JP2009231477A - Manufacturing method of transformer - Google Patents

Manufacturing method of transformer Download PDF

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JP2009231477A
JP2009231477A JP2008074047A JP2008074047A JP2009231477A JP 2009231477 A JP2009231477 A JP 2009231477A JP 2008074047 A JP2008074047 A JP 2008074047A JP 2008074047 A JP2008074047 A JP 2008074047A JP 2009231477 A JP2009231477 A JP 2009231477A
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transformer
magnetostriction
iron core
grain
noise
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JP5082966B2 (en
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Misao Namikawa
操 浪川
Masayoshi Ishida
昌義 石田
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JFE Steel Corp
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Abstract

<P>PROBLEM TO BE SOLVED: To provide a method of manufacturing a transformer, using a grain-oriented electromagnetic steel plate, in which a transformer of low noise, with less variations in noise, is stably obtained. <P>SOLUTION: This method is for manufacturing a transformer, comprising an iron core which includes a grain-oriented electromagnetic steel plate. An AC magnetostrictive parameter λ<SB>b</SB>for the grain-oriented electromagnetic steel plate used for the iron core which is defined in formula; λ<SB>b</SB>=max(λ<SB>P-P15/50</SB>, λ<SB>P-P16/50</SB>, λ<SB>P-P17/50</SB>, λ<SB>P-P18/50</SB>)+λ<SB>0-P19/50</SB>(a magnetostriction 0-peak value in 50 Hz-1.7T, for example, is represented as λ<SB>0-P17/50</SB>, and peak-peak value in 50 Hz-1.7T is represented as λ<SB>P-P17/50</SB>), is 1.91×10<SP>-6</SP>or smaller. <P>COPYRIGHT: (C)2010,JPO&INPIT

Description

本発明は、トランスの製造方法に関し、特に、方向性電磁鋼板を用いて騒音の小さいトランスを製造する方法に関するものである。   The present invention relates to a method for manufacturing a transformer, and more particularly to a method for manufacturing a transformer with low noise using a grain-oriented electrical steel sheet.

トランス(変圧器)は、その鉄心(コア)に、方向性電磁鋼板を積層したもの(積鉄心)、あるいは巻いたもの(巻鉄心)を用いるのが普通である。トランスに求められる重要な特性としては、鉄損(無負荷損)特性、励磁電流特性に優れることが挙げられる。さらに、昨今では、トランスが設置される周辺環境への配慮などから、騒音特性に優れる、即ち、低騒音であることも重要となってきている。   As the transformer (transformer), it is common to use a laminate of grain-oriented electrical steel sheets (stacked iron core) or a wound one (rolled iron core). Important characteristics required for the transformer include excellent iron loss (no load loss) characteristics and exciting current characteristics. Furthermore, in recent years, it has become important to have excellent noise characteristics, that is, low noise, in consideration of the surrounding environment where the transformer is installed.

トランスの騒音は、鉄心に使用される電磁鋼板の磁歪特性に大きく依存することが知られている。また、方向性電磁鋼板の磁歪特性は、鋼板が有する磁束密度B(磁界の強さ800A/mにおける磁束密度)で決まるとされており、Bが高いものほど磁歪(磁気歪みとも言う)が小さいことが知られている(たとえば非特許文献1参照)。そこで、低騒音トランスを製造するには、磁歪が小さい方向性電磁鋼板を鉄心に用いるのが普通である。
IEEE Transactions 8(1972)p.677
It is known that the noise of a transformer greatly depends on the magnetostriction characteristics of an electromagnetic steel sheet used for an iron core. In addition, the magnetostriction characteristic of the grain-oriented electrical steel sheet is determined by the magnetic flux density B 8 (magnetic flux density at a magnetic field strength of 800 A / m) that the steel sheet has, and the higher B 8 is, the magnetostriction (also referred to as magnetostriction). Is known to be small (see Non-Patent Document 1, for example). Therefore, in order to manufacture a low-noise transformer, it is common to use a grain-oriented electrical steel sheet having a small magnetostriction for the iron core.
IEEE Transactions 8 (1972) p. 677

ところで、磁束密度Bの高い方向性電磁鋼板を用いて、複数台のトランスを製造した場合、そのトランスの騒音値は、Bの低い方向性電磁鋼板を用いて製造した場合と比較して、確かに平均値で見ると低いものが得られる。しかし、個々のトランスの騒音値について見ると、Bが同じレベルの方向性電磁鋼板を用いているにもかかわらず、騒音値にかなりのばらつきが見られることがある。 Meanwhile, by using the high-oriented electrical steel sheet having a magnetic flux density B 8, if you produce a plurality of transformers, the noise value of the transformer, as compared with the case of producing using a low oriented electrical steel sheets B 8 If you look at the average value, you can get a low one. However, looking at the noise level of the individual transformers, B 8 is despite the use of a grain-oriented electrical steel sheet of the same level, there may be a significant variation observed in the noise level.

従来、このようなばらつきは、ある程度やむを得ないものとされてきた。しかしながら、近年における環境重視の社会においては、斯かるばらつきは許容されないものとなりつつある。   Conventionally, such variations have been unavoidable to some extent. However, this variation is becoming unacceptable in an environment-oriented society in recent years.

そこで、本発明の目的は、方向性電磁鋼板を用いてトランスを製造する方法において、低騒音でかつ騒音のばらつきが小さいトランスを安定して得ることができるトランスの製造方法を提案することにある。   Accordingly, an object of the present invention is to propose a method of manufacturing a transformer that can stably obtain a transformer with low noise and small noise variation in a method of manufacturing a transformer using grain-oriented electrical steel sheets. .

発明者らは、従来技術が抱える上記問題点、即ち、Bが同じレベルの方向性電磁鋼板を用いているにもかかわらず、製造されたトランスの騒音特性にかなりのばらつきが見られるという問題点の原因を探るべく検討を重ねた。その結果、トランスの騒音特性に影響を及ぼす方向性電磁鋼板の因子としては、従来から知られている磁束密度B以外に、磁歪の高調波成分があり、この高調波成分が大きいほど騒音が大きいこと、そして、上記磁歪の高調波成分を小さくするためには、発明者らが新たに見出した交流磁歪パラメータλを適正範囲に制御する必要がある、即ち、低騒音のトランスを安定して製造するには、交流磁歪パラメータλを適正範囲に制御した方向性電磁鋼板を用いることが重要であることを見出し、本発明を完成させた。 The inventors have found that the above-mentioned problems of the prior art, that is, the noise characteristics of the manufactured transformers show considerable variation despite the fact that B 8 uses directional electrical steel sheets of the same level. We studied repeatedly to find out the cause of the point. As a result, the factors affecting oriented electrical steel sheet by the noise characteristics of the transformer, in addition to the magnetic flux density B 8 known from the prior art, there are harmonic components of magnetostrictive noise larger the harmonic components larger, and, in order to reduce the harmonic components of the magnetostriction, it is necessary to control the AC magnetostriction parameter lambda b that inventors have newly found the proper range, i.e., stable and low-noise transformer to produce Te is found that is possible to use a grain-oriented electrical steel sheet having a controlled AC magnetostriction parameter lambda b within a proper range is important, and completed the present invention.

すなわち、本発明は、方向性電磁鋼板からなる鉄心を有するトランスの製造方法であって、その鉄心に用いる方向性電磁鋼板として、下記式;
λ=max(λP−P15/50、λP−P16/50、λP−P17/50、λP−P18/50)+λ0−P19/50
ここで、上式においては、例えば、50Hz−1.7Tにおける磁歪0−peak値をλ0−P17/50、50Hz−1.7Tにおけるpeak−peak値をλP−P17/50のように表す。
で定義される交流磁歪パラメータλが1.91×10−6以下のものを用いることを特徴とするトランスの製造方法である。
That is, this invention is a manufacturing method of the transformer which has an iron core which consists of grain-oriented electrical steel sheets, Comprising: As a grain-oriented electrical steel sheet used for the iron core, following formula | equation;
[lambda] b = max ([lambda] P-P15 / 50 , [lambda] P-P16 / 50 , [lambda] P-P17 / 50 , [lambda] P-P18 / 50 ) + [lambda] 0-P19 / 50
Here, in the above formula, for example, the magnetostriction 0-peak value at 50 Hz-1.7 T is expressed as λ 0-P17 / 50 , and the peak-peak value at 50 Hz-1.7 T is expressed as λ P-P17 / 50. .
A transformer manufacturing method characterized in that an AC magnetostriction parameter λ b defined by the following is used: 1.91 × 10 −6 or less.

また、本発明は、方向性電磁鋼板からなる鉄心を有するトランスの製造方法であって、その鉄心に用いる方向性電磁鋼板として、下記式;
λ=max(λP−P15/50、λP−P16/50、λP−P17/50、λP−P18/50)+λ0−P19/50
ここで、上式においては、例えば、50Hz−1.7Tにおける磁歪0−peak値をλ0−P17/50、50Hz−1.7Tにおけるpeak−peak値をλP−P17/50のように表す。
で定義される交流磁歪パラメータλが、製造するトランスに許容される騒音値のばらつきから定められるλの最大値以下あるいは最大値と最小値の範囲内のものを用いることを特徴とするトランスの製造方法である。
Moreover, this invention is a manufacturing method of the transformer which has an iron core which consists of a grain-oriented electrical steel sheet, Comprising: As a grain-oriented electrical steel sheet used for the iron core, following formula | equation;
[lambda] b = max ([lambda] P-P15 / 50 , [lambda] P-P16 / 50 , [lambda] P-P17 / 50 , [lambda] P-P18 / 50 ) + [lambda] 0-P19 / 50
Here, in the above formula, for example, the magnetostriction 0-peak value at 50 Hz-1.7 T is expressed as λ 0-P17 / 50 , and the peak-peak value at 50 Hz-1.7 T is expressed as λ P-P17 / 50. .
The transformer is characterized in that the AC magnetostriction parameter λ b defined in (1) is less than or equal to the maximum value of λ b determined from the variation in the noise value allowed for the transformer to be manufactured or within the range between the maximum value and the minimum value. It is a manufacturing method.

また、本発明における上記鉄心は、積鉄心または巻鉄心であることを特徴とする。   In the present invention, the iron core is a stacked iron core or a wound iron core.

本発明によれば、トランスの実機騒音性能を正確に予測できるパラメータ(交流磁歪パラメータλ)を用いて選択した方向性電磁鋼板のみを使用して鉄心を製造するので、同一設計のトランスを複数台製造する場合でも、低騒音でかつ騒音値のばらつきの小さいトランスを安定して製造することが可能となる。 According to the present invention, since the iron core is manufactured using only the directional electrical steel sheet selected using the parameter (AC magnetostriction parameter λ b ) that can accurately predict the actual machine noise performance of the transformer, a plurality of transformers of the same design are used. Even when a stand is manufactured, it is possible to stably manufacture a transformer with low noise and small variation in noise value.

方向性電磁鋼板を鉄心に用いたトランスの騒音性能は、方向性電磁鋼板の磁歪特性に依存し、また、その方向性電磁鋼板の磁歪特性は、鋼板の磁束密度B(磁界の強さ800A/mのときの磁束密度)に依存する。そのため、トランスの騒音特性は、鉄心に用いる鋼板の磁束密度Bでほぼ決まるとされてきた。しかし、Bレベルがほぼ等しい方向性電磁鋼板を用いたにもかかわらず、製造時期や製造ロッドが異なると、トランスの騒音特性が異なるという現象がしばしば観察された。 The noise performance of a transformer using a grain-oriented electrical steel sheet as an iron core depends on the magnetostriction characteristics of the grain-oriented electrical steel sheet, and the magnetostriction characteristics of the grain-oriented electrical steel sheet depend on the magnetic flux density B 8 (magnetic field strength 800A). Magnetic flux density at / m). Therefore, the noise characteristics of the transformer has been substantially determined by a magnetic flux density B 8 of steel sheets used for the core. However, even though B 8 levels with approximately equal oriented electrical steel sheet, the manufacturing time and manufacturing rods are different, the noise characteristics of the transformer phenomenon different were frequently observed.

発明者らは、上記ばらつきの原因を解明すべく製造時期や製造ロッドが異なる方向性電磁鋼板を複数用意し、素材の磁歪特性を詳しく調べるとともに、モデルトランスを製造して、騒音特性との関係を調査した。その結果、Bレベルがほぼ等しい方向性電磁鋼板であっても、製造時期や製造ロッドによって磁歪高調波成分に違いが見られ、この高調波成分の違いとトランスの騒音特性の違いとが対応していることを見出した。 Inventors prepared a plurality of grain-oriented electrical steel sheets with different production times and production rods to elucidate the cause of the variation, investigated the magnetostriction characteristics of the materials in detail, manufactured a model transformer, and the relationship with the noise characteristics. investigated. As a result, even approximately equal oriented electrical steel sheet B 8 levels, the difference in the magnetostrictive harmonic component by the production time and production rod is observed, the corresponding and the difference between the difference and the transformer noise characteristics of the harmonic components I found out.

磁歪は、電磁鋼板の磁束密度が変化したときに電磁鋼板の形状(寸法)がそれに従って変化することに起因しているが、磁束密度の変化と形状変化の関係は一般には非線形である。したがって、交流励磁を正弦波形で行い、磁束密度変化を正弦波としても、磁歪波形は歪んだ波形となってしまう。この波形は、接続された電気系統の電圧周波数の2倍の周波数をもつ基本波成分とその整数倍の周波数をもつ高調波成分とで構成される。そして、後者の高調波成分は、空気に伝播すると、耳障りな音として人に感知され、騒音レベルを上昇させることとなる。   Magnetostriction is caused by a change in the shape (dimension) of the magnetic steel sheet when the magnetic flux density of the magnetic steel sheet changes, but the relationship between the change in magnetic flux density and the shape change is generally non-linear. Therefore, even if AC excitation is performed with a sine waveform and the change in magnetic flux density is a sine wave, the magnetostrictive waveform is distorted. This waveform is composed of a fundamental wave component having a frequency twice the voltage frequency of the connected electrical system and a harmonic component having a frequency that is an integer multiple of the fundamental wave component. Then, when the latter harmonic component is propagated to the air, it is perceived by a person as an unpleasant sound and raises the noise level.

従って、低騒音のトランスを製造するには、鉄心に用いる方向性電磁鋼板の磁歪高調波成分を予め測定しておき、高調波成分のレベルを基準として、使用する鋼板を取捨選択すれば、低騒音のトランスを製造することが可能となる。しかし、磁歪高調波成分を実機の生産管理に使用するには、磁歪高調波成分の測定に極めて手間がかかったり、その測定のための新たな設備投資が必要となったりするため好ましくない。   Therefore, in order to produce a low noise transformer, the magnetostrictive harmonic component of the grain-oriented electrical steel sheet used for the iron core is measured in advance, and the steel sheet to be used is selected based on the level of the harmonic component. A noise transformer can be manufactured. However, in order to use the magnetostrictive harmonic component for production management of an actual machine, it is not preferable because the measurement of the magnetostrictive harmonic component is extremely time-consuming and requires a new equipment investment for the measurement.

そこで、発明者らは、従来から実機の生産管理に用いている磁歪特性(磁歪0−peak値およびpeak−peak値)から磁歪高調波成分を予測することができないか、さらに検討を進めた。その結果、例えば、50Hz−1.7Tにおける磁歪0−peak値(磁束密度0の時の磁歪と最大磁歪との差)をλ0−P17/50、peak−peak値(最大磁歪と最小磁歪の差)をλP−P17/50のように表すとき、
λ=max(λP−P15/50、λP−P16/50、λP−P17/50、λP−P18/50)+λ0−P19/50
で定義される交流磁歪パラメータλと磁歪高調波特性との間に極めて強い相関があることを見出した。ここで、max(λP−P15/50、λP−P16/50、λP−P17/50、λP−P18/50)は、λP−P15/50、λP−P16/50、λP−P17/50およびλP−P18/50の中の最大磁歪値を意味する。
Therefore, the inventors have further investigated whether it is possible to predict the magnetostrictive harmonic component from the magnetostriction characteristics (the magnetostriction 0-peak value and the peak-peak value) conventionally used for production management of actual machines. As a result, for example, the magnetostriction 0-peak value (difference between the magnetostriction and the maximum magnetostriction when the magnetic flux density is 0) at 50 Hz-1.7 T is λ 0-P17 / 50 , and the peak-peak value (the maximum magnetostriction and the minimum magnetostriction). When the difference is expressed as λ P-P17 / 50 ,
[lambda] b = max ([lambda] P-P15 / 50 , [lambda] P-P16 / 50 , [lambda] P-P17 / 50 , [lambda] P-P18 / 50 ) + [lambda] 0-P19 / 50
It was found that there is a very strong correlation between the AC magnetostriction parameter λb defined by (1) and the magnetostrictive harmonic characteristics. Here, max (λ P-P15 / 50 , λ P-P16 / 50 , λ P-P17 / 50 , λ P-P18 / 50 ) is λ P-P15 / 50 , λ P-P16 / 50 , λ It means the maximum magnetostriction value in P-P17 / 50 and λ P-P18 / 50 .

なお、上記のように、交流磁歪パラメータλと磁歪高調波特性との間に相関がある理由については、必ずしも十分に解明されていないが、上記λが方向性電磁鋼板の磁区構造、特に磁歪の原因である90度磁区の存在量を表す良いパラメータとなっているためと考えられる。 As described above, the reason why there is a correlation between the AC magnetostrictive parameter λ b and the magnetostrictive harmonic characteristics is not necessarily fully understood, but the λ b is a magnetic domain structure of a grain-oriented electrical steel sheet, In particular, this is considered to be a good parameter representing the abundance of the 90-degree magnetic domain that is the cause of magnetostriction.

そこで、発明者らは、トランスの騒音の低減目標を、鉄心を50Hz−1.75Tで励磁したときに、鉄心表面から30cm離れた位置で測定した騒音値が54dBA以下と設定し、この騒音値を達成するために、鉄心の素材となる方向性電磁鋼板が有すべき交流磁歪パラメータλを調査した。その結果、λ≦1.91×10−6なる関係を満たす方向性電磁鋼板を選択して鉄心を製造すれば、上記騒音目標を達成できること、さらに、λ≦1.71×10−6なる関係を満たせば、より低騒音のトランスを製造できることがわかった。 Therefore, the inventors set the noise reduction target of the transformer as a noise value measured at a position 30 cm away from the iron core surface when the iron core is excited at 50 Hz-1.75 T. In order to achieve the above, the AC magnetostriction parameter λ b that the grain-oriented electrical steel sheet that is the material of the iron core should have was investigated. As a result, the above noise target can be achieved by selecting a grain oriented electrical steel sheet satisfying the relationship of λ b ≦ 1.91 × 10 −6 and manufacturing the iron core, and further, λ b ≦ 1.71 × 10 −6. It was found that a transformer with lower noise can be manufactured if the following relationship is satisfied.

また、λ≦1.91×10−6なる関係を満たしていない場合であっても、製造するトランスに許容される騒音値に応じてλの許容範囲の上限値を定め、λがその許容範囲内にある方向性電磁鋼板のみを選択して鉄心を製造するようにすれば、同一設計で複数台のトランスを製造する場合にも、騒音特性のばらつきを小さくすることが可能であることがわかった。なお、必要に応じて、λの許容範囲の上限値だけでなく下限値を設けてもよいことは勿論である。 Moreover, lambda even if they do not meet the b ≦ 1.91 × 10 -6 the relationship, define the upper limit of the allowable range of lambda b in accordance with the noise value allowed to the transformer to produce, lambda b is If only the grain-oriented electrical steel sheets within the permissible range are selected and the iron core is manufactured, it is possible to reduce the variation in noise characteristics even when manufacturing a plurality of transformers with the same design. I understood it. If necessary, it may be provided lower limit not only the upper limit of the allowable range of lambda b is a matter of course.

表1に示したように、製造時期や製造ロッドが異なる板厚が0.3mmの方向性電磁鋼板の中から選択した磁束密度Bの値がほぼ等しいA〜Kの11種類の鋼板(コイル)を用意し、これらを幅150mmにスリット加工したのち斜角切断、Vノッチ切断して3相3脚のモデルトランスを作製した。上記モデルトランスは、脚、ヨークの幅は150mm、外寸は750mm×750mmの100枚積みとし、接合はVノッチ、ステップラップ(2by6)とした。 As shown in Table 1, 11 types of steel A~K value of the magnetic flux density B 8 selected from the oriented electrical steel sheet manufacturing time and manufacturing rods have different plate thickness 0.3mm is approximately equal to (coil ) Were prepared, slitted to a width of 150 mm, and then a bevel cut and V-notch cut were performed to produce a three-phase, three-leg model transformer. The model transformer had a leg and yoke with a width of 150 mm, an outer dimension of 100 sheets of 750 mm × 750 mm, and a V-notch and a step wrap (2 by 6).

また、上記150mm幅のスリットコイルのそれぞれから、幅100mm×長さ400mmの単板を10枚ずつ採取し、50Hz−1.5T,1.6T,1.7Tおよび1.8Tにおける交流磁歪のpeak−peak値(λP−P15/50、λP−P16/50、λP−P17/50、λP−P18/50)と50Hz−1.9Tにおける交流磁歪の0−peak値(λ0−P19/50)を測定し、下式;
λ=max(λP−P15/50、λP−P16/50、λP−P17/50、λP−P18/50)+λ0−P19/50
から、交流磁歪パラメータλを算出し、それぞれ10枚の平均値を求めた。
In addition, ten single plates each having a width of 100 mm and a length of 400 mm were sampled from each of the 150 mm-width slit coils, and the peak of AC magnetostriction at 50 Hz-1.5T, 1.6T, 1.7T, and 1.8T was obtained. -Peak value (λ P-P15 / 50 , λ P-P16 / 50 , λ P-P17 / 50 , λ P-P18 / 50 ) and 0-peak value of AC magnetostriction at 50 Hz-1.9T (λ 0- P19 / 50 ) and the following formula:
[lambda] b = max ([lambda] P-P15 / 50 , [lambda] P-P16 / 50 , [lambda] P-P17 / 50 , [lambda] P-P18 / 50 ) + [lambda] 0-P19 / 50
From calculates the AC magnetostriction parameter lambda b, to obtain an average value of 10 sheets, respectively.

また、上記の作製した3相3脚のモデルトランスの騒音特性を、トランスの中央脚センターから30cm離れた位置で、50Hz−1.75Tにおける騒音値(Aスケール)を測定した。   Moreover, the noise value (A scale) in 50Hz-1.75T was measured for the noise characteristic of the produced three-phase / three-leg model transformer at a position 30 cm away from the center leg center of the transformer.

Figure 2009231477
Figure 2009231477

上記交流磁歪パラメータλおよびトランスの騒音値の測定結果を表1に併記するとともに、その結果を図1および図2に示した。図1から、トランスの騒音値は、磁束密度Bに依存しているが、同じBレベルでも騒音値がばらついていることがわかる。また、図2から、トランス騒音値は、交流磁歪パラメータλとよい相関があり、λ≦1.91×10−6の条件を満たす方向性電磁鋼板を用いて鉄心を作製すれば、54dBA以下の低騒音トランスを製造することができ、特に、λ≦1.71×10−6である方向性電磁鋼板を用いた場合には、52dBA以下という極めて低騒音のトランスを製造することができることがわかる。 The measurement results of the AC magnetostriction parameter lambda b and trans noise values with are shown in Table 1, and the results are shown in FIGS. FIG. 1 shows that the noise value of the transformer depends on the magnetic flux density B 8 , but the noise value varies even at the same B 8 level. Further, from FIG. 2, the transformer noise value has a good correlation with the AC magnetostriction parameter λ b, and if an iron core is made using a grain oriented electrical steel sheet that satisfies the condition of λ b ≦ 1.91 × 10 −6 , 54 dBA The following low noise transformers can be manufactured. In particular, when a grain-oriented electrical steel sheet having λ b ≦ 1.71 × 10 −6 is used, it is possible to manufacture a very low noise transformer of 52 dBA or less. I understand that I can do it.

表1の鋼板G〜Kを用いて、それぞれの鋼板から、実施例1と同様にして、3相3脚のモデルトランスを10台ずつ作製し、実施例1と同様にして、トランスの騒音値を測定し、10台のトランスの騒音値のばらつき(最大値−最小値)を求めた。それと同時に、各モデルトランスに用いた鋼板から、サンプルを採取し、実施例1と同様にして、50Hz−1.5T,1.6T,1.7Tおよび1.8Tにおける交流磁歪のpeak−peak値(λP−P15/50、λP−P16/50、λP−P17/50、λP−P18/50)と50Hz−1.9Tにおける交流磁歪の0−peak値(λ0−P17/50)を測定し、交流磁歪パラメータλを算出し、各鋼板のλのばらつき(最大値−最小値)を求めた。 Using the steel plates G to K in Table 1, ten three-phase, three-leg model transformers were produced from each steel plate in the same manner as in Example 1, and the noise level of the transformer was determined in the same manner as in Example 1. The noise value variation (maximum value-minimum value) of 10 transformers was obtained. At the same time, a sample was taken from the steel plate used for each model transformer, and the peak-peak value of AC magnetostriction at 50 Hz-1.5T, 1.6T, 1.7T and 1.8T was obtained in the same manner as in Example 1. (Λ P-P15 / 50 , λ P-P16 / 50 , λ P-P17 / 50 , λ P-P18 / 50 ) and 0-peak value (λ 0-P17 / 50 ) of AC magnetostriction at 50 Hz-1.9T. ) Was measured, the AC magnetostriction parameter λ b was calculated, and the variation (maximum value−minimum value) of λ b of each steel sheet was obtained.

上記測定の結果を表2に示した。表2から、λ≦1.91×10−6の条件を満たしていない鋼板を用いてトランスを製造する場合であっても、鋼板の交流磁歪パラメータλのばらつきを小さく抑えることにより、トランスの騒音特性のバラツキを小さくでき、例えば、交流磁歪パラメータλを±0.05×10−6の範囲の鋼板を選択してトランスを製造すれば、騒音のばらつきの目標を±1.5dBA以下としたとき、これを達成することが可能であることがわかる。 The measurement results are shown in Table 2. From Table 2, even when the transformer is manufactured using a steel sheet that does not satisfy the condition of λ b ≦ 1.91 × 10 −6 , the transformer can be reduced by suppressing variations in the AC magnetostriction parameter λ b of the steel sheet. of can reduce variations in noise characteristics, for example, be manufactured transformer AC magnetostriction parameter lambda b select steel ranging from ± 0.05 × 10 -6, the target of the dispersion of the noise ± 1.5DBA less It can be seen that this can be achieved.

Figure 2009231477
Figure 2009231477

磁束密度Bがトランスの騒音に及ぼす影響を示すグラフである。The magnetic flux density B 8 is a graph showing the effect on the transformer noise. 鋼板の交流磁歪パラメータλがトランスの騒音に及ぼす影響を示すグラフである。It is a graph which shows the influence which AC magnetostriction parameter (lambda) b of a steel plate has on the noise of a transformer.

Claims (3)

方向性電磁鋼板からなる鉄心を有するトランスの製造方法であって、その鉄心に用いる方向性電磁鋼板として、下記式で定義される交流磁歪パラメータλが1.91×10−6以下のものを用いることを特徴とするトランスの製造方法。

λ=max(λP−P15/50、λP−P16/50、λP−P17/50、λP−P18/50)+λ0−P19/50
ここで、上式においては、例えば、50Hz−1.7Tにおける磁歪0−peak値をλ0−P17/50、50Hz−1.7Tにおけるpeak−peak値をλP−P17/50のように表す。
A method of manufacturing a transformer having an iron core made of grain-oriented electrical steel sheets, wherein an AC magnetostriction parameter λ b defined by the following formula is 1.91 × 10 −6 or less as a grain-oriented magnetic steel sheet used for the iron core. A method of manufacturing a transformer, characterized by being used.
Λ b = max (λ P-P15 / 50 , λ P-P16 / 50 , λ P-P17 / 50 , λ P-P18 / 50 ) + λ 0-P19 / 50
Here, in the above formula, for example, the magnetostriction 0-peak value at 50 Hz-1.7 T is expressed as λ 0-P17 / 50 , and the peak-peak value at 50 Hz-1.7 T is expressed as λ P-P17 / 50. .
方向性電磁鋼板からなる鉄心を有するトランスの製造方法であって、その鉄心に用いる方向性電磁鋼板として、下記式で定義される交流磁歪パラメータλが、製造するトランスに許容される騒音値のばらつきから定められるλの最大値以下あるいは最大値と最小値の範囲内のものを用いることを特徴とするトランスの製造方法。

λ=max(λP−P15/50、λP−P16/50、λP−P17/50、λP−P18/50)+λ0−P19/50
ここで、上式においては、例えば、50Hz−1.7Tにおける磁歪0−peak値をλ0−P17/50、50Hz−1.7Tにおけるpeak−peak値をλP−P17/50のように表す。
A method of manufacturing a transformer having an iron core made of grain-oriented electrical steel sheets, wherein the magnetostrictive parameter λ b defined by the following equation is a noise value allowed for the transformer to be produced as a grain-oriented magnetic steel sheet used for the iron core. the method of manufacturing a transformer, which comprises using those within the maximum value or less or the maximum and minimum values of lambda b defined by the variation.
Λ b = max (λ P-P15 / 50 , λ P-P16 / 50 , λ P-P17 / 50 , λ P-P18 / 50 ) + λ 0-P19 / 50
Here, in the above formula, for example, the magnetostriction 0-peak value at 50 Hz-1.7 T is expressed as λ 0-P17 / 50 , and the peak-peak value at 50 Hz-1.7 T is expressed as λ P-P17 / 50. .
上記鉄心は積鉄心または巻鉄心であることを特徴とする請求項1または2に記載のトランスの製造方法。 3. The method of manufacturing a transformer according to claim 1, wherein the iron core is a stacked iron core or a wound iron core.
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JP2017128765A (en) * 2016-01-20 2017-07-27 新日鐵住金株式会社 Oriented electromagnetic steel sheet, manufacturing method of oriented electromagnetic steel sheet, iron core for transformer or reactor and noise evaluation method

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JP2011090456A (en) * 2009-10-21 2011-05-06 Jfe Steel Corp Order receiving and shipping method for grain oriented magnetic steel sheet for transformer
JPWO2016125504A1 (en) * 2015-02-05 2017-06-08 Jfeスチール株式会社 Directional electrical steel sheet, method for manufacturing the same, and method for predicting transformer noise characteristics
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JP2017128765A (en) * 2016-01-20 2017-07-27 新日鐵住金株式会社 Oriented electromagnetic steel sheet, manufacturing method of oriented electromagnetic steel sheet, iron core for transformer or reactor and noise evaluation method

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