JPH09243686A - Method for measuring ground impedance - Google Patents

Method for measuring ground impedance

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Publication number
JPH09243686A
JPH09243686A JP7928996A JP7928996A JPH09243686A JP H09243686 A JPH09243686 A JP H09243686A JP 7928996 A JP7928996 A JP 7928996A JP 7928996 A JP7928996 A JP 7928996A JP H09243686 A JPH09243686 A JP H09243686A
Authority
JP
Japan
Prior art keywords
ground
voltage
impedance
integration unit
grounding
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.)
Withdrawn
Application number
JP7928996A
Other languages
Japanese (ja)
Inventor
Kazuhiko Akiyama
和彦 秋山
Kazuo Hamasato
和雄 浜里
Akira Ishizawa
昭 石沢
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.)
Nippon Telegraph and Telephone Corp
Original Assignee
Nippon Telegraph and Telephone Corp
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 Nippon Telegraph and Telephone Corp filed Critical Nippon Telegraph and Telephone Corp
Priority to JP7928996A priority Critical patent/JPH09243686A/en
Publication of JPH09243686A publication Critical patent/JPH09243686A/en
Withdrawn legal-status Critical Current

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Abstract

PROBLEM TO BE SOLVED: To facilitate measurement of ground impedance by obtaining impedance associated with ground such as impedance of a ground-concerned part, ground impedance, and impedance between devices as a matrix. SOLUTION: An admittance matrix from respective admittance when only voltage Va is applied from a voltage source Sa and only voltage Vb is applied from a voltage source Vb , and this is converted into an impedance matrix [Z]. [Z] indicates entire impedance viewed from a ground integration part C. With only the voltage Va or voltage Vb applied, ground impedance Rc is obtained from voltage Vo to an auxiliary electrode Paux and current Ic flowing in the ground integration part C. If respective impedance matrixes for a circuit network Z1 including devices A, B having the integration ground part C as a common return and a circuit network Z2 including only the ground impedance Rc are [Z1], [Z2] respectively, [Z1] can be obtained as a matrix with Rc subtracted from respective components of [Z1].

Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【発明の属する技術分野】本発明は、個々に接地された
N(≧2)個の装置と、該N個の装置の接地を共通に行
なう接地統合部とからなる接地システムにおいて、補助
接地を設けて接地インピーダンスを測定する方法に関す
るものである。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a grounding system comprising N (≧ 2) devices which are individually grounded, and a grounding integrated part which grounds the N devices in common. The present invention relates to a method for providing and measuring ground impedance.

【0002】[0002]

【従来の技術】接地インピーダンスの測定には、従来か
ら、電流印加補助電極と電圧測定補助電極を用いるいわ
ゆる3端子法が使用されている。図7はこの従来技術を
説明するための図であり、Pは接地インピーダンスを測
定すべき被測定接地電極、Piは電流印加用補助電極、
Pvは電圧測定用補助電極、Sは交流の測定用電圧源、
Iは電流測定器、Vは電圧測定器である。また、Rpは
被測定接地電極Pの接地インピーダンス、Rvは電圧測
定用補助電極Pvの接地インピーダンス、Riは電流印
加用補助電極Piの接地インピーダンスである。
2. Description of the Related Art Conventionally, a so-called three-terminal method using a current application auxiliary electrode and a voltage measurement auxiliary electrode has been used for measuring ground impedance. FIG. 7 is a diagram for explaining this conventional technique, where P is a ground electrode to be measured whose ground impedance is to be measured, Pi is an auxiliary electrode for applying current,
Pv is an auxiliary electrode for voltage measurement, S is an alternating voltage source for measurement,
I is a current measuring device and V is a voltage measuring device. Further, Rp is the ground impedance of the measured ground electrode P, Rv is the ground impedance of the voltage measurement auxiliary electrode Pv, and Ri is the ground impedance of the current application auxiliary electrode Pi.

【0003】接地インピーダンスRpの測定にあたって
は、測定用電圧源Sを被測定接地電極Pと電流印加用補
助電極Piとの間に接続して電流iを流し、被測定接地
電極Pの電圧Vpを、電圧測定用補助電極Pvを基準に
電圧測定器Vで測定する。つまり電極Pと電極Pvとの
間の電圧Vpを電圧測定器Vで測定する。このとき、電
圧測定器Vの内部抵抗が大きいので、電極Pvには電流
が流れず、したがって電極Pvの接地インピーダンスR
vによる電圧降下は発生せず、前記測定された電圧Vp
は接地インピーダンスRpによる電圧降下となる。よっ
て、接地インピーダンスRpは、Rp=Vp/iにより
求められる。
In measuring the ground impedance Rp, a voltage source S for measurement is connected between the ground electrode P to be measured and an auxiliary electrode Pi for current application to pass a current i, and the voltage Vp of the ground electrode P to be measured is set. , The voltage measuring auxiliary electrode Pv is used as a reference to measure with a voltage measuring device V. That is, the voltage Vp between the electrode P and the electrode Pv is measured by the voltage measuring device V. At this time, since the internal resistance of the voltage measuring device V is large, no current flows through the electrode Pv, and therefore the ground impedance R of the electrode Pv is reduced.
There is no voltage drop due to v, and the measured voltage Vp
Is a voltage drop due to the ground impedance Rp. Therefore, the ground impedance Rp is obtained by Rp = Vp / i.

【0004】図6は複数の接地を有するシステムを示し
たものであり、A、Bは個別に接地インピーダンスR
a、Rbの接地電極で接地された装置、Cはその装置
A、Bの接地を接地インピーダンスRcの接地電極で共
通に接地する接地統合部である。ここでは、接地統合部
Cの接地インピーダンスRcは所定の基準に沿った接地
により所定の値に設定されているが、装置A、Bの個々
の接地電極の接地インピーダンスRa、Rbは不明な場
合がある。
FIG. 6 shows a system having a plurality of grounds, where A and B are grounding impedances R individually.
A device grounded by the ground electrodes of a and Rb, and C is a ground integration unit that grounds the devices A and B in common by the ground electrodes of the ground impedance Rc. Here, the ground impedance Rc of the ground integration unit C is set to a predetermined value by grounding along a predetermined reference, but the ground impedances Ra and Rb of the individual ground electrodes of the devices A and B may be unknown. is there.

【0005】[0005]

【発明が解決しようとする課題】しかし、従来の接地イ
ンピーダンスの測定方法では、接地インピーダンスR
a、Rbを知るためには接地を切り離して測定する必要
があり、またその接地インピーダンスRa、Rbおよび
装置A、B間の相互インピーダンスRabを含む接地シ
ステムの接地インピーダンスを測定することはできなか
った。
However, in the conventional ground impedance measuring method, the ground impedance R
In order to know a and Rb, it is necessary to measure the ground separately, and it has not been possible to measure the ground impedance of the ground system including the ground impedances Ra and Rb and the mutual impedance Rab between the devices A and B. .

【0006】本発明の目的は、個々に接地されたN個の
装置と該複数の装置の接地を共通に行なう接地統合部と
からなる接地システムにおいて、接地統合部を除く他の
接地インピーダンスをマトリクスとして測定することが
でき、またそのとき各接地を切り離すことなく接地イン
ピーダンスを測定することができるようにした接地イン
ピーダンスの測定方法を提供せんとするものである。
An object of the present invention is to provide a grounding system comprising N individually grounded devices and a grounding integration part for common grounding of the plurality of devices, and to matrix the grounding impedances other than the grounding integration part. It is intended to provide a method for measuring the ground impedance, which enables the measurement of the ground impedance without disconnecting each ground at that time.

【0007】[0007]

【課題を解決するための手段】第1の発明は、個々に接
地されたN(≧2)個の装置と、該N個の装置の接地を
共通に行なう接地統合部とからなる接地システムにおい
て、補助接地を設け、前記N個の接地の内の1つの接地
に電圧を印加して前記N個の接地に流れる電流を各々測
定してアドミッタンスを得、このアドミッタンス測定を
前記N個の接地の残りの接地の各々に電圧を印加し行な
ってアドミッタンスマトリクスを得、該アドミッタンス
マトリクスから前記N個の接地、前記接地統合部の接
地、および前記複数の装置を含む全体のインピーダンス
マトリクスを得ること、前記N個の接地のいずれか1つ
に電圧を印加して、前記接地統合部の接地に流れる電流
と、前記補助電極を基準として測定した前記接地統合部
の電圧とから前記接地統合部の接地インピーダンスを得
ること、又は前記接地統合部の接地に電圧を印加して、
前記接地統合部の接地に流れる電流と、前記補助電極を
基準として測定した前記接地統合部の電圧から前記印加
した電圧を減算した電圧とから前記接地統合部の接地イ
ンピーダンスを得ること、前記インピーダンスマトリク
スから前記接地インピーダンスを減じて、前記接地シス
テムの内の前記接地統合部の接地インピーダンスを除く
インピーダンスマトリクスを得ること、特徴とする接地
インピーダンス測定方法として構成した。
A first aspect of the present invention is a grounding system comprising N (≧ 2) devices that are individually grounded and a grounding integration unit that commonly grounds the N devices. , An auxiliary ground is provided, a voltage is applied to one of the N grounds to measure an electric current flowing through each of the N grounds to obtain an admittance, and this admittance measurement is performed for each of the N grounds. Applying a voltage to each of the remaining grounds to obtain an admittance matrix from which a total impedance matrix including the N grounds, the ground integration ground, and the plurality of devices is obtained. A voltage is applied to any one of the N grounds, and the connection is made from the current flowing to the ground of the ground integration unit and the voltage of the ground integration unit measured with the auxiliary electrode as a reference. To obtain a ground impedance of the integration unit, or by applying a voltage to ground of the ground integration unit,
Obtaining a ground impedance of the ground integrating unit from a current flowing to the ground of the ground integrating unit and a voltage obtained by subtracting the applied voltage from a voltage of the ground integrating unit measured with the auxiliary electrode as a reference; and the impedance matrix The ground impedance is subtracted from the ground impedance to obtain an impedance matrix excluding the ground impedance of the ground integration part of the ground system, and the ground impedance measuring method is configured.

【0008】第2の発明は、第1の発明において、前記
電圧の印加および/又は前記電流の測定を、変流器で行
なうことを特徴とする接地インピーダンス測定方法とし
て構成した。
According to a second aspect of the present invention, the grounding impedance measuring method according to the first aspect is characterized in that the voltage application and / or the current measurement is performed by a current transformer.

【0009】第3の発明は、第2の発明において、前記
変流器を、接地線に着脱可能な変流器であることを特徴
とする接地インピーダンス測定方法として構成した。
According to a third aspect of the present invention, in the second aspect of the present invention, the current transformer is a current transformer which is attachable to and detachable from a ground line.

【0010】第4の発明は、第2、第3の発明におい
て、前記電圧を印加する変流器が、印加電圧モニタ用の
補正巻線を具備することを特徴とする接地インピーダン
ス測定方法として構成した。
According to a fourth aspect of the present invention, in the second and third aspects, the current transformer for applying the voltage is provided with a correction winding for monitoring the applied voltage. did.

【0011】第5の発明は、第1乃至4の発明におい
て、前記接地統合部の接地インピーダンスの測定につい
て、前記接地統合部の接地に電圧を印加して行なう測
定、前記N個の接地の1以上に電圧を印加して行なう測
定の少なくとも2以上を実施し、それら測定結果の平均
値を用いることを特徴とする接地インピーダンス測定方
法として構成した。
In a fifth aspect based on the first to fourth aspects, the measurement of the ground impedance of the ground integration section is performed by applying a voltage to the ground of the ground integration section, and the one of the N grounds. At least two or more measurements performed by applying a voltage as described above were performed, and an average value of the measurement results was used to constitute a ground impedance measuring method.

【0012】第6の発明は、第2乃至4のの発明におい
て、前記接地統合部の接地インピーダンスの測定を、前
記接地統合部の接地に前記変流器を介して電圧を印加し
て行なう際に、前記補助電極を基準として電圧を測定す
る電圧測定手段と前記接地統合部との間の接地線を、前
記変流器に貫通させたことを特徴とする接地インピーダ
ンス測定方法として構成した。
According to a sixth aspect of the present invention, in the second to fourth aspects, when the ground impedance of the ground integration section is measured by applying a voltage to the ground of the ground integration section via the current transformer. In addition, the grounding wire between the voltage measuring means for measuring the voltage with the auxiliary electrode as a reference and the grounding integrated portion is penetrated through the current transformer.

【0013】[0013]

【発明の実施の形態】BEST MODE FOR CARRYING OUT THE INVENTION

[第1の実施の形態]図1は本発明の第1の実施の形態
の接地インピーダンスの測定方法を説明するための図で
あり、図6、図7におけるものと同一のものには同一の
符号を付してその詳しい説明は省略する。Saは装置A
と接地統合部Cとの間に電圧Vaを印加する測定用電圧
源、Sbは装置Bと接地統合部Cとの間に電圧Vbを印
加する測定用電圧源、Scは接地統合部Cとその接地と
の間に電圧Vcを印加する測定用電圧源である。Paux
は接地統合部Cの電圧を測定するために設けた補助電
極、Raux は補助電極Paux の接地インピーダンスであ
る。
[First Embodiment] FIG. 1 is a diagram for explaining a ground impedance measuring method according to a first embodiment of the present invention. The same components as those in FIGS. Reference numerals are given and detailed description thereof is omitted. Sa is device A
Between the device B and the ground integration unit C, a measurement voltage source that applies the voltage Va between the device B and the ground integration unit C, and Sc represents the ground integration unit C and the same. It is a voltage source for measurement that applies a voltage Vc to the ground. Paux
Is an auxiliary electrode provided for measuring the voltage of the ground integration portion C, and Raux is the ground impedance of the auxiliary electrode Paux.

【0014】さて、接地インピースダンスの測定は次の
通り行なう。まず、電圧源Saからの電圧Vaのみを印
加し(電圧Vb、Vcは印加せずその部分は短絡す
る。)、このとき電流測定器Iにより、装置Aを経由し
て流れる電流Ia、装置Bを経由して流れる電流Ibを
得て、yaa=Ia/Va、yab=Ib/Vaからアドミ
ッタンスyaa、yabを得る。
The ground in-piece dance is measured as follows. First, only the voltage Va from the voltage source Sa is applied (the voltage Vb and Vc are not applied and the part is short-circuited). At this time, the current measuring instrument I causes the current Ia flowing through the device A and the device B to flow. The electric current Ib flowing through is obtained, and the admittances yaa and yab are obtained from yaa = Ia / Va and yab = Ib / Va.

【0015】次に、測定用電圧源Sbからの電圧Vbの
みを印加し(電圧Va Vcは印加せずその部分は短絡
する。)、このとき電流測定器Iにより、装置Aを経由
して流れる電流Ia、装Bを経由して流れる電流Ibを
得て、yba=Ia/Vb、ybb=Ib/Vbからアドミ
ッタンスyba、ybbを得る。
Next, only the voltage Vb from the measuring voltage source Sb is applied (the voltage Va Vc is not applied and the portion is short-circuited), and at this time, the current is measured by the device A to flow through the device A. The current Ia and the current Ib flowing through the device B are obtained, and the admittances yba and ybb are obtained from yba = Ia / Vb and ybb = Ib / Vb.

【0016】これらを接地統合部Cから装置A側と装置
B側を見た4端子網のアドミッタンスマトリクスの形で
表すと、次の式(1)に示すようになる。
When these are expressed in the form of an admittance matrix of a four-terminal network in which the device A side and the device B side are viewed from the ground integration unit C, the following equation (1) is obtained.

【数1】 そこで、これを公知の方法、例えば、[Equation 1] Therefore, this is a known method, for example,

【数2】 なる公式を用いてインピーダンスマトリクス[Z]に変
換する。この4端子網のインピーダンスマトリクス
[Z]は、接地統合部Cからみた全体のインピーダンス
を表すものである。
[Equation 2] The impedance matrix [Z] is converted using the following formula. The impedance matrix [Z] of this four-terminal network represents the overall impedance as viewed from the ground integration section C.

【0017】次に、電圧源Sa、又はSbから電圧Va
又はVbを印加したとき(電圧Vcは印加せずその部分
を短絡する。)の補助電極Paux に対する接地統合部C
の電圧Voとその接地統合部Cの接地を流れる電流Ic
を測定する。この電圧Voは電流Icが流れたことによ
って、接地インピーダンスRcに発生する電圧である。
よって、接地インピーダンスRcの値は、次のようにし
て得られる。 Rc=Vo/Ic ・・・・(3)
Next, the voltage Va is supplied from the voltage source Sa or Sb.
Alternatively, when Vb is applied (the voltage Vc is not applied and the portion is short-circuited), the ground integration portion C for the auxiliary electrode Paux is provided.
Voltage Vo and the current Ic flowing through the ground of the ground integration unit C
Is measured. The voltage Vo is a voltage generated in the ground impedance Rc due to the flow of the current Ic.
Therefore, the value of the ground impedance Rc is obtained as follows. Rc = Vo / Ic ... (3)

【0018】又は、電圧源Scから電圧Vcを印加した
とき(電圧Va、Vbは印加せずその部分は短絡す
る。)の補助電極Paux に対する接地統合部Cの電圧V
oを測定し、その接地統合部Cを流れる電流Icを測定
する。なお、このときは、発生する電圧Voに、接地イ
ンピーダンスRcによる電圧降下以外に電圧源Scの電
圧Vcも含まれるので、その電圧Vcを減じて接地イン
ピーダンスRcに発生する正確な電圧を得る。よってこ
のときは、接地インピーダンスRcの値は次のようにし
て得られる。 Rc=(Vo−Vc)/Ic ・・・・(4)
Alternatively, when the voltage Vc is applied from the voltage source Sc (the voltages Va and Vb are not applied and the portions are short-circuited), the voltage V of the ground integration portion C with respect to the auxiliary electrode Paux.
o is measured, and the current Ic flowing through the ground integration portion C is measured. At this time, since the generated voltage Vo includes the voltage Vc of the voltage source Sc in addition to the voltage drop due to the ground impedance Rc, the voltage Vc is subtracted to obtain an accurate voltage generated in the ground impedance Rc. Therefore, at this time, the value of the ground impedance Rc is obtained as follows. Rc = (Vo-Vc) / Ic ... (4)

【0019】次に、図1を変形して、接地インピーダン
スRcを、理想的な接地(接地抵抗0Ω)とそれに直列
挿入したインピーダンスRcとして表すと、図2に示す
ようになる。さらに、この図2の回路の回路網Zを接地
統合部Cを共通帰線とする装置A、Bを含む第1の回路
網Z1と、接地インピーダンスRcのみの第2の回路網
Z2の縦続接続として表すと、図3に示すようになる。
Next, by modifying FIG. 1 and expressing the ground impedance Rc as an ideal ground (ground resistance 0Ω) and an impedance Rc inserted in series with it, it becomes as shown in FIG. Further, the circuit network Z of the circuit of FIG. 2 is cascade-connected to the first circuit network Z1 including the devices A and B having the common integration line C as the common return line and the second circuit network Z2 having only the ground impedance Rc. When expressed as, it becomes as shown in FIG.

【0020】第1の回路網Z1のインピーダンスマトリ
クスを[Z1]とし、第2の回路網Z2のインピーダン
スマトリクスを[Z2]とすると、図3の全体の回路網
Zのインピーダンスマトリクスを前記した[Z]とする
と、インピーダンスマトリクス[Z1]は、公知の公式
より、 [Z1]=[Z]−[Z2] ・・・・(5) で与えられる。ここで、第2の回路網Z2のインピーダ
ンスは、接地インピーダンスRcである。したがって、
インピーダンスマトクリス[Z1]は、インピーダンス
マトリクス[Z]の各要素より接地インピーダンスRc
を減じたものとして表される。
Assuming that the impedance matrix of the first network Z1 is [Z1] and the impedance matrix of the second network Z2 is [Z2], the impedance matrix of the entire network Z of FIG. ], The impedance matrix [Z1] is given by [Z1] = [Z] − [Z2] ... (5) from a known formula. Here, the impedance of the second network Z2 is the ground impedance Rc. Therefore,
The impedance matrix [Z1] is the ground impedance Rc from each element of the impedance matrix [Z].
Is represented by the subtraction of.

【0021】このようにして得られた回路網Z1のイン
ピーダンスマトリクス[Z1]は、装置A、Bの接地関
連部分のインピーダンス、接地統合部Cを共通帰線とし
た接地インピーダンスRa、Rb、相互インピーダンス
Rab等を含む接地システムの全体の接地に係るインピ
ーダンスを2端子網で表すインピーダンスマトリクスで
ある。
The impedance matrix [Z1] of the network Z1 thus obtained is the impedance of the ground-related parts of the devices A and B, the ground impedances Ra and Rb with the ground integration part C as a common return line, and the mutual impedance. It is an impedance matrix showing the impedance related to the entire grounding of the grounding system including Rab and the like by a two-terminal network.

【0022】以上から、本測定法によれば、接地統合部
Cを基準(共通帰線)としたシステム全体の接地インピ
ーダンスをインピーダンスマトリクスの形で測定するこ
とができる。なお、これまでの説明で明らかなように、
接地統合部Cの大地に対するインピーダンスRcは、式
(3)又は(4)により得ることができる。
From the above, according to the present measuring method, the ground impedance of the entire system with the ground integration section C as a reference (common return line) can be measured in the form of an impedance matrix. In addition, as is clear from the above description,
The impedance Rc of the ground integration part C with respect to the ground can be obtained by the equation (3) or (4).

【0023】なお、上記では接地システムが具備する装
置がA、Bで示すように2個、つまりN=2の場合であ
ったが、N=3個以上であっても同様にその接地システ
ムの全体を表すインピーダンスマトクリクスを測定する
ことができる。N=3の場合は6端子網として、N=4
の場合は8端子網として表される。
In the above description, the grounding system has two devices as shown by A and B, that is, N = 2. However, even if N = 3 or more, the grounding system of the grounding system also has the same configuration. It is possible to measure the overall impedance matrix. When N = 3, a 6-terminal network is used, N = 4
In the case of, it is represented as an 8-terminal network.

【0024】[第2の実施の形態]前記した接地インピ
ーダンスRcの測定について、測定用電圧源の電圧の印
加部位を複数箇所使用できる(第1の実施の形態では3
箇所)ことから、実際の測定では複数の個々の印加部位
に個々に電圧を印加して複数の測定を行ない、得られた
値の平均値を出してこれを用いることにより、測定の精
度を向上させることができる。なお、複数の印加部位の
個々に同時に測定用電圧源の電圧を印加し、そのときの
測定をもって平均値としても良い。
[Second Embodiment] Regarding the measurement of the ground impedance Rc described above, a plurality of sites to which the voltage of the measurement voltage source is applied can be used (in the first embodiment, 3).
Therefore, in actual measurement, voltage is individually applied to multiple individual application sites to perform multiple measurements, and the average value of the obtained values is calculated and used to improve the measurement accuracy. Can be made. It is also possible to apply the voltage of the measurement voltage source to each of the plurality of application sites at the same time and use the measurement at that time as the average value.

【0025】[第3の実施の形態]図4は本発明の第3
の実施の形態を説明するための図である。ここでは、測
定用電圧源Sからの電圧の印加を変流器を用いて行な
う。図4において、CTは巻線数mの変流器、Leは測
定用電圧を印加すべき接地線である。図4の(a)に示
すように、接地線Leに対して変流器CTを結合させる
ことによりm対1の変流器が構成でき、公知の原理によ
り測定用電圧源Sの電圧の1/m倍の電圧を接地線Le
に印加できる。また図4の(b)に示すように、接地線
Leをn回巻くことよりm対nの変流器が構成でき、測
定用電圧源Sの電圧のn/m倍の電圧を接地線Leに印
加できる。以上において、変流器CTを、接地線Leに
対して着脱できるクランプ形のものにすることにより、
接地線Leを切断することなくその現状を保持したま
ま、所望の電圧の印加を行なうことができる。
[Third Embodiment] FIG. 4 shows a third embodiment of the present invention.
It is a figure for explaining an embodiment. Here, the voltage from the measurement voltage source S is applied by using a current transformer. In FIG. 4, CT is a current transformer having a winding number of m, and Le is a ground wire to which a measurement voltage is applied. As shown in FIG. 4A, a current transformer of m: 1 can be constructed by coupling a current transformer CT to the ground line Le, and the voltage of the measurement voltage source S of 1 / M times the voltage to ground wire Le
Can be applied to. Further, as shown in FIG. 4B, by winding the ground wire Le n times, an m: n current transformer can be configured, and a voltage n / m times the voltage of the measurement voltage source S can be applied to the ground wire Le. Can be applied to. In the above, by making the current transformer CT into a clamp type that can be attached to and detached from the ground wire Le,
It is possible to apply a desired voltage without disconnecting the ground line Le while maintaining the current state.

【0026】印加電圧は、図4の(c)に示すように、
補正用巻線Lc並びに終端抵抗Rmからなるモニタ回路
を付加することによって、接地線Leに印加される電圧
と同じ電圧を終端抵抗Rmの両端に発生させて電圧測定
器Vでモニタ可能にし、変流器の結合量の誤差を補正す
ることができる。なお、終端抵抗Rmの値は電圧を印加
している部位のインピーダンスに近い値が最適である
が、これを削除することも可能である。
The applied voltage is, as shown in FIG.
By adding a monitor circuit composed of the correction winding Lc and the terminating resistor Rm, the same voltage as the voltage applied to the ground line Le is generated at both ends of the terminating resistor Rm so that the voltage measuring device V can monitor the voltage. It is possible to correct the error in the coupling amount of the sink. The value of the terminating resistor Rm is optimally a value close to the impedance of the portion to which the voltage is applied, but it can be deleted.

【0027】なお、ここでは電圧の印加に変流器を使用
しているが、この変流器は、接地線に対して同様に結合
することにより、電流の測定においても使用することが
できることは勿論である。以上から、接地線を切断する
ことなくその接地線に測定用電圧を印加したり、あるい
はその接地線に流れる電流を測定することができ、接地
システムの現状を変更することなく接地インピーダンス
の測定ができるようになる。
Although a current transformer is used here to apply a voltage, this current transformer can also be used in current measurement by similarly coupling it to the ground line. Of course. From the above, it is possible to apply a measurement voltage to the ground wire without disconnecting the ground wire or measure the current flowing through the ground wire, and to measure the ground impedance without changing the current status of the ground system. become able to.

【0028】[第4の実施の形態]図5は本発明の第5
の実施の形態を示す図である。前述した第1の実施の形
態で説明したように、測定用電圧源Scから電圧Vcを
接地インピーダンスRcに印加し、その接地インピーダ
ンスRcの値を測定する場合、接地統合部Cに対する測
定電圧Voから測定用電圧源の電圧Vcを減じる演算が
必要である。
[Fourth Embodiment] FIG. 5 shows a fifth embodiment of the present invention.
It is a figure showing an embodiment. As described in the first embodiment, when the voltage Vc is applied to the ground impedance Rc from the measurement voltage source Sc and the value of the ground impedance Rc is measured, the measured voltage Vo for the ground integration unit C is changed. A calculation for reducing the voltage Vc of the measuring voltage source is required.

【0029】ここでは、その演算を不要とするために、
図5に示すように、接地インピーダンスRcに接続され
る接地線Leの他に、電圧を印加している変流器CTを
貫通するように接地線Laを接地統合部Cから配置し、
その貫通した接地線Laと補助電極Paux との間に電圧
測定器Vを接続して、接地インピーダンスRcに発生す
る電圧Voを測定する。
Here, in order to make the calculation unnecessary,
As shown in FIG. 5, in addition to the ground line Le connected to the ground impedance Rc, the ground line La is arranged from the ground integration section C so as to penetrate the current transformer CT that applies a voltage,
A voltage measuring device V is connected between the penetrating ground line La and the auxiliary electrode Paux to measure the voltage Vo generated in the ground impedance Rc.

【0030】これにより、変流器CTを貫通した接地線
Laに印加された測定用電圧源Scの電圧Vcと、接地
線Leに印加された測定用電圧源Scの電圧Vcが打ち
消し合うので、電圧測定器Vの測定電圧Voをそのまま
使用して、式(3)に示したような演算のみで接地イン
ピーダンスRcを得ることができる。つまり、式(4)
にあるような演算が不要となる。
As a result, the voltage Vc of the measuring voltage source Sc applied to the ground line La penetrating the current transformer CT and the voltage Vc of the measuring voltage source Sc applied to the ground line Le cancel each other. Using the measured voltage Vo of the voltage measuring device V as it is, the ground impedance Rc can be obtained only by the calculation shown in the equation (3). That is, equation (4)
There is no need for the calculation like in.

【0031】[0031]

【発明の効果】以上から本発明によれば、個々に接地さ
れたN(≧2)個の装置と、該複数の装置の接地を共通
に行なう接地統合部とからなる接地システムにおいて、
N個の装置の接地関連部分のインピーダンス、N個の装
置の接地インピーダンス、N個の装置の相互間のインピ
ーダンス等の接地に係るインピーダンスをマトリクスと
して得ることができるので、接地システムの接地インピ
ーダンスの把握が容易となる。
As described above, according to the present invention, in a grounding system comprising N (≧ 2) individually grounded devices and a grounding integrated section for commonly grounding the plurality of devices,
It is possible to obtain the impedance related to grounding such as the impedance of the ground-related part of the N devices, the ground impedance of the N devices, the impedance between the N devices, and the like, so that the ground impedance of the grounding system can be grasped. Will be easier.

【0032】また、特に着脱形の変流器を用いて接地線
に電圧を印加したり、その接地線の電流を測定すること
により、その接地インピーダンス測定において、現状を
変更することなく、つまり接地を切り離すことなくそれ
を実現することができる。
In particular, by applying a voltage to the ground wire or measuring the current of the ground wire by using a detachable current transformer, the ground impedance can be measured without changing the present condition, that is, the ground. Can be achieved without disconnecting.

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

【図1】 本発明の第1の実施の形態の測定方法を説明
するための接地システムを示す回路図である。
FIG. 1 is a circuit diagram showing a ground system for explaining a measuring method according to a first embodiment of the present invention.

【図2】 図1に示した接地システムの回路の一部を変
更した接地システムを示す回路図である。
FIG. 2 is a circuit diagram showing a grounding system in which a part of the circuit of the grounding system shown in FIG. 1 is modified.

【図3】 図2に示した接地システムを回路網として説
明するための回路図である。
FIG. 3 is a circuit diagram for explaining the grounding system shown in FIG. 2 as a circuit network.

【図4】 本発明の第3の実施の形態を示す図で、測定
用電源による電圧の印加を変流器を使用して行なう場合
を示す図である。
FIG. 4 is a diagram showing a third embodiment of the present invention and is a diagram showing a case where a voltage is applied by a measurement power source using a current transformer.

【図5】 本発明の第4の実施の形態を示す図で、測定
用電源の電圧をキャンセルできるようにした場合の説明
図である。
FIG. 5 is a diagram showing a fourth embodiment of the present invention, and is an explanatory diagram in the case where the voltage of the measurement power supply can be canceled.

【図6】 従来の接地システムの回路図である。FIG. 6 is a circuit diagram of a conventional grounding system.

【図7】 従来の接地インピーダンスの測定方法を説明
するための回路図である。
FIG. 7 is a circuit diagram for explaining a conventional ground impedance measuring method.

【符号の説明】[Explanation of symbols]

A、B:装置、C:接地統合部、Ra、Rb、Rc、R
v、Raux :接地インピーダンス、Rab:相互インピ
ーダンス、Pi:電流印加補助電極、Pv:電圧測定用
補助電極、Paux :補助電極、P:被測定接地電極、
S、Sa、Sb、Sc:測定用電圧源、I:電流測定
器、V:電圧測定器、CT:変流器、Le、La:接地
線、Lc:補正巻線。
A, B: Device, C: Ground integration unit, Ra, Rb, Rc, R
v, Raux: ground impedance, Rab: mutual impedance, Pi: current application auxiliary electrode, Pv: voltage measurement auxiliary electrode, Paux: auxiliary electrode, P: ground electrode to be measured,
S, Sa, Sb, Sc: voltage source for measurement, I: current measuring device, V: voltage measuring device, CT: current transformer, Le, La: ground wire, Lc: correction winding.

Claims (6)

【特許請求の範囲】[Claims] 【請求項1】個々に接地されたN(≧2)個の装置と、
該N個の装置の接地を共通に行なう接地統合部とからな
る接地システムにおいて、補助接地を設け、 前記N個の接地の内の1つの接地に電圧を印加して前記
N個の接地に流れる電流を各々測定してアドミッタンス
を得、このアドミッタンス測定を前記N個の接地の残り
の接地の各々に電圧を印加し行なってアドミッタンスマ
トリクスを得、該アドミッタンスマトリクスから前記N
個の接地、前記接地統合部の接地、および前記複数の装
置を含む全体のインピーダンスマトリクスを得ること、 前記N個の接地のいずれか1つに電圧を印加して、前記
接地統合部の接地に流れる電流と、前記補助電極を基準
として測定した前記接地統合部の電圧とから前記接地統
合部の接地インピーダンスを得ること、又は前記接地統
合部の接地に電圧を印加して、前記接地統合部の接地に
流れる電流と、前記補助電極を基準として測定した前記
接地統合部の電圧から前記印加した電圧を減算した電圧
とから前記接地統合部の接地インピーダンスを得るこ
と、 前記インピーダンスマトリクスから前記接地インピーダ
ンスを減じて、前記接地システムの内の前記接地統合部
の接地インピーダンスを除くインピーダンスマトリクス
を得ること、 特徴とする接地インピーダンス測定方法。
1. N (≧ 2) individually grounded devices,
In a grounding system comprising a grounding integration unit for commonly grounding the N devices, an auxiliary ground is provided, and a voltage is applied to one of the N grounds to flow to the N grounds. Each of the currents is measured to obtain an admittance, and the admittance measurement is performed by applying a voltage to each of the remaining grounds of the N grounds to obtain an admittance matrix. From the admittance matrix, the N
To obtain a total impedance matrix including a plurality of grounds, the ground integration unit ground, and the plurality of devices, and applying a voltage to any one of the N grounds to connect the ground integration unit grounds. Obtaining the grounding impedance of the grounding integration unit from the flowing current and the voltage of the grounding integration unit measured with the auxiliary electrode as a reference, or by applying a voltage to the ground of the ground integration unit, Obtaining the ground impedance of the ground integration unit from the current flowing to the ground and the voltage obtained by subtracting the applied voltage from the voltage of the ground integration unit measured with the auxiliary electrode as a reference, the ground impedance from the impedance matrix Subtracting to obtain an impedance matrix excluding the ground impedance of the ground integration part of the ground system, Ground impedance measurement method and butterflies.
【請求項2】前記電圧の印加および/又は前記電流の測
定を、変流器で行なうことを特徴とする請求項1に記載
の接地インピーダンス測定方法。
2. The ground impedance measuring method according to claim 1, wherein the voltage application and / or the current measurement is performed by a current transformer.
【請求項3】前記変流器が、接地線に着脱可能な変流器
であることを特徴とする請求項2に記載の接地インピー
ダンス測定方法。
3. The ground impedance measuring method according to claim 2, wherein the current transformer is a current transformer that can be attached to and detached from a ground wire.
【請求項4】前記電圧を印加する変流器が、印加電圧モ
ニタ用の補正巻線を具備することを特徴とする請求項2
又は3に記載の接地インピーダンス測定方法。
4. The current transformer for applying the voltage comprises a correction winding for monitoring the applied voltage.
Alternatively, the ground impedance measuring method described in 3 above.
【請求項5】前記接地統合部の接地インピーダンスの測
定について、前記接地統合部の接地に電圧を印加して行
なう測定、前記N個の接地の1以上に電圧を印加して行
なう測定の少なくとも2以上を実施し、それら測定結果
の平均値を用いることを特徴とする請求項1乃至4に記
載の接地インピーダンス測定方法。
5. At least two of the measurement of the ground impedance of the ground integration unit, that is, the measurement performed by applying a voltage to the ground of the ground integration unit and the measurement performed by applying a voltage to one or more of the N grounds. The ground impedance measuring method according to any one of claims 1 to 4, wherein the above is performed and an average value of the measurement results is used.
【請求項6】前記接地統合部の接地インピーダンスの測
定を、前記接地統合部の接地に前記変流器を介して電圧
を印加して行なう際に、前記補助電極を基準として電圧
を測定する電圧測定手段と前記接地統合部との間の接地
線を、前記変流器に貫通させたことを特徴とする請求項
2乃至4に記載の接地インピーダンス測定方法。
6. A voltage for measuring a voltage with reference to the auxiliary electrode when the ground impedance of the ground integration unit is measured by applying a voltage to the ground of the ground integration unit via the current transformer. The grounding impedance measuring method according to claim 2, wherein a grounding wire between the measuring means and the grounding integrated portion is penetrated through the current transformer.
JP7928996A 1996-03-08 1996-03-08 Method for measuring ground impedance Withdrawn JPH09243686A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP7928996A JPH09243686A (en) 1996-03-08 1996-03-08 Method for measuring ground impedance

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP7928996A JPH09243686A (en) 1996-03-08 1996-03-08 Method for measuring ground impedance

Publications (1)

Publication Number Publication Date
JPH09243686A true JPH09243686A (en) 1997-09-19

Family

ID=13685709

Family Applications (1)

Application Number Title Priority Date Filing Date
JP7928996A Withdrawn JPH09243686A (en) 1996-03-08 1996-03-08 Method for measuring ground impedance

Country Status (1)

Country Link
JP (1) JPH09243686A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2009258011A (en) * 2008-04-18 2009-11-05 J-Power Systems Corp Partial discharge measuring method

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2009258011A (en) * 2008-04-18 2009-11-05 J-Power Systems Corp Partial discharge measuring method

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