JP2002299021A - Heating coil for induction heating device - Google Patents

Heating coil for induction heating device

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Publication number
JP2002299021A
JP2002299021A JP2001104098A JP2001104098A JP2002299021A JP 2002299021 A JP2002299021 A JP 2002299021A JP 2001104098 A JP2001104098 A JP 2001104098A JP 2001104098 A JP2001104098 A JP 2001104098A JP 2002299021 A JP2002299021 A JP 2002299021A
Authority
JP
Japan
Prior art keywords
coil
heating coil
induction heating
magnetic
heating device
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.)
Pending
Application number
JP2001104098A
Other languages
Japanese (ja)
Inventor
Atsushi Fujita
篤志 藤田
Motonari Hirota
泉生 弘田
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Panasonic Holdings Corp
Original Assignee
Matsushita Electric Industrial Co Ltd
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Application filed by Matsushita Electric Industrial Co Ltd filed Critical Matsushita Electric Industrial Co Ltd
Priority to JP2001104098A priority Critical patent/JP2002299021A/en
Publication of JP2002299021A publication Critical patent/JP2002299021A/en
Pending legal-status Critical Current

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  • Induction Heating Cooking Devices (AREA)

Abstract

PROBLEM TO BE SOLVED: To provide a small and low-cost induction heating device by realizing a simple-structured inexpensive heating coil, without increasing the loss. SOLUTION: In the heating coil for the induction heating device, an electrical conductor 13 is wound around spirally separated by intervals, and a magnetic material 14 is inserted into approx, one turn part of the intervals, so that the magnetic materials are distributed continuously or separately, and the magnetic material is not inserted into at least one interval adjacent to the magnetic material.

Description

【発明の詳細な説明】DETAILED DESCRIPTION OF THE INVENTION

【0001】[0001]

【発明の属する技術分野】本発明は一般家庭及びレスト
ラン、あるいは工場などで使用される誘導加熱装置に関
するもので、さらに詳しくはその加熱コイルに関するも
のである。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to an induction heating device used in ordinary households, restaurants, factories, and the like, and more particularly to a heating coil thereof.

【0002】[0002]

【従来の技術】従来の誘導加熱装置の加熱構造を誘導加
熱調理器を例に取り上げ、説明する。
2. Description of the Related Art The heating structure of a conventional induction heating apparatus will be described by taking an induction heating cooker as an example.

【0003】図7は従来の誘導加熱調理器の断面図で、
1は高周波磁界を発生する加熱コイルを、2は加熱コイ
ル1から発生する高周波磁界によって誘導加熱される被
加熱物を、3は加熱コイル1に高周波電流を供給するイ
ンバータ回路で図には特に記載していないが、加熱コイ
ル1と接続されている。4は被加熱物2がその上面に載
置されるトッププレートでその材質はセラミックであ
る。5は筐体、6は加熱コイル1を載置するコイル台で
ある。
FIG. 7 is a sectional view of a conventional induction heating cooker.
1 is a heating coil for generating a high-frequency magnetic field, 2 is an object to be heated which is induction-heated by a high-frequency magnetic field generated from the heating coil 1, and 3 is an inverter circuit for supplying a high-frequency current to the heating coil 1. Not connected, but connected to heating coil 1. Reference numeral 4 denotes a top plate on which the object to be heated 2 is placed on its upper surface, the material being ceramic. Reference numeral 5 denotes a housing, and 6 denotes a coil table on which the heating coil 1 is placed.

【0004】加熱コイル1のコイル線は、直径0.3m
m〜0.5mm程度の素線を30本程度撚り合わせたも
ので構成(リッツワイヤ構成)されている。この撚りピ
ッチは数cm程度で、それぞれの素線は1ターン中に数
回被加熱物2の下面に対して上下の位置関係を繰り返す
構成となっている。
[0004] The coil wire of the heating coil 1 has a diameter of 0.3 m.
It is configured by twisting about 30 strands of about m to 0.5 mm (Litz wire configuration). The twist pitch is about several centimeters, and each element wire is configured to repeat the vertical positional relationship with the lower surface of the object 2 several times during one turn.

【0005】一方、リッツワイヤを用いない簡易な構成
で加熱コイル1を実現する構成として平板コイルを層状
に構成する方式が公開実用新案公報S62-106497などに提
案されている。この方式では、加熱コイル1を例えばプ
レス方式により作成することが可能となり、コスト的に
非常に廉価なものができる可能性がある。また、コイル
を絶縁層と交互に積層させる構造とすることで、コイル
1枚の厚さを薄くすることが可能となり、表皮抵抗の上
昇を抑える構造とすることができる。
On the other hand, as a configuration for realizing the heating coil 1 with a simple configuration that does not use a litz wire, a system in which a flat coil is configured in a layered manner has been proposed in, for example, Japanese Utility Model Publication S62-106497. In this method, the heating coil 1 can be formed by, for example, a press method, and there is a possibility that a very inexpensive one can be obtained. Further, by adopting a structure in which the coil is alternately laminated with the insulating layer, the thickness of one coil can be reduced, and a structure in which an increase in skin resistance can be suppressed.

【0006】[0006]

【発明が解決しようとする課題】しかしながら、リッツ
ワイヤ構成による加熱コイルや、ターン数を多くした平
板コイル等では、近接するコイル電流からの磁界の影響
を受けやすい。図8は、近接するコイル周辺の電磁環境
模式図で、7はコイル線、8は前記コイル線より生じる
磁束を示している。図8中、コイル線7には紙面手前か
ら向こう側に電流が流れるものとしている。コイル線7
の電流は、近接する互いのコイル線から生じる磁束8に
より、近接するコイル線より遠ざかる方向へ分布が偏
る。図8中、コイル線7の色の濃淡は、電流密度を表し
ており、濃い部分では電流密度が高いことを示してい
る。この電流分布の偏りを生じさせる一連の現象を一般
に近接効果と呼ぶ。この近接効果により、加熱コイル抵
抗が大きくなり、加熱コイル損失が増加する。コイル線
7間の距離が近いほど、近接効果の影響が大きくなるた
め、リッツワイヤ構成による加熱コイルや、ターン数を
多くした平板コイル等では、加熱コイル損失が増加し、
冷却、効率の面で不利である。
However, a heating coil having a litz wire configuration or a flat coil having a large number of turns is easily affected by a magnetic field from an adjacent coil current. FIG. 8 is a schematic diagram of an electromagnetic environment around a neighboring coil, where 7 is a coil wire, and 8 is a magnetic flux generated from the coil wire. In FIG. 8, it is assumed that a current flows through the coil wire 7 from the near side of the drawing to the other side. Coil wire 7
Is distributed in a direction away from the adjacent coil wires due to the magnetic flux 8 generated from the adjacent coil wires. In FIG. 8, the shade of the color of the coil wire 7 indicates the current density, and a dark portion indicates that the current density is high. A series of phenomena causing the bias of the current distribution is generally called a proximity effect. Due to this proximity effect, the heating coil resistance increases and the heating coil loss increases. Since the effect of the proximity effect increases as the distance between the coil wires 7 decreases, the heating coil loss increases in a heating coil having a litz wire configuration or a flat coil having a large number of turns.
It is disadvantageous in terms of cooling and efficiency.

【0007】また、発明者らは、近接効果の低減を目的
として、コイル間全てに磁性体を挿入した構成を検討し
た。これは磁界がコイル間に挿入した磁性体に集中し、
コイルを通過する磁界が低減され、結果近接効果の影響
が小さくなることを狙いとしている。しかしながら実験
より、部分的には近接効果低減の効果が得られないとい
う結果が得られた。コイル周辺の電磁環境を考慮する
と、図9に示すように、加熱コイル周辺の磁束分布は長
辺が加熱コイルに平行で扁平な同心楕円状であり、磁界
の向きがコイル面に略平行となる部分がある。そのた
め、ある磁性体を通過しようとする磁界が、隣接する磁
性体に引き寄せられやすくなり、コイルを通過するもの
と考えられる。その結果、近接効果が顕著となる部分が
存在する。
Further, the present inventors have studied a configuration in which a magnetic body is inserted between all the coils for the purpose of reducing the proximity effect. This is because the magnetic field concentrates on the magnetic material inserted between the coils,
The aim is to reduce the magnetic field passing through the coil, thereby reducing the effect of the proximity effect. However, the experiment showed that the effect of reducing the proximity effect was not obtained partially. Considering the electromagnetic environment around the coil, as shown in FIG. 9, the magnetic flux distribution around the heating coil is a flat concentric ellipse whose long side is parallel to the heating coil, and the direction of the magnetic field is substantially parallel to the coil surface. There are parts. Therefore, it is considered that a magnetic field that is going to pass through a certain magnetic body is easily attracted to an adjacent magnetic body and passes through a coil. As a result, there is a portion where the proximity effect becomes significant.

【0008】本発明は上記従来の課題を解決するもの
で、簡素かつ容易な工法でかつ従来加熱コイルの同様以
下の損失となる加熱コイルを実現し、冷却性能等に余裕
を持たせ、結果安価な誘導加熱装置を提供することを目
的とするものである。
The present invention solves the above-mentioned conventional problems, and realizes a heating coil having a loss similar to or less than that of a conventional heating coil by a simple and easy method, allowing a margin in cooling performance and the like, and as a result, it is inexpensive. It is an object of the present invention to provide a simple induction heating device.

【0009】[0009]

【課題を解決するための手段】上記課題を解決するため
に、本発明の誘導加熱装置用加熱コイルは電気導体を間
隔を設けて渦巻き状に巻回し、前記間隔の略1ターン分
に連続的あるいは離散的に分布するように磁性体を挿入
し、前記磁性体に径方向に隣り合う少なくとも一つの間
隔には、他の磁性体を挿入しないように、磁性体を径方
向に複数分布させたものである。これにより、磁界の向
きがコイル面に対して略平行となる部分で、ある磁性体
を通過しようとする磁界が、隣接する磁性体に引き寄せ
られないようにして近接効果を抑え、低損失化した誘導
加熱装置用加熱コイルとすることができる。
In order to solve the above-mentioned problems, a heating coil for an induction heating device according to the present invention is formed by winding an electric conductor spirally at intervals, and continuously winding the electric conductor for approximately one turn of the interval. Alternatively, a magnetic body is inserted so as to be discretely distributed, and a plurality of magnetic bodies are radially distributed so as not to insert another magnetic body in at least one interval radially adjacent to the magnetic body. Things. Thereby, in a portion where the direction of the magnetic field is substantially parallel to the coil surface, the magnetic field that is going to pass through a certain magnetic body is not attracted to the adjacent magnetic body, so that the proximity effect is suppressed and the loss is reduced. It can be a heating coil for an induction heating device.

【0010】[0010]

【発明の実施の形態】請求項1に記載の発明は、電気導
体を間隔を設けて渦巻き状に巻回し、前記間隔の略1タ
ーン分に連続的あるいは離散的に分布するように磁性体
を挿入し、前記磁性体に径方向に隣り合う少なくとも一
つの間隔には、他の磁性体を挿入しないように、磁性体
を径方向に複数分布させたことにより、磁界の向きがコ
イル面に対して略平行となる部分での近接効果を抑え、
低損失化し誘導加熱装置用加熱コイルを提供することが
可能となる。
According to the first aspect of the present invention, an electric conductor is spirally wound at intervals and a magnetic material is distributed so as to be distributed continuously or discretely for approximately one turn of the interval. Inserted, in at least one interval radially adjacent to the magnetic body, a plurality of magnetic bodies are distributed in the radial direction so as not to insert another magnetic body, so that the direction of the magnetic field with respect to the coil surface And suppress the proximity effect in the part that is almost parallel,
It is possible to provide a heating coil for an induction heating device with reduced loss.

【0011】請求項2に記載の発明は、請求項1に記載
の構成で、特に、少なくとも中周部の電気導体間に磁性
体を挿入することにより、磁界の向きがコイル面に対し
て略平行となりやすい中周部での近接効果を抑え、効果
的に誘導加熱装置用加熱コイルを低損失化することが可
能となる。
According to a second aspect of the present invention, in the configuration according to the first aspect, in particular, by inserting a magnetic body between at least middle electric conductors, the direction of the magnetic field is substantially equal to the coil surface. It is possible to suppress the proximity effect in the middle portion, which is likely to be parallel, and effectively reduce the loss of the heating coil for the induction heating device.

【0012】請求項3に記載の発明は、請求項1または
2に記載の電気導体の断面コーナー部は曲線状あるいは
直線上にカットされた形状とすることにより、磁界が通
過し、電流が集中しやすい電気導体断面角部をなくすこ
とで近接効果を抑え、誘導加熱装置用加熱コイルを低損
失化することが可能である。
According to a third aspect of the present invention, the electric conductor according to the first or second aspect is formed such that a cross-sectional corner of the electric conductor is formed into a curved shape or a straight line so that a magnetic field passes therethrough and a current is concentrated. Eliminating the corner portions of the electric conductor that is easy to perform suppresses the proximity effect and makes it possible to reduce the loss of the heating coil for the induction heating device.

【0013】[0013]

【実施例】(実施例1)以下、本発明の第1の実施例に
ついて図面を参照しながら説明する。図1は加熱コイル
断面を示している。13は電気導体、14は磁性体で構
成される。前記磁性体14は、前記電気導体13間の1
つおきに挿入されている。また、本実施の形態では、前
記磁性体14が挿入されていない前記電気導体13間に
挿入される非磁性体は、空気で構成されている例を挙げ
ている。
(Embodiment 1) Hereinafter, a first embodiment of the present invention will be described with reference to the drawings. FIG. 1 shows a cross section of the heating coil. 13 is an electric conductor, and 14 is a magnetic material. The magnetic body 14 is provided between the electric conductors 13.
Every other is inserted. Further, in the present embodiment, an example is described in which the nonmagnetic material inserted between the electric conductors 13 into which the magnetic material 14 is not inserted is made of air.

【0014】上記の構成において、誘導加熱を行う際、
前記電気導体13に流れる高周波電流により、高周波磁
界が発生する。このとき図2に示すように、加熱コイル
周辺の磁束分布は長辺が加熱コイルに平行で扁平な同心
楕円状となっており、磁界の向きがコイル面に対して略
平行となる部分が大きい。そのため、隣接する前記磁性
体14間距離が近ければ、磁界が前記磁性体14に引き
寄せられ、前記電気導体13を通過する磁界が増加し、
近接効果により損失が増加する。しかしながら本実施の
形態では、隣接する前記磁性体14間距離を大きくする
ことにより、近接効果を抑え、前記電気導体13を通過
する磁界が効果的に前記磁性体14に集中し、前記電気
導体13には磁界が通過しない構成としている。従っ
て、加熱コイルを低損失化することが可能となる。
In the above configuration, when performing induction heating,
A high-frequency magnetic field is generated by the high-frequency current flowing through the electric conductor 13. At this time, as shown in FIG. 2, the magnetic flux distribution around the heating coil has a long side parallel to the heating coil and has a flat concentric elliptical shape, and a portion where the direction of the magnetic field is substantially parallel to the coil surface is large. . Therefore, if the distance between the adjacent magnetic bodies 14 is short, the magnetic field is attracted to the magnetic bodies 14 and the magnetic field passing through the electric conductor 13 increases,
Proximity effects increase losses. However, in the present embodiment, the proximity effect is suppressed by increasing the distance between the adjacent magnetic members 14, the magnetic field passing through the electric conductor 13 is effectively concentrated on the magnetic member 14, and the electric conductor 13 Has a configuration in which a magnetic field does not pass through. Therefore, it is possible to reduce the loss of the heating coil.

【0015】なお、本実施例では、前記磁性体14を前
記電気導体13間の1つおきに挿入した一例を挙げた
が、磁性体14を挿入しない間隔を間に2つ以上設けて
もよい。
In this embodiment, an example is described in which the magnetic members 14 are inserted at every other position between the electric conductors 13. However, two or more intervals where the magnetic members 14 are not inserted may be provided. .

【0016】また、磁性体14は1ターン分全てに挿入
しても良いが、部分的にあるいは間隔を設けて離散的に
配置してもよい。
The magnetic body 14 may be inserted into the entire turn for one turn, or may be arranged partially or discretely with an interval.

【0017】(実施例2)次に、本発明の第2の実施例
について図面を参照しながら説明する。図3は加熱コイ
ル断面を示している。18は電気導体、19は磁性体で
構成される。前記磁性体19は、前記電気導体18中周
部導体間の1つおきに挿入されている。なお、ここでの
中周部とは、内周部と外周部の中間部を指している。ま
た、本実施の形態では、前記磁性体19が挿入されてい
ない前記電気導体18間に挿入される非磁性体は、空気
で構成されている例を挙げている。
(Embodiment 2) Next, a second embodiment of the present invention will be described with reference to the drawings. FIG. 3 shows a cross section of the heating coil. Reference numeral 18 denotes an electric conductor, and 19 denotes a magnetic material. The magnetic body 19 is inserted every other one of the middle conductors of the electric conductor 18. Here, the middle part refers to an intermediate part between the inner part and the outer part. Further, in the present embodiment, an example is described in which the non-magnetic material inserted between the electric conductors 18 into which the magnetic material 19 is not inserted is made of air.

【0018】上記の構成において、特に磁界の向きがコ
イル面に対して略平行となりやすい中周部で、近接する
電気導体からの磁界の影響を効果的に低減し、近接効果
を抑え、加熱コイルを低損失化することが可能となる。
In the above configuration, particularly in the middle portion where the direction of the magnetic field tends to be substantially parallel to the coil surface, the effect of the magnetic field from the adjacent electric conductor is effectively reduced, the proximity effect is suppressed, and the heating coil is prevented. Can be reduced.

【0019】なお、本実施例では、前記磁性体19を前
記電気導体18間の1つおきに挿入した一例を挙げた
が、これに限るものではない。
In this embodiment, an example is described in which the magnetic body 19 is inserted between every other one of the electric conductors 18. However, the present invention is not limited to this.

【0020】また、発明者らの実験により、特に内周よ
り3ターン以上、外周より1ターン以内の部分で本実施
例で述べた構成とするのが効果的であると判明してい
る。
Further, it has been found from experiments by the inventors that it is effective to adopt the configuration described in the present embodiment particularly at a portion that is three turns or more from the inner circumference and one turn or less from the outer circumference.

【0021】(実施例3)次に、本発明の第3の実施例
について図面を参照しながら説明する。図4は加熱コイ
ル断面を示している。20は電気導体で構成される。前
記電気導体20角部は曲面状としている。
(Embodiment 3) Next, a third embodiment of the present invention will be described with reference to the drawings. FIG. 4 shows a cross section of the heating coil. Reference numeral 20 is composed of an electric conductor. The corners of the electric conductor 20 are curved.

【0022】上記の構成において、特に磁界が通過しや
すい前記電気導体20角部形状を曲面状とすることで、
通過する磁界を低減し、近接効果を抑えることで、電流
集中を少なくして加熱コイルを低損失化することが可能
となる。
[0022] In the above configuration, particularly, the shape of the corner of the electric conductor 20 through which the magnetic field easily passes is made to be a curved surface,
By reducing the passing magnetic field and suppressing the proximity effect, it becomes possible to reduce the concentration of current and reduce the loss of the heating coil.

【0023】(実施例4)次に本発明の第4の実施例に
ついて図面を参照しながら説明する。実施例3では単一
の電気導体で構成したが、本実施例では図5に示すよう
に、4個のそれぞれ絶縁された電気導体21を積層状に
形成し、一番上の層と下の層のみ角部を曲面状にしてい
る。この構成によっても、角部での電流集中を少なくし
て近接効果を抑制することができる。
(Embodiment 4) Next, a fourth embodiment of the present invention will be described with reference to the drawings. In the third embodiment, a single electric conductor is used. However, in this embodiment, as shown in FIG. 5, four insulated electric conductors 21 are formed in a laminated shape, and the uppermost layer and the lower layer are formed. Only the layer has curved corners. With this configuration also, the proximity effect can be suppressed by reducing the current concentration at the corners.

【0024】(実施例5)次に本発明の第4の実施例に
ついて図面を参照しながら説明する。実施例4では4個
のそれぞれ絶縁された電気導体21を積層状に形成し、
一番上の層と下の層のみ角部を曲面状にしたが、本実施
例では、図6に示すように、各層で断面形状で角部を曲
線状あるいは、直線的に角部をカットした形状にしてい
る。こも構成によっても、角部での電流集中を少なくし
て近接効果を抑制することができる。
Embodiment 5 Next, a fourth embodiment of the present invention will be described with reference to the drawings. In the fourth embodiment, four insulated electric conductors 21 are formed in a laminated shape,
Only the uppermost layer and the lower layer have curved corners. However, in this embodiment, as shown in FIG. 6, the corners are cut in a curved line or cut straight in each layer. Shape. Also with this configuration, the proximity effect can be suppressed by reducing the current concentration at the corners.

【0025】[0025]

【発明の効果】以上のように、請求項1〜3に記載の発
明によれば、磁界による近接効果を抑え、加熱コイルを
低損失化することが可能となる。
As described above, according to the first to third aspects of the present invention, it is possible to suppress the proximity effect due to the magnetic field and reduce the loss of the heating coil.

【図面の簡単な説明】[Brief description of the drawings]

【図1】本発明の実施例1における誘導加熱装置用加熱
コイルの概略構成を示す断面図
FIG. 1 is a cross-sectional view illustrating a schematic configuration of a heating coil for an induction heating device according to a first embodiment of the present invention.

【図2】同、磁束分布を示す図FIG. 2 is a diagram showing the same magnetic flux distribution.

【図3】本発明の実施例2における誘導加熱装置用加熱
コイルの概略構成を示す断面図
FIG. 3 is a cross-sectional view illustrating a schematic configuration of a heating coil for an induction heating device according to a second embodiment of the present invention.

【図4】本発明の実施例3における誘導加熱装置用加熱
コイルの概略構成を示す断面図の一例を示す図
FIG. 4 is a diagram illustrating an example of a cross-sectional view illustrating a schematic configuration of a heating coil for an induction heating device according to a third embodiment of the present invention.

【図5】本発明の実施例4における誘導加熱装置用加熱
コイルの概略構成を示す断面図の一例を示す図
FIG. 5 is a diagram illustrating an example of a cross-sectional view illustrating a schematic configuration of a heating coil for an induction heating device according to a fourth embodiment of the present invention.

【図6】本発明の実施例5における誘導加熱装置用加熱
コイルの概略構成を示す断面図の一例を示す図
FIG. 6 is a diagram illustrating an example of a cross-sectional view illustrating a schematic configuration of a heating coil for an induction heating device according to a fifth embodiment of the present invention.

【図7】従来の誘導加熱装置の概略構成を示す断面図FIG. 7 is a sectional view showing a schematic configuration of a conventional induction heating device.

【図8】近接するコイル周辺の電磁環境模式図FIG. 8 is a schematic diagram of an electromagnetic environment around a nearby coil;

【図9】従来の誘導加熱装置の磁束分布を示す図FIG. 9 is a diagram showing a magnetic flux distribution of a conventional induction heating device.

【符号の説明】[Explanation of symbols]

9 電気導体 10 磁性体 9 Electric conductor 10 Magnetic material

───────────────────────────────────────────────────── フロントページの続き Fターム(参考) 3K051 AA08 AD03 CD43  ──────────────────────────────────────────────────続 き The continuation of the front page F term (reference) 3K051 AA08 AD03 CD43

Claims (3)

【特許請求の範囲】[Claims] 【請求項1】 電気導体を間隔を設けて渦巻き状に巻回
し、前記間隔の略1ターン分に連続的あるいは離散的に
分布するように磁性体を挿入し、前記磁性体に径方向に
隣り合う少なくとも一つの間隔には、他の磁性体を挿入
しないように、磁性体を径方向に複数分布させた誘導加
熱装置用加熱コイル。
An electric conductor is spirally wound with an interval therebetween, and a magnetic material is inserted so as to be distributed continuously or discretely for approximately one turn of the interval, and is radially adjacent to the magnetic material. A heating coil for an induction heating device in which a plurality of magnetic materials are distributed in a radial direction so that another magnetic material is not inserted into at least one matching interval.
【請求項2】 少なくとも中周部の電気導体間に磁性体
を挿入する請求項1に記載の誘導加熱装置用加熱コイ
ル。
2. The heating coil for an induction heating device according to claim 1, wherein a magnetic material is inserted between at least the electric conductors in the middle part.
【請求項3】 電気導体の断面コーナー部は曲線状ある
いは直線上にカットされた形状とする請求項1または2
に記載の誘導加熱装置用加熱コイル。
3. The electric conductor according to claim 1, wherein a cross-sectional corner of the electric conductor has a curved shape or a shape cut in a straight line.
4. The heating coil for an induction heating device according to claim 1.
JP2001104098A 2001-04-03 2001-04-03 Heating coil for induction heating device Pending JP2002299021A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP2001104098A JP2002299021A (en) 2001-04-03 2001-04-03 Heating coil for induction heating device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP2001104098A JP2002299021A (en) 2001-04-03 2001-04-03 Heating coil for induction heating device

Publications (1)

Publication Number Publication Date
JP2002299021A true JP2002299021A (en) 2002-10-11

Family

ID=18957007

Family Applications (1)

Application Number Title Priority Date Filing Date
JP2001104098A Pending JP2002299021A (en) 2001-04-03 2001-04-03 Heating coil for induction heating device

Country Status (1)

Country Link
JP (1) JP2002299021A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
DE102020206747A1 (en) 2020-05-29 2021-12-02 Würth Elektronik eiSos Gmbh & Co. KG Coil arrangement for wireless electromagnetic energy transmission

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
DE102020206747A1 (en) 2020-05-29 2021-12-02 Würth Elektronik eiSos Gmbh & Co. KG Coil arrangement for wireless electromagnetic energy transmission

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