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JPS5943895B2 - battery charging circuit - Google Patents
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JPS5943895B2 - battery charging circuit - Google Patents

battery charging circuit

Info

Publication number
JPS5943895B2
JPS5943895B2 JP12215377A JP12215377A JPS5943895B2 JP S5943895 B2 JPS5943895 B2 JP S5943895B2 JP 12215377 A JP12215377 A JP 12215377A JP 12215377 A JP12215377 A JP 12215377A JP S5943895 B2 JPS5943895 B2 JP S5943895B2
Authority
JP
Japan
Prior art keywords
voltage
battery
inverter
charging
transistor
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
JP12215377A
Other languages
Japanese (ja)
Other versions
JPS5454247A (en
Inventor
啓壽 福島
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.)
Sanyo Electric Co Ltd
Original Assignee
Sanyo 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 Sanyo Electric Co Ltd filed Critical Sanyo Electric Co Ltd
Priority to JP12215377A priority Critical patent/JPS5943895B2/en
Publication of JPS5454247A publication Critical patent/JPS5454247A/en
Publication of JPS5943895B2 publication Critical patent/JPS5943895B2/en
Expired legal-status Critical Current

Links

Classifications

    • Y02E60/12

Landscapes

  • Secondary Cells (AREA)

Description

【発明の詳細な説明】 本発明は商用電源の整流電圧にてトランジスタインバー
タを作動させ、そのインバータ出力を整流した半波電流
により電池を充電する回路に関する。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a circuit that operates a transistor inverter using a rectified voltage of a commercial power source and charges a battery with a half-wave current obtained by rectifying the inverter output.

この種回路で前記インバータ出力を大きくすることによ
り電池を急速充電することができる。
With this type of circuit, the battery can be charged quickly by increasing the inverter output.

急速充電するときには電池の過充電を防止するために電
池電圧を検出して所定電圧に達するとき急速充電を停止
するようになされる。しかしながらこの種従来装置にお
いては、電池電圧の検出を充電電流が流れるときに行う
ため、電池の内部インピーダンスによろ電圧降下分を含
めて検出することになり、電池電圧の検出としては誤検
出となる。
In order to prevent overcharging of the battery during rapid charging, the battery voltage is detected and the rapid charging is stopped when a predetermined voltage is reached. However, in this type of conventional device, the battery voltage is detected when the charging current flows, so the voltage drop is included in the detection due to the internal impedance of the battery, resulting in false detection of the battery voltage. .

特にインバータ出力を整流した半波電流はパルス電流と
なり、その波高値が平均光電電流値より大きいため、パ
ルス充電電流が流れるときに電池電圧を検出する場合に
は、見かけ上大きな電池電圧となり、ただちに充電を停
止することになり、電池を充分に充電することができな
い欠点がある。本発明はかかる点に鑑み発明されたもの
にして以下本発明の一実施例を図面に基いて説明する。
In particular, the half-wave current obtained by rectifying the inverter output becomes a pulse current, and its peak value is larger than the average photoelectric current value. Therefore, when detecting the battery voltage when a pulse charging current flows, the battery voltage appears to be large, and immediately This has the disadvantage that charging is stopped and the battery cannot be sufficiently charged. The present invention was invented in view of this point, and one embodiment of the present invention will be described below with reference to the drawings.

第1図において1は全波整流回路にしてその交流入力端
は商用電源2に接続され、その直流出力端には逆流阻止
ダイオード3及び平滑コンデンサ4の直列回路が接続さ
れる。5はトランジスタインバータにして、平滑コンデ
ンサ4の両端には発振トランス6の1次コイルTと発振
トランジスタ8のコレクタ・エミッタの直列回路が接続
され、トランジスタ8のベース・エミッタ間には発振ト
ランス6の帰還コイル9、インバータ5の発振周波数決
定用の抵抗10及びコンデンサ11の直列回路が接続さ
れる。
In FIG. 1, 1 is a full-wave rectifier circuit whose AC input end is connected to a commercial power source 2, and whose DC output end is connected to a series circuit of a reverse current blocking diode 3 and a smoothing capacitor 4. 5 is a transistor inverter, and a series circuit of the primary coil T of the oscillation transformer 6 and the collector-emitter of the oscillation transistor 8 is connected to both ends of the smoothing capacitor 4. A series circuit including a feedback coil 9, a resistor 10 for determining the oscillation frequency of the inverter 5, and a capacitor 11 is connected.

前記1次コイル7の両端にはスパイク電圧吸収用の抵抗
12及びコンデンサ13の直列回路が接続される。また
発振トランス6の2次コイル14は整流用ダイオード1
5を介して被充電電池16に接続される。次に17は基
準電圧回路にして抵抗18とツェナーダイオード19の
直列回路を全波整流回路1の直流出力端に接続してツェ
ナーダイオード19の両端間に定電圧を得、抵抗20及
び21により分圧している。
A series circuit of a resistor 12 and a capacitor 13 for absorbing spike voltage is connected to both ends of the primary coil 7. In addition, the secondary coil 14 of the oscillation transformer 6 is connected to the rectifier diode 1.
5 to the battery to be charged 16 . Next, 17 is a reference voltage circuit, and a series circuit of a resistor 18 and a Zener diode 19 is connected to the DC output terminal of the full-wave rectifier circuit 1 to obtain a constant voltage across the Zener diode 19, which is divided by resistors 20 and 21. It's pressing.

この分圧点22はプログラマフッいユニジヤンクシヨン
・トランジスタ(以下PUTと云う)23のアノード電
圧となる。またPUT23のゲートは抵抗24を介して
電池16の陽極に接続されると共にPUT23のカソー
ドは抵抗25を介して発振トランジスタ8のベースに接
続されてベースバイアス回路を構成する。以上の構成に
おいて基準電圧回路17の分圧点22の電圧は第2図に
示すようにツエナーダイオード19を接続しないときの
電圧波形V1に対し波形2となり、基準定電圧V。
This voltage division point 22 becomes the anode voltage of a programmer's uniform union transistor (hereinafter referred to as PUT) 23. Further, the gate of PUT 23 is connected to the anode of battery 16 via resistor 24, and the cathode of PUT 23 is connected to the base of oscillation transistor 8 via resistor 25 to form a base bias circuit. In the above configuration, the voltage at the voltage dividing point 22 of the reference voltage circuit 17 has a waveform 2, which is a reference constant voltage V, as compared to the voltage waveform V1 when the Zener diode 19 is not connected, as shown in FIG.

を有する。一方充電開始時の電池電圧は各半サイクルに
おける波形2の基準定電圧。より低い。従つて分圧点電
圧V2が電池電圧より高いとき、即ちPUT23のアノ
ード電圧がゲート電圧より高いときPUT23が導通し
て発振トランジスタ8にベース電流が流れ、インバータ
5が発振する。またPUT23は一旦導通するとその保
持電流に低下する迄導通するが、各半サイクルの終了時
点で保持電流以下になるため、PUT23が遮断するこ
とになりインバータ5は各半サイクル毎に発振する。こ
のようにインバータ5が各半サイクル毎に発振して、そ
の発振出力は整流用ダイオード15により整流され、パ
ルス状半波電流により電池16が充電される。
has. On the other hand, the battery voltage at the start of charging is the reference constant voltage of waveform 2 in each half cycle. lower. Therefore, when the voltage dividing point voltage V2 is higher than the battery voltage, that is, when the anode voltage of the PUT 23 is higher than the gate voltage, the PUT 23 becomes conductive, the base current flows through the oscillation transistor 8, and the inverter 5 oscillates. Further, once the PUT 23 is conductive, it continues to conduct until the current drops to the holding current, but at the end of each half cycle, the holding current becomes less than the holding current, so the PUT 23 is cut off, and the inverter 5 oscillates every half cycle. In this way, the inverter 5 oscillates every half cycle, and the oscillation output is rectified by the rectifying diode 15, and the battery 16 is charged by the pulsed half-wave current.

第2図において3は電池電圧波形を示し、パルス状波形
部31はインバータ5の発振出力による充電中を示し、
その下包絡線V32が時間と共に上昇して電池電圧が上
昇するのを表わしている。また第1の半サイクルの充電
終了時点P1と第2の半サイクルの充電開始時点P2と
の間の連絡線部33はパルス状半波電流によつて電池内
で化学反応が急激に生じた後に安定状態に移行して、電
池電圧が低下することを表わしており、充電の進行によ
りこの連絡線部V33が徐々に上昇する。同図aは電池
電圧が低いとき、bは電池電圧が高いときを示す。而し
て充電が充分に進行していない電池電圧の低いときは、
第2図aに示された如く電池電圧波形V3の連絡線部3
3は充分に上昇していないので未だ低い。
In FIG. 2, 3 indicates the battery voltage waveform, and the pulse-like waveform portion 31 indicates charging by the oscillation output of the inverter 5,
The lower envelope curve V32 rises with time, indicating that the battery voltage increases. Further, the connection line section 33 between the charging end point P1 of the first half cycle and the charging start point P2 of the second half cycle is connected to the connecting line section 33 after a chemical reaction occurs rapidly within the battery due to the pulsed half-wave current. This indicates that the battery voltage is reduced as the battery enters a stable state, and as charging progresses, this connection line portion V33 gradually rises. In the figure, a shows a state when the battery voltage is low, and b shows a state when the battery voltage is high. However, when the battery voltage is low and charging is not progressing sufficiently,
Connecting line portion 3 of battery voltage waveform V3 as shown in FIG. 2a.
3 is still low because it hasn't risen enough.

従つてこの電池電圧波形3の連絡線部33は点P3後に
おいて基準電圧回路17の分圧点電圧V2より低くなる
。この結果PUT23のゲート電圧がアノード電圧より
低くなつて該PUT23が導通し、発振トランジスタ8
のベースに電流が通じ、該発振トランジスタ8は導通し
て発振を開始する。ただし、この発振トランジスタ8の
発振によるインバータ5の出力電圧は、前記発振トラン
ジスタ8の発振直後においては未だ前記電池電圧より低
く、二次コイル14から電池に向かう電流が生じず、電
池16に電流が供給されないので結局前記発振トランジ
スタ8の発振直後においては電池16を充電するには至
つていない。やがて第1の半サイクルで充電された電池
16内部での化学反応が安定し、前記連絡線部V33は
更に低下する。また前記インバータ5の出力電圧も上昇
する。そして図のパルス状波形部31で示Aれるように
充電電流が電池16に供給される。ここで充電開始点P
2は前記パルス状波形部31の上包絡線34と前記連絡
線部33との交点になつており、充電が充分に進行して
ない電池電圧の低いときは、前記点P3でPUT23が
導通するが実際に電池16が充電Aれるのは前記点P2
以降になる。このようにして電池電圧が高くなるときに
は、第2図bに示す如く連絡線部33が基準定電圧。以
下になる点P4に至るとき、インバータ5が発振作動す
る。このため各半サイクルのパルス状波形部V3,の期
間T1が電池電圧の低いときのそれT2に比し短かくな
る。従つて電池16の平均充電電流は第3図中1に示す
如く所定充電時点t後徐々に低下する。これに対し電池
16の平均充電電圧は同図中で示すように、時点t迄上
昇し続けた後は一定電圧になる。以上の如く本発明によ
れば、非充電時の電池電圧と基準定電圧とをゲート・ア
ノード間で比較するPUTを設け、このPUTをインバ
ータの発振トランジスタのベースバイアス回路に介挿し
たから、非充電時の電池電圧を検出することができ、充
電電流が流れているときに電池電圧を検出する場合に比
し、電池電圧の検出誤差を少なくすることができる。ま
た非充電時の電池電圧を検出するため、充電電流として
波高値の高いパルス電流を用いることができ、トランジ
スタインバータを用いて電池を所望の電圧に充電するこ
とができる。
Therefore, the connection line portion 33 of the battery voltage waveform 3 becomes lower than the voltage division point voltage V2 of the reference voltage circuit 17 after the point P3. As a result, the gate voltage of the PUT 23 becomes lower than the anode voltage, the PUT 23 becomes conductive, and the oscillation transistor 8
A current flows through the base of the oscillation transistor 8, and the oscillation transistor 8 becomes conductive and starts oscillating. However, the output voltage of the inverter 5 due to the oscillation of the oscillation transistor 8 is still lower than the battery voltage immediately after the oscillation of the oscillation transistor 8, and no current flows from the secondary coil 14 to the battery, and no current flows to the battery 16. Since the voltage is not supplied, the battery 16 cannot be charged immediately after the oscillation transistor 8 oscillates. Eventually, the chemical reaction inside the battery 16 charged in the first half cycle becomes stable, and the connection line portion V33 further decreases. Furthermore, the output voltage of the inverter 5 also increases. A charging current is then supplied to the battery 16 as shown by the pulse-like waveform portion 31 in the figure. Here is the charging starting point P
2 is the intersection of the upper envelope 34 of the pulse waveform section 31 and the connection line section 33, and when charging is not progressing sufficiently and the battery voltage is low, the PUT 23 becomes conductive at the point P3. However, the battery 16 is actually charged at the point P2.
It will be later. When the battery voltage increases in this manner, the connecting line portion 33 is at the reference constant voltage as shown in FIG. 2b. When the point P4 is reached as below, the inverter 5 operates to oscillate. Therefore, the period T1 of the pulse waveform portion V3 of each half cycle is shorter than the period T2 when the battery voltage is low. Therefore, the average charging current of the battery 16 gradually decreases after the predetermined charging time t, as shown at 1 in FIG. On the other hand, as shown in the figure, the average charging voltage of the battery 16 continues to rise until time t, and then becomes a constant voltage. As described above, according to the present invention, a PUT is provided for comparing the battery voltage during non-charging with a reference constant voltage between the gate and anode, and this PUT is inserted into the base bias circuit of the oscillation transistor of the inverter. Therefore, the battery voltage detection error can be reduced compared to the case where the battery voltage is detected when the charging current is flowing. Furthermore, in order to detect the battery voltage when not being charged, a pulse current with a high peak value can be used as the charging current, and the battery can be charged to a desired voltage using a transistor inverter.

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

図面は本発明の一実施例を示し、第1図は本発明による
充電回路図、第2図A,bは電池電圧が低いとき及び高
いときの電池電圧波形図、第3図は電池の充電特性図で
ある。 5・・・・・・インバータ、16・・・・・・電池、2
3・・・・・・PUT、8・・・・・・発振トランジス
タ。
The drawings show an embodiment of the present invention; FIG. 1 is a charging circuit diagram according to the present invention, FIGS. 2A and b are battery voltage waveform diagrams when the battery voltage is low and high, and FIG. 3 is a battery charging diagram. It is a characteristic diagram. 5...Inverter, 16...Battery, 2
3...PUT, 8...Oscillation transistor.

Claims (1)

【特許請求の範囲】[Claims] 1 商用電源の整流電圧にてトランジスタインバータを
作動させ、そのインバータ出力を整流した半波電流によ
り電池を充電するものにおいて、前記整流電圧によつて
作動する基準電圧回路を設け、該基準電圧回路にアノー
ド側が接続されたプログラマブル・ユニジャンクシヨン
・トランジスタのカソード側を前記インバータの発振ト
ランジスタのベースバイアス回路に接続し、前記電池を
前記プログラマブル・ユニジヤンクシヨン・トランジス
タのゲート側に接続し、前記基準電圧と電池電圧とを、
該プログラマブル・ユニジャンクシヨン・トランジスタ
の導通・非導通によつて比較検出することによつて充電
電流が流れない時の電池電圧を検出すると共に、前記プ
ログラマブル・ユニジャンクシヨン・トランジスタの動
作によつて前記インバータの出力を制御して成る電池の
充電回路。
1. In a device that operates a transistor inverter with the rectified voltage of a commercial power supply and charges a battery with a half-wave current obtained by rectifying the inverter output, a reference voltage circuit that operates with the rectified voltage is provided, and the reference voltage circuit is The cathode side of the programmable unijunction transistor whose anode side is connected is connected to the base bias circuit of the oscillation transistor of the inverter, the battery is connected to the gate side of the programmable unijunction transistor, and the reference voltage and the battery voltage,
By comparing and detecting conduction and non-conduction of the programmable unijunction transistor, the battery voltage when no charging current flows is detected, and the battery voltage is detected by the operation of the programmable unijunction transistor. A battery charging circuit configured to control the output of the inverter.
JP12215377A 1977-10-07 1977-10-07 battery charging circuit Expired JPS5943895B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP12215377A JPS5943895B2 (en) 1977-10-07 1977-10-07 battery charging circuit

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP12215377A JPS5943895B2 (en) 1977-10-07 1977-10-07 battery charging circuit

Publications (2)

Publication Number Publication Date
JPS5454247A JPS5454247A (en) 1979-04-28
JPS5943895B2 true JPS5943895B2 (en) 1984-10-25

Family

ID=14828907

Family Applications (1)

Application Number Title Priority Date Filing Date
JP12215377A Expired JPS5943895B2 (en) 1977-10-07 1977-10-07 battery charging circuit

Country Status (1)

Country Link
JP (1) JPS5943895B2 (en)

Also Published As

Publication number Publication date
JPS5454247A (en) 1979-04-28

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