JPH07217835A - Electromagnetic wave heater - Google Patents
Electromagnetic wave heaterInfo
- Publication number
- JPH07217835A JPH07217835A JP902994A JP902994A JPH07217835A JP H07217835 A JPH07217835 A JP H07217835A JP 902994 A JP902994 A JP 902994A JP 902994 A JP902994 A JP 902994A JP H07217835 A JPH07217835 A JP H07217835A
- Authority
- JP
- Japan
- Prior art keywords
- waveguide
- electromagnetic wave
- container
- shape
- wedge
- 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.)
- Granted
Links
Landscapes
- Constitution Of High-Frequency Heating (AREA)
- Gasification And Melting Of Waste (AREA)
- Drying Of Solid Materials (AREA)
Abstract
Description
【0001】[0001]
【産業上の利用分野】本発明は、マイクロ波を含む電磁
波を用いて物体を加熱させる場合の加熱装置の構成に関
するものである。特に生ものやプラスチック等の産業廃
棄物の焼却または乾燥に適している。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a heating device for heating an object using electromagnetic waves including microwaves. It is particularly suitable for incineration or drying of raw materials and industrial waste such as plastics.
【0002】[0002]
【従来の技術】マイクロ波を用いた加熱装置は産業用を
はじめ家庭用の電子レンジなどで既に広く使用されてい
る。水等の誘電損失の大きい物質がマイクロ波にさらさ
れると誘電損失の大きさに比例した発熱を起こすことを
利用して物質を暖めるものである。加熱装置の多く(例
えば文献:「日経ニューマテリアル1992年3月30
日号、87頁)は図6に示すように、アプリケータ7内
にターンテーブル8をおき、その上に加熱対象物を乗せ
て回転させる。マイクロ波をアプリケータ7内に天井面
または横の壁面から放出して対象物全体を均一に加熱で
きるように工夫している。ところがこの場合、アプリケ
ータ7内の金属壁面にマイクロ波を不規則に反射させて
対象物に照射させるため、マイクロ波は充分に対象物に
吸収されずに多くは反射してしまう。対象物の形状、大
きさにも依るがおよそマイクロ波出力の約半分程度しか
加熱に寄与していないのが現状である。2. Description of the Related Art A heating device using microwaves is already widely used in industrial and domestic microwave ovens. When a substance having a large dielectric loss, such as water, is exposed to microwaves, heat is generated in proportion to the magnitude of the dielectric loss, thereby heating the substance. Many heating devices (for example, reference: “Nikkei New Material March 30, 1992)
As shown in FIG. 6, a turntable 8 is placed in the applicator 7, and an object to be heated is placed thereon and rotated. The device is devised so that the microwave can be emitted into the applicator 7 from the ceiling surface or the lateral wall surface to uniformly heat the entire object. However, in this case, since the microwave is irregularly reflected on the metal wall surface in the applicator 7 to irradiate the object, the microwave is not sufficiently absorbed by the object and is largely reflected. At present, only about half of the microwave output contributes to heating, depending on the shape and size of the object.
【0003】効率の良い加熱をするために、アプリケー
タ7全体を共振器のように設計して、アプリケータ7に
最大限のマイクロ波出力を導入できるように工夫したも
のが図7である(文献:特公昭56−54548号公
報)。この場合は対象物の蓋や温度変化で誘電率が大き
く変化する。そこで、図7の中に示されているインピー
ダンス調整器9で共振状態を常に最適に合わせて対象物
の誘電率の変化に追従させている。FIG. 7 shows a device in which the entire applicator 7 is designed like a resonator in order to efficiently heat the device, and is devised so that the maximum microwave output can be introduced into the applicator 7 ( Reference: Japanese Patent Publication No. 56-54548). In this case, the permittivity changes greatly depending on the lid of the object and the temperature change. Therefore, the impedance adjuster 9 shown in FIG. 7 always adjusts the resonance state to the optimum state to follow the change of the dielectric constant of the object.
【0004】[0004]
【発明が解決しようとする課題】このような共振型のシ
ステムでは、マイクロ波を送り込む導波管の途中にパワ
ーモニタを導入して入射波と反射波をモニターし、反射
波が常に最低になるように調節棒をチューニングしなけ
ればならない。このためパワーモニタ及び調整用の可動
部とそれを制御するフィードバック系を加える必要があ
り、システムが高価になるという欠点があった。In such a resonance type system, a power monitor is introduced in the middle of a waveguide for feeding a microwave to monitor an incident wave and a reflected wave, and the reflected wave is always minimized. You have to tune the adjusting rod like so. For this reason, it is necessary to add a power monitor and a movable part for adjustment and a feedback system for controlling the movable part, which has a drawback that the system becomes expensive.
【0005】本発明は、簡単な構成で広い誘電率の範囲
で効率の良い加熱が可能な電磁波加熱装置を提供するこ
とにある。An object of the present invention is to provide an electromagnetic wave heating device having a simple structure and capable of efficiently heating in a wide dielectric constant range.
【0006】[0006]
【課題を解決するための手段】本発明の電磁波加熱装置
は、電磁波発生装置と、電磁波を誘導する導波路と、加
熱対象物を入れる容器を有し、前記容器は非磁性、低誘
電損失で、かつ凸な形状であり、前記導波路の中に位置
し、容器の凸の方向が電磁波の方向に対向して配置され
ていることを特徴とする。An electromagnetic wave heating device of the present invention has an electromagnetic wave generator, a waveguide for guiding electromagnetic waves, and a container for containing an object to be heated, said container being non-magnetic and having a low dielectric loss. , And has a convex shape, and is located in the waveguide, and the container is arranged so that the direction of the convex of the container faces the direction of the electromagnetic wave.
【0007】または容器の形状は、円錐型または角錘型
または楔型またはおわん型であることを特徴とする。Alternatively, the shape of the container is conical, pyramidal, wedge-shaped, or bowl-shaped.
【0008】または導波路がテーパ型であることを特徴
とする。Alternatively, the waveguide is tapered.
【0009】または導波路または容器に、開口部を有し
かつ電磁波を遮蔽する蓋があることを特徴とする。Alternatively, the waveguide or the container is provided with a lid having an opening and shielding electromagnetic waves.
【0010】または導波路の中に複数の凸の形状の容器
が設置されていることを特徴とする。Alternatively, a plurality of convex-shaped containers are installed in the waveguide.
【0011】または電磁波発生装置と、電磁波を誘導す
る導波路と、加熱対象物を入れる容器と、前記導波路の
蓋を有し、前記導波路の蓋は長辺が加熱する電磁波の波
長の2分の1以下の矩形導波管の長辺の面に棒状のフェ
ライトを長辺に平行に装着したことを特徴とする。この
フェライトにより、その面のみが開放壁となっている。Alternatively, it has an electromagnetic wave generator, a waveguide for guiding the electromagnetic wave, a container for containing an object to be heated, and a lid for the waveguide, and the lid of the waveguide has a long side of the wavelength of the electromagnetic wave for heating. It is characterized in that rod-shaped ferrite is mounted parallel to the long side on the surface of the long side of the rectangular waveguide of one-half or less. Due to this ferrite, only that surface is an open wall.
【0012】[0012]
【実施例】次に、本発明について図面を参照して説明す
る。図1(a)は本発明の一実施例を示す電磁波加熱装
置の構成図である。マイクロ波発生装置1のマグネトロ
ンから導波路2にマイクロ波が導かれる。導波路2は縦
型に配置し、下から上にマイクロ波出力が導かれる。導
波路2の途中に下向きに樹脂性の楔型容器3が置かれ、
その中に加熱対象物4が入れられている。装置の蓋は導
波路の端に取り付けられており、開口部があり気体は抜
けるがマイクロ波は漏れないような電磁遮蔽構造のもの
とし、ここでは穴径の小さなパンチングメタル5を使用
している。図1(b)は蓋の遮蔽構造の構成を変えたも
ので他は同じである。即ち、上述の電磁遮蔽構造の蓋を
楔型容器に取り付けたものである。DESCRIPTION OF THE PREFERRED EMBODIMENTS Next, the present invention will be described with reference to the drawings. FIG. 1A is a configuration diagram of an electromagnetic wave heating apparatus showing an embodiment of the present invention. Microwaves are guided from the magnetron of the microwave generator 1 to the waveguide 2. The waveguide 2 is arranged vertically, and the microwave output is guided from the bottom to the top. A resinous wedge-shaped container 3 is placed downward in the middle of the waveguide 2,
The object to be heated 4 is placed therein. The lid of the device is attached to the end of the waveguide and has an electromagnetic shield structure with an opening so that gas can escape but microwave does not leak. Here, punching metal 5 with a small hole diameter is used. . FIG. 1 (b) is the same as the other one except that the structure of the cover shielding structure is changed. That is, the lid of the above-mentioned electromagnetic shielding structure is attached to the wedge-shaped container.
【0013】本発明の特徴は、加熱容器に樹脂やガラス
などの低誘電損失材質で且つ楔型のものを使用している
ことである。楔型容器3の中に誘電損失の大きな加熱対
象物4として水を入れると、水の形状が楔型になる。楔
型の損失体は実質的に楔の先端方向から進行してきたマ
イクロ波を良く吸収する。これは電波暗室などで用いる
電波吸収体も同様の形状をしていることからも明らかで
ある。A feature of the present invention is that the heating container is made of a low dielectric loss material such as resin or glass and has a wedge shape. When water is put into the wedge-shaped container 3 as the heating object 4 having a large dielectric loss, the shape of the water becomes wedge-shaped. The wedge-shaped loss body substantially absorbs the microwave traveling from the tip end direction of the wedge. This is also clear from the fact that the electromagnetic wave absorber used in an anechoic chamber has a similar shape.
【0014】さらに、もう1つの構成上の特徴は楔型容
器3が導波路2の途中に置かれていることである。具体
的には、導波路2を縦向きに配置し、マイクロ波が下か
ら上に進行するようにする。さらに、楔型容器3の先端
を下に向けると、中身の加熱対象物4がこぼれず、ま
た、自然と容器の楔型にならって加熱対象物4が楔状に
なり、その先端をマイクロ波の進行方向に対向させるこ
とができ、かつ、マイクロ波を楔の先端方向に平行に照
射することができる。このため、効率よく電磁波の吸収
がなされる。従来の電子レンジ等のアプリケータ内に楔
型容器を下向きに配置しても楔の角の方向から入射する
マイクロ波の成分以外は楔型容器に効率的には吸収され
ない。効率よく加熱させるためには楔型が導波路2の途
中になければならない。Further, another structural feature is that the wedge-shaped container 3 is placed in the middle of the waveguide 2. Specifically, the waveguide 2 is arranged vertically so that microwaves travel from bottom to top. Furthermore, when the tip of the wedge-shaped container 3 is directed downward, the heating object 4 inside does not spill, and the heating object 4 naturally becomes a wedge shape of the container, and the heating object 4 becomes a wedge shape, and the tip of the microwave-shaped object 3 is heated. The microwaves can be opposed to each other in the traveling direction, and the microwaves can be irradiated in parallel with the tip direction of the wedge. Therefore, electromagnetic waves are efficiently absorbed. Even if the wedge-shaped container is arranged downward in an applicator such as a conventional microwave oven, the components other than the microwave components incident from the direction of the angle of the wedge are not efficiently absorbed by the wedge-shaped container. In order to heat efficiently, a wedge shape must be in the middle of the waveguide 2.
【0015】ここでは、分かりやすくするため、楔型容
器3を用いて本発明を説明したが、円錐型、角錘、おわ
ん型の各容器の場合も、程度の差はあるが同様の効率を
期待することができる。つまり、前記と同様下から上に
マイクロ波が進行するような導波路の途中に円錐、角錘
およびおわん型容器の先端をマイクロ波に対向するよう
に下向きに配置し、容器の中に加熱対象物を入れて加熱
することによって効率よい加熱を実現できる。先に述べ
たように、従来型電子レンジなどのように様々な方向か
ら電磁波が照射されるアプリケータ内に円錐、角錘、お
わん型容器を置く場合と本質的に異なることは言うまで
もない。Although the present invention has been described here by using the wedge-shaped container 3 for the sake of clarity, the same efficiency can be obtained in the case of each of the conical, pyramidal, and bowl-shaped containers, although the degree is different. Can be expected. That is, similar to the above, the cone, the pyramid, and the tip of the bowl-shaped container are arranged downward so as to face the microwave in the middle of the waveguide in which the microwave propagates from bottom to top, and the heating target is placed in the container. Efficient heating can be realized by putting and heating an object. As described above, it goes without saying that this is essentially different from the case where a cone, a pyramid, or a bowl-shaped container is placed in an applicator that is irradiated with electromagnetic waves from various directions, such as a conventional microwave oven.
【0016】また、説明では、楔型容器を1つ用いた場
合を示したが、大容量で加熱させたい場合等、導波路と
容器を大きくする際には次のようにすればよい。導波路
を拡大する場合は図2(a)に示すように、よく設計さ
れたテーパ型導波管などを用いて導波路の繋ぎ目で反射
をできるだけ押さえる。そして、大きな楔型容器3をテ
ーパの先に置く。または、図2(b)に示すように、テ
ーパ型導波管に楔型やその他前述の形の凸形の複数の容
器を配置すればよい。In the description, the case where one wedge-shaped container is used is shown. However, when the waveguide and the container are enlarged, such as when heating with a large capacity, the following may be done. When the waveguide is enlarged, as shown in FIG. 2A, a well-designed tapered waveguide or the like is used to suppress reflection at the joint of the waveguides as much as possible. Then, the large wedge-shaped container 3 is placed at the tip of the taper. Alternatively, as shown in FIG. 2B, a plurality of wedge-shaped or other convex containers of the above-described shape may be arranged in the tapered waveguide.
【0017】本発明の効果を示すため、楔型と、4角錘
(ピラミッド型)の高さ15cmの場合について電波吸収
量を計算した結果を図3(a)及び(b)に示す。ε′
とε″は誘電率の実部と虚部である。図中で10dBの
吸収量は照射したマイクロ波の1/10が反射する。つ
まり、残り90%が吸収されることを示している。20
dBの場合では1/100、つまり、99%の吸収効率
になることを示している。楔型よりピラミッド型の方が
同じ誘電率では吸収量が大きく、また、同じ吸収量では
より広い誘電率の範囲の対象物を暖めることができるこ
とが分かる。In order to show the effect of the present invention, the calculation results of the electromagnetic wave absorption amount in the case of a wedge type and a quadrangular pyramid (pyramid type) having a height of 15 cm are shown in FIGS. 3 (a) and 3 (b). ε ′
And ε ″ are the real part and the imaginary part of the dielectric constant. In the figure, the absorption amount of 10 dB reflects 1/10 of the irradiated microwave, that is, the remaining 90% is absorbed. 20
In the case of dB, it is shown that the absorption efficiency is 1/100, that is, 99%. It can be seen that the pyramid type has a larger absorption amount with the same permittivity than the wedge type, and the same absorption amount can warm an object in a wider permittivity range.
【0018】蓋の構造としては、先に述べたように気体
は通すが電磁波は通さない電磁遮蔽構造のものとして、
パンチングメタルを使用した例を示したが、このほか、
図4(a)に示すように遮断モードの導波管を用いるこ
ともできる。本発明の蓋の構造は、図4(b)に示すよ
うに、長辺が加熱する電磁波の波長の2分の1以下の矩
形導波管を有する蓋で、その導波管の長辺の面に磁性体
であるフェライトを棒状にして長辺に平行に装着してそ
の面のみを開放壁にしたものである。これにより、導波
管の長さを大幅に短くすることができる。これは、導波
管の長辺を含む壁に磁性体棒を配列すると、この壁は透
磁率が大きいほど開放壁に近い特性を有することが理論
的に導かれており、また、矩形導波管の断面の長辺をa
とし短辺をbとすると、図4(a)の場合の減衰常数が
π/aであるのに対し、図4(b)のように長辺を含む
一つの面を開放壁にした場合の減衰常数は{(π/a)
2+(π/b)2}1/2 であり、その差の分だけ減衰常
数を大きくできるからである。加熱装置の周波数が2.
45GHzであるならば、磁性体はフェライトが適当で
あり、フェライト棒の直径は1mm程度で十分であるの
で、実質的に排気の妨げにはならない。The structure of the lid is, as described above, an electromagnetic shielding structure that allows gas to pass but does not allow electromagnetic waves to pass.
I showed an example using punching metal, but in addition to this,
It is also possible to use a cut-off mode waveguide as shown in FIG. The structure of the lid of the present invention is, as shown in FIG. 4 (b), a lid having a rectangular waveguide whose long side is equal to or less than ½ of the wavelength of the electromagnetic wave to be heated. The surface is an open wall in which ferrite, which is a magnetic material, is formed into a rod shape and mounted parallel to the long side. This can significantly reduce the length of the waveguide. It is theoretically derived that when magnetic rods are arranged on the wall including the long side of the waveguide, the wall has a characteristic closer to an open wall as the magnetic permeability increases, and the rectangular waveguide is used. The long side of the cross section of the pipe is a
Letting b be the short side, the damping constant in the case of FIG. 4 (a) is π / a, whereas one side including the long side is an open wall as shown in FIG. 4 (b). The damping constant is {(π / a)
2+ (π / b) 2} 1/2 , and the damping constant can be increased by the difference. The frequency of the heating device is 2.
If the frequency is 45 GHz, ferrite is suitable as the magnetic material, and the diameter of the ferrite rod is about 1 mm, so that it does not substantially hinder the exhaust.
【0019】この電磁遮蔽構造の蓋として、遮断モード
の導波管の長さを図4の(a)と(b)で比較する。長
辺55mm、短辺27.5mmの矩形導波管の場合、その長
さLと遮蔽量の関係は図5に示すようになっている。実
用上十分な遮蔽量である90dBを得るのに、比較のた
めの図4(a)に示す構造のものでは20cmの長さが必
要であるのに対して、本発明の図4(b)に示す構造の
ものでは10cm以下で十分であり、導波管をおよそ1/
2以下に短縮することができ、装置の小型化が可能にな
る。As the lid of this electromagnetic shielding structure, the lengths of the waveguides in the cutoff mode are compared in FIGS. 4 (a) and 4 (b). In the case of a rectangular waveguide having a long side of 55 mm and a short side of 27.5 mm, the relationship between the length L and the shielding amount is as shown in FIG. In order to obtain a practically sufficient shield amount of 90 dB, the structure shown in FIG. 4 (a) for comparison requires a length of 20 cm, whereas FIG. 4 (b) of the present invention. With the structure shown in Fig. 10, 10 cm or less is sufficient, and
It can be shortened to 2 or less, and the device can be downsized.
【0020】[0020]
【発明の効果】本発明の電磁波加熱装置を用いることに
よって簡単な構成で且つ水を含む物質などの広い誘電率
の範囲の加熱対象物を効率よく加熱できる。加熱時にガ
スの発生または状態の変化により誘電率が変わりやすい
物質の加熱や溶解に適している。また装置の小型化が可
能となる。By using the electromagnetic wave heating device of the present invention, it is possible to efficiently heat an object to be heated having a wide dielectric constant range such as a substance containing water with a simple structure. It is suitable for heating or melting substances whose permittivity is likely to change due to the generation of gas or changes in state during heating. Further, the device can be downsized.
【0021】さらに、生ものやプラスチック等の産業廃
棄物の焼却または乾燥に適している。また高融点の物質
の溶解にも適しており、この場合は容器を非磁性、低誘
電損失のセラミックで作製すればよい。Further, it is suitable for incineration or drying of raw materials and industrial waste such as plastics. It is also suitable for melting a substance having a high melting point. In this case, the container may be made of a non-magnetic, low dielectric loss ceramic.
【図1】本発明の一実施例を示す電磁波加熱装置の構成
を示した図である。FIG. 1 is a diagram showing a configuration of an electromagnetic wave heating apparatus showing an embodiment of the present invention.
【図2】本発明の他の実施例を示した図である。FIG. 2 is a diagram showing another embodiment of the present invention.
【図3】(a)は楔型容器(高さ10cm)の場合の加熱
対象物の誘電率と電波吸収効率の関係を示した図、
(b)はピラミッド型容器(高さ10cm)の場合の同様
の関係を示した図である。FIG. 3A is a diagram showing a relationship between a dielectric constant of a heating target and a radio wave absorption efficiency in the case of a wedge-shaped container (height 10 cm);
(B) is a figure showing the same relationship in the case of a pyramid type container (height 10 cm).
【図4】本発明の電磁遮蔽構造のための蓋を説明するた
めの図である。(a)は比較のための図であり、(b)
は本発明を説明するための図である。FIG. 4 is a view for explaining a lid for the electromagnetic shield structure of the present invention. (A) is a diagram for comparison, (b)
FIG. 4 is a diagram for explaining the present invention.
【図5】本発明を説明するための図で、遮蔽量と辺の長
さの関係を示す図である。FIG. 5 is a diagram for explaining the present invention and is a diagram showing a relationship between a shielding amount and a side length.
【図6】従来の電子レンジの構造を示した図である。FIG. 6 is a diagram showing a structure of a conventional microwave oven.
【図7】従来の共振型アプリケータの構造を示した図で
ある。FIG. 7 is a view showing a structure of a conventional resonance type applicator.
1 電磁波発生装置 2 導波路 3 楔型容器 4 加熱対象物 5 パンチングメタル 6 テーパ型導波路 7 アプリケータ 8 ターンテーブル 9 インピーダンス調整器 1 Electromagnetic Wave Generator 2 Waveguide 3 Wedge Type Container 4 Heating Object 5 Punching Metal 6 Tapered Waveguide 7 Applicator 8 Turntable 9 Impedance Adjuster
フロントページの続き (51)Int.Cl.6 識別記号 庁内整理番号 FI 技術表示箇所 H05B 6/80 Z Continuation of front page (51) Int.Cl. 6 Identification number Office reference number FI technical display area H05B 6/80 Z
Claims (7)
路と、加熱対象物を入れる容器を有し、前記容器は非磁
性、低誘電損失で、かつ凸な形状であり、前記導波路の
中に位置し、容器の凸の方向が電磁波の方向に対向して
配置されていることを特徴とする電磁波加熱装置。1. An electromagnetic wave generator, a waveguide for inducing an electromagnetic wave, and a container for containing an object to be heated, the container having a non-magnetic, low dielectric loss, and convex shape. An electromagnetic wave heating device, characterized in that it is positioned inside and the convex direction of the container is arranged to face the electromagnetic wave direction.
たは楔型またはおわん型であることを特徴とする請求項
1記載の電磁波加熱装置。2. The electromagnetic wave heating device according to claim 1, wherein the container has a conical shape, a pyramidal shape, a wedge shape, or a bowl shape.
する請求項1記載の電磁波加熱装置。3. The electromagnetic wave heating device according to claim 1, wherein the waveguide is tapered.
しかつ電磁波を遮蔽する蓋があることを特徴とする請求
項1または請求項2または請求項3記載の電磁波加熱装
置。4. The electromagnetic wave heating device according to claim 1, wherein the waveguide or the container has a lid which has an opening and shields electromagnetic waves.
設置されていることを特徴とする請求項1または請求項
2または請求項3または請求項4記載の電磁波加熱装
置。5. The electromagnetic wave heating device according to claim 1, wherein a plurality of convex-shaped containers are installed in the waveguide.
路と、加熱対象物を入れる容器と、前記導波路の蓋を有
し、前記導波路の蓋は長辺が加熱する電磁波の波長の2
分の1以下の矩形導波管の長辺の面に棒状の磁性体を長
辺に平行に装着したことを特徴とする電磁波加熱装置。6. An electromagnetic wave generator, a waveguide for inducing electromagnetic waves, a container for containing an object to be heated, and a lid for the waveguide, the long side of the waveguide having a wavelength of the electromagnetic wave for heating. Two
An electromagnetic wave heating device, characterized in that a rod-shaped magnetic body is mounted parallel to the long side on the surface of the long side of a rectangular waveguide of one-tenth or less.
長の2分の1以下の矩形導波管の長辺の面に棒状の磁性
体を長辺に平行に装着した蓋を有することを特徴とする
請求項1記載の電磁波加熱装置。7. The waveguide has a lid in which a rod-shaped magnetic body is mounted parallel to the long side on the surface of the long side of a rectangular waveguide whose long side is one-half or less of the wavelength of an electromagnetic wave to be heated. The electromagnetic wave heating device according to claim 1, wherein:
Priority Applications (2)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP6009029A JP2746095B2 (en) | 1994-01-31 | 1994-01-31 | Electromagnetic wave heating device and electromagnetic wave heating method |
| US08/381,444 US5523548A (en) | 1994-01-31 | 1995-01-31 | Electromagnetic wave heater having a cone-shaped container whose tapered portion is pointed and directed toward the electromagnetic wave generator |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP6009029A JP2746095B2 (en) | 1994-01-31 | 1994-01-31 | Electromagnetic wave heating device and electromagnetic wave heating method |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH07217835A true JPH07217835A (en) | 1995-08-18 |
| JP2746095B2 JP2746095B2 (en) | 1998-04-28 |
Family
ID=11709236
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP6009029A Expired - Lifetime JP2746095B2 (en) | 1994-01-31 | 1994-01-31 | Electromagnetic wave heating device and electromagnetic wave heating method |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JP2746095B2 (en) |
Citations (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS5415138A (en) * | 1977-07-06 | 1979-02-03 | Mitsubishi Electric Corp | Electric feeding device |
| JPH0259596U (en) * | 1988-10-24 | 1990-05-01 |
-
1994
- 1994-01-31 JP JP6009029A patent/JP2746095B2/en not_active Expired - Lifetime
Patent Citations (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS5415138A (en) * | 1977-07-06 | 1979-02-03 | Mitsubishi Electric Corp | Electric feeding device |
| JPH0259596U (en) * | 1988-10-24 | 1990-05-01 |
Also Published As
| Publication number | Publication date |
|---|---|
| JP2746095B2 (en) | 1998-04-28 |
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