JPH0113065B2 - - Google Patents
Info
- Publication number
- JPH0113065B2 JPH0113065B2 JP55056720A JP5672080A JPH0113065B2 JP H0113065 B2 JPH0113065 B2 JP H0113065B2 JP 55056720 A JP55056720 A JP 55056720A JP 5672080 A JP5672080 A JP 5672080A JP H0113065 B2 JPH0113065 B2 JP H0113065B2
- Authority
- JP
- Japan
- Prior art keywords
- circuit
- capacitor
- coaxial cable
- voltage
- resistor
- 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
Links
- 239000003990 capacitor Substances 0.000 claims description 23
- 238000005259 measurement Methods 0.000 claims description 10
- 239000004020 conductor Substances 0.000 claims description 8
- 238000010586 diagram Methods 0.000 description 2
- 230000000630 rising effect Effects 0.000 description 1
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01R—MEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
- G01R15/00—Details of measuring arrangements of the types provided for in groups G01R17/00 - G01R29/00, G01R33/00 - G01R33/26 or G01R35/00
- G01R15/04—Voltage dividers
- G01R15/06—Voltage dividers having reactive components, e.g. capacitive transformer
Description
【発明の詳細な説明】
本発明は分圧主回路、同軸ケーブル及び出力回
路とを備えて測定点よりブラウン管オシログラフ
装置等の測定器まで高電圧を低減して導く高電圧
測定用分圧回路に関するものである。DETAILED DESCRIPTION OF THE INVENTION The present invention provides a voltage dividing circuit for high voltage measurement, which comprises a voltage dividing main circuit, a coaxial cable, and an output circuit, and reduces and guides high voltage from a measuring point to a measuring device such as a cathode ray tube oscillography device. It is related to.
高電圧測定用分圧回路は、高電圧を測定する必
要上、高電圧が印加される分圧主回路と測定器に
つながれる出力回路とは離れた場所に置かれ、両
者は同軸ケーブルで結ばれている。 Because it is necessary to measure high voltage, the voltage divider circuit for high voltage measurement is placed in a separate location from the main voltage divider circuit to which high voltage is applied and the output circuit connected to the measuring instrument, and the two are connected by a coaxial cable. It is.
このため分圧主回路及び出力回路と同軸ケーブ
ルとのインピーダンスマツチングが必要とする。
同軸ケーブルの特性インピーダンスは50Ω〜75Ω
であるから、数KΩまでの低抵抗の分圧主回路及
び出力回路ではインピーダンスマツチングは容易
であるが、高抵抗又は高インピーダンスの容量分
圧型の分圧主回路ではインピーダンスマツチング
は困難である。 For this reason, impedance matching between the voltage dividing main circuit and output circuit and the coaxial cable is required.
The characteristic impedance of coaxial cable is 50Ω to 75Ω
Therefore, impedance matching is easy for voltage divider main circuits and output circuits with low resistance up to several kilohms, but impedance matching is difficult for capacitive voltage divider main circuits with high resistance or high impedance. .
容量分圧型の分圧主回路を備えた従来の高電圧
測定用分圧回路は、第1図に示すように容量が
C0、C1の分用の第1、第2のコンデンサ1,2
及び抵抗値が後述する同軸ケーブルの特性インピ
ーダンスZ0に等しい抵抗値Rに選定されているマ
ツチング用の第1の抵抗器3を備えた容量分圧型
の分圧主回路4と、特性インピーダンスがZ0の同
軸ケーブル5と、抵抗値がRのマツチング抵抗器
6及び容量がC2の第2のコンデンサ7とを備え
た出力回路8とにより構成されていて、高周波成
分のみインピーダンスマツチングを取つていた。 A conventional voltage divider circuit for high voltage measurement equipped with a capacitive voltage divider type main voltage divider circuit has a capacitance as shown in Figure 1.
First and second capacitors 1 and 2 for C 0 and C 1
and a capacitive voltage dividing main circuit 4 equipped with a first matching resistor 3 whose resistance value is selected to have a resistance value R equal to the characteristic impedance Z 0 of the coaxial cable, which will be described later; 0 coaxial cable 5, an output circuit 8 comprising a matching resistor 6 with a resistance value of R and a second capacitor 7 with a capacitance of C2 , and performs impedance matching only on high frequency components. was.
従つて、従来の高電圧測定用分圧回路では、低
周波成分のインピーダンスマツチングが行われて
いず、全体の周波数応答特性が平坦でなく、測定
範囲が限定される欠点があつた。 Therefore, in the conventional voltage divider circuit for high voltage measurement, impedance matching of low frequency components is not performed, the overall frequency response characteristic is not flat, and the measurement range is limited.
また、従来はインピーダンスマツチングがうま
く行えなかつたので、直流から高周波までの周波
数特性の優れた高電圧測定用分圧回路は存在しな
かつた。 Furthermore, because impedance matching has not been performed well in the past, there has been no voltage divider circuit for measuring high voltages with excellent frequency characteristics from direct current to high frequencies.
本発明の目的は、広帯域で高インピーダンスの
高電圧測定用分圧回路を提供するにある。 SUMMARY OF THE INVENTION An object of the present invention is to provide a wideband, high impedance voltage dividing circuit for high voltage measurement.
以下本発明の具体例を第2図を参照して詳細に
説明する。本実施例では、分圧主回路4及び同軸
ケーブル5は従来通りである。分圧主回路4は、
容量がC0、C1で直列接続され一端が接地された
分圧用の第1、第2のコンデンサ1,2と、抵抗
値が同軸ケーブル5の特性ピーダンスZ0に等しい
抵抗値Rに選定されていて両コンデンサ1,2の
分圧点に一端が接続された第1の抵抗器3とで構
成されている。同軸ケーブル5は、その中心導体
5aの一端に抵抗器3の他端が接続されている。
同軸ケーブル5の外部導体5bはコンデンサ2と
同様に接地されている。 Hereinafter, a specific example of the present invention will be explained in detail with reference to FIG. In this embodiment, the voltage dividing main circuit 4 and coaxial cable 5 are the same as before. The voltage dividing main circuit 4 is
First and second capacitors 1 and 2 are connected in series with capacitances C 0 and C 1 and one end is grounded, and the resistance value R is selected to be equal to the characteristic pedance Z 0 of the coaxial cable 5. and a first resistor 3 whose one end is connected to the voltage dividing point of both capacitors 1 and 2. The other end of the resistor 3 is connected to one end of the center conductor 5a of the coaxial cable 5.
The outer conductor 5b of the coaxial cable 5 is grounded similarly to the capacitor 2.
出力回路8は、抵抗値が(1−r)Rの第2の
抵抗器9と、抵抗値がrRの第3の抵抗器10と、
容量がC2の第2のコンデンサ7とが直列接続さ
れ、この直列回路の第2の抵抗器9側の端部が同
軸ケーブル5の中心導体5aの他端に接続され、
第2のコンデンサ7側の端部が接地され、第2、
第3の抵抗器9,10の分圧点Qが出力端子11
に接続され、第2のコンデンサ7のアース端が出
力端子12に接続されて構成されている。こゝ
で、r=2C1/C2である。 The output circuit 8 includes a second resistor 9 having a resistance value of (1-r)R, a third resistor 10 having a resistance value rR,
A second capacitor 7 having a capacitance of C2 is connected in series, and the end of this series circuit on the second resistor 9 side is connected to the other end of the center conductor 5a of the coaxial cable 5.
The end on the second capacitor 7 side is grounded, and the second capacitor 7 side is grounded.
The voltage dividing point Q of the third resistors 9 and 10 is the output terminal 11
The ground terminal of the second capacitor 7 is connected to the output terminal 12. Here, r=2C 1 /C 2 .
次にこのような高電圧測定用分圧回路が広帯域
の応答特性を有し、且つ同軸ケーブル5とのイン
ピーダンスマツチングが取られていることを説明
する。 Next, it will be explained that such a voltage dividing circuit for high voltage measurement has a wide band response characteristic and impedance matching with the coaxial cable 5 is achieved.
第2図において、コンデンサ2に電圧「1」の
ステツプ電圧がt=0に与えられたとすると、出
力電圧vはラプラス表示で表わして
v=r(S+2/ra2)/2a1a2∞
〓
〓k=0
〔a1a2/(S+a1)(S+a2)〕k+1e-2kST………(1
)
で与えられる。こゝで、
a1=1/2Z0C1、a2=1/2Z0C2、S=プラス演算子
である。さて、
2/r=a1/a2
となるようにrを選ぶと、(1)式は
vc=S+a1/a1 2 ∞
〓
〓k=0
〔a1a2/(S+a1)(S+a2)〕k+1e-2kST………(2
)
となる。こゝで
C1≪C2即ちa2≪a1
とすると、(2)式はほヾステツプ関数となる。この
ステツプ関数の電圧はt=0で
に分圧され、且つt=∞で
となる。こゝで、C3は同軸ケーブル5の静電容
量である。 In Fig. 2, if a step voltage of voltage "1" is applied to capacitor 2 at t=0, the output voltage v is expressed in Laplace notation as follows: v=r(S+2/ra 2 )/2a 1 a 2∞ 〓 〓 k=0 [a 1 a 2 / (S+a 1 ) (S+a 2 )] k+1 e -2kST ………(1
) is given by Here, a 1 = 1/2Z 0 C 1 , a 2 = 1/2Z 0 C 2 , and S = plus operator. Now, if we choose r so that 2/r=a 1 /a 2 , equation (1) becomes v c = S + a 1 / a 1 2 ∞ 〓 〓 k=0 [a 1 a 2 / (S + a 1 ) (S+a 2 )] k+1 e -2kST ………(2
) becomes. Here, if C 1 ≪C 2 , that is, a 2 ≪a 1 , then equation (2) becomes a step function. The voltage of this step function is t=0. and at t=∞ becomes. Here, C 3 is the capacitance of the coaxial cable 5.
上式は入力のステツプ関数に対してC1/C2倍
のステツプ関数の応答性が得られることを意味し
ている。このことはあらゆる周波数に対して同一
分圧比の出力が得られることを意味し、同軸ケー
ブル5のインピーダンスマツチングが取れている
ことを意味する。 The above equation means that a step function response of C 1 /C 2 times the input step function can be obtained. This means that an output with the same voltage division ratio can be obtained for all frequencies, and means that the impedance matching of the coaxial cable 5 is achieved.
実験例
第2図の回路において、C0=6.4pF、C1=1nF、
C2=64nF、R=50Ωとし、同軸ケーブル5は特
性インピーダンスZ0が50Ωのものを10m用いた。
r=2C1/C2=1/32と定め、且つコンデンサ1に
並列に500MΩ、コンデンサ2に並列に50KΩの
抵抗器をそれぞれつないで200KVシールド型分
圧回路を作成した。この分圧回路の入力に立上り
1nSのステツプ電圧を印加し、分圧された出力波
形を観測したところ、立上り5nSのステツプ電圧
が得られた。分圧比は1:104であつた。Experimental example In the circuit shown in Figure 2, C 0 = 6.4pF, C 1 = 1nF,
C 2 = 64 nF, R = 50 Ω, and a 10 m coaxial cable 5 with a characteristic impedance Z 0 of 50 Ω was used.
A 200KV shielded voltage divider circuit was created by setting r=2C 1 /C 2 =1/32 and connecting a 500MΩ resistor in parallel to capacitor 1 and a 50KΩ resistor in parallel to capacitor 2. The input rise of this voltage divider circuit
When a step voltage of 1 nS was applied and the divided output waveform was observed, a step voltage with a rising edge of 5 nS was obtained. The partial pressure ratio was 1: 104 .
また、直流、50Hz、1KHz、10MHz、100MHzの
周波数の電圧を測定し、分圧比が1:104である
ことを確認した。 We also measured voltages at frequencies of DC, 50Hz, 1KHz, 10MHz, and 100MHz, and confirmed that the voltage division ratio was 1: 104 .
以上説明したように本発明によれば、直流から
高周波までの広帯域の周波数応答特性がほゞ一様
で且つ高インピーダンスの高電圧測定用分圧回路
を提供することができる。 As explained above, according to the present invention, it is possible to provide a voltage dividing circuit for high voltage measurement that has substantially uniform frequency response characteristics over a wide band from direct current to high frequencies and has high impedance.
第1図は従来の分圧回路の結線図、第2図は本
発明に係る分圧回路の一実施例を示す結線図であ
る。
1,2……第1、第2のコンデンサ、3……第
1の抵抗器、4……分圧主回路、5……同軸ケー
ブル、5a……中心導体、5b……外部導体、7
……第3のコンデンサ、8……出力回路、9,1
0……第2、第3の抵抗器、11,12……出力
端子。
FIG. 1 is a wiring diagram of a conventional voltage dividing circuit, and FIG. 2 is a wiring diagram showing an embodiment of the voltage dividing circuit according to the present invention. 1, 2...First and second capacitors, 3...First resistor, 4...Voltage dividing main circuit, 5...Coaxial cable, 5a...Center conductor, 5b...Outer conductor, 7
...Third capacitor, 8...Output circuit, 9,1
0... Second and third resistors, 11, 12... Output terminals.
Claims (1)
続される出力回路とが同軸ケーブルで接続され、
前記分圧主回路は容量がC0の第1のコンデンサ
と容量がC1の第2のコンデンサと前記同軸ケー
ブルの特性インピーダンスに等しい抵抗値Rをも
つ第1の抵抗器とを含み、前記第1、第2のコン
デンサの直列接続により形成された直列回路の前
記第1のコンデンサ側に入力端子が設けられ、こ
の直列回路の前記第2のコンデンサ側が接地さ
れ、前記第1、第2のコンデンサの分圧点に前記
第1の抵抗器の一端が接続され、前記第1の抵抗
器の他端が前記同軸ケーブルの中心導体に接続さ
れて成り、前記同軸ケーブルの外部導体は接地さ
れている高電圧測定用分圧回路において、前記出
力回路は抵抗値が(1−r)R(たヾし、r=
2C1/C2)の第2の抵抗器と、抵抗値がrRの第3
の抵抗器と、容量がC2の第3のコンデンサとを
含み、前記第2、第3の抵抗器と前記第3のコン
デンサがこれらの順序で直列接続されて直列回路
が形成され、この直列回路における前記第2の抵
抗器側が前記同軸ケーブルの中心導体に接続さ
れ、この直列回路における前記第3のコンデンサ
側が接地され、前記第2、第3の抵抗器の分圧点
が出力端子に接続されて成つていることを特徴と
する高電圧測定用分圧回路。1 The main voltage dividing circuit to which high voltage is applied and the output circuit connected to the measuring instrument are connected by a coaxial cable,
The voltage dividing main circuit includes a first capacitor having a capacitance of C 0 , a second capacitor having a capacitance of C 1 , and a first resistor having a resistance value R equal to the characteristic impedance of the coaxial cable; 1. An input terminal is provided on the first capacitor side of a series circuit formed by connecting second capacitors in series, the second capacitor side of this series circuit is grounded, and the input terminal is connected to the first and second capacitors. One end of the first resistor is connected to a voltage dividing point, the other end of the first resistor is connected to the center conductor of the coaxial cable, and the outer conductor of the coaxial cable is grounded. In the voltage divider circuit for high voltage measurement, the output circuit has a resistance value of (1-r)R(t), where r=
2C 1 /C 2 ) and a third resistor with resistance rR.
and a third capacitor having a capacitance of C2 , the second and third resistors and the third capacitor are connected in series in this order to form a series circuit, and this series The second resistor side in the circuit is connected to the center conductor of the coaxial cable, the third capacitor side in this series circuit is grounded, and voltage dividing points of the second and third resistors are connected to an output terminal. A voltage divider circuit for high voltage measurement, characterized by comprising:
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP5672080A JPS56153257A (en) | 1980-04-28 | 1980-04-28 | Voltage dividing circuit for measurement of high voltage |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP5672080A JPS56153257A (en) | 1980-04-28 | 1980-04-28 | Voltage dividing circuit for measurement of high voltage |
Publications (2)
Publication Number | Publication Date |
---|---|
JPS56153257A JPS56153257A (en) | 1981-11-27 |
JPH0113065B2 true JPH0113065B2 (en) | 1989-03-03 |
Family
ID=13035318
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP5672080A Granted JPS56153257A (en) | 1980-04-28 | 1980-04-28 | Voltage dividing circuit for measurement of high voltage |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS56153257A (en) |
Families Citing this family (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS6382367A (en) * | 1986-09-26 | 1988-04-13 | Toshiba Corp | Fault locator for closed type switch gear |
US4935693A (en) * | 1987-10-14 | 1990-06-19 | Square D Company | Line secured current and voltage sensing apparatus |
US5252913A (en) * | 1987-10-14 | 1993-10-12 | Square D Company | Line sensor with corona shield |
-
1980
- 1980-04-28 JP JP5672080A patent/JPS56153257A/en active Granted
Also Published As
Publication number | Publication date |
---|---|
JPS56153257A (en) | 1981-11-27 |
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