JPH06207972A - Measuring method for rotating magnetic field iron loss at outer core - Google Patents

Measuring method for rotating magnetic field iron loss at outer core

Info

Publication number
JPH06207972A
JPH06207972A JP288393A JP288393A JPH06207972A JP H06207972 A JPH06207972 A JP H06207972A JP 288393 A JP288393 A JP 288393A JP 288393 A JP288393 A JP 288393A JP H06207972 A JPH06207972 A JP H06207972A
Authority
JP
Japan
Prior art keywords
outer core
magnetic field
iron loss
rotating magnetic
measuring
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.)
Withdrawn
Application number
JP288393A
Other languages
Japanese (ja)
Inventor
Tomoyuki Abe
智之 阿部
Tsutomu Kaido
力 開道
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.)
Nippon Steel Corp
Original Assignee
Nippon Steel Corp
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 Nippon Steel Corp filed Critical Nippon Steel Corp
Priority to JP288393A priority Critical patent/JPH06207972A/en
Publication of JPH06207972A publication Critical patent/JPH06207972A/en
Withdrawn legal-status Critical Current

Links

Abstract

PURPOSE:To easily measure the iron loss of outer core including all effects by measuring rotatory force induced in the outer core. CONSTITUTION:If there is iron loss in an outer core 4 used in a rotating magnetic field, rotatory force is induced in the outer core 4. By letting the iron loss W (W), the induced rotatory force T (Nm), rotation number of the rotating magnetic field n (rpm) and the ratio of the circumference of a circle to its diameter pi, W is expressed as W=2pinT/60, and the iron loss of a magnetic material in a rotating magnetic field is measured only from the induced rotational force. The rotational force is not related with the outer core conditions, it can be evaluated in actually used state including all effects of shape, distortion, magnetic flux distribution, centrifugal force, plate number in the case of plate, layering method, fixing method, etc. For constitution, the two outer cores 4 as the sample are layered and fixed with a sample holder 8, which is rotated with an angle velocity of n0 in the rotating magnetic field of rotation number n+n0 given by three-phase power 1, magnetic field generation coil 2 and iron core 3, and induced rotatory force T and the rotation number n are detected 5.

Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【産業上の利用分野】本発明は、回転機などのアクチュ
エータや、発電機に使用されるアウターコアの回転磁界
中でのエネルギー損失の測定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 method for measuring energy loss in an rotating magnetic field of an actuator such as a rotating machine or an outer core used in a generator.

【0002】[0002]

【従来の技術】けい素鋼板などのアウターコアを回転機
に使用した場合の鉄損の評価は、JIS C2550に
記載されている電磁鋼板試験方法が一般的である。しか
し、この方法は、励磁方向が一方向で、回転機内部のア
ウターコアのような回転磁界が生じている場所での鉄損
評価には適さない。
2. Description of the Related Art The evaluation of iron loss when an outer core such as a silicon steel plate is used in a rotating machine is generally conducted by the electromagnetic steel plate test method described in JIS C2550. However, this method is not suitable for iron loss evaluation in a place where a rotating magnetic field is generated, such as the outer core inside the rotating machine, where the excitation direction is one direction.

【0003】回転磁界内での鉄損評価は、鉄損による温
度上昇を熱電対やサーミスタで測定して行う方法や、磁
束密度と磁界の大きさを2次元で測定して鉄損を求める
方法がある。これらの方法は、局所的な鉄損を求めた
り、均一磁束分布でしか測定できない。また、インナー
コアに限っていえば、回転磁界内でのインナーコアにか
かる回転力を測定することによる方法があるが、アウタ
ーコアの鉄損を測定できない。また、回転機のモデル機
を作製し、鉄損を評価することは、回転機の機械的な損
失や、巻線による損失などの影響が多すぎ、また、時間
と費用を要するため不可能に近い。
Iron loss evaluation in a rotating magnetic field is carried out by measuring the temperature rise due to iron loss with a thermocouple or thermistor, or by measuring the magnetic flux density and the magnitude of the magnetic field two-dimensionally to obtain the iron loss. There is. These methods can obtain local iron loss and can measure only with a uniform magnetic flux distribution. Further, if it is limited to the inner core, there is a method by measuring the rotational force applied to the inner core in the rotating magnetic field, but the iron loss of the outer core cannot be measured. In addition, it is impossible to make a model of a rotating machine and evaluate the iron loss because the mechanical loss of the rotating machine and the loss due to the winding are too much influence, and it takes time and cost. near.

【0004】以上より、一般に回転機はロータよりもス
テータの方が鉄損が大きく、かつステータがアウターに
なっている場合が多いにも関わらず、現在の測定法では
回転機中で実際に使用されている状態でのアウターコア
の鉄損を十分評価できない。従って、回転機にアウター
コアを使用する際に、アウターコアの位置付けが明らか
にできないために、磁性材料の選択や最適形状の設計が
十分にできない。
From the above, in general, in a rotating machine, although the stator has a larger iron loss than the rotor and the stator is often the outer side, the current measuring method actually uses the rotating machine in the rotating machine. It is not possible to fully evaluate the iron loss of the outer core in the state of being installed. Therefore, when the outer core is used in the rotating machine, it is not possible to clearly position the outer core, so that the selection of the magnetic material and the design of the optimum shape cannot be sufficiently performed.

【0005】[0005]

【発明が解決しようとする課題】この発明は、上記の問
題点を解決するためになされ、回転磁界中で使用される
アウターコアの鉄損を、形状、歪み、磁束分布、遠心
力、板状の場合は枚数、積層方法、接着方法、固定方法
などのあらゆる影響を含むアウターコアの回転磁界内鉄
損測定方法、あるいは回転機内鉄損測定方法を提供する
ものである。
SUMMARY OF THE INVENTION The present invention has been made to solve the above-mentioned problems, and the iron loss of the outer core used in a rotating magnetic field can be determined by the shape, strain, magnetic flux distribution, centrifugal force, plate shape, etc. In the case of (1), the present invention provides a method of measuring iron loss in a rotating magnetic field of an outer core or a method of measuring iron loss in a rotating machine, which includes all effects such as the number of sheets, a laminating method, a bonding method, and a fixing method.

【0006】[0006]

【課題を解決するための手段】本発明は、回転磁界中で
使用されるアウターコアの、前記回転磁界中で消費され
る鉄損を測定するにあたり、前記アウターコアに誘起さ
れる回転力を測定することにより鉄損を容易に求めるこ
とを特徴とするアウターコアの回転磁界鉄損測定方法で
ある。
According to the present invention, in measuring the iron loss of an outer core used in a rotating magnetic field, which is consumed in the rotating magnetic field, the rotating force induced in the outer core is measured. This is a method for measuring the rotating field iron loss of the outer core, which is characterized in that the iron loss is easily obtained by performing the above.

【0007】回転磁界中で使用されているアウターコア
に鉄損があると、そのアウターコアに回転力が誘起され
る。このときの鉄損W(W)は、誘起される回転力T(N
m)、鉄損を起こすアウターコアに対する回転磁界の回転
数をn(rpm)、円周率をπとすると、W=2πnT/6
0で表すことができ、回転磁界中での磁性材料の鉄損は
誘起される回転力だけで測定することができる。回転力
はアウターコアの条件に関係ないので、形状、歪み、磁
束分布、遠心力、板状の場合は枚数、積層方法、接着方
法、固定方法などの影響を全て含む、実際にアウターコ
アが使用されている状態で鉄損を評価することになる。
When the outer core used in the rotating magnetic field has iron loss, a rotating force is induced in the outer core. At this time, the iron loss W (W) is the induced rotational force T (N
m), the rotating speed of the rotating magnetic field with respect to the outer core that causes iron loss is n (rpm), and the pi is π, W = 2πnT / 6
It can be represented by 0, and the iron loss of the magnetic material in the rotating magnetic field can be measured only by the induced rotational force. Rotational force is not related to the condition of the outer core, so the outer core is actually used, including the influence of shape, strain, magnetic flux distribution, centrifugal force, number of sheets in case of plate shape, lamination method, bonding method, fixing method, etc. The iron loss will be evaluated under the condition.

【0008】本発明のアウターコアの回転磁界鉄損測定
方法でのアウターコアとは、ステータでもロータでもど
ちらでもよく、また、電機子コアでも、界磁コアのどち
らでもよく、外側にあるコアのことをいう。試料を励磁
するときの磁束分布が一定の大きさである必要はなく、
外側にあるコアに回転磁界がかかればよい。
The outer core in the method for measuring the iron loss of the rotating magnetic field of the outer core of the present invention may be either a stator or a rotor, and may be an armature core or a field core. Say that. The magnetic flux distribution when exciting the sample does not have to be a constant magnitude,
A rotating magnetic field should be applied to the outer core.

【0009】本発明の回転磁界とは、鉄損の測定を行う
アウターコア(以後測定試料と記す)に対する磁界の動
きを示すものであり、測定試料と外部磁場のどちらか一
方、あるいは双方が回転し、測定試料に対して相対的に
磁界が回転する場合をいい、外部磁場は電磁石、もしく
は永久磁石でもよい。外部磁界は一定の大きさと方向を
もつ必要はなく、場所によって変化してもよく、磁束分
布をもってもよい。更に、外部磁界と測定試料の位置関
係により磁束分布が変化しても、一回転して同じ角度で
同じ磁束分布になればよい。
The rotating magnetic field of the present invention indicates the movement of a magnetic field with respect to an outer core (hereinafter referred to as a measurement sample) for measuring iron loss, and either one or both of the measurement sample and the external magnetic field rotates. The magnetic field rotates relative to the measurement sample, and the external magnetic field may be an electromagnet or a permanent magnet. The external magnetic field does not have to have a constant magnitude and direction, may change depending on the location, and may have a magnetic flux distribution. Further, even if the magnetic flux distribution changes depending on the positional relationship between the external magnetic field and the measurement sample, it is sufficient that the magnetic flux distribution makes one rotation and the same magnetic flux distribution at the same angle.

【0010】測定試料に対する相対的な回転数n(rpm)
の回転磁界中で停止しているアウターコアの回転磁界に
よる鉄損を測定する場合に、アウターコアを磁気特性に
あまり影響しない程度の低い回転数n0 で回転させ、外
部回転磁界の回転数をn+n0 (rpm)で回転させること
により、摩擦力による測定誤差を低減してもよい。当然
回転数は、外部回転磁界の回転方向を考慮する必要があ
る。この場合、外部磁場が電磁石による場合、磁束が0
のときの回転力T0 を測定しておき、外部磁場を印加し
たときの回転力T1 との差T1 −T0 を測定すること
や、外部磁場が永久磁石による場合、磁束が0の状態を
つくるために測定試料を永久磁石の影響を受けない程度
に離して回転力T0 ′を測定しておき、外部磁場を印加
するために測定試料を回転磁界中に挿入したときの回転
力T1 ′との差を測定することで測定誤差を低減しても
よい。
Relative speed n (rpm) relative to the measurement sample
When measuring the iron loss due to the rotating magnetic field of the outer core stopped in the rotating magnetic field, the outer core is rotated at a low rotating speed n 0 that does not affect the magnetic characteristics so much that the rotating speed of the external rotating magnetic field is By rotating at n + n 0 (rpm), measurement error due to frictional force may be reduced. As a matter of course, the rotation speed needs to consider the rotation direction of the external rotating magnetic field. In this case, when the external magnetic field is an electromagnet, the magnetic flux is 0
Leave measuring the rotational force T 0 when the, or measuring the difference T 1 -T 0 of the rotational force T 1 of the time of applying an external magnetic field, when the external magnetic field by the permanent magnets, the magnetic flux is zero In order to create the state, the rotational force T 0 ′ is measured by separating the measurement sample so that it is not affected by the permanent magnet, and the rotational force when the measurement sample is inserted into the rotating magnetic field to apply the external magnetic field. The measurement error may be reduced by measuring the difference from T 1 ′.

【0011】電磁石は、コアに巻線して、試料に磁界を
与えるものであるが、その巻線方法は、従来のモータな
どで使用されている巻線方法や、その他の可能な巻線方
法でもよい。コアは、ティースのついたものや、必要な
ければティースのないものでもよい。永久磁石や、電磁
石の極数は、二極だけでなく、四極以上でもよい。
The electromagnet is wound around the core to give a magnetic field to the sample. The winding method is the winding method used in the conventional motors or other possible winding methods. But it's okay. The core may be with teeth or without teeth if not required. The number of poles of the permanent magnet or electromagnet is not limited to two, and may be four or more.

【0012】アウターコアとは、いかなる種類の磁性材
料、形状、使用法でもよく、けい素鋼板などのような、
板状のものを1枚もしくは2枚以上積層したものから、
磁性材料との複合材料の成形品や、フェライト、アルミ
ダイキャスト製品、付属品が付いている場合などの1体
または数個のものよりなるものでもよい。
The outer core may be any kind of magnetic material, shape and usage, such as silicon steel plate.
From one plate or a laminate of two or more,
It may be a molded product of a composite material with a magnetic material, a ferrite, an aluminum die-cast product, or one or several pieces such as those with accessories.

【0013】アウターコアの応用製品とは、モータなど
のアクチュエータや、発電機など、アウターコアが回転
磁界の生じている場所で用いられている場合のことをい
う。積層法とは、アウターコアが板状の場合、2枚以上
のコアを角度を変えて積む、まわし積みを行うことがあ
るが、このようなアウターコアの積み方のことをいう。
測定試料と試料ホルダーの固定は、歪みが入らないよう
に押え込んだり、はめ込んだり、両面もしくは片面テー
プを用いたり、接着剤でとめたり、実機の固定法または
これに準ずる方法でもよい。
The applied product of the outer core refers to a case where the outer core is used in a place where a rotating magnetic field is generated, such as an actuator such as a motor or a generator. The laminating method refers to a method of stacking outer cores, in which two or more cores are stacked at different angles when the outer cores are plate-shaped, but the outer cores are stacked.
The sample to be measured and the sample holder may be fixed by pressing, fitting, using a double-sided or single-sided tape, fixing with an adhesive, fixing the actual machine, or a method similar to this, so that distortion does not enter.

【0014】[0014]

【実施例】本発明を実施例の図を参照しながら説明す
る。 実施例1 図1および図2は、三相電源1、磁界発生コイル2と鉄
心3により得られる回転数n+n0 の回転磁界中で、単
純化した形状であるティースなしのアウターコア4を2
枚積層して、角速度n0 で回転させ、回転数nの回転磁
界による鉄損を測定する装置であり、5は測定試料であ
るアウターコア4に誘起する回転力と回転数を検出する
検出器、6は試料であるアウターコア4を一定回転、も
しくは静止させるモータとブレーキであり、8はアウタ
ーコアを固定する試料ホルダーである。
The present invention will be described with reference to the drawings of the embodiments. Example 1 FIGS. 1 and 2 show a simplified outer core 4 without teeth in a rotating magnetic field of a rotational speed n + n 0 obtained by a three-phase power source 1, a magnetic field generating coil 2 and an iron core 3.
An apparatus for measuring iron loss due to a rotating magnetic field having a rotation speed n by laminating the sheets and rotating them at an angular velocity n 0 , and 5 is a detector for detecting the rotation force and the rotation speed induced in the outer core 4 as a measurement sample. , 6 are motors and brakes for rotating or stopping the outer core 4 which is a sample at a constant speed, and 8 is a sample holder for fixing the outer core.

【0015】図2は図1のA方向から見た矢視図であ
る。この場合も回転数n+n0 で回転する座標軸で考え
ると、アウターコア4には回転数nの回転磁界がかかる
ので、W=2πnT/60の関係式により、アウターコ
ア4に誘起する回転力Tを測定することで回転磁界によ
る鉄損Wを求めることができる。アウターコア4が停止
状態である場合には、摩擦力による回転力の不安定が生
じるので、この実施例では、アウターコア4をその影響
がなくなる、できるだけ低い回転数で回転させ、測定精
度を高めている。試料ホルダー8とアウターコア4の固
定は、試料ホルダー8にはアウターコア4に合う適当な
形状のものを使用してアウターコア4をはめ込んでもよ
いし、接着剤でアウターコア4に歪みが入らないように
アウターコア4を試料ホルダー8に固定してもよいし、
鉄損に影響を及ぼさない押え板でアウターコア4を固定
してもよい。
FIG. 2 is a view seen from the direction A in FIG. Also in this case, considering the coordinate axis rotating at the rotation speed n + n 0 , the rotating magnetic field having the rotation speed n is applied to the outer core 4, so that the rotating force T induced on the outer core 4 is calculated by the relational expression W = 2πnT / 60. By measuring, the iron loss W due to the rotating magnetic field can be obtained. When the outer core 4 is in a stopped state, the rotational force becomes unstable due to frictional force. Therefore, in this embodiment, the outer core 4 is rotated at a rotational speed as low as possible so that the influence thereof is eliminated, thereby improving the measurement accuracy. ing. The sample holder 8 and the outer core 4 may be fixed by fitting the outer core 4 to the sample holder 8 by using an appropriate shape that fits the outer core 4 or by using an adhesive so that the outer core 4 is not distorted. As described above, the outer core 4 may be fixed to the sample holder 8,
The outer core 4 may be fixed by a holding plate that does not affect the iron loss.

【0016】実施例2 図3および図4は直流電流により発生する磁界中で、実
際の形状であるティースつきのアウターコア12一枚を
回転させることによりアウターコア12に回転磁界をか
け、回転磁界による鉄損を回転力によって測定する装置
である。図4は図3のB方向から見た矢視図である。9
は直流電源、10は直流磁界を発生させるためのコイ
ル、11は直流磁界を発生させるための鉄心、12は回
転磁界による鉄損を測定する試料であるアウターコア、
13は測定試料であるアウターコア12に誘起する回転
力と回転数を検出する検出器で、14は試料であるアウ
ターコア12を一定回転もしくは静止させるモータとブ
レーキ、16はアウターコアを固定する試料ホルダーで
ある。前記実施例1と同じように、試料であるアウター
コア12には、アウターコア12が回転することで相対
的に回転磁界がかかっているので、アウターコア12の
回転磁界による鉄損が求められる。
Embodiment 2 In FIGS. 3 and 4, a rotating magnetic field is applied to the outer core 12 by rotating one outer core 12 with teeth, which is an actual shape, in a magnetic field generated by a direct current, and It is a device that measures iron loss by rotational force. FIG. 4 is a view seen from the direction B in FIG. 9
Is a DC power supply, 10 is a coil for generating a DC magnetic field, 11 is an iron core for generating a DC magnetic field, 12 is an outer core which is a sample for measuring iron loss due to a rotating magnetic field,
Reference numeral 13 is a detector for detecting the rotational force and the number of revolutions induced in the outer core 12 which is a measurement sample, 14 is a motor and a brake for rotating or stopping the outer core 12 which is a sample at a constant speed, and 16 is a sample for fixing the outer core. It is a holder. As in Example 1, the outer core 12 as a sample is relatively subjected to a rotating magnetic field as the outer core 12 rotates, so iron loss due to the rotating magnetic field of the outer core 12 is required.

【0017】実施例3 図5および図6は永久磁石18により発生する磁界中
で、実際の形状であるティースつきかつ巻線が施された
状態のアウターコア12一枚を、永久磁石を回転させる
ことによりアウターコア12に回転磁界をかけ、回転磁
界による鉄損を回転力によって測定する装置である。図
6は図5のC方向から見た矢視図である。17は永久磁
石を回転させるモータ、18は磁界を発生させるための
永久磁石、19は回転磁界による鉄損を測定する試料で
あるアウターコア、20は測定試料であるアウターコア
19に誘起する回転力と回転数を検出する検出器で、2
1は試料であるアウターコア19を一定回転もしくは静
止させるモータとブレーキ、23はアウターコアを固定
する試料ホルダー、24は誘導電流が流れないように短
絡していない巻線である。前記実施例1と同じように、
試料であるアウターコア19には、永久磁石18が回転
することで、相対的に回転磁界がかかっているので、ア
ウターコア12の回転磁界による鉄損が求められる。ア
ウターコア19が停止状態である場合には、摩擦力によ
る回転力の不安定が生じるので、この実施例3では実施
例1と同様に、アウターコア19を摩擦力の影響がなく
なる、できるだけ低い回転数で回転させ、測定精度を高
めている。
Embodiment 3 FIG. 5 and FIG. 6 rotate the permanent magnet in the magnetic field generated by the permanent magnet 18 by rotating one outer core 12 having an actual shape with teeth and wound. With this, a rotating magnetic field is applied to the outer core 12, and the iron loss due to the rotating magnetic field is measured by the rotating force. FIG. 6 is a view seen from the direction C in FIG. Reference numeral 17 is a motor for rotating a permanent magnet, 18 is a permanent magnet for generating a magnetic field, 19 is an outer core that is a sample for measuring iron loss due to a rotating magnetic field, and 20 is a rotational force induced in an outer core 19 that is a measurement sample. And a detector that detects the number of revolutions, 2
Reference numeral 1 is a motor and a brake for rotating or stationary the outer core 19 which is a sample, 23 is a sample holder for fixing the outer core, and 24 is a winding which is not short-circuited so that an induced current does not flow. As in Example 1 above,
Since the rotating magnetic field is relatively applied to the outer core 19 as a sample by the rotation of the permanent magnet 18, the iron loss due to the rotating magnetic field of the outer core 12 is required. When the outer core 19 is in the stopped state, the rotational force becomes unstable due to the frictional force. Therefore, in the third embodiment, as in the first embodiment, the outer core 19 is not affected by the frictional force, and the rotational speed is as low as possible. Rotate by a number to improve measurement accuracy.

【0018】実施例4 アウターコアが板状で、2枚以上積層し、前記図1、ま
たは図2で測定した場合、層間の絶縁が破れると、測定
試料の渦電流損の増加分ΔWにともない、ΔW=2πn
ΔT/60で表される分だけ回転力がΔTだけ増える。
層間の絶縁が破れていない測定試料Aと、層間の絶縁が
破れた測定試料Bの回転力を測定する。ただし、AとB
は、測定試料は2枚以上積層したもので、単位体積当た
りの鉄損に影響を及ぼす要因が、前記層間抵抗以外全く
同じ条件である。測定試料A,Bの単位体積当たりの鉄
損に差が現れたとき、層間の絶縁が破れていることにな
るので、このことを用いて層間の絶縁破壊の検出が可能
である。表1は周波数50Hz、磁束密度1.0Tで、外
径17cm程度、内径6cm程度、板厚0.5mm程度のアウ
ターコアの絶縁が破れた場合の前記図1の測定法で測定
した鉄損を示している。
Example 4 In the case where two or more outer cores are laminated in a plate shape and are measured in FIG. 1 or 2, when the insulation between layers is broken, the eddy current loss of the measurement sample is increased by ΔW. , ΔW = 2πn
The rotational force increases by ΔT by the amount represented by ΔT / 60.
The rotational force of measurement sample A in which the insulation between layers is not broken and measurement sample B in which the insulation between layers is broken are measured. However, A and B
Is a laminate of two or more measurement samples, and the factors that affect the iron loss per unit volume are exactly the same except the interlayer resistance. When a difference appears in the iron loss per unit volume of the measurement samples A and B, it means that the insulation between layers is broken, and this can be used to detect the insulation breakdown between layers. Table 1 shows the iron loss measured by the measuring method of FIG. 1 when the insulation of the outer core with a frequency of 50 Hz, a magnetic flux density of 1.0 T, an outer diameter of about 17 cm, an inner diameter of about 6 cm, and a plate thickness of about 0.5 mm is broken. Shows.

【0019】[0019]

【表1】 [Table 1]

【0020】[0020]

【発明の効果】本発明の測定法によると、従来法ではで
きなかった実機状態での鉄損の測定、つまり、いかなる
複雑な形状やあらゆる使用状況でも回転磁界でのアウタ
ーコアの鉄損を測定することが容易に可能になり、しか
も、アウターコア全体で消費する全鉄損を容易に測定す
ることができる。これはアウターコアが用いられている
製品内で生じる回転磁界でもよく、アウターコアの応用
される状態での全鉄損を直接測定できる。従って、モー
タなどのアクチュエータや、発電機の設計を行う上で必
要な鉄損に関する情報を直接得ることができる。
According to the measuring method of the present invention, it is possible to measure the iron loss in the actual machine state, which is not possible by the conventional method, that is, the iron loss of the outer core in the rotating magnetic field under any complicated shape and any usage condition. In addition, it is possible to easily measure the total iron loss consumed in the entire outer core. This may be a rotating magnetic field generated in the product in which the outer core is used, and the total iron loss in the applied state of the outer core can be directly measured. Therefore, it is possible to directly obtain information about the iron loss necessary for designing actuators such as motors and generators.

【0021】この発明は、アクチュエータや発電機だけ
でなく、回転磁界の生じている所で使用されるアウター
コアに適用できる。また、逆に、実機のアウターコアの
状態だけでなく、実機枚数以下の一枚などで測定可能で
あり、設計のための簡易試験、コア形状決定に役立てる
ことができる。実機状態で鉄損の測定ができるため、コ
ア加工時の歪みの影響や、歪み取り焼鈍後のコアの鉄損
を測定でき、モータなどに組立以前に、より実際的な評
価が可能で非常に便利である。この鉄損評価方法は、モ
ータなどでの機械損失などの影響がきわめて小さくでき
るので、従来のモータなどでの全エネルギー損失から機
械損、銅損などを除いて求める鉄損評価法より精度が高
い。コアに巻線を施した状態や、コアをケースに固定し
た状態で、モータに完全に組立される以前にコア鉄損の
評価ができる。以上のように、モータなどの鉄損低減お
よび設計、モータなどの損失低減方策探索には非常に有
効な手段である。
The present invention can be applied not only to an actuator and a generator, but also to an outer core used where a rotating magnetic field is generated. On the contrary, not only the condition of the outer core of the actual machine but also the actual number of sheets less than the actual machine can be measured, which can be used for a simple test for design and determination of the core shape. Since the iron loss can be measured in the actual machine state, it is possible to measure the effect of strain during core processing and the core loss of the core after strain relief annealing, and it is possible to make a more practical evaluation before assembling the motor etc. It is convenient. This iron loss evaluation method is much more accurate than the iron loss evaluation method found by excluding mechanical loss, copper loss, etc. from total energy loss in conventional motors, etc., because the effects of mechanical loss in motors, etc. can be made extremely small. . The core iron loss can be evaluated before the motor is completely assembled with the core wound and the core fixed to the case. As described above, it is a very effective means for iron loss reduction and design of motors and the like, and search for loss reduction measures for motors and the like.

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

【図1】回転磁界を励磁コイルで発生することで回転磁
界中で測定を実施している例である。
FIG. 1 is an example in which measurement is performed in a rotating magnetic field by generating a rotating magnetic field with an exciting coil.

【図2】図1の矢視図である。FIG. 2 is a view on arrow in FIG.

【図3】測定試料が回転することで測定試料に対する回
転磁界を発生している例である。
FIG. 3 is an example in which a rotating magnetic field for the measurement sample is generated by rotating the measurement sample.

【図4】図3の矢視図である。FIG. 4 is a view on arrow of FIG.

【図5】回転磁界による鉄損を回転力によって測定する
装置の例である。
FIG. 5 is an example of an apparatus for measuring iron loss due to a rotating magnetic field by a rotating force.

【図6】図5のC方向から見た矢視図である。FIG. 6 is a view seen from the direction C in FIG.

【符号の説明】[Explanation of symbols]

1 回転磁界を発生させる三相電源 2,10 磁界を発生させるコイル 3,11 鉄心 4,12,19 回転磁界による鉄損を測定する試料で
あるアウターコア 5,13,20 アウターコアに誘起する回転力と回転
数を検出する検出器 6,14,21 試料であるアウターコアを一定回転、
もしくは静止させるモータとブレーキ 8,16,23 試料を回転させるモータ 9 直流電源 17 永久磁石を回転させるモータ 18 永久磁石 24 短絡していない巻線
1 Three-phase power supply that generates a rotating magnetic field 2,10 Coil that generates a magnetic field 3,11 Iron core 4,12,19 Outer core that is a sample for measuring iron loss due to a rotating magnetic field 5,13,20 Rotation induced in the outer core Detector for detecting force and rotation speed 6, 14, 21 Constant rotation of outer core, which is a sample,
Alternatively, a motor and a brake to be stationary 8,16,23 A motor for rotating a sample 9 A DC power supply 17 A motor for rotating a permanent magnet 18 A permanent magnet 24 A winding which is not short-circuited

Claims (10)

【特許請求の範囲】[Claims] 【請求項1】 回転磁界内で使用されるアウターコア
の、前記回転磁界中で消費される時のエネルギー損失を
測定するにあたり、前記アウターコアに誘起される回転
力を測定することにより、エネルギー損失を求めること
を特徴とするアウターコアの回転磁界鉄損測定方法。
1. When measuring the energy loss of an outer core used in a rotating magnetic field when it is consumed in the rotating magnetic field, the energy loss is measured by measuring the rotational force induced in the outer core. A method for measuring the iron loss of a rotating magnetic field of an outer core, which comprises:
【請求項2】 回転磁界中でのエネルギー損失を測定す
るアウターコアが、形状、歪み、磁束分布、遠心力など
のような、エネルギー損失に影響するあらゆる要因を含
むことを特徴とする請求項1記載のアウターコアの回転
磁界鉄損測定方法。
2. The outer core for measuring energy loss in a rotating magnetic field includes all factors that affect energy loss, such as shape, strain, magnetic flux distribution, centrifugal force and the like. A method for measuring a rotating magnetic field iron loss of an outer core as described.
【請求項3】 回転磁界中でのエネルギー損失を測定す
るアウターコアが、アウターコアの応用製品に使用され
る状態であることを特徴とする請求項1または2記載の
アウターコアの回転磁界鉄損測定方法。
3. The rotating magnetic field iron loss of an outer core according to claim 1, wherein the outer core for measuring energy loss in a rotating magnetic field is in a state of being used in an applied product of the outer core. Measuring method.
【請求項4】 板状のアウターコアを使用する場合に、
積層法がアウターコアの応用製品に使用される状態であ
ることを特徴とする請求項1,2または3記載のアウタ
ーコアの回転磁界鉄損測定方法。
4. When using a plate-shaped outer core,
The method for measuring the iron loss of an outer core according to claim 1, 2, or 3, wherein the lamination method is used for an outer core application product.
【請求項5】 板状のアウターコアを使用する場合に、
接着法がアウターコアの応用製品に使用される状態であ
ることを特徴とする請求項1,2,3または4記載のア
ウターコアの回転磁界鉄損測定方法。
5. When using a plate-shaped outer core,
The method for measuring the iron loss of an outer core according to claim 1, 2, 3 or 4, wherein the bonding method is in a state of being used for an outer core application product.
【請求項6】 板状のアウターコアを使用する場合に、
固定法がアウターコアの応用製品に使用される状態であ
ることを特徴とする請求項1,2,3,4または5記載
のアウターコアの回転磁界鉄損測定方法。
6. When using a plate-shaped outer core,
The method for measuring a rotating magnetic field iron loss of an outer core according to claim 1, 2, 3, 4 or 5, wherein the fixing method is a state in which the fixing method is used for an applied product of the outer core.
【請求項7】 板状のアウターコアを使用する場合に、
積層枚数が1枚、もしくはアウターコアの応用製品に使
用される状態の枚数未満であることを特徴とする請求項
1,2,3,4,5または6記載のアウターコアの回転
磁界鉄損測定方法。
7. When using a plate-shaped outer core,
The outer magnetic core iron loss measurement of the outer core according to claim 1, 2, 3, 4, 5 or 6, wherein the number of laminated layers is one or less than the number of sheets used in an applied product of the outer core. Method.
【請求項8】 板状のアウターコアを使用する場合に、
積層枚数がアウターコアの応用製品に使用される状態で
あることを特徴とする請求項1,2,3,4,5,6ま
たは7記載のアウターコアの回転磁界鉄損測定方法。
8. When using a plate-shaped outer core,
The method for measuring the iron loss of an outer core according to claim 1, 2, 3, 4, 5, 6 or 7, wherein the number of laminated layers is in a state of being used for an outer core application product.
【請求項9】 回転数がn(rpm)の回転磁界中で停止し
ているアウターコアの回転磁界によるエネルギー損失を
測定することにおいて、前記アウターコアを回転数n0
(rpm)ほど回転させ、外部の回転磁界の回転数をn+n
0 (rpm)とすることを特徴とする請求項1,2,3,
4,5,6,7または8記載のアウターコアの回転磁界
鉄損測定方法。
9. In measuring the energy loss due to the rotating magnetic field of the outer core stopped in a rotating magnetic field having a rotating speed of n (rpm), the outer core is rotated at a rotating speed of n 0.
Rotate about (rpm) and change the rotation speed of the external rotating magnetic field to n + n
It is set to 0 (rpm), Claims 1, 2, 3,
4, 5, 6, 7 or 8 outer core magnetic field magnetic field iron loss measuring method.
【請求項10】 アウターコアを励磁する場合におい
て、励磁を永久磁石を用いる、あるいは電磁石を用いて
回転磁界を発生させることを特徴とする請求項1,2,
3,4,5,6,7,8または9記載のアウターコアの
回転磁界鉄損測定方法。
10. When exciting the outer core, exciting is performed by using a permanent magnet or an electromagnet to generate a rotating magnetic field.
A rotating magnetic field iron loss measuring method for an outer core according to 3, 4, 5, 6, 7, 8 or 9.
JP288393A 1993-01-11 1993-01-11 Measuring method for rotating magnetic field iron loss at outer core Withdrawn JPH06207972A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP288393A JPH06207972A (en) 1993-01-11 1993-01-11 Measuring method for rotating magnetic field iron loss at outer core

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP288393A JPH06207972A (en) 1993-01-11 1993-01-11 Measuring method for rotating magnetic field iron loss at outer core

Publications (1)

Publication Number Publication Date
JPH06207972A true JPH06207972A (en) 1994-07-26

Family

ID=11541763

Family Applications (1)

Application Number Title Priority Date Filing Date
JP288393A Withdrawn JPH06207972A (en) 1993-01-11 1993-01-11 Measuring method for rotating magnetic field iron loss at outer core

Country Status (1)

Country Link
JP (1) JPH06207972A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2013069467A1 (en) * 2011-11-07 2013-05-16 日産自動車株式会社 Magnetic body evaluation device and method

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2013069467A1 (en) * 2011-11-07 2013-05-16 日産自動車株式会社 Magnetic body evaluation device and method
CN103930775A (en) * 2011-11-07 2014-07-16 日产自动车株式会社 Magnetic body evaluation device and method
JPWO2013069467A1 (en) * 2011-11-07 2015-04-02 日産自動車株式会社 Magnetic body evaluation apparatus and method
US10241080B2 (en) 2011-11-07 2019-03-26 Nissan Motor Co., Ltd. Magnet evaluation device and method

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