JP3779558B2 - Insulator - Google Patents

Insulator Download PDF

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Publication number
JP3779558B2
JP3779558B2 JP2001132398A JP2001132398A JP3779558B2 JP 3779558 B2 JP3779558 B2 JP 3779558B2 JP 2001132398 A JP2001132398 A JP 2001132398A JP 2001132398 A JP2001132398 A JP 2001132398A JP 3779558 B2 JP3779558 B2 JP 3779558B2
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Japan
Prior art keywords
shade
insulator
diameter
shades
ellipse
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Expired - Fee Related
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JP2001132398A
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Japanese (ja)
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JP2002329433A (en
Inventor
佳典 嶋田
冨美朗 島田
明由 飯田
充雄 岩崎
哲 稲玉
耕司 渡邉
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Hitachi Ltd
Central Japan Railway Co
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Hitachi Ltd
Central Japan Railway Co
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Priority to JP2001132398A priority Critical patent/JP3779558B2/en
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Description

【0001】
【発明の属する技術分野】
本発明は、絶縁碍子に係り、特に高速走行する鉄道車両の集電装置に用いられるものに好適な低騒音絶縁碍子に関する。
【0002】
【従来の技術】
鉄道車両の高速化に伴う空力騒音は、速度の6〜8乗程度に比例して増加するため、車両速度の向上に伴い急激に増加する。一方、環境の保全に対する要求は今後ますます高まるものと考えられる。このため、高速で走行する車両では、主たる空力音源である集電装置の低騒音化が求められており、集電装置の一部品である絶縁碍子も低騒音化のための重要な構成要素である。
【0003】
従来、鉄道車両用絶縁碍子としては、一般に円柱状の碍子胴に笠が複数個設けられている碍子が使われている。
【0004】
高速車両用の低騒音絶縁碍子については、公知の技術として、特開平8−336203号明細書がある。これは従来の碍子の笠面に列車走行方向に設けた襞により、列車走行の直角方向の碍子の表面漏れ距離を拡大することで、碍子の列車走行直角方向の笠径寸法を小さく出来て、高速走行時の空気抵抗を小さくし、空力騒音も小さくしようとするものである。
【0005】
また、特開平8−322102号明細書がある。これは、従来の碍子の笠面に表面粗さ要素を全面に配置し、笠間に発生する音響共鳴を抑制し、低騒音化を図るものである。
【0006】
また、他の形状の絶縁碍子の公知の技術としては、[No.96-51]日本機械学会第51回交通・物流部門大会講演論文集381〜382頁に長円またはだ円形状の碍子胴に笠が複数個設けられている構造の絶縁碍子が発表されている。
【0007】
【発明が解決しようとする課題】
本発明の目的は、鉄道車両用集電装置に用いるのに必要な電気絶縁性能を有しながら高速走行時の空力騒音を、上記した公知例の低騒音絶縁碍子とは別途の手段により、より以上低騒音化した絶縁碍子を提供する事にある。
【0008】
【課題を解決するための手段】
本発明の特徴は、胴と、該胴の長手方向の周囲に複数段の笠を配置して構成される絶縁碍子の横断面形状をだ円もしくは長円とし、笠径寸法を3種類以上として大径の笠に隣接して小径の笠が配置され、前記小径の笠に隣接して中径の笠が配置され、前記中径の笠の両側に前記小径の笠が配置され、前記大径の笠、中径の笠及び小径の笠が交互にかつ、繰り返し配置されており、前記各笠の間の前記胴円周部に形成される溝形状が断面U字形にする事により、最大径の碍子笠先端間の空間絶縁距離を確保しつつ、笠間隔を小とする。また、碍子を長円もしくはだ円とした事により、周方向の面積が増大するために碍子全体の絶縁抵抗の低下が生じる。これを防ぐ目的で笠密度を向上し碍子の表面漏れ距離を増大し、碍子全体の絶縁性能を確保する。さらに、笠底部の碍子胴円周部での気流の増速機能を抑制し、また、笠面にだ円又は長円の長径方向に平行で、かつ、前記胴より外周側に突起を設けて笠間の流れの剥離を抑制することにより、碍子後方の渦の領域を制御して、かつ渦径を縮小する事により騒音低減を図るものである。
【0009】
【発明の実施の形態】
図1に従来技術による絶縁碍子1の正面図を示し、図2に側面図を示す。軸A方向が列車の走行方向である。また、図3に図2の断面I−Iを示す。図4に図2の断面II−IIを示す。
【0010】
図3において、従来技術の絶縁碍子を車両速度(350km/h程度)と同一の流速の気流中に置いた場合の電子計算機による断面I−Iに相当する笠間の高さ位置における流れのシミュレーション結果の概略を示している。この結果に基づき、代表的に1対の笠間の流れについて考察する。
【0011】
流体力学の教科書(例えば、牧野光雄著「流体抵抗と流線型」産業図書(株))によると、円柱面に沿う流れでは増速がおこり、主流速よりも早い流れが生ずる場合があり、平板面に沿う流れでは増速は起こらないと教えている。図3に示す様に、電子計算機によるだ円断面形状の碍子について笠間の流れの解析結果をみると、だ円柱面即ち碍子胴面近傍で主流速102よりも早い部分101が発生し、次第に成長し笠径全体に及ぶと胴面で剥離が生じ逆流域104が生ずる事が判明した。
【0012】
また、流れの境界層の内部にはその流速分布に起因する強い渦度が潜在しており、図4に断面II−IIにおいて気流の後方より見た、主流と直交する方向に軸を持つ渦(以下、横渦と称す)の渦度分布のシミュレーション結果の一例を示している。
【0013】
図4の強い渦度領域105は、碍子胴円周部で成長し、今、正に胴部より剥離した直後で、笠外周方向へ移動し、笠面の境界層内の強い渦度領域106を巻き込んで笠外周方向へ滑動しようとしている所である。
【0014】
境界層が胴面及び笠面に張り付いている間は渦度は境界層内に潜在していると考えることが出来、動的な渦として振る舞うことはないが、境界層が一旦剥離すると渦度は動的な渦として顕在化し軸変換も含め自由に振る舞うようになる。
【0015】
このような機構により、笠間で創成された渦は、笠間隔に依存した渦列として流れの後方へ放出され、これらの渦列が碍子騒音の主因であると考えられる。
【0016】
このように、従来技術の絶縁碍子での騒音の主因を碍子胴部より剥離した強い渦度領域105が引金となり、笠面の強い渦度領域106と共に笠面を滑動することであると考えると、騒音低減のためにはこれを抑制する手段を設ければ良い。
【0017】
図5に、本発明の一実施例の絶縁碍子の正面図を示し、図6に側面図を示す。軸A方向が列車の走行方向である。また、図7に図5の断面III−IIIを示す。
【0018】
図8に図5のVI部の拡大図を示す。この図では笠11〜13と3種類の笠を交互にかつ、繰り返し配置し、かつ、笠底部の碍子胴円周部にU字形をした溝形状14を設け、かつ、その溝形状14で笠11〜13を連結して配置した形状としている。図8に示すように、笠11〜13は、笠11の笠径が最も大きく、笠12は笠11よりも小さく、笠13が笠12よりも小さく、該笠13が最も笠径が小さい構造となっている。前記笠11に隣接して笠13が配置され、前記笠13に隣接して笠12が配置されている。また、笠12の両側に笠13が配置された構造となっている。このように大径の笠11に隣接して小径の笠13を配置し、中径の笠12を前記笠13に隣接させるとともに、該中径の笠12の両側に小径の笠13を配置しており、このような笠11〜13の配置を繰り返す構造となっている。
【0019】
絶縁碍子の横断面形状をだ円または長円形状とすることにより、円柱部の曲率変化をなだらかにし、胴面での剥離を遅らせる事が出来て、碍子後方の渦流の範囲を狭めることになり、結果として碍子騒音の低減に有効である。本発明ではさらに、笠間の碍子胴面の面積を絶縁性能を確保しつつ小さくすることにより碍子笠間での気流の流速を低減し、騒音低減を促進することが出来る。
【0020】
すなわち、碍子笠を3種類以上とし、これを交互にかつ、繰り返し配置することにより、最大径の碍子笠先端間の空間絶縁間隔(約50mm程度)を確保しつつ、笠の間隔を約10〜15mm程度以下とする。このことにより、碍子胴面の境界層は細かく分断され、かつ、笠面の境界層との干渉が起こり、弱い流れとなり、弱い渦度を持つことになる。
【0021】
さらに、碍子胴円周部をU字形をした溝形状14とすることにより胴面での境界層が厚くなり、すなわち、渦度が弱くなり剥離する力も弱くなる。
【0022】
これらの結果として、笠間より放出された渦列の渦度も弱くなり、かつ、渦径が小さくなることにより、騒音周波数がより高周波側へ移動し、聴感補正効果も加わり体感的に騒音が低減される。
【0023】
空力音は同じ強さの渦でも物体の近くにある渦からは大きな騒音が出て、物体から離れた渦からは小さな騒音が出る。本発明ではこの事に注目し、流れの剥離が遅れると物体と渦の距離が大きくなり、結果として騒音が低減することになるので、下記の考案を行った。
【0024】
図9に図7の笠11、12に突起21を碍子の長軸方向に、碍子胴径よりも外周側の笠面に取り付けた図を示す。この突起21は、図10(図断面)、図11(図5のIVIV断面)の通り、列車走行方向に、碍子の長軸方向に取り付けられている。
【0025】
このような構造とする事により、碍子胴面で剥離した強い渦度105が笠面の強い渦度領域106を巻き込んで滑り出る時の抵抗を増大し、結果として妨害する事になり、剥離を遅らせることが出来る。これにより碍子と後方の渦流の領域との距離を拡大するが出来て、碍子騒音低減に有効である。
【0026】
【発明の効果】
以上説明したように、本発明によれば、笠底部の碍子胴面に断面がU字形をした溝形状を碍子胴円周方向に設けかつ、径寸法を3種類とする笠を交互にかつ、繰り返して配置し、かつ溝で連結して配置した事により、碍子胴面での気流の増速を抑え、笠間の流れの渦度を弱め、剥離する力を弱める事ができる。また、笠表面に列車走行方向に突起を設ける事により、この突起が抵抗になって碍子胴面と笠面の強い渦度領域との剥離を遅らせる事ができ、碍子と後方の渦流の領域との距離を拡大する事が出来る。その結果として絶縁碍子の高速走行時の空力騒音を低減できる。そして、結果として低騒音の高速鉄道車両用集電装置を提供できる事になる。
【図面の簡単な説明】
【図1】従来例の絶縁碍子の全体構造を示す正面図。
【図2】従来例の絶縁碍子の全体構造を示す側面図。
【図3】従来例の絶縁碍子を車両速度と同一の流速の気流中に置いた場合の電子計算機による流れのシミュレーション結果を示す図2のI−I断面図。
【図4】従来例の絶縁碍子の電子計算機による横渦の渦度分布のシミュレーション結果を示す図2のII−II断面図。
【図5】本発明の一実施例の絶縁碍子の全体構造を示す正面図。
【図6】本発明の一実施例の絶縁碍子の全体構造を示す側面図。
【図7】本発明の一実施例を示す図5のIII−IIIに沿って断面した断面図。
【図8】本発明の一実施例を示す図5のVI部の拡大図。
【図9】本発明の一実施例の笠に突起を付けた場合を示す図5のVI部の拡大図。
【図10】本発明の一実施例の笠に突起を付けた場合を示す図5のIV−IVに沿って断面した断面図。
【図11】本発明の一実施例の笠に突起を付けた場合を示す図5のV−Vに沿って断面した断面図。
【符号の説明】
1…従来例の絶縁碍子
2…絶縁碍子
11…笠(大径)
12…笠(中径)
13…笠(小径)
14…U字溝形状
21…突起
101…流れの増速域
102…流れの主流速域
103…流れの減速域
104…流れの逆流域
105…碍子胴部で成長した強い横渦の領域
106…笠面の強い横渦の領域
107…流れの逆流域による弱い横渦の領域
[0001]
BACKGROUND OF THE INVENTION
The present invention relates to an insulator, and more particularly to a low noise insulator suitable for use in a current collector for a railway vehicle that travels at high speed.
[0002]
[Prior art]
Since the aerodynamic noise accompanying the increase in the speed of the railway vehicle increases in proportion to the sixth to eighth power of the speed, it rapidly increases as the vehicle speed increases. On the other hand, the demand for environmental conservation is expected to increase in the future. For this reason, in vehicles that run at high speeds, it is required to reduce the noise of the current collector, which is the main aerodynamic sound source, and the insulator, which is a component of the current collector, is also an important component for reducing noise. is there.
[0003]
Conventionally, as an insulator for a railway vehicle, an insulator in which a plurality of shades are provided on a cylindrical insulator body is generally used.
[0004]
Japanese Unexamined Patent Publication No. 8-336203 is known as a low-noise insulator for high-speed vehicles. This is because the surface leakage distance of the insulator in the direction perpendicular to the train travel is increased by the cage provided on the shade surface of the conventional insulator in the train travel direction, thereby reducing the diameter of the insulator in the direction perpendicular to the train travel of the insulator. It is intended to reduce the air resistance during high-speed driving and to reduce aerodynamic noise.
[0005]
Japanese Patent Laid-Open No. 8-322102 is also available. This is because a surface roughness element is arranged on the entire surface of the shade of a conventional insulator to suppress acoustic resonance generated between the shades, thereby reducing noise.
[0006]
In addition, as a known technique of other shape insulators, [No. 96-51] The 51st Transportation and Logistics Division Annual Proceedings of the Japan Society of Mechanical Engineers, pages 381-382, ellipse or ellipse shape insulators An insulator with a structure in which a plurality of shades are provided on the earth has been announced.
[0007]
[Problems to be solved by the invention]
The object of the present invention is to reduce the aerodynamic noise during high-speed running while having the electrical insulation performance necessary for use in a railway vehicle current collector by means other than the above-mentioned known low-noise insulator. The object is to provide an insulator with low noise.
[0008]
[Means for Solving the Problems]
A feature of the present invention is that the cross-sectional shape of an insulator formed by arranging a barrel and a plurality of stages of shades around the barrel in the longitudinal direction is an ellipse or an ellipse, and has three or more types of shade diameters. A small-diameter shade is arranged adjacent to the large-diameter shade, a medium-diameter shade is arranged adjacent to the small-diameter shade, the small-diameter shade is arranged on both sides of the medium-diameter shade, and the large-diameter shade is arranged. The shades of medium diameter, shades of medium diameter, and shades of small diameter are alternately and repeatedly arranged, and the groove formed on the trunk circumference between the shades has a U-shaped cross section. The space between the shades is made small while securing the space insulation distance between the tops of the shades. In addition, when the insulator is an ellipse or an ellipse, the area in the circumferential direction increases, so that the insulation resistance of the insulator as a whole decreases. To prevent this, the shade density is increased, the surface leakage distance of the insulator is increased, and the insulation performance of the insulator is ensured. Furthermore, the speed increasing function of the airflow at the circumferential part of the insulator trunk at the bottom of the shade bottom is suppressed , and the projection is provided on the shaded face parallel to the major axis direction of the ellipse or ellipse and on the outer circumferential side from the trunk. By suppressing the separation of the flow between the shades, the vortex area behind the insulator is controlled and the vortex diameter is reduced to reduce noise.
[0009]
DETAILED DESCRIPTION OF THE INVENTION
FIG. 1 shows a front view of a conventional insulator 1 and FIG. 2 shows a side view thereof. The direction of axis A is the traveling direction of the train. FIG. 3 shows a cross section II of FIG. FIG. 4 shows a section II-II in FIG.
[0010]
In FIG. 3, the simulation result of the flow in the height position between the shades corresponding to the cross-section II by the computer when the insulator of the prior art is placed in the air flow having the same flow velocity as the vehicle speed (about 350 km / h) The outline of is shown. Based on this result, the flow between a pair of shades is considered.
[0011]
According to fluid dynamics textbooks (eg, Mitsuo Makino, “Fluid Resistance and Streamlined” Industrial Book Co., Ltd.), the flow along the cylinder surface increases in speed and may flow faster than the main flow velocity. It is taught that the speed does not increase in the flow along. As shown in FIG. 3, when the analysis result of the flow between the caps is observed with respect to the insulator having an elliptical cross section by an electronic computer, a portion 101 faster than the main flow velocity 102 is generated in the vicinity of the elliptical cylinder surface, that is, the insulator body surface, and gradually grows. It has been found that when the entire diameter of the cocoon is reached, separation occurs on the body surface and a reverse flow region 104 is generated.
[0012]
In addition, a strong vorticity due to the flow velocity distribution is latent inside the boundary layer of the flow, and a vortex having an axis in a direction perpendicular to the main flow as seen from the rear of the air flow in section II-II in FIG. An example of a simulation result of a vorticity distribution (hereinafter referred to as a horizontal vortex) is shown.
[0013]
The strong vorticity region 105 in FIG. 4 grows around the circumference of the insulator trunk, and immediately after peeling off from the trunk, moves to the outer circumference of the shade, and the strong vorticity region 106 in the boundary layer of the shade surface. It is a place that is going to slide around the shade around the shade.
[0014]
While the boundary layer sticks to the body surface and the shade surface, the vorticity can be considered to be hidden in the boundary layer and does not behave as a dynamic vortex. The degree becomes manifest as a dynamic vortex and behaves freely including axis transformation.
[0015]
By such a mechanism, the vortex created in the shade is discharged to the rear of the flow as a vortex train depending on the shade spacing, and these vortex trains are considered to be the main cause of the insulator noise.
[0016]
Thus, it is considered that the strong vorticity region 105 that peels off the main cause of noise in the insulator of the prior art from the insulator body is a trigger and slides on the shade surface together with the strong vorticity region 106 of the shade surface. In order to reduce noise, a means for suppressing this may be provided.
[0017]
FIG. 5 shows a front view of an insulator according to an embodiment of the present invention, and FIG. 6 shows a side view. The direction of axis A is the traveling direction of the train. FIG. 7 shows a section III-III in FIG.
[0018]
FIG. 8 is an enlarged view of the VI part in FIG. In this figure, the shades 11 to 13 and the three types of shades are arranged alternately and repeatedly, and a U-shaped groove shape 14 is provided on the circumference of the insulator body at the bottom of the shade. It is set as the shape which connected and arranged 11-13. As shown in FIG. 8, the shade 11 to 13 has the largest shade diameter of the shade 11, the shade 12 is smaller than the shade 11, the shade 13 is smaller than the shade 12, and the shade 13 has the smallest shade diameter. It has become. A shade 13 is disposed adjacent to the shade 11, and a shade 12 is disposed adjacent to the shade 13. Further, the shade 13 is arranged on both sides of the shade 12. In this way, the small-diameter shade 13 is arranged adjacent to the large-diameter shade 11, the medium-diameter shade 12 is arranged adjacent to the shade 13, and the small-diameter shade 13 is arranged on both sides of the medium-diameter shade 12. The arrangement of the shades 11 to 13 is repeated.
[0019]
By making the cross-sectional shape of the insulator an ellipse or an ellipse, it is possible to smooth the change in the curvature of the cylindrical part, delay the peeling on the body surface, and narrow the range of vortex flow behind the insulator. As a result, it is effective in reducing the insulator noise. Furthermore, in the present invention, by reducing the area of the insulator body surface between the shades while ensuring the insulation performance, the flow velocity of the airflow between the shade shades can be reduced, and noise reduction can be promoted.
[0020]
In other words, three or more types of cocoon shades are used, and these are arranged alternately and repeatedly, so that a space insulation interval (about 50 mm) between the cocoon shade tips with the maximum diameter is secured, and the shade spacing is about 10 to 10 mm. It is about 15 mm or less. As a result, the boundary layer of the insulator body surface is finely divided, and interference with the boundary layer of the shade surface occurs, resulting in a weak flow and a weak vorticity.
[0021]
Furthermore, by making the circumferential part of the insulator body into a U-shaped groove shape 14, the boundary layer on the body surface becomes thick, that is, the vorticity becomes weak and the peeling force also becomes weak.
[0022]
As a result, the vorticity of the vortex train released from Kasama also becomes weaker and the vortex diameter becomes smaller, so that the noise frequency moves to the higher frequency side and the auditory correction effect is also added to reduce the noise sensibly. Is done.
[0023]
Aerodynamic sound produces a loud noise from a vortex near the object, and a small noise from a vortex far from the object, even if the vortex has the same strength. In the present invention, attention is paid to this, and if the separation of the flow is delayed, the distance between the object and the vortex is increased, and as a result, noise is reduced.
[0024]
FIG. 9 is a view in which the projections 21 are attached to the shades 11 and 12 of FIG. 7 in the longitudinal direction of the insulator on the shade surface on the outer peripheral side of the insulator body diameter. The projection 21 is, FIG. 10 (V in Fig. 5 - V cross section), Fig. 11 (IV in FIG. 5 - IV cross section) as, in the train travel direction, is mounted in the longitudinal direction of the insulator.
[0025]
By adopting such a structure, the strong vorticity 105 peeled off on the insulator body surface increases the resistance when the strong vorticity region 106 on the shade surface slid out and slides out. Can be delayed. As a result, the distance between the insulator and the rear vortex region can be increased, which is effective in reducing insulator noise.
[0026]
【The invention's effect】
As described above, according to the present invention, a groove shape having a U-shaped cross section is provided in the insulator barrel circumferential direction on the insulator barrel surface of the shade bottom portion, and the shades having three types of diameter dimensions are alternately and By arranging repeatedly and connecting with a groove, it is possible to suppress the increase in the airflow on the insulator body surface, weaken the vorticity of the flow between the shades, and weaken the peeling force. In addition, by providing a projection on the shade surface in the train running direction, this projection becomes a resistance, and the separation between the insulator body surface and the strong vorticity region of the shade surface can be delayed. The distance can be expanded. As a result, it is possible to reduce aerodynamic noise when the insulator is running at high speed. As a result, a low-noise high-speed railway vehicle current collector can be provided.
[Brief description of the drawings]
FIG. 1 is a front view showing the overall structure of a conventional insulator.
FIG. 2 is a side view showing the overall structure of a conventional insulator.
3 is a cross-sectional view taken along the line II of FIG. 2 showing a flow simulation result by an electronic computer when the insulator of the conventional example is placed in an airflow having the same flow velocity as the vehicle speed.
4 is a cross-sectional view taken along the line II-II in FIG. 2 showing a simulation result of a vorticity distribution of a transverse vortex by an electronic computer of a conventional insulator.
FIG. 5 is a front view showing an overall structure of an insulator according to an embodiment of the present invention.
FIG. 6 is a side view showing the overall structure of an insulator according to an embodiment of the present invention.
7 is a cross-sectional view taken along the line III-III of FIG. 5 showing an embodiment of the present invention.
8 is an enlarged view of a VI part in FIG. 5 showing an embodiment of the present invention.
9 is an enlarged view of a portion VI in FIG. 5 showing a case where a protrusion is attached to the shade of one embodiment of the present invention.
10 is a cross-sectional view taken along the line IV-IV in FIG. 5 showing a case where a protrusion is attached to the shade of one embodiment of the present invention.
11 is a cross-sectional view taken along line V-V in FIG. 5 showing a case where a protrusion is attached to the shade of one embodiment of the present invention.
[Explanation of symbols]
DESCRIPTION OF SYMBOLS 1 ... Conventional insulator 2 ... Insulator 11 ... Shade (large diameter)
12 ... Shade (medium diameter)
13 ... Shade (small diameter)
14 ... U-shaped groove shape 21 ... Protrusion 101 ... Flow speed increasing area 102 ... Flow main flow velocity area 103 ... Flow deceleration area 104 ... Flow reverse flow area 105 ... Strong transverse vortex area 106 grown in the insulator body ... Strong transverse vortex region 107 with a shaded surface ... weak transverse vortex region due to the reverse flow region

Claims (1)

胴と、該胴の長手方向の周囲に複数段の笠を配置して構成される絶縁碍子であって、
前記胴及び笠の横断面形状がだ円又は長円であり、
前記笠は、その径寸法が3種類であり、大径の笠に隣接して小径の笠が配置され、前記小径の笠に隣接して中径の笠が配置され、前記中径の笠の両側に前記小径の笠が配置され、前記大径の笠、中径の笠及び小径の笠が繰り返して配置されており、
前記各笠の間の前記胴円周部に形成される溝形状が断面U字形であり、
前記笠は、その表面に突起を有し、
前記突起は、前記だ円又は長円の長径方向に平行で、かつ、前記胴より外周側の前記笠に設置されている
ことを特徴とする絶縁碍子。
An insulator formed by arranging a barrel and a plurality of shades around the barrel in the longitudinal direction;
The cross-sectional shape of the trunk and the shade is an ellipse or an ellipse,
The shade has three types of diameters, a small-diameter shade is arranged adjacent to the large-diameter shade, a medium-diameter shade is arranged adjacent to the small-diameter shade, The small-diameter shade is arranged on both sides, the large-diameter shade, the medium-diameter shade and the small-diameter shade are repeatedly arranged,
The groove shape formed in the trunk circumference between the shades is a U-shaped cross section,
The shade has a protrusion on its surface,
The said insulator is parallel to the major axis direction of the said ellipse or an ellipse, and is installed in the said shade on the outer peripheral side from the said trunk | drum, The insulator characterized by the above-mentioned.
JP2001132398A 2001-04-27 2001-04-27 Insulator Expired - Fee Related JP3779558B2 (en)

Priority Applications (1)

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JP2001132398A JP3779558B2 (en) 2001-04-27 2001-04-27 Insulator

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Application Number Priority Date Filing Date Title
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JP3779558B2 true JP3779558B2 (en) 2006-05-31

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Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP5323407B2 (en) * 2008-06-30 2013-10-23 株式会社ビスキャス Bird damage prevention polymer insulator and polymer type arrester
CN104590030A (en) * 2014-12-12 2015-05-06 株洲鼎顺新材料科技有限公司 Bus brace and pantograph brace porcelain insulator on roof of electric locomotive

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