JPS5931293B2 - Manufacturing method of cylindrical element wire for electric motor - Google Patents
Manufacturing method of cylindrical element wire for electric motorInfo
- Publication number
- JPS5931293B2 JPS5931293B2 JP12564379A JP12564379A JPS5931293B2 JP S5931293 B2 JPS5931293 B2 JP S5931293B2 JP 12564379 A JP12564379 A JP 12564379A JP 12564379 A JP12564379 A JP 12564379A JP S5931293 B2 JPS5931293 B2 JP S5931293B2
- Authority
- JP
- Japan
- Prior art keywords
- wire
- ring
- hollow truncated
- truncated cone
- electric motor
- 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
Classifications
-
- H—ELECTRICITY
- H02—GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
- H02K—DYNAMO-ELECTRIC MACHINES
- H02K3/00—Details of windings
- H02K3/04—Windings characterised by the conductor shape, form or construction, e.g. with bar conductors
Landscapes
- Engineering & Computer Science (AREA)
- Power Engineering (AREA)
- Windings For Motors And Generators (AREA)
- Manufacture Of Motors, Generators (AREA)
Description
【発明の詳細な説明】
この発明は、電動機用線輪の製造方法に係り、特に中空
円錐台形状の線輪から円筒形の要素線輪を形成する方法
に関する。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a method of manufacturing a wire for an electric motor, and more particularly to a method of forming a cylindrical element wire from a hollow truncated cone-shaped wire.
一般に、コアレスモーフの回転子、スロットルモータの
回転子及びブラシレスモーフ例えば、ホールモータの回
転磁界を生じさせる固定子として円筒形状の波巻線輪体
が用いれている。Generally, a cylindrical wave-wound ring body is used as a rotor of a coreless morph, a rotor of a throttle motor, and a stator for generating a rotating magnetic field of a brushless morph, such as a Hall motor.
従来、このような波巻線輪体を製造する方法とし、ハネ
カム力式と称せられる方法が知られている。Conventionally, a method called a honeycomb force method is known as a method for manufacturing such a wave-wound ring body.
このハネカム力式にあっては、端面における折返しにお
いて、張力による導線のすべりをおさえながら巻くので
高速の機械巻が困難であり、特に、軸方向に長く、小径
の波巻線輪体を形成する際には、導線のすべりを防止の
ため、ひっかけピンを挿入して行なうため非能率的であ
る問題がある。In this honeycomb force type, high-speed mechanical winding is difficult because the winding is done while suppressing the slippage of the conductor due to tension when folding at the end face.In particular, it is difficult to wind the wire at high speed mechanically, and it is especially difficult to form a wave winding wheel that is long in the axial direction and has a small diameter. In some cases, a hook pin is inserted to prevent the conductor from slipping, which is inefficient.
このハネカム力式以外に非金属のボビンに斜めに機械巻
する方法もあるが、整列巻が困難であり、ボビンが導線
の張力に耐えるために厚手のものとなり、ギャップが増
したり、ボビンの両端部に不作用部が累積したりする欠
点がある。In addition to this honeycomb force method, there is also a method of mechanical winding diagonally on a non-metallic bobbin, but it is difficult to wind in an aligned manner, and the bobbin has to be thick to withstand the tension of the conductor, resulting in an increased gap or There is a drawback that inactive parts accumulate in some parts.
従来、固定子及び回転子間のエアーギャップを小さくす
ることができる電機子として特開昭52−20208号
公報に開示されるようなプリントコイルが知られている
が、このプリントコイルは、偏平状の電機子に適用する
場合に限られ円筒状の電機子には、適用することは困難
であるとされ、円筒状の電機子を製造する場合には、依
然導線を機械巻きする方法が採用されている。Conventionally, a printed coil as disclosed in Japanese Patent Application Laid-Open No. 52-20208 has been known as an armature that can reduce the air gap between the stator and rotor. It is said that it is difficult to apply to cylindrical armatures, and when manufacturing cylindrical armatures, the method of mechanically winding the conductor wire is still used. ing.
本発明は、上記のような事情に鑑みなされたものであっ
て、電流密度を大きくすることができ、しかもエアーギ
ャップを小さくすることができる電動機用円筒形要素線
輪の製造方法を提供するにある。The present invention has been made in view of the above-mentioned circumstances, and an object of the present invention is to provide a method for manufacturing a cylindrical element wire for an electric motor, which can increase the current density and reduce the air gap. be.
以下、この発明の一実施例を図面を参照しながら説明す
る。An embodiment of the present invention will be described below with reference to the drawings.
第1図に外径gl、内径g2.導体幅Bの円環状線輪、
そして第2図には太径dl。Figure 1 shows outer diameter gl, inner diameter g2. An annular wire ring with a conductor width B,
Figure 2 shows the large diameter dl.
小径d2.頂角δ、導体幅B、頂点から大径におろした
母線の長さがRの中空円錐台状線輪が示されている。Small diameter d2. A hollow truncated conical wire ring having an apex angle δ, a conductor width B, and a length R of a generatrix extending from the apex to a large diameter is shown.
上記円環状線輪あるいは中空円錐台状線輪をその円周に
そって偶数等分2n(n=1゜2.3.・・・)し、そ
の等分点において、円環状線輪の場合は半径に対しであ
る特定の角度φで、また中空円錐台状線輪の場合は母線
に対してφの角度で表面に折曲げて外表面を互いに略密
着し、次に隣接する等分点において裏側へ折曲げて内表
面を互いに略密着することを繰返すと、第3図に示され
たような直径り、高さLの仮想円筒に嵌る形状の線輪が
形成される。Divide the above circular ring or hollow truncated conical ring into an even number of equal parts 2n (n=1゜2.3...) along its circumference, and at the equally divided points, in the case of a circular ring is bent on the surface at a certain angle φ with respect to the radius, or in the case of a hollow truncated conical wire ring at an angle φ with respect to the generatrix, so that the outer surfaces are almost in close contact with each other, and then the adjacent equally divided points By repeatedly bending the wires to the back side and bringing the inner surfaces into substantially close contact with each other, a wire ring having a shape that fits into an imaginary cylinder having a diameter and a height L as shown in FIG. 3 is formed.
この第3図の線−輪を平面上に展開したものが第4図で
ある。FIG. 4 shows the lines and rings in FIG. 3 developed on a plane.
第4図において、lは2B等分された円環状線輪あるい
は中空πD
円錐台状線輪の弦の長さである。In FIG. 4, l is the length of the chord of a circular ring or a hollow πD truncated conical ring divided into 2B equal parts.
またーは、弦n lの線輪が仮想円筒πDに占める長さである。Also, the string n This is the length that the wire ring of l occupies in the virtual cylinder πD.
上述したように、円環状線輪の場合は半径に対して、中
空円錐台状線輪の場合は母線に対して、ある特定の角度
φで表側あるいは裏側へ折曲げて第3図のような形状の
線輪を形成したのであるが、第4図のlと、このlが仮
想円筒の円周と接する点における垂線とのなす角を調べ
てみると、図に示されているようにやはりφの角度を持
つことが分かる。As mentioned above, in the case of a circular ring, it is bent to the front side or back side at a certain angle φ with respect to the radius, and in the case of a hollow truncated conical ring, with respect to the generatrix, as shown in Figure 3. When we examine the angle between l in Figure 4 and the perpendicular at the point where l touches the circumference of the virtual cylinder, we find that it is as shown in the figure. It can be seen that it has an angle of φ.
そこで第4図より、という関係式が導かれしたがって
となり、折曲げ角φは仮想円筒の直径りと、高さLと、
等分数2nから求められる。Therefore, from Fig. 4, the following relational expression is derived, and the bending angle φ is the diameter of the virtual cylinder, the height L,
It is found from the equal fraction 2n.
次に、第1図において20等分された線輪の弦の長さl
は、
である。Next, in Figure 1, the length l of the chord of the wire wheel divided into 20 equal parts is
is .
また、第4図から分かるように
L : 1cosφ (2)
であるから、これを上式に代入すると
が得られ、これが円環状線輪の外径g1を求める式であ
る。Also, as can be seen from Figure 4, L: 1cosφ (2)
Therefore, by substituting this into the above equation, we obtain the following, which is the equation for determining the outer diameter g1 of the annular wire ring.
内径g2は、glとg2の間に
g2二gl−2B (4)という関
係があるので、導体幅Bを決めてやることにより内径g
2も求まる。Since there is a relationship between gl and g2 as g22gl-2B (4), the inner diameter g2 can be determined by determining the conductor width B.
2 can also be found.
次に、第2図の中空円錐状線輪において、その太径d、
1は、
である。Next, in the hollow conical wire ring in FIG. 2, its large diameter d,
1 is.
また、この第2図の中空円錐台状線輪を平面上に展開し
た5図において、2B等分された線輪の弦の長さlは、
である。In addition, in FIG. 5, which shows the hollow truncated conical wire wheel in FIG. 2 developed on a plane, the chord length l of the wire wheel divided into 2B equal parts is as follows.
ただしTは上記中空円錐台状線輪を平面上に展開したと
きの中心角。However, T is the central angle when the above-mentioned hollow truncated circular ring is developed on a plane.
この式と(2)と(5)式より、 が得られる。From this equation and equations (2) and (5), is obtained.
ところで第2図の頂角δと第5図の中心角Tの間には、 という関 係があるのでこれを上式に代入すると、 が得られる。By the way, between the apex angle δ in Fig. 2 and the central angle T in Fig. 5, Seki called Since there is a relation, substituting this into the above formula, we get is obtained.
これが、中空円錐状線輪の太径dlを求める式である。This is the formula for determining the diameter dl of the hollow conical wire ring.
この式のLの代わりにDを用いると、第4図より、 であるから、 この式と(5)式と(6)式から− が得られる。If D is used instead of L in this equation, from Figure 4, Because it is, From this equation, equation (5), and equation (6), − is obtained.
中空円錐状線輪の太径diと小径d2の間には、その導
体幅がBの場合、第2図から明らかなように
という関係がある。As is clear from FIG. 2, there is a relationship between the large diameter di and the small diameter d2 of the hollow conical wire when the conductor width is B.
したがって小径d2は導体幅Bが決定されると求まる。Therefore, the small diameter d2 is determined when the conductor width B is determined.
ところで、中空円錐状線輪の太径dlを求める式(7)
でδ=180・の場合を考えると、dlはとなり、これ
は円
環状線輪の外径g1を求める式(3)と一致する。By the way, the formula (7) for determining the diameter dl of the hollow conical wire ring is
Considering the case where δ=180·, dl becomes, which agrees with equation (3) for determining the outer diameter g1 of the circular ring.
また中空円錐状線輪の小径d2を求める式(8)におい
て、やはりδ=180°の場合を考えるとd2=dl−
2Bとなり、これも円環状線輪の内径に2を求める式と
一致する。Also, in equation (8) for determining the small diameter d2 of the hollow conical wire ring, if we also consider the case of δ = 180°, then d2 = dl-
2B, which also agrees with the formula for calculating the inner diameter of the circular ring.
このように、中空円錐台状線輪の太径dl、小径d2を
求める式において、δ=180’の場合は円環状線輪の
外径gl、内径g2を求める式と等しくなるので、中空
円錐台状線輪の式(7)あるいは(7)オよび(8)は
その特殊な場合として円環状線輪の式(3)と(4)を
含んでいる。In this way, in the formula for determining the large diameter dl and small diameter d2 of the hollow truncated conical wire, if δ = 180', it is equal to the formula for determining the outer diameter gl and inner diameter g2 of the circular truncated wire. Equations (7) or (7) o and (8) for the trapezoidal wire include equations (3) and (4) for the toroidal wire as special cases.
従って、この明細書及び特許請求の範囲においては、円
環状線輪は、中空円錐台状線輪の一例であるので単に中
空円錐台状線輪と記載した場合には、円環状線輪を含む
ものとする。Therefore, in this specification and claims, the toroidal wire is an example of a hollow truncated conical wire, so when it is simply described as a hollow truncated conical wire, it includes the toroidal wire. shall be held.
以上のようにこの発明においては、円筒状の要素線輪は
導線が整列巻回されている中空円錐台形線輪を単に折り
曲げだけで形成されることから、これに組合わせた電機
子には、空間的な無駄が生ぜず、電流密度を大きくする
ことができる。As described above, in this invention, the cylindrical element wire ring is formed by simply bending the hollow truncated conical wire ring around which the conducting wires are wound in an aligned manner. There is no spatial waste, and the current density can be increased.
また、本発明の円筒形状の要素線輪は、十分に薄く形成
でき、これを組合わせた電機子もまた薄くすることがで
きる。Further, the cylindrical element wire of the present invention can be formed sufficiently thin, and the armature in which it is combined can also be made thin.
したがって、電動機の回転子及び固定子間のエアーギャ
ップをできる限り小さくすることができ、結果として大
きなトルクを得ることができる。Therefore, the air gap between the rotor and stator of the electric motor can be made as small as possible, and as a result, a large torque can be obtained.
第1図は円環状線輪、第2図は中空円錐状線輪、第3図
は円環状線輪あるいは中空円錐状線輪から形成された円
筒形要素線輪、第4図は第3図の展開図、第5図は第2
図の展開図である。
gl・・・・・・外径、g2・・・・・・内径、l・・
・・・・弦の長さ。
dl・・・・・・大径、d2・・・・・・小径、δ・・
・・・・頂角、B・・・・・・導体幅、φ・・・・・・
折曲げ角、D・・・・・・仮想円筒の直径、L・・・・
・・仮想円筒の高さ、T・・・・・・展開された中空円
錐状線輪の中心角。Figure 1 shows an annular wire ring, Figure 2 shows a hollow conical wire ring, Figure 3 shows a cylindrical element wire formed from a circular ring or a hollow conical wire ring, and Figure 4 shows a 3rd figure. Developed diagram of , Figure 5 is the second
FIG. gl...outer diameter, g2...inner diameter, l...
・・・The length of the string. dl...Large diameter, d2...Small diameter, δ...
...Apex angle, B...Conductor width, φ...
Bending angle, D...Diameter of virtual cylinder, L...
...Height of the virtual cylinder, T... Central angle of the expanded hollow conical ring.
Claims (1)
を形成し、この中空円錐台形状線輪を折曲げ線に沿って
折曲げて電動機用円筒形要素線輪を形成する方法におい
て、鞘己折曲げ線は、中空円錐台形状の線輪の頂点とこ
の線輪体の円周に沿って定められた等分点とを結ぶ母線
に対してその円周方向に等しい角度を成し、中空円錐台
形状の線輪の面に対して異なる方向に中空円錐台形状の
線輪を折曲げ線に沿って折曲げることによって折曲げ線
で区分された中空円錐台形状の線輪部分の外表面は、互
いに略密着され、中空円錐台形状の線輪部分の内表面は
、互いに略密着さね、この中空円錐台形状の線輪が仮想
円筒面に沿って波形状に展開されることを特徴とする電
動機用円筒形要素線輪を形成する方法。 2 形成されるべき円筒形要素線輪の直径がD、その円
筒部の長さがL、等分点が2n、中空円錐台形状の線輪
の幅及び頂角が夫々B及びδであるとき、折曲げ角は、
下記φで定まり、また中空円錐台形状の線輪の大径部の
直径が下記dl及び小径部の直径が下記d2で定められ
ることを特徴とする特許請求の範囲第1項記載の電動機
用円筒形線輪を形成する方法。[Scope of Claims] 1 A substantially hollow truncated cone-shaped wire ring is formed in which conductive wires are closely wound, and this hollow truncated cone-shaped wire ring is bent along a bending line to form a cylindrical element wire for an electric motor. In the method of forming a ring, the sheath bending line is the circumference of the hollow truncated cone with respect to the generating line connecting the apex of the ring and the equally dividing points defined along the circumference of the ring. A hollow cone that is divided by a bending line by bending a hollow truncated cone-shaped wire in different directions with respect to the plane of the hollow truncated-cone-shaped wire, making equal angles to the direction and along the bending line. The outer surfaces of the trapezoidal wire ring portions are in close contact with each other, and the inner surfaces of the hollow truncated cone wire portions are in approximate contact with each other. A method for forming a cylindrical element wire for an electric motor, characterized in that it is developed into a wave shape. 2 When the diameter of the cylindrical element wire to be formed is D, the length of the cylindrical part is L, the equal dividing point is 2n, and the width and apex angle of the hollow truncated cone-shaped wire are B and δ, respectively. , the bending angle is
A cylinder for an electric motor according to claim 1, characterized in that the diameter of the large diameter portion of the hollow truncated conical wire ring is determined by the following dl, and the diameter of the small diameter portion is determined by the following d2. How to form a shape ring.
Priority Applications (6)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP12564379A JPS5931293B2 (en) | 1979-09-29 | 1979-09-29 | Manufacturing method of cylindrical element wire for electric motor |
US06/139,725 US4401907A (en) | 1979-04-21 | 1980-04-14 | Electric motor coil element and method of manufacturing the same |
GB8012493A GB2059300B (en) | 1979-04-21 | 1980-04-16 | Electric motor coil element and method of manufacturing the same |
DE3014943A DE3014943C2 (en) | 1979-04-21 | 1980-04-18 | Cantilever winding for an electric motor |
SG340/84A SG34084G (en) | 1979-04-21 | 1984-05-03 | Electric motor coil element and method of manufacturing the same |
HK624/84A HK62484A (en) | 1979-04-21 | 1984-08-09 | Electric motor coil element and method of manufacturing the same |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP12564379A JPS5931293B2 (en) | 1979-09-29 | 1979-09-29 | Manufacturing method of cylindrical element wire for electric motor |
Publications (2)
Publication Number | Publication Date |
---|---|
JPS5649656A JPS5649656A (en) | 1981-05-06 |
JPS5931293B2 true JPS5931293B2 (en) | 1984-08-01 |
Family
ID=14915092
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP12564379A Expired JPS5931293B2 (en) | 1979-04-21 | 1979-09-29 | Manufacturing method of cylindrical element wire for electric motor |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS5931293B2 (en) |
-
1979
- 1979-09-29 JP JP12564379A patent/JPS5931293B2/en not_active Expired
Also Published As
Publication number | Publication date |
---|---|
JPS5649656A (en) | 1981-05-06 |
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