JP2005150066A - Efficient heater coil for induction heating - Google Patents

Efficient heater coil for induction heating Download PDF

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JP2005150066A
JP2005150066A JP2003420151A JP2003420151A JP2005150066A JP 2005150066 A JP2005150066 A JP 2005150066A JP 2003420151 A JP2003420151 A JP 2003420151A JP 2003420151 A JP2003420151 A JP 2003420151A JP 2005150066 A JP2005150066 A JP 2005150066A
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Prior art keywords
coil
induction heating
heating
thickness
hollow conductor
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JP2003420151A
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Japanese (ja)
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Isamu Hosono
勇 細野
Takashi Kitamura
隆 北村
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HAGOROMO DENKI KK
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HAGOROMO DENKI KK
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Abstract

<P>PROBLEM TO BE SOLVED: To reduce loss of a heating coil in order to reduce power consumption of an induction heating device. <P>SOLUTION: The wall thickness of a part corresponding to the inner periphery of the coil of a hollow conductor for the heating coil of the induction heating device is made to be about two times or more of the permeation depth of electric current. <P>COPYRIGHT: (C)2005,JPO&NCIPI

Description

発明の詳細な説明Detailed Description of the Invention

産業上の利用分野Industrial application fields

本発明は、例えば熱間鍛造の用いる金属を加熱する為の誘導加熱装置において、加熱装置の消費電力を低減する目的で、その加熱効率を向上する為に用いられるものである。  The present invention is used, for example, in an induction heating apparatus for heating a metal used for hot forging, in order to reduce the power consumption of the heating apparatus, and to improve the heating efficiency.

通常、コイルに高周波電流を通電すると、表皮 効果によって電流はコイルの内周部分に集中して流れ、内周からの距離が離れるに従って電流は指数関数的に減少する。ここで導体の比抵抗をρ(μΩcm)、周波数をf(Hz)、コイルの最内周を流れる電流をi、導体内の内周からの距離をxとすると導体内の電流分布iは1式で表わされる。

Figure 2005150066
ここで1式のδを電流浸透深さと言い2式で求められる。
Figure 2005150066
コイル内に流れる全電流Iは1式を積分する事によって求められ、3式に示す如くになる。
Figure 2005150066
この式からコイル内に流れる電流は巾δの導体にiの電流が均等に流れると考えて良いと言う想定の基に、従来はコイル中空導体の肉厚tはt≒δに設定されている。但し周波数が4KHz程度になると、中空導体の強度の問題からt>δになる場合も有るが、これはあくまで強度上からの選定であり、効率を考慮したものではない。Normally, when a high-frequency current is applied to a coil, the current flows in a concentrated manner on the inner periphery of the coil due to the skin effect, and the current decreases exponentially as the distance from the inner periphery increases. Here, if the specific resistance of the conductor is ρ (μΩcm), the frequency is f (Hz), the current flowing through the innermost circumference of the coil is i 0 , and the distance from the inner circumference of the conductor is x, the current distribution i in the conductor is It is expressed by one set.
Figure 2005150066
Here, δ in equation (1) is called current penetration depth and is obtained by equation (2).
Figure 2005150066
The total current I flowing in the coil is obtained by integrating the equation (1), as shown in the equation (3).
Figure 2005150066
Based on the assumption that the current flowing in the coil can be considered to be equivalent to the current i 0 flowing in the conductor of width δ from this equation, the thickness t of the coil hollow conductor is conventionally set to t≈δ. Yes. However, when the frequency is about 4 KHz, there may be a case where t> δ due to the problem of the strength of the hollow conductor, but this is a selection from the viewpoint of strength only and does not take efficiency into consideration.

本発明が解決しようとする課題Problems to be solved by the present invention

従来の手法に従うと、周波数によってコイル抵抗は決まってしまい、それ以上のコイル損失の低減は望めない。本発明はこの点を打破し、コイル抵抗による損失をより低減しようとするものである。  According to the conventional method, the coil resistance is determined by the frequency, and further reduction of the coil loss cannot be expected. The present invention overcomes this point and intends to further reduce the loss due to coil resistance.

課題を解決する為の手段Means to solve the problem

本発明は、上記問題点を解決する為に為されたもので、中空導体の肉厚tを少なくともコイル内周に相当する部分に付いて大幅に厚くする事によってコイル抵抗による損失を低減せしめようとするものである。  The present invention has been made in order to solve the above-mentioned problems. By reducing the thickness t of the hollow conductor at least at the portion corresponding to the inner circumference of the coil, the loss due to the coil resistance will be reduced. It is what.

作用Action

1図に加熱用コイルの正面図及びコイル導体として用いられる中空導体の断面図を示す。従来の手法によれば、3式を基に電流が浸透深さδの巾に均等に流れるとして中空導体の肉厚tをδ近辺に選んでいる。しかしコイル各部の損失は電流の2乗に比例する為、その全損失Pは4式で表わされる事となる。

Figure 2005150066
FIG. 1 shows a front view of a heating coil and a cross-sectional view of a hollow conductor used as a coil conductor. According to the conventional method, the thickness t of the hollow conductor is selected in the vicinity of δ, assuming that the current flows uniformly in the width of the penetration depth δ based on the three formulas. However, since the loss of each part of the coil is proportional to the square of the current, the total loss Pc is expressed by the following equation (4).
Figure 2005150066

3式では中空導体の肉厚は無限大として計算していた。しかし中空導体の肉厚をtとし、導体各部に流れる電流をi’とすると3式は5式となり、この時のコイル最内周に流れる電流i’と3式のiとの間には6式の関係が成り立つ。

Figure 2005150066
ここで4式に6式を代入すると7式が得られる。
Figure 2005150066
In Equation 3, the thickness of the hollow conductor was calculated as infinite. However, if the thickness of the hollow conductor is t and the current flowing through each part of the conductor is i ′, the formula 3 becomes the formula 5, and the current i 0 ′ flowing in the innermost coil circumference at this time is between the current i 0 ′ and the formula i 0. Holds the relationship of the six formulas.
Figure 2005150066
Here, when formula 6 is substituted into formula 4, formula 7 is obtained.
Figure 2005150066

従来手法によるコイル損失Pc0の計算値は8式のとうりとなり

Figure 2005150066
7式と8式を比較すると9式が得られる。
Figure 2005150066
9式を図示すると2図に示す如くになる。図において横軸は
(中空導体の肉厚t/電流浸透深さδ)を表わし、縦軸は(本発明による計算で求めたコイル導体損失P/従来計算で求めたコイル導体損失Pc0)である。
図示のように中空導体の肉厚tをδの2倍以上に選べばコイルの抵抗損失はt≒δに選んだ場合に比べて60%程度に低減し得る事がわかる。The calculated value of coil loss P c0 by the conventional method is as follows:
Figure 2005150066
Comparing formula 7 and formula 8, formula 9 is obtained.
Figure 2005150066
The formula 9 is illustrated as shown in FIG. In the figure, the horizontal axis represents (thickness t of hollow conductor / current penetration depth δ), and the vertical axis (coil conductor loss P c obtained by calculation according to the present invention / coil conductor loss P c0 obtained by conventional calculation). It is.
As shown in the figure, it can be seen that if the thickness t of the hollow conductor is selected to be twice or more than δ, the resistance loss of the coil can be reduced to about 60% compared to the case where t≈δ is selected.

この場合、コイル導体の肉厚が大きくなる事によって、冷却水路が狭くなり冷却水が不足する場合には、3図に示す如く異型銅管を用いコイル内周に相当する部分のみの肉厚を大きく選べば良い。  In this case, when the thickness of the coil conductor is increased and the cooling water passage becomes narrow and the cooling water is insufficient, the thickness of only the portion corresponding to the inner circumference of the coil is formed using a modified copper pipe as shown in FIG. Choose bigger.

発明の効果The invention's effect

本発明の効果は下記のとうりである。  The effects of the present invention are as follows.

誘導加熱装置のコイル抵抗損失を大幅に低減して、消費電力の低減を図る事が出来る。  The coil resistance loss of the induction heating device can be greatly reduced, and the power consumption can be reduced.

異型銅管を用いる事によって、コイル抵抗損失を低減しつつ、冷却水量を確保する事が出来る。  By using an atypical copper tube, the amount of cooling water can be secured while reducing coil resistance loss.

誘導加熱装置の加熱コイルの正面図及びコイル用中空導体の断面図である。  It is the front view of the heating coil of an induction heating apparatus, and sectional drawing of the hollow conductor for coils. 中空導体の肉厚とコイルの抵抗損失の関係を示すグラフである。  It is a graph which shows the relationship between the thickness of a hollow conductor, and the resistance loss of a coil. 請求項2に使用される異型銅管の断面図である。  It is sectional drawing of the atypical copper pipe used for Claim 2.

符号の説明Explanation of symbols

1 誘導加熱用コイル
2 誘導加熱用コイルに用いられる中空導体の断面
t 中空導体の肉厚
t’ 異型銅管のコイル内周部に相当する部分の肉厚
DESCRIPTION OF SYMBOLS 1 Coil for induction heating 2 Cross section t of hollow conductor used for induction heating coil Thickness of hollow conductor t 'Thickness of a portion corresponding to the inner peripheral portion of a copper wire

Claims (2)

金属を加熱する場合に用いる誘導加熱装置の加熱コイルに於いて、少なくとも該コイル用中空導体のコイル内周に相当する部分の肉厚を、電流浸透深さの2倍程度以上に選ぶ事を特徴とする誘導加熱用加熱コイル。In the heating coil of the induction heating device used for heating metal, the thickness of at least the portion corresponding to the inner circumference of the coil hollow conductor is selected to be at least twice the current penetration depth. A heating coil for induction heating. 金属を加熱する場合に用いる誘導加熱装置の加熱コイルに於いて、少なくとも該加熱コイル用中空導体のコイル内周に相当する部分の肉厚を大きくし、且つ十分な冷却水量を得る為一辺のみ肉厚の厚い角型異型中空導体を用い、厚い部分の肉厚を電流浸透深さの2倍以上に選ぶ事をと特徴とする誘導加熱用加熱コイル。In the heating coil of the induction heating device used for heating the metal, at least the thickness corresponding to the inner circumference of the hollow conductor for the heating coil is increased and only one side is thick in order to obtain a sufficient amount of cooling water. A heating coil for induction heating, characterized by using a thick rectangular irregular hollow conductor and selecting the thickness of the thick part to be at least twice the current penetration depth.
JP2003420151A 2003-11-13 2003-11-13 Efficient heater coil for induction heating Pending JP2005150066A (en)

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Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP5492337B1 (en) * 2013-09-05 2014-05-14 北芝電機株式会社 High frequency induction melting furnace

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP5492337B1 (en) * 2013-09-05 2014-05-14 北芝電機株式会社 High frequency induction melting furnace
WO2015002327A1 (en) * 2013-09-05 2015-01-08 北芝電機株式会社 High-frequency induction melting furnace
JP2015053110A (en) * 2013-09-05 2015-03-19 北芝電機株式会社 High-frequency induction melting furnace

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