JPH0646609B2 - Oil-filled induction device - Google Patents

Oil-filled induction device

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Publication number
JPH0646609B2
JPH0646609B2 JP61211095A JP21109586A JPH0646609B2 JP H0646609 B2 JPH0646609 B2 JP H0646609B2 JP 61211095 A JP61211095 A JP 61211095A JP 21109586 A JP21109586 A JP 21109586A JP H0646609 B2 JPH0646609 B2 JP H0646609B2
Authority
JP
Japan
Prior art keywords
oil
dielectric constant
low
electric field
linear
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 - Lifetime
Application number
JP61211095A
Other languages
Japanese (ja)
Other versions
JPS6366910A (en
Inventor
貞夫 古川
馨 遠藤
裕幸 藤田
充正 橋本
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Hitachi Ltd
Original Assignee
Hitachi Ltd
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Priority to JP61211095A priority Critical patent/JPH0646609B2/en
Publication of JPS6366910A publication Critical patent/JPS6366910A/en
Publication of JPH0646609B2 publication Critical patent/JPH0646609B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明は油入誘導電器に関するものである。TECHNICAL FIELD The present invention relates to an oil-filled induction electric device.

〔従来の技術〕[Conventional technology]

従来の油入誘導電器は特開昭53-74231号公報に記載され
ているように、高低圧巻線間に配置した複数の絶縁筒の
うち中間に配置された絶縁筒のみ低誘電率の絶縁材料で
構成し、油隙に加わる電界を緩和して高低圧巻線間の絶
縁距離すなわち主絶縁距離の短縮を図つている。しかし
実際上,絶縁性能を決定する主要因となる高低圧巻線表
面の局部的な油隙の電界緩和については配慮されていな
かつた。
As described in Japanese Patent Laid-Open No. 53-74231, the conventional oil-filled induction device has an insulating material with a low dielectric constant only in the insulating cylinder arranged in the middle among a plurality of insulating cylinders arranged between high and low voltage windings. In order to reduce the insulation distance between the high and low voltage windings, that is, the main insulation distance, the electric field applied to the oil gap is relaxed. However, in practice, no consideration was given to the local relaxation of the electric field of the oil gap on the surface of the high and low voltage windings, which is the main factor that determines the insulation performance.

〔発明が解決しようとする問題点〕[Problems to be solved by the invention]

一般に不平等な電界下では一つの部位でそれを構成する
機材の誘電率を変えた場合に、それが他の部位の電界に
及ぼす影響は距離と共に小さくなる傾向がある。高低圧
巻線表面の電界は不平等電界である。上記従来技術は巻
線表面から離れた部位の誘電率を変えたものであり、絶
縁上肝心な巻線表面の油隙電界に関しては緩和効果が小
さかつた。また、高低圧巻線間には絶縁筒の他に絶縁距
離を確保するための直線スペーサも配置されており、そ
れと接する巻線表面ではむしろ直線スペーサによる電界
集中が大きく、単に絶縁筒のみ低誘電率化しても巻線表
面の油隙電界の緩和効果が小さかつた。また、一般に低
誘電率絶縁物は通常の絶縁材料に比べて2倍ないしそれ
以上高価であり、効果的に用いることで使用量を少なく
し、コストアツプを押える必要がある。
In general, under an unequal electric field, when the permittivity of the equipment constituting one part is changed in one part, the influence that it has on the electric field in other parts tends to decrease with distance. The electric field on the surface of the high and low voltage windings is an unequal electric field. The above-mentioned conventional technique changes the permittivity of the portion distant from the winding surface, and has a small relaxation effect on the oil gap electric field on the winding surface which is essential for insulation. In addition to the insulating cylinder, a linear spacer is also arranged between the high and low voltage windings to secure the insulation distance, and the electric field concentration due to the linear spacer is rather large on the surface of the winding in contact with it, and only the insulating cylinder has a low dielectric constant. The effect of relaxing the electric field in the oil gap on the surface of the winding was small even if it was made. In general, a low dielectric constant insulator is twice or more expensive as compared with a normal insulating material, and it is necessary to reduce the amount of use and to reduce the cost by effectively using it.

本発明は以上の点に鑑みなされたものであり、巻線表面
の油隙電界を緩和し、主絶縁距離を短縮することを可能
とした油入誘導電器を提供することを目的とするもので
ある。
The present invention has been made in view of the above points, and an object thereof is to provide an oil-filled induction electric device capable of relaxing an oil gap electric field on a winding surface and shortening a main insulation distance. is there.

〔問題点を解決するための手段〕[Means for solving problems]

上記目的は、外側絶縁筒,外側直線スペーサ,内側直線
スペーサの少なくとも外側絶縁筒,外側直線スペーサ
を、内側絶縁筒の誘電率より小さい誘電率の低誘電率絶
縁物で形成することにより、達成される。
The above object is achieved by forming at least the outer insulating cylinder and the outer linear spacer of the outer insulating cylinder, the outer linear spacer, and the inner linear spacer with a low dielectric constant insulator having a dielectric constant smaller than that of the inner insulating cylinder. It

〔作用〕[Action]

少なくとも外側絶縁筒,外側直線スペーサを低誘電率絶
縁物で形成したので、少なくとも外側絶縁筒,外側直線
スペーサの内部では誘電率が小さい。従つてその分外側
絶縁筒、外側直線スペーサ内部に電界が集中する。これ
によつて隣接する油隙、すなわち高低圧巻線表面の油隙
の電界が緩和されるようになり、主絶縁距離が短縮でき
る。また、この場合に低誘電率絶縁物表面のパルプ繊維
層は、低誘電率絶縁物表面の絶縁上有害な毛羽立ちを押
え、毛羽立ちによる絶縁性能の低下を防止する。
Since at least the outer insulating cylinder and the outer linear spacer are formed of a low dielectric constant insulator, the dielectric constant is small at least inside the outer insulating cylinder and the outer linear spacer. Therefore, the electric field concentrates inside the outer insulating cylinder and the outer linear spacer. As a result, the electric field of the oil gaps adjacent to each other, that is, the oil gaps on the high and low voltage winding surfaces is alleviated, and the main insulation distance can be shortened. Further, in this case, the pulp fiber layer on the surface of the low-dielectric-constant insulator suppresses fluff that is harmful to the insulation on the surface of the low-dielectric-constant insulator, and prevents deterioration of the insulating performance due to the fluff.

〔実施例〕〔Example〕

以下、図示した実施例に基づいて本発明を説明する。第
1図から第3図には本発明の一実施例が示されている。
同図に示されているように油入誘導電器は同心状に配置
された高圧巻線1および低圧巻線2と、これら高圧巻線
1と低圧巻線2との間に配置された複数の絶縁筒3およ
び直線スペーサ4とを備えている。そしてこれら絶縁筒
3および直線スペーサ4は、高低圧巻線1、2間にこれ
ら高低圧巻線1、2に夫々接して配置される外側直線ス
ペーサ4a、4c、これら外側直線スペーサ4a、4c
間にこれら外側直線スペーサ4a、4cに夫々接して配
置される外側絶縁筒3a、3cおよびこれら外側絶縁筒
3a、3c間に配置される内側絶縁筒3b、内側直線ス
ペーサ4bを有しており、高低圧巻線1、2、絶縁筒3
(外側絶縁筒3a、3c、内側絶縁筒3b)、直線スペ
ーサ4(外側直線スペーサ4a、4c、内側直線スペー
サ4b)の間には油層5が形成されている。このように
高圧巻線1と低圧巻線2との間には絶縁筒3と直線スペ
ーサ4とが交互に複数個配置されており、これらが鉱油
中に浸漬されて複合絶縁層すなわち変圧器における主絶
縁6が形成される。なお高圧巻線1は中央部が高圧端子
7であり、ここに電圧Vが発生する。上下端は中性点端
子8,8aであり、ここには電圧が発生しない。この主
絶縁6では鉱油自体の絶縁破壊強度が、巻線被覆や絶縁
筒3および直線スペーサ4を構成する固体絶縁物よりも
低いため、まず油層5から絶縁破壊が生じる。絶縁筒3
は油隙を細分割し、油隙長が短いほど油隙の絶縁破壊強
度が高い現象を示す,所謂油隙長の効果によつて油層5
の絶縁強度を高めると共に、例え油隙が絶縁破壊を生じ
てもストリーマの進展を阻止し、高圧巻線1,低圧巻線
2間の絶縁破壊を防止する役目を果している。直線スペ
ーサ4は油層5を所定の油隙長に保つ役目を果してい
る。
Hereinafter, the present invention will be described based on the illustrated embodiments. 1 to 3 show an embodiment of the present invention.
As shown in the figure, the oil-filled induction electric device is composed of a high-voltage winding 1 and a low-voltage winding 2 arranged concentrically, and a plurality of high-voltage windings 1 and 2 arranged between the high-voltage winding 1 and the low-voltage winding 2. The insulating cylinder 3 and the linear spacer 4 are provided. These insulating cylinders 3 and linear spacers 4 are outer linear spacers 4a and 4c arranged between the high and low voltage windings 1 and 2 in contact with the high and low voltage windings 1 and 2, respectively, and these outer linear spacers 4a and 4c.
The outer insulating cylinders 3a and 3c arranged in contact with the outer linear spacers 4a and 4c, respectively, and the inner insulating cylinder 3b and the inner linear spacer 4b arranged between the outer insulating cylinders 3a and 3c, High and low voltage windings 1 and 2, insulating tube 3
An oil layer 5 is formed between the (outer insulating cylinders 3a, 3c, the inner insulating cylinder 3b) and the linear spacer 4 (the outer linear spacers 4a, 4c, the inner linear spacer 4b). Thus, a plurality of insulating cylinders 3 and linear spacers 4 are alternately arranged between the high-voltage winding 1 and the low-voltage winding 2, and these are immersed in mineral oil to form a composite insulating layer, that is, in a transformer. The main insulation 6 is formed. The high-voltage winding 1 has a high-voltage terminal 7 at the center, and a voltage V is generated there. The upper and lower ends are the neutral point terminals 8 and 8a, and no voltage is generated here. Since the dielectric breakdown strength of the mineral oil itself in this main insulation 6 is lower than that of the solid insulating material forming the winding coating, the insulating cylinder 3 and the linear spacer 4, the dielectric breakdown first occurs from the oil layer 5. Insulation tube 3
Shows a phenomenon that the oil gap is subdivided, and the shorter the oil gap length, the higher the dielectric breakdown strength of the oil gap.
It also has the function of increasing the insulation strength, preventing the streamer from developing even if an oil gap causes dielectric breakdown, and preventing the dielectric breakdown between the high voltage winding 1 and the low voltage winding 2. The linear spacer 4 serves to keep the oil layer 5 at a predetermined oil gap length.

このように構成された油入誘導電器で本実施例では外側
絶縁筒3a,3c,外側直線スペーサ4a,4cを、内
側絶縁筒3b,内側直線スペーサ4bの誘電率より小さ
い誘電率の低誘電率絶縁物9で形成した。このようにす
ることにより外側絶縁筒3a,3c,外側直線スペーサ
4a,4cは、内側絶縁筒3b,内側直線スペーサ4b
の誘電率より小さい誘電率の低誘電率絶縁物9で形成さ
れるようになつて、外側絶縁筒3a、3c、外側直線ス
ペーサ4a、4cに電界が集中するようになつてその分
高低圧巻線1,2表面の油隙の電界が緩和されるように
なり、巻線表面の油隙電界を緩和し、主絶縁距離を短縮
することを可能とした油入誘導電器を得ることができ
る。
In the oil-filled induction electric device configured as described above, the outer insulating cylinders 3a and 3c and the outer linear spacers 4a and 4c in the present embodiment have a low dielectric constant smaller than that of the inner insulating cylinder 3b and the inner linear spacer 4b. It is formed of the insulator 9. By doing so, the outer insulating cylinders 3a and 3c and the outer linear spacers 4a and 4c become the inner insulating cylinder 3b and the inner linear spacer 4b.
Is formed of a low dielectric constant insulator 9 having a dielectric constant smaller than that of the electric field, and the electric field is concentrated on the outer insulating cylinders 3a and 3c and the outer linear spacers 4a and 4c. The electric field of the oil gap on the surfaces 1 and 2 is relaxed, the electric field of the oil gap on the surface of the winding is relaxed, and the oil-filled induction electric device capable of shortening the main insulation distance can be obtained.

すなわち外側絶縁筒3a,3c,外側直線スペーサ4
a,4cを低誘電率絶縁物9で形成したが、この低誘電
率絶縁物9を低誘電率部9aと、この低誘電率部9aを
被覆したパルプ繊維9bとで形成した。すなわちパルプ
繊維と低誘電率で耐油性の高い合成繊維、例えばポリエ
チレンテレフタレート(PET),ポリプロピレン(P
P)繊維のいずれかとを混抄して低誘導電率部9aを形
成し、表面にパルプ100%のパルス繊維9bを抄き合
せた。因みに内側絶縁筒3b,内側直線スペーサ4bは
通常の絶縁紙で構成してある。このようにすることによ
り高低圧巻線1,2表面の油隙の電界が緩和されるよう
になるが、従来例と比較検討した結果を次に述べる。
That is, the outer insulating cylinders 3a and 3c, the outer linear spacer 4
Although a and 4c are formed of the low dielectric constant insulator 9, the low dielectric constant insulator 9 is formed of the low dielectric constant portion 9a and the pulp fiber 9b covering the low dielectric constant portion 9a. That is, pulp fibers and synthetic fibers having a low dielectric constant and high oil resistance, such as polyethylene terephthalate (PET) and polypropylene (P
The P) fiber was mixed with any of the fibers to form a low inductive conductivity section 9a, and pulsed fibers 9b of 100% pulp were mixed on the surface. Incidentally, the inner insulating cylinder 3b and the inner linear spacer 4b are made of ordinary insulating paper. By doing so, the electric field in the oil gaps on the surfaces of the high and low voltage windings 1 and 2 can be relaxed. The results of a comparative study with the conventional example will be described below.

本実施例の主絶縁6の中央部の電界を数値電界計算法で
調査した結果が第4図に示されている。図中で点線で示
してあるのは等電位線10である。同図に示されている
ように中間部分では等電位線10はほぼ平行で均等な電
界に近いが、高圧巻線1および低圧巻線2の表面近傍で
は巻線表面の凹凸のため等電位線10が波打つて不平等
電界になつている。この高圧巻線1の表面近傍の電界分
布が第5図に示されている。通常高圧巻線1を構成する
電線11の絶縁被覆12と外側直線スペーサ4aとの間
の油隙13で最も電界が集中していて、ここで最初に放
電が生じ、それが発端になつて全体の絶縁破壊を生じる
場合が多い。ところで本実施例の場合、同図から明らか
なように油隙13近傍の等電位線10の間隔が殆ど狭ま
らず、油隙13での電界集中が小さい。これに対し従来
例の電界分布は第6図に示されているように、油隙13
近傍で電界が集中している。このように本実施例が従来
に比べて良好な結果を示したのは従来例の外側直線スペ
ーサ4aおよび外側絶縁筒3aは誘導率が大きいので、
夫々の内部が電界緩和され、その電界緩和された分が誘
電率の小さい油隙13にしわ寄せされるのに対し、本実
施例では隣接する外側直線スペーサ4aおよび外側絶縁
筒3aの誘電率が小さいので、夫々の内部で電界が集中
するためである。
FIG. 4 shows the results of an investigation of the electric field in the central portion of the main insulation 6 of this example by the numerical electric field calculation method. The equipotential lines 10 are shown by dotted lines in the figure. As shown in the figure, the equipotential lines 10 are almost parallel and close to a uniform electric field in the middle portion, but near the surfaces of the high voltage winding 1 and the low voltage winding 2, the equipotential lines 10 are uneven due to the unevenness of the winding surfaces. 10 is undulating and becomes an unequal electric field. The electric field distribution near the surface of the high voltage winding 1 is shown in FIG. Usually, the electric field is most concentrated in the oil gap 13 between the insulating coating 12 of the electric wire 11 that constitutes the high-voltage winding 1 and the outer linear spacer 4a, and the electric discharge occurs first here, and then it becomes the starting point and the whole In many cases, dielectric breakdown occurs. By the way, in the case of the present embodiment, as is clear from the figure, the interval between the equipotential lines 10 near the oil gap 13 is not narrowed, and the electric field concentration in the oil gap 13 is small. On the other hand, the electric field distribution of the conventional example is as shown in FIG.
The electric field is concentrated in the vicinity. As described above, the present example shows a better result than the conventional one because the outer linear spacer 4a and the outer insulating cylinder 3a of the conventional example have a large inductivity.
The inside of each of them is relaxed by an electric field, and the amount of the relaxed electric field is wrinkled into the oil gap 13 having a small dielectric constant, whereas in the present embodiment, the dielectric constants of the outer linear spacer 4a and the outer insulating cylinder 3a adjacent to each other are small. Therefore, the electric field is concentrated inside each of them.

一方,油隙の絶縁強度は隣接する絶縁物の表面状態,特
に毛羽立ちの影響を受け、毛羽立ちが大きいほど低下す
る傾向がある。この点通常の低誘電率絶縁物はパルプ繊
維と低誘電率の合成繊維とが混抄されているが、このま
まではパルプ繊維と合成繊維との結合が弱いので毛羽立
ち易く、通常の絶縁紙よりも油隙の絶縁強度を低下させ
る。
On the other hand, the insulation strength of the oil gap is influenced by the surface condition of the adjacent insulating material, particularly the fuzz, and tends to decrease as the fuzz increases. In this respect, the usual low-dielectric-constant insulator is a mixture of pulp fibers and synthetic fibers with low-dielectric constant. Reduces the insulation strength of the gap.

ところで本実施例の場合は低誘電率部9aである合成繊
維の表面を100%のパルプ繊維9bで被覆したので、
通常の絶縁紙と同程度の表面状態が得られ、油隙の絶縁
強度を低下させることがない。
By the way, in the case of the present embodiment, since the surface of the synthetic fiber which is the low dielectric constant portion 9a is covered with 100% pulp fiber 9b,
A surface condition similar to that of ordinary insulating paper is obtained, and the insulating strength of the oil gap is not reduced.

従って従来の油隙の電界を本実施例の油隙の許容電界と
すれば、高圧巻線1と低圧巻線2との間の絶縁距離すな
わち主絶縁距離を短縮して、本実施例を採用した場合の
油隙の電界を許容電界まで高めても、主絶縁6の絶縁強
度は変らない。従って本実施例によれば主絶縁6の絶縁
強度を低下させることなく、従来よりも主絶縁距離を短
縮することができ、巻線の小形化ができる。因みに従来
主絶縁距離が70mmで絶縁筒3が5個,その厚さが夫夫
5mmの場合について試算すると、比誘電率が3.5程度
の低誘電率絶縁物9を用いた場合、従来と比較して主絶
縁距離が10mm,比率にして15%程度短縮できる。全
ての絶縁筒3および直線スペーサ4を低誘電率絶縁物9
で構成した場合でも15mmの短縮であり、本実施例の効
果は大きい。また、主絶縁距離が短縮することによつて
当然巻線径が小さくなるので、変圧器タンク幅や長さも
短縮でき、タンクの小形化および油量の低減ができる。
Therefore, if the electric field of the conventional oil gap is set as the allowable electric field of the oil gap of this embodiment, the insulation distance between the high-voltage winding 1 and the low-voltage winding 2, that is, the main insulation distance is shortened, and this embodiment is adopted. Even if the electric field of the oil gap in this case is increased to the allowable electric field, the insulation strength of the main insulation 6 does not change. Therefore, according to the present embodiment, the main insulation distance can be shortened and the winding can be miniaturized as compared with the conventional case without lowering the insulation strength of the main insulation 6. By the way, when the conventional main insulation distance is 70 mm, the number of insulating cylinders 3 is 5, and the thickness thereof is 5 mm, it is calculated as follows when the low dielectric constant insulator 9 having a relative dielectric constant of about 3.5 is used. In comparison, the main insulation distance can be shortened by 10 mm, and the ratio can be reduced by about 15%. All the insulating cylinders 3 and the linear spacers 4 are made of a low dielectric constant insulator 9
Even in the case of the above construction, the length is reduced by 15 mm, and the effect of this embodiment is great. In addition, since the winding diameter is naturally reduced by shortening the main insulation distance, the width and length of the transformer tank can be shortened, and the tank can be downsized and the amount of oil can be reduced.

第7図には本発明の他の実施例が示されている。本実施
例では外側絶縁筒3a,3c,外側直線スペーサ4a,
4cおよび内側直線スペーサ4bを低誘電率絶縁物で形
成した。このようにすることにより外側絶縁筒3a,3
c,外側直線スペーサ4a,4cおよび内側直線スペー
サ4bが低誘電率絶縁物で形成されるようになつて、前
述の場合よりも低誘電率絶縁物の少しの増加で巻線表面
の電界を前述の場合より緩和することができ、主絶縁6
aの距離を前述の場合よりも短縮することができる。
FIG. 7 shows another embodiment of the present invention. In this embodiment, the outer insulating cylinders 3a and 3c, the outer linear spacer 4a,
4c and the inner linear spacer 4b are formed of a low dielectric constant insulator. By doing so, the outer insulating cylinders 3a, 3
Since the outer linear spacers 4a, 4c and the inner linear spacers 4b are formed of a low dielectric constant insulator, the electric field on the winding surface can be reduced by a slight increase of the low dielectric constant insulator as compared with the above case. The main insulation can be relaxed more than 6
The distance a can be shortened as compared with the above case.

すなわち高圧巻線1の表面近傍の電界分布が示されてい
る第8図に示されているように、実線表示の本実施例の
等電位線14の方が点線表示の前述の等電位線10に比
べ高圧巻線1から離れて内側寄りである。これは内側直
線スペーサ4b内部で誘電率が小さくなつた分電界集中
して等電位線14の間隔が狭まつたためで、高圧巻線1
表面の油隙13では等電位線14の間隔が前述の場合よ
りも広くなつている。すなわち前述の場合よりも電界緩
和される。この場合に、直線スペーサ4は全部合せても
絶縁筒3の体積の1/10程度なので、内側直線スペー
サ4bを低誘電率絶縁物にしても、前述の場合に比べ低
誘電率絶縁物の使用量は僅かしか増加しない。
That is, as shown in FIG. 8 in which the electric field distribution near the surface of the high-voltage winding 1 is shown, the equipotential line 14 of this embodiment shown in solid line is the equipotential line 10 shown in dotted line. Compared to the above, the inner side is separated from the high voltage winding 1. This is because the electric field is concentrated in the inner linear spacer 4b due to the decrease in the dielectric constant and the interval between the equipotential lines 14 is narrowed.
In the oil gap 13 on the surface, the equipotential lines 14 are wider than in the case described above. That is, the electric field is relaxed more than in the above case. In this case, even if all of the linear spacers 4 are combined, it is about 1/10 of the volume of the insulating cylinder 3. Therefore, even if the inner linear spacer 4b is made of a low dielectric constant insulator, a low dielectric constant insulator is used as compared with the above case. The quantity only increases slightly.

第9図には本発明の更に他の実施例が示されている。本
実施例では外側絶縁筒3aを上部3a1,中央部3a2,下部
3a3の3部構造とし、夫々を順にテーパ接合して一体と
した。中央部3a2は長さを絶縁筒3aの全長の1/2程
度とし、低誘電率絶縁物で構成した。同様にしてもう一
方の外側絶縁筒3cおよび外側直線スペーサ4a,4c
についても3c1,3c2,3c3,4a1,4a2,4a3および4c1,4c2,4c3
の3部構造とし、夫々の中央部3c2,4a2および4c2を低誘
電率絶縁物で構成し、上部3c1,4a1,4c1および下部3c3,4
a3,4c3は通常の絶縁紙で構成して、主絶縁6bを形成し
た。このようにすることにより前述の場合に比べ、絶縁
強度を下げることなくコスト低減できる。
FIG. 9 shows still another embodiment of the present invention. In this embodiment the top 3a 1 the outer insulating tube 3a, the central portion 3a 2, lower
3a 3 has a three-part structure, and each of them is taper-joined in order to be integrated. The central portion 3a 2 has a length of about ½ of the entire length of the insulating cylinder 3a and is made of a low dielectric constant insulator. Similarly, the other outer insulating cylinder 3c and outer linear spacers 4a, 4c
For 3c 1 also, 3c 2, 3c 3, 4a 1, 4a 2, 4a 3 and 4c 1, 4c 2, 4c 3
And a central part 3c 2 , 4a 2 and 4c 2 is composed of a low dielectric constant insulator, and an upper part 3c 1 , 4a 1 , 4c 1 and a lower part 3c 3 , 4
The a 3 and 4c 3 were made of ordinary insulating paper to form the main insulating 6b. By doing so, the cost can be reduced without lowering the insulation strength as compared with the case described above.

本実施例の高圧巻線1の高圧端子7に雷インパルス電圧
が加わつた場合の高圧巻線1と低圧巻線2との間の差電
圧の分布が第10図に示されている。同図で横軸は高圧
端子の位置を0%,中性点端子の位置を100%とした
高圧巻線の縦方向位置であり、縦軸は縦方向の各位置に
おける高圧巻線と低圧巻線との間の差電圧である。一般
に差電圧の分布は巻線の電位振動現象によつて高圧端子
近傍で持ち上がる傾向を示す。そのため同図に示されて
いるように、高圧端子から相当離れた位置まで印加電圧
と同等ないしそれ以上の差電圧が生じる。このような傾
向が最も大きい場合,高圧端子から50%位置近くまで
及ぶ。ところで本実施例の場合、この50%位置までは
低誘電率絶縁物で構成したので、前述の第1図の実施例
と同等の絶縁強度がある。残りの領域は差電圧が小さい
ので、通常の絶縁紙でも絶縁上問題がない。すなわち高
価な低誘電率絶縁物の使用量を減らして前述の場合と同
等の絶縁強度が得られる。
FIG. 10 shows the distribution of the voltage difference between the high voltage winding 1 and the low voltage winding 2 when a lightning impulse voltage is applied to the high voltage terminal 7 of the high voltage winding 1 of this embodiment. In the figure, the horizontal axis is the vertical position of the high voltage winding with the position of the high voltage terminal being 0% and the position of the neutral point terminal being 100%, and the vertical axis is the high voltage winding and low voltage winding at each position in the vertical direction. It is the voltage difference between the lines. Generally, the distribution of the differential voltage tends to rise near the high voltage terminal due to the potential oscillation phenomenon of the winding. Therefore, as shown in the same figure, a differential voltage equal to or higher than the applied voltage is generated up to a position far away from the high voltage terminal. When this tendency is the largest, it extends from the high-voltage terminal to a position close to 50%. By the way, in the case of the present embodiment, since up to this 50% position is made of the low dielectric constant insulator, it has the same insulation strength as that of the embodiment shown in FIG. Since the remaining area has a small voltage difference, normal insulating paper will not cause any insulation problems. That is, the amount of expensive low-dielectric-constant insulator is reduced to obtain the same insulation strength as in the above case.

第11図には本発明の更に他の実施例が示されている。
本実施例は高圧巻線1を上端が高圧端子7,下端が中性
点端子8となる所謂巻通し巻線で構成した場合である。
外側絶縁筒3a,3cおよび外側直線ペーサ4a,4c
を夫々3a4,3a5,3c4,3c5および4a4,4a5,4c4,4c5の上下2
部構造とし、上部3a4,3c4,4a4,4c4を低誘電率絶縁物で
構成し、下部3a5,3c5,4a5,4c5は通常の絶縁紙で構成し
て、主絶縁6cを形成した。このように高圧巻線1と低
圧巻線2との間の差電圧が大きい上部は低誘電率絶縁物
で構成し、差電圧の小さい下部は通常の絶縁紙で構成し
たので、絶縁的には前述の場合と類似しており、前述の
場合と同等な効果が得られる。
FIG. 11 shows still another embodiment of the present invention.
In this embodiment, the high-voltage winding 1 is composed of a so-called winding wire having a high-voltage terminal 7 at the upper end and a neutral point terminal 8 at the lower end.
Outer insulating cylinders 3a, 3c and outer linear pacers 4a, 4c
3a 4 , 3a 5 , 3c 4 , 3c 5 and 4a 4 , 4a 5 , 4c 4 , 4c 5 up and down 2 respectively
Partial structure, the upper part 3a 4 , 3c 4 , 4a 4 , 4c 4 is composed of low dielectric constant insulator, the lower part 3a 5 , 3c 5 , 4a 5 , 4c 5 is composed of normal insulating paper 6c was formed. In this way, the upper part where the differential voltage between the high voltage winding 1 and the low voltage winding 2 is large is made of a low dielectric constant insulator, and the lower part where the differential voltage is small is made of ordinary insulating paper. It is similar to the above case, and the same effect as the above case can be obtained.

〔発明の効果〕〔The invention's effect〕

上述のように本発明は巻線表面の油隙電界を緩和し、主
絶縁距離を短縮できるようになつて、巻線表面の油隙電
界を緩和し、主絶縁距離を短縮することを可能とした油
入誘導電器を得ることができる。
As described above, according to the present invention, the oil gap electric field on the winding surface can be relaxed and the main insulation distance can be shortened. Therefore, the oil gap electric field on the winding surface can be mitigated and the main insulation distance can be shortened. It is possible to obtain the oil-filled induction device.

【図面の簡単な説明】[Brief description of drawings]

第1図は本発明の油入誘導電器の一実施例の縦断側面
図、第2図は同じ一実施例の低誘電率絶縁物の縦断側面
図、第3図は第1図の上面図、第4図は同じく一実施例
の主絶縁中央部の電界分布を示す電界分布図、第5図は
同じく一実施例の高圧巻線表面近傍の電界分布を示す拡
大電界分布図、第6図は従来の油入誘導電器の高圧巻線
表面近傍の電界分布を示す拡大電界分布図、第7図は本
発明の油入誘導電器の他の実施例の縦断側面図、第8図
は同じく他の実施例の高圧巻線表面近傍の電界分布を示
す拡大電界分布図、第9図は本発明の油入誘導電器の更
に他の実施例の縦断側面図、第10図は同じく更に他の
実施例の巻線の雷インパルス差電圧分布図、第11図は
本発明の油入誘導電器の更に他の実施例の縦断側面図で
ある。 1…高圧巻線、2…低圧巻線、3…絶縁筒、3a…外側
絶縁筒、3b…内側絶縁筒、3c…外側絶縁筒、4…直
線スペーサ、4a…外側直線スペーサ、4b…内側直線
スペーサ、4c…外側直線スペーサ、5…油層、6,6
a,6b,6c…主絶縁、9…低誘電率絶縁物、9a…
低誘電率部、9b…パルプ繊維、13…油隙。
1 is a vertical sectional side view of an embodiment of the oil-filled induction device of the present invention, FIG. 2 is a vertical sectional side view of a low dielectric constant insulator of the same embodiment, and FIG. 3 is a top view of FIG. FIG. 4 is an electric field distribution diagram showing the electric field distribution in the central portion of the main insulation of the same embodiment, FIG. 5 is an enlarged electric field distribution diagram showing the electric field distribution in the vicinity of the surface of the high voltage winding of the embodiment, and FIG. FIG. 7 is an enlarged electric field distribution diagram showing an electric field distribution in the vicinity of the high voltage winding surface of a conventional oil-filled induction device, FIG. 7 is a vertical side view of another embodiment of the oil-filled induction device of the present invention, and FIG. An enlarged electric field distribution diagram showing an electric field distribution in the vicinity of the surface of the high-voltage winding of the embodiment, FIG. 9 is a vertical sectional side view of still another embodiment of the oil-filled induction machine of the present invention, and FIG. 10 is still another embodiment. FIG. 11 is a vertical cross-sectional side view of yet another embodiment of the oil-filled induction device according to the present invention. DESCRIPTION OF SYMBOLS 1 ... High voltage winding, 2 ... Low voltage winding, 3 ... Insulating cylinder, 3a ... Outer insulating cylinder, 3b ... Inner insulating cylinder, 3c ... Outer insulating cylinder, 4 ... Linear spacer, 4a ... Outer linear spacer, 4b ... Inner linear Spacer, 4c ... Outer linear spacer, 5 ... Oil layer, 6, 6
a, 6b, 6c ... Main insulation, 9 ... Low dielectric constant insulator, 9a ...
Low dielectric constant part, 9b ... Pulp fiber, 13 ... Oil gap.

Claims (3)

【特許請求の範囲】[Claims] 【請求項1】同心状に配置された低圧巻線および高圧巻
線と、これら低圧巻線と高圧巻線との間に配置された複
数の絶縁筒および直線スペーサとを備え、これら絶縁筒
および直線スペーサは、前記高低圧巻線間にこれら高低
圧巻線に夫々接して配置される外側直線スペーサ、これ
ら外側直線スペーサ間にこれら外側直線スペーサに夫々
接して配置される外側絶縁筒およびこれら外側絶縁筒間
に配置される内側絶縁筒、内側直線スペーサを有してお
り、前記高低圧巻線、絶縁筒、直線スペーサの間には油
層が形成されている油入誘導電器において、前記外側絶
縁筒、外側直線スペーサ、内側直線スペーサの少なくと
も外側絶縁筒、外側直線スペーサを、前記内側絶縁筒の
誘電率より小さい誘電率の低誘電率絶縁物で形成したこ
とを特徴とする油入誘導電器。
1. A low-voltage winding and a high-voltage winding arranged concentrically, and a plurality of insulating cylinders and linear spacers arranged between the low-voltage winding and the high-voltage winding. The linear spacers are outer linear spacers arranged between the high and low voltage windings so as to be in contact with the high and low voltage windings, outer insulating cylinders arranged between the outer linear spacers and are respectively in contact with the outer linear spacers, and outer insulating cylinders thereof. In an oil-filled induction machine having an inner insulating cylinder and an inner linear spacer arranged between them, and an oil layer being formed between the high and low voltage windings, the insulating cylinder, and the linear spacer, the outer insulating cylinder, the outer An oil characterized in that at least the outer insulating cylinder and the outer linear spacer of the linear spacer and the inner linear spacer are formed of a low dielectric constant insulator having a dielectric constant smaller than that of the inner insulating cylinder. Induction apparatus.
【請求項2】前記低誘電率絶縁物が、低誘電率部と、こ
の低誘電率部の表面に設けられたパルプ繊維とで形成さ
れたものである特許請求の範囲第1項記載の油入誘導電
器。
2. The oil according to claim 1, wherein the low dielectric constant insulator is formed of a low dielectric constant portion and pulp fibers provided on the surface of the low dielectric constant portion. Induction electric appliance.
【請求項3】前記低誘電率部が、パルプ繊維とポリエチ
レンテレフタレート、ポリプロピレン繊維のいずれかと
が混抄されたものである特許請求の範囲第2項記載の油
入誘導電器。
3. The oil-filled induction device according to claim 2, wherein the low dielectric constant portion is a mixture of pulp fiber and any one of polyethylene terephthalate and polypropylene fiber.
JP61211095A 1986-09-08 1986-09-08 Oil-filled induction device Expired - Lifetime JPH0646609B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP61211095A JPH0646609B2 (en) 1986-09-08 1986-09-08 Oil-filled induction device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP61211095A JPH0646609B2 (en) 1986-09-08 1986-09-08 Oil-filled induction device

Publications (2)

Publication Number Publication Date
JPS6366910A JPS6366910A (en) 1988-03-25
JPH0646609B2 true JPH0646609B2 (en) 1994-06-15

Family

ID=16600329

Family Applications (1)

Application Number Title Priority Date Filing Date
JP61211095A Expired - Lifetime JPH0646609B2 (en) 1986-09-08 1986-09-08 Oil-filled induction device

Country Status (1)

Country Link
JP (1) JPH0646609B2 (en)

Families Citing this family (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0499289A (en) * 1990-08-08 1992-03-31 Sumitomo Metal Ind Ltd Etching method
JPH05190354A (en) * 1992-01-10 1993-07-30 Toshiba Corp Stationary induction machine
JP2013055279A (en) * 2011-09-06 2013-03-21 Hitachi Ltd Stationary induction apparatus

Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS54131717A (en) * 1978-04-05 1979-10-13 Hitachi Ltd Inter-winding insulation apparatus of oil-filled transformer

Patent Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS54131717A (en) * 1978-04-05 1979-10-13 Hitachi Ltd Inter-winding insulation apparatus of oil-filled transformer

Also Published As

Publication number Publication date
JPS6366910A (en) 1988-03-25

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