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JPS6132783B2 - - Google Patents
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JPS6132783B2 - - Google Patents

Info

Publication number
JPS6132783B2
JPS6132783B2 JP7161177A JP7161177A JPS6132783B2 JP S6132783 B2 JPS6132783 B2 JP S6132783B2 JP 7161177 A JP7161177 A JP 7161177A JP 7161177 A JP7161177 A JP 7161177A JP S6132783 B2 JPS6132783 B2 JP S6132783B2
Authority
JP
Japan
Prior art keywords
charging
pulse
current
pulse current
battery
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
JP7161177A
Other languages
Japanese (ja)
Other versions
JPS547136A (en
Inventor
Kyoshi Inoe
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.)
Inoue Japax Research Inc
Original Assignee
Inoue Japax Research Inc
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 Inoue Japax Research Inc filed Critical Inoue Japax Research Inc
Priority to JP7161177A priority Critical patent/JPS547136A/en
Publication of JPS547136A publication Critical patent/JPS547136A/en
Publication of JPS6132783B2 publication Critical patent/JPS6132783B2/ja
Granted legal-status Critical Current

Links

Classifications

    • Y02E60/12

Landscapes

  • Secondary Cells (AREA)

Description

【発明の詳細な説明】[Detailed description of the invention]

本発明は、鉛蓄電池等の2次電池の充電方法に
関し、特に充電時に間歇的なパルス電流を用いて
充電することにより、電解液の飛散損耗を防止
し、かつ電池内の充電エネルギーの損失をも低減
させるものである。 電解液中に一対の電極を浸漬し、これに直流を
印加して電気分解すると、溶液中の陰イオンは陽
極に、陽イオンは陰極に引かれるから、陰陽両イ
オンの濃度は、それぞれ陽極および陰極付近で大
きくなり、イオン濃度は不均一となり、その結果
一種の濃淡電池ができて、外部から加えた直流電
圧とは反対の方向に起電力を生ずる。この現象を
成極作用(分極作用)といつているが、この作用
が電池の損失〔充電容量(IH)−放電容量
(IH)〕を増大せしめているので、電池製作にあ
たつては前記成極作用を除去するため多くの努力
が払われ、溶液を撹拌したり消毒剤を使用する等
の方法がとられてきたが、満足すべき結果を得る
に至つていない。 又近時電池の充電に際し、商用周波数を全波整
流した直流電力に1〜100KHzの高周波電力を重
畳して加えることも、例えば特公昭46−4936号公
報に記載されているように提案されている。この
場合は電解液中の陽イオン、陰イオンの移動によ
る前記イオン濃度の不均一が高周波電力によつて
分散せしめられて均一になり、成極作用を軽減せ
しめ局部電池形成のために消費される損失エネル
ギが低減せしめられるのであると解されていた。 しかし、高周波分が直流電力に重畳され、どち
らかというと直流電力にのつているという傾向か
ら、電極間には電圧が常時印加された状態であつ
て、高周波による濃度の不均一の分散は行われて
も、依然として直流分による成極作用は存在して
いる。又上記の場合高周波電力でも化学的な変化
のエネルギ蓄積力を有するが、上記直流電圧に重
畳する場合の高周波の電力は小さく、例えば多量
のエネルギーを蓄積せしめ放電容量を増大せしめ
る等に寄与していない。 本発明ではこれらの点を考虜して間歇的にパル
ス電流を用いて充電することを発明し、特定のパ
ルス電流条件とすることにより電解液の発散を防
止するようにしたものであり、充電パルス電流の
条件としては、パルス巾(パルス電流の特続時
間)が最大でも200μs、好ましくは50μs以下
のほぼ矩形波パルス電流とし、又パルス電流間の
休止時間を少くとも前記パルス巾の2倍から30倍
程度とすることにより、パルス電流印加の休止に
より成極作用が起る前にパルス電流をきり、新に
パルス電流の印加によりイオン濃度の不均一な状
態での通電による充電を行なわず、電池内のエネ
ルギー損失を低減させ、熱損失を小にして液の蒸
発を少くしたものであり、化学エネルギとしての
蓄積つまりはエネルギ蓄積密度を増すことができ
る。又充電による化学エネルギーの蓄積を電極表
層部だけでなく内部深部まで可能とすることがで
きる。 パルス電流のパルス巾としては、最大でも200
μs、好ましくは50μs以下で、通常5〜30μs
程度を利用するのがよく、パルス電流の休止時間
は前記パルス巾の少くとも9倍から30倍までで、
通常3〜4倍乃至10数倍位がよく、30倍以上で
は、充電の時間的能率等の点から好ましくなく又
休止時間が2倍以下の短かい場合はパルス電流の
間が短かくなりすぎて成極作用を促進することと
なり、結局パルス電流間の間隔を適宜に設けるこ
とにより成極作用を少くさせるのである。 本発明は自動車エンジン、固定電池、充電器、
急速充電器等いずれにも用いて可である。 なお、パルス電流の振巾は、前記休止時間が3
倍以上であれば、格別注意をすることなく数10A
以上として得るものであるが、パルス電流を形成
するトランジスタ等のスイツチ応答速度、電流振
巾に応じた必要個数、充電電源の電圧(パルス電
流の電圧)電池の電極端子間充電抵抗等にもよる
が、必要な平均充電電流が得られるように設定す
ればよい。 本発明を実施例により説明すると、寸法160mm
×100mm×5mmの鉛電極と、比重約1.23の硫酸液
約450c.c.から成る鉛蓄電池に於て、パルス巾20μ
s、休止巾60μs、電流振巾3A(平均約1A)の
パルス電流により室温20℃一定として15時間の充
電を行なつた場合と、平均電流1Aの直流による
充電を行なつた場合の平均ガス発生量(c.c./mi
n)と液の損耗量(%)とを測定した所下記の通
りであつた。なお、液温は前者約28℃、後者約40
゜Cとなていた。
The present invention relates to a method of charging a secondary battery such as a lead-acid battery, and in particular, uses intermittent pulse current during charging to prevent electrolyte scattering and loss and to reduce loss of charging energy within the battery. It also reduces When a pair of electrodes is immersed in an electrolytic solution and a direct current is applied to electrolyze it, the anions in the solution are attracted to the anode and the cations are attracted to the cathode. It becomes larger near the cathode, and the ion concentration becomes non-uniform, resulting in a kind of concentration cell, producing an electromotive force in the opposite direction to the externally applied DC voltage. This phenomenon is called polarization effect (polarization effect), and since this effect increases battery loss [charge capacity (IH) - discharge capacity (IH)], the above-mentioned Many efforts have been made to eliminate the polarization effect, including methods such as stirring the solution and using disinfectants, but no satisfactory results have been achieved. Recently, when charging a battery, it has been proposed to superimpose high frequency power of 1 to 100 KHz on DC power obtained by full-wave rectification of the commercial frequency, as described in Japanese Patent Publication No. 46-4936, for example. There is. In this case, the non-uniformity of the ion concentration due to the movement of cations and anions in the electrolyte is dispersed and made uniform by high-frequency power, which reduces the polarization effect and is consumed to form a local battery. It was understood that the loss energy was reduced. However, because the high frequency component tends to be superimposed on the DC power, and rather increases with the DC power, a voltage is constantly applied between the electrodes, and uneven concentration dispersion due to the high frequency is not possible. However, the polarization effect due to the DC component still exists. In the above case, high-frequency power also has the ability to store energy for chemical changes, but the high-frequency power when superimposed on the DC voltage is small, and does not contribute to, for example, storing a large amount of energy and increasing discharge capacity. do not have. The present invention takes these points into account and devises a method of charging using pulsed current intermittently, and by setting specific pulsed current conditions, the dispersion of the electrolyte is prevented. The conditions for the pulse current are that the pulse width (special time of the pulse current) is at most 200 μs, preferably 50 μs or less, and the rest period between the pulse currents is at least twice the pulse width. By increasing the voltage by about 30 times from 1 to 30, the pulse current is stopped before the polarization effect occurs by stopping the application of the pulse current, and by applying a new pulse current, charging is not performed by energization in a state where the ion concentration is uneven. , which reduces energy loss within the battery, reduces heat loss, and reduces evaporation of the liquid, which can increase the storage of chemical energy, that is, the energy storage density. Furthermore, chemical energy can be stored not only in the surface layer of the electrode but also deep inside the electrode. The maximum pulse width of the pulse current is 200
μs, preferably 50 μs or less, usually 5 to 30 μs
The rest time of the pulse current is at least 9 times to 30 times the width of the pulse, and
Normally, 3 to 4 times to about 10 times is better. If it is more than 30 times, it is not preferable from the point of view of charging time efficiency, etc., and if the rest time is short, less than twice, the interval between pulse currents becomes too short. This promotes the polarization effect, and ultimately the polarization effect can be reduced by appropriately providing intervals between pulse currents. The present invention relates to automobile engines, fixed batteries, chargers,
It can be used for any quick charger etc. Note that the amplitude of the pulse current is determined by the above-mentioned pause time of 3
If it is more than twice that, several 10A can be applied without special precautions.
The above is what you get, but it depends on the response speed of the switch such as the transistor that forms the pulse current, the required number according to the current amplitude, the voltage of the charging power source (the voltage of the pulse current), the charging resistance between the electrode terminals of the battery, etc. However, it should be set so that the required average charging current can be obtained. To explain the present invention using an example, the size is 160 mm.
In a lead-acid battery consisting of lead electrodes of ×100 mm ×5 mm and approximately 450 c.c. of sulfuric acid solution with a specific gravity of approximately 1.23, a pulse width of 20 μ
Average gas when charging for 15 hours with a constant room temperature of 20℃ using a pulse current with a pause width of 60μs and a current amplitude of 3A (average approx. 1A), and when charging with direct current with an average current of 1A. Generation amount (cc/mi
n) and the amount of liquid loss (%) were measured and found to be as follows. The liquid temperature is approximately 28℃ for the former and approximately 40℃ for the latter.
It was ℃.

【表】 即ち、本発明によれば、ガス発生量が多いにも
かかわらず、液の蒸発その他による飛散損耗量は
少なく、充電の際に於ける成極作用発生その他に
よるエネルギ損失は少なく、液損耗量の少ない点
で特に優れたものであつた。
[Table] That is, according to the present invention, although the amount of gas generated is large, the amount of scattering loss due to liquid evaporation and other causes is small, the energy loss due to polarization and other causes during charging is small, and the liquid It was particularly excellent in terms of low wear and tear.

Claims (1)

【特許請求の範囲】[Claims] 1 電池を充電する場合にパルス電流のパルス巾
を200μs以下に設定し、このパルス電流間の休
止時間をパルス電流のパルス巾の2倍から30倍と
する間歇的なパルス電流で充電することにより、
熱損失を小にして液の蒸発を少なくしたことを特
徴とする電池充電方法。
1. When charging a battery, the pulse width of the pulse current is set to 200 μs or less, and the rest time between pulse currents is set to 2 to 30 times the pulse width of the pulse current. By charging with intermittent pulse current. ,
A battery charging method characterized by reducing heat loss and liquid evaporation.
JP7161177A 1977-06-18 1977-06-18 Method of charging battery Granted JPS547136A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP7161177A JPS547136A (en) 1977-06-18 1977-06-18 Method of charging battery

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP7161177A JPS547136A (en) 1977-06-18 1977-06-18 Method of charging battery

Publications (2)

Publication Number Publication Date
JPS547136A JPS547136A (en) 1979-01-19
JPS6132783B2 true JPS6132783B2 (en) 1986-07-29

Family

ID=13465610

Family Applications (1)

Application Number Title Priority Date Filing Date
JP7161177A Granted JPS547136A (en) 1977-06-18 1977-06-18 Method of charging battery

Country Status (1)

Country Link
JP (1) JPS547136A (en)

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5878222U (en) * 1981-11-24 1983-05-26 株式会社クボタ Transmission structure for traveling in work vehicles
JP3108529B2 (en) * 1992-02-17 2000-11-13 エムアンドシー株式会社 Battery charging method and device

Also Published As

Publication number Publication date
JPS547136A (en) 1979-01-19

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