JPS58181292A - High frequency heater - Google Patents

High frequency heater

Info

Publication number
JPS58181292A
JPS58181292A JP6588282A JP6588282A JPS58181292A JP S58181292 A JPS58181292 A JP S58181292A JP 6588282 A JP6588282 A JP 6588282A JP 6588282 A JP6588282 A JP 6588282A JP S58181292 A JPS58181292 A JP S58181292A
Authority
JP
Japan
Prior art keywords
heating chamber
frequency
electric field
standing wave
heating device
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
JP6588282A
Other languages
Japanese (ja)
Other versions
JPS6364874B2 (en
Inventor
博文 吉村
公明 山口
淳三 田中
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.)
Panasonic Holdings Corp
Original Assignee
Matsushita Electric Industrial 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 Matsushita Electric Industrial Co Ltd filed Critical Matsushita Electric Industrial Co Ltd
Priority to JP6588282A priority Critical patent/JPS58181292A/en
Publication of JPS58181292A publication Critical patent/JPS58181292A/en
Publication of JPS6364874B2 publication Critical patent/JPS6364874B2/ja
Granted legal-status Critical Current

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  • Constitution Of High-Frequency Heating (AREA)

Abstract

(57)【要約】本公報は電子出願前の出願データであるた
め要約のデータは記録されません。
(57) [Summary] This bulletin contains application data before electronic filing, so abstract data is not recorded.

Description

【発明の詳細な説明】 本発明は導波管と加熱室とを開口で結合しスタラーを有
する高周波加熱装置に関するものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a high frequency heating device that connects a waveguide and a heating chamber through an opening and has a stirrer.

従来、高周波加熱装置の加熱室に主に垂直方向の電界成
分を有する定在波モードを励振させることは、種々の負
荷に対して安定して定在波モードが励振する為、電子レ
ンジなどの食品を加熱する機器の分布を良くする条件と
しては非常に重要な項目である。しかし第1図のように
高周波発振器3t゛−′ であるマグネトロン1からの高周波電磁波を導波管2を
通じて開口3により加熱室4と結合すると電界5の方向
が開口3で水平方向に変化する為、加熱室2には垂直電
界を有する定在波モードが励振できなかった。
Conventionally, exciting a standing wave mode that mainly has a vertical electric field component in the heating chamber of a high-frequency heating device has been used in microwave ovens, etc., because the standing wave mode is stably excited under various loads. This is a very important condition for improving the distribution of food heating equipment. However, as shown in Fig. 1, when the high-frequency electromagnetic waves from the magnetron 1, which is a high-frequency oscillator 3t'-', are coupled to the heating chamber 4 through the waveguide 2 and the opening 3, the direction of the electric field 5 changes horizontally at the opening 3. , a standing wave mode having a vertical electric field could not be excited in the heating chamber 2.

又、第2図のように導波管2と加熱室4をアンテナ6で
結合すると加熱室4に垂直電界5を有する定在波モード
を励振することは可能である。しかしこの構造は加熱室
4内にアンテナ6の先端が突出てしまい、加熱室4の有
効体積が小さくなるばかりでなくアンテナ6に食品かす
かつくと高周波電界で火花放電が生じることもあった。
Further, when the waveguide 2 and the heating chamber 4 are coupled by an antenna 6 as shown in FIG. 2, it is possible to excite a standing wave mode having a vertical electric field 5 in the heating chamber 4. However, with this structure, the tip of the antenna 6 protrudes into the heating chamber 4, which not only reduces the effective volume of the heating chamber 4, but also causes spark discharge in the high-frequency electric field if the antenna 6 comes into contact with food particles.

又、アンテナ6が必要なので構成が複雑になり、コスト
アップにつながっていた。
Furthermore, since the antenna 6 is required, the configuration becomes complicated, leading to an increase in cost.

又偶数と奇数の電界の強さの変化を有する定在波モード
は、負荷を中央に置いた時、中央が強く加熱さ扛、中央
が電波の吸収などで弱くなるのを補正して分布の均一性
は良いのだが、この定在波モードは加熱室4の中央の電
界がない為、中央がら励振できなかった。1〜たがって
、複数の負荷を置いた場合、そ扛ぞ牡の負荷の加熱度合
が異ってし壕っていた。さらに高周波発振器からの電波
の方向性も生じて、加熱室の高周波発振器の取り付けた
側とその逆側では加熱度合が異なってしまっていた。
In addition, in the standing wave mode, which has a change in electric field strength between even and odd numbers, when the load is placed at the center, the center is strongly heated and the center is weakened due to radio wave absorption, etc., and the distribution is corrected. Although the uniformity was good, this standing wave mode could not be excited from the center because there was no electric field at the center of the heating chamber 4. 1. Therefore, when multiple loads were placed, each load would be heated to a different degree. Furthermore, the directionality of the radio waves from the high-frequency oscillator also occurred, resulting in a difference in the degree of heating between the side of the heating chamber where the high-frequency oscillator was attached and the opposite side.

本発明は導波管の開化により加熱室と結合する構成にお
いて、加熱室内に定在波モードを励振させ、力l熱分布
を良くすることを目的とし1す。
An object of the present invention is to improve the power/heat distribution by exciting a standing wave mode in the heating chamber in a configuration in which the waveguide is connected to the heating chamber by opening the waveguide.

丑だ、垂直電界を持つ定在波モードを励振させる負荷の
変動に対しても安定した分布性能を得ることを目的とす
る。
The purpose is to obtain stable distribution performance even with load fluctuations that excite standing wave modes with vertical electric fields.

上記目的を達する為、本発明は加熱室寸法を定在波モー
ドが共振する寸法としその定在波モードの電界方向及び
位置を、導波管の電界方向及び位置と一致させた寸法の
異なる複数の開口を有することにより、加熱室壁の中央
より励振できない定在波モードを励振し、かつ、高周波
発振器の電波の方向性もなくし複数の負荷を同一に加熱
することも′″cきるものである。
In order to achieve the above object, the present invention provides a plurality of heating chambers with different dimensions in which the dimensions of the heating chamber are such that the standing wave mode resonates, and the electric field direction and position of the standing wave mode are made to match the electric field direction and position of the waveguide. By having this opening, it is possible to excite the standing wave mode that cannot be excited from the center of the heating chamber wall, and also eliminate the directionality of the radio waves of the high frequency oscillator, making it possible to heat multiple loads at the same time. be.

以下、不発明の一実施例について図面に基づき5 ゛’
ニー: 説明する。
Hereinafter, an embodiment of the non-invention will be described based on the drawings.
Nee: Explain.

第3図において、ドア7はハンドル8により開閉自在に
設けらf制(財)つまみ9により高周波発振器であるマ
グネトロン1の発振を制(財)できる。又本実施例はガ
スや電気などで空気をあたため、オーブン料理もできる
」二うになっている為、温度制御つまみ10が設けらn
ている。
In FIG. 3, a door 7 is provided so that it can be opened and closed by a handle 8, and an f-control knob 9 can control the oscillation of a magnetron 1, which is a high frequency oscillator. In addition, since this embodiment is designed to heat the air using gas or electricity and can also be used for cooking in an oven, a temperature control knob 10 is not provided.
ing.

第4図において、高周波発振器であるマグネトロン1か
らの高周波電磁波は導波管2を通り開口3a、3bを通
過して加熱室4内に入る。加熱室4内にはマグネトロン
1や電気部品などを冷却する為のファン11の風が入り
、電波を攪拌するスタラー12を風力で回転して不体外
部へ出ていく。
In FIG. 4, high-frequency electromagnetic waves from a magnetron 1, which is a high-frequency oscillator, pass through a waveguide 2, pass through openings 3a and 3b, and enter a heating chamber 4. Air from a fan 11 for cooling the magnetron 1, electrical parts, etc. enters the heating chamber 4, rotates a stirrer 12 that stirs the radio waves, and exits to the outside of the incorporeal body.

−万加熱室4の寸法は の式に基すいている。ここでλは波長、人+B+Cは加
熱室4の幅、奥行、高さの寸法、m、  n。
- The dimensions of the heating chamber 4 are based on the formula: Here, λ is the wavelength, and Person+B+C are the width, depth, and height dimensions of the heating chamber 4, m, and n.

pはそnぞ扛の方向において生じる定在波モードの電界
の変化の数で整数である。本発明の一実施1例。場合は
。−4,。−5,p−81選ぶよ、λ6ベー二′ =122mmの場合はA=290 mm 、  B=2
90mm程度となる。
p is the number of changes in the electric field of the standing wave mode that occur in each direction of the wave, and is an integer. One example of implementation of the present invention. In case. -4,. -5, choose p-81. If λ6 beanie' = 122 mm, A = 290 mm, B = 2
It will be about 90mm.

第5図は第4図のX−X断面を模式的に示した図である
。第6図において、加熱室4内には定在波モード4,5
.Oモードが生じている。こ扛は幅方向に4つの電界の
変化があり、奥行方向に5つの電界の変化があり、高さ
方向には電界の変化がないので電界5はすべて垂直にな
る。この電界6は模式的に■印や■印で示しており、■
は紙面より上向き■は紙面よジ下向きの状態を示す。4
゜5、  Oモードの加熱パターン部分13はハツチン
グを施した様になり加熱室4の中央が強く加熱を扛る。
FIG. 5 is a diagram schematically showing a cross section taken along line XX in FIG. 4. In FIG. 6, there are standing wave modes 4 and 5 in the heating chamber 4.
.. O mode is occurring. This knife has four electric field changes in the width direction, five electric field changes in the depth direction, and no electric field changes in the height direction, so all electric fields 5 are vertical. This electric field 6 is schematically indicated by ■ or ■.
indicates that the image is facing upwards from the paper surface, and ■ indicates that it is facing downwards from the paper surface. 4
5. The heating pattern portion 13 in the O mode looks like a hatched area, and the center of the heating chamber 4 is heated strongly.

又、加熱パターン部分13は規則的の為、熱電導やスタ
ラー12などの攪拌によりさらに均一に加熱さnる。又
、導波管2は加熱室4内の定住波モードと同一になるよ
うに導波管2の幅を選んでいる。そして開口3a、3b
は複数個設けてあり、そnぞnの電界最大点に位置して
いて開口31Lと開口3bの大きさは少し変えてマグネ
トロン1が7−’ −’ らの電波の指向性による定在波モードの対称性の歪を防
止して、複数の負荷が入っても同一に加熱するようにな
っている。又、開口3a、3bには開口3a、3bに水
平な電界が生じないように短絡部14が設けら扛てお9
垂直電界だけを励振するようになっている。こ扛らを確
認するには厚紙16に感熱材を塗り厚紙15が電界によ
り加熱さt1感熱材の色が変化するので確認することが
できる。たとえば第5図のD−D面に厚紙15を入扛る
と変色する部分16は第6図のようになる。
Furthermore, since the heating pattern portion 13 is regular, it can be heated more uniformly by thermal conduction or stirring by the stirrer 12 or the like. Further, the width of the waveguide 2 is selected so as to be the same as the settled wave mode in the heating chamber 4. and openings 3a, 3b
A plurality of are provided, and each one is located at the maximum electric field point, and the sizes of the aperture 31L and the aperture 3b are slightly changed, so that the magnetron 1 has a standing wave due to the directivity of the radio waves 7-'-' etc. This prevents distortion of mode symmetry and ensures uniform heating even when multiple loads are applied. Further, a short circuit portion 14 is provided in the openings 3a and 3b so that a horizontal electric field is not generated in the openings 3a and 3b.
It is designed to excite only the vertical electric field. To confirm this, a heat-sensitive material is applied to the cardboard 16, and when the cardboard 15 is heated by the electric field, the color of the heat-sensitive material changes at t1. For example, when the cardboard 15 is placed on the surface DD in FIG. 5, the discolored portion 16 becomes as shown in FIG. 6.

以上のように、本発明によtば次の効果を得る。As described above, the present invention provides the following effects.

(1)中央を強くする定在波モードなので負荷の中央が
電波の吸収により加熱が弱くなるのを防いでいて均一度
が良い。
(1) Since it is a standing wave mode that strengthens the center, it prevents the center of the load from becoming weaker in heating due to absorption of radio waves, resulting in good uniformity.

(2)定在波モードの電界に合致した複数の開口を有し
ているのでお互いの開口間での電波の干渉がない。
(2) Since it has a plurality of apertures that match the electric field of the standing wave mode, there is no interference of radio waves between the apertures.

(3)複数の開口の大きさを変えて電波の放射量を調整
しているので、定在波モードの対称性が良くなり、マグ
ネトロンの指向性もなくなるので犬さい負荷でも一方が
強く加熱さ扛たす複数の負荷が不均一に力[1熱さtた
Vすることはない。
(3) Since the amount of radio wave radiation is adjusted by changing the size of multiple apertures, the symmetry of the standing wave mode is improved and the directivity of the magnetron is eliminated, so even with a small load, one side will not heat up strongly. Multiple loads cannot be applied unevenly.

(4)垂@電界だけなので負荷の変化に対して分布の変
化が少ない。
(4) Since there is only a vertical electric field, there is little change in distribution with respect to changes in load.

(5)スタラーなどとの絹合わせてさらに分布性能が向
上する。
(5) Distribution performance is further improved by combining silk with stirrer etc.

(6)学なる開口だけなので構成が非常に簡単な為安価
に製造できる。
(6) Since the structure is very simple since there is only one opening, it can be manufactured at low cost.

(7)定在波モードが生じているので負荷が変動しても
マグネトロンからのインピーダンスの変動が少ないので
出力効率が良い。
(7) Since a standing wave mode occurs, even if the load changes, there is little change in impedance from the magnetron, so output efficiency is good.

(8)負荷のない状態でもカロ熱室内に電波が送9込ま
するので反射が少なくマグネトロンに悪影響を与えない
(8) Even when there is no load, the radio waves are transmitted into the Calothermal chamber, so there is little reflection and there is no adverse effect on the magnetron.

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

第1図は従来の高周波加熱装置の正面断面図、第2図は
従来の他の高周波加熱装置の正面断面図、第3図は不発
明の一実施例である高周波加熱装置の外観斜視図、第4
図は同装置の正面断面図、第5図は同装置の電界の状態
を示す状態図、第6図9 ′”−’ は同装置の高周波電磁波による電界パターンの実験結果
を示す試験紙の状態図である。 1・・・・・・高周波発振器、2・・・・・・導波管、
3a、 3b・・・・・・開口、4・・・・・・加熱室
、14・・・・・・短絡部。 代理人の氏名 弁理士 中 尾 敏 男 ほか1名第1
図 2 第2図 第3図 7  10 第4図 第5図 第6図 6
FIG. 1 is a front sectional view of a conventional high-frequency heating device, FIG. 2 is a front sectional view of another conventional high-frequency heating device, and FIG. 3 is an external perspective view of a high-frequency heating device that is an embodiment of the invention. Fourth
The figure is a front sectional view of the same device, Figure 5 is a state diagram showing the state of the electric field of the same device, and Figure 6 9'''-' is the state of a test paper showing the experimental results of the electric field pattern due to high frequency electromagnetic waves of the same device. It is a figure. 1... High frequency oscillator, 2... Waveguide,
3a, 3b...Opening, 4...Heating chamber, 14...Short circuit part. Name of agent: Patent attorney Toshio Nakao and 1 other person No. 1
Figure 2 Figure 2 Figure 3 Figure 7 10 Figure 4 Figure 5 Figure 6 Figure 6

Claims (1)

【特許請求の範囲】 (1)被加熱物を収納する加熱室と、前記加熱室内に高
周波電磁波を給電する高周波発振器と、前記加熱室と前
記高周波発振器とを結合する導波管とを備え、前記導波
管と前記加熱室とを複数の開口で結合し、前記加熱室内
の定在波モードの電界位置及び方向を前記導波管の電界
方向及び位置と一致させ、前記定在波モードの電界最大
点に前記複数の開口を設ける構成とした高周波加熱装置
。 (2)複数の開口の大きさを異ならせる構成とした特許
請求の範囲第1項記載の高周波加熱装置。 (3)開口に前記導波管の前記高周波電磁波の進行方向
と平行な短絡部を設ける構成とした特許請求の範囲第1
項記載の高周波加熱装置。 (4)複数の開口は加熱室の上面か下面に設ける構成と
した特許請求の範囲第1項記載の高周波加2ベーミ゛ 熱装置。 (6)開口を有する加熱室壁のほぼ中央に、回転するス
タラーの回転軸を設ける構成とした特許請求の範囲第1
項記載の高周波加熱装置。 (6)定在波モードは加熱室の幅方向に偶数個と奥行方
向に奇数個の電界の強さの変化をする構成とした特許請
求の範囲第4項記載の高周波加熱装置。 (′7)定在波モードは に垂直電界を有する構成とし
た特許請求の範囲第1項記載の高周波加熱装置。
[Scope of Claims] (1) A heating chamber for storing an object to be heated, a high-frequency oscillator for feeding high-frequency electromagnetic waves into the heating chamber, and a waveguide for coupling the heating chamber and the high-frequency oscillator, The waveguide and the heating chamber are coupled through a plurality of openings, the electric field position and direction of the standing wave mode in the heating chamber are made to match the electric field direction and position of the waveguide, and the standing wave mode is A high-frequency heating device configured to provide the plurality of openings at the maximum electric field point. (2) The high-frequency heating device according to claim 1, wherein the plurality of openings are configured to have different sizes. (3) Claim 1, wherein the opening is provided with a short-circuit portion parallel to the traveling direction of the high-frequency electromagnetic wave of the waveguide.
The high-frequency heating device described in Section 1. (4) The high-frequency two-beam heating device according to claim 1, wherein the plurality of openings are provided on the upper surface or the lower surface of the heating chamber. (6) Claim 1 in which the rotating shaft of the rotating stirrer is provided approximately at the center of the heating chamber wall having an opening.
The high-frequency heating device described in Section 1. (6) The high-frequency heating device according to claim 4, wherein the standing wave mode is configured to change the strength of an even number of electric fields in the width direction of the heating chamber and an odd number of electric fields in the depth direction. ('7) The high-frequency heating device according to claim 1, wherein the standing wave mode has a vertical electric field.
JP6588282A 1982-04-19 1982-04-19 High frequency heater Granted JPS58181292A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP6588282A JPS58181292A (en) 1982-04-19 1982-04-19 High frequency heater

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP6588282A JPS58181292A (en) 1982-04-19 1982-04-19 High frequency heater

Publications (2)

Publication Number Publication Date
JPS58181292A true JPS58181292A (en) 1983-10-22
JPS6364874B2 JPS6364874B2 (en) 1988-12-13

Family

ID=13299788

Family Applications (1)

Application Number Title Priority Date Filing Date
JP6588282A Granted JPS58181292A (en) 1982-04-19 1982-04-19 High frequency heater

Country Status (1)

Country Link
JP (1) JPS58181292A (en)

Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5628198U (en) * 1980-07-15 1981-03-16

Family Cites Families (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5520604A (en) * 1978-07-28 1980-02-14 Nippon Auto Toroole Kk Rotary biological sewage treating apparatus driven by buoyancy of gas including oxygen

Patent Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5628198U (en) * 1980-07-15 1981-03-16

Also Published As

Publication number Publication date
JPS6364874B2 (en) 1988-12-13

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