JP5229646B2 - Current fuse - Google Patents
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- JP5229646B2 JP5229646B2 JP2011035143A JP2011035143A JP5229646B2 JP 5229646 B2 JP5229646 B2 JP 5229646B2 JP 2011035143 A JP2011035143 A JP 2011035143A JP 2011035143 A JP2011035143 A JP 2011035143A JP 5229646 B2 JP5229646 B2 JP 5229646B2
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Description
本発明は電気部品の電流ヒューズに関するものである。The present invention relates to a current fuse for an electrical component.
電流ヒューズが過電流を爆発的に遮断する際に発生する衝撃波をヒューズの容器内で反射・収束させてヒューズ線上に焦点を結ばせ、衝撃波が起こす気圧上昇によりアーク発生を抑制し電流を安定的に遮断する衝撃波活用のヒューズは特許文献1)にて公知であるが、衝撃波は持続時間が短いためアーク抑制に必要な気圧上昇状態が持続せず安定した遮断が得られない場合がある。The shock wave generated when the current fuse explosively interrupts the overcurrent is reflected and converged in the fuse container to focus on the fuse wire, and the arc generation is suppressed by the pressure rise caused by the shock wave, and the current is stabilized. A shock wave-utilizing fuse that is interrupted in a short time is known in Patent Document 1). However, since the shock wave has a short duration, there is a case where the atmospheric pressure increase state necessary for arc suppression does not continue and a stable interruption may not be obtained.
衝撃波をヒューズ線上に反射収束させて衝撃波が発生する気圧上昇状態の持続時間を引延ばしアーク発生の抑制に必要十分な時間を得ることを課題とする。It is an object of the present invention to obtain a sufficient time necessary for suppressing the occurrence of arc by extending the duration of the atmospheric pressure rise state in which the shock wave is generated by reflecting and converging the shock wave on the fuse wire.
過大電流により爆発的にヒューズ線が溶融・気化して衝撃波が発生しこれを未溶融の残余ヒューズ線の上を狙って反射収束すると衝撃波に伴う気圧上昇により、アーク発生の電圧条件を高くさせるのでアーク発生を未然に抑制するのが衝撃波活用ヒューズの基本概念である。遮断時にアーク発生が起こるか、あるいは抑制できるかはヒューズの印加電圧とヒューズ線周りの雰囲気の気圧とによって判断できることがパッシェンの法則(非特許文献1)から導かれる。As the fuse wire explosively melts and vaporizes due to an excessive current, a shock wave is generated and reflected on the unfused residual fuse wire to converge and increase the pressure condition due to the shock wave, increasing the voltage condition for arc generation. The basic concept of a shock wave-utilizing fuse is to suppress arc generation. It is derived from Paschen's law (Non-Patent Document 1) that whether arc generation occurs or can be suppressed at the time of interruption can be determined by the applied voltage of the fuse and the atmospheric pressure around the fuse wire.
これは遮断電流が極めて短時間の場合、また比較的小型のヒューズにおいては正確に具現化する。
しかしながらヒューズが大型となる場合は必ずしも効果的に作用しない。This is precisely realized when the interrupting current is very short and in relatively small fuses.
However, it does not always work effectively when the fuse is large.
ヒューズ両端の電圧・電流によりオシロスコープにて遮断動作を観察すると過大電流の印加直後に一旦、電流が遮断されるように低下するが電流は再び増加しアークが発生して遮断が失敗する。(図1)When observing the breaking operation with an oscilloscope by the voltage and current across the fuse, the current once drops to be cut off immediately after the application of the excessive current, but the current increases again and an arc is generated and the breaking fails. (Figure 1)
過大電流による衝撃波と圧力増加の測定結果を図2(非特許文献2)に示す。
この測定例では、衝撃波による圧力増加は20〜30気圧に達しており、パッシェンの法則(非特許文献1)によるアーク発生電圧を大きく上回るのでどのヒューズにもアーク発生はないはずである。
しかし同図から明らかなように衝撃波の持続時間は長くても200ナノ秒(−0.000002秒)である。
同図は開放空間の測定結果であるので包装ヒューズの場合はこれより長く持続するとみられるが、その場合においても気圧は瞬時に上昇した後に比較的速やかにヒューズ容器全体に拡散するものと見られる。FIG. 2 (Non-Patent Document 2) shows the measurement results of shock wave and pressure increase due to excessive current.
In this measurement example, the pressure increase due to the shock wave has reached 20 to 30 atmospheres, and since the arc generation voltage according to Paschen's law (Non-patent Document 1) is greatly exceeded, no arc should occur in any fuse.
However, as is clear from the figure, the duration of the shock wave is at most 200 nanoseconds (-0.000002 seconds).
Since this figure is a measurement result of open space, it seems that it will last longer than this in the case of a packaged fuse, but even in that case, it seems that the air pressure rises instantaneously and then diffuses to the entire fuse container relatively quickly .
ヒューズが小型の場合はこれでも満足な結果が得られるが、常用のヒューズにおいては遮断に要する時間が、0.001秒〜0.010秒であるため衝撃波による電流遮断に必要な圧力の持続時間が若干不足するという課題がある。Satisfactory results can be obtained even if the fuse is small, but the duration of the pressure required to cut off the current due to the shock wave is low because the time required to cut off the normal fuse is 0.001 to 0.010 seconds. There is a problem that is slightly lacking.
ヒューズ線が爆発的に溶融・気化した時に発生した衝撃波をヒューズ容器の凹球面内壁で反射し焦点に収束させる段階までは、特許文献(1)に準ずるが本発明では焦点近傍の内壁に細孔を設けて収束によりエネルギー密度の高くなった衝撃波を細孔を通して封止した小空間に導くところに特徴がある。The process up to the stage where the shock wave generated when the fuse wire is explosively melted and vaporized is reflected by the concave spherical inner wall of the fuse container and converged to the focal point is in accordance with Patent Document (1). It is characterized in that a shock wave whose energy density is increased by convergence is guided to a small space sealed through the pores.
まず、衝撃波の細孔を通り抜けに関して(非特許文献2)によれば衝撃波が細孔を抜けるプロセスが解明されている。(図3)First, according to the shock wave passing through the pore (Non-Patent Document 2), the process by which the shock wave passes through the pore is elucidated. (Figure 3)
つぎに当該細孔以外は閉じられた小空間において、衝撃波はエネルギー保存則によってその運動エネルギーがすべて圧力のエネルギーになり、小空間の気圧が上昇する。これは衝撃波の状態方程式(ランキン・ユゴニオの状態方程式)の展開による。(非特許文献3)Next, in a small space closed except for the pores, the kinetic energy of the shock wave becomes the energy of pressure by the energy conservation law, and the atmospheric pressure in the small space rises. This is due to the development of the shock wave equation of state (Rankin Yugonio's equation of state). (Non Patent Literature 3)
小空間にはヒューズ線の未溶解残存部分が位置しておりパッシェンの法則がこの場所で適用され、上昇した気圧雰囲気により発弧が抑制される。
衝撃波が進入した細孔から上昇した圧力が漏れ終わるまで若干時間が掛かるので、その間に遮断動作が終了する。An undissolved remaining portion of the fuse wire is located in the small space, and Paschen's law is applied at this location, and the arc is suppressed by the increased atmospheric pressure.
Since it takes some time until the pressure that has risen from the pores into which the shock wave has entered leaks, the blocking operation is completed during that time.
図4に実施例1を示す。ヒューズの楕円凹曲面壁にヒューズ線を通す細孔の断面積を拡げることにより衝撃波の通路を確保し、これを隣接する小空間に連通させる衝撃波活用ヒューズを示す。
図6に本発明品の遮断試験の結果を示す。Example 1 is shown in FIG. A shock wave-use fuse that secures a shock wave path by expanding the cross-sectional area of the hole through which the fuse wire passes on the elliptical concave curved wall of the fuse and communicates it with the adjacent small space is shown.
FIG. 6 shows the result of the blocking test of the product of the present invention.
図4の実施例におけるヒューズ線の経路と共用の連通路に加えてヒューズの楕円凹曲面壁に別途細孔を穿って衝撃波の通路を確保し、隣接する小室に連通させる衝撃波活用ヒューズを図5に示す。
これは実施例1において溶融したヒューズ線がヒューズ線の細孔を塞いだ場合においても衝撃波の通路を確保するためである。In addition to the communication path shared with the fuse wire path in the embodiment of FIG. 4, a shock wave-utilizing fuse that secures a shock wave path by making a separate hole in the elliptical concave curved wall of the fuse and communicates with an adjacent small chamber is shown in FIG. Shown in
This is to secure a shock wave path even when the fused fuse wire in Example 1 blocks the pores of the fuse wire.
1 絶縁部材
2 通電部材
3 ヒューズ線
4 反射凹曲面
5 衝撃波の収束焦点
6 はんだ
7 連通経路
8 小空間
9 追加の連通経路DESCRIPTION OF SYMBOLS 1 Insulation member 2 Current supply member 3 Fuse wire 4 Reflective concave curved surface 5 Convergence focal point 6 of shock wave Solder 7 Communication path 8 Small space 9 Additional communication path
本発明によるヒューズの消弧技術は消弧砂を構成要件としないので設置場所の振動のため消弧砂によるヒューズ線の摩耗劣化などが懸念されるヒューズに適する。また消弧砂を構成要件としないので遮断電流が定格電流の2倍程度の比較的軽度の過電流の場合に再発弧の懸念なく確実な遮断が可能である。Since the arc extinguishing technique of the fuse according to the present invention does not include arc extinguishing sand, it is suitable for a fuse in which the wear deterioration of the fuse wire due to the arc extinguishing sand is concerned due to vibration of the installation place. Moreover, since arc-extinguishing sand is not a constituent requirement, when the breaking current is a relatively light overcurrent that is about twice the rated current, reliable breaking can be achieved without concern about re-arcing.
Claims (1)
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JP2011035143A JP5229646B2 (en) | 2011-02-03 | 2011-02-03 | Current fuse |
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JP2011035143A JP5229646B2 (en) | 2011-02-03 | 2011-02-03 | Current fuse |
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JP2012164619A JP2012164619A (en) | 2012-08-30 |
JP5229646B2 true JP5229646B2 (en) | 2013-07-03 |
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JP2011035143A Expired - Fee Related JP5229646B2 (en) | 2011-02-03 | 2011-02-03 | Current fuse |
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EP3500024A1 (en) | 2012-07-25 | 2019-06-19 | Sun Patent Trust | Base station apparatus, terminal apparatus, transmission method, and reception method |
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US4904977A (en) * | 1988-06-13 | 1990-02-27 | Mahieu William R | Supersonic expulsion fuse |
JP3966114B2 (en) * | 2002-07-01 | 2007-08-29 | 忠司 梅田 | Current fuse |
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