JPH0574561A - High frequency heating device - Google Patents
High frequency heating deviceInfo
- Publication number
- JPH0574561A JPH0574561A JP23591591A JP23591591A JPH0574561A JP H0574561 A JPH0574561 A JP H0574561A JP 23591591 A JP23591591 A JP 23591591A JP 23591591 A JP23591591 A JP 23591591A JP H0574561 A JPH0574561 A JP H0574561A
- Authority
- JP
- Japan
- Prior art keywords
- frequency
- heating chamber
- heating
- ghz
- resonance
- 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.)
- Pending
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- Constitution Of High-Frequency Heating (AREA)
Abstract
(57)【要約】
【目的】 本発明は、加熱室の高さを120mm以下に薄
型化しても、高周波エネルギーを加熱室内に導くことが
可能で被加熱物を均一に加熱することを目的とする。
【構成】 加熱室1の高さを120mm以下の立方体状に
形成し、高周波発生装置7で発生させるマイクロ波の周
波数を5.8GHzに設定したことを特徴とする。
(57) [Summary] [Object] The present invention aims to uniformly heat an object to be heated by allowing high-frequency energy to be introduced into the heating chamber even if the height of the heating chamber is reduced to 120 mm or less. To do. [Structure] The heating chamber 1 is formed in a cubic shape with a height of 120 mm or less, and a microwave frequency generated by the high frequency generator 7 is set to 5.8 GHz.
Description
【0001】[0001]
【産業上の利用分野】本発明は、被加熱物を誘電加熱に
より調理する高周波加熱装置に関する。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a high frequency heating device for cooking an object to be heated by dielectric heating.
【0002】[0002]
【従来の技術】高周波加熱装置は、マイクロ波による誘
電加熱のみの単機能型から、電熱加熱装置を内蔵した複
合機能型のものへと発展し、マイクロ波と電熱装置の複
合的な加熱により、きめ細かい調理ができるようになっ
てきている。図3は、従来の複合機能型の高周波加熱装
置を示している。同図において、商用交流電源からの交
流電力が電源回路3により高周波発生装置であるマグネ
トロン2を駆動するのに必要な電力に変換される。マグ
ネトロン2から発生したマイクロ波は、導波管4を通し
て加熱室10内に放射され、低回転するターンテーブル
5上の被加熱物8を誘電加熱するようになっている。6
は魚調理などに使用する電熱加熱用のヒータである。2. Description of the Related Art A high-frequency heating device has evolved from a single-function type in which only dielectric heating by microwaves is used to a multi-function type in which an electric heating device is built in. Fine cooking is becoming possible. FIG. 3 shows a conventional multi-functional high-frequency heating device. In the figure, AC power from a commercial AC power supply is converted by a power supply circuit 3 into power necessary for driving a magnetron 2 which is a high frequency generator. Microwaves generated from the magnetron 2 are radiated into the heating chamber 10 through the waveguide 4 and dielectrically heat the object 8 to be heated on the turntable 5 rotating at a low speed. 6
Is a heater for electric heating used for fish cooking.
【0003】従来の高周波加熱装置は、このような構成
のもとで複合機能調理が実現されていたが、さらに以下
の理由により加熱室10の薄型化が望まれていた。即
ち、被加熱物8の大きさに対して加熱室10の形状が大
きく加熱室10自体の熱損失が無視できないこと、また
電熱加熱用のヒータ6により輻射加熱を行う場合、ヒー
タ6から被加熱物8までの距離が大きく、ヒータ6の加
熱効率が悪いことである。この他、今後予測される高周
波加熱装置の車載化などを考慮すると、加熱室10の薄
型化は益々必要になってくる。これに対し、従来の加熱
室10の高さを単に低くすればよいかというと、マイク
ロ波加熱の点で次のような問題が生じてくる。In the conventional high-frequency heating apparatus, the multi-function cooking is realized under such a structure, but it has been desired to make the heating chamber 10 thinner for the following reasons. That is, the shape of the heating chamber 10 is large relative to the size of the object to be heated 8 and the heat loss of the heating chamber 10 itself cannot be ignored, and when radiant heating is performed by the heater 6 for electric heating, the heater 6 is not heated. The distance to the object 8 is large, and the heating efficiency of the heater 6 is poor. In addition to this, in consideration of future in-vehicle mounting of a high-frequency heating device, the heating chamber 10 needs to be thinner. On the other hand, as to whether the height of the conventional heating chamber 10 should be simply lowered, the following problems arise in terms of microwave heating.
【0004】広く民生用に用いられている高周波加熱装
置は、そのマイクロ波周波数としてI.S.M.(工業
・科学・医療用)周波数バンドの一つである2.45G
Hzを使用している。ところで、加熱室10は直六面体
共振器として考えられ、次式のように共振器形状から決
まる共振周波数で加熱を行っている。A high-frequency heating device widely used for consumer use has a microwave frequency of I.S. S. M. 2.45G which is one of the frequency bands (for industrial, scientific and medical use)
Hz is used. By the way, the heating chamber 10 is considered as a rectangular parallelepiped resonator, and is heated at a resonance frequency determined by the resonator shape as shown in the following equation.
【0005】 f(Hz)=[1/2(ε・μ)1/2 ] ・[(m/W)2 +(n/D)2 +(p/H)2 ]1/2 ここで、W,D,Hは加熱室10の幅、奥行き、高さ
(単位mm)、またε,μは加熱室10内媒体の誘電率、
透磁率である。m,n,pは各方向の電磁界の変化数で
あり、共振モードの次数(零又は正の整数)を示す。F (Hz) = [1/2 (ε · μ) 1/2 ] · [(m / W) 2 + (n / D) 2 + (p / H) 2 ] 1/2 where: W, D, and H are the width, depth, and height (unit: mm) of the heating chamber 10, and ε and μ are the dielectric constants of the medium in the heating chamber 10,
Permeability. m, n, and p are the numbers of changes in the electromagnetic field in each direction, and indicate the order of the resonance mode (zero or a positive integer).
【0006】いま、従来の高周波加熱装置の一例として
W=285mm、D=284mm、H=193mmという加熱
室寸法を考える。ターンテーブル5の回転により加熱室
10のインピーダンスが変化し、これによりマグネトロ
ン2の発振周波数も中心周波数から±20MHz以内で
変化することを考慮すると、この場合、2.45GHz
を中心に±20MHz内にある共振周波数及び共振モー
ドは図4のようになる。図中()内の数字は共振モード
の次数を示す。これに対し、高さを低くすると近接する
共振モード数が減少するか、或いは共振モードが存在し
なくなる。図5はH=81mmにした場合の共振周波数及
び共振モードであるが、±20MHz内に共振モードが
1つしかない。As an example of a conventional high-frequency heating apparatus, consider a heating chamber size of W = 285 mm, D = 284 mm, H = 193 mm. Considering that the rotation of the turntable 5 changes the impedance of the heating chamber 10 and the oscillation frequency of the magnetron 2 also changes within ± 20 MHz from the center frequency, in this case, 2.45 GHz.
The resonance frequency and the resonance mode within ± 20 MHz centering around are as shown in FIG. The numbers in parentheses in the figure indicate the order of the resonance mode. On the other hand, when the height is lowered, the number of resonance modes in proximity to each other is reduced, or the resonance modes do not exist. FIG. 5 shows the resonance frequency and the resonance mode when H = 81 mm, but there is only one resonance mode within ± 20 MHz.
【0007】同じ変動周波数幅でも共振モードは多数あ
る方がよい。即ち、複数のモードの何れかが共振もしく
はそれに近い状態になるため、発振周波数が変っても高
周波エネルギーは加熱室10に導かれ易い。しかも共振
モード毎に電磁界の変化数m,n,pは異なるため、加
熱室10内の電磁界分布は絶えず変化することになり均
一加熱に効果がある。通常、中心周波数付近とその低周
波側及び高周波側とで3つ以上のモード数があるのがよ
いと考えられている。It is better that there are a large number of resonance modes even with the same fluctuating frequency width. That is, since any one of the plurality of modes is in resonance or in a state close to resonance, high-frequency energy is easily guided to the heating chamber 10 even if the oscillation frequency changes. Moreover, since the number of changes m, n, p of the electromagnetic field differs for each resonance mode, the distribution of the electromagnetic field in the heating chamber 10 constantly changes, which is effective for uniform heating. Generally, it is considered preferable that there are three or more modes near the center frequency and on the low frequency side and the high frequency side.
【0008】H=81mmの加熱室10では、図5に示す
ように2.45GHz帯では共振モードが1つしかな
く、マグネトロン2の発振周波数が共振周波数から離れ
た場合、高周波エネルギーが加熱室10に入りにくくな
る。また、電磁界分布が固定されるため、均一加熱がさ
れにくい。上記の幅・奥行の寸法例W=285mm、D=
284mmの場合、H=62mm以下では共振モードはな
い。また、H=62mm以上120mm以下の間では、共振
モード数は2.45GHz±20MHzで最大2つしか
存在しないため、均一加熱の点で不十分である。In the heating chamber 10 of H = 81 mm, there is only one resonance mode in the 2.45 GHz band as shown in FIG. 5, and when the oscillation frequency of the magnetron 2 is far from the resonance frequency, high frequency energy is generated in the heating chamber 10. It becomes difficult to enter. Moreover, since the electromagnetic field distribution is fixed, uniform heating is difficult. Dimension example of the above width and depth W = 285mm, D =
In the case of 284 mm, there is no resonance mode below H = 62 mm. Further, when H = 62 mm or more and 120 mm or less, the number of resonance modes is 2.45 GHz ± 20 MHz, and there are only two resonance modes at maximum, which is insufficient in terms of uniform heating.
【0009】[0009]
【発明が解決しようとする課題】従来の高周波加熱装置
は、加熱室の薄型化を行うため、その高さを120mm以
下にした場合、マイクロ波周波数2.45GHzでは均
一加熱が難しく加熱むらが大きくなる。また高さを62
mm以下まで薄くすると加熱室に高周波エネルギーが入ら
なくなるという問題があった。In the conventional high-frequency heating device, since the heating chamber is made thin, if the height is set to 120 mm or less, uniform heating is difficult at a microwave frequency of 2.45 GHz and heating unevenness is large. Become. The height is 62
If the thickness is reduced to less than mm, there is a problem that high frequency energy cannot enter the heating chamber.
【0010】そこで、本発明は、加熱室の高さを120
mm以下に薄型化しても高周波エネルギーを加熱室内に導
くことができて被加熱物を均一に加熱することができる
高周波加熱装置を提供することを目的とする。Therefore, according to the present invention, the height of the heating chamber is set to 120.
An object of the present invention is to provide a high-frequency heating device that can guide high-frequency energy into the heating chamber even if it is thinned to less than mm, and can uniformly heat an object to be heated.
【0011】[0011]
【課題を解決するための手段】本発明は上記課題を解決
するために、加熱室に収納した被加熱物を高周波発生装
置で発生させたマイクロ波で加熱する高周波加熱装置で
あって、前記加熱室は高さが120mm以下の直方体状に
形成し、前記高周波発生装置で発生させるマイクロ波の
周波数は5.8GHzに設定してなることを要旨とす
る。In order to solve the above problems, the present invention is a high frequency heating apparatus for heating an object to be heated housed in a heating chamber with microwaves generated by a high frequency generating apparatus. The gist is that the chamber is formed in a rectangular parallelepiped shape having a height of 120 mm or less, and the frequency of the microwave generated by the high frequency generator is set to 5.8 GHz.
【0012】[0012]
【作用】高さが120mm以下の薄型の直方体状加熱室の
場合、加熱室の寸法から決まる共振モードは2.45G
Hzよりも5.8GHzの方が多数存在する。したがっ
て、加熱室のインピーダンス変化により高周波発生装置
の発振周波数が変化しても、高周波エネルギーは加熱室
に導かれ易くなり、また、被加熱物の均一加熱が可能と
なる。In the case of a thin rectangular parallelepiped heating chamber with a height of 120 mm or less, the resonance mode determined by the dimensions of the heating chamber is 2.45G.
There are more 5.8 GHz than Hz. Therefore, even if the oscillation frequency of the high frequency generator changes due to the impedance change of the heating chamber, the high frequency energy is easily guided to the heating chamber, and the object to be heated can be uniformly heated.
【0013】[0013]
【実施例】以下、本発明の実施例を図1及び図2に基づ
いて説明する。Embodiments of the present invention will be described below with reference to FIGS.
【0014】なお、図1において前記図3における機器
及び部材等と同一ないし均等のものは、前記と同一符号
を以って示し、重複した説明を省略する。It is to be noted that, in FIG. 1, the same or equivalent parts as the devices and members in FIG. 3 are designated by the same reference numerals as those described above, and the duplicated description will be omitted.
【0015】この実施例では、加熱室1の形状が幅、奥
行は従来と同じでW=285mm、D=284mmである
が、高さがH=81mmで薄型の直方体状に形成されてい
る。また、高周波発生装置であるマグネトロン7の発振
周波数は5.8GHzに設定されている。In this embodiment, the heating chamber 1 has the same width and depth as the conventional one, W = 285 mm and D = 284 mm, but has a height H = 81 mm and is formed in a thin rectangular parallelepiped shape. The oscillation frequency of the magnetron 7, which is a high frequency generator, is set to 5.8 GHz.
【0016】図2は、このような加熱室1の形状に対す
る共振周波数及び共振モードを示している。比較のた
め、マグネトロン7の周波数変動幅は2.45GHzの
場合と同様に±20MHzにしてある。従来の2.45
GHz±20MHzでは、前記図5に示したように共振
モード数は1つしかなかったのに対し、5.8GHz±
高周波側にバランスよく存在している。これにより、マ
グネトロンの発振周波数が変化しても加熱室1に高周波
エネルギーが入りにくくなるということはない。また、
図5と比較して分るように、各共振モードの次数が高
い、即ち、一方向に対する電磁界の変化数が多いため、
2.45GHz±20MHZよりもさらに均一な加熱が
期待できる。5.8GHz±20MHzでは、加熱室1
は、H=26mmまでは3個以上のモード数が存在するた
め、本実施例のように高さを81mmに限定する必要はな
い。FIG. 2 shows the resonance frequency and the resonance mode for the shape of the heating chamber 1 as described above. For comparison, the frequency variation width of the magnetron 7 is set to ± 20 MHz as in the case of 2.45 GHz. Conventional 2.45
At GHz ± 20 MHz, there was only one resonance mode number as shown in FIG. 5, whereas at 5.8 GHz ±
It exists in good balance on the high frequency side. As a result, even if the oscillating frequency of the magnetron changes, it is not difficult for high-frequency energy to enter the heating chamber 1. Also,
As can be seen from comparison with FIG. 5, since the order of each resonance mode is high, that is, the number of changes in the electromagnetic field in one direction is large,
More uniform heating can be expected than 2.45 GHz ± 20 MHZ. At 5.8 GHz ± 20 MHz, heating chamber 1
Since there are three or more modes up to H = 26 mm, it is not necessary to limit the height to 81 mm as in this embodiment.
【0017】[0017]
【発明の効果】以上説明したように、本発明によれば、
高周波発生装置で発生させるマイクロ波の周波数を5.
8GHzに設定したため、加熱室の高さを120mm以下
に薄型化しても、加熱室内の共振モード数が多くなって
高周波エネルギーを加熱室内に導くことができ、また被
加熱物を均一に加熱することができる。As described above, according to the present invention,
The frequency of the microwave generated by the high frequency generator is set to 5.
Since it is set to 8 GHz, even if the height of the heating chamber is reduced to 120 mm or less, the number of resonance modes in the heating chamber increases and high-frequency energy can be introduced into the heating chamber, and the object to be heated is uniformly heated. You can
【図1】本発明に係る高周波加熱装置の実施例の構成を
示す斜視図である。FIG. 1 is a perspective view showing a configuration of an embodiment of a high-frequency heating device according to the present invention.
【図2】本実施例の加熱室形状から決まる5.8GHz
帯の共振周波数及び共振モードを示す図である。FIG. 2 is 5.8 GHz determined from the shape of the heating chamber of this embodiment.
It is a figure which shows the resonance frequency and resonance mode of a band.
【図3】従来の高周波加熱装置の構成を示す斜視図であ
る。FIG. 3 is a perspective view showing a configuration of a conventional high-frequency heating device.
【図4】従来例の加熱室形状から決まる2.45GHz
帯の共振周波数及び共振モードを示す図である。FIG. 4 is 2.45 GHz determined from the shape of the heating chamber of the conventional example.
It is a figure which shows the resonance frequency and resonance mode of a band.
【図5】加熱室を薄型化したとき、その加熱室形状から
決まる2.45GHz帯の共振周波数及び共振モードを
示す図である。FIG. 5 is a diagram showing a resonance frequency and a resonance mode in a 2.45 GHz band determined by the shape of the heating chamber when the heating chamber is made thin.
1 加熱室 7 マグネトロン(高周波発生装置) 8 被加熱物 1 Heating chamber 7 Magnetron (high frequency generator) 8 Object to be heated
Claims (1)
装置で発生させたマイクロ波で加熱する高周波加熱装置
であって、 前記加熱室は高さが120mm以下の直方体状に形成し、
前記高周波発生装置で発生させるマイクロ波の周波数は
5.8GHzに設定してなることを特徴とする高周波加
熱装置。1. A high-frequency heating device for heating an object to be heated housed in a heating chamber with microwaves generated by a high-frequency generator, wherein the heating chamber is formed in a rectangular parallelepiped shape having a height of 120 mm or less,
The high frequency heating device is characterized in that the frequency of the microwave generated by the high frequency generator is set to 5.8 GHz.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP23591591A JPH0574561A (en) | 1991-09-17 | 1991-09-17 | High frequency heating device |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP23591591A JPH0574561A (en) | 1991-09-17 | 1991-09-17 | High frequency heating device |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPH0574561A true JPH0574561A (en) | 1993-03-26 |
Family
ID=16993127
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP23591591A Pending JPH0574561A (en) | 1991-09-17 | 1991-09-17 | High frequency heating device |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0574561A (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| WO2012117677A1 (en) * | 2011-03-02 | 2012-09-07 | 三菱電機株式会社 | Cooking device |
-
1991
- 1991-09-17 JP JP23591591A patent/JPH0574561A/en active Pending
Cited By (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| WO2012117677A1 (en) * | 2011-03-02 | 2012-09-07 | 三菱電機株式会社 | Cooking device |
| CN103403455A (en) * | 2011-03-02 | 2013-11-20 | 三菱电机株式会社 | heating cooker |
| JPWO2012117677A1 (en) * | 2011-03-02 | 2014-07-07 | 三菱電機株式会社 | Cooker |
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