Deprecated: The each() function is deprecated. This message will be suppressed on further calls in /home/zhenxiangba/zhenxiangba.com/public_html/phproxy-improved-master/index.php on line 456
JPH0459367B2 - - Google Patents
[go: Go Back, main page]

JPH0459367B2 - - Google Patents

Info

Publication number
JPH0459367B2
JPH0459367B2 JP59085753A JP8575384A JPH0459367B2 JP H0459367 B2 JPH0459367 B2 JP H0459367B2 JP 59085753 A JP59085753 A JP 59085753A JP 8575384 A JP8575384 A JP 8575384A JP H0459367 B2 JPH0459367 B2 JP H0459367B2
Authority
JP
Japan
Prior art keywords
heated
coil
induction heating
heating device
heated material
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
Application number
JP59085753A
Other languages
Japanese (ja)
Other versions
JPS60230934A (en
Inventor
Juji Ishizaka
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.)
Meidensha Electric Manufacturing Co Ltd
Original Assignee
Meidensha Electric Manufacturing 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 Meidensha Electric Manufacturing Co Ltd filed Critical Meidensha Electric Manufacturing Co Ltd
Priority to JP59085753A priority Critical patent/JPS60230934A/en
Publication of JPS60230934A publication Critical patent/JPS60230934A/en
Publication of JPH0459367B2 publication Critical patent/JPH0459367B2/ja
Granted legal-status Critical Current

Links

Classifications

    • CCHEMISTRY; METALLURGY
    • C21METALLURGY OF IRON
    • C21DMODIFYING THE PHYSICAL STRUCTURE OF FERROUS METALS; GENERAL DEVICES FOR HEAT TREATMENT OF FERROUS OR NON-FERROUS METALS OR ALLOYS; MAKING METAL MALLEABLE, e.g. BY DECARBURISATION OR TEMPERING
    • C21D1/00General methods or devices for heat treatment, e.g. annealing, hardening, quenching or tempering
    • C21D1/34Methods of heating
    • C21D1/42Induction heating
    • YGENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
    • Y02TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
    • Y02PCLIMATE CHANGE MITIGATION TECHNOLOGIES IN THE PRODUCTION OR PROCESSING OF GOODS
    • Y02P10/00Technologies related to metal processing
    • Y02P10/25Process efficiency

Landscapes

  • Chemical & Material Sciences (AREA)
  • Engineering & Computer Science (AREA)
  • Physics & Mathematics (AREA)
  • Thermal Sciences (AREA)
  • Crystallography & Structural Chemistry (AREA)
  • Mechanical Engineering (AREA)
  • Materials Engineering (AREA)
  • Metallurgy (AREA)
  • Organic Chemistry (AREA)
  • General Induction Heating (AREA)
  • Heat Treatment Of Articles (AREA)

Description

【発明の詳細な説明】[Detailed description of the invention]

(技術分野) 本発明は誘導加熱装置に係り、とくに断面の形
状が丸材、扁平材などで所定の長さを有する被加
熱材の端部を連続的に加熱する誘導加熱装置に関
する。 (従来技術) 所定の長さと断面を有する被加熱材、例えば丸
棒状金属材、扁平金属板等の端部を加熱する手段
として誘導加熱装置が使用されるが、従来の装置
は被加熱材を加熱するための搬送装置が複雑で、
コストアツプとなり、またコイル効果が悪いとい
う欠点があつた。 従来の誘導加熱装置を第1図〜第3図を参照し
て説明すると次のとおりである。各図において、
1は誘導加熱用のコイル、2は例えば金属丸棒の
ごとき所定長さの被加熱材である。図ので示す
矢印は被加熱材2が移動しながら送られている方
向を示している。 第1図の誘導加熱装置はいわゆるオープンタイ
プと呼ばれるもので、同図AおよびBに示すよう
にコイル1が被加熱材2を挾んで上下平行に配設
され、かつ被加熱材の軸線方向と直交するように
配設してある。このオープンタイプによると、図
から判るようにコイル1は被加熱材2が一方向に
連続移動するのを妨げないように配設してあるの
で、被加熱材2の搬送装置は、シンプルかつ安価
にできるが、コイル1内に位置する被加熱材2の
占積率が小さくなり、そのためコイル効果が悪い
という欠点がある。 第2図はいわゆるセミオープンタイプと呼ばれ
るもので、この場合も第1図のオープンタイプに
近い程度にコイル効果が悪いだけでなく、同図B
から判るようにコイル1の一部は被加熱材2の一
方向の移動を妨げるところに位置しているので、
図のように被加熱材2を横方向のみならず軸方向
にも移動させることが必要となり、このため搬送
装置が複雑かつコスト高となるという欠点があ
る。 上記搬送装置を簡単にし、かつコイル効率を高
くするには、第3図のような構成になるが、この
場合は、被加熱材2がライン上を横方向に流れる
途中において、ラインから外れた位置にある各誘
導加熱のコイル1を被加熱材2の端部の位置まで
出し入れする移動機構が余分に必要となり、全体
的にみて決して構成が簡単になるとは云えない。
このように、従来の誘導加熱装置のいずれにもそ
れぞれ一長一短があり、必ずしも満足できるもの
ではなかつた。 (発明の目的) 本発明は上記従来の欠点を改良したもので、被
加熱材の搬送機構は、従来のオープンタイプと同
様簡単な一方向の送り機構ですみ、しかもコイル
効率が従来に比べて著るしく高く、よつて設備コ
スト及びランニングコストが高周波に比べて安く
てすむ中周波を使用できる誘導加熱装置を提供す
ることを目的とする。 (発明の概要) 上記目的を達成するため本発明に係る誘導加熱
装置は、所定の長さを有する適宜断面形状の被加
熱材の端部を上下側から挾み、かつ被加熱材の軸
方向と平行するコイル導体部分からなる誘導加熱
コイルを相対向して設け、この相対する各コイル
導体に流れる電流の方向を同一とすることにより
被加熱材の軸方向と直交する磁束を形成して、該
被加熱材の端部を誘導加熱することを第1の特徴
とする。 また、上記の被加熱材とコイルとの位置関係
は、被加熱材の断面の中央部に磁極を形成し、被
加熱材の磁極を挾んだ両端部に誘起2次電流通路
を形成して発熱させることを第2の特徴とする。 さらに、上記被加熱材とコイルとの位置を被加
熱材の断面に複数の磁極を形成し、被加熱材の端
部の各磁極を挾んだ部分に夫々の誘起2次電流通
路を形成して発熱させるようにしたことを第3の
特徴とする。 (実施例) 以下本発明の実施例を第4図〜第7図を参照し
て説明する。 図において、コイル1は扁平な角筒状で、内部
に冷却水孔3を有し被加熱材の軸方向と平行な導
体1aの外側にコ字状断面の鉄心1bを積層した
部分と連結部の導体1cで構成される。このコイ
ル1は図に示すように被加熱材2の両側を挾んで
平行に相対して配設されたコイル1と1とからな
る。各コイル1,1はそれぞれ平面上に配設され
ており、したがつて、被加熱材2が連続的に一方
向に移送されていくのを遮えぎるコイル導体はな
く、したがつて被加熱材2は一方向に連続して移
送できる。さらに、コイル1は、被加熱材2の軸
方向に平行に設け、かつ相対するコイル導体1
a,1aに流れる電流の方向を同一とすることに
より、任意長さの被加熱材2の軸方向と直交する
磁束を形成するように設けている。 第4図、第5図には、それぞれ丸材及び扁平材
の2種の被加熱材2,2のピツチとボールピツチ
Sを同じに合せることにより被加熱材2の断面の
中央部に被加熱材2の軸方向に直交する磁極を形
成し、磁極を挾んだ両端部に電流通路を形成し発
熱させるコイル1と被加熱材2との配置関係及び
電流の流れる方向を示している。 被加熱材2を挾んで相対向して配設するコイル
導体1a,1aは任意の複数列だけ配設するがよ
く、一方それに合せて被加熱材2がボールピツチ
Sと等しい間隔で複数個配設され、この複数の被
加熱材2は、これらが一組をなして、多数組の被
加熱材2が連続してコイル導体1aのボールピツ
チまたはその整数倍ごとに間欠移送されながら加
熱処理されるのである。 被加熱材2とコイル導体1aの関係は、上述の
ように該被加熱材2の中央部に磁極を形成してお
り、これにより、コイル効果が最もよいが、これ
に限定されるものではなく、磁極が被加熱材2の
一部にかかつていればもちろん誘導加熱される。 つぎに、第7図は異形の被加熱材2の一例とし
て中央部が突出して肉厚部となつている偏平材と
コイル導体1aとの配置関係を示している。すな
わち、この場合は磁極中心を異形位置、つまり肉
厚部からずらすように配置する。前述の関係は第
7図A,Bに示すようにコイル導体1aの幅を大
小に変えて配置するか、または第7図Cに示すよ
うにコイル導体1aの間の配置を適当に選択する
ことによつて実現することができる。 上記第7図の場合は、被加熱材2のピツチはボ
ールピツチの2倍の関係であり、被加熱材中の誘
起電流の通路を有効に設けるため肉厚の厚い部分
と磁極センターとはなるべく、≧Δ/2(但
し、は肉厚部の中心と磁極中心間の距離、Δ
は電流の滲透深さである。)の関係が成立するよ
うにずらすことが望ましい。このように被加熱材
2とコイル導体1aを配置すると、コイル電流と
被加熱材2に誘起される2次電流は第7図B,C
のように流れ、図から分るように異形被加熱材2
の肉厚部はより多くの電流が流れ、したがつて肉
厚部もその両側の肉薄部と均等に加熱される。 なお、上記においては異形の被加熱材2の一例
として、偏平金属材の中央部が肉厚部となつた例
を示し、それに対応したコイル導体1aの配置例
を示したが、異形の被加熱材2は上記構造のもの
に限定されず、それ以外、例えば肉厚部が中央部
から外れた位置にあるような断面形状のものであ
つてよく、この場合は、その断面形状に対応して
コイル導体1aの配置間隔を変え、肉厚部も均等
に加熱されるように配慮するものである。 しかして、例えば第2図に示す従来のオープン
タイプの誘導加熱装置と本発明に係る装置とのト
ータル効率を比較すると次のようになる。 すなわち、被加熱材2として、幅b、厚さaの
フラツトバーまたはa〓の丸バーにおいて、上記従
来の加熱方式によると、誘起電流は被加熱材の断
面は流れるので a≧2.5Δ ≧158ρ/μa2 (lx,μ(透磁率)=1、ρ(比抵抗値)=100、
a=0.6cm(周波数)≧43889Hz) と高い周波数となり、トータル効率=0.336 (変換効率=0.6、伝送効率=0.8、コイル効率
=0.7)となる。 これに対して、本発明の誘導加熱装置による場
合は、誘起電流は被加熱材の軸方向に沿つて流れ
るので加熱のための周波数として中間波(例えば
50〜20000Hz)を使用できるので、変換効率、お
よび伝送効率が格段に良くなることなどから、ト
ータル効率=0.737(変換効率=0.97、伝送効率=
0.95、コイル効率=0.8)と高くできるのでその
ランニングコストは従来の高周波数を用いた装置
に比べ1/2以下にすることができる。 (発明の効果) 以上の通りであり、本発明に係る誘導加熱装置
によると、被加熱材を挾んで相対峙するコイルは
互に上下側に分離した構成であつて、被加熱材を
連続的に移送する方向に、その移送を妨げるコイ
ルが位置することがないので、被加熱材の搬送機
構は単なる横送り機構で材料の端部を揃えるのみ
の簡単な機構を使うことができ、装置のコストダ
ウンが図れる。また、相対するコイルが互に分離
しているので、その間隔を自在に調整することが
できて、被加熱材の径の変化に対しても容易に適
応することができる。 しかも、上記コイルは、被加熱材の軸方向に対
して平行に配置し、直交磁束を形成するように設
けたので、前述の通り高周波でなく中周波を使用
して誘導加熱することが可能となり、従来に比べ
てコイルのトータル効率が向上し、したがつて従
来の高周波に比べて設備コスト、ランニングコス
トを著るしく低廉ならしめることができる。 因みに、本発明の装置と従来装置との比較例を
示すと下表のようになる。
(Technical Field) The present invention relates to an induction heating device, and more particularly to an induction heating device that continuously heats an end portion of a material to be heated, which has a round or flat cross-sectional shape and has a predetermined length. (Prior Art) An induction heating device is used as a means for heating the end of a material to be heated having a predetermined length and cross section, such as a round metal material or a flat metal plate. The conveyor device for heating is complicated,
There were disadvantages of increased costs and poor coil effect. A conventional induction heating device will be explained with reference to FIGS. 1 to 3 as follows. In each figure,
1 is a coil for induction heating, and 2 is a material to be heated having a predetermined length, such as a round metal bar. The arrow shown in the figure indicates the direction in which the heated material 2 is being fed while moving. The induction heating device shown in Fig. 1 is of a so-called open type, and as shown in A and B of the figure, a coil 1 is disposed vertically in parallel with a material to be heated 2 in between, and parallel to the axial direction of the material to be heated. They are arranged orthogonally. According to this open type, as can be seen from the figure, the coil 1 is arranged so as not to obstruct the continuous movement of the heated material 2 in one direction, so the conveyance device for the heated material 2 is simple and inexpensive. However, the space factor of the heated material 2 located inside the coil 1 becomes small, which has the disadvantage that the coil effect is poor. Figure 2 shows what is called a semi-open type, and in this case as well, not only is the coil effect as poor as that of the open type in Figure 1, but also
As can be seen from the figure, a part of the coil 1 is located in a place that prevents the heated material 2 from moving in one direction.
As shown in the figure, it is necessary to move the heated material 2 not only in the lateral direction but also in the axial direction, which has the disadvantage that the conveying device becomes complicated and costly. In order to simplify the above-mentioned conveying device and increase the coil efficiency, a configuration as shown in Fig. 3 is adopted, but in this case, while the heated material 2 is flowing horizontally on the line, the An extra moving mechanism is required to move each induction heating coil 1 in and out of the position to the end of the heated material 2, and the overall structure cannot be said to be simple.
As described above, all of the conventional induction heating devices have their own advantages and disadvantages, and are not necessarily satisfactory. (Objective of the Invention) The present invention improves the above-mentioned conventional drawbacks.The conveying mechanism for the heated material is a simple one-way feeding mechanism similar to the conventional open type, and the coil efficiency is higher than that of the conventional one. It is an object of the present invention to provide an induction heating device that can use medium frequency waves, which are significantly expensive and whose equipment costs and running costs are lower than those of high frequencies. (Summary of the Invention) In order to achieve the above object, an induction heating device according to the present invention sandwiches the ends of a material to be heated having a predetermined length and an appropriate cross-sectional shape from the upper and lower sides, and Induction heating coils consisting of coil conductor portions parallel to each other are provided facing each other, and by making the direction of current flowing through each of the opposing coil conductors the same, a magnetic flux perpendicular to the axial direction of the heated material is formed, The first feature is that the end portion of the material to be heated is heated by induction. In addition, the above-mentioned positional relationship between the heated material and the coil is such that a magnetic pole is formed in the center of the cross section of the heated material, and an induced secondary current path is formed at both ends of the heated material that sandwich the magnetic pole. The second feature is that it generates heat. Furthermore, the position of the heated material and the coil is such that a plurality of magnetic poles are formed in the cross section of the heated material, and each induced secondary current path is formed in a portion sandwiching each magnetic pole at the end of the heated material. The third feature is that it generates heat. (Example) Examples of the present invention will be described below with reference to FIGS. 4 to 7. In the figure, a coil 1 has a flat rectangular cylindrical shape, has a cooling water hole 3 inside, and has a connecting part and a part in which an iron core 1b with a U-shaped cross section is laminated on the outside of a conductor 1a parallel to the axial direction of the heated material. It is composed of a conductor 1c. As shown in the figure, this coil 1 consists of two coils 1 and 1 disposed in parallel and facing each other, sandwiching both sides of a heated material 2. Each coil 1, 1 is arranged on a plane, and therefore there is no coil conductor that blocks the heated material 2 from being continuously transferred in one direction. The material 2 can be transported continuously in one direction. Furthermore, the coil 1 is provided parallel to the axial direction of the heated material 2, and has coil conductors 1 facing each other.
By making the direction of the current flowing through a and 1a the same, a magnetic flux is formed that is perpendicular to the axial direction of the heated material 2 having an arbitrary length. In FIGS. 4 and 5, two types of heated materials 2, 2, round and flat, respectively, are made to have the same pitch and ball pitch S, so that the heated material 2 is placed in the center of the cross section of the heated material 2. The diagram shows the arrangement relationship between a coil 1 and a heated material 2, which form magnetic poles perpendicular to the axial direction of the coil 1 and generate heat by forming current paths at both ends sandwiching the magnetic poles, and the direction in which the current flows. The coil conductors 1a, 1a, which are arranged facing each other with the material to be heated 2 in between, may be arranged in arbitrary plural rows, while the material to be heated 2 is arranged in plural numbers at intervals equal to the ball pitch S. The plurality of heated materials 2 are heat-treated as they form one set and are continuously transferred intermittently at every ball pitch of the coil conductor 1a or every integral multiple thereof. be. The relationship between the heated material 2 and the coil conductor 1a is such that a magnetic pole is formed in the center of the heated material 2 as described above, which provides the best coil effect, but the present invention is not limited to this. Of course, if the magnetic pole covers a part of the material 2 to be heated, induction heating will occur. Next, FIG. 7 shows, as an example of the irregularly shaped heated material 2, the arrangement relationship between a flat material whose center part is a protruding thick part and a coil conductor 1a. That is, in this case, the center of the magnetic pole is placed at the irregular position, that is, shifted from the thick part. The above relationship can be achieved by arranging the coil conductors 1a with different widths as shown in FIGS. 7A and B, or by appropriately selecting the arrangement between the coil conductors 1a as shown in FIG. 7C. This can be realized by In the case of FIG. 7 above, the pitch of the heated material 2 is twice the pitch of the ball, and in order to effectively provide a path for the induced current in the heated material, the thick part and the magnetic pole center should be arranged as much as possible. ≧Δ/2 (however, is the distance between the center of the thick part and the center of the magnetic pole, Δ
is the current penetration depth. ) is desirable. When the heated material 2 and the coil conductor 1a are arranged in this way, the coil current and the secondary current induced in the heated material 2 are as shown in Fig. 7B and C.
As can be seen from the figure, the irregularly shaped heated material 2
More current flows through the thicker part of the tube, so the thicker part is heated equally with the thinner parts on both sides. In addition, in the above, as an example of the irregularly shaped heated material 2, an example was shown in which the central part of the flat metal material became a thick part, and an example of the arrangement of the coil conductor 1a corresponding to this was shown. The material 2 is not limited to the structure described above, and may have a cross-sectional shape in which the thick part is located away from the center. The arrangement interval of the coil conductors 1a is changed to ensure that the thick portions are evenly heated. For example, when comparing the total efficiency of the conventional open type induction heating device shown in FIG. 2 and the device according to the present invention, the results are as follows. In other words, when the material to be heated 2 is a flat bar with width b and thickness a or a round bar with width a, according to the above conventional heating method, the induced current flows through the cross section of the material to be heated. a≧2.5Δ ≧158ρ/μa 2 (lx, μ (magnetic permeability) = 1, ρ (specific resistance value) = 100,
a = 0.6 cm (frequency) ≧ 43889 Hz), resulting in a high frequency, and total efficiency = 0.336 (conversion efficiency = 0.6, transmission efficiency = 0.8, coil efficiency = 0.7). On the other hand, in the case of the induction heating device of the present invention, the induced current flows along the axial direction of the material to be heated, so the frequency for heating is an intermediate wave (e.g.
50 to 20000Hz), the conversion efficiency and transmission efficiency are much improved, so the total efficiency = 0.737 (conversion efficiency = 0.97, transmission efficiency =
0.95, coil efficiency = 0.8), the running cost can be reduced to less than half that of conventional equipment using high frequencies. (Effects of the Invention) As described above, according to the induction heating device according to the present invention, the coils facing each other with the material to be heated between them are separated into upper and lower sides, and the material to be heated is continuously heated. Since there are no coils located to obstruct the transfer in the direction of transfer, the transfer mechanism for the material to be heated can be a simple mechanism that only aligns the edges of the material with a lateral feed mechanism. Cost reduction can be achieved. Further, since the opposing coils are separated from each other, the interval between them can be adjusted freely, and it is possible to easily adapt to changes in the diameter of the heated material. Moreover, since the above-mentioned coil is arranged parallel to the axial direction of the material to be heated so as to form orthogonal magnetic flux, it is possible to perform induction heating using medium frequency instead of high frequency as mentioned above. , the total efficiency of the coil is improved compared to the conventional one, and therefore the equipment cost and running cost can be significantly reduced compared to the conventional high frequency. Incidentally, a comparison example between the device of the present invention and the conventional device is shown in the table below.

【表】 本発明は従来装置に比べ上記のような諸効果を
有するものである。
[Table] The present invention has the above-mentioned effects compared to conventional devices.

【図面の簡単な説明】[Brief explanation of the drawing]

第1図A,B、第2図A,B、第3図A,Bは
それぞれ従来の誘導加熱装置の平面図と斜視図、
第4図Aと第5図は本発明に係る誘導加熱装置の
説明図、第4図Bは斜視図、第6図はコイル導体
の詳細を示す斜視図、第7図A,Bは他の実施例
の説明図と斜視図、第7図Cはさらに別の実施例
の斜視図である。 1…コイル、1a…コイル導体、2…被加熱
材。
Figures 1A and B, Figures 2A and B, and Figures 3A and B are respectively a plan view and a perspective view of a conventional induction heating device.
4A and 5 are explanatory diagrams of the induction heating device according to the present invention, FIG. 4B is a perspective view, FIG. 6 is a perspective view showing details of the coil conductor, and FIGS. 7A and B are other illustrations. Explanatory drawings and perspective views of the embodiment, FIG. 7C is a perspective view of yet another embodiment. 1... Coil, 1a... Coil conductor, 2... Heated material.

Claims (1)

【特許請求の範囲】 1 所定の長さを有する棒材条材等の被加熱材の
端部を上下側から挾み、かつ被加熱材の軸方向と
平行するコイル導体部分からなる誘導加熱コイル
を相対向して設け、この相対向する各コイル導体
に流れる電流の方向を同一として被加熱材の軸方
向と直交する磁束を形成することを特徴とする誘
導加熱装置。 2 上記コイル導体は、被加熱材の断面の中央部
に磁極が形成されるよう所定の間隔を隔てて配設
したことを特徴とする特許請求の範囲第1項に記
載の誘導加熱装置。 3 上記コイル導体は被加熱材の断面に複数の磁
極が形成されるように所定の間隔を隔てて配置し
たことを特徴とする特許請求の範囲第1項に記載
の誘導加熱装置。
[Scope of Claims] 1. An induction heating coil that sandwiches the ends of a material to be heated, such as a bar or strip, having a predetermined length from above and below, and is comprised of a coil conductor portion parallel to the axial direction of the material to be heated. An induction heating device characterized in that the coil conductors facing each other face each other, and the direction of current flowing through the facing coil conductors is the same to form a magnetic flux perpendicular to the axial direction of the heated material. 2. The induction heating device according to claim 1, wherein the coil conductors are arranged at predetermined intervals so that a magnetic pole is formed in the center of the cross section of the material to be heated. 3. The induction heating device according to claim 1, wherein the coil conductors are arranged at predetermined intervals so that a plurality of magnetic poles are formed in the cross section of the material to be heated.
JP59085753A 1984-04-27 1984-04-27 Induction heater Granted JPS60230934A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP59085753A JPS60230934A (en) 1984-04-27 1984-04-27 Induction heater

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP59085753A JPS60230934A (en) 1984-04-27 1984-04-27 Induction heater

Publications (2)

Publication Number Publication Date
JPS60230934A JPS60230934A (en) 1985-11-16
JPH0459367B2 true JPH0459367B2 (en) 1992-09-22

Family

ID=13867615

Family Applications (1)

Application Number Title Priority Date Filing Date
JP59085753A Granted JPS60230934A (en) 1984-04-27 1984-04-27 Induction heater

Country Status (1)

Country Link
JP (1) JPS60230934A (en)

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0794684B2 (en) * 1990-10-05 1995-10-11 富士電子工業株式会社 Induction hardening and tempering device for rod-shaped workpieces
JP6866410B2 (en) * 2019-02-20 2021-04-28 島田理化工業株式会社 Induction heating method using a tunnel type heating coil

Also Published As

Publication number Publication date
JPS60230934A (en) 1985-11-16

Similar Documents

Publication Publication Date Title
JPH01157085A (en) Induction heater
EP0400112A1 (en) High-voltage winding for core-form power transformers
CA1139383A (en) Spiralled printed inductance
US4527032A (en) Radio frequency induction heating device
AU3266193A (en) Induction furnace
US3965378A (en) Pole coil for electric machines and apparatus
JPH0459367B2 (en)
US356902A (en) Elihu thomson
JP2000150259A (en) High frequency coil and high frequency transformer
CN86101224B (en) Method for manufacturing electromagnetic element
JPS58137989A (en) Induction heater of strip metal material
GB2121260A (en) Transverse flux induction heater
EP0339827B1 (en) Flat voltage transformer
JPH088051A (en) Method and apparatus for induction heating of metal plate
JPH08168229A (en) Linear motor
JPH077703B2 (en) Heating coil for thin plate soaking
JP3031213B2 (en) Electromagnetic induction equipment
JP2002015901A (en) Water-cooled resistor
JP2002043044A (en) Heating coil for induction heating device
EP3467851A1 (en) Transformer core with reduced building factor
JPS6137741B2 (en)
JPS625038Y2 (en)
JP2545869Y2 (en) High frequency heating coil
JP3074316B2 (en) Sheet coil lamination or loading products
JPH0237689A (en) Induction heating coil device