JPS604802A - How to measure the distance to the disconnection point - Google Patents
How to measure the distance to the disconnection pointInfo
- Publication number
- JPS604802A JPS604802A JP11447683A JP11447683A JPS604802A JP S604802 A JPS604802 A JP S604802A JP 11447683 A JP11447683 A JP 11447683A JP 11447683 A JP11447683 A JP 11447683A JP S604802 A JPS604802 A JP S604802A
- Authority
- JP
- Japan
- Prior art keywords
- capacitance
- distance
- point
- cable
- measured
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Granted
Links
Landscapes
- Measurement Of Length, Angles, Or The Like Using Electric Or Magnetic Means (AREA)
- Locating Faults (AREA)
Abstract
(57)【要約】本公報は電子出願前の出願データであるた
め要約のデータは記録されません。(57) [Summary] This bulletin contains application data before electronic filing, so abstract data is not recorded.
Description
【発明の詳細な説明】
(イ)産業上の利用分野
この発明は、たとえば地中埋設、海底敷設電線等の断線
障害箇所を検出するのに有効な断線箇所までの距離測定
方法に関する。DETAILED DESCRIPTION OF THE INVENTION (a) Field of Industrial Application The present invention relates to a distance measuring method to a disconnection point that is effective for detecting a disconnection point in, for example, underground or undersea cables.
←)従来技術
一般に、絶縁ケープ/I/(電線等)内に断線事故が生
じた場合、ケーブルの被覆を取除くことなしに断線箇所
を発見することは極めて難しい。とりわけ、直接手にす
るととの困難な地中埋設電線。←) Prior Art Generally, when a breakage occurs in an insulating cape/I/(electric wire, etc.), it is extremely difficult to find the breakage point without removing the cable sheath. In particular, underground power lines are difficult to handle directly.
海底敷設電線等の断線障害箇所までの距離を知ることは
不可能に近い。近年、これを解決する方法として、ケー
フ諏しにパルス電圧を導入し5反則電圧の遅れを検出す
る方法や、同−条件線の容量と比較することによシ算出
する方法が試みられているが、なお確実な測定結果を得
るにいたっていない。It is almost impossible to know the distance to the point of disconnection in submarine power lines, etc. In recent years, attempts have been made to solve this problem by introducing a pulse voltage into the Keff voltage and detecting the delay in the 5-fault voltage, or by calculating the delay by comparing it with the capacitance of the line under the same conditions. However, reliable measurement results have not yet been obtained.
(ハ)目的
この発明の目的は、ケーブル芯線が外皮で被覆されてい
るケーブルでも、また地中埋設や海底敷設されているケ
ーブルであっても、ケーブルが少なくとも1苅の芯線を
含む場合、断線箇所を正確。(c) Purpose The purpose of this invention is to prevent cable breakage in the case where the cable includes at least one core wire, even if the cable core wire is covered with an outer sheath, or even if the cable is buried underground or laid on the seabed. Accurate location.
容易に発見し得る断線箇所までの距離測定方法を提供す
ることである。It is an object of the present invention to provide a method for measuring the distance to a disconnection point that can be easily discovered.
に)IM成
手記1」的を達成するために、この発明は対線の一方端
末を短絡状態とし、前記対線の各々と他の同一対象物体
間の静電容量CA、CBと、前記対線双方を一括したも
のと前記同一対象物体間の静電容量CWをそれぞれ計測
し、これら計測した静電容量CA、CB、CWと既知の
ケーブルの全長L Tとから、LS=(CW+CB4C
A)、LT/CWの演算をなすことにより、断線箇所ま
での距離LSを算出するようにしている。In order to achieve the objective of IM Completion Note 1, this invention short-circuits one terminal of the pair of wires, and reduces the capacitance CA, CB between each of the pair of wires and another identical target object, and the pair of wires. Measure the capacitance CW of both lines together and the same target object, and from these measured capacitances CA, CB, CW and the known total length of the cable, LS = (CW + CB4C
A) The distance LS to the disconnection point is calculated by calculating LT/CW.
(ト)実施例 以下、実施例によシこの発明の詳細な説明する。(g) Examples Hereinafter, the present invention will be explained in detail by way of examples.
第1図は、この発明の一実施例を示す概略図である。同
図において1は断線箇所までの距離を測定すべきケーブ
ルであって、1対の芯線2,3及びシールド導体4より
なるものである。5は容量測定演算器であり、各芯線2
,3とシールド導体間の静電容量:を測定するとともに
、測定した静電容量に基づいて断線箇所までの距離を演
算するものである。芯線2,3の一端A、Bはそれぞれ
スイッチSA、SBを介して容量測定演算器5に接続さ
れ、まだ、芯線2,3の一端A、BはスイッチSWを介
して互いに共通接続されるようになっている。さらにま
た測定時には芯線2,3の他端が短絡される(F点)。FIG. 1 is a schematic diagram showing an embodiment of the present invention. In the figure, reference numeral 1 denotes a cable whose distance to the disconnection point is to be measured, and is composed of a pair of core wires 2 and 3 and a shield conductor 4. 5 is a capacitance measurement calculator, and each core wire 2
, 3 and the shield conductor, and calculates the distance to the disconnection point based on the measured capacitance. One ends A and B of the core wires 2 and 3 are connected to the capacitance measuring calculator 5 through switches SA and SB, respectively, and one ends A and B of the core wires 2 and 3 are still commonly connected to each other through a switch SW. It has become. Furthermore, during measurement, the other ends of the core wires 2 and 3 are short-circuited (point F).
もつとも他端に電子回路等の低インピーダンヌ回路が接
続されており、略短絡状態の場合にはそのitでよい。Of course, a low impedance circuit such as an electronic circuit is connected to the other end, and in the case of a substantially short-circuited state, it is sufficient.
今、芯線口のD点が断線しているとして、一端BよりD
点までの距離L Sをめる方法を説明する。Now, suppose that point D of the core wire opening is broken, and from one end B to D
We will explain how to calculate the distance LS to the point.
先ず、スイッチSW、SBを開放した状態でスイッチS
Aをオンし、容量測定演算器5で芯線2とシールド導体
4間の静電容量CAを測定する。First, with switches SW and SB open, switch S
A is turned on, and the capacitance CA between the core wire 2 and the shield conductor 4 is measured by the capacitance measurement calculator 5.
次にスイッチSBをオンし、スイッチSW、SAをオフ
にした状態とし、芯線6とシールド導体4間の静電容量
CBを測定する。続いて、スイッチSWをオンし、スイ
ッチSAもしくはスイッチSBのいずれかをオンにし、
芯線2,3を一括したものとシールド導体4間の静電容
量CWを測定する。これらの静電容量CA、CB、CW
を測定すると、容量測定演算器5は、別に入力される既
知のケーブル1)長LTと静電容量CA、CB、CWと
により次式の演算を行ない。Next, the switch SB is turned on, the switches SW and SA are turned off, and the capacitance CB between the core wire 6 and the shield conductor 4 is measured. Next, turn on switch SW, turn on either switch SA or switch SB,
The capacitance CW between the core wires 2 and 3 collectively and the shield conductor 4 is measured. These capacitances CA, CB, CW
When , the capacitance measurement calculator 5 calculates the following equation using the known cable 1) length LT and the capacitances CA, CB, and CW that are input separately.
L3=(CW+CB−CA)・LT/CW ・・・(1
)一端A、Bから断線箇所り点までの距離LSを算出す
る。L3=(CW+CB-CA)・LT/CW...(1
) Calculate the distance LS from one end A, B to the point where the wire breaks.
次に」二線(1)式によシ、断線箇所までの距離LSが
算出され得る理由について説明する。Next, the reason why the distance LS to the disconnection point can be calculated using the two-line equation (1) will be explained.
第1図において、A点とシールド導体4との静電界ji
ljcAは、芯線2のAE(F一点:断線箇所り点に対
応する芯線2の位置)の静電容量をCAE。In FIG. 1, the electrostatic field ji between point A and the shield conductor 4
ljcA is the CAE capacitance of the core wire 2 (one point F: the position of the core wire 2 corresponding to the point where the wire is broken).
対の芯線2,3の点EF、DFの静電容量をCEDFと
すると。Let CEDF be the capacitance at points EF and DF of the pair of core wires 2 and 3.
CA:CAE+CEDF ・−・−(2)である。一方
、B点とシールド導体4との静電容量CBは、芯線ろの
BDの静電容量CBDである。CA: CAE+CEDF ・−・−(2). On the other hand, the capacitance CB between point B and the shield conductor 4 is the capacitance CBD of the core wire BD.
捷だ1対の芯線2と6は71静電容量測定端に対しz1
称であるから。The core wires 2 and 6 of the pair of wires are z1 for the 71 capacitance measurement end.
Because it is a nickname.
CAE=CBD=CB ・=・ (a)である。ケープ
/V 1は全域に亘って同じ形であり。CAE=CBD=CB .=. (a). Cape/V 1 has the same shape throughout.
芯線2,3の一括の静電容量CWはケーブルの長さLに
比例する。しだがって、ケーブルの単位長さ当υの静電
容量をCoとすると
CW = Co X LT ・・・・・(4)CEDF
=Co X LR−−(5)ただしLR: DF (
EF )間の距離となる。壕だ(2)式から
CEDF=CA−C1・・・・・・(6)(3)式と(
6)式より
CEDF−CA−CB =、−9(7)B点より断線箇
所り点までの距離L SはLS=LT−LR・・・・・
・(8)
この(8)式に1 (4)(5)式のLT、LRを入れ
るとこの(9)式に(7)式のCEDFを入れるとLS
= (cw+ CB −CA)/Co −−−−−−
Q(1また(4)式より
Co = CW / LT −−−=−0υこのθ1)
式のCoを(1C1式に入れると。The collective capacitance CW of the core wires 2 and 3 is proportional to the length L of the cable. Therefore, if the capacitance per unit length υ of the cable is Co, then CW = Co X LT (4) CEDF
=Co X LR--(5) However, LR: DF (
EF). From equation (2), CEDF=CA-C1...(6), equation (3) and (
From formula 6), CEDF-CA-CB =, -9 (7) Distance LS from point B to the point of disconnection is LS = LT-LR...
・(8) If we insert LT and LR from equations (4) and (5) into equation (8), and CEDF from equation (7) into equation (9), we get LS
= (cw+ CB −CA)/Co −−−−−−
Q (1 or from equation (4), Co = CW / LT --- = -0υ this θ1)
If we put Co in the formula into the formula (1C1).
LS=(CW−1−CB−CA)、LT/CWとなり、
当初の(1)式が得られる。すなわち既知のケーブル1
の全長LTと測定した静電容量CA。LS=(CW-1-CB-CA), LT/CW,
The original equation (1) is obtained. i.e. known cable 1
Total length LT and measured capacitance CA.
CB、CWより断線箇所までの距離LSを算出できる。The distance LS to the disconnection point can be calculated from CB and CW.
第1図の実施例に使用される容量測定演算器の一例を第
2図に示している。この容量測定演算器はケーブル長が
大きいときに、有効である。An example of a capacitance measuring calculator used in the embodiment of FIG. 1 is shown in FIG. This capacitance measurement calculator is effective when the cable length is long.
第2図においてCXは未知静電容量であシ、ヌイツチS
1により、電源10と、抵抗Rにそれぞれ並列に切換え
て接続されるようになっている。In Figure 2, CX is an unknown capacitance, and Nichitsu S
1, the power supply 10 and the resistor R are switched in parallel and connected to each other.
11はコンパレータであって、入力電圧E(抵抗Rの端
子電圧)が+、限電圧EOよりも小で、下限71工圧E
Cよりも犬の時、出力信号VGを出力する。11 is a comparator, and the input voltage E (terminal voltage of resistor R) is +, which is smaller than the limit voltage EO, and the lower limit 71 engineering pressure E.
When C is a dog, an output signal VG is output.
12はパルス列信号VPを出力するパルス列発生器、1
3はコンパレータ11より出力信号VCが入力される間
、パルス列発生器12よシのパルス(言号VCを出力す
るゲート回路、14はゲート回路13よりのパルス信号
VCを受けてカウントするカウンタ、15はカウンタ1
4のカランI・値を測定静電容量として記憶して、」−
記(1)式等の演算を行なう記憶演算回路である。12 is a pulse train generator that outputs a pulse train signal VP;
3 is a gate circuit that outputs the pulse (word VC) from the pulse train generator 12 while the output signal VC from the comparator 11 is input; 14 is a counter that receives and counts the pulse signal VC from the gate circuit 13; 15; is counter 1
Memorize the Curran I value of 4 as the measured capacitance, and
This is a memory calculation circuit that performs calculations such as the following equation (1).
この容量測定演算器では、先ずスイッチS1をa側に倒
し、電源10の電圧ESで被…l]定静電容量CXを充
電する。次にスイッチS1をb側に倒すと、被測定静電
容量CXに充電されていた電荷は抵抗Rを通じて放電す
る。この場合の抵抗Rの両端電圧Eは第6図(a)に示
すようにts時点からtoは電圧Eが上限電圧Eoに達
しだ時点を示し。In this capacitance measurement calculator, first, the switch S1 is turned to the a side, and the constant capacitance CX is charged with the voltage ES of the power supply 10. Next, when the switch S1 is turned to the b side, the charge stored in the capacitance to be measured CX is discharged through the resistor R. In this case, the voltage E across the resistor R is from time ts to the time when the voltage E reaches the upper limit voltage Eo, as shown in FIG. 6(a).
jcは電圧Eが下限電圧Ecに達した時点を示してオリ
、時点toからtcの間、コンパレータ11は出力信号
VG[第6図の(b) 参照]を出力し、この出力信号
VGが加えられる間ゲート回路1ろはパルス信号VC〔
第6図の(d)参照〕を出力する。この出力されたパル
ス信号はカウンタ14でカウントされるが、カウント値
はtoからtcの期間が長い稈犬となる。このtoから
tcまでの期間は被測定静電容量CXに比例するものな
ので、カウンタ14のカラン日丸は被測定静電容量CX
に対応することになり、そのカウント値から被測定静電
容fi<CXを知ることができる。被測定静電容量CX
として、第1図で示しだ静電容量CA、CB、CWを測
定し、静電容量CA、CB、CWに対応するものとして
カウンタ14のパルスカウント値NA、NB、NWが得
られると、(1)式に対応してLS−(NW−NA4−
NB)・LT/NW ・・・・・・α埠よゆ、断線箇所
までの距離LSを算出できる。jc indicates the point in time when the voltage E reaches the lower limit voltage Ec. During the period from time to to tc, the comparator 11 outputs the output signal VG [see (b) in FIG. 6], and this output signal VG Gate circuit 1 Loha pulse signal VC [
(See FIG. 6(d))] is output. This output pulse signal is counted by the counter 14, and the count value has a long period from to to tc. Since the period from to to tc is proportional to the capacitance to be measured CX, the counter 14's counter 14 is the capacitance to be measured CX.
Therefore, from the count value, it is possible to know that the capacitance to be measured fi<CX. Capacitance to be measured CX
As shown in FIG. 1, the capacitances CA, CB, and CW are measured and the pulse count values NA, NB, and NW of the counter 14 are obtained as those corresponding to the capacitances CA, CB, and CW. 1) Corresponding to equation LS-(NW-NA4-
NB)・LT/NW ・・・・・・Distance LS to the disconnection point can be calculated.
捷だパルス数NW、NA、NBを計測する代りに。Instead of measuring the number of pulses NW, NA, and NB.
各静電容量接続時における第6図(a)のtoからtc
lでの時間LW、tA、tBを計測し。From to to tc in Figure 6(a) when each capacitance is connected
Measure the times LW, tA, and tB at l.
LS、−(tW−LA+tB)・LT/lW ・・・・
・・0の式より、断線箇所までの距離LSを算出しても
」:い、上記02式は各静電容量をパルヌ数に換算して
、θ1式は時間に換算してそれぞれ距離LSをめるよう
にしたものである。LS, -(tW-LA+tB)・LT/lW...
... Even if you calculate the distance LS to the disconnection point from the formula 0, the above formula 02 converts each capacitance to Pärnu number, and the θ1 formula converts the distance LS to time. It was designed to make it easier to read.
なお、未知静電容量の測定については第2図に示すよう
に未知静電容量への充電とその充電電荷の抵抗を通じて
の放電特性を利用する場合について説明したが、この発
明においては未知静電容量の測定は他の測定原理のもの
を用いてもよい。Regarding the measurement of unknown capacitance, as shown in FIG. Other measurement principles may be used to measure the capacitance.
また上記実施例では、1列の芯線とシールド導体を有す
るケーブルの断線箇所までの距離測定方法について説明
しだが、シールド導体を持たないケーブルであっても、
1対の芯線とコンジット導体管あるいは大地間等との静
電容量を測定することにより、同様に断線箇所までの距
離を測定することができる。In addition, in the above embodiment, a method for measuring the distance to the disconnection point of a cable having one row of core wires and a shield conductor was explained, but even if the cable does not have a shield conductor,
By measuring the capacitance between a pair of core wires and a conduit conductor pipe or the ground, the distance to the disconnection point can be similarly measured.
(へ)効果
この発明によれば、ケーブルの2芯線の各々の一端の静
電容量及び両芯線を一括した場合の一端の静電容量を測
定するのみであるから容易に断線箇所までの距離を測定
することができる。しかも静電容量の測定は比較的正確
に行なえるので、断線箇所までの距離測定も精度良く行
なうことができる。(F) Effect According to the present invention, since only the capacitance at one end of each of the two core wires of the cable and the capacitance at one end when both core wires are bundled are measured, the distance to the disconnection point can be easily determined. can be measured. Moreover, since the capacitance can be measured relatively accurately, the distance to the disconnection point can also be measured with high accuracy.
第1図は、この発明の一実施例を示す概略図。
第2図は同実施例に使用される容量測定演算器の−・例
を示すブロック図、第6図は同容量測定演算器の動作を
説明するだめの信号タイムチャートである1、
1 : ケーフ゛ル、 2 ・ 3 : 芯線、 4
: シールド導体、5:容量測定演算器。
特許出願人 株式会社島津製作所
代理人 弁理士 中 村 茂 信
第1図
第3図
(d) VcFIG. 1 is a schematic diagram showing an embodiment of the present invention. FIG. 2 is a block diagram showing an example of the capacitance measurement calculator used in the same embodiment, and FIG. 6 is a signal time chart for explaining the operation of the capacitance measurement calculator. , 2 ・3: Core wire, 4
: Shield conductor, 5: Capacitance measurement calculator. Patent applicant Shimadzu Corporation Representative Patent attorney Shigeru Nakamura Figure 1 Figure 3 (d) Vc
Claims (1)
所までの距離測定方法であって。 AiJ記対線対線方端末を短絡状態とし、前記対線の各
々と他の同一対象物体間の静電容量CA。 CBと、前記列線双方を一括したものと前記同一対象物
体間の静電容量CWをそれぞれ計測し。 これら計測しだCA、CB、CWと既知のケーブルの全
長LTとにより、LS =(CW十CB−CA)・LT
/CWの演算をなすことによシ断線箇所までの距離L
Sを算出するようにした断線箇所までの距離測定方法。 (2+ mJ記同一対象物体はケーブルのシールド導体
であることを特徴とする特許請求の範囲第1項記載の断
線箇所までの距離測定方法。(1) A method for measuring the distance to a break point in a cable consisting of a pair of wires covered with an outer sheath. AiJ is the capacitance CA between each pair of wires and another identical target object when the terminals of the pair of wires are short-circuited. CB, the capacitance CW of both the column lines collectively, and the capacitance CW between the same target object were measured. Using these measurements CA, CB, CW and the known total length LT of the cable, LS = (CW + CB - CA) · LT
By calculating /CW, the distance L to the disconnection point can be calculated.
A distance measurement method to a disconnection point that calculates S. (2+ mJ) A distance measuring method to a disconnection point according to claim 1, wherein the same target object is a shield conductor of a cable.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP11447683A JPS604802A (en) | 1983-06-23 | 1983-06-23 | How to measure the distance to the disconnection point |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP11447683A JPS604802A (en) | 1983-06-23 | 1983-06-23 | How to measure the distance to the disconnection point |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS604802A true JPS604802A (en) | 1985-01-11 |
| JPH0434702B2 JPH0434702B2 (en) | 1992-06-08 |
Family
ID=14638688
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP11447683A Granted JPS604802A (en) | 1983-06-23 | 1983-06-23 | How to measure the distance to the disconnection point |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS604802A (en) |
Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| DE3610646A1 (en) * | 1985-03-28 | 1986-11-06 | Roman Koller | System for measuring the length of resistor ladders |
| US5639390A (en) * | 1993-12-24 | 1997-06-17 | Tokyo Electron Limited | Conductor pattern check apparatus for locating and repairing open circuits |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN102353320A (en) * | 2011-07-06 | 2012-02-15 | 宝钢发展有限公司 | Temperature sensing cable ranging method and range finder |
-
1983
- 1983-06-23 JP JP11447683A patent/JPS604802A/en active Granted
Cited By (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| DE3610646A1 (en) * | 1985-03-28 | 1986-11-06 | Roman Koller | System for measuring the length of resistor ladders |
| US5639390A (en) * | 1993-12-24 | 1997-06-17 | Tokyo Electron Limited | Conductor pattern check apparatus for locating and repairing open circuits |
| US5844199A (en) * | 1993-12-24 | 1998-12-01 | Tokyo Electron Ltd | Conductor pattern check apparatus for locating and repairing short and open circuits |
Also Published As
| Publication number | Publication date |
|---|---|
| JPH0434702B2 (en) | 1992-06-08 |
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