JPS6047829B2 - Magnetic flux detection method for rotating electrical machines - Google Patents
Magnetic flux detection method for rotating electrical machinesInfo
- Publication number
- JPS6047829B2 JPS6047829B2 JP53008026A JP802678A JPS6047829B2 JP S6047829 B2 JPS6047829 B2 JP S6047829B2 JP 53008026 A JP53008026 A JP 53008026A JP 802678 A JP802678 A JP 802678A JP S6047829 B2 JPS6047829 B2 JP S6047829B2
- Authority
- JP
- Japan
- Prior art keywords
- magnetic flux
- rotor
- magnetic field
- rotating electrical
- detection method
- 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
Links
Description
【発明の詳細な説明】
本発明は、スリップリング等の回転体との接触機構を介
さずに回転電機の2次電流の実際値を導出する回転電機
の磁束検出方法に係る。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a magnetic flux detection method for a rotating electrical machine that derives an actual value of a secondary current of the rotating electrical machine without using a contact mechanism such as a slip ring with a rotating body.
交流回転電機の動特性運転の手段として、空隙主磁束の
空間的位置・大きさの実際値を把握した磁界オリエンテ
ーション制御による、いわゆるベクトル制御法がある。As a means of dynamically operating an AC rotating electrical machine, there is a so-called vector control method, which uses magnetic field orientation control based on the actual values of the spatial position and magnitude of the main magnetic flux in the air gap.
それには回転電機の2次電流つまりそれによる磁束の検
出を無接触で行なうことが理想的である。ここに本発明
は、固定子の空隙面に磁界検出素子を2個整置すること
により、望まれる磁界の検出ができる手法を提供しよう
とするものである。For this purpose, it is ideal to detect the secondary current of the rotating electric machine, that is, the magnetic flux caused by it, without contact. Here, the present invention attempts to provide a method in which a desired magnetic field can be detected by arranging two magnetic field detection elements on the air gap surface of the stator.
本発明の原理はこうである。たとえば、第1図に示すよ
うに、導体1に紙面の表面の方向に向けて電流を通じる
と、点線で表わし、かつ矢印の方向性をもつた磁束が生
起する。The principle of the present invention is as follows. For example, as shown in FIG. 1, when a current is passed through the conductor 1 toward the surface of the paper, magnetic flux is generated, which is represented by a dotted line and has the direction of the arrow.
そこで同一線上で、第1図ではX軸上の導体1の中心よ
り等距離の点A、Bにおいては、y軸方向の磁束成分の
位相が電気角て1800違つていることがわかる。Therefore, it can be seen that, on the same line, the phases of the magnetic flux components in the y-axis direction differ by 1800 electrical degrees at points A and B, which are equidistant from the center of the conductor 1 on the X-axis in FIG.
第2図は、本発明の一実施例の説明図である。FIG. 2 is an explanatory diagram of one embodiment of the present invention.
たとえば、導体をスキューした回転子を有するかご形誘
導電動機の固定子空隙面を考えよう。さて、第2図は固
定子空隙面に投影した回転子の部分展開図で、3は導体
、4は短絡環、θはスキュー角(機械角)、れは回転子
鉄心積厚、を。は固定子空隙面に投影した回転子のスロ
ットピッチ、、mはその中心線、aは回転子の軸、Al
、A。は距離1を隔てた中心線mに関して対象の位置で
ある。しかして、スキュー角θを考慮してロータスズロ
ッドのパーミアンスが同じになるところを導出すれはて
ある。For example, consider the stator air plane of a squirrel cage induction motor with a rotor with skewed conductors. Now, Figure 2 is a partially developed view of the rotor projected onto the stator gap plane, where 3 is the conductor, 4 is the short-circuit ring, θ is the skew angle (mechanical angle), and is the rotor core thickness. is the slot pitch of the rotor projected onto the stator gap plane, m is its center line, a is the axis of the rotor, Al
,A. is the position of the object with respect to the centerline m separated by a distance 1. Therefore, the point at which the permeance of the lotus tin rods becomes the same can be derived by considering the skew angle θ.
かご形回転子の導体にスキューを施すと、導体に流れる
2次電流は、軸方向成分と円周方向成分とに分けられる
。When the conductors of the squirrel cage rotor are skewed, the secondary current flowing through the conductors is divided into an axial component and a circumferential component.
それらの作る磁界を固定子空隙面において、同一軸a方
向線上て(1式)の距離lだけ離れ、かつ鉄心積厚の中
心mに対して対称な2点・A1とA2て観測すると、軸
方向成分の電流が作る磁束は同位相となるが、円周方向
の電流が作る磁束の位相は電気角1800違つている。
また、回転磁界についてみると同位相になつている。し
たがつて、磁界検出器を設置し、両者の検出出力を引算
、つまり差を求めることにより、導体に流れる電流の円
周方向成分の作る磁界の量のみが残り、結局、2次電流
に比例した量を取り出す,ことができる。ここで、同一
パーミアンスの突極の点として、中心線mと軸aの交点
〜もある。If we observe the magnetic field generated by these on the stator gap plane at two points A1 and A2, which are spaced apart by a distance l on the same axis a direction line (equation 1) and symmetrical with respect to the center m of the core thickness, we can see that the axis The magnetic fluxes produced by the currents in the directional components have the same phase, but the phases of the magnetic fluxes produced by the currents in the circumferential direction differ by 1800 electrical degrees.
Furthermore, when looking at the rotating magnetic fields, they are in the same phase. Therefore, by installing a magnetic field detector and subtracting the detection outputs of the two, that is, finding the difference, only the amount of magnetic field created by the circumferential component of the current flowing through the conductor remains, and in the end, it becomes the secondary current. It is possible to take out a proportionate amount. Here, as points of salient poles having the same permeance, there is also the intersection of the center line m and the axis a.
第3図は、本発明の他の実施例の断面図を示す。FIG. 3 shows a cross-sectional view of another embodiment of the invention.
5は電動機固定子、6は回転子、7はフレーニム、8は
コイルエンド、10・11は磁界検出器てある。5 is a motor stator, 6 is a rotor, 7 is a frame, 8 is a coil end, and 10 and 11 are magnetic field detectors.
つまり、この他の実施例は電動機の固定子5・回転子6
の空隙面に磁束検出素子を設置する代りに回転子軸を含
む断面に平行な成分の磁界を検出できるようにして、固
定子鉄心に磁界検出器10,11を設置するようにした
ものである。In other words, in this other embodiment, the stator 5 and rotor 6 of the electric motor are
Instead of installing a magnetic flux detection element on the air gap surface, magnetic field detectors 10 and 11 are installed on the stator core so as to be able to detect magnetic field components parallel to the cross section including the rotor axis. .
もつとも、回転子6に空隙を介して対向する固定子5の
内周面に、(1)式が成立する1を距てて磁界検出器1
0,11を、設置してもよいことは明らかである。従来
の電動機の2次電流は巻線形を除き計算により導出して
いるが、回転子の温度が変化すれば抵抗値が変り、電流
の実際値は計算値と異なつてくる。However, the magnetic field detector 1 is installed on the inner peripheral surface of the stator 5, which faces the rotor 6 through an air gap, at a distance of 1 for which equation (1) holds.
It is clear that 0 and 11 may be installed. The secondary current of conventional motors is derived by calculation, excluding the windings, but if the temperature of the rotor changes, the resistance value will change, and the actual value of the current will differ from the calculated value.
このことは、制御を行なう場合、指令値と実際値とが異
なることにり、良好な制御ができなくなる。本発明によ
れば、回転子の回路定数の温度変化等周囲環境に無関係
に、かつ無接触で、電流の実際値を知得でき、良好な回
転電機の運転制御が可能となる。This means that when performing control, the command value and actual value are different, making it impossible to perform good control. According to the present invention, the actual value of the current can be obtained without contact, regardless of the surrounding environment such as a temperature change in the circuit constant of the rotor, and the operation of the rotating electric machine can be properly controlled.
第1図は導線電流と磁束の関係図、第2図は本発明の一
実施例の説明図、第3図は本発明の他の実施例の構成図
てある。
1・・・・・・導体、2・・・・・・磁束、3・・・・
・・回転電機2次導体、4・・・・・・短絡環、5・・
・・・・固定子、6・・・・・・回転子でその鉄心の積
厚方向の中心線をMl7・・・・・・フレーム、8・・
・・・・コイルエンド、10・11・・・・・・磁界検
出器、a・・・・・・回転電機回転軸。FIG. 1 is a diagram showing the relationship between conductor current and magnetic flux, FIG. 2 is an explanatory diagram of one embodiment of the present invention, and FIG. 3 is a diagram of the configuration of another embodiment of the present invention. 1...Conductor, 2...Magnetic flux, 3...
...Rotating electric machine secondary conductor, 4...Short-circuit ring, 5...
...Stator, 6...Rotor, set the center line of the core in the stacking thickness direction Ml7...Frame, 8...
... Coil end, 10/11 ... Magnetic field detector, a ... Rotating electric machine rotating shaft.
Claims (1)
子空隙面において、鉄心積厚の中心に対し対象でかつ相
互の距離lについてl=(t_2/2)cotθ t_2は、固定子空隙面に投影した回転子のスロットピ
ッチ、θはスキュー角(機械角度) となるような2点にそれぞれ磁界検出器を設け、それら
磁界検出器の検出出力の差を求めるようにしたことを特
徴とする回転電機の磁束検出方法。[Claims] 1 In the stator gap plane of a motor equipped with a rotor with skewed conductors, l = (t_2/2)cotθ t_2 is symmetrical with respect to the center of the core thickness and for a mutual distance l, Magnetic field detectors were installed at two points such that the slot pitch of the rotor projected onto the stator air gap surface, and θ was the skew angle (mechanical angle), and the difference between the detection outputs of these magnetic field detectors was determined. A magnetic flux detection method for a rotating electrical machine, characterized by:
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP53008026A JPS6047829B2 (en) | 1978-01-25 | 1978-01-25 | Magnetic flux detection method for rotating electrical machines |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP53008026A JPS6047829B2 (en) | 1978-01-25 | 1978-01-25 | Magnetic flux detection method for rotating electrical machines |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS54101101A JPS54101101A (en) | 1979-08-09 |
| JPS6047829B2 true JPS6047829B2 (en) | 1985-10-23 |
Family
ID=11681818
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP53008026A Expired JPS6047829B2 (en) | 1978-01-25 | 1978-01-25 | Magnetic flux detection method for rotating electrical machines |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS6047829B2 (en) |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP4899485B2 (en) * | 2006-01-13 | 2012-03-21 | 日産自動車株式会社 | Motor drive control device |
-
1978
- 1978-01-25 JP JP53008026A patent/JPS6047829B2/en not_active Expired
Also Published As
| Publication number | Publication date |
|---|---|
| JPS54101101A (en) | 1979-08-09 |
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