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JPH0575981B2 - - Google Patents
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JPH0575981B2 - - Google Patents

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Publication number
JPH0575981B2
JPH0575981B2 JP1358789A JP1358789A JPH0575981B2 JP H0575981 B2 JPH0575981 B2 JP H0575981B2 JP 1358789 A JP1358789 A JP 1358789A JP 1358789 A JP1358789 A JP 1358789A JP H0575981 B2 JPH0575981 B2 JP H0575981B2
Authority
JP
Japan
Prior art keywords
cable
voltage
transformer
conductor
output
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
JP1358789A
Other languages
Japanese (ja)
Other versions
JPH02194371A (en
Inventor
Hiroshi Takechi
Atsushi Iga
Yasutaka Fujiwara
Jiro Kawai
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.)
Shikoku Research Institute Inc
Shikoku Electric Power Co Inc
SWCC Corp
Original Assignee
Shikoku Research Institute Inc
Shikoku Electric Power Co Inc
Showa Electric Wire and Cable Co
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 Shikoku Research Institute Inc, Shikoku Electric Power Co Inc, Showa Electric Wire and Cable Co filed Critical Shikoku Research Institute Inc
Priority to JP1358789A priority Critical patent/JPH02194371A/en
Publication of JPH02194371A publication Critical patent/JPH02194371A/en
Publication of JPH0575981B2 publication Critical patent/JPH0575981B2/ja
Granted legal-status Critical Current

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  • Testing Relating To Insulation (AREA)

Description

【発明の詳細な説明】 (産業上の利用分野) 本発明は、活線状態のケーブルの誘電体損測定
方法に関する。
DETAILED DESCRIPTION OF THE INVENTION (Field of Industrial Application) The present invention relates to a method for measuring dielectric loss of a live cable.

(従来の技術) 電力ケーブルの絶縁体の誘電体損は、ケーブル
の性能を定める重要な要素のひとつである。一般
にケーブルの誘電体損はtanδを用いて評価され
る。未だ布設されていない出荷前のケーブルにつ
いてのtanδは、シエーリングブリツジ等を使用し
て測定される。一方、活線状態のケーブルについ
てのtanδの測定は、次のようにして行なわれる。
(Prior Art) The dielectric loss of the insulator of a power cable is one of the important factors that determines the performance of the cable. Generally, the dielectric loss of a cable is evaluated using tanδ. The tan δ of a cable that has not yet been installed and is yet to be shipped is measured using a shearing bridge or the like. On the other hand, the measurement of tan δ for a live cable is performed as follows.

第6図にその測定方法の説明図を示す。 FIG. 6 shows an explanatory diagram of the measuring method.

図に示したケーブル1は、その導体2の一端2
aが交流電源3に接続され、他端2bが負荷4に
接続されている。そして、その一端2aは、(検
出用抵抗器5に接続されている。一方、このケー
ブル1のシース7は、片端が接地線8を介して直
接接地されている。通常、ケーブルシース7の両
端を直接接地すると、ケーブルシース7に大きな
誘導電流が循環するため、実線路ではこのように
接地方法を採用する場合が多い。この接地線8に
は、電流測定のためのカレントトランス9が装着
されている。
The cable 1 shown in the figure has one end 2 of its conductor 2.
A is connected to the AC power supply 3, and the other end 2b is connected to the load 4. One end 2a of the cable 1 is connected to a detection resistor 5.On the other hand, one end of the sheath 7 of the cable 1 is directly grounded via a grounding wire 8.Normally, both ends of the cable sheath 7 If the wire is directly grounded, a large induced current will circulate in the cable sheath 7, so this grounding method is often adopted in actual lines.A current transformer 9 for current measurement is attached to this ground wire 8. ing.

上記検出用抵抗器5には、電圧測定用端子10
を設け、上記カレントトランス9の出力の一端9
aは接地し、他端9bに充電電流測定用端子12
を設ける。
The detection resistor 5 has a voltage measurement terminal 10.
and one end 9 of the output of the current transformer 9
A is grounded, and the other end 9b is a charging current measurement terminal 12.
will be established.

このように結線すると、ケーブルシース7が片
端接地のため、接地線8には、ケーブル1の静電
容量に基づく充電電流のみが流れる。従つて、電
圧測定用端子10の出力電圧は、ケーブル1の導
体2に印加される交番電圧Eに比例し、充電電流
測定用端子12の出力電圧は、ケーブル1の充電
電流Iに比例する。tanδは、この交番電圧Eと充
電電流Iの位相角から求めることができる。一般
には交番電圧Eと充電電流Iとのベクトル積を両
者のスカラー積が除算してtanδを求めるようにし
ている。
When connected in this manner, only the charging current based on the capacitance of the cable 1 flows through the ground wire 8 because the cable sheath 7 is grounded at one end. Therefore, the output voltage of the voltage measuring terminal 10 is proportional to the alternating voltage E applied to the conductor 2 of the cable 1, and the output voltage of the charging current measuring terminal 12 is proportional to the charging current I of the cable 1. tan δ can be determined from the phase angle between this alternating voltage E and charging current I. Generally, tan δ is determined by dividing the vector product of alternating voltage E and charging current I by the scalar product of both.

尚、実際に、図中一点鎖線で囲んだ検出部13
と、演算等のデータ処理を行なう測定部14とを
一体にした活線tanδ測定器も既に市販されている
(シヨウチエツカTD:昭和電線電纜株式会社商
標)。
In addition, in reality, the detection unit 13 surrounded by a dashed line in the figure
A live line tan δ measuring device that integrates a measuring unit 14 for performing data processing such as calculations is already commercially available (Showa Cable TD: trademark of Showa Cable and Cable Co., Ltd.).

(発明が解決しようとする課題) ところで、上記のように測定の際、第6図に示
した検出部13の検出用抵抗器5の一端を、次の
ようにケーブル導体2の一端2aに装着して電圧
を取出す。
(Problem to be Solved by the Invention) By the way, during the measurement as described above, one end of the detection resistor 5 of the detection unit 13 shown in FIG. 6 is attached to one end 2a of the cable conductor 2 as follows. and extract the voltage.

第7図は、その電圧取出し法の説明図である。 FIG. 7 is an explanatory diagram of the voltage extraction method.

図において、検出用抵抗器5は絶縁体棒15の
内部に埋込まれており、検出用抵抗器5の先端5
aにはフツク16が取付けられている。このフツ
ク16がケーブルヘツド17の近傍のリード線1
8に装着される。検出用抵抗器5の後端5bは、
第6図に示した検出部13の電圧測定用端子10
に接続される。
In the figure, the detection resistor 5 is embedded inside the insulator rod 15, and the tip 5 of the detection resistor 5
A hook 16 is attached to a. This hook 16 is connected to the lead wire 1 near the cable head 17.
It is installed on 8. The rear end 5b of the detection resistor 5 is
Voltage measurement terminal 10 of the detection unit 13 shown in FIG.
connected to.

しかしながら、上記の方法を実施する場合、作
業者はゴム手袋等を使用して、絶縁体棒15の後
端側を掴み、ケーブルヘツド17の近傍に組立て
られた図示しない足場上で上記装着作業を行なう
ことになる。
However, when carrying out the above method, the operator uses rubber gloves or the like to grasp the rear end side of the insulator rod 15, and performs the above installation work on a scaffold (not shown) assembled near the cable head 17. I will do it.

従つて、このような作業は、活線状態のケーブ
ル導体に近付くという危険を伴う一方、足場の組
立て、その他長時間の準備作業を必要とするとい
う問題があつた。
Therefore, such work involves the danger of getting close to live cable conductors, and at the same time poses problems in that it requires assembling scaffolding and other preparatory work over a long period of time.

本発明は以上の点に着目してなされたもので、
安全に短時間で測定作業を行なうことができるケ
ーブルの誘電体損測定方法を提供することを目的
とするものである。
The present invention has been made focusing on the above points,
The object of the present invention is to provide a method for measuring dielectric loss of a cable, which allows measurement work to be carried out safely and in a short time.

(課題を解決するための手段) 本発明のケーブルの誘電体損測定方法は、ケー
ブル線路に予め設置された計器用変圧器の出力を
検出し、かつ、前記計器用変圧器の入力電圧と出
力電圧との間の位相のずれを補正して、ケーブル
の導体に印加された交番電圧を測定する一方、前
記ケーブルの充電電流を測定して、前記交番電圧
と前記充電電流との関係により誘電体損を求める
ことを特徴とするものである。
(Means for Solving the Problems) A method for measuring dielectric loss of a cable according to the present invention detects the output of a voltage transformer installed in advance on a cable line, and detects the input voltage and output voltage of the voltage transformer. The alternating voltage applied to the conductor of the cable is measured by correcting the phase shift between the voltage and the charging current of the cable. It is characterized by seeking losses.

(作用) 以上の方法は、ケーブル線路監視用計器を動作
させるための既設の計器用変圧器を、ケーブル導
体に印加された交番電圧を測定するために使用す
る。しかし、計器用変圧器は通常、入力電圧と出
力電圧の間に一定の位相のずれを生じさせる。そ
こで、このずれを位相補正回路等を用いて補正し
て、その後、ケーブルの充電電流との関係より、
ケーブルの誘電体損を測定する。このようにすれ
ば、計器用変圧器の出力電圧は比較的低圧だか
ら、危険な高電圧高所作業を回避し、かつ、作業
を簡略化することができる。
(Operation) In the above method, an existing instrument transformer for operating a cable line monitoring instrument is used to measure the alternating voltage applied to the cable conductor. However, potential transformers typically introduce a certain phase shift between the input voltage and the output voltage. Therefore, this deviation is corrected using a phase correction circuit, etc., and then, from the relationship with the cable charging current,
Measure the dielectric loss of the cable. In this way, since the output voltage of the potential transformer is relatively low, dangerous high-voltage work at high places can be avoided and the work can be simplified.

(実施例) 以下、本発明を図の実施例を用いて詳細に説明
する。
(Examples) Hereinafter, the present invention will be explained in detail using examples shown in the drawings.

第1図は、本発明のケーブルの誘電体損測定方
法の実施例説明図である。
FIG. 1 is an explanatory diagram of an embodiment of the method for measuring dielectric loss of a cable according to the present invention.

図において、ケーブル1の導体2は、ケーブル
ヘツド17とリード線18を介してその一端2a
が交流電源3に接続されている。また、この導体
2の一端2aには、計器用変圧器20が接続され
ている。更に、ケーブル1のシース7は接地線8
により接地され、ここに変流器9が取付けられて
いる。
In the figure, the conductor 2 of the cable 1 is connected to one end 2a via a cable head 17 and a lead wire 18.
is connected to the AC power supply 3. Furthermore, an instrument transformer 20 is connected to one end 2a of the conductor 2. Furthermore, the sheath 7 of the cable 1 is connected to the ground wire 8
The current transformer 9 is attached to the ground.

上記計器用変圧器20の出力は、位相補正回路
21を介して測定部22に入力するよう結線され
る。また、この測定部22には、変流器9の出力
が合わせて入力するよう結線されている。
The output of the instrument transformer 20 is wired to be input to a measuring section 22 via a phase correction circuit 21 . Further, the measuring section 22 is connected so that the output of the current transformer 9 is also input thereto.

上記計器用変圧器20は、一般に、変電所等の
ケーブル線路中の主要部分に既に設置されている
ものを使用する。即ち、送変電用設備の運転状態
を監視するために、通常、電圧計や電流計が各所
に取付けられる。これらの計器類を動作させるた
めに、計器用変圧器が変流器が設置されており、
それを利用する。
The above-mentioned instrument transformer 20 is generally one that is already installed in a main part of a cable line at a substation or the like. That is, in order to monitor the operating status of power transmission and substation equipment, voltmeters and ammeters are usually installed at various locations. In order to operate these instruments, a voltage transformer and a current transformer are installed.
Take advantage of it.

第2図に、ごく一般的な計器用変圧器の結線例
を示す。
Figure 2 shows an example of wiring for a very common potential transformer.

図の計器用変圧器20は、一次側をケーブル導
体に接続し、二次側から計器類を動作させるため
の電圧を取出すトランスから成る。例えば、この
入力電圧20aは3800V程度とされ、出力電圧2
0bは110Vに設置される。
The illustrated instrument transformer 20 consists of a transformer whose primary side is connected to a cable conductor and whose secondary side extracts a voltage for operating instruments. For example, this input voltage 20a is about 3800V, and the output voltage 20a is about 3800V.
0b is installed at 110V.

また、第3図に変流器9の結線図を示す。この
変流器9は、既に第6図に説明したものと同一の
構成のものである。
Further, a wiring diagram of the current transformer 9 is shown in FIG. This current transformer 9 has the same structure as that already explained in FIG.

次に、第1図に示した位相補正回路21は、上
記計器用変圧器20の入力電圧20aと出力電圧
20bとの間の位相のずれを補正するための回路
で、既知の図示しないコンデンサと抵抗を組み合
わせた梯子型回路等から構成される。
Next, the phase correction circuit 21 shown in FIG. 1 is a circuit for correcting the phase shift between the input voltage 20a and the output voltage 20b of the above-mentioned voltage transformer 20, and is a circuit that uses a known capacitor (not shown). It consists of a ladder-type circuit that combines resistors.

第4図に、その回路動作の説明図を示す。 FIG. 4 shows an explanatory diagram of the circuit operation.

図のように、計器用変圧器の出力電圧E′は、ケ
ーブル導体に印加された交番電圧Eに対し、例え
ばその電圧位相がαだけずれを生じる。第2図に
示したようなトランス型の計器用変圧器の場合、
出力電圧の位相は入力電圧の位相に比べて遅れ、
コンデンサ分圧型の場合には進む傾向にある。
As shown in the figure, the voltage phase of the output voltage E' of the potential transformer deviates, for example, by α with respect to the alternating voltage E applied to the cable conductor. In the case of a transformer-type potential transformer as shown in Figure 2,
The phase of the output voltage is delayed compared to the phase of the input voltage,
In the case of capacitor voltage division type, there is a tendency to advance.

第1図の位相補正回路21は、これを補正し、
元のケーブル導体に印加された交番用電圧と同位
相の交番電圧21aを、測定部22に対して出力
する。
The phase correction circuit 21 in FIG. 1 corrects this,
An alternating voltage 21a having the same phase as the alternating voltage applied to the original cable conductor is output to the measuring section 22.

測定部22は、既に第7図で説明した既知の
tanδ測定回路から構成されておりり、位相補正回
路21から出力される交番電圧21aと、変流器
9から出力される充電電流9cとの位相角を求
め、tanδの測定を行なう。
The measuring section 22 uses the known method already explained in FIG.
It consists of a tan δ measurement circuit, which determines the phase angle between the alternating voltage 21a output from the phase correction circuit 21 and the charging current 9c output from the current transformer 9, and measures tan δ.

即ち、第5図に示すように、交番電圧Eに対し
充電電流Iは(π/4)−δだけ位相が進み、ケ
ーブル絶縁体の直流抵抗分rにより、図のtanδ、
即ちr/ωcに相当する分、誘電損失が生じる。
尚、ωは電源の角周波数、cはケーブル絶縁体の
静電容量である。この原理に基づき、既知の方法
によりtanδを算出すればよい。
That is, as shown in FIG. 5, the charging current I has a phase advance of (π/4)-δ with respect to the alternating voltage E, and due to the direct current resistance r of the cable insulator, tanδ in the figure
That is, a dielectric loss occurs by an amount corresponding to r/ωc.
Note that ω is the angular frequency of the power source, and c is the capacitance of the cable insulator. Based on this principle, tan δ may be calculated by a known method.

本発明は以上の実施例に限定されない。 The present invention is not limited to the above embodiments.

ケーブルの充電電流は、必ずしも変流器によら
ず、他の方法によつて測定しても差し支えない。
また、上記位相補正回路は、測定部の内部に一体
に組み込まれるようにしても差し支えない。
The charging current of the cable is not necessarily measured using a current transformer, but may be measured using other methods.
Furthermore, the phase correction circuit may be integrated into the measuring section.

(発明の効果) 以上説明した本発明の方法によれば、ケーブル
線路に予め設置された計器用変圧器を用いて、ケ
ーブルの導体に印加された交番電圧を測定するた
め、高圧高所作業を回避することができる。更
に、測定の準備作業等を安全に、かつ、迅速に行
なうことができ、作業能率の向上を図ることがで
きる。
(Effects of the Invention) According to the method of the present invention explained above, the alternating voltage applied to the conductor of the cable is measured using the instrument transformer installed in advance on the cable line, so high-voltage work at high places is not required. can be avoided. Furthermore, preparation work for measurement, etc. can be performed safely and quickly, and work efficiency can be improved.

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

第1図は本発明のケーブルの誘電体損測定方法
の実施例説明図、第2図は計器用変圧器の結線
図、第3図は変流器の結線図、第4図は位相補正
回路の動作説明図、第5図は測定部の動作説明
図、第6図は従来のケーブルの誘電体損測定方法
の説明図、第7図はその電圧取出し法の説明図で
ある。 1……ケーブル、2……導体、3……交流電
源、7……シース、8……接地線、9……変流
器、17……ケーブルヘツド、20……計器用変
圧器、21……位相補正回路、22……測定部。
Fig. 1 is an explanatory diagram of an embodiment of the cable dielectric loss measurement method of the present invention, Fig. 2 is a wiring diagram of a potential transformer, Fig. 3 is a wiring diagram of a current transformer, and Fig. 4 is a phase correction circuit. 5 is an explanatory diagram of the operation of the measuring section, FIG. 6 is an explanatory diagram of a conventional cable dielectric loss measurement method, and FIG. 7 is an explanatory diagram of the voltage extraction method. DESCRIPTION OF SYMBOLS 1... Cable, 2... Conductor, 3... AC power supply, 7... Sheath, 8... Ground wire, 9... Current transformer, 17... Cable head, 20... Instrument transformer, 21... ...Phase correction circuit, 22...Measurement section.

Claims (1)

【特許請求の範囲】[Claims] 1 ケーブル線路に予め設置された計器用変圧器
の出力を検出し、かつ、前記計器用変圧器の入力
電圧と出力電圧との間の位相のずれを補正して、
ケーブルの導体に印加された交番電圧を測定する
一方、前記ケーブルの充電電流を測定して、前記
交番電圧と前記充電電流との関係により誘電体損
を求めることを特徴とするケーブルの誘電体損測
定方法。
1. Detecting the output of a potential transformer installed in advance on a cable line, and correcting the phase shift between the input voltage and output voltage of the potential transformer,
A dielectric loss of a cable, characterized in that an alternating voltage applied to a conductor of the cable is measured, and a charging current of the cable is measured, and the dielectric loss is determined from the relationship between the alternating voltage and the charging current. Measuring method.
JP1358789A 1989-01-23 1989-01-23 Measurement of dielectric loss of cable Granted JPH02194371A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP1358789A JPH02194371A (en) 1989-01-23 1989-01-23 Measurement of dielectric loss of cable

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP1358789A JPH02194371A (en) 1989-01-23 1989-01-23 Measurement of dielectric loss of cable

Publications (2)

Publication Number Publication Date
JPH02194371A JPH02194371A (en) 1990-07-31
JPH0575981B2 true JPH0575981B2 (en) 1993-10-21

Family

ID=11837321

Family Applications (1)

Application Number Title Priority Date Filing Date
JP1358789A Granted JPH02194371A (en) 1989-01-23 1989-01-23 Measurement of dielectric loss of cable

Country Status (1)

Country Link
JP (1) JPH02194371A (en)

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2535292B2 (en) * 1992-10-23 1996-09-18 大電株式会社 A method for diagnosing deterioration of cable insulation performance.
CN110133456B (en) * 2019-05-21 2021-03-19 深圳供电局有限公司 Construction method of criterion system for ultra-low frequency dielectric loss testing of cable insulation

Also Published As

Publication number Publication date
JPH02194371A (en) 1990-07-31

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