JPH07111217A - Method of estimating noise level of transformer - Google Patents
Method of estimating noise level of transformerInfo
- Publication number
- JPH07111217A JPH07111217A JP5223994A JP5223994A JPH07111217A JP H07111217 A JPH07111217 A JP H07111217A JP 5223994 A JP5223994 A JP 5223994A JP 5223994 A JP5223994 A JP 5223994A JP H07111217 A JPH07111217 A JP H07111217A
- Authority
- JP
- Japan
- Prior art keywords
- magnetostriction
- transformer
- sound pressure
- noise
- frequency
- 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.)
- Granted
Links
Landscapes
- Regulation Of General Use Transformers (AREA)
Abstract
Description
【0001】[0001]
【産業上の利用分野】本発明は産業上で電力、配電用変
圧器に用いられる騒音レベル予測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 noise level predicting method used industrially for power and distribution transformers.
【0002】[0002]
【従来の技術】電気、電子機器に幅広く使用される磁性
材料において、励磁した場合の長さ変化は一つの材料特
性であり、また品質管理における評価項目の一つであ
る。励磁前後の長さ比を磁気ひずみと呼んでいる。磁気
ひずみは変圧器騒音の原因の一つである。他に変圧器騒
音の一因として電磁力があるが、鋼板間のギャップ、巻
線の緩み等にみられる変圧器の製造法に起因するものな
ので、本件ではこれらの条件を一定とした場合における
磁性材料の影響を検討することとした。2. Description of the Related Art In magnetic materials widely used in electric and electronic devices, the change in length when excited is one of the material characteristics and one of the evaluation items in quality control. The length ratio before and after excitation is called magnetostriction. Magnetostriction is one of the causes of transformer noise. Another cause of transformer noise is electromagnetic force, but this is due to the transformer manufacturing method, which can be seen in the gaps between steel sheets, loose windings, etc. We decided to study the effect of magnetic materials.
【0003】従来、磁性材料の磁気ひずみ測定法として
ストレインゲージを用いる方法、差動トランスを用いる
方法、近年ではレーザードップラー振動計を用いる方法
がある。ストレインゲージ法では材料にストレインゲー
ジという5mm程のセンサーを装着し、その長さ変化を電
気信号に変換して磁気ひずみを測定する。差動トランス
法では磁気ひずみによる振動を振動伝達治具によって差
動トランスまで伝達し、電気信号に変換し測定する。従
来法では商用周波数以上の高い周波数において磁気ひず
みによる振動速度が速くなるため測定が困難であった。Conventionally, there are a method using a strain gauge, a method using a differential transformer, and a method using a laser Doppler vibrometer in recent years as a method for measuring magnetostriction of a magnetic material. In the strain gauge method, a strain gauge of about 5 mm is attached to the material, and the change in length is converted into an electric signal to measure magnetostriction. In the differential transformer method, vibration due to magnetostriction is transmitted to a differential transformer by a vibration transmission jig and converted into an electrical signal for measurement. In the conventional method, the measurement was difficult because the vibration speed due to magnetostriction was high at frequencies higher than the commercial frequency.
【0004】近年、電子回路による制御機器が発展し、
高調波を含んだ励磁電流が変圧器に流れ、また高磁束密
度設計の変圧器ではひずみ波による高調波が発生するの
で、変圧器からくる騒音も同様に高調波成分を含んでい
る。この高調波は励磁周波数の高い磁気ひずみから生ず
るものである。In recent years, control devices using electronic circuits have been developed,
Excitation current containing harmonics flows through the transformer, and harmonics due to distorted waves are generated in transformers with a high magnetic flux density design, so noise from the transformer also contains harmonic components. This harmonic is caused by magnetostriction with a high excitation frequency.
【0005】従来の磁気ひずみの評価は商用周波数にお
ける磁束密度を磁性材料に加えることで行っていた。こ
の値が大きい場合、騒音が大きいと予測される。しかし
ながら、磁性材料中には高磁束密度になればなるほど歪
んだ磁束が流れ、商用周波数励磁のみの測定では実際の
状態を知ることが困難である。また、商用周波数以上で
使用される変圧器では使用周波数の磁気ひずみのデータ
が少なく、組み上げた変圧器の騒音を測定しなければ評
価できない。Conventional evaluation of magnetostriction has been carried out by adding a magnetic flux density at a commercial frequency to a magnetic material. If this value is large, noise is predicted to be large. However, the higher the magnetic flux density is, the more distorted magnetic flux flows in the magnetic material, and it is difficult to know the actual state by measuring only commercial frequency excitation. Also, for transformers used at commercial frequencies and above, there is little data on magnetostriction at the frequencies used, and evaluation cannot be done without measuring the noise of the assembled transformer.
【0006】更に、励磁波形を制御したパルス励磁等は
多くの高調波を含有しており、この環境下で使用される
変圧器においては高調波を含んだ磁気ひずみのデータが
少ないという理由で、実際組み上げられた変圧器の騒音
を測定しなければ騒音の評価ができない。Further, pulse excitation or the like in which the excitation waveform is controlled contains many harmonics, and the transformer used in this environment has a small amount of magnetostrictive data including harmonics. The noise cannot be evaluated unless the noise of the assembled transformer is measured.
【0007】以上に述べたように、磁気ひずみの測定は
産業上における磁性材料の基本的に重要な品質評価項目
であるが、従来は高調波成分の磁気ひずみ評価は行われ
ていなかった。また、商用周波数以上の高い周波数で使
われる変圧器の騒音の評価は困難であった。As described above, the measurement of magnetostriction is a fundamentally important quality evaluation item for magnetic materials in industry, but the magnetostriction evaluation of harmonic components has not been conventionally performed. In addition, it was difficult to evaluate the noise of transformers used at higher frequencies than commercial frequencies.
【0008】[0008]
【発明が解決しようとする課題】本発明の課題は、変圧
器用磁性材料の磁気ひずみデータに基いて、該磁性材料
を用いて構成された変圧器の騒音レベルを予測すること
である。また、本発明は、任意波形励磁の磁気ひずみ波
形を周波数分析し、この大きさを音圧に変換し、聴感補
正を行う変圧器の騒音レベル予測方法を提供する。An object of the present invention is to predict the noise level of a transformer constructed using the magnetic material based on the magnetostriction data of the magnetic material for the transformer. The present invention also provides a noise level prediction method for a transformer that performs frequency analysis on a magnetostrictive waveform of arbitrary waveform excitation, converts the magnitude into sound pressure, and performs auditory correction.
【0009】[0009]
【課題を解決するための手段】本発明の第1の要旨は、
変圧器用磁性材料の磁気ひずみを可聴周波数範囲で測定
し、得られた磁気ひずみを音圧に変換し、さらに聴感補
正を施すことを特徴とする変圧器の騒音レベル予測方法
にある。The first gist of the present invention is as follows.
A method of predicting a noise level of a transformer is characterized in that the magnetostriction of a magnetic material for a transformer is measured in an audible frequency range, the obtained magnetostriction is converted into a sound pressure, and then the audibility is corrected.
【0010】また、本発明の第2の要旨は、任意の波形
で励磁された変圧器用磁性材料の磁気ひずみ波形を周波
数分析し、各周波数における磁気ひずみを音圧に変換
し、さらに聴感補正を施すことを特徴とする変圧器の騒
音レベル予測方法にある。The second gist of the present invention is to perform a frequency analysis on the magnetostrictive waveform of the magnetic material for a transformer excited by an arbitrary waveform, convert the magnetostriction at each frequency into sound pressure, and further perform auditory correction. It is a method of predicting noise level of a transformer, which is characterized by applying it.
【0011】従来の磁気ひずみ評価法を改善するため、
レーザードップラー振動計を用いた磁気ひずみ測定装置
を利用する。この装置は従来使われている差動トランス
法と比べ、高い周波数励磁の磁気ひずみを測定できる。
この装置を用い、50Hzから2kHz までの磁気ひずみを
測定する。得られた磁気ひずみを時間微分し、変位速度
vを計算する。ここで、磁気ひずみにより生じる変位が
同じ変位速度vで周りの空気粒子を移動させるとする。
変位速度に音圧を表す式を適用し、磁気ひずみを音圧で
表す。ここで用いる式を次に示す。 p=ρcv ここでp:音圧、ρ:媒質の密度、c:音の速度、v:
空気粒子の速度(磁気ひずみの変位速度)とする。空気
中ではρc=413(Kg/m2 s )である。これに聴感補
正を施し、磁気ひずみから得られたA特性の音圧レベル
(JEM−1117;変圧器の騒音レベル測定方法)と
する。In order to improve the conventional magnetostrictive evaluation method,
A magnetostriction measuring device using a laser Doppler vibrometer is used. This device can measure the magnetostriction of high frequency excitation as compared with the differential transformer method used conventionally.
This device is used to measure magnetostriction from 50Hz to 2kHz. The obtained magnetostriction is time-differentiated to calculate the displacement velocity v. Here, it is assumed that the surrounding air particles are moved at the same displacement velocity v that is caused by magnetostriction.
Applying the formula expressing sound pressure to the displacement velocity, the magnetostriction is expressed by sound pressure. The formula used here is shown below. p = ρcv where p: sound pressure, ρ: density of medium, c: speed of sound, v:
The velocity of air particles (magnetostrictive displacement velocity). In air, ρc = 413 (Kg / m 2 s). This is audibly corrected to obtain a sound pressure level of A characteristic obtained from magnetostriction (JEM-1117; method of measuring noise level of transformer).
【0012】[0012]
【作用】この手法により従来において明確な知見として
得られなかった商用周波数から2kHz までの磁気ひずみ
が測定できる。これはレーザードップラー振動計を用い
ることで高い周波数の磁気ひずみ振動でも測定可能にな
ったからである。[Function] By this method, magnetostriction from commercial frequency up to 2 kHz, which has not been obtained as clear knowledge in the past, can be measured. This is because it is possible to measure even high-frequency magnetostrictive vibration by using the laser Doppler vibrometer.
【0013】さらに聴感補正を行うことで、実際人間の
耳で感じられる音圧(騒音)を予測でき、従来では磁気
ひずみと騒音の相関を見い出し難かったが、高調波成分
の磁気ひずみを考慮に入れることで更に実際の騒音に近
づいた騒音予測ができる。Further, the sound pressure (noise) actually perceived by the human ear can be predicted by performing the auditory sense correction, and it has been difficult to find the correlation between the magnetostriction and the noise in the past. By inserting it, it is possible to predict the noise closer to the actual noise.
【0014】上記の理由から、変圧器を製造することな
く、変圧器用磁性材料の磁気ひずみを測定することだけ
で、該磁性材料を用いて構成された変圧器の騒音レベル
を予測可能となる。For the above reasons, it is possible to predict the noise level of a transformer constructed using the magnetic material only by measuring the magnetostriction of the magnetic material for the transformer without manufacturing the transformer.
【0015】[0015]
〔実施例1〕図1は各励磁周波数において、磁気ひずみ
を測定した例である。高い周波数では磁気ひずみが小さ
くなることがわかる。[Embodiment 1] FIG. 1 shows an example of measuring magnetostriction at each excitation frequency. It can be seen that the magnetostriction decreases at high frequencies.
【0016】例として、グレード(JIS)がG13と
G9Hの電磁鋼板を測定した。高い周波数においてグレ
ードが高いG9Hではグレードの低いG13と比較し磁
気ひずみが小さくなっている。更に磁気ひずみを音圧に
変換し、聴感補正を施し、A特性の音圧に変換すると、
図2に示す曲線になる。周波数の高い領域(1〜2kHz
)ではG13が大きな音圧を示し、ひずみ波形が重畳
した磁界中では大きな騒音が生じると容易に予測され
る。As an example, electromagnetic steel sheets of grade (JIS) G13 and G9H were measured. At high frequencies, G9H having a high grade has a smaller magnetostriction than G13 having a low grade. Furthermore, when the magnetostriction is converted into sound pressure, the audibility correction is applied, and the sound pressure is converted into the A characteristic,
It becomes the curve shown in FIG. High frequency range (1-2kHz
), G13 shows a large sound pressure, and it is easily predicted that a large noise is generated in the magnetic field on which the distorted waveform is superimposed.
【0017】〔実施例2〕図3、4は50Hz、60Hzの
周波数において、正弦波励磁で磁気ひずみを測定した例
を示す。励磁波形は任意で、使用状態に合わせたもので
もよい。磁気ひずみは周波数分析により、FFTの波形
分析プログラムで各周波数成分を求めた。直接スペクト
ラムアナライザーで周波数成分を求めてもよい。上記の
操作を施し、各周波数における音圧を求め、これを聴感
補正する。基本波よりも高調波のほうが音圧として高い
ことがわかる。[Embodiment 2] FIGS. 3 and 4 show examples in which magnetostriction was measured by sinusoidal excitation at frequencies of 50 Hz and 60 Hz. The excitation waveform is arbitrary and may be one that matches the usage condition. The magnetostriction was obtained by frequency analysis, and each frequency component was obtained by an FFT waveform analysis program. The frequency component may be directly obtained by a spectrum analyzer. The sound pressure at each frequency is obtained by performing the above operation, and the audibility is corrected. It can be seen that the harmonics have higher sound pressure than the fundamental wave.
【0018】例として、グレード(JIS)が27G1
30と27P95の電磁鋼板を測定した。高い周波数に
おいてグレードが高い27P95ではグレードの低い2
7G130と比較して全体的に音圧が小さい。これは5
0、60Hz共にいえることである(図5、6)。As an example, the grade (JIS) is 27G1
Magnetic steel sheets of 30 and 27P95 were measured. High grade at high frequency 27P95 low grade 2
Sound pressure is low as a whole compared to 7G130. This is 5
This is true for both 0 and 60 Hz (Figs. 5 and 6).
【0019】これが高調波を含んだ波形の場合は周波数
が高い部分で音圧が高くなる事が評価でき、これに近い
1.9Tでの励磁ではひずみ波形のため高調波成分の大
きさが、大きいことが図中から理解できる。When this is a waveform containing harmonics, it can be evaluated that the sound pressure becomes high at a high frequency portion. Excitation at 1.9T, which is close to this, is a distorted waveform and the magnitude of the harmonic component is It can be understood from the figure that it is large.
【0020】[0020]
【発明の効果】以上説明したように、本発明によれば変
圧器に使用される磁性材料の磁気ひずみを測定すること
で、高調波成分を含む励磁から発生した騒音をA特性音
圧を利用することで評価できる。また、本予測法に基づ
いた、可聴周波数範囲のA特性音圧を測定する機器を製
造ラインに設置することで低騒音材料を製造するための
品質管理ができ、更には現在の騒音問題に対し明確な材
料開発の指針を与え、産業上の利益は極めて大きい。As described above, according to the present invention, by measuring the magnetostriction of the magnetic material used for the transformer, the noise generated from the excitation including the harmonic component is utilized as the A characteristic sound pressure. It can be evaluated by doing. In addition, by installing a device for measuring A-weighted sound pressure in the audible frequency range on the manufacturing line based on this prediction method, quality control for manufacturing low noise materials can be performed, and further, for the present noise problem It gives clear guidelines for material development, and the industrial benefits are extremely large.
【図1】磁気ひずみの周波数依存性を比較したデータで
ある。FIG. 1 is data comparing the frequency dependence of magnetostriction.
【図2】図1の特性をA特性音圧に変換し、比較した図
である。FIG. 2 is a diagram in which the characteristics shown in FIG. 1 are converted into A characteristic sound pressure and compared.
【図3】グレード(JIS)が27G130の電磁鋼板
における磁気ひずみを周波数分析し、A特性音圧に変換
した図である。FIG. 3 is a diagram in which a magnetostriction in an electromagnetic steel sheet having a grade (JIS) of 27G130 is subjected to frequency analysis and converted into A characteristic sound pressure.
【図4】図3と同じ鋼板を用い磁気ひずみを周波数分析
し、A特性音圧に変換した図である。FIG. 4 is a diagram in which magnetostriction is subjected to frequency analysis using the same steel plate as in FIG. 3 and converted into A characteristic sound pressure.
【図5】グレード(JIS)が27P95の電磁鋼板に
おける磁気ひずみを周波数分析し、A特性音圧に変換し
た図である。FIG. 5 is a diagram in which magnetostriction in an electromagnetic steel sheet having a grade (JIS) of 27P95 is frequency analyzed and converted into A characteristic sound pressure.
【図6】図5と同じ鋼板を用い磁気ひずみを周波数分析
し、A特性音圧に変換した図である。FIG. 6 is a diagram in which magnetostriction is subjected to frequency analysis using the same steel plate as in FIG. 5 and converted into A characteristic sound pressure.
Claims (2)
波数範囲で測定し、得られた磁気ひずみを音圧に変換
し、聴感補正を施すことを特徴とする変圧器の騒音レベ
ル予測方法。1. A noise level predicting method for a transformer, comprising: measuring magnetostriction of a magnetic material for a transformer in an audible frequency range; converting the obtained magnetostriction into sound pressure;
料の磁気ひずみ波形を周波数分析し、各周波数における
磁気ひずみを音圧に変換し、さらに聴感補正を施すこと
を特徴とする変圧器の騒音レベル予測方法。2. A transformer which is characterized in that a magnetostriction waveform of a magnetic material for a transformer excited by an arbitrary waveform is subjected to frequency analysis, magnetostriction at each frequency is converted into sound pressure, and further auditory sensation correction is performed. Noise level prediction method.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP05223994A JP3456742B2 (en) | 1993-08-18 | 1994-03-23 | Noise level prediction method of transformer |
Applications Claiming Priority (3)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP20429193 | 1993-08-18 | ||
JP5-204291 | 1993-08-18 | ||
JP05223994A JP3456742B2 (en) | 1993-08-18 | 1994-03-23 | Noise level prediction method of transformer |
Publications (2)
Publication Number | Publication Date |
---|---|
JPH07111217A true JPH07111217A (en) | 1995-04-25 |
JP3456742B2 JP3456742B2 (en) | 2003-10-14 |
Family
ID=26392840
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP05223994A Expired - Fee Related JP3456742B2 (en) | 1993-08-18 | 1994-03-23 | Noise level prediction method of transformer |
Country Status (1)
Country | Link |
---|---|
JP (1) | JP3456742B2 (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2012069620A (en) * | 2010-09-22 | 2012-04-05 | Jfe Steel Corp | Magnetic steel sheet for laminate core |
Families Citing this family (6)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP5736634B2 (en) * | 2008-03-04 | 2015-06-17 | 新日鐵住金株式会社 | Evaluation method of magnetostriction or noise of magnetic steel sheet for three-phase transformer core excited by sine wave |
JP6090503B2 (en) * | 2016-04-05 | 2017-03-08 | Jfeスチール株式会社 | Noise prediction method for transformer |
RU2764622C1 (en) | 2018-07-31 | 2022-01-18 | Ниппон Стил Корпорейшн | Anisotropic electrical steel sheet |
KR102457420B1 (en) | 2018-07-31 | 2022-10-24 | 닛폰세이테츠 가부시키가이샤 | grain-oriented electrical steel sheet |
US11851726B2 (en) | 2018-07-31 | 2023-12-26 | Nippon Steel Corporation | Grain oriented electrical steel sheet |
CN115053000B (en) | 2020-02-05 | 2024-04-02 | 日本制铁株式会社 | Grain oriented electromagnetic steel sheet |
-
1994
- 1994-03-23 JP JP05223994A patent/JP3456742B2/en not_active Expired - Fee Related
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2012069620A (en) * | 2010-09-22 | 2012-04-05 | Jfe Steel Corp | Magnetic steel sheet for laminate core |
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Publication number | Publication date |
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