JPS607058A - Method of welding terminal for current collection - Google Patents
Method of welding terminal for current collectionInfo
- Publication number
- JPS607058A JPS607058A JP58113306A JP11330683A JPS607058A JP S607058 A JPS607058 A JP S607058A JP 58113306 A JP58113306 A JP 58113306A JP 11330683 A JP11330683 A JP 11330683A JP S607058 A JPS607058 A JP S607058A
- Authority
- JP
- Japan
- Prior art keywords
- welding
- electrode plate
- current collecting
- plate
- collecting terminal
- 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.)
- Granted
Links
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01M—PROCESSES OR MEANS, e.g. BATTERIES, FOR THE DIRECT CONVERSION OF CHEMICAL ENERGY INTO ELECTRICAL ENERGY
- H01M50/00—Constructional details or processes of manufacture of the non-active parts of electrochemical cells other than fuel cells, e.g. hybrid cells
- H01M50/50—Current conducting connections for cells or batteries
- H01M50/531—Electrode connections inside a battery casing
- H01M50/538—Connection of several leads or tabs of wound or folded electrode stacks
-
- Y—GENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
- Y02—TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
- Y02E—REDUCTION OF GREENHOUSE GAS [GHG] EMISSIONS, RELATED TO ENERGY GENERATION, TRANSMISSION OR DISTRIBUTION
- Y02E60/00—Enabling technologies; Technologies with a potential or indirect contribution to GHG emissions mitigation
- Y02E60/10—Energy storage using batteries
Landscapes
- Chemical & Material Sciences (AREA)
- Chemical Kinetics & Catalysis (AREA)
- Electrochemistry (AREA)
- General Chemical & Material Sciences (AREA)
- Connection Of Batteries Or Terminals (AREA)
Abstract
Description
【発明の詳細な説明】
本発明はN1−cd電池の如く捲回された極板が容器内
に収容された構造を有する電池に係わり、前記極板の端
部1こ集電用端子(タブ)を溶接する方法に関するもの
である。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a battery having a structure in which a wound electrode plate is housed in a container, such as an N1-CD battery. ).
衆知の通り可搬形の電気、電子機器用電源とる。即ち大
きな電流で放電した際に電池電圧の低下が出来るだけ小
さいことが要求されるわけで、このためには電池の内部
抵抗を極力小さくすることが不可欠な問題となる。As everyone knows, it is a portable power source for electrical and electronic devices. That is, it is required that the drop in battery voltage be as small as possible when discharging with a large current, and for this purpose it is essential to reduce the internal resistance of the battery as much as possible.
この問題の1つの解決手段として多点集電方式と称する
ものが採用されている。これは極板の1ケ所に集電用端
子を取4−3け、極板内部で発生した電流をここに集め
る従来の方式と異なり、一枚の極板の多数の場所から電
流を築める方式で1発生した電流が集電用端子に到達す
るまでの距離か短かくなるため1こ、結果的に電池の内
部抵抗を小さくすることが出来るわけである。As one means of solving this problem, a so-called multi-point current collection system has been adopted. This differs from the conventional method in which 4-3 current collecting terminals are placed at one location on the electrode plate and the current generated inside the plate is collected there. In this method, the distance that the generated current takes to reach the current collecting terminal is shortened, and as a result, the internal resistance of the battery can be reduced.
第1図は各点集電方式を用いた場合の集電用端子と極板
との接続状態の一例を示したものである。同図に於て1
は極板であり、この極板lはセパレータを介して相手径
(例えばlが陽極板であれば相手径は陽極板となる)と
重ね合され図の如く捲回されている。(セパレータ、相
手極は同図には示していない)また2は集電用端子て、
これは同図の如く捲回された極板の端部3が形成する平
面上に位置し1例えば該集電用端子2に形成しCある突
起部(プロジェクション)4と前記極板lの端部3(厳
密には極板1を構成する芯材の端部)とは溶接等の手段
により電気的に接続(図中のa −、−e )され、こ
の部分より集電がなされるわけである。FIG. 1 shows an example of the connection state between the current collecting terminal and the electrode plate when the point current collecting method is used. In the same figure 1
is an electrode plate, and this electrode plate l is overlapped with a mating diameter (for example, if l is an anode plate, the mating diameter becomes an anode plate) via a separator, and is wound as shown in the figure. (The separator and the other electrode are not shown in the figure.) Also, 2 is the current collecting terminal.
As shown in the same figure, this is located on a plane formed by the end 3 of the wound electrode plate 1, for example, a projection 4 formed on the current collecting terminal 2 and the end of the electrode plate 1. It is electrically connected to part 3 (strictly speaking, the end of the core material constituting electrode plate 1) by means such as welding (a-, -e in the figure), and current is collected from this part. It is.
さて、本発明の対象としているのは上述した集電用端子
2と極板1との接続方法である。この接続には従来より
抵抗溶接が用いられているが、この種の溶接は必ずしも
容易なものではなく、溶接強度のバラツキが著しく、信
頼性に欠けることが多い。その理由は下記の如きもので
ある。Now, the object of the present invention is a method of connecting the current collecting terminal 2 and the electrode plate 1 described above. Resistance welding has conventionally been used for this connection, but this type of welding is not necessarily easy, and the welding strength often varies significantly and is often unreliable. The reason is as follows.
第2図は第1図に示した集電用端子2と極板1との接続
部についてより詳細に示したものである。すなわち前記
極板1は芯材5によって活物質6が保持された構造にな
っており、前述した極板1の端部3は同図に示した如(
芯材5が活物質の存在する部分より多少とび出してにの
部分が集電用端子2と接続されることになる。FIG. 2 shows in more detail the connection between the current collecting terminal 2 and the electrode plate 1 shown in FIG. That is, the electrode plate 1 has a structure in which the active material 6 is held by the core material 5, and the end portion 3 of the electrode plate 1 described above is formed as shown in the figure.
A portion of the core material 5 that slightly protrudes from the portion where the active material is present is connected to the current collecting terminal 2.
芯材5はNi−Cd電池の場合1通常は表面にN1めつ
きがなされたpeより成るパンチングメタルが用いられ
、相手方の集電用端子2もほぼ同一の材質のものか用い
られているが、ここて問題1こしなければならないのは
、両者の肉厚である。芯材5は一般的に50〜80μm
の厚さのものが使用されるのに対して、集電用端子2の
方は極板全体からの電流かここに集められることを考慮
し0.15〜0.2 mm厚さのものが使用される。両
者lヨこの肉厚の差にもとず(溶接部の熱容量の差は良
好な溶接部を?Mる上て致命的と言っても良い。両者の
接触面積が著しく小さい上にこれだけ熱容量が異なると
溶接電流か流れても集電用端子2の突起部4の方での温
度上昇はわずかであり、その一部が溶融することも期待
できない。一方熱容量の小さい芯材5の方は逆に必要以
上に溶融が起ってしまう。溶融した金属が集電用端子2
の突起部4表面にぬれそくれれば一応溶接はされるが、
突起部4の温度上昇がわずかであるために、これにぬれ
なかったり、ぬれても不十分なため結局溶接がうまくゆ
かないといった結果になる。またこの溶接に於ては第1
図に見られる如<、1本の突起部4が多数(同図a %
e )の位置で極板1と溶接されねばならないが、溶
接電流通電前の両者の接触状態のバラツキ、シリーズタ
イプの溶接を行なわねばならないため1こ、溶接に無効
な電流が集電用端子2内を流れることによる有効な電流
の不規則な変動等により、実際に溶接されねばならない
溶接点数の半分以下しか溶接されないといったことが問
題となっていた。In the case of Ni-Cd batteries, the core material 5 is usually a punched metal made of PE with N1 plating on the surface, and the opposing current collecting terminal 2 is also made of almost the same material. The first problem here is the thickness of both parts. Core material 5 generally has a thickness of 50 to 80 μm
In contrast, the current collecting terminal 2 should have a thickness of 0.15 to 0.2 mm, considering that the current from the entire plate is collected here. used. Based on this difference in wall thickness between the two (the difference in heat capacity of the welded part can be said to be fatal for making a good welded part), the contact area between the two is extremely small and the heat capacity is Otherwise, even if welding current flows, the temperature rise at the protrusion 4 of the current collecting terminal 2 will be slight, and we cannot expect that part of it will melt.On the other hand, the opposite is true for the core material 5, which has a small heat capacity. The melted metal will melt more than necessary.
If the surface of the protrusion 4 gets wet, welding will be completed, but
Since the temperature rise of the protrusion 4 is slight, it may not be wetted by the protrusion 4, or even if it is wetted, the welding will not be successful as a result. Also, in this welding, the first
As seen in the figure, one protrusion 4 is numerous (a%
It must be welded to the electrode plate 1 at position e), but since there are variations in the contact state between the two before the welding current is applied and series type welding has to be performed, the current that is ineffective for welding is transferred to the current collecting terminal 2. The problem has been that less than half of the number of welding points that actually need to be welded are welded due to irregular fluctuations in the effective current flowing through the welding.
本発明は上述した如き問題点を解決し1強度的にも電気
的にもすぐれた。信頼性の高い接続部を提供するもので
ある。The present invention solves the above-mentioned problems and has excellent strength and electrical properties. This provides a highly reliable connection.
次1こ本発明の詳細について述べる。本発明の要点は前
述した集電用端子2のもつ熱容量と極板1の芯材5の有
するそれの違いにもとづく溶接部の熱的アンバランスを
高いエネルギー密度を有する溶接用熱源の使用によって
補償することと、新しい溶接方法の適用蚤こよって、シ
リーズタイプの抵抗溶接特有の溶接電流の分流に関連し
て生じる不都合を排除することにより、すぐれた品質の
溶接部を得ることを可能ならしめる点1こある。Next, details of the present invention will be described. The main point of the present invention is to compensate for the thermal imbalance in the welding zone due to the difference between the heat capacity of the current collecting terminal 2 and that of the core material 5 of the electrode plate 1 by using a welding heat source with high energy density. and the application of the new welding method, thereby making it possible to obtain welds of excellent quality by eliminating the disadvantages associated with the shunting of the welding current peculiar to series type resistance welding. There is one.
即ち溶接用熱源としてレーザ光または電子ビームを使用
する。衆知の如くレーザ光は本質的に位相のそσった波
形を有する極めて性質の良い光であるために、これをレ
ンズあるいは凹面鏡を用いて集光した場合ICは極めて
高い工矛ルギー密度が得られる。電子ビームも同様であ
り真空中でマグネチックレンズにより集束させることに
よって同様な状態を得ることが出来る。That is, a laser beam or an electron beam is used as a heat source for welding. As is well known, laser light is essentially a light with very good properties and has a waveform with a different phase. Therefore, if this laser light is focused using a lens or a concave mirror, an extremely high energy density can be achieved in an IC. It will be done. The same is true for electron beams, and a similar state can be obtained by focusing them with a magnetic lens in a vacuum.
両者とも10’W/c、−m程度のエネルギー密度が得
られるか、この値は例えばアークの108〜4W /d
という値と比べると著しく大きいことが理解できよう。For both, an energy density of about 10'W/c, -m can be obtained, or this value is, for example, 108 to 4 W/d of the arc.
It can be seen that this value is significantly larger than that of .
それ故例えば3000℃以上の融点を有するWの溶解等
にも極めて有効な熱源として利用されている。またいづ
れも極めて小さな直径に絞ることが可能であるため、必
要な場所で、しかも極めて小さな領域だけを所定の温度
まで加熱したいという目的には非常に有効な熱源である
。この様な熱源を使用すれば、芯材5先端部■こ比べ極
めて熱容量の大きな集電用端子2の方も適当な温度に加
熱することが可能であり、しかも芯月5の方も過剰に溶
融させないという、溶接に適したヒートバランスを達成
させることも可能となる。また抵抗溶接の場合1こけ分
流効果によって集電用端子2内部を溶接1こ寄与しない
電流が相当流れるために、溶接とは無関係な場所での異
常な温度上昇か生じ、溶接用電極との溶着が起ったり、
局部的な溶断が生じたりするカーレーザ溶接あるいは電
子ビーム溶接の場合には、微小領域の局部加熱が可能な
ために上述した様な不都合は排除できる。Therefore, it is used as an extremely effective heat source, for example, for melting W, which has a melting point of 3000° C. or higher. In addition, since each type of heat source can be condensed to an extremely small diameter, it is an extremely effective heat source for heating only an extremely small area to a predetermined temperature where necessary. If such a heat source is used, it is possible to heat the current collecting terminal 2, which has an extremely large heat capacity compared to the tip of the core material 5, to an appropriate temperature, and the core material 5 can also be heated to an appropriate temperature. It is also possible to achieve a heat balance suitable for welding that does not cause melting. In addition, in the case of resistance welding, a considerable amount of current that does not contribute to welding flows inside the current collecting terminal 2 due to the shunting effect, which causes an abnormal temperature rise in areas unrelated to welding, which can lead to welding with the welding electrode. happens,
In the case of Kerr laser welding or electron beam welding, in which localized melting occurs, the above-mentioned disadvantages can be eliminated because local heating of minute areas can be performed.
ただしレーザ溶接、電子ビーム溶接ともに問題がないわ
けではない。それは被溶接材料同士の接触の問題である
。すなわち前述した如くし一ザ溶接、電子ビーム溶接等
の高エネルギー密度を有する熱源を使用する場合には、
不必要な場所に熱影響を及ぼさず必要な部分のみを溶接
することになるため1例えば被溶接材料の一部が溶融す
るとしてもその領域は極めてわずかなものとなる。例え
ば被溶接材料間1こすき間があったりすると、それを埋
めつくすだけの溶融金属は存在しないことが多いわけで
ある。それ故この種の溶接方法を採る場合には溶接しよ
うとする場所で被溶接材料同士が緊密な接触状態を呈し
ていることが必要となるわけである。However, both laser welding and electron beam welding are not without problems. It is a problem of contact between the materials to be welded. In other words, as mentioned above, when using a heat source with high energy density such as single welding or electron beam welding,
Since only the necessary parts are welded without exerting a heat influence on unnecessary places, for example, even if a part of the material to be welded melts, the area will be extremely small. For example, if there is a gap between the materials to be welded, there is often not enough molten metal to fill the gap. Therefore, when using this type of welding method, it is necessary that the materials to be welded be in close contact with each other at the location to be welded.
この目的のために通常は抵抗溶接の場合と同じく集電用
端子側に突起部を設ける。もちろん集電用端子が平面状
のものであっても前述した如く集電用端子2と捲回され
た極板芯材5との接触状態が溶接しようとする部分に於
て一様に緊密であればその必要はないが、捲回の精度が
それほど良くない場合が多いため、突起部を設ける方が
賢明である。For this purpose, a protrusion is usually provided on the current collecting terminal side as in the case of resistance welding. Of course, even if the current collecting terminal is planar, as mentioned above, the contact between the current collecting terminal 2 and the wound electrode plate core material 5 is uniformly tight at the part to be welded. Although it is not necessary if there is a protrusion, it is wise to provide a protrusion because the winding accuracy is often not so good.
突起部の形状、寸法等についてはそれなりに検討を要す
ところであるが1例えば第1図に示した如く、集電用端
子2の中心部から放射状に伸びた形のものが溶接のやり
易さから言って最も好ましいと思われる。なぜならば集
電用端子2と極板1の芯材5の先端との接触部すなわち
溶接せんとする部分はこの放射状に伸びた突起部4の中
心部に位置しており、例えば第3図1こ矢印で示した如
く電子ビームあるいはレーザビームを突起部4の中心線
に沿って走査させることにより、突起部4の下にあるす
べての極板芯材5の先端を一度に溶接することが出来る
からである。また放射状に伸びる突起部4の数は。Although the shape and dimensions of the protrusions require some consideration, 1 For example, as shown in Figure 1, it is easier to weld if the protrusions extend radially from the center of the current collecting terminal 2. That seems to be the most preferable option. This is because the contact area between the current collecting terminal 2 and the tip of the core material 5 of the electrode plate 1, that is, the area to be welded, is located at the center of this radially extending protrusion 4. For example, as shown in FIG. By scanning the electron beam or laser beam along the center line of the protrusion 4 as shown by the arrow, the tips of all the electrode plate core materials 5 below the protrusion 4 can be welded at once. It is from. Also, how many protrusions 4 extend radially?
抵抗溶接の場合には溶接電流の分流を極力少な1 (す
るという目的のために制限され、4本程度が限度である
が、レーザ溶接あるいは電子ビーム溶接の場合には特に
限定する必要はない。集電性能から見れば多いほど好ま
しいことは言うまでもないが、この本数は要求される溶
接強度、製造コスト等を考え合せた上で決定されるもの
である。また突起部先端の鋭さは慎重な検討のもとに決
定されねばならない。当然のことながら溶接時には適当
な治具を用いて集電用端子2を極板芯材先端に加圧接触
せしめてからレーザビーム、電子ビームを照射するわけ
であるが、この時の加圧力は芯材5先端に異常な変形を
生じさせない程度のものでなければならない。我々の検
討結果によれば5〜6−以上の圧力をかけることは適当
ではない。そして5〜6〜の圧力下に於て突起部4の先
端が、その下に位置するすべての芯材5先端tこ適度t
こくい込み、両者が緊密な接触状態を呈するためには、
芯材5先端が形成する凹凸が±O1〜0.2朋以下の場
合。In the case of resistance welding, the number of branches of welding current is limited to as little as possible (1), and the limit is about four, but in the case of laser welding or electron beam welding, there is no need to limit it in particular. It goes without saying that more is better in terms of current collection performance, but this number is determined after considering the required welding strength, manufacturing cost, etc. Also, the sharpness of the tip of the protrusion must be carefully considered. Naturally, during welding, the current collector terminal 2 is pressed into contact with the tip of the electrode plate core material using an appropriate jig, and then the laser beam or electron beam is irradiated. However, the pressing force at this time must be such that it does not cause abnormal deformation to the tip of the core material 5. According to our study results, it is not appropriate to apply a pressure of 5 to 6 or more. Then, under a pressure of
In order for the two to be in close contact,
When the unevenness formed by the tip of the core material 5 is ±01 to 0.2 mm or less.
前記突起部4先端のなす角度(第3図のα)は90°以
下であることが必要であることが明らかになっている。It has become clear that the angle formed by the tip of the projection 4 (α in FIG. 3) needs to be 90° or less.
次に本発明の実施例について説明する。Hr−cd 電
池用極板lと集電用端子2との接続に関し、本発明によ
る方法で溶接した場合と従来の抵抗溶接法で溶接した場
合につき溶接状態を比較した。比較実験に使用した極板
はいづれの場合にも同一のものを使用したが、芯材2は
厚さ80μmのFe製のもので表面に7〜8μmのNi
めっきを施したものである。なお極板1の捲回数は6タ
ーンである。次に集電用端子2であるが1本発明による
溶接方法と従来法とでは突起部4の寸法、形状、本数と
に違いがあるがその他は同一とした。すなわち材質はC
景0.12%の圧延鋼板に4〜5μmのNi めっきを
施したものであり、円形部の外径は19朋、また集電部
7の寸法は幅81nm 、長さ13朋、そして肉厚は0
2關である。Next, examples of the present invention will be described. With regard to the connection between the Hr-cd battery electrode plate 1 and the current collector terminal 2, welding conditions were compared between welding by the method according to the present invention and welding by the conventional resistance welding method. The same electrode plate was used in each case for the comparative experiments, but the core material 2 was made of Fe with a thickness of 80 μm, and the surface was coated with 7 to 8 μm of Ni.
It is plated. Note that the number of turns of the electrode plate 1 is 6 turns. Next, regarding the current collecting terminal 2, there are differences in the dimensions, shape, and number of protrusions 4 between the welding method according to the present invention and the conventional method, but other aspects are the same. In other words, the material is C
The outer diameter of the circular part is 19 mm, and the dimensions of the current collecting part 7 are 81 nm wide, 13 mm long, and thick. is 0
There are two issues.
円板部に設けた突起部4はいづれの場合にも中心から外
周部に向って放射状に伸びるもの(第1図、第3図参照
)としたが、その本数は従来法の場合4本(これは抵抗
溶接時の分流効果を最少限に(いとめる上で最も有利な
本数であることを確認した上で決定)、本発明1こよる
方法では6本とした。また突起部4の先端の角度は従来
法1本発明による方法いづれの場合Iこも75°である
。In each case, the projections 4 provided on the disc part were designed to extend radially from the center toward the outer periphery (see Figures 1 and 3), but the number of projections 4 was 4 in the conventional method (see Figures 1 and 3). In order to minimize the shunt effect during resistance welding (determined after confirming that this is the most advantageous number for stopping the welding), this number was set at 6 in the method according to the present invention 1. Also, the tip of the protrusion 4 The angle I is 75° in both the conventional method and the method according to the present invention.
次に溶接条件であるが、従来法の場合1こはコンデンサ
放電形の溶接電源を用い、電極はψ5.0闘のCr−C
u製のものを使用、電極間隔(中心間距離11L4mm
、電極加圧力50即、溶接エネルギー180W8で溶接
した。本発明による方法の場合にはレーザ溶接を適用し
た。光源はCO,ガスレーザを使用しビーム径をy30
.5 mmとし、溶接エネルギー50 Jouleで突
起部4の中心部を集電用端子2の中央から外周へ向って
ビームを。Next, regarding the welding conditions, in the case of the conventional method, a capacitor discharge type welding power source is used, and the electrode is Cr-C with a diameter of ψ5.0.
Use one manufactured by u, electrode spacing (center distance 11L4mm)
Welding was carried out using an electrode pressure of 50 and a welding energy of 180 W8. In the case of the method according to the invention laser welding was applied. The light source is CO, gas laser is used, and the beam diameter is y30.
.. 5 mm, and a beam was applied to the center of the protrusion 4 from the center of the current collecting terminal 2 toward the outer periphery using welding energy of 50 Joule.
スキャンさせて溶接した。I scanned it and welded it.
この様にして溶接したサンプルを各々50ケづつ製作し
、集電部7を垂直に折曲げてこの部分をつかみ引、Lげ
る方法によって集電用端子2を剥離さぜるのに要する最
大荷重を測定して、両心接方法の優劣を比較した。その
結果を第1表に示す。この結果より明らかな如(1本発
明1こよる方法を用いれば溶接強度そのものが大幅會こ
上昇するとともに量産品として最も重要視しなければな
らないバラツキが小さくなり極めて信頼性が向上してい
る。Fifty samples were each made by welding in this manner, and the current collecting terminal 2 was peeled off by bending the current collecting part 7 vertically, grasping this part, and pulling it. The load was measured and the superiority and inferiority of the two-center contact method was compared. The results are shown in Table 1. As is clear from the results (1) If the method according to the present invention is used, the welding strength itself is greatly increased, and the variation, which is the most important thing for mass-produced products, is reduced, and reliability is extremely improved.
第 1 表
なお本文においては電子ビーム溶接についての実験結果
を記さながったが、同様な比較実験を行なったところ、
はぼレーザ溶接と同様な結果となったことを付記してお
く。Table 1 Although the experimental results for electron beam welding are not listed in the main text, we conducted a similar comparative experiment and found that
It should be noted that the results were similar to those of Habo laser welding.
以上のように本発明によれば、多点集電方式の電池にお
いて、集電用端子と極板端部との溶接強度か大幅1こ向
上すると共にそのバラツキも小さく (it頼性が向上
する等工業的価値大である。As described above, according to the present invention, in a multi-point current collection type battery, the welding strength between the current collection terminal and the electrode plate end is significantly improved by one point, and the variation is also small (IT reliability is improved). It has great industrial value.
第1図は多点集電方式を採用したN1−cd電池1こ於
ける集電用端子と極板との接続状態を示す要部斜視図、
第2図は第1図の一部拡大の詳細説明図、第3図は本発
明の実施例の集電用端子と極板との接続方法に於て用い
る集電用端子形状の一例を示した図で、(a)は上面図
、(b)は側面図、(clは(blにおけるA部拡大図
である。
1は極板、2は集電用端子、3は極板端部。
4は突起部、5は芯材
第1図
第3図FIG. 1 is a perspective view of the main parts showing the connection state between the current collecting terminal and the electrode plate in one N1-CD battery that adopts the multi-point current collecting system.
Fig. 2 is a detailed explanatory diagram of a partially enlarged view of Fig. 1, and Fig. 3 shows an example of the shape of the current collecting terminal used in the method of connecting the current collecting terminal and the electrode plate according to the embodiment of the present invention. In the figures, (a) is a top view, (b) is a side view, and (cl is an enlarged view of part A in (bl). 1 is an electrode plate, 2 is a current collecting terminal, and 3 is an end of the electrode plate. 4 is the protrusion, 5 is the core material (Figure 1, Figure 3)
Claims (1)
用端子と極板端部とを複数の点に於て電気的Iこ接続す
る。多点集電方式の電池に於て。 前記集電用端子にその中央部から外周部に放射状に伸び
、その先端角が90°以下である連続した突起部を設け
、該突起部先端と極板の構成材料である極板端部に露出
している芯材先端とを緊密に接触させた後、前記突起部
の中心部にレーザなビームあるいは電子ビームを照射す
ることにより、集電用端子と極板とを接続することを特
徴とする集電用端子の溶接方法。[Scope of Claims] The end portion 1ζ of the wound electrode plate is brought into contact with the current collecting terminal, and the current collecting terminal and the end portion of the electrode plate are electrically connected at a plurality of points. In batteries with multi-point current collection system. The current collecting terminal is provided with a continuous projection extending radially from the center to the outer periphery and having a tip angle of 90° or less, and the tip of the projection and the end of the electrode plate that is the constituent material of the electrode plate are provided. The current collecting terminal and the electrode plate are connected by bringing the exposed tip of the core material into close contact and then irradiating the center of the protrusion with a laser beam or an electron beam. Welding method for current collector terminals.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP58113306A JPS607058A (en) | 1983-06-23 | 1983-06-23 | Method of welding terminal for current collection |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP58113306A JPS607058A (en) | 1983-06-23 | 1983-06-23 | Method of welding terminal for current collection |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS607058A true JPS607058A (en) | 1985-01-14 |
| JPH024102B2 JPH024102B2 (en) | 1990-01-26 |
Family
ID=14608886
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP58113306A Granted JPS607058A (en) | 1983-06-23 | 1983-06-23 | Method of welding terminal for current collection |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS607058A (en) |
Cited By (9)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| EP0769211A4 (en) * | 1994-07-06 | 2000-02-16 | Elmer Hughett | Small battery cell |
| EP1076371A1 (en) * | 1999-08-10 | 2001-02-14 | Sanyo Electric Co., Ltd. | Nonaqueous electrolyte secondary cells and process for fabricating same |
| JP2001297746A (en) * | 2000-04-12 | 2001-10-26 | Matsushita Electric Ind Co Ltd | Method for manufacturing prismatic alkaline storage battery |
| EP1109238A3 (en) * | 1999-12-14 | 2003-05-28 | Matsushita Electric Industrial Co., Ltd. | Battery manufacturing method and apparatus |
| EP1087451A3 (en) * | 1999-09-21 | 2003-07-23 | Matsushita Electric Industrial Co., Ltd. | Electrode plate unit for rechargeable battery and manufacturing method thereof |
| KR100578800B1 (en) * | 2004-02-16 | 2006-05-11 | 삼성에스디아이 주식회사 | Secondary battery |
| EP1484808A4 (en) * | 2002-03-13 | 2006-05-17 | Sanyo Electric Co | Secondary battery |
| EP1983595A1 (en) * | 2007-04-11 | 2008-10-22 | Saft Groupe Sa | Connection system for an electrochemical cell |
| JP2024505869A (en) * | 2021-10-22 | 2024-02-08 | エルジー エナジー ソリューション リミテッド | Cylindrical batteries, battery packs containing them, and automobiles |
-
1983
- 1983-06-23 JP JP58113306A patent/JPS607058A/en active Granted
Cited By (18)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| EP0769211A4 (en) * | 1994-07-06 | 2000-02-16 | Elmer Hughett | Small battery cell |
| EP1076371A1 (en) * | 1999-08-10 | 2001-02-14 | Sanyo Electric Co., Ltd. | Nonaqueous electrolyte secondary cells and process for fabricating same |
| KR100754705B1 (en) * | 1999-08-10 | 2007-09-03 | 산요덴키가부시키가이샤 | Non-water electrolyte secondary battery |
| KR100675700B1 (en) * | 1999-08-10 | 2007-02-01 | 산요덴키가부시키가이샤 | Non-aqueous electrolyte secondary battery and manufacturing method thereof |
| US6995333B2 (en) | 1999-08-10 | 2006-02-07 | Sanyo Electric Co., Ltd. | Process for fabricating nonaqueous electrolyte secondary cells |
| US6692863B1 (en) | 1999-08-10 | 2004-02-17 | Sanyo Electric Co., Ltd. | Nonaqueous electrolyte secondary cells and process for fabricating same |
| US6730438B2 (en) | 1999-08-10 | 2004-05-04 | Sanyo Electric Co., Ltd. | Nonaqueous electrolyte secondary cells and process for fabricating same |
| US6899973B2 (en) | 1999-08-10 | 2005-05-31 | Sanyo Electric Co., Ltd. | Nonaqueous electrolyte secondary cells |
| US6761993B1 (en) | 1999-09-21 | 2004-07-13 | Matsushita Electric Industrial Co., Ltd. | Electrode plate unit for rechargeable battery and manufacturing method thereof |
| EP1087451A3 (en) * | 1999-09-21 | 2003-07-23 | Matsushita Electric Industrial Co., Ltd. | Electrode plate unit for rechargeable battery and manufacturing method thereof |
| US6746494B2 (en) | 1999-12-14 | 2004-06-08 | Matsushita Electric Industrial Co., Ltd. | Battery manufacturing method and apparatus |
| EP1109238A3 (en) * | 1999-12-14 | 2003-05-28 | Matsushita Electric Industrial Co., Ltd. | Battery manufacturing method and apparatus |
| JP2001297746A (en) * | 2000-04-12 | 2001-10-26 | Matsushita Electric Ind Co Ltd | Method for manufacturing prismatic alkaline storage battery |
| EP1484808A4 (en) * | 2002-03-13 | 2006-05-17 | Sanyo Electric Co | Secondary battery |
| US7273678B2 (en) | 2002-03-13 | 2007-09-25 | Sanyo Electric Co., Ltd. | Secondary cell |
| KR100578800B1 (en) * | 2004-02-16 | 2006-05-11 | 삼성에스디아이 주식회사 | Secondary battery |
| EP1983595A1 (en) * | 2007-04-11 | 2008-10-22 | Saft Groupe Sa | Connection system for an electrochemical cell |
| JP2024505869A (en) * | 2021-10-22 | 2024-02-08 | エルジー エナジー ソリューション リミテッド | Cylindrical batteries, battery packs containing them, and automobiles |
Also Published As
| Publication number | Publication date |
|---|---|
| JPH024102B2 (en) | 1990-01-26 |
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