JPH0216076B2 - - Google Patents

Info

Publication number
JPH0216076B2
JPH0216076B2 JP56196046A JP19604681A JPH0216076B2 JP H0216076 B2 JPH0216076 B2 JP H0216076B2 JP 56196046 A JP56196046 A JP 56196046A JP 19604681 A JP19604681 A JP 19604681A JP H0216076 B2 JPH0216076 B2 JP H0216076B2
Authority
JP
Japan
Prior art keywords
output
differentiating means
signal
amplitude
noise
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 - Lifetime
Application number
JP56196046A
Other languages
Japanese (ja)
Other versions
JPS5896473A (en
Inventor
Seiichi Hashimoto
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.)
Panasonic Holdings Corp
Original Assignee
Matsushita Electric Industrial 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 Matsushita Electric Industrial Co Ltd filed Critical Matsushita Electric Industrial Co Ltd
Priority to JP56196046A priority Critical patent/JPS5896473A/en
Publication of JPS5896473A publication Critical patent/JPS5896473A/en
Publication of JPH0216076B2 publication Critical patent/JPH0216076B2/ja
Granted legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H04ELECTRIC COMMUNICATION TECHNIQUE
    • H04NPICTORIAL COMMUNICATION, e.g. TELEVISION
    • H04N5/00Details of television systems
    • H04N5/14Picture signal circuitry for video frequency region
    • H04N5/21Circuitry for suppressing or minimising disturbance, e.g. moiré or halo

Landscapes

  • Engineering & Computer Science (AREA)
  • Multimedia (AREA)
  • Signal Processing (AREA)
  • Picture Signal Circuits (AREA)
  • Signal Processing Not Specific To The Method Of Recording And Reproducing (AREA)

Description

【発明の詳細な説明】 この発明は磁気記録再生装置やビデオデイスク
装置等に応用して、記録・再生されたビデオ信号
に含まれる特定域の雑音信号成分を軽減する雑音
除去装置に関するものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a noise removal device that is applied to magnetic recording and reproducing devices, video disk devices, etc., and reduces noise signal components in a specific range included in recorded and reproduced video signals. .

従来の家庭用磁気記録再生装置においては使用
する周波数帯域に余裕があり、再生されたビデオ
信号の全周波数帯域にわたりノイズが含まれてい
ても、視覚的には高周波帯域のノイズが目立つ程
度であつた。このため従来高周波帯域のノイズの
除去を主目的として雑音除去が行なわれていた
が、近年家庭用磁気記録再生装置の小型化が進む
につれて高密度化や短波長域の使用等により、ノ
イズの成分も従来と異なり従来よりも低周波帯域
のノイズの除去が必要となつてきた。しかしなが
ら従来の雑音除去装置では低周波帯域のノイズを
除去しようとすると、高周波数成分を含む信号の
エツジ部分で雑音が除去されない部分の幅がその
低周波帯域に比例して広くなるという欠点があつ
た。すなわち、従来の雑音除去装置を具体的に説
明すると、第1図において、1はビデオ信号の入
力端子、2はビデオ信号から高域周波数成分を分
離する微分手段(これは低域を遮断する特定域の
高域を通過するフイルタ特性を持つものなら何で
も良い)、3は増幅器、4は振幅制限器、5は減
衰器、6は混合器、7は出力端子であつて、入力
端子であつて、入力端子1から入力されたビデオ
信号は微分手段2で高域周波数成分が分離され、
増幅器3で増幅され、振幅制限器4で一定振幅に
制限され、減衰器5で適当なレベルに減衰され
る。混合器6は前記入力端子1から入力されたビ
デオ信号と前記減衰器5の出力信号を互いに逆相
で混合し、出力端子7に雑音が軽減されたビデオ
信号を出力する。第2図は微分手段の具体回路で
あつて、8は微分手段の入力端子、9は容量、1
0は抵抗、11は微分手段の出力端子であ、容量
9の容量値をC.抵抗10の抵抗値をRとすると微
分手段の伝達特性は、SRC/(SRC+1)とな
る(Sはラプラス変換変数)。いま、微分手段2
の入力端子8に第3図aに示すビデオ信号が入力
された場合、微分手段2の出力端子11には第3
図bに示す信号が出力される。すなわち入力信号
がステツプ状に一定レベルだけ変化した時、変化
の瞬間微分手段2の出力も同じレベルだけ変化
し、その後入力信号の変化の正負にしたがつて放
電または充電電流が流れ、微分手段2の出力電位
は抵抗の一端が結合されている基準点の電位に向
つて変化する。なお、ここでは容量9から抵抗1
0を介して基準点へ電流が流れる場合を放電、こ
れとは逆方向に容量9へ電流が流れる場合を充電
と表現している。この場合の充放電の時定数は
RCである。そして微分手段2の信号を増幅し、
振幅制限を加えた場合の波形は第3図cのように
なる。いま入力信号に対して振幅制限されるレベ
ルをVB、増幅器3の増幅度をKとすると、振幅
制限器4の出力波形は微分手段2の出力がVB
超える部分については振幅制限されるので、レベ
ルがKVBのフラツト信号となる。このフラツト
部分の時間幅は入力信号の変化レベルと微分回路
の時定数RCで決定される。たとえば時刻t=0
でレベルVAだけ変化するステツプ信号を仮定す
ると、微分手段2の出力電圧vは、 v=VAe−1/RCt となり、これが振幅制限レベルVBに達する時間t1
は、 t1=RC ln(VB/VA) となる。すなわち、この時間間隔だけ微分信号は
振幅制限される。第3図dは振幅制限された出力
を減衰器5で所定のレベルに減衰して入力信号と
逆位相の関係で混合器6により混合した出力波形
である。
Conventional household magnetic recording and reproducing devices have ample frequency range to use, and even if the reproduced video signal contains noise across the entire frequency band, the noise in the high frequency band is visually noticeable. Ta. For this reason, noise removal has conventionally been carried out with the main purpose of removing noise in the high frequency band, but in recent years, with the miniaturization of household magnetic recording and reproducing devices, the increase in density and the use of short wavelength bands have made it possible to eliminate noise components. However, unlike in the past, it has become necessary to remove noise in a lower frequency band than in the past. However, when attempting to remove noise in the low frequency band with conventional noise removal devices, the width of the edge portion of the signal containing high frequency components where noise is not removed increases in proportion to the low frequency band. Ta. That is, to explain the conventional noise removal device in detail, in FIG. 3 is an amplifier, 4 is an amplitude limiter, 5 is an attenuator, 6 is a mixer, 7 is an output terminal, and 7 is an input terminal. , the video signal input from the input terminal 1 is separated into high frequency components by the differentiating means 2,
The signal is amplified by an amplifier 3, limited to a constant amplitude by an amplitude limiter 4, and attenuated to an appropriate level by an attenuator 5. The mixer 6 mixes the video signal input from the input terminal 1 and the output signal of the attenuator 5 in opposite phases, and outputs a video signal with reduced noise to the output terminal 7. Figure 2 shows a specific circuit of the differentiating means, where 8 is the input terminal of the differentiating means, 9 is the capacitor, and 1
0 is a resistor, 11 is an output terminal of the differentiating means, and the capacitance value of capacitor 9 is C. If the resistance value of resistor 10 is R, the transfer characteristic of the differentiating means is SRC/(SRC+1) (S is Laplace transform variable). Now, differentiation means 2
When the video signal shown in FIG. 3a is input to the input terminal 8 of the differentiating means 2, the third
The signal shown in Figure b is output. In other words, when the input signal changes stepwise by a certain level, the output of the differentiating means 2 changes by the same level at the moment of the change, and then a discharge or charging current flows according to the sign or negative of the change in the input signal, and the output of the differentiating means 2 changes by the same level. The output potential of changes toward the potential of the reference point to which one end of the resistor is coupled. In addition, here, from capacitance 9 to resistance 1
The case where current flows to the reference point via 0 is called discharge, and the case where current flows to the capacitor 9 in the opposite direction is called charge. The charging/discharging time constant in this case is
It is RC. Then, the signal of the differentiating means 2 is amplified,
The waveform when amplitude limitation is applied is as shown in FIG. 3c. Assuming that the level at which the amplitude of the input signal is limited is V B and the amplification degree of the amplifier 3 is K, the output waveform of the amplitude limiter 4 is amplitude limited for the portion where the output of the differentiating means 2 exceeds V B. Therefore, it becomes a flat signal with a level of KV B. The time width of this flat portion is determined by the change level of the input signal and the time constant RC of the differentiator circuit. For example, time t=0
Assuming a step signal that changes by level V A at
is, t 1 = RC ln(V B /V A ). That is, the amplitude of the differential signal is limited by this time interval. FIG. 3d shows an output waveform obtained by attenuating the amplitude-limited output to a predetermined level by an attenuator 5 and mixing it by a mixer 6 in a phase opposite to that of the input signal.

つぎに、入力信号に第3図aのように高周波の
ノイズNが重畳している場合を考えると、微分手
段2の出力にもその通過帯域に応じてノイズNが
重畳する。このノイズNのうち振幅制限器4でリ
ミツトされない部分は第3図cのように残り、混
合器6においてキヤンセルされる。
Next, considering the case where high frequency noise N is superimposed on the input signal as shown in FIG. 3a, the noise N is also superimposed on the output of the differentiating means 2 according to its pass band. The portion of this noise N that is not limited by the amplitude limiter 4 remains as shown in FIG. 3c and is canceled by the mixer 6.

しかしながら、このノイズ成分のうちリミツト
される部分についてはクリツプかれてノイズを取
り残すことができないため、混合器6の出力では
ノイズがキヤンセルされず、第3図dのN′のよ
うになる。しかもこのリミツトされた部分は一定
の直流レベルを持つているので、混合器6の出力
において、直流成分が減少、言いかえると信号成
分が減少してしまう。要するに、この雑音除去装
置は、入力信号のフラツトな部分については雑音
が除去されるが、直流レベルが変化する部分、交
流成分を持つ部分については雑音除去効果がな
く、逆に信号成分が減少するという欠点がある。
さらに、微分手段2の出力信号がリミツトされフ
ラツトとなる部分の時間幅t1は微分手段2の時定
数RCに比例し、この時定数は微分手段2の通過
帯域を表わし、低周波のノイズを通過させるため
にはRCを大きくしなければならず、そのため時
間幅t1が大きくなつてしまう。
However, since the limited portion of this noise component is clipped and the noise cannot be left behind, the output of the mixer 6 does not cancel the noise, resulting in a signal N' in FIG. 3d. Moreover, since this limited portion has a constant DC level, the DC component at the output of the mixer 6 is reduced, or in other words, the signal component is reduced. In short, this noise removal device removes noise from flat parts of the input signal, but has no noise removal effect from parts where the DC level changes or parts with AC components, and conversely the signal components decrease. There is a drawback.
Furthermore, the time width t 1 of the portion where the output signal of the differentiating means 2 is limited and becomes flat is proportional to the time constant RC of the differentiating means 2, and this time constant represents the pass band of the differentiating means 2 and suppresses low frequency noise. In order to allow the signal to pass, RC must be increased, which increases the time width t1 .

したがつて、この発明の目的は、特にビデオ信
号に含まれる急峻なレベル変化の直後すなわちビ
デオ信号のエツジ部分における残留ノイズの軽減
を促進し、そのエツジ部分における信号成分の欠
除が少量で補正が簡単な雑音除去装置を提供する
ことである。
Therefore, it is an object of the present invention to promote the reduction of residual noise, especially immediately after a sharp level change included in a video signal, that is, at the edge portion of the video signal, and to compensate for the loss of signal components at the edge portion with a small amount. The object of the present invention is to provide a simple noise removal device.

この発明の一実施例を第4図ないし第7図に示
す。まず第4図において、第1図と同等の動作を
するものについては同一符号を付している。すな
わち1は入力端子、2は微分手段、3は増幅器、
4は振幅制限器(リミツタ手段)、5は減衰器、
6は混合器、7は出力端子、12は振幅制限器4
の動作を検出して微分手段2の充放電電流を増大
させる急速充放電回路である。この動作を第5図
を用いて説明する。ここでは簡単のため入力信号
として、第5図aに示すようにt=0でレベル
VAに変化するステツプ信号を用い、微分手段2
としては第2図に示したものを用いている。第5
図bは微分手段2の出力であつて、t=0でレベ
ルVAに一瞬変化し、その後は、この実施例によ
る急速放電回路12がない場合、前述の第3図で
示したように時定数RCで放電し(第5図bの破
線)、このとき振幅制限器4で振幅制限される期
間は、 t1=−RC ln(VB/VA) となるが、これに対してこの実施例の場合急速充
放電回路12があるため、微分手段2の出力レベ
ルの絶対値が振幅制限器4の振幅制限するレベル
VBを越えている時急速充放電回路12が動作し
て、微分手段2の出力が正の時は放電回路を、ま
た負の時は充電回路をそれぞれ動作させて、第5
図bの実線で示すように放電速度が速くなる。そ
の結果、時間t1より短かい時間t2でレベルVBに達
する。微分手段2の出力がレベルVB達すると、
放電は微分手段2で決る時定数RCとなり、振幅
制限器4の出力には時間t2だけ振幅制限された信
号が取り出されることとなる(第5図c)。ここ
で、充放電電流を十分に大きくすると時間t2を十
分に小さくすることができることはいうまでもな
い。そのため、t2以降については微分手段の通過
帯域に従つたノイズを取り出すことができる。第
5図dは混合器の出力波形である。こうして、急
速充放電回路12の電流を適当な値に選ぶことに
より、入力信号のレベル変動直後のノイズも分離
することができ、また、振幅制限器4の出力にお
いてフラツト部分がきわめて少なくなるので、こ
の部分による信号成分の損失も少なくなる。また
入力信号から振幅制限器の出力を差引いたこの雑
音除去装置の出力は時間t2を十分に小さくした
時、第5図dのように入力信号を若干デイエンフ
アシスした特性となる。したがつて、これはエン
フアシスすることにより補正できる。
An embodiment of this invention is shown in FIGS. 4 to 7. First, in FIG. 4, parts that operate in the same way as in FIG. 1 are given the same reference numerals. That is, 1 is an input terminal, 2 is a differentiating means, 3 is an amplifier,
4 is an amplitude limiter (limiter means); 5 is an attenuator;
6 is a mixer, 7 is an output terminal, 12 is an amplitude limiter 4
This is a rapid charging/discharging circuit that increases the charging/discharging current of the differentiating means 2 by detecting the operation of the differential means 2. This operation will be explained using FIG. 5. Here, for simplicity, we will use the input signal as the level at t=0 as shown in Figure 5a.
Using a step signal that changes to V A , differentiating means 2
The one shown in Figure 2 is used. Fifth
Figure b shows the output of the differentiating means 2, which instantaneously changes to level V A at t=0, and after that, if there is no rapid discharge circuit 12 according to this embodiment, the output changes over time as shown in Figure 3 above. Discharge occurs at a constant RC (dashed line in Figure 5b), and the period during which the amplitude is limited by the amplitude limiter 4 is t 1 = -RC ln (V B /V A ); In the case of the embodiment, since the rapid charge/discharge circuit 12 is provided, the absolute value of the output level of the differentiating means 2 is the level at which the amplitude limiter 4 limits the amplitude.
When the output of the differentiating means 2 is positive, the quick charging/discharging circuit 12 is operated, and when the output of the differentiating means 2 is positive, the discharging circuit is operated, and when it is negative, the charging circuit is operated.
As shown by the solid line in Figure b, the discharge rate becomes faster. As a result, level V B is reached in time t 2 which is shorter than time t 1 . When the output of differentiating means 2 reaches level V B ,
The discharge has a time constant RC determined by the differentiating means 2, and a signal whose amplitude is limited by time t2 is taken out at the output of the amplitude limiter 4 (FIG. 5c). Here, it goes without saying that if the charging/discharging current is made sufficiently large, the time t 2 can be made sufficiently small. Therefore, after t2 , it is possible to extract noise according to the passband of the differentiating means. FIG. 5d shows the output waveform of the mixer. In this way, by selecting the current of the rapid charge/discharge circuit 12 to an appropriate value, it is possible to separate the noise immediately after the level fluctuation of the input signal, and since the flat portion in the output of the amplitude limiter 4 is extremely reduced, Loss of signal components due to this portion is also reduced. Furthermore, when the time t 2 is made sufficiently small, the output of this noise canceling device, which is obtained by subtracting the output of the amplitude limiter from the input signal, has a characteristic in which the input signal is slightly de-emphasized, as shown in FIG. 5d. Therefore, this can be corrected by emphasis.

なお急速充放電回路12の電流としては、定電
流であつても良いし、微分手段の出力レベルに比
例したものであつても良い。後者の場合は実質的
に微分手段を構成する抵抗の値を小さくして、時
定数を小さくするのと同等である。
Note that the current of the rapid charge/discharge circuit 12 may be a constant current or may be proportional to the output level of the differentiating means. The latter case is essentially equivalent to reducing the time constant by reducing the value of the resistance constituting the differentiating means.

第6図は前記微分手段2.振幅制限器4および
急速充放電回路12の具体回路であつて、8は微
分手段の入力端子であり、容量9および抵抗10
は微分手段を構成し、抵抗13.トランジスタ1
4,15および電圧源16は振幅制限器を構成
し、抵抗17およびトランジスタ18は充電回路
を構成し、さらに抵抗19およびトランジスタ2
0は放電回路を構成している。電圧源21は急速
充放電回路の出力を適当にバイアスするためのも
のであつて、これはまた増幅器3の入力バイアス
電源を兼ねることができる。振幅制限器のリミツ
タ特性は、抵抗13とトランジスタ14,15の
導通および遮断特性により決り、電圧源16の電
圧値をE16.トランジスタ14,15のベース・エ
ミツタ間電圧値をVBEとすると、増幅器3の出力
電圧がE16−VBE以上、E16+VBE以下でトランジ
スタ14,15は遮断して、振幅制限器出力には
入力信号がそのまま減衰器5に出力され、E16
VBE以下ではトランジスタ14が導通、E16+VBE
以上ではトランジスタ16が導通して、その出力
はそれぞれほぼE16−VBE・E16+VBEとなる。さ
らに、トランジスタ14,15が遮断時には抵抗
17,19に電流が流れないが、いずれかの導通
時には抵抗17,19に電流が流れ、発生する電
圧が一定値に達すると急速充放電回路を構成する
トランジスタ18,20のいずれかが動作する。
すなわち、微分手段2の出力が一定値を越すと急
速充放電回路を動作させ、微分手段の充放電電流
を増加して、充放電を速くすることとなる。な
お、トランジスタ14,15のベース間に適当な
電位を与えてリミツタ特性を変えることもでき
る。
FIG. 6 shows the differentiating means 2. A concrete circuit of the amplitude limiter 4 and the rapid charging/discharging circuit 12, in which 8 is an input terminal of a differentiating means, a capacitor 9 and a resistor 10
constitutes a differentiating means, and resistor 13. transistor 1
4, 15 and voltage source 16 constitute an amplitude limiter, resistor 17 and transistor 18 constitute a charging circuit, and further resistor 19 and transistor 2
0 constitutes a discharge circuit. The voltage source 21 is for appropriately biasing the output of the rapid charge/discharge circuit, and can also serve as the input bias power supply for the amplifier 3. The limiter characteristics of the amplitude limiter are determined by the conduction and cutoff characteristics of the resistor 13 and the transistors 14 and 15, and when the voltage value of the voltage source 16 is E16 and the base-emitter voltage value of the transistors 14 and 15 is VBE , When the output voltage of the amplifier 3 is more than E 16 −V BE and less than E 16 +V BE , the transistors 14 and 15 are cut off, and the input signal is directly outputted to the attenuator 5 as the amplitude limiter output, and E 16
Below V BE , transistor 14 is conductive, E 16 +V BE
In the above case, the transistor 16 becomes conductive, and its output becomes approximately E 16 −V BE and E 16 +V BE , respectively. Further, when the transistors 14 and 15 are cut off, no current flows through the resistors 17 and 19, but when either of them is turned on, current flows through the resistors 17 and 19, and when the generated voltage reaches a certain value, a rapid charge/discharge circuit is formed. Either transistor 18 or 20 operates.
That is, when the output of the differentiating means 2 exceeds a certain value, the rapid charging/discharging circuit is operated to increase the charging/discharging current of the differentiating means to speed up charging and discharging. Note that the limiter characteristics can also be changed by applying an appropriate potential between the bases of the transistors 14 and 15.

なお、急速充放電回路の構成は種々の変形が考
えられるが、たとえば抵抗17をトランジスタ1
8と同じ特性を持つダイオードに置き換え、トラ
ンジスタ18のコレクタをトランジスタ20のベ
ースに結合し、トランジスタ20のコレクタに適
当な値を持つ抵抗を挿入し、トランジスタ20の
エミツタを抵抗19の接地側を抵抗10と電圧源
21の接続点に接続するようにして、振幅制限器
を構成するトランジスタ14,15が導通する
時、微分手段2を構成する抵抗10に並列に適当
な値の抵抗を挿入することにより微分手段2の時
定数を小さくすることもできる。
Note that various modifications of the configuration of the rapid charge/discharge circuit are possible; for example, the resistor 17 may be replaced with the transistor 1.
8, connect the collector of transistor 18 to the base of transistor 20, insert a resistor with an appropriate value into the collector of transistor 20, connect the emitter of transistor 20 to the ground side of resistor 19, and connect the collector of transistor 18 to the base of transistor 20. 10 and the voltage source 21, and insert a resistor of an appropriate value in parallel with the resistor 10 constituting the differentiating means 2 when the transistors 14 and 15 constituting the amplitude limiter become conductive. It is also possible to reduce the time constant of the differentiating means 2.

第7図はこの発明の他の実施例であつて、振幅
制限器と急速充放電回路を兼用するものである。
図において、8は微分手段の入力端子であり、容
量9および抵抗10は微分手段を構成し、電圧源
21によりその電圧値E21でバイヤスされている。
増幅器22は適当な増幅度と極性を持つている。
ダイオード23,24は振幅制限器を構成し、互
いに逆極性に結合されている。いま増幅器22は
十分大きな入力インピーダンスと十分小さな出力
インピーダンスを持ちその増幅度Kが正の時、出
力は入力と同相.負の時逆相とする。また、増幅
器22の入力と出力の直流電位は等しいものとす
る。同図に示すように、微分手段を構成する容量
9および抵抗10に直接増幅器22の入力端子を
結合し、振幅制限器を構成するダイオード23,
24の並列結合の一端は増幅器22の入力端子
に、他端は出力端子に結合される。これにより、
ダイオード23,24の一端には微分手段の出力
信号が、他端にはこれをK倍した交流信号が印加
される。したがつて、ダイオード23,24の両
端には微分手段の交流出力信号を(1−K)倍し
た信号が印加される。いまこの微分手段の出力信
号を(1−K)倍した信号の絶対値がダイオード
の導通電位VDを越えない時は出力としてそのま
ま取り出され、VDを越える時はダイオードが導
通し、導通電位VDとなる。このとき微分手段の
出力にはVD/1−Kなる電圧が発生する。ここで増 幅度Kは1以下の値であつて、リミツタ特性は増
幅度Kが1以下零以上で導通電位VDより大きい
値には増幅度Kが負の時、すなわち増幅器22の
入出力が逆極性の時、導通電位VDより小さい値
となり、したがつて増幅度Kの値を適当に選ぶこ
とにより任意のリミツタ特性を得ることができ
る。特に増幅度Kの負の時有用であつて、零の時
は増幅器22がないのに等しく、ダイオード2
3,24の他端は電圧源21に結合されているの
に等しい。またダイオード23,24は急速充放
電回路を兼ねており、微分手段出力がE21
VD/1−Kより小さくなろうとするとダイオード2 3により充電され、E21+VD/1−Kより大きくなろ うとするとダイオード24により放電される。こ
の時の充放電抵抗は増幅器22の出力インピーダ
ンスが十分小である時、ダイオード23,24の
導通抵抗となり十分に小さく、充放電は非常に速
くなる。なお、充放電の時定数を適当な値に設定
した時は微分手段の出力とダイオード23,2
4、増幅器22の入力端子の接続点間に適当な抵
抗を挿入すれば良い。
FIG. 7 shows another embodiment of the present invention, which serves as both an amplitude limiter and a rapid charge/discharge circuit.
In the figure, 8 is an input terminal of the differentiating means, and a capacitor 9 and a resistor 10 constitute the differentiating means, which is biased by a voltage source 21 at its voltage value E 21 .
Amplifier 22 has appropriate amplification and polarity.
The diodes 23 and 24 constitute an amplitude limiter and are coupled with opposite polarities. Now, the amplifier 22 has a sufficiently large input impedance and a sufficiently small output impedance, and when its amplification degree K is positive, the output is in phase with the input. When negative, the phase is reversed. Further, it is assumed that the input and output DC potentials of the amplifier 22 are equal. As shown in the figure, the input terminal of an amplifier 22 is directly coupled to a capacitor 9 and a resistor 10 which constitute a differentiating means, and a diode 23, which constitutes an amplitude limiter,
One end of the parallel combination of 24 is coupled to the input terminal of amplifier 22, and the other end is coupled to the output terminal. This results in
An output signal from the differentiating means is applied to one end of the diodes 23 and 24, and an AC signal obtained by multiplying this by K is applied to the other end. Therefore, a signal obtained by multiplying the AC output signal of the differentiating means by (1-K) is applied to both ends of the diodes 23 and 24. Now, when the absolute value of the signal obtained by multiplying the output signal of this differentiating means by (1-K) does not exceed the conduction potential V D of the diode, it is taken out as an output, and when it exceeds V D , the diode becomes conductive and the conduction potential It becomes V D. At this time, a voltage V D /1-K is generated at the output of the differentiating means. Here, the amplification degree K is a value of 1 or less, and the limiter characteristic is that when the amplification degree K is less than 1 or more than zero and is greater than the conduction potential V D , when the amplification degree K is negative, that is, the input and output of the amplifier 22 is When the polarity is reversed, the value becomes smaller than the conduction potential V D. Therefore, by appropriately selecting the value of the amplification degree K, arbitrary limiter characteristics can be obtained. This is particularly useful when the amplification factor K is negative; when it is zero, it is equivalent to the absence of the amplifier 22, and the diode 2
The other ends of 3 and 24 are equivalent to being coupled to voltage source 21. In addition, the diodes 23 and 24 also serve as a rapid charging/discharging circuit, and the output of the differentiating means is E 21
When it tries to become smaller than V D /1-K, it is charged by the diode 23, and when it tries to become larger than E 21 +V D /1-K, it is discharged by the diode 24. When the output impedance of the amplifier 22 is sufficiently small, the charging and discharging resistance at this time becomes the conduction resistance of the diodes 23 and 24, which is sufficiently small, and the charging and discharging becomes very fast. Note that when the charging/discharging time constant is set to an appropriate value, the output of the differentiating means and the diodes 23, 2
4. An appropriate resistor may be inserted between the connection points of the input terminals of the amplifier 22.

以上のように、この発明の雑音除去装置は、微
分回路で分離された高域周波数成分の振幅がリミ
ツタ手段の振幅制限レベルを超えている期間中急
速充放電回路により微分手段を流れる充放電電流
を増大させたので、入力信号のエツジ部分におい
て、微分回路で分離された高域周波数成分の振幅
がリミツタ手段の振幅制限レベルを超えている期
間を短くすることができ、入力信号の低周波帯域
のノイズまで除去しても、従来の欠点である入力
信号のエツジ部分のノイズの残留が極めて少な
く、しかも信号波形の欠除が少なくて欠除された
部分の波形が自然な形であつて、これを補正する
にはビデオ信号に若干のエンフアシス特性を加え
るだけ、また磁気記録再生装置において再生回路
のデイエンフアシス特性を若干減らすだけでよ
く、極めて忠実な再生信号を得ることができると
いう効果がある。
As described above, in the noise eliminating device of the present invention, the charging/discharging current flows through the differentiating means by the rapid charging/discharging circuit during the period when the amplitude of the high frequency component separated by the differentiating circuit exceeds the amplitude limit level of the limiter means. As a result, the period during which the amplitude of the high frequency component separated by the differentiating circuit exceeds the amplitude limit level of the limiter means in the edge portion of the input signal can be shortened, and the low frequency band of the input signal can be increased. Even if the noise of the edge part of the input signal is removed, there is very little residual noise in the edge part of the input signal, which is a drawback of the conventional method, and there is little deletion of the signal waveform, so the waveform of the deleted part has a natural shape. In order to correct this, it is only necessary to add a slight emphasis characteristic to the video signal, or to slightly reduce the de-emphasis characteristic of the reproduction circuit in the magnetic recording/reproducing device, and the effect is that an extremely faithful reproduction signal can be obtained.

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

第1図は従来の雑音除去装置のブロツク図、第
2図はその微分手段の回路図、第3図は従来の雑
音除去装置の動作波形図、第4図はこの発明の一
実施例のブロツク図、第5図はその動作波形図、
第6図は第4図の要部具体回路図、第7図はこの
発明の他の実施例の回路図である。 1…入力端子、2…微分手段、3…増幅器、4
…振幅制限器、5…減衰器、6…混合器、7…出
力端子、9…容量、10…抵抗、12…急速充放
電回路、13,17,19…抵抗、14,15,
18,20…トランジスタ、16,21…電圧
源、22…増幅器、23,24…ダイオード。
FIG. 1 is a block diagram of a conventional noise removing device, FIG. 2 is a circuit diagram of its differentiating means, FIG. 3 is an operating waveform diagram of a conventional noise removing device, and FIG. 4 is a block diagram of an embodiment of the present invention. Figure 5 is the operating waveform diagram,
FIG. 6 is a specific circuit diagram of the main part of FIG. 4, and FIG. 7 is a circuit diagram of another embodiment of the present invention. 1...Input terminal, 2...Differentiating means, 3...Amplifier, 4
... Amplitude limiter, 5... Attenuator, 6... Mixer, 7... Output terminal, 9... Capacitance, 10... Resistor, 12... Rapid charge/discharge circuit, 13, 17, 19... Resistor, 14, 15,
18, 20... Transistor, 16, 21... Voltage source, 22... Amplifier, 23, 24... Diode.

Claims (1)

【特許請求の範囲】[Claims] 1 入力信号中の高域周波数成分を分離する微分
手段と、この微分手段で分離された高域周波数成
分の振幅を制限するリミツタ手段と、前記微分回
路で分離された高域周波数成分の振幅が前記リミ
ツタ手段の振幅制限レベルを超えている期間中前
記微分手段を流れる充放電電流を増大させる急速
充放電回路と、前記リミツタ手段で得られた高域
周波数成分と前記入力信号とを互いに逆位相でか
つ適当なレベル関係で合成する混合器とを備えた
雑音除去装置。
1 Differentiating means for separating high frequency components in an input signal; limiter means for limiting the amplitude of the high frequency components separated by the differentiating means; and limiter means for limiting the amplitude of the high frequency components separated by the differentiating circuit. a rapid charging/discharging circuit that increases the charging/discharging current flowing through the differentiating means during a period in which the amplitude limit level of the limiter means is exceeded; and a high frequency component obtained by the limiter means and the input signal that are in opposite phases to each other. A noise removal device equipped with a mixer for synthesizing at a high level and with an appropriate level relationship.
JP56196046A 1981-12-04 1981-12-04 Noise removal device Granted JPS5896473A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP56196046A JPS5896473A (en) 1981-12-04 1981-12-04 Noise removal device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP56196046A JPS5896473A (en) 1981-12-04 1981-12-04 Noise removal device

Publications (2)

Publication Number Publication Date
JPS5896473A JPS5896473A (en) 1983-06-08
JPH0216076B2 true JPH0216076B2 (en) 1990-04-16

Family

ID=16351288

Family Applications (1)

Application Number Title Priority Date Filing Date
JP56196046A Granted JPS5896473A (en) 1981-12-04 1981-12-04 Noise removal device

Country Status (1)

Country Link
JP (1) JPS5896473A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH09178807A (en) * 1995-12-25 1997-07-11 Nec Corp Automatic handler for ic inspection

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH09178807A (en) * 1995-12-25 1997-07-11 Nec Corp Automatic handler for ic inspection

Also Published As

Publication number Publication date
JPS5896473A (en) 1983-06-08

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