JPS618909A - Winding construction of stationary induction electric apparatus - Google Patents
Winding construction of stationary induction electric apparatusInfo
- Publication number
- JPS618909A JPS618909A JP12960384A JP12960384A JPS618909A JP S618909 A JPS618909 A JP S618909A JP 12960384 A JP12960384 A JP 12960384A JP 12960384 A JP12960384 A JP 12960384A JP S618909 A JPS618909 A JP S618909A
- Authority
- JP
- Japan
- Prior art keywords
- vertical
- duct
- winding
- vertical duct
- stationary induction
- 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
- H01F—MAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
- H01F27/00—Details of transformers or inductances, in general
- H01F27/28—Coils; Windings; Conductive connections
- H01F27/2876—Cooling
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01F—MAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
- H01F27/00—Details of transformers or inductances, in general
- H01F27/28—Coils; Windings; Conductive connections
- H01F27/32—Insulating of coils, windings, or parts thereof
- H01F27/322—Insulating of coils, windings, or parts thereof the insulation forming channels for circulation of the fluid
Landscapes
- Engineering & Computer Science (AREA)
- Power Engineering (AREA)
- Coils Of Transformers For General Uses (AREA)
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】 〔発明の利用分野〕 本発明は静止誘導電器の巻線構造に関するものである。[Detailed description of the invention] [Field of application of the invention] The present invention relates to a winding structure for a stationary induction appliance.
第2図にはSFsガス絶縁変圧器の従来例が示されてい
る。同図に示されているように円筒巻線1は、鉄心脚に
巻回された内側絶縁筒2の外周に複数の垂直ダクト3を
形成するように各巻線単位(以下、コイルと称する)4
を垂直スペーサ5を介して巻回すると共に、水平スペー
サ6を上下端部に配置し、垂直ダクト3と連通ずる水平
ダクト7を設けて形成されている。この垂直ダクト3の
間隔δはほぼ等間隔に構成されている。なお同図におい
て8は絶縁リング、9は外側絶縁筒である。FIG. 2 shows a conventional example of an SFs gas insulated transformer. As shown in the figure, the cylindrical winding 1 is arranged so that each winding unit (hereinafter referred to as a coil) 4 forms a plurality of vertical ducts 3 on the outer periphery of an inner insulating cylinder 2 wound around a core leg.
is wound with a vertical spacer 5 in between, horizontal spacers 6 are arranged at the upper and lower ends, and a horizontal duct 7 communicating with the vertical duct 3 is provided. The vertical ducts 3 are arranged at substantially equal intervals δ. In the figure, 8 is an insulating ring, and 9 is an outer insulating cylinder.
このように構成されたSF6ガス絶縁変圧器では、冷却
媒体は図中に矢印で示されているように巻線下部おいて
水平ダクト7から流入し、この流入した冷媒はコイル4
間の垂直ダクト3を上昇して各コイル4を冷却する。と
ころでこの冷媒流量は各垂直ダクト3でほぼ等しく、巻
線1の最内周側および最外周側の垂直ダクト3では与え
られる熱量が中央部の垂直ダクト3の約1/2と小さい
ため、冷却媒体の温度上昇が他の垂直ダク)3における
冷媒の温度上昇より小さくなる。最内周側および最外周
側の垂直ダクト3に与えられる熱量が中央部の垂直ダク
ト3の約1/2と小さいのは、中央部の垂直ダクト3に
与えられる熱量はその垂直ダクト3をはさんでいる両側
のコイル4から与えられるのに対し、最内周側および最
外周側の垂直ダクト3に与えられる熱量はその最内周側
または最外周側のコイル4から与えられるだけであるか
らである。In the SF6 gas insulated transformer configured in this way, the cooling medium flows from the horizontal duct 7 at the bottom of the winding as shown by the arrow in the figure, and this flowing cooling medium flows into the coil 4.
Each coil 4 is cooled by rising through a vertical duct 3 between them. By the way, this refrigerant flow rate is almost equal in each vertical duct 3, and the amount of heat given to the vertical ducts 3 on the innermost and outermost sides of the winding 1 is about 1/2 that of the vertical duct 3 in the center, so cooling is The temperature rise of the medium is smaller than the temperature rise of the refrigerant in the other vertical ducts (3). The reason why the amount of heat given to the vertical ducts 3 on the innermost and outermost sides is about 1/2 that of the vertical duct 3 in the center is that the amount of heat given to the vertical ducts 3 in the center is smaller than that of the vertical ducts 3 in the center. The amount of heat given to the vertical ducts 3 on the innermost and outermost sides is only given from the coils 4 on the innermost and outermost sides, whereas the heat is given from the coils 4 on both sides of the sandwich. It is.
従って各コイル4の平均温度上昇は縦軸に温度をとシ横
軸にコイル番号をとって温度とコイル番号との関係が示
されている第3図のように、最内周側のコイル(屋1)
および最外周側のコイル(屋4)の温度が低く、中央部
のコイル(崖2゜3)の温度が高く、各コイルの温度が
不均一になる傾向があった。Therefore, the average temperature rise of each coil 4 is shown in Figure 3, where the temperature is plotted on the vertical axis and the coil number is plotted on the horizontal axis, showing the relationship between temperature and coil number. Ya1)
Also, the temperature of the outermost coil (house 4) was low, and the temperature of the central coil (cliff 2°3) was high, and the temperature of each coil tended to be uneven.
本発明は以上の点に鑑みなされたものでおり、各コイル
の温度上昇を均等化することを可能としj
た静止誘導電器の巻線構造を提供することを目的とす
るものである〜
〔発明の概要〕
すなわち本発明は内側絶縁筒の外周に径方向に複数の垂
直ダクトを形成するように垂直スペーサを介して同心円
筒状に巻回された複数の円筒巻線またはシート巻線の巻
線単位を、前記垂直ダクトと連通し前記巻線単位の上下
端部に水平ダクトを形成する上、下水平スペーサ間に配
置した静止誘導電器の巻線構造において、最内周側およ
び最外周側の前記垂直ダクトの径方向寸法を、この他の
部分の前記垂直ダクトの径方向寸法より小さくしたこと
を特徴とするものであり、これによって最内周側および
最外周側の垂直ダクトの径方向寸法はこの他の部分の垂
直ダクトの径方向寸法より小さく形成されるようになる
。The present invention was made in view of the above points, and makes it possible to equalize the temperature rise of each coil.
It is an object of the present invention to provide a winding structure for a stationary induction electric appliance. upper and lower horizontal spacers that communicate a plurality of winding units of cylindrical windings or sheet windings wound in a concentric cylindrical shape with the vertical duct to form horizontal ducts at the upper and lower ends of the winding units; In the winding structure of the stationary induction electric device arranged between the coils, the radial dimension of the vertical ducts on the innermost and outermost periphery sides is smaller than the radial dimension of the vertical ducts in other parts. As a result, the radial dimensions of the vertical ducts on the innermost circumferential side and the outermost circumferential side are formed to be smaller than the radial dimensions of the vertical ducts on the other parts.
以下、図示した実施例に基づいて本発明を説明する。第
1図には本発明の一実施例が示されている。なお従来と
同じ部品には同じ符号を付したので説明を省略する。本
実施例では最内周側およびI&、A□。よ@l’、)
3゜□イオエ6.オ、。 fの他の部分の垂直ダ
クト3の径方向寸法δ2より小さくした。このようにす
ることにより最内周側および最外周側の垂直ダクト3の
径方向寸法δlはこの他の部分の垂直ダクト3の径方向
寸法δ2ることかできる。The present invention will be explained below based on the illustrated embodiments. FIG. 1 shows an embodiment of the invention. Note that parts that are the same as those in the conventional system are given the same reference numerals, and therefore their explanations will be omitted. In this embodiment, the innermost circumferential side, I&, and A□. Yo@l',)
3゜□Ioe6. Oh,. It is made smaller than the radial dimension δ2 of the vertical duct 3 in other parts of f. By doing this, the radial dimension δl of the vertical duct 3 on the innermost and outermost periphery sides can be made equal to the radial dimension δ2 of the vertical duct 3 on the other parts.
この垂直ダクト3の径方向寸法δ1.δ2は次に述べる
ようにして定めることができる。一般に垂直ダクト3の
冷媒流量Q(m”/S)は、垂直ダクト3相互間の圧力
損失h(■Aq)が等しくなるように配分される。垂直
ダクト3の圧力損失りは、垂直ダクト3を第4図にも示
されているように径方向寸法δ(m)、長さL (m)
、奥行方向の長さW (m )の矩形ダクトとみなすこ
とができ、0)式を川伝て近似的に求めることができる
。The radial dimension δ1 of this vertical duct 3. δ2 can be determined as described below. Generally, the refrigerant flow rate Q (m"/S) of the vertical ducts 3 is distributed so that the pressure loss h (■Aq) between the vertical ducts 3 is equal. The pressure loss of the vertical ducts 3 is As shown in Fig. 4, the radial dimension δ (m) and the length L (m)
, and can be regarded as a rectangular duct with a length in the depth direction W (m ), and equation 0) can be approximately obtained by following the river.
ここでγは冷媒の比重量(K9/m” )、gは重力加
速度(m/S2 )、λは管摩擦損失係数である。Here, γ is the specific weight of the refrigerant (K9/m''), g is the gravitational acceleration (m/S2), and λ is the pipe friction loss coefficient.
普通8Fgガスのように粘度が小さい冷媒では流量Qが
多少変化しても管摩擦損失係数λはほぼ一定の値となる
。従って(1)式のλL/4gW”の値も本考察におい
ては一定と考えて4よい。このλL/4gW’の値をC
とすれば、圧力損失りは(2)式で表わされ、Q2/δ
8に比例する。In the case of a refrigerant with a low viscosity such as 8Fg gas, the pipe friction loss coefficient λ remains approximately constant even if the flow rate Q changes somewhat. Therefore, the value of λL/4gW' in equation (1) can also be considered constant in this discussion.The value of λL/4gW' can be
Then, the pressure loss is expressed by equation (2), and Q2/δ
Proportional to 8.
一方、最内周側および最外周側の垂直ダクト3に加えら
れる熱量は上述のように中央部の垂直ダクト3の約1/
2になっているので、各垂直ダクト3の冷媒の温度上昇
を均等にするには、最内周側および最外周側の垂直ダク
ト3を流れる流量もこの他の中央部垂直ダクト3の流量
の約1/2にする必要がある。これを実現するには(2
)式において、圧力損失りが一定の条件で冷媒流量Qを
1/2にした場合の垂直ダクト3の径方向寸法(間隔)
δ1を求めればよい。そしてこの他の部分である中央部
の垂直ダクト3の径方向寸法(間−)を上述のようにδ
2とすれば、
(1/2Q>” / al” = Q”/ δ、s
・(3)となる。従って、
となり、最内周側および最外周側の垂直ダクト3の径方
向寸法δ1とこの他の部分の垂直ダクト3の径方向寸法
δ2との関係が得られる。そして実際の製品の製作にお
いて、垂直ダクト3の冷媒流量Qのばらつきとして±2
0−程度が許容されるとすれば、垂直ダクト間隔に関す
る許容値は(5)式%式%
従ってδ1とδ2との関係は理論的には(4)式の値と
なるが、実用的には(5)式で与えられる範囲に設定さ
れる。On the other hand, the amount of heat applied to the innermost and outermost vertical ducts 3 is about 1/1 of that of the central vertical duct 3, as described above.
2, so in order to equalize the temperature rise of the refrigerant in each vertical duct 3, the flow rate flowing through the innermost and outermost vertical ducts 3 should also be equal to the flow rate of the other central vertical ducts 3. It needs to be reduced to about 1/2. To achieve this (2
) formula, the radial dimension (spacing) of the vertical duct 3 when the refrigerant flow rate Q is halved under the condition that the pressure loss is constant.
All you have to do is find δ1. The other part, the radial dimension (distance) of the vertical duct 3 in the center, is set to δ as described above.
2, (1/2Q>”/al”=Q”/δ, s
・(3) becomes. Therefore, the relationship between the radial dimension δ1 of the vertical duct 3 on the innermost circumferential side and the outermost circumferential side and the radial direction dimension δ2 of the vertical duct 3 in other parts is obtained. In the actual manufacturing of the product, the variation in the refrigerant flow rate Q of the vertical duct 3 is ±2.
If approximately 0 is allowed, then the permissible value for the vertical duct spacing is (5) formula % formula % Therefore, the relationship between δ1 and δ2 is theoretically the value of formula (4), but in practice is set within the range given by equation (5).
、 このユうに最内周側および最外周
側の垂直ダクト3の径方向寸法δ、をこの他の部分の垂
直ダクト3の径方向寸法δ3より小さくすることにより
、最内周側および最外周側の垂直ダクト3を流れる冷媒
の流量を減少させ、その分だけ中央部の垂直ダクト3を
流れる冷媒流量を増加させることかできるようになる。, By making the radial dimension δ of the vertical duct 3 on the innermost and outermost peripheral sides smaller than the radial dimension δ3 of the vertical duct 3 in other parts, the innermost and outermost peripheral It becomes possible to reduce the flow rate of refrigerant flowing through the vertical duct 3 in the center, and increase the flow rate of refrigerant flowing through the vertical duct 3 in the center by that amount.
すなわち各垂直ダクト3に与えられる熱量の大小に応じ
て冷媒の流量が調整できるようになって、各垂直ダクト
3における冷媒の温度上昇を均等化することができるよ
うになシ、縦軸に温度をとり、横軸にコイル番号をとっ
て温度とコイル番号との関係が示されている第5図にも
示されているように、各コイル4の温度上昇を均等にす
ることができる。そして巻線1全体の径方向寸法を殆ん
ど増加させることなく巻線1の温度分布が均等化できる
ので、最も高い所の温度上昇が低下した分だけ冷却器台
数の減少や電流密度の増大により、静止誘導電器全体が
小型化できる。In other words, the flow rate of the refrigerant can be adjusted according to the amount of heat given to each vertical duct 3, and the temperature rise of the refrigerant in each vertical duct 3 can be equalized. As shown in FIG. 5, where the relationship between temperature and coil number is shown by taking the coil number on the horizontal axis, the temperature rise of each coil 4 can be made equal. Furthermore, since the temperature distribution of the winding 1 can be equalized without increasing the radial dimension of the entire winding 1, the number of coolers can be reduced and the current density can be increased by the reduction in temperature rise at the highest point. As a result, the entire stationary induction appliance can be downsized.
なお全体の垂直ダクト30寸法は、例えば周辺部の垂直
ダクト3を従来構造より小さくした場合には、中央部の
垂直ダクト3を従来構造より太きくとつ−〔、全体の冷
媒の流量を減少させないよう 11に設定
してもよい。Note that the dimensions of the entire vertical duct 30 are such that, for example, if the vertical duct 3 at the periphery is made smaller than the conventional structure, the vertical duct 3 at the center is made thicker than the conventional structure, which reduces the overall refrigerant flow rate. You may set it to 11 to prevent this.
なおまた本実施例は円筒巻線の場合について説明したが
、シート巻線の場合も同様にして実施できるととは云う
までもない。Furthermore, although this embodiment has been described in the case of a cylindrical winding, it goes without saying that the same can be applied to the case of a sheet winding.
上述のように本発明は各垂直ダクトに与えられる熱量の
大小に応じて冷媒が流れるようになって、各コイルの温
度上昇を均等化することができるようKなシ、各コイル
の温度上昇を均等化することを可能とした静止誘導電器
の巻線構造を得ることができる。As described above, the present invention allows the refrigerant to flow in accordance with the amount of heat given to each vertical duct, so that the temperature rise in each coil can be equalized. It is possible to obtain a winding structure for a stationary induction appliance that enables equalization.
第1図は本発明の静止誘導電器の巻線構造の一実施例の
縦断側面図、第2図は従来の静止誘導電器の巻線構造の
縦断側面図、第3図は従来の静止誘導電器の巻線構造の
径方向の温度分布図、第4図は本発明の静止誘導電器の
巻線構造の一実施例の垂直ダクトの斜視図、第5図は同
じく一実施例の径方向の温度分布図である。
1・・・円筒巻線、2・・・内側絶縁筒、3・・・垂直
ダクト、4・・・コイル(巻線単位)、5・・・垂直ス
ペーサ、6・・・水平スペーサ、7・・・水平ダクト、
9川外側絶縁筒、δl・・・最内周および最外周側の垂
直ダクトの径方向寸法、δ2・・−最内周および最外周
側以外の垂直ダクトの径方向寸法。FIG. 1 is a vertical side view of an embodiment of the winding structure of a stationary induction electric appliance according to the present invention, FIG. FIG. 4 is a perspective view of a vertical duct of an embodiment of the winding structure of the stationary induction electric appliance of the present invention, and FIG. 5 is a radial temperature distribution diagram of the winding structure of the present invention. It is a distribution map. DESCRIPTION OF SYMBOLS 1... Cylindrical winding, 2... Inner insulating tube, 3... Vertical duct, 4... Coil (winding unit), 5... Vertical spacer, 6... Horizontal spacer, 7...・Horizontal duct,
9 Outer insulation cylinder, δl...Radial dimension of the vertical duct on the innermost and outermost periphery sides, δ2...-Radial dimension of the vertical ducts other than the innermost and outermost periphery sides.
Claims (1)
成するように垂直スペーサを介して同心円筒状に巻回さ
れた複数の円筒巻線またはシート巻線の巻線単位を、前
記垂直ダクトと連通し前記巻線単位の上下端部に水平ダ
クトを形成する上、下水平スペーサ間に配置した静止誘
導電器の巻線構造において、最内周側および最外周側の
前記垂直ダクトの径方向寸法を、この他の部分の前記垂
直ダクトの径方向寸法より小さくしたことを特徴とする
静止誘導電器の巻線構造。1. Winding units of a plurality of cylindrical windings or sheet windings that are wound in a concentric cylindrical shape via vertical spacers so as to form a plurality of vertical ducts in the radial direction on the outer circumference of the inner insulating cylinder, In a winding structure of a stationary induction appliance arranged between upper and lower horizontal spacers that communicate with a duct to form a horizontal duct at the upper and lower ends of the winding unit, the diameter of the vertical duct on the innermost and outermost sides. A winding structure for a stationary induction electric appliance, characterized in that the directional dimension is smaller than the radial dimension of the vertical duct in other parts.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP12960384A JPS618909A (en) | 1984-06-22 | 1984-06-22 | Winding construction of stationary induction electric apparatus |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP12960384A JPS618909A (en) | 1984-06-22 | 1984-06-22 | Winding construction of stationary induction electric apparatus |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS618909A true JPS618909A (en) | 1986-01-16 |
| JPH0351083B2 JPH0351083B2 (en) | 1991-08-05 |
Family
ID=15013538
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP12960384A Granted JPS618909A (en) | 1984-06-22 | 1984-06-22 | Winding construction of stationary induction electric apparatus |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS618909A (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US10438734B2 (en) | 2015-08-14 | 2019-10-08 | Abb Schweiz Ag | Cooling of a static electric induction system |
Citations (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS4116508Y1 (en) * | 1964-09-12 | 1966-07-30 |
-
1984
- 1984-06-22 JP JP12960384A patent/JPS618909A/en active Granted
Patent Citations (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS4116508Y1 (en) * | 1964-09-12 | 1966-07-30 |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US10438734B2 (en) | 2015-08-14 | 2019-10-08 | Abb Schweiz Ag | Cooling of a static electric induction system |
Also Published As
| Publication number | Publication date |
|---|---|
| JPH0351083B2 (en) | 1991-08-05 |
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