisers, e.g. transversal

Landscapes

  • Engineering & Computer Science (AREA)
  • Computer Networks & Wireless Communication (AREA)
  • Signal Processing (AREA)
  • Filters That Use Time-Delay Elements (AREA)
  • Cable Transmission Systems, Equalization Of Radio And Reduction Of Echo (AREA)

Description

【発明の詳細な説明】 この発明は信号波形の等化を行う波形等化器に
関するものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a waveform equalizer that equalizes signal waveforms.

従来、この種の装置として第1図に示すものが
あつた。図において、1は入力端子、2はこの入
力端子1に入力された信号を減衰させることなく
所定時間T(秒)だけ遅延させて出力する遅延回
路としてのタツプ付遅延線、3は該遅延線2から
出力される信号の極性を反転する機能をもつ振幅
調整ボリユーム、4は該ボリユーム3から出力さ
れる信号を加算する加算器、5は該加算器4から
出力された信号の位相を変化させる移相器、6は
該移相器5からの出力信号と上記振幅調整ボリユ
ーム3の1つからの出力信号とを加算する加算
器、7は出力端子である。
Conventionally, there has been a device of this type as shown in FIG. In the figure, 1 is an input terminal, 2 is a delay line with a tap that serves as a delay circuit that delays the signal input to input terminal 1 by a predetermined time T (seconds) without attenuating it, and outputs the signal, and 3 is the delay line. 2 is an amplitude adjustment volume having a function of inverting the polarity of the signal output from the volume 3; 4 is an adder for adding the signal output from the volume 3; and 5 is for changing the phase of the signal output from the adder 4. A phase shifter 6 is an adder for adding the output signal from the phase shifter 5 and an output signal from one of the amplitude adjustment volumes 3, and 7 is an output terminal.

次に動作について説明する。 Next, the operation will be explained.

入力端子1に入力された信号は、一部はタツプ
付遅延線2に入力され所定時間T(秒)だけ遅延
されて出力され、一部は振幅調整ボリユーム3に
て適当な振幅に調整されて出力される。次に上記
所定時間T(秒)だけ遅延された信号は同様にし
て一部がタツプ付遅延線2に入力されて合計2T
だけ遅延されて出力され、一部は振幅調整ボリユ
ーム3に入力され適当な振幅に調整されて時間T
だけ遅延された信号として出力される。このよう
にして、タツプ付遅延線2の遅延時間がすべてT
であるから、時間0,T,2T,…,nT(nはタ
ツプ付遅延線の個数)だけ遅延された(n+1)
個の信号が振幅調整ボリユーム3から出力され
る。このうちn個の信号は、加算器4によつて加
算され、移相器5によつて0゜又は90゜移相された
後出力されて加算器6への入力信号(以下エコー
信号と呼ぶ)となる。又、残りの1個の信号(以
下これを主信号と呼ぶ)は直接加算器6に入力さ
れ、加算される。従つて、出力端子7では主信号
とエコー信号とが合成された信号が得られること
になる。
A portion of the signal input to the input terminal 1 is input to the delay line 2 with a tap, delayed by a predetermined time T (seconds), and output, and a portion is adjusted to an appropriate amplitude by the amplitude adjustment volume 3. Output. Next, a portion of the signal delayed by the predetermined time T (seconds) is similarly input to the delay line 2 with a tap, for a total of 2T.
A portion is input to the amplitude adjustment volume 3 and adjusted to an appropriate amplitude for a time T.
output as a delayed signal. In this way, the delay time of the tapped delay line 2 is all T.
Therefore, it was delayed by the time 0, T, 2T, ..., nT (n is the number of tapped delay lines) (n+1)
signals are output from the amplitude adjustment volume 3. Of these, n signals are added by an adder 4, phase-shifted by 0° or 90° by a phase shifter 5, and then output as an input signal to an adder 6 (hereinafter referred to as an echo signal). ). Further, the remaining one signal (hereinafter referred to as the main signal) is directly input to the adder 6 and added. Therefore, at the output terminal 7, a signal obtained by combining the main signal and the echo signal is obtained.

以上の説明は一般の場合であるが、次にn=2
の場合についてさらに詳細に説明する。
The above explanation is for the general case, but next, n=2
The case will be explained in more detail.

第2図はn=2の場合の従来回路のブロツク構
成を示し、図aは移相器の移相値が0゜(従つて図
面では移相器は省略されている)の場合であり、
図bは移相器の移相値が90゜の場合である。
Figure 2 shows the block configuration of the conventional circuit when n=2, and Figure a shows the case where the phase shift value of the phase shifter is 0° (therefore, the phase shifter is omitted in the drawing).
Figure b shows the case where the phase shift value of the phase shifter is 90°.

第2図a,bにおいて、1,7はそれぞれ入力
端子および出力端子、21〜24は所定の遅延時
間Tをもつタツプ付遅延線、31〜36は振幅調
整ボリユーム、41,42は加算器、51は90゜
移相器、61は加算器である。
In FIGS. 2a and 2b, 1 and 7 are input terminals and output terminals, respectively, 21 to 24 are delay lines with taps having a predetermined delay time T, 31 to 36 are amplitude adjustment volumes, 41 and 42 are adders, 51 is a 90° phase shifter, and 61 is an adder.

いま、入力端子1にきわめて細いパルスが入力
された場合を考える。但し、振幅調整ボリユーム
32,35によつて主信号の振幅は1に正規化さ
れているものとする。即ち、振幅調整ボリユーム
31〜33から出力された信号の振幅値(タツプ
係数)を各々a-1,1,a1とし、同様に、振幅調
整ボリユーム34〜36から出力された信号の振
幅値を各々b-1,1,b1とする。第2図aの場合
の時間応答の一例を第3図に示す。この場合3つ
の信号はすべて同相であり、かつ各信号間には時
間Tずつ時間遅れがある。
Now, consider the case where an extremely thin pulse is input to input terminal 1. However, it is assumed that the amplitude of the main signal is normalized to 1 by the amplitude adjustment volumes 32 and 35. That is, the amplitude values (tap coefficients) of the signals output from the amplitude adjustment volumes 31 to 33 are respectively a -1 , 1, and a 1 , and similarly, the amplitude values of the signals output from the amplitude adjustment volumes 34 to 36 are Let b -1 , 1 and b 1 respectively. FIG. 3 shows an example of the time response in the case of FIG. 2a. In this case, all three signals are in phase, and there is a time delay of T between each signal.

第2図a,bの各回路の周波数特性をそれぞれ
Fa(f),Fb(f)とすると、 Fa(f)=1+a-1e+j2fT+a1e-j2fT=1+(a1+a
-1)cos2πfT−j(a1−a-1)sin2πfT……(1) Fb(f)=1+j〔b-1e+j2fT+b1e-j2fT〕=1+
(b1−b-1)sin2πfT+j(b1+b-1)cos2πfT……(2) となり、振幅および群遅延の変動項をそれぞれG
(f)(dB),τ(f)(秒)とすると、 () a1=a-1=b1=b-1=k(|k|≪1)の
とき Ga(f)≒17.372kcos(2πfT) τa(f)=0 (dB) (秒)(3) Gb(f)≒0 τb(f)≒2kTsin(2πfT) (dB) (秒)(4) () a1=−a1=k,b1=−b-1=k(|k|≪
1)のとき Ga(f)≒0 τa(f)≒2kTcos(2πfT) (dB) (秒)(5) Gb(f)≒17.372ksin(2πfT) τb(f)=0(dB) (秒)(6) となり、タツプ係数a-1,a1(|a-1|=|a1|)
の極性に応じて振幅特性又は遅延特性の一方が余
弦形又は正弦形の変動を行い、他方は変動なしと
なる。この時の特性を第4図および第5図に示
す。第4図および第5図はそれぞれ第2図aおよ
びbの回路の各種特性を示し、両図のa,dはそ
れぞれ主信号およびエコー信号の時間応答、両図
b,eはそれぞれ振幅特性、両図c,fは群遅延
特性を示す。第4図b,fの特性を余弦形と呼
び、第5図c,eの特性を正弦形と呼ぶ。これら
の特性を用いて振幅歪又は等化歪の等化を行うこ
とができる。
The frequency characteristics of each circuit in Figure 2 a and b are
Fa (f), Fb (f), Fa (f) = 1 + a -1 e +j2fT +a 1 e -j2fT = 1 + (a 1 + a
-1 ) cos2πfT−j (a 1 −a -1 ) sin2πfT……(1) Fb (f) = 1 + j [b -1 e +j2fT +b 1 e -j2fT ] = 1+
(b 1 −b -1 ) sin2πfT + j (b 1 + b -1 ) cos2πfT...(2), and the fluctuation terms of amplitude and group delay are respectively
(f) (dB), τ(f) (seconds), () a 1 = a -1 = b 1 = b -1 = k (|k|≪1) then Ga(f)≒17.372kcos (2πfT) τa(f)=0 (dB) (seconds) (3) Gb(f)≒0 τb(f)≒2kTsin(2πfT) (dB) (seconds)(4) () a 1 = −a 1 =k,b 1 =-b -1 =k(|k|≪
1) When Ga(f)≒0 τa(f)≒2kTcos(2πfT) (dB) (sec)(5) Gb(f)≒17.372ksin(2πfT) τb(f)=0(dB) (sec) (6), and the tap coefficient a -1 , a 1 (|a -1 |= |a 1 |)
Depending on the polarity of the amplitude characteristic or the delay characteristic, either the amplitude characteristic or the delay characteristic fluctuates in a cosine or sine shape, and the other does not fluctuate. The characteristics at this time are shown in FIGS. 4 and 5. Figures 4 and 5 show various characteristics of the circuits in Figures 2a and b, respectively, where a and d in both figures show the time response of the main signal and echo signal, respectively, b and e in both figures show the amplitude characteristics, respectively, Both figures c and f show group delay characteristics. The characteristics shown in FIG. 4 b and f are called cosine shapes, and the characteristics shown in FIGS. 5 c and e are called sine shapes. These characteristics can be used to equalize amplitude distortion or equalization distortion.

従来の波形等化器は以上のように構成されてい
るので、振幅又は群遅延の等化を行う場合は余弦
形もしくは正弦形のいずれか一方の特性しか得る
ことができず、波形等化器を設計するうえで不便
であつた。
Conventional waveform equalizers are configured as described above, so when equalizing amplitude or group delay, only cosine or sine characteristics can be obtained, and the waveform equalizer This was inconvenient when designing.

この発明は上記のような従来のものの欠点を除
去するためになされたもので、従来の余弦形及び
正弦形の等化器を組合わせ、かつタツプ係数を特
定の関係で重み付けすることにより、余弦形の周
波数特性を水平方向に所望量だけずらせた余弦形
の周波数特性を得ることができる波形等化器を提
供することを目的としている。
This invention was made in order to eliminate the drawbacks of the conventional ones as described above, and by combining the conventional cosine type and sine type equalizers and weighting the tap coefficients in a specific relationship, the cosine equalizer It is an object of the present invention to provide a waveform equalizer that can obtain a cosine-shaped frequency characteristic that is horizontally shifted by a desired amount.

以下、この発明の一実施例を図について説明す
る。
An embodiment of the present invention will be described below with reference to the drawings.

第6図は本発明の一実施例による波形等化器を
示し、図において、第1図と同一の符号は第1図
と同一のものを示し、201は入力信号を分岐す
る分岐回路、202は該分岐回路201の出力を
90゜移相する90゜移相器、301〜304は入力信
号を所定時間Tだけ遅延するタツプ付遅延線、3
51,352はそれぞれ上記タツプ付遅延線30
2,304の出力の位相を0゜もしくは180゜変化さ
せる機能をもつインバータ・ノンインバータ選択
回路、401は該インバータ・ノンインバータ選
択回路351および上記分岐回路201の出力を
加算する加算器、402は上記90゜移相器202
および上記インバータ・ノンインバータ選択回路
352の出力を加算する加算器、501,502
はそれぞれ特定の関係で重み付けされ、上記加算
器401,402の出力を調整する振幅調整ボリ
ユーム、601は該両振幅調整ボリユーム50
1,502の出力およびタツプ付遅延線301の
出力を加算する加算器である。
FIG. 6 shows a waveform equalizer according to an embodiment of the present invention, in which the same reference numerals as in FIG. 1 indicate the same components as in FIG. is the output of the branch circuit 201.
90° phase shifter that shifts the phase by 90°; 301 to 304 are delay lines with taps that delay the input signal by a predetermined time T;
51 and 352 are the delay lines 30 with taps, respectively.
2,304 is an inverter/non-inverter selection circuit having a function of changing the phase of the output by 0° or 180°; 401 is an adder that adds the outputs of the inverter/non-inverter selection circuit 351 and the branch circuit 201; The above 90° phase shifter 202
and adders 501 and 502 that add the outputs of the inverter/non-inverter selection circuit 352;
are respectively weighted in a specific relationship and are amplitude adjustment volumes that adjust the outputs of the adders 401 and 402; 601 is the amplitude adjustment volume 50
1,502 and the output of the tapped delay line 301.

なお、上記回路301,302,351,40
1により、上記分岐回路201の出力の一方aを
時間Tだけ遅延した主信号と、上記出力aとこれ
を2Tだけ遅延した信号又はその反転信号とを加
算した加算エコー信号とを形成する第1の遅延回
路網8を構成しており、また上記回路303,3
04,352,402により、上記移相器202
の出力bから加算エコー信号を形成する第2の遅
延回路網9を構成している。
Note that the above circuits 301, 302, 351, 40
1, a first signal that forms a main signal obtained by delaying one of the outputs a of the branch circuit 201 by a time T, and an added echo signal obtained by adding the above output a and a signal obtained by delaying the output a by 2T or its inverted signal. The circuits 303 and 3 constitute a delay circuit network 8.
04,352,402, the phase shifter 202
A second delay circuit network 9 is configured to form an added echo signal from the output b of the .

以上のように構成された波形等化器の動作につ
いて、第6図、第7図を参照して説明する。ただ
し、任意の信号波形は極めて細いパルスの線型和
として表わされるので、以下、この極めて細いパ
ルスを入力信号として扱う。
The operation of the waveform equalizer configured as above will be explained with reference to FIGS. 6 and 7. However, since any signal waveform is expressed as a linear sum of extremely thin pulses, these extremely thin pulses will be treated as input signals below.

入力端子1に入力された振幅1の信号は分岐回
路201により2つに分けられ、一方の信号aは
遅延時間Tをもつタツプ付遅延線301に入力さ
れる。そして、該タツプ付遅延線301により時
間Tだけ遅延された信号は、一部は減衰すること
なく加算器601に入力されて主信号となり、一
部は同様にタツプ付遅延線302に入力されて合
計2T遅延された後、インバータ・ノンインバー
タ選択回路351に入力される。該回路351の
出力は加算器401で遅延線301を通つていな
い遅延時間ゼロの信号と加算され、振幅調整ボリ
ユーム501を介して、エコー信号として加算器
601に入力される。
A signal with an amplitude of 1 input to input terminal 1 is divided into two by branch circuit 201, and one signal a is input to tapped delay line 301 having delay time T. A portion of the signal delayed by the time T by the tapped delay line 301 is input to the adder 601 without attenuation and becomes the main signal, and a portion is similarly input to the tapped delay line 302. After being delayed by a total of 2T, it is input to the inverter/non-inverter selection circuit 351. The output of the circuit 351 is added in an adder 401 to a signal with zero delay time that has not passed through the delay line 301, and is inputted to the adder 601 as an echo signal via an amplitude adjustment volume 501.

また、上記分岐回路201の他方の出力は90゜
移相器202によつて位相が90゜回転され、該信
号bは、一部は遅延なしに加算器402の入力と
なり、一部はタツプ付遅延線303,304を経
て計2T遅延された後、インバータ・ノンインバ
ータ選択回路352を経て加算器402に入力さ
れて加算され、その出力信号は振幅調整ボリユー
ム502で振幅調整された後、エコー信号として
加算器601に入力される。従つて、出力端子7
には主信号と2組のエコー信号が出力されること
になる。
Further, the phase of the other output of the branch circuit 201 is rotated by 90° by a 90° phase shifter 202, and part of the signal b becomes an input to an adder 402 without delay, and a part is input to an adder 402 with a tap. After being delayed by a total of 2T via delay lines 303 and 304, the signal is input to an adder 402 via an inverter/non-inverter selection circuit 352 and added, and the output signal is amplitude-adjusted by an amplitude adjustment volume 502 and then converted into an echo signal. It is input to the adder 601 as . Therefore, output terminal 7
A main signal and two sets of echo signals are output.

いま、インバータ・ノンインバータ選択回路3
51,352において、それぞれノンインバー
タ、インバータを選択するものとし、又、振幅調
整用ボリユーム501,502により振幅がそれ
ぞれkcosθ0,ksinθ0(ただし、k,θ0は定数であ
り、kはエコー信号と主信号との振幅比、θ0は余
弦形特性を基準として周波数軸上で本波形等化器
の群遅延又は振幅特性を水平方向にずらせる量で
ある。)となるように調整されたものとすると、
等化器全体の伝達関数F1(ω)はω=2πfとして、 F1(ω)=1+2kcos(ωT−θ0) ……(7) となり、振幅特性及び群遅延特性G1(ω),τ1
(ω)はそれぞれ G1(ω)=20log10〔1 +2kcos(ωT−θ0)〕 τ1(ω)=0 (dB) (秒)(8) となる。この特性を第7図a,bに実線で示す。
この図からわかるように、遅延特性は不変のまま
で、振幅特性のみを任意の周波数θ0/Tだけ水平
方向(周波数軸方向)にずらすことができる。θ0
=0の場合は第7図aに破線で示す特性となり、
これは第2図aでa1=a-1=kとした場合に一致
し、又、θ0=π/2の場合は第2図bでb1=b-1
=kとした場合に一致することは明白である。
Now, inverter/non-inverter selection circuit 3
In 51 and 352, non-inverter and inverter are selected, respectively, and the amplitudes are set to kcosθ 0 and ksinθ 0 respectively by amplitude adjustment volumes 501 and 502 (however, k and θ 0 are constants, and k is an echo signal and the main signal, and θ 0 is the amount by which the group delay or amplitude characteristic of this waveform equalizer is shifted in the horizontal direction on the frequency axis based on the cosine characteristic. Assuming that,
The transfer function F 1 (ω) of the entire equalizer is F 1 (ω) = 1 + 2kcos (ωT - θ 0 ) ...(7) where ω = 2πf, and the amplitude characteristics and group delay characteristics G 1 (ω), τ 1
(ω) is G 1 (ω) = 20log 10 [1 + 2kcos (ωT - θ 0 )] τ 1 (ω) = 0 (dB) (second) (8). This characteristic is shown by solid lines in FIGS. 7a and 7b.
As can be seen from this figure, only the amplitude characteristic can be shifted in the horizontal direction (frequency axis direction) by an arbitrary frequency θ 0 /T while the delay characteristic remains unchanged. θ 0
When = 0, the characteristics are shown by the broken line in Figure 7a,
This corresponds to the case where a 1 = a -1 = k in Figure 2 a, and when θ 0 = π/2, b 1 = b -1 in Figure 2 b.
It is clear that they match when =k.

次に、インバータ・ノンインバータ選択回路3
51,352において、それぞれインバータ、ノ
ンインバータを選択するものとし、又振幅調整ボ
リユーム501,502により振幅がそれぞれ
kcosθ0,ksinθ0となるよう調整されたものとする
と、等化器全体の伝達関数F2(ω)は F2(ω)=1−j2ksin(ωT−θ0) ……(9) となり、k≪1の場合の振幅及び群遅延特性G2
(ω),τ2(ω)はそれぞれ となる。この特性を第7図c,dに実線で示す。
この図からわかるように、振幅特性は不変のまま
で、群遅延特性のみを任意の周波数θ0/Tだけ水
平方向(周波数軸方向)にずらすことができる。
又、θ0=0の場合の特性を第7図dに破線で示
す。これは第2図aでa1=−a-1=kとした場合
に一致する。
Next, inverter/non-inverter selection circuit 3
Inverter and non-inverter are selected in 51 and 352, respectively, and the amplitude is adjusted by amplitude adjustment volume 501 and 502, respectively.
Assuming that the adjustment is made so that kcosθ 0 and ksinθ 0 , the transfer function F 2 (ω) of the entire equalizer becomes F 2 (ω)=1−j2ksin(ωT−θ 0 ) ……(9), Amplitude and group delay characteristics G 2 when k≪1
(ω) and τ 2 (ω) are respectively becomes. This characteristic is shown by solid lines in FIG. 7c and d.
As can be seen from this figure, only the group delay characteristic can be shifted in the horizontal direction (frequency axis direction) by an arbitrary frequency θ 0 /T while the amplitude characteristic remains unchanged.
Further, the characteristic when θ 0 =0 is shown by a broken line in FIG. 7d. This corresponds to the case where a 1 =−a −1 =k in FIG. 2a.

なお、上記実施例では主信号の前後にエコー信
号を各1個ずつ用いた場合について示したが、こ
れは1個のみの場合に限定されるものではなく、
複数個のエコー信号を用いて等化することもで
き、この場合は更に複数な周波数特性の等化が可
能となる。
In addition, although the above embodiment shows the case where one echo signal is used before and after the main signal, this is not limited to the case where only one echo signal is used.
Equalization can also be performed using a plurality of echo signals, and in this case, it becomes possible to equalize a plurality of frequency characteristics.

又、上記実施例ではインバータ・ノンインバー
タ選択回路と振幅調整ボリユームを別々に構成し
たが、これは極性反転機能をもつボリユーム1個
によつても構成できる。また遅延回路としてのタ
ツプ付遅延線をシフトレジスタあるいはケーブル
等の遅延素子で置き換えてもよく、さらに分岐回
路と90゜移相器を90゜ハイブリツド回路で構成して
もよい。
Further, in the above embodiment, the inverter/non-inverter selection circuit and the amplitude adjustment volume were constructed separately, but this can also be constructed with a single volume having a polarity inversion function. Further, the tapped delay line serving as the delay circuit may be replaced with a delay element such as a shift register or a cable, and furthermore, the branch circuit and the 90° phase shifter may be constructed with a 90° hybrid circuit.

以上のように、この発明によれば、正弦形等化
器と余弦形等化器とを組合わせ、かつタツプ係数
を特定の関係で重み付けすることにより、振幅あ
るいは群遅延のいずれか一方のみを余弦形の周波
数特性を所望の周波数だけずらせた余弦形の周波
数特性とすることができる効果がある。
As described above, according to the present invention, by combining a sine equalizer and a cosine equalizer and weighting the tap coefficients in a specific relationship, only either the amplitude or the group delay can be adjusted. There is an effect that the cosine-shaped frequency characteristic can be changed to a cosine-shaped frequency characteristic shifted by a desired frequency.

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

第1図は従来の波形等化器のブロツク構成図、
第2図a,bはそれぞれ第1図の波形等化器の素
子数が小さい場合のブロツク構成図、第3図は第
2図aの波形等化器の時間応答波形を示す図、第
4図および第5図は振幅等化器と遅延等化器の周
波数特性を示す図、第6図は本発明の一実施例に
よる波形等化器のブロツク構成図、第7図は第6
図の波形等化器の振幅および群遅延の周波数特性
図である。 201…分岐回路、202…移相器、8,9…
第1および第2の遅延回路網、501,502…
振幅調整ボリユーム(振幅調整回路)、601…
加算器。なお、図中同一符号は同一又は相当部分
を示す。
Figure 1 is a block diagram of a conventional waveform equalizer.
Figures 2a and 2b are block diagrams of the waveform equalizer in Figure 1 when the number of elements is small, Figure 3 is a diagram showing the time response waveform of the waveform equalizer in Figure 2a, and Figure 4 5 and 5 are diagrams showing frequency characteristics of an amplitude equalizer and a delay equalizer, FIG. 6 is a block diagram of a waveform equalizer according to an embodiment of the present invention, and FIG.
FIG. 4 is a frequency characteristic diagram of amplitude and group delay of the waveform equalizer shown in FIG. 201... Branch circuit, 202... Phase shifter, 8, 9...
First and second delay networks, 501, 502...
Amplitude adjustment volume (amplitude adjustment circuit), 601...
Adder. Note that the same reference numerals in the figures indicate the same or equivalent parts.

Claims (1)

【特許請求の範囲】 1 入力信号を分岐する分岐回路と、 この分岐回路の一方の出力を所定時間Tだけ遅
延して主信号を作成するとともに上記分岐回路の
一方の出力とこれを時間2Tだけ遅延した信号又
は該遅延信号の反転信号のいずれか一方とを加算
してエコー信号を作成する第1の遅延回路網と、 上記分岐回路の他方の出力を90゜移相する移相
器と、 この移相器の出力とこれを時間2Tだけ遅延し
た信号又は該遅延信号の反転信号のいずれか一方
とを加算してエコー信号を作成する第2の遅延回
路網と、 エコー信号と主信号との振幅比をk、余弦形特
性を基準として周波数軸上で本波形等化器の群遅
延又は振幅特性を水平方向にずらせる量をθ0とし
たとき、上記第1、第2の遅延回路網のエコー信
号出力にkcosθ0,ksinθ0なる重みを付けて振幅調
整する第1、第2の振幅調整回路と、 この両振幅調整回路の出力と上記第1の遅延回
路網の主信号出力とを加算する加算回路とを備
え、 上記第1、第2の振幅調整回路により振幅調整
を行なうことにより、群遅延又は振幅特性が余弦
形の周波数特性を水平方向に所望量だけずらせる
ようにしたことを特徴とする波形等化器。
[Claims] 1. A branch circuit that branches an input signal, and one output of this branch circuit that is delayed by a predetermined time T to create a main signal, and which is connected to the output of one of the branch circuits by a time 2T. a first delay circuit network that creates an echo signal by adding either the delayed signal or an inverted signal of the delayed signal; and a phase shifter that shifts the phase of the other output of the branch circuit by 90 degrees. a second delay circuit network that creates an echo signal by adding the output of the phase shifter and either a signal delayed by a time of 2T or an inverted signal of the delayed signal; and the echo signal and the main signal. The first and second delay circuits first and second amplitude adjustment circuits that adjust the amplitude by weighting the echo signal output of the network with kcos θ 0 and ksin θ 0 ; the outputs of both amplitude adjustment circuits and the main signal output of the first delay circuit network; and an adder circuit for adding , and by adjusting the amplitude by the first and second amplitude adjustment circuits, the frequency characteristic whose group delay or amplitude characteristic is a cosine shape is shifted by a desired amount in the horizontal direction. A waveform equalizer characterized by:
JP12491081A 1981-08-07 1981-08-07 Waveform equalizer Granted JPS5825707A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP12491081A JPS5825707A (en) 1981-08-07 1981-08-07 Waveform equalizer

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP12491081A JPS5825707A (en) 1981-08-07 1981-08-07 Waveform equalizer

Publications (2)

Publication Number Publication Date
JPS5825707A JPS5825707A (en) 1983-02-16
JPH0117289B2 true JPH0117289B2 (en) 1989-03-29

Family

ID=14897133

Family Applications (1)

Application Number Title Priority Date Filing Date
JP12491081A Granted JPS5825707A (en) 1981-08-07 1981-08-07 Waveform equalizer

Country Status (1)

Country Link
JP (1) JPS5825707A (en)

Families Citing this family (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS59161117A (en) * 1983-03-04 1984-09-11 Nec Corp Switched capacitor type cable equalizer
JPS6335021A (en) * 1986-07-30 1988-02-15 Nec Corp Automatic equalizer
JPS6335022A (en) * 1986-07-30 1988-02-15 Nec Corp Automatic equalizer
JPH0775332B2 (en) * 1987-10-14 1995-08-09 キヤノン株式会社 Receiver

Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS52109319A (en) * 1976-03-10 1977-09-13 Sharp Corp Receiver equipped with adapted type digital modem
JPS55149517A (en) * 1979-05-09 1980-11-20 Nec Corp Amplitude variable filter

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS52109319A (en) * 1976-03-10 1977-09-13 Sharp Corp Receiver equipped with adapted type digital modem
JPS55149517A (en) * 1979-05-09 1980-11-20 Nec Corp Amplitude variable filter

Also Published As

Publication number Publication date
JPS5825707A (en) 1983-02-16

Similar Documents

Publication Publication Date Title
JP3357956B2 (en) Decision feedback equalizer
JPH0575393A (en) Equalizer for data receiver
US4491808A (en) Equalizer circuit for use in communication unit
JPH0117289B2 (en)
JPS6017119B2 (en) artificial reverberation device
US6898281B1 (en) System and method for filtering echo/NEXT signal interferrence
US4779217A (en) Octave multiple filter
US4607241A (en) Transversal filter equalizer with minimally interactive adjustments
US4757516A (en) Transversal equalizer
US9118511B1 (en) Reflective analog finite impulse response filter
JPH0117288B2 (en)
JPS5812419A (en) Waveform equalizer
JPS59112714A (en) Automatic waveform equalizer
JPH02159129A (en) Equalizer
US6025750A (en) Digital filter with long impulse response
JPH0624397B2 (en) DC compensation circuit
JPS6369309A (en) Transversal type equalizer
JPS6166418A (en) Automatic equalizer
JPH0411038B2 (en)
JPS62172809A (en) Digital filter
JPS6384324A (en) Automatic equalizer
JPH04373208A (en) Waveform equalizing circuit
JPH0212063B2 (en)
JPS61172429A (en) Group delay equalizer
JPS6114689B2 (en)