JPH02155194A - Microwave oven - Google Patents

Microwave oven

Info

Publication number
JPH02155194A
JPH02155194A JP31036088A JP31036088A JPH02155194A JP H02155194 A JPH02155194 A JP H02155194A JP 31036088 A JP31036088 A JP 31036088A JP 31036088 A JP31036088 A JP 31036088A JP H02155194 A JPH02155194 A JP H02155194A
Authority
JP
Japan
Prior art keywords
conductor
heating chamber
plate
radiation
pierce
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
Application number
JP31036088A
Other languages
Japanese (ja)
Other versions
JP2736793B2 (en
Inventor
Kazuo Kaneko
一男 金子
Yasushi Iwabuchi
岩淵 康司
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.)
Hitachi Heating Appliances Co Ltd
Original Assignee
Hitachi Heating Appliances 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 Hitachi Heating Appliances Co Ltd filed Critical Hitachi Heating Appliances Co Ltd
Priority to JP31036088A priority Critical patent/JP2736793B2/en
Publication of JPH02155194A publication Critical patent/JPH02155194A/en
Application granted granted Critical
Publication of JP2736793B2 publication Critical patent/JP2736793B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

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  • Constitution Of High-Frequency Heating (AREA)

Abstract

PURPOSE:To efficiently use space of a microwave oven and easily clean it by utilizing radiation of radiating elements for a flat antenna from an edge of a flat conductor placed parallel to an earth plane. CONSTITUTION:A dielectric plate 10 is fixed as sandwiched between a wall face 1 of a heating chamber and a radiation plate 11 made of almost a metal plate in which length L of one leg thereof is about a half wave length of the used frequency. Drilled on the wall face 1 of the heating chamber is a throughhole 23 whose diameter is equal to an inner diameter of an outer conductor 8. A pierce conductor (an inner conductor) 9 is made to pierce in the center of the throughhole 23 and also is made to pierce in the dielectric plate 10. Then, the pierce conductor 9 is fixed to the radiation plate 11 by a fixing screw 12 to electrically connected thereto. Microwave produced by a magnetron 3 is introduced by a coaxial line composed of the outer and the inner conductors 8 and 9 and radiated into a heating chamber 2 by the dielectric plate 10 and the radiation plate 11 to heat food 5 to be heated. Since, there is no protrusion, space of a microwave oven is efficiently used and the microwave oven is easily cleaned.

Description

【発明の詳細な説明】 産業上の利用分野 本発明は加熱室に収納した食品にマイクロ波を照射して
加熱する高周波加熱装置に係り、特にマグネトロンで発
生したマイクロ波を加熱室内に照射する給電装置に関す
るものである。
[Detailed Description of the Invention] Industrial Application Field The present invention relates to a high-frequency heating device that heats food stored in a heating chamber by irradiating microwaves, and particularly relates to a power supply device that irradiates microwaves generated by a magnetron into the heating chamber. It is related to the device.

従来の技術 高周波加熱装置に割当てられている周波数帯の一つであ
る915MIIzの発振源を用いた従来の給電装置は、
特公昭63−40035号公報に記載のように給電用ア
ンテナが加熱室内に突き出た形となっていた。
Conventional technology A conventional power supply device using an oscillation source of 915MIIz, which is one of the frequency bands assigned to high-frequency heating devices,
As described in Japanese Patent Publication No. 63-40035, the feeding antenna was shaped to protrude into the heating chamber.

発明が解決しようとする課題 この場合、アンテナが突き出た分だけ被加熱食品を収納
するスペース効率が低下すると共に、加熱室内を清掃す
るに際して、アンテナがじゃまになって清掃しにくいと
いう不便があった。
Problems to be Solved by the Invention In this case, there was an inconvenience in that the space efficiency for storing the heated food decreased due to the protruding antenna, and it was difficult to clean the inside of the heating chamber because the antenna got in the way. .

課題を解決するための手段 本発明の目的は高周波加熱装置の給電装置を改良するこ
とにより、スペース効率の向上と、清掃のし易い高周波
加熱装置を提供することにある。
Means for Solving the Problems An object of the present invention is to provide a high-frequency heating device that improves space efficiency and is easy to clean by improving the power supply device of the high-frequency heating device.

上記目的は平面アンテナの放射素子を応用することによ
り達成される。
The above object is achieved by applying a radiating element of a planar antenna.

作用 平面アンテナ用の放射素子はアース平面(この場合は加
熱室壁面)と平行に置かれた平面導体の縁部からの放射
を利用する。そこで突起部分がなく、スペース効率と清
掃性を向上させることができる。
The radiating element for a working planar antenna utilizes radiation from the edge of a planar conductor placed parallel to the earth plane (in this case the heating chamber wall). Therefore, there are no protruding parts, which improves space efficiency and cleaning efficiency.

実施例 以下、本発明の一実施例の構成及び作用を第1図〜第5
図により説明する。第1図において、マグネトロン3で
発生したマイクロ波は外導体8゜内導体9によって構成
される同軸線路によって導かれ、誘電体板10と金属板
(以下放射板と言う)11によって加熱室2内に放射さ
れて、被加熱食品5を加熱する構造となっている。なお
、1は加熱室壁面、4は被加熱食品5をむらなく加熱す
るための回転載置台、6はモータ機構であり、そして7
はその回転を伝達する暉動軸である。
EXAMPLE Below, the structure and operation of an example of the present invention are shown in FIGS. 1 to 5.
This will be explained using figures. In FIG. 1, microwaves generated by a magnetron 3 are guided by a coaxial line composed of an outer conductor 8 and an inner conductor 9, and are guided into a heating chamber 2 by a dielectric plate 10 and a metal plate (hereinafter referred to as a radiation plate) 11. The structure is such that the food to be heated 5 is heated by the radiation. In addition, 1 is a heating chamber wall surface, 4 is a rotating mounting table for evenly heating the food to be heated 5, 6 is a motor mechanism, and 7
is the axle that transmits the rotation.

第2図および第3図は第1図の要部の拡大図である。第
2図において、誘電体板10は加熱室壁面1と放射板1
1にはさまれる形で取り付けられている。加熱室壁面1
には外導体8の内径と等しい径の貫通穴23があけられ
ており、その中央を貫通導体(以下内導体と言う)9が
貫通し、同時に誘電体10をも貫通して放射板11に固
定ねじ12で固定されている。放射板11は第3図に示
すように矩形である。したがって、誘電体板もこれに見
合ってやや大きな矩形である。放射板11は導体である
から、放射板(金属板)を図のように成形して取り付け
てもよく、また、誘電体板10上にあらかじめ蒸着した
導体膜でもよい。放射板(金属板)11に対する固定ね
じの位置は第3図のように、幅Wの中央で。
2 and 3 are enlarged views of the main parts of FIG. 1. In FIG. 2, a dielectric plate 10 is connected to a heating chamber wall surface 1 and a radiation plate 1.
It is attached in a way that it is sandwiched between 1. Heating chamber wall 1
A through hole 23 with a diameter equal to the inner diameter of the outer conductor 8 is bored in the through hole 23 , and a through hole 23 (hereinafter referred to as the inner conductor) passes through the center of the through hole 23 , and at the same time passes through the dielectric 10 to form the radiation plate 11 . It is fixed with a fixing screw 12. The radiation plate 11 is rectangular as shown in FIG. Therefore, the dielectric plate is also relatively large and rectangular. Since the radiation plate 11 is a conductor, the radiation plate (metal plate) may be formed and attached as shown in the figure, or it may be a conductive film deposited on the dielectric plate 10 in advance. The position of the fixing screw relative to the radiation plate (metal plate) 11 is at the center of the width W, as shown in FIG.

端からQの位置に置かれている。It is placed at position Q from the end.

このような構造にすることにより、マイクロ波が加熱室
2内にすみやかに放射される理由を第4図により説明す
る。
The reason why microwaves are quickly radiated into the heating chamber 2 with such a structure will be explained with reference to FIG. 4.

第4図は第2図の構造を概念的に示したものである。し
たがって、第2図の外導体8と加熱室壁面1は一体にし
て接地導体23として示している。
FIG. 4 conceptually shows the structure of FIG. 2. Therefore, the outer conductor 8 and the heating chamber wall surface 1 in FIG. 2 are shown as a ground conductor 23 in one piece.

また、固定ねじ12は省略している。マグネトロン3で
発生したマイクロ波は内導体9と接地導体28で構成さ
れる同軸線路を伝送するが、その時、同軸線路内には1
3.13Aで示される電界が発生する。
Further, the fixing screw 12 is omitted. The microwave generated by the magnetron 3 is transmitted through a coaxial line consisting of an inner conductor 9 and a ground conductor 28, but at that time, there is a
An electric field of 3.13A is generated.

この電界がさらに進行すると図の左右に分かれて。As this electric field progresses further, it splits into the left and right sides of the figure.

電界14,14Aとなる。この時、放射板(金属板)1
1の長さ(第3図の寸法L)が使用周波数の約半波長な
らば共振して、電界は15.15Aで示すごとく外部へ
放射され、やがて16.17のように図の下方へ進行し
て行く。Lの長さは約半波長の時、放射すると述べたが
、詳しくは、 λ。
The electric field becomes 14.14A. At this time, radiation plate (metal plate) 1
If the length of 1 (dimension L in Figure 3) is approximately half the wavelength of the frequency used, it will resonate and the electric field will be radiated to the outside as shown at 15.15A, and will eventually move downward in the figure as shown at 16.17. I'll go. I mentioned that radiation occurs when the length of L is about half a wavelength, but in detail, λ.

L押0・49 ■7(1) である。ただしλ。は使用周波数の波長、εrは誘電体
板10の比誘電率である。また、放射板(金属板)11
の端部からの距@Qは同軸線路から放射板(金属板)1
1側を見た放射インピーダンスを決定する要因で、Qが
小さい程放射インピーダンスは大きくなり、Qが増すと
逆に小さくなる(Q=L/Zで最小)。この放射インピ
ーダンスは同軸線路の特性インピーダンスに等しくする
ことが望ましい。
Press L 0.49 ■7 (1). However, λ. is the wavelength of the frequency used, and εr is the relative dielectric constant of the dielectric plate 10. In addition, the radiation plate (metal plate) 11
The distance from the end of @Q is from the coaxial line to the radiation plate (metal plate) 1
This is a factor that determines the radiation impedance when looking at the 1 side. The smaller Q is, the larger the radiation impedance is, and as Q increases, it becomes smaller (minimum at Q=L/Z). It is desirable that this radiation impedance be equal to the characteristic impedance of the coaxial line.

もし、寸法りが(1)式で示す寸法よりはずれている場
合は共振は起らず、したがって放射されずにマイクロ波
は放射板11の端で反射され、同軸線路側にもどされる
こととなる。したがって、第3図の寸法Wを共振しない
寸法に選ぶことにより、同図の上下方向には放射されず
、左右方向にのみ放射されることとなる。
If the dimensions deviate from the dimensions shown in equation (1), resonance will not occur, and therefore the microwave will not be radiated, but will be reflected at the end of the radiation plate 11 and returned to the coaxial line side. . Therefore, by selecting the dimension W in FIG. 3 to a dimension that does not resonate, the radiation will not be radiated in the vertical direction in the figure, but will be radiated only in the horizontal direction.

このように、本実施例によれば、マイクロ波の加熱室2
内への給電装置を極めて偏平に出来るために、スペース
効率を上げることが可能となると同時に、清掃性も向上
させることができる。なお、本実施例は915MIIz
帯の高周波加熱装置に限るものではなく、2.45GH
z帯の高周波加熱装置にも適用できることは言うまでも
ない。
In this way, according to this embodiment, the microwave heating chamber 2
Since the power feeding device inside can be made extremely flat, space efficiency can be increased, and at the same time, cleaning efficiency can also be improved. Note that this example uses 915MIIz
It is not limited to belt high frequency heating equipment, but is 2.45GH
Needless to say, the present invention can also be applied to a Z-band high-frequency heating device.

さらに1本実施例には次のような利点がある。Furthermore, this embodiment has the following advantages.

第2図において、放射する周波数は(1)式によって決
定されることはすでに述べたが、放射し易い周波数範囲
、すなわち、帯域幅BWは BW=128f0′・九       (2)で表わさ
れる。ただし、BWの単位はMH2,foは使用周波数
で単位はG11z、f−は誘電体板の厚さで、単位はイ
ンチである。この帯域BWをはずれる周波数に対しては
放射しにくくなって反射が増すことは言うまでもない。
In FIG. 2, it has already been mentioned that the radiating frequency is determined by equation (1), but the frequency range where it is easy to radiate, that is, the bandwidth BW is expressed as BW=128f0'·9 (2). However, the unit of BW is MH2, fo is the operating frequency in G11z, and f- is the thickness of the dielectric plate in inches. Needless to say, it becomes difficult to radiate frequencies outside this band BW, and reflection increases.

(1)式から明らかなように、BWは厚さえに比例する
から、光を変えることによって自由にBWを決定するこ
とができる。
As is clear from equation (1), the BW is proportional to the thickness, so the BW can be freely determined by changing the light.

このことは以下に述べるような利点となる。This provides advantages as described below.

一般にマグネトロンは中心周波数f、をはさんで上下の
周波数に比較的レベルの大きい不要な周波数を発振する
。第5図にその様子を示す。20はマグネトロンの発振
スペクトラムである。例えば、2.45GHz帯のマグ
ネトロンではf、は2.45Gllz、その上下にΔf
=zoo〜300MHzの不要な周波数が存在する。周
知のように、この帯域の高周波加熱装置に割当てられて
いる周波数は2.45±0.05Gl−1zであるから
J。±Δfの外部への漏洩は許されない。したがって、
この種の高周波加熱装置の設計に際しては種々の工夫を
必要としていた。しかしながら、本実施例の場合は先に
述べたBWを自由に変えられるから、例えば第5図19
で示すような反射が得られるように、誘電体板10の厚
さを選にば孔±Δfのマイクロ波の放射を抑圧すること
ができる。すなわち、給電装置そのものにフィルタ効果
を持たせることが容易に可能となるわけである。
Generally, a magnetron oscillates unnecessary frequencies with relatively high levels at frequencies above and below the center frequency f. Figure 5 shows the situation. 20 is the oscillation spectrum of the magnetron. For example, in a 2.45GHz band magnetron, f is 2.45Gllz, and Δf is above and below it.
There are unnecessary frequencies from =zoo to 300MHz. As is well known, the frequency assigned to high frequency heating devices in this band is 2.45±0.05Gl-1z. Leakage of ±Δf to the outside is not allowed. therefore,
When designing this type of high-frequency heating device, various measures were required. However, in the case of this embodiment, since the BW mentioned above can be changed freely, for example, as shown in FIG.
If the thickness of the dielectric plate 10 is selected so as to obtain the reflection shown in the figure, it is possible to suppress the microwave radiation of the holes ±Δf. In other words, it is possible to easily provide a filter effect to the power supply device itself.

第6図は本発明の他の実施例である。放射板(金属板)
11に対する内導体9の接続される位置がコーナ寄りに
なっていることと、放射板11の寸法が(1)式で示さ
れるそれと±Δだけ異なった寸法になっている点が第2
図との差異である。このようにして、Δの寸法をうまく
選ぶことにより、放射される電界21と、これと直交す
るtけ界22は大きさが等しく、同時に、位相を90’
ずらすことができるので円偏波を発生させることができ
る。円偏波の発生により、被加熱食品5の加熱ムラを少
なくすることができる。
FIG. 6 shows another embodiment of the invention. Radiation plate (metal plate)
The second point is that the position where the inner conductor 9 is connected to 11 is closer to the corner, and the dimensions of the radiation plate 11 are different from those shown by equation (1) by ±Δ.
This is the difference from the figure. In this way, by judiciously choosing the dimension of Δ, the radiated electric field 21 and the orthogonal t field 22 are of equal magnitude and at the same time have a phase of 90'.
Since it can be shifted, circularly polarized waves can be generated. By generating circularly polarized waves, uneven heating of the heated food 5 can be reduced.

第7図は本発明の更に他の実施例である。これまでの説
明は第1図で述べたように、同軸m路を用いた場合につ
いて説明したが、第7図のごとく、導波管内に設けられ
た結合導体24を放射板(金属板)11に接続すること
によって同様な効果を得ることができる。
FIG. 7 shows yet another embodiment of the present invention. The explanation so far has been given for the case where a coaxial m-path is used as described in FIG. 1, but as shown in FIG. 7, the coupling conductor 24 provided in the waveguide is A similar effect can be obtained by connecting to.

なお、この実施例は一見、特公昭62−59436号公
報の回転アンテナと類似しているが、放射板(金属板)
11の構造並びに放射原理は全く異なるものである。
At first glance, this embodiment is similar to the rotating antenna disclosed in Japanese Patent Publication No. 62-59436, but the radiation plate (metal plate)
The structure and radiation principle of No. 11 are completely different.

第8図は本発明の更に他の実施例である。マグネトロン
アンテナ26と放射板(金yAFi)11を直接接続し
たもので、同軸線路や導波管をはぶいた分だけ、低コス
ト化できる。なお、27.27Aはマグネトロン3を加
熱室壁面に固定するためのねじである。
FIG. 8 shows yet another embodiment of the present invention. The magnetron antenna 26 and the radiation plate (gold YAFi) 11 are directly connected, and the cost can be reduced by eliminating the coaxial line and waveguide. Note that 27.27A is a screw for fixing the magnetron 3 to the wall surface of the heating chamber.

発明の効果 以上述べたごとく、本発明によれば、加熱室のスペース
効率を向上させ、清掃し易くなるばかりではなく、マグ
ネトロンの発生する不要な周波数成分を除去するフィル
タ効果が得られる上に、容易に円偏波を発生できるので
、加熱ムラをも少なくした高周波加熱装置を提供するこ
とができる。
Effects of the Invention As described above, the present invention not only improves the space efficiency of the heating chamber and makes it easier to clean, but also provides a filter effect that removes unnecessary frequency components generated by the magnetron. Since circularly polarized waves can be easily generated, it is possible to provide a high-frequency heating device with reduced heating unevenness.

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

第1図は本発明の一実施例の断面図、第2.第3図は第
1図の要部の拡大図、第4図は本発明の動作説明図、第
5図は本発明のフィルタ効果の説明図、第6、第7、第
8図は本発明の他の実施例を示す図である。 9・・・貫通導体、    10・・・誘電体板、11
・・・金属板(放射板)。
FIG. 1 is a sectional view of one embodiment of the present invention, and FIG. Fig. 3 is an enlarged view of the main part of Fig. 1, Fig. 4 is an explanatory diagram of the operation of the present invention, Fig. 5 is an explanatory diagram of the filter effect of the present invention, and Figs. 6, 7, and 8 are diagrams of the present invention. It is a figure showing other examples of. 9... Penetrating conductor, 10... Dielectric plate, 11
...Metal plate (radiation plate).

Claims (1)

【特許請求の範囲】 1、一辺が使用周波数の略半波長のほぼ正方形の金属板
と加熱室壁面とでこの金属板とほぼ同一形状の誘電体板
をサンドイッチ状にはさみ、この加熱室壁面を貫通する
貫通導体の一端と上記金属板を電気的に接続せしめたこ
とを特徴とする高周波加熱装置。 2、上記貫通導体を、マグネトロンで発生したマイクロ
波を上記加熱室に導くための同軸線路の内導体としたこ
とを特徴とする特許請求の範囲第1項記載の高周波加熱
装置。 3、上記貫通導体を、マグネトロンで発生したマイクロ
波を上記加熱室に導くための導波管内に配置したことを
特徴とする特許請求の範囲第1項記載の高周波加熱装置
。 4、上記貫通導体を上記マグネトロンのアンテナとした
ことを特徴とする特許請求の範囲第1項記載の高周波加
熱装置。
[Claims] 1. A dielectric plate having approximately the same shape as the metal plate is sandwiched between a substantially square metal plate whose sides are approximately half the wavelength of the operating frequency and the heating chamber wall surface, and the heating chamber wall surface is A high-frequency heating device characterized in that one end of a penetrating conductor and the metal plate are electrically connected. 2. The high-frequency heating device according to claim 1, wherein the through conductor is an inner conductor of a coaxial line for guiding microwaves generated by a magnetron to the heating chamber. 3. The high frequency heating device according to claim 1, wherein the through conductor is disposed within a waveguide for guiding microwaves generated by a magnetron to the heating chamber. 4. The high-frequency heating device according to claim 1, wherein the through conductor is an antenna of the magnetron.
JP31036088A 1988-12-08 1988-12-08 High frequency heating equipment Expired - Fee Related JP2736793B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP31036088A JP2736793B2 (en) 1988-12-08 1988-12-08 High frequency heating equipment

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP31036088A JP2736793B2 (en) 1988-12-08 1988-12-08 High frequency heating equipment

Publications (2)

Publication Number Publication Date
JPH02155194A true JPH02155194A (en) 1990-06-14
JP2736793B2 JP2736793B2 (en) 1998-04-02

Family

ID=18004300

Family Applications (1)

Application Number Title Priority Date Filing Date
JP31036088A Expired - Fee Related JP2736793B2 (en) 1988-12-08 1988-12-08 High frequency heating equipment

Country Status (1)

Country Link
JP (1) JP2736793B2 (en)

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2009230881A (en) * 2008-03-19 2009-10-08 Mitsubishi Electric Corp High-frequency heater
JP2009252620A (en) * 2008-04-09 2009-10-29 Panasonic Corp Microwave processing device
WO2010032345A1 (en) * 2008-09-17 2010-03-25 パナソニック株式会社 Microwave heating device
JP5560366B1 (en) * 2013-12-18 2014-07-23 株式会社日立パワーソリューションズ Microwave heating device

Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
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JP2009252620A (en) * 2008-04-09 2009-10-29 Panasonic Corp Microwave processing device
WO2010032345A1 (en) * 2008-09-17 2010-03-25 パナソニック株式会社 Microwave heating device
US8901470B2 (en) 2008-09-17 2014-12-02 Panasonic Corporation Microwave heating apparatus
JP5560366B1 (en) * 2013-12-18 2014-07-23 株式会社日立パワーソリューションズ Microwave heating device

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