JPH0252833B2 - - Google Patents

Info

Publication number
JPH0252833B2
JPH0252833B2 JP57007198A JP719882A JPH0252833B2 JP H0252833 B2 JPH0252833 B2 JP H0252833B2 JP 57007198 A JP57007198 A JP 57007198A JP 719882 A JP719882 A JP 719882A JP H0252833 B2 JPH0252833 B2 JP H0252833B2
Authority
JP
Japan
Prior art keywords
voltage
test piece
sine wave
digital
magnetomotive force
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
Application number
JP57007198A
Other languages
Japanese (ja)
Other versions
JPS58124975A (en
Inventor
Atsuo Kosukegawa
Kunihiko Takahashi
Masahiro Inoe
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.)
Japan Electric Meters Inspection Corp JEMIC
Original Assignee
Japan Electric Meters Inspection Corp JEMIC
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 Japan Electric Meters Inspection Corp JEMIC filed Critical Japan Electric Meters Inspection Corp JEMIC
Priority to JP719882A priority Critical patent/JPS58124975A/en
Publication of JPS58124975A publication Critical patent/JPS58124975A/en
Publication of JPH0252833B2 publication Critical patent/JPH0252833B2/ja
Granted legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01RMEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
    • G01R33/00Arrangements or instruments for measuring magnetic variables
    • G01R33/12Measuring magnetic properties of articles or specimens of solids or fluids
    • G01R33/123Measuring loss due to hysteresis

Landscapes

  • Physics & Mathematics (AREA)
  • Condensed Matter Physics & Semiconductors (AREA)
  • General Physics & Mathematics (AREA)
  • Measuring Magnetic Variables (AREA)

Description

【発明の詳細な説明】 本発明は鉄損測定装置、特に被試験片に交流の
起磁力を与え、それによつて被試験片に誘導され
る磁束と起磁力との積に基づいて、被試験片の鉄
損を測定する鉄損測定装置に関するものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention provides an iron loss measuring device, in particular, an iron loss measurement device that applies alternating current magnetomotive force to a test piece, and uses the product of the magnetic flux induced in the test piece and the magnetomotive force. This invention relates to an iron loss measuring device for measuring iron loss of a piece.

一般に交流で用いる磁性材料にあつては、鉄損
は発熱による温度上昇をもたらすため、機器設計
上からも常に鉄損測定は欠かせないもとなつてい
る。電磁機器に用いられる電気鉄板の鉄損測定は
一般にエプスタイン装置あるいは単板試験装置に
被試験片を挿入し、磁束正弦波を所定の値に設定
して行なうようにしている。
Generally speaking, in the case of magnetic materials used in alternating current, iron loss causes a rise in temperature due to heat generation, so iron loss measurement is always essential from the standpoint of equipment design. Iron loss measurements of electrical iron plates used in electromagnetic equipment are generally carried out by inserting a test piece into an Epstein apparatus or a single plate testing apparatus, and setting a magnetic flux sine wave to a predetermined value.

例えばエプスタイン装置では、第1図に示すよ
うに、試験片Cを正方形の窓孔が形成されるよう
に窓枠状に配置し、一方の相対向する試験片対に
励磁巻線W11,W12を、また他方の相対する試験
片対に励磁巻線W21,W22をそれぞれ巻装し、検
出巻線W21,W22から磁束φの時間微分に比例し
た電圧V〓を得る。この電圧V〓を周期T、周波数
f=1/T、で所定の絶体値を有する正弦波電圧と するために、励磁巻線W11、W12には制御用差動
増幅器2により、負帰還入力される電圧V〓が正
弦波発振器1の出力電圧に一致するのに必要な励
磁電流IHが流される。この励磁電流IHもしくはそ
れに比例する電流を電力計3の電流コイルWAに
流すと共に、この電力計の電流コイルWVに電圧
V〓を印加する。電流IHは起磁力Hと比例関係にあ
ることから、電力計3により励磁電流IHと電圧V〓
とから電力を求めれば、それは次式に従つて鉄損
Eを表わすもとなるのである。
For example, in the Epstein apparatus, as shown in FIG. 1, test pieces C are arranged in a window frame shape to form a square window hole, and excitation windings W 11 , W are attached to one pair of opposing test pieces. 12 and the other opposing pair of test pieces are wound with excitation windings W 21 and W 22 , respectively, and a voltage V〓 proportional to the time differential of the magnetic flux φ is obtained from the detection windings W 21 and W 22 . In order to make this voltage V〓 a sinusoidal voltage having a predetermined absolute value with a period T and a frequency f=1/T, the excitation windings W 11 and W 12 are connected to a control differential amplifier 2 with a negative An excitation current IH necessary for the feedback input voltage V= to match the output voltage of the sine wave oscillator 1 is caused to flow. This exciting current I H or a current proportional to it is passed through the current coil WA of the wattmeter 3, and a voltage is applied to the current coil WV of this wattmeter.
Apply V〓. Since the current I H is proportional to the magnetomotive force H, the wattmeter 3 calculates the excitation current I H and the voltage V〓
If we calculate the electric power from

E=1/T∫T OIH・V〓dt∝1/T∫T OHdφ/dtdt =f∫Hdφ ……(1) ところで、通常の鉄損測定の場合は低力率であ
つて、一般的な電流力計型の電力計では高精度な
測定結果は得られない。そのため種々の原理の高
精度乗算器を利用した電子式電力計が用いられて
いる。しかし、この種の電子式電力計を用いた鉄
損測定装置は高価になるのが欠点である。
E=1/T∫ T O I H・V〓dt∝1/T∫ T O Hdφ/dtdt = f∫Hdφ ...(1) By the way, in the case of normal iron loss measurement, the power factor is low, Highly accurate measurement results cannot be obtained with a general amperometric power meter. For this reason, electronic power meters are used that utilize high-precision multipliers based on various principles. However, a drawback of this type of iron loss measuring device using an electronic wattmeter is that it is expensive.

本発明の目的は上記欠点を除去し、高精度であ
りながら回路構成が簡単で安価に構成し得る鉄損
測定装置を提供することにある。
SUMMARY OF THE INVENTION An object of the present invention is to eliminate the above-mentioned drawbacks and provide an iron loss measuring device that is highly accurate, has a simple circuit configuration, and can be constructed at low cost.

この目的を達成するために本発明は、D−A変
換器を用いて起磁力を与えるための励磁電流を制
御すると共に、そのD−A変換器の入力デイジタ
ル信号と励磁電流信号とから乗算型D−A変換器
を用いて鉄損を求めるようにしたものである。
In order to achieve this object, the present invention uses a D-A converter to control an excitation current for giving a magnetomotive force, and uses a multiplication type from an input digital signal of the D-A converter and an excitation current signal. The iron loss is determined using a DA converter.

第2図は本発明の一実施例を示すもである。こ
の装置においては、発振器4の出力パルスをカウ
ンタ5が計数し、その計数値をアドレスとしてデ
イジタル記憶素子6が、予め記憶されていたデイ
ジタルデータを出力する。デイジタル記憶素子6
には正弦波の瞬時値が一周期分記憶されており、
その記憶データをD−A変換器7のデイジタル入
力とすることにより、発振器4のパルス周波数と
デイジタル記憶素子6のアドレス数とで決まる周
波数の正弦波アナログ電圧V〓を出力する。差動
増幅器2は、検出コイルW21,W22によつて検出
された被試験片Cの磁束φの時間微分値に相当す
る電圧V〓を帰還信号としてこれがD−A変換器
7の出力電圧V〓と一致するように動作する。差
動増幅器2から励磁巻線W11,W12に供給される
励磁電流IHは被試験片Cに加えられる起磁力Hに
比例するので、これを電流−電圧変換器8を介し
て電圧信号VHに変換して乗算型D−A変換器9
の一方の入力端に入力する。乗算型D−A変換器
9の他方の入力端子には、デイジタル記憶素子6
のデイジタルデータが電圧V〓の関数としてD−
A変換器7と同時に入力される。変換器9は両入
力の積に相当する電圧(または電流)信号Zを出
力する。したがつて、この信号Zを電圧計(また
は電流計)10で測定すると、その指示値は、
V〓=V〓の安定状態にあれば、 M∝1/T∫T OV〓・IHdt∝1/T∫T Odφ/dt・Hdt =f・Hdφ ……(2) となり、所期の鉄損を知ることができる。
FIG. 2 shows an embodiment of the present invention. In this device, a counter 5 counts the output pulses of an oscillator 4, and a digital storage element 6 outputs pre-stored digital data using the counted value as an address. Digital storage element 6
The instantaneous value of the sine wave is stored for one cycle,
By using the stored data as a digital input to the DA converter 7, a sine wave analog voltage V〓 of a frequency determined by the pulse frequency of the oscillator 4 and the number of addresses of the digital storage element 6 is outputted. The differential amplifier 2 uses the voltage V corresponding to the time differential value of the magnetic flux φ of the test piece C detected by the detection coils W 21 and W 22 as a feedback signal, and converts this into the output voltage of the D-A converter 7. It operates to match V〓. Since the excitation current I H supplied from the differential amplifier 2 to the excitation windings W 11 and W 12 is proportional to the magnetomotive force H applied to the test piece C, this is converted into a voltage signal via the current-voltage converter 8. Converting to V H and multiplying type D-A converter 9
input to one input end of the . A digital storage element 6 is connected to the other input terminal of the multiplication type DA converter 9.
The digital data of D- as a function of the voltage V〓
It is input simultaneously to the A converter 7. The converter 9 outputs a voltage (or current) signal Z corresponding to the product of both inputs. Therefore, when this signal Z is measured with a voltmeter (or ammeter) 10, the indicated value is:
If V〓=V〓, then M∝1/T∫ T O V〓・I H dt∝1/T∫ T O dφ/dt・Hdt = f・Hdφ ……(2), where You can know the iron loss of the period.

第3図は本発明を鉄損の単板試験に適用する場
合の実施例を示すものである。この装置では、励
磁コイルW1を巻装したコ字型の固定鉄心Sと、
磁束を正弦波波形にするための帰還用磁束検出コ
イルW2および磁束検出用検出コイルWDを巻装し
た被試験片Cとで閉じた磁路を構成するようにし
ている。検出コイルWDは被試験片Cに加えられ
る起磁力Hを検出するために設けられているもの
である。その場合、この検出コイルWDに誘起す
る電圧VHDは起磁力Hの時間微分に比例するとい
う事実が利用される。
FIG. 3 shows an embodiment in which the present invention is applied to a single plate test for iron loss. In this device, a U-shaped fixed iron core S around which an excitation coil W 1 is wound,
A closed magnetic path is constituted by the feedback magnetic flux detection coil W 2 for making the magnetic flux into a sinusoidal waveform and the test piece C around which the magnetic flux detection detection coil W D is wound. The detection coil W D is provided to detect the magnetomotive force H applied to the test piece C. In that case, the fact that the voltage V HD induced in this detection coil W D is proportional to the time differential of the magnetomotive force H is utilized.

第3図の装置においては、デイジタル記憶素子
6に記憶されている正弦波電圧に対して90℃位相
の遅れた電圧信号をデイジタル量で記憶している
第2のデイジタル記憶素子11が設けられてい
る。したがつて、共通のカウンタ5で同一アドレ
スのデータを呼出された結果として両デイジタル
記憶素子6,11の出力側に得られる正弦波信号
は互いに90℃位相がずれている。正弦波電圧信号
を時間積分したものは、もとの信号よりも90゜だ
け遅れており、その振幅はもとの信号に比例する
ことを考慮すれば、デイジタル記憶素子11から
出力されるデイジタル信号Dは結局、被試験片C
の磁束φに比例し、 D∝φ ……(3) と表わされる。乗算型D−A変換器9は、このデ
イジタル信号Dと磁界検出用検出コイルWDに誘
起された電圧VHDとの乗算を実行して出力するの
で、その出力Zを電圧計(または電流計)を通し
て平均値として読取ると、その指示値Mは、 M∝1/T∫T OD・VHDdt∝1/T∫T OdH/dtdt =f・φdH ……(4) となり、鉄損Eを知ることができる。
In the device shown in FIG. 3, a second digital storage element 11 is provided which stores in digital quantity a voltage signal whose phase is delayed by 90 degrees with respect to the sine wave voltage stored in the digital storage element 6. There is. Therefore, the sine wave signals obtained at the output sides of both digital storage elements 6, 11 as a result of reading data at the same address by the common counter 5 are out of phase with each other by 90 degrees. Considering that the time-integrated sinusoidal voltage signal lags the original signal by 90° and its amplitude is proportional to the original signal, the digital signal output from the digital storage element 11 After all, D is the test piece C
is proportional to the magnetic flux φ, and is expressed as D∝φ...(3). The multiplication type D-A converter 9 multiplies this digital signal D by the voltage V HD induced in the magnetic field detection detection coil W D and outputs the result, so the output Z is measured by a voltmeter (or ammeter). ), the indicated value M is M∝1/T∫ T O D・V HD dt∝1/T∫ T O dH/dtdt = f・φdH ……(4), and the iron loss You can know E.

以上述べた構成の本発明によれば、何ら複雑な
装置や回路を必要とせずに、極めて般的な安価な
電気回路素子のみを用いて広い周波数範囲で高精
度な鉄損測定が可能となる。
According to the present invention having the configuration described above, it is possible to measure iron loss with high accuracy over a wide frequency range using only extremely common and inexpensive electric circuit elements, without requiring any complicated equipment or circuits. .

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

第1図は従来の鉄損測定装置の構成を示すブロ
ツク図、第2図および第3図は本発明による鉄損
測定装置の異なる実施例を示すブロツク図であ
る。 1……正弦波発振器、2……差動増幅器、3…
…電力計、4……発振器、5……カウンタ、6,
11……デイジタル記憶素子、7……D−A変換
器、8……電流−電圧変換器、9……乗算型D−
A変換器、10……平均値指示型電圧計。
FIG. 1 is a block diagram showing the configuration of a conventional iron loss measuring device, and FIGS. 2 and 3 are block diagrams showing different embodiments of the iron loss measuring device according to the present invention. 1...Sine wave oscillator, 2...Differential amplifier, 3...
... Wattmeter, 4... Oscillator, 5... Counter, 6,
11...Digital storage element, 7...DA converter, 8...Current-voltage converter, 9...Multiplication type D-
A converter, 10...Average value indicating type voltmeter.

Claims (1)

【特許請求の範囲】 1 被試験片に交流の起磁力を与え、それによつ
て被試験片に誘導される磁束と前記起磁力との積
に基づいて、被試験片の鉄損を測定する鉄損測定
装置において、 交流の1周期にわたる正弦波瞬時値をデイジタ
ル正弦波信号として記憶しているデイジタル記憶
素子と、 このデイジタル記憶素子に記憶されているデイ
ジタル正弦波信号に基づいてアナログ正弦波交流
電圧を発生するD−A変換器と、 このD−A変換器の出力交流電圧を入力とし、
前記被試験片に誘導される磁束による電圧を帰還
信号とし、この帰還に係る電圧を前記D−A変換
器の出力交流電圧に一致させるような起磁力を前
記被試験片に与える差動増幅器と、 前記被試験片の磁束に対応する前記デイジタル
正弦波信号と前記起磁力に対応する電圧または電
流との乗算を行う乗算型D−A変換器と、 この乗算型D−A変換器の出力の平均値を求め
る回路装置と を備えたことを特徴とする鉄損測定装置。 2 前記起磁力に対応する電圧または電流を表わ
す信号として被試験片に起磁力を与えるための励
磁電流が用いられ、前記磁束に対応するデイジタ
ル正弦波信号として前記デイジタル記憶素子の出
力デイジタル電圧信号が用いられることを特徴と
する特許請求の範囲第1項記載の鉄損測定装置。 3 前記起磁力に対応する電圧または電流を表わ
す信号として被試験片の近傍に配置した磁界検出
用検出コイルの誘起電圧が用いられ、前記磁束に
対応するデイジタル正弦波信号として前記デイジ
タル記憶素子の記憶データに基づいて発生される
正弦波交流電圧よりも90°位相の遅れた正弦波交
流電圧に対応するデイジタル信号が用いられるこ
とを特徴とする特許請求の範囲第1項記載の鉄損
測定装置。
[Claims] 1. An iron test piece in which an alternating current magnetomotive force is applied to a test piece and the iron loss of the test piece is measured based on the product of the magnetic flux induced in the test piece and the magnetomotive force. A loss measuring device includes a digital storage element that stores the instantaneous value of a sine wave over one cycle of alternating current as a digital sine wave signal, and an analog sine wave AC voltage based on the digital sine wave signal stored in this digital storage element. A D-A converter that generates , and the output AC voltage of this D-A converter as input,
A differential amplifier that uses a voltage due to magnetic flux induced in the test piece as a feedback signal and applies a magnetomotive force to the test piece so as to make the feedback voltage match the output AC voltage of the D-A converter. , a multiplication type DA converter that multiplies the digital sine wave signal corresponding to the magnetic flux of the test piece by a voltage or current corresponding to the magnetomotive force; and an output of the multiplication type DA converter. An iron loss measuring device comprising: a circuit device for calculating an average value. 2. An excitation current for applying a magnetomotive force to the test piece is used as a signal representing a voltage or current corresponding to the magnetomotive force, and an output digital voltage signal of the digital storage element is used as a digital sine wave signal corresponding to the magnetic flux. An iron loss measuring device according to claim 1, which is used in the iron loss measuring device. 3. An induced voltage of a magnetic field detection detection coil placed near the test piece is used as a signal representing voltage or current corresponding to the magnetomotive force, and is stored in the digital storage element as a digital sine wave signal corresponding to the magnetic flux. 2. The iron loss measuring device according to claim 1, wherein a digital signal corresponding to a sine wave AC voltage whose phase is delayed by 90 degrees from a sine wave AC voltage generated based on the data is used.
JP719882A 1982-01-20 1982-01-20 Iron loss measuring device Granted JPS58124975A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP719882A JPS58124975A (en) 1982-01-20 1982-01-20 Iron loss measuring device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP719882A JPS58124975A (en) 1982-01-20 1982-01-20 Iron loss measuring device

Publications (2)

Publication Number Publication Date
JPS58124975A JPS58124975A (en) 1983-07-25
JPH0252833B2 true JPH0252833B2 (en) 1990-11-14

Family

ID=11659329

Family Applications (1)

Application Number Title Priority Date Filing Date
JP719882A Granted JPS58124975A (en) 1982-01-20 1982-01-20 Iron loss measuring device

Country Status (1)

Country Link
JP (1) JPS58124975A (en)

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN101865882B (en) * 2010-06-08 2012-06-06 中国人民解放军海军工程大学 Automatic measuring system for iron loss of magnetic material
JP6922260B2 (en) * 2017-03-03 2021-08-18 日本製鉄株式会社 Signal generator and signal generation method

Family Cites Families (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5165676A (en) * 1974-12-03 1976-06-07 Nippon Steel Corp HOJIRYOKUSOKUTEISOCHI
JPS5674666A (en) * 1979-11-26 1981-06-20 Nec Corp Voltage level generator

Also Published As

Publication number Publication date
JPS58124975A (en) 1983-07-25

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