JP2003021657A - Potential detector - Google Patents

Potential detector

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Publication number
JP2003021657A
JP2003021657A JP2001205278A JP2001205278A JP2003021657A JP 2003021657 A JP2003021657 A JP 2003021657A JP 2001205278 A JP2001205278 A JP 2001205278A JP 2001205278 A JP2001205278 A JP 2001205278A JP 2003021657 A JP2003021657 A JP 2003021657A
Authority
JP
Japan
Prior art keywords
resistor
conductor
potential
temperature characteristic
intermediate electrode
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.)
Pending
Application number
JP2001205278A
Other languages
Japanese (ja)
Inventor
Aya Yamamoto
綾 山本
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.)
Mitsubishi Electric Corp
Original Assignee
Mitsubishi Electric 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 Mitsubishi Electric Corp filed Critical Mitsubishi Electric Corp
Priority to JP2001205278A priority Critical patent/JP2003021657A/en
Publication of JP2003021657A publication Critical patent/JP2003021657A/en
Pending legal-status Critical Current

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Abstract

PROBLEM TO BE SOLVED: To provide an inexpensive potential detector having reduced fluctuation of a measuring potential caused by temperature conversion, concerning a potential-dividing type potential detector having an intermediate electrode provided between a conductor and a reference potential, for measuring the potential induced in the intermediate electrode, in order to measure the potential of the conductor. SOLUTION: This detector is equipped with a resistor having a characteristic capable of compensating the temperature change of a capacitance formed between the conductor 1 which is a potential measuring object and the intermediate electrode 5, placed between a structure 2 having reference potential to the intermediate electrode 5 and the conductor 1. The resistor may be constituted from an electrical network of the resistor formed by combining a resistor 8 having a prescribed temperature characteristic and resistors 9, 10 having a stable temperature characteristic, or constituted from a single resistor having a prescribed temperature characteristic A.

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】この発明は電位検出器に関
し、特に、導体の電位を測定する目的で、導体と基準電
位との間に中間電極を設け、この中間電極に誘起する電
位を計測する分圧型の電位検出器に関するものである。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a potential detector, and in particular, for the purpose of measuring the potential of a conductor, an intermediate electrode is provided between the conductor and a reference potential and the potential induced in this intermediate electrode is measured. The present invention relates to a pressure type electric potential detector.

【0002】[0002]

【従来の技術】図7は従来の分圧型電位検出器(以下、
分圧型PDとする。)の構成を示した概略構成図であ
る。図において、1は導体、2は構造物、3は誘電率μ
1の物質であり静電容量C1を形成しており、4は誘電
率μ2の物質であり、静電容量C2を形成しており、5
は中間電極である。
2. Description of the Related Art FIG. 7 shows a conventional voltage division type potential detector (hereinafter referred to as
It is a partial pressure type PD. 2] is a schematic configuration diagram showing the configuration of FIG. In the figure, 1 is a conductor, 2 is a structure, and 3 is a dielectric constant μ.
1 is a substance that forms an electrostatic capacitance C1, 4 is a substance having a dielectric constant of μ2, and forms an electrostatic capacitance C2.
Is an intermediate electrode.

【0003】図8は例えば特開平8−75795号公報
に示された従来のガス絶縁電気機器用変圧器を示す構成
図である。図8において、101は接地容器、101a
は接地容器101の端部に外側に突出して形成されたフ
ランジ、102はこの接地容器101の連結部において
フランジ101a間に取り付けられた絶縁スペーサ、1
03は絶縁スペーサ102によって支持された主回路導
体、104は導体103を収納している接地容器、10
4aは接地容器104の端部に外側に突出して形成され
たフランジである。
FIG. 8 is a block diagram showing a conventional transformer for gas-insulated electrical equipment disclosed in, for example, Japanese Patent Laid-Open No. 8-75795. In FIG. 8, 101 is a grounded container, 101a
Is a flange formed on the end of the grounding container 101 so as to project outward, 102 is an insulating spacer attached between the flanges 101a at the connection part of the grounding container 101,
Reference numeral 03 designates a main circuit conductor supported by the insulating spacer 102, 104 designates a ground container housing the conductor 103, 10
Reference numeral 4a is a flange formed on the end of the ground container 104 so as to project outward.

【0004】また、105は接地容器101のフランジ
部101aに形成された所定の径と深さの段差部で、複
数のネジ穴が形成されている。106は接地容器101
において、フランジ101aから所定の距離の位置に形
成された接続口で、開口部に密封端子107が取り付け
られている。108は径が接地容器101の内径より小
さい所定の径と長さに形成された筒状部材、109は筒
状部材108の一端の外側に突出して形成された第1の
フランジで、外形は段差部105と嵌合して取り付け部
を形成するようにされ、複数の取り付け穴が形成されて
いる。そして各フランジ109、110は互いに平行
で、第1のフランジ109の取り付け面と第2のフラン
ジ110のネジ穴とは直角となるようにされている。
Reference numeral 105 denotes a stepped portion having a predetermined diameter and depth formed on the flange portion 101a of the ground container 101, and has a plurality of screw holes formed therein. 106 is the ground container 101
In, the sealed terminal 107 is attached to the opening at a connection port formed at a predetermined distance from the flange 101a. Reference numeral 108 denotes a tubular member formed to have a predetermined diameter and length smaller than the inner diameter of the grounding container 101, and 109 denotes a first flange projecting outside one end of the tubular member 108, and the outer shape has a step. A plurality of mounting holes are formed by fitting with the portion 105 to form a mounting portion. The flanges 109 and 110 are parallel to each other, and the mounting surface of the first flange 109 and the screw hole of the second flange 110 are perpendicular to each other.

【0005】また、111は外径が筒状部材108とほ
ぼ同じ径で所定の厚さと長さに形成された円筒状の二次
側電極、112は二次側電極111の厚さ方向の中心部
に形成された複数の貫通穴、113は貫通穴112の両
端部に嵌着された一対の絶縁部材で、外径が二次側電極
111の厚さとほぼ同じ径で、中心部に所定の径のボル
ト穴が形成されている。114は二次側電極111の他
端部に配置される端部電極、115は端部電極114、
絶縁部材113、二次側電極111、絶縁部材113を
それぞれ貫通して第2のフランジ110に締め付ける締
付ネジである。
Reference numeral 111 denotes a cylindrical secondary electrode having an outer diameter substantially the same as that of the tubular member 108 and having a predetermined thickness and length, and 112 a center of the secondary electrode 111 in the thickness direction. A plurality of through holes formed in the portion, 113 is a pair of insulating members fitted to both ends of the through hole 112, and has an outer diameter substantially the same as the thickness of the secondary electrode 111 and a predetermined center portion. A bolt hole having a diameter is formed. 114 is an end electrode arranged at the other end of the secondary electrode 111, 115 is an end electrode 114,
It is a tightening screw that penetrates the insulating member 113, the secondary electrode 111, and the insulating member 113 and is fastened to the second flange 110.

【0006】このように他端部に端部電極114と二次
側電極111が取り付けられた筒状部材108は、一端
部が接地容器101の段差部105に嵌合して位置決め
され、取り付けネジ116によって接地容器101に固
着される。そして、二次側電極111は接続口106に
配置された信号変換器117とリード線118によって
接続される。このようにしてコンデンサ型分圧器部が形
成されている。
The cylindrical member 108 having the end electrode 114 and the secondary electrode 111 attached to the other end in this manner is positioned by fitting one end into the step portion 105 of the grounding container 101, and then mounting screw. It is fixed to the ground container 101 by 116. Then, the secondary electrode 111 is connected to the signal converter 117 arranged at the connection port 106 by the lead wire 118. In this way, the capacitor type voltage divider unit is formed.

【0007】[0007]

【発明が解決しようとする課題】電位検出器の一つの実
例である従来の分圧型PDの場合、誘電率μ1の物質3
は、SF6ガスなどの特定の誘電率を持った絶縁物であ
った。このため、誘電率μ1の物質3における誘電率μ
1の温度特性が、電位検出器の出力に影響を与えるとい
う問題点があった。
In the case of the conventional partial pressure type PD which is one example of the potential detector, the substance 3 having a dielectric constant μ1 is used.
Was an insulator having a specific dielectric constant such as SF6 gas. Therefore, the dielectric constant μ of the substance 3 having the dielectric constant μ1
There is a problem that the temperature characteristic of 1 affects the output of the potential detector.

【0008】また、中間電極5、構造物2の間の空間に
充填される絶縁物の誘電率の温度変化によっても、電位
検出器の出力に影響が出るなどの問題点があった。
Further, there is a problem that the output of the potential detector is affected by the temperature change of the dielectric constant of the insulator filled in the space between the intermediate electrode 5 and the structure 2.

【0009】加えて、導体1、中間電極5、構造物2の
温度変化によって相互の位置関係が変化するため、電位
検出器の出力が変動するという問題点があった。
In addition, there is a problem that the output of the potential detector fluctuates because the mutual positional relationship changes due to the temperature change of the conductor 1, the intermediate electrode 5, and the structure 2.

【0010】この発明は、かかる問題点を解決するため
になされたものであり、温度変化による影響を抑制でき
る電位検出器を得ることを目的とする。
The present invention has been made to solve the above problems, and an object thereof is to obtain a potential detector capable of suppressing the influence of temperature change.

【0011】[0011]

【課題を解決するための手段】この発明は、電位の測定
対象である導体と、前記導体に対する基準電位を有する
構造物と、前記構造物と前記導体との間に設けられ、前
記導体に印加された交流電圧を分圧する中間電極と、前
記導体と前記中間電極との間に設けられ、所定の誘電率
μ1を有して、所定の静電容量C1を形成する物質と、
前記構造物と前記中間電極との間に設けられ、前記静電
容量C1の温度変化を補償する特定の温度特性Aを有す
る抵抗手段とを備えた電位検出器である。
The present invention provides a conductor whose potential is to be measured, a structure having a reference potential with respect to the conductor, and a structure which is provided between the structure and the conductor and which is applied to the conductor. An intermediate electrode that divides the generated AC voltage; a substance that is provided between the conductor and the intermediate electrode, has a predetermined dielectric constant μ1, and forms a predetermined capacitance C1;
The potential detector is provided between the structure and the intermediate electrode, and includes a resistance unit having a specific temperature characteristic A for compensating the temperature change of the capacitance C1.

【0012】また、前記抵抗手段の両端の電圧を積分す
るための積分器をさらに備えている。
Further, an integrator for integrating the voltage across the resistance means is further provided.

【0013】また、前記抵抗手段は、所定の温度特性B
を有する抵抗体と温度特性が安定な複数の抵抗体とを組
合せた抵抗網から構成され、前記抵抗網全体の温度特性
が前記温度特性Aと同等である。
Further, the resistance means has a predetermined temperature characteristic B.
And a resistance network in which a plurality of resistors having stable temperature characteristics are combined, and the temperature characteristics of the entire resistance network are equivalent to the temperature characteristics A.

【0014】また、前記特定の温度特性Bを有する抵抗
体は白金から構成されている。
The resistor having the specific temperature characteristic B is made of platinum.

【0015】また、前記特定の温度特性Bを有する抵抗
体は銅から構成されている。
The resistor having the specific temperature characteristic B is made of copper.

【0016】また、前記構造物と前記中間電極との間に
充填され、前記抵抗手段と並列回路を構成する誘電率μ
2の物質をさらに備えている。
The dielectric constant μ is filled between the structure and the intermediate electrode and forms a parallel circuit with the resistance means.
It further comprises two substances.

【0017】また、前記抵抗手段の両端にコンデンサを
さらに設けている。
Further, capacitors are further provided at both ends of the resistance means.

【0018】[0018]

【発明の実施の形態】実施の形態1.図1は、この発明
の実施の形態1である電位検出器を示すもので、図にお
いて、1は導体、2は導体1に対して基準電圧を持つ構
造物、3は誘電率μ1の絶縁物からなり、導体1を支持
している物質、5は物質3の導体1とは反対側の端部に
設けられ、導体1に印加された交流電圧を分圧する中間
電極、6は中間電極5と構造物2との間に設けられ、所
定の温度特性Aを持つ抵抗体を示す。
BEST MODE FOR CARRYING OUT THE INVENTION Embodiment 1. 1 shows a potential detector according to a first embodiment of the present invention, in which 1 is a conductor, 2 is a structure having a reference voltage with respect to conductor 1, and 3 is an insulator having a dielectric constant μ1. A material supporting the conductor 1, 5 is provided at the end of the material 3 opposite to the conductor 1, and is an intermediate electrode for dividing the AC voltage applied to the conductor 1, and 6 is an intermediate electrode 5. A resistor provided between the structure 2 and the predetermined temperature characteristic A is shown.

【0019】次に図1に示した電位検出器の動作につい
て説明する。図1において、導体1には、構造物2を基
準電位とする交流電圧が印加される。導体1に印加され
た交流電圧は、中間電極5によって分圧される。この時
の分圧比は、導体1の形状と中間電極5の形状及び誘電
率μ1の物質3が持つ誘電率によって決定されるインピ
ーダンスZ1と温度特性Aを持つ抵抗体6の抵抗値の比
によって決定される。インピーダンスZ1は、周知のと
おり、導体1と中間電極5が形成する実効的な電極の面
積S、導体1と中間電極5との実効的な距離d、誘電率
μ1の物質3の誘電率μ1から計算される静電容量C=
μ1×S÷dから求められ、インピーダンスZ1は、導
体1に印加される交流電圧をVi、前記交流電圧Viの
周波数をfとし、複素表示をjとすると、Z1=d÷
(j×2×π×f×μ1×S)となる。中間電極5に発
生する電圧Voは、導体1に印加される交流電圧をV
i、前記交流電圧Viの周波数をf、温度特性Aを持つ
抵抗体6の抵抗値をRとすると、Vo=Vi×R÷(Z
1+R)=Vi×R÷((d÷(j×2×π×f×μ1
×S))+R)である。
Next, the operation of the potential detector shown in FIG. 1 will be described. In FIG. 1, an AC voltage having the structure 2 as a reference potential is applied to the conductor 1. The AC voltage applied to the conductor 1 is divided by the intermediate electrode 5. The voltage division ratio at this time is determined by the ratio of the impedance Z1 determined by the shape of the conductor 1 and the shape of the intermediate electrode 5 and the dielectric constant of the substance 3 having the dielectric constant μ1 to the resistance value of the resistor 6 having the temperature characteristic A. To be done. As is well known, the impedance Z1 is calculated from the effective electrode area S formed by the conductor 1 and the intermediate electrode 5, the effective distance d between the conductor 1 and the intermediate electrode 5, and the dielectric constant μ1 of the substance 3 having the dielectric constant μ1. Calculated capacitance C =
Impedance Z1 is obtained from μ1 × S ÷ d, where Z1 = d ÷ when the alternating voltage applied to the conductor 1 is Vi, the frequency of the alternating voltage Vi is f, and the complex display is j.
(J × 2 × π × f × μ1 × S). The voltage Vo generated at the intermediate electrode 5 is the AC voltage applied to the conductor 1
i, the frequency of the AC voltage Vi is f, and the resistance value of the resistor 6 having the temperature characteristic A is R, Vo = Vi × R ÷ (Z
1 + R) = Vi × R ÷ ((d ÷ (j × 2 × π × f × μ1
× S)) + R).

【0020】R≪Z1で用いる場合、Vo=Vi×R÷
Z1=j×2×π×f×R×μ1×S×Vi÷dとな
る。
When using R << Z1, Vo = Vi × R ÷
Z1 = j × 2 × π × f × R × μ1 × S × Vi ÷ d.

【0021】本発明における電位検出器の温度が変化す
ると、誘電率μ1の物質3の誘電率μ1が変化すると共
に、導体1、中間電極5、構造物2の相対的な位置関係
も変化し、導体1と中間電極5が形成する実効的な電極
の面積S及び導体1と中間電極5との実効的な距離dが
変化する。従って、導体1と中間電極5とその間の空間
を埋める誘電率μ1の物質3が形成する静電容量が変化
し、インピーダンスZ1が変化する。本実施の形態にお
ける抵抗体6は、この時のμ1、S、dの変化に起因す
るインピーダンスZ1の温度変化と同等な変化を示す温
度特性Aを有している。このような抵抗体6を選ぶこと
により、本実施の形態においては、電位検出器の出力電
圧Voの温度による変化を抑制でき、安定した出力とす
ることができる。
When the temperature of the potential detector in the present invention changes, the dielectric constant μ1 of the substance 3 having the dielectric constant μ1 changes, and the relative positional relationship between the conductor 1, the intermediate electrode 5, and the structure 2 also changes, The effective electrode area S formed by the conductor 1 and the intermediate electrode 5 and the effective distance d between the conductor 1 and the intermediate electrode 5 change. Therefore, the capacitance formed by the conductor 1, the intermediate electrode 5, and the substance 3 having a dielectric constant μ1 that fills the space between them changes, and the impedance Z1 changes. The resistor 6 in the present embodiment has a temperature characteristic A showing a change equivalent to the temperature change of the impedance Z1 due to the change of μ1, S, d at this time. By selecting such a resistor 6, in the present embodiment, a change in the output voltage Vo of the potential detector due to the temperature can be suppressed and a stable output can be obtained.

【0022】以上のように、本実施の形態においては、
物質3の誘電率μ1、導体1と中間電極5が形成する実
効的な電極の面積S及び導体1と中間電極5との実効的
な距離dの変化に起因するインピーダンスZ1の温度変
化と同等な変化を示す温度特性Aを有する抵抗体6を、
中間電極と構造物との間に導入することにより、電位検
出器の出力電圧Voの温度による変化を抑制でき、温度
に対して安定な出力を得られる電位検出器を得ることが
できる。
As described above, in the present embodiment,
The dielectric constant μ1 of the substance 3, the effective electrode area S formed by the conductor 1 and the intermediate electrode 5, and the temperature change of the impedance Z1 due to the change of the effective distance d between the conductor 1 and the intermediate electrode 5 are equivalent to The resistor 6 having the temperature characteristic A indicating the change is
By introducing between the intermediate electrode and the structure, it is possible to suppress the change of the output voltage Vo of the potential detector due to the temperature, and it is possible to obtain the potential detector that can obtain a stable output with respect to the temperature.

【0023】実施の形態2.図2は、この発明の実施の
形態2である電位検出器を示すもので、図において、1
は導体、2は構造物、3は誘電率μ1の物質、5は中間
電極、6は温度特性Aを持つ抵抗体、7は抵抗体6の両
端の電圧Vrを積分する積分器を示す。
Embodiment 2. FIG. 2 shows a potential detector according to a second embodiment of the present invention.
Is a conductor, 2 is a structure, 3 is a substance having a dielectric constant of μ1, 5 is an intermediate electrode, 6 is a resistor having a temperature characteristic A, and 7 is an integrator for integrating the voltage Vr across the resistor 6.

【0024】次に動作について説明する。温度特性Aを
持つ抵抗体6の両端の電圧Vrは、上述の実施の形態1
の出力電圧Voと同じく、Vr=j×2×π×f×R×
μ1×S×Vi÷dとなるため、導体1に印加される交
流電圧Viを微分した波形となる。電位検出器の出力と
して、当該交流電圧Viに比例した電圧波形を得るため
には、温度特性Aを持つ抵抗体6の両端の電圧Vrを積
分器7によって積分することで、交流電圧Viに比例し
た出力電圧Voを得ることができる。
Next, the operation will be described. The voltage Vr across the resistor 6 having the temperature characteristic A is the same as in the first embodiment.
Of the output voltage Vo of Vr = j × 2 × π × f × R ×
Since μ1 × S × Vi ÷ d, the waveform is a waveform obtained by differentiating the AC voltage Vi applied to the conductor 1. In order to obtain a voltage waveform proportional to the AC voltage Vi as the output of the potential detector, the voltage Vr across the resistor 6 having the temperature characteristic A is integrated by the integrator 7 to be proportional to the AC voltage Vi. The output voltage Vo can be obtained.

【0025】以上のように、本実施の形態においては、
上述の実施の形態1の構成に、さらに、温度特性Aを持
つ抵抗体6の両端の電圧Vrを積分するための積分器7
を設けて、電圧Vrを積分することにより、導体1に印
加される交流電圧Viに比例した出力電圧Voを得るよ
うにしたので、温度変化による影響を受けることなく、
温度に対して安定な出力を得られる電位検出器を得るこ
とができる。
As described above, in the present embodiment,
In addition to the configuration of the first embodiment described above, an integrator 7 for integrating the voltage Vr across the resistor 6 having the temperature characteristic A is further added.
Is provided and the output voltage Vo proportional to the AC voltage Vi applied to the conductor 1 is obtained by integrating the voltage Vr.
It is possible to obtain a potential detector that can obtain a stable output with respect to temperature.

【0026】実施の形態3.図3はこの発明の実施の形
態3である電位検出器を示すもので、図3において、1
は導体、2は構造物、3は誘電率μ1の物質、5は中間
電極、8は温度特性Bを持つ抵抗体、9及び10は所定
の抵抗値を有する温度特性の安定した抵抗体を示す。
Embodiment 3. 3 shows a potential detector according to a third embodiment of the present invention. In FIG.
Is a conductor, 2 is a structure, 3 is a substance having a dielectric constant of μ1, 5 is an intermediate electrode, 8 is a resistor having a temperature characteristic B, and 9 and 10 are resistors having a predetermined resistance value and having a stable temperature characteristic. .

【0027】次に動作について説明する。温度特性Bを
持つ抵抗体8、抵抗体9、抵抗体10からなる抵抗網の
合成抵抗は、実施の形態1と同様に導体1と中間電極5
に挟まれた誘電率μ1の物質3が形成する静電容量の温
度による変化を補償しようとするものである。図3に示
した実施の形態3では、例えば温度特性Bを持つ抵抗体
8の材料に白金などの固定の温度特性を持った抵抗を用
いた場合であっても、抵抗体9と抵抗体10の抵抗値の
値を適切に選択することによって、合成抵抗値や温度係
数を白金の温度係数の範囲内で任意に設定することがで
きる。導体1と構造物2間の電圧をVi、導体1と中間
電極5の間に誘電率μ1の物質3によって形成される静
電容量のインピーダンスをZ1、温度特性Bを持つ抵抗
体8の抵抗値をR8、抵抗体9の抵抗値をR9、抵抗体
10の抵抗値をR10とすると、Z1=d÷(j×2×
π×f×μ1×S)、温度特性Bを持つ抵抗体8、抵抗
体9、抵抗体10の合成抵抗をRgとするとRg=R1
0×(R8+R9)÷(R8+R9+R10)、中間電
極5の電位をVmとすると、Vm=Rg÷(Z1+R
g)×Vi、出力電圧とするとVo=Vm×R9÷(R
8+R9)=Rg×R9÷((R8+R9)×(Z1+
Rg))×Vi、Rg≪Z1とすると、Vo=Vi×R
g×R9÷((R8+R9)×(Z1))=Vi×R1
0×(R8+R9)÷(R8+R9+R10)×R9÷
((R8+R9)×(Z1))=Vi×R10×R9÷
(R8+R9+R10)÷(Z1)となる。よって、温
度上昇によって、導体1と中間電極5の間に誘電率μ1
の物質3の静電容量が増大することによりインピーダン
スZ1が低下する場合、温度特性Bを持つ抵抗体8の抵
抗値R8が温度によって増大するため、出力電圧の変化
が低減される。
Next, the operation will be described. The combined resistance of the resistor network including the resistor 8, the resistor 9, and the resistor 10 having the temperature characteristic B is the same as that in the first embodiment.
This is intended to compensate for the change due to temperature in the electrostatic capacitance formed by the substance 3 having a dielectric constant μ1 sandwiched between the two. In the third embodiment shown in FIG. 3, for example, even when a resistor having a fixed temperature characteristic such as platinum is used as the material of the resistor 8 having the temperature characteristic B, the resistor 9 and the resistor 10 are used. By appropriately selecting the value of the resistance value of, the combined resistance value and the temperature coefficient can be arbitrarily set within the range of the temperature coefficient of platinum. The voltage between the conductor 1 and the structure 2 is Vi, the impedance of the capacitance formed by the substance 3 having a dielectric constant μ1 between the conductor 1 and the intermediate electrode 5 is Z1, and the resistance value of the resistor 8 having the temperature characteristic B. Is R8, the resistance value of the resistor 9 is R9, and the resistance value of the resistor 10 is R10, Z1 = d ÷ (j × 2 ×
π × f × μ1 × S), and the combined resistance of the resistor 8, resistor 9, and resistor 10 having the temperature characteristic B is Rg, Rg = R1
0 × (R8 + R9) ÷ (R8 + R9 + R10), where Vm is the potential of the intermediate electrode 5, Vm = Rg ÷ (Z1 + R
g) × Vi, where Vo = Vm × R9 ÷ (R
8 + R9) = Rg × R9 ÷ ((R8 + R9) × (Z1 +
If Rg)) × Vi and Rg << Z1, then Vo = Vi × R
g × R9 ÷ ((R8 + R9) × (Z1)) = Vi × R1
0 × (R8 + R9) ÷ (R8 + R9 + R10) × R9 ÷
((R8 + R9) × (Z1)) = Vi × R10 × R9 ÷
(R8 + R9 + R10) ÷ (Z1). Therefore, the dielectric constant μ1 between the conductor 1 and the intermediate electrode 5 is increased due to the temperature rise.
When the impedance Z1 decreases due to the increase in the capacitance of the substance 3, the resistance value R8 of the resistor 8 having the temperature characteristic B increases with temperature, and thus the change in the output voltage is reduced.

【0028】一方、図3の例では負の温度係数に対応し
ているが、温度特性Bを持つ抵抗体8と抵抗体9の位置
を入れ替えることで、正の温度係数にも対応可能であ
る。この場合の出力電圧は、Vo=Vi×R10×R8
÷(R8+R9+R10)÷(Z1)で表される。温度
上昇によって、導体1と中間電極5の間に誘電率μ1の
物質3の静電容量が低下することによりインピーダンス
Z1が増大する場合、分子のR8の値も増大し、インピ
ーダンスZ1の増大分がキャンセルされるため、温度の
影響を低減した電位検出器を実現できる。
On the other hand, although the example of FIG. 3 corresponds to a negative temperature coefficient, it is also possible to correspond to a positive temperature coefficient by exchanging the positions of the resistors 8 and 9 having the temperature characteristic B. . The output voltage in this case is Vo = Vi × R10 × R8
÷ (R8 + R9 + R10) ÷ (Z1) When the impedance Z1 increases due to the decrease in the capacitance of the substance 3 having a dielectric constant μ1 between the conductor 1 and the intermediate electrode 5 due to the temperature increase, the value of R8 of the molecule also increases, and the increase in impedance Z1 is Since it is canceled, a potential detector with reduced influence of temperature can be realized.

【0029】以上のように、本実施の形態においては、
上述の実施の形態1及び2で示した特定の温度特性Aを
有する抵抗体の代わりに、任意の温度特性を持たせるた
めに、所定の温度特性Bを有する抵抗体8と、温度特性
が安定な複数の抵抗体とを組み合わせた抵抗体の回路網
を設けるようにしたので、温度変化による影響を抑制
し、温度に対して安定な出力を得られる電位検出器を得
ることができる。
As described above, in the present embodiment,
Instead of the resistor having the specific temperature characteristic A shown in the first and second embodiments described above, the resistor 8 having a predetermined temperature characteristic B and the temperature characteristic are stable in order to have an arbitrary temperature characteristic. Since the resistor circuit network in which a plurality of resistors are combined is provided, it is possible to obtain the potential detector that can suppress the influence of the temperature change and obtain a stable output with respect to the temperature.

【0030】実施の形態4.図4はこの発明の実施の形
態4である電位検出器を示すもので、図4において、1
は導体、2は構造物、3は誘電率μ1の物質、5は中間
電極、8は温度特性Bを持つ抵抗体、9及び10は所定
の抵抗値を有し、温度特性が安定している抵抗体を示
す。図3の示す実施の形態3の例では、温度特性Bを持
つ抵抗体8として、白金から構成されたものを選択した
場合について説明したが、温度特性Bを持つ抵抗体8と
して、銅を採用しても良い。銅の抵抗温度係数は常温域
でおよそ0.4%/℃であり、白金と類似の温度特性が
得られるにも係らず、単価が安いため、安価な電位検出
器を実現できる特長がある。
Fourth Embodiment 4 shows a potential detector according to a fourth embodiment of the present invention. In FIG.
Is a conductor, 2 is a structure, 3 is a substance having a dielectric constant of μ1, 5 is an intermediate electrode, 8 is a resistor having a temperature characteristic B, 9 and 10 have a predetermined resistance value, and the temperature characteristic is stable. Indicates a resistor. In the example of the third embodiment shown in FIG. 3, although the case where the resistor 8 having the temperature characteristic B is made of platinum is described, copper is adopted as the resistor 8 having the temperature characteristic B. You may. The temperature coefficient of resistance of copper is about 0.4% / ° C. in the normal temperature range, and although the temperature characteristic similar to that of platinum can be obtained, the unit price is low, so that an inexpensive potential detector can be realized.

【0031】実施の形態5.図5はこの発明の実施の形
態5である電位検出器を示すもので、実施の形態3およ
び実施の形態4に示した温度特性Bを持つ抵抗体8、抵
抗体9、抵抗体10から成る抵抗網と並列に誘電率μ2
の物質4を中間電極5と構造物2の間に充填することに
よって、コンデンサを形成したものである。当該コンデ
ンサによって、電位検出器の出力に重畳するサージを抑
制し、サージの影響を受け難い電位検出器を実現でき
る。合せて、誘電率μ2の物質4は、中間電極5の支持
物、例えば支持碍子などの支持する機能をも兼用してい
るため、安価な電位検出器を実現できる特長がある。
Embodiment 5. FIG. 5 shows a potential detector according to a fifth embodiment of the present invention, which comprises a resistor 8, a resistor 9, and a resistor 10 having the temperature characteristic B shown in the third and fourth embodiments. Dielectric constant μ2 in parallel with resistor network
The substance 4 is filled between the intermediate electrode 5 and the structure 2 to form a capacitor. With the capacitor, a surge that is superimposed on the output of the potential detector can be suppressed, and a potential detector that is less susceptible to the surge can be realized. In addition, since the substance 4 having a dielectric constant μ2 also has a function of supporting the support of the intermediate electrode 5, for example, a support insulator, there is an advantage that an inexpensive potential detector can be realized.

【0032】実施の形態6.図6はこの発明の実施の形
態6である電位検出器を示すもので、実施の形態3およ
び実施の形態4に示した温度特性Bを持つ抵抗体8、抵
抗体9、抵抗体10から成る抵抗網と並列に、サージ吸
収用のコンデンサ11を取付けたものである。当該コン
デンサ11は、外付けのコンデンサであり、中間電極5
と構造物2の間に誘導する外来サージを抑制する。コン
デンサ11によってサージが抑制されるため、温度特性
Bを持つ抵抗体8、抵抗体9、抵抗体10の各抵抗素子
は、使用電圧、耐電圧の低いものを選択することができ
るため、安価な電位検出器を実現できる特長がある。
Sixth Embodiment FIG. 6 shows a potential detector according to a sixth embodiment of the present invention, which comprises a resistor 8, a resistor 9, and a resistor 10 having the temperature characteristic B shown in the third and fourth embodiments. A surge absorbing capacitor 11 is attached in parallel with the resistor network. The capacitor 11 is an external capacitor, and the intermediate electrode 5
The external surge induced between the structure and the structure 2 is suppressed. Since the surge is suppressed by the capacitor 11, each of the resistance elements having the temperature characteristic B, that is, the resistance element 8, the resistance element 9, and the resistance element 10 having low working voltage and withstand voltage can be selected. It has the feature of realizing a potential detector.

【0033】[0033]

【発明の効果】この発明は、電位の測定対象である導体
と、前記導体に対する基準電位を有する構造物と、前記
構造物と前記導体との間に設けられ、前記導体に印加さ
れた交流電圧を分圧する中間電極と、前記導体と前記中
間電極との間に設けられ、所定の誘電率μ1を有して、
所定の静電容量C1を形成する物質と、前記構造物と前
記中間電極との間に設けられ、前記静電容量C1の温度
変化を補償する特定の温度特性Aを有する抵抗手段とを
備えた電位検出器であるので、温度変化による影響を抑
制し、温度に対して安定な出力を得ることができる。
The present invention provides a conductor whose potential is to be measured, a structure having a reference potential with respect to the conductor, and an AC voltage applied to the conductor, which is provided between the structure and the conductor. Is provided between the conductor and the intermediate electrode, and has a predetermined dielectric constant μ1.
A substance that forms a predetermined capacitance C1 and a resistance means that is provided between the structure and the intermediate electrode and has a specific temperature characteristic A that compensates for a temperature change of the capacitance C1 are provided. Since it is a potential detector, it is possible to suppress the influence of temperature change and obtain a stable output with respect to temperature.

【0034】また、前記抵抗手段の両端の電圧を積分す
るための積分器をさらに備えているので、導体に印加さ
れた電圧に比例した出力電圧が得られるので、温度変化
による影響を抑制し、温度に対して安定な出力を得るこ
とができる。
Further, since the integrator for integrating the voltage across the resistance means is further provided, an output voltage proportional to the voltage applied to the conductor can be obtained, so that the influence of temperature change can be suppressed. It is possible to obtain a stable output with respect to temperature.

【0035】また、前記抵抗手段は、所定の温度特性B
を有する抵抗体と温度特性が安定な複数の抵抗体とを組
合せた抵抗網から構成され、前記抵抗網全体の温度特性
が前記温度特性Aと同等であるので、抵抗網を構成する
抵抗体の組み合わせを工夫することにより、任意の温度
特性を容易に持たせることができる。
The resistance means has a predetermined temperature characteristic B.
Of the resistors constituting the resistor network, since the resistor network having a plurality of resistors having stable temperature characteristics is combined, and the temperature characteristic of the entire resistor network is equivalent to the temperature characteristic A. By devising a combination, it is possible to easily have an arbitrary temperature characteristic.

【0036】また、前記特定の温度特性Bを有する抵抗
体は白金から構成されているので、確実に温度変化を補
償することができる。
Further, since the resistor having the specific temperature characteristic B is made of platinum, it is possible to reliably compensate the temperature change.

【0037】また、前記特定の温度特性Bを有する抵抗
体は銅から構成されているので、安価な電位検出器を得
ることができる。
Since the resistor having the specific temperature characteristic B is made of copper, an inexpensive potential detector can be obtained.

【0038】また、前記構造物と前記中間電極との間に
充填され、前記抵抗手段と並列回路を構成する誘電率μ
2の物質をさらに備えているので、電位検出器の出力に
重畳するサージを抑制し、サージの影響を受け難い電位
検出器を得ることができる。
A dielectric constant μ which is filled between the structure and the intermediate electrode and constitutes a parallel circuit with the resistance means.
Since the substance of No. 2 is further provided, it is possible to obtain a potential detector that suppresses a surge that is superimposed on the output of the potential detector and is not easily affected by the surge.

【0039】また、前記抵抗手段の両端にコンデンサを
さらに設けているので、中間電極と構造物の間に誘導す
る外来サージを抑制することができる。
Further, since capacitors are further provided at both ends of the resistance means, an external surge induced between the intermediate electrode and the structure can be suppressed.

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

【図1】 本発明の実施の形態1の電位検出器の構成図
である。
FIG. 1 is a configuration diagram of a potential detector according to a first embodiment of the present invention.

【図2】 本発明の実施の形態2の電位検出器の構成図
である。
FIG. 2 is a configuration diagram of a potential detector according to a second embodiment of the present invention.

【図3】 本発明の実施の形態3の電位検出器の構成図
である。
FIG. 3 is a configuration diagram of a potential detector according to a third embodiment of the present invention.

【図4】 本発明の実施の形態4の電位検出器の構成図
である。
FIG. 4 is a configuration diagram of a potential detector according to a fourth embodiment of the present invention.

【図5】 本発明の実施の形態5の電位検出器の構成図
である。
FIG. 5 is a configuration diagram of a potential detector according to a fifth embodiment of the present invention.

【図6】 本発明の実施の形態6の電位検出器の構成図
である。
FIG. 6 is a configuration diagram of a potential detector according to a sixth embodiment of the present invention.

【図7】 従来の分圧型PDの構成図である。FIG. 7 is a configuration diagram of a conventional partial pressure type PD.

【図8】 従来のガス絶縁電気機器用変圧器の構成図で
ある。
FIG. 8 is a block diagram of a conventional transformer for gas insulated electrical equipment.

【符号の説明】[Explanation of symbols]

1 導体、2 構造物、3 誘電率μ1の物質、4 誘
電率μ2の物質、5中間電極、6 温度特性Aの抵抗
体、7 積分器、8 温度特性Bの抵抗体、9抵抗体、
10 抵抗体、11 コンデンサ、101 接地容器、
101a フランジ、102 絶縁スペーサ、103
主回路導体、104 接地容器、104a フランジ、
105 段差部、106 接続口、107 密封端子、
108筒状部材、109 フランジ、110 フラン
ジ、111 二次電極、112貫通穴、113 絶縁部
材、114端部電極、115 締付ネジ、116 取り
付けネジ、117信号変換器、118 リード線。
DESCRIPTION OF SYMBOLS 1 conductor, 2 structure, 3 substance of permittivity μ1, 4 substance of permittivity μ2, 5 intermediate electrode, 6 resistor of temperature characteristic A, 7 integrator, 8 resistor of temperature characteristic B, 9 resistor,
10 resistor, 11 capacitor, 101 grounding container,
101a flange, 102 insulating spacer, 103
Main circuit conductor, 104 grounding container, 104a flange,
105 step, 106 connection port, 107 sealed terminal,
108 tubular member, 109 flange, 110 flange, 111 secondary electrode, 112 through hole, 113 insulating member, 114 end electrode, 115 tightening screw, 116 mounting screw, 117 signal converter, 118 lead wire.

Claims (7)

【特許請求の範囲】[Claims] 【請求項1】 電位の測定対象である導体と、 前記導体に対する基準電位を有する構造物と、 前記構造物と前記導体との間に設けられ、前記導体に印
加された交流電圧を分圧する中間電極と、 前記導体と前記中間電極との間に設けられ、所定の誘電
率μ1を有して、所定の静電容量C1を形成する物質
と、 前記構造物と前記中間電極との間に設けられ、前記静電
容量C1の温度変化を補償する所定の温度特性Aを有す
る抵抗手段とを備えたことを特徴とする電位検出器。
1. A conductor whose potential is to be measured, a structure having a reference potential with respect to the conductor, and an intermediate that is provided between the structure and the conductor and divides an AC voltage applied to the conductor. An electrode, a substance provided between the conductor and the intermediate electrode, having a predetermined dielectric constant μ1 and forming a predetermined capacitance C1, and provided between the structure and the intermediate electrode. And a resistance means having a predetermined temperature characteristic A for compensating the temperature change of the capacitance C1.
【請求項2】 前記抵抗手段の両端の電圧を積分するた
めの積分器をさらに備えたことを特徴とする請求項1に
記載の電位検出器。
2. The potential detector according to claim 1, further comprising an integrator for integrating the voltage across the resistance means.
【請求項3】 前記抵抗手段は、所定の温度特性Bを有
する抵抗体と温度特性が安定な複数の抵抗体とを組合せ
た抵抗網から構成され、前記抵抗網全体の温度特性が前
記温度特性Aと同等であることを特徴とする請求項1ま
たは2に記載の電位検出器。
3. The resistance means is composed of a resistor network in which a resistor having a predetermined temperature characteristic B and a plurality of resistors having stable temperature characteristics are combined, and the temperature characteristic of the entire resistor network is the temperature characteristic. It is equivalent to A, The potential detector of Claim 1 or 2 characterized by the above-mentioned.
【請求項4】 前記特定の温度特性Bを有する抵抗体は
白金から構成されていることを特徴とする請求項1ない
し3のいずれかに記載の電位検出器。
4. The potential detector according to claim 1, wherein the resistor having the specific temperature characteristic B is made of platinum.
【請求項5】 前記特定の温度特性Bを有する抵抗体は
銅から構成されていることを特徴とする請求項1ないし
3のいずれかに記載の電位検出器。
5. The potential detector according to claim 1, wherein the resistor having the specific temperature characteristic B is made of copper.
【請求項6】 前記構造物と前記中間電極との間に充填
され、前記抵抗手段と並列回路を構成する誘電率μ2の
物質をさらに備えたことを特徴とする請求項1ないし5
のいずれかに記載の電位検出器。
6. The method according to claim 1, further comprising a substance having a dielectric constant of μ2, which is filled between the structure and the intermediate electrode and forms a parallel circuit with the resistance means.
The potential detector according to any one of 1.
【請求項7】 前記抵抗手段の両端にコンデンサをさら
に設けたことを特徴とする請求項1ないし5のいずれか
に記載の電位検出器。
7. The potential detector according to claim 1, further comprising capacitors provided at both ends of the resistance means.
JP2001205278A 2001-07-05 2001-07-05 Potential detector Pending JP2003021657A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP2001205278A JP2003021657A (en) 2001-07-05 2001-07-05 Potential detector

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP2001205278A JP2003021657A (en) 2001-07-05 2001-07-05 Potential detector

Publications (1)

Publication Number Publication Date
JP2003021657A true JP2003021657A (en) 2003-01-24

Family

ID=19041618

Family Applications (1)

Application Number Title Priority Date Filing Date
JP2001205278A Pending JP2003021657A (en) 2001-07-05 2001-07-05 Potential detector

Country Status (1)

Country Link
JP (1) JP2003021657A (en)

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