JPS62213104A - Amorphous core transformer - Google Patents
Amorphous core transformerInfo
- Publication number
- JPS62213104A JPS62213104A JP5594986A JP5594986A JPS62213104A JP S62213104 A JPS62213104 A JP S62213104A JP 5594986 A JP5594986 A JP 5594986A JP 5594986 A JP5594986 A JP 5594986A JP S62213104 A JPS62213104 A JP S62213104A
- Authority
- JP
- Japan
- Prior art keywords
- iron core
- core
- amorphous
- plates
- iron
- 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.)
- Pending
Links
Landscapes
- Manufacturing Cores, Coils, And Magnets (AREA)
Abstract
Description
【発明の詳細な説明】
(発明の属する技術分野)
本発明は、アモルファス磁性材料の単板を複数枚積重ね
てMM鉄心とするアモルファス鉄心変圧器に関する。DETAILED DESCRIPTION OF THE INVENTION (Technical field to which the invention pertains) The present invention relates to an amorphous core transformer in which a plurality of single plates of amorphous magnetic material are stacked to form an MM core.
(従来技術とその問題点)
一般に、磁性材料は応力またはひずみに対して鋭敏であ
るからけい素鋼帯で変圧器鉄心を組み立てる場合、この
応力またはひずみの影響を考慮しないと組み立てた変圧
器に必要な特性が得られず、特に鉄損に対して悪い影響
を与えることが知られている。従来けい素鋼帯を積層し
て変圧器鉄心を組み立てる場合は、けい素鋼帯を適当な
幅の短冊または額縁形に切断して、ひずみ取り焼なまし
を施した後、この焼なましだ単板を積重ねて厚い鉄板な
どの間に挾みボルトなどで1〜3ky/aSの圧力で締
付けている。(Prior art and its problems) In general, magnetic materials are sensitive to stress or strain, so when assembling a transformer core with silicon steel strips, if the effects of this stress or strain are not taken into account, the assembled transformer It is known that the necessary characteristics cannot be obtained, and that it has a particularly negative effect on iron loss. Conventionally, when assembling a transformer core by laminating silicon steel strips, the silicon steel strips are cut into strips or picture frame shapes of an appropriate width, and then subjected to strain relief annealing. The veneers are stacked, placed between thick iron plates, etc., and tightened with bolts or the like at a pressure of 1 to 3 ky/aS.
一方、アモルファス磁性材料は高透磁率低損失であり、
これを理想的な構成で変圧器鉄心を組み立てると、鉄損
と励磁電流が小さく、鉄損は方向性けい素鋼帯のような
現用の最高級けい素鋼帯を用いた場合より /3〜/4
に低減できるといわれている。しかしアモルファス磁性
材料はけい素鋼帯よりもさらに応力またはひずみに対し
て敏感であり、けい素鋼帯と同じ手法で変圧器鉄心を製
作してもその特徴を生かした特性が得難いという欠点が
ある。特に、アモルファス磁性材料はその製造上厚さは
30μ簿程度と薄い帯状のため主として巻鉄心として用
いられる場合が多く、巻き上げて成形した鉄心に磁界を
かけて焼なましを施し、磁気特性を改善して用いている
。しかし大形変圧器では当然コイル内に鉄心を挿入して
組立てることになるから、アモルファス磁性材料の薄板
を所定の形に切断して単板とし、この単板を複数枚積重
ねて形成したいわゆる積層鉄心を用いねばならない。勿
論このような積層用アモルファス磁性材料も焼なましを
施してひずみ取りがなされたものを使用するが、このよ
うな磁気的に敏感な材料は組立て時において、応力が加
えられると再び特性が劣化してしまうという欠点があり
、組み立て時にこの応力の増加による磁気特性の劣化を
防止しなければならない。On the other hand, amorphous magnetic materials have high magnetic permeability and low loss,
If this transformer core is assembled in an ideal configuration, the iron loss and excitation current will be small, and the iron loss will be /3~ compared to when using the highest grade silicon steel strip currently in use, such as grain-oriented silicon steel strip. /4
It is said that it can be reduced to However, amorphous magnetic materials are more sensitive to stress or strain than silicon steel strips, and the disadvantage is that even if a transformer core is manufactured using the same method as silicon steel strips, it is difficult to obtain properties that take advantage of its characteristics. . In particular, amorphous magnetic materials are manufactured in the form of thin strips with a thickness of about 30 μm, so they are often used primarily as wound cores.The rolled and formed cores are annealed by applying a magnetic field to improve their magnetic properties. It is used as However, since large transformers naturally have to be assembled by inserting an iron core into the coil, a thin plate of amorphous magnetic material is cut into a predetermined shape to make a veneer, and multiple veneers are stacked to form a so-called laminated structure. An iron core must be used. Of course, such amorphous magnetic materials for lamination are also annealed to remove strain, but such magnetically sensitive materials will deteriorate again when stress is applied during assembly. However, during assembly, it is necessary to prevent deterioration of the magnetic properties due to this increase in stress.
(発明の目的)
本発明の目的は、アモルファス磁性材料を積層して鉄心
を組み立てるときの締付圧力を限定して、鉄心に与える
応力による鉄損の増加を抑制したアモルファス鉄心変圧
器を提供することにある。(Object of the Invention) An object of the present invention is to provide an amorphous core transformer in which an increase in core loss due to stress applied to the core is suppressed by limiting the tightening pressure when assembling the core by laminating amorphous magnetic materials. There is a particular thing.
(発明の要点)
本発明は、アモルファス磁性材料の単板を複数とするも
ので、積層鉄心に圧力を加えて締付けるとこの圧力に関
係してアモルファス磁性材料に応力が加わり、磁気特性
が劣化し、特に鉄損が増加することに鑑み、この締付は
圧力を限定して磁気特性の劣化を防止し、焼なました状
態に近い特性をそのまま再現したアモルファス鉄心変圧
器を提供しようというものである。なお、積層鉄心は焼
なましたアモルファス磁性材料の単板を複数枚積重ねる
と工作に都合がよい。(Summary of the Invention) The present invention uses a plurality of single plates made of amorphous magnetic material, and when the laminated core is tightened with pressure, stress is applied to the amorphous magnetic material in relation to this pressure, causing deterioration of magnetic properties. In particular, in view of the increase in iron loss, this tightening is intended to limit the pressure and prevent deterioration of magnetic properties, thereby providing an amorphous core transformer that reproduces properties close to those in the annealed state. be. Note that it is convenient to construct the laminated core by stacking multiple veneers of annealed amorphous magnetic material.
(発明の実施例)
以下図面を参照しながら本発明の詳細な説明する。まず
本発明者等は上述のような要求事項を満たすように以下
の研究を行った結果、本発明に到達し゛たものである。(Embodiments of the Invention) The present invention will be described in detail below with reference to the drawings. First, the present inventors conducted the following research to satisfy the above-mentioned requirements, and as a result, they arrived at the present invention.
まず厚さ25μ島1幅50.5msの単板を6枚重ねて
接合し、磁界生焼なましを施した?e 78. Si9
. B13原子%の帯状アモルファス磁性材料の長さを
短冊状に切断しくこれを以後単板と略称する)、これを
エプスタイン粋のように4辺に配置したコイル内に第2
図に示すように4隅を1枚毎にラップさせて、外側寸法
401m5の4辺形の磁気回路を構成して、締付けせず
に鉄損を測定した。その結果50Hzで最も使用される
磁束密度1.3Tにおける鉄損W、 watt / &
9は、第3図に示すように枠の一辺の積重ね枚数N(
ここでは実際のWIWJ枚数はHの6倍である)が10
枚までの間は枚数Nの増加とともに鉄損W、は増加する
が、以後はほぼ一定になり、約0.18watt/hg
と十分低い値で安定している。これは自由状態で僅かに
変形していた単板が、積重ねられることにより自重で変
形が矯正されて逆に応力が加わり、鉄損W、が増加した
ものと考えられる。First, six veneers with a thickness of 25 μm and a width of 50.5 ms were stacked and bonded, and subjected to magnetic field annealing. e78. Si9
.. The length of the strip-shaped amorphous magnetic material containing 13 at.
As shown in the figure, the four corners of each sheet were wrapped to form a quadrilateral magnetic circuit with an outer dimension of 401 m5, and the iron loss was measured without tightening. As a result, the iron loss W at 50Hz and the most used magnetic flux density of 1.3T, watt / &
9 is the number of sheets stacked on one side of the frame N(
Here, the actual number of WIWJ sheets is 6 times that of H) is 10
The iron loss W increases as the number N increases until the number of sheets N increases, but after that it remains almost constant and is approximately 0.18 watt/hg.
It is stable at a sufficiently low value. This is thought to be because the veneers, which had been slightly deformed in their free state, were stacked together, correcting the deformation due to their own weight, and conversely applying stress, which increased the iron loss W.
次に、同じように単板を各辺20枚ずつ前述のコイル内
に組込んで非磁性板を重ね、次第に加圧したときの加圧
力Pay/cm’と損失w、watt/Ayとの関係を
第4図に示す。ここで曲線Aは鉄損。Next, in the same way, 20 veneers on each side are assembled into the above-mentioned coil, non-magnetic plates are stacked, and pressure is gradually applied. The relationship between the pressing force Pay/cm' and the loss w and watt/Ay. is shown in Figure 4. Here, curve A is iron loss.
曲線Bはヒステリシス損1曲線0はうず電流損である。Curve B is hysteresis loss and curve 0 is eddy current loss.
勿論ヒステリシス損とうす電流損の和が鉄損であるが、
うず電流損が加圧力に関係せず、はぼ一定であることは
単板が応力以外の影響を受けていないことを示している
。またヒステリシス損、したがって鉄損は加圧力0.5
kg/amまではその増加率は高(,0,5&ダ76m
を超えると安定するがなおほぼ直線的に増加している。Of course, the sum of hysteresis loss and thin current loss is iron loss, but
The fact that the eddy current loss is not related to the applied force and is almost constant indicates that the veneer is not affected by anything other than stress. Also, the hysteresis loss, and therefore the iron loss, is the applied force of 0.5
The increase rate is high up to kg/am (,0,5&da76m
It stabilizes when it exceeds , but it still increases almost linearly.
この結果から、アモルファス磁性材料を積層して組立て
る鉄心の鉄損増加を防止するには締付圧力を小さくする
ことが不可欠で、一般に目標とされる5 0 H2,1
,3Tにおける鉄損を0.23 watt/ kjl
1Ij4度以下に抑制するには第4図から締付圧力は0
.5kg/ays以下にする必要がある。勿論鉄心の形
状を保持する締付圧力は必要であるから、O−05k
9 / C鴇 ないし0.5にダ/emの締付圧を鉄
心に与えれば、所期目的を達成することができる。From this result, it is essential to reduce the tightening pressure in order to prevent an increase in iron loss in the core assembled by laminating amorphous magnetic materials, and the general target is 50 H2,1.
, the iron loss at 3T is 0.23 watt/kjl
1Ij To suppress it to 4 degrees or less, the tightening pressure should be 0 from Figure 4.
.. It is necessary to keep it below 5kg/ays. Of course, tightening pressure is necessary to maintain the shape of the iron core, so O-05k
If a clamping pressure of 9/C to 0.5 da/em is applied to the iron core, the desired purpose can be achieved.
次にこのような締付力が鉄心に与えられた変圧器の具体
的な構成を示す。第1図において、1はアモルファス磁
性材料の単板を複数枚積層した鉄心で、その脚1cLは
断面を円形に近付けるために一定の厚さごとに幅の異な
る単板を積重ねて段部1bを形成しである。そしてこの
積重ねた両面にヨークICの面まで達する長さの鉄心当
板2を当て、さらにその外側の脚1αに当木3を当て、
段部1bには丸棒のくさび4を挾み、例えばガ玉ス繊維
強化プラスチックのバンド5を巻き付け、鉄心1.鉄心
当板2.当木3.くさび4を一体として脚1cLを0.
05〜0.5 kg76% の圧力で締付ける。この
とき当木3は外面に丸みをもたせ、くさまだ当木3はバ
ンド5%息に1個ずつ用いるが、各バンド5が一様の圧
力で鉄心1を締付けるように留意する。勿論ヨークIC
の部分も図には示してないが脚15cに準じてバンドで
締付ける。このような構成により、アモルファス磁性材
料を鉄心とする変圧器が得られる。Next, a specific configuration of a transformer in which such a tightening force is applied to the core will be shown. In Fig. 1, reference numeral 1 denotes an iron core made of a plurality of laminated veneers made of amorphous magnetic material, and its leg 1cL is made by laminating veneers of different widths at regular thickness intervals to form a stepped portion 1b in order to approximate a circular cross section. It is formed. Then, apply a core contact plate 2 long enough to reach the surface of the yoke IC to both sides of the stack, and apply a contact plate 3 to the outer leg 1α.
A round bar wedge 4 is placed between the stepped portions 1b, and a band 5 made of, for example, fiber-reinforced plastic is wrapped around the iron core 1. Iron core backing plate 2. Toki 3. Wedge 4 is integrated and leg 1 cL is 0.
05~0.5 kg Tighten with 76% pressure. At this time, the outer surface of the wood 3 is rounded, and one piece of wood 3 is used for each 5% band, but care must be taken so that each band 5 tightens the iron core 1 with uniform pressure. Of course York IC
Although this part is not shown in the figure, tighten it with a band in the same way as leg 15c. With such a configuration, a transformer having an iron core made of an amorphous magnetic material can be obtained.
なお、アモルファス合金(1+lθ−B−81系)の密
度は約’ty/Cmであるから、積層単板を50 am
厚とした場合、積層単板の自重により下層の単板には3
50 g / c♂の圧力が加わる。したがって変圧器
を大型にして鉄心の厚さを増す場合には、第1図に示す
ように、鉄心をたて構造とし、更に吊り上げ構造によっ
て自重の影響を少なくすることが好ましい。Note that the density of the amorphous alloy (1+lθ-B-81 series) is approximately 'ty/Cm, so the laminated veneer is
When considering the thickness, due to the weight of the laminated veneer, the lower layer veneer has a thickness of 3
A pressure of 50 g/c♂ is applied. Therefore, when increasing the size of the transformer and increasing the thickness of the core, it is preferable to make the core vertical, as shown in FIG. 1, and to further reduce the influence of its own weight by using a suspended structure.
(発明の効果)
以上述べたように本発明によれば、アモルファス磁性材
料を積重ねて積層鉄心を形成し、この鉄心を0.05k
g/c鴇 ないしo、’shgyc簿の圧力で締付ける
ことにより、鉄心の磁気特性の応力による劣化を防ぎ、
所望の特性を得ることができ効果は大きい。(Effects of the Invention) As described above, according to the present invention, amorphous magnetic materials are stacked to form a laminated iron core, and this iron core has a thickness of 0.05k.
By tightening with g/c pressure, the magnetic properties of the core are prevented from deteriorating due to stress.
The desired characteristics can be obtained and the effect is great.
第1図ないし第4図は本発明によるアモルファス鉄心変
圧器の実施例を示し、第1図はアモルファス鉄心変圧器
の鉄心の一部を示す斜視図、第2図はアモルファス磁性
材料の鉄損測定に用いた試料の寸法図、第3図は積層鉄
心の積重ね枚数と鉄損との関係を示す曲liJ図、第4
図は積層鉄心の締付圧力と損失との関係を示す曲線図で
ある。
第1図1 to 4 show an embodiment of an amorphous core transformer according to the present invention, FIG. 1 is a perspective view showing a part of the core of the amorphous core transformer, and FIG. 2 is a measurement of iron loss of amorphous magnetic material. Figure 3 is a curved liJ diagram showing the relationship between the number of laminated cores and iron loss, Figure 4 is a dimensional diagram of the sample used in
The figure is a curve diagram showing the relationship between the clamping pressure and loss of the laminated core. Figure 1
Claims (1)
立てた積層鉄心を有するアモルファス鉄心変圧器におい
て、前記積層鉄心を0.05kg/cm^2ないし0.
5kg/cm^2の圧力で締付けることを特徴とするア
モルファス鉄心変圧器。 2)特許請求の範囲第1項記載のアモルファス鉄心変圧
器において、積層鉄心は焼なましを施したアモルファス
磁性材料を積重ねて組み立てたものであることを特徴と
するアモルファス鉄心変圧器。[Scope of Claims] 1) In an amorphous core transformer having a laminated core assembled by stacking a plurality of veneers of amorphous magnetic material, the laminated core has a weight of 0.05 kg/cm^2 to 0.05 kg/cm^2.
An amorphous iron core transformer characterized by tightening with a pressure of 5 kg/cm^2. 2) The amorphous core transformer according to claim 1, wherein the laminated core is assembled by stacking annealed amorphous magnetic materials.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP5594986A JPS62213104A (en) | 1986-03-13 | 1986-03-13 | Amorphous core transformer |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP5594986A JPS62213104A (en) | 1986-03-13 | 1986-03-13 | Amorphous core transformer |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS62213104A true JPS62213104A (en) | 1987-09-19 |
Family
ID=13013322
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP5594986A Pending JPS62213104A (en) | 1986-03-13 | 1986-03-13 | Amorphous core transformer |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS62213104A (en) |
-
1986
- 1986-03-13 JP JP5594986A patent/JPS62213104A/en active Pending
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