Deprecated: The each() function is deprecated. This message will be suppressed on further calls in /home/zhenxiangba/zhenxiangba.com/public_html/phproxy-improved-master/index.php on line 456
JP5001225B2 - Static induction machine - Google Patents
[go: Go Back, main page]

JP5001225B2 - Static induction machine - Google Patents

Static induction machine Download PDF

Info

Publication number
JP5001225B2
JP5001225B2 JP2008169811A JP2008169811A JP5001225B2 JP 5001225 B2 JP5001225 B2 JP 5001225B2 JP 2008169811 A JP2008169811 A JP 2008169811A JP 2008169811 A JP2008169811 A JP 2008169811A JP 5001225 B2 JP5001225 B2 JP 5001225B2
Authority
JP
Japan
Prior art keywords
tank
rib
heat
cooling medium
outside air
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 - Fee Related
Application number
JP2008169811A
Other languages
Japanese (ja)
Other versions
JP2010010511A (en
Inventor
則行 林
尚英 松尾
和元 福井
賢治 中ノ上
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Hitachi Industrial Equipment Systems Co Ltd
Original Assignee
Hitachi Industrial Equipment Systems Co Ltd
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Application filed by Hitachi Industrial Equipment Systems Co Ltd filed Critical Hitachi Industrial Equipment Systems Co Ltd
Priority to JP2008169811A priority Critical patent/JP5001225B2/en
Publication of JP2010010511A publication Critical patent/JP2010010511A/en
Application granted granted Critical
Publication of JP5001225B2 publication Critical patent/JP5001225B2/en
Expired - Fee Related legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Images

Landscapes

  • Transformer Cooling (AREA)

Description

本発明は変圧器やリアクトルなどの静止誘導電器に係り、特に、電器本体を収納するタンク内に冷却媒体を充填しタンク外面に複数の放熱リブを備えた静止誘導電器に関する。   The present invention relates to a static induction appliance such as a transformer or a reactor, and more particularly to a static induction appliance in which a cooling medium is filled in a tank that houses an electric appliance body and a plurality of heat radiation ribs are provided on the outer surface of the tank.

電器本体を収納するタンク内に冷却媒体を充填しタンク外面に複数の放熱リブを備えた静止誘導電器は、例えば特許文献1に開示されているように、既に提案されている。   A static induction electric appliance in which a cooling medium is filled in a tank that houses an electric appliance main body and a plurality of heat radiating ribs are provided on the outer surface of the tank has already been proposed, as disclosed in, for example, Japanese Patent Application Laid-Open No. H10-228707.

特開平1−108713号公報JP-A-1-108713

上記特許文献1に記載の静止誘導電器は、図11及び図12に示すように、電器本体1が収納されたタンク4の周壁の周囲にタンク4の高さ方向に長い複数の放熱リブ15を形成している。前記放熱リブ15は、前記タンク4に充填した冷却媒体8が流通できるように前記タンク4内に臨んで開口する空間15Aが形成されている。   As shown in FIGS. 11 and 12, the stationary induction device described in Patent Document 1 includes a plurality of heat radiation ribs 15 that are long in the height direction of the tank 4 around the peripheral wall of the tank 4 in which the main body 1 is housed. Forming. The heat radiating rib 15 is formed with a space 15 </ b> A that opens into the tank 4 so that the cooling medium 8 filled in the tank 4 can flow therethrough.

このように構成された静止誘導電器においては、電器本体1から発生した損失により発熱して昇温するが、これらの熱は冷却媒体8に伝えられて冷却される。そして熱を吸収した冷却媒体8は、放熱リブ15の空間15Aを流通することで、吸収した熱をタンク4の外部に放出する。   In the static induction appliance configured as described above, the heat is generated by the loss generated from the electric appliance body 1 and the temperature rises. However, the heat is transmitted to the cooling medium 8 and cooled. Then, the cooling medium 8 that has absorbed the heat flows through the space 15 </ b> A of the heat radiating rib 15, thereby releasing the absorbed heat to the outside of the tank 4.

ところで、電器本体1の近傍の冷却媒体8は、伝わった熱により昇温して密度が小さくなり、矢印で示すように、タンク4内を上昇する。一方、タンク4の上方の昇温された冷却媒体8は、電器本体1から離れているタンク4の周壁や放熱リブ15を通して外部の空気Aによって冷却される。冷却されて温度が低下した冷却媒体8は密度が大きくなるので、タンク4や放熱リブ15に沿ってタンク4の下方に向って流れる。タンク4の下方に至った冷却媒体8は、再び電器本体1から熱を奪い、上方に向って流れを生じ、タンク4内を自然対流によりa→b→c→d→e→aの順に循環する。   By the way, the cooling medium 8 in the vicinity of the electric appliance main body 1 rises in temperature due to the transmitted heat, and its density decreases, and as shown by the arrow, it rises in the tank 4. On the other hand, the heated cooling medium 8 above the tank 4 is cooled by the external air A through the peripheral wall of the tank 4 and the heat dissipating ribs 15 that are separated from the main body 1. Since the cooling medium 8 that has been cooled to lower the temperature has a higher density, it flows along the tank 4 and the heat radiating ribs 15 toward the lower side of the tank 4. The cooling medium 8 reaching the lower side of the tank 4 again takes heat from the electric body 1 and generates a flow upward, and circulates in the tank 4 in the order of a → b → c → d → e → a by natural convection. To do.

一般的に、冷却媒体8が自然対流する駆動力ΔPdriveは、冷却媒体8の比重量γ、体積膨張率β、放熱リブ15の中心高さと巻線中心高さの差Δh、冷却媒体8のタンク上下部における温度差Δθを用いて、ΔPdrive=γ・β・Δh・Δθで表されるとされている。   In general, the driving force ΔPdrive for natural convection of the cooling medium 8 includes the specific weight γ of the cooling medium 8, the volume expansion coefficient β, the difference Δh between the center height of the heat radiating rib 15 and the winding center height, and the tank of the cooling medium 8. It is assumed that ΔPdrive = γ · β · Δh · Δθ is expressed by using the temperature difference Δθ between the upper and lower portions.

図11に示す冷却媒体8の自然対流によるa→b→c→d→e→aの循環に対応したタンク4の高さ方向における冷却媒体8の位置と温度との関係を表したのが図13である。この図13において、面積o−b−c,d−oから面積o−a−e−oを引いた値がΔh・Δθと等しくなり、この差し引いた値が駆動力ΔPdriveに比例する。   The relationship between the position of the cooling medium 8 and the temperature in the height direction of the tank 4 corresponding to the circulation of a → b → c → d → e → a by natural convection of the cooling medium 8 shown in FIG. 11 is shown. 13. In FIG. 13, a value obtained by subtracting the area oa-eo from the areas oc-c and d-o is equal to Δh · Δθ, and this subtracted value is proportional to the driving force ΔPdrive.

ところが、実際の静止誘導電器である変圧器を用いて行った温度上昇試験において、タンク4の高さ方向の各位置における冷却媒体8である絶縁油の温度を詳細に測定した結果、放熱リブ15内を下降する絶縁油の温度変化は、図13のc,d−o−eに示す直線的な温度低下ではなく、図14に示すc,d−o−eのように、タンク4の上部での温度低下が小さく、タンク4の下方部で急激に温度が低下することが判った。   However, as a result of measuring in detail the temperature of the insulating oil that is the cooling medium 8 at each position in the height direction of the tank 4 in a temperature rise test performed using a transformer that is an actual static induction electric appliance, The temperature change of the insulating oil descending inside is not the linear temperature decrease shown in c, d-oe in FIG. 13 but the upper part of the tank 4 like c, d-oe shown in FIG. It was found that the temperature drop at the bottom of the tank 4 was small, and the temperature suddenly dropped at the lower part of the tank 4.

これらのことから、自然対流を引き起こす冷却媒体8の駆動力は、図14における面積o−b−c,d−oから面積o−a−e−oを引いた値に比例するため、冷却媒体8の循環流量は、一般的に考慮されていたよりも実際は少なくなっている。   From these facts, the driving force of the cooling medium 8 causing the natural convection is proportional to the value obtained by subtracting the area oa-eo from the areas obac, do in FIG. The circulating flow rate of 8 is actually less than generally considered.

以上から、タンク4の上下部における冷却媒体8の温度差が大きくなって、タンク4の上部における冷却媒体8の温度が高くなり、電器本体1の冷却を十分に行えない問題がある。   From the above, there is a problem that the temperature difference of the cooling medium 8 at the upper and lower parts of the tank 4 becomes large, the temperature of the cooling medium 8 at the upper part of the tank 4 becomes high, and the electric appliance body 1 cannot be sufficiently cooled.

このように放熱リブ15内を下降する冷却媒体8の温度がタンク4の上方部では僅かしか低下せず、下方部において急激に低下する理由を、図15に基づいて説明する。   The reason why the temperature of the cooling medium 8 descending in the heat radiating rib 15 in this way only slightly decreases in the upper part of the tank 4 and rapidly decreases in the lower part will be described with reference to FIG.

隣接する冷却リブ15間に下端部から流入した空気Aは、上端部に至るまで放熱リブ15に接触しているので、放熱リブ15の周囲の空気Aの温度分布15Iは二点差線に示すようになり、放熱リブ15の上方に行くにしたがって昇温した空気Aの分布が広くなる。このため、放熱リブ15の上方部では温度の低い外気での冷却は望めず冷却媒体8からの熱の伝達は少ない。一方、放熱リブ15の下方部では空気Aの温度が低いので昇温した空気Aの分布は狭く冷却媒体8からの熱の伝達が多くなる。したがって、放熱リブ15内を下降する冷却媒体8の温度はタンク4の上方部では僅かしか低下せず、下方部において急激に低下するのである。   Since the air A flowing in from the lower end between the adjacent cooling ribs 15 is in contact with the heat radiating rib 15 until reaching the upper end, the temperature distribution 15I of the air A around the heat radiating rib 15 is shown by a two-dotted line. And the distribution of the heated air A becomes wider as it goes above the heat radiating rib 15. For this reason, cooling with outside air having a low temperature cannot be expected in the upper part of the heat radiating rib 15, and heat transfer from the cooling medium 8 is small. On the other hand, since the temperature of the air A is low in the lower part of the heat radiating rib 15, the distribution of the heated air A is narrow and the heat transfer from the cooling medium 8 is increased. Therefore, the temperature of the cooling medium 8 descending in the heat radiating rib 15 is only slightly lowered at the upper part of the tank 4 and is rapidly lowered at the lower part.

本発明の目的は、放熱リブの上方部においても冷却媒体の冷却を十分に行うことで、タンク内を冷却媒体が自然対流する駆動力を増加させ、全体の冷却性能を向上することができる静止誘導電器を提供することにある。   The object of the present invention is to sufficiently cool the cooling medium also in the upper part of the heat radiating rib, thereby increasing the driving force for the natural convection of the cooling medium in the tank and improving the overall cooling performance. It is to provide an induction machine.

本発明は上記目的を達成するために、電器本体を収容し内部に冷却媒体を充填したタンクの周壁の周囲に上下方向に長い放熱リブを複数設け、隣接する放熱リブ間の高さ方向の中間部に、放熱リブ間に沿って上方に流れる外気を撹乱する外気撹乱手段を設けたのである。   In order to achieve the above object, the present invention provides a plurality of vertically extending heat dissipating ribs around the peripheral wall of a tank that contains an electric body and is filled with a cooling medium, and is located in the height direction between adjacent heat dissipating ribs. The outside air disturbing means for disturbing the outside air flowing upward along the space between the heat radiating ribs is provided in the section.

上述のように、外気撹乱手段を設けたので、冷却リブの下方部を冷却して昇温した外気が途中で外気撹乱手段により乱され、これによって周囲の温度が低い外気が放熱リブ間に呼び込まれて混じるので昇温した外気の温度を低下させる。そして、この温度が下がった外気によって放熱リブの上方部を冷却することができる。その結果、放熱リブ上方部の周囲の昇温した外気の分布は、放熱リブ下方部における昇温した外気の分布に接近するようになり、冷却媒体の冷却を促進してタンク内を自然対流する冷却媒体の駆動力を増加させることができるのである。   As described above, since the outside air disturbing means is provided, the outside air heated by cooling the lower portion of the cooling rib is disturbed by the outside air disturbing means in the middle, and thereby the outside air having a low ambient temperature is called between the heat dissipating ribs. Since it is mixed and mixed, the temperature of the heated outside air is lowered. And the upper part of a thermal radiation rib can be cooled with the external air which this temperature fell. As a result, the distribution of the heated outside air around the upper portion of the heat dissipating rib comes closer to the distribution of the heated air at the lower portion of the heat dissipating rib, which promotes cooling of the cooling medium and causes natural convection in the tank. The driving force of the cooling medium can be increased.

以上説明したように本発明によれば、放熱リブの上方部においても冷却媒体の冷却を十分に行うことで、タンク内を冷却媒体が自然対流する駆動力を増加させ、全体の冷却性能を向上することができる静止誘導電器を得ることができる。   As described above, according to the present invention, the cooling medium is sufficiently cooled even in the upper part of the heat radiating rib, thereby increasing the driving force for the natural convection of the cooling medium in the tank and improving the overall cooling performance. A static induction device that can be obtained can be obtained.

以下本発明による静止誘導電器の第1の実施の形態を、図1及び図2に示す変圧器に基づいて説明する。   Hereinafter, a first embodiment of a static induction apparatus according to the present invention will be described based on a transformer shown in FIGS. 1 and 2.

本実施の形態による変圧器は、鉄心2に装着された巻線3とからなる電器本体1と、この電器本体1を収納するタンク4と、このタンク内に充填された絶縁油,空気,窒素ガス,6弗化硫黄ガス等の冷却媒体8とから構成され、前記タンク4の周壁には冷却媒体8を流通させる空間5A,6Aを内部に形成した下方放熱リブ5と上方放熱リブ6とが設けられている。   The transformer according to the present embodiment includes an electric body 1 composed of a winding 3 attached to an iron core 2, a tank 4 that houses the electric body 1, and insulating oil, air, and nitrogen filled in the tank. The lower heat-dissipating rib 5 and the upper heat-dissipating rib 6 are formed in the peripheral wall of the tank 4 and have spaces 5A and 6A through which the coolant 8 flows. Is provided.

下方放熱リブ5と上方放熱リブ6の空間5A,6Aは、夫々タンク4の内部に臨んで開口しており、冷却媒体8がタンク4内とこれら空間5A,6A内を流通するようにしている。また、下方放熱リブ5と上方放熱リブ6は、タンク4の周壁の回りに複数設けられていると共に、タンク4の周壁の高さ方向に沿って同一線上に並んで形成されている。   The spaces 5A, 6A of the lower heat radiating rib 5 and the upper heat radiating rib 6 are opened facing the inside of the tank 4, respectively, so that the cooling medium 8 flows through the tank 4 and the spaces 5A, 6A. . A plurality of the lower radiating ribs 5 and the upper radiating ribs 6 are provided around the peripheral wall of the tank 4, and are formed side by side along the same line along the height direction of the peripheral wall of the tank 4.

そして、下方放熱リブ5と上方放熱リブ6との間には、前記タンク4の周方向に連続した空気流路7が形成されている。   An air flow path 7 continuous in the circumferential direction of the tank 4 is formed between the lower heat radiating rib 5 and the upper heat radiating rib 6.

本実施の形態による変圧器は上記構成としたことにより、電器本体1での発熱は、冷却媒体8の自然対流によってタンク4や下方放熱リブ5及び上方放熱リブ6に伝達され、タンク4や下方放熱リブ5及び上方放熱リブ6の外面に接触して流れる外気A1,A2によって冷却される。   Since the transformer according to the present embodiment has the above-described configuration, heat generated in the electric body 1 is transmitted to the tank 4, the lower radiating rib 5, and the upper radiating rib 6 by natural convection of the cooling medium 8. Cooling is performed by the outside air A <b> 1 and A <b> 2 flowing in contact with the outer surfaces of the heat radiating rib 5 and the upper heat radiating rib 6.

このときの外気A1,A2の流れは、図3に示すようになる。即ち、隣接する下方放熱リブ5間に下方から流入する外気A1は、下方放熱リブ5の外面からの熱を奪って昇温して徐々に密度が小さくなり、自然対流によって下方放熱リブ5近傍を層状になって上方に向って流れる。下方放熱リブ5に接する外気A1は、下方放熱リブ5の下端から上端に至るまで常に接触しているので、下方放熱リブ5に接して昇温した外気A1は下端で狭く上端で広くなる温度分布5Iとなる。   The flow of the outside air A1, A2 at this time is as shown in FIG. That is, the outside air A1 flowing from below between the adjacent lower radiating ribs 5 is deprived of heat from the outer surface of the lower radiating ribs 5 and gradually decreases in density. Layered and flows upward. Since the outside air A1 in contact with the lower radiating rib 5 is always in contact from the lower end to the upper end of the lower radiating rib 5, the outside air A1 heated in contact with the lower radiating rib 5 has a temperature distribution that is narrow at the lower end and wide at the upper end. 5I.

したがって、下方放熱リブ5と上方放熱リブ6とが上下に連なる一体構成の場合には、上方放熱リブ6の近傍に上昇してきた昇温された外気の温度分布はかなり広くなる。そのために、タンク4の上方部における冷却媒体8の温度と外気温度とが近接してしまい、その結果、昇温した冷却媒体8の熱を、上方放熱リブ6を介して外気に伝達する効率が低下し、昇温した冷却媒体8を十分に冷却することができなくなる。   Therefore, in the case of an integrated configuration in which the lower heat radiating rib 5 and the upper heat radiating rib 6 are vertically connected, the temperature distribution of the heated outside air rising in the vicinity of the upper heat radiating rib 6 is considerably widened. Therefore, the temperature of the cooling medium 8 in the upper part of the tank 4 and the outside air temperature are close to each other. As a result, the efficiency of transferring the heat of the raised cooling medium 8 to the outside air via the upper heat radiation rib 6 is improved. The temperature of the cooling medium 8 is lowered and cannot be sufficiently cooled.

この点、本実施の形態によれば、下方放熱リブ5近傍の昇温された外気A1の温度分布5Iが広くなる前に、下方放熱リブ5と上方放熱リブ6との間に、外気を撹乱する外気撹乱手段である空気流路7が形成されているので、隣接する下方放熱リブ5間やその近傍を層状になって上方に向って流れる外気A1は、空気流路7に流れ込む温度の低い外気A3によって流れが撹乱される。即ち、隣接する下方放熱リブ5間を昇温しながら上昇してきた外気A1は、空気流路7部で昇温していない外気A3によって撹乱されて混合し、それによって高くなった温度が低下する。   In this regard, according to the present embodiment, the outside air is disturbed between the lower heat release rib 5 and the upper heat release rib 6 before the temperature distribution 5I of the heated outside air A1 in the vicinity of the lower heat release rib 5 becomes wider. Since the air flow path 7 that is the outside air disturbing means is formed, the outside air A1 that flows between the adjacent lower heat radiation ribs 5 and the vicinity thereof in a layered manner and flows upward is low in temperature flowing into the air flow path 7. The flow is disturbed by the outside air A3. That is, the outside air A1 that has risen while raising the temperature between the adjacent lower heat radiation ribs 5 is disturbed and mixed by the outside air A3 that has not risen in temperature in the air flow path 7 part, thereby lowering the increased temperature. .

撹乱によって温度が低下した空気は外気A2となって隣接する上方放熱リブ6間に流れ込み、前述の上方放熱リブ6に沿って上昇し、下方放熱リブ5の外気A1と相似の温度分布6Iとなって冷却媒体8の冷却を行うことができる。   The air whose temperature has decreased due to the disturbance becomes the outside air A2 and flows between the adjacent upper heat dissipating ribs 6, rises along the above upper heat dissipating ribs 6, and has a temperature distribution 6I similar to the outside air A1 of the lower heat dissipating ribs 5. Thus, the cooling medium 8 can be cooled.

その結果、下から上まで連続して形成された放熱リブに比べて、上方放熱リブ6を冷却する外気A2の温度を低くすることができる。また、上方放熱リブ6は、外気A2による冷却が上方放熱リブ6の下端から発生するため、上方放熱リブ6近傍の高さ方向における昇温した外気A2の温度分布6Iは下方放熱リブ5の温度分布5Iと相似になる。その結果、タンク4の上方部における冷却媒体8の温度と上方放熱リブ6の近傍の外気A2の温度との温度差が大きくなり、上方放熱リブ6から多くの熱が外気A2に伝わり、タンク4の上方部における昇温した冷却媒体8を十分に冷却することができる。   As a result, the temperature of the outside air A2 that cools the upper heat radiation rib 6 can be lowered as compared with the heat radiation rib formed continuously from the bottom to the top. Further, since the upper heat radiation rib 6 is cooled by the outside air A2 from the lower end of the upper heat radiation rib 6, the temperature distribution 6I of the heated outside air A2 in the height direction near the upper heat radiation rib 6 is the temperature of the lower heat radiation rib 5. Similar to distribution 5I. As a result, the temperature difference between the temperature of the cooling medium 8 in the upper part of the tank 4 and the temperature of the outside air A2 in the vicinity of the upper radiating rib 6 becomes large, and a large amount of heat is transferred from the upper radiating rib 6 to the outside air A2. It is possible to sufficiently cool the heated cooling medium 8 in the upper part of the.

以上から、タンク4と下方放熱リブ5及び上方放熱リブ6内を循環する冷却媒体8の温度変化は、図4に示すようになる。即ち、タンク4内を上昇する冷却媒体8の各位置における温度変化は、a−b−c,dとなって従来と変わらないが、下方放熱リブ5及び上方放熱リブ6内を下降する冷却媒体8の各位置における温度変化は、c,d−e,f−g,h−iとなり、ほぼ直線状に温度が低下することになる。これは図13に示す温度変化に近似する温度変化となり、面積o−b−c,d−e,f−g,h−0から面積o−a−i−oを差し引いた値が大きくなり、それに比例して冷却媒体8の自然対流の駆動力が増大するので、冷却媒体8の循環流量を増加させることができる。   From the above, the temperature change of the cooling medium 8 circulating in the tank 4, the lower heat radiating rib 5, and the upper heat radiating rib 6 is as shown in FIG. That is, the temperature change at each position of the cooling medium 8 rising in the tank 4 is abc, d, which is the same as the conventional one, but the cooling medium descending in the lower heat radiation rib 5 and the upper heat radiation rib 6. The change in temperature at each position of 8 is c, de, fg, and hi, and the temperature is reduced substantially linearly. This is a temperature change that approximates the temperature change shown in FIG. 13, and a value obtained by subtracting the area oaio from the areas obac, de, fg, and h-0 increases. Since the driving force of the natural convection of the cooling medium 8 increases in proportion thereto, the circulation flow rate of the cooling medium 8 can be increased.

冷却媒体8の循環流量の増加により、タンク4内の高さ方向における冷却媒体8の温度差が小さくなると共に、電器本体1から冷却媒体8への熱伝達率が大きくなる。それにより、電器本体1の温度上昇は抑えられ、変圧器の冷却性能を向上できるので、容量の増加や小型化を実現できる。   The increase in the circulation flow rate of the cooling medium 8 reduces the temperature difference of the cooling medium 8 in the height direction in the tank 4 and increases the heat transfer coefficient from the electric body 1 to the cooling medium 8. Thereby, the temperature rise of the electric body 1 can be suppressed and the cooling performance of the transformer can be improved, so that the capacity can be increased and the size can be reduced.

以上の実施の形態は、上下2分割した放熱リブ5,6の分割部にタンク4の周壁に沿って空気流路7を形成したものであるが、放熱リブを上下3分割以上にして空気流路を2つ以上形成するようにすることで、タンク4内の高さ方向における冷却媒体8の温度差をさらに小さくすることができ、さらに電器本体1から冷却媒体8への熱伝達率を大きくすることができる。   In the above embodiment, the air flow path 7 is formed along the peripheral wall of the tank 4 in the divided part of the heat radiating ribs 5 and 6 divided into the upper and lower parts. By forming two or more paths, the temperature difference of the cooling medium 8 in the height direction in the tank 4 can be further reduced, and the heat transfer rate from the electric appliance body 1 to the cooling medium 8 can be further increased. can do.

また、外気撹乱手段として、放熱リブ5,6間をタンク4の周壁の周囲に沿って貫く空気流路7を形成したが、放熱リブ5,6を一体化した構成において、放熱リブに上昇する外気の流れを阻止する障害物を設けて外気撹乱手段としたりして、周囲の温度の低い外気を混入するようにしてもよい。   Moreover, although the air flow path 7 which penetrates between the radiation ribs 5 and 6 along the circumference | surroundings of the surrounding wall of the tank 4 was formed as an external air disturbance means, in the structure which integrated the radiation ribs 5 and 6, it raises to a radiation rib. An obstacle that blocks the flow of outside air may be provided as outside air disturbing means, so that outside air having a low ambient temperature may be mixed.

さらに、放熱リブ5,6を一体化した構成において、放熱リブの高さ方向に中間部に、温度の低い外気を放熱リブ側に導入する外気導入手段を設け、昇温した外気の温度を低下させるようにしてもよい。   Further, in the structure in which the heat radiating ribs 5 and 6 are integrated, an outside air introduction means for introducing outside air having a low temperature to the heat radiating rib side is provided in the middle portion in the height direction of the heat radiating ribs to lower the temperature of the heated outside air. You may make it make it.

次に、本発明による静止誘導電器の第2の実施の形態を、図5〜図7に示す変圧器に基づいて説明する。尚、図1〜図3の符号と同一符号は同一構成部品を示すので、再度の詳細な説明は省略する。   Next, a second embodiment of the static induction device according to the present invention will be described based on the transformer shown in FIGS. Since the same reference numerals as those in FIGS. 1 to 3 indicate the same components, detailed description thereof will not be repeated.

本実施の形態において、第1の実施の形態と異なる構成は、P1ピッチを有する下方放熱リブ5と、P1ピッチと同じピッチとなるP2ピッチを有する上方放熱リブ6とを、タンク4の周壁の周方向に対して1/2ピッチずらして設置した点である。   In the present embodiment, the configuration different from the first embodiment is that a lower heat radiating rib 5 having a P1 pitch and an upper heat radiating rib 6 having a P2 pitch that is the same as the P1 pitch are arranged on the peripheral wall of the tank 4. It is a point installed with a 1/2 pitch shift with respect to the circumferential direction.

このような構成では、隣接する下方放熱リブ5間を上昇してくる外気A1の内、昇温された外気の温度分布5Iの外側を流れる温度の低い外気A1が、上方放熱リブ6に沿って流れるようになるので、上方放熱リブ6に接触して流れる外気A2は、第1の実施の形態の外気A2よりも温度が低くなり、上方放熱リブ6近傍の昇温した外気A2の温度分布6Iを、より下方放熱リブ5近傍の温度分布5Iに近付けることができる。勿論、下方放熱リブ5と上方放熱リブ6との間に形成した空気流路7に流れ込む外気A3による外気A2の低温度化も考慮すると、第1の実施の形態に比べて変圧器の冷却性能はより向上できることは云うまでもない。   In such a configuration, of the outside air A1 rising between the adjacent lower heat radiating ribs 5, the low temperature outside air A1 flowing outside the temperature distribution 5I of the heated outside air along the upper heat radiating ribs 6. Since the outside air A2 flowing in contact with the upper radiating rib 6 becomes lower in temperature than the outside air A2 of the first embodiment, the temperature distribution 6I of the heated outside air A2 in the vicinity of the upper radiating rib 6 is increased. Can be made closer to the temperature distribution 5I in the vicinity of the lower heat radiation rib 5. Of course, considering the lower temperature of the outside air A2 due to the outside air A3 flowing into the air flow path 7 formed between the lower radiating rib 5 and the upper radiating rib 6, the cooling performance of the transformer as compared with the first embodiment. Needless to say, can be improved.

ところで、本実施の形態においては、下方放熱リブ5と上方放熱リブ6とを周方向に1/2ピッチずらしたものであるが、下方放熱リブ5と上方放熱リブ6とが周方向にずれていれば第1の実施の形態に比べて変圧器の冷却性能を向上できるので、必ずしも1/2ピッチずらすことに限定されるものではない。   By the way, in this embodiment, the lower radiating rib 5 and the upper radiating rib 6 are shifted by 1/2 pitch in the circumferential direction, but the lower radiating rib 5 and the upper radiating rib 6 are shifted in the circumferential direction. If so, the cooling performance of the transformer can be improved as compared with the first embodiment, and therefore, the present invention is not necessarily limited to being shifted by 1/2 pitch.

図8は、本発明による静止誘導電器の第3の実施の形態を示すもので、第1の実施の形態と異なる構成は、下方放熱リブ9と上方放熱リブ10の形状が異なる点である。   FIG. 8 shows a third embodiment of a static induction electric machine according to the present invention, and a configuration different from the first embodiment is that the shapes of the lower heat radiating rib 9 and the upper heat radiating rib 10 are different.

即ち、本実施の形態においては、上方放熱リブ10のタンク4の周壁からの張り出し寸法L2を下方放熱リブ9の張り出し寸法L1よりも大きく形成すると共に、上方放熱リブ10の高さ寸法H2を下方放熱リブ9の高さ寸法H1よりも大きく形成したのである。   That is, in the present embodiment, the projecting dimension L2 of the upper radiating rib 10 from the peripheral wall of the tank 4 is formed larger than the projecting dimension L1 of the lower radiating rib 9, and the height dimension H2 of the upper radiating rib 10 is set downward. It is formed larger than the height dimension H1 of the heat dissipating rib 9.

このように形成することで、上方放熱リブ10の冷却媒体8との伝熱面積が下方放熱リブ9よりも大きくなり、さらに、上方放熱リブ10の先端部は下方放熱リブ9を冷却し終えた外気の影響を受けないので、外気による冷却効率が向上するのである。   By forming in this way, the heat transfer area of the upper heat dissipation rib 10 with the cooling medium 8 is larger than that of the lower heat dissipation rib 9, and the tip of the upper heat dissipation rib 10 has finished cooling the lower heat dissipation rib 9. Since it is not affected by the outside air, the cooling efficiency by the outside air is improved.

尚、上方放熱リブ10の張り出し寸法L2と下方放熱リブ9の張り出し寸法L1とを同じにして上方放熱リブ10の高さ寸法H2を下方放熱リブ9の高さ寸法H1よりも大きく形成してもよく、上方放熱リブ10の高さ寸法H2と下方放熱リブ9の高さ寸法H1とを同じにして上方放熱リブ10のタンク4の張り出し寸法L2を下方放熱リブ9の張り出し寸法L1よりも大きく形成しても、第1の実施の形態と同等以上の効果を奏することができる。   Even if the protruding dimension L2 of the upper radiating rib 10 and the protruding dimension L1 of the lower radiating rib 9 are made the same, the height dimension H2 of the upper radiating rib 10 is made larger than the height dimension H1 of the lower radiating rib 9. Well, the height dimension H2 of the upper heat radiation rib 10 and the height dimension H1 of the lower heat radiation rib 9 are the same, and the projecting dimension L2 of the tank 4 of the upper heat radiation rib 10 is formed larger than the projecting dimension L1 of the lower heat radiation rib 9. Even so, an effect equal to or greater than that of the first embodiment can be obtained.

図9は、本発明による静止誘導電器の第4の実施の形態を示すもので、第1の実施の形態と異なる構成は、上方放熱リブ12のリブピッチを下方放熱リブ11のリブピッチよりも小さく、例えば1/2ピッチにしたものである。   FIG. 9 shows a fourth embodiment of a static induction electric machine according to the present invention. The structure different from the first embodiment is that the rib pitch of the upper heat radiating rib 12 is smaller than the rib pitch of the lower heat radiating rib 11. For example, the pitch is ½ pitch.

このように構成することで、上方放熱リブ12の冷却媒体8との伝熱面積は、下方放熱リブ11の伝熱面積のほぼ2倍になり、その分、上方放熱リブ12での冷却媒体8の降温作用を大きくすることができる。その結果、上方放熱リブ12内を下降する冷却媒体8の駆動力が増加して循環流量が多くなり、変圧器の冷却性能を第1や第2の実施の形態に比べてより向上させることができる。   With this configuration, the heat transfer area of the upper heat dissipating rib 12 with the cooling medium 8 is almost twice the heat transfer area of the lower heat dissipating rib 11. The temperature lowering effect can be increased. As a result, the driving force of the cooling medium 8 descending in the upper heat radiating rib 12 is increased, the circulation flow rate is increased, and the cooling performance of the transformer can be further improved as compared with the first and second embodiments. it can.

尚、本実施の形態を、第3の実施の形態のいずれかの構成、あるいは全部の構成と組み合わせて上方放熱リブ12の伝熱面積を下方放熱リブ11の伝熱面積よりも増加させることでも、冷却媒体8の駆動力を増加させて循環流量を多くし、変圧器の冷却性能をより向上させることができる。即ち、上方放熱リブの張り出し寸法を下方放熱リブよりも大きい、上方放熱リブの高さ寸法が下方放熱リブよりも大きい、隣接する上方放熱リブの間隔が下方放熱リブよりも狭い、の3つの構成のうち少なくとも1つの構成及び全部の構成の組み合わせ、または3つの構成からの選択的組み合わせは、変圧器の仕様や容量、さらには設置場所を考慮して設計製作することで、冷却性能をより向上させることができる。   The present embodiment may be combined with any one of the configurations of the third embodiment or the entire configuration to increase the heat transfer area of the upper heat dissipation rib 12 more than the heat transfer area of the lower heat dissipation rib 11. By increasing the driving force of the cooling medium 8 and increasing the circulation flow rate, the cooling performance of the transformer can be further improved. That is, there are three configurations in which the projecting dimension of the upper heat dissipation rib is larger than that of the lower heat dissipation rib, the height dimension of the upper heat dissipation rib is larger than that of the lower heat dissipation rib, and the interval between adjacent upper heat dissipation ribs is narrower than that of the lower heat dissipation rib. The combination of at least one and all of the configurations, or the selective combination from the three configurations, is designed and manufactured taking into consideration the specifications and capacity of the transformer, as well as the installation location, thereby further improving the cooling performance Can be made.

図10は、本発明による静止誘導電器の第5の実施の形態を示すもので、第1の実施の形態と異なる構成は、タンク4の周壁への放熱リブの取り付け範囲である。   FIG. 10 shows a fifth embodiment of the static induction electric machine according to the present invention, and a different configuration from the first embodiment is an attachment range of the heat radiation rib to the peripheral wall of the tank 4.

本実施の形態では、上方放熱リブ14のタンク4の周壁への取り付け範囲を、下方放熱リブ13の取り付け範囲よりも広範囲にしたのである。   In the present embodiment, the attachment range of the upper heat radiation rib 14 to the peripheral wall of the tank 4 is made wider than the attachment range of the lower heat radiation rib 13.

このように構成することで、上方放熱リブ14の数が下方放熱リブ13よりも多くなり、その結果、上方放熱リブ14の伝熱面積を下方放熱リブ13よりも大きくすることができ、結果的に、第3の実施の形態と同様な効果を奏することができる。   By configuring in this way, the number of the upper radiating ribs 14 is larger than that of the lower radiating ribs 13, and as a result, the heat transfer area of the upper radiating ribs 14 can be made larger than that of the lower radiating ribs 13. In addition, the same effects as those of the third embodiment can be obtained.

以上説明したように本発明の各実施の形態によれば変圧器の内部構造を変えることなく変圧器の冷却効率を向上させることができ、利用の可能性は極めて高い。   As described above, according to each embodiment of the present invention, the cooling efficiency of the transformer can be improved without changing the internal structure of the transformer, and the possibility of use is extremely high.

ところで、上記各実施の形態においては、放熱リブとして内側に空間が形成され、この空間をタンク4内に臨ませることで、冷却媒体8を空間内に流通させる構成を説明したが、放熱リブとして板材からなる放熱フィンを用いても本発明を適用できることは云うまでもない。また、各実施の形態は静止誘導電器として変圧器を一例に説明したが、例えばリアクトル等のように、電器本体がタンク内に収納され、タンク内に冷却媒体が充填され、しかもタンク周壁に放熱リブが設けられている静止誘導電器であれば本発明は適用できる。   By the way, in each said embodiment, although the space was formed inside as a heat radiating rib and the structure which distribute | circulates the cooling medium 8 in space by facing this space in the tank 4 was demonstrated, as a heat radiating rib, It goes without saying that the present invention can be applied even if a heat radiating fin made of a plate material is used. Each embodiment has been described by taking a transformer as an example of a static induction electric appliance. However, for example, as in a reactor, the electric appliance body is housed in a tank, the tank is filled with a cooling medium, and heat is radiated to the tank peripheral wall. The present invention can be applied to any static induction machine provided with a rib.

本発明による静止誘導電器の第1の実施の形態を示す変圧器の縦断面図。BRIEF DESCRIPTION OF THE DRAWINGS FIG. 1 is a longitudinal sectional view of a transformer showing a first embodiment of a static induction electric machine according to the present invention. 図1の外観図。The external view of FIG. 図2の放熱リブ近傍の温度分布と外気の流れを示す模式図。FIG. 3 is a schematic diagram showing a temperature distribution in the vicinity of a heat radiating rib in FIG. 2 and a flow of outside air. 図1の変圧器内部の冷却媒体の各位置における温度を示す関係図。FIG. 2 is a relationship diagram illustrating temperatures at respective positions of a cooling medium inside the transformer of FIG. 1. 本発明による静止誘導電器の第2の実施の形態を示す変圧器の図2相当図。FIG. 2 is a diagram corresponding to FIG. 2 of a transformer illustrating a second embodiment of a static induction electric machine according to the present invention. 図5の放熱リブ近傍の温度分布と外気の流れを示す模式図。FIG. 6 is a schematic diagram showing a temperature distribution in the vicinity of the heat dissipating ribs in FIG. 5 and a flow of outside air. 図5のA−A線に沿う拡大断面図。The expanded sectional view which follows the AA line of FIG. 本発明による静止誘導電器の第3の実施の形態を示す変圧器の放熱リブの拡大側面図。The expansion side view of the radiation rib of the transformer which shows 3rd Embodiment of the static induction | electrical_connection apparatus by this invention. 本発明による静止誘導電器の第4の実施の形態を示す変圧器の図2相当図。The equivalent figure of FIG. 2 of the transformer which shows 4th Embodiment of the static induction machine by this invention. 本発明による静止誘導電器の第5の実施の形態を示す変圧器の図2相当図。FIG. 2 is a diagram corresponding to FIG. 2 of a transformer showing a fifth embodiment of a static induction electric machine according to the present invention. 従来の変圧器を示す図1相当図。The equivalent figure of FIG. 1 which shows the conventional transformer. 図11の外観図。The external view of FIG. 図11における冷却媒体の各位置における温度を示す想定関係図。FIG. 12 is an assumed relationship diagram illustrating temperatures at respective positions of the cooling medium in FIG. 11. 図11における冷却媒体の各位置における温度を示す実測関係図。FIG. 12 is an actual measurement relationship diagram illustrating temperatures at respective positions of the cooling medium in FIG. 11. 図12の放熱リブ近傍の温度分布と外気の流れを示す模式図。FIG. 13 is a schematic diagram showing a temperature distribution in the vicinity of the heat dissipating ribs in FIG. 12 and a flow of outside air.

符号の説明Explanation of symbols

1…電器本体、2…鉄心、3…巻線、4…タンク、5,9,11,13…下方放熱リブ、5A…空間、5I,6I,15I…温度分布、6,10,12,14…上方放熱リブ、6A…空間、7…空気流路、8…冷却媒体、15…放熱リブ。   DESCRIPTION OF SYMBOLS 1 ... Electric appliance main body, 2 ... Iron core, 3 ... Winding, 4 ... Tank, 5, 9, 11, 13 ... Lower radiating rib, 5A ... Space, 5I, 6I, 15I ... Temperature distribution, 6, 10, 12, 14 ... upper heat radiation rib, 6A ... space, 7 ... air flow path, 8 ... cooling medium, 15 ... heat radiation rib.

Claims (5)

電器本体と、この電器本体を収容し内部に冷却媒体を充填したタンクと、このタンクの周壁の周囲に複数設けた上下方向に長い放熱リブとを備えた静止誘導電器において、前記放熱リブを高さ方向に複数に分割して前記タンクの周方向に空気流路を形成して外気撹乱手段を構成し、かつ、上部に位置する放熱リブと下部に位置する放熱リブとを周方向に同じピッチに形成すると共に、上部に位置する放熱リブと下部に位置する放熱リブを前記タンクの周壁の周方向にずらして配置したことを特徴とする静止誘導電器。 In a static induction appliance comprising an electrical appliance main body, a tank containing the electrical appliance main body and filled with a cooling medium, and a plurality of vertically extending thermal radiating ribs provided around the peripheral wall of the tank, Divided into multiple in the vertical direction to form an air flow path in the circumferential direction of the tank to constitute the outside air disturbing means, and the upper and lower radiating ribs have the same pitch in the circumferential direction And a heat induction rib located in the upper part and a heat radiation rib located in the lower part are arranged shifted in the circumferential direction of the peripheral wall of the tank. 前記上部に位置する放熱リブと前記下部に位置する放熱リブを前記タンクの周壁の周方向に1/2ピッチずらして配置したことを特徴とする請求項1記載の静止誘導電器。   The static induction device according to claim 1, wherein the heat dissipating rib located in the upper part and the heat dissipating rib located in the lower part are arranged with a 1/2 pitch shift in the circumferential direction of the peripheral wall of the tank. 上部に位置する放熱リブは、下部に位置する放熱リブよりも前記タンクの周方向に広い範囲で設置されていることを特徴とする請求項1又は2記載の静止誘導電器。   The static induction device according to claim 1 or 2, wherein the heat dissipating rib located in the upper part is installed in a wider range in the circumferential direction of the tank than the heat dissipating rib located in the lower part. 前記放熱リブは、前記タンクに充填された冷却媒体が流通する空間が前記タンクの内側に開口していることを特徴とする請求項1〜3のいずれかに記載の静止誘導電器。   The static induction machine according to claim 1, wherein a space in which the cooling medium filled in the tank flows is opened inside the tank. 前記放熱リブは、中実の板状に形成された放熱フィンであることを特徴とする請求項1〜3のいずれかに記載の静止誘導電器。   The static induction apparatus according to claim 1, wherein the heat radiation rib is a heat radiation fin formed in a solid plate shape.
JP2008169811A 2008-06-30 2008-06-30 Static induction machine Expired - Fee Related JP5001225B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP2008169811A JP5001225B2 (en) 2008-06-30 2008-06-30 Static induction machine

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP2008169811A JP5001225B2 (en) 2008-06-30 2008-06-30 Static induction machine

Publications (2)

Publication Number Publication Date
JP2010010511A JP2010010511A (en) 2010-01-14
JP5001225B2 true JP5001225B2 (en) 2012-08-15

Family

ID=41590621

Family Applications (1)

Application Number Title Priority Date Filing Date
JP2008169811A Expired - Fee Related JP5001225B2 (en) 2008-06-30 2008-06-30 Static induction machine

Country Status (1)

Country Link
JP (1) JP5001225B2 (en)

Family Cites Families (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5667732U (en) * 1979-10-30 1981-06-05
JPS583020U (en) * 1981-06-26 1983-01-10 株式会社東芝 Oil-immersed transformer cooling system
JPS6367712A (en) * 1986-09-09 1988-03-26 Hitachi Ltd Tank for oil-filled electric machinery and apparatus
JP2009260012A (en) * 2008-04-16 2009-11-05 Hitachi Industrial Equipment Systems Co Ltd Static induction electrical apparatus

Also Published As

Publication number Publication date
JP2010010511A (en) 2010-01-14

Similar Documents

Publication Publication Date Title
Segal et al. An investigation of power transformer cooling with magnetic fluids
Dixit et al. Thermal analysis of natural cooling type distribution transformer retrofilled with natural ester oil
JP5070011B2 (en) Radiator and transformer attached to it
CN103337339A (en) Heat dissipating method for oil-immersed transformer and radiator thereof
KR20150048384A (en) Oil immersed transformer
JP7228377B2 (en) static induction electric machine
JP5001225B2 (en) Static induction machine
JP5867074B2 (en) Power supply unit and cooling device for power supply
JP6946218B2 (en) Static inducer
JP5701335B2 (en) Power converter
US12027309B2 (en) Superconducting electromagnet device
JP5606494B2 (en) Railway vehicle power converter
CN208171053U (en) Based on the gas condenser that can be recycled
JP6505616B2 (en) Stationary induction equipment
JP2009123755A (en) Railway vehicle power converter
CN110491640B (en) Method for accelerating oil cooling of oil-immersed self-cooling transformer
JP2022130235A (en) Oil-filled transformer tank and oil-filled transformer
JP5873699B2 (en) Electronic component unit
KR20140055603A (en) Water cooling type mold transformer
US1641702A (en) Means for cooling transformers
KR20090072414A (en) Inflow transformer
JP2026036437A (en) Oil-filled transformer
KR101099190B1 (en) oil filled transformer
JP7600438B2 (en) Static Inductor Unit
KR20260028012A (en) Water-cooled submarine power unit

Legal Events

Date Code Title Description
A621 Written request for application examination

Free format text: JAPANESE INTERMEDIATE CODE: A621

Effective date: 20100428

A131 Notification of reasons for refusal

Free format text: JAPANESE INTERMEDIATE CODE: A131

Effective date: 20110920

A521 Written amendment

Free format text: JAPANESE INTERMEDIATE CODE: A523

Effective date: 20111118

A02 Decision of refusal

Free format text: JAPANESE INTERMEDIATE CODE: A02

Effective date: 20111213

A521 Written amendment

Free format text: JAPANESE INTERMEDIATE CODE: A523

Effective date: 20120216

A911 Transfer to examiner for re-examination before appeal (zenchi)

Free format text: JAPANESE INTERMEDIATE CODE: A911

Effective date: 20120223

TRDD Decision of grant or rejection written
A01 Written decision to grant a patent or to grant a registration (utility model)

Free format text: JAPANESE INTERMEDIATE CODE: A01

Effective date: 20120515

A01 Written decision to grant a patent or to grant a registration (utility model)

Free format text: JAPANESE INTERMEDIATE CODE: A01

A61 First payment of annual fees (during grant procedure)

Free format text: JAPANESE INTERMEDIATE CODE: A61

Effective date: 20120517

R150 Certificate of patent or registration of utility model

Ref document number: 5001225

Country of ref document: JP

Free format text: JAPANESE INTERMEDIATE CODE: R150

Free format text: JAPANESE INTERMEDIATE CODE: R150

FPAY Renewal fee payment (event date is renewal date of database)

Free format text: PAYMENT UNTIL: 20150525

Year of fee payment: 3

LAPS Cancellation because of no payment of annual fees