JPS6187301A - Lightning arrestor - Google Patents
Lightning arrestorInfo
- Publication number
- JPS6187301A JPS6187301A JP59208052A JP20805284A JPS6187301A JP S6187301 A JPS6187301 A JP S6187301A JP 59208052 A JP59208052 A JP 59208052A JP 20805284 A JP20805284 A JP 20805284A JP S6187301 A JPS6187301 A JP S6187301A
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- Prior art keywords
- voltage
- lightning arrester
- resistance element
- nonlinear resistance
- ratio
- Prior art date
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Abstract
(57)【要約】本公報は電子出願前の出願データであるた
め要約のデータは記録されません。(57) [Summary] This bulletin contains application data before electronic filing, so abstract data is not recorded.
Description
【発明の詳細な説明】
〔産業上の利用分野〕
この発明は、酸化亜鉛形避雷装置、特にその内謬!(収
容する非直線抵抗素子の配列の仕方に工夫ゲ凝らした避
雷装置に関するものである。[Detailed Description of the Invention] [Industrial Field of Application] This invention relates to a zinc oxide type lightning arrester, especially its inner features! (This relates to a lightning arrester in which the arrangement of the non-linear resistance elements to be accommodated is ingenious.
避雷装置は、1!力系統に発生する異常電圧を抑制し、
系統に接続される各種の被保護機器の絶縁破壊事故を防
止する。一般に避雷装置は、一定の過電圧レベルになれ
ば電流を放電し、また常規の運転電圧などの一定の電圧
レベルでは何ら動作せず、普通の絶縁物に近い特性を示
す。Lightning arrester is 1! suppresses abnormal voltages that occur in power systems,
Prevent insulation breakdown accidents of various protected devices connected to the grid. In general, lightning arresters discharge current when a certain overvoltage level is reached, and do not operate at a certain voltage level such as normal operating voltage, exhibiting characteristics similar to ordinary insulators.
このような避雷装置として、現在、酸化亜鉛形避雷装置
が主流となっており、その代表的な例を説明する。第3
図は碍子形の酸化亜鉛形避雷装置を示す側断面図であり
1図においC(1)は碍管容器であってその両端部にフ
ランジ(2)を有している。Zinc oxide type lightning arresters are currently the mainstream type of lightning arrester, and a typical example thereof will be described. Third
The figure is a side sectional view showing an insulator-shaped zinc oxide type lightning arrester. In figure 1, C (1) is an insulator tube container, which has flanges (2) at both ends.
(3)は酸化亜鉛を主成分とする金属酸化物の焼結体か
ら成る非直線抵抗素子を複数枚(、?/)〜(3n)直
列接続して構成された非直線抵抗素子柱である。(3) is a non-linear resistance element column constructed by connecting in series a plurality of non-linear resistance elements (,?/) to (3n) made of a sintered body of metal oxide whose main component is zinc oxide. .
この非直線抵抗素子柱(3)は、バネ(4’lを介して
密閉用フタCj)にバネ圧で固定される。This non-linear resistance element column (3) is fixed to the sealing lid Cj via a spring (4'l) with spring pressure.
次に動作について説明する。この第3図の避雷装置に雷
サージなどの異常電圧が襲来すると、過電圧に対して非
直線抵抗素子柱(3)は、その抵抗が大幅に小さくなり
、従って密閉用フタ(!r)およびバネ(lI)を介し
てサージ電流を流し、これにより過電圧を固定レベル以
下に抑制する。一方、異常電圧抑制後は、非直1liI
i!抵抗素子柱<3)の抵抗が非常に高くなるため、非
直線抵抗素子柱(3)は普通の絶縁物に近い特性を示す
。このような通常の連続使用電圧に対しては、避雷装置
内部の電圧分担が避雷装置の課電寿命や熱安定性に影響
するようになる。Next, the operation will be explained. When an abnormal voltage such as a lightning surge hits the lightning arrester shown in Fig. 3, the resistance of the non-linear resistance element column (3) becomes significantly smaller against the overvoltage, and the sealing cover (!r) and spring A surge current is caused to flow through (lI), thereby suppressing the overvoltage below a fixed level. On the other hand, after abnormal voltage suppression, non-direct 1liI
i! Since the resistance of the resistive element pillar (<3) becomes very high, the nonlinear resistive element pillar (3) exhibits characteristics close to those of an ordinary insulator. For such normal continuous operating voltages, the voltage distribution within the lightning arrester will affect the energized life and thermal stability of the lightning arrester.
以下、この特性を図を用いて説明する。This characteristic will be explained below using figures.
第7図は、第3図に示した避雷装置の等価回路を示す回
路図で、簡単化のため非直線抵抗素子柱(,7)がダ枚
の非直線抵抗素子(31)〜(,7u)から成る場合を
示す。およびC(3i〜Cef1は各非直線抵抗素子(
3/)、(3,2)、(3コ)、(,71I)のそれぞ
れ非直線抵抗および消電容量であり、 Cst % C
ssは対地浮遊容量である。避雷装置の形状や大きさに
もよるが、概略、系統電圧/JダkV以上のi!雷装置
では、対地浮遊容量Cst −C5Jの並列静電容?値
は各非直線抵抗素子の静電容量Ce1− Ceaの百列
静延答量値より犬きくなる。さらに通常の連続使用電圧
では、各非直線抵抗素子の抵抗よりもその静電容量によ
る容i1Jアクタンスの方が小さく。FIG. 7 is a circuit diagram showing an equivalent circuit of the lightning arrester shown in FIG. ). and C (3i to Cef1 are each nonlinear resistance element (
Cst % C
ss is the ground floating capacitance. It depends on the shape and size of the lightning arrester, but in general, the i! In lightning equipment, the parallel capacitance of ground stray capacitance Cst - C5J? The value is much greater than the 100 series static response value of the capacitance Ce1-Cea of each non-linear resistance element. Further, at normal continuous operating voltages, the capacitance i1J actance due to the capacitance of each nonlinear resistance element is smaller than the resistance of each nonlinear resistance element.
数%〜約約20程程である。このため1通常の連続使用
電圧では、対地浮遊容量Cst〜Cs、yのV響を父け
、非直線抵抗素子柱3の電圧分担が不平等になる。即ち
、第1I図の等価回路から分るように各非直線抵抗素子
に流れる電流をIel〜Ie<+とすると、高圧側程非
直戯抵抗素子に流れる電流Ieが大きく、それによる電
圧降下も大きくなるためである。It ranges from several percent to about 20 percent. For this reason, at a normal continuous operating voltage, the voltage distribution of the non-linear resistance element pillar 3 becomes unequal due to the V effect of the stray capacitance to ground Cst to Cs,y. That is, as can be seen from the equivalent circuit in Figure 1I, if the current flowing through each non-linear resistance element is Iel~Ie<+, the higher the voltage side, the larger the current Ie flowing through the non-linear resistance element, and the resulting voltage drop will also be This is because it becomes bigger.
第3図(a) 、 (blは、それぞれ第3図:/C示
した辷1装置の非直線抵抗素子柱(1)の電位分布特性
および素子1枚当りの電圧特性を示す。破線は対地浮遊
容量Cst % C5Jがないと仮定したときに得られ
る電圧分担が平等な場合で、連続使用電圧において各非
直線抵抗素子柱加わる電圧は第5図(b)から均等であ
ることが分る。しかし、対地浮遊容量を含めると破線の
カーブはそれぞれ実線の電圧分担不平等のカーブとなり
、@!r図(b)から分るように高圧側の非直線抵抗素
子に他の非直線抵抗素子より大きな電圧が加わるように
なる。Figures 3(a) and (bl respectively show the potential distribution characteristics of the non-linear resistance element column (1) and the voltage characteristics per element of the device shown in Figure 3:/C. Assuming that there is no stray capacitance Cst % C5J, the resulting voltage sharing is equal, and it can be seen from FIG. 5(b) that the voltages applied to each non-linear resistance element column are equal at continuous operating voltages. However, if stray capacitance to ground is included, each broken line curve becomes a solid line curve with unequal voltage distribution, and as shown in @!r figure (b), the nonlinear resistance element on the high voltage side is A large voltage will be applied.
このように、避雷装置の電圧分担が不平等であると、一
部の非直線抵抗素子に設定値以上の電圧が加わるように
なり、この部分の非直線抵抗素子が大きく課電劣化を起
こし、ひいては避雷装置全体の課電寿命を短クシ、熱安
定性を悪化する可能性があった。このため大きな定格の
避雷装置では。In this way, if the voltage distribution of the lightning arrester is unequal, a voltage higher than the set value will be applied to some non-linear resistance elements, causing significant deterioration of the non-linear resistance elements in these parts. In turn, this could shorten the lifespan of the entire lightning arrester and deteriorate its thermal stability. For this reason large rated lightning arresters.
電圧分担均一化のための分圧コンデンサを付加したり、
大形の分圧シールドを必要とするので装置が大形で高価
なものとなる問題点があった。Adding a voltage dividing capacitor to equalize voltage sharing,
Since a large partial pressure shield is required, there is a problem that the device becomes large and expensive.
この発明は、このような問題点を解消するためになされ
たもので、各非直線抵抗素子の電圧分担が均一な避雷装
置を得ることを目的とする。The present invention was made to solve these problems, and an object of the present invention is to obtain a lightning arrester in which each nonlinear resistance element shares a uniform voltage.
この発明に係る避雷装置は、比VNmA/Zcの大きい
非直線抵抗素子を高圧側に配置したものである。The lightning arrester according to the present invention has a non-linear resistance element having a large ratio VNmA/Zc arranged on the high voltage side.
この発明においては、比vNm人/Zcの大きい非直線
抵抗素子を高圧側に配置し、しかも高圧側から接地側に
順番に配列することにより、避雷装置の電圧分担が平等
になる。、
〔実施例〕
以下、この発明の考え方を図面について説明する。第2
図は、各非直線抵抗素子の電圧−電流(V−I)特性を
示す図である。避雷器直列ギャップに対応させるため、
動作開始電圧が設定されており、それは電流NmA (
通常l〜JmAの電流を使用する)での電圧を言う。こ
のV−I特性は。In this invention, by arranging non-linear resistance elements with a large ratio vNm/Zc on the high voltage side and arranging them in order from the high voltage side to the ground side, the voltage distribution of the lightning arrester becomes equal. , [Example] The concept of this invention will be explained below with reference to the drawings. Second
The figure is a diagram showing voltage-current (VI) characteristics of each nonlinear resistance element. In order to correspond to the lightning arrester series gap,
The operation start voltage is set, and it is the current NmA (
Normally, a current of 1 to JmA is used). This VI characteristic is.
広い電流範囲特に珈仏〜/ OKAにお(、・て、電圧
の変化が少ない優れた非直線性を糸しており、この領域
では、非直線抵抗素子を大量に製作した場合でも、はぼ
同一の安定なV−Iカーブが得られる。一方、 NmA
以下の小電流領域のV−I特性は。Wide current range, especially OKA (,・), has excellent nonlinearity with little voltage change, and in this region, even if nonlinear resistance elements are manufactured in large quantities, The same stable V-I curve is obtained.On the other hand, NmA
The following is the V-I characteristic in the small current region.
あまり非直線性を示さず、かつ、素子大iff炸時には
1図中斜線で示すようなバラツキが大きく。It does not show much non-linearity, and when the element size IF bursts, there is a large variation as shown by diagonal lines in Figure 1.
これは同一電圧に対して最大約±2Q%程度もある。This is about ±2Q% at maximum for the same voltage.
一方、非直線抵抗素子の課電寿命は1図中に示した連続
使用電圧と動作開始電圧の比、即ち課電率Pに依存する
。一般に課電率Pが10%増加すると1課電寿命は約1
桁縮まるとされており、避雷装置の電圧分担の不平等性
をなくし平均した一定の課電率で使用することが避雷装
置の寿命を高める方法である。On the other hand, the life of the non-linear resistance element when applied with electricity depends on the ratio of the continuous operating voltage and the operation start voltage shown in FIG. 1, that is, the application rate P. Generally, when the charging rate P increases by 10%, the charging life per charging is approximately 1
It is said that the lifetime of the lightning arrester can be increased by an order of magnitude, and one way to extend the life of the lightning arrester is to eliminate the inequality in the voltage distribution of the lightning arrester and use it at a constant average charge rate.
この発明は、非直線抵抗素子が持っているこのような特
性を利用したものである。先ず、各非直線抵抗素子の動
作開始電圧VNmAを測定する。医用素子数で割った平
均的なもの)で漏れ電流を測定する。そして両者の比か
らインピーダンスZcを求める。このようにして求めた
Zcと上述のVNmAとから更に比−エヌν・を下記の
ようにして求c
める。This invention utilizes such characteristics of non-linear resistance elements. First, the operation start voltage VNmA of each nonlinear resistance element is measured. The average value divided by the number of medical elements) is used to measure leakage current. Then, the impedance Zc is determined from the ratio of the two. From the Zc thus obtained and the VNmA mentioned above, the ratio -Nv.c is further calculated as follows.
ここで、比vxmA/ Zcは、非直線抵抗素子の適用
を決める指標で、大きな値を持つ素子程高課高率の所に
配置するのがこの発明の考え方である。Here, the ratio vxmA/Zc is an index that determines the application of the nonlinear resistance element, and the idea of the present invention is that the element having a larger value is placed at a location with a higher duty ratio.
以下、この比の導出について説明する。動作開始it圧
vNm人、インピーダンスZcの非直線抵抗素子に連続
使用電圧(P X VNz* )を課電したとき。The derivation of this ratio will be explained below. Operation starts when the pressure is vNm and a continuous working voltage (P x VNz *) is applied to the nonlinear resistance element of impedance Zc.
非直線抵抗素子に流れる電流をIeとすると1次式の関
係が成立する。If the current flowing through the non-linear resistance element is Ie, a linear relationship holds true.
Zc
Pを移項すると
Zc
ここで、避雷装置の各非直線抵抗素子の課電率Pを一定
にするためには、P=一定とおいて0次式を成立させる
必要がある。Zc When P is transferred, Zc Here, in order to make the charging rate P of each non-linear resistance element of the lightning arrester constant, it is necessary to establish a zero-order equation with P=constant.
vNm人
oc工6
Zc
第7図の等価回路について述べたように、高圧側にある
電圧分担が高い非直線抵抗素子には他のの大きい非直線
抵抗素子を配置すれば、上式を満足することが可能であ
る。vNm oct 6 Zc As mentioned about the equivalent circuit in Figure 7, if the nonlinear resistance element with a high voltage share on the high voltage side is placed with another nonlinear resistance element with a large voltage, the above equation will be satisfied. Is possible.
なお、この発明による避雷装置の構造は、第1図のもの
と全く同じであり、雷サージなどの異常電圧抑効果は何
ら変化しない。The structure of the lightning arrester according to the present invention is exactly the same as that shown in FIG. 1, and the effect of suppressing abnormal voltages such as lightning surges does not change at all.
次にこの発明による避雷装置の通常の連続使用電圧にお
ける電圧分担特性について説明する。第1図(a) 、
(b)は、この発明における非直線抵抗素子柱(3)
の電圧分担特性の一例で、それぞれ電圧分布特性および
素子1枚当りの電圧特性である。図中の実線は、高電圧
側から接地側に向って比VgIA/Zcの大きい非直線
抵抗素子から順番に配列した場合であり、任意に配列し
た第S図(a) 、 (blの場合と比較Tると、高圧
側部分にある非直線抵抗素子に加わる電圧は大幅に小さ
くなり、破線の電圧分担平等の場合に近い特性を示す。Next, the voltage sharing characteristics of the lightning arrester according to the present invention at normal continuous operating voltage will be explained. Figure 1(a),
(b) is the nonlinear resistance element column (3) in the present invention.
These are an example of the voltage sharing characteristics of , and are the voltage distribution characteristics and the voltage characteristics per element, respectively. The solid line in the figure shows the case where nonlinear resistance elements are arranged in order from the high voltage side to the ground side, starting with the ratio VgIA/Zc. In comparison T, the voltage applied to the non-linear resistance element in the high voltage side portion becomes significantly smaller, and exhibits characteristics similar to the case of equal voltage sharing as shown by the broken line.
また、他の実施例として、上述のZcの代りに非直線抵
抗素子の容−1i 1Jアクタンスl/ωCe を用
いても同様な効果が得られる。これは2通常の連続使用
電圧付近では非直線抵抗素子の抵抗がl/ωCeより十
分大きく、無視できるためである。Furthermore, as another embodiment, the same effect can be obtained by using the capacitance -1i 1J actance l/ωCe of the non-linear resistance element in place of the above-mentioned Zc. This is because the resistance of the nonlinear resistance element is sufficiently larger than l/ωCe near the normal continuous operating voltage and can be ignored.
この発明は以上説明したとおり避雷装置の高圧したこと
により、避雷装置の電圧分担が平等になり、一部の高課
電率の非直線抵抗素子が大きく課電劣化するようなこと
がなくなる。このことは。In the present invention, as explained above, by increasing the voltage of the lightning arrester, the voltage distribution of the lightning arrester becomes equal, and some of the non-linear resistance elements with a high charge rate are prevented from being significantly deteriorated by the charge. About this.
避雷装置全体の課電寿命を長くするのみならす熱安定性
も向上させることが可能になり、大きな定格の避雷装置
では、!圧分担均−化のための分圧コンデンサをより小
容量のものにできたり、小形の分圧シールドで済むとい
う効果を生じる。Not only does it extend the energized life of the entire lightning arrester, but it also improves its thermal stability, and for lightning arresters with large ratings! This has the effect that the capacitance of the voltage dividing capacitor for equalizing the voltage distribution can be made smaller, and that a small voltage dividing shield can be used.
第1図はこの発明による避雷装置中の非直線抵抗素子柱
の電圧分布特性(a)と素子1枚当りの電圧特性(b)
を示す図、第2図をま各非直線抵抗素子の電圧−電流(
V−I)特性を示す図、第3図は現在使用中の避雷装置
を示す側断面口、第を図は第3図に示した避雷装置の等
価回路を示す回路図、第3図は従来の避雷装置における
非直線抵抗素子柱の電圧分布特性(atと素子1枚当り
の電圧特性(b)を示す図である。
図において、(3)は非直線抵抗素子柱、(31)〜(
3n)は非直線抵抗素子、 V、、人は′非直線抵抗素
子の動作開始電圧、 Zcは非直線抵抗素子のインピ
ーダンスである。
なお、各図中同一符号は同一または相当部分を示す。
竿1図
(Q) (b)
篤2図
!Figure 1 shows the voltage distribution characteristics (a) of the nonlinear resistance element pillar in the lightning arrester according to the present invention and the voltage characteristics per element (b).
Figure 2 shows the voltage-current of each non-linear resistance element (
V-I) A diagram showing the characteristics, Figure 3 is a side cross-sectional view showing the lightning arrester currently in use, Figure 3 is a circuit diagram showing the equivalent circuit of the lightning arrester shown in Figure 3, and Figure 3 is the conventional lightning arrester. It is a diagram showing the voltage distribution characteristics (at) and the voltage characteristics (b) per element of the nonlinear resistance element pillar in the lightning arrester. In the figure, (3) is the nonlinear resistance element pillar, (31) to (
3n) is a non-linear resistance element, V is the operation start voltage of the non-linear resistance element, and Zc is the impedance of the non-linear resistance element. Note that the same reference numerals in each figure indicate the same or corresponding parts. Rod 1 figure (Q) (b) Atsushi 2 figure!
Claims (4)
線抵抗素子を複数枚直列接続して構成された非直線抵抗
素子柱を備える避雷装置において、各非直線抵抗素子に
ついて、測定した動作開始電圧V_N_m_Aと所定の
電圧において測定した漏れ電流とからインピーダンスZ
cを求め、これらのV_N_m_AとZcから更に比V
_N_m_A/Zcを求め、この比の大きい非直線抵抗
素子を前記避雷装置の高圧側に配置したことを特徴とす
る避雷装置。(1) Measured operation of each nonlinear resistance element in a lightning arrester equipped with a nonlinear resistance element column configured by connecting multiple nonlinear resistance elements in series, each made of a metal oxide whose main component is zinc oxide. The impedance Z is determined from the starting voltage V_N_m_A and the leakage current measured at a given voltage.
c, and further calculate the ratio V from these V_N_m_A and Zc.
_N_m_A/Zc is determined, and a nonlinear resistance element having a large ratio is arranged on the high voltage side of the lightning arrester.
m_A/Zcの大きい非直線抵抗素子から順番に配列し
たことを特徴とする特許請求の範囲第1項記載の避雷装
置。(2) From the high voltage side of the lightning arrester to the ground side, the ratio V_N_
2. The lightning arrester according to claim 1, wherein the nonlinear resistance elements are arranged in order of increasing m_A/Zc.
あることを特徴とする特許請求の範囲第1項または第2
項記載の避雷装置。(3) Claim 1 or 2, characterized in that the predetermined voltage for measuring leakage current is a continuous use voltage.
Lightning arrester as described in section.
1/(ωCe)を使用することを特徴とする特許請求の
範囲第1項または第2項記載の避雷装置。(4) The lightning arrester according to claim 1 or 2, characterized in that the capacitive reactance 1/(ωCe) of the nonlinear resistance element is used in place of Zc.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP59208052A JPS6187301A (en) | 1984-10-05 | 1984-10-05 | Lightning arrestor |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP59208052A JPS6187301A (en) | 1984-10-05 | 1984-10-05 | Lightning arrestor |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS6187301A true JPS6187301A (en) | 1986-05-02 |
| JPH0577165B2 JPH0577165B2 (en) | 1993-10-26 |
Family
ID=16549843
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP59208052A Granted JPS6187301A (en) | 1984-10-05 | 1984-10-05 | Lightning arrestor |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS6187301A (en) |
Citations (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS4929437A (en) * | 1972-07-20 | 1974-03-15 | ||
| JPS54144956A (en) * | 1978-05-02 | 1979-11-12 | Tokyo Shibaura Electric Co | Gapless lightning arrestor |
| JPS5596585A (en) * | 1979-01-18 | 1980-07-22 | Tokyo Shibaura Electric Co | Method of assembling arrester |
-
1984
- 1984-10-05 JP JP59208052A patent/JPS6187301A/en active Granted
Patent Citations (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS4929437A (en) * | 1972-07-20 | 1974-03-15 | ||
| JPS54144956A (en) * | 1978-05-02 | 1979-11-12 | Tokyo Shibaura Electric Co | Gapless lightning arrestor |
| JPS5596585A (en) * | 1979-01-18 | 1980-07-22 | Tokyo Shibaura Electric Co | Method of assembling arrester |
Also Published As
| Publication number | Publication date |
|---|---|
| JPH0577165B2 (en) | 1993-10-26 |
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