JP2009129550A - Clad cable, litz wire, collective wire, and coil - Google Patents
Clad cable, litz wire, collective wire, and coil Download PDFInfo
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Abstract
Description
本発明は、クラッド電線、リッツ線、集合線およびコイルに関し、さらに詳しくは、高周波回路、直流重畳高周波回路、低周波重畳高周波回路または周波数が変動する高周波回路において損失を低減することが出来るクラッド電線、リッツ線、集合線およびコイルに関する。 The present invention relates to a clad wire, a litz wire, a collective wire, and a coil. More specifically, the present invention relates to a clad wire that can reduce loss in a high-frequency circuit, a DC superposition high-frequency circuit, a low-frequency superposition high-frequency circuit, or a high-frequency circuit whose frequency varies. , Litz wire, assembly wire and coil.
従来、チョークコイル,トランス,インダクタンスには、複数の絶縁銅線を寄り合わせたリッツ線が一般に用いられている。
また、半田付け性改善のための錫めっき銅線や銅めっきアルミニウム線が知られている(例えば、特許文献1参照。)。
In addition, tin-plated copper wires and copper-plated aluminum wires for improving solderability are known (see, for example, Patent Document 1).
銅線、又は、複数の絶縁銅線を撚り合わせたリッツ線でも、高周波においては損失が増加する。
逆にアルミ線や銅めっきアルミ線では、同断面積の銅線より条件によっては高周波で損失が小さくなる場合があるが、直流や低周波では損失が大きくなる。
すなわち、従来の電線では、高周波回路、直流重畳高周波回路、低周波重畳高周波回路または周波数が変動する高周波回路において適さない場合がある問題点があった。
そこで、本発明の目的は、高周波回路、直流重畳高周波回路、低周波重畳高周波回路または周波数が変動する高周波回路において損失を低減することが出来るクラッド電線、リッツ線、集合線およびコイルを提供することにある。
Even with a litz wire obtained by twisting a copper wire or a plurality of insulated copper wires, loss increases at high frequencies.
On the contrary, in the case of an aluminum wire or a copper-plated aluminum wire, the loss may be reduced at a high frequency depending on conditions, but the loss is increased at a direct current or a low frequency.
That is, the conventional electric wire has a problem that it may not be suitable for a high-frequency circuit, a DC superimposed high-frequency circuit, a low-frequency superimposed high-frequency circuit, or a high-frequency circuit in which the frequency varies.
Accordingly, an object of the present invention is to provide a clad wire, a litz wire, a collecting wire, and a coil that can reduce loss in a high-frequency circuit, a DC superimposed high-frequency circuit, a low-frequency superimposed high-frequency circuit, or a high-frequency circuit in which the frequency varies. It is in.
第1の観点では、本発明は、電線断面積の5%以上、50%以下の断面積となる厚さのアルミニウム層を銅線の外周面に形成してなるクラッド電線を提供する。
上記第1の観点によるクラッド電線では、直径が0.3mm、アルミ面積率が5%(アルミ厚さ3.8μm)〜10%(7.7μm)の絶縁クラッド電線を使用した152ターンのコイルにおいて、略800kHz以上で、同条件の銅線コイルより損失が減少した。また、略400kHz〜1000kHzの周波数範囲で周波数を変動させた場合、平均した同一実効値電流では、同条件の銅線コイルより損失が低減した。
また、直径が1.1mm、アルミ面積率が5%(アルミ厚さ13.9μm)〜50%(161μm)の絶縁クラッド電線を使用した27ターン2層巻コイルにおいて、略50kHz〜100kHzの範囲で、同条件の銅線より損失が減少した。また、30kHz〜100kHzの周波数範囲で周波数を変動させた場合、平均した同一実効値電流では、同条件の銅線より損失が減少した。
なお、アルミ面積率が50%を越えると、全体損失特性がアルミ線に近づき、直流抵抗や低周波損失が増加するので、好ましくない。
In a first aspect, the present invention provides a clad electric wire obtained by forming an aluminum layer having a thickness of 5% or more and 50% or less of the cross-sectional area of the electric wire on the outer peripheral surface of the copper wire.
In the clad wire according to the first aspect, in a 152-turn coil using an insulated clad wire having a diameter of 0.3 mm and an aluminum area ratio of 5% (aluminum thickness 3.8 μm) to 10% (7.7 μm) At about 800 kHz or higher, the loss was reduced from the copper wire coil under the same conditions. Further, when the frequency was varied in the frequency range of about 400 kHz to 1000 kHz, the loss was reduced as compared with the copper wire coil under the same conditions at the same average effective current.
Further, in a 27-turn double-layer coil using an insulating clad wire having a diameter of 1.1 mm and an aluminum area ratio of 5% (aluminum thickness 13.9 μm) to 50% (161 μm), in a range of approximately 50 kHz to 100 kHz. Loss decreased compared to copper wire under the same conditions. In addition, when the frequency was varied in the frequency range of 30 kHz to 100 kHz, the loss decreased compared to the copper wire under the same conditions at the same average effective current.
If the aluminum area ratio exceeds 50%, the overall loss characteristic approaches that of an aluminum wire, and the DC resistance and low-frequency loss increase, which is not preferable.
第2の観点では、本発明は、前記第1の観点によるクラッド電線に絶縁被覆を施した絶縁電線を素線として含むリッツ線を提供する。
上記第2の観点によるリッツ線でも、上記第1の観点によるクラッド線を用いているため、同様の効果が得られる。
In a second aspect, the present invention provides a litz wire including an insulated wire obtained by applying an insulation coating to the clad wire according to the first aspect.
The Litz wire according to the second aspect can obtain the same effect because the clad wire according to the first aspect is used.
第3の観点では、本発明は、前記第1の観点によるクラッド電線に絶縁被覆を施した絶縁電線を複数束ねた集合線を提供する。
上記第3の観点による集合線でも、上記第1の観点によるクラッド線を用いているため、同様の効果が得られる。なお、リッツ線は複数の素線を撚って束ねた電線であり、集合線は複数の素線を撚らずに束ねた電線である。
In a third aspect, the present invention provides a collective line in which a plurality of insulated wires obtained by applying an insulation coating to the clad wire according to the first aspect are bundled.
Even in the collective line according to the third aspect, since the clad line according to the first aspect is used, the same effect can be obtained. The litz wire is an electric wire in which a plurality of strands are twisted and bundled, and the assembly wire is an electric wire in which a plurality of strands are bundled without being twisted.
第4の観点では、本発明は、前記第1の観点によるクラッド電線または前記第2の観点によるリッツ電線または前記第3の観点による集合線のいずれかを巻回してなるコイルを提供する。
上記第4の観点によるコイルでは、前記第1の観点によるクラッド電線または前記第2の観点によるリッツ電線または前記第3の観点による集合線を用いているため、同様の効果が得られる。
In a fourth aspect, the present invention provides a coil formed by winding either the clad electric wire according to the first aspect, the Litz electric wire according to the second aspect, or the assembly wire according to the third aspect.
Since the coil according to the fourth aspect uses the clad electric wire according to the first aspect, the Litz electric wire according to the second aspect, or the assembly wire according to the third aspect, the same effect can be obtained.
本発明のクラッド電線、リッツ線、集合線およびコイルによれば、高周波回路、直流重畳高周波回路、低周波重畳高周波回路または周波数が変動する高周波回路において損失を低減することが出来る。また、軽量化することも出来る。 According to the clad wire, litz wire, assembly wire, and coil of the present invention, loss can be reduced in a high-frequency circuit, a DC superimposed high-frequency circuit, a low-frequency superimposed high-frequency circuit, or a high-frequency circuit in which the frequency varies. Moreover, it can also be reduced in weight.
以下、図に示す実施の形態により本発明をさらに詳細に説明する。なお、これにより本発明が限定されるものではない。 Hereinafter, the present invention will be described in more detail with reference to embodiments shown in the drawings. Note that the present invention is not limited thereby.
図1は、実施例1に係るクラッド電線10を示す断面図である。
このクラッド電線10は、コアとなる銅線1と、その外周面に形成されたクラッドとなるアルミニウム層2とを具備してなる。
FIG. 1 is a cross-sectional view illustrating a
The
アルミニウム層2の厚さtは、クラッド電線10の断面積の5%以上、50%以下である。
The thickness t of the aluminum layer 2 is not less than 5% and not more than 50% of the cross-sectional area of the
図2は、実施例2に係る絶縁クラッド電線20を示す断面図である。
この絶縁クラッド電線20は、クラッド電線10の外周面にエナメル絶縁被覆3を形成したものである。
FIG. 2 is a cross-sectional view illustrating the insulated
The insulated
図3は、直径が1.1mm、アルミ面積率が5%〜50%の絶縁クラッド電線を2層27ターンに巻回したソレノイドコイルの特性図である。
この特性図の縦軸は、ソレノイドコイルの高周波抵抗Raを絶縁銅線を用いた同構造のコイルにおける高周波抵抗Rcに対する相対値Ra/Rcで示している。従って、縦軸の値が「1」より小さい周波数領域が、絶縁銅線を用いた同構造のコイルより損失が小さい領域である。
図3から判るように、50kHz〜100kHzで使用すれば、絶縁銅線を用いた同構造のコイルやアルミニウム線を用いた同構造のコイルより損失が小さくなることが判る。また、200kHzより低い周波数では、アルミニウム線を用いた同構造のコイルより損失が小さくなることが判る。
FIG. 3 is a characteristic diagram of a solenoid coil in which an insulating clad wire having a diameter of 1.1 mm and an aluminum area ratio of 5% to 50% is wound around two layers and 27 turns.
The vertical axis of this characteristic diagram indicates the high-frequency resistance Ra of the solenoid coil as a relative value Ra / Rc with respect to the high-frequency resistance Rc in the coil having the same structure using an insulated copper wire. Therefore, the frequency region where the value on the vertical axis is smaller than “1” is a region where the loss is smaller than that of the coil having the same structure using the insulated copper wire.
As can be seen from FIG. 3, the loss is smaller when used at 50 kHz to 100 kHz than the coil having the same structure using an insulated copper wire or the coil having the same structure using an aluminum wire. Further, it can be seen that at frequencies lower than 200 kHz, the loss is smaller than that of the coil having the same structure using an aluminum wire.
図4は、直径が0.14mm、アルミ面積率が10%〜50%の絶縁クラッド電線を素線とする素線数58本のリッツ線を1層21ターンに巻回したソレノイドコイルの特性図である。
図4から判るように、400kHz〜1000kHzで使用すれば、絶縁銅線を用いた同構造のコイルより損失が小さくなることが判る。また、500kHzより低い周波数では、アルミニウム線を用いた同構造のソレノイドコイルより損失が小さくなることが判る。
FIG. 4 is a characteristic diagram of a solenoid coil in which a litz wire having 58 strands wound around an insulated clad wire having a diameter of 0.14 mm and an aluminum area ratio of 10% to 50% is wound in 21 turns per layer. It is.
As can be seen from FIG. 4, when used at 400 kHz to 1000 kHz, it can be seen that the loss is smaller than that of the coil having the same structure using an insulated copper wire. Further, it can be seen that at frequencies lower than 500 kHz, the loss is smaller than that of the solenoid coil having the same structure using an aluminum wire.
図5は、直径が0.05mm、アルミ面積率が10%〜50%の絶縁クラッド電線を素線とする素線数1500本のリッツ線を2層40ターンに巻回した渦巻きコイルの特性図である。
図5から判るように、70kHz〜100kHzで使用すれば、絶縁銅線を用いた同構造のコイルより損失が小さくなることが判る。また、85kHzより低い周波数では、アルミニウム線を用いた同構造のコイルより損失が小さくなることが判る。
FIG. 5 is a characteristic diagram of a spiral coil in which 1500 layers of litz wire having a diameter of 0.05 mm and an aluminum area ratio of 10% to 50% are wound in two layers and 40 turns. It is.
As can be seen from FIG. 5, when used at 70 kHz to 100 kHz, the loss is smaller than that of the coil having the same structure using an insulated copper wire. It can also be seen that at a frequency lower than 85 kHz, the loss is smaller than that of the coil having the same structure using an aluminum wire.
図6は、直径が0.5mm、アルミ面積率が5%〜30%の絶縁クラッド電線を1層93ターンに巻回したソレノイドコイルの特性図である。
図6から判るように、アルミ面積率が5%のものは、100kHz〜2000kHzで使用すれば、絶縁銅線を用いた同構造のコイルより損失が小さくなることが判る。
FIG. 6 is a characteristic diagram of a solenoid coil in which an insulating clad wire having a diameter of 0.5 mm and an aluminum area ratio of 5% to 30% is wound around 93 turns per layer.
As can be seen from FIG. 6, when the aluminum area ratio is 5%, the loss is smaller than that of the coil having the same structure using the insulated copper wire when used at 100 kHz to 2000 kHz.
図7は、直径が0.3mm、アルミ面積率が5%〜30%の絶縁クラッド電線を1層125ターンに巻回したソレノイドコイルの特性図である。
図7から判るように、アルミ面積率が5%のものは、500kHz〜1000kHzで使用すれば、絶縁銅線を用いた同構造のコイルより損失が小さくなることが判る。
FIG. 7 is a characteristic diagram of a solenoid coil in which an insulating clad wire having a diameter of 0.3 mm and an aluminum area ratio of 5% to 30% is wound around 125 turns per layer.
As can be seen from FIG. 7, when the aluminum area ratio is 5%, the loss is smaller than that of the coil having the same structure using the insulated copper wire when used at 500 kHz to 1000 kHz.
図8は、実施例2の絶縁クラッド電線20を撚らずに束ねて被覆チューブ101で被覆した集合線100の斜視図である。
FIG. 8 is a perspective view of a
図9の(a)は、実施例2の絶縁クラッド電線20の外周に接着層4を形成した接着層付き絶縁クラッド電線30の斜視図である。
図9の(b)は、接着層付き絶縁クラッド電線30を撚らずに束ねて接着層4で一体化した集合線200の斜視図である。
FIG. 9A is a perspective view of an insulating
FIG. 9B is a perspective view of the
本発明のクラッド電線、リッツ線、集合線およびコイルは、高周波回路、直流重畳高周波回路、低周波重畳高周波回路または周波数が変動する高周波回路において好適に使用できる。具体例としては、チョークコイル,トランス,インダクター,TV用偏向ヨークなどの電磁誘導利用装置に利用できる。 The clad wire, litz wire, collective wire, and coil of the present invention can be suitably used in a high frequency circuit, a DC superimposed high frequency circuit, a low frequency superimposed high frequency circuit, or a high frequency circuit in which the frequency varies. As a specific example, the present invention can be used for electromagnetic induction utilizing devices such as choke coils, transformers, inductors, and TV deflection yokes.
1 銅線
2 アルミニウム層
3 絶縁被覆
4 被覆チューブ
10 クラッド電線
20 絶縁クラッド電線
30 接着層付き絶縁クラッド電線
100,200 集合線
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