JPH0249472B2 - - Google Patents
Info
- Publication number
- JPH0249472B2 JPH0249472B2 JP57092290A JP9229082A JPH0249472B2 JP H0249472 B2 JPH0249472 B2 JP H0249472B2 JP 57092290 A JP57092290 A JP 57092290A JP 9229082 A JP9229082 A JP 9229082A JP H0249472 B2 JPH0249472 B2 JP H0249472B2
- Authority
- JP
- Japan
- Prior art keywords
- phase
- measurement signal
- electric field
- voltage
- distribution line
- 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
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Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01R—MEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
- G01R29/00—Arrangements for measuring or indicating electric quantities not covered by groups G01R19/00 - G01R27/00
- G01R29/18—Indicating phase sequence; Indicating synchronism
Landscapes
- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Testing Of Short-Circuits, Discontinuities, Leakage, Or Incorrect Line Connections (AREA)
Description
【発明の詳細な説明】
本発明は、配電線のある区間の両端の相が一致
していることを活線状態で判別することのできる
相判別装置に関する。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a phase determination device that can determine whether phases at both ends of a certain section of a distribution line match in a live line state.
従来、配電線区間の両端で、色別表示された各
相は、端子ごとに、その端子における位相順(あ
るいは相回転)により決められており、一端側
(送信側)における色別表示すなわち黒相、赤相、
白相は他端側(受信側)における色別表示すなわ
ち黒相、赤相、白相とは相順については一致して
いるが、一端側の黒相と他端側の黒相、一端側の
赤相と他端側の赤相、一端側の白相と他端側の白
相とは必らずしも一致していない場合があつた。
しかし、配電線運用上、一端側における色別表示
つまり黒相、赤相、白相に一致して他端側の色別
表示を決定したい場合があり、それために相判別
装置が必要となる。 Conventionally, each phase, which is displayed in different colors at both ends of a distribution line section, is determined by the phase order (or phase rotation) at that terminal for each terminal. phase, red phase,
The white phase corresponds to the color-coded display on the other end (receiving side), that is, black phase, red phase, and white phase, but the black phase on one end side, the black phase on the other end side, and the red phase on one end side match. There were cases in which the phase and the red phase on the other end side did not necessarily match, and the white phase on one end side and the white phase on the other end side did not necessarily match.
However, when operating a power distribution line, there are cases where it is desired to determine the color-coded display at the other end in accordance with the color-coded display at one end, that is, the black, red, and white phases, and a phase discrimination device is required for this purpose.
従来、この種の相判別装置は、第1図に示すよ
うに、配電線に電圧を印加しない状態(死線時)
で、たとえば他端側(受信側)に異なる抵抗値の
抵抗R1,R2,R3を各相に挿入し、一端側(送信
側)で各相の抵抗値を抵抗計Rによつて測定する
ことにより、その両端の相の抵抗値が一致してい
る相を検出して相判別を行なつていた。 Conventionally, this type of phase discrimination device has been used when no voltage is applied to the distribution line (dead line), as shown in Figure 1.
For example, insert resistors R 1 , R 2 , and R 3 with different resistance values into each phase at the other end (receiving side), and measure the resistance value of each phase with a resistance meter R at one end (transmitting side). By measuring, a phase in which the resistance values of the phases at both ends are the same is detected and phase discrimination is performed.
しかしながら、このような相判別装置は、相判
定を行なうために、一旦、送電線を停止する必要
があり、かつ両端間で抵抗値確認のための情報交
換が必要となり、繁雑であつた。また、相判別を
行なうためには配電線の被覆をはがして抵抗R1,
R2,R3を接続し、また接地もとらなければなら
ないため作業に手間がかかつた。 However, such a phase determination device is complicated because it requires the power transmission line to be temporarily stopped in order to perform phase determination, and it also requires information exchange between both ends to confirm the resistance value. In addition, in order to perform phase discrimination, the coating of the distribution line is removed and the resistance R 1 ,
The work was time-consuming because R 2 and R 3 had to be connected and grounding had to be established as well.
本発明は上記に鑑み、配電線を活線のままで、
かつ相判別を行なう一方の端側の情報のみで相判
別が可能であり、さらに判別に際して他端側(受
信側)で手間のかかる作業を必要としない相判別
装置を提供することを目的とする。 In view of the above, the present invention has been developed to keep the distribution line live,
It is an object of the present invention to provide a phase discrimination device which is capable of phase discrimination using only information on one end of the phase discrimination, and does not require time-consuming work on the other end (receiving side) for discrimination. .
次に本発明の実施例を図面に基づいて詳細に説
明する。 Next, embodiments of the present invention will be described in detail based on the drawings.
第2図には配電線のある区間A−B間において
A地点の(送信側)黒相、赤相、白相がB地点
(受信側)のどの相と一致しているかを判別する
場合の実施例が示されている。この第2図におい
て、1は特定の相電圧(たとえば黒相電圧)をと
り出す電圧変成器である。電圧変成器1の出力a
(第3図参照)は、波形整形回路2に与えられ、
短形波に整形される。波形整形回路2の出力bお
よび測定用信号発生器3の出力cは同期回路4に
与えられ、測定用信号dは波形整形回路2の出力
の相電圧の特定位相(例えば0゜)に同期して出力
される。同期回路4の出力dは信号結合器5に与
えられ、相電圧(黒相電圧)に重畳される。測定
用信号dの重畳している黒相電圧は第3図におい
て波形図eで示されている。従つて、電圧変成器
1、波形整形回路2、測定用信号発生器3、同期
回路4および信号結合器5によつて、測定用信号
発生装置が構成される。 Figure 2 shows how to determine which phase of the black, red, and white phases at point A (on the transmitting side) match the phases at point B (on the receiving side) between A and B in a certain section of the distribution line. An example is shown. In FIG. 2, reference numeral 1 denotes a voltage transformer that takes out a specific phase voltage (eg, black phase voltage). Output a of voltage transformer 1
(see FIG. 3) is given to the waveform shaping circuit 2,
Shaped into a rectangular wave. The output b of the waveform shaping circuit 2 and the output c of the measurement signal generator 3 are given to a synchronization circuit 4, and the measurement signal d is synchronized with a specific phase (for example, 0°) of the phase voltage of the output of the waveform shaping circuit 2. is output. The output d of the synchronous circuit 4 is given to the signal combiner 5 and superimposed on the phase voltage (black phase voltage). The black phase voltage on which the measurement signal d is superimposed is shown by a waveform diagram e in FIG. Therefore, the voltage transformer 1, the waveform shaping circuit 2, the measurement signal generator 3, the synchronization circuit 4, and the signal combiner 5 constitute a measurement signal generation device.
相判別を行なうB地点(受信側)においては、
以下に説明する電界センサ6、信号電圧分離回路
7、波形整形回路8、および相判別回路9からな
る測定用信号検生装置が設けられている。電界セ
ンサ6は、1つの検出部を有し、この検出部を各
相の電界中に順次設置することにより各相毎に順
次測定を行なうようにし、電界の位相に応じた検
出信号を出力する。 At point B (receiving side) where phase discrimination is performed,
A measurement signal detection device is provided which includes an electric field sensor 6, a signal voltage separation circuit 7, a waveform shaping circuit 8, and a phase discrimination circuit 9, which will be described below. The electric field sensor 6 has one detection section, and by sequentially installing this detection section in the electric field of each phase, it sequentially measures each phase, and outputs a detection signal according to the phase of the electric field. .
電界センサ6の構成および原理を第4図ないし
第7図に基づいて説明する。第4図は電界センサ
6の原理説明図であり、図において電界Eはポツ
ケルス効果を有する電気光学結晶10に加えられ
る。電気光学結晶10は例えばLiNbo3が用いら
れる。入射光は偏光子11を通して直線偏光とさ
れたのち電気光学結晶10に加えられる。この直
線偏光が電気光学結晶10に入射されると、この
振動方向の光は存在できず、互いに直角な2つの
光波にわかれる。一方の光波は電気光学結晶10
に電界が印加されると速度が速くなり(速波
L1)、他方の光波は速度が遅くなる(遅波L2)。
このため、結晶10の出射面から光が出射する
時、振動が鉛直方向の光と水平方向の光は位相差
Γを生ずる。よつて出射光の合成ベクトル図は第
5図に示すように位相差Γに応じて楕円、円ある
いは直線となる。第5図においてイはΓ=0、ロ
は0<Γ<π/2、ハはΓ=π/2、ニはπ/2<Γ<
π、
ホはΓ=πのときの状態を示している。この位相
差Γは次式にて表わされる。 The structure and principle of the electric field sensor 6 will be explained based on FIGS. 4 to 7. FIG. 4 is a diagram explaining the principle of the electric field sensor 6, in which an electric field E is applied to an electro-optic crystal 10 having a Pockels effect. For example, LiNbo 3 is used as the electro-optic crystal 10. The incident light is linearly polarized through a polarizer 11 and then applied to an electro-optic crystal 10 . When this linearly polarized light is incident on the electro-optic crystal 10, light in this vibration direction cannot exist, and it is split into two light waves that are perpendicular to each other. One light wave is an electro-optic crystal 10
When an electric field is applied to
L 1 ), the other light wave becomes slower (slow wave L 2 ).
Therefore, when light is emitted from the output surface of the crystal 10, a phase difference Γ occurs between the light whose vibration is in the vertical direction and the light whose vibration is in the horizontal direction. Therefore, the composite vector diagram of the emitted light becomes an ellipse, a circle, or a straight line depending on the phase difference Γ, as shown in FIG. In Figure 5, A is Γ=0, B is 0<Γ<π/2, C is Γ=π/2, and D is π/2<Γ<
π and ho indicate the state when Γ=π. This phase difference Γ is expressed by the following equation.
Γ=hlv/d ……(1)
但し(1)式においてhは比例定数、lは結晶10
中の光路長、dは結晶10の厚さ、vは結晶に印
加される電圧を示している。(1)式からも明らかな
ように位相差Γは結晶に印加される電圧V、すな
わちE(=v/d)に比例する。この現象はポツ
ケルス効果あるいは一次電気光学効果として良く
知られている。電気光学結晶10からの出射光は
1/4波長板12を通して位相差ΓR=π/2を加
え、次に検光子13を通して斜め方向(水平方向
に対し45゜の方向)の成分だけを選び出す。この
選び出された光強度Iは、
I=sin2(Γ/2+π/4) ……(2)
となり、位相差Γは電気光学結晶10に印加され
る電圧Vに比例するので、光強度Iと電圧Vは第
6図に示すような変化を示す。そのため、電圧V
がV=V0sin wtで与えられると光強度Iは第7
図に示すように電圧Vで変調され、Voが小さい
場合は光強度Iも正弦波であると近似できる。し
たがつて検光子13により選び出された光を電気
信号に変換することにより電圧を検出することが
できる。 Γ=hlv/d...(1) However, in equation (1), h is the proportionality constant and l is the crystal 10
d is the thickness of the crystal 10, and v is the voltage applied to the crystal. As is clear from equation (1), the phase difference Γ is proportional to the voltage V applied to the crystal, that is, E (=v/d). This phenomenon is well known as the Pockels effect or first-order electro-optic effect. The light emitted from the electro-optic crystal 10 is passed through a quarter-wave plate 12 to which a phase difference Γ R =π/2 is added, and then passed through an analyzer 13 to select only the components in the oblique direction (45° to the horizontal direction). . This selected light intensity I is I=sin 2 (Γ/2+π/4) ...(2), and since the phase difference Γ is proportional to the voltage V applied to the electro-optic crystal 10, the light intensity I and the voltage V show changes as shown in FIG. Therefore, the voltage V
is given by V=V0sin wt, the light intensity I is the 7th
As shown in the figure, when the light is modulated by the voltage V and Vo is small, the light intensity I can also be approximated as a sine wave. Therefore, the voltage can be detected by converting the light selected by the analyzer 13 into an electrical signal.
第8図は前述のような電気光学結晶を用いた電
界センサ6の構成図を示すものであり、第4図に
示すような電気光学結晶10、偏光子11、波長
板12、検光子13からなる検出部14と、光フ
アイバ15,16、電気一光変換器17、光一電
気変換器18から構成されている。検出部14は
配電線の周囲の電界の影響を受ける位置に設けら
れ、また光一電気変換器18の出力は増巾等の信
号処理をされたのち第2図に示す信号電圧分離回
路7に入力される。 FIG. 8 shows a configuration diagram of an electric field sensor 6 using an electro-optic crystal as described above, and includes an electro-optic crystal 10, a polarizer 11, a wavelength plate 12, an analyzer 13 as shown in FIG. It consists of a detection unit 14, optical fibers 15 and 16, an electrical-to-optical converter 17, and an optical-to-electrical converter 18. The detection unit 14 is installed at a position that is affected by the electric field around the distribution line, and the output of the Koichi electric converter 18 is subjected to signal processing such as amplification and then input to the signal voltage separation circuit 7 shown in FIG. be done.
第2図に示す測定用信号発生装置の動作を第9
図に示す波形図に基づいて説明する。第9図に示
すように各相電圧U1、V1、W1には測定用信号d
が重畳されている。なお、A地点(送信側)では
黒相電圧一相にしか測定用信号dを重畳させてい
ないにもかかわらず、B地点(受信側)では3つ
の相電圧U1、V1、W1に測定用信号dが重畳され
た形になつているが、これは、主として配電用変
圧器を通した電源側における回り込み現象のため
である。この測定用信号dは黒相、赤相、白相の
3相すべてに重畳するようにしても良いことは勿
論である。 The operation of the measurement signal generator shown in FIG.
The explanation will be based on the waveform diagram shown in the figure. As shown in Fig. 9, each phase voltage U 1 , V 1 , W 1 has a measurement signal d.
are superimposed. Note that although the measurement signal d is superimposed on only one phase of the black phase voltage at point A (transmission side), three phase voltages U 1 , V 1 , and W 1 are superimposed at point B (reception side). The measurement signal d is superimposed, but this is mainly due to a wrap-around phenomenon on the power supply side through the distribution transformer. Of course, this measurement signal d may be superimposed on all three phases: black phase, red phase, and white phase.
電界センサ6は設置された相の相電圧による電
界により変調された光を電気信号に変換して出力
する。この電界センサ6の出力は信号電圧分離回
路7に与えられる。この信号電圧分離回路7は測
定用信号を抽出するためのフイルタを有してお
り、測定用信号X1と相電圧による信号X2を出力
する。この信号X2は電界センサ6がどの相に設
置されるかによつて位相が120゜ずつ異なつてい
る。この信号X1とX2は波形整形回路8に加えら
れる。波形整形回路8は、例えば信号X2の波形
が0゜を横切る時点でそれぞれ出力パルスを発生
し、例えば120゜経過後そのパルスを終了させる単
定定マルチバイブレータからなる。この単安定マ
ルチバイブレータの出力信号X3は電界センサ6
が設置される相に対応して第9図の信号U2、V2、
W2のようになる。測定用信号X2の取出しも別の
単安定マルチバイブレータによつて行なわれ、第
9図の信号X3を出力する波形整形回路8の出力
信号X3とX4は相判別回路9に与えられる。この
相判別回路9は、例えば、信号X3とX4を入力と
するAND回路からなる。第9図から理解できる
ように電界センサ6がU相に設置された場合には
このAND回路から出力信号が出される。従つて、
このU相がA地点(送信側)における黒相に対応
していることが判る。この相判別回路9では、測
定用信号とB地点の各相電圧の同期を検出してお
り、測定用信号と同期した相がA地点の特定の相
と一致していることになる。 The electric field sensor 6 converts light modulated by an electric field caused by the phase voltage of the installed phase into an electric signal and outputs the electric signal. The output of this electric field sensor 6 is given to a signal voltage separation circuit 7. This signal voltage separation circuit 7 has a filter for extracting a measurement signal, and outputs a measurement signal X 1 and a signal X 2 based on the phase voltage. The phase of this signal X 2 differs by 120° depending on which phase the electric field sensor 6 is installed. These signals X 1 and X 2 are applied to the waveform shaping circuit 8. The waveform shaping circuit 8 is composed of a single constant multivibrator that generates an output pulse each time the waveform of the signal X 2 crosses 0°, for example, and terminates the pulse after 120° has passed, for example. The output signal X 3 of this monostable multivibrator is the electric field sensor 6
The signals U 2 , V 2 , and
It will look like W 2 . The measurement signal X 2 is also taken out by another monostable multivibrator, and the output signals X 3 and X 4 of the waveform shaping circuit 8 which outputs the signal X 3 shown in FIG. 9 are given to the phase discrimination circuit 9. . This phase discrimination circuit 9 is composed of, for example, an AND circuit that receives signals X 3 and X 4 as inputs. As can be understood from FIG. 9, when the electric field sensor 6 is installed in the U phase, an output signal is output from this AND circuit. Therefore,
It can be seen that this U phase corresponds to the black phase at point A (transmission side). This phase determination circuit 9 detects synchronization between the measurement signal and each phase voltage at point B, and the phase synchronized with the measurement signal matches the specific phase at point A.
一方、B地点の相回転方向は公知の手段で判別
できるので、B地点の他の2つの相判別は容易に
できる。 On the other hand, since the phase rotation direction at point B can be determined by known means, the other two phases at point B can be easily determined.
なお、相回転が未知の場合には、B地点で測定
用信号X3を120゜毎回転させて(つまり、遅延素子
により120゜遅らせて)、それぞれその信号X3と同
期した相電圧を検出することにより他の2つの相
の相判別ができる。つまり、測定用信号X3を120゜
遅らせると、これは信号V2と同期し、さらに120゜
遅らせるとW2と同期することになる。 If the phase rotation is unknown, rotate the measurement signal X 3 every 120 degrees at point B (that is, delay it by 120 degrees with a delay element), and detect the phase voltages that are synchronized with each signal X 3 . By doing so, it is possible to distinguish between the other two phases. That is, if the measurement signal X 3 is delayed by 120°, it will be synchronized with the signal V 2 , and if it is delayed by a further 120°, it will be synchronized with W 2 .
配電線に重畳されている信号を検出する方式と
しては従来、配電線の被覆の上に電極をあて、そ
の間の静電容量を使用した分圧器が用いられてい
るが、この方式では気象条件等により分圧器の位
相の変化が生じるため、相判別に適用しようとす
ると正確な相電圧波形の検出が困難であるばかり
でなく、必らずアースをとる必要があり、作業が
煩雑となる。これに対して、本発明は配電線の周
囲あるいは周囲空間に形成された電界中に電気光
学結晶からなる検出部を設置して電界に基づいて
相電圧波形を検出するようにしたものである。電
界強度は場所によつて変化するが、電界の位相は
場所に依存せず、配電線の電圧の位相と一致す
る。よつて電気光学結晶からなる検出部の設置場
所にかかわりなく、正確な位相の相電圧波形の検
出が可能となる。また、検出部を配電線の周囲あ
るいは周囲空間の電界中に設置するのみで相電圧
波形の検出が可能であるため、検出部の設置や接
地の手間が省ける。さらに、検出部と配電線は非
接触でも良いこと、光信号の伝送に絶縁性の高い
光フアイバを用いていること等のため、感電の恐
れの少ない高電気絶縁性の検出が可能である。そ
して、配電線区間の両端の情報交換を行なわず、
かつ活線のままで、一端側の相に一致した相を他
端側において判別することが可能となる。 The conventional method for detecting signals superimposed on distribution lines is to use a voltage divider that places electrodes on the coating of the distribution line and uses the capacitance between them. This causes a change in the phase of the voltage divider, so when applied to phase discrimination, it is not only difficult to accurately detect the phase voltage waveform, but also requires grounding, which complicates the work. In contrast, in the present invention, a detection section made of an electro-optic crystal is installed in an electric field formed around the distribution line or in the surrounding space, and the phase voltage waveform is detected based on the electric field. Although the electric field strength varies depending on location, the phase of the electric field is independent of location and matches the phase of the voltage on the distribution line. Therefore, it is possible to detect a phase voltage waveform with an accurate phase regardless of the installation location of the detection section made of an electro-optic crystal. Furthermore, since phase voltage waveforms can be detected simply by installing the detection section around the distribution line or in the electric field in the surrounding space, the effort of installing and grounding the detection section can be saved. Furthermore, since the detection unit and the power distribution line may be in non-contact, and a highly insulating optical fiber is used for optical signal transmission, detection with high electrical insulation is possible with less risk of electric shock. Then, information is not exchanged between both ends of the distribution line section,
In addition, it is possible to determine the phase matching the phase at one end at the other end while the wire remains live.
第1図は従来の相判別装置のブロツク図、第2
図は本発明による相判別装置の一例を示すブロツ
ク図、第3図および第9図はそれぞれ第2図にお
ける各構成要素の一部の出力波形を示す波形図、
第4図は電気光学結晶の原理説明図、第5図は電
気光学結晶からの出射光の合成ベクトル図、第6
図は光強度Iと電圧Vとの関係図、第7図は光強
度Iの変調を説明するための図、第8図は電界セ
ンサの構成を示すブロツク図である。
1……電圧変成器、2……波形整形回路、3…
…測定用信号発生器、4……同期回路、5……信
号結合器、6……電界センサ、7……信号電圧分
離回路、8……波形整形回路、9……相判別回
路、10……電気光学結晶、11……偏光子、1
2……波長板、13……検光子、14……検出
部、15,16……光フアイバ、17……電気一
光変換器、18……光一電気変換器。
Figure 1 is a block diagram of a conventional phase discrimination device, Figure 2 is a block diagram of a conventional phase discrimination device.
The figure is a block diagram showing an example of the phase discrimination device according to the present invention, and FIGS. 3 and 9 are waveform diagrams showing the output waveforms of some of the components in FIG. 2, respectively.
Figure 4 is a diagram explaining the principle of electro-optic crystal, Figure 5 is a composite vector diagram of the light emitted from the electro-optic crystal, and Figure 6 is a diagram explaining the principle of electro-optic crystal.
7 is a diagram for explaining the modulation of the light intensity I, and FIG. 8 is a block diagram showing the configuration of the electric field sensor. 1... Voltage transformer, 2... Waveform shaping circuit, 3...
...Measurement signal generator, 4...Synchronization circuit, 5...Signal coupler, 6...Electric field sensor, 7...Signal voltage separation circuit, 8...Waveform shaping circuit, 9...Phase discrimination circuit, 10... ...Electro-optic crystal, 11...Polarizer, 1
2... Wave plate, 13... Analyzer, 14... Detection section, 15, 16... Optical fiber, 17... Electric-to-optical converter, 18... Optical-to-electrical converter.
Claims (1)
その一端側のある特定相の相電圧に同期して、特
定周波数の測定用信号を配電線に重畳させる測定
用信号発生装置と、他端側(受信側)の配電線の
周囲あるいは周囲空間に形成された電界中に設置
されたポツケルス効果を有する電気光学結晶から
なる検出部と、該検出部を通過して前記電界によ
り変調された光信号より前記測定用信号および相
電圧波形を検出する検出手段と、該検出手段の検
出結果に基づいて前記一端側のある特定相に対応
する前記他端側の相を判別する判別手段からなる
ことを特徴とする相判別装置。1 Installed at one end (transmission side) of the distribution line section,
A measurement signal generator that superimposes a measurement signal of a specific frequency on the distribution line in synchronization with the phase voltage of a specific phase on one end, and a measurement signal generator that superimposes a measurement signal of a specific frequency on the distribution line on the other end (receiving side) or in the surrounding space. a detection section made of an electro-optic crystal having a Pockels effect installed in the formed electric field; and detection for detecting the measurement signal and the phase voltage waveform from an optical signal that passes through the detection section and is modulated by the electric field. and a determining means for determining a phase on the other end side that corresponds to a certain specific phase on the one end side based on the detection result of the detecting means.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP57092290A JPS58208672A (en) | 1982-05-31 | 1982-05-31 | Phase discriminator |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP57092290A JPS58208672A (en) | 1982-05-31 | 1982-05-31 | Phase discriminator |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS58208672A JPS58208672A (en) | 1983-12-05 |
| JPH0249472B2 true JPH0249472B2 (en) | 1990-10-30 |
Family
ID=14050274
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP57092290A Granted JPS58208672A (en) | 1982-05-31 | 1982-05-31 | Phase discriminator |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS58208672A (en) |
Families Citing this family (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH068833B2 (en) * | 1985-03-06 | 1994-02-02 | エナジーサポート株式会社 | Fault current detection display device |
| JPS62180289A (en) * | 1986-02-04 | 1987-08-07 | Taihei Dengiyou Kk | Cable route surveying method |
| FR2664059B1 (en) * | 1990-06-28 | 1992-09-25 | Electricite De France | DEVICE FOR TRACKING THE PHASES OF A LOW-VOLTAGE POLYPHASE ELECTRICITY DISTRIBUTION NETWORK. |
| US20110285382A1 (en) * | 2010-05-18 | 2011-11-24 | General Electric Company | Power meter phase identification |
-
1982
- 1982-05-31 JP JP57092290A patent/JPS58208672A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS58208672A (en) | 1983-12-05 |
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