JPS636876Y2 - - Google Patents

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Publication number
JPS636876Y2
JPS636876Y2 JP2126885U JP2126885U JPS636876Y2 JP S636876 Y2 JPS636876 Y2 JP S636876Y2 JP 2126885 U JP2126885 U JP 2126885U JP 2126885 U JP2126885 U JP 2126885U JP S636876 Y2 JPS636876 Y2 JP S636876Y2
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JP
Japan
Prior art keywords
magnetic field
frequency magnetic
frequency
generated
generating means
Prior art date
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Expired
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JP2126885U
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Japanese (ja)
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JPS61138187U (en
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Description

【考案の詳細な説明】 〔産業上の利用分野〕 本考案は電気暖房器に関し、特に高周波誘導加
熱を利用した電気暖房器に関する。
[Detailed Description of the Invention] [Industrial Application Field] The present invention relates to an electric heater, and particularly to an electric heater using high-frequency induction heating.

周知の如く、物体はその温度に応じてその表面
から電磁波を放射することが知られている。この
とき放射される電磁波の放射エネルギ密度E〓は、
電磁波の波長λと物体の温度(絶対温度)Tのみ
に依存し、良く知られたプランクの放射式、 E〓=8πhc/λ5・1/exp(hc/kTλ)−1 で表わされる。ここでhはプランク定数、kはボ
ルツマン定数、cは光速度である。一般に、この
放射される電磁波は、赤外線(波長が0.75μmか
ら数mmの範囲)の範囲にあり、第6図に示される
ように、放射エネルギ密度E〓のピークは、温度T
が高い程波長λの短い方に、逆に温度Tが低い程
波長λの長い方にあらわれる。なお、物体が電磁
波を放射するという事実は、例えば、人体が放射
する赤外線を波布が感知して、人を襲うというこ
とからも、良く知られている。このように、人体
等の物体は、その温度に応じた電磁波、すなわち
赤外線を外部に放射しているが、逆に、赤外線
は、熱線ともいわれるように、熱作用が大きく、
人体等の物体中で吸収を受ける。このとき吸収さ
れる赤外線の播長範囲は、主に5μm〜20μmの範
囲で顕著である。前述したように、温度Tが高い
と放射エネルギ密度E〓のピークが短波長側にくる
ので、吸収されないエネルギが大きくなる。従つ
て、温度は最大400℃程度とし、好ましくは260℃
程度が良い。
As is well known, it is known that an object emits electromagnetic waves from its surface depending on its temperature. The radiant energy density E〓 of the electromagnetic waves emitted at this time is
It depends only on the wavelength λ of the electromagnetic wave and the temperature (absolute temperature) T of the object, and is expressed by the well-known Planck radiation equation, E=8πhc/λ 5・1/exp(hc/kTλ)−1. Here, h is Planck's constant, k is Boltzmann's constant, and c is the speed of light. Generally, this radiated electromagnetic wave is in the infrared range (wavelength ranges from 0.75 μm to several mm), and as shown in Figure 6, the peak of the radiant energy density E〓 is at a temperature T
The higher the temperature T, the shorter the wavelength λ, and conversely, the lower the temperature T, the longer the wavelength λ. The fact that objects emit electromagnetic waves is well known, for example because wave cloth detects infrared rays emitted by the human body and attacks people. In this way, objects such as the human body emit electromagnetic waves, or infrared rays, to the outside according to their temperature, but on the other hand, infrared rays have a large thermal effect, and are also called heat rays.
Absorbed in objects such as the human body. The propagation range of the infrared rays absorbed at this time is remarkable mainly in the range of 5 μm to 20 μm. As mentioned above, when the temperature T is high, the peak of the radiant energy density E is on the short wavelength side, so the amount of energy that is not absorbed increases. Therefore, the maximum temperature should be around 400℃, preferably 260℃.
Good condition.

このような赤外線の性質を利用した電気暖房器
として、従来から電気こたつや電気ストーブ等が
知られている。しかしながら、この種の電気暖房
器は、発熱体に直接電流を流す構成であるため、
該発熱体に絶縁体を施すことを要し、又、該暖房
器が古くなると絶縁体が剥離し感電を起こすおそ
れがあつた。
Electric kotatsus, electric stoves, and the like have been known as electric heaters that utilize the properties of infrared rays. However, this type of electric heater is configured to pass current directly to the heating element, so
It is necessary to apply an insulator to the heating element, and when the heater gets old, there is a risk that the insulator may peel off and cause an electric shock.

〔従来の技術〕[Conventional technology]

そこで、本考案は、上記欠点を解消するものと
して、昭和59年9月11日に提出した特願昭59−
188895号、発明の名称「遠赤外線暖房器」におい
て、高周波誘導加熱を応用した電気暖房器をすで
に提案している。
Therefore, the present invention was proposed in a patent application filed on September 11, 1980, in order to eliminate the above-mentioned drawbacks.
No. 188895, titled "Far-infrared heater", has already proposed an electric heater that applies high-frequency induction heating.

この提案した電気暖房器は、高周波電流を発生
する高周波電流発生器と、該高周波電流により高
周波磁界を発生する渦巻状に巻回された1個の誘
導コイルからなる高周波磁界発生器と、該高周波
磁界の変化による電磁誘導作用により生ずる渦電
流損とヒステリシス損で加熱され、該加熱された
温度に対応した赤外線を放射する鉄系金属磁性体
を含む赤外線放射部材とを有している。
This proposed electric heater consists of a high-frequency current generator that generates a high-frequency current, a high-frequency magnetic field generator consisting of one spirally wound induction coil that generates a high-frequency magnetic field by the high-frequency current, and a high-frequency magnetic field generator that generates a high-frequency magnetic field using the high-frequency current. It has an infrared ray emitting member including an iron-based metal magnetic material that is heated by eddy current loss and hysteresis loss caused by electromagnetic induction due to changes in the magnetic field and emits infrared rays corresponding to the heated temperature.

第4図はこの電気暖房器に使用されている高周
波誘導加熱装置を示したブロツク図、第5図は第
4図に示した高周波誘導加熱装置の高周波磁界発
生器と被加熱体なる赤外線放射部材の配置関係を
示した図で、aは正面図、bはaのB−B′線か
ら見た断面図、cは磁界の強さを示した図であ
る。
Fig. 4 is a block diagram showing the high frequency induction heating device used in this electric heater, and Fig. 5 shows the high frequency magnetic field generator and the infrared radiation member which is the heated object of the high frequency induction heating device shown in Fig. 4. FIG. 2 is a diagram showing the arrangement relationship between the two, in which a is a front view, b is a cross-sectional view taken along line B-B' of a, and c is a diagram showing the strength of the magnetic field.

第4図に示されるように、従来の高周波誘導加
熱装置10′は、高周波電流発振器11と該高周
波電流発振器11に結線された電力増幅器12と
該電力増幅器12に結線された高周波磁界発生器
13′とからなり、該高周波磁界発生器13′は、
渦巻状に巻回された1個の誘導コイルから構成さ
れている。
As shown in FIG. 4, the conventional high-frequency induction heating device 10' includes a high-frequency current oscillator 11, a power amplifier 12 connected to the high-frequency current oscillator 11, and a high-frequency magnetic field generator 13 connected to the power amplifier 12. ', and the high frequency magnetic field generator 13' is
It consists of a single spirally wound induction coil.

第5図を参照すると、上記高周波磁界発生器1
3′と赤外線放射部材20とは、互いの面が平行
になるように、かつ互いの中心が一致する如く、
近接して配置されている。
Referring to FIG. 5, the high frequency magnetic field generator 1
3' and the infrared radiation member 20, so that their surfaces are parallel to each other and their centers coincide.
located close together.

このような構成において、ある時刻における高
周波電流発器11から発生された電流Iが、第5
図aの矢印の方向、換言すると、第5図bの及
び○・で示される方向(ここで、は紙面上方より
下方への方向、○・は紙面下方より上方の方向を示
す。)に、流れていたとする。このとき、高周波
磁界発生器13′より発生する磁界は、第5図a
において、中心付近で一番強く、紙面上方より下
方、すなわち方向、周縁付近では紙面下方より
上方、すなわち○・方向で、その強さは第5図cの
ように表わされる。ここで、第5図bの点線は磁
界の流れる方向を示している。
In such a configuration, the current I generated from the high frequency current generator 11 at a certain time is the fifth
In the direction of the arrow in Figure a, in other words, in the direction indicated by and ○• in Figure 5b (here, indicates the direction downward from the top of the paper, and ○ indicates the direction upward from the bottom of the paper). Suppose it was flowing. At this time, the magnetic field generated by the high frequency magnetic field generator 13' is as shown in FIG.
The strength is strongest near the center, below the top of the page, that is, in the direction, and near the periphery, above the bottom of the page, ie, in the ◯ direction, and its strength is expressed as shown in Figure 5c. Here, the dotted line in FIG. 5b indicates the direction in which the magnetic field flows.

このようにして、赤外線放射部材20の内部を
磁界、すなわち磁束が通過するが、そのとき電磁
誘導により、その磁束の変化を妨げる向きに誘導
電流、すなわち渦電流が流れ、強磁性材料なる赤
外線放射部材20に、渦電流損失及びヒステリシ
ス損失が生じ、赤外線放射部材20は加熱され
る。このとき、加熱された温度に応じた赤外線
が、赤外線放射部材20の表面より放射される。
In this way, a magnetic field, that is, magnetic flux, passes through the inside of the infrared radiating member 20, but at this time, due to electromagnetic induction, an induced current, that is, eddy current flows in a direction that prevents changes in the magnetic flux, and the infrared rays emitted by the ferromagnetic material Eddy current losses and hysteresis losses occur in the member 20, and the infrared radiating member 20 is heated. At this time, infrared rays corresponding to the heated temperature are emitted from the surface of the infrared radiating member 20.

〔考案が解決しようとする問題点〕[Problem that the invention attempts to solve]

このような従来の構造では、第5図cに示され
たように、赤外線放射部材20を通過する磁束が
その中心付近のみ大きく、赤外線放射部材20は
中心部分のみ加熱されることになる。そのため、
赤外線放射部材20では、その温度分布が不均一
となり、膨張の度合が各点で異なり、結果とし
て、そりを生じてしまう欠点があつた。
In such a conventional structure, as shown in FIG. 5c, the magnetic flux passing through the infrared radiation member 20 is large only near its center, and the infrared radiation member 20 is heated only at its center. Therefore,
The infrared ray radiating member 20 has the disadvantage that its temperature distribution is non-uniform and the degree of expansion differs at each point, resulting in warpage.

〔問題点を解決するための手段〕[Means for solving problems]

本考案による電気暖房器は、高周波電流発生手
段と、該高周波電流発生手段から発生される高周
波電流により高周波磁界を発生する高周波磁界発
生手段と、該高周波磁界発生手段から発生される
高周波磁界による電磁誘導作用により生ずるエネ
ルギ損失で加熱され、該加熱温度に対応した赤外
線を放射する放射手段とを有して成る電気暖房器
において、前記高周波磁界発生手段は、発生する
高周波磁界の方向が互いの逆方向の少なくとも2
つの領域に区分され、相隣接した前記区分領域の
内部より発生する高周波磁界の方向が互いに逆
で、かつ該区分領域の周囲を流れる前記高周波電
流の方向が全て同一回転方向になるように、複数
のコイルが前記放射手段を覆う如く配置されてい
る。
The electric heater according to the present invention includes a high-frequency current generating means, a high-frequency magnetic field generating means for generating a high-frequency magnetic field by the high-frequency current generated from the high-frequency current generating means, and an electromagnetic field generated by the high-frequency magnetic field generated from the high-frequency magnetic field generating means. In an electric heater comprising a radiation means that is heated by energy loss caused by induction and emits infrared rays corresponding to the heating temperature, the high-frequency magnetic field generating means is configured such that the directions of the generated high-frequency magnetic fields are opposite to each other. at least 2 of the directions
The plurality of regions are divided into two regions, and the directions of high-frequency magnetic fields generated from inside the adjacent divided regions are opposite to each other, and the directions of the high-frequency currents flowing around the divided regions are all in the same rotational direction. A coil is arranged to cover the radiation means.

〔作 用〕[Effect]

このように高周波磁界発生手段として複数のコ
イルを配列すると、発生する高周波磁界が一箇所
に集中されることなく分散されることになるの
で、それにより加熱される放射手段は均一に加熱
されることになり、放射手段のそりの発生を防止
できる。又、各コイルは、相隣接した区分領域よ
り発生する高周波磁界の方向が逆で、かつ該区分
領域の周囲を流れる高周波電流の方向が同一回転
方向になるように、配列されているので、ある区
分領域で発生した高周波磁界が他の区分領域で発
生した高周波磁界により打ち消されることを防止
でき、効率良く高周波磁界が発生される。
When multiple coils are arranged as a high-frequency magnetic field generating means in this way, the generated high-frequency magnetic field is not concentrated in one place but is dispersed, so that the radiation means heated thereby is heated uniformly. This makes it possible to prevent the radiation means from warping. Furthermore, each coil is arranged so that the direction of the high-frequency magnetic field generated by the adjacent segmented regions is opposite, and the direction of the high-frequency current flowing around the segmented regions is in the same rotational direction. It is possible to prevent the high frequency magnetic field generated in the divided area from being canceled by the high frequency magnetic field generated in other divided areas, and the high frequency magnetic field is efficiently generated.

〔実施例〕〔Example〕

以下、図面を参照して本考案の実施例について
説明する。
Embodiments of the present invention will be described below with reference to the drawings.

第1図は本考案による電気暖房器に使用される
高周波誘導加熱装置の一実施例の構成を示したブ
ロツク図、第2図は第1図に示した高周波誘導加
熱装置の高周波磁界発生器と赤外線放射部材の配
置関係を示した図で、aは正面図、bはaのA−
A′線から見た断面図である。
Fig. 1 is a block diagram showing the configuration of an embodiment of the high frequency induction heating device used in an electric heater according to the present invention, and Fig. 2 shows the high frequency magnetic field generator of the high frequency induction heating device shown in Fig. 1. Figures illustrating the arrangement of infrared radiation members, a is a front view, and b is a side view of a.
It is a sectional view seen from line A'.

本考案の高周波誘導加熱装置10は、第4図に
示したものと同様に、高周波電流発振器11と該
高周波電流発振器11に結線された電力増幅器1
2と、該電力増幅器12に結線された高周波磁界
発生器13とから成るが、この高周波磁界発生器
13は、後述するように、従来の高周波磁界発生
器13′と異なつている。
The high-frequency induction heating device 10 of the present invention includes a high-frequency current oscillator 11 and a power amplifier 1 connected to the high-frequency current oscillator 11, as shown in FIG.
2 and a high frequency magnetic field generator 13 connected to the power amplifier 12, but this high frequency magnetic field generator 13 is different from a conventional high frequency magnetic field generator 13', as will be described later.

第2図を参照すると、本考案に係る高周波磁界
発生器13は、図示の如く複数のコイルを配列し
て赤外線放射部材20を覆い、互いの面が平行に
なるように近接して配置されるが、発生する高周
波磁界が細長い5つの領域に区分されている。こ
こでは、この区分された5つの領域を、領域〜
領域と呼ぶことにする。
Referring to FIG. 2, the high frequency magnetic field generator 13 according to the present invention has a plurality of coils arranged as shown in the figure to cover the infrared radiation member 20, and arranged close to each other so that their surfaces are parallel to each other. However, the generated high-frequency magnetic field is divided into five elongated regions. Here, these five divided areas are defined as area ~
Let's call it a region.

今、高周波電流発振器11から発生された電流
Iが、第2図aに示されるように、矢印の方向よ
り流れていたとする。このとき、第2図aにおい
て、領域ではその周囲の導線を流れる電流方向
が全て右回り、領域では全て左回り、領域で
は全て右回り、領域では全て左回り、領域で
は全て右回りとなる。従つて、その時発生する磁
界の方向は、第2図aにおいて、領域の内側で
は紙面上方より下方の方向(以下、方向と呼
ぶ。)、領域の内部では紙面下方より上方の方向
(以下、○・方向と呼ぶ。)、領域の内部では方
向、領域の内部では○・方向、領域の内部では
方向となる。即ち、周囲をコイルで囲まれた5
つの領域〜は、各領域の中心位置が互いにず
れており、かつ相隣接した領域の内部を通る磁界
の方向が互いに逆で、各領域の周囲のコイルを流
れる電流方向が全て同一回転方向である。
Now, assume that the current I generated from the high frequency current oscillator 11 is flowing in the direction of the arrow, as shown in FIG. 2a. At this time, in FIG. 2a, the direction of the current flowing through the conductors around the area is all clockwise, all the area is counterclockwise, all the area is clockwise, the area is all counterclockwise, and the area is all clockwise. Therefore, in FIG. 2a, the direction of the magnetic field generated at that time is a direction below the top of the page (hereinafter referred to as the "direction") inside the area, and a direction above the bottom of the page (hereinafter referred to as ○) inside the area. ), inside the area is the direction, inside the area is the ○ direction, and inside the area is the direction. That is, 5 surrounded by coils.
In the two regions, the centers of each region are shifted from each other, the directions of the magnetic fields passing through the interior of adjacent regions are opposite to each other, and the current direction flowing through the coils around each region is all in the same rotation direction. .

又、このとき発生する磁界(磁束)は、第2図
bの点線で示されるように、赤外線放射部材20
の内部と通り、赤外線放射部材20では、電磁誘
導により、その磁束の変化を妨げる向きに誘導電
流が流れ、渦電流損失及びヒステリシス損失のエ
ネルギ損失により加熱される。そして、赤外線放
射部材20は、その加熱された温度に対応した赤
外線を放射し、その近傍にある人体等の被放射体
を暖める。なお、このときの加熱された温度は、
前述したように、約260℃に選ばれる。しかし、
この温度に限定されるものではない。
Also, the magnetic field (magnetic flux) generated at this time is caused by the infrared radiation member 20, as shown by the dotted line in FIG. 2b.
In the infrared radiation member 20, an induced current flows in a direction that prevents changes in the magnetic flux due to electromagnetic induction, and heat is generated due to energy loss due to eddy current loss and hysteresis loss. The infrared radiating member 20 emits infrared rays corresponding to the heated temperature, thereby warming a radiated object such as a human body in the vicinity thereof. The heated temperature at this time is
As mentioned above, the temperature is chosen to be approximately 260°C. but,
It is not limited to this temperature.

第2図に示されるように、赤外線放射部材20
を通過する磁束は、一箇所に集中されることなく
分散されているので、赤外線放射部材20は均一
に加熱され、従来のようなそりの発生を防止でき
る。又、前述ししたように、隣接した領域の内部
を通る磁界の方向が互いに逆で、各領域の周囲の
コイルを流れる電流方向が全て同一回転方向であ
るので、従来のように、磁界が集中したり、互い
に打消すということを防止でき、効率良く磁界を
発生できる。なお、第2図bにおいて、及び○・
は電流の方向を示し、は紙面上方より下方の方
向、○・は紙面下方より上方の方向である。
As shown in FIG. 2, an infrared radiation member 20
Since the magnetic flux passing through the infrared radiation member 20 is dispersed without being concentrated in one place, the infrared radiation member 20 is heated uniformly, and warping as in the conventional case can be prevented. In addition, as mentioned above, the directions of the magnetic fields passing through the interior of adjacent regions are opposite to each other, and the current direction flowing through the coils around each region is all in the same rotational direction, so the magnetic field is not concentrated as in the conventional case. It is possible to prevent magnetic fields from causing or canceling each other out, and it is possible to efficiently generate a magnetic field. In addition, in Fig. 2 b, and ○・
indicates the direction of the current, ◯ indicates the direction below the top of the paper, and ◯ indicates the direction above the bottom of the paper.

第3図は本考案による高周波誘導加熱装置の高
周波磁界発生器と赤外線放射部材の配置関係の他
の一実施例を示した正面図である。本実施例で
は、高周波磁界発生器13より発生される高周波
磁界が、3×7=21の領域に区分されている。こ
の実施例の場合も、高周波磁界発生器13は、赤
外線放射部材20を覆い、互いの面が平行になる
ように近接して配置されている。更に、本実施例
の場合も、コイルで囲まれた各領域の中心位置が
互いにずれており、かつ互いに隣接した領域の内
部を通る磁界の方向が互いに逆で、各領域の周囲
のコイルを流れる電流方向が全て同一回転方向と
なつている。従つて、第2図における実施例と同
様の効果を有することは明らかである。
FIG. 3 is a front view showing another embodiment of the arrangement relationship between the high frequency magnetic field generator and the infrared radiation member of the high frequency induction heating device according to the present invention. In this embodiment, the high frequency magnetic field generated by the high frequency magnetic field generator 13 is divided into 3×7=21 regions. In this embodiment as well, the high frequency magnetic field generator 13 covers the infrared radiation member 20 and is disposed close to each other so that their surfaces are parallel to each other. Furthermore, in the case of this embodiment as well, the center positions of the regions surrounded by the coils are shifted from each other, and the directions of the magnetic fields passing through the interiors of adjacent regions are opposite to each other, and the magnetic fields flow through the coils around each region. All current directions are the same direction of rotation. Therefore, it is clear that this embodiment has the same effect as the embodiment shown in FIG.

なお、区分された領域の周囲のコイルの巻数
は、任意で適当に選択される。
Note that the number of turns of the coil around the divided area is arbitrarily and appropriately selected.

更に、上述した実施例は、全て1本の導線のみ
を使用しているが、各領域或いは複数領域を一組
みとして、複数の導線を使用して良いのは勿論で
ある。
Furthermore, although all of the embodiments described above use only one conductive wire, it goes without saying that a plurality of conductive wires may be used for each area or for a set of multiple areas.

又、上述した実施例では、赤外線放射部材が高
周波磁界発生器の片方の面側のみに設けられてい
るが、赤外線放射部材は、高周波磁界発生器の両
方の面に設けても良いのは勿論である。更に、赤
外線放射部材及び高周波磁界発生器は、平面状の
形に限定されず、例えば球面等他の形状でも良
い。
Further, in the above-described embodiment, the infrared radiation member is provided on only one side of the high frequency magnetic field generator, but it is of course possible to provide the infrared radiation member on both sides of the high frequency magnetic field generator. It is. Furthermore, the infrared radiation member and the high frequency magnetic field generator are not limited to a planar shape, but may have other shapes such as a spherical surface.

〔考案の効果〕[Effect of idea]

以上の説明で明らかなように、本考案によれ
ば、赤外線放射手段を覆う高周波磁界発生手段と
して、発生する高周波磁界の方向が互いに逆方向
の少なくとも2つの領域に区分し、相隣接した区
分領域の内部より発生する高周波磁界の方向が互
いに逆で、かつ区分領域の周囲を流れる高周波電
流の方向が全て同一回転方向となるように、複数
のコイルを配置したので、加熱される赤外線放射
手段は均一に加熱され、そりの発生を防止できる
と共に、効率良く高周波磁界を発生させることが
できる利点を有する。
As is clear from the above description, according to the present invention, the high-frequency magnetic field generating means covering the infrared ray emitting means is divided into at least two regions in which the directions of the generated high-frequency magnetic fields are opposite to each other, and the divided regions are adjacent to each other. The plurality of coils are arranged so that the directions of the high-frequency magnetic fields generated from inside the section are opposite to each other, and the directions of the high-frequency currents flowing around the divided areas are all in the same rotational direction. It has the advantage that it can be heated uniformly, prevent warping, and efficiently generate a high-frequency magnetic field.

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

第1図は本考案による電気暖房器に使用される
高周波誘導加熱装置の一実施例の構成を示したブ
ロツク図、第2図は第1図に示した高周波誘導加
熱装置の高周波磁界発生器と赤外線放射部材の配
置関係を示した図、第3図は本考案による高周波
誘導加熱装置の高周波磁界発生器と赤外線放射部
材の配置関係の他の一実施例を示した正面図、第
4図は従来の電気暖房器を使用されていた高周波
誘導加熱装置の構成を示したブロツク図、第5図
は第4図に示した高周波誘導加熱装置の高周波磁
界発生器と赤外線放射部材の配置関係を示した
図、第6図は温度をパラメータとしたときの波長
に対する放射エネルギ密度の関係の一例を示した
図である。 10……高周波誘導加熱装置、13……高周波
磁界発生器、20……赤外線放射部材。
Fig. 1 is a block diagram showing the configuration of an embodiment of the high frequency induction heating device used in an electric heater according to the present invention, and Fig. 2 shows the high frequency magnetic field generator of the high frequency induction heating device shown in Fig. 1. FIG. 3 is a front view showing another embodiment of the arrangement relationship between the high frequency magnetic field generator and the infrared radiation member of the high frequency induction heating device according to the present invention, and FIG. 4 is a diagram showing the arrangement relationship of the infrared radiation member. A block diagram showing the configuration of a high-frequency induction heating device that uses a conventional electric heater, and FIG. 5 shows the arrangement relationship between the high-frequency magnetic field generator and the infrared radiation member of the high-frequency induction heating device shown in FIG. FIG. 6 is a diagram showing an example of the relationship between radiant energy density and wavelength when temperature is used as a parameter. 10... High frequency induction heating device, 13... High frequency magnetic field generator, 20... Infrared radiation member.

Claims (1)

【実用新案登録請求の範囲】[Scope of utility model registration request] 高周波電流発生手段と、該高周波電流発生手段
から発生される高周波電流により高周波磁界を発
生する高周波磁界発生手段と、該高周波磁界発生
手段から発生される高周波磁界による電磁誘導作
用により生ずるエネルギ損失で加熱され、該加熱
温度に対応した赤外線を放射する放射手段とを有
して成る電気暖房器において、前記高周波磁界発
生手段は、発生する高周波磁界の方向が互いに逆
方向の少なくとも2つの領域に区分され、相隣接
した前記区分領域の内部より発生する高周波磁界
の方向が互いに逆で、かつ該区分領域の周囲を流
れる前記高周波電流の方向が全て同一回転方向と
なるように、複数のコイルが前記放射手段を覆う
如く配置されていることを特徴とする電気暖房
器。
A high-frequency current generating means, a high-frequency magnetic field generating means for generating a high-frequency magnetic field by the high-frequency current generated by the high-frequency current generating means, and heating due to energy loss caused by the electromagnetic induction effect of the high-frequency magnetic field generated from the high-frequency magnetic field generating means. and a radiation means for emitting infrared rays corresponding to the heating temperature, wherein the high frequency magnetic field generating means is divided into at least two regions in which the directions of the generated high frequency magnetic fields are opposite to each other. , a plurality of coils rotate the radiation so that the directions of high-frequency magnetic fields generated from inside the adjacent divided regions are opposite to each other, and the directions of the high-frequency currents flowing around the divided regions are all in the same rotational direction. An electric heater characterized by being arranged so as to cover the means.
JP2126885U 1985-02-19 1985-02-19 Expired JPS636876Y2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP2126885U JPS636876Y2 (en) 1985-02-19 1985-02-19

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP2126885U JPS636876Y2 (en) 1985-02-19 1985-02-19

Publications (2)

Publication Number Publication Date
JPS61138187U JPS61138187U (en) 1986-08-27
JPS636876Y2 true JPS636876Y2 (en) 1988-02-26

Family

ID=30512512

Family Applications (1)

Application Number Title Priority Date Filing Date
JP2126885U Expired JPS636876Y2 (en) 1985-02-19 1985-02-19

Country Status (1)

Country Link
JP (1) JPS636876Y2 (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP5117992B2 (en) * 2008-10-23 2013-01-16 株式会社ダイヘン Heating coil unit of electromagnetic induction heating cooker

Also Published As

Publication number Publication date
JPS61138187U (en) 1986-08-27

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