JP2011115008A - Magnetic core with coil, and armature - Google Patents

Magnetic core with coil, and armature Download PDF

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JP2011115008A
JP2011115008A JP2009271565A JP2009271565A JP2011115008A JP 2011115008 A JP2011115008 A JP 2011115008A JP 2009271565 A JP2009271565 A JP 2009271565A JP 2009271565 A JP2009271565 A JP 2009271565A JP 2011115008 A JP2011115008 A JP 2011115008A
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winding
magnetic core
flat surface
substantially flat
layer
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JP5463878B2 (en
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Yoshinari Asano
能成 浅野
Atsushi Kito
敦之 木藤
Shin Nakamasu
伸 中増
Tatsushi Yasumoto
竜志 安本
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Daikin Industries Ltd
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Daikin Industries Ltd
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Abstract

<P>PROBLEM TO BE SOLVED: To provide a magnetic core with coil around which magnetic core the coil is wound so that a cross point is placed on a prescribed side face of the magnetic core, without applying excessive tensile force to the coil. <P>SOLUTION: According to the magnetic core with the coil (12), the coil has a nonperpendicular portion (12h) whose coil direction (P1) is not perpendicular to a pillar axis (P2) direction only on an approximately flat surface (10b). The coil is wound into a coil, in line from one end side (P-) toward the other end side (P+) of the pillar axis (P2) direction of the magnetic core to form one coil layer (12P1). A next coil layer (12P2) is formed on the one coil layer, such that the next coil layer is coiled in line from the other end side (P+) toward the one end side (P-) so that a cross point (K) of the next coil layer, and the one coil layer is placed on the substantially flat surface and at a place other than the approximately flat surface, is located in grooves 12a between the coils of the one coil layer. The width W of the substantially flat surface is set so that the width W satisfies formula 1: W+D≥D/tanθ+(n-1)Dsinθ, and where 0°<θ<90°, with respect to D the diameter of the coil and θ the angle between the coil direction (P1) and a surface perpendicular to the pillar axis (P2). <P>COPYRIGHT: (C)2011,JPO&INPIT

Description

本発明は、アキシャルギャップ型回転電機での使用に適した巻線付き磁芯および電機子に関する。   The present invention relates to a magnetic core with windings and an armature suitable for use in an axial gap type rotating electrical machine.

磁芯に巻線を巻回するとき、占積率を上げるために、俵積み状に(即ち2層目以上の各巻線がその下層の巻線間の溝内に配置する様に)整列巻きする事が望ましい。しかし巻線が下層の巻線と交差する交差点(クロスポイント)では、俵積み状に整列巻きできないので、占積率が悪化する。   When winding the windings around the magnetic core, in order to increase the space factor, the windings are arranged in a stacked manner (ie, each winding in the second layer or more is placed in a groove between the lower windings). It is desirable to do. However, at the intersection where the winding intersects with the lower layer winding (cross point), the winding factor cannot be aligned in a stacked manner, so that the space factor deteriorates.

例えばアキシャルギャップ型回転電機では、この様なクロスポイントが磁芯における周方向側の側面(即ち隣接する磁芯と対向する側面)に存在すると、当該側面で巻線が俵積みされる場合と比較して巻線の巻回数(周回数とも言う)が低減し、回転電機の性能が低下するという問題が生じる。またこの様なクロスポイントが磁芯における外周側(即ち回転電機の中心軸に対する径方向外側)の側面に存在すると、当該側面で巻線が俵積みされる場合と比較して巻回数が低減するか、または磁芯の配置がより一層内周側に配置されて、回転電機の回転出力が低下するという問題が生じる。そのため、クロスポイントは、磁芯における内周側の側面に収まる様に配置される事が望ましい。   For example, in an axial gap type rotating electrical machine, when such a cross point exists on the side surface on the circumferential side of the magnetic core (that is, the side surface facing the adjacent magnetic core), the winding is stacked on the side surface. As a result, the number of winding turns (also referred to as the number of turns) is reduced, resulting in a problem that the performance of the rotating electrical machine is degraded. In addition, when such a cross point is present on the outer peripheral side of the magnetic core (that is, the radially outer side with respect to the central axis of the rotating electrical machine), the number of turns is reduced compared to the case where the windings are stacked on the side. Alternatively, the magnetic core is further arranged on the inner peripheral side, which causes a problem that the rotational output of the rotating electrical machine is reduced. For this reason, it is desirable that the cross points be arranged so as to fit on the inner peripheral side surface of the magnetic core.

しかし、クロスポイントは、巻線の巻き進む方向(巻線方向)と反対側にずれる傾向があるので、1つの側面に納めるのは難しい。特にアキシャルギャップ型回転電機においては巻線の占積率を高めるべく、磁芯が当該回転電機の中心軸方向から見て略台形柱状に形成され、その略台形の短辺に対応する側面が内周側(即ち回転電機の中心軸に対する径方向内側)に向けられる様にして、複数の磁芯が環状に配置される場合が多い。そしてこの場合には、磁芯における内周側の側面は、略台形の短辺に対応する側面となり幅が狭くなるので、尚更、クロスポイントを磁芯における内周側の側面に納めるのは難しい。   However, since the cross point tends to shift to the opposite side to the winding direction (winding direction) of the winding, it is difficult to fit the cross point on one side. In particular, in an axial gap type rotating electrical machine, in order to increase the space factor of the winding, the magnetic core is formed in a substantially trapezoidal column shape when viewed from the central axis direction of the rotating electrical machine, and the side surface corresponding to the short side of the approximately trapezoidal shape is inside. In many cases, a plurality of magnetic cores are arranged in an annular shape so as to be directed to the circumferential side (that is, radially inside with respect to the central axis of the rotating electrical machine). In this case, the inner peripheral side surface of the magnetic core is a side surface corresponding to the substantially trapezoidal short side and the width is narrowed. Therefore, it is more difficult to fit the cross point on the inner peripheral side surface of the magnetic core. .

尚、クロスポイントを内周側の側面に納めることに関する先行技術文献として特許文献1がある。   Note that there is Patent Document 1 as a prior art document relating to storing the cross point on the inner peripheral side surface.

特開2008−312319号公報JP 2008-31319 A

そのため、従来では、巻線に過度の張力(巻線が過度に延びる程の張力)を掛けることで、無理矢理に、クロスポイントが磁芯の内周側の側面に収まる様にしていた。そのため、巻線に過度の負担が掛かり、巻線にダメージを与えたり、断面積が小さくなり巻線抵抗が大きくなるという問題があった。   For this reason, conventionally, by applying excessive tension to the winding (tensile enough to extend the winding), the cross point is forced to fit on the inner peripheral side surface of the magnetic core. For this reason, there is a problem that an excessive load is applied to the winding, and the winding is damaged, or the sectional area is reduced and the winding resistance is increased.

この発明の課題は、上記のような問題点を解決するためになされたものであり、巻線に過度な張力を掛けなくても、磁芯の所定側の側面にクロスポイントが収まる様に巻線が整列巻きにより積層巻きされた巻線付き磁芯および電機子を提供することにある。   An object of the present invention is to solve the above-described problems, and the winding is performed so that the cross point is accommodated on a predetermined side surface of the magnetic core without applying excessive tension to the winding. An object of the present invention is to provide a wound core and an armature in which wires are laminated and wound by aligned winding.

上記課題を解決する為に、本発明の第1の態様は、その外周面(10b)の所定側の側面に略矩形状の略平坦面(10a)を有する柱状の磁芯(10)と、断面が円状であって前記外周面に巻回される巻線(12)と、を備え、前記巻線は、その巻線方向(P1)が前記略平坦面上のみで前記磁芯の柱軸(P2)方向に対して直交しない非直交部分(12h)を有し、且つ前記磁芯における前記柱軸方向の一方端側(P−)から他方端側(P+)に向けて整列巻きされて一の巻線層(12P1)を形成し、前記一の巻線層上に、前記略平坦面に前記一の巻線層の巻線との交差点(K)が収まり且つ前記略平坦面以外では前記一の巻線層の各巻線間の溝12a内に配置される様にして、前記他方端から前記一方端に向けて整列巻きされて次の巻線層(12P2)を形成し、前記一の巻線層の周回数をnとし、前記略平坦面の前記柱軸方向に直交する方向の幅をWとし、前記巻線の直径をDとし、前記柱軸に垂直な面(S1)に対する前記非直交部分の巻線方向の角度をθとし、前記幅Wは、式1を満たす様に設定されるものである。   In order to solve the above problems, a first aspect of the present invention includes a columnar magnetic core (10) having a substantially rectangular substantially flat surface (10a) on a predetermined side surface of the outer peripheral surface (10b); And a winding (12) wound around the outer peripheral surface, the winding having a winding direction (P1) only on the substantially flat surface and the magnetic core column. It has a non-orthogonal portion (12h) that is not orthogonal to the direction of the axis (P2) and is aligned and wound from one end side (P−) to the other end side (P +) in the column axis direction of the magnetic core. One winding layer (12P1) is formed, and the intersection (K) with the winding of the one winding layer is accommodated on the substantially flat surface on the one winding layer, and other than the substantially flat surface. Then, the winding is aligned and wound from the other end to the one end so as to be disposed in the groove 12a between the windings of the one winding layer. Forming a layer (12P2), wherein the number of turns of the one winding layer is n, the width of the substantially flat surface in the direction perpendicular to the column axis direction is W, the diameter of the winding is D, The angle in the winding direction of the non-orthogonal portion with respect to the plane (S1) perpendicular to the column axis is θ, and the width W is set so as to satisfy Equation 1.

本発明の第2の態様は、第1の態様に記載の巻線付き磁芯であって、前記磁芯(10)は、略台形柱状に形成され、前記略平坦面(10a)は、前記略台形柱状の略台形の短辺に対応する側面であるものである。   A second aspect of the present invention is the magnetic core with winding according to the first aspect, wherein the magnetic core (10) is formed in a substantially trapezoidal columnar shape, and the substantially flat surface (10a) It is a side surface corresponding to the short side of the substantially trapezoidal columnar substantially trapezoid.

本発明の第3の態様は、第1または2の態様に記載の巻線付き磁芯であって、前記外周面(10b)において前記略平坦面(10a)とそれに隣接する他の側面(10k1,10k2)との境界である角部(10d)にエッジ緩和構造が施された場合において、前記略平坦面の前記幅(W)は、前記エッジ緩和構造が施されなかった場合の幅であるものである。   A third aspect of the present invention is the core with a winding according to the first or second aspect, wherein the outer peripheral surface (10b) has the substantially flat surface (10a) and another side surface (10k1) adjacent thereto. , 10k2), when the edge relaxation structure is applied to the corner (10d), the width (W) of the substantially flat surface is the width when the edge relaxation structure is not applied. Is.

本発明の第4の態様は、第2の態様に記載の巻線付き磁芯を用いた電機子であって、電機子用ヨーク(20)と、前記電機子用ヨークの片面(20b)に、前記柱軸(P2)方向が前記片面に垂直となり且つ前記略平坦面(10a)が内周側に向けられて、環状に複数配設された前記巻線付き磁芯(1)と、を備えるものである。   According to a fourth aspect of the present invention, there is provided an armature using the magnetic core with winding according to the second aspect, wherein the armature yoke (20) is provided on one side (20b) of the armature yoke. A plurality of annularly arranged magnetic cores (1) in which the column axis (P2) direction is perpendicular to the one surface and the substantially flat surface (10a) is directed to the inner peripheral side. It is to be prepared.

本発明の第1の態様によれば、巻線(12)に過度の張力を掛けなくても、巻線(12)の交差点(K)が所定側の側面である略平坦面(10a)に収まる様にして、巻線(12)を磁芯(10)の外周に整列巻きにより積層巻きできる。   According to the first aspect of the present invention, the intersection (K) of the winding (12) is formed on the substantially flat surface (10a), which is the side surface on the predetermined side, without applying excessive tension to the winding (12). The winding (12) can be laminated and wound on the outer periphery of the magnetic core (10) by aligned winding so as to fit.

本発明の第2の態様によれば、略台形の短辺に対応する側面(10a)に巻線(12)の交差点(K)が収まる様に、巻線(12)を磁芯(10)の外周に整列巻きする事ができる。   According to the second aspect of the present invention, the winding (12) is connected to the magnetic core (10) so that the intersection (K) of the winding (12) is accommodated in the side surface (10a) corresponding to the short side of the substantially trapezoid. Can be aligned and wound around

本発明の第3の態様によれば、磁芯(10)の角部(10d)にエッジ緩和構造が施されている場合でも、略平坦面(10a)の幅(W)を正確に決定できる。   According to the third aspect of the present invention, the width (W) of the substantially flat surface (10a) can be accurately determined even when the corner portion (10d) of the magnetic core (10) is provided with an edge relaxation structure. .

本発明の第4の態様によれば、巻線(12)の交差点(K)が磁芯(10)における内周側の側面(10a)に収まるので、磁芯(10)における外周側の側面(10e)での巻線層全体の厚さを薄くでき、その分、磁芯(10)をより一層外周側に配置できて回転電機の出力を向上できる。また巻線の交差点(K)が磁芯(10)における内周側の側面(10a)に収まるので、磁芯(10)における周方向側の側面(10k)での巻線層全体の厚さを薄くでき、その分、巻線(12)を多く巻回できて回転電機の出力を向上できる。   According to the fourth aspect of the present invention, the intersection (K) of the windings (12) is accommodated in the inner peripheral side surface (10a) of the magnetic core (10), and therefore the outer peripheral side surface of the magnetic core (10). The thickness of the entire winding layer in (10e) can be reduced, and accordingly, the magnetic core (10) can be further arranged on the outer peripheral side, and the output of the rotating electrical machine can be improved. Further, since the winding intersection (K) is accommodated on the inner peripheral side surface (10a) of the magnetic core (10), the thickness of the entire winding layer on the peripheral side surface (10k) of the magnetic core (10). Thus, the winding (12) can be wound many times and the output of the rotating electrical machine can be improved.

第1実施形態に係る巻線付き磁芯1の斜視図である。It is a perspective view of magnetic core 1 with a winding concerning a 1st embodiment. 磁芯本体10Aの柱軸P2に垂直な面での断面図である。It is sectional drawing in a surface perpendicular | vertical to the column axis P2 of 10 A of magnetic core main bodies. 巻線付き磁芯1を略平坦面10a側から見た側面図である。It is the side view which looked at the magnetic core 1 with a coil | winding from the substantially flat surface 10a side. 1層目の1周目の巻線12が磁芯10に巻回された状態を説明する図である。It is a figure explaining the state by which the coil | winding 12 of the 1st round of the 1st layer was wound by the magnetic core 10. FIG. 1層目の2周目の巻線12が磁芯10に巻回された状態を説明する図である。It is a figure explaining the state by which the winding 12 of the 2nd round of the 1st layer was wound around the magnetic core 10. FIG. 第2実施形態に係る電機子30の分解斜視図である。It is a disassembled perspective view of the armature 30 which concerns on 2nd Embodiment. 電機子30を回転軸Qの巻線付き磁芯1側から見た平面図である。4 is a plan view of the armature 30 as viewed from the side of the winding core 1 of the rotation axis Q. FIG.

<第1実施形態>
この実施の形態に係る巻線付き磁芯1は、アキシャルギャップ型回転電機用電機子に使用されるものであり、図1の様に、磁芯10と、磁芯10の外周(即ち磁芯10の後述の柱軸P2周りの外周)に巻回される巻線12とを備えている。
<First Embodiment>
A winding core 1 according to this embodiment is used for an armature for an axial gap type rotating electrical machine. As shown in FIG. 1, the core 10 and the outer periphery of the core 10 (that is, the core). 10 and a winding 12 wound around an outer periphery of a column axis P2 (described later).

磁芯10は、図1の様に、その外周面10bの所定側の側面に略矩形状の略平坦面10aを有する柱状(ここでは略台形柱状)に形成されている。尚、図1中の符号P2は磁芯10の柱軸であり、符号P3は、柱軸P2に直交し且つ略平坦面10aに平行な横軸であり、符号P4は、柱軸P2に直交し且つ略平坦面10aに直交する縦軸である。   As shown in FIG. 1, the magnetic core 10 is formed in a columnar shape (substantially trapezoidal columnar shape here) having a substantially rectangular substantially flat surface 10 a on a predetermined side surface of the outer peripheral surface 10 b. 1 is a column axis of the magnetic core 10, the symbol P3 is a horizontal axis perpendicular to the column axis P2 and parallel to the substantially flat surface 10a, and the symbol P4 is orthogonal to the column axis P2. The vertical axis is orthogonal to the substantially flat surface 10a.

磁芯10は、磁芯本体10Aと、第1の張出部10Bと、第2の張出部10Cとを備えている。   The magnetic core 10 includes a magnetic core body 10A, a first overhang portion 10B, and a second overhang portion 10C.

磁芯本体10Aは、図1の様に、略角柱状(ここでは略台形柱状)に形成されており、その略台形の短辺に対応する側面が略平坦面10aとなっている。磁芯本体10Aの外周面(即ち柱軸P2周りの外周面)10b1の各角部10d,10fは、図2の様に、エッジ緩和構造(例えば面取り)が施されて例えば丸みを有する様に形成されている。   As shown in FIG. 1, the magnetic core body 10A is formed in a substantially prismatic shape (here, a substantially trapezoidal column), and a side surface corresponding to the short side of the substantially trapezoid is a substantially flat surface 10a. As shown in FIG. 2, the corners 10d and 10f of the outer peripheral surface (ie, the outer peripheral surface around the column axis P2) 10b1 of the magnetic core body 10A are provided with an edge relaxation structure (for example, chamfering) and have, for example, roundness. Is formed.

第1の張出部10Bは、図1の様に、磁芯本体10Aにおける柱軸P2方向の一方側P+に設けられており、磁芯本体10Aの外周側(即ち柱軸P2周りの外周側)に張り出す様に形成されている。より詳細には、第1の張出部10Bは、例えば略台形状の板状に形成され、その短辺側が磁芯本体10Aの略台形の短辺側と同じ側に向けられ、その長辺側が磁芯本体10Aの略台形の長辺側と同じ側に向けられて設けられている。そして第1の張出部10Bは、例えば、その縦軸P4方向の幅(即ちその短辺と長辺との間の幅)が磁芯本体10Aの縦軸P4方向の幅と同じ大きさに形成され、その横軸P3方向の両側の縁部10gが磁芯本体10Aから張り出す様に形成されている。   As shown in FIG. 1, the first overhanging portion 10B is provided on one side P + of the magnetic core body 10A in the direction of the column axis P2, and the outer peripheral side of the magnetic core body 10A (that is, the outer peripheral side around the column axis P2). ). More specifically, the first overhanging portion 10B is formed, for example, in a substantially trapezoidal plate shape, and its short side is directed to the same side as the short side of the substantially trapezoidal shape of the magnetic core body 10A. The side is provided so as to face the same side as the substantially trapezoidal long side of the magnetic core body 10A. The first projecting portion 10B has, for example, a width in the direction of the vertical axis P4 (that is, a width between the short side and the long side) of the same length as the width of the magnetic core body 10A in the direction of the vertical axis P4. The edge portions 10g on both sides in the direction of the horizontal axis P3 are formed so as to protrude from the magnetic core body 10A.

第2の張出部10Cは、磁芯本体10Aにおける柱軸P2方向の他方側P−に設けられており、磁芯本体10Aの外周側に張り出す様に形成されている。より詳細には、第2の張出部10Cは、例えば略矩形状の板状に形成され、その略矩形における縦軸P4方向に平行な一対の辺の長さ(即ち縦軸P4方向の長さ)は磁芯本体10Aの縦軸P4方向の長さと略同じ長さに形成され、その略矩形における横軸P3方向に平行な一対の辺の長さ(即ち横軸P3方向の長さ)は磁芯本体10Aの略台形の長辺の長さと略同じ長さに形成されている。   The second projecting portion 10C is provided on the other side P- of the magnetic core body 10A in the direction of the column axis P2, and is formed so as to project to the outer peripheral side of the magnetic core body 10A. More specifically, the second overhanging portion 10C is formed in, for example, a substantially rectangular plate shape, and the length of a pair of sides parallel to the vertical axis P4 direction in the substantially rectangular shape (that is, the length in the vertical axis P4 direction). Is a length substantially equal to the length of the magnetic core body 10A in the direction of the vertical axis P4, and the length of a pair of sides parallel to the direction of the horizontal axis P3 in the substantially rectangular shape (that is, the length in the direction of the horizontal axis P3). Is formed to have substantially the same length as the length of the substantially trapezoidal long side of the magnetic core body 10A.

尚ここでは、第2の張出部10Cにおける柱軸P2方向の他方側P−の面(即ち磁芯本体10A側と反対側の面)10jには、凸状部10iが設けられている。凸状部10iは、直方体状に形成されており、面10jにおける横軸P3方向の中央において、その長手方向が縦軸P4方向に沿う様に設けられている。凸状部10iは、その横軸P3方向の長さW2が第2の張出部10Cの横軸P3方向の長さW1よりも短く、その縦軸P4方向の長さが第2の張出部10Cの横軸P3方向の長さと略同じ長さの直方体状に形成されている。   Here, a convex portion 10i is provided on the surface 10j on the other side P− of the second overhanging portion 10C in the column axis P2 direction (that is, the surface opposite to the magnetic core body 10A side) 10j. The convex portion 10i is formed in a rectangular parallelepiped shape, and is provided in the center of the surface 10j in the direction of the horizontal axis P3 so that the longitudinal direction thereof is along the direction of the vertical axis P4. The convex portion 10i has a length W2 in the horizontal axis P3 direction shorter than a length W1 in the horizontal axis P3 direction of the second overhang portion 10C, and a length in the vertical axis P4 direction of the second overhang portion. The portion 10C is formed in a rectangular parallelepiped shape having substantially the same length as the length in the horizontal axis P3 direction.

尚、磁芯10は略台形柱状に形成されている。この点に関し、磁芯10は、略台形柱状の磁芯本体10Aを有し、その筒軸P2方向の両側P+,P−において磁芯本体10Aの外周側に張り出した第1および第2の張出部10B,10Cを有しているが、ここでは、主要部で大部分を占める磁芯本体10Aが略台形柱状なので、第1および第2の張出部10B,10Cを含めた全体も略台形柱状とみなしている。   The magnetic core 10 is formed in a substantially trapezoidal column shape. In this regard, the magnetic core 10 has a substantially trapezoidal columnar magnetic core body 10A, and first and second tensions projecting to the outer peripheral side of the magnetic core body 10A on both sides P + and P− in the direction of the cylinder axis P2. Although the protruding portions 10B and 10C are provided, here, the magnetic core body 10A occupying most of the main portion is substantially trapezoidal columnar, so the whole including the first and second protruding portions 10B and 10C is also substantially omitted. Considered trapezoidal columnar.

尚、磁芯10は、磁性体により形成されている。ここでは磁芯10は、図1の様に、複数の磁性体板10rが縦軸P4方向に積層されて形成されている。したがって、磁芯10の柱軸P2に直交する面での断面形状は、外側が、磁性体板の板厚毎の階段状になっている。   The magnetic core 10 is made of a magnetic material. Here, the magnetic core 10 is formed by laminating a plurality of magnetic plates 10r in the direction of the vertical axis P4 as shown in FIG. Accordingly, the cross-sectional shape of the surface of the magnetic core 10 perpendicular to the column axis P2 is stepped for each plate thickness of the magnetic plate.

巻線12は、例えば断面が円形の丸線である。尚、巻線12は、自己融着線である事が望ましいが、必須ではない。巻線12は、過度の張力(即ち巻線12が過度に引き延ばされる程の張力)が掛からない様にして、図3の様に、磁芯本体10Aの外周面10b1において、絶縁層を介して整列巻きされ(即ち互いに平行に隙間無く配置されて巻回され)、且つクロスポイント(即ち2層目以降の巻線12がその下層(磁芯本体10A側)の巻線12と交差する交差点)Kが略平坦面10a側に収まる様に積層巻きされる。尚、図3では、1層目の各巻線12は実線で図示され、2層目の巻線12は点線で図示され、3層目以降の巻線12は図示省略されている。   The winding 12 is, for example, a round wire having a circular cross section. The winding 12 is preferably a self-bonding wire, but is not essential. As shown in FIG. 3, the winding 12 is not provided with an insulating layer on the outer peripheral surface 10 b 1 of the magnetic core body 10 </ b> A so as not to apply excessive tension (that is, tension enough to cause the winding 12 to be excessively stretched). Are wound in an aligned manner (that is, wound in a parallel arrangement with no gaps), and cross points (that is, intersections where the second and subsequent windings 12 intersect with the lower layer (magnetic core body 10A side) windings 12). ) Stacked and wound so that K is within the substantially flat surface 10a side. In FIG. 3, each winding 12 in the first layer is illustrated by a solid line, the second winding 12 is illustrated by a dotted line, and the third and subsequent windings 12 are not illustrated.

尚ここでは、図2を参照して、巻線12は、外周面10b1の側面10k1における柱筒軸P2方向の他方側P−の辺の略平坦面10a側の端部付近の位置10tから、側面10k1→側面10k3→側面10k2→略平坦面10aの順で(即ち図2上で時計回りに)巻回され、筒軸P2方向の一方側P+に向かって(紙面手前に向かって)1層目が整列巻きされる。   Here, referring to FIG. 2, the winding 12 has a position 10t near the end on the substantially flat surface 10a side of the side P-side in the column cylinder axis P2 direction on the side surface 10k1 of the outer peripheral surface 10b1. One layer is wound in the order of the side surface 10k1, the side surface 10k3, the side surface 10k2, and the substantially flat surface 10a (ie, clockwise in FIG. 2) toward one side P + in the direction of the cylinder axis P2 (toward the front of the page). The eyes are aligned and wound.

より詳細には、図3の様に、1層目では、巻線12は、略平坦面10a以外の側面10k1〜10k3(図2参照)上では、その巻線方向P1が筒軸P2方向に直交し、略平坦面10a上では、次の周回へとずれるために筒軸P2方向に直交しない非直交部分12hを有する様に、磁芯本体10Aの外周面10b1において筒軸P2方向の他方側P−から一方側P+まで整列巻きされて、1層目の巻線層12P1を形成している。尚、1層目の巻線層12P1の周回数はnに設定されており、磁芯本体10Aの外周面10b1の筒軸P2方向の長さはnDに設定されている。   More specifically, as shown in FIG. 3, in the first layer, the winding 12 has a winding direction P1 in the direction of the cylinder axis P2 on the side surfaces 10k1 to 10k3 (see FIG. 2) other than the substantially flat surface 10a. The other side in the cylinder axis P2 direction on the outer peripheral surface 10b1 of the magnetic core body 10A so as to have a non-orthogonal portion 12h not orthogonal to the cylinder axis P2 direction on the substantially flat surface 10a so as to shift to the next round. The winding is aligned from P− to one side P + to form a first winding layer 12P1. The number of turns of the first winding layer 12P1 is set to n, and the length of the outer peripheral surface 10b1 of the magnetic core body 10A in the direction of the cylinder axis P2 is set to nD.

尚、巻線層12P1の1周目の巻線12(以降、k周目の巻線12を巻線12−kと呼ぶ)が巻回されると、図4の様に、巻線12−1における略平坦面10a上の全ての部分が非直交部分12hとなる。更に2周目の巻線12−2が整列巻きにより巻回されると、2周目の巻線12−2は1周目の巻線12−1と密着する様に1周目の巻線12−1側に押し付け気味に巻回されるので、図5の様に、1周目の巻線12−1は、2周目の巻線12−2からの圧力Fにより筒軸P2方向の他方側P−に押される。そのため、巻線12−1における略平坦面10a上の巻線方向P1の上流側の部分12iは、筒軸P2に対して直交する。一般に、k+1周目の巻線12−(k+1)はk周目の巻線12−kと密着する様にk周目の巻線12−k側に押し付け気味に巻回される。そのためk周目の巻線12−kは、k+1周目の巻線12−(k+1)からの圧力Fにより筒軸P2方向の他方側P−に押されるので、巻線12−kの部分12iは、筒軸P2に対して直交する。   When the first winding 12 of the winding layer 12P1 (hereinafter, the kth winding 12 is referred to as a winding 12-k) is wound, as shown in FIG. 1 are all non-orthogonal portions 12h on the substantially flat surface 10a. Further, when the winding 12-2 of the second turn is wound by the aligned winding, the winding 12-2 of the second turn is wound in the first turn so as to be in close contact with the winding 12-1 of the first turn. Since the coil 12-1 is pressed toward the 12-1 side, the winding 12-1 in the first turn is moved in the direction of the cylinder axis P2 by the pressure F from the winding 12-2 in the second turn as shown in FIG. It is pushed to the other side P-. Therefore, the upstream portion 12i in the winding direction P1 on the substantially flat surface 10a of the winding 12-1 is orthogonal to the cylinder axis P2. In general, the winding 12- (k + 1) of the (k + 1) th turn is pressed and wound to the winding 12-k side of the kth turn so as to be in close contact with the winding 12-k of the kth turn. Therefore, the winding 12-k of the k-th turn is pushed to the other side P- in the direction of the cylinder axis P2 by the pressure F from the winding 12- (k + 1) of the (k + 1) -th turn, so that the portion 12i of the winding 12-k Is orthogonal to the cylinder axis P2.

そして巻線層12P1が形成された状態では、巻線層12P1のk周目の巻線12−kは、k+1周目以降の各周回の巻線12からの圧力の合力Fをk+1周目の巻線12−(k+1)から受ける。そのため巻線12−kは、1周目側に在るほど巻線12−(k+1)から大きな圧力Fを受ける。そして巻線12−kが巻線12−(k+1)から受ける圧力Fが大きいほど、巻線12−kの部分12iは長くなる。従って、1周目側の周回の巻線12ほどその部分12iは長くなり、最終周目(n周目)側の周回の巻線12ほどその部分12iは短くなり、(n−1)周目の巻線12−(n−1)では、その部分12iは無くなる。   In the state where the winding layer 12P1 is formed, the winding 12-k in the k-th turn of the winding layer 12P1 uses the resultant force F of the pressure from the winding 12 in each turn after the k + 1-th turn as the k + 1-th turn. Received from winding 12- (k + 1). Therefore, the winding 12-k receives a larger pressure F from the winding 12- (k + 1) as it is closer to the first turn. As the pressure F received by the winding 12-k from the winding 12- (k + 1) increases, the portion 12i of the winding 12-k becomes longer. Accordingly, the portion 12i becomes longer as the winding 12 on the first turn side becomes longer, and the portion 12i becomes shorter as the turn 12 on the last turn (nth turn) side, and the (n-1) th turn. In the winding 12- (n-1), the portion 12i is eliminated.

尚、1層目の巻線層12P1の最終周目の巻線12−nの非直交部分12hは、その巻線方向P1が2層目の巻線層12P2の1周目の巻線12−1の巻き始め位置方向にずれるので、1層目の巻線層12P1の他の巻線12−1,…,12−(n−2)の非直交部分12hに対して整列巻されない。同様に2層目以降の各巻線層12P2,…の最終周目の巻線12の非直交部分12hも、それと同じ巻線層の他の巻線12の非直交部分12hに対して整列巻されない。   The non-orthogonal portion 12h of the winding 12-n on the final circumference of the first winding layer 12P1 has a winding direction P1 of the first winding 12- of the winding layer 12P2 on the second layer. 1 is not aligned and wound around the non-orthogonal portion 12h of the other windings 12-1,..., 12- (n-2) of the first winding layer 12P1. Similarly, the non-orthogonal portion 12h of the winding 12 on the final circumference of the second and subsequent winding layers 12P2,... Is not aligned with the non-orthogonal portion 12h of the other winding 12 of the same winding layer. .

また図5の様に、巻線層12P1のk周目の巻線12−kは、k−1周目の巻線12−(k−1)側に押し付けられるのでその反作用によりk−1周目の巻線12−(k−1)からの圧力Faを受け、その圧力Faにより筒軸P2方向の一方側P+に押される。そのため巻線12−kにおける略平坦面10a上の下流側の部分12j(図3参照)は、筒軸P2に対して直交する。そのため、上述と同様に、巻線層12P1が形成された状態では、1周目側の周回の巻線12ほどその部分12jは短くなり、1周目の巻線12ではその部分12jは無くなり、最終周目側の周回の巻線12ほどその部分12iは長くなる。尚、(n−1)周目の巻線12−(n−1)がn−2周目の巻線12−(n−2)から受ける圧力Faは、筒軸P2方向の対称性を考慮すると、1周目の巻線12−1が2周目の巻線12−2から受ける圧力Fと同じになるので、(n−1)周目の巻線12−(n−1)の部分12jは、1周目の巻線12−1の部分12iの長さと同じ長さになる。   Further, as shown in FIG. 5, the winding 12-k of the kth turn of the winding layer 12P1 is pressed against the winding 12- (k-1) side of the k-1th turn. The pressure Fa from the winding 12- (k-1) of the eye is received, and the pressure Fa is pushed to one side P + in the direction of the cylinder axis P2. Therefore, the downstream portion 12j (see FIG. 3) on the substantially flat surface 10a in the winding 12-k is orthogonal to the cylinder axis P2. Therefore, similarly to the above, in the state where the winding layer 12P1 is formed, the portion 12j becomes shorter in the winding 12 on the first turn side, and the portion 12j disappears in the winding 12 in the first turn. The portion 12i becomes longer as the winding 12 around the final circumference. Note that the pressure Fa received by the winding 12- (n-1) in the (n-1) th turn from the winding 12- (n-2) in the n-2th turn considers the symmetry in the direction of the cylinder axis P2. Then, since the first winding 12-1 has the same pressure F received from the second winding 12-2, the (n-1) th winding 12- (n-1) portion 12j has the same length as the length of the portion 12i of the winding 12-1 in the first turn.

そしてこの様に巻線層12P1が形成された状態では、巻線層12P1における最終周目以外の各巻線12の非直交部分12hを合わせた部分H1は、筒軸P2方向に直交する面(例えば第2の張出部10Cの筒軸P2方向の一方側P+の面)S1に対して所定角θだけ傾斜した略矩形を形成する。尚、所定角θは、巻線層12P1の各巻線12の非直交部分12hの巻線方向P1と面S1との成す角度であり、0°<θ<90°の範囲の角度である。   In the state in which the winding layer 12P1 is formed in this way, a portion H1 including the non-orthogonal portions 12h of the windings 12 other than the final circumference in the winding layer 12P1 is a plane orthogonal to the direction of the cylinder axis P2 (for example, A substantially rectangular shape that is inclined by a predetermined angle θ with respect to the surface S1 of the second projecting portion 10C on the one side P + in the cylinder axis P2 direction is formed. The predetermined angle θ is an angle formed by the winding direction P1 of the non-orthogonal portion 12h of each winding 12 of the winding layer 12P1 and the surface S1, and is an angle in a range of 0 ° <θ <90 °.

そしてこの実施形態では、略矩形H1の面S1への射影成分H1a(=D/tanθ°+(n−1)Dsinθ)が略平坦面10aの筒軸P2方向に直交する方向の幅Wと巻線12の半径D/2の2倍との和(W+D)以下になる様に(即ち式1の関係が成立する様に)設定されている(この関係を第1の関係と呼ぶ)。   In this embodiment, the projection component H1a (= D / tan θ ° + (n−1) Dsinθ) onto the surface S1 of the substantially rectangular H1 has a width W and a winding in a direction perpendicular to the direction of the cylinder axis P2 of the substantially flat surface 10a. It is set to be equal to or less than the sum (W + D) of twice the radius D / 2 of the line 12 (that is, the relationship of Formula 1 is established) (this relationship is called the first relationship).

Figure 2011115008
Figure 2011115008

即ちこの実施形態では、過度の張力が掛からない様に1層目の巻線層12P1が形成されたときに、式1の関係が成立する様に、略平坦面10aの幅Wおよび巻線12の直径Dが設定されている。式1の関係が成立する状態では、巻線12に過度の張力が掛からないで1層目の巻線層12P1の各巻線12の非直交部分12hが略平坦面10aに収まる。   That is, in this embodiment, when the first winding layer 12P1 is formed so that excessive tension is not applied, the width W of the substantially flat surface 10a and the winding 12 are set so that the relationship of Formula 1 is satisfied. The diameter D is set. In a state where the relationship of Expression 1 is satisfied, the winding 12 is not excessively tensioned, and the non-orthogonal portion 12h of each winding 12 of the first winding layer 12P1 fits on the substantially flat surface 10a.

尚ここでは、図2の様に、磁芯本体10Aの外周面10b1において略平坦面10aとそれに隣接する他の側面10k1,10k2との境界である角部10dにエッジ緩和構造が施されている場合は、略平坦面10aの幅Wは、エッジ緩和構造が施されなかった場合の略平坦面10aの幅が採用される。   Here, as shown in FIG. 2, the edge relaxation structure is applied to the corner 10d which is the boundary between the substantially flat surface 10a and the other side surfaces 10k1 and 10k2 adjacent to the outer peripheral surface 10b1 of the magnetic core body 10A. In this case, the width W of the substantially flat surface 10a is the width of the substantially flat surface 10a when the edge relaxation structure is not applied.

そして2層目では、巻線12は、略平坦面10a以外の側面10k1〜10k3上では、1層目の各巻線12間の窪みにより形成された溝12a内に配置されることで、1層目の場合と同様に、その巻線方向P1が筒軸P2方向に対して直交し、且つ略平坦面10a上では、その巻線方向P1が次の周回へとずれるために筒軸P2方向に直交しない非直交部分12hを有する様に、磁芯本体10Aの外周面10b1における筒軸P2方向の一方側P+から他方側P−まで整列巻きされて、2層目の巻線層12P2を形成している。   In the second layer, the winding 12 is arranged in the groove 12a formed by the depression between the windings 12 in the first layer on the side surfaces 10k1 to 10k3 other than the substantially flat surface 10a. As in the case of the eye, the winding direction P1 is orthogonal to the direction of the cylinder axis P2, and on the substantially flat surface 10a, the winding direction P1 shifts to the next round, so A second winding layer 12P2 is formed by aligning winding from one side P + to the other side P− in the cylinder axis P2 direction on the outer peripheral surface 10b1 of the magnetic core body 10A so as to have a non-orthogonal portion 12h that is not orthogonal. ing.

この状態では、2層目の巻線層12P2における最終周目以外の各巻線12の非直交部分12hを合わせた部分は、1層目の略矩形H1と同様に、筒軸P2に対して所定角度(2層目の巻線層12P2における最終周目以外の各巻線12の非直交部分12hと面S1との間の角度)だけ傾斜した略矩形(不図示)となる。そしてその略矩形の面S1への射影成分H2aは、図3の様に、和(W+D+2d1)内に収まる様に制限される(これを第2の関係と呼ぶ)。尚、図3中の符号d1は、各側面10k1,10k3上での各巻線層12P1,12P2間の間隔である。   In this state, the portion including the non-orthogonal portion 12h of each winding 12 other than the final circumference in the second winding layer 12P2 is predetermined with respect to the cylinder axis P2 in the same manner as the first rectangle H1. It becomes a substantially rectangular shape (not shown) inclined by an angle (angle between the non-orthogonal portion 12h of each winding 12 other than the last circumference in the second winding layer 12P2 and the surface S1). Then, the projection component H2a onto the substantially rectangular surface S1 is limited so as to be within the sum (W + D + 2d1) as shown in FIG. 3 (this is referred to as a second relationship). In addition, the code | symbol d1 in FIG. 3 is the space | interval between each winding layer 12P1, 12P2 on each side surface 10k1, 10k3.

尚、第2の関係では、射影成分H2aが第1の関係の場合の和(W+D)よりも広い和(W+D+2d1)内に制限されるので、第2の関係は、第1の関係が成立する下では自動的に満たされる。尚、d1は√3・D/2である。   In the second relationship, since the projection component H2a is limited to a sum (W + D + 2d1) wider than the sum (W + D) in the first relationship, the second relationship is the first relationship. Below will be charged automatically. Note that d1 is √3 · D / 2.

そして略平坦面10a以外の側面10k1〜10k3では、各巻線層12P1,12P2の巻線12は互いに平行になり互いに交差しないので、第1および第2の関係が成立することで、1層目の各巻線12と2層目の各巻線12との各交差点Kは、略平坦面10aに収まる。即ち当該交差点Kは、略平坦面10a以外の側面10k1〜10k3上にはみ出さない様に制限される。   On the side surfaces 10k1 to 10k3 other than the substantially flat surface 10a, the windings 12 of the winding layers 12P1 and 12P2 are parallel to each other and do not intersect with each other. Each intersection point K between each winding 12 and each winding 12 in the second layer falls within the substantially flat surface 10a. That is, the intersection K is limited so as not to protrude on the side surfaces 10k1 to 10k3 other than the substantially flat surface 10a.

同様に、3層目以降の奇数層は、1層目の場合と同様に、且つその下層の巻線12間の溝12a内、およびその下層の両端の巻線12と第1および第2の張出部10B,10Cとの間の溝12b,12c内に配置される様に整列巻きされ、4層目以降の偶数層は、2層目の場合と同様にその下層の巻線12間の溝12a内に配置する様に整列巻きされて、所定の積層数だけ積層巻きされる。この様に、第1の関係(即ち式1)が成立すると、巻線12に過度の張力が掛からず、各側面10k1〜10k3では、各巻線層12P1,12P2,…の巻線12は互いに平行になり、略平坦面10aには、各巻線層12P1,12P2,…の巻線12の非直交部分12hが収まるので、巻線12に過度の張力が掛からずに各巻線層12P1,12P2,…間の全ての交差点Kが略平坦面10aに収まる。   Similarly, the odd-numbered layers after the third layer are the same as in the first layer and in the groove 12a between the lower-layer windings 12 and the first and second windings 12 at both ends of the lower layer. The windings are aligned so as to be arranged in the grooves 12b and 12c between the overhanging portions 10B and 10C, and the even layers after the fourth layer are between the lower windings 12 as in the case of the second layer. The coils are aligned and wound so as to be disposed in the groove 12a, and are wound in a predetermined number of layers. In this way, when the first relationship (ie, Expression 1) is established, excessive tension is not applied to the winding 12, and the windings 12 of the winding layers 12P1, 12P2,... Are parallel to each other on the side surfaces 10k1 to 10k3. Since the non-orthogonal portion 12h of the winding 12 of each winding layer 12P1, 12P2,... Is accommodated on the substantially flat surface 10a, each winding layer 12P1, 12P2,. All the intersections K in between fit within the substantially flat surface 10a.

尚ここでは、磁芯本体10Aの柱軸P2方向の長さが巻線12の直径Dのn倍(即ちnD)となる場合で説明した。この場合は、1層目,2層目,3層目,…の各巻線層12P1,12P2,12P3,…の周回数はそれぞれn,n−1,n,…の様になり、2層目以降の各巻線層の周回数は1層目の巻線層の周回数以下になるので、1層目の巻線層が式1の関係を満たせば、即ち1層目の巻線層の各周回の巻線12の非直交部分12hが略平坦面10aに収まれば、2層目以降の各巻線層の各周回の巻線12の非直交部分12hも略平坦面10aに収まる。従って各巻線層間における巻線12の交差点Kは略平坦面10aに収まる。磁芯本体10Aの柱軸P2方向の長さが巻線12の直径Dの(n−1/2)倍(即ち(n+1/2)D)となる場合は、1層目,2層目,3層目,…の各巻線層12P1,12P2,12P3,…の周回数はそれぞれn,n,n,…の様に同じとなるが、この場合も、上記のnD倍の場合と同様に、2層目以降の各巻線層の周回数は1層目の巻線層の周回数以下になるので、1層目の巻線層が式1の関係を満たせば、2層目以降の各巻線層の各周回の巻線12の非直交部分12hも略平坦面10aに収まり、従って各巻線層間における巻線12の交差点Kは略平坦面10aに収まる。   Here, the case where the length of the magnetic core body 10A in the direction of the column axis P2 is n times the diameter D of the winding 12 (that is, nD) has been described. In this case, the number of turns of the first, second, third,... Winding layers 12P1, 12P2, 12P3,... Becomes n, n-1, n,. Since the number of turns of the subsequent winding layers is equal to or less than the number of turns of the first winding layer, if the first winding layer satisfies the relationship of Equation 1, each of the first winding layers If the non-orthogonal portion 12h of the winding 12 is fitted on the substantially flat surface 10a, the non-orthogonal portion 12h of each winding 12 of each winding layer after the second layer is also fitted on the substantially flat surface 10a. Therefore, the crossing point K of the winding 12 between the winding layers falls within the substantially flat surface 10a. When the length of the magnetic core body 10A in the direction of the column axis P2 is (n−½) times the diameter D of the winding 12 (that is, (n + ½) D), the first layer, the second layer, The number of turns of each of the winding layers 12P1, 12P2, 12P3,... Of the third layer,... Is the same as n, n, n,. Since the number of turns of each winding layer after the second layer is equal to or less than the number of turns of the first winding layer, if the first winding layer satisfies the relationship of Equation 1, each winding after the second layer The non-orthogonal portion 12h of each winding 12 of the layer also fits on the substantially flat surface 10a. Therefore, the intersection K of the winding 12 between the winding layers fits on the substantially flat surface 10a.

以上の様に構成された巻線付き磁芯1によれば、略平坦面10aの幅Wが式1を満たす様に設定されるので、巻線12に過度の張力を掛けなくても、各巻線層12P1,12P2,…間における巻線12の交差点Kが略平坦面10aに収まる様にして、巻線12を磁芯10の外周面10bに整列巻きにより積層巻きできる。   According to the magnetic core 1 with the winding configured as described above, the width W of the substantially flat surface 10a is set so as to satisfy the expression 1, so that each winding can be performed without applying excessive tension to the winding 12. The winding 12 can be laminated and wound on the outer peripheral surface 10b of the magnetic core 10 by aligned winding so that the intersection K of the winding 12 between the wire layers 12P1, 12P2,.

また磁芯10が略台形柱状に形成される場合において、磁芯10におけるその略台形の短辺に対応する側面10aに各巻線層間における巻線12の交差点Kが収まる様に、巻線12を磁芯10の外周面10bに整列巻きにより積層巻きできる。   When the magnetic core 10 is formed in a substantially trapezoidal columnar shape, the winding 12 is arranged so that the intersection K of the winding 12 between the winding layers is accommodated on the side surface 10a corresponding to the short side of the substantially trapezoid in the magnetic core 10. The outer peripheral surface 10b of the magnetic core 10 can be laminated and wound by aligned winding.

また磁芯10の角部10dにエッジ緩和構造が施されている場合の略平坦面10aの幅Wは、エッジ緩和構造が施されていない場合の略平坦面の幅が採用されるので、磁芯10の角部10dにエッジ緩和構造が施されている場合でも、略平坦面10aの幅Wを正確に決定できる。   Further, since the width W of the substantially flat surface 10a when the edge relaxation structure is applied to the corner portion 10d of the magnetic core 10, the width of the substantially flat surface when the edge relaxation structure is not applied is adopted. Even when the corner 10d of the core 10 is provided with an edge relaxation structure, the width W of the substantially flat surface 10a can be accurately determined.

<第2実施形態>
この実施形態に係る電機子30は、第1実施形態の巻線付き磁芯1を用いたアキシャルギャップ型回転電機用電機子である。この電機子30は、図6および図7の様に、巻線付き磁芯1と、ヨーク20とを備えている。尚、図6中の符号Qは、電機子30の回転軸であり、符号Qrは、回転軸Qに対する径方向であり、符号Qφは、回転軸Qに対する周方向である。
Second Embodiment
The armature 30 according to this embodiment is an armature for an axial gap type rotating electrical machine using the winding core 1 according to the first embodiment. As shown in FIGS. 6 and 7, the armature 30 includes a magnetic core 1 with a winding and a yoke 20. 6 is the rotation axis of the armature 30, Qr is the radial direction with respect to the rotation axis Q, and Qφ is the circumferential direction with respect to the rotation axis Q.

巻線付き磁芯1は、第1実施形態の巻線付き磁芯1と同様に構成されている。即ち巻線付き磁芯1は、各巻線層間における巻線12の交差点Kが磁芯10の略矩形面(即ち略台形の短辺に対応する側面)10aに収まる様に、磁芯10の外周面に巻線12が整列巻きにより積層巻きされて構成されている。   The wound core 1 is configured in the same manner as the wound core 1 of the first embodiment. That is, in the magnetic core 1 with windings, the outer periphery of the magnetic core 10 is arranged such that the intersection K of the windings 12 between the winding layers falls within the substantially rectangular surface 10a of the magnetic core 10 (that is, the side surface corresponding to the short side of the substantially trapezoid). A winding 12 is laminated and wound on the surface by aligned winding.

ヨーク20は、ヨーク本体20hと、ヨーク本体20hの下面に配設される磁芯固定板20gとを備えている。   The yoke 20 includes a yoke body 20h and a magnetic core fixing plate 20g disposed on the lower surface of the yoke body 20h.

ヨーク本体20hは、磁性体により円環板状に形成されている。ここではヨーク本体20hは、例えば、複数の磁性体板24を回転軸Q方向に積層して円環板状に形成されている。ヨーク本体20hには、磁芯10の第2の張出部10Cが嵌合する嵌合部22dが複数形成されている。各嵌合部22dは、ヨーク本体20hの上下面を貫通すると共にヨーク本体20hの内周側面で開放口22cを有する様にして、径方向Qrに沿って放射状に形成されている。   The yoke body 20h is formed in an annular plate shape from a magnetic material. Here, the yoke body 20h is formed in an annular plate shape, for example, by laminating a plurality of magnetic plates 24 in the direction of the rotation axis Q. A plurality of fitting portions 22d into which the second overhanging portion 10C of the magnetic core 10 is fitted are formed in the yoke body 20h. Each fitting portion 22d is formed radially along the radial direction Qr so as to penetrate the upper and lower surfaces of the yoke body 20h and to have an opening 22c on the inner peripheral side surface of the yoke body 20h.

磁芯固定板20gは、例えばステンレス等の非磁性金属によりヨーク本体20hと略同じ直径の円環板状に形成されている。磁芯固定板20gには、その上下面を貫通する様に、巻線付き磁芯1の凸状部17が嵌合する嵌合孔20mが形成されている。   The magnetic core fixing plate 20g is formed in an annular plate shape having a diameter substantially the same as that of the yoke body 20h, for example, by a nonmagnetic metal such as stainless steel. The magnetic core fixing plate 20g is formed with a fitting hole 20m into which the convex portion 17 of the magnetic core 1 with winding is fitted so as to penetrate the upper and lower surfaces thereof.

この電機子30では、以下の様にして、ヨーク20に磁芯10が配設される。即ち、ヨーク20の各嵌合部22dに、その上方側から、各磁芯10の柱軸P2方向がヨーク20の片面20bに垂直となり、且つ各磁芯10の略平坦面10aが径方向Qrの内側に向けられ、且つ第2の張出部10Cの径方向Qrの外側の外側面10C1が嵌合部22dの径方向Qrの外側の内側面22daに当接する様にして、磁芯10の第2の張出部10Cが嵌合部22dに嵌合される。この嵌合状態では、磁芯10の凸状部10iは、ヨーク20の嵌合孔20mに嵌合している。そして磁芯固定板20gの下面側から、凸状部10iと嵌合孔20mとの接触箇所を溶接により互いに固定する。この様にして、図7の様に、ヨーク20の主面20bに複数の磁芯10が環状に配設される。なお、ヨーク本体20hは、嵌合部22dの径方向内側が開口することにより、磁芯10を通る磁束の変化により磁芯10のまわりに発生する渦電流の経路を遮断するとともに、巻線12の巻き始めを磁芯10まわりに導くための空間となっている。   In this armature 30, the magnetic core 10 is disposed on the yoke 20 as follows. That is, the column axis P2 direction of each magnetic core 10 is perpendicular to the one surface 20b of the yoke 20 from the upper side to each fitting portion 22d of the yoke 20, and the substantially flat surface 10a of each magnetic core 10 is in the radial direction Qr. Of the magnetic core 10 so that the outer surface 10C1 on the outer side in the radial direction Qr of the second overhanging portion 10C contacts the inner side surface 22da on the outer side in the radial direction Qr of the fitting portion 22d. 10C of 2nd overhang | projection parts are fitted by the fitting part 22d. In this fitted state, the convex portion 10 i of the magnetic core 10 is fitted in the fitting hole 20 m of the yoke 20. And the contact location of the convex part 10i and the fitting hole 20m is mutually fixed by welding from the lower surface side of the magnetic core fixing plate 20g. In this way, as shown in FIG. 7, the plurality of magnetic cores 10 are annularly arranged on the main surface 20 b of the yoke 20. The yoke body 20h opens the radial inner side of the fitting portion 22d, thereby interrupting the path of eddy current generated around the magnetic core 10 due to the change of the magnetic flux passing through the magnetic core 10, and the winding 12 Is a space for guiding the start of winding around the magnetic core 10.

以上の様に構成された電機子30によれば、各巻線付き磁芯1の各巻線層間における巻線12の交差点Kは磁芯10の内周側の側面10aに収まるので、磁芯10の外周側の側面10k3での巻線層全体の厚さを薄くでき、その分、磁芯10をより一層外周側に配置できて、この電機子30を用いた回転電機の出力を向上できる。   According to the armature 30 configured as described above, the intersection point K of the winding 12 between the winding layers of the core 1 with each winding is within the side surface 10a on the inner peripheral side of the magnetic core 10, so The thickness of the entire winding layer on the outer peripheral side surface 10k3 can be reduced, and the magnetic core 10 can be further arranged on the outer peripheral side, and the output of the rotating electric machine using this armature 30 can be improved.

また巻線12の交差点Kが磁芯10の内周側の側面10aに収まるので、磁芯10の周方向Qφ側の側面10k1,10k2での巻線層全体の厚さを薄くでき、その分、巻線12を多く巻回できて、この電機子30を用いた回転電機の出力を向上できる。   Further, since the intersection point K of the windings 12 is accommodated on the side surface 10a on the inner peripheral side of the magnetic core 10, the thickness of the entire winding layer on the side surfaces 10k1 and 10k2 on the circumferential direction Qφ side of the magnetic core 10 can be reduced. Since many windings 12 can be wound, the output of the rotating electrical machine using this armature 30 can be improved.

なお、本実施形態では、第1の張出部10Bをロータに対向させ、第2の張出部10Cをヨーク20に嵌合させているが、両側ともロータに対向させてもよい。また、第1及び第2の張出部10B,10C、及び、凸状部10iも任意である。張出部がない場合は、絶縁体で張出部を形成しても良い。   In the present embodiment, the first overhanging portion 10B is opposed to the rotor and the second overhanging portion 10C is fitted to the yoke 20, but both sides may be opposed to the rotor. Moreover, the 1st and 2nd overhang | projection parts 10B and 10C and the convex-shaped part 10i are also arbitrary. When there is no overhanging portion, the overhanging portion may be formed of an insulator.

1 巻線付き磁芯
10 磁芯
10a 略平坦面
10b 巻線の外周面
10b1 巻線本体の外周面
10d 角部
12 巻線
12a 溝
12P1,12P2 巻線層
20 ヨーク
W 略平坦面の幅
θ 巻線方向と筒軸に直交する面との間の角度
D 巻線の直径
P1 巻線方向
P2 磁芯の筒軸
K 交差点(クロスポイント)
DESCRIPTION OF SYMBOLS 1 Magnetic core with winding 10 Magnetic core 10a Almost flat surface 10b Outer peripheral surface of winding 10b1 Outer peripheral surface of winding main body 10d Corner 12 Winding 12a Groove 12P1, 12P2 Winding layer 20 Yoke W Width of substantially flat surface θ winding Angle between line direction and plane perpendicular to cylinder axis D Winding diameter P1 Winding direction P2 Core axis of magnetic core K Crossing point

Claims (4)

その外周面(10b)の所定側の側面に略矩形状の略平坦面(10a)を有する柱状の磁芯(10)と、
断面が円状であって前記外周面に巻回される巻線(12)と、
を備え、
前記巻線は、その巻線方向(P1)が前記略平坦面上のみで前記磁芯の柱軸(P2)方向に対して直交しない非直交部分(12h)を有し、且つ前記磁芯における前記柱軸方向の一方端側(P−)から他方端側(P+)に向けて整列巻きされて一の巻線層(12P1)を形成し、前記一の巻線層上に、前記略平坦面に前記一の巻線層の巻線との交差点(K)が収まり且つ前記略平坦面以外では前記一の巻線層の各巻線間の溝12a内に配置される様にして、前記他方端から前記一方端に向けて整列巻きされて次の巻線層(12P2)を形成し、
前記一の巻線層の周回数をnとし、前記略平坦面の前記柱軸方向に直交する方向の幅をWとし、前記巻線の直径をDとし、前記柱軸に垂直な面(S1)に対する前記一の巻線層における最終周目以外の前記各巻線の前記非直交部分の巻線方向の角度をθとし、
前記幅Wは、式1を満たす様に設定されることを特徴とする巻線付き磁芯。
Figure 2011115008
A columnar magnetic core (10) having a substantially rectangular substantially flat surface (10a) on a predetermined side surface of the outer peripheral surface (10b);
A winding (12) having a circular cross section and wound around the outer peripheral surface;
With
The winding has a non-orthogonal portion (12h) whose winding direction (P1) is only on the substantially flat surface and is not orthogonal to the column axis (P2) direction of the magnetic core, and in the magnetic core One winding layer (12P1) is formed by being aligned and wound from one end side (P−) to the other end side (P +) in the column axis direction, and the substantially flat surface is formed on the one winding layer. The crossing point (K) with the winding of the one winding layer is accommodated on the surface, and the other side is disposed in the groove 12a between the windings of the one winding layer except for the substantially flat surface. The next winding layer (12P2) is formed by aligning winding from one end toward the one end,
The number of turns of the one winding layer is n, the width of the substantially flat surface in the direction orthogonal to the column axis direction is W, the diameter of the winding is D, and the surface perpendicular to the column axis (S1 The angle of the winding direction of the non-orthogonal portion of each winding other than the last circumference in the one winding layer with respect to
The width W is set so as to satisfy Formula 1;
Figure 2011115008
請求項1に記載の巻線付き磁芯であって、
前記磁芯(10)は、略台形柱状に形成され、
前記略平坦面(10a)は、前記略台形柱状の略台形の短辺に対応する側面であることを特徴とする巻線付き磁芯。
The magnetic core with winding according to claim 1,
The magnetic core (10) is formed in a substantially trapezoidal columnar shape,
The said substantially flat surface (10a) is a side surface corresponding to the short side of the said substantially trapezoid pillar-shaped substantially trapezoid, The magnetic core with a coil | winding characterized by the above-mentioned.
請求項1または2に記載の巻線付き磁芯であって、
前記外周面(10b)において前記略平坦面(10a)とそれに隣接する他の側面(10k1,10k2)との境界である角部(10d)にエッジ緩和構造が施された場合において、
前記略平坦面の前記幅(W)は、前記エッジ緩和構造が施されなかった場合の幅であることを特徴とする巻線付き磁芯。
The magnetic core with winding according to claim 1 or 2,
In the case where the edge relaxation structure is applied to the corner (10d) which is the boundary between the substantially flat surface (10a) and the other side surface (10k1, 10k2) adjacent thereto on the outer peripheral surface (10b),
The magnetic core with windings, wherein the width (W) of the substantially flat surface is a width when the edge relaxation structure is not applied.
請求項2に記載の巻線付き磁芯を用いた電機子であって、
電機子用ヨーク(20)と、
前記電機子用ヨークの片面(20b)に、前記柱軸(P2)方向が前記片面に垂直となり且つ前記略平坦面(10a)が内周側に向けられて、環状に複数配設された前記巻線付き磁芯(1)と、
を備えることを特徴とする電機子。
An armature using the magnetic core with winding according to claim 2,
An armature yoke (20);
The armature yoke is provided with a plurality of annular surfaces on one side (20b) of which the column axis (P2) direction is perpendicular to the one side and the substantially flat surface (10a) is directed to the inner peripheral side. A wound core (1),
An armature comprising:
JP2009271565A 2009-11-30 2009-11-30 Winding core and armature Expired - Fee Related JP5463878B2 (en)

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Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPWO2015159329A1 (en) * 2014-04-14 2017-04-13 株式会社日立産機システム Axial air gap type rotating electrical machine
EP3136564B1 (en) * 2014-04-23 2020-05-27 Hitachi Industrial Equipment Systems Co., Ltd. Axial air-gap rotary electric machine
KR20210004717A (en) * 2019-07-05 2021-01-13 엘지전자 주식회사 Stator

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JP2000245092A (en) * 1998-12-24 2000-09-08 Toyota Motor Corp Concentrated wound coil and winding apparatus
JP2008199791A (en) * 2007-02-13 2008-08-28 Daikin Ind Ltd Armature, rotary electric machine, compressor, blower, and air conditioner

Patent Citations (2)

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Publication number Priority date Publication date Assignee Title
JP2000245092A (en) * 1998-12-24 2000-09-08 Toyota Motor Corp Concentrated wound coil and winding apparatus
JP2008199791A (en) * 2007-02-13 2008-08-28 Daikin Ind Ltd Armature, rotary electric machine, compressor, blower, and air conditioner

Cited By (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPWO2015159329A1 (en) * 2014-04-14 2017-04-13 株式会社日立産機システム Axial air gap type rotating electrical machine
US10763716B2 (en) 2014-04-14 2020-09-01 Hitachi Industrial Equipment Systems Co., Ltd. Axial-air-gap dynamo-electric machine with a tubular-shaped stator bobbin
EP3136564B1 (en) * 2014-04-23 2020-05-27 Hitachi Industrial Equipment Systems Co., Ltd. Axial air-gap rotary electric machine
US11251670B2 (en) 2014-04-23 2022-02-15 Hitachi Industrial Equipment Systems Co., Ltd. Axial air-gap rotary electric machine having a different number of internal side layers and external side layers
KR20210004717A (en) * 2019-07-05 2021-01-13 엘지전자 주식회사 Stator
KR102214080B1 (en) * 2019-07-05 2021-02-09 엘지전자 주식회사 Stator

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