JPS61121285A - Waveguide tube filter for high frequency heater - Google Patents
Waveguide tube filter for high frequency heaterInfo
- Publication number
- JPS61121285A JPS61121285A JP24370784A JP24370784A JPS61121285A JP S61121285 A JPS61121285 A JP S61121285A JP 24370784 A JP24370784 A JP 24370784A JP 24370784 A JP24370784 A JP 24370784A JP S61121285 A JPS61121285 A JP S61121285A
- Authority
- JP
- Japan
- Prior art keywords
- waveguide
- window
- electric field
- window plate
- high frequency
- 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
Links
Landscapes
- 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】
産業上の利用分野
本発明は、電子レンジ等の高周波加熱器に用いられる導
波管フィルタ装置に関するものである。DETAILED DESCRIPTION OF THE INVENTION Field of the Invention The present invention relates to a waveguide filter device used in a high frequency heater such as a microwave oven.
従来の技術
電子レンジ等に用いられる高周波発振@(マグネトロン
)は基本tLf o (915MHzや2450MHz
)の他に高調波nfo(n:整数)電波を発生する。Conventional technology The high frequency oscillation @ (magnetron) used in microwave ovens etc. is basically tLf o (915MHz or 2450MHz
), harmonic nfo (n: integer) radio waves are generated.
これらの高調波は、通信等に悪影響を与えるために抑止
する手段が必要となる。These harmonics adversely affect communications and the like, so a means to suppress them is required.
導波管に周i&選択性をもたせることは解決手段として
有効であり通過帯域性フィルタとして“共振窓”を設け
る構成(特開昭52−56425号公報)(小口「マイ
クロ波およびミリ波回路」P171丸善1964)が提
案されている。Providing frequency i and selectivity to the waveguide is effective as a solution, and a configuration in which a "resonance window" is provided as a passband filter (Japanese Patent Application Laid-Open No. 52-56425) (Oguchi "Microwave and Millimeter Wave Circuits") P171 Maruzen 1964) has been proposed.
発明が解決しようとする問題点
ところが、文献で公知の事実を電子レンジ等に適用する
場合には、導波管の長さが通信用の場合にくらべて管内
波長で故波長程度と短わく、マグネトロンから出た電波
が完全に整のっていない状態での使用をする必要がある
ことや、食品負荷の逮いて不整合状態で使用するためK
、工夫が必要となる。Problems to be Solved by the Invention However, when applying the facts known in the literature to microwave ovens, etc., the length of the waveguide is shorter than that for communication, as the internal wavelength is about the same wavelength. It is necessary to use the radio waves emitted from the magnetron when they are not completely aligned, and because the radio waves emitted from the magnetron must be used in an inconsistent state due to food loads.
, some ingenuity is required.
すなわち“共振窓”の゛取付は方法を工夫しないと、窓
を設けることでかえってマグネトロンからの高調波が出
やすい条件やある高調波には効果があるが別の高調波が
増加する条件をつくることに本発明の導波管フィルタは
導波管(幅a、高さb)にa’Xb’の矩形窓を施こし
た平板の取付は位置を不整合にともなう定圧波の電界強
度との関係で決めてやる工夫をしているものであ′る。In other words, unless you devise a method for installing a "resonant window," installing a window can create conditions where harmonics from the magnetron are more likely to come out, or where it is effective against some harmonics but increases other harmonics. In particular, in the waveguide filter of the present invention, the installation of a flat plate with a rectangular window of a'Xb' on the waveguide (width a, height b) is difficult to achieve due to the electric field strength of the constant pressure wave due to positional mismatch. We are trying to decide based on the relationship.
作 用
上記寸法幅a、高さb、幅a′、高さb′は本質的に次
の関係にある。Function The dimensions width a, height b, width a', and height b' essentially have the following relationship.
λ:基本波foに対する波長
本発明のフィルタは導波管が短かいことと不整合の結果
発生する歪んだ定在波のバクーンを実測し、電界強度の
弱い部分をさけて窓を設けることにより、全ての高調波
に数dB以上の抑止作用をもたせうることを゛実験的に
確認して構成したものである実施例
以下本発明の一実施例の導波管フィルタを図面を参照し
て説明する。第1図に示すように電子レンジは、底板1
、ボディカバ2、加熱室3、導波管4、窓板5、マグネ
トロン6からなりマグネトロン6へは電源7から給電し
ている。加熱室内には受皿8や回転車9があり、駆動軸
10により回転するように受皿10は回転自在に設けら
れている。底板1には脚11が設けである。λ: Wavelength for the fundamental wave fo The filter of the present invention was created by actually measuring the distortion of standing waves that occur as a result of short waveguides and mismatching, and by providing windows to avoid areas where the electric field strength is weak. Embodiment The waveguide filter according to an embodiment of the present invention will be explained with reference to the drawings. do. As shown in Figure 1, the microwave oven has a bottom plate 1
, a body cover 2, a heating chamber 3, a waveguide 4, a window plate 5, and a magnetron 6, and power is supplied to the magnetron 6 from a power source 7. A saucer 8 and a rotary wheel 9 are disposed inside the heating chamber, and the saucer 10 is rotatably provided so as to be rotated by a drive shaft 10. The bottom plate 1 is provided with legs 11.
第2図には導波管壁12及び加熱室壁13に窓11をも
つ窓板5の取付は状態を示している(第1図のA−A矢
視図)。窓板5はビス15により加熱室壁面に固定され
ている。窓板5は電界の強い位置に設けている。第3図
には窓板がないときの導波管の上部からみた導波管内の
電界分布を示している。B点に設けたマグネトロンアン
テナを中心に等電位線が広がる様子が理解できよう。マ
グネトロンからの距離96難のところ(×印)が電界の
弱い位置、(○印)部が強い位置(△印)が中間位置と
なる。負荷は水11である。測定はり1,4の孔を1辺
が2簡の正三角形の頂点に多数配置したパンチング孔を
設は導波管上壁面に長さ4fiの探針を入れて行なった
。信号波にはSGを用い、マグネトロンアンテナとして
は動作点測定用プローグを用いた。FIG. 2 shows how the window plate 5 having the window 11 is installed on the waveguide wall 12 and the heating chamber wall 13 (as viewed along the line A--A in FIG. 1). The window plate 5 is fixed to the heating chamber wall surface with screws 15. The window plate 5 is provided at a position where the electric field is strong. FIG. 3 shows the electric field distribution inside the waveguide when viewed from the top of the waveguide when there is no window plate. You can see how the equipotential lines spread around the magnetron antenna installed at point B. The position where the electric field is 96 degrees away from the magnetron (marked with an x) is the position where the electric field is weak, and the position where the electric field is strong (marked with △) is the intermediate position. The load is water 11. A probe with a length of 4 fi was inserted into the upper wall of the waveguide to form a large number of punched holes in the measurement beams 1 and 4 at the vertices of an equilateral triangle with 2 sides on each side. An SG was used for the signal wave, and a probe for operating point measurement was used as the magnetron antenna.
この関係は負荷の種類で各車変化するが、逆転する程に
は変化しないように通常の電子レンジは設計される。第
4図にはこの様子を正断面fat図(窓板5は省略して
いる)との関係で水負荷11時の電界強度例゛を相対値
でfb1図に示している。Although this relationship varies from vehicle to vehicle depending on the type of load, ordinary microwave ovens are designed so that it does not change to the extent that it is reversed. In FIG. 4, an example of the electric field strength at the time of water load 11 is shown in the fb1 diagram as a relative value in relation to the front cross-sectional fat diagram (the window plate 5 is omitted).
第5図には、基本波2450MHzの電子レンジ(松下
電器製NE−651)セットに窓寸法a=63.6mM
L 、 b’= 81allの窓14を設けた窓板5を
場所を変えて高調波の漏波を測定した結果を窓14がな
い場合との比較で示したグラフである。導波管4はa=
92ffl+11.b=32fifiである。Figure 5 shows a microwave oven set with a fundamental wave of 2450 MHz (Matsushita Electric NE-651) with window size a = 63.6 mm.
It is a graph showing the results of measuring harmonic leakage by changing the location of the window plate 5 provided with the windows 14 of L, b'=81all, in comparison with the case where the windows 14 are not provided. The waveguide 4 is a=
92ffl+11. b=32fifi.
電界の弱い場所に窓板5を設けると(×印のデータ)窓
板5がない場合よりも輻射電力が増加し、電界の強い場
所に窓板5を設けることで基本波fOの2〜6倍高調波
が4〜11 dB位減少していることが読みとれる。同
じセットで窓形状を(a′=65.2M 、 b’=
10.5M)にした場合(a’=70.2゜b’=16
)にした場合も同様の傾向を示す。また、a = 73
ttun 、 b= 31 amの導波管4を有する
試作セットに次の窓寸法の組合わせで”11しても電界
の強い位置に設けた場合に大きなフィルタ効果が。When the window plate 5 is installed in a place where the electric field is weak (data marked with an x), the radiated power increases compared to when there is no window plate 5, and by providing the window plate 5 in a place where the electric field is strong, the radiated power increases from 2 to 6 of the fundamental wave fO. It can be seen that the harmonics are reduced by about 4 to 11 dB. The same set has a window shape (a'=65.2M, b'=
10.5M) (a'=70.2°b'=16
) shows a similar tendency. Also, a = 73
Even if the prototype set with the waveguide 4 with ttun and b = 31 am has the following window size combination of 11, a large filter effect can be obtained when it is installed in a position where the electric field is strong.
確認できた。It could be confirmed.
圃
第6図には、水負荷21を加熱室内に置いたときの動作
点を窓板5なしく・)、窓板5を電界の弱い所(×)、
電界の強い所(○)、中間位置(△)に置いた場合につ
いて示した。導波管長が長く、整合負荷であれば、窓1
4の寸法(a′、b′)を以前に示した関係式で設計す
ることで、窓14け並列共振の“共振窓”として作用し
窓板5の取付は位置で変化しないはずであるが、実際に
は変化している。この結果は窓寸法を以前の関係式で示
される大きさを基本とし電界の強い場所に窓板金膜ける
ことで必らずしも“共振”させなくともフィルタとして
作用することを示している。In Fig. 6 of the field, the operating points when the water load 21 is placed in the heating chamber are shown without the window plate 5 (), with the window plate 5 in a weak electric field (×),
The cases where the electric field is placed in a strong electric field (◯) and in an intermediate position (△) are shown. If the waveguide length is long and the load is matched, window 1
By designing the dimensions (a', b') of 4 using the relational expression shown earlier, the 14 windows will act as a "resonant window" with parallel resonance, and the mounting of the window plate 5 should not change depending on the position. , is actually changing. This result shows that by setting the window size to the size shown by the previous relational expression and placing a window metal film in a place where the electric field is strong, it can act as a filter without necessarily causing "resonance".
実施例は矩形の窓14で示しだが窓形伊は多くの変形例
が考えられる。Although the embodiment shows a rectangular window 14, many variations of the window shape are possible.
発明の効果
以上のように本発明による導波管フィルタは、短かくか
つ不整合で使われる電子レンジの導波管に、定在波の電
界強度の弱いところを避けて窓板を設けることにより、
広範囲の高調波に対して安定したフィルタ効果を生じさ
せることができるものである。Effects of the Invention As described above, the waveguide filter according to the present invention can be realized by providing a window plate in a short and mismatched waveguide of a microwave oven, avoiding areas where the electric field strength of standing waves is weak. ,
It is possible to produce a stable filter effect over a wide range of harmonics.
第1図は本発明の一実施例における電子レンジ正断面図
、第2図は第1図のA−A断面矢視図、第3図は電界分
布図、第4図(alI/i導波管の断面図、第4図(b
)は導波管の各部における電界強度を示す図、第5図は
窓板取付は位置の変化による輻射電力測定値を示す図、
第6図は窓板取付は位置の変化にともなう動作点の変化
を窓板なしの場合との比較で示した図である。
4・・・・導波管、5・・・窓板、14・・・・窓、×
印・・・・・・電界の弱い所。
代理人の氏名 弁理士 中 尾 敏 男 ほか1名第4
図
第5図
gd6rence ylaneFIG. 1 is a front cross-sectional view of a microwave oven according to an embodiment of the present invention, FIG. 2 is a cross-sectional view taken along the line A-A in FIG. 1, FIG. 3 is an electric field distribution diagram, and FIG. Cross-sectional view of the tube, Figure 4 (b
) is a diagram showing the electric field strength at each part of the waveguide, Figure 5 is a diagram showing the measured value of the radiated power due to changes in the position of the window plate installation,
FIG. 6 is a diagram showing the change in the operating point due to the change in position when the window plate is attached, in comparison with the case without the window plate. 4...Waveguide, 5...Window plate, 14...Window, ×
Mark: A place where the electric field is weak. Name of agent: Patent attorney Toshio Nakao and 1 other person No. 4
Figure 5 gd6rence ylane
Claims (3)
導波管内の基本波の電界強度の弱い位置をさけて導波管
壁面に直角に取りつけた高周波加熱装置用導波管フィル
タ装置。(1) A window plate with a window smaller than the cross-sectional shape of the waveguide,
A waveguide filter device for high-frequency heating equipment that is installed at right angles to the waveguide wall, avoiding locations where the electric field strength of the fundamental wave is weak within the waveguide.
幅a、高さbとしたとき、これらの寸法関係を、本質的
に a′/b′=(a/b)/{√[1−(λ/2a)^2
]/√[1−(λ/2a′)^2]}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用導
波管フィルタ装置。(2) When the window is rectangular with dimensions a' in length and b' in width, and the width of the waveguide is a and height b, the relationship between these dimensions is essentially a'/b' = (a/ b)/{√[1-(λ/2a)^2
]/√[1-(λ/2a')^2]} The waveguide filter device for a high-frequency heating device according to claim 1, characterized in that:
強い位置に窓板を取りつけ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用導波管フィルタ装
置。(3) A waveguide filter device for a high-frequency heating device according to claim 1, characterized in that a window plate is attached at a position next to the magnetron antenna where the electric field strength of the fundamental wave is strongest.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP24370784A JPS61121285A (en) | 1984-11-19 | 1984-11-19 | Waveguide tube filter for high frequency heater |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP24370784A JPS61121285A (en) | 1984-11-19 | 1984-11-19 | Waveguide tube filter for high frequency heater |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS61121285A true JPS61121285A (en) | 1986-06-09 |
Family
ID=17107785
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP24370784A Pending JPS61121285A (en) | 1984-11-19 | 1984-11-19 | Waveguide tube filter for high frequency heater |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS61121285A (en) |
-
1984
- 1984-11-19 JP JP24370784A patent/JPS61121285A/en active Pending
Similar Documents
Publication | Publication Date | Title |
---|---|---|
US3767884A (en) | Energy seal for high frequency energy apparatus | |
US4700034A (en) | Electromagnetic energy seal of a microwave oven | |
US4053731A (en) | Microwave energy oven seal | |
JPS6353678B2 (en) | ||
KR890004507B1 (en) | Device for preventing electromagnetic wave in microwaves range | |
JP3786031B2 (en) | High frequency circuit device and transmission / reception device | |
KR900008074B1 (en) | Microwave sealing device | |
US7091457B2 (en) | Meta-surface waveguide for uniform microwave heating | |
JPS61121285A (en) | Waveguide tube filter for high frequency heater | |
US3838368A (en) | Waveguide filter for microwave heating apparatus | |
JP3112023B2 (en) | Microwave application equipment | |
JP3329235B2 (en) | filter | |
EP0809419A2 (en) | Multimode electromagnetic wave energy rejection filter arrangement for a slot waveguide | |
JPH02155194A (en) | Microwave oven | |
JPS5832239Y2 (en) | high frequency heater | |
JPS61237393A (en) | High frequency heater | |
JPS607038Y2 (en) | High frequency heating device | |
JPS60262384A (en) | High frequency heater | |
JPS6070690A (en) | Radio wave sealing device | |
JP3039589U (en) | Microwave integrated circuit case | |
KR0165056B1 (en) | Magnetron apparatus of microwave oven | |
JPS61121284A (en) | Waveguide tube filter for high frequency heater | |
KR890006156Y1 (en) | Heating radiators for microwave apparatus | |
JP3972466B2 (en) | microwave | |
US4542352A (en) | Cavity oscillator with undesired mode absorbing waveguides for linear FM |