JPH0126155B2 - - Google Patents

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Publication number
JPH0126155B2
JPH0126155B2 JP2849784A JP2849784A JPH0126155B2 JP H0126155 B2 JPH0126155 B2 JP H0126155B2 JP 2849784 A JP2849784 A JP 2849784A JP 2849784 A JP2849784 A JP 2849784A JP H0126155 B2 JPH0126155 B2 JP H0126155B2
Authority
JP
Japan
Prior art keywords
magnetic
cores
heated
width
heater
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
Application number
JP2849784A
Other languages
Japanese (ja)
Other versions
JPS60175390A (en
Inventor
Haruo Hoshika
Takashi Yamashita
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.)
Shinko Electric Co Ltd
Original Assignee
Shinko Electric 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 Shinko Electric Co Ltd filed Critical Shinko Electric Co Ltd
Priority to JP2849784A priority Critical patent/JPS60175390A/en
Publication of JPS60175390A publication Critical patent/JPS60175390A/en
Publication of JPH0126155B2 publication Critical patent/JPH0126155B2/ja
Granted legal-status Critical Current

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  • General Induction Heating (AREA)

Description

【発明の詳細な説明】 本発明は交叉磁界型誘導加熱器における加熱温
度の分布を均一に調整するための装置に関し、本
件出願人の先願に係る特願昭58−206911号(昭和
58年11月5日出願)に関連する。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a device for uniformly adjusting the distribution of heating temperature in a cross-magnetic field type induction heater, and relates to a device for uniformly adjusting the distribution of heating temperature in a cross-magnetic field type induction heater.
(filed on November 5, 1958).

従来この種の交叉磁界型誘導加熱器として第1
図に示すごときものが一般に使用されており、被
加熱物1を上方および下方から加熱するために交
叉磁界型誘導加熱器2Aおよび2Bが上下一対配
置されている。加熱器2Aおよび2Bにはそれぞ
れコイル3Aおよび3Bが各磁極(ポール)毎に
巻かれていて、このコイル3A,3Bに印加され
る交番電流によつて各磁界から交番磁界が発生す
る。被加熱物1がこの交番磁界内に置かれると、
電磁誘導によつて被加熱物中にうず電流が流れ、
このうず電流によつてジユール熱が発生し、被加
熱物自体が加熱されるものである。
The first cross-magnetic field type induction heater of this type
The one shown in the figure is generally used, and a pair of crossed magnetic field type induction heaters 2A and 2B are arranged above and below to heat the object 1 from above and below. Coils 3A and 3B are wound around each magnetic pole in the heaters 2A and 2B, respectively, and an alternating magnetic field is generated from each magnetic field by alternating current applied to the coils 3A and 3B. When the heated object 1 is placed within this alternating magnetic field,
Eddy current flows through the heated object due to electromagnetic induction,
This eddy current generates Joule heat, which heats the object itself.

このような交叉磁界型誘導加熱器においては、
加熱に際してエツヂ効果が発生するため被加熱物
の端部と中央部とが均一に加熱されないという難
点があつた。すなわち、第1図に実線で示すよう
に、加熱器2A,2Bの誘電子の幅、すなわち加
熱器2A,2Bの横幅Wと実質的に等しい幅より
も小さい横幅寸法をもつ被加熱物1が加熱される
場合には、その端部が中央部よりも過熱されるも
のであり、一方点線で示すように横幅寸法の大き
な被加熱物1Aの場合には、その端部が中央部に
較べて充分に加熱され得ないという不都合があつ
た。以上述べたエツヂ効果は被加熱物の横幅方向
に関するものであるが、縦方向についても全く同
様のエツヂ効果が発生する。すなわち、誘電子の
磁極間隔(N極ポールとS極ポールとの間隔)よ
りも被加熱物の縦幅が小さい場合にはその端部が
過熱され、大きい場合にはその端部の加熱が不充
分となる不都合があつた。前述した本件出願人の
先願に係る発明は、磁気抵抗の小さい磁性体を使
用して誘電子から発生する磁束を増強せしめ、そ
れによつてエツヂ効果に起因する加熱温度分布の
不均一を改善または解消せんとするものである。
In such a crossed magnetic field type induction heater,
There was a problem in that the edges and the center of the object to be heated were not heated uniformly because an edge effect occurred during heating. That is, as shown by the solid line in FIG. 1, the heated object 1 has a width smaller than the width of the dielectric of the heaters 2A, 2B, that is, the width substantially equal to the width W of the heaters 2A, 2B. When heated, the edges are heated more than the center. On the other hand, in the case of the heated object 1A having a large width as shown by the dotted line, the edges are heated more than the center. There was an inconvenience that it could not be heated sufficiently. The edge effect described above relates to the width direction of the object to be heated, but the same edge effect also occurs in the vertical direction. In other words, if the vertical width of the object to be heated is smaller than the magnetic pole spacing of the dielectric (the spacing between the N pole and the S pole), the ends of the object will be overheated, and if it is larger, the ends will not be heated. There were enough inconveniences. The above-mentioned invention related to the applicant's earlier application uses a magnetic material with low magnetic resistance to enhance the magnetic flux generated from the inductor, thereby improving or improving the non-uniform heating temperature distribution caused by the edge effect. This is something that we are trying to resolve.

本発明は、このようなエツヂ効果に起因する加
熱温度分布の不均一を、磁気抵抗の大きな非磁性
導電体を使用して誘電子から発生する磁束を減殺
せしめることにより、改善または解消せんとする
調節装置を提供するものである。
The present invention aims to improve or eliminate the uneven heating temperature distribution caused by the edge effect by using a non-magnetic conductor with high magnetic resistance to attenuate the magnetic flux generated from the inductor. A regulating device is provided.

以下図面を参照して本発明の実施例につき詳説
する。
Embodiments of the present invention will be described in detail below with reference to the drawings.

第2図に示される交叉磁界型誘導加熱器におい
て、第1図に示したものと同一または同等の部材
については第1図の符合と同一のものを付し、そ
の説明を省略する。横幅寸法の小さな被加熱物1
Aが加熱器2A,2B間に置かれる場合には、前
述したエツヂ効果による温度分布の不均一、すな
わち中央部に対する端部の過熱を避けるため、第
3図に示すような直方体を側面の対角線に沿つて
切断した形状の例えばアルミニユムや銅などの非
磁性導電体コア4を、第2図に示す如く被加熱物
1Aの端部に4個(4A,4A′,4B,4B′)配置
する。4Aと4A′で示す2個のコアが1組とし
て両端部に配置される。非磁性導電体からなるコ
アが存在することによつてそこを通過する磁束の
磁気抵抗が増大する結果磁束密度が減少する。す
なわち、非磁性導電体は、その内部を通過する磁
束エネルギーが過電流に伴う熱エネルギーとして
消費されるので、磁束の通過を減殺する働きをす
る。そのため被加熱物1Aの端部はコアが存在し
ない場合に較べてより弱く加熱され、そのため中
央部とほぼ均一に加熱することが可能である。な
お、被加熱物の横幅Wに対応してコアの位置を調
節可能とすることが望ましく、そのために例えば
ねじ手段またはカム手段(図示しない)を利用す
ることができる。
In the cross-magnetic field type induction heater shown in FIG. 2, members that are the same or equivalent to those shown in FIG. 1 are given the same reference numerals as in FIG. 1, and their explanations will be omitted. Object to be heated with small width dimension 1
When A is placed between the heaters 2A and 2B, in order to avoid uneven temperature distribution due to the edge effect mentioned above, that is, overheating of the ends relative to the center, a rectangular parallelepiped as shown in Fig. Four non-magnetic conductive cores 4 (4A, 4A', 4B, 4B') made of aluminum, copper or the like are placed at the end of the object to be heated 1A, as shown in FIG. . Two cores, designated 4A and 4A', are arranged as a set at both ends. Due to the presence of the core made of a non-magnetic conductor, the magnetic resistance of the magnetic flux passing through it increases, resulting in a decrease in magnetic flux density. That is, since the magnetic flux energy passing through the non-magnetic conductor is consumed as thermal energy due to overcurrent, the non-magnetic conductor functions to reduce the passage of magnetic flux. Therefore, the ends of the object to be heated 1A are heated more weakly than in the case where there is no core, and therefore it is possible to heat the object almost uniformly with the center. Note that it is desirable to be able to adjust the position of the core in accordance with the width W of the object to be heated, and for this purpose, for example, screw means or cam means (not shown) can be used.

第4図を参照すれば前述各コアの縦方向配列の
様子が明らかとなる。すなわち、3つのコア4A
−1,4A−2,4A−3はポールピツチ2Pで
配列された磁極N、S、Nと同一の間隔で配列さ
れている。第4図は上方の加熱器2Aのみを示
し、下方の加熱器の図示を省略した図面であるか
ら、第2図の実施例においては上方加熱器2Aの
ために使用されるコアとして6個、同様に下方加
熱器2Bのために6個、合計12個のコアが使用さ
れるものである。第4図に示すようにコア4A−
1,4A−2,4A−3が各磁極の真下に置かれ
た場合には、前述のとおり磁極からの磁束密度が
コアによつて減少され、コアの近傍における被加
熱物への加熱が減殺される。一方、第4図のコア
を第5図に示す位置に移動させたとすると、すな
わち各コアが磁極と磁極の間に位置するときは、
各磁極からの磁束は磁気抵抗の大きなコア内を通
過し難いため磁極からの磁束は妨げられず、よつ
て発生する熱は増大する。各組のコアが第4図に
示す位置から第5図の位置に一体的に移動可能と
し、その移動量を調節することによつて被加熱物
1Aの加熱を弱から強へと連続的に調節すること
が可能となる。これらの複数コアを一体的に移動
せしめる手段としては第4図に示すように各コア
4A−1,4A−2,4A−3を例えばプラスチ
ツク材のブロツク5中に組み入れてモールド成形
し一体構成物とすることが出来、それを適当な例
えばカム手段またはねじ手段(図示しない)を使
用して移動せしめることが可能である。
Referring to FIG. 4, the manner in which the cores are arranged in the vertical direction becomes clear. That is, three cores 4A
-1, 4A-2, 4A-3 are arranged at the same intervals as the magnetic poles N, S, and N arranged at the pole pitch 2P. Since FIG. 4 shows only the upper heater 2A and omits the illustration of the lower heater, in the embodiment of FIG. 2, six cores are used for the upper heater 2A, Similarly, 6 cores are used for the lower heater 2B, for a total of 12 cores. As shown in Figure 4, core 4A-
When 1, 4A-2, and 4A-3 are placed directly under each magnetic pole, the magnetic flux density from the magnetic poles is reduced by the core as described above, and the heating of the heated object near the core is reduced. be done. On the other hand, if the cores in FIG. 4 are moved to the positions shown in FIG. 5, that is, when each core is located between the magnetic poles,
Since it is difficult for the magnetic flux from each magnetic pole to pass through the core, which has a large magnetic resistance, the magnetic flux from the magnetic poles is not blocked, and therefore the heat generated increases. The cores of each set can be integrally moved from the position shown in Fig. 4 to the position shown in Fig. 5, and by adjusting the amount of movement, the heating of the heated object 1A can be continuously changed from weak to strong. It becomes possible to adjust. As a means for integrally moving these plurality of cores, as shown in FIG. 4, each core 4A-1, 4A-2, 4A-3 is assembled into a block 5 made of plastic material and molded to form an integral structure. and it is possible to move it using suitable e.g. cam means or screw means (not shown).

以上述べたように、被加熱物の横幅W′が狭い
場合には加熱器2Aの横幅方向において、コア4
4A,4B,4A′,4B′を第2図に示すように
配置し、且つ長手方向においては第4図に示すよ
うに磁極の真下かあるいはそれに近い位置に配置
することによつて被加熱物1Aの端部の過熱を防
止することが出来、その中央部との不均一を軽減
することが可能となる。一方、被加熱物の横幅
W′が大きい場合には、エツヂ効果によつてその
端部が中央部に比べて加熱され難いため、コアを
幅方向においては第2図の配置のままとし、縦方
向における配列を第5図に示すように磁極間に置
くか、またはそれに近い位置とすることによつ
て、端部の加熱を増強せしめ、その中央部との不
均一を避けることが可能となる。
As mentioned above, when the width W' of the object to be heated is narrow, the core 4
By arranging 4A, 4B, 4A', and 4B' as shown in Fig. 2, and arranging them in the longitudinal direction directly under or close to the magnetic poles as shown in Fig. 4, the object to be heated can be heated. It is possible to prevent overheating of the ends of 1A, and it is possible to reduce unevenness with respect to the center part. On the other hand, the width of the heated object
When W' is large, the edges are less likely to be heated than the center due to the edge effect, so the cores are arranged in the width direction as shown in Figure 2, and in the longitudinal direction as shown in Figure 5. By placing it between the magnetic poles or in a position close to them as shown in Figure 2, it is possible to intensify the heating at the ends and avoid non-uniformity with respect to the center.

以上述べた実施例では、コアの形状を第3図に
示すようなものとして説明したが、本発明はこの
形状には限定されず、第3図における斜面が直線
ではなく例えば曲線を呈するものでも支障ない。
すなわち、加熱器の横幅方向においてその端部に
向つて次第に厚さが増加し、磁極の縦方向幅aと
ほぼ等しい縦幅を有する形状のものであればよ
い。また、実施例においては上下一対の加熱器が
示されたが、どちらか一方の加熱器によつても本
発明の所期効果は達成され得るものである。
In the embodiments described above, the shape of the core was explained as shown in FIG. 3, but the present invention is not limited to this shape, and the slope shown in FIG. 3 may be curved, for example, instead of a straight line. No problem.
That is, it is sufficient that the heater has a shape in which the thickness gradually increases toward the ends in the width direction of the heater, and the vertical width is approximately equal to the vertical width a of the magnetic pole. Further, although a pair of upper and lower heaters is shown in the embodiment, the desired effects of the present invention can be achieved with either one of the heaters.

さらにまた、第2図に示す実施例においては、
2個1組のコアが2組、すなわちコア4A,4B
の組とコア4A′,4B′のそれぞれの組を図面上
左、右に設置した場合について述べたが、本発明
はそれに限定されず、例えば上方側のコア4Aと
4A′をそれぞれ右左に配置してもよく、または
下方側のコア4Bと4B′のみをそれぞれ右左に
配置した構成であつても本発明の所期の目的およ
び効果は達成され得るものである。なお、本発明
の先行技術として、実用新案公報第371698号公報
(実公昭24−9782号)のものがあるが、同公報の
記載は、高周波焼き入用誘導体に「反磁性体の遮
蔽板5」が用いられる点と、「反磁性体(非磁性
体)を遮蔽体に使用することにより減磁作用があ
る」が公知であることを示すものに過ぎない。
Furthermore, in the embodiment shown in FIG.
Two sets of two cores, namely cores 4A and 4B
Although the case has been described in which the sets of cores 4A' and 4B' are placed on the left and right in the drawing, the present invention is not limited thereto. For example, the upper cores 4A and 4A' may be placed on the right and left, respectively. Alternatively, the intended objects and effects of the present invention can be achieved even if only the lower cores 4B and 4B' are arranged on the right and left sides, respectively. In addition, as a prior art of the present invention, there is Utility Model Publication No. 371698 (Utility Model Publication No. 24-9782), but the publication describes that a diamagnetic shielding plate 5 is used for the induction hardening dielectric. ” is used and that “using a diamagnetic material (non-magnetic material) as a shielding material has a demagnetizing effect” is known.

従つて、本発明のものとは、次のように顕著な
相違点がある。即ち、 先行技術のものでは、非磁性体を遮蔽板とし
て唯単に、配置したものであるのに対し、本発
明のものでは、複数個の非磁性導電体のコアと
して複数個の磁極に対応して配置し、しかも、
上記複数コアは一体的に縦方向に移動可能に配
置するようにしている。
Therefore, there are significant differences from the present invention as follows. That is, in the prior art, a non-magnetic material is simply arranged as a shielding plate, whereas in the present invention, a plurality of non-magnetic conductive cores are arranged to correspond to a plurality of magnetic poles. and place it, and
The plurality of cores are arranged so as to be integrally movable in the vertical direction.

この結果、本発明のものでは、各非磁性導電
体が各磁極からの磁束を幅方向に亙つて均一と
なるように適正に減少させ、被加熱物の加熱温
度分布を均一にするという作用・効果は1個の
遮蔽板をただ配置したに過ぎない先行技術のも
のにくらべ、はるかに、優れているといえる。
As a result, in the present invention, each non-magnetic conductor appropriately reduces the magnetic flux from each magnetic pole so that it becomes uniform across the width, and the heating temperature distribution of the heated object is made uniform. It can be said that the effect is far superior to that of the prior art in which only one shielding plate is disposed.

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

第1図は従来の交叉磁界型加熱器を示す正面
図、第2図は本発明の一実施例を示す正面図、第
3図は非磁性導電体コアを示す斜視図、第4図、
第5図は前記実施例における磁極と非磁性導電体
コアの配列関係を示すための側面図である。 1,1A……被加熱物、2A,2B……加熱
器、3A,3B……コイル、4,4A,4B……
非磁性導電体コア、5……プラスチツク部材、
S,N……磁極、2P……ポールピツチ。
FIG. 1 is a front view showing a conventional cross-field heater, FIG. 2 is a front view showing an embodiment of the present invention, FIG. 3 is a perspective view showing a non-magnetic conductive core, and FIG.
FIG. 5 is a side view showing the arrangement relationship between the magnetic poles and the nonmagnetic conductive core in the embodiment. 1, 1A... Heated object, 2A, 2B... Heater, 3A, 3B... Coil, 4, 4A, 4B...
Non-magnetic conductive core, 5... plastic member,
S, N...magnetic pole, 2P...pole pitch.

Claims (1)

【特許請求の範囲】 1 交叉磁界型誘導加熱器とこの誘導加熱器によ
つて加熱されるべき被加熱物の間に次の構成の複
数個の非磁性導電体コアを配置することによつて
前記被加熱物の加熱温度分布が均一となるように
調整可能としたことを特徴とする交叉磁界型誘導
加熱器の加熱温度分布調整装置。 a 上記複数個の各コアの形状は前記横幅方向に
おいてその端部に向かつて次第に厚さを増加さ
せ、縦方向において前記磁極の縦方向幅とほぼ
等しい幅を有するようにする。 b 上記各コアは前記加熱器の横幅方向の一方端
部または両端部において、前記加熱器の縦方向
に配列された複数個の磁極のそれぞれに対応し
て配置される。 c 上記複数個のコアは一体的に縦方向に移動可
能なように配置される。
[Claims] 1. By arranging a plurality of non-magnetic conductive cores having the following configuration between a crossed magnetic field type induction heater and an object to be heated by the induction heater. A heating temperature distribution adjusting device for a crossed magnetic field type induction heater, characterized in that the heating temperature distribution of the object to be heated can be adjusted so as to be uniform. a. The shape of each of the plurality of cores is such that the thickness gradually increases toward the end in the width direction, and the width in the longitudinal direction is approximately equal to the longitudinal width of the magnetic pole. b. Each of the cores is arranged at one or both ends of the heater in the width direction, corresponding to each of the plurality of magnetic poles arranged in the longitudinal direction of the heater. c. The plurality of cores are arranged so as to be integrally movable in the vertical direction.
JP2849784A 1984-02-20 1984-02-20 Heating temperature distribution regulator for ac field induction heater Granted JPS60175390A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP2849784A JPS60175390A (en) 1984-02-20 1984-02-20 Heating temperature distribution regulator for ac field induction heater

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP2849784A JPS60175390A (en) 1984-02-20 1984-02-20 Heating temperature distribution regulator for ac field induction heater

Publications (2)

Publication Number Publication Date
JPS60175390A JPS60175390A (en) 1985-09-09
JPH0126155B2 true JPH0126155B2 (en) 1989-05-22

Family

ID=12250306

Family Applications (1)

Application Number Title Priority Date Filing Date
JP2849784A Granted JPS60175390A (en) 1984-02-20 1984-02-20 Heating temperature distribution regulator for ac field induction heater

Country Status (1)

Country Link
JP (1) JPS60175390A (en)

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0542635Y2 (en) * 1986-12-05 1993-10-27
JP2006294396A (en) * 2005-04-11 2006-10-26 Shimada Phys & Chem Ind Co Ltd Induction heating device

Also Published As

Publication number Publication date
JPS60175390A (en) 1985-09-09

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