JPH023288B2 - - Google Patents
Info
- Publication number
- JPH023288B2 JPH023288B2 JP59204084A JP20408484A JPH023288B2 JP H023288 B2 JPH023288 B2 JP H023288B2 JP 59204084 A JP59204084 A JP 59204084A JP 20408484 A JP20408484 A JP 20408484A JP H023288 B2 JPH023288 B2 JP H023288B2
- Authority
- JP
- Japan
- Prior art keywords
- coil
- core
- rotary transformer
- raw material
- manufacturing
- 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
- 239000002994 raw material Substances 0.000 claims description 26
- 238000000034 method Methods 0.000 claims description 23
- 238000010304 firing Methods 0.000 claims description 21
- 238000004519 manufacturing process Methods 0.000 claims description 21
- 239000011230 binding agent Substances 0.000 claims description 14
- 229910001035 Soft ferrite Inorganic materials 0.000 claims description 8
- 239000006247 magnetic powder Substances 0.000 claims description 8
- 238000005238 degreasing Methods 0.000 claims description 4
- 238000010438 heat treatment Methods 0.000 claims description 2
- 238000004898 kneading Methods 0.000 claims 1
- 230000035699 permeability Effects 0.000 description 13
- 238000000605 extraction Methods 0.000 description 11
- 238000000748 compression moulding Methods 0.000 description 8
- 230000008878 coupling Effects 0.000 description 5
- 238000010168 coupling process Methods 0.000 description 5
- 238000005859 coupling reaction Methods 0.000 description 5
- 238000005498 polishing Methods 0.000 description 5
- 239000000843 powder Substances 0.000 description 5
- 238000010586 diagram Methods 0.000 description 4
- 238000001746 injection moulding Methods 0.000 description 4
- 238000003754 machining Methods 0.000 description 4
- 230000006835 compression Effects 0.000 description 2
- 238000007906 compression Methods 0.000 description 2
- 230000000694 effects Effects 0.000 description 2
- 230000004907 flux Effects 0.000 description 2
- 238000000227 grinding Methods 0.000 description 2
- 238000002347 injection Methods 0.000 description 2
- 239000007924 injection Substances 0.000 description 2
- 239000000314 lubricant Substances 0.000 description 2
- 238000002156 mixing Methods 0.000 description 2
- 238000007517 polishing process Methods 0.000 description 2
- 238000012805 post-processing Methods 0.000 description 2
- 239000002002 slurry Substances 0.000 description 2
- 239000000853 adhesive Substances 0.000 description 1
- 230000001070 adhesive effect Effects 0.000 description 1
- 238000006243 chemical reaction Methods 0.000 description 1
- 230000008602 contraction Effects 0.000 description 1
- 230000006866 deterioration Effects 0.000 description 1
- 238000009434 installation Methods 0.000 description 1
- 239000000463 material Substances 0.000 description 1
- 239000000203 mixture Substances 0.000 description 1
- 239000002245 particle Substances 0.000 description 1
- 230000002093 peripheral effect Effects 0.000 description 1
- 239000011148 porous material Substances 0.000 description 1
- 238000012545 processing Methods 0.000 description 1
- 229920006395 saturated elastomer Polymers 0.000 description 1
- 230000008054 signal transmission Effects 0.000 description 1
- 239000007790 solid phase Substances 0.000 description 1
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01F—MAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
- H01F41/00—Apparatus or processes specially adapted for manufacturing or assembling magnets, inductances or transformers; Apparatus or processes specially adapted for manufacturing materials characterised by their magnetic properties
- H01F41/02—Apparatus or processes specially adapted for manufacturing or assembling magnets, inductances or transformers; Apparatus or processes specially adapted for manufacturing materials characterised by their magnetic properties for manufacturing cores, coils, or magnets
- H01F41/0206—Manufacturing of magnetic cores by mechanical means
- H01F41/0246—Manufacturing of magnetic circuits by moulding or by pressing powder
Landscapes
- Engineering & Computer Science (AREA)
- Power Engineering (AREA)
- Manufacturing & Machinery (AREA)
- Recording Or Reproducing By Magnetic Means (AREA)
Description
【発明の詳細な説明】
〔発明の利用分野〕
本発明は、ロータリトランス、特にそれのコア
の製造方法に関する。DETAILED DESCRIPTION OF THE INVENTION [Field of Application of the Invention] The present invention relates to a rotary transformer, and in particular to a method for manufacturing a core thereof.
回転部電気回路と静止部電気回路とを有する装
置、例えば回転ヘツド型VTRの回転ドラム装置
には、回転部と静止部との相互間の電気信号伝達
手段としてロータリトランスが広く採用されてい
る。
2. Description of the Related Art Rotary transformers are widely used as means for transmitting electric signals between the rotating part and the stationary part in devices having an electric circuit for a rotating part and an electric circuit for a stationary part, for example, a rotating drum apparatus of a rotating head type VTR.
第8図はこの種のロータリトランスのうちの偏
平型と呼ばれるロータリトランスの断面図、第9
図は第8図に示すロータリトランスのステータ側
コアの平面図、第10図は第8図に示すロータリ
トランスのロータ側コアの平面図である。 Figure 8 is a cross-sectional view of a rotary transformer called a flat type among this type of rotary transformer.
8 is a plan view of the stator side core of the rotary transformer shown in FIG. 8, and FIG. 10 is a plan view of the rotor side core of the rotary transformer shown in FIG. 8.
これらの図において、1はステータ側コア、2
はロータ側コアであり、両コア1,2は40〜
70μm程度の磁気ギヤツプGを介して対向してい
る。ステータ側コア1の上面には、同心円状の複
数本のコイル溝1aと、これらコイル溝1aに直
交する複数本のコイル引出溝1bとがそれぞれ設
けられており、各コイル溝1aにはコイル3が所
定ターン数巻回され、それぞれのコイル3は各コ
イル引出溝1bを通つて静止部電気回路(図示せ
ず)に接続されている。 In these figures, 1 is the stator side core, 2
is the rotor side core, and both cores 1 and 2 are 40~
They face each other via a magnetic gap G of about 70 μm. A plurality of concentric coil grooves 1a and a plurality of coil extraction grooves 1b orthogonal to these coil grooves 1a are provided on the upper surface of the stator side core 1, and each coil groove 1a has a coil 3. is wound a predetermined number of turns, and each coil 3 is connected to a stationary part electric circuit (not shown) through each coil lead-out groove 1b.
一方、ロータ側コア2の下面にも、上述したス
テータ側コア1と同様に、同心円状の複数本のコ
イル溝2aと、各コイル溝2aに直交する複数本
のコイル引出溝2bとが設けられており、各コイ
ル溝2aにはコイル4が所定ターン数巻回され、
それぞれのコイル4は各コイル引出溝2bを通つ
て回転部電気回路(図示せず)に接続されてい
る。 On the other hand, the lower surface of the rotor side core 2 is also provided with a plurality of concentric coil grooves 2a and a plurality of coil extraction grooves 2b orthogonal to each coil groove 2a, similarly to the stator side core 1 described above. A coil 4 is wound in each coil groove 2a with a predetermined number of turns.
Each coil 4 is connected to a rotating part electric circuit (not shown) through each coil extraction groove 2b.
このように構成されたロータリトランスにおい
て、各コイル4に回転部からの電気信号が電流波
形として加えられると、これによつて磁束が発生
し、該磁束の一部は各コイル4に対向するそれぞ
れのコイル3に鎖交し、各コイル3に電圧を誘起
する。このコイル3の誘起電圧は、両コイル3,
4間の結合係数Kが一定であればコイル4に加え
られた電圧に比例するため、相対的に回転運動す
るコイル3,4間で信号の伝達ができる。 In the rotary transformer configured as described above, when an electric signal from the rotating part is applied to each coil 4 as a current waveform, a magnetic flux is generated, and a part of the magnetic flux is distributed to each coil 4 facing each other. The coils 3 are linked to each other, and a voltage is induced in each coil 3. The induced voltage of this coil 3 is
If the coupling coefficient K between coils 4 and 4 is constant, it will be proportional to the voltage applied to coil 4, so that signals can be transmitted between coils 3 and 4 that rotate relative to each other.
そして、従来、かかるロータリトランスのコア
1,2の製造方法としては、ソフトフエライト磁
性粉末を金型内で一軸方向に圧縮する圧縮成形法
が一般的に用いられている。以下、この圧縮成形
法によるロータリトランスの製造方法について説
明する。 Conventionally, as a method for manufacturing the cores 1 and 2 of such a rotary transformer, a compression molding method is generally used in which soft ferrite magnetic powder is compressed in a uniaxial direction within a mold. A method for manufacturing a rotary transformer using this compression molding method will be described below.
まず、ソフトフエライト磁性粉末に適量の潤滑
剤(粉末)を混合して粉末状の原材料を造粒し、
これを金型に入れ、機械プレスや油圧プレスで一
軸方向に加圧することによつて、コイル溝とコイ
ル引出溝とを有するコア素体を成形する。次に、
このコア素体を適当な雰囲気中で高温(1000〜
1400℃程度)に加熱し、粉末間の固相化学反応を
進めながら高密度化し、所望の磁気的性質と機械
的強さをもつコア1,2の焼結体を得る。 First, the powdered raw material is granulated by mixing an appropriate amount of lubricant (powder) with soft ferrite magnetic powder.
This is placed in a mold and pressurized in a uniaxial direction using a mechanical press or a hydraulic press to form a core body having a coil groove and a coil extraction groove. next,
This core body is heated to a high temperature (1000 ~
(approximately 1,400°C), the powder is densified while proceeding with a solid phase chemical reaction between the powders, and a sintered body of cores 1 and 2 having desired magnetic properties and mechanical strength is obtained.
このようにして得られたコア1,2は、原材料
の粉末同志、あるいは原材料と金型間の摩擦によ
り、圧縮成形時の加圧力が金型内に充填された原
材料に均一に伝達されず、そのため、コア素体を
焼成した際に部分的に収縮率が異なり、変形やソ
リなどを生じる。そこで、焼成後のコア1,2に
表面研摩や研削などの機械加工を施し、両面の平
行度や平面度を出し、最後に各コイル溝1a,1
bにコイル3,4を巻装・接着して、第8図に示
すロータリトランスを得る。 In the cores 1 and 2 obtained in this way, the pressure force during compression molding is not uniformly transmitted to the raw material filled in the mold due to friction between the raw material powders or between the raw material and the mold. Therefore, when the core body is fired, the shrinkage rate differs locally, causing deformation and warping. Therefore, the cores 1 and 2 after firing are subjected to mechanical processing such as surface polishing and grinding to achieve parallelism and flatness on both sides, and finally each coil groove 1a, 1
Coils 3 and 4 are wound and glued around b to obtain the rotary transformer shown in FIG.
しかしながら、かかる従来のロータリトランス
の製造方法においては、コイル溝やコイル引出溝
を有する複雑形状のコア素体を圧縮成形法にて製
造してなるため、金型内の原材料の充填度に不均
一性を生じ、その結果、上述の如く、焼成後のコ
ア1,2に変形やソリを生じるという不具合があ
る。これら変形やソリは僅かなものであるが、ロ
ータリトランスでは両コア1,2間の磁気ギヤツ
プGに高精度が要求されるため、コア1,2の表
面の平行度を10μm以下に保たなければならず、
そのため、表面研摩などの機械加工によつてコア
1,2の表面を精度出しするという煩雑な加工が
必要であつた。 However, in such conventional manufacturing methods for rotary transformers, a complex-shaped core body with coil grooves and coil extraction grooves is manufactured by compression molding, so the degree of filling of raw materials in the mold is uneven. As a result, as mentioned above, the cores 1 and 2 after firing are deformed and warped. Although these deformations and warps are slight, rotary transformers require high precision in the magnetic gap G between both cores 1 and 2, so the parallelism of the surfaces of cores 1 and 2 must be maintained at 10 μm or less. Not necessarily,
Therefore, it has been necessary to perform complicated machining such as surface polishing to improve the precision of the surfaces of the cores 1 and 2.
また、焼成時における原材料の熱収縮率は10〜
20%にもおよぶため、金型内の原材料の充填度に
不均一性を生じると、部分的な収縮率の違いによ
りコイル溝1a,2aの溝径精度や同心度が得ら
れず、予め所定形状に成形されたコイル3,4を
各コイル溝1a,2a内に接着・固定する作業が
困難になるという不具合も生じる。 In addition, the heat shrinkage rate of raw materials during firing is 10~
20%, so if there is non-uniformity in the degree of filling of the raw material in the mold, the groove diameter accuracy and concentricity of the coil grooves 1a and 2a cannot be obtained due to the difference in local shrinkage rates, and the predetermined Another problem arises in that it becomes difficult to adhere and fix the shaped coils 3 and 4 into the respective coil grooves 1a and 2a.
また、第11図は、円筒型(同軸型)と呼ばれ
るロータリトランスの断面図であつて、上述した
第8図に対応する部分には同一符号を付けてあ
る。 Moreover, FIG. 11 is a cross-sectional view of a rotary transformer called a cylindrical type (coaxial type), and parts corresponding to those in FIG. 8 described above are given the same reference numerals.
かかる円筒型ロータリトランスのコア1,2の
製造方法も、基本的には偏平型ロータリトランス
のコア1,2と同様に、ソフトフエライト磁性粉
末に適量の潤滑剤(粉末)を混合して粉末状とし
た原材料を圧縮成形し、これを焼結するものであ
るが、この場合、複雑形状のコア素体を金型で成
形することが困難であるため、まず円筒状のコア
素体を圧縮成形した後、これにコイル溝1a,2
aを機械加工により形成し、その後に焼成すると
いう煩雑な工程が採用されている。 The method for manufacturing the cores 1 and 2 of such a cylindrical rotary transformer is basically the same as the cores 1 and 2 of the flat rotary transformer, in which soft ferrite magnetic powder is mixed with an appropriate amount of lubricant (powder). The raw material is compression molded and then sintered. However, in this case, it is difficult to mold the complex-shaped core body with a mold, so first the cylindrical core body is compression molded. After that, insert coil grooves 1a and 2 into this.
A complicated process is employed in which a is formed by machining and then fired.
しかしながら、円筒型ロータリトランスにおい
ては、磁気ギヤツプGの寸法精度は、コア1の内
径寸法とコア2の外径寸法とによつて決まるた
め、コア1,2の径にミクロンオーダの寸法精度
が要求され、そのため、金型内の原材料の充填度
に不均一性を生じ易い圧縮成形法では、焼成後に
コア1,2の周面を研摩するという煩雑な加工が
必要であつた。 However, in a cylindrical rotary transformer, the dimensional accuracy of the magnetic gap G is determined by the inner diameter dimension of core 1 and the outer diameter dimension of core 2, so dimensional precision on the order of microns is required for the diameters of cores 1 and 2. Therefore, in the compression molding method, which tends to cause non-uniform filling of the raw material in the mold, the complicated process of polishing the peripheral surfaces of the cores 1 and 2 after firing is necessary.
本発明の目的は、上述した従来技術の欠点を除
き、コアの表面研摩加工を省略し、安価なロータ
リトランスの製造方法を提供するにある。
SUMMARY OF THE INVENTION An object of the present invention is to provide an inexpensive method for manufacturing a rotary transformer that eliminates the drawbacks of the prior art described above, omits surface polishing of the core.
この目的を達成するために、本発明は、ソフト
フエライト磁性粉末に15〜50容量%のバインダを
加熱混練してスラリー状の原材料を得た後、この
原材料を金型内に射出してコイル溝を有するコア
素体を成形し、しかる後、このコア素体を300〜
500℃の温度で脱脂し、さらに1000〜1400℃の温
度で焼成してコアを製造するようにした点に特徴
がある。
In order to achieve this objective, the present invention heats and kneads 15 to 50% by volume of binder with soft ferrite magnetic powder to obtain a slurry-like raw material, and then injects this raw material into a mold to form coil grooves. After that, this core element is molded with 300 ~
The unique feature is that the core is manufactured by degreasing at a temperature of 500°C and then firing at a temperature of 1000 to 1400°C.
すなわち、本発明は、特公昭55−33173号公報
などに示された永久磁石の製造方法として知られ
ている射出成形法を利用してコア素体を成形し、
このコア素体を脱脂・焼成してコアを製造するよ
うにしたものである。かかる射出成形法は、原材
料の流動性を良くするために多量のバインダ(結
合剤)が必要であり、そのため、焼成後のコアが
多孔質となつてコアの透磁率μが劣化することが
わかつており、それ故、従来は高い透磁率が必要
とされているロータリトランスの製造方法には不
適であるとされていた。 That is, the present invention molds the core body using an injection molding method known as a method for producing permanent magnets as disclosed in Japanese Patent Publication No. 55-33173.
This core body is degreased and fired to produce a core. This injection molding method requires a large amount of binder to improve the fluidity of the raw materials, and as a result, the core after firing becomes porous and the magnetic permeability μ of the core deteriorates. Therefore, it was conventionally considered to be unsuitable for the manufacturing method of rotary transformers, which require high magnetic permeability.
しかしながら、本発明者らは、コア間の磁気ギ
ヤツプを介して使用されるロータリトランスにお
いては、信号伝達経路中のコアの透磁率μの影響
が直線的にあらわれないことを実験的に見出し
た。 However, the present inventors have experimentally found that in a rotary transformer used through a magnetic gap between cores, the influence of the magnetic permeability μ of the core in the signal transmission path does not appear linearly.
すなわち、第12図は、磁気ギヤツプGを約
50μmとし、ロータリトランスの使用条件を同一
にした場合におけるコアの透磁率μと結合係数K
との関係を示す説明図であり、横軸に透磁率μ
を、縦軸に結合係数Kをとつてある。 That is, FIG. 12 shows that the magnetic gap G is approximately
Core magnetic permeability μ and coupling coefficient K when the diameter is 50 μm and the usage conditions of the rotary transformer are the same.
This is an explanatory diagram showing the relationship between the magnetic permeability μ and the horizontal axis.
, and the coupling coefficient K is plotted on the vertical axis.
この第12図から明らかなように、結合係数K
は、透磁率μがある値A以下になると急激に劣化
し、透磁率μがA点からB点の所定範囲にある間
は比例的に変化し、さらに透磁率μがB点を越え
るとほぼ飽和状態になることがわかる。 As is clear from FIG. 12, the coupling coefficient K
deteriorates rapidly when the magnetic permeability μ becomes less than a certain value A, and changes proportionally while the magnetic permeability μ is within a predetermined range from point A to point B, and when the magnetic permeability μ exceeds point B, it deteriorates rapidly. It can be seen that it becomes saturated.
そこで、本発明者らは、原材料におけるバイン
ダの容積比の増大にともなう透磁率μの劣化と、
バインダの容積比の増大にともなう原材料の流動
性との関係を検討し、原材料におけるバインダの
容積比を15〜50%と特定した。 Therefore, the present inventors investigated the deterioration of the magnetic permeability μ due to the increase in the volume ratio of the binder in the raw material.
We investigated the relationship between increasing the volume ratio of binder and the fluidity of raw materials, and determined that the volume ratio of binder in raw materials was 15 to 50%.
以下、本発明の実施例を図面により説明する。 Embodiments of the present invention will be described below with reference to the drawings.
第1図は本発明によるロータリトランスの製造
方法を説明する工程図である。 FIG. 1 is a process diagram illustrating a method for manufacturing a rotary transformer according to the present invention.
この第1図に示すように、原材料の流動性を良
くするために、ソフトフエライト磁性粉末にバイ
ンダ(結合材)を混合し、これらを加熱混練して
スラリー状とする。この時のバインダの比率は、
ソフトフエライト磁性粉末の粒径によつて多少異
なるが、少なすぎると、原材料の流動性が低下し
て射出困難となり、しかも後工程の焼成時に亀裂
が入るため、15容積%以上と特定した。 As shown in FIG. 1, in order to improve the fluidity of the raw materials, a binder (binding material) is mixed with soft ferrite magnetic powder, and the mixture is heated and kneaded to form a slurry. The binder ratio at this time is
It varies somewhat depending on the particle size of the soft ferrite magnetic powder, but if it is too small, the fluidity of the raw material will decrease and injection will be difficult, and cracks will appear during the post-process firing, so we specified it as 15% by volume or more.
次に、この原材料を金型内に圧入して、コイル
溝やコイル引出溝を有するコア素体を射出成形す
る。この射出成形されたコア素体は多量のバイン
ダを含むため、これを3〜5℃/hrというゆつく
りした昇温速度で300〜500℃まで昇温し、バイン
ダを脱脂する。 Next, this raw material is press-fitted into a mold to injection mold a core element having a coil groove and a coil extraction groove. Since this injection-molded core body contains a large amount of binder, it is heated to 300 to 500°C at a slow heating rate of 3 to 5°C/hr to degrease the binder.
第2図は、この時のバインダの配合比%と透磁
率μとの関係を示す説明図で、横軸に原材料中に
おけるバインダの容積比%を、縦軸に透磁率μを
とつてある。この第2図から、原材料中における
バインダの容積比が50%を越えると脱脂が不充分
となり、その後の焼成工程においてソフトフエラ
イト磁性粉末間に非磁性の空孔が多量に発生し、
それらの反磁界の影響により透磁率μが急激に劣
化することがわかるため、原材料中におけるバイ
ンダの容積比は50%以下と特定した。 FIG. 2 is an explanatory diagram showing the relationship between the blending ratio % of the binder and the magnetic permeability μ, in which the horizontal axis represents the volume ratio % of the binder in the raw material, and the vertical axis represents the magnetic permeability μ. From this figure 2, it can be seen that when the volume ratio of the binder in the raw material exceeds 50%, degreasing becomes insufficient, and a large number of non-magnetic pores are generated between the soft ferrite magnetic powders in the subsequent firing process.
Since it was found that the magnetic permeability μ deteriorated rapidly due to the influence of these demagnetizing fields, the volume ratio of the binder in the raw material was specified to be 50% or less.
次に、脱脂後のコア素体を1000〜1400℃の高温
で数時間(ピーク温度で2〜6時間)焼成し、コ
イル溝やコイル引出溝を有するコア(製品)を得
る。このようにして得られたステータ側およびロ
ータ側コアは、流動性の良いスラリー状の原材料
を金型に射出するため、金型内における原材料の
充填度は均一となり、その後の工程時に変形やソ
リは発生しない。従つて、従来の圧縮成形法では
必要不可欠であつた焼成後の表面研摩加工を省略
することができ、しかも、コイル溝やコイル引出
溝の寸法も精度良く出すことができるため、コイ
ルの取付作業も非常に簡単になる。 Next, the core body after degreasing is fired at a high temperature of 1000 to 1400° C. for several hours (2 to 6 hours at peak temperature) to obtain a core (product) having coil grooves and coil extraction grooves. The stator side and rotor side cores obtained in this way are made by injecting slurry raw material with good fluidity into the mold, so the degree of filling of the raw material in the mold is uniform, and there is no deformation or warping during the subsequent process. does not occur. Therefore, it is possible to omit the surface polishing process after firing, which was indispensable in the conventional compression molding method, and the dimensions of the coil groove and coil pull-out groove can be precisely determined, making the coil installation work easier. will also be very easy.
第3図は上述した製造方法によつて製造された
コアの一実施例を示す平面図、第4図は第3図の
A−A′断面図であつて、5はコイル溝3と反対
側のコア1表面に設けられた凹部、6は該凹部5
内に形成されたゲート部であり、先に説明した第
8図に対する部分には同一符号を付けてある。 FIG. 3 is a plan view showing an embodiment of the core manufactured by the above-described manufacturing method, and FIG. 4 is a sectional view taken along line A-A' in FIG. A recess 6 is provided on the surface of the core 1.
This is a gate portion formed inside, and portions corresponding to those in FIG. 8 described above are given the same reference numerals.
すなわち、本発明によるロータリトランスの製
造方法によれば、射出成形法によつてコアを製造
するため、コア1に必ずゲート部6が突出した状
態で残る。そこで、このゲート部6の後処理を不
要とするために、本実施例においては、コイル溝
1aと反対側のコア1表面に凹部5を設けるとと
もに、ゲート部6がこの凹部5内に位置するよう
にし、ロータリトランスの使用形態にゲート部6
が支障をきたさないように工夫してある。 That is, according to the rotary transformer manufacturing method according to the present invention, since the core is manufactured by injection molding, the gate portion 6 always remains in the core 1 in a protruding state. Therefore, in order to eliminate the need for post-processing of the gate portion 6, in this embodiment, a recess 5 is provided on the surface of the core 1 opposite to the coil groove 1a, and the gate portion 6 is located within the recess 5. In this way, the gate part 6 is
It has been devised so that it does not cause any problems.
なお、上述した第3図および第4図に示したコ
ア1はステータ側コアについての説明であるが、
かかるコア構造がロータ側のコア2にも適用可能
なことは勿論である。また、ゲート部6を上記実
施例で示した以外の位置、例えば、コア1の最大
外径よりも凹んだ部分の外周面(第3図において
矢印Bで示す部分)に形成しても良い。この場合
も、ゲート部6がコア1の最大外周面よりも突出
しなければ、ゲート部6を研削するなでの後処理
が不要となるため、ロータリトランスの使用に際
し実質的な支障はない。 Note that the core 1 shown in FIGS. 3 and 4 above is an explanation of the stator side core,
Of course, such a core structure can also be applied to the core 2 on the rotor side. Further, the gate portion 6 may be formed at a position other than that shown in the above embodiment, for example, on the outer circumferential surface of a portion recessed from the maximum outer diameter of the core 1 (the portion indicated by arrow B in FIG. 3). In this case as well, if the gate portion 6 does not protrude beyond the maximum outer circumferential surface of the core 1, there is no need for post-processing by grinding the gate portion 6, so there is no substantial problem in using the rotary transformer.
第5図は本発明によるロータリトランスの製造
方法によつて製造されたコア1,2の他の実施例
を示す断面図である。 FIG. 5 is a sectional view showing another embodiment of the cores 1 and 2 manufactured by the rotary transformer manufacturing method according to the present invention.
本実施例では、コイル溝1a,2aと反対側の
コア1,2の表面に複数本の凹溝7を同心円状に
設け、該凹溝7によつてコア1,2の最外周を除
く部分の肉厚が均一になるようにし、焼成時のコ
ア1,2に変形やソリが一層発生しにくくしてあ
る。 In this embodiment, a plurality of concave grooves 7 are provided concentrically on the surface of the cores 1 and 2 on the opposite side to the coil grooves 1a and 2a, and the grooves 7 form a portion of the cores 1 and 2 excluding the outermost periphery. The thickness of the cores 1 and 2 is made uniform, thereby making it more difficult for the cores 1 and 2 to be deformed or warped during firing.
第6図は本発明によるロータリトランスの製造
方法によつて製造されたコア2のさらに他の実施
例を示す断面図、第7図は第6図のC−C′拡大断
面図であり、8はコイルに相当する導電ペースト
である。 FIG. 6 is a cross-sectional view showing still another embodiment of the core 2 manufactured by the rotary transformer manufacturing method according to the present invention, and FIG. 7 is an enlarged cross-sectional view taken along line C-C' in FIG. is a conductive paste that corresponds to a coil.
これらの図において、導電ペースト8は、焼成
前の各コイル溝2aおよび共通のコイル引出溝2
b内にそれぞれ印刷された後、焼成と同一条件で
同時焼付けされており、従つて、焼成後のコイル
溝2aおよびコイル引出溝2b内に所定形状のコ
イルを接着固定する従来例に比べて、生産性を一
層向上させることができる。かかる導電ペースト
8によるコイルの形成方法は、コイルの巻数が1
ターンですむロータ側のコア2に適しており、複
数ターン必要なステータ側のコア1の場合は、従
来例と同様に、焼成後のコイル溝1aおよびコイ
ル引出溝1bに所定形状のコイル3を接着固定す
る必要がある。また、かかる導電ペースト8によ
るコイルの形成方法は、焼成時の熱収縮が均一で
ある本発明によるロータ側コア2において著しい
効果を奏するものであつて、従来の圧縮成形法に
よるロータ側コア2に適用した場合は、焼成時の
熱収縮が不均一であるため亀裂が起り易く、不向
きである。 In these figures, the conductive paste 8 is applied to each coil groove 2a and the common coil extraction groove 2 before firing.
After being printed in each area b, they are simultaneously baked under the same conditions as firing. Therefore, compared to the conventional example in which a coil of a predetermined shape is adhesively fixed in the coil groove 2a and coil extraction groove 2b after firing, Productivity can be further improved. The method for forming a coil using the conductive paste 8 is such that the number of turns of the coil is 1.
It is suitable for the rotor side core 2 which requires only one turn, and in the case of the stator side core 1 which requires multiple turns, the coil 3 of a predetermined shape is inserted into the coil groove 1a and coil extraction groove 1b after firing, as in the conventional example. Needs to be fixed with adhesive. Furthermore, the method of forming a coil using the conductive paste 8 is extremely effective in the rotor-side core 2 according to the present invention, which has uniform heat shrinkage during firing, and is superior to the rotor-side core 2 formed by the conventional compression molding method. When applied, cracks are likely to occur due to uneven thermal contraction during firing, making it unsuitable.
なお、上述した各実施例は、本発明による製造
方法をいずれも偏平型のロータリトランスに適用
したものについて説明したが、本発明による製造
方法を第11図に示した円筒型(同軸型)のロー
タリトランスに適用できるのは勿論のことであ
る。この円筒型ロータリトランスの場合、偏平型
ロータリトランスに比べてコア形状が複雑である
ため、従来は圧縮成形後に機械加工によつてコイ
ル溝を形成し、さらに焼成後に表面研摩加工する
という複雑な工程を必要としていたが、本発明に
よれば、これらコイル溝の機械加工と焼成後の表
面研摩加工とを省略できるため、円筒型ロータリ
トランスにおいて一層顕著な効果を奏する。 In each of the above-mentioned embodiments, the manufacturing method according to the present invention was applied to a flat rotary transformer, but the manufacturing method according to the present invention was applied to a cylindrical (coaxial type) transformer as shown in FIG. Of course, it can be applied to rotary transformers. In the case of this cylindrical rotary transformer, the core shape is more complex than that of a flat rotary transformer, so conventionally the coil grooves were formed by machining after compression molding, and the surface was polished after firing. However, according to the present invention, the machining of these coil grooves and the surface polishing after firing can be omitted, so that a more remarkable effect is achieved in a cylindrical rotary transformer.
以上説明したように、本発明によれば、射出成
形法によつて金型内の原材料の充填度を均一にで
きるため、その後の焼成時にコアに変形やソリを
生じることがなく、それ故、従来不可欠であつた
焼成後のコアの表面研摩加工を省略でき、安価な
ロータリトランスを提供できる。
As explained above, according to the present invention, since the degree of filling of the raw material in the mold can be made uniform by the injection molding method, deformation or warpage does not occur in the core during subsequent firing, and therefore, The surface polishing process of the core after firing, which was conventionally indispensable, can be omitted, and an inexpensive rotary transformer can be provided.
第1図は本発明によるロータリトランスの製造
方法の一実施例を示す工程図、第2図は第1図に
示す脱脂工程時におけるバインダの配合比と透磁
率との関係を示す説明図、第3図は本発明に係る
製造方法によつて製造されたステータ側コアの平
面図、第4図は第3図のA−A′線断面図、第5
図は本発明に係る製造方法によつて製造されたコ
アの他の実施例を示す断面図、第6図は本発明に
係る製造方法によつて製造されたロータ側コアの
さらに他の実施例を示す平面図、第7図はそれの
C−C′線断面図、第8図は本発明が対象とする偏
平型ロータリトランスの断面図、第9図はそれの
ステータ側コアの平面図、第10図はそれのロー
タ側コアの平面図、第11図は本発明が対象とす
る円筒型ロータリトランスの断面図、第12図は
ロータリトランスにおけるコアの透磁率μと結合
係数Kとの関係を示す説明図である。
1,2……コア、1a,2a……コイル溝、1
b,2b……コイル引出溝、3,4……コイル、
5……凹部、6……ゲート部、7……凹溝、8…
…導電ペースト。
FIG. 1 is a process diagram showing an example of the method for manufacturing a rotary transformer according to the present invention, FIG. 3 is a plan view of a stator side core manufactured by the manufacturing method according to the present invention, FIG. 4 is a sectional view taken along line A-A' in FIG. 3, and FIG.
The figure is a sectional view showing another example of the core manufactured by the manufacturing method according to the present invention, and FIG. 6 is a further example of the rotor-side core manufactured by the manufacturing method according to the present invention. 7 is a sectional view taken along the line C-C', FIG. 8 is a sectional view of the flat rotary transformer to which the present invention is applied, and FIG. 9 is a plan view of the stator side core thereof. Fig. 10 is a plan view of the rotor side core, Fig. 11 is a sectional view of the cylindrical rotary transformer to which the present invention is applied, and Fig. 12 is the relationship between the magnetic permeability μ of the core and the coupling coefficient K in the rotary transformer. FIG. 1, 2...Core, 1a, 2a...Coil groove, 1
b, 2b... Coil extraction groove, 3, 4... Coil,
5... Concave portion, 6... Gate portion, 7... Concave groove, 8...
...Conductive paste.
Claims (1)
溝を有し、前記ステータ側コアに所定の磁気ギヤ
ツプを介して対向するロータ側コアとを備えたロ
ータリトランスの製造方法において、ソフトフエ
ライト磁性粉末に15〜50容積%のバインダを加熱
混練してスラリー状の原材料を得た後、この原材
料を金型内に射出してコイル溝を有するコア素体
を成形し、しかる後、このコア素体を300〜500℃
の温度で脱脂し、さらに、1000〜1400℃の温度で
焼成して前記コアを製造したことを特徴とするロ
ータリトランスの製造方法。1. A method for manufacturing a rotary transformer comprising a stator-side core having a coil groove and a rotor-side core having a coil groove and facing the stator-side core via a predetermined magnetic gap, in which soft ferrite magnetic powder is After heating and kneading ~50% by volume of binder to obtain a slurry-like raw material, this raw material is injected into a mold to form a core body with coil grooves. ~500℃
A method for manufacturing a rotary transformer, characterized in that the core is manufactured by degreasing at a temperature of 1000 to 1400°C and further firing at a temperature of 1000 to 1400°C.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP59204084A JPS6184006A (en) | 1984-10-01 | 1984-10-01 | Manufacturing method of rotary transformer |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP59204084A JPS6184006A (en) | 1984-10-01 | 1984-10-01 | Manufacturing method of rotary transformer |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS6184006A JPS6184006A (en) | 1986-04-28 |
| JPH023288B2 true JPH023288B2 (en) | 1990-01-23 |
Family
ID=16484516
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP59204084A Granted JPS6184006A (en) | 1984-10-01 | 1984-10-01 | Manufacturing method of rotary transformer |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS6184006A (en) |
Families Citing this family (8)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS6318609A (en) * | 1986-07-11 | 1988-01-26 | Sony Corp | Rotary transformer |
| JPS6319805A (en) * | 1986-07-12 | 1988-01-27 | Sony Corp | Rotary transformer |
| IT1208358B (en) * | 1987-03-31 | 1989-06-12 | Brussino Massimo | PROCEDURE FOR THE PRODUCTION OF MAGNETIC PLASTIC LAMINATE AND MAGNETIC LAMINATE OBTAINED WITH THIS PROCEDURE |
| JPH0257277U (en) * | 1988-10-19 | 1990-04-25 | ||
| US5126906A (en) * | 1989-04-17 | 1992-06-30 | Hitachi, Ltd. | Rotary magnetic head device with rotary transformer having high coupling coefficient |
| US7106163B2 (en) | 1998-03-27 | 2006-09-12 | The Furukawa Electric Co., Ltd. | Core |
| DE20116068U1 (en) * | 2001-09-29 | 2003-02-13 | ebm Werke GmbH & Co. KG, 74673 Mulfingen | External rotor motor |
| DE102021213294A1 (en) | 2021-11-25 | 2023-05-25 | Mahle International Gmbh | Rotary transformer for a separately excited synchronous machine |
-
1984
- 1984-10-01 JP JP59204084A patent/JPS6184006A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS6184006A (en) | 1986-04-28 |
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