JPS6255730B2 - - Google Patents
Info
- Publication number
- JPS6255730B2 JPS6255730B2 JP55074955A JP7495580A JPS6255730B2 JP S6255730 B2 JPS6255730 B2 JP S6255730B2 JP 55074955 A JP55074955 A JP 55074955A JP 7495580 A JP7495580 A JP 7495580A JP S6255730 B2 JPS6255730 B2 JP S6255730B2
- Authority
- JP
- Japan
- Prior art keywords
- current
- main thyristor
- circuit
- diode
- linear resistor
- 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
Links
- 239000004020 conductor Substances 0.000 claims description 6
- 229910000859 α-Fe Inorganic materials 0.000 claims description 2
- 238000011084 recovery Methods 0.000 description 9
- 238000010586 diagram Methods 0.000 description 6
- XLOMVQKBTHCTTD-UHFFFAOYSA-N Zinc monoxide Chemical compound [Zn]=O XLOMVQKBTHCTTD-UHFFFAOYSA-N 0.000 description 4
- 238000009825 accumulation Methods 0.000 description 3
- 239000003990 capacitor Substances 0.000 description 3
- 230000000694 effects Effects 0.000 description 3
- 229920006395 saturated elastomer Polymers 0.000 description 3
- 239000004065 semiconductor Substances 0.000 description 3
- 239000000919 ceramic Substances 0.000 description 2
- 238000000034 method Methods 0.000 description 2
- 239000011787 zinc oxide Substances 0.000 description 2
- 229910000976 Electrical steel Inorganic materials 0.000 description 1
- 238000010521 absorption reaction Methods 0.000 description 1
- 230000003292 diminished effect Effects 0.000 description 1
- 230000001052 transient effect Effects 0.000 description 1
- 238000004804 winding Methods 0.000 description 1
Classifications
-
- H—ELECTRICITY
- H03—ELECTRONIC CIRCUITRY
- H03K—PULSE TECHNIQUE
- H03K17/00—Electronic switching or gating, i.e. not by contact-making and –breaking
- H03K17/16—Modifications for eliminating interference voltages or currents
Landscapes
- Thyristor Switches And Gates (AREA)
Description
【発明の詳細な説明】
本発明は、半導体整流素子及びその転流回路を
有する直流しや断装置に係り、特に直流回路に存
在するインダクタンスの蓄積エネルギを非直線抵
抗体で消費させる様にした直流しや断装置に関す
る。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a DC/disconnection device having a semiconductor rectifying element and its commutation circuit, and in particular to a DC circuit in which the stored energy of inductance present in the DC circuit is consumed by a non-linear resistor. Regarding DC current and disconnection devices.
第1図に示す様に、例えば電鉄変電所等の直流
き電線保護用の直流しや断装置1は、主サイリス
タ11とこれらの電流零点を作るコンデンサ12
a,リアクトル12b、補助サイリスタ12cの
直列回路より成る転流回路12と主サイリスタ1
1と逆並列接続されたダイオード13及び直流回
路のインダクタンスに蓄積されたエネルギを消費
し、直流電流の限流しや断をすみやかに行う為の
非直線抵抗体14で構成されている。 As shown in FIG. 1, a DC/disconnection device 1 for protecting DC feeder lines at, for example, electric railway substations, includes a main thyristor 11 and a capacitor 12 that creates a current zero point for these.
A, a commutation circuit 12 consisting of a series circuit of a reactor 12b, and an auxiliary thyristor 12c, and a main thyristor 1
1, a diode 13 connected in antiparallel to the DC circuit, and a non-linear resistor 14 that consumes the energy stored in the inductance of the DC circuit and quickly limits or cuts off the DC current.
この様な直流しや断装置1に使用される非直線
抵抗体14としては、酸化亜鉛セラミツクスが用
いられており、これの電気的等価回路は、第2図
に示す様に非直線抵抗体14aと静電容量14b
の並列回路で表わされる。 Zinc oxide ceramics are used as the non-linear resistor 14 used in such a DC/disconnection device 1, and the electrical equivalent circuit of this is shown in FIG. and capacitance 14b
is represented by a parallel circuit.
ところが一般に直流しや断装置1に課せられ
る、しや断時の吸収エネルギは極めて大きく、こ
の為には酸化亜鉛セラミツクスの大容量(大口
径)のものを多数並列接続して非直線抵抗体14
全体を構成しなければならない。従つて非直線抵
抗体14の等価静電容量14bはかなり大きくな
る(例えば0.2μF程度)。 However, in general, the absorption energy imposed on the direct current or disconnection device 1 at the time of shear disconnection is extremely large, and for this purpose, a large number of large capacity (large diameter) zinc oxide ceramics are connected in parallel to form a nonlinear resistor 14.
must form a whole. Therefore, the equivalent capacitance 14b of the nonlinear resistor 14 becomes considerably large (for example, about 0.2 μF).
上記の様に、主サイリスタ11に直接並列に静
電容量が存在すると、主サイリスタ11のター
ン・オンdi/dt(電流上昇率)耐量の面で問題を
生じる。従つて第3図に示す様にリアクトル15
で非直線抵抗体14の等価静電容量14bより突
入する電流上昇率を低減させる方法も考えられる
が下記の不具合が生じる。第4図の動作説明図に
於て主サイリスタ11の電流20のオフ後t1に続
いて起こるダイオード13の電流21オフ時t2
に、このダイオード13のキヤリア蓄積効果によ
り主サイリスタ11のターン・オン時順方向回復
電圧22にV22のヒゲ状の電圧が発生する。この
順方向回復電圧V22は第4図に示す様に、コンデ
ンサの反転電圧をVC、転流回路のリアクトル1
2b等でなる等価インダクタンスをL、ダイオー
ドの回復電流の電流上昇率による転回路の電流変
化率をdi/dtとすれば、V22=VC+Ldi/dtと表わ
さ
れ、Ldi/dtに依存したひげ状の大きな電圧が生じ
る。この順方向回復電圧V22は、主サイリスタ1
1と直接並列に非直線抵抗体14が接続されてい
れば、この制限電圧を越えることはない、しかし
第3図の回路では、リアクトル15により、前記
順方向回復電圧V22を非直線抵抗体14で制限す
る能力は薄れてしまう。言い換えれば、非直線抵
抗体14の制限電圧を下げる必要が生じ、直流限
流しや断能力を低下させ、非直線抵抗体のストレ
スをも増加させてしまう。 As described above, if a capacitance exists directly in parallel with the main thyristor 11, a problem arises in terms of the turn-on di/dt (current rise rate) withstand capability of the main thyristor 11. Therefore, as shown in Fig. 3, the reactor 15
A method of reducing the rate of increase in the current flowing in from the equivalent capacitance 14b of the non-linear resistor 14 can also be considered, but the following problems occur. In the operation explanatory diagram of FIG. 4, the current 21 of the diode 13 is turned off at t 2 following t 1 after the current 20 of the main thyristor 11 is turned off.
Furthermore, due to the carrier accumulation effect of the diode 13, a whisker-like voltage of V22 is generated in the forward recovery voltage 22 when the main thyristor 11 is turned on. As shown in Fig. 4, this forward recovery voltage V 22 is determined by the inversion voltage of the capacitor V C and the reactor 1 of the commutation circuit.
If L is the equivalent inductance of 2b, etc., and di/dt is the current change rate of the switching circuit due to the current increase rate of the recovery current of the diode, then it is expressed as V 22 = V C + Ldi/dt, and it depends on Ldi/dt. A large whisker-like voltage is generated. This forward recovery voltage V 22 is the main thyristor 1
If a non-linear resistor 14 is connected directly in parallel with the non-linear resistor 1, this limit voltage will not be exceeded.However, in the circuit of FIG . The ability to limit at 14 is diminished. In other words, it becomes necessary to lower the limiting voltage of the non-linear resistor 14, which reduces DC current limiting and breaking ability, and increases stress on the non-linear resistor.
本発明の目的は上記の事情に鑑みてなされたも
ので、非直線抵抗体14の制限電圧を下げずに、
主サイリスタ11のターン・オンdi/dtを抑制す
ることが出来る直流しや断装置を提供することに
ある。 The object of the present invention has been made in view of the above circumstances, and it is an object of the present invention to
The object of the present invention is to provide a direct current and disconnection device capable of suppressing the turn-on di/dt of the main thyristor 11.
以下本発明の一実施例を第5図に示す直流しや
断装置の概略構成図を参照して説明する。 An embodiment of the present invention will be described below with reference to a schematic diagram of a direct current disconnection device shown in FIG.
図中31aは主サイリスタ11とダイオード1
3及び転流回路12に対する共通接続導体であ
り、該導体31aを例えばフエライトコア或は珪
素鋼板を巻回して成る貫通形コア32aに貫通さ
せて可飽和リアクトルを構成する。 In the figure, 31a is the main thyristor 11 and diode 1.
3 and the commutation circuit 12, and the conductor 31a is passed through a through-type core 32a formed by winding a ferrite core or a silicon steel plate, for example, to constitute a saturable reactor.
この様な構成とすることで、主サイリスタ11
のターン・オン時(しや断器入)の非直線抵抗体
14の静電容量よりの突入電流を小さくしてdi/
dtを抑制し、又、回路電流の領域では該貫通形コ
ア32a及び導体31aからなる可飽和リアクト
ルが飽和する様に選定すると、上記ダイオード1
3のキヤリ蓄積効果による主サイリスタ11のし
や断時順方向回復電圧V22は、非直線抵抗体の制
限電圧以下に挿えることが出来る。 With this configuration, the main thyristor 11
Di/
dt is suppressed and the saturable reactor consisting of the through-type core 32a and the conductor 31a is selected so as to be saturated in the circuit current region, the diode 1
The forward recovery voltage V 22 of the main thyristor 11 due to the carry accumulation effect of No. 3 can be set below the limit voltage of the non-linear resistor.
第6図は、本発明の他の実施例であり、主サイ
リスタ11とダイオード13の共通接続導体31
bを貫通形コア32bに貫通させて可飽和リアク
トルを構成したものである。この構成では、ダイ
オード13の逆回復現象の大半の電流領域で、該
可飽和リアクトルが飽和する様にコアを選定すれ
ば、転流回路電流は安定しているので例えば第5
図の実施例に於て、回路電流が小さい場合でも
(例えば事故時等の大電流しや断でなく、軽負荷
時の小電流しや断時)ダイオード13による順方
向回復電圧V22を適切に抑制でき、主サイリスタ
11のターン・オン時のdi/dtも適切に抑制可能
となる。 FIG. 6 shows another embodiment of the present invention, in which a common connection conductor 31 of the main thyristor 11 and the diode 13 is connected.
b is passed through the through-type core 32b to constitute a saturable reactor. In this configuration, if the core is selected so that the saturable reactor is saturated in most of the current range where the reverse recovery phenomenon occurs in the diode 13, the commutating circuit current is stable.
In the embodiment shown in the figure, even when the circuit current is small (for example, not during a large current interruption during an accident, but during a small current interruption during a light load), the forward recovery voltage V 22 by the diode 13 can be adjusted appropriately. It is also possible to appropriately suppress di/dt when the main thyristor 11 is turned on.
第7図は、本発明の更らに他の実施例であり、
主サイリスタ11の接続導31cとダイオード1
3の接続導体31dとを共通の貫通形コア32c
に対し、図中の如く、主サイリスタ11の順方向
電流経路とダイオード13の順方向電流経路が共
に同一の面より貫通させた構成である。この構成
では、可飽和リアクトルとしての飽和特性は、第
6図の実施例と同じくダイオード13の逆回復電
流領域の大半で飽和する様にしておけば良い。こ
の方式の特徴は、コアのヒステリシス特性より見
ると、ダイオード13の逆回復電流による磁場
が、主サイリスタ11の順方向電流により生じる
磁場とは逆極性(コアがリセツトされる)となる
ので、鉄心の電圧・時間積が大きく取れる利点が
ある。 FIG. 7 shows still another embodiment of the present invention,
Connection conductor 31c of main thyristor 11 and diode 1
A common through-type core 32c with the connection conductor 31d of No. 3
On the other hand, as shown in the figure, the forward current path of the main thyristor 11 and the forward current path of the diode 13 are both penetrated from the same plane. In this configuration, the saturation characteristic as a saturable reactor may be set such that it is saturated in most of the reverse recovery current region of the diode 13, as in the embodiment shown in FIG. The feature of this method is that, from the hysteresis characteristics of the core, the magnetic field caused by the reverse recovery current of the diode 13 has a polarity opposite to the magnetic field generated by the forward current of the main thyristor 11 (the core is reset). It has the advantage of being able to obtain a large voltage/time product.
以上述べた様に、非直線抵抗体を用いた半導体
直流しや断器に於て、本発明の如く可飽和リアク
トルを用いることで、非直流抵抗体の静電容量か
らの流入による主サイリスタ11の電流上昇率
di/dtが抑制出来、又適切な飽和特性を選択する
ことで半導体キヤリア蓄積効果に起因する過渡的
過電圧を、適切な値以下に抑制出来るので直流電
流の限流しやがよりすみやかとなるなど有利な点
が多い。 As described above, by using a saturable reactor as in the present invention in a semiconductor DC circuit or a circuit breaker using a non-linear resistor, the main thyristor 11 due to the inflow from the capacitance of the non-DC resistor. current increase rate of
di/dt can be suppressed, and by selecting appropriate saturation characteristics, transient overvoltage caused by semiconductor carrier accumulation effect can be suppressed to below an appropriate value, which is advantageous in that DC current can be more quickly limited. There are many points.
第1図は、非直線抵抗体を用いた直流しや断装
置の原理構成図、第2図は非直線抵抗体の電気的
等価回路、第3図は、従来装置の構成図、第4図
は直流しや断装置の動作説明図、第5図は本発明
の一実施例を示す概略構成図、第6図乃至第7図
は本発明の他の実施例を示す概略構成図である。
11…主サイリスタ、12a…転流コンデンサ
(充電回路は図示していない)、12b…転流リア
クトル、12c…補助サイリスタ、13…ダイオ
ード、14…非直線抵抗体、32a〜c…貫通形
コア。
Fig. 1 is a principle block diagram of a direct current and disconnection device using a non-linear resistor, Fig. 2 is an electrical equivalent circuit of a non-linear resistor, Fig. 3 is a block diagram of a conventional device, and Fig. 4 FIG. 5 is a schematic diagram showing one embodiment of the present invention, and FIGS. 6 to 7 are schematic diagrams showing other embodiments of the present invention. DESCRIPTION OF SYMBOLS 11... Main thyristor, 12a... Commutation capacitor (charging circuit not shown), 12b... Commutation reactor, 12c... Auxiliary thyristor, 13... Diode, 14... Non-linear resistor, 32a-c... Through-hole core.
Claims (1)
と、前記主サイリスタに並列接続される転流回路
及び非直線抵抗体から成る直流しや断装置におい
て、前記主サイリスタと非直線抵抗体との並列回
路内で且つ前記主サイリスタに直列にフエライト
コア等の貫通形コアに導体を貫通させて成る可飽
和リアクトルを接続したことを特徴とする直流し
や断装置。1. In a direct current or disconnection device consisting of a diode connected in anti-parallel to the main thyristor, a commutation circuit and a non-linear resistor connected in parallel to the main thyristor, in a parallel circuit between the main thyristor and the non-linear resistor. A direct current or disconnection device characterized in that a saturable reactor formed by passing a conductor through a through-type core such as a ferrite core is connected in series to the main thyristor.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP7495580A JPS572125A (en) | 1980-06-05 | 1980-06-05 | Direct current breaking device |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP7495580A JPS572125A (en) | 1980-06-05 | 1980-06-05 | Direct current breaking device |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS572125A JPS572125A (en) | 1982-01-07 |
| JPS6255730B2 true JPS6255730B2 (en) | 1987-11-20 |
Family
ID=13562245
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP7495580A Granted JPS572125A (en) | 1980-06-05 | 1980-06-05 | Direct current breaking device |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS572125A (en) |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS6173819A (en) * | 1984-09-17 | 1986-04-16 | Ito Seitetsushiyo:Kk | Soaking treatment device for cold billet and hot billet |
-
1980
- 1980-06-05 JP JP7495580A patent/JPS572125A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS572125A (en) | 1982-01-07 |
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