JPH0352586B2 - - Google Patents
Info
- Publication number
- JPH0352586B2 JPH0352586B2 JP57205847A JP20584782A JPH0352586B2 JP H0352586 B2 JPH0352586 B2 JP H0352586B2 JP 57205847 A JP57205847 A JP 57205847A JP 20584782 A JP20584782 A JP 20584782A JP H0352586 B2 JPH0352586 B2 JP H0352586B2
- Authority
- JP
- Japan
- Prior art keywords
- current
- circuit
- loss
- sample
- measured
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Expired - Lifetime
Links
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01R—MEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
- G01R33/00—Arrangements or instruments for measuring magnetic variables
- G01R33/12—Measuring magnetic properties of articles or specimens of solids or fluids
- G01R33/123—Measuring loss due to hysteresis
Landscapes
- Physics & Mathematics (AREA)
- Condensed Matter Physics & Semiconductors (AREA)
- General Physics & Mathematics (AREA)
- Measuring Magnetic Variables (AREA)
- Investigating Or Analyzing Materials By The Use Of Magnetic Means (AREA)
Description
本発明は電気的損失測定方法に係り、特に被測
定試料の鉄損あるいは渦電流損を高精度で測定す
るのに好適な電気的損失測定方法に関するもので
ある。
電力ケーブルに隣接する鋼材あるいは電力ケー
ブルの金属シースなどは、電力ケーブルの導体に
電流を流すと、それによつて発生する磁速によつ
て渦電流が流れ、それに見合つた損失が発生す
る。これらの損失が大きいと、電力ケーブルの許
容電流が制限されることになる。したがつて、こ
れらの材料の鉄損、シース損等を精度よく測定す
ることは電力ケーブル設計上重要な課題である。
鉄損等の測定方法としては、従来、温度上昇法
や回路損失測定法がある。温度上昇法は、通電回
路に電流を流した後の試料の温度上昇を測定して
鉄損等を求めるようにするが、これは外気条件の
影響を受けやすく、温度測定点を多点とする必要
があるという欠点をもつている。また、回路損測
定法は通電回路に通電した状態で試料を設置した
ときと設置しないときとの通電回路の損失を求
め、両者の差から試料の損失を求めるものである
が、これには通電回路自体の損失が大きいため、
測定誤差が大きくなるという欠点がある。
本発明は上記に鑑みてなされたもので、その目
的とするところは、被測定試料の鉄損あるいは渦
電流損を簡単に、しかも、高精度で測定すること
ができる電気的損失測定方法を提供することにあ
る。
本発明の特徴は、相互リアクタと2台の変流器
とを挿入した通電回路を設け、この通電回路に交
流電流を流したときに発生する磁束を検出するサ
ーチコイルを設置し、このサーチコイルに上記相
互リアクタの2次回路に並列に接続した第1の可
変抵抗器と上記2台の変流器のうちの一方の変流
器の2次側に接続した第2の可変抵抗器とを直列
に接続し、上記通電回路の近傍に被測定試料を設
置しないときと設置したときの出力電圧の差と上
記2台の変流器のうちの他方の変流器の2次側電
流とを用いて上記被測定試料の鉄損あるいは渦電
流損を測定する方法において、前記通電回路の近
傍に被測定試料を設置しないときの前記サーチコ
イルに前記第1,2の可変抵抗器を直列に接続し
た回路の出力電圧が零となるように前記第1,2
の可変抵抗器を調整しておく点にある。
一般に、交流損失は、通電回路の電圧降下と通
電電流の内積として求められ、この近傍に設置し
た鋼材等の鉄損もその一部として計測される。
ところで、全電圧降下は、鉄損に関係する電圧
と鉄損に関係しない電圧の和となつているので、
鉄損に関係しない電圧を別の回路を付加すること
により相殺し、実質上零とすれば、該全電圧降下
を鉄損に関係する電圧成分のみにでき、これから
求められる交流損失を鉄損として計測できる様に
なり、精度の良い鉄損測定回路(手段)を実現で
きる。
以下本発明の方法の一実施例を図を用いて詳細
に説明する。
図は本発明の測定方法の一実施例を説明するた
めの測定装置の一例を示す回路図で、単相測定の
例を示してある。まず、2本の導体1を布設し、
2本の導体1の片端は短絡し、他端間に通電用ト
ランス2を接続して通電回路を構成する。
次いで導体1の外周に電圧リード線(絶縁線)
3を一定ピツチでスパイラル状に巻回し、通電回
路に通電したときに発生する磁束のうち適当な部
分だけの磁束を検出するサーチコイルとする。ま
た上記通電回路に相互リアクタ4および変流器
5,6を挿入し、相互リアクタ4の2次回路に並
列に接続した可変抵抗器7と変流器5の2次側に
標準抵抗器8とともに並列に接続した可変抵抗器
9とをそれぞれ電圧リード線3に直列に接続し、
この回路の出力電圧はパワーメーター10に入力
する。
一方、通電回路の通電電流は変流器6を介して
パワーメーター10に入力する。
次に、測定方法について説明する。通電トラン
ス2より通電回路に電流Iを流し、電圧リード線
3及び可変抵抗器7,9の回路からパワーメータ
10に入力する入力電圧Vが零になるように可変
抵抗器7,9を調整する。このときの入力電圧V
の監視はオシロスコープ11を用いて行う。この
場合、パワーメータ10の出力は零となる。この
状態で被測定試料12を電圧リード線3の近傍の
所定位置に設置し、そのときのパワーメータ10
の出力から被測定試料12の渦電流損(または鉄
損)を測定する。
上記した本発明に係る測定方法によれば、被測
定試料12の渦電流損あるいは鉄損を簡単に、し
かも、高精度で測定することができる。また、パ
ワーメータ10の前段に高精度増幅器を設置すれ
ば微小の損失でも測定可能となる。
第1表は被測定試料12が75×40×900(単位
mm)の溝形鋼で、通電電流2000A(周波数50Hz)、
被測定試料12の通電導体よりの距離80mmのとき
の従来の回路損測定法と本発明に係る測定方法の
場合の測定結果の比較を示したものである。
The present invention relates to an electrical loss measuring method, and particularly to an electrical loss measuring method suitable for measuring iron loss or eddy current loss of a sample to be measured with high accuracy. When current is passed through the conductor of the power cable, eddy currents flow in the steel material adjacent to the power cable or the metal sheath of the power cable due to the magnetic velocity generated by the current, and a commensurate loss occurs. If these losses are large, the allowable current of the power cable will be limited. Therefore, accurately measuring the core loss, sheath loss, etc. of these materials is an important issue in power cable design. Conventional methods for measuring iron loss and the like include a temperature rise method and a circuit loss measurement method. The temperature rise method measures the temperature rise of the sample after passing a current through the current-carrying circuit to determine iron loss, etc. However, this method is easily affected by outside air conditions and requires multiple temperature measurement points. It has the disadvantage of being necessary. In addition, the circuit loss measurement method calculates the loss in the current-carrying circuit when the sample is installed and when the sample is not installed with the current flowing in the circuit, and calculates the loss of the sample from the difference between the two. Since the loss of the circuit itself is large,
The disadvantage is that the measurement error increases. The present invention has been made in view of the above, and its purpose is to provide an electrical loss measuring method that can easily and highly accurately measure the iron loss or eddy current loss of a sample to be measured. It's about doing. The present invention is characterized by providing a current carrying circuit in which a mutual reactor and two current transformers are inserted, and installing a search coil that detects the magnetic flux generated when alternating current is passed through this current carrying circuit. a first variable resistor connected in parallel to the secondary circuit of the mutual reactor and a second variable resistor connected to the secondary side of one of the two current transformers. The difference in output voltage when the sample to be measured is not installed in the vicinity of the current-carrying circuit and when it is installed in the vicinity of the current-carrying circuit and the secondary current of the other current transformer among the two current transformers described above are calculated as follows: In the method for measuring the iron loss or eddy current loss of the sample to be measured using the method, the first and second variable resistors are connected in series to the search coil when the sample to be measured is not installed near the energized circuit. the first and second circuits so that the output voltage of the circuit becomes zero.
The point is to adjust the variable resistor. Generally, alternating current loss is determined as the inner product of the voltage drop in a current-carrying circuit and the current flowing, and the iron loss of steel materials installed in the vicinity is also measured as part of the calculation. By the way, the total voltage drop is the sum of the voltage related to iron loss and the voltage not related to iron loss, so
If the voltage unrelated to iron loss is offset by adding another circuit and made virtually zero, the total voltage drop can be made into only the voltage component related to iron loss, and the AC loss calculated from this can be expressed as iron loss. It becomes possible to measure iron loss, and a highly accurate iron loss measurement circuit (means) can be realized. An embodiment of the method of the present invention will be described in detail below with reference to the drawings. The figure is a circuit diagram showing an example of a measuring device for explaining an embodiment of the measuring method of the present invention, and shows an example of single-phase measurement. First, two conductors 1 are laid,
One end of the two conductors 1 is short-circuited, and a current-carrying transformer 2 is connected between the other ends to form a current-carrying circuit. Next, connect the voltage lead wire (insulated wire) to the outer circumference of conductor 1.
3 is spirally wound at a constant pitch to form a search coil that detects only a suitable portion of the magnetic flux generated when the current is applied to the current-carrying circuit. In addition, a mutual reactor 4 and current transformers 5 and 6 are inserted into the above-mentioned energizing circuit, and a variable resistor 7 connected in parallel to the secondary circuit of the mutual reactor 4 and a standard resistor 8 are connected to the secondary side of the current transformer 5. The variable resistors 9 connected in parallel are each connected in series to the voltage lead wire 3,
The output voltage of this circuit is input to a power meter 10. On the other hand, the energizing current of the energizing circuit is input to the power meter 10 via the current transformer 6. Next, the measurement method will be explained. A current I is passed through the current carrying circuit from the current carrying transformer 2, and the variable resistors 7 and 9 are adjusted so that the input voltage V input to the power meter 10 from the voltage lead wire 3 and the circuit of the variable resistors 7 and 9 becomes zero. . Input voltage V at this time
Monitoring is performed using an oscilloscope 11. In this case, the output of the power meter 10 becomes zero. In this state, the sample to be measured 12 is installed at a predetermined position near the voltage lead wire 3, and the power meter 10 at that time is
The eddy current loss (or iron loss) of the sample to be measured 12 is measured from the output. According to the above-described measuring method according to the present invention, the eddy current loss or iron loss of the sample to be measured 12 can be easily measured with high accuracy. Moreover, if a high-precision amplifier is installed before the power meter 10, even minute losses can be measured. Table 1 shows that the sample to be measured 12 is 75 x 40 x 900 (unit:
mm) channel steel, carrying current 2000A (frequency 50Hz),
This figure shows a comparison of measurement results between the conventional circuit loss measurement method and the measurement method according to the present invention when the distance from the current-carrying conductor of the sample 12 to be measured is 80 mm.
【表】
試料なしの場合のデータ。
第1表の結果より、上記した本発明に係る測定
方法によれば、従来の回路損測定法の場合よりも
誤差が大幅に小さくなり、高精度の測定が可能で
あることがわかる。
なお、上記した例では、鉄損の測定結果を示し
てあるが、シース損(渦電流損)などの測定につ
いても同様であることはいうまでもない。
以上説明したように、本発明によれば、被測定
試料の鉄損あるいは渦電流損を簡単に、しかも、
高精度で測定できるという効果がある。[Table] Data without sample.
From the results in Table 1, it can be seen that according to the measurement method according to the present invention described above, the error is significantly smaller than in the conventional circuit loss measurement method, and highly accurate measurement is possible. In addition, although the above-mentioned example shows the measurement results of iron loss, it goes without saying that the same applies to measurements of sheath loss (eddy current loss) and the like. As explained above, according to the present invention, iron loss or eddy current loss of a sample to be measured can be easily measured.
This has the effect of being able to measure with high precision.
図は本発明の電気的損失測定方法の一実施例を
説明するための測定装置の一例を示す回路図であ
る。
1:導体、2:通電用トランス、3:電圧リー
ド線(サーチコイル)、4:相互リアクタ、5,
6:変流器、7,9:可変抵抗器、10:パワー
メータ、12:被測定試料。
The figure is a circuit diagram showing an example of a measuring device for explaining an embodiment of the electrical loss measuring method of the present invention. 1: Conductor, 2: Current transformer, 3: Voltage lead wire (search coil), 4: Mutual reactor, 5,
6: Current transformer, 7, 9: Variable resistor, 10: Power meter, 12: Sample to be measured.
Claims (1)
電回路を設け、該通電回路に交流電流を流したと
きに発生する磁束を検出するサーチコイルを設置
し、該サーチコイルに前記相互リアクタの2次回
路に並列に接続した第1の可変抵抗器と前記2台
の変流器のうちの一方の変流器の2次側に接続し
た第2の可変抵抗器とを直列に接続し、前記通電
回路の近傍に被測定試料を設置しないときと設置
したときの出力電圧の差と前記2台の変流器のう
ちの他方の変流器の2次側電流とを用いて前記被
測定試料の鉄損あるいは渦電流損を測定する方法
において、前記通電回路の近傍に被測定試料を設
置しないときの前記サーチコイルに前記第1,2
の可変抵抗器を直列に接続した回路の出力電圧が
零となるように前記第1,2の可変抵抗器を調整
しておくことを特徴とする電気的損失測定方法。1 An energizing circuit in which a mutual reactor and two current transformers are inserted is provided, a search coil is installed to detect the magnetic flux generated when an alternating current is passed through the energizing circuit, and the search coil is connected to the mutual reactor. A first variable resistor connected in parallel to the secondary circuit and a second variable resistor connected to the secondary side of one of the two current transformers are connected in series, The measurement target is measured using the difference in output voltage when the measurement target is not installed near the energized circuit and when the measurement target is installed in the vicinity of the current-carrying circuit, and the secondary current of the other current transformer of the two current transformers. In the method for measuring iron loss or eddy current loss of a sample, the first and second search coils are used when the sample to be measured is not installed near the energized circuit.
An electrical loss measuring method characterized in that the first and second variable resistors are adjusted so that the output voltage of a circuit in which the variable resistors are connected in series becomes zero.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP20584782A JPS5995481A (en) | 1982-11-24 | 1982-11-24 | Electrical loss measurement method |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP20584782A JPS5995481A (en) | 1982-11-24 | 1982-11-24 | Electrical loss measurement method |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5995481A JPS5995481A (en) | 1984-06-01 |
| JPH0352586B2 true JPH0352586B2 (en) | 1991-08-12 |
Family
ID=16513692
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP20584782A Granted JPS5995481A (en) | 1982-11-24 | 1982-11-24 | Electrical loss measurement method |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS5995481A (en) |
Family Cites Families (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS55121162A (en) * | 1979-03-13 | 1980-09-18 | Hitachi Cable Ltd | Measuring method of iron loss and so on |
-
1982
- 1982-11-24 JP JP20584782A patent/JPS5995481A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5995481A (en) | 1984-06-01 |
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