JPH0247765B2 - - Google Patents
Info
- Publication number
- JPH0247765B2 JPH0247765B2 JP55022755A JP2275580A JPH0247765B2 JP H0247765 B2 JPH0247765 B2 JP H0247765B2 JP 55022755 A JP55022755 A JP 55022755A JP 2275580 A JP2275580 A JP 2275580A JP H0247765 B2 JPH0247765 B2 JP H0247765B2
- Authority
- JP
- Japan
- Prior art keywords
- circuit
- voltage
- current
- current supply
- supply circuit
- 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
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Classifications
-
- H—ELECTRICITY
- H04—ELECTRIC COMMUNICATION TECHNIQUE
- H04M—TELEPHONIC COMMUNICATION
- H04M19/00—Current supply arrangements for telephone systems
- H04M19/001—Current supply source at the exchanger providing current to substations
- H04M19/008—Using DC/DC converters
Landscapes
- Engineering & Computer Science (AREA)
- Signal Processing (AREA)
- Devices For Supply Of Signal Current (AREA)
- Cable Transmission Systems, Equalization Of Radio And Reduction Of Echo (AREA)
- Control Of Voltage And Current In General (AREA)
- Continuous-Control Power Sources That Use Transistors (AREA)
Description
【発明の詳細な説明】
本発明は電流供給回路、特に電話機加入者線路
への通話電流供給回路に関するものである。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a current supply circuit, and more particularly to a communication current supply circuit for a telephone subscriber line.
従来、電話交換機のライン回路から電話機への
直流通話電流の供給回路は、第1図に示す如く、
直流電圧Eと内部抵抗Rとからなり、トランスT
の1次側巻線W1,W1′を介して電話機TELに矢
印方向に電流ILを供給している。図において、RL
は加入者線路の等価抵抗、Cは内部抵抗Rを交流
的に短絡するためのコンデンサ、W2,W2′は上
記トランスの2次側巻線を示す。 Conventionally, the circuit for supplying DC talking current from the line circuit of a telephone exchange to a telephone set was as shown in Fig. 1.
It consists of a DC voltage E and an internal resistance R, and the transformer T
A current I L is supplied to the telephone TEL in the direction of the arrow through the primary windings W 1 and W 1 '. In the figure, R L
is the equivalent resistance of the subscriber line, C is a capacitor for AC short-circuiting the internal resistance R, and W 2 and W 2 ' are the secondary windings of the transformer.
上記電流供給回路の内部抵抗Rは、線路の抵抗
RLが小さいときに通話電流が過大になるのを抑
制するためのものであり、システム仕様により決
まる固定値をもつ。ここで、トランスの1次側巻
線W1,W1′と電話機TELの直流抵抗を無視する
と、第1図回路は直流的に第2図の回路と等価に
なる。 The internal resistance R of the above current supply circuit is the line resistance
This is to prevent the communication current from becoming excessive when R L is small, and has a fixed value determined by the system specifications. Here, if the DC resistance of the primary windings W 1 and W 1 ' of the transformer and the telephone TEL are ignored, the circuit of FIG. 1 becomes equivalent to the circuit of FIG. 2 in terms of DC.
第2図に示す回路図から、直流通話電流ILの大
きさは次式(1)で表わされ、ILとRLとの関係は第3
図の実線のようになる。 From the circuit diagram shown in Figure 2, the magnitude of the DC talking current I L is expressed by the following equation (1), and the relationship between I L and R L is expressed as
It will look like the solid line in the figure.
IL=E/R+RL …(1)
既存のシステムではR=440Ω、E=−48Vで
あるから、線路抵抗RLを零とすればIL=0.11Aと
なり、内部抵抗Rによる消費電力は約5.3Wにな
る。 I L = E/R + R L ...(1) In the existing system, R = 440Ω and E = -48V, so if the line resistance R L is set to zero, I L = 0.11 A, and the power consumption due to the internal resistance R is It becomes about 5.3W.
つまり、上記従来の直流電流供給回路では、内
部抵抗Rで無効に電力が消費され、この電力消費
は線路抵抗RLが小さければ数ワツトになるため、
それによる発熱が交換機の小型化を困難にしてい
る。 In other words, in the conventional DC current supply circuit described above, power is wasted in the internal resistance R, and this power consumption becomes several watts if the line resistance R L is small.
The heat generated by this makes it difficult to downsize the exchange.
上記問題の解決策としては、電源Eと抵抗Rか
らなる通話電流供給回路を例えば定電流回路に置
き換え、第3図に破線で示す如く直流電流ILが線
路抵抗RLに関係なく一定に流れるようにする案
が考えられる。しかしながら、この案は次の理由
から現行の電話システムには適用できない。 As a solution to the above problem, the communication current supply circuit consisting of the power source E and the resistor R is replaced with, for example, a constant current circuit, and the DC current I L flows constantly regardless of the line resistance R L as shown by the broken line in Fig. 3. There is a plan to do so. However, this proposal cannot be applied to current telephone systems for the following reasons.
すなわち、電話機には音声の通話レベルを均一
化するための通話ロス補償回路が取り付けてあ
り、この回路は抵抗(R+RL)の大小に応じて、
RLが小さいときは音声信号に対するアツテネー
タを挿入し、RLが大きいときはアツテネータを
除去する如く動作する。この場合、線路抵抗の大
小は線路に流れる直流通話電流ILの大きさによつ
て判断できるようになつているため、上述の如く
ILを定電流化してしまうと抵抗の大小を判定でき
ず、通話ロス補償機能を発揮できないという問題
がでてくる。 In other words, the telephone is equipped with a call loss compensation circuit to equalize the voice call level, and this circuit operates according to the size of the resistance (R + R L ).
When R L is small, an attenuator for the audio signal is inserted, and when R L is large, the attenuator is removed. In this case, the magnitude of the line resistance can be determined by the magnitude of the DC talking current I L flowing through the line, so as mentioned above,
If I L is set to a constant current, the magnitude of the resistance cannot be determined, and the problem arises that the call loss compensation function cannot be achieved.
本発明は上記事由に対処すべくなされたもので
あり、現状の電話システムに適合でき、しかも発
熱の問題を解決して交換機を小型できる新規な通
話電流供給回路の提供を目的とするものである。 The present invention has been made to address the above-mentioned reasons, and aims to provide a novel call current supply circuit that is compatible with the current telephone system, solves the problem of heat generation, and allows the switching equipment to be made smaller. .
本発明による通話電流供給回路は、所定の直流
電圧Eを発生する電圧源と、上記電圧源に接続さ
れ上記直流電圧Eをデユーテイーに応じた電圧
E0に変換して加入者線路に印加する第1回路と、
上記加入者線路に流れる直流通話電流ILを検出
し、E−E0が通話電流ILに比例するように上記第
1回路のデユーテイを制御する第2回路とからな
ることを特徴とする。 The communication current supply circuit according to the present invention includes a voltage source that generates a predetermined DC voltage E, and a voltage source that is connected to the voltage source and converts the DC voltage E into a voltage according to a duty.
a first circuit that converts E into 0 and applies it to the subscriber line;
It is characterized by comprising a second circuit that detects the DC talk current IL flowing through the subscriber line and controls the duty of the first circuit so that E-E 0 is proportional to the talk current IL .
すなわち
第(1)式から
RL・IL(=E0)=E−R・IL …(2)
すなわち、E−E0=R・ILであるから(E−
E0)をILに比例するように制御すれば、第1図の
従来回路と同様に加入者線路抵抗RLに依存した
値をもつ直流通話電流ILを供給でき、(E−E0)
を消費電力の小さい例えばスイツチング・レギユ
レータで発生するようにすれば、所期の目的が達
せられる。この場合比例定数Rが等価内部抵抗を
あらわしている。 That is, from equation (1), R L・I L (=E 0 )=E−R・I L …(2) In other words, since E−E 0 =R・I L (E−
If E 0 ) is controlled to be proportional to I L , it is possible to supply a DC talking current I L whose value depends on the subscriber line resistance R L as in the conventional circuit shown in FIG. 1, and (E − E 0 )
The desired purpose can be achieved by generating this with a switching regulator that consumes little power, such as a switching regulator. In this case, the proportionality constant R represents the equivalent internal resistance.
以下、本発明の1実施例について図面を参照し
て説明する。 Hereinafter, one embodiment of the present invention will be described with reference to the drawings.
第4図は等価回路で示した加入者線路と接続し
た本発明による通話電流供給回路を示し、図にお
いて、トランジスタ10、ダイオード11、イン
ダクタ12、キヤパシタ13からなる第1回路A
は、トランジスタ10の導通期間TONにインダク
タ12にエネルギーを貯え、これをトランジスタ
10の遮断期間TOFFに負荷側、つまり加入者線路
側に放出するスイツチング・レギユレータを構成
している。 FIG. 4 shows a communication current supply circuit according to the present invention connected to a subscriber line shown in an equivalent circuit.
constitutes a switching regulator that stores energy in the inductor 12 during the conduction period T ON of the transistor 10, and releases it to the load side, that is, the subscriber line side, during the cut-off period T OFF of the transistor 10.
ここで、第1回路の出力電圧、すなわちキヤパ
シタ13の端子電圧をE0、直流電源電圧をEと
すると、インダクタ12の蓄積エネルギー(E−
E0)・IL・TONが放出エネルギーE0・IL・TOFFと等
しいことから、
E0/E=TON/TON+TOFF=TON/T …(3)
但しT=TON+TOFF
なる関係が成立し、出力電圧E0はトランジスタ
10の導通時間のデユーテイに比例する。 Here, if the output voltage of the first circuit, that is, the terminal voltage of the capacitor 13 is E 0 and the DC power supply voltage is E, then the accumulated energy of the inductor 12 (E-
Since E 0 )・I L・T ON is equal to the released energy E 0・I L・T OFF , E 0 /E=T ON /T ON +T OFF =T ON /T …(3) However, T=T A relationship of ON + T OFF is established, and the output voltage E 0 is proportional to the duty of the conduction time of the transistor 10.
本発明では上記第1回路を次のように制御す
る。第(2)式と書き直すと
E0/E=1−R・IL/E …(4)
となる。 In the present invention, the first circuit is controlled as follows. When rewritten as equation (2), E 0 /E=1−R・I L /E (4) is obtained.
従つて、上記第(3)式と第(4)式から、第1回路を
通話電流供給回路として動作させるに必要な条件
は
TON/T=1−R・IL/E …(5)
である。 Therefore, from equations (3) and (4) above, the necessary conditions for operating the first circuit as a talking current supply circuit are T ON /T=1-R・I L /E (5) It is.
第4図において、トランジスタ14〜17、抵
抗素子18、定電流回路19、鋸歯状波電圧発生
回路20からなる第2回路Bは、上述した条件に
従つて第1回路Aのデユーテイを制御するための
ものである。 In FIG. 4, a second circuit B consisting of transistors 14 to 17, a resistive element 18, a constant current circuit 19, and a sawtooth voltage generating circuit 20 is used to control the duty of the first circuit A according to the above-mentioned conditions. belongs to.
トランジスタ15と加入者線路に直列に接続さ
れたトランジスタ14とは電流ミラー回路を構成
しており、トランジスタ15のコレクタ電流ICは
直流通話電流ILに比例する。 Transistor 15 and transistor 14 connected in series to the subscriber line constitute a current mirror circuit, and collector current I C of transistor 15 is proportional to DC talk current I L .
ここで両者の比例定数をk、抵抗素子18の抵
抗値をR18とすると、トランジスタ15のコレク
タ電位Vtは、
Vt=E−k・IL・R18 …(6)
となり、上記抵抗値R18を従来回路における内部
抵抗Rの設計目標値、例えば440Ωの1/kに選
べば、
Vt=E−R・IL …(7)
または
Vt/E=1−R・IL/E …(8)
が成立し、第(5)式の右辺と一致する。従つて、
VtとEとの比率で第1回路のトランジスタ10
の導通期間を決めれば、本発明による第4図の通
話電流発生回路は、電流電圧Eと出力電圧E0と
の関係が第(4)式を満足し、E−E0=R・ILの関係
から、この回路の内部抵抗が目標値Rに等しくな
ることがわかる。 Here, if the proportionality constant of both is k and the resistance value of the resistance element 18 is R 18 , then the collector potential V t of the transistor 15 is V t =E−k・I L・R 18 (6), and the above resistance If the value R 18 is chosen to be 1/k of the design target value of the internal resistance R in the conventional circuit, for example 440Ω, then V t =E−R・I L …(7) or V t /E=1−R・I L /E...(8) holds true and matches the right side of equation (5). Therefore,
Transistor 10 of the first circuit in the ratio of V t and E
If the conduction period of is determined, then in the talking current generating circuit of FIG. 4 according to the present invention, the relationship between the current voltage E and the output voltage E0 satisfies the equation (4), and E- E0 = R・I L It can be seen from the relationship that the internal resistance of this circuit is equal to the target value R.
鋸歯状波電圧発生回路20は、第5図Aに示す
如く、振幅E、周期Tの鋸歯状波電圧Vrを発生
する。この電圧Vrを比較器を構成する一方のト
ランジスタ17のベースに入力し、比較器の他方
のトランジスタ16のベースに前記した検出電圧
Vtを入力すると、上記トランジスタ17は第5
図Bに示す如くVt/Eのデユーテイ比でオン動
作する。従つてトランジスタ17で第1回路のト
ランジスタ10を駆動すると、第1回路は第(5)式
の条件を満足し、第(1)式および第3図に示した従
来のRを用いた電流供給回路と等価な回路として
動作する。 The sawtooth wave voltage generating circuit 20 generates a sawtooth wave voltage V r having an amplitude E and a period T, as shown in FIG. 5A. This voltage Vr is inputted to the base of one transistor 17 constituting the comparator, and the above-mentioned detection voltage is applied to the base of the other transistor 16 of the comparator.
When V t is input, the transistor 17
As shown in Figure B, it operates on at a duty ratio of V t /E. Therefore, when the transistor 10 of the first circuit is driven by the transistor 17, the first circuit satisfies the condition of equation (5), and the current supply using the conventional R shown in equation (1) and FIG. It operates as a circuit equivalent to the circuit.
上記本発明の回路構成によれば、スイツチン
グ・レギユレータ(第1回路)のオン・オフ動作
により、従来回路の内部抵抗素子Rと等価な機能
を得ているため、第1回路における消費電力を極
めて小さくできる。また、第2回路においても、
抵抗素子18に流れる電流ICを加入者回路の通話
電流ILよりも充分に小さくすることができるた
め、内部抵抗に相当する抵抗素子18の電力消費
を極めて小さくすることが可能となる。 According to the above circuit configuration of the present invention, the on/off operation of the switching regulator (first circuit) achieves a function equivalent to that of the internal resistance element R of the conventional circuit, and therefore the power consumption in the first circuit can be extremely reduced. Can be made smaller. Also, in the second circuit,
Since the current I C flowing through the resistive element 18 can be made sufficiently smaller than the communication current I L of the subscriber circuit, it is possible to extremely reduce the power consumption of the resistive element 18, which corresponds to the internal resistance.
例えば、トランジスタ15のエミツタ面積をト
ランジスタ14のエミツタ面積よりも小さくする
ことによりIC=1/100・IL、すなわちk=1/100に設
計した場合、E=−48Vのときの抵抗素子18で
の消費電力は約50mVにすぎない。また、トラン
ジスタ10の電流増幅率βを100とすれば、定電
流源19を流れる電流は1/100ILとなるため、この
電流による消費電力も50mW程度にすぎない。ト
ランジスタ14には電流ILが流れるが、ベース、
エミツタ間の電圧VBEが小さいため、その消費電
力も数10mWにすぎない。従つて、通話電流供給
回路としての消費電力を数100mWに抑えること
ができ、従来の抵抗Rを用いた回路に比較して交
換機内での発熱を著しく低減できる。 For example, if the emitter area of transistor 15 is designed to be smaller than that of transistor 14 so that I C =1/100・I L , that is, k=1/100, the resistance element 18 when E=-48V The power consumption is only about 50mV. Further, if the current amplification factor β of the transistor 10 is 100, the current flowing through the constant current source 19 is 1/100I L , so the power consumption due to this current is only about 50 mW. A current I L flows through the transistor 14, but the base
Since the voltage V BE between the emitters is small, its power consumption is only a few tens of mW. Therefore, power consumption as a communication current supply circuit can be suppressed to several hundred mW, and heat generation within the exchange can be significantly reduced compared to a conventional circuit using a resistor R.
尚、本発明は例えば第2回路の通話電流検出素
子14としてホール素子を用いるとか、全体寸法
の小型化を図るために回路A,BをそれぞれIC
化に適した回路構成とし、全体をワンチツプの
IC装置にまとめる等、実施例以外にも種々の変
形を可能とするものである。 Incidentally, in the present invention, for example, a Hall element may be used as the communication current detection element 14 of the second circuit, or circuits A and B may be integrated into ICs in order to reduce the overall size.
The circuit configuration is suitable for
Various modifications other than the embodiments are possible, such as combining them into an IC device.
第1図は加入者線路に接続された従来の電流供
給回路の構成を示す図、第2図は第1図回路の直
流等価回路図、第3図は上記加入者回路における
電流−負荷特性を説明するための図、第4図は本
発明による電流供給回路の1実施例を示す回路
図、第5図A,Bは上記実施例における第2回路
Bの動作説明のための信号波形図である。第4図
においてEは直流電圧源、Aは電圧E0を出力す
る第1回路、Bは上記第1回路のデユーテイを制
御する第2回路、Tはトランス、RLは加入者線
路の等価抵抗を示す。
Figure 1 is a diagram showing the configuration of a conventional current supply circuit connected to a subscriber line, Figure 2 is a DC equivalent circuit diagram of the circuit in Figure 1, and Figure 3 shows the current-load characteristics in the subscriber circuit. 4 is a circuit diagram showing one embodiment of the current supply circuit according to the present invention, and FIGS. 5A and 5B are signal waveform diagrams for explaining the operation of the second circuit B in the above embodiment. be. In Figure 4, E is a DC voltage source, A is a first circuit that outputs voltage E0 , B is a second circuit that controls the duty of the first circuit, T is a transformer, and R L is the equivalent resistance of the subscriber line. shows.
Claims (1)
路に該加入者線路の抵抗値に依存した値の直流通
話電流ILを供給する電流供給回路であつて、直流
電圧Eを発生する電圧源と、上記電圧源に接続さ
れ上記直流電圧Eをデユーテイに応じた電圧E0
に変換して上記加入者線路に印加する第1回路路
と、上記加入者線路に流れる直流通話電流ILを検
出し、E−E0がILに比例するように上記第1回路
のデユーテイを制御する第2回路とを有し、前記
第1回路が、前記電圧源に対して互いに直列に接
続されたトランジスタとインダクタとキヤパシタ
を含み、上記キヤパシタの両端に上記トランジス
タの導通時間に比例して電圧E0を出力するスイ
ツチングレギユレータからなり、上記第2回路が
上記加入者線路の直流通話電流ILを検出する第1
手段と、上記直流電圧Eから上記直流通話電流IL
と上記電流供給回路に要求される内部抵抗Rとの
積を差し引いた値に相当する検出電圧Vtを発生
する第2手段と、上記直流電圧Eと検出電圧Vt
との比率に応じて上記トランジスタの導通期間を
制御する第3手段とからなることを特徴とする電
流供給回路。 2 前記第1手段が、前記直流通話電流ILの1/
k(但し、k>1)の検出電流を出力するトラン
ジスタ回路からなり、前記第2手段が、前記電圧
源と上記トランジスタ回路との間に接続された抵
抗素子からなり、該抵抗素子が前記内部抵抗Rの
k倍の抵抗値を有し、前記検出電圧Vtが上記抵
抗素子の端子電圧として出力されることを特徴と
する第1項記載の電流供給回路。[Scope of Claims] 1. A current supply circuit having a predetermined internal resistance R and supplying a DC talking current I L to a subscriber line of a telephone set with a value depending on the resistance value of the subscriber line, the current supply circuit having a predetermined internal resistance R, A voltage source that generates voltage E, and a voltage source connected to the voltage source that converts the DC voltage E into a voltage E 0 according to the duty.
The DC talking current I L flowing through the subscriber line is detected, and the duty cycle of the first circuit is adjusted so that E-E 0 is proportional to I L. the first circuit includes a transistor, an inductor, and a capacitor connected in series with respect to the voltage source, and a conduction time proportional to the conduction time of the transistor is connected to both ends of the capacitor. The second circuit includes a switching regulator that outputs a voltage E0 , and the second circuit detects the DC talking current I L of the subscriber line.
and means for converting the DC talking current I L from the DC voltage E.
and an internal resistance R required for the current supply circuit .
and third means for controlling the conduction period of the transistor according to the ratio of the current supply circuit to the current supply circuit. 2. The first means is configured to control the DC talking current I L by 1/
k (k>1), the second means comprises a resistor connected between the voltage source and the transistor circuit, and the resistor is connected to the internal 2. The current supply circuit according to claim 1, wherein the current supply circuit has a resistance value k times as large as the resistance R, and the detection voltage V t is output as a terminal voltage of the resistance element.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP2275580A JPS56120252A (en) | 1980-02-27 | 1980-02-27 | Current supply circuit |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP2275580A JPS56120252A (en) | 1980-02-27 | 1980-02-27 | Current supply circuit |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS56120252A JPS56120252A (en) | 1981-09-21 |
| JPH0247765B2 true JPH0247765B2 (en) | 1990-10-22 |
Family
ID=12091495
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP2275580A Granted JPS56120252A (en) | 1980-02-27 | 1980-02-27 | Current supply circuit |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS56120252A (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH056671U (en) * | 1991-07-12 | 1993-01-29 | 東芝硝子株式会社 | Reflective lamp |
Family Cites Families (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS4828922A (en) * | 1971-08-19 | 1973-04-17 | ||
| JPS54114714A (en) * | 1978-02-27 | 1979-09-07 | Yuasa Battery Co Ltd | Dc power device |
| JPS556659A (en) * | 1978-06-30 | 1980-01-18 | Toshiba Corp | Constant-current circuit |
-
1980
- 1980-02-27 JP JP2275580A patent/JPS56120252A/en active Granted
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH056671U (en) * | 1991-07-12 | 1993-01-29 | 東芝硝子株式会社 | Reflective lamp |
Also Published As
| Publication number | Publication date |
|---|---|
| JPS56120252A (en) | 1981-09-21 |
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