JPH0441525B2 - - Google Patents

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Publication number
JPH0441525B2
JPH0441525B2 JP4440284A JP4440284A JPH0441525B2 JP H0441525 B2 JPH0441525 B2 JP H0441525B2 JP 4440284 A JP4440284 A JP 4440284A JP 4440284 A JP4440284 A JP 4440284A JP H0441525 B2 JPH0441525 B2 JP H0441525B2
Authority
JP
Japan
Prior art keywords
agc
voltage
signal
stage
amplifier
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
JP4440284A
Other languages
Japanese (ja)
Other versions
JPS60189305A (en
Inventor
Katsuharu Kimura
Takashi Matsura
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.)
NEC Corp
Original Assignee
Nippon Electric 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 Nippon Electric Co Ltd filed Critical Nippon Electric Co Ltd
Priority to JP4440284A priority Critical patent/JPS60189305A/en
Publication of JPS60189305A publication Critical patent/JPS60189305A/en
Publication of JPH0441525B2 publication Critical patent/JPH0441525B2/ja
Granted legal-status Critical Current

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  • Control Of Amplification And Gain Control (AREA)
  • Circuits Of Receivers In General (AREA)

Description

【発明の詳細な説明】 (技術分野) 本発明は、移動無線機等における受信機の中間
周波増幅回路に関し、特に受信機の受信電界強度
の検出機能を備えた中間周波増幅回路に関する。
Detailed Description of the Invention (Technical Field) The present invention relates to an intermediate frequency amplification circuit of a receiver in a mobile radio device, etc., and more particularly to an intermediate frequency amplification circuit having a function of detecting the received electric field strength of the receiver.

(従来技術) 第1図は、受信電界強度の検出機能を備えた従
来の中間周波増幅回路の回路図である。この中間
周波増幅回路は縦続接続した3段の増幅器を備え
る。第1段増幅器はトランジスタQ1〜Q10からな
り、第2段増幅器はトランジスタQ11〜Q19から
なり、第3段増幅器はトランジスタQ20〜Q27
らなつている。入力IF信号の強度、即ち受信電
界強度は、これら各段の出力をコンデンサC8
C9,C10介して整流し、夫々の段の整流電圧を加
算して検出し、端子5から出力していた。しか
し、この従来の回路では、電圧加算して検出電界
強度のダイナミツクレンジを拡大するには、高い
電源電圧が必要である。また、電圧加算型なので
各段の整流電圧をトランジスタQ39,Q40,Q41
Q42で加算しているが、この加算した部分の線形
性が悪くなり、第2図に示すように電界検出電圧
に凸凹が出ることがしばしば見られる。また信号
の整流はダイオードQ28,Q29,Q30;Q32,Q33
Q34;Q35,Q36,Q37を使つて行つているので特
に温度特性が悪くなり、温度特性を補償するには
回路が複雑になるという欠点がある。また、整流
器には各々に3つのコンデンサC8,C9,C10が必
要となる。これらのコンデンサは、中間周波数を
下げると所要の容量が大きくなる。従つて、これ
らのコンデンサC8,C9,C10がIC化されるのは、
中間周波数が10.7MHz以上である場合が一般的で
ある。中間周波数を下げるとコンデンサのIC内
蔵は難しくなり、各段毎に外付コンデンサ用の端
子が必要になり、IC化は不利であつた。また中
間周波数を10MHz以上に高くすれば、当然各段の
増幅器に電流を流さないと増幅度が取れないか
ら、消費電流が大きくなる。
(Prior Art) FIG. 1 is a circuit diagram of a conventional intermediate frequency amplification circuit equipped with a reception field strength detection function. This intermediate frequency amplification circuit includes three stages of cascaded amplifiers. The first stage amplifier consists of transistors Q1 to Q10 , the second stage amplifier consists of transistors Q11 to Q19 , and the third stage amplifier consists of transistors Q20 to Q27 . The strength of the input IF signal, that is, the received electric field strength, is determined by connecting the outputs of these stages to capacitors C 8 ,
It rectified through C 9 and C 10 , added the rectified voltages of each stage, detected it, and outputted it from terminal 5. However, in this conventional circuit, a high power supply voltage is required to expand the dynamic range of the detected electric field strength by adding voltages. In addition, since it is a voltage addition type, the rectified voltage of each stage is connected to transistors Q 39 , Q 40 , Q 41 ,
Although addition is performed using Q42 , the linearity of this added portion deteriorates, and as shown in FIG. 2, it is often seen that unevenness appears in the electric field detection voltage. In addition, signal rectification is performed using diodes Q 28 , Q 29 , Q 30 ; Q 32 , Q 33 ,
Since this is done using Q 34 , Q 35 , Q 36 , and Q 37 , the temperature characteristics are particularly poor, and the disadvantage is that the circuit becomes complicated to compensate for the temperature characteristics. Also, each rectifier requires three capacitors C 8 , C 9 , and C 10 . The required capacitance of these capacitors increases as the intermediate frequency is lowered. Therefore, these capacitors C 8 , C 9 , and C 10 are integrated into ICs because
Generally, the intermediate frequency is 10.7MHz or higher. Lowering the intermediate frequency made it difficult to incorporate a capacitor into an IC, and each stage required a terminal for an external capacitor, making it disadvantageous to use an IC. Furthermore, if the intermediate frequency is increased to 10 MHz or higher, current consumption will increase because the degree of amplification cannot be achieved unless current is passed through the amplifiers in each stage.

(発明の目的) 本発明の目的は、電界検出電圧の直線性、温度
特性に優れ、低電源電圧で動作し、IC化したと
きに所要の外付け部分の少い、入力電界検出機能
を有する中間周波数増幅回路の提供にある。
(Objective of the Invention) The object of the present invention is to have an input electric field detection function that has excellent linearity and temperature characteristics of the electric field detection voltage, operates at a low power supply voltage, and requires few external parts when integrated into an IC. The present invention provides an intermediate frequency amplification circuit.

(発明の構成) 本発明の構成は、縦続接続されそれぞれ中間周
波信号を入力信号とし出力信号の強度が前記入力
信号の強度と第一の直流電圧信号であるAGC電
圧との積にほぼ比例するn段(n>1)のAGC
増幅器と、第n段目の前記AGC増幅器の前記出
力信号を整流し前記出力信号の強度に比例する第
二の直流電圧信号を出力する整流回路と、前記第
二の直流電圧信号を入力し第一段目の前記AGC
増幅器の前記入力信号の強度のn乗根に逆比例す
る前記第一の直流電圧信号を生成するAGC電圧
制御回路とを備えて構成される。
(Structure of the Invention) The structure of the present invention is such that the cascade-connected intermediate frequency signals are respectively input signals, and the intensity of the output signal is approximately proportional to the product of the intensity of the input signal and the AGC voltage that is the first DC voltage signal. AGC with n stages (n>1)
an amplifier, a rectifier circuit that rectifies the output signal of the n-th stage AGC amplifier and outputs a second DC voltage signal proportional to the intensity of the output signal; The AGC in the first stage
and an AGC voltage control circuit that generates the first DC voltage signal that is inversely proportional to the nth root of the intensity of the input signal of the amplifier.

(実施例) 次に実施例を挙げ本発明を詳細に説明する。(Example) Next, the present invention will be explained in detail with reference to Examples.

第3図は本発明の一実施例の回路図である。こ
の実施例は縦続に接続されたn段のAGC増幅器
A1〜Aoと、整流器6と、AGC制御回路7と、整
流用コンデンサCrecと、IF信号の入力端子1及
び1′と、AGC電圧VAGCの出力端子2及び2′と
増幅されたIF信号の出力端子3及び3′とからな
る。
FIG. 3 is a circuit diagram of one embodiment of the present invention. This example uses n-stage AGC amplifiers connected in cascade.
A 1 to A o , rectifier 6, AGC control circuit 7, rectifying capacitor Crec, IF signal input terminals 1 and 1', AGC voltage V AGC output terminals 2 and 2', and amplified IF It consists of signal output terminals 3 and 3'.

第1段増幅器A1は、電流源I1と、トランジスタ
Q11及びQ11′並びに抵抗素子REIを有する第1の差
動増幅器と、トランジスタQ12及びQ12′を有する
第2の差動増幅器と、トランジスタQ13及び
Q13′を有する第3の差動増幅器と、抵抗素子RC1
とからなる。第2段から第n段に到る各増幅器
A2〜Aoにも同様の回路である。
The first stage amplifier A 1 consists of a current source I 1 and a transistor
A first differential amplifier having transistors Q 11 and Q 11 ′ and a resistive element R EI , a second differential amplifier having transistors Q 12 and Q 12 ′, and a transistor Q 13 and
a third differential amplifier with Q 13 ′ and a resistive element R C1
It consists of. Each amplifier from the second stage to the nth stage
A similar circuit is used for A 2 to A o .

出力IF信号の電圧V0(出力電圧)は、整流器6
と整流用コンデンサCrecにより整流され、AGC
制御回路7は、差動回路を組合わせた周知のギル
バート掛算器等を用いて構成され、各増幅器A1
〜AoにAGC電圧VAGCを負帰還し、出力電圧V0
一定になるように制御する。AGC制御回路7は、
出力のAGC電圧 VAGCが VAGC≦2VT+REiIi ……(1) となるように設定してある。但し、VTは次式で
与えられる。
The voltage V 0 (output voltage) of the output IF signal is
is rectified by the rectifying capacitor Crec, and the AGC
The control circuit 7 is configured using a well-known Gilbert multiplier or the like combined with a differential circuit, and each amplifier A 1
AGC voltage V AGC is negatively fed back to Ao , and the output voltage V0 is controlled to be constant. The AGC control circuit 7 is
The output AGC voltage V AGC is set so that V AGC ≦2V T + R Ei I i ...(1). However, V T is given by the following formula.

VT=kT/g ……(2) ここで、kはボルツマン定数、Tは絶対温度、
gは電子の単位電荷である。
V T =kT/g...(2) Here, k is Boltzmann's constant, T is absolute temperature,
g is the unit charge of an electron.

入力信号の電圧(入力電圧)VINが VIN≦2VT ……(3) のときは、第1段増幅器A1の出力電圧V01は近似
的に V01=RC1/2VT・I1/2VT+RE1I1 ・VAGC・VIN ……(4) となる。また、第2段増幅器A2はこの電圧V01
入力とするから、出力電圧V02は V02=RC2/2VT・I2/2VT+RE2I2 ・VAGC・V01 ……(5) となる。以下の増幅器A3〜Aoも同様に作動し、
第i段増幅器の出力電圧V0iは、 V0i=Ki・VAGC・V0(i-1) ……(6) である(Kiは定数)。従つて、第i段増幅器にお
いては、出力電圧(出力信号の強度)V0iに対す
る前段〔(i−1)段〕増幅器の出力電圧V0(i-1)
とAGC電圧VAGCとの積の比は一定値Kiである
(但し、第1段増幅器A1においては、V00=VIN
ある)。
When the input signal voltage (input voltage) V IN is V IN ≦2V T ...(3), the output voltage V 01 of the first stage amplifier A 1 is approximately V 01 = R C1 /2V T・I 1 /2V T +R E1 I 1・V AGC・V IN ……(4). Also, since the second stage amplifier A 2 receives this voltage V 01 as input, the output voltage V 02 is V 02 = R C2 /2V T・I 2 /2V T +R E2 I 2・V AGC・V 01 …… (5) becomes. The amplifiers A 3 to A o below operate similarly,
The output voltage V 0i of the i-th stage amplifier is V 0i =K i ·V AGC ·V 0(i-1) (6) (K i is a constant). Therefore, in the i-th stage amplifier, the output voltage V 0 (i-1) of the previous stage [(i-1) stage] amplifier with respect to the output voltage (output signal strength) V 0i
The ratio of the product of the AGC voltage V AGC and the AGC voltage V AGC is a constant value K i (however, in the first stage amplifier A 1 , V 00 =V IN ).

前述の如くに各増幅器が作動するから、入力電
圧VINに対する出力電圧V0の関係は次の(7)式で与
えられる。但し、出力端子3,3′間に接続され
る負荷の抵抗成分をRLとする。
Since each amplifier operates as described above, the relationship between the output voltage V 0 and the input voltage V IN is given by the following equation (7). However, let R L be the resistance component of the load connected between the output terminals 3 and 3'.

V0=RC1/2VT・I1/2VT+REII1 ・VAGC×……×RLRCo/2VT(RCo+RL) ・Io/2VT+REoIo・VAGC・VIN= RCI×……×RCo/(2VTn・RL/(RCo+RL)・ I1×……×Io/(2VT+RE1I1)×……×(2VT+REo
Io) ・(VAGCn・VIN ……(7) この(7)式からVAGCを求めると となる。
V 0 = R C1 /2V T・I 1 /2V T +R EI I 1・V AGC ×……×R L R Co /2V T (R Co +R L ) ・I o /2V T +R Eo I o・V AGC・V IN = R CI ×……×R Co / (2V T ) n・R L / (R Co + R L )・I 1 ×……×I o / (2V T + R E1 I 1 ) ×…… ×(2V T +R Eo
I o ) ・(V AGC ) n・V IN ……(7) Calculating V AGC from this equation (7), becomes.

このように、AGC電圧VAGCは、入力電圧がVIN
のときに1/nINに比例した値であり、VIN
圧縮して表現している。従つて、入力電圧VIN
ダイナミツクレンジに対してVAGCのダイナミツ
クレンジはdB値で1/nに圧縮されることがわ
かる。今、入力電圧VINのダイナミツクレンジと
dB値での圧縮比1/nとの積が20dB程度になれ
ばVAGCのダイナミツクレンジは高々1桁しか変
化しない。従つてその場合にはほぼ擬似対数圧縮
特性が得られると考えて良い。今、この実施例の
入力電圧VINのダイナミツクレンジを60dBとする
と、VAGCのダイナミツクレンジは、n=3とす
れば20dBとなり1桁しか変化しない。
In this way, the AGC voltage V AGC is the input voltage V IN
It is a value proportional to 1/ nIN when , and is expressed by compressing V IN . Therefore, it can be seen that the dynamic range of V AGC is compressed to 1/n in dB value with respect to the dynamic range of input voltage V IN . Now, the dynamic range of input voltage V IN and
If the product of the dB value and the compression ratio 1/n is about 20 dB, the dynamic range of V AGC will change by at most one order of magnitude. Therefore, in that case, it can be considered that almost pseudo-logarithmic compression characteristics can be obtained. Now, if the dynamic range of the input voltage V IN in this embodiment is 60 dB, then the dynamic range of V AGC will be 20 dB if n=3, which will change by only one order of magnitude.

第4図は第3図実施例の入力電圧VINとAGC電
圧VAGCOとの関係を示す図である。本図では、VIN
=0dBのときVAGCVAGCOとして、VINが0dBから
60dBまで変化したときのVAGC/VAGCOを、増幅器
の段数nをパラメータとして、示してある。本図
からわかる様に、入力電圧VIVはAGC電圧VAGC
より検出出来、しかも入力電圧VINとAGC電圧
VAGCとはほぼ擬似対数特性の関係で得られる。
FIG. 4 is a diagram showing the relationship between the input voltage V IN and the AGC voltage V AGCO in the embodiment shown in FIG. In this diagram, V IN
= 0dB, V AGC V AGCO , V IN from 0dB
V AGC /V AGCO when it changes up to 60 dB is shown using the number of amplifier stages n as a parameter. As can be seen from this figure, input voltage V IV can be detected by AGC voltage V AGC , and input voltage V IN and AGC voltage
V AGC is obtained from a relationship with almost pseudo-logarithmic characteristics.

(発明の効果) 以上に詳しく述べたように、本発明の中間周波
増幅回路は、多段のAGC増幅器から成るAGC回
路で構成し、AGC回路最終段出力電圧V0が一定
となるときのAGC電圧VAGCにより中間周波増幅
回路の入力電界レベルVINを検出する方式であ
る。この中間周波増幅回路では、整流器が1つだ
けで足りるから、整流器用のコンデンサも1個で
済む。中間周波数が低くてコンデンサが内蔵でき
ない場合でも、外付コンデンサ用の端子を1本追
加するのみで対処出来る。従つて、コンデンサを
1個だけ外付けすれば、中間周波数を下げること
により各段のAGC増幅器に流す電流値を小さく
しても必要な利得が得られるから、低消費電流化
が可能となる。また、整流電圧の加算等を行つて
いないので、電界検出電圧もほぼ対数圧縮されて
単調な曲線となる。また、電界検出電圧の温度特
性も単調であるから温度補償も容易に行なえる。
また、本方式によれば低電圧化も図れ、2V程度
の低い電源電圧でも回路が実現出来て、利点が多
い。
(Effects of the Invention) As described in detail above, the intermediate frequency amplifier circuit of the present invention is configured with an AGC circuit consisting of multi-stage AGC amplifiers, and the AGC voltage when the final stage output voltage V 0 of the AGC circuit is constant. This method uses V AGC to detect the input electric field level V IN of the intermediate frequency amplifier circuit. This intermediate frequency amplification circuit requires only one rectifier, and therefore only one rectifier capacitor. Even if the intermediate frequency is too low to incorporate a built-in capacitor, it can be handled by simply adding one terminal for an external capacitor. Therefore, by attaching only one external capacitor, the necessary gain can be obtained even if the value of current flowing through the AGC amplifiers in each stage is reduced by lowering the intermediate frequency, thereby making it possible to reduce current consumption. Further, since addition of rectified voltages is not performed, the electric field detection voltage is also almost logarithmically compressed and becomes a monotonous curve. Further, since the temperature characteristic of the electric field detection voltage is also monotonic, temperature compensation can be easily performed.
Additionally, this method has many advantages, as it allows for lower voltages, and the circuit can be realized with a power supply voltage as low as 2V.

以上、要するに、本発明によれば、電界検出電
圧の直線性、温度特性に優れ、低電源電圧で動作
し、IC化したときの所要の外付け部品数の少い、
入力電界検出機能を有する中間周波増幅回路が提
供できる。
In summary, according to the present invention, the linearity of the electric field detection voltage and temperature characteristics are excellent, the operation is performed at a low power supply voltage, and the number of external components required when integrated into an IC is small.
An intermediate frequency amplification circuit having an input electric field detection function can be provided.

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

第1図は従来の中間周波増幅回路の回路図、第
2図はこの従来回路の特性図、第3図は本発明の
一実施例の回路図、第4図はこの実施例の特性図
である。 1,1′……中間周波信号入力端子、2,2′…
…AGC電圧出力端子、3,3′……増幅された中
間周波信号の出力端子、5……電界強度検出電圧
出力端子、6……整流器、7……AGC制御回路、
A1〜Ao……AGC増幅器、I1〜Io……定電流源。
Figure 1 is a circuit diagram of a conventional intermediate frequency amplification circuit, Figure 2 is a characteristic diagram of this conventional circuit, Figure 3 is a circuit diagram of an embodiment of the present invention, and Figure 4 is a characteristic diagram of this embodiment. be. 1, 1'...Intermediate frequency signal input terminal, 2, 2'...
...AGC voltage output terminal, 3, 3'... Output terminal of amplified intermediate frequency signal, 5... Field strength detection voltage output terminal, 6... Rectifier, 7... AGC control circuit,
A1 ~ Ao ...AGC amplifier, I1 ~ Io ...constant current source.

Claims (1)

【特許請求の範囲】 1 縦続接続されそれぞれ中間周波信号を入力信
号とし出力信号の強度が前記入力信号の強度と第
一の直流電圧信号であるAGC電圧との積にほぼ
比例するn段(n>1)のAGC増幅器と、 第n段目の前記AGC増幅器の前記出力信号を
整流し前記出力信号の強度に比例する第二の直流
電圧信号を出力する整流回路と、 前記第二の直流電圧信号を入力し第一段目の前
記AGC増幅器の前記入力信号の強度のn乗根に
逆比例する前記第一の直流電圧信号を生成する
AGC電圧制御回路とを備えることを特徴とする
中間周波増幅回路。
[Claims] 1. n stages (n >1); a rectifier circuit that rectifies the output signal of the n-th stage AGC amplifier and outputs a second DC voltage signal proportional to the intensity of the output signal; and the second DC voltage. input the signal and generate the first DC voltage signal that is inversely proportional to the nth root of the intensity of the input signal of the first stage AGC amplifier.
An intermediate frequency amplification circuit comprising an AGC voltage control circuit.
JP4440284A 1984-03-08 1984-03-08 Intermediate frequency amplifier circuit Granted JPS60189305A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP4440284A JPS60189305A (en) 1984-03-08 1984-03-08 Intermediate frequency amplifier circuit

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP4440284A JPS60189305A (en) 1984-03-08 1984-03-08 Intermediate frequency amplifier circuit

Publications (2)

Publication Number Publication Date
JPS60189305A JPS60189305A (en) 1985-09-26
JPH0441525B2 true JPH0441525B2 (en) 1992-07-08

Family

ID=12690513

Family Applications (1)

Application Number Title Priority Date Filing Date
JP4440284A Granted JPS60189305A (en) 1984-03-08 1984-03-08 Intermediate frequency amplifier circuit

Country Status (1)

Country Link
JP (1) JPS60189305A (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP4753171B2 (en) * 2004-03-05 2011-08-24 株式会社パックプラス Spout and packaging

Also Published As

Publication number Publication date
JPS60189305A (en) 1985-09-26

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