JP3536375B2 - Sheet coil type resolver - Google Patents
Sheet coil type resolverInfo
- Publication number
- JP3536375B2 JP3536375B2 JP24200794A JP24200794A JP3536375B2 JP 3536375 B2 JP3536375 B2 JP 3536375B2 JP 24200794 A JP24200794 A JP 24200794A JP 24200794 A JP24200794 A JP 24200794A JP 3536375 B2 JP3536375 B2 JP 3536375B2
- Authority
- JP
- Japan
- Prior art keywords
- phase
- spiral
- coil
- phase coil
- hole
- 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 - Lifetime
Links
Landscapes
- Measurement Of Length, Angles, Or The Like Using Electric Or Magnetic Means (AREA)
- Transmission And Conversion Of Sensor Element Output (AREA)
- Windings For Motors And Generators (AREA)
Description
【発明の詳細な説明】
【0001】
【産業上の利用分野】本発明は、導体をシートコイルに
よって構成したレゾルバに関する。
【0002】
【従来の技術】従来、モータなどに用いられるシートコ
イルとして、薄膜絶縁シート層を挟んで、その両側に金
属からなる平面渦巻き状の導体を対向させ、それらの内
側どうしをスルーホールを通じて電気的に接続したもの
が開示されている(例えば、特公昭61−56700
号)。このシートコイルを、例えば、図3に示したよう
に、回転子に設けた1相の励磁相コイルに励磁電圧Eθ
を印加して、固定子に設けた2相の検出相コイルα、β
に検出電圧Eα,Eβを出力する。6極の1相励磁2相
検出形のレゾルバに適用する場合、励磁相コイルを図5
に、検出コイルを図4に示すように構成することは考え
られる。図5において、1は励磁相コイルで、6極の渦
巻き中心部から渦巻状に巻いて広がるそれぞれ6個の渦
巻導体11a,11bを備えたコイルパターン1a、1
bからなり、コイルパターン1a、1bはポリイミドシ
ートなどからなる円板状の絶縁シート2を挟んで表裏に
対向させて貼り付けてある。実線で示すコイルパターン
1aと点線で示すコイルパターン1bを同一方向から見
ると、逆方向に巻いた形になっている。それぞれ極の渦
巻き中心部にはスルーホール12を設け、渦巻導体11
aと11bの内側端を接続し、渦巻導体11a,11b
の外側端はそれぞれ隣接する渦巻導体11a,11bの
外側端と接続するようにしてあり、隣接する2か所の渦
巻導体11bの外側端+θ、−θは励磁電源に接続して
ある。6極のレゾルバでは、極ピッチは機械角が60度
であり、励磁相コイル1の1個の渦巻導体が占める角度
は機械角60度となっている。したがって、表裏あわせ
て、6×2=12個の渦巻導体を配置したことになる。
図4において、3は検出相コイルで、2相の検出相コイ
ルを形成するために、1極についてそれぞれ2個の渦巻
導体31a,31bを備えたコイルパターン31と,渦
巻導体32a,32bを備えたコイルパターン32が、
円板状の絶縁シート4を挟んで表裏に対向するように貼
り付けてある。すなわち、図4に示す+α端子に接続さ
れた1個の渦巻導体31aは絶縁シート4の表側に設け
られ、渦巻導体31aの外側端から巻かれた導体の内側
端が渦巻の中心でスルーホール33aを介して裏側の渦
巻導体32aの内側端に接続され、渦巻導体32aの外
側端は隣接する極の渦巻導体32aの外側端に接続さ
れ、その裏側の渦巻導体32aの渦巻き中心部のスルー
ホール33aから表側の渦巻導体31aに接続され、順
次6極にわたって接続されて、最後の渦巻導体31aの
外側端は−α端子に接続されて検出相コイル3αを完成
する。+β端子に接続された検出相コイル3βの1個の
渦巻導体31bは、検出相コイル3αに対して電気角で
90度の位相差を持つため、機械角で30度の位相差を
持つように検出相コイル3αの渦巻導体31aに隣接し
て絶縁シート4の表側に設けられる。渦巻導体31bの
外側端から巻かれた導体は、内側端が渦巻の渦巻き中心
部でスルーホール33bを介して裏側の渦巻導体32b
の内側端に接続され、渦巻導体32bの外側端は隣接す
る極の渦巻導体32bの外側端に接続され、その裏側の
渦巻導体32bの渦巻き中心部のスルーホール33bか
ら表側の渦巻導体31bに接続され、順次6極にわたっ
て接続されて、最後の渦巻導体31bの外側端は−β端
子に接続されて検出相コイル3βを完成する。絶縁シー
ト4の表側に設けられた渦巻導体31a,31bおよび
絶縁シート4の裏側に設けられた渦巻導体32a,32
bは、それぞれ1極について2個備えているので、6極
では12個となり、1個の渦巻導体の占める角度は機械
角で30度となる。
【0003】
【発明が解決しようとする課題】ところが、従来技術で
は、励磁相コイルの1個の渦巻導体が占める角度は機械
角で60度であるのに対し、検出相コイルの1個の渦巻
導体が占める角度は機械角で30度となる。1極の中に
入る検出相コイルのα相、β相のそれぞれの巻数を合わ
せた巻数は、1極の中に入る励磁相コイルの巻数とほぼ
同じであるが、α相、β相のそれぞれの相の占める1極
あたりの面積は励磁相コイルのほぼ半分である。ところ
で、一般に、検出相コイルの鎖交磁束Φは、次の(1)
式で表される。
Φ=n・HI ・μ0 ・(S/g) …(1)
ここで、nは検出相コイルの巻数、HI は励磁相コイル
によって発生する起磁力、μ0 は透磁率、Sは励磁相コ
イルの磁束が検出相コイルに鎖交する面積、gはギャッ
プ値である。したがって、検出相コイルのα相、β相の
それぞれの相の占める1極あたりの面積は励磁相コイル
のほぼ半分であるから、検出相コイルが励磁相コイルが
発生する磁束を十分に鎖交磁束として利用していないこ
とになり、検出相コイルの誘起電圧は十分に大きくする
ことができず、消費電力の増加につながるという欠点が
あった。本発明は、検出相コイルの鎖交磁束面積を大き
くすることにより、誘起電圧を大きくし、消費電力を低
減できるレゾルバを提供することを目的とするものであ
る。
【0004】
【課題を解決するための手段】上記問題を解決するため
に、本発明は、極対数Xの各1極分の角度が電気角で1
80°となるように平面状シートコイルによって形成し
た1相から構成されると共に、絶縁シートの両方の面に
設け、一方の面のコイルパターンに設けた渦巻き中心部
のスルーホールと他方の面のコイルパターンに設けた渦
巻き中心部のスルーホールとを接続して1回路を形成
し,その1回路の一部を開放してその両端を励磁電源端
子に接続した励磁相コイルと、前記励磁相コイルに空隙
を介して対向する平面状シートコイルによって形成した
互いに電気角で90°の位相差を持つα相コイルおよび
β相コイルの2相から構成されると共に、絶縁シートの
一方の面に設け、隣り合う1対の渦巻き導体どうしを直
列に接続したX対の渦巻導体からなるα相コイルパター
ンと、前記絶縁シートの他方の面に設け、隣り合う1対
の渦巻き導体どうしを直列に接続したX対の渦巻導体か
らなるβ相コイルパターンと、前記渦巻導体の渦巻き中
心部に設けた第1のスルーホールを有してなる検出相コ
イルとを備えたシートコイル形レゾルバにおいて、前記
検出相コイルは、前記渦巻き中心部と同径の位置で前記
渦巻導体どうしの間に設けた第2のスルーホールと、前
記渦巻導体どうしの間に設けた二つの第1のスルーホー
ルにそれぞれ接続する2本のα相口出線と、前記α相口
出線に接続する第1のスルーホールを除く前記渦巻導体
どうしの間に設けた第1のスルーホールに接続して前記
隣接する1対のα相コイルを接続するα相渡線と、前記
渦巻導体どうしの間に設けた二つの第2のスルーホール
にそれぞれ接続する2本のβ相口出線と、前記β相口出
線に接続する第2のスルーホールを除く前記渦巻導体ど
うしの間に設けた第2のスルーホールに接続して前記隣
接する1対のβ相コイルを接続するβ相渡線とを備えた
ものである。
【0005】
【作用】上記手段により、検出相コイルは、絶縁シート
の一方の面にα相コイルのみを形成するX対の渦巻導体
からなるコイルパターンを、他方の面にはβ相コイルの
みを形成するX対の渦巻導体からなるコイルパターンを
設けてあるので、検出相コイルの1個の渦巻導体の占め
る面積は、励磁相コイルの1個の渦巻導体の占める面積
とほぼ同じとなり、従来に比べて鎖交磁束は大幅に増え
る。その結果、検出相コイルの誘起電圧は増大し、消費
電力は低減する。また、検出相コイルと同一のコイルパ
ターンを絶縁シートの両面に貼り付けて励磁相コイルを
形成しているので、検出コイルと励磁コイルのコイルパ
ターンを共用できるので、コイルパターンの製作工数を
大幅に低減できる。
【0006】
【実施例】以下、本発明を図に示す実施例について説明
する。図1は本発明の第1の実施例の検出相コイルを示
す平面図である。なお、励磁相コイル1は、図5により
従来例で説明した構成と同じものである。図において、
5は検出相コイルで、円板状の絶縁シート6の一方の面
(表面)にα相コイル5Aを形成し、他方の面(裏面)
にβ相コイル5Bを形成している。α相コイル5Aのコ
イルパターン5aは、図1の実線で示すように、6極の
渦巻き中心部から渦巻状に巻いて広がるそれぞれ6個
(3対)の渦巻導体51aからなり、それぞれ1極分の
占める角度が電気角でほぼ180°になるように絶縁シ
ート6の表面に配置してある。また、隣接する2個(1
対)の渦巻導体51aの外側導体を接続してあり、各渦
巻導体51aの渦巻き中心部にスルーホール53Aaを
設けてある。互いに接続されてそれぞれ1対をなす渦巻
導体51aどうしの間には、渦巻き中心部のスルーホー
ル53Aaと同径の位置にスルーホール53Abを設け
てある。3対のうちの1対の渦巻導体51aどうしの間
には外周方向に向かって伸びるβ相口出線52aを設け
てスルーホール53Abに接続し、その他の対の渦巻導
体51aどうしの間には、裏面に設けたβ相コイル5B
の隣接する1対の渦巻導体51bどうしの渦巻き中心部
を接続するβ相渡線54aを設けてある。β相コイル5
Bのコイルパターン5bは、図1の点線で示すように、
α相コイル5Aと同一のコイルパターンとし、絶縁シー
ト6の裏面にα相コイル5Aに対して電気角で90°の
位相差を持つように配置してある。すなわち、隣接する
2個(1対)の渦巻導体51bの外側導体を接続してあ
り、各渦巻導体51bの渦巻き中心部にスルーホール5
3Baを設けてある。互いに接続されてそれぞれ1対を
なす渦巻導体51bどうしの間には、渦巻き中心部のス
ルーホール53Baと同径の位置にスルーホール53B
bを設けてある。3対のうちの1対の渦巻導体51bど
うしの間には外周方向に向かって伸びるα相口出線52
bを設けてスルーホール53Bbに接続し、その他の対
の渦巻導体51bどうしの間には、表面に設けたα相コ
イル5Aの隣接する1対の渦巻導体51aどうしの渦巻
き中心部を接続するα相渡線54bを設けてある。
【0007】α相コイル5Aは、外周側に設けた+α端
子から裏側に設けたα相口出線52b、スルーホール5
3Bbを介して、表側に設けたコイルパターン5aのス
ルーホール53Aaに接続され、渦巻導体51aはスル
ーホール53Aaから外側に広がって隣接する渦巻導体
51の外側導体に接続される。隣接する渦巻導体51a
は外側導体から渦巻き中心部に向かって巻かれた後、渦
巻き中心部のスルーホール53Aaから裏面に設けたス
ルーホール53Bb、α相渡線54bを介して隣接する
渦巻導体51aの中心のスルーホール53Aaに接続さ
れる。このパターンをくり返し、一回りしてスルーホー
ル53Bb、α相口出線52bを介して外周側に設けた
−α端子に接続されて、6極のα相コイル5Aaを形成
している。β相コイル5Bは、外周側に設けた+β端子
から中心に向かって伸びる表面に設けたβ相口出線52
a、スルーホール53Abを介して、裏面に設けたコイ
ルパターン5bのスルーホール53Baに接続され、渦
巻導体51bは外側に広がって隣接する渦巻導体51b
の外側導体に接続される。隣接する渦巻導体51bは外
側側導体から中心に向かって巻かれた後、渦巻き中心部
のスルーホール53Baから表面に設けたスルーホール
53Ab、β相渡線52aを介して隣接する渦巻導体5
1bの渦巻き中心部のスルーホール53Baに接続され
る。このパターンをくり返して、一回りしてスルーホー
ル53Ab、β相口出52aを介して外周側に設けた−
β端子に接続されて6極のβ相コイルを形成している。
6極のレゾルバでは、α相、β相とも、検出相コイルの
1個の渦巻導体が占める角度は、渡線の幅を引いたほぼ
機械角60度となっている。また、α相、β相は互い
に、機械角で30度、電気角で90度位相がずれた状態
となっている。
【0008】ここで、従来例と上記実施例の検出相コイ
ルを比較してみると、1極の中に入る検出相コイルのα
相、β相のそれぞれの巻数を合わせた巻数は、両方ほぼ
同じである。α相、β相のそれぞれの相の占める1極あ
たりの面積は、従来の検出相コイルは励磁相コイルのほ
ぼ半分であった。しかし、上記実施例では励磁相コイル
と同じ面積となっている。すなわち、上記実施例の検出
相コイルのα相、β相のそれぞれの相の占める1極あた
りの面積は、従来のほぼ2倍になっている。実際の検出
相コイルでは、渦巻導体間の渡線を設ける必要から、従
来の検出相コイルの場合に比べて、実施例で完全に2倍
の面積を持つことはできなかったが、実験では鎖交磁束
は従来例の約1.5倍になった。更に、検出相コイルの
誘起電圧を定数とした場合、励磁相コイルの励磁電流
は、鎖交磁束に比例するため、従来例に比べて、約2/
3となっている。したがって、励磁相コイルの銅損は約
4/9に低減している。また、本発明による検出相コイ
ルのコイルパターンのパターンは励磁相コイルとほぼ同
じであるため、検出相コイルの巻数を最も大きくするこ
とができ、コイルの占積率も向上する。
【0009】図2(a),(b)は第2の実施例を示す
励磁相コイル7の同じ方向から見た平面図で、(a)は
円板状の絶縁シート8の表側に設けたコイルパターン7
a、(b)は絶縁シート8の裏側に設けたコイルパター
ン7bで、表裏とも第1の実施例の検出相コイルのコイ
ルパターンと形状を同一に形成してある。このコイルパ
ターン7a,7bは絶縁シート8の表側と裏側のコイル
パターンが位相差のないように配置し、表裏のコイルパ
ターン7a,7bを渦巻導体71a,71bの渦巻き中
心部に設けたスルーホール73a,73bで接続して1
回路を形成し、渦巻導体71bの外側導体の一部を開放
して、その端部を絶縁シート8の外周側に引き出し、励
磁電源端子+θ、−θに接続してある。したがって、各
渦巻導体71a,71bの占める角度は電気角で180
°となっており、1相6極の励磁相コイルを形成してあ
る。なお、検出相コイルとして使用した径方向渡線72
および外周側渡線74は使用しないが、励磁相コイルに
は影響がない。このように、励磁相コイルと検出相コイ
ル共に、渦巻導体を有する1種類のコイルパターンから
構成できるので、従来コイルパターンが2種類は必要で
あった場合に比べて製作コストを大幅に低減できる。
【0010】
【発明の効果】以上述べたように、本発明によれば、検
出相コイルの1極当たりのターン数は従来と同じである
のにもかかわらず、鎖交磁束が大幅に増え、励磁相コイ
ルの励磁電流が低減し、消費電力を大幅に低減できる。
また励磁相コイルと検出相コイルのコイルパターンを同
一にすることができるので、製作コストを大幅に低減で
きる効果がある。Description: BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a resolver in which a conductor is formed by a sheet coil. 2. Description of the Related Art Conventionally, as a sheet coil used in a motor or the like, a flat spiral conductor made of metal is opposed to both sides of a thin-film insulating sheet layer with a thin-film insulating sheet layer therebetween. An electric connection is disclosed (for example, Japanese Patent Publication No. 61-56700).
issue). For example, as shown in FIG. 3, an excitation voltage Eθ is applied to a one-phase excitation phase coil provided on the rotor, as shown in FIG.
Is applied to the two-phase detection phase coils α and β provided on the stator.
Output the detection voltages Eα and Eβ. When applied to a 6-pole, 1-phase excitation, 2-phase detection type resolver, the excitation phase coil is connected as shown in FIG.
In addition, it is conceivable that the detection coil is configured as shown in FIG. In FIG. 5, reference numeral 1 denotes an exciting phase coil, and coil patterns 1a, 1b each having six spiral conductors 11a, 11b spirally extending from the center of a six-pole spiral.
b, and the coil patterns 1a and 1b are affixed to the front and back with the disc-shaped insulating sheet 2 made of a polyimide sheet or the like interposed therebetween. When viewed from the same direction, the coil pattern 1a indicated by a solid line and the coil pattern 1b indicated by a dotted line are wound in opposite directions. A through hole 12 is provided at the center of the spiral of each pole, and the spiral conductor 11
a and 11b are connected to each other and spiral conductors 11a and 11b
Are connected to the outer ends of the adjacent spiral conductors 11a and 11b, respectively, and the outer ends + θ and −θ of two adjacent spiral conductors 11b are connected to an excitation power supply. In a six-pole resolver, the pole pitch has a mechanical angle of 60 degrees, and the angle occupied by one spiral conductor of the exciting phase coil 1 is a mechanical angle of 60 degrees. Therefore, 6 × 2 = 12 spiral conductors are arranged on both sides.
In FIG. 4, reference numeral 3 denotes a detection phase coil, which is provided with a coil pattern 31 having two spiral conductors 31a and 31b for one pole and spiral conductors 32a and 32b in order to form a two-phase detection phase coil. Coil pattern 32
It is attached so as to face the front and back with the disk-shaped insulating sheet 4 interposed therebetween. That is, one spiral conductor 31a connected to the + α terminal shown in FIG. 4 is provided on the front side of the insulating sheet 4, and the inner end of the conductor wound from the outer end of the spiral conductor 31a has a through hole 33a at the center of the spiral. Is connected to the inner end of the spiral conductor 32a on the back side, the outer end of the spiral conductor 32a is connected to the outer end of the spiral conductor 32a of the adjacent pole, and the through hole 33a at the center of the spiral of the spiral conductor 32a on the back side is connected. Are connected to the spiral conductor 31a on the front side, and are sequentially connected over six poles. The outer end of the last spiral conductor 31a is connected to the -α terminal to complete the detection phase coil 3α. Since one spiral conductor 31b of the detection phase coil 3β connected to the + β terminal has a phase difference of 90 degrees in electrical angle with respect to the detection phase coil 3α, it has a phase difference of 30 degrees in mechanical angle. It is provided on the front side of the insulating sheet 4 adjacent to the spiral conductor 31a of the detection phase coil 3α. The conductor wound from the outer end of the spiral conductor 31b has an inner end at the center of the spiral of the spiral through the through-hole 33b and the spiral conductor 32b on the back side.
The outer end of the spiral conductor 32b is connected to the outer end of the spiral conductor 32b of the adjacent pole, and the spiral conductor 32b on the back side is connected from the through hole 33b at the center of the spiral to the front spiral conductor 31b. Are sequentially connected over six poles, and the outer end of the last spiral conductor 31b is connected to the -β terminal to complete the detection phase coil 3β. The spiral conductors 31a and 31b provided on the front side of the insulating sheet 4 and the spiral conductors 32a and 32 provided on the back side of the insulating sheet 4
Since two poles b are provided for each pole, there are 12 poles for 6 poles, and the angle occupied by one spiral conductor is 30 degrees in mechanical angle. In the prior art, however, the angle occupied by one spiral conductor of the exciting phase coil is 60 degrees in mechanical angle, whereas the angle of one spiral of the detecting phase coil is one. The angle occupied by the conductor is 30 degrees in mechanical angle. The total number of turns of the α-phase and β-phases of the detection phase coil included in one pole is almost the same as the number of turns of the excitation phase coil included in one pole. The area per pole occupied by the phase is approximately half that of the exciting phase coil. By the way, in general, the flux linkage Φ of the detection phase coil is expressed by the following (1)
It is represented by an equation. Φ = n · H I · μ 0 · (S / g) ... (1) where, n represents the detected phase coil turns, H I is the magnetomotive force generated by the excitation phase coil, mu 0 is the permeability, S is The area where the magnetic flux of the exciting phase coil is linked to the detection phase coil, g is a gap value. Therefore, since the area per pole occupied by the α-phase and β-phase of the detection phase coil is almost half of the excitation phase coil, the detection phase coil sufficiently links the magnetic flux generated by the excitation phase coil. As a result, the induced voltage of the detection phase coil cannot be sufficiently increased, which leads to an increase in power consumption. An object of the present invention is to provide a resolver that can increase induced voltage and reduce power consumption by increasing the interlinkage magnetic flux area of a detection phase coil. In order to solve the above-mentioned problem, the present invention is directed to the present invention, in which the angle of each pole of the pole pair X is 1 electrical angle.
It is composed of one phase formed by a flat sheet coil so as to form an angle of 80 °.
The spiral center provided on the coil pattern on one side
Vortex in the through hole of the other side and the coil pattern on the other side
Form one circuit by connecting through-hole at center of winding
Open a part of the circuit and connect both ends to the excitation power supply end.
And excitation phase coil connected to the child, composed of two phases of α-phase coil and β-phase coils having a phase difference of 90 ° in electrical angle from each other which is formed by a planar sheet coil opposed via a gap in the excitation phase coil As well as the insulation sheet
It is provided on one side and a pair of adjacent spiral conductors are
Α-phase coil pattern consisting of X pairs of spiral conductors connected in a row
And an adjacent pair provided on the other surface of the insulating sheet.
X pairs of spiral conductors connected in series with each other
Β-phase coil pattern and the spiral of the spiral conductor
A detection coil having a first through hole provided in a core portion , wherein the detection phase coil has the same diameter as the center of the spiral at the position having the same diameter.
A second through hole provided between the spiral conductors;
Two first through hoes provided between the spiral conductors
Two α-phase outlets respectively connected to the
The spiral conductor excluding a first through hole connected to an outgoing line;
Connected to the first through hole provided between
An α-phase connecting wire connecting a pair of adjacent α-phase coils;
Two second through holes provided between spiral conductors
And two β-phase outlets respectively connected to the
The spiral conductor except for the second through hole connected to the wire
Connected to the second through hole provided between
And a β-phase connecting wire connecting a pair of β-phase coils in contact with each other. According to the above-mentioned means, the detection phase coil has a coil pattern composed of X pairs of spiral conductors forming only an α phase coil on one surface of the insulating sheet and only a β phase coil on the other surface. Since the coil pattern composed of the X pairs of spiral conductors to be formed is provided, the area occupied by one spiral conductor of the detection phase coil is substantially the same as the area occupied by one spiral conductor of the excitation phase coil. In comparison, the linkage flux is greatly increased. As a result, the induced voltage of the detection phase coil increases, and the power consumption decreases. In addition, since the same coil pattern as the detection phase coil is attached to both sides of the insulating sheet to form the excitation phase coil, the coil pattern for the detection coil and the excitation coil can be shared. Can be reduced. An embodiment of the present invention will be described below with reference to the drawings. FIG. 1 is a plan view showing a detection phase coil according to a first embodiment of the present invention. The exciting phase coil 1 has the same configuration as that described in the conventional example with reference to FIG. In the figure,
Reference numeral 5 denotes a detection phase coil, in which an α-phase coil 5A is formed on one surface (front surface) of a disc-shaped insulating sheet 6 and the other surface (back surface).
Is formed with a β-phase coil 5B. As shown by the solid line in FIG. 1, the coil pattern 5a of the α-phase coil 5A is composed of six (three pairs) spiral conductors 51a, each of which is spirally wound from the center of the six-pole spiral and spreads one by one. Are arranged on the surface of the insulating sheet 6 so that the angle occupied by the electrical sheet becomes approximately 180 degrees in electrical angle. In addition, two adjacent (1
The outer conductor of the spiral conductor 51a of the (pair) is connected, and a through hole 53Aa is provided at the center of the spiral of each spiral conductor 51a. A through-hole 53Ab is provided between the pair of spiral conductors 51a connected to each other and at the same diameter as the through-hole 53Aa at the center of the spiral. A β-phase lead wire 52a extending toward the outer peripheral direction is provided between one pair of the spiral conductors 51a of the three pairs and connected to the through hole 53Ab. , Β-phase coil 5B provided on the back side
Is provided with a .beta.-phase interconnecting line 54a connecting the center of the spiral between a pair of adjacent spiral conductors 51b. β phase coil 5
As shown by the dotted line in FIG. 1, the coil pattern 5b of B
It has the same coil pattern as the α-phase coil 5A, and is arranged on the back surface of the insulating sheet 6 so as to have a phase difference of 90 ° in electrical angle with respect to the α-phase coil 5A. That is, the outer conductors of two adjacent (one pair) spiral conductors 51b are connected, and a through hole 5 is formed at the center of the spiral of each spiral conductor 51b.
3Ba is provided. Between the pair of spiral conductors 51b connected to each other, a through hole 53B is formed at the same diameter as the through hole 53Ba at the center of the spiral.
b is provided. Α-phase lead wire 52 extending toward the outer peripheral direction between a pair of spiral conductors 51b of the three pairs
b is connected to the through hole 53Bb, and between the other pair of spiral conductors 51b, the spiral center of a pair of adjacent spiral conductors 51a of the α-phase coil 5A provided on the surface is connected. A phase transfer line 54b is provided. The α-phase coil 5A is connected to an α-phase lead wire 52b and a through hole 5
Via 3Bb, it is connected to the through hole 53Aa of the coil pattern 5a provided on the front side, and the spiral conductor 51a is connected to the outer conductor of the adjacent spiral conductor 51 which extends outward from the through hole 53Aa. Adjacent spiral conductor 51a
Is wound from the outer conductor toward the center of the spiral, and then through the through hole 53Aa at the center of the spiral, the through hole 53Bb provided on the back surface, and the through hole 53Aa at the center of the adjacent spiral conductor 51a via the α-phase transition wire 54b. Connected to. This pattern is repeated, and the circuit is turned around and connected to the -α terminal provided on the outer peripheral side via the through-hole 53Bb and the α-phase lead wire 52b to form a six-pole α-phase coil 5Aa. The β-phase coil 5B has a β-phase lead wire 52 provided on a surface extending from the + β terminal provided on the outer peripheral side toward the center.
a, the spiral conductor 51b is connected to the through-hole 53Ba of the coil pattern 5b provided on the back surface through the through-hole 53Ab, and the spiral conductor 51b spreads outward and is adjacent to the spiral conductor 51b.
Is connected to the outer conductor. The adjacent spiral conductor 51b is wound from the outer conductor toward the center, and then through the through hole 53Ba at the center of the spiral, the through hole 53Ab provided on the surface, and the adjacent spiral conductor 5 via the β-phase transition line 52a.
1b is connected to the through hole 53Ba at the center of the spiral. This pattern was repeated, and the circuit was turned around and provided on the outer peripheral side through the through-hole 53Ab and the β-phase outlet 52a.
It is connected to the β terminal to form a 6-pole β-phase coil.
In the six-pole resolver, the angle occupied by one spiral conductor of the detection phase coil in both the α phase and the β phase is approximately 60 degrees of the mechanical angle obtained by subtracting the width of the crossover. The α phase and β phase are out of phase with each other by 30 degrees in mechanical angle and 90 degrees in electrical angle. Here, a comparison between the detection phase coils of the conventional example and the above-mentioned embodiment will be described.
The number of turns obtained by adding the number of turns of each of the phase and the β phase is substantially the same. The area per pole occupied by each of the α-phase and the β-phase is approximately half that of the conventional detection phase coil compared to the excitation phase coil. However, in the above embodiment, it has the same area as the exciting phase coil. That is, the area per pole occupied by each of the α phase and the β phase of the detection phase coil of the above embodiment is almost twice as large as that of the related art. In the actual detection phase coil, since it is necessary to provide the wiring between the spiral conductors, the area could not be completely doubled in the embodiment in comparison with the case of the conventional detection phase coil. Interchange magnetic flux was about 1.5 times that of the conventional example. Further, when the induced voltage of the detection phase coil is a constant, the excitation current of the excitation phase coil is proportional to the interlinkage magnetic flux.
It is 3. Therefore, the copper loss of the exciting phase coil is reduced to about 4/9. In addition, since the pattern of the coil pattern of the detection phase coil according to the present invention is substantially the same as that of the excitation phase coil, the number of turns of the detection phase coil can be maximized, and the space factor of the coil is improved. FIGS. 2 (a) and 2 (b) are plan views of the exciting phase coil 7 according to the second embodiment viewed from the same direction. FIG. 2 (a) is provided on the front side of a disc-shaped insulating sheet 8. Coil pattern 7
(a) and (b) are coil patterns 7b provided on the back side of the insulating sheet 8, and have the same shape on both sides as the coil pattern of the detection phase coil of the first embodiment. The coil patterns 7a and 7b are arranged so that the front and back coil patterns of the insulating sheet 8 have no phase difference, and the front and back coil patterns 7a and 7b are provided at the center of the spiral of the spiral conductors 71a and 71b. , 73b and 1
A circuit is formed, a part of the outer conductor of the spiral conductor 71b is opened, and its end is pulled out to the outer peripheral side of the insulating sheet 8 and connected to the excitation power supply terminals + θ, -θ. Therefore, the angle occupied by each of the spiral conductors 71a and 71b is 180 electrical degrees.
° to form a one-phase six-pole excitation phase coil. Note that the radial wiring 72 used as the detection phase coil was used.
Also, the outer transition wire 74 is not used, but does not affect the exciting phase coil. As described above, since both the excitation phase coil and the detection phase coil can be composed of one type of coil pattern having a spiral conductor, the production cost can be greatly reduced as compared with the case where two types of conventional coil patterns are required. As described above, according to the present invention, although the number of turns per pole of the detection phase coil is the same as that of the prior art, the flux linkage is greatly increased. The exciting current of the exciting phase coil is reduced, and the power consumption can be greatly reduced.
Further, since the coil patterns of the excitation phase coil and the detection phase coil can be made identical, there is an effect that the manufacturing cost can be greatly reduced.
【図面の簡単な説明】
【図1】 本発明の第1の実施例の検出相コイルを示す
平断面図である。
【図2】 本発明の第2の実施例の励磁相コイルを示す
平断面図である。
【図3】 レゾルバの結線図である。
【図4】 従来例の検出相コイルを示す平断面図であ
る。
【図5】 従来例の励磁相コイルを示す平断面図であ
る。
【符号の説明】
1、7 励磁相コイル、1a,1b、5a,5b,7
a,7b コイルパターン、11a.11b、31、3
2、51a,51b、71a,71b 渦巻導体、1
2、33a,33b,53Aa,53Ab,53Ba,
53Bb,73a,73b スルーホール,2,4,
6,8 絶縁シート、3、5 検出相コイル、5A α
相コイル、5B β相コイル、52a β相口出線,5
2b α相口出線、54a β相渡線,54b α相渡
線BRIEF DESCRIPTION OF THE DRAWINGS FIG. 1 is a plan sectional view showing a detection phase coil according to a first embodiment of the present invention. FIG. 2 is a plan sectional view showing an exciting phase coil according to a second embodiment of the present invention. FIG. 3 is a connection diagram of a resolver. FIG. 4 is a plan sectional view showing a conventional detection phase coil. FIG. 5 is a plan sectional view showing a conventional excitation phase coil. [Description of Signs] 1, 7 Excitation phase coils, 1a, 1b, 5a, 5b, 7
a, 7b coil pattern, 11a. 11b, 31, 3
2, 51a, 51b, 71a, 71b spiral conductor, 1
2, 33a, 33b, 53Aa, 53Ab, 53Ba,
53Bb, 73a, 73b Through hole, 2, 4,
6,8 Insulation sheet, 3,5 Detection phase coil, 5A α
Phase coil, 5B β phase coil, 52a β phase lead wire, 5
2b α-phase exit line, 54a β-phase transition line, 54b α-phase transition line
───────────────────────────────────────────────────── フロントページの続き (56)参考文献 特開 平4−222447(JP,A) 特開 昭63−65302(JP,A) (58)調査した分野(Int.Cl.7,DB名) H02K 3/26 G01B 7/00 G01B 7/30 101 G01D 5/245 101 H02K 24/00 ────────────────────────────────────────────────── ─── Continuation of the front page (56) References JP-A-4-222447 (JP, A) JP-A-63-65302 (JP, A) (58) Fields investigated (Int. Cl. 7 , DB name) H02K 3/26 G01B 7/00 G01B 7/30 101 G01D 5/245 101 H02K 24/00
Claims (1)
0°となるように平面状シートコイルによって形成した
1相から構成されると共に、絶縁シート(8)の両方の
面に設け、一方の面のコイルパターン(7a)に設けた
渦巻き中心部のスルーホール(73a)と他方の面のコ
イルパターン(7b)に設けた渦巻き中心部のスルーホ
ール(73b)とを接続して1回路を形成し,その1回
路の一部を開放してその両端を励磁電源端子(+θ、−
θ)に接続した励磁相コイル(7)と、 前記励磁相コイル(7)に空隙を介して対向する平面状
シートコイルによって形成した互いに電気角で90°の
位相差を持つα相コイル(5A)およびβ相コイル(5
B)の2相から構成されると共に、絶縁シート(6)の
一方の面に設け、隣り合う1対の渦巻き導体(51a)
どうしを直列に接続したX対の渦巻導体からなるα相コ
イルパターン(5a)と、前記絶縁シート(6)の他方
の面に設け、隣り合う1対の渦巻き導体(51b)どう
しを直列に接続したX対の渦巻導体からなるβ相コイル
パターン(5b)と、前記渦巻導体(51a)の渦巻き
中心部に設けた第1のスルーホール(53Aa、53B
b)を有してなる検出相コイル(5)とを備えたシート
コイル形レゾルバにおいて、 前記検出相コイル(5)は、前記渦巻き中心部と同径の
位置で前記渦巻導体(51a)どうしの間に設けた第2
のスルーホール(53Ab、53Ba)と、 前記渦巻導体(51b)どうしの間に設けた二つの第1
のスルーホール(53Aa、53Bb)にそれぞれ接続
する2本のα相口出線(52b)と、 前記α相口出線(52b)に接続する第1のスルーホー
ル(53Aa、53Bb)を除く前記渦巻導体(51
b)どうしの間に設けた第1のスルーホール(53A
a、53Bb)に接続して前記隣接する1対のα相コイ
ルを接続するα相渡線(54b)と、 前記渦巻導体(51a)どうしの間に設けた二つの第2
のスルーホール(53Ab、53Ba)にそれぞれ接続
する2本のβ相口出線(52a)と、 前記β相口出線(52a)に接続する第2のスルーホー
ル(53Ab、53Ba)を除く前記渦巻導体(51
a)どうしの間に設けた第2のスルーホール(53A
b、53Ba)に接続して前記隣接する1対のβ相コイ
ルを接続するβ相渡線(54a) とを備えたことを特徴
とするシートコイル型レゾルバ。(57) [Claims 1] The angle of each pole of the number X of pole pairs is 18 in electrical angle.
It is composed of one phase formed by a planar sheet coil so as to be 0 °, and both of the insulating sheet (8)
Provided on one side, and provided on the coil pattern (7a) on one side.
The through hole (73a) at the center of the spiral and the
Through hole at the center of the spiral provided in the oil pattern (7b)
(73b) to form one circuit, and
Open a part of the path and connect both ends to the excitation power supply terminals (+ θ,-
and excitation phase coils connected to θ) (7), α-phase coils having a phase difference of 90 ° in electrical angle from each other which is formed by a planar sheet coil opposed via a gap in the excitation phase coil (7) (5A ) And β-phase coil (5
B) and the insulating sheet (6)
A pair of adjacent spiral conductors (51a) provided on one surface
Α-phase core consisting of X pairs of spiral conductors connected in series
The other side of the insulating pattern (6)
And a pair of adjacent spiral conductors (51b)
Β-phase coil consisting of X pairs of spiral conductors connected in series
A pattern (5b) and a spiral of the spiral conductor (51a)
The first through holes (53Aa, 53B
b) a detection coil having a detection phase coil (5) , wherein the detection phase coil (5) has the same diameter as the center of the spiral.
At a position between the spiral conductors (51a).
Of the spiral conductor (51b) and two first holes provided between the spiral conductors ( 51B) .
Through holes (53Aa, 53Bb)
Two α-phase outlets (52b) to be connected to each other and a first through hole connected to the α-phase outlet (52b).
(53Aa, 53Bb) except for the spiral conductor (51
b) First through holes (53A) provided between
a, 53Bb) connected to the pair of adjacent α-phase coils.
Α connecting wire (54b) connecting the two spiral conductors (51a) and two second
Through holes (53Ab, 53Ba)
Two β-phase outlets (52a) and a second through-hole connected to the β-phase outlet (52a).
(53Ab, 53Ba) except for the spiral conductor (51
a) A second through hole (53A) provided between
b, 53Ba) connected to the pair of adjacent β-phase coils.
And a β- phase transition wire (54a) for connecting the coil to the sheet coil type resolver.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP24200794A JP3536375B2 (en) | 1994-09-08 | 1994-09-08 | Sheet coil type resolver |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP24200794A JP3536375B2 (en) | 1994-09-08 | 1994-09-08 | Sheet coil type resolver |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH0884449A JPH0884449A (en) | 1996-03-26 |
| JP3536375B2 true JP3536375B2 (en) | 2004-06-07 |
Family
ID=17082878
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP24200794A Expired - Lifetime JP3536375B2 (en) | 1994-09-08 | 1994-09-08 | Sheet coil type resolver |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JP3536375B2 (en) |
Families Citing this family (6)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US6628038B1 (en) | 1999-01-14 | 2003-09-30 | Kabushiki Kaisha Yaskawa Kenki | Resolver using sheet coil |
| KR100311900B1 (en) * | 1999-02-20 | 2001-11-02 | 제환영 | A Thin Film Coil for Motors or Generators |
| JP4602749B2 (en) | 2004-12-10 | 2010-12-22 | ミネベア株式会社 | Flat type resolver |
| US8710829B2 (en) | 2009-06-19 | 2014-04-29 | Minebea Co., Ltd. | Sheet coil type resolver |
| JP5755099B2 (en) * | 2011-10-06 | 2015-07-29 | 愛三工業株式会社 | Angle sensor |
| US10295374B1 (en) * | 2016-07-13 | 2019-05-21 | Igarashi Electric Works Ltd. | Rotation angle detecting device and an electric motor provided with the rotation angle detecting device |
-
1994
- 1994-09-08 JP JP24200794A patent/JP3536375B2/en not_active Expired - Lifetime
Also Published As
| Publication number | Publication date |
|---|---|
| JPH0884449A (en) | 1996-03-26 |
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