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JPH0757046B2 - Tightening method for power lines - Google Patents
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JPH0757046B2 - Tightening method for power lines - Google Patents

Tightening method for power lines

Info

Publication number
JPH0757046B2
JPH0757046B2 JP14498488A JP14498488A JPH0757046B2 JP H0757046 B2 JPH0757046 B2 JP H0757046B2 JP 14498488 A JP14498488 A JP 14498488A JP 14498488 A JP14498488 A JP 14498488A JP H0757046 B2 JPH0757046 B2 JP H0757046B2
Authority
JP
Japan
Prior art keywords
sag
wire
gyro
angle
power transmission
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
JP14498488A
Other languages
Japanese (ja)
Other versions
JPH01315210A (en
Inventor
栄一 瀬川
征廣 照沼
勝吉 藤倉
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 Cable Ltd
Original Assignee
Hitachi Cable 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 Cable Ltd filed Critical Hitachi Cable Ltd
Priority to JP14498488A priority Critical patent/JPH0757046B2/en
Publication of JPH01315210A publication Critical patent/JPH01315210A/en
Publication of JPH0757046B2 publication Critical patent/JPH0757046B2/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、送電線の緊線において高精度に弛度を監視
し、経済的に弛度の変動を適確に把持しつつ効率よく弛
度設定をする送電線の緊線工法に関するものである。
DETAILED DESCRIPTION OF THE INVENTION [Industrial field of application] The present invention monitors sag in a tight line of a power transmission line with high accuracy, and efficiently and efficiently grasps fluctuations in sag economically and efficiently. It is related to the tight line construction method of the power transmission line that sets the degree.

[従来の技術] 近年、架空送電線は益々超々高圧化され、導体も多導体
大サイズ化されるようになって、鉄塔が大型化する一方
架線径間も一層長大化の傾向にある。
[Prior Art] In recent years, the overhead power transmission lines have become ultra-higher in voltage, and the conductors have become larger in size, and the size of the towers has increased. On the other hand, the span between overhead lines tends to become longer.

このような架空送電線路の大型化に伴い、その立地条件
等をも併せ、その架線にはいくつかの新たな問題点が露
呈されるようになった。
With the increase in size of such overhead power transmission lines, some new problems have come to be exposed in the overhead lines, including their location conditions.

架空送電線を架線する場合には、第5図に示すように、
鉄塔T1,T2間において送電線1に過大な架線張力が負荷
されたりしないように所定の設計弛度dが定められ、架
線に際し送電線1を当該弛度dに調整するいわゆる緊線
作業が行なわれる。
When an overhead power transmission line is installed, as shown in Fig. 5,
A predetermined design sag d is set so that excessive overhead line tension is not applied to the power transmission line 1 between the steel towers T 1 and T 2 , and so-called tight line work is performed to adjust the power transmission line 1 to the sag d during the overhead line. Is performed.

従来、この緊線作業を行なうには、第6図に示すような
表示目盛付きのバーテックス4を鉄塔T2側に設置し、鉄
塔T1側には望遠鏡付きコンパス3を取付け、バーテック
ス4をコンパス3より視準して送電線1が弛度dとなる
よう電線1の張力を調整し、弛度設定を行なっていた。
Conventionally, in order to perform this tight line work, a vertex 4 with a display scale as shown in Fig. 6 is installed on the tower T 2 side, a compass 3 with a telescope is installed on the tower T 1 side, and the vertex 4 is placed on the compass. By collimating from 3, the tension of the electric wire 1 was adjusted so that the transmission line 1 had a sag d, and the sag was set.

第4図は、緊線作業における電線1の張力調整状況を示
す説明図である。鉄塔アームTaに碍子連2を取付け、電
線1にはカムアロング5を取付けて、前記碍子連2とカ
ムアロング5との間を滑車6,6で連結し、ワイヤ7によ
って前記滑車6,6を動かして調整する。そのようにし
て、前記バーテックスによる弛度監視作業者と滑車によ
る張力調整作業者との間で連絡を取り合いながら弛度d
になったことを確認したら、電線1の端末に引留クラン
プを取付け、前記碍子連2に連結して、緊線作業は終了
する。
FIG. 4 is an explanatory diagram showing a tension adjustment state of the electric wire 1 in the wire tension work. The insulator string 2 is attached to the steel tower arm Ta, the cam along 5 is attached to the electric wire 1, the insulator string 2 and the cam along 5 are connected by pulleys 6 and 6, and the pulleys 6 and 6 are moved by the wire 7. adjust. In this way, the sag monitoring operator using the vertex and the tension adjusting operator using the pulley are in contact with each other while the sag d is maintained.
When it is confirmed that the above condition is satisfied, a strain clamp is attached to the end of the electric wire 1, and the electric wire 1 is connected to the insulator string 2.

[発明が解決しようとする課題] 上記の通り、緊線作業には弛度望遠鏡によるバーテック
スへの視準が行なわれるが、鉄塔が大型化し径間が長大
化した結果、当該視準距離が非常に長くなり、バーテッ
クスが具合よく見えないことが多くなった。とくに、送
電線路の立地条件が酷しくなり山岳地に建設されること
が多くなったため、霧やガスといった視界にとっての妨
害物が生じ易く、あるいは逆光などなど、前記視準を一
層困難にする要素も増大している。さらに、電線が4導
体以上の多導体構成となったため、視準の折にどの電線
を見ているのかも不確かとなり、見分けができないとい
った新たな問題点も出現している。
[Problems to be Solved by the Invention] As described above, collimation to a vertex by a sag telescope is performed for tight line work, but as a result of a large tower and a large span, the collimation distance is extremely small. It became very long and I could not see the vertex properly. In particular, because the location conditions of power transmission lines have become severe and construction has often been carried out in mountainous areas, obstacles to the field of view such as fog and gas are likely to occur, or elements that make the collimation more difficult, such as backlighting. Is also increasing. Furthermore, since the electric wire has a multi-conductor structure of four or more conductors, it is uncertain which electric wire to look at when collimating, and there is a new problem that it cannot be distinguished.

このため、最近、視準によることなく高精度に弛度を設
定し得る新たな緊線工法に対する要望が非常に高まって
きている。
For this reason, recently, there has been a great demand for a new tie wire construction method capable of setting the sag with high accuracy without collimation.

また、弛度そのものについてみた場合、本来の弛度は、
第7図に示すように鉄塔アームTaの直下であるP1を観測
点とする弛度d0でなければならないが、実際の観測点は
鉄塔脚P2であり、測定弛度d1は本来の弛度d0に対し第7
図に示すΔdなる誤差を生ずる。この誤差は鉄塔が大型
化するほど大きくなるから、水平角があったり高低差の
大きな鉄塔間においては、無視できない値となってい
る。
Also, when looking at the sag itself, the original sag is
As shown in FIG. 7, the sag d 0 should be the observation point at P 1 directly under the steel tower arm Ta, but the actual observation point is the tower leg P 2 and the measured sag d 1 is originally 7th for the sag d 0 of
The error Δd shown in the figure occurs. This error increases as the size of the tower increases, so it is a value that cannot be ignored between towers with horizontal angles and large height differences.

このほか、測定時の外気温による補正も必要であるが、
その補正をどのようにして行なうかという別な問題もあ
る。
In addition to this, it is necessary to correct by the outside temperature at the time of measurement,
Another problem is how to make that correction.

本発明の目的は、上記した従来の視準による緊線作業を
排除し、緊線中の電線のカテナリ角を修正監視可能な角
度測定装置により弛度を連続的にきわめて高精度に測定
しつつ緊線作業を行ない得る新規な架空線の緊線工法を
提供しようとするものである。
The object of the present invention is to eliminate the above-mentioned conventional collimation work for tight binding, while continuously measuring the sag with extremely high accuracy by an angle measuring device capable of correcting and monitoring the catenary angle of the wire in the tight binding. The purpose of the present invention is to provide a new overhead wire tension line construction method capable of performing a tension line work.

[課題を解決するための手段] 本発明は、鉄塔における碍子連と電線とに別個に高精度
に角度測定が可能なジャイロを取付けて角度を測定し、
その結果を演算器に入力して碍子連の重量による電線の
カテナリ角の補正を行ない、別途演算器に予め知られた
径間長や高低差、温度条件などをインプットしておいて
経済的な弛度を連続的に演算させ、その結果に基いて効
率よく弛度設定を行なうものである。
[Means for Solving the Problem] The present invention measures the angle by separately attaching a gyro capable of highly accurate angle measurement to an insulator string and an electric wire in a steel tower,
The result is input to the calculator to correct the catenary angle of the wire due to the weight of the insulator string, and the calculator separately inputs the previously known span length, height difference, temperature conditions, etc. The degree of sag is continuously calculated, and the degree of sag is efficiently set based on the result.

[作用] 電線のカテナリ角と径間長および高低差が定まれば、電
線弛度は定まる。しかし、単に架線作業中の電線のカテ
ナリ角のみを如何程高精度に測定しても正しい弛度は得
られない。碍子連には大きな重量があり、それによって
カテナリ角が変動しているからである。碍子連によるカ
テナリへの影響は碍子連そのものの構成によるのは当然
のことながら鉄塔の高低差あるいは径間長によっても異
なるから、これを実測しなればわからない。実測するこ
とで電線のカテナリ角の変動がわかり、これを予め演算
器に組み込まれたプログラムに従い補正演算させること
により、直ちに適確な弛度を演算表示させ、その表示に
従い電線の張力調整をすれば、きわめて効率よく高精度
の弛度設定ができることになる。
[Operation] If the catenary angle of the wire, the span length, and the height difference are determined, the wire sag is determined. However, even if only the catenary angle of the electric wire during the overhead wire work is measured with high accuracy, the correct sag cannot be obtained. This is because the insulator has a large weight and the catenary angle fluctuates accordingly. The influence of Insulators on the catenary depends on the composition of Insulators themselves, but it also depends on the height difference and span length of the tower, so it is not possible to measure it. By actually measuring, the change in the catenary angle of the wire can be known.By correcting this according to the program installed in the calculator in advance, the correct slack can be immediately calculated and displayed, and the wire tension can be adjusted according to the display. In this case, it is possible to set the sag with high efficiency and high accuracy.

[実施例] 以下に、本発明について実施例図面を参照し順次説明す
る。
[Embodiment] The present invention will be sequentially described below with reference to the drawings of embodiments.

第1図は、鉄塔T1,T2間に架線される電線1の弛度dを
計算式により求めようとする際の各要素の構成を示す説
明図である。
FIG. 1 is an explanatory diagram showing the configuration of each element when the sag d of the electric wire 1 that is installed between the steel towers T 1 and T 2 is calculated by a calculation formula.

第1図に示すθはカテナリ角(度)、Sは径間長
(m)、hは支持点の高低差(m)、dは弛度(m)で
ある。
In FIG. 1, θ is the catenary angle (degree), S is the span length (m), h is the height difference (m) of the supporting points, and d is the sag (m).

上記構成における弛度計算の一般式はつぎの通りであ
る。(低い側の鉄塔の場合) ここに、 但し、To:水平張力 w:電線の単位重量 式(1)、(2)より 上記(3)式において、径間長Sおよび高低差hは既知
であるから、カテナリ角θさえ定まれば(3)式により
弛度dが定まる。
The general formula for calculating the sag in the above configuration is as follows. (In the case of the lower tower) here, However, To: Horizontal tension w: Unit weight of wire From formulas (1) and (2) Since the span length S and the height difference h are known in the equation (3), the sag d is determined by the equation (3) as long as the catenary angle θ is determined.

しかしながら、すでに説明したように、単に電線1の角
度のみ測定しても第1図に示す真のθははわからない。
碍子連の重量により変動し、得られた値は真のθではな
いからである。
However, as described above, the true θ shown in FIG. 1 cannot be found by simply measuring only the angle of the electric wire 1.
This is because the value varies depending on the weight of the insulator and the obtained value is not true θ.

第2および第3図は、上記真のθの補正値を得るべく、
電線1と碍子連2にそれぞれジャイロ10aおよび10bを取
付け、これらジャイロ10a,10bをリード線11a,11bにより
演算器12に接続した本発明に係る実施例を示す説明図で
ある。
In order to obtain the true correction value of θ,
It is explanatory drawing which shows the Example which concerns on this invention which attached the gyros 10a and 10b to the electric wire 1 and the insulator series 2, respectively, and connected these gyros 10a, 10b to the calculator 12 by the lead wires 11a, 11b.

ジャイロ10a,10bはきわめて微小な角度を測定し得るこ
とが必要であり、従来のメカニカルなジャイロあるいは
電気的なジャイロを用いてもよいが、光ファイバを用い
た光ジャイロスコープを使用することが好ましい。光ジ
ャイロスコープは、そのドリフトが0.01゜/S以下という
高い精度を有している上、応答速度がきわめて速く、し
かも小型軽量であるから、鉄塔上に搬入して第2図の如
く取付ける上でも非常に好都合である。
The gyros 10a and 10b are required to be able to measure extremely minute angles, and a conventional mechanical gyro or an electric gyro may be used, but it is preferable to use an optical gyroscope using an optical fiber. . The optical gyroscope has a high degree of drift of 0.01 ° / S or less, has an extremely fast response speed, and is small and lightweight, so it can be mounted on a steel tower and mounted as shown in Fig. 2. Very convenient.

ジャイロ10aにより電線の現実のカテナリ角θを測定
し、もう一方のジャイロ10bにより碍子連の角度θ
測定する。これら測定結果を演算器に入力させて演算せ
しめれば、補正された真のカテナリ角θを容易に知るこ
とができる。それにより別途入力してある径間長S、高
低差h、さらに必要に応じ温度条件その他の必要データ
を加味して演算せしめれば、弛度dを容易に求め得るか
ら、これを演算器の表示装置により表示し、作業者はそ
の結果を直読し乍ら精確に弛度設定を行ない緊線作業を
行なうことができる。
The actual catenary angle θ 1 of the electric wire is measured by the gyro 10a, and the angle θ 2 of the insulator is measured by the other gyro 10b. The corrected true catenary angle θ can be easily known by inputting these measurement results into a calculator for calculation. Accordingly, the sag d can be easily calculated by taking into consideration the span length S, the height difference h, which have been separately input, and the temperature condition and other necessary data, if necessary. The result can be displayed on the display device, and the operator can read the result directly and set the sag accurately to perform the tight-tie work.

なお、ジャイロと表示器との間をワイヤレスに結合する
ことも可能であり、それにより作業をより簡易化させる
ことが可能となる。
Note that it is possible to wirelessly connect the gyro and the display, which makes it possible to further simplify the work.

また、本発明の技術思想は、送電線のみならずワイヤロ
ープの架線などにも応用することができる。
Further, the technical idea of the present invention can be applied not only to a power transmission line but also to a wire rope overhead line and the like.

[発明の効果] 以上の通り、本発明に係る緊線工法によれば、つぎのよ
うなすぐれた効果を発揮することができる。
[Effects of the Invention] As described above, according to the cording method according to the present invention, the following excellent effects can be exhibited.

(1) バーテックスの取付け、取外しが不要となり、
そのための工数や労務費を低減することができる。
(1) No need to install or remove the vertex,
The man-hours and labor costs for that can be reduced.

(2) 弛度を数値として直読できるので作業能率を大
巾に向上させることができる。
(2) Since the sag can be directly read as a numerical value, the work efficiency can be greatly improved.

(3) 多導体のそれぞれに取付けてやれば電線の不揃
が一目瞭然となり、従来例に比べ調整作業が著しく容易
となる。
(3) If they are attached to each of the multiple conductors, the irregularities of the electric wires can be seen at a glance, and the adjustment work becomes significantly easier than in the conventional example.

(4) 外気温など外乱要因に対する電線弛度の補正を
計算で直ちに行ない得るため、緊線の精度を大巾に高め
ることができる。
(4) Since the wire slackness can be immediately corrected by a calculation for a disturbance factor such as the outside air temperature, the tight line accuracy can be greatly improved.

(5) 光ファイバを使用すれば誘導による影響がな
く、片側活線のままで緊線作業を行なうことができる。
(5) If an optical fiber is used, there is no influence of induction, and it is possible to carry out the tight-tie work with one side live.

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

第1図は、弛度計算に必要な要素を示す説明図、第2お
よび3図は本発明を実施している様子を示す説明図、第
4図は電線の緊線作業状況を示す説明図、第5図は従来
の弛度測定方法を示す説明図、第6図はバーテックスの
見取図、第7図は真の弛度と測定弛度の関係を示す説明
図である。 1:電線、 2:碍子連、 10a,10b:ジャイロ、 12:演算表示器。
FIG. 1 is an explanatory diagram showing the elements necessary for the sag calculation, FIGS. 2 and 3 are explanatory diagrams showing a state in which the present invention is being carried out, and FIG. 4 is an explanatory diagram showing a wire tight working condition of an electric wire. FIG. 5 is an explanatory diagram showing a conventional sag measuring method, FIG. 6 is a sketch of a vertex, and FIG. 7 is an explanatory diagram showing the relationship between true sag and measured sag. 1: Electric wire, 2: Insulator series, 10a, 10b: Gyro, 12: Calculation display.

Claims (2)

【特許請求の範囲】[Claims] 【請求項1】電線の所定位置と碍子連の所定位置にそれ
ぞれ高精度に角度を測定し得るジャイロを設置し、電線
側ジャイロにより測定した角度と碍子連側にジャイロに
より測定した角度のそれぞれを演算器に入力すると共
に、予め測定された径間長、高低差などの必要データを
別途前記演算器に入力させ、碍子連の重量による電線の
カテナリ角の変動を補正して演算表示させることにより
緊線中の電線の正確な弛度を確認しつつ弛度調整をする
送電線の緊線工法。
1. A gyro capable of highly accurately measuring an angle is installed at a predetermined position of an electric wire and a predetermined position of an insulator string, and the angle measured by the gyro on the wire side and the angle measured by the gyro on the insulator string side are respectively set. By inputting the necessary data such as span length and height difference measured in advance into the calculator as well as inputting into the calculator, the fluctuation of the catenary angle of the wire due to the weight of the insulator is corrected and the calculation is displayed. Tightening method for power transmission lines that adjusts the slack while confirming the exact slack of the wires.
【請求項2】ジャイロが光ジャイロスコープである請求
項1記載の送電線の緊線工法。
2. The method of tightening a power transmission line according to claim 1, wherein the gyro is an optical gyroscope.
JP14498488A 1988-06-13 1988-06-13 Tightening method for power lines Expired - Lifetime JPH0757046B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP14498488A JPH0757046B2 (en) 1988-06-13 1988-06-13 Tightening method for power lines

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP14498488A JPH0757046B2 (en) 1988-06-13 1988-06-13 Tightening method for power lines

Publications (2)

Publication Number Publication Date
JPH01315210A JPH01315210A (en) 1989-12-20
JPH0757046B2 true JPH0757046B2 (en) 1995-06-14

Family

ID=15374776

Family Applications (1)

Application Number Title Priority Date Filing Date
JP14498488A Expired - Lifetime JPH0757046B2 (en) 1988-06-13 1988-06-13 Tightening method for power lines

Country Status (1)

Country Link
JP (1) JPH0757046B2 (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
KR101314638B1 (en) * 2013-08-16 2013-10-04 (주)한백 Electric wire tension method using portable winch
KR20200039971A (en) * 2018-10-08 2020-04-17 한국전력공사 Checking devcie of installation for suspension insulator
WO2022158947A1 (en) * 2021-01-25 2022-07-28 엑사이트 Method for estimating overhead power transmission line by using acceleration and angular velocity or imu sensor

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
KR101314638B1 (en) * 2013-08-16 2013-10-04 (주)한백 Electric wire tension method using portable winch
KR20200039971A (en) * 2018-10-08 2020-04-17 한국전력공사 Checking devcie of installation for suspension insulator
WO2022158947A1 (en) * 2021-01-25 2022-07-28 엑사이트 Method for estimating overhead power transmission line by using acceleration and angular velocity or imu sensor

Also Published As

Publication number Publication date
JPH01315210A (en) 1989-12-20

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