JPH0216558B2 - - Google Patents
Info
- Publication number
- JPH0216558B2 JPH0216558B2 JP11371483A JP11371483A JPH0216558B2 JP H0216558 B2 JPH0216558 B2 JP H0216558B2 JP 11371483 A JP11371483 A JP 11371483A JP 11371483 A JP11371483 A JP 11371483A JP H0216558 B2 JPH0216558 B2 JP H0216558B2
- Authority
- JP
- Japan
- Prior art keywords
- frequency
- antenna
- heating chamber
- heated
- reflection
- 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
Links
- 238000010438 heat treatment Methods 0.000 claims description 20
- 239000000284 extract Substances 0.000 claims 1
- 230000007423 decrease Effects 0.000 description 3
- 238000010586 diagram Methods 0.000 description 2
- 230000005684 electric field Effects 0.000 description 2
Landscapes
- Constitution Of High-Frequency Heating (AREA)
Description
【発明の詳細な説明】
産業上の利用分野
本発明はたとえばI.S.M.(工業、科学、医事用)
周波数帯の一つである915MHz帯を使用した高周
波加熱装置にかかり、特に反射電力に弱いトラン
ジスタ等の固体能動素子からなる高周波発生装置
を使用した場合の加熱室の改善に関するものであ
る。[Detailed description of the invention] Industrial application field The present invention is applicable to ISM (industrial, scientific, medical) applications, for example.
This application concerns the improvement of heating chambers when using high-frequency heating devices that use the 915 MHz band, which is one of the frequency bands, and is made of solid-state active elements such as transistors that are particularly susceptible to reflected power.
従来例の構成とその問題点
近年トランジスタ技術の進歩に伴ない、従来広
く使用されて来たマグネトロンに代り高周波発生
装置をトランジスタ等の固体能動素子で構成し、
低電圧化、軽量小型化、長寿命化をはかることが
検討されている。従来高周波加熱装置として広く
民生用に用いられている電子レンジの場合、その
ほとんどが、I.S.M.周波数の1つである2450MHz
を使している。しかしながら、トランジスタの能
力は一般に使用周波数fの1乗から2乗に比例し
て低下すると言われ、2450MHzで大出力、高効率
のトランジスタを作ることは困難が大きい。従つ
てトランジスタ化をはかるには、現在の技術をも
つてしてももう1つのI.S.M.周波数帯である
915MHz帯という低い周波数を使わざるを得ない
のが現状である。Conventional configurations and their problems In recent years, with advances in transistor technology, high-frequency generators have been constructed with solid-state active elements such as transistors, instead of the conventionally widely used magnetrons.
Aiming for lower voltage, lighter weight, smaller size, and longer life is being considered. In the case of microwave ovens, which are conventionally widely used as high-frequency heating devices for consumer use, most of them operate at 2450MHz, which is one of the ISM frequencies.
is using. However, it is generally said that the performance of a transistor decreases in proportion to the first to the second power of the operating frequency f, and it is extremely difficult to produce a transistor with high output and high efficiency at 2450 MHz. Therefore, even with current technology, it is necessary to use another ISM frequency band for transistorization.
Currently, we have no choice but to use the low frequency of the 915MHz band.
ところが、本発明にかかる915MHz帯の周波数
を利用し、トランジスタ等の固体能動素子で構成
した高周波発生装置を使用した場合、第1図に示
すように、高周波発生装置1と加熱室2へ電波を
放出するアンテナ3の間にサーキユレータ4と無
反射終端5を介在させる構成を取るのが一般的で
あつた。このようにマグネトロンで2450MHzを使
用した高周波加熱装置では一般に使用されない。
サーキユレータといつた高価な部品を使うのは、
次の2つの理由による。 However, when using a high-frequency generator constructed of solid-state active elements such as transistors using a frequency in the 915 MHz band according to the present invention, as shown in FIG. It has been common practice to have a configuration in which a circulator 4 and a non-reflection termination 5 are interposed between the emitting antenna 3. Thus, it is generally not used in high-frequency heating devices that use a magnetron at 2450MHz.
Using expensive parts such as circulators is
This is due to the following two reasons.
まず第1の理由は本発明にかかる915MHzとい
う周波数が2450MHzに対して波長が約3倍で、自
由空間波長でいえば33cmもあり、本発明にかかる
一般民生用の高周波加熱装置の場合、その加熱室
の大きさに波長がほぼ対応することにある。この
ため、2450MHzに比較して、加熱室2で共振可能
なモード数が大巾に減少し、従つて被加熱物であ
る負荷が変動するとアンテナ3から5加熱室2側
を見たインピーダンスが大巾に変動する。従つて
加熱室2を設計する際は、できるだけ広い範囲の
負荷に対してインピーダンス整合の取れるよう工
夫はするが、一般に空や空に近い軽負荷状態ま
で、定在波比を低く抑えることは困難である。こ
のため、こうした軽負荷時には、ほとんどの電波
が反射することになる。これに対し、トランジス
タを用いた高周波加熱装置は、マグネトロン以上
に反射電力に弱く、従つてサーキユレータ4を用
いて反射電力を無反射終端5へ吸収させ、高周波
発生装置1へ戻らないようにするためである。 The first reason is that the frequency of 915MHz according to the present invention is about three times the wavelength of 2450MHz, and the free space wavelength is 33 cm. The reason is that the wavelength roughly corresponds to the size of the heating chamber. Therefore, compared to 2450MHz, the number of modes that can resonate in heating chamber 2 is greatly reduced, and therefore, when the load, which is the object to be heated, changes, the impedance of antennas 3 to 5 when looking at the heating chamber 2 side increases. It fluctuates widely. Therefore, when designing the heating chamber 2, efforts are made to achieve impedance matching over a wide range of loads as much as possible, but it is generally difficult to keep the standing wave ratio low even under empty or light load conditions close to empty. It is. Therefore, during such light loads, most of the radio waves are reflected. On the other hand, a high-frequency heating device using a transistor is more susceptible to reflected power than a magnetron, and therefore a circulator 4 is used to absorb the reflected power to the non-reflection terminal 5 to prevent it from returning to the high-frequency generator 1. It is.
しかしながら、このサーキユレータ4は高価な
部品であるばかりでなく、一般の電子レンジのよ
うに何百Wという大電力のものは非常に大型で作
り悪いという問題があつた。 However, this circulator 4 is not only an expensive component, but also has the problem that it is very large and poorly made in the case of a high-power microwave oven of hundreds of watts, such as a general microwave oven.
発明の目的
本発明はかかる従来の問題点を解消するもの
で、サーキユレータといつた高価な部品を使用せ
ずに高周波発生装置への反射電力を低減すること
を目的としたものである。OBJECTS OF THE INVENTION The present invention solves these conventional problems and aims to reduce the reflected power to the high frequency generator without using expensive parts such as circulators.
発明の構成
上記目的を達成するため本発明は、高周波発生
装置で発生した高周波を加熱室内へ導く出力アン
テナ以外に、加熱室からの反射電波を取り出す第
2のアンテナと、このアンテナで取り出した電波
を吸収する無反射終端を設けた構成になつてい
る。Structure of the Invention In order to achieve the above object, the present invention provides, in addition to an output antenna that guides the high frequency waves generated by the high frequency generator into the heating chamber, a second antenna that takes out the reflected radio waves from the heating chamber, and a second antenna that takes out the radio waves taken out by this antenna. It has a configuration with a non-reflection termination that absorbs.
この構成により、軽負荷時に負荷への電波の吸
収量が減つた場合、第2のアンテナを通じて無反
射終端へ電波が吸収され、サーキユレータを使わ
ず高周波発生装置への反射を小さく抑えることに
なる。 With this configuration, when the amount of radio waves absorbed by the load decreases when the load is light, the radio waves are absorbed to the non-reflection termination through the second antenna, and the reflection to the high frequency generator can be suppressed to a small level without using a circulator.
実施例の説明
以下、本発明の一実施例を第2図を用いて説明
する。第2図において、7は第2のアンテナ、8
は無反射終端、6は被加熱物である。DESCRIPTION OF EMBODIMENTS An embodiment of the present invention will be described below with reference to FIG. In FIG. 2, 7 is the second antenna, 8
6 is a non-reflective termination, and 6 is an object to be heated.
負荷となる被加熱物6が大きいとき、アンテナ
3から放出された電波はほとんど被加熱物6に吸
収され加熱室2内の電界強度は小さいため、アン
テナ7から無反射終端8へ吸収される電力はわず
かである。これに対し、被加熱物6が小さくなり
被加熱物6へ吸収される電波が減少するに従い、
加熱室2内の電界強度が大きくなり、アンテナ7
から無反射終端8へ吸収される電力が増大する。
この結果被加熱物6が小さい軽負荷時にも高周波
発振器1への反射電力は低く抑えられる一方、被
加熱物6が大きい場合に無反射終端8へ吸収され
る電力はわずかで、効率の低下も少ない。 When the heated object 6 serving as a load is large, most of the radio waves emitted from the antenna 3 are absorbed by the heated object 6 and the electric field strength inside the heating chamber 2 is small, so that the electric power absorbed from the antenna 7 to the non-reflection terminal 8 is small. is small. On the other hand, as the heated object 6 becomes smaller and the radio waves absorbed by the heated object 6 decrease,
The electric field strength inside the heating chamber 2 increases, and the antenna 7
The power absorbed into the non-reflection termination 8 increases.
As a result, the reflected power to the high-frequency oscillator 1 can be kept low even when the object to be heated 6 is small and under light load, while when the object to be heated 6 is large, the power absorbed by the non-reflection terminal 8 is small, and there is no reduction in efficiency. few.
発明の効果
上記説明のとおり、本発明によれば従来のよう
にサーキユレータといつた高価で構造の複雑な部
品を使用することなく、軽負荷時も高周波発生装
置への反射電力を小さく抑えることができるの
で、安価でしかも信頼性の高い高周波加熱装置
を、トランジスタ等の固体能動素子を用いた高周
波発生装置により実現することができる。Effects of the Invention As explained above, according to the present invention, it is possible to suppress the reflected power to the high frequency generator to a small level even during light loads without using expensive and complicated components such as circulators as in the past. Therefore, an inexpensive and highly reliable high-frequency heating device can be realized by a high-frequency generating device using solid-state active elements such as transistors.
第1図はトランジスタ等の固体能動素子を用い
た高周波発生装置を用いた従来の高周波加熱装置
の構成図、第2図は本発明の一実施例の高周波加
熱装置の構成図である。
1……高周波発生装置、2……加熱室、3……
出力アンテナ、4……サーキユレータ、5……無
反射終端、6……被加熱物、7……受電アンテ
ナ、8……無反射終端。
FIG. 1 is a block diagram of a conventional high-frequency heating device using a high-frequency generator using solid-state active elements such as transistors, and FIG. 2 is a block diagram of a high-frequency heating device according to an embodiment of the present invention. 1... High frequency generator, 2... Heating chamber, 3...
Output antenna, 4... Circulator, 5... Non-reflection termination, 6... Heated object, 7... Power receiving antenna, 8... Non-reflection termination.
Claims (1)
素子からなる高周波発生装置と、被加熱物を収納
する加熱室と、前記高周波発生装置で発生した高
周波を前記加熱室へ導く第1のアンテナと、前記
加熱室内の高周波を取り出す第2アンテナと、取
り出された高周波を吸収する無反射終端とを具備
した高周波加熱装置。1: a high-frequency generator comprising a solid-state active element such as a transistor that generates a high-frequency wave; a heating chamber that stores an object to be heated; a first antenna that guides the high-frequency wave generated by the high-frequency generator to the heating chamber; A high-frequency heating device comprising a second antenna that extracts indoor high-frequency waves and a non-reflection termination that absorbs the extracted high-frequency waves.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP58113714A JPS607096A (en) | 1983-06-23 | 1983-06-23 | High frequency heating device |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP58113714A JPS607096A (en) | 1983-06-23 | 1983-06-23 | High frequency heating device |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS607096A JPS607096A (en) | 1985-01-14 |
| JPH0216558B2 true JPH0216558B2 (en) | 1990-04-17 |
Family
ID=14619286
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP58113714A Granted JPS607096A (en) | 1983-06-23 | 1983-06-23 | High frequency heating device |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS607096A (en) |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2010086697A (en) * | 2008-09-30 | 2010-04-15 | Micro Denshi Kk | Microwave drying device |
-
1983
- 1983-06-23 JP JP58113714A patent/JPS607096A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS607096A (en) | 1985-01-14 |
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