JPS6224969Y2 - - Google Patents

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Publication number
JPS6224969Y2
JPS6224969Y2 JP9206380U JP9206380U JPS6224969Y2 JP S6224969 Y2 JPS6224969 Y2 JP S6224969Y2 JP 9206380 U JP9206380 U JP 9206380U JP 9206380 U JP9206380 U JP 9206380U JP S6224969 Y2 JPS6224969 Y2 JP S6224969Y2
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JP
Japan
Prior art keywords
detection
circuit
output
voltage
stage
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Expired
Application number
JP9206380U
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Japanese (ja)
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JPS5715506U (en
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Description

【考案の詳細な説明】 本考案はたとえば移動無線通信のように、測定
すべき電界の強さが広範囲に変化する電界の強度
測定用などの受信機に用いられる検波回路の改良
に関する。さらに詳しく言えばこのような受信機
の入力信号強度に応じた中間周波増幅部の出力よ
り適当なレベルの検波用入力を取出し、これを包
絡線検波して得られた検波電圧を利用して電界
(強度)を検出せんとする電界検出器などに使用
される検波回路に関するものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to an improvement in a detection circuit used in a receiver for measuring the strength of an electric field in which the strength of the electric field to be measured changes over a wide range, such as in mobile radio communications. More specifically, the detection input of an appropriate level is extracted from the output of the intermediate frequency amplification section according to the input signal strength of such a receiver, and the detected voltage obtained by envelope detection is used to generate the electric field. This relates to a detection circuit used in electric field detectors that detect (intensity).

従来の電界検出器などでは受信機の中間周波増
幅部からコンデンサ結合等によつて適当レベルの
出力を取出し、半導体ダイオードを用いた倍電圧
整流器や半波整流器によつて包絡線検波を行つて
いる。しかしこの回路では検波器の入力電圧がダ
イオードの順電圧(Vf)(順電圧は検波電流が流
れ始める正電圧で、しきい電圧またはオフセツト
電圧ともいう)以上にならぬ場合には検波出力は
零であつて動作しない。従つて検波電圧範囲は狭
い。また検波器は入力側増幅器の負荷となるの
で、増幅器の利得も検波器の入力インピーダンス
分だけ低下するなどの欠点がある。さらに検波出
力電圧は一般にこれを電圧比較回路(コンパレー
タ)に入力させ、標準電圧(可変とす)と比較し
てレベルを決定するが、上記検波器出力はO
(V)から出力されるので、検波後コンパレータ
に入力させる電圧は相当大きな値とする必要があ
り、検波範囲はますます狭くなることが欠点であ
る。
In conventional electric field detectors, an appropriate level of output is obtained from the receiver's intermediate frequency amplification section through capacitor coupling, etc., and envelope detection is performed using a voltage doubler rectifier or half-wave rectifier using semiconductor diodes. . However, in this circuit, if the input voltage of the detector does not exceed the forward voltage (V f ) of the diode (forward voltage is the positive voltage at which the detection current begins to flow, and is also called the threshold voltage or offset voltage), the detection output will be It is zero and does not work. Therefore, the detection voltage range is narrow. Furthermore, since the wave detector becomes a load on the input side amplifier, there is a drawback that the gain of the amplifier is also reduced by the input impedance of the wave detector. Furthermore, the detected output voltage is generally input to a voltage comparison circuit (comparator) and compared with a standard voltage (variable) to determine the level.
(V), the voltage input to the comparator after detection needs to be a considerably large value, and the disadvantage is that the detection range becomes increasingly narrow.

本考案の回路では検波ダイオードにあらかじめ
適当な正バイアス電圧をかけて順電圧(Vf)を
相殺して検波範囲を広げると同時に、検波器出力
に検波出力とは別に適当な電圧をあらかじめ与え
ておいてコンパレータの動作を容易とすることが
特徴で、以下詳細に説明する。
In the circuit of the present invention, an appropriate positive bias voltage is applied to the detection diode in advance to cancel out the forward voltage (V f ) to widen the detection range, and at the same time, an appropriate voltage is applied to the detector output in advance in addition to the detection output. The feature is that the operation of the comparator is facilitated in this case, and will be explained in detail below.

第1図および第2図は本考案の基礎となる検波
回路図で、第3図は本考案を実施した検波回路の
構成例図である。(たゞしコンパレータ以下は図
示省略してある)。これらの図において1は受信
機または受信部中の中間周波増幅部、2はコレク
タ接地回路を用いた緩衝増幅器(エミツタフオロ
ア)、3,3a,3bは検波器(ダイオード)、4
は平滑回路、5はコンパレータへの出力端子であ
る。検波器の入力であるコレクタ接地回路2には
中間周波増幅部1の適当な出力(一般に最終段ま
たはこれに近い段)が与えられる。コレクタ接地
回路は周知のように入力インピーダンスが大きく
出力インピーダンスは低いが、その出力すなわち
エミツタ接地間の抵抗両端の電圧をダイオード3
を通じて適当な大きさの抵抗RとコンデンサCの
並列回路に与えると、このRとCの両端の電圧が
検波出力になる。検波出力はたとえばコンパレー
タに入力させて基準電圧と比較させて電界レベル
決定を行うように使用されるが、コンパレータに
必要なバイアス電圧はコレクタ接地回路2の固定
バイアス抵抗R1によつて決められる例が第1図
である。また第2図は中間周波増幅部の直流電圧
を利用してバイアス電圧を得る回路である。
FIGS. 1 and 2 are detection circuit diagrams that are the basis of the present invention, and FIG. 3 is a diagram showing an example of the configuration of a detection circuit implementing the present invention. (The components below the comparator are omitted from the diagram). In these figures, 1 is an intermediate frequency amplification section in the receiver or receiving section, 2 is a buffer amplifier (emitter follower) using a collector grounding circuit, 3, 3a, 3b are detectors (diodes), and 4
5 is a smoothing circuit, and 5 is an output terminal to the comparator. An appropriate output (generally the final stage or a stage close to this) of the intermediate frequency amplification section 1 is applied to the collector grounded circuit 2 which is the input of the detector. As is well known, the input impedance of the common collector circuit is large and the output impedance is low.
When the voltage is applied to a parallel circuit of a resistor R and a capacitor C of an appropriate size through a parallel circuit of a resistor R and a capacitor C, the voltage across R and C becomes the detected output. The detection output is used, for example, to determine the electric field level by inputting it into a comparator and comparing it with a reference voltage, but the bias voltage required for the comparator is determined by the fixed bias resistor R 1 of the collector grounding circuit 2. is shown in Figure 1. Further, FIG. 2 shows a circuit that obtains a bias voltage using the DC voltage of an intermediate frequency amplification section.

本考案はこれらの回路を基礎として検波範囲を
さらに拡げたもので、第3図にその具体的な回路
例を示してある。すなわち、たとえば第2図のよ
うな検波回路を2組用いてそのそれぞれの入力は
中間周波増幅部1の異つたレベルの段から一般に
は連続した段から別々に得るようにし、各検波回
路3aと3bの出力の合成には、各々のダイオー
ドD1,D2に直列に高抵抗R1をそれぞれ接続した
ものを共通の負荷である抵抗R2とコンデンサC2
の並列回路に共通に接続する。この並列回路の両
端の電圧が検波出力となりコンパレータに供給さ
れる。なおこれらの回路素子R1,R2,C1,C2
は検波特性に最適な値に選ぶことはいうまでもな
い。
The present invention further expands the detection range based on these circuits, and a specific example of the circuit is shown in FIG. That is, for example, two sets of detection circuits as shown in FIG. To synthesize the output of 3b, a high resistance R 1 is connected in series with each diode D 1 and D 2 , and a common load is a resistance R 2 and a capacitor C 2.
Commonly connected to parallel circuits. The voltage across this parallel circuit becomes the detected output and is supplied to the comparator. It goes without saying that these circuit elements R 1 , R 2 , C 1 , C 2 , etc. are selected to have optimal values for the detection characteristics.

次に本考案回路の効果を従来の回路に比べて説
明する。第4図は検波範囲(検出ダイナミツクレ
ンジという)を広げるために用いられる従来の検
波回路の一例図、第5図は本考案による検波回路
図である。これらの図から第1段について従来方
式の場合の検波(出力)電圧Vpは Vp=R/R+R(Vi1−Vf) ……(1) 本考案方式(第5図)の場合の検波電圧は Vp=R/R+R(V1+Vi1−Vf) ……(2) たゞしVi1,Vi2は中間周波増幅部の各段の出
力電圧、Vfは検波器ダイオードの順電圧、V1
コレクタ接地回路によるダイオードの固定バイア
ス電圧である。
Next, the effects of the circuit of the present invention will be explained in comparison with conventional circuits. FIG. 4 is a diagram of an example of a conventional detection circuit used to widen the detection range (referred to as detection dynamics range), and FIG. 5 is a diagram of a detection circuit according to the present invention. From these figures, the detection (output) voltage V p in the case of the conventional method for the first stage is V p = R 2 /R 1 + R 2 (V i1 - V f )...(1) Invented method (Fig. 5) ), the detected voltage is V p =R 2 /R 1 +R 2 (V 1 +V i1 −V f )...(2) where V i1 and V i2 are the output voltages of each stage of the intermediate frequency amplification section , V f is the forward voltage of the detector diode, and V 1 is the fixed bias voltage of the diode by the common collector circuit.

さて前記のようにR1をR2に比べて遥かに大き
く選定するから検波出力(Vp)側から見た検波
器側は定電流源とみなされるため2段接続した場
合の合成検波出力電圧は各段の出力電圧の和とな
る。従つて第4図の場合は(1)式は Vp=R/R+R{(Vi1−Vf) +(Vi2−Vf)} ……(3) となり、本考案の第5図の場合は(2)式から Vp=R/R+R{(V1+Vi1−Vf) +(V1+Vi2−Vf)} ……(4) と表わされる。(たゞしダイオードD2の固定バイ
アス電圧V2は便宜上V2=V1とした) 第6図は本考案検波回路と従来の検波回路の特
性比較図で、第6図Aは出力を取り出す増幅器の
利得を同一としたときの検波特性でB1は(1)式に
よる、またA1は(2)式による入,出力特性をそれ
ぞれ示している。また第6図Bは2段検波回路の
特性比較図でA1,B1はA図の通りで、A2,B2
A1,B1に前段の検波特性を加えた特性であるか
らB1とB2による合成特性は(3)式を、A1とA2によ
る合成特性は(4)式をそれぞれ図示している。
Now, as mentioned above, since R 1 is selected to be much larger than R 2 , the detector side viewed from the detection output (V p ) side is considered to be a constant current source, so the composite detection output voltage when two stages are connected. is the sum of the output voltages of each stage. Therefore, in the case of Fig. 4, equation (1) becomes V p = R 2 /R 1 + R 2 {(V i1 - V f ) + (V i2 - V f )}...(3), and the present invention's formula In the case of Fig. 5, from equation (2), it is expressed as V p = R 2 /R 1 +R 2 {(V 1 +V i1 −V f ) +(V 1 +V i2 −V f )} ...(4) . (The fixed bias voltage V 2 of the diode D 2 is assumed to be V 2 = V 1 for convenience.) Figure 6 is a characteristic comparison diagram of the inventive detector circuit and the conventional detector circuit, and Figure 6 A shows the output. When the gain of the amplifier is the same, B 1 shows the detection characteristics according to equation (1), and A 1 shows the input and output characteristics according to equation (2). Also, Figure 6B is a characteristic comparison diagram of the two-stage detection circuit, where A 1 and B 1 are as in Figure A, and A 2 and B 2 are as shown in Figure A.
Since the characteristics are obtained by adding the detection characteristics of the previous stage to A 1 and B 1 , the combined characteristics of B 1 and B 2 are shown in equation (3), and the combined characteristics of A 1 and A 2 are shown in equation (4). There is.

次にこれらの特性を用いて検波回路の動作と本
考案回路の効果をさらに具体的に説明する。
Next, the operation of the detection circuit and the effect of the circuit of the present invention will be explained in more detail using these characteristics.

まず本考案による第5図と従来の第4図とを比
較すれば明らかなように本考案においては、 (イ) 中間周波増幅器の出力の一部を取り出して直
接ダイオードにて整流する代りに入力インピー
ダンスが大きく、出力インピーダンスが低いエ
ミツタフオロア(コレクタ接地)回路にて取り
出しているので増幅器への負荷効果が小さく、
増幅器入力の高レベル時のエミツタフオロアの
入力電圧が従来のものより高レベルに達し、増
幅器の低レベル出力から飽和出力に達するまで
検波できる。これに対し第4図のような従来の
ダイオード負荷回路では平滑回路のR,Cが無
視できなくなつて負荷効果によつて最大検波出
力電圧は低くなる。しかし、エミツタフオロア
は出力インピーダンスが低いので平滑回路の
R,Cによる変化はない。
First, if you compare Figure 5 according to the present invention with the conventional Figure 4, it will be clear that in the present invention, (a) instead of extracting a part of the output of the intermediate frequency amplifier and directly rectifying it with a diode, Since the output is taken out using an emitter follower (collector grounded) circuit with high impedance and low output impedance, the load effect on the amplifier is small.
When the input voltage of the emitter follower is at a high level, the input voltage of the emitter follower reaches a higher level than that of the conventional type, and detection is possible from the low level output of the amplifier until it reaches the saturated output. On the other hand, in the conventional diode load circuit as shown in FIG. 4, R and C of the smoothing circuit cannot be ignored, and the maximum detection output voltage becomes low due to the load effect. However, since the output impedance of the emitter follower is low, there is no change due to R and C of the smoothing circuit.

(ロ) 検波用ダイオードD1,D2等に固定バイアス
用直流電流を流すことによつてダイオードの順
電圧以下の交流電圧も検波できるので検波器の
ダイナミツクレンジが広がる。従来の回路では
第6図に示すように入力Vfまでの部分は検波
されないからダイナミツクレンジは狭くなる。
(b) By passing a fixed bias DC current through the detection diodes D1 , D2 , etc., it is possible to detect AC voltages that are lower than the forward voltage of the diodes, thereby expanding the dynamic range of the detector. In the conventional circuit, as shown in FIG. 6, the portion up to the input V f is not detected, so the dynamic range is narrow.

(ハ) エミツタフオロア回路の信号出力に適当なバ
イアス電圧を与えることにより検波器の出力の
信号処理を容易にした。
(c) Signal processing of the detector output is facilitated by applying an appropriate bias voltage to the signal output of the emitter follower circuit.

などの効果がある。続いて回路の動作を説明す
る。
There are effects such as Next, the operation of the circuit will be explained.

まず第2図のような検波器が1段の場合検波器
入力を取出す増幅器の利得を同一として従来のダ
イオード検波回路と本考案回路の検波特性を示す
と前記のように第6図AのB1およびA1特性のよ
うになる。この特性は入力電圧Viと検波出力電
圧Vp間の特性を表わしA1は本考案回路の特性、
B1は従来のダイオード検波回路の特性である。
B1特性は入力電圧が順電圧Vfを越えるまで出力
pはゼロであるのに対してA1特性は前記バイア
ス電圧によりVfを打消し微小入力からその飽和
出力の前まで検波出力を直線的に発生させること
ができる。Vfは0.6V程度であるが電源電圧の低
いICやトランジスタ回路ではこれによつて大き
な影響を持つている。A図中のDRA,DRBは出力
のダイナミツクレンジ、Visは飽和レベルをそれ
ぞれ表している。一般にDRA>DRBである。
First, when the detector has one stage as shown in Fig. 2, the detection characteristics of the conventional diode detection circuit and the circuit of the present invention are shown as B in Fig. 6A, assuming that the gain of the amplifier that takes out the detector input is the same. 1 and A 1 characteristics. This characteristic represents the characteristic between the input voltage V i and the detected output voltage V p , where A 1 is the characteristic of the circuit of the present invention,
B 1 is a characteristic of a conventional diode detection circuit.
In the B 1 characteristic, the output V p is zero until the input voltage exceeds the forward voltage V f , whereas in the A 1 characteristic, the bias voltage cancels V f and the detected output is increased from the minute input to before its saturated output. It can be generated linearly. Although V f is about 0.6V, it has a large effect on ICs and transistor circuits with low power supply voltages. In figure A, DR A and DR B represent the output dynamic range, and V is the saturation level, respectively. In general, DR A > DR B.

次に第4図,第5図のように多段(ここでは2
段)にした検波回路について説明する。第5図の
回路では各段検波器の出力は前記のようにインピ
ーダンスが小さくかつダイオードD1,D2に直列
に接続した抵抗R1(R1≫R2)によつて電流源とし
て動作される。従つてその共通負荷R2に流れる
電流は各段よりの出力電圧に応じた検波電流の和
となり検波出力5は各段の検波電圧を加え合わせ
たものとなる。従つて検波出力が最初に飽和電圧
に達するのは最終段検波器であつてその特性は第
6図AのA1のようになる。またその前段増幅器
による検波出力は最終段がその飽和電圧Visに到
達する前から僅かに発生し始めているが、前段が
入力電圧に比例した検波電圧を発生しているとき
後段の検波器は一定の電圧しか出力できない。従
つて2段検波器の合成特性は第6図BのA1,A2
の合成直線となる。なお第6図BのB1,B2は従
来のダイオードのみの場合(第4図)の後段とこ
れに前段のを加えた検波特性であるが合成特性は
各段検波回路の出力の和になると仮定した場合で
ある。
Next, as shown in Figures 4 and 5, there are multiple stages (here, 2 stages).
The following describes the detection circuit in the following stage. In the circuit shown in Figure 5, the output of each stage detector is operated as a current source by the resistor R 1 (R 1 ≫ R 2 ), which has low impedance and is connected in series with the diodes D 1 and D 2 as described above. Ru. Therefore, the current flowing through the common load R2 is the sum of the detected currents corresponding to the output voltages from each stage, and the detected output 5 is the sum of the detected voltages from each stage. Therefore, the detection output reaches the saturation voltage first in the final stage detector, and its characteristics are as shown in A1 in FIG. 6A. In addition, the detection output from the pre-stage amplifier begins to generate slightly before the final stage reaches its saturation voltage V is , but while the pre-stage is generating a detected voltage proportional to the input voltage, the output from the post-stage detector remains constant. It can only output voltage of . Therefore, the composite characteristics of the two-stage detector are A 1 and A 2 in Figure 6B.
becomes the composite straight line. Note that B 1 and B 2 in Fig. 6B are the detection characteristics obtained by adding the latter stage and the previous stage in the case of conventional diodes only (Fig. 4), but the composite characteristic is the sum of the outputs of each stage detection circuit. This is the case assuming that.

合成検波特性A1とA2あるいはB1とB2を連続し
た直線とするには各段の増幅器の利得あるいは検
波入力電圧を実測によつて多少の調整をすること
が必要である。このとき従来の回路では本考案の
回路と比べて第6図Bの特性から明らかなように
利得を下げて合成する操作が必要で、検波入力電
圧のダイナミツクレンジDRB2は本考案回路より
さらに狭くなる。第6図Bのように合成特性に多
少の不連続点があることを許したとしてもB1
B2の検波器出力は少なくとも1段当たり順電圧
fに相当するV01だけ小さくなり、入力ダイナ
ミツクレンジは2段合成では2Vfだけ狭くなつて
いる。この例のように多段合成検波回路では出力
ダイナミツクレンジは段数が多くしかも合成検波
出力が増大する限り従来のダイオード検波回路に
比べてかなり大きくすることができる。
In order to make the composite detection characteristics A 1 and A 2 or B 1 and B 2 a continuous straight line, it is necessary to make some adjustments to the gain of the amplifier in each stage or the detection input voltage by actual measurement. At this time, in the conventional circuit, compared to the circuit of the present invention, it is necessary to lower the gain and perform synthesis, as is clear from the characteristics shown in Figure 6B, and the dynamic range DR B2 of the detection input voltage is even greater than that of the circuit of the present invention. It gets narrower. Even if we allow some discontinuities in the composite characteristics as shown in Figure 6B, B 1 and
The detector output of B 2 is reduced by at least V 01 corresponding to the forward voltage V f per stage, and the input dynamic range is narrowed by 2 V f in the two-stage combination. In a multi-stage composite detection circuit as in this example, the output dynamic range can be made considerably larger than that of a conventional diode detection circuit as long as the number of stages is large and the composite detection output increases.

以上のように本考案の検波回路は検波範囲が広
いという著しい特長が得られるが、そのほかにコ
レクタ接地のため入力インピーダンスが高く、中
間周波増幅器の負荷インピーダンスにほとんど影
響を与えないこと、コンパレータ入力のバイアス
を別に設けなくてもよいこと等の利点があり、電
界検出器等に実用して優れた効果が得られてい
る。
As mentioned above, the detection circuit of the present invention has the remarkable feature of wide detection range, but in addition, the input impedance is high because the collector is grounded, so it has almost no effect on the load impedance of the intermediate frequency amplifier, and the comparator input It has advantages such as not requiring a separate bias, and has been used in electric field detectors and the like with excellent effects.

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

第1図および第2図は本考案の基礎となる回路
図、第3図および第5図は本考案による検波回路
の構成例図、第4図は検波範囲を拡げるための従
来の検波回路構成図、第6図は本考案検波回路と
従来の回路の特性比較図で、A図は1段当たりの
特性比較図、B図は2段検波回路の特性比較図で
ある。 1……中間周波増幅部、2……コレクタ接地回
路、3,3a,3b……検波ダイオード、4……
平滑回路、5……コンパレータへの出力端子。
Figures 1 and 2 are circuit diagrams that are the basis of the present invention, Figures 3 and 5 are configuration examples of a detection circuit according to the present invention, and Figure 4 is a conventional detection circuit configuration for expanding the detection range. 6 are characteristic comparison diagrams of the detection circuit of the present invention and a conventional circuit. Figure A is a comparison diagram of characteristics per stage, and Figure B is a comparison diagram of characteristics of a two-stage detection circuit. 1... Intermediate frequency amplification section, 2... Collector grounding circuit, 3, 3a, 3b... Detection diode, 4...
Smoothing circuit, 5... Output terminal to comparator.

Claims (1)

【実用新案登録請求の範囲】[Scope of utility model registration request] 受信機中間周波増幅部の出力レベルの異なる連
続複数段毎の出力の一部をそれぞれ取り出してベ
ース側入力とすると共にそのエミツタと接地間に
検波用ダイオードの順電圧をゼロとするバイアス
電圧を発生するバイアス用抵抗を接続した前記各
段毎のコレクタ接地トランジスタ(エミツタフオ
ロア)と、一端接地の抵抗R2とコンデンサC2
並列回路よりなる複数段共通の負荷と、前記各段
毎のコレクタ接地トランジスタのエミツタ接地間
抵抗と前記共通負荷との間に接続した検波ダイオ
ードと前記負荷抵抗R2より数倍以上大なる抵抗
R1の直列回路とより成り、前記各段の検波ダイ
オードの出力が前記共通負荷に加算合成されるよ
うに構成したことを特徴とする検波回路。
A portion of the output from each successive stage with different output levels of the receiver intermediate frequency amplification section is taken out and used as the base side input, and a bias voltage is generated between the emitter and ground to zero the forward voltage of the detection diode. A common load for multiple stages consisting of a parallel circuit of a resistor R 2 and a capacitor C 2 with one end grounded, and a common collector transistor for each stage (emitter follower) to which a bias resistor is connected. A detection diode connected between the emitter-to-ground resistance and the common load, and a resistance several times larger than the load resistance R2 .
1. A detection circuit comprising a series circuit of R1 , the detection circuit being configured such that the outputs of the detection diodes in each stage are added and combined to the common load.
JP9206380U 1980-07-02 1980-07-02 Expired JPS6224969Y2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP9206380U JPS6224969Y2 (en) 1980-07-02 1980-07-02

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP9206380U JPS6224969Y2 (en) 1980-07-02 1980-07-02

Publications (2)

Publication Number Publication Date
JPS5715506U JPS5715506U (en) 1982-01-26
JPS6224969Y2 true JPS6224969Y2 (en) 1987-06-26

Family

ID=29454023

Family Applications (1)

Application Number Title Priority Date Filing Date
JP9206380U Expired JPS6224969Y2 (en) 1980-07-02 1980-07-02

Country Status (1)

Country Link
JP (1) JPS6224969Y2 (en)

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP4821618B2 (en) * 2007-01-15 2011-11-24 パナソニック株式会社 Output power detector for high frequency power amplifier
JP2020114007A (en) * 2020-03-25 2020-07-27 新日本無線株式会社 Low noise amplification device

Also Published As

Publication number Publication date
JPS5715506U (en) 1982-01-26

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